From 3a93d9cbe7b37fc4eaaa6311aa22af12614de5fa Mon Sep 17 00:00:00 2001 From: shinkoo Date: Sat, 1 Oct 2022 23:13:37 +0200 Subject: [PATCH] 2005-09-14 --- exforall/100/10010.x4 | 1013 +++++++-------- exforall/100/10029.x4 | 120 +- exforall/101/10166.x4 | 22 +- exforall/102/10231.x4 | 15 +- exforall/103/10307.x4 | 15 +- exforall/103/10355.x4 | 17 +- exforall/106/10629.x4 | 15 +- exforall/107/10704.x4 | 76 +- exforall/108/10842.x4 | 74 +- exforall/109/10927.x4 | 13 +- exforall/111/11165.x4 | 53 +- exforall/117/11739.x4 | 59 +- exforall/120/12021.x4 | 31 +- exforall/121/12162.x4 | 227 ++-- exforall/123/12323.x4 | 113 +- exforall/123/12365.x4 | 43 +- exforall/124/12450.x4 | 43 +- exforall/125/12532.x4 | 41 +- exforall/125/12562.x4 | 63 +- exforall/125/12563.x4 | 46 +- exforall/125/12592.x4 | 37 +- exforall/126/12612.x4 | 39 +- exforall/126/12634.x4 | 541 ++++---- exforall/127/12736.x4 | 2745 +++++++++++++++++++++-------------------- exforall/127/12755.x4 | 275 +++-- exforall/127/12787.x4 | 151 +-- exforall/128/12843.x4 | 130 +- exforall/129/12922.x4 | 54 +- exforall/129/12983.x4 | 35 +- exforall/130/13022.x4 | 29 +- exforall/131/13105.x4 | 139 +-- exforall/133/13336.x4 | 64 +- exforall/133/13359.x4 | 167 +-- exforall/134/13454.x4 | 41 +- exforall/135/13523.x4 | 127 +- exforall/135/13588.x4 | 25 +- exforall/136/13610.x4 | 29 +- exforall/136/13647.x4 | 26 +- exforall/136/13665.x4 | 25 +- exforall/136/13671.x4 | 23 +- exforall/136/13675.x4 | 123 +- exforall/136/13698.x4 | 12 +- exforall/137/13738.x4 | 23 +- exforall/137/13744.x4 | 24 +- exforall/137/13746.x4 | 33 +- exforall/138/13811.x4 | 21 +- exforall/138/13832.x4 | 19 +- exforall/138/13839.x4 | 15 +- exforall/138/13855.x4 | 28 +- exforall/139/13909.x4 | 825 ++++++------- exforall/139/13917.x4 | 25 +- exforall/139/13957.x4 | 27 +- exforall/139/13961.x4 | 37 +- exforall/139/13990.x4 | 19 +- exforall/140/14009.x4 | 48 + exforall/140/14010.x4 | 260 ++++ exforall/140/14011.x4 | 718 +++++++++++ exforall/140/14012.x4 | 109 ++ exforall/140/14013.x4 | 47 + exforall/140/14014.x4 | 148 +++ exforall/140/14015.x4 | 74 ++ exforall/140/14016.x4 | 186 +++ exforall/140/14017.x4 | 46 + exforall/140/14018.x4 | 607 +++++++++ exforall/140/14019.x4 | 54 + exforall/140/14020.x4 | 98 ++ exforall/140/14021.x4 | 501 ++++++++ exforall/140/14022.x4 | 789 ++++++++++++ exforall/140/14023.x4 | 582 +++++++++ exforall/140/14024.x4 | 124 ++ exforall/140/14025.x4 | 62 + exforall/140/14026.x4 | 95 ++ exforall/140/14027.x4 | 241 ++++ exforall/140/14028.x4 | 499 ++++++++ exforall/140/14029.x4 | 37 + exforall/140/14030.x4 | 1195 ++++++++++++++++++ exforall/E06/E0682.x4 | 51 +- exforall/E12/E1277.x4 | 52 +- exforall/E16/E1601.x4 | 97 +- exforall/E16/E1669.x4 | 65 +- exforall/E16/E1670.x4 | 265 ++-- exforall/E17/E1703.x4 | 53 +- exforall/E17/E1711.x4 | 449 ++++--- exforall/E17/E1721.x4 | 136 +- exforall/E17/E1744.x4 | 134 +- exforall/E17/E1750.x4 | 737 ++++++----- exforall/E17/E1769.x4 | 231 ++-- exforall/E18/E1803.x4 | 23 +- exforall/E18/E1860.x4 | 25 +- exforall/E18/E1876.x4 | 199 +++ exforall/E18/E1877.x4 | 116 ++ exforall/E18/E1878.x4 | 127 ++ exforall/E18/E1879.x4 | 111 ++ exforall/E18/E1881.x4 | 142 +++ exforall/E18/E1882.x4 | 129 ++ exforall/E18/E1883.x4 | 1335 ++++++++++++++++++++ exforall/E18/E1884.x4 | 370 ++++++ exforall/E18/E1885.x4 | 121 ++ exforall/E18/E1886.x4 | 1120 +++++++++++++++++ exforall/E18/E1887.x4 | 66 + exforall/E18/E1888.x4 | 155 +++ exforall/E18/E1889.x4 | 245 ++++ exforall/E18/E1890.x4 | 101 ++ exforall/E18/E1891.x4 | 942 ++++++++++++++ exforall/E18/E1892.x4 | 187 +++ exforall/E18/E1893.x4 | 2076 +++++++++++++++++++++++++++++++ exforall/E18/E1894.x4 | 616 +++++++++ exforall/E18/E1895.x4 | 354 ++++++ exforall/E18/E1896.x4 | 189 +++ exforall/E18/E1897.x4 | 784 ++++++++++++ exforall/E18/E1898.x4 | 1216 ++++++++++++++++++ exforall/E18/E1899.x4 | 317 +++++ exforall/E19/E1900.x4 | 1389 +++++++++++++++++++++ exforall/F00/F0079.x4 | 1267 +++++++++++++++++++ exforall/F00/F0087.x4 | 311 +++++ exforall/F00/F0088.x4 | 396 ++++++ exforall/F00/F0089.x4 | 487 ++++++++ exforall/F01/F0145.x4 | 94 ++ exforall/F01/F0157.x4 | 539 ++++++++ exforall/F02/F0231.x4 | 251 ++++ exforall/F02/F0239.x4 | 1373 ++++++++++++++++++++- exforall/F02/F0253.x4 | 419 +++++++ exforall/F02/F0256.x4 | 927 +++++++++++++- exforall/F02/F0258.x4 | 112 ++ exforall/F02/F0259.x4 | 1177 +++++++++++++++++- exforall/F02/F0264.x4 | 175 +++ exforall/F02/F0272.x4 | 96 ++ exforall/F04/F0497.x4 | 860 +++++++++++++ exforall/F05/F0502.x4 | 64 + exforall/F05/F0506.x4 | 1410 +++++++++++++++++++++ exforall/F05/F0534.x4 | 1690 +++++++++++++++++++++++++ exforall/F05/F0570.x4 | 1247 +++++++++++++++++++ exforall/F05/F0578.x4 | 433 +++++++ exforall/F05/F0579.x4 | 162 +++ exforall/F05/F0581.x4 | 64 + exforall/F05/F0586.x4 | 591 +++++++++ exforall/F05/F0595.x4 | 706 +++++++++++ exforall/F05/F0597.x4 | 501 ++++++++ exforall/F05/F0598.x4 | 468 +++++++ exforall/F06/F0608.x4 | 706 +++++++++++ exforall/F06/F0618.x4 | 146 +++ exforall/F06/F0629.x4 | 629 ++++++++++ exforall/F06/F0655.x4 | 959 ++++++++++++++ exforall/F06/F0658.x4 | 494 ++++++++ exforall/F06/F0678.x4 | 101 ++ exforall/F06/F0686.x4 | 93 +- exforall/F06/F0694.x4 | 59 + exforall/F06/F0696.x4 | 686 ++++++++++ exforall/F06/F0697.x4 | 417 +++++++ exforall/F06/F0699.x4 | 123 ++ exforall/F07/F0700.x4 | 1460 ++++++++++++++++++++++ exforall/F07/F0703.x4 | 208 ++++ exforall/F07/F0706.x4 | 534 ++++++++ exforall/F07/F0707.x4 | 212 ++++ exforall/F07/F0708.x4 | 346 ++++++ exforall/F07/F0709.x4 | 1494 ++++++++++++++++++++++ exforall/F07/F0710.x4 | 88 ++ exforall/F07/F0712.x4 | 142 +++ exforall/F07/F0713.x4 | 595 +++++++++ exforall/F07/F0714.x4 | 235 ++++ exforall/F07/F0715.x4 | 813 ++++++++++++ exforall/F07/F0717.x4 | 869 +++++++++++++ exforall/F07/F0719.x4 | 589 +++++++++ exforall/F07/F0720.x4 | 197 +++ exforall/F07/F0722.x4 | 509 ++++++++ exforall/F07/F0724.x4 | 506 ++++++++ exforall/G40/G4001.x4 | 110 ++ exforall/J18/J1880.x4 | 282 +++++ exforall/L00/L0074.x4 | 78 ++ exforall/L00/L0075.x4 | 31 + exforall/L00/L0076.x4 | 57 + exforall/L00/L0077.x4 | 382 ++++++ exforall/L00/L0078.x4 | 241 ++++ exforall/L00/L0079.x4 | 112 ++ exforall/L00/L0080.x4 | 191 +++ exforall/L00/L0081.x4 | 195 +++ exforall/L00/L0082.x4 | 389 ++++++ exforall/L00/L0083.x4 | 1633 ++++++++++++++++++++++++ exforall/L00/L0084.x4 | 61 + exforall/L00/L0085.x4 | 526 ++++++++ exforall/L00/L0086.x4 | 131 ++ exforall/L00/L0087.x4 | 228 ++++ exforall/L00/L0089.x4 | 160 +++ exforall/L00/L0090.x4 | 102 ++ exforall/L00/L0091.x4 | 175 +++ exforall/L00/L0092.x4 | 63 + exforall/L00/L0093.x4 | 43 + exforall/L00/L0094.x4 | 198 +++ exforall/L00/L0095.x4 | 82 ++ exforall/L00/L0096.x4 | 73 ++ exforall/L00/L0097.x4 | 197 +++ exforall/L00/L0098.x4 | 72 ++ exforall/L00/L0099.x4 | 89 ++ exforall/L01/L0100.x4 | 92 ++ exforall/L01/L0101.x4 | 233 ++++ exforall/L01/L0102.x4 | 162 +++ exforall/L01/L0103.x4 | 36 + exforall/L01/L0104.x4 | 490 ++++++++ exforall/R00/R0014.x4 | 556 ++++----- exforall/S00/S0045.x4 | 73 ++ exforall/S00/S0046.x4 | 158 +++ 201 files changed, 60548 insertions(+), 5460 deletions(-) create mode 100644 exforall/140/14009.x4 create mode 100644 exforall/140/14010.x4 create mode 100644 exforall/140/14011.x4 create mode 100644 exforall/140/14012.x4 create mode 100644 exforall/140/14013.x4 create mode 100644 exforall/140/14014.x4 create mode 100644 exforall/140/14015.x4 create mode 100644 exforall/140/14016.x4 create mode 100644 exforall/140/14017.x4 create mode 100644 exforall/140/14018.x4 create mode 100644 exforall/140/14019.x4 create mode 100644 exforall/140/14020.x4 create mode 100644 exforall/140/14021.x4 create mode 100644 exforall/140/14022.x4 create mode 100644 exforall/140/14023.x4 create mode 100644 exforall/140/14024.x4 create mode 100644 exforall/140/14025.x4 create mode 100644 exforall/140/14026.x4 create mode 100644 exforall/140/14027.x4 create mode 100644 exforall/140/14028.x4 create mode 100644 exforall/140/14029.x4 create mode 100644 exforall/140/14030.x4 create mode 100644 exforall/E18/E1876.x4 create mode 100644 exforall/E18/E1877.x4 create mode 100644 exforall/E18/E1878.x4 create mode 100644 exforall/E18/E1879.x4 create mode 100644 exforall/E18/E1881.x4 create mode 100644 exforall/E18/E1882.x4 create mode 100644 exforall/E18/E1883.x4 create mode 100644 exforall/E18/E1884.x4 create mode 100644 exforall/E18/E1885.x4 create mode 100644 exforall/E18/E1886.x4 create mode 100644 exforall/E18/E1887.x4 create mode 100644 exforall/E18/E1888.x4 create mode 100644 exforall/E18/E1889.x4 create mode 100644 exforall/E18/E1890.x4 create mode 100644 exforall/E18/E1891.x4 create mode 100644 exforall/E18/E1892.x4 create mode 100644 exforall/E18/E1893.x4 create mode 100644 exforall/E18/E1894.x4 create mode 100644 exforall/E18/E1895.x4 create mode 100644 exforall/E18/E1896.x4 create mode 100644 exforall/E18/E1897.x4 create mode 100644 exforall/E18/E1898.x4 create mode 100644 exforall/E18/E1899.x4 create mode 100644 exforall/E19/E1900.x4 create mode 100644 exforall/F00/F0079.x4 create mode 100644 exforall/F00/F0087.x4 create mode 100644 exforall/F00/F0088.x4 create mode 100644 exforall/F00/F0089.x4 create mode 100644 exforall/F01/F0145.x4 create mode 100644 exforall/F01/F0157.x4 create mode 100644 exforall/F02/F0231.x4 create mode 100644 exforall/F02/F0253.x4 create mode 100644 exforall/F02/F0258.x4 create mode 100644 exforall/F02/F0264.x4 create mode 100644 exforall/F02/F0272.x4 create mode 100644 exforall/F04/F0497.x4 create mode 100644 exforall/F05/F0502.x4 create mode 100644 exforall/F05/F0506.x4 create mode 100644 exforall/F05/F0534.x4 create mode 100644 exforall/F05/F0570.x4 create mode 100644 exforall/F05/F0578.x4 create mode 100644 exforall/F05/F0579.x4 create mode 100644 exforall/F05/F0581.x4 create mode 100644 exforall/F05/F0586.x4 create mode 100644 exforall/F05/F0595.x4 create mode 100644 exforall/F05/F0597.x4 create mode 100644 exforall/F05/F0598.x4 create mode 100644 exforall/F06/F0608.x4 create mode 100644 exforall/F06/F0618.x4 create mode 100644 exforall/F06/F0629.x4 create mode 100644 exforall/F06/F0655.x4 create mode 100644 exforall/F06/F0658.x4 create mode 100644 exforall/F06/F0678.x4 create mode 100644 exforall/F06/F0694.x4 create mode 100644 exforall/F06/F0696.x4 create mode 100644 exforall/F06/F0697.x4 create mode 100644 exforall/F06/F0699.x4 create mode 100644 exforall/F07/F0700.x4 create mode 100644 exforall/F07/F0703.x4 create mode 100644 exforall/F07/F0706.x4 create mode 100644 exforall/F07/F0707.x4 create mode 100644 exforall/F07/F0708.x4 create mode 100644 exforall/F07/F0709.x4 create mode 100644 exforall/F07/F0710.x4 create mode 100644 exforall/F07/F0712.x4 create mode 100644 exforall/F07/F0713.x4 create mode 100644 exforall/F07/F0714.x4 create mode 100644 exforall/F07/F0715.x4 create mode 100644 exforall/F07/F0717.x4 create mode 100644 exforall/F07/F0719.x4 create mode 100644 exforall/F07/F0720.x4 create mode 100644 exforall/F07/F0722.x4 create mode 100644 exforall/F07/F0724.x4 create mode 100644 exforall/G40/G4001.x4 create mode 100644 exforall/J18/J1880.x4 create mode 100644 exforall/L00/L0074.x4 create mode 100644 exforall/L00/L0075.x4 create mode 100644 exforall/L00/L0076.x4 create mode 100644 exforall/L00/L0077.x4 create mode 100644 exforall/L00/L0078.x4 create mode 100644 exforall/L00/L0079.x4 create mode 100644 exforall/L00/L0080.x4 create mode 100644 exforall/L00/L0081.x4 create mode 100644 exforall/L00/L0082.x4 create mode 100644 exforall/L00/L0083.x4 create mode 100644 exforall/L00/L0084.x4 create mode 100644 exforall/L00/L0085.x4 create mode 100644 exforall/L00/L0086.x4 create mode 100644 exforall/L00/L0087.x4 create mode 100644 exforall/L00/L0089.x4 create mode 100644 exforall/L00/L0090.x4 create mode 100644 exforall/L00/L0091.x4 create mode 100644 exforall/L00/L0092.x4 create mode 100644 exforall/L00/L0093.x4 create mode 100644 exforall/L00/L0094.x4 create mode 100644 exforall/L00/L0095.x4 create mode 100644 exforall/L00/L0096.x4 create mode 100644 exforall/L00/L0097.x4 create mode 100644 exforall/L00/L0098.x4 create mode 100644 exforall/L00/L0099.x4 create mode 100644 exforall/L01/L0100.x4 create mode 100644 exforall/L01/L0101.x4 create mode 100644 exforall/L01/L0102.x4 create mode 100644 exforall/L01/L0103.x4 create mode 100644 exforall/L01/L0104.x4 create mode 100644 exforall/S00/S0045.x4 create mode 100644 exforall/S00/S0046.x4 diff --git a/exforall/100/10010.x4 b/exforall/100/10010.x4 index 297ea9e6d..a21633d58 100644 --- a/exforall/100/10010.x4 +++ b/exforall/100/10010.x4 @@ -1,6 +1,6 @@ -ENTRY 10010 19990617 19990622 -SUBENT 10010001 19990617 19990622 -BIB 8 19 +ENTRY 10010 20050707 20050909 1336 +SUBENT 10010001 20050707 20050909 1336 +BIB 8 21 INSTITUTE (1USAANL,3SAFPEL) REFERENCE (J,NSE,41,63,197007) (R,ANL-7636,196911) @@ -20,9 +20,11 @@ HISTORY (19740612C) (19850307A) Subentry 10 deleted, duplicate of subentry 7. BIB correction. (19931229U) Converted to lower case -ENDBIB 19 + (20050707C) DR Legendre coefficient divided by 1000 + to follow ANL report (subentry 3) +ENDBIB 21 NOCOMMON 0 0 -ENDSUBENT 22 +ENDSUBENT 24 SUBENT 10010002 19990617 19990622 BIB 9 13 REACTION (83-BI-209(N,EL)83-BI-209,,SIG) @@ -145,7 +147,7 @@ MEV B NO-DIM 1.500 4.93 2. ENDDATA 98 ENDSUBENT 120 -SUBENT 10010003 19990617 19990622 +SUBENT 10010003 19990617 20050909 1336 BIB 9 14 REACTION (83-BI-209(N,EL)83-BI-209,,DA,,LEG/RS) METHOD (TOF) Time-of-flight @@ -170,433 +172,433 @@ ENDCOMMON 3 DATA 5 427 NUMBER EN DATA DATA-ERR MISC NO-DIM MEV NO-DIM NO-DIM NO-DIM - 1. .300 414. 55. - 1. .340 415. 84. - 1. .344 283. 81. - 1. .400 400. 88. - 1. .405 322. 89. - 1. .420 457. 83. - 1. .450 309. 88. - 1. .460 464. 58. - 1. .480 448. 61. - 1. .490 397. 78. - 1. .505 404. 69. - 1. .515 424. 66. - 1. .540 403. 66. - 1. .545 555. 61. - 1. .560 332. 64. - 1. .565 289. 65. - 1. .580 303. 61. - 1. .600 370. 68. 1. - 1. .600 389. 62. 2. - 1. .600 346. 69. 3. - 1. .605 280. 65. - 1. .620 494. 62. - 1. .640 450. 68. - 1. .650 547. 65. - 1. .660 484. 62. - 1. .680 518. 68. - 1. .700 370. 68. 1. - 1. .700 430. 66. 2. - 1. .720 474. 65. - 1. .740 490. 69. - 1. .750 344. 66. - 1. .760 585. 60. - 1. .775 552. 60. - 1. .780 484. 69. - 1. .800 598. 63. - 1. .820 557. 64. - 1. .825 482. 60. - 1. .840 461. 60. - 1. .850 609. 66. 1. - 1. .850 535. 54. 2. - 1. .855 498. 63. - 1. .860 507. 68. - 1. .875 595. 71. - 1. .880 553. 65. - 1. .900 403. 67. 1. - 1. .900 469. 63. 2. - 1. .900 409. 61. 3. - 1. .900 520. 68. 4. - 1. .900 388. 60. 5. - 1. .920 494. 60. - 1. .925 585. 58. 1. - 1. .925 674. 60. 2. - 1. .940 564. 60. 1. - 1. .940 575. 60. 2. - 1. .950 561. 70. 1. - 1. .950 549. 60. 2. - 1. .960 500. 60. 1. - 1. .960 524. 60. 2. - 1. .975 653. 104. 1. - 1. .975 546. 91. 2. - 1. .980 495. 100. 1. - 1. .980 484. 109. 2. - 1. 1.000 545. 147. 1. - 1. 1.000 601. 70. 2. - 1. 1.000 416. 139. 3. - 1. 1.020 590. 131. 1. - 1. 1.020 529. 134. 2. - 1. 1.025 577. 98. - 1. 1.040 638. 137. 1. - 1. 1.040 587. 132. 2. - 1. 1.050 619. 113. 1. - 1. 1.050 612. 139. 2. - 1. 1.060 524. 136. 1. - 1. 1.060 598. 134. 2. - 1. 1.080 573. 60. - 1. 1.100 775. 90. - 1. 1.150 699. 130. - 1. 1.200 695. 127. - 1. 1.250 770. 129. - 1. 1.300 780. 136. - 1. 1.350 600. 160. - 1. 1.380 867. 131. 1. - 1. 1.380 807. 131. 2. - 1. 1.400 883. 131. 1. - 1. 1.400 688. 148. 2. - 1. 1.400 862. 131. 3. - 1. 1.420 746. 138. 1. - 1. 1.420 826. 135. 2. - 1. 1.440 804. 139. 1. - 1. 1.440 751. 130. 2. - 1. 1.450 858. 143. 1. - 1. 1.450 738. 161. 2. - 1. 1.450 875. 122. 3. - 1. 1.460 542. 151. - 1. 1.500 915. 107. 1. - 1. 1.500 1033. 105. 2. - 2. .300 318. 81. - 2. .340 69. 81. - 2. .344 267. 80. - 2. .400 129. 56. - 2. .405 325. 86. - 2. .420 98. 122. - 2. .450 440. 60. 1. - 2. .460 254. 61. - 2. .480 222. 75. - 2. .490 484. 111. - 2. .505 254. 61. - 2. .515 296. 64. - 2. .540 273. 64. - 2. .545 489. 86. - 2. .560 386. 66. - 2. .565 365. 67. - 2. .580 454. 61. - 2. .600 413. 64. 1. - 2. .600 405. 71. 2. - 2. .600 375. 66. 3. - 2. .605 358. 68. - 2. .620 421. 67. - 2. .640 497. 61. - 2. .650 589. 60. - 2. .660 472. 63. - 2. .680 446. 67. - 2. .700 461. 69. 1. - 2. .700 438. 65. 2. - 2. .720 470. 61. - 2. .740 466. 57. - 2. .750 412. 53. - 2. .760 513. 58. 1. - 2. .760 476. 61. 2. - 2. .775 409. 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9.08E-01 1.22E-01 1. + 3. 1.000 8.23E-01 1.69E-01 2. + 3. 1.000 8.61E-01 1.86E-01 3. + 3. 1.020 9.43E-01 1.31E-01 1. + 3. 1.020 8.31E-01 1.43E-01 2. + 3. 1.025 8.27E-01 1.72E-01 + 3. 1.040 9.37E-01 1.30E-01 1. + 3. 1.040 8.69E-01 1.34E-01 2. + 3. 1.050 1.01E+00 1.36E-01 1. + 3. 1.050 9.35E-01 1.97E-01 2. + 3. 1.060 9.51E-01 1.42E-01 1. + 3. 1.060 9.01E-01 1.47E-01 2. + 3. 1.080 1.01E+00 1.04E-01 + 3. 1.100 9.46E-01 1.62E-01 + 3. 1.150 1.19E+00 1.55E-01 + 3. 1.200 1.13E+00 1.48E-01 + 3. 1.250 1.23E+00 1.56E-01 + 3. 1.300 1.22E+00 1.64E-01 + 3. 1.350 1.28E+00 1.00E-01 + 3. 1.380 1.36E+00 1.55E-01 1. + 3. 1.380 1.34E+00 1.55E-01 2. + 3. 1.400 1.16E+00 1.87E-01 1. + 3. 1.400 1.50E+00 1.56E-01 2. + 3. 1.400 1.50E+00 1.55E-01 3. + 3. 1.420 1.29E+00 1.68E-01 1. + 3. 1.420 1.31E+00 1.65E-01 2. + 3. 1.440 1.46E+00 1.37E-01 1. + 3. 1.440 1.45E+00 1.38E-01 2. + 3. 1.450 1.53E+00 1.10E-01 1. + 3. 1.450 1.61E+00 2.21E-01 2. + 3. 1.450 1.42E+00 7.80E-02 3. + 3. 1.460 1.35E+00 1.92E-01 + 3. 1.500 1.52E+00 1.05E-01 1. + 3. 1.500 1.58E+00 8.20E-02 2. + 4. .300 6.60E-02 7.10E-02 + 4. .340 2.00E-02 8.50E-02 + 4. .344 4.20E-02 8.20E-02 + 4. .400 7.40E-02 9.10E-02 + 4. .405 3.00E-02 8.00E-02 + 4. .420 1.31E-01 2.00E-01 + 4. .450 1.73E-01 5.70E-02 + 4. .460 1.11E-01 5.70E-02 + 4. .480 7.90E-02 1.23E-01 + 4. .490 7.80E-02 1.52E-01 + 4. .505 1.50E-01 6.90E-02 + 4. .515 0.00E+00 6.00E-02 + 4. .540 6.60E-02 6.00E-02 + 4. .545 2.90E-02 1.21E-01 + 4. .560 -6.00E-03 6.90E-02 + 4. .565 1.28E-01 6.20E-02 + 4. .580 3.30E-02 6.10E-02 + 4. .600 -5.80E-02 6.40E-02 1. + 4. .600 1.23E-01 9.60E-02 2. + 4. .600 8.90E-02 1.17E-01 3. + 4. .605 1.34E-01 6.60E-02 + 4. .620 4.50E-02 7.80E-02 + 4. .640 1.90E-02 6.80E-02 + 4. .650 1.12E-01 6.10E-02 + 4. .660 4.10E-02 6.40E-02 + 4. .680 -2.10E-02 6.40E-02 + 4. .700 2.30E-02 6.40E-02 1. + 4. .700 1.35E-01 6.60E-02 2. + 4. .720 3.80E-02 8.40E-02 + 4. .740 2.40E-02 9.50E-02 + 4. .750 1.02E-01 8.90E-02 + 4. .760 5.40E-02 9.50E-02 + 4. .775 2.49E-01 6.70E-02 + 4. .780 1.61E-01 6.90E-02 + 4. .800 1.71E-01 6.70E-02 + 4. .820 2.45E-01 6.90E-02 + 4. .825 2.72E-01 1.19E-01 + 4. .840 6.50E-02 9.70E-02 + 4. .850 1.65E-01 7.10E-02 1. + 4. .850 2.92E-01 1.33E-01 2. + 4. .855 3.19E-01 1.05E-01 + 4. .860 1.58E-01 9.20E-02 + 4. .875 1.30E-01 1.42E-01 + 4. .880 2.91E-01 6.10E-02 + 4. .900 6.00E-02 1.03E-01 1. + 4. .900 2.27E-01 9.20E-02 2. + 4. .900 6.10E-02 6.00E-02 3. + 4. .900 5.10E-02 7.50E-02 4. + 4. .900 2.07E-01 6.30E-02 5. + 4. .920 2.04E-01 6.00E-02 + 4. .925 3.41E-01 1.40E-01 1. + 4. .925 2.17E-01 1.74E-01 2. + 4. .940 1.38E-01 6.00E-02 1. + 4. .940 2.33E-01 6.00E-02 2. + 4. .950 3.41E-01 7.00E-02 1. + 4. .950 3.37E-01 1.45E-01 2. + 4. .960 1.20E-01 6.00E-02 1. + 4. .960 1.15E-01 6.00E-02 2. + 4. .975 2.42E-01 1.08E-01 1. + 4. .975 4.21E-01 2.18E-01 2. + 4. .980 1.31E-01 1.01E-01 1. + 4. .980 7.20E-02 1.09E-01 2. + 4. 1.000 3.95E-01 1.68E-01 1. + 4. 1.000 2.13E-01 1.95E-01 2. + 4. 1.000 4.22E-01 1.15E-01 3. + 4. 1.020 5.84E-01 1.38E-01 1. + 4. 1.020 1.84E-01 1.59E-01 2. + 4. 1.025 3.72E-01 2.36E-01 + 4. 1.040 5.17E-01 1.38E-01 1. + 4. 1.040 9.90E-02 1.36E-01 2. + 4. 1.050 3.91E-01 1.37E-01 1. + 4. 1.050 5.21E-01 2.71E-01 2. + 4. 1.060 9.70E-02 1.58E-01 1. + 4. 1.060 5.00E-01 1.63E-01 2. + 4. 1.080 1.20E-01 2.43E-01 + 4. 1.100 3.45E-01 1.80E-01 + 4. 1.150 5.75E-01 1.61E-01 + 4. 1.200 3.22E-01 1.54E-01 + 4. 1.250 5.24E-01 1.58E-01 + 4. 1.300 5.80E-01 1.71E-01 + 4. 1.350 5.20E-01 1.30E-01 + 4. 1.380 6.09E-01 1.70E-01 1. + 4. 1.380 6.42E-01 1.70E-01 2. + 4. 1.400 5.24E-01 1.96E-01 1. + 4. 1.400 7.08E-01 1.71E-01 2. + 4. 1.400 7.20E-01 1.70E-01 3. + 4. 1.420 6.26E-01 1.86E-01 1. + 4. 1.420 6.44E-01 1.87E-01 2. + 4. 1.440 7.05E-01 1.32E-01 1. + 4. 1.440 6.77E-01 1.33E-01 2. + 4. 1.450 7.95E-01 1.48E-01 1. + 4. 1.450 8.34E-01 2.45E-01 2. + 4. 1.450 7.83E-01 1.05E-01 3. + 4. 1.460 8.39E-01 1.17E-01 + 4. 1.500 9.03E-01 1.40E-01 1. + 4. 1.500 6.57E-01 9.20E-02 2. + 5. .940 3.50E-02 6.00E-02 1. + 5. .940 4.40E-02 6.70E-02 2. + 5. .950 2.90E-02 7.00E-02 1. + 5. .950 0.00E+00 5.00E-02 2. + 5. .960 5.70E-02 7.20E-02 1. + 5. .960 0.00E+00 6.00E-02 2. + 5. .975 -1.30E-02 1.09E-01 1. + 5. .975 0.00E+00 8.00E-02 2. + 5. .980 4.80E-02 1.09E-01 1. + 5. .980 0.00E+00 1.50E-01 2. + 5. 1.000 0.00E+00 1.30E-01 1. + 5. 1.000 0.00E+00 1.70E-01 2. + 5. 1.000 0.00E+00 8.00E-02 3. + 5. 1.020 0.00E+00 1.40E-01 1. + 5. 1.020 0.00E+00 1.60E-01 2. + 5. 1.025 0.00E+00 1.00E-01 + 5. 1.040 1.08E-01 1.52E-01 1. + 5. 1.040 4.00E-02 1.35E-01 2. + 5. 1.050 0.00E+00 5.00E-02 1. + 5. 1.050 -1.70E-02 1.38E-01 2. + 5. 1.060 0.00E+00 1.50E-01 + 5. 1.080 0.00E+00 1.00E-01 + 5. 1.100 -4.90E-02 1.85E-01 + 5. 1.150 7.80E-02 1.62E-01 + 5. 1.200 -7.40E-02 1.55E-01 + 5. 1.250 -3.30E-02 1.60E-01 + 5. 1.300 -1.87E-01 1.73E-01 + 5. 1.350 -1.00E-02 1.20E-01 + 5. 1.380 1.25E-01 1.97E-01 1. + 5. 1.380 1.38E-01 1.97E-01 2. + 5. 1.400 1.99E-01 1.99E-01 1. + 5. 1.400 2.00E-01 1.98E-01 2. + 5. 1.400 -2.22E-01 1.99E-01 3. + 5. 1.420 -8.40E-02 1.20E-01 1. + 5. 1.420 0.00E+00 5.00E-02 2. + 5. 1.440 1.26E-01 1.30E-01 1. + 5. 1.440 1.26E-01 3.20E-02 2. + 5. 1.450 2.82E-01 2.51E-01 1. + 5. 1.450 0.00E+00 5.00E-02 2. + 5. 1.450 0.00E+00 4.00E-02 3. + 5. 1.460 2.24E-01 1.60E-01 + 5. 1.500 0.00E+00 1.00E-01 1. + 5. 1.500 3.90E-02 9.30E-02 2. ENDDATA 429 ENDSUBENT 452 SUBENT 10010004 19990617 19990622 @@ -681,7 +683,7 @@ ADEG MEV MB/SR MB/SR 150. 1.233 12.6 1.1 ENDDATA 64 ENDSUBENT 80 -SUBENT 10010005 19990617 19990622 +SUBENT 10010005 19990617 20050909 1336 BIB 6 8 REACTION (83-BI-209(N,INL)83-BI-209,PAR,DA,,LEG/RS) MONITOR (6-C-0(N,EL)6-C-0,,DA) Elastic from ANL-5567 (Rev) @@ -701,7 +703,7 @@ DATA 4 14 NUMBER EN DATA DATA-ERR NO-DIM MEV NO-DIM NO-DIM 1. 1.090 -0.096 0.069 - 1. 1.140 -0.101 0.071 + 1. 1.140 -0.101 0.071 1. 1.170 -0.012 0.091 1. 1.195 -0.065 0.085 1. 1.213 -0.176 0.081 @@ -716,8 +718,8 @@ NO-DIM MEV NO-DIM NO-DIM 2. 1.306 0.004 0.098 ENDDATA 16 ENDSUBENT 33 -SUBENT 10010006 19990617 19990622 -BIB 5 7 +SUBENT 10010006 20050707 20050909 1336 +BIB 5 8 REACTION (83-BI-209(N,INL)83-BI-209,PAR,DA) MONITOR (6-C-0(N,EL)6-C-0,,DA) Elastic from ANL-5567 (Rev) CORRECTION Corrected for multiple scattering. @@ -725,7 +727,8 @@ ERR-ANALYS Data error given does not include uncertainty in C standard. HISTORY (19850307A) Data heading corrected. (19931229A) MONITOR SF4 added. -ENDBIB 7 + (20050707C) DR Format updated +ENDBIB 8 COMMON 3 3 E-LVL E-RSL ANG KEV KEV ADEG @@ -734,74 +737,74 @@ ENDCOMMON 3 DATA 3 66 EN DATA DATA-ERR KEV MB/SR MB/SR - 0.1020 +04 0.400 +01 0.10 +01 - 0.1040 +04 0.610 +01 0.70 +00 - 0.1050 +04 0.670 +01 0.70 +00 - 0.1060 +04 0.620 +01 0.60 +00 - 0.1070 +04 0.740 +01 0.60 +00 - 0.1080 +04 0.880 +01 0.60 +00 - 0.1085 +04 0.102 +02 0.80 +00 - 0.1090 +04 0.120 +02 0.90 +00 - 0.1100 +04 0.910 +01 0.70 +00 - 0.1110 +04 0.075 +02 0.05 +01 - 0.1120 +04 0.1040 +02 0.12 +01 - 0.1125 +04 0.094 +02 0.09 +01 - 0.1130 +04 0.100 +02 0.12 +01 - 0.1139 +04 0.099 +02 0.07 +01 - 0.1147 +04 0.093 +02 0.06 +01 - 0.1160 +04 0.116 +02 0.09 +01 - 0.1165 +04 0.144 +02 0.28 +01 - 0.1170 +04 0.142 +02 0.09 +01 - 0.1175 +04 0.165 +02 0.21 +01 - 0.1180 +04 0.125 +02 0.10 +01 - 0.1186 +04 0.111 +02 0.08 +01 - 0.1190 +04 0.120 +02 0.16 +01 - 0.1195 +04 0.114 +02 0.21 +01 - 0.1200 +04 0.097 +02 0.09 +01 - 0.1212 +04 0.118 +02 0.07 +01 - 0.1222 +04 0.131 +02 0.09 +01 - 0.1233 +04 0.150 +02 0.10 +01 - 0.1238 +04 0.145 +02 0.09 +01 - 0.1243 +04 0.126 +02 0.08 +01 - 0.1253 +04 0.123 +02 0.08 +01 - 0.1262 +04 0.098 +02 0.06 +01 - 0.1270 +04 0.146 +02 0.09 +01 - 0.1275 +04 0.129 +02 0.09 +01 - 0.1280 +04 0.127 +02 0.16 +01 - 0.1289 +04 0.116 +02 0.09 +01 - 0.1300 +04 0.103 +02 0.07 +01 - 0.1307 +04 0.107 +02 0.09 +01 - 0.1313 +04 0.110 +02 0.07 +01 - 0.1326 +04 0.133 +02 0.10 +01 - 0.1333 +04 0.144 +02 0.10 +01 - 0.1340 +04 0.162 +02 0.09 +01 - 0.1353 +04 0.149 +02 0.11 +01 - 0.1366 +04 0.153 +02 0.12 +01 - 0.1373 +04 0.135 +02 0.09 +01 - 0.1380 +04 0.112 +02 0.08 +01 - 0.1386 +04 0.124 +02 0.09 +01 - 0.1392 +04 0.161 +02 0.13 +01 - 0.1400 +04 0.170 +02 0.10 +01 - 0.1405 +04 0.146 +02 0.10 +01 - 0.1410 +04 0.133 +02 0.10 +01 - 0.1416 +04 0.160 +02 0.14 +01 - 0.1420 +04 0.160 +02 0.12 +01 - 0.1425 +04 0.132 +02 0.08 +01 - 0.1430 +04 0.130 +02 0.11 +01 - 0.1440 +04 0.130 +02 0.08 +01 - 0.1445 +04 0.134 +02 0.10 +01 - 0.1450 +04 0.159 +02 0.09 +01 - 0.1455 +04 0.153 +02 0.11 +01 - 0.1460 +04 0.148 +02 0.10 +01 - 0.1466 +04 0.172 +02 0.11 +01 - 0.1470 +04 0.186 +02 0.13 +01 - 0.1475 +04 0.187 +02 0.11 +01 - 0.1480 +04 0.166 +02 0.11 +01 - 0.1485 +04 0.178 +02 0.12 +01 - 0.1490 +04 0.157 +02 0.11 +01 - 0.1500 +04 0.150 +02 0.16 +01 + 0.1020E+04 0.400E+01 0.10E+01 + 0.1040E+04 0.610E+01 0.70E+00 + 0.1050E+04 0.670E+01 0.70E+00 + 0.1060E+04 0.620E+01 0.60E+00 + 0.1070E+04 0.740E+01 0.60E+00 + 0.1080E+04 0.880E+01 0.60E+00 + 0.1085E+04 0.102E+02 0.80E+00 + 0.1090E+04 0.120E+02 0.90E+00 + 0.1100E+04 0.910E+01 0.70E+00 + 0.1110E+04 0.075E+02 0.05E+01 + 0.1120E+04 0.104E+02 0.12E+01 + 0.1125E+04 0.094E+02 0.09E+01 + 0.1130E+04 0.100E+02 0.12E+01 + 0.1139E+04 0.099E+02 0.07E+01 + 0.1147E+04 0.093E+02 0.06E+01 + 0.1160E+04 0.116E+02 0.09E+01 + 0.1165E+04 0.144E+02 0.28E+01 + 0.1170E+04 0.142E+02 0.09E+01 + 0.1175E+04 0.165E+02 0.21E+01 + 0.1180E+04 0.125E+02 0.10E+01 + 0.1186E+04 0.111E+02 0.08E+01 + 0.1190E+04 0.120E+02 0.16E+01 + 0.1195E+04 0.114E+02 0.21E+01 + 0.1200E+04 0.097E+02 0.09E+01 + 0.1212E+04 0.118E+02 0.07E+01 + 0.1222E+04 0.131E+02 0.09E+01 + 0.1233E+04 0.150E+02 0.10E+01 + 0.1238E+04 0.145E+02 0.09E+01 + 0.1243E+04 0.126E+02 0.08E+01 + 0.1253E+04 0.123E+02 0.08E+01 + 0.1262E+04 0.098E+02 0.06E+01 + 0.1270E+04 0.146E+02 0.09E+01 + 0.1275E+04 0.129E+02 0.09E+01 + 0.1280E+04 0.127E+02 0.16E+01 + 0.1289E+04 0.116E+02 0.09E+01 + 0.1300E+04 0.103E+02 0.07E+01 + 0.1307E+04 0.107E+02 0.09E+01 + 0.1313E+04 0.110E+02 0.07E+01 + 0.1326E+04 0.133E+02 0.10E+01 + 0.1333E+04 0.144E+02 0.10E+01 + 0.1340E+04 0.162E+02 0.09E+01 + 0.1353E+04 0.149E+02 0.11E+01 + 0.1366E+04 0.153E+02 0.12E+01 + 0.1373E+04 0.135E+02 0.09E+01 + 0.1380E+04 0.112E+02 0.08E+01 + 0.1386E+04 0.124E+02 0.09E+01 + 0.1392E+04 0.161E+02 0.13E+01 + 0.1400E+04 0.170E+02 0.10E+01 + 0.1405E+04 0.146E+02 0.10E+01 + 0.1410E+04 0.133E+02 0.10E+01 + 0.1416E+04 0.160E+02 0.14E+01 + 0.1420E+04 0.160E+02 0.12E+01 + 0.1425E+04 0.132E+02 0.08E+01 + 0.1430E+04 0.130E+02 0.11E+01 + 0.1440E+04 0.130E+02 0.08E+01 + 0.1445E+04 0.134E+02 0.10E+01 + 0.1450E+04 0.159E+02 0.09E+01 + 0.1455E+04 0.153E+02 0.11E+01 + 0.1460E+04 0.148E+02 0.10E+01 + 0.1466E+04 0.172E+02 0.11E+01 + 0.1470E+04 0.186E+02 0.13E+01 + 0.1475E+04 0.187E+02 0.11E+01 + 0.1480E+04 0.166E+02 0.11E+01 + 0.1485E+04 0.178E+02 0.12E+01 + 0.1490E+04 0.157E+02 0.11E+01 + 0.1500E+04 0.150E+02 0.16E+01 ENDDATA 68 -ENDSUBENT 84 +ENDSUBENT 85 SUBENT 10010007 19990617 19990622 BIB 5 6 REACTION (83-BI-209(N,INL)83-BI-209,PAR,SIG) diff --git a/exforall/100/10029.x4 b/exforall/100/10029.x4 index 9742c7aed..d293f90af 100644 --- a/exforall/100/10029.x4 +++ b/exforall/100/10029.x4 @@ -1,8 +1,8 @@ -ENTRY 10029 19990719 19990812 -SUBENT 10029001 19990719 19990812 -BIB 14 34 +ENTRY 10029 20050627 20050909 1336 +SUBENT 10029001 20050627 20050909 1336 +BIB 14 36 INSTITUTE (1USAMIT) -REFERENCE (J,NP,137,85,196911) +REFERENCE (J,NP/A,137,85,196911) AUTHOR (V.C.ROGERS,L.E.BEGHIAN,F.M.CLIKEMAN) TITLE The energy level structure of 45Sc from the (n,n'gamma) reaction @@ -35,10 +35,12 @@ STATUS (APRVD) APPROVED BY AUTHOR HISTORY (19690505C) (19800723A) Converted to REACTION formalism (19990719A) Converted to new date formats, lower case. -ENDBIB 34 + (20050627C) DR Reference corrected (NP->NP/A) + Data aligned +ENDBIB 36 NOCOMMON 0 0 -ENDSUBENT 37 -SUBENT 10029002 19990719 19990812 +ENDSUBENT 39 +SUBENT 10029002 20050627 20050909 1336 BIB 1 1 REACTION (21-SC-45(N,INL)21-SC-45,PAR,SIG,G) ENDBIB 1 @@ -50,40 +52,40 @@ ENDCOMMON 3 DATA 4 70 E EN DATA DATA-ERR KEV MEV MB MB - 364. 0.46 34.0 12.0 - 364. 0.61 38.0 12.0 - 364. 0.77 52.0 12.0 - 364. 0.98 71.0 14.0 + 364. 0.46 34.0 12.0 + 364. 0.61 38.0 12.0 + 364. 0.77 52.0 12.0 + 364. 0.98 71.0 14.0 364. 1.16 108.0 16.0 364. 1.34 121.0 18.0 364. 1.42 111.0 17.0 364. 1.62 153.0 22.0 364. 1.69 154.0 22.0 - 376. 0.46 4.0 4.0 - 376. 0.61 8.0 7.0 - 376. 0.77 3.0 3.0 - 376. 0.98 10.0 8.0 - 376. 1.16 7.0 7.0 - 376. 1.34 6.0 6.0 - 376. 1.42 5.0 5.0 - 376. 1.62 6.0 6.0 - 376. 1.69 9.0 8.0 - 532. 0.61 26.0 8.0 - 532. 0.77 34.0 9.0 - 532. 0.98 54.0 11.0 - 532. 1.16 80.0 16.0 - 532. 1.34 74.0 14.0 - 532. 1.42 66.0 13.0 - 532. 1.62 48.0 9.0 - 532. 1.69 73.0 14.0 - 544. 0.61 16.0 8.0 - 544. 0.77 22.0 8.0 - 544. 0.98 51.0 12.0 - 544. 1.16 47.0 11.0 - 544. 1.34 49.0 11.0 - 544. 1.42 22.0 8.0 - 544. 1.61 47.0 11.0 - 544. 1.69 59.0 13.0 + 376. 0.46 4.0 4.0 + 376. 0.61 8.0 7.0 + 376. 0.77 3.0 3.0 + 376. 0.98 10.0 8.0 + 376. 1.16 7.0 7.0 + 376. 1.34 6.0 6.0 + 376. 1.42 5.0 5.0 + 376. 1.62 6.0 6.0 + 376. 1.69 9.0 8.0 + 532. 0.61 26.0 8.0 + 532. 0.77 34.0 9.0 + 532. 0.98 54.0 11.0 + 532. 1.16 80.0 16.0 + 532. 1.34 74.0 14.0 + 532. 1.42 66.0 13.0 + 532. 1.62 48.0 9.0 + 532. 1.69 73.0 14.0 + 544. 0.61 16.0 8.0 + 544. 0.77 22.0 8.0 + 544. 0.98 51.0 12.0 + 544. 1.16 47.0 11.0 + 544. 1.34 49.0 11.0 + 544. 1.42 22.0 8.0 + 544. 1.61 47.0 11.0 + 544. 1.69 59.0 13.0 722. 0.77 22.0 7.0 722. 0.98 91.0 16.0 722. 1.16 134.0 23.0 @@ -93,33 +95,33 @@ KEV MEV MB MB 722. 1.69 143.0 24.0 893. 1.61 17.0 7.0 893. 1.69 61.0 16.0 - 926. 1.16 14.0 8.0 - 926. 1.34 9.0 7.0 - 926. 1.42 8.0 6.0 - 926. 1.61 13.0 8.0 - 926. 1.69 16.0 8.0 - 962. 0.98 8.0 7.0 - 962. 1.16 34.0 11.0 - 962. 1.34 40.0 13.0 - 962. 1.42 38.0 12.0 - 962. 1.61 40.0 13.0 - 962. 1.69 33.0 11.0 - 974. 0.98 15.0 8.0 - 974. 1.16 46.0 12.0 - 974. 1.34 66.0 14.0 - 974. 1.42 64.0 14.0 - 974. 1.61 66.0 14.0 - 974. 1.69 56.0 13.0 + 926. 1.16 14.0 8.0 + 926. 1.34 9.0 7.0 + 926. 1.42 8.0 6.0 + 926. 1.61 13.0 8.0 + 926. 1.69 16.0 8.0 + 962. 0.98 8.0 7.0 + 962. 1.16 34.0 11.0 + 962. 1.34 40.0 13.0 + 962. 1.42 38.0 12.0 + 962. 1.61 40.0 13.0 + 962. 1.69 33.0 11.0 + 974. 0.98 15.0 8.0 + 974. 1.16 46.0 12.0 + 974. 1.34 66.0 14.0 + 974. 1.42 64.0 14.0 + 974. 1.61 66.0 14.0 + 974. 1.69 56.0 13.0 1238. 1.34 29.0 8.0 1238. 1.42 100.0 20.0 1238. 1.61 110.0 22.0 1238. 1.69 135.0 27.0 -1412. 1.42 8.0 7.0 -1412. 1.61 43.0 17.0 -1412. 1.69 90.0 33.0 -1437. 1.61 28.0 13.0 -1437. 1.69 38.0 15.0 -1664. 1.69 21.0 11.0 +1412. 1.42 8.0 7.0 +1412. 1.61 43.0 17.0 +1412. 1.69 90.0 33.0 +1437. 1.61 28.0 13.0 +1437. 1.69 38.0 15.0 +1664. 1.69 21.0 11.0 ENDDATA 72 ENDSUBENT 82 ENDENTRY 2 diff --git a/exforall/101/10166.x4 b/exforall/101/10166.x4 index 01e8bf94a..e196b4fab 100644 --- a/exforall/101/10166.x4 +++ b/exforall/101/10166.x4 @@ -1,10 +1,10 @@ -ENTRY 10166 20001214 20010328 -SUBENT 10166001 20001214 20010328 -BIB 12 26 +ENTRY 10166 20050627 20050909 1336 +SUBENT 10166001 20050627 20050909 1336 +BIB 12 28 INSTITUTE (1USAANL) -REFERENCE (J,PR/C,1,683,197002) - (J,JNE,26,75,1975) Corrected data. -AUTHOR (A.DE VOLPI,K.G.PORGES) +REFERENCE (J,PR/C,1,683,1970) + (J,JNE,26,75,1972) Corrected data. +AUTHOR (A.DeVolpi,K.G.Porges) TITLE Neutron Yield of 252Cf Based on Absolute Measurement of the Neutron Rate and Fission Ratio. METHOD (MANGB) Manganese bath facility for measurement of @@ -27,11 +27,13 @@ HISTORY (19711228C) (19820527A) Converted to REACTION formalism (20001214A) Converted to new date formats, lower case. Subentry 2 deleted. Data unit updated. -ENDBIB 26 + (20050627C) DR Reference corrected + Units updated +ENDBIB 28 NOCOMMON 0 0 -ENDSUBENT 29 +ENDSUBENT 31 NOSUBENT 10166002 20001214 20010328 -SUBENT 10166003 20001214 20010328 +SUBENT 10166003 20050627 20050909 1336 BIB 3 5 REACTION (98-CF-252(0,F),,NU) CORRECTION Value increased by De Volpi as a result of re-evaluated @@ -42,7 +44,7 @@ ENDBIB 5 NOCOMMON 0 0 DATA 2 1 DATA DATA-ERR -PART/FIS PART/FIS +PRT/FIS PRT/FIS 3.729 0.015 ENDDATA 3 ENDSUBENT 13 diff --git a/exforall/102/10231.x4 b/exforall/102/10231.x4 index 8a7a86f58..77a801ccb 100644 --- a/exforall/102/10231.x4 +++ b/exforall/102/10231.x4 @@ -1,9 +1,9 @@ -ENTRY 10231 20010309 20010426 -SUBENT 10231001 20010309 20010426 -BIB 15 31 +ENTRY 10231 20050627 20050909 1336 +SUBENT 10231001 20050627 20050909 1336 +BIB 15 32 INSTITUTE (1USAANL) -REFERENCE (J,NIM,2,193,197207) -AUTHOR (D.L.SMITH) +REFERENCE (J,NIM,10,193,1972) +AUTHOR (D.L.Smith) TITLE Fast-neutron flux measurement with a lithium-drifted germanium detector FACILITY (ACCEL) Argonne fast neutron generator @@ -32,9 +32,10 @@ HISTORY (19720117C) (19781107U) Blank REFERENCE deleted (19821015A) Converted to REACTION formalism. (20010309A) Updated to new date formats, lower case. -ENDBIB 31 + (20050627C) DR Reference corrected +ENDBIB 32 NOCOMMON 0 0 -ENDSUBENT 34 +ENDSUBENT 35 SUBENT 10231002 20010309 20010426 BIB 2 2 REACTION (32-GE-72(N,INL)32-GE-72,PAR,SIG) diff --git a/exforall/103/10307.x4 b/exforall/103/10307.x4 index e24ff4010..95c1fda45 100644 --- a/exforall/103/10307.x4 +++ b/exforall/103/10307.x4 @@ -1,9 +1,9 @@ -ENTRY 10307 20020823 20020925 -SUBENT 10307001 20020823 20020925 -BIB 11 19 +ENTRY 10307 20050627 20050909 1336 +SUBENT 10307001 20050627 20050909 1336 +BIB 11 20 INSTITUTE (1USAWSU) -REFERENCE (J,CJP,51,121,197301) - (J,NIM,114,591,1971) Experimental technique +REFERENCE (J,CJP,51,121,1973) + (J,NIM,114,591,1974) Experimental technique AUTHOR (M.C.Gupta,G.E.Tripard) TITLE Fast Neutron Scattering at 180 degrees from Pb and Sn INC-SOURCE (D-D) D(d,n) source @@ -20,13 +20,14 @@ HISTORY (19740528C) VM (19830118A) Converted to REACTION formalism (20020823A) Updated to new date formats, lower case. Reactions corrected. -ENDBIB 19 + (20050627C) DR Reference corrected +ENDBIB 20 COMMON 1 3 EN MEV 3.65 ENDCOMMON 3 -ENDSUBENT 26 +ENDSUBENT 27 SUBENT 10307002 20020823 20020925 BIB 1 1 REACTION (50-SN-0(N,EL)50-SN-0,,DA) diff --git a/exforall/103/10355.x4 b/exforall/103/10355.x4 index 6eab3a44e..6c95e17a5 100644 --- a/exforall/103/10355.x4 +++ b/exforall/103/10355.x4 @@ -1,9 +1,9 @@ -ENTRY 10355 20021120 20030219 -SUBENT 10355001 20021120 20030219 -BIB 12 35 +ENTRY 10355 20050627 20050909 1336 +SUBENT 10355001 20050627 20050909 1336 +BIB 12 36 INSTITUTE (1USADAV) -REFERENCE (J,PR/C,16,49,197708) - (J,PRL,31,640,197309) +REFERENCE (J,PR/C,16,499,1977) + (J,PRL,31,640,1973) AUTHOR (T.C.Montgomery,F.P.Brady,B.E.Bonner,W.B.Broste, M.W.Mc Naughton) TITLE Neutron-proton differential cross section measurements @@ -15,7 +15,7 @@ MONITOR (1-H-1(N,EL)1-H-1,,SIG) Normalization obtained by a preliminary fit integrated to total cross section. Forward and backward data renormalized to agree at angles of overlap. -MONIT-REF (,F.P.Brady+,J,PRL,25,1682,1970) +MONIT-REF (,F.P.Brady+,J,PRL,25,1628,1970) CORRECTION Corrected for: . detector efficiency uncertainty, . neutron attenuation (up to 0.5%), @@ -36,13 +36,14 @@ HISTORY (19731031C) subentry 1 COMMON. (19830422A) Reaction corrected. (20011120A) Converted to new date formats, lower case. -ENDBIB 35 + (20050627C) DR Reference corrected +ENDBIB 36 COMMON 1 3 EN-ERR MEV 0.1 ENDCOMMON 3 -ENDSUBENT 42 +ENDSUBENT 43 SUBENT 10355002 20021120 20030219 BIB 5 12 REACTION (1-H-1(N,EL)1-H-1,,DA) diff --git a/exforall/106/10629.x4 b/exforall/106/10629.x4 index 07d01c7a1..f755515d2 100644 --- a/exforall/106/10629.x4 +++ b/exforall/106/10629.x4 @@ -1,9 +1,9 @@ -ENTRY 10629 20040726 -SUBENT 10629001 20040726 -BIB 14 27 +ENTRY 10629 20050630 20050909 1336 +SUBENT 10629001 20050630 20050909 1336 +BIB 14 28 INSTITUTE (1USAORL,1USALAS) -REFERENCE (J,PR/C,18,1320,197809) - (C,75WASH,2,576,197503) +REFERENCE (J,PR/C,18,1328,1978) + (C,75WASH,2,576,1975) AUTHOR (M.S.Moore,J.D.Moses,G.A.Keyworth,J.W.T.Dabbs,N.W.Hill) TITLE Spin determination of resonance structure in (235U+n) below 25 keV @@ -28,13 +28,14 @@ HISTORY (19780525A) Preliminary data replaced. (19810827A) SAN 2,4 corrected. (19831102A) BIB, COMMON corrections. (20040726A) Converted to new date formats, lower case. -ENDBIB 27 + (20050630C) DR Reference corrected (p.1320 ->1328) +ENDBIB 28 COMMON 3 3 EN-NRM-MIN EN-NRM-MAX MONIT EV EV B*EV 7.8 11. 241.24 ENDCOMMON 3 -ENDSUBENT 34 +ENDSUBENT 35 SUBENT 10629002 20040726 BIB 7 14 REACTION 1(92-U-235(N,0),,EN) diff --git a/exforall/107/10704.x4 b/exforall/107/10704.x4 index 0e6a339d6..4a7a51950 100644 --- a/exforall/107/10704.x4 +++ b/exforall/107/10704.x4 @@ -1,26 +1,26 @@ -ENTRY 10704 810827 -SUBENT 10704001 810827 -BIB 11 20 +ENTRY 10704 20050630 20050909 1336 +SUBENT 10704001 20050630 20050909 1336 +BIB 10 20 INSTITUTE (1USABRN) -REFERENCE (J,JP/G,3,1393,7710) - (T,PALMER,75) -AUTHOR (D.C.PALMER,D.R.MAXSON,J.R.BADING) -TITLE CL-35,CL-37,AND AR-36(N,D) REACTIONS AT 14.1 MEV. -FACILITY BROWN UNIVERSITY NEUTRON GENERATOR -N-SOURCE (D-T) DEUTERONS ON TRITIUM -DETECTOR (TELES)REACTION DEUTERONS MEASURED BY A NEW - TIME-OF-FLIGHT COUNTER TELESCOPE CONSISTING OF TWO - PROPORTIONAL COUNTERS AND A NAI(TL) CRYSTAL FOR THE - ENERGY SPREAD AND ENERGY DETECTORS RESPECTIVELY. - SOLID-STATE DETECTOR USED TO COUNT ASSOCIATED ALPHAS - FROM T(D,N) REACTION. -MONITOR FLUX MONITORED BY COUNTING ASSOCIATED ALPHA PARTICLES - FROM T(D,N)HE-4 REACTION. -ERR-ANALYS (DATA-ERR)MAINLY STATISTICAL ERRORS WITH GEOMETRICAL, - COUNTER EFFICIENCY, AND TELESCOPE ANGULAR SETTING - CONTRIBUTED SMALLER ERRORS. -STATUS (APRVD) APPROVED BY D.R.MAXSON, 78/4/13. -HISTORY (780126C) +REFERENCE (J,JP/G,3,1363,1977) + (T,PALMER,1975) +AUTHOR (D.C.Palmer,D.R.Maxson,J.R.Bading) +TITLE Cl-35,Cl-37,and Ar-36(n,d) Reactions at 14.1 MeV. +FACILITY Brown University Neutron Generator +DETECTOR (TELES) Reaction deuterons measured by a new + time-of-flight counter telescope consisting of two + proportional counters and a NaI(TL) crystal for the + energy spread and energy detectors respectively. + Solid state detector used to count associated alphas + from T(D,N) reaction. +MONITOR Flux monitored by counting associated alpha particles + from T(D,N)He-4 reaction. +ERR-ANALYS (DATA-ERR) Mainly statistical errors with geometrical, + counter efficiency, and telescope angular setting + contributed smaller errors. +STATUS (APRVD) Approved by D.R. Maxson, 78/4/13. +HISTORY (19780126C) + (20050630C) DR Reference corrected and format updated ENDBIB 20 COMMON 1 3 EN @@ -28,14 +28,14 @@ MEV 14.1 ENDCOMMON 3 ENDSUBENT 27 -SUBENT 10704002 780223 +SUBENT 10704002 19780223 20050909 1336 BIB 2 4 REACTION (17-CL-35(N,D)16-S-34,PAR,DA) -SAMPLE PB-CL(2) TARGET, ENRICHED TO 99.32 PERCENT CL-35, - VACUUM EVAPORATED ONTO THICK GOLD FOILS TO 6.71 - MG/CM**2. +SAMPLE Pb-Cl(2) target, enriched to 99.32 percent Cl-35, + vacuum evaporated onto thick gold foils to 6.71 + mg/cm**2. ENDBIB 4 -NOCOMMON +NOCOMMON 0 0 DATA 6 13 E-EXC ANG +ANG-RSL -ANG-RSL DATA DATA-ERR MEV ADEG ADEG ADEG MB/SR MB/SR @@ -54,14 +54,14 @@ MEV ADEG ADEG ADEG MB/SR MB/SR 2.13 52.9 5.1 5.2 -0.05 0.32 ENDDATA 15 ENDSUBENT 24 -SUBENT 10704003 780223 +SUBENT 10704003 19780223 20050909 1336 BIB 3 6 REACTION (17-CL-37(N,D)16-S-36,PAR,DA) -SAMPLE PB-CL(2) TARGET, ENRICHED TO 90.36 PERCENT CL-37, - VACUUM EVAPORATED ONTO THICK GOLD FOILS TO 7.25 - MG/CM**2. -CORRECTION CONTRIBUTION FROM 10.PCT.CL-35 SUBTRACTED POINT BY - POINT. +SAMPLE Pb-Cl(2) target, enriched to 90.36 percent Cl-37, + vacuum evaporated onto thick gold foils to 7.25 + mg/cm**2. +CORRECTION Contribution from 10.PCT.Cl-35 subtracted point by + point. ENDBIB 6 COMMON 1 3 E-EXC @@ -78,14 +78,14 @@ ADEG ADEG ADEG MB/SR MB/SR 52.7 5.2 5.2 0.48 0.48 ENDDATA 7 ENDSUBENT 22 -SUBENT 10704004 780223 +SUBENT 10704004 19780223 20050909 1336 BIB 2 4 REACTION (18-AR-36(N,D)17-CL-35,PAR,DA) -SAMPLE ARGON GAS CELL SAMPLE ENRICHED TO 99.8 PERCENT AR-36. - AVERAGE GAS PRESSURE 79.5 CM.HG, AVERAGE THICKNESS - 2.85 MG/CM**2. +SAMPLE Argon gas cell sample enriched to 99.8 percent AR-36. + Average gas pressure 79.5 cm.Hg, average thickness + 2.85 mg/cm**2. ENDBIB 4 -NOCOMMON +NOCOMMON 0 0 DATA 7 10 E-EXC E-EXC ANG +ANG-RSL -ANG-RSL DATA DATA-ERR diff --git a/exforall/108/10842.x4 b/exforall/108/10842.x4 index 69e94dd87..5d1e76900 100644 --- a/exforall/108/10842.x4 +++ b/exforall/108/10842.x4 @@ -1,10 +1,10 @@ -ENTRY 10842 940517 -SUBENT 10842001 940517 -BIB 13 52 +ENTRY 10842 20050706 20050909 1336 +SUBENT 10842001 20050706 20050909 1336 +BIB 13 53 INSTITUTE (1USAORL,1USAVBT) -REFERENCE (J,PR,19,335,7902) -AUTHOR (M.MIZUMOTO,S.RAMAN,R.L.MACKLIN,G.G.SLAUGHTER, - J.A.HARVEY,J.H.HAMILTON) +REFERENCE (J,PR/C,19,335,1979) +AUTHOR (M.Mizumoto,S.Raman,R.L.Macklin,G.G.Slaughter, + J.A.Harvey,J.H.Hamilton) TITLE Low energy neutron resonances in 206Pb FACILITY (LINAC,1USAORL) Oak Ridge electron linear accelerator SAMPLE For transmission measurement- @@ -49,15 +49,16 @@ STATUS **** Capture cross section requires a correction by a factor of 1.0360 due to error in processing code (private communication, Macklin and Winters, 9/24/80). -HISTORY (790402C) - (801205A) Status comment added. - (940517A) Illegal pointer deleted. Converted to lower +HISTORY (19790402C) + (19801205A) Status comment added. + (19940517A) Illegal pointer deleted. Converted to lower + (20050706C) DR Reference corrected and format updated case. -ENDBIB 52 +ENDBIB 53 NOCOMMON 0 0 -ENDSUBENT 55 -SUBENT 10842002 820812 -BIB 4 24 +ENDSUBENT 56 +SUBENT 10842002 19820812 20050909 1336 +BIB 4 25 REACTION 1(82-PB-206(N,0),,EN) 2(82-PB-206(N,0),,L) 3(82-PB-206(N,0),,J) @@ -66,23 +67,24 @@ REACTION 1(82-PB-206(N,0),,EN) 6(82-PB-206(N,G),,WID) 7(((82-PB-206(N,EL),,WID,,G)*(82-PB-206(N,G),,WID))/ (82-PB-206(N,TOT),,WID)) -COMMENT 2VALUES OBTAINED FROM RESONANCE SHAPES. S-WAVE POSSIBIL- - ITY EXCLUDED BY ABSENCE OF INTERFERENCE FOR WEIGHTED - NEUTRON WIDTHS ON THE ORDER OF 0.04*ENERGY RESOLUTION. -FLAG (1.) BASED ON TRANSMISSION MEASUREMENTS OF SHAPE OR - PEAK CROSS SECTIONS. - (2.)D-WAVE POSSIBILITY LESS THAN 1-PERCENT BASED ON - BAYES THEOREM. VALUES OBTAINED FROM TRANSMISSION - MEASUREMENTS OF SHAPE OR PEAK CROSS SECTIONS. - (3.) BASED ON OBSERVATION OF STRONG GAMMA TRANSITIONS - TO KNOWN J=5/2 FINAL STATES. S-WAVE POSSIBILITY EX- - CLUDED BY THESE TRANSITIONS. - (4.) BASED ON OBSERVATION OF STRONG GAMMA TRANSITIONS - TO KNOWN J=5/2 FINAL STATES. S-WAVE POSSIBILITY EX- - CLUDED BY THESE TRANSITIONS. D-WAVE POSSIBILITY LESS - THAN 1-PERCENT BASED ON BAYES THEOREM. -HISTORY (820812A) CORRECTED REACTION. -ENDBIB 24 +COMMENT 2Values obtained from resonance shapes. S-Wave possibil- + ity excluded by abscence of interference for weighted + neutron widths on the order of 0.04*energy resolution. +FLAG (1.) Based on transmission measurements of shape or + peak cross sections. + (2.)D-Wave possibility less than 1-percent based on + Bayes theorem. Values obtained from transmission + measurements of shape or peak cross sections. + (3.) Based on observation of strong gamma transitions + to known J=5/2 final states. S-Wave possibility ex- + cluded by these transitions. + (4.) Based on observation of strong gamma transitions + to known J=5/2 final states. S-Wave possibility ex- + cluded by these transitions. D-Wave possibility less + than 1-percent based on Bayes theorem. +HISTORY (19820812A) Corrected reaction. + (20050706C) Format updated +ENDBIB 25 COMMON 1 3 DATA-ERR 1 PER-CENT @@ -162,11 +164,11 @@ EV EV NO-DIM NO-DIM 85.2 0.8 0.25 0.02 0.25 0.02 1. 2. ENDDATA 72 -ENDSUBENT 105 -SUBENT 10842003 790827 +ENDSUBENT 106 +SUBENT 10842003 19790827 20050909 1336 BIB 2 2 REACTION (82-PB-206(N,EL),,STF) -HISTORY (790827C) +HISTORY (19790827C) ENDBIB 2 COMMON 1 3 MOMENTUM L @@ -181,13 +183,13 @@ KEV KEV NO-DIM NO-DIM 4.7600E+01 3.2000E-05 1.3000E-05 ENDDATA 5 ENDSUBENT 16 -SUBENT 10842004 821119 +SUBENT 10842004 19821119 20050909 1336 BIB 3 5 REACTION 1(82-PB-206(N,0),,EN) 2(82-PB-206(N,EL),,WID,,G) 3(82-PB-206(N,0),,L) -STATUS DATA TAKEN FROM FIGURE 2 IN ARTICLE. -HISTORY (821119C) +STATUS Data taken from figure 2 in article. +HISTORY (19821119C) ENDBIB 5 NOCOMMON 0 0 DATA 3 16 diff --git a/exforall/109/10927.x4 b/exforall/109/10927.x4 index 11fc3fb2e..4b35fc967 100644 --- a/exforall/109/10927.x4 +++ b/exforall/109/10927.x4 @@ -1,8 +1,8 @@ -ENTRY 10927 20030226 20030411 -SUBENT 10927001 20030226 20030411 -BIB 11 12 +ENTRY 10927 20050708 20050909 1336 +SUBENT 10927001 20050708 20050909 1336 +BIB 11 13 INSTITUTE (1USAORL) -REFERENCE (J,PR/C,22,328,197807) +REFERENCE (J,PR/C,22,328,1980) AUTHOR (S.Raman,G.G.Slaughter,J.C.Wells Jr,B.J.Allen) TITLE Valence neutron capture gamma-ray spectrum in 54Fe FACILITY (LINAC,1USAORL) Oak Ridge Electron Linear Accelerator @@ -13,9 +13,10 @@ DETECTOR (GELI) 37-cm**2 germanium-lithium detector STATUS (APRVD) Approved by S.Raman,19 81/3/23. HISTORY (19810123C) (20030226C) Converted to new date formats, lower case. -ENDBIB 12 + (20050708C) DR Reference corrected +ENDBIB 13 NOCOMMON 0 0 -ENDSUBENT 15 +ENDSUBENT 16 SUBENT 10927002 20030226 20030411 BIB 1 2 REACTION 1(26-FE-54(N,0),,J) diff --git a/exforall/111/11165.x4 b/exforall/111/11165.x4 index 26e412451..85211db9f 100644 --- a/exforall/111/11165.x4 +++ b/exforall/111/11165.x4 @@ -1,42 +1,43 @@ -ENTRY 11165 800814 -SUBENT 11165001 800814 -BIB 6 8 +ENTRY 11165 20050708 20050909 1336 +SUBENT 11165001 20050708 20050909 1336 +BIB 6 9 INSTITUTE (1USALRL) -REFERENCE (J,NP/A,38,300,62) -AUTHOR (J.BENVENISTE,A.E.MITCHELL,C.D.SCHRADER,J.H.ZENGER) -TITLE GAMMA RAYS FROM THE INTERACTION OF 14-MEV NEUTRONS WITH - LITHIUM. +REFERENCE (J,NP,38,300,1962) +AUTHOR (J.Benveniste,A.E.Mitchell,C.D.Schrader,J.H.Zenger) +TITLE Gamma rays from the interaction of 14-MeV neutrons with + lithium. STATUS (SCSRS) -HISTORY (760628T) TRANSLATED FROM SCISRS - (800814A) CONVERTED TO REACTION FORMALISM -ENDBIB 8 +HISTORY (19760628T) Translated from SCISRS + (19800814A) Converted to reaction formalism + (20050708C) DR Format updated and reference corrected +ENDBIB 9 NOCOMMON 0 0 -ENDSUBENT 11 -SUBENT 11165002 800814 +ENDSUBENT 12 +SUBENT 11165002 19800814 20050909 1336 BIB 2 2 REACTION (3-LI-7(N,INL)3-LI-7,PAR,SIG,G) -ANALYSIS VALUE 4PI TIMES AVG.CROSS SECTION FROM 30-150 DEGREES. +ANALYSIS Value 4PI times avg. cross section from 30-150 Degrees. ENDBIB 2 COMMON 1 3 E MEV - .478 +0.478 ENDCOMMON 3 DATA 3 12 EN DATA DATA-ERR MEV B B - 1.357 +01 1.08 -01 1.2 -02 - 1.365 +01 8.6 -02 1.0 -02 - 1.374 +01 8.6 -02 1.0 -02 - 1.384 +01 8.7 -02 1.0 -02 - 1.395 +01 8.2 -02 1.0 -02 - 1.407 +01 7.7 -02 9. -03 - 1.418 +01 7.5 -02 9. -03 - 1.428 +01 7.8 -02 9. -03 - 1.440 +01 9.1 -02 1.0 -02 - 1.460 +01 9.9 -02 1.1 -02 - 1.466 +01 8.0 -02 9. -03 - 1.475 +01 1.15 -01 1.3 -02 + 1.357E+01 1.08E-01 1.2E-02 + 1.365E+01 8.6E-02 1.0E-02 + 1.374E+01 8.6E-02 1.0E-02 + 1.384E+01 8.7E-02 1.0E-02 + 1.395E+01 8.2E-02 1.0E-02 + 1.407E+01 7.7E-02 9.0E-03 + 1.418E+01 7.5E-02 9.0E-03 + 1.428E+01 7.8E-02 9.0E-03 + 1.440E+01 9.1E-02 1.0E-02 + 1.460E+01 9.9E-02 1.1E-02 + 1.466E+01 8.0E-02 9.0E-03 + 1.475E+01 1.15E-01 1.3E-02 ENDDATA 14 ENDSUBENT 25 ENDENTRY 2 diff --git a/exforall/117/11739.x4 b/exforall/117/11739.x4 index 6ce99bc65..4d89fed7a 100644 --- a/exforall/117/11739.x4 +++ b/exforall/117/11739.x4 @@ -1,70 +1,71 @@ -ENTRY 11739 860113 -SUBENT 11739001 860113 -BIB 7 11 +ENTRY 11739 20050708 20050909 1336 +SUBENT 11739001 20050708 20050909 1336 +BIB 7 12 INSTITUTE (1USAORL) -REFERENCE (J,JNE,11,95,60) -AUTHOR (F.J.JOHNSTON,J.HALPERIN,R.W.STOUGHTON) -TITLE THE THERMAL NEUTRON ABSORPTION CROSS-SECTION OF TH232 - AND THE RESONANCE INTEGRALS OF TH232, TH233, AND CO59. -MONITOR (79-AU-197(N,G)79-AU-198,,SIG) - (79-AU-197(N,G)79-AU-198,,RI) +REFERENCE (J,JNE/A,11,95,1960) +AUTHOR (F.J.Johnston,J.Halperin,R.W.Stoughton) +TITLE The thermal neutron absorption cross-section of Th232 + and the resonance integrals of Th232, Th233, and Co59. +MONITOR ((MONIT1)79-AU-197(N,G)79-AU-198,,SIG) + ((MONIT2)79-AU-197(N,G)79-AU-198,,RI) STATUS (SCSRS) -HISTORY (760730T) TRANSLATED FROM SCISRS - (840731A) REACTION PRODUCTS ADDED. - (860113U) REACTION PRODUCT ADDED TO MONITOR, ASSUMED. -ENDBIB 11 +HISTORY (19760730T) Translated from SCISRS + (19840731A) Reaction products added. + (19860113U) Reaction product added to monitor, ASSUMED. + (20050708C) DR Format updated and reference corrected +ENDBIB 12 COMMON 2 3 MONIT1 MONIT2 B B 98.8 1565. ENDCOMMON 3 -ENDSUBENT 18 -SUBENT 11739002 860113 +ENDSUBENT 19 +SUBENT 11739002 19860113 20050909 1336 BIB 3 3 REACTION (27-CO-59(N,G)27-CO-60,,RI) -METHOD (ACTIV) ACTIVATION -MONITOR (27-CO-59(N,G)27-CO-60,,SIG) +METHOD (ACTIV) Activation +MONITOR ((MONIT3)27-CO-59(N,G)27-CO-60,,SIG) ENDBIB 3 NOCOMMON 0 0 DATA 4 1 EN-MIN DATA DATA-ERR MONIT3 MEV B B B - 5. -07 7.5 +01 5. +00 37. + 5.00E-07 7.5E+01 5.0E+00 37. ENDDATA 3 ENDSUBENT 11 -SUBENT 11739003 860113 +SUBENT 11739003 19860113 20050909 1336 BIB 3 3 REACTION (90-TH-232(N,G)90-TH-233,,RI) -METHOD (ACTIV) ACTIVATION. COUNTED PA-233 DECAY BETAS. -MONITOR (90-TH-232(N,G)90-TH-233,,SIG) +METHOD (ACTIV) activation. Counted Pa-233 decay betas. +MONITOR ((MONIT3)90-TH-232(N,G)90-TH-233,,SIG) ENDBIB 3 NOCOMMON 0 0 DATA 4 1 EN-MIN DATA DATA-ERR MONIT3 MEV B B B - 5. -07 8.5 +01 8. +00 7.6 + 5.0E-07 8.5E+01 8.0E+00 7.6 ENDDATA 3 ENDSUBENT 11 -SUBENT 11739004 860113 +SUBENT 11739004 19860113 20050909 1336 BIB 5 6 REACTION (90-TH-233(N,G)90-TH-234,,SIG,,MXW) -METHOD (ACTIV) ACTIVATION +METHOD (ACTIV) activation DECAY-DATA (90-TH-234,24.1D,DG) ASSUMED (ASSUM1,90-TH-232(N,G)90-TH-233,,SIG) (ASSUM2,90-TH-232(N,G)90-TH-233,,RI) -INC-SPECT SUB-CD SPECTRUM. +INC-SPECT SUB-CD Spectrum. ENDBIB 6 NOCOMMON 0 0 DATA 5 1 EN-DUMMY DATA DATA-ERR ASSUM1 ASSUM2 MEV B B B B - 2.53 -08 1.450 +03 1.00 +02 10.0 66.7 + 2.53E-08 1.450E+03 1.00E+02 10.0 66.7 ENDDATA 3 ENDSUBENT 14 -SUBENT 11739005 860113 +SUBENT 11739005 19860113 20050909 1336 BIB 4 5 REACTION (90-TH-233(N,G)90-TH-234,,RI) -METHOD (ACTIV) ACTIVATION +METHOD (ACTIV) activation DECAY-DATA (90-TH-234,24.1D,DG) ASSUMED (ASSUM1,90-TH-232(N,G)90-TH-233,,SIG) (ASSUM2,90-TH-232(N,G)90-TH-233,,RI) @@ -73,7 +74,7 @@ NOCOMMON 0 0 DATA 5 1 EN-MIN DATA DATA-ERR ASSUM1 ASSUM2 MEV B B B B - 5. -07 4.00 +02 1.00 +02 10.0 66.1 + 5.0E-07 4.00E+02 1.00E+02 10.0 66.1 ENDDATA 3 ENDSUBENT 13 ENDENTRY 5 diff --git a/exforall/120/12021.x4 b/exforall/120/12021.x4 index 39144736c..ef217ce99 100644 --- a/exforall/120/12021.x4 +++ b/exforall/120/12021.x4 @@ -1,31 +1,32 @@ -ENTRY 12021 760802 -SUBENT 12021001 760802 -BIB 6 8 +ENTRY 12021 20050708 20050909 1336 +SUBENT 12021001 20050708 20050909 1336 +BIB 6 9 INSTITUTE (1USAANL) -REFERENCE (J,JNE,12,16,60) -AUTHOR (D.C.STUPEGIA) -TITLE THE THERMAL NEUTRON CROSS-SECTION OF THE REACTION - CS137(N,GAMMA)CS138. +REFERENCE (J,JNE/A,12,16,1960) +AUTHOR (D.C.Stupegia) +TITLE The thermal neutron cross-section of the reaction + Cs137(n,gamma)Cs138. STATUS (SCSRS) -HISTORY (760802T) TRANSLATED FROM SCISRS - (830802A) CONVERTED TO RECTION FORMALISM -ENDBIB 8 +HISTORY (19760802T) Translated from SCISRS + (19830802A) Converted to reaction formalism + (20050708C) DR Format updated and reference corrected +ENDBIB 9 NOCOMMON 0 0 -ENDSUBENT 11 -SUBENT 12021002 830802 +ENDSUBENT 12 +SUBENT 12021002 19830802 20050909 1336 BIB 5 6 REACTION (55-CS-137(N,G)55-CS-138,,SIG,,MXW) -METHOD (ACTIV) ACTIVATION +METHOD (ACTIV) Activation DECAY-DATA (55-CS-138,32.MIN,DG,2210.,0.18) (55-CS-137,30.YR) MONITOR (79-AU-197(N,G)79-AU-198,,SIG) -INC-SPECT THERMAL SPECTRUM +INC-SPECT Thermal spectrum ENDBIB 6 NOCOMMON 0 0 DATA 4 1 EN-DUMMY DATA DATA-ERR MONIT MEV B B B - 2.53 -08 1.10 -01 3.3 -02 99. + 2.53E-08 1.10E-01 3.3E-02 99. ENDDATA 3 ENDSUBENT 14 ENDENTRY 2 diff --git a/exforall/121/12162.x4 b/exforall/121/12162.x4 index a60622b61..a1a7ea1fa 100644 --- a/exforall/121/12162.x4 +++ b/exforall/121/12162.x4 @@ -1,24 +1,25 @@ -ENTRY 12162 821012 -SUBENT 12162001 821012 -BIB 8 9 +ENTRY 12162 20050711 20050909 1336 +SUBENT 12162001 20050711 20050909 1336 +BIB 8 10 INSTITUTE (1USAANL) -REFERENCE (J,JNE,19,767,65) -AUTHOR (D.C.STUPEGIA,M.SCHMIDT,A.A.MADSON) -TITLE FAST NEUTRON CAPTURE IN RHENIUM. +REFERENCE (J,JNE/AB,19,767,1965) +AUTHOR (D.C.Stupegia,M.Schmidt,A.A.Madson) +TITLE Fast neutron capture in Rhenium. METHOD (ACTIV). DETECTOR (NAICR). STATUS (SCSRS) -HISTORY (760803T) TRANSLATED FROM SCISRS - (821012A) CONVERTED TO REACTION FORMALISM -ENDBIB 9 +HISTORY (19760803T) Translated from SCISRS + (19821012A) Converted to reaction formalism + (20050708C) DR Format updated and reference corrected +ENDBIB 10 NOCOMMON 0 0 -ENDSUBENT 12 -SUBENT 12162002 870505 +ENDSUBENT 13 +SUBENT 12162002 19870505 20050909 1336 BIB 4 4 REACTION (75-RE-185(N,G)75-RE-186-G,,SIG) DECAY-DATA (75-RE-186-G,90.HR,DG,137.) MONITOR (75-RE-185(N,G)75-RE-186-G,,SIG) -HISTORY (870505A) REACTION, DECAY DATA CORRECTED. +HISTORY (19870505A) Reaction, Decay data corrected. ENDBIB 4 COMMON 2 3 EN-NRM MONIT @@ -28,86 +29,86 @@ ENDCOMMON 3 DATA 4 33 EN EN-RSL DATA DATA-ERR MEV MEV B B - 4.6 -03 1.5 -03 5.92 +00 5.8 -01 - 4.9 -03 3.5 -03 5.460 +00 5.35 -01 - 1.22 -02 2.4 -03 2.920 +00 2.85 -01 - 1.9 -02 9. -03 2.260 +00 2.40 -01 - 2.9 -02 2. -03 1.710 +00 1.67 -01 - 4.3 -02 9. -03 1.510 +00 1.48 -01 - 6.6 -02 1.1 -02 1.140 +00 1.12 -01 - 9.3 -02 8. -03 1.060 +00 1.04 -01 - 1.78 -01 2.8 -02 7.05 -01 7.5 -02 - 2.63 -01 3.0 -02 6.30 -01 4.2 -02 - 3.75 -01 3.0 -02 5.70 -01 3.6 -02 - 4.72 -01 2.8 -02 4.60 -01 2.8 -02 - 5.30 -01 4.2 -02 4.00 -01 2.6 -02 - 5.69 -01 3.0 -02 3.90 -01 2.3 -02 - 6.09 -01 1.4 -02 4.35 -01 2.7 -02 - 6.69 -01 3.2 -02 4.75 -01 2.9 -02 - 7.03 -01 3.0 -02 4.10 -01 2.6 -02 - 7.66 -01 3.3 -02 4.25 -01 2.6 -02 - 8.70 -01 3.6 -02 4.05 -01 2.5 -02 - 9.48 -01 4.7 -02 4.35 -01 2.2 -02 - 1.035 +00 2.4 -02 3.70 -01 2.2 -02 - 1.090 +00 5.4 -02 3.60 -01 2.3 -02 - 1.160 +00 5.0 -02 3.55 -01 2.2 -02 - 1.258 +00 3.5 -02 3.85 -01 2.6 -02 - 1.358 +00 4.9 -02 2.97 -01 2.5 -02 - 1.484 +00 2.5 -02 2.25 -01 1.2 -02 - 1.562 +00 4.9 -02 2.30 -01 1.6 -02 - 1.758 +00 6.0 -02 2.40 -01 1.5 -02 - 1.886 +00 2.9 -02 1.85 -01 1.1 -02 - 1.992 +00 3.1 -02 1.250 -01 7.5 -03 - 2.087 +00 1. -03 1.050 -01 6.2 -03 - 2.148 +00 6.8 -02 1.200 -01 7.7 -03 - 2.644 +00 7.4 -02 1.200 -01 7.7 -03 + 4.6E-03 1.5E-03 5.92E+00 5.8E-01 + 4.9E-03 3.5E-03 5.46E+00 5.35E-01 + 1.22E-02 2.4E-03 2.92E+00 2.85E-01 + 1.9E-02 9.0E-03 2.26E+00 2.40E-01 + 2.9E-02 2.0E-03 1.71E+00 1.67E-01 + 4.3E-02 9.0E-03 1.51E+00 1.48E-01 + 6.6E-02 1.1E-02 1.14E+00 1.12E-01 + 9.3E-02 8.0E-03 1.06E+00 1.04E-01 + 1.78E-01 2.8E-02 7.05E-01 7.5E-02 + 2.63E-01 3.0E-02 6.30E-01 4.2E-02 + 3.75E-01 3.0E-02 5.70E-01 3.6E-02 + 4.72E-01 2.8E-02 4.60E-01 2.8E-02 + 5.30E-01 4.2E-02 4.00E-01 2.6E-02 + 5.69E-01 3.0E-02 3.90E-01 2.3E-02 + 6.09E-01 1.4E-02 4.35E-01 2.7E-02 + 6.69E-01 3.2E-02 4.75E-01 2.9E-02 + 7.03E-01 3.0E-02 4.10E-01 2.6E-02 + 7.66E-01 3.3E-02 4.25E-01 2.6E-02 + 8.70E-01 3.6E-02 4.05E-01 2.5E-02 + 9.48E-01 4.7E-02 4.35E-01 2.2E-02 + 1.035E+00 2.4E-02 3.70E-01 2.2E-02 + 1.090E+00 5.4E-02 3.60E-01 2.3E-02 + 1.160E+00 5.0E-02 3.55E-01 2.2E-02 + 1.258E+00 3.5E-02 3.85E-01 2.6E-02 + 1.358E+00 4.9E-02 2.97E-01 2.5E-02 + 1.484E+00 2.5E-02 2.25E-01 1.2E-02 + 1.562E+00 4.9E-02 2.30E-01 1.6E-02 + 1.758E+00 6.0E-02 2.40E-01 1.5E-02 + 1.886E+00 2.9E-02 1.85E-01 1.1E-02 + 1.992E+00 3.1E-02 1.25E-01 7.5E-03 + 2.087E+00 1.0E-03 1.05E-01 6.2E-03 + 2.148E+00 6.8E-02 1.20E-01 7.7E-03 + 2.644E+00 7.4E-02 1.20E-01 7.7E-03 ENDDATA 35 ENDSUBENT 48 -SUBENT 12162003 821012 +SUBENT 12162003 19821012 20050909 1336 BIB 3 4 REACTION (75-RE-187(N,G)75-RE-188-M,,SIG) -DECAY-DATA (75-RE-188-M,18.7MIN,,64.) +DECAY-DATA (75-RE-188-M,18.7MIN,DG,64.) MONITOR (75-RE-187(N,G)75-RE-188,,SIG) - RELATIVE TO THERMAL CAPTURE=1.25B + Relative to thermal capture=1.25B ENDBIB 4 -COMMON 3 3 -HL EN-NRM MONIT -MIN EV B - 18.7 0.0253 1.25 +COMMON 2 3 +EN-NRM MONIT +EV B + 0.0253 1.25 ENDCOMMON 3 DATA 3 27 EN EN-RSL DATA MEV MEV B - 4.9 -03 3.5 -03 9.83 -02 - 1.22 -02 2.4 -03 6.81 -02 - 3.0 -02 5. -03 3.67 -02 - 4.3 -02 9. -03 3.29 -02 - 9.3 -02 8. -03 2.06 -02 - 1.78 -01 2.8 -02 2.10 -02 - 2.65 -01 3.0 -02 1.97 -02 - 2.79 -01 3.2 -02 1.92 -02 - 3.75 -01 3.0 -02 1.54 -02 - 4.72 -01 2.8 -02 1.2 -02 - 5.30 -01 4.2 -02 1.06 -02 - 5.69 -01 3.0 -02 1.15 -02 - 6.09 -01 1.4 -02 1.43 -02 - 6.69 -01 3.2 -02 1.08 -02 - 7.03 -01 3.0 -02 1.00 -02 - 7.66 -01 3.3 -02 1.08 -02 - 8.70 -01 3.6 -02 1.02 -02 - 9.77 -01 2.5 -02 8.9 -03 - 1.090 +00 5.4 -02 8.0 -03 - 1.160 +00 5.0 -02 7.6 -03 - 1.206 +00 2.6 -02 8.9 -03 - 1.258 +00 3.5 -02 8.6 -03 - 1.758 +00 6.0 -02 6.0 -03 - 1.992 +00 3.1 -02 6.1 -03 - 2.087 +00 3.1 -02 5.9 -03 - 2.148 +00 6.8 -02 4.5 -03 - 2.644 +00 7.4 -02 3.9 -03 + 4.9E-03 3.5E-03 9.83E-02 + 1.22E-02 2.4E-03 6.81E-02 + 3.0E-02 5.0E-03 3.67E-02 + 4.3E-02 9.0E-03 3.29E-02 + 9.3E-02 8.0E-03 2.06E-02 + 1.78E-01 2.8E-02 2.10E-02 + 2.65E-01 3.0E-02 1.97E-02 + 2.79E-01 3.2E-02 1.92E-02 + 3.75E-01 3.0E-02 1.54E-02 + 4.72E-01 2.8E-02 1.2E-02 + 5.30E-01 4.2E-02 1.06E-02 + 5.69E-01 3.0E-02 1.15E-02 + 6.09E-01 1.4E-02 1.43E-02 + 6.69E-01 3.2E-02 1.08E-02 + 7.03E-01 3.0E-02 1.00E-02 + 7.66E-01 3.3E-02 1.08E-02 + 8.70E-01 3.6E-02 1.02E-02 + 9.77E-01 2.5E-02 8.9E-03 + 1.090E+00 5.4E-02 8.0E-03 + 1.160E+00 5.0E-02 7.6E-03 + 1.206E+00 2.6E-02 8.9E-03 + 1.258E+00 3.5E-02 8.6E-03 + 1.758E+00 6.0E-02 6.0E-03 + 1.992E+00 3.1E-02 6.1E-03 + 2.087E+00 3.1E-02 5.9E-03 + 2.148E+00 6.8E-02 4.5E-03 + 2.644E+00 7.4E-02 3.9E-03 ENDDATA 29 ENDSUBENT 42 -SUBENT 12162004 821012 +SUBENT 12162004 19821012 20050909 1336 BIB 3 3 REACTION (75-RE-187(N,G)75-RE-188,,SIG) DECAY-DATA (75-RE-188-G,17.HR,DG,155.) @@ -121,39 +122,39 @@ ENDCOMMON 3 DATA 4 33 EN EN-RSL DATA DATA-ERR MEV MEV B B - 4.6 -03 1.5 -03 6.69 +00 6.8 -01 - 4.9 -03 3.5 -03 5.21 +00 5.3 -01 - 1.22 -02 2.4 -03 3.06 +00 3.0 -01 - 1.9 -02 9. -03 2.05 +00 2.0 -01 - 2.9 -02 2. -03 1.64 +00 1.7 -01 - 4.3 -02 9. -03 1.05 +00 1.0 -01 - 6.6 -02 1.1 -02 8.35 -01 8.2 -02 - 9.3 -02 8. -03 7.20 -01 7.0 -02 - 1.78 -01 2.8 -02 6.25 -01 4.0 -02 - 2.65 -01 3.0 -02 5.15 -01 3.1 -02 - 3.75 -01 3.0 -02 3.72 -01 2.2 -02 - 4.72 -01 2.8 -02 3.22 -01 1.9 -02 - 5.30 -01 4.2 -02 2.97 -01 1.8 -02 - 5.69 -01 3.0 -02 2.90 -01 1.7 -02 - 6.09 -01 1.4 -02 3.24 -01 2.0 -02 - 6.69 -01 3.2 -02 2.74 -01 1.6 -02 - 7.03 -01 3.0 -02 2.48 -01 1.5 -02 - 7.66 -01 3.3 -02 2.45 -01 1.5 -02 - 8.70 -01 3.6 -02 2.17 -01 1.4 -02 - 9.77 -01 2.5 -02 1.99 -01 1.3 -02 - 1.035 +00 2.4 -02 2.09 -01 1.3 -02 - 1.090 +00 5.4 -02 1.80 -01 1.1 -02 - 1.160 +00 5.0 -02 1.620 -01 9.7 -03 - 1.258 +00 3.5 -02 1.480 -01 9.1 -03 - 1.358 +00 4.9 -02 1.38 -01 9. -03 - 1.484 +00 2.5 -02 1.210 -01 7.6 -03 - 1.562 +00 4.9 -02 1.04 -01 8. -03 - 1.758 +00 6.0 -02 1.080 -01 6.7 -03 - 1.886 +00 2.9 -02 9.98 -02 6. -04 - 1.992 +00 3.1 -02 8.94 -02 5.4 -03 - 2.087 +00 3.1 -02 8.23 -02 5.0 -03 - 2.148 +00 6.8 -02 7.44 -02 4.5 -03 - 2.644 +00 7.4 -02 5.98 -02 3.8 -03 + 4.6E-03 1.5E-03 6.69E+00 6.8E-01 + 4.9E-03 3.5E-03 5.21E+00 5.3E-01 + 1.22E-02 2.4E-03 3.06E+00 3.0E-01 + 1.9E-02 9.0E-03 2.05E+00 2.0E-01 + 2.9E-02 2.0E-03 1.64E+00 1.7E-01 + 4.3E-02 9.0E-03 1.05E+00 1.0E-01 + 6.6E-02 1.1E-02 8.35E-01 8.2E-02 + 9.3E-02 8.0E-03 7.20E-01 7.0E-02 + 1.78E-01 2.8E-02 6.25E-01 4.0E-02 + 2.65E-01 3.0E-02 5.15E-01 3.1E-02 + 3.75E-01 3.0E-02 3.72E-01 2.2E-02 + 4.72E-01 2.8E-02 3.22E-01 1.9E-02 + 5.30E-01 4.2E-02 2.97E-01 1.8E-02 + 5.69E-01 3.0E-02 2.90E-01 1.7E-02 + 6.09E-01 1.4E-02 3.24E-01 2.0E-02 + 6.69E-01 3.2E-02 2.74E-01 1.6E-02 + 7.03E-01 3.0E-02 2.48E-01 1.5E-02 + 7.66E-01 3.3E-02 2.45E-01 1.5E-02 + 8.70E-01 3.6E-02 2.17E-01 1.4E-02 + 9.77E-01 2.5E-02 1.99E-01 1.3E-02 + 1.035E+00 2.4E-02 2.09E-01 1.3E-02 + 1.090E+00 5.4E-02 1.80E-01 1.1E-02 + 1.160E+00 5.0E-02 1.62E-01 9.7E-03 + 1.258E+00 3.5E-02 1.48E-01 9.1E-03 + 1.358E+00 4.9E-02 1.38E-01 9.0E-03 + 1.484E+00 2.5E-02 1.21E-01 7.6E-03 + 1.562E+00 4.9E-02 1.04E-01 8.0E-03 + 1.758E+00 6.0E-02 1.08E-01 6.7E-03 + 1.886E+00 2.9E-02 9.98E-02 6.0E-04 + 1.992E+00 3.1E-02 8.94E-02 5.4E-03 + 2.087E+00 3.1E-02 8.23E-02 5.0E-03 + 2.148E+00 6.8E-02 7.44E-02 4.5E-03 + 2.644E+00 7.4E-02 5.98E-02 3.8E-03 ENDDATA 35 ENDSUBENT 47 ENDENTRY 4 diff --git a/exforall/123/12323.x4 b/exforall/123/12323.x4 index 2874b3f2d..f09a65dc3 100644 --- a/exforall/123/12323.x4 +++ b/exforall/123/12323.x4 @@ -1,17 +1,18 @@ -ENTRY 12323 841005 -SUBENT 12323001 841005 -BIB 6 7 +ENTRY 12323 20050711 20050909 1336 +SUBENT 12323001 20050711 20050909 1336 +BIB 6 8 INSTITUTE (1USAANL) -REFERENCE (J,JNE,16,201,62) -AUTHOR (D.C.STUPEGIA) -TITLE NEUTRON TOTAL CROSS SECTION OF U233. +REFERENCE (J,JNE/AB,16,201,1962) +AUTHOR (D.C.Stupegia) +TITLE Neutron total cross section of U233. STATUS (SCSRS) -HISTORY (760804T) TRANSLATED FROM SCISRS - (841005A) CONVERTED TO REACTION FORMALISM -ENDBIB 7 +HISTORY (19760804T) Translated from SCISRS + (19841005A) Converted to reaction formalism + (20050710C) DR Format updated and reference corrected +ENDBIB 8 NOCOMMON 0 0 -ENDSUBENT 10 -SUBENT 12323002 841005 +ENDSUBENT 11 +SUBENT 12323002 19841005 20050909 1336 BIB 1 1 REACTION (92-U-233(N,TOT),,SIG) ENDBIB 1 @@ -19,51 +20,51 @@ NOCOMMON 0 0 DATA 4 45 EN EN-RSL DATA DATA-ERR MEV MEV B B - 3.4 -03 1.2 -03 1.71 +01 5. -01 - 9.4 -03 1.4 -03 1.45 +01 2. -01 - 2.04 -02 1.5 -03 1.41 +01 2. -01 - 2.57 -02 1.6 -03 1.30 +01 3. -01 - 3.11 -02 1.8 -03 1.33 +01 3. -01 - 3.46 -02 1.8 -03 1.33 +01 2. -01 - 3.65 -02 1.8 -03 1.30 +01 2. -01 - 3.87 -02 1.8 -03 1.32 +01 2. -01 - 4.05 -02 1.8 -03 1.28 +01 3. -01 - 4.22 -02 1.9 -03 1.25 +01 2. -01 - 4.41 -02 1.9 -03 1.23 +01 2. -01 - 5.39 -02 1.9 -03 1.23 +01 2. -01 - 5.82 -02 1.9 -03 1.230 +01 1.8 -01 - 6.40 -02 1.9 -03 1.190 +01 1.7 -01 - 7.48 -02 1.9 -03 1.200 +01 1.5 -01 - 9.61 -02 1.9 -03 1.110 +01 1.4 -01 - 1.185 -01 2.0 -03 1.080 +01 1.4 -01 - 1.408 -01 2.1 -03 1.070 +01 1.4 -01 - 1.636 -01 2.2 -03 1.020 +01 1.5 -01 - 1.866 -01 2.3 -03 1.010 +01 1.6 -01 - 2.355 -01 5.7 -03 9.78 +00 1.3 -01 - 2.582 -01 2.4 -03 9.42 +00 1.6 -01 - 3.020 -01 5.7 -03 8.94 +00 1.6 -01 - 3.060 -01 2.5 -03 9.10 +00 1.6 -01 - 3.447 -01 5.8 -03 8.79 +00 1.4 -01 - 3.668 -01 5.8 -03 8.46 +00 1.3 -01 - 3.878 -01 5.9 -03 8.49 +00 1.3 -01 - 4.087 -01 6.0 -03 8.25 +00 1.3 -01 - 4.503 -01 6.1 -03 8.19 +00 1.3 -01 - 4.915 -01 6.1 -03 7.72 +00 1.3 -01 - 5.325 -01 6.2 -03 7.77 +00 1.3 -01 - 5.732 -01 6.3 -03 7.40 +00 1.3 -01 - 6.158 -01 6.4 -03 7.43 +00 1.3 -01 - 6.552 -01 6.5 -03 7.15 +00 1.4 -01 - 7.366 -01 6.7 -03 6.99 +00 1.4 -01 - 8.175 -01 6.8 -03 6.69 +00 1.4 -01 - 8.977 -01 6.9 -03 6.51 +00 1.4 -01 - 9.776 -01 7.0 -03 6.45 +00 1.4 -01 - 1.0576 +00 7.1 -03 6.37 +00 1.4 -01 - 1.1365 +00 7.4 -03 6.44 +00 1.4 -01 - 1.2163 +00 7.4 -03 6.23 +00 1.4 -01 - 1.2959 +00 7.5 -03 6.22 +00 1.4 -01 - 1.3745 +00 7.6 -03 6.15 +00 1.5 -01 - 1.4537 +00 7.8 -03 6.12 +00 1.5 -01 - 1.6112 +00 8.0 -03 6.39 +00 1.5 -01 + 3.4E-03 1.2E-03 1.71E+01 5.0E-01 + 9.4E-03 1.4E-03 1.45E+01 2.0E-01 + 2.04E-02 1.5E-03 1.41E+01 2.0E-01 + 2.57E-02 1.6E-03 1.30E+01 3.0E-01 + 3.11E-02 1.8E-03 1.33E+01 3.0E-01 + 3.46E-02 1.8E-03 1.33E+01 2.0E-01 + 3.65E-02 1.8E-03 1.30E+01 2.0E-01 + 3.87E-02 1.8E-03 1.32E+01 2.0E-01 + 4.05E-02 1.8E-03 1.28E+01 3.0E-01 + 4.22E-02 1.9E-03 1.25E+01 2.0E-01 + 4.41E-02 1.9E-03 1.23E+01 2.0E-01 + 5.39E-02 1.9E-03 1.23E+01 2.0E-01 + 5.82E-02 1.9E-03 1.23E+01 1.8E-01 + 6.40E-02 1.9E-03 1.19E+01 1.7E-01 + 7.48E-02 1.9E-03 1.20E+01 1.5E-01 + 9.61E-02 1.9E-03 1.11E+01 1.4E-01 + 1.185E-01 2.0E-03 1.08E+01 1.4E-01 + 1.408E-01 2.1E-03 1.07E+01 1.4E-01 + 1.636E-01 2.2E-03 1.02E+01 1.5E-01 + 1.866E-01 2.3E-03 1.01E+01 1.6E-01 + 2.355E-01 5.7E-03 9.78E+00 1.3E-01 + 2.582E-01 2.4E-03 9.42E+00 1.6E-01 + 3.020E-01 5.7E-03 8.94E+00 1.6E-01 + 3.060E-01 2.5E-03 9.10E+00 1.6E-01 + 3.447E-01 5.8E-03 8.79E+00 1.4E-01 + 3.668E-01 5.8E-03 8.46E+00 1.3E-01 + 3.878E-01 5.9E-03 8.49E+00 1.3E-01 + 4.087E-01 6.0E-03 8.25E+00 1.3E-01 + 4.503E-01 6.1E-03 8.19E+00 1.3E-01 + 4.915E-01 6.1E-03 7.72E+00 1.3E-01 + 5.325E-01 6.2E-03 7.77E+00 1.3E-01 + 5.732E-01 6.3E-03 7.40E+00 1.3E-01 + 6.158E-01 6.4E-03 7.43E+00 1.3E-01 + 6.552E-01 6.5E-03 7.15E+00 1.4E-01 + 7.366E-01 6.7E-03 6.99E+00 1.4E-01 + 8.175E-01 6.8E-03 6.69E+00 1.4E-01 + 8.977E-01 6.9E-03 6.51E+00 1.4E-01 + 9.776E-01 7.0E-03 6.45E+00 1.4E-01 + 1.0576E+00 7.1E-03 6.37E+00 1.4E-01 + 1.1365E+00 7.4E-03 6.44E+00 1.4E-01 + 1.2163E+00 7.4E-03 6.23E+00 1.4E-01 + 1.2959E+00 7.5E-03 6.22E+00 1.4E-01 + 1.3745E+00 7.6E-03 6.15E+00 1.5E-01 + 1.4537E+00 7.8E-03 6.12E+00 1.5E-01 + 1.6112E+00 8.0E-03 6.39E+00 1.5E-01 ENDDATA 47 ENDSUBENT 53 ENDENTRY 2 diff --git a/exforall/123/12365.x4 b/exforall/123/12365.x4 index ac6528bd9..562d1c0e4 100644 --- a/exforall/123/12365.x4 +++ b/exforall/123/12365.x4 @@ -1,35 +1,36 @@ -ENTRY 12365 860527 -SUBENT 12365001 860527 -BIB 9 12 +ENTRY 12365 20050711 20050909 1336 +SUBENT 12365001 20050711 20050909 1336 +BIB 9 13 INSTITUTE (1CANCRC) -REFERENCE (J,JNE,16,195,62) -AUTHOR (M.J.CABELL,L.J.SLEE) -TITLE THE RATIO OF NEUTRON CAPTURE FO FISSION FOR 233-U. -FACILITY (REAC) PLUTO REACTOR. -INC-SPECT REACTOR SPECTRUM R=0.022+-0.004, T=40 DEGR(C). -METHOD SAMPLES ANALYSED BY ISOTOPIC DILUTION AND MASS - SPECTROMETRY. +REFERENCE (J,JNE/AB,16,195,1962) +AUTHOR (M.J.Cabell,L.J.Slee) +TITLE The ratio of neutron capture to fission for 233-U. +FACILITY (REAC) Pluto reactor. +INC-SPECT Reactor spectrum R=0.022+-0.004, T=40 Degr(C). +METHOD Samples analyzed by isotopic dilution and mass + spectrometry. STATUS (SCSRS) -HISTORY (760804T) TRANSLATED FROM SCISRS - (820519A) CONVERTED TO REACTION FORMALISM - (860527A) COMPLETE UPDATE OF BIB. -ENDBIB 12 +HISTORY (19760804T) Translated from SCISRS + (19820519A) Converted to reaction formalism + (19860527A) Complete update of bib. + (20050710C) DR Format updated and reference corrected +ENDBIB 13 NOCOMMON 0 0 -ENDSUBENT 15 -SUBENT 12365002 860527 +ENDSUBENT 16 +SUBENT 12365002 19860527 20050909 1336 BIB 3 6 REACTION (92-U-233(N,ABS),,ALF) -FACILITY (SPECM) MASS SPECTROMETER -ANALYSIS FROM AVERAGE OF MEASUREMENTS IN 3 POSITIONS OF REACTOR - USING WESTCOTT'S 1960 G FACTORS. - UPDATED USING 1964 WESTCOTT'S TABLES BY OKAZAKI, ETAL, +FACILITY (SPECM) Mass spectrometer +ANALYSIS From average of measurements in 3 positions of reactor + using Westcott's 1960 G factors. + Updated using 1964 Westcott's tables by Okazaki, Etal, AECL-2148(64). ENDBIB 6 NOCOMMON 0 0 DATA 3 1 EN DATA DATA-ERR MEV NO-DIM NO-DIM - 2.53 -08 9.17 -02 2.2 -03 + 2.53E-08 9.17E-02 2.2E-03 ENDDATA 3 ENDSUBENT 14 ENDENTRY 2 diff --git a/exforall/124/12450.x4 b/exforall/124/12450.x4 index e86cc1f2d..b03b8144b 100644 --- a/exforall/124/12450.x4 +++ b/exforall/124/12450.x4 @@ -1,35 +1,36 @@ -ENTRY 12450 830809 -SUBENT 12450001 830809 -BIB 6 7 +ENTRY 12450 20050711 20050909 1336 +SUBENT 12450001 20050711 20050909 1336 +BIB 6 8 INSTITUTE (1USAANL) -REFERENCE (J,JNE,15,200,61) -AUTHOR (D.C.STUPEGIA,R.R.HENRICH,G.H.MC CLOUD) -TITLE NEUTRON CAPTURE CROSS SECTION OF U236. +REFERENCE (J,JNE/AB,15,200,1961) +AUTHOR (D.C.Stupegia,R.R.Henrich,G.H.McCloud) +TITLE Neutron cpature cross section of U236. STATUS (SCSRS) -HISTORY (760804T) TRANSLATED FROM SCISRS - (830809A) CONVERTED TO REACTION FORMALISM -ENDBIB 7 +HISTORY (19760804T) Translated from SCISRS + (19830809A) Convertes to reaction formalism + (20050710C) DR Format updated and reference corrected +ENDBIB 8 NOCOMMON 0 0 -ENDSUBENT 10 -SUBENT 12450002 830809 +ENDSUBENT 11 +SUBENT 12450002 19830809 20050909 1336 BIB 3 4 REACTION (92-U-236(N,G)92-U-237,,SIG) -METHOD (ACTIV) ACTIVATION +METHOD (ACTIV) Activation MONITOR (92-U-235(N,F),,SIG) - RELATIVE TO U235 FISSION. + Relative to U235 fission. ENDBIB 4 NOCOMMON 0 0 DATA 4 8 EN DATA DATA-ERR DATA-MAX MEV MB MB MB - 3.00 -01 2.65 +02 3.0 +01 - 4.57 -01 2.57 +02 2.0 +01 - 6.55 -01 2.73 +02 2.1 +01 - 7.50 -01 2.99 +02 2.1 +01 - 9.40 -01 3.24 +02 2.8 +01 - 1.200 +00 2.68 +02 1.9 +01 - 1.446 +00 2.16 +02 1.9 +01 - 1.732 +00 1.00 +02 + 3.00E-01 2.65E+02 3.0E+01 + 4.57E-01 2.57E+02 2.0E+01 + 6.55E-01 2.73E+02 2.1E+01 + 7.50E-01 2.99E+02 2.1E+01 + 9.40E-01 3.24E+02 2.8E+01 + 1.200E+00 2.68E+02 1.9E+01 + 1.446E+00 2.16E+02 1.9E+01 + 1.732E+00 1.00E+02 ENDDATA 10 ENDSUBENT 19 ENDENTRY 2 diff --git a/exforall/125/12532.x4 b/exforall/125/12532.x4 index bffc14b9d..1cc7b29f9 100644 --- a/exforall/125/12532.x4 +++ b/exforall/125/12532.x4 @@ -1,32 +1,33 @@ -ENTRY 12532 841004 -SUBENT 12532001 841004 -BIB 6 8 +ENTRY 12532 20050713 20050909 1336 +SUBENT 12532001 20050713 20050909 1336 +BIB 6 9 INSTITUTE (1USAANL) -REFERENCE (J,JNE,11,21,59) - (C,55GENEVA,7,261,55) -AUTHOR (A.H.JAFFEY,C.T.HIBDON,R.SJOBLOM) -TITLE THERMAL NEUTRON NU BAR FOR 241PU. +REFERENCE (J,JNE/A,11,21,1959) + (C,55GENEVA,7,261,1955) +AUTHOR (A.H.Jaffey,C.T.Hibdon,R.Sjoblom) +TITLE Thermal neutron nu bar for 241Pu. STATUS (SCSRS) -HISTORY (760804T) TRANSLATED FROM SCISRS - (841004A) CONVERTED TO REACTION FORMALISM -ENDBIB 8 +HISTORY (19760804T) Translated from SCISRS + (19841004A) Converted to reaction formalism + (20050713C) DR Format updated and reference corrected +ENDBIB 9 NOCOMMON 0 0 -ENDSUBENT 11 -SUBENT 12532002 841004 +ENDSUBENT 12 +SUBENT 12532002 19841004 20050909 1336 BIB 4 7 REACTION (94-PU-241(N,F),,NU,,MXW) -METHOD RING GEOMETRY -MONITOR MEASURED G*FISSION C/S*NU RELATIVE TO U-233, U-235, AND - PU-239. CALCULATED G*FISSION C/S*NU = 3162+-72 FOR - PU-241 FROM AVERAGE FOR 3 STANDARDS. ASSUMED PU-241 - G*FISSION C/S = 1070+-14 B. -INC-SPECT THERMAL SPECTRUM +METHOD Ring geometry +MONITOR Measured g*fission C/S*nu relative to U-233, U-235, and + Pu-239. Calculated g*fission C/S*nu = 3162+-72 for + Pu-241 from average for 3 standards. Assumed Pu-241 + g*fission C/S = 1070+-14 B. +INC-SPECT Thermal spectrum ENDBIB 7 NOCOMMON 0 0 DATA 3 1 EN-DUMMY DATA DATA-ERR -MEV NO-DIM NO-DIM - 2.53 -08 2.96 +00 8. -02 +MEV PRT/FIS PRT/FIS + 2.53E-08 2.96E+00 0.02 ENDDATA 3 ENDSUBENT 15 ENDENTRY 2 diff --git a/exforall/125/12562.x4 b/exforall/125/12562.x4 index a4d509b95..e2361d0aa 100644 --- a/exforall/125/12562.x4 +++ b/exforall/125/12562.x4 @@ -1,64 +1,65 @@ -ENTRY 12562 841004 -SUBENT 12562001 841004 -BIB 6 8 +ENTRY 12562 20050713 20050909 1336 +SUBENT 12562001 20050713 20050909 1336 +BIB 6 9 INSTITUTE (1USAANL) -REFERENCE (J,JIN,27,33,64) -AUTHOR (D.METTA,H.DIAMOND,R.F.BARNES,J.MILSTED,J.GRAY JR, - D.J.HENDERSON,C.M.STEVENS) -TITLE NUCLEAR CONSTANTS OF NINE TRANSPLUTONIUM NUCLIDES. +REFERENCE (J,JIN,27,33,1965) +AUTHOR (D.Metta,H.Diamond,R.F.Barnes,J.Milsted,J.Gray Jr, + D.J.Henderson,C.M.Stevens) +TITLE Nuclear constants of nine transplutonium nuclides. STATUS (SCSRS) -HISTORY (760804T) TRANSLATED FROM SCISRS - (841004A) CONVERTED TO REACTION FORMALISM -ENDBIB 8 +HISTORY (19760804T) Translated from SCISRS + (19841004A) Converted to reaction formalism + (20050713C) DR Format updated and reference corrected +ENDBIB 9 NOCOMMON 0 0 -ENDSUBENT 11 -SUBENT 12562002 841004 +ENDSUBENT 12 +SUBENT 12562002 19841004 20050909 1336 BIB 4 6 REACTION (98-CF-249(N,F),,SIG,,MXW) -DETECTOR (FISCH) BACK-TO-BACK FISSION COUNTER +DETECTOR (FISCH) Back-to-back fission counter MONITOR (92-U-233(N,F),,SIG) - BASED ON U233 THERMAL FISSION=526B AND - CF249 HALF-LIFE=320YR. -INC-SPECT THERMAL SPECTRUM + Based on U233 thermal fission=526B and + Cf249 Half-life=320Yr. +INC-SPECT Thermal spectrum ENDBIB 6 NOCOMMON 0 0 DATA 3 1 EN-DUMMY DATA DATA-ERR MEV B B - 2.53 -08 1.735 +03 7.0 +01 + 2.53E-08 1.735E+03 7.0E+01 ENDDATA 3 ENDSUBENT 14 -SUBENT 12562003 841004 +SUBENT 12562003 19841004 20050909 1336 BIB 3 3 REACTION (98-CF-250(N,F),,SIG,,MXW) -REFERENCE (W,DIAMOND,64) -INC-SPECT THERMAL SPECTRUM +REFERENCE (W,DIAMOND,1964) +INC-SPECT Thermal spectrum ENDBIB 3 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA-MAX MEV B - 2.53 -08 3.50 +02 + 2.53e-08 3.50E+02 ENDDATA 3 ENDSUBENT 11 -SUBENT 12562004 841004 +SUBENT 12562004 19841004 20050909 1336 BIB 6 10 REACTION (98-CF-251(N,F),,SIG,,MXW) -SAMPLE SAMPLE COMPOSITION - CF-249 (7.6+-0.8 PERCENT), - CF-250 (33.3+-1.1 PERCENT), CF-251(12.7+-0.6 PERCENT), - CF-252 (46.4+-1.5 PERCENT) -DETECTOR (FISCH) BACK-TO-BACK FISSION COUNTER +SAMPLE Sample composition - Cf-249 (7.6+-0.8 percent), + Cf-250 (33.3+-1.1 percent), Cf-251(12.7+-0.6 percent), + Cf-252 (46.4+-1.5 percent) +DETECTOR (FISCH) Back-to-back fission counter MONITOR (94-PU-239(N,F),,SIG) - BASED ON PU239 FISSION=803B FOR THERMAL - SPECTRUM AT 65 DEGR, CF-249 FISSION = 1735+-70 B. -COMMENT ASSUMED NO FISSION FROM CF250 AND CF252. -INC-SPECT THERMAL SPECTRUM + Based on Pu239 fission=803B for thermal + spectrum at 65 Degr, Cf-249 fission = 1735+-70 B. +COMMENT Assumed no fission from Cf250 and Cf252. +INC-SPECT Thermal spectrum ENDBIB 10 NOCOMMON 0 0 DATA 3 1 EN-DUMMY DATA DATA-ERR MEV B B - 2.53 -08 3.000 +03 2.60 +02 + 2.53E-08 3.000E+03 2.60E+02 ENDDATA 3 ENDSUBENT 18 ENDENTRY 4 diff --git a/exforall/125/12563.x4 b/exforall/125/12563.x4 index 4922b2dfc..142d3dfe3 100644 --- a/exforall/125/12563.x4 +++ b/exforall/125/12563.x4 @@ -1,34 +1,32 @@ -ENTRY 12563 841004 -SUBENT 12563001 841004 -BIB 6 8 +ENTRY 12563 20050713 20050909 1336 +SUBENT 12563001 20050713 20050909 1336 +BIB 6 9 INSTITUTE (1USALAS) -REFERENCE (J,JNE,20,588,66) -AUTHOR (K.WOLFSBERG,G.P.FORD,H.L.SMITH) -TITLE THERMAL NEUTRON-INDUCED FISSION CROSS SECTION OF - AM242M. +REFERENCE (J,JNE/AB,20,588,1966) +AUTHOR (K.Wolfsberg,G.P.Ford,H.L.Smith) +TITLE Thermal neutron-induced fission cross section of + Am242m. STATUS (SCSRS) -HISTORY (760804T) TRANSLATED FROM SCISRS - (841004A) CONVERTED TO REACTION FORMALISM -ENDBIB 8 +HISTORY (19760804T) Translated from SCISRS + (19841004A) Converted to reaction formalism + (20050713C) DR Format updated and reference corrected +ENDBIB 9 NOCOMMON 0 0 -ENDSUBENT 11 -SUBENT 12563002 841004 -BIB 4 5 +ENDSUBENT 12 +SUBENT 12563002 19841004 20050909 1336 +BIB 5 6 REACTION (95-AM-242-M1(N,F),,SIG,,MXW) -DETECTOR (FISCH) IONIZATION CHAMBER +DECAY-DATA (95-AM-242-M1,152.YR) +DETECTOR (FISCH) Ionization chamber MONITOR (92-U-235(N,F),,SIG) - BASED ON U235 THERMAL FISSION=569+-4B. -INC-SPECT THERMAL SPECTRUM -ENDBIB 5 -COMMON 1 3 -HL -YR - 152. -ENDCOMMON 3 + Based on U235 thermal fission=569+-4B. +INC-SPECT Thermal spectrum +ENDBIB 6 +NOCOMMON 0 0 DATA 5 1 EN-DUMMY DATA DATA-ERR MONIT MONIT-ERR MEV B B B B - 2.53 -08 7.200 +03 3.00 +02 569. 4. + 2.53E-08 7.200E+03 3.00E+02 569. 4. ENDDATA 3 -ENDSUBENT 17 +ENDSUBENT 14 ENDENTRY 2 diff --git a/exforall/125/12592.x4 b/exforall/125/12592.x4 index 574568dde..47ce3a4c4 100644 --- a/exforall/125/12592.x4 +++ b/exforall/125/12592.x4 @@ -1,26 +1,27 @@ -ENTRY 12592 780324 -SUBENT 12592001 780324 -BIB 10 11 +ENTRY 12592 20050714 20050909 1336 +SUBENT 12592001 20050714 20050909 1336 +BIB 10 12 INSTITUTE (1USAMIT) -REFERENCE (J,PR,75,781,5408) -AUTHOR (G.A.BAZORGAN,J.W.IRVINE JR.,C.D.CORYELL) -TITLE PREPARATION AND HALF-LIFE OF CR-55 -N-SOURCE (REAC)BROOKHAVEN REACTOR -SAMPLE HIGH-PURITY CR METAL 2-3 MILLIGRAMS. -METHOD 10 SEC IRRADIATION OF CR-54 WITH GOLD FOIL OF 0.001 IN. - THICKNESS,COMPARING ACTIVITIES. -DETECTOR (GEMUC)END-WINDOW GEIGER MUELLER TUBE. -INC-SPECT REACTOR PILE SPECTRUM -HISTORY (780224C) -ENDBIB 11 -NOCOMMON -ENDSUBENT 14 -SUBENT 12592002 780324 +REFERENCE (J,PR,95,781,1954) +AUTHOR (G.A.Bazorgan,J.W.Irvine Jr.,C.D.Coryell) +TITLE Preparation and half-life of Cr-55 +FACILITY (REAC) Brookhaven reactor +SAMPLE High-purity Cr metal 2-3 milligrams. +METHOD 10 sec irradiation of Cr-54 with gold foil of 0.001 in. + thickness,comparing activities. +DETECTOR (GEMUC) End-window Geiger Mueller tube. +INC-SPECT Reactor pile spectrum +HISTORY (19780224C) + (20050714C) DR Format updated and reference corrected +ENDBIB 12 +NOCOMMON 0 0 +ENDSUBENT 15 +SUBENT 12592002 19780324 20050909 1336 BIB 2 2 REACTION (24-CR-54(N,G)24-CR-55,,SIG,,SPA) MONITOR (79-AU-197(N,G)79-AU-198,,SIG,,SPA) ENDBIB 2 -NOCOMMON +NOCOMMON 0 0 DATA 4 1 EN-DUMMY DATA DATA-ERR MONIT EV B B B diff --git a/exforall/126/12612.x4 b/exforall/126/12612.x4 index b7bc0c62d..d5742dbdc 100644 --- a/exforall/126/12612.x4 +++ b/exforall/126/12612.x4 @@ -1,31 +1,32 @@ -ENTRY 12612 830808 -SUBENT 12612001 830808 -BIB 11 16 +ENTRY 12612 20050714 20050909 1336 +SUBENT 12612001 20050714 20050909 1336 +BIB 11 17 INSTITUTE (1USAMHG) -REFERENCE (J,PR,90,140,5305) -AUTHOR (W.MEINKE) -TITLE HALF-LIFE OF PD-109 AND NEUTRON ACTIVATION CROSS - SECTION OF PD-102 -N-SOURCE (REAC) CHALK RIVER NRX REACTOR -INC-SPECT PILE SPECTRUM -METHOD (ACTIV) ACTIVATION -DETECTOR (GEMUC) CHLORINE-QUENCHED ARGON-FILLED GEIGER-MULLER - TUBE. +REFERENCE (J,PR,90,410,1953) +AUTHOR (W.Meinke) +TITLE Half-life of Pd-109 and neutron activation cross + section of Pd-102 +FACILITY (REAC) Chalk River NRX reactor +INC-SPECT Pile spectrum +METHOD (ACTIV) Activation +DETECTOR (GEMUC) Chlorine-quenched argon-filled Geiger-Muller + tube. DECAY-DATA (47-AG-111-G,7.6D) (46-PD-103,17.D) (46-PD-109-G,13.6HR) -ERR-ANALYS ERROR BASED ON 20 PERCENT ERROR OF PD-108 CROSS SECTION -HISTORY (780502C) - (820827U) DECAY DATA CORRECTED. -ENDBIB 16 +ERR-ANALYS Error based on 20 percent error of Pd-108 cross section +HISTORY (19780502C) + (19820827U) Decay data corrected. + (20050714C) DR Format updated and reference corrected +ENDBIB 17 NOCOMMON 0 0 -ENDSUBENT 19 -SUBENT 12612002 780525 +ENDSUBENT 20 +SUBENT 12612002 19780525 20050909 1336 BIB 2 2 REACTION (46-PD-102(N,G)46-PD-103,,SIG,,SPA) MONITOR (46-PD-108(N,G)46-PD-109,,SIG,,SPA) ENDBIB 2 -NOCOMMON +NOCOMMON 0 0 DATA 4 1 EN-DUMMY DATA MONIT MONIT-ERR EV B B B diff --git a/exforall/126/12634.x4 b/exforall/126/12634.x4 index 05ca5c3fd..abffc117b 100644 --- a/exforall/126/12634.x4 +++ b/exforall/126/12634.x4 @@ -1,934 +1,935 @@ -ENTRY 12634 860811 -SUBENT 12634001 860811 -BIB 11 17 +ENTRY 12634 20050714 20050909 1336 +SUBENT 12634001 20050714 20050909 1336 +BIB 11 18 INSTITUTE (1USACOL) -REFERENCE (J,PR,48,256,3508) -AUTHOR (J.R.DUNNING,G.B.PEGRAM,G.A.FINK,D.P.MITCHELL) -TITLE INTERACTION OF NEUTRONS WITH MATTER. -INC-SOURCE RADON-BE SOURCE. HE-4 -BE REACTION. -INC-SPECT MEASUREMENTS WERE MADE FOR SLOW AND FAST NEUTRONS, - THE EXACT NEUTRON ENERGIES WERE NOT DETERMINED. - 0.025 EV FOR SLOW NEUTRONS AND 5 MEV FOR FAST - NEUTRONS ARE ENTERED BY THE COMPILER. -DETECTOR (IOCH) IONIZATION CHAMBER. -SAMPLE NATURAL SAMPLES OR COMPOUNDS WERE USED. -ERR-ANALYS ERRORS ARE OF THE ORDER OF 10 PERCENT FOR LOWER - CROSS SECTIONS AND ABOUT 25 PERCENT FOR THE LARGER - CROSS SECTIONS. -STATUS DATA TAKEN FROM TABLE IV OF THE JOURNAL ARTICLE. -HISTORY (840307C) - (860811A) DATA AT 5 MEV DELETED. NOT THIS EXPERIMENT. -ENDBIB 17 -NOCOMMON 0 0 -ENDSUBENT 20 -SUBENT 12634002 860811 +REFERENCE (J,PR,48,265,1935) +AUTHOR (J.R.Dunning,G.B.Pegram,G.A.Fink,D.P.Mitchell) +TITLE Interaction of neutrons with matter. +INC-SOURCE Radon-Be source. He-4 -Be reaction. +INC-SPECT Measurements were made for slow and fast neutrons, + the exact neutron energies were not determined. + 0.025 eV for slow neutrons and 5 MeV for fast + neutrons are entered by the compiler. +DETECTOR (IOCH) Ionization chamber. +SAMPLE Natural samples or compounds were used. +ERR-ANALYS Errors are of the order of 10 percent for lower + cross sections and about 25 percent for the larger + cross sections. +STATUS Data taken from Table IV of the journal article. +HISTORY (19840307C) + (19860811A) Data at 5 MeV deleted. Not this experiment. + (20050714C) DR Format updated and reference corrected +ENDBIB 18 +NOCOMMON 0 0 +ENDSUBENT 21 +SUBENT 12634002 19860811 20050909 1336 BIB 2 2 REACTION (1-H-1(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND (CH2)N. +SAMPLE Compound (CH2)N. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 35. + 2.5E-08 35. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634003 860811 +SUBENT 12634003 19860811 20050909 1336 BIB 2 2 REACTION (1-H-2(N,TOT),,SIG,,MXW) -SAMPLE D2O HEAVY WATER. +SAMPLE D2O heavy water. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 4.0 + 2.5E-08 4.0 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634004 860811 +SUBENT 12634004 19860811 20050909 1336 BIB 2 2 REACTION (3-LI-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND LIF +SAMPLE Compound LiF ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 45. + 2.5E-08 45. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634005 860811 +SUBENT 12634005 19860811 20050909 1336 BIB 2 2 REACTION (4-BE-9(N,TOT),,SIG,,MXW) -SAMPLE NATURAL BE. +SAMPLE Natural Be. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 5.3 + 2.5E-08 5.3 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634006 860811 +SUBENT 12634006 19860811 20050909 1336 BIB 2 2 REACTION (5-B-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND B4C. +SAMPLE Compound B4C. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 360. + 2.5E-08 360. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634007 860811 +SUBENT 12634007 19860811 20050909 1336 BIB 2 2 REACTION (6-C-0(N,TOT),,SIG,,MXW) -SAMPLE NAT CARBON SAMPLE. +SAMPLE Nat carbon sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 4.1 + 2.5E-08 4.1 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634008 860811 +SUBENT 12634008 19860811 20050909 1336 BIB 2 2 REACTION (7-N-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND NAN3. +SAMPLE Compound NaN3. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 11.3 + 2.5E-08 11.3 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634009 840531 +SUBENT 12634009 19840531 20050909 1336 BIB 2 2 REACTION (8-O-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND SIO2. +SAMPLE Compound SiO2. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 3.3 + 2.5E-08 3.3 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634010 840531 +SUBENT 12634010 19840531 20050909 1336 BIB 2 2 REACTION (9-F-19(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND NAF. +SAMPLE Compound NaF. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 2.5 + 2.5E-08 2.5 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634011 840531 +SUBENT 12634011 19840531 20050909 1336 BIB 2 2 REACTION (11-NA-23(N,TOT),,SIG,,MXW) -SAMPLE NA SAMPLE. +SAMPLE Na sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 4.2 + 2.5E-08 4.2 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634012 840531 +SUBENT 12634012 19840531 20050909 1336 BIB 2 2 REACTION (12-MG-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL MG SAMPLE. +SAMPLE Natural Mg sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 3.5 + 2.5E-08 3.5 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634013 860811 +SUBENT 12634013 19860811 20050909 1336 BIB 2 2 REACTION (13-AL-27(N,TOT),,SIG,,MXW) -SAMPLE AL SAMPLE. +SAMPLE Al sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 1.5 + 2.5E-08 1.5 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634014 840531 +SUBENT 12634014 19840531 20050909 1336 BIB 2 2 REACTION (14-SI-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL SI. +SAMPLE Natural Si. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 2.5 + 2.5E-08 2.5 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634015 840531 +SUBENT 12634015 19840531 20050909 1336 BIB 2 2 REACTION (15-P-31(N,TOT),,SIG,,MXW) -SAMPLE NATURAL P SAMPLE. +SAMPLE Natural P sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 14.7 + 2.5E-08 14.7 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634016 860811 +SUBENT 12634016 19860811 20050909 1336 BIB 2 2 REACTION (16-S-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL S SAMPLE. +SAMPLE Natural S sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 1.4 + 2.5E-08 1.4 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634017 840531 +SUBENT 12634017 19840531 20050909 1336 BIB 2 2 REACTION (17-CL-0(N,TOT),,SIG,,MXW) -SAMPLE NACL SAMPLE. +SAMPLE NaCl sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 39. + 2.5E-08 39. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634018 840531 +SUBENT 12634018 19840531 20050909 1336 BIB 2 2 REACTION (19-K-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL K SAMPLE. +SAMPLE Natural K sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 8.2 + 2.5E-08 8.2 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634019 840531 +SUBENT 12634019 19840531 20050909 1336 BIB 2 2 REACTION (20-CA-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND CAO SAMPLE. +SAMPLE Compound CaO sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 11.0 + 2.5E-08 11.0 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634020 840531 +SUBENT 12634020 19840531 20050909 1336 BIB 2 2 REACTION (22-TI-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND TIO2 SAMPLE. +SAMPLE Compound TiO2 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 11.9 + 2.5E-08 11.9 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634021 840531 +SUBENT 12634021 19840531 20050909 1336 BIB 2 2 REACTION (23-V-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND V2O5 SAMPLE. +SAMPLE Compound V2O5 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 10. + 2.5E-08 10. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634022 840531 +SUBENT 12634022 19840531 20050909 1336 BIB 2 2 REACTION (24-CR-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL CR SAMPLE. +SAMPLE Natural Cr sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 4.9 + 2.5E-08 4.9 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634023 840531 +SUBENT 12634023 19840531 20050909 1336 BIB 2 2 REACTION (25-MN-55(N,TOT),,SIG,,MXW) -SAMPLE NATURAL MN SAMPLE. +SAMPLE Natural Mn sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 14.3 + 2.5E-08 14.3 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634024 860811 +SUBENT 12634024 19860811 20050909 1336 BIB 2 2 REACTION (26-FE-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL FE SAMPLE. +SAMPLE Natural Fe sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 12.0 + 2.5E-08 12.0 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634025 840531 +SUBENT 12634025 19840531 20050909 1336 BIB 2 2 REACTION (27-CO-59(N,TOT),,SIG,,MXW) -SAMPLE NATURAL CO SAMPLE. +SAMPLE Natural Co sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 35. + 2.5E-08 35. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634026 840531 +SUBENT 12634026 19840531 20050909 1336 BIB 2 2 REACTION (28-NI-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL NI SAMPLE. +SAMPLE Natural Ni sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 15.4 + 2.5E-08 15.4 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634027 860811 +SUBENT 12634027 19860811 20050909 1336 BIB 2 2 REACTION (29-CU-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL CU SAMPLE. +SAMPLE Natural Cu sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 7.5 + 2.5E-08 7.5 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634028 860811 +SUBENT 12634028 19860811 20050909 1336 BIB 2 2 REACTION (30-ZN-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL ZN SAMPLE. +SAMPLE Natural Zn sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 4.7 + 2.5E-08 4.7 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634029 840531 +SUBENT 12634029 19840531 20050909 1336 BIB 3 5 REACTION (32-GE-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND GEO2 SAMPLE. -COMMENT THE REPORTED CROSS SECTION IS ONLY APPROXIMATE EITHER - BECAUSE A SMALL AMOUNT OF THE SAMPLE MATERIAL WAS - AVAILABLE OR BECAUSE OF OTHER FACTORS. +SAMPLE Compound GeO2 sample. +COMMENT The reported cross section is only approximate either + because a small amount of the sample material was + available or because of other factors. ENDBIB 5 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 75. + 2.5E-08 75. ENDDATA 3 ENDSUBENT 13 -SUBENT 12634030 840531 +SUBENT 12634030 19840531 20050909 1336 BIB 2 2 REACTION (33-AS-75(N,TOT),,SIG,,MXW) -SAMPLE NATURAL AS SAMPLE. +SAMPLE Natural As sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 8.6 + 2.5E-08 8.6 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634031 840531 +SUBENT 12634031 19840531 20050909 1336 BIB 2 2 REACTION (34-SE-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL SE SAMPLE. +SAMPLE Natural Se sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 19. + 2.5E-08 19. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634032 840531 +SUBENT 12634032 19840531 20050909 1336 BIB 2 2 REACTION (35-BR-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND KBR SAMPLE. +SAMPLE Compound KBr sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 11.8 + 2.5E-08 11.8 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634033 840531 +SUBENT 12634033 19840531 20050909 1336 BIB 3 5 REACTION (38-SR-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND SRCRO4 SAMPLE. -COMMENT THE REPORTED CROSS SECTION IS ONLY APPROXIMATE EITHER - BECAUSE A SMALL AMOUNT OF THE SAMPLE MATERIAL WAS - AVAILABLE OR BECAUSE OF OTHER FACTORS. +SAMPLE Compound SrCrO4 sample. +COMMENT The reported cross section is only approximate either + because a small amount of the sample material was + available or because of other factors. ENDBIB 5 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 9. + 2.5E-08 9. ENDDATA 3 ENDSUBENT 13 -SUBENT 12634034 840531 +SUBENT 12634034 19840531 20050909 1336 BIB 2 2 REACTION (39-Y-89(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND Y2O3 SAMPLE. +SAMPLE Compound Y2O3 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 800. + 2.5E-08 800. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634035 840531 +SUBENT 12634035 19840531 20050909 1336 BIB 2 2 REACTION (40-ZR-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND ZRO2 SAMPLE. +SAMPLE Compound ZrO2 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 16.7 + 2.5E-08 16.7 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634036 840531 +SUBENT 12634036 19840531 20050909 1336 BIB 3 5 REACTION (41-NB-93(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND NB2O5 SAMPLE. -COMMENT THE REPORTED CROSS SECTION IS ONLY APPROXIMATE EITHER - BECAUSE A SMALL AMOUNT OF THE SAMPLE MATERIAL WAS - AVAILABLE OR BECAUSE OF OTHER FACTORS. +SAMPLE Compound Nb2O5 sample. +COMMENT The reported cross section is only approximate either + because a small amount of the sample material was + available or because of other factors. ENDBIB 5 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 14. + 2.5E-08 14. ENDDATA 3 ENDSUBENT 13 -SUBENT 12634037 840531 +SUBENT 12634037 19840531 20050909 1336 BIB 2 2 REACTION (42-MO-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL MO SAMPLE. +SAMPLE Natural Mo sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 7.1 + 2.5E-08 7.1 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634038 840531 +SUBENT 12634038 19840531 20050909 1336 BIB 2 2 REACTION (44-RU-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL RU SAMPLE. +SAMPLE Natural Ru sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 12.5 + 2.5E-08 12.5 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634039 840531 +SUBENT 12634039 19840531 20050909 1336 BIB 2 2 REACTION (45-RH-103(N,TOT),,SIG,,MXW) -SAMPLE NATURAL RH SAMPLE. +SAMPLE Natural Rh sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 115. + 2.5E-08 115. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634040 840531 +SUBENT 12634040 19840531 20050909 1336 BIB 2 2 REACTION (46-PD-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL PD SAMPLE. +SAMPLE Natural Pd sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 10. + 2.5E-08 10. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634041 840531 +SUBENT 12634041 19840531 20050909 1336 BIB 2 2 REACTION (47-AG-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL AG SAMPLE. +SAMPLE Natural Ag sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 55. + 2.5E-08 55. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634042 840531 +SUBENT 12634042 19840531 20050909 1336 BIB 2 2 REACTION (48-CD-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL CD SAMPLE. +SAMPLE Natural Cd sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 3300. + 2.5E-08 3300. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634043 840531 +SUBENT 12634043 19840531 20050909 1336 BIB 2 2 REACTION (50-SN-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL SN SAMPLE. +SAMPLE Natural Sn sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 2 EN-DUMMY DATA MEV B -2.5 -08 4.0 + 2.5E-08 4.0 5.0 4.3 ENDDATA 4 ENDSUBENT 11 -SUBENT 12634044 840531 +SUBENT 12634044 19840531 20050909 1336 BIB 2 2 REACTION (51-SB-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL SB SAMPLE. +SAMPLE Natural Sb sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 8.1 + 2.5E-08 8.1 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634045 840531 +SUBENT 12634045 19840531 20050909 1336 BIB 2 2 REACTION (52-TE-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL TE SAMPLE. +SAMPLE Natural Te sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 8.2 + 2.5E-08 8.2 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634046 840531 +SUBENT 12634046 19840531 20050909 1336 BIB 2 2 REACTION (53-I-127(N,TOT),,SIG,,MXW) -SAMPLE NATURAL I SAMPLE. +SAMPLE Natural I sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 2 EN-DUMMY DATA MEV B -2.5 -08 9.4 + 2.5E-08 9.4 5.0 4.6 ENDDATA 4 ENDSUBENT 11 -SUBENT 12634047 840531 +SUBENT 12634047 19840531 20050909 1336 BIB 2 2 REACTION (56-BA-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND BAO SAMPLE. +SAMPLE Compound BaO sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 140. + 2.5E-08 140. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634048 840531 +SUBENT 12634048 19840531 20050909 1336 BIB 2 2 REACTION (57-LA-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND LA2O3 SAMPLE. +SAMPLE Compound La2O3 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 80. + 2.5E-08 80. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634049 840531 +SUBENT 12634049 19840531 20050909 1336 BIB 3 5 REACTION (58-CE-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND CEO2 SAMPLE. -COMMENT THE REPORTED CROSS SECTION IS ONLY APPROXIMATE EITHER - BECAUSE A SMALL AMOUNT OF THE SAMPLE MATERIAL WAS - AVAILABLE OR BECAUSE OF OTHER FACTORS. +SAMPLE Compound CeO2 sample. +COMMENT The reported cross section is only approximate either + because a small amount of the sample material was + available or because of other factors. ENDBIB 5 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 25. + 2.5E-08 25. ENDDATA 3 ENDSUBENT 13 -SUBENT 12634050 840531 +SUBENT 12634050 19840531 20050909 1336 BIB 2 2 REACTION (59-PR-141(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND PR2O3 SAMPLE. +SAMPLE Compound Pr2O3 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 25. + 2.5E-08 25. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634051 840531 +SUBENT 12634051 19840531 20050909 1336 BIB 2 2 REACTION (60-ND-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND ND2O3 SAMPLE. +SAMPLE Compound Nd2O3 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 220. + 2.5E-08 220. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634052 840531 +SUBENT 12634052 19840531 20050909 1336 BIB 2 2 REACTION (62-SM-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND SM2O3 SAMPLE. +SAMPLE Compound Sm2O3 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 4700. + 2.5E-08 4700. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634053 840531 +SUBENT 12634053 19840531 20050909 1336 BIB 3 6 REACTION (63-EU-0(N,TOT),,SIG,,MXW) -SAMPLE MIXTURE OF EU+GD+AL -COMMENT THE ENTERED VALUE IS THE UPPER LIMIT ESTIMATED. - THE REPORTED CROSS SECTION IS ONLY APPROXIMATE EITHER - BECAUSE A SMALL AMOUNT OF THE SAMPLE MATERIAL WAS - AVAILABLE OR BECAUSE OF OTHER FACTORS. +SAMPLE Mixture of Eu+Gd+Al +COMMENT The entered value is the upper limit extimated. + The reported cross section is only approximate either + because a small amount of the sample material was + available or because of other factors. ENDBIB 6 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 1000. + 2.5E-08 1000. ENDDATA 3 ENDSUBENT 14 -SUBENT 12634054 840531 +SUBENT 12634054 19840531 20050909 1336 BIB 2 2 REACTION (64-GD-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND GD2O3 SAMPLE. +SAMPLE Compound Gd2O3 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 30000. + 2.5E-08 30000. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634055 840531 +SUBENT 12634055 19840531 20050909 1336 BIB 3 6 REACTION (65-TB-159(N,TOT),,SIG,,MXW) -SAMPLE MIXTURE OF TB + AL -COMMENT ESTIMATED UPPER LIMIT IS GIVEN. - THE REPORTED CROSS SECTION IS ONLY APPROXIMATE EITHER - BECAUSE A SMALL AMOUNT OF THE SAMPLE MATERIAL WAS - AVAILABLE OR BECAUSE OF OTHER FACTORS. +SAMPLE Mixture of Tb + Al +COMMENT The entered value is the upper limit extimated. + The reported cross section is only approximate either + because a small amount of the sample material was + available or because of other factors. ENDBIB 6 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 1000. + 2.5E-08 1000. ENDDATA 3 ENDSUBENT 14 -SUBENT 12634056 840531 +SUBENT 12634056 19840531 20050909 1336 BIB 2 2 REACTION (66-DY-0(N,TOT),,SIG,,MXW) -SAMPLE MIXTURE OF DY + AL SAMPLE. +SAMPLE Mixture of Dy + Al sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 700. + 2.5E-08 700. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634057 840531 +SUBENT 12634057 19840531 20050909 1336 BIB 3 5 REACTION (67-HO-165(N,TOT),,SIG,,MXW) -SAMPLE MIXTURE OF HO+AL SAMPLE. -COMMENT THE REPORTED CROSS SECTION IS ONLY APPROXIMATE EITHER - BECAUSE A SMALL AMOUNT OF THE SAMPLE MATERIAL WAS - AVAILABLE OR BECAUSE OF OTHER FACTORS. +SAMPLE Mixture of Ho+Al sample. +COMMENT The reported cross section is only approximate either + because a small amount of the sample material was + available or because of other factors. ENDBIB 5 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 400. + 2.5E-08 400. ENDDATA 3 ENDSUBENT 13 -SUBENT 12634058 840531 +SUBENT 12634058 19840531 20050909 1336 BIB 2 2 REACTION (68-ER-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND ER2O3 SAMPLE. +SAMPLE Compound Er2O3 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 120. + 2.5E-08 120. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634059 840531 +SUBENT 12634059 19840531 20050909 1336 BIB 3 5 REACTION (69-TM-169(N,TOT),,SIG,,MXW) -SAMPLE MIXTURE OF TM+AL SAMPLE. -COMMENT THE REPORTED CROSS SECTION IS ONLY APPROXIMATE EITHER - BECAUSE A SMALL AMOUNT OF THE SAMPLE MATERIAL WAS - AVAILABLE OR BECAUSE OF OTHER FACTORS. +SAMPLE Mixture of Tm+Al sample. +COMMENT The reported cross section is only approximate either + because a small amount of the sample material was + available or because of other factors. ENDBIB 5 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 500. + 2.5E-08 500. ENDDATA 3 ENDSUBENT 13 -SUBENT 12634060 840531 +SUBENT 12634060 19840531 20050909 1336 BIB 2 2 REACTION (70-YB-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND YB2O3 SAMPLE. +SAMPLE Compound Yb2O3 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 90. + 2.5E-08 90. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634061 840531 +SUBENT 12634061 19840531 20050909 1336 BIB 3 5 REACTION (71-LU-0(N,TOT),,SIG,,MXW) -SAMPLE MIXTURE OF LU+AL SAMPLE. -COMMENT THE REPORTED CROSS SECTION IS ONLY APPROXIMATE EITHER - BECAUSE A SMALL AMOUNT OF THE SAMPLE MATERIAL WAS - AVAILABLE OR BECAUSE OF OTHER FACTORS. +SAMPLE Mixture of Lu+Al sample. +COMMENT The reported cross section is only approximate either + because a small amount of the sample material was + available or because of other factors. ENDBIB 5 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 400. + 2.5E-08 400. ENDDATA 3 ENDSUBENT 13 -SUBENT 12634062 840531 +SUBENT 12634062 19840531 20050909 1336 BIB 2 2 REACTION (73-TA-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL TA SAMPLE. +SAMPLE Natural Ta sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 27. + 2.5E-08 27. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634063 840531 +SUBENT 12634063 19840531 20050909 1336 BIB 2 2 REACTION (74-W-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL W SAMPLE. +SAMPLE Natural W sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 2 EN-DUMMY DATA MEV B -2.5 -08 23. + 2.5E-08 23. 5.0 5.3 ENDDATA 4 ENDSUBENT 11 -SUBENT 12634064 840531 +SUBENT 12634064 19840531 20050909 1336 BIB 2 2 REACTION (75-RE-187(N,TOT),,SIG,,MXW) -SAMPLE NATURAL RE SAMPLE. +SAMPLE Natural Re sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 89. + 2.5E-08 89. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634065 840531 +SUBENT 12634065 19840531 20050909 1336 BIB 2 2 REACTION (76-OS-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL OS SAMPLE. +SAMPLE Natural Os sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 27. + 2.5E-08 27. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634066 840531 +SUBENT 12634066 19840531 20050909 1336 BIB 2 2 REACTION (77-IR-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL IR SAMPLE. +SAMPLE Natural Ir sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 285. + 2.5E-08 285. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634067 840531 +SUBENT 12634067 19840531 20050909 1336 BIB 2 2 REACTION (78-PT-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL PT SAMPLE. +SAMPLE Natural Pt sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 25. + 2.5E-08 25. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634068 840531 +SUBENT 12634068 19840531 20050909 1336 BIB 2 2 REACTION (79-AU-197(N,TOT),,SIG,,MXW) -SAMPLE NATURAL AU SAMPLE. +SAMPLE Natural Au sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 88. + 2.5E-08 88. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634069 840531 +SUBENT 12634069 19840531 20050909 1336 BIB 2 2 REACTION (80-HG-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND HGO SAMPLE. +SAMPLE Compound HgO sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 2 EN-DUMMY DATA MEV B -2.5 -08 380. + 2.5E-08 380. 5.0 5.8 ENDDATA 4 ENDSUBENT 11 -SUBENT 12634070 840531 +SUBENT 12634070 19840531 20050909 1336 BIB 2 2 REACTION (81-TL-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL TL SAMPLE. +SAMPLE Natural Tl sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 11. + 2.5E-08 11. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634071 840531 +SUBENT 12634071 19840531 20050909 1336 BIB 2 2 REACTION (82-PB-0(N,TOT),,SIG,,MXW) -SAMPLE NATURAL PB SAMPLE. +SAMPLE Natural Pb sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 2 EN-DUMMY DATA MEV B -2.5 -08 8.6 + 2.5E-08 8.6 5.0 5.7 ENDDATA 4 ENDSUBENT 11 -SUBENT 12634072 840531 +SUBENT 12634072 19840531 20050909 1336 BIB 2 2 REACTION (83-BI-209(N,TOT),,SIG,,MXW) -SAMPLE NATURAL BI SAMPLE. +SAMPLE Natural Bi sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 8.2 + 2.5E-08 8.2 ENDDATA 3 ENDSUBENT 10 -SUBENT 12634073 840531 +SUBENT 12634073 19840531 20050909 1336 BIB 2 2 REACTION (90-TH-232(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND THO2 SAMPLE. +SAMPLE Compound ThO2 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 32. + 2.5E-08 32. ENDDATA 3 ENDSUBENT 10 -SUBENT 12634074 840531 +SUBENT 12634074 19840531 20050909 1336 BIB 2 2 REACTION (92-U-0(N,TOT),,SIG,,MXW) -SAMPLE COMPOUND UO2 SAMPLE. +SAMPLE Compound UO2 sample. ENDBIB 2 NOCOMMON 0 0 DATA 2 1 EN-DUMMY DATA MEV B -2.5 -08 43. + 2.5E-08 43. ENDDATA 3 ENDSUBENT 10 ENDENTRY 74 diff --git a/exforall/127/12736.x4 b/exforall/127/12736.x4 index b434a34b0..a88e44ba4 100644 --- a/exforall/127/12736.x4 +++ b/exforall/127/12736.x4 @@ -1,1385 +1,1386 @@ -ENTRY 12736 841207 -SUBENT 12736001 841207 -BIB 12 31 +ENTRY 12736 20050715 20050909 1336 +SUBENT 12736001 20050715 20050909 1336 +BIB 12 32 INSTITUTE (1USAORL) -REFERENCE (J,PR/C,24,505,8108) -AUTHOR (G.F.AUCHAMPAUGH,S.PLATTARD,N.W.HILL,G.DE SAUSSURE, - R.B.PEREZ,J.A.HARVEY) -TITLE COMPONENTS FOR THE 1.4,1.6 AND 1.7-MEV STRUCTURE IN - THE FISSION OF 232-TH+N. +REFERENCE (J,PR/C,24,503,1981) +AUTHOR (G.F.Auchampaugh,S.Plattard,N.W.Hill,G.De Saussure, + R.B.Perez,J.A.Harvey) +TITLE Components for the 1.4,1.6 and 1.7-MeV structure in + the fission of 232-Th+N. FACILITY (LINAC) ORELA -METHOD (TOF) NOMINAL TIME RESOLUTION OF 0.15 NS/M - THE 235-U DATA WERE REPEATEDLY SMOOTHED WITH A - THIRD-DEGREE 7-POINT SMOOTHING POLYNOMIAL BEFORE - FORMING THE RATIOS. -INC-SOURCE (PHOTO) WATER COOLED TANTALUM TARGET -DETECTOR FISSION-FRAGMENT DETECTOR CONSISTED OF- - SIX-CELL GAS SCINTILLATOR FILLED WITH A 0.98 PERCENT HE - 2 PECENT N2 MIXTURE AT STP. - FIVE CELLS CONTAIN NATURAL THORIUM, TWO CELLS VIEWED - FRAGMENTS EMITTED 0-90 DEG. TO THE NEUTRON BEAM - DIRECTION. THE OTHER THREE VIEWED FRAGMENTS EMITTED - FROM 0-23, 0-33.7 AND 0-51.7 DEG. - ONE CELL CONTAINED 93 PERCENT ENRICHED 235-U, WHICH - IS USED TO MEASURE NEUTRON SPECTRUM - EACH CELL IS VIEWED BY TWO XP 2020 Q,5-CM -DIAMETER - PHOTO MULTIPLIER TUBES. -ERR-ANALYS (ERR-S) STATISTICAL UNCERTAINTY -CORRECTION THE DATA WERE CORRECTED FOR- - DEAD TIME CORRECTION - TIME INDEPENDENT BACKGROUND - FLUX DATA CORRECED THE 238-U CONTRIBUTION (7 PERCENT) -STATUS DATA FROM PRIVATE COMM., DE SAUSSURE, 84/6/11. - (APRVD) G. DE SAUSSURE, 84/12/17. -HISTORY (840717C) -ENDBIB 31 +METHOD (TOF) Nominal time resolution of 0.15 ns/m + The 235-U data were repeatedly smoothed with a + third-degree 7-point smoothing polynomial before + forming the ratios. +INC-SOURCE (PHOTO) Water cooled tantalum target +DETECTOR Fission-fragment detector consisted of- + six-cell gas scintillator filled with a 0.98 percent He + 2 tercent N2 mixture at stp + Five cells contain natural thorium, two cells viewed + fragments emitted 0-90 deg. to the neutron beam + direction. The other three viewed fragments emitted + from 0-23, 0-33.7 and 0-51.7 deg. + One cell contained 93 percent enriched 235-U, which + is used to measure neutron spectrum + Each cell is viewed by two XP 2020 Q,5-cm -diameter + photo multiplier tubes. +ERR-ANALYS (ERR-S) Statistical uncertainty +CORRECTION The data were corrected for- + Dead time correction + Time independent background + Flux data corrected for the 238-U contribution (7 %) +STATUS Data from private comm., De Saussure, 84/6/11. + (APRVD) G. De Saussure, 84/12/17. +HISTORY (19840717C) + (20050715C) DR Format updated and reference corrected +ENDBIB 32 NOCOMMON 0 0 -ENDSUBENT 34 -SUBENT 12736002 841207 +ENDSUBENT 35 +SUBENT 12736002 19841207 20050909 1336 BIB 1 3 REACTION ((90-TH-232(N,F),,SIG,,FCT)/(92-U-235(N,F),,SIG,,FCT)) - ANGLE-INTEGRATED CROSS SECTION RATIOS TAKEN FOR THE - ANGULAR INTERVALS 0-23.4, 0-33.7, 0-51.7, 0-90 DEGREES. + Angle-integrated cross section ratios taken for the + angular intervals 0-23.4, 0-33.7, 0-51.7, 0-90 Degrees. ENDBIB 3 NOCOMMON 0 0 DATA 3 1335 EN DATA ERR-S MEV NO-DIM NO-DIM -7.17554E-018.70309E-061.67995E-05 -7.18366E-016.13851E-054.37718E-05 -7.19179E-013.39335E-053.28435E-05 -7.19994E-014.69862E-053.87912E-05 -7.20810E-013.45067E-053.33983E-05 -7.22447E-012.69310E-052.93380E-05 -7.23267E-015.99139E-054.32757E-05 -7.24089E-017.17783E-054.71622E-05 -7.24912E-017.31593E-054.75596E-05 -7.25737E-015.92937E-054.28277E-05 -7.26563E-016.67223E-054.53306E-05 -7.27391E-018.07261E-054.96747E-05 -7.28219E-014.47712E-053.69622E-05 -7.29050E-013.03179E-053.04316E-05 -7.29881E-013.84838E-053.41846E-05 -7.30715E-014.80454E-053.80776E-05 -7.31549E-015.74434E-054.14909E-05 -7.32385E-018.02335E-054.89109E-05 -7.33223E-016.72461E-054.49162E-05 -7.34061E-016.89386E-054.57924E-05 -7.34902E-011.07604E-045.76024E-05 -7.35743E-011.56380E-046.96824E-05 -7.36587E-011.47219E-046.74632E-05 -7.37431E-011.08821E-045.76381E-05 -7.38277E-011.60990E-046.95322E-05 -7.39125E-011.16962E-045.89323E-05 -7.39974E-015.75001E-054.12638E-05 -7.40824E-016.33397E-054.32822E-05 -7.41676E-011.23267E-046.04109E-05 -7.42530E-018.25017E-054.96080E-05 -7.43385E-011.34153E-046.33259E-05 -7.44241E-011.20697E-046.00584E-05 -7.45099E-017.20070E-054.63237E-05 -7.45958E-019.42621E-055.27748E-05 -7.46819E-017.91236E-054.82341E-05 -7.47681E-011.30743E-046.18882E-05 -7.48545E-017.91715E-054.82633E-05 -7.49411E-011.08172E-045.65082E-05 -7.50277E-012.75510E-052.87615E-05 -7.51146E-011.00202E-045.46248E-05 -7.52016E-011.46409E-046.60607E-05 -7.52887E-018.26157E-054.96765E-05 -7.53760E-019.42453E-055.29732E-05 -7.54634E-011.01903E-045.49439E-05 -7.55510E-019.92324E-055.40958E-05 -7.56387E-018.07111E-054.87516E-05 -7.57266E-015.21580E-053.92383E-05 -7.58147E-014.04019E-053.45520E-05 -7.59029E-015.18448E-053.90026E-05 -7.59913E-011.35221E-046.26225E-05 -7.60798E-017.98752E-054.80282E-05 -7.61684E-011.32452E-046.16708E-05 -7.62573E-011.17934E-045.81460E-05 -7.63462E-011.38421E-046.29364E-05 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4.5725E-03 + 7.6959E+00 2.2617E-01 4.5727E-03 + 7.7246E+00 2.2568E-01 4.5628E-03 + 7.7535E+00 2.2140E-01 4.4866E-03 + 7.7826E+00 2.1478E-01 4.3739E-03 + 7.8118E+00 2.1123E-01 4.3202E-03 + 7.8412E+00 2.1406E-01 4.3812E-03 + 7.8708E+00 2.1130E-01 4.3529E-03 + 7.9005E+00 2.1124E-01 4.3697E-03 + 7.9304E+00 2.1459E-01 4.4450E-03 + 7.9605E+00 2.1433E-01 4.4643E-03 + 7.9907E+00 2.1331E-01 4.4759E-03 + 8.0211E+00 2.1857E-01 4.5960E-03 + 8.0517E+00 2.1481E-01 4.5561E-03 + 8.0825E+00 2.1273E-01 4.5373E-03 + 8.1134E+00 2.1298E-01 4.5543E-03 + 8.1445E+00 2.1246E-01 4.5575E-03 + 8.1758E+00 2.0787E-01 4.4908E-03 + 8.2073E+00 2.0102E-01 4.3824E-03 + 8.2390E+00 2.0460E-01 4.4530E-03 + 8.2709E+00 2.0363E-01 4.4427E-03 + 8.3029E+00 2.0992E-01 4.5694E-03 + 8.3351E+00 2.0729E-01 4.5541E-03 + 8.3675E+00 2.1067E-01 4.6559E-03 + 8.4001E+00 2.1341E-01 4.7411E-03 + 8.4329E+00 2.1140E-01 4.7221E-03 + 8.4659E+00 2.1087E-01 4.7144E-03 + 8.4991E+00 2.0691E-01 4.6438E-03 + 8.5325E+00 2.0777E-01 4.6722E-03 + 8.5661E+00 2.0536E-01 4.6518E-03 + 8.5998E+00 2.0054E-01 4.5877E-03 + 8.6338E+00 1.9671E-01 4.5340E-03 + 8.6680E+00 1.9761E-01 4.5596E-03 + 8.7024E+00 1.9390E-01 4.4953E-03 + 8.7370E+00 1.9536E-01 4.5275E-03 + 8.7718E+00 1.9516E-01 4.5321E-03 + 8.8068E+00 1.9148E-01 4.4796E-03 + 8.8420E+00 1.9629E-01 4.5980E-03 + 8.8775E+00 1.9674E-01 4.6460E-03 + 8.9131E+00 2.0225E-01 4.7946E-03 + 8.9490E+00 2.0051E-01 4.8004E-03 + 8.9850E+00 1.9800E-01 4.7840E-03 + 9.0213E+00 1.9909E-01 4.8318E-03 + 9.0579E+00 1.9518E-01 4.7733E-03 + 9.0946E+00 1.9245E-01 4.7253E-03 + 9.1316E+00 1.9090E-01 4.6918E-03 + 9.1688E+00 1.8699E-01 4.6155E-03 + 9.2062E+00 1.8489E-01 4.5908E-03 + 9.2439E+00 1.8735E-01 4.6764E-03 + 9.2818E+00 1.9286E-01 4.8397E-03 + 9.3199E+00 1.9611E-01 4.9658E-03 + 9.3582E+00 1.9578E-01 5.0146E-03 + 9.3968E+00 1.9407E-01 5.0179E-03 + 9.4357E+00 1.9363E-01 5.0253E-03 + 9.4748E+00 1.9226E-01 4.9975E-03 + 9.5141E+00 1.8486E-01 4.8442E-03 + 9.5537E+00 1.8704E-01 4.9055E-03 + 9.5935E+00 1.8989E-01 4.9978E-03 + 9.6336E+00 1.8758E-01 4.9870E-03 + 9.6739E+00 1.8065E-01 4.8674E-03 + 9.7145E+00 1.7971E-01 4.8610E-03 + 9.7553E+00 1.7968E-01 4.8682E-03 + 9.7964E+00 1.7376E-01 4.7549E-03 + 9.8378E+00 1.7108E-01 4.7208E-03 + 9.8794E+00 1.7860E-01 4.9126E-03 + 9.9213E+00 1.8163E-01 5.0054E-03 + 9.9635E+00 1.8607E-01 5.1307E-03 + 1.0005E+01 1.8388E-01 5.1197E-03 + 1.0048E+01 1.8763E-01 5.2530E-03 + 1.0091E+01 1.9144E-01 5.3926E-03 + 1.0134E+01 1.9156E-01 5.4399E-03 + 1.0178E+01 1.9383E-01 5.5193E-03 + 1.0222E+01 1.9581E-01 5.5749E-03 + 1.0266E+01 1.9183E-01 5.4791E-03 + 1.0310E+01 1.8805E-01 5.3776E-03 + 1.0355E+01 1.8720E-01 5.3449E-03 + 1.0400E+01 1.8120E-01 5.2139E-03 + 1.0445E+01 1.8076E-01 5.2417E-03 + 1.0491E+01 1.8356E-01 5.3765E-03 + 1.0537E+01 1.8716E-01 5.5452E-03 + 1.0583E+01 1.9347E-01 5.7670E-03 + 1.0629E+01 1.9898E-01 5.9405E-03 + 1.0676E+01 2.0268E-01 6.0447E-03 + 1.0723E+01 2.0592E-01 6.1314E-03 + 1.0771E+01 1.9874E-01 5.9741E-03 + 1.0818E+01 1.9228E-01 5.8359E-03 + 1.0866E+01 1.8475E-01 5.6579E-03 + 1.0915E+01 1.8159E-01 5.5698E-03 + 1.0963E+01 1.7634E-01 5.4320E-03 + 1.1012E+01 1.7898E-01 5.5101E-03 + 1.1062E+01 1.7759E-01 5.5160E-03 + 1.1111E+01 1.7629E-01 5.5320E-03 + 1.1161E+01 1.7661E-01 5.5773E-03 + 1.1212E+01 1.7526E-01 5.5745E-03 + 1.1263E+01 1.7484E-01 5.6073E-03 + 1.1314E+01 1.8436E-01 5.9174E-03 + 1.1365E+01 1.8928E-01 6.1250E-03 + 1.1417E+01 1.8568E-01 6.1013E-03 + 1.1469E+01 1.9008E-01 6.2642E-03 + 1.1521E+01 1.8705E-01 6.2087E-03 + 1.1574E+01 1.8297E-01 6.1041E-03 + 1.1627E+01 1.8206E-01 6.0634E-03 + 1.1681E+01 1.8547E-01 6.1200E-03 + 1.1735E+01 1.8548E-01 6.0757E-03 + 1.1789E+01 1.6829E-01 5.5794E-03 + 1.1844E+01 1.4064E-01 4.8214E-03 + 1.1899E+01 1.2082E-01 4.2993E-03 + 1.1955E+01 9.9161E-02 3.7784E-03 + 1.2010E+01 8.2071E-02 3.4348E-03 + 1.2067E+01 7.7231E-02 3.5097E-03 ENDDATA 1337 ENDSUBENT 1345 ENDENTRY 2 diff --git a/exforall/127/12755.x4 b/exforall/127/12755.x4 index 0247932f1..987104ef6 100644 --- a/exforall/127/12755.x4 +++ b/exforall/127/12755.x4 @@ -1,58 +1,59 @@ -ENTRY 12755 821130 -SUBENT 12755001 821130 -BIB 13 30 +ENTRY 12755 20050715 20050909 1336 +SUBENT 12755001 20050715 20050909 1336 +BIB 13 31 INSTITUTE (1USAORL,2GERKFK) -REFERENCE (J,PR/C,26,26,8210) -AUTHOR (H.BEER,R.L.MACKLIN) -TITLE 178,179,180-HF ANS 180-TA(N,GAMMA) CROSS SECTIONS AND - THEIR CONTRIBUTION TO STELLAR NUCLEOSYNTHESIS -FACILITY (LINAC,1USAORL) OAK RIDGE ELECTRON LINEAR ACCELERATOR -INC-SPECT ENERGY RESOLUTION BETTER THAN 0.2 PERCENT. -METHOD (TOF) 40.12 METER FLIGHT PATH -DETECTOR (SCIN) 2 4-CM. THICK BY 10-CM. DIAMETER NON-HYDROGENOUS - LIQUID SCINTILLATORS FOR CAPTURE EVENTS. - (SCIN) 0.05 CM. THICK 6-LI GLASS SCINTILLATOR AS FLUX - MONITOR 43 CM IN FRONT OF THE SAMPLE -MONITOR (3-LI-6(N,T)2-HE-4,,SIG) FROM ENDF/B-V -CORRECTION DATA ARE CORRECTED FOR DEAD-TIME, TIME-DEPENDENT AND - TIME-INDEPENDENT BACKGROUNDS, SCATTERED NEUTRONS, - GAMMA-RAY ABSORPTION, ISOTOPIC IMPURITIES AND - DETECTOR EFFICIENCY. -ERR-ANALYS SYSTEMATIC UNCERTAINTIES IN PERCENT ARE- - DETECTOR CALIBRATION 2. - STANDARD CROSS SECTION 1. - 3. - PULSE HEIGHT WEIGHTING 1. - SAMPLE SCATTERED NEUTRONS LT 1.6 - GAMMA-RAY SELF-ABSORPTION 0.4 - MULTIPLE SCATTERING 0.5 - DETECTOR BIAS EXTRAPOLATION 0.4 - SAMPLE MISALIGNMENT LT 0.2 - DRIFT OF ELECTRONICS LT 0.4 - RESONANCE FITTING 3.0 -STATUS (APRVD) APPROVED BY R.L.MACKLIN, 82/12/13. -HISTORY (821128C) -ENDBIB 30 +REFERENCE (J,PR/C,26,1404,1982) +AUTHOR (H.Beer,R.L.Macklin) +TITLE 178,179,180-Hf and 180-Ta(n,gamma) cross sections and + their contribution to stellar nucleosynthesis +FACILITY (LINAC,1USAORL) Oak Ridge Electron Linear Accelerator +METHOD (TOF) 40.12 meter flight path +INC-SPECT Energy resolution better than 0.2 percent. +DETECTOR (SCIN) 2 4-cm. thick by 10-cm. diameter non-hydrogenous + liquid scintillators for capture events. + (SCIN) 0.05 cm. thick 6-Li glass scintillator as flux + monitor 43 cm in front of the sample +MONITOR (3-LI-6(N,T)2-HE-4,,SIG) from ENDF/B-V +CORRECTION Data are corrected for dead-time, time-dependent and + time-independent backgrounds, scattered neutrons, + gamma-ray absorption, isotopic impurities and + detector efficiency. +ERR-ANALYS Systematic uncertainties in percent are- + Detector calibration 2. + Standard cross section 1. - 3. + Pulse height weighting 1. + Sample scattered neutrons LT 1.6 + Gamma-ray self-absorption 0.4 + Multiple scattering 0.5 + Datector bias extrapolation 0.4 + Sample misalignment LT 0.2 + Drift of electronics LT 0.4 + Resonance fitting 3.0 +STATUS (APRVD) Approved by R.L.Macklin, 82/12/13. +HISTORY (19821128C) + (20050715C) DR Format updated and reference corrected +ENDBIB 31 NOCOMMON 0 0 -ENDSUBENT 33 -SUBENT 12755002 840917 +ENDSUBENT 34 +SUBENT 12755002 19840917 20050909 1336 BIB 6 17 REACTION 1(72-HF-178(N,0),,EN) 2(((72-HF-178(N,EL),,WID,,G)*(72-HF-178(N,G),,WID))/ (72-HF-178(N,TOT),,WID)) -SAMPLE HF(O)2 POWDER WITH A 10 PERCENT SULFUR BINDER. THE - ISOTOPIC PERCENT FRACTIONS ARE - 174-HF LESS THAN 0.05 - 176-HF 0.022 - 177-HF 1.54 - 178-HF 94.72 - 179-HF 1.84 - 180-HF 1.69 - THE SAMPLES ARE 2.6 X 2.6 CM WITH THICHNESSES OF - 0.14 AND 0.16 CM RESPECTIVELY. +SAMPLE Hf(O)2 powder with a 10 percent sulfur binder. The + isotopic percent fractions are + 174-Hf less than 0.05 + 176-Hf 0.022 + 177-Hf 1.54 + 178-Hf 94.72 + 179-Hf 1.84 + 180-Hf 1.69 + The samples are 2.6 X 2.6 cm with thicknesses of + 0.14 and 0.16 cm respectively. ANALYSIS (SHAPE) -ERR-ANALYS (DATA-ERR)STATISTICAL UNCERTAINTY ONLY. -FLAG (1.) PROBABLE DOUBLET OR MULTIPLET -HISTORY (840917A) 2 RESONACE ENERGIES CORRECTED. +ERR-ANALYS (DATA-ERR) Statistical uncertainty only. +FLAG (1.) Probable doublet or multiplet +HISTORY (19840917A) 2 Resonance energies corrected. ENDBIB 17 NOCOMMON 0 0 DATA 4 184 @@ -244,22 +245,22 @@ EV MILLI-EV MILLI-EV NO-DIM 8924. 13.0 1.6 ENDDATA 186 ENDSUBENT 208 -SUBENT 12755003 821130 +SUBENT 12755003 19821130 20050909 1336 BIB 4 14 REACTION 1(72-HF-179(N,0),,EN) 2(((72-HF-179(N,EL),,WID,,G)*(72-HF-179(N,G),,WID))/ (72-HF-179(N,TOT),,WID)) -SAMPLE HF(O)2 POWDER WITH A 10 PERCENT SULFUR BINDER. THE - ISOTOPIC PERCENT FRACTIONS ARE - 174-HF LESS THAN 0.05 - 176-HF 0.56 - 177-HF 3.42 - 178-HF 5.42 - 179-HF 81.85 - 180-HF 8.74 - THE SAMPLES ARE 2.6 X 2.6 CM X 0.15 CM THICK +SAMPLE Hf(O)2 powder with a 10 percent sulfur binder. The + isotopic percent fractions are + 174-Hf less than 0.05 + 176-Hf 0.56 + 177-Hf 3.42 + 178-Hf 5.42 + 179-Hf 81.85 + 180-Hf 8.74 + The samples are 2.6 X 2.6 cm X 0.15 cm thick ANALYSIS (SHAPE) -ERR-ANALYS (DATA-ERR)STATISTICAL UNCERTAINTY ONLY. +ERR-ANALYS (DATA-ERR) Statistical uncertainties only. ENDBIB 14 NOCOMMON 0 0 DATA 3 41 @@ -308,23 +309,23 @@ EV MILLI-EV MILLI-EV 3069. 46.9 2.4 ENDDATA 43 ENDSUBENT 62 -SUBENT 12755004 821130 +SUBENT 12755004 19821130 20050909 1336 BIB 5 15 REACTION 1(72-HF-180(N,0),,EN) 2(((72-HF-180(N,EL),,WID,,G)*(72-HF-180(N,G),,WID))/ (72-HF-180(N,TOT),,WID)) -SAMPLE HF(O)2 POWDER WITH A 10 PERCENT SULFUR BINDER. THE - ISOTOPIC PERCENT FRACTIONS ARE - 174-HF LESS THAN 0.05 - 176-HF 0.23 - 177-HF 1.0 - 178-HF 2.22 - 179-HF 2.66 - 180-HF 93.89 - THE SAMPLES ARE 2.6 X 2.6 CM X 0.15 CM THICK +SAMPLE Hf(O)2 powder with a 10 percent sulfur binder. The + isotopic percent fractions are + 174-Hf less than 0.05 + 176-Hf 0.23 + 177-Hf 1.0 + 178-Hf 2.22 + 179-Hf 2.66 + 180-Hf 93.89 + The samples are 2.6 X 2.6 cm X 0.15 cm thick ANALYSIS (SHAPE) -ERR-ANALYS (DATA-ERR)STATISTICAL UNCERTAINTY ONLY. -FLAG (1.) PROBABLE DOUBLET OR MULTIPLET +ERR-ANALYS (DATA-ERR) Statistical uncertainties only. +FLAG (1.) Probable doublet or multiplet ENDBIB 15 NOCOMMON 0 0 DATA 4 135 @@ -467,23 +468,23 @@ EV MILLI-EV MILLI-EV NO-DIM 9865. 22.5 1.3 ENDDATA 137 ENDSUBENT 157 -SUBENT 12755005 821130 +SUBENT 12755005 19821130 20050909 1336 BIB 4 15 REACTION 1(72-HF-178(N,0),,EN) 2(72-HF-178(N,EL),,WID,,G) 3(72-HF-178(N,G),,WID) -SAMPLE HF(O)2 POWDER WITH A 10 PERCENT SULFUR BINDER. THE - ISOTOPIC PERCENT FRACTIONS ARE - 174-HF LESS THAN 0.05 - 176-HF 0.022 - 177-HF 1.54 - 178-HF 94.72 - 179-HF 1.84 - 180-HF 1.69 - THE SAMPLES ARE 2.6 X 2.6 CM WITH THICHNESSES OF - 0.14 AND 0.16 CM RESPECTIVELY. +SAMPLE Hf(O)2 powder with a 10 percent sulfur binder. The + isotopic percent fractions are + 174-Hf less than 0.05 + 176-Hf 0.022 + 177-Hf 1.54 + 178-Hf 94.72 + 179-Hf 1.84 + 180-Hf 1.69 + The samples are 2.6 X 2.6 cm with thicknesses of + 0.14 and 0.16 cm respectively. ANALYSIS (SHAPE) -ERR-ANALYS (DATA-ERR)STATISTICAL UNCERTAINTY ONLY. +ERR-ANALYS (DATA-ERR) Statistical uncertainty only. ENDBIB 15 COMMON 1 3 MOMENTUM L @@ -499,22 +500,22 @@ EV EV EV MILLI-EV MILLI-EV 7497. 7.11 0.32 72.6 2.1 ENDDATA 6 ENDSUBENT 30 -SUBENT 12755006 821130 +SUBENT 12755006 19821130 20050909 1336 BIB 4 14 REACTION 1(72-HF-180(N,0),,EN) 2(72-HF-180(N,EL),,WID,,G) 3(72-HF-180(N,G),,WID) -SAMPLE HF(O)2 POWDER WITH A 10 PERCENT SULFUR BINDER. THE - ISOTOPIC PERCENT FRACTIONS ARE - 174-HF LESS THAN 0.05 - 176-HF 0.23 - 177-HF 1.0 - 178-HF 2.22 - 179-HF 2.66 - 180-HF 93.89 - THE SAMPLES ARE 2.6 X 2.6 CM X 0.15 CM THICK +SAMPLE Hf(O)2 powder with a 10 percent sulfur binder. The + isotopic percent fractions are + 174-Hf less than 0.05 + 176-Hf 0.23 + 177-Hf 1.0 + 178-Hf 2.22 + 179-Hf 2.66 + 180-Hf 93.89 + The samples are 2.6 x 2.6 cm x 0.15 cm thick ANALYSIS (SHAPE) -ERR-ANALYS (DATA-ERR)STATISTICAL UNCERTAINTY ONLY. +ERR-ANALYS (DATA-ERR) Statistical uncertainty only. ENDBIB 14 COMMON 1 3 MOMENTUM L @@ -536,21 +537,21 @@ EV EV EV MILLI-EV MILLI-EV 6977. 2.60 0.14 96.5 3.7 ENDDATA 12 ENDSUBENT 35 -SUBENT 12755007 821130 +SUBENT 12755007 19821130 20050909 1336 BIB 3 13 REACTION (72-HF-178(N,G)72-HF-179,,SIG,,AV) -SAMPLE HF(O)2 POWDER WITH A 10 PERCENT SULFUR BINDER. THE - ISOTOPIC PERCENT FRACTIONS ARE +SAMPLE Hf(O)2 powder with a 10 percent sulfur binder. The + isotopic percent fractions are 174-HF LESS THAN 0.05 176-HF 0.022 177-HF 1.54 178-HF 94.72 179-HF 1.84 180-HF 1.69 - THE SAMPLES ARE 2.6 X 2.6 CM WITH THICHNESSES OF - 0.14 AND 0.16 CM RESPECTIVELY. -CORRECTION DATA CORRECTED FOR AVERAGE RESONANCE SELF-PROTECTION - AND IN-SAMPLE SCATTERING. + The samples are 2.6 x 2.6 cm with thicknesses of + 0.14 and 0.16 cm respectively. +CORRECTION Data corrected for average resonance self-protection + and in-sample scattering. ENDBIB 13 NOCOMMON 0 0 DATA 3 30 @@ -588,20 +589,20 @@ KEV KEV MB 1800. 1900. 71. ENDDATA 32 ENDSUBENT 50 -SUBENT 12755008 821130 +SUBENT 12755008 19821130 20050909 1336 BIB 3 12 REACTION (72-HF-179(N,G)72-HF-180,,SIG,,AV) -SAMPLE HF(O)2 POWDER WITH A 10 PERCENT SULFUR BINDER. THE - ISOTOPIC PERCENT FRACTIONS ARE - 174-HF LESS THAN 0.05 - 176-HF 0.56 - 177-HF 3.42 - 178-HF 5.42 - 179-HF 81.85 - 180-HF 8.74 - THE SAMPLES ARE 2.6 X 2.6 CM X 0.15 CM THICK -CORRECTION DATA CORRECTED FOR AVERAGE RESONANCE SELF-PROTECTION - AND IN-SAMPLE SCATTERING. +SAMPLE Hf(O)2 powder with a 10 percent sulfur binder. The + isotopic percent fractions are + 174-Hf less than 0.05 + 176-Hf 0.56 + 177-Hf 3.42 + 178-Hf 5.42 + 179-Hf 81.85 + 180-Hf 8.74 + The samples are 2.6 x 2.6 cm x 0.15 cm thick +CORRECTION Data corrected for average resonance self-protection + and in-sample scattering. ENDBIB 12 NOCOMMON 0 0 DATA 3 31 @@ -640,20 +641,20 @@ KEV KEV MB 1900. 2000. 63. ENDDATA 33 ENDSUBENT 50 -SUBENT 12755009 821130 +SUBENT 12755009 19821130 20050909 1336 BIB 3 12 REACTION (72-HF-180(N,G)72-HF-181,,SIG,,AV) -SAMPLE HF(O)2 POWDER WITH A 10 PERCENT SULFUR BINDER. THE - ISOTOPIC PERCENT FRACTIONS ARE - 174-HF LESS THAN 0.05 - 176-HF 0.23 - 177-HF 1.0 - 178-HF 2.22 - 179-HF 2.66 - 180-HF 93.89 - THE SAMPLES ARE 2.6 X 2.6 CM X 0.15 CM THICK -CORRECTION DATA CORRECTED FOR AVERAGE RESONANCE SELF-PROTECTION - AND IN-SAMPLE SCATTERING. +SAMPLE Hf(O)2 powder with a 10 percent sulfur binder. The + isotopic percent fractions are + 174-Hf less than 0.05 + 176-Hf 0.23 + 177-Hf 1.0 + 178-Hf 2.22 + 179-Hf 2.66 + 180-Hf 93.89 + The samples are 2.6 x 2.6 cm x 0.15 cm thick +CORRECTION Data corrected for average resonance self-protection + and in-sample scattering. ENDBIB 12 NOCOMMON 0 0 DATA 3 30 @@ -691,7 +692,7 @@ KEV KEV MB 1800. 1900. 32. ENDDATA 32 ENDSUBENT 49 -SUBENT 12755010 821130 +SUBENT 12755010 19821130 20050909 1336 BIB 3 4 REACTION 1(72-HF-178(N,EL),,STF,,,DERIV) 2(72-HF-178(N,G),,STF,,,DERIV) @@ -706,12 +707,12 @@ ENDCOMMON 3 DATA 6 3 MOMENTUM L DATA 1DATA-ERR 1DATA 2DATA-ERR 2ASSUM NO-DIM NO-DIM NO-DIM NO-DIM NO-DIM NO-DIM - 0. 11.32 -04 0.36 -04 1.84 -04 - 1. 0.51 -04 0.03 -04 - 2. 1.66 -04 0.36 -04 + 0. 11.32E-04 0.36E-04 1.84E-04 + 1. 0.51E-04 0.03E-04 + 2. 1.66E-04 0.36E-04 ENDDATA 5 ENDSUBENT 18 -SUBENT 12755011 821130 +SUBENT 12755011 19821130 20050909 1336 BIB 2 3 REACTION 1(72-HF-179(N,EL),,STF,,,DERIV) 2(72-HF-179(N,G),,STF,,,DERIV) @@ -725,12 +726,12 @@ ENDCOMMON 3 DATA 5 3 MOMENTUM L DATA 1DATA-ERR 1DATA 2DATA-ERR 2 NO-DIM NO-DIM NO-DIM NO-DIM NO-DIM - 0. 1.84 -04 0.21 -04 150. -04 12. -04 - 1. 0.83 -04 0.10 -04 - 2. 2.10 -04 0.17 -04 + 0. 1.84E-04 0.21E-04 1.50E-02 1.2E-03 + 1. 0.83E-04 0.10E-04 + 2. 2.10E-04 0.17E-04 ENDDATA 5 ENDSUBENT 17 -SUBENT 12755012 821130 +SUBENT 12755012 19821130 20050909 1336 BIB 3 4 REACTION 1(72-HF-180(N,EL),,STF,,,DERIV) 2(72-HF-180(N,G),,STF,,,DERIV) @@ -745,9 +746,9 @@ ENDCOMMON 3 DATA 6 3 MOMENTUM L DATA 1DATA-ERR 1DATA 2DATA-ERR 2ASSUM NO-DIM NO-DIM NO-DIM NO-DIM NO-DIM NO-DIM - 0. 5.31 -04 0.32 -04 1.84 -04 - 1. 0.44 -04 0.05 -04 - 2. 1.08 -04 0.10 -04 + 0. 5.31E-04 0.32E-04 1.84E-04 + 1. 0.44E-04 0.05E-04 + 2. 1.08E-04 0.10E-04 ENDDATA 5 ENDSUBENT 18 ENDENTRY 12 diff --git a/exforall/127/12787.x4 b/exforall/127/12787.x4 index 6da0b286b..2095ee140 100644 --- a/exforall/127/12787.x4 +++ b/exforall/127/12787.x4 @@ -1,37 +1,38 @@ -ENTRY 12787 821101 -SUBENT 12787001 821101 -BIB 11 11 +ENTRY 12787 20050715 20050909 1336 +SUBENT 12787001 20050715 20050909 1336 +BIB 12 13 INSTITUTE (1USALRL) -REFERENCE (J,PR/C,26,696,8209) -AUTHOR (J.C.BROWNE,B.L.BERMAN) -TITLE NEUTRON-CAPTURE RESONANCES FOR 82-SE +REFERENCE (J,PR/C,26,969,1982) +AUTHOR (J.C.Browne,B.L.Berman) +TITLE Neutron-capture resonances for 82-Se FACILITY (LINAC) -METHOD (TOF) CAPTURE GAMMAS MEASURED. -DETECTOR (SCIN) C(6)O(6) SCINTILLATORS. +INC-SOURCE (EVAP) 100 MeV electrons on H(2)O cooled Ta. +METHOD (TOF) Capture gammas measured. +DETECTOR (SCIN) C(6)O(6) scintillators. MONITOR (5-B-10(N,A)3-LI-7,,SIG) -ERR-ANALYS (DATA-ERR) STATISTICAL UNCERTAINTIES -STATUS (APRVD) APPROVED BY J.C.BROWNE, 82/11/23. -HISTORY (821021C) -ENDBIB 11 +ERR-ANALYS (DATA-ERR) statistical uncertainties +STATUS (APRVD) Approved by J.C.Browne, 82/11/23. +HISTORY (19821021C) + (20050715C) DR Format updated and reference corrected +ENDBIB 13 NOCOMMON 0 0 -ENDSUBENT 14 -SUBENT 12787002 821101 -BIB 3 14 +ENDSUBENT 16 +SUBENT 12787002 19821101 20050909 1336 +BIB 3 13 REACTION (34-SE-0(N,0),,EN) -SAMPLE 2 GR. POWDERED METAL NATURAL SELENIUM - ISOTOPE ATOM PERCENT - 74-SE 0.9 - 76-SE 9.0 - 77-SE 7.6 - 78-SE 23.5 - 80-SE 49.8 - 82-SE 9.2 -FLAG (1.) NOT POSSIBLE TO ASSIGN TO 82-SE - (2.) WEAK - (3.) DOUBLET (DEFINITE,PROBABLE,POSSIBLE) - (4.) TRIPLET - (5.) COMPLEX -ENDBIB 14 +SAMPLE 2 gr. powdered metal natural selenium + Isotope Atom percent + 74-Se 0.9 + 76-Se 9.0 + 77-Se 7.6 + 78-Se 23.5 + 80-Se 49.8 + 82-Se 9.2 +FLAG (2.) Weak + (3.) Doublet (definite,probable,possible) + (4.) Triplet + (5.) Complex +ENDBIB 13 COMMON 1 3 FLAG NO-DIM @@ -143,55 +144,55 @@ EV EV NO-DIM 9410. 30. 9590. 15. 9840. 30. - 10.34+03 0.04 +03 - 10.50+03 0.02 +03 - 10.92+03 0.02 +03 - 11.10+03 0.02 +03 - 11.32+03 0.02 +03 - 11.61+03 0.03 +03 - 11.80+03 0.03 +03 - 12.05+03 0.03 +03 - 12.37+03 0.03 +03 - 13.00+03 0.03 +03 - 14.2 +03 0.1 +03 3. - 14.75+03 0.05 +03 3. - 15.17+03 0.03 +03 - 15.6 +03 0.1 +03 - 16.9 +03 0.1 +03 3. - 17.7 +03 0.1 +03 - 17.9 +03 0.1 +03 - 18.2 +03 0.1 +03 - 18.6 +03 0.1 +03 - 20.5 +03 0.15 +03 - 21.7 +03 0.15 +03 - 22.6 +03 0.15 +03 - 23.5 +03 0.1 +03 - 23.8 +03 0.1 +03 - 24.3 +03 0.1 +03 - 24.9 +03 0.1 +03 - 25.5 +03 0.1 +03 - 25.9 +03 0.1 +03 - 26.3 +03 0.1 +03 - 26.8 +03 0.1 +03 - 29.1 +03 0.15 +03 3. - 30.8 +03 0.2 +03 - 39.2 +03 0.2 +03 + 10.34E+03 0.04E+03 + 10.50E+03 0.02E+03 + 10.92E+03 0.02E+03 + 11.10E+03 0.02E+03 + 11.32E+03 0.02E+03 + 11.61E+03 0.03E+03 + 11.80E+03 0.03E+03 + 12.05E+03 0.03E+03 + 12.37E+03 0.03E+03 + 13.00E+03 0.03E+03 + 14.20E+03 0.1E+03 3. + 14.75E+03 0.05E+03 3. + 15.17E+03 0.03E+03 + 15.6E+03 0.1E+03 + 16.9E+03 0.1E+03 3. + 17.7E+03 0.1E+03 + 17.9E+03 0.1E+03 + 18.2E+03 0.1E+03 + 18.6E+03 0.1E+03 + 20.5E+03 0.15E+03 + 21.7E+03 0.15E+03 + 22.6E+03 0.15E+03 + 23.5E+03 0.1E+03 + 23.8E+03 0.1E+03 + 24.3E+03 0.1E+03 + 24.9E+03 0.1E+03 + 25.5E+03 0.1E+03 + 25.9E+03 0.1E+03 + 26.3E+03 0.1E+03 + 26.8E+03 0.1E+03 + 29.1E+03 0.15E+03 3. + 30.8E+03 0.2E+03 + 39.2E+03 0.2E+03 ENDDATA 138 -ENDSUBENT 161 -SUBENT 12787003 821101 +ENDSUBENT 160 +SUBENT 12787003 19821101 20050909 1336 BIB 3 12 REACTION (34-SE-82(N,0),,EN) -SAMPLE 2 GR. POWDERED METAL ENRICHED SELENIUM - ISOTOPE ATOM PERCENT - 74-SE LT 0.1 - 76-SE 1.3 - 77-SE 0.96 - 78-SE 3.76 - 80-SE 6.17 - 82-SE 87.8 -FLAG (1.) WEAK, COMPLEX, MAY HAVE COMPONENTS NOT FROM 82-SE - (2.) WEAK - (3.) POSSIBLY COMPLEX +SAMPLE 2 gr. powdered metal enriched selenium + Isotope Atom percent + 74-Se LT 0.1 + 76-Se 1.3 + 77-Se 0.96 + 78-Se 3.76 + 80-Se 6.17 + 82-Se 87.8 +FLAG (1.) Weak, complex, may have components not from 82-Se + (2.) Weak + (3.) Possibly complex ENDBIB 12 NOCOMMON 0 0 DATA 3 7 diff --git a/exforall/128/12843.x4 b/exforall/128/12843.x4 index bc3110d99..5fe58228a 100644 --- a/exforall/128/12843.x4 +++ b/exforall/128/12843.x4 @@ -1,34 +1,36 @@ -ENTRY 12843 840322 -SUBENT 12843001 840322 -BIB 16 22 +ENTRY 12843 20050718 20050909 1336 +SUBENT 12843001 20050718 20050909 1336 +BIB 16 24 INSTITUTE (1CANALA) -REFERENCE (J,PR/C,28,1212,8210) -AUTHOR (S.T.LAM,L.L.YU,H.W.FIELDING,W.K.DAWSON,G.C.NEILSON) -TITLE NEUTRON INDUCED FISSION OF 232-TH NEAR THRESHOLD. +REFERENCE (J,PR/C,28,1212,1983) +AUTHOR (S.T.Lam,L.L.Yu,H.W.Fielding,W.K.Dawson,G.C.Neilson) +TITLE Neutron induced fission of 232-Th near threshold. FACILITY (VDG) -METHOD (TOF) TIME-OF-FLIGHT +METHOD (TOF) Time-of-flight INC-SOURCE (P-T) -MONITOR CF-252 SOURCE WAS USED FOR CALIBRATION. -DETECTOR (SOLST) ORTEC HEAVY-ION SURFACE BARRIER DETECTOR. -SAMPLE LARGE SPHERICAL 232TH -66 CM2 AND 490 MICROGMS/CM2. -ANALYSIS SEE REF-PHYS.REV. C22,2485,1980. - FRAGMENT MASSES WERE DEDUCED FROM FRAGMENT ENERGIES - AND FRAGMENT FLIGHT TIMES. -ERR-ANALYS (ERR-S) STATISTICAL UNCERTAINTIES. -CORRECTION THE PULSE-HEIGHT DEFECT OF THE HEAVY-ION DETECTOR - WAS CORRECTED BY THE METHOD DESCRIBED IN REF- - H.W.SCHMITT+,PHYS.REV.137B,837,1965. -COMMENT FISSION-FRAGMENT YIELD PEAK-TO-VALLEY RATIO AT 1.6, - 3.1 AND 5.2 MEV WERE 129+-35, 63+-11 AND 29+-3 - RESPECTIVELY. -STATUS (APRVD) S.T.LAM, 84/3/12. -HISTORY (840112C) -ENDBIB 22 +MONITOR Cf-252 source was used for calibration. +DETECTOR (SOLST) Ortec heavy-ion surface barrier detector. +SAMPLE Large spherical 232Th -66 cm2 and 490 microgms/cm2. +ANALYSIS See Ref-Phys.Rev. C22,2485,1980. + Fragment masses were deduced from fragment energies + and fragment flight times. +ERR-ANALYS (ERR-S) Statistical uncertainties. +CORRECTION The pulse-height defect of the heavy-ion detector + was corrected by the method described in Ref- + H.W.Schmitt+,Phys.Rev.137B,837,1965. +COMMENT Fission-fragment yield peak-to-valley ratio at 1.6, + 3.1 and 5.2 MeV were 129+-35, 63+-11 and 29+-3 + respectively. +STATUS (APRVD) S.T.Lam, 84/3/12. +HISTORY (19840112C) + (20050718C) DR Format updated and reference corrected + SF8 deleted (FIS) +ENDBIB 24 NOCOMMON 0 0 -ENDSUBENT 25 -SUBENT 12843002 840322 +ENDSUBENT 27 +SUBENT 12843002 19840322 20050909 1336 BIB 1 1 -REACTION (90-TH-232(N,F),,AP,LF,FIS) +REACTION (90-TH-232(N,F),,AP,LF) ENDBIB 1 NOCOMMON 0 0 DATA 5 3 @@ -39,9 +41,9 @@ MEV MEV MEV NO-DIM NO-DIM 5.2 0.25 0.25 89.0 0.2 ENDDATA 5 ENDSUBENT 11 -SUBENT 12843003 840322 +SUBENT 12843003 19840322 20050909 1336 BIB 1 1 -REACTION (90-TH-232(N,F),,AP,HF,FIS) +REACTION (90-TH-232(N,F),,AP,HF) ENDBIB 1 NOCOMMON 0 0 DATA 5 3 @@ -52,15 +54,15 @@ MEV MEV MEV NO-DIM NO-DIM 5.2 0.25 0.25 140.3 0.2 ENDDATA 5 ENDSUBENT 11 -SUBENT 12843004 840322 +SUBENT 12843004 19840322 20050909 1336 BIB 3 7 -REACTION (90-TH-232(N,F),,AKE,LF,FIS) -CORRECTION THE LIGHT AND HEAVY FRAGMENT MEAN KINETIC ENERGIES - WERE CORRECTED FOR LOSS IN THE TARGET. -COMMENT THE MEAN KINETIC ENEGIES FOR THE LIGHT FISSION - FRAGMENT GROUPS WERE DETERMINED FROM THE DATA BY - EXCLUDING THE EVENTS IN THE VALLEY REGION DUE TO - POOR STATISTICS. +REACTION (90-TH-232(N,F),,AKE,LF) +CORRECTION The light and heavy fragment mean kinetic energies + were corrected from loss in the target. +COMMENT The mean kinetic energies for the light fission + fragment group were determined from the data by + excluding the events in the valley region due to + poor statistics. ENDBIB 7 NOCOMMON 0 0 DATA 5 3 @@ -71,15 +73,15 @@ MEV MEV MEV MEV MEV 5.2 0.25 0.25 98.08 0.02 ENDDATA 5 ENDSUBENT 17 -SUBENT 12843005 840322 +SUBENT 12843005 19840322 20050909 1336 BIB 3 7 -REACTION (90-TH-232(N,F),,AKE,HF,FIS) -CORRECTION THE LIGHT AND HEAVY FRAGMENT MEAN KINETIC ENERGIES - WERE CORRECTED FOR LOSS IN THE TARGET. -COMMENT THE MEAN KINETIC ENEGIES FOR THE HEAVY FISSION - FRAGMENT GROUPS WERE DETERMINED FROM THE DATA BY - EXCLUDING THE EVENTS IN THE VALLEY REGION DUE TO - POOR STATISTICS. +REACTION (90-TH-232(N,F),,AKE,HF) +CORRECTION The light and heavy fragment mean kinetic energies + were corrected from loss in the target. +COMMENT The mean kinetic energies for the light fission + fragment group were determined from the data by + excluding the events in the valley region due to + poor statistics. ENDBIB 7 NOCOMMON 0 0 DATA 5 3 @@ -90,14 +92,14 @@ MEV MEV MEV MEV MEV 5.2 0.25 0.25 65.40 0.10 ENDDATA 5 ENDSUBENT 17 -SUBENT 12843006 840322 +SUBENT 12843006 19840322 20050909 1336 BIB 2 6 -REACTION (90-TH-232(N,F),,AKE,FF,FIS) -ERR-ANALYS STATISTICAL UNCERTAINTY FOR KINETIC ENERGY= 100KEV. - SYSTEMATIC UNCERTAINTY FOR KINETIC ENERGY = 1 MEV. - THIS MAIN SOURCE OF ERROR IN THE ENERGY DETERMINATION - WAS DUE TO THE CORRECTION OF PULSE-HEIGHT DEFECT OF - THE HEAVY-ION DETECTOR. +REACTION (90-TH-232(N,F),,AKE,FF) +ERR-ANALYS Statistical uncertainty for kinetic energy= 100KeV. + Systematic uncertainty for kinetic energy = 1 MEV. + This main source of error in the energy determination + was due to the correction of pulse-height defect of + the heavy-ion detector. ENDBIB 6 NOCOMMON 0 0 DATA 5 3 @@ -108,18 +110,18 @@ MEV MEV MEV MEV MEV 5.2 0.25 0.25 163.48 0.10 ENDDATA 5 ENDSUBENT 16 -SUBENT 12843007 840322 +SUBENT 12843007 19840322 20050909 1336 BIB 3 10 -REACTION (90-TH-232(N,F),PRE,AKE,FF,FIS) -ERR-ANALYS STATISTICAL UNCERTAINTY FOR KINETIC ENERGY= 100KEV. - SYSTEMATIC UNCERTAINTY FOR KINETIC ENERGY = 1 MEV. - THIS MAIN SOURCE OF ERROR IN THE ENERGY DETERMINATION - WAS DUE TO THE CORRECTION OF PULSE-HEIGHT DEFECT OF - THE HEAVY-ION DETECTOR. +REACTION (90-TH-232(N,F),PRE,AKE,FF) +ERR-ANALYS Statistical uncertainty for kinetic energy= 100KeV. + Systematic uncertainty for kinetic energy = 1 MEV. + This main source of error in the energy determination + was due to the correction of pulse-height defect of + the heavy-ion detector. ASSUMED (ASSUM,90-TH-232(N,F),,NU) - IN CALCULATING THE PRIMARY(OR PRE-) NEUTRON AVERAGE - TOTAL KINETIC ENERGIES THE AVERAGE NUMBER OF NEUTRONS - PER FISSION WERE ASSUMED TO BE 2.35. + In calculating the primary(or pre-) neutron average + total kinetic energies the average number of neutrons + per fission were assumed to be 2.35. ENDBIB 10 COMMON 1 3 ASSUM @@ -134,10 +136,10 @@ MEV MEV MEV MEV MEV 5.2 0.25 0.25 165.30 0.10 ENDDATA 5 ENDSUBENT 24 -SUBENT 12843008 840322 +SUBENT 12843008 19840322 20050909 1336 BIB 2 2 -REACTION (90-TH-232(N,F)MASS,CHN,FY,,FIS) -STATUS DATA OBTAINED FROM THE AUTHOR ON TAPE NOV. 15,83. +REACTION (90-TH-232(N,F)MASS,CHN,FY) +STATUS Data obtained from the author on tape Nov. 15,83. ENDBIB 2 NOCOMMON 0 0 DATA 5 156 diff --git a/exforall/129/12922.x4 b/exforall/129/12922.x4 index 66b7cf866..368ba2fdf 100644 --- a/exforall/129/12922.x4 +++ b/exforall/129/12922.x4 @@ -1,41 +1,43 @@ -ENTRY 12922 860324 -SUBENT 12922001 860324 -BIB 12 18 +ENTRY 12922 19860324 20050909 1336 +SUBENT 12922001 19860324 20050909 1336 +BIB 12 20 INSTITUTE (1USAORL) -REFERENCE (J,PR/C,31,2041,8506) -AUTHOR (B.FOGELBERG,J.A.HARVEY,M.MIZUMOTO,S.RAMAN) -TITLE TEST OF FERMI GAS MODEL PREDICTIONS OF LEVEL - DENSITY IN 137XE. +REFERENCE (J,PR/C,31,2041,1985) +AUTHOR (B.Fogelberg,J.A.Harvey,M.Mizumoto,S.Raman) +TITLE Test of fermi gas model predictions of level + Density in 137Xe. FACILITY (LINAC) ORELA +METHOD (TOF) 80-M Flight path. INC-SOURCE (EVAP) -SAMPLE SAMPLE WITH XE-136 93.6 PERCENT - XE-134 5.7 PERCENT - XE-132 0.6 PERCENT - XE-131 0.1 PERCENT -METHOD (TOF) 80-M FLIGHT PATH. -DETECTOR (GLASD) LI-6 GLASS DETECTOR FOR LOW ENERGY REGION. - (SCIN) LIQUID SCINTILLATOR ABOVE 15 KEV. -ERR-ANALYS NO DETAILS AVAILABLE. -STATUS NO REPLY TO AUTHOR PROOF. -HISTORY (850607C) - (860324A) REFERENCE, BIB UPDATE. -ENDBIB 18 +SAMPLE Sample with Xe-136 93.6 percent + Xe-134 5.7 percent + Xe-132 0.6 percent + Xe-131 0.1 percent +DETECTOR (GLASD) Li-6 glass detector for low energy region. + (SCIN) Liquid scintillator above 15 KeV. +ERR-ANALYS No Details available. +STATUS No reply to author proof. +HISTORY (19850607C) + (19860324A) Reference, bib update. + (20050608C) DR Format updated and reaction 2 in + subsection 2 corrected +ENDBIB 20 COMMON 1 3 EN-RSL PER-CENT 0.1 ENDCOMMON 3 -ENDSUBENT 25 -SUBENT 12922002 860923 +ENDSUBENT 27 +SUBENT 12922002 19860923 20050909 1336 BIB 3 8 REACTION 1(54-XE-136(N,0),,EN) - 2(54-XE-136(N,EL),,WID/RED) + 2(54-XE-136(N,EL),,WID,,G) 3(54-XE-136(N,0),,L) 4(54-XE-136(N,0),,J) -FLAG (1.) SPIN ASSIGNMENT UNCERTAIN - (2.) MOMENTUM 1 0R 2. -HISTORY (860324A) DATA REPLACED. - (860923A) FIELD HEADING CORRECTED. +FLAG (1.) Spin assignment uncertain + (2.) Momentum 1 or 2. +HISTORY (19860324A) Data replaced. + (19860923A) Field heading corrected. ENDBIB 8 COMMON 1 3 DATA-ERR 1 diff --git a/exforall/129/12983.x4 b/exforall/129/12983.x4 index dc000617b..f97209aeb 100644 --- a/exforall/129/12983.x4 +++ b/exforall/129/12983.x4 @@ -1,31 +1,32 @@ -ENTRY 12983 861201 -SUBENT 12983001 861201 -BIB 13 14 +ENTRY 12983 20050718 20050909 1336 +SUBENT 12983001 20050718 20050909 1336 +BIB 13 15 INSTITUTE (1CANMCM) -REFERENCE (J,NIM,248,416,8608) -AUTHOR (C.M.CONNEELY,W.V.PRESTWICH,T.J.KENNETT) -TITLE THE THERMAL NEUTRON CAPTURE CROSS SECTION OF 9BE +REFERENCE (J,NIM/A,248,416,1986) +AUTHOR (C.M.Conneely,W.V.Prestwich,T.J.Kennett) +TITLE The thermal neutron capture cross section of 9Be METHOD (ACTIV) -DETECTOR PAIR SPECTROMETER, GE DETECTOR, NAI(TL) ANNULUS -FACILITY (REAC) MCMASTER UNIVERSITY REACTOR +DETECTOR Pair spectrometer, Ge detector, NaI(Tl) annulus +FACILITY (REAC) McMaster university reactor INC-SOURCE (REAC) MONITOR (7-N-14(N,G)7-N-15,,SIG) -SAMPLE BE-O, 99 PERCENT PURE -ERR-ANALYS ERROR INCLUDES STATISTICAL UNCERTAINTIES FROM SPECTRAL - ANALYSIS, YIELDS AND EFFICIENCY MODEL -STATUS (APRVD) W.V.PRESTWICH, 87/1/28. -HISTORY (861121C) -ENDBIB 14 +SAMPLE Be-O, 99 percent pure +ERR-ANALYS Error includes statistical uncertainties from spectral + analysis, yields and efficiency model +STATUS (APRVD) W.V.Prestwich, 87/1/28. +HISTORY (19861121C) + (20050718C) DR Format updated and reference corrected +ENDBIB 15 COMMON 3 3 EN MONIT MONIT-ERR EV MB MB 0.0253 77.2 2.1 ENDCOMMON 3 -ENDSUBENT 21 -SUBENT 12983002 861201 +ENDSUBENT 22 +SUBENT 12983002 19861201 20050909 1336 BIB 2 2 REACTION (4-BE-9(N,G)4-BE-10,,SIG) -ANALYSIS AVERAGE OF 3 MEASUREMENTS +ANALYSIS Average of 3 measurements ENDBIB 2 NOCOMMON 0 0 DATA 2 1 diff --git a/exforall/130/13022.x4 b/exforall/130/13022.x4 index 75481d40e..bd4c72adf 100644 --- a/exforall/130/13022.x4 +++ b/exforall/130/13022.x4 @@ -1,28 +1,29 @@ -ENTRY 13022 890207 -SUBENT 13022001 890207 -BIB 9 11 +ENTRY 13022 20050719 20050909 1336 +SUBENT 13022001 20050719 20050909 1336 +BIB 9 12 INSTITUTE (1USABRN) -REFERENCE (J,NP/A,9,273,59) -AUTHOR (H.P.EUBANK,R.A.PECK JR,F.L.HASSLER) -TITLE PROTON DISTRIBUTIONS FROM S32(N,P)P32 +REFERENCE (J,NP,9,273,1959) +AUTHOR (H.P.Eubank,R.A.Peck Jr,F.L.Hassler) +TITLE Proton distributions from S32(n,p)P32 FACILITY (CCW) INC-SOURCE (D-T) DETECTOR (PROPC) -STATUS DATA TAKEN FROM ARTICLE. - ANGULAR DISTRIBUTION DATA NOT AVAILABLE. GRAPHS IN - ARTICLE. -HISTORY (890127C) -ENDBIB 11 +STATUS Data taken from article. + Angular distribution data not available. Graphs in + article. +HISTORY (19890127C) + (20050719C) DR Format updated and reference corrected +ENDBIB 12 COMMON 1 3 EN MEV 14.1 ENDCOMMON 3 -ENDSUBENT 18 -SUBENT 13022002 890207 +ENDSUBENT 19 +SUBENT 13022002 19890207 20050909 1336 BIB 2 2 REACTION (16-S-32(N,X)1-H-1,PAR,SIG) -ANALYSIS (INTAD) ASSUMING NO APPRECIABLE YIELD PAST 90 DEG +ANALYSIS (INTAD) Assuming no appreciable yield past 90 Deg ENDBIB 2 NOCOMMON 0 0 DATA 3 1 diff --git a/exforall/131/13105.x4 b/exforall/131/13105.x4 index 1e321d513..6fbcc62b7 100644 --- a/exforall/131/13105.x4 +++ b/exforall/131/13105.x4 @@ -1,27 +1,28 @@ -ENTRY 13105 870505 -SUBENT 13105001 870505 -BIB 14 17 +ENTRY 13105 20050718 20050909 1336 +SUBENT 13105001 20050718 20050909 1336 +BIB 14 18 INSTITUTE (1USATNL) -REFERENCE (J,JP/G,11,379,8305) -AUTHOR (W.TORNOW,R.L.WALTER,R.C.BYRD) -TITLE PHASE-SHIFT-ANALYSIS APPROACH TO ELASTIC NEUTRON - SCATTERING FROM 12C BETWEEN 9 AND 12 MEV -INC-SOURCE (D-D) MONOENERGETIC SPECTRUM +REFERENCE (J,JP/G,11,379,1985) +AUTHOR (W.Tornow,R.L.Walter,R.C.Byrd) +TITLE Phase-shift-analysis approach to elastic neutron + scattering from 12C between 9 and 12 MeV +INC-SOURCE (D-D) Monoenergetic spectrum FACILITY (VDGT) METHOD (TOF) -DETECTOR (STANK) NE 213 AND NE 218 -SAMPLE GRAPHITE SAMPLE, 2.9 CM DIAMETER BY 3.8 CM HIGH -MONITOR ZERO-DEGREE NEUTRON MONITOR AND INTEGRATED CHARGE IN - GAS CELL -ERR-ANALYS OVERALL UNCERTAINTY NOT INCLUDING 3 PERCENT SCALE - UNCERTAINTY -CORRECTION MULTIPLE SCATTERING AND FINITE GEOMETRY CORRECTIONS -STATUS (APRVD) W.TORNOW, 87/5/4. -HISTORY (870227C) -ENDBIB 17 +DETECTOR (STANK) Ne 213 and Ne 218 +SAMPLE Graphite sample, 2.9 cm diameter by 3.8 cm high +MONITOR Zero-degree neutron monitor and integrated charge in + gas cell +ERR-ANALYS Overall uncertainty not including 3 percent scale + uncertainty +CORRECTION Multiple scattering anf finite geometry corrections +STATUS (APRVD) W.Tornow, 87/5/4. +HISTORY (19870227C) + (20050718C) DR Format updated and reference corrected +ENDBIB 18 NOCOMMON 0 0 -ENDSUBENT 20 -SUBENT 13105002 870505 +ENDSUBENT 21 +SUBENT 13105002 19870505 20050909 1336 BIB 1 1 REACTION (6-C-12(N,EL)6-C-12,,POL/DA,,ANA) ENDBIB 1 @@ -33,60 +34,60 @@ ENDCOMMON 3 DATA 4 54 EN ANG-CM DATA DATA-ERR MEV ADEG NO-DIM NO-DIM - 9.20 43.12 -0.547 0.053 - 9.20 63.69 -0.560 0.107 - 9.20 85.09 0.852 0.078 - 9.20 104.76 0.378 0.061 - 9.20 133.46 -0.387 0.057 - 9.20 152.13 -0.226 0.086 - 9.35 43.10 -0.475 0.054 - 9.35 63.69 -0.547 0.108 - 9.35 85.09 0.892 0.082 - 9.35 104.76 0.628 0.088 - 9.35 133.50 -0.317 0.059 - 9.35 152.13 -0.609 0.093 - 9.50 43.10 -0.447 0.049 - 9.50 63.69 -0.720 0.066 - 9.50 85.09 0.820 0.078 - 9.50 104.76 0.406 0.093 - 9.50 133.50 -0.326 0.064 - 9.50 152.13 -0.490 0.093 - 9.70 43.10 -0.444 0.023 - 9.70 63.69 -0.681 0.072 - 9.70 85.09 0.445 0.048 - 9.70 104.76 0.066 0.037 - 9.70 133.50 -0.404 0.075 - 9.70 152.13 -0.372 0.054 - 10.22 43.10 -0.532 0.023 - 10.22 63.69 -0.872 0.058 - 10.22 85.09 0.363 0.053 - 10.22 104.76 0.074 0.036 - 10.22 133.50 0.296 0.070 - 10.22 152.13 0.394 0.050 - 10.50 43.10 -0.557 0.025 - 10.50 63.69 -0.903 0.056 - 10.50 85.09 0.404 0.059 - 10.50 104.76 0.109 0.038 - 10.50 133.50 0.109 0.063 - 10.50 152.13 0.520 0.058 - 10.69 43.10 -0.508 0.033 - 10.69 63.69 -0.945 0.064 - 10.69 85.09 0.413 0.064 - 10.69 104.76 0.040 0.042 - 10.69 133.50 0.127 0.065 - 10.69 152.13 0.592 0.058 - 11.20 85.09 0.119 0.057 + 9.20 43.12 -0.547 0.053 + 9.20 63.69 -0.560 0.107 + 9.20 85.09 0.852 0.078 + 9.20 104.76 0.378 0.061 + 9.20 133.46 -0.387 0.057 + 9.20 152.13 -0.226 0.086 + 9.35 43.10 -0.475 0.054 + 9.35 63.69 -0.547 0.108 + 9.35 85.09 0.892 0.082 + 9.35 104.76 0.628 0.088 + 9.35 133.50 -0.317 0.059 + 9.35 152.13 -0.609 0.093 + 9.50 43.10 -0.447 0.049 + 9.50 63.69 -0.720 0.066 + 9.50 85.09 0.820 0.078 + 9.50 104.76 0.406 0.093 + 9.50 133.50 -0.326 0.064 + 9.50 152.13 -0.490 0.093 + 9.70 43.10 -0.444 0.023 + 9.70 63.69 -0.681 0.072 + 9.70 85.09 0.445 0.048 + 9.70 104.76 0.066 0.037 + 9.70 133.50 -0.404 0.075 + 9.70 152.13 -0.372 0.054 + 10.22 43.10 -0.532 0.023 + 10.22 63.69 -0.872 0.058 + 10.22 85.09 0.363 0.053 + 10.22 104.76 0.074 0.036 + 10.22 133.50 0.296 0.070 + 10.22 152.13 0.394 0.050 + 10.50 43.10 -0.557 0.025 + 10.50 63.69 -0.903 0.056 + 10.50 85.09 0.404 0.059 + 10.50 104.76 0.109 0.038 + 10.50 133.50 0.109 0.063 + 10.50 152.13 0.520 0.058 + 10.69 43.10 -0.508 0.033 + 10.69 63.69 -0.945 0.064 + 10.69 85.09 0.413 0.064 + 10.69 104.76 0.040 0.042 + 10.69 133.50 0.127 0.065 + 10.69 152.13 0.592 0.058 + 11.20 85.09 0.119 0.057 11.20 104.76 -0.237 0.048 11.20 133.50 -0.101 0.053 - 11.20 152.13 0.463 0.061 - 11.50 85.09 0.086 0.053 + 11.20 152.13 0.463 0.061 + 11.50 85.09 0.086 0.053 11.50 104.76 -0.264 0.042 11.50 133.50 -0.027 0.058 - 11.50 152.13 0.781 0.053 - 11.74 85.09 0.270 0.048 + 11.50 152.13 0.781 0.053 + 11.74 85.09 0.270 0.048 11.74 104.76 -0.208 0.041 - 11.74 133.50 0.002 0.037 - 11.74 152.13 0.815 0.057 + 11.74 133.50 0.002 0.037 + 11.74 152.13 0.815 0.057 ENDDATA 56 ENDSUBENT 66 ENDENTRY 2 diff --git a/exforall/133/13336.x4 b/exforall/133/13336.x4 index f4674d313..d905c10ec 100644 --- a/exforall/133/13336.x4 +++ b/exforall/133/13336.x4 @@ -1,44 +1,46 @@ -ENTRY 13336 900522 -SUBENT 13336001 900522 -BIB 14 27 +ENTRY 13336 20050719 20050909 1336 +SUBENT 13336001 20050719 20050909 1336 +BIB 14 28 INSTITUTE (1USAARK) -REFERENCE (J,JIN,37,2243,76) -AUTHOR (J.T.HARVEY,D.E.ADAMS,W.D.JAMES,J.N.BECK,J.L.MEASON, - P.K.KURODA) -TITLE DISTRIBUTION OF FISSION YIELDS IN THE 3.0 MEV NEUTRON- - INDUCED FISSION OF 238U +REFERENCE (J,JIN,37,2243,1975) +AUTHOR (J.T.Harvey,D.E.Adams,W.D.James,J.N.Beck,J.L.Meason, + P.K.Kuroda) +TITLE Distribution of fission yields in the 3.0 MeV neutron- + induced fission of 238U FACILITY (CCW) INC-SOURCE (D-D) -SAMPLE DEPLETED URANIUM, 99.989% 238U, 0.011% 235U +SAMPLE Depleted uranium, 99.989% 238U, 0.011% 235U METHOD (RCHEM) -DETECTOR (PROPC) OMNIGUARD LOW BACKGROUND BETA COUNTER +DETECTOR (PROPC) Omniguard low background beta counter MONITOR (92-U-238(N,F)56-BA-140,CUM,FY) - FROM FISSION-NEUTRON SPECTRUM VALUE OF 6.02+-0.12 OF - MEEK AND RIDER, NEDO-12154-1 (1974) -CORRECTION SHORT-LIVED SAMPLE DATA CORRECTED FOR SELF-ABSORPTION - AND SELF-SCATTERING - CORRECTED FOR LOSS OF YIELD DUE TO DECAY OF ISOMERS - IN SOME CASES CORRECTIONS APPLIED FOR: - - FRACTIONAL CHAIN YIELDS - - LACK OF SATURATION OF ACTIVITIES DUE TO CHANGE OF - FLUX DURING IRRADIATION - - GROWTH AND DECAY OF DAUGHTER ACTIVITIES -ERR-ANALYS (DATA-ERR) MOST PROBABLE ERRORS, ARISING MAINLY FROM - COUNTING STATISTICS AND DECAY CURVE RESOLUTION -STATUS (RIDER) REFERENCE 75HAR1 -HISTORY (891023C) VM - (900522U) BIB CORRECTIONS -ENDBIB 27 + From fission neutron spectrum value of 6.02+-0.12 of + Meek and Rider, NEDO-12154-1 (1974) +CORRECTION Short-lived sample data corrected for self-absorption + and self-scattering + Corrected for loss of yield due to decay of isomers + in some cases corrections applied for: + - Fractional chain yields + - Lack of saturation of activities due to change of + flux during irradiation + - Growth and decay of daughter activities +ERR-ANALYS (DATA-ERR) Most probable errors, arising mainly from + counting statistics and decay curve resolution +STATUS (RIDER) Reference 75HAR1 +HISTORY (19891023C) VM + (19900522U) BIB corrections + (20050719C) DR Format updated and reference corrected +ENDBIB 28 COMMON 4 3 EN EN-RSL MONIT MONIT-ERR MEV MEV PC/FIS PC/FIS 3.0 0.3 6.16 0.03 ENDCOMMON 3 -ENDSUBENT 34 -SUBENT 13336002 891027 -BIB 1 1 +ENDSUBENT 35 +SUBENT 13336002 19891027 20050909 1336 +BIB 2 2 REACTION (92-U-238(N,F)ELEM/MASS,CUM,FY) -ENDBIB 1 +ERR-ANALYS No information +ENDBIB 2 NOCOMMON 0 0 DATA 5 31 MASS ELEMENT ISOMER DATA DATA-ERR @@ -75,5 +77,5 @@ NO-DIM NO-DIM NO-DIM PC/FIS PC/FIS 149. 61. 1.83 0.22 151. 61. 0.69 0.08 ENDDATA 33 -ENDSUBENT 39 +ENDSUBENT 40 ENDENTRY 2 diff --git a/exforall/133/13359.x4 b/exforall/133/13359.x4 index af1fa6426..5e6e12445 100644 --- a/exforall/133/13359.x4 +++ b/exforall/133/13359.x4 @@ -1,104 +1,105 @@ -ENTRY 13359 891122 -SUBENT 13359001 891122 -BIB 10 13 -INSTITUTE (1USAUI ) -REFERENCE (J,NIM/B,147,487,7712) - (T,DIIORIO,77) PH.D THESIS, UNIV. OF ILLINOIS, URBANA -AUTHOR (G.DIIORIO,B.W.WEHRING) -TITLE DIRECT PHYSICAL MEASUREMENT OF MASS YIELDS FOR 235U +ENTRY 13359 20050719 20050909 1336 +SUBENT 13359001 20050719 20050909 1336 +BIB 10 14 +INSTITUTE (1USAUI) +REFERENCE (J,NIM,147,487,1977) + (T,Diiorio,1977) PH.D Thesis, Univ. of Illinois, Urbana +AUTHOR (G.Diiorio,B.W.Wehring) +TITLE Direct physical measurement of mass yields for 235U (N(TH),F) FACILITY (REAC) TRIGA -INC-SOURCE THRU NEUTRON BEAM PORT -SAMPLE FOIL ENRICED TO 93.4% 235U -METHOD (ASEP) HIAWATHA -STATUS (RIDER) REFERENCE 76DII1 - DATA TAKEN FROM THESIS -HISTORY (891121C) VM -ENDBIB 13 +INC-SOURCE Thru neutron beam port +SAMPLE Foil enriched to 93.4% 235U +METHOD (ASEP) Hiawatha +STATUS (RIDER) Reference 76DII1 + Data taken from thesis +HISTORY (19891121C) VM + (20050719C) DR Format updated and reference corrected +ENDBIB 14 COMMON 1 3 EN-DUMMY EV 0.0253 ENDCOMMON 3 -ENDSUBENT 20 -SUBENT 13359002 891122 +ENDSUBENT 21 +SUBENT 13359002 19891122 20050909 1336 BIB 4 7 REACTION (92-U-235(N,F)MASS,CHN,FY,,MXW) -MONITOR DATA FOR HEAVY MASS PEAK NORMALIZED TO MEEK AND RIDER, +MONITOR Data for heavy mass peak normalized to Meek and Rider, NEDO-12154-1 (1974) -CORRECTION ADJUSTED FOR DELAYED NEUTRONS FOR A = 84-98, 133-145 - CORRECTED FOR BACKGROUND, MISIDENTIFIED CHARGE STATES -ERR-ANALYS (DATA-ERR) STANDARD UNCERTAINTY BASED ON COUNTING - STATISTICS +CORRECTION Adjusted for delayed neutrons for A = 84-98, 133-145 + Corrected for background, misidentified charge states +ERR-ANALYS (DATA-ERR) Standard deviation based on counting + statistics ENDBIB 7 NOCOMMON 0 0 DATA 3 64 MASS DATA DATA-ERR NO-DIM PC/FIS PC/FIS - 77. 0.0082 .001 - 78. 0.0216 .002 - 79. 0.0439 .003 - 80. 0.130 .006 - 81. 0.190 .007 - 82. 0.321 .009 - 83. 0.560 .012 - 84. 1.03 .019 + 77. 0.0082 0.001 + 78. 0.0216 0.002 + 79. 0.0439 0.003 + 80. 0.130 0.006 + 81. 0.190 0.007 + 82. 0.321 0.009 + 83. 0.560 0.012 + 84. 1.03 0.019 85. 1.34 0.022 - 86. 1.99 .023 - 87. 2.60 .029 - 88. 3.63 .043 - 89. 4.84 .064 - 90. 5.88 .045 - 91. 6.01 .041 - 92. 6.01 .043 - 93. 6.34 .050 - 94. 6.43 .049 - 95. 6.61 .042 - 96. 6.35 .040 - 97. 6.01 .098 - 98. 5.60 .097 - 99. 6.04 .038 -100. 6.17 .038 -101. 5.14 .035 -102. 4.26 .032 -103. 2.94 .027 -104. 1.87 .021 -105. 0.957 .015 -106. 0.436 .010 -107. 0.139 .006 -108. 0.067 .004 -109. 0.038 .003 -110. 0.033 .003 -125. 0.0294 .005 -126. 0.0585 .007 -127. 0.1233 .009 -128. 0.3600 .011 -129. 0.8039 .016 -130. 1.8124 .023 -131. 2.925 .040 -132. 4.203 .048 -133. 6.555 .060 -134. 7.651 .064 -135. 6.557 .060 -136. 6.223 .067 + 86. 1.99 0.023 + 87. 2.60 0.029 + 88. 3.63 0.043 + 89. 4.84 0.064 + 90. 5.88 0.045 + 91. 6.01 0.041 + 92. 6.01 0.043 + 93. 6.34 0.050 + 94. 6.43 0.049 + 95. 6.61 0.042 + 96. 6.35 0.040 + 97. 6.01 0.098 + 98. 5.60 0.097 + 99. 6.04 0.038 +100. 6.17 0.038 +101. 5.14 0.035 +102. 4.26 0.032 +103. 2.94 0.027 +104. 1.87 0.021 +105. 0.957 0.015 +106. 0.436 0.010 +107. 0.139 0.006 +108. 0.067 0.004 +109. 0.038 0.003 +110. 0.033 0.003 +125. 0.0294 0.005 +126. 0.0585 0.007 +127. 0.1233 0.009 +128. 0.3600 0.011 +129. 0.8039 0.016 +130. 1.8124 0.023 +131. 2.925 0.040 +132. 4.203 0.048 +133. 6.555 0.060 +134. 7.651 0.064 +135. 6.557 0.060 +136. 6.223 0.067 137. 6.458 0.076 -138. 6.811 .077 -139. 6.321 .076 -140. 6.070 .063 -141. 6.019 .053 -142. 5.639 .051 -143. 6.087 .052 -144. 5.595 .049 +138. 6.811 0.077 +139. 6.321 0.076 +140. 6.070 0.063 +141. 6.019 0.053 +142. 5.639 0.051 +143. 6.087 0.052 +144. 5.595 0.049 145. 4.131 0.041 -146. 3.000 .035 -147. 2.295 .031 -148. 1.645 .026 -149. 0.967 .047 -150. 0.667 .018 -151. 0.417 .015 -152. 0.275 .013 -153. 0.105 .011 -154. 0.056 .009 +146. 3.000 0.035 +147. 2.295 0.031 +148. 1.645 0.026 +149. 0.967 0.047 +150. 0.667 0.018 +151. 0.417 0.015 +152. 0.275 0.013 +153. 0.105 0.011 +154. 0.056 0.009 ENDDATA 66 ENDSUBENT 78 ENDENTRY 2 diff --git a/exforall/134/13454.x4 b/exforall/134/13454.x4 index 58ab96d81..6bc1a6a6a 100644 --- a/exforall/134/13454.x4 +++ b/exforall/134/13454.x4 @@ -1,26 +1,27 @@ -ENTRY 13454 900122 -SUBENT 13454001 900122 -BIB 8 13 +ENTRY 13454 20050720 20050909 1336 +SUBENT 13454001 20050720 20050909 1336 +BIB 7 10 INSTITUTE (1USAANL) -REFERENCE (J,PR,5,1725,7205) -AUTHOR (K.F.FLYNN,E.P.HORWITZ,C.A.A.BLOOMQVIST,R.F.BARNES, - R.K.SJOBLOM,P.R.FIELDS,L.E.GLENDENIN) -TITLE DISTRIBUTION OF MASS IN THE SPONTANEOUS FISSION OF - 256FM. +REFERENCE (J,PR/C,5,1725,1972) +AUTHOR (K.F.Flynn,E.P.Horwitz,C.A.A.Bloomqvist,R.F.Barnes, + R.K.Sjoblom,P.R.Fields,L.E.Glendenin) +TITLE Distribution of mass in the spontaneous fission of + 256Fm. METHOD (RCHEM) -ERR-ANALYS (DATA-ERR) EVALUATED ON BASIS OF: - - NUMBER OF MEASUREMENTS - - STATISTICAL ERROR IN COUNT-RATE DETERMINATION - - UNCERTAINTIES IN DECAY SCHEME -STATUS DATA UPDATED AS PER ROCHESTER CONF., VOL.2, 19 (1973) -HISTORY (900119C) VM -ENDBIB 13 +STATUS Data updated as per Rochester conf., Vol.2, 19 (1973) +HISTORY (19900119C) VM + (20050720C) DR Format updated and reference corrected +ENDBIB 10 NOCOMMON 0 0 -ENDSUBENT 16 -SUBENT 13454002 900122 -BIB 1 1 +ENDSUBENT 13 +SUBENT 13454002 19900122 20050909 1336 +BIB 2 5 REACTION (100-FM-256(0,F)ELEM/MASS,CUM,FY) -ENDBIB 1 +ERR-ANALYS (DATA-ERR) Evaluated on basis of: + - Number of measurements + - Statistical error in count-rate determination + - Uncertainties in decay scheme +ENDBIB 5 NOCOMMON 0 0 DATA 5 27 MASS ELEMENT ISOMER DATA DATA-ERR @@ -53,5 +54,5 @@ NO-DIM NO-DIM NO-DIM PC/FIS PC/FIS 157. 63. 0.49 0.07 159. 64. 0.47 0.07 ENDDATA 29 -ENDSUBENT 35 +ENDSUBENT 39 ENDENTRY 2 diff --git a/exforall/135/13523.x4 b/exforall/135/13523.x4 index 8d443574e..abd1ae022 100644 --- a/exforall/135/13523.x4 +++ b/exforall/135/13523.x4 @@ -1,42 +1,43 @@ -ENTRY 13523 920423 -SUBENT 13523001 920423 -BIB 8 13 +ENTRY 13523 20050720 20050909 1336 +SUBENT 13523001 20050720 20050909 1336 +BIB 8 14 INSTITUTE (1USAANL) -REFERENCE (J,JP/G,18,629,8204) - (R,ANL-NDM-120,9107) -AUTHOR (A.B.SMITH,P.T.GUENTHER,J.F.WHALEN,S..CHIBA) -TITLE FAST-NEUTRON TOTAL AND SCATTERING CROSS SECTIONS OF - 58NI AND NUCLEAR MODELS -FACILITY (DYNAM) TANDEM DYNAMITRON -SAMPLE METALLIC NICKEL, ENRICHED TO MORE THAN 99 ATOM% 58NI. - SAMPLE CONTAINED A FRACTIONAL PERCENT OF CARBON, BUT, - OTHERWISE, APPEARED TO BE CHEMICALLY PURE. -STATUS (APRVD) A.B.SMITH, 91/11/19 -HISTORY (911101C) - (920423A) REFERENCE UPDATE -ENDBIB 13 +REFERENCE (J,JP/G,18,629,1992) + (R,ANL-NDM-120,1991) +AUTHOR (A.B.Smith,P.T.Guenther,J.F.Whalen,S.Chiba) +TITLE Fast-neutron total and scattering cross sections of + 58Ni and nuclear models +FACILITY (DYNAM) Tandem Dynamitron +SAMPLE Metallic nickel, enriched to more than 99 atom% 58Ni. + Sample contained a fractional percent of carbon, but, + otherwise, appeared to be chemecally pure. +STATUS (APRVD) A.B.Smith, 91/11/19 +HISTORY (19911101C) + (19920423A) Reference update + (20050720C) DR Format updated and reference corrected +ENDBIB 14 NOCOMMON 0 0 -ENDSUBENT 16 -SUBENT 13523002 920622 +ENDSUBENT 17 +SUBENT 13523002 19920622 20050909 1336 BIB 11 18 REACTION (28-NI-58(N,EL)28-NI-58,,DA) INC-SOURCE (D-D) -INC-SPECT MEAN ENERGY DETERMINED TO ABOUT 10 KEV. -METHOD (TOF). FLIGHT PATH ABOUT 5 M. -DETECTOR (SCIN) ORGANIC LIQUID SCINTILLATORS. -MONITOR (1-H-1(N,EL)1-H-1,,DA) POLYETHYLENE - RELATIVE ENERGY DEPENDENCE OF DETECTORS DETERMINED - RELATIVE TO NEUTRONS EMIITED BY 252CF SPONTANEOUS - FISSION. -CORRECTION CORRECTED FOR MULTIPLE-EVENT, ANGULAR-RESOLUTION, AND - BEAM-ATTENUATION EFFECTS -ERR-ANALYS (DATA-ERR) ESTIMATE OF TOTAL UNCERTAINTY. INCLUDES ALL - KNOWN STATISTICAL AND SYSTEMATIC UNCERTAINTIES, PLUS - A 0.5 MB/SR CONTRIBUTION FOR UNDENTIFIED UNCERTAINTY - SOURCES. -STATUS DATA RECEIVED BY EMAIL FROM A.B.SMITH, 91/10/31 -COMMENT MULTIPLE MEASUREMENTS AT SAME ANGLE -HISTORY (920622U) COMMENT ADDED +INC-SPECT Mean energy determined to about 10 KeV. +METHOD (TOF). Flight path about 5 m. +DETECTOR (SCIN) Organic liquid scintillators. +MONITOR (1-H-1(N,EL)1-H-1,,DA) Polyethylene + Relative energy dependence of detectors determined + Relative to neutrons emitted by 252Cf spontaneous + fission. +CORRECTION Corrected for multiple-event, angular-resolution, and + beam-attenuation effects +ERR-ANALYS (DATA-ERR) Estimate of total uncertainty. Includes all + known statistical and systematic uncertainties, plus + a 0.5 mb/sr contribution for undentified uncertainty + sources. +STATUS Data received by email from A.B.Smith, 91/10/31 +COMMENT Multiple measurements at same angle +HISTORY (19920622U) Comment added ENDBIB 18 COMMON 2 3 EN-ERR ANG-ERR @@ -997,24 +998,24 @@ MEV ADEG B/SR PER-CENT 9.990 0.1620E+03 0.1830E-01 0.8180E+01 ENDDATA 951 ENDSUBENT 978 -SUBENT 13523003 911112 +SUBENT 13523003 20050720 20050909 1336 BIB 9 16 REACTION (28-NI-58(N,INL)28-NI-58,PAR,DA) INC-SOURCE (D-D) -INC-SPECT MEAN ENERGY DETERMINED TO ABOUT 50 KEV. -METHOD (TOF). FLIGHT PATH 15.68 M. -DETECTOR (SCIN) ORGANIC LIQUID SCINTILLATORS. -MONITOR (1-H-1(N,EL)1-H-1,,DA) POLYETHYLENE - RELATIVE ENERGY DEPENDENCE OF DETECTORS DETERMINED - RELATIVE TO NEUTRONS EMIITED BY 252CF SPONTANEOUS - FISSION. -CORRECTION CORRECTED FOR MULTIPLE-EVENT, ANGULAR-RESOLUTION, AND - BEAM-ATTENUATION EFFECTS -ERR-ANALYS (DATA-ERR) ESTIMATE OF TOTAL UNCERTAINTY. INCLUDES ALL - KNOWN STATISTICAL AND SYSTEMATIC UNCERTAINTIES, PLUS - A 0.5 MB/SR CONTRIBUTION FOR UNDENTIFIED UNCERTAINTY - SOURCES. -STATUS DATA RECEIVED BY EMAIL FROM A.B.SMITH, 91/10/31 +INC-SPECT Mean energy determined to about 50 KeV. +METHOD (TOF). Flight path 15.68 m. +DETECTOR (SCIN) Organic liquid scintillators. +MONITOR (1-H-1(N,EL)1-H-1,,DA) Polyethylene + Relative energy dependence of detectors determined + relative to neutrons emitted by 252Cf spontaneous + fission. +CORRECTION Corrected for multiple-event, angular-resolution, and + beam-attenuation effects +ERR-ANALYS (DATA-ERR) Estimate of total uncertainty. Includes all + known statistical and systematic uncertainties, plus + a 0.5 mb/sr contribution for undentified uncertainty + sources. +STATUS Data received by email from A.B.Smith, 91/10/31 ENDBIB 16 COMMON 2 3 E-EXC EN-ERR @@ -1333,22 +1334,22 @@ MEV ADEG B/SR PER-CENT 9.999 0.1536E+03 0.3955E-02 0.2528E+02 ENDDATA 309 ENDSUBENT 334 -SUBENT 13523004 911112 +SUBENT 13523004 19911112 20050909 1336 BIB 9 14 REACTION (28-NI-58(N,TOT),,SIG,,AV) -INC-SOURCE WHITE NEUTRON SOURCE. THICK TARGETS OF LITHIUM AND - BERYLLIUM BOMBARDED BY 7.0 MEV DEUTERONS -INC-SPECT MEAN ENERGY DETERMINED TO ABOUT 50 KEV. -METHOD ROTATING-SAMPLE METHOD -DETECTOR (SCIN) PROTON RECIL SCINTILLATOR -ANALYSIS AVERAGED OVER INCIDENT ENERGY IN BINS OF: - 10 KEV UP TO 4 MEV; - 50 KEV FROM 4-6 MEV; - 100 KEV FROM 6-8 MEV; - 250 KEV FROM 8-10 MEV. -CORRECTION CORRECTED FOR DEADTIME. -ERR-ANALYS (DATA-ERR) STATISTICAL UNCERTAINTY -STATUS DATA RECEIVED FROM A.B.SMITH, 91/11/12 +INC-SOURCE White neutron source. Thick targets of lithium and + beryllium bombarbed by 7.0 MeV deuterons +INC-SPECT Mean energy determined to about 50 keV. +METHOD Rotating-sample method +DETECTOR (SCIN) Proton recil scintillator +ANALYSIS Averaged over incident energy in bins of: + 10 keV up to 4 MeV; + 50 keV from 4-6 MeV; + 100 keV from 6-8 MeV; + 250 keV from 8-10 MeV. +CORRECTION Corrected for deadtime. +ERR-ANALYS (DATA-ERR) Statistical uncertainty +STATUS Data received from A.B.Smith, 91/11/12 ENDBIB 14 NOCOMMON 0 0 DATA 3 71 diff --git a/exforall/135/13588.x4 b/exforall/135/13588.x4 index 2ed5fd043..e874839a7 100644 --- a/exforall/135/13588.x4 +++ b/exforall/135/13588.x4 @@ -1,11 +1,11 @@ -ENTRY 13588 20000215 20000306 -SUBENT 13588001 20000215 20000306 -BIB 11 15 +ENTRY 13588 20050720 20050909 1336 +SUBENT 13588001 20050720 20050909 1336 +BIB 11 16 INSTITUTE (1USAORL,1USALAS,3POLIPJ) -REFERENCE (J,PR/C,48/2,553,199308) -AUTHOR (M.C.MOXON,J.A.HARVEY,S.RAMAN,J.E.LYNN,W.RATYNSKI) -TITLE Neutron resonance parameters and thermal-neutron captur - by 43Ca +REFERENCE (J,PR/C,48,553,1993) +AUTHOR (M.C.Moxon,J.A.Harvey,S.Raman,J.E.Lynn,W.Ratynski) +TITLE Neutron resonance parameters and thermal-neutron + capture by 43Ca FACILITY (LINAC,1USAORL) ORELA INC-SOURCE (PHOTO) Photoneutrons from 19-ns wide elctron pulses and water-moderated Ta target @@ -15,16 +15,17 @@ CORRECTION Corrected for deadtime of the digitizer and for background. STATUS (APRVD) Approved by D. Wiarda, 14 February 2000. HISTORY (19931028C) - (20000210A) Converted to new date format, BIB uodate. -ENDBIB 15 + (20000210A) Converted to new date format, BIB update. + (20050720C) DR Reference corrected +ENDBIB 16 NOCOMMON 0 0 -ENDSUBENT 18 -SUBENT 13588002 20000214 20000306 +ENDSUBENT 19 +SUBENT 13588002 20000214 20050909 1336 BIB 4 7 REACTION 1(20-CA-43(N,0),,EN) 2(20-CA-43(N,0),,J) 3(20-CA-43(N,EL),,WID) -ANALYSIS Least-squares fit using REFIT to determine R-matrix +ANALYSIS Least-square fit using REFIT to determine R-matrix parameters ERR-ANALYS No information STATUS Data taken from article. diff --git a/exforall/136/13610.x4 b/exforall/136/13610.x4 index ac3e8494d..96a779069 100644 --- a/exforall/136/13610.x4 +++ b/exforall/136/13610.x4 @@ -1,13 +1,13 @@ -ENTRY 13610 960325 -SUBENT 13610001 960325 -BIB 12 25 +ENTRY 13610 20050720 20050909 1336 +SUBENT 13610001 20050720 20050909 1336 +BIB 12 26 INSTITUTE (1USALAS,1USATEX,1USATAM,1USAMTU,1USAANL,3CRORBZ, 1USAWSU) and U. of Central Arkansas. -REFERENCE (J,PR/C,48,256,9507) -AUTHOR (M.W.MC NAUGHTON,K.JOHNSTON,D.R.SWENSON,D.TUPA, - R.L.YORK,D.A.AMBROSE,P.COFFEY,K.H.MC NAUGHTON, - P.J.RILEY,G.GLASS,J.C.HIEBERT,R.H.JEPPESEN,H.SPINKA, - I.SUPEK,G.E.TRIPARD,H.WOOLVERTON) +REFERENCE (J,PR/C,48,256,1993) +AUTHOR (M.W.MC Naughton,K.Johnston,D.R.Swenson,D.Tupa, + R.L.York,D.A.Ambrose,P.Coffey,K.H.McNaughton, + P.J.Riley,G.Glass,J.C.Hiebert,R.H.Jeppesen,H.Spinka, + I.Supek,G.E.Tripard,H.Woolverton) TITLE np-elastic analyzing power A(N0) and spin transfer K(NN) FACILITY (MESON,1USALAS) LAMPF @@ -25,10 +25,11 @@ ERR-ANALYS (DATA-ERR1) Overall point-to-point uncertainty uncertainty in neutron-beam polarization. STATUS Data taken from tables in article. Not proofread by author. -HISTORY (960320C) -ENDBIB 25 +HISTORY (19960320C) + (20050720C) DR Format updated and reference corrected +ENDBIB 26 NOCOMMON 0 0 -ENDSUBENT 28 +ENDSUBENT 29 SUBENT 13610002 960325 BIB 2 2 REACTION (1-H-1(N,EL)1-H-1,,POL/DA,,ANA) @@ -130,16 +131,16 @@ MEV ADEG NO-DIM NO-DIM PER-CENT 788. 57.31 -0.209 0.005 2.0 ENDDATA 92 ENDSUBENT 99 -SUBENT 13610003 970423 +SUBENT 13610003 19970423 20050909 1336 BIB 4 4 REACTION (1-H-1(N,EL)1-H-1,NN,POL/DA,,K) METHOD Left-right asymmetry and analyzing power measured. STATUS (DEP,13610002) -HISTORY (970423A) REACTION corrected. +HISTORY (19970423A) REACTION corrected. ENDBIB 4 NOCOMMON 0 0 DATA 5 96 -EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 +EN ANG-CM DATA DATA-ERR1 DATA-ERR2 MEV ADEG NO-DIM NO-DIM PER-CENT 485. 160.45 0.316 0.049 2.0 485. 157.84 0.303 0.043 2.0 diff --git a/exforall/136/13647.x4 b/exforall/136/13647.x4 index 31f6896dc..78f04d5b1 100644 --- a/exforall/136/13647.x4 +++ b/exforall/136/13647.x4 @@ -1,9 +1,9 @@ -ENTRY 13647 970620 -SUBENT 13647001 970620 -BIB 13 22 +ENTRY 13647 20050720 20050909 1336 +SUBENT 13647001 20050720 20050909 1336 +BIB 13 23 INSTITUTE (1USAORL,1USADNS) -REFERENCE (J,PR/C,78,2704,9704) -AUTHOR (K.H.GUBER,R.R.SPENCER,P.E.KOEHLER,R.R.WINTERS) +REFERENCE (J,PRL,78,2704,1997) +AUTHOR (K.H.Guber,R.R.Spencer,P.E.Koehler,R.R.Winters) TITLE New 142,144Nd(n,gamma) Cross Sections and the s-process Origin of the Nd Anomalies in Presolar Meteoric Silicon Carbide Grains @@ -22,10 +22,11 @@ CORRECTION Corrected for background, sample impurities. ERR-ANALYS No information STATUS Data taken from article. No reply to author proof, 97/6/20. -HISTORY (970416C) -ENDBIB 22 +HISTORY (19970416C) + (20050720C) DR Format updated and reference corrected +ENDBIB 23 NOCOMMON 0 0 -ENDSUBENT 25 +ENDSUBENT 26 SUBENT 13647002 970620 BIB 2 2 REACTION (60-ND-142(N,G)60-ND-143,,SIG) @@ -59,11 +60,12 @@ KEV MB MB 50.0 29.6 3.0 ENDDATA 8 ENDSUBENT 15 -SUBENT 13647005 970620 -BIB 2 2 +SUBENT 13647005 19970620 20050909 1336 +BIB 3 3 REACTION (60-ND-144(N,G)60-ND-145,,SIG,,SPA,DERIV) INC-SPECT Calculated Maxwellian averages from measured data. -ENDBIB 2 +STATUS Dta taken from Table 1 +ENDBIB 3 NOCOMMON 0 0 DATA 3 6 KT DATA DATA-ERR @@ -75,5 +77,5 @@ KEV MB MB 30.0 73.2 6.1 50.0 60.1 6.0 ENDDATA 8 -ENDSUBENT 15 +ENDSUBENT 16 ENDENTRY 5 diff --git a/exforall/136/13665.x4 b/exforall/136/13665.x4 index c03a547f8..6b39661f4 100644 --- a/exforall/136/13665.x4 +++ b/exforall/136/13665.x4 @@ -1,10 +1,10 @@ -ENTRY 13665 971110 -SUBENT 13665001 971110 -BIB 11 13 +ENTRY 13665 20050721 20050909 1336 +SUBENT 13665001 20050721 20050909 1336 +BIB 10 13 INSTITUTE (1USABNL) -REFERENCE (J,PR,110,472,5806) -AUTHOR (J.D.FOX,R.L.ZIMMERMAN,D.J.HUGHES,H.PALEVSKY, - M.K.BRUSSEL,R.E.CHRIEN) +REFERENCE (J,PR,110,1472,1958) +AUTHOR (J.D.Fox,R.L.Zimmerman,D.J.Hughes,H.Palevsky, + M.K.Brussel,R.E.Chrien) TITLE Measurement of Spins of Levels Excited by Slow Neutron Capture FACILITY (CHOPF) @@ -12,18 +12,19 @@ SAMPLE Natural tungsten. METHOD (TOF,PHD) DETECTOR (NAICR) ERR-ANALYS No information. -STATUS Data taken from article. -HISTORY (971110C) +HISTORY (19971110C) + (20050721C) DR Format updated and reference corrected ENDBIB 13 NOCOMMON 0 0 ENDSUBENT 16 -SUBENT 13665002 971110 -BIB 2 4 +SUBENT 13665002 19971110 20050909 1336 +BIB 3 5 REACTION (74-W-183(N,0),,J) FLAG (1.) One, but not both of these resonances has spin 1. There is a slight preference for assigning 1 to the 48.1-eV resonance. -ENDBIB 4 +STATUS Data taken from article. +ENDBIB 5 NOCOMMON 0 0 DATA 3 4 EN-RES DATA FLAG @@ -33,5 +34,5 @@ EV NO-DIM NO-DIM 46.6 0. 1. 48.1 1. 1. ENDDATA 6 -ENDSUBENT 15 +ENDSUBENT 16 ENDENTRY 2 diff --git a/exforall/136/13671.x4 b/exforall/136/13671.x4 index 504a7a2bc..92a58404d 100644 --- a/exforall/136/13671.x4 +++ b/exforall/136/13671.x4 @@ -1,9 +1,9 @@ -ENTRY 13671 971106 -SUBENT 13671001 971106 -BIB 12 23 +ENTRY 13671 20050721 20050909 1336 +SUBENT 13671001 20050721 20050909 1336 +BIB 11 23 INSTITUTE (1USABNL) -REFERENCE (J,PR,180,1112,6904) -AUTHOR (J.A.MORAGUES,M.A.J.MARISCOTTI,W.GELLETLY,W.R.KANE) +REFERENCE (J,PR,180,1105,1969) +AUTHOR (J.A.Moragues,M.A.J.Mariscotti,W.Gelletly,W.R.Kane) TITLE 138Ba(n,gamma)139Ba reaction and evidence for direct capture FACILITY (REAC) Brookhaven graphite research reactor. @@ -22,8 +22,8 @@ MONITOR In low energy region, 411.795-keV gamma from 198Au and from 60Co and 1173.23-keV gamma of 15N from the 14N(n,gamma)15N reaction were used. ERR-ANALYS No information on source of uncertainties. -STATUS Data taken from article -HISTORY (970710C) YH +HISTORY (19970710C) YH + (20050721C) DR Format updated and reference corrected ENDBIB 23 COMMON 1 3 EN-DUMMY @@ -31,10 +31,11 @@ EV 0.0253 ENDCOMMON 3 ENDSUBENT 30 -SUBENT 13671002 971106 -BIB 1 1 +SUBENT 13671002 19971106 20050909 1336 +BIB 2 2 REACTION (56-BA-138(N,G)56-BA-139,,SPC,,SPA/REL) -ENDBIB 1 +STATUS Data taken from article +ENDBIB 2 NOCOMMON 0 0 DATA 5 17 E E-ERR DATA DATA-ERR DATA-MAX @@ -57,5 +58,5 @@ KEV KEV ARB-UNITS ARB-UNITS ARB-UNITS 3641.4 0.7 20. 3. 4096.1 0.7 60. 7. ENDDATA 19 -ENDSUBENT 25 +ENDSUBENT 26 ENDENTRY 2 diff --git a/exforall/136/13675.x4 b/exforall/136/13675.x4 index 1aa68f2dd..397217b82 100644 --- a/exforall/136/13675.x4 +++ b/exforall/136/13675.x4 @@ -1,9 +1,9 @@ -ENTRY 13675 970718 -SUBENT 13675001 970718 -BIB 10 11 +ENTRY 13675 20050721 20050909 1336 +SUBENT 13675001 20050721 20050909 1336 +BIB 10 12 INSTITUTE (1CANCRC) -REFERENCE (J,PR,89,1012,5301) -AUTHOR (G.A.BARTHOLOME,B.B.KINSEY) +REFERENCE (J,PR,89,386,1953) +AUTHOR (G.A.Bartholome,B.B.Kinsey) TITLE Neutron capture gamma-rays from scandium, vanadium, manganese, cobalt, and copper FACILITY (REAC) @@ -11,15 +11,16 @@ INC-SPECT Reactor spectrum DETECTOR Pair spectrometer ERR-ANALYS No information STATUS Data taken from article -HISTORY (970714C) YH -ENDBIB 11 +HISTORY (19970714C) YH + (20050721C) DR Format updated and reference corrected +ENDBIB 12 COMMON 2 3 EN-DUMMY E-NRM EV MEV 0.025 9.0 ENDCOMMON 3 -ENDSUBENT 18 -SUBENT 13675002 970718 +ENDSUBENT 19 +SUBENT 13675002 19970718 20050909 1336 BIB 4 5 REACTION (21-SC-45(N,G)21-SC-46,,SPC,,SPA) SAMPLE Four grams of scandium oxide @@ -34,7 +35,7 @@ B ENDCOMMON 3 DATA 3 8 E E-ERR DATA -MEV MEV GAM/100N +MEV MEV PC/INC 8.85 0.08 0.3 8.539 0.010 2.5 8.31 0.02 1. @@ -45,7 +46,7 @@ MEV MEV GAM/100N 6.35 0.01 2. ENDDATA 10 ENDSUBENT 24 -SUBENT 13675003 970718 +SUBENT 13675003 19970718 20050909 1336 BIB 4 6 REACTION (23-V-0(N,G),,SPC,,SPA) SAMPLE 300 grams of V2O5 powder enclosed in a Dural container @@ -61,26 +62,26 @@ B ENDCOMMON 3 DATA 3 16 E E-ERR DATA -MEV MEV GAM/100N +MEV MEV PC/INC 7.305 0.007 11. 7.154 0.008 18.5 6.686 0.008 14. -6.62 0.02 0.7 +6.62 0.02 0.7 6.508 0.006 25. -5.879 0.015 3. -5.744 0.008 9. +5.879 0.015 3. +5.744 0.008 9. 5.511 0.008 10. -5.21 0.01 6. -4.98 0.02 2. -4.85 0.02 2. -4.45 0.02 3. -4.15 0.03 4. -3.73 0.03 3. -3.59 0.02 3. -3.36 0.02 2. +5.21 0.01 6. +4.98 0.02 2. +4.85 0.02 2. +4.45 0.02 3. +4.15 0.03 4. +3.73 0.03 3. +3.59 0.02 3. +3.36 0.02 2. ENDDATA 18 ENDSUBENT 33 -SUBENT 13675004 970718 +SUBENT 13675004 19970718 20050909 1336 BIB 4 5 REACTION (25-MN-55(N,G)25-MN-56,,SPC,,SPA) SAMPLE Sample consist of 1400g of manganese dioxide @@ -95,28 +96,28 @@ B ENDCOMMON 3 DATA 3 18 E E-ERR DATA -MEV MEV GAM/100N +MEV MEV PC/INC 7.261 0.0006 12. -7.15 0.02 4. -7.048 0.008 6.5 -6.779 0.008 2.5 -6.43 0.01 0.5 -6.11 0.01 1. -5.91 0.02 0.5 -5.77 0.01 1. -5.63 0.02 0.3 -5.528 0.01 4. -5.21 0.01 3. -5.04 0.02 6. -4.81 0.01 2. -4.72 0.02 2. -4.55 0.01 2. -4.24 0.01 2. -4.10 0.03 1. -3.82 0.02 1. +7.15 0.02 4. +7.048 0.008 6.5 +6.779 0.008 2.5 +6.43 0.01 0.5 +6.11 0.01 1. +5.91 0.02 0.5 +5.77 0.01 1. +5.63 0.02 0.3 +5.528 0.01 4. +5.21 0.01 3. +5.04 0.02 6. +4.81 0.01 2. +4.72 0.02 2. +4.55 0.01 2. +4.24 0.01 2. +4.10 0.03 1. +3.82 0.02 1. ENDDATA 20 ENDSUBENT 34 -SUBENT 13675005 970718 +SUBENT 13675005 19970718 20050909 1336 BIB 4 6 REACTION (27-CO-59(N,G)27-CO-60,,SPC,,SPA) SAMPLE Sample consisted of 750 grams of very pure cobalt metal @@ -132,9 +133,9 @@ B ENDCOMMON 3 DATA 3 21 E E-ERR DATA -MEV MEV GAM/100N -7.486 0.006 3.0 -7.201 0.006 4.0 +MEV MEV PC/INC +7.486 0.006 3. +7.201 0.006 4. 7.041 0.01 1.3 6.974 0.01 2.5 6.867 0.006 7. @@ -156,7 +157,7 @@ MEV MEV GAM/100N 3.36 0.02 1. ENDDATA 23 ENDSUBENT 38 -SUBENT 13675006 970718 +SUBENT 13675006 19970718 20050909 1336 BIB 4 6 REACTION (29-CU-0(N,G),,SPC,,SPA) SAMPLE Cylindrical bar of very pure copper, 2300 grams, @@ -172,21 +173,21 @@ B ENDCOMMON 3 DATA 3 14 E E-ERR DATA -MEV MEV GAM/100N +MEV MEV PC/INC 7.914 0.006 20. -7.634 0.006 9. -7.296 0.009 5.5 -7.16 0.02 1. -7.01 0.02 2. -6.69 0.03 3. -6.41 0.02 1. -6.05 0.02 1. -5.75 0.03 0.2 -5.64 0.03 0.5 -5.43 0.02 1. -5.31 0.03 1. -5.18 0.02 0.6 -5.07 0.02 0.7 +7.634 0.006 9. +7.296 0.009 5.5 +7.16 0.02 1. +7.01 0.02 2. +6.69 0.03 3. +6.41 0.02 1. +6.05 0.02 1. +5.75 0.03 0.2 +5.64 0.03 0.5 +5.43 0.02 1. +5.31 0.03 1. +5.18 0.02 0.6 +5.07 0.02 0.7 ENDDATA 16 ENDSUBENT 31 ENDENTRY 6 diff --git a/exforall/136/13698.x4 b/exforall/136/13698.x4 index 098163f4d..b637f9d2e 100644 --- a/exforall/136/13698.x4 +++ b/exforall/136/13698.x4 @@ -1,11 +1,10 @@ -ENTRY 13698 20030107 20030306 -SUBENT 13698001 20030107 20030306 +ENTRY 13698 20050722 20050909 1336 +SUBENT 13698001 20050722 20050909 1336 BIB 13 46 INSTITUTE (1USABRK,1USAVBT,1USAORL,3RUMBUC,2GERFRK,4ZZZDUB, - 1USAUSA,1USAINL,1USALRL,3CPRBJG,1USAMHG,3BZLBZL) - USA - Mississippi State University + 1USAMSS,1USAINL,1USALRL,3CPRBJG,1USAMHG,3BZLUFR) Brazil - U. Fed. do Rio de Janeiro -REFERENCE (J,PR,57,2370,199805) +REFERENCE (J,PR/C,57,2370,1998) AUTHOR (A.V.Ramayya,J.H.Hamilton,J.K.Hwang,L.K.Peker, J.Kormicki,B.R.S.Babu,T.N.Ginter,A.Sandulescu, A.Florescu,F.Carstoiu,W.Greiner,G.M.Ter-Akopian, @@ -47,10 +46,11 @@ STATUS Data taken from table in reference. HISTORY (19980807C) (20010212A) Authors converted to lower case. (20030107A) BIB update. + (20050722C) DR Reference corrected ENDBIB 46 NOCOMMON 0 0 ENDSUBENT 49 -SUBENT 13698002 20030107 20030306 +SUBENT 13698002 20030107 20050909 1336 BIB 3 3 REACTION (98-CF-252(0,F)ELEM/MASS,TER,FY/CRL,LF/HF) ERR-ANALYS (DATA-ERR) No information on source of uncertainties. diff --git a/exforall/137/13738.x4 b/exforall/137/13738.x4 index f5a38c4c4..db4ec5286 100644 --- a/exforall/137/13738.x4 +++ b/exforall/137/13738.x4 @@ -1,10 +1,10 @@ -ENTRY 13738 20000327 20000619 -SUBENT 13738001 20000327 20000619 -BIB 11 17 -INSTITUTE (1USAORL,1USAKTY,1CANQU ) -REFERENCE (J,PR/C,34/2,429,198608) -AUTHOR (D.J.HOREN,C.H.JOHNSON,J.L.FOWLER,A.D.MACKELLAR, - B.CASTEL) +ENTRY 13738 20050722 20050909 1336 +SUBENT 13738001 20050722 20050909 1336 +BIB 11 18 +INSTITUTE (1USAORL,1USAKTY,1CANQU) +REFERENCE (J,PR/C,34,429,1986) +AUTHOR (D.J.Horen,C.H.Johnson,J.L.Fowler,A.D.Mackellar, + B.Castel) TITLE 208Pb+n reaction and the mean nuclear field near threshold FACILITY (LINAC) ORELA @@ -18,10 +18,11 @@ DETECTOR (SCIN) 7.62cm diam x 2 cm thick NE110 Plastic scintillator CORRECTION Corrected for dead-time and background. HISTORY (20000223C) TK -ENDBIB 17 + (20050722C) DR Format updated and reference corrected +ENDBIB 18 NOCOMMON 0 0 -ENDSUBENT 20 -SUBENT 13738002 20000327 20000619 +ENDSUBENT 21 +SUBENT 13738002 20000327 20050909 1336 BIB 4 8 REACTION 1(82-PB-208(N,0),,EN) 2(82-PB-208(N,0),,L) @@ -30,7 +31,7 @@ REACTION 1(82-PB-208(N,0),,EN) 5(82-PB-208(N,TOT),,WID/RED,,RMT) ERR-ANALYS (DATA-ERR) No information on source of uncertainties. FLAG (1.) Spin and momentum l values assumed. -STATUS Data obtained from publication. +STATUS Data taken from Table 1 ENDBIB 8 COMMON 1 3 DATA-ERR 1 diff --git a/exforall/137/13744.x4 b/exforall/137/13744.x4 index b5685e74c..02f47f959 100644 --- a/exforall/137/13744.x4 +++ b/exforall/137/13744.x4 @@ -1,6 +1,6 @@ -ENTRY 13744 20011226 -SUBENT 13744001 20011226 -BIB 8 12 +ENTRY 13744 20050707 20050909 1336 +SUBENT 13744001 20050707 20050909 1336 +BIB 8 14 INSTITUTE (1USAKAP,1USARPI) REFERENCE (J,NSE,134,50,2000) AUTHOR (G.Leinweber,J.Burke,C.R.Lubitz,H.D.Knox,N.J.Drindak, @@ -13,9 +13,11 @@ FACILITY (LINAC,1USARPI) INC-SOURCE (PHOTO) Electrons on water-cooled tantalum target. STATUS (APRVD) Approved by G. Leinweber, 21 December 2001. HISTORY (20011212C) -ENDBIB 12 + (20050707C) DR Subentries 13-15 corrected "TOT" is + changed by "EL" +ENDBIB 14 NOCOMMON 0 0 -ENDSUBENT 15 +ENDSUBENT 17 SUBENT 13744002 20011213 20020410 BIB 6 8 REACTION (40-ZR-0(N,TOT),,SIG,,RAW) Transmission @@ -43232,13 +43234,13 @@ EV NO-DIM NO-DIM .10014E+02 .000015 .000149 ENDDATA 2054 ENDSUBENT 2070 -SUBENT 13744013 20011213 20020410 +SUBENT 13744013 20011213 20050909 1336 BIB 5 11 REACTION 1(40-ZR-91(N,0),,EN) 2(40-ZR-91(N,0),,L) 3(40-ZR-91(N,0),,J) 4(40-ZR-91(N,G),,WID) - 5(40-ZR-91(N,TOT),,WID) + 5(40-ZR-91(N,EL ),,WID) ANALYSIS (MLA) Least-squares multilevel R-matrix code REFIT. CORRECTION Capture data corrected for self-shielding and multiple scattering. @@ -43264,13 +43266,13 @@ MILLI-EV MILLI-EV 6284. 107. ENDDATA 14 ENDSUBENT 30 -SUBENT 13744014 20040802 +SUBENT 13744014 20040802 20050909 1336 BIB 6 12 REACTION 1(40-ZR-94(N,0),,EN) 2(40-ZR-94(N,0),,L) 3(40-ZR-94(N,0),,J) 4(40-ZR-94(N,G),,WID) - 5(40-ZR-94(N,TOT),,WID) + 5(40-ZR-94(N,EL),,WID) ANALYSIS (MLA) Least-squares multilevel R-matrix code REFIT. CORRECTION Capture data corrected for self-shielding and multiple scattering. @@ -43289,13 +43291,13 @@ MILLI-EV 35. ENDDATA 6 ENDSUBENT 23 -SUBENT 13744015 20011213 20020410 +SUBENT 13744015 20011213 20050909 1336 BIB 5 11 REACTION 1(40-ZR-96(N,0),,EN) 2(40-ZR-96(N,0),,L) 3(40-ZR-96(N,0),,J) 4(40-ZR-96(N,G),,WID) - 5(40-ZR-96(N,TOT),,WID) + 5(40-ZR-96(N,EL),,WID) ANALYSIS (MLA) Least-squares multilevel R-matrix code REFIT. CORRECTION Capture data corrected for self-shielding and multiple scattering. diff --git a/exforall/137/13746.x4 b/exforall/137/13746.x4 index c9ef75616..51982fdec 100644 --- a/exforall/137/13746.x4 +++ b/exforall/137/13746.x4 @@ -1,8 +1,8 @@ -ENTRY 13746 20010907 20030306 -SUBENT 13746001 20010907 20030306 -BIB 12 35 +ENTRY 13746 20050722 20050909 1336 +SUBENT 13746001 20050722 20050909 1336 +BIB 13 48 INSTITUTE (1USAANL) -REFERENCE (J,PR/C,61,04761,200004) +REFERENCE (J,PR/C,61,047601,2000) AUTHOR (J.K.Hwang,A.V.Ramayya,J.H.Hamilton,C.J.Beyer, J.Kormicki,X.Q.Zhang,A.Rodin,A.Formichev,J.Kliman, L.Krupa,G.M.Ter Akopyan,Yu.Ts.Oganessian, G.Hubarian, @@ -33,16 +33,6 @@ CORRECTION Corrected for: . 6.2-MeV decay alpha particles from accidental contamination of surface of Au foil with the source material. -STATUS Data taken from Table I in reference. - No reply to author proof from J.K. Hwang -HISTORY (20010730C) IS -ENDBIB 35 -NOCOMMON 0 0 -ENDSUBENT 38 -SUBENT 13746002 20010730 20030306 -BIB 6 30 -REACTION ((98-CF-252(0,F)ELEM/MASS,TER,FY,LCP)/ - (98-CF-252(0,F)ELEM,TER,FY)) ANALYSIS Shape of energy spectrum of ternary alpha particles analyzed. Low energy tail was attributed to alpha particles originating from 5He emission. Contribution @@ -55,6 +45,17 @@ ANALYSIS Shape of energy spectrum of ternary alpha particles The small additional spread in momentum which is contribution of the breakup of 5He to distribution imparted by the fission is neglected in this approach. +STATUS Data taken from Table I in reference. + No reply to author proof from J.K. Hwang +HISTORY (20010730C) IS + (20050722C) DR Reference corrected +ENDBIB 48 +NOCOMMON 0 0 +ENDSUBENT 51 +SUBENT 13746002 20010730 20050909 1336 +BIB 5 18 +REACTION ((98-CF-252(0,F)ELEM/MASS,TER,FY,LCP)/ + (98-CF-252(0,F)ELEM,TER,FY)) ERR-ANALYS (+DATA-ERR) Absolute uncertainty given. (-DATA-ERR) Absolute uncertainty given. Uncertainties depend on low-energy cutoff of alpha @@ -71,7 +72,7 @@ CRITIQUE ** BY AUTHOR ** Application of method with 5He-particle disributions are independent of mass. REL-REF (D,,Cheifetz+,J,PRL,29,805,1972) HISTORY (20030107A) Reaction updated. -ENDBIB 30 +ENDBIB 18 COMMON 1 3 ELEMENT NO-DIM @@ -83,5 +84,5 @@ NO-DIM NO-DIM NO-DIM NO-DIM 4. 79.6 24.4 12.0 5. 20.4 2.9 21.9 ENDDATA 4 -ENDSUBENT 43 +ENDSUBENT 31 ENDENTRY 2 diff --git a/exforall/138/13811.x4 b/exforall/138/13811.x4 index eb1437994..1722bc876 100644 --- a/exforall/138/13811.x4 +++ b/exforall/138/13811.x4 @@ -1,8 +1,8 @@ -ENTRY 13811 20010629 20010913 -SUBENT 13811001 20010629 20010913 -BIB 16 39 +ENTRY 13811 20050722 20050909 1336 +SUBENT 13811001 20050722 20050909 1336 +BIB 16 40 INSTITUTE (1USAANL) -REFERENCE (J,NIM,56,325,1966) +REFERENCE (J,NIM,56,325,1967) AUTHOR (G.E.Thomas, D.E.Blatchley, L.M.Bollinger) TITLE High-Sensitivity Neutron-Capture Gamma-Ray Facility FACILITY (REAC) Reactor CP-5. @@ -40,13 +40,14 @@ ERR-ANALYS (DATA-ERR) Calculated by combining the statistical (E-ERR) Estimated systematic uncertainty STATUS Data taken from Tables 2, 3, 4, 5, 6 of reference HISTORY (20010626C) IS -ENDBIB 39 + (20050722C) DR Reference corrected +ENDBIB 40 COMMON 1 3 EN-DUMMY EV 0.0253 ENDCOMMON 3 -ENDSUBENT 46 +ENDSUBENT 47 SUBENT 13811002 20010629 20010913 BIB 2 2 REACTION (7-N-14(N,G)7-N-15,,SPC,,SPA) @@ -81,10 +82,10 @@ KEV KEV PC/REAC PC/REAC 1679. 2. 9.2 0.5 ENDDATA 25 ENDSUBENT 32 -SUBENT 13811003 20010629 20010913 +SUBENT 13811003 20010629 20050909 1336 BIB 2 2 REACTION (6-C-12(N,G)6-C-13,,SPC,,SPA) -SAMPLE Graphite +SAMPLE Natural Graphite ENDBIB 2 NOCOMMON 0 0 DATA 3 3 @@ -95,10 +96,10 @@ KEV PC/REAC PC/REAC 1262. 34. 2. ENDDATA 5 ENDSUBENT 12 -SUBENT 13811004 20010629 20010913 +SUBENT 13811004 20010629 20050909 1336 BIB 2 3 REACTION (6-C-13(N,G)6-C-14,,SPC,,SPA) -SAMPLE Normal graphite (1.1% 13C) and 1-g sample of 13C that +SAMPLE Natural graphite (1.1% 13C) and 1-g sample of 13C that is 94% isotopically pure. ENDBIB 3 NOCOMMON 0 0 diff --git a/exforall/138/13832.x4 b/exforall/138/13832.x4 index c3afea3b7..262cd1ec4 100644 --- a/exforall/138/13832.x4 +++ b/exforall/138/13832.x4 @@ -1,8 +1,8 @@ -ENTRY 13832 20020501 20020815 -SUBENT 13832001 20020501 20020815 -BIB 15 37 +ENTRY 13832 20050722 20050909 1336 +SUBENT 13832001 20050722 20050909 1336 +BIB 14 37 INSTITUTE (1USAANL) -REFERENCE (J,PR,129,1113,196302) +REFERENCE (J,PR,129,1691,1963) AUTHOR (R.K.Smither) TITLE Gamma-Ray Spectrum from Thermal-Neutron Capture in Hf177 and Associated Energy Levels in Hf178. @@ -36,8 +36,8 @@ ERR-ANALYS (E-ERR) Probable error in gamma-ray energies; reflects in line intensities; reflects both statistical and systematic errors. Lower limit 10%. ADD-RES Level scheme of Hf178. -STATUS Data taken from Table I of reference. HISTORY (20020409C) IS + (20050722C) DR Reference corrected ENDBIB 37 COMMON 1 3 EN-DUMMY @@ -45,10 +45,11 @@ EV 0.0253 ENDCOMMON 3 ENDSUBENT 44 -SUBENT 13832002 20020501 20020815 -BIB 1 1 +SUBENT 13832002 20020501 20050909 1336 +BIB 2 2 REACTION (72-HF-177(N,G)72-HF-178,,SPC,,SPA) -ENDBIB 1 +STATUS Data taken from Table I of reference. +ENDBIB 2 COMMON 1 3 DATA-ERR PER-CENT @@ -275,5 +276,5 @@ KEV KEV PC/REAC 53.90 0.01 0.012 52.74 0.01 0.018 ENDDATA 219 -ENDSUBENT 229 +ENDSUBENT 230 ENDENTRY 2 diff --git a/exforall/138/13839.x4 b/exforall/138/13839.x4 index cc16c787c..7b496b517 100644 --- a/exforall/138/13839.x4 +++ b/exforall/138/13839.x4 @@ -1,8 +1,8 @@ -ENTRY 13839 20030910 20031024 -SUBENT 13839001 20030910 20031024 -BIB 13 21 +ENTRY 13839 20050722 20050909 1336 +SUBENT 13839001 20050722 20050909 1336 +BIB 13 22 INSTITUTE (1USABNL,2FR ILL,1USAANL) -REFERENCE (J,NP/A,376,149,1986) +REFERENCE (J,NP/A,376,149,1982) AUTHOR (K.Schreckenbach,A.I.Namenson,W.F.Davidson,T.Von Egidy, H.G.Borner,J.A.Pinston,R.K.Smither.D.D.Warner, R.F.Casten,M.L.Stelts,D.H.White.W.Stoffl) @@ -22,10 +22,11 @@ CORRECTION Intensities corrected for detector efficiency. STATUS (COREL,22473001) Data taken at ILL. HISTORY (20020528C) IS + VM (20030910A) Status updated. -ENDBIB 21 + (20050722C) DR Reference corrected +ENDBIB 22 NOCOMMON 0 0 -ENDSUBENT 24 -SUBENT 13839002 20030106 20030306 +ENDSUBENT 25 +SUBENT 13839002 20030106 20050909 1336 BIB 3 4 REACTION (62-SM-154(N,G)62-SM-155,,SPC,,REL/SPA) ERR-ANALYS (E-EXC-ERR) Statistical uncertainties given. diff --git a/exforall/138/13855.x4 b/exforall/138/13855.x4 index 92cbaacd4..03c83b13e 100644 --- a/exforall/138/13855.x4 +++ b/exforall/138/13855.x4 @@ -1,8 +1,8 @@ -ENTRY 13855 20021202 20030219 -SUBENT 13855001 20021202 20030219 -BIB 10 12 +ENTRY 13855 20050722 20050909 1336 +SUBENT 13855001 20050722 20050909 1336 +BIB 9 12 INSTITUTE (1CANCRC) -REFERENCE (J,PR,82,380,195305) +REFERENCE (J,PR,82,380,1951) AUTHOR (B.B.Kinsey,G.A.Bartholomew,W.H.Walker) TITLE Neutron Capture gamma-rays from Lead and Bismuth FACILITY (REAC) @@ -11,8 +11,8 @@ DETECTOR (BPAIR) ERR-ANALYS Data subject to large error (possibly 20%) involved in the assumption that neutron flux in samples is the same for the same pile power. -STATUS (OUTDT) HISTORY (20021202C) + (20050722C) DR Reference corrected ENDBIB 12 COMMON 1 3 EN-DUMMY @@ -20,29 +20,31 @@ EV 0.0253 ENDCOMMON 3 ENDSUBENT 19 -SUBENT 13855002 20021202 20030219 -BIB 2 3 +SUBENT 13855002 20021202 20050909 1336 +BIB 3 4 REACTION (82-PB-207(N,G)82-PB-208,,SPC,,SPA) SAMPLE Two samples: 1) chemically pure metallic lead, 2) PbO in Dural conatainer. -ENDBIB 3 +STATUS (OUTDT) +ENDBIB 4 NOCOMMON 0 0 DATA 2 1 E DATA-APRX MEV PRT/REAC 7.380 1.3 ENDDATA 3 -ENDSUBENT 11 -SUBENT 13855003 20021202 20030219 -BIB 2 2 +ENDSUBENT 12 +SUBENT 13855003 20021202 20050909 1336 +BIB 3 3 REACTION (83-BI-209(N,G)83-BI-210,,SPC,,SPA) SAMPLE Natural bismuth sample. -ENDBIB 2 +STATUS (OUTDT) +ENDBIB 3 NOCOMMON 0 0 DATA 2 1 E DATA-APRX MEV PRT/REAC 4.170 1.6 ENDDATA 3 -ENDSUBENT 10 +ENDSUBENT 11 ENDENTRY 3 diff --git a/exforall/139/13909.x4 b/exforall/139/13909.x4 index b478ec79d..ce4628f11 100644 --- a/exforall/139/13909.x4 +++ b/exforall/139/13909.x4 @@ -1,8 +1,8 @@ -ENTRY 13909 20041026 -SUBENT 13909001 20041026 -BIB 7 10 +ENTRY 13909 20041026 20050909 1336 +SUBENT 13909001 20041026 20050909 1336 +BIB 7 11 INSTITUTE (1USAORL,1USADNS) -REFERENCE (J,PR/C,64,065802,200112) +REFERENCE (J,PR/C,64,065802,2001) AUTHOR (P.E.Koehler,J.A.Harvey,R.R.Winters,K.H.Guber, R.R.Spencer) TITLE High-resolution capture and transmission measurements @@ -11,9 +11,10 @@ TITLE High-resolution capture and transmission measurements FACILITY (LINAC,1USAORL) ORELA. STATUS No reply from P. Koehler to author proof. HISTORY (20040825C) -ENDBIB 10 + (20050627C) DR Subentry 5 corrected (J -> 2J) +ENDBIB 11 NOCOMMON 0 0 -ENDSUBENT 13 +ENDSUBENT 14 SUBENT 13909002 20040826 BIB 4 6 REACTION (50-SN-116(N,G)50-SN-117,,SIG) @@ -49,7 +50,7 @@ ENDBIB 4 NOCOMMON 0 0 NODATA 0 0 ENDSUBENT 8 -SUBENT 13909005 20040826 +SUBENT 13909005 20040826 20050909 1336 BIB 6 12 REACTION 1(50-SN-116(N,0),,EN) 2(50-SN-116(N,0),,J) @@ -70,441 +71,441 @@ DATA 1DATA 2DATA 3DATA 4DATA-ERR 4DATA 5 DATA-ERR 5ASSUM FLAG KEV NO-DIM NO-DIM MILLI-EV MILLI-EV MILLI-EV MILLI-EV MILLI-EV NO-DIM - 0.1112 1. -1. 70.01 0.24 52.31 + 0.1112 0.5 1. 70.01 0.24 52.31 0.46 - 0.1477 3. -1. 3.273 0.039 92.1 + 0.1477 1.5 -1. 3.273 0.039 92.1 7.6 - 0.6326 3. -1. 21.33 0.39 100.0 + 0.6326 1.5 -1. 21.33 0.39 100.0 7.0 - 0.7482 1. 1. 7.33 0.14 51. + 0.7482 0.5 1. 7.33 0.14 51. 13. - 0.7777 1. -1. 4.35 0.12 65. + 0.7777 0.5 -1. 4.35 0.12 65. 12. 1. - 0.9773 1. -1. 13.60 0.27 116. + 0.9773 0.5 -1. 13.60 0.27 116. 25. 1. - 1.2596 1. -1. 2.52 0.14 + 1.2596 0.5 -1. 2.52 0.14 89.43 1. - 1.3389 1. 1. 128.1 2.7 55.54 + 1.3389 0.5 1. 128.1 2.7 55.54 0.94 - 1.5481 1. 1. 2021.8 8.1 62.00 + 1.5481 0.5 1. 2021.8 8.1 62.00 0.84 - 1.6230 1. -1. 18.31 0.48 + 1.6230 0.5 -1. 18.31 0.48 89.43 1. - 1.7874 1. 1. 334.7 5.5 60.33 + 1.7874 0.5 1. 334.7 5.5 60.33 0.93 - 1.9272 1. -1. 9.62 0.35 + 1.9272 0.5 -1. 9.62 0.35 89.43 1. - 2.0170 3. -1. 34.9 1.1 95.6 + 2.0170 1.5 -1. 34.9 1.1 95.6 10.0 - 2.1615 1. -1. 23.88 0.70 + 2.1615 0.5 -1. 23.88 0.70 89.43 1. - 2.2928 3. -1. 23.96 0.63 + 2.2928 1.5 -1. 23.96 0.63 89.43 1. - 2.4410 1. -1. 2.44 0.28 + 2.4410 0.5 -1. 2.44 0.28 89.43 1. - 2.6594 1. 1. 117.1 3.5 49.8 + 2.6594 0.5 1. 117.1 3.5 49.8 1.4 - 2.8460 3. -1. 16.50 0.61 + 2.8460 1.5 -1. 16.50 0.61 89.43 1. - 3.3316 1. -1. 5.43 0.52 + 3.3316 0.5 -1. 5.43 0.52 89.43 1. - 3.3419 1. 1. 1080. 16. 44.9 + 3.3419 0.5 1. 1080. 16. 44.9 1.1 - 3.3600 1. 1. 1909. 20. 43.8 + 3.3600 0.5 1. 1909. 20. 43.8 1.4 - 3.3924 3. -1. 32.4 1.0 + 3.3924 1.5 -1. 32.4 1.0 89.43 1. - 3.4753 3. -1. 36.6 1.2 + 3.4753 1.5 -1. 36.6 1.2 89.43 1. - 3.7426 1. -1. 42.8 1.8 + 3.7426 0.5 -1. 42.8 1.8 89.43 1. - 3.9607 3. -1. 7.64 0.71 + 3.9607 1.5 -1. 7.64 0.71 89.43 1. - 4.0665 1. 1. 74.7 3.6 47.4 + 4.0665 0.5 1. 74.7 3.6 47.4 2.4 1. - 4.4136 3. -1. 640. 23. 95.1 + 4.4136 1.5 -1. 640. 23. 95.1 2.2 - 4.5099 1. -1. 6.06 0.80 + 4.5099 0.5 -1. 6.06 0.80 89.43 1. - 4.5208 3. -1. 43.1 1.7 + 4.5208 1.5 -1. 43.1 1.7 89.43 1. - 4.5732 1. 1. 1766. 25. 56.5 + 4.5732 0.5 1. 1766. 25. 56.5 1.7 - 4.8441 1. -1. 11.9 1.0 + 4.8441 0.5 -1. 11.9 1.0 89.43 1. - 5.2114 3. -1. 200.0 8.4 71.5 + 5.2114 1.5 -1. 200.0 8.4 71.5 2.5 - 5.2714 1. -1. 257. 10. 77.1 + 5.2714 0.5 -1. 257. 10. 77.1 2.5 - 5.5320 1. -1. 6.6 1.1 + 5.5320 0.5 -1. 6.6 1.1 89.43 1. - 5.5682 1. -1. 160.0 8.1 114.6 + 5.5682 0.5 -1. 160.0 8.1 114.6 5.1 1. - 5.5835 1. -1. 116.6 7.0 114.0 + 5.5835 0.5 -1. 116.6 7.0 114.0 6.6 1. - 5.6755 3. -1. 78.4 3.0 + 5.6755 1.5 -1. 78.4 3.0 89.43 1. - 5.7974 3. -1. 174.2 8.7 79.4 + 5.7974 1.5 -1. 174.2 8.7 79.4 2.9 - 5.8766 1. 1. 644. 26. 50.1 + 5.8766 0.5 1. 644. 26. 50.1 1.9 - 6.0069 1. -1. 42.3 2.7 + 6.0069 0.5 -1. 42.3 2.7 89.43 1. - 6.0701 1. -1. 122.0 8.4 79.9 + 6.0701 0.5 -1. 122.0 8.4 79.9 4.3 1. - 6.1309 3. -1. 75.4 3.5 + 6.1309 1.5 -1. 75.4 3.5 89.43 1. - 6.3933 3. -1. 36.9 2.0 + 6.3933 1.5 -1. 36.9 2.0 89.43 1. - 6.5102 1. 1. 1714. 38. 58.0 + 6.5102 0.5 1. 1714. 38. 58.0 2.1 - 6.6649 1. -1. 661. 28. 79.9 + 6.6649 0.5 -1. 661. 28. 79.9 2.6 - 6.7433 1. 1. 1814. 41. 51.4 + 6.7433 0.5 1. 1814. 41. 51.4 2.2 - 6.8252 3. -1. 52.9 3.2 + 6.8252 1.5 -1. 52.9 3.2 89.43 1. - 7.1741 1. -1. 11.0 1.6 + 7.1741 0.5 -1. 11.0 1.6 89.43 1. - 7.2075 3. -1. 450. 25. 95.0 + 7.2075 1.5 -1. 450. 25. 95.0 3.2 - 7.4059 1. 1. 452. 22. 50.1 + 7.4059 0.5 1. 452. 22. 50.1 2.2 - 7.4518 3. -1. 458. 25. 75.1 + 7.4518 1.5 -1. 458. 25. 75.1 2.5 - 7.6678 3. -1. 43.1 2.8 + 7.6678 1.5 -1. 43.1 2.8 89.43 1. - 7.8585 1. -1. 1687. 49. 49.8 + 7.8585 0.5 -1. 1687. 49. 49.8 2.3 - 8.0161 3. -1. 22.9 1.8 + 8.0161 1.5 -1. 22.9 1.8 89.43 1. - 8.3282 3. -1. 40.1 3.1 + 8.3282 1.5 -1. 40.1 3.1 89.43 1. - 8.5058 3. -1. 43.0 3.0 + 8.5058 1.5 -1. 43.0 3.0 89.43 1. - 8.5364 1. +1. 874. 41. 50.9 + 8.5364 0.5 +1. 874. 41. 50.9 2.5 - 8.6933 3. -1. 239. 19. 100.2 + 8.6933 1.5 -1. 239. 19. 100.2 5.2 - 8.8340 3. -1. 278. 21. 86.6 + 8.8340 1.5 -1. 278. 21. 86.6 4.4 - 8.8667 1. -1. 287. 21. 91.6 + 8.8667 0.5 -1. 287. 21. 91.6 4.7 1. - 8.9195 1. 1. 1504. 52. 60.6 + 8.9195 0.5 1. 1504. 52. 60.6 3.1 - 9.0332 1. -1. 14.7 2.2 + 9.0332 0.5 -1. 14.7 2.2 89.43 1. - 9.0943 3. -1. 56.2 4.0 + 9.0943 1.5 -1. 56.2 4.0 89.43 1. - 9.2563 1. 1. 693. 38. 59.8 + 9.2563 0.5 1. 693. 38. 59.8 3.0 - 9.3272 3. -1. 419. 29. 58.1 + 9.3272 1.5 -1. 419. 29. 58.1 2.3 - 9.4289 1. 1. 303. 22. 44.1 + 9.4289 0.5 1. 303. 22. 44.1 2.8 - 9.6063 1. -1. 20.6 2.3 + 9.6063 0.5 -1. 20.6 2.3 89.43 1. - 9.8222 1. -1. 50.8 5.7 + 9.8222 0.5 -1. 50.8 5.7 89.43 1. - 10.2008 1. 1. 282. 25. 54.0 + 10.2008 0.5 1. 282. 25. 54.0 4.0 - 10.3648 1. -1. 157. 21. 77.2 + 10.3648 0.5 -1. 157. 21. 77.2 5.7 1. - 10.4275 3. -1. 72.4 4.9 + 10.4275 1.5 -1. 72.4 4.9 89.43 1. - 10.7351 3. -1. 259. 26. 70.2 + 10.7351 1.5 -1. 259. 26. 70.2 3.9 - 10.8251 1. 1. 1911. 73. 61.3 + 10.8251 0.5 1. 1911. 73. 61.3 3.7 - 10.9893 3. -1. 323. 31. 57.7 + 10.9893 1.5 -1. 323. 31. 57.7 3.0 1. - 11.1159 1. +1. 206. 27. 59.1 + 11.1159 0.5 +1. 206. 27. 59.1 5.0 1. - 11.1462 3. -1. 59.5 4.4 + 11.1462 1.5 -1. 59.5 4.4 89.43 1. - 11.2215 3. -1. 57.4 4.0 + 11.2215 1.5 -1. 57.4 4.0 89.43 1. - 11.3960 3. -1. 329. 32. 86.9 + 11.3960 1.5 -1. 329. 32. 86.9 4.4 - 11.6935 1. -1. 577. 44. 53.2 + 11.6935 0.5 -1. 577. 44. 53.2 3.7 - 11.9821 3. -1. 57.4 4.8 + 11.9821 1.5 -1. 57.4 4.8 89.43 1. - 12.1453 1. -1. 40.2 5.5 + 12.1453 0.5 -1. 40.2 5.5 89.43 1. - 12.1775 3. -1. 267. 32. 63.8 + 12.1775 1.5 -1. 267. 32. 63.8 5.1 1. - 12.1989 1. -1. 303. 35. 109.5 + 12.1989 0.5 -1. 303. 35. 109.5 8.1 1. - 12.2536 3. -1. 561. 54. 78.8 + 12.2536 1.5 -1. 561. 54. 78.8 4.0 - 12.2800 1. -1. 30.6 5.3 + 12.2800 0.5 -1. 30.6 5.3 89.43 1. - 12.6449 1. 1. 483. 46. 71.1 + 12.6449 0.5 1. 483. 46. 71.1 5.3 - 12.6869 3. -1. 782. 58. 66.2 + 12.6869 1.5 -1. 782. 58. 66.2 3.3 - 12.8540 1. -1. 45.9 6.8 + 12.8540 0.5 -1. 45.9 6.8 89.43 1. - 12.9168 3. -1. 524. 52. 70.1 + 12.9168 1.5 -1. 524. 52. 70.1 4.0 - 13.0365 3. -1. 810. 59. 80.7 + 13.0365 1.5 -1. 810. 59. 80.7 3.6 - 13.1406 3. -1. 514. 48. 80.9 + 13.1406 1.5 -1. 514. 48. 80.9 4.6 - 13.2309 3. -1. 45.7 5.2 + 13.2309 1.5 -1. 45.7 5.2 89.43 1. - 13.3870 1. -1. 1919. 98. 100.9 + 13.3870 0.5 -1. 1919. 98. 100.9 5.3 - 13.7271 1. -1. 29.9 4.6 + 13.7271 0.5 -1. 29.9 4.6 89.43 1. - 13.8604 3. -1. 1229. 85. 74.8 + 13.8604 1.5 -1. 1229. 85. 74.8 3.7 - 13.9040 1. 1. 4580. 120. 54.1 + 13.9040 0.5 1. 4580. 120. 54.1 4.6 - 14.0545 3. -1. 198. 40. 68.1 + 14.0545 1.5 -1. 198. 40. 68.1 6.3 1. - 14.4312 3. -1. 182. 38. 97.7 + 14.4312 1.5 -1. 182. 38. 97.7 9.0 1. - 14.4904 3. -1. 146. 15. + 14.4904 1.5 -1. 146. 15. 89.43 1. - 14.5853 1. -1. 22.1 4.6 + 14.5853 0.5 -1. 22.1 4.6 89.43 1. - 14.7143 3. -1. 505. 60. 90.7 + 14.7143 1.5 -1. 505. 60. 90.7 5.6 - 15.0469 1. -1. 44.4 8.1 + 15.0469 0.5 -1. 44.4 8.1 89.43 1. - 15.1500 1. -1. 22.9 4.9 + 15.1500 0.5 -1. 22.9 4.9 89.43 1. - 15.1900 1. -1. 15.0 4.0 + 15.1900 0.5 -1. 15.0 4.0 89.43 1. - 15.2800 1. -1. 17.4 4.0 + 15.2800 0.5 -1. 17.4 4.0 89.43 1. - 15.5022 3. -1. 566. 67. 73.9 + 15.5022 1.5 -1. 566. 67. 73.9 5.9 - 15.5209 1. -1. 4490. 160. 81.7 + 15.5209 0.5 -1. 4490. 160. 81.7 7.8 - 15.7251 1. -1. 1052. 99. 109.0 + 15.7251 0.5 -1. 1052. 99. 109.0 9.5 - 15.7485 3. -1. 940. 100. 132.5 + 15.7485 1.5 -1. 940. 100. 132.5 7.1 - 15.9324 1. -1. 45.8 9.1 + 15.9324 0.5 -1. 45.8 9.1 89.43 1. - 16.1308 1. 1. 668. 71. 47.4 + 16.1308 0.5 1. 668. 71. 47.4 5.6 - 16.2721 3. -1. 594. 79. 73.3 + 16.2721 1.5 -1. 594. 79. 73.3 4.9 1. - 16.5375 1. 1. 2310. 130. 45.4 + 16.5375 0.5 1. 2310. 130. 45.4 5.1 - 16.5728 3. -1. 392. 65. 63.7 + 16.5728 1.5 -1. 392. 65. 63.7 5.5 1. - 16.6910 3. -1. 91. 12. + 16.6910 1.5 -1. 91. 12. 89.43 1. - 16.7482 3. -1. 148. 40. + 16.7482 1.5 -1. 148. 40. 89.43 1. - 16.7538 1. 1. 11990. 250. 70. + 16.7538 0.5 1. 11990. 250. 70. 18. - 16.8006 3. -1. 80. 13. + 16.8006 1.5 -1. 80. 13. 89.43 1. - 17.1698 3. -1. 265. 55. 88.3 + 17.1698 1.5 -1. 265. 55. 88.3 8.2 - 17.4062 1. 1. 221. 52. 52.8 + 17.4062 0.5 1. 221. 52. 52.8 8.1 1. - 17.5978 1. 1. 1490. 120. 45.0 + 17.5978 0.5 1. 1490. 120. 45.0 5.1 - 17.6447 3. -1. 339. 68. 81.1 + 17.6447 1.5 -1. 339. 68. 81.1 7.3 - 17.7120 1. -1. 40.7 8.1 + 17.7120 0.5 -1. 40.7 8.1 89.43 1. - 17.9696 3. -1. 1020. 140. 107.9 + 17.9696 1.5 -1. 1020. 140. 107.9 6.1 - 18.0320 1. -1. 157. 45. 63. + 18.0320 0.5 -1. 157. 45. 63. 11. 1. - 18.1875 3. -1. 326. 63. 100.0 + 18.1875 1.5 -1. 326. 63. 100.0 7.5 - 18.2320 1. -1. 36.5 8.7 + 18.2320 0.5 -1. 36.5 8.7 89.43 1. - 18.2750 3. -1. 181. 52. 110. + 18.2750 1.5 -1. 181. 52. 110. 15. - 18.3632 3. -1. 770. 100. 94.7 + 18.3632 1.5 -1. 770. 100. 94.7 6.3 - 18.4902 3. -1. 1280. 140. 59.9 + 18.4902 1.5 -1. 1280. 140. 59.9 4.0 - 18.9053 3. -1. 105. 16. + 18.9053 1.5 -1. 105. 16. 89.43 1. - 19.0522 3. -1. 293. 67. 104.9 + 19.0522 1.5 -1. 293. 67. 104.9 9.4 - 19.1900 1. 1. 446. 84. 41.2 + 19.1900 0.5 1. 446. 84. 41.2 6.2 1. - 19.2224 3. -1. 140. 18. + 19.2224 1.5 -1. 140. 18. 89.43 1. - 19.4938 1. 1. 1260. 120. 61.8 + 19.4938 0.5 1. 1260. 120. 61.8 7.6 - 19.5250 3. -1. 83. 14. 89.4 + 19.5250 1.5 -1. 83. 14. 89.4 1. - 19.6054 3. -1. 194. 57. 128. + 19.6054 1.5 -1. 194. 57. 128. 20. - 19.7640 1. -1. 33.2 8.6 + 19.7640 0.5 -1. 33.2 8.6 89.43 1. - 19.8557 3. -1. 477. 90. 102.9 + 19.8557 1.5 -1. 477. 90. 102.9 8.7 - 20.2860 1. -1. 50. 12. + 20.2860 0.5 -1. 50. 12. 89.43 1. - 20.3311 3. -1. 104. 16. + 20.3311 1.5 -1. 104. 16. 89.43 - 20.5028 3. -1. 960. 130. 92.9 + 20.5028 1.5 -1. 960. 130. 92.9 7.1 - 20.5350 3. -1. 120. 25. + 20.5350 1.5 -1. 120. 25. 89.43 1. - 20.6815 3. -1. 1630. 180. 67.1 + 20.6815 1.5 -1. 1630. 180. 67.1 5.0 - 20.7432 1. 1. 1990. 160. 54.3 + 20.7432 0.5 1. 1990. 160. 54.3 6.7 - 20.9200 3. -1. 45.0 8.5 + 20.9200 1.5 -1. 45.0 8.5 89.43 1. - 21.0800 3. -1. 320. 80. 120. + 21.0800 1.5 -1. 320. 80. 120. 19. 1. - 21.0990 1. 1. 900. 120. 47.5 + 21.0990 0.5 1. 900. 120. 47.5 8.9 1. - 21.1952 1. 1. 1730. 160. 70.5 + 21.1952 0.5 1. 1730. 160. 70.5 7.4 - 21.2950 3. -1. 900. 130. 85.2 + 21.2950 1.5 -1. 900. 130. 85.2 7.2 - 21.3181 1. -1. 5300. 280. 60.7 + 21.3181 0.5 -1. 5300. 280. 60.7 9.0 - 21.4004 3. -1. 6260. 360. 68.6 + 21.4004 1.5 -1. 6260. 360. 68.6 4.8 - 21.4878 3. -1. 2190. 240. 100.4 + 21.4878 1.5 -1. 2190. 240. 100.4 5.6 - 21.8423 3. -1. 286. 76. 117. + 21.8423 1.5 -1. 286. 76. 117. 13. - 22.0180 3. -1. 32.8 6.5 + 22.0180 1.5 -1. 32.8 6.5 89.43 1. - 22.1676 1. -1. 415. 97. 61. + 22.1676 0.5 -1. 415. 97. 61. 12. 1. - 22.2001 3. -1. 1340. 180. 75.6 + 22.2001 1.5 -1. 1340. 180. 75.6 6.4 - 22.2580 3. -1. 30.9 7.7 + 22.2580 1.5 -1. 30.9 7.7 89.43 1. - 22.4000 1. -1. 40.5 8.2 + 22.4000 0.5 -1. 40.5 8.2 89.43 1. - 22.4750 3. -1. 109. 19. + 22.4750 1.5 -1. 109. 19. 89.43 1. - 22.5586 1. -1. 2650. 210. 85.0 + 22.5586 0.5 -1. 2650. 210. 85.0 8.8 - 22.6154 3. -1. 363. 83. 128. + 22.6154 1.5 -1. 363. 83. 128. 14. - 22.8820 3. -1. 45. 10. + 22.8820 1.5 -1. 45. 10. 89.43 1. - 23.0575 3. -1. 1350. 170. 67.5 + 23.0575 1.5 -1. 1350. 170. 67.5 5.6 1. - 23.1823 3. -1. 1820. 220. 62.5 + 23.1823 1.5 -1. 1820. 220. 62.5 5.7 - 23.2770 1. -1. 24.5 6.1 + 23.2770 0.5 -1. 24.5 6.1 89.43 1. - 23.3360 3. -1. 29.2 7.5 + 23.3360 1.5 -1. 29.2 7.5 89.43 1. - 23.5150 3. -1. 271. 75. 84. + 23.5150 1.5 -1. 271. 75. 84. 13. - 23.5671 1. -1. 1190. 160. 65.6 + 23.5671 0.5 -1. 1190. 160. 65.6 9.2 1. - 23.7065 1. 1. 1320. 170. 66.4 + 23.7065 0.5 1. 1320. 170. 66.4 8.7 1. - 24.0366 3. -1. 2160. 260. 72.4 + 24.0366 1.5 -1. 2160. 260. 72.4 5.5 - 24.1508 3. -1. 720. 150. 62.1 + 24.1508 1.5 -1. 720. 150. 62.1 6.0 1. - 24.2280 3. -1. 248. 74. 116. + 24.2280 1.5 -1. 248. 74. 116. 15. 1. - 24.6899 3. -1. 360. 100. 88. + 24.6899 1.5 -1. 360. 100. 88. 13. - 24.7313 1. 1. 2620. 290. 56. + 24.7313 0.5 1. 2620. 290. 56. 14. - 24.7500 3. -1. 400. 120. 93. + 24.7500 1.5 -1. 400. 120. 93. 15. 1. - 24.8550 3. -1. 55. 14. + 24.8550 1.5 -1. 55. 14. 89.43 1. - 24.8950 3. -1. 55. 13. + 24.8950 1.5 -1. 55. 13. 89.43 1. - 25.0787 1. -1. 720. 140. 111. + 25.0787 0.5 -1. 720. 140. 111. 12. 1. - 25.2500 3. -1. 49.1 9.9 + 25.2500 1.5 -1. 49.1 9.9 89.43 1. - 25.3260 3. -1. 34.0 9.5 + 25.3260 1.5 -1. 34.0 9.5 89.43 1. - 25.3840 3. -1. 248. 71. 120. + 25.3840 1.5 -1. 248. 71. 120. 18. 1. - 25.5290 3. -1. 62. 12. + 25.5290 1.5 -1. 62. 12. 89.43 1. - 25.9521 3. -1. 820. 160. 101.4 + 25.9521 1.5 -1. 820. 160. 101.4 8.9 - 26.0020 3. -1. 60. 14. + 26.0020 1.5 -1. 60. 14. 89.43 1. - 26.0609 1. -1. 590. 130. 79. + 26.0609 0.5 -1. 590. 130. 79. 12. 1. - 26.1809 3. -1. 4760. 420. 64.4 + 26.1809 1.5 -1. 4760. 420. 64.4 5.7 - 26.2750 3. -1. 194. 75. 72. + 26.2750 1.5 -1. 194. 75. 72. 12. 1. - 26.4482 3. -1. 1790. 270. 79.2 + 26.4482 1.5 -1. 1790. 270. 79.2 6.2 - 26.6320 3. -1. 340. 110. 109. + 26.6320 1.5 -1. 340. 110. 109. 11. 1. - 26.6810 3. -1. 65. 18. + 26.6810 1.5 -1. 65. 18. 89.43 1. - 26.7516 1. -1. 2070. 260. 104. + 26.7516 0.5 -1. 2070. 260. 104. 11. 1. - 26.8210 3. -1. 89. 20. + 26.8210 1.5 -1. 89. 20. 89.43 1. - 26.9968 1. 1. 2910. 390. 52. + 26.9968 0.5 1. 2910. 390. 52. 18. - 27.0050 3. -1. 1060. 350. 110. + 27.0050 1.5 -1. 1060. 350. 110. 15. 1. - 27.2360 1. -1. 209. 74. 108. + 27.2360 0.5 -1. 209. 74. 108. 27. 1. - 27.2702 1. -1. 2030. 260. 84. + 27.2702 0.5 -1. 2030. 260. 84. 13. 1. - 27.4817 3. -1. 12030. 560. 174.6 + 27.4817 1.5 -1. 12030. 560. 174.6 9.6 - 27.6877 1. 1. 6440. 380. 65. + 27.6877 0.5 1. 6440. 380. 65. 10. - 27.8481 3. -1. 5950. 520. 84.5 + 27.8481 1.5 -1. 5950. 520. 84.5 7.7 - 27.8764 1. 1. 590. 160. 57. + 27.8764 0.5 1. 590. 160. 57. 15. 1. - 27.9280 1. -1. 1300. 230. 94. + 27.9280 0.5 -1. 1300. 230. 94. 12. 1. - 28.1809 3. -1. 1440. 250. 95.6 + 28.1809 1.5 -1. 1440. 250. 95.6 9.4 - 28.2100 1. -1. 700. 170. 70. + 28.2100 0.5 -1. 700. 170. 70. 13. 1. - 28.3700 1. -1. 40. 10. + 28.3700 0.5 -1. 40. 10. 89.43 1. - 28.5072 3. -1. 2760. 380. 59.6 + 28.5072 1.5 -1. 2760. 380. 59.6 7.2 1. - 28.5480 1. -1. 900. 200. 100. + 28.5480 0.5 -1. 900. 200. 100. 16. 1. - 28.6027 1. 1. 3810. 340. 64. + 28.6027 0.5 1. 3810. 340. 64. 11. - 28.9300 3. -1. 1200. 240. 95. + 28.9300 1.5 -1. 1200. 240. 95. 10. - 28.9644 3. -1. 5120. 540. 107. + 28.9644 1.5 -1. 5120. 540. 107. 11. - 29.1140 3. -1. 3970. 460. 95.1 + 29.1140 1.5 -1. 3970. 460. 95.1 8.0 - 29.1862 1. 1. 2260. 280. 23.5 + 29.1862 0.5 1. 2260. 280. 23.5 5.9 - 29.4070 3. -1. 126. 25. + 29.4070 1.5 -1. 126. 25. 89.43 1. - 29.5650 3. -1. 143. 26. + 29.5650 1.5 -1. 143. 26. 89.43 1. - 29.8170 3. -1. 1230. 340. 100. + 29.8170 1.5 -1. 1230. 340. 100. 17. 1. - 29.8189 1. 1. 4070. 390. 60. + 29.8189 0.5 1. 4070. 390. 60. 23. ENDDATA 436 ENDSUBENT 453 -SUBENT 13909006 20040826 +SUBENT 13909006 20040826 20050909 1336 BIB 6 12 REACTION 1(50-SN-120(N,0),,EN) 2(50-SN-120(N,0),,J) @@ -517,7 +518,7 @@ ANALYSIS (RFN) Analyzed capture and transmission data using REL-REF (R,10639005,CARLTON+,J,PR/C,14,1439,1976). ERR-ANALYS (DATA-ERR) Errors fron fitting procedures. FLAG (1.) Spin, parity assignment uncertain. -STATUS Data taken from Table II in reference. +STATUS Data taken from Table III in reference. ENDBIB 12 NOCOMMON 0 0 DATA 9 187 @@ -525,379 +526,379 @@ DATA 1DATA 2DATA 3DATA 4DATA-ERR 4DATA 5 DATA-ERR 5ASSUM FLAG KEV NO-DIM NO-DIM MILLI-EV MILLI-EV MILLI-EV MILLI-EV MILLI-EV NO-DIM - 0.3643 3. -1. 2.912 0.016 125. + 0.3643 1.5 -1. 2.912 0.016 125. 16. - 0.4261 1. 1. 10.140 0.080 246. + 0.4261 0.5 1. 10.140 0.080 246. 20. - 0.9198 3. -1. 20.53 0.38 + 0.9198 1.5 -1. 20.53 0.38 80.37 - 0.9486 1. 1. 123.86 0.65 44.29 + 0.9486 0.5 1. 123.86 0.65 44.29 0.72 - 1.2831 3. -1. 11.84 0.30 + 1.2831 1.5 -1. 11.84 0.30 80.37 - 1.4200 3. -1. 50.4 1.1 + 1.4200 1.5 -1. 50.4 1.1 80.37 - 1.7134 1. 1. 165.3 1.8 90.3 + 1.7134 0.5 1. 165.3 1.8 90.3 1.6 - 2.7726 1. 1. 2.31 0.28 + 2.7726 0.5 1. 2.31 0.28 80.37 1. - 2.8368 3. -1. 55.4 1.7 + 2.8368 1.5 -1. 55.4 1.7 80.37 - 3.1184 1. 1. 734.9 3.7 32.39 + 3.1184 0.5 1. 734.9 3.7 32.39 0.67 - 3.8489 3. -1. 137.8 3.0 85.6 + 3.8489 1.5 -1. 137.8 3.0 85.6 4.4 - 4.2034 3. -1. 467. 2.0 + 4.2034 1.5 -1. 467. 2.0 80.37 - 4.3283 3. -1. 32.9 1.5 + 4.3283 1.5 -1. 32.9 1.5 80.37 - 4.3556 1. 1. 414.4 4.5 31.43 + 4.3556 0.5 1. 414.4 4.5 31.43 0.90 - 5.0221 1. -1. 66.6 1.6 104.8 + 5.0221 0.5 -1. 66.6 1.6 104.8 5.7 - 5.0672 1. 1. 537.0 8.3 132.4 + 5.0672 0.5 1. 537.0 8.3 132.4 2.7 - 5.1941 3. -1. 82.4 3.4 + 5.1941 1.5 -1. 82.4 3.4 80.37 - 6.6768 3. -1. 209.0 5.4 226. + 6.6768 1.5 -1. 209.0 5.4 226. 35. - 6.9783 1. 1. 229.6 5.9 64.5 + 6.9783 0.5 1. 229.6 5.9 64.5 2.8 - 7.1185 1. 1. 120.4 3.2 36.7 + 7.1185 0.5 1. 120.4 3.2 36.7 2.8 - 7.3060 1. 1. 541.1 8.7 33.6 + 7.3060 0.5 1. 541.1 8.7 33.6 1.5 - 7.4995 3. -1. 150.2 4.2 67.4 + 7.4995 1.5 -1. 150.2 4.2 67.4 3.9 - 7.7778 1. -1. 6.8 1.3 + 7.7778 0.5 -1. 6.8 1.3 80.37 1. - 8.1642 1. 1. 973. 16. 80.1 + 8.1642 0.5 1. 973. 16. 80.1 2.4 - 8.6119 3. -1. 199.7 5.9 76. + 8.6119 1.5 -1. 199.7 5.9 76. 13. - 8.6671 1. 1. 92.5 3.7 34.1 + 8.6671 0.5 1. 92.5 3.7 34.1 3.2 - 8.9477 1. 1. 7561. 3. 30.5 + 8.9477 0.5 1. 7561. 3. 30.5 2.4 - 9.1219 3. -1. 66.2 4.7 + 9.1219 1.5 -1. 66.2 4.7 80.37 - 9.5489 1. 1. 1708. 22. 65.1 + 9.5489 0.5 1. 1708. 22. 65.1 2.3 - 9.5708 1. -1. 6.9 1.6 + 9.5708 0.5 -1. 6.9 1.6 80.37 1. - 10.3232 1. 1. 339. 13. 74.7 + 10.3232 0.5 1. 339. 13. 74.7 5.3 - 10.5720 3. -1. 24.7 2.8 + 10.5720 1.5 -1. 24.7 2.8 80.37 1. - 10.8858 3. -1. 717. 29. 74.7 + 10.8858 1.5 -1. 717. 29. 74.7 2.5 - 11.2843 3. -1. 983. 28. 60.4 + 11.2843 1.5 -1. 983. 28. 60.4 2.1 - 11.4889 1. 1. 334. 11. 30.1 + 11.4889 0.5 1. 334. 11. 30.1 2.5 - 11.6627 3. -1. 157.6 8.5 86.1 + 11.6627 1.5 -1. 157.6 8.5 86.1 7.3 - 11.7909 1. 1. 646. 16. 34.4 + 11.7909 0.5 1. 646. 16. 34.4 2.6 - 12.3527 3. -1. 103.3 9.7 + 12.3527 1.5 -1. 103.3 9.7 80.37 1. - 12.6864 1. 1. 38.0 5.6 + 12.6864 0.5 1. 38.0 5.6 80.37 1. - 12.8708 3. -1. 827. 29. 83.9 + 12.8708 1.5 -1. 827. 29. 83.9 3.3 - 13.0527 1. 1. 589. 17. 30.1 + 13.0527 0.5 1. 589. 17. 30.1 2.7 - 13.7430 1. 1. 16.2 3.1 + 13.7430 0.5 1. 16.2 3.1 80.37 1. - 13.8825 3. -1. 53.6 6.1 + 13.8825 1.5 -1. 53.6 6.1 80.37 1. - 14.2634 3. -1. 163. 12. 84.1 + 14.2634 1.5 -1. 163. 12. 84.1 7.6 - 14.7318 1. 1. 252. 14. 74.1 + 14.7318 0.5 1. 252. 14. 74.1 7.7 - 15.1672 3. -1. 29.2 4.2 + 15.1672 1.5 -1. 29.2 4.2 80.37 1. - 15.6257 3. -1. 30.2 4.4 + 15.6257 1.5 -1. 30.2 4.4 80.37 1. - 16.0266 1. -1. 8.6 2.1 + 16.0266 0.5 -1. 8.6 2.1 80.37 1. - 16.1445 1. 1. 4684. 49. 74.3 + 16.1445 0.5 1. 4684. 49. 74.3 4.7 - 16.2180 1. 1. 10.8 2.5 + 16.2180 0.5 1. 10.8 2.5 80.37 1. - 16.5300 1. 1. 13.0 3.0 + 16.5300 0.5 1. 13.0 3.0 80.37 1. - 16.6078 3. -1. 5623. 72. 83.3 + 16.6078 1.5 -1. 5623. 72. 83.3 3.2 - 16.7122 1. 1. 240. 15. 56.2 + 16.7122 0.5 1. 240. 15. 56.2 4.9 1. - 17.1837 3. -1. 9999. 80. 67.4 + 17.1837 1.5 -1. 9999. 80. 67.4 3.2 - 17.3490 3. -1. 480. 28. 46.6 + 17.3490 1.5 -1. 480. 28. 46.6 3.3 - 17.4373 3. -1. 121. 13. 111. + 17.4373 1.5 -1. 121. 13. 111. 10. - 18.0292 1. 1. 1013. 31. 38.7 + 18.0292 0.5 1. 1013. 31. 38.7 3.6 - 18.2308 3. -1. 321. 25. 73.9 + 18.2308 1.5 -1. 321. 25. 73.9 5.4 - 18.3352 3. -1. 61.5 9.0 + 18.3352 1.5 -1. 61.5 9.0 80.37 1. - 18.8144 3. -1. 296. 22. 54.8 + 18.8144 1.5 -1. 296. 22. 54.8 5.9 - 18.9499 1. 1. 1093. 34. 46.4 + 18.9499 0.5 1. 1093. 34. 46.4 4.0 - 19.2395 1. -1. 20.0 4.2 + 19.2395 0.5 -1. 20.0 4.2 80.37 1. - 19.2713 1. 1. 2015. 40. 43.1 + 19.2713 0.5 1. 2015. 40. 43.1 4.8 - 19.3074 3. -1. 1401. 77. 74.0 + 19.3074 1.5 -1. 1401. 77. 74.0 4.5 - 19.6341 1. 1. 178. 17. 44.3 + 19.6341 0.5 1. 178. 17. 44.3 7.5 1. - 20.9766 1. 1. 3732. 52. 40.0 + 20.9766 0.5 1. 3732. 52. 40.0 4.0 - 21.4176 1. 1. 793. 48. 77.4 + 21.4176 0.5 1. 793. 48. 77.4 9.8 - 21.8764 1. -1. 1344. 62. 73.2 + 21.8764 0.5 -1. 1344. 62. 73.2 5.5 - 22.1978 3. -1. 714. 54. 46.4 + 22.1978 1.5 -1. 714. 54. 46.4 3.0 - 22.6767 3. -1. 461. 36. 176.6 + 22.6767 1.5 -1. 461. 36. 176.6 9.0 - 22.7344 3. -1. 591. 38. 57.3 + 22.7344 1.5 -1. 591. 38. 57.3 4.3 - 23.0402 1. 1. 6116. 65. 40.3 + 23.0402 0.5 1. 6116. 65. 40.3 6.2 - 23.3145 3. -1. 7060. 120. 85.2 + 23.3145 1.5 -1. 7060. 120. 85.2 4.3 - 23.6008 1. 1. 1848. 77. 70.9 + 23.6008 0.5 1. 1848. 77. 70.9 6.1 - 23.6693 1. 1. 1301. 49. 45.4 + 23.6693 0.5 1. 1301. 49. 45.4 5.5 - 24.0436 3. -1. 1550. 100. 81.6 + 24.0436 1.5 -1. 1550. 100. 81.6 4.2 - 24.4557 3. -1. 453. 40. 53.7 + 24.4557 1.5 -1. 453. 40. 53.7 3.7 - 24.8345 1. 1. 7072. 95. 59.3 + 24.8345 0.5 1. 7072. 95. 59.3 7.0 - 25.1818 3. -1. 2430. 140. 49.3 + 25.1818 1.5 -1. 2430. 140. 49.3 3.8 - 25.5296 1. 1. 3365. 95. 67.7 + 25.5296 0.5 1. 3365. 95. 67.7 6.9 - 26.0004 3. -1. 1290. 94. 73.4 + 26.0004 1.5 -1. 1290. 94. 73.4 4.2 - 26.1365 3. -1. 27.8 5.8 + 26.1365 1.5 -1. 27.8 5.8 80.37 1. - 26.2243 1. 1. 4989. 73. 46.9 + 26.2243 0.5 1. 4989. 73. 46.9 6.8 - 26.2931 3. -1. 1028. 82. 51.8 + 26.2931 1.5 -1. 1028. 82. 51.8 4.0 - 26.4916 1. 1. 2062. 94. 88.2 + 26.4916 0.5 1. 2062. 94. 88.2 7.1 - 26.6368 3. -1. 32.7 7.2 + 26.6368 1.5 -1. 32.7 7.2 80.37 1. - 27.1443 3. -1. 8530. 150. 64.0 + 27.1443 1.5 -1. 8530. 150. 64.0 4.4 - 27.4067 3. -1. 2390. 140. 54.8 + 27.4067 1.5 -1. 2390. 140. 54.8 4.4 - 27.8270 3. -1. 249. 29. 65.1 + 27.8270 1.5 -1. 249. 29. 65.1 8.6 - 27.9603 1. 1. 630. 47. 28.0 + 27.9603 0.5 1. 630. 47. 28.0 6.1 - 28.2584 1. 1. 5090. 110. 40.9 + 28.2584 0.5 1. 5090. 110. 40.9 5.9 - 28.3820 1. -1. 22.7 5.5 + 28.3820 0.5 -1. 22.7 5.5 80.37 1. - 28.5241 3. -1. 7440. 160. 140.3 + 28.5241 1.5 -1. 7440. 160. 140.3 6.9 - 28.6110 1. 1. 537. 46. 18.9 + 28.6110 0.5 1. 537. 46. 18.9 5.0 - 29.1740 3. -1. 3260. 160. 60.1 + 29.1740 1.5 -1. 3260. 160. 60.1 4.9 - 29.3341 1. 1. 1605. 67. 19.2 + 29.3341 0.5 1. 1605. 67. 19.2 5.0 - 29.6696 1. 1. 1526. 93. 75. + 29.6696 0.5 1. 1526. 93. 75. 12. - 30.5050 3. -1. 110. 25. + 30.5050 1.5 -1. 110. 25. 80.37 1. - 30.6219 1. 1. 3032. 83. 22.9 + 30.6219 0.5 1. 3032. 83. 22.9 6.2 - 31.0200 1. 1. 30.3 9.6 + 31.0200 0.5 1. 30.3 9.6 80.37 1. - 31.2339 1. -1. 27.3 6.6 + 31.2339 0.5 -1. 27.3 6.6 80.37 1. - 31.7156 3. -1. 9030. 180. 55.9 + 31.7156 1.5 -1. 9030. 180. 55.9 7.6 - 31.7400 3. -1. 81. 23. + 31.7400 1.5 -1. 81. 23. 80.37 1. - 32.0761 1. 1. 678. 71. 75. + 32.0761 0.5 1. 678. 71. 75. 14. - 32.7155 1. 1. 1983. 85. 35.5 + 32.7155 0.5 1. 1983. 85. 35.5 8.8 - 32.8118 3. -1. 11720. 210. 79.9 + 32.8118 1.5 -1. 11720. 210. 79.9 9.0 - 32.9698 3. -1. 14370. 210. 79.3 + 32.9698 1.5 -1. 14370. 210. 79.3 8.2 - 33.1126 1. 1. 49. 13. + 33.1126 0.5 1. 49. 13. 80.37 1. - 33.2010 1. 1. 43. 11. + 33.2010 0.5 1. 43. 11. 80.37 1. - 33.2594 1. 1. 4220. 150. 68. + 33.2594 0.5 1. 4220. 150. 68. 13. - 33.4287 1. 1. 60. 16. + 33.4287 0.5 1. 60. 16. 80.37 1. - 33.4685 3. -1. 1270. 120. 67.1 + 33.4685 1.5 -1. 1270. 120. 67.1 9.1 - 34.1544 3. -1. 111. 25. + 34.1544 1.5 -1. 111. 25. 80.37 1. - 34.7475 3. -1. 120. 27. + 34.7475 1.5 -1. 120. 27. 80.37 1. - 35.0470 1. 1. 572. 72. 25.5 + 35.0470 0.5 1. 572. 72. 25.5 7.5 - 35.1202 1. 1. 2980. 170. 55. + 35.1202 0.5 1. 2980. 170. 55. 13. - 35.1658 1. 1. 990. 120. 91. + 35.1658 0.5 1. 990. 120. 91. 17. - 35.9805 1. 1. 69. 91. 95. + 35.9805 0.5 1. 69. 91. 95. 18. 1. - 36.0545 1. 1. 3430. 130. 48. + 36.0545 0.5 1. 3430. 130. 48. 13. - 36.1900 3. -1. 47. 15. + 36.1900 1.5 -1. 47. 15. 80.37 1. - 36.2650 1. 1. 41. 14. + 36.2650 0.5 1. 41. 14. 80.37 1. - 36.4650 1. 1. 2690. 120. 49. + 36.4650 0.5 1. 2690. 120. 49. 10. - 37.4100 1. -1. 40. 14. + 37.4100 0.5 -1. 40. 14. 80.37 1. - 37.4750 3. -1. 155. 43. + 37.4750 1.5 -1. 155. 43. 80.37 1. - 37.6260 1. 1. 982. 93. 73. + 37.6260 0.5 1. 982. 93. 73. 15. 1. - 37.7800 3. -1. 46. 14. + 37.7800 1.5 -1. 46. 14. 80.37 1. - 37.9031 3. -1. 6600. 350. 62. + 37.9031 1.5 -1. 6600. 350. 62. 12. - 37.9384 3. -1. 2940. 300. 70. + 37.9384 1.5 -1. 2940. 300. 70. 13. - 38.1652 1. 1. 3720. 180. 77. + 38.1652 0.5 1. 3720. 180. 77. 15. - 38.5796 3. -1. 15400. 280. 61.1 + 38.5796 1.5 -1. 15400. 280. 61.1 8.6 - 38.8671 1. 1. 1650. 110. 33.0 + 38.8671 0.5 1. 1650. 110. 33.0 9.9 - 39.0600 1. 1. 46. 13. + 39.0600 0.5 1. 46. 13. 80.37 1. - 39.2750 1. -1. 3280. 190. 64. + 39.2750 0.5 -1. 3280. 190. 64. 13. - 39.4100 1. 1. 57. 18. + 39.4100 0.5 1. 57. 18. 80.37 1. - 39.7650 1. -1. 61. 20. + 39.7650 0.5 -1. 61. 20. 80.37 1. - 39.9100 3. -1. 200. 60. + 39.9100 1.5 -1. 200. 60. 80.37 1. - 40.0283 3. -1. 3830. 250. 75.6 + 40.0283 1.5 -1. 3830. 250. 75.6 9.1 - 40.1402 1. 1. 3450. 130. 33. + 40.1402 0.5 1. 3450. 130. 33. 10. - 40.5500 1. -1. 62. 22. + 40.5500 0.5 -1. 62. 22. 80.37 1. - 40.8804 1. 1. 5190. 200. 88. + 40.8804 0.5 1. 5190. 200. 88. 18. - 40.9941 1. -1. 1450. 140. 75. + 40.9941 0.5 -1. 1450. 140. 75. 19. - 41.2240 3. -1. 136. 46. + 41.2240 1.5 -1. 136. 46. 80.37 1. - 41.6750 3. -1. 134. 47. + 41.6750 1.5 -1. 134. 47. 80.37 1. - 41.9000 3. -1. 74. 19. + 41.9000 1.5 -1. 74. 19. 80.37 1. - 42.3100 1. 1. 67. 27. + 42.3100 0.5 1. 67. 27. 80.37 1. - 42.4724 3. -1. 9780. 310. 63.0 + 42.4724 1.5 -1. 9780. 310. 63.0 9.9 - 42.6899 3. -1. 3550. 280. 82. + 42.6899 1.5 -1. 3550. 280. 82. 13. - 43.4881 1. 1. 1630. 130. 32.2 + 43.4881 0.5 1. 1630. 130. 32.2 8.7 - 43.5960 1. 1. 72. 28. + 43.5960 0.5 1. 72. 28. 80.37 1. - 43.8118 3. -1. 6620. 330. 61. + 43.8118 1.5 -1. 6620. 330. 61. 11. - 43.8500 3. -1. 155. 38. + 43.8500 1.5 -1. 155. 38. 80.37 1. - 44.1306 1. 1. 970. 130. 76. + 44.1306 0.5 1. 970. 130. 76. 18. - 44.2600 3. -1. 22.7 9.1 + 44.2600 1.5 -1. 22.7 9.1 80.37 1. - 44.5938 3. -1. 30290. 360. 84. + 44.5938 1.5 -1. 30290. 360. 84. 12. - 45.4852 1. 1. 1470. 130. 33. + 45.4852 0.5 1. 1470. 130. 33. 10. - 45.5432 3. -1. 12380. 350. 162. + 45.5432 1.5 -1. 12380. 350. 162. 17. - 46.4071 3. -1. 116. 39. + 46.4071 1.5 -1. 116. 39. 80.37 1. - 46.6000 1. 1. 34. 13. + 46.6000 0.5 1. 34. 13. 80.37 1. - 46.6956 3. -1. 60. 20. + 46.6956 1.5 -1. 60. 20. 80.37 1. - 47.4697 1. -1. 1570. 160. 47. + 47.4697 0.5 -1. 1570. 160. 47. 14. - 47.5665 1. 1. 6170. 250. 72. + 47.5665 0.5 1. 6170. 250. 72. 20. - 47.6913 1. 1. 7970. 200. 47. + 47.6913 0.5 1. 7970. 200. 47. 14. - 48.1178 1. 1. 3420. 230. 49. + 48.1178 0.5 1. 3420. 230. 49. 14. - 48.3752 3. -1. 5900. 380. 79. + 48.3752 1.5 -1. 5900. 380. 79. 12. - 48.7768 1. -1. 1270. 150. 103. + 48.7768 0.5 -1. 1270. 150. 103. 25. - 49.3018 1. 1. 6140. 220. 26.5 + 49.3018 0.5 1. 6140. 220. 26.5 9.1 - 49.3367 1. 1. 6340. 340. 94. + 49.3367 0.5 1. 6340. 340. 94. 22. - 49.4665 3. -1. 10720. 410. 82. + 49.4665 1.5 -1. 10720. 410. 82. 14. - 50.1199 1. 1. 2600. 240. 83. + 50.1199 0.5 1. 2600. 240. 83. 21. - 50.3709 1. 1. 710. 120. 48. + 50.3709 0.5 1. 710. 120. 48. 14. 1. - 50.4588 1. 1. 5520. 280. 70. + 50.4588 0.5 1. 5520. 280. 70. 18. - 50.6569 3. -1. 5120. 400. 70. + 50.6569 1.5 -1. 5120. 400. 70. 13. - 51.0908 3. -1. 780. 140. 82. + 51.0908 1.5 -1. 780. 140. 82. 17. - 51.3186 3. -1. 5630. 410. 84. + 51.3186 1.5 -1. 5630. 410. 84. 13. - 51.5306 3. -1. 66. 23. + 51.5306 1.5 -1. 66. 23. 80.37 1. - 51.8986 1. 1. 9100. 300. 95. + 51.8986 0.5 1. 9100. 300. 95. 22. - 52.0846 3. -1. 4430. 420. 72. + 52.0846 1.5 -1. 4430. 420. 72. 17. - 52.1338 1. 1. 2180. 270. 99. + 52.1338 0.5 1. 2180. 270. 99. 26. - 52.5100 3. -1. 35. 12. + 52.5100 1.5 -1. 35. 12. 80.37 1. - 52.6808 3. -1. 14570. 440. 76. + 52.6808 1.5 -1. 14570. 440. 76. 13. - 53.0057 3. -1. 2350. 280. 75. + 53.0057 1.5 -1. 2350. 280. 75. 14. - 53.1376 1. 1. 2310. 190. 40. + 53.1376 0.5 1. 2310. 190. 40. 14. - 53.4492 3. -1. 1410. 210. 87. + 53.4492 1.5 -1. 1410. 210. 87. 15. - 53.6553 1. 1. 4770. 290. 73. + 53.6553 0.5 1. 4770. 290. 73. 19. - 54.2225 3. -1. 32320. 440. 51. + 54.2225 1.5 -1. 32320. 440. 51. 12. - 54.4086 1. 1. 26040. 10. 30. + 54.4086 0.5 1. 26040. 10. 30. 10. - 54.9284 1. -1. 1340. 190. 95. + 54.9284 0.5 -1. 1340. 190. 95. 26. 1. ENDDATA 378 ENDSUBENT 395 diff --git a/exforall/139/13917.x4 b/exforall/139/13917.x4 index 7cbcac635..5b91d1d18 100644 --- a/exforall/139/13917.x4 +++ b/exforall/139/13917.x4 @@ -1,15 +1,16 @@ -ENTRY 13917 20050105 -SUBENT 13917001 20050105 -BIB 5 5 +ENTRY 13917 20050720 20050909 1336 +SUBENT 13917001 20050720 20050909 1336 +BIB 5 6 INSTITUTE (1USABNL,2NEDRCN) -REFERENCE (J,NP/A,337,401,197911) +REFERENCE (J,NP/A,337,401,1980) AUTHOR (H.I.Liou,R.E.Chrien,J.Kopecky,J.A.Konter) TITLE Study of the 45Sc(n,gamma) reaction. HISTORY (20050105C) DR -ENDBIB 5 + (20050720C) DR Reference corrected +ENDBIB 6 NOCOMMON 0 0 -ENDSUBENT 8 -SUBENT 13917002 20050105 +ENDSUBENT 9 +SUBENT 13917002 20050105 20050909 1336 BIB 7 9 REACTION (21-SC-45(N,G)21-SC-46,,SPC,,MXW) FACILITY (REAC,2NEDRCN) Circular polarization spectrometer at @@ -19,7 +20,7 @@ DETECTOR (GELI) Two GeLi. detectors 15 % efficiency. SAMPLE Sc2O3 sample of 5g, 99.999 % in 45Sc, packed in a thin cylindrical teflon holder ERR-ANALYS (DATA-ERR) Statistical and systematics uncertainties -STATUS Data taken from table I of the journal article +STATUS Data taken from table I ENDBIB 9 COMMON 1 3 EN-DUMMY @@ -107,7 +108,7 @@ KEV KEV PC/REAC PC/REAC 5055.4 0.8 0.57 0.12 ENDDATA 78 ENDSUBENT 96 -SUBENT 13917003 20050105 +SUBENT 13917003 20050105 20050909 1336 BIB 7 9 REACTION (21-SC-45(N,G)21-SC-46,,SPC,,AV) FACILITY (REAC,1USABNL) 22 m flight path @@ -117,7 +118,7 @@ DETECTOR (GELI) One GeLi. detectors 10 % efficiency, 7 keV FWHM SAMPLE Sc2O3 sample of 27.78g, 99.9 % in 45Sc, 7.62cm x7.62cm in a thin Al container ERR-ANALYS (ERR-S) Statistical uncertainties -STATUS Data taken from table 2 of the journal article +STATUS Data taken from table 2 ENDBIB 9 COMMON 2 3 EN-MIN EN-MAX @@ -185,7 +186,7 @@ KEV KEV PC/REAC PC/REAC 1618.8 0.1 1.7 0.1 ENDDATA 58 ENDSUBENT 76 -SUBENT 13917004 20050105 +SUBENT 13917004 20050105 20050909 1336 BIB 6 8 REACTION (21-SC-45(N,G),,SPC,,RES) FACILITY (REAC,1USABNL) 48 m flight path @@ -194,7 +195,7 @@ DETECTOR (GELI) One GeLi. detectors 10 % efficiency, 7 keV FWHM SAMPLE Sc2O3 sample of 354.2g, 99.9 % in 45Sc, 15.2cm x20.3cm in a thin Al container ERR-ANALYS (DATA-ERR) No information given -STATUS Data taken from table 3 of the journal article +STATUS Data taken from table 3 ENDBIB 8 NOCOMMON 0 0 DATA 4 57 diff --git a/exforall/139/13957.x4 b/exforall/139/13957.x4 index d501d3129..23ae5e594 100644 --- a/exforall/139/13957.x4 +++ b/exforall/139/13957.x4 @@ -1,26 +1,27 @@ -ENTRY 13957 20050124 20050610 1332 -SUBENT 13957001 20050124 20050610 1332 -BIB 7 8 +ENTRY 13957 20050720 20050909 1336 +SUBENT 13957001 20050720 20050909 1336 +BIB 7 9 INSTITUTE (1USAKTY) -REFERENCE (J,PR/C,63,014606,2000) -AUTHOR (Gang Chen,M.Li,J.L.Weil,M.T.McEllistrem) +REFERENCE (J,PR/C,63,014606,2001) +AUTHOR (G.Chen,M.Li,J.L.Weil,M.T.McEllistrem) TITLE Neutron scattering in 140,142Ce and strengths of neutrons and protons in collective levels of 140Ce FACILITY (VDG,1USAKTY) 7.5 MeV neutrons DETECTOR (SCIN) Liquid scintillator NE-218 HISTORY (20050124C) DR -ENDBIB 8 + (20050720C) DR Reference corrected +ENDBIB 9 COMMON 1 3 EN MEV 7.5 ENDCOMMON 3 -ENDSUBENT 15 -SUBENT 13957002 20050124 20050610 1332 +ENDSUBENT 16 +SUBENT 13957002 20050124 20050909 1336 BIB 3 3 REACTION (58-CE-140(N,EL)58-CE-140,,DA) ERR-ANALYS No information given -STATUS (CURVE) Data taken from Fig. 3 of the journal article +STATUS (CURVE) Data taken from Fig. 3 ENDBIB 3 NOCOMMON 0 0 DATA 2 20 @@ -48,11 +49,11 @@ ADEG MB/SR 1.497E+02 1.465E+01 ENDDATA 22 ENDSUBENT 30 -SUBENT 13957003 20050124 20050610 1332 +SUBENT 13957003 20050124 20050909 1336 BIB 3 3 REACTION (58-CE-142(N,EL)58-CE-142,,DA) ERR-ANALYS No information given -STATUS (CURVE) Data taken from Fig. 4 of the journal article +STATUS (CURVE) Data taken from Fig. 4 ENDBIB 3 NOCOMMON 0 0 DATA 2 12 @@ -72,11 +73,11 @@ ADEG MB/SR 1.498E+02 1.767E+01 ENDDATA 14 ENDSUBENT 22 -SUBENT 13957004 20050124 20050610 1332 +SUBENT 13957004 20050124 20050909 1336 BIB 3 3 REACTION (58-CE-140(N,INL)58-CE-140,PAR,DA) ERR-ANALYS (DATA-ERR) No information given -STATUS (CURVE) Data taken from Figs. 5,6 and 7 of the article +STATUS (CURVE) Data taken from Figs. 5,6 and 7 ENDBIB 3 NOCOMMON 0 0 DATA 4 60 diff --git a/exforall/139/13961.x4 b/exforall/139/13961.x4 index 74a55f457..8299d7c5b 100644 --- a/exforall/139/13961.x4 +++ b/exforall/139/13961.x4 @@ -1,8 +1,8 @@ -ENTRY 13961 20050418 20050707 1335 -SUBENT 13961001 20050418 20050707 1335 -BIB 8 11 +ENTRY 13961 20050418 20050909 1336 +SUBENT 13961001 20050418 20050909 1336 +BIB 8 12 INSTITUTE (1USAORL) -REFERENCE (J,NST,2,346,2002) +REFERENCE (J,NSTS,2,346,2002) AUTHOR (K.H.Guber,L.C.Leal,R.O.Sayer,R.R.Spencer,P.E.Koehler, T.E.Valentine,,H.Derrien,J.A.Harvey) TITLE Neutron Cross Sections Measurements for Light Elements @@ -12,15 +12,16 @@ METHOD (TOF) DETECTOR (SCIN) Li6 glass scintillator HISTORY (20050203C) DR (20050418C) DR Entries 3 and 6 divided in subentries -ENDBIB 11 + (20050627C) DR reference NST changed to NSTS +ENDBIB 12 NOCOMMON 0 0 -ENDSUBENT 14 -SUBENT 13961002 20050418 20050707 1335 +ENDSUBENT 15 +SUBENT 13961002 20050418 20050909 1336 BIB 4 4 REACTION (17-CL-35(N,G)17-CL-36,,SIG) SAMPLE Natural CCl4 and high purity samples of Al ERR-ANALYS No information -STATUS Data taken from Table 1 in the journal article. +STATUS Data taken from Table 1 ENDBIB 4 NOCOMMON 0 0 DATA 3 20 @@ -48,12 +49,12 @@ KEV KEV MB 4.5E+02 5.0E+02 1.38 ENDDATA 22 ENDSUBENT 31 -SUBENT 13961003 20050418 20050707 1335 +SUBENT 13961003 20050418 20050909 1336 BIB 4 4 REACTION (17-CL-37(N,G)17-CL-38,,SIG) SAMPLE Natural CCl4 and high purity samples of Al ERR-ANALYS No information -STATUS Data taken from Table 1 in the journal article. +STATUS Data taken from Table 1 ENDBIB 4 NOCOMMON 0 0 DATA 3 20 @@ -81,12 +82,12 @@ KEV KEV MB 4.5E+02 5.0E+02 0.09 ENDDATA 22 ENDSUBENT 31 -SUBENT 13961004 20050418 20050707 1335 +SUBENT 13961004 20050418 20050909 1336 BIB 4 4 REACTION (13-AL-27(N,G)13-AL-28,,SIG) SAMPLE Natural CCl4 and high purity samples of Al ERR-ANALYS No information -STATUS Data taken from Table 1 in the journal article. +STATUS Data taken from Table 1 ENDBIB 4 NOCOMMON 0 0 DATA 3 20 @@ -114,11 +115,11 @@ KEV KEV MB 4.5E+02 5.0E+02 0.22 ENDDATA 22 ENDSUBENT 31 -SUBENT 13961005 20050418 20050707 1335 +SUBENT 13961005 20050418 20050909 1336 BIB 3 3 REACTION (14-SI-28(N,G)14-SI-29,,SIG) ERR-ANALYS No information -STATUS Data taken from Table 2 in the journal article. +STATUS Data taken from Table 2 ENDBIB 3 NOCOMMON 0 0 DATA 3 24 @@ -150,11 +151,11 @@ KEV KEV MB 6.5E+02 7.0E+02 0.02 ENDDATA 26 ENDSUBENT 34 -SUBENT 13961006 20050418 20050707 1335 +SUBENT 13961006 20050418 20050909 1336 BIB 3 3 REACTION (14-SI-29(N,G)14-SI-30,,SIG) ERR-ANALYS No information -STATUS Data taken from Table 2 in the journal article. +STATUS Data taken from Table 2 ENDBIB 3 NOCOMMON 0 0 DATA 3 24 @@ -186,11 +187,11 @@ KEV KEV MB 6.5E+02 7.0E+02 0.38 ENDDATA 26 ENDSUBENT 34 -SUBENT 13961007 20050418 20050707 1335 +SUBENT 13961007 20050418 20050909 1336 BIB 3 3 REACTION (14-SI-30(N,G)14-SI-31,,SIG) ERR-ANALYS No information -STATUS Data taken from Table 2 in the journal article. +STATUS Data taken from Table 2 ENDBIB 3 NOCOMMON 0 0 DATA 3 24 diff --git a/exforall/139/13990.x4 b/exforall/139/13990.x4 index 05909163d..10b33df84 100644 --- a/exforall/139/13990.x4 +++ b/exforall/139/13990.x4 @@ -1,24 +1,25 @@ -ENTRY 13990 20050504 20050707 1335 -SUBENT 13990001 20050504 20050707 1335 -BIB 9 15 -INSTITUTE Science Applications International Corporation, Santa - Clara, CA, USA +ENTRY 13990 20050504 20050909 1336 +SUBENT 13990001 20050504 20050909 1336 +BIB 9 16 +INSTITUTE (1USAUSA) Science Applications International + Corporation, Santa Clara, CA, USA REFERENCE (J,NIM/B,99,505,1995) AUTHOR (J.Bendahan,J.Clayton,K.Fankhauser,T.Gozani, J.Krivicich,R.Loveman,E.Pentaleri,P.Ryge,P.Sawa, J.Stevenson) TITLE Measurements and analysis of carbon and oxygen neutron inelastic cross sections below 10 MeV -FACILITY SAIC Pulse Fast Neutron Analysis experimenal facility +FACILITY SAIC Pulse Fast Neutron Analysis experimenal facility INC-SOURCE (D-D) The deuteron beam had a typical pulse width of about 1.2 ns. DETECTOR (SCIN) Plastic scintillators SAMPLE Carbon and oxygen samples were placed on a goniometer - table. Typically, seven 3 in. X 3 in. + table. Typically, seven 3 in. x 3 in. HISTORY (20050504C) DR -ENDBIB 15 + (20050708C) DR Institute code added +ENDBIB 16 NOCOMMON 0 0 -ENDSUBENT 18 +ENDSUBENT 19 SUBENT 13990002 20050504 20050707 1335 BIB 4 4 REACTION (6-C-0(N,INL)6-C-0,PAR,DA,G) diff --git a/exforall/140/14009.x4 b/exforall/140/14009.x4 new file mode 100644 index 000000000..8d0bab81c --- /dev/null +++ b/exforall/140/14009.x4 @@ -0,0 +1,48 @@ +ENTRY 14009 20050608 20050909 1336 +SUBENT 14009001 20050608 20050909 1336 +BIB 9 10 +INSTITUTE (1USAINU) +REFERENCE (J,NP/A,684,569,2001) +AUTHOR (J.Sowinski) +TITLE Investigation of the three-nucleon force at IUCF +FACILITY (CYCLO,1USAINU) Indiana university cyclotron + facility +INC-SPECT 187 MeV polarized protons +SAMPLE Liquid D2 target +DETECTOR (SCIN) Plastic scintillator +HISTORY (20050608C) DR +ENDBIB 10 +NOCOMMON 0 0 +ENDSUBENT 13 +SUBENT 14009002 20050608 20050909 1336 +BIB 4 4 +REACTION (1-H-2(N,EL)1-H-2,,POL/DA,,ANA) +COMMENT Data presented as preliminary +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Figure 2 +ENDBIB 4 +COMMON 1 3 +EN +MEV +187. +ENDCOMMON 3 +DATA 3 14 +ANG-CM DATA DATA-ERR +ADEG NO-DIM NO-DIM + 5.46E+01 -5.20E-01 1.06E-01 + 5.75E+01 -4.38E-01 + 6.69E+01 -4.27E-01 + 7.05E+01 -3.95E-01 + 7.40E+01 -3.46E-01 + 7.69E+01 -3.13E-01 + 8.07E+01 -2.54E-01 + 8.15E+01 -2.02E-01 + 8.51E+01 -1.65E-01 + 8.89E+01 -1.10E-01 + 9.30E+01 -7.83E-02 8.87E-02 + 1.02E+02 -1.84E-02 + 1.07E+02 2.63E-02 + 1.12E+02 9.82E-02 +ENDDATA 16 +ENDSUBENT 29 +ENDENTRY 2 diff --git a/exforall/140/14010.x4 b/exforall/140/14010.x4 new file mode 100644 index 000000000..a9d9743d0 --- /dev/null +++ b/exforall/140/14010.x4 @@ -0,0 +1,260 @@ +ENTRY 14010 20050627 20050909 1336 +SUBENT 14010001 20050627 20050909 1336 +BIB 9 29 +INSTITUTE (1USALAS) + Massachussets General Hospital, MA, USA +REFERENCE (J,NIM/B,234,419,2005) +AUTHOR (J.M.Sisterson,J.Ullmann) +TITLE Measurements of energy integrated cross sections for + reactions producing relatively short-lived + radionuclides using neutron beams with an energy range + of 0.1-750 MeV +FACILITY (LINAC,1USALAS) WNR Facility at the LANSCE accelerator +METHOD (TOF) + Non-destructive gamma-ray spectroscopy +SAMPLE Target Thickness (cm) Purity (%) Weight (g) + C 0.1 99.95 0.32 + SiO2 0.3 99.9 16.6 + Mg 0.3 99.9 13.0 + Al 0.1 99.999 0.46 + 0.1 99.999 6.8 + Si 0.1 99.999 4.6 + Ti 0.1 99.6 0.74 + Fe 0.05 99.5 0.7 + 0.1 99.99+ 20.44 + Ni 0.1 99.98 1.52 + 0.1 99.98 22.43 + Cu 0.1 99.99+ 1.59 + Au 0.025 99.95 0.91 +DETECTOR (GE-IN) High purity Ge detectors plus pulse height + analyzers with computer data acquisition systems were + used to collect the gamma-ray spectra for gamma rays + with energies in the range 0-3 MeV. +HISTORY (20050627C) DR +ENDBIB 29 +NOCOMMON 0 0 +ENDSUBENT 32 +SUBENT 14010002 20050627 20050909 1336 +BIB 3 3 +REACTION (6-C-0(N,X)4-BE-7,,SIG,,AV) +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 1 +EN-MIN EN-MAX DATA DATA-ERR +MEV MEV MB MB +2.5 750. 7.1 0.8 +ENDDATA 3 +ENDSUBENT 11 +SUBENT 14010003 20050627 20050909 1336 +BIB 4 4 +REACTION (14-SI-OXI(N,X)ELEM/MASS,,SIG,,AV) +SAMPLE SiO2 +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 4 +ENDBIB 4 +NOCOMMON 0 0 +DATA 6 4 +ELEMENT MASS EN-MIN EN-MAX DATA DATA-ERR +NO-DIM NO-DIM MEV MEV MB MB + 4. 7. 2.5 750. 6.7 0.8 +11. 22. 2.5 750. 9.1 1.1 +11. 24. 1.25 750. 6.4 0.8 +11. 24. 2.5 750. 6.9 0.8 +ENDDATA 6 +ENDSUBENT 15 +SUBENT 14010004 20050627 20050909 1336 +BIB 3 3 +REACTION (14-SI-0(N,X)ELEM/MASS,,SIG,,AV) +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 6 4 +ELEMENT MASS EN-MIN EN-MAX DATA DATA-ERR +NO-DIM NO-DIM MEV MEV MB MB + 4. 7. 0.7 750. 1.7 0.4 + 4. 7. 2.5 750. 1.7 0.4 +11. 22. 0.7 750. 9.7 1.2 +11. 24. 0.7 750. 6.4 0.7 +ENDDATA 6 +ENDSUBENT 14 +SUBENT 14010005 20050627 20050909 1336 +BIB 3 3 +REACTION (12-MG-0(N,X)ELEM/MASS,,SIG,,AV) +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 6 3 +ELEMENT MASS EN-MIN EN-MAX DATA DATA-ERR +NO-DIM NO-DIM MEV MEV MB MB + 4. 7. 1.25 750. 1.4 0.2 +11. 22. 1.25 750. 20.4 2.3 +11. 24. 1.25 750. 27.1 3.1 +ENDDATA 5 +ENDSUBENT 13 +SUBENT 14010006 20050627 20050909 1336 +BIB 3 3 +REACTION (13-AL-27(N,X)ELEM/MASS,,SIG,,AV) +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 6 8 +ELEMENT MASS EN-MIN EN-MAX DATA DATA-ERR +NO-DIM NO-DIM MEV MEV MB MB + 4. 7. 0.7 750. 1.3 0.3 + 4. 7. 1.25 750. 1.5 0.2 + 4. 7. 2.5 750. 1.5 0.3 +11. 22. 0.7 750. 9.1 1.1 +11. 22. 1.25 750. 7.7 1.0 +11. 22. 2.5 750. 7.8 1.0 +11. 24. 1.25 750. 23.6 2.7 +11. 24. 2.5 750. 19. 2.2 +ENDDATA 10 +ENDSUBENT 18 +SUBENT 14010007 20050627 20050909 1336 +BIB 3 3 +REACTION (79-AU-197(N,4N)79-AU-194,,SIG,,AV) +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 5 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 3 +EN-MIN EN-MAX DATA DATA-ERR +MEV MEV MB MB +0.7 750. 131. 15. +1.25 750. 113. 13. +2.5 750. 145. 17. +ENDDATA 5 +ENDSUBENT 13 +SUBENT 14010008 20050627 20050909 1336 +BIB 3 3 +REACTION (79-AU-197(N,G)79-AU-198,,SIG,,AV) +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 5 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 3 +EN-MIN EN-MAX DATA DATA-ERR +MEV MEV MB MB +0.7 750. 8.3 1.1 +1.25 750. 15.1 1.8 +2.5 750. 12.7 1.5 +ENDDATA 5 +ENDSUBENT 13 +SUBENT 14010009 20050627 20050909 1336 +BIB 3 3 +REACTION (22-TI-0(N,X)ELEM/MASS,,SIG,,AV) +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 6 +ENDBIB 3 +NOCOMMON 0 0 +DATA 6 2 +ELEMENT MASS EN-MIN EN-MAX DATA DATA-ERR +NO-DIM NO-DIM MEV MEV MB MB +21. 46. 2.5 750. 49.8 5.9 +21. 48. 2.5 750. 9.9 1.1 +ENDDATA 4 +ENDSUBENT 12 +SUBENT 14010010 20050627 20050909 1336 +BIB 3 3 +REACTION (26-FE-0(N,X)ELEM/MASS,,SIG,,AV) +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 6 +ENDBIB 3 +NOCOMMON 0 0 +DATA 6 6 +ELEMENT MASS EN-MIN EN-MAX DATA DATA-ERR +NO-DIM NO-DIM MEV MEV MB MB +21. 46. 2.5 750. 4.3 0.6 +21. 48. 2.5 750. 0.34 0.05 +23. 48. 2.5 750. 10.0 1.1 +24. 51. 2.5 750. 40.4 4.6 +25. 52. 2.5 750. 9.6 1.1 +25. 54. 2.5 750. 69.7 8.0 +ENDDATA 8 +ENDSUBENT 16 +SUBENT 14010011 20050627 20050909 1336 +BIB 4 5 +REACTION (28-NI-0(N,X)ELEM/MASS,,SIG,,AV) +COMMENT Co56 and Co57 cross sections are from a cumulative + measurement +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 6 +ENDBIB 5 +NOCOMMON 0 0 +DATA 6 36 +ELEMENT MASS EN-MIN EN-MAX DATA DATA-ERR +NO-DIM NO-DIM MEV MEV MB MB +21. 46. 0.7 750. 1.7 0.2 +21. 46. 1.25 750. 1.4 0.2 +21. 46. 2.5 750. 1.5 0.2 +23. 48. 0.7 750. 6.7 0.8 +23. 48. 1.25 750. 5.8 0.7 +23. 48. 2.5 750. 7.1 0.8 +24. 51. 0.7 750. 33.2 3.8 +24. 51. 1.25 750. 24.7 2.8 +24. 51. 2.5 750. 23.0 2.6 +25. 52. 0.7 750. 12.4 1.4 +25. 52. 1.25 750. 7.7 0.9 +25. 52. 2.5 750. 8.9 1.0 +25. 54. 0.7 750. 23.2 4.4 +25. 54. 1.25 750. 17.5 2.3 +25. 54. 2.5 750. 16.5 2.3 +26. 59. 0.7 750. 0.9 0.2 +26. 59. 1.25 750. 0.6 0.1 +26. 59. 2.5 750. 0.5 0.1 +27. 56. 0.7 750. 42.1 4.8 +27. 56. 1.25 750. 29.4 3.3 +27. 56. 2.5 750. 31.4 3.6 +27. 57. 0.7 750. 200.0 22.7 +27. 57. 1.25 750. 130.0 15.0 +27. 57. 2.5 750. 159.0 18.0 +27. 58. 0.7 750. 183.0 20.8 +27. 58. 1.25 750. 110.0 13.1 +27. 58. 2.5 750. 130.0 14.8 +27. 60. 0.7 750. 9.2 1.3 +27. 60. 1.25 750. 6.5 0.8 +27. 60. 2.5 750. 7.0 0.9 +28. 56. 0.7 750. 2.5 0.3 +28. 56. 1.25 750. 1.3 0.2 +28. 56. 2.5 750. 1.4 0.3 +28. 57. 0.7 750. 22.9 2.6 +28. 57. 1.25 750. 15.6 1.8 +28. 57. 2.5 750. 16.6 1.9 +ENDDATA 38 +ENDSUBENT 48 +SUBENT 14010012 20050627 20050909 1336 +BIB 4 5 +REACTION (29-CU-0(N,X)ELEM/MASS,,SIG,,AV) +COMMENT Co56 and Co57 cross sections are from a cumulative + measurement +ERR-ANALYS (DATA-ERR) No information +STATUS Data taken from Table 6 +ENDBIB 5 +NOCOMMON 0 0 +DATA 6 17 +ELEMENT MASS EN-MIN EN-MAX DATA DATA-ERR +NO-DIM NO-DIM MEV MEV MB MB +21. 46. 0.7 750. 1.2 0.2 +21. 46. 1.25 750. 1.0 0.1 +23. 48. 1.25 750. 14.9 1.7 +24. 51. 0.7 750. 12.8 2.2 +24. 51. 1.25 750. 8.2 0.9 +25. 52. 0.7 750. 3.5 0.4 +25. 52. 1.25 750. 1.7 0.2 +25. 54. 0.7 750. 16.0 2.4 +25. 54. 1.25 750. 9.8 1.2 +26. 59. 0.7 750. 3.9 0.6 +26. 59. 1.25 750. 2.2 0.2 +27. 56. 1.25 750. 3.4 0.4 +27. 57. 1.25 750. 19.2 2.3 +27. 58. 1.25 750. 28.4 3.2 +27. 59. 1.25 750. 14.5 1.7 +28. 57. 0.7 750. 0.5 0.1 +28. 57. 1.25 750. 0.3 0.04 +ENDDATA 19 +ENDSUBENT 29 +ENDENTRY 12 diff --git a/exforall/140/14011.x4 b/exforall/140/14011.x4 new file mode 100644 index 000000000..519936a54 --- /dev/null +++ b/exforall/140/14011.x4 @@ -0,0 +1,718 @@ +ENTRY 14011 20050629 20050909 1336 +SUBENT 14011001 20050629 20050909 1336 +BIB 9 11 +INSTITUTE (1USALAS,1USANIS,1USAORL) +REFERENCE (C,91JUELIC,,732,1991) +AUTHOR (P.W.Lisowski,A.Gavron,W.E.Parker,S.J.Balestrini, + A.D.Carlson,O.A.Wasson,N.W.Hill) +TITLE Fission cross sections ratios for 233, 234,236U + relative to 235U from 0.5 to 400 MeV +FACILITY (LINAC,1USALAS) LANSCE Linac and WNR facility +SAMPLE Different foils of 234,235,236 and 238U +METHOD (TOF) +DETECTOR (IOCH) Fission ionization chamber +HISTORY (20050629C) DR +ENDBIB 11 +NOCOMMON 0 0 +ENDSUBENT 14 +SUBENT 14011002 20050629 20050909 1336 +BIB 3 3 +REACTION ((92-U-238(N,F),,SIG)/(92-U-235(N,F),,SIG)) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 137 +EN DATA DATA-ERR +MEV NO-DIM NO-DIM + 1.44E+00 1.26E-01 + 1.49E+00 1.91E-01 + 1.53E+00 2.50E-01 + 1.58E+00 2.80E-01 + 1.62E+00 3.04E-01 + 1.67E+00 3.30E-01 + 1.72E+00 3.51E-01 + 1.77E+00 3.65E-01 + 1.84E+00 3.81E-01 + 1.93E+00 4.07E-01 + 2.05E+00 4.09E-01 + 2.11E+00 4.28E-01 + 2.18E+00 4.40E-01 + 2.25E+00 4.28E-01 + 2.37E+00 4.36E-01 + 2.51E+00 4.38E-01 + 2.67E+00 4.24E-01 + 2.81E+00 4.42E-01 + 2.99E+00 4.27E-01 + 3.11E+00 4.45E-01 + 3.29E+00 4.47E-01 + 3.43E+00 4.55E-01 + 3.59E+00 4.63E-01 + 3.77E+00 4.72E-01 + 3.88E+00 4.86E-01 + 4.09E+00 4.74E-01 + 4.20E+00 4.94E-01 + 4.45E+00 4.94E-01 + 4.73E+00 5.23E-01 + 4.90E+00 5.15E-01 + 5.04E+00 5.03E-01 + 5.30E+00 5.15E-01 + 5.58E+00 5.23E-01 + 5.81E+00 5.35E-01 + 6.04E+00 5.47E-01 + 6.32E+00 5.58E-01 + 6.43E+00 5.76E-01 + 6.65E+00 6.04E-01 + 6.92E+00 6.18E-01 + 7.20E+00 6.16E-01 + 7.62E+00 5.96E-01 + 7.93E+00 5.70E-01 + 8.25E+00 5.62E-01 + 8.73E+00 5.62E-01 + 9.13E+00 5.71E-01 + 9.50E+00 5.67E-01 + 9.83E+00 5.85E-01 + 1.04E+01 5.77E-01 + 1.10E+01 5.69E-01 + 1.15E+01 5.79E-01 + 1.21E+01 5.94E-01 + 1.27E+01 5.76E-01 + 1.33E+01 5.46E-01 + 1.37E+01 5.30E-01 + 1.43E+01 5.44E-01 + 1.47E+01 5.60E-01 + 1.51E+01 5.86E-01 + 1.53E+01 5.64E-01 + 1.58E+01 6.00E-01 + 1.64E+01 6.07E-01 + 1.74E+01 6.35E-01 + 1.81E+01 6.33E-01 + 1.86E+01 6.45E-01 + 1.89E+01 6.63E-01 + 1.96E+01 6.43E-01 + 1.99E+01 6.90E-01 + 2.08E+01 6.86E-01 + 2.14E+01 7.10E-01 + 2.20E+01 7.22E-01 + 2.28E+01 7.38E-01 + 2.40E+01 7.41E-01 + 2.48E+01 7.27E-01 + 2.54E+01 7.53E-01 + 2.64E+01 7.51E-01 + 2.73E+01 7.39E-01 + 2.86E+01 7.43E-01 + 2.96E+01 7.63E-01 + 3.08E+01 7.65E-01 + 3.19E+01 7.78E-01 + 3.28E+01 7.94E-01 + 3.37E+01 8.06E-01 + 3.57E+01 7.86E-01 + 3.73E+01 8.06E-01 + 3.91E+01 8.30E-01 + 4.06E+01 8.29E-01 + 4.18E+01 8.41E-01 + 4.33E+01 8.49E-01 + 4.40E+01 8.27E-01 + 4.58E+01 8.53E-01 + 4.76E+01 8.61E-01 + 5.01E+01 8.45E-01 + 5.27E+01 8.45E-01 + 5.46E+01 8.62E-01 + 5.84E+01 8.64E-01 + 6.11E+01 8.78E-01 + 6.50E+01 8.60E-01 + 6.92E+01 8.40E-01 + 7.16E+01 8.58E-01 + 7.41E+01 8.77E-01 + 7.45E+01 8.52E-01 + 7.89E+01 8.71E-01 + 8.25E+01 8.79E-01 + 8.63E+01 8.73E-01 + 9.35E+01 8.83E-01 + 9.84E+01 8.85E-01 + 1.04E+02 8.84E-01 + 1.06E+02 9.12E-01 + 1.09E+02 8.88E-01 + 1.15E+02 8.62E-01 + 1.20E+02 8.84E-01 + 1.26E+02 9.00E-01 + 1.33E+02 8.84E-01 + 1.40E+02 8.86E-01 + 1.48E+02 8.95E-01 + 1.59E+02 8.87E-01 + 1.69E+02 8.87E-01 + 1.80E+02 9.03E-01 + 1.91E+02 8.95E-01 + 1.99E+02 8.83E-01 + 2.07E+02 9.20E-01 + 2.13E+02 8.61E-01 + 2.18E+02 8.92E-01 + 2.24E+02 9.14E-01 + 2.39E+02 8.90E-01 + 2.51E+02 8.96E-01 + 2.68E+02 9.08E-01 + 2.83E+02 8.78E-01 + 2.93E+02 8.95E-01 + 3.05E+02 9.37E-01 3.18E-02 + 3.15E+02 9.01E-01 + 3.30E+02 9.01E-01 + 3.45E+02 8.53E-01 3.57E-02 + 3.63E+02 9.13E-01 + 3.63E+02 8.81E-01 + 3.80E+02 9.72E-01 4.57E-02 + 3.93E+02 9.05E-01 + 4.05E+02 7.97E-01 4.76E-02 +ENDDATA 139 +ENDSUBENT 147 +SUBENT 14011003 20050629 20050909 1336 +BIB 3 3 +REACTION ((92-U-236(N,F),,SIG)/(92-U-235(N,F),,SIG)) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 177 +EN DATA DATA-ERR +MEV NO-DIM NO-DIM + 7.67E-01 7.62E-02 + 7.89E-01 9.24E-02 + 8.07E-01 1.34E-01 + 8.39E-01 1.41E-01 + 8.63E-01 1.53E-01 + 8.83E-01 1.87E-01 + 9.13E-01 2.34E-01 + 9.38E-01 2.84E-01 + 9.76E-01 2.90E-01 + 1.02E+00 2.84E-01 + 1.06E+00 3.07E-01 + 1.09E+00 3.53E-01 + 1.12E+00 3.92E-01 + 1.15E+00 4.42E-01 + 1.18E+00 4.67E-01 + 1.22E+00 5.03E-01 + 1.26E+00 5.66E-01 + 1.29E+00 5.54E-01 + 1.34E+00 5.68E-01 + 1.40E+00 5.66E-01 + 1.42E+00 5.78E-01 + 1.47E+00 5.52E-01 + 1.52E+00 5.26E-01 + 1.55E+00 5.13E-01 + 1.60E+00 5.34E-01 + 1.64E+00 5.50E-01 + 1.70E+00 5.80E-01 + 1.73E+00 5.64E-01 + 1.80E+00 5.80E-01 + 1.87E+00 5.86E-01 + 1.95E+00 5.95E-01 + 2.02E+00 6.29E-01 + 2.11E+00 6.35E-01 + 2.19E+00 6.49E-01 + 2.32E+00 6.53E-01 + 2.41E+00 6.58E-01 + 2.52E+00 6.58E-01 + 2.63E+00 6.47E-01 + 2.72E+00 6.58E-01 + 2.81E+00 6.70E-01 + 2.89E+00 6.84E-01 + 2.99E+00 6.98E-01 + 3.08E+00 6.88E-01 + 3.18E+00 7.06E-01 + 3.35E+00 7.10E-01 + 3.50E+00 7.14E-01 + 3.64E+00 7.25E-01 + 3.73E+00 7.35E-01 + 3.88E+00 7.43E-01 + 4.03E+00 7.43E-01 + 4.20E+00 7.37E-01 + 4.29E+00 7.21E-01 + 4.46E+00 7.57E-01 + 4.62E+00 7.53E-01 + 4.81E+00 7.57E-01 + 5.00E+00 7.45E-01 + 5.17E+00 7.53E-01 + 5.29E+00 7.71E-01 + 5.47E+00 7.76E-01 + 5.66E+00 7.98E-01 + 5.82E+00 8.02E-01 + 5.99E+00 8.12E-01 + 6.27E+00 8.18E-01 + 6.55E+00 8.51E-01 + 6.78E+00 8.67E-01 + 6.93E+00 8.91E-01 + 7.21E+00 8.65E-01 + 7.46E+00 8.59E-01 + 7.59E+00 8.75E-01 + 7.94E+00 8.37E-01 + 8.22E+00 8.53E-01 + 8.70E+00 8.35E-01 + 8.95E+00 8.45E-01 + 9.26E+00 8.24E-01 + 9.57E+00 8.29E-01 + 1.00E+01 8.29E-01 + 1.05E+01 8.08E-01 + 1.10E+01 8.14E-01 + 1.14E+01 8.17E-01 + 1.18E+01 8.02E-01 + 1.21E+01 8.11E-01 + 1.25E+01 7.74E-01 + 1.30E+01 7.58E-01 + 1.33E+01 7.38E-01 + 1.38E+01 7.28E-01 + 1.40E+01 7.20E-01 + 1.45E+01 7.52E-01 + 1.52E+01 7.64E-01 + 1.59E+01 8.15E-01 + 1.69E+01 8.25E-01 + 1.79E+01 8.29E-01 + 1.90E+01 8.51E-01 + 1.97E+01 8.57E-01 + 2.05E+01 8.49E-01 + 2.13E+01 8.70E-01 + 2.20E+01 8.96E-01 + 2.28E+01 8.96E-01 + 2.35E+01 8.90E-01 + 2.47E+01 8.84E-01 + 2.57E+01 9.00E-01 + 2.73E+01 8.90E-01 + 2.83E+01 9.00E-01 + 2.94E+01 8.94E-01 + 3.08E+01 8.92E-01 + 3.24E+01 8.88E-01 + 3.39E+01 8.80E-01 + 3.51E+01 9.04E-01 + 3.59E+01 8.88E-01 + 3.71E+01 9.17E-01 + 3.91E+01 9.11E-01 + 4.04E+01 9.37E-01 + 4.16E+01 9.23E-01 + 4.30E+01 9.13E-01 + 4.52E+01 9.13E-01 + 4.71E+01 9.15E-01 + 4.95E+01 9.25E-01 + 5.04E+01 9.15E-01 + 5.24E+01 9.01E-01 + 5.42E+01 9.15E-01 + 5.45E+01 9.31E-01 + 5.61E+01 9.11E-01 + 5.77E+01 9.41E-01 + 5.94E+01 9.27E-01 + 6.18E+01 9.13E-01 + 6.46E+01 9.31E-01 + 6.65E+01 9.17E-01 + 6.87E+01 9.43E-01 + 6.99E+01 9.25E-01 + 7.32E+01 9.17E-01 + 7.70E+01 9.25E-01 + 7.97E+01 9.11E-01 + 8.24E+01 9.07E-01 + 8.52E+01 9.29E-01 + 8.67E+01 9.50E-01 + 9.02E+01 9.37E-01 + 9.28E+01 9.11E-01 + 9.44E+01 9.31E-01 + 9.87E+01 9.31E-01 + 1.02E+02 9.11E-01 + 1.05E+02 9.25E-01 + 1.08E+02 9.34E-01 + 1.10E+02 9.19E-01 + 1.13E+02 9.46E-01 + 1.16E+02 9.32E-01 + 1.21E+02 9.30E-01 + 1.26E+02 9.34E-01 + 1.31E+02 9.40E-01 + 1.35E+02 9.32E-01 + 1.38E+02 9.48E-01 + 1.43E+02 9.26E-01 + 1.44E+02 9.40E-01 + 1.50E+02 9.48E-01 + 1.55E+02 9.34E-01 + 1.59E+02 9.22E-01 + 1.62E+02 9.12E-01 + 1.70E+02 9.18E-01 + 1.78E+02 9.34E-01 + 1.85E+02 9.46E-01 + 1.90E+02 9.32E-01 + 1.96E+02 9.24E-01 + 2.00E+02 9.08E-01 + 2.06E+02 9.30E-01 + 2.20E+02 9.30E-01 + 2.31E+02 9.30E-01 + 2.48E+02 9.26E-01 + 2.55E+02 9.38E-01 2.42E-02 + 2.67E+02 9.18E-01 + 2.81E+02 8.74E-01 3.23E-02 + 2.89E+02 9.02E-01 2.83E-02 + 3.00E+02 9.14E-01 + 3.14E+02 8.88E-01 + 3.27E+02 9.16E-01 3.44E-02 + 3.37E+02 8.92E-01 + 3.50E+02 8.74E-01 + 3.68E+02 8.82E-01 + 3.79E+02 9.24E-01 3.84E-02 + 3.97E+02 9.04E-01 3.64E-02 +ENDDATA 179 +ENDSUBENT 187 +SUBENT 14011004 20050629 20050909 1336 +BIB 3 3 +REACTION ((92-U-234(N,F),,SIG)/(92-U-235(N,F),,SIG)) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 168 +EN DATA DATA-ERR +MEV NO-DIM NO-DIM + 6.25E-01 7.50E-01 2.39E-02 + 6.47E-01 8.20E-01 1.99E-02 + 6.62E-01 8.78E-01 1.59E-02 + 6.81E-01 8.98E-01 2.19E-02 + 7.05E-01 1.00E+00 2.19E-02 + 7.21E-01 1.02E+00 2.19E-02 + 7.46E-01 1.11E+00 1.99E-02 + 7.68E-01 1.19E+00 1.79E-02 + 7.85E-01 1.26E+00 1.99E-02 + 8.08E-01 1.21E+00 1.59E-02 + 8.36E-01 1.18E+00 1.59E-02 + 8.59E-01 1.13E+00 1.39E-02 + 8.89E-01 1.09E+00 1.99E-02 + 9.09E-01 1.02E+00 + 9.46E-01 9.89E-01 + 9.95E-01 9.61E-01 + 1.01E+00 9.41E-01 + 1.05E+00 1.02E+00 + 1.09E+00 1.04E+00 + 1.12E+00 1.05E+00 + 1.18E+00 1.04E+00 + 1.22E+00 1.05E+00 + 1.26E+00 1.07E+00 + 1.32E+00 1.08E+00 + 1.37E+00 1.11E+00 + 1.42E+00 1.12E+00 + 1.45E+00 1.14E+00 + 1.53E+00 1.13E+00 + 1.54E+00 1.18E+00 + 1.59E+00 1.22E+00 + 1.63E+00 1.22E+00 + 1.69E+00 1.24E+00 + 1.73E+00 1.24E+00 + 1.79E+00 1.25E+00 + 1.85E+00 1.21E+00 + 1.92E+00 1.23E+00 + 1.95E+00 1.22E+00 + 2.00E+00 1.24E+00 + 2.06E+00 1.20E+00 + 2.17E+00 1.20E+00 + 2.28E+00 1.19E+00 + 2.30E+00 1.21E+00 + 2.42E+00 1.21E+00 + 2.53E+00 1.22E+00 + 2.62E+00 1.25E+00 + 2.69E+00 1.25E+00 + 2.83E+00 1.25E+00 + 2.91E+00 1.27E+00 + 2.95E+00 1.28E+00 + 3.05E+00 1.29E+00 + 3.17E+00 1.30E+00 + 3.30E+00 1.29E+00 + 3.44E+00 1.29E+00 + 3.62E+00 1.29E+00 + 3.74E+00 1.30E+00 + 3.89E+00 1.30E+00 + 3.94E+00 1.28E+00 + 4.05E+00 1.31E+00 + 4.12E+00 1.30E+00 + 4.28E+00 1.28E+00 + 4.41E+00 1.29E+00 + 4.56E+00 1.27E+00 + 4.69E+00 1.29E+00 + 4.85E+00 1.29E+00 + 4.99E+00 1.26E+00 + 5.25E+00 1.28E+00 + 5.47E+00 1.30E+00 + 5.62E+00 1.31E+00 + 5.78E+00 1.29E+00 + 6.02E+00 1.28E+00 + 6.19E+00 1.23E+00 + 6.33E+00 1.21E+00 + 6.74E+00 1.20E+00 + 7.05E+00 1.23E+00 + 7.38E+00 1.23E+00 + 7.63E+00 1.25E+00 + 7.94E+00 1.26E+00 + 8.31E+00 1.26E+00 + 8.65E+00 1.26E+00 + 8.94E+00 1.27E+00 + 9.15E+00 1.24E+00 + 9.52E+00 1.24E+00 + 9.90E+00 1.24E+00 + 1.03E+01 1.23E+00 + 1.08E+01 1.22E+00 + 1.11E+01 1.21E+00 + 1.18E+01 1.20E+00 + 1.21E+01 1.18E+00 + 1.25E+01 1.15E+00 + 1.29E+01 1.13E+00 + 1.33E+01 1.08E+00 + 1.37E+01 1.02E+00 + 1.43E+01 1.02E+00 + 1.46E+01 1.03E+00 + 1.53E+01 1.04E+00 + 1.60E+01 1.07E+00 + 1.63E+01 1.10E+00 + 1.70E+01 1.10E+00 + 1.79E+01 1.10E+00 + 1.90E+01 1.13E+00 + 1.99E+01 1.12E+00 + 2.07E+01 1.12E+00 + 2.16E+01 1.10E+00 + 2.22E+01 1.11E+00 + 2.28E+01 1.08E+00 + 2.40E+01 1.08E+00 + 2.56E+01 1.09E+00 + 2.69E+01 1.09E+00 + 2.85E+01 1.10E+00 + 2.93E+01 1.07E+00 + 3.07E+01 1.07E+00 + 3.19E+01 1.06E+00 + 3.34E+01 1.06E+00 + 3.47E+01 1.05E+00 + 3.65E+01 1.06E+00 + 3.85E+01 1.06E+00 + 4.07E+01 1.07E+00 + 4.21E+01 1.06E+00 + 4.38E+01 1.06E+00 + 4.61E+01 1.06E+00 + 4.85E+01 1.07E+00 + 5.05E+01 1.07E+00 + 5.31E+01 1.05E+00 + 5.49E+01 1.07E+00 + 5.65E+01 1.05E+00 + 5.68E+01 1.08E+00 + 5.95E+01 1.08E+00 + 6.15E+01 1.04E+00 + 6.15E+01 1.06E+00 + 6.55E+01 1.06E+00 + 6.74E+01 1.06E+00 + 7.01E+01 1.07E+00 + 7.54E+01 1.04E+00 + 7.98E+01 1.05E+00 + 8.26E+01 1.06E+00 + 8.59E+01 1.07E+00 + 8.99E+01 1.07E+00 + 9.57E+01 1.06E+00 + 1.00E+02 1.06E+00 + 1.05E+02 1.05E+00 + 1.12E+02 1.04E+00 + 1.15E+02 1.05E+00 + 1.21E+02 1.04E+00 + 1.32E+02 1.07E+00 + 1.40E+02 1.06E+00 + 1.48E+02 1.06E+00 + 1.56E+02 1.06E+00 + 1.63E+02 1.05E+00 + 1.70E+02 1.05E+00 + 1.80E+02 1.04E+00 + 1.87E+02 1.05E+00 + 1.96E+02 1.05E+00 + 2.10E+02 1.03E+00 1.39E-02 + 2.15E+02 1.07E+00 1.59E-02 + 2.24E+02 1.03E+00 + 2.40E+02 1.04E+00 2.19E-02 + 2.53E+02 1.03E+00 2.19E-02 + 2.59E+02 1.05E+00 2.39E-02 + 2.66E+02 1.02E+00 + 2.74E+02 1.01E+00 + 2.86E+02 1.02E+00 + 3.05E+02 1.04E+00 2.79E-02 + 3.23E+02 1.04E+00 2.79E-02 + 3.43E+02 1.00E+00 2.19E-02 + 3.61E+02 1.01E+00 + 3.74E+02 1.04E+00 3.79E-02 + 3.84E+02 1.00E+00 + 3.95E+02 9.26E-01 3.19E-02 +ENDDATA 170 +ENDSUBENT 178 +SUBENT 14011005 20050629 20050909 1336 +BIB 3 3 +REACTION ((92-U-233(N,F),,SIG)/(92-U-235(N,F),,SIG)) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 170 +EN DATA DATA-ERR +MEV NO-DIM NO-DIM + 5.83E-01 1.82E+00 4.23E-02 + 6.24E-01 1.76E+00 3.63E-02 + 6.61E-01 1.75E+00 3.83E-02 + 6.80E-01 1.68E+00 2.82E-02 + 6.99E-01 1.74E+00 2.42E-02 + 7.15E-01 1.75E+00 2.61E-02 + 7.49E-01 1.70E+00 2.22E-02 + 7.83E-01 1.71E+00 3.22E-02 + 8.29E-01 1.70E+00 2.82E-02 + 8.63E-01 1.67E+00 2.42E-02 + 8.83E-01 1.62E+00 2.21E-02 + 9.04E-01 1.59E+00 1.81E-02 + 9.56E-01 1.61E+00 2.62E-02 + 9.78E-01 1.59E+00 2.21E-02 + 1.01E+00 1.58E+00 + 1.05E+00 1.58E+00 + 1.10E+00 1.59E+00 + 1.14E+00 1.60E+00 + 1.18E+00 1.57E+00 + 1.22E+00 1.58E+00 + 1.26E+00 1.59E+00 + 1.32E+00 1.58E+00 + 1.35E+00 1.61E+00 + 1.39E+00 1.58E+00 + 1.48E+00 1.57E+00 + 1.54E+00 1.58E+00 + 1.56E+00 1.59E+00 + 1.62E+00 1.56E+00 + 1.67E+00 1.56E+00 + 1.75E+00 1.55E+00 + 1.82E+00 1.55E+00 + 1.85E+00 1.57E+00 + 1.94E+00 1.57E+00 + 1.98E+00 1.58E+00 + 2.06E+00 1.54E+00 + 2.13E+00 1.57E+00 + 2.29E+00 1.57E+00 + 2.39E+00 1.55E+00 + 2.46E+00 1.57E+00 + 2.57E+00 1.56E+00 + 2.69E+00 1.55E+00 + 2.80E+00 1.57E+00 + 2.90E+00 1.58E+00 + 3.03E+00 1.58E+00 + 3.12E+00 1.58E+00 + 3.27E+00 1.57E+00 + 3.42E+00 1.58E+00 + 3.56E+00 1.56E+00 + 3.68E+00 1.53E+00 + 3.83E+00 1.54E+00 + 4.05E+00 1.55E+00 + 4.24E+00 1.49E+00 + 4.42E+00 1.51E+00 + 4.57E+00 1.52E+00 + 4.73E+00 1.52E+00 + 5.00E+00 1.50E+00 + 5.18E+00 1.48E+00 + 5.35E+00 1.52E+00 + 5.67E+00 1.54E+00 + 5.86E+00 1.57E+00 + 6.06E+00 1.57E+00 + 6.24E+00 1.56E+00 + 6.42E+00 1.51E+00 + 6.68E+00 1.48E+00 + 6.80E+00 1.42E+00 + 7.08E+00 1.41E+00 + 7.32E+00 1.35E+00 + 7.54E+00 1.33E+00 + 7.75E+00 1.34E+00 + 8.16E+00 1.31E+00 + 8.54E+00 1.34E+00 + 8.54E+00 1.32E+00 + 8.93E+00 1.35E+00 + 9.24E+00 1.30E+00 + 9.62E+00 1.32E+00 + 1.01E+01 1.34E+00 + 1.03E+01 1.32E+00 + 1.08E+01 1.33E+00 + 1.11E+01 1.34E+00 + 1.15E+01 1.33E+00 + 1.20E+01 1.31E+00 + 1.24E+01 1.28E+00 + 1.29E+01 1.27E+00 + 1.32E+01 1.23E+00 + 1.37E+01 1.22E+00 + 1.42E+01 1.18E+00 + 1.46E+01 1.18E+00 + 1.51E+01 1.15E+00 + 1.59E+01 1.16E+00 + 1.67E+01 1.18E+00 + 1.76E+01 1.18E+00 + 1.85E+01 1.18E+00 + 1.93E+01 1.19E+00 + 2.04E+01 1.18E+00 + 2.10E+01 1.16E+00 + 2.15E+01 1.17E+00 + 2.25E+01 1.15E+00 + 2.41E+01 1.13E+00 + 2.56E+01 1.13E+00 + 2.68E+01 1.11E+00 + 2.76E+01 1.14E+00 + 2.85E+01 1.12E+00 + 2.95E+01 1.09E+00 + 3.02E+01 1.14E+00 + 3.14E+01 1.10E+00 + 3.25E+01 1.09E+00 + 3.44E+01 1.10E+00 + 3.52E+01 1.09E+00 + 3.69E+01 1.10E+00 + 3.88E+01 1.10E+00 + 3.99E+01 1.09E+00 + 4.18E+01 1.10E+00 + 4.30E+01 1.11E+00 + 4.47E+01 1.10E+00 + 4.65E+01 1.08E+00 + 4.89E+01 1.11E+00 + 5.09E+01 1.09E+00 + 5.24E+01 1.08E+00 + 5.45E+01 1.10E+00 + 5.80E+01 1.11E+00 + 6.04E+01 1.10E+00 + 6.21E+01 1.09E+00 + 6.61E+01 1.12E+00 + 6.73E+01 1.08E+00 + 7.04E+01 1.10E+00 + 7.49E+01 1.10E+00 + 7.58E+01 1.09E+00 + 7.97E+01 1.10E+00 + 8.30E+01 1.09E+00 + 8.73E+01 1.11E+00 + 9.14E+01 1.08E+00 + 9.72E+01 1.07E+00 + 1.04E+02 1.08E+00 + 1.10E+02 1.09E+00 + 1.15E+02 1.09E+00 + 1.22E+02 1.09E+00 + 1.27E+02 1.08E+00 + 1.32E+02 1.09E+00 + 1.35E+02 1.08E+00 + 1.39E+02 1.10E+00 + 1.43E+02 1.08E+00 + 1.48E+02 1.07E+00 + 1.52E+02 1.09E+00 + 1.58E+02 1.07E+00 + 1.65E+02 1.07E+00 + 1.71E+02 1.06E+00 + 1.76E+02 1.09E+00 + 1.88E+02 1.07E+00 + 1.96E+02 1.07E+00 + 2.06E+02 1.04E+00 2.01E-02 + 2.13E+02 1.07E+00 2.01E-02 + 2.18E+02 1.09E+00 1.81E-02 + 2.28E+02 1.08E+00 + 2.38E+02 1.07E+00 + 2.47E+02 1.08E+00 + 2.53E+02 1.09E+00 + 2.60E+02 1.07E+00 + 2.69E+02 1.04E+00 2.82E-02 + 2.79E+02 1.07E+00 2.01E-02 + 2.88E+02 1.04E+00 2.21E-02 + 2.95E+02 1.06E+00 2.62E-02 + 3.07E+02 1.06E+00 2.21E-02 + 3.23E+02 1.07E+00 + 3.25E+02 1.04E+00 + 3.34E+02 1.07E+00 3.83E-02 + 3.48E+02 1.03E+00 3.23E-02 + 3.54E+02 1.05E+00 3.22E-02 + 3.76E+02 1.08E+00 4.83E-02 + 3.90E+02 1.02E+00 4.43E-02 + 3.98E+02 1.06E+00 5.04E-02 +ENDDATA 172 +ENDSUBENT 180 +ENDENTRY 5 diff --git a/exforall/140/14012.x4 b/exforall/140/14012.x4 new file mode 100644 index 000000000..01ba09aa5 --- /dev/null +++ b/exforall/140/14012.x4 @@ -0,0 +1,109 @@ +ENTRY 14012 20050628 20050909 1336 +SUBENT 14012001 20050628 20050909 1336 +BIB 9 15 +INSTITUTE (1USAORU) +REFERENCE (J,PR/C,71,054322,2005) +AUTHOR (C.L.Duncan,K.S.Krane) +TITLE Neutron capture cross section of 102Pd +FACILITY (REAC,1USAORU) Oregon State TRIGA reactor (OSTR) +METHOD (ACTIV) Three different irradiation facilities: + the thermal column (TC), in-core irradiation tube + (ICIT), and cadmium-lined in-core irradiation tube + (CLICIT) +SAMPLE Samples of 103Pd were produced by irradiating Pd metal + foils (mass 10-100 mg, thickness 0.025 mm) of natural + isotopic abundance (1.02% of 102Pd) +DETECTOR (GE-IN) High-purity Ge detector nominal volume= + 169 cm3, efficiency=35 % compared with NaI at 1332 keV +HISTORY (20050628C) DR +ENDBIB 15 +NOCOMMON 0 0 +ENDSUBENT 18 +SUBENT 14012002 20050628 20050909 1336 +BIB 4 4 +REACTION (46-PD-102(N,G)46-PD-103,,SIG,,MXW) +DECAY-DATA (46-PD-103,17.D) +ERR-ANALYS (ERR-T) Total uncertainties +STATUS Data taken from the text +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN-DUMMY DATA ERR-T +MEV B B + 2.53E-08 1.82 0.20 +ENDDATA 3 +ENDSUBENT 12 +SUBENT 14012003 20050628 20050909 1336 +BIB 4 4 +REACTION (46-PD-108(N,G)46-PD-109,,SIG,,MXW) +DECAY-DATA (46-PD-109-G,13.7D) +ERR-ANALYS (ERR-T) Total uncertainties +STATUS Data taken from the text +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN-DUMMY DATA ERR-T +MEV B B + 2.53E-08 8.5 0.9 +ENDDATA 3 +ENDSUBENT 12 +SUBENT 14012004 20050628 20050909 1336 +BIB 5 5 +REACTION (46-PD-108(N,G)46-PD-109-G,,SIG,,MXW) +DECAY-DATA (46-PD-109-G,13.7D) +ASSUMED (ASSUM1,46-PD-108(N,G)46-PD-109-M,,SIG,,MXW) +ERR-ANALYS (ERR-T) Total uncertainties +STATUS (DEP,14012003) Data taken from the text +ENDBIB 5 +NOCOMMON 0 0 +DATA 4 1 +EN-DUMMY DATA ERR-T ASSUM1 +MEV B B B + 2.53E-08 8.3 0.9 0.183 +ENDDATA 3 +ENDSUBENT 13 +SUBENT 14012005 20050628 20050909 1336 +BIB 4 5 +REACTION (46-PD-102(N,G)46-PD-103,,RI,,RV) + Resonance integral at epithermal flux +DECAY-DATA (46-PD-103,17.D) +ERR-ANALYS (ERR-T) Total uncertainties +STATUS Data taken from the text +ENDBIB 5 +NOCOMMON 0 0 +DATA 3 1 +EN-MAX DATA ERR-T +EV B B +0.5 23. 4. +ENDDATA 3 +ENDSUBENT 13 +SUBENT 14012006 20050628 20050909 1336 +BIB 4 4 +REACTION (46-PD-108(N,G)46-PD-109,,RI,,RV) +DECAY-DATA (46-PD-109-G,13.7D) +ERR-ANALYS (ERR-T) Total uncertainties +STATUS Data taken from the text +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN-MAX DATA ERR-T +MEV B B +0.5 122. 18. +ENDDATA 3 +ENDSUBENT 12 +SUBENT 14012007 20050628 20050909 1336 +BIB 5 5 +REACTION (46-PD-108(N,G)46-PD-109-G,,RI,,RV) +DECAY-DATA (46-PD-109-G,13.7D) +ASSUMED (ASSUM1,46-PD-108(N,G)46-PD-109-M,,SIG,,MXW) +ERR-ANALYS (ERR-T) Total uncertainties +STATUS Data taken from the text +ENDBIB 5 +NOCOMMON 0 0 +DATA 4 1 +EN-MAX DATA ERR-T ASSUM1 +MEV B B B +0.5 120. 18. 0.183 +ENDDATA 3 +ENDSUBENT 13 +ENDENTRY 7 diff --git a/exforall/140/14013.x4 b/exforall/140/14013.x4 new file mode 100644 index 000000000..9e484562b --- /dev/null +++ b/exforall/140/14013.x4 @@ -0,0 +1,47 @@ +ENTRY 14013 20050628 20050909 1336 +SUBENT 14013001 20050628 20050909 1336 +BIB 8 16 +INSTITUTE (1USAKTY,2GERKLN,1USASTB) +REFERENCE (J,PR/C,71,054304,2005) +AUTHOR (C.Fransen,V.Werner,D.Bandyopadhyay,N.Boukharouba, + S.R.Lesher,M.T.McEllistrem,J.Jolie,N.Pietralla, + P.VonBrentano,S.W.Yates) +TITLE Investigation of low-spin states in 92Zr with the + (n,n'gamma) reaction +FACILITY (VDG,1USAKTY) 7MV electrostatic accelerator at + the University of Kentucky +SAMPLE Massive 41.1415 g metallic cylindrical Zr sample + with a diameter of 2 cm and a length of 2 cm was + enriched in 92Zr to 95.16 %. +DETECTOR (GE-IN) Compton-suppressed HPGe detector with an + efficiency of 55% relative to a 7.6 x 7.6 cm NaI + detector. +HISTORY (20050628C) DR +ENDBIB 16 +NOCOMMON 0 0 +ENDSUBENT 19 +SUBENT 14013002 20050628 20050909 1336 +BIB 4 4 +REACTION (40-ZR-92(N,INL)40-ZR-92,PAR,SIG,,REL) +EN-SEC (E-EXC,40-ZR-92) +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 4 +ENDBIB 4 +COMMON 1 3 +E-EXC +MEV +3.2629 +ENDCOMMON 3 +DATA 2 7 +EN DATA +MEV ARB-UNITS + 3.39E+00 9.68E-01 + 3.50E+00 2.51E+00 + 3.60E+00 3.60E+00 + 3.70E+00 4.24E+00 + 3.80E+00 4.39E+00 + 3.90E+00 4.79E+00 + 4.00E+00 4.56E+00 +ENDDATA 9 +ENDSUBENT 22 +ENDENTRY 2 diff --git a/exforall/140/14014.x4 b/exforall/140/14014.x4 new file mode 100644 index 000000000..3772eb6b7 --- /dev/null +++ b/exforall/140/14014.x4 @@ -0,0 +1,148 @@ +ENTRY 14014 20050628 20050909 1336 +SUBENT 14014001 20050628 20050909 1336 +BIB 9 13 +INSTITUTE (1USALRL,1USAINL,1USALAS) +REFERENCE (C,2001BERKEL,,673,2001) +AUTHOR (W.Younes,J.A.Becker,L.A.Bernstein,P.E.Garrett, + C.A.McGraph,D.P.McNabb,R.O.Nelson,G.D.Johns, + W.S.Wilburn,D.M.Drake) +TITLE Transition from asymmetric to symmetric fission in the + 235U(n,f) reaction +FACILITY (LINAC,1USALAS) LANSCE Linac and WNR facility +SAMPLE 93.2 % enriched U235 metal sample, 617 +/- 44 mg/cm2 +METHOD (TOF) +DETECTOR (GE-IN) GEANIE spectrometer at WNR, 11 compton + suppressed planar detector, 15 coaxial detectors. +HISTORY (20050628C) DR +ENDBIB 13 +NOCOMMON 0 0 +ENDSUBENT 16 +SUBENT 14014002 20050628 20050909 1336 +BIB 3 3 +REACTION (92-U-235(N,F)MASS,CHN,FY) +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 5 116 +EN EN-ERR MASS DATA DATA-ERR +MEV MEV NO-DIM PC/FIS PC/FIS + 5.1 0.1 8.80E+01 3.40E+00 + 5.1 0.1 8.90E+01 4.33E+00 1.09E+00 + 5.1 0.1 9.40E+01 5.84E+00 + 5.1 0.1 9.80E+01 4.74E+00 7.54E-01 + 5.1 0.1 1.00E+02 6.32E+00 + 5.1 0.1 1.02E+02 2.21E+00 4.76E-01 + 5.1 0.1 1.05E+02 2.89E-01 3.51E-01 + 5.1 0.1 1.07E+02 1.91E+00 6.38E-01 + 5.1 0.1 1.31E+02 3.02E+00 1.61E+00 + 5.1 0.1 1.37E+02 6.01E+00 + 5.1 0.1 1.38E+02 7.42E+00 + 5.1 0.1 1.39E+02 6.71E+00 + 5.1 0.1 1.39E+02 2.71E+00 1.93E+00 + 5.1 0.1 1.39E+02 4.65E+00 + 5.1 0.1 1.42E+02 3.46E+00 + 5.1 0.1 1.43E+02 5.15E+00 + 5.1 0.1 1.43E+02 4.37E+00 + 5.1 0.1 1.44E+02 3.10E+00 + 5.1 0.1 1.44E+02 2.70E+00 + 5.1 0.1 1.46E+02 4.39E-01 7.24E-01 + 5.1 0.1 1.46E+02 3.66E+00 + 5.1 0.1 1.47E+02 1.17E+00 3.09E-01 + 5.1 0.1 1.48E+02 1.80E+00 3.87E-01 +15.1 0.7 8.80E+01 3.59E+00 +15.1 0.7 9.40E+01 4.54E+00 +15.1 0.7 9.50E+01 6.66E+00 1.36E+00 +15.1 0.7 9.70E+01 6.06E+00 +15.1 0.7 9.90E+01 4.21E+00 +15.1 0.7 1.00E+02 6.46E+00 +15.1 0.7 1.01E+02 2.60E+00 5.34E-01 +15.1 0.7 1.06E+02 1.28E+00 2.99E-01 +15.1 0.7 1.08E+02 2.06E+00 2.91E-01 +15.1 0.7 1.31E+02 4.44E+00 7.90E-01 +15.1 0.7 1.37E+02 5.32E+00 +15.1 0.7 1.37E+02 4.93E+00 +15.1 0.7 1.40E+02 6.47E+00 +15.1 0.7 1.40E+02 3.58E+00 +15.1 0.7 1.40E+02 3.99E+00 +15.1 0.7 1.43E+02 3.07E+00 +15.1 0.7 1.45E+02 3.56E+00 1.11E+00 +15.1 0.7 1.46E+02 2.08E+00 +15.1 0.7 1.46E+02 2.36E+00 +15.1 0.7 1.47E+02 1.36E+00 1.81E-01 +15.1 0.7 1.47E+02 9.35E-01 1.57E-01 +19.6 1.0 8.70E+01 2.54E+00 5.48E-01 +19.6 1.0 9.30E+01 5.10E+00 +19.6 1.0 9.50E+01 4.20E+00 1.10E+00 +19.6 1.0 9.70E+01 5.97E+00 +19.6 1.0 9.90E+01 4.80E+00 +19.6 1.0 9.90E+01 6.31E+00 +19.6 1.0 1.01E+02 3.25E+00 6.69E-01 +19.6 1.0 1.05E+02 1.91E+00 3.76E-01 +19.6 1.0 1.07E+02 3.26E+00 +19.6 1.0 1.31E+02 4.62E+00 1.03E+00 +19.6 1.0 1.36E+02 4.31E+00 +19.6 1.0 1.39E+02 5.67E+00 9.04E-01 +19.6 1.0 1.39E+02 3.84E+00 +19.6 1.0 1.39E+02 1.51E+00 7.24E-01 +19.6 1.0 1.39E+02 4.70E+00 +19.6 1.0 1.40E+02 3.31E+00 +19.6 1.0 1.42E+02 3.01E+00 +19.6 1.0 1.43E+02 2.35E+00 5.28E-01 +19.6 1.0 1.44E+02 1.11E+00 +19.6 1.0 1.45E+02 3.26E+00 6.10E-01 +19.6 1.0 1.46E+02 2.46E+00 +19.6 1.0 1.46E+02 2.24E+00 +19.6 1.0 1.48E+02 1.23E+00 2.19E-01 +19.6 1.0 1.48E+02 9.76E-01 1.38E-01 +50.0 4.2 8.70E+01 1.99E+00 3.37E-01 +50.0 4.2 8.80E+01 1.73E+00 +50.0 4.2 9.30E+01 4.86E+00 +50.0 4.2 9.50E+01 3.14E+00 4.18E-01 +50.0 4.2 9.70E+01 4.79E+00 +50.0 4.2 9.90E+01 2.93E+00 +50.0 4.2 9.90E+01 5.78E+00 +50.0 4.2 1.01E+02 3.68E+00 7.93E-01 +50.0 4.2 1.05E+02 2.98E+00 4.23E-01 +50.0 4.2 1.07E+02 2.76E+00 +50.0 4.2 1.32E+02 2.03E+00 4.96E-01 +50.0 4.2 1.37E+02 1.05E+00 2.58E-01 +50.0 4.2 1.37E+02 2.23E+00 +50.0 4.2 1.38E+02 3.43E+00 +50.0 4.2 1.39E+02 3.98E+00 7.83E-01 +50.0 4.2 1.39E+02 2.74E+00 +50.0 4.2 1.40E+02 8.70E-01 8.86E-01 +50.0 4.2 1.42E+02 1.82E+00 +50.0 4.2 1.42E+02 1.65E+00 +50.0 4.2 1.44E+02 8.57E-01 5.55E-01 +50.0 4.2 1.44E+02 2.61E+00 5.63E-01 +50.0 4.2 1.46E+02 2.76E+00 +50.0 4.2 1.46E+02 7.51E-01 +50.0 4.2 1.48E+02 9.50E-01 1.69E-01 +50.0 4.2 1.48E+02 4.97E-01 1.71E-01 +84.4 9.5 8.70E+01 1.69E+00 +84.4 9.5 8.80E+01 2.01E+00 2.68E-01 +84.4 9.5 9.30E+01 3.98E+00 +84.4 9.5 9.50E+01 4.77E+00 +84.4 9.5 9.90E+01 2.10E+00 +84.4 9.5 9.95E+01 4.34E+00 +84.4 9.5 1.01E+02 6.33E-01 5.21E-01 +84.4 9.5 1.05E+02 2.37E+00 +84.4 9.5 1.07E+02 2.79E+00 +84.4 9.5 1.31E+02 1.44E+00 4.25E-01 +84.4 9.5 1.37E+02 2.69E+00 +84.4 9.5 1.37E+02 1.65E+00 +84.4 9.5 1.37E+02 8.41E-01 2.13E-01 +84.4 9.5 1.39E+02 2.26E+00 +84.4 9.5 1.40E+02 3.02E+00 +84.4 9.5 1.41E+02 1.22E+00 +84.4 9.5 1.41E+02 1.04E+00 +84.4 9.5 1.43E+02 1.72E+00 2.60E-01 +84.4 9.5 1.43E+02 1.51E+00 +84.4 9.5 1.44E+02 3.10E+00 +84.4 9.5 1.45E+02 7.38E-01 1.73E-01 +84.4 9.5 1.46E+02 3.17E-01 1.09E-01 +84.4 9.5 1.48E+02 7.62E-01 +ENDDATA 118 +ENDSUBENT 126 +ENDENTRY 2 diff --git a/exforall/140/14015.x4 b/exforall/140/14015.x4 new file mode 100644 index 000000000..0f9eeefb6 --- /dev/null +++ b/exforall/140/14015.x4 @@ -0,0 +1,74 @@ +ENTRY 14015 20050628 20050909 1336 +SUBENT 14015001 20050628 20050909 1336 +BIB 9 11 +INSTITUTE (1USANIS,1USALAS,1USAORL) +REFERENCE (C,91JUELIC,,518,1991) +AUTHOR (A.D.Carlson,O.A.Wasson,P.W.Lisowski,J.L.Ullmann, + N.W.Hill) +TITLE Measurements of the 235U(n,f) cross section in the + 3 to 30 MeV neutron energy region +FACILITY (LINAC,1USALAS) LANSCE Linac and WNR facility +SAMPLE 200 microg/cm2 235U deposit +METHOD (TOF) +DETECTOR (IOCH) Fission ionization chamber +HISTORY (20050628C) DR +ENDBIB 11 +NOCOMMON 0 0 +ENDSUBENT 14 +SUBENT 14015002 20050628 20050909 1336 +BIB 3 3 +REACTION (92-U-235(N,F),,SIG) +ERR-ANALYS Statistical uncertainties between 1 and 2 % +STATUS (CURVE) Data read from Fig. 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 2 44 +EN DATA +MEV B + 2.09E+00 1.25E+00 + 2.13E+00 1.26E+00 + 2.16E+00 1.22E+00 + 2.21E+00 1.20E+00 + 2.23E+00 1.17E+00 + 2.27E+00 1.19E+00 + 2.32E+00 1.15E+00 + 2.35E+00 1.11E+00 + 2.40E+00 1.11E+00 + 2.47E+00 1.10E+00 + 2.52E+00 1.08E+00 + 2.60E+00 1.08E+00 + 2.66E+00 1.08E+00 + 2.72E+00 1.03E+00 + 2.81E+00 1.04E+00 + 2.92E+00 1.08E+00 + 3.01E+00 1.21E+00 + 3.14E+00 1.39E+00 + 3.29E+00 1.55E+00 + 3.42E+00 1.70E+00 + 3.56E+00 1.77E+00 + 3.75E+00 1.78E+00 + 3.94E+00 1.78E+00 + 4.13E+00 1.79E+00 + 4.37E+00 1.72E+00 + 4.62E+00 1.73E+00 + 4.93E+00 1.71E+00 + 5.26E+00 1.70E+00 + 5.66E+00 1.83E+00 + 6.08E+00 1.99E+00 + 6.59E+00 2.08E+00 + 7.14E+00 2.11E+00 + 7.79E+00 2.13E+00 + 8.56E+00 2.15E+00 + 9.43E+00 2.08E+00 + 1.04E+01 2.05E+00 + 1.16E+01 2.03E+00 + 1.31E+01 2.11E+00 + 1.49E+01 2.16E+00 + 1.69E+01 2.05E+00 + 1.96E+01 2.14E+00 + 2.25E+01 2.08E+00 + 2.63E+01 2.17E+00 + 2.99E+01 2.21E+00 +ENDDATA 46 +ENDSUBENT 54 +ENDENTRY 2 diff --git a/exforall/140/14016.x4 b/exforall/140/14016.x4 new file mode 100644 index 000000000..a07554f8e --- /dev/null +++ b/exforall/140/14016.x4 @@ -0,0 +1,186 @@ +ENTRY 14016 20050629 20050909 1336 +SUBENT 14016001 20050629 20050909 1336 +BIB 9 11 +INSTITUTE (1USALAS,1USANIS,1USAORL) +REFERENCE (C,91UPPSAL,,177,1991) +AUTHOR (P.W.Lisowski,A.Gavron,W.E.Parker,J.L.Ullmann, + S.J.Balestrini,A.D.Carlson,O.A.Wasson,N.W.Hill) +TITLE Fission cross sections in the intermediate energy + region +FACILITY (LINAC,1USALAS) LANSCE Linac and WNR facility +SAMPLE 200 microg/cm2 235U deposit +METHOD (TOF) +DETECTOR (IOCH) Fission ionization chamber +HISTORY (20050629C) DR +ENDBIB 11 +NOCOMMON 0 0 +ENDSUBENT 14 +SUBENT 14016002 20050629 20050909 1336 +BIB 3 3 +REACTION (92-U-235(N,F),,SIG) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 72 +EN DATA DATA-ERR +MEV B B + 3.02E+01 2.05E+00 3.05E-02 + 3.11E+01 2.02E+00 3.45E-02 + 3.21E+01 2.13E+00 3.25E-02 + 3.30E+01 2.06E+00 3.45E-02 + 3.41E+01 2.07E+00 3.45E-02 + 3.51E+01 2.03E+00 3.86E-02 + 3.61E+01 1.97E+00 3.86E-02 + 3.72E+01 1.98E+00 3.65E-02 + 3.84E+01 1.94E+00 4.26E-02 + 3.96E+01 2.01E+00 4.87E-02 + 4.07E+01 1.99E+00 5.08E-02 + 4.20E+01 1.93E+00 4.67E-02 + 4.32E+01 1.95E+00 5.69E-02 + 4.46E+01 1.94E+00 5.08E-02 + 4.60E+01 1.92E+00 5.89E-02 + 4.74E+01 1.86E+00 5.89E-02 + 4.88E+01 1.82E+00 5.89E-02 + 5.02E+01 1.83E+00 6.30E-02 + 5.18E+01 1.79E+00 5.89E-02 + 5.35E+01 1.68E+00 5.69E-02 + 5.50E+01 1.84E+00 6.91E-02 + 5.66E+01 1.90E+00 8.53E-02 + 5.83E+01 1.79E+00 7.72E-02 + 6.03E+01 1.75E+00 7.11E-02 + 6.18E+01 1.86E+00 + 6.39E+01 1.76E+00 + 6.59E+01 1.74E+00 + 6.78E+01 1.74E+00 + 6.98E+01 1.70E+00 + 7.20E+01 1.71E+00 + 7.41E+01 1.71E+00 + 7.62E+01 1.71E+00 + 7.87E+01 1.68E+00 + 8.14E+01 1.69E+00 + 8.39E+01 1.65E+00 + 8.65E+01 1.63E+00 + 8.93E+01 1.57E+00 1.62E-02 + 9.21E+01 1.56E+00 2.23E-02 + 9.49E+01 1.54E+00 1.83E-02 + 9.75E+01 1.57E+00 2.03E-02 + 1.00E+02 1.55E+00 1.83E-02 + 1.03E+02 1.48E+00 1.62E-02 + 1.06E+02 1.54E+00 2.23E-02 + 1.10E+02 1.49E+00 1.82E-02 + 1.13E+02 1.50E+00 1.82E-02 + 1.17E+02 1.53E+00 2.23E-02 + 1.21E+02 1.46E+00 2.23E-02 + 1.24E+02 1.48E+00 2.23E-02 + 1.28E+02 1.45E+00 2.03E-02 + 1.32E+02 1.44E+00 1.82E-02 + 1.36E+02 1.48E+00 2.23E-02 + 1.40E+02 1.45E+00 1.62E-02 + 1.44E+02 1.43E+00 2.03E-02 + 1.49E+02 1.44E+00 2.44E-02 + 1.53E+02 1.47E+00 2.03E-02 + 1.58E+02 1.43E+00 2.03E-02 + 1.63E+02 1.43E+00 2.64E-02 + 1.68E+02 1.42E+00 2.64E-02 + 1.73E+02 1.42E+00 2.43E-02 + 1.78E+02 1.46E+00 2.64E-02 + 1.84E+02 1.44E+00 2.64E-02 + 1.89E+02 1.45E+00 2.84E-02 + 1.95E+02 1.41E+00 2.23E-02 + 2.01E+02 1.44E+00 2.64E-02 + 2.06E+02 1.45E+00 3.04E-02 + 2.13E+02 1.42E+00 3.25E-02 + 2.19E+02 1.48E+00 3.25E-02 + 2.26E+02 1.43E+00 3.04E-02 + 2.33E+02 1.47E+00 3.66E-02 + 2.41E+02 1.41E+00 3.65E-02 + 2.48E+02 1.44E+00 3.86E-02 + 2.55E+02 1.44E+00 4.06E-02 +ENDDATA 74 +ENDSUBENT 82 +SUBENT 14016003 20050629 20050909 1336 +BIB 3 3 +REACTION (92-U-238(N,F),,SIG) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 2 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 72 +EN DATA DATA-ERR +MEV B B + 3.04E+01 1.64E+00 1.82E-02 + 3.12E+01 1.66E+00 2.02E-02 + 3.22E+01 1.68E+00 2.02E-02 + 3.32E+01 1.67E+00 2.02E-02 + 3.43E+01 1.63E+00 1.82E-02 + 3.53E+01 1.65E+00 1.62E-02 + 3.64E+01 1.64E+00 1.82E-02 + 3.75E+01 1.69E+00 2.02E-02 + 3.86E+01 1.69E+00 1.82E-02 + 3.98E+01 1.69E+00 1.82E-02 + 4.09E+01 1.71E+00 1.82E-02 + 4.22E+01 1.65E+00 1.62E-02 + 4.35E+01 1.68E+00 1.62E-02 + 4.48E+01 1.66E+00 1.82E-02 + 4.62E+01 1.69E+00 1.82E-02 + 4.76E+01 1.65E+00 1.82E-02 + 4.90E+01 1.64E+00 1.82E-02 + 5.05E+01 1.63E+00 2.02E-02 + 5.20E+01 1.65E+00 1.62E-02 + 5.35E+01 1.63E+00 1.82E-02 + 5.52E+01 1.63E+00 2.02E-02 + 5.68E+01 1.62E+00 2.22E-02 + 5.85E+01 1.63E+00 2.02E-02 + 6.03E+01 1.60E+00 1.82E-02 + 6.22E+01 1.57E+00 1.82E-02 + 6.40E+01 1.56E+00 1.82E-02 + 6.58E+01 1.51E+00 1.82E-02 + 6.79E+01 1.53E+00 1.82E-02 + 6.98E+01 1.55E+00 2.22E-02 + 7.21E+01 1.49E+00 1.82E-02 + 7.45E+01 1.52E+00 1.82E-02 + 7.68E+01 1.50E+00 2.02E-02 + 7.91E+01 1.50E+00 1.62E-02 + 8.16E+01 1.48E+00 1.82E-02 + 8.41E+01 1.46E+00 1.82E-02 + 8.67E+01 1.46E+00 2.02E-02 + 8.95E+01 1.45E+00 2.02E-02 + 9.24E+01 1.44E+00 1.82E-02 + 9.51E+01 1.44E+00 1.82E-02 + 9.78E+01 1.42E+00 1.41E-02 + 1.00E+02 1.40E+00 2.02E-02 + 1.04E+02 1.43E+00 2.02E-02 + 1.07E+02 1.38E+00 2.02E-02 + 1.10E+02 1.34E+00 1.62E-02 + 1.13E+02 1.33E+00 1.61E-02 + 1.17E+02 1.34E+00 1.82E-02 + 1.21E+02 1.36E+00 2.02E-02 + 1.24E+02 1.35E+00 1.82E-02 + 1.28E+02 1.32E+00 2.22E-02 + 1.32E+02 1.32E+00 1.82E-02 + 1.36E+02 1.31E+00 1.82E-02 + 1.40E+02 1.31E+00 2.03E-02 + 1.45E+02 1.31E+00 2.02E-02 + 1.49E+02 1.30E+00 1.82E-02 + 1.54E+02 1.29E+00 2.23E-02 + 1.58E+02 1.28E+00 1.82E-02 + 1.64E+02 1.30E+00 2.03E-02 + 1.69E+02 1.29E+00 1.82E-02 + 1.73E+02 1.31E+00 2.63E-02 + 1.79E+02 1.31E+00 2.63E-02 + 1.84E+02 1.30E+00 2.43E-02 + 1.90E+02 1.30E+00 2.23E-02 + 1.96E+02 1.27E+00 2.23E-02 + 2.01E+02 1.34E+00 2.63E-02 + 2.08E+02 1.25E+00 2.83E-02 + 2.14E+02 1.30E+00 2.43E-02 + 2.20E+02 1.32E+00 2.63E-02 + 2.27E+02 1.31E+00 2.63E-02 + 2.34E+02 1.28E+00 3.04E-02 + 2.41E+02 1.30E+00 3.04E-02 + 2.49E+02 1.29E+00 3.04E-02 + 2.57E+02 1.29E+00 3.24E-02 +ENDDATA 74 +ENDSUBENT 82 +ENDENTRY 3 diff --git a/exforall/140/14017.x4 b/exforall/140/14017.x4 new file mode 100644 index 000000000..70eac2f5c --- /dev/null +++ b/exforall/140/14017.x4 @@ -0,0 +1,46 @@ +ENTRY 14017 20050630 20050909 1336 +SUBENT 14017001 20050630 20050909 1336 +BIB 10 18 +INSTITUTE (1USAINU,2SWDUPP,1USAOHO) +REFERENCE (J,NIM/A,527,432,2004) +AUTHOR (T.Peterson,S.E.Vigdor,C.Allgower,B.Bergenwall, + L.C.Bland,J.Blomgren,J.Doskow,T.Hossbach,W.W.Jacobs, + C.Johansson,T.Kinashia,J.Klug,A.V.Klyachko, + P.Nadel-Turonski,L.Nilsson,N.Olsson,M.Planinic,S.Pomp, + J.Rapaport,T.Rinckel,E.J.Stephenson,U.Tippawan, + S.W.Wissink,Y.Zhou) +TITLE Development of a tagged neutron facility at intermediat + energies +FACILITY (LINAC,1USAINU) Tagged neutron source +INC-SOURCE (P-D) Electron-cooled circulating proton beam of 200 Me + bombarding energy incident on a deuterium gas jet + target. +SAMPLE CH2 target +DETECTOR (PSSSD) Double-sided silicon strip detectors +METHOD (EDE) +HISTORY (20050630C) DR +ENDBIB 18 +NOCOMMON 0 0 +ENDSUBENT 21 +SUBENT 14017002 20050630 20050909 1336 +BIB 3 3 +REACTION (1-H-1(N,EL)1-H-1,,DA) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 16 +ENDBIB 3 +COMMON 1 3 +EN +MEV +193. +ENDCOMMON 3 +DATA 3 5 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR MB/SR + 1.25E+02 3.93E+00 + 1.31E+02 4.31E+00 + 1.37E+02 4.96E+00 + 1.43E+02 5.46E+00 2.47E-01 + 1.50E+02 6.08E+00 3.00E-01 +ENDDATA 7 +ENDSUBENT 19 +ENDENTRY 2 diff --git a/exforall/140/14018.x4 b/exforall/140/14018.x4 new file mode 100644 index 000000000..7788748af --- /dev/null +++ b/exforall/140/14018.x4 @@ -0,0 +1,607 @@ +ENTRY 14018 20050630 20050909 1336 +SUBENT 14018001 20050630 20050909 1336 +BIB 7 8 +INSTITUTE (1USAPPO) +REFERENCE (W,YOUNG,1968) Private communication +AUTHOR (T.E.Young) +TITLE Low energy neutron total cross sections for natural + Lu, 175Lu, 176Lu +FACILITY MTR Fast Chopper +METHOD (TOF) +HISTORY (20050630C) DR +ENDBIB 8 +NOCOMMON 0 0 +ENDSUBENT 11 +SUBENT 14018002 20050630 20050909 1336 +BIB 4 4 +REACTION (71-LU-0(N,TOT),,SIG) +ERR-ANALYS No information +SAMPLE Packed powder sample Lu2O3, 1/n=57.5 b/a +STATUS Data received on tables +ENDBIB 4 +NOCOMMON 0 0 +DATA 2 132 +EN DATA +EV B + 4.61596 60.60 + 4.40407 36.54 + 4.20644 21.72 + 4.02181 16.90 + 3.84909 14.07 + 3.68725 14.31 + 3.49892 14.75 + 3.32465 15.86 + 3.19445 19.18 + 3.04217 27.06 + 2.87339 63.04 + 2.74324 129.76 + 2.62174 163.11 + 2.48630 68.83 + 2.36109 35.65 + 2.26384 23.78 + 2.17247 19.47 + 2.05357 17.10 + 1.94417 16.05 + 1.85721 15.75 + 1.77596 20.01 + 1.68773 43.81 + 1.60591 91.42 + 1.52990 48.03 + 1.45916 22.95 + 1.39322 16.97 + 1.32319 13.99 + 1.25831 14.02 + 1.19808 13.09 + 1.14208 13.33 + 1.08992 13.00 + 1.03539 12.93 + 0.98486 12.97 + 0.93794 12.84 + 0.89429 12.87 + 0.85362 12.74 + 0.81160 13.47 + 0.77261 13.27 + 0.73636 12.97 + 0.70261 13.67 + 0.66809 13.71 + 0.63606 13.59 + 0.60627 13.49 + 0.57611 13.85 + 0.54814 14.81 + 0.52215 14.49 + 0.49798 14.90 + 0.47544 15.09 + 0.45271 15.52 + 0.43001 16.19 + 0.41042 16.45 + 0.39079 16.92 + 0.37128 17.80 + 0.35435 18.95 + 0.33748 19.85 + 0.32077 20.92 + 0.30621 22.75 + 0.29174 24.28 + 0.27746 27.40 + 0.26421 30.65 + 0.25189 34.49 + 0.24040 39.46 + 0.22848 47.00 + 0.21741 56.92 + 0.20714 69.83 + 0.19709 87.98 + 0.18775 113.13 + 0.17906 144.59 + 0.17057 185.33 + 0.16231 235.77 + 0.15463 283.36 + 0.14718 318.77 + 0.14025 320.39 + 0.13379 320.39 + 0.12727 291.44 + 0.12122 257.79 + 0.11559 224.97 + 0.10993 195.64 + 0.10468 172.71 + 0.09980 153.75 + 0.09493 138.62 + 0.09040 126.40 + 0.08619 117.00 + 0.08201 109.10 + 0.07813 102.76 + 0.07440 97.34 + 0.07083 92.96 + 0.06751 89.29 + 0.06424 86.47 + 0.06120 84.13 + 0.05286 82.30 + 0.05251 81.12 + 0.05236 79.84 + 0.05033 78.86 + 0.04798 78.16 + 0.04568 77.43 + 0.04350 77.08 + 0.04142 76.78 + 0.03944 77.04 + 0.03756 76.97 + 0.03577 77.36 + 0.03408 77.69 + 0.03246 78.43 + 0.03093 78.93 + 0.02945 79.79 + 0.02805 80.35 + 0.02672 81.41 + 0.02544 82.34 + 0.02423 83.27 + 0.02308 84.60 + 0.02198 85.56 + 0.02092 86.54 + 0.01992 88.05 + 0.01897 88.99 + 0.01807 89.75 + 0.01721 91.19 + 0.01639 92.25 + 0.01561 94.00 + 0.01487 95.95 + 0.01416 97.27 + 0.01349 100.09 + 0.01285 102.27 + 0.01223 104.76 + 0.01165 105.45 + 0.01109 108.36 + 0.01056 112.35 + 0.01006 113.38 + 0.00958 116.63 + 0.00912 119.23 + 0.00869 117.97 + 0.00828 114.86 + 0.00799 111.18 +ENDDATA 134 +ENDSUBENT 143 +SUBENT 14018003 20050630 20050909 1336 +BIB 5 6 +REACTION (71-LU-0(N,TOT),,SIG) +ERR-ANALYS No information +SAMPLE Pressed sample, Lu2O3+ Al powder pressed + 1/n=161.8 +CORRECTION sigma(n,tot)=82. barns at 0.0253 eV +STATUS Data received on tables +ENDBIB 6 +NOCOMMON 0 0 +DATA 2 130 +EN DATA +EV B +4.45565 51.87 +4.25458 27.38 +4.06681 20.14 +3.89121 15.94 +3.72674 14.51 +3.49892 13.01 +3.29136 17.83 +3.16309 20.45 +3.04217 25.47 +2.87339 73.50 +2.71827 248.36 +2.62174 328.56 +2.48630 111.21 +2.36109 38.64 +2.24511 21.12 +2.13747 19.44 +2.03739 16.76 +1.94417 13.18 +1.85721 15.19 +1.77596 15.81 +1.69992 38.11 +1.60591 103.88 +1.51949 52.78 +1.45916 22.72 +1.40237 13.90 +1.33165 14.33 +1.26615 14.94 +1.20537 11.99 +1.14886 13.98 +1.09624 10.87 +1.03539 13.18 +0.97947 12.74 +0.93794 12.67 +0.89899 14.39 +0.85362 13.60 +0.81160 13.92 +0.77261 10.73 +0.73636 9.42 +0.70261 10.86 +0.66508 13.11 +0.63606 12.69 +0.60889 14.38 +0.57853 13.86 +0.55039 12.63 +0.52425 15.40 +0.49993 12.38 +0.47726 11.98 +0.45271 14.05 +0.43001 14.83 +0.40897 15.66 +0.38944 16.29 +0.37128 18.67 +0.35415 16.23 +0.33856 19.30 +0.32178 20.40 +0.30621 22.31 +0.29174 23.27 +0.27828 24.92 +0.26421 29.39 +0.25119 34.45 +0.24040 38.31 +0.22908 46.64 +0.21141 56.01 +0.20662 69.89 +0.19660 90.72 +0.18730 111.13 +0.17864 152.49 +0.17057 194.84 +0.16231 249.18 +0.15463 303.47 +0.14749 343.00 +0.14025 358.42 +0.13352 344.27 +0.12727 312.28 +0.12099 270.42 +0.11515 234.89 +0.10973 203.85 +0.10468 179.86 +0.09997 160.19 +0.09493 143.57 +0.09025 130.24 +0.08619 119.91 +0.08214 111.18 +0.07813 104.52 +0.07440 98.89 +0.07093 94.54 +0.06751 91.05 +0.06415 87.16 +0.06103 85.28 +0.05813 83.29 +0.05544 82.32 +0.05279 80.47 +0.05033 79.55 +0.04792 78.70 +0.04558 77.86 +0.04350 77.50 +0.04146 76.89 +0.03948 77.27 +0.03756 76.24 +0.03577 76.65 +0.03411 76.81 +0.03243 78.03 +0.03087 77.89 +0.02943 79.13 +0.02803 78.63 +0.02668 80.62 +0.02542 82.02 +0.02421 82.87 +0.02304 83.48 +0.02196 83.47 +0.02092 84.60 +0.01992 85.00 +0.01896 86.57 +0.01807 87.38 +0.01721 86.71 +0.01639 89.18 +0.01561 90.96 +0.01486 93.10 +0.01415 94.56 +0.01346 95.37 +0.01283 97.63 +0.01223 100.39 +0.01165 101.48 +0.01110 102.69 +0.01056 106.54 +0.01005 111.73 +0.00958 107.48 +0.00913 113.09 +0.00869 113.84 +0.00828 110.63 +ENDDATA 132 +ENDSUBENT 143 +SUBENT 14018004 20050630 20050909 1336 +BIB 5 10 +REACTION (71-LU-175(N,TOT),,SIG) +ERR-ANALYS No information +SAMPLE Sample enriched to 99.924 %, + 1/n=47.74 b/a +CORRECTION Analysis to date for 175Lu: + (a) with measured total cross section described by + potential scattering plus resonance, + sigma(n,tot)=25.9 barns at 0.0253 eV + sigma(n,g) = 18.4 barns at 0.0253 eV +STATUS Data received on tables +ENDBIB 10 +NOCOMMON 0 0 +DATA 2 168 +EN DATA +EV B +1706.69713 32.01 + 803.80776 29.36 + 465.73936 26.34 + 333.48439 24.33 + 213.31537 25.04 + 158.08726 27.01 + 121.82880 26.32 + 96.75154 18.16 + 78.68960 13.29 + 65.25090 16.30 + 54.98235 21.84 + 46.95995 23.64 + 40.57335 24.83 + 35.40626 26.35 + 31.16686 28.63 + 27.64567 23.55 + 24.68917 26.91 + 22.18277 26.30 + 20.03953 18.89 + 18.11253 19.39 + 16.58960 40.70 + 15.18954 79.06 + 13.95952 58.87 + 12.87308 38.08 + 11.90970 48.01 + 11.84877 34.12 + 11.27873 15.95 + 9.58647 9.04 + 8.96186 7.59 + 8.31637 8.29 + 7.88276 8.61 + 7.41487 8.85 + 6.98744 9.78 + 6.59593 13.82 + 6.23642 19.68 + 5.90553 36.04 + 5.51571 90.94 + 5.18496 154.06 + 4.93322 116.65 + 4.69938 60.97 + 4.48179 31.90 + 4.27896 19.40 + 4.05173 14.66 + 3.82828 12.95 + 3.66774 12.73 + 3.51709 12.29 + 3.37554 13.47 + 3.20500 16.82 + 3.03241 25.62 + 2.88691 48.18 + 2.75164 107.44 + 2.61393 148.73 + 2.49718 80.99 + 2.37116 36.51 + 2.25445 21.76 + 2.16071 17.49 + 2.06447 15.32 + 1.95169 12.90 + 1.86423 11.28 + 1.78253 11.13 + 1.68168 11.09 + 1.59843 10.80 + 1.53691 10.52 + 1.46405 10.06 + 1.38868 10.21 + 1.31899 9.67 + 1.25441 10.21 + 1.19446 10.19 + 1.13171 10.84 + 1.08677 10.09 + 1.03831 10.28 + 0.99302 10.05 + 0.94501 10.32 + 0.89710 10.07 + 0.85580 10.28 + 0.81363 10.12 + 0.77449 10.22 + 0.73812 10.58 + 0.70066 10.40 + 0.66991 10.48 + 0.61746 10.47 + 0.60497 10.77 + 0.57490 10.97 + 0.54701 11.30 + 0.52111 11.26 + 0.49701 10.77 + 0.47453 11.44 + 0.45355 11.09 + 0.43224 11.35 + 0.41125 11.50 + 0.39137 11.69 + 0.37325 11.74 + 0.35494 11.50 + 0.33693 12.00 + 0.32120 11.88 + 0.30668 12.13 + 0.29135 12.30 + 0.27706 12.87 + 0.26459 12.43 + 0.25220 12.83 + 0.24012 12.80 + 0.22875 13.10 + 0.21829 13.21 + 0.20792 13.16 + 0.19781 13.44 + 0.18843 13.45 + 0.17925 13.72 + 0.17040 13.97 + 0.16249 13.82 + 0.15480 13.79 + 0.14732 14.31 + 0.14039 14.25 + 0.13366 14.52 + 0.12716 14.67 + 0.12110 14.72 + 0.11547 15.08 + 0.11004 15.27 + 0.10478 15.55 + 0.09971 15.66 + 0.09501 15.97 + 0.09047 16.23 + 0.08613 16.33 + 0.08207 16.64 + 0.07819 16.98 + 0.07446 17.09 + 0.07088 17.28 + 0.06756 17.41 + 0.06437 17.57 + 0.06124 17.95 + 0.05833 18.45 + 0.05555 18.80 + 0.05290 19.23 + 0.05036 19.60 + 0.04795 19.99 + 0.04571 20.23 + 0.04352 20.50 + 0.04144 20.81 + 0.03946 21.29 + 0.03406 22.55 + 0.03245 23.36 + 0.03092 23.89 + 0.02947 24.48 + 0.02806 24.76 + 0.02671 25.54 + 0.02543 26.07 + 0.02422 26.70 + 0.02307 27.05 + 0.02199 27.55 + 0.02094 28.16 + 0.01994 28.50 + 0.01900 28.95 + 0.01809 28.65 + 0.01723 29.30 + 0.01641 29.96 + 0.01563 30.85 + 0.01489 32.26 + 0.01417 32.00 + 0.01349 33.74 + 0.01285 34.84 + 0.01224 35.85 + 0.01166 35.86 + 0.01110 37.18 + 0.01057 37.48 + 0.01007 38.41 + 0.00959 37.70 + 0.00914 37.73 + 0.00870 35.06 + 0.00829 31.92 +ENDDATA 170 +ENDSUBENT 185 +SUBENT 14018005 20050630 20050909 1336 +BIB 5 6 +REACTION (71-LU-176(N,TOT),,SIG) +ERR-ANALYS No information +SAMPLE Sample enriched to 71.1446 %, + 1/n=8129 b/a +CORRECTION sigma(n,tot)=2220. barns at 0.0253 eV +STATUS Data received on tables +ENDBIB 6 +NOCOMMON 0 0 +DATA 2 100 +EN DATA +EV B + 3.23912 90.93 + 3.05385 -167.00 + 2.93902 -89.17 + 2.77856 128.47 + 2.63089 103.97 + 2.53889 193.46 + 2.40968 7.74 + 2.29008 5.12 + 2.17918 34.61 + 2.07614 97.80 + 1.98024 -55.32 + 1.89083 69.94 + 1.80735 129.58 + 1.70437 1081.17 + 1.63280 3352.05 + 1.56565 364.23 + 1.48237 874.98 + 1.40556 262.53 + 1.33458 88.16 + 1.26883 130.47 + 1.20783 -108.89 + 1.15113 22.97 + 1.09832 79.41 + 1.04907 103.00 + 1.00316 198.30 + 0.96001 11.41 + 0.90998 48.69 + 0.86377 74.84 + 0.82899 21.21 + 0.78131 27.43 + 0.74444 77.06 + 0.71012 -202.62 + 0.67812 22.27 + 0.64249 -104.97 + 0.61490 107.85 + 0.58906 59.14 + 0.56014 272.99 + 0.53329 168.05 + 0.50834 27.78 + 0.48131 -6.45 + 0.45650 104.88 + 0.43668 239.68 + 0.41514 133.45 + 0.39517 288.03 + 0.37660 174.18 + 0.35931 258.50 + 0.34318 385.39 + 0.32604 349.47 + 0.31016 352.82 + 0.29541 438.48 + 0.28168 667.22 + 0.26890 779.18 + 0.25552 868.45 + 0.24312 1052.83 + 0.23160 1434.45 + 0.21974 1661.07 + 0.20983 2081.76 + 0.20057 2619.32 + 0.19098 3711.25 + 0.18207 4845.89 + 0.17296 6577.37 + 0.16452 8637.92 + 0.15669 10799.81 + 0.14940 12453.21 + 0.14261 13130.75 + 0.13571 13108.53 + 0.12931 11963.96 + 0.12287 10462.49 + 0.11689 8986.69 + 0.11135 7742.17 + 0.10580 6592.61 + 0.10102 5808.76 + 0.09622 5185.65 + 0.09145 4622.75 + 0.08731 4240.64 + 0.08318 3847.35 + 0.07909 3516.45 + 0.07529 3308.77 + 0.07176 3128.98 + 0.06847 2995.80 + 0.06522 2810.94 + 0.06202 2677.15 + 0.05906 2568.93 + 0.05630 2511.99 + 0.05359 2427.61 + 0.05094 2380.76 + 0.04849 2353.31 + 0.04621 2312.91 + 0.04409 2252.72 + 0.04201 2241.40 + 0.03999 2178.92 + 0.03811 2163.80 + 0.03628 2192.78 + 0.03452 2166.10 + 0.03287 2128.05 + 0.03134 2196.91 + 0.02986 2122.34 + 0.02843 2162.91 + 0.02705 2206.06 + 0.02577 2218.87 +ENDDATA 102 +ENDSUBENT 113 +ENDENTRY 5 diff --git a/exforall/140/14019.x4 b/exforall/140/14019.x4 new file mode 100644 index 000000000..844786c03 --- /dev/null +++ b/exforall/140/14019.x4 @@ -0,0 +1,54 @@ +ENTRY 14019 20050630 20050909 1336 +SUBENT 14019001 20050630 20050909 1336 +BIB 9 13 +INSTITUTE (1USALTI) +REFERENCE (P,DOE-NDC-12,151,1978) + (C,76LOWELL,,1332,1976) +AUTHOR (G.H.R.Kegel,L.E.Beghian,G.P.Couchell,J.J.Egan, + T.V.Marcella,A. Mittler,D.J.Pullen,W.A.Schier, + E.Sheldon,M.A.Doyle,S.Jain,J.Menachery,S.Mathew, + N.B.Sullivan,A.Wang) +TITLE Neutron Scattering on heavy deformed nuclei +FACILITY (VDG,1USALOW) +METHOD (TOF) +SAMPLE Small uranium disk +DETECTOR (SCIN) Plastic scintillator +HISTORY (20050630C) DR +ENDBIB 13 +NOCOMMON 0 0 +ENDSUBENT 16 +SUBENT 14019002 20050630 20050909 1336 +BIB 3 3 +REACTION (92-U-238(N,INL)92-U-238,,DA) +ERR-ANALYS (ERR-T) Total uncertainties +STATUS Data read from Table B-1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 5 +EN ANG DATA ERR-T +MEV ADEG MB/SR MB/SR +0.100 120. 43.3 5.5 +0.112 135. 56.6 7.6 +0.127 135. 65.9 7.2 +0.135 130. 76.6 10.1 +0.149 130. 125.2 17.5 +ENDDATA 7 +ENDSUBENT 15 +SUBENT 14019003 20050630 20050909 1336 +BIB 3 3 +REACTION (92-U-238(N,INL)92-U-238,,SIG) +ERR-ANALYS (ERR-T) Total uncertainties +STATUS Data read from Table B-1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 5 +EN DATA ERR-T +MEV B B +0.100 0.526 0.072 +0.112 0.762 0.109 +0.127 0.887 0.102 +0.135 0.994 0.140 +0.149 1.625 0.241 +ENDDATA 7 +ENDSUBENT 15 +ENDENTRY 3 diff --git a/exforall/140/14020.x4 b/exforall/140/14020.x4 new file mode 100644 index 000000000..19f5007a8 --- /dev/null +++ b/exforall/140/14020.x4 @@ -0,0 +1,98 @@ +ENTRY 14020 20050701 20050909 1336 +SUBENT 14020001 20050701 20050909 1336 +BIB 9 11 +INSTITUTE (1USAORL) +REFERENCE (P,ORNL-3692,,1964) +AUTHOR (W.F.Kiker) +TITLE Correlated energy and time-of-flight measurements of + fission fragments +FACILITY (REAC,1USAORL) + (VDG,1USAORL) +METHOD (TOF) +SAMPLE Small uranium disk +DETECTOR (SIBAR) Solid state detector (no information) +HISTORY (20050630C) DR +ENDBIB 11 +NOCOMMON 0 0 +ENDSUBENT 14 +SUBENT 14020002 20050701 20050909 1336 +BIB 3 3 +REACTION (98-CF-252(0,F)MASS,CHN,FY) +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 25 and 26 +ENDBIB 3 +NOCOMMON 0 0 +DATA 2 68 +MASS DATA +NO-DIM PC/FIS + 9.20E+01 7.02E-01 + 9.40E+01 1.01E+00 + 9.50E+01 1.20E+00 + 9.60E+01 1.43E+00 + 9.70E+01 1.74E+00 + 9.80E+01 2.21E+00 + 9.90E+01 3.10E+00 + 1.00E+02 3.50E+00 + 1.01E+02 4.40E+00 + 1.02E+02 5.41E+00 + 1.03E+02 5.56E+00 + 1.04E+02 5.92E+00 + 1.05E+02 5.94E+00 + 1.06E+02 5.76E+00 + 1.07E+02 6.54E+00 + 1.08E+02 6.22E+00 + 1.09E+02 5.34E+00 + 1.10E+02 4.96E+00 + 1.11E+02 4.94E+00 + 1.12E+02 4.34E+00 + 1.13E+02 3.81E+00 + 1.14E+02 3.29E+00 + 1.15E+02 2.76E+00 + 1.16E+02 2.17E+00 + 1.17E+02 2.28E-01 + 1.18E+02 2.17E-01 + 1.19E+02 1.95E-01 + 1.20E+02 1.66E-01 + 1.21E+02 1.35E-01 + 1.22E+02 1.38E-01 + 1.24E+02 8.00E-02 + 1.25E+02 9.28E-02 + 1.26E+02 1.25E-01 + 1.27E+02 1.66E-01 + 1.28E+02 1.83E-01 + 1.29E+02 5.61E-01 + 1.30E+02 1.07E+00 + 1.31E+02 2.32E+00 + 1.32E+02 2.86E+00 + 1.34E+02 3.49E+00 + 1.35E+02 4.05E+00 + 1.36E+02 4.96E+00 + 1.37E+02 5.48E+00 + 1.38E+02 5.28E+00 + 1.39E+02 5.57E+00 + 1.40E+02 5.83E+00 + 1.41E+02 5.87E+00 + 1.42E+02 5.63E+00 + 1.43E+02 5.69E+00 + 1.44E+02 5.59E+00 + 1.45E+02 5.21E+00 + 1.46E+02 4.61E+00 + 1.47E+02 4.48E+00 + 1.48E+02 3.76E+00 + 1.49E+02 2.76E+00 + 1.50E+02 2.38E+00 + 1.51E+02 2.01E+00 + 1.52E+02 1.94E+00 + 1.53E+02 1.50E+00 + 1.54E+02 1.02E+00 + 1.55E+02 8.65E-01 + 1.56E+02 7.47E-01 + 1.57E+02 5.80E-01 + 1.58E+02 4.15E-01 + 1.59E+02 3.01E-01 + 1.60E+02 3.89E-01 + 1.62E+02 1.04E-01 + 1.63E+02 1.47E-01 +ENDDATA 70 +ENDSUBENT 78 +ENDENTRY 2 diff --git a/exforall/140/14021.x4 b/exforall/140/14021.x4 new file mode 100644 index 000000000..33b4a8b98 --- /dev/null +++ b/exforall/140/14021.x4 @@ -0,0 +1,501 @@ +ENTRY 14021 20050701 20050909 1336 +SUBENT 14021001 20050701 20050909 1336 +BIB 9 15 +INSTITUTE (1USALAS,1USAMSU,1USALRL) +REFERENCE (J,PR/C,71,064314,2005) +AUTHOR (N.Fotiades,R.O.Nelson,M.Devlin,K.Starosta,J.A.Becker, + L.A.Bernstein,P.E.Garrett,W.Younes) +TITLE States in 197Au from the (n,n'g) reaction +FACILITY (ACCEL,1USALAS)LANSCE accelerator and WNR neutron + source +METHOD (TOF) +SAMPLE 197Au target in the present experiment consisted of one + foil, 1.5 g/cm2 thick. +DETECTOR (GE-IN) GEANIE spectrometer with 11 Compton-suppressed + planar Ge detectors (low-energy photon + spectrometers; LEPS), 9 Compton-suppressed coaxial Ge + detectors, and 6 unsuppressed coaxial Ge detectors. +HISTORY (20050701C) DR +ENDBIB 15 +NOCOMMON 0 0 +ENDSUBENT 18 +SUBENT 14021002 20050701 20050909 1336 +BIB 4 7 +REACTION (79-AU-197(N,INL)79-AU-197,,SPC,,REL) + Intensity normalized to 1000 for gamma-ray energy of + 279 keV +EN-SEC (E,G) + (E-EXC,79-AU-197) Initial level of excitation +ERR-ANALYS No information +STATUS Data read from table 1 +ENDBIB 7 +COMMON 2 3 +EN-MIN EN-MAX +MEV MEV +1. 70. +ENDCOMMON 3 +DATA 4 93 +E E-EXC DATA DATA-MIN +KEV KEV ARB-UNITS ARB-UNITS + 174.8 584. 477. + 176.0 1295. 23. + 189.2 737. 7. + 191.4 269. 424. + 201.6 279. 18. + 233.6 502. 11. + 234.4 737. 7. + 236.5 1004. 9. + 259.6 1555. 8. + 268.5 548. 52. + 268.8 269. 52. + 279.0 279. 1000. + 305.0 584. 9. + 308.0 856. 39. + 308.0 1045. 39. + 322.9 1060. 22. + 330.2 1375. 10. + 341.0 1277. 9. + 358.0 767. 251. + 364.0 948. 126. + 366.3 1370. 5. + 376.0 1231. 11. + 421.9 1370. 26. + 425.0 502. 13. + 429.2 1836. 13. + 433.1 936. 18. + 457.9 737. 191. + 468.1 737. 20. + 488.0 1533. 9. + 497.6 1045. 8. + 502.5 502. 276. + 519.7 1375. 7. + 529.0 1266. 5. + 535.0 1119. 59. + 538.6 948. 76. + 540.0 1277. 11. + 542.5 1045. 10. + 547.5 548. 433. + 557.1 1060. 22. + 558.8 1414. 19. + 568.9 1572. 18. + 576.5 856. 179. + 594.4 1004. 79. + 606.6 1555. 14. + 611.9 1379. 26. + 616.2 1119. 8. + 619.4 888. 5. + 638.2 1642. 20. + 638.6 1375. 20. + 639.7 1407. 41. + 657.1 936. 15. + 667.1 936. 30. + 677.8 1414. 14. + 684.2 1231. 46. + 702.9 1470. 22. + 711.0 1295. 44. + 716.0 1720. 4. + 718.8 1574. 26. + 732.3 1963. 6. + 745.6 1513. 15. + 763.2 1266. 5. + 766.3 1045. 49. + 774.6 1277. 11. + 776.1 1045. 32. + 791.6 1911. 7. + 795.0 1743. 4. + 797.2 1801. 10. + 805.4 1572. 7. + 810.8 888. 26. + 813.6 1933. 6. + 825.0 1773. 11. + 827.6 1375. 6. + 839.8 1119. 11. + 850.5 1798. 9. + 858.6 936. 10. + 860.0 1627. 14. + 869.9 1874. 4. + 871.5 1151. 12. + 881.9 1151. 17. + 895.3 2014. 7. + 913.0 1680. 13. + 920.3 1868. 7. + 926.0 1663. 9. + 936.2 936. 36. + 952.5 1720. 5. + 970.8 1555. 7. + 973.0 1242. 9. + 978.3 1481. 7. +1073.4 1151. 15. +1139.5 1217. 7. +1150.2 1151. 6. +1217.7 1217. 52. +1242.2 1242. 29. +ENDDATA 95 +ENDSUBENT 111 +SUBENT 14021003 20050701 20050909 1336 +BIB 4 5 +REACTION (79-AU-197(N,INL)79-AU-197,PAR,SIG,G,REL) +EN-SEC (E,G) Transition gamma ray + (LVL-INI,79-AU-197) Initial level +ERR-ANALYS (DATA-ERR) No information +STATUS Data received in tables from the author +ENDBIB 5 +NOCOMMON 0 0 +DATA 6 181 +E LVL-INI EN EN-RSL DATA DATA-ERR +KEV KEV MEV MEV ARB-UNITS ARB-UNITS +174.8 584. 1.104 0.033 98.6438 0.623891 +174.8 584. 1.173 0.058 128.901 0.664334 +174.8 584. 1.3 0.073 158.466 0.722574 +174.8 584. 1.454 0.086 196.544 0.77955 +174.8 584. 1.638 0.103 230.246 0.824317 +174.8 584. 1.859 0.125 269.032 0.873698 +174.8 584. 2.128 0.153 325.922 0.943785 +174.8 584. 2.461 0.19 370.004 0.987345 +174.8 584. 2.879 0.241 384.415 0.984428 +174.8 584. 3.414 0.312 388.058 0.98148 +174.8 584. 4.116 0.414 365.058 0.939555 +174.8 584. 4.29 0.094 359.663 1.98805 +174.8 584. 4.478 0.1 359.319 1.9799 +174.8 584. 4.679 0.107 349.74 1.94982 +174.8 584. 4.894 0.114 323.233 1.85167 +174.8 584. 5.123 0.122 320.9 1.83933 +174.8 584. 5.37 0.131 319.103 1.8487 +174.8 584. 5.634 0.141 313.913 1.84609 +174.8 584. 5.919 0.152 298.187 1.80885 +174.8 584. 6.226 0.164 284.413 1.76984 +174.8 584. 6.558 0.177 274.733 1.75517 +174.8 584. 6.917 0.192 254.758 1.67667 +174.8 584. 7.307 0.208 250.548 1.67233 +174.8 584. 7.731 0.227 247.319 1.68863 +174.8 584. 8.192 0.248 246.508 1.69452 +174.8 584. 8.697 0.271 209.341 1.5946 +174.8 584. 9.25 0.297 162.051 1.4173 +174.8 584. 9.858 0.327 114.688 1.2431 +174.8 584. 10.528 0.362 80.9123 1.10974 +174.8 584. 11.269 0.401 55.4372 0.99417 +174.8 584. 12.092 0.446 42.0685 0.941655 +174.8 584. 13.01 0.498 32.4284 0.90477 +174.8 584. 14.037 0.558 27.5207 0.882143 +358.0 767. 1.104 0.033 1.76485 0.268734 +358.0 767. 1.173 0.058 3.57137 0.268711 +358.0 767. 1.3 0.073 5.74651 0.284995 +358.0 767. 1.454 0.086 9.01373 0.309656 +358.0 767. 1.638 0.103 13.7668 0.342395 +358.0 767. 1.859 0.125 23.36 0.392958 +358.0 767. 2.128 0.153 34.7423 0.446229 +358.0 767. 2.461 0.19 48.9276 0.497385 +358.0 767. 2.879 0.241 69.0064 0.550734 +358.0 767. 3.414 0.312 100.979 0.627832 +358.0 767. 4.116 0.414 146.595 0.709219 +358.0 767. 4.29 0.094 164.215 1.58008 +358.0 767. 4.478 0.1 178.035 1.62746 +358.0 767. 4.679 0.107 191.514 1.65785 +358.0 767. 4.894 0.114 194.195 1.64084 +358.0 767. 5.123 0.122 207.884 1.67724 +358.0 767. 5.37 0.131 225.366 1.75809 +358.0 767. 5.634 0.141 243.629 1.81665 +358.0 767. 5.919 0.152 255.734 1.84742 +358.0 767. 6.226 0.164 270.079 1.89243 +358.0 767. 6.558 0.177 287.216 1.94009 +358.0 767. 6.917 0.192 292.18 1.93046 +358.0 767. 7.307 0.208 314.448 1.99068 +358.0 767. 7.731 0.227 343.58 2.0845 +358.0 767. 8.192 0.248 380.528 2.2031 +358.0 767. 8.697 0.271 377.777 2.19058 +358.0 767. 9.25 0.297 339.071 2.06655 +358.0 767. 9.858 0.327 269.341 1.85589 +358.0 767. 10.528 0.362 210.225 1.68816 +358.0 767. 11.269 0.401 154.923 1.50577 +358.0 767. 12.092 0.446 117.184 1.39138 +358.0 767. 13.01 0.498 88.7474 1.27672 +358.0 767. 14.037 0.558 68.8363 1.20866 +558.8 1414. 1.173 0.058 0.0207801 0.134378 +558.8 1414. 1.3 0.073 0.0249432 0.139871 +558.8 1414. 1.454 0.086 0.485486 0.15462 +558.8 1414. 1.638 0.103 2.01448 0.171983 +558.8 1414. 1.859 0.125 3.36069 0.192675 +558.8 1414. 2.128 0.153 3.56116 0.208702 +558.8 1414. 2.461 0.19 4.04961 0.21795 +558.8 1414. 2.879 0.241 4.79686 0.231732 +558.8 1414. 3.414 0.312 5.8925 0.249621 +558.8 1414. 4.116 0.414 6.94471 0.260638 +558.8 1414. 4.29 0.094 7.77968 0.569884 +558.8 1414. 4.478 0.1 7.9651 0.579572 +558.8 1414. 4.679 0.107 8.48771 0.573557 +558.8 1414. 4.894 0.114 7.71326 0.557701 +558.8 1414. 5.123 0.122 8.43128 0.571929 +558.8 1414. 5.37 0.131 10.2873 0.587636 +558.8 1414. 5.634 0.141 10.5096 0.598461 +558.8 1414. 5.919 0.152 10.4872 0.607245 +558.8 1414. 6.226 0.164 10.7665 0.605657 +558.8 1414. 6.558 0.177 10.8477 0.608889 +558.8 1414. 6.917 0.192 10.5729 0.582822 +558.8 1414. 7.307 0.208 10.5951 0.59967 +558.8 1414. 7.731 0.227 10.8688 0.610391 +558.8 1414. 8.192 0.248 11.2387 0.630045 +558.8 1414. 8.697 0.271 10.4661 0.608767 +558.8 1414. 9.25 0.297 9.94519 0.565261 +558.8 1414. 9.858 0.327 6.11101 0.515158 +558.8 1414. 10.528 0.362 4.58371 0.488299 +576.5 856. 1.104 0.033 2.07667 0.030441 +576.5 856. 1.173 0.058 2.64273 0.0321011 +576.5 856. 1.3 0.073 3.30551 0.0349135 +576.5 856. 1.454 0.086 3.95033 0.037316 +576.5 856. 1.638 0.103 4.45571 0.0388688 +576.5 856. 1.859 0.125 4.76955 0.0397794 +576.5 856. 2.128 0.153 5.13813 0.0408988 +576.5 856. 2.461 0.19 5.70119 0.0425329 +576.5 856. 2.879 0.241 6.24192 0.0438149 +576.5 856. 3.414 0.312 7.11553 0.0464455 +576.5 856. 4.116 0.414 7.83225 0.0475757 +576.5 856. 4.29 0.094 8.40806 0.104313 +576.5 856. 4.478 0.1 8.53231 0.105221 +576.5 856. 4.679 0.107 8.72254 0.105697 +576.5 856. 4.894 0.114 8.57967 0.102714 +576.5 856. 5.123 0.122 8.95266 0.104191 +576.5 856. 5.37 0.131 9.36332 0.107375 +576.5 856. 5.634 0.141 10.115 0.110825 +576.5 856. 5.919 0.152 9.90446 0.1103 +576.5 856. 6.226 0.164 9.83652 0.110144 +576.5 856. 6.558 0.177 10.2675 0.111607 +576.5 856. 6.917 0.192 9.77685 0.107598 +576.5 856. 7.307 0.208 10.2296 0.110327 +576.5 856. 7.731 0.227 10.4093 0.112541 +576.5 856. 8.192 0.248 10.5773 0.11445 +576.5 856. 8.697 0.271 9.87259 0.110856 +576.5 856. 9.25 0.297 8.15303 0.101277 +576.5 856. 9.858 0.327 6.25696 0.0909861 +576.5 856. 10.528 0.362 4.66938 0.081973 +594.4 1004. 1.638 0.103 3.39367 0.665205 +594.4 1004. 1.859 0.125 11.1775 0.754023 +594.4 1004. 2.128 0.153 20.5768 0.830319 +594.4 1004. 2.461 0.19 28.9854 0.904087 +594.4 1004. 2.879 0.241 41.4673 0.968195 +594.4 1004. 3.414 0.312 54.3954 1.06612 +594.4 1004. 4.116 0.414 69.4706 1.12273 +594.4 1004. 4.29 0.094 74.9407 2.44327 +594.4 1004. 4.478 0.1 79.0313 2.49228 +594.4 1004. 4.679 0.107 82.048 2.48185 +594.4 1004. 4.894 0.114 81.0999 2.42708 +594.4 1004. 5.123 0.122 82.5785 2.48174 +594.4 1004. 5.37 0.131 88.018 2.55143 +594.4 1004. 5.634 0.141 96.5891 2.60168 +594.4 1004. 5.919 0.152 94.2359 2.57472 +594.4 1004. 6.226 0.164 97.1229 2.60062 +594.4 1004. 6.558 0.177 98.8045 2.64776 +594.4 1004. 6.917 0.192 100.087 2.5286 +594.4 1004. 7.307 0.208 96.914 2.61453 +594.4 1004. 7.731 0.227 103.565 2.68078 +594.4 1004. 8.192 0.248 109.525 2.72118 +594.4 1004. 8.697 0.271 108.769 2.67189 +594.4 1004. 9.25 0.297 87.9736 2.47637 +594.4 1004. 9.858 0.327 66.0161 2.19661 +594.4 1004. 10.528 0.362 44.3656 1.98794 +594.4 1004. 11.269 0.401 27.3302 1.79874 +594.4 1004. 12.092 0.446 16.1816 1.69695 +594.4 1004. 13.01 0.498 11.8826 1.60857 +594.4 1004. 14.037 0.558 7.12987 1.56461 +684.2 1231. 1.104 0.033 0.03568 0.0561467 +684.2 1231. 1.173 0.058 0.04578 0.052946 +684.2 1231. 1.3 0.073 0.49916 0.0616158 +684.2 1231. 1.454 0.086 1.44636 0.077278 +684.2 1231. 1.638 0.103 2.31948 0.0882252 +684.2 1231. 1.859 0.125 3.0953 0.0996266 +684.2 1231. 2.128 0.153 3.70693 0.106953 +684.2 1231. 2.461 0.19 4.18515 0.112566 +684.2 1231. 2.879 0.241 4.61621 0.119139 +684.2 1231. 3.414 0.312 5.69271 0.130203 +684.2 1231. 4.116 0.414 7.05613 0.138058 +684.2 1231. 4.29 0.094 7.74056 0.304251 +684.2 1231. 4.478 0.1 7.71656 0.305614 +684.2 1231. 4.679 0.107 8.48339 0.309481 +684.2 1231. 4.894 0.114 8.66585 0.300559 +684.2 1231. 5.123 0.122 8.21784 0.304524 +684.2 1231. 5.37 0.131 8.5949 0.316595 +684.2 1231. 5.634 0.141 10.0776 0.325374 +684.2 1231. 5.919 0.152 9.67899 0.322921 +684.2 1231. 6.226 0.164 10.1076 0.32909 +684.2 1231. 6.558 0.177 10.0964 0.327608 +684.2 1231. 6.917 0.192 10.2565 0.324964 +684.2 1231. 7.307 0.208 10.8651 0.328804 +684.2 1231. 7.731 0.227 10.7333 0.335314 +684.2 1231. 8.192 0.248 10.8599 0.346119 +684.2 1231. 8.697 0.271 10.9425 0.334287 +684.2 1231. 9.25 0.297 7.93639 0.3016 +684.2 1231. 9.858 0.327 6.45623 0.275498 +684.2 1231. 10.528 0.362 4.67873 0.250171 +ENDDATA 183 +ENDSUBENT 193 +SUBENT 14021004 20050701 20050909 1336 +BIB 4 5 +REACTION (77-IR-193(N,INL)77-IR-193,PAR,SIG,G,REL) +EN-SEC (E,G) Transition gamma ray + (LVL-INI,77-IR-193) Initial level +ERR-ANALYS (DATA-ERR) No information +STATUS Data received in tables from the author +ENDBIB 5 +NOCOMMON 0 0 +DATA 6 157 +E LVL-INI EN EN-RSL DATA DATA-ERR +KEV KEV MEV MEV ARB-UNITS ARB-UNITS +180.1 180.0 0.213 0.008 0.214284 0.0595232 +180.1 180.0 0.229 0.008 0.251165 0.0627912 +180.1 180.0 0.246 0.009 0.244627 0.0612032 +180.1 180.0 0.265 0.011 0.757824 0.0873955 +180.1 180.0 0.287 0.012 1.30621 0.114797 +180.1 180.0 0.312 0.013 2.11277 0.143017 +180.1 180.0 0.339 0.015 3.60454 0.180944 +180.1 180.0 0.371 0.017 5.32339 0.221839 +180.1 180.0 0.408 0.02 5.49887 0.226861 +180.1 180.0 0.45 0.023 7.00583 0.245591 +180.1 180.0 0.499 0.027 7.81271 0.24682 +180.1 180.0 0.556 0.032 7.63456 0.238757 +180.1 180.0 0.624 0.038 8.92514 0.241451 +180.1 180.0 0.705 0.046 8.0316 0.231648 +180.1 180.0 0.804 0.056 8.53639 0.232074 +180.1 180.0 0.925 0.069 8.91106 0.231208 +180.1 180.0 1.075 0.086 8.43875 0.227137 +180.1 180.0 1.104 0.033 8.54932 0.285614 +180.1 180.0 1.173 0.058 8.65513 0.288304 +180.1 180.0 1.3 0.073 9.46795 0.290945 +180.1 180.0 1.454 0.086 9.87022 0.298573 +180.1 180.0 1.638 0.103 10.3551 0.302156 +180.1 180.0 1.859 0.125 9.4994 0.301804 +180.1 180.0 2.128 0.153 9.82186 0.309427 +180.1 180.0 2.461 0.19 9.42169 0.311494 +180.1 180.0 2.879 0.241 8.85625 0.317579 +180.1 180.0 3.414 0.312 8.43819 0.322152 +180.1 180.0 4.116 0.414 7.90633 0.309294 +180.1 180.0 4.29 0.094 7.6931 0.660948 +180.1 180.0 4.478 0.1 7.29477 0.649728 +180.1 180.0 4.679 0.107 7.38414 0.661831 +180.1 180.0 4.894 0.114 7.57185 0.649157 +180.1 180.0 5.123 0.122 6.19972 0.649241 +180.1 180.0 5.37 0.131 5.55471 0.652821 +180.1 180.0 5.634 0.141 7.26607 0.659208 +180.1 180.0 5.919 0.152 6.10009 0.657379 +180.1 180.0 6.226 0.164 5.84888 0.664726 +180.1 180.0 6.558 0.177 6.2319 0.680131 +180.1 180.0 6.917 0.192 4.66482 0.639532 +180.1 180.0 7.307 0.208 5.78423 0.684306 +180.1 180.0 7.731 0.227 5.86642 0.705391 +180.1 180.0 8.192 0.248 5.06322 0.715834 +180.1 180.0 8.697 0.271 5.36613 0.726087 +180.1 180.0 9.25 0.297 3.68891 0.69602 +180.1 180.0 9.858 0.327 3.56882 0.670242 +180.1 180.0 10.528 0.362 2.63295 0.668062 +180.1 180.0 11.269 0.401 1.20247 0.654918 +180.1 180.0 12.092 0.446 2.62463 0.695832 +180.1 180.0 13.01 0.498 2.5307 0.710871 +180.1 180.0 14.037 0.558 1.35462 0.719118 +269.5 833. 1.104 0.033 0.644109 0.0734426 +269.5 833. 1.173 0.058 1.02526 0.0806323 +269.5 833. 1.3 0.073 1.40615 0.0878846 +269.5 833. 1.454 0.086 1.86953 0.09167 +269.5 833. 1.638 0.103 2.67994 0.101551 +269.5 833. 1.859 0.125 3.10356 0.107345 +269.5 833. 2.128 0.153 4.16057 0.117274 +269.5 833. 2.461 0.19 4.99893 0.125432 +269.5 833. 2.879 0.241 5.43545 0.130877 +269.5 833. 3.414 0.312 6.48983 0.141024 +269.5 833. 4.116 0.414 7.37314 0.142165 +269.5 833. 4.29 0.094 8.02698 0.31473 +269.5 833. 4.478 0.1 7.78025 0.304399 +269.5 833. 4.679 0.107 7.82453 0.314554 +269.5 833. 4.894 0.114 8.45143 0.308035 +269.5 833. 5.123 0.122 8.61481 0.314494 +269.5 833. 5.37 0.131 8.55826 0.319619 +269.5 833. 5.634 0.141 8.96128 0.311865 +269.5 833. 5.919 0.152 8.74178 0.315985 +269.5 833. 6.226 0.164 8.06299 0.318701 +269.5 833. 6.558 0.177 9.35778 0.337545 +269.5 833. 6.917 0.192 9.45824 0.323875 +269.5 833. 7.307 0.208 9.33492 0.340041 +269.5 833. 7.731 0.227 10.25 0.348777 +269.5 833. 8.192 0.248 9.19447 0.349028 +269.5 833. 8.697 0.271 8.98757 0.357202 +269.5 833. 9.25 0.297 6.72005 0.328385 +269.5 833. 9.858 0.327 4.44677 0.301024 +269.5 833. 10.528 0.362 2.80407 0.288148 +269.5 833. 11.269 0.401 2.41106 0.277295 +269.5 833. 12.092 0.446 2.19102 0.283229 +269.5 833. 13.01 0.498 1.77377 0.286293 +269.5 833. 14.037 0.558 1.96932 0.292836 +357.8 358.0 0.339 0.015 0.0213787 0.00801701 +357.8 358.0 0.371 0.017 0.860168 0.0351459 +357.8 358.0 0.408 0.02 1.7831 0.046245 +357.8 358.0 0.45 0.023 2.56279 0.0521606 +357.8 358.0 0.499 0.027 3.48939 0.0561971 +357.8 358.0 0.556 0.032 3.49883 0.0540678 +357.8 358.0 0.624 0.038 4.32828 0.0559041 +357.8 358.0 0.705 0.046 4.63402 0.0553722 +357.8 358.0 0.804 0.056 4.91234 0.0546889 +357.8 358.0 0.925 0.069 5.47737 0.0550433 +357.8 358.0 1.075 0.086 5.90609 0.0546095 +357.8 358.0 1.104 0.033 5.88449 0.0685237 +357.8 358.0 1.173 0.058 6.4104 0.0694365 +357.8 358.0 1.3 0.073 6.54874 0.0697346 +357.8 358.0 1.454 0.086 6.74417 0.0694883 +357.8 358.0 1.638 0.103 7.02306 0.0692456 +357.8 358.0 1.859 0.125 7.08115 0.0689934 +357.8 358.0 2.128 0.153 7.65691 0.0720536 +357.8 358.0 2.461 0.19 8.20309 0.0739307 +357.8 358.0 2.879 0.241 8.59471 0.0760612 +357.8 358.0 3.414 0.312 9.20793 0.0782394 +357.8 358.0 4.116 0.414 9.22772 0.0761699 +357.8 358.0 4.29 0.094 9.46929 0.166449 +357.8 358.0 4.478 0.1 9.24473 0.161651 +357.8 358.0 4.679 0.107 9.77573 0.166602 +357.8 358.0 4.894 0.114 9.29793 0.161593 +357.8 358.0 5.123 0.122 9.16038 0.161787 +357.8 358.0 5.37 0.131 9.39967 0.164369 +357.8 358.0 5.634 0.141 9.50763 0.161163 +357.8 358.0 5.919 0.152 8.97088 0.159813 +357.8 358.0 6.226 0.164 9.22777 0.163075 +357.8 358.0 6.558 0.177 9.43458 0.167899 +357.8 358.0 6.917 0.192 8.56245 0.159734 +357.8 358.0 7.307 0.208 8.95942 0.167268 +357.8 358.0 7.731 0.227 8.67937 0.164624 +357.8 358.0 8.192 0.248 8.93452 0.172977 +357.8 358.0 8.697 0.271 7.99111 0.170299 +357.8 358.0 9.25 0.297 6.2469 0.157617 +357.8 358.0 9.858 0.327 4.81802 0.141924 +357.8 358.0 10.528 0.362 3.59249 0.133488 +357.8 358.0 11.269 0.401 2.83551 0.127644 +357.8 358.0 12.092 0.446 2.70365 0.126475 +357.8 358.0 13.01 0.498 2.30363 0.125565 +357.8 358.0 14.037 0.558 1.9627 0.124976 +451.4 930.0 1.104 0.033 0.205936 0.148364 +451.4 930.0 1.173 0.058 0.189236 0.158339 +451.4 930.0 1.859 0.125 0.312497 0.17591 +451.4 930.0 2.128 0.153 0.166761 0.182938 +451.4 930.0 2.461 0.19 0.552254 0.19116 +451.4 930.0 2.879 0.241 0.597204 0.199634 +451.4 930.0 3.414 0.312 1.69215 0.217083 +451.4 930.0 4.116 0.414 2.34947 0.214841 +451.4 930.0 4.29 0.094 2.80129 0.474234 +451.4 930.0 4.478 0.1 2.77325 0.465211 +451.4 930.0 4.679 0.107 2.94513 0.463617 +451.4 930.0 4.894 0.114 3.94953 0.458031 +451.4 930.0 5.123 0.122 4.47992 0.476051 +451.4 930.0 5.37 0.131 4.46721 0.480569 +451.4 930.0 5.634 0.141 4.70131 0.478546 +451.4 930.0 5.919 0.152 5.47978 0.47941 +451.4 930.0 6.226 0.164 5.58069 0.506502 +451.4 930.0 6.558 0.177 6.71942 0.511214 +451.4 930.0 6.917 0.192 7.08589 0.505141 +451.4 930.0 7.307 0.208 8.6118 0.536393 +451.4 930.0 7.731 0.227 8.92176 0.555801 +451.4 930.0 8.192 0.248 9.81052 0.583027 +451.4 930.0 8.697 0.271 10.0514 0.584178 +451.4 930.0 9.25 0.297 8.88066 0.548394 +451.4 930.0 9.858 0.327 8.06426 0.510874 +451.4 930.0 10.528 0.362 6.33901 0.500592 +451.4 930.0 11.269 0.401 3.95401 0.471397 +451.4 930.0 12.092 0.446 3.38407 0.462881 +451.4 930.0 13.01 0.498 3.23486 0.475163 +451.4 930.0 14.037 0.558 2.60951 0.412027 +ENDDATA 159 +ENDSUBENT 169 +ENDENTRY 4 diff --git a/exforall/140/14022.x4 b/exforall/140/14022.x4 new file mode 100644 index 000000000..67fffda4f --- /dev/null +++ b/exforall/140/14022.x4 @@ -0,0 +1,789 @@ +ENTRY 14022 20050706 20050909 1336 +SUBENT 14022001 20050706 20050909 1336 +BIB 10 13 +INSTITUTE (1USALTI) +REFERENCE (C,88MITO,,853,1988) +AUTHOR (W.A.Schier,D.J.Pullen,G.P.Couchell,M.H.Haghighi, + E.S.Jacobs,M.F.Villani,P.R.Bennett) +TITLE Measured composite delayed neutron spectra from fission + of U-235, U-238 and Pu-239 and derived six-group + spectra +FACILITY (ACCEL,1USALTI) +INC-SOURCE (P-LI7) +METHOD (TOF) +SAMPLE No information +DETECTOR (SCIN) Li-6 glass and BC501 liquid scintillators +HISTORY (20050701C) DR +ENDBIB 13 +NOCOMMON 0 0 +ENDSUBENT 16 +SUBENT 14022002 20050706 20050909 1336 +BIB 4 6 +REACTION (94-PU-239(N,F),DL/GRP,DE,N,REL) + For time interval 0.17 to 0.37 sec. +MISC-COL (MISC1) Lower limit of tima interval + (MISC2) Upper limit of tima interval +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 6 +COMMON 3 3 +EN-DUMMY MISC1 MISC2 +EV SEC SEC +0.0253 0.17 0.37 +ENDCOMMON 3 +DATA 2 74 +E DATA +MEV ARB-UNITS + 0.00E+00 1.67E+02 + 6.18E-04 1.27E+02 + 3.02E-03 2.17E+02 + 3.00E-02 8.52E+01 + 3.54E-02 1.18E+02 + 5.22E-02 9.97E+01 + 5.94E-02 1.81E+02 + 7.70E-02 1.39E+02 + 7.77E-02 2.18E+02 + 1.03E-01 1.33E+02 + 1.11E-01 1.76E+02 + 1.21E-01 1.60E+02 + 1.34E-01 1.80E+02 + 1.47E-01 1.59E+02 + 1.61E-01 1.50E+02 + 1.74E-01 1.38E+02 + 1.97E-01 1.30E+02 + 2.03E-01 1.45E+02 + 2.26E-01 1.36E+02 + 2.62E-01 1.35E+02 + 2.73E-01 1.10E+02 + 2.91E-01 1.36E+02 + 3.25E-01 1.12E+02 + 3.44E-01 1.23E+02 + 3.70E-01 1.14E+02 + 4.03E-01 1.10E+02 + 4.13E-01 1.05E+02 + 4.38E-01 1.10E+02 + 4.61E-01 1.06E+02 + 4.78E-01 9.46E+01 + 4.98E-01 8.66E+01 + 5.14E-01 9.25E+01 + 5.34E-01 7.79E+01 + 5.57E-01 7.25E+01 + 5.66E-01 8.04E+01 + 5.86E-01 7.30E+01 + 6.02E-01 7.63E+01 + 6.12E-01 7.29E+01 + 6.25E-01 6.29E+01 + 6.45E-01 6.55E+01 + 6.61E-01 5.02E+01 + 6.90E-01 6.00E+01 + 7.00E-01 6.39E+01 + 7.20E-01 5.72E+01 + 7.30E-01 5.26E+01 + 7.56E-01 5.25E+01 + 7.66E-01 4.58E+01 + 7.85E-01 4.44E+01 + 8.37E-01 3.49E+01 + 8.60E-01 3.35E+01 + 8.86E-01 2.88E+01 + 9.03E-01 3.20E+01 + 9.42E-01 3.25E+01 + 9.81E-01 3.17E+01 + 1.02E+00 2.56E+01 + 1.05E+00 1.81E+01 + 1.09E+00 2.26E+01 + 1.13E+00 2.05E+01 + 1.15E+00 1.45E+01 + 1.19E+00 1.49E+01 + 1.23E+00 1.68E+01 + 1.25E+00 1.07E+01 + 1.27E+00 1.06E+01 + 1.30E+00 1.38E+01 + 1.32E+00 1.18E+01 + 1.35E+00 9.70E+00 + 1.39E+00 1.02E+01 + 1.40E+00 6.85E+00 + 1.47E+00 7.90E+00 + 1.50E+00 3.80E+00 + 1.58E+00 3.48E+00 + 1.60E+00 1.43E+00 + 1.72E+00 9.46E-01 + 1.89E+00 2.36E-01 +ENDDATA 76 +ENDSUBENT 91 +SUBENT 14022003 20050706 20050909 1336 +BIB 4 6 +REACTION (94-PU-239(N,F),DL/GRP,DE,N,REL) + For time interval 0.41 to 0.85 sec. +MISC-COL (MISC1) Lower limit of tima interval + (MISC2) Upper limit of tima interval +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 6 +COMMON 3 3 +EN-DUMMY MISC1 MISC2 +EV SEC SEC +0.0253 0.41 0.85 +ENDCOMMON 3 +DATA 2 65 +E DATA +MEV ARB-UNITS + 0.00E+00 1.93E+02 + 2.54E-02 3.07E+01 + 4.46E-02 4.77E+01 + 6.62E-02 1.21E+02 + 7.84E-02 1.70E+02 + 1.11E-01 1.32E+02 + 1.20E-01 1.68E+02 + 1.46E-01 1.44E+02 + 1.53E-01 1.57E+02 + 1.69E-01 1.54E+02 + 1.95E-01 1.57E+02 + 2.01E-01 1.67E+02 + 2.11E-01 1.36E+02 + 2.37E-01 1.25E+02 + 2.37E-01 1.46E+02 + 2.50E-01 1.31E+02 + 2.76E-01 1.32E+02 + 2.92E-01 1.30E+02 + 3.02E-01 1.21E+02 + 3.25E-01 1.31E+02 + 3.35E-01 1.14E+02 + 3.61E-01 1.14E+02 + 3.83E-01 1.18E+02 + 3.87E-01 1.09E+02 + 4.06E-01 1.18E+02 + 4.26E-01 1.04E+02 + 4.58E-01 1.04E+02 + 4.75E-01 9.65E+01 + 4.97E-01 9.71E+01 + 5.04E-01 8.96E+01 + 5.33E-01 9.97E+01 + 5.52E-01 8.33E+01 + 5.66E-01 7.02E+01 + 5.69E-01 8.25E+01 + 6.04E-01 7.83E+01 + 6.47E-01 6.31E+01 + 6.86E-01 6.37E+01 + 7.08E-01 5.88E+01 + 7.18E-01 5.20E+01 + 7.54E-01 5.19E+01 + 7.90E-01 4.42E+01 + 8.32E-01 4.14E+01 + 8.74E-01 2.96E+01 + 9.16E-01 2.88E+01 + 9.39E-01 3.21E+01 + 9.75E-01 2.66E+01 + 1.00E+00 2.30E+01 + 1.05E+00 1.88E+01 + 1.09E+00 1.94E+01 + 1.14E+00 2.06E+01 + 1.17E+00 1.37E+01 + 1.21E+00 1.15E+01 + 1.24E+00 1.00E+01 + 1.26E+00 1.27E+01 + 1.30E+00 7.85E+00 + 1.34E+00 8.43E+00 + 1.37E+00 1.10E+01 + 1.40E+00 7.57E+00 + 1.44E+00 8.14E+00 + 1.46E+00 3.96E+00 + 1.53E+00 4.43E+00 + 1.55E+00 3.02E+00 + 1.61E+00 7.87E-01 + 1.67E+00 1.31E+00 + 1.69E+00 5.62E-01 +ENDDATA 67 +ENDSUBENT 82 +SUBENT 14022004 20050706 20050909 1336 +BIB 4 6 +REACTION (94-PU-239(N,F),DL/GRP,DE,N,REL) + For time interval 0.79 to 1.25 sec. +MISC-COL (MISC1) Lower limit of tima interval + (MISC2) Upper limit of tima interval +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 6 +COMMON 3 3 +EN-DUMMY MISC1 MISC2 +EV SEC SEC +0.0253 0.79 1.25 +ENDCOMMON 3 +DATA 2 57 +E DATA +MEV ARB-UNITS + 0.00E+00 2.00E+02 + 1.92E-02 5.88E+00 + 2.06E-02 6.43E+01 + 4.19E-02 1.10E+02 + 6.19E-02 9.19E+01 + 7.92E-02 1.60E+02 + 9.38E-02 1.05E+02 + 9.88E-02 1.53E+02 + 1.40E-01 1.60E+02 + 1.47E-01 1.67E+02 + 1.63E-01 1.51E+02 + 1.83E-01 1.55E+02 + 1.86E-01 1.47E+02 + 2.06E-01 1.44E+02 + 2.32E-01 1.25E+02 + 2.45E-01 1.32E+02 + 2.62E-01 1.18E+02 + 2.84E-01 1.20E+02 + 2.91E-01 1.11E+02 + 3.33E-01 1.12E+02 + 3.65E-01 1.17E+02 + 3.88E-01 1.03E+02 + 4.08E-01 1.02E+02 + 4.24E-01 1.08E+02 + 4.40E-01 9.61E+01 + 4.56E-01 1.02E+02 + 4.79E-01 9.39E+01 + 4.99E-01 9.78E+01 + 5.15E-01 8.58E+01 + 5.22E-01 9.44E+01 + 5.45E-01 7.77E+01 + 5.70E-01 8.62E+01 + 5.90E-01 7.35E+01 + 6.10E-01 7.01E+01 + 6.33E-01 6.33E+01 + 6.81E-01 5.98E+01 + 7.21E-01 5.36E+01 + 7.66E-01 5.14E+01 + 7.86E-01 4.47E+01 + 8.05E-01 4.46E+01 + 8.21E-01 4.78E+01 + 8.54E-01 4.10E+01 + 8.83E-01 3.62E+01 + 9.32E-01 2.94E+01 + 9.77E-01 2.78E+01 + 1.03E+00 2.69E+01 + 1.06E+00 2.01E+01 + 1.11E+00 1.85E+01 + 1.17E+00 1.76E+01 + 1.22E+00 1.34E+01 + 1.27E+00 1.18E+01 + 1.32E+00 9.62E+00 + 1.37E+00 7.39E+00 + 1.43E+00 3.79E+00 + 1.47E+00 3.58E+00 + 1.52E+00 4.01E+00 + 1.55E+00 5.40E-01 +ENDDATA 59 +ENDSUBENT 74 +SUBENT 14022005 20050706 20050909 1336 +BIB 4 6 +REACTION (94-PU-239(N,F),DL/GRP,DE,N,REL) + For time interval 1.2 to 1.9 sec. +MISC-COL (MISC1) Lower limit of tima interval + (MISC2) Upper limit of tima interval +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 6 +COMMON 3 3 +EN-DUMMY MISC1 MISC2 +EV SEC SEC +0.0253 1.2 1.9 +ENDCOMMON 3 +DATA 2 56 +E DATA +MEV ARB-UNITS + 0.00E+00 6.08E+01 + 4.03E-02 2.34E+01 + 4.74E-02 1.10E+02 + 6.86E-02 8.29E+01 + 7.66E-02 1.54E+02 + 9.64E-02 1.01E+02 + 1.01E-01 1.27E+02 + 1.17E-01 1.22E+02 + 1.31E-01 1.02E+02 + 1.48E-01 1.49E+02 + 1.64E-01 1.39E+02 + 1.90E-01 1.44E+02 + 2.00E-01 1.36E+02 + 2.26E-01 1.33E+02 + 2.39E-01 1.36E+02 + 2.53E-01 1.22E+02 + 2.62E-01 1.33E+02 + 2.84E-01 1.41E+02 + 2.98E-01 1.24E+02 + 3.33E-01 1.24E+02 + 3.44E-01 1.06E+02 + 3.66E-01 1.15E+02 + 4.00E-01 9.69E+01 + 4.09E-01 1.00E+02 + 4.54E-01 1.01E+02 + 4.81E-01 9.75E+01 + 5.14E-01 8.15E+01 + 5.40E-01 8.49E+01 + 5.62E-01 8.42E+01 + 5.66E-01 7.87E+01 + 5.95E-01 7.66E+01 + 6.02E-01 6.76E+01 + 6.41E-01 6.61E+01 + 6.58E-01 5.85E+01 + 6.93E-01 5.91E+01 + 7.19E-01 5.84E+01 + 7.49E-01 5.00E+01 + 7.94E-01 5.48E+01 + 8.24E-01 4.09E+01 + 8.53E-01 3.88E+01 + 8.95E-01 3.74E+01 + 9.18E-01 3.53E+01 + 9.53E-01 3.52E+01 + 9.83E-01 3.10E+01 + 1.03E+00 2.68E+01 + 1.09E+00 2.53E+01 + 1.10E+00 1.84E+01 + 1.13E+00 1.63E+01 + 1.18E+00 1.69E+01 + 1.19E+00 9.99E+00 + 1.28E+00 1.19E+01 + 1.30E+00 7.75E+00 + 1.38E+00 8.32E+00 + 1.39E+00 4.85E+00 + 1.45E+00 3.38E+00 + 1.53E+00 3.25E+00 +ENDDATA 58 +ENDSUBENT 73 +SUBENT 14022006 20050706 20050909 1336 +BIB 4 6 +REACTION (94-PU-239(N,F),DL/GRP,DE,N,REL) + For time interval 2.1 to 3.9 sec. +MISC-COL (MISC1) Lower limit of tima interval + (MISC2) Upper limit of tima interval +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 6 +COMMON 3 3 +EN-DUMMY MISC1 MISC2 +EV SEC SEC +0.0253 2.1 3.9 +ENDCOMMON 3 +DATA 2 53 +E DATA +MEV ARB-UNITS + 6.37E-03 1.55E+02 + 2.89E-02 4.20E+00 + 3.17E-02 1.26E+02 + 5.02E-02 1.01E+02 + 5.65E-02 1.42E+02 + 8.22E-02 1.48E+02 + 8.39E-02 1.27E+02 + 1.01E-01 1.48E+02 + 1.02E-01 1.36E+02 + 1.12E-01 1.81E+02 + 1.39E-01 1.70E+02 + 1.54E-01 1.84E+02 + 1.61E-01 1.76E+02 + 1.84E-01 1.76E+02 + 2.30E-01 1.40E+02 + 2.49E-01 1.47E+02 + 2.68E-01 1.45E+02 + 2.86E-01 1.34E+02 + 2.91E-01 1.45E+02 + 3.16E-01 1.29E+02 + 3.25E-01 1.36E+02 + 3.32E-01 1.25E+02 + 3.63E-01 1.15E+02 + 3.75E-01 1.18E+02 + 4.12E-01 1.18E+02 + 4.35E-01 1.09E+02 + 4.55E-01 1.02E+02 + 4.79E-01 9.16E+01 + 5.10E-01 7.49E+01 + 5.49E-01 7.49E+01 + 5.89E-01 6.59E+01 + 6.02E-01 6.73E+01 + 6.53E-01 5.41E+01 + 6.89E-01 5.41E+01 + 7.05E-01 4.79E+01 + 7.55E-01 4.44E+01 + 7.78E-01 3.89E+01 + 8.28E-01 2.77E+01 + 8.61E-01 2.78E+01 + 8.84E-01 3.13E+01 + 9.04E-01 2.71E+01 + 9.59E-01 2.64E+01 + 9.82E-01 2.30E+01 + 1.01E+00 1.60E+01 + 1.05E+00 1.61E+01 + 1.07E+00 1.33E+01 + 1.11E+00 1.33E+01 + 1.14E+00 9.21E+00 + 1.23E+00 7.88E+00 + 1.35E+00 5.18E+00 + 1.39E+00 3.82E+00 + 1.42E+00 2.45E+00 + 1.54E+00 1.14E+00 +ENDDATA 55 +ENDSUBENT 70 +SUBENT 14022007 20050706 20050909 1336 +BIB 4 6 +REACTION (94-PU-239(N,F),DL/GRP,DE,N,REL) + For time interval 4.7 to 10.2 sec. +MISC-COL (MISC1) Lower limit of tima interval + (MISC2) Upper limit of tima interval +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 6 +COMMON 3 3 +EN-DUMMY MISC1 MISC2 +EV SEC SEC +0.0253 4.7 10.2 +ENDCOMMON 3 +DATA 2 47 +E DATA +MEV ARB-UNITS + 9.35E-03 1.34E+02 + 3.68E-02 3.22E+01 + 4.51E-02 9.39E+01 + 6.30E-02 1.59E+02 + 8.07E-02 9.95E+01 + 8.82E-02 1.30E+02 + 1.02E-01 1.51E+02 + 1.19E-01 1.47E+02 + 1.48E-01 2.00E+02 + 1.61E-01 1.62E+02 + 1.76E-01 1.80E+02 + 1.99E-01 1.74E+02 + 2.16E-01 1.58E+02 + 2.26E-01 1.63E+02 + 2.49E-01 1.56E+02 + 2.72E-01 1.59E+02 + 2.81E-01 1.69E+02 + 3.15E-01 1.47E+02 + 3.55E-01 1.49E+02 + 4.02E-01 1.31E+02 + 4.16E-01 1.18E+02 + 4.32E-01 1.23E+02 + 4.59E-01 1.11E+02 + 4.80E-01 9.78E+01 + 5.04E-01 7.96E+01 + 5.23E-01 8.73E+01 + 5.40E-01 7.46E+01 + 5.67E-01 6.34E+01 + 6.03E-01 6.12E+01 + 6.30E-01 5.21E+01 + 6.64E-01 4.44E+01 + 6.96E-01 4.71E+01 + 7.53E-01 3.59E+01 + 7.85E-01 3.94E+01 + 7.92E-01 3.09E+01 + 8.32E-01 2.95E+01 + 8.62E-01 2.18E+01 + 9.04E-01 2.24E+01 + 9.70E-01 1.33E+01 + 1.00E+00 1.32E+01 + 1.03E+00 9.04E+00 + 1.13E+00 8.97E+00 + 1.22E+00 8.19E+00 + 1.24E+00 1.16E+00 + 1.30E+00 1.12E+00 + 1.39E+00 1.75E+00 + 1.53E+00 1.65E+00 +ENDDATA 49 +ENDSUBENT 64 +SUBENT 14022008 20050706 20050909 1336 +BIB 4 6 +REACTION (94-PU-239(N,F),DL/GRP,DE,N,REL) + For time interval 12.5 to 29.0 sec. +MISC-COL (MISC1) Lower limit of tima interval + (MISC2) Upper limit of tima interval +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 6 +COMMON 3 3 +EN-DUMMY MISC1 MISC2 +EV SEC SEC +0.0253 12.5 29.0 +ENDCOMMON 3 +DATA 2 35 +E DATA +MEV ARB-UNITS + 2.80E-01 1.21E+02 + 3.02E-01 1.39E+02 + 3.19E-01 1.22E+02 + 3.23E-01 1.56E+02 + 3.43E-01 1.56E+02 + 3.85E-01 1.58E+02 + 4.07E-01 1.26E+02 + 4.34E-01 1.16E+02 + 4.40E-01 1.29E+02 + 4.56E-01 1.34E+02 + 4.70E-01 1.18E+02 + 4.98E-01 9.46E+01 + 5.20E-01 1.06E+02 + 5.27E-01 9.89E+01 + 5.57E-01 9.39E+01 + 5.64E-01 8.69E+01 + 5.84E-01 8.12E+01 + 5.89E-01 6.43E+01 + 6.01E-01 7.27E+01 + 6.58E-01 6.07E+01 + 6.90E-01 6.14E+01 + 7.39E-01 6.14E+01 + 7.70E-01 4.73E+01 + 7.99E-01 4.94E+01 + 8.63E-01 2.89E+01 + 9.05E-01 3.46E+01 + 9.35E-01 2.82E+01 + 9.42E-01 2.19E+01 + 1.02E+00 1.90E+01 + 1.09E+00 1.76E+01 + 1.15E+00 9.89E+00 + 1.23E+00 4.94E+00 + 1.30E+00 2.12E+00 + 1.35E+00 7.06E-01 + 1.41E+00 1.41E+00 +ENDDATA 37 +ENDSUBENT 52 +SUBENT 14022009 20050706 20050909 1336 +BIB 5 8 +REACTION (92-U-238(N,F),DL/GRP,DE,N,REL) + For time interval 0.79 to 1.25 sec. +MISC-COL (MISC1) Lower limit of tima interval + (MISC2) Upper limit of tima interval +ERR-ANALYS No information +COMMENT Incident neutron energy given as "fast neutrons" in + the text +STATUS (CURVE) Data read from Fig. 4 +ENDBIB 8 +COMMON 3 3 +EN-MIN-APX MISC1 MISC2 +MEV SEC SEC +1. 0.79 1.25 +ENDCOMMON 3 +DATA 2 96 +E DATA +MEV ARB-UNITS + 1.42E-02 1.60E+02 + 1.97E-02 4.85E+01 + 3.48E-02 7.69E+01 + 4.91E-02 6.81E+01 + 6.20E-02 8.44E+01 + 7.95E-02 1.21E+02 + 8.72E-02 1.33E+02 + 9.40E-02 1.07E+02 + 1.10E-01 1.19E+02 + 1.34E-01 1.23E+02 + 1.44E-01 1.57E+02 + 1.47E-01 1.43E+02 + 1.66E-01 1.47E+02 + 1.83E-01 1.49E+02 + 1.86E-01 1.33E+02 + 1.89E-01 1.38E+02 + 2.11E-01 1.31E+02 + 2.22E-01 1.37E+02 + 2.59E-01 1.14E+02 + 2.79E-01 1.04E+02 + 3.09E-01 1.09E+02 + 3.28E-01 1.07E+02 + 3.50E-01 1.05E+02 + 3.59E-01 9.98E+01 + 3.70E-01 1.02E+02 + 3.87E-01 9.57E+01 + 4.19E-01 1.03E+02 + 4.42E-01 9.85E+01 + 4.69E-01 1.00E+02 + 4.88E-01 1.04E+02 + 5.13E-01 9.68E+01 + 5.36E-01 8.56E+01 + 5.61E-01 8.61E+01 + 5.94E-01 7.64E+01 + 6.14E-01 6.85E+01 + 6.34E-01 6.67E+01 + 6.53E-01 6.76E+01 + 6.61E-01 5.88E+01 + 6.80E-01 6.54E+01 + 7.08E-01 5.84E+01 + 7.39E-01 6.08E+01 + 7.69E-01 5.48E+01 + 7.91E-01 5.43E+01 + 8.25E-01 4.32E+01 + 8.47E-01 4.32E+01 + 8.69E-01 3.86E+01 + 8.89E-01 4.00E+01 + 9.22E-01 3.96E+01 + 9.66E-01 4.16E+01 + 9.96E-01 4.11E+01 + 1.02E+00 3.75E+01 + 1.05E+00 3.42E+01 + 1.06E+00 2.96E+01 + 1.10E+00 2.78E+01 + 1.14E+00 2.74E+01 + 1.18E+00 2.56E+01 + 1.23E+00 2.43E+01 + 1.25E+00 2.20E+01 + 1.29E+00 2.06E+01 + 1.33E+00 1.88E+01 + 1.40E+00 1.75E+01 + 1.45E+00 1.62E+01 + 1.50E+00 1.44E+01 + 1.53E+00 1.12E+01 + 1.61E+00 9.53E+00 + 1.65E+00 1.05E+01 + 1.70E+00 8.28E+00 + 1.75E+00 8.36E+00 + 1.82E+00 8.46E+00 + 2.02E+00 4.72E+00 + 2.05E+00 4.35E+00 + 2.08E+00 4.23E+00 + 2.11E+00 4.24E+00 + 2.14E+00 4.07E+00 + 2.19E+00 4.01E+00 + 2.23E+00 3.06E+00 + 2.28E+00 3.02E+00 + 2.30E+00 2.65E+00 + 2.37E+00 2.63E+00 + 2.40E+00 2.09E+00 + 2.48E+00 1.98E+00 + 2.53E+00 1.89E+00 + 2.64E+00 1.76E+00 + 2.70E+00 1.67E+00 + 2.72E+00 1.27E+00 + 2.81E+00 1.23E+00 + 2.83E+00 1.07E+00 + 2.95E+00 9.86E-01 + 3.08E+00 8.29E-01 + 3.10E+00 5.28E-01 + 3.24E+00 4.64E-01 + 3.25E+00 3.26E-01 + 3.38E+00 3.31E-01 + 3.47E+00 2.65E-01 + 3.48E+00 1.73E-01 + 3.75E+00 2.07E-01 +ENDDATA 98 +ENDSUBENT 115 +SUBENT 14022010 20050706 20050909 1336 +BIB 5 8 +REACTION (92-U-238(N,F),DL/GRP,DE,N,REL) + For time interval 1.2 to 1.9 sec. +MISC-COL (MISC1) Lower limit of tima interval + (MISC2) Upper limit of tima interval +ERR-ANALYS No information +COMMENT Incident neutron energy given as "fast neutrons" in + the text +STATUS (CURVE) Data read from Fig. 4 +ENDBIB 8 +COMMON 3 3 +EN-MIN-APX MISC1 MISC2 +MEV SEC SEC +1. 1.2 1.9 +ENDCOMMON 3 +DATA 2 111 +E DATA +MEV ARB-UNITS + 1.96E-02 9.55E+01 + 2.73E-02 8.43E+00 + 4.07E-02 2.33E+01 + 6.34E-02 1.10E+02 + 8.56E-02 1.00E+02 + 9.62E-02 1.17E+02 + 1.45E-01 1.27E+02 + 1.53E-01 1.41E+02 + 1.72E-01 1.48E+02 + 1.83E-01 1.39E+02 + 2.08E-01 1.47E+02 + 2.42E-01 1.09E+02 + 2.67E-01 1.03E+02 + 2.83E-01 1.05E+02 + 2.95E-01 1.00E+02 + 3.11E-01 1.05E+02 + 3.33E-01 9.98E+01 + 3.50E-01 1.03E+02 + 3.58E-01 9.93E+01 + 3.72E-01 1.01E+02 + 3.80E-01 9.75E+01 + 4.02E-01 9.66E+01 + 4.24E-01 9.81E+01 + 4.35E-01 9.57E+01 + 4.52E-01 1.01E+02 + 4.71E-01 1.01E+02 + 4.90E-01 1.06E+02 + 5.10E-01 9.49E+01 + 5.51E-01 8.94E+01 + 5.73E-01 8.15E+01 + 5.84E-01 8.29E+01 + 6.15E-01 7.22E+01 + 6.37E-01 7.37E+01 + 6.62E-01 6.49E+01 + 6.87E-01 6.44E+01 + 7.17E-01 6.12E+01 + 7.58E-01 5.99E+01 + 8.05E-01 5.39E+01 + 8.27E-01 5.44E+01 + 8.47E-01 4.88E+01 + 8.77E-01 4.52E+01 + 9.21E-01 4.34E+01 + 9.63E-01 4.25E+01 + 9.87E-01 4.49E+01 + 1.01E+00 4.68E+01 + 1.05E+00 4.40E+01 + 1.07E+00 4.03E+01 + 1.09E+00 3.80E+01 + 1.12E+00 3.30E+01 + 1.14E+00 3.11E+01 + 1.16E+00 2.88E+01 + 1.20E+00 2.70E+01 + 1.23E+00 2.61E+01 + 1.27E+00 2.53E+01 + 1.30E+00 2.35E+01 + 1.35E+00 2.17E+01 + 1.40E+00 1.85E+01 + 1.46E+00 1.86E+01 + 1.50E+00 1.77E+01 + 1.53E+00 1.64E+01 + 1.58E+00 1.50E+01 + 1.63E+00 1.19E+01 + 1.67E+00 1.10E+01 + 1.73E+00 9.73E+00 + 1.82E+00 9.40E+00 + 1.91E+00 8.14E+00 + 2.01E+00 6.42E+00 + 2.04E+00 6.35E+00 + 2.05E+00 5.63E+00 + 2.09E+00 5.61E+00 + 2.13E+00 4.80E+00 + 2.18E+00 4.67E+00 + 2.21E+00 4.67E+00 + 2.25E+00 4.60E+00 + 2.27E+00 4.51E+00 + 2.31E+00 4.33E+00 + 2.33E+00 4.24E+00 + 2.36E+00 4.22E+00 + 2.39E+00 3.10E+00 + 2.41E+00 2.99E+00 + 2.47E+00 2.90E+00 + 2.49E+00 2.46E+00 + 2.53E+00 2.49E+00 + 2.55E+00 2.35E+00 + 2.57E+00 2.35E+00 + 2.59E+00 2.12E+00 + 2.67E+00 2.08E+00 + 2.69E+00 2.02E+00 + 2.70E+00 1.83E+00 + 2.74E+00 1.86E+00 + 2.76E+00 1.72E+00 + 2.81E+00 1.73E+00 + 2.83E+00 1.47E+00 + 2.94E+00 1.42E+00 + 2.96E+00 1.25E+00 + 3.08E+00 1.24E+00 + 3.10E+00 1.06E+00 + 3.22E+00 1.10E+00 + 3.24E+00 8.01E-01 + 3.37E+00 8.17E-01 + 3.39E+00 6.09E-01 + 3.50E+00 6.22E-01 + 3.52E+00 5.31E-01 + 3.65E+00 5.46E-01 + 3.66E+00 4.31E-01 + 3.73E+00 4.16E-01 + 3.75E+00 5.59E-01 + 3.90E+00 6.00E-01 + 3.91E+00 4.37E-01 + 3.95E+00 4.42E-01 + 3.98E+00 3.76E-01 +ENDDATA 113 +ENDSUBENT 130 +ENDENTRY 10 diff --git a/exforall/140/14023.x4 b/exforall/140/14023.x4 new file mode 100644 index 000000000..08d09c5ef --- /dev/null +++ b/exforall/140/14023.x4 @@ -0,0 +1,582 @@ +ENTRY 14023 20050708 20050909 1336 +SUBENT 14023001 20050708 20050909 1336 +BIB 10 12 +INSTITUTE (1USAORL) +REFERENCE (C,88MITO,,71,1988) +AUTHOR (R.L.Macklin,R.B.Perez,G.DeSaussure,R.W.Ingle) +TITLE High Energy Resolution Measurement of the 238U neutron + capture yield in the energy region between 1 and 100 + keV +FACILITY (LINAC,1USAORL) ORELA +INC-SOURCE Pulsed beam of neutrons +METHOD (TOF) 150 meter flight path +SAMPLE High purity disk of 238U +DETECTOR (SCIN) Large liquid scintillator tank (ORELAST) +HISTORY (20050706C) DR +ENDBIB 12 +NOCOMMON 0 0 +ENDSUBENT 15 +SUBENT 14023002 20050708 20050909 1336 +BIB 4 4 +REACTION (92-U-238(N,G)92-U-239,,SIG) +SAMPLE 0.00309 atoms/barn +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 1 +ENDBIB 4 +COMMON 1 3 +THICKNESS +ATOMS/B +0.00309 +ENDCOMMON 3 +DATA 2 177 +EN DATA +EV B + 2.5414E+03 3.41E-01 + 2.5424E+03 4.17E-01 + 2.5432E+03 5.05E-01 + 2.5445E+03 6.70E-01 + 2.5450E+03 7.58E-01 + 2.5453E+03 1.13E+00 + 2.5457E+03 1.75E+00 + 2.5460E+03 2.37E+00 + 2.5462E+03 3.39E+00 + 2.5465E+03 4.44E+00 + 2.5468E+03 5.66E+00 + 2.5471E+03 6.55E+00 + 2.5473E+03 7.44E+00 + 2.5480E+03 7.57E+00 + 2.5482E+03 7.39E+00 + 2.5486E+03 6.42E+00 + 2.5489E+03 5.32E+00 + 2.5494E+03 4.00E+00 + 2.5499E+03 2.91E+00 + 2.5503E+03 1.99E+00 + 2.5507E+03 1.40E+00 + 2.5512E+03 9.85E-01 + 2.5518E+03 6.97E-01 + 2.5526E+03 5.86E-01 + 2.5532E+03 4.53E-01 + 2.5538E+03 3.31E-01 + 2.5548E+03 5.40E-01 + 2.5566E+03 4.83E-01 + 2.5571E+03 5.60E-01 + 2.5573E+03 9.91E-01 + 2.5576E+03 1.54E+00 + 2.5578E+03 2.73E+00 + 2.5586E+03 6.59E+00 + 2.5586E+03 4.26E+00 + 2.5586E+03 8.36E+00 + 2.5597E+03 9.70E+00 + 2.5599E+03 8.34E+00 + 2.5604E+03 6.94E+00 + 2.5610E+03 5.12E+00 + 2.5612E+03 3.50E+00 + 2.5618E+03 2.31E+00 + 2.5620E+03 1.50E+00 + 2.5632E+03 5.88E-01 + 2.5633E+03 8.64E-01 + 2.5640E+03 4.33E-01 + 2.5652E+03 3.76E-01 + 2.5663E+03 2.98E-01 + 2.5673E+03 1.65E-01 + 2.5682E+03 2.52E-01 + 2.5694E+03 4.83E-01 + 2.5699E+03 2.40E-01 + 2.5718E+03 4.04E-01 + 2.5722E+03 3.15E-01 + 2.5730E+03 2.48E-01 + 2.5740E+03 1.59E-01 + 2.5743E+03 3.14E-01 + 2.5749E+03 4.13E-01 + 2.5754E+03 5.67E-01 + 2.5761E+03 7.21E-01 + 2.5764E+03 5.00E-01 + 2.5770E+03 4.66E-01 + 2.5784E+03 8.41E-01 + 2.5792E+03 1.10E+00 + 2.5792E+03 2.01E+00 + 2.5795E+03 2.99E+00 + 2.5798E+03 4.81E+00 + 2.5802E+03 6.71E+00 + 2.5804E+03 8.40E+00 + 2.5806E+03 9.27E+00 + 2.5811E+03 9.18E+00 + 2.5816E+03 8.02E+00 + 2.5821E+03 6.24E+00 + 2.5826E+03 4.57E+00 + 2.5829E+03 2.90E+00 + 2.5834E+03 1.91E+00 + 2.5837E+03 1.41E+00 + 2.5844E+03 9.35E-01 + 2.5845E+03 6.92E-01 + 2.5857E+03 4.59E-01 + 2.5862E+03 3.70E-01 + 2.5868E+03 4.03E-01 + 2.5874E+03 2.36E-01 + 2.5877E+03 3.69E-01 + 2.5891E+03 3.23E-01 + 2.5900E+03 3.12E-01 + 2.5911E+03 2.00E-01 + 2.5921E+03 3.21E-01 + 2.5928E+03 3.98E-01 + 2.5934E+03 4.64E-01 + 2.5940E+03 5.74E-01 + 2.5945E+03 6.84E-01 + 2.5951E+03 9.70E-01 + 2.5952E+03 1.47E+00 + 2.5955E+03 2.19E+00 + 2.5961E+03 3.38E+00 + 2.5962E+03 4.63E+00 + 2.5965E+03 5.87E+00 + 2.5969E+03 6.89E+00 + 2.5972E+03 7.16E+00 + 2.5976E+03 7.38E+00 + 2.5982E+03 6.55E+00 + 2.5986E+03 5.25E+00 + 2.5991E+03 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2.6217E+03 2.51E+00 + 2.6219E+03 1.15E+00 + 2.6224E+03 7.71E-01 + 2.6231E+03 3.51E-01 + 2.6241E+03 2.06E-01 + 2.6250E+03 3.60E-01 + 2.6258E+03 2.82E-01 + 2.6269E+03 3.70E-01 + 2.6275E+03 2.48E-01 + 2.6284E+03 3.57E-01 + 2.6297E+03 2.13E-01 + 2.6305E+03 3.33E-01 + 2.6311E+03 5.21E-01 + 2.6314E+03 8.30E-01 + 2.6317E+03 1.11E+00 + 2.6320E+03 1.82E+00 + 2.6326E+03 2.12E+00 + 2.6332E+03 2.03E+00 + 2.6335E+03 1.85E+00 + 2.6338E+03 1.59E+00 + 2.6341E+03 1.00E+00 + 2.6349E+03 7.83E-01 + 2.6356E+03 1.02E+00 + 2.6356E+03 1.23E+00 + 2.6377E+03 1.07E+00 + 2.6383E+03 8.13E-01 + 2.6386E+03 5.92E-01 + 2.6393E+03 3.04E-01 + 2.6401E+03 4.25E-01 +ENDDATA 179 +ENDSUBENT 192 +SUBENT 14023003 20050708 20050909 1336 +BIB 4 4 +REACTION (92-U-238(N,G)92-U-239,,SIG) +SAMPLE 0.01236 atoms/barn +ERR-ANALYS (ERR-S) Statistical error +STATUS (CURVE) Data read from Figs. 1 and 2 +ENDBIB 4 +COMMON 1 3 +THICKNESS +ATOMS/B +0.01236 +ENDCOMMON 3 +DATA 3 352 +EN DATA ERR-S +EV B B + 2.5414E+03 1.53E-01 + 2.5434E+03 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2.3646E+04 4.69E-01 2.51E-02 + 2.3650E+04 4.88E-01 2.62E-02 + 2.3654E+04 5.03E-01 2.74E-02 + 2.3658E+04 4.94E-01 2.17E-02 + 2.3661E+04 4.08E-01 2.51E-02 + 2.3664E+04 3.90E-01 2.51E-02 + 2.3668E+04 3.71E-01 2.51E-02 + 2.3672E+04 4.09E-01 2.62E-02 + 2.3676E+04 4.26E-01 2.51E-02 + 2.3679E+04 4.75E-01 2.73E-02 + 2.3683E+04 5.17E-01 2.39E-02 + 2.3687E+04 4.44E-01 2.62E-02 + 2.3692E+04 3.64E-01 2.39E-02 +ENDDATA 354 +ENDSUBENT 367 +ENDENTRY 3 diff --git a/exforall/140/14024.x4 b/exforall/140/14024.x4 new file mode 100644 index 000000000..dc374e944 --- /dev/null +++ b/exforall/140/14024.x4 @@ -0,0 +1,124 @@ +ENTRY 14024 20050708 20050909 1336 +SUBENT 14024001 20050708 20050909 1336 +BIB 10 18 +INSTITUTE (1USAORL) +REFERENCE (C,88MITO,,213,1988) +AUTHOR (J.K.Dickens,D.C.Larson) +TITLE 10,11B(n,xg) reactions for incident neutron energies + between 0.1 and 25 MeV +FACILITY (LINAC,1USAORL) ORELA +INC-SOURCE Pulsed beam of neutrons +METHOD (TOF) 22 meter flight path +SAMPLE - Natural isotopic composition, 54g of metallic boron + in powder form enclosed in a 9 g CH2 bottle, 1.8cm + radius by 5.8cm height + - Isotopically enriched to 95 % in 10B in the same + bottle + - Isotopically enriched to 95 % in 10B in a thin- + walled Al container of 0.5 g, 0.48 cm radius and + 10 cm height +DETECTOR (GE-IN) +HISTORY (20050708C) DR +ENDBIB 18 +NOCOMMON 0 0 +ENDSUBENT 21 +SUBENT 14024002 20050708 20050909 1336 +BIB 4 4 +REACTION (5-B-10(N,INL)5-B-10,PAR,SIG,G) +EN-SEC (E,G) Gamma-ray energy from 5-B-10 decay +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Figs. 1 to 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 5 53 +E EN EN-RSL DATA DATA-ERR +MEV MEV MEV MB MB +0.414 2.71E+00 3.57E-01 2.02E+00 1.46E-01 +0.414 3.44E+00 4.11E-01 7.89E+00 4.34E-01 +0.414 4.26E+00 4.33E-01 1.40E+01 6.90E-01 +0.414 5.14E+00 4.77E-01 1.67E+01 8.25E-01 +0.414 6.07E+00 4.57E-01 1.77E+01 9.75E-01 +0.414 6.97E+00 4.24E-01 1.72E+01 6.56E-01 +0.414 7.82E+00 3.44E-01 1.61E+01 9.78E-01 +0.414 8.60E+00 3.54E-01 1.22E+01 8.84E-01 +0.414 9.41E+00 3.87E-01 8.18E+00 1.02E+00 +0.414 1.01E+01 2.77E-01 9.21E+00 8.76E-01 +0.414 1.08E+01 3.85E-01 8.64E+00 1.13E+00 +0.414 1.16E+01 3.16E-01 6.86E+00 1.10E+00 +0.414 1.28E+01 9.30E-01 5.01E+00 7.16E-01 +0.414 1.43E+01 4.31E-01 4.04E+00 8.33E-01 +0.414 1.74E+01 2.72E+00 4.62E+00 7.19E-01 +0.718 1.06E+00 8.60E-02 1.24E+00 2.31E-01 +0.718 1.40E+00 2.97E-01 5.28E+00 +0.718 1.97E+00 3.42E-01 5.31E+01 +0.718 2.66E+00 3.72E-01 3.67E+01 +0.718 3.41E+00 3.82E-01 4.56E+01 +0.718 4.22E+00 4.17E-01 7.07E+01 +0.718 5.11E+00 4.13E-01 9.32E+01 +0.718 6.00E+00 4.58E-01 8.66E+01 +0.718 6.92E+00 3.78E-01 8.86E+01 +0.718 7.74E+00 3.22E-01 7.05E+01 +0.718 8.51E+00 3.19E-01 5.77E+01 +0.718 9.29E+00 3.48E-01 4.94E+01 +0.718 1.00E+01 4.08E+01 +0.718 1.06E+01 3.93E+01 +0.718 1.14E+01 3.39E+01 +0.718 1.27E+01 8.59E-01 3.03E+01 2.82E+00 +0.718 1.41E+01 5.90E-01 2.71E+01 2.31E+00 +0.718 1.54E+01 8.42E-01 2.22E+01 2.07E+00 +0.718 1.70E+01 8.60E-01 2.24E+01 1.72E+00 +0.718 1.90E+01 1.37E+00 1.68E+01 1.56E+00 +0.718 2.11E+01 9.71E-01 1.51E+01 1.53E+00 +0.718 2.33E+01 1.07E+00 1.21E+01 1.42E+00 +1.022 2.14E+00 2.20E-01 2.31E-01 1.65E-01 +1.022 2.69E+00 3.46E-01 2.75E+00 3.34E-01 +1.022 3.41E+00 3.73E-01 8.18E+00 4.45E-01 +1.022 4.23E+00 4.08E-01 1.35E+01 +1.022 5.11E+00 4.61E-01 1.82E+01 +1.022 6.02E+00 3.94E-01 1.73E+01 +1.022 6.94E+00 4.32E-01 1.88E+01 +1.022 7.77E+00 3.67E-01 1.55E+01 1.13E+00 +1.022 8.49E+00 3.74E-01 9.30E+00 8.60E-01 +1.022 9.37E+00 3.56E-01 8.99E+00 8.30E-01 +1.022 1.00E+01 2.65E-01 9.66E+00 1.27E+00 +1.022 1.08E+01 3.47E-01 7.10E+00 1.07E+00 +1.022 1.16E+01 3.38E-01 7.76E+00 1.10E+00 +1.022 1.28E+01 1.03E+00 5.56E+00 7.32E-01 +1.022 1.42E+01 5.43E-01 2.97E+00 7.67E-01 +1.022 1.72E+01 2.85E+00 3.31E+00 3.38E-01 +ENDDATA 55 +ENDSUBENT 64 +SUBENT 14024003 20050708 20050909 1336 +BIB 4 4 +REACTION (5-B-11(N,INL)5-B-11,PAR,SIG,G) +EN-SEC (E,G) Gamma-ray energy from 5-B-11 decay +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Figs. 4 and 5 +ENDBIB 4 +NOCOMMON 0 0 +DATA 5 20 +E EN EN-RSL DATA DATA-ERR +MEV MEV MEV MB MB +0.478 1.20E+01 7.63E-01 1.81E+01 2.79E+00 +0.478 1.32E+01 5.03E-01 2.19E+01 3.90E+00 +0.478 1.52E+01 1.80E+00 3.26E+01 3.33E+00 +0.478 1.93E+01 2.91E+00 3.32E+01 3.96E+00 +2.125 2.65E+00 3.83E-01 1.10E+01 +2.125 3.40E+00 3.59E-01 2.66E+01 +2.125 4.19E+00 4.42E-01 8.03E+01 +2.125 5.09E+00 4.26E-01 1.37E+02 +2.125 6.00E+00 4.27E-01 1.19E+02 +2.125 6.89E+00 4.48E-01 1.08E+02 +2.125 7.71E+00 4.31E-01 1.00E+02 +2.125 8.45E+00 3.45E-01 9.60E+01 +2.125 9.21E+00 3.77E-01 9.76E+01 7.56E+00 +2.125 1.00E+01 2.61E-01 8.34E+01 7.96E+00 +2.125 1.06E+01 3.41E-01 9.69E+01 1.01E+01 +2.125 1.14E+01 3.99E-01 8.35E+01 1.02E+01 +2.125 1.27E+01 9.08E-01 4.83E+01 5.05E+00 +2.125 1.42E+01 4.13E-01 4.20E+01 1.14E+01 +2.125 1.63E+01 1.51E+00 2.24E+01 3.60E+00 +2.125 2.00E+01 1.98E+00 9.87E+00 4.94E+00 +ENDDATA 22 +ENDSUBENT 31 +ENDENTRY 3 diff --git a/exforall/140/14025.x4 b/exforall/140/14025.x4 new file mode 100644 index 000000000..1702416db --- /dev/null +++ b/exforall/140/14025.x4 @@ -0,0 +1,62 @@ +ENTRY 14025 20050711 20050909 1336 +SUBENT 14025001 20050711 20050909 1336 +BIB 10 11 +INSTITUTE (1USAORL) +REFERENCE (C,91JUELIC,,163,1991) +AUTHOR (J.Schmiedmayer,P.Riehs,J.A.Harvey,N.W.Hill) +TITLE Electric properties of the neutron from precision + cross section measurements +FACILITY (LINAC,1USAORL) ORELA +INC-SOURCE Pulsed beam of neutrons +METHOD (TOF) 18 meter flight path +SAMPLE Liquid (natural) Pb at 350 degree C, 0.1559 a/barn +DETECTOR (SCIN) 6Li glass scintillator, 1 mm thick +HISTORY (20050710C) DR +ENDBIB 11 +NOCOMMON 0 0 +ENDSUBENT 14 +SUBENT 14025002 20050711 20050909 1336 +BIB 3 3 +REACTION (82-PB-0(N,EL)82-PB-0,,SIG) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 32 +EN DATA DATA-ERR +EV B B + 1.64E-01 1.1291E+01 1.15E-02 + 2.12E-01 1.1293E+01 9.32E-03 + 2.77E-01 1.1299E+01 1.00E-02 + 3.58E-01 1.1299E+01 9.33E-03 + 4.53E-01 1.1323E+01 9.70E-03 + 5.79E-01 1.1333E+01 9.32E-03 + 7.56E-01 1.1329E+01 9.70E-03 + 9.76E-01 1.1326E+01 1.04E-02 + 1.27E+00 1.1324E+01 1.04E-02 + 1.66E+00 1.1331E+01 1.04E-02 + 2.07E+00 1.1337E+01 1.08E-02 + 2.70E+00 1.1307E+01 1.15E-02 + 3.54E+00 1.1329E+01 1.04E-02 + 4.46E+00 1.1324E+01 1.08E-02 + 5.73E+00 1.1380E+01 1.34E-02 + 7.55E+00 1.1348E+01 1.53E-02 + 9.83E+00 1.1322E+01 1.49E-02 + 1.25E+01 1.1346E+01 1.53E-02 + 1.66E+01 1.1351E+01 1.68E-02 + 2.08E+01 1.1303E+01 1.64E-02 + 2.74E+01 1.1359E+01 1.64E-02 + 3.48E+01 1.1322E+01 1.64E-02 + 4.50E+01 1.1336E+01 1.64E-02 + 5.75E+01 1.1338E+01 1.94E-02 + 7.36E+01 1.1357E+01 2.08E-02 + 9.71E+01 1.1347E+01 2.16E-02 + 1.26E+02 1.1330E+01 2.12E-02 + 1.62E+02 1.1364E+01 2.20E-02 + 2.12E+02 1.1389E+01 1.67E-02 + 2.66E+02 1.1352E+01 2.12E-02 + 3.51E+02 1.1313E+01 2.64E-02 + 4.50E+02 1.1360E+01 2.61E-02 +ENDDATA 34 +ENDSUBENT 42 +ENDENTRY 2 diff --git a/exforall/140/14026.x4 b/exforall/140/14026.x4 new file mode 100644 index 000000000..3eeab5e75 --- /dev/null +++ b/exforall/140/14026.x4 @@ -0,0 +1,95 @@ +ENTRY 14026 20050711 20050909 1336 +SUBENT 14026001 20050711 20050909 1336 +BIB 9 10 +INSTITUTE (1USAINL) +REFERENCE (P,NCSAC-33,89,1970) +AUTHOR (T.E.Young) +TITLE Neutron total cross section of 175Lu, 176Lu and natural + Lu +FACILITY (REAC,1USAINL) MTR Fast Chopper reactor +INC-SOURCE Thermal neutrons +SAMPLE Natural Lu, 175Lu and 176Lu, no details +DETECTOR No details +HISTORY (20050710C) DR +ENDBIB 10 +NOCOMMON 0 0 +ENDSUBENT 13 +SUBENT 14026002 20050711 20050909 1336 +BIB 3 3 +REACTION (71-LU-0(N,TOT),,SIG) +ERR-ANALYS (+DATA-ERR) No information +STATUS Data read from Table B-1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 1 +EN DATA +DATA-ERR -DATA-ERR +EV B B B + 2.53E-2 71. 6. 2. +ENDDATA 3 +ENDSUBENT 11 +SUBENT 14026003 20050711 20050909 1336 +BIB 3 3 +REACTION (71-LU-0(N,G),,SIG) +ERR-ANALYS (+DATA-ERR) No information +STATUS Data read from Table B-1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 1 +EN DATA +DATA-ERR -DATA-ERR +EV B B B + 2.53E-2 65. 6. 2. +ENDDATA 3 +ENDSUBENT 11 +SUBENT 14026004 20050711 20050909 1336 +BIB 3 3 +REACTION (71-LU-175(N,TOT),,SIG) +ERR-ANALYS (+DATA-ERR) No information +STATUS Data read from Table B-1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 1 +EN DATA +DATA-ERR -DATA-ERR +EV B B B + 2.53E-2 21.5 4.0 1.0 +ENDDATA 3 +ENDSUBENT 11 +SUBENT 14026005 20050711 20050909 1336 +BIB 3 3 +REACTION (71-LU-175(N,G)71-LU-176,,SIG) +ERR-ANALYS (+DATA-ERR) No information +STATUS Data read from Table B-1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 1 +EN DATA +DATA-ERR -DATA-ERR +EV B B B + 2.53E-2 15.5 4.0 1.0 +ENDDATA 3 +ENDSUBENT 11 +SUBENT 14026006 20050711 20050909 1336 +BIB 3 3 +REACTION (71-LU-176(N,TOT),,SIG) +ERR-ANALYS (DATA-ERR) No information +STATUS Data read from Table B-1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +EV B B + 2.53E-2 2134. 60. +ENDDATA 3 +ENDSUBENT 11 +SUBENT 14026007 20050711 20050909 1336 +BIB 3 3 +REACTION (71-LU-176(N,G)71-LU-177,,SIG) +ERR-ANALYS (DATA-ERR) No information +STATUS Data read from Table B-1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +EV B B + 2.53E-2 2129. 60. +ENDDATA 3 +ENDSUBENT 11 +ENDENTRY 7 diff --git a/exforall/140/14027.x4 b/exforall/140/14027.x4 new file mode 100644 index 000000000..0f5eb63ae --- /dev/null +++ b/exforall/140/14027.x4 @@ -0,0 +1,241 @@ +ENTRY 14027 20050711 20050909 1336 +SUBENT 14027001 20050711 20050909 1336 +BIB 9 11 +INSTITUTE (1USALAS) +REFERENCE (C,94GATLIN,,179,1994) +AUTHOR (P.E.Koehler,F.Kappeler) +TITLE Measurements of (n,g) cross sections for very small + stable and radioactive samples of interest to the s- + and p- process +FACILITY (ACCEL,1USALAS) LANSCE Neutron source +INC-SOURCE Spallation from proton + W +SAMPLE Natural Lu, 175Lu and 176Lu, no details +DETECTOR (SCIN) A pair of deuterated benzene C6D6 scintillators +HISTORY (20050710C) DR +ENDBIB 11 +NOCOMMON 0 0 +ENDSUBENT 14 +SUBENT 14027002 20050711 20050909 1336 +BIB 3 3 +REACTION (77-IR-191(N,G)77-IR-192,,SIG) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 95 +EN DATA DATA-ERR +EV B B + 1.06E+03 1.84E+01 2.17E+00 + 1.07E+03 1.44E+01 1.69E+00 + 1.10E+03 1.15E+01 1.36E+00 + 1.18E+03 1.41E+01 1.48E+00 + 1.23E+03 1.22E+01 1.59E+00 + 1.26E+03 8.57E+00 1.44E+00 + 1.29E+03 1.39E+01 0.00E+00 + 1.30E+03 1.26E+01 0.00E+00 + 1.31E+03 1.46E+01 1.53E+00 + 1.34E+03 9.37E+00 1.33E+00 + 1.40E+03 1.35E+01 1.09E+00 + 1.44E+03 1.46E+01 1.72E+00 + 1.45E+03 7.59E+00 1.37E+00 + 1.51E+03 8.02E+00 1.04E+00 + 1.55E+03 9.27E+00 7.51E-01 + 1.59E+03 1.26E+01 1.49E+00 + 1.63E+03 1.28E+01 1.50E+00 + 1.64E+03 9.70E+00 1.26E+00 + 1.70E+03 1.03E+01 1.48E+00 + 1.74E+03 8.21E+00 9.66E-01 + 1.80E+03 1.00E+01 1.18E+00 + 1.87E+03 7.77E+00 1.20E+00 + 1.91E+03 8.98E+00 1.16E+00 + 1.96E+03 1.11E+01 1.44E+00 + 1.99E+03 1.03E+01 8.41E-01 + 2.01E+03 9.29E+00 9.79E-01 + 2.11E+03 1.06E+01 1.51E+00 + 2.15E+03 8.31E+00 1.18E+00 + 2.23E+03 1.06E+01 1.51E+00 + 2.29E+03 7.96E+00 1.23E+00 + 2.37E+03 7.70E+00 1.19E+00 + 2.45E+03 7.87E+00 1.02E+00 + 2.55E+03 8.14E+00 1.16E+00 + 2.61E+03 8.61E+00 1.33E+00 + 2.67E+03 4.93E+00 9.62E-01 + 2.75E+03 7.45E+00 9.70E-01 + 2.84E+03 7.71E+00 7.17E-01 + 2.96E+03 7.71E+00 6.23E-01 + 3.10E+03 8.33E+00 8.77E-01 + 3.27E+03 5.11E+00 9.95E-01 + 3.31E+03 8.53E+00 1.00E+00 + 3.51E+03 6.90E+00 1.07E+00 + 3.55E+03 5.71E+00 7.43E-01 + 3.73E+03 5.59E+00 8.70E-01 + 3.81E+03 6.91E+00 8.13E-01 + 3.88E+03 5.35E+00 6.96E-01 + 3.99E+03 4.58E+00 8.31E-01 + 4.08E+03 5.35E+00 9.72E-01 + 4.25E+03 4.73E+00 9.22E-01 + 4.36E+03 5.29E+00 7.56E-01 + 4.50E+03 5.53E+00 8.61E-01 + 4.61E+03 5.92E+00 9.21E-01 + 4.79E+03 3.32E+00 8.27E-01 + 4.92E+03 5.42E+00 7.74E-01 + 5.13E+03 5.12E+00 8.63E-01 + 5.24E+03 6.92E+00 9.01E-01 + 5.48E+03 5.36E+00 9.03E-01 + 5.66E+03 4.74E+00 9.24E-01 + 5.82E+03 3.47E+00 8.18E-01 + 6.05E+03 4.29E+00 7.80E-01 + 6.20E+03 4.80E+00 8.72E-01 + 6.47E+03 3.67E+00 4.78E-01 + 6.67E+03 4.29E+00 8.94E-01 + 6.95E+03 4.39E+00 7.98E-01 + 7.26E+03 3.29E+00 7.75E-01 + 7.48E+03 4.86E+00 8.82E-01 + 7.80E+03 3.98E+00 7.75E-01 + 8.07E+03 3.64E+00 8.57E-01 + 8.45E+03 4.86E+00 8.83E-01 + 8.73E+03 4.60E+00 7.75E-01 + 9.18E+03 4.16E+00 7.56E-01 + 9.49E+03 4.16E+00 6.48E-01 + 9.96E+03 4.26E+00 6.08E-01 + 1.04E+04 3.49E+00 6.33E-01 + 1.08E+04 5.21E+00 1.15E+00 + 1.14E+04 4.87E+00 1.08E+00 + 1.19E+04 4.41E+00 9.18E-01 + 1.26E+04 4.46E+00 8.10E-01 + 1.31E+04 3.95E+00 8.75E-01 + 1.38E+04 3.42E+00 8.04E-01 + 1.47E+04 3.82E+00 7.45E-01 + 1.55E+04 2.31E+00 6.43E-01 + 1.64E+04 3.06E+00 7.63E-01 + 1.74E+04 3.16E+00 6.17E-01 + 1.82E+04 2.96E+00 6.57E-01 + 1.96E+04 3.17E+00 6.59E-01 + 2.07E+04 3.96E+00 7.19E-01 + 2.24E+04 3.50E+00 6.83E-01 + 2.38E+04 2.29E+00 4.78E-01 + 2.56E+04 1.82E+00 5.30E-01 + 2.73E+04 2.17E+00 5.42E-01 + 2.93E+04 2.78E+00 5.41E-01 + 3.17E+04 1.86E+00 5.17E-01 + 3.43E+04 2.97E+00 9.98E-01 + 3.73E+04 2.08E+00 7.00E-01 +ENDDATA 97 +ENDSUBENT 105 +SUBENT 14027003 20050711 20050909 1336 +BIB 3 3 +REACTION (77-IR-193(N,G)77-IR-194,,SIG) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 5 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 104 +EN DATA DATA-ERR +EV B B + 1.03E+03 5.13E+00 1.10E+00 + 1.05E+03 7.58E+00 1.32E+00 + 1.07E+03 9.02E+00 1.69E+00 + 1.10E+03 9.34E+00 1.38E+00 + 1.12E+03 1.11E+01 1.35E+00 + 1.15E+03 1.18E+01 1.14E+00 + 1.18E+03 1.16E+01 1.26E+00 + 1.22E+03 1.00E+01 1.22E+00 + 1.23E+03 5.96E+00 9.63E-01 + 1.26E+03 6.17E+00 4.41E-01 + 1.27E+03 5.83E+00 1.42E+00 + 1.31E+03 4.37E+00 8.85E-01 + 1.34E+03 5.83E+00 7.87E-01 + 1.36E+03 9.79E+00 1.32E+00 + 1.41E+03 8.43E+00 1.25E+00 + 1.47E+03 5.83E+00 9.42E-01 + 1.48E+03 5.51E+00 8.16E-01 + 1.50E+03 7.87E+00 9.61E-01 + 1.54E+03 6.55E+00 1.23E+00 + 1.58E+03 8.53E+00 1.26E+00 + 1.60E+03 9.91E+00 1.21E+00 + 1.65E+03 5.84E+00 1.02E+00 + 1.68E+03 4.23E+00 1.03E+00 + 1.69E+03 7.44E+00 1.10E+00 + 1.74E+03 7.61E+00 1.12E+00 + 1.76E+03 5.33E+00 1.15E+00 + 1.86E+03 7.36E+00 9.93E-01 + 1.86E+03 6.19E+00 1.08E+00 + 1.91E+03 6.79E+00 1.09E+00 + 1.95E+03 8.26E+00 6.92E-01 + 2.02E+03 9.27E+00 1.13E+00 + 2.04E+03 6.79E+00 9.17E-01 + 2.11E+03 5.91E+00 8.76E-01 + 2.12E+03 4.43E+00 9.59E-01 + 2.20E+03 5.99E+00 9.66E-01 + 2.27E+03 3.00E+00 9.55E-01 + 2.34E+03 4.70E+00 8.86E-01 + 2.41E+03 7.45E+00 1.00E+00 + 2.45E+03 6.06E+00 9.78E-01 + 2.55E+03 6.20E+00 8.37E-01 + 2.62E+03 5.53E+00 8.19E-01 + 2.67E+03 4.14E+00 8.97E-01 + 2.76E+03 4.34E+00 1.00E+00 + 2.85E+03 5.04E+00 1.09E+00 + 2.99E+03 5.47E+00 8.84E-01 + 3.10E+03 4.76E+00 8.98E-01 + 3.14E+03 3.22E+00 7.42E-01 + 3.27E+03 2.74E+00 6.32E-01 + 3.31E+03 5.54E+00 8.94E-01 + 3.46E+03 3.62E+00 7.31E-01 + 3.51E+03 4.40E+00 8.30E-01 + 3.62E+03 2.50E+00 6.85E-01 + 3.70E+03 3.66E+00 5.91E-01 + 3.81E+03 4.35E+00 6.45E-01 + 3.92E+03 3.58E+00 6.26E-01 + 3.98E+03 4.01E+00 5.95E-01 + 4.16E+03 2.81E+00 6.08E-01 + 4.30E+03 2.71E+00 6.64E-01 + 4.40E+03 3.26E+00 5.27E-01 + 4.51E+03 3.27E+00 7.06E-01 + 4.69E+03 4.89E+00 5.97E-01 + 4.80E+03 2.01E+00 6.72E-01 + 4.93E+03 3.93E+00 6.88E-01 + 5.16E+03 2.88E+00 5.83E-01 + 5.28E+03 3.58E+00 7.26E-01 + 5.45E+03 3.80E+00 6.65E-01 + 5.64E+03 3.31E+00 6.24E-01 + 5.88E+03 3.05E+00 5.76E-01 + 6.02E+03 3.51E+00 6.61E-01 + 6.22E+03 3.67E+00 6.92E-01 + 6.51E+03 2.57E+00 7.04E-01 + 6.71E+03 3.16E+00 6.40E-01 + 6.94E+03 3.43E+00 6.00E-01 + 7.27E+03 1.90E+00 6.36E-01 + 7.47E+03 3.64E+00 6.36E-01 + 7.80E+03 2.82E+00 6.10E-01 + 8.12E+03 3.10E+00 6.26E-01 + 8.47E+03 2.82E+00 6.51E-01 + 8.83E+03 3.03E+00 8.29E-01 + 9.20E+03 2.96E+00 8.09E-01 + 9.58E+03 3.10E+00 7.58E-01 + 1.00E+04 2.64E+00 7.61E-01 + 1.05E+04 3.03E+00 7.85E-01 + 1.08E+04 2.76E+00 8.39E-01 + 1.14E+04 3.00E+00 7.33E-01 + 1.21E+04 2.70E+00 7.00E-01 + 1.25E+04 2.77E+00 6.38E-01 + 1.32E+04 1.32E+00 6.13E-01 + 1.38E+04 1.83E+00 5.83E-01 + 1.46E+04 3.04E+00 5.31E-01 + 1.55E+04 1.71E+00 4.93E-01 + 1.65E+04 1.67E+00 5.32E-01 + 1.73E+04 2.05E+00 5.03E-01 + 1.83E+04 2.13E+00 5.21E-01 + 1.96E+04 1.47E+00 5.14E-01 + 2.09E+04 2.36E+00 5.78E-01 + 2.23E+04 1.09E+00 4.33E-01 + 2.35E+04 1.42E+00 4.54E-01 + 2.54E+04 1.25E+00 3.62E-01 + 2.71E+04 1.18E+00 4.14E-01 + 2.89E+04 1.97E+00 3.99E-01 + 3.15E+04 1.35E+00 4.29E-01 + 3.42E+04 1.15E+00 6.51E-01 + 3.75E+04 1.07E+00 5.14E-01 +ENDDATA 106 +ENDSUBENT 114 +ENDENTRY 3 diff --git a/exforall/140/14028.x4 b/exforall/140/14028.x4 new file mode 100644 index 000000000..3cae4fa3f --- /dev/null +++ b/exforall/140/14028.x4 @@ -0,0 +1,499 @@ +ENTRY 14028 20050712 20050909 1336 +SUBENT 14028001 20050712 20050909 1336 +BIB 9 18 +INSTITUTE (1USALRL,1USALAS) +REFERENCE (J,PR/C,57,2799,1998) +AUTHOR (L.A.Bernstein,J.A.Becker,W.Younes,D.E.Archer, + K.Hauschild,G.D.Johns,R.O.Nelson,W.S.Wilburn, + D.M.Drake) +TITLE Probing reaction dynamics with the 196Pt(n,xngamma) + reactions for x <= 15 +FACILITY (ACCEL,1USALAS) LANSCE Neutron source and WNR facility +INC-SOURCE Spallation from proton + W +SAMPLE 97.4% isotopically enriched 196Pt sample, two + 0.54 gm/cm2 foils, was placed at the focal point + of GEANIE. +DETECTOR (GE-IN) GEANIE detector: combination of Compton + suppressed coaxial Ge detectors with approximately + 25% of the efficiency of a 3 inch33 inch NaIcrystal + and planar Ge detectors (LEPS, low energy photon + spectrometers). +HISTORY (20050712C) DR +ENDBIB 18 +NOCOMMON 0 0 +ENDSUBENT 21 +SUBENT 14028002 20050712 20050909 1336 +BIB 3 3 +REACTION (78-PT-196(N,3N)78-PT-194,,SIG,,REL) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 28 +EN DATA DATA-ERR +MEV ARB-UNITS ARB-UNITS + 1.10E+01 1.85E-02 + 1.27E+01 5.57E-02 + 1.60E+01 7.28E-01 8.17E-02 + 1.87E+01 9.81E-01 + 3.09E+01 9.92E-01 + 3.42E+01 8.66E-01 + 3.59E+01 6.65E-01 + 3.86E+01 3.68E-01 + 4.08E+01 2.67E-01 + 4.19E+01 2.26E-01 + 4.64E+01 2.11E-01 + 5.08E+01 2.41E-01 + 5.52E+01 2.52E-01 + 5.91E+01 2.19E-01 + 6.35E+01 2.00E-01 + 6.90E+01 1.85E-01 + 7.34E+01 2.15E-01 + 8.01E+01 2.15E-01 + 8.56E+01 2.19E-01 + 9.28E+01 2.00E-01 + 1.01E+02 2.19E-01 + 1.11E+02 2.30E-01 + 1.20E+02 2.15E-01 + 1.30E+02 1.74E-01 + 1.44E+02 1.82E-01 + 1.56E+02 2.49E-01 + 1.72E+02 2.19E-01 + 1.87E+02 1.97E-01 +ENDDATA 30 +ENDSUBENT 38 +SUBENT 14028003 20050712 20050909 1336 +BIB 3 3 +REACTION (78-PT-196(N,5N)78-PT-192,,SIG,,REL) +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 2 25 +EN DATA +MEV ARB-UNITS + 2.71E+01 1.11E-02 + 2.99E+01 3.33E-02 + 3.21E+01 1.33E-01 + 3.43E+01 3.33E-01 + 3.71E+01 5.66E-01 + 3.87E+01 6.48E-01 + 4.37E+01 6.70E-01 + 4.81E+01 6.74E-01 + 5.09E+01 6.11E-01 + 5.42E+01 5.11E-01 + 5.92E+01 3.74E-01 + 6.31E+01 3.03E-01 + 6.70E+01 2.51E-01 + 7.20E+01 2.44E-01 + 7.86E+01 2.70E-01 + 8.42E+01 2.70E-01 + 9.25E+01 2.74E-01 + 1.00E+02 2.44E-01 + 1.10E+02 2.22E-01 + 1.19E+02 2.22E-01 + 1.30E+02 2.22E-01 + 1.44E+02 2.03E-01 + 1.57E+02 1.88E-01 + 1.71E+02 2.29E-01 + 1.87E+02 2.37E-01 +ENDDATA 27 +ENDSUBENT 35 +SUBENT 14028004 20050712 20050909 1336 +BIB 3 3 +REACTION (78-PT-196(N,7N)78-PT-190,,SIG,,REL) +ERR-ANALYS No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 2 21 +EN DATA +MEV ARB-UNITS + 3.72E+01 3.70E-02 + 3.94E+01 7.40E-02 + 4.49E+01 8.51E-02 + 4.94E+01 1.00E-01 + 5.10E+01 1.40E-01 + 5.49E+01 2.07E-01 + 5.87E+01 3.77E-01 + 6.31E+01 4.62E-01 + 6.69E+01 5.40E-01 + 7.25E+01 4.77E-01 + 7.81E+01 4.11E-01 + 8.37E+01 3.66E-01 + 9.15E+01 3.33E-01 + 1.00E+02 2.88E-01 + 1.09E+02 2.59E-01 + 1.19E+02 2.59E-01 + 1.31E+02 2.55E-01 + 1.43E+02 2.37E-01 + 1.56E+02 2.14E-01 + 1.72E+02 2.11E-01 + 1.88E+02 2.44E-01 +ENDDATA 23 +ENDSUBENT 31 +SUBENT 14028005 20050712 20050909 1336 +BIB 3 3 +REACTION (78-PT-196(N,9N)78-PT-188,,SIG,,REL) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 24 +EN DATA DATA-ERR +MEV ARB-UNITS ARB-UNITS + 1.44E+01 5.99E-03 + 1.93E+01 5.99E-03 + 2.43E+01 5.99E-03 + 3.43E+01 5.99E-03 + 3.76E+01 2.69E-02 + 4.21E+01 5.99E-03 + 4.65E+01 8.98E-03 + 5.09E+01 1.19E-02 + 5.59E+01 1.19E-02 + 5.92E+01 3.59E-02 + 6.31E+01 3.29E-02 + 6.70E+01 5.39E-02 + 7.25E+01 1.10E-01 + 7.86E+01 2.12E-01 + 8.42E+01 2.87E-01 + 9.19E+01 3.65E-01 + 1.00E+02 3.53E-01 + 1.09E+02 3.53E-01 + 1.20E+02 3.62E-01 + 1.30E+02 3.38E-01 + 1.42E+02 3.26E-01 + 1.56E+02 3.20E-01 5.09E-02 + 1.71E+02 3.17E-01 5.39E-02 + 1.87E+02 3.80E-01 6.59E-02 +ENDDATA 26 +ENDSUBENT 34 +SUBENT 14028006 20050712 20050909 1336 +BIB 3 3 +REACTION (78-PT-196(N,11N)78-PT-186,,SIG,,REL) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 15 +EN DATA DATA-ERR +MEV ARB-UNITS ARB-UNITS + 5.15E+01 5.97E-03 + 5.53E+01 2.68E-02 + 6.03E+01 1.49E-02 + 6.53E+01 1.49E-02 + 7.14E+01 1.19E-02 + 7.80E+01 3.58E-02 + 8.63E+01 8.35E-02 + 9.52E+01 1.13E-01 + 1.05E+02 1.31E-01 + 1.15E+02 1.16E-01 + 1.26E+02 1.16E-01 + 1.40E+02 1.43E-01 + 1.54E+02 2.44E-01 3.58E-02 + 1.69E+02 2.02E-01 4.17E-02 + 1.86E+02 1.64E-01 4.17E-02 +ENDDATA 17 +ENDSUBENT 25 +SUBENT 14028007 20050712 20050909 1336 +BIB 3 3 +REACTION (78-PT-196(N,13N)78-PT-184,,SIG,,REL) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 8 +EN DATA DATA-ERR +MEV ARB-UNITS ARB-UNITS + 9.49E+01 9.02E-03 + 1.05E+02 5.41E-02 + 1.16E+02 9.92E-02 + 1.27E+02 1.71E-01 + 1.40E+02 1.89E-01 4.21E-02 + 1.55E+02 1.23E-01 5.11E-02 + 1.71E+02 1.32E-01 5.41E-02 + 1.87E+02 9.02E-03 4.51E-02 +ENDDATA 10 +ENDSUBENT 18 +SUBENT 14028008 20050712 20050909 1336 +BIB 4 12 +REACTION ((78-PT-196(N,3N)78-PT-194,PAR,SIG)// + (78-PT-196(N,3N)78-PT-194,PAR,SIG)) + Ratio of high level transition to 2+ -> 0+ +EN-SEC (E-LVL-DN,78-PT-194) Transition of the + denominator 2+ -> 0+ + (E-LVL-INI,78-PT-194) Decaying level of + transition (numerator) + (E-LVL-FIN,78-PT-194) Final level of + transition (numerator) + (E-LVL-NM,78-PT-194) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 4 +ENDBIB 12 +COMMON 1 3 +E-LVL-DN +MEV +0.3284 +ENDCOMMON 3 +DATA 6 87 +E-LVL-NM E-LVL-INI E-LVL-FIN EN DATA DATA-ERR +MEV MEV MEV MEV NO-DIM NO-DIM +0.483 0.8113 0.3284 1.50E+01 1.26E-01 +0.483 0.8113 0.3284 1.83E+01 1.63E-01 +0.483 0.8113 0.3284 2.11E+01 2.31E-01 +0.483 0.8113 0.3284 2.23E+01 2.87E-01 +0.483 0.8113 0.3284 2.51E+01 3.27E-01 +0.483 0.8113 0.3284 2.74E+01 4.16E-01 +0.483 0.8113 0.3284 2.84E+01 3.72E-01 +0.483 0.8113 0.3284 3.29E+01 4.29E-01 +0.483 0.8113 0.3284 3.51E+01 3.74E-01 +0.483 0.8113 0.3284 3.72E+01 3.03E-01 +0.483 0.8113 0.3284 4.11E+01 2.98E-01 +0.483 0.8113 0.3284 4.16E+01 2.53E-01 +0.483 0.8113 0.3284 4.60E+01 2.28E-01 +0.483 0.8113 0.3284 4.88E+01 2.54E-01 +0.483 0.8113 0.3284 5.65E+01 2.39E-01 +0.483 0.8113 0.3284 6.37E+01 2.39E-01 +0.483 0.8113 0.3284 6.76E+01 3.24E-01 +0.483 0.8113 0.3284 7.20E+01 2.43E-01 +0.483 0.8113 0.3284 7.91E+01 2.31E-01 +0.483 0.8113 0.3284 8.63E+01 2.00E-01 +0.483 0.8113 0.3284 9.29E+01 2.19E-01 +0.483 0.8113 0.3284 1.00E+02 2.06E-01 +0.483 0.8113 0.3284 1.11E+02 1.93E-01 +0.483 0.8113 0.3284 1.20E+02 2.22E-01 +0.483 0.8113 0.3284 1.32E+02 1.98E-01 +0.483 0.8113 0.3284 1.46E+02 2.13E-01 +0.483 0.8113 0.3284 1.58E+02 7.50E-02 +0.483 0.8113 0.3284 1.71E+02 4.55E-02 +0.483 0.8113 0.3284 1.89E+02 4.00E-02 +0.563 1.3739 0.8113 1.82E+01 5.02E-02 +0.563 1.3739 0.8113 1.87E+01 1.99E-01 +0.563 1.3739 0.8113 2.15E+01 3.32E-01 +0.563 1.3739 0.8113 2.48E+01 4.16E-01 +0.563 1.3739 0.8113 2.81E+01 5.59E-01 2.97E-02 +0.563 1.3739 0.8113 2.92E+01 6.76E-01 3.16E-02 +0.563 1.3739 0.8113 3.37E+01 6.54E-01 3.90E-02 +0.563 1.3739 0.8113 3.53E+01 5.09E-01 2.41E-02 +0.563 1.3739 0.8113 3.97E+01 2.79E-01 +0.563 1.3739 0.8113 4.41E+01 3.01E-01 +0.563 1.3739 0.8113 4.91E+01 2.86E-01 +0.563 1.3739 0.8113 5.13E+01 3.16E-01 +0.563 1.3739 0.8113 5.52E+01 1.84E-01 +0.563 1.3739 0.8113 6.02E+01 2.56E-01 +0.563 1.3739 0.8113 6.68E+01 1.90E-01 +0.563 1.3739 0.8113 7.34E+01 1.93E-01 +0.563 1.3739 0.8113 7.73E+01 1.36E-01 +0.563 1.3739 0.8113 8.50E+01 1.90E-01 +0.563 1.3739 0.8113 9.22E+01 1.41E-01 +0.563 1.3739 0.8113 1.01E+02 1.19E-01 +0.563 1.3739 0.8113 1.09E+02 1.40E-01 +0.563 1.3739 0.8113 1.19E+02 1.51E-01 +0.563 1.3739 0.8113 1.32E+02 1.42E-01 +0.563 1.3739 0.8113 1.44E+02 7.15E-02 +0.563 1.3739 0.8113 1.56E+02 9.76E-02 +0.563 1.3739 0.8113 1.72E+02 9.21E-02 +0.563 1.3739 0.8113 1.87E+02 1.16E-01 +0.607 1.2295 0.622 9.39E+00 3.51E-01 +0.607 1.2295 0.622 1.32E+01 3.35E-02 +0.607 1.2295 0.622 1.76E+01 1.86E-02 +0.607 1.2295 0.622 1.87E+01 2.98E-02 +0.607 1.2295 0.622 2.26E+01 3.17E-02 +0.607 1.2295 0.622 2.54E+01 4.47E-02 +0.607 1.2295 0.622 2.81E+01 5.77E-02 +0.607 1.2295 0.622 3.03E+01 6.89E-02 +0.607 1.2295 0.622 3.14E+01 1.04E-01 +0.607 1.2295 0.622 3.64E+01 1.17E-01 +0.607 1.2295 0.622 3.70E+01 1.45E-01 +0.607 1.2295 0.622 3.81E+01 1.65E-01 +0.607 1.2295 0.622 4.08E+01 1.65E-01 +0.607 1.2295 0.622 4.41E+01 1.58E-01 +0.607 1.2295 0.622 4.64E+01 1.65E-01 +0.607 1.2295 0.622 5.19E+01 1.60E-01 +0.607 1.2295 0.622 5.52E+01 1.84E-01 +0.607 1.2295 0.622 5.91E+01 2.27E-01 +0.607 1.2295 0.622 6.29E+01 2.73E-01 2.60E-02 +0.607 1.2295 0.622 7.29E+01 3.42E-01 2.23E-02 +0.607 1.2295 0.622 7.95E+01 3.94E-01 3.53E-02 +0.607 1.2295 0.622 8.61E+01 4.15E-01 2.78E-02 +0.607 1.2295 0.622 9.33E+01 4.46E-01 3.90E-02 +0.607 1.2295 0.622 1.01E+02 4.70E-01 3.34E-02 +0.607 1.2295 0.622 1.10E+02 5.08E-01 4.27E-02 +0.607 1.2295 0.622 1.20E+02 5.78E-01 4.64E-02 +0.607 1.2295 0.622 1.31E+02 6.97E-01 5.20E-02 +0.607 1.2295 0.622 1.44E+02 7.89E-01 6.69E-02 +0.607 1.2295 0.622 1.58E+02 7.16E-01 6.87E-02 +0.607 1.2295 0.622 1.72E+02 6.29E-01 6.13E-02 +0.607 1.2295 0.622 1.88E+02 6.90E-01 7.24E-02 +ENDDATA 89 +ENDSUBENT 110 +SUBENT 14028009 20050712 20050909 1336 +BIB 4 12 +REACTION ((78-PT-196(N,5N)78-PT-192,PAR,SIG)// + (78-PT-196(N,5N)78-PT-192,PAR,SIG)) + Ratio of high level transition to 2+ -> 0+ +EN-SEC (E-LVL-DN,78-PT-192) Transition of the + denominator 2+ -> 0+ + (E-LVL-INI,78-PT-192) Decaying level of + transition (numerator) + (E-LVL-FIN,78-PT-192) Final level of + transition (numerator) + (E-LVL-NM,78-PT-192) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 4 +ENDBIB 12 +COMMON 1 3 +E-LVL-DN +MEV +0.3165 +ENDCOMMON 3 +DATA 6 69 +E-LVL-NM E-LVL-INI E-LVL-FIN EN DATA DATA-ERR +MEV MEV MEV MEV NO-DIM NO-DIM +0.468 0.7846 0.3165 1.04E+01 5.70E-03 +0.468 0.7846 0.3165 1.16E+01 5.76E-02 +0.468 0.7846 0.3165 1.60E+01 1.33E-01 +0.468 0.7846 0.3165 1.71E+01 1.80E-01 +0.468 0.7846 0.3165 2.15E+01 2.69E-01 +0.468 0.7846 0.3165 2.43E+01 3.82E-01 +0.468 0.7846 0.3165 2.81E+01 4.95E-01 +0.468 0.7846 0.3165 3.14E+01 5.56E-01 +0.468 0.7846 0.3165 3.59E+01 5.88E-01 2.96E-02 +0.468 0.7846 0.3165 4.03E+01 5.05E-01 2.22E-02 +0.468 0.7846 0.3165 4.64E+01 4.53E-01 3.70E-02 +0.468 0.7846 0.3165 5.02E+01 4.18E-01 2.40E-02 +0.468 0.7846 0.3165 5.58E+01 3.94E-01 +0.468 0.7846 0.3165 6.24E+01 3.75E-01 2.96E-02 +0.468 0.7846 0.3165 7.01E+01 2.99E-01 +0.468 0.7846 0.3165 7.79E+01 2.90E-01 +0.468 0.7846 0.3165 8.72E+01 2.20E-01 +0.468 0.7846 0.3165 9.83E+01 2.07E-01 +0.468 0.7846 0.3165 1.09E+02 2.03E-01 +0.468 0.7846 0.3165 1.22E+02 2.35E-01 2.22E-02 +0.468 0.7846 0.3165 1.37E+02 3.09E-01 3.89E-02 +0.468 0.7846 0.3165 1.51E+02 2.54E-01 3.89E-02 +0.468 0.7846 0.3165 1.69E+02 3.21E-01 4.08E-02 +0.468 0.7846 0.3165 1.87E+02 3.01E-01 4.63E-02 +0.589 1.201 0.6124 3.31E+00 1.86E-02 +0.589 1.201 0.6124 1.43E+01 1.31E-02 +0.589 1.201 0.6124 1.82E+01 2.43E-02 +0.589 1.201 0.6124 2.15E+01 2.43E-02 +0.589 1.201 0.6124 2.43E+01 3.18E-02 +0.589 1.201 0.6124 2.76E+01 3.74E-02 +0.589 1.201 0.6124 2.98E+01 5.97E-02 +0.589 1.201 0.6124 3.48E+01 7.83E-02 +0.589 1.201 0.6124 3.92E+01 9.32E-02 +0.589 1.201 0.6124 4.53E+01 8.77E-02 +0.589 1.201 0.6124 5.02E+01 8.96E-02 +0.589 1.201 0.6124 5.52E+01 7.67E-02 +0.589 1.201 0.6124 6.24E+01 7.49E-02 +0.589 1.201 0.6124 6.85E+01 7.50E-02 +0.589 1.201 0.6124 7.67E+01 7.51E-02 +0.589 1.201 0.6124 8.72E+01 1.16E-01 +0.589 1.201 0.6124 9.83E+01 1.36E-01 +0.589 1.201 0.6124 1.09E+02 1.75E-01 +0.589 1.201 0.6124 1.22E+02 1.87E-01 +0.589 1.201 0.6124 1.36E+02 2.44E-01 3.15E-02 +0.589 1.201 0.6124 1.51E+02 2.76E-01 3.33E-02 +0.589 1.201 0.6124 1.69E+02 2.54E-01 3.89E-02 +0.589 1.201 0.6124 1.86E+02 2.19E-01 4.08E-02 +0.599 1.384 0.7845 7.18E+00 2.56E-01 9.46E-02 +0.599 1.384 0.7845 1.32E+01 9.44E-03 +0.599 1.384 0.7845 1.82E+01 9.51E-03 +0.599 1.384 0.7845 1.98E+01 3.92E-02 +0.599 1.384 0.7845 2.54E+01 7.08E-02 +0.599 1.384 0.7845 2.81E+01 1.07E-01 +0.599 1.384 0.7845 3.14E+01 1.32E-01 +0.599 1.384 0.7845 3.70E+01 1.58E-01 +0.599 1.384 0.7845 3.92E+01 1.11E-01 +0.599 1.384 0.7845 4.53E+01 9.89E-02 +0.599 1.384 0.7845 5.08E+01 1.04E-01 +0.599 1.384 0.7845 5.69E+01 9.34E-02 +0.599 1.384 0.7845 6.24E+01 5.27E-02 +0.599 1.384 0.7845 6.96E+01 6.20E-02 +0.599 1.384 0.7845 7.95E+01 6.40E-02 +0.599 1.384 0.7845 8.83E+01 6.97E-02 +0.599 1.384 0.7845 9.83E+01 6.06E-02 +0.599 1.384 0.7845 1.09E+02 6.81E-02 +0.599 1.384 0.7845 1.22E+02 3.67E-02 +0.599 1.384 0.7845 1.35E+02 5.73E-02 +0.599 1.384 0.7845 1.52E+02 3.71E-02 +0.599 1.384 0.7845 1.67E+02 5.58E-02 2.59E-02 +ENDDATA 71 +ENDSUBENT 92 +SUBENT 14028010 20050712 20050909 1336 +BIB 4 12 +REACTION ((78-PT-196(N,7N)78-PT-190,PAR,SIG)// + (78-PT-196(N,7N)78-PT-190,PAR,SIG)) + Ratio of high level transition to 2+ -> 0+ +EN-SEC (E-LVL-DN,78-PT-190) Transition of the + denominator 2+ -> 0+ + (E-LVL-INI,78-PT-190) Decaying level of + transition (numerator) + (E-LVL-FIN,78-PT-192) Final level of + transition (numerator) + (E-LVL-NM,78-PT-190) +ERR-ANALYS (DATA-ERR) No information +STATUS (CURVE) Data read from Fig. 4 +ENDBIB 12 +COMMON 1 3 +E-LVL-DN +MEV +0.2958 +ENDCOMMON 3 +DATA 6 50 +E-LVL-NM E-LVL-INI E-LVL-FIN EN DATA DATA-ERR +MEV MEV MEV MEV NO-DIM NO-DIM +0.441 0.737 0.2958 4.47E+01 6.12E-02 +0.441 0.737 0.2958 4.66E+01 1.44E-01 3.89E-02 +0.441 0.737 0.2958 5.09E+01 1.68E-01 2.96E-02 +0.441 0.737 0.2958 5.48E+01 1.35E-01 +0.441 0.737 0.2958 5.91E+01 1.81E-01 +0.441 0.737 0.2958 6.25E+01 2.24E-01 +0.441 0.737 0.2958 6.77E+01 3.71E-01 2.96E-02 +0.441 0.737 0.2958 7.25E+01 5.43E-01 2.96E-02 +0.441 0.737 0.2958 7.78E+01 7.19E-01 3.89E-02 +0.441 0.737 0.2958 8.55E+01 6.99E-01 4.08E-02 +0.441 0.737 0.2958 9.27E+01 5.88E-01 5.56E-02 +0.441 0.737 0.2958 1.00E+02 5.00E-01 3.89E-02 +0.441 0.737 0.2958 1.09E+02 4.48E-01 4.45E-02 +0.441 0.737 0.2958 1.19E+02 4.21E-01 4.26E-02 +0.441 0.737 0.2958 1.31E+02 4.37E-01 4.82E-02 +0.441 0.737 0.2958 1.43E+02 4.43E-01 5.00E-02 +0.441 0.737 0.2958 1.56E+02 4.17E-01 5.93E-02 +0.441 0.737 0.2958 1.71E+02 4.26E-01 5.93E-02 +0.441 0.737 0.2958 1.87E+02 4.41E-01 6.49E-02 +0.531 1.1282 0.5976 4.90E+01 9.27E-03 +0.531 1.1282 0.5976 5.04E+01 2.96E-02 +0.531 1.1282 0.5976 5.33E+01 2.96E-02 +0.531 1.1282 0.5976 5.86E+01 2.04E-02 +0.531 1.1282 0.5976 6.25E+01 4.08E-02 +0.531 1.1282 0.5976 6.73E+01 9.64E-02 +0.531 1.1282 0.5976 7.25E+01 1.72E-01 +0.531 1.1282 0.5976 7.74E+01 2.44E-01 +0.531 1.1282 0.5976 8.50E+01 2.63E-01 +0.531 1.1282 0.5976 9.27E+01 2.63E-01 +0.531 1.1282 0.5976 1.00E+02 2.82E-01 +0.531 1.1282 0.5976 1.09E+02 3.50E-01 2.41E-02 +0.531 1.1282 0.5976 1.19E+02 3.54E-01 2.78E-02 +0.531 1.1282 0.5976 1.31E+02 4.04E-01 2.04E-02 +0.531 1.1282 0.5976 1.42E+02 3.78E-01 3.52E-02 +0.531 1.1282 0.5976 1.56E+02 4.65E-01 6.12E-02 +0.531 1.1282 0.5976 1.71E+02 5.52E-01 7.05E-02 +0.531 1.1282 0.5976 1.87E+02 5.93E-01 7.05E-02 +0.725 1.4645 0.737 6.82E+01 2.96E-02 +0.725 1.4645 0.737 7.21E+01 1.11E-01 +0.725 1.4645 0.737 7.83E+01 2.05E-01 +0.725 1.4645 0.737 8.41E+01 3.19E-01 2.59E-02 +0.725 1.4645 0.737 9.23E+01 3.20E-01 2.96E-02 +0.725 1.4645 0.737 1.00E+02 2.72E-01 2.78E-02 +0.725 1.4645 0.737 1.10E+02 1.74E-01 2.22E-02 +0.725 1.4645 0.737 1.19E+02 1.50E-01 +0.725 1.4645 0.737 1.30E+02 1.31E-01 2.41E-02 +0.725 1.4645 0.737 1.43E+02 1.05E-01 +0.725 1.4645 0.737 1.57E+02 1.57E-01 3.33E-02 +0.725 1.4645 0.737 1.72E+02 1.05E-01 3.33E-02 +0.725 1.4645 0.737 1.87E+02 8.71E-02 3.52E-02 +ENDDATA 52 +ENDSUBENT 73 +ENDENTRY 10 diff --git a/exforall/140/14029.x4 b/exforall/140/14029.x4 new file mode 100644 index 000000000..d625ada12 --- /dev/null +++ b/exforall/140/14029.x4 @@ -0,0 +1,37 @@ +ENTRY 14029 20050712 20050909 1336 +SUBENT 14029001 20050712 20050909 1336 +BIB 10 14 +INSTITUTE (1CANCRC) +REFERENCE (C,85SANTA,1,537,1985) +AUTHOR (R.T.Jones,J.S.Merrit,A.Okazaki) +TITLE A measurement of the thermal neutron capture cross + section of Th232 +FACILITY (REAC) NRU Reactor +INC-SOURCE Graphite thermal column +SAMPLE Thin disks of thorium metal and of sintered thoria + ThO2 +DETECTOR (GE-IN) +METHOD (ACTIV) Measurement of beta emission from decay of + Th233 (to Pa233) in coincidence the 311.9 keV of + Pa233 +HISTORY (20050712C) DR +ENDBIB 14 +NOCOMMON 0 0 +ENDSUBENT 17 +SUBENT 14029002 20050712 20050909 1336 +BIB 4 6 +REACTION (90-TH-232(N,G)90-TH-233,,SIG,,MXW) +ERR-ANALYS (ERR-T) Total uncertainty +ASSUMED (ASSUM1,(79-AU-197(N,G)79-AU-198,,SIG,,MXW)) + Measurement relative to Au197 with a thermal capture + cross section of 98.8 barns +STATUS Data read from the text +ENDBIB 6 +NOCOMMON 0 0 +DATA 4 1 +EN DATA ERR-T ASSUM1 +MEV B B B + 2.53E-08 7.33 0.06 98.8 +ENDDATA 3 +ENDSUBENT 14 +ENDENTRY 2 diff --git a/exforall/140/14030.x4 b/exforall/140/14030.x4 new file mode 100644 index 000000000..100885b4a --- /dev/null +++ b/exforall/140/14030.x4 @@ -0,0 +1,1195 @@ +ENTRY 14030 20050715 20050909 1336 +SUBENT 14030001 20050715 20050909 1336 +BIB 11 18 +INSTITUTE (1USAANL,2JPNJAE) +REFERENCE (J,ANE,23,459,1996) + (P,ANL-NDM-135,1995) +AUTHOR (A.B.Smith,S.Chiba) +TITLE Neutron Scattering from elemental uranium and thorium +FACILITY Argonne multi-detecttor system +INC-SOURCE (D-D) Deuterium gas target in a cell 2 cm long +METHOD (TOF) +SAMPLE Solid metal cylinders 2cm in dimater, 2 cm long at 16cm + from the neutron source, at 0 degree source-reaction + angle. Targets 99.9 % pure. +CORRECTION About 0.75 % contribution of the minor isotopes in the + uranium sample was ignored throughout it would have + distorted the measured results by amounts less than + the experimental uncertainties. +DETECTOR (SCIN) Cylindrical liquid hydrogenous scintillators, + 12 cm diameter, 2 cm thick +HISTORY (20050715C) DR +ENDBIB 18 +NOCOMMON 0 0 +ENDSUBENT 21 +SUBENT 14030002 20050715 20050909 1336 +BIB 3 3 +REACTION (92-U-0(N,SCT)92-U-0,,DA) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS Data received from A. B. Smith +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 618 +EN ANG DATA ERR-T +MEV ADEG B/SR PER-CENT + 4.5 1.790E+01 4.880E+00 3.000E+00 + 4.5 2.090E+01 3.947E+00 3.000E+00 + 4.5 2.090E+01 3.925E+00 3.000E+00 + 4.5 2.580E+01 2.513E+00 3.000E+00 + 4.5 2.580E+01 2.379E+00 3.000E+00 + 4.5 2.770E+01 1.976E+00 3.000E+00 + 4.5 2.880E+01 1.620E+00 3.000E+00 + 4.5 3.080E+01 1.315E+00 3.000E+00 + 4.5 3.080E+01 1.358E+00 3.000E+00 + 4.5 3.570E+01 6.351E-01 3.000E+00 + 4.5 3.570E+01 5.979E-01 3.000E+00 + 4.5 3.870E+01 3.293E-01 3.000E+00 + 4.5 4.370E+01 1.248E-01 3.000E+00 + 4.5 4.670E+01 7.192E-02 4.171E+00 + 4.5 4.670E+01 7.938E-02 3.779E+00 + 4.5 5.160E+01 4.740E-02 6.329E+00 + 4.5 5.160E+01 5.529E-02 5.426E+00 + 4.5 5.460E+01 6.062E-02 4.949E+00 + 4.5 5.910E+01 7.805E-02 3.844E+00 + 4.5 6.210E+01 9.118E-02 3.290E+00 + 4.5 6.210E+01 8.960E-02 3.348E+00 + 4.5 6.710E+01 1.100E-01 3.000E+00 + 4.5 6.710E+01 1.072E-01 3.000E+00 + 4.5 7.010E+01 1.080E-01 3.000E+00 + 4.5 7.470E+01 1.209E-01 3.000E+00 + 4.5 7.760E+01 1.187E-01 3.000E+00 + 4.5 7.760E+01 1.177E-01 3.000E+00 + 4.5 8.280E+01 1.062E-01 3.000E+00 + 4.5 8.280E+01 1.140E-01 3.000E+00 + 4.5 8.560E+01 1.048E-01 3.000E+00 + 4.5 9.000E+01 8.997E-02 3.334E+00 + 4.5 9.300E+01 7.586E-02 3.955E+00 + 4.5 9.300E+01 8.032E-02 3.735E+00 + 4.5 9.800E+01 5.515E-02 5.440E+00 + 4.5 9.800E+01 5.457E-02 5.498E+00 + 4.5 1.010E+02 4.502E-02 6.664E+00 + 4.5 1.056E+02 3.260E-02 9.202E+00 + 4.5 1.085E+02 2.403E-02 1.248E+01 + 4.5 1.085E+02 2.516E-02 1.192E+01 + 4.5 1.134E+02 2.127E-02 1.410E+01 + 4.5 1.134E+02 1.989E-02 1.508E+01 + 4.5 1.164E+02 2.531E-02 1.185E+01 + 4.5 1.210E+02 3.219E-02 9.320E+00 + 4.5 1.239E+02 3.785E-02 7.926E+00 + 4.5 1.239E+02 3.769E-02 7.960E+00 + 4.5 1.289E+02 4.737E-02 6.333E+00 + 4.5 1.289E+02 4.842E-02 6.196E+00 + 4.5 1.319E+02 5.513E-02 5.442E+00 + 4.5 1.365E+02 5.999E-02 5.001E+00 + 4.5 1.395E+02 6.013E-02 4.989E+00 + 4.5 1.395E+02 6.337E-02 4.734E+00 + 4.5 1.443E+02 5.611E-02 5.347E+00 + 4.5 1.443E+02 5.314E-02 5.645E+00 + 4.5 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2.543E-02 7.865E+00 +10.0 1.136E+02 2.277E-02 8.783E+00 +10.0 1.166E+02 1.894E-02 1.056E+01 +10.0 1.225E+02 1.651E-02 1.211E+01 +10.0 1.255E+02 1.301E-02 1.537E+01 +10.0 1.290E+02 9.657E-03 2.071E+01 +10.0 1.320E+02 9.843E-03 2.032E+01 +10.0 1.385E+02 9.784E-03 2.044E+01 +10.0 1.415E+02 1.301E-02 1.537E+01 +10.0 1.445E+02 1.380E-02 1.449E+01 +10.0 1.475E+02 1.735E-02 1.153E+01 +10.0 1.485E+02 1.414E-02 1.414E+01 +10.0 1.514E+02 1.517E-02 1.318E+01 +10.0 1.544E+02 1.167E-02 1.714E+01 +10.0 1.574E+02 1.087E-02 1.840E+01 +ENDDATA 620 +ENDSUBENT 628 +SUBENT 14030003 20050715 20050909 1336 +BIB 3 3 +REACTION (90-TH-232(N,SCT)90-TH-232,,DA) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS Data received from A. B. Smith +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 528 +EN ANG DATA ERR-T +MEV ADEG B/SR PER-CENT + 4.5 1.790E+01 4.891E+00 4.000E+00 + 4.5 2.090E+01 4.005E+00 4.000E+00 + 4.5 2.580E+01 2.552E+00 4.000E+00 + 4.5 2.770E+01 2.019E+00 4.000E+00 + 4.5 2.880E+01 1.701E+00 4.000E+00 + 4.5 3.080E+01 1.421E+00 4.000E+00 + 4.5 3.570E+01 6.741E-01 4.000E+00 + 4.5 3.870E+01 3.404E-01 4.000E+00 + 4.5 4.370E+01 1.247E-01 4.000E+00 + 4.5 4.670E+01 7.075E-02 4.240E+00 + 4.5 5.160E+01 4.259E-02 7.044E+00 + 4.5 5.460E+01 4.334E-02 6.922E+00 + 4.5 5.910E+01 6.684E-02 4.488E+00 + 4.5 6.210E+01 7.878E-02 4.000E+00 + 4.5 6.710E+01 1.022E-01 4.000E+00 + 4.5 7.010E+01 1.093E-01 4.000E+00 + 4.5 7.470E+01 1.154E-01 4.000E+00 + 4.5 7.760E+01 1.231E-01 4.000E+00 + 4.5 8.280E+01 1.174E-01 4.000E+00 + 4.5 8.560E+01 1.183E-01 4.000E+00 + 4.5 9.000E+01 8.186E-02 4.000E+00 + 4.5 9.300E+01 7.957E-02 4.000E+00 + 4.5 9.800E+01 5.600E-02 5.357E+00 + 4.5 1.010E+02 4.463E-02 6.722E+00 + 4.5 1.056E+02 2.826E-02 1.062E+01 + 4.5 1.085E+02 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1.010E+02 2.016E-02 9.921E+00 + 8.4 1.055E+02 2.633E-02 7.596E+00 + 8.4 1.085E+02 3.308E-02 6.046E+00 + 8.4 1.134E+02 3.885E-02 5.148E+00 + 8.4 1.164E+02 4.047E-02 4.942E+00 + 8.4 1.209E+02 3.665E-02 5.457E+00 + 8.4 1.239E+02 3.159E-02 6.331E+00 + 8.4 1.289E+02 1.971E-02 1.015E+01 + 8.4 1.319E+02 1.329E-02 1.505E+01 + 8.4 1.364E+02 9.557E-03 2.093E+01 + 8.4 1.394E+02 8.760E-03 2.283E+01 + 8.4 1.443E+02 1.121E-02 1.784E+01 + 8.4 1.463E+02 1.167E-02 1.714E+01 + 8.4 1.473E+02 1.458E-02 1.372E+01 + 8.4 1.493E+02 1.511E-02 1.324E+01 + 8.4 1.542E+02 1.536E-02 1.302E+01 + 8.4 1.572E+02 1.805E-02 1.108E+01 + 9.06 1.826E+01 2.574E+00 4.000E+00 + 9.06 2.221E+01 1.330E+00 4.000E+00 + 9.06 2.617E+01 5.690E-01 4.000E+00 + 9.06 2.816E+01 3.919E-01 4.000E+00 + 9.06 2.905E+01 3.049E-01 4.000E+00 + 9.06 2.905E+01 3.049E-01 4.000E+00 + 9.06 3.234E+01 2.157E-01 4.000E+00 + 9.06 3.632E+01 2.277E-01 4.000E+00 + 9.06 3.911E+01 2.467E-01 4.000E+00 + 9.06 3.911E+01 2.467E-01 4.000E+00 + 9.06 4.409E+01 2.269E-01 4.000E+00 + 9.06 4.758E+01 1.789E-01 4.000E+00 + 9.06 5.157E+01 1.049E-01 4.000E+00 + 9.06 5.456E+01 6.874E-02 4.000E+00 + 9.06 5.456E+01 6.874E-02 4.000E+00 + 9.06 5.955E+01 4.849E-02 4.743E+00 + 9.06 6.304E+01 6.244E-02 4.000E+00 + 9.06 6.704E+01 9.622E-02 4.000E+00 + 9.06 7.003E+01 1.059E-01 4.000E+00 + 9.06 7.003E+01 1.059E-01 4.000E+00 + 9.06 7.602E+01 1.158E-01 4.000E+00 + 9.06 7.902E+01 1.051E-01 4.000E+00 + 9.06 8.301E+01 7.726E-02 4.000E+00 + 9.06 8.601E+01 5.618E-02 4.094E+00 + 9.06 8.601E+01 5.618E-02 4.094E+00 + 9.06 9.150E+01 3.396E-02 6.773E+00 + 9.06 9.449E+01 3.093E-02 7.436E+00 + 9.06 9.849E+01 2.602E-02 8.839E+00 + 9.06 1.015E+02 2.794E-02 8.232E+00 + 9.06 1.015E+02 2.794E-02 8.232E+00 + 9.06 1.070E+02 2.870E-02 8.014E+00 + 9.06 1.100E+02 3.693E-02 6.228E+00 + 9.06 1.140E+02 3.437E-02 6.692E+00 + 9.06 1.170E+02 3.348E-02 6.870E+00 + 9.06 1.170E+02 3.348E-02 6.870E+00 + 9.06 1.229E+02 3.010E-02 7.641E+00 + 9.06 1.259E+02 2.176E-02 1.057E+01 + 9.06 1.294E+02 1.541E-02 1.493E+01 + 9.06 1.324E+02 1.167E-02 1.971E+01 + 9.06 1.324E+02 1.167E-02 1.971E+01 + 9.06 1.389E+02 1.027E-02 2.240E+01 + 9.06 1.419E+02 1.149E-02 2.002E+01 + 9.06 1.449E+02 1.603E-02 1.435E+01 + 9.06 1.479E+02 1.947E-02 1.181E+01 + 9.06 1.479E+02 1.947E-02 1.181E+01 + 9.06 1.489E+02 1.664E-02 1.382E+01 + 9.06 1.518E+02 1.823E-02 1.262E+01 + 9.06 1.548E+02 1.899E-02 1.211E+01 + 9.06 1.578E+02 1.693E-02 1.359E+01 + 9.06 1.578E+02 1.693E-02 1.359E+01 + 9.5 1.776E+01 2.214E+00 4.000E+00 + 9.5 2.171E+01 1.013E+00 4.000E+00 + 9.5 2.567E+01 4.309E-01 4.000E+00 + 9.5 2.766E+01 2.876E-01 4.000E+00 + 9.5 2.855E+01 2.414E-01 4.000E+00 + 9.5 3.184E+01 2.073E-01 4.000E+00 + 9.5 3.582E+01 2.647E-01 4.000E+00 + 9.5 3.861E+01 2.876E-01 4.000E+00 + 9.5 4.359E+01 2.335E-01 4.000E+00 + 9.5 4.708E+01 1.772E-01 4.000E+00 + 9.5 5.107E+01 1.124E-01 4.000E+00 + 9.5 5.406E+01 6.870E-02 4.000E+00 + 9.5 5.905E+01 5.153E-02 4.852E+00 + 9.5 6.254E+01 7.817E-02 4.000E+00 + 9.5 6.654E+01 1.061E-01 4.000E+00 + 9.5 6.953E+01 1.135E-01 4.000E+00 + 9.5 7.552E+01 1.099E-01 4.000E+00 + 9.5 7.852E+01 8.964E-02 4.000E+00 + 9.5 8.251E+01 6.377E-02 4.000E+00 + 9.5 8.551E+01 5.060E-02 4.941E+00 + 9.5 9.100E+01 2.690E-02 9.294E+00 + 9.5 9.399E+01 2.828E-02 8.840E+00 + 9.5 9.799E+01 2.788E-02 8.967E+00 + 9.5 1.010E+02 2.937E-02 8.512E+00 + 9.5 1.065E+02 2.969E-02 8.420E+00 + 9.5 1.095E+02 2.973E-02 8.409E+00 + 9.5 1.135E+02 3.230E-02 7.740E+00 + 9.5 1.165E+02 2.948E-02 8.480E+00 + 9.5 1.224E+02 2.454E-02 1.019E+01 + 9.5 1.254E+02 1.594E-02 1.568E+01 + 9.5 1.289E+02 1.117E-02 2.238E+01 + 9.5 1.319E+02 9.674E-03 2.584E+01 + 9.5 1.384E+02 1.012E-02 2.470E+01 + 9.5 1.414E+02 1.218E-02 2.053E+01 + 9.5 1.444E+02 1.796E-02 1.392E+01 + 9.5 1.474E+02 1.711E-02 1.461E+01 + 9.5 1.484E+02 1.863E-02 1.342E+01 + 9.5 1.513E+02 1.923E-02 1.300E+01 + 9.5 1.543E+02 2.012E-02 1.243E+01 + 9.5 1.573E+02 1.746E-02 1.432E+01 +10.0 1.786E+01 1.985E+00 4.000E+00 +10.0 2.181E+01 8.667E-01 4.000E+00 +10.0 2.577E+01 2.960E-01 3.800E+00 +10.0 2.776E+01 2.288E-01 3.800E+00 +10.0 2.865E+01 1.989E-01 3.800E+00 +10.0 3.193E+01 2.127E-01 3.800E+00 +10.0 3.592E+01 2.899E-01 3.800E+00 +10.0 3.870E+01 3.180E-01 3.800E+00 +10.0 4.369E+01 2.605E-01 3.800E+00 +10.0 4.718E+01 1.709E-01 3.800E+00 +10.0 5.117E+01 9.548E-02 3.800E+00 +10.0 5.416E+01 6.009E-02 4.160E+00 +10.0 5.915E+01 5.525E-02 4.525E+00 +10.0 6.264E+01 7.905E-02 3.800E+00 +10.0 6.664E+01 1.053E-01 3.800E+00 +10.0 6.963E+01 1.199E-01 3.800E+00 +10.0 7.562E+01 1.046E-01 3.800E+00 +10.0 7.862E+01 8.319E-02 3.800E+00 +10.0 8.261E+01 5.295E-02 4.721E+00 +10.0 8.561E+01 3.753E-02 6.661E+00 +10.0 9.110E+01 2.345E-02 1.066E+01 +10.0 9.409E+01 2.761E-02 9.055E+00 +10.0 9.809E+01 2.653E-02 9.423E+00 +10.0 1.011E+02 3.312E-02 7.548E+00 +10.0 1.066E+02 3.071E-02 8.141E+00 +10.0 1.096E+02 3.000E-02 8.333E+00 +10.0 1.136E+02 2.498E-02 1.001E+01 +10.0 1.166E+02 2.255E-02 1.109E+01 +10.0 1.225E+02 1.813E-02 1.379E+01 +10.0 1.255E+02 1.197E-02 2.089E+01 +10.0 1.290E+02 8.959E-03 2.790E+01 +10.0 1.320E+02 1.048E-02 2.385E+01 +10.0 1.385E+02 1.150E-02 2.174E+01 +10.0 1.415E+02 1.358E-02 1.841E+01 +10.0 1.445E+02 1.671E-02 1.496E+01 +10.0 1.475E+02 1.921E-02 1.301E+01 +10.0 1.485E+02 1.708E-02 1.464E+01 +10.0 1.514E+02 1.599E-02 1.563E+01 +10.0 1.544E+02 1.647E-02 1.518E+01 +ENDDATA 530 +ENDSUBENT 538 +ENDENTRY 3 diff --git a/exforall/E06/E0682.x4 b/exforall/E06/E0682.x4 index a0752f926..ffaebe15e 100644 --- a/exforall/E06/E0682.x4 +++ b/exforall/E06/E0682.x4 @@ -1,6 +1,6 @@ -ENTRY E0682 20050224 -SUBENT E0682001 20050224 -BIB 12 64 +ENTRY E0682 20050914 20050914 E032 +SUBENT E0682001 20050914 20050914 E032 +BIB 12 63 TITLE Elastic scattering of 56 MeV polarized deuterons from complex nuclei AUTHOR (K.Hatanaka, K.Imai, S.Kobayashi, T.Matsusue, @@ -11,15 +11,14 @@ INSTITUTE (2JPNOSA) Research Center for Nuclear Physics REFERENCE (J,NP/A,340,(1),93,198005) PART-DET (D) INC-SOURCE Beam intensity is 5 to 20 nA. - (ATOMI) See Table 1 in p95 of reference for detail. + (ATOMI) POL-BM: Monitored by NaI(Tl) scintillatorSee + Table 1 in p95 of reference for detail. SAMPLE Target is self supported. for solid target (foil) METHOD (EDE) FACILITY (ISOCY,2JPNOSA) AVF cyclotron at Research Center for Nuclear Physics DETECTOR (SI) To detect deuteron, transmission type (HPGE) To detect deuteron, cooled by liquid nitrogen - (NAICR) To monitor beam current and polarization, NaI - (Tl) scintillator ADD-RES E0682.005:8-O-16(D,EL)8-O-16 Optical potential parameter See NRDF D0682 DATA,4 for detail. @@ -65,13 +64,13 @@ ADD-RES E0682.005:8-O-16(D,EL)8-O-16 (COMP) Optical model (With and without tensor potentials) HISTORY (20041124T) Converted from NRDF D682 -ENDBIB 64 -COMMON 3 3 -EN POL-BM E-RSL -MEV NO-DIM KEV - 56. 0.75 200. +ENDBIB 63 +COMMON 4 3 +EN POL-BM POL-BM-ERR E-RSL +MEV NO-DIM NO-DIM KEV + 56.0 0.75 0.05 200.0 ENDCOMMON 3 -ENDSUBENT 71 +ENDSUBENT 70 SUBENT E0682002 20050224 BIB 5 13 REACTION (8-O-16(D,EL)8-O-16,,DA) @@ -1194,8 +1193,8 @@ ADEG MB/SR MB/SR 74.60 1.44 0.049 ENDDATA 31 ENDSUBENT 53 -SUBENT E0682031 20050224 -BIB 5 12 +SUBENT E0682031 20050914 20050914 E032 +BIB 6 14 REACTION (26-FE-54(D,EL)26-FE-54,,POL/DA,,ANA) EN-SEC ANG-CM is polar angle between beam and deuteron in center of mass system @@ -1203,16 +1202,18 @@ SAMPLE - Target enrichment is 96.81%. - Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 1.55 mg/cm**2. -ERR-ANALYS (ERR-S) Statistical error +ERR-ANALYS (ERR-S) Statistical uncertainty (ERR-SYS) Uncertainty due to normalization of analyzing power of carbon polarimeter STATUS (TABLE) Data (Fig.2, p98 in reference) received from K.Hatanaka -ENDBIB 12 +HISTORY (20050629A) On. Signature of Ay values corrected + (56.80 to 72.07 deg) +ENDBIB 14 COMMON 1 3 ERR-SYS PER-CENT - 10. + 10.0 ENDCOMMON 3 DATA 3 29 ANG-CM DATA-CM ERR-S @@ -1238,16 +1239,16 @@ ADEG NO-DIM NO-DIM 49.12 -0.326 0.018 51.69 -0.265 0.022 54.25 -0.046 0.025 - 56.80 -0.268 0.027 - 59.36 -0.254 0.026 - 61.91 -0.259 0.028 - 64.45 -0.163 0.031 - 66.99 -0.183 0.037 - 69.53 -0.364 0.073 - 72.07 -0.467 0.073 + 56.80 0.268 0.027 + 59.36 0.254 0.026 + 61.91 0.259 0.028 + 64.45 0.163 0.031 + 66.99 0.183 0.037 + 69.53 0.364 0.073 + 72.07 0.467 0.073 74.60 0.576 0.044 ENDDATA 31 -ENDSUBENT 52 +ENDSUBENT 54 SUBENT E0682032 20050224 BIB 5 12 REACTION (26-FE-54(D,EL)26-FE-54,NN,POL/DA,,ANA) diff --git a/exforall/E12/E1277.x4 b/exforall/E12/E1277.x4 index 4f5d6a49c..b4b1cbb70 100644 --- a/exforall/E12/E1277.x4 +++ b/exforall/E12/E1277.x4 @@ -1,28 +1,32 @@ -ENTRY E1277 910814 -SUBENT E1277001 910814 -BIB 8 19 -TITLE BREAKUP EFFECTS OF 6.7LI ON ELASTIC AND INELASTIC - SCATTERING FROM 12C AT 18-28 MEV/NUCLEON -AUTHOR (K.KATORI,T.SHIMODA,T.FUKUDA,S.SHIMOURA,A.SAKAGUCHI, - M.TANAKA,T.YAMAGATA,N.TAKAHASHI,H.OGATA,M.KAMIMURA, - Y.SAKURAGI) -INSTITUTE (2JPNOSA) - (2JPNKTO) - (2JPNJPN) KOBE TOKIWA JUNIOR COLLEGE - (2JPNKON) - (2JPNKYU) - (2JPNTOK) INSTITUTE FOR NUCLEAR STUDY, TOKYO UNIV. -REFERENCE (J,NP/A,480,33,88) -FACILITY (CYCLO,2JPNOSA) -INC-SOURCE INTERNAL COLD CATHOD ION SOURCE BY BACK-BOMBARING A - NATURAL LI.F CRISTAL (ENRICHED LI.F FOR 6LI) BY XE OR - AR ION - BEAM-ENERGY-SPREAD IS BETWEEN 300. AND 400.KEV -STATUS DATA CONVERTED FROM NRDF -HISTORY (910814T) CONVERTED FROM NRDF DATA NO. D1277 -ENDBIB 19 +ENTRY E1277 20050914 20050914 E032 +SUBENT E1277001 20050914 20050914 E032 +BIB 8 23 +TITLE Breakup effects of 6,7Li on elastic and inelastic + scattering from 12C at 18-28 MeV/nucleon +AUTHOR (K.Katori, T.Shimoda, T.Fukuda, S.Shimoura, + A.Sakaguchi, M.Tanaka, T.Yamagata, N.Takahashi, + H.Ogata, M.Kamimura, Y.Sakuragi) +INSTITUTE (2JPNOSA) Laboratory of Nuclear Studies + (2JPNKTO) Department of Physics + (2JPNKTJ) + (2JPNKON) Department of Physics + (2JPNOSA) College of General Education + (2JPNOSA) Research Center for Nuclear Physics + (2JPNKYU) Department of Physics + (2JPNTOK) Institute for Nuclear Study +REFERENCE (J,NP/A,480,(2),323,198804) +FACILITY (CYCLO,2JPNOSA) Research Center for Nuclear Physics +INC-SOURCE Internal cold cathod ion source by back-bombaring a + natural LiF cristal (enriched LiF for 6Li) by Xe or Ar + ion. + Beam-energy-spread is between 300 and 400 keV. +STATUS Data converted from NRDF +HISTORY (19910814T) Converted from NRDF Data No.D1277. + (20050606A) On. INSTITUTE and REFERENCE corrected. + Changed to lowercase and 4-digit year. +ENDBIB 23 NOCOMMON 0 0 -ENDSUBENT 22 +ENDSUBENT 26 SUBENT E1277002 910814 BIB 8 12 REACTION (6-C-12(3-LI-6,EL)6-C-12,,DA) diff --git a/exforall/E16/E1601.x4 b/exforall/E16/E1601.x4 index 7cc931657..77ab5b9c3 100644 --- a/exforall/E16/E1601.x4 +++ b/exforall/E16/E1601.x4 @@ -1,6 +1,6 @@ -ENTRY E1601 20040311 20040318 -SUBENT E1601001 20040311 20040318 -BIB 11 39 +ENTRY E1601 20050914 20050914 E032 +SUBENT E1601001 20050914 20050914 E032 +BIB 11 38 TITLE Core-excited states of 12(Lambda)C hypernuclei formed in the (pi+,K+) reaction AUTHOR (T.Hasegawa, O.Hashimoto, S.Homma, T.Miyachi, T.Nagae, @@ -8,52 +8,52 @@ AUTHOR (T.Hasegawa, O.Hashimoto, S.Homma, T.Miyachi, T.Nagae, K.Aoki, H.Noumi, H.Bhang, M.Youn, Y.Gavrilov, S.Ajimura, T.Kishimoto, A.Ohkusu, K.Maeda, R.Sawafta, R.P.Redwine) -INSTITUTE (2JPNTOK)Institute for Nuclear Study (INS) - (2JPNKTO)Department of Physics +INSTITUTE (2JPNTOK) Institute for Nuclear Study (INS) + (2JPNKTO) Department of Physics (2JPNLEP) - (3KORNSU)Department of Physics + (3KORNSU) Department of Physics (4RUSJIA) - (2JPNOSA)Department of Physics - (2JPNTOH)Department of Physics - (1USABNL)Physics Department - (1USAMIT)Laboratory for Nuclear Science + (2JPNOSA) Department of Physics + (2JPNTOH) Department of Physics + (1USABNL) Physics Department + (1USAMIT) Laboratory for Nuclear Science REFERENCE (J,PRL,74,(2),224,19950109) PART-DET (KP) -EN-SEC ANG-MIN is minimum polar angle between beam and - positive kaon in laboratory system - ANG-MAX is maximum polar angle between beam and - positive kaon in laboratory system +EN-SEC ANG is polar angle between beam and positive kaon in + laboratory system INC-SOURCE Beam intensity: 3*10**6/spill SAMPLE - Target is natural. - Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 890 mg/cm**2. -FACILITY (SYNCH,2JPNLEP)K6 beam channel -DETECTOR Solid angle of detector is 100msr. - Detector resolution is about 1.9MeV.(1.9+-0.1 MeV - - full width at half minimum) - Drift chamber - (MAGSP)Large superconducting dipole magnet - spectrometer SKS [T. Shintomi et al., IEEE - Trans. Magnetics, MAG-28(1992)585] to - determines the momena of kaons from target. - (CEREN)Used as trigger counters in the identification - of kaons -HISTORY (20030822T)Data converted from NRDF D1601 -ENDBIB 39 -COMMON 3 3 -ANG-MIN ANG-MAX MOM -ADEG ADEG GEV/C - 2.0 14.0 1.06 +FACILITY (SYNCH,2JPNLEP) K6 beam channel +DETECTOR - Solid angle of detector is 100 msr. + - E-RSL is about 1.9 MeV.(1.9+-0.1 MeV - full width at + half minimum) + - Drift chamber + (MAGSP) Large superconducting dipole magnet + spectrometer SKS [T. Shintomi et al., IEEE + Trans. Magnetics, MAG-28(1992)585] to + determines the momena of kaons from target. + (CEREN) Used as trigger counters in the identification + of kaons +HISTORY (20030822T) Data converted from NRDF D1601 + (20050812A) On. REACTION corrected (CP-D/430) +ENDBIB 38 +COMMON 4 3 +MOM E-RSL ANG-MIN ANG-MAX +GEV/C MEV ADEG ADEG + 1.06 1.9 2.0 14.0 ENDCOMMON 3 -ENDSUBENT 46 -SUBENT E1601002 20040311 20040318 -BIB 4 4 -REACTION (6-C-12(PIP,X)1-KP-0,,DA/DE,,IPA) -EN-SEC E-EXC: Excitation energy of 12(Lambda)C -ANALYSIS (INTAD)integrated from 2 to 14 deg -STATUS (CURVE)Data scanned from Fig.2, p225 in reference -ENDBIB 4 +ENDSUBENT 45 +SUBENT E1601002 20050914 20050914 E032 +BIB 5 5 +REACTION (6-C-12(PIP,X)1-KP-0,,IPA/DE) +EN-SEC (E-EXC,6-C-12) Excitation energy of 12(Lambda)C +ANALYSIS (INTAD) integrated from 2 to 14 deg +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (CURVE) Data scanned from Fig.2, p225 in reference +ENDBIB 5 NOCOMMON 0 0 DATA 3 99 E-EXC DATA DATA-ERR @@ -158,18 +158,19 @@ MEV MU-B/MEV MU-B/MEV 3.527E+01 2.840E-01 2.322E-02 3.570E+01 2.350E-01 2.064E-02 ENDDATA 101 -ENDSUBENT 110 -SUBENT E1601003 20040311 20040318 -BIB 5 8 -REACTION (6-C-12(PIP,X)1-KP-0,PAR,DA,,IPA) -EN-SEC (E-EXC,RSD)Excitation energy of 12(Lambda)C -ANALYSIS (INTAD)integrated from 2 to 14 deg +ENDSUBENT 111 +SUBENT E1601003 20050914 20050914 E032 +BIB 6 9 +REACTION (6-C-12(PIP,X)1-KP-0,PAR,IPA) +EN-SEC (E-EXC,6-C-12) Excitation energy of 12(Lambda)C +ANALYSIS (INTAD) integrated from 2 to 14 deg +ERR-ANALYS (DATA-ERR) No information on source of uncertainties FLAG (1.) First 1- state of 12(Lambda)C is assigned (2.) Second 1- state of 12(Lambda)C may be assigned (3.) Third 1- state of 12(Lambda)C may be assigned (4.) 2+ state of 12(Lambda)C is assigned -STATUS (TABLE)Data taken from Table 1, p226 in reference -ENDBIB 8 +STATUS (TABLE) Data taken from Table 1, p226 in reference +ENDBIB 9 NOCOMMON 0 0 DATA 5 4 E-EXC E-EXC-ERR DATA DATA-ERR FLAG @@ -179,5 +180,5 @@ MEV MEV MICRO-B MICRO-B NO-DIM 6.89 0.42 0.19 0.02 3.0 10.68 0.12 0.88 0.06 4.0 ENDDATA 6 -ENDSUBENT 19 +ENDSUBENT 20 ENDENTRY 3 diff --git a/exforall/E16/E1669.x4 b/exforall/E16/E1669.x4 index 158fb41ab..c8b8ed6ab 100644 --- a/exforall/E16/E1669.x4 +++ b/exforall/E16/E1669.x4 @@ -1,49 +1,28 @@ -ENTRY E1669 20001027 20010402 -SUBENT E1669001 20001027 20010402 -BIB 12 22 -TITLE COULOMB EXCITATION OF 11BE -AUTHOR (T.NAKAMURA,T.MOTOBAYASHI,Y.ANDO,A.MENGONI,T.NISHIO, - H.SAKURAI,S.SHIMOURA,T.TERANISHI,Y.YANAGISAWA, - M.ISHIHARA) -INSTITUTE (2JPNTOK) - (2JPNYOK) RIKKYO UNIV. - (2JPNJCL) INSTITUTE FOR PHYSICAL AND CHEMICAL - RESEARCH -REFERENCE (J,PL/B,394,11,1997) -METHOD (TOF,EDE) -FACILITY (CYCLO,2JPNJCL) -DETECTOR (SOLST) - OVERALL-ENERGY-RESOLUTION IS 50.KEV -INC-SOURCE (SPALL) -SAMPLE CHEMICAL-FORM OF TARGET IS ELEMENT - PHYSICAL-FORM OF TARGET IS SLD - TARGET-THICKNESS=350.MG/CM**2 - TARGET-BACKING IS SELF -PART-DET (4-BE-11) -STATUS DATA CONVERTED FROM NRDF +ENTRY E1669 20050914 20050914 E032 +SUBENT E1669001 20050914 20050914 E032 +BIB 5 12 +TITLE Coulomb excitation of 11Be +AUTHOR (T.Nakamura, T.Motobayashi, Y.Ando, A.Mengoni, + T.Nishio, H.Sakurai, S.Shimoura, T.Teranishi, + Y.Yanagisawa, M.Ishihara) +INSTITUTE (2JPNTOK) Department of Physics + (2JPNYOK) Department of Physics + (2JPNIPC) +REFERENCE (J,PL/B,394,(1-2),11,199702) HISTORY (19990514T) CONVERTED FROM NRDF DATA NO. D1669 (20001027A) DATE is corrected -ENDBIB 22 + (20050812A) INSTITUTE and REFERENCE corrected. + Changed to lowercase. +ENDBIB 12 NOCOMMON 0 0 -ENDSUBENT 25 -SUBENT E1669002 20001027 20010402 -BIB 1 1 +ENDSUBENT 15 +SUBENT E1669002 20050914 20050914 E032 +BIB 2 2 REACTION (82-PB-208(4-BE-11,4-BE-11)82-PB-208,PAR,DA) -ENDBIB 1 -COMMON 2 3 -EN LVL-NUMB -MEV NO-DIM -702.9 1. -ENDCOMMON 3 -DATA 4 5 -ANG-CM DATA +DATA-ERR -DATA-ERR -ADEG B/SR B/SR B/SR - 4.513E-01 7.561E+01 +6.952E+00 -7.049E+00 - 1.428E+00 4.069E+01 +3.299E+00 -2.455E+00 - 2.393E+00 1.605E+01 +1.836E+00 -1.870E+00 - 3.398E+00 5.403E+00 +2.872E-01 -4.496E-01 - 4.348E+00 1.408E+00 +9.007E-02 -1.046E-01 -ENDDATA 7 -ENDSUBENT 17 +HISTORY (20050812D) On. Duplication of EXFOR E1806.003 +ENDBIB 2 +NOCOMMON 0 0 +NODATA 0 0 +ENDSUBENT 6 NOSUBENT E1669003 20001027 20010402 ENDENTRY 3 diff --git a/exforall/E16/E1670.x4 b/exforall/E16/E1670.x4 index f0e69dd14..3adf6b945 100644 --- a/exforall/E16/E1670.x4 +++ b/exforall/E16/E1670.x4 @@ -1,19 +1,20 @@ -ENTRY E1670 20040311 20040318 -SUBENT E1670001 20040311 20040318 -BIB 15 62 +ENTRY E1670 20050914 20050914 E032 +SUBENT E1670001 20050914 20050914 E032 +BIB 15 61 TITLE Isobalic analog state of 11Li AUTHOR (T.Teranishi, S.Shimoura, Y.Ando, M.Hirai, N.Iwasa, T.Kikuchi, S.Moriya, T.Motobayashi, H.Murakami, T.Nakamura, T.Nishio, H.Sakurai, T.Uchibori, Y.Watanabe, Y.Yanagisawa, M.Ishihara) INSTITUTE (2JPNIPC) - (2JPNYOK)Department of Physics - (2JPNTOK)Department of Physics + (2JPNYOK) Department of Physics + (2JPNTOK) Department of Physics (2GERGSI) -REFERENCE (J,PL/B,407,110,19970828)Main reference - (J,NP/A,630,387,19980216) - Proceedings of The Sixth International Conference on - Nucleus-Nucleus Collisions (Gatlinburg, 1997) +REFERENCE (J,PL/B,407,(2),110,199708) Main reference + (J,NP/A,630,(1-2),387,199802) + S.Shimoura+, Proceedings of The Sixth International + Conference on Nucleus-Nucleus Collisions (Gatlinburg, + 1997) PART-DET (P) (N) (3-LI-9) @@ -22,21 +23,21 @@ INC-SPECT EN: at the middle of the target SAMPLE - Target enrichment is unknown. - Physical-form of target is solid. - Target is self supported. -METHOD (COINC)Detect 9Li, proton and neutron in coincidence. - (TOF)To determine velocities of charged particles and - neutrons over the 3.1 m flight path between the - target and the hodoscope. -FACILITY (PRJFS,2JPNIPC)A primary 18O beam of 100 AMeV - bombarded a 9Be target of 1.4 g/cm2 - thickness. Reaction products were - analyzed by the projectile fragment - separator RIPS [T.Kubo et al., Nucl. - Instr. Meth. B70(1992)309] to obtain a - radioactive 11Li beam. +METHOD (COINC) Detect 9Li, proton and neutron in coincidence. + (TOF) To determine velocities of charged particles and + neutrons over the 3.1 m flight path between the + target and the hodoscope. +FACILITY (PRJFS,2JPNIPC) A primary 18O beam of 100 AMeV + bombarded a 9Be target of 1.4 g/cm2 + thickness. Reaction products were + analyzed by the projectile fragment + separator RIPS [T.Kubo et al., Nucl. + Instr. Meth. B70(1992)309] to obtain a + radioactive 11Li beam. ANALYSIS Invariant mass method -DETECTOR (SCIN)To detect decay particles from 11Be. The - hodoscope consisted of a 5-mm thick Delta E - plane and two 60-mm thick E planes. +DETECTOR (SCIN) To detect decay particles from 11Be. The + hodoscope consisted of a 5-mm thick Delta E + plane and two 60-mm thick E planes. CORRECTION In the reference data given are not corrected for acceptance. In this work, 11Be*(IAS) decays in two ways: 11Be*(IAS) - larger than 9Li+p+n (direct decay) @@ -45,87 +46,85 @@ CORRECTION In the reference data given are not corrected for acceptance. To avoid ambiguity due to this assumption, authors gave raw data (not corrected by acceptance) in the reference. -ADD-RES Subentry 004:1-H-1(3-LI-11,4-BE-11)0-NN-1 - Energy spectrum (Fermi transition part) - See NRDF D1670 DATA,3 for detail. - Subentry 005:1-H-1(3-LI-11,4-BE-11)0-NN-1 - Angular distribution (Fermi transition - part) - See NRDF D1670 DATA,4 for detail. - Subentry 006:1-H-1(3-LI-11,4-BE-11)0-NN-1 - Excitation energy and width of IAS of - 11Li. This is obtained by fitting Fermi - part of energy spectrum (Fig.2c) with - Gaussian function over the region of 0.4 - MeV < Ed < 1.6 MeV. Effects of the - detector acceptance and the Ed resolution - were taken into account in the fitting - procedure. - See NRDF D1670 DATA,5 for detail. -HISTORY (20030818T)Data converted from NRDF D1670 -ENDBIB 62 +ADD-RES E1670.004:1-H-1(3-LI-11,4-BE-11)0-NN-1 + Energy spectrum (Fermi transition part) + See NRDF D1670 DATA,3 for detail. + E1670.005:1-H-1(3-LI-11,4-BE-11)0-NN-1 + Angular distribution (Fermi transition part) + See NRDF D1670 DATA,4 for detail. + E1670.006:1-H-1(3-LI-11,4-BE-11)0-NN-1 + Excitation energy and width of IAS of 11Li. + This is obtained by fitting Fermi part of + energy spectrum (Fig.2c) with Gaussian + function over the region of 0.4 MeV < Ed < + 1.6 MeV. Effects of the detector acceptance + and the Ed resolution were taken into + account in the fitting procedure. + See NRDF D1670 DATA,5 for detail. +HISTORY (20030818T) Data converted from NRDF D1670 +ENDBIB 61 COMMON 2 3 EN EN-RSL MEV/A PER-CENT 64.0 6.0 ENDCOMMON 3 -ENDSUBENT 69 -SUBENT E1670002 20040311 20040318 -BIB 6 27 -REACTION (1-H-1(3-LI-11,N)4-BE-11,,DA/DE,RSD,IPA/RAW) - DATA: Uncorrected for detector acceptance -EN-SEC ANG-MIN is polar angle between beam and 11Be in - laboratory system - ANG-MAX is polar angle between beam and 11Be in - laboratory system - (E-EXC,4-BE-11)Excitation energy of 11Be. This energy - is calculated by E(d) + 20.14 MeV where - E(d) is decay energy defined in p112 of - the reference and 20.14 MeV is - threshold energy for the 9Li + p + n - channel [G.Audi, A.H.Wapstra, Nucl. - Phys. A 595(1995)409]. -MISC-COL (MISC1)Decay energy E(d) defined in p112 of the - reference - (MISC2)Detector acceptance. True energy spectrum can - be obtained by dividing tabulated data by this - acceptance. +ENDSUBENT 68 +SUBENT E1670002 20050914 20050914 E032 +BIB 7 27 +REACTION (1-H-1(3-LI-11,N)4-BE-11,,IPA/DE,,RAW) + Uncorrected for detector acceptance +EN-SEC ANG is polar angle between beam and 11Be in laboratory + system + (E-EXC,4-BE-11) Excitation energy of 11Be. This energy + is calculated by E(d) + 20.14 MeV + where E(d) is decay energy defined in + p112 of the reference and 20.14 MeV is + threshold energy for the 9Li + p + n + channel [G.Audi, A.H.Wapstra, Nucl. + Phys. A 595(1995)409]. +MISC-COL (MISC1) Decay energy E(d) defined in p112 of the + reference + (MISC2) Detector acceptance. True energy spectrum can + be obtained by dividing tabulated data by this + acceptance. SAMPLE - Chemical-form of target is CH2. (CH2)n and C target are used, C target was used to subtract the contributions of carbon nuclei in the (CH2)n target. - Target-thickness: 191 and 188 mg/cm2 for (CH2)n and C target, respectively. -ERR-ANALYS (ERR-1)Mainly due to the uncertainty in neutron - detection efficiency -STATUS (TABLE)Data (Fig.2(a), p112 in reference) received by - e-mail from T.Teranishi (2003.09.17) +ERR-ANALYS (ERR-S) Statistical uncertainty + (ERR-SYS) Mainly due to the uncertainty in neutron + detection efficiency +STATUS (TABLE) Data (Fig.2(a), p112 in reference) received by + e-mail from T.Teranishi (2003.09.17) +HISTORY (20050812A) On. REACTION corrected (CP-D/430) ENDBIB 27 COMMON 3 3 -ANG-MIN ANG-MAX ERR-1 +ANG-MIN ANG-MAX ERR-SYS ADEG ADEG PER-CENT 0.0 5.0 10.0 ENDCOMMON 3 DATA 5 100 E-EXC MISC1 DATA ERR-S MISC2 MEV MEV MB/MEV MB/MEV NO-DIM - 20.19 0.05 0.0 0.0 0.03 + 20.19 0.05 0.00 0.00 0.030 20.29 0.15 0.02 0.01 0.095 20.39 0.25 -0.04 0.03 0.155 - 20.49 0.35 0.0 0.05 0.2 + 20.49 0.35 0.00 0.05 0.200 20.59 0.45 0.17 0.07 0.236 - 20.69 0.55 0.3 0.08 0.265 - 20.79 0.65 0.58 0.1 0.287 - 20.89 0.75 1.0 0.12 0.306 + 20.69 0.55 0.30 0.08 0.265 + 20.79 0.65 0.58 0.10 0.287 + 20.89 0.75 1.00 0.12 0.306 20.99 0.85 1.29 0.13 0.322 21.09 0.95 1.96 0.16 0.336 21.19 1.05 1.97 0.16 0.347 21.29 1.15 1.83 0.15 0.358 21.39 1.25 1.24 0.13 0.368 21.49 1.35 0.81 0.12 0.376 - 21.59 1.45 1.1 0.11 0.382 - 21.69 1.55 0.62 0.1 0.387 - 21.79 1.65 0.72 0.1 0.391 - 21.89 1.75 0.68 0.1 0.394 + 21.59 1.45 1.10 0.11 0.382 + 21.69 1.55 0.62 0.10 0.387 + 21.79 1.65 0.72 0.10 0.391 + 21.89 1.75 0.68 0.10 0.394 21.99 1.85 0.49 0.09 0.397 22.09 1.95 0.47 0.08 0.398 22.19 2.05 0.39 0.08 0.399 @@ -135,12 +134,12 @@ MEV MEV MB/MEV MB/MEV NO-DIM 22.59 2.45 0.42 0.08 0.394 22.69 2.55 0.28 0.08 0.392 22.79 2.65 0.38 0.07 0.388 - 22.89 2.75 0.3 0.08 0.384 - 22.99 2.85 0.15 0.07 0.38 + 22.89 2.75 0.30 0.08 0.384 + 22.99 2.85 0.15 0.07 0.380 23.09 2.95 0.24 0.07 0.374 23.19 3.05 0.26 0.08 0.369 23.29 3.15 0.33 0.07 0.364 - 23.39 3.25 0.3 0.07 0.358 + 23.39 3.25 0.30 0.07 0.358 23.49 3.35 0.33 0.06 0.351 23.59 3.45 0.23 0.06 0.344 23.69 3.55 0.26 0.07 0.338 @@ -151,13 +150,13 @@ MEV MEV MB/MEV MB/MEV NO-DIM 24.19 4.05 0.15 0.06 0.303 24.29 4.15 0.22 0.06 0.295 24.39 4.25 0.09 0.06 0.287 - 24.49 4.35 0.18 0.05 0.28 + 24.49 4.35 0.18 0.05 0.280 24.59 4.45 0.14 0.06 0.273 24.69 4.55 0.09 0.05 0.266 24.79 4.65 0.19 0.05 0.259 24.89 4.75 0.12 0.05 0.252 24.99 4.85 0.13 0.05 0.245 - 25.09 4.95 0.1 0.04 0.238 + 25.09 4.95 0.10 0.04 0.238 25.19 5.05 0.17 0.05 0.232 25.29 5.15 0.02 0.04 0.225 25.39 5.25 0.04 0.03 0.219 @@ -165,11 +164,11 @@ MEV MEV MB/MEV MB/MEV NO-DIM 25.59 5.45 0.07 0.04 0.207 25.69 5.55 0.11 0.04 0.201 25.79 5.65 0.04 0.04 0.195 - 25.89 5.75 0.1 0.04 0.19 + 25.89 5.75 0.10 0.04 0.190 25.99 5.85 0.09 0.04 0.185 - 26.09 5.95 0.06 0.04 0.18 + 26.09 5.95 0.06 0.04 0.180 26.19 6.05 0.06 0.04 0.174 - 26.29 6.15 0.08 0.04 0.17 + 26.29 6.15 0.08 0.04 0.170 26.39 6.25 0.02 0.04 0.165 26.49 6.35 0.09 0.04 0.161 26.59 6.45 0.07 0.04 0.156 @@ -179,10 +178,10 @@ MEV MEV MB/MEV MB/MEV NO-DIM 26.99 6.85 0.05 0.03 0.141 27.09 6.95 0.06 0.03 0.137 27.19 7.05 0.04 0.03 0.133 - 27.29 7.15 0.04 0.03 0.13 - 27.39 7.25 0.0 0.03 0.127 + 27.29 7.15 0.04 0.03 0.130 + 27.39 7.25 0.00 0.03 0.127 27.49 7.35 0.03 0.03 0.123 - 27.59 7.45 0.03 0.03 0.12 + 27.59 7.45 0.03 0.03 0.120 27.69 7.55 0.03 0.03 0.117 27.79 7.65 0.07 0.03 0.115 27.89 7.75 0.01 0.02 0.112 @@ -194,13 +193,13 @@ MEV MEV MB/MEV MB/MEV NO-DIM 28.49 8.35 0.03 0.03 0.097 28.59 8.45 0.02 0.02 0.095 28.69 8.55 0.08 0.03 0.093 - 28.79 8.65 0.0 0.02 0.091 + 28.79 8.65 0.00 0.02 0.091 28.89 8.75 0.01 0.02 0.089 28.99 8.85 0.01 0.02 0.087 29.09 8.95 0.02 0.02 0.085 29.19 9.05 0.04 0.02 0.083 29.29 9.15 0.01 0.02 0.082 - 29.39 9.25 0.0 0.02 0.08 + 29.39 9.25 0.00 0.02 0.080 29.49 9.35 -0.01 0.03 0.078 29.59 9.45 -0.01 0.02 0.077 29.69 9.55 0.02 0.02 0.075 @@ -210,60 +209,60 @@ MEV MEV MB/MEV MB/MEV NO-DIM 30.09 9.95 0.02 0.02 0.069 ENDDATA 102 ENDSUBENT 138 -SUBENT E1670003 20040311 20040318 -BIB 6 27 -REACTION (1-H-2(3-LI-11,2N)4-BE-11,,DA/DE,RSD,IPA/RAW) - DATA: Uncorrected for detector acceptance -EN-SEC ANG-MIN is polar angle between beam and 11Be in - laboratory system - ANG-MAX is polar angle between beam and 11Be in - laboratory system - (E-EXC,4-BE-11)Excitation energy of 11Be. This energy - is calculated by E(d) + 20.14 MeV where - E(d) is decay energy defined in p112 of - the reference and 20.14 MeV is - threshold energy for the 9Li + p + n - channel [G.Audi, A.H.Wapstra, Nucl. - Phys. A 595(1995)409]. -MISC-COL (MISC1)Decay energy E(d) defined in p112 of the - reference - (MISC2)Detector acceptance. True energy spectrum can - be obtained by dividing tabulated data by this - acceptance. +SUBENT E1670003 20050914 20050914 E032 +BIB 7 27 +REACTION (1-H-2(3-LI-11,2N)4-BE-11,,IPA/DE,,RAW) + Uncorrected for detector acceptance +EN-SEC ANG is polar angle between beam and 11Be in laboratory + system + (E-EXC,4-BE-11) Excitation energy of 11Be. This energy + is calculated by E(d) + 20.14 MeV + where E(d) is decay energy defined in + p112 of the reference and 20.14 MeV is + threshold energy for the 9Li + p + n + channel [G.Audi, A.H.Wapstra, Nucl. + Phys. A 595(1995)409]. +MISC-COL (MISC1) Decay energy E(d) defined in p112 of the + reference + (MISC2) Detector acceptance. True energy spectrum can + be obtained by dividing tabulated data by this + acceptance. SAMPLE - Chemical-form of target is CD2. (CD2)n and C target are used, C target was used to subtract the contributions of carbon nuclei in the (CH2)n target. - Target-thickness: 206 and 188 mg/cm2 for (CD2)n and C target, respectively. -ERR-ANALYS (ERR-1)Mainly due to the uncertainty in neutron - detection efficiency -STATUS (TABLE)Data (Fig.2(b), p112 in reference) received by - e-mail from T.Teranishi (2003.09.17) +ERR-ANALYS (ERR-S) Statistical uncertainty + (ERR-SYS) Mainly due to the uncertainty in neutron + detection efficiency +STATUS (TABLE) Data (Fig.2(b), p112 in reference) received by + e-mail from T.Teranishi (2003.09.17) +HISTORY (20050812A) On. REACTION corrected (CP-D/430) ENDBIB 27 COMMON 3 3 -ANG-MIN ANG-MAX ERR-1 +ANG-MIN ANG-MAX ERR-SYS ADEG ADEG PER-CENT 0.0 5.0 10.0 ENDCOMMON 3 DATA 5 100 E-EXC MISC1 DATA ERR-S MISC2 MEV MEV MB/MEV MB/MEV NO-DIM - 20.19 0.05 0.0 0.0 0.03 + 20.19 0.05 0.00 0.00 0.030 20.29 0.15 0.03 0.01 0.095 20.39 0.25 -0.03 0.03 0.155 - 20.49 0.35 -0.04 0.05 0.2 + 20.49 0.35 -0.04 0.05 0.200 20.59 0.45 0.04 0.06 0.236 20.69 0.55 0.14 0.07 0.265 20.79 0.65 0.25 0.08 0.287 - 20.89 0.75 0.51 0.1 0.306 + 20.89 0.75 0.51 0.10 0.306 20.99 0.85 0.72 0.11 0.322 21.09 0.95 0.73 0.12 0.336 21.19 1.05 0.67 0.12 0.347 21.29 1.15 0.77 0.12 0.358 - 21.39 1.25 0.6 0.1 0.368 - 21.49 1.35 0.6 0.1 0.376 + 21.39 1.25 0.60 0.10 0.368 + 21.49 1.35 0.60 0.10 0.376 21.59 1.45 0.55 0.09 0.382 - 21.69 1.55 0.5 0.09 0.387 + 21.69 1.55 0.50 0.09 0.387 21.79 1.65 0.43 0.09 0.391 21.89 1.75 0.43 0.08 0.394 21.99 1.85 0.43 0.08 0.397 @@ -276,13 +275,13 @@ MEV MEV MB/MEV MB/MEV NO-DIM 22.69 2.55 0.24 0.07 0.392 22.79 2.65 0.31 0.07 0.388 22.89 2.75 0.23 0.07 0.384 - 22.99 2.85 0.21 0.07 0.38 - 23.09 2.95 0.2 0.07 0.374 + 22.99 2.85 0.21 0.07 0.380 + 23.09 2.95 0.20 0.07 0.374 23.19 3.05 0.14 0.07 0.369 23.29 3.15 0.23 0.06 0.364 23.39 3.25 0.11 0.06 0.358 23.49 3.35 0.32 0.06 0.351 - 23.59 3.45 0.3 0.06 0.344 + 23.59 3.45 0.30 0.06 0.344 23.69 3.55 0.16 0.06 0.338 23.79 3.65 0.12 0.06 0.331 23.89 3.75 0.19 0.06 0.324 @@ -291,7 +290,7 @@ MEV MEV MB/MEV MB/MEV NO-DIM 24.19 4.05 0.18 0.06 0.303 24.29 4.15 0.24 0.05 0.295 24.39 4.25 0.08 0.05 0.287 - 24.49 4.35 0.09 0.05 0.28 + 24.49 4.35 0.09 0.05 0.280 24.59 4.45 0.12 0.05 0.273 24.69 4.55 0.21 0.05 0.266 24.79 4.65 0.16 0.04 0.259 @@ -305,11 +304,11 @@ MEV MEV MB/MEV MB/MEV NO-DIM 25.59 5.45 0.19 0.05 0.207 25.69 5.55 0.11 0.04 0.201 25.79 5.65 0.09 0.04 0.195 - 25.89 5.75 0.09 0.04 0.19 + 25.89 5.75 0.09 0.04 0.190 25.99 5.85 0.05 0.04 0.185 - 26.09 5.95 0.08 0.04 0.18 + 26.09 5.95 0.08 0.04 0.180 26.19 6.05 0.09 0.04 0.174 - 26.29 6.15 0.09 0.04 0.17 + 26.29 6.15 0.09 0.04 0.170 26.39 6.25 0.04 0.04 0.165 26.49 6.35 0.05 0.03 0.161 26.59 6.45 0.09 0.04 0.156 @@ -319,15 +318,15 @@ MEV MEV MB/MEV MB/MEV NO-DIM 26.99 6.85 0.08 0.04 0.141 27.09 6.95 0.03 0.03 0.137 27.19 7.05 0.12 0.04 0.133 - 27.29 7.15 0.1 0.03 0.13 + 27.29 7.15 0.10 0.03 0.130 27.39 7.25 0.08 0.04 0.127 27.49 7.35 0.05 0.03 0.123 - 27.59 7.45 0.05 0.03 0.12 + 27.59 7.45 0.05 0.03 0.120 27.69 7.55 0.01 0.03 0.117 27.79 7.65 0.09 0.03 0.115 27.89 7.75 0.02 0.03 0.112 27.99 7.85 0.05 0.03 0.109 - 28.09 7.95 0.1 0.03 0.107 + 28.09 7.95 0.10 0.03 0.107 28.19 8.05 0.04 0.03 0.104 28.29 8.15 0.07 0.03 0.101 28.39 8.25 0.04 0.03 0.099 @@ -339,8 +338,8 @@ MEV MEV MB/MEV MB/MEV NO-DIM 28.99 8.85 0.03 0.02 0.087 29.09 8.95 0.03 0.02 0.085 29.19 9.05 0.04 0.02 0.083 - 29.29 9.15 0.0 0.02 0.082 - 29.39 9.25 -0.02 0.02 0.08 + 29.29 9.15 0.00 0.02 0.082 + 29.39 9.25 -0.02 0.02 0.080 29.49 9.35 0.03 0.03 0.078 29.59 9.45 0.01 0.02 0.077 29.69 9.55 0.04 0.02 0.075 diff --git a/exforall/E17/E1703.x4 b/exforall/E17/E1703.x4 index 27284d786..2a26324a1 100644 --- a/exforall/E17/E1703.x4 +++ b/exforall/E17/E1703.x4 @@ -1,5 +1,5 @@ -ENTRY E1703 20050224 -SUBENT E1703001 20050224 +ENTRY E1703 20050914 20050914 E032 +SUBENT E1703001 20050914 20050914 E032 BIB 8 35 TITLE Particle decays from 12B and 12N mirror nuclei AUTHOR (T.Inomata, H.Akimune, I.Daito, H.Ejiri, H.Fujimura, @@ -39,31 +39,36 @@ HISTORY (20020705T) Data converted from NRDF D1703 ENDBIB 35 NOCOMMON 0 0 ENDSUBENT 38 -SUBENT E1703002 20021015 20021021 -BIB 8 18 -REACTION (6-C-12(D,HE2+N)5-B-11,SEQ/PAR,DA/CRL,N/HE2,REL) +SUBENT E1703002 20050914 20050914 E032 +BIB 11 23 +REACTION (6-C-12(D,HE2+N)5-B-11,SEQ/PAR,DA/DA,N/HE2,REL) PART-DET (N) (HE2) -INC-SOURCE Beam intensity is less than 0.05NA. -SAMPLE Target-thickness is 30mg/cm**2. -DETECTOR Solid angle of detector is 2.4MSR.(for - Large-acceptance spectrometer (LAS)) - Detector resolution is 600KEV.(for final-state - spectrum of neutron) - (MAGSP)with plastic scintillator to detect two protons - decay from 2He -ADD-RES (COMP)ANGCOR, See [M. N. Harakeh and L. W. Put, KVI - internal report, KVI 67 (1979)]. -EN-SEC ANG1 is polar angle between beam and 2He - ANG2-CM is polar angle between beam and neutron +EN-SEC - ANG1 is polar angle between beam and 2He in + laboratory system + - ANG2-CM is polar angle between beam and neutron in + center of mass system (E-LVL1,5-B-11) (E-LVL2,5-B-12) -STATUS (CURVE)Data scanned from Fig.6, p3159 in reference -ENDBIB 18 -COMMON 4 3 -EN ANG1 E-LVL1 E-LVL2 -MEV ADEG MEV MEV - 200.0 0.0 0.0 7.7 +INC-SOURCE Beam intensity is less than 0.05 nA. +SAMPLE Target-thickness is 30 mg/cm**2. +METHOD (COINC) Detect 2He and neutron in coincidence. +DETECTOR - Solid angle of detector is 2.4 msr.(for + Large-acceptance spectrometer (LAS)) + - E-RSL: for final-state spectrum of neutron + (MAGSP) With plastic scintillator to detect two + protons decay from 2He + (SCIN) To detect decay neutron from 12B +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) ANGCOR, See [M. N. Harakeh and L. W. Put, KVI + internal report, KVI 67 (1979)]. +STATUS (CURVE) Data scanned from Fig.6, p3159 in reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 23 +COMMON 5 3 +EN E-RSL ANG1 E-LVL1 E-LVL2 +MEV KEV ADEG MEV MEV + 200.0 600.0 0.0 0.0 7.7 ENDCOMMON 3 DATA 4 11 ANG2-CM DATA +DATA-ERR -DATA-ERR @@ -80,7 +85,7 @@ ADEG ARB-UNITS ARB-UNITS ARB-UNITS 1.556E+02 6.129E-02 5.054E-03 5.054E-03 1.608E+02 5.690E-02 6.498E-03 6.498E-03 ENDDATA 13 -ENDSUBENT 40 +ENDSUBENT 45 SUBENT E1703003 20021015 20021021 BIB 9 21 REACTION (6-C-12(HE3,T+P)6-C-11,SEQ/PAR,DA/DA,P/T) diff --git a/exforall/E17/E1711.x4 b/exforall/E17/E1711.x4 index f7308931f..2327957be 100644 --- a/exforall/E17/E1711.x4 +++ b/exforall/E17/E1711.x4 @@ -1,43 +1,78 @@ -ENTRY E1711 20030306 20030310 -SUBENT E1711001 20030306 20030310 -BIB 8 30 +ENTRY E1711 20050914 20050914 E032 +SUBENT E1711001 20050914 20050914 E032 +BIB 9 65 TITLE Azimuthal distribution, azimuthal correlation, and reactionplane dispersion in the reaction 10.6 MeV/nucleon 84Kr on 27Al AUTHOR (W.Q.Shen, W.Ye, Y.G.Ma, J.Feng, J.S.Wang, - K.Yuasa-Nakagawa, T.Nakagawa, K.Yoshida, J.Kasagi, - Y.Futami, S.M.Lee, K.Furutaka, K.Matsuda) -INSTITUTE (3CPRCPR)China Center of Advanced Science and - Technology (World Laboratory), Beijing + K.Yuasa-Nakagawa, T.Nakagawa, K.Yoshida, J.Kasagi, + Y.Futami, S.M.Lee, K.Furutaka, K.Matsuda) +INSTITUTE (3CPRCPR) China Center of Advanced Science and + Technology (World Laboratory), Beijing (3CPRNRS) - (3CPRFUD)Fudan - T.D.Lee Physics Laboratory + (3CPRFUD) Fudan - T.D.Lee Physics Laboratory (2JPNIPC) - (2JPNTOH)Laboratory of Nuclear Science - (2JPNTSU)Insitute of Physics - (2JPNTIT)Department of Physics -REFERENCE (J,PR/C,56,1996,199710) -SAMPLE Target enrichment is unknown. - Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 0.6mg/cm**2. - Target is self supported. + (2JPNTOH) Laboratory of Nuclear Science + (2JPNTSU) Insitute of Physics + (2JPNTIT) Department of Physics +REFERENCE (J,PR/C,56,(4),1996,199710) +SAMPLE - Target enrichment is unknown. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 0.6 mg/cm**2. + - Target is self supported. FACILITY (CYCLO,2JPNIPC) -DETECTOR Solid angle of detector is 9.42sr.(for charged +DETECTOR Solid angle of detector is 9.42 sr.(for charged particle detection, ) - (TELES)consists of two channel plate detectors(CPD) - and a solid state detector(SSD), to detect - fragment - (SCIN)with a thick BaF2 crystal, to detect charged - particles (proton, alpha) with polar angle range - from 10deg to 160deg -HISTORY (20020805T)Data converted from NRDF D1711 -ENDBIB 30 + (TELES) Consists of two channel plate detectors(CPD) + and a solid state detector(SSD), to detect + fragment + (SCIN) With a thick BaF2 crystal, to detect charged + particles (proton, alpha) with polar angle + range from 10deg to 160deg +ADD-RES E1711.018:36-KR-84(13-AL-27,F+P)MASS + Angular distribution (anisotropic + coefficient of azimutial distribution (see + eq.1 in text)) + See NRDF D1711 DATA,17 for detail. + E1711.019:36-KR-84(13-AL-27,F+2P)MASS + Angular correlation (anisotropic coefficient + of azimutial correlation (see eqs.2 and 5 in + text)) + See NRDF D1711 DATA,18 for detail. + E1711.020:36-KR-84(13-AL-27,F+A)MASS + Angular distribution (anisotropic + coefficient of azimutial distribution (see + eq.1 in text)) + See NRDF D1711 DATA,19 for detail. + E1711.021:36-KR-84(13-AL-27,F+2A)MASS + Angular correlation (anisotropic coefficient + of azimutial correlation (see eqs.2 and 5 in + text)) + See NRDF D1711 DATA,20 for detail. + E1711.022:36-KR-84(13-AL-27,F+2P)MASS + Angular correlation (anisotropic coefficient + of azimutial correlation (see eqs.2 and 5 in + text)) + See NRDF D1711 DATA,21 for detail. + E1711.023:36-KR-84(13-AL-27,F+P+A)MASS + Angular correlation (anisotropic coefficient + of azimutial correlation (see eqs.2 and 5 in + text)) + See NRDF D1711 DATA,22 for detail. + E1711.024:36-KR-84(13-AL-27,F+2A)MASS + Angular correlation (anisotropic coefficient + of azimutial correlation (see eqs.2 and 5 in + text)) + See NRDF D1711 DATA,23 for detail. +HISTORY (20020805T) Data converted from NRDF D1711 +ENDBIB 65 COMMON 1 3 EN MEV/A 10.6 ENDCOMMON 3 -ENDSUBENT 37 +ENDSUBENT 72 SUBENT E1711002 20030306 20030310 BIB 5 10 REACTION (36-KR-84(13-AL-27,P+F)MASS,,DA,,REL) @@ -150,20 +185,24 @@ NO-DIM NO-DIM ADEG ARB-UNITS 80.0 100.0 1.619E+02 4.926E+04 ENDDATA 7 ENDSUBENT 26 -SUBENT E1711006 20030306 20030310 -BIB 5 11 -REACTION (36-KR-84(13-AL-27,2P+F)MASS,,DA/CRL,P/P/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (P) -EN-SEC ANG1 is azimuthal angle between two protons - ANG2 is polar angle between beam and fission fragment +SUBENT E1711006 20050914 20050914 E032 +BIB 7 15 +REACTION (36-KR-84(13-AL-27,2P+F)MASS,,DA/DA,P+P/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (P) + (FF) +EN-SEC - ANG1 is azimuthal angle between two protons + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect proton, proton and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2(left), p1998 in - reference -ENDBIB 11 +STATUS (CURVE) Data scanned from Fig.2(left), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 15 COMMON 1 3 ANG2 ADEG @@ -181,21 +220,25 @@ NO-DIM NO-DIM ADEG ARB-UNITS 20.0 40.0 1.630E+02 1.929E+02 20.0 40.0 1.853E+02 2.102E+02 ENDDATA 10 -ENDSUBENT 30 -SUBENT E1711007 20030306 20030310 -BIB 5 11 -REACTION (36-KR-84(13-AL-27,2P+F)MASS,,DA/CRL,P/P/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (P) -EN-SEC ANG1 is azimuthal angle between two protons - ANG2 is polar angle between beam and fission fragment +ENDSUBENT 34 +SUBENT E1711007 20050914 20050914 E032 +BIB 7 15 +REACTION (36-KR-84(13-AL-27,2P+F)MASS,,DA/DA,P+P/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (P) + (FF) +EN-SEC - ANG1 is azimuthal angle between two protons + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect proton, proton and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (left), p1998 in - reference -ENDBIB 11 +STATUS (CURVE) Data scanned from Fig.2 (left), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 15 COMMON 1 3 ANG2 ADEG @@ -213,21 +256,25 @@ NO-DIM NO-DIM ADEG ARB-UNITS 40.0 60.0 1.503E+02 1.022E+03 40.0 60.0 1.743E+02 1.055E+03 ENDDATA 10 -ENDSUBENT 30 -SUBENT E1711008 20030306 20030310 -BIB 5 11 -REACTION (36-KR-84(13-AL-27,2P+F)MASS,,DA/CRL,P/P/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (P) -EN-SEC ANG1 is azimuthal angle between two protons - ANG2 is polar angle between beam and fission fragment +ENDSUBENT 34 +SUBENT E1711008 20050914 20050914 E032 +BIB 7 15 +REACTION (36-KR-84(13-AL-27,2P+F)MASS,,DA/DA,P+P/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (P) + (FF) +EN-SEC - ANG1 is azimuthal angle between two protons + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect proton, proton and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (left), p1998 in - reference -ENDBIB 11 +STATUS (CURVE) Data scanned from Fig.2 (left), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 15 COMMON 1 3 ANG2 ADEG @@ -245,21 +292,25 @@ NO-DIM NO-DIM ADEG ARB-UNITS 60.0 80.0 1.500E+02 3.394E+03 60.0 80.0 1.740E+02 3.394E+03 ENDDATA 10 -ENDSUBENT 30 -SUBENT E1711009 20030306 20030310 -BIB 5 11 -REACTION (36-KR-84(13-AL-27,2P+F)MASS,,DA/CRL,P/P/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (P) -EN-SEC ANG1 is azimuthal angle between two protons - ANG2 is polar angle between beam and fission fragment +ENDSUBENT 34 +SUBENT E1711009 20050914 20050914 E032 +BIB 7 15 +REACTION (36-KR-84(13-AL-27,2P+F)MASS,,DA/DA,P+P/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (P) + (FF) +EN-SEC - ANG1 is azimuthal angle between two protons + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect proton, proton and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (left), p1998 in - reference -ENDBIB 11 +STATUS (CURVE) Data scanned from Fig.2 (left), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 15 COMMON 1 3 ANG2 ADEG @@ -277,22 +328,26 @@ NO-DIM NO-DIM ADEG ARB-UNITS 80.0 100.0 1.460E+02 2.579E+03 80.0 100.0 1.700E+02 2.563E+03 ENDDATA 10 -ENDSUBENT 30 -SUBENT E1711010 20030306 20030310 -BIB 5 12 -REACTION (36-KR-84(13-AL-27,P+A+F)MASS,,DA/CRL,P/A/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (P) +ENDSUBENT 34 +SUBENT E1711010 20050914 20050914 E032 +BIB 7 16 +REACTION (36-KR-84(13-AL-27,P+A+F)MASS,,DA/DA,P+A/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (P) (A) -EN-SEC ANG1 is azimuthal angle between proton and alpha - ANG2 is polar angle between beam and fission fragment + (FF) +EN-SEC - ANG1 is azimuthal angle between proton and alpha + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect proton, alpha and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (center), p1998 in - reference -ENDBIB 12 +STATUS (CURVE) Data scanned from Fig.2 (center), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 16 COMMON 1 3 ANG2 ADEG @@ -310,22 +365,26 @@ NO-DIM NO-DIM ADEG ARB-UNITS 20.0 40.0 1.442E+02 4.310E+01 20.0 40.0 1.671E+02 6.475E+01 ENDDATA 10 -ENDSUBENT 31 -SUBENT E1711011 20030306 20030310 -BIB 5 12 -REACTION (36-KR-84(13-AL-27,P+A+F)MASS,,DA/CRL,P/A/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (P) +ENDSUBENT 35 +SUBENT E1711011 20050914 20050914 E032 +BIB 7 16 +REACTION (36-KR-84(13-AL-27,P+A+F)MASS,,DA/DA,P+A/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (P) (A) -EN-SEC ANG1 is azimuthal angle between proton and alpha - ANG2 is polar angle between beam and fission fragment + (FF) +EN-SEC - ANG1 is azimuthal angle between proton and alpha + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect proton, alpha and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (center), p1998 in - reference -ENDBIB 12 +STATUS (CURVE) Data scanned from Fig.2 (center), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 16 COMMON 1 3 ANG2 ADEG @@ -343,22 +402,26 @@ NO-DIM NO-DIM ADEG ARB-UNITS 40.0 60.0 2.845E+02 1.941E+02 40.0 60.0 3.295E+02 2.515E+02 ENDDATA 10 -ENDSUBENT 31 -SUBENT E1711012 20030306 20030310 -BIB 5 12 -REACTION (36-KR-84(13-AL-27,P+A+F)MASS,,DA/CRL,P/A/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (P) +ENDSUBENT 35 +SUBENT E1711012 20050914 20050914 E032 +BIB 7 16 +REACTION (36-KR-84(13-AL-27,P+A+F)MASS,,DA/DA,P+A/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (P) (A) -EN-SEC ANG1 is azimuthal angle between proton and alpha - ANG2 is polar angle between beam and fission fragment + (FF) +EN-SEC - ANG1 is azimuthal angle between proton and alpha + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect proton, alpha and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (center), p1998 in - reference -ENDBIB 12 +STATUS (CURVE) Data scanned from Fig.2 (center), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 16 COMMON 1 3 ANG2 ADEG @@ -376,22 +439,26 @@ NO-DIM NO-DIM ADEG ARB-UNITS 60.0 80.0 1.422E+02 9.596E+02 60.0 80.0 1.661E+02 1.399E+03 ENDDATA 10 -ENDSUBENT 31 -SUBENT E1711013 20030306 20030310 -BIB 5 12 -REACTION (36-KR-84(13-AL-27,P+A+F)MASS,,DA/CRL,P/A/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (P) +ENDSUBENT 35 +SUBENT E1711013 20050914 20050914 E032 +BIB 7 16 +REACTION (36-KR-84(13-AL-27,P+A+F)MASS,,DA/DA,P+A/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (P) (A) -EN-SEC ANG1 is azimuthal angle between proton and alpha - ANG2 is polar angle between beam and fission fragment + (FF) +EN-SEC - ANG1 is azimuthal angle between proton and alpha + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect proton, alpha and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (center), p1998 in - reference -ENDBIB 12 +STATUS (CURVE) Data scanned from Fig.2 (center), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 16 COMMON 1 3 ANG2 ADEG @@ -409,21 +476,25 @@ NO-DIM NO-DIM ADEG ARB-UNITS 80.0 100.0 1.443E+02 8.235E+02 80.0 100.0 1.672E+02 1.317E+03 ENDDATA 10 -ENDSUBENT 31 -SUBENT E1711014 20030306 20030310 -BIB 5 11 -REACTION (36-KR-84(13-AL-27,2A+F)MASS,,DA/CRL,A/A/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (A) -EN-SEC ANG1 is azimuthal angle between two alphas - ANG2 is polar angle between beam and fission fragment +ENDSUBENT 35 +SUBENT E1711014 20050914 20050914 E032 +BIB 7 15 +REACTION (36-KR-84(13-AL-27,2A+F)MASS,,DA/DA,A+A/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (A) + (FF) +EN-SEC - ANG1 is azimuthal angle between two alphas + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect alpha, alpha and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (right), p1998 in - reference -ENDBIB 11 +STATUS (CURVE) Data scanned from Fig.2 (right), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 15 COMMON 1 3 ANG2 ADEG @@ -441,21 +512,25 @@ NO-DIM NO-DIM ADEG ARB-UNITS 20.0 40.0 1.570E+02 2.000E+01 20.0 40.0 1.804E+02 2.292E+01 ENDDATA 10 -ENDSUBENT 30 -SUBENT E1711015 20030306 20030310 -BIB 5 11 -REACTION (36-KR-84(13-AL-27,2A+F)MASS,,DA/CRL,A/A/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (A) -EN-SEC ANG1 is azimuthal angle between two alphas - ANG2 is polar angle between beam and fission fragment +ENDSUBENT 34 +SUBENT E1711015 20050914 20050914 E032 +BIB 7 15 +REACTION (36-KR-84(13-AL-27,2A+F)MASS,,DA/DA,A+A/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (A) + (FF) +EN-SEC - ANG1 is azimuthal angle between two alphas + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect alpha, alpha and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (right), p1998 in - reference -ENDBIB 11 +STATUS (CURVE) Data scanned from Fig.2 (right), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 15 COMMON 1 3 ANG2 ADEG @@ -473,21 +548,25 @@ NO-DIM NO-DIM ADEG ARB-UNITS 40.0 60.0 1.522E+02 1.233E+02 40.0 60.0 1.764E+02 1.733E+02 ENDDATA 10 -ENDSUBENT 30 -SUBENT E1711016 20030306 20030310 -BIB 5 11 -REACTION (36-KR-84(13-AL-27,2A+F)MASS,,DA/CRL,A/A/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (A) -EN-SEC ANG1 is azimuthal angle between two alphas - ANG2 is polar angle between beam and fission fragment +ENDSUBENT 34 +SUBENT E1711016 20050914 20050914 E032 +BIB 7 15 +REACTION (36-KR-84(13-AL-27,2A+F)MASS,,DA/DA,A+A/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (A) + (FF) +EN-SEC - ANG1 is azimuthal angle between two alphas + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect alpha, alpha and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (right), p1998 in - reference -ENDBIB 11 +STATUS (CURVE) Data scanned from Fig.2 (right), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 15 COMMON 1 3 ANG2 ADEG @@ -505,21 +584,25 @@ NO-DIM NO-DIM ADEG ARB-UNITS 60.0 80.0 1.487E+02 5.142E+02 60.0 80.0 1.708E+02 7.411E+02 ENDDATA 10 -ENDSUBENT 30 -SUBENT E1711017 20030306 20030310 -BIB 5 11 -REACTION (36-KR-84(13-AL-27,2A+F)MASS,,DA/CRL,A/A/FF,REL) - DATA: after phi=90deg symmetrization, no explanation - is given for the unit, but may be relative count -PART-DET fission fragment - (A) -EN-SEC ANG1 is azimuthal angle between two alphas - ANG2 is polar angle between beam and fission fragment +ENDSUBENT 34 +SUBENT E1711017 20050914 20050914 E032 +BIB 7 15 +REACTION (36-KR-84(13-AL-27,2A+F)MASS,,DA/DA,A+A/FF,REL) + after phi=90deg symmetrization, no explanation is + given for the unit, but may be relative count +PART-DET (A) + (FF) +EN-SEC - ANG1 is azimuthal angle between two alphas + - ANG2 is polar angle between beam and fission + fragment in laboratory system +METHOD (COINC) Detect alpha, alpha and fission fragment in + coincidence. COMMENT MASS-MIN: minimum mass number of coincident fragment MASS-MAX: maximum mass number of coincident fragment -STATUS (CURVE)Data scanned from Fig.2 (right), p1998 in - reference -ENDBIB 11 +STATUS (CURVE) Data scanned from Fig.2 (right), p1998 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-C/350) +ENDBIB 15 COMMON 1 3 ANG2 ADEG @@ -537,7 +620,7 @@ NO-DIM NO-DIM ADEG ARB-UNITS 80.0 100.0 1.474E+02 4.117E+02 80.0 100.0 1.698E+02 6.470E+02 ENDDATA 10 -ENDSUBENT 30 +ENDSUBENT 34 NOSUBENT E1711018 20030306 20030310 NOSUBENT E1711019 20030306 20030310 NOSUBENT E1711020 20030306 20030310 diff --git a/exforall/E17/E1721.x4 b/exforall/E17/E1721.x4 index be7060883..60b244895 100644 --- a/exforall/E17/E1721.x4 +++ b/exforall/E17/E1721.x4 @@ -1,6 +1,6 @@ -ENTRY E1721 20030627 20030925 -SUBENT E1721001 20030627 20030925 -BIB 10 44 +ENTRY E1721 20050914 20050914 E032 +SUBENT E1721001 20050914 20050914 E032 +BIB 11 43 TITLE Quadrupole deformation of 12Be studied by proton inelastic scattering AUTHOR (H.Iwasaki, T.Motobayashi, H.Akiyoshi, Y.Ando, @@ -8,60 +8,63 @@ AUTHOR (H.Iwasaki, T.Motobayashi, H.Akiyoshi, Y.Ando, M.Hirai, I.Hisanaga, N.Iwasa, T.Kijima, T.Minemura, T.Nakamura, M.Notani, S.Ozawa, H.Sakurai, S.Shimoura, S.Takeuchi, T.Teranishi, Y.Yanagisawa, M.Ishihara) -INSTITUTE (2JPNTOK)Department of Physics - (2JPNYOK)Department of Physics +INSTITUTE (2JPNTOK) Department of Physics + (2JPNYOK) Department of Physics (2JPNIPC) -REFERENCE (J,PL/B,481,7,200005) -INC-SPECT Beam Resolution: angular spreads were limited to - +-1.7deg -SAMPLE Target enrichment is unknown. - Chemical-form of target: CH2 and C are used - Physical-form of target is solid. - Target-thickness: 90.2mg/cm2 89.8mg/cm2 for (CH2)n and - C target, respectively. - Backing is unknown. -FACILITY (PRJFS,2JPNIPC)Secondary beams of 10Be and 12Be were - produced and separated by the RIKEN - Projectile Fragment Separator [T.Kubo - et al., Nucl.Instrum.Methods - B70(1992)309] using a 100MeV/u 18O - primary beam incident on a 1.11g/cm2 - 9Be target. -DETECTOR Detector resolution is 7.0%.(for 1275-keV gamma-ray - detection by NaI counter) - Efficiency: 83+-4(80+-4)% for the 10Be(12Be) - scattering at plastic scintillator hodoscope, - 4.6(7.1)% for 3.37(2.10)MeV gamma-ray emitted from - 10Be(12Be) in flight for NaI scintillators - (SCIN)Plastic Scintillator to detect outgoing - particles - (SCIN)NaI scintillators to detect de-excitation - gamma-rays -ADD-RES Subentry 008:1-H-1(4-BE-10,INL)1-H-1 - Deformation parameter - See NRDF D1721 DATA,7 for detail. - Subentry 009:1-H-1(4-BE-12,INL)1-H-1 - Deformation parameter - See NRDF D1721 DATA,8 for detail. -HISTORY (20020905T)Data converted from NRDF D1721 - (20030625A)REACTION are corrected -ENDBIB 44 -COMMON 1 3 -EN-RSL -PER-CENT - 1.0 +REFERENCE (J,PL/B,481,(1),7,200005) +INC-SPECT EN-RSL: angular spreads were limited to +-1.7deg +SAMPLE - Target enrichment is unknown. + - Chemical-form of target: CH2 and C are used + - Physical-form of target is solid. + - Target-thickness: 90.2mg/cm2 89.8mg/cm2 for (CH2)n + and C target, respectively. + - Backing is unknown. +METHOD (TOF) + (EDE) +FACILITY (PRJFS,2JPNIPC) Secondary beams of 10Be and 12Be were + produced and separated by the RIKEN + Projectile Fragment Separator [T.Kubo + et al., Nucl.Instrum.Methods + B70(1992)309] using a 100MeV/u 18O + primary beam incident on a 1.11g/cm2 + 9Be target. +DETECTOR - E-RSL: for 1275-keV gamma-ray detection by NaI + counter + - Efficiency: 83+-4(80+-4)% for the 10Be(12Be) + scattering at plastic scintillator hodoscope, + 4.6(7.1)% for 3.37(2.10)MeV gamma-ray emitted from + 10Be(12Be) in flight for NaI scintillators + (SCIN) To detect outgoing particles + (NAICR) To detect de-excitation gamma-rays +ADD-RES E1721.008:1-H-1(4-BE-10,INL)1-H-1 + Deformation parameter + See NRDF D1721 DATA,7 for detail. + E1721.009:1-H-1(4-BE-12,INL)1-H-1 + Deformation parameter + See NRDF D1721 DATA,8 for detail. +HISTORY (20020905T) Data converted from NRDF D1721 + (20030625A) REACTION are corrected +ENDBIB 43 +COMMON 2 3 +EN-RSL E-RSL +PER-CENT PER-CENT + 1.0 7.0 ENDCOMMON 3 -ENDSUBENT 51 -SUBENT E1721002 20030627 20030925 -BIB 4 7 -REACTION (1-H-1(4-BE-10,INL)1-H-1,,DA/DE,G,IPA/REL) - DATA: counts/20keV +ENDSUBENT 50 +SUBENT E1721002 20050914 20050914 E032 +BIB 7 11 +REACTION (1-H-1(4-BE-10,INL)1-H-1,,IPA/DE,G,REL) + counts/20keV PART-DET (G) (4-BE-10) -EN-SEC (E,G) - ANG is polar angle between beam and gamma -STATUS (CURVE)Data scanned from Fig.1(top), p9 in reference -ENDBIB 7 +EN-SEC ANG is polar angle between beam and prompt gamma in + laboratory system + (E,G) +METHOD (COINC) Detect prompt gamma and 10Be in coincidence. +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (CURVE) Data scanned from Fig.1(top), p9 in reference +HISTORY (20050812A) On. REACTION corrected (CP-D/430) +ENDBIB 11 COMMON 3 3 EN ANG-MIN ANG-MAX MEV/A ADEG ADEG @@ -160,19 +163,22 @@ MEV ARB-UNITS ARB-UNITS ARB-UNITS 3.867E+00 8.174E+00 1.692E+01 1.230E+01 3.892E+00 3.502E+00 1.538E+01 1.230E+01 ENDDATA 91 -ENDSUBENT 107 -SUBENT E1721003 20030627 20030925 -BIB 4 9 -REACTION (1-H-1(4-BE-12,INL)1-H-1,,DA/DE,G,IPA/REL) - DATA: raw data (contain the contribution of - efficiency) +ENDSUBENT 111 +SUBENT E1721003 20050914 20050914 E032 +BIB 7 12 +REACTION (1-H-1(4-BE-12,INL)1-H-1,,IPA/DE,G,REL) + raw data (contain the contribution of efficiency) PART-DET (G) (4-BE-12) -EN-SEC (E,G) - ANG is polar angle between beam and gamma -STATUS (CURVE)Data scanned from Fig.1(bottom), p9 in - reference -ENDBIB 9 +EN-SEC ANG is polar angle between beam and prompt gamma in + laboratory system + (E,G) +METHOD (COINC) Detect prompt gamma and 12Be in coincidence. +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (CURVE) Data scanned from Fig.1(bottom), p9 in + reference +HISTORY (20050812A) On. REACTION corrected (CP-D/430) +ENDBIB 12 COMMON 3 3 EN ANG-MIN ANG-MAX MEV/A ADEG ADEG @@ -270,7 +276,7 @@ MEV ARB-UNITS ARB-UNITS ARB-UNITS 3.000E+00 1.941E+01 1.528E+01 1.375E+01 3.023E+00 2.084E+01 1.834E+01 1.681E+01 ENDDATA 90 -ENDSUBENT 108 +ENDSUBENT 111 SUBENT E1721004 20030627 20030925 BIB 4 4 REACTION (1-H-1(4-BE-10,INL)1-H-1,PAR,SIG) diff --git a/exforall/E17/E1744.x4 b/exforall/E17/E1744.x4 index 840b9ee22..cccc85ddc 100644 --- a/exforall/E17/E1744.x4 +++ b/exforall/E17/E1744.x4 @@ -1,84 +1,90 @@ -ENTRY E1744 20030306 20030310 -SUBENT E1744001 20030306 20030310 -BIB 9 28 +ENTRY E1744 20050914 20050914 E032 +SUBENT E1744001 20050914 20050914 E032 +BIB 11 33 TITLE Low-lying intruder 1- state in 12Be and the melting of the N=8 shell closure AUTHOR (H.Iwasaki, T.Motobayashi, H.Akiyoshi, Y.Ando, - N.Fukuda, H.Fujiwara, Zs.Fulop, K.I.Hahn, - Y.Higurashi, M.Hirai, I.Hisanaga, N.Iwasa, T.Kijima, - A.Mengoni, T.Minemura, T.Nakamura, M.Notani, S.Ozawa, - H.Sagawa, H.Sakurai, S.Shimoura, S.Takeuchi, - T.Teranishi, Y.Yanagisawa, M.Ishihara) -INSTITUTE (2JPNTOK)Department of Physics - (2JPNYOK)Department of Physics + N.Fukuda, H.Fujiwara, Zs.Fulop, K.I.Hahn, Y.Higurashi, + M.Hirai, I.Hisanaga, N.Iwasa, T.Kijima, A.Mengoni, + T.Minemura, T.Nakamura, M.Notani, S.Ozawa, H.Sagawa, + H.Sakurai, S.Shimoura, S.Takeuchi, T.Teranishi, + Y.Yanagisawa, M.Ishihara) +INSTITUTE (2JPNTOK) Department of Physics + (2JPNYOK) Department of Physics (2JPNIPC) - (2ITYBOL)Applied Physics Division - (2JPNJPN)Center for Mathematical Science, the - University of Aizu -REFERENCE (J,PL/B,491,8,200010) -PART-DET (4-BE-12) -SAMPLE Target is natural. - Chemical-form of target is element. - Physical-form of target is solid. -FACILITY (PRJFS,2JPNIPC)Radioactive 12Be beam was produced by - the fragment separator RIPS [T.Kubo et - al., Nucl. Instrum. Methods Phys. Res. - B70(1992)309] via fragmentation - reactions of a 100 MeV/u 18O primary - beam on a 1.11g/cm2 9Be target. + (2ITYBOL) Applied Physics Division + (2JPNJPN) Center for Mathematical Science, the + University of Aizu +REFERENCE (J,PL/B,491,(1-2),8,200010) +PART-DET (G) + (4-BE-12) +SAMPLE - Target is natural. + - Chemical-form of target is element. + - Physical-form of target is solid. +METHOD (COINC) Detect prompt gamma and 12Be in coincidence. +FACILITY (PRJFS,2JPNIPC) Radioactive 12Be beam was produced by + the fragment separator RIPS [T.Kubo et + al., Nucl. Instrum. Methods Phys. Res. + B70(1992)309] via fragmentation + reactions of a 100 MeV/u 18O primary + beam on a 1.11g/cm2 9Be target. DETECTOR Detector resolution: for NaI, 7.0%(FWHM) for the 1275-KeV Gamma ray + (SCIN) + (NAICR) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties HISTORY (20020218C) -ENDBIB 28 +ENDBIB 33 NOCOMMON 0 0 -ENDSUBENT 31 -SUBENT E1744002 20030306 20030310 -BIB 5 7 -REACTION (82-PB-208(4-BE-12,INL)82-PB-208,PAR,DA,,IPA) -PART-DET (G) - (4-BE-12) -SAMPLE Target-thickness is 350.8mg/cm**2. -EN-SEC ANG-CM is polar angle between beam and 12Be - (E-LVL,82-PB-208) -STATUS (TABLE)Data taken from Table 1, p11 in reference -ENDBIB 7 +ENDSUBENT 36 +SUBENT E1744002 20050914 20050914 E032 +BIB 6 10 +REACTION (82-PB-208(4-BE-12,INL)82-PB-208,PAR,IPA) +EN-SEC ANG-CM is polar angle between beam and 12Be in center + of mass system + (E-LVL,4-BE-12) +LEVEL-PROP ((1.)4-BE-12,E-LVL=2.11,SPIN=2.0,PARITY=+1.0) + ((2.)4-BE-12,E-LVL=2.68,SPIN=1.0,PARITY=-1.0) +SAMPLE Target-thickness is 350.8 mg/cm**2. +STATUS (TABLE) Data taken from Table 1, p11 in reference +HISTORY (20050812A) On. REACTION corrected (CP-D/430), + LEVEL-PROP added +ENDBIB 10 COMMON 2 3 EN ANG-CM-MAX MEV/A ADEG 53.3 7.3 ENDCOMMON 3 -DATA 6 2 -E-LVL E-LVL-ERR SPIN J PARITY DATA DATA-ERR -MEV MEV NO-DIM NO-DIM MB MB - 2.68 0.03 1.0 -1.0 46.5 11.5 - 2.11 0.02 2.0 1.0 81.8 12.8 +DATA 5 2 +E-LVL E-LVL-ERR DATA DATA-ERR LVL-FLAG +MEV MEV MB MB NO-DIM + 2.11 0.02 81.8 12.8 1.0 + 2.68 0.03 46.5 11.5 2.0 ENDDATA 4 -ENDSUBENT 20 -SUBENT E1744003 20030306 20030310 -BIB 5 8 -REACTION (6-C-12(4-BE-12,INL)6-C-12,PAR,DA,,IPA) - DATA-MAX: Upper limit of integrated cross section -PART-DET (G) - (4-BE-12) -SAMPLE Target-thickness is 89.8mg/cm**2. -EN-SEC ANG-CM is polar angle between beam and 12Be - (E-LVL,6-C-12) -STATUS (TABLE)Data taken from Table 1, p11 in reference -ENDBIB 8 +ENDSUBENT 23 +SUBENT E1744003 20050914 20050914 E032 +BIB 6 10 +REACTION (6-C-12(4-BE-12,INL)6-C-12,PAR,IPA) +EN-SEC ANG-CM is polar angle between beam and 12Be in center + of mass system + (E-LVL,4-BE-12) +LEVEL-PROP ((1.)4-BE-12,E-LVL=2.11,SPIN=2.0,PARITY=+1.0) + ((2.)4-BE-12,E-LVL=2.68,SPIN=1.0,PARITY=-1.0) +SAMPLE Target-thickness is 89.8 mg/cm**2. +STATUS (TABLE) Data taken from Table 1, p11 in reference +HISTORY (20050812A) On. REACTION corrected (CP-D/430), + LEVEL-PROP added +ENDBIB 10 COMMON 2 3 EN ANG-CM-MAX MEV ADEG 54.0 13.9 ENDCOMMON 3 -DATA 7 2 -E-LVL E-LVL-ERR SPIN J PARITY DATA DATA-MAX -DATA-ERR -MEV MEV NO-DIM NO-DIM MB MB -MB - 2.68 0.03 1.0 -1.0 4.9 - - 2.11 0.02 2.0 1.0 54.9 - 7.1 -ENDDATA 8 -ENDSUBENT 25 +DATA 6 2 +E-LVL E-LVL-ERR DATA DATA-ERR DATA-MAX LVL-FLAG +MEV MEV MB MB MB NO-DIM + 2.11 0.02 54.9 7.1 1.0 + 2.68 0.03 4.9 2.0 +ENDDATA 4 +ENDSUBENT 23 ENDENTRY 3 diff --git a/exforall/E17/E1750.x4 b/exforall/E17/E1750.x4 index 0828f3929..73b11d4f9 100644 --- a/exforall/E17/E1750.x4 +++ b/exforall/E17/E1750.x4 @@ -1,35 +1,40 @@ -ENTRY E1750 20030606 20030610 -SUBENT E1750001 20030606 20030610 -BIB 8 26 +ENTRY E1750 20050914 20050914 E032 +SUBENT E1750001 20050914 20050914 E032 +BIB 10 31 TITLE Measurements of double differential neutron production cross sections by 135 MeV/nucleon He, C, Ne and 95 MeV/nucleon Ar ions AUTHOR (H.Sato, T.Kurosawa, H.Iwase, T.Nakamura, Y.Uwamino, N.Nakao) -INSTITUTE (2JPNTOH)Cyclotron and Radioisotope Center +INSTITUTE (2JPNTOH) Cyclotron and Radioisotope Center (2JPNETL) (2JPNIPC) (2JPNKEK) -REFERENCE (J,PR/C,64,034607,200109) -SAMPLE Target is natural.The enrichments of targets are not - given in the reference. But compiler asked T.Kurosawa. - Backing is unknown. +REFERENCE (J,PR/C,64,(3),034607,200109) +PART-DET (N) +SAMPLE - Target is natural. The enrichments of targets are + not given in the reference. But compiler asked + T.Kurosawa. + - Backing is unknown. +METHOD (TOF) + (EDE) FACILITY (CYCLO,2JPNIPC) -DETECTOR Detector resolution: The energy resolutions of the - measured neutron spectra are about 3% for neutrons - having energies near 100 MeV. - Calibration: Each E counter was calibrated with a 60Co - Gamma-ray source. - Efficiency: The neutron detection efficiencies were - calculated with the Monte Carlo code of Cecil et al. - for all energy ranges. References is R. A. Cecil, B. - D. Anderson, and R. Madey, Nucl. Instrum. Methods 161, - 439 (1979). - (SCIN) +DETECTOR - Detector resolution: The energy resolutions of the + measured neutron spectra are about 3% for neutrons + having energies near 100 MeV. + - Efficiency: The neutron detection efficiencies were + calculated with the Monte Carlo code of Cecil et al. + for all energy ranges. References is R. A. Cecil, B. + D. Anderson, and R. Madey, Nucl. Instrum. Methods + 161, 439 (1979). + (MAGSP) + (SCIN) Used as Delta-E counter + (SCIN) Used as E counter, calibrated with a 60Co + gamma-ray source HISTORY (20020201C) -ENDBIB 26 +ENDBIB 31 NOCOMMON 0 0 -ENDSUBENT 29 +ENDSUBENT 34 SUBENT E1750002 20030606 20030610 BIB 9 21 REACTION (6-C-0(A,X)0-NN-1,,DA/DE) @@ -6339,30 +6344,33 @@ ADEG MB/SR 80.0 6.331E+02 ENDDATA 5 ENDSUBENT 30 -SUBENT E1750037 20030606 20030610 -BIB 7 17 -REACTION (6-C-0(A,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 216mg/cm**2. +SUBENT E1750037 20050914 20050914 E032 +BIB 7 20 +REACTION (6-C-12(A,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 216 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION and Mass number of - target are modified. -ENDBIB 17 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION and Mass number of + target are modified. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 20 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6370,30 +6378,33 @@ ADEG ADEG MB 0.0 90.0 1.801E+02 0.0 180.0 1.965E+02 ENDDATA 4 -ENDSUBENT 30 -SUBENT E1750038 20030606 20030610 -BIB 7 16 -REACTION (13-AL-27(A,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 162mg/cm**2. +ENDSUBENT 33 +SUBENT E1750038 20050914 20050914 E032 +BIB 7 19 +REACTION (13-AL-27(A,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 162 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6401,30 +6412,33 @@ ADEG ADEG MB 0.0 90.0 4.039E+02 0.0 180.0 4.489E+02 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750039 20030606 20030610 -BIB 7 16 -REACTION (29-CU-0(A,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 267.6mg/cm**2. +ENDSUBENT 32 +SUBENT E1750039 20050914 20050914 E032 +BIB 7 19 +REACTION (29-CU-0(A,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 267.6 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6432,30 +6446,33 @@ ADEG ADEG MB 0.0 90.0 7.937E+02 0.0 180.0 9.752E+02 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750040 20030606 20030610 -BIB 7 16 -REACTION (82-PB-0(A,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 340.2mg/cm**2. +ENDSUBENT 32 +SUBENT E1750040 20050914 20050914 E032 +BIB 7 19 +REACTION (82-PB-0(A,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 340.2 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6463,30 +6480,33 @@ ADEG ADEG MB 0.0 90.0 1.950E+03 0.0 180.0 2.654E+03 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750041 20030606 20030610 -BIB 7 16 -REACTION (6-C-0(6-C-12,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 216mg/cm**2. +ENDSUBENT 32 +SUBENT E1750041 20050914 20050914 E032 +BIB 7 19 +REACTION (6-C-12(6-C-12,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 216 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6494,30 +6514,33 @@ ADEG ADEG MB 0.0 90.0 4.238E+02 0.0 180.0 4.489E+02 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750042 20030606 20030610 -BIB 7 16 -REACTION (13-AL-27(6-C-12,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 162mg/cm**2. +ENDSUBENT 32 +SUBENT E1750042 20050914 20050914 E032 +BIB 7 19 +REACTION (13-AL-27(6-C-12,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 162 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6525,30 +6548,33 @@ ADEG ADEG MB 0.0 90.0 9.499E+02 0.0 180.0 1.051E+03 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750043 20030606 20030610 -BIB 7 16 -REACTION (29-CU-0(6-C-12,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 267.6mg/cm**2. +ENDSUBENT 32 +SUBENT E1750043 20050914 20050914 E032 +BIB 7 19 +REACTION (29-CU-0(6-C-12,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 267.6 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6556,30 +6582,33 @@ ADEG ADEG MB 0.0 90.0 1.866E+03 0.0 180.0 2.066E+03 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750044 20030606 20030610 -BIB 7 16 -REACTION (82-PB-0(6-C-12,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 340.2mg/cm**2. +ENDSUBENT 32 +SUBENT E1750044 20050914 20050914 E032 +BIB 7 19 +REACTION (82-PB-0(6-C-12,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 340.2 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6587,30 +6616,33 @@ ADEG ADEG MB 0.0 90.0 4.587E+03 0.0 180.0 5.623E+03 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750045 20030606 20030610 -BIB 7 16 -REACTION (6-C-0(10-NE-20,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 216mg/cm**2. +ENDSUBENT 32 +SUBENT E1750045 20050914 20050914 E032 +BIB 7 19 +REACTION (6-C-12(10-NE-20,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 216 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6618,30 +6650,33 @@ ADEG ADEG MB 0.0 90.0 7.173E+02 0.0 180.0 7.785E+02 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750046 20030606 20030610 -BIB 7 16 -REACTION (13-AL-27(10-NE-20,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 216mg/cm**2. +ENDSUBENT 32 +SUBENT E1750046 20050914 20050914 E032 +BIB 7 19 +REACTION (13-AL-27(10-NE-20,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 216 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6649,30 +6684,33 @@ ADEG ADEG MB 0.0 90.0 1.457E+03 0.0 180.0 1.691E+03 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750047 20030606 20030610 -BIB 7 16 -REACTION (29-CU-0(10-NE-20,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 267.6mg/cm**2. +ENDSUBENT 32 +SUBENT E1750047 20050914 20050914 E032 +BIB 7 19 +REACTION (29-CU-0(10-NE-20,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 267.6 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6680,30 +6718,33 @@ ADEG ADEG MB 0.0 90.0 2.958E+03 0.0 180.0 3.495E+03 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750048 20030606 20030610 -BIB 7 16 -REACTION (82-PB-0(10-NE-20,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 340.2mg/cm**2. +ENDSUBENT 32 +SUBENT E1750048 20050914 20050914 E032 +BIB 7 19 +REACTION (82-PB-0(10-NE-20,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 340.2 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6711,30 +6752,33 @@ ADEG ADEG MB 0.0 90.0 7.764E+03 0.0 180.0 9.276E+03 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750049 20030606 20030610 -BIB 7 16 -REACTION (6-C-0(18-AR-40,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 216mg/cm**2. +ENDSUBENT 32 +SUBENT E1750049 20050914 20050914 E032 +BIB 7 19 +REACTION (6-C-12(18-AR-40,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 216 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6742,30 +6786,33 @@ ADEG ADEG MB 0.0 90.0 3.366E+03 0.0 180.0 3.495E+03 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750050 20030606 20030610 -BIB 7 16 -REACTION (13-AL-27(18-AR-40,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 162mg/cm**2. +ENDSUBENT 32 +SUBENT E1750050 20050914 20050914 E032 +BIB 7 19 +REACTION (13-AL-27(18-AR-40,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 162 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6773,30 +6820,33 @@ ADEG ADEG MB 0.0 90.0 5.612E+03 0.0 180.0 6.061E+03 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750051 20030606 20030610 -BIB 7 16 -REACTION (29-CU-0(18-AR-40,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 267.6mg/cm**2. +ENDSUBENT 32 +SUBENT E1750051 20050914 20050914 E032 +BIB 7 19 +REACTION (29-CU-0(18-AR-40,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 267.6 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6804,30 +6854,33 @@ ADEG ADEG MB 0.0 90.0 9.667E+03 0.0 180.0 1.077E+04 ENDDATA 4 -ENDSUBENT 29 -SUBENT E1750052 20030606 20030610 -BIB 7 16 -REACTION (82-PB-0(18-AR-40,X)0-NN-1,,DA,,IPA) - DATA: The neutron production cross section integrated - over energies above 20 MeV, and also over - partial angular range. -MONITOR The total normalization uncertainty is within 17%. -PART-DET (N) -SAMPLE Chemical-form of target is element. - Physical-form of target is solid. - Target-thickness is 340.2mg/cm**2. +ENDSUBENT 32 +SUBENT E1750052 20050914 20050914 E032 +BIB 7 19 +REACTION (82-PB-0(18-AR-40,X)0-NN-1,PAR,IPA) + The neutron production cross section integrated over + energies above 20 MeV, and also over partial angular + range. +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 340.2 mg/cm**2. ERR-ANALYS The statistical uncertainties vary from 2 to 5% for the low- to medium-energy (about 10-100 MeV) region of the spectra and increase to about 30% at the highest energies. -STATUS (CURVE)Data scanned from Fig.13-14, p034607-10-11 in - reference -HISTORY (20030530A)Free text on REACTION is corrected. -ENDBIB 16 -COMMON 1 3 -EN -MEV/A - 135.0 +COMMENT The total normalization uncertainty is within 17%. +STATUS (CURVE) Data scanned from Fig.13-14, p034607-10-11 in + reference +HISTORY (20030530A) Free text on REACTION is corrected. + (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 19 +COMMON 2 3 +EN E-MIN +MEV/A MEV + 135.0 10.0 ENDCOMMON 3 DATA 3 2 ANG-MIN ANG-MAX DATA @@ -6835,5 +6888,5 @@ ADEG ADEG MB 0.0 90.0 2.224E+04 0.0 180.0 2.524E+04 ENDDATA 4 -ENDSUBENT 29 +ENDSUBENT 32 ENDENTRY 52 diff --git a/exforall/E17/E1769.x4 b/exforall/E17/E1769.x4 index 79788c37e..f3a6bbca8 100644 --- a/exforall/E17/E1769.x4 +++ b/exforall/E17/E1769.x4 @@ -1,37 +1,40 @@ -ENTRY E1769 20030606 20030610 -SUBENT E1769001 20030606 20030610 -BIB 9 28 +ENTRY E1769 20050914 20050914 E032 +SUBENT E1769001 20050914 20050914 E032 +BIB 11 31 TITLE Double-differential cross sections for the neutron production from heavy-ion reactions at energies E/A = 290-600 MeV AUTHOR (Y.Iwata, T.Murakami, H.Sato, H.Iwase, T.Nakamura, T.Kurosawa, L.Heilbronn, R.M.Ronningen, K.Ieki, Y.Tozawa, K.Niita) -INSTITUTE (2JPNIRS)Department of Accelerator Physics and - Engineering - (2JPNTOH)Cyclotron and Radioisotope Center +INSTITUTE (2JPNIRS) Department of Accelerator Physics and + Engineering + (2JPNTOH) Cyclotron and Radioisotope Center (1USABRK) - (1USAMSU)National Superconducting Cyclotron Laboratory - (2JPNYOK)Department of Physics - (2JPNJPN)Research Organization for Information Science - and Technology, Tokai, Naka, Ibaraki -REFERENCE (J,PR/C,64,054609,200111) + (1USAMSU) National Superconducting Cyclotron + Laboratory + (2JPNYOK) Department of Physics + (2JPNJPN) Research Organization for Information + Science and Technology, Tokai, Naka, Ibaraki +REFERENCE (J,PR/C,64,(5),054609,200111) +PART-DET (N) INC-SOURCE Beam intensity: A few times 10**4 - 10**5 particles per pulse -SAMPLE Target is natural. - Chemical-form of target is element. - Physical-form of target is solid. - Backing is unknown. -FACILITY (SYNCH,2JPNIRS)Heavy Ion Medical Accelerator in Chiba - (HIMAC) facility +SAMPLE - Target is natural. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Backing is unknown. +METHOD (TOF) +FACILITY (SYNCH,2JPNIRS) Heavy Ion Medical Accelerator in Chiba + (HIMAC) facility DETECTOR Detector resolution: The energy resolutions are shown in Table I in reference. - (SCIN)NE102A plastic scintillator and NE213 liquid - scintillator + (SCIN) NE102A plastic scintillator + (SCIN) NE213 liquid scintillator HISTORY (20020801C) -ENDBIB 28 +ENDBIB 31 NOCOMMON 0 0 -ENDSUBENT 31 +ENDSUBENT 34 SUBENT E1769002 20030606 20030610 BIB 6 8 REACTION (6-C-0(6-C-12,X)0-NN-1,,DA/DE) @@ -6710,16 +6713,18 @@ ADEG B/SR B/SR B/SR 80.0 5.42 0.7 0.72 ENDDATA 9 ENDSUBENT 25 -SUBENT E1769146 20030606 20030610 -BIB 5 7 -REACTION (6-C-0(6-C-12,X)0-NN-1,,DA,,IPA) -PART-DET (N) +SUBENT E1769146 20050914 20050914 E032 +BIB 6 9 +REACTION (6-C-12(6-C-12,X)0-NN-1,,IPA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system SAMPLE Target-thickness: 1.80 and 9.00 g/cm**2 for E/A = 290.0 and 400.0 MeV, respectively -EN-SEC ANG is polar angle between beam and neutron -STATUS (TABLE)Data taken from Table.IV, p054609-7 in - reference. -ENDBIB 7 +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table.IV, p054609-7 in + reference. +HISTORY (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 9 COMMON 2 3 ANG-MIN ANG-MAX ADEG ADEG @@ -6731,17 +6736,19 @@ MEV/A B B B 290.0 1.86 0.29 0.42 400.0 1.43 0.36 0.37 ENDDATA 4 -ENDSUBENT 20 -SUBENT E1769147 20030606 20030610 -BIB 5 7 -REACTION (29-CU-0(6-C-12,X)0-NN-1,,DA,,IPA) -PART-DET (N) +ENDSUBENT 22 +SUBENT E1769147 20050914 20050914 E032 +BIB 6 9 +REACTION (29-CU-0(6-C-12,X)0-NN-1,,IPA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system SAMPLE Target-thickness: 4.47 and 13.4 g/cm**2 for E/A = 290.0 and 400.0 MeV, respectively -EN-SEC ANG is polar angle between beam and neutron -STATUS (TABLE)Data taken from Table.IV, p054609-7 in - reference. -ENDBIB 7 +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table.IV, p054609-7 in + reference. +HISTORY (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 9 COMMON 2 3 ANG-MIN ANG-MAX ADEG ADEG @@ -6751,19 +6758,21 @@ DATA 4 2 EN DATA +DATA-ERR -DATA-ERR MEV/A B B B 290.0 6.08 0.86 1.13 - 400.0 6.08 1.2 1.25 + 400.0 6.08 1.20 1.25 ENDDATA 4 -ENDSUBENT 20 -SUBENT E1769148 20030606 20030610 -BIB 5 7 -REACTION (82-PB-0(6-C-12,X)0-NN-1,,DA,,IPA) -PART-DET (N) +ENDSUBENT 22 +SUBENT E1769148 20050914 20050914 E032 +BIB 6 9 +REACTION (82-PB-0(6-C-12,X)0-NN-1,,IPA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system SAMPLE Target-thickness: 2.27 and 9.08 g/cm**2 for E/A = 290.0 and 400.0 MeV, respectively -EN-SEC ANG is polar angle between beam and neutron -STATUS (TABLE)Data taken from Table.IV, p054609-7 in - reference. -ENDBIB 7 +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table.IV, p054609-7 in + reference. +HISTORY (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 9 COMMON 2 3 ANG-MIN ANG-MAX ADEG ADEG @@ -6775,17 +6784,19 @@ MEV/A B B B 290.0 22.1 3.3 6.7 400.0 17.0 2.7 3.0 ENDDATA 4 -ENDSUBENT 20 -SUBENT E1769149 20030606 20030610 -BIB 5 7 -REACTION (6-C-0(10-NE-20,X)0-NN-1,,DA,,IPA) -PART-DET (N) +ENDSUBENT 22 +SUBENT E1769149 20050914 20050914 E032 +BIB 6 9 +REACTION (6-C-12(10-NE-20,X)0-NN-1,,IPA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system SAMPLE Target-thickness: 1.80 and 3.60 g/cm**2 for E/A = 400.0 and 600.0 MeV, respectively -EN-SEC ANG is polar angle between beam and neutron -STATUS (TABLE)Data taken from Table.IV, p054609-7 in - reference. -ENDBIB 7 +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table.IV, p054609-7 in + reference. +HISTORY (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 9 COMMON 2 3 ANG-MIN ANG-MAX ADEG ADEG @@ -6795,18 +6806,20 @@ DATA 4 2 EN DATA +DATA-ERR -DATA-ERR MEV/A B B B 400.0 4.37 0.68 0.98 - 600.0 3.74 0.62 0.7 + 600.0 3.74 0.62 0.70 ENDDATA 4 -ENDSUBENT 20 -SUBENT E1769150 20030606 20030610 -BIB 5 6 -REACTION (29-CU-0(10-NE-20,X)0-NN-1,,DA,,IPA) -PART-DET (N) -SAMPLE Target-thickness is 4470mg/cm**2. -EN-SEC ANG is polar angle between beam and neutron -STATUS (TABLE)Data taken from Table.IV, p054609-7 in - reference. -ENDBIB 6 +ENDSUBENT 22 +SUBENT E1769150 20050914 20050914 E032 +BIB 6 8 +REACTION (29-CU-0(10-NE-20,X)0-NN-1,,IPA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system +SAMPLE Target-thickness is 4470 mg/cm**2. +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table.IV, p054609-7 in + reference. +HISTORY (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 8 COMMON 2 3 ANG-MIN ANG-MAX ADEG ADEG @@ -6818,17 +6831,19 @@ MEV/A B B B 400.0 15.8 2.3 2.8 600.0 18.7 2.6 3.2 ENDDATA 4 -ENDSUBENT 19 -SUBENT E1769151 20030606 20030610 -BIB 5 7 -REACTION (82-PB-0(10-NE-20,X)0-NN-1,,DA,,IPA) -PART-DET (N) +ENDSUBENT 21 +SUBENT E1769151 20050914 20050914 E032 +BIB 6 9 +REACTION (82-PB-0(10-NE-20,X)0-NN-1,,IPA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system SAMPLE Target-thickness: 2.27 and 4.54 g/cm**2 for E/A = 400.0 and 600.0 MeV, respectively -EN-SEC ANG is polar angle between beam and neutron -STATUS (TABLE)Data taken from Table.IV, p054609-7 in - reference. -ENDBIB 7 +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table.IV, p054609-7 in + reference. +HISTORY (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 9 COMMON 2 3 ANG-MIN ANG-MAX ADEG ADEG @@ -6840,17 +6855,19 @@ MEV/A B B B 400.0 52.8 7.4 14.2 600.0 57.2 8.0 10.9 ENDDATA 4 -ENDSUBENT 20 -SUBENT E1769152 20030606 20030610 -BIB 5 7 -REACTION (6-C-0(18-AR-40,X)0-NN-1,,DA,,IPA) -PART-DET (N) +ENDSUBENT 22 +SUBENT E1769152 20050914 20050914 E032 +BIB 6 9 +REACTION (6-C-12(18-AR-40,X)0-NN-1,,IPA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system SAMPLE Target-thickness: 0.720 and 1.08 g/cm**2 for E/A = 400.0 and 560.0 MeV, respectively -EN-SEC ANG is polar angle between beam and neutron -STATUS (TABLE)Data taken from Table.IV, p054609-7 in - reference. -ENDBIB 7 +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table.IV, p054609-7 in + reference. +HISTORY (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 9 COMMON 2 3 ANG-MIN ANG-MAX ADEG ADEG @@ -6862,17 +6879,19 @@ MEV/A B B B 400.0 10.7 1.7 4.1 560.0 9.6 1.57 3.19 ENDDATA 4 -ENDSUBENT 20 -SUBENT E1769153 20030606 20030610 -BIB 5 7 -REACTION (29-CU-0(18-AR-40,X)0-NN-1,,DA,,IPA) -PART-DET (N) +ENDSUBENT 22 +SUBENT E1769153 20050914 20050914 E032 +BIB 6 9 +REACTION (29-CU-0(18-AR-40,X)0-NN-1,,IPA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system SAMPLE Target-thickness: 1.34 and 1.79 g/cm**2 for E/A = 400.0 and 560.0 MeV, respectively -EN-SEC ANG is polar angle between beam and neutron -STATUS (TABLE)Data taken from Table.IV, p054609-7 in - reference. -ENDBIB 7 +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table.IV, p054609-7 in + reference. +HISTORY (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 9 COMMON 2 3 ANG-MIN ANG-MAX ADEG ADEG @@ -6884,17 +6903,19 @@ MEV/A B B B 400.0 37.0 5.1 11.9 560.0 49.0 6.4 12.4 ENDDATA 4 -ENDSUBENT 20 -SUBENT E1769154 20030606 20030610 -BIB 5 7 -REACTION (82-PB-0(18-AR-40,X)0-NN-1,,DA,,IPA) -PART-DET (N) +ENDSUBENT 22 +SUBENT E1769154 20050914 20050914 E032 +BIB 6 9 +REACTION (82-PB-0(18-AR-40,X)0-NN-1,,IPA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system SAMPLE Target-thickness: 1.70 and 2.27 g/cm**2 for E/A = 400.0 and 560.0 MeV, respectively -EN-SEC ANG is polar angle between beam and neutron -STATUS (TABLE)Data taken from Table.IV, p054609-7 in - reference. -ENDBIB 7 +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table.IV, p054609-7 in + reference. +HISTORY (20050813A) On. REACTION corrected (CP-D/430) +ENDBIB 9 COMMON 2 3 ANG-MIN ANG-MAX ADEG ADEG @@ -6906,7 +6927,7 @@ MEV/A B B B 400.0 96.9 13.7 31.6 560.0 102.0 14.0 27.0 ENDDATA 4 -ENDSUBENT 20 +ENDSUBENT 22 SUBENT E1769155 20030606 20030610 BIB 4 6 REACTION (6-C-0(6-C-12,X)0-NN-1,,SIG) diff --git a/exforall/E18/E1803.x4 b/exforall/E18/E1803.x4 index e9df12083..d5498f900 100644 --- a/exforall/E18/E1803.x4 +++ b/exforall/E18/E1803.x4 @@ -1,5 +1,5 @@ -ENTRY E1803 20050224 -SUBENT E1803001 20050224 +ENTRY E1803 20050914 20050914 E032 +SUBENT E1803001 20050914 20050914 E032 BIB 13 55 TITLE Study of resonance states in 12N using a radioactive ion beam of 11C @@ -16,7 +16,7 @@ INSTITUTE (2JPNTOK) Center for Nuclear Study (CNS) (3HUNDEB) (2JPNYMG) Department of Physics REFERENCE (J,PL/B,556,(1-2),27,200303) -REL-REF (N,,A.H.Hernandez+,J,NP/A,143,(4),569,199810) +REL-REF (N,,A.H.Hernandez+,J,NIM/B,143,(4),569,199810) Thick target method (N,,S.Kubono,J,NP/A,693,(1-2),221,200110) Thick target method @@ -188,11 +188,11 @@ MEV MB/SR MB/SR 3.0375 118.1 8.2 ENDDATA 107 ENDSUBENT 127 -SUBENT E1803003 20050224 -BIB 5 14 -REACTION 1(1-H-1(6-C-11,TOT),,J) +SUBENT E1803003 20050914 20050914 E032 +BIB 6 15 +REACTION 1(1-H-1(6-C-11,0),,J) Tentative value for 3.6 MeV level - 2(1-H-1(6-C-11,TOT),,PTY) + 2(1-H-1(6-C-11,0),,PTY) MISC-COL (MISC1) Excitation energy (11N) = center of mass energy (11C+p) + 0.601 MeV (MISC2) Resonance width in [F. Ajzenberg-Selove, Nucl. @@ -204,13 +204,14 @@ COMMENT EN-RES-CM: Resonance energy in [F. Ajzenberg-Selove, Nucl. Phys. A506(1996)1] used in the derivation of J-pi STATUS (TABLE) Data taken from Table 2, p31 in reference -ENDBIB 14 +HISTORY (20050813A) On. REACTION (sf3) corrected +ENDBIB 15 NOCOMMON 0 0 DATA 5 2 EN-RES-CM MISC1 MISC2 DATA 1DATA 2 MEV MEV MEV NO-DIM NO-DIM - 2.53 3.1 0.22 3. -1. - 2.96 3.6 0.22 2. +1. + 2.53 3.1 0.22 3.0 -1.0 + 2.96 3.6 0.22 2.0 +1.0 ENDDATA 4 -ENDSUBENT 23 +ENDSUBENT 24 ENDENTRY 3 diff --git a/exforall/E18/E1860.x4 b/exforall/E18/E1860.x4 index f632b15a3..bf5d52dfb 100644 --- a/exforall/E18/E1860.x4 +++ b/exforall/E18/E1860.x4 @@ -1,5 +1,5 @@ -ENTRY E1860 20050224 -SUBENT E1860001 20050224 +ENTRY E1860 20050914 20050914 E032 +SUBENT E1860001 20050914 20050914 E032 BIB 11 21 TITLE The Al27(p,p)Al27 reaction AUTHOR (T.Awaya) @@ -26,7 +26,7 @@ ENDBIB 21 COMMON 1 3 ERR-1 PER-CENT - 1. + 1.0 ENDCOMMON 3 ENDSUBENT 28 SUBENT E1860002 20050224 @@ -319,14 +319,14 @@ KEV NO-DIM 1.217E+03 9.855E-01 ENDDATA 53 ENDSUBENT 68 -SUBENT E1860007 20050224 -BIB 7 13 +SUBENT E1860007 20050914 20050914 E032 +BIB 8 14 REL-REF (R,,S.L.Andersen+,J,NP,9,(3),509,195801) Resonance energies are taken from this literature. (R,,A.M.Lane+,J,RMP,30,(2),257,195804) Descriptsion for the R-matrix formalism -REACTION 1(13-AL-27(P,EL),,J) - 2(13-AL-27(P,EL),,PTY) +REACTION 1(13-AL-27(P,0),,J) + 2(13-AL-27(P,0),,PTY) 3(13-AL-27(P,EL),,WID) PART-DET (P) ANALYSIS (RFN) @@ -334,14 +334,15 @@ COMMENT EN-RES: These energies taken from [S.L. Andersen et al., Nucl. Phys. 9(1958/59)509] FLAG (1.) Jpi of 1117.2keV value is 3- or 4-. STATUS (TABLE) Data taken from Table 2, p677 in reference -ENDBIB 13 +HISTORY (20050813A) On. REACTION (sf3) corrected +ENDBIB 14 NOCOMMON 0 0 DATA 5 3 EN-RES DATA 1DATA 2DATA 3FLAG KEV NO-DIM NO-DIM KEV NO-DIM - 1117.2 0.80 1. - 1182.0 2. +1. 0.28 - 1198.0 3. -1. 6.3 + 1117.2 0.80 1.0 + 1182.0 2.0 +1.0 0.28 + 1198.0 3.0 -1.0 6.3 ENDDATA 5 -ENDSUBENT 23 +ENDSUBENT 24 ENDENTRY 7 diff --git a/exforall/E18/E1876.x4 b/exforall/E18/E1876.x4 new file mode 100644 index 000000000..2a977a7db --- /dev/null +++ b/exforall/E18/E1876.x4 @@ -0,0 +1,199 @@ +ENTRY E1876 20050914 20050914 E032 +SUBENT E1876001 20050914 20050914 E032 +BIB 11 21 +TITLE Excitation functions for the reactions induced by + alpha particles on 109Ag +AUTHOR (S.Fukushima, S.Kume, H.Okamura, K.Otozai, K.Sakamoto, + Y.Yoshizawa, S.Hayashi) +INSTITUTE (2JPNOSA) Faculty of Science + (2JPNJPN) Osaka Public Health Institute, Osaka +REFERENCE (J,NP,69,(2),273,196507) +SAMPLE Chemical-form of target is element. +METHOD (STTA) Stacks consisted of the 109Ag foils and + aluminium foils or of the natural silver foils + only. + (EDEG) Energy degradation by aluminium foils +ANALYSIS (DECAY) Initial activities were computed by the + least-squares method using know half-lives. +ERR-ANALYS (ERR-T) Uncertainties in beta- and gamma-ray counting + fluctuations, decay curve analyses and adopted + nuclear data (half-lives, branching ratios) +ADD-RES (COMP) Statistical model (Using level density + expressions based on the Fermi gas model) +STATUS (TABLE) Data taken from Table 1, p276 in reference +HISTORY (20040225C) Kc + On +ENDBIB 21 +NOCOMMON 0 0 +ENDSUBENT 24 +SUBENT E1876002 20050914 20050914 E032 +BIB 7 17 +REACTION (47-AG-109(A,N)49-IN-112-G,,SIG) +DECAY-DATA (49-IN-112-G,14.4MIN,B) + Beta rays higher than 0.3 MeV were counted. +SAMPLE - Target enrichment is 99.8%. + - Physical-form of target is solid. + - Target-thickness is 8 mg/cm**2. + - Backing: Electro-deposited onto iron foils +FACILITY (CYCLO,2JPNOSA) 110 cm cyclotron +DETECTOR Anthracene crystal +ADD-RES (DECAY) The half-life of the shorter-lived isomer was + determined to be 14.4+-0.2 min from the + analysis of the present data by use of 20.8 + min for the longer-lived isomer. +COMMENT Disintegration rate of 112In was determined from the + annihilation radiation measurement with NaI(Tl) + crystal which was calibrated with a 22Na standard + source. The position branching was taken to be 21.6%. +ENDBIB 17 +NOCOMMON 0 0 +DATA 3 6 +EN-CM DATA ERR-T +MEV MB MB + 9.7 0.0007 0.0004 + 11.5 0.016 0.006 + 13.8 0.09 0.03 + 15.2 0.09 0.03 + 17.5 0.06 0.02 + 19.5 0.04 0.02 +ENDDATA 8 +ENDSUBENT 30 +SUBENT E1876003 20050914 20050914 E032 +BIB 6 15 +REACTION (47-AG-109(A,N)49-IN-112-M,,SIG) +DECAY-DATA (49-IN-112-M,20.8MIN,B) + Beta rays higher than 0.3 MeV were counted. The + half-life of the longer-lived isomer was obtaned as + the weighted mean value of the published data. +SAMPLE - Target enrichment is 99.8%. + - Physical-form of target is solid. + - Target-thickness is 8 mg/cm**2. + - Backing: Electro-deposited onto iron foils +FACILITY (CYCLO,2JPNOSA) 110 cm cyclotron +DETECTOR Anthracene crystal +COMMENT Disintegration rate of 112In was determined from the + annihilation radiation measurement with NaI(Tl) + crystal which was calibrated with a 22Na standard + source. The position branching was taken to be 21.6%. +ENDBIB 15 +NOCOMMON 0 0 +DATA 3 6 +EN-CM DATA ERR-T +MEV MB MB + 9.7 0.0005 0.0002 + 11.5 0.014 0.004 + 13.8 0.18 0.04 + 15.2 0.26 0.06 + 17.5 0.30 0.07 + 19.5 0.21 0.05 +ENDDATA 8 +ENDSUBENT 28 +SUBENT E1876004 20050914 20050914 E032 +BIB 7 15 +REACTION (47-AG-109(A,2N)49-IN-111,,SIG) +DECAY-DATA (49-IN-111-G,2.8D,DG,170.) + (49-IN-111-G,2.8D,DG,240.) +SAMPLE - Target is natural. + - Physical-form of target is solid. Rolled foils + - Target-thickness is 7 to 10 mg/cm**2. +METHOD (CHSEP) +FACILITY (CYCLO,2JPNTOK) 160 cm variable energy cyclotron at + Institute for Nuclear Study +DETECTOR (NAICR) To detect the sum peak of the 170 and 240 keV + gamma rays +COMMENT Authors assumed that the 10 min isomer of 111In decays + only to the 2.8 day isomer. + The disintegration rate of 111In was determined by + means of gamma-gamma coincidence method. +ENDBIB 15 +NOCOMMON 0 0 +DATA 3 23 +EN-CM DATA ERR-T +MEV MB MB + 13.6 0.006 0.005 + 15.4 0.10 + 17.1 0.30 0.08 + 18.6 0.52 + 20.0 0.69 0.07 + 21.2 0.81 + 22.5 0.88 + 24.0 1.03 0.09 + 25.3 1.10 + 25.5 0.97 + 26.6 0.95 + 28.1 0.90 0.08 + 29.1 0.78 + 30.2 0.61 + 31.1 0.53 + 31.9 0.48 0.07 + 32.9 0.36 0.06 + 33.6 0.32 + 34.4 0.27 0.04 + 35.2 0.24 + 36.1 0.19 + 37.0 0.15 0.02 + 38.1 0.12 +ENDDATA 25 +ENDSUBENT 45 +SUBENT E1876005 20050914 20050914 E032 +BIB 5 12 +REACTION (47-AG-109(A,3N)49-IN-110-M,,SIG) +DECAY-DATA (49-IN-110-M,66.MIN,B+,2200.) +SAMPLE - Target is natural. + - Physical-form of target is solid. Rolled foils + - Target-thickness is 7 to 10 mg/cm**2. +FACILITY (CYCLO,2JPNTOK) 160 cm variable energy cyclotron at + Institute for Nuclear Study +DETECTOR (GEMUC) To detect 2.2 MeV positrons. An aluminium + absorber was used to cut down beta rays with + energies lower than 1.5 MeV. Thus the + interference of the 1.29 MeV positions from + the 58 min isomer of 108In was minimized. +ENDBIB 12 +NOCOMMON 0 0 +DATA 3 11 +EN-CM DATA ERR-T +MEV MB MB + 26.9 0.08 0.01 + 28.1 0.11 0.02 + 29.3 0.11 + 30.4 0.13 0.02 + 31.4 0.15 0.02 + 32.3 0.20 + 33.4 0.20 0.03 + 34.4 0.21 + 35.2 0.16 0.04 + 36.1 0.14 + 37.0 0.19 0.03 +ENDDATA 13 +ENDSUBENT 30 +SUBENT E1876006 20050914 20050914 E032 +BIB 5 8 +REACTION (47-AG-109(A,3N)49-IN-110-G,,SIG) +DECAY-DATA (49-IN-110-G,4.9HR,DG,884.) +SAMPLE - Target is natural. + - Physical-form of target is solid. Rolled foils + - Target-thickness is 7 to 10 mg/cm**2. +FACILITY (CYCLO,2JPNTOK) 160 cm variable energy cyclotron at + Institute for Nuclear Study +DETECTOR (NAICR) To detect 0.884 MeV gamma rays +ENDBIB 8 +NOCOMMON 0 0 +DATA 3 13 +EN-CM DATA ERR-T +MEV MB MB + 26.6 0.16 + 26.9 0.19 0.05 + 27.8 0.25 + 28.1 0.28 0.08 + 29.6 0.44 + 30.9 0.54 + 31.9 0.60 0.10 + 33.1 0.67 0.09 + 34.1 0.71 + 35.2 0.76 + 36.1 0.81 + 37.0 0.73 0.10 + 38.1 0.76 +ENDDATA 15 +ENDSUBENT 28 +ENDENTRY 6 diff --git a/exforall/E18/E1877.x4 b/exforall/E18/E1877.x4 new file mode 100644 index 000000000..e065c2a24 --- /dev/null +++ b/exforall/E18/E1877.x4 @@ -0,0 +1,116 @@ +ENTRY E1877 20050914 20050914 E032 +SUBENT E1877001 20050914 20050914 E032 +BIB 12 29 +TITLE Excitation functions for proton-induced reactions of + 140Ce and 142Ce up to Ep=15 MeV +AUTHOR (M.Furukawa) +INSTITUTE (2JPNTOK) Department of Chemistry, Faculty of Science +REFERENCE (J,NP/A,90,(2),253,196701) + Misprinted as Vol.67 at the top of the first page +INC-SOURCE Beam intensity is about 0.5 micro-Ampere. +SAMPLE - Target is natural. + - Chemical-form of target: Ceric oxide or cerous + fluoride + - Physical-form of target is solid. + - Target-thickness is about 5 mg/cm**2. + - Backing is aluminium. Deposited on aluminium foil +METHOD (ACTIV) Irradiated between 0.5 min and 2 h + (EDEG) Degraded by aluminium placed between targets. + The stopping power was taken from the + compilation of Sternheimer [R.M. Sternheimer, + Phys. Rev. 115(1959)137]. +FACILITY (CYCLO,2JPNTOK) Institute for Nuclear Study +ERR-ANALYS (ERR-T) Uncertainties in target thickness, beam + currents and disintegration rates of residual + nuclei +ADD-RES (COMP) Statistical model + (TRCS) The sum of measured cross sections for 140Ce is + compared with the calculation on the basis of + the continuum theory [M.M. Shapiro, Phys. Rev. + 90(1953)171]. +STATUS (TABLE) Data taken from Table 2, p255 in reference +HISTORY (20040226C) Kc + On +ENDBIB 29 +NOCOMMON 0 0 +ENDSUBENT 32 +SUBENT E1877002 20050914 20050914 E032 +BIB 5 7 +REL-REF (D,P0033001,J.P.Blaser+,J,HPA,24,441,1951) +REACTION (58-CE-140(P,N)59-PR-140,,SIG) +DECAY-DATA (59-PR-140,3.4MIN,AR,0.51,1.08) +METHOD (COINC) Detect annihilation radiation and annihilation + radiation in coincidence. +DETECTOR (NAICR) To detect 0.51 MeV gamma from positron + annihilation +ENDBIB 7 +NOCOMMON 0 0 +DATA 3 14 +EN DATA ERR-T +MEV MB MB + 5.57 7.6 2.0 + 6.64 41.0 + 7.18 86.0 + 7.50 91.0 + 8.19 160.0 25.0 + 8.68 225.0 + 9.72 426.0 + 10.05 563.0 + 11.31 807.0 130.0 + 11.83 950.0 + 12.68 946.0 + 13.33 815.0 145.0 + 13.87 772.0 + 14.59 558.0 100.0 +ENDDATA 16 +ENDSUBENT 28 +SUBENT E1877003 20050914 20050914 E032 +BIB 5 7 +REACTION (58-CE-140(P,2N)59-PR-139,,SIG) +DECAY-DATA (59-PR-139,140.D,DG,166.,0.82) + Conversion electron emission is taken into account for + given abundance. +RAD-DET (58-CE-139-G,DG) +METHOD (CHSEP) +DETECTOR (NAICR) To detect 166 keV decay gamma from 139Ce +ENDBIB 7 +NOCOMMON 0 0 +DATA 3 3 +EN DATA ERR-T +MEV MB MB + 13.28 91.0 15.0 + 14.04 281.0 42.0 + 14.58 447.0 67.0 +ENDDATA 5 +ENDSUBENT 17 +SUBENT E1877004 20050914 20050914 E032 +BIB 6 7 +REL-REF (D,P0033001,J.P.Blaser+,J,HPA,24,441,1951) + (D,B0052019,H.G.Blosser+,J,PR,100,(5),1340,195512) +REACTION (58-CE-142(P,N)59-PR-142,,SIG) +DECAY-DATA (59-PR-142-G,19.2HR,B-,,1.00) +METHOD (CHSEP) +ANALYSIS (DECAY) +DETECTOR (GEMUC) To detect negatons from 142Pr +ENDBIB 7 +NOCOMMON 0 0 +DATA 3 15 +EN DATA ERR-T +MEV MB MB + 5.76 6.9 1.4 + 6.47 21.8 + 7.09 58.6 + 7.97 114.5 16.0 + 8.67 108.0 + 9.21 87.0 + 9.37 95.5 13.5 + 9.74 80.7 + 10.04 83.5 + 11.00 51.3 7.3 + 11.66 48.6 + 12.49 33.0 + 13.28 34.2 + 14.04 29.4 5.0 + 14.58 29.5 +ENDDATA 17 +ENDSUBENT 29 +ENDENTRY 4 diff --git a/exforall/E18/E1878.x4 b/exforall/E18/E1878.x4 new file mode 100644 index 000000000..406b89f06 --- /dev/null +++ b/exforall/E18/E1878.x4 @@ -0,0 +1,127 @@ +ENTRY E1878 20050914 20050914 E032 +SUBENT E1878001 20050914 20050914 E032 +BIB 12 24 +TITLE Cross sections and reaction mechanisms of (p,pxn) + reactions on 208Pb in the 24-52 MeV range +AUTHOR (H.Kawakami, M.Koike, K.Komura, M.Sakai, N.Yoshikawa, + R.Donangelo, J.O.Rasmussen) +INSTITUTE (2JPNTOK) Institute for Nuclear Study + (1USABRK) +REFERENCE (J,NP/A,262,(1),52,197605) +INC-SOURCE Beam intensity is about 1 nA. +SAMPLE - Target enrichment is 99.9%. + - Chemical-form of target is element. + - Physical-form of target is solid. Metallic foil + - Target-thickness is 8.3 mg/cm**2. Rolled 12.8 mg/cm2 + target was also used for the lifetime measurement at + 44 MeV +METHOD (EDEG) Incident proton energy was adjusted by carbon + plate absorbers. +FACILITY (CYCLO,2JPNTOK) Institute for Nuclear Study +DETECTOR (GELI) Energy resolution was 2.5 keV (FWHM) at 1.33 + MeV. Detection efficiency was calibrated with + IAEA standard sources 137Cs and 60Co. +ERR-ANALYS (ERR-T) Overall errors for cross section + (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table 1, p53 in reference +HISTORY (20040226C) Sr + On +ENDBIB 24 +COMMON 1 3 +ERR-T +PER-CENT + 25.0 +ENDCOMMON 3 +ENDSUBENT 31 +SUBENT E1878002 20050914 20050914 E032 +BIB 3 7 +REACTION (82-PB-208(P,X)82-PB-207-M,,SIG) +DECAY-DATA (82-PB-207-M,0.80SEC,DG,569.8) + Isomeric transition from 207Pb (13/2+) + (82-PB-207-M,0.80SEC,DG,1063.7) + Isomeric transition from 207Pb (13/2+) +ADD-RES (COMP) Reaction cross section according to Wong et al. + [C.Y. Wong, Phys. Rev. Lett. 31(1973)766] +ENDBIB 7 +NOCOMMON 0 0 +DATA 3 5 +EN DATA DATA-ERR +MEV MB MB + 24.0 21.0 4.0 + 28.0 45.0 9.0 + 36.0 58.0 12.0 + 44.0 58.0 12.0 + 52.0 65.0 13.0 +ENDDATA 7 +ENDSUBENT 19 +SUBENT E1878003 20050914 20050914 E032 +BIB 6 10 +REACTION (82-PB-208(P,X)82-PB-207,PAR,SIG) +PART-DET (G) 569.8 keV prompt gamma of 207Pb, 5/2- to 1/2- + transition +EN-SEC (E-LVL,82-PB-207) +LEVEL-PROP (82-PB-207,E-LVL=0.5698,SPIN=2.5,PARITY=-1.) +ADD-RES (COMP) Reaction cross section according to Wong et al. + [C.Y. Wong, Phys. Rev. Lett. 31(1973)766] +COMMENT Cross section refers to prompt gamma-decay and does + not include the delayed feeding from the high spin + isomers. +ENDBIB 10 +COMMON 1 3 +E-LVL +KEV + 569.8 +ENDCOMMON 3 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 44.0 120.0 25.0 +ENDDATA 3 +ENDSUBENT 22 +SUBENT E1878004 20050914 20050914 E032 +BIB 5 7 +REACTION (82-PB-208(P,X)82-PB-206,PAR,SIG) +PART-DET (G) 802.9 keV prompt gamma of 206mPb, Isomeric + transition decay from 206Pb (7-) +EN-SEC (E-LVL,82-PB-206) +LEVEL-PROP (82-PB-206,E-LVL=2.2,SPIN=7.,PARITY=-1.) +ADD-RES (COMP) Reaction cross section accorging to Wong et al. + [C.Y. Wong, Phys. Rev. Lett. 31(1973)766] +ENDBIB 7 +COMMON 1 3 +E-LVL +MEV + 2.2 +ENDCOMMON 3 +DATA 3 5 +EN DATA DATA-ERR +MEV MB MB + 24.0 2.0 1.0 + 28.0 8.0 3.0 + 36.0 34.0 11.0 + 44.0 57.0 18.0 + 52.0 57.0 18.0 +ENDDATA 7 +ENDSUBENT 23 +SUBENT E1878005 20050914 20050914 E032 +BIB 5 8 +REACTION (82-PB-208(P,X)82-PB-206,PAR,SIG) +PART-DET (G) 802.9 keV prompt gamma of 206Pb, 2+ to 0+ (g.s.) + transition +EN-SEC (E-LVL,82-PB-206) +LEVEL-PROP (82-PB-206,E-LVL=0.8029,SPIN=2.,PARITY=+1.) +COMMENT Cross section refers to prompt gamma-decay and does + not include the delayed feeding from the high spin + isomers. +ENDBIB 8 +COMMON 1 3 +E-LVL +KEV + 802.9 +ENDCOMMON 3 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 44.0 95.0 20.0 +ENDDATA 3 +ENDSUBENT 20 +ENDENTRY 5 diff --git a/exforall/E18/E1879.x4 b/exforall/E18/E1879.x4 new file mode 100644 index 000000000..1165bd478 --- /dev/null +++ b/exforall/E18/E1879.x4 @@ -0,0 +1,111 @@ +ENTRY E1879 20050914 20050914 E032 +SUBENT E1879001 20050914 20050914 E032 +BIB 13 24 +TITLE Excitation functions for the (d,p) reactions on 96Ru, + 102Ru and 104Ru +AUTHOR (A.Mito, K.Komura, T.Mitsugashira, K.Otozai) +INSTITUTE (2JPNOSA) Faculty of Science +REFERENCE (J,NP/A,129,(1),165,196905) +INC-SOURCE Beam intensity is 0.5 micro-Ampere. +SAMPLE - Target is natural. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is about 3 mg/cm**2. + - Backing is copper. Electrodeposited onto copper + foils +METHOD (STTA) Stacked with aluminium foils for energy + degration + (ACTIV) Irradiated for 20 min + (CHSEP) Separation of ruthenium from rhodium +FACILITY (CYCLO,2JPNKTO) 11.2 and 12.1 MeV deuteron + (CYCLO,2JPNOSA) 14.6 MeV deuteron +DETECTOR (NAICR) To measure activities of each counting source +ERR-ANALYS (DATA-ERR) Standard deviation +ADD-RES (COMP) Semi-classical model (Modified Peaslee's theory + [K. Otozai et al., Nucl. Phys. 81(1966)322]) +STATUS (TABLE) Data taken from Table 2, p168 in reference +HISTORY (20040226C) Ic + On +ENDBIB 24 +COMMON 1 3 +EN-RSL +MEV + 0.1 +ENDCOMMON 3 +ENDSUBENT 31 +SUBENT E1879002 20050914 20050914 E032 +BIB 3 5 +REL-REF (R,,S.Katcoff,J,PR,111,(2),575,195806) + Half-life of product + (R,,T.von Cretzu+,J,ADP,17,1,1966) Decay scheme +REACTION (44-RU-96(D,P)44-RU-97,,SIG) +DECAY-DATA (44-RU-97,2.88D,DG,216.) +ENDBIB 5 +NOCOMMON 0 0 +DATA 3 10 +EN-CM DATA DATA-ERR +MEV MB MB + 4.4 20.0 + 5.9 110.0 + 6.5 190.0 + 7.1 240.0 + 8.0 330.0 + 8.7 350.0 + 9.8 360.0 + 11.7 320.0 20.0 + 12.7 290.0 + 14.0 230.0 60.0 +ENDDATA 12 +ENDSUBENT 22 +SUBENT E1879003 20050914 20050914 E032 +BIB 3 4 +REL-REF (R,,K.F.Flynn+,J,NSE,22,416,1965) Half-life of product + (R,,A.Mukerji+,J,NP,67,(2),466,196505) Decay scheme +REACTION (44-RU-102(D,P)44-RU-103,,SIG) +DECAY-DATA (44-RU-103-G,39.5D,DG,498.) +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 10 +EN-CM DATA DATA-ERR +MEV MB MB + 4.4 20.0 + 5.9 120.0 + 6.5 190.0 + 7.1 220.0 + 8.0 240.0 + 8.7 280.0 + 9.8 280.0 + 11.7 230.0 30.0 + 12.7 220.0 + 14.0 190.0 40.0 +ENDDATA 12 +ENDSUBENT 21 +SUBENT E1879004 20050914 20050914 E032 +BIB 4 10 +REL-REF (R,,H.W.Brandhorst+,J,PR,125,(4),1323,196202) + Half-life of product + (R,,W.R.Pierson,J,PR,140B,(6),1516,196512) + Decay scheme +REACTION (44-RU-104(D,P)44-RU-105,,SIG) +DECAY-DATA (44-RU-105,4.43HR,DG,306.) + Delayed gamma from 105Rh (35.88 h) + (44-RU-105,4.43HR,DG,319.) + Delayed gamma from 105Rh (35.88 h) +RAD-DET (45-RH-105-G,DG) +ENDBIB 10 +NOCOMMON 0 0 +DATA 3 10 +EN-CM DATA DATA-ERR +MEV MB MB + 4.4 30.0 + 5.9 120.0 + 6.5 140.0 + 7.1 140.0 + 8.0 180.0 + 8.7 220.0 + 9.8 210.0 + 11.7 150.0 + 12.7 140.0 + 14.0 140.0 30.0 +ENDDATA 12 +ENDSUBENT 27 +ENDENTRY 4 diff --git a/exforall/E18/E1881.x4 b/exforall/E18/E1881.x4 new file mode 100644 index 000000000..ab439f667 --- /dev/null +++ b/exforall/E18/E1881.x4 @@ -0,0 +1,142 @@ +ENTRY E1881 20050914 20050914 E032 +SUBENT E1881001 20050914 20050914 E032 +BIB 13 35 +TITLE Excitation functions for the reactions induced by + deuterons on 142Ce up to 14.2 MeV +AUTHOR (K.Otozai, S.Kume, M.Koyama, T.Mitsuji, T.Nishi, + I.Fujiwara) +INSTITUTE (2JPNOSA) Faculty of Science + (2JPNKTO) Faculty of Science + (2JPNKTO) Engineering Research Institute +REFERENCE (J,NP,81,(2),322,196606) +SAMPLE - Target is natural. + - Chemical-form of target: Cerium oxide + - Physical-form of target is solid. + - Target-thickness is 1 to 5 mg/cm**2. + - Backing is aluminium. Deposited on aluminium foil +METHOD (STTA) Deuteron energy at each cerium oxide target was + estimated from the range-energy relation given + by Bichsel et al. [H. Bichsel et al., Phys. + Rev. 105(1957)1788]. + (ACTIV) 1 h (350 to 900 micro-Coulomb) at Osaka Univ. + and 1.5 h (1300 to 1400 micro-Coulomb) at + Kyoto Univ. +FACILITY (CYCLO,2JPNOSA) 11.2 MeV deuteron from 110 cm + cyclotron + (CYCLO,2JPNKTO) 14.4 MeV deuteron from 105 cm + cyclotron +DETECTOR (SCIN) Anthracene scintillator to detect beta rays +ERR-ANALYS (ERR-T) Uncertainties in target thickness, countings, + decay analyses, half-lives and counting + efficiency measurements +ADD-RES (COMP) 1. Statistical model + 2. Peaslee theory for stripping process [D.C. + Peaslee, Phys. Rev. 74(1948)1001] +FLAG (1.) Experiments by cyclotron at Osaka University + (2.) Experiments by cyclotron at Kyoto University +STATUS (TABLE) Data taken from Table 1, p325 in reference +HISTORY (20040227C) Ic + On +ENDBIB 35 +NOCOMMON 0 0 +ENDSUBENT 38 +SUBENT E1881002 20050914 20050914 E032 +BIB 4 10 +REACTION (58-CE-142(D,P)58-CE-143,,SIG) +DECAY-DATA (58-CE-143,33.4HR,B-) +RAD-DET (59-PR-143,B-) +METHOD (CHSEP) After two weeks from the first chemical + separation, when the activities of 143Ce had + completely decayed to 143Pr, praseodymium was + again separated from cerium by ion exchange + technique. In this way, 141Ce from + 140Ce(d,p)141Ce and 143Ce from 142Ce(d,p)143Ce + are distinguished from each other. +ENDBIB 10 +NOCOMMON 0 0 +DATA 4 10 +EN-CM DATA ERR-T FLAG +MEV MB MB NO-DIM + 3.9 0.70 0.05 1.0 + 5.5 20.0 1.0 1.0 + 6.7 66.0 4.0 1.0 + 7.0 74.0 7.0 2.0 + 8.0 124.0 7.0 1.0 + 9.5 230.0 10.0 1.0 + 10.4 230.0 20.0 2.0 + 10.8 190.0 10.0 1.0 + 12.6 140.0 20.0 2.0 + 14.0 170.0 20.0 2.0 +ENDDATA 12 +ENDSUBENT 27 +SUBENT E1881003 20050914 20050914 E032 +BIB 6 10 +REACTION (58-CE-142(D,N)59-PR-143,,SIG) +DECAY-DATA (59-PR-143,13.76D,B-) +METHOD (CHSEP) +ANALYSIS (DECAY) 142Pr and 143Pr were distinguished from each + other by analysing decay curve. +DETECTOR 2 pi gas-flow counter used supplementally +CORRECTION 143Pr produced by the decay of 143Ce from the (d,p) + reaction till the time of the separation of both + elements was subtracted in the calculation of the + cross section of the (d,n) reactio by authors. +ENDBIB 10 +NOCOMMON 0 0 +DATA 4 9 +EN-CM DATA ERR-T FLAG +MEV MB MB NO-DIM + 5.5 1.8 0.5 1.0 + 6.7 8.8 0.8 1.0 + 7.0 18.0 2.0 2.0 + 8.0 24.0 1.0 1.0 + 9.5 37.0 3.0 1.0 + 10.4 50.0 7.0 2.0 + 10.8 54.0 3.0 1.0 + 12.6 60.0 10.0 2.0 + 14.0 56.0 7.0 2.0 +ENDDATA 11 +ENDSUBENT 26 +SUBENT E1881004 20050914 20050914 E032 +BIB 4 7 +REACTION (58-CE-142(D,2N)59-PR-142-G,,SIG) +DECAY-DATA (59-PR-142-G,19.14HR,B-) + T1/2=19.14+-0.05 hour is determined in this + experiment. +METHOD (CHSEP) +ANALYSIS (DECAY) 142Pr and 143Pr were distinguished from each + other by analysing decay curve. +ENDBIB 7 +NOCOMMON 0 0 +DATA 4 9 +EN-CM DATA ERR-T FLAG +MEV MB MB NO-DIM + 5.5 8.0 1.0 1.0 + 6.7 60.0 8.0 1.0 + 7.0 77.0 7.0 2.0 + 8.0 230.0 10.0 1.0 + 9.5 540.0 30.0 1.0 + 10.4 650.0 80.0 2.0 + 10.8 730.0 50.0 1.0 + 12.6 750.0 80.0 2.0 + 14.0 530.0 50.0 2.0 +ENDDATA 11 +ENDSUBENT 23 +SUBENT E1881005 20050914 20050914 E032 +BIB 3 3 +REACTION (58-CE-142(D,A)57-LA-140,,SIG) +DECAY-DATA (57-LA-140,40.23HR,B-) +METHOD (CHSEP) +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 6 +EN-CM DATA ERR-T FLAG +MEV MB MB NO-DIM + 7.0 0.58 0.05 2.0 + 9.5 1.24 0.07 1.0 + 10.4 1.7 0.1 2.0 + 10.8 1.9 0.1 1.0 + 12.6 1.7 0.2 2.0 + 14.0 1.9 0.2 2.0 +ENDDATA 8 +ENDSUBENT 16 +ENDENTRY 5 diff --git a/exforall/E18/E1882.x4 b/exforall/E18/E1882.x4 new file mode 100644 index 000000000..abb8a9890 --- /dev/null +++ b/exforall/E18/E1882.x4 @@ -0,0 +1,129 @@ +ENTRY E1882 20050914 20050914 E032 +SUBENT E1882001 20050914 20050914 E032 +BIB 15 30 +TITLE Spallation of niobium by 12 GeV protons +AUTHOR (T.Tominaka, S.Ban, H.Ikeda, K.Katoh, K.Kondo, + M.Takasaki, A.Yamamoto, H.Hirabayashi, Y.Narahara) +INSTITUTE (2JPNLEP) + (2JPNTSU) Institute of Physics +REFERENCE (J,NP/A,414,(3),385,198402) +REL-REF (R,,C.M.Lederer+,B,LEDERER-7,,1978) Decay data +MONIT-REF ((MONIT),J.B.Cumming+,J,NIM,180,(1),37,198102) +INC-SOURCE Beam intensity: about 1.2e11 protons/pulse +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness: 50 micro-meter thick for each + stack +METHOD (EXTB) Exposed for 3 min + (GSPEC) Measured commencing at 75 min after the + irradiation and continuing intermittently for + 200 days +FACILITY (SYNCH,2JPNLEP) +DETECTOR (GELI) Resolution is 2.0 keV at 1332 keV. Efficiency + is 10 % relative to 7.6 cm x 7.6 cm NaI. +ERR-ANALYS (ERR-1) Uncertainty due to the secondary emission + chamber calibration + (DATA-ERR) Systematic error of about 10% resulting + from the secondary emission chamber + calibration has not been incorporated in. +COMMENT EN-NRM: Incident energy for adopted monitor cross + section which is independent between 10 and 28 GeV + [J.B. Cumming, Ann. Rev. Nucl. Sci. 13(1963)261]. +STATUS (TABLE) Data taken from Table 1, p387 in reference +HISTORY (20040228C) Kc + On +ENDBIB 30 +COMMON 4 3 +EN EN-NRM MONIT ERR-1 +GEV GEV MB PER-CENT + 12.0 28.0 7.92 10.0 +ENDCOMMON 3 +ENDSUBENT 37 +SUBENT E1882002 20050914 20050914 E032 +BIB 3 3 +REACTION (41-NB-93(P,X)ELEM/MASS,IND,SIG) +MONITOR ((MONIT)13-AL-27(P,N+3P)11-NA-24,,SIG) +PART-DET (DG) Gamma energies and half-lives are not given. +ENDBIB 3 +NOCOMMON 0 0 +DATA 5 25 +ELEMENT MASS ISOMER DATA DATA-ERR +NO-DIM NO-DIM NO-DIM MB MB + 5.0 7.0 9.72 2.56 + 21.0 44.0 1.0 2.36 0.21 + 21.0 46.0 2.36 0.40 + 21.0 47.0 1.32 0.46 + 21.0 48.0 0.31 0.12 + 23.0 48.0 2.63 0.12 + 25.0 54.0 5.26 0.56 + 27.0 56.0 1.56 0.33 + 27.0 58.0 6.37 1.08 + 31.0 66.0 4.01 0.48 + 33.0 72.0 7.76 0.60 + 33.0 74.0 2.36 0.31 + 34.0 75.0 4.17 0.86 + 35.0 76.0 5.98 1.57 + 35.0 77.0 10.5 1.4 + 37.0 82.0 1.0 4.70 0.75 + 37.0 83.0 5.2 2.8 + 37.0 84.0 2.74 0.22 + 39.0 86.0 5.74 0.41 + 39.0 86.0 1.0 6.55 0.49 + 39.0 87.0 2.88 0.92 + 39.0 88.0 10.9 2.3 + 39.0 90.0 1.0 1.05 0.05 + 41.0 90.0 12.8 4.2 + 41.0 92.0 1.0 15.6 1.4 +ENDDATA 27 +ENDSUBENT 35 +SUBENT E1882003 20050914 20050914 E032 +BIB 4 5 +REACTION (41-NB-93(P,X)ELEM/MASS,CUM,SIG) +MONITOR ((MONIT)13-AL-27(P,N+3P)11-NA-24,,SIG) +PART-DET (DG) Gamma energies and half-lives are not given + except the half-life of 84Y (39 min). +FLAG (1.) Include partial contribution from precursors +ENDBIB 5 +NOCOMMON 0 0 +DATA 6 20 +ELEMENT MASS ISOMER DATA DATA-ERR FLAG +NO-DIM NO-DIM NO-DIM MB MB NO-DIM + 11.0 24.0 3.64 0.23 + 20.0 47.0 1.02 0.12 + 25.0 56.0 1.18 0.27 + 30.0 65.0 8.08 0.89 + 31.0 67.0 8.40 0.53 + 32.0 69.0 8.57 0.74 + 33.0 71.0 6.81 1.94 + 34.0 73.0 4.82 0.43 1.0 + 35.0 75.0 4.64 0.60 + 36.0 76.0 1.55 0.62 + 36.0 77.0 2.24 0.17 + 36.0 79.0 11.9 0.91 + 37.0 81.0 16.4 2.5 1.0 + 38.0 82.0 6.63 0.88 + 38.0 83.0 11.8 1.3 + 39.0 84.0 1.0 2.23 0.29 1.0 + 39.0 87.0 1.0 22.8 4.0 + 40.0 86.0 3.56 0.24 + 40.0 88.0 13.6 3.8 + 40.0 89.0 31.8 2.3 +ENDDATA 22 +ENDSUBENT 32 +SUBENT E1882004 20050914 20050914 E032 +BIB 3 6 +REACTION (41-NB-93(P,X)ELEM/MASS,,SIG) + Authors cannot determine the type of yield (cumulative + or independent) +MONITOR ((MONIT)13-AL-27(P,N+3P)11-NA-24,,SIG) +PART-DET (DG) Gamma energies and half-lives are not given + except the half-life of 89Nb (66 min). +ENDBIB 6 +NOCOMMON 0 0 +DATA 5 2 +ELEMENT MASS ISOMER DATA DATA-ERR +NO-DIM NO-DIM NO-DIM MB MB + 25.0 52.0 1.61 0.10 + 41.0 89.0 1.0 1.18 0.18 +ENDDATA 4 +ENDSUBENT 15 +ENDENTRY 4 diff --git a/exforall/E18/E1883.x4 b/exforall/E18/E1883.x4 new file mode 100644 index 000000000..a3d806faf --- /dev/null +++ b/exforall/E18/E1883.x4 @@ -0,0 +1,1335 @@ +ENTRY E1883 20050914 20050914 E032 +SUBENT E1883001 20050914 20050914 E032 +BIB 13 27 +TITLE Alpha-particle doorway states in 28Si +AUTHOR (K.Katori, K.Furuno, T.Ooi, S.Hanashima) +INSTITUTE (2JPNTSU) Institute of Physics and Tandem Accelerator + Center +REFERENCE (J,PR/C,21,(4),1387,198004) +PART-DET (6-C-12) +EN-SEC (E-LVL1,6-C-12) +INC-SOURCE Charge of incident ion is 5+, 6+, 7+. +SAMPLE - Target is natural. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 0.029 mg/cm**2. Measured by the + energy-loss method with an 241Am alpha source. + - Target is self supported. +FACILITY (VDGT,2JPNTSU) 12 UD Pelletron +DETECTOR - Solid angle of detector is 0.94 msr.(Corresponding + to Delta-theta (lab) = +-0.72 deg or + Delta-theta(c.m.) = +-1.5 deg) + - E-RSL is about 70 keV. + (MAGSP) ESP-90 magnetic spectrograph [J.E. Spencer et + al., Nucl. Instrum. Methods 49(1976)181]. + (SI) Two 47 mm Si position-sensitive detectors +ERR-ANALYS (ERR-T) Including uncertainties of the charge + collection, target thickness, and detection + efficiency +ADD-RES (COMP) Statistical model (Hauser-Feshbach theory) +HISTORY (20040413C) Ic + On +ENDBIB 27 +COMMON 3 3 +E-RSL E-LVL1 ERR-T +KEV MEV PER-CENT + 70.0 0.0 20.0 +ENDCOMMON 3 +ENDSUBENT 34 +SUBENT E1883002 20050914 20050914 E032 +BIB 5 8 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG is polar angle between beam and 12C in laboratory + system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.049,SPIN=0.,PARITY=+1.) +ADD-RES (COMP) Band-crossing model [T. Matsuse et al., Phys. + Rev. 59(1978)1904] +STATUS (CURVE) Data scanned from Fig.2, p1389 in reference +ENDBIB 8 +COMMON 3 3 +ANG ANG-ERR E-LVL2 +ADEG ADEG MEV + 7.0 0.72 6.049 +ENDCOMMON 3 +DATA 2 102 +EN-CM DATA-CM +MEV MB/SR + 22.63 0.25 + 22.78 0.30 + 22.85 0.34 + 22.93 0.26 + 23.04 0.26 + 23.07 0.36 + 23.18 0.25 + 23.26 0.36 + 23.33 0.55 + 23.52 0.82 + 23.55 0.87 + 23.67 0.97 + 23.81 0.85 + 23.85 0.76 + 23.92 0.81 + 24.07 0.81 + 24.15 0.83 + 24.22 0.76 + 24.26 0.83 + 24.41 0.78 + 24.48 0.93 + 24.52 0.87 + 24.70 0.62 + 24.78 0.47 + 24.85 0.38 + 25.00 0.32 + 25.03 0.41 + 25.18 0.30 + 25.22 0.34 + 25.33 0.41 + 25.40 0.26 + 25.52 0.32 + 25.55 0.41 + 25.66 0.28 + 25.77 0.30 + 26.00 0.38 + 26.07 0.28 + 26.18 0.28 + 26.29 0.26 + 26.33 0.28 + 26.37 0.19 + 26.40 0.20 + 26.51 0.34 + 26.55 0.24 + 26.70 0.28 + 26.81 0.24 + 26.85 0.28 + 26.96 0.24 + 27.03 0.28 + 27.07 0.36 + 27.22 0.32 + 27.29 0.32 + 27.33 0.26 + 27.51 0.24 + 27.59 0.22 + 27.66 0.34 + 27.85 0.41 + 27.96 0.47 + 28.03 0.43 + 28.14 0.47 + 28.29 0.49 + 28.44 0.47 + 28.51 0.32 + 28.59 0.18 + 28.70 0.13 + 28.77 0.24 + 28.92 0.20 + 29.03 0.18 + 29.10 0.13 + 29.25 0.14 + 29.33 0.18 + 29.44 0.18 + 29.55 0.16 + 29.81 0.12 + 29.99 0.09 + 30.07 0.14 + 30.18 0.18 + 30.33 0.09 + 30.44 0.12 + 30.55 0.16 + 30.58 0.09 + 30.70 0.10 + 30.81 0.09 + 30.95 0.08 + 31.07 0.08 + 31.14 0.08 + 31.32 0.10 + 31.47 0.10 + 31.51 0.18 + 31.66 0.27 + 31.77 0.37 + 31.84 0.25 + 31.92 0.33 + 32.03 0.37 + 32.21 0.39 + 32.21 0.27 + 32.36 0.35 + 32.40 0.25 + 32.51 0.18 + 32.62 0.14 + 32.73 0.10 + 32.84 0.10 +ENDDATA 104 +ENDSUBENT 121 +SUBENT E1883003 20050914 20050914 E032 +BIB 5 8 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG is polar angle between beam and 12C in laboratory + system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.131,SPIN=3.,PARITY=-1.) +ADD-RES (COMP) Band-crossing model [T. Matsuse et al., Phys. + Rev. 59(1978)1904] +STATUS (CURVE) Data scanned from Fig.2, p1389 in reference +ENDBIB 8 +COMMON 3 3 +ANG ANG-ERR E-LVL2 +ADEG ADEG MEV + 7.0 0.72 6.131 +ENDCOMMON 3 +DATA 2 121 +EN-CM DATA-CM +MEV MB/SR + 22.80 3.903 + 22.85 3.666 + 22.94 2.953 + 23.07 2.335 + 23.14 1.632 + 23.19 1.110 + 23.34 1.157 + 23.46 1.185 + 23.49 1.005 + 23.59 1.080 + 23.65 1.527 + 23.76 1.565 + 23.92 1.583 + 23.93 1.051 + 24.02 1.108 + 24.14 1.108 + 24.22 1.288 + 24.31 1.127 + 24.42 1.089 + 24.50 1.411 + 24.58 1.535 + 24.69 1.668 + 24.74 2.086 + 24.82 2.456 + 24.91 2.247 + 25.01 2.351 + 25.08 2.218 + 25.19 2.075 + 25.27 2.151 + 25.35 2.664 + 25.46 2.692 + 25.51 3.034 + 25.65 2.265 + 25.67 2.141 + 25.78 1.932 + 25.85 1.561 + 25.97 1.552 + 26.03 1.694 + 26.14 1.684 + 26.21 1.627 + 26.33 1.627 + 26.41 1.769 + 26.48 1.598 + 26.54 1.484 + 26.59 1.588 + 26.73 1.569 + 26.88 1.531 + 26.90 1.331 + 26.99 1.246 + 27.08 1.094 + 27.16 1.322 + 27.27 1.245 + 27.35 1.188 + 27.44 1.112 + 27.52 0.922 + 27.58 0.855 + 27.71 0.789 + 27.80 0.731 + 27.92 0.874 + 27.95 0.807 + 28.05 1.244 + 28.19 1.310 + 28.28 1.434 + 28.38 1.576 + 28.38 1.310 + 28.49 1.462 + 28.62 1.196 + 28.66 1.509 + 28.78 1.594 + 28.82 1.499 + 28.91 1.794 + 28.99 1.832 + 29.08 1.565 + 29.17 2.249 + 29.28 2.202 + 29.34 2.334 + 29.47 2.325 + 29.49 2.876 + 29.59 3.123 + 29.65 3.246 + 29.73 3.721 + 29.86 3.825 + 29.96 4.100 + 30.11 4.148 + 30.11 3.787 + 30.22 3.701 + 30.32 3.653 + 30.34 1.687 + 30.48 2.437 + 30.59 1.791 + 30.64 1.563 + 30.76 1.658 + 30.79 1.430 + 30.88 1.239 + 30.98 1.068 + 31.09 1.163 + 31.23 1.305 + 31.29 1.467 + 31.35 1.799 + 31.44 1.942 + 31.50 1.561 + 31.65 1.932 + 31.68 1.276 + 31.83 1.228 + 31.85 0.991 + 31.95 0.848 + 32.10 1.399 + 32.17 0.819 + 32.25 0.914 + 32.29 1.323 + 32.40 1.218 + 32.46 1.037 + 32.61 0.876 + 32.71 1.208 + 32.74 1.008 + 32.88 0.904 + 32.90 1.160 + 32.99 0.865 + 33.11 0.970 + 33.20 0.865 + 33.41 0.931 +ENDDATA 123 +ENDSUBENT 140 +SUBENT E1883004 20050914 20050914 E032 +BIB 6 11 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG is polar angle between beam and 12C in laboratory + system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.049,SPIN=0.,PARITY=+1.) + (8-O-16,E-LVL=6.131,SPIN=3.,PARITY=-1.) +ADD-RES (COMP) Band-crossing model [T. Matsuse et al., Phys. + Rev. 59(1978)1904] +COMMENT 0+ and 3- states were not separated in the higher + energy region (Elab=77-88 MeV). +STATUS (CURVE) Data scanned from Fig.2, p1389 in reference +ENDBIB 11 +COMMON 4 3 +ANG ANG-ERR E-LVL2 E-LVL2 +ADEG ADEG MEV MEV + 7.0 0.72 6.049 6.131 +ENDCOMMON 3 +DATA 2 26 +EN-CM DATA-CM +MEV MB/SR + 33.60 0.893 + 33.79 0.978 + 33.98 0.997 + 34.19 1.053 + 34.34 0.920 + 34.49 1.024 + 34.74 0.958 + 34.85 1.052 + 35.03 1.100 + 35.21 1.042 + 35.41 1.108 + 35.56 1.184 + 35.73 1.127 + 35.88 1.089 + 36.07 0.927 + 36.22 0.832 + 36.43 0.736 + 36.56 0.651 + 36.77 0.669 + 36.92 0.593 + 37.13 0.621 + 37.36 0.564 + 37.45 0.535 + 37.68 0.525 + 37.83 0.458 + 37.98 0.335 +ENDDATA 28 +ENDSUBENT 48 +SUBENT E1883005 20050914 20050914 E032 +BIB 5 8 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG is polar angle between beam and 12C in laboratory + system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.919,SPIN=2.,PARITY=+1.) +ADD-RES (COMP) Band-crossing model [T. Matsuse et al., Phys. + Rev. 59(1978)1904] +STATUS (CURVE) Data scanned from Fig.2, p1389 in reference +ENDBIB 8 +COMMON 3 3 +ANG ANG-ERR E-LVL2 +ADEG ADEG MEV + 7.0 0.72 6.919 +ENDCOMMON 3 +DATA 2 150 +EN-CM DATA-CM +MEV MB/SR + 22.65 1.65 + 22.77 1.42 + 22.79 1.07 + 22.91 1.00 + 23.01 0.90 + 23.14 0.86 + 23.26 0.86 + 23.31 1.05 + 23.39 1.29 + 23.44 1.55 + 23.52 1.64 + 23.60 1.82 + 23.70 1.70 + 23.77 1.55 + 23.89 1.39 + 23.97 1.58 + 24.07 1.39 + 24.14 1.38 + 24.27 1.44 + 24.32 1.30 + 24.44 1.12 + 24.51 1.16 + 24.59 1.18 + 24.67 1.30 + 24.82 1.26 + 24.84 1.44 + 24.90 1.77 + 24.97 1.83 + 25.07 1.75 + 25.17 1.52 + 25.22 1.80 + 25.40 1.77 + 25.42 1.54 + 25.52 1.65 + 25.65 1.65 + 25.72 1.51 + 25.77 1.61 + 25.84 1.56 + 25.97 1.45 + 26.04 1.56 + 26.17 1.52 + 26.19 1.43 + 26.32 1.41 + 26.34 1.30 + 26.47 1.24 + 26.56 1.18 + 26.64 1.26 + 26.69 1.36 + 26.79 1.45 + 26.89 1.44 + 26.94 1.62 + 27.05 1.84 + 27.15 1.74 + 27.27 1.57 + 27.39 1.61 + 27.47 1.62 + 27.47 1.52 + 27.59 1.61 + 27.67 1.67 + 27.77 1.61 + 27.85 1.78 + 27.92 1.71 + 28.04 1.61 + 28.14 1.52 + 28.19 1.41 + 28.29 1.48 + 28.34 1.31 + 28.42 1.36 + 28.54 1.32 + 28.59 1.31 + 28.67 1.31 + 28.72 1.37 + 28.77 1.29 + 28.84 1.24 + 28.94 1.32 + 29.02 1.41 + 29.14 1.48 + 29.19 1.42 + 29.34 1.42 + 29.39 1.54 + 29.44 1.62 + 29.52 1.67 + 29.64 1.48 + 29.72 1.31 + 29.79 1.26 + 29.91 1.00 + 29.96 0.83 + 30.06 0.85 + 30.16 0.89 + 30.29 0.83 + 30.29 1.11 + 30.41 1.06 + 30.46 1.12 + 30.57 1.23 + 30.69 1.22 + 30.76 0.89 + 30.86 0.70 + 30.96 0.73 + 31.01 0.83 + 31.11 0.90 + 31.21 0.83 + 31.31 0.84 + 31.36 0.58 + 31.43 0.72 + 31.56 0.71 + 31.63 0.79 + 31.76 0.82 + 31.86 0.82 + 31.88 0.76 + 31.99 0.90 + 32.09 0.92 + 32.13 0.77 + 32.26 0.80 + 32.36 0.63 + 32.41 0.67 + 32.46 0.69 + 32.49 0.86 + 32.58 0.64 + 32.68 0.71 + 32.76 0.73 + 32.86 0.64 + 32.98 0.69 + 33.04 0.84 + 33.21 0.86 + 33.41 0.95 + 33.61 0.95 + 33.79 0.82 + 33.96 0.73 + 34.08 0.63 + 34.21 0.65 + 34.43 0.60 + 34.63 0.56 + 34.81 0.56 + 34.98 0.63 + 35.18 0.54 + 35.33 0.52 + 35.46 0.43 + 35.68 0.33 + 35.85 0.31 + 36.00 0.24 + 36.20 0.18 + 36.38 0.20 + 36.55 0.27 + 36.70 0.25 + 36.95 0.26 + 37.13 0.21 + 37.25 0.18 + 37.43 0.24 + 37.58 0.20 + 37.83 0.20 +ENDDATA 152 +ENDSUBENT 169 +SUBENT E1883006 20050914 20050914 E032 +BIB 4 6 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG is polar angle between beam and 12C in laboratory + system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=7.117,SPIN=1.,PARITY=-1.) +STATUS (CURVE) Data scanned from Fig.2, p1389 in reference +ENDBIB 6 +COMMON 3 3 +ANG ANG-ERR E-LVL2 +ADEG ADEG MEV + 7.0 0.72 7.117 +ENDCOMMON 3 +DATA 2 132 +EN-CM DATA-CM +MEV MB/SR + 22.66 0.113 + 22.79 0.179 + 22.83 0.103 + 22.99 0.122 + 23.04 0.160 + 23.18 0.121 + 23.29 0.159 + 23.37 0.102 + 23.48 0.206 + 23.57 0.149 + 23.67 0.254 + 23.78 0.206 + 23.88 0.206 + 23.94 0.149 + 24.03 0.072 + 24.18 0.110 + 24.28 0.072 + 24.35 0.119 + 24.52 0.157 + 24.64 0.157 + 24.66 0.176 + 24.75 0.242 + 24.83 0.204 + 24.92 0.175 + 25.02 0.156 + 25.11 0.204 + 25.19 0.194 + 25.28 0.156 + 25.38 0.213 + 25.45 0.260 + 25.55 0.298 + 25.66 0.317 + 25.78 0.307 + 25.87 0.269 + 25.97 0.174 + 26.08 0.202 + 26.16 0.154 + 26.23 0.173 + 26.33 0.220 + 26.50 0.163 + 26.54 0.201 + 26.65 0.239 + 26.73 0.201 + 26.90 0.210 + 27.01 0.162 + 27.11 0.210 + 27.18 0.162 + 27.28 0.143 + 27.36 0.152 + 27.51 0.104 + 27.60 0.142 + 27.68 0.104 + 27.79 0.151 + 27.87 0.113 + 27.96 0.075 + 28.04 0.122 + 28.17 0.141 + 28.31 0.160 + 28.46 0.141 + 28.59 0.188 + 28.69 0.121 + 28.78 0.150 + 28.88 0.159 + 28.93 0.216 + 29.05 0.149 + 29.14 0.158 + 29.27 0.215 + 29.43 0.167 + 29.48 0.148 + 29.54 0.205 + 29.71 0.243 + 29.82 0.186 + 29.92 0.148 + 30.04 0.109 + 30.13 0.147 + 30.28 0.099 + 30.30 0.185 + 30.45 0.109 + 30.53 0.194 + 30.64 0.146 + 30.76 0.194 + 30.85 0.213 + 31.00 0.184 + 31.12 0.146 + 31.23 0.164 + 31.34 0.193 + 31.46 0.211 + 31.50 0.192 + 31.59 0.154 + 31.71 0.145 + 31.80 0.192 + 31.93 0.201 + 32.07 0.201 + 32.24 0.191 + 32.33 0.238 + 32.41 0.181 + 32.50 0.200 + 32.58 0.152 + 32.69 0.200 + 32.73 0.238 + 32.85 0.162 + 32.94 0.228 + 33.07 0.237 + 33.11 0.161 + 33.23 0.113 + 33.40 0.132 + 33.61 0.151 + 33.78 0.141 + 33.95 0.103 + 34.14 0.131 + 34.25 0.093 + 34.40 0.140 + 34.65 0.206 + 34.86 0.186 + 35.09 0.158 + 35.18 0.214 + 35.37 0.167 + 35.54 0.147 + 35.75 0.166 + 35.94 0.137 + 36.13 0.108 + 36.30 0.136 + 36.40 0.060 + 36.59 0.098 + 36.80 0.202 + 36.93 0.145 + 37.12 0.202 + 37.25 0.144 + 37.50 0.087 + 37.62 0.134 + 37.86 0.058 + 38.03 0.105 +ENDDATA 134 +ENDSUBENT 149 +SUBENT E1883007 20050914 20050914 E032 +BIB 4 6 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG is polar angle between beam and 12C in laboratory + system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=10.353,SPIN=4.,PARITY=+1.) +STATUS (CURVE) Data scanned from Fig.2, p1389 in reference +ENDBIB 6 +COMMON 3 3 +ANG ANG-ERR E-LVL2 +ADEG ADEG MEV + 7.0 0.72 10.353 +ENDCOMMON 3 +DATA 2 92 +EN-CM DATA-CM +MEV MB/SR + 26.65 1.35 + 26.93 1.28 + 27.05 1.40 + 27.20 1.39 + 27.32 1.36 + 27.53 1.24 + 27.77 1.49 + 27.87 1.75 + 27.92 1.84 + 28.01 1.95 + 28.12 1.85 + 28.19 1.75 + 28.27 1.59 + 28.41 2.05 + 28.53 2.63 + 28.67 2.80 + 28.87 3.06 + 29.02 3.18 + 29.17 3.25 + 29.26 3.31 + 29.37 3.26 + 29.41 3.52 + 29.48 3.61 + 29.61 3.75 + 29.65 4.06 + 29.77 4.09 + 29.78 4.04 + 29.91 3.67 + 30.01 3.52 + 30.09 3.28 + 30.14 3.10 + 30.29 1.98 + 30.36 2.15 + 30.51 2.13 + 30.53 2.28 + 30.60 2.52 + 30.72 2.72 + 30.81 2.24 + 30.86 2.31 + 30.98 2.46 + 31.10 2.87 + 31.15 2.67 + 31.18 2.52 + 31.25 2.50 + 31.35 2.66 + 31.43 2.39 + 31.52 2.80 + 31.62 2.78 + 31.67 2.92 + 31.80 2.92 + 31.82 2.80 + 31.93 2.53 + 32.01 2.41 + 32.08 2.44 + 32.18 2.37 + 32.33 2.44 + 32.41 2.06 + 32.54 2.09 + 32.55 2.46 + 32.66 2.12 + 32.71 1.98 + 32.81 2.27 + 32.91 2.12 + 33.01 2.01 + 33.07 1.73 + 33.29 1.86 + 33.46 1.95 + 33.69 1.80 + 33.87 1.88 + 34.04 1.92 + 34.19 1.92 + 34.32 1.81 + 34.57 1.68 + 34.67 1.76 + 34.84 1.67 + 35.04 1.65 + 35.19 1.65 + 35.45 1.60 + 35.55 1.50 + 35.75 1.50 + 35.95 1.54 + 36.07 1.67 + 36.22 1.56 + 36.45 1.60 + 36.60 1.50 + 36.72 1.37 + 36.97 1.43 + 37.10 1.31 + 37.30 1.35 + 37.45 1.30 + 37.62 1.37 + 37.85 1.42 +ENDDATA 94 +ENDSUBENT 109 +SUBENT E1883008 20050914 20050914 E032 +BIB 4 6 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG is polar angle between beam and 12C in laboratory + system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=11.095,SPIN=4.,PARITY=+1.) +STATUS (CURVE) Data scanned from Fig.2, p1389 in reference +ENDBIB 6 +COMMON 3 3 +ANG ANG-ERR E-LVL2 +ADEG ADEG MEV + 7.0 0.72 11.095 +ENDCOMMON 3 +DATA 2 83 +EN-CM DATA-CM +MEV MB/SR + 27.92 0.29 + 28.07 0.30 + 28.17 0.36 + 28.21 0.42 + 28.31 0.39 + 28.33 0.59 + 28.46 0.65 + 28.61 0.75 + 28.68 0.77 + 28.82 1.07 + 28.95 1.00 + 29.10 1.03 + 29.23 0.94 + 29.33 0.88 + 29.43 0.94 + 29.45 1.03 + 29.55 0.97 + 29.65 0.91 + 29.73 0.83 + 29.83 0.75 + 29.93 0.81 + 29.98 0.70 + 30.11 0.69 + 30.16 0.63 + 30.29 0.45 + 30.36 0.49 + 30.44 0.45 + 30.54 0.35 + 30.61 0.43 + 30.71 0.51 + 30.79 0.35 + 30.86 0.40 + 30.94 0.28 + 31.04 0.34 + 31.11 0.40 + 31.24 0.37 + 31.32 0.31 + 31.49 0.34 + 31.62 0.29 + 31.72 0.27 + 31.79 0.33 + 31.86 0.41 + 31.92 0.35 + 32.04 0.42 + 32.11 0.46 + 32.19 0.54 + 32.28 0.61 + 32.36 0.54 + 32.43 0.70 + 32.53 0.81 + 32.61 0.75 + 32.71 0.72 + 32.80 0.82 + 32.83 0.75 + 32.93 0.73 + 33.06 0.51 + 33.23 0.60 + 33.41 0.49 + 33.59 0.42 + 33.79 0.37 + 33.99 0.37 + 34.19 0.39 + 34.34 0.43 + 34.49 0.33 + 34.72 0.31 + 34.84 0.27 + 35.04 0.30 + 35.22 0.31 + 35.37 0.25 + 35.54 0.23 + 35.69 0.21 + 35.87 0.21 + 36.10 0.15 + 36.25 0.12 + 36.42 0.15 + 36.60 0.13 + 36.80 0.11 + 36.97 0.12 + 37.12 0.18 + 37.32 0.17 + 37.50 0.12 + 37.67 0.17 + 37.82 0.18 +ENDDATA 85 +ENDSUBENT 100 +SUBENT E1883009 20050914 20050914 E032 +BIB 6 8 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.049,SPIN=0.,PARITY=+1.) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 8 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 23.7 6.049 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR MB/SR + 13.0 6.440E-01 3.500E-02 + 13.0 5.920E-01 2.560E-02 + 13.7 8.670E-01 3.750E-02 + 13.9 9.340E-01 5.080E-02 + 13.9 7.960E-01 2.570E-02 + 14.1 7.320E-01 3.170E-02 + 16.0 7.390E-01 4.020E-02 + 16.0 6.650E-01 5.120E-02 + 18.5 4.840E-01 4.280E-02 + 18.5 4.260E-01 3.280E-02 + 20.8 3.140E-01 3.870E-02 + 22.9 2.540E-01 2.540E-02 + 24.6 2.360E-01 2.080E-02 + 26.1 2.700E-01 3.020E-02 + 27.2 3.310E-01 3.310E-02 + 28.9 3.170E-01 2.800E-02 + 31.0 2.700E-01 2.700E-02 + 32.4 3.170E-01 2.800E-02 + 33.1 2.510E-01 2.510E-02 + 35.0 2.190E-01 2.190E-02 + 36.2 1.700E-01 2.100E-02 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1883010 20050914 20050914 E032 +BIB 6 8 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.049,SPIN=0.,PARITY=+1.) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 8 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 24.3 6.049 +ENDCOMMON 3 +DATA 3 18 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR MB/SR + 12.3 4.980E-01 3.560E-02 + 13.0 5.800E-01 5.010E-02 + 14.0 7.530E-01 7.650E-02 + 15.3 9.660E-01 5.490E-02 + 16.5 7.630E-01 4.340E-02 + 17.8 5.710E-01 4.930E-02 + 18.5 3.720E-01 2.110E-02 + 20.0 3.420E-01 2.950E-02 + 21.0 1.910E-01 1.650E-02 + 21.5 2.490E-01 2.150E-02 + 23.0 2.480E-01 1.780E-02 + 24.8 3.230E-01 2.790E-02 + 26.0 3.500E-01 2.510E-02 + 28.0 3.700E-01 3.200E-02 + 29.8 3.360E-01 2.400E-02 + 30.5 2.880E-01 2.490E-02 + 32.8 2.510E-01 1.790E-02 + 35.0 2.310E-01 1.990E-02 +ENDDATA 20 +ENDSUBENT 37 +SUBENT E1883011 20050914 20050914 E032 +BIB 6 8 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.049,SPIN=0.,PARITY=+1.) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 8 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 25.2 6.049 +ENDCOMMON 3 +DATA 3 18 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR MB/SR + 12.1 1.900E-01 1.680E-02 + 13.0 1.310E-01 1.620E-02 + 14.6 1.180E-01 9.050E-03 + 16.3 1.080E-01 1.080E-02 + 16.3 1.850E-01 2.070E-02 + 17.9 1.760E-01 2.590E-02 + 18.8 1.700E-01 2.510E-02 + 20.0 1.580E-01 1.580E-02 + 20.9 1.260E-01 1.560E-02 + 21.5 8.790E-02 1.190E-02 + 22.7 8.070E-02 9.970E-03 + 23.6 6.000E-02 1.110E-02 + 24.9 4.850E-02 1.080E-02 + 26.9 9.040E-02 1.560E-02 + 29.8 1.550E-01 1.370E-02 + 31.6 1.440E-01 1.950E-02 + 33.9 1.120E-01 1.260E-02 + 35.9 1.220E-01 1.660E-02 +ENDDATA 20 +ENDSUBENT 37 +SUBENT E1883012 20050914 20050914 E032 +BIB 6 8 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.049,SPIN=0.,PARITY=+1.) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 8 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 28.2 6.049 +ENDCOMMON 3 +DATA 3 19 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR MB/SR + 12.0 5.350E-01 3.040E-02 + 12.5 4.920E-01 2.800E-02 + 12.8 6.050E-01 1.700E-02 + 14.0 6.580E-01 2.780E-02 + 14.0 6.060E-01 1.700E-02 + 15.0 4.120E-01 2.340E-02 + 15.5 3.390E-01 2.930E-02 + 16.3 2.180E-01 1.240E-02 + 17.5 1.680E-01 1.200E-02 + 18.3 1.440E-01 1.680E-02 + 20.0 1.440E-01 1.250E-02 + 20.3 1.750E-01 9.950E-03 + 20.8 1.660E-01 2.300E-03 + 21.8 2.340E-01 1.330E-02 + 22.5 3.260E-01 2.820E-02 + 24.5 3.500E-01 1.990E-02 + 26.5 3.360E-01 3.920E-02 + 28.8 1.800E-01 2.110E-02 + 31.3 1.660E-01 1.190E-02 +ENDDATA 21 +ENDSUBENT 38 +SUBENT E1883013 20050914 20050914 E032 +BIB 5 7 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.131,SPIN=3.,PARITY=-1.) +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 7 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 23.7 6.131 +ENDCOMMON 3 +DATA 2 16 +ANG-CM DATA-CM +ADEG MB/SR + 15.3 1.930E+00 + 16.4 1.700E+00 + 16.6 1.550E+00 + 18.6 1.500E+00 + 20.6 1.370E+00 + 22.6 1.090E+00 + 24.8 8.320E-01 + 26.1 6.380E-01 + 27.9 5.730E-01 + 29.5 5.320E-01 + 30.8 4.980E-01 + 32.2 4.530E-01 + 33.8 4.330E-01 + 34.7 4.970E-01 + 36.2 4.660E-01 + 38.0 3.810E-01 +ENDDATA 18 +ENDSUBENT 34 +SUBENT E1883014 20050914 20050914 E032 +BIB 5 7 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.131,SPIN=3.,PARITY=-1.) +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 7 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 24.3 6.131 +ENDCOMMON 3 +DATA 2 18 +ANG-CM DATA-CM +ADEG MB/SR + 10.8 1.500E+00 + 12.1 1.400E+00 + 13.3 1.500E+00 + 14.1 1.600E+00 + 15.1 1.730E+00 + 16.7 2.070E+00 + 17.4 2.210E+00 + 19.2 2.270E+00 + 19.9 1.980E+00 + 21.1 1.770E+00 + 22.9 1.590E+00 + 24.1 1.400E+00 + 26.6 1.240E+00 + 27.8 1.040E+00 + 28.7 9.420E-01 + 31.2 9.790E-01 + 32.7 9.650E-01 + 33.3 1.020E+00 +ENDDATA 20 +ENDSUBENT 36 +SUBENT E1883015 20050914 20050914 E032 +BIB 5 7 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.131,SPIN=3.,PARITY=-1.) +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 7 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 25.2 6.131 +ENDCOMMON 3 +DATA 2 17 +ANG-CM DATA-CM +ADEG MB/SR + 14.2 3.480E+00 + 15.8 3.510E+00 + 16.8 3.660E+00 + 18.2 3.360E+00 + 19.1 4.070E+00 + 20.0 4.290E+00 + 21.1 4.470E+00 + 22.4 4.470E+00 + 23.6 4.520E+00 + 24.1 3.930E+00 + 25.0 3.360E+00 + 27.3 2.570E+00 + 29.8 2.190E+00 + 31.8 2.860E+00 + 33.7 3.310E+00 + 35.8 3.240E+00 + 37.9 2.280E+00 +ENDDATA 19 +ENDSUBENT 35 +SUBENT E1883016 20050914 20050914 E032 +BIB 5 7 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.131,SPIN=3.,PARITY=-1.) +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 7 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 28.2 6.131 +ENDCOMMON 3 +DATA 2 14 +ANG-CM DATA-CM +ADEG MB/SR + 11.6 1.690E+00 + 12.6 1.760E+00 + 14.6 1.880E+00 + 15.1 1.520E+00 + 16.3 1.460E+00 + 17.1 1.130E+00 + 18.3 7.740E-01 + 19.3 6.260E-01 + 20.3 5.590E-01 + 21.6 6.080E-01 + 23.8 8.860E-01 + 25.6 8.600E-01 + 28.3 5.960E-01 + 30.3 3.690E-01 +ENDDATA 16 +ENDSUBENT 32 +SUBENT E1883017 20050914 20050914 E032 +BIB 5 7 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.919,SPIN=2.,PARITY=+1.) +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 7 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 23.7 6.919 +ENDCOMMON 3 +DATA 2 16 +ANG-CM DATA-CM +ADEG MB/SR + 13.7 2.300E+00 + 14.8 1.600E+00 + 15.0 1.910E+00 + 17.2 2.030E+00 + 19.3 2.340E+00 + 21.1 2.540E+00 + 23.6 2.350E+00 + 25.3 1.700E+00 + 26.5 1.160E+00 + 28.1 1.240E+00 + 28.9 1.440E+00 + 30.8 1.570E+00 + 32.5 1.650E+00 + 33.0 1.440E+00 + 35.5 1.480E+00 + 37.1 1.370E+00 +ENDDATA 18 +ENDSUBENT 34 +SUBENT E1883018 20050914 20050914 E032 +BIB 5 7 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.919,SPIN=2.,PARITY=+1.) +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 7 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 24.3 6.919 +ENDCOMMON 3 +DATA 2 17 +ANG-CM DATA-CM +ADEG MB/SR + 13.3 2.430E+00 + 15.0 1.790E+00 + 15.7 1.460E+00 + 16.9 1.990E+00 + 18.1 2.300E+00 + 18.8 2.530E+00 + 19.8 2.740E+00 + 21.2 2.970E+00 + 22.4 2.630E+00 + 23.4 2.400E+00 + 25.1 2.010E+00 + 27.0 1.760E+00 + 28.9 1.760E+00 + 29.9 1.910E+00 + 31.3 1.960E+00 + 33.2 1.990E+00 + 35.6 2.130E+00 +ENDDATA 19 +ENDSUBENT 35 +SUBENT E1883019 20050914 20050914 E032 +BIB 5 7 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.919,SPIN=2.,PARITY=+1.) +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 7 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 25.2 6.919 +ENDCOMMON 3 +DATA 2 15 +ANG-CM DATA-CM +ADEG MB/SR + 13.7 2.490E+00 + 15.5 2.290E+00 + 16.2 2.490E+00 + 17.9 2.550E+00 + 18.3 2.740E+00 + 19.9 2.910E+00 + 20.8 2.740E+00 + 22.7 2.630E+00 + 23.8 2.350E+00 + 27.2 2.300E+00 + 29.2 2.330E+00 + 30.9 2.010E+00 + 33.2 1.820E+00 + 35.7 1.840E+00 + 38.0 1.730E+00 +ENDDATA 17 +ENDSUBENT 33 +SUBENT E1883020 20050914 20050914 E032 +BIB 5 7 +REACTION (6-C-12(8-O-16,INL)6-C-12,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 12C in center + of mass system + (E-LVL2,8-O-16) +LEVEL-PROP (8-O-16,E-LVL=6.919,SPIN=2.,PARITY=+1.) +ADD-RES (COMP) S-matrix theory +STATUS (CURVE) Data scanned from Fig.7, p1395 in reference +ENDBIB 7 +COMMON 2 3 +EN-CM E-LVL2 +MEV MEV + 28.2 6.919 +ENDCOMMON 3 +DATA 2 14 +ANG-CM DATA-CM +ADEG MB/SR + 16.2 1.540E+00 + 17.5 1.630E+00 + 18.6 1.540E+00 + 19.3 1.330E+00 + 20.5 1.290E+00 + 21.7 1.200E+00 + 22.6 1.120E+00 + 23.8 1.080E+00 + 25.0 1.050E+00 + 25.7 1.170E+00 + 27.5 1.440E+00 + 30.1 1.220E+00 + 32.2 1.040E+00 + 34.6 9.690E-01 +ENDDATA 16 +ENDSUBENT 32 +ENDENTRY 20 diff --git a/exforall/E18/E1884.x4 b/exforall/E18/E1884.x4 new file mode 100644 index 000000000..844e86d1d --- /dev/null +++ b/exforall/E18/E1884.x4 @@ -0,0 +1,370 @@ +ENTRY E1884 20050914 20050914 E032 +SUBENT E1884001 20050914 20050914 E032 +BIB 12 27 +TITLE Spectroscopic tool for proton-rich nuclei: The + (3He,6He) reaction +AUTHOR (S.Kubono, N.Ikeda, T.Nomura, Y.Fuchi, H.Kawashima, + S.Kato, H.Miyatake, H.Orihara) +INSTITUTE (2JPNTOK) Institute for Nuclear Study + (2JPNYMG) Physics Department + (2JPNOSA) College of General Education + (2JPNTOH) Cyclotron-Radioisotope Center +REFERENCE (J,PR/C,43,(4),1821,199104) +PART-DET (2-HE-6) +INC-SOURCE Beam intensity is 0.5 to 1.0 micro-Ampere. +SAMPLE - Target enrichment is unknown. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Backing is unknown. +METHOD (EDE) + (TOF) +FACILITY (CYCLO,2JPNTOK) Sector-focusing cyclotron at Institute + for Nuclear Study +DETECTOR Solid angle of detector is 5.0 msr. + (MAGSP) To analyze momentum of 6He. QDD-type + high-resolution magnetic spectrograph [S.Kato + et al., Nucl. Instrum. Methods 154(1978)19] + (PROPC) To detect 6He [M.H. Tanaka et al., Nucl. + Instrum. Methods 195(1982)509] +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +HISTORY (20040413C) Kc + On +ENDBIB 27 +COMMON 1 3 +EN +MEV + 73.71 +ENDCOMMON 3 +ENDSUBENT 34 +SUBENT E1884002 20050914 20050914 E032 +BIB 6 13 +REACTION (12-MG-24(HE3,2-HE-6)12-MG-21,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 6He in center + of mass system + (E-LVL,12-MG-21) +LEVEL-PROP (12-MG-21,E-LVL=0.0,SPIN=2.5,PARITY=+1.) +MISC-COL (MISC1) Polar angle between beam and 6He in lab. + system. + (MISC2) Transferred orbital angular momentum +ADD-RES (COMP) DWBA (Distorted wave Born approximation) (xact + finite-range DWBA calculations using the code + TWOFNR [M.Igarashi, unpublished]) +STATUS (TABLE) Data (Fig.1, p1822 in reference) received by + mail from S.Kubono (2004.04.13) +ENDBIB 13 +COMMON 2 3 +E-LVL MISC2 +MEV NO-DIM + 0.0 2.0 +ENDCOMMON 3 +DATA 4 14 +ANG-CM MISC1 DATA-CM DATA-ERR +ADEG ADEG NB/SR NB/SR + 7.5 6.0 541.643 16.797 + 8.8 7.0 519.934 16.648 + 10.6 8.5 403.822 14.555 + 12.5 10.0 423.520 14.784 + 13.8 11.0 417.646 14.739 + 15.0 12.0 298.539 13.147 + 16.3 13.0 317.108 12.981 + 17.5 14.0 308.006 12.684 + 20.0 16.0 246.995 9.845 + 22.5 18.0 186.763 8.537 + 24.9 20.0 152.677 7.792 + 27.4 22.0 158.705 7.965 + 31.1 25.0 103.972 8.262 + 34.8 28.0 69.842 6.951 +ENDDATA 16 +ENDSUBENT 38 +SUBENT E1884003 20050914 20050914 E032 +BIB 5 12 +REACTION (12-MG-24(HE3,2-HE-6)12-MG-21,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 6He in center + of mass system + (E-LVL,12-MG-21) +MISC-COL (MISC1) Polar angle between beam and 6He in lab. + system. + (MISC2) Transferred orbital angular momentum +ADD-RES (COMP) DWBA (Distorted wave Born approximation) (xact + finite-range DWBA calculations using the code + TWOFNR [M.Igarashi, unpublished]) +STATUS (TABLE) Data (Fig.1, p1822 in reference) received by + mail from S.Kubono (2004.04.13) +ENDBIB 12 +COMMON 2 3 +E-LVL MISC2 +MEV NO-DIM + 0.208 0.0 +ENDCOMMON 3 +DATA 4 14 +ANG-CM MISC1 DATA-CM DATA-ERR +ADEG ADEG NB/SR NB/SR + 7.4 6.0 32.458 4.737 + 8.8 7.0 25.472 4.439 + 10.6 8.5 31.015 4.502 + 12.5 10.0 48.599 5.326 + 13.8 11.0 40.646 4.942 + 15.0 12.0 37.738 5.131 + 16.3 13.0 31.209 4.330 + 17.5 14.0 24.703 3.839 + 20.0 16.0 34.857 3.841 + 22.5 18.0 50.080 4.518 + 25.0 20.0 50.310 4.586 + 27.4 22.0 37.298 3.955 + 31.1 25.0 35.405 5.021 + 34.8 28.0 10.309 2.844 +ENDDATA 16 +ENDSUBENT 37 +SUBENT E1884004 20050914 20050914 E032 +BIB 5 12 +REACTION (12-MG-24(HE3,2-HE-6)12-MG-21,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 6He in center + of mass system + (E-LVL,12-MG-21) +MISC-COL (MISC1) Polar angle between beam and 6He in lab. + system. + (MISC2) Transferred orbital angular momentum +ADD-RES (COMP) DWBA (Distorted wave Born approximation) (xact + finite-range DWBA calculations using the code + TWOFNR [M.Igarashi, unpublished]) +STATUS (TABLE) Data (Fig.1, p1822 in reference) received by + mail from S.Kubono (2004.04.13) +ENDBIB 12 +COMMON 2 3 +E-LVL MISC2 +MEV NO-DIM + 1.089 1.0 +ENDCOMMON 3 +DATA 4 14 +ANG-CM MISC1 DATA-CM DATA-ERR +ADEG ADEG NB/SR NB/SR + 7.5 6.0 302.182 9.865 + 8.8 7.0 243.585 11.690 + 10.7 8.5 143.393 8.976 + 12.6 10.0 70.812 6.347 + 13.8 11.0 72.921 6.531 + 15.1 12.0 56.615 6.278 + 16.3 13.0 66.135 6.298 + 17.6 14.0 81.794 6.714 + 20.0 16.0 124.978 7.137 + 22.5 18.0 111.691 6.673 + 25.0 20.0 111.079 6.693 + 27.5 22.0 104.184 6.529 + 31.2 25.0 87.815 7.720 + 34.9 28.0 51.919 6.097 +ENDDATA 16 +ENDSUBENT 37 +SUBENT E1884005 20050914 20050914 E032 +BIB 4 9 +REACTION (12-MG-24(HE3,2-HE-6)12-MG-21,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 6He in center + of mass system + (E-LVL,12-MG-21) +MISC-COL (MISC1) Polar angle between beam and 6He in lab. + system. + (MISC2) Transferred orbital angular momentum +STATUS (TABLE) Data (Fig.2, p1822 in reference) received by + mail from S.Kubono (2004.04.13) +ENDBIB 9 +COMMON 2 3 +E-LVL MISC2 +MEV NO-DIM + 1.651 1.0 +ENDCOMMON 3 +DATA 4 14 +ANG-CM MISC1 DATA-CM DATA-ERR +ADEG ADEG NB/SR NB/SR + 7.5 6.0 259.112 9.202 + 8.8 7.0 213.086 11.114 + 10.7 8.5 141.454 8.961 + 12.6 10.0 84.509 6.870 + 13.8 11.0 84.144 6.881 + 15.1 12.0 83.029 7.240 + 16.3 13.0 111.878 7.944 + 17.6 14.0 116.055 7.909 + 20.1 16.0 148.393 7.694 + 22.6 18.0 109.478 6.568 + 25.1 20.0 105.858 6.480 + 27.5 22.0 109.154 6.693 + 31.2 25.0 96.483 7.968 + 35.0 28.0 102.323 8.187 +ENDDATA 16 +ENDSUBENT 34 +SUBENT E1884006 20050914 20050914 E032 +BIB 4 9 +REACTION (12-MG-24(HE3,2-HE-6)12-MG-21,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 6He in center + of mass system + (E-LVL,12-MG-21) +MISC-COL (MISC1) Polar angle between beam and 6He in lab. + system. + (MISC2) Transferred orbital angular momentum +STATUS (TABLE) Data (Fig.2, p1822 in reference) received by + mail from S.Kubono (2004.04.13) +ENDBIB 9 +COMMON 3 3 +E-LVL E-LVL MISC2 +MEV MEV NO-DIM + 1.998 2.048 1.0 +ENDCOMMON 3 +DATA 4 14 +ANG-CM MISC1 DATA-CM DATA-ERR +ADEG ADEG NB/SR NB/SR + 7.6 6.0 248.810 9.081 + 8.8 7.0 198.088 10.721 + 10.7 8.5 164.757 9.594 + 12.6 10.0 120.608 8.110 + 13.8 11.0 104.393 7.572 + 15.1 12.0 112.700 8.341 + 16.3 13.0 98.738 7.513 + 17.6 14.0 110.380 7.721 + 20.1 16.0 136.650 7.445 + 22.6 18.0 142.512 7.471 + 25.1 20.0 134.554 7.297 + 27.6 22.0 133.499 7.361 + 31.3 25.0 120.718 8.999 + 35.0 28.0 112.386 8.605 +ENDDATA 16 +ENDSUBENT 34 +SUBENT E1884007 20050914 20050914 E032 +BIB 4 8 +REACTION (12-MG-24(HE3,2-HE-6)12-MG-21,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 6He in center + of mass system + (E-LVL,12-MG-21) +MISC-COL (MISC1) Polar angle between beam and 6He in lab. + system. +STATUS (TABLE) Data (not shown in reference) received by mail + from S.Kubono (2004.04.13) +ENDBIB 8 +COMMON 1 3 +E-LVL +MEV + 3.086 +ENDCOMMON 3 +DATA 4 14 +ANG-CM MISC1 DATA-CM DATA-ERR +ADEG ADEG NB/SR NB/SR + 7.6 6.0 25.600 4.177 + 8.8 7.0 9.341 3.109 + 10.7 8.5 10.833 2.871 + 12.6 10.0 17.262 3.309 + 13.9 11.0 8.892 2.660 + 15.1 12.0 18.845 3.730 + 16.4 13.0 8.920 2.527 + 17.7 14.0 13.919 3.064 + 20.2 16.0 13.285 2.530 + 22.7 18.0 11.123 2.542 + 25.2 20.0 17.534 2.817 + 27.7 22.0 14.617 2.570 + 31.4 25.0 5.920 2.293 + 35.1 28.0 8.974 2.676 +ENDDATA 16 +ENDSUBENT 33 +SUBENT E1884008 20050914 20050914 E032 +BIB 4 8 +REACTION (12-MG-24(HE3,2-HE-6)12-MG-21,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 6He in center + of mass system + (E-LVL,12-MG-21) +MISC-COL (MISC1) Polar angle between beam and 6He in lab. + system. +STATUS (TABLE) Data (not shown in reference) received by mail + from S.Kubono (2004.04.13) +ENDBIB 8 +COMMON 1 3 +E-LVL +MEV + 3.244 +ENDCOMMON 3 +DATA 4 14 +ANG-CM MISC1 DATA-CM DATA-ERR +ADEG ADEG NB/SR NB/SR + 7.6 6.0 72.745 6.217 + 8.8 7.0 60.472 5.900 + 10.7 8.5 61.060 5.743 + 12.6 10.0 33.538 4.356 + 13.9 11.0 39.519 4.712 + 15.1 12.0 29.075 4.407 + 16.4 13.0 49.555 5.150 + 17.7 14.0 42.188 4.838 + 20.2 16.0 54.246 4.638 + 22.7 18.0 38.188 4.061 + 25.2 20.0 30.917 3.592 + 27.7 22.0 41.603 4.089 + 31.4 25.0 23.642 3.965 + 35.1 28.0 17.921 3.534 +ENDDATA 16 +ENDSUBENT 33 +SUBENT E1884009 20050914 20050914 E032 +BIB 5 12 +REACTION (12-MG-24(HE3,2-HE-6)12-MG-21,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 6He in center + of mass system + (E-LVL,12-MG-21) +MISC-COL (MISC1) Polar angle between beam and 6He in lab. + system. + (MISC2) Transferred orbital angular momentum +ADD-RES (COMP) DWBA (Distorted wave Born approximation) (xact + finite-range DWBA calculations using the code + TWOFNR [M.Igarashi, unpublished]) +STATUS (TABLE) Data (Fig.1, p1822 in reference) received by + mail from S.Kubono (2004.04.13) +ENDBIB 12 +COMMON 2 3 +E-LVL MISC2 +MEV NO-DIM + 3.347 4.0 +ENDCOMMON 3 +DATA 4 14 +ANG-CM MISC1 DATA-CM DATA-ERR +ADEG ADEG NB/SR NB/SR + 7.6 6.0 23.102 4.023 + 8.8 7.0 27.979 4.335 + 10.7 8.5 40.806 4.792 + 12.6 10.0 54.659 5.417 + 13.9 11.0 55.732 5.492 + 15.1 12.0 32.792 4.624 + 16.4 13.0 36.671 4.487 + 17.7 14.0 37.714 4.656 + 20.2 16.0 18.054 2.854 + 22.7 18.0 20.730 3.163 + 25.2 20.0 25.702 3.311 + 27.7 22.0 14.243 2.542 + 31.4 25.0 16.549 3.395 + 35.1 28.0 17.921 3.534 +ENDDATA 16 +ENDSUBENT 37 +SUBENT E1884010 20050914 20050914 E032 +BIB 4 6 +REACTION (12-MG-24(HE3,2-HE-6)12-MG-21,PAR,DA) +EN-SEC ANG-CM is polar angle between beam and 6He in center + of mass system + (E-LVL,12-MG-21) +MISC-COL (MISC) Transferred orbital angular momentum +STATUS (CURVE) Data scanned from Fig.2, p1822 in reference +ENDBIB 6 +COMMON 2 3 +E-LVL MISC +MEV NO-DIM + 3.752 1.0 +ENDCOMMON 3 +DATA 3 14 +ANG-CM DATA-CM DATA-ERR +ADEG NB/SR NB/SR + 7.532E+00 4.923E+01 5.091E+00 + 8.875E+00 1.822E+01 3.746E+00 + 1.062E+01 1.317E+01 3.023E+00 + 1.255E+01 6.359E+00 2.439E+00 + 1.378E+01 1.735E+01 3.566E+00 + 1.512E+01 1.217E+01 3.395E+00 + 1.623E+01 1.217E+01 2.942E+00 + 1.763E+01 1.304E+01 3.152E+00 + 2.014E+01 1.330E+01 2.577E+00 + 2.265E+01 1.933E+01 3.075E+00 + 2.505E+01 1.081E+01 2.614E+00 + 2.756E+01 7.227E+00 2.292E+00 + 3.129E+01 6.359E+00 2.439E+00 + 3.521E+01 1.572E+01 3.993E+00 +ENDDATA 16 +ENDSUBENT 31 +ENDENTRY 10 diff --git a/exforall/E18/E1885.x4 b/exforall/E18/E1885.x4 new file mode 100644 index 000000000..eeecf75a7 --- /dev/null +++ b/exforall/E18/E1885.x4 @@ -0,0 +1,121 @@ +ENTRY E1885 20050914 20050914 E032 +SUBENT E1885001 20050914 20050914 E032 +BIB 11 29 +TITLE Half-life of 228Pu and alpha decay of 228Np +AUTHOR (K.Nishio, H.Ikezoe, S.Mitsuoka, K.Satou, C.J.Lin) +INSTITUTE (2JPNJAE) Advanced Science Research Center + (3CPRAEP) +REFERENCE (J,PR/C,68,(6),064305,200312) +INC-SOURCE Beam intensity is 40 to 50 particle-nA. +INC-SPECT EN: Energy at the half depth of the target layer + determined by calculating the energy loss of beam in + the Al foil and target +SAMPLE - Target enrichment is 98%. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 0.39 mg/cm**2. + - Backing is aluminium. + - Backing-thickness: 1.2 micro-meter thick foil +FACILITY (VDGT,2JPNJAE) +DETECTOR (MAGSP) JAERI Recoil Mass Separator used to separate + evaporation residue from the primary beams and + other reaction products. + (SI) Double-sided position-sensitive silicon detector + (73x55 mm**2) to construct alpha-decay chain. + Typical energy resolution of PSD for alpha + particle from an 241Am source. +ADD-RES E1885.005:78-PT-198(16-S-34,4N)94-PU-228 + 78-PT-198(16-S-34,3N+P)93-NP-228 + 78-PT-198(16-S-34,3N+A)92-U-225 + Half life time + See NRDF D1885 DATA,4 for detail. +HISTORY (20040413C) Kc + On +ENDBIB 29 +NOCOMMON 0 0 +ENDSUBENT 32 +SUBENT E1885002 20050914 20050914 E032 +BIB 6 19 +REL-REF (N,,R.B.Firestone,B,FIRESTONE,,1996) + Kinetic energy of alpha particles and half-life of + this literature are tabulated for other than 228Pu. + (N,,A.N.Andreyev+,J,ZP/A,347,(3),225,199409) + Kinetic energy of alpha particles and half-life of + this literature are tabulated for 228Pu. +REACTION (78-PT-198(16-S-34,4N)94-PU-228,,SIG) + Upper limit of cross section is obtained when + candidate of decay chain was not observed +DECAY-DATA (94-PU-228,,A,7810.) + (92-U-224,0.9MSEC,A,8466.) + (90-TH-220,9.7MICROSEC,A,8790.) + (88-RA-216,0.18MICROSEC,A,9349.) + (86-RN-212,23.9MIN,A,6264.) +ERR-ANALYS (ERR-S) Statistical uncertainty +COMMENT T1/2 (228Pu) = 1.1+2.0-0.5 sec is determined by + authors. +STATUS (TABLE) Data (Fig.3, p064305-5 in reference) received + by e-mail from K.Nishio (2004.04.13) +ENDBIB 19 +NOCOMMON 0 0 +DATA 5 2 +EN-CM DATA DATA-MAX +ERR-S -ERR-S +MEV NB NB NB NB + 141.0 1.791 2.162 1.267 + 143.0 0.8834 +ENDDATA 4 +ENDSUBENT 28 +SUBENT E1885003 20050914 20050914 E032 +BIB 6 19 +REL-REF (N,,R.B.Firestone,B,FIRESTONE,,1996) + Kinetic energy of alpha particles and half-life of + this literature are tabulated for other than 228Np. + (N,,S.A.Kreek+,J,PR/C,50,(5),2288,199411) + Kinetic energy of alpha particles and half-life of + this literature are tabulated for 228Np. +REACTION (78-PT-198(16-S-34,3N+P)93-NP-228,,SIG) + Upper limit of cross section is obtained when + candidate of decay chain was not observed +DECAY-DATA (93-NP-228,61.4SEC,A) + (91-PA-224,0.79SEC,A,7488.,0.70) + (89-AC-220,26.4MSEC,A,7855.,0.26) + (87-FR-216,0.7MICROSEC,A,9005.) + (85-AT-212-G,0.314SEC,A,7679.,0.82) + (85-AT-212-G,0.314SEC,A,7045.,0.0045) +ERR-ANALYS (ERR-S) Statistical uncertainty +COMMENT T1/2 (228Np) = 56+45-17 sec is determined by authors. +STATUS (TABLE) Data (Fig.3, p064305-5 in reference) received + by e-mail from K.Nishio (2004.04.13) +ENDBIB 19 +NOCOMMON 0 0 +DATA 5 2 +EN-CM DATA DATA-MAX +ERR-S -ERR-S +MEV NB NB NB NB + 141.0 1.234 + 143.0 6.083 3.937 2.721 +ENDDATA 4 +ENDSUBENT 28 +SUBENT E1885004 20050914 20050914 E032 +BIB 6 13 +REL-REF (N,,R.B.Firestone,B,FIRESTONE,,1996) + Kinetic energy of alpha particles and half-life of + this literature are tabulated. +REACTION (78-PT-198(16-S-34,3N+A)92-U-225,,SIG) +DECAY-DATA (92-U-225,95.MSEC,A,7879.,0.85) + (92-U-225,95.MSEC,A,7821.,0.15) + (90-TH-221,1.68MSEC,A,8472.,0.39) + (90-TH-221,1.68MSEC,A,8146.,0.56) + (86-RN-213,25.MSEC,A,8088.) +ERR-ANALYS (ERR-S) Statistical uncertainty +COMMENT T1/2 (225U) = 135+93-39 msec is determined by authors. +STATUS (TABLE) Data (Fig.3, p064305-5 in reference) received + by e-mail from K.Nishio (2004.04.13) +ENDBIB 13 +NOCOMMON 0 0 +DATA 4 2 +EN-CM DATA +ERR-S -ERR-S +MEV NB NB NB + 141.0 5.537 4.153 2.769 + 143.0 2.731 3.296 1.931 +ENDDATA 4 +ENDSUBENT 22 +NOSUBENT E1885005 20050914 20050914 E032 +ENDENTRY 5 diff --git a/exforall/E18/E1886.x4 b/exforall/E18/E1886.x4 new file mode 100644 index 000000000..e15d0c826 --- /dev/null +++ b/exforall/E18/E1886.x4 @@ -0,0 +1,1120 @@ +ENTRY E1886 20050914 20050914 E032 +SUBENT E1886001 20050914 20050914 E032 +BIB 12 112 +TITLE Systematic study of L<=3 giant resonances in Sm + isotopes via multipole decomposition analysis +AUTHOR (M.Itoh, H.Sakaguchi, M.Uchida, T.Ishikawa, T.Kawabata, + T.Murakami, H.Takeda, T.Taki, S.Terashima, + N.Tsukahara, Y.Yasuda, M.Yosoi, U.Garg, M.Hedden, + B.Kharraja, M.Koss, B.K.Nayak, S.Zhu, H.Fujimura, + M.Fujiwara, K.Hara, H.P.Yoshida, H.Akimune, + M.N.Harakeh, M.Volkerts) +INSTITUTE (2JPNKTO) Department of Physics + (1USANOT) Physics Department + (2JPNOSA) Research Center for Nuclear Physics (RCNP) + (2JPNJAE) Advanced Science Research Center + (2JPNKON) Department of Physics + (2NEDKVI) +REFERENCE (J,PR/C,68,(6),064602,200312) + (T,Itoh,79,200301) + Numerical data for double differential cross section +PART-DET (A) +INC-SOURCE - Beam intensity is 1 to 20 nA. + - Charge of incident ion is +2. +SAMPLE - Target enrichment is unknown. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 2 to 10 mg/cm**2. + - Target is self supported. +METHOD Ray-tracing technique was used to reconstruct the + horizontal scattering angle. +FACILITY (CYCLO,2JPNOSA) AVF cyclotron and ring cyclotron at + Research Center for Nuclear Physics + (RCNP) +DETECTOR (MAGSP) To analyze inelastically scattered particles. + Grand Raiden [M.Fujiwara et al., Nucl. + Instrum. Methods Phys. Res. A 422(1999)484] + (MWDC) To measure alpha particle in focal plane + (SCIN) Plastic scintillation counter to generate + trigger signals and to identify alpha particles +ADD-RES E1886.023:62-SM-144(A,INL)62-SM-144 + Strength function + See NRDF D1886 DATA,22 for detail. + E1886.024:62-SM-144(A,INL)62-SM-144 + Strength function + See NRDF D1886 DATA,23 for detail. + E1886.025:62-SM-144(A,INL)62-SM-144 + Strength function + See NRDF D1886 DATA,24 for detail. + E1886.026:62-SM-144(A,INL)62-SM-144 + Strength function + See NRDF D1886 DATA,25 for detail. + E1886.027:62-SM-148(A,INL)62-SM-148 + Strength function + See NRDF D1886 DATA,26 for detail. + E1886.028:62-SM-148(A,INL)62-SM-148 + Strength function + See NRDF D1886 DATA,27 for detail. + E1886.029:62-SM-148(A,INL)62-SM-148 + Strength function + See NRDF D1886 DATA,28 for detail. + E1886.030:62-SM-148(A,INL)62-SM-148 + Strength function + See NRDF D1886 DATA,29 for detail. + E1886.031:62-SM-150(A,INL)62-SM-150 + Strength function + See NRDF D1886 DATA,30 for detail. + E1886.032:62-SM-150(A,INL)62-SM-150 + Strength function + See NRDF D1886 DATA,31 for detail. + E1886.033:62-SM-150(A,INL)62-SM-150 + Strength function + See NRDF D1886 DATA,32 for detail. + E1886.034:62-SM-150(A,INL)62-SM-150 + Strength function + See NRDF D1886 DATA,33 for detail. + E1886.035:62-SM-152(A,INL)62-SM-152 + Strength function + See NRDF D1886 DATA,34 for detail. + E1886.036:62-SM-152(A,INL)62-SM-152 + Strength function + See NRDF D1886 DATA,35 for detail. + E1886.037:62-SM-152(A,INL)62-SM-152 + Strength function + See NRDF D1886 DATA,36 for detail. + E1886.038:62-SM-152(A,INL)62-SM-152 + Strength function + See NRDF D1886 DATA,37 for detail. + E1886.039:62-SM-154(A,INL)62-SM-154 + Strength function + See NRDF D1886 DATA,38 for detail. + E1886.040:62-SM-154(A,INL)62-SM-154 + Strength function + See NRDF D1886 DATA,39 for detail. + E1886.041:62-SM-154(A,INL)62-SM-154 + Strength function + See NRDF D1886 DATA,40 for detail. + E1886.042:62-SM-154(A,INL)62-SM-154 + Strength function + See NRDF D1886 DATA,41 for detail. + E1886.043:62-SM-144(A,INL)62-SM-144 + Energy weighted sum rule + See NRDF D1886 DATA,42 for detail. + E1886.044:62-SM-148(A,INL)62-SM-148 + Energy weighted sum rule + See NRDF D1886 DATA,43 for detail. + E1886.045:62-SM-150(A,INL)62-SM-150 + Energy weighted sum rule + See NRDF D1886 DATA,44 for detail. + E1886.046:62-SM-152(A,INL)62-SM-152 + Energy weighted sum rule + See NRDF D1886 DATA,45 for detail. + E1886.047:62-SM-154(A,INL)62-SM-154 + Energy weighted sum rule + See NRDF D1886 DATA,46 for detail. +HISTORY (20050402C) Kc + Sr + On +ENDBIB 112 +COMMON 1 3 +EN +MEV + 386.0 +ENDCOMMON 3 +ENDSUBENT 119 +SUBENT E1886002 20050914 20050914 E032 +BIB 4 7 +REACTION (62-SM-144(A,INL)62-SM-144,,DA/DE,A/RSD) +EN-SEC ANG-CM is varies from 0.70 deg (at 8.5 MeV) to 0.68 + deg (at 32.5 MeV) + (E-EXC,62-SM-144) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data (Fig. 4, p064602-4 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 7 +COMMON 1 3 +ANG-CM +ADEG + 0.7 +ENDCOMMON 3 +DATA 3 25 +E-EXC DATA-CM DATA-ERR +MEV MB/SR/MEV MB/SR/MEV + 8.5 41.704 0.983 + 9.5 47.303 0.761 + 10.5 54.619 0.915 + 11.5 75.753 0.905 + 12.5 97.215 0.811 + 13.5 118.630 0.912 + 14.5 145.780 1.173 + 15.5 148.630 1.033 + 16.5 104.080 0.981 + 17.5 70.428 0.728 + 18.5 56.359 0.627 + 19.5 50.297 0.584 + 20.5 46.753 0.600 + 21.5 47.687 0.575 + 22.5 49.597 0.514 + 23.5 47.315 0.628 + 24.5 45.165 0.588 + 25.5 42.281 0.538 + 26.5 39.968 0.531 + 27.5 37.305 0.525 + 28.5 34.716 0.522 + 29.5 32.929 0.536 + 30.5 30.842 0.551 + 31.5 30.912 0.539 + 32.5 29.351 0.548 +ENDDATA 27 +ENDSUBENT 43 +SUBENT E1886003 20050914 20050914 E032 +BIB 4 7 +REACTION (62-SM-148(A,INL)62-SM-148,,DA/DE,A/RSD) +EN-SEC ANG-CM is varies from 0.70 deg (at 8.5 MeV) to 0.68 + deg (at 32.5 MeV) + (E-EXC,62-SM-148) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data (Fig. 4, p064602-4 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 7 +COMMON 1 3 +ANG-CM +ADEG + 0.7 +ENDCOMMON 3 +DATA 3 25 +E-EXC DATA-CM DATA-ERR +MEV MB/SR/MEV MB/SR/MEV + 8.5 60.243 0.699 + 9.5 62.805 0.685 + 10.5 76.623 0.691 + 11.5 98.299 0.712 + 12.5 115.530 0.728 + 13.5 130.010 0.745 + 14.5 138.190 0.773 + 15.5 128.170 0.791 + 16.5 93.612 0.768 + 17.5 69.089 0.730 + 18.5 58.574 0.707 + 19.5 53.729 0.687 + 20.5 52.100 0.684 + 21.5 53.631 0.695 + 22.5 52.999 0.700 + 23.5 51.100 0.699 + 24.5 48.402 0.686 + 25.5 44.541 0.657 + 26.5 41.511 0.629 + 27.5 37.610 0.605 + 28.5 36.810 0.598 + 29.5 35.057 0.595 + 30.5 33.337 0.598 + 31.5 31.601 0.601 + 32.5 32.541 0.602 +ENDDATA 27 +ENDSUBENT 43 +SUBENT E1886004 20050914 20050914 E032 +BIB 4 7 +REACTION (62-SM-150(A,INL)62-SM-150,,DA/DE,A/RSD) +EN-SEC ANG-CM is varies from 0.70 deg (at 8.5 MeV) to 0.68 + deg (at 32.5 MeV) + (E-EXC,62-SM-150) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data (Fig. 4, p064602-4 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 7 +COMMON 1 3 +ANG-CM +ADEG + 0.7 +ENDCOMMON 3 +DATA 3 25 +E-EXC DATA-CM DATA-ERR +MEV MB/SR/MEV MB/SR/MEV + 8.5 62.770 0.756 + 9.5 71.959 0.748 + 10.5 89.273 0.756 + 11.5 111.490 0.780 + 12.5 127.050 0.794 + 13.5 138.280 0.812 + 14.5 139.060 0.835 + 15.5 128.160 0.854 + 16.5 99.235 0.833 + 17.5 72.978 0.791 + 18.5 66.416 0.767 + 19.5 58.996 0.745 + 20.5 55.730 0.742 + 21.5 56.896 0.750 + 22.5 56.961 0.760 + 23.5 54.189 0.754 + 24.5 50.323 0.741 + 25.5 48.259 0.710 + 26.5 41.949 0.677 + 27.5 40.609 0.655 + 28.5 38.246 0.647 + 29.5 37.422 0.642 + 30.5 36.137 0.647 + 31.5 35.560 0.651 + 32.5 33.892 0.650 +ENDDATA 27 +ENDSUBENT 43 +SUBENT E1886005 20050914 20050914 E032 +BIB 4 7 +REACTION (62-SM-152(A,INL)62-SM-152,,DA/DE,A/RSD) +EN-SEC ANG-CM is Varies from 0.70 deg (at 8.5 MeV) to 0.68 + deg (at 32.5 MeV) + (E-EXC,62-SM-152) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data (Fig. 4, p064602-4 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 7 +COMMON 1 3 +ANG-CM +ADEG + 0.7 +ENDCOMMON 3 +DATA 3 25 +E-EXC DATA-CM DATA-ERR +MEV MB/SR/MEV MB/SR/MEV + 8.5 64.538 0.600 + 9.5 78.254 0.597 + 10.5 99.433 0.607 + 11.5 119.960 0.624 + 12.5 130.190 0.630 + 13.5 129.000 0.635 + 14.5 130.110 0.652 + 15.5 125.850 0.677 + 16.5 100.710 0.664 + 17.5 75.263 0.629 + 18.5 62.013 0.605 + 19.5 56.855 0.588 + 20.5 53.752 0.582 + 21.5 54.447 0.589 + 22.5 51.712 0.593 + 23.5 50.405 0.591 + 24.5 46.412 0.579 + 25.5 44.538 0.557 + 26.5 40.498 0.529 + 27.5 39.284 0.515 + 28.5 35.795 0.506 + 29.5 35.636 0.502 + 30.5 32.469 0.507 + 31.5 32.103 0.510 + 32.5 30.876 0.509 +ENDDATA 27 +ENDSUBENT 43 +SUBENT E1886006 20050914 20050914 E032 +BIB 4 7 +REACTION (62-SM-154(A,INL)62-SM-154,,DA/DE,A/RSD) +EN-SEC ANG-CM is Varies from 0.70 deg (at 8.5 MeV) to 0.68 + deg (at 32.5 MeV) + (E-EXC,62-SM-154) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data (Fig. 4, p064602-4 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 7 +COMMON 1 3 +ANG-CM +ADEG + 0.7 +ENDCOMMON 3 +DATA 3 25 +E-EXC DATA-CM DATA-ERR +MEV MB/SR/MEV MB/SR/MEV + 8.5 64.268 1.239 + 9.5 84.250 1.309 + 10.5 105.750 1.343 + 11.5 127.790 1.353 + 12.5 129.790 1.368 + 13.5 126.870 1.331 + 14.5 128.090 1.289 + 15.5 125.310 1.258 + 16.5 102.810 1.191 + 17.5 74.838 1.120 + 18.5 62.431 1.085 + 19.5 54.915 1.066 + 20.5 54.703 1.065 + 21.5 50.330 1.066 + 22.5 49.634 1.063 + 23.5 47.123 1.052 + 24.5 44.322 1.050 + 25.5 39.839 1.044 + 26.5 38.296 1.039 + 27.5 35.035 1.036 + 28.5 33.842 1.026 + 29.5 32.835 1.035 + 30.5 32.796 1.030 + 31.5 30.882 1.030 + 32.5 28.470 1.028 +ENDDATA 27 +ENDSUBENT 43 +SUBENT E1886007 20050914 20050914 E032 +BIB 5 7 +REACTION (62-SM-144(A,EL)62-SM-144,,DA) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 5, p064602-4 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 7 +NOCOMMON 0 0 +DATA 3 59 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR MB/SR + 2.76 223400.000 6713.000 + 3.17 82680.000 2491.000 + 3.57 35230.000 1068.000 + 3.98 30100.000 913.700 + 4.38 26500.000 801.300 + 4.79 18060.000 542.600 + 5.20 8374.000 252.200 + 5.61 2164.000 65.880 + 5.91 466.100 14.670 + 6.22 571.600 18.080 + 6.32 1297.000 39.620 + 6.73 2438.000 73.840 + 7.14 2566.000 77.680 + 7.45 1587.000 47.760 + 7.55 1758.000 53.450 + 7.86 694.200 20.960 + 8.27 151.800 4.684 + 8.68 96.820 3.034 + 9.09 290.000 8.832 + 9.50 452.200 13.660 + 9.91 414.100 12.510 + 10.33 256.800 7.794 + 10.74 113.400 3.492 + 11.15 44.340 1.418 + 11.56 54.740 1.712 + 11.97 89.680 2.761 + 12.38 100.200 3.076 + 12.79 82.130 2.535 + 13.21 50.800 1.594 + 13.62 21.950 0.738 + 14.03 15.220 0.534 + 14.44 16.230 0.565 + 14.85 20.740 0.701 + 15.26 20.530 0.695 + 15.67 14.600 0.475 + 16.09 10.060 0.338 + 16.50 6.113 0.218 + 16.91 4.104 0.157 + 17.32 4.068 0.156 + 17.73 4.195 0.155 + 18.14 3.920 0.146 + 18.55 3.061 0.120 + 18.96 2.165 0.092 + 19.38 1.331 0.065 + 19.79 0.946 0.054 + 20.20 0.888 0.052 + 20.61 0.791 0.048 + 21.02 0.764 0.047 + 21.43 0.632 0.042 + 21.84 0.398 0.027 + 22.25 0.272 0.021 + 22.67 0.199 0.018 + 23.08 0.174 0.017 + 23.49 0.161 0.016 + 23.90 0.118 0.013 + 24.31 0.111 0.012 + 24.72 0.079 0.010 + 25.13 0.062 0.009 + 25.54 0.037 0.007 +ENDDATA 61 +ENDSUBENT 73 +SUBENT E1886008 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-144(A,INL)62-SM-144,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-144) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 12.5 0.5 +ENDCOMMON 3 +DATA 3 34 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.70 97.215 0.811 + 1.49 71.458 1.200 + 2.04 61.538 0.781 + 2.42 67.743 0.803 + 2.81 73.827 0.777 + 3.01 71.586 0.774 + 3.21 70.483 0.794 + 3.41 60.229 0.729 + 3.81 46.044 0.644 + 4.21 36.022 0.557 + 4.51 32.542 0.391 + 4.91 35.235 0.458 + 5.31 36.222 0.498 + 5.71 32.555 0.390 + 6.01 24.219 0.276 + 6.42 17.256 0.234 + 6.82 13.835 0.209 + 7.22 13.012 0.201 + 7.53 12.970 0.199 + 7.93 13.613 0.204 + 8.33 12.586 0.197 + 8.74 10.046 0.175 + 9.04 8.151 0.159 + 9.44 6.218 0.140 + 9.85 5.626 0.134 + 10.25 5.924 0.134 + 10.55 5.531 0.123 + 10.96 5.409 0.123 + 11.36 4.243 0.109 + 11.77 3.453 0.098 + 12.07 2.829 0.077 + 12.47 2.533 0.073 + 12.88 2.315 0.071 + 13.28 2.152 0.068 +ENDDATA 36 +ENDSUBENT 53 +SUBENT E1886009 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-144(A,INL)62-SM-144,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-144) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 15.5 0.5 +ENDCOMMON 3 +DATA 3 34 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.69 148.630 1.033 + 1.49 78.145 1.319 + 2.03 54.494 0.762 + 2.41 52.874 0.702 + 2.80 55.757 0.710 + 3.00 54.494 0.670 + 3.20 55.317 0.734 + 3.40 51.598 0.649 + 3.79 42.762 0.620 + 4.19 33.828 0.519 + 4.49 29.856 0.372 + 4.89 29.695 0.373 + 5.29 29.200 0.373 + 5.69 27.603 0.451 + 5.99 21.003 0.286 + 6.39 17.177 0.234 + 6.79 13.558 0.207 + 7.19 11.877 0.193 + 7.49 11.374 0.186 + 7.89 11.158 0.186 + 8.30 10.778 0.181 + 8.70 9.109 0.167 + 9.00 7.428 0.151 + 9.40 5.945 0.135 + 9.80 5.476 0.132 + 10.21 5.290 0.128 + 10.51 4.597 0.113 + 10.91 4.236 0.108 + 11.31 3.783 0.103 + 11.71 3.147 0.093 + 12.02 2.587 0.074 + 12.42 2.475 0.073 + 12.82 2.348 0.071 + 13.22 1.924 0.064 +ENDDATA 36 +ENDSUBENT 53 +SUBENT E1886010 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-144(A,INL)62-SM-144,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-144) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 24.5 0.5 +ENDCOMMON 3 +DATA 3 34 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.69 45.165 0.588 + 1.47 42.521 1.089 + 2.00 33.937 0.700 + 2.38 31.427 0.615 + 2.77 29.427 0.547 + 2.96 27.762 0.467 + 3.16 28.016 0.572 + 3.35 27.869 0.463 + 3.74 27.802 0.497 + 4.14 25.239 0.468 + 4.43 23.815 0.308 + 4.83 20.711 0.315 + 5.22 18.294 0.298 + 5.62 16.717 0.282 + 5.91 15.301 0.216 + 6.31 13.617 0.205 + 6.70 11.993 0.201 + 7.10 10.507 0.229 + 7.40 9.694 0.186 + 7.79 8.190 0.161 + 8.19 7.220 0.150 + 8.59 6.860 0.145 + 8.88 6.195 0.139 + 9.28 5.557 0.133 + 9.68 4.914 0.124 + 10.08 4.124 0.113 + 10.37 3.498 0.098 + 10.77 3.340 0.096 + 11.17 3.040 0.093 + 11.56 2.526 0.085 + 11.86 2.403 0.071 + 12.26 2.062 0.066 + 12.65 1.817 0.062 + 13.05 1.542 0.058 +ENDDATA 36 +ENDSUBENT 53 +SUBENT E1886011 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-148(A,INL)62-SM-148,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-148) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 12.5 0.5 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.70 115.530 0.728 + 2.03 70.013 0.929 + 2.42 73.094 0.918 + 2.81 76.150 0.923 + 3.01 75.093 0.861 + 3.21 69.955 0.870 + 3.41 65.747 0.798 + 3.80 51.728 0.715 + 4.20 42.901 0.650 + 4.50 41.172 1.374 + 4.90 40.255 1.527 + 5.30 37.884 1.486 + 5.71 32.900 1.135 + 6.01 26.036 0.332 + 6.41 18.505 0.280 + 6.81 14.749 0.251 + 7.22 14.006 0.244 + 7.52 14.443 0.220 + 7.92 13.729 0.215 + 8.32 11.646 0.198 + 8.73 8.718 0.171 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1886012 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-148(A,INL)62-SM-148,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-148) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 15.5 0.5 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.69 128.170 0.791 + 2.03 55.623 0.870 + 2.41 54.714 0.792 + 2.80 58.532 0.819 + 3.00 58.295 0.751 + 3.19 56.132 0.781 + 3.39 51.999 0.708 + 3.79 44.678 0.661 + 4.19 35.680 0.587 + 4.48 30.809 0.506 + 4.88 30.829 1.067 + 5.28 28.884 1.034 + 5.68 25.632 1.244 + 5.98 20.630 0.711 + 6.38 17.709 0.276 + 6.79 13.659 0.243 + 7.19 12.605 0.230 + 7.49 11.738 0.198 + 7.89 11.741 0.199 + 8.29 10.279 0.186 + 8.69 8.719 0.171 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1886013 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-148(A,INL)62-SM-148,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-148) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 24.5 0.5 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.69 48.402 0.686 + 2.00 35.351 0.791 + 2.38 33.966 0.665 + 2.77 32.116 0.629 + 2.96 33.478 0.585 + 3.15 31.769 0.602 + 3.35 33.147 0.576 + 3.74 33.658 0.572 + 4.13 29.569 0.542 + 4.43 27.883 0.486 + 4.82 24.109 0.484 + 5.22 21.280 0.464 + 5.61 19.524 0.453 + 5.91 18.285 0.283 + 6.30 15.676 0.262 + 6.70 12.815 0.484 + 7.09 11.468 0.529 + 7.39 9.521 0.342 + 7.79 8.750 0.172 + 8.18 8.102 0.165 + 8.58 7.732 0.161 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1886014 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-150(A,INL)62-SM-150,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-150) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 12.5 0.5 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.70 127.050 0.794 + 2.03 78.685 2.122 + 2.42 82.130 2.183 + 2.81 81.352 2.197 + 3.01 75.114 1.227 + 3.21 71.196 1.954 + 3.40 62.410 1.107 + 3.80 51.015 1.034 + 4.20 42.410 0.910 + 4.50 39.814 1.474 + 4.90 38.496 1.665 + 5.30 41.262 1.575 + 5.71 31.614 1.125 + 6.01 24.350 0.450 + 6.41 18.799 0.400 + 6.81 15.576 0.367 + 7.21 14.559 0.349 + 7.52 14.766 0.277 + 7.92 13.772 0.270 + 8.32 11.880 0.249 + 8.72 8.998 0.217 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1886015 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-150(A,INL)62-SM-150,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-150) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 15.5 0.5 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.69 128.160 0.854 + 2.02 59.388 1.671 + 2.41 58.461 1.627 + 2.80 59.582 1.645 + 3.00 57.292 1.300 + 3.19 55.371 1.554 + 3.39 53.305 1.061 + 3.79 43.870 0.920 + 4.18 34.414 0.845 + 4.48 30.802 0.650 + 4.88 31.014 1.002 + 5.28 30.544 1.309 + 5.68 24.546 1.462 + 5.98 21.156 0.781 + 6.38 17.516 0.386 + 6.78 14.280 0.350 + 7.18 12.330 0.322 + 7.48 12.182 0.253 + 7.89 11.729 0.246 + 8.29 10.486 0.234 + 8.69 8.748 0.213 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1886016 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-150(A,INL)62-SM-150,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-150) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 24.5 0.5 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.68 50.323 0.741 + 2.00 40.606 1.286 + 2.38 36.144 1.103 + 2.77 35.150 1.058 + 2.96 34.310 5.500 + 3.15 32.282 1.000 + 3.35 34.821 2.331 + 3.74 33.196 1.154 + 4.13 29.022 2.497 + 4.43 28.166 0.704 + 4.82 24.484 0.750 + 5.21 22.670 1.097 + 5.61 20.165 1.491 + 5.91 17.668 0.388 + 6.30 15.225 0.517 + 6.70 13.966 0.629 + 7.09 11.477 0.591 + 7.39 10.002 0.381 + 7.79 9.393 0.224 + 8.18 8.503 0.212 + 8.58 7.623 0.201 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1886017 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-152(A,INL)62-SM-152,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-152) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 12.5 0.5 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.70 130.190 0.630 + 2.03 72.486 0.887 + 2.42 74.087 0.895 + 2.81 75.189 0.886 + 3.01 70.746 0.883 + 3.21 67.604 0.816 + 3.40 59.324 0.809 + 3.80 46.169 0.693 + 4.20 37.733 0.631 + 4.50 36.000 0.993 + 4.90 37.174 1.053 + 5.30 33.964 0.956 + 5.70 28.757 0.443 + 6.00 22.067 0.368 + 6.41 17.712 0.331 + 6.81 15.188 0.307 + 7.21 13.975 0.293 + 7.51 13.629 0.199 + 7.92 12.560 0.190 + 8.32 10.803 0.176 + 8.72 8.647 0.158 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1886018 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-152(A,INL)62-SM-152,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-152) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 15.5 0.5 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.69 125.850 0.677 + 2.02 53.699 0.798 + 2.41 53.278 0.764 + 2.80 55.485 0.761 + 3.00 52.587 0.849 + 3.19 52.902 0.735 + 3.39 47.437 0.788 + 3.79 40.978 0.663 + 4.18 32.732 0.602 + 4.48 30.255 0.445 + 4.88 29.917 0.454 + 5.28 29.732 0.859 + 5.68 24.898 0.743 + 5.98 20.599 0.609 + 6.38 16.489 0.316 + 6.78 13.693 0.291 + 7.18 12.366 0.277 + 7.48 11.317 0.180 + 7.88 11.116 0.179 + 8.28 9.842 0.168 + 8.69 8.206 0.153 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1886019 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-152(A,INL)62-SM-152,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-152) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 24.5 0.5 +ENDCOMMON 3 +DATA 3 21 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.68 46.412 0.579 + 2.00 34.561 0.759 + 2.38 32.633 0.726 + 2.76 30.395 0.664 + 2.96 30.104 0.603 + 3.15 31.049 0.639 + 3.35 29.200 0.601 + 3.74 27.197 0.590 + 4.13 26.051 0.543 + 4.42 24.427 0.404 + 4.82 21.980 0.406 + 5.21 19.978 0.394 + 5.61 18.129 0.381 + 5.90 15.860 0.312 + 6.30 14.351 0.297 + 6.69 12.808 0.413 + 7.09 9.876 0.349 + 7.39 9.343 0.273 + 7.78 8.249 0.154 + 8.18 7.371 0.146 + 8.57 6.718 0.139 +ENDDATA 23 +ENDSUBENT 40 +SUBENT E1886020 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-154(A,INL)62-SM-154,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-154) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 12.5 0.5 +ENDCOMMON 3 +DATA 3 22 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.69 129.790 1.368 + 1.49 105.060 2.854 + 2.03 78.785 1.024 + 2.42 78.089 0.950 + 2.81 77.917 0.976 + 3.01 76.374 0.860 + 3.20 68.897 0.862 + 3.40 67.807 0.799 + 3.80 55.178 0.728 + 4.20 46.629 0.656 + 4.50 45.389 1.479 + 4.90 42.845 1.534 + 5.30 42.428 1.530 + 5.70 35.297 1.175 + 6.00 25.100 0.333 + 6.40 20.382 0.302 + 6.81 16.675 0.273 + 7.21 14.940 0.258 + 7.51 11.907 0.183 + 7.91 11.165 0.177 + 8.32 9.549 0.164 + 8.72 7.349 0.144 +ENDDATA 24 +ENDSUBENT 41 +SUBENT E1886021 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-154(A,INL)62-SM-154,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-154) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 15.5 0.5 +ENDCOMMON 3 +DATA 3 22 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.69 125.310 1.258 + 1.48 82.216 2.352 + 2.02 57.002 0.876 + 2.41 55.987 0.814 + 2.80 58.151 0.800 + 2.99 56.302 0.720 + 3.19 53.219 0.768 + 3.39 53.280 0.689 + 3.78 45.009 0.673 + 4.18 37.694 0.595 + 4.48 34.584 0.482 + 4.88 32.695 0.480 + 5.28 33.210 1.123 + 5.68 30.963 1.260 + 5.98 22.610 0.799 + 6.38 19.247 0.295 + 6.78 14.800 0.257 + 7.18 12.605 0.237 + 7.48 10.019 0.168 + 7.88 9.973 0.168 + 8.28 9.028 0.160 + 8.68 7.456 0.144 +ENDDATA 24 +ENDSUBENT 41 +SUBENT E1886022 20050914 20050914 E032 +BIB 5 8 +REACTION (62-SM-154(A,INL)62-SM-154,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,62-SM-154) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 6, p064602-5 in reference) taken + from doctoral thesis of M. Itoh +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 24.5 0.5 +ENDCOMMON 3 +DATA 3 22 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.68 44.322 1.050 + 1.47 39.791 1.919 + 2.00 36.036 0.823 + 2.38 34.360 0.673 + 2.76 32.259 0.643 + 2.96 32.831 0.628 + 3.15 29.548 0.595 + 3.35 33.863 0.559 + 3.74 32.216 0.549 + 4.13 30.335 0.523 + 4.42 29.039 0.443 + 4.82 26.758 0.433 + 5.21 23.243 0.404 + 5.60 20.930 0.383 + 5.90 17.479 0.280 + 6.30 16.106 0.271 + 6.69 13.708 0.498 + 7.09 11.657 0.534 + 7.38 8.500 0.299 + 7.78 7.409 0.145 + 8.18 6.802 0.139 + 8.57 6.143 0.132 +ENDDATA 24 +ENDSUBENT 41 +NOSUBENT E1886023 20050914 20050914 E032 +NOSUBENT E1886024 20050914 20050914 E032 +NOSUBENT E1886025 20050914 20050914 E032 +NOSUBENT E1886026 20050914 20050914 E032 +NOSUBENT E1886027 20050914 20050914 E032 +NOSUBENT E1886028 20050914 20050914 E032 +NOSUBENT E1886029 20050914 20050914 E032 +NOSUBENT E1886030 20050914 20050914 E032 +NOSUBENT E1886031 20050914 20050914 E032 +NOSUBENT E1886032 20050914 20050914 E032 +NOSUBENT E1886033 20050914 20050914 E032 +NOSUBENT E1886034 20050914 20050914 E032 +NOSUBENT E1886035 20050914 20050914 E032 +NOSUBENT E1886036 20050914 20050914 E032 +NOSUBENT E1886037 20050914 20050914 E032 +NOSUBENT E1886038 20050914 20050914 E032 +NOSUBENT E1886039 20050914 20050914 E032 +NOSUBENT E1886040 20050914 20050914 E032 +NOSUBENT E1886041 20050914 20050914 E032 +NOSUBENT E1886042 20050914 20050914 E032 +NOSUBENT E1886043 20050914 20050914 E032 +NOSUBENT E1886044 20050914 20050914 E032 +NOSUBENT E1886045 20050914 20050914 E032 +NOSUBENT E1886046 20050914 20050914 E032 +NOSUBENT E1886047 20050914 20050914 E032 +ENDENTRY 47 diff --git a/exforall/E18/E1887.x4 b/exforall/E18/E1887.x4 new file mode 100644 index 000000000..b150602c5 --- /dev/null +++ b/exforall/E18/E1887.x4 @@ -0,0 +1,66 @@ +ENTRY E1887 20050914 20050914 E032 +SUBENT E1887001 20050914 20050914 E032 +BIB 14 43 +TITLE Half-life of the electron capture decaying isotope + 236Am +AUTHOR (K.Tsukada, S.Ichikawa, Y.Hatsukawa, I.Nishinaka, + K.Hata, Y.Nagame, Y.Oura, T.Ohyama, K.Sueki, + H.Nakahara, M.Asai, Y.Kojima, T.Hirose, H.Yamamoto, + K.Kawade) +INSTITUTE (2JPNJAE) + (2JPNTMU) Department of Chemistry + (2JPNNAG) Department of Energy Engineering and Science +REFERENCE (J,PR/C,57,(4),2057,199804) +REL-REF (A,,H.L.Hall,R,LBL-27878,1989) + Half-life of 236Am obtained by 237Np(3He,4n) is + 3.73+-0.28 min in this work. +DECAY-DATA (95-AM-236,4.4MIN,XR) + Decay data for Pu K(alpha 1) X-ray in present + experiment. T1/2= 4.4+-1.0 min. + (95-AM-236,4.5MIN,XR) + Decay data for Pu K(alpha 2) X-ray in present + experiment. T1/2= 4.5+-1.5 min. +INC-SOURCE - Beam intensity is 100 to 300 particle-nA. + - Charge of incident ion is 3+. +SAMPLE - Target enrichment is 93%. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 0.2 mg/cm**2. + - Backing is aluminium. Electrodeposited + - Backing-thickness is 0.8 mg/cm**2. +METHOD (STTA) Stack of fifteen 235U targets was bombarded. + (HEJET) Products attached to KCL clusters were swept + out of the target chamber with He gas + (OLMS) JAERI-ISOL [S. Ichikawa et al., Nucl. Instrum. + Meth. A374(1996)330]. Mass resolution A/Delta-A + is about 600 for 221Fr. +FACILITY (VDGT,2JPNJAE) +ANALYSIS (DECAY) Decay curves for Pu K(alpha 1) and Pu + K(alpha2) X-ray. Evaluated half-life of 236Am + is 4.4+-0.8 min. +DETECTOR (GELI) Planartype Ge detector (FWHM= 0.57 keV at 122 + keV) + (HPGE) Coaxial n-type Ge detector (FWHM= 1.8 keV at + 1.33 MeV) +STATUS (TABLE) Data taken from text, p2059 in reference +HISTORY (20040415C) Kc + On +ENDBIB 43 +COMMON 2 3 +EN-MIN EN-MAX +MEV MEV + 46.0 50.0 +ENDCOMMON 3 +ENDSUBENT 50 +SUBENT E1887002 20050914 20050914 E032 +BIB 1 2 +REACTION (92-U-235(3-LI-6,5N)95-AM-236,,SIG,,AV) + Average for incident energy range +ENDBIB 2 +NOCOMMON 0 0 +DATA 1 1 +DATA-APRX +MICRO-B + 70.0 +ENDDATA 3 +ENDSUBENT 10 +ENDENTRY 2 diff --git a/exforall/E18/E1888.x4 b/exforall/E18/E1888.x4 new file mode 100644 index 000000000..7cf99e21a --- /dev/null +++ b/exforall/E18/E1888.x4 @@ -0,0 +1,155 @@ +ENTRY E1888 20050914 20050914 E032 +SUBENT E1888001 20050914 20050914 E032 +BIB 12 36 +TITLE alpha-decays of neutron-deficient americium isotopes +AUTHOR (M.Sakama, M.Asai, K.Tsukada, S.Ichikawa, I.Nishinaka, + Y.Nagame, H.Haba, S.Goto, M.Shibata, K.Kawade, + Y.Kojima, Y.Oura, M.Ebihara, H.Nakahara) +INSTITUTE (2JPNTKS) Department of Radiologic Science and + Engineering, School of Health Sciences + (2JPNJAE) Advanced Science Research Center + (2JPNIPC) Cyclotron Center + (2JPNNII) Department of Chemistry + (2JPNNAG) Radioisotope Research Center + (2JPNNAG) Department of Energy Engineering and Science + (2JPNHIR) Graduate School of Engineering + (2JPNTMU) Department of Chemistry +REFERENCE (J,PR/C,69,(1),014308,200401) +INC-SOURCE Beam intensity is 250 to 340 particle-nA. +SAMPLE - Target enrichment is unknown. + - Chemical-form of target: UO2(NO3)2 + - Backing is aluminium. UO2(NO3)2 in 2-propanol is + electrodeposited onto aluminum backing foil. + - Backing-thickness is 0.9 mg/cm**2. +METHOD (STTA) A stack of 21 targets set in a multiple-target + chamber with 5 mm spacing + (HEJET) Products attached to the PbI2 aerosol clusters + were swept out of the target chamber + (OLMS) JAERI-ISOL. Mass resolution of A/Delta A is + about 850 at the mass number A=208 [S. Ichikawa + et al., Nucl. Instrum. Methods B187(2002)548]. +FACILITY (VDGT,2JPNJAE) +ANALYSIS (DECAY) +DETECTOR (SI) To measure alpha particles with efficiency of + 85%. Energy resolution is about 45 keV. + (GELI) To measure X rays following EC decay. Coaxial + type. FWHM= 0.66 keV at 122 keV gamma-ray. +STATUS (TABLE) Data taken from Table 1, p014308-7 in + reference +HISTORY (20040414C) Kc + On +ENDBIB 36 +NOCOMMON 0 0 +ENDSUBENT 39 +SUBENT E1888002 20050914 20050914 E032 +BIB 5 11 +REL-REF (D,,H.L.Hall+,R,LBL-27878,1989) + Energy and intensity of alpha for 236Am are 6410 keV + and (4.2+-0.6)e-4 in this work. +REACTION (92-U-235(3-LI-6,5N)95-AM-236,,SIG,,AV) +DECAY-DATA (95-AM-236,3.1MIN,A,6150.,4.0E-5) + Decay data in present experiment. T1/2= 3.1+-1.3 min + and intensity I=(4.0+-1.0)e-5. + (95-AM-236,3.6MIN,XR) + Decay data in present experiment. T1/2= 3.6+-0.1 min. +SAMPLE Target-thickness is 0.16 to 0.42 mg/cm**2. +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ENDBIB 11 +COMMON 2 3 +EN-MIN EN-MAX +MEV MEV + 39.0 48.0 +ENDCOMMON 3 +DATA 2 1 +DATA DATA-ERR +MICRO-B MICRO-B + 125.0 46.0 +ENDDATA 3 +ENDSUBENT 23 +SUBENT E1888003 20050914 20050914 E032 +BIB 7 17 +REL-REF (A,,J.Guo+,J,ZP/A,355,(2),111,199607) + Half-life of 235Am is 15+-5 min in this work. +REACTION (92-U-233(3-LI-6,4N)95-AM-235,,SIG,,AV) +DECAY-DATA (95-AM-235,10.7MIN,A,6457.,4.0E-3) + Decay data in present experiment. T1/2= 10.7+-0.7 min + and intensity I=(4.0+-0.5)e-3. + (95-AM-235,9.5MIN,XR) + Decay data in present experiment. T1/2= 9.5+-1.2 min. +SAMPLE Target-thickness is 0.05 to 0.13 mg/cm**2. +DETECTOR (GE) Used for alpha-gamma and gamma-gamma coincidence + measurements. +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +COMMENT Comment by authors: No alpha-gamma coincidence event + was observed. This result suggests that the level fed + by the 6457 keV alpha transition is either the ground + state of 231Np or a low lying level that decays via + internal conversion. +ENDBIB 17 +COMMON 2 3 +EN-MIN EN-MAX +MEV MEV + 34.0 42.0 +ENDCOMMON 3 +DATA 2 1 +DATA DATA-ERR +MICRO-B MICRO-B + 31.0 12.0 +ENDDATA 3 +ENDSUBENT 29 +SUBENT E1888004 20050914 20050914 E032 +BIB 7 14 +REL-REF (D,,H.L.Hall+,J,PR/C,41,(2),618,199002) + Energy and intensity of alpha for 234Am are 6460 keV + and (3.9+-1.2)e-4 in this work. +REACTION (92-U-233(3-LI-6,5N)95-AM-234,,SIG,,AV) +DECAY-DATA (95-AM-234,,A) + The 6.46 MeV alpha group for 234Am reported by Hall is + not observed. + (95-AM-234,3.5MIN,XR) + Decay data in present experiment. T1/2= 3.5+-1.3 min. +RAD-DET (94-PU-234,A) +SAMPLE Target-thickness is 0.05 to 0.13 mg/cm**2. +METHOD (COINC) Detect alphas in coincidence. Alpha chain from + 234Pu to 210Pb is detected. +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ENDBIB 14 +COMMON 2 3 +EN-MIN EN-MAX +MEV MEV + 39.0 48.0 +ENDCOMMON 3 +DATA 2 1 +DATA DATA-ERR +MICRO-B MICRO-B + 9.0 5.0 +ENDDATA 3 +ENDSUBENT 26 +SUBENT E1888005 20050914 20050914 E032 +BIB 5 14 +REL-REF (A,,R.L.Hahn+,J,NP/A,113,(1),206,196805) + Half-life, alpha energy and abundance of 229Np is + 4.0+-0.2 min, 6890+-20 keV, and larger than 0.50, + respectively, in this work. +REACTION (92-U-233(3-LI-6,6N)95-AM-233,,SIG,,AV) +DECAY-DATA (95-AM-233,3.2MIN,A,6780.) + Decay data in present experiment. T1/2= 3.2+-0.8 min + and intensity I>3e-2. + (93-NP-229,4.0MIN,A,6893.,0.68) + Decay data in present experiment. T1/2= 4.0+-0.4 min + and intensity I= 0.68+-0.11. +SAMPLE Target-thickness is 0.05 to 0.13 mg/cm**2. +METHOD (COINC) Detect alphas in coincidence. Alpha chain from + 225Pa to 213At is detected. +ENDBIB 14 +COMMON 2 3 +EN-MIN EN-MAX +MEV MEV + 52.0 60.0 +ENDCOMMON 3 +DATA 1 1 +DATA-MAX +MICRO-B + 0.9 +ENDDATA 3 +ENDSUBENT 26 +ENDENTRY 5 diff --git a/exforall/E18/E1889.x4 b/exforall/E18/E1889.x4 new file mode 100644 index 000000000..e521ce0ee --- /dev/null +++ b/exforall/E18/E1889.x4 @@ -0,0 +1,245 @@ +ENTRY E1889 20050914 20050914 E032 +SUBENT E1889001 20050914 20050914 E032 +BIB 10 34 +TITLE One-neutron halo structure in 15C +AUTHOR (D.Q.Fang, T.Yamaguchi, T.Zheng, A.Ozawa, M.Chiba, + R.Kanungo, T.Kato, K.Morimoto, T.Ohnishi, T.Suda, + Y.Yamaguchi, A.Yoshida, K.Yoshida, I.Tanihata) +INSTITUTE (2JPNIPC) + (3CPRNRS) + (3CPRBJG) Department of Technical Physics + (2JPNTOH) Department of Physics + (2JPNNII) Department of Physics +REFERENCE (J,PR/C,69,(3),034613,200403) +REL-REF (N,E1791001,T.Zheng+,J,NP/A,709,(1-4),103,200210) + Reaction cross sectons for 12C and 16C beams obtained + in this work are compared with those for 14C and 15C + beams obtained in present work. Detailed description + of the method to obtain reaction cross section is also + found in this reference. +SAMPLE - Target enrichment is unknown. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Backing is unknown. +METHOD (TOF) To identify particle and to determine + longitudinal momentum distributions + (EDE) To identify particle with ToF +FACILITY (CYCLO,2JPNIPC) Primary beam of 110 MeV/A 22Ne was + used to bombard on a Be target to + produce the secondary beams of 14,15C. + (PRJFS,2JPNIPC) RIKEN Projectile fragment Separator + (RIPS) +DETECTOR (PPAC) To monitor beam size and emittance angle + (SCIN) To give ToF signal + (SI) To measure energy loss (Delta E) + (NAICR) To measure total energy (E) with energy + resolution of 0.7% in FWHM for 110 MeV/A 22Ne +HISTORY (20040415C) Kc + On +ENDBIB 34 +NOCOMMON 0 0 +ENDSUBENT 37 +SUBENT E1889002 20050914 20050914 E032 +BIB 6 10 +REACTION (6-C-12(6-C-15,X)6-C-14,LP,DP) +PART-DET (6-C-14) +MOM-SEC (MOM-SEC,6-C-14) + Longitudinal momemtum in projectile rest frame +MISC-COL (MISC) FWHM of gaussian fit to longitudinal momentum + distribution +ERR-ANALYS (ERR-T) Statistical error as well as error arising + from background subtraction +STATUS (TABLE) Data (Fig.3a, p034613-3 in reference) received + by e-mail from D.Q.Fang (2004.04.19) +ENDBIB 10 +COMMON 3 3 +EN MISC MISC-ERR +MEV/A MEV/C MEV/C + 83.0 71.0 9.0 +ENDCOMMON 3 +DATA 3 19 +MOM-SEC DATA ERR-T +MEV/C MB/MEV/C MB/MEV/C + -236.8 0.0387 0.0231 + -210.5 0.0553 0.0236 + -184.2 0.0441 0.0214 + -157.9 0.1011 0.0184 + -131.6 0.0968 0.0279 + -105.3 0.1773 0.0338 + -78.9 0.2577 0.0507 + -52.6 0.498 0.0448 + -26.3 0.9203 0.153 + 0.0 1.1569 0.3922 + 26.3 0.9033 0.1908 + 52.6 0.6699 0.0932 + 78.9 0.3436 0.0424 + 105.3 0.1635 0.023 + 131.6 0.071 0.0213 + 157.9 0.0321 0.0126 + 184.2 0.0151 0.0087 + 210.5 0.0053 0.0046 + 236.8 0.0013 0.0019 +ENDDATA 21 +ENDSUBENT 40 +SUBENT E1889003 20050914 20050914 E032 +BIB 6 10 +REACTION (6-C-12(6-C-15,X)6-C-13,LP,DP) +PART-DET (6-C-13) +MOM-SEC (MOM-SEC,6-C-13) + Longitudinal momemtum in projectile rest frame +MISC-COL (MISC) FWHM of gaussian fit to longitudinal momentum + distribution +ERR-ANALYS (ERR-T) Statistical error as well as error arising + from background subtraction +STATUS (TABLE) Data (Fig.3b, p034613-3 in reference) received + by e-mail from D.Q.Fang (2004.04.19) +ENDBIB 10 +COMMON 3 3 +EN MISC MISC-ERR +MEV/A MEV/C MEV/C + 83.0 223.0 28.0 +ENDCOMMON 3 +DATA 3 19 +MOM-SEC DATA ERR-T +MEV/C MB/MEV/C MB/MEV/C + -236.8 0.1338 0.081 + -210.5 0.1736 0.0745 + -184.2 0.2002 0.0675 + -157.9 0.2432 0.0686 + -131.6 0.2828 0.1056 + -105.3 0.3709 0.1375 + -78.9 0.4115 0.1256 + -52.6 0.417 0.1925 + -26.3 0.5138 0.5 + 0.0 0.0812 0.4911 + 26.3 0.5196 0.2452 + 52.6 0.3485 0.1215 + 78.9 0.3018 0.1109 + 105.3 0.2127 0.0717 + 131.6 0.1279 0.0489 + 157.9 0.0684 0.0429 + 184.2 0.0212 0.0273 + 210.5 0.0147 0.0135 + 236.8 0.0057 0.0204 +ENDDATA 21 +ENDSUBENT 40 +SUBENT E1889004 20050914 20050914 E032 +BIB 6 10 +REACTION (6-C-12(6-C-14,X)6-C-13,LP,DP) +PART-DET (6-C-13) +MOM-SEC (MOM-SEC,6-C-13) + Longitudinal momemtum in projectile rest frame +MISC-COL (MISC) FWHM of gaussian fit to longitudinal momentum + distribution +ERR-ANALYS (ERR-T) Statistical error as well as error arising + from background subtraction +STATUS (TABLE) Data (Fig.3c, p034613-3 in reference) received + by e-mail from D.Q.Fang (2004.04.19) +ENDBIB 10 +COMMON 3 3 +EN MISC MISC-ERR +MEV/A MEV/C MEV/C + 83.0 195.0 21.0 +ENDCOMMON 3 +DATA 3 15 +MOM-SEC DATA ERR-T +MEV/C MB/MEV/C MB/MEV/C + -233.3 0.0577 0.0056 + -200.0 0.0704 0.0142 + -166.7 0.096 0.0321 + -133.3 0.1417 0.0098 + -100.0 0.2175 0.0541 + -66.7 0.2664 0.0411 + -33.3 0.3739 0.22 + 0.0 0.102 0.3074 + 33.3 0.2622 0.0885 + 66.7 0.2049 0.0395 + 100.0 0.1107 0.0026 + 133.3 0.0754 0.0093 + 166.7 0.0311 0.0111 + 200.0 0.0022 0.0015 + 233.3 0.0 0.0012 +ENDDATA 17 +ENDSUBENT 36 +SUBENT E1889005 20050914 20050914 E032 +BIB 3 3 +REACTION (6-C-12(6-C-15,X)6-C-14,,SIG) +PART-DET (6-C-14) +STATUS (TABLE) Data taken from text, p034613-3 in reference +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA ERR-T +MEV/A MB MB + 83.0 146.0 23.0 +ENDDATA 3 +ENDSUBENT 11 +SUBENT E1889006 20050914 20050914 E032 +BIB 3 3 +REACTION (6-C-12(6-C-15,X)6-C-13,,SIG) +PART-DET (6-C-13) +STATUS (TABLE) Data taken from text, p034613-3 in reference +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA ERR-T +MEV/A MB MB + 83.0 177.0 93.0 49.0 +ENDDATA 3 +ENDSUBENT 11 +SUBENT E1889007 20050914 20050914 E032 +BIB 3 3 +REACTION (6-C-12(6-C-14,X)6-C-13,,SIG) +PART-DET (6-C-13) +STATUS (TABLE) Data taken from text, p034613-3 in reference +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA ERR-T +MEV/A MB MB + 83.0 67.0 14.0 +ENDDATA 3 +ENDSUBENT 11 +SUBENT E1889008 20050914 20050914 E032 +BIB 7 11 +REACTION (6-C-12(6-C-14,NON),,SIG) + Reaction cross section +PART-DET (6-C-14) +SAMPLE Target-thickness is 375 mg/cm**2. The uncertainty in + thickness was less than 1%. +ERR-ANALYS (ERR-T) Statistical error and error from background + and target thickness +ADD-RES (COMP) Glauber approximation +COMMENT EN: Incident energy at the middle of reaction target +STATUS (TABLE) Data taken from Table 1, p034613-4 in + reference +ENDBIB 11 +NOCOMMON 0 0 +DATA 3 1 +EN DATA ERR-T +MEV/A MB MB + 83.0 1075.0 61.0 +ENDDATA 3 +ENDSUBENT 19 +SUBENT E1889009 20050914 20050914 E032 +BIB 7 11 +REACTION (6-C-12(6-C-15,NON),,SIG) + Reaction cross section +PART-DET (6-C-15) +SAMPLE Target-thickness is 375 mg/cm**2. The uncertainty in + thickness was less than 1%. +ERR-ANALYS (ERR-T) Statistical error and error from background + and target thickness +ADD-RES (COMP) Glauber approximation +COMMENT EN: Incident energy at the middle of reaction target +STATUS (TABLE) Data taken from Table 1, p034613-4 in + reference +ENDBIB 11 +NOCOMMON 0 0 +DATA 3 2 +EN DATA ERR-T +MEV/A MB MB + 51.0 1560.0 44.0 + 83.0 1319.0 40.0 +ENDDATA 4 +ENDSUBENT 20 +ENDENTRY 9 diff --git a/exforall/E18/E1890.x4 b/exforall/E18/E1890.x4 new file mode 100644 index 000000000..5d19f6ac0 --- /dev/null +++ b/exforall/E18/E1890.x4 @@ -0,0 +1,101 @@ +ENTRY E1890 20050914 20050914 E032 +SUBENT E1890001 20050914 20050914 E032 +BIB 14 41 +TITLE Precise measurement of the cross section of + 3He(3He,2p)4He by using 3He doubly charged beam +AUTHOR (N.Kudomi, M.Komori, K.Takahisa, S.Yoshida, K.Kume, + H.Ohsumi, T.Itahashi) +INSTITUTE (2JPNOSA) Research Center for Nuclear Physics + (2JPNIRS) + (2JPNWER) + (2JPNJPN) Faculty of Culture and Education, Saga + University, Saga +REFERENCE (J,PR/C,69,(1),015802,200401) +REL-REF (N,,T.Itahashi+,J,RSI,69,(2),1032,199802) + Performance and design of ion source + (N,,T.Itahashi+,J,RSI,71,(2),1075,200002) + Performance and design of ion source +PART-DET (P) + (A) +INC-SOURCE - Beam intensity is 200 micro-Ampere. + - Charge of incident ion is 2+. +INC-SPECT EN: Effective reaction energy has 0.15% error, taking + into account accuracy of 0.1% for acceleration + voltage, 10% for stopping power, and 0.09% for energy + spread in target +SAMPLE - Chemical-form of target is element. + - Physical-form of target is gas. Windowless gas + target consists of a differential pumping and gas + circulation/purification system + - Target-thickness: 0.75 Torr +METHOD (COINC) Detect proton, proton and alpha in + coincidence. + (EDE) 4 delta E-E counter telescopes +FACILITY (ACCEL,2JPNOSA) NANOGUN ECR ion source with specially + designed ceramic insulator +DETECTOR (SOLST) Delta E counters with FWHM of 100-120 keV for + 5.48 MeV alpha particle + (SOLST) E counters with FWHM of 70-100 keV for 5.48 + MeV alpha particle +ERR-ANALYS (ERR-1) Uncertainty in reaction energy + (ERR-2) Uncertainty in beam intensity + (ERR-3) Uncertainty in target density + (ERR-4) Uncertainty in detection efficiency +HISTORY (20040416C) Kc + On +ENDBIB 41 +COMMON 4 3 +ERR-1 ERR-2 ERR-3 ERR-4 +PER-CENT PER-CENT PER-CENT PER-CENT + 0.15 2.0 1.3 3.0 +ENDCOMMON 3 +ENDSUBENT 48 +SUBENT E1890002 20050914 20050914 E032 +BIB 2 3 +REACTION (2-HE-3(HE3,2P)2-HE-4,,SIG) +STATUS (TABLE) Data taken from Table 2, p015802-11 in + reference +ENDBIB 3 +NOCOMMON 0 0 +DATA 2 8 +EN-CM DATA +KEV MB + 31.2 2.460E-10 + 33.1 4.520E-10 + 35.2 9.460E-10 + 37.3 1.830E-09 + 39.3 3.440E-09 + 41.3 5.790E-09 + 43.3 9.550E-09 + 45.3 1.530E-08 +ENDDATA 10 +ENDSUBENT 18 +SUBENT E1890003 20050914 20050914 E032 +BIB 4 8 +REL-REF (A,,A.Krauss+,J,NP/A,467,(2),273,198706) + The accuracy of both statistical and systematic + uncertainties of the present measurement is better + than that in this work. +REACTION (2-HE-3(HE3,2P)2-HE-4,,SIG,,SFC) +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data taken from Table 2, p015802-11 in + reference +ENDBIB 8 +COMMON 1 3 +ERR-SYS +PER-CENT + 3.8 +ENDCOMMON 3 +DATA 3 8 +EN-CM DATA ERR-S +KEV B*MEV B*MEV + 31.2 6.40 0.39 + 33.1 5.48 0.22 + 35.2 5.62 0.21 + 37.3 5.46 0.20 + 39.3 5.69 0.25 + 41.3 5.51 0.18 + 43.3 5.43 0.14 + 45.3 5.39 0.09 +ENDDATA 10 +ENDSUBENT 27 +ENDENTRY 3 diff --git a/exforall/E18/E1891.x4 b/exforall/E18/E1891.x4 new file mode 100644 index 000000000..73d9897de --- /dev/null +++ b/exforall/E18/E1891.x4 @@ -0,0 +1,942 @@ +ENTRY E1891 20050914 20050914 E032 +SUBENT E1891001 20050914 20050914 E032 +BIB 9 35 +TITLE Gamow-Teller transitions in the (7Li, 7Be) reaction at + 65A MeV +AUTHOR (S.Nakayama, H.Akimune, I.Daito, H.Fujimura, Y.Fujita, + M.Fujiwara, K.Fushimi, T.Inomata, K.Ishibashi, + H.Kohri, N.Koori, K.Takahisa, A.Tamii, M.Tanaka, + H.Toyokawa, T.Yamagata) +INSTITUTE (2JPNTKS) Department of Physics + (2JPNOSA) Research Center for Nuclear Physics + (2JPNOSA) Department of Physics + (2JPNKTO) Department of Physics + (2JPNKTJ) + (2JPNJSR) + (2JPNKON) Department of Physics +REFERENCE (J,PR/C,60,(4),047303,199910) +INC-SOURCE - Beam intensity is about 1 nA. + - Charge of incident ion is 3+. +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target is self supported. +FACILITY (CYCLO,2JPNOSA) Research Center for Nuclear Physics +DETECTOR E-RSL is about 500 keV.(Mainly due to beam energy + spreading) + (MAGSP) Grand RAIDEN spectrograph [M. Fujiwara et al., + Nucl. Instrum. Meth. A422(1999)484] to analyze + 7Be ejectiles. The aperture of entrance slit + of the Grand RAIDEN was set to be +-25 mr + horizontally and +-15 mr vertically. The + angular resolution in horizontal (theta) was + about 2mr, but in vertical (phi) was only + about 10mr. + (SCIN) GSO gamma-detector system NYMPHS [S. Nakayama + et al., Nucl. Instrum. Meth. A404(1998)34] to + detect 7Be 0.43 MeV gamma-ray. The total + absolute detection efficiency was about 0.2. +HISTORY (20040520C) Sr + On +ENDBIB 35 +COMMON 2 3 +EN E-RSL +MEV/A KEV + 65.0 500.0 +ENDCOMMON 3 +ENDSUBENT 42 +SUBENT E1891002 20050914 20050914 E032 +BIB 6 11 +REACTION (3-LI-6(3-LI-7,2-HE-6)4-BE-7,PAR,DA/DE,,REL) + Data given in count +PART-DET (4-BE-7) +EN-SEC ANG is polar angle between beam and 7Be in laboratory + system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.0,SPIN=1.5,PARITY=-1.) +SAMPLE - Target enrichment is 96.5%. + - Target-thickness is 2.5 mg/cm**2. +STATUS (CURVE) Data scanned from Fig.1, p047303-2 in + reference +ENDBIB 11 +COMMON 2 3 +ANG E-LVL +ADEG MEV + 0.3 0.0 +ENDCOMMON 3 +DATA 2 106 +Q-VAL DATA +MEV ARB-UNITS + -1.452E+00 2.012E+02 + -1.652E+00 4.905E+02 + -1.890E+00 6.602E+02 + -2.086E+00 6.852E+02 + -2.281E+00 6.239E+02 + -2.514E+00 5.570E+02 + -2.786E+00 4.206E+02 + -3.018E+00 2.981E+02 + -3.212E+00 1.951E+02 + -3.406E+00 1.282E+02 + -3.640E+00 8.083E+01 + -3.914E+00 5.013E+01 + -4.277E+00 6.595E+02 + -4.484E+00 1.313E+03 + -4.709E+00 7.512E+02 + -4.936E+00 3.225E+02 + -5.169E+00 2.473E+02 + -5.402E+00 1.359E+02 + -5.635E+00 6.072E+01 + -5.752E+00 3.008E+01 + -6.183E+00 3.829E+01 + -6.222E+00 6.889E+01 + -6.379E+00 8.554E+01 + -6.536E+00 9.384E+01 + -6.731E+00 7.151E+01 + -6.926E+00 6.589E+01 + -7.122E+00 6.304E+01 + -7.357E+00 6.019E+01 + -7.591E+00 6.568E+01 + -7.748E+00 6.285E+01 + -8.139E+00 7.386E+01 + -8.452E+00 6.263E+01 + -8.648E+00 7.926E+01 + -8.883E+00 7.919E+01 + -9.196E+00 7.909E+01 + -9.431E+00 8.458E+01 + -9.626E+00 7.896E+01 + -9.939E+00 7.886E+01 + -1.017E+01 8.157E+01 + -1.037E+01 8.151E+01 + -1.064E+01 8.420E+01 + -1.084E+01 8.414E+01 + -1.104E+01 8.408E+01 + -1.135E+01 8.398E+01 + -1.154E+01 7.836E+01 + -1.178E+01 7.828E+01 + -1.201E+01 8.099E+01 + -1.217E+01 8.651E+01 + -1.240E+01 7.531E+01 + -1.252E+01 8.640E+01 + -1.272E+01 8.356E+01 + -1.287E+01 7.516E+01 + -1.307E+01 7.510E+01 + -1.326E+01 7.504E+01 + -1.346E+01 7.498E+01 + -1.370E+01 7.212E+01 + -1.393E+01 7.205E+01 + -1.416E+01 6.641E+01 + -1.440E+01 6.633E+01 + -1.460E+01 6.906E+01 + -1.483E+01 7.177E+01 + -1.506E+01 7.169E+01 + -1.526E+01 6.885E+01 + -1.542E+01 6.602E+01 + -1.565E+01 6.594E+01 + -1.585E+01 6.588E+01 + -1.604E+01 6.860E+01 + -1.624E+01 6.576E+01 + -1.647E+01 6.569E+01 + -1.663E+01 6.564E+01 + -1.686E+01 6.278E+01 + -1.714E+01 5.991E+01 + -1.737E+01 5.706E+01 + -1.761E+01 5.420E+01 + -1.788E+01 5.968E+01 + -1.808E+01 5.405E+01 + -1.831E+01 5.398E+01 + -1.851E+01 5.392E+01 + -1.870E+01 5.664E+01 + -1.902E+01 5.654E+01 + -1.921E+01 5.648E+01 + -1.937E+01 5.922E+01 + -1.964E+01 6.191E+01 + -1.980E+01 6.465E+01 + -2.007E+01 6.178E+01 + -2.031E+01 6.171E+01 + -2.054E+01 6.163E+01 + -2.078E+01 5.878E+01 + -2.097E+01 5.872E+01 + -2.121E+01 5.308E+01 + -2.144E+01 5.579E+01 + -2.168E+01 5.849E+01 + -2.191E+01 5.564E+01 + -2.214E+01 5.557E+01 + -2.238E+01 5.271E+01 + -2.261E+01 5.264E+01 + -2.285E+01 4.978E+01 + -2.305E+01 4.972E+01 + -2.328E+01 4.965E+01 + -2.348E+01 4.958E+01 + -2.371E+01 4.673E+01 + -2.395E+01 4.666E+01 + -2.410E+01 5.217E+01 + -2.434E+01 5.210E+01 + -2.453E+01 5.204E+01 + -2.480E+01 3.804E+01 +ENDDATA 108 +ENDSUBENT 128 +SUBENT E1891003 20050914 20050914 E032 +BIB 7 13 +REACTION (3-LI-6(3-LI-7,2-HE-6)4-BE-7,PAR,DA/DE,,REL) + Data given in count +PART-DET (G) 0.43 MeV prompt gamma of 7Be + (4-BE-7) +EN-SEC ANG is polar angle between beam and 7Be in laboratory + system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.43,SPIN=0.5,PARITY=-1.) +SAMPLE - Target enrichment is 96.5%. + - Target-thickness is 2.5 mg/cm**2. +METHOD (COINC) Detect 7Be and prompt gamma in coincidence. +STATUS (CURVE) Data scanned from Fig.1, p047303-2 in + reference +ENDBIB 13 +COMMON 2 3 +ANG E-LVL +ADEG MEV + 0.3 0.43 +ENDCOMMON 3 +DATA 2 138 +Q-VAL DATA +MEV ARB-UNITS + 4.950E+00 -5.027E+00 + 4.703E+00 -2.594E+00 + 4.491E+00 -2.657E+00 + 4.314E+00 -2.022E-01 + 4.102E+00 -2.774E+00 + 3.854E+00 -5.357E+00 + 3.642E+00 -2.913E+00 + 3.465E+00 -2.966E+00 + 3.288E+00 -3.019E+00 + 3.076E+00 -3.083E+00 + 2.829E+00 -3.158E+00 + 2.616E+00 -3.221E+00 + 2.440E+00 -3.275E+00 + 2.263E+00 -3.328E+00 + 2.051E+00 -5.900E+00 + 1.909E+00 -5.943E+00 + 1.733E+00 -5.996E+00 + 1.485E+00 -6.070E+00 + 1.273E+00 -6.134E+00 + 1.061E+00 -6.198E+00 + 8.486E-01 -6.262E+00 + 6.720E-01 -8.823E+00 + 4.952E-01 -8.877E+00 + 3.182E-01 -6.422E+00 + 1.061E-01 -6.486E+00 + -1.766E-01 -1.159E+01 + -3.888E-01 -9.143E+00 + -5.656E-01 -9.196E+00 + -7.778E-01 -9.260E+00 + -1.061E+00 -6.837E+00 + -1.203E+00 1.068E+01 + -1.455E+00 1.059E+02 + -1.709E+00 2.413E+02 + -1.927E+00 3.641E+02 + -2.104E+00 3.641E+02 + -2.350E+00 3.314E+02 + -2.559E+00 2.812E+02 + -2.803E+00 2.033E+02 + -2.942E+00 1.406E+02 + -3.222E+00 8.783E+01 + -3.433E+00 4.763E+01 + -3.644E+00 2.500E+01 + -3.855E+00 1.490E+01 + -4.070E+00 7.002E+01 + -4.341E+00 5.566E+02 + -4.540E+00 1.036E+03 + -4.734E+00 6.618E+02 + -4.964E+00 2.830E+02 + -5.169E+00 1.324E+02 + -5.378E+00 6.711E+01 + -5.589E+00 2.692E+01 + -6.048E+00 1.173E+01 + -6.261E+00 4.177E+01 + -6.509E+00 5.674E+01 + -6.650E+00 4.666E+01 + -6.933E+00 3.905E+01 + -7.145E+00 3.397E+01 + -7.357E+00 3.893E+01 + -7.605E+00 3.634E+01 + -7.781E+00 3.127E+01 + -8.029E+00 4.123E+01 + -8.241E+00 3.615E+01 + -8.453E+00 3.358E+01 + -8.630E+00 3.603E+01 + -8.878E+00 3.847E+01 + -9.090E+00 3.841E+01 + -9.231E+00 4.087E+01 + -9.514E+00 4.079E+01 + -9.726E+00 4.072E+01 + -9.938E+00 3.815E+01 + -1.019E+01 3.306E+01 + -1.040E+01 3.299E+01 + -1.065E+01 3.543E+01 + -1.082E+01 3.788E+01 + -1.100E+01 4.034E+01 + -1.128E+01 3.524E+01 + -1.149E+01 2.765E+01 + -1.171E+01 3.260E+01 + -1.188E+01 3.756E+01 + -1.210E+01 2.998E+01 + -1.231E+01 2.991E+01 + -1.259E+01 2.732E+01 + -1.280E+01 2.475E+01 + -1.301E+01 2.468E+01 + -1.323E+01 2.713E+01 + -1.344E+01 2.205E+01 + -1.365E+01 2.449E+01 + -1.393E+01 2.441E+01 + -1.415E+01 2.434E+01 + -1.436E+01 2.428E+01 + -1.453E+01 1.419E+01 + -1.475E+01 2.416E+01 + -1.499E+01 2.409E+01 + -1.524E+01 2.652E+01 + -1.542E+01 1.894E+01 + -1.567E+01 2.388E+01 + -1.588E+01 2.382E+01 + -1.613E+01 2.375E+01 + -1.634E+01 1.114E+01 + -1.648E+01 2.113E+01 + -1.676E+01 2.105E+01 + -1.697E+01 1.847E+01 + -1.719E+01 1.841E+01 + -1.740E+01 1.584E+01 + -1.761E+01 1.577E+01 + -1.782E+01 1.571E+01 + -1.804E+01 1.565E+01 + -1.828E+01 1.557E+01 + -1.853E+01 1.550E+01 + -1.871E+01 1.795E+01 + -1.892E+01 1.789E+01 + -1.913E+01 1.782E+01 + -1.938E+01 2.026E+01 + -1.955E+01 1.268E+01 + -1.980E+01 1.511E+01 + -2.002E+01 1.505E+01 + -2.026E+01 1.247E+01 + -2.048E+01 9.895E+00 + -2.069E+01 1.736E+01 + -2.086E+01 1.479E+01 + -2.111E+01 1.221E+01 + -2.136E+01 1.464E+01 + -2.157E+01 9.565E+00 + -2.175E+01 7.003E+00 + -2.200E+01 1.195E+01 + -2.228E+01 1.437E+01 + -2.249E+01 9.288E+00 + -2.270E+01 1.173E+01 + -2.288E+01 1.168E+01 + -2.309E+01 9.107E+00 + -2.334E+01 1.154E+01 + -2.355E+01 6.461E+00 + -2.376E+01 6.397E+00 + -2.398E+01 8.841E+00 + -2.419E+01 8.777E+00 + -2.443E+01 8.703E+00 + -2.465E+01 6.131E+00 + -2.489E+01 6.056E+00 +ENDDATA 140 +ENDSUBENT 162 +SUBENT E1891004 20050914 20050914 E032 +BIB 6 11 +REACTION (6-C-12(3-LI-7,4-BE-7)5-B-12,PAR,DA/DE,,REL) + Data given in count +PART-DET (4-BE-7) +EN-SEC ANG is polar angle between beam and 7Be in laboratory + system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.0,SPIN=1.5,PARITY=-1.) +SAMPLE - Target enrichment is 98.9%. + - Target-thickness is 1.0 mg/cm**2. +STATUS (CURVE) Data scanned from Fig.1, p047303-2 in + reference +ENDBIB 11 +COMMON 2 3 +ANG E-LVL +ADEG MEV + 0.3 0.0 +ENDCOMMON 3 +DATA 2 57 +Q-VAL DATA +MEV ARB-UNITS + -1.696E+00 8.357E+01 + -1.876E+00 2.732E+02 + -2.115E+00 2.880E+02 + -2.309E+00 2.079E+02 + -2.568E+00 1.246E+02 + -2.795E+00 6.276E+01 + -3.021E+00 3.098E+01 + -3.247E+00 1.582E+01 + -3.474E+00 9.568E+00 + -3.680E+00 3.016E+00 + -1.414E+01 1.663E+00 + -1.435E+01 7.761E+01 + -1.454E+01 2.052E+02 + -1.480E+01 7.294E+01 + -1.503E+01 -5.032E+00 + -1.522E+01 2.266E+01 + -1.540E+01 3.296E+01 + -1.571E+01 3.357E+01 + -1.587E+01 7.946E-01 + -1.612E+01 1.505E+01 + -1.635E+01 2.137E+01 + -1.722E+01 1.723E+01 + -1.745E+01 1.028E+01 + -1.767E+01 3.903E+00 + -1.793E+01 8.716E+00 + -1.825E+01 1.197E+01 + -1.847E+01 2.113E+01 + -1.873E+01 2.976E+01 + -1.896E+01 5.803E+01 + -1.918E+01 7.012E+01 + -1.941E+01 4.585E+01 + -1.960E+01 2.793E+01 + -1.986E+01 2.501E+01 + -2.006E+01 2.050E+01 + -2.024E+01 2.439E+01 + -2.047E+01 2.321E+01 + -2.070E+01 3.473E+01 + -2.096E+01 3.239E+01 + -2.111E+01 3.873E+01 + -2.138E+01 4.101E+01 + -2.156E+01 5.427E+01 + -2.179E+01 6.059E+01 + -2.194E+01 6.519E+01 + -2.209E+01 6.402E+01 + -2.232E+01 5.995E+01 + -2.247E+01 7.033E+01 + -2.270E+01 6.106E+01 + -2.292E+01 5.007E+01 + -2.315E+01 5.120E+01 + -2.330E+01 3.617E+01 + -2.357E+01 3.787E+01 + -2.383E+01 3.669E+01 + -2.402E+01 4.244E+01 + -2.417E+01 2.568E+01 + -2.440E+01 2.565E+01 + -2.470E+01 2.619E+01 + -2.492E+01 1.751E+01 +ENDDATA 59 +ENDSUBENT 79 +SUBENT E1891005 20050914 20050914 E032 +BIB 7 13 +REACTION (6-C-12(3-LI-7,4-BE-7)5-B-12,PAR,DA/DE,,REL) + Data given in count +PART-DET (G) 0.43 MeV prompt gamma of 7Be + (4-BE-7) +EN-SEC ANG is polar angle between beam and 7Be in laboratory + system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.43,SPIN=0.5,PARITY=-1.) +SAMPLE - Target enrichment is 98.9%. + - Target-thickness is 1.0 mg/cm**2. +METHOD (COINC) Detect 7Be and prompt gamma in coincidence. +STATUS (CURVE) Data scanned from Fig.1, p047303-2 in + reference +ENDBIB 13 +COMMON 2 3 +ANG E-LVL +ADEG MEV + 0.3 0.43 +ENDCOMMON 3 +DATA 2 137 +Q-VAL DATA +MEV ARB-UNITS + 4.932E+00 -1.157E+00 + 4.667E+00 -1.157E+00 + 4.478E+00 -1.157E+00 + 4.250E+00 -1.157E+00 + 3.985E+00 -1.157E+00 + 3.758E+00 -1.157E+00 + 3.531E+00 -1.157E+00 + 3.341E+00 -1.157E+00 + 3.190E+00 -1.157E+00 + 2.962E+00 -1.157E+00 + 2.697E+00 -1.157E+00 + 2.508E+00 -1.157E+00 + 2.281E+00 -1.157E+00 + 2.053E+00 -1.157E+00 + 1.788E+00 -1.157E+00 + 1.675E+00 -1.157E+00 + 1.447E+00 -1.736E+00 + 1.258E+00 -1.157E+00 + 9.928E-01 -1.157E+00 + 8.034E-01 -1.157E+00 + 6.519E-01 -1.157E+00 + 4.246E-01 -1.157E+00 + 1.595E-01 -1.157E+00 + -2.984E-02 -5.787E-01 + -3.329E-01 -1.157E+00 + -5.602E-01 -1.157E+00 + -8.253E-01 -5.787E-01 + -1.091E+00 -1.157E+00 + -1.242E+00 -1.157E+00 + -1.507E+00 3.472E+00 + -1.692E+00 4.803E+01 + -1.912E+00 1.175E+02 + -2.136E+00 1.516E+02 + -2.329E+00 1.157E+02 + -2.560E+00 7.928E+01 + -2.791E+00 4.051E+01 + -3.021E+00 1.678E+01 + -3.262E+00 9.650E+00 + -3.412E+00 2.695E+00 + -3.628E+00 -1.736E+00 + -3.856E+00 -5.787E-01 + -4.131E+00 9.082E-01 + -4.234E+00 -1.736E+00 + -4.462E+00 -1.736E+00 + -4.727E+00 -1.736E+00 + -4.916E+00 -1.736E+00 + -5.181E+00 -1.157E+00 + -5.371E+00 -1.736E+00 + -5.598E+00 5.787E-01 + -5.787E+00 -1.736E+00 + -6.015E+00 -1.157E+00 + -6.280E+00 -1.736E+00 + -6.431E+00 -1.736E+00 + -6.659E+00 -1.736E+00 + -6.886E+00 0.000E+00 + -7.156E+00 -4.635E-01 + -7.340E+00 -1.736E+00 + -7.606E+00 -1.736E+00 + -7.833E+00 -1.157E+00 + -8.060E+00 -1.736E+00 + -8.287E+00 -1.157E+00 + -8.515E+00 -1.736E+00 + -8.745E+00 -5.760E-01 + -8.894E+00 -1.736E+00 + -9.123E+00 -6.028E-01 + -9.310E+00 -1.736E+00 + -9.537E+00 -1.157E+00 + -9.765E+00 -1.157E+00 + -1.003E+01 5.787E-01 + -1.029E+01 -6.859E-01 + -1.045E+01 1.040E+00 + -1.064E+01 -7.100E-01 + -1.090E+01 4.287E-01 + -1.113E+01 4.126E-01 + -1.136E+01 1.554E+00 + -1.158E+01 -1.736E+00 + -1.181E+01 2.315E+00 + -1.196E+01 -1.961E+00 + -1.219E+01 1.495E+00 + -1.238E+01 -1.157E+00 + -1.261E+01 -1.157E+00 + -1.283E+01 -1.157E+00 + -1.306E+01 -1.736E+00 + -1.328E+01 8.386E-01 + -1.355E+01 -1.736E+00 + -1.374E+01 2.277E-01 + -1.393E+01 0.000E+00 + -1.419E+01 8.297E+00 + -1.435E+01 6.037E+01 + -1.460E+01 1.447E+02 + -1.483E+01 6.250E+01 + -1.502E+01 9.974E+00 + -1.529E+01 9.377E+00 + -1.548E+01 1.515E+01 + -1.571E+01 6.944E+00 + -1.598E+01 -4.051E+00 + -1.616E+01 4.107E+00 + -1.631E+01 9.305E+00 + -1.661E+01 6.968E+00 + -1.680E+01 3.483E+00 + -1.699E+01 2.891E+00 + -1.722E+01 4.611E+00 + -1.744E+01 6.910E+00 + -1.767E+01 -1.208E+00 + -1.786E+01 2.251E+00 + -1.820E+01 3.384E+00 + -1.832E+01 1.032E+01 + -1.854E+01 1.725E+01 + -1.877E+01 2.649E+01 + -1.900E+01 4.861E+01 + -1.927E+01 5.266E+01 + -1.946E+01 3.183E+01 + -1.968E+01 2.064E+01 + -1.988E+01 1.215E+01 + -2.014E+01 1.215E+01 + -2.033E+01 4.630E+00 + -2.052E+01 9.259E+00 + -2.079E+01 1.273E+01 + -2.098E+01 1.736E+01 + -2.123E+01 6.642E+00 + -2.145E+01 1.588E+01 + -2.161E+01 2.108E+01 + -2.187E+01 3.495E+01 + -2.206E+01 2.047E+01 + -2.233E+01 2.971E+01 + -2.255E+01 3.085E+01 + -2.275E+01 1.852E+01 + -2.293E+01 2.851E+01 + -2.317E+01 1.910E+01 + -2.338E+01 1.575E+01 + -2.365E+01 1.052E+01 + -2.384E+01 2.208E+01 + -2.406E+01 1.223E+01 + -2.421E+01 1.511E+01 + -2.452E+01 1.682E+01 + -2.476E+01 7.523E+00 + -2.497E+01 1.795E+01 +ENDDATA 139 +ENDSUBENT 161 +SUBENT E1891006 20050914 20050914 E032 +BIB 6 11 +REACTION (14-SI-28(3-LI-7,4-BE-7)13-AL-28,PAR,DA/DE,,REL) + Data given in count +PART-DET (4-BE-7) +EN-SEC ANG is polar angle between beam and 7Be in laboratory + system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.0,SPIN=1.5,PARITY=-1.) +SAMPLE - Target enrichment is 92.2%. + - Target-thickness is 1.4 mg/cm**2. +STATUS (CURVE) Data scanned from Fig.1, p047303-2 in + reference +ENDBIB 11 +COMMON 2 3 +ANG E-LVL +ADEG MEV + 0.3 0.0 +ENDCOMMON 3 +DATA 2 97 +Q-VAL DATA +MEV ARB-UNITS + -1.481E+00 1.746E+01 + -1.698E+00 1.166E+02 + -1.843E+00 2.891E+02 + -2.059E+00 3.408E+02 + -2.276E+00 2.829E+02 + -2.493E+00 1.899E+02 + -2.782E+00 1.197E+02 + -2.999E+00 6.607E+01 + -3.215E+00 3.526E+01 + -3.432E+00 1.677E+01 + -3.649E+00 4.444E+00 + -3.866E+00 1.356E+00 + -5.564E+00 1.546E+01 + -5.997E+00 5.593E+00 + -6.322E+00 3.734E+00 + -6.539E+00 6.806E+00 + -6.720E+00 2.343E+01 + -6.936E+00 6.716E+01 + -7.117E+00 5.976E+01 + -7.334E+00 4.312E+01 + -7.551E+00 1.133E+02 + -7.767E+00 1.885E+02 + -8.273E+00 2.338E+01 + -8.634E+00 4.554E+01 + -8.887E+00 2.890E+01 + -9.140E+00 2.150E+01 + -9.393E+00 2.026E+01 + -9.465E+00 2.950E+01 + -9.754E+00 3.072E+01 + -9.971E+00 1.038E+01 + -1.022E+01 3.317E+01 + -1.040E+01 7.382E+01 + -1.062E+01 7.319E+01 + -1.087E+01 5.224E+01 + -1.105E+01 5.531E+01 + -1.127E+01 8.672E+01 + -1.153E+01 1.033E+02 + -1.174E+01 9.595E+01 + -1.192E+01 7.007E+01 + -1.210E+01 9.224E+01 + -1.239E+01 6.389E+01 + -1.261E+01 4.972E+01 + -1.279E+01 6.080E+01 + -1.301E+01 7.619E+01 + -1.322E+01 4.169E+01 + -1.347E+01 5.523E+01 + -1.362E+01 6.385E+01 + -1.387E+01 6.569E+01 + -1.405E+01 6.137E+01 + -1.431E+01 9.647E+01 + -1.456E+01 1.260E+02 + -1.474E+01 9.646E+01 + -1.496E+01 9.275E+01 + -1.521E+01 9.829E+01 + -1.546E+01 1.229E+02 + -1.564E+01 1.315E+02 + -1.586E+01 1.032E+02 + -1.604E+01 1.137E+02 + -1.629E+01 1.167E+02 + -1.658E+01 1.130E+02 + -1.676E+01 9.516E+01 + -1.694E+01 8.776E+01 + -1.716E+01 1.112E+02 + -1.745E+01 1.124E+02 + -1.756E+01 1.290E+02 + -1.785E+01 1.321E+02 + -1.806E+01 1.154E+02 + -1.824E+01 1.037E+02 + -1.853E+01 1.019E+02 + -1.864E+01 9.386E+01 + -1.889E+01 9.385E+01 + -1.911E+01 9.507E+01 + -1.940E+01 9.137E+01 + -1.962E+01 8.889E+01 + -1.987E+01 9.012E+01 + -2.001E+01 6.239E+01 + -2.030E+01 6.238E+01 + -2.048E+01 7.162E+01 + -2.066E+01 9.440E+01 + -2.092E+01 8.331E+01 + -2.113E+01 1.005E+02 + -2.135E+01 9.684E+01 + -2.157E+01 8.205E+01 + -2.175E+01 9.190E+01 + -2.200E+01 8.511E+01 + -2.222E+01 9.496E+01 + -2.247E+01 9.680E+01 + -2.269E+01 9.372E+01 + -2.287E+01 8.878E+01 + -2.312E+01 9.124E+01 + -2.334E+01 7.213E+01 + -2.363E+01 7.520E+01 + -2.395E+01 7.765E+01 + -2.417E+01 8.997E+01 + -2.442E+01 8.626E+01 + -2.464E+01 7.701E+01 + -2.486E+01 6.715E+01 +ENDDATA 99 +ENDSUBENT 119 +SUBENT E1891007 20050914 20050914 E032 +BIB 7 13 +REACTION (14-SI-28(3-LI-7,4-BE-7)13-AL-28,PAR,DA/DE,,REL) + Data given in count +PART-DET (G) 0.43 MeV prompt gamma of 7Be + (4-BE-7) +EN-SEC ANG is polar angle between beam and 7Be in laboratory + system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.43,SPIN=0.5,PARITY=-1.) +SAMPLE - Target enrichment is 92.2%. + - Target-thickness is 1.4 mg/cm**2. +METHOD (COINC) Detect 7Be and prompt gamma in coincidence. +STATUS (CURVE) Data scanned from Fig.1, p047303-2 in + reference +ENDBIB 13 +COMMON 2 3 +ANG E-LVL +ADEG MEV + 0.3 0.43 +ENDCOMMON 3 +DATA 2 137 +Q-VAL DATA +MEV ARB-UNITS + 4.796E+00 -1.948E-01 + 4.607E+00 -2.017E-01 + 4.418E+00 -2.086E-01 + 4.154E+00 -8.621E-01 + 3.890E+00 -8.717E-01 + 3.663E+00 -8.800E-01 + 3.474E+00 -2.431E-01 + 3.248E+00 -8.952E-01 + 3.021E+00 -2.597E-01 + 2.795E+00 -2.680E-01 + 2.606E+00 -2.749E-01 + 2.417E+00 -2.818E-01 + 2.190E+00 -2.901E-01 + 1.926E+00 -2.998E-01 + 1.775E+00 -9.491E-01 + 1.586E+00 -3.122E-01 + 1.359E+00 -3.205E-01 + 1.133E+00 3.150E-01 + 9.063E-01 -3.371E-01 + 6.798E-01 -3.454E-01 + 5.665E-01 -3.495E-01 + 3.776E-01 -3.564E-01 + 1.888E-01 -3.633E-01 + 0.000E+00 -3.702E-01 + -2.266E-01 -3.785E-01 + -4.154E-01 -1.029E+00 + -6.042E-01 -3.923E-01 + -8.686E-01 2.418E-01 + -1.057E+00 -4.089E-01 + -1.322E+00 8.690E-01 + -1.586E+00 1.373E+01 + -1.775E+00 6.008E+01 + -2.002E+00 1.438E+02 + -2.153E+00 1.792E+02 + -2.379E+00 1.592E+02 + -2.643E+00 1.070E+02 + -2.908E+00 6.261E+01 + -3.097E+00 3.106E+01 + -3.323E+00 1.238E+01 + -3.512E+00 4.008E+00 + -3.776E+00 2.711E+00 + -3.965E+00 -5.153E-01 + -4.230E+00 1.188E-01 + -4.456E+00 1.105E-01 + -4.758E+00 9.947E-02 + -5.060E+00 8.842E-02 + -5.287E+00 -5.636E-01 + -5.476E+00 8.442E+00 + -5.740E+00 7.145E+00 + -5.929E+00 7.004E-01 + -6.156E+00 1.980E+00 + -6.382E+00 7.122E+00 + -6.571E+00 1.098E+01 + -6.798E+00 2.127E+01 + -7.024E+00 3.285E+01 + -7.251E+00 3.155E+01 + -7.477E+00 3.670E+01 + -7.666E+00 7.403E+01 + -7.855E+00 1.133E+02 + -8.119E+00 7.916E+01 + -8.346E+00 1.413E+01 + -8.535E+00 1.606E+01 + -8.724E+00 2.120E+01 + -8.988E+00 2.183E+01 + -9.214E+00 1.539E+01 + -9.441E+00 1.473E+01 + -9.630E+00 2.567E+01 + -9.857E+00 2.309E+01 + -1.008E+01 1.664E+01 + -1.027E+01 2.565E+01 + -1.054E+01 5.010E+01 + -1.069E+01 5.911E+01 + -1.091E+01 2.241E+01 + -1.114E+01 3.141E+01 + -1.140E+01 4.041E+01 + -1.159E+01 6.101E+01 + -1.182E+01 3.460E+01 + -1.201E+01 2.752E+01 + -1.220E+01 1.850E+01 + -1.250E+01 1.849E+01 + -1.269E+01 1.333E+01 + -1.291E+01 3.972E+01 + -1.307E+01 4.937E+01 + -1.333E+01 3.004E+01 + -1.356E+01 2.167E+01 + -1.378E+01 3.646E+01 + -1.401E+01 3.324E+01 + -1.420E+01 2.357E+01 + -1.443E+01 5.833E+01 + -1.465E+01 6.025E+01 + -1.488E+01 5.123E+01 + -1.507E+01 3.127E+01 + -1.533E+01 3.319E+01 + -1.548E+01 5.636E+01 + -1.571E+01 5.506E+01 + -1.597E+01 4.604E+01 + -1.620E+01 4.346E+01 + -1.639E+01 4.924E+01 + -1.658E+01 5.567E+01 + -1.684E+01 3.893E+01 + -1.703E+01 3.892E+01 + -1.726E+01 3.698E+01 + -1.748E+01 3.311E+01 + -1.771E+01 3.439E+01 + -1.794E+01 4.146E+01 + -1.813E+01 3.695E+01 + -1.835E+01 4.209E+01 + -1.854E+01 5.432E+01 + -1.877E+01 3.821E+01 + -1.903E+01 4.915E+01 + -1.926E+01 4.850E+01 + -1.949E+01 5.106E+01 + -1.964E+01 6.071E+01 + -1.990E+01 5.620E+01 + -2.013E+01 4.782E+01 + -2.028E+01 2.593E+01 + -2.054E+01 2.527E+01 + -2.081E+01 2.269E+01 + -2.100E+01 2.976E+01 + -2.122E+01 4.134E+01 + -2.145E+01 3.425E+01 + -2.164E+01 3.875E+01 + -2.187E+01 2.587E+01 + -2.209E+01 3.809E+01 + -2.232E+01 2.778E+01 + -2.255E+01 3.550E+01 + -2.281E+01 3.227E+01 + -2.292E+01 4.128E+01 + -2.319E+01 4.256E+01 + -2.341E+01 3.611E+01 + -2.364E+01 3.095E+01 + -2.375E+01 2.966E+01 + -2.406E+01 2.836E+01 + -2.425E+01 4.123E+01 + -2.451E+01 4.251E+01 + -2.474E+01 3.091E+01 + -2.492E+01 4.056E+01 +ENDDATA 139 +ENDSUBENT 161 +SUBENT E1891008 20050914 20050914 E032 +BIB 8 20 +REACTION (6-C-12(3-LI-7,4-BE-7)5-B-12,PAR,DA) +PART-DET (4-BE-7) +EN-SEC ANG-CM is polar angle between beam and 7Be in center + of mass system + (E-LVL1,4-BE-7) + (E-LVL2,5-B-12) +LEVEL-PROP (4-BE-7,E-LVL=0.0,SPIN=1.5,PARITY=-1.) + (5-B-12,E-LVL=0.0,SPIN=1.,PARITY=+1.) +SAMPLE - Target enrichment is 98.9%. + - Target-thickness is 1.0 mg/cm**2. +ERR-ANALYS (ERR-S) Statistical uncertainty + (ERR-SYS) Uncertainties in target thickness, + accumulated beam-current and procedure to + separate the 7Be(g.s) and 7Be(1st) spectra +ADD-RES (COMP) DWBA (Distorted wave Born approximation) (Three + calculations (full effictive NN interaction, + central part only, tensor part only) were + performed.) +STATUS (CURVE) Data scanned from Fig.2, p047303-3 in + reference +ENDBIB 20 +COMMON 3 3 +E-LVL1 E-LVL2 ERR-SYS +MEV MEV PER-CENT + 0.0 0.0 20.0 +ENDCOMMON 3 +DATA 4 8 +ANG-CM ANG-ERR DATA-CM ERR-S +ADEG ADEG MB/SR MB/SR + 5.284E-01 4.272E-01 4.245E+00 2.011E-01 + 1.291E+00 3.958E-01 3.582E+00 2.774E-01 + 1.551E+00 4.167E-01 3.770E+00 1.802E-01 + 2.044E+00 2.917E-01 2.710E+00 2.150E-01 + 2.555E+00 3.125E-01 2.455E+00 2.358E-01 + 2.816E+00 2.917E-01 2.164E+00 3.329E-01 + 3.577E+00 3.021E-01 2.007E+00 2.982E-01 + 4.348E+00 3.021E-01 2.023E+00 3.120E-01 +ENDDATA 10 +ENDSUBENT 39 +SUBENT E1891009 20050914 20050914 E032 +BIB 7 13 +REACTION ((6-C-12(3-LI-7,4-BE-7)5-B-12,PAR,DA)// + (6-C-12(3-LI-7,4-BE-7)5-B-12,PAR,DA)) +PART-DET (G) 0.43 MeV prompt gamma of 7Be + (4-BE-7) +EN-SEC ANG-CM is polar angle between beam and 7Be in center + of mass system +SAMPLE - Target enrichment is 98.9%. + - Target-thickness is 1.0 mg/cm**2. +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +COMMENT E-LVL-NM: Level energy for numerator of ratio + E-LVL-DN: Level energy for denominator of ratio +STATUS (CURVE) Data scanned from Fig.4, p047303-3 in + reference +ENDBIB 13 +COMMON 2 3 +E-LVL-NM E-LVL-DN +MEV MEV + 0.43 0.0 +ENDCOMMON 3 +DATA 3 7 +ANG-CM DATA-CM DATA-ERR +ADEG NO-DIM NO-DIM + 6.281E-01 8.113E-01 8.690E-02 + 1.399E+00 8.168E-01 9.392E-02 + 2.168E+00 7.824E-01 9.392E-02 + 2.739E+00 7.812E-01 1.127E-01 + 3.317E+00 7.988E-01 1.245E-01 + 3.878E+00 7.155E-01 1.198E-01 + 4.454E+00 8.764E-01 1.362E-01 +ENDDATA 9 +ENDSUBENT 31 +ENDENTRY 9 diff --git a/exforall/E18/E1892.x4 b/exforall/E18/E1892.x4 new file mode 100644 index 000000000..91cb1f1a3 --- /dev/null +++ b/exforall/E18/E1892.x4 @@ -0,0 +1,187 @@ +ENTRY E1892 20050914 20050914 E032 +SUBENT E1892001 20050914 20050914 E032 +BIB 12 22 +TITLE Status of the CYRIC neutron TOF facilities upgrade +AUTHOR (H.Orihara, S.Nishihara, K.Furukawa, M.Kabasawa, + T.Kawamura, Y.Takahashi, T.Nakagawa, K.Maeda) +INSTITUTE (2JPNTOH) Cyclotron and Radioisotope Center + (2JPNTOH) Department of Physics, Faculty of Science + (2JPNTOH) College of General Education +REFERENCE (J,NIM/A,257,(2),189,198706) +DECAY-DATA (4-BE-7,53.3D,DG,478.,0.104) +PART-DET (N) +SAMPLE - Target enrichment is unknown. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Backing is unknown. +METHOD (TOF) The overall time resolution is 1067 ps, which + corresponds to an energy resolution of 108 keV + for 30 MeV neutrons detected at a flight path of + 44.2 m. +FACILITY (CYCLO,2JPNTOH) Cyclotron and Radioisotope Center +DETECTOR E-RSL: Measured by 30 MeV neutrons from 34S(p,n0)34Cl + (SCIN) NE213 to provide the signal for neutron arrival +STATUS (TABLE) Data taken from Table 2, p195 in reference +HISTORY (20040416C) Ic + On +ENDBIB 22 +COMMON 2 3 +EN E-RSL +MEV KEV + 35.0 108.0 +ENDCOMMON 3 +ENDSUBENT 29 +SUBENT E1892002 20050914 20050914 E032 +BIB 4 6 +REACTION (3-LI-7(P,N)4-BE-7,PAR,DA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.0,SPIN=1.5,PARITY=-1.) +ERR-ANALYS (ERR-S) Statistical uncertainty +ENDBIB 6 +COMMON 1 3 +E-LVL +MEV + 0.0 +ENDCOMMON 3 +DATA 3 32 +ANG DATA ERR-S +ADEG MB/SR MB/SR + 0.0 23.022 0.058 + 3.0 22.239 0.083 + 5.0 20.394 0.067 + 10.0 17.568 0.076 + 12.5 14.936 0.069 + 15.0 11.772 0.062 + 17.5 9.699 0.082 + 20.0 7.614 0.050 + 22.5 5.972 0.044 + 25.0 4.608 0.039 + 30.0 3.006 0.032 + 35.0 2.286 0.028 + 40.0 2.124 0.027 + 45.0 1.944 0.027 + 50.0 1.800 0.026 + 55.0 1.422 0.024 + 60.0 1.134 0.021 + 65.0 0.814 0.019 + 70.0 0.616 0.017 + 75.0 0.429 0.014 + 80.0 0.309 0.0098 + 85.0 0.243 0.011 + 90.0 0.207 0.0076 + 95.0 0.174 0.0072 + 100.0 0.167 0.0072 + 105.0 0.139 0.0076 + 110.0 0.122 0.0065 + 115.0 0.110 0.0063 + 120.0 0.0909 0.0059 + 130.0 0.0699 0.0042 + 140.0 0.0607 0.0043 + 145.0 0.0693 0.0047 +ENDDATA 34 +ENDSUBENT 49 +SUBENT E1892003 20050914 20050914 E032 +BIB 4 6 +REACTION (3-LI-7(P,N)4-BE-7,PAR,DA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.429,SPIN=0.5,PARITY=-1.) +ERR-ANALYS (ERR-S) Statistical uncertainty +ENDBIB 6 +COMMON 1 3 +E-LVL +MEV + 0.429 +ENDCOMMON 3 +DATA 3 32 +ANG DATA ERR-S +ADEG MB/SR MB/SR + 0.0 9.639 0.038 + 3.0 9.405 0.056 + 5.0 9.261 0.045 + 10.0 7.245 0.049 + 12.5 6.143 0.044 + 15.0 5.085 0.040 + 17.5 4.303 0.037 + 20.0 3.483 0.034 + 22.5 2.834 0.031 + 25.0 2.340 0.028 + 30.0 1.593 0.023 + 35.0 1.224 0.021 + 40.0 0.927 0.018 + 45.0 0.806 0.017 + 50.0 0.634 0.016 + 55.0 0.509 0.014 + 60.0 0.399 0.013 + 65.0 0.311 0.012 + 70.0 0.219 0.010 + 75.0 0.161 0.0090 + 80.0 0.110 0.0053 + 85.0 0.102 0.0075 + 90.0 0.0842 0.0049 + 95.0 0.0597 0.0043 + 100.0 0.0669 0.0046 + 105.0 0.0549 0.0045 + 110.0 0.0485 0.0042 + 115.0 0.0370 0.0038 + 120.0 0.0329 0.0037 + 130.0 0.0187 0.0024 + 140.0 0.0104 0.0019 + 145.0 0.0127 0.0021 +ENDDATA 34 +ENDSUBENT 49 +SUBENT E1892004 20050914 20050914 E032 +BIB 4 7 +REL-REF (A,B0127003,S.D.Schery+,J,NIM,147,(2),399,197712) +REACTION (3-LI-7(P,N)4-BE-7,PAR,DA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.0,SPIN=1.5,PARITY=-1.) + (4-BE-7,E-LVL=0.429,SPIN=0.5,PARITY=-1.) +ENDBIB 7 +COMMON 2 3 +E-LVL E-LVL +MEV MEV + 0.0 0.429 +ENDCOMMON 3 +DATA 2 32 +ANG DATA +ADEG MB/SR + 0.0 32.661 + 3.0 31.664 + 5.0 29.655 + 10.0 24.813 + 12.5 21.079 + 15.0 16.857 + 17.5 14.002 + 20.0 11.097 + 22.5 8.806 + 25.0 6.948 + 30.0 4.599 + 35.0 3.510 + 40.0 3.051 + 45.0 2.750 + 50.0 2.434 + 55.0 1.931 + 60.0 1.533 + 65.0 1.125 + 70.0 0.835 + 75.0 0.590 + 80.0 0.419 + 85.0 0.345 + 90.0 0.291 + 95.0 0.234 + 100.0 0.234 + 105.0 0.194 + 110.0 0.171 + 115.0 0.147 + 120.0 0.124 + 130.0 0.0886 + 140.0 0.0711 + 145.0 0.0820 +ENDDATA 34 +ENDSUBENT 50 +ENDENTRY 4 diff --git a/exforall/E18/E1893.x4 b/exforall/E18/E1893.x4 new file mode 100644 index 000000000..4a22d8b50 --- /dev/null +++ b/exforall/E18/E1893.x4 @@ -0,0 +1,2076 @@ +ENTRY E1893 20050914 20050914 E032 +SUBENT E1893001 20050914 20050914 E032 +BIB 10 29 +TITLE Measurements of differential thick target neutron + yields and 7Be production in the Li, 9Be(d,n) + reactions for 25 MeV deuterons +AUTHOR (T.Aoki, M.Hagiwara, M.Baba, M.Sugimoto, T.Miura, + N.Kawata, A.Yamadera) +INSTITUTE (2JPNTOH) Cyclotron and Radioisotope Center + (2JPNJAE) +REFERENCE (J,NST,41,(4),399,200404) +INC-SOURCE Beam intensity is <5 nA. +SAMPLE - Target is natural. + - Chemical-form of target is element. + - Physical-form of target is solid. Metallic plate + - Target-thickness: about 7.5 mm (Li) and about 3 mm + (Be), to stop the incident beam within target + targets +FACILITY (ISOCY,2JPNTOH) K=110 MeV AVF cyclotron at Cyclotron + and Radioisotope Center +DETECTOR (SCIN) To detect neutron (NE213). Efficiency curves + were obtained by revised version of Monte Carlo + Code SCINFUL [J.K.Dickens, ORNL-6436, Oak Ridge + National Laboratory, 1988]. + (HPGE) To analyze gamma ray from target (EURICIS + MESURESE GPC50-195-R, 50% efficiency). + Efficiency was determined by Monte Carlo Code + EGS4 [W.Nelson et al., SLAC-265, Stanford + University, Stanford, 1985]. +STATUS (APRVD) Compiled file is reviewed by M.Hagiwara + (2004.05.10). +HISTORY (20040508C) Kc + On +ENDBIB 29 +COMMON 1 3 +EN +MEV + 25.0 +ENDCOMMON 3 +ENDSUBENT 36 +SUBENT E1893002 20050914 20050914 E032 +BIB 8 22 +REL-REF (A,,M.A.Lone+,J,NIM,143,(2),331,197706) + Taking into account the difference in incident energy, + the present data and those by Lone et al. are in good + agreement in most of the energy range although the + latter data are systematically higher in the few MeV + region. +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +ADD-RES (COMP) Monte-Carlo method (Simulation code McDelicious + for the Li(d,n) neutron spectrum [S.P. Simakov + et al., J. Nucl. Mater., 307-311(2002)1710].) +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 22 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 0.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 4.770E+09 3.470E+08 + 1.100E+00 4.440E+09 3.230E+08 + 1.200E+00 4.370E+09 3.170E+08 + 1.300E+00 4.270E+09 3.100E+08 + 1.400E+00 4.310E+09 3.130E+08 + 1.500E+00 4.120E+09 2.990E+08 + 1.600E+00 4.160E+09 3.020E+08 + 1.700E+00 3.960E+09 2.880E+08 + 1.800E+00 3.910E+09 2.840E+08 + 1.900E+00 4.000E+09 2.910E+08 + 2.000E+00 3.870E+09 2.810E+08 + 2.100E+00 3.890E+09 2.830E+08 + 2.200E+00 3.900E+09 2.830E+08 + 2.300E+00 3.830E+09 2.780E+08 + 2.400E+00 3.880E+09 2.820E+08 + 2.500E+00 3.900E+09 2.840E+08 + 2.600E+00 3.940E+09 2.870E+08 + 2.700E+00 3.960E+09 2.880E+08 + 2.800E+00 4.030E+09 2.930E+08 + 2.900E+00 4.000E+09 2.910E+08 + 3.000E+00 4.090E+09 2.970E+08 + 3.100E+00 4.230E+09 3.070E+08 + 3.200E+00 4.330E+09 3.150E+08 + 3.300E+00 4.360E+09 3.170E+08 + 3.400E+00 4.440E+09 3.230E+08 + 3.500E+00 4.570E+09 3.320E+08 + 3.600E+00 4.580E+09 3.330E+08 + 3.700E+00 4.610E+09 3.360E+08 + 3.800E+00 4.780E+09 3.480E+08 + 3.900E+00 4.850E+09 3.530E+08 + 4.000E+00 4.940E+09 3.590E+08 + 4.100E+00 5.100E+09 3.700E+08 + 4.200E+00 5.220E+09 3.790E+08 + 4.300E+00 5.220E+09 3.790E+08 + 4.400E+00 5.260E+09 3.820E+08 + 4.500E+00 5.220E+09 3.800E+08 + 4.600E+00 5.290E+09 3.840E+08 + 4.700E+00 5.090E+09 3.700E+08 + 4.800E+00 5.070E+09 3.680E+08 + 4.900E+00 4.960E+09 3.610E+08 + 5.000E+00 4.920E+09 3.580E+08 + 6.000E+00 6.780E+09 4.870E+08 + 7.000E+00 7.610E+09 5.470E+08 + 8.000E+00 8.590E+09 6.170E+08 + 9.000E+00 9.260E+09 6.650E+08 + 1.000E+01 9.640E+09 6.930E+08 + 1.100E+01 9.190E+09 6.600E+08 + 1.200E+01 8.600E+09 6.180E+08 + 1.300E+01 7.590E+09 5.450E+08 + 1.400E+01 6.300E+09 4.530E+08 + 1.500E+01 5.030E+09 3.610E+08 + 1.600E+01 3.790E+09 2.730E+08 + 1.700E+01 2.700E+09 1.950E+08 + 1.800E+01 1.880E+09 1.360E+08 + 1.900E+01 1.320E+09 9.590E+07 + 2.000E+01 8.740E+08 6.360E+07 + 2.100E+01 5.750E+08 4.220E+07 + 2.200E+01 3.620E+08 2.690E+07 + 2.300E+01 1.250E+08 9.800E+06 + 2.400E+01 7.720E+07 6.380E+06 + 2.500E+01 8.010E+07 6.580E+06 + 2.600E+01 7.330E+07 6.100E+06 + 2.700E+01 5.840E+07 5.020E+06 + 2.800E+01 4.060E+07 3.720E+06 + 2.900E+01 3.630E+07 3.400E+06 + 3.000E+01 3.230E+07 3.100E+06 + 3.100E+01 2.840E+07 2.820E+06 + 3.200E+01 2.820E+07 2.810E+06 + 3.300E+01 2.940E+07 2.910E+06 + 3.400E+01 2.610E+07 2.660E+06 + 3.500E+01 2.120E+07 2.300E+06 + 3.600E+01 1.710E+07 1.980E+06 + 3.700E+01 8.560E+06 1.280E+06 + 3.800E+01 5.840E+06 1.020E+06 + 3.900E+01 2.520E+06 6.630E+05 + 4.000E+01 1.390E+06 5.060E+05 + 4.100E+01 5.920E+05 3.650E+05 + 4.200E+01 2.170E+05 2.750E+05 +ENDDATA 80 +ENDSUBENT 111 +SUBENT E1893003 20050914 20050914 E032 +BIB 6 13 +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 5.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 4.770E+09 3.470E+08 + 1.100E+00 4.550E+09 3.310E+08 + 1.200E+00 4.470E+09 3.250E+08 + 1.300E+00 4.120E+09 3.000E+08 + 1.400E+00 4.280E+09 3.110E+08 + 1.500E+00 3.990E+09 2.900E+08 + 1.600E+00 4.130E+09 3.010E+08 + 1.700E+00 3.930E+09 2.860E+08 + 1.800E+00 3.850E+09 2.800E+08 + 1.900E+00 3.830E+09 2.790E+08 + 2.000E+00 3.770E+09 2.740E+08 + 2.100E+00 3.710E+09 2.700E+08 + 2.200E+00 3.740E+09 2.720E+08 + 2.300E+00 3.720E+09 2.710E+08 + 2.400E+00 3.670E+09 2.680E+08 + 2.500E+00 3.770E+09 2.750E+08 + 2.600E+00 3.710E+09 2.710E+08 + 2.700E+00 3.770E+09 2.740E+08 + 2.800E+00 3.840E+09 2.800E+08 + 2.900E+00 3.830E+09 2.790E+08 + 3.000E+00 3.870E+09 2.820E+08 + 3.100E+00 3.880E+09 2.830E+08 + 3.200E+00 4.090E+09 2.980E+08 + 3.300E+00 4.070E+09 2.960E+08 + 3.400E+00 4.060E+09 2.960E+08 + 3.500E+00 4.170E+09 3.040E+08 + 3.600E+00 4.330E+09 3.160E+08 + 3.700E+00 4.380E+09 3.190E+08 + 3.800E+00 4.330E+09 3.160E+08 + 3.900E+00 4.480E+09 3.270E+08 + 4.000E+00 4.520E+09 3.300E+08 + 4.100E+00 4.580E+09 3.340E+08 + 4.200E+00 4.820E+09 3.510E+08 + 4.300E+00 4.760E+09 3.470E+08 + 4.400E+00 4.710E+09 3.430E+08 + 4.500E+00 4.750E+09 3.460E+08 + 4.600E+00 4.760E+09 3.470E+08 + 4.700E+00 4.560E+09 3.330E+08 + 4.800E+00 4.560E+09 3.330E+08 + 4.900E+00 4.490E+09 3.280E+08 + 5.000E+00 4.400E+09 3.210E+08 + 6.000E+00 5.450E+09 3.920E+08 + 7.000E+00 5.920E+09 4.260E+08 + 8.000E+00 6.600E+09 4.750E+08 + 9.000E+00 7.020E+09 5.050E+08 + 1.000E+01 7.180E+09 5.170E+08 + 1.100E+01 6.810E+09 4.900E+08 + 1.200E+01 6.360E+09 4.580E+08 + 1.300E+01 5.670E+09 4.080E+08 + 1.400E+01 4.750E+09 3.420E+08 + 1.500E+01 3.800E+09 2.740E+08 + 1.600E+01 2.940E+09 2.120E+08 + 1.700E+01 2.110E+09 1.520E+08 + 1.800E+01 1.500E+09 1.090E+08 + 1.900E+01 1.070E+09 7.730E+07 + 2.000E+01 7.200E+08 5.240E+07 + 2.100E+01 4.920E+08 3.600E+07 + 2.200E+01 2.820E+08 2.100E+07 + 2.300E+01 1.200E+08 9.310E+06 + 2.400E+01 9.300E+07 7.320E+06 + 2.500E+01 8.700E+07 6.890E+06 + 2.600E+01 8.470E+07 6.730E+06 + 2.700E+01 6.920E+07 5.610E+06 + 2.800E+01 6.380E+07 5.210E+06 + 2.900E+01 5.520E+07 4.600E+06 + 3.000E+01 5.130E+07 4.310E+06 + 3.100E+01 5.480E+07 4.570E+06 + 3.200E+01 5.060E+07 4.270E+06 + 3.300E+01 5.330E+07 4.480E+06 + 3.400E+01 5.320E+07 4.470E+06 + 3.500E+01 4.990E+07 4.240E+06 + 3.600E+01 3.660E+07 3.280E+06 + 3.700E+01 2.000E+07 2.050E+06 + 3.800E+01 1.230E+07 1.450E+06 + 3.900E+01 6.080E+06 9.390E+05 + 4.000E+01 1.620E+06 4.770E+05 + 4.100E+01 1.400E+06 4.510E+05 + 4.200E+01 1.170E+05 2.270E+05 +ENDDATA 80 +ENDSUBENT 102 +SUBENT E1893004 20050914 20050914 E032 +BIB 6 13 +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 10.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 5.520E+09 4.020E+08 + 1.100E+00 5.120E+09 3.730E+08 + 1.200E+00 4.970E+09 3.620E+08 + 1.300E+00 4.680E+09 3.410E+08 + 1.400E+00 4.660E+09 3.400E+08 + 1.500E+00 4.420E+09 3.220E+08 + 1.600E+00 4.550E+09 3.320E+08 + 1.700E+00 4.350E+09 3.170E+08 + 1.800E+00 4.370E+09 3.190E+08 + 1.900E+00 4.180E+09 3.050E+08 + 2.000E+00 4.160E+09 3.030E+08 + 2.100E+00 4.050E+09 2.950E+08 + 2.200E+00 4.070E+09 2.970E+08 + 2.300E+00 3.970E+09 2.900E+08 + 2.400E+00 4.020E+09 2.930E+08 + 2.500E+00 4.030E+09 2.940E+08 + 2.600E+00 4.110E+09 3.000E+08 + 2.700E+00 4.100E+09 2.990E+08 + 2.800E+00 4.070E+09 2.970E+08 + 2.900E+00 4.110E+09 3.000E+08 + 3.000E+00 4.100E+09 2.990E+08 + 3.100E+00 4.170E+09 3.050E+08 + 3.200E+00 4.280E+09 3.120E+08 + 3.300E+00 4.320E+09 3.150E+08 + 3.400E+00 4.320E+09 3.150E+08 + 3.500E+00 4.410E+09 3.220E+08 + 3.600E+00 4.510E+09 3.290E+08 + 3.700E+00 4.410E+09 3.220E+08 + 3.800E+00 4.560E+09 3.330E+08 + 3.900E+00 4.640E+09 3.380E+08 + 4.000E+00 4.630E+09 3.380E+08 + 4.100E+00 4.540E+09 3.310E+08 + 4.200E+00 4.690E+09 3.420E+08 + 4.300E+00 4.740E+09 3.460E+08 + 4.400E+00 4.720E+09 3.450E+08 + 4.500E+00 4.700E+09 3.430E+08 + 4.600E+00 4.740E+09 3.460E+08 + 4.700E+00 4.540E+09 3.310E+08 + 4.800E+00 4.380E+09 3.200E+08 + 4.900E+00 4.410E+09 3.220E+08 + 5.000E+00 4.300E+09 3.140E+08 + 6.000E+00 4.230E+09 3.060E+08 + 7.000E+00 4.360E+09 3.160E+08 + 8.000E+00 4.570E+09 3.310E+08 + 9.000E+00 4.630E+09 3.350E+08 + 1.000E+01 4.660E+09 3.370E+08 + 1.100E+01 4.330E+09 3.130E+08 + 1.200E+01 4.070E+09 2.940E+08 + 1.300E+01 3.700E+09 2.680E+08 + 1.400E+01 3.200E+09 2.320E+08 + 1.500E+01 2.640E+09 1.910E+08 + 1.600E+01 2.140E+09 1.550E+08 + 1.700E+01 1.620E+09 1.180E+08 + 1.800E+01 1.200E+09 8.710E+07 + 1.900E+01 8.880E+08 6.470E+07 + 2.000E+01 6.200E+08 4.530E+07 + 2.100E+01 4.480E+08 3.290E+07 + 2.200E+01 2.870E+08 2.130E+07 + 2.300E+01 1.350E+08 1.030E+07 + 2.400E+01 1.190E+08 9.120E+06 + 2.500E+01 1.240E+08 9.510E+06 + 2.600E+01 1.340E+08 1.020E+07 + 2.700E+01 1.170E+08 8.980E+06 + 2.800E+01 1.100E+08 8.500E+06 + 2.900E+01 1.170E+08 9.020E+06 + 3.000E+01 1.210E+08 9.250E+06 + 3.100E+01 1.190E+08 9.170E+06 + 3.200E+01 1.290E+08 9.900E+06 + 3.300E+01 1.320E+08 1.010E+07 + 3.400E+01 1.330E+08 1.020E+07 + 3.500E+01 1.160E+08 8.940E+06 + 3.600E+01 9.070E+07 7.120E+06 + 3.700E+01 5.260E+07 4.360E+06 + 3.800E+01 3.480E+07 3.060E+06 + 3.900E+01 1.680E+07 1.720E+06 + 4.000E+01 5.590E+06 8.220E+05 + 4.100E+01 1.410E+06 3.920E+05 + 4.200E+01 3.310E+05 2.140E+05 +ENDDATA 80 +ENDSUBENT 102 +SUBENT E1893005 20050914 20050914 E032 +BIB 6 13 +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 15.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 3.880E+09 2.850E+08 + 1.100E+00 3.600E+09 2.640E+08 + 1.200E+00 3.460E+09 2.540E+08 + 1.300E+00 3.270E+09 2.400E+08 + 1.400E+00 3.310E+09 2.430E+08 + 1.500E+00 3.150E+09 2.320E+08 + 1.600E+00 3.200E+09 2.350E+08 + 1.700E+00 3.010E+09 2.210E+08 + 1.800E+00 2.950E+09 2.170E+08 + 1.900E+00 2.920E+09 2.150E+08 + 2.000E+00 2.910E+09 2.140E+08 + 2.100E+00 2.770E+09 2.040E+08 + 2.200E+00 2.810E+09 2.070E+08 + 2.300E+00 2.760E+09 2.030E+08 + 2.400E+00 2.710E+09 1.990E+08 + 2.500E+00 2.740E+09 2.020E+08 + 2.600E+00 2.700E+09 1.980E+08 + 2.700E+00 2.720E+09 2.000E+08 + 2.800E+00 2.760E+09 2.030E+08 + 2.900E+00 2.750E+09 2.020E+08 + 3.000E+00 2.760E+09 2.030E+08 + 3.100E+00 2.750E+09 2.030E+08 + 3.200E+00 2.760E+09 2.030E+08 + 3.300E+00 2.800E+09 2.060E+08 + 3.400E+00 2.770E+09 2.040E+08 + 3.500E+00 2.820E+09 2.070E+08 + 3.600E+00 2.780E+09 2.050E+08 + 3.700E+00 2.850E+09 2.100E+08 + 3.800E+00 2.830E+09 2.080E+08 + 3.900E+00 2.810E+09 2.070E+08 + 4.000E+00 2.810E+09 2.070E+08 + 4.100E+00 2.800E+09 2.060E+08 + 4.200E+00 2.920E+09 2.150E+08 + 4.300E+00 2.880E+09 2.120E+08 + 4.400E+00 2.840E+09 2.100E+08 + 4.500E+00 2.820E+09 2.080E+08 + 4.600E+00 2.710E+09 2.000E+08 + 4.700E+00 2.650E+09 1.950E+08 + 4.800E+00 2.570E+09 1.900E+08 + 4.900E+00 2.490E+09 1.840E+08 + 5.000E+00 2.440E+09 1.800E+08 + 6.000E+00 3.470E+09 2.530E+08 + 7.000E+00 3.330E+09 2.430E+08 + 8.000E+00 3.260E+09 2.380E+08 + 9.000E+00 3.180E+09 2.320E+08 + 1.000E+01 3.060E+09 2.240E+08 + 1.100E+01 2.800E+09 2.050E+08 + 1.200E+01 2.590E+09 1.890E+08 + 1.300E+01 2.350E+09 1.720E+08 + 1.400E+01 2.080E+09 1.520E+08 + 1.500E+01 1.780E+09 1.300E+08 + 1.600E+01 1.450E+09 1.060E+08 + 1.700E+01 1.120E+09 8.190E+07 + 1.800E+01 8.670E+08 6.360E+07 + 1.900E+01 6.800E+08 4.990E+07 + 2.000E+01 4.920E+08 3.620E+07 + 2.100E+01 3.830E+08 2.830E+07 + 2.200E+01 2.610E+08 1.940E+07 + 2.300E+01 1.620E+08 1.210E+07 + 2.400E+01 1.520E+08 1.150E+07 + 2.500E+01 1.540E+08 1.160E+07 + 2.600E+01 1.530E+08 1.150E+07 + 2.700E+01 1.540E+08 1.160E+07 + 2.800E+01 1.520E+08 1.150E+07 + 2.900E+01 1.540E+08 1.160E+07 + 3.000E+01 1.560E+08 1.170E+07 + 3.100E+01 1.620E+08 1.210E+07 + 3.200E+01 1.630E+08 1.230E+07 + 3.300E+01 1.740E+08 1.300E+07 + 3.400E+01 1.600E+08 1.210E+07 + 3.500E+01 1.440E+08 1.090E+07 + 3.600E+01 1.020E+08 7.810E+06 + 3.700E+01 5.720E+07 4.540E+06 + 3.800E+01 3.750E+07 3.100E+06 + 3.900E+01 2.080E+07 1.870E+06 + 4.000E+01 4.420E+06 6.140E+05 + 4.100E+01 1.810E+06 3.730E+05 + 4.200E+01 1.070E+06 2.900E+05 +ENDDATA 80 +ENDSUBENT 102 +SUBENT E1893006 20050914 20050914 E032 +BIB 7 16 +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +ADD-RES (COMP) Monte-Carlo method (Simulation code McDelicious + for the Li(d,n) neutron spectrum [S.P. Simakov + et al., J. Nucl. Mater., 307-311(2002)1710].) +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 16 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 20.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 5.240E+09 3.890E+08 + 1.100E+00 4.810E+09 3.570E+08 + 1.200E+00 4.610E+09 3.420E+08 + 1.300E+00 4.420E+09 3.280E+08 + 1.400E+00 4.280E+09 3.180E+08 + 1.500E+00 4.140E+09 3.080E+08 + 1.600E+00 4.160E+09 3.090E+08 + 1.700E+00 3.900E+09 2.900E+08 + 1.800E+00 3.870E+09 2.870E+08 + 1.900E+00 3.720E+09 2.770E+08 + 2.000E+00 3.680E+09 2.740E+08 + 2.100E+00 3.630E+09 2.700E+08 + 2.200E+00 3.570E+09 2.650E+08 + 2.300E+00 3.510E+09 2.610E+08 + 2.400E+00 3.510E+09 2.610E+08 + 2.500E+00 3.460E+09 2.580E+08 + 2.600E+00 3.430E+09 2.550E+08 + 2.700E+00 3.400E+09 2.530E+08 + 2.800E+00 3.390E+09 2.520E+08 + 2.900E+00 3.330E+09 2.480E+08 + 3.000E+00 3.360E+09 2.500E+08 + 3.100E+00 3.340E+09 2.490E+08 + 3.200E+00 3.470E+09 2.590E+08 + 3.300E+00 3.400E+09 2.530E+08 + 3.400E+00 3.360E+09 2.500E+08 + 3.500E+00 3.370E+09 2.510E+08 + 3.600E+00 3.390E+09 2.530E+08 + 3.700E+00 3.360E+09 2.500E+08 + 3.800E+00 3.360E+09 2.500E+08 + 3.900E+00 3.420E+09 2.550E+08 + 4.000E+00 3.350E+09 2.500E+08 + 4.100E+00 3.320E+09 2.470E+08 + 4.200E+00 3.400E+09 2.540E+08 + 4.300E+00 3.340E+09 2.490E+08 + 4.400E+00 3.350E+09 2.500E+08 + 4.500E+00 3.290E+09 2.450E+08 + 4.600E+00 3.290E+09 2.450E+08 + 4.700E+00 3.130E+09 2.340E+08 + 4.800E+00 3.050E+09 2.270E+08 + 4.900E+00 2.890E+09 2.160E+08 + 5.000E+00 2.840E+09 2.130E+08 + 6.000E+00 2.510E+09 1.860E+08 + 7.000E+00 2.280E+09 1.690E+08 + 8.000E+00 2.150E+09 1.590E+08 + 9.000E+00 1.990E+09 1.470E+08 + 1.000E+01 1.870E+09 1.380E+08 + 1.100E+01 1.680E+09 1.240E+08 + 1.200E+01 1.560E+09 1.150E+08 + 1.300E+01 1.400E+09 1.040E+08 + 1.400E+01 1.230E+09 9.100E+07 + 1.500E+01 1.050E+09 7.800E+07 + 1.600E+01 8.610E+08 6.380E+07 + 1.700E+01 6.630E+08 4.930E+07 + 1.800E+01 5.380E+08 4.000E+07 + 1.900E+01 4.100E+08 3.050E+07 + 2.000E+01 3.200E+08 2.390E+07 + 2.100E+01 2.540E+08 1.900E+07 + 2.200E+01 1.610E+08 1.220E+07 + 2.300E+01 1.400E+08 1.060E+07 + 2.400E+01 1.420E+08 1.080E+07 + 2.500E+01 1.430E+08 1.080E+07 + 2.600E+01 1.490E+08 1.120E+07 + 2.700E+01 1.380E+08 1.040E+07 + 2.800E+01 1.450E+08 1.100E+07 + 2.900E+01 1.500E+08 1.140E+07 + 3.000E+01 1.470E+08 1.110E+07 + 3.100E+01 1.540E+08 1.160E+07 + 3.200E+01 1.500E+08 1.140E+07 + 3.300E+01 1.430E+08 1.090E+07 + 3.400E+01 1.300E+08 9.860E+06 + 3.500E+01 9.140E+07 7.030E+06 + 3.600E+01 5.190E+07 4.110E+06 + 3.700E+01 3.120E+07 2.580E+06 + 3.800E+01 1.900E+07 1.670E+06 + 3.900E+01 4.830E+06 5.930E+05 + 4.000E+01 1.510E+06 2.980E+05 + 4.100E+01 9.400E+05 2.360E+05 + 4.200E+01 6.730E+05 2.030E+05 +ENDDATA 80 +ENDSUBENT 105 +SUBENT E1893007 20050914 20050914 E032 +BIB 6 13 +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 25.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 5.140E+09 3.890E+08 + 1.100E+00 4.720E+09 3.570E+08 + 1.200E+00 4.520E+09 3.420E+08 + 1.300E+00 4.320E+09 3.270E+08 + 1.400E+00 4.200E+09 3.180E+08 + 1.500E+00 4.050E+09 3.060E+08 + 1.600E+00 3.980E+09 3.010E+08 + 1.700E+00 3.800E+09 2.870E+08 + 1.800E+00 3.670E+09 2.780E+08 + 1.900E+00 3.570E+09 2.700E+08 + 2.000E+00 3.510E+09 2.650E+08 + 2.100E+00 3.450E+09 2.610E+08 + 2.200E+00 3.450E+09 2.610E+08 + 2.300E+00 3.310E+09 2.510E+08 + 2.400E+00 3.250E+09 2.460E+08 + 2.500E+00 3.230E+09 2.450E+08 + 2.600E+00 3.230E+09 2.450E+08 + 2.700E+00 3.300E+09 2.500E+08 + 2.800E+00 3.170E+09 2.400E+08 + 2.900E+00 3.090E+09 2.340E+08 + 3.000E+00 3.110E+09 2.350E+08 + 3.100E+00 3.120E+09 2.360E+08 + 3.200E+00 3.170E+09 2.400E+08 + 3.300E+00 3.130E+09 2.370E+08 + 3.400E+00 3.040E+09 2.310E+08 + 3.500E+00 3.110E+09 2.360E+08 + 3.600E+00 3.030E+09 2.300E+08 + 3.700E+00 3.010E+09 2.280E+08 + 3.800E+00 3.000E+09 2.270E+08 + 3.900E+00 2.940E+09 2.230E+08 + 4.000E+00 2.930E+09 2.220E+08 + 4.100E+00 2.950E+09 2.240E+08 + 4.200E+00 2.970E+09 2.260E+08 + 4.300E+00 2.910E+09 2.210E+08 + 4.400E+00 2.870E+09 2.180E+08 + 4.500E+00 2.800E+09 2.130E+08 + 4.600E+00 2.700E+09 2.050E+08 + 4.700E+00 2.610E+09 1.990E+08 + 4.800E+00 2.560E+09 1.950E+08 + 4.900E+00 2.460E+09 1.870E+08 + 5.000E+00 2.340E+09 1.780E+08 + 6.000E+00 2.370E+09 1.780E+08 + 7.000E+00 2.090E+09 1.570E+08 + 8.000E+00 1.900E+09 1.430E+08 + 9.000E+00 1.720E+09 1.300E+08 + 1.000E+01 1.570E+09 1.180E+08 + 1.100E+01 1.360E+09 1.020E+08 + 1.200E+01 1.220E+09 9.170E+07 + 1.300E+01 1.070E+09 8.050E+07 + 1.400E+01 9.190E+08 6.930E+07 + 1.500E+01 7.540E+08 5.690E+07 + 1.600E+01 6.130E+08 4.630E+07 + 1.700E+01 4.880E+08 3.690E+07 + 1.800E+01 3.940E+08 2.990E+07 + 1.900E+01 3.090E+08 2.350E+07 + 2.000E+01 2.410E+08 1.840E+07 + 2.100E+01 2.060E+08 1.570E+07 + 2.200E+01 1.390E+08 1.070E+07 + 2.300E+01 1.250E+08 9.610E+06 + 2.400E+01 1.190E+08 9.170E+06 + 2.500E+01 1.200E+08 9.260E+06 + 2.600E+01 1.190E+08 9.150E+06 + 2.700E+01 1.110E+08 8.570E+06 + 2.800E+01 1.120E+08 8.630E+06 + 2.900E+01 1.090E+08 8.410E+06 + 3.000E+01 1.050E+08 8.120E+06 + 3.100E+01 1.050E+08 8.100E+06 + 3.200E+01 9.890E+07 7.660E+06 + 3.300E+01 8.790E+07 6.830E+06 + 3.400E+01 7.860E+07 6.130E+06 + 3.500E+01 5.960E+07 4.710E+06 + 3.600E+01 3.320E+07 2.730E+06 + 3.700E+01 2.090E+07 1.790E+06 + 3.800E+01 1.310E+07 1.210E+06 + 3.900E+01 3.870E+06 4.840E+05 + 4.000E+01 1.050E+06 2.250E+05 + 4.100E+01 6.160E+05 1.750E+05 + 4.200E+01 1.690E+05 1.060E+05 +ENDDATA 80 +ENDSUBENT 102 +SUBENT E1893008 20050914 20050914 E032 +BIB 6 13 +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 30.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 3.880E+09 3.000E+08 + 1.100E+00 3.570E+09 2.760E+08 + 1.200E+00 3.340E+09 2.580E+08 + 1.300E+00 3.180E+09 2.460E+08 + 1.400E+00 3.120E+09 2.410E+08 + 1.500E+00 2.970E+09 2.300E+08 + 1.600E+00 2.950E+09 2.280E+08 + 1.700E+00 2.780E+09 2.150E+08 + 1.800E+00 2.710E+09 2.100E+08 + 1.900E+00 2.700E+09 2.090E+08 + 2.000E+00 2.610E+09 2.020E+08 + 2.100E+00 2.520E+09 1.950E+08 + 2.200E+00 2.480E+09 1.920E+08 + 2.300E+00 2.460E+09 1.900E+08 + 2.400E+00 2.420E+09 1.870E+08 + 2.500E+00 2.410E+09 1.860E+08 + 2.600E+00 2.400E+09 1.860E+08 + 2.700E+00 2.360E+09 1.830E+08 + 2.800E+00 2.330E+09 1.800E+08 + 2.900E+00 2.300E+09 1.780E+08 + 3.000E+00 2.280E+09 1.770E+08 + 3.100E+00 2.310E+09 1.790E+08 + 3.200E+00 2.340E+09 1.820E+08 + 3.300E+00 2.270E+09 1.760E+08 + 3.400E+00 2.260E+09 1.750E+08 + 3.500E+00 2.220E+09 1.720E+08 + 3.600E+00 2.200E+09 1.700E+08 + 3.700E+00 2.210E+09 1.720E+08 + 3.800E+00 2.170E+09 1.690E+08 + 3.900E+00 2.170E+09 1.680E+08 + 4.000E+00 2.140E+09 1.660E+08 + 4.100E+00 2.150E+09 1.670E+08 + 4.200E+00 2.110E+09 1.640E+08 + 4.300E+00 2.140E+09 1.660E+08 + 4.400E+00 2.090E+09 1.620E+08 + 4.500E+00 2.060E+09 1.600E+08 + 4.600E+00 2.020E+09 1.570E+08 + 4.700E+00 1.940E+09 1.510E+08 + 4.800E+00 1.910E+09 1.490E+08 + 4.900E+00 1.810E+09 1.400E+08 + 5.000E+00 1.740E+09 1.350E+08 + 6.000E+00 1.790E+09 1.380E+08 + 7.000E+00 1.600E+09 1.230E+08 + 8.000E+00 1.450E+09 1.120E+08 + 9.000E+00 1.290E+09 9.950E+07 + 1.000E+01 1.160E+09 8.910E+07 + 1.100E+01 9.770E+08 7.530E+07 + 1.200E+01 8.510E+08 6.560E+07 + 1.300E+01 7.150E+08 5.520E+07 + 1.400E+01 5.950E+08 4.590E+07 + 1.500E+01 4.780E+08 3.690E+07 + 1.600E+01 3.760E+08 2.910E+07 + 1.700E+01 2.970E+08 2.300E+07 + 1.800E+01 2.380E+08 1.850E+07 + 1.900E+01 1.850E+08 1.440E+07 + 2.000E+01 1.540E+08 1.210E+07 + 2.100E+01 1.170E+08 9.190E+06 + 2.200E+01 9.040E+07 7.130E+06 + 2.300E+01 8.030E+07 6.350E+06 + 2.400E+01 8.160E+07 6.450E+06 + 2.500E+01 7.850E+07 6.210E+06 + 2.600E+01 7.150E+07 5.670E+06 + 2.700E+01 6.730E+07 5.350E+06 + 2.800E+01 6.500E+07 5.170E+06 + 2.900E+01 6.250E+07 4.980E+06 + 3.000E+01 5.760E+07 4.600E+06 + 3.100E+01 5.380E+07 4.310E+06 + 3.200E+01 4.890E+07 3.940E+06 + 3.300E+01 4.450E+07 3.600E+06 + 3.400E+01 3.260E+07 2.680E+06 + 3.500E+01 1.890E+07 1.630E+06 + 3.600E+01 1.050E+07 9.780E+05 + 3.700E+01 6.940E+06 6.990E+05 + 3.800E+01 2.770E+06 3.580E+05 + 3.900E+01 6.160E+05 1.500E+05 + 4.000E+01 4.250E+05 1.260E+05 + 4.100E+01 2.510E+05 1.000E+05 + 4.200E+01 1.970E+05 9.130E+04 +ENDDATA 80 +ENDSUBENT 102 +SUBENT E1893009 20050914 20050914 E032 +BIB 6 13 +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 40.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 3.770E+09 3.120E+08 + 1.100E+00 3.470E+09 2.870E+08 + 1.200E+00 3.310E+09 2.740E+08 + 1.300E+00 3.150E+09 2.610E+08 + 1.400E+00 3.090E+09 2.560E+08 + 1.500E+00 2.930E+09 2.430E+08 + 1.600E+00 2.890E+09 2.400E+08 + 1.700E+00 2.760E+09 2.290E+08 + 1.800E+00 2.660E+09 2.200E+08 + 1.900E+00 2.650E+09 2.190E+08 + 2.000E+00 2.590E+09 2.140E+08 + 2.100E+00 2.500E+09 2.070E+08 + 2.200E+00 2.480E+09 2.060E+08 + 2.300E+00 2.430E+09 2.010E+08 + 2.400E+00 2.410E+09 1.990E+08 + 2.500E+00 2.380E+09 1.970E+08 + 2.600E+00 2.350E+09 1.940E+08 + 2.700E+00 2.340E+09 1.940E+08 + 2.800E+00 2.260E+09 1.880E+08 + 2.900E+00 2.260E+09 1.870E+08 + 3.000E+00 2.200E+09 1.820E+08 + 3.100E+00 2.200E+09 1.830E+08 + 3.200E+00 2.220E+09 1.840E+08 + 3.300E+00 2.200E+09 1.830E+08 + 3.400E+00 2.210E+09 1.830E+08 + 3.500E+00 2.130E+09 1.770E+08 + 3.600E+00 2.110E+09 1.750E+08 + 3.700E+00 2.060E+09 1.710E+08 + 3.800E+00 2.070E+09 1.720E+08 + 3.900E+00 2.060E+09 1.710E+08 + 4.000E+00 2.050E+09 1.710E+08 + 4.100E+00 2.030E+09 1.690E+08 + 4.200E+00 2.060E+09 1.710E+08 + 4.300E+00 1.980E+09 1.650E+08 + 4.400E+00 1.930E+09 1.610E+08 + 4.500E+00 1.920E+09 1.600E+08 + 4.600E+00 1.870E+09 1.550E+08 + 4.700E+00 1.800E+09 1.500E+08 + 4.800E+00 1.760E+09 1.470E+08 + 4.900E+00 1.700E+09 1.410E+08 + 5.000E+00 1.630E+09 1.360E+08 + 6.000E+00 1.510E+09 1.250E+08 + 7.000E+00 1.330E+09 1.100E+08 + 8.000E+00 1.170E+09 9.680E+07 + 9.000E+00 1.010E+09 8.330E+07 + 1.000E+01 8.690E+08 7.160E+07 + 1.100E+01 7.090E+08 5.850E+07 + 1.200E+01 6.010E+08 4.960E+07 + 1.300E+01 5.020E+08 4.150E+07 + 1.400E+01 3.990E+08 3.300E+07 + 1.500E+01 3.130E+08 2.590E+07 + 1.600E+01 2.490E+08 2.060E+07 + 1.700E+01 2.010E+08 1.670E+07 + 1.800E+01 1.500E+08 1.250E+07 + 1.900E+01 1.190E+08 9.960E+06 + 2.000E+01 9.970E+07 8.340E+06 + 2.100E+01 7.200E+07 6.060E+06 + 2.200E+01 5.990E+07 5.050E+06 + 2.300E+01 5.530E+07 4.670E+06 + 2.400E+01 5.180E+07 4.390E+06 + 2.500E+01 4.590E+07 3.900E+06 + 2.600E+01 4.170E+07 3.550E+06 + 2.700E+01 3.950E+07 3.380E+06 + 2.800E+01 3.710E+07 3.170E+06 + 2.900E+01 3.760E+07 3.220E+06 + 3.000E+01 3.730E+07 3.190E+06 + 3.100E+01 3.620E+07 3.100E+06 + 3.200E+01 3.720E+07 3.190E+06 + 3.300E+01 3.350E+07 2.880E+06 + 3.400E+01 2.810E+07 2.440E+06 + 3.500E+01 1.890E+07 1.680E+06 + 3.600E+01 1.190E+07 1.100E+06 + 3.700E+01 7.160E+06 7.110E+05 + 3.800E+01 2.700E+06 3.310E+05 + 3.900E+01 6.210E+05 1.340E+05 + 4.000E+01 1.380E+05 6.880E+04 + 4.100E+01 1.200E+05 6.600E+04 + 4.200E+01 1.340E+05 6.870E+04 +ENDDATA 80 +ENDSUBENT 102 +SUBENT E1893010 20050914 20050914 E032 +BIB 7 16 +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +ADD-RES (COMP) Monte-Carlo method (Simulation code McDelicious + for the Li(d,n) neutron spectrum [S.P. Simakov + et al., J. Nucl. Mater., 307-311(2002)1710].) +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 16 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 60.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 3.340E+09 3.710E+08 + 1.100E+00 3.190E+09 3.550E+08 + 1.200E+00 3.020E+09 3.360E+08 + 1.300E+00 2.870E+09 3.190E+08 + 1.400E+00 2.900E+09 3.220E+08 + 1.500E+00 2.710E+09 3.020E+08 + 1.600E+00 2.760E+09 3.070E+08 + 1.700E+00 2.570E+09 2.860E+08 + 1.800E+00 2.530E+09 2.820E+08 + 1.900E+00 2.450E+09 2.720E+08 + 2.000E+00 2.390E+09 2.660E+08 + 2.100E+00 2.380E+09 2.650E+08 + 2.200E+00 2.350E+09 2.610E+08 + 2.300E+00 2.270E+09 2.530E+08 + 2.400E+00 2.270E+09 2.530E+08 + 2.500E+00 2.270E+09 2.530E+08 + 2.600E+00 2.210E+09 2.460E+08 + 2.700E+00 2.150E+09 2.400E+08 + 2.800E+00 2.120E+09 2.360E+08 + 2.900E+00 2.030E+09 2.260E+08 + 3.000E+00 2.040E+09 2.270E+08 + 3.100E+00 1.990E+09 2.210E+08 + 3.200E+00 1.960E+09 2.180E+08 + 3.300E+00 1.930E+09 2.150E+08 + 3.400E+00 1.910E+09 2.130E+08 + 3.500E+00 1.870E+09 2.090E+08 + 3.600E+00 1.820E+09 2.030E+08 + 3.700E+00 1.790E+09 1.990E+08 + 3.800E+00 1.770E+09 1.970E+08 + 3.900E+00 1.720E+09 1.920E+08 + 4.000E+00 1.670E+09 1.860E+08 + 4.100E+00 1.640E+09 1.830E+08 + 4.200E+00 1.620E+09 1.810E+08 + 4.300E+00 1.590E+09 1.770E+08 + 4.400E+00 1.530E+09 1.700E+08 + 4.500E+00 1.460E+09 1.630E+08 + 4.600E+00 1.370E+09 1.530E+08 + 4.700E+00 1.310E+09 1.460E+08 + 4.800E+00 1.260E+09 1.410E+08 + 4.900E+00 1.170E+09 1.300E+08 + 5.000E+00 1.110E+09 1.240E+08 + 6.000E+00 8.960E+08 9.950E+07 + 7.000E+00 7.160E+08 7.950E+07 + 8.000E+00 5.720E+08 6.360E+07 + 9.000E+00 4.580E+08 5.090E+07 + 1.000E+01 3.660E+08 4.070E+07 + 1.100E+01 2.880E+08 3.200E+07 + 1.200E+01 2.380E+08 2.650E+07 + 1.300E+01 1.960E+08 2.180E+07 + 1.400E+01 1.590E+08 1.770E+07 + 1.500E+01 1.290E+08 1.440E+07 + 1.600E+01 9.810E+07 1.090E+07 + 1.700E+01 7.720E+07 8.620E+06 + 1.800E+01 6.620E+07 7.400E+06 + 1.900E+01 5.720E+07 6.390E+06 + 2.000E+01 5.470E+07 6.120E+06 + 2.100E+01 5.390E+07 6.030E+06 + 2.200E+01 5.150E+07 5.760E+06 + 2.300E+01 4.640E+07 5.200E+06 + 2.400E+01 4.170E+07 4.680E+06 + 2.500E+01 3.720E+07 4.180E+06 + 2.600E+01 3.290E+07 3.700E+06 + 2.700E+01 3.050E+07 3.430E+06 + 2.800E+01 2.700E+07 3.040E+06 + 2.900E+01 2.440E+07 2.750E+06 + 3.000E+01 2.200E+07 2.490E+06 + 3.100E+01 1.750E+07 1.990E+06 + 3.200E+01 1.190E+07 1.370E+06 + 3.300E+01 6.080E+06 7.210E+05 + 3.400E+01 3.620E+06 4.470E+05 + 3.500E+01 2.120E+06 2.810E+05 + 3.600E+01 6.700E+05 1.150E+05 + 3.700E+01 2.920E+05 6.870E+04 + 3.800E+01 1.140E+05 4.310E+04 + 3.900E+01 1.030E+05 4.140E+04 + 4.000E+01 2.380E+04 2.640E+04 + 4.100E+01 1.030E+05 4.190E+04 + 4.200E+01 6.980E+04 3.590E+04 +ENDDATA 80 +ENDSUBENT 105 +SUBENT E1893011 20050914 20050914 E032 +BIB 7 16 +REACTION (3-LI-7(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +ADD-RES (COMP) Monte-Carlo method (Simulation code McDelicious + for the Li(d,n) neutron spectrum [S.P. Simakov + et al., J. Nucl. Mater., 307-311(2002)1710].) +STATUS (TABLE) Data (Fig.3, p402 in reference) received by + e-mail from M.Hagiwara (2004.3.13) +ENDBIB 16 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 90.0 5.0 +ENDCOMMON 3 +DATA 3 78 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 2.640E+09 1.530E+08 + 1.100E+00 2.480E+09 1.440E+08 + 1.200E+00 2.340E+09 1.360E+08 + 1.300E+00 2.270E+09 1.320E+08 + 1.400E+00 2.220E+09 1.290E+08 + 1.500E+00 2.160E+09 1.250E+08 + 1.600E+00 2.180E+09 1.260E+08 + 1.700E+00 2.040E+09 1.180E+08 + 1.800E+00 2.040E+09 1.190E+08 + 1.900E+00 1.960E+09 1.140E+08 + 2.000E+00 1.890E+09 1.100E+08 + 2.100E+00 1.840E+09 1.070E+08 + 2.200E+00 1.820E+09 1.060E+08 + 2.300E+00 1.760E+09 1.020E+08 + 2.400E+00 1.740E+09 1.010E+08 + 2.500E+00 1.710E+09 9.910E+07 + 2.600E+00 1.640E+09 9.550E+07 + 2.700E+00 1.610E+09 9.350E+07 + 2.800E+00 1.580E+09 9.210E+07 + 2.900E+00 1.520E+09 8.870E+07 + 3.000E+00 1.460E+09 8.500E+07 + 3.100E+00 1.420E+09 8.290E+07 + 3.200E+00 1.410E+09 8.250E+07 + 3.300E+00 1.360E+09 7.960E+07 + 3.400E+00 1.290E+09 7.550E+07 + 3.500E+00 1.250E+09 7.340E+07 + 3.600E+00 1.220E+09 7.150E+07 + 3.700E+00 1.160E+09 6.820E+07 + 3.800E+00 1.130E+09 6.610E+07 + 3.900E+00 1.060E+09 6.240E+07 + 4.000E+00 1.010E+09 5.940E+07 + 4.100E+00 9.760E+08 5.750E+07 + 4.200E+00 9.950E+08 5.860E+07 + 4.300E+00 9.230E+08 5.450E+07 + 4.400E+00 8.540E+08 5.060E+07 + 4.500E+00 8.340E+08 4.940E+07 + 4.600E+00 7.860E+08 4.670E+07 + 4.700E+00 7.370E+08 4.380E+07 + 4.800E+00 7.020E+08 4.190E+07 + 4.900E+00 6.510E+08 3.890E+07 + 5.000E+00 6.240E+08 3.740E+07 + 6.000E+00 4.050E+08 2.330E+07 + 7.000E+00 2.970E+08 1.710E+07 + 8.000E+00 2.220E+08 1.280E+07 + 9.000E+00 1.710E+08 9.860E+06 + 1.000E+01 1.320E+08 7.590E+06 + 1.100E+01 1.070E+08 6.170E+06 + 1.200E+01 9.700E+07 5.610E+06 + 1.300E+01 8.530E+07 4.940E+06 + 1.400E+01 7.310E+07 4.240E+06 + 1.500E+01 6.200E+07 3.600E+06 + 1.600E+01 4.830E+07 2.820E+06 + 1.700E+01 3.990E+07 2.330E+06 + 1.800E+01 3.370E+07 1.980E+06 + 1.900E+01 2.870E+07 1.690E+06 + 2.000E+01 2.560E+07 1.510E+06 + 2.100E+01 2.240E+07 1.330E+06 + 2.200E+01 1.930E+07 1.150E+06 + 2.300E+01 1.790E+07 1.070E+06 + 2.400E+01 1.680E+07 1.010E+06 + 2.500E+01 1.430E+07 8.580E+05 + 2.600E+01 1.220E+07 7.380E+05 + 2.700E+01 9.940E+06 6.100E+05 + 2.800E+01 6.080E+06 3.880E+05 + 2.900E+01 3.280E+06 2.260E+05 + 3.000E+01 1.780E+06 1.380E+05 + 3.100E+01 9.610E+05 8.810E+04 + 3.200E+01 2.700E+05 4.140E+04 + 3.300E+01 1.390E+05 3.030E+04 + 3.400E+01 1.240E+05 2.880E+04 + 3.500E+01 1.020E+05 2.650E+04 + 3.600E+01 7.380E+04 2.350E+04 + 3.700E+01 6.900E+04 2.300E+04 + 3.800E+01 6.930E+04 2.290E+04 + 3.900E+01 1.040E+05 2.690E+04 + 4.000E+01 8.210E+04 2.440E+04 + 4.100E+01 1.070E+05 2.740E+04 + 4.200E+01 7.070E+04 2.320E+04 +ENDDATA 80 +ENDSUBENT 105 +SUBENT E1893012 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 0.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 6.620E+09 5.350E+08 + 1.100E+00 6.010E+09 4.860E+08 + 1.200E+00 5.590E+09 4.520E+08 + 1.300E+00 5.280E+09 4.270E+08 + 1.400E+00 5.010E+09 4.050E+08 + 1.500E+00 4.810E+09 3.890E+08 + 1.600E+00 4.770E+09 3.860E+08 + 1.700E+00 4.440E+09 3.600E+08 + 1.800E+00 4.400E+09 3.570E+08 + 1.900E+00 4.290E+09 3.470E+08 + 2.000E+00 4.270E+09 3.460E+08 + 2.100E+00 4.120E+09 3.340E+08 + 2.200E+00 4.140E+09 3.350E+08 + 2.300E+00 4.120E+09 3.340E+08 + 2.400E+00 4.190E+09 3.390E+08 + 2.500E+00 4.190E+09 3.400E+08 + 2.600E+00 4.270E+09 3.460E+08 + 2.700E+00 4.310E+09 3.490E+08 + 2.800E+00 4.400E+09 3.560E+08 + 2.900E+00 4.640E+09 3.760E+08 + 3.000E+00 4.630E+09 3.750E+08 + 3.100E+00 4.660E+09 3.780E+08 + 3.200E+00 4.440E+09 3.600E+08 + 3.300E+00 4.400E+09 3.560E+08 + 3.400E+00 4.340E+09 3.520E+08 + 3.500E+00 4.250E+09 3.450E+08 + 3.600E+00 4.230E+09 3.430E+08 + 3.700E+00 4.270E+09 3.460E+08 + 3.800E+00 4.260E+09 3.450E+08 + 3.900E+00 4.220E+09 3.420E+08 + 4.000E+00 4.200E+09 3.410E+08 + 4.100E+00 4.270E+09 3.460E+08 + 4.200E+00 4.260E+09 3.450E+08 + 4.300E+00 4.210E+09 3.410E+08 + 4.400E+00 4.210E+09 3.420E+08 + 4.500E+00 4.270E+09 3.460E+08 + 4.600E+00 4.210E+09 3.420E+08 + 4.700E+00 4.110E+09 3.340E+08 + 4.800E+00 4.050E+09 3.290E+08 + 4.900E+00 3.970E+09 3.230E+08 + 5.000E+00 3.930E+09 3.190E+08 + 6.000E+00 6.730E+09 5.410E+08 + 7.000E+00 7.420E+09 5.970E+08 + 8.000E+00 8.180E+09 6.580E+08 + 9.000E+00 8.540E+09 6.860E+08 + 1.000E+01 8.680E+09 6.980E+08 + 1.100E+01 8.200E+09 6.590E+08 + 1.200E+01 7.560E+09 6.080E+08 + 1.300E+01 6.690E+09 5.380E+08 + 1.400E+01 5.660E+09 4.560E+08 + 1.500E+01 4.690E+09 3.770E+08 + 1.600E+01 3.840E+09 3.090E+08 + 1.700E+01 3.080E+09 2.480E+08 + 1.800E+01 2.470E+09 1.990E+08 + 1.900E+01 2.040E+09 1.640E+08 + 2.000E+01 1.550E+09 1.250E+08 + 2.100E+01 1.120E+09 9.050E+07 + 2.200E+01 7.160E+08 5.830E+07 + 2.300E+01 3.300E+08 2.730E+07 + 2.400E+01 1.530E+08 1.300E+07 + 2.500E+01 1.250E+08 1.080E+07 + 2.600E+01 1.130E+08 9.860E+06 + 2.700E+01 8.350E+07 7.450E+06 + 2.800E+01 4.900E+07 4.650E+06 + 2.900E+01 1.100E+07 1.490E+06 + 3.000E+01 1.400E+06 4.990E+05 + 3.100E+01 1.160E+05 2.660E+05 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893013 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 5.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 6.260E+09 5.080E+08 + 1.100E+00 5.690E+09 4.610E+08 + 1.200E+00 5.190E+09 4.200E+08 + 1.300E+00 4.820E+09 3.910E+08 + 1.400E+00 4.710E+09 3.820E+08 + 1.500E+00 4.350E+09 3.530E+08 + 1.600E+00 4.350E+09 3.530E+08 + 1.700E+00 4.090E+09 3.320E+08 + 1.800E+00 4.020E+09 3.260E+08 + 1.900E+00 3.930E+09 3.190E+08 + 2.000E+00 3.830E+09 3.110E+08 + 2.100E+00 3.780E+09 3.070E+08 + 2.200E+00 3.710E+09 3.020E+08 + 2.300E+00 3.680E+09 2.990E+08 + 2.400E+00 3.690E+09 3.000E+08 + 2.500E+00 3.660E+09 2.980E+08 + 2.600E+00 3.810E+09 3.100E+08 + 2.700E+00 3.810E+09 3.090E+08 + 2.800E+00 3.990E+09 3.240E+08 + 2.900E+00 4.130E+09 3.350E+08 + 3.000E+00 4.060E+09 3.300E+08 + 3.100E+00 4.000E+09 3.250E+08 + 3.200E+00 3.950E+09 3.210E+08 + 3.300E+00 3.840E+09 3.120E+08 + 3.400E+00 3.760E+09 3.060E+08 + 3.500E+00 3.690E+09 3.000E+08 + 3.600E+00 3.710E+09 3.010E+08 + 3.700E+00 3.630E+09 2.960E+08 + 3.800E+00 3.700E+09 3.010E+08 + 3.900E+00 3.630E+09 2.960E+08 + 4.000E+00 3.630E+09 2.950E+08 + 4.100E+00 3.590E+09 2.920E+08 + 4.200E+00 3.630E+09 2.950E+08 + 4.300E+00 3.650E+09 2.970E+08 + 4.400E+00 3.630E+09 2.960E+08 + 4.500E+00 3.610E+09 2.940E+08 + 4.600E+00 3.530E+09 2.870E+08 + 4.700E+00 3.410E+09 2.780E+08 + 4.800E+00 3.440E+09 2.800E+08 + 4.900E+00 3.350E+09 2.730E+08 + 5.000E+00 3.270E+09 2.670E+08 + 6.000E+00 3.960E+09 3.190E+08 + 7.000E+00 4.130E+09 3.320E+08 + 8.000E+00 4.350E+09 3.500E+08 + 9.000E+00 4.390E+09 3.530E+08 + 1.000E+01 4.320E+09 3.480E+08 + 1.100E+01 3.920E+09 3.160E+08 + 1.200E+01 3.630E+09 2.920E+08 + 1.300E+01 3.200E+09 2.580E+08 + 1.400E+01 2.690E+09 2.170E+08 + 1.500E+01 2.250E+09 1.810E+08 + 1.600E+01 1.850E+09 1.490E+08 + 1.700E+01 1.500E+09 1.210E+08 + 1.800E+01 1.230E+09 9.970E+07 + 1.900E+01 1.010E+09 8.180E+07 + 2.000E+01 7.980E+08 6.470E+07 + 2.100E+01 5.870E+08 4.770E+07 + 2.200E+01 3.870E+08 3.160E+07 + 2.300E+01 2.070E+08 1.710E+07 + 2.400E+01 1.330E+08 1.110E+07 + 2.500E+01 1.070E+08 9.030E+06 + 2.600E+01 9.240E+07 7.850E+06 + 2.700E+01 7.080E+07 6.120E+06 + 2.800E+01 3.420E+07 3.160E+06 + 2.900E+01 8.560E+06 1.050E+06 + 3.000E+01 3.780E+06 6.220E+05 + 3.100E+01 3.400E+06 5.850E+05 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893014 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 10.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 7.830E+09 6.370E+08 + 1.100E+00 6.980E+09 5.680E+08 + 1.200E+00 6.380E+09 5.200E+08 + 1.300E+00 5.920E+09 4.830E+08 + 1.400E+00 5.800E+09 4.720E+08 + 1.500E+00 5.440E+09 4.430E+08 + 1.600E+00 5.380E+09 4.390E+08 + 1.700E+00 5.040E+09 4.110E+08 + 1.800E+00 4.890E+09 3.990E+08 + 1.900E+00 4.710E+09 3.840E+08 + 2.000E+00 4.690E+09 3.830E+08 + 2.100E+00 4.540E+09 3.700E+08 + 2.200E+00 4.460E+09 3.640E+08 + 2.300E+00 4.360E+09 3.560E+08 + 2.400E+00 4.420E+09 3.610E+08 + 2.500E+00 4.370E+09 3.570E+08 + 2.600E+00 4.500E+09 3.670E+08 + 2.700E+00 4.570E+09 3.730E+08 + 2.800E+00 4.600E+09 3.750E+08 + 2.900E+00 4.790E+09 3.910E+08 + 3.000E+00 4.720E+09 3.850E+08 + 3.100E+00 4.640E+09 3.790E+08 + 3.200E+00 4.580E+09 3.740E+08 + 3.300E+00 4.360E+09 3.560E+08 + 3.400E+00 4.220E+09 3.450E+08 + 3.500E+00 4.170E+09 3.410E+08 + 3.600E+00 4.050E+09 3.310E+08 + 3.700E+00 3.960E+09 3.240E+08 + 3.800E+00 3.960E+09 3.240E+08 + 3.900E+00 4.010E+09 3.280E+08 + 4.000E+00 3.830E+09 3.130E+08 + 4.100E+00 3.910E+09 3.200E+08 + 4.200E+00 3.900E+09 3.190E+08 + 4.300E+00 3.840E+09 3.150E+08 + 4.400E+00 3.860E+09 3.160E+08 + 4.500E+00 3.700E+09 3.030E+08 + 4.600E+00 3.750E+09 3.070E+08 + 4.700E+00 3.600E+09 2.950E+08 + 4.800E+00 3.540E+09 2.900E+08 + 4.900E+00 3.450E+09 2.820E+08 + 5.000E+00 3.430E+09 2.820E+08 + 6.000E+00 4.430E+09 3.600E+08 + 7.000E+00 4.560E+09 3.700E+08 + 8.000E+00 4.740E+09 3.850E+08 + 9.000E+00 4.740E+09 3.840E+08 + 1.000E+01 4.640E+09 3.770E+08 + 1.100E+01 4.280E+09 3.470E+08 + 1.200E+01 4.000E+09 3.240E+08 + 1.300E+01 3.640E+09 2.960E+08 + 1.400E+01 3.230E+09 2.620E+08 + 1.500E+01 2.790E+09 2.270E+08 + 1.600E+01 2.420E+09 1.970E+08 + 1.700E+01 2.030E+09 1.650E+08 + 1.800E+01 1.690E+09 1.370E+08 + 1.900E+01 1.430E+09 1.170E+08 + 2.000E+01 1.140E+09 9.290E+07 + 2.100E+01 8.970E+08 7.330E+07 + 2.200E+01 6.010E+08 4.930E+07 + 2.300E+01 3.590E+08 2.960E+07 + 2.400E+01 2.740E+08 2.270E+07 + 2.500E+01 2.560E+08 2.130E+07 + 2.600E+01 2.400E+08 2.000E+07 + 2.700E+01 1.860E+08 1.560E+07 + 2.800E+01 9.480E+07 8.210E+06 + 2.900E+01 1.540E+07 1.710E+06 + 3.000E+01 1.510E+06 4.130E+05 + 3.100E+01 5.760E+05 2.720E+05 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893015 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 15.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 5.210E+09 4.290E+08 + 1.100E+00 4.650E+09 3.830E+08 + 1.200E+00 4.380E+09 3.600E+08 + 1.300E+00 4.010E+09 3.300E+08 + 1.400E+00 3.840E+09 3.170E+08 + 1.500E+00 3.700E+09 3.050E+08 + 1.600E+00 3.570E+09 2.940E+08 + 1.700E+00 3.350E+09 2.760E+08 + 1.800E+00 3.310E+09 2.730E+08 + 1.900E+00 3.170E+09 2.610E+08 + 2.000E+00 3.080E+09 2.540E+08 + 2.100E+00 3.010E+09 2.480E+08 + 2.200E+00 2.950E+09 2.430E+08 + 2.300E+00 2.940E+09 2.430E+08 + 2.400E+00 2.870E+09 2.370E+08 + 2.500E+00 2.870E+09 2.370E+08 + 2.600E+00 2.950E+09 2.430E+08 + 2.700E+00 2.990E+09 2.460E+08 + 2.800E+00 3.010E+09 2.490E+08 + 2.900E+00 3.100E+09 2.560E+08 + 3.000E+00 3.090E+09 2.550E+08 + 3.100E+00 2.970E+09 2.450E+08 + 3.200E+00 2.890E+09 2.390E+08 + 3.300E+00 2.760E+09 2.280E+08 + 3.400E+00 2.660E+09 2.200E+08 + 3.500E+00 2.580E+09 2.140E+08 + 3.600E+00 2.510E+09 2.070E+08 + 3.700E+00 2.500E+09 2.070E+08 + 3.800E+00 2.430E+09 2.010E+08 + 3.900E+00 2.480E+09 2.050E+08 + 4.000E+00 2.360E+09 1.950E+08 + 4.100E+00 2.270E+09 1.880E+08 + 4.200E+00 2.300E+09 1.910E+08 + 4.300E+00 2.330E+09 1.930E+08 + 4.400E+00 2.260E+09 1.870E+08 + 4.500E+00 2.210E+09 1.830E+08 + 4.600E+00 2.200E+09 1.820E+08 + 4.700E+00 2.080E+09 1.720E+08 + 4.800E+00 1.980E+09 1.650E+08 + 4.900E+00 1.910E+09 1.590E+08 + 5.000E+00 1.910E+09 1.590E+08 + 6.000E+00 2.620E+09 2.150E+08 + 7.000E+00 2.470E+09 2.020E+08 + 8.000E+00 2.400E+09 1.970E+08 + 9.000E+00 2.270E+09 1.860E+08 + 1.000E+01 2.090E+09 1.710E+08 + 1.100E+01 1.860E+09 1.530E+08 + 1.200E+01 1.720E+09 1.410E+08 + 1.300E+01 1.570E+09 1.290E+08 + 1.400E+01 1.410E+09 1.150E+08 + 1.500E+01 1.220E+09 1.010E+08 + 1.600E+01 1.060E+09 8.680E+07 + 1.700E+01 8.950E+08 7.360E+07 + 1.800E+01 7.670E+08 6.310E+07 + 1.900E+01 6.600E+08 5.430E+07 + 2.000E+01 5.450E+08 4.500E+07 + 2.100E+01 4.550E+08 3.760E+07 + 2.200E+01 3.180E+08 2.640E+07 + 2.300E+01 2.190E+08 1.820E+07 + 2.400E+01 1.910E+08 1.590E+07 + 2.500E+01 1.690E+08 1.410E+07 + 2.600E+01 1.510E+08 1.260E+07 + 2.700E+01 1.200E+08 1.010E+07 + 2.800E+01 5.550E+07 4.810E+06 + 2.900E+01 9.190E+06 9.980E+05 + 3.000E+01 2.810E+06 4.420E+05 + 3.100E+01 2.010E+05 1.580E+05 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893016 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 20.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 7.780E+09 6.500E+08 + 1.100E+00 6.930E+09 5.790E+08 + 1.200E+00 6.340E+09 5.300E+08 + 1.300E+00 5.850E+09 4.890E+08 + 1.400E+00 5.590E+09 4.670E+08 + 1.500E+00 5.210E+09 4.360E+08 + 1.600E+00 5.080E+09 4.250E+08 + 1.700E+00 4.790E+09 4.000E+08 + 1.800E+00 4.570E+09 3.820E+08 + 1.900E+00 4.440E+09 3.710E+08 + 2.000E+00 4.340E+09 3.630E+08 + 2.100E+00 4.190E+09 3.510E+08 + 2.200E+00 4.050E+09 3.390E+08 + 2.300E+00 3.930E+09 3.290E+08 + 2.400E+00 3.950E+09 3.310E+08 + 2.500E+00 3.970E+09 3.320E+08 + 2.600E+00 4.000E+09 3.350E+08 + 2.700E+00 4.100E+09 3.440E+08 + 2.800E+00 4.160E+09 3.480E+08 + 2.900E+00 4.150E+09 3.470E+08 + 3.000E+00 4.090E+09 3.430E+08 + 3.100E+00 4.020E+09 3.370E+08 + 3.200E+00 3.860E+09 3.230E+08 + 3.300E+00 3.580E+09 3.000E+08 + 3.400E+00 3.490E+09 2.920E+08 + 3.500E+00 3.320E+09 2.780E+08 + 3.600E+00 3.300E+09 2.760E+08 + 3.700E+00 3.170E+09 2.660E+08 + 3.800E+00 3.050E+09 2.560E+08 + 3.900E+00 3.050E+09 2.560E+08 + 4.000E+00 2.940E+09 2.470E+08 + 4.100E+00 2.910E+09 2.450E+08 + 4.200E+00 2.880E+09 2.420E+08 + 4.300E+00 2.780E+09 2.340E+08 + 4.400E+00 2.720E+09 2.280E+08 + 4.500E+00 2.660E+09 2.230E+08 + 4.600E+00 2.590E+09 2.180E+08 + 4.700E+00 2.480E+09 2.080E+08 + 4.800E+00 2.380E+09 2.010E+08 + 4.900E+00 2.340E+09 1.970E+08 + 5.000E+00 2.260E+09 1.900E+08 + 6.000E+00 2.220E+09 1.850E+08 + 7.000E+00 2.020E+09 1.690E+08 + 8.000E+00 1.930E+09 1.610E+08 + 9.000E+00 1.790E+09 1.490E+08 + 1.000E+01 1.650E+09 1.380E+08 + 1.100E+01 1.480E+09 1.230E+08 + 1.200E+01 1.370E+09 1.140E+08 + 1.300E+01 1.260E+09 1.050E+08 + 1.400E+01 1.130E+09 9.430E+07 + 1.500E+01 9.900E+08 8.260E+07 + 1.600E+01 8.500E+08 7.100E+07 + 1.700E+01 7.280E+08 6.080E+07 + 1.800E+01 6.400E+08 5.350E+07 + 1.900E+01 5.360E+08 4.480E+07 + 2.000E+01 4.570E+08 3.830E+07 + 2.100E+01 3.820E+08 3.200E+07 + 2.200E+01 2.520E+08 2.120E+07 + 2.300E+01 2.030E+08 1.710E+07 + 2.400E+01 1.900E+08 1.600E+07 + 2.500E+01 1.700E+08 1.440E+07 + 2.600E+01 1.440E+08 1.220E+07 + 2.700E+01 9.280E+07 7.910E+06 + 2.800E+01 2.330E+07 2.120E+06 + 2.900E+01 2.560E+06 3.640E+05 + 3.000E+01 1.330E+06 2.460E+05 + 3.100E+01 8.670E+05 1.970E+05 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893017 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 25.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 5.550E+09 4.740E+08 + 1.100E+00 5.050E+09 4.320E+08 + 1.200E+00 4.650E+09 3.970E+08 + 1.300E+00 4.360E+09 3.720E+08 + 1.400E+00 4.170E+09 3.560E+08 + 1.500E+00 3.880E+09 3.310E+08 + 1.600E+00 3.820E+09 3.270E+08 + 1.700E+00 3.590E+09 3.070E+08 + 1.800E+00 3.490E+09 2.990E+08 + 1.900E+00 3.370E+09 2.880E+08 + 2.000E+00 3.200E+09 2.740E+08 + 2.100E+00 3.160E+09 2.700E+08 + 2.200E+00 3.060E+09 2.620E+08 + 2.300E+00 2.970E+09 2.550E+08 + 2.400E+00 2.950E+09 2.530E+08 + 2.500E+00 2.990E+09 2.560E+08 + 2.600E+00 2.970E+09 2.550E+08 + 2.700E+00 3.030E+09 2.600E+08 + 2.800E+00 2.920E+09 2.500E+08 + 2.900E+00 2.960E+09 2.540E+08 + 3.000E+00 2.860E+09 2.450E+08 + 3.100E+00 2.740E+09 2.350E+08 + 3.200E+00 2.630E+09 2.250E+08 + 3.300E+00 2.550E+09 2.190E+08 + 3.400E+00 2.450E+09 2.110E+08 + 3.500E+00 2.320E+09 1.990E+08 + 3.600E+00 2.290E+09 1.960E+08 + 3.700E+00 2.220E+09 1.910E+08 + 3.800E+00 2.150E+09 1.850E+08 + 3.900E+00 2.110E+09 1.820E+08 + 4.000E+00 2.070E+09 1.780E+08 + 4.100E+00 1.960E+09 1.690E+08 + 4.200E+00 1.970E+09 1.690E+08 + 4.300E+00 1.940E+09 1.670E+08 + 4.400E+00 1.850E+09 1.590E+08 + 4.500E+00 1.820E+09 1.570E+08 + 4.600E+00 1.750E+09 1.510E+08 + 4.700E+00 1.700E+09 1.460E+08 + 4.800E+00 1.600E+09 1.380E+08 + 4.900E+00 1.540E+09 1.330E+08 + 5.000E+00 1.510E+09 1.300E+08 + 6.000E+00 1.690E+09 1.440E+08 + 7.000E+00 1.480E+09 1.260E+08 + 8.000E+00 1.360E+09 1.160E+08 + 9.000E+00 1.230E+09 1.050E+08 + 1.000E+01 1.090E+09 9.250E+07 + 1.100E+01 9.510E+08 8.110E+07 + 1.200E+01 8.470E+08 7.230E+07 + 1.300E+01 7.620E+08 6.500E+07 + 1.400E+01 6.590E+08 5.630E+07 + 1.500E+01 5.630E+08 4.800E+07 + 1.600E+01 4.580E+08 3.920E+07 + 1.700E+01 3.860E+08 3.300E+07 + 1.800E+01 3.300E+08 2.820E+07 + 1.900E+01 2.760E+08 2.370E+07 + 2.000E+01 2.390E+08 2.050E+07 + 2.100E+01 1.910E+08 1.640E+07 + 2.200E+01 1.370E+08 1.180E+07 + 2.300E+01 1.100E+08 9.550E+06 + 2.400E+01 9.780E+07 8.470E+06 + 2.500E+01 8.600E+07 7.470E+06 + 2.600E+01 6.960E+07 6.080E+06 + 2.700E+01 4.860E+07 4.290E+06 + 2.800E+01 1.590E+07 1.490E+06 + 2.900E+01 3.340E+06 4.140E+05 + 3.000E+01 1.210E+06 2.170E+05 + 3.100E+01 5.910E+05 1.510E+05 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893018 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 30.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 5.880E+09 5.170E+08 + 1.100E+00 5.230E+09 4.600E+08 + 1.200E+00 4.870E+09 4.280E+08 + 1.300E+00 4.540E+09 3.990E+08 + 1.400E+00 4.280E+09 3.770E+08 + 1.500E+00 4.010E+09 3.530E+08 + 1.600E+00 3.860E+09 3.390E+08 + 1.700E+00 3.570E+09 3.140E+08 + 1.800E+00 3.530E+09 3.110E+08 + 1.900E+00 3.370E+09 2.970E+08 + 2.000E+00 3.220E+09 2.830E+08 + 2.100E+00 3.070E+09 2.700E+08 + 2.200E+00 2.990E+09 2.640E+08 + 2.300E+00 2.930E+09 2.580E+08 + 2.400E+00 2.900E+09 2.550E+08 + 2.500E+00 2.920E+09 2.570E+08 + 2.600E+00 2.950E+09 2.600E+08 + 2.700E+00 3.010E+09 2.650E+08 + 2.800E+00 2.960E+09 2.600E+08 + 2.900E+00 2.900E+09 2.560E+08 + 3.000E+00 2.850E+09 2.510E+08 + 3.100E+00 2.690E+09 2.370E+08 + 3.200E+00 2.610E+09 2.300E+08 + 3.300E+00 2.490E+09 2.200E+08 + 3.400E+00 2.360E+09 2.080E+08 + 3.500E+00 2.290E+09 2.020E+08 + 3.600E+00 2.200E+09 1.940E+08 + 3.700E+00 2.110E+09 1.870E+08 + 3.800E+00 2.050E+09 1.810E+08 + 3.900E+00 2.010E+09 1.770E+08 + 4.000E+00 1.910E+09 1.680E+08 + 4.100E+00 1.880E+09 1.660E+08 + 4.200E+00 1.850E+09 1.630E+08 + 4.300E+00 1.800E+09 1.590E+08 + 4.400E+00 1.740E+09 1.540E+08 + 4.500E+00 1.700E+09 1.500E+08 + 4.600E+00 1.600E+09 1.420E+08 + 4.700E+00 1.540E+09 1.360E+08 + 4.800E+00 1.500E+09 1.330E+08 + 4.900E+00 1.420E+09 1.260E+08 + 5.000E+00 1.380E+09 1.230E+08 + 6.000E+00 1.440E+09 1.260E+08 + 7.000E+00 1.260E+09 1.100E+08 + 8.000E+00 1.140E+09 1.000E+08 + 9.000E+00 1.010E+09 8.900E+07 + 1.000E+01 9.030E+08 7.930E+07 + 1.100E+01 7.740E+08 6.800E+07 + 1.200E+01 6.820E+08 5.990E+07 + 1.300E+01 5.950E+08 5.220E+07 + 1.400E+01 5.030E+08 4.420E+07 + 1.500E+01 4.170E+08 3.670E+07 + 1.600E+01 3.380E+08 2.970E+07 + 1.700E+01 2.770E+08 2.440E+07 + 1.800E+01 2.360E+08 2.080E+07 + 1.900E+01 1.940E+08 1.710E+07 + 2.000E+01 1.640E+08 1.450E+07 + 2.100E+01 1.280E+08 1.130E+07 + 2.200E+01 9.250E+07 8.230E+06 + 2.300E+01 7.680E+07 6.850E+06 + 2.400E+01 6.730E+07 6.020E+06 + 2.500E+01 5.780E+07 5.190E+06 + 2.600E+01 4.350E+07 3.930E+06 + 2.700E+01 2.260E+07 2.100E+06 + 2.800E+01 4.230E+06 4.820E+05 + 2.900E+01 1.760E+06 2.550E+05 + 3.000E+01 1.330E+06 2.140E+05 + 3.100E+01 8.060E+05 1.600E+05 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893019 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 40.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 6.490E+09 6.190E+08 + 1.100E+00 5.680E+09 5.420E+08 + 1.200E+00 5.320E+09 5.080E+08 + 1.300E+00 4.870E+09 4.650E+08 + 1.400E+00 4.660E+09 4.440E+08 + 1.500E+00 4.330E+09 4.130E+08 + 1.600E+00 4.190E+09 4.000E+08 + 1.700E+00 3.820E+09 3.640E+08 + 1.800E+00 3.730E+09 3.560E+08 + 1.900E+00 3.560E+09 3.400E+08 + 2.000E+00 3.410E+09 3.250E+08 + 2.100E+00 3.230E+09 3.090E+08 + 2.200E+00 3.150E+09 3.010E+08 + 2.300E+00 3.080E+09 2.940E+08 + 2.400E+00 3.060E+09 2.930E+08 + 2.500E+00 3.140E+09 3.000E+08 + 2.600E+00 3.130E+09 2.990E+08 + 2.700E+00 3.130E+09 2.990E+08 + 2.800E+00 3.000E+09 2.870E+08 + 2.900E+00 2.890E+09 2.770E+08 + 3.000E+00 2.740E+09 2.620E+08 + 3.100E+00 2.690E+09 2.570E+08 + 3.200E+00 2.610E+09 2.500E+08 + 3.300E+00 2.460E+09 2.350E+08 + 3.400E+00 2.340E+09 2.240E+08 + 3.500E+00 2.230E+09 2.130E+08 + 3.600E+00 2.190E+09 2.100E+08 + 3.700E+00 2.060E+09 1.980E+08 + 3.800E+00 2.020E+09 1.930E+08 + 3.900E+00 1.940E+09 1.860E+08 + 4.000E+00 1.850E+09 1.770E+08 + 4.100E+00 1.820E+09 1.740E+08 + 4.200E+00 1.760E+09 1.690E+08 + 4.300E+00 1.740E+09 1.670E+08 + 4.400E+00 1.680E+09 1.620E+08 + 4.500E+00 1.640E+09 1.570E+08 + 4.600E+00 1.520E+09 1.460E+08 + 4.700E+00 1.490E+09 1.440E+08 + 4.800E+00 1.450E+09 1.400E+08 + 4.900E+00 1.380E+09 1.320E+08 + 5.000E+00 1.310E+09 1.260E+08 + 6.000E+00 1.130E+09 1.070E+08 + 7.000E+00 9.670E+08 9.220E+07 + 8.000E+00 8.500E+08 8.100E+07 + 9.000E+00 7.220E+08 6.880E+07 + 1.000E+01 6.070E+08 5.780E+07 + 1.100E+01 5.060E+08 4.820E+07 + 1.200E+01 4.290E+08 4.090E+07 + 1.300E+01 3.530E+08 3.370E+07 + 1.400E+01 2.910E+08 2.780E+07 + 1.500E+01 2.300E+08 2.190E+07 + 1.600E+01 1.790E+08 1.710E+07 + 1.700E+01 1.420E+08 1.360E+07 + 1.800E+01 1.170E+08 1.120E+07 + 1.900E+01 9.840E+07 9.470E+06 + 2.000E+01 8.130E+07 7.830E+06 + 2.100E+01 6.520E+07 6.300E+06 + 2.200E+01 4.700E+07 4.570E+06 + 2.300E+01 3.870E+07 3.780E+06 + 2.400E+01 3.750E+07 3.660E+06 + 2.500E+01 3.170E+07 3.110E+06 + 2.600E+01 2.560E+07 2.530E+06 + 2.700E+01 1.220E+07 1.250E+06 + 2.800E+01 1.910E+06 2.620E+05 + 2.900E+01 8.120E+05 1.500E+05 + 3.000E+01 5.140E+05 1.160E+05 + 3.100E+01 4.420E+05 1.080E+05 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893020 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spectra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 60.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 4.700E+09 6.310E+08 + 1.100E+00 4.270E+09 5.730E+08 + 1.200E+00 3.940E+09 5.290E+08 + 1.300E+00 3.630E+09 4.870E+08 + 1.400E+00 3.490E+09 4.680E+08 + 1.500E+00 3.260E+09 4.380E+08 + 1.600E+00 3.190E+09 4.280E+08 + 1.700E+00 2.930E+09 3.940E+08 + 1.800E+00 2.820E+09 3.780E+08 + 1.900E+00 2.730E+09 3.660E+08 + 2.000E+00 2.640E+09 3.540E+08 + 2.100E+00 2.550E+09 3.420E+08 + 2.200E+00 2.450E+09 3.290E+08 + 2.300E+00 2.350E+09 3.150E+08 + 2.400E+00 2.350E+09 3.150E+08 + 2.500E+00 2.340E+09 3.150E+08 + 2.600E+00 2.250E+09 3.030E+08 + 2.700E+00 2.190E+09 2.940E+08 + 2.800E+00 2.050E+09 2.760E+08 + 2.900E+00 1.970E+09 2.650E+08 + 3.000E+00 1.880E+09 2.530E+08 + 3.100E+00 1.790E+09 2.400E+08 + 3.200E+00 1.690E+09 2.270E+08 + 3.300E+00 1.570E+09 2.120E+08 + 3.400E+00 1.500E+09 2.020E+08 + 3.500E+00 1.460E+09 1.960E+08 + 3.600E+00 1.400E+09 1.880E+08 + 3.700E+00 1.350E+09 1.820E+08 + 3.800E+00 1.300E+09 1.750E+08 + 3.900E+00 1.240E+09 1.680E+08 + 4.000E+00 1.190E+09 1.600E+08 + 4.100E+00 1.130E+09 1.530E+08 + 4.200E+00 1.110E+09 1.500E+08 + 4.300E+00 1.110E+09 1.500E+08 + 4.400E+00 1.060E+09 1.430E+08 + 4.500E+00 1.020E+09 1.380E+08 + 4.600E+00 9.410E+08 1.270E+08 + 4.700E+00 8.960E+08 1.210E+08 + 4.800E+00 8.550E+08 1.150E+08 + 4.900E+00 8.240E+08 1.110E+08 + 5.000E+00 7.670E+08 1.040E+08 + 6.000E+00 7.020E+08 9.410E+07 + 7.000E+00 5.630E+08 7.550E+07 + 8.000E+00 4.550E+08 6.100E+07 + 9.000E+00 3.660E+08 4.910E+07 + 1.000E+01 2.980E+08 4.000E+07 + 1.100E+01 2.400E+08 3.220E+07 + 1.200E+01 2.000E+08 2.680E+07 + 1.300E+01 1.650E+08 2.210E+07 + 1.400E+01 1.350E+08 1.810E+07 + 1.500E+01 1.050E+08 1.420E+07 + 1.600E+01 8.580E+07 1.150E+07 + 1.700E+01 6.980E+07 9.390E+06 + 1.800E+01 5.850E+07 7.870E+06 + 1.900E+01 4.720E+07 6.370E+06 + 2.000E+01 3.410E+07 4.610E+06 + 2.100E+01 2.700E+07 3.660E+06 + 2.200E+01 2.270E+07 3.080E+06 + 2.300E+01 1.900E+07 2.580E+06 + 2.400E+01 1.600E+07 2.180E+06 + 2.500E+01 1.060E+07 1.450E+06 + 2.600E+01 3.660E+06 5.270E+05 + 2.700E+01 9.630E+05 1.650E+05 + 2.800E+01 4.300E+05 9.240E+04 + 2.900E+01 2.690E+05 6.980E+04 + 3.000E+01 1.560E+05 5.320E+04 + 3.100E+01 8.570E+04 4.220E+04 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893021 20050914 20050914 E032 +BIB 6 13 +REACTION (4-BE-9(D,X)0-NN-1,,TTY/PY/DA/DE) +PART-DET (N) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E,N) +METHOD (TOF) + (BCINT) To normalize spetra +ERR-ANALYS (ERR-T) Quadratic sum of statistical error, detector + efficiency, and the data correction for + neutron attenuation. + (ERR-1) Uncertainty in efficiency +STATUS (TABLE) Data (Fig.7, p403 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +COMMON 2 3 +ANG ERR-1 +ADEG PER-CENT + 90.0 5.0 +ENDCOMMON 3 +DATA 3 67 +E DATA ERR-T +MEV P/MEVMUCSR P/MEVMUCSR + 1.000E+00 2.620E+09 1.520E+08 + 1.100E+00 2.380E+09 1.380E+08 + 1.200E+00 2.210E+09 1.280E+08 + 1.300E+00 2.080E+09 1.210E+08 + 1.400E+00 1.970E+09 1.140E+08 + 1.500E+00 1.810E+09 1.050E+08 + 1.600E+00 1.790E+09 1.040E+08 + 1.700E+00 1.600E+09 9.290E+07 + 1.800E+00 1.570E+09 9.120E+07 + 1.900E+00 1.480E+09 8.610E+07 + 2.000E+00 1.400E+09 8.120E+07 + 2.100E+00 1.320E+09 7.680E+07 + 2.200E+00 1.280E+09 7.470E+07 + 2.300E+00 1.240E+09 7.230E+07 + 2.400E+00 1.220E+09 7.100E+07 + 2.500E+00 1.190E+09 6.920E+07 + 2.600E+00 1.200E+09 7.010E+07 + 2.700E+00 1.250E+09 7.290E+07 + 2.800E+00 1.180E+09 6.920E+07 + 2.900E+00 1.060E+09 6.210E+07 + 3.000E+00 9.850E+08 5.770E+07 + 3.100E+00 9.330E+08 5.470E+07 + 3.200E+00 8.840E+08 5.190E+07 + 3.300E+00 8.130E+08 4.780E+07 + 3.400E+00 7.760E+08 4.560E+07 + 3.500E+00 7.250E+08 4.280E+07 + 3.600E+00 7.050E+08 4.160E+07 + 3.700E+00 6.670E+08 3.940E+07 + 3.800E+00 6.220E+08 3.680E+07 + 3.900E+00 6.010E+08 3.560E+07 + 4.000E+00 5.730E+08 3.400E+07 + 4.100E+00 5.540E+08 3.290E+07 + 4.200E+00 5.220E+08 3.110E+07 + 4.300E+00 5.260E+08 3.130E+07 + 4.400E+00 4.950E+08 2.960E+07 + 4.500E+00 4.590E+08 2.750E+07 + 4.600E+00 4.460E+08 2.670E+07 + 4.700E+00 4.120E+08 2.480E+07 + 4.800E+00 3.830E+08 2.310E+07 + 4.900E+00 3.820E+08 2.310E+07 + 5.000E+00 3.430E+08 2.090E+07 + 6.000E+00 2.970E+08 1.710E+07 + 7.000E+00 2.180E+08 1.260E+07 + 8.000E+00 1.630E+08 9.390E+06 + 9.000E+00 1.220E+08 7.050E+06 + 1.000E+01 9.540E+07 5.510E+06 + 1.100E+01 7.270E+07 4.210E+06 + 1.200E+01 5.690E+07 3.300E+06 + 1.300E+01 4.210E+07 2.450E+06 + 1.400E+01 3.250E+07 1.900E+06 + 1.500E+01 2.550E+07 1.500E+06 + 1.600E+01 2.050E+07 1.210E+06 + 1.700E+01 1.500E+07 8.990E+05 + 1.800E+01 1.120E+07 6.780E+05 + 1.900E+01 9.160E+06 5.620E+05 + 2.000E+01 7.660E+06 4.770E+05 + 2.100E+01 6.500E+06 4.100E+05 + 2.200E+01 4.150E+06 2.730E+05 + 2.300E+01 1.760E+06 1.340E+05 + 2.400E+01 9.800E+05 8.660E+04 + 2.500E+01 5.560E+05 5.980E+04 + 2.600E+01 3.800E+05 4.780E+04 + 2.700E+01 2.100E+05 3.530E+04 + 2.800E+01 1.670E+05 3.170E+04 + 2.900E+01 7.370E+04 2.330E+04 + 3.000E+01 4.770E+04 2.040E+04 + 3.100E+01 1.730E+04 1.660E+04 +ENDDATA 69 +ENDSUBENT 91 +SUBENT E1893022 20050914 20050914 E032 +BIB 6 15 +REL-REF (N,,M.Baba+,J,JNM,307-311,1715,2002) + (A,,Von Mollendorff+,C,98MARSEI,,1445,199809) + (A,A0331002,S.Mukhammedov+,J,AE,61,(3),211,1986) + (A,A0194002,P.P.Dmitriev+,R,INDC(CCP)-208/L,1983) +REACTION (3-LI-7(D,X)4-BE-7,,TTY,,PHY) + Corrected for decays during irradiation (Comment from + M. Hagiwara, 20050810) +DECAY-DATA (4-BE-7,,DG,478.) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Computer code IRAC [S.Tanaka et al., Proc. 8th + Int. Conf. of Radiation Shielding, Arlington, + Apr. 1994, American Nuclear Society, Vol.2, + p965(1994)] +STATUS (TABLE) Data (Fig.9, p404 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 15 +NOCOMMON 0 0 +DATA 2 1 +DATA ERR-T +DPS/MUAHR DPS/MUAHR + 6.210E+06 1.110E+06 +ENDDATA 3 +ENDSUBENT 23 +SUBENT E1893023 20050914 20050914 E032 +BIB 6 13 +REL-REF (A,A0194003,P.P.Dmitriev+,R,INDC(CCP)-208/L,1983) + (A,A0269004,I.O.Konstantinov+,J,AE,58,140,1985) +REACTION (4-BE-9(D,X)4-BE-7,,TTY,,PHY) + Corrected for decays during irradiation (Comment from + M. Hagiwara, 20050810) +DECAY-DATA (4-BE-7,,DG,478.) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Computer code IRAC [S.Tanaka et al., Proc. 8th + Int. Conf. of Radiation Shielding, Arlington, + Apr. 1994, American Nuclear Society, Vol.2, + p965(1994)] +STATUS (TABLE) Data (Fig.10, p404 in reference) received by + e-mail from M.Hagiwara (2004.5.10) +ENDBIB 13 +NOCOMMON 0 0 +DATA 2 1 +DATA ERR-T +DPS/MUAHR DPS/MUAHR + 2.160E+05 4.510E+04 +ENDDATA 3 +ENDSUBENT 21 +ENDENTRY 23 diff --git a/exforall/E18/E1894.x4 b/exforall/E18/E1894.x4 new file mode 100644 index 000000000..6cbfa6133 --- /dev/null +++ b/exforall/E18/E1894.x4 @@ -0,0 +1,616 @@ +ENTRY E1894 20050914 20050914 E032 +SUBENT E1894001 20050914 20050914 E032 +BIB 13 48 +TITLE Experimental studies on the proton-induced activation + reactions of molybdenum in the energy range 22-67 MeV +AUTHOR (M.S.Uddin, M.Hagiwara, F.Tarkanyi, F.Ditroi, M.Baba) +INSTITUTE (2JPNTOH) Cyclotron and Radioisotope Center + (3HUNDEB) +REFERENCE (J,ARI,60,(6),911,200406) + (W,Takacs,20040520) S.Takacs, Quantity specification + (W,Hagiwara,20040526) + M.Hagiwara, Gamma energy and quantity specification +INC-SOURCE Beam intensity is about 25 nA. +SAMPLE - Target is natural. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness: 49.58 micro-meter (Mo), 104.2 + micro-meter (Cu) and 102 micro-meter (Al) +METHOD (STTA) Stack was assembled from molybdenum, copper and + aluminium as Cu-Al-Mo and 10 groups were set + together in an aluminium holder for + irradiation. + (EDEG) Energy degradation along the stack was + determined using the computer program SRIM-2002 + [J.F. Ziegler et al., The stopping and range of + ions in solids, Pergamon, New York, 1984.] + assuming the incident energy was 70 MeV. +FACILITY (ISOCY,2JPNTOH) k=90 MeV AVF Cyclotron at Cyclotron + and Radioisotope Center +ANALYSIS (DECAY) Two or more radionuclides emitted gamma-rays + having very close energies, which were + difficult to separate by the graphical + analysis of the multicomponent decay curve, + were analyzed using the difference in + half-life of the nuclides by plotting the + photon emission rate as a function of time. +DETECTOR (HPGE) To measure activities of radioactive products + of the target and monitors. The efficiency + versus energy curve of the detector was + determined experimentally using standard + gamma-ray point sources with known strength, + 152Eu, 133Ba, 241Am. 60Co and 137Cs. Efficiency + is also calculated using the EGS4 Monte Carlo + Code [Nelson et al, 1985]. +ERR-ANALYS (ERR-1) Uncertainty in monitor flux + (ERR-2) Uncertainty in efficiency calibration of gamma + ray + (ERR-S) Maximum statistical uncertainty (0.3-5%) +COMMENT Gamma energies given (except 90Tc and 90Nb) are + obtained by private communication with authors. +HISTORY (20040512C) Kc + On +ENDBIB 48 +COMMON 3 3 +ERR-1 ERR-2 ERR-S +PER-CENT PER-CENT PER-CENT + 5.8 3.0 5.0 +ENDCOMMON 3 +ENDSUBENT 55 +SUBENT E1894002 20050914 20050914 E032 +BIB 4 5 +REACTION (13-AL-27(P,X)11-NA-24,CUM,SIG) +DECAY-DATA (11-NA-24,,DG) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.2, p914 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 5 +NOCOMMON 0 0 +DATA 3 9 +EN DATA ERR-T +MEV MB MB + 30.726 0.34 0.02 + 36.718 0.75 0.05 + 42.056 1.66 0.11 + 46.943 3.39 0.23 + 51.476 5.78 0.38 + 55.705 8.34 0.5 + 59.732 9.5 0.6 + 63.511 10.8 0.7 + 67.154 11.0 0.7 +ENDDATA 11 +ENDSUBENT 21 +SUBENT E1894003 20050914 20050914 E032 +BIB 4 5 +REACTION (13-AL-27(P,X)11-NA-22,CUM,SIG) +DECAY-DATA (11-NA-22,,DG) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.2, p914 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 5 +NOCOMMON 0 0 +DATA 3 9 +EN DATA ERR-T +MEV MB MB + 30.726 0.81 0.07 + 36.718 16.3 1.8 + 42.056 34.5 3.5 + 46.943 37.1 3.8 + 51.476 35.9 3.7 + 55.705 29.7 2.9 + 59.732 26.7 2.8 + 63.511 22.6 2.5 + 67.154 20.0 2.5 +ENDDATA 11 +ENDSUBENT 21 +SUBENT E1894004 20050914 20050914 E032 +BIB 4 5 +REACTION (29-CU-0(P,X)30-ZN-65,,SIG) +DECAY-DATA (30-ZN-65,,DG) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.2, p914 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 5 +NOCOMMON 0 0 +DATA 3 8 +EN DATA ERR-T +MEV MB MB + 26.984 11.8 1.3 + 39.213 7.61 0.8 + 49.048 5.84 0.7 + 53.435 5.78 0.7 + 57.552 6.11 0.8 + 61.472 5.50 0.7 + 65.194 5.49 0.7 + 68.788 4.94 0.7 +ENDDATA 10 +ENDSUBENT 20 +SUBENT E1894005 20050914 20050914 E032 +BIB 4 5 +REACTION (29-CU-0(P,X)30-ZN-62,,SIG) +DECAY-DATA (30-ZN-62,,DG) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.2, p914 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 5 +NOCOMMON 0 0 +DATA 3 8 +EN DATA ERR-T +MEV MB MB + 26.984 55.8 5.2 + 39.213 14.0 1.3 + 49.048 12.0 1.14 + 53.435 11.5 1.10 + 57.552 10.8 0.9 + 61.472 9.46 0.9 + 65.194 8.81 0.8 + 68.788 8.24 0.8 +ENDDATA 10 +ENDSUBENT 20 +SUBENT E1894006 20050914 20050914 E032 +BIB 4 5 +REACTION (29-CU-0(P,X)27-CO-56,CUM,SIG) +DECAY-DATA (27-CO-56,,DG) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.2, p914 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 5 +NOCOMMON 0 0 +DATA 3 5 +EN DATA ERR-T +MEV MB MB + 53.435 0.36 0.07 + 57.552 1.93 0.2 + 61.472 5.12 0.5 + 65.194 9.16 0.8 + 68.788 12.2 1.1 +ENDDATA 7 +ENDSUBENT 17 +SUBENT E1894007 20050914 20050914 E032 +BIB 5 14 +REL-REF (A,D4115002,S.Takacs+,J,JRN,257,(1),195,200307) + Agree in lower energy region + (D,O0737002,B.Scholten+,J,ARI,51,(1),69,199907) + Disagree except data at 22 and 35 MeV + (A,A0510250,V.N.Levkovskij,B,LEVKOVSKIJ,,1991) + Agree in lower energy region + (D,C0068003,M.C.Lagunas-Solar+,J,ARI,42,(7),643,1991) +REACTION (42-MO-100(P,X)42-MO-99,CUM,SIG,,A) + Isotopic aboundance of 100Mo (9.6%) normalized to 100% +DECAY-DATA (42-MO-99,66.HR,DG,140.0) + (42-MO-99,66.HR,DG,739.5) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.3, p915 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 14 +NOCOMMON 0 0 +DATA 3 10 +EN DATA ERR-T +MEV MB MB + 22.343 18.19 1.37 + 29.671 28.28 3.07 + 35.8 69.67 7.49 + 41.239 99.34 10.59 + 46.193 95.17 10.15 + 50.781 84.97 9.06 + 55.055 75.56 8.06 + 59.093 74.29 7.92 + 62.903 76.71 8.18 + 66.58 80.45 8.58 +ENDDATA 12 +ENDSUBENT 31 +SUBENT E1894008 20050914 20050914 E032 +BIB 5 8 +REL-REF (D,C0068012,M.C.Lagunas-Solar+,J,ARI,42,(7),643,1991) + Larger than present data +REACTION (42-MO-0(P,X)42-MO-93-M,CUM,SIG) +DECAY-DATA (42-MO-93-M,,DG,263.1) + (42-MO-93-M,,DG,684.7) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.4, p915 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 8 +NOCOMMON 0 0 +DATA 3 8 +EN DATA ERR-T +MEV MB MB + 29.671 1.87 0.76 + 35.8 5.19 1.23 + 41.239 7.42 1.55 + 50.781 10.12 1.67 + 55.055 11.42 1.69 + 59.093 11.75 1.81 + 62.903 12.89 2.00 + 66.58 13.38 1.80 +ENDDATA 10 +ENDSUBENT 23 +SUBENT E1894009 20050914 20050914 E032 +BIB 5 14 +REL-REF (D,C0068010,M.C.Lagunas-Solar+,J,ARI,42,(7),643,1991) + Higher than present data + (A,D4110002,S.Takacs+,J,NIM/B,198,(3-4),183,200212) + (A,,F.Tarkanyi+,R,IAEA-1211,49,2000) + (N,,C.Birattari+,J,NSTS,2,(2),1302,200110) + No comments for the comparison with present data +REACTION (42-MO-0(P,X)43-TC-96,,SIG) + ground + metastable (Comment from S. Takacs, + 2004.05.20) +DECAY-DATA (43-TC-96,,DG,778.2) + (43-TC-96-G,,DG,812.5) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.5, p916 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 14 +NOCOMMON 0 0 +DATA 3 10 +EN DATA ERR-T +MEV MB MB + 22.343 89.91 6.24 + 29.671 175.70 12.50 + 35.8 136.60 9.46 + 41.239 67.83 4.75 + 46.193 57.19 4.01 + 50.781 59.44 4.18 + 55.055 55.37 3.90 + 59.093 49.30 3.46 + 62.903 43.59 3.09 + 66.58 38.05 2.74 +ENDDATA 12 +ENDSUBENT 31 +SUBENT E1894010 20050914 20050914 E032 +BIB 5 12 +REL-REF (A,D4073003,S.M.Kormali+,J,JRC,31,(2),437,1976) + (N,C0068006,M.C.Lagunas-Solar+,J,ARI,42,(7),643,1991) + Consistent with present data from 35 up to 67 MeV + (A,A0510001,V.N.Levkovskij,B,LEVKOVSKIJ,,1991) + (A,,C.Birattari+,J,NSTS,2,(2),1302,200110) +REACTION (42-MO-0(P,X)43-TC-94,,SIG) + ground + metastable (Comment from S. Takacs, + 2004.05.20) +DECAY-DATA (43-TC-94,,DG,871.1) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.6, p916 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 12 +NOCOMMON 0 0 +DATA 3 9 +EN DATA ERR-T +MEV MB MB + 22.343 69.33 4.93 + 29.671 77.13 5.59 + 35.8 75.62 5.68 + 41.239 64.12 5.08 + 50.781 57.08 4.55 + 55.055 61.27 4.73 + 59.093 54.79 4.46 + 62.903 47.07 4.22 + 66.58 40.15 3.46 +ENDDATA 11 +ENDSUBENT 28 +SUBENT E1894011 20050914 20050914 E032 +BIB 5 13 +REL-REF (N,C0068008,M.C.Lagunus-Solar+,J,ARI,42,(7),643,1991) + No comments for the comparison with present data + (A,A0510001,V.N.Levkovskij,B,LEVKOVSKIJ,,1991) + Comparable with present data + (A,,C.Birattari+,J,NSTS,2,(2),1302,200210) + Comparable with present data +REACTION (42-MO-0(P,X)43-TC-95-G,,SIG) + ground (Comment from S. Takacs, 2004.05.20) +DECAY-DATA (43-TC-95-G,20.HR,DG,765.8) + (43-TC-95-G,20.HR,DG,947.6) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.7, p916 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 13 +NOCOMMON 0 0 +DATA 3 10 +EN DATA ERR-T +MEV MB MB + 22.343 105.93 10.54 + 29.671 98.19 9.78 + 35.8 94.26 9.39 + 41.239 111.48 11.11 + 46.193 96.52 9.56 + 50.781 74.23 7.41 + 55.055 57.55 5.78 + 59.093 51.78 5.18 + 62.903 49.65 4.97 + 66.58 47.49 4.75 +ENDDATA 12 +ENDSUBENT 30 +SUBENT E1894012 20050914 20050914 E032 +BIB 5 12 +REL-REF (N,C0068008,M.C.Lagnust-Solar+,J,ARI,42,(7),643,1991) + No comments for the comparison with present data + (A,A0510001,V.N.Levkovskij,B,LEVKOVSKIJ,,1991) + Comparable with present data + (A,,C.Birattari+,J,NSTS,2,(2),1302,200210) + Comparable with present data +REACTION (42-MO-0(P,X)43-TC-95-M,,SIG) + metastable (Comment from S. Takacs, 2004.05.20) +DECAY-DATA (43-TC-95-M,61.D,DG,582.1) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.8, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 12 +NOCOMMON 0 0 +DATA 3 10 +EN DATA ERR-T +MEV MB MB + 22.343 37.43 2.46 + 29.671 26.26 1.99 + 35.8 20.90 1.52 + 41.239 23.82 1.64 + 46.193 21.21 1.46 + 50.781 16.98 1.35 + 55.055 13.40 1.17 + 59.093 10.85 0.97 + 62.903 11.50 0.99 + 66.58 11.33 1.06 +ENDDATA 12 +ENDSUBENT 29 +SUBENT E1894013 20050914 20050914 E032 +BIB 6 17 +REL-REF (N,A0510001,V.N.Levkovskij,B,LEVKOVSKIJ,,1991) + No comments for the comparison with present data +REACTION 1(42-MO-0(P,X)41-NB-90,CUM,SIG) + Ground state+two metastable states using the intense + independent 1129.2 keV gamma line + 2(42-MO-0(P,X)41-NB-90,CUM,SIG) + Ground state+two metastable states using the 141.2 keV + gamma line separated from 140.5 keV gamma line from + the decay of 99Mo to 99mTc. +DECAY-DATA (41-NB-90-G,14.6HR,DG,141.2) + (41-NB-90-G,14.6HR,DG,1129.2) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Intranuclear cascade model (Particle and Heavy + Ion Transport code System (PHITS) [H. Iwase et + al., J. Nucl. Sci. Technol. 39(2002)1142].) +STATUS (TABLE) Data (Fig.9, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 17 +NOCOMMON 0 0 +DATA 5 10 +EN DATA 1ERR-T 1DATA 2ERR-T 2 +MEV MB MB MB MB + 22.343 2.43 0.18 7.60 0.60 + 29.671 6.69 0.52 21.00 1.65 + 35.8 79.68 6.07 87.46 6.68 + 41.239 133.23 10.10 133.76 10.20 + 46.193 119.00 7.00 119.18 9.04 + 50.781 107.39 8.00 106.20 8.11 + 55.055 90.39 6.88 90.56 6.92 + 59.093 87.04 6.63 88.33 6.75 + 62.903 90.69 6.90 92.53 7.08 + 66.58 99.07 7.53 99.12 7.55 +ENDDATA 12 +ENDSUBENT 34 +SUBENT E1894014 20050914 20050914 E032 +BIB 4 5 +REACTION (42-MO-0(P,X)41-NB-92-M,,SIG) +DECAY-DATA (41-NB-92-M,,DG,934.4) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.10, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 5 +NOCOMMON 0 0 +DATA 3 10 +EN DATA ERR-T +MEV MB MB + 22.343 1.73 0.14 + 29.671 2.95 0.23 + 35.8 3.48 0.26 + 41.239 5.13 0.38 + 46.193 7.29 0.52 + 50.781 7.88 0.57 + 55.055 7.52 0.55 + 59.093 7.71 0.55 + 62.903 8.60 0.62 + 66.58 8.97 0.65 +ENDDATA 12 +ENDSUBENT 22 +SUBENT E1894015 20050914 20050914 E032 +BIB 4 6 +REACTION (42-MO-0(P,X)41-NB-96,IND,SIG) +DECAY-DATA (41-NB-96,,DG,460.0) + (41-NB-96,,DG,568.9) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.10, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 6 +NOCOMMON 0 0 +DATA 3 10 +EN DATA ERR-T +MEV MB MB + 22.343 2.66 0.63 + 29.671 4.98 0.92 + 35.8 4.28 0.86 + 41.239 2.76 0.73 + 46.193 3.19 0.74 + 50.781 3.52 0.78 + 55.055 4.15 0.78 + 59.093 4.17 0.78 + 62.903 4.09 0.65 + 66.58 4.56 0.81 +ENDDATA 12 +ENDSUBENT 23 +SUBENT E1894016 20050914 20050914 E032 +BIB 5 8 +REL-REF (N,A0510001,V.N.Levkovskij,B,LEVKOVSKIJ,,1991) + No comments for the comparison with present data +REACTION (42-MO-0(P,X)41-NB-95-G,CUM,SIG) + Ground state+metastable state +DECAY-DATA (41-NB-95-G,,DG,765.8) +ERR-ANALYS (ERR-T) Total uncertainty +STATUS (TABLE) Data (Fig.11, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 8 +NOCOMMON 0 0 +DATA 3 10 +EN DATA ERR-T +MEV MB MB + 22.343 2.74 0.23 + 29.671 2.88 0.24 + 35.8 4.02 0.31 + 41.239 4.47 0.34 + 46.193 4.78 0.36 + 50.781 5.52 0.42 + 55.055 6.50 0.48 + 59.093 7.06 0.51 + 62.903 7.88 0.57 + 66.58 8.38 0.61 +ENDDATA 12 +ENDSUBENT 25 +SUBENT E1894017 20050914 20050914 E032 +BIB 5 8 +REACTION (42-MO-0(P,X)40-ZR-86,CUM,SIG) +DECAY-DATA (40-ZR-86,,DG,242.8) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Intranuclear cascade model (Particle and Heavy + Ion Transport code System (PHITS) [H. Iwase et + al., J. Nucl. Sci. Technol. 39(2002)1142].) +STATUS (TABLE) Data (Fig.12, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 8 +NOCOMMON 0 0 +DATA 3 5 +EN DATA ERR-T +MEV MB MB + 50.781 1.08 0.43 + 55.055 4.13 0.60 + 59.093 7.46 0.91 + 62.903 9.00 1.04 + 66.58 9.55 1.10 +ENDDATA 7 +ENDSUBENT 20 +SUBENT E1894018 20050914 20050914 E032 +BIB 5 8 +REACTION (42-MO-0(P,X)40-ZR-88,CUM,SIG) +DECAY-DATA (40-ZR-88,,DG,372.7) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Intranuclear cascade model (Particle and Heavy + Ion Transport code System (PHITS) [H. Iwase et + al., J. Nucl. Sci. Technol. 39(2002)1142].) +STATUS (TABLE) Data (Fig.12, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 8 +NOCOMMON 0 0 +DATA 3 9 +EN DATA ERR-T +MEV MB MB + 29.671 5.64 0.49 + 35.8 10.40 0.82 + 41.239 7.41 0.60 + 46.193 4.52 0.38 + 50.781 6.12 0.52 + 55.055 9.38 0.75 + 59.093 15.09 1.23 + 62.903 35.71 2.02 + 66.58 33.73 2.73 +ENDDATA 11 +ENDSUBENT 24 +SUBENT E1894019 20050914 20050914 E032 +BIB 5 8 +REACTION (42-MO-0(P,X)40-ZR-89-G,CUM,SIG) +DECAY-DATA (40-ZR-89-G,,DG,909.1) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Intranuclear cascade model (Particle and Heavy + Ion Transport code System (PHITS) [H. Iwase et + al., J. Nucl. Sci. Technol. 39(2002)1142].) +STATUS (TABLE) Data (Fig.12, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 8 +NOCOMMON 0 0 +DATA 3 10 +EN DATA ERR-T +MEV MB MB + 22.343 3.24 0.38 + 29.671 2.74 0.41 + 35.8 4.02 0.61 + 41.239 9.20 1.07 + 46.193 29.64 2.92 + 50.781 54.31 5.37 + 55.055 73.28 7.22 + 59.093 79.75 7.85 + 62.903 77.99 7.68 + 66.58 73.57 7.72 +ENDDATA 12 +ENDSUBENT 25 +SUBENT E1894020 20050914 20050914 E032 +BIB 5 10 +REACTION (42-MO-0(P,X)39-Y-86-G,CUM,SIG) +DECAY-DATA (39-Y-86-G,,DG,627.7) + (39-Y-86-G,,DG,443.3) + (39-Y-86,,DG,1153.1) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Intranuclear cascade model (Particle and Heavy + Ion Transport code System (PHITS) [H. Iwase et + al., J. Nucl. Sci. Technol. 39(2002)1142].) +STATUS (TABLE) Data (Fig.13, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 10 +NOCOMMON 0 0 +DATA 3 7 +EN DATA ERR-T +MEV MB MB + 41.239 0.54 0.06 + 46.193 0.68 0.07 + 50.781 2.36 0.27 + 55.055 7.59 0.98 + 59.093 13.47 1.81 + 62.903 18.14 2.22 + 66.58 19.11 2.41 +ENDDATA 9 +ENDSUBENT 24 +SUBENT E1894021 20050914 20050914 E032 +BIB 5 8 +REACTION (42-MO-0(P,X)39-Y-87-G,CUM,SIG) +DECAY-DATA (39-Y-87-G,,DG,484.8) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Intranuclear cascade model (Particle and Heavy + Ion Transport code System (PHITS) [H. Iwase et + al., J. Nucl. Sci. Technol. 39(2002)1142].) +STATUS (TABLE) Data (Fig.13, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 8 +NOCOMMON 0 0 +DATA 3 8 +EN DATA ERR-T +MEV MB MB + 35.8 4.94 0.97 + 41.239 77.13 4.86 + 46.193 135.88 8.28 + 50.781 183.67 11.20 + 55.055 152.94 9.34 + 59.093 102.74 6.31 + 62.903 162.30 9.93 + 66.58 179.43 11.00 +ENDDATA 10 +ENDSUBENT 23 +SUBENT E1894022 20050914 20050914 E032 +BIB 5 8 +REACTION (42-MO-0(P,X)39-Y-88,CUM,SIG) +DECAY-DATA (39-Y-88-G,,DG,1836.1) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Intranuclear cascade model (Particle and Heavy + Ion Transport code System (PHITS) [H. Iwase et + al., J. Nucl. Sci. Technol. 39(2002)1142].) +STATUS (TABLE) Data (Fig.13, p917 in reference) are received + by e-mail from M.S.Uddin (2004.5.11) +ENDBIB 8 +NOCOMMON 0 0 +DATA 3 9 +EN DATA ERR-T +MEV MB MB + 29.671 0.69 0.10 + 35.8 1.35 0.15 + 41.239 1.06 0.14 + 46.193 0.77 0.12 + 50.781 1.06 0.15 + 55.055 1.61 0.18 + 59.093 2.81 0.23 + 62.903 4.65 0.38 + 66.58 6.16 0.50 +ENDDATA 11 +ENDSUBENT 24 +ENDENTRY 22 diff --git a/exforall/E18/E1895.x4 b/exforall/E18/E1895.x4 new file mode 100644 index 000000000..3d56ba0f7 --- /dev/null +++ b/exforall/E18/E1895.x4 @@ -0,0 +1,354 @@ +ENTRY E1895 20050914 20050914 E032 +SUBENT E1895001 20050914 20050914 E032 +BIB 10 36 +TITLE Subbarrier fusion in the systems 11,10Be+209Bi +AUTHOR (C.Signorini, A.Yoshida, Y.Watanabe, D.Pierroutsakou, + L.Stroe, T.Fukuda, M.Mazzocco, N.Fukuda, Y.Mizoi, + M.Ishihara, H.Sakurai, A.Diaz-Torres, K.Hagino) +INSTITUTE (2ITYITY) Physics Department and INFN, Padova + (2JPNIPC) + (2ITYNAP) + (2ITYPAD) + (2JPNKEK) + (2JPNTOK) Physics Department + (2GERFRK) Institut fuer Theoretische Physik + (2JPNKTO) Yukawa Institute for Theoretical Physics +REFERENCE (J,NP/A,735,(3-4),329,200405) +REL-REF (N,,C.Signorini+,J,EPJ/A,5,(1),7,199905) + 9Be+209Bi data given in this reference are compared + with present 11, 10Be+209Bi data. +INC-SPECT EN: Energy of secondary beam measured by + time-of-flight method using plastic scintillator +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 0.7 to 0.8 mg/cm**2. + - Backing is mylar film. + - Backing-thickness: 0.07 micro-gram/cm**2 or 0.9 + micro-meter thick +FACILITY (CYCLO,2JPNIPC) Around 65 AMeV 13C beam with about 100 + pnA or 450 pnA intensity onto a 12 mm + thick beryllium target to produce + fragmentation of Be nuclei as + secondary beam + (PRJFS,2JPNIPC) RIPS fragment separator [T.Kubo et + al., Nucl. Instrum. Meth. + B70(1992)309]. +DETECTOR (SI) To detect fission fragments and alpha particles + emitted from the ground states of evaporation + residues +HISTORY (20040512C) Ic + On +ENDBIB 36 +NOCOMMON 0 0 +ENDSUBENT 39 +SUBENT E1895002 20050914 20050914 E032 +BIB 4 8 +REACTION 1(83-BI-209(4-BE-11,5N)87-FR-215,,SIG) + Experiment 1 + 2(83-BI-209(4-BE-11,5N)87-FR-215,,SIG) + Experiment 2 +DECAY-DATA (87-FR-215,90.NSEC,A,9360.) +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig. 5, p335 in reference) received by + e-mail from A.Yoshida (2004.4.20) +ENDBIB 8 +NOCOMMON 0 0 +DATA 5 15 +EN-CM DATA 1ERR-S 1DATA 2ERR-S 2 +MEV MB MB MB MB + 40.9 8.8 3.7 + 42.6 29.0 6.1 + 44.0 53.1 19.0 + 44.3 101.5 10.4 + 46.0 146.8 23.3 + 46.01 182.5 14.0 + 47.7 311.3 17.7 + 48.0 298.1 26.2 + 49.4 417.7 21.0 + 50.0 433.9 25.2 + 51.1 461.3 23.4 + 52.0 489.3 21.0 + 52.9 482.3 24.3 + 54.0 536.9 46.7 + 54.7 451.9 24.8 +ENDDATA 17 +ENDSUBENT 30 +SUBENT E1895003 20050914 20050914 E032 +BIB 4 8 +REACTION 1(83-BI-209(4-BE-11,4N)87-FR-216,,SIG) + Experiment 1 + 2(83-BI-209(4-BE-11,4N)87-FR-216,,SIG) + Experiment 2 +DECAY-DATA (87-FR-216,700.NSEC,A,9005.) +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig. 5, p335 in reference) received by + e-mail from A.Yoshida (2004.4.20) +ENDBIB 8 +NOCOMMON 0 0 +DATA 5 19 +EN-CM DATA 1ERR-S 1DATA 2ERR-S 2 +MEV MB MB MB MB + 37.6 42.5 11.1 + 38.0 65.7 34.8 + 39.2 90.5 14.3 + 40.0 149.2 45.7 + 40.9 172.5 20.2 + 42.0 328.0 61.6 + 42.6 223.5 24.1 + 44.0 276.6 50.0 + 44.3 282.3 27.0 + 46.0 492.4 60.8 + 46.01 261.7 24.7 + 47.7 13.6 24.3 + 48.0 580.9 67.8 + 49.4 141.5 19.4 + 50.0 504.5 64.8 + 51.1 34.4 18.0 + 52.0 345.1 53.6 + 52.9 73.6 16.5 + 54.0 750.4 118.7 +ENDDATA 21 +ENDSUBENT 34 +SUBENT E1895004 20050914 20050914 E032 +BIB 4 8 +REACTION 1(83-BI-209(4-BE-11,F),,SIG) + Experiment 1 + 2(83-BI-209(4-BE-11,F),,SIG) + Experiment 2 +PART-DET (FF) +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig. 5, p335 in reference) received by + e-mail from A.Yoshida (2004.4.20) +ENDBIB 8 +NOCOMMON 0 0 +DATA 5 19 +EN-CM DATA 1ERR-S 1DATA 2ERR-S 2 +MEV MB MB MB MB + 35.9 10.8 7.6 + 37.6 13.5 7.8 + 39.2 16.0 8.0 + 40.9 39.7 12.0 + 42.0 28.8 12.7 + 42.6 35.3 11.2 + 44.0 10.3 7.3 + 44.3 45.5 12.6 + 46.0 36.9 13.7 + 46.01 103.4 19.2 + 47.7 150.7 23.0 + 48.0 19.7 11.2 + 49.4 193.6 26.8 + 50.0 108.7 31.7 + 51.1 185.0 26.7 + 52.0 226.5 52.9 + 52.9 294.3 35.2 + 54.0 149.1 49.7 + 54.7 337.0 38.2 +ENDDATA 21 +ENDSUBENT 34 +SUBENT E1895005 20050914 20050914 E032 +BIB 4 8 +REACTION 1(83-BI-209(4-BE-10,4N)87-FR-215,,SIG) + Experiment 1 + 2(83-BI-209(4-BE-10,4N)87-FR-215,,SIG) + Experiment 2 +DECAY-DATA (87-FR-215,90.NSEC,A,9360.) +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig. 6, p335 in reference) received by + e-mail from A.Yoshida (2004.4.20) +ENDBIB 8 +NOCOMMON 0 0 +DATA 5 17 +EN-CM DATA 1ERR-S 1DATA 2ERR-S 2 +MEV MB MB MB MB + 39.4 12.1 3.9 + 41.0 48.9 7.2 + 42.0 20.974 12.2 + 42.7 139.6 11.3 + 44.0 104.5 11.2 + 44.4 266.6 15.7 + 46.0 274.6 7.6 + 46.2 386.4 19.0 + 47.9 479.2 21.7 + 48.0 421.8 10.1 + 49.6 491.8 22.9 + 50.0 473.1 10.3 + 51.3 416.2 21.8 + 52.0 489.6 10.8 + 53.0 325.6 20.5 + 54.0 311.0 13.1 + 54.7 239.7 19.6 +ENDDATA 19 +ENDSUBENT 32 +SUBENT E1895006 20050914 20050914 E032 +BIB 4 8 +REACTION 1(83-BI-209(4-BE-10,3N)87-FR-216,,SIG) + Experiment 1 + 2(83-BI-209(4-BE-10,3N)87-FR-216,,SIG) + Experiment 2 +DECAY-DATA (87-FR-216,700.NSEC,A,9005.) +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig. 6, p335 in reference) received by + e-mail from A.Yoshida (2004.4.20) +ENDBIB 8 +NOCOMMON 0 0 +DATA 5 19 +EN-CM DATA 1ERR-S 1DATA 2ERR-S 2 +MEV MB MB MB MB + 37.7 81.1 13.2 + 38.0 39.9 29.1 + 39.4 78.6 12.3 + 40.0 126.4 37.1 + 41.0 149.3 32.3 + 42.0 183.6 33.0 + 42.7 248.6 30.6 + 44.0 342.7 29.9 + 44.4 178.2 20.2 + 46.0 307.0 20.3 + 46.2 75.7 21.7 + 47.9 48.6 11.4 + 48.0 438.1 26.7 + 49.6 36.2 10.4 + 50.0 379.4 27.2 + 51.3 32.5 10.2 + 52.0 331.6 28.1 + 53.0 31.4 10.8 + 54.0 298.2 34.2 +ENDDATA 21 +ENDSUBENT 34 +SUBENT E1895007 20050914 20050914 E032 +BIB 4 8 +REACTION 1(83-BI-209(4-BE-10,F),,SIG) + Experiment 1 + 2(83-BI-209(4-BE-10,F),,SIG) + Experiment 2 +PART-DET (FF) +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig. 6, p335 in reference) received by + e-mail from A.Yoshida (2004.4.20) +ENDBIB 8 +NOCOMMON 0 0 +DATA 5 21 +EN-CM DATA 1ERR-S 1DATA 2ERR-S 2 +MEV MB MB MB MB + 31.1 0.0 0.0 + 32.7 0.0 0.0 + 34.4 4.8 4.8 + 36.1 12.2 7.0 + 37.7 14.3 7.2 + 39.4 16.3 7.3 + 41.0 42.4 11.3 + 42.7 38.5 10.7 + 44.0 17.5 7.7 + 44.4 73.3 15.0 + 46.0 30.6 10.2 + 46.2 82.6 15.9 + 47.9 152.0 21.7 + 48.0 60.1 15.9 + 49.6 132.1 20.6 + 50.0 42.8 15.9 + 51.3 258.2 30.2 + 52.0 115.5 30.5 + 53.0 199.7 28.0 + 54.0 124.8 36.3 + 54.7 220.4 30.9 +ENDDATA 23 +ENDSUBENT 36 +SUBENT E1895008 20050914 20050914 E032 +BIB 4 15 +REACTION (83-BI-209(4-BE-11,FUS),,SIG,,,DERIV) + sig(fusion) = sig(215Fr)+sig(216Fr)+sig(fission) +ERR-ANALYS (ERR-T) Absolute uncertainty evaluated from the + comparison of the cross sections for the 3n + evaporation channel leading to 215Fr in the + system 9Be+209Bi measured in [C. Signorini et + al., Eur. Phys. J. A5(1999)7] and in a + calibration run during this experiment + (ERR-S) Statistical uncertainty +ADD-RES (COMP) Coupled channel method (CDCC [N. Austern et + al., Phys. Rep. 154(1987)125] and CCFUL [H. + Hagino et al., Comput. Phys. Commun. + 123(1999)143]) +STATUS (TABLE) Data (Fig. 7, p335 in reference) received by + e-mail from A.Yoshida (2004.4.20) +ENDBIB 15 +COMMON 1 3 +ERR-T +PER-CENT + 30.0 +ENDCOMMON 3 +DATA 3 21 +EN-CM DATA ERR-S +MEV MB MB + 35.9 10.8 7.6 + 37.6 56.0 13.5 + 38.0 65.7 34.8 + 39.2 106.5 16.4 + 40.0 149.2 45.7 + 40.9 221.0 23.8 + 42.0 356.8 62.896 + 42.6 287.9 27.3 + 44.0 340.0 53.984 + 44.3 429.3 31.5 + 46.0 676.1 66.537 + 46.01 547.6 34.3 + 47.7 675.5 37.9 + 48.0 898.7 73.544 + 49.4 752.7 39.2 + 50.0 1047.1 76.413 + 51.1 680.7 39.8 + 52.0 1060.9 78.182 + 52.9 850.2 45.8 + 54.0 1436.4 136.9 + 54.7 788.9 45.5 +ENDDATA 23 +ENDSUBENT 47 +SUBENT E1895009 20050914 20050914 E032 +BIB 4 15 +REACTION (83-BI-209(4-BE-10,FUS),,SIG,,,DERIV) + sig(fusion) = sig(215Fr)+sig(216Fr)+sig(fission) +ERR-ANALYS (ERR-T) Absolute uncertainty evaluated from the + comparison of the cross sections for the 3n + evaporation channel leading to 215Fr in the + system 9Be+209Bi measured in [C. Signorini et + al., Eur. Phys. J. A5(1999)7] and in a + calibration run during this experiment + (ERR-S) Statistical uncertainty +ADD-RES (COMP) Coupled channel method (CDCC [N. Austern et + al., Phys. Rep. 154(1987)125] and CCFUL [H. + Hagino et al., Comput. Phys. Commun. + 123(1999)143]) +STATUS (TABLE) Data (Fig. 7, p335 in reference) received by + e-mail from A.Yoshida (2004.4.20) +ENDBIB 15 +COMMON 1 3 +ERR-T +PER-CENT + 30.0 +ENDCOMMON 3 +DATA 3 22 +EN-CM DATA ERR-S +MEV MB MB + 34.4 4.8 4.8 + 36.1 12.2 7.0 + 37.7 95.4 15.036 + 38.0 39.9 29.1 + 39.4 107.0 14.825 + 40.0 126.4 37.1 + 41.0 240.6 34.969 + 42.0 204.57 35.183 + 42.7 426.7 34.32 + 44.0 464.7 32.844 + 44.4 518.1 29.657 + 46.0 612.2 23.956 + 46.2 544.7 32.936 + 47.9 679.8 32.737 + 48.0 920.0 32.676 + 49.6 660.1 32.51 + 50.0 895.3 33.147 + 51.3 706.9 38.618 + 52.0 936.7 42.854 + 53.0 556.7 36.344 + 54.0 734.0 51.565 + 54.7 460.1 36.592 +ENDDATA 24 +ENDSUBENT 48 +ENDENTRY 9 diff --git a/exforall/E18/E1896.x4 b/exforall/E18/E1896.x4 new file mode 100644 index 000000000..41a6f3860 --- /dev/null +++ b/exforall/E18/E1896.x4 @@ -0,0 +1,189 @@ +ENTRY E1896 20050914 20050914 E032 +SUBENT E1896001 20050914 20050914 E032 +BIB 11 42 +TITLE Trinucleon cluster structures in 6Li +AUTHOR (S.Nakayama, T.Yamagata, H.Akimune, M.Fujiwara, + K.Fushimi, M.B.Greenfield, K.Hara, K.Y.Hara, + H.Hashimoto, K.Ichihara, K.Kawase, H.Matsui, + K.Nakanishi, M.Sakama, M.Tanaka, M.Yosoi) +INSTITUTE (2JPNTKS) Department of Physics + (2JPNKON) Department of Physics + (2JPNOSA) Research Center for Nuclear Physics + (2JPNJAE) Advanced Science Research Center + (2JPNICU) Department of Physics + (2JPNTKS) School of Health Science + (2JPNKTJ) + (2JPNKTO) Department of Physics +REFERENCE (J,PR/C,69,(4),041304,200404) +INC-SOURCE Charge of incident ion is 2+. +SAMPLE - Target enrichment is 99.9%. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Target-thickness is 0.5 mg/cm**2. + - Target is self supported. +METHOD (EDE) To identify alpha particles + (TOF) To identify decay particles +FACILITY (CYCLO,2JPNOSA) Research Center for Nuclear Physics +DETECTOR (MAGSP) To analyze alpha particles. Magnetic + spectrometer Grand RAIDEN [M. Fujiwara et al., + Nucl. Instrum. Meth. A422(1999)484]. Angular + acceptance of +-15 mr horizontally and +-15 mr + vertically with respect to theta(lab)=0 deg. + (MWDC) To detect alpha particles + (SCIN) Used as Delta E-E counter to identify alpha + particles + (SI) To detect triton and 3He. Positioned from + theta(lab)=90 to 160 deg at 10 deg intervals. +ADD-RES E1896.004:3-LI-7(HE3,A+T)2-HE-3 + Angular correlation (Angular correlation + between triton and 3He) + See NRDF D1896 DATA,3 for detail. + E1896.005:3-LI-7(HE3,A+T)2-HE-3 + 3-LI-7(HE3,A)3-LI-6 + Branching ratio + See NRDF D1896 DATA,4 for detail. +HISTORY (20040519C) Sr + On +ENDBIB 42 +COMMON 2 3 +EN E-RSL +MEV KEV + 450.0 300.0 +ENDCOMMON 3 +ENDSUBENT 49 +SUBENT E1896002 20050914 20050914 E032 +BIB 4 8 +REACTION (3-LI-7(HE3,A)3-LI-6,,DA/DE,A/RSD,REL) + Unit is counts. +PART-DET (A) +EN-SEC ANG is polar angle between beam and alpha in + laboratory system + (E-EXC,3-LI-6) +STATUS (UNOBT) Data (Fig.1(a), p041304-2 in reference) + unobtainable +ENDBIB 8 +COMMON 1 3 +ANG +ADEG + 0.0 +ENDCOMMON 3 +NODATA 0 0 +ENDSUBENT 16 +SUBENT E1896003 20050914 20050914 E032 +BIB 6 14 +REACTION (3-LI-7(HE3,A+T)2-HE-3,SEQ,DA/DE,,REL/MSC) + Energy spectrum for 6Li in counts. +PART-DET (A) + (T) + (HE3) +EN-SEC ANG is polar angle between beam and alpha in + laboratory system + (E-EXC,3-LI-6) +METHOD (COINC) Detect alpha, triton and 3He in coincidence. +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (CURVE) Data scanned from Fig.1(a), p041304-2 in + reference. Data points lower than excitation + energy of 17 MeV not available due to high + density of symbols. +ENDBIB 14 +COMMON 1 3 +ANG +ADEG + 0.0 +ENDCOMMON 3 +DATA 3 71 +E-EXC DATA ERR-S +MEV ARB-UNITS ARB-UNITS + 1.728E+01 6.145E+02 7.264E+01 + 1.745E+01 7.680E+02 6.459E+01 + 1.779E+01 7.924E+02 7.270E+01 + 1.796E+01 9.783E+02 7.270E+01 + 1.836E+01 1.188E+03 1.131E+02 + 1.853E+01 1.084E+03 1.050E+02 + 1.887E+01 9.464E+02 1.211E+02 + 1.927E+01 1.060E+03 1.131E+02 + 1.945E+01 1.359E+03 1.292E+02 + 1.973E+01 1.108E+03 1.292E+02 + 1.996E+01 1.456E+03 1.858E+02 + 2.035E+01 1.238E+03 1.534E+02 + 2.058E+01 1.375E+03 9.693E+01 + 2.098E+01 1.311E+03 1.777E+02 + 2.120E+01 1.004E+03 1.615E+02 + 2.149E+01 1.053E+03 1.534E+02 + 2.172E+01 1.303E+03 1.939E+02 + 2.194E+01 1.134E+03 1.777E+02 + 2.234E+01 1.182E+03 2.019E+02 + 2.268E+01 1.190E+03 2.504E+02 + 2.291E+01 9.967E+02 1.777E+02 + 2.314E+01 1.118E+03 2.020E+02 + 2.347E+01 8.920E+02 2.020E+02 + 2.382E+01 8.679E+02 2.100E+02 + 2.410E+01 1.005E+03 2.262E+02 + 2.450E+01 1.030E+03 2.827E+02 + 2.461E+01 8.359E+02 2.262E+02 + 2.501E+01 7.392E+02 2.019E+02 + 2.518E+01 1.006E+03 2.504E+02 + 2.558E+01 9.979E+02 2.908E+02 + 2.575E+01 9.092E+02 2.827E+02 + 2.620E+01 9.740E+02 2.666E+02 + 2.642E+01 4.329E+02 1.939E+02 + 2.671E+01 8.854E+02 2.827E+02 + 2.688E+01 9.743E+02 2.666E+02 + 2.728E+01 8.129E+02 1.939E+02 + 2.745E+01 5.707E+02 2.181E+02 + 2.796E+01 8.052E+02 2.180E+02 + 2.819E+01 8.699E+02 2.585E+02 + 2.836E+01 7.650E+02 2.100E+02 + 2.870E+01 8.055E+02 2.665E+02 + 2.898E+01 6.279E+02 2.342E+02 + 2.927E+01 5.554E+02 2.181E+02 + 2.966E+01 6.040E+02 2.585E+02 + 2.983E+01 3.375E+02 1.373E+02 + 3.018E+01 7.012E+02 2.746E+02 + 3.040E+01 7.417E+02 2.504E+02 + 3.074E+01 5.722E+02 2.181E+02 + 3.097E+01 5.885E+02 2.019E+02 + 3.103E+01 7.016E+02 6.459E+01 + 3.137E+01 7.098E+02 2.423E+02 + 3.148E+01 5.968E+02 2.423E+02 + 3.160E+01 6.130E+02 1.534E+02 + 3.199E+01 5.243E+02 9.690E+01 + 3.211E+01 7.586E+02 2.181E+02 + 3.250E+01 4.518E+02 1.858E+02 + 3.273E+01 6.135E+02 2.342E+02 + 3.307E+01 3.229E+02 1.454E+02 + 3.336E+01 3.715E+02 1.777E+02 + 3.364E+01 8.320E+02 2.908E+02 + 3.381E+01 3.878E+02 1.616E+02 + 3.421E+01 3.961E+02 1.453E+02 + 3.449E+01 4.447E+02 1.777E+02 + 3.483E+01 5.095E+02 2.342E+02 + 3.506E+01 1.784E+02 1.211E+02 + 3.506E+01 2.107E+02 1.534E+02 + 3.534E+01 3.481E+02 1.615E+02 + 3.551E+01 2.836E+02 1.615E+02 + 3.603E+01 4.050E+02 1.857E+02 + 3.665E+01 3.891E+02 2.100E+02 + 3.711E+01 3.974E+02 2.181E+02 +ENDDATA 73 +ENDSUBENT 96 +NOSUBENT E1896004 20050914 20050914 E032 +NOSUBENT E1896005 20050914 20050914 E032 +SUBENT E1896006 20050914 20050914 E032 +BIB 3 6 +REACTION 1(1-H-3(HE3,0),,EN) + 2(1-H-3(HE3,TOT),,WID) + Full width at half maximum +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data taken from Table I, p041304-4 in + reference +ENDBIB 6 +NOCOMMON 0 0 +DATA 5 3 +MOMENTUM L DATA-CM 1DATA-ERR 1DATA-CM 2DATA-ERR 2 +NO-DIM MEV MEV MEV MEV + 1.0 18.0 0.5 5.0 0.5 + 1.0 22.0 1.0 8.0 1.0 + 29.0 2.0 10.0 2.0 +ENDDATA 5 +ENDSUBENT 16 +ENDENTRY 6 diff --git a/exforall/E18/E1897.x4 b/exforall/E18/E1897.x4 new file mode 100644 index 000000000..8baf5a26f --- /dev/null +++ b/exforall/E18/E1897.x4 @@ -0,0 +1,784 @@ +ENTRY E1897 20050914 20050914 E032 +SUBENT E1897001 20050914 20050914 E032 +BIB 11 32 +TITLE Excitations of the alpha cluster in A=6 and 7 nuclei +AUTHOR (T.Yamagata, S.Nakayama, H.Akimune, M.Fujiwara, + K.Fushimi, M.B.Greenfield, K.Hara, K.Y.Hara, + H.Hashimoto, K.Ichihara, K.Kawase, M.Kinoshita, + Y.Matsui, K.Nakanishi, M.Tanaka, H.Utsunomiya, + M.Yosoi) +INSTITUTE (2JPNKON) Department of Physics + (2JPNTKS) Department of Physics + (2JPNOSA) Research Center for Nuclear Physics + (2JPNJAE) Advanced Science Research Center + (2JPNICU) Department of Physics + (2JPNKTJ) + (2JPNKTO) Department of Physics +REFERENCE (J,PR/C,69,(4),044313,200404) +MISC-COL (MISC1) Scattering angle in laboratory system + (MISC2) Momentum transfer +SAMPLE - Chemical-form of target is element. + - Physical-form of target is solid. Metallic foils + - Target is self supported. +METHOD (EDE) +FACILITY (CYCLO,2JPNOSA) Research Center for Nuclear Physics +DETECTOR Calibration: Calibration of excitation energies + carried out by observing known states with 12C targets + (MAGSP) Grand Raiden to analyze reaction particles [M. + Fujiwara et al., Nucl. Instrum. Meth. + A422(1999)484] + (MWDC) To detect reaction particles + (SCIN) Delta-E telescope to detect reaction particles +ADD-RES (COMP) PWBA (Plane wave Born approximation) (To assign + transferred orbital angular momentum) + (STRUC) Excitation energies and width of resonances +HISTORY (20040519C) Ic + On +ENDBIB 32 +NOCOMMON 0 0 +ENDSUBENT 35 +SUBENT E1897002 20050914 20050914 E032 +BIB 8 14 +REACTION (3-LI-6(P,INL)3-LI-6,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-6) +LEVEL-PROP (3-LI-6,E-LVL=2.186,SPIN=3.,PARITY=+1.) +SAMPLE - Target enrichment is 95.4%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (a), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 14 +COMMON 3 3 +EN E-RSL E-LVL +MEV KEV MEV + 300.0 120.0 2.186 +ENDCOMMON 3 +DATA 5 11 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 3.275 2.7 0.1932 0.07759701 0.00410753 + 5.458 4.5 0.3212 0.3788134 0.03739787 + 7.882 6.5 0.4634 0.89239537 0.07501542 + 9.699 8.0 0.5699 1.32740729 0.07213960 + 12.119 10.0 0.7116 2.04388697 0.10246345 + 15.141 12.5 0.888 2.55650254 0.12817447 + 18.156 15.0 1.0634 2.33814281 0.11715529 + 21.166 17.5 1.2378 2.02354407 0.10139594 + 24.167 20.0 1.4109 1.63619971 0.08386842 + 27.758 23.0 1.6166 1.1294329 0.05759233 + 31.334 26.0 1.82 0.70217429 0.03568619 +ENDDATA 13 +ENDSUBENT 36 +SUBENT E1897003 20050914 20050914 E032 +BIB 8 14 +REACTION (3-LI-6(P,INL)3-LI-6,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-6) +LEVEL-PROP (3-LI-6,E-LVL=3.562,SPIN=0.,PARITY=+1.) +SAMPLE - Target enrichment is 95.4%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (a), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 14 +COMMON 3 3 +EN E-RSL E-LVL +MEV KEV MEV + 300.0 120.0 3.562 +ENDCOMMON 3 +DATA 5 6 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 3.276 2.7 0.1941 5.06210341 0.25311219 + 5.46 4.7 0.3215 2.14546043 0.10727572 + 7.885 6.5 0.4634 1.19545689 0.05977651 + 9.702 8.0 0.5696 0.55853433 0.02793036 + 12.123 10.0 0.713 0.26876242 0.01344620 + 15.146 12.5 0.8872 0.04093571 0.00205723 +ENDDATA 8 +ENDSUBENT 31 +SUBENT E1897004 20050914 20050914 E032 +BIB 7 13 +REACTION (3-LI-6(P,INL)3-LI-6,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-6) +SAMPLE - Target enrichment is 95.4%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (b), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 13 +COMMON 4 3 +EN E-RSL E-LVL E-LVL-ERR +MEV KEV MEV MEV + 300.0 120.0 12.0 1.0 +ENDCOMMON 3 +DATA 5 10 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 3.284 2.7 0.2119 3.66977179 0.30581431 + 5.472 4.5 0.331 2.7568436 0.15315797 + 7.903 6.5 0.4682 3.68086999 0.30673916 + 9.724 8.0 0.5721 4.3011846 0.38403433 + 12.151 10.0 0.7111 4.31228483 0.38502543 + 15.18 12.5 0.8848 5.5676006 0.46396671 + 18.204 15.0 1.0579 4.04086371 0.38854458 + 21.221 17.5 1.2302 4.69058388 0.54723478 + 24.222 20.0 1.3925 4.60117384 1.08755017 + 29.016 24.0 1.6616 2.64235678 0.66058919 +ENDDATA 12 +ENDSUBENT 34 +SUBENT E1897005 20050914 20050914 E032 +BIB 7 13 +REACTION (3-LI-6(P,INL)3-LI-6,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-6) +SAMPLE - Target enrichment is 95.4%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (c), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 13 +COMMON 4 3 +EN E-RSL E-LVL E-LVL-ERR +MEV KEV MEV MEV + 300.0 120.0 18.0 1.0 +ENDCOMMON 3 +DATA 6 10 +ANG-CM MISC1 MISC2 DATA-CM +ERR-T -ERR-T +ADEG ADEG 1/FM MB/SR MB/SR MB/SR + 3.29 2.7 0.2363 0.07398182 0.05178727 0.05178727 + 5.482 4.5 0.3461 0.09780935 0.02963919 0.02963919 + 7.916 6.5 0.4777 0.13359188 0.03710885 0.03710885 + 9.741 8.0 0.5788 0.17840721 0.05946906 0.05946906 + 12.172 10.0 0.7151 0.20869233 0.04471978 0.04471978 + 15.207 12.5 0.8862 0.08980859 0.04490429 0.04490429 + 18.236 15.0 1.0573 0.03008646 0.06017291 0.03008645 + 21.258 17.5 1.2278 0.0151322 0.06052879 0.01513219 + 24.264 20.0 1.3885 0.24293103 0.16195402 0.24293103 + 29.067 24.0 1.6554 0.17055314 0.0 0.17055313 +ENDDATA 12 +ENDSUBENT 34 +SUBENT E1897006 20050914 20050914 E032 +BIB 7 13 +REACTION (3-LI-6(P,INL)3-LI-6,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-6) +SAMPLE - Target enrichment is 95.4%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (d), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 13 +COMMON 4 3 +EN E-RSL E-LVL E-LVL-ERR +MEV KEV MEV MEV + 300.0 120.0 27.0 1.5 +ENDCOMMON 3 +DATA 6 10 +ANG-CM MISC1 MISC2 DATA-CM +ERR-T -ERR-T +ADEG ADEG 1/FM MB/SR MB/SR MB/SR + 3.297 2.7 0.2787 0.92571265 0.23142816 0.23142816 + 5.495 4.5 0.375 1.04317328 0.14488517 0.14488517 + 7.936 6.5 0.4974 1.27679933 0.17410899 0.17410899 + 9.765 8.0 0.5938 1.50907374 0.20314454 0.20314454 + 12.202 10.0 0.7254 2.09178067 0.23242007 0.23242007 + 15.243 12.5 0.8922 2.32699403 0.29087425 0.29087425 + 18.279 15.0 1.0599 1.9441661 0.34308813 0.34308813 + 21.309 17.5 1.2276 1.63702823 0.40925705 0.40925705 + 24.323 20.0 1.386 0.97761949 0.58657169 0.58657169 + 29.137 24.0 1.6494 0.61774461 0.46330845 0.46330845 +ENDDATA 12 +ENDSUBENT 34 +SUBENT E1897007 20050914 20050914 E032 +BIB 8 14 +REACTION (3-LI-7(P,INL)3-LI-7,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-7) +LEVEL-PROP (3-LI-7,E-LVL=0.48,SPIN=0.5,PARITY=-1.) +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (e), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 14 +COMMON 3 3 +EN E-RSL E-LVL +MEV KEV MEV + 300.0 120.0 0.48 +ENDCOMMON 3 +DATA 5 10 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 5.323 4.5 0.3213 1.33899955 0.10300410 + 7.688 6.5 0.4639 1.09156550 0.08701803 + 9.46 8.0 0.5706 1.24945776 0.07437243 + 11.821 10.0 0.7126 1.23545449 0.06292899 + 14.77 12.5 0.8894 1.59898038 0.08052779 + 17.713 15.0 1.0653 1.89309424 0.09524453 + 20.651 17.5 1.2403 1.55580101 0.07831180 + 23.582 20.0 1.414 1.03568108 0.05758001 + 27.09 23.0 1.6206 0.76219044 0.04132083 + 30.586 26.0 1.825 0.56155207 0.03032818 +ENDDATA 12 +ENDSUBENT 35 +SUBENT E1897008 20050914 20050914 E032 +BIB 8 14 +REACTION (3-LI-7(P,INL)3-LI-7,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-7) +LEVEL-PROP (3-LI-7,E-LVL=4.652,SPIN=3.5,PARITY=-1.) +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (e), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 14 +COMMON 3 3 +EN E-RSL E-LVL +MEV KEV MEV + 300.0 120.0 4.652 +ENDCOMMON 3 +DATA 5 11 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 3.197 2.7 0.1951 0.04992369 0.00268119 + 5.328 4.5 0.322 0.39548236 0.04404081 + 7.694 6.5 0.4635 0.96893396 0.07639287 + 9.468 8.0 0.5696 1.99919048 0.10538804 + 11.832 10.0 0.7108 2.79452046 0.14022446 + 14.782 12.5 0.8869 4.07291704 0.20389422 + 17.728 15.0 1.0621 4.25718240 0.21311211 + 20.669 17.5 1.2363 3.31257202 0.16585244 + 23.603 20.0 1.4093 2.68804282 0.13784966 + 27.113 23.0 1.6152 1.63058252 0.08341666 + 30.612 26.0 1.8188 0.94106986 0.04837064 +ENDDATA 13 +ENDSUBENT 36 +SUBENT E1897009 20050914 20050914 E032 +BIB 7 13 +REACTION (3-LI-7(P,INL)3-LI-7,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-7) +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (f), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 13 +COMMON 4 3 +EN E-RSL E-LVL E-LVL-ERR +MEV KEV MEV MEV + 300.0 120.0 9.5 1.0 +ENDCOMMON 3 +DATA 5 10 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 3.2 2.7 0.2037 1.35057229 0.15006358 + 5.333 4.5 0.3264 0.82645691 0.09391555 + 7.702 6.5 0.4655 0.97805122 0.09404338 + 9.478 8.0 0.5704 1.35607082 0.11300590 + 11.844 10.0 0.7105 1.51011912 0.24539435 + 14.798 12.5 0.8852 2.27289595 0.32199359 + 17.747 15.0 1.0594 2.35852061 0.24726425 + 20.69 17.5 1.2326 2.67609529 0.21026463 + 23.619 20.0 1.3959 3.03986993 0.54283391 + 28.301 24.0 1.6667 1.21775237 0.36532571 +ENDDATA 12 +ENDSUBENT 34 +SUBENT E1897010 20050914 20050914 E032 +BIB 7 13 +REACTION (3-LI-7(P,INL)3-LI-7,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-7) +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (g), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 13 +COMMON 4 3 +EN E-RSL E-LVL E-LVL-ERR +MEV KEV MEV MEV + 300.0 120.0 17.0 1.0 +ENDCOMMON 3 +DATA 5 10 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 3.205 2.7 0.222 2.83366786 0.28336678 + 5.341 4.5 0.3371 2.02689282 0.26349606 + 7.713 6.5 0.4719 2.43559227 0.26385582 + 9.491 8.0 0.5747 3.2518446 0.34550848 + 11.86 10.0 0.7125 2.85175495 0.32591485 + 14.818 12.5 0.8852 3.43398426 0.28616535 + 17.77 15.0 1.0577 3.03800524 0.34896006 + 20.718 17.5 1.2294 2.64054295 0.22692166 + 23.651 20.0 1.3914 2.81199990 0.82016664 + 28.339 24.0 1.6603 2.62875345 0.78862603 +ENDDATA 12 +ENDSUBENT 34 +SUBENT E1897011 20050914 20050914 E032 +BIB 7 13 +REACTION (3-LI-7(P,INL)3-LI-7,PAR,DA) +PART-DET (P) +EN-SEC ANG-CM is polar angle between beam and proton in + center of mass system + (E-LVL,3-LI-7) +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 15 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.2 (h), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 13 +COMMON 4 3 +EN E-RSL E-LVL E-LVL-ERR +MEV KEV MEV MEV + 300.0 120.0 29.0 1.5 +ENDCOMMON 3 +DATA 6 10 +ANG-CM MISC1 MISC2 DATA-CM +ERR-T -ERR-T +ADEG ADEG 1/FM MB/SR MB/SR MB/SR + 3.215 2.7 0.2893 0.93038773 0.26167154 0.26167154 + 5.358 4.5 0.3826 1.08088441 0.17623115 0.17623115 + 7.739 6.5 0.5027 1.52947266 0.32354229 0.32354229 + 9.523 8.0 0.598 2.00257024 0.20614693 0.20614693 + 11.899 10.0 0.7284 2.30198948 0.29512685 0.29512685 + 14.867 12.5 0.8942 2.60690133 0.32586266 0.32586266 + 17.83 15.0 1.0612 2.37626526 0.41584642 0.41584642 + 20.786 17.5 1.2284 1.07635085 0.41858088 0.41858088 + 23.73 20.0 1.3865 0.19983039 0.59949119 0.19983039 + 28.433 24.0 1.6498 0.44830622 0.33622967 0.44830622 +ENDDATA 12 +ENDSUBENT 34 +SUBENT E1897012 20050914 20050914 E032 +BIB 9 16 +REACTION (3-LI-6(HE3,T)4-BE-6,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-6) +LEVEL-PROP (4-BE-6,E-LVL=0.0,SPIN=0.,PARITY=+1.) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 95.4%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (a), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 16 +COMMON 4 3 +EN E-RSL E-LVL MISC3 +MEV KEV MEV NO-DIM + 450.0 340.0 0.0 0.0 +ENDCOMMON 3 +DATA 5 7 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.04 33.7 1.685 + 1.3 0.9 0.131 30.3 1.515 + 2.5 1.7 0.248 16.7 0.835 + 3.1 2.1 0.307 11.2 0.56 + 4.0 2.7 0.395 7.42 0.371 + 4.9 3.3 0.482 4.51 0.2255 + 5.8 3.9 0.57 2.75 0.1375 +ENDDATA 9 +ENDSUBENT 34 +SUBENT E1897013 20050914 20050914 E032 +BIB 8 15 +REACTION (3-LI-6(HE3,T)4-BE-6,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-6) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 95.4%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (b), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 15 +COMMON 5 3 +EN E-RSL E-LVL E-LVL-ERR MISC3 +MEV KEV MEV MEV NO-DIM + 450.0 340.0 8.5 1.0 1.0 +ENDCOMMON 3 +DATA 5 7 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.133 0.75 0.1875 + 1.3 0.9 0.18 0.83 0.2075 + 1.8 0.234 1.05 0.2625 + 3.1 2.1 0.33 1.64 0.41 + 4.0 2.7 0.41 1.81 0.4525 + 4.9 3.3 0.495 1.93 0.4825 + 5.8 3.9 0.585 1.64 0.41 +ENDDATA 9 +ENDSUBENT 33 +SUBENT E1897014 20050914 20050914 E032 +BIB 8 15 +REACTION (3-LI-6(HE3,T)4-BE-6,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-6) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 95.4%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (b), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 15 +COMMON 5 3 +EN E-RSL E-LVL E-LVL-ERR MISC3 +MEV KEV MEV MEV NO-DIM + 450.0 340.0 15.0 1.0 1.0 +ENDCOMMON 3 +DATA 5 7 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.19 0.05 0.01 + 1.3 0.9 0.231 0.067 0.0134 + 1.8 0.323 0.071 0.0142 + 3.1 2.1 0.359 0.099 0.0198 + 4.0 2.7 0.435 0.16 0.032 + 4.9 3.3 0.515 0.17 0.034 + 5.8 3.9 0.597 0.23 0.046 +ENDDATA 9 +ENDSUBENT 33 +SUBENT E1897015 20050914 20050914 E032 +BIB 8 15 +REACTION (3-LI-6(HE3,T)4-BE-6,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-6) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 95.4%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (b), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 15 +COMMON 5 3 +EN E-RSL E-LVL E-LVL-ERR MISC3 +MEV KEV MEV MEV NO-DIM + 450.0 340.0 23.5 1.5 1.0 +ENDCOMMON 3 +DATA 5 7 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.267 0.47 0.141 + 1.4 0.9 0.297 0.44 0.132 + 1.8 0.373 0.46 0.138 + 3.2 2.1 0.404 0.51 0.153 + 4.1 2.7 0.472 0.68 0.204 + 5.0 3.3 0.547 0.78 0.234 + 5.9 3.9 0.624 0.85 0.255 +ENDDATA 9 +ENDSUBENT 33 +SUBENT E1897016 20050914 20050914 E032 +BIB 9 17 +REACTION (3-LI-7(HE3,T)4-BE-7,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=0.0,SPIN=1.5,PARITY=-1.) + (4-BE-7,E-LVL=0.43,SPIN=0.5,PARITY=-1.) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (c), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 17 +COMMON 5 3 +EN E-RSL E-LVL E-LVL MISC3 +MEV KEV MEV MEV NO-DIM + 450.0 340.0 0.0 0.43 0.0 +ENDCOMMON 3 +DATA 5 7 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.01 58.7 2.935 + 1.3 0.9 0.131 49.8 2.49 + 2.5 1.7 0.248 24.2 1.21 + 3.1 2.1 0.307 27.7 1.385 + 4.0 2.7 0.395 17.7 0.885 + 4.9 3.3 0.482 11.5 0.575 + 5.8 3.9 0.57 7.6 0.38 +ENDDATA 9 +ENDSUBENT 35 +SUBENT E1897017 20050914 20050914 E032 +BIB 9 16 +REACTION (3-LI-7(HE3,T)4-BE-7,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=9.9,SPIN=1.5,PARITY=-1.) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (c), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 16 +COMMON 4 3 +EN E-RSL E-LVL MISC3 +MEV KEV MEV NO-DIM + 450.0 340.0 9.9 0.0 +ENDCOMMON 3 +DATA 5 4 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.1 0.2 0.04 + 1.3 0.9 0.166 0.17 0.034 + 3.1 2.1 0.322 0.11 0.022 + 4.0 2.7 0.406 0.099 0.0198 +ENDDATA 6 +ENDSUBENT 31 +SUBENT E1897018 20050914 20050914 E032 +BIB 8 15 +REACTION (3-LI-7(HE3,T)4-BE-7,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-7) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (d), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 15 +COMMON 5 3 +EN E-RSL E-LVL E-LVL-ERR MISC3 +MEV KEV MEV MEV NO-DIM + 450.0 340.0 9.5 1.0 1.0 +ENDCOMMON 3 +DATA 5 6 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.1 0.33 0.0825 + 1.3 0.9 0.166 0.52 0.13 + 3.1 2.1 0.322 0.95 0.2375 + 4.0 2.7 0.406 0.94 0.235 + 4.9 3.3 0.491 0.91 0.2275 + 5.8 3.9 0.577 0.76 0.19 +ENDDATA 8 +ENDSUBENT 32 +SUBENT E1897019 20050914 20050914 E032 +BIB 8 15 +REACTION (3-LI-7(HE3,T)4-BE-7,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-7) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (d), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 15 +COMMON 5 3 +EN E-RSL E-LVL E-LVL-ERR MISC3 +MEV KEV MEV MEV NO-DIM + 450.0 340.0 17.0 1.0 1.0 +ENDCOMMON 3 +DATA 5 6 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.2 0.53 0.1325 + 1.3 0.9 0.236 0.65 0.1625 + 3.1 2.1 0.363 1.27 0.3175 + 4.0 2.7 0.438 1.47 0.3675 + 4.9 3.3 0.518 1.43 0.3575 + 5.8 3.9 0.599 1.31 0.3275 +ENDDATA 8 +ENDSUBENT 32 +SUBENT E1897020 20050914 20050914 E032 +BIB 8 15 +REACTION (3-LI-7(HE3,T)4-BE-7,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-7) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (d), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 15 +COMMON 5 3 +EN E-RSL E-LVL E-LVL-ERR MISC3 +MEV KEV MEV MEV NO-DIM + 450.0 340.0 28.0 1.5 1.0 +ENDCOMMON 3 +DATA 5 6 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.29 0.26 0.078 + 1.4 0.9 0.321 0.26 0.078 + 3.2 2.1 0.438 0.39 0.117 + 4.1 2.7 0.478 0.52 0.156 + 5.0 3.3 0.56 0.52 0.156 + 5.9 3.9 0.635 0.49 0.147 +ENDDATA 8 +ENDSUBENT 32 +SUBENT E1897021 20050914 20050914 E032 +BIB 9 16 +REACTION (3-LI-7(HE3,T)4-BE-7,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=4.5,SPIN=3.5,PARITY=-1.) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (e), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 16 +COMMON 4 3 +EN E-RSL E-LVL MISC3 +MEV KEV MEV NO-DIM + 450.0 340.0 4.5 2.0 +ENDCOMMON 3 +DATA 5 6 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.01 0.0163 0.00489 + 1.3 0.9 0.131 0.0163 0.00489 + 3.1 2.1 0.307 0.029 0.0087 + 4.0 2.7 0.395 0.049 0.0147 + 4.9 3.3 0.482 0.082 0.0246 + 5.8 3.9 0.57 0.082 0.0246 +ENDDATA 8 +ENDSUBENT 33 +SUBENT E1897022 20050914 20050914 E032 +BIB 9 16 +REACTION (3-LI-7(HE3,T)4-BE-7,PAR,DA) +PART-DET (T) +EN-SEC ANG-CM is polar angle between beam and triton in + center of mass system + (E-LVL,4-BE-7) +LEVEL-PROP (4-BE-7,E-LVL=7.1,SPIN=2.5,PARITY=-1.) +MISC-COL (MISC3) Transferred orbital angular momentum assigned + by PWBA analysis +SAMPLE - Target enrichment is 99.9%. + - Target-thickness is 20 mg/cm**2. +DETECTOR E-RSL: Mainly due to the energy spread of incident + beam +ERR-ANALYS (ERR-T) Mainly due to fitting procedure +STATUS (TABLE) Data (Fig.3 (e), p044313-4 in reference) + received by e-mail from T.Yamagata + (2005.05.06) +ENDBIB 16 +COMMON 4 3 +EN E-RSL E-LVL MISC3 +MEV KEV MEV NO-DIM + 450.0 340.0 7.1 2.0 +ENDCOMMON 3 +DATA 5 6 +ANG-CM MISC1 MISC2 DATA-CM ERR-T +ADEG ADEG 1/FM MB/SR MB/SR + 0.0 0.0 0.01 0.0163 0.00489 + 1.3 0.9 0.131 0.0163 0.00489 + 3.1 2.1 0.307 0.016 0.0048 + 4.0 2.7 0.395 0.026 0.0078 + 4.9 3.3 0.482 0.043 0.0129 + 5.8 3.9 0.57 0.043 0.0129 +ENDDATA 8 +ENDSUBENT 33 +ENDENTRY 22 diff --git a/exforall/E18/E1898.x4 b/exforall/E18/E1898.x4 new file mode 100644 index 000000000..9686d809f --- /dev/null +++ b/exforall/E18/E1898.x4 @@ -0,0 +1,1216 @@ +ENTRY E1898 20050914 20050914 E032 +SUBENT E1898001 20050914 20050914 E032 +BIB 14 58 +TITLE Polarization transfer and spin response functions of + the 2H(p,n) reaction at 345 MeV +AUTHOR (T.Wakasa, H.Sakai, M.Ichimura, K.Hatanaka, + M.B.Greenfield, M.Hatano, J.Kamiya, H.Kato, Y.Maeda, + H.Okamura, T.Ohnishi, H.Otsu, K.Sekiguchi, K.Suda, + A.Tamii, T.Uesaka, T.Yagita, K.Yako) +INSTITUTE (2JPNKYU) Department of Physics + (2JPNTOK) Department of Physics + (2JPNIPC) + (2JPNHOS) Faculty of Computer and Information Sciences + (2JPNOSA) Research Center for Nuclear Physics + (2JPNICU) Division of Natural Science + (2JPNJAE) Accelerator Group + (2JPNTOH) Cyclotron and Radioisotope Center + (2JPNTOH) Department of Physics + (2JPNSUU) Department of Physics + (2JPNTOK) Center for Nuclear Study +REFERENCE (J,PR/C,69,(4),044602,200404) +REL-REF (N,E1718001,T.Wakasa+,J,PR/C,59,(6),3177,199906) + Polarization transfer coefficients at 22 deg given for + 346 MeV proton +MONIT-REF (C0518001,T.N.Taddeucci+,J,PRL,73,(26),3516,199412) + sigma(c.m. 0deg)=27.0+-0.8 mb/sr in + 7Li(p,n)7Be(g.s.+0.43 MeV) is used to determine the + product of detection efficiency and transmission + factor along the flight path of air +PART-DET (N) +INC-SOURCE Beam intensity: About 10 and 50 nA for cross section + and Dij measurements, respectively + (POLIS) POL-BM: Measured by beam line polarimeters by + using p+p elastc scattering with CH2 target + (1.1 mg/cm2). The effective analyzing power of + the polarimeter is 0.430+-0.003 (sys.) at + Tp=345 MeV. +SAMPLE - Target is natural. + - Chemical-form of target is CD2. Data for 2H(p,n) + were deduced from the cross sectino weighted + difference between CD2 and 12C results. + - Physical-form of target is solid. + - Backing is unknown. +METHOD (TOF) + (DSCAT) Neutron polarization is analyzed by using the + n+p scattering in neutron detector/polarimeter + NPOL2. +FACILITY (ISOCY,2JPNOSA) AVF cyclotron (up to 59.7 MeV) at + Research Center for Nuclear Physics + (CYCLO,2JPNOSA) Ring cyclotron (up to 345 MeV) at + Research Center for Nuclear Physics +DETECTOR Efficiency: Detection efficiency of NPOL2 (neutron + detector / polarimeter) is determined to be 0.14+-0.01 + (SCIN) Liquid (BC519) and plastic (BC408) + scintillators + (SCIN) Plastic scintillators used as veto counters for + charged particles +ADD-RES (COMP) PWIA (Plane wave impulse approximation) (PWIA + code [A. Itabashi et al., Prog. Theor. Phys. + 91(1994)69]) +HISTORY (20040914C) Kc + On +ENDBIB 58 +COMMON 2 3 +EN-ERR POL-BM +MEV NO-DIM + 1.0 0.7 +ENDCOMMON 3 +ENDSUBENT 65 +SUBENT E1898002 20050914 20050914 E032 +BIB 5 9 +REACTION (1-H-2(P,X)0-NN-1,,DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 222 mg/cm2 for CD2 and 172 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.1, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 9 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 345.0 2.0 16.0 +ENDCOMMON 3 +DATA 3 185 +E-DGD DATA ERR-S +MEV MB/SR/MEV MB/SR/MEV + 13.00 0.0044 0.0009 + 14.00 0.0151 0.0014 + 15.00 0.0970 0.0032 + 16.00 0.2457 0.0050 + 17.00 0.3315 0.0058 + 18.00 0.3505 0.0062 + 19.00 0.3493 0.0069 + 20.00 0.3751 0.0074 + 21.00 0.4175 0.0074 + 22.00 0.4325 0.0087 + 23.00 0.4732 0.0104 + 24.00 0.5331 0.0102 + 25.00 0.6121 0.0095 + 26.00 0.6286 0.0093 + 27.00 0.6757 0.0095 + 28.00 0.6872 0.0098 + 29.00 0.7272 0.0100 + 30.00 0.7317 0.0100 + 31.00 0.7083 0.0100 + 32.00 0.6834 0.0099 + 33.00 0.6580 0.0099 + 34.00 0.6236 0.0098 + 35.00 0.6009 0.0097 + 36.00 0.5648 0.0096 + 37.00 0.5099 0.0094 + 38.00 0.4940 0.0094 + 39.00 0.4490 0.0093 + 40.00 0.4221 0.0091 + 41.00 0.3727 0.0090 + 42.00 0.3475 0.0090 + 43.00 0.3124 0.0089 + 44.00 0.2911 0.0088 + 45.00 0.2673 0.0088 + 46.00 0.2278 0.0086 + 47.00 0.2381 0.0086 + 48.00 0.2066 0.0086 + 49.00 0.2039 0.0084 + 50.00 0.1792 0.0084 + 51.00 0.1873 0.0084 + 52.00 0.1330 0.0083 + 53.00 0.1531 0.0082 + 54.00 0.1331 0.0082 + 55.00 0.1375 0.0081 + 56.00 0.1149 0.0079 + 57.00 0.1077 0.0081 + 58.00 0.1259 0.0080 + 59.00 0.0877 0.0078 + 60.00 0.0952 0.0078 + 61.00 0.1017 0.0077 + 62.00 0.0807 0.0076 + 63.00 0.0676 0.0075 + 64.00 0.0526 0.0073 + 65.00 0.0620 0.0073 + 66.00 0.0732 0.0074 + 67.00 0.0803 0.0072 + 68.00 0.0653 0.0072 + 69.00 0.0399 0.0070 + 70.00 0.0625 0.0071 + 71.00 0.0415 0.0069 + 72.00 0.0543 0.0068 + 73.00 0.0293 0.0067 + 74.00 0.0452 0.0067 + 75.00 0.0399 0.0066 + 76.00 0.0413 0.0065 + 77.00 0.0298 0.0064 + 78.00 0.0432 0.0064 + 79.00 0.0437 0.0063 + 80.00 0.0405 0.0063 + 81.00 0.0435 0.0062 + 82.00 0.0373 0.0062 + 83.00 0.0303 0.0061 + 84.00 0.0319 0.0060 + 85.00 0.0225 0.0059 + 86.00 0.0407 0.0059 + 87.00 0.0321 0.0058 + 88.00 0.0336 0.0058 + 89.00 0.0217 0.0056 + 90.00 0.0250 0.0057 + 91.00 0.0238 0.0055 + 92.00 0.0164 0.0055 + 93.00 0.0285 0.0055 + 94.00 0.0170 0.0054 + 95.00 0.0256 0.0054 + 96.00 0.0289 0.0054 + 97.00 0.0318 0.0052 + 98.00 0.0174 0.0052 + 99.00 0.0211 0.0052 + 100.00 0.0166 0.0051 + 101.00 0.0128 0.0051 + 102.00 0.0216 0.0050 + 103.00 0.0140 0.0050 + 104.00 0.0085 0.0049 + 105.00 0.0225 0.0049 + 106.00 0.0195 0.0049 + 107.00 0.0138 0.0049 + 108.00 0.0160 0.0048 + 109.00 0.0138 0.0048 + 110.00 0.0185 0.0047 + 111.00 0.0208 0.0047 + 112.00 0.0144 0.0046 + 113.00 0.0138 0.0046 + 114.00 0.0198 0.0046 + 115.00 0.0146 0.0046 + 116.00 0.0142 0.0044 + 117.00 0.0202 0.0046 + 118.00 0.0137 0.0044 + 119.00 0.0094 0.0044 + 120.00 0.0179 0.0043 + 121.00 0.0148 0.0043 + 122.00 0.0191 0.0043 + 123.00 0.0123 0.0043 + 124.00 0.0148 0.0043 + 125.00 0.0118 0.0042 + 126.00 0.0159 0.0043 + 127.00 0.0118 0.0041 + 128.00 0.0044 0.0041 + 129.00 0.0146 0.0041 + 130.00 0.0186 0.0041 + 131.00 0.0165 0.0041 + 132.00 0.0134 0.0042 + 133.00 0.0198 0.0040 + 134.00 0.0100 0.0040 + 135.00 0.0082 0.0040 + 136.00 0.0154 0.0040 + 137.00 0.0143 0.0040 + 138.00 0.0104 0.0040 + 139.00 0.0121 0.0039 + 140.00 0.0155 0.0039 + 141.00 0.0168 0.0039 + 142.00 0.0122 0.0039 + 143.00 0.0109 0.0038 + 144.00 0.0105 0.0039 + 145.00 0.0131 0.0039 + 146.00 0.0113 0.0038 + 147.00 0.0117 0.0038 + 148.00 0.0120 0.0039 + 149.00 0.0108 0.0038 + 150.00 0.0123 0.0037 + 151.00 0.0113 0.0038 + 152.00 0.0167 0.0039 + 153.00 0.0124 0.0037 + 154.00 0.0173 0.0037 + 155.00 0.0081 0.0036 + 156.00 0.0100 0.0037 + 157.00 0.0077 0.0038 + 158.00 0.0121 0.0037 + 159.00 0.0202 0.0037 + 160.00 0.0160 0.0037 + 161.00 0.0150 0.0036 + 162.00 0.0101 0.0037 + 163.00 0.0070 0.0037 + 164.00 0.0031 0.0036 + 165.00 0.0130 0.0036 + 166.00 0.0082 0.0036 + 167.00 0.0053 0.0036 + 168.00 0.0138 0.0037 + 169.00 0.0190 0.0037 + 170.00 0.0145 0.0036 + 171.00 0.0144 0.0036 + 172.00 0.0104 0.0036 + 173.00 0.0104 0.0036 + 174.00 0.0163 0.0037 + 175.00 0.0150 0.0036 + 176.00 0.0168 0.0036 + 177.00 0.0115 0.0037 + 178.00 0.0117 0.0037 + 179.00 0.0177 0.0036 + 180.00 0.0108 0.0037 + 181.00 0.0145 0.0036 + 182.00 0.0042 0.0035 + 183.00 0.0103 0.0035 + 184.00 0.0135 0.0036 + 185.00 0.0033 0.0036 + 186.00 0.0122 0.0036 + 187.00 0.0143 0.0035 + 188.00 0.0097 0.0035 + 189.00 0.0065 0.0036 + 190.00 0.0113 0.0035 + 191.00 0.0042 0.0035 + 192.00 0.0110 0.0036 + 193.00 0.0074 0.0036 + 194.00 0.0124 0.0035 + 195.00 0.0131 0.0036 + 196.00 0.0067 0.0035 + 197.00 0.0145 0.0035 +ENDDATA 187 +ENDSUBENT 205 +SUBENT E1898003 20050914 20050914 E032 +BIB 5 9 +REACTION (1-H-2(P,X)0-NN-1,,DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 222 mg/cm2 for CD2 and 172 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.1, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 9 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 346.0 2.0 22.0 +ENDCOMMON 3 +DATA 3 175 +E-DGD DATA ERR-S +MEV MB/SR/MEV MB/SR/MEV + 23.00 0.0095 0.0034 + 24.00 0.0104 0.0045 + 25.00 0.0036 0.0069 + 26.00 -0.0016 0.0065 + 27.00 0.0124 0.0052 + 28.00 0.0252 0.0048 + 29.00 0.0489 0.0050 + 30.00 0.0691 0.0055 + 31.00 0.0699 0.0056 + 32.00 0.0573 0.0055 + 33.00 0.0741 0.0057 + 34.00 0.0793 0.0058 + 35.00 0.0837 0.0060 + 36.00 0.0938 0.0062 + 37.00 0.0966 0.0063 + 38.00 0.1080 0.0066 + 39.00 0.1207 0.0066 + 40.00 0.1259 0.0068 + 41.00 0.1335 0.0069 + 42.00 0.1687 0.0073 + 43.00 0.1873 0.0076 + 44.00 0.1996 0.0078 + 45.00 0.2246 0.0082 + 46.00 0.2349 0.0083 + 47.00 0.2740 0.0087 + 48.00 0.2966 0.0090 + 49.00 0.3165 0.0092 + 50.00 0.3171 0.0093 + 51.00 0.3558 0.0096 + 52.00 0.3381 0.0096 + 53.00 0.3748 0.0098 + 54.00 0.3826 0.0100 + 55.00 0.3671 0.0099 + 56.00 0.3693 0.0099 + 57.00 0.3758 0.0100 + 58.00 0.3779 0.0101 + 59.00 0.3515 0.0098 + 60.00 0.3344 0.0097 + 61.00 0.3194 0.0097 + 62.00 0.3161 0.0096 + 63.00 0.3052 0.0095 + 64.00 0.2639 0.0092 + 65.00 0.2636 0.0092 + 66.00 0.2524 0.0091 + 67.00 0.2411 0.0089 + 68.00 0.2179 0.0088 + 69.00 0.2013 0.0086 + 70.00 0.1810 0.0084 + 71.00 0.1784 0.0084 + 72.00 0.1717 0.0083 + 73.00 0.1690 0.0083 + 74.00 0.1567 0.0081 + 75.00 0.1484 0.0081 + 76.00 0.1385 0.0080 + 77.00 0.1209 0.0078 + 78.00 0.1316 0.0079 + 79.00 0.1071 0.0076 + 80.00 0.1108 0.0078 + 81.00 0.0997 0.0076 + 82.00 0.0828 0.0073 + 83.00 0.0879 0.0075 + 84.00 0.0775 0.0074 + 85.00 0.0718 0.0072 + 86.00 0.0770 0.0073 + 87.00 0.0934 0.0074 + 88.00 0.0711 0.0072 + 89.00 0.0625 0.0071 + 90.00 0.0640 0.0071 + 91.00 0.0497 0.0069 + 92.00 0.0509 0.0068 + 93.00 0.0606 0.0069 + 94.00 0.0502 0.0068 + 95.00 0.0517 0.0067 + 96.00 0.0378 0.0066 + 97.00 0.0536 0.0067 + 98.00 0.0438 0.0066 + 99.00 0.0453 0.0066 + 100.00 0.0468 0.0065 + 101.00 0.0458 0.0065 + 102.00 0.0426 0.0063 + 103.00 0.0273 0.0063 + 104.00 0.0299 0.0063 + 105.00 0.0312 0.0062 + 106.00 0.0324 0.0062 + 107.00 0.0327 0.0062 + 108.00 0.0222 0.0060 + 109.00 0.0291 0.0060 + 110.00 0.0236 0.0058 + 111.00 0.0190 0.0059 + 112.00 0.0162 0.0058 + 113.00 0.0131 0.0057 + 114.00 0.0275 0.0058 + 115.00 0.0231 0.0058 + 116.00 0.0182 0.0057 + 117.00 0.0161 0.0056 + 118.00 0.0243 0.0056 + 119.00 0.0217 0.0056 + 120.00 0.0202 0.0055 + 121.00 0.0232 0.0056 + 122.00 0.0234 0.0055 + 123.00 0.0180 0.0054 + 124.00 0.0175 0.0053 + 125.00 0.0212 0.0054 + 126.00 0.0300 0.0055 + 127.00 0.0116 0.0052 + 128.00 0.0133 0.0052 + 129.00 0.0151 0.0052 + 130.00 0.0105 0.0051 + 131.00 0.0182 0.0051 + 132.00 0.0128 0.0051 + 133.00 0.0176 0.0050 + 134.00 0.0236 0.0052 + 135.00 0.0127 0.0051 + 136.00 0.0126 0.0049 + 137.00 0.0124 0.0049 + 138.00 0.0186 0.0050 + 139.00 0.0120 0.0048 + 140.00 0.0030 0.0047 + 141.00 0.0181 0.0048 + 142.00 0.0094 0.0047 + 143.00 0.0145 0.0048 + 144.00 0.0178 0.0049 + 145.00 0.0194 0.0048 + 146.00 0.0160 0.0047 + 147.00 0.0077 0.0045 + 148.00 0.0101 0.0046 + 149.00 0.0136 0.0047 + 150.00 0.0101 0.0046 + 151.00 0.0131 0.0045 + 152.00 0.0046 0.0044 + 153.00 0.0156 0.0045 + 154.00 0.0105 0.0044 + 155.00 0.0071 0.0044 + 156.00 0.0133 0.0044 + 157.00 0.0094 0.0043 + 158.00 0.0166 0.0045 + 159.00 0.0137 0.0044 + 160.00 0.0120 0.0043 + 161.00 0.0137 0.0044 + 162.00 0.0105 0.0043 + 163.00 0.0150 0.0044 + 164.00 0.0065 0.0042 + 165.00 0.0094 0.0042 + 166.00 0.0126 0.0042 + 167.00 0.0052 0.0041 + 168.00 0.0167 0.0043 + 169.00 0.0102 0.0041 + 170.00 0.0059 0.0041 + 171.00 0.0094 0.0041 + 172.00 0.0096 0.0042 + 173.00 0.0094 0.0041 + 174.00 0.0058 0.0040 + 175.00 0.0103 0.0042 + 176.00 0.0066 0.0041 + 177.00 0.0183 0.0042 + 178.00 0.0086 0.0040 + 179.00 0.0143 0.0041 + 180.00 0.0073 0.0039 + 181.00 0.0077 0.0040 + 182.00 0.0203 0.0041 + 183.00 0.0069 0.0038 + 184.00 0.0205 0.0043 + 185.00 0.0107 0.0041 + 186.00 0.0133 0.0040 + 187.00 0.0078 0.0039 + 188.00 0.0071 0.0039 + 189.00 0.0036 0.0038 + 190.00 0.0072 0.0039 + 191.00 0.0157 0.0040 + 192.00 0.0061 0.0039 + 193.00 0.0122 0.0039 + 194.00 0.0122 0.0039 + 195.00 0.0088 0.0039 + 196.00 0.0123 0.0040 + 197.00 0.0023 0.0038 +ENDDATA 177 +ENDSUBENT 195 +SUBENT E1898004 20050914 20050914 E032 +BIB 5 9 +REACTION (1-H-2(P,X)0-NN-1,,DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 222 mg/cm2 for CD2 and 172 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.1, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 9 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 345.0 2.0 27.0 +ENDCOMMON 3 +DATA 3 180 +E-DGD DATA ERR-S +MEV MB/SR/MEV MB/SR/MEV + 18.00 0.0010 0.0010 + 19.00 -0.0011 0.0007 + 20.00 -0.0001 0.0008 + 21.00 0.0007 0.0008 + 22.00 0.0002 0.0008 + 23.00 0.0009 0.0016 + 24.00 0.0017 0.0026 + 25.00 0.0021 0.0026 + 26.00 -0.0010 0.0026 + 27.00 -0.0062 0.0043 + 28.00 0.0044 0.0049 + 29.00 0.0092 0.0042 + 30.00 0.0047 0.0036 + 31.00 -0.0021 0.0034 + 32.00 -0.0037 0.0032 + 33.00 0.0031 0.0035 + 34.00 -0.0018 0.0034 + 35.00 0.0031 0.0037 + 36.00 0.0034 0.0038 + 37.00 0.0000 0.0039 + 38.00 -0.0039 0.0039 + 39.00 0.0065 0.0041 + 40.00 0.0027 0.0042 + 41.00 0.0040 0.0042 + 42.00 0.0239 0.0046 + 43.00 0.0208 0.0047 + 44.00 0.0229 0.0048 + 45.00 0.0217 0.0048 + 46.00 0.0342 0.0050 + 47.00 0.0252 0.0049 + 48.00 0.0282 0.0051 + 49.00 0.0230 0.0050 + 50.00 0.0225 0.0051 + 51.00 0.0281 0.0053 + 52.00 0.0189 0.0052 + 53.00 0.0318 0.0054 + 54.00 0.0415 0.0056 + 55.00 0.0364 0.0057 + 56.00 0.0458 0.0058 + 57.00 0.0518 0.0060 + 58.00 0.0601 0.0061 + 59.00 0.0590 0.0061 + 60.00 0.0627 0.0062 + 61.00 0.0741 0.0065 + 62.00 0.0856 0.0066 + 63.00 0.0743 0.0066 + 64.00 0.0936 0.0069 + 65.00 0.1007 0.0070 + 66.00 0.1181 0.0073 + 67.00 0.1267 0.0074 + 68.00 0.1402 0.0076 + 69.00 0.1526 0.0079 + 70.00 0.1584 0.0078 + 71.00 0.1589 0.0080 + 72.00 0.1787 0.0082 + 73.00 0.1765 0.0082 + 74.00 0.1941 0.0085 + 75.00 0.2005 0.0087 + 76.00 0.2172 0.0088 + 77.00 0.2229 0.0088 + 78.00 0.2187 0.0087 + 79.00 0.2138 0.0088 + 80.00 0.2121 0.0087 + 81.00 0.2181 0.0089 + 82.00 0.2204 0.0089 + 83.00 0.2067 0.0088 + 84.00 0.2146 0.0089 + 85.00 0.2035 0.0087 + 86.00 0.1975 0.0086 + 87.00 0.1959 0.0087 + 88.00 0.1787 0.0084 + 89.00 0.1830 0.0085 + 90.00 0.1687 0.0084 + 91.00 0.1517 0.0082 + 92.00 0.1550 0.0082 + 93.00 0.1578 0.0082 + 94.00 0.1560 0.0082 + 95.00 0.1174 0.0078 + 96.00 0.1331 0.0079 + 97.00 0.1366 0.0080 + 98.00 0.1123 0.0078 + 99.00 0.1121 0.0077 + 100.00 0.1027 0.0076 + 101.00 0.0963 0.0074 + 102.00 0.0801 0.0072 + 103.00 0.0885 0.0073 + 104.00 0.0975 0.0074 + 105.00 0.0669 0.0072 + 106.00 0.0803 0.0072 + 107.00 0.0739 0.0071 + 108.00 0.0672 0.0071 + 109.00 0.0850 0.0072 + 110.00 0.0487 0.0069 + 111.00 0.0430 0.0068 + 112.00 0.0654 0.0070 + 113.00 0.0467 0.0068 + 114.00 0.0415 0.0068 + 115.00 0.0343 0.0066 + 116.00 0.0494 0.0069 + 117.00 0.0472 0.0068 + 118.00 0.0402 0.0066 + 119.00 0.0353 0.0066 + 120.00 0.0363 0.0065 + 121.00 0.0437 0.0066 + 122.00 0.0358 0.0065 + 123.00 0.0388 0.0065 + 124.00 0.0318 0.0065 + 125.00 0.0283 0.0064 + 126.00 0.0236 0.0063 + 127.00 0.0211 0.0062 + 128.00 0.0406 0.0064 + 129.00 0.0330 0.0064 + 130.00 0.0239 0.0062 + 131.00 0.0182 0.0061 + 132.00 0.0246 0.0061 + 133.00 0.0239 0.0059 + 134.00 0.0280 0.0062 + 135.00 0.0235 0.0060 + 136.00 0.0202 0.0059 + 137.00 0.0086 0.0058 + 138.00 0.0141 0.0058 + 139.00 0.0195 0.0058 + 140.00 0.0237 0.0059 + 141.00 0.0226 0.0059 + 142.00 0.0161 0.0058 + 143.00 0.0169 0.0056 + 144.00 0.0158 0.0058 + 145.00 0.0143 0.0056 + 146.00 0.0111 0.0056 + 147.00 0.0196 0.0056 + 148.00 0.0165 0.0056 + 149.00 0.0072 0.0055 + 150.00 0.0136 0.0055 + 151.00 0.0192 0.0054 + 152.00 0.0254 0.0058 + 153.00 0.0104 0.0055 + 154.00 0.0233 0.0055 + 155.00 0.0142 0.0054 + 156.00 0.0207 0.0054 + 157.00 0.0197 0.0055 + 158.00 0.0122 0.0053 + 159.00 -0.0014 0.0050 + 160.00 0.0139 0.0052 + 161.00 0.0162 0.0053 + 162.00 0.0113 0.0052 + 163.00 0.0044 0.0051 + 164.00 0.0129 0.0053 + 165.00 0.0087 0.0050 + 166.00 0.0081 0.0051 + 167.00 0.0035 0.0050 + 168.00 0.0138 0.0052 + 169.00 0.0099 0.0050 + 170.00 0.0045 0.0050 + 171.00 0.0156 0.0052 + 172.00 0.0107 0.0050 + 173.00 0.0055 0.0048 + 174.00 0.0090 0.0049 + 175.00 0.0064 0.0049 + 176.00 0.0101 0.0049 + 177.00 0.0144 0.0050 + 178.00 0.0071 0.0047 + 179.00 0.0117 0.0049 + 180.00 0.0063 0.0047 + 181.00 0.0071 0.0048 + 182.00 0.0093 0.0049 + 183.00 0.0058 0.0048 + 184.00 0.0097 0.0046 + 185.00 0.0017 0.0046 + 186.00 0.0064 0.0046 + 187.00 0.0111 0.0047 + 188.00 0.0085 0.0047 + 189.00 0.0074 0.0046 + 190.00 0.0054 0.0046 + 191.00 0.0071 0.0046 + 192.00 0.0091 0.0048 + 193.00 0.0053 0.0047 + 194.00 0.0038 0.0045 + 195.00 0.0118 0.0048 + 196.00 0.0159 0.0047 + 197.00 -0.0028 0.0045 +ENDDATA 182 +ENDSUBENT 200 +SUBENT E1898005 20050914 20050914 E032 +BIB 5 9 +REACTION (1-H-2(P,X)0-NN-1,,POL/DA/DE,,ANA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 222 mg/cm2 for CD2 and 172 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.1, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 9 +COMMON 2 3 +EN ANG +MEV ADEG + 345.0 16.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-S +MEV NO-DIM NO-DIM + 20.00 0.118 0.002 + 25.00 0.128 0.002 + 30.00 0.128 0.001 + 35.00 0.130 0.002 + 40.00 0.129 0.002 + 45.00 0.135 0.003 + 50.00 0.129 0.004 + 55.00 0.137 0.005 + 60.00 0.134 0.007 + 65.00 0.127 0.008 + 70.00 0.146 0.009 + 75.00 0.120 0.010 + 80.00 0.135 0.012 + 85.00 0.119 0.013 + 90.00 0.102 0.014 + 95.00 0.124 0.015 + 100.00 0.078 0.016 + 105.00 0.070 0.017 + 110.00 0.085 0.017 + 115.00 0.024 0.017 + 120.00 0.052 0.017 + 125.00 0.048 0.018 + 130.00 0.022 0.019 + 135.00 0.009 0.019 + 140.00 0.004 0.019 + 145.00 -0.070 0.019 + 150.00 -0.063 0.020 + 155.00 -0.039 0.020 + 160.00 -0.037 0.020 + 165.00 -0.077 0.021 + 170.00 -0.087 0.020 + 175.00 -0.063 0.022 + 180.00 -0.104 0.021 + 185.00 -0.075 0.021 + 190.00 -0.091 0.021 + 195.00 -0.106 0.022 +ENDDATA 38 +ENDSUBENT 56 +SUBENT E1898006 20050914 20050914 E032 +BIB 5 9 +REACTION (1-H-2(P,X)0-NN-1,,POL/DA/DE,,ANA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 222 mg/cm2 for CD2 and 172 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.1, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 9 +COMMON 2 3 +EN ANG +MEV ADEG + 346.0 22.0 +ENDCOMMON 3 +DATA 3 44 +E-DGD DATA ERR-S +MEV NO-DIM NO-DIM + 30.00 0.004 0.008 + 35.00 0.058 0.005 + 40.00 0.143 0.004 + 45.00 0.154 0.003 + 50.00 0.161 0.002 + 55.00 0.165 0.002 + 60.00 0.163 0.002 + 65.00 0.163 0.002 + 70.00 0.167 0.003 + 75.00 0.165 0.004 + 80.00 0.178 0.005 + 85.00 0.168 0.006 + 90.00 0.157 0.007 + 95.00 0.166 0.008 + 100.00 0.152 0.010 + 105.00 0.146 0.011 + 110.00 0.138 0.012 + 115.00 0.127 0.013 + 120.00 0.124 0.014 + 125.00 0.114 0.015 + 130.00 0.102 0.016 + 135.00 0.094 0.016 + 140.00 0.078 0.017 + 145.00 0.078 0.018 + 150.00 0.086 0.018 + 155.00 0.034 0.019 + 160.00 0.036 0.019 + 165.00 0.002 0.020 + 170.00 0.002 0.019 + 175.00 0.025 0.019 + 180.00 0.010 0.020 + 185.00 -0.023 0.020 + 190.00 -0.052 0.021 + 195.00 -0.048 0.021 + 200.00 -0.037 0.021 + 205.00 -0.046 0.021 + 210.00 -0.044 0.020 + 215.00 -0.074 0.017 + 220.00 -0.076 0.024 + 225.00 -0.018 0.022 + 230.00 -0.035 0.024 + 235.00 -0.033 0.023 + 240.00 0.001 0.023 + 245.00 -0.069 0.025 +ENDDATA 46 +ENDSUBENT 64 +SUBENT E1898007 20050914 20050914 E032 +BIB 5 9 +REACTION (1-H-2(P,X)0-NN-1,,POL/DA/DE,,ANA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 222 mg/cm2 for CD2 and 172 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.1, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 9 +COMMON 2 3 +EN ANG +MEV ADEG + 345.0 27.0 +ENDCOMMON 3 +DATA 3 31 +E-DGD DATA ERR-S +MEV NO-DIM NO-DIM + 45.00 -0.166 0.010 + 50.00 0.030 0.008 + 55.00 0.121 0.006 + 60.00 0.156 0.004 + 65.00 0.172 0.003 + 70.00 0.183 0.002 + 75.00 0.194 0.002 + 80.00 0.190 0.002 + 85.00 0.193 0.002 + 90.00 0.193 0.002 + 95.00 0.191 0.003 + 100.00 0.194 0.003 + 105.00 0.185 0.004 + 110.00 0.183 0.005 + 115.00 0.175 0.006 + 120.00 0.167 0.007 + 125.00 0.176 0.008 + 130.00 0.169 0.009 + 135.00 0.152 0.009 + 140.00 0.153 0.010 + 145.00 0.139 0.011 + 150.00 0.114 0.012 + 155.00 0.087 0.013 + 160.00 0.084 0.014 + 165.00 0.090 0.013 + 170.00 0.072 0.014 + 175.00 0.045 0.015 + 180.00 0.047 0.015 + 185.00 0.016 0.016 + 190.00 0.024 0.016 + 195.00 0.025 0.015 +ENDDATA 33 +ENDSUBENT 51 +SUBENT E1898008 20050914 20050914 E032 +BIB 5 9 +REACTION (1-H-2(P,X)0-NN-1,,POL/DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 662 mg/cm2 for CD2 and 682 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.1, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 9 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 345.0 3.0 16.0 +ENDCOMMON 3 +DATA 3 17 +E-DGD DATA ERR-S +MEV NO-DIM NO-DIM + 20.00 0.1541 0.0167 + 25.00 0.1799 0.0141 + 30.00 0.1432 0.0116 + 35.00 0.1603 0.0127 + 40.00 0.1542 0.0167 + 45.00 0.1404 0.0233 + 50.00 0.2472 0.0325 + 55.00 0.1804 0.0417 + 60.00 0.2106 0.0535 + 65.00 0.2062 0.0626 + 72.50 0.3418 0.0548 + 87.50 0.1515 0.0511 + 107.50 0.3493 0.0634 + 127.50 0.1382 0.0720 + 147.50 0.2355 0.0788 + 167.50 0.1989 0.0926 + 187.50 0.2244 0.1079 +ENDDATA 19 +ENDSUBENT 37 +SUBENT E1898009 20050914 20050914 E032 +BIB 5 9 +REACTION (1-H-2(P,X)0-NN-1,,POL/DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 662 mg/cm2 for CD2 and 682 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.1, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 9 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 346.0 3.0 22.0 +ENDCOMMON 3 +DATA 3 16 +E-DGD DATA ERR-S +MEV NO-DIM NO-DIM + 32.50 0.2147 0.0268 + 40.00 0.2083 0.0241 + 45.00 0.1898 0.0173 + 50.00 0.1796 0.0133 + 55.00 0.1893 0.0117 + 60.00 0.1650 0.0118 + 65.00 0.1768 0.0135 + 70.00 0.1952 0.0164 + 75.00 0.1793 0.0205 + 80.00 0.1619 0.0254 + 87.50 0.1847 0.0236 + 102.50 0.1861 0.0250 + 122.50 0.1754 0.0350 + 142.50 0.2803 0.0430 + 162.50 0.1171 0.0507 + 182.50 0.1750 0.0580 +ENDDATA 18 +ENDSUBENT 36 +SUBENT E1898010 20050914 20050914 E032 +BIB 5 9 +REACTION (1-H-2(P,X)0-NN-1,,POL/DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 662 mg/cm2 for CD2 and 682 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.1, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 9 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 345.0 3.0 27.0 +ENDCOMMON 3 +DATA 3 19 +E-DGD DATA ERR-S +MEV NO-DIM NO-DIM + 47.50 0.2104 0.0448 + 55.00 0.2449 0.0442 + 60.00 0.2192 0.0309 + 65.00 0.2250 0.0220 + 70.00 0.2239 0.0165 + 75.00 0.2180 0.0135 + 80.00 0.2031 0.0123 + 85.00 0.2309 0.0126 + 90.00 0.2491 0.0143 + 95.00 0.2191 0.0171 + 100.00 0.2332 0.0210 + 105.00 0.2640 0.0255 + 110.00 0.2536 0.0315 + 115.00 0.2609 0.0377 + 122.50 0.2612 0.0337 + 132.50 0.1957 0.0432 + 147.50 0.2560 0.0404 + 167.50 0.2374 0.0543 + 187.50 0.2871 0.0695 +ENDDATA 21 +ENDSUBENT 39 +SUBENT E1898011 20050914 20050914 E032 +BIB 5 11 +REACTION 1(1-H-2(P,X)0-NN-1,SS,POL/DA/DE,,D) + 2(1-H-2(P,X)0-NN-1,SL,POL/DA/DE,,D) + 3(1-H-2(P,X)0-NN-1,NN,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 662 mg/cm2 for CD2 and 682 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.2, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 11 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 345.0 3.0 16.0 +ENDCOMMON 3 +DATA 7 17 +E-DGD DATA 1ERR-S 1DATA 2ERR-S 2DATA 3 +ERR-S 3 +MEV NO-DIM NO-DIM NO-DIM NO-DIM NO-DIM +NO-DIM + 20.00 -0.5678 0.0198 0.0207 0.0216 0.0581 + 0.0221 + 25.00 -0.6348 0.0166 0.0379 0.0181 0.1009 + 0.0186 + 30.00 -0.6503 0.0138 0.1042 0.0151 0.0744 + 0.0153 + 35.00 -0.6331 0.0152 0.0928 0.0167 0.0611 + 0.0168 + 40.00 -0.6491 0.0200 0.0677 0.0218 0.0689 + 0.0221 + 45.00 -0.6460 0.0280 0.1291 0.0304 0.0530 + 0.0308 + 50.00 -0.6327 0.0393 0.0683 0.0424 0.0127 + 0.0428 + 55.00 -0.5753 0.0507 0.1192 0.0546 0.0647 + 0.0550 + 60.00 -0.6056 0.0657 0.0874 0.0704 -0.0040 + 0.0707 + 65.00 -0.6106 0.0773 0.0101 0.0829 -0.0270 + 0.0826 + 72.50 -0.5507 0.0684 0.1083 0.0733 0.1481 + 0.0723 + 87.50 -0.5372 0.0651 0.0777 0.0697 0.0795 + 0.0674 + 107.50 -0.3535 0.0837 0.2393 0.0896 0.0865 + 0.0837 + 127.50 -0.2789 0.0984 -0.1233 0.1052 0.0005 + 0.0950 + 147.50 -0.3428 0.1121 0.1005 0.1199 0.0065 + 0.1039 + 167.50 -0.2183 0.1384 0.1677 0.1479 -0.2814 + 0.1222 + 187.50 -0.0478 0.1709 -0.0505 0.1829 -0.0302 + 0.1423 +ENDDATA 38 +ENDSUBENT 58 +NOSUBENT E1898012 20050914 20050914 E032 +SUBENT E1898013 20050914 20050914 E032 +BIB 5 11 +REACTION 1(1-H-2(P,X)0-NN-1,SS,POL/DA/DE,,D) + 2(1-H-2(P,X)0-NN-1,SL,POL/DA/DE,,D) + 3(1-H-2(P,X)0-NN-1,NN,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 662 mg/cm2 for CD2 and 682 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.2, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 11 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 345.0 3.0 27.0 +ENDCOMMON 3 +DATA 7 19 +E-DGD DATA 1ERR-S 1DATA 2ERR-S 2DATA 3 +ERR-S 3 +MEV NO-DIM NO-DIM NO-DIM NO-DIM NO-DIM +NO-DIM + 47.50 0.1441 0.0623 -0.2813 0.0627 -0.1141 + 0.0597 + 55.00 -0.0940 0.0622 -0.1549 0.0626 -0.0823 + 0.0589 + 60.00 -0.1588 0.0438 -0.2034 0.0440 -0.0426 + 0.0411 + 65.00 -0.1303 0.0317 -0.1908 0.0317 -0.0899 + 0.0293 + 70.00 -0.1239 0.0240 -0.2192 0.0240 -0.1067 + 0.0220 + 75.00 -0.1150 0.0199 -0.2352 0.0199 -0.0700 + 0.0180 + 80.00 -0.0760 0.0183 -0.2273 0.0183 -0.0900 + 0.0164 + 85.00 -0.1038 0.0189 -0.2403 0.0189 -0.0805 + 0.0168 + 90.00 -0.1243 0.0215 -0.2329 0.0215 -0.0509 + 0.0191 + 95.00 -0.1187 0.0259 -0.3014 0.0260 -0.0422 + 0.0228 + 100.00 -0.1470 0.0317 -0.2164 0.0319 -0.0522 + 0.0279 + 105.00 -0.1037 0.0388 -0.2508 0.0391 -0.0406 + 0.0340 + 110.00 -0.1919 0.0480 -0.2401 0.0484 -0.0043 + 0.0420 + 115.00 -0.2605 0.0579 -0.2950 0.0583 0.0592 + 0.0503 + 122.50 -0.1988 0.0522 -0.1365 0.0527 -0.0405 + 0.0450 + 132.50 -0.1880 0.0678 -0.1907 0.0685 0.0246 + 0.0575 + 147.50 -0.2329 0.0649 -0.1838 0.0655 -0.0140 + 0.0538 + 167.50 -0.1169 0.0905 -0.1347 0.0915 0.1601 + 0.0724 + 187.50 -0.0373 0.1210 -0.1228 0.1222 -0.0908 + 0.0928 +ENDDATA 42 +ENDSUBENT 62 +SUBENT E1898014 20050914 20050914 E032 +BIB 5 10 +REACTION 1(1-H-2(P,X)0-NN-1,LS,POL/DA/DE,,D) + 2(1-H-2(P,X)0-NN-1,LL,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 662 mg/cm2 for CD2 and 682 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.2, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 10 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 345.0 3.0 16.0 +ENDCOMMON 3 +DATA 5 17 +E-DGD DATA 1ERR-S 1DATA 2ERR-S 2 +MEV NO-DIM NO-DIM NO-DIM NO-DIM + 20.00 -0.1109 0.0198 -0.4643 0.0216 + 25.00 -0.0451 0.0166 -0.3690 0.0181 + 30.00 -0.0339 0.0138 -0.3695 0.0151 + 35.00 -0.0360 0.0152 -0.3829 0.0167 + 40.00 -0.0042 0.0200 -0.3646 0.0218 + 45.00 -0.0137 0.0281 -0.3934 0.0304 + 50.00 0.0582 0.0393 -0.4054 0.0424 + 55.00 -0.0010 0.0508 -0.3685 0.0546 + 60.00 0.0659 0.0657 -0.3282 0.0704 + 65.00 0.0783 0.0773 -0.3920 0.0829 + 72.50 0.1045 0.0685 -0.3591 0.0733 + 87.50 0.0837 0.0652 -0.3370 0.0698 + 107.50 0.0681 0.0837 -0.4452 0.0896 + 127.50 0.0682 0.0982 -0.3925 0.1049 + 147.50 0.0321 0.1112 -0.3945 0.1189 + 167.50 0.1598 0.1359 -0.3034 0.1452 + 187.50 0.0007 0.1643 0.2626 0.1757 +ENDDATA 19 +ENDSUBENT 38 +SUBENT E1898015 20050914 20050914 E032 +BIB 5 10 +REACTION 1(1-H-2(P,X)0-NN-1,LS,POL/DA/DE,,D) + 2(1-H-2(P,X)0-NN-1,LL,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 662 mg/cm2 for CD2 and 682 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.2, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 10 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 346.0 3.0 22.0 +ENDCOMMON 3 +DATA 5 16 +E-DGD DATA 1ERR-S 1DATA 2ERR-S 2 +MEV NO-DIM NO-DIM NO-DIM NO-DIM + 32.50 -0.1703 0.0647 -0.6634 0.0439 + 40.00 -0.0756 0.0587 -0.5785 0.0396 + 45.00 -0.0688 0.0422 -0.5833 0.0284 + 50.00 -0.0031 0.0327 -0.5725 0.0219 + 55.00 -0.0690 0.0287 -0.5437 0.0193 + 60.00 -0.0576 0.0293 -0.5464 0.0198 + 65.00 -0.0133 0.0335 -0.5578 0.0228 + 70.00 -0.0899 0.0412 -0.5652 0.0279 + 75.00 -0.0710 0.0519 -0.4224 0.0353 + 80.00 0.0592 0.0647 -0.5715 0.0442 + 87.50 0.0217 0.0609 -0.4725 0.0416 + 102.50 0.0261 0.0659 -0.5230 0.0452 + 122.50 0.1760 0.0960 -0.3958 0.0659 + 142.50 0.0871 0.1224 -0.1914 0.0840 + 162.50 -0.3736 0.1519 -0.1973 0.1037 + 182.50 -0.1799 0.1809 -0.4491 0.1237 +ENDDATA 18 +ENDSUBENT 37 +SUBENT E1898016 20050914 20050914 E032 +BIB 5 10 +REACTION 1(1-H-2(P,X)0-NN-1,LS,POL/DA/DE,,D) + 2(1-H-2(P,X)0-NN-1,LL,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer from projectile to target +SAMPLE Target-thickness: 662 mg/cm2 for CD2 and 682 mg/cm2 + for C +ERR-ANALYS (ERR-S) Statistical uncertainty +STATUS (TABLE) Data (Fig.2, p044602-4 in reference) received + by e-mail from T.Wakasa (2004.05.24) +ENDBIB 10 +COMMON 3 3 +EN E-RSL ANG +MEV MEV ADEG + 345.0 3.0 27.0 +ENDCOMMON 3 +DATA 5 19 +E-DGD DATA 1ERR-S 1DATA 2ERR-S 2 +MEV NO-DIM NO-DIM NO-DIM NO-DIM + 47.50 -0.1978 0.0623 -0.7065 0.0627 + 55.00 -0.0423 0.0622 -0.7176 0.0625 + 60.00 0.0058 0.0438 -0.6146 0.0440 + 65.00 -0.0611 0.0316 -0.6345 0.0317 + 70.00 -0.1433 0.0240 -0.6595 0.0239 + 75.00 -0.1114 0.0199 -0.6205 0.0199 + 80.00 -0.0945 0.0183 -0.6478 0.0182 + 85.00 -0.0922 0.0189 -0.6554 0.0189 + 90.00 -0.1068 0.0215 -0.6507 0.0215 + 95.00 -0.1399 0.0258 -0.5902 0.0259 + 100.00 -0.0980 0.0317 -0.5886 0.0318 + 105.00 0.0011 0.0388 -0.5444 0.0390 + 110.00 -0.1019 0.0480 -0.5663 0.0483 + 115.00 -0.0607 0.0578 -0.6502 0.0583 + 122.50 -0.0536 0.0522 -0.5186 0.0527 + 132.50 -0.0483 0.0677 -0.4047 0.0685 + 147.50 -0.0498 0.0649 -0.4581 0.0655 + 167.50 0.0833 0.0906 -0.3304 0.0915 + 187.50 0.0472 0.1210 -0.1928 0.1222 +ENDDATA 21 +ENDSUBENT 40 +ENDENTRY 16 diff --git a/exforall/E18/E1899.x4 b/exforall/E18/E1899.x4 new file mode 100644 index 000000000..c65041471 --- /dev/null +++ b/exforall/E18/E1899.x4 @@ -0,0 +1,317 @@ +ENTRY E1899 20050914 20050914 E032 +SUBENT E1899001 20050914 20050914 E032 +BIB 12 69 +TITLE Systematics of the bimodal isoscalar giant dipole + resonance +AUTHOR (M.Uchida, H.Sakaguchi, M.Itoh, M.Yosoi, T.Kawabata, + Y.Yasuda, H.Takeda, T.Murakami, S.Terashima, S.Kishi, + U.Garg, P.Boutachkov, M.Hedden, B.Kharraja, M.Koss, + B.K.Nayak, S.Zhu, M.Fujiwara, H.Fujimura, H.P.Yoshida, + K.Hara, H.Akimune, M.N.Harakeh) +INSTITUTE (2JPNKTO) Department of Physics + (1USANOT) Physics Department + (2JPNOSA) Research Center for Nuclear Physics + (2JPNJAE) Advanced Science Research Center + (2JPNKON) Department of Physics + (2NEDKVI) +REFERENCE (J,PR/C,69,(5),051301,200405) Main reference + (T,Uchida,115,200306) + Numerical data for double differential cross section +REL-REF (N,E1886002,M.Itoh+,J,PR/C,68,(6),064602,200312) + Spectrum for 144Sm shown in Fig.1(c) of the main + reference given +PART-DET (A) +INC-SOURCE Charge of incident ion is +2. +SAMPLE - Target enrichment is unknown. + - Chemical-form of target is element. + - Physical-form of target is solid. + - Target is self supported. +FACILITY (CYCLO,2JPNOSA) Ring cyclotron at Research Center for + Nuclear Physics (RCNP) +DETECTOR (MAGSP) To analyze inelastically scattered particles, + Grand Raiden [M.Fujiwara et al., Nucl. + Instrum. Methods Phys. Res. A 422, 484 + (1999)]. + (MWDC) Focal-plane detection system [T. Noro et al., + RCNP Annual Report, 1991, p177] + (SCIN) Two plastic scintillation counters. Focal-plane + detection system. +ADD-RES E1899.007:40-ZR-90(A,INL)40-ZR-90 + Strength function (Strength distribution for + T=0, L=0 transitions, ISGMR) + See NRDF D1899 DATA,6 for detail. + E1899.008:40-ZR-90(A,INL)40-ZR-90 + Strength function (Strength distribution for + T=0, L=1 transitions, ISGDR) + See NRDF D1899 DATA,7 for detail. + E1899.009:50-SN-116(A,INL)50-SN-116 + Strength function (Strength distribution for + T=0, L=0 transitions, ISGMR) + See NRDF D1899 DATA,8 for detail. + E1899.010:50-SN-116(A,INL)50-SN-116 + Strength function (Strength distribution for + T=0, L=1 transitions, ISGDR) + See NRDF D1899 DATA,9 for detail. + E1899.011:82-PB-208(A,INL)82-PB-208 + Strength function (Strength distribution for + T=0, L=0 transitions, ISGMR) + See NRDF D1899 DATA,10 for detail. + E1899.012:82-PB-208(A,INL)82-PB-208 + Strength function (Strength distribution for + T=0, L=1 transitions, ISGDR) + See NRDF D1899 DATA,11 for detail. + E1899.013:40-ZR-90(A,INL)40-ZR-90 + Energy weighted sum rule + See NRDF D1899 DATA,12 for detail. + E1899.014:50-SN-116(A,INL)50-SN-116 + Energy weighted sum rule + See NRDF D1899 DATA,13 for detail. + E1899.015:82-PB-208(A,INL)82-PB-208 + Energy weighted sum rule + See NRDF D1899 DATA,14 for detail. +HISTORY (20041107C) Kc + Sr + On +ENDBIB 69 +COMMON 1 3 +EN +MEV + 386.0 +ENDCOMMON 3 +ENDSUBENT 76 +SUBENT E1899002 20050914 20050914 E032 +BIB 4 7 +REACTION (40-ZR-90(A,INL)40-ZR-90,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-EXC,40-ZR-90) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data (Fig.1 (a), p051301-2 in reference) taken + from doctorial thesis of M. Uchida +ENDBIB 7 +COMMON 1 3 +ANG-CM +ADEG + 0.69 +ENDCOMMON 3 +DATA 3 26 +E-EXC DATA-CM DATA-ERR +MEV MB/SR/MEV MB/SR/MEV + 8.5 27.89 0.40 + 9.5 32.77 0.45 + 10.5 31.17 0.44 + 11.5 37.87 0.51 + 12.5 48.47 0.62 + 13.5 65.15 0.79 + 14.5 87.89 1.02 + 15.5 113.13 1.28 + 16.5 123.23 1.38 + 17.5 98.99 1.14 + 18.5 70.45 0.84 + 19.5 53.37 0.67 + 20.5 42.66 0.56 + 21.5 39.61 0.53 + 22.5 37.45 0.50 + 23.5 36.91 0.50 + 24.5 36.92 0.50 + 25.5 35.53 0.48 + 26.5 33.82 0.46 + 27.5 33.07 0.46 + 28.5 30.47 0.43 + 29.5 29.13 0.41 + 30.5 27.15 0.39 + 31.5 26.04 0.38 + 32.5 24.53 0.36 + 33.5 0.00 0.00 +ENDDATA 28 +ENDSUBENT 44 +SUBENT E1899003 20050914 20050914 E032 +BIB 4 7 +REACTION (50-SN-116(A,INL)50-SN-116,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-EXC,50-SN-116) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data (Fig.1 (b), p051301-2 in reference) taken + from doctorial thesis of M. Uchida +ENDBIB 7 +COMMON 1 3 +ANG-CM +ADEG + 0.68 +ENDCOMMON 3 +DATA 3 24 +E-EXC DATA-CM DATA-ERR +MEV MB/SR/MEV MB/SR/MEV + 8.5 49.60 0.58 + 9.5 44.97 0.53 + 10.5 52.85 0.61 + 11.5 72.68 0.81 + 12.5 93.48 1.02 + 13.5 112.09 1.21 + 14.5 129.92 1.39 + 15.5 130.86 1.40 + 16.5 106.60 1.15 + 17.5 74.76 0.83 + 18.5 55.92 0.64 + 19.5 45.54 0.53 + 20.5 43.64 0.52 + 21.5 42.41 0.50 + 22.5 42.58 0.50 + 23.5 40.97 0.49 + 24.5 39.04 0.47 + 25.5 37.05 0.45 + 26.5 35.83 0.44 + 27.5 33.24 0.41 + 28.5 30.99 0.39 + 29.5 29.04 0.37 + 30.5 27.07 0.35 + 31.5 27.34 0.35 +ENDDATA 26 +ENDSUBENT 42 +SUBENT E1899004 20050914 20050914 E032 +BIB 4 7 +REACTION (82-PB-208(A,INL)82-PB-208,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-EXC,82-PB-208) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +STATUS (TABLE) Data (Fig.1 (d), p051301-2 in reference) taken + from doctorial thesis of M. Uchida +ENDBIB 7 +COMMON 1 3 +ANG-CM +ADEG + 0.67 +ENDCOMMON 3 +DATA 3 24 +E-EXC DATA-CM DATA-ERR +MEV MB/SR/MEV MB/SR/MEV + 8.5 60.95 1.69 + 9.5 105.41 2.02 + 10.5 138.09 2.29 + 11.5 161.39 2.48 + 12.5 179.75 2.65 + 13.5 208.24 2.91 + 14.5 150.04 2.41 + 15.5 87.45 1.90 + 16.5 66.48 1.74 + 17.5 64.02 1.75 + 18.5 66.71 1.76 + 19.5 64.53 1.77 + 20.5 64.03 1.76 + 21.5 64.62 1.79 + 22.5 54.28 1.73 + 23.5 52.98 1.71 + 24.5 47.72 1.70 + 25.5 41.32 1.68 + 26.5 38.98 1.70 + 27.5 39.03 1.70 + 28.5 36.11 1.70 + 29.5 36.05 1.70 + 30.5 33.19 1.70 + 31.5 35.49 1.73 +ENDDATA 26 +ENDSUBENT 42 +SUBENT E1899005 20050914 20050914 E032 +BIB 5 8 +REACTION (50-SN-116(A,INL)50-SN-116,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,50-SN-116) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA : Distorted wave Born approximation +STATUS (TABLE) Data (Fig. 2(a), p051301-2 in reference) taken + from doctorial thesis of M. Uchida +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 15.5 0.5 +ENDCOMMON 3 +DATA 3 26 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.68 130.86 1.40 + 0.96 111.09 1.20 + 2.11 54.42 0.93 + 2.71 50.91 0.87 + 3.11 51.56 0.85 + 3.31 52.37 0.88 + 3.71 49.70 0.82 + 4.32 36.44 0.64 + 4.63 29.01 0.50 + 5.24 26.38 0.46 + 5.85 26.45 0.46 + 6.15 23.22 0.39 + 6.76 17.32 0.31 + 7.36 11.94 0.23 + 7.66 11.82 0.21 + 8.26 11.60 0.20 + 8.86 10.64 0.19 + 9.15 8.82 0.15 + 9.75 6.61 0.12 + 10.33 5.12 0.10 + 10.63 4.80 0.08 + 11.21 4.54 0.08 + 11.78 3.87 0.07 + 12.07 3.33 0.07 + 12.64 2.52 0.06 + 13.20 2.03 0.05 +ENDDATA 28 +ENDSUBENT 45 +SUBENT E1899006 20050914 20050914 E032 +BIB 5 8 +REACTION (50-SN-116(A,INL)50-SN-116,,DA/DE,A/RSD) +EN-SEC ANG-CM is polar angle between beam and alpha in center + of mass system + (E-LVL,50-SN-116) +ERR-ANALYS (DATA-ERR) No information on source of uncertainties +ADD-RES (COMP) DWBA (Distorted wave Born approximation) +STATUS (TABLE) Data (Fig. 2(b), p051301-2 in reference) taken + from doctorial thesis of M. Uchida +ENDBIB 8 +COMMON 2 3 +E-LVL E-LVL-ERR +MEV MEV + 25.5 0.5 +ENDCOMMON 3 +DATA 3 26 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR/MEV MB/SR/MEV + 0.68 37.05 0.45 + 0.96 35.67 0.44 + 2.11 29.21 0.60 + 2.71 28.39 0.56 + 3.11 25.33 0.48 + 3.31 26.36 0.51 + 3.71 26.46 0.49 + 4.32 24.31 0.46 + 4.63 20.90 0.38 + 5.24 18.98 0.35 + 5.85 16.02 0.31 + 6.15 13.27 0.25 + 6.76 12.55 0.24 + 7.36 10.95 0.21 + 7.66 9.83 0.18 + 8.26 7.94 0.15 + 8.86 6.66 0.13 + 9.15 5.75 0.11 + 9.75 5.17 0.10 + 10.33 4.31 0.09 + 10.63 3.57 0.07 + 11.21 3.10 0.06 + 11.78 2.61 0.05 + 12.07 2.40 0.05 + 12.64 2.14 0.05 + 13.20 1.70 0.04 +ENDDATA 28 +ENDSUBENT 45 +NOSUBENT E1899007 20050914 20050914 E032 +NOSUBENT E1899008 20050914 20050914 E032 +NOSUBENT E1899009 20050914 20050914 E032 +NOSUBENT E1899010 20050914 20050914 E032 +NOSUBENT E1899011 20050914 20050914 E032 +NOSUBENT E1899012 20050914 20050914 E032 +NOSUBENT E1899013 20050914 20050914 E032 +NOSUBENT E1899014 20050914 20050914 E032 +NOSUBENT E1899015 20050914 20050914 E032 +ENDENTRY 15 diff --git a/exforall/E19/E1900.x4 b/exforall/E19/E1900.x4 new file mode 100644 index 000000000..c72473759 --- /dev/null +++ b/exforall/E19/E1900.x4 @@ -0,0 +1,1389 @@ +ENTRY E1900 20050914 20050914 E032 +SUBENT E1900001 20050914 20050914 E032 +BIB 12 37 +TITLE Pionic enhancement in quasielastic (p,n) reactions at + 345 MeV +AUTHOR (T.Wakasa, H.Sakai, M.Ichimura, K.Hatanaka, + M.B.Greenfield, M.Hatano, J.Kamiya, H.Kato, + K.Kawahigashi, Y.Maeda, Y.Nakaoka, H.Okamura, + T.Ohnishi, H.Otsu, K.Sekiguchi, K.Suda, A.Tamii, + T.Uesaka, T.Yagita, K.Yako) +INSTITUTE (2JPNKYU) Department of Physics + (2JPNTOK) Department of Physics + (2JPNIPC) + (2JPNHOS) Faculty of Computer and Information Sciences + (2JPNOSA) Research Center for Nuclear Physics + (2JPNICU) Division of Natural Science + (2JPNJAE) Accelerator Group + (2JPNJPN) Department of Information Sciences, Kanagawa + University, Hiratsuka, Kanagawa + (2JPNTOH) Cyclotron and Radioisotope Center + (2JPNTOH) Department of Physics + (2JPNSUU) Department of Physics + (2JPNTOK) Center for Nuclear Study +REFERENCE (J,PR/C,69,(5),054609,200405) +PART-DET (N) +SAMPLE - Target is natural. + - Chemical-form of target is element. + - Physical-form of target is solid. +METHOD (TOF) Neutron Time-Of-Flight (NTOF) facility [H. Sakai + et al., Nucl. Instrum. Methods Phys. Res. A 369, + 120 (1996)] +FACILITY (CYCLO,2JPNOSA) Research Center for Nuclear Physics +DETECTOR Calibration: CD2 target was used for calibration of + effective analyzing powers of the neutron + detector/polarimeter NPOL2 [H.Sakai, et al., Nucl. + Instrum. Methods Phys. Res. A 369(1996)120] +ADD-RES (COMP) DWIA (Distorted wave impulse approximation) +COMMENT 7Li target was used for normalization of the cross + sections. +HISTORY (20050414C) Kc + On +ENDBIB 37 +COMMON 2 3 +EN POL-BM +MEV NO-DIM + 345.0 0.7 +ENDCOMMON 3 +ENDSUBENT 44 +SUBENT E1900002 20050914 20050914 E032 +BIB 6 14 +REACTION (6-C-12(P,N)7-N-12,,DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 10 nA. +SAMPLE Target-thickness is 172 mg/cm**2. +ERR-ANALYS (ERR-T) Total uncertainty + (ERR-1) Uncertainties of the determination of the + integrated beam current + (ERR-2) Uncertainties of the 7Li cross section + (ERR-3) Uncertainties of the thickness of the 12C + target +STATUS (UNOBT) Data (Fig.1, p054609 in reference) + unobtainable +ENDBIB 14 +COMMON 4 3 +ANG ERR-1 ERR-2 ERR-3 +ADEG PER-CENT PER-CENT PER-CENT + 16.0 2.0 3.0 3.0 +ENDCOMMON 3 +NODATA 0 0 +ENDSUBENT 22 +SUBENT E1900003 20050914 20050914 E032 +BIB 6 14 +REACTION (6-C-12(P,N)7-N-12,,DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 10 nA. +SAMPLE Target-thickness is 172 mg/cm**2. +ERR-ANALYS (ERR-T) Total uncertainty + (ERR-1) Uncertainties of the determination of the + integrated beam current + (ERR-2) Uncertainties of the 7Li cross section + (ERR-3) Uncertainties of the thickness of the 12C + target +STATUS (UNOBT) Data (Fig.1, p054609 in reference) + unobtainable +ENDBIB 14 +COMMON 4 3 +ANG ERR-1 ERR-2 ERR-3 +ADEG PER-CENT PER-CENT PER-CENT + 22.0 2.0 3.0 3.0 +ENDCOMMON 3 +NODATA 0 0 +ENDSUBENT 22 +SUBENT E1900004 20050914 20050914 E032 +BIB 6 14 +REACTION (6-C-12(P,N)7-N-12,,DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 10 nA. +SAMPLE Target-thickness is 172 mg/cm**2. +ERR-ANALYS (ERR-T) Total uncertainty + (ERR-1) Uncertainties of the determination of the + integrated beam current + (ERR-2) Uncertainties of the 7Li cross section + (ERR-3) Uncertainties of the thickness of the 12C + target +STATUS (UNOBT) Data (Fig.1, p054609 in reference) + unobtainable +ENDBIB 14 +COMMON 4 3 +ANG ERR-1 ERR-2 ERR-3 +ADEG PER-CENT PER-CENT PER-CENT + 27.0 2.0 3.0 3.0 +ENDCOMMON 3 +NODATA 0 0 +ENDSUBENT 22 +SUBENT E1900005 20050914 20050914 E032 +BIB 5 9 +REACTION (6-C-12(P,N)7-N-12,,POL/DA/DE,,ANA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +SAMPLE Target-thickness is 172 mg/cm**2. +ADD-RES (COMP) Random phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.2, p054609-3 in + reference +ENDBIB 9 +COMMON 1 3 +ANG +ADEG + 16.0 +ENDCOMMON 3 +DATA 2 36 +E-DGD DATA +MEV NO-DIM + 1.990E+01 1.267E-01 + 2.533E+01 1.427E-01 + 3.011E+01 1.053E-01 + 3.522E+01 1.107E-01 + 4.002E+01 1.200E-01 + 4.513E+01 1.267E-01 + 4.993E+01 1.347E-01 + 5.568E+01 1.347E-01 + 5.984E+01 1.413E-01 + 6.559E+01 1.427E-01 + 7.006E+01 1.467E-01 + 7.517E+01 1.480E-01 + 8.029E+01 1.467E-01 + 8.508E+01 1.413E-01 + 9.019E+01 1.400E-01 + 9.530E+01 1.347E-01 + 1.001E+02 1.267E-01 + 1.052E+02 1.187E-01 + 1.100E+02 1.067E-01 + 1.151E+02 1.027E-01 + 1.202E+02 8.933E-02 + 1.250E+02 7.867E-02 + 1.301E+02 7.333E-02 + 1.349E+02 5.600E-02 + 1.403E+02 4.400E-02 + 1.451E+02 4.267E-02 + 1.502E+02 2.933E-02 + 1.553E+02 1.333E-02 + 1.601E+02 5.333E-03 + 1.649E+02 -5.333E-03 + 1.703E+02 -1.067E-02 + 1.751E+02 -2.400E-02 + 1.802E+02 -2.667E-02 + 1.853E+02 -3.200E-02 + 1.904E+02 -3.333E-02 + 1.952E+02 -3.600E-02 +ENDDATA 38 +ENDSUBENT 56 +SUBENT E1900006 20050914 20050914 E032 +BIB 5 9 +REACTION (6-C-12(P,N)7-N-12,,POL/DA/DE,,ANA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +SAMPLE Target-thickness is 172 mg/cm**2. +ADD-RES (COMP) Random phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.2, p054609-3 in + reference +ENDBIB 9 +COMMON 1 3 +ANG +ADEG + 22.0 +ENDCOMMON 3 +DATA 2 35 +E-DGD DATA +MEV NO-DIM + 2.524E+01 2.338E-01 + 3.003E+01 2.203E-01 + 3.514E+01 2.122E-01 + 4.026E+01 1.959E-01 + 4.505E+01 1.851E-01 + 4.984E+01 1.703E-01 + 5.527E+01 1.689E-01 + 5.974E+01 1.635E-01 + 6.518E+01 1.622E-01 + 6.997E+01 1.635E-01 + 7.508E+01 1.622E-01 + 7.987E+01 1.608E-01 + 8.498E+01 1.662E-01 + 9.010E+01 1.649E-01 + 9.489E+01 1.676E-01 + 9.968E+01 1.635E-01 + 1.051E+02 1.662E-01 + 1.102E+02 1.581E-01 + 1.150E+02 1.541E-01 + 1.198E+02 1.541E-01 + 1.252E+02 1.473E-01 + 1.300E+02 1.378E-01 + 1.348E+02 1.284E-01 + 1.399E+02 1.216E-01 + 1.450E+02 1.095E-01 + 1.505E+02 1.027E-01 + 1.553E+02 9.459E-02 + 1.601E+02 8.243E-02 + 1.652E+02 7.297E-02 + 1.703E+02 6.351E-02 + 1.754E+02 5.135E-02 + 1.799E+02 3.784E-02 + 1.856E+02 2.838E-02 + 1.898E+02 2.703E-02 + 1.952E+02 2.027E-02 +ENDDATA 37 +ENDSUBENT 55 +SUBENT E1900007 20050914 20050914 E032 +BIB 5 9 +REACTION (6-C-12(P,N)7-N-12,,POL/DA/DE,,ANA) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +SAMPLE Target-thickness is 172 mg/cm**2. +ADD-RES (COMP) Random phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.2, p054609-3 in + reference +ENDBIB 9 +COMMON 1 3 +ANG +ADEG + 27.0 +ENDCOMMON 3 +DATA 2 35 +E-DGD DATA +MEV NO-DIM + 2.524E+01 2.038E-01 + 3.003E+01 2.387E-01 + 3.514E+01 2.226E-01 + 4.026E+01 2.293E-01 + 4.537E+01 2.253E-01 + 4.984E+01 2.199E-01 + 5.527E+01 2.078E-01 + 5.974E+01 2.065E-01 + 6.550E+01 2.024E-01 + 7.029E+01 1.970E-01 + 7.540E+01 1.930E-01 + 8.019E+01 1.917E-01 + 8.530E+01 1.876E-01 + 9.010E+01 1.876E-01 + 9.489E+01 1.849E-01 + 9.968E+01 1.836E-01 + 1.051E+02 1.796E-01 + 1.099E+02 1.782E-01 + 1.150E+02 1.755E-01 + 1.201E+02 1.742E-01 + 1.249E+02 1.742E-01 + 1.300E+02 1.648E-01 + 1.351E+02 1.581E-01 + 1.403E+02 1.540E-01 + 1.454E+02 1.460E-01 + 1.498E+02 1.406E-01 + 1.553E+02 1.325E-01 + 1.601E+02 1.258E-01 + 1.649E+02 1.151E-01 + 1.700E+02 1.043E-01 + 1.751E+02 9.624E-02 + 1.802E+02 8.414E-02 + 1.853E+02 7.608E-02 + 1.904E+02 6.667E-02 + 1.949E+02 5.726E-02 +ENDDATA 37 +ENDSUBENT 55 +SUBENT E1900008 20050914 20050914 E032 +BIB 6 10 +REACTION (6-C-12(P,N)7-N-12,,POL/DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.2, p054609-3 in + reference +ENDBIB 10 +COMMON 1 3 +ANG +ADEG + 16.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 1.997E+01 2.389E-01 2.404E-02 + 2.486E+01 2.029E-01 1.683E-02 + 3.003E+01 1.837E-01 1.803E-02 + 3.521E+01 1.548E-01 1.683E-02 + 3.980E+01 1.560E-01 1.202E-02 + 4.524E+01 1.692E-01 1.082E-02 + 4.984E+01 1.716E-01 1.202E-02 + 5.528E+01 1.861E-01 1.202E-02 + 5.987E+01 2.017E-01 1.202E-02 + 6.503E+01 2.005E-01 1.322E-02 + 7.021E+01 1.740E-01 1.562E-02 + 7.479E+01 2.017E-01 1.562E-02 + 8.024E+01 2.041E-01 1.562E-02 + 8.511E+01 2.317E-01 1.562E-02 + 8.999E+01 2.221E-01 1.683E-02 + 9.515E+01 2.353E-01 1.803E-02 + 9.975E+01 1.981E-01 1.923E-02 + 1.049E+02 2.089E-01 1.683E-02 + 1.101E+02 1.945E-01 1.683E-02 + 1.150E+02 2.293E-01 1.803E-02 + 1.201E+02 2.305E-01 2.043E-02 + 1.250E+02 2.101E-01 2.404E-02 + 1.302E+02 2.353E-01 2.163E-02 + 1.350E+02 2.389E-01 2.404E-02 + 1.402E+02 1.680E-01 2.524E-02 + 1.451E+02 2.269E-01 2.404E-02 + 1.500E+02 1.680E-01 2.524E-02 + 1.554E+02 2.221E-01 2.524E-02 + 1.606E+02 2.209E-01 2.644E-02 + 1.646E+02 1.584E-01 2.764E-02 + 1.701E+02 1.572E-01 2.885E-02 + 1.749E+02 1.945E-01 2.885E-02 + 1.801E+02 1.764E-01 3.125E-02 + 1.850E+02 1.788E-01 3.245E-02 + 1.904E+02 2.101E-01 3.365E-02 + 1.956E+02 2.233E-01 3.606E-02 +ENDDATA 38 +ENDSUBENT 57 +SUBENT E1900009 20050914 20050914 E032 +BIB 6 10 +REACTION (6-C-12(P,N)7-N-12,,POL/DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.2, p054609-3 in + reference +ENDBIB 10 +COMMON 1 3 +ANG +ADEG + 22.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.493E+01 2.499E-01 1.453E-02 + 3.009E+01 2.547E-01 1.816E-02 + 3.524E+01 2.487E-01 1.574E-02 + 4.011E+01 2.499E-01 1.453E-02 + 4.527E+01 2.281E-01 1.453E-02 + 4.986E+01 2.148E-01 1.211E-02 + 5.530E+01 2.148E-01 1.211E-02 + 5.989E+01 2.220E-01 1.090E-02 + 6.504E+01 2.039E-01 1.090E-02 + 6.991E+01 2.087E-01 1.211E-02 + 7.479E+01 2.184E-01 1.211E-02 + 7.994E+01 2.184E-01 1.211E-02 + 8.539E+01 2.208E-01 9.685E-03 + 8.997E+01 2.172E-01 9.685E-03 + 9.513E+01 2.184E-01 1.211E-02 + 1.000E+02 2.208E-01 9.685E-03 + 1.052E+02 2.220E-01 1.090E-02 + 1.100E+02 2.378E-01 1.090E-02 + 1.149E+02 2.196E-01 1.090E-02 + 1.203E+02 2.329E-01 1.332E-02 + 1.249E+02 2.341E-01 1.453E-02 + 1.301E+02 2.547E-01 1.211E-02 + 1.350E+02 2.172E-01 1.332E-02 + 1.398E+02 2.051E-01 1.574E-02 + 1.450E+02 2.390E-01 1.332E-02 + 1.501E+02 2.172E-01 1.574E-02 + 1.550E+02 2.208E-01 1.574E-02 + 1.602E+02 2.414E-01 1.695E-02 + 1.648E+02 2.208E-01 1.574E-02 + 1.699E+02 2.281E-01 1.816E-02 + 1.748E+02 2.172E-01 1.937E-02 + 1.799E+02 1.966E-01 1.816E-02 + 1.851E+02 2.039E-01 1.695E-02 + 1.903E+02 1.881E-01 1.937E-02 + 1.951E+02 2.317E-01 2.058E-02 + 2.000E+02 1.930E-01 +ENDDATA 38 +ENDSUBENT 57 +SUBENT E1900010 20050914 20050914 E032 +BIB 6 10 +REACTION (6-C-12(P,N)7-N-12,,POL/DA/DE) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.2, p054609-3 in + reference +ENDBIB 10 +COMMON 1 3 +ANG +ADEG + 27.0 +ENDCOMMON 3 +DATA 3 35 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.538E+01 3.083E-01 2.752E-02 + 3.029E+01 2.945E-01 2.064E-02 + 3.520E+01 3.083E-01 2.179E-02 + 4.038E+01 2.773E-01 1.950E-02 + 4.529E+01 3.025E-01 1.491E-02 + 5.020E+01 2.979E-01 1.376E-02 + 5.539E+01 2.796E-01 1.720E-02 + 6.030E+01 2.647E-01 1.376E-02 + 6.548E+01 2.658E-01 1.261E-02 + 6.985E+01 2.589E-01 1.261E-02 + 7.503E+01 2.658E-01 9.174E-03 + 8.022E+01 2.624E-01 9.174E-03 + 8.513E+01 2.360E-01 1.491E-02 + 9.004E+01 2.463E-01 1.376E-02 + 9.523E+01 2.532E-01 1.261E-02 + 1.001E+02 2.440E-01 1.261E-02 + 1.050E+02 2.440E-01 1.261E-02 + 1.102E+02 2.394E-01 1.147E-02 + 1.154E+02 2.417E-01 1.147E-02 + 1.203E+02 2.612E-01 1.032E-02 + 1.250E+02 2.463E-01 1.376E-02 + 1.302E+02 2.716E-01 1.606E-02 + 1.353E+02 2.681E-01 1.261E-02 + 1.400E+02 2.567E-01 1.261E-02 + 1.449E+02 2.475E-01 1.491E-02 + 1.503E+02 2.544E-01 1.491E-02 + 1.553E+02 2.555E-01 1.376E-02 + 1.604E+02 2.739E-01 1.606E-02 + 1.648E+02 2.532E-01 1.606E-02 + 1.703E+02 2.578E-01 1.720E-02 + 1.752E+02 2.704E-01 1.720E-02 + 1.801E+02 2.406E-01 1.950E-02 + 1.850E+02 2.498E-01 1.950E-02 + 1.905E+02 2.028E-01 1.950E-02 + 1.954E+02 2.016E-01 2.408E-02 +ENDDATA 37 +ENDSUBENT 56 +SUBENT E1900011 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,SS,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 16.0 +ENDCOMMON 3 +DATA 3 37 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 1.605E+01 -2.898E-01 1.878E-01 + 2.069E+01 -7.020E-01 3.061E-02 + 2.595E+01 -6.367E-01 2.449E-02 + 3.040E+01 -5.918E-01 2.653E-02 + 3.530E+01 -6.327E-01 2.653E-02 + 4.058E+01 -6.204E-01 2.449E-02 + 4.546E+01 -6.265E-01 2.041E-02 + 4.993E+01 -6.327E-01 2.041E-02 + 5.522E+01 -6.429E-01 2.041E-02 + 6.010E+01 -6.408E-01 1.633E-02 + 6.539E+01 -6.633E-01 1.837E-02 + 7.066E+01 -6.245E-01 1.837E-02 + 7.513E+01 -6.082E-01 1.837E-02 + 7.999E+01 -5.816E-01 1.633E-02 + 8.529E+01 -6.122E-01 2.449E-02 + 8.973E+01 -5.306E-01 2.653E-02 + 9.500E+01 -4.878E-01 3.469E-02 + 9.989E+01 -5.286E-01 3.061E-02 + 1.051E+02 -4.408E-01 3.061E-02 + 1.104E+02 -4.510E-01 2.653E-02 + 1.149E+02 -3.633E-01 3.061E-02 + 1.198E+02 -4.184E-01 3.469E-02 + 1.250E+02 -3.939E-01 3.469E-02 + 1.295E+02 -2.694E-01 3.673E-02 + 1.351E+02 -2.551E-01 3.469E-02 + 1.392E+02 -2.265E-01 3.265E-02 + 1.449E+02 -2.102E-01 4.082E-02 + 1.498E+02 -2.184E-01 3.673E-02 + 1.546E+02 -2.041E-01 5.102E-02 + 1.595E+02 -2.122E-01 4.286E-02 + 1.644E+02 -2.204E-01 4.490E-02 + 1.696E+02 -8.980E-02 5.102E-02 + 1.745E+02 -1.122E-01 5.102E-02 + 1.794E+02 -1.857E-01 5.714E-02 + 1.838E+02 -6.122E-03 5.510E-02 + 1.896E+02 -1.327E-01 6.122E-02 + 1.940E+02 -1.571E-01 5.714E-02 +ENDDATA 39 +ENDSUBENT 60 +SUBENT E1900012 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,NN,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 16.0 +ENDCOMMON 3 +DATA 3 37 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 1.617E+01 -2.550E-01 1.755E-01 + 2.105E+01 1.883E-01 3.774E-02 + 2.556E+01 1.392E-01 2.454E-02 + 3.045E+01 1.277E-01 3.019E-02 + 3.571E+01 1.729E-01 2.076E-02 + 4.135E+01 1.464E-01 2.265E-02 + 4.586E+01 1.746E-01 1.887E-02 + 5.038E+01 1.575E-01 1.887E-02 + 5.526E+01 1.707E-01 1.698E-02 + 6.015E+01 1.498E-01 1.509E-02 + 6.579E+01 1.497E-01 1.700E-02 + 7.068E+01 1.175E-01 1.887E-02 + 7.519E+01 1.193E-01 2.076E-02 + 8.045E+01 1.475E-01 2.076E-02 + 8.534E+01 1.210E-01 2.454E-02 + 9.060E+01 1.021E-01 2.266E-02 + 9.586E+01 1.190E-01 2.642E-02 + 1.004E+02 9.000E-02 2.454E-02 + 1.053E+02 6.594E-02 2.265E-02 + 1.109E+02 1.224E-01 2.830E-02 + 1.154E+02 8.462E-02 2.642E-02 + 1.207E+02 4.301E-02 3.020E-02 + 1.252E+02 1.840E-02 2.454E-02 + 1.301E+02 6.736E-02 3.208E-02 + 1.357E+02 6.348E-02 3.020E-02 + 1.398E+02 3.026E-03 2.831E-02 + 1.455E+02 2.367E-02 3.208E-02 + 1.500E+02 -3.301E-02 3.774E-02 + 1.549E+02 -4.443E-02 3.208E-02 + 1.602E+02 -4.453E-02 3.774E-02 + 1.650E+02 -3.111E-03 3.963E-02 + 1.703E+02 5.339E-02 3.963E-02 + 1.752E+02 -1.651E-02 4.152E-02 + 1.797E+02 -4.867E-02 4.151E-02 + 1.850E+02 -7.519E-02 4.340E-02 + 1.898E+02 -7.717E-02 4.529E-02 + 1.951E+02 -7.160E-02 5.095E-02 +ENDDATA 39 +ENDSUBENT 60 +SUBENT E1900013 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,LL,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 16.0 +ENDCOMMON 3 +DATA 3 37 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 1.603E+01 -4.274E-01 1.697E-01 + 2.098E+01 -3.491E-01 3.426E-02 + 2.481E+01 -4.731E-01 3.426E-02 + 3.102E+01 -4.617E-01 2.447E-02 + 3.560E+01 -4.388E-01 2.610E-02 + 4.147E+01 -4.437E-01 1.958E-02 + 4.607E+01 -3.948E-01 1.794E-02 + 5.064E+01 -3.915E-01 1.958E-02 + 5.652E+01 -3.817E-01 1.958E-02 + 6.044E+01 -3.785E-01 2.284E-02 + 6.565E+01 -3.899E-01 1.958E-02 + 7.120E+01 -3.785E-01 1.958E-02 + 7.513E+01 -3.687E-01 1.958E-02 + 8.100E+01 -3.589E-01 2.121E-02 + 8.556E+01 -3.768E-01 2.284E-02 + 9.014E+01 -3.638E-01 2.773E-02 + 9.602E+01 -3.540E-01 2.773E-02 + 9.992E+01 -3.752E-01 2.284E-02 + 1.058E+02 -3.442E-01 2.773E-02 + 1.110E+02 -4.111E-01 2.773E-02 + 1.150E+02 -3.361E-01 3.100E-02 + 1.208E+02 -3.736E-01 3.100E-02 + 1.250E+02 -3.654E-01 3.263E-02 + 1.303E+02 -3.768E-01 3.263E-02 + 1.358E+02 -3.719E-01 3.426E-02 + 1.401E+02 -2.985E-01 3.426E-02 + 1.456E+02 -3.083E-01 3.915E-02 + 1.502E+02 -3.475E-01 4.078E-02 + 1.551E+02 -3.475E-01 4.241E-02 + 1.600E+02 -3.018E-01 4.405E-02 + 1.652E+02 -4.013E-01 4.568E-02 + 1.704E+02 -2.855E-01 4.731E-02 + 1.750E+02 -3.393E-01 5.220E-02 + 1.802E+02 -3.246E-01 5.057E-02 + 1.851E+02 -3.393E-01 5.383E-02 + 1.896E+02 -3.997E-01 5.710E-02 + 1.949E+02 -3.638E-01 5.546E-02 +ENDDATA 39 +ENDSUBENT 60 +SUBENT E1900014 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,SL,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 16.0 +ENDCOMMON 3 +DATA 3 37 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 1.609E+01 1.074E-01 1.782E-01 + 2.036E+01 6.768E-03 3.300E-02 + 2.594E+01 5.302E-02 2.145E-02 + 3.087E+01 3.491E-02 2.640E-02 + 3.547E+01 4.485E-02 1.980E-02 + 4.072E+01 5.479E-02 2.310E-02 + 4.598E+01 7.134E-02 2.310E-02 + 4.992E+01 7.632E-02 2.145E-02 + 5.550E+01 8.132E-02 2.145E-02 + 6.076E+01 7.146E-02 1.815E-02 + 6.502E+01 1.375E-01 1.815E-02 + 7.061E+01 1.045E-01 1.815E-02 + 7.488E+01 1.244E-01 2.145E-02 + 8.013E+01 1.343E-01 2.145E-02 + 8.539E+01 1.657E-01 1.980E-02 + 8.998E+01 1.427E-01 2.475E-02 + 9.557E+01 1.526E-01 2.805E-02 + 9.984E+01 1.312E-01 2.640E-02 + 1.048E+02 1.543E-01 2.310E-02 + 1.103E+02 1.478E-01 2.805E-02 + 1.149E+02 1.577E-01 2.805E-02 + 1.202E+02 1.693E-01 3.300E-02 + 1.248E+02 1.793E-01 3.135E-02 + 1.300E+02 1.644E-01 3.135E-02 + 1.356E+02 1.909E-01 3.300E-02 + 1.396E+02 9.852E-02 3.630E-02 + 1.452E+02 1.266E-01 3.960E-02 + 1.498E+02 1.597E-01 3.795E-02 + 1.547E+02 -3.690E-04 4.125E-02 + 1.596E+02 -1.023E-02 4.785E-02 + 1.645E+02 1.020E-01 4.455E-02 + 1.698E+02 3.936E-02 4.785E-02 + 1.747E+02 -2.661E-02 4.950E-02 + 1.796E+02 4.439E-02 5.446E-02 + 1.846E+02 -2.817E-02 6.105E-02 + 1.898E+02 3.623E-02 5.940E-02 + 1.951E+02 -6.635E-03 6.270E-02 +ENDDATA 39 +ENDSUBENT 60 +SUBENT E1900015 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,LS,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 16.0 +ENDCOMMON 3 +DATA 3 39 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 1.650E+01 2.248E-01 1.712E-01 + 2.071E+01 3.533E-02 3.825E-02 + 2.177E+01 -1.568E-02 2.004E-02 + 2.613E+01 2.495E-03 1.640E-02 + 3.048E+01 -1.758E-02 2.186E-02 + 3.558E+01 9.695E-03 2.004E-02 + 4.067E+01 2.604E-02 2.186E-02 + 4.539E+01 2.418E-02 1.822E-02 + 5.047E+01 2.231E-02 2.004E-02 + 5.559E+01 7.509E-02 1.821E-02 + 6.067E+01 7.686E-02 2.186E-02 + 6.079E+01 2.390E-01 + 6.614E+01 1.114E-01 1.822E-02 + 7.087E+01 1.205E-01 2.004E-02 + 7.523E+01 1.387E-01 1.822E-02 + 8.070E+01 1.659E-01 2.186E-02 + 8.618E+01 2.151E-01 2.550E-02 + 9.086E+01 1.677E-01 2.368E-02 + 9.594E+01 1.621E-01 2.733E-02 + 1.007E+02 2.113E-01 2.733E-02 + 1.058E+02 1.839E-01 2.915E-02 + 1.109E+02 2.367E-01 2.733E-02 + 1.156E+02 2.111E-01 3.461E-02 + 1.206E+02 1.838E-01 3.461E-02 + 1.254E+02 2.311E-01 3.097E-02 + 1.305E+02 2.055E-01 3.461E-02 + 1.359E+02 2.091E-01 3.644E-02 + 1.406E+02 2.273E-01 3.644E-02 + 1.457E+02 1.763E-01 3.643E-02 + 1.508E+02 1.817E-01 4.008E-02 + 1.555E+02 1.780E-01 4.008E-02 + 1.609E+02 1.342E-01 4.372E-02 + 1.649E+02 1.269E-01 4.554E-02 + 1.703E+02 1.232E-01 4.919E-02 + 1.754E+02 1.578E-01 4.918E-02 + 1.805E+02 1.304E-01 5.283E-02 + 1.859E+02 1.067E-01 5.101E-02 + 1.905E+02 -4.455E-02 5.101E-02 + 1.953E+02 6.413E-03 6.557E-02 +ENDDATA 41 +ENDSUBENT 62 +SUBENT E1900016 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,SS,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 22.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.536E+01 -3.582E-01 3.253E-02 + 3.027E+01 -3.848E-01 3.659E-02 + 3.517E+01 -3.605E-01 3.456E-02 + 4.049E+01 -3.423E-01 3.253E-02 + 4.499E+01 -3.302E-01 3.050E-02 + 4.990E+01 -3.547E-01 2.845E-02 + 5.521E+01 -3.426E-01 2.643E-02 + 5.930E+01 -2.000E-01 3.050E-02 + 6.503E+01 -3.021E-01 2.644E-02 + 6.994E+01 -3.571E-01 2.237E-02 + 7.566E+01 -3.572E-01 2.237E-02 + 8.016E+01 -3.919E-01 2.846E-02 + 8.466E+01 -4.184E-01 2.440E-02 + 8.998E+01 -4.043E-01 2.440E-02 + 9.530E+01 -3.535E-01 2.440E-02 + 9.980E+01 -4.105E-01 3.050E-02 + 1.051E+02 -3.761E-01 2.846E-02 + 1.096E+02 -4.229E-01 2.644E-02 + 1.149E+02 -3.743E-01 3.050E-02 + 1.202E+02 -4.577E-01 3.253E-02 + 1.247E+02 -3.358E-01 3.456E-02 + 1.301E+02 -4.294E-01 3.456E-02 + 1.350E+02 -3.401E-01 3.863E-02 + 1.395E+02 -4.093E-01 3.456E-02 + 1.452E+02 -3.566E-01 3.658E-02 + 1.497E+02 -3.424E-01 4.066E-02 + 1.550E+02 -2.836E-01 4.471E-02 + 1.599E+02 -2.837E-01 4.473E-02 + 1.648E+02 -3.997E-01 5.081E-02 + 1.701E+02 -2.697E-01 4.676E-02 + 1.751E+02 -2.210E-01 5.286E-02 + 1.800E+02 -1.906E-01 5.895E-02 + 1.849E+02 -2.863E-01 5.693E-02 + 1.898E+02 -2.071E-01 6.098E-02 + 1.951E+02 -2.905E-01 6.099E-02 + 2.000E+02 -2.114E-01 +ENDDATA 38 +ENDSUBENT 59 +SUBENT E1900017 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,NN,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 22.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.538E+01 6.728E-02 2.377E-02 + 3.046E+01 7.072E-02 2.886E-02 + 3.519E+01 7.246E-02 2.886E-02 + 4.061E+01 4.704E-02 2.207E-02 + 4.501E+01 3.010E-02 2.037E-02 + 5.076E+01 1.996E-02 1.867E-02 + 5.550E+01 4.886E-02 2.037E-02 + 5.956E+01 2.513E-02 1.698E-02 + 6.497E+01 4.555E-02 1.867E-02 + 6.971E+01 3.710E-02 1.528E-02 + 7.513E+01 5.922E-02 1.528E-02 + 7.986E+01 5.416E-02 1.528E-02 + 8.426E+01 6.778E-02 1.868E-02 + 9.002E+01 5.934E-02 1.867E-02 + 9.509E+01 7.806E-02 1.867E-02 + 9.949E+01 6.282E-02 1.697E-02 + 1.049E+02 5.268E-02 1.697E-02 + 1.096E+02 5.442E-02 2.037E-02 + 1.147E+02 6.974E-02 2.207E-02 + 1.201E+02 5.281E-02 2.207E-02 + 1.249E+02 6.473E-02 2.207E-02 + 1.299E+02 9.024E-02 2.207E-02 + 1.347E+02 5.293E-02 2.207E-02 + 1.398E+02 4.109E-02 1.867E-02 + 1.452E+02 3.944E-02 2.037E-02 + 1.496E+02 7.683E-02 2.546E-02 + 1.550E+02 7.264E-03 2.207E-02 + 1.597E+02 3.107E-02 2.207E-02 + 1.645E+02 -1.812E-02 2.546E-02 + 1.702E+02 2.098E-02 2.546E-02 + 1.746E+02 3.629E-02 2.886E-02 + 1.797E+02 2.106E-02 3.056E-02 + 1.848E+02 4.122E-03 3.056E-02 + 1.895E+02 -2.810E-02 3.395E-02 + 1.949E+02 -1.277E-02 3.226E-02 + 1.997E+02 -2.631E-02 1.528E-02 +ENDDATA 38 +ENDSUBENT 59 +SUBENT E1900018 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,LL,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 22.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.553E+01 -5.603E-01 2.287E-02 + 3.114E+01 -5.161E-01 3.104E-02 + 3.541E+01 -5.013E-01 2.451E-02 + 4.060E+01 -5.781E-01 2.124E-02 + 4.553E+01 -5.601E-01 2.124E-02 + 5.076E+01 -5.862E-01 2.124E-02 + 5.538E+01 -5.420E-01 1.961E-02 + 5.994E+01 -5.959E-01 1.961E-02 + 6.555E+01 -5.354E-01 1.961E-02 + 7.047E+01 -5.354E-01 1.961E-02 + 7.572E+01 -5.304E-01 1.797E-02 + 8.032E+01 -5.190E-01 1.307E-02 + 8.526E+01 -4.846E-01 1.960E-02 + 9.016E+01 -5.025E-01 1.961E-02 + 9.577E+01 -4.567E-01 1.961E-02 + 1.000E+02 -4.534E-01 1.961E-02 + 1.053E+02 -4.125E-01 2.124E-02 + 1.099E+02 -4.550E-01 2.124E-02 + 1.155E+02 -4.370E-01 2.287E-02 + 1.207E+02 -4.549E-01 2.287E-02 + 1.256E+02 -4.058E-01 2.287E-02 + 1.305E+02 -4.189E-01 2.777E-02 + 1.351E+02 -4.025E-01 2.451E-02 + 1.407E+02 -3.779E-01 2.451E-02 + 1.457E+02 -3.665E-01 2.614E-02 + 1.502E+02 -3.730E-01 2.778E-02 + 1.555E+02 -3.844E-01 3.268E-02 + 1.604E+02 -3.533E-01 3.431E-02 + 1.653E+02 -3.679E-01 3.267E-02 + 1.706E+02 -3.074E-01 3.431E-02 + 1.756E+02 -2.813E-01 3.431E-02 + 1.805E+02 -3.008E-01 3.268E-02 + 1.857E+02 -2.795E-01 3.921E-02 + 1.903E+02 -3.203E-01 3.758E-02 + 1.959E+02 -2.582E-01 4.084E-02 + 2.008E+02 -2.435E-01 1.471E-02 +ENDDATA 38 +ENDSUBENT 59 +SUBENT E1900019 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,SL,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 22.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.526E+01 -9.360E-02 2.480E-02 + 3.088E+01 -8.703E-02 2.645E-02 + 3.550E+01 -1.152E-01 2.645E-02 + 4.048E+01 -5.901E-02 2.810E-02 + 4.509E+01 -1.119E-01 2.480E-02 + 5.005E+01 -8.719E-02 2.314E-02 + 5.535E+01 -5.914E-02 2.314E-02 + 5.963E+01 -1.055E-01 1.984E-02 + 6.492E+01 -1.038E-01 2.314E-02 + 7.022E+01 -8.736E-02 2.149E-02 + 7.550E+01 -1.056E-01 1.984E-02 + 8.046E+01 -9.901E-02 2.480E-02 + 8.477E+01 -8.252E-02 1.819E-02 + 8.971E+01 -1.189E-01 1.983E-02 + 9.501E+01 -1.090E-01 2.314E-02 + 9.963E+01 -1.074E-01 1.984E-02 + 1.053E+02 -1.009E-01 1.984E-02 + 1.099E+02 -9.264E-02 2.315E-02 + 1.152E+02 -1.257E-01 2.645E-02 + 1.201E+02 -7.289E-02 2.480E-02 + 1.251E+02 -1.374E-01 2.480E-02 + 1.301E+02 -7.959E-02 2.480E-02 + 1.350E+02 -6.145E-02 2.645E-02 + 1.403E+02 -7.141E-02 2.645E-02 + 1.449E+02 -4.004E-02 2.645E-02 + 1.496E+02 -9.958E-02 2.975E-02 + 1.552E+02 -1.112E-01 2.975E-02 + 1.598E+02 -1.013E-01 3.471E-02 + 1.648E+02 -1.047E-01 3.637E-02 + 1.707E+02 -9.976E-02 3.968E-02 + 1.750E+02 -2.089E-01 3.471E-02 + 1.803E+02 -1.907E-01 3.637E-02 + 1.846E+02 -1.561E-01 3.967E-02 + 1.902E+02 -1.578E-01 4.463E-02 + 1.948E+02 -1.876E-01 4.298E-02 + 1.998E+02 -2.157E-01 1.488E-02 +ENDDATA 38 +ENDSUBENT 59 +SUBENT E1900020 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,LS,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 22.0 +ENDCOMMON 3 +DATA 3 35 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.587E+01 1.648E-02 3.297E-02 + 3.097E+01 5.678E-02 4.212E-02 + 3.534E+01 -5.495E-03 3.663E-02 + 4.080E+01 -7.326E-03 3.480E-02 + 4.517E+01 -2.015E-02 3.114E-02 + 5.027E+01 -7.143E-02 2.564E-02 + 5.537E+01 -9.158E-03 2.381E-02 + 6.011E+01 -5.861E-02 2.747E-02 + 6.557E+01 -2.747E-02 2.564E-02 + 6.995E+01 1.465E-02 2.930E-02 + 7.577E+01 1.832E-02 3.114E-02 + 8.087E+01 -2.564E-02 2.564E-02 + 8.488E+01 1.832E-03 2.381E-02 + 8.998E+01 5.495E-03 2.747E-02 + 9.545E+01 1.832E-03 2.564E-02 + 1.005E+02 -1.465E-02 2.564E-02 + 1.053E+02 5.311E-02 3.297E-02 + 1.097E+02 5.495E-03 2.747E-02 + 1.155E+02 4.212E-02 2.747E-02 + 1.206E+02 2.564E-02 2.930E-02 + 1.260E+02 3.663E-02 3.297E-02 + 1.301E+02 5.128E-02 3.663E-02 + 1.352E+02 7.509E-02 3.663E-02 + 1.403E+02 8.791E-02 3.846E-02 + 1.457E+02 9.341E-02 3.846E-02 + 1.501E+02 1.007E-01 3.846E-02 + 1.552E+02 1.996E-01 4.396E-02 + 1.607E+02 1.447E-01 4.396E-02 + 1.654E+02 1.813E-01 4.579E-02 + 1.709E+02 1.044E-01 4.396E-02 + 1.749E+02 1.465E-01 5.311E-02 + 1.803E+02 7.692E-02 5.128E-02 + 1.851E+02 8.791E-02 6.044E-02 + 1.898E+02 1.190E-01 5.678E-02 + 1.953E+02 -3.846E-02 6.044E-02 +ENDDATA 37 +ENDSUBENT 58 +SUBENT E1900021 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,SS,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 27.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.013E+01 -2.329E-01 1.934E-01 + 2.569E+01 -1.076E-01 3.475E-02 + 3.017E+01 -2.436E-01 2.720E-02 + 3.538E+01 -1.833E-01 3.022E-02 + 4.117E+01 -1.758E-01 2.417E-02 + 4.544E+01 -1.699E-01 2.719E-02 + 5.059E+01 -2.137E-01 2.115E-02 + 5.516E+01 -1.927E-01 2.266E-02 + 6.066E+01 -1.610E-01 1.964E-02 + 6.583E+01 -1.747E-01 2.115E-02 + 7.040E+01 -1.627E-01 2.115E-02 + 7.556E+01 -1.930E-01 2.266E-02 + 8.041E+01 -2.293E-01 1.814E-02 + 8.561E+01 -1.886E-01 2.115E-02 + 9.017E+01 -2.007E-01 1.964E-02 + 9.532E+01 -2.431E-01 2.115E-02 + 1.005E+02 -2.069E-01 1.965E-02 + 1.057E+02 -2.463E-01 1.814E-02 + 1.105E+02 -2.418E-01 1.964E-02 + 1.154E+02 -1.996E-01 1.813E-02 + 1.209E+02 -2.480E-01 1.965E-02 + 1.255E+02 -2.481E-01 2.569E-02 + 1.309E+02 -2.497E-01 2.116E-02 + 1.355E+02 -2.498E-01 2.115E-02 + 1.407E+02 -2.408E-01 2.115E-02 + 1.462E+02 -2.469E-01 2.418E-02 + 1.507E+02 -2.455E-01 2.267E-02 + 1.559E+02 -2.486E-01 2.569E-02 + 1.605E+02 -1.897E-01 2.719E-02 + 1.657E+02 -2.140E-01 2.568E-02 + 1.711E+02 -2.140E-01 3.173E-02 + 1.760E+02 -2.443E-01 2.720E-02 + 1.806E+02 -2.248E-01 3.022E-02 + 1.858E+02 -2.052E-01 3.625E-02 + 1.910E+02 -1.207E-01 3.777E-02 + 1.958E+02 -2.129E-01 3.475E-02 +ENDDATA 38 +ENDSUBENT 59 +SUBENT E1900022 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,NN,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 27.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.004E+01 -2.661E-01 1.916E-01 + 2.557E+01 5.469E-03 4.223E-02 + 2.982E+01 4.773E-02 2.564E-02 + 3.588E+01 9.604E-02 3.167E-02 + 4.071E+01 3.575E-02 2.413E-02 + 4.554E+01 4.111E-03 2.564E-02 + 5.069E+01 3.582E-02 2.413E-02 + 5.522E+01 -3.358E-03 2.262E-02 + 6.036E+01 -1.388E-02 2.111E-02 + 6.581E+01 1.482E-02 1.961E-02 + 7.065E+01 1.335E-02 2.111E-02 + 7.579E+01 -3.203E-03 2.262E-02 + 8.033E+01 -1.071E-02 1.810E-02 + 8.577E+01 -1.670E-02 1.960E-02 + 9.062E+01 1.350E-02 1.659E-02 + 9.546E+01 1.052E-02 1.961E-02 + 1.006E+02 2.413E-02 1.659E-02 + 1.055E+02 1.964E-02 1.961E-02 + 1.109E+02 2.270E-02 1.809E-02 + 1.154E+02 1.369E-02 1.659E-02 + 1.206E+02 5.143E-02 1.961E-02 + 1.251E+02 5.297E-02 1.810E-02 + 1.309E+02 3.190E-02 1.809E-02 + 1.357E+02 6.210E-02 1.961E-02 + 1.406E+02 6.667E-02 2.111E-02 + 1.457E+02 5.011E-02 2.111E-02 + 1.505E+02 4.562E-02 1.961E-02 + 1.560E+02 5.019E-02 2.111E-02 + 1.608E+02 3.665E-02 1.810E-02 + 1.654E+02 1.557E-02 2.564E-02 + 1.711E+02 3.975E-02 2.111E-02 + 1.750E+02 3.676E-02 2.413E-02 + 1.805E+02 3.378E-02 2.715E-02 + 1.856E+02 3.231E-02 2.715E-02 + 1.908E+02 2.783E-02 2.715E-02 + 1.956E+02 6.406E-02 3.016E-02 +ENDDATA 38 +ENDSUBENT 59 +SUBENT E1900023 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,LL,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 27.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 2.018E+01 -5.055E-01 1.943E-01 + 2.519E+01 -7.472E-01 3.791E-02 + 2.935E+01 -6.603E-01 2.528E-02 + 3.507E+01 -6.698E-01 2.686E-02 + 4.049E+01 -6.382E-01 2.370E-02 + 4.462E+01 -6.288E-01 2.528E-02 + 5.003E+01 -6.256E-01 2.212E-02 + 5.481E+01 -5.924E-01 2.054E-02 + 6.021E+01 -6.193E-01 2.054E-02 + 6.530E+01 -6.082E-01 2.054E-02 + 6.976E+01 -5.766E-01 2.212E-02 + 7.548E+01 -5.893E-01 1.738E-02 + 7.993E+01 -5.814E-01 2.054E-02 + 8.534E+01 -5.689E-01 1.896E-02 + 8.984E+01 -5.335E-01 1.908E-02 + 9.489E+01 -5.326E-01 1.738E-02 + 9.969E+01 -5.175E-01 2.066E-02 + 1.051E+02 -5.278E-01 1.896E-02 + 1.102E+02 -4.947E-01 1.896E-02 + 1.153E+02 -4.773E-01 1.896E-02 + 1.200E+02 -4.805E-01 1.580E-02 + 1.251E+02 -4.489E-01 2.212E-02 + 1.302E+02 -4.568E-01 1.896E-02 + 1.353E+02 -4.378E-01 1.896E-02 + 1.401E+02 -4.425E-01 2.528E-02 + 1.452E+02 -3.825E-01 2.370E-02 + 1.500E+02 -3.999E-01 2.528E-02 + 1.557E+02 -3.857E-01 2.212E-02 + 1.605E+02 -3.778E-01 2.212E-02 + 1.652E+02 -3.525E-01 3.002E-02 + 1.706E+02 -3.746E-01 3.002E-02 + 1.751E+02 -3.177E-01 2.844E-02 + 1.802E+02 -3.146E-01 3.160E-02 + 1.853E+02 -3.272E-01 3.476E-02 + 1.900E+02 -3.272E-01 3.791E-02 + 1.948E+02 -2.577E-01 3.791E-02 +ENDDATA 38 +ENDSUBENT 59 +SUBENT E1900024 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,SL,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 27.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 1.948E+01 -2.766E-02 2.006E-01 + 2.496E+01 -1.387E-01 4.255E-02 + 2.953E+01 -7.340E-02 2.736E-02 + 3.470E+01 -1.327E-01 3.192E-02 + 3.988E+01 -1.222E-01 2.888E-02 + 4.475E+01 -1.025E-01 2.584E-02 + 4.992E+01 -1.512E-01 2.736E-02 + 5.449E+01 -1.315E-01 2.432E-02 + 5.997E+01 -1.195E-01 2.281E-02 + 6.514E+01 -1.469E-01 2.432E-02 + 6.941E+01 -1.409E-01 2.280E-02 + 7.489E+01 -1.197E-01 2.280E-02 + 7.976E+01 -1.653E-01 1.976E-02 + 8.493E+01 -1.852E-01 1.824E-02 + 8.980E+01 -1.549E-01 1.976E-02 + 9.498E+01 -1.549E-01 1.977E-02 + 9.954E+01 -1.824E-01 1.672E-02 + 1.047E+02 -1.657E-01 1.976E-02 + 1.102E+02 -1.947E-01 1.825E-02 + 1.148E+02 -1.446E-01 1.976E-02 + 1.196E+02 -1.948E-01 1.824E-02 + 1.245E+02 -1.843E-01 1.824E-02 + 1.300E+02 -1.798E-01 2.280E-02 + 1.349E+02 -1.981E-01 2.128E-02 + 1.400E+02 -1.678E-01 2.128E-02 + 1.452E+02 -1.876E-01 2.129E-02 + 1.498E+02 -1.755E-01 2.280E-02 + 1.549E+02 -1.543E-01 2.736E-02 + 1.601E+02 -1.681E-01 2.736E-02 + 1.650E+02 -1.910E-01 3.040E-02 + 1.702E+02 -9.377E-02 3.039E-02 + 1.747E+02 -1.227E-01 3.040E-02 + 1.799E+02 -1.319E-01 3.496E-02 + 1.854E+02 -1.290E-01 3.800E-02 + 1.900E+02 -1.594E-01 3.952E-02 + 1.948E+02 -1.534E-01 3.800E-02 +ENDDATA 38 +ENDSUBENT 59 +SUBENT E1900025 20050914 20050914 E032 +BIB 8 12 +REACTION (6-C-12(P,N)7-N-12,LS,POL/DA/DE,,D) +EN-SEC ANG is polar angle between beam and neutron in + laboratory system + (E-DGD,N) Energy transfer omega(lab)=E(p)-E(n) +INC-SOURCE Beam intensity is about 50 nA. +SAMPLE Target-thickness is 682 mg/cm**2. +METHOD (DSCAT) +ERR-ANALYS (ERR-T) Total uncertainty +ADD-RES (COMP) Randum phase approximation (RPA combined with + DWIA) +STATUS (CURVE) Data scanned from Fig.3, p054609-4 in + reference +ENDBIB 12 +COMMON 1 3 +ANG +ADEG + 27.0 +ENDCOMMON 3 +DATA 3 36 +E-DGD DATA ERR-T +MEV NO-DIM NO-DIM + 1.998E+01 -4.785E-02 1.937E-01 + 2.563E+01 4.160E-02 4.139E-02 + 3.025E+01 1.680E-02 2.649E-02 + 3.553E+01 -6.331E-03 2.814E-02 + 4.085E+01 6.491E-02 2.980E-02 + 4.512E+01 3.714E-04 2.649E-02 + 5.042E+01 8.693E-03 2.318E-02 + 5.536E+01 -2.769E-02 2.483E-02 + 6.065E+01 -3.427E-02 2.483E-02 + 6.561E+01 -3.588E-02 1.987E-02 + 7.024E+01 -1.267E-02 1.821E-02 + 7.553E+01 -1.262E-02 1.821E-02 + 8.015E+01 -3.742E-02 1.821E-02 + 8.545E+01 -5.917E-03 1.656E-02 + 9.040E+01 -3.568E-02 1.821E-02 + 9.537E+01 -1.080E-02 2.152E-02 + 1.003E+02 -2.566E-02 2.152E-02 + 1.056E+02 -6.039E-02 1.986E-02 + 1.106E+02 -2.226E-02 1.986E-02 + 1.155E+02 -4.209E-02 1.821E-02 + 1.205E+02 -2.053E-02 1.986E-02 + 1.251E+02 -3.932E-03 1.986E-02 + 1.304E+02 -2.233E-03 1.655E-02 + 1.354E+02 -1.213E-02 1.821E-02 + 1.403E+02 -8.773E-03 1.987E-02 + 1.460E+02 4.260E-02 1.986E-02 + 1.506E+02 4.264E-02 2.483E-02 + 1.556E+02 5.261E-02 2.483E-02 + 1.609E+02 7.749E-02 2.980E-02 + 1.655E+02 -6.909E-03 2.980E-02 + 1.711E+02 2.128E-02 3.311E-02 + 1.757E+02 6.106E-02 2.980E-02 + 1.810E+02 3.461E-02 3.476E-02 + 1.856E+02 6.114E-02 3.477E-02 + 1.906E+02 7.442E-02 4.139E-02 + 1.955E+02 3.639E-02 3.807E-02 +ENDDATA 38 +ENDSUBENT 59 +ENDENTRY 25 diff --git a/exforall/F00/F0079.x4 b/exforall/F00/F0079.x4 new file mode 100644 index 000000000..87cf4507e --- /dev/null +++ b/exforall/F00/F0079.x4 @@ -0,0 +1,1267 @@ +ENTRY F0079 20050419 20050831 F021 +SUBENT F0079001 20050419 20050831 F021 +BIB 10 32 +TITLE The interaction of 38 MeV tritons with 12,13C; + collective model studies and single-nucleon transfer + reactions. +AUTHOR (P.J.Simmonds,K.I.Pearce,P.R.Hayes,N.M.Clarke, + R.J.Griffiths,M.C.Mannion,C.A.Ogilvie) +INSTITUTE (2UK KCL,2UK BIR) +REFERENCE (J,NP/A,482,653,1988) +FACILITY (VDGT,2UK ALD) +DETECTOR (TELES)Six semi-conductor detector telescopes, three + mounted on each of two independently rotating arms. + Each detector telescope consisted of two passing + detectors (DE) and one thick stopping detector (E). + The scattering angle could be set between 7.5 and 170 + degr. with an accuracy of better than one minute of arc +SAMPLE The targets were self supporting foils of 12C (nominal + 0.1 mg/cm2) and 13C (0.15 mg/cm2). Absolute cross + sections were calculated, and then the overall + normalisations were checked by optical model searches + on the data below 40 degr. c.m. This led to revised + target thicknesses of 0.095 mg/cm2 (12C) and 0.146 + mg/cm2 (13C). +ANALYSIS Optical model fits. +ERR-ANALYS (ERR-DIG)Digitizing error + (ANG-ERR-D)Digitizing error + An overall error is about +-5%.The non-unity of this + value is a result of systematic errors in the + measurement of the quantity of beam passed through the + target, the solid angle of detection and the target + thickness. The latter contribution is generally the + dominant term. All of the elastic and inelastic data + were renormalised by this factor. +HISTORY (20041207C) +ENDBIB 32 +COMMON 3 3 +EN ERR-DIG EN-RSL +MEV PER-CENT KEV + 38. 0.2 100. +ENDCOMMON 3 +ENDSUBENT 39 +SUBENT F0079002 20050419 20050831 F021 +BIB 3 3 +REACTION (6-C-12(T,EL)6-C-12,,DA,,RTH) +ERR-ANALYS (DATA-ERR)Error from the graphic bars +STATUS (CURVE)Fig.6 +ENDBIB 3 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.12 +ENDCOMMON 3 +DATA 3 28 +ANG-CM DATA-CM DATA-ERR +ADEG NO-DIM NO-DIM + 8.4042 3.6557 2.4473 + 9.9722 4.4723 1.6572 + 11.539 5.5825 1.3711 + 13.116 5.4731 0.99805 + 14.961 4.4771 + 16.284 3.4474 + 17.623 1.7048 + 19.244 0.48964 + 20.695 0.12068E-01 + 22.391 0.54185 + 23.921 1.8503 + 25.732 3.8202 + 27.031 5.6014 + 30.169 7.8921 + 33.330 6.0793 + 36.242 3.1946 + 39.430 1.1686 + 42.586 1.0364 + 45.450 1.9747 + 48.326 2.7266 + 51.750 2.0586 + 54.410 0.81608 + 57.350 0.20364 + 63.315 1.5260 + 69.060 3.5582 + 74.830 4.2702 + 80.071 5.6665 + 85.581 6.2740 +ENDDATA 30 +ENDSUBENT 42 +SUBENT F0079003 20050419 20050831 F021 +BIB 2 2 +REACTION (6-C-12(T,INL)6-C-12,PAR,DA) +STATUS (CURVE)Fig.6 +ENDBIB 2 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.24 +ENDCOMMON 3 +DATA 3 99 +E-LVL ANG-CM DATA-CM +MEV ADEG MB/SR + 4.4300 8.4401 14.569 + 4.4300 10.016 14.002 + 4.4300 11.591 14.867 + 4.4300 15.006 13.461 + 4.4300 16.580 14.580 + 4.4300 18.158 12.683 + 4.4300 19.735 11.033 + 4.4300 21.316 8.3472 + 4.4300 22.895 6.4425 + 4.4300 24.740 4.2395 + 4.4300 26.061 2.5758 + 4.4300 27.380 1.7994 + 4.4300 30.526 2.4273 + 4.4300 33.930 4.3286 + 4.4300 36.813 5.8390 + 4.4300 40.226 6.0784 + 4.4300 43.380 4.9813 + 4.4300 46.009 4.0820 + 4.4300 49.163 3.4813 + 4.4300 52.054 2.9689 + 4.4300 55.467 2.9698 + 4.4300 58.354 3.2820 + 4.4300 64.134 2.7445 + 4.4300 70.175 2.4855 + 4.4300 75.690 2.3424 + 4.4300 80.944 1.9587 + 4.4300 86.726 1.4245 + 7.6500 14.073 0.45524 + 7.6500 15.627 0.73486 + 7.6500 17.193 0.89735 + 7.6500 20.602 0.99228 + 7.6500 22.190 0.75093 + 7.6500 23.775 0.61546 + 7.6500 25.631 0.41329 + 7.6500 27.231 0.23660 + 7.6500 28.820 0.17552 + 7.6500 31.706 0.18647 + 7.6500 34.839 0.27806 + 7.6500 38.514 0.28392 + 7.6500 41.412 0.22819 + 7.6500 44.587 0.13332 + 7.6500 47.751 0.10093 + 7.6500 50.626 0.13353 + 7.6500 53.779 0.12841 + 7.6500 56.933 0.11867 + 7.6500 59.837 0.84620E-01 + 7.6500 65.936 0.22288E-01 + 7.6500 71.745 0.10890E-01 + 7.6500 77.523 0.10692E-01 + 7.6500 83.051 0.77828E-02 + 7.6500 88.552 0.10511E-01 + 9.6400 10.730 0.82369 + 9.6400 12.305 0.92937 + 9.6400 13.878 1.3619 + 9.6400 15.453 1.5367 + 9.6400 17.291 1.6323 + 9.6400 18.866 1.6324 + 9.6400 23.855 1.6002 + 9.6400 25.432 1.3354 + 9.6400 27.271 1.0704 + 9.6400 28.585 0.87548 + 9.6400 31.738 0.67415 + 9.6400 34.891 0.46947 + 9.6400 38.304 0.50885 + 9.6400 41.453 0.66097 + 9.6400 44.867 0.64789 + 9.6400 47.493 0.63505 + 9.6400 50.906 0.68833 + 9.6400 53.795 0.56300 + 9.6400 56.684 0.55185 + 9.6400 60.360 0.54093 + 9.6400 66.139 0.40016 + 9.6400 72.179 0.33398 + 9.6400 77.694 0.30823 + 9.6400 83.471 0.29614 + 9.6400 88.984 0.30222 + 14.080 16.744 0.17310 + 14.080 18.303 0.35711 + 14.080 20.143 0.32959 + 14.080 21.454 0.35726 + 14.080 23.551 0.41138 + 14.080 26.964 0.41993 + 14.080 28.280 0.36486 + 14.080 29.591 0.39549 + 14.080 33.273 0.31716 + 14.080 36.694 0.22543 + 14.080 39.844 0.23955 + 14.080 43.256 0.25457 + 14.080 46.413 0.19218 + 14.080 49.565 0.18101 + 14.080 52.717 0.17395 + 14.080 56.129 0.18485 + 14.080 59.021 0.16064 + 14.080 62.174 0.14534 + 14.080 67.952 0.13694 + 14.080 74.518 0.12647 + 14.080 80.035 0.11218 + 14.080 85.815 0.97523E-01 + 14.080 91.331 0.91882E-01 +ENDDATA 101 +ENDSUBENT 112 +SUBENT F0079004 20050419 20050831 F021 +BIB 3 3 +REACTION (6-C-13(T,EL)6-C-13,,DA,,RTH) +ERR-ANALYS (DATA-ERR)Error from the graphic bars +STATUS (CURVE)Fig.8 +ENDBIB 3 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.29 +ENDCOMMON 3 +DATA 3 20 +ANG-CM DATA-CM DATA-ERR +ADEG NO-DIM NO-DIM + 10.174 2.9397 1.6969 + 13.548 4.6641 1.4116 + 16.698 3.7460 + 19.639 1.1507 + 22.379 0.11989 + 28.708 5.1805 + 31.830 7.0023 + 35.243 5.4036 + 37.899 2.5783 + 41.093 0.92967 + 46.821 1.4469 + 49.945 1.8789 + 52.848 1.1631 + 55.785 0.38709 + 58.935 0.31089 + 64.836 2.4007 + 67.421 4.1254 + 70.551 4.7509 + 73.166 4.7549 + 74.897 5.3672 +ENDDATA 22 +ENDSUBENT 34 +SUBENT F0079005 20050419 20050831 F021 +BIB 2 2 +REACTION (6-C-13(T,INL)6-C-13,PAR,DA) +STATUS (CURVE)Fig.8 +ENDBIB 2 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.29 +ENDCOMMON 3 +DATA 3 76 +E-LVL ANG-CM DATA-CM +MEV ADEG MB/SR + 3.0800 8.4318 6.2554 + 3.0800 14.690 1.0532 + 3.0800 17.938 0.46792 + 3.0800 21.054 0.54980 + 3.0800 27.079 0.51025 + 3.0800 30.265 0.35785 + 3.0800 33.326 0.93010E-01 + 3.0800 36.370 0.27232E-01 + 3.0800 39.418 0.52554E-01 + 3.0800 45.337 0.10577 + 3.0800 48.474 0.10603 + 3.0800 51.378 0.87141E-01 + 3.0800 54.510 0.90894E-01 + 3.0800 57.361 0.10892 + 3.0800 62.882 0.87934E-01 + 3.0800 66.001 0.10129 + 3.0800 68.912 0.78432E-01 + 3.0800 71.545 0.68399E-01 + 3.0800 74.438 0.60857E-01 + 3.6800 12.377 3.7786 + 3.6800 15.779 3.7159 + 3.6800 18.937 3.2465 + 3.6800 22.111 2.5707 + 3.6800 28.296 0.84176 + 3.6800 31.413 0.96871 + 3.6800 34.487 1.4684 + 3.6800 37.609 1.6246 + 3.6800 40.741 1.6945 + 3.6800 46.571 1.0209 + 3.6800 49.724 0.92780 + 3.6800 52.615 0.84296 + 3.6800 55.488 0.86186 + 3.6800 58.869 0.97274 + 3.6800 64.390 0.80280 + 3.6800 67.016 0.74372 + 3.6800 70.178 0.63712 + 3.6800 72.793 0.63857 + 3.6800 75.672 0.62769 + 3.8500 12.352 1.4376 + 3.8500 15.498 1.3579 + 3.8500 18.627 1.4455 + 3.8500 22.020 1.5088 + 3.8500 27.892 0.68316 + 3.8500 30.864 0.36189 + 3.8500 34.070 0.22942 + 3.8500 36.955 0.21665 + 3.8500 40.309 0.29303 + 3.8500 45.860 0.19763 + 3.8500 49.271 0.18302 + 3.8500 52.462 0.12819 + 3.8500 55.086 0.12103 + 3.8500 57.977 0.10982 + 3.8500 63.777 0.80233E-01 + 3.8500 66.653 0.80435E-01 + 3.8500 69.541 0.74457E-01 + 3.8500 72.462 0.55352E-01 + 3.8500 75.537 0.84360E-01 + 7.5500 9.8683 5.1613 + 7.5500 12.766 4.5930 + 7.5500 16.182 4.1719 + 7.5500 22.549 2.5007 + 7.5500 28.449 1.0890 + 7.5500 31.286 1.3600 + 7.5500 34.646 1.6994 + 7.5500 37.512 1.8095 + 7.5500 40.631 2.0056 + 7.5500 46.447 1.4092 + 7.5500 49.591 1.3586 + 7.5500 52.743 1.2585 + 7.5500 55.368 1.1886 + 7.5500 58.498 1.2410 + 7.5500 64.038 0.94411 + 7.5500 67.179 0.92847 + 7.5500 69.808 0.85963 + 7.5500 72.952 0.82870 + 7.5500 75.570 0.81454 +ENDDATA 78 +ENDSUBENT 89 +SUBENT F0079006 20050419 20050831 F021 +BIB 3 3 +REACTION (6-C-12(T,A)5-B-11,PAR,DA) +ERR-ANALYS (DATA-ERR)Error from the graphic bars +STATUS (CURVE)Fig.9,10 +ENDBIB 3 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.44 +ENDCOMMON 3 +DATA 4 226 +E-LVL ANG-CM DATA-CM DATA-ERR +MEV ADEG MB/SR MB/SR + 0.0000 9.9409 38.450 + 0.0000 11.099 30.653 + 0.0000 13.440 23.338 + 0.0000 15.174 16.242 + 0.0000 16.909 11.303 + 0.0000 19.256 9.0029 + 0.0000 19.820 7.1807 + 0.0000 22.209 7.8447 + 0.0000 25.199 8.9615 + 0.0000 27.558 7.8122 + 0.0000 29.923 7.1247 + 0.0000 33.446 5.1801 + 0.0000 36.387 4.1240 + 0.0000 39.959 4.3025 + 0.0000 49.408 2.7195 + 0.0000 52.355 2.2650 + 0.0000 55.909 2.0638 + 0.0000 58.874 1.9681 + 0.0000 61.846 1.9636 + 0.0000 67.752 1.4908 + 0.0000 74.272 1.2954 + 0.0000 79.620 1.2901 + 0.0000 84.975 1.3441 + 0.0000 90.900 1.1684 + 2.1450 9.2819 5.1057 + 2.1450 11.037 4.2629 + 2.1450 12.176 3.1142 + 2.1450 14.476 1.9005 + 2.1450 16.168 1.0612 + 2.1450 17.315 0.81067 + 2.1450 19.091 0.77400 + 2.1450 20.895 0.88369 + 2.1450 23.929 1.3179 + 2.1450 26.327 1.5039 + 2.1450 28.131 1.7170 + 2.1450 32.306 1.8707 + 2.1450 35.256 1.6316 + 2.1450 38.815 1.5553 + 2.1450 48.198 0.68975 + 2.1450 51.778 0.75187 + 2.1450 55.343 0.74950 + 2.1450 58.280 0.59779 + 2.1450 61.202 0.43602 + 2.1450 66.928 0.10848 + 2.1450 72.941 0.16874 + 2.1450 78.332 0.21960 + 2.1450 84.205 0.13970 + 2.1450 90.064 0.81271E-01 + 4.4450 8.6583 0.35795 + 4.4450 11.028 0.34123 + 4.4450 12.246 0.40902 + 4.4450 14.646 0.46791 + 4.4450 17.037 0.51143 + 4.4450 20.603 0.50970 + 4.4450 24.140 0.42330 + 4.4450 25.901 0.36856 + 4.4450 28.879 0.38467 + 4.4450 31.895 0.50426 + 4.4450 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50.054 0.10356 + 6.8600 53.316 0.11896 + 6.8600 56.097 0.11467 + 6.8600 61.665 0.11429 + 6.8600 67.215 0.95558E-01 + 6.8600 72.773 0.85714E-01 + 6.8600 77.859 0.71684E-01 + 6.8600 82.970 0.76675E-01 + 7.5000 13.975 2.1084 + 7.5000 14.890 1.5911 + 7.5000 16.753 1.8305 + 7.5000 18.130 1.3335 + 7.5000 21.377 1.2864 + 7.5000 23.697 1.2856 + 7.5000 25.558 1.4278 + 7.5000 28.798 1.1967 + 7.5000 34.342 0.70525 + 7.5000 43.132 0.40093 + 7.5000 46.377 0.37339 + 7.5000 49.162 0.37311 + 7.5000 51.955 0.46038 + 7.5000 55.200 0.42876 + 7.5000 60.759 0.34672 + 7.5000 66.326 0.33425 + 7.5000 71.427 0.31114 + 7.5000 76.534 0.33335 + 7.5000 82.096 0.28920 + 7.6900 14.485 1.6497 + 7.6900 15.397 1.0818 + 7.6900 17.716 1.0439 + 7.6900 18.631 0.73435 + 7.6900 21.872 0.59429 + 7.6900 23.253 0.44848 + 7.6900 25.109 0.44830 + 7.6900 26.044 0.53434 + 7.6900 29.284 0.43243 + 7.6900 35.287 0.19241 + 7.6900 44.535 0.79745E-01 + 7.6900 46.864 0.10194 + 7.6900 49.642 0.85460E-01 + 7.6900 52.874 0.56010E-01 + 7.6900 55.667 0.71593E-01 + 7.6900 61.219 0.45279E-01 + 7.6900 66.777 0.34139E-01 + 7.6900 72.354 0.43611E-01 + 7.6900 77.000 0.50145E-01 + 7.6900 83.020 0.36498E-01 + 8.2000 8.0404 33.991 + 8.2000 11.239 10.091 + 8.2000 14.019 9.0597 + 8.2000 15.857 5.9004 + 8.2000 17.233 3.9829 + 8.2000 19.076 2.8872 + 8.2000 21.852 2.3290 + 8.2000 23.706 2.2463 + 8.2000 25.085 1.6285 + 8.2000 26.489 2.1661 + 8.2000 28.799 1.6862 + 8.2000 32.967 1.3597 + 8.2000 35.262 0.74072 + 8.2000 44.032 0.23584 + 8.2000 46.796 0.14298 + 8.2000 50.073 0.29175 + 8.2000 52.841 0.19687 + 9.5000 7.9144 1.2340 + 9.5000 9.2846 0.75122 + 9.5000 10.675 0.72482 + 9.5000 12.048 0.47366 + 9.5000 14.834 0.49039 + 9.5000 16.689 0.47309 + 9.5000 17.621 0.52601 + 9.5000 21.337 0.56409 + 9.5000 22.737 0.67315 + 9.5000 24.597 0.74826 + 9.5000 25.993 0.80290 + 9.5000 28.780 0.86123 + 9.5000 31.561 0.80175 + 9.5000 34.811 0.82997 + 9.5000 43.144 0.54140 + 9.5000 45.929 0.54101 + 9.5000 49.167 0.43706 + 9.5000 51.945 0.37905 + 9.5000 55.195 0.39238 + 9.5000 60.757 0.34006 + 9.5000 66.325 0.33957 + 9.5000 71.422 0.28408 + 9.5000 76.985 0.25507 + 9.5000 82.541 0.19185 + 10.750 8.6210 9.0129 + 10.750 9.9926 6.0834 + 10.750 13.224 4.4074 + 10.750 14.603 3.4314 + 10.750 15.986 2.8693 + 10.750 19.208 1.7390 + 10.750 22.440 1.2599 + 10.750 23.822 1.0535 + 10.750 25.205 0.88091 + 10.750 27.054 0.76326 + 10.750 29.808 0.43078 + 10.750 33.057 0.43035 + 10.750 35.375 0.41496 + 10.750 44.620 0.20999 + 10.750 47.389 0.15769 + 10.750 50.175 0.16328 + 10.750 53.398 0.98960E-01 + 10.750 56.176 0.88834E-01 + 10.750 61.271 0.74196E-01 + 10.750 67.753 0.55653E-010.90906E-02 + 10.750 72.850 0.48172E-01 + 10.750 77.976 0.73816E-01 + 10.750 83.043 0.36092E-01 +ENDDATA 227 +ENDSUBENT 239 +SUBENT F0079010 20050419 20050831 F021 +BIB 2 2 +REACTION (6-C-13(T,D)6-C-14,PAR,DA) +STATUS (CURVE)Fig.15,16 +ENDBIB 2 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.29 +ENDCOMMON 3 +DATA 3 136 +E-LVL ANG-CM DATA-CM +MEV ADEG MB/SR + 0.0000 8.7033 14.336 + 0.0000 11.382 11.670 + 0.0000 14.811 5.6020 + 0.0000 17.464 1.9479 + 0.0000 20.884 0.67720 + 0.0000 26.655 1.2163 + 0.0000 29.346 1.5373 + 0.0000 32.406 1.1800 + 0.0000 35.462 0.78218 + 0.0000 38.139 0.60042 + 0.0000 44.267 0.46062 + 0.0000 46.572 0.51776 + 0.0000 50.019 0.44686 + 0.0000 52.697 0.36375 + 0.0000 55.762 0.32331 + 0.0000 61.117 0.20202 + 0.0000 63.802 0.20794 + 0.0000 66.867 0.18482 + 0.0000 69.547 0.15953 + 0.0000 72.613 0.15036 + 6.0940 8.7568 5.4239 + 6.0940 11.416 0.69586 + 6.0940 14.875 1.2508 + 6.0940 17.567 2.3842 + 6.0940 20.635 2.3837 + 6.0940 26.751 0.44767 + 6.0940 29.811 0.24174 + 6.0940 33.267 0.35387 + 6.0940 35.955 0.46068 + 6.0940 39.408 0.53332 + 6.0940 44.771 0.30534 + 6.0940 47.452 0.24143 + 6.0940 50.899 0.16975 + 6.0940 53.581 0.13034 + 6.0940 56.648 0.12655 + 6.0940 62.398 0.10301 + 6.0940 65.084 0.11247 + 6.0940 67.769 0.11579 + 6.0940 70.837 0.11577 + 6.0940 73.520 0.10599 + 7.0000 15.055 1.6363 + 7.0000 21.295 0.54666 + 7.0000 27.143 0.19962 + 7.0000 29.821 0.23888 + 7.0000 33.292 0.21246 + 7.0000 36.388 0.16776 + 7.0000 39.007 0.42190 + 7.0000 44.886 0.10471 + 7.0000 47.836 0.52160 + 7.0000 50.594 0.22731 + 7.0000 56.752 0.21482 + 7.0000 62.116 0.28138 + 7.0000 64.878 0.11555 + 7.0000 68.325 0.13832 + 7.0000 70.649 0.11247 + 7.0000 73.717 0.12685 + 7.3410 9.3286 45.532 + 7.3410 12.773 34.924 + 7.3410 15.447 23.818 + 7.3410 18.117 14.441 + 7.3410 21.558 9.8478 + 7.3410 27.287 4.3185 + 7.3410 30.737 4.0695 + 7.3410 33.415 3.1218 + 7.3410 36.473 2.2579 + 7.3410 39.533 1.6818 + 7.3410 45.264 0.75953 + 7.3410 48.329 0.69504 + 7.3410 51.010 0.61764 + 7.3410 54.076 0.56520 + 7.3410 57.147 0.61701 + 7.3410 62.889 0.43314 + 7.3410 65.190 0.43298 + 7.3410 68.254 0.37358 + 7.3410 70.936 0.33198 + 7.3410 73.623 0.37325 + 8.3200 9.3746 0.92685 + 8.3200 12.532 0.51681 + 8.3200 16.075 0.28826 + 8.3200 18.852 0.15604 + 8.3200 21.552 0.14747 + 8.3200 28.159 0.90040E-01 + 8.3200 30.875 0.75674E-01 + 8.3200 33.956 0.73669E-01 + 8.3200 37.057 0.61935E-01 + 8.3200 39.761 0.56841E-01 + 8.3200 45.591 0.36780E-01 + 8.3200 48.279 0.37957E-01 + 8.3200 51.736 0.39195E-01 + 8.3200 54.817 0.38157E-01 + 8.3200 57.493 0.43000E-01 + 8.3200 63.249 0.47173E-01 + 8.3200 65.573 0.42029E-01 + 8.3200 69.071 0.32368E-01 + 8.3200 71.795 0.25654E-01 + 8.3200 74.483 0.26475E-01 + 9.8000 9.8037 3.1378 + 9.8000 12.770 2.2817 + 9.8000 15.914 1.3533 + 9.8000 19.032 0.98437 + 9.8000 22.161 0.65605 + 9.8000 28.407 0.31803 + 9.8000 31.495 0.29207 + 9.8000 34.198 0.26814 + 9.8000 36.935 0.18938 + 9.8000 40.415 0.16412 + 9.8000 46.232 0.11284 + 9.8000 48.925 0.11306 + 9.8000 51.997 0.11667 + 9.8000 55.100 0.95353E-01 + 9.8000 57.818 0.77910E-01 + 9.8000 63.587 0.78242E-01 + 9.8000 66.350 0.45062E-01 + 9.8000 69.789 0.53809E-01 + 9.8000 72.511 0.42703E-01 + 9.8000 75.166 0.57265E-01 + 10.400 9.9124 5.6340 + 10.400 12.728 1.6306 + 10.400 16.212 1.2899 + 10.400 19.319 0.96153 + 10.400 22.046 0.67547 + 10.400 28.261 0.36442 + 10.400 30.979 0.27974 + 10.400 34.467 0.21484 + 10.400 37.561 0.18025 + 10.400 40.650 0.16044 + 10.400 46.448 0.11979 + 10.400 49.528 0.11651 + 10.400 52.240 0.94883E-01 + 10.400 54.566 0.79571E-01 + 10.400 58.027 0.79732E-01 + 10.400 63.816 0.65050E-01 + 10.400 66.890 0.67122E-01 + 10.400 69.559 0.85162E-01 + 10.400 72.280 0.63469E-01 + 10.400 75.753 0.56507E-01 +ENDDATA 138 +ENDSUBENT 149 +SUBENT F0079011 20050419 20050831 F021 +BIB 2 2 +REACTION (6-C-13(T,D)6-C-14,PAR,DA) +STATUS (CURVE)Fig.15 +ENDBIB 2 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.29 +ENDCOMMON 3 +DATA 4 20 +E-LVL-MIN E-LVL-MAX ANG-CM DATA-CM +MEV MEV ADEG MB/SR + 6.5800 6.7280 8.3828 70.804 + 6.5800 6.7280 11.831 55.895 + 6.5800 6.7280 14.894 38.072 + 6.5800 6.7280 17.573 25.179 + 6.5800 6.7280 21.019 16.651 + 6.5800 6.7280 26.760 7.5007 + 6.5800 6.7280 29.443 6.6639 + 6.5800 6.7280 32.891 5.1077 + 6.5800 6.7280 35.571 3.6908 + 6.5800 6.7280 38.635 2.6668 + 6.5800 6.7280 44.377 1.2373 + 6.5800 6.7280 47.437 0.70598 + 6.5800 6.7280 50.509 0.92057 + 6.5800 6.7280 53.194 0.97634 + 6.5800 6.7280 56.262 1.0053 + 6.5800 6.7280 61.628 0.77045 + 6.5800 6.7280 64.698 0.89276 + 6.5800 6.7280 67.380 0.72594 + 6.5800 6.7280 70.447 0.70465 + 6.5800 6.7280 73.133 0.74734 +ENDDATA 22 +ENDSUBENT 33 +ENDENTRY 11 diff --git a/exforall/F00/F0087.x4 b/exforall/F00/F0087.x4 new file mode 100644 index 000000000..706dd948f --- /dev/null +++ b/exforall/F00/F0087.x4 @@ -0,0 +1,311 @@ +ENTRY F0087 20050518 20050831 F022 +SUBENT F0087001 20050518 20050831 F022 +BIB 13 25 +TITLE A study of 52V with 51V(t,d) reaction. +AUTHOR (O.Karban,J.B.A.England,D.Barker,M.Mannion,J.M.Nelson, + C.A.Ogilvie,L.Potvin,L.Zybert,R.Zybert,N.M.Clarke, + K.I.Pearce,D.L.Watson,M.D.Cohler) +INSTITUTE (2UK BIR,2UK KCL,2UK UK) +REFERENCE (J,NP/A,472,189,1987) +FACILITY (VDGT,2UK ALD) +DETECTOR (SOLST) Ten semiconductor detector telescopes in a 1 m + diameter scattering chamber. +METHOD (BCINT) +SAMPLE Self-supporting vanadium target was used. Target + thickness was 1.98+-0.04 mg/cm2. +ANALYSIS Deuteron spectra were analyzed using a gaussian + peak-fitting programme which provided peak centroids, + integrals and background subtraction for each deuteron + group. +MONITOR 1(23-V-51(N,G)23-V-52,PAR,DA) Energy calibration of + spectra was based on measured excitation energies. + 2(6-C-12(T,D)6-C-13,PAR,DA) This reaction was used in + high excitation region. +MONIT-REF 1(,J.B.M. de Haas+,J,NP/A,419,101,1984) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bars +HISTORY (20041217C) +ENDBIB 25 +COMMON 4 3 +EN EN-RSL ANG-ERR-D ERR-DIG +MEV KEV ADEG PER-CENT + 33. 65. 0.4 0.1 +ENDCOMMON 3 +ENDSUBENT 32 +SUBENT F0087002 20050518 20050831 F022 +BIB 2 2 +REACTION (23-V-51(T,D)23-V-52,PAR,DA) +STATUS (CURVE)Fig.3 +ENDBIB 2 +NOCOMMON 0 0 +DATA 4 264 +E-LVL ANG-CM DATA-CM DATA-ERR +MEV ADEG MB/SR MB/SR +0.20000E-01 7.6479 29.867 +0.20000E-01 9.0094 21.953 +0.20000E-01 10.520 14.505 +0.20000E-01 11.720 7.6551 +0.20000E-01 12.769 4.3373 +0.20000E-01 14.279 2.7659 +0.20000E-01 16.109 3.0757 +0.20000E-01 16.879 4.0852 +0.20000E-01 18.410 5.3615 +0.20000E-01 20.696 5.8221 +0.20000E-01 22.211 4.4339 +0.20000E-01 23.575 3.5403 +0.20000E-01 24.936 2.5114 +0.20000E-01 26.294 1.6400 +0.20000E-01 26.743 1.2640 +0.20000E-01 28.409 0.94006 +0.20000E-01 30.241 1.1091 +0.20000E-01 32.225 1.2778 +0.20000E-01 34.662 1.2773 +0.20000E-01 37.691 0.73205 +0.20000E-01 39.357 0.53804 +0.20000E-01 40.113 0.44518 +0.20000E-01 41.627 0.33110 +0.20000E-01 43.912 0.34293 +0.20000E-01 45.890 0.32311 +0.20000E-01 47.714 0.28359 +0.20000E-01 49.381 0.21853 +0.20000E-01 51.050 0.17656 +0.20000E-01 51.645 0.10869 +0.20000E-01 53.156 0.72668E-01 +0.20000E-01 54.817 0.45256E-01 +0.20000E-01 57.256 0.48565E-01 +0.20000E-01 58.483 0.65267E-01 +0.20000E-01 59.711 0.94166E-01 +0.20000E-01 62.001 0.11510 +0.20000E-01 64.436 0.10717 +0.20000E-01 67.471 0.75105E-01 +0.20000E-01 69.896 0.50208E-01 +0.20000E-01 72.318 0.30896E-01 +0.20000E-01 74.756 0.31999E-01 +0.20000E-01 77.796 0.27100E-01 +0.20000E-01 80.087 0.33918E-01 +0.20000E-01 82.680 0.40010E-01 +0.20000E-01 85.567 0.31939E-01 +0.20000E-01 87.693 0.26109E-01 +0.20000E-01 90.123 0.20844E-01 +0.20000E-01 92.706 0.16838E-01 +0.20000E-01 95.286 0.12821E-01 +0.20000E-01 98.332 0.12966E-01 +0.20000E-01 100.77 0.12216E-01 +0.20000E-01 102.89 0.10226E-01 +0.20000E-01 105.48 0.88682E-02 +0.20000E-01 108.22 0.82565E-02 +0.20000E-01 110.80 0.69929E-02 +0.20000E-01 113.23 0.59934E-02 +0.20000E-01 116.13 0.62806E-02 +0.20000E-01 117.49 0.46713E-02 +0.20000E-01 120.84 0.41970E-02 +0.20000E-01 123.57 0.32335E-02 +0.20000E-01 128.45 0.44468E-02 + 1.5690 7.2483 10.291 + 1.5690 8.7447 7.4485 + 1.5690 10.033 5.0328 + 1.5690 10.896 3.5710 + 1.5690 12.186 2.3660 + 1.5690 13.675 1.9842 + 1.5690 14.953 1.6314 + 1.5690 16.321 1.8546 + 1.5690 18.009 1.9493 + 1.5690 19.596 1.9127 + 1.5690 20.558 1.5571 + 1.5690 21.730 1.2929 + 1.5690 22.905 1.0022 + 1.5690 24.401 0.73258 + 1.5690 25.365 0.57342 + 1.5690 26.642 0.49037 + 1.5690 28.024 0.41936 + 1.5690 29.495 0.49583 + 1.5690 30.664 0.43666 + 1.5690 32.034 0.47727 + 1.5690 33.514 0.47758 + 1.5690 34.364 0.43310 + 1.5690 36.503 0.26800 + 1.5690 38.213 0.18471 + 1.5690 39.803 0.16921 + 1.5690 40.554 0.13639 + 1.5690 42.042 0.11551 + 1.5690 43.737 0.10687 + 1.5690 45.109 0.11342 + 1.5690 46.691 0.12038 + 1.5690 48.176 0.10813 + 1.5690 49.347 0.92465E-01 + 1.5690 50.621 0.82238E-01 + 1.5690 51.374 0.64366E-01 + 1.5690 52.653 0.52407E-01 + 1.5690 54.274 0.26125E-01 + 1.5690 56.065 0.29127E-01 + 1.5690 57.655 0.26946E-01 + 1.5690 59.341 0.29456E-01 + 1.5690 61.773 0.29488E-01 + 1.5690 64.527 0.25987E-01 + 1.5690 67.187 0.18636E-01 + 1.5690 69.732 0.15789E-01 + 1.5690 72.166 0.14902E-01 + 1.5690 74.694 0.17802E-01 + 1.5690 77.340 0.16477E-01 + 1.5690 79.884 0.14519E-01 + 1.5690 82.222 0.11261E-01 + 1.5690 84.655 0.10946E-01 + 1.5690 87.418 0.82445E-02 + 1.5690 90.273 0.79370E-02 + 1.7750 6.8881 6.6041 + 1.7750 8.7498 5.4244 + 1.7750 9.8975 4.6797 + 1.7750 11.474 3.8815 + 1.7750 12.485 3.1558 + 1.7750 14.341 2.7776 + 1.7750 15.491 2.3263 + 1.7750 16.783 1.9485 + 1.7750 18.213 1.7317 + 1.7750 19.788 1.4650 + 1.7750 20.943 1.1450 + 1.7750 22.236 0.95904 + 1.7750 23.402 0.65281 + 1.7750 24.973 0.58597 + 1.7750 26.405 0.50061 + 1.7750 28.546 0.43633 + 1.7750 30.404 0.37653 + 1.7750 32.256 0.35163 + 1.7750 34.249 0.33165 + 1.7750 35.256 0.28051 + 1.7750 36.265 0.23033 + 1.7750 37.418 0.18544 + 1.7750 38.854 0.15229 + 1.7750 40.710 0.13404 + 1.7750 41.009 0.11112 + 1.7750 42.146 0.11008 + 1.7750 43.564 0.11345 + 1.7750 45.694 0.11354 + 1.7750 46.984 0.97955E-01 + 1.7750 48.413 0.87057E-01 + 1.7750 49.702 0.75854E-01 + 1.7750 50.851 0.64797E-01 + 1.7750 51.591 0.44100E-01 + 1.7750 51.701 0.66767E-01 + 1.7750 53.157 0.42000E-01 + 1.7750 54.009 0.42431E-01 + 1.7750 54.748 0.29164E-01 + 1.7750 56.876 0.30065E-01 + 1.7750 58.424 0.35934E-01 + 1.7750 59.841 0.37773E-01 + 1.7750 60.834 0.38162E-01 + 1.7750 62.116 0.36341E-01 + 1.7750 64.695 0.27050E-01 + 1.7750 67.415 0.20741E-01 + 1.7750 69.979 0.18809E-01 + 1.7750 72.548 0.15918E-01 + 1.7750 75.399 0.14016E-01 + 1.7750 78.258 0.10962E-01 + 1.7750 81.528 0.10550E-01 + 1.7750 83.243 0.91942E-02 + 1.7750 85.665 0.83374E-02 + 1.7750 88.516 0.72688E-02 + 1.7750 91.366 0.64635E-02 + 1.7750 93.517 0.49550E-020.56818E-03 + 1.7750 96.634 0.54218E-020.44627E-03 + 1.7750 99.032 0.67435E-020.77408E-03 + 1.7750 101.76 0.48254E-020.39690E-03 + 1.7750 104.47 0.38112E-020.43748E-03 + 1.7750 106.76 0.31001E-020.22185E-03 + 1.7750 109.18 0.29828E-020.34239E-03 + 1.7750 111.47 0.24263E-020.27822E-03 + 1.7750 113.88 0.23810E-020.24724E-03 + 1.7750 116.57 0.26833E-020.27862E-03 + 1.7750 118.72 0.22261E-020.25540E-03 + 1.7750 121.28 0.19989E-020.25120E-03 + 2.1550 7.2550 4.4533 + 2.1550 8.2871 3.2960 + 2.1550 10.068 3.6806 + 2.1550 12.573 3.4527 + 2.1550 15.378 2.3414 + 2.1550 17.554 1.5508 + 2.1550 20.352 0.89773 + 2.1550 23.030 0.36114 0.32721E-01 + 2.1550 25.751 0.39372 0.27063E-01 + 2.1550 28.472 0.43955 0.33460E-01 + 2.1550 31.072 0.33039 0.27195E-01 + 2.1550 33.672 0.24444 + 2.1550 36.265 0.15560 + 2.1550 38.655 0.11604 + 2.1550 41.368 0.10630 + 2.1550 43.975 0.92861E-01 + 2.1550 46.584 0.87802E-01 + 2.1550 49.185 0.67582E-01 + 2.1550 51.780 0.44404E-01 + 2.1550 54.058 0.27172E-01 + 2.1550 56.564 0.26102E-01 + 2.1550 59.597 0.28008E-010.21314E-02 + 2.1550 61.695 0.34117E-010.33973E-02 + 2.1550 64.184 0.22241E-010.18539E-02 + 2.1550 66.793 0.20374E-010.25675E-02 + 2.1550 69.388 0.13600E-010.18347E-02 + 2.1550 71.684 0.12658E-010.15052E-02 + 2.1550 74.497 0.10462E-010.12249E-02 + 2.1550 76.985 0.66073E-020.71584E-03 + 2.1550 79.505 0.89904E-020.12136E-02 + 4.3070 6.9277 8.1287 + 4.3070 9.4513 6.5143 + 4.3070 12.074 6.1660 + 4.3070 14.807 4.9026 + 4.3070 17.643 4.1533 + 4.3070 20.280 2.6241 + 4.3070 22.808 1.8820 + 4.3070 25.869 1.0475 + 4.3070 28.294 0.69403 + 4.3070 31.031 0.50977 + 4.3070 33.859 0.53069 + 4.3070 36.387 0.38062 + 4.3070 39.125 0.26239 + 4.3070 41.759 0.18377 + 4.3070 44.597 0.14612 + 4.3070 47.426 0.15092 + 4.3070 49.520 0.16086 + 4.3070 52.350 0.15969 + 4.3070 54.145 0.11182 + 4.3070 56.873 0.10336 + 4.3070 59.601 0.93293E-01 + 4.3070 62.229 0.77174E-01 + 4.3070 64.643 0.69103E-01 + 4.3070 67.162 0.63366E-01 + 4.3070 69.679 0.60936E-01 + 4.3070 72.515 0.50811E-010.55149E-02 + 4.3070 75.044 0.35586E-01 + 4.3070 77.256 0.26135E-010.21822E-02 + 4.3070 80.094 0.21280E-010.17768E-02 + 4.3070 82.618 0.16786E-010.12791E-02 + 4.3070 86.084 0.13778E-010.13745E-02 + 5.4640 7.6177 1.3346 + 5.4640 10.264 1.0473 + 5.4640 12.740 0.38695 0.44947E-01 + 5.4640 15.259 0.46380 0.37851E-01 + 5.4640 18.319 0.42918 0.46081E-01 + 5.4640 20.864 0.31381 0.30989E-01 + 5.4640 23.414 0.20884 0.24252E-01 + 5.4640 25.978 0.10561 0.11340E-01 + 5.4640 31.273 0.63023E-010.84288E-02 + 5.4640 34.264 0.28559E-01 + 5.4640 36.794 0.28135E-010.30199E-02 + 5.4640 39.126 0.21562E-010.25025E-02 + 5.4640 41.683 0.12363E-010.11142E-02 + 5.4640 44.415 0.14474E-01 + 5.4640 46.838 0.14484E-01 + 5.4640 49.481 0.12293E-01 + 5.4640 52.129 0.94224E-020.92920E-03 + 5.4640 54.865 0.99622E-020.10700E-02 + 5.4640 57.127 0.38884E-020.41750E-03 + 5.4640 59.967 0.42758E-020.42237E-03 + 5.4640 62.079 0.38940E-020.32195E-03 + 5.4640 64.705 0.45589E-020.50612E-03 + 5.4640 67.350 0.36626E-020.45752E-03 + 5.4640 69.541 0.56424E-020.65522E-03 + 5.4640 72.518 0.33648E-020.42032E-03 + 5.4640 75.034 0.42943E-020.46123E-03 + 5.4640 77.604 0.19458E-020.24306E-03 +ENDDATA 266 +ENDSUBENT 273 +ENDENTRY 2 diff --git a/exforall/F00/F0088.x4 b/exforall/F00/F0088.x4 new file mode 100644 index 000000000..1b4437a32 --- /dev/null +++ b/exforall/F00/F0088.x4 @@ -0,0 +1,396 @@ +ENTRY F0088 20050503 20050831 F021 +SUBENT F0088001 20050503 20050831 F021 +BIB 12 33 +TITLE Deep proton-hole states in 147Pr, 151Pm and 155Eu. +AUTHOR (L.Zybert,J.B.A.England,G.M.Field,O.Karban,R.Zybert, + M.Becha,C.N.Pinder,G.C.Morrison,M.Bentley,P.Fallon, + R.Moktah,J.W.Roberts,J.F.Sharpey-Schafer) +INSTITUTE (2UK BIR) + (2UK LVP) +REFERENCE (J,NP/A,510,441,1990) +FACILITY (VDGT,2UK ALD) +INC-SOURCE Incident beams of tritons were used. Beam currents + varied from 20 to 100 nA. +DETECTOR (TELES,SIBAR) Array of ten telescopes was used, with + surface barrier detectors of 100 microns thickness as + delta E detectors. + (SILI) Telescopes with 5 mm thick lithium drifted + detectors as E-detectors were used. + Hardware particle-identification system was used for + conversion of analog signals into spectra. + Energy resolution of telescopes at most forward angles + was affected by signal pile-up due to high counting + rates. Average value was 80-100 keV. +SAMPLE Targets were self-supporting, made from isotopically + enriched material and rolled to following thicknesses: + 148Nd(87.9%) 0.367+-0.02 mg/cm2, 152Sm(98.3%) 0.437+- + 0.01 mg/cm2 and 156Gd(93.6%) 0.592+-0.014 mg/cm2. +METHOD (EDE) +MONITOR Target thicknesses were obtained from measurements of + Rutherford cross sections using the 25 MeV alpha- + particle beam from Radial Ridge cyclotron at the + University of Birmingham. + Energy calibration of spectra was achieved using peaks + from (t,a) reaction on 16O and 12C. +ERR-ANALYS (DATA-ERR) Error in absolute cross-section. +HISTORY (20040927C) +ENDBIB 33 +COMMON 2 3 +ANG-RSL DATA-ERR +ADEG PER-CENT + 0.6 5. +ENDCOMMON 3 +ENDSUBENT 40 +SUBENT F0088002 20050503 20050831 F021 +BIB 3 5 +REACTION (62-SM-152(T,A)61-PM-151,PAR,DA) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR1) Error from the graphic bars +STATUS (CURVE)Fig.2 +ENDBIB 5 +COMMON 3 3 +EN ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT + 35.32 0.1 0.1 +ENDCOMMON 3 +DATA 5 79 +E-EXC-MIN E-EXC-MAX ANG-CM DATA-CM DATA-ERR1 +MEV MEV ADEG MB/SR MB/SR + 0.0000 0.23000 10.174 1.1518 + 0.0000 0.23000 11.970 1.1050 + 0.0000 0.23000 13.888 0.97795 + 0.0000 0.23000 15.505 0.81622 + 0.0000 0.23000 16.957 0.55295 + 0.0000 0.23000 18.883 0.47270 + 0.0000 0.23000 20.479 0.43275 + 0.0000 0.23000 25.412 0.27606 + 0.0000 0.23000 27.515 0.17078 0.23214E-01 + 0.0000 0.23000 29.400 0.10932 0.17800E-01 + 0.0000 0.23000 30.929 0.13518 0.25426E-01 + 0.0000 0.23000 32.553 0.10898 0.15207E-01 + 0.0000 0.23000 34.482 0.92090E-010.12872E-01 +0.23000 0.48000 10.142 3.1084 +0.23000 0.48000 11.752 2.6604 +0.23000 0.48000 13.762 2.4970 +0.23000 0.48000 15.247 2.3405 +0.23000 0.48000 16.837 2.1944 +0.23000 0.48000 18.936 1.3511 +0.23000 0.48000 20.480 0.95253 +0.23000 0.48000 25.678 0.75946 +0.23000 0.48000 27.438 0.52363 +0.23000 0.48000 29.560 0.28769 0.46015E-01 +0.23000 0.48000 30.735 0.26338 0.38831E-01 +0.23000 0.48000 32.588 0.31753 0.37402E-01 +0.23000 0.48000 34.538 0.23994 0.35377E-01 +0.48000 0.80000 10.035 2.9207 +0.48000 0.80000 11.788 2.0638 +0.48000 0.80000 13.824 1.6997 +0.48000 0.80000 15.185 1.7460 +0.48000 0.80000 17.158 1.1779 +0.48000 0.80000 18.999 0.90374 +0.48000 0.80000 20.412 0.71742 0.10832 +0.48000 0.80000 25.397 0.57473 +0.48000 0.80000 27.456 0.42595 +0.48000 0.80000 29.440 0.27100 0.37284E-01 +0.48000 0.80000 30.949 0.22551 0.34173E-01 +0.48000 0.80000 32.410 0.23723 +0.48000 0.80000 34.423 0.21966 0.27310E-01 +0.80000 1.2000 9.9206 1.5191 +0.80000 1.2000 11.842 1.3643 +0.80000 1.2000 13.693 1.0581 +0.80000 1.2000 14.891 0.89638 +0.80000 1.2000 16.602 0.80458 +0.80000 1.2000 18.615 0.49265 +0.80000 1.2000 20.145 0.39043 0.49370E-01 +0.80000 1.2000 25.113 0.36165 0.42151E-01 +0.80000 1.2000 27.102 0.24507 0.23566E-01 +0.80000 1.2000 29.047 0.12813 0.18589E-01 +0.80000 1.2000 30.458 0.16670 0.25918E-01 +0.80000 1.2000 32.056 0.15472 0.17994E-01 +0.80000 1.2000 34.263 0.15742 0.18388E-01 + 1.2000 1.8000 9.9813 1.4062 + 1.2000 1.8000 11.834 1.0920 + 1.2000 1.8000 13.883 0.89981 + 1.2000 1.8000 14.941 0.88177 + 1.2000 1.8000 16.794 0.68471 0.76600E-01 + 1.2000 1.8000 18.889 0.46755 + 1.2000 1.8000 20.389 0.42255 0.52669E-01 + 1.2000 1.8000 25.308 0.31232 + 1.2000 1.8000 27.322 0.29632 + 1.2000 1.8000 29.180 0.14720 0.20358E-01 + 1.2000 1.8000 30.708 0.11829 0.20268E-01 + 1.2000 1.8000 32.249 0.13848 0.13892E-01 + 1.2000 1.8000 34.210 0.10631 0.12886E-01 + 1.8000 10.000 10.100 13.468 2.9249 + 1.8000 10.000 11.738 10.851 1.7420 + 1.8000 10.000 13.984 14.125 2.9420 + 1.8000 10.000 15.374 13.078 3.6416 + 1.8000 10.000 17.027 9.9411 1.2992 + 1.8000 10.000 18.947 6.1320 + 1.8000 10.000 20.511 4.3960 0.99453 + 1.8000 10.000 22.293 4.5259 0.85698 + 1.8000 10.000 25.317 5.0763 1.2389 + 1.8000 10.000 27.341 4.6552 + 1.8000 10.000 29.190 2.5254 0.45493 + 1.8000 10.000 30.670 2.4792 0.34823 + 1.8000 10.000 32.297 3.0741 + 1.8000 10.000 34.232 2.6588 +ENDDATA 81 +ENDSUBENT 95 +SUBENT F0088003 20050503 20050831 F021 +BIB 3 3 +REACTION (62-SM-152(T,A)61-PM-151,PAR,DA) +ERR-ANALYS (DATA-ERR1) Error in cross-section +STATUS (TABLE)Table 3 +ENDBIB 3 +COMMON 2 3 +ANG EN +ADEG MEV + 11.75 35.32 +ENDCOMMON 3 +DATA 4 6 +E-EXC-MIN E-EXC-MAX DATA DATA-ERR1 +MEV MEV MU-B/SR MU-B/SR + 0.0000 0.23000 1105.0 +0.23000 0.48000 2588.0 +0.48000 0.80000 2069.0 +0.80000 1.2000 1369.0 + 1.2000 1.8000 1093.0 + 1.8000 10.000 14703. 1957.0 +ENDDATA 8 +ENDSUBENT 20 +SUBENT F0088004 20050503 20050831 F021 +BIB 3 5 +REACTION (64-GD-156(T,A)63-EU-155,PAR,DA) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR1) Error from the graphic bars +STATUS (CURVE)Fig.5 +ENDBIB 5 +COMMON 3 3 +EN ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT + 35.32 0.1 0.1 +ENDCOMMON 3 +DATA 5 41 +E-EXC-MIN E-EXC-MAX ANG-CM DATA-CM DATA-ERR1 +MEV MEV ADEG MB/SR MB/SR + 0.0000 0.23000 12.576 1.1942 + 0.0000 0.23000 15.131 1.0571 0.12769 + 0.0000 0.23000 17.798 0.32697 0.10977 + 0.0000 0.23000 20.214 0.34073 + 0.0000 0.23000 22.617 0.37642 + 0.0000 0.23000 25.189 0.30703 + 0.0000 0.23000 27.878 0.23629 + 0.0000 0.23000 30.459 0.18393 0.20230E-01 +0.23000 0.55000 12.621 2.3352 +0.23000 0.55000 15.103 1.7352 0.24765 +0.23000 0.55000 17.776 1.4215 0.16395 +0.23000 0.55000 20.476 0.59028 +0.23000 0.55000 22.901 0.58681 +0.23000 0.55000 25.225 0.56923 +0.23000 0.55000 27.660 0.31225 0.31909E-01 +0.23000 0.55000 30.605 0.18672 +0.85000 1.0600 12.811 0.80842 +0.85000 1.0600 15.224 0.85247 +0.85000 1.0600 17.713 0.62544 0.69457E-01 +0.85000 1.0600 20.370 0.33860 0.60270E-01 +0.85000 1.0600 22.764 0.39209 0.43543E-01 +0.85000 1.0600 25.260 0.45949 0.57037E-01 +0.85000 1.0600 27.915 0.15214 0.29189E-01 +0.85000 1.0600 30.546 0.15498 0.29784E-01 + 1.0600 2.0000 12.871 2.3955 + 1.0600 2.0000 15.330 2.0924 + 1.0600 2.0000 17.846 1.3468 + 1.0600 2.0000 20.378 0.79847 + 1.0600 2.0000 22.832 0.71401 + 1.0600 2.0000 25.267 0.70967 + 1.0600 2.0000 28.094 0.47351 0.32214E-01 + 1.0600 2.0000 30.641 0.25857 0.23185E-01 + 2.0000 10.500 10.161 12.806 3.7823 + 2.0000 10.500 12.807 12.727 2.1662 + 2.0000 10.500 15.163 10.736 1.2924 + 2.0000 10.500 17.788 6.4604 0.71110 + 2.0000 10.500 20.282 4.5230 0.50161 + 2.0000 10.500 22.918 4.7649 0.62313 + 2.0000 10.500 25.344 4.9593 0.44173 + 2.0000 10.500 28.091 2.7191 0.59108 + 2.0000 10.500 30.585 1.9037 0.22955 +ENDDATA 43 +ENDSUBENT 57 +SUBENT F0088005 20050503 20050831 F021 +BIB 3 3 +REACTION (64-GD-156(T,A)63-EU-155,PAR,DA) +ERR-ANALYS (DATA-ERR1) Error in cross-section +STATUS (TABLE)Table 4 +ENDBIB 3 +COMMON 2 3 +ANG EN +ADEG MEV + 12.5 35.32 +ENDCOMMON 3 +DATA 4 5 +E-EXC-MIN E-EXC-MAX DATA DATA-ERR1 +MEV MEV MU-B/SR MU-B/SR + 0.0000 0.23000 1178.0 +0.23000 0.55000 2284.0 +0.85000 1.0600 802.00 + 1.0600 2.0000 2375.0 + 2.0000 10.500 12670. 2345.0 +ENDDATA 7 +ENDSUBENT 19 +SUBENT F0088006 20050503 20050831 F021 +BIB 3 3 +REACTION (60-ND-148(T,A)59-PR-147,PAR,DA) +ERR-ANALYS (DATA-ERR1) Error in cross-section +STATUS (TABLE)Table 5 +ENDBIB 3 +COMMON 3 3 +ANG EN EN-RSL +ADEG MEV KEV + 12.5 37.32 70. +ENDCOMMON 3 +DATA 4 9 +E-EXC E-EXC-ERR DATA DATA-ERR1 +MEV MEV MU-B/SR MU-B/SR + 0.0000 0.20000E-01 2156.0 129.00 +0.60000E-010.23000E-01 880.00 136.00 +0.12600 0.23000E-01 158.00 82.000 +0.22500 0.13000E-01 89.000 20.000 +0.35200 0.90000E-02 1000.0 49.000 +0.43300 0.15000E-01 254.00 40.000 +0.62500 0.20000E-01 131.00 40.000 +0.68800 0.10000E-01 404.00 109.00 +0.76700 0.11000E-01 722.00 109.00 +ENDDATA 11 +ENDSUBENT 23 +SUBENT F0088007 20050503 20050831 F021 +BIB 3 3 +REACTION (60-ND-148(T,A)59-PR-147,PAR,DA) +ERR-ANALYS (DATA-ERR1) Error in cross-section +STATUS (TABLE)Table 5 +ENDBIB 3 +COMMON 2 3 +ANG EN-RSL +ADEG KEV + 12.5 70. +ENDCOMMON 3 +DATA 5 2 +EN E-EXC-MIN E-EXC-MAX DATA DATA-ERR1 +MEV MEV MEV MU-B/SR MU-B/SR + 37.320 2.2000 8.4000 13585. 1190.0 + 35.320 2.0000 8.6000 12689. 2122.0 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0088008 20050503 20050831 F021 +BIB 3 5 +REACTION (60-ND-148(T,A)59-PR-147,PAR,DA) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR1) Error from the graphic bars +STATUS (CURVE)Fig.9 +ENDBIB 5 +COMMON 3 3 +EN ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT + 37.32 0.1 0.1 +ENDCOMMON 3 +DATA 4 45 +E-EXC ANG-CM DATA-CM DATA-ERR1 +MEV ADEG MB/SR MB/SR + 0.0000 12.931 2.1215 + 0.0000 15.462 1.4000 0.13855 + 0.0000 18.003 0.71625 0.10005 + 0.0000 20.530 0.53069 0.68837E-01 + 0.0000 23.043 0.59644 0.17008 + 0.0000 25.359 0.46281 0.59997E-01 + 0.0000 27.902 0.22346 0.24422E-01 + 0.0000 30.839 0.21862 + 0.0000 33.278 0.10077 0.30730E-01 +0.60000E-01 12.881 0.86262 0.19967 +0.60000E-01 15.391 1.1008 +0.60000E-01 18.122 0.94801 0.10358 +0.60000E-01 20.664 0.40783 0.56939E-01 +0.60000E-01 23.077 0.39885 0.15909 +0.60000E-01 25.705 0.32418 0.57881E-01 +0.60000E-01 28.031 0.17173 0.20518E-01 +0.60000E-01 30.868 0.14121 0.22494E-01 +0.60000E-01 33.286 0.11882 0.31877E-01 +0.35200 12.805 0.99078 0.66420E-01 +0.35200 15.430 0.81426 +0.35200 17.953 0.51288 0.39885E-01 +0.35200 20.581 0.30140 0.20205E-01 +0.35200 22.995 0.25643 0.22661E-01 +0.35200 25.619 0.22852 0.29612E-01 +0.35200 27.941 0.71084E-010.15969E-01 +0.35200 30.771 0.78915E-010.19127E-01 +0.35200 33.085 0.47458E-010.80171E-02 +0.68800 12.831 0.40782 0.11739 +0.68800 15.553 0.46452 0.60871E-01 +0.68800 17.971 0.40415 0.44642E-01 +0.68800 20.426 0.14446 0.31481E-01 +0.68800 22.939 0.15884 0.99424E-01 +0.68800 25.666 0.15907 0.24043E-01 +0.68800 27.914 0.53619E-010.91575E-02 +0.68800 30.952 0.57610E-010.13082E-01 +0.68800 33.158 0.53764E-010.97036E-02 +0.76700 12.995 0.73020 0.10260 +0.76700 15.635 0.61348 0.41407E-01 +0.76700 18.175 0.35093 0.31228E-01 +0.76700 20.715 0.21278 0.23398E-01 +0.76700 23.140 0.22829 0.47435E-01 +0.76700 25.991 0.18308 0.25723E-01 +0.76700 28.114 0.82957E-010.12481E-01 +0.76700 30.855 0.90053E-010.10829E-01 +0.76700 33.398 0.44276E-010.79546E-02 +ENDDATA 47 +ENDSUBENT 61 +SUBENT F0088009 20050503 20050831 F021 +BIB 3 5 +REACTION (60-ND-148(T,A)59-PR-147,PAR,DA) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR1) Error from the graphic bars +STATUS (CURVE)Fig.9 +ENDBIB 5 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.1 0.1 +ENDCOMMON 3 +DATA 6 29 +EN E-EXC-MIN E-EXC-MAX ANG-CM DATA-CM DATA-ERR1 +MEV MEV MEV ADEG MB/SR MB/SR + 35.320 2.0000 8.6000 11.968 11.927 + 35.320 2.0000 8.6000 12.705 13.096 2.6050 + 35.320 2.0000 8.6000 14.075 13.887 + 35.320 2.0000 8.6000 15.449 12.075 + 35.320 2.0000 8.6000 17.039 7.5725 0.75541 + 35.320 2.0000 8.6000 18.095 7.2286 2.3110 + 35.320 2.0000 8.6000 19.054 3.9863 0.48040 + 35.320 2.0000 8.6000 20.538 2.5889 0.96591 + 35.320 2.0000 8.6000 22.218 4.1796 0.71219 + 35.320 2.0000 8.6000 23.064 3.6339 0.58367 + 35.320 2.0000 8.6000 24.431 4.5376 0.54675 + 35.320 2.0000 8.6000 25.802 4.7006 0.51794 + 35.320 2.0000 8.6000 27.602 3.2365 0.32286 + 35.320 2.0000 8.6000 28.028 2.4746 0.24681 + 35.320 2.0000 8.6000 29.296 2.2025 0.59551 + 35.320 2.0000 8.6000 30.354 1.8064 0.25433 + 35.320 2.0000 8.6000 32.356 2.0310 0.18109 + 35.320 2.0000 8.6000 33.199 2.1534 + 35.320 2.0000 8.6000 34.995 1.8946 0.47960 + 37.320 2.2000 8.4000 10.360 13.411 + 37.320 2.2000 8.4000 12.889 14.737 + 37.320 2.2000 8.4000 15.636 12.089 + 37.320 2.2000 8.4000 18.075 6.8203 + 37.320 2.2000 8.4000 20.407 3.9852 + 37.320 2.2000 8.4000 23.249 5.2191 + 37.320 2.2000 8.4000 25.679 4.3313 + 37.320 2.2000 8.4000 28.123 2.0031 + 37.320 2.2000 8.4000 30.762 1.8043 + 37.320 2.2000 8.4000 33.294 1.7638 +ENDDATA 31 +ENDSUBENT 45 +ENDENTRY 9 diff --git a/exforall/F00/F0089.x4 b/exforall/F00/F0089.x4 new file mode 100644 index 000000000..15f2f738c --- /dev/null +++ b/exforall/F00/F0089.x4 @@ -0,0 +1,487 @@ +ENTRY F0089 20050503 20050831 F021 +SUBENT F0089001 20050503 20050831 F021 +BIB 12 41 +TITLE The giant dipole resonance built on excited states in + 113,114Sn and level densities in the vicinity of the + neutron separation energy. +AUTHOR (A.Stolk,A.Balanda,M.N.Haraken,W.H.A.Hesselink, + J.Penninga,H.Rijneveld) +INSTITUTE (2NEDFUL) +REFERENCE (J,NP/A,505,241,1989) +FACILITY (ISOCY) +SAMPLE 5.2 mg/cm2 110Cd target, enriched to 96%, was placed + at angle of 55 degrees with respect to beam axis. + 110Cd target contained 1.6% 111Cd and 1.1% 112Cd + impurity. Contributions of these impurities to gamma + ray spectra were determined in two additional runs + using 4 mg/cm2 111Cd target and 5.2 mg/cm2 112Cd + target. +DETECTOR (NAICR) Prompt high-energy gamma-rays were detected + with large (diameter 40 cm, length 40 cm) NaI(Tl) + detector,consisting of 6 identical, optically-separated + segments and a small-diameter(8 cm)detector, used as + single-photon spectrometer. Delayed gamma-rays were + detected with three NaI(Tl) detectors, two of which had + diameters of 28 cm and lengths of 28 cm and third one + had diameter of 13 cm and length of 13 cm, placed as + close to target as possible(10 cm). + (GE) Ge detector was used for normalization of cross + section. +METHOD (GSPEC) + (TOF) +MONITOR (48-CD-112(A,2N)50-SN-114,,DE,G)Total efficiency for + detection of gamma-rays depopulating 7- isomer in 114Sn + was checked. + Detector response function was determined at number of + gamma-ray energies using 11B(P,G) and 12C(P,G) + reactions at Ep=7.24 and 14.24 MeV. + Absolute normalization of spectra was made using cross + section for 2+ to 0+ transition in 112 Sn. +CORRECTION Spectra were corrected for contrbution of target + impurities. +ERR-ANALYS (E-ERR-DIG) Digitizing error + (ERR-DIG) Digitizing error +HISTORY (20041004C) +ENDBIB 41 +COMMON 3 3 +EN-RSL E-ERR-DIG ERR-DIG +PER-CENT MEV PER-CENT + 7.1 0.02 0.1 +ENDCOMMON 3 +ENDSUBENT 48 +SUBENT F0089002 20050503 20050831 F021 +BIB 2 2 +REACTION (48-CD-110(A,N)50-SN-113,,DE,G) +STATUS (CURVE)Fig.5,7 +ENDBIB 2 +NOCOMMON 0 0 +DATA 3 249 +EN E DATA +MEV MEV MB/MEV + 24.000 5.0556 1.7489 + 24.000 5.1614 1.9697 + 24.000 5.2791 2.3361 + 24.000 5.3848 2.6310 + 24.000 5.4911 2.9254 + 24.000 5.6158 2.8625 + 24.000 5.7215 3.2239 + 24.000 5.8467 3.1144 + 24.000 5.9681 3.3337 + 24.000 6.0615 3.6113 + 24.000 6.1957 3.9676 + 24.000 6.3166 4.3018 + 24.000 6.4394 4.4309 + 24.000 6.5476 4.6804 + 24.000 6.6732 4.4639 + 24.000 6.7850 4.2555 + 24.000 6.8675 4.2667 + 24.000 6.9230 4.2197 + 24.000 7.0073 4.0192 + 24.000 7.1357 3.5495 + 24.000 7.2476 3.3838 + 24.000 7.3334 3.1015 + 24.000 7.3884 3.1069 + 24.000 7.4907 2.6379 + 24.000 7.5727 2.6790 + 24.000 7.7186 2.1362 + 24.000 7.8442 2.0374 + 24.000 7.9589 1.7985 + 24.000 8.0721 1.6498 + 24.000 8.1835 1.5931 + 24.000 8.3147 1.3028 + 24.000 8.4574 1.1363 + 24.000 8.5550 1.0968 + 24.000 8.6706 0.94369 + 24.000 8.7825 0.89965 + 24.000 8.9032 0.67223 + 24.000 9.0251 0.71039 + 24.000 9.1104 0.65951 + 24.000 9.2511 0.60554 + 24.000 9.3658 0.53453 + 24.000 9.4861 0.40457 + 24.000 9.5856 0.37097 + 24.000 9.7410 0.33213 + 24.000 9.8652 0.32919 + 24.000 9.9692 0.18300 + 24.000 10.077 0.28776 + 24.000 10.188 0.27787 + 24.000 10.317 0.16484 + 24.000 10.432 0.10028 + 24.000 10.561 0.18409 + 24.000 10.669 0.19696 + 24.000 10.760 0.15281 + 24.000 10.903 0.13329 + 24.000 11.022 0.15212 + 24.000 11.151 0.13263 + 24.000 11.267 0.76653E-01 + 24.000 11.396 0.66832E-01 + 24.000 11.491 0.70564E-01 + 24.000 11.624 0.36823E-01 + 24.000 11.737 0.72968E-01 + 24.000 11.857 0.55939E-01 + 24.000 11.950 0.60597E-01 + 24.000 12.092 0.79701E-01 + 24.000 12.220 0.47891E-01 + 24.000 12.313 0.53226E-01 + 24.000 12.396 0.52686E-01 + 24.000 12.464 0.25079E-01 + 24.000 12.578 0.32957E-01 + 24.000 12.697 0.17637E-01 + 24.000 12.818 0.27746E-01 + 24.000 12.940 0.10024E-02 + 24.000 13.054 0.58391E-02 + 24.000 13.168 0.16364E-01 + 24.000 13.252 0.33240E-01 + 24.000 13.411 0.39984E-01 + 24.000 13.518 0.20060E-01 + 24.000 13.622 0.16390E-01 + 24.000 13.739 0.94725E-02 + 24.000 13.871 0.34952E-02 + 24.000 13.955 0.15141E-01 + 24.000 14.082 0.13895E-01 + 24.000 14.201 0.11561E-02 + 24.000 14.312 0.15511E-01 + 24.000 14.433 0.16817E-01 + 24.000 14.554 0.58924E-02 + 24.000 14.663 0.27946E-01 + 24.000 14.788 0.18606E-01 + 24.000 14.908 0.10007E-02 + 24.000 15.018 0.13951E-01 + 24.000 15.134 0.11851E-01 + 24.000 15.363 0.98947E-03 + 24.000 15.610 0.99727E-03 + 24.000 15.858 0.99233E-03 + 24.000 16.147 0.98871E-03 + 24.000 16.313 0.92758E-02 + 24.000 16.450 0.98552E-03 + 24.000 16.547 0.93449E-02 + 24.000 16.560 0.98897E-03 + 24.000 16.767 0.92904E-02 + 24.000 16.874 0.69389E-02 + 24.000 17.014 0.99053E-03 + 24.000 17.121 0.10546E-01 + 24.000 17.241 0.11731E-01 + 24.000 17.370 0.69590E-02 + 24.000 17.496 0.99296E-03 + 24.000 17.675 0.99861E-03 + 24.000 17.813 0.99020E-03 + 24.000 17.946 0.34539E-02 + 24.000 18.084 0.34248E-02 + 24.000 18.198 0.10024E-02 + 24.000 18.289 0.11430E-02 + 24.000 18.446 0.98469E-03 + 24.000 18.583 0.98900E-03 + 24.000 18.790 0.99549E-03 + 24.000 18.993 0.22784E-02 + 24.000 19.148 0.99402E-03 + 24.000 19.354 0.98780E-03 + 24.000 19.473 0.11419E-02 + 24.000 19.602 0.99559E-03 + 24.000 19.740 0.98720E-03 + 24.000 19.831 0.11257E-02 + 24.000 19.927 0.11291E-02 + 24.000 20.042 0.99673E-03 + 26.000 5.0622 1.8270 + 26.000 5.1598 2.6014 + 26.000 5.2647 2.6941 + 26.000 5.3864 3.4347 + 26.000 5.5040 3.5131 + 26.000 5.6248 4.2647 + 26.000 5.7433 4.5809 + 26.000 5.8591 4.2485 + 26.000 5.9656 4.7935 + 26.000 6.0830 4.8432 + 26.000 6.2015 5.2023 + 26.000 6.3160 4.4833 + 26.000 6.4354 5.0572 + 26.000 6.5634 4.4653 + 26.000 6.6415 4.4596 + 26.000 6.7820 3.8416 + 26.000 6.9124 3.8807 + 26.000 7.0152 3.5998 + 26.000 7.0895 2.9200 + 26.000 7.1544 2.8814 + 26.000 7.2449 2.7735 + 26.000 7.3603 2.5100 + 26.000 7.4752 2.2167 + 26.000 7.5771 1.9580 + 26.000 7.6925 1.7721 + 26.000 7.8348 1.6835 + 26.000 7.9363 1.4511 + 26.000 8.0519 1.3294 + 26.000 8.1810 1.2479 + 26.000 8.3221 1.1152 + 26.000 8.4254 1.0601 + 26.000 8.5522 0.88045 + 26.000 8.6712 0.96916 + 26.000 8.7886 0.97922 + 26.000 8.9204 0.52339 + 26.000 9.0117 0.52905 + 26.000 9.1024 0.51550 + 26.000 9.2450 0.49576 + 26.000 9.3613 0.47118 + 26.000 9.5006 0.38179 + 26.000 9.6199 0.42543 + 26.000 9.7218 0.37579 + 26.000 9.8353 0.30838 + 26.000 9.9658 0.31152 + 26.000 10.081 0.27850 + 26.000 10.208 0.23996 + 26.000 10.324 0.21452 + 26.000 10.426 0.19900 + 26.000 10.560 0.23282 + 26.000 10.670 0.15902 + 26.000 10.787 0.16067 + 26.000 10.899 0.11955 + 26.000 11.031 0.12997 + 26.000 11.151 0.15778 + 26.000 11.254 0.14636 + 26.000 11.387 0.84188E-01 + 26.000 11.513 0.13215 + 26.000 11.633 0.76030E-01 + 26.000 11.744 0.10957 + 26.000 11.867 0.36338E-01 + 26.000 11.986 0.41495E-01 + 26.000 12.087 0.70126E-01 + 26.000 12.212 0.52169E-01 + 26.000 12.318 0.57437E-01 + 26.000 12.449 0.59459E-01 + 26.000 12.562 0.46462E-01 + 26.000 12.670 0.57813E-01 + 26.000 12.799 0.12958E-01 + 26.000 12.894 0.67539E-01 + 26.000 13.016 0.42854E-01 + 26.000 13.155 0.96162E-03 + 26.000 13.254 0.12706E-01 + 26.000 13.363 0.66211E-01 + 26.000 13.474 0.11909E-01 + 26.000 13.604 0.58428E-02 + 26.000 13.709 0.24728E-01 + 26.000 13.828 0.27219E-01 + 26.000 13.948 0.15853E-01 + 26.000 14.092 0.97055E-03 + 26.000 14.209 0.95692E-03 + 26.000 14.315 0.35351E-01 + 26.000 14.431 0.16722E-01 + 26.000 14.534 0.15703E-01 + 26.000 14.658 0.10855E-01 + 26.000 14.774 0.20728E-01 + 26.000 14.890 0.96859E-02 + 26.000 15.043 0.96743E-03 + 26.000 15.134 0.96600E-03 + 26.000 15.248 0.13566E-01 + 26.000 15.251 0.96416E-03 + 26.000 15.483 0.68093E-02 + 26.000 15.616 0.97026E-03 + 26.000 15.727 0.11622E-01 + 26.000 15.844 0.28386E-02 + 26.000 15.956 0.87377E-02 + 26.000 16.085 0.96290E-03 + 26.000 16.188 0.77019E-02 + 26.000 16.320 0.97105E-03 + 26.000 16.416 0.10679E-01 + 26.000 16.556 0.88674E-02 + 26.000 16.665 0.29057E-02 + 26.000 16.801 0.96347E-03 + 26.000 16.912 0.28241E-02 + 26.000 17.062 0.97121E-03 + 26.000 17.192 0.96916E-03 + 26.000 17.365 0.48630E-02 + 26.000 17.505 0.97612E-03 + 26.000 17.596 0.97468E-03 + 26.000 17.717 0.48353E-02 + 26.000 17.843 0.97076E-03 + 26.000 17.935 0.96933E-03 + 26.000 17.951 0.48169E-02 + 26.000 18.181 0.38031E-02 + 26.000 18.443 0.97319E-03 + 26.000 18.612 0.97052E-03 + 26.000 18.781 0.96785E-03 + 26.000 18.950 0.96519E-03 + 26.000 19.120 0.97439E-03 + 26.000 19.236 0.18836E-02 + 26.000 19.380 0.97028E-03 + 26.000 19.485 0.98056E-03 + 26.000 19.601 0.19188E-02 + 26.000 19.732 0.97662E-03 + 26.000 19.836 0.97497E-03 + 26.000 19.947 0.28930E-02 + 26.000 20.045 0.98364E-03 +ENDDATA 251 +ENDSUBENT 258 +SUBENT F0089003 20050503 20050831 F021 +BIB 3 3 +REACTION (48-CD-110(A,G)50-SN-114,,DE) +ERR-ANALYS (DATA-ERR) Error from the graphic bars +STATUS (CURVE)Fig.6,8 +ENDBIB 3 +NOCOMMON 0 0 +DATA 5 163 +EN E E-ERR-DIG DATA DATA-ERR +MEV MEV MEV MU-B/MEV MU-B/MEV + 24.000 8.1116 0.87586E-01 26.730 6.6220 + 24.000 8.4679 0.10942 14.580 5.7308 + 24.000 8.8149 0.98505E-01 12.558 4.7863 + 24.000 9.1687 0.87586E-01 3.6365 4.1176 + 24.000 9.5090 0.98505E-01 16.417 3.6726 + 24.000 9.8520 0.10942 18.012 3.2832 + 24.000 10.218 0.10942 14.156 2.6701 + 24.000 10.557 0.10966 19.146 2.1150 + 24.000 10.914 0.98505E-01 14.732 1.7244 + 24.000 11.267 0.98274E-01 21.893 1.6688 + 24.000 11.491 20.471 2.7825 + 24.000 11.603 27.717 2.7825 + 24.000 11.737 13.819 2.5044 + 24.000 11.850 21.010 2.6145 + 24.000 11.974 17.350 2.4476 + 24.000 12.082 20.312 2.3931 + 24.000 12.202 20.213 2.3375 + 24.000 12.309 20.781 2.1706 + 24.000 12.423 22.407 2.2263 + 24.000 12.554 19.695 2.1138 + 24.000 12.675 19.429 1.8357 + 24.000 12.785 22.057 2.1695 + 24.000 12.904 24.852 2.1138 + 24.000 13.032 17.687 1.8357 + 24.000 13.149 18.423 2.1138 + 24.000 13.264 14.373 1.7812 + 24.000 13.394 12.105 1.8913 + 24.000 13.493 14.509 1.7244 + 24.000 13.615 16.803 1.8369 + 24.000 13.740 15.537 1.7801 + 24.000 13.860 13.045 1.5019 + 24.000 13.982 7.2152 1.4463 + 24.000 14.088 13.404 1.4475 + 24.000 14.211 10.078 1.3907 + 24.000 14.334 9.3122 1.3350 + 24.000 14.444 6.4302 1.3362 + 24.000 14.574 6.8336 1.1125 + 24.000 14.689 8.0147 1.4475 + 24.000 14.806 6.2464 1.0013 + 24.000 14.922 7.0937 1.0569 + 24.000 15.039 5.2142 1.1125 + 24.000 15.156 3.5571 0.77878 + 24.000 15.271 4.5713 0.77878 + 24.000 15.374 6.0850 1.0013 + 24.000 15.499 5.0966 0.72315 + 24.000 15.610 4.6634 0.66752 + 24.000 15.730 2.0050 0.72315 + 24.000 15.840 4.5212 0.61190 + 24.000 15.954 3.2535 0.77995 + 24.000 16.079 4.8251 0.66752 + 24.000 16.198 4.9493 0.61190 + 24.000 16.317 2.6804 0.72315 + 24.000 16.437 2.7489 0.50064 + 24.000 16.553 1.0919 0.66870 + 24.000 16.674 0.93789 0.55627 + 24.000 16.784 0.78276 0.61190 + 24.000 16.902 1.1851 0.55627 + 24.000 17.017 2.5330 0.66752 + 24.000 17.135 0.31971 0.50182 + 24.000 17.245 0.10895 + 24.000 17.363 0.62252 + 24.000 17.491 1.4710 + 24.000 17.590 1.2591 + 24.000 17.712 0.77137 0.33494 + 24.000 17.846 0.22920 + 24.000 17.950 1.3535 0.44502 + 24.000 18.064 0.36395 + 24.000 18.183 0.48812 + 24.000 18.303 0.66793 + 24.000 18.422 0.90336 + 24.000 18.534 0.30321 + 24.000 18.653 0.42739 + 24.000 18.782 1.1090 + 24.000 18.893 0.62011 + 24.000 19.005 0.19966E-01 + 24.000 19.131 1.0910 + 24.000 19.244 0.26832 + 24.000 19.365 0.11436 + 24.000 19.474 0.70484E-01 + 24.000 19.603 0.69648 + 24.000 19.710 1.1532 + 24.000 19.833 0.55427 + 24.000 19.955 0.66550E-01 + 26.000 8.7954 0.10945 33.132 5.8222 + 26.000 9.4923 0.10945 28.271 4.5331 + 26.000 9.8577 0.10978 23.068 4.0300 + 26.000 10.214 0.10945 18.203 3.2457 + 26.000 10.574 0.98474E-01 15.911 2.7985 + 26.000 10.924 0.98799E-01 15.522 2.2954 + 26.000 11.261 0.10945 20.563 2.0701 + 26.000 11.520 10.285 3.0204 + 26.000 11.625 17.039 2.9662 + 26.000 11.749 13.832 3.0780 + 26.000 11.856 19.019 2.7985 + 26.000 11.974 22.414 2.7985 + 26.000 12.096 15.010 2.6867 + 26.000 12.215 14.601 2.8544 + 26.000 12.330 13.688 2.7968 + 26.000 12.446 16.636 2.3496 + 26.000 12.560 19.249 2.7426 + 26.000 12.693 15.648 2.5749 + 26.000 12.794 21.564 2.3513 + 26.000 12.912 15.391 2.3496 + 26.000 13.049 14.419 2.3513 + 26.000 13.150 22.349 1.9040 + 26.000 13.256 17.913 1.9583 + 26.000 13.389 12.466 2.0158 + 26.000 13.497 15.975 2.1276 + 26.000 13.610 16.517 2.0142 + 26.000 13.737 13.756 2.0701 + 26.000 13.850 14.243 1.7906 + 26.000 13.968 13.833 1.7906 + 26.000 14.068 17.791 1.7906 + 26.000 14.190 17.885 1.8465 + 26.000 14.319 9.9200 1.8465 + 26.000 14.428 9.7917 1.4535 + 26.000 14.546 9.2704 1.4551 + 26.000 14.675 6.8451 1.1756 + 26.000 14.783 8.4514 1.2874 + 26.000 14.904 8.4891 1.3992 + 26.000 15.019 11.158 1.1740 + 26.000 15.144 8.1733 1.0638 + 26.000 15.252 5.8631 1.0622 + 26.000 15.377 6.6276 0.78430 + 26.000 15.505 4.0346 0.78430 + 26.000 15.606 8.2717 1.0063 + 26.000 15.741 3.1597 0.84021 + 26.000 15.840 5.1031 0.55904 + 26.000 15.971 3.0691 0.72840 + 26.000 16.078 4.3959 0.78265 + 26.000 16.208 4.0407 0.67249 + 26.000 16.322 4.8069 0.61659 + 26.000 16.442 2.7186 0.67084 + 26.000 16.563 2.7005 0.56069 + 26.000 16.676 1.3965 0.78265 + 26.000 16.785 3.2265 0.78430 + 26.000 16.915 2.8153 0.72675 + 26.000 17.029 3.4697 0.72675 + 26.000 17.139 1.6626 0.72675 + 26.000 17.255 2.7642 0.61494 + 26.000 17.376 0.89953 0.50313 + 26.000 17.489 1.3303 0.56069 + 26.000 17.610 1.4239 0.33707 + 26.000 17.726 0.56719 + 26.000 17.853 1.7230 0.56069 + 26.000 17.965 0.13954 + 26.000 18.087 0.34500 + 26.000 18.214 1.3890 0.39133 + 26.000 18.308 0.59150 + 26.000 18.430 0.74105 + 26.000 18.547 0.10795 + 26.000 18.660 0.59458 + 26.000 18.790 0.29525 + 26.000 18.915 1.0038 + 26.000 19.026 1.2109 + 26.000 19.141 0.24242 + 26.000 19.254 0.67314 + 26.000 19.376 0.93450 + 26.000 19.498 1.0841 + 26.000 19.613 0.17143 + 26.000 19.724 0.37854 + 26.000 19.834 0.25023 + 26.000 19.955 0.28797 +ENDDATA 165 +ENDSUBENT 173 +ENDENTRY 3 diff --git a/exforall/F01/F0145.x4 b/exforall/F01/F0145.x4 new file mode 100644 index 000000000..b51d0083c --- /dev/null +++ b/exforall/F01/F0145.x4 @@ -0,0 +1,94 @@ +ENTRY F0145 20050517 20050831 F022 +SUBENT F0145001 20050517 20050831 F022 +BIB 12 36 +TITLE The polarization of protons from the 2H(d,p)3H reaction + for deutron energies below 1 MeV. +AUTHOR (P.Kozma,P.Bem) +INSTITUTE (3CZRUJF) +REFERENCE (J,NP/A,442,17,1985) +FACILITY (VDG) +INC-SOURCE Magnetically-analyzed deuteron beam. The mean reaction + energy calculated from the energy loss of the deuterons + on appropriate foils of a sandwich target was taken to + be Ed0-1/2DeltaEd0, Ed0 being the energy of deuterons + which passed the first gold foil of the target block + and DeltaEd the energy the energy thickness of the + (CD2)n foil. For measurements covering the range of + mean energies of 1200 t0 300 keV the DeltaEd thickness + of the target ranged from 30 to 90 keV. +SAMPLE Target consisted of a deuterated-polyethylene (CD2)n + foil of thickness 0.5 mg/cm2 sandwiched between two + gold layers. Thickness and homogenity of targets were + determined with an accuracy of 0.01 mg/cm2. +DETECTOR (SI) Polarimeter consisted of two silicon + detectors as a target and two silicon detectors for the + detection of protons scattered to the left and right at + 95 degrees lab. angle. The analyzing power of the + polarimeter was determined to an accuracy of 3%. + The average detection efficiency of the polarimeter + was 2.5*10-6. +METHOD (DSCAT) +CORRECTION The correction of measured asymmetry data for a + nonsymmetrical arrangment of the two "left" and "right" + scattering planes in the present polarimeter was + calculated to be less than 1% in the whole range of + reaction angles. +ERR-ANALYS (DATA-ERR) Errors correspond to the statistical + uncertainty and to errors in the background + subtraction. +HISTORY (20050201C) +ENDBIB 36 +NOCOMMON 0 0 +ENDSUBENT 39 +SUBENT F0145002 20050517 20050831 F022 +BIB 2 2 +REACTION (1-H-2(D,P)1-H-3,,POL/DA) +STATUS (TABLE) Table 1 +ENDBIB 2 +COMMON 1 3 +EN-MEAN +KEV + 975. +ENDCOMMON 3 +DATA 3 7 +ANG DATA DATA-ERR +ADEG NO-DIM NO-DIM + 15.000 -.64000E-010.29000E-01 + 30.000 -.12200 0.24000E-01 + 45.000 -.14700 0.17000E-01 + 60.000 -.10600 0.18000E-01 + 70.000 -.31000E-010.17000E-01 + 80.000 0.40000E-020.16000E-01 + 85.000 0.35000E-010.25000E-01 +ENDDATA 9 +ENDSUBENT 20 +SUBENT F0145003 20050517 20050831 F022 +BIB 2 2 +REACTION (1-H-2(D,P)1-H-3,,POL/DA) +STATUS (TABLE) Table 2 +ENDBIB 2 +COMMON 1 3 +ANG +ADEG + 45. +ENDCOMMON 3 +DATA 3 14 +EN-MEAN DATA DATA-ERR +KEV NO-DIM NO-DIM + 250.00 -.65000E-010.38000E-01 + 312.00 -.96000E-010.31000E-01 + 377.00 -.11900 0.19000E-01 + 455.00 -.11500 0.18000E-01 + 509.00 -.14400 0.18000E-01 + 564.00 -.14200 0.17000E-01 + 620.00 -.14300 0.17000E-01 + 676.00 -.15300 0.18000E-01 + 743.00 -.14700 0.19000E-01 + 798.00 -.15100 0.18000E-01 + 860.00 -.14100 0.19000E-01 + 906.00 -.14600 0.20000E-01 + 962.00 -.13800 0.18000E-01 + 975.00 -.14700 0.17000E-01 +ENDDATA 16 +ENDSUBENT 27 +ENDENTRY 3 diff --git a/exforall/F01/F0157.x4 b/exforall/F01/F0157.x4 new file mode 100644 index 000000000..d8552109a --- /dev/null +++ b/exforall/F01/F0157.x4 @@ -0,0 +1,539 @@ +ENTRY F0157 20050503 20050831 F021 +SUBENT F0157001 20050503 20050831 F021 +BIB 11 36 +TITLE Spectroscopic information on 36Cl from the (d,p) + reaction. +AUTHOR (S.Piskor,P.Franc,W.Schaferlingova,J.Kremenek) +INSTITUTE (3CZRUJF) +REFERENCE (J,NP/A,481,269,1988) +FACILITY (CYCLO) +DETECTOR (MAGSP) The multi-angle magnetic spectrograph, giving + in a single run eleven spectra in the range from 0-90 + degrees reaction angle, was used for the momentum + analysis of the protons. + (PLATE)The detection of protons was accomplished by + means of 700 mm long nuclear emulsion plates + Ilford L4,located in the focal planes of the + spectrograph channels. +SAMPLE Chlorine targets of natural abundance were used,i.e. + containing 75.77% of 35Cl and 24.33% of 37Cl, + consisting of 50 mu-g/cm2 thick layers of CdCl2 + evaporated on 10 mu-g/cm2 carbon backing. +MONITOR The target thickness and therefore the absolute cross + section was calibrated at angle 21 degr. by putting + the deuteron elastic scattering cross section equal + to 0.78 *sigmaR. +COMMENT Targets used in the experiments contained some amount + of admixtures,namely H,C,N,O,Na,Si,S,Cd and 37Cl. To + facilitate the analysis of the complex proton spectra + eleven additional spectra from (d,p)reaction on 100 + mu-g/cm2 SiO2 target,taken with the same experimental + set-up were processed. These additional spectra, + along with kinematical shifts of spectral lines with + reaction angle,cross-checked the correct + identification of spectral lines. +ERR-ANALYS (DATA-ERR) Accuracy of absolute cross section + normalisation. + The level energies of some states were measured with + a precision of 70-80 eV. +HISTORY (20041207C) +ENDBIB 36 +COMMON 3 3 +EN ANG-NRM DATA-ERR +MEV ADEG PER-CENT + 12.3 21. 10. +ENDCOMMON 3 +ENDSUBENT 43 +SUBENT F0157002 20050503 20050831 F021 +BIB 3 5 +REACTION (17-CL-35(D,P)17-CL-36,PAR,DA) +ERR-ANALYS (ANG-ERR-D)Digitizing error + (ERR-DIG)Digitizing error + (DATA-ERR1)Error from the graphic bars +STATUS (CURVE)Fig.4 +ENDBIB 5 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.5 0.2 +ENDCOMMON 3 +DATA 4 394 +E-LVL ANG-CM DATA-CM DATA-ERR1 +KEV ADEG MB/SR MB/SR + 0.0000 2.4239 1.4501 0.12350 + 0.0000 6.6071 1.2016 0.10777 + 0.0000 8.9416 1.2814 0.12641 + 0.0000 12.833 1.0831 0.11645 + 0.0000 17.988 1.2752 0.15386 + 0.0000 22.074 1.2502 0.13442 + 0.0000 24.797 1.3939 0.13128 + 0.0000 36.666 0.59840 0.78753E-01 + 0.0000 43.866 0.27258 0.89067E-01 + 0.0000 52.039 0.10919 0.29229E-01 + 788.25 13.117 0.30910 0.97029E-01 + 788.25 17.233 0.48770 0.83735E-01 + 788.25 20.869 0.58878 0.88851E-01 + 788.25 24.793 0.56030 0.57890E-01 + 788.25 31.586 0.35863 0.60098E-01 + 788.25 35.701 0.29412 0.61128E-01 + 788.25 50.817 0.51622E-010.17750E-01 + 1165.1 1.4493 2.7235 0.13815 + 1165.1 5.2055 1.9742 0.15210 + 1165.1 9.8271 1.1916 0.66653E-01 + 1165.1 13.392 0.97747 0.96354E-01 + 1165.1 16.850 0.36691 0.49046E-01 + 1165.1 20.898 0.32417 0.55565E-01 + 1165.1 35.836 0.16694 0.45914E-01 + 1601.4 1.1386 1.7284 0.43405 + 1601.4 5.2579 1.3880 0.34338 + 1601.4 10.359 0.91770 0.19533 + 1601.4 30.274 0.16191 0.97866E-01 + 1601.4 35.962 0.11887 0.69935E-01 + 1951.2 4.7716 0.77216 0.18377 + 1951.2 10.661 1.0388 0.15416 + 1951.2 14.136 1.3432 0.15427 + 1951.2 16.744 1.2289 0.12114 + 1951.2 20.511 1.1468 0.10669 + 1951.2 35.481 0.89592 0.10020 + 1951.2 47.553 0.72452 0.84205E-01 + 1951.2 57.506 0.22022 0.78367E-01 + 1959.2 4.4660 2.9091 0.20844 + 1959.2 10.485 1.1716 0.13106 + 1959.2 14.272 0.54186 0.13707 + 1959.2 16.505 0.24329 0.99220E-01 + 1959.2 20.194 0.88758E-010.58691E-01 + 1959.2 35.437 0.22591 0.98581E-01 + 1959.2 47.476 0.19949E-010.50758E-01 + 2467.9 2.9373 2.3339 0.13005 + 2467.9 11.364 3.3621 0.18734 + 2467.9 15.046 3.3458 0.13458 + 2467.9 16.015 3.1850 0.21079 + 2467.9 20.087 2.7071 0.17916 + 2467.9 27.068 1.7460 0.11555 + 2467.9 35.112 1.5439 0.17226 + 2467.9 46.844 0.71578 0.15911 + 2467.9 60.998 0.35209 0.97784E-01 + 2492.3 4.4022 0.91510 0.10233 + 2492.3 11.150 0.52116 0.62725E-01 + 2492.3 15.107 0.28527 0.68956E-01 + 2492.3 15.979 0.20488 0.66213E-01 + 2492.3 19.932 0.14076 0.62963E-01 + 2492.3 27.056 0.12756 0.51258E-01 + 2492.3 34.947 0.13474 0.57266E-01 + 2492.3 46.901 0.48238E-010.37174E-01 + 2518.5 4.3244 0.60826 0.88686E-01 + 2518.5 11.268 1.0250 0.10071 + 2518.5 15.606 1.1422 0.87574E-01 + 2518.5 19.849 1.3704 0.12855 + 2518.5 26.985 2.2868 0.15236 + 2518.5 35.083 2.7299 0.19440 + 2518.5 46.642 1.0974 0.88136E-01 + 2518.5 60.996 0.40371 0.91208E-01 + 2810.9 15.995 0.56866 0.80920E-01 + 2810.9 20.190 0.67628 0.89120E-01 + 2810.9 28.091 1.0560 0.10418 + 2810.9 35.409 0.99515 0.10905 + 2810.9 47.215 0.40815 0.61530E-01 + 2810.9 59.119 0.13869 0.60213E-01 + 2863.6 5.2496 0.29218 0.76033E-01 + 2863.6 12.434 0.29362 0.70974E-01 + 2863.6 16.027 0.35955 0.48000E-01 + 2863.6 20.007 0.36491 0.59465E-01 + 2863.6 27.774 0.31618 0.57983E-01 + 2863.6 34.958 0.21718 0.44859E-01 + 2863.6 46.704 0.14129 0.58018E-01 + 2896.4 4.6935 4.0127 0.22513 + 2896.4 12.694 5.7358 0.26198 + 2896.4 16.304 5.1170 0.28709 + 2896.4 20.498 3.8562 0.21635 + 2896.4 27.813 1.2878 0.12168 + 2896.4 35.130 0.91893 0.95882E-01 + 2896.4 47.129 0.85296 0.98394E-01 + 2896.4 59.713 0.31301 0.60146E-01 + 2896.4 65.469 0.28483 0.21741E-01 + 2994.9 4.0109 2.5486 0.15568 + 2994.9 12.251 3.3777 0.20633 + 2994.9 15.935 3.0448 0.12277 + 2994.9 19.619 2.4258 0.13550 + 2994.9 27.472 0.75956 0.74764E-01 + 2994.9 34.550 0.41160 0.60196E-01 + 2994.9 46.377 0.48932 0.72605E-01 + 2994.9 59.078 0.18670 0.47212E-01 + 3099.8 3.3737 0.36377E-010.19297E-01 + 3099.8 19.540 0.25749 0.53362E-01 + 3099.8 27.968 0.34471 0.53307E-01 + 3099.8 34.944 0.39591 0.61226E-01 + 3099.8 46.382 0.23688 0.51765E-01 + 3099.8 59.087 0.59399E-010.19983E-01 + 3207.4 0.80846 1.3797 0.11375 + 3207.4 3.8963 1.5314 0.12626 + 3207.4 12.485 2.0325 0.12443 + 3207.4 15.867 1.9834 0.16353 + 3207.4 16.351 1.9254 0.15875 + 3207.4 19.743 1.4962 0.99481E-01 + 3207.4 34.682 0.29532 0.10806 + 3207.4 46.381 0.24014 0.60837E-01 + 3207.4 59.160 0.12081 0.60409E-01 + 3332.3 1.1972 3.9895 0.20186 + 3332.3 3.9951 5.3910 0.27277 + 3332.3 12.772 7.2842 0.33088 + 3332.3 16.146 6.7308 0.34056 + 3332.3 16.725 6.3751 0.28958 + 3332.3 19.713 5.3634 0.21602 + 3332.3 28.290 1.4146 0.13143 + 3332.3 34.652 0.86343 0.80223E-01 + 3332.3 46.223 0.80965 0.84005E-01 + 3332.3 59.335 0.38230 0.87998E-01 + 3332.3 65.022 0.23450 0.59247E-01 + 3635.0 1.0240 1.2463 0.12279 + 3635.0 3.2517 1.3760 0.10596 + 3635.0 12.843 1.6857 0.11194 + 3635.0 15.362 1.6447 0.10921 + 3635.0 16.719 1.5888 0.14792 + 3635.0 19.144 1.2909 0.13421 + 3635.0 28.364 0.29870 0.74453E-01 + 3635.0 33.986 0.23678 0.45360E-01 + 3635.0 45.905 0.24159 0.51051E-01 + 3635.0 59.191 0.77487E-010.47948E-01 + 3635.0 64.231 0.73758E-010.43773E-01 + 3723.4 17.255 0.18595 0.60929E-01 + 3723.4 19.216 0.17607 0.57104E-01 + 3723.4 29.215 0.30242 0.58111E-01 + 3723.4 34.608 0.38951 0.48844E-01 + 3723.4 46.176 0.16263 0.52745E-01 + 3723.4 60.294 0.59390E-010.39555E-01 + 3962.6 1.0617 2.3208 0.13032 + 3962.6 2.4168 2.0806 0.95107E-01 + 3962.6 12.781 2.3786 0.13356 + 3962.6 14.330 2.1218 0.16208 + 3962.6 16.557 1.9891 0.13266 + 3962.6 18.009 1.7831 0.11892 + 3962.6 28.361 0.39784 0.12911 + 3962.6 45.018 0.31181 0.10737 + 3962.6 60.408 0.90059E-010.50570E-01 + 3992.1 1.1413 2.9251 0.14833 + 3992.1 2.1063 3.1816 0.15355 + 3992.1 12.712 4.1542 0.21065 + 3992.1 14.157 3.8001 0.19270 + 3992.1 16.661 3.3248 0.18592 + 3992.1 18.010 3.1641 0.19350 + 3992.1 28.399 0.69278 0.72040E-01 + 3992.1 44.878 0.54875 0.69169E-01 + 3992.1 48.538 0.47535 0.65239E-01 + 3992.1 60.379 0.16324 0.40713E-01 + 3992.1 63.464 0.16326 0.50589E-01 + 4032.0 1.3758 2.9170 0.13265 + 4032.0 2.5304 3.0196 0.20033 + 4032.0 13.016 3.0642 0.18718 + 4032.0 14.556 3.1407 0.14282 + 4032.0 17.056 2.8733 0.14554 + 4032.0 18.306 2.3464 0.11885 + 4032.0 28.974 0.52754 0.78276E-01 + 4032.0 45.038 0.42225 0.60263E-01 + 4032.0 48.597 0.41601 0.81289E-01 + 4032.0 60.616 0.16267 0.39928E-01 + 4032.0 63.693 0.11229 0.41017E-01 + 4060.5 1.7606 0.36494 0.51829E-01 + 4060.5 12.872 0.36850 0.70537E-01 + 4060.5 14.224 0.36128 0.72028E-01 + 4060.5 16.736 0.34047 0.65172E-01 + 4060.5 17.991 0.27124 0.63523E-01 + 4060.5 28.612 0.79635E-010.46588E-01 + 4060.5 33.346 0.79237E-010.47940E-01 + 4060.5 44.840 0.44222E-010.35857E-01 + 4138.8 1.1703 1.1458 0.11303 + 4138.8 2.2320 1.3356 0.10998 + 4138.8 13.134 1.4890 0.12261 + 4138.8 14.196 1.4744 0.11353 + 4138.8 16.800 1.2773 0.98360E-01 + 4138.8 17.861 1.0904 0.11336 + 4138.8 28.758 0.25853 0.60593E-01 + 4138.8 33.195 0.17665 0.42070E-01 + 4138.8 44.870 0.21210 0.74845E-01 + 4138.8 64.547 0.58620E-010.38075E-01 + 4315.7 1.1484 1.3800 0.84188E-01 + 4315.7 13.287 1.5924 0.80553E-01 + 4315.7 17.237 1.3072 0.79746E-01 + 4315.7 32.847 0.20343 0.56549E-01 + 4315.7 44.503 0.23825 0.51172E-01 + 4315.7 59.438 0.69730E-010.41045E-01 + 4496.3 13.666 3.8089 0.23242 + 4496.3 17.332 3.1109 0.14131 + 4496.3 29.290 0.70746 0.88971E-01 + 4496.3 32.955 0.49338 0.67906E-01 + 4496.3 44.537 0.44034 0.41392E-01 + 4496.3 60.070 0.16896 0.58443E-01 + 4551.7 1.8010 0.51395 0.72880E-01 + 4551.7 13.740 0.30919 0.49029E-01 + 4551.7 29.434 0.16605 0.64158E-01 + 4551.7 32.803 0.14041 0.66102E-01 + 4551.7 44.354 0.25727E-010.15499E-01 + 4598.6 1.8685 3.0063 0.15211 + 4598.6 13.605 2.9625 0.11932 + 4598.6 17.453 2.5422 0.11548 + 4598.6 32.755 0.48660 0.69368E-01 + 4598.6 44.396 0.38590 0.55012E-01 + 4598.6 59.984 0.16271 0.61904E-01 + 4753.8 2.0135 0.78763 0.85130E-01 + 4753.8 13.869 0.72372 0.61970E-01 + 4753.8 17.464 0.60808 0.57572E-01 + 4753.8 30.970 0.21397 0.39469E-01 + 4753.8 43.992 0.23283 0.48529E-01 + 4956.5 14.232 1.0932 0.78477E-01 + 4956.5 17.916 0.94699 0.67979E-01 + 4956.5 31.100 0.19610 0.39171E-01 + 4956.5 44.091 0.17849 0.41201E-01 + 4997.8 2.5497 1.0791 0.79646E-01 + 4997.8 16.994 1.1216 0.11172 + 4997.8 18.256 1.0347 0.10307 + 4997.8 30.003 0.45539 0.71545E-01 + 4997.8 32.329 0.47084 0.75851E-01 + 4997.8 43.869 0.40471 0.53725E-01 + 4997.8 61.057 0.10078 0.44844E-01 + 5079.2 1.1493 0.52501 0.16223 + 5079.2 2.8134 0.50697 0.93879E-01 + 5079.2 13.092 0.52496 0.12008 + 5079.2 14.659 0.48706 0.11884 + 5079.2 18.476 0.45871 0.12384 + 5079.2 61.051 0.27004E-010.16909E-01 + 5150.4 1.1887 0.79871 0.14790 + 5150.4 2.9894 0.61295 0.93144E-01 + 5150.4 17.090 0.50957 0.12433 + 5150.4 18.990 0.50704 0.87655E-01 + 5150.4 48.195 0.79895E-010.39992E-01 + 5204.9 0.86872 2.5028 0.16604 + 5204.9 3.0150 2.6167 0.11899 + 5204.9 13.064 2.5911 0.11783 + 5204.9 14.722 2.4060 0.10941 + 5204.9 16.479 2.1582 0.87020E-01 + 5204.9 18.723 1.7887 0.99913E-01 + 5204.9 21.748 1.3233 0.60175E-01 + 5204.9 30.531 0.46195 0.68544E-01 + 5204.9 32.092 0.41642 0.86299E-01 + 5204.9 43.799 0.42476 0.81305E-01 + 5204.9 61.558 0.11244 0.41074E-01 + 5263.1 1.1523 3.0398 0.26637 + 5263.1 2.6082 2.9511 0.18028 + 5263.1 12.993 2.4831 0.16474 + 5263.1 15.031 2.4956 0.13940 + 5263.1 16.488 2.1840 0.12199 + 5263.1 18.623 2.0891 0.13860 + 5263.1 31.157 0.47695 0.53336E-01 + 5263.1 43.097 0.33428 0.51502E-01 + 5263.1 49.892 0.27168 0.69703E-01 + 5308.1 0.97957 2.9538 0.29009 + 5308.1 3.1147 2.8537 0.15905 + 5308.1 13.013 2.5356 0.18077 + 5308.1 14.857 2.4376 0.13586 + 5308.1 16.313 2.2751 0.13867 + 5308.1 18.352 1.8958 0.13548 + 5308.1 43.496 0.34953 0.79049E-01 + 5308.1 50.097 0.26133 0.69778E-01 + 5463.4 0.75898 4.3317 0.19676 + 5463.4 3.3553 4.0028 0.18182 + 5463.4 12.682 4.0427 0.20455 + 5463.4 14.990 3.3679 0.19369 + 5463.4 16.240 3.4014 0.18978 + 5463.4 18.933 2.6839 0.34644 + 5463.4 31.051 0.73287 0.68890E-01 + 5463.4 43.071 0.52395 0.71745E-01 + 5463.4 49.995 0.37457 0.60980E-01 + 5578.3 0.57655 0.81990 0.10302 + 5578.3 3.5788 0.84454 0.10612 + 5578.3 12.498 0.64711 0.86236E-01 + 5578.3 15.504 0.64712 0.91742E-01 + 5578.3 16.085 0.80792 0.92589E-01 + 5578.3 19.284 0.76527 0.87702E-01 + 5578.3 43.232 0.19914 0.47309E-01 + 5578.3 50.407 0.19239 0.11162 + 5619.2 0.57531 3.4055 0.16418 + 5619.2 3.4921 3.6314 0.16513 + 5619.2 12.942 3.3883 0.15408 + 5619.2 15.449 2.9070 0.14725 + 5619.2 16.413 2.8081 0.14224 + 5619.2 19.498 2.3738 0.15748 + 5619.2 31.353 0.64715 0.63700E-01 + 5619.2 43.020 0.46470 0.68953E-01 + 5619.2 50.637 0.30986 0.90606E-01 + 5694.4 0.57343 0.81708 0.91401E-01 + 5694.4 3.6498 1.0723 0.10559 + 5694.4 12.203 0.92903 0.11186 + 5694.4 16.046 0.69400 0.75909E-01 + 5694.4 19.121 0.56110 0.89689E-01 + 5694.4 31.226 0.17047 0.56243E-01 + 5694.4 43.047 0.15064 0.38104E-01 + 5831.9 0.57411 0.50891 0.13954 + 5831.9 4.1148 0.78925 0.18150 + 5831.9 12.249 0.56442 0.14454 + 5831.9 15.885 0.57567 0.14742 + 5831.9 19.713 0.46112 0.16671 + 5831.9 31.005 0.99019E-010.60024E-01 + 5831.9 42.488 0.89279E-010.47498E-01 + 5898.5 0.58393 3.1793 0.21316 + 5898.5 4.1539 3.1481 0.21107 + 5898.5 12.535 2.9666 0.15077 + 5898.5 16.190 2.2700 0.12722 + 5898.5 20.133 1.8435 0.13248 + 5898.5 31.678 0.54463 0.68807E-01 + 5898.5 42.834 0.33845 0.69008E-01 + 5898.5 51.201 0.24043 0.60969E-01 + 5912.0 0.55768 2.3601 0.12564 + 5912.0 4.1229 2.3484 0.14702 + 5912.0 12.460 2.2906 0.17521 + 5912.0 16.328 1.8404 0.93842E-01 + 5912.0 20.100 1.4070 0.12412 + 5912.0 31.801 0.41191 0.85685E-01 + 5912.0 42.826 0.26591 0.61767E-01 + 5912.0 51.143 0.19928 0.63398E-01 + 6051.1 0.56060 1.0074 0.12986 + 6051.1 4.1648 0.94496 0.11343 + 6051.1 12.187 0.87780 0.11511 + 6051.1 16.236 0.66945 0.73003E-01 + 6051.1 32.146 0.18231 0.70393E-01 + 6051.1 42.359 0.15886 0.41828E-01 + 6084.8 0.57150 5.8440 0.30884 + 6084.8 4.3084 6.1401 0.27891 + 6084.8 12.342 5.2694 0.26662 + 6084.8 16.389 4.2620 0.19360 + 6084.8 20.823 2.9291 0.17873 + 6084.8 31.330 0.98413 0.91438E-01 + 6084.8 32.679 0.91844 0.95292E-01 + 6084.8 42.698 0.84882 0.69753E-01 + 6084.8 51.757 0.49326 0.56579E-01 + 6236.4 0.55230 0.96075 0.95860E-01 + 6236.4 4.1260 0.88240 0.11540 + 6236.4 11.990 0.80641 0.12279 + 6236.4 15.570 0.73694 0.11533 + 6236.4 17.021 0.72234 0.11609 + 6236.4 20.892 0.71516 0.11192 + 6236.4 27.472 0.50127 0.11294 + 6236.4 31.053 0.32921 0.11623 + 6236.4 42.374 0.28762 0.89032E-01 + 6236.4 46.051 0.27221 0.87066E-01 + 6236.4 51.762 0.10517 0.52984E-01 + 6253.6 0.81057 1.8854 0.14716 + 6253.6 4.7812 2.0023 0.15628 + 6253.6 11.465 1.7404 0.12646 + 6253.6 15.146 1.4679 0.10666 + 6253.6 16.502 1.3548 0.98444E-01 + 6253.6 20.184 0.98320 0.92791E-01 + 6253.6 26.676 0.58984 0.68734E-01 + 6253.6 30.164 0.42167 0.66045E-01 + 6253.6 41.788 0.29997 0.52003E-01 + 6253.6 45.566 0.24428 0.67898E-01 + 6253.6 51.284 0.13257 0.53839E-01 + 6340.4 2.9126 1.1262 0.85784E-01 + 6340.4 11.068 0.95641 0.99568E-01 + 6340.4 14.854 0.91473 0.90240E-01 + 6340.4 18.447 0.62165 0.68125E-01 + 6340.4 41.748 0.11602 0.56854E-01 + 6504.6 20.618 1.1562 0.21922 + 6504.6 26.565 0.61842 0.12473 + 6504.6 30.271 0.45341 0.63223E-01 + 6504.6 32.708 0.38824 0.62394E-01 + 6504.6 36.414 0.29628 0.82289E-01 + 6504.6 41.679 0.30839 0.67077E-01 + 6504.6 52.113 0.24866 0.79533E-01 + 6576.7 0.67961 0.90532 0.15216 + 6576.7 10.874 0.84025 0.11598 + 6576.7 14.466 0.66511 0.91808E-01 + 6576.7 16.990 0.63917 0.10654 + 6576.7 20.680 0.39850 0.56935E-01 + 6576.7 26.117 0.21296 0.80843E-01 + 6576.7 36.311 0.15723 0.68484E-01 + 6673.1 1.4563 1.6718 0.16455 + 6673.1 10.485 1.4063 0.12323 + 6673.1 14.272 1.2677 0.97526E-01 + 6673.1 25.922 0.51069 0.89511E-01 + 6673.1 29.515 0.37966 0.66546E-01 + 6673.1 41.165 0.29364 0.67654E-01 + 6997.1 1.5384 1.6103 0.19469 + 6997.1 9.9038 1.2015 0.14527 + 6997.1 13.461 1.0614 0.12832 + 6997.1 17.596 0.65912 0.15494 + 6997.1 21.442 0.59389 0.99620E-01 + 6997.1 29.038 0.24069 0.59301E-01 + 6997.1 40.481 0.23714 0.11457 +ENDDATA 396 +ENDSUBENT 410 +SUBENT F0157003 20050503 20050831 F021 +BIB 2 4 +REACTION 1(17-CL-35(D,0),,EN) + 2(17-CL-35(D,P),,WID/STR) + 3(17-CL-35(D,0),,L) +STATUS (TABLE)Tbl.3,4 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 67 +DATA 1DATA 2DATA 3 +KEV MEV NO-DIM + 0.0000 0.19000 0.0000 + 0.0000 5.8900 2.0000 + 788.25 2.2300 2.0000 + 1165.1 0.34000 0.0000 + 1165.1 0.94000 2.0000 + 1601.4 0.22000 0.0000 + 1951.2 0.30000 1.0000 + 1951.2 3.9900 3.0000 + 1959.2 0.39000 0.0000 + 2467.9 0.90000 1.0000 + 2467.9 4.5800 3.0000 + 2492.3 0.12000 0.0000 + 2492.3 0.30000 2.0000 + 2518.5 10.170 3.0000 + 2810.9 4.0800 3.0000 + 2863.6 0.95000 2.0000 + 2896.4 1.4500 1.0000 + 2896.4 2.0500 3.0000 + 2994.9 0.90000 1.0000 + 3099.8 1.4600 3.0000 + 3207.4 0.53000 1.0000 + 3332.3 1.8600 1.0000 + 3600.2 0.80000E-01 1.0000 + 3635.0 0.43000 1.0000 + 3723.4 1.1200 3.0000 + 3962.6 0.55000 1.0000 + 3992.1 0.94000 1.0000 + 4032.0 0.78000 1.0000 + 4060.5 0.90000E-01 1.0000 + 4138.8 0.34000 1.0000 + 4315.7 0.37000 1.0000 + 4496.3 0.89000 1.0000 + 4551.7 0.30000E-01 0.0000 + 4551.7 0.33000 2.0000 + 4598.6 0.70000 1.0000 + 4753.8 0.15000 1.0000 + 4753.8 0.44000 3.0000 + 4956.5 0.25000 1.0000 + 4997.8 0.24000 1.0000 + 4997.8 1.1000 3.0000 + 5079.2 0.11000 1.0000 + 5150.4 0.14000 1.0000 + 5204.9 0.53000 1.0000 + 5263.1 0.56000 1.0000 + 5308.1 0.55000 1.0000 + 5463.4 0.78000 1.0000 + 5578.3 0.11000 1.0000 + 5578.3 0.75000 3.0000 + 5619.2 0.66000 1.0000 + 5694.4 0.17000 1.0000 + 5831.9 0.11000 1.0000 + 5898.5 0.53000 1.0000 + 5912.0 0.41000 1.0000 + 6051.1 0.16000 1.0000 + 6084.8 0.91000 1.0000 + 6084.8 0.82000 3.0000 + 6236.4 0.10000 1.0000 + 6236.4 0.67000 3.0000 + 6253.6 0.27000 1.0000 + 6253.6 0.45000 3.0000 + 6340.4 0.17000 1.0000 + 6504.6 0.38000 1.0000 + 6504.6 0.24000 3.0000 + 6576.7 0.14000 1.0000 + 6673.1 0.21000 1.0000 + 6673.1 0.38000 3.0000 + 6997.1 0.20000 1.0000 +ENDDATA 69 +ENDSUBENT 78 +ENDENTRY 3 diff --git a/exforall/F02/F0231.x4 b/exforall/F02/F0231.x4 new file mode 100644 index 000000000..dec1b4409 --- /dev/null +++ b/exforall/F02/F0231.x4 @@ -0,0 +1,251 @@ +ENTRY F0231 20050512 20050831 F022 +SUBENT F0231001 20050512 20050831 F022 +BIB 6 9 +TITLE Contribution into the experimetal study of reaction + 7Li(da)5He for lower energy. +AUTHOR (J.Decharge,G.Surget,G.Bruno,M.Y.Decharge) +INSTITUTE (2FR VNV,2FR BRC) +REFERENCE (J,JPR,33,485,1972) +COMMENT No infromation about experiment technique. + Experiment description is given in the Thesis + by Surget (G.), Orsay (June 1971). +HISTORY (20050425C) +ENDBIB 9 +NOCOMMON 0 0 +ENDSUBENT 12 +SUBENT F0231002 20050512 20050831 F022 +BIB 3 5 +REACTION (3-LI-7(D,A)2-HE-5,,DA,,LEG/REL) +ERR-ANALYS (EN-ERR-DIG) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bars +STATUS (CURVE)Fig.4 (a,b) +ENDBIB 5 +COMMON 2 3 +EN-ERR-DIG ERR-DIG +MEV ARB-UNITS + 0.003 0.2 +ENDCOMMON 3 +DATA 4 198 +NUMBER EN DATA DATA-ERR +NO-DIM MEV ARB-UNITS ARB-UNITS + 0.0000 0.44691 21.877 1.5079 + 0.0000 0.47249 21.777 + 0.0000 0.49368 22.753 1.6170 + 0.0000 0.52125 23.731 1.0789 + 0.0000 0.54664 25.248 + 0.0000 0.57207 26.333 + 0.0000 0.59956 28.066 + 0.0000 0.62687 31.199 + 0.0000 0.64954 37.564 + 0.0000 0.67003 44.359 + 0.0000 0.69756 45.768 0.86203 + 0.0000 0.72112 44.698 + 0.0000 0.74700 42.012 + 0.0000 0.77086 38.463 + 0.0000 0.79883 36.209 + 0.0000 0.82469 33.738 + 0.0000 0.85047 31.914 + 0.0000 0.87618 30.737 + 0.0000 0.90195 29.021 + 0.0000 0.92551 27.950 + 0.0000 0.95118 27.096 + 0.0000 0.97677 26.889 + 0.0000 0.99786 28.619 + 0.0000 1.0085 29.053 + 0.0000 1.0191 29.380 + 0.0000 1.0254 30.244 0.86204 + 0.0000 1.0425 29.603 + 0.0000 1.0490 28.850 + 0.0000 1.0748 26.272 + 0.0000 1.0989 21.430 + 0.0000 1.1247 18.744 + 0.0000 1.1461 17.997 + 0.0000 1.1761 17.036 + 0.0000 1.2017 16.290 + 0.0000 1.2487 15.550 + 0.0000 1.2978 14.703 + 0.0000 1.3489 14.503 + 0.0000 1.4000 14.626 + 0.0000 1.4490 15.288 + 0.0000 1.5001 15.627 1.2937 + 0.0000 1.5468 16.503 + 0.0000 1.5935 18.350 + 0.0000 1.6445 19.443 + 0.0000 1.6933 20.535 + 0.0000 1.7463 22.491 + 0.0000 1.7910 23.475 + 0.0000 1.8419 24.999 + 0.0000 1.8929 25.769 + 0.0000 1.9439 27.078 + 0.0000 1.9905 29.355 1.2937 + 1.0000 0.44669 -3.5683 1.6120 + 1.0000 0.47399 -2.4959 + 1.0000 0.49675 -3.2006 1.6535 + 1.0000 0.52163 -3.6987 1.1985 + 1.0000 0.54857 -4.2797 + 1.0000 0.57370 -3.6618 + 1.0000 0.59439 -4.2836 + 1.0000 0.61958 -3.3351 + 1.0000 0.64662 -3.5027 + 1.0000 0.66752 -3.1325 + 1.0000 0.69457 -3.2175 + 1.0000 0.71924 -4.7076 1.0333 + 1.0000 0.74623 -5.0820 + 1.0000 0.77521 -5.8698 + 1.0000 0.79820 -5.4998 + 1.0000 0.81923 -4.5509 + 1.0000 0.84639 -4.1398 + 1.0000 0.87171 -2.6126 + 1.0000 0.90091 -2.4085 + 1.0000 0.92617 -1.1706 + 1.0000 0.95134 -.34606 + 1.0000 0.97439 0.35465 + 1.0000 0.99520 0.27021 1.1985 + 1.0000 1.0055 -.26802 + 1.0000 1.0261 -1.3445 + 1.0000 1.0358 -4.4454 + 1.0000 1.0480 -5.7691 + 1.0000 1.0748 -7.2595 1.0333 + 1.0000 1.0978 -6.5587 + 1.0000 1.1251 -5.7757 + 1.0000 1.1480 -5.4884 + 1.0000 1.1712 -4.3743 + 1.0000 1.1983 -4.2526 + 1.0000 1.2485 -3.0169 + 1.0000 1.2966 -2.1530 + 1.0000 1.3509 -1.7443 + 1.0000 1.4009 -1.2939 + 1.0000 1.4470 0.66209E-01 + 1.0000 1.4989 -.76492 1.2400 + 1.0000 1.5492 0.59482 + 1.0000 1.5974 1.9961 + 1.0000 1.6495 1.9916 + 1.0000 1.6975 2.7315 + 1.0000 1.7497 3.2231 + 1.0000 1.7996 3.0535 + 1.0000 1.8476 3.5867 + 1.0000 1.8997 3.4169 + 1.0000 1.9433 2.8758 + 1.0000 1.9933 3.0369 1.0747 + 1.0000 2.0538 3.6104 0.37200 + 1.0000 2.0870 3.0289 0.33085 + 2.0000 0.45272 0.66459 1.4928 + 2.0000 0.47564 0.98676 + 2.0000 0.50269 0.66327 1.5332 + 2.0000 0.52979 1.0257 1.2105 + 2.0000 0.55473 0.33911 + 2.0000 0.57975 0.74192 + 2.0000 0.60256 -.59015 + 2.0000 0.62958 -1.3575 + 2.0000 0.65443 -3.2948 + 2.0000 0.67921 -6.3215 + 2.0000 0.70191 -9.1868 + 2.0000 0.72899 -9.0665 1.0490 + 2.0000 0.75195 -8.3408 + 2.0000 0.77697 -7.9380 + 2.0000 0.80201 -7.1721 + 2.0000 0.82501 -5.8816 + 2.0000 0.85004 -5.2367 + 2.0000 0.87921 -4.9550 + 2.0000 0.90007 -4.4310 + 2.0000 0.93136 -3.7056 + 2.0000 0.95434 -2.6572 + 2.0000 0.97730 -1.9315 + 2.0000 1.0024 -.72176 1.8560 + 2.0000 1.0107 -.31851 + 2.0000 1.0315 -.72253 + 2.0000 1.0399 -.36846E-01 + 2.0000 1.0524 -.40030 + 2.0000 1.0773 -1.4097 + 2.0000 1.1001 -2.3786 + 2.0000 1.1251 -2.2986 1.1297 + 2.0000 1.1522 -2.5414 + 2.0000 1.1793 -2.0579 + 2.0000 1.2001 -1.6146 + 2.0000 1.2522 -.97046 + 2.0000 1.3022 -.72969 + 2.0000 1.3564 -.56973 + 2.0000 1.4044 0.92186 + 2.0000 1.4524 2.0503 + 2.0000 1.5003 2.5736 1.2910 + 2.0000 1.5524 3.3388 + 2.0000 1.6004 4.2655 + 2.0000 1.6525 4.9097 + 2.0000 1.7005 6.1189 + 2.0000 1.7546 6.6823 + 2.0000 1.8026 7.5283 + 2.0000 1.8506 8.7779 + 2.0000 1.9007 10.955 + 2.0000 1.9507 11.317 + 2.0000 1.9987 12.688 1.0490 + 3.0000 0.45009 1.2121 2.7758 + 3.0000 0.47523 1.8630 + 3.0000 0.49810 1.6978 2.8167 + 3.0000 0.52533 2.4303 1.9593 + 3.0000 0.54591 1.3264 + 3.0000 0.57505 1.2423 + 3.0000 0.60220 1.6074 + 3.0000 0.62727 1.9726 + 3.0000 0.64991 0.78692 + 3.0000 0.67901 0.53954 + 3.0000 0.69957 -.64596 + 3.0000 0.72676 -.11762 + 3.0000 0.74975 0.24780 + 3.0000 0.77878 -.28531 + 3.0000 0.80193 0.77403 + 3.0000 0.82674 -.36425E-02 + 3.0000 0.84974 0.40260 + 3.0000 0.87667 -.21197 + 3.0000 0.90166 -.21409 + 3.0000 0.92450 -.54259 + 3.0000 0.94959 -.54883E-01 + 3.0000 0.97421 -1.7306 + 3.0000 0.99689 -2.7938 1.9591 + 3.0000 1.0050 -3.9782 + 3.0000 1.0214 -4.7552 + 3.0000 1.0401 -4.9609 1.7960 + 3.0000 1.0487 -4.0228 + 3.0000 1.0738 -3.4126 + 3.0000 1.0991 -1.8636 + 3.0000 1.1265 -.68217 + 3.0000 1.1534 -1.2967 + 3.0000 1.1766 -.11496 + 3.0000 1.2036 -.23971 + 3.0000 1.2516 0.20523 + 3.0000 1.3036 -.44094E-01 + 3.0000 1.3515 -.25225 + 3.0000 1.4015 -.11578E-01 + 3.0000 1.4537 0.63710 + 3.0000 1.5014 -.60875E-01 + 3.0000 1.5513 -.43248 + 3.0000 1.6014 -.69354E-01 + 3.0000 1.6555 -.33128E-01 + 3.0000 1.6993 0.28971 + 3.0000 1.7536 0.69330 + 3.0000 1.8450 -.83840E-02 + 3.0000 1.8996 2.0688 + 3.0000 1.9497 2.1870 + 3.0000 1.9954 1.8157 1.9591 +ENDDATA 200 +ENDSUBENT 214 +SUBENT F0231003 20050512 20050831 F022 +BIB 3 6 +REACTION 1(3-LI-7(D,0),,EN) + 2(3-LI-7(D,0),,J) + 3(3-LI-7(D,0),,PTY) + 4(3-LI-7(D,TOT),,WID) +ERR-ANALYS No information about the uncertainties is given. +STATUS (TABLE) Table 2. +ENDBIB 6 +NOCOMMON 0 0 +DATA 4 4 +DATA 1DATA 2DATA 3DATA-CM 4 +MEV NO-DIM NO-DIM KEV +0.28500 1.5000 -1.0000 0.25000 +0.70700 1.5000 -1.0000 215.00 + 1.0400 1.5000 1.0000 105.00 + 2.1800 1.5000 1.0000 980.00 +ENDDATA 6 +ENDSUBENT 17 +ENDENTRY 3 diff --git a/exforall/F02/F0239.x4 b/exforall/F02/F0239.x4 index d60e9f3c3..85946c28e 100644 --- a/exforall/F02/F0239.x4 +++ b/exforall/F02/F0239.x4 @@ -1,22 +1,1351 @@ -ENTRY F0239 19990508 20000121 -SUBENT F0239001 19990508 20000121 -BIB 7 13 -TITLE Glost anomaly in 8Be studied with 9Be(d,p) at - E(p)= 14.3 and 26.2 MEV -AUTHOR (F.D.BECCHETTI,C.A.FIELDS,R.S.RAYMOND,H.C.BHANG, - D.OVERWAY) -INSTITUTE (1USACLU,1USAMHG) -REFERENCE (J,PR/C,24,2401,198112) -SAMPLE Self-supporting 9Be targets thicknesses 0.15 and - 2.6 mu-g/cm**2 -DETECTOR (TELES) Deltae-e Si counter telescope consisting of - detectors 200 and 5000 mu-m thick and spectrometer. -HISTORY (19850228C) - (19990507A) CNPD: corrected 4-dig. year - (19990507D) Entry deleted. New name:T0040 -ENDBIB 13 -NOCOMMON 0 0 -ENDSUBENT 16 -NOSUBENT F0239002 19990508 20000121 -NOSUBENT F0239003 19990508 20000121 -ENDENTRY 3 +ENTRY F0239 20050628 20050831 F021 +SUBENT F0239001 20050628 20050831 F021 +BIB 11 22 +TITLE New analytical developments in prompt gamma-ray + spectrometry with low-energy tritons and alpha + particles. +AUTHOR (B.Borderie,J.N.Barrandon) +INSTITUTE (2FR STR) +REFERENCE (J,NIM,156,483,1978) +FACILITY (VDG) +DETECTOR (GELI) 60 cm3 Ge(Li) detector coupled with 4096 channel + analyzer was used. + Faraday cup was isolated from the beam line by + insulator and protected by a negative ring voltage. +SAMPLE Targets were thick enough to stop particles and were + typically 0.1 to 2 mm thick. +METHOD (BCINT) + (GSPEC) +MONITOR Detector was calibrated for efficiency with a + standardized radiocativity source of 152Eu. + The detection limits were calculated for a pure niobium + target with a current beam of 500 nA and an irradiation + time of 1 h. +ERR-ANALYS Overall accuracy of data is from 10 to 15%. +HISTORY (20050222C) +ENDBIB 22 +COMMON 2 3 +EN-RSL ANG +KEV ADEG + 3.5 90. +ENDCOMMON 3 +ENDSUBENT 29 +SUBENT F0239002 20050628 20050831 F021 +BIB 3 3 +REACTION (3-LI-0(T,INL)3-LI-0,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 2.0000 478.00 0.36100E+07 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239003 20050628 20050831 F021 +BIB 3 3 +REACTION (6-C-0(T,X)7-N-14,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 2. +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 193.00 30000. + 1632.0 0.24600E+07 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239004 20050628 20050831 F021 +BIB 3 3 +REACTION (8-O-0(T,X)9-F-18,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 2. +ENDCOMMON 3 +DATA 2 5 +E DATA +KEV PRT/MUC/SR + 185.00 51400. + 659.00 0.39200E+06 + 937.00 0.10800E+07 + 1042.0 0.85100E+06 + 1081.0 0.44000E+06 +ENDDATA 7 +ENDSUBENT 19 +SUBENT F0239005 20050628 20050831 F021 +BIB 3 3 +REACTION (8-O-0(T,X)8-O-18,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 2.0000 1982.0 0.11300E+07 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239006 20050628 20050831 F021 +BIB 3 3 +REACTION (9-F-19(T,INL)9-F-19,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 2. +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 110.00 60800. + 197.00 0.32700E+07 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239007 20050628 20050831 F021 +BIB 3 3 +REACTION (9-F-19(T,D)9-F-20,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 2.0000 656.00 0.16400E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239008 20050628 20050831 F021 +BIB 3 3 +REACTION (9-F-19(T,P)9-F-21,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 2.0000 280.00 0.38200E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239009 20050628 20050831 F021 +BIB 3 4 +REACTION ((9-F-19(T,P)9-F-21,PAR,TTY/MLT/DA,G)+ + (9-F-19(T,N)10-NE-21,PAR,TTY/MLT/DA,G)) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 2.0000 350.00 0.17800E+07 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239010 20050628 20050831 F021 +BIB 3 3 +REACTION (11-NA-23(T,A)10-NE-22,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 2.0000 1275.0 0.41900E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239011 20050628 20050831 F021 +BIB 3 3 +REACTION (11-NA-23(T,P)11-NA-25,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 2.0000 90.000 0.35500E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239012 20050628 20050831 F021 +BIB 3 3 +REACTION (11-NA-23(T,D)11-NA-24,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 2. +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 472.00 0.14300E+06 + 877.00 0.30900E+06 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239013 20050628 20050831 F021 +BIB 3 3 +REACTION (12-MG-0(T,X)13-AL-26,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 2. +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 417.00 0.26400E+06 + 830.00 0.25500E+06 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239014 20050628 20050831 F021 +BIB 3 3 +REACTION (12-MG-0(T,X)11-NA-23,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 2.0000 440.00 0.17300E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239015 20050628 20050831 F021 +BIB 3 3 +REACTION (14-SI-0(T,X)15-P-30,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3. +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 677.00 0.40000E+06 + 709.00 0.40800E+06 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239016 20050628 20050831 F021 +BIB 3 3 +REACTION (16-S-0(T,X)17-CL-34,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3. +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 461.00 0.44100E+06 + 665.00 0.19000E+06 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239017 20050628 20050831 F021 +BIB 3 3 +REACTION (16-S-0(T,X)16-S-33,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.0000 840.00 0.45100E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239018 20050628 20050831 F021 +BIB 3 3 +REACTION (22-TI-0(T,X)23-V-50,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 4 +EN E DATA +MEV KEV PRT/MUC/SR + 3.0000 94.000 0.39400E+06 + 3.0000 226.00 0.59900E+06 + 3.5000 94.000 0.15000E+07 + 3.5000 226.00 0.16600E+07 +ENDDATA 6 +ENDSUBENT 14 +SUBENT F0239019 20050628 20050831 F021 +BIB 3 4 +REACTION ((23-V-0(T,X)23-V-52,PAR,TTY/MLT/DA,G)+ + (23-V-0(T,X)23-V-53,PAR,TTY/MLT/DA,G)) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 2 3 +E E +KEV KEV + 125. 129. +ENDCOMMON 3 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.0000 124.00 63200. +ENDDATA 3 +ENDSUBENT 16 +SUBENT F0239020 20050628 20050831 F021 +BIB 3 3 +REACTION (22-TI-0(T,X)23-V-48,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 305.00 51100. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239021 20050628 20050831 F021 +BIB 3 3 +REACTION (22-TI-0(T,X)22-TI-49,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 342.00 69800. + 1381.0 0.37600E+06 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239022 20050628 20050831 F021 +BIB 3 3 +REACTION (22-TI-0(T,X)22-TI-50,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 1554.0 17800. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239023 20050628 20050831 F021 +BIB 3 3 +REACTION (24-CR-0(T,X)25-MN-55,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 126.00 50800. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239024 20050628 20050831 F021 +BIB 3 3 +REACTION (24-CR-0(T,X)25-MN-54,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 157.00 0.37100E+06 + 251.00 85700. +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239025 20050628 20050831 F021 +BIB 3 3 +REACTION (24-CR-0(T,X)25-MN-56,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 211.00 0.10200E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239026 20050628 20050831 F021 +BIB 3 3 +REACTION (24-CR-0(T,X)24-CR-53,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 564.00 0.11400E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239027 20050628 20050831 F021 +BIB 3 3 +REACTION (24-CR-0(T,X)24-CR-54,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 835.00 0.19600E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239028 20050628 20050831 F021 +BIB 3 3 +REACTION (25-MN-55(T,D)25-MN-56,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 104.00 37800. + 211.00 0.13200E+06 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239029 20050628 20050831 F021 +BIB 3 3 +REACTION (25-MN-55(T,A)24-CR-54,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 835.00 0.80000E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239030 20050628 20050831 F021 +BIB 3 3 +REACTION (26-FE-0(T,X)27-CO-58,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 116.00 25500. + 367.00 0.10700E+06 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239031 20050628 20050831 F021 +BIB 3 3 +REACTION (26-FE-0(T,X)26-FE-57,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 122.00 25500. + 352.00 71700. +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239032 20050628 20050831 F021 +BIB 3 3 +REACTION (26-FE-0(T,X)26-FE-58,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 811.00 0.10400E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239033 20050628 20050831 F021 +BIB 3 3 +REACTION (26-FE-0(T,X)25-MN-55,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 126.00 13200. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239034 20050628 20050831 F021 +BIB 3 3 +REACTION (27-CO-59(T,D)27-CO-60,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 4 +E DATA +KEV PRT/MUC/SR + 230.00 31000. + 277.00 11600. + 556.00 32700. + 945.00 59700. +ENDDATA 6 +ENDSUBENT 18 +SUBENT F0239035 20050628 20050831 F021 +BIB 3 3 +REACTION (27-CO-59(T,N)28-NI-61,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 283.00 8900.0 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239036 20050628 20050831 F021 +BIB 3 4 +REACTION ((28-NI-0(T,X)29-CU-64,PAR,TTY/MLT/DA,G)+ + (28-NI-0(T,X)28-NI-63,PAR,TTY/MLT/DA,G)) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 4 1 +EN E E DATA +MEV KEV KEV PRT/MUC/SR + 3.5000 159.00 160.00 6180.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239037 20050628 20050831 F021 +BIB 3 3 +REACTION (28-NI-0(T,X)29-CU-62,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 244.00 19800. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239038 20050628 20050831 F021 +BIB 3 3 +REACTION (28-NI-0(T,X)28-NI-59,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 340.00 21400. + 460.00 30800. +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239039 20050628 20050831 F021 +BIB 3 3 +REACTION (28-NI-0(T,X)28-NI-60,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 3 +E DATA +KEV PRT/MUC/SR + 826.00 22200. + 1173.0 21900. + 1332.0 84500. +ENDDATA 5 +ENDSUBENT 17 +SUBENT F0239040 20050628 20050831 F021 +BIB 3 3 +REACTION (29-CU-0(T,X)30-ZN-65,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 115.00 20700. + 155.00 10600. +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239041 20050628 20050831 F021 +BIB 3 3 +REACTION (29-CU-0(T,X)29-CU-64,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 3 +E DATA +KEV PRT/MUC/SR + 159.00 16900. + 205.00 13700. + 278.00 16400. +ENDDATA 5 +ENDSUBENT 17 +SUBENT F0239042 20050628 20050831 F021 +BIB 3 3 +REACTION (30-ZN-0(T,X)30-ZN-65,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 115.00 11200. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239043 20050628 20050831 F021 +BIB 3 3 +REACTION (30-ZN-0(T,X)31-GA-68,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 175.00 19500. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239044 20050628 20050831 F021 +BIB 3 3 +REACTION (30-ZN-0(T,X)30-ZN-67,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 93.000 13400. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239045 20050628 20050831 F021 +BIB 3 3 +REACTION (31-GA-0(T,X)32-GE-71,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRT/MUC/SR + 175.00 32700. + 831.00 33700. +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239046 20050628 20050831 F021 +BIB 3 3 +REACTION (32-GE-0(T,X)32-GE-71,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 175.00 12400. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239047 20050628 20050831 F021 +BIB 3 3 +REACTION (32-GE-0(T,X)32-GE-74,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRT/MUC/SR + 3.5000 596.00 27700. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239048 20050628 20050831 F021 +BIB 3 4 +REACTION (33-AS-75(T,INL)33-AS-75,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 3 +E DATA +KEV PRD/MUC/SR + 199.00 22700. + 265.00 6460.0 + 279.00 37900. +ENDDATA 5 +ENDSUBENT 18 +SUBENT F0239049 20050628 20050831 F021 +BIB 3 4 +REACTION (34-SE-0(T,INL)34-SE-77,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 239.00 13100. + 440.00 3750.0 +ENDDATA 4 +ENDSUBENT 17 +SUBENT F0239050 20050628 20050831 F021 +BIB 3 4 +REACTION (34-SE-0(T,INL)34-SE-76,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 559.00 5740.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239051 20050628 20050831 F021 +BIB 3 4 +REACTION (34-SE-0(T,INL)34-SE-78,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 614.00 10900. +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239052 20050628 20050831 F021 +BIB 3 4 +REACTION (34-SE-0(T,INL)34-SE-80,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 666.00 8640.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239053 20050628 20050831 F021 +BIB 3 4 +REACTION (42-MO-0(T,INL)42-MO-95,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 204.00 3890.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239054 20050628 20050831 F021 +BIB 3 4 +REACTION (42-MO-0(T,INL)42-MO-100,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 534.00 3300.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239055 20050628 20050831 F021 +BIB 3 4 +REACTION (46-PD-0(T,INL)46-PD-104,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 556.00 2080.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239056 20050628 20050831 F021 +BIB 3 4 +REACTION (46-PD-0(T,INL)46-PD-105,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 280.00 850.00 + 441.00 4020.0 +ENDDATA 4 +ENDSUBENT 17 +SUBENT F0239057 20050628 20050831 F021 +BIB 3 4 +REACTION (46-PD-0(T,INL)46-PD-108,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 434.00 17100. +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239058 20050628 20050831 F021 +BIB 3 4 +REACTION (46-PD-0(T,INL)46-PD-110,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 374.00 13300. +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239059 20050628 20050831 F021 +BIB 3 4 +REACTION (47-AG-0(T,INL)47-AG-107,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 325.00 23900. + 423.00 12000. +ENDDATA 4 +ENDSUBENT 17 +SUBENT F0239060 20050628 20050831 F021 +BIB 3 4 +REACTION (47-AG-0(T,INL)47-AG-109,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 311.00 26500. + 415.00 13300. +ENDDATA 4 +ENDSUBENT 17 +SUBENT F0239061 20050628 20050831 F021 +BIB 3 4 +REACTION (48-CD-0(T,INL)48-CD-111,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 342.00 1280.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239062 20050628 20050831 F021 +BIB 3 4 +REACTION (48-CD-0(T,INL)48-CD-112,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 617.00 1600.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239063 20050628 20050831 F021 +BIB 3 4 +REACTION (48-CD-0(T,INL)48-CD-113,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 299.00 2300.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239064 20050628 20050831 F021 +BIB 3 4 +REACTION (48-CD-0(T,INL)48-CD-114,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 556.00 3300.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239065 20050628 20050831 F021 +BIB 3 4 +REACTION (73-TA-0(T,INL)73-TA-181,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 3 +E DATA +KEV PRD/MUC/SR + 136.00 0.12200E+06 + 165.00 6380.0 + 301.00 4040.0 +ENDDATA 5 +ENDSUBENT 18 +SUBENT F0239066 20050628 20050831 F021 +BIB 3 4 +REACTION (74-W-0(T,INL)74-W-182,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 100.00 39000. +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239067 20050628 20050831 F021 +BIB 3 4 +REACTION (74-W-0(T,INL)74-W-184,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 111.00 46500. +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239068 20050628 20050831 F021 +BIB 3 4 +REACTION (74-W-0(T,INL)74-W-186,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 122.00 46400. +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239069 20050628 20050831 F021 +BIB 3 4 +REACTION (75-RE-0(T,INL)75-RE-185,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 125.00 26700. + 159.00 2990.0 +ENDDATA 4 +ENDSUBENT 17 +SUBENT F0239070 20050628 20050831 F021 +BIB 3 4 +REACTION (75-RE-0(T,INL)75-RE-187,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 134.00 42800. + 167.00 4310.0 +ENDDATA 4 +ENDSUBENT 17 +SUBENT F0239071 20050628 20050831 F021 +BIB 3 4 +REACTION (78-PT-0(T,INL)78-PT-194,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 328.00 7670.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239072 20050628 20050831 F021 +BIB 3 4 +REACTION (78-PT-0(T,INL)78-PT-195,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 98.000 2700.0 + 211.00 5700.0 +ENDDATA 4 +ENDSUBENT 17 +SUBENT F0239073 20050628 20050831 F021 +BIB 3 4 +REACTION (78-PT-0(T,INL)78-PT-196,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 356.00 3270.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239074 20050628 20050831 F021 +BIB 3 4 +REACTION (79-AU-197(T,INL)79-AU-197,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 3 +ENDBIB 4 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 191.00 1530.0 + 279.00 7360.0 +ENDDATA 4 +ENDSUBENT 17 +SUBENT F0239075 20050628 20050831 F021 +BIB 3 3 +REACTION (3-LI-0(A,INL)3-LI-7,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 478.00 0.65200E+07 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239076 20050628 20050831 F021 +BIB 3 3 +REACTION (5-B-0(A,P)6-C-13,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 169.00 67100. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239077 20050628 20050831 F021 +BIB 3 3 +REACTION (5-B-0(A,INL)5-B-10,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 717.00 30700. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239078 20050628 20050831 F021 +BIB 3 3 +REACTION (8-O-0(A,N)10-NE-21,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 350.00 1280.0 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239079 20050628 20050831 F021 +BIB 3 3 +REACTION (9-F-19(A,INL)9-F-19,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 110.00 50700. + 197.00 0.11900E+06 +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239080 20050628 20050831 F021 +BIB 3 3 +REACTION (9-F-19(A,N)11-NA-22,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 583.00 25000. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239081 20050628 20050831 F021 +BIB 3 3 +REACTION (9-F-19(A,P)10-NE-22,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 1275.0 0.24800E+06 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239082 20050628 20050831 F021 +BIB 3 3 +REACTION (11-NA-23(A,INL)11-NA-23,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 440.00 33400. +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0239083 20050628 20050831 F021 +BIB 3 3 +REACTION (11-NA-23(A,P)12-MG-26,PAR,TTY/MLT/DA,G) +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 3 +COMMON 1 3 +EN +MEV + 3.5 +ENDCOMMON 3 +DATA 2 2 +E DATA +KEV PRD/MUC/SR + 1130.0 9500.0 + 1809.0 51100. +ENDDATA 4 +ENDSUBENT 16 +SUBENT F0239084 20050628 20050831 F021 +BIB 3 4 +REACTION (22-TI-0(A,INL)22-TI-47,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 159.00 2160.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239085 20050628 20050831 F021 +BIB 3 4 +REACTION (23-V-0(A,INL)23-V-51,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 320.00 2660.0 +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239086 20050628 20050831 F021 +BIB 3 4 +REACTION (25-MN-55(A,INL)25-MN-55,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 126.00 28000. +ENDDATA 3 +ENDSUBENT 12 +SUBENT F0239087 20050628 20050831 F021 +BIB 3 4 +REACTION (26-FE-0(A,INL)26-FE-57,PAR,TTY/MLT/DA,G) + Coulomb excitation +PART-DET (G) +STATUS (TABLE) Table 4 +ENDBIB 4 +NOCOMMON 0 0 +DATA 3 1 +EN E DATA +MEV KEV PRD/MUC/SR + 3.5000 122.00 440.00 +ENDDATA 3 +ENDSUBENT 12 +ENDENTRY 87 diff --git a/exforall/F02/F0253.x4 b/exforall/F02/F0253.x4 new file mode 100644 index 000000000..22780807a --- /dev/null +++ b/exforall/F02/F0253.x4 @@ -0,0 +1,419 @@ +ENTRY F0253 20050627 20050831 F022 +SUBENT F0253001 20050627 20050831 F022 +BIB 11 21 +TITLE 7Li+d-2a+n reaction.Experimental results at Ed=1.0 MeV. +AUTHOR (V.D'Amico,G.Fazio,S.Jannelli,F.Mezzanares,R.Potenza) +INSTITUTE (2ITYMES,2ITYLNS,2ITYCAT,2ITYSIC) +REFERENCE (J,NC/A,22,313,1974) +FACILITY (VDG,2ITYCAT) 2.7 MV +DETECTOR (SIBAR)Two movable surface barrier detectors supplied + by ORTEC. One of the detectors was fixed at an + angle of 88.4 degr., while the second one was + allowed to rotate between 30 and 110 degrees. +MONITOR One of the detectors remained in a fixed position and + acted also as a beam monitor. +SAMPLE A natural Li target 0.5 mg/cm2 thick, evaporated on a + polyvinilformal backing of 0.1 mu-m was used. +METHOD (BCINT) + (COINC) + (DSCAT) +ERR-ANALYS (DATA-ERR1)The errors of the absolute values of + cross-sections. + (ERR-DIG)Digitizing error + (DATA-ERR2)Error from the graphic bars +HISTORY (20050523C) +ENDBIB 21 +COMMON 2 3 +EN DATA-ERR1 +MEV PER-CENT + 1. 15. +ENDCOMMON 3 +ENDSUBENT 28 +SUBENT F0253002 20050627 20050831 F022 +BIB 3 6 +REACTION (3-LI-7(D,N+A)2-HE-4,,DA/DA,A/A) + ANG1 and ANG2 are the angles of detection of the + "first" and the "second" alpha particle, + correspondingly. +ERR-ANALYS (ANG-ERR-D)Digitizing error +STATUS (CURVE)Fig.2 +ENDBIB 6 +COMMON 3 3 +ANG1 ANG-ERR-D ERR-DIG +ADEG ADEG MB/SR2 + 88.4 0.06 0.21 +ENDCOMMON 3 +DATA 3 43 +ANG2 DATA DATA-ERR2 +ADEG MB/SR2 MB/SR2 +-42.102 4.8892 +-43.936 5.8661 +-45.955 7.0968 +-47.800 10.677 +-49.732 12.953 +-51.769 18.350 +-53.809 24.527 +-55.846 30.184 +-57.898 38.966 +-59.951 48.268 +-61.734 58.362 +-63.864 85.109 +-65.791 128.27 +-67.750 199.81 +-69.866 244.27 1.5623 +-71.173 187.45 3.3849 +-71.966 201.49 +-73.047 155.62 +-73.890 139.18 +-74.919 123.26 2.3434 +-76.266 96.389 +-77.803 71.335 +-77.876 66.906 +-79.509 84.816 2.0862 +-79.828 73.868 +-81.403 99.333 +-83.402 138.06 2.0830 +-85.243 182.53 +-87.484 213.70 3.3849 +-87.951 257.95 1.8226 +-89.551 205.29 +-89.979 177.41 +-91.314 147.94 1.5623 +-91.887 132.56 +-93.915 93.943 +-95.840 73.822 +-97.893 62.031 +-99.826 43.734 +-101.97 30.637 +-104.02 19.888 +-105.83 15.397 +-107.91 9.0732 +-109.98 1.1875 1.3019 +ENDDATA 45 +ENDSUBENT 60 +SUBENT F0253003 20050627 20050831 F022 +BIB 5 12 +REACTION (3-LI-7(D,N+A)2-HE-4,,DA/DA/DE,A/A/N) + ANG1 is the angle of detection for the "first" alpha + particle, ANG2 is the polar angle of the "second" + emitted alpha particle in the system where the + alpha-neutron complex is at rest. + Internal energy spectra is given. +EN-SEC (E-CM,A/N) E is the internal energy of the alpha-n + system. +FLAG (1.) Azimuth angle is 0 degree. + (2.) Azimuth angle is 180 degrees. +ERR-ANALYS (E-ERR-DIG) Digitizing error +STATUS (CURVE)Fig.3 +ENDBIB 12 +COMMON 4 3 +ANG1 ANG2-ERR E-ERR-DIG ERR-DIG +ADEG ADEG MEV MB/SR2/MEV + 88.4 10. 0.1 0.01 +ENDCOMMON 3 +DATA 5 45 +ANG2 E-CM DATA-CM DATA-ERR2 FLAG +ADEG MEV MB/SR2/MEV MB/SR2/MEV NO-DIM + 0.0000 0.68311E-010.19588E-010.65383E-02 1.0000 + 0.0000 0.15816 0.50513E-010.58838E-02 1.0000 + 0.0000 0.32008 0.16797 0.17023E-01 1.0000 + 0.0000 0.58214 0.32880 0.15714E-01 1.0000 + 0.0000 0.86826 0.45237 0.26827E-01 1.0000 + 0.0000 1.3180 0.40081 0.24216E-01 1.0000 + 90.000 0.93165E-010.43422E-010.71667E-02 2.0000 + 90.000 0.14348 0.12711 0.58896E-02 1.0000 + 90.000 0.17761 0.31434 0.13736E-01 1.0000 + 90.000 0.25547 0.17609 0.12379E-01 2.0000 + 90.000 0.30089 0.47817 0.22898E-01 1.0000 + 90.000 0.36617 0.63011 0.38616E-01 1.0000 + 90.000 0.50209 0.45492 0.14342E-01 2.0000 + 90.000 0.54770 1.0100 0.37968E-01 1.0000 + 90.000 0.84541 1.2003 0.33381E-01 1.0000 + 90.000 0.84750 1.1263 0.62563E-01 2.0000 + 90.000 1.1826 0.84745 0.23571E-01 1.0000 + 90.000 1.2165 1.2888 0.52781E-01 2.0000 + 90.000 1.5856 0.63673 0.24213E-01 1.0000 + 90.000 1.6448 1.0037 0.23463E-01 2.0000 + 90.000 2.0255 0.48956 0.18984E-01 1.0000 + 90.000 2.2055 0.81020 0.39091E-01 2.0000 + 90.000 2.3221 0.42265 0.13742E-01 1.0000 + 90.000 2.7611 0.73332 0.31273E-01 2.0000 + 90.000 2.8498 0.41764 0.22262E-01 1.0000 + 90.000 3.3043 0.72353 0.43652E-01 2.0000 + 90.000 3.3540 0.37202 0.17675E-01 1.0000 + 90.000 3.7682 0.64774 0.29318E-01 2.0000 + 90.000 3.9687 0.31611 0.20947E-01 1.0000 + 90.000 4.1691 0.58093 0.36502E-01 2.0000 + 90.000 4.6070 0.55720 0.21500E-01 2.0000 + 90.000 4.7572 0.29845 0.19632E-01 1.0000 + 90.000 4.9864 0.48382 0.45615E-01 2.0000 + 90.000 5.5604 0.40634 0.23472E-01 2.0000 + 180.00 0.82809E-010.35494E-010.84389E-02 2.0000 + 180.00 0.20041 0.79187E-010.17508E-01 2.0000 + 180.00 0.34112 0.15598 0.21377E-01 2.0000 + 180.00 0.55441 0.28996 0.20747E-01 2.0000 + 180.00 0.79833 0.35923 0.27225E-01 2.0000 + 180.00 1.0621 0.36116 0.39533E-01 2.0000 + 180.00 1.3864 0.24272 0.45346E-01 2.0000 + 180.00 1.7730 0.12573 0.24607E-01 2.0000 + 180.00 2.2379 0.86026E-010.22034E-01 2.0000 + 180.00 2.7472 0.40600E-010.14251E-01 2.0000 + 180.00 3.3940 0.18182E-010.11669E-01 2.0000 +ENDDATA 47 +ENDSUBENT 68 +SUBENT F0253004 20050627 20050831 F022 +BIB 4 11 +REACTION (3-LI-7(D,A+N)2-HE-4,,DA/DA/DE,A/A/N) + ANG1 is an angle of alpha particle detection. + ANG2 is a relative angle that can be interpreted as + the angle of the alpha-particle in the centre of mass + of the alpha-n system when the motion of this latter is + described in the system of the centre of mass of the + three particles. +EN-SEC (E-CM,A/N) E is the internal energy of the alpha-n + system. +ERR-ANALYS (ANG-ERR-D)Digitizing error +STATUS (CURVE)Fig.4 +ENDBIB 11 +COMMON 3 3 +ANG1 ANG-ERR-D ERR-DIG +ADEG ADEG MB/SR2/MEV + 88.4 0.23 0.01 +ENDCOMMON 3 +DATA 5 112 +E-CM E-ERR ANG2-CM DATA-CM DATA-ERR2 +MEV MEV ADEG MB/SR2/MEV MB/SR2/MEV +0.30000 0.10000 -175.21 0.12289 0.23949E-01 +0.30000 0.10000 -154.69 0.12911 0.23078E-01 +0.30000 0.10000 -134.58 0.14903 0.20481E-01 +0.30000 0.10000 -124.11 0.83348E-010.13631E-01 +0.30000 0.10000 -114.15 0.22447 0.11120E-01 +0.30000 0.10000 -104.31 0.17507 0.23898E-01 +0.30000 0.10000 -94.432 0.17522 0.23061E-01 +0.30000 0.10000 -84.310 0.17535 0.19627E-01 +0.30000 0.10000 -65.058 0.21327 0.35872E-01 +0.30000 0.10000 -54.859 0.22707 0.25623E-01 +0.30000 0.10000 -45.138 0.11444 0.76869E-02 +0.30000 0.10000 -34.888 0.17950 0.20498E-01 +0.30000 0.10000 -15.299 0.10718 0.24786E-01 +0.30000 0.10000 -5.2980 0.21327 0.25606E-01 +0.30000 0.10000 5.1283 0.13990 0.11103E-01 +0.30000 0.10000 14.531 0.22553 0.30713E-01 +0.30000 0.10000 24.664 0.27009 0.93779E-02 +0.30000 0.10000 34.523 0.22410 0.40997E-01 +0.30000 0.10000 43.837 0.37894 0.11957E-01 +0.30000 0.10000 53.907 0.41240 0.22207E-01 +0.30000 0.10000 63.383 0.29894 0.40143E-01 +0.30000 0.10000 82.771 0.36078 0.55534E-01 +0.30000 0.10000 92.384 0.52585 0.41031E-01 +0.30000 0.10000 102.28 0.44397 0.24803E-01 +0.30000 0.10000 112.35 0.47658 0.41031E-01 +0.30000 0.10000 122.54 0.32034 0.60658E-01 +0.30000 0.10000 132.64 0.27433 0.48701E-01 +0.30000 0.10000 142.16 0.25315 0.47830E-01 +0.30000 0.10000 151.72 0.28151 0.35035E-01 +0.50000 0.10000 -175.42 0.26290 0.25690E-01 +0.50000 0.10000 -165.26 0.26472 0.34296E-01 +0.50000 0.10000 -145.27 0.25465 0.21460E-01 +0.50000 0.10000 -135.22 0.39965 0.30011E-01 +0.50000 0.10000 -125.33 0.31489 0.24030E-01 +0.50000 0.10000 -104.76 0.52426 0.23976E-01 +0.50000 0.10000 -94.958 0.46523 0.21442E-01 +0.50000 0.10000 -85.156 0.44735 0.24030E-01 +0.50000 0.10000 -75.189 0.49805 0.27422E-01 +0.50000 0.10000 -64.664 0.52041 0.32564E-01 +0.50000 0.10000 -54.406 0.37562 0.26565E-01 +0.50000 0.10000 -45.183 0.34150 0.26601E-01 +0.50000 0.10000 -34.810 0.25670 0.11979E-01 +0.50000 0.10000 -25.224 0.32458 0.30814E-01 +0.50000 0.10000 -5.6221 0.32911 0.26583E-01 +0.50000 0.10000 4.4372 0.31379 0.17121E-01 +0.50000 0.10000 14.346 0.31391 0.25744E-01 +0.50000 0.10000 24.689 0.42802 0.27404E-01 +0.50000 0.10000 34.544 0.54131 0.15407E-01 +0.50000 0.10000 44.450 0.58172 0.34260E-01 +0.50000 0.10000 54.525 0.77301 0.63414E-01 +0.50000 0.10000 64.209 0.69427 0.25708E-01 +0.50000 0.10000 74.096 0.64981 0.27404E-01 +0.50000 0.10000 84.099 0.91055 0.98585E-01 +0.50000 0.10000 94.480 0.99036 0.37741E-01 +0.50000 0.10000 104.72 0.96388 0.32564E-01 +0.50000 0.10000 124.75 0.79692 0.83142E-01 +0.50000 0.10000 134.60 0.66416 0.48882E-01 +0.50000 0.10000 143.73 0.61461 0.71983E-01 +0.50000 0.10000 144.62 0.42694 0.18014E-01 +0.50000 0.10000 146.37 0.44809 0.12854E-01 +0.50000 0.10000 149.81 0.41697 0.13675E-01 +0.90000 0.30000 -176.19 0.29842 0.60847E-01 +0.90000 0.30000 -166.14 0.31321 0.31693E-01 +0.90000 0.30000 -156.41 0.45568 0.68556E-01 +0.90000 0.30000 -145.81 0.48072 0.58246E-01 +0.90000 0.30000 -135.92 0.70202 0.65955E-01 +0.90000 0.30000 -126.18 0.84621 0.72823E-01 +0.90000 0.30000 -116.67 0.89702 0.83071E-01 +0.90000 0.30000 -106.41 1.1440 0.78804E-01 +0.90000 0.30000 -94.701 1.1964 0.61688E-01 +0.90000 0.30000 -86.141 1.2044 0.67669E-01 +0.90000 0.30000 -75.626 1.1660 0.86513E-01 +0.90000 0.30000 -65.886 1.0712 0.11138 +0.90000 0.30000 -55.421 0.68837 0.17972E-01 +0.90000 0.30000 -45.979 0.67835 0.68540E-01 +0.90000 0.30000 -35.648 0.55603 0.32549E-01 +0.90000 0.30000 -25.729 0.49628 0.32549E-01 +0.90000 0.30000 -15.422 0.51276 0.30806E-01 +0.90000 0.30000 -4.8382 0.44012 0.39387E-01 +0.90000 0.30000 4.4260 0.44297 0.28282E-01 +0.90000 0.30000 15.148 0.54082 0.46270E-01 +0.90000 0.30000 24.959 0.50765 0.21429E-01 +0.90000 0.30000 34.786 0.62099 0.56518E-01 +0.90000 0.30000 44.291 0.71892 0.59975E-01 +0.90000 0.30000 53.935 0.84427 0.75393E-01 +0.90000 0.30000 63.923 0.94132 0.92540E-01 +0.90000 0.30000 73.777 1.1078 0.55646E-01 +0.90000 0.30000 83.493 1.1037 0.59944E-01 +0.90000 0.30000 93.342 1.0303 0.74552E-01 +0.90000 0.30000 103.57 1.0314 0.49696E-01 +0.90000 0.30000 113.85 1.0907 0.56564E-01 +0.90000 0.30000 124.48 0.93150 0.56549E-01 +0.90000 0.30000 133.95 0.97374 0.50553E-01 +0.90000 0.30000 144.21 0.83772 0.59103E-01 +0.90000 0.30000 154.34 0.72312 0.62529E-01 + 2.6000 1.2000 -150.41 0.23455 0.56568E-01 + 2.6000 1.2000 -130.68 0.42090 0.48872E-01 + 2.6000 1.2000 -110.90 0.65868 0.48872E-01 + 2.6000 1.2000 -90.141 0.81494 0.41997E-01 + 2.6000 1.2000 -70.698 0.99445 0.48872E-01 + 2.6000 1.2000 -50.808 0.95955 0.52300E-01 + 2.6000 1.2000 -29.887 0.64420 0.22267E-01 + 2.6000 1.2000 -9.6861 0.41293 0.36015E-01 + 2.6000 1.2000 10.728 0.38486 0.19713E-01 + 2.6000 1.2000 30.740 0.41255 0.48872E-01 + 2.6000 1.2000 49.768 0.52092 0.31712E-01 + 2.6000 1.2000 69.851 0.47743 0.36890E-01 + 2.6000 1.2000 90.951 0.44245 0.26552E-01 + 2.6000 1.2000 110.61 0.40929 0.36015E-01 + 2.6000 1.2000 130.18 0.32041 0.29998E-01 + 2.6000 1.2000 149.01 0.22728 0.29123E-01 + 2.6000 1.2000 159.17 0.18453 0.24838E-01 +ENDDATA 114 +ENDSUBENT 134 +SUBENT F0253005 20050627 20050831 F022 +BIB 3 4 +REACTION 1(3-LI-7(D,N+A)2-HE-4,PAR,POL/DA) + 2(3-LI-7(D,N+A)2-HE-4,PAR,POL/DA,,ASY) +MONITOR (2-HE-4(N,EL)2-HE-4,PAR,POL/DA) +STATUS (CURVE)Fig.5 +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG NO-DIM + 0.25 0.1 +ENDCOMMON 3 +DATA 7 50 +E E-ERR DATA 1DATA-ERR 1ANG DATA 2 +DATA-ERR2 +MEV MEV NO-DIM NO-DIM ADEG NO-DIM +NO-DIM +0.30000 0.10000 -.77000 0.12000 9.3618 0.69734E-01 +0.89457 +0.30000 0.10000 -.77000 0.12000 34.507 0.81819E-01 +0.83142 +0.30000 0.10000 -.77000 0.12000 44.829 0.18602 +0.57884 +0.30000 0.10000 -.77000 0.12000 54.494 0.28713 +0.67356 +0.30000 0.10000 -.77000 0.12000 65.343 0.16911 +0.79940 +0.30000 0.10000 -.77000 0.12000 84.302 0.33558 +0.64221 +0.30000 0.10000 -.77000 0.12000 94.647 0.44504 +0.64176 +0.30000 0.10000 -.77000 0.12000 104.24 0.43245 +0.63146 +0.30000 0.10000 -.77000 0.12000 114.60 0.34922 +0.64199 +0.30000 0.10000 -.77000 0.12000 130.05 0.39919 +0.97876 +0.30000 0.10000 -.77000 0.12000 154.80 0.37130 +0.85293 +0.30000 0.10000 -.77000 0.12000 175.13 0.16594 +0.10529 +0.50000 0.10000 -.51000 0.70000E-01 4.8051 0.24933E-01 +0.66120 +0.50000 0.10000 -.51000 0.70000E-01 29.938 0.22155 +0.64020 +0.50000 0.10000 -.51000 0.70000E-01 44.895 0.24394 +0.68270 +0.50000 0.10000 -.51000 0.70000E-01 60.477 0.22003 +0.66170 +0.50000 0.10000 -.51000 0.70000E-01 80.250 0.22924 +0.68295 +0.50000 0.10000 -.51000 0.70000E-01 95.674 0.34823 +0.58745 +0.50000 0.10000 -.51000 0.70000E-01 105.81 0.29450 +0.62995 +0.50000 0.10000 -.51000 0.70000E-01 130.20 0.33678 +0.71394 +0.50000 0.10000 -.51000 0.70000E-01 145.47 0.38119 +0.65095 +0.50000 0.10000 -.51000 0.70000E-01 165.58 0.19602 +0.68270 +0.50000 0.10000 -.51000 0.70000E-01 175.34 0.10872 +0.70319 +0.90000 0.30000 -.10000E-010.40000E-01 4.4229 0.52054E-02 +0.66936 +0.90000 0.30000 -.10000E-010.40000E-01 14.619 0.29397E-01 +0.64812 +0.90000 0.30000 -.10000E-010.40000E-01 24.614 0.15355E-01 +0.72219 +0.90000 0.30000 -.10000E-010.40000E-01 35.086 0.51201E-01 +0.68978 +0.90000 0.30000 -.10000E-010.40000E-01 44.806 0.25504E-01 +0.66909 +0.90000 0.30000 -.10000E-010.40000E-01 54.599 0.95446E-01 +0.65874 +0.90000 0.30000 -.10000E-010.40000E-01 65.539 -.65379E-01 +0.70040 +0.90000 0.30000 -.10000E-010.40000E-01 74.957 -.26208E-01 +0.67971 +0.90000 0.30000 -.10000E-010.40000E-01 85.430 -.30747E-01 +0.67998 +0.90000 0.30000 -.10000E-010.40000E-01 95.512 -.69244E-01 +0.62605 +0.90000 0.30000 -.10000E-010.40000E-01 104.81 -.53438E-01 +0.65902 +0.90000 0.30000 -.10000E-010.40000E-01 115.46 0.99288E-01 +0.70095 +0.90000 0.30000 -.10000E-010.40000E-01 125.27 0.50199E-01 +0.70095 +0.90000 0.30000 -.10000E-010.40000E-01 135.49 0.15941 +0.66881 +0.90000 0.30000 -.10000E-010.40000E-01 145.25 0.26443 +0.65874 +0.90000 0.30000 -.10000E-010.40000E-01 155.53 0.22272 +0.70095 +0.90000 0.30000 -.10000E-010.40000E-01 165.83 0.22670 +0.63723 +0.90000 0.30000 -.10000E-010.40000E-01 175.65 0.13723 +0.69033 + 2.5000 1.3000 -.37000 0.80000E-01 10.153 -.41807E-01 +0.67899 + 2.5000 1.3000 -.37000 0.80000E-01 29.807 -.22482 +0.62646 + 2.5000 1.3000 -.37000 0.80000E-01 50.391 -.30706 +0.65777 + 2.5000 1.3000 -.37000 0.80000E-01 70.097 -.35308 +0.68961 + 2.5000 1.3000 -.37000 0.80000E-01 90.080 -.30144 +0.72145 + 2.5000 1.3000 -.37000 0.80000E-01 110.33 -.23814 +0.66811 + 2.5000 1.3000 -.37000 0.80000E-01 130.55 -.13979 +0.61611 + 2.5000 1.3000 -.37000 0.80000E-01 150.42 0.14889E-01 +0.64795 + 2.5000 1.3000 -.37000 0.80000E-01 170.60 0.23325 +0.71110 +ENDDATA 104 +ENDSUBENT 117 +ENDENTRY 5 diff --git a/exforall/F02/F0256.x4 b/exforall/F02/F0256.x4 index a8edbf9e1..0f8aafda4 100644 --- a/exforall/F02/F0256.x4 +++ b/exforall/F02/F0256.x4 @@ -1,30 +1,899 @@ -ENTRY F0256 19990508 20000121 -SUBENT F0256001 19990508 20000121 -BIB 9 17 -TITLE Measurement of the Be-7(p,g)B-8 reaction cross section - low energies -AUTHOR (B.W.FILIPPONE,A.J.ELWYN,C.N.DAVIDS,D.D.KOETKE) -INSTITUTE (1USAANL) -REFERENCE (J,PRL,50,412,198302) -SAMPLE The target consisted of 81.2+-6.0 mCi of Be-7 (produced - the Li-7(p,n)Be-7 reaction) electrodeposited on a - 0.25-mm-diam circle. -FACILITY (DYNAM) -ERR-ANALYS (EN-ERR) Digitizing error - (DATA-ERR) Error from graphic bars (statistical) - and digitizing -DETECTOR (SOLST) Silicon surface-barrier detector with a 300-mm2 - active area and 23-mu-m depletion depth. -HISTORY (19850408C) - (19990409A) CNPD: corrected 4-dig. year - (19990507D) Entry deleted. New entry named T0042. -ENDBIB 17 +ENTRY F0256 20050415 20050831 F021 +SUBENT F0256001 20050415 20050831 F021 +BIB 8 10 +TITLE Nuclear matter density effects in monopole transitions. +AUTHOR (M.Pignanelli,S.Micheletti,R.De Leo,S.Brandenburg, + M.N.Harakeh) +INSTITUTE (2ITYMIL,2ITYBAU,2NEDGRN) +REFERENCE (J,PR/C,33,40,1986) +FACILITY (ISOCY,2ITYMIL) +DETECTOR (MAGSP)The QMG/2 magnetic spectrograph. +ERR-ANALYS (ANG-ERR-D)Digitizing error + (ERR-DIG)Digitizing error +HISTORY (20041001C) +ENDBIB 10 COMMON 1 3 -EN-ERR -MEV - 0.007 -ENDCOMMON 3 -ENDSUBENT 24 -NOSUBENT F0256002 19990508 20000121 -NOSUBENT F0256003 19990508 20000121 -ENDENTRY 3 +ERR-DIG +PER-CENT + 0.2 +ENDCOMMON 3 +ENDSUBENT 17 +SUBENT F0256002 20050415 20050831 F021 +BIB 2 2 +REACTION (12-MG-24(A,INL)12-MG-24,PAR,DA) +STATUS (CURVE)Fig.1,9 +ENDBIB 2 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.17 +ENDCOMMON 3 +DATA 4 113 +E-LVL EN ANG-CM DATA-CM +MEV MEV ADEG MB/SR + 1.3700 120.00 4.8611 87.798 + 1.3700 120.00 5.5433 150.09 + 1.3700 120.00 6.8836 191.39 + 1.3700 120.00 8.2141 173.45 + 1.3700 120.00 9.0347 111.76 + 1.3700 120.00 10.180 53.728 + 1.3700 120.00 11.145 15.860 + 1.3700 120.00 12.478 15.465 + 1.3700 120.00 13.668 35.415 + 1.3700 120.00 14.848 56.252 + 1.3700 120.00 16.179 52.240 + 1.3700 120.00 17.170 38.021 + 1.3700 120.00 18.318 19.666 + 1.3700 120.00 19.301 10.945 + 1.3700 120.00 20.467 10.937 + 1.3700 120.00 21.646 16.545 + 1.3700 120.00 22.987 21.619 + 1.3700 120.00 24.154 21.603 + 1.3700 120.00 25.148 17.763 + 1.3700 120.00 26.306 12.927 + 1.3700 120.00 27.464 9.6398 + 1.3700 120.00 28.630 9.6329 + 1.3700 120.00 29.633 10.613 + 1.3700 120.00 30.968 11.135 + 1.3700 120.00 32.135 11.402 + 1.3700 120.00 33.464 9.8413 + 1.3700 120.00 34.460 8.4963 + 1.3700 120.00 35.622 7.1576 + 1.3700 120.00 36.450 6.0311 + 1.3700 120.00 37.949 5.7386 + 1.3700 120.00 38.945 5.0766 + 1.3700 120.00 40.610 4.8300 + 1.3700 120.00 43.934 3.5103 + 1.3700 120.00 46.421 2.2050 + 1.3700 120.00 48.745 1.6036 + 1.3700 120.00 50.737 1.2247 + 1.3700 120.00 52.895 0.91272 + 1.3700 120.00 55.218 0.63215 + 1.3700 120.00 57.374 0.43788 + 1.3700 120.00 59.699 0.32630 + 1.3700 120.00 61.854 0.22057 + 1.3700 120.00 64.177 0.15277 + 1.3700 120.00 67.324 0.77019E-01 + 1.3700 120.00 70.474 0.43865E-01 + 1.3700 120.00 73.627 0.27543E-01 + 6.4300 40.000 7.0917 2.8317 + 6.4300 40.000 9.2657 0.61681 + 6.4300 40.000 10.103 0.34829 + 6.4300 40.000 11.561 0.75899 + 6.4300 40.000 12.325 1.8551 + 6.4300 40.000 14.639 2.9795 + 6.4300 40.000 16.748 3.1490 + 6.4300 40.000 18.987 1.7426 + 6.4300 40.000 23.261 0.35115 + 6.4300 40.000 24.863 0.48463 + 6.4300 40.000 26.475 0.77881 + 6.4300 40.000 28.066 0.92308 + 6.4300 40.000 29.452 0.71997 + 6.4300 40.000 31.368 0.59428 + 6.4300 40.000 32.558 0.34191 + 6.4300 40.000 34.817 0.25170 + 6.4300 40.000 36.574 0.26109 + 6.4300 40.000 38.169 0.32763 + 6.4300 40.000 41.894 0.58915 + 6.4300 40.000 43.994 0.54503 + 6.4300 40.000 47.299 0.36450 + 6.4300 40.000 50.432 0.25812 + 6.4300 40.000 54.455 0.21678 + 6.4300 120.00 5.0815 1.1501 + 6.4300 120.00 6.6676 1.2903 + 6.4300 120.00 7.9745 4.5437 + 6.4300 120.00 8.6956 6.1924 + 6.4300 120.00 10.059 3.2630 + 6.4300 120.00 12.273 1.1218 + 6.4300 120.00 13.338 1.3606 + 6.4300 120.00 14.425 2.3850 + 6.4300 120.00 15.657 2.5254 + 6.4300 120.00 16.703 2.2904 + 6.4300 120.00 17.893 1.2307 + 6.4300 120.00 19.260 0.68733 + 6.4300 120.00 20.125 0.56585 + 6.4300 120.00 21.214 1.0113 + 6.4300 120.00 22.622 1.0916 + 6.4300 120.00 23.495 1.0293 + 6.4300 120.00 25.037 0.56373 + 6.4300 120.00 25.896 0.42123 + 6.4300 120.00 27.079 0.20544 + 6.4300 120.00 27.942 0.16588 + 6.4300 120.00 29.178 0.18616 + 6.4300 120.00 30.599 0.24871 + 6.4300 120.00 32.002 0.24367 + 6.4300 120.00 32.677 0.15900 + 6.4300 120.00 34.430 0.15574 + 6.4300 120.00 35.300 0.13855 + 6.4300 120.00 36.182 0.14962 + 6.4300 120.00 37.061 0.15542 + 6.4300 120.00 38.290 0.15832 + 6.4300 120.00 39.333 0.13547 + 6.4300 120.00 40.553 0.11817 + 6.4300 120.00 41.950 0.10714 + 6.4300 120.00 44.047 0.93400E-01 + 6.4300 120.00 46.304 0.64515E-01 + 6.4300 120.00 48.569 0.50059E-01 + 6.4300 120.00 51.189 0.41962E-01 + 6.4300 120.00 53.273 0.29556E-01 + 6.4300 120.00 55.187 0.22939E-01 + 6.4300 120.00 57.625 0.17120E-01 + 6.4300 120.00 59.883 0.12057E-01 + 6.4300 120.00 62.311 0.77061E-02 + 6.4300 120.00 63.879 0.64648E-02 + 6.4300 120.00 66.979 0.25438E-02 + 6.4300 120.00 70.288 0.17220E-02 + 6.4300 120.00 72.895 0.11663E-02 +ENDDATA 115 +ENDSUBENT 126 +SUBENT F0256003 20050415 20050831 F021 +BIB 2 2 +REACTION (6-C-12(P,EL)6-C-12,,DA,,RTH) +STATUS (CURVE)Fig.4 +ENDBIB 2 +COMMON 2 3 +EN ANG-ERR-D +MEV ADEG + 35.0 0.32 +ENDCOMMON 3 +DATA 2 34 +ANG-CM DATA-CM +ADEG NO-DIM + 8.6181 3.2591 + 15.163 8.5062 + 20.192 15.535 + 26.446 20.653 + 31.144 22.085 + 36.258 22.119 + 40.591 18.424 + 44.946 15.131 + 46.927 13.773 + 52.425 13.657 + 58.292 16.482 + 62.984 19.345 + 68.087 21.461 + 73.182 22.301 + 78.291 22.335 + 82.625 20.506 + 87.754 17.481 + 92.492 14.907 + 98.016 13.322 + 102.31 12.364 + 108.23 11.581 + 113.46 11.376 + 118.52 10.858 + 122.47 10.553 + 127.14 9.7901 + 131.81 9.5228 + 136.67 9.2619 + 141.72 9.1782 + 146.46 9.1810 + 151.19 9.2711 + 155.42 8.6036 + 160.25 8.1343 + 164.91 7.1346 + 170.01 6.2573 +ENDDATA 36 +ENDSUBENT 47 +SUBENT F0256004 20050415 20050831 F021 +BIB 2 2 +REACTION (12-MG-24(P,EL)12-MG-24,,DA,,RTH) +STATUS (CURVE)Fig.4 +ENDBIB 2 +COMMON 2 3 +EN ANG-ERR-D +MEV ADEG + 35.0 0.32 +ENDCOMMON 3 +DATA 2 30 +ANG-CM DATA-CM +ADEG NO-DIM + 19.042 8.0456 + 22.574 8.2709 + 26.513 8.0476 + 32.055 6.8876 + 37.210 5.7612 + 42.674 6.7959 + 49.698 8.4702 + 55.973 9.0334 + 61.881 8.6700 + 68.203 7.6274 + 71.373 6.8966 + 74.534 6.4686 + 78.076 6.3810 + 83.573 6.5902 + 88.279 6.9321 + 93.396 6.7762 + 100.09 6.4741 + 106.41 5.7480 + 112.33 5.1739 + 117.85 4.9430 + 124.14 4.9440 + 130.03 5.0596 + 136.73 4.7899 + 142.64 4.5345 + 148.15 4.4123 + 153.67 4.2154 + 158.00 4.1016 + 162.33 3.9545 + 166.68 3.5922 + 171.02 3.4004 +ENDDATA 32 +ENDSUBENT 43 +SUBENT F0256005 20050415 20050831 F021 +BIB 2 2 +REACTION (14-SI-28(P,EL)14-SI-28,,DA,,RTH) +STATUS (CURVE)Fig.4 +ENDBIB 2 +COMMON 2 3 +EN ANG-ERR-D +MEV ADEG + 35.0 0.32 +ENDCOMMON 3 +DATA 2 25 +ANG-CM DATA-CM +ADEG NO-DIM + 14.978 2.5775 + 20.807 4.5074 + 27.525 3.9117 + 33.539 1.8884 + 39.436 2.0599 + 45.201 5.6119 + 51.839 8.5071 + 59.330 8.1614 + 67.275 5.1720 + 72.446 3.6729 + 78.355 3.6770 + 84.227 4.7620 + 90.904 5.5011 + 96.833 4.7734 + 102.39 3.5387 + 109.15 2.3740 + 115.10 1.8112 + 122.20 1.6175 + 130.09 1.5743 + 136.01 1.4673 + 142.31 1.4276 + 147.82 1.4706 + 153.33 1.5588 + 160.04 1.3920 + 166.38 1.1408 +ENDDATA 27 +ENDSUBENT 38 +SUBENT F0256006 20050415 20050831 F021 +BIB 2 2 +REACTION (12-MG-24(P,INL)12-MG-24,PAR,DA) +STATUS (CURVE)Fig.5,8 +ENDBIB 2 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.3 +ENDCOMMON 3 +DATA 5 198 +E-LVL EN ANG-CM DATA-CM DATA-ERR +MEV MEV ADEG MB/SR MB/SR + 1.3700 35.000 15.840 20.872 + 1.3700 35.000 21.224 19.732 + 1.3700 35.000 25.839 18.919 + 1.3700 35.000 31.224 17.634 + 1.3700 35.000 36.999 15.099 + 1.3700 35.000 41.637 9.8793 + 1.3700 35.000 46.276 6.2836 + 1.3700 35.000 52.059 4.7368 + 1.3700 35.000 61.682 3.7268 + 1.3700 35.000 67.451 3.5234 + 1.3700 35.000 72.448 3.4753 + 1.3700 35.000 77.076 2.6948 + 1.3700 35.000 82.874 1.5746 + 1.3700 35.000 87.120 1.1702 + 1.3700 35.000 92.900 0.90744 + 1.3700 35.000 97.141 0.73413 + 1.3700 35.000 102.15 0.59396 + 1.3700 35.000 107.54 0.55363 + 1.3700 35.000 112.92 0.54609 + 1.3700 35.000 122.95 0.29739 + 1.3700 35.000 132.97 0.19744 + 1.3700 35.000 141.81 0.19481 + 1.3700 35.000 151.39 0.30233 + 1.3700 35.000 161.40 0.24470 + 6.4300 24.800 10.189 1.9824 + 6.4300 24.800 15.380 1.2936 + 6.4300 24.800 19.665 0.72350 + 6.4300 24.800 25.857 0.30781 + 6.4300 24.800 30.594 0.18755 0.15386 + 6.4300 24.800 35.756 0.14525 0.14192 + 6.4300 24.800 40.865 0.15572 + 6.4300 24.800 47.829 0.17283 + 6.4300 24.800 51.561 0.16432 + 6.4300 24.800 56.723 0.12725 + 6.4300 24.800 61.928 0.76229 + 6.4300 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0.17750E-01 + 7.6500 29.500 43.514 0.22973 0.20116E-01 + 7.6500 29.500 48.507 0.27137 0.27555E-01 + 7.6500 29.500 53.444 0.25483 + 7.6500 29.500 59.614 0.23557 + 7.6500 29.500 64.580 0.25001 + 7.6500 29.500 70.380 0.27350 + 7.6500 29.500 74.475 0.24166 + 7.6500 29.500 80.237 0.22687 + 7.6500 29.500 84.756 0.20984 + 7.6500 29.500 90.101 0.19403 + 7.6500 29.500 94.992 0.15165 + 7.6500 29.500 99.500 0.13398 + 7.6500 29.500 104.81 0.10631 + 7.6500 29.500 109.28 0.83104E-01 + 7.6500 29.500 114.60 0.67993E-01 + 7.6500 29.500 118.71 0.64852E-01 + 7.6500 29.500 123.66 0.63760E-01 + 7.6500 29.500 129.49 0.80045E-01 + 7.6500 29.500 133.25 0.94593E-01 + 7.6500 29.500 138.67 0.11877 + 7.6500 29.500 142.83 0.13404 + 7.6500 29.500 147.39 0.14896 + 7.6500 29.500 152.34 0.14645 + 7.6500 29.500 157.67 0.12935 + 7.6500 29.500 161.75 0.10426 + 7.6500 29.500 165.79 0.74366E-01 + 7.6500 29.500 169.39 0.47662E-01 + 7.6500 35.200 9.8627 1.8817 0.10714 + 7.6500 35.200 15.488 1.0418 0.92537E-01 + 7.6500 35.200 20.701 0.57686 0.59327E-01 + 7.6500 35.200 26.727 0.30482 0.27034E-01 + 7.6500 35.200 31.202 0.23746 0.27699E-01 + 7.6500 35.200 36.237 0.32826 + 7.6500 35.200 42.886 0.39443 + 7.6500 35.200 47.857 0.42546 + 7.6500 35.200 52.368 0.38108 + 7.6500 35.200 57.300 0.35202 + 7.6500 35.200 63.473 0.33011 + 7.6500 35.200 68.825 0.31450 + 7.6500 35.200 72.959 0.32392 + 7.6500 35.200 78.303 0.29918 + 7.6500 35.200 83.234 0.27637 + 7.6500 35.200 88.543 0.22201 + 7.6500 35.200 93.426 0.17027 + 7.6500 35.200 97.917 0.14113 + 7.6500 35.200 102.79 0.10493 + 7.6500 35.200 108.07 0.74463E-01 + 7.6500 35.200 113.41 0.66675E-01 + 7.6500 35.200 117.52 0.62573E-01 + 7.6500 35.200 122.47 0.64427E-01 + 7.6500 35.200 127.06 0.76282E-01 + 7.6500 35.200 131.25 0.99137E-01 + 7.6500 35.200 137.09 0.12678 + 7.6500 35.200 142.07 0.14106 + 7.6500 35.200 146.21 0.14756 + 7.6500 35.200 150.75 0.14731 + 7.6500 35.200 156.10 0.13819 + 7.6500 35.200 160.17 0.11456 + 7.6500 35.200 165.06 0.87858E-01 + 7.6500 35.200 169.10 0.64338E-01 + 7.6500 39.900 21.774 0.51471 0.60043E-01 + 7.6500 39.900 27.467 0.31784 0.23709E-01 + 7.6500 39.900 32.925 0.54616 + 7.6500 39.900 38.326 0.67768 0.50551E-01 + 7.6500 39.900 43.682 0.64603 0.48131E-01 + 7.6500 39.900 49.430 0.54397 + 7.6500 39.900 53.926 0.42399 + 7.6500 39.900 59.657 0.32529 + 7.6500 39.900 64.999 0.28697 + 7.6500 39.900 70.366 0.29107 + 7.6500 39.900 74.894 0.27326 + 7.6500 39.900 79.830 0.24869 + 7.6500 39.900 85.167 0.21269 + 7.6500 39.900 90.491 0.16834 + 7.6500 39.900 94.981 0.12720 + 7.6500 39.900 101.12 0.94602E-01 + 7.6500 39.900 105.21 0.77255E-01 + 7.6500 39.900 110.11 0.57473E-01 + 7.6500 39.900 115.45 0.49922E-01 + 7.6500 39.900 119.99 0.50646E-01 + 7.6500 39.900 125.38 0.56378E-01 + 7.6500 39.900 130.36 0.68885E-01 + 7.6500 39.900 134.92 0.79113E-01 + 7.6500 39.900 139.09 0.98193E-01 + 7.6500 39.900 143.23 0.10437 + 7.6500 39.900 148.18 0.10753 + 7.6500 39.900 152.72 0.10909 + 7.6500 39.900 157.67 0.10400 + 7.6500 39.900 161.76 0.87608E-01 + 7.6500 39.900 166.68 0.69345E-01 + 7.6500 39.900 170.77 0.58413E-01 +ENDDATA 132 +ENDSUBENT 144 +SUBENT F0256009 20050415 20050831 F021 +BIB 2 2 +REACTION (6-C-12(A,INL)6-C-12,PAR,DA) +STATUS (CURVE)Fig.7 +ENDBIB 2 +COMMON 3 3 +EN E-LVL ANG-ERR-D +MEV MEV ADEG + 120. 7.65 0.17 +ENDCOMMON 3 +DATA 2 39 +ANG-CM DATA-CM +ADEG MB/SR + 5.0761 3.7961 + 6.3460 1.3967 + 7.8036 2.4282 + 9.1034 5.0466 + 10.234 6.3630 + 11.840 5.5144 + 12.958 3.4049 + 14.235 1.9227 + 15.516 1.3213 + 16.969 1.7576 + 18.260 2.2160 + 19.870 2.3371 + 20.994 2.0256 + 22.278 1.7245 + 23.879 1.0839 + 24.997 0.69354 + 26.282 0.58001 + 27.734 0.75784 + 29.184 0.85843 + 30.634 0.93828 + 31.760 0.92146 + 33.205 0.77059 + 34.490 0.69214 + 35.615 0.62169 + 36.738 0.53884 + 39.474 0.56815 + 42.045 0.46661 + 44.617 0.39012 + 47.346 0.27775 + 49.915 0.20864 + 52.319 0.12207 + 55.211 0.95021E-01 + 57.776 0.55594E-01 + 60.182 0.36856E-01 + 62.909 0.21951E-01 + 65.149 0.10744E-01 + 66.581 0.42457E-02 + 69.152 0.36787E-02 + 71.238 0.26667E-02 +ENDDATA 41 +ENDSUBENT 52 +SUBENT F0256010 20050415 20050831 F021 +BIB 2 2 +REACTION (12-MG-24(A,EL)12-MG-24,,DA) +STATUS (CURVE)Fig.9 +ENDBIB 2 +COMMON 2 3 +EN ANG-ERR-D +MEV ADEG + 120. 0.1 +ENDCOMMON 3 +DATA 2 46 +ANG-CM DATA-CM +ADEG MB/SR + 4.7435 14854. + 5.5670 11132. + 7.0209 3045.8 + 8.1290 595.80 + 9.2248 83.311 + 10.280 368.21 + 11.467 623.51 + 12.799 593.71 + 13.782 358.54 + 14.918 151.08 + 16.206 42.344 + 17.365 33.286 + 18.383 53.732 + 19.565 78.793 + 20.895 69.819 + 21.882 48.688 + 23.030 28.022 + 24.014 17.754 + 25.015 17.740 + 26.689 20.957 + 27.692 22.503 + 29.026 21.948 + 30.352 17.250 + 31.345 13.891 + 32.170 10.922 + 33.330 9.0077 + 34.327 7.9839 + 35.661 7.9758 + 36.491 7.0702 + 37.821 6.2649 + 38.982 5.1667 + 40.310 4.3639 + 41.471 3.6863 + 43.959 2.5069 + 46.276 1.5124 + 48.434 1.1323 + 50.753 0.71667 + 53.242 0.49920 + 55.229 0.33961 + 58.052 0.23650 + 60.038 0.15708 + 62.191 0.10185 + 64.011 0.67654E-01 + 67.323 0.35318E-01 + 70.640 0.20787E-01 + 73.787 0.11116E-01 +ENDDATA 48 +ENDSUBENT 59 +ENDENTRY 10 diff --git a/exforall/F02/F0258.x4 b/exforall/F02/F0258.x4 new file mode 100644 index 000000000..5fcc9fa30 --- /dev/null +++ b/exforall/F02/F0258.x4 @@ -0,0 +1,112 @@ +ENTRY F0258 20050623 20050831 F021 +SUBENT F0258001 20050623 20050831 F021 +BIB 9 21 +TITLE An investigation of oxygen indiffusion during laser + cleaning/annealing of silicon by means of the + 16O(a,a0)16O resonance scattering. +AUTHOR (Z.L.Wang,J.F.M.Westendorp,F.W.Saris) +INSTITUTE (2NEDNED) FOM-Institute for Atomic and Molecular + Physics +REFERENCE (J,NIM,211,193,1983) +FACILITY (VDG,2NEDUTR) 3.8 MV Van de Graff accelerator +INC-SPECT Energy stability of the ion beam is better than 250 eV + at 2 MeV. The energy spread for 2MeV He+ is about + 200 eV. +SAMPLE Series of Si<100> samples, having CVD-grown oxide + layers on the front surface, was used. The oxygen + densities of these layers were measured with RBS at + 2 MeV. Samples were mounted on a three-axis goniometer, + allowing channeling experiments. +DETECTOR (SIBAR) Surface barrier detector has an energy + resolution of 20 keV and a solid angle about 5 msr. + The scattering angle could be varied from 100 to + 173 degrees. +HISTORY (20050207C) +ENDBIB 21 +NOCOMMON 0 0 +ENDSUBENT 24 +SUBENT F0258002 20050623 20050831 F021 +BIB 4 6 +REACTION (8-O-16(A,EL)8-O-16,,DA,,REL) +SAMPLE Thickness of target was 177angstroem, areal density was + (8.14+-0.31)*10**16 at/cm2. +ERR-ANALYS (EN-ERR-DIG) Digitizing error + (ERR-DIG) Digitizing error +STATUS (CURVE)Fig.1 +ENDBIB 6 +COMMON 3 3 +ANG EN-ERR-DIG ERR-DIG +ADEG KEV ARB-UNITS + 164. 0.1 0.2 +ENDCOMMON 3 +DATA 2 11 +EN DATA +KEV ARB-UNITS + 3028.9 30.765 + 3032.9 39.304 + 3035.9 53.771 + 3038.8 75.309 + 3040.7 100.91 + 3042.6 119.06 + 3044.7 115.66 + 3046.7 84.322 + 3048.8 53.589 + 3050.5 35.531 + 3054.7 14.851 +ENDDATA 13 +ENDSUBENT 28 +SUBENT F0258003 20050623 20050831 F021 +BIB 6 12 +REACTION 1(8-O-16(A,0),,EN) + 2(8-O-16(A,TOT),,WID) +SAMPLE Thickness of target was 177angstroem, areal density was + (8.14+-0.31)*10**16 at/cm2. +METHOD Scattering angle in these measurements was fixed at 164 + degrees. +ANALYSIS Rutherford background was substracted. In the + calculation of resonance energy the energy loss over + the oxide layer was taken into account. +ERR-ANALYS (DATA-ERR) Estimated uncertainty in the energy + calibration of the accelerator +STATUS Data from text. +ENDBIB 12 +NOCOMMON 0 0 +DATA 4 1 +DATA 1DATA-ERR 1DATA 2DATA-ERR 2 +KEV KEV KEV KEV + 3042.0 3.0000 10.200 0.40000 +ENDDATA 3 +ENDSUBENT 20 +SUBENT F0258004 20050623 20050831 F021 +BIB 4 16 +REACTION (8-O-16(A,EL)8-O-16,,DA,,AV) +FLAG (1.) Thickness of target was 261 angstroem, areal + density was (1.2+-0.03)*10**17 at/cm2, energy loss was + 5.3 keV, energy straggling was 1.27 keV. + (2.) Thickness of target was 177 angstroem, areal + density was (8.14+-0.31)*10**16, energy loss was 3.6 + keV, energy straggling was 1.02 keV. + (3.) Thickness of target was 90 angstroem, areal + density was (4.15+-0.14)*10**16, energy loss was 1.8 + keV, energy straggling was 0.76 keV. +ANALYSIS Nuclear resonance cross section is averaged over the + thickness analysed. This averaged cross section was + measured by comparing the 16O(a,a0)16 yield at the + resonance energy with that at 2MeV,i.e. for Rutherford + backscattering using the standard samples. +STATUS (TABLE)Table 2 +ENDBIB 16 +COMMON 2 3 +ANG EN +ADEG MEV + 164. 2. +ENDCOMMON 3 +DATA 2 3 +DATA FLAG +B/SR NO-DIM +0.74000 1.0000 +0.72100 2.0000 +0.72900 3.0000 +ENDDATA 5 +ENDSUBENT 30 +ENDENTRY 4 diff --git a/exforall/F02/F0259.x4 b/exforall/F02/F0259.x4 index 6582b55fe..05c5739b8 100644 --- a/exforall/F02/F0259.x4 +++ b/exforall/F02/F0259.x4 @@ -1,28 +1,1151 @@ -ENTRY F0259 19990508 20000121 -SUBENT F0259001 19990508 20000121 -BIB 10 15 -TITLE Polarization and cross section measurements of - the 9Be(3He,p)11B reaction -AUTHOR (J.POULIOT,R.ROY,P.BRICAULT,L.POTVIN,R.J.SLOBODRIAN) -INSTITUTE (1CANLUQ) -REFERENCE (J,CJP,61,1609,198312) -SAMPLE Target of 9Be, 710 mu-g/cm2 thick. -FACILITY (VDG) -METHOD (EDE) -ERR-ANALYS (DATA-ERR) Absolute error - (DATA-ERR1) Error from graphic bars (statistical in - a few points) and digitizing -DETECTOR (TELES) -HISTORY (19850408C) - (19990409A) CNPD: corrected 4-dig. year - (19990507D) Entry deleted. New entry named T0043. -ENDBIB 15 -COMMON 1 3 -DATA-ERR -PER-CENT - 5. +ENTRY F0259 20050418 20050831 F021 +SUBENT F0259001 20050418 20050831 F021 +BIB 8 20 +TITLE Study of 190Ir via single-proton and single-neutron + transfer reaction. +AUTHOR (P.E.Carrett,D.G.Burke) +INSTITUTE (1CANMCM) + (2SWTFRS) +REFERENCE (J,NP/A,581,267,1995) +FACILITY (VDGT,1CANMCM) +SAMPLE All targets were produced by vacuum evaporation of + metal samples onto carbon foil backings of thickness + about 30 mu-g/cm2. Compositions of metal samples were + indicated by supplier. +DETECTOR (MAGSP) + Products of reactions were analysed by Enge + split-pole magnetic spectrograph and detected with + photographic plates placed in focal plane. + (SIBAR) Surface barrier detector was placed at an angle + of 30 degrees to beam direction. It recorded numbers + of elastic-scattering events to determine absolute + cross sections. +HISTORY (20041125C) +ENDBIB 20 +NOCOMMON 0 0 +ENDSUBENT 23 +SUBENT F0259002 20050418 20050831 F021 +BIB 4 9 +REACTION (77-IR-191(D,T)77-IR-190,PAR,DA) +SAMPLE Targets enriched to either 94.66% or 96.19% 191Ir with + the thickness of 30 and 45 mu-g/cm**2 respectively were + used. +ERR-ANALYS (E-LVL-ERR) Uncertainty includes both statistical error + on mean and error due to calibration of spectrograph. + (DATA-ERR) Uncertainty is addition in quadrature of + statistical uncertainty plus reproducilibity error. +STATUS (TABLE) Table 1 +ENDBIB 9 +COMMON 3 3 +EN EN-RSL ANG +MEV KEV ADEG + 18. 5.7 45. ENDCOMMON 3 -ENDSUBENT 22 -NOSUBENT F0259002 19990508 20000121 -NOSUBENT F0259003 19990508 20000121 -ENDENTRY 3 +DATA 4 62 +E-LVL-MEAN E-LVL-ERR DATA DATA-ERR +KEV KEV MU-B/SR MU-B/SR + 0.0000 74.000 9.0000 + 25.900 0.10000 176.00 19.000 + 38.100 0.20000 23.000 4.0000 + 83.000 0.10000 560.00 70.000 + 144.00 0.20000 37.000 5.0000 + 173.80 0.20000 260.00 60.000 + 183.20 0.40000 90.000 12.000 + 198.90 0.20000 140.00 16.000 + 223.40 0.20000 477.00 50.000 + 241.70 0.60000 13.000 3.0000 + 266.80 0.30000 121.00 14.000 + 278.90 0.30000 119.00 15.000 + 284.90 0.30000 49.000 10.000 + 313.40 0.40000 97.000 15.000 + 331.70 0.40000 52.000 5.0000 + 347.80 0.40000 282.00 30.000 + 366.70 0.40000 106.00 15.000 + 375.70 0.40000 39.000 8.0000 + 408.00 0.40000 29.000 4.0000 + 426.70 0.40000 48.000 6.0000 + 441.70 0.50000 72.000 10.000 + 452.30 0.60000 16.000 6.0000 + 478.50 0.50000 84.000 11.000 + 485.80 0.50000 210.00 23.000 + 496.40 0.50000 144.00 15.000 + 510.90 0.50000 188.00 21.000 + 542.50 0.70000 36.000 5.0000 + 589.30 0.60000 256.00 47.000 + 602.70 0.60000 194.00 21.000 + 612.80 0.70000 155.00 17.000 + 619.10 0.70000 42.000 6.0000 + 633.00 0.70000 15.000 4.0000 + 655.30 0.70000 25.000 4.0000 + 669.00 0.70000 73.000 10.000 + 684.70 0.70000 150.00 17.000 + 705.20 0.80000 21.000 4.0000 + 722.10 0.70000 75.000 10.000 + 743.50 0.70000 92.000 10.000 + 755.70 0.80000 39.000 6.0000 + 772.50 1.1000 29.000 5.0000 + 787.50 0.90000 36.000 5.0000 + 794.90 0.90000 16.000 4.0000 + 806.20 0.90000 18.000 3.0000 + 823.60 0.90000 24.000 5.0000 + 835.90 0.90000 19.000 4.0000 + 843.50 0.90000 32.000 6.0000 + 862.00 1.0000 14.000 4.0000 + 902.10 1.0000 11.000 3.0000 + 929.40 1.0000 47.000 5.0000 + 960.10 1.0000 20.000 4.0000 + 971.20 1.0000 22.000 5.0000 + 993.20 1.1000 51.000 7.0000 + 1006.4 1.4000 15.000 3.0000 + 1014.8 1.4000 15.000 3.0000 + 1026.8 1.4000 30.000 5.0000 + 1034.4 1.6000 17.000 3.0000 + 1062.9 1.8000 11.000 3.0000 + 1082.8 1.2000 8.0000 3.0000 + 1092.4 1.5000 13.000 3.0000 + 1115.6 1.7000 10.000 3.0000 + 1135.9 1.9000 6.0000 4.0000 + 1143.0 1.8000 13.000 5.0000 +ENDDATA 64 +ENDSUBENT 82 +SUBENT F0259003 20050418 20050831 F021 +BIB 4 8 +REACTION (77-IR-191(D,T)77-IR-190,PAR,DA) +SAMPLE Targets enriched to either 94.66% or 96.19% 191Ir with + the thickness of 30 and 45 mu-g/cm**2 respectively were + used. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from graphic bars +STATUS (CURVE)FIG.4 a,b,c,d,e +ENDBIB 8 +COMMON 4 3 +EN EN-RSL ANG-ERR-D ERR-DIG +MEV KEV ADEG PER-CENT + 18. 5.7 0.1 0.1 +ENDCOMMON 3 +DATA 4 878 +E-LVL ANG DATA DATA-ERR +KEV ADEG MU-B/SR MU-B/SR + 0.0000 5.9550 13.406 3.7540 + 0.0000 7.9788 13.288 4.0236 + 0.0000 10.004 19.074 6.1334 + 0.0000 12.505 29.381 6.2896 + 0.0000 15.005 33.534 8.6861 + 0.0000 17.506 44.857 8.6507 + 0.0000 20.005 31.524 5.7494 + 0.0000 22.626 66.113 11.658 + 0.0000 25.126 63.820 11.715 + 0.0000 30.126 57.916 9.9616 + 0.0000 35.007 62.145 10.504 + 0.0000 40.127 83.126 12.595 + 0.0000 45.126 65.511 10.105 + 0.0000 50.126 56.887 9.7846 + 0.0000 60.125 42.519 7.4972 + 0.0000 70.005 32.061 6.1831 + 25.900 5.8990 140.23 24.171 + 25.900 7.9252 197.90 26.055 + 25.900 9.9496 218.08 28.747 + 25.900 12.449 199.62 32.349 + 25.900 14.946 135.31 19.174 + 25.900 17.445 110.42 13.439 + 25.900 19.946 121.68 19.719 + 25.900 22.447 158.59 28.986 + 25.900 24.948 185.91 24.477 + 25.900 29.949 203.05 26.733 + 25.900 35.067 161.34 19.637 + 25.900 40.067 184.17 58.210 + 25.900 44.948 177.74 21.633 + 25.900 49.947 143.76 27.467 + 25.900 59.944 91.577 13.905 + 25.900 69.942 68.393 9.6914 + 83.000 6.0456 404.90 41.012 + 83.000 8.0577 442.00 57.748 + 83.000 9.9519 536.05 70.036 + 83.000 12.437 540.75 70.650 + 83.000 15.040 411.99 53.828 + 83.000 17.525 370.82 48.448 + 83.000 20.010 367.56 48.023 + 83.000 22.496 486.64 73.317 + 83.000 24.982 595.39 71.910 + 83.000 29.952 600.58 72.537 + 83.000 34.922 495.14 59.802 + 83.000 39.893 564.71 73.780 + 83.000 44.863 564.66 79.398 + 83.000 49.833 430.19 51.958 + 83.000 59.773 319.20 35.429 + 83.000 69.594 198.74 24.004 + 144.00 6.0222 30.906 5.2838 + 144.00 8.0484 36.827 7.0591 + 144.00 10.075 49.181 7.4072 + 144.00 12.574 32.283 4.9542 + 144.00 15.075 29.056 4.8865 + 144.00 17.456 23.957 4.2029 + 144.00 20.077 25.921 3.5897 + 144.00 22.579 30.350 5.5018 + 144.00 25.082 36.164 5.4467 + 144.00 30.086 43.089 6.4896 + 144.00 35.087 32.541 5.9431 + 144.00 39.971 33.696 5.4165 + 144.00 45.094 36.777 5.9117 + 144.00 50.096 30.320 10.064 + 144.00 59.977 14.384 3.8013 + 144.00 69.981 10.766 2.8452 + 173.80 5.7815 100.90 14.065 + 173.80 7.9304 108.15 16.154 + 173.80 9.8422 132.10 15.818 + 173.80 12.349 144.08 20.085 + 173.80 14.855 139.13 18.021 + 173.80 17.361 145.29 20.253 + 173.80 19.868 150.41 18.011 + 173.80 22.378 203.91 28.426 + 173.80 25.004 230.28 43.768 + 173.80 30.017 240.44 33.518 + 173.80 34.910 257.68 28.358 + 173.80 39.923 278.58 73.130 + 173.80 44.934 257.51 64.266 + 173.80 49.944 212.58 91.819 + 173.80 59.966 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17.877 46.162 6.1034 + 722.10 20.481 45.348 14.380 + 722.10 22.967 55.608 10.207 + 722.10 25.452 66.399 10.125 + 722.10 30.423 77.885 12.676 + 722.10 35.393 62.390 10.154 + 722.10 40.364 73.183 13.434 + 722.10 45.216 71.255 12.335 + 722.10 50.185 42.974 6.1154 + 722.10 60.126 45.718 6.9712 + 722.10 69.947 31.774 5.5003 + 743.50 6.2866 55.189 8.2825 + 743.50 8.3130 70.504 12.011 + 743.50 10.338 96.591 12.571 + 743.50 12.850 81.122 39.002 + 743.50 15.365 60.285 9.2231 + 743.50 17.875 57.220 13.579 + 743.50 20.386 51.088 7.6670 + 743.50 22.891 62.477 9.3763 + 743.50 25.396 76.406 22.540 + 743.50 30.410 92.650 16.871 + 743.50 35.431 80.602 14.559 + 743.50 40.457 53.948 9.1903 + 743.50 45.465 88.825 11.560 + 743.50 50.367 73.326 7.3988 + 743.50 60.415 39.466 18.795 + 743.50 70.337 28.592 5.4097 + 755.70 6.4312 28.360 5.6406 + 755.70 8.4606 30.391 5.7312 + 755.70 10.489 38.710 6.9748 + 755.70 12.877 35.817 6.0252 + 755.70 15.505 29.878 4.7259 + 755.70 17.895 22.084 5.1881 + 755.70 20.401 29.626 5.5868 + 755.70 23.028 28.870 6.3973 + 755.70 25.415 32.026 6.8803 + 755.70 30.547 46.040 7.7450 + 755.70 35.564 37.104 7.2065 + 755.70 40.579 35.542 9.4989 + 755.70 45.593 37.438 7.0601 + 755.70 50.608 38.097 5.2703 + 755.70 60.519 33.478 5.3116 + 755.70 70.434 16.493 3.9830 + 772.50 6.4869 8.5891 3.4089 + 772.50 8.2823 5.8652 2.1674 + 772.50 10.437 12.140 3.1609 + 772.50 13.070 11.926 3.0268 + 772.50 15.344 8.7429 2.6117 + 772.50 17.977 11.821 3.7489 + 772.50 20.490 12.033 3.2896 + 772.50 23.004 9.2210 2.7053 + 772.50 25.637 16.125 3.4346 + 772.50 30.664 21.229 5.9401 + 772.50 35.571 24.905 4.5724 + 772.50 40.717 26.267 8.8013 + 772.50 45.625 27.703 5.3782 + 772.50 50.652 21.997 2.9108 + 772.50 60.586 13.746 3.9336 + 772.50 70.640 13.992 3.2695 + 787.50 6.5229 28.222 5.7502 + 787.50 8.4371 25.386 5.1722 + 787.50 10.588 46.689 9.9041 + 787.50 13.221 33.678 6.5053 + 787.50 15.494 32.510 9.2673 + 787.50 18.007 20.181 4.6967 + 787.50 20.638 29.503 6.4629 + 787.50 23.031 23.246 4.6048 + 787.50 25.542 29.506 6.3267 + 787.50 30.684 51.470 10.918 + 787.50 35.590 25.623 4.7095 + 787.50 40.614 28.239 7.3238 + 787.50 45.637 34.908 6.0137 + 787.50 50.423 20.015 3.2418 + 787.50 60.472 14.958 3.0685 + 787.50 70.402 9.0438 2.4044 + 794.90 6.4812 16.320 3.9997 + 794.90 8.6155 21.244 5.2182 + 794.90 10.516 18.298 7.8699 + 794.90 13.006 24.241 4.7803 + 794.90 15.505 11.590 3.3624 + 794.90 17.998 11.389 3.0883 + 794.90 20.487 15.766 4.3756 + 794.90 22.983 10.713 5.3613 + 794.90 25.475 12.440 3.4523 + 794.90 30.572 26.027 6.9679 + 794.90 35.443 16.486 4.0404 + 794.90 40.543 25.811 5.6289 + 794.90 45.413 15.924 3.7965 + 794.90 50.635 17.698 3.0324 + 794.90 60.489 12.680 3.0233 + 794.90 70.463 8.6187 2.3919 + 806.20 6.2464 3.8794 1.8112 + 806.20 8.3825 7.2134 2.1961 + 806.20 10.406 6.8407 2.4090 + 806.20 12.906 5.4340 2.3242 + 806.20 17.903 5.5325 1.9164 + 806.20 20.286 3.8479 2.2471 + 806.20 23.011 13.540 2.9746 + 806.20 25.509 13.784 3.3103 + 806.20 30.393 7.1575 2.7606 + 806.20 35.503 13.913 3.1524 + 806.20 40.499 15.616 6.3568 + 806.20 45.614 17.998 3.5757 + 806.20 50.383 6.1628 1.2679 + 806.20 60.492 9.6021 2.3703 + 806.20 70.373 4.4842 1.5533 + 823.60 6.4302 8.4252 2.4420 + 823.60 8.4516 8.5001 2.3679 + 823.60 10.352 11.159 2.8603 + 823.60 12.850 9.6978 2.6890 + 823.60 15.345 13.186 3.5723 + 823.60 17.844 10.224 2.5035 + 823.60 20.460 10.406 2.7523 + 823.60 22.953 19.237 4.5106 + 823.60 25.330 19.752 3.9977 + 823.60 30.442 23.341 4.7240 + 823.60 35.437 21.572 3.9147 + 823.60 40.430 25.943 6.0829 + 823.60 45.425 22.948 5.1330 + 823.60 50.423 12.201 3.7616 + 823.60 60.411 11.993 3.0942 + 823.60 70.397 15.611 3.2937 + 835.90 6.4421 14.513 3.1987 + 835.90 8.3449 11.388 2.7564 + 835.90 10.484 26.610 5.8648 + 835.90 12.981 19.823 5.4346 + 835.90 15.479 18.337 5.4401 + 835.90 17.976 17.110 4.4738 + 835.90 20.473 16.816 3.5294 + 835.90 22.970 17.561 5.8718 + 835.90 25.467 18.338 3.9486 + 835.90 30.579 29.273 5.5356 + 835.90 35.454 19.151 4.2209 + 835.90 40.567 31.923 6.3669 + 835.90 45.561 18.823 3.7950 + 835.90 50.555 23.989 3.8049 + 835.90 60.425 12.422 3.7877 + 835.90 70.413 9.9184 2.8428 + 843.50 6.4900 14.207 3.6049 + 843.50 8.2761 13.235 2.9103 + 843.50 10.180 15.119 4.2295 + 843.50 12.916 21.180 5.7891 + 843.50 15.419 12.114 4.4757 + 843.50 17.916 21.183 4.7933 + 843.50 20.416 21.755 4.4803 + 843.50 22.915 26.445 6.5343 + 843.50 25.533 35.126 5.7162 + 843.50 30.533 34.513 6.6986 + 843.50 35.534 27.900 4.3268 + 843.50 40.533 32.445 6.2207 + 843.50 45.533 31.598 6.0582 + 843.50 50.535 24.435 3.7894 + 843.50 60.534 27.187 4.7059 + 843.50 70.536 16.697 3.5557 + 862.00 6.4809 7.1443 2.1667 + 862.00 8.3862 4.2479 1.7225 + 862.00 10.517 7.0213 2.2570 + 862.00 12.893 5.9396 2.2817 + 862.00 17.992 8.5279 2.6901 + 862.00 20.374 4.2513 2.1509 + 862.00 23.092 11.512 9.0059 + 862.00 25.469 9.0752 2.4089 + 862.00 30.455 8.6868 2.7402 + 862.00 35.554 12.583 3.1755 + 862.00 40.540 12.151 3.3812 + 862.00 45.642 13.751 3.2876 + 862.00 50.399 6.6773 1.4141 + 862.00 60.484 8.9373 2.3723 + 862.00 70.461 5.0876 2.0630 + 902.10 15.266 4.9227 1.9346 + 902.10 17.751 4.5099 1.8434 + 902.10 20.118 3.6549 1.4557 + 902.10 22.722 7.8996 4.0475 + 902.10 25.207 6.4020 2.0474 + 902.10 30.177 7.6276 2.4393 + 902.10 35.266 9.3299 2.6413 + 902.10 40.237 8.5475 2.2566 + 902.10 45.207 11.116 2.5685 + 902.10 50.177 9.5783 1.4683 + 902.10 60.118 9.9198 2.4246 + 902.10 70.059 4.7951 1.6180 + 929.40 6.3641 23.213 5.7031 + 929.40 8.2662 26.031 6.0464 + 929.40 10.286 35.749 6.5147 + 929.40 12.903 34.210 6.5204 + 929.40 15.400 33.615 5.4309 + 929.40 17.779 26.499 4.2813 + 929.40 20.394 29.717 4.8017 + 929.40 22.890 41.904 6.7710 + 929.40 25.386 49.543 9.5468 + 929.40 30.380 49.987 8.0770 + 929.40 35.375 43.803 7.7184 + 929.40 40.487 53.648 9.2202 + 929.40 45.482 47.012 5.7052 + 929.40 50.476 37.063 5.1556 + 929.40 60.465 31.081 7.4287 + 929.40 70.337 16.055 4.4663 + 960.10 6.2469 12.989 3.0911 + 960.10 8.2675 17.267 5.0811 + 960.10 10.289 18.214 4.8725 + 960.10 12.787 12.991 3.8891 + 960.10 15.283 16.964 4.0882 + 960.10 17.900 12.317 4.9640 + 960.10 20.278 10.589 2.7633 + 960.10 22.894 13.109 2.8900 + 960.10 25.390 19.217 3.9467 + 960.10 30.384 17.740 4.7458 + 960.10 35.378 19.392 4.1401 + 960.10 40.490 21.578 3.9730 + 960.10 45.485 19.920 3.6853 + 960.10 50.479 17.126 4.9118 + 960.10 60.350 8.5589 2.3452 + 960.10 70.337 12.661 3.7111 + 971.20 6.1196 6.6317 2.3428 + 971.20 8.2590 7.4282 3.1013 + 971.20 10.391 19.549 4.3665 + 971.20 12.775 10.438 3.8040 + 971.20 15.271 10.716 3.0881 + 971.20 17.769 10.171 2.8677 + 971.20 20.264 13.328 2.6096 + 971.20 22.874 24.322 4.0685 + 971.20 25.372 21.531 4.5513 + 971.20 30.484 24.331 4.9339 + 971.20 35.482 15.739 4.7294 + 971.20 40.356 17.478 3.9040 + 971.20 45.467 22.121 4.7906 + 971.20 50.462 20.457 3.1223 + 971.20 60.333 15.895 3.2232 + 971.20 70.325 10.195 2.4140 + 993.20 6.0849 8.0010 2.4602 + 993.20 8.1053 13.059 2.9261 + 993.20 10.244 19.022 3.8699 + 993.20 12.738 16.976 4.0325 + 993.20 15.352 27.707 5.2473 + 993.20 17.846 30.505 4.8965 + 993.20 20.340 29.974 5.1120 + 993.20 22.954 44.433 7.1248 + 993.20 25.449 52.009 8.3396 + 993.20 30.437 50.658 8.6395 + 993.20 35.425 51.099 8.1937 + 993.20 40.413 54.322 8.7105 + 993.20 45.401 49.767 8.9995 + 993.20 50.389 51.087 7.6755 + 993.20 60.365 40.333 6.4674 + 993.20 70.221 30.480 6.7935 + 1006.4 6.2143 11.975 2.9323 + 1006.4 8.2314 6.0381 1.9703 + 1006.4 10.255 12.185 3.1441 + 1006.4 12.751 13.538 3.1342 + 1006.4 15.245 9.1200 3.2912 + 1006.4 17.742 14.269 3.0107 + 1006.4 20.236 9.5280 2.5202 + 1006.4 22.852 13.654 5.0037 + 1006.4 25.347 13.653 2.9750 + 1006.4 30.339 16.853 4.2382 + 1006.4 35.211 14.138 3.4621 + 1006.4 40.320 13.178 4.5307 + 1006.4 45.312 15.030 3.4796 + 1006.4 50.302 10.861 2.3666 + 1006.4 60.284 11.445 3.6668 + 1014.8 6.3094 11.273 2.7965 + 1014.8 8.3332 9.6029 2.5096 + 1014.8 10.238 9.1030 2.7855 + 1014.8 12.857 10.312 2.8959 + 1014.8 15.238 7.2208 3.3160 + 1014.8 20.238 5.1930 1.9832 + 1014.8 22.857 11.579 4.9142 + 1014.8 25.357 17.289 3.4522 + 1014.8 30.357 9.6889 3.2578 + 1014.8 35.357 13.593 3.2804 + 1014.8 40.476 13.961 5.0186 + 1014.8 45.357 15.399 3.3997 + 1014.8 50.476 8.8630 1.8950 + 1014.8 60.595 15.399 3.6116 + 1026.8 6.1413 7.3966 2.2064 + 1026.8 8.0416 7.2694 2.0920 + 1026.8 10.296 11.039 2.8271 + 1026.8 12.790 11.040 2.8273 + 1026.8 15.167 8.6531 3.4293 + 1026.8 17.775 18.938 4.0950 + 1026.8 20.273 9.9472 3.0452 + 1026.8 22.880 30.301 7.1642 + 1026.8 25.374 27.537 4.1964 + 1026.8 30.246 15.918 4.9688 + 1026.8 35.352 21.216 4.4425 + 1026.8 40.340 19.116 4.1335 + 1026.8 45.326 29.798 4.3201 + 1026.8 50.316 23.562 6.3368 + 1026.8 60.293 19.462 4.2085 + 1034.4 8.0044 3.3464 1.6552 + 1034.4 15.129 8.0967 3.4717 + 1034.4 17.622 8.5327 2.2508 + 1034.4 20.235 12.108 3.3485 + 1034.4 22.728 15.880 3.9824 + 1034.4 25.220 14.422 3.5219 + 1034.4 30.207 21.192 5.1752 + 1034.4 35.190 10.803 2.9189 + 1034.4 40.296 21.942 5.3585 + 1034.4 45.280 17.173 3.0069 + 1034.4 50.264 12.753 2.9442 + 1034.4 60.235 12.862 2.9694 +ENDDATA 880 +ENDSUBENT 897 +SUBENT F0259004 20050418 20050831 F021 +BIB 5 10 +REACTION (77-IR-191(D,T)77-IR-190,PAR,DA) +SAMPLE Targets enriched to either 94.66% or 96.19% 191Ir with + the thickness of 30 and 45 mu-g/cm**2 respectively were + used. +COMMENT For the angles 6.0,8.1,10.1,12.6,15.1 sross-section + values are out of the plot area. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from graphic bars +STATUS (CURVE)FIG.4a +ENDBIB 10 +COMMON 5 3 +EN E-LVL EN-RSL ANG-ERR-D ERR-DIG +MEV KEV KEV ADEG PER-CENT + 18. 38.1 5.7 0.1 0.1 +ENDCOMMON 3 +DATA 3 11 +ANG DATA DATA-ERR +ADEG MU-B/SR MU-B/SR + 17.592 1.1869 0.10099 + 20.085 15.646 7.1752 + 22.589 10.866 5.0870 + 25.212 10.211 4.2752 + 30.096 21.747 4.0224 + 35.103 16.656 3.7862 + 40.109 14.449 3.5783 + 45.113 23.151 4.1136 + 50.118 27.172 5.0016 + 60.251 18.378 3.5319 + 70.144 15.115 3.4304 +ENDDATA 13 +ENDSUBENT 32 +SUBENT F0259005 20050418 20050831 F021 +BIB 4 9 +REACTION (76-OS-189(A,T)77-IR-190,PAR,DA) +SAMPLE Target of 189Os was approximately 33 mu-g/cm2 and had + composition of 0.06% 186Os,0.41% 187Os, 1.23% 188Os, + 81.14% 189Os, 14.10% 190Os and 3.06% 192Os. +ERR-ANALYS (E-LVL-ERR) Uncertainty includes both statistical error + on mean and error due to calibration of spectrograph. + (DATA-ERR) Uncertainty is addition in quadrature of + statistical uncertainty plus reproducilibity error. +STATUS (TABLE) Table 2 +ENDBIB 9 +COMMON 3 3 +EN EN-RSL ANG +MEV KEV ADEG + 30. 10. 50. +ENDCOMMON 3 +DATA 4 32 +E-LVL-MEAN E-LVL-ERR DATA DATA-ERR +KEV KEV MU-B/SR MU-B/SR + 26.700 0.80000 7.3000 9.0000 + 84.000 0.80000 57.000 6.0000 + 145.80 0.80000 25.000 3.0000 + 173.50 0.80000 11.800 14.000 + 183.80 0.80000 9.8000 14.000 + 199.70 0.90000 3.8000 5.0000 + 225.90 0.80000 8.5000 10.000 + 244.70 0.80000 9.9000 14.000 + 268.80 1.1000 5.7000 8.0000 + 282.90 1.6000 7.1000 10.000 + 313.30 0.80000 31.000 4.0000 + 380.60 0.80000 25.000 4.0000 + 429.00 2.1000 4.0000 6.0000 + 441.60 0.80000 3.6000 7.0000 + 456.60 1.4000 4.1000 13.000 + 465.10 1.6000 19.000 3.0000 + 497.80 0.90000 2.2000 6.0000 + 511.10 1.3000 3.2000 7.0000 + 551.00 0.90000 1.9000 4.0000 + 589.90 1.3000 5.0000 6.0000 + 622.20 1.3000 4.1000 6.0000 + 671.50 1.3000 2.5000 4.0000 + 694.00 0.90000 2.2000 3.0000 + 717.00 1.7000 9.1000 11.000 + 741.90 1.3000 8.5000 12.000 + 758.90 0.90000 34.000 5.0000 + 804.90 1.3000 19.000 2.0000 + 817.70 0.90000 21.000 2.0000 + 847.90 0.90000 11.000 1.0000 + 869.50 0.90000 14.000 2.0000 + 891.10 0.90000 42.000 6.0000 + 925.00 0.90000 22.000 4.0000 +ENDDATA 34 +ENDSUBENT 52 +SUBENT F0259006 20050418 20050831 F021 +BIB 4 9 +REACTION (76-OS-189(HE3,D)77-IR-190,PAR,DA) +SAMPLE Target of 189Os was approximately 33 microg/cm2 and had + composition of 0.06% 186Os,0.41% 187Os, 1.23% 188Os, + 81.14% 189Os, 14.10% 190Os and 3.06% 192Os. +ERR-ANALYS (E-LVL-ERR) Uncertainty includes both statistical error + on mean and error due to calibration of spectrograph. + (DATA-ERR) Uncertainty is addition in quadrature of + statistical uncertainty plus reproducilibity error. +STATUS (TABLE) Table 2 +ENDBIB 9 +COMMON 3 3 +EN EN-RSL ANG +MEV KEV ADEG + 28. 15. 35. +ENDCOMMON 3 +DATA 4 31 +E-LVL-MEAN E-LVL-ERR DATA DATA-ERR +KEV KEV MU-B/SR MU-B/SR + 27.100 1.1000 3.7000 9.0000 + 84.200 0.90000 35.000 4.0000 + 146.00 0.90000 28.000 3.0000 + 175.70 1.6000 6.0000 14.000 + 185.50 1.6000 11.800 18.000 + 196.80 1.9000 4.9000 8.0000 + 227.00 1.9000 13.400 17.000 + 245.50 1.1000 9.0000 13.000 + 270.30 1.4000 9.5000 14.000 + 284.80 1.9000 8.4000 16.000 + 311.10 1.1000 16.000 2.0000 + 379.00 0.90000 37.000 4.0000 + 431.40 1.3000 6.3000 9.0000 + 450.00 2.1000 8.7000 24.000 + 465.90 2.1000 6.8000 29.000 + 499.30 1.6000 2.4000 14.000 + 511.10 1.6000 4.1000 7.0000 + 550.90 2.7000 4.7000 9.0000 + 589.60 1.6000 3.1000 16.000 + 620.70 1.3000 6.0000 9.0000 + 670.00 1.4000 4.5000 7.0000 + 694.50 1.4000 3.2000 9.0000 + 714.90 2.2000 3.3000 6.0000 + 741.30 1.3000 6.5000 9.0000 + 759.40 1.3000 8.9000 13.000 + 802.40 2.7000 10.000 3.0000 + 821.80 1.6000 8.8000 12.000 + 845.60 1.4000 10.100 13.000 + 867.40 1.3000 8.0000 1.0000 + 891.80 1.3000 10.600 13.000 + 923.70 1.3000 14.400 16.000 +ENDDATA 33 +ENDSUBENT 51 +ENDENTRY 6 diff --git a/exforall/F02/F0264.x4 b/exforall/F02/F0264.x4 new file mode 100644 index 000000000..2ef4add50 --- /dev/null +++ b/exforall/F02/F0264.x4 @@ -0,0 +1,175 @@ +ENTRY F0264 20050415 20050831 F021 +SUBENT F0264001 20050415 20050831 F021 +BIB 14 30 +TITLE The elastic scattering of polarized 3He by 2H at 22.5, + 24, 27, 30 and 33 MeV. +AUTHOR (N.T.Okumusoglu,C.O.Blyth) +INSTITUTE (2TUKTUK,2UK BIR) +REFERENCE (J,NP/A,671,33,2000) +FACILITY (CYCLO,2UK BIR) +INC-SOURCE (POLIS)Beams of polarised 3HE nuclei were used. +INC-SPECT Beams were accelerated to 33 MeV energy and reduced to + the required energy. +DETECTOR (TELES) Particles were being detected by + the EDE detector telescopes covered by Al absorber + foils which removed most unwanted particles and ensured + that those detected had suitable energies for the + thickness of surface barrier detectors. Measurements + at each angle were made with two counter telescopes + placed one on each side of the incident beam and the + results combined. + (SIBAR) +MONITOR (2-HE-4(HE3,EL)2-HE-4,,SIG) The calibration was + normalized. +MONIT-REF (,D.D.Armstrong+,J,PRL,23,135,1969) +METHOD (EDE) +SAMPLE Target of 140 mg/cm2 thickness. +ERR-ANALYS (ANG-ERR) Angular acceptance of the counter telescopes. + (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bars. + The calculated and the observed energy losses agreed + to better than 0.2 MeV. +HISTORY (20041201C) +ENDBIB 30 +COMMON 3 3 +ANG-ERR ANG-ERR-D ERR-DIG +ADEG ADEG NO-DIM + 1. 0.2 0.001 +ENDCOMMON 3 +ENDSUBENT 37 +SUBENT F0264002 20050415 20050831 F021 +BIB 2 2 +REACTION (1-H-2(HE3,EL)1-H-2,,POL/DA,,ANA) +STATUS (CURVE)Fig.2 +ENDBIB 2 +NOCOMMON 0 0 +DATA 4 123 +EN ANG DATA DATA-ERR +MEV ADEG NO-DIM NO-DIM + 22.500 25.593 -.37846E-01 + 22.500 40.561 -.10562 + 22.500 55.294 -.10672 0.23263E-01 + 22.500 75.597 0.32585 0.40306E-01 + 22.500 80.441 0.20767 0.23253E-01 + 22.500 95.303 -.41486E-010.20163E-01 + 22.500 120.22 -.35960 0.31004E-01 + 22.500 125.33 -.49796 + 22.500 130.12 -.47041 0.31004E-01 + 22.500 135.37 -.35298 0.55808E-01 + 22.500 138.26 -.30823 0.49617E-01 + 22.500 145.79 0.21675 0.43406E-01 + 22.500 148.70 0.28940 0.35665E-01 + 22.500 150.88 0.29234 + 22.500 156.04 0.24390 0.21713E-01 + 22.500 158.86 0.16927 0.20163E-01 + 24.000 25.741 -.40377E-01 + 24.000 40.602 -.10860 + 24.000 55.229 -.11585 + 24.000 75.751 0.34452 + 24.000 75.757 0.30895 + 24.000 80.210 0.19981 + 24.000 85.324 0.11356 0.73683E-01 + 24.000 87.993 0.60276E-010.73677E-01 + 24.000 95.548 -.46239E-010.17790E-01 + 24.000 109.98 -.19577 0.25400E-01 + 24.000 115.54 -.30742 0.30493E-01 + 24.000 116.65 -.32009 0.38109E-01 + 24.000 120.43 -.35811 0.27941E-01 + 24.000 125.55 -.46468 0.30487E-01 + 24.000 128.42 -.43412 0.38109E-01 + 24.000 130.42 -.48235 0.27947E-01 + 24.000 134.84 -.39077 0.38109E-01 + 24.000 135.95 -.38312 0.33028E-01 + 24.000 138.58 -.23570 0.30482E-01 + 24.000 140.77 -.13148 0.27952E-01 + 24.000 145.81 0.17860 0.30487E-01 + 24.000 148.90 0.24728 0.53353E-01 + 24.000 151.11 0.30068 0.15244E-01 + 24.000 153.11 0.24230 0.12703E-01 + 24.000 155.10 0.25251 0.15243E-01 + 24.000 156.00 0.22459 0.17784E-01 + 24.000 158.88 0.17893 0.15244E-01 + 27.000 25.490 -.53368E-010.18573E-01 + 27.000 30.665 -.69228E-01 + 27.000 45.916 -.11988 + 27.000 55.573 -.17012 0.20131E-01 + 27.000 65.022 0.13101 0.24764E-01 + 27.000 65.719 0.15727 0.37156E-01 + 27.000 70.433 0.28848 0.26312E-01 + 27.000 75.609 0.27417 0.23226E-01 + 27.000 80.477 0.19952 0.23216E-01 + 27.000 85.640 0.16199 0.17025E-01 + 27.000 90.485 0.47094E-010.92764E-02 + 27.000 95.367 -.43437E-020.17015E-01 + 27.000 100.50 -.92948E-010.23206E-01 + 27.000 105.66 -.14131 0.12382E-01 + 27.000 110.38 -.23608 0.18583E-01 + 27.000 115.50 -.34170 + 27.000 115.63 -.35564 + 27.000 120.38 -.39160 0.21659E-01 + 27.000 125.67 -.46009 0.23206E-01 + 27.000 130.40 -.52854 0.20121E-01 + 27.000 135.65 -.40820 0.66554E-01 + 27.000 140.71 -.15318 0.44875E-01 + 27.000 146.05 0.12039 0.21659E-01 + 27.000 149.03 0.31984 0.18583E-01 + 27.000 150.93 0.30267 0.23216E-01 + 27.000 156.24 0.28680 0.15467E-01 + 30.000 25.536 -.52091E-01 + 30.000 40.608 -.11001 0.17655E-01 + 30.000 49.031 -.14527 0.17657E-01 + 30.000 50.804 -.15030 0.17657E-01 + 30.000 55.679 -.15784 0.20179E-01 + 30.000 65.198 0.66709E-010.40359E-01 + 30.000 65.863 0.54101E-010.40358E-01 + 30.000 70.289 0.17520 0.40358E-01 + 30.000 75.383 0.25091 0.40356E-01 + 30.000 80.261 0.18283 0.32789E-01 + 30.000 85.582 0.13999 0.30270E-01 + 30.000 88.243 0.11226 0.27746E-01 + 30.000 95.561 -.12042E-020.22701E-01 + 30.000 110.42 -.23569 0.20177E-01 + 30.000 115.52 -.26593 0.55491E-01 + 30.000 120.62 -.38192 0.37835E-01 + 30.000 125.72 -.48783 0.37835E-01 + 30.000 128.38 -.50799 0.27745E-01 + 30.000 130.38 -.56852 + 30.000 130.60 -.58113 + 30.000 134.59 -.53066 0.25222E-01 + 30.000 135.69 -.47768 0.42880E-01 + 30.000 138.57 -.35154 0.42879E-01 + 30.000 146.08 0.64694E-010.42880E-01 + 30.000 148.95 0.27911 0.22700E-01 + 30.000 151.16 0.41281 0.15133E-01 + 30.000 153.16 0.37247 0.30268E-01 + 30.000 154.93 0.36743 0.22701E-01 + 30.000 156.26 0.33970 0.30268E-01 + 30.000 158.93 0.29683 0.25224E-01 + 33.000 29.681 -.55841E-01 + 33.000 31.044 -.59069E-01 + 33.000 35.941 -.84474E-01 + 33.000 40.431 -.10828 + 33.000 42.610 -.11470 + 33.000 45.873 -.13529 + 33.000 48.868 -.14803 0.15663E-01 + 33.000 51.047 -.15445 0.14106E-01 + 33.000 55.699 -.12971 0.12512E-01 + 33.000 60.652 -.50172E-010.18796E-01 + 33.000 70.484 0.22483 0.10964E-01 + 33.000 75.808 0.23229 0.17230E-01 + 33.000 85.442 0.13450 0.14097E-01 + 33.000 90.585 0.55818E-01 + 33.000 100.33 -.87403E-010.14097E-01 + 33.000 105.74 -.18333 0.18786E-01 + 33.000 110.60 -.26982 0.20353E-01 + 33.000 120.50 -.39582 0.15663E-01 + 33.000 125.62 -.51679 0.26628E-01 + 33.000 130.93 -.52813 0.17211E-01 + 33.000 136.00 -.49246 0.29751E-01 + 33.000 146.08 -.75791E-020.39149E-01 + 33.000 151.03 0.33825 0.26628E-01 + 33.000 156.11 0.39585 0.31327E-01 +ENDDATA 125 +ENDSUBENT 132 +ENDENTRY 2 diff --git a/exforall/F02/F0272.x4 b/exforall/F02/F0272.x4 new file mode 100644 index 000000000..0f8f4409b --- /dev/null +++ b/exforall/F02/F0272.x4 @@ -0,0 +1,96 @@ +ENTRY F0272 20050526 20050831 F021 +SUBENT F0272001 20050526 20050831 F021 +BIB 10 19 +TITLE Hyperfine interaction studies of light nuclei in + highly ionized atoms recoiling in vacuum. +AUTHOR (Z.Berant,M.B.Goldberg,G.Goldring,S.S.Hanna, + H.M.Loebenstein,I.Plesser,M.Popp,J.S.Sokolowski, + P.N.Tandon,Y.Wolfson) +INSTITUTE (3ISLWZI) +REFERENCE (J,NP/A,178,155,1971) +FACILITY (VDG) +DETECTOR (NAICR)12.7 cm*12.7 cm for gamma rays detection. + (SCIN)for the measurements on the 5+/2 level in 19F + 3.8 cm*1.3 cm scintillators were used. +METHOD (GSPEC) + (COINC) +CORRECTION Relativistic corrections to account for movement of the + gamma-emitting source were applied in all cases. +ERR-ANALYS (ANG-ERR-D)Digitizing error + (ERR-DIG)Digitizing error + (DATA-ERR)Error from the graphic bars +HISTORY (20050113C) +ENDBIB 19 +NOCOMMON 0 0 +ENDSUBENT 22 +SUBENT F0272002 20050526 20050831 F021 +BIB 3 5 +REACTION (6-C-12(A,INL)6-C-12,PAR,DA/DA,A/G,REL) + ANG-MIN and ANG-MAX are the angles of alpha particles + detection.ANG2 is an angle of gamma particles detection +SAMPLE Natural enriched targets with the thickness of 20-40keV +STATUS (CURVE)Fig.1 +ENDBIB 5 +COMMON 6 3 +EN E-LVL ANG-MIN ANG-MAX ANG-ERR-D ERR-DIG +MEV MEV ADEG ADEG ADEG ARB-UNITS + 17. 4.43 165. 175. 0.11 0.01 +ENDCOMMON 3 +DATA 3 5 +ANG2 DATA DATA-ERR +ADEG ARB-UNITS ARB-UNITS +0.10690E-01 2.0158 0.85264E-01 + 19.135 1.7482 0.92944E-01 + 44.899 0.93114 0.77512E-01 + 69.864 0.99768 0.69832E-01 + 89.664 1.2571 0.69761E-01 +ENDDATA 7 +ENDSUBENT 21 +SUBENT F0272003 20050526 20050831 F021 +BIB 4 8 +REACTION (9-F-19(P,A)8-O-16,PAR,DA/DA,A/G,REL) + ANG-MIN and ANG-MAX are the angles of alpha particles + detection.ANG2 is an angle of gamma particles detection +SAMPLE Natural enriched LiF targets with the thickness of + 20-40 keV. +FLAG (1.)Recoil in vacuum. + (2.)Recoil in aluminium (thick (0.5 mg/cm2) foil). +STATUS (CURVE)Fig.3 +ENDBIB 8 +COMMON 6 3 +EN ANG-MIN ANG-MAX E-LVL ANG-ERR-D ERR-DIG +KEV ADEG ADEG MEV ADEG ARB-UNITS + 873. 165. 175. 6.13 0.14 0.02 +ENDCOMMON 3 +DATA 4 26 +ANG2 DATA DATA-ERR FLAG +ADEG ARB-UNITS ARB-UNITS NO-DIM +0.20200E-02 2.5377 0.66245E-01 2.0000 +0.11450E-01 2.2102 0.36802E-01 1.0000 + 14.893 1.8877 0.55221E-01 2.0000 + 19.896 1.5607 0.40500E-01 1.0000 + 24.856 1.4139 0.47843E-01 2.0000 + 24.862 1.3918 0.36820E-01 1.0000 + 29.830 1.2120 0.33122E-01 1.0000 + 29.838 1.1788 0.51524E-01 2.0000 + 34.777 1.1241 0.29425E-01 1.0000 + 34.806 0.99896 0.36803E-01 2.0000 + 39.721 1.0510 0.25745E-01 1.0000 + 39.912 1.0142 0.33122E-01 2.0000 + 44.818 1.1066 0.29442E-01 1.0000 + 45.006 1.0809 0.44180E-01 2.0000 + 54.861 1.0745 0.29442E-01 1.0000 + 55.020 1.1775 0.33139E-01 2.0000 + 59.789 1.0712 0.29442E-01 1.0000 + 59.957 1.1338 0.36803E-01 2.0000 + 64.920 0.97971 0.25762E-01 1.0000 + 65.066 1.1343 0.47843E-01 2.0000 + 70.044 0.91395 0.29442E-01 1.0000 + 70.047 0.90291 0.36785E-01 2.0000 + 75.190 0.75618 0.29459E-01 1.0000 + 75.379 0.72675 0.33139E-01 2.0000 + 90.051 0.40794 0.22081E-01 2.0000 + 90.206 0.52941 0.18401E-01 1.0000 +ENDDATA 28 +ENDSUBENT 45 +ENDENTRY 3 diff --git a/exforall/F04/F0497.x4 b/exforall/F04/F0497.x4 new file mode 100644 index 000000000..3e075d59c --- /dev/null +++ b/exforall/F04/F0497.x4 @@ -0,0 +1,860 @@ +ENTRY F0497 20050428 20050831 F021 +SUBENT F0497001 20050428 20050831 F021 +BIB 10 11 +TITLE Experimental basis of alpha-particle nuclear matter + existence. +AUTHOR (S.Ya.Aisina,K.A.Kuterbekov,N.N.Pavlova,A.V.Yushkov) +INSTITUTE (4KASKAZ) +REFERENCE (J,IZV,53,37,1989) +FACILITY (CYCLO) +DETECTOR Alpha-spectrometer. +SAMPLE Light and medium nuclei with A=12-64. +INC-SOURCE Pulsed beam of accelerated alpha-particles. +STATUS Data were approved by authors for 24Mg only. +HISTORY (20031104C) +ENDBIB 11 +COMMON 1 3 +EN-RSL +PER-CENT + 0.5 +ENDCOMMON 3 +ENDSUBENT 18 +SUBENT F0497002 20050428 20050831 F021 +BIB 3 5 +REACTION (6-C-12(A,EL)6-C-12,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bars +STATUS (CURVE)FIG.2 +ENDBIB 5 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.2 0.1 +ENDCOMMON 3 +DATA 4 163 +EN ANG-CM DATA-CM DATA-ERR +MEV ADEG NO-DIM NO-DIM + 29.300 12.765 1.1612 0.34986 + 29.300 14.121 0.48074 0.11579 + 29.300 16.786 0.66387 0.17989 + 29.300 17.819 0.39333 0.11872 + 29.300 19.361 0.19743 0.53397E-01 + 29.300 22.001 0.94887E-01 + 29.300 23.282 0.46452 + 29.300 24.609 1.1902 + 29.300 25.675 1.7973 + 29.300 27.239 2.7195 + 29.300 28.411 3.7325 + 29.300 29.590 4.6543 + 29.300 31.661 6.1112 + 29.300 31.977 4.8142 + 29.300 33.372 4.7271 + 29.300 34.757 5.3598 + 29.300 36.165 4.3442 + 29.300 37.274 3.6021 + 29.300 38.382 2.9867 + 29.300 39.892 2.3644 + 29.300 41.209 1.6992 + 29.300 42.387 2.1702 + 29.300 43.596 1.7576 + 29.300 44.868 2.4132 + 29.300 46.050 2.8683 + 29.300 47.449 2.6845 + 29.300 48.427 3.4260 + 29.300 49.905 4.2773 + 29.300 51.296 4.4062 + 29.300 52.489 4.5354 + 29.300 53.697 3.7621 + 29.300 55.093 3.6065 + 29.300 56.294 3.2928 + 29.300 57.598 2.8668 + 29.300 58.511 2.2639 + 40.400 14.471 0.65652 0.19469 + 40.400 15.804 0.38344 0.11351 + 40.400 17.261 0.16098 0.42952E-01 + 40.400 18.681 0.28203E-010.83785E-02 + 40.400 19.812 0.17255E-010.40764E-02 + 40.400 21.027 0.20218 0.53841E-01 + 40.400 22.251 0.53509 0.12668 + 40.400 23.497 1.0419 0.27745 + 40.400 24.861 1.5653 0.61226 + 40.400 26.136 2.0402 0.66930 + 40.400 27.519 2.3640 0.70105 + 40.400 28.822 2.1119 0.49999 + 40.400 30.210 2.2798 0.53974 + 40.400 31.538 1.4292 0.38060 + 40.400 32.856 1.0324 0.24442 + 40.400 34.194 0.56173 0.14959 + 40.400 36.803 0.26980E-010.55957E-02 + 40.400 37.882 0.13187 0.35049E-01 + 40.400 39.163 0.63000 0.16777 + 40.400 40.430 0.92402 0.27354 + 40.400 41.780 1.6768 0.60146 + 40.400 42.853 2.2894 0.67772 + 40.400 44.035 2.7140 0.72272 + 40.400 45.162 1.7407 0.41124 + 40.400 46.628 2.5551 0.75639 + 40.400 47.934 2.1773 0.57871 + 40.400 49.236 1.9451 0.51698 + 40.400 50.742 1.6201 0.43061 + 40.400 52.957 1.1471 0.30489 + 40.400 53.948 1.2363 0.36664 + 40.400 54.756 1.0514 0.31069 + 40.400 55.326 1.5377 0.40871 + 40.400 56.110 1.8200 0.53780 + 40.400 56.897 2.0547 0.67185 + 40.400 57.972 2.7398 0.72960 + 40.400 59.545 3.5754 1.0565 + 40.400 60.422 4.6526 1.3773 + 40.400 61.718 4.5680 1.2165 + 40.400 62.900 5.4152 1.6030 + 40.400 64.187 5.9829 1.7680 + 40.400 65.892 4.9874 1.4738 + 45.000 39.471 0.92714 0.22496 + 45.000 40.239 1.3708 + 45.000 40.819 1.7511 0.47920 + 45.000 41.597 2.2937 + 45.000 42.180 2.7914 0.67876 + 45.000 43.472 2.8755 0.87673 + 45.000 44.556 3.3410 0.91606 + 45.000 45.648 3.5231 1.0761 + 45.000 46.747 3.2913 0.90068 + 45.000 47.851 2.9293 0.89473 + 45.000 48.952 2.6710 0.81438 + 45.000 49.953 2.4942 0.76047 + 45.000 50.367 2.0089 + 45.000 51.061 2.0642 0.76432 + 45.000 51.964 1.8807 + 45.000 52.849 2.1832 0.66565 + 45.000 54.136 2.4186 0.73875 + 45.000 55.224 2.6771 0.81771 + 45.000 56.314 2.8924 0.88186 + 45.000 57.594 3.5303 1.1894 + 45.000 59.958 5.0065 1.3674 + 45.000 61.233 6.5715 2.6502 + 45.000 62.437 5.7111 1.9240 + 45.000 63.726 6.1754 2.0839 + 45.000 64.236 5.2229 + 45.000 64.932 5.2383 + 45.000 65.729 5.2560 + 45.000 66.528 5.0242 + 45.000 67.429 4.6897 + 50.500 10.731 1.3216 0.34991 + 50.500 12.924 1.2725 0.37517 + 50.500 14.061 0.72746 + 50.500 14.646 0.85961 0.25344 + 50.500 15.498 0.40673 0.14548 + 50.500 16.424 0.27384 0.72507E-01 + 50.500 17.525 0.67178E-01 + 50.500 17.549 0.48352E-01 + 50.500 17.804 0.87093E-010.28311E-01 + 50.500 18.065 0.38309E-01 + 50.500 18.787 0.10309 0.27240E-01 + 50.500 18.826 0.61485E-01 + 50.500 19.249 0.16524 0.43753E-01 + 50.500 19.473 0.11903 + 50.500 19.694 0.33502 + 50.500 19.872 0.44447 0.11769 + 50.500 20.665 0.46741 + 50.500 20.827 0.76609 + 50.500 20.916 0.88241 + 50.500 22.364 1.5974 + 50.500 23.740 2.0321 0.47734 + 50.500 25.119 2.4665 0.44081 + 50.500 26.710 2.5420 0.67306 + 50.500 27.721 2.0662 + 50.500 34.386 0.58346 + 50.500 35.433 1.1052 0.22792 + 50.500 36.585 1.9518 0.40349 + 50.500 37.945 3.0675 0.72212 + 50.500 39.532 3.3134 0.97513 + 50.500 40.711 4.1139 1.2107 + 50.500 41.994 4.7622 1.2609 + 50.500 43.385 4.9038 1.2984 + 50.500 44.880 4.8199 + 50.500 46.085 4.2073 + 50.500 47.387 3.7613 + 50.500 48.688 3.4425 + 50.500 49.875 3.8006 + 50.500 51.075 3.5597 + 50.500 52.168 3.6610 + 50.500 53.065 3.5894 + 50.500 53.956 3.8659 + 50.500 54.736 4.7919 + 50.500 55.738 4.3803 + 50.500 56.931 4.5069 1.6095 + 50.500 58.219 4.8621 1.5805 + 50.500 59.513 4.8884 1.5837 + 50.500 60.706 5.0297 1.6322 + 50.500 61.701 5.0506 + 50.500 62.487 5.8344 2.0803 + 50.500 63.979 5.8709 2.4798 + 50.500 64.887 4.9994 1.7825 + 50.500 66.281 5.0286 1.7958 + 50.500 67.201 3.6329 1.1809 + 50.500 68.607 3.1000 0.91567 + 50.500 69.616 2.5797 0.84138 + 50.500 71.032 1.9119 0.62254 + 50.500 72.448 1.4170 0.41703 + 50.500 73.765 1.0498 0.30952 +ENDDATA 165 +ENDSUBENT 179 +SUBENT F0497003 20050428 20050831 F021 +BIB 3 4 +REACTION (12-MG-24(A,EL)12-MG-24,,DA) +ERR-ANALYS (DATA-ERR) Definition error +STATUS (TABLE,APRVD) Data correspond to data from fig. 3 of + the reference. +ENDBIB 4 +COMMON 2 3 +EN EN-ERR +MEV MEV + 50.5 0.5 +ENDCOMMON 3 +DATA 3 36 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR PER-CENT + 31.340 55.237 2.1800 + 31.690 52.046 1.5000 + 32.030 51.665 1.5000 + 32.380 37.001 1.1200 + 32.610 42.655 1.2500 + 32.950 38.033 1.1700 + 33.300 30.983 0.44000 + 33.640 28.056 1.2000 + 33.760 26.065 1.2200 + 33.980 23.315 0.80000 + 34.210 22.457 0.60000 + 34.350 21.605 0.34000 + 34.560 19.304 0.50000 + 34.790 15.698 0.50000 + 35.020 15.518 0.50000 + 35.240 13.047 0.50000 + 35.470 13.185 0.44000 + 35.590 11.527 0.40000 + 35.870 10.111 0.37000 + 35.930 9.5386 0.62000 + 36.040 9.7767 0.30000 + 36.270 7.4175 0.24000 + 36.730 6.2878 0.20000 + 36.840 6.8180 0.23000 + 37.070 7.2813 0.24000 + 37.760 7.6596 0.27000 + 38.100 7.7610 0.28000 + 38.210 8.4576 0.58000 + 38.440 8.3363 0.30000 + 38.780 8.8337 0.30000 + 39.130 10.400 0.30000 + 39.470 11.731 0.35000 + 39.700 12.419 0.37000 + 40.040 14.191 0.40000 + 40.490 9.1443 0.30000 + 41.060 15.662 0.43000 +ENDDATA 38 +ENDSUBENT 51 +SUBENT F0497004 20050428 20050831 F021 +BIB 3 3 +REACTION (12-MG-24(A,INL)12-MG-24,PAR,DA) +ERR-ANALYS (DATA-ERR) Definition error +STATUS (TABLE,APRVD) +ENDBIB 3 +COMMON 3 3 +EN EN-ERR E-LVL +MEV MEV MEV + 50.5 0.5 1.368 +ENDCOMMON 3 +DATA 3 37 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR PER-CENT + 31.420 18.398 0.95000 + 31.760 19.480 0.30000 + 32.110 3.3040 0.80000 + 32.450 5.0750 0.80000 + 32.680 8.7440 0.80000 + 33.030 1.0000 0.80000 + 33.370 23.420 0.50000 + 33.720 22.534 1.1000 + 33.830 27.140 1.2500 + 34.060 22.980 8.0000 + 34.290 23.377 0.65000 + 34.400 24.644 0.37000 + 34.630 24.873 0.60000 + 34.800 24.760 0.70000 + 35.000 24.693 0.70000 + 35.320 23.150 0.80000 + 35.550 23.447 0.65000 + 35.670 21.620 0.60000 + 35.900 20.800 0.40000 + 36.010 20.377 1.0000 + 36.130 19.937 0.50000 + 36.350 20.018 0.45000 + 36.810 13.496 0.40000 + 36.930 10.384 0.44000 + 37.160 19.828 0.45000 + 37.840 13.935 0.43000 + 38.190 12.844 0.36000 + 38.300 14.029 0.80000 + 38.530 13.856 0.40000 + 38.870 12.475 0.40000 + 39.210 13.724 0.40000 + 39.500 12.514 0.40000 + 39.780 11.110 0.34000 + 40.130 11.373 0.35000 + 40.580 6.6743 0.25000 + 41.150 8.2510 0.30000 + 42.290 8.2017 0.30000 +ENDDATA 39 +ENDSUBENT 51 +SUBENT F0497005 20050428 20050831 F021 +BIB 2 3 +REACTION (12-MG-24(A,EL)12-MG-24,,DA) +STATUS (TABLE,APRVD) Data sent by authors. Corresponding + figure is 4 in reference. +ENDBIB 3 +COMMON 2 3 +EN EN-ERR +MEV MEV + 39.0 0.5 +ENDCOMMON 3 +DATA 2 76 +ANG-CM DATA-CM +ADEG MB/SR + 19.790 456.00 + 20.850 410.00 + 22.110 355.00 + 23.270 210.00 + 24.420 169.00 + 25.580 89.500 + 26.730 20.000 + 27.310 9.1500 + 27.890 2.7600 + 28.460 4.2100 + 29.040 6.6500 + 30.190 20.000 + 31.340 31.000 + 32.490 50.000 + 33.630 51.000 + 34.780 49.500 + 35.920 38.000 + 37.870 27.600 + 38.210 16.100 + 39.350 9.2300 + 40.490 3.4400 + 41.020 1.9000 + 42.760 2.2600 + 43.890 4.7300 + 43.920 7.4200 + 46.150 9.6400 + 47.280 10.200 + 48.400 9.5800 + 49.530 9.5200 + 50.650 7.8500 + 51.770 6.5200 + 52.890 4.5000 + 54.000 3.0700 + 55.110 3.3300 + 56.230 2.2800 + 57.340 2.5000 + 58.440 2.8000 + 59.550 2.8300 + 60.650 3.2900 + 61.750 4.5600 + 62.850 4.8800 + 63.940 4.5800 + 65.040 4.5400 + 66.130 4.2800 + 67.210 3.2300 + 68.300 2.4700 + 69.380 1.8700 + 70.460 1.2700 + 71.540 1.1100 + 72.620 1.0300 + 73.690 0.94000 + 74.760 0.95000 + 75.830 0.94000 + 76.890 1.0500 + 77.950 1.0800 + 79.010 0.89000 + 80.070 1.1200 + 81.120 1.1300 + 82.170 0.79000 + 83.220 0.82000 + 84.260 0.68000 + 85.310 0.62000 + 86.350 0.48000 + 87.380 0.40000 + 88.420 0.26000 + 89.450 0.24000 + 90.470 0.20000 + 91.500 0.17000 + 92.520 0.19800 + 93.540 0.20000 + 94.560 0.27000 + 95.570 0.25000 + 96.580 0.23000 + 97.590 0.18000 + 98.590 0.14900 + 99.590 0.12800 +ENDDATA 78 +ENDSUBENT 90 +SUBENT F0497006 20050428 20050831 F021 +BIB 2 3 +REACTION (12-MG-24(A,EL)12-MG-24,,DA,,RTH) +STATUS (TABLE,APRVD) Data sent by authors. Corresponding + figure is 4 in reference. +ENDBIB 3 +COMMON 2 3 +EN EN-ERR +MEV MEV + 39.0 0.5 +ENDCOMMON 3 +DATA 2 76 +ANG-CM DATA-CM +ADEG NO-DIM + 19.790 0.60740 + 20.850 0.67680 + 22.110 0.71850 + 23.270 0.51990 + 24.420 0.50550 + 25.580 0.32180 + 26.730 0.85520E-01 + 27.310 0.42550E-01 + 27.890 0.13930E-01 + 28.460 0.23020E-01 + 29.040 0.39330E-01 + 30.190 0.13770 + 31.340 0.24700 + 32.490 0.45830 + 33.630 0.53490 + 34.780 0.59130 + 35.920 0.51450 + 37.870 0.42170 + 38.210 0.27650 + 39.350 0.17750 + 40.490 0.73800E-01 + 41.020 0.45320E-01 + 42.760 0.59730E-01 + 43.890 0.13810 + 43.920 0.23860 + 46.150 0.31050 + 47.280 0.39470 + 48.400 0.40500 + 49.530 0.43870 + 50.650 0.39340 + 51.770 0.35450 + 52.890 0.26490 + 54.000 0.19520 + 55.110 0.22840 + 56.230 0.16830 + 57.340 0.19820 + 58.440 0.25810 + 59.550 0.25760 + 60.650 0.32000 + 61.750 0.47340 + 62.850 0.53970 + 63.940 0.53890 + 65.040 0.56750 + 66.130 0.56760 + 67.210 0.45380 + 68.300 0.36720 + 69.380 0.29370 + 70.460 0.21050 + 71.540 0.19430 + 72.620 0.18930 + 73.690 0.18190 + 74.760 0.19320 + 75.830 0.20060 + 76.890 0.23490 + 77.950 0.25310 + 79.010 0.21820 + 80.070 0.28700 + 81.120 0.30240 + 82.170 0.22060 + 83.220 0.23870 + 84.260 0.20620 + 85.310 0.19560 + 86.350 0.15750 + 87.380 0.13630 + 88.420 0.91997E-01 + 89.450 0.88090 + 90.470 0.76090E-01 + 91.500 0.66990E-01 + 92.520 0.77500E-01 + 93.540 0.84380E-01 + 94.560 0.11770 + 95.570 0.11260 + 96.580 0.10690 + 97.590 0.86330E-01 + 98.590 0.74160E-01 + 99.590 0.66220E-01 +ENDDATA 78 +ENDSUBENT 90 +SUBENT F0497007 20050428 20050831 F021 +BIB 2 2 +REACTION (12-MG-24(A,INL)12-MG-24,PAR,DA) +STATUS (TABLE,APRVD) +ENDBIB 2 +COMMON 3 3 +EN EN-ERR E-LVL +MEV MEV MEV + 39.0 0.5 1.368 +ENDCOMMON 3 +DATA 2 76 +ANG-CM DATA-CM +ADEG MB/SR + 19.850 22.800 + 21.010 20.100 + 22.180 21.800 + 23.340 26.100 + 24.500 45.500 + 25.660 55.000 + 26.810 54.800 + 27.390 41.200 + 27.970 29.890 + 28.550 20.340 + 29.120 15.240 + 30.280 17.020 + 31.430 13.130 + 32.580 5.8990 + 33.730 4.2590 + 34.880 4.3840 + 36.030 5.0330 + 37.170 7.2490 + 38.320 10.860 + 39.460 11.680 + 40.600 11.250 + 41.740 10.130 + 42.880 8.5290 + 44.010 5.3780 + 45.150 4.2280 + 46.280 3.4190 + 47.410 2.3630 + 48.540 2.0540 + 49.670 2.6910 + 50.790 3.2750 + 51.910 3.8400 + 53.030 4.9640 + 54.150 5.5640 + 55.270 5.4910 + 56.380 5.8070 + 57.490 5.4890 + 58.600 5.3160 + 59.710 4.3900 + 60.810 3.7250 + 61.910 2.2000 + 63.050 2.1650 + 64.110 1.8780 + 65.210 1.7660 + 66.300 2.2220 + 67.390 2.6860 + 68.480 2.5520 + 69.560 3.0290 + 70.640 2.4170 + 71.720 2.3250 + 72.800 2.2060 + 73.870 2.4230 + 74.940 2.3780 + 76.010 1.9540 + 77.080 1.8890 + 78.150 1.5500 + 79.200 1.3640 + 80.250 1.2460 + 81.310 1.2530 + 82.370 0.94630 + 83.420 0.92960 + 84.460 0.91260 + 85.500 0.93460 + 86.550 0.82180 + 87.580 0.93980 + 88.620 0.87120 + 89.650 0.75030 + 90.680 0.74320 + 91.700 0.74180 + 92.720 0.65870 + 93.740 0.64500 + 94.750 0.67250 + 95.770 0.62900 + 96.790 0.45370 + 97.790 0.36280 + 98.800 0.31120 + 99.800 0.29300 +ENDDATA 78 +ENDSUBENT 89 +SUBENT F0497008 20050428 20050831 F021 +BIB 3 5 +REACTION (28-NI-60(A,EL)28-NI-60,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + Experimental errors were not greater than point sizes. +STATUS (CURVE)Fig.4 (a) +ENDBIB 5 +COMMON 3 3 +EN ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT + 32.3 0.2 0.1 +ENDCOMMON 3 +DATA 2 6 +ANG-CM DATA-CM +ADEG NO-DIM + 22.064 0.52653 + 28.647 0.31262 + 42.331 0.17156 + 53.906 0.66962E-01 + 70.086 0.29984E-01 + 85.170 0.19882E-01 +ENDDATA 8 +ENDSUBENT 22 +SUBENT F0497009 20050428 20050831 F021 +BIB 3 5 +REACTION (28-NI-58(A,EL)28-NI-58,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + Experimental errors were not greater than point sizes. +STATUS (CURVE)Fig.4 (b) +ENDBIB 5 +COMMON 3 3 +EN ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT +50. 0.5 0.1 +ENDCOMMON 3 +DATA 2 4 +ANG-CM DATA-CM +ADEG NO-DIM + 23.516 0.15363 + 33.933 0.15468 + 43.831 0.10182 + 53.963 0.68821E-01 +ENDDATA 6 +ENDSUBENT 20 +SUBENT F0497010 20050428 20050831 F021 +BIB 3 5 +REACTION (26-FE-58(A,EL)26-FE-58,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + Experimental errors were not greater than point sizes. +STATUS (CURVE)Fig.4 (b) +ENDBIB 5 +COMMON 3 3 +EN ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT + 64.3 0.2 0.1 +ENDCOMMON 3 +DATA 2 7 +ANG-CM DATA-CM +ADEG NO-DIM + 20.758 0.60133 + 30.458 0.39712 + 39.684 0.23972 + 47.038 0.12569 + 55.579 0.84115E-01 + 64.099 0.46414E-01 + 74.924 0.22502E-01 +ENDDATA 9 +ENDSUBENT 23 +SUBENT F0497011 20050428 20050831 F021 +BIB 3 5 +REACTION (20-CA-42(A,EL)20-CA-42,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + Experimental errors were not greater than point sizes. +STATUS (CURVE)Fig.4 (b) +ENDBIB 5 +COMMON 3 3 +EN ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT + 42. 0.2 0.1 +ENDCOMMON 3 +DATA 2 5 +ANG-CM DATA-CM +ADEG NO-DIM + 15.991 0.70640 + 27.804 0.50041 + 37.735 0.22280 + 49.060 0.10437 + 60.855 0.52817E-01 +ENDDATA 7 +ENDSUBENT 21 +SUBENT F0497012 20050428 20050831 F021 +BIB 3 5 +REACTION (14-SI-30(A,EL)14-SI-30,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + Experimental errors were not greater than point sizes. +STATUS (CURVE)Fig.4 (b) +ENDBIB 5 +COMMON 3 3 +EN ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT + 41. 0.2 0.1 +ENDCOMMON 3 +DATA 2 6 +ANG-CM DATA-CM +ADEG NO-DIM + 30.764 0.65512 + 42.526 0.37816 + 57.384 0.40454 + 71.438 0.18760 + 83.627 0.81936E-01 + 91.959 0.69787E-01 +ENDDATA 8 +ENDSUBENT 22 +SUBENT F0497013 20050428 20050831 F021 +BIB 3 5 +REACTION (14-SI-28(A,EL)14-SI-28,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + Experimental errors were not greater than point sizes. +STATUS (CURVE)Fig.4 (b) +ENDBIB 5 +COMMON 3 3 +EN ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT + 39. 0.2 0.1 +ENDCOMMON 3 +DATA 2 6 +ANG-CM DATA-CM +ADEG NO-DIM + 22.123 0.75374 + 34.855 0.53640 + 48.734 0.32760 + 63.376 0.43533 + 80.704 0.18415 + 94.053 0.52479E-01 +ENDDATA 8 +ENDSUBENT 22 +SUBENT F0497014 20050428 20050831 F021 +BIB 3 4 +REACTION (30-ZN-64(A,EL)30-ZN-64,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error +STATUS (CURVE)Fig.5 +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.3 0.1 +ENDCOMMON 3 +DATA 3 17 +EN ANG-CM DATA-CM +MEV ADEG NO-DIM + 29.300 33.554 0.16940 + 29.300 46.018 0.16840 + 29.300 58.972 0.57887E-01 + 29.300 71.304 0.33543E-01 + 29.300 86.092 0.19447E-01 + 38.000 19.529 0.51454 + 38.000 27.834 0.26594 + 38.000 37.627 0.15803 + 38.000 49.886 0.67494E-01 + 38.000 60.240 0.40817E-01 + 38.000 73.792 0.21488E-01 + 50.500 15.588 0.25011 + 50.500 24.104 0.18816 + 50.500 30.952 0.11784 + 50.500 40.250 0.73221E-01 + 50.500 50.160 0.32973E-01 + 50.500 61.433 0.10953E-01 +ENDDATA 19 +ENDSUBENT 32 +SUBENT F0497015 20050428 20050831 F021 +BIB 3 4 +REACTION (30-ZN-66(A,EL)30-ZN-66,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error +STATUS (CURVE)Fig.5 +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.3 0.1 +ENDCOMMON 3 +DATA 3 17 +EN ANG-CM DATA-CM +MEV ADEG NO-DIM + 29.300 33.724 0.20162 + 29.300 46.383 0.19024 + 29.300 56.675 0.77786E-01 + 29.300 70.715 0.41692E-01 + 29.300 84.168 0.27060E-01 + 38.000 18.217 0.50996 + 38.000 28.974 0.22545 + 38.000 38.572 0.14489 + 38.000 48.763 0.66315E-01 + 38.000 60.076 0.31435E-01 + 38.000 71.729 0.21857E-01 + 50.500 13.906 0.22914 + 50.500 23.187 0.15943 + 50.500 31.871 0.13787 + 50.500 41.208 0.65406E-01 + 50.500 49.739 0.44712E-01 + 50.500 58.722 0.18133E-01 +ENDDATA 19 +ENDSUBENT 32 +SUBENT F0497016 20050428 20050831 F021 +BIB 3 4 +REACTION (30-ZN-68(A,EL)30-ZN-68,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error +STATUS (CURVE)Fig.5 +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.3 0.1 +ENDCOMMON 3 +DATA 3 17 +EN ANG-CM DATA-CM +MEV ADEG NO-DIM + 29.300 45.631 0.18370 + 29.300 56.866 0.75784E-01 + 29.300 69.771 0.41684E-01 + 29.300 83.614 0.24162E-01 + 38.000 9.5338 1.0216 + 38.000 18.409 0.48825 + 38.000 27.475 0.22343 + 38.000 38.575 0.13993 + 38.000 48.205 0.63484E-01 + 38.000 59.882 0.33701E-01 + 38.000 71.177 0.19516E-01 + 50.500 23.535 0.19310 + 50.500 29.573 0.17889 + 50.500 39.661 0.86375E-01 + 50.500 50.094 0.51850E-01 + 50.500 59.609 0.26372E-01 + 50.500 71.154 0.17889E-01 +ENDDATA 19 +ENDSUBENT 32 +SUBENT F0497017 20050428 20050831 F021 +BIB 3 4 +REACTION (30-ZN-70(A,EL)30-ZN-70,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error +STATUS (CURVE)Fig.5 +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.3 0.1 +ENDCOMMON 3 +DATA 3 15 +EN ANG-CM DATA-CM +MEV ADEG NO-DIM + 29.300 44.877 0.18208 + 29.300 56.698 0.62573E-01 + 29.300 69.978 0.35025E-01 + 29.300 83.629 0.20838E-01 + 38.000 17.089 0.53253 + 38.000 27.295 0.20658 + 38.000 38.407 0.11256 + 38.000 48.212 0.58191E-01 + 38.000 60.275 0.27588E-01 + 38.000 70.815 0.16830E-01 + 50.500 22.956 0.21247 + 50.500 30.913 0.15435 + 50.500 40.214 0.93430E-01 + 50.500 49.001 0.40268E-01 + 50.500 57.956 0.19777E-01 +ENDDATA 17 +ENDSUBENT 30 +ENDENTRY 17 diff --git a/exforall/F05/F0502.x4 b/exforall/F05/F0502.x4 new file mode 100644 index 000000000..0f5120309 --- /dev/null +++ b/exforall/F05/F0502.x4 @@ -0,0 +1,64 @@ +ENTRY F0502 20050419 20050831 F021 +SUBENT F0502001 20050419 20050831 F021 +BIB 12 42 +TITLE Low-energy measurement of the 7Be(p,g)8B cross section. +AUTHOR (F.Hammache,G.Bogaert,P.Aguer,C.Angulo,S.Barhoumi, + L.Brillard,J.F.Chemin,G.Claverie,A.Coc,M.Hussonnois, + M.Jacotin,J.Kiener,A.Lefebvre,C.Le Naour,S.Ouichaoui, + J.N.Scheurer,V.Tatischeff,J.P.Thibaud, + E.Virassamynaiken) +INSTITUTE (2FR PAR,2FR BOR,2BLGLVN,3ALGALG) +REFERENCE (J,PRL,86,3985,2001) +FACILITY (ACCEL,2FR PAR) +DETECTOR (SIBAR)Alpha particles with energies below 3.5 MeV and + emission angles between approximately 95 and 150 degr. + with respect to the beam direction were deflected + towards the solenoid axis and detected in an array of + 6*4 Si detectors (22 mm*45 mm*0.1 mm).The detectors + were mounted in cylindrical geometry (internal diameter + of 4 cm) aligned on the solenoid axis.Alpha particles + were detected at distances ranging from 18 to 36.5 cm + from the target. + (SCIN)Beta particles (Emax=14 MeV) were detected in + a set of 6 successive cylindrical plastic scintillators + (diameter 20 mm and thickness 3,3,8,8,8 and 10 mm) + centered on the field axis and 22 cm away from the + target. + The solenoidal superconducting magnet SOLENO + (3.2 T at the center,1.22 m long,32 cm of internal + diameter) in order to detect both alpha and beta + particles with high efficiency (11.5% and 25%, + respectively) due to the focusing power of the field. + Off-beam detection was necessary to avoid any + contamination in both alpha and beta+ coincidence + spectra arising from the channel 7Li(p,g1)8Be*(2alpha). +METHOD (GSPEC) + (TOF) +SAMPLE Highly radioactive 7Be target (132 mCi). +MONITOR (4-BE-9(P,A)3-LI-6,,SIG) + (4-BE-9(P,D)4-BE-8,,SIG) +CORRECTION Kinematics correction of 9.6% was applied to the + experimental efficiency value to take into account the + 8Be* in flight decay in the 7Li(p,g1)8Be* reaction. +ERR-ANALYS (DATA-ERR)Definition error + Uncertainty on the effective energy is 2.5 keV. +HISTORY (20041221C) +ENDBIB 42 +NOCOMMON 0 0 +ENDSUBENT 45 +SUBENT F0502002 20050419 20050831 F021 +BIB 2 2 +REACTION (4-BE-7(P,G)5-B-8,,SIG,,SFC) +STATUS Data from text. +ENDBIB 2 +NOCOMMON 0 0 +DATA 3 4 +EN-CM DATA-CM DATA-ERR +KEV B*EV B*EV + 0.0000 18.800 1.7000 + 111.70 15.800 2.7000 + 134.70 19.500 3.1000 + 185.80 17.200 2.1000 +ENDDATA 6 +ENDSUBENT 13 +ENDENTRY 2 diff --git a/exforall/F05/F0506.x4 b/exforall/F05/F0506.x4 new file mode 100644 index 000000000..7f1d21b61 --- /dev/null +++ b/exforall/F05/F0506.x4 @@ -0,0 +1,1410 @@ +ENTRY F0506 20050427 20050831 F021 +SUBENT F0506001 20050427 20050831 F021 +BIB 11 22 +TITLE Scattering of 25.6 MeV protons on 94Mo, 96Mo and 100Mo. +AUTHOR (E.Fretwurst,G.Lindstrom,K.F.Von Reden,V.Riech, + S.I.Vasiljev,P.P.Zarubin,O.M.Knyazkov,I.N.Kuchtina) +INSTITUTE (2GERHAM,4RUSSUL) +REFERENCE (J,NP/A,468,247,1987) +FACILITY (ISOCY,2GERHAM) +INC-SPECT Energy spread was 10 keV. +SAMPLE Mo metallic, self-supporting targets with a high degree + of homogeneity were employed. +DETECTOR (SOLST) 2 silicon semiconductor detectors mounted on a + coolable turntable were used in the angular range + between 7.5 and 168 degrees in steps of 2.5 to 5 + degrees. +MONITOR Target thicknesses were determined by weighing and by + measurement of the energy loss of alfa-particles. + Monitor detectors were used at +-25 degrees. + Absolute energy calibration was carried out using the + peak positions of the well-known quadrupole and + octupole one-phonon states and the ground state. +ERR-ANALYS Absolute integrated cross sections for the elastic + scattering were fixed to about +-1%. +HISTORY (20041201C) +ENDBIB 22 +COMMON 2 3 +EN-RSL EN +KEV MEV + 20. 25.6 +ENDCOMMON 3 +ENDSUBENT 29 +SUBENT F0506002 20050427 20050831 F021 +BIB 4 6 +REACTION (42-MO-94(P,INL)42-MO-94,PAR,SIG) +SAMPLE Target thickness was 670 mu-g/cm2, target homogeneity + was 0.2%/mm, isotopic enrichment was 88.4%. +ERR-ANALYS (E-LVL-ERR) Overall mean error taking into account + uncertanties of calibration. +STATUS (TABLE) Table 2 +ENDBIB 6 +COMMON 1 3 +E-LVL-ERR +KEV + 5. +ENDCOMMON 3 +DATA 2 20 +E-LVL DATA +KEV MB + 0.0000 1384.0 + 871.00 13.600 + 1573.0 2.1800 + 1741.0 0.16000 + 1864.0 0.31000 + 2066.0 1.1700 + 2421.0 0.39000 + 2534.0 14.600 + 2610.0 1.6700 + 2768.0 1.1000 + 2868.0 0.87000 + 2960.0 0.21000 + 3012.0 0.88000 + 3166.0 0.26000 + 3202.0 0.24000 + 3262.0 0.17000 + 3532.0 0.60000 + 3702.0 0.43000 + 3852.0 0.35000 + 4095.0 0.85000 +ENDDATA 22 +ENDSUBENT 37 +SUBENT F0506003 20050427 20050831 F021 +BIB 4 6 +REACTION (42-MO-96(P,INL)42-MO-96,PAR,SIG) +SAMPLE Target thickness was 390 mu-g/cm2, isotopic + enrichment was 96.7%. +ERR-ANALYS (E-LVL-ERR) Overall mean error taking into account + uncertanties of calibration. +STATUS (TABLE) Table 3 +ENDBIB 6 +COMMON 1 3 +E-LVL-ERR +KEV + 5. +ENDCOMMON 3 +DATA 2 29 +E-LVL DATA +KEV MB + 0.0000 1412.0 + 778.00 19.900 + 1148.0 0.21000 + 1498.0 1.1900 + 1627.0 1.4900 + 1870.0 1.7400 + 2234.0 16.600 + 2432.0 0.44000 + 2481.0 1.5300 + 2625.0 0.92000 + 2734.0 1.5100 + 2807.0 1.1100 + 2875.0 0.27000 + 2981.0 0.49000 + 3020.0 2.2800 + 3088.0 0.24000 + 3182.0 1.2200 + 3287.0 0.30000 + 3342.0 0.22000 + 3430.0 0.89000 + 3549.0 0.29000 + 3597.0 0.25000 + 3694.0 0.52000 + 3736.0 0.48000 + 3866.0 0.39000 + 3965.0 0.44000 + 4038.0 0.34000 + 4098.0 0.50000 + 4215.0 0.57000 +ENDDATA 31 +ENDSUBENT 46 +SUBENT F0506004 20050427 20050831 F021 +BIB 4 6 +REACTION (42-MO-100(P,INL)42-MO-100,PAR,SIG) +SAMPLE Target thickness was 590 mu-g/cm2, target homogeneity + was 0.7%/mm, isotopic enrichment was 93.8%. +ERR-ANALYS (E-LVL-ERR) Overall mean error taking into account + uncertanties of calibration. +STATUS (TABLE) Table 4 +ENDBIB 6 +COMMON 1 3 +E-LVL-ERR +KEV + 5. +ENDCOMMON 3 +DATA 2 26 +E-LVL DATA +KEV MB + 0.0000 1526.0 + 535.00 29.000 + 694.00 0.33000 + 1063.0 2.2000 + 1135.0 1.4900 + 1463.0 0.30000 + 1908.0 13.900 + 2101.0 0.59000 + 2158.0 0.64000 + 2202.0 0.50000 + 2288.0 0.70000 + 2342.0 0.94000 + 2371.0 1.5300 + 2418.0 1.2000 + 2516.0 1.5200 + 2565.0 0.71000 + 2610.0 1.2300 + 2658.0 0.40000 + 2740.0 0.43000 + 2812.0 0.90000 + 2838.0 1.0000 + 2931.0 0.80000 + 3000.0 0.60000 + 3050.0 0.95000 + 3296.0 0.37000 + 3365.0 0.50000 +ENDDATA 28 +ENDSUBENT 43 +SUBENT F0506005 20050427 20050831 F021 +BIB 4 6 +REACTION (42-MO-94(P,EL)42-MO-94,,DA,,RTH) +SAMPLE Target thickness was 670 mu-g/cm2, target homogeneity + was 0.2%/mm, isotopic enrichment was 88.4%. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error +STATUS (CURVE)Fig.2 +ENDBIB 6 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.1 0.1 +ENDCOMMON 3 +DATA 2 37 +ANG-CM DATA-CM +ADEG NO-DIM + 7.5129 0.84020 + 10.066 0.74419 + 12.622 0.66571 + 15.186 0.61956 + 17.629 0.65591 + 20.203 0.63511 + 22.625 0.61505 + 25.341 0.57233 + 30.326 0.51076 + 35.349 0.53936 + 40.485 0.48126 + 45.498 0.25158 + 50.608 0.10369 + 55.665 0.24420 + 60.719 0.56947 + 65.638 0.74046 + 70.586 0.56399 + 75.553 0.24187 + 80.755 0.77046E-01 + 85.651 0.17444 + 90.694 0.38714 + 95.758 0.48857 + 100.73 0.40681 + 105.79 0.26182 + 110.60 0.11119 + 115.66 0.70157E-01 + 120.64 0.12277 + 125.76 0.19075 + 130.67 0.23604 + 135.62 0.18705 + 140.53 0.11921 + 145.21 0.54270E-01 + 150.30 0.39724E-01 + 155.31 0.75995E-01 + 158.11 0.10508 + 165.08 0.18906 + 168.12 0.18664 +ENDDATA 39 +ENDSUBENT 54 +SUBENT F0506006 20050427 20050831 F021 +BIB 4 8 +REACTION (42-MO-96(P,EL)42-MO-96,,DA,,RTH) +SAMPLE Target thickness was 390 mu-g/cm2, isotopic + enrichment was 96.7%. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bar results from + peak-integrating procedure and is related to statistics +STATUS (CURVE)Fig.2 +ENDBIB 8 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.1 0.1 +ENDCOMMON 3 +DATA 3 43 +ANG-CM DATA-CM DATA-ERR +ADEG NO-DIM NO-DIM + 9.8484 0.76066 + 12.541 0.63483 + 15.100 0.57357 + 17.705 0.63801 + 20.288 0.64278 + 22.853 0.59827 + 25.121 0.57379 + 28.289 0.52328 + 30.425 0.54873 + 35.314 0.62742 + 38.350 0.62561 + 40.313 0.59428 + 42.394 0.48653 + 45.346 0.33300 + 50.396 0.10198 + 52.503 0.94024E-01 + 55.549 0.19318 + 60.659 0.59456 + 65.759 0.88805 + 70.591 0.78493 + 72.678 0.66198 + 75.628 0.44863 + 80.546 0.15022 + 82.601 0.10920 + 85.560 0.15250 + 90.769 0.37001 + 95.731 0.58657 + 100.76 0.63820 + 105.70 0.46728 + 110.71 0.23715 + 115.69 0.10273 + 120.76 0.13490 + 125.75 0.24810 + 130.67 0.32586 + 135.65 0.27680 + 140.77 0.22596 + 145.48 0.11700 + 150.47 0.53784E-010.13100E-01 + 155.14 0.92318E-010.95389E-02 + 159.29 0.23098 + 160.39 0.26506 + 165.30 0.33132 + 169.25 0.33668 +ENDDATA 45 +ENDSUBENT 62 +SUBENT F0506007 20050427 20050831 F021 +BIB 4 8 +REACTION (42-MO-100(P,EL)42-MO-100,,DA,,RTH) +SAMPLE Target thickness was 590 mu-g/cm2, target homogeneity + was 0.7%/mm, isotopic enrichment was 93.8%. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bars results from + peak-integrating procedure and is related to statistics +STATUS (CURVE)Fig.2 +ENDBIB 8 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.1 0.1 +ENDCOMMON 3 +DATA 3 42 +ANG-CM DATA-CM DATA-ERR +ADEG NO-DIM NO-DIM + 7.5998 0.88242 + 10.150 0.76661 + 12.691 0.64020 + 15.111 0.61400 + 17.687 0.60052 + 20.294 0.67443 + 22.998 0.59165 + 25.409 0.54545 + 30.445 0.61118 + 31.482 0.54234 + 36.388 0.67086 + 41.565 0.71539 + 45.650 0.33973 + 50.714 0.11074 + 55.627 0.14110 + 56.613 0.19724 + 60.778 0.52236 + 66.822 0.90308 + 71.820 0.85551 + 75.664 0.53583 + 77.752 0.45211 + 80.741 0.18533 + 85.830 0.13313 + 90.802 0.22147 0.34255E-01 + 96.956 0.62736 + 101.98 0.65601 + 105.86 0.49568 + 110.91 0.29517 + 115.89 0.12941 + 120.90 0.13137 + 126.82 0.25073 + 131.91 0.36318 + 134.82 0.39979 + 139.92 0.30775 + 141.70 0.25719 + 144.52 0.19262 + 150.55 0.16033 + 152.40 0.18019 + 155.49 0.22773 + 159.50 0.30212 + 165.34 0.41215 + 169.29 0.40659 +ENDDATA 44 +ENDSUBENT 61 +SUBENT F0506008 20050427 20050831 F021 +BIB 4 8 +REACTION (42-MO-94(P,INL)42-MO-94,PAR,DA) +SAMPLE Target thickness was 670 mu-g/cm2, target homogeneity + was 0.2%/mm, iostopic enrichment was 88.4%. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bar results from + peak-integrating procedure and is related to statistics +STATUS (CURVE)Fig.4,7,8 +ENDBIB 8 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.2 0.1 +ENDCOMMON 3 +DATA 4 402 +E-LVL ANG-CM DATA-CM DATA-ERR +KEV ADEG MB/SR MB/SR + 870.00 10.224 1.8645 0.48115 + 870.00 15.063 2.5453 0.15761 + 870.00 17.599 4.8742 0.39822 + 870.00 20.316 6.6375 0.27692 + 870.00 22.711 9.3621 0.45251 + 870.00 25.336 8.5621 0.41529 + 870.00 30.318 8.9237 0.37078 + 870.00 31.186 7.2690 0.25237 + 870.00 36.251 4.8765 0.17629 + 870.00 41.350 4.0780 0.14742 + 870.00 45.434 1.7714 0.61803E-01 + 870.00 50.431 1.7944 0.78125E-01 + 870.00 55.606 1.7300 + 870.00 56.501 1.7817 0.10417 + 870.00 60.536 1.4987 + 870.00 71.541 0.95649 0.41819E-01 + 870.00 75.671 0.89518 0.38973E-01 + 870.00 77.763 0.94987 0.39629E-01 + 870.00 80.732 0.60483 0.80187E-01 + 870.00 85.711 0.63486 0.27640E-01 + 870.00 90.753 0.44445 0.18543E-01 + 870.00 96.630 0.35902 0.19831E-01 + 870.00 101.62 0.36630 0.21416E-01 + 870.00 105.77 0.33321 + 870.00 110.63 0.33038 + 870.00 115.75 0.26476 + 870.00 120.65 0.24106 + 870.00 126.62 0.21820 + 870.00 129.65 0.16479 0.22507E-01 + 870.00 131.76 0.22266 + 870.00 134.62 0.23313 0.81341E-02 + 870.00 139.55 0.20054 + 870.00 141.70 0.19265 0.67217E-02 + 870.00 144.59 0.18923 0.78946E-02 + 870.00 150.35 0.25314 0.10561E-01 + 870.00 152.26 0.28426 0.99180E-02 + 870.00 155.22 0.32188 + 870.00 159.29 0.34234 0.17451E-01 + 870.00 165.09 0.31649 0.16133E-01 + 870.00 168.92 0.22283 0.80965E-02 + 1573.0 15.025 0.98401 0.11036 + 1573.0 17.487 1.1710 0.22698 + 1573.0 20.141 0.82841 0.92911E-01 + 1573.0 25.241 0.64970 0.56000E-01 + 1573.0 30.305 0.86716 0.63683E-01 + 1573.0 31.325 0.71684 0.61786E-01 + 1573.0 36.358 0.83033 0.60978E-01 + 1573.0 41.374 0.88547 0.65028E-01 + 1573.0 45.393 0.63272 0.38491E-01 + 1573.0 50.348 0.50819 0.30915E-01 + 1573.0 55.404 0.65467 0.48078E-01 + 1573.0 56.344 0.37526 0.27558E-01 + 1573.0 60.374 0.28112 0.20645E-01 + 1573.0 66.345 0.37036 0.27198E-01 + 1573.0 71.384 0.21877 0.13309E-01 + 1573.0 75.455 0.19797 0.17064E-01 + 1573.0 77.566 0.18831 0.16231E-01 + 1573.0 80.386 0.14297 0.17957E-01 + 1573.0 85.322 0.10572 0.64316E-02 + 1573.0 90.407 0.77243E-010.86632E-02 + 1573.0 96.397 0.55052E-010.61744E-02 + 1573.0 101.38 0.49760E-010.69037E-02 + 1573.0 105.50 0.57707E-010.20814E-02 + 1573.0 110.30 0.46359E-010.34045E-02 + 1573.0 115.44 0.43921E-010.26812E-02 + 1573.0 120.29 0.42623E-010.15374E-02 + 1573.0 126.33 0.38472E-010.23405E-02 + 1573.0 129.41 0.47960E-010.35324E-02 + 1573.0 131.37 0.45629E-010.33607E-02 + 1573.0 134.27 0.49961E-010.36691E-02 + 1573.0 139.12 0.50830E-010.30922E-02 + 1573.0 141.23 0.47782E-010.35090E-02 + 1573.0 144.09 0.43824E-010.32184E-02 + 1573.0 150.14 0.40983E-010.24932E-02 + 1573.0 152.11 0.40877E-010.24954E-02 + 1573.0 154.98 0.39772E-010.29208E-02 + 1573.0 158.91 0.38189E-010.32916E-02 + 1573.0 164.85 0.42144E-010.36325E-02 + 1573.0 168.73 0.31953E-010.19506E-02 + 1741.0 20.168 0.15378 0.34157E-01 + 1741.0 25.354 0.88748E-010.34768E-01 + 1741.0 30.403 0.54986E-010.13831E-01 + 1741.0 31.358 0.67916E-010.25479E-01 + 1741.0 41.446 0.49897E-010.69038E-02 + 1741.0 50.321 0.90139E-020.30926E-02 + 1741.0 56.512 0.16323E-010.43484E-02 + 1741.0 66.364 0.16304E-010.43393E-02 + 1741.0 77.669 0.12245E-010.34461E-02 + 1741.0 85.503 0.48844E-020.80972E-03 + 1741.0 96.586 0.10741E-010.16362E-02 + 1741.0 105.51 0.49292E-020.74974E-03 + 1741.0 115.54 0.13760E-020.36621E-03 + 1741.0 120.48 0.20421E-020.33852E-03 + 1741.0 126.61 0.57910E-020.45908E-03 + 1741.0 129.56 0.78405E-020.15199E-02 + 1741.0 131.34 0.65530E-020.59144E-03 + 1741.0 134.34 0.58006E-020.82585E-03 + 1741.0 139.37 0.66391E-020.74528E-03 + 1741.0 141.32 0.59548E-020.82527E-03 + 1741.0 144.41 0.39238E-020.54379E-03 + 1741.0 150.22 0.24002E-020.43110E-03 + 1741.0 152.27 0.17405E-020.38702E-03 + 1741.0 155.05 0.22219E-020.39909E-03 + 1741.0 165.01 0.37300E-020.61834E-03 + 1741.0 168.83 0.84787E-020.94990E-03 + 1864.0 25.255 0.31956 0.51907E-01 + 1864.0 30.333 0.22531 0.16555E-01 + 1864.0 31.406 0.11884 0.28167E-01 + 1864.0 36.458 0.37066E-010.11005E-01 + 1864.0 41.494 0.43448E-010.72143E-02 + 1864.0 45.423 0.82805E-010.71407E-02 + 1864.0 50.424 0.82261E-010.13659E-01 + 1864.0 55.537 0.68432E-010.41651E-02 + 1864.0 56.461 0.73372E-010.72747E-02 + 1864.0 60.527 0.64844E-010.81336E-02 + 1864.0 66.493 0.20684E-010.34394E-02 + 1864.0 71.493 0.20548E-010.23058E-02 + 1864.0 77.549 0.19909E-010.35817E-02 + 1864.0 80.510 0.28948E-010.77248E-02 + 1864.0 85.477 0.24662E-010.18121E-02 + 1864.0 90.536 0.16008E-010.55018E-02 + 1864.0 101.52 0.11199E-010.34975E-02 + 1864.0 110.51 0.14018E-010.85321E-03 + 1864.0 115.53 0.14949E-010.90987E-03 + 1864.0 120.57 0.17942E-010.10920E-02 + 1864.0 126.58 0.14220E-010.10448E-02 + 1864.0 129.51 0.18156E-010.13340E-02 + 1864.0 131.56 0.13005E-010.11243E-02 + 1864.0 134.42 0.11511E-010.12917E-02 + 1864.0 139.43 0.12132E-010.89138E-03 + 1864.0 141.55 0.59526E-020.34886E-02 + 1864.0 144.29 0.12489E-010.91766E-03 + 1864.0 150.29 0.18963E-010.18801E-02 + 1864.0 152.26 0.19139E-010.14062E-02 + 1864.0 155.01 0.20715E-010.10026E-02 + 1864.0 159.10 0.21347E-010.15684E-02 + 1864.0 165.01 0.21181E-010.15563E-02 + 1864.0 168.96 0.21832E-010.16041E-02 + 2421.0 25.390 0.12397 0.29145E-01 + 2421.0 36.505 0.10882 0.17411E-01 + 2421.0 41.482 0.10587 0.12808E-01 + 2421.0 45.393 0.81126E-010.72580E-02 + 2421.0 50.371 0.49997E-010.11045E-01 + 2421.0 55.484 0.59726E-010.70500E-02 + 2421.0 56.464 0.42129E-010.19976E-01 + 2421.0 60.665 0.62926E-010.80161E-02 + 2421.0 66.709 0.31189E-010.62496E-02 + 2421.0 75.813 0.16227E-010.25963E-02 + 2421.0 85.552 0.17515E-010.20073E-02 + 2421.0 96.535 0.15823E-010.26366E-02 + 2421.0 110.41 0.14584E-010.15766E-02 + 2421.0 115.42 0.14935E-010.12413E-02 + 2421.0 120.35 0.10738E-010.89250E-03 + 2421.0 126.33 0.96905E-020.74575E-03 + 2421.0 129.28 0.10832E-010.11028E-02 + 2421.0 131.21 0.80361E-020.96964E-03 + 2421.0 134.32 0.57878E-020.24573E-02 + 2421.0 139.22 0.79757E-020.11192E-02 + 2421.0 141.24 0.68239E-020.11371E-02 + 2421.0 150.05 0.72059E-020.96326E-03 + 2421.0 152.17 0.89842E-020.17389E-02 + 2421.0 155.11 0.78573E-020.11538E-02 + 2421.0 159.07 0.12861E-010.19729E-02 + 2421.0 164.95 0.98933E-020.11322E-02 + 2421.0 168.85 0.93636E-020.14349E-02 + 2534.0 12.657 1.3293 0.48587 + 2534.0 14.912 1.3810 0.85517E-01 + 2534.0 17.483 1.8669 0.29314 + 2534.0 20.003 2.0830 0.11506 + 2534.0 22.525 1.7366 0.20841 + 2534.0 25.096 2.3476 + 2534.0 30.257 4.1405 + 2534.0 31.245 3.5705 + 2534.0 36.097 4.7711 + 2534.0 41.182 5.4542 + 2534.0 45.317 3.7871 + 2534.0 50.301 2.9491 + 2534.0 55.371 1.9504 + 2534.0 56.414 2.0234 + 2534.0 60.474 1.6194 + 2534.0 66.493 1.3270 + 2534.0 71.664 1.2883 + 2534.0 75.502 1.1799 + 2534.0 77.582 1.2789 + 2534.0 80.615 0.95896 + 2534.0 85.601 0.99231 + 2534.0 90.722 0.79515 + 2534.0 96.745 0.64696 + 2534.0 101.59 0.37108 0.24496E-01 + 2534.0 105.54 0.36233 + 2534.0 110.59 0.33229 + 2534.0 115.62 0.32027 + 2534.0 120.58 0.34584 + 2534.0 126.53 0.32434 + 2534.0 129.49 0.36724 + 2534.0 131.70 0.31713 + 2534.0 134.58 0.31370 + 2534.0 139.56 0.24778 + 2534.0 141.57 0.22968 + 2534.0 144.49 0.21162 + 2534.0 150.49 0.24217 + 2534.0 152.29 0.24968 + 2534.0 155.39 0.29717 + 2534.0 159.13 0.32503 + 2534.0 165.27 0.37467 + 2534.0 168.98 0.32875 + 2768.0 25.438 0.24034 0.38351E-01 + 2768.0 30.438 0.24192 0.23053E-01 + 2768.0 31.547 0.26023 0.46719E-01 + 2768.0 36.524 0.25315 0.20986E-01 + 2768.0 41.543 0.26218 0.25517E-01 + 2768.0 45.647 0.21519 0.14200E-01 + 2768.0 50.527 0.22673 0.14676E-01 + 2768.0 55.558 0.19130 0.89070E-02 + 2768.0 56.618 0.15306 0.19447E-01 + 2768.0 60.586 0.16049 0.80099E-02 + 2768.0 66.645 0.12925 0.99210E-02 + 2768.0 71.699 0.11284 0.79720E-02 + 2768.0 75.730 0.10380 0.79832E-02 + 2768.0 80.568 0.52777E-010.24508E-01 + 2768.0 85.614 0.71016E-01 + 2768.0 90.731 0.43560E-010.78203E-02 + 2768.0 96.622 0.10407 0.73525E-02 + 2768.0 101.53 0.91912E-010.24143E-01 + 2768.0 105.62 0.59062E-01 + 2768.0 110.49 0.61175E-01 + 2768.0 115.49 0.49040E-01 + 2768.0 120.63 0.48798E-01 + 2768.0 126.34 0.36718E-01 + 2768.0 129.39 0.38098E-010.20013E-02 + 2768.0 131.43 0.33740E-010.15709E-02 + 2768.0 134.46 0.42485E-010.22318E-02 + 2768.0 139.37 0.37520E-010.16745E-02 + 2768.0 141.48 0.36601E-010.16233E-02 + 2768.0 144.40 0.31299E-010.14573E-02 + 2768.0 150.34 0.41367E-010.19261E-02 + 2768.0 152.22 0.36640E-010.21447E-02 + 2768.0 155.15 0.31331E-010.15637E-02 + 2768.0 159.21 0.30506E-010.20171E-02 + 2768.0 165.21 0.28167E-010.15576E-02 + 2768.0 169.03 0.18948E-010.15708E-02 + 3202.0 20.196 0.14772 0.45322E-01 + 3202.0 31.081 0.10413 0.27074E-01 + 3202.0 36.082 0.66490E-010.11391E-01 + 3202.0 41.079 0.47366E-010.81144E-02 + 3202.0 45.166 0.37181E-010.63696E-02 + 3202.0 50.316 0.25230E-010.81447E-02 + 3202.0 55.296 0.26526E-010.57004E-02 + 3202.0 56.498 0.29968E-010.82534E-02 + 3202.0 60.450 0.16331E-010.42459E-02 + 3202.0 66.625 0.22446E-010.35274E-02 + 3202.0 71.506 0.73408E-020.11536E-02 + 3202.0 75.451 0.46291E-020.22027E-02 + 3202.0 77.556 0.56959E-020.30228E-02 + 3202.0 85.580 0.10323 + 3202.0 96.391 0.12781E-010.23734E-02 + 3202.0 115.27 0.94808E-020.66727E-03 + 3202.0 120.25 0.10854E-010.11092E-02 + 3202.0 126.31 0.69323E-020.89629E-03 + 3202.0 129.19 0.53091E-020.12195E-02 + 3202.0 131.29 0.72002E-020.93128E-03 + 3202.0 139.14 0.63127E-020.81649E-03 + 3202.0 141.13 0.41264E-020.82592E-03 + 3202.0 144.12 0.76799E-020.99332E-03 + 3202.0 150.02 0.55394E-020.56612E-03 + 3202.0 151.96 0.86928E-020.13661E-02 + 3202.0 154.99 0.80880E-020.10461E-02 + 3202.0 164.93 0.11683E-010.10837E-02 + 3202.0 168.72 0.78290E-020.98044E-03 + 3262.0 25.165 1.1073 0.82493 + 3262.0 30.029 0.54328 0.15710 + 3262.0 31.217 0.82985 0.22706 + 3262.0 36.233 0.39745 0.14030 + 3262.0 41.193 0.63792 0.82035E-01 + 3262.0 45.300 0.32843 0.13238 + 3262.0 50.444 0.26142 0.96584E-01 + 3262.0 55.416 0.32157 0.83063E-01 + 3262.0 56.333 0.25562 0.77929E-01 + 3262.0 66.480 0.12715 0.30921E-01 + 3262.0 71.618 0.11561 0.22986E-01 + 3262.0 75.671 0.18550 0.21329E-01 + 3262.0 77.639 0.16647 0.35537E-01 + 3262.0 80.637 0.26382 0.84599E-01 + 3262.0 85.614 0.28756 0.33064E-01 + 3262.0 115.27 0.65558E-010.84306E-02 + 3262.0 120.40 0.80646E-010.71241E-02 + 3262.0 126.30 0.55532E-010.56409E-02 + 3262.0 129.33 0.44173E-010.10082E-01 + 3262.0 131.30 0.36424E-010.10531E-01 + 3262.0 139.35 0.15286E-010.53951E-02 + 3262.0 150.18 0.34483E-010.44309E-02 + 3262.0 152.12 0.47251E-010.80441E-02 + 3262.0 155.12 0.78594E-010.90329E-02 + 3262.0 159.05 0.70573E-010.14036E-01 + 3262.0 164.91 0.11892 0.96473E-02 + 3262.0 168.87 0.66630E-010.90003E-02 + 3456.0 20.414 0.25473 0.42340E-01 + 3456.0 25.399 0.23722 0.41820E-01 + 3456.0 30.216 0.32161 0.46878E-01 + 3456.0 36.106 0.30693 + 3456.0 41.223 0.43684 + 3456.0 45.314 0.31531 + 3456.0 50.296 0.31197 + 3456.0 55.436 0.26690 + 3456.0 56.641 0.28368 + 3456.0 60.580 0.20977 + 3456.0 66.634 0.14968 + 3456.0 71.636 0.95733E-01 + 3456.0 75.722 0.77064E-010.71205E-02 + 3456.0 77.519 0.10566 + 3456.0 80.543 0.94828E-010.12831E-01 + 3456.0 85.683 0.82118E-01 + 3456.0 90.784 0.16409 + 3456.0 96.556 0.76604E-010.62303E-02 + 3456.0 101.55 0.55982E-010.81598E-02 + 3456.0 105.48 0.51489E-01 + 3456.0 110.48 0.37175E-01 + 3456.0 115.32 0.26839E-01 + 3456.0 120.30 0.28557E-01 + 3456.0 126.35 0.21649E-010.33775E-02 + 3456.0 129.35 0.34341E-01 + 3456.0 131.32 0.33135E-01 + 3456.0 134.33 0.38355E-01 + 3456.0 139.32 0.34442E-01 + 3456.0 141.28 0.34047E-01 + 3456.0 144.29 0.39412E-01 + 3456.0 150.32 0.45112E-01 + 3456.0 152.13 0.46243E-01 + 3456.0 155.15 0.50382E-01 + 3456.0 159.22 0.52948E-01 + 3456.0 164.95 0.62844E-010.55637E-02 + 3456.0 168.90 0.41168E-01 + 3532.0 10.153 1.2686 0.54236 + 3532.0 15.206 0.22432 0.72152E-01 + 3532.0 17.558 1.0469 0.23537 + 3532.0 20.193 0.19657 0.72851E-01 + 3532.0 22.632 0.11125 0.10353 + 3532.0 25.173 0.20412 0.51545E-01 + 3532.0 29.901 0.63813E-010.11253E-01 + 3532.0 31.099 0.80371E-010.26506E-01 + 3532.0 41.064 0.77705E-010.89596E-02 + 3532.0 45.146 0.67256E-010.77547E-02 + 3532.0 50.166 0.26798E-010.38235E-02 + 3532.0 55.315 0.18205E-010.49950E-02 + 3532.0 60.354 0.45205E-020.23064E-02 + 3532.0 66.479 0.21376E-010.61985E-02 + 3532.0 71.465 0.19662E-010.30786E-02 + 3532.0 75.392 0.18751E-010.48588E-02 + 3532.0 77.351 0.20422E-010.56056E-02 + 3532.0 85.350 0.21483E-010.33646E-02 + 3532.0 96.405 0.92204E-020.50456E-02 + 3532.0 105.33 0.53556E-020.10680E-02 + 3532.0 110.30 0.89238E-020.11503E-02 + 3532.0 115.09 0.20879E-010.10385E-02 + 3532.0 120.12 0.73693E-020.84970E-03 + 3532.0 126.16 0.66180E-020.58623E-03 + 3532.0 129.18 0.68687E-020.12708E-02 + 3532.0 131.00 0.47765E-020.74830E-03 + 3532.0 134.16 0.60924E-020.11271E-02 + 3532.0 139.16 0.41386E-020.82531E-03 + 3532.0 141.11 0.61036E-020.10421E-02 + 3532.0 143.99 0.46217E-020.85528E-03 + 3532.0 149.99 0.10058E-010.10241E-02 + 3532.0 151.97 0.76141E-020.87793E-03 + 3532.0 154.97 0.11649E-010.11865E-02 + 3532.0 158.87 0.21123E-010.21525E-02 + 3532.0 164.77 0.17008E-010.15066E-02 + 3532.0 168.70 0.15265E-010.15549E-02 + 3796.0 15.331 0.39091 0.83576E-01 + 3796.0 20.355 0.15036 0.43549E-01 + 3796.0 25.361 0.87306E-010.29453E-01 + 3796.0 30.176 0.12422 0.17703E-01 + 3796.0 31.243 0.99916E-010.26996E-01 + 3796.0 36.220 0.11158 0.14368E-01 + 3796.0 41.216 0.80572E-010.74409E-02 + 3796.0 45.466 0.47920E-010.54683E-02 + 3796.0 50.463 0.34186E-010.44002E-02 + 3796.0 55.427 0.51057E-010.51949E-02 + 3796.0 56.491 0.43106E-010.88629E-02 + 3796.0 60.577 0.34285E-010.56959E-02 + 3796.0 66.611 0.38766E-010.48357E-02 + 3796.0 71.604 0.30103E-010.34351E-02 + 3796.0 75.692 0.23088E-010.42677E-02 + 3796.0 77.794 0.29434E-010.50180E-02 + 3796.0 85.677 0.14263E-010.28416E-02 + 3796.0 105.63 0.76408E-020.11953E-02 + 3796.0 110.43 0.17648E-01 + 3796.0 115.42 0.13704E-010.12126E-02 + 3796.0 120.55 0.14581E-010.16793E-02 + 3796.0 126.61 0.92182E-02 + 3796.0 129.46 0.14268E-010.16276E-02 + 3796.0 131.45 0.64185E-020.82616E-03 + 3796.0 134.44 0.13947E-010.12334E-02 + 3796.0 139.46 0.59103E-020.92460E-03 + 3796.0 141.42 0.67563E-020.10570E-02 + 3796.0 144.44 0.66003E-020.11256E-02 + 3796.0 150.29 0.12871E-010.14824E-02 + 3796.0 152.12 0.87399E-020.11254E-02 + 3796.0 155.28 0.13046E-010.12048E-02 + 3796.0 159.21 0.10760E-010.15335E-02 + 3796.0 165.38 0.14769E-01 + 3796.0 169.16 0.13098E-010.12096E-02 +ENDDATA 404 +ENDSUBENT 421 +SUBENT F0506009 20050427 20050831 F021 +BIB 4 8 +REACTION (42-MO-96(P,INL)42-MO-96,PAR,DA) +SAMPLE Target thickness was 390 mu-g/cm2, isotopic + enrichment was 96.7%. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bars results from + peak-integrating procedure and is related to statistics +STATUS (CURVE)Fig.1,3b,5,9 +ENDBIB 8 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.1 0.1 +ENDCOMMON 3 +DATA 4 366 +E-LVL ANG-CM DATA-CM DATA-ERR +KEV ADEG MB/SR MB/SR + 778.00 10.222 4.1011 0.56057 + 778.00 12.646 3.0628 0.44351 + 778.00 15.230 3.4318 0.27949 + 778.00 17.526 8.3538 0.55265 + 778.00 20.109 9.0976 0.32960 + 778.00 22.694 10.488 0.43855 + 778.00 25.279 12.265 + 778.00 28.315 11.421 + 778.00 30.440 10.485 + 778.00 35.595 6.4605 + 778.00 38.480 6.3232 0.17749 + 778.00 40.595 3.4281 + 778.00 42.413 2.7688 + 778.00 45.605 3.0803 0.88960E-01 + 778.00 50.614 2.6521 + 778.00 52.741 2.7285 + 778.00 55.625 2.5048 + 778.00 60.632 1.9520 0.42117E-01 + 778.00 65.486 1.4167 + 778.00 70.648 1.2730 + 778.00 72.774 1.2284 + 778.00 75.812 1.2282 0.42942E-01 + 778.00 80.822 1.1355 + 778.00 82.794 1.0132 + 778.00 85.828 0.83000 0.23303E-01 + 778.00 90.984 0.54915 + 778.00 96.144 0.43720 + 778.00 101.16 0.47271 + 778.00 106.02 0.50030 + 778.00 110.88 0.44955 + 778.00 115.88 0.35034 0.12693E-01 + 778.00 120.74 0.28292 + 778.00 125.75 0.25970 0.94089E-02 + 778.00 130.61 0.25965 0.11329E-01 + 778.00 135.62 0.23497 0.13768E-01 + 778.00 140.63 0.23829 + 778.00 145.34 0.21412 0.93423E-02 + 778.00 150.35 0.23989 0.86912E-02 + 778.00 155.37 0.30989 0.86965E-02 + 778.00 159.32 0.35724 + 778.00 160.39 0.37547 0.10846E-01 + 778.00 165.09 0.32559 + 778.00 169.03 0.22968 + 1148.0 19.897 0.17103 0.43962E-01 + 1148.0 22.478 0.17282 0.82152E-01 + 1148.0 30.141 0.55525E-010.74448E-02 + 1148.0 35.101 0.26957E-010.57862E-02 + 1148.0 52.347 0.11617E-010.23331E-02 + 1148.0 60.392 0.11714E-010.23525E-02 + 1148.0 65.405 0.12379E-010.23170E-02 + 1148.0 70.567 0.12496E-010.20042E-02 + 1148.0 75.558 0.96969E-020.16841E-02 + 1148.0 85.727 0.95484E-020.12802E-02 + 1148.0 90.775 0.16691E-010.11868E-02 + 1148.0 95.651 0.21922E-010.18289E-02 + 1148.0 100.63 0.13846E-010.98363E-03 + 1148.0 105.62 0.10868E-010.10414E-02 + 1148.0 110.71 0.39640E-020.10766E-02 + 1148.0 120.59 0.44781E-020.48556E-03 + 1148.0 125.77 0.65185E-020.87443E-03 + 1148.0 130.65 0.80854E-020.87670E-03 + 1148.0 135.68 0.11244E-010.93728E-03 + 1148.0 140.38 0.10721E-010.89371E-03 + 1148.0 145.03 0.46965E-020.44973E-03 + 1148.0 150.02 0.35215E-020.47216E-03 + 1148.0 158.93 0.18921E-020.38000E-03 + 1148.0 159.87 0.28552E-020.34599E-03 + 1148.0 164.94 0.72798E-020.60685E-03 + 1148.0 168.75 0.83384E-020.59236E-03 + 1498.0 17.386 0.77029 0.17543 + 1498.0 19.938 0.49337 0.59538E-01 + 1498.0 22.509 0.42989 0.11007 + 1498.0 24.802 0.55195 0.52665E-01 + 1498.0 27.997 0.61787 + 1498.0 30.106 0.48596 + 1498.0 35.107 0.42790 + 1498.0 38.134 0.37278 + 1498.0 40.244 0.29656 + 1498.0 42.357 0.24693 + 1498.0 45.369 0.17126 + 1498.0 50.508 0.12143 + 1498.0 52.463 0.91255E-010.98588E-02 + 1498.0 55.494 0.85128E-01 + 1498.0 60.503 0.84971E-01 + 1498.0 70.527 0.92742E-01 + 1498.0 72.492 0.82691E-01 + 1498.0 75.529 0.83546E-01 + 1498.0 80.676 0.67919E-01 + 1498.0 82.641 0.59872E-01 + 1498.0 85.659 0.45491E-010.34888E-02 + 1498.0 90.646 0.32257E-01 + 1498.0 95.632 0.22613E-010.18782E-02 + 1498.0 100.67 0.34413E-01 + 1498.0 105.68 0.33195E-01 + 1498.0 110.55 0.40682E-01 + 1498.0 115.70 0.36646E-01 + 1498.0 120.70 0.33391E-01 + 1498.0 125.68 0.21860E-01 + 1498.0 130.52 0.15501E-01 + 1498.0 135.67 0.13649E-010.20007E-02 + 1498.0 140.39 0.15622E-01 + 1498.0 145.28 0.25459E-01 + 1498.0 149.99 0.29140E-010.35183E-02 + 1498.0 155.01 0.37377E-010.31045E-02 + 1498.0 158.82 0.44792E-01 + 1498.0 160.04 0.45286E-01 + 1498.0 164.89 0.40797E-01 + 1498.0 168.67 0.35532E-01 + 1627.0 12.308 0.96158 0.44043 + 1627.0 20.015 0.59323 0.71812E-01 + 1627.0 25.001 0.42505 0.56930E-01 + 1627.0 28.037 0.42454 0.45956E-01 + 1627.0 30.164 0.43898 0.15309E-01 + 1627.0 35.179 0.47459 0.33680E-01 + 1627.0 38.369 0.49052 0.28841E-01 + 1627.0 40.487 0.44729 0.15599E-01 + 1627.0 42.457 0.42697 0.14891E-01 + 1627.0 45.484 0.37181 0.12967E-01 + 1627.0 50.468 0.26039 0.15310E-01 + 1627.0 52.583 0.22683 0.10609E-01 + 1627.0 55.446 0.16834 0.14018E-01 + 1627.0 60.442 0.13834 0.98176E-02 + 1627.0 65.593 0.12037 0.85421E-02 + 1627.0 70.607 0.12866 0.91301E-02 + 1627.0 72.725 0.11732 0.83255E-02 + 1627.0 75.607 0.11323 0.94294E-02 + 1627.0 80.601 0.90955E-010.53479E-02 + 1627.0 82.716 0.79233E-010.56229E-02 + 1627.0 85.745 0.72225E-010.51255E-02 + 1627.0 90.745 0.62845E-010.44599E-02 + 1627.0 95.596 0.57902E-010.34045E-02 + 1627.0 100.76 0.57127E-010.19252E-02 + 1627.0 105.77 0.57014E-010.54576E-02 + 1627.0 110.76 0.49046E-010.40843E-02 + 1627.0 115.76 0.41713E-010.24526E-02 + 1627.0 120.77 0.39770E-010.18600E-02 + 1627.0 125.78 0.39240E-010.27847E-02 + 1627.0 130.78 0.38717E-010.18107E-02 + 1627.0 135.79 0.37767E-010.26826E-02 + 1627.0 140.50 0.37697E-010.22165E-02 + 1627.0 145.19 0.30632E-010.21738E-02 + 1627.0 150.20 0.32740E-010.23234E-02 + 1627.0 155.06 0.34996E-010.24835E-02 + 1627.0 159.17 0.36994E-010.26253E-02 + 1627.0 160.07 0.36145E-010.21275E-02 + 1627.0 164.94 0.40442E-010.23779E-02 + 1627.0 168.88 0.38575E-010.27375E-02 + 2235.0 12.543 1.6587 0.40880 + 2235.0 14.970 1.5120 0.26849 + 2235.0 17.410 2.0231 0.26807 + 2235.0 19.989 1.8574 0.12268 + 2235.0 22.576 2.1559 0.19026 + 2235.0 25.167 2.8238 + 2235.0 28.212 3.4940 + 2235.0 30.194 4.4169 + 2235.0 35.367 5.7024 + 2235.0 38.254 5.9074 + 2235.0 40.378 5.5801 + 2235.0 42.350 5.1232 + 2235.0 45.384 4.6370 + 2235.0 50.535 3.2031 + 2235.0 52.504 2.6623 + 2235.0 55.533 2.1053 + 2235.0 60.540 1.7745 + 2235.0 65.397 1.6405 + 2235.0 70.407 1.5058 + 2235.0 72.532 1.4634 + 2235.0 75.570 1.4946 + 2235.0 80.580 1.3817 + 2235.0 82.707 1.4213 + 2235.0 85.737 1.1400 + 2235.0 90.741 0.88235 + 2235.0 95.743 0.66378 + 2235.0 100.90 0.53995 + 2235.0 105.75 0.45189 + 2235.0 110.76 0.39748 + 2235.0 115.62 0.39173 + 2235.0 120.64 0.40288 + 2235.0 125.49 0.36201 + 2235.0 130.65 0.30730 + 2235.0 135.35 0.23617 + 2235.0 140.35 0.19075 + 2235.0 145.21 0.14869 + 2235.0 150.07 0.16419 + 2235.0 155.25 0.24435 + 2235.0 159.05 0.27565 + 2235.0 160.11 0.28969 + 2235.0 164.98 0.32446 + 2235.0 168.92 0.29364 + 2739.0 25.230 0.32795 0.52511E-01 + 2739.0 28.422 0.30181 0.35505E-01 + 2739.0 30.238 0.30242 + 2739.0 35.398 0.27550 + 2739.0 40.553 0.26046 + 2739.0 42.514 0.27091 + 2739.0 45.554 0.24927 + 2739.0 50.581 0.20564 + 2739.0 52.550 0.20355 + 2739.0 55.600 0.17606 + 2739.0 60.569 0.20539 + 2739.0 65.707 0.21439 + 2739.0 70.592 0.16622 + 2739.0 72.710 0.16662 + 2739.0 75.757 0.14772 + 2739.0 80.684 0.89415E-01 + 2739.0 82.808 0.86361E-01 + 2739.0 85.830 0.88826E-01 + 2739.0 90.709 0.71473E-01 + 2739.0 95.725 0.62725E-010.74029E-02 + 2739.0 100.74 0.55734E-01 + 2739.0 105.76 0.47130E-01 + 2739.0 110.61 0.45097E-01 + 2739.0 115.63 0.38610E-01 + 2739.0 120.47 0.38820E-01 + 2739.0 125.48 0.36244E-01 + 2739.0 130.63 0.34266E-01 + 2739.0 135.49 0.30821E-010.32021E-02 + 2739.0 140.34 0.30607E-01 + 2739.0 145.17 0.33146E-01 + 2739.0 150.20 0.25387E-010.37025E-02 + 2739.0 154.98 0.37928E-01 + 2739.0 159.06 0.39057E-01 + 2739.0 160.08 0.48862E-01 + 2739.0 165.10 0.41833E-01 + 2739.0 168.91 0.37120E-01 + 2807.0 25.108 0.19996 0.20812E-01 + 2807.0 28.128 0.20824 + 2807.0 28.160 0.17296 + 2807.0 30.261 0.19142 + 2807.0 35.223 0.23178 + 2807.0 38.314 0.15847 0.27663E-01 + 2807.0 40.203 0.25107 + 2807.0 42.323 0.24858 + 2807.0 45.246 0.18761 + 2807.0 50.277 0.15100 + 2807.0 52.265 0.13372 + 2807.0 55.359 0.90299E-01 + 2807.0 70.449 0.47665E-01 + 2807.0 72.536 0.57527E-01 + 2807.0 75.534 0.67803E-01 + 2807.0 80.536 0.64895E-01 + 2807.0 82.656 0.64251E-01 + 2807.0 85.468 0.38324E-010.39888E-02 + 2807.0 95.519 0.26411E-010.31120E-02 + 2807.0 100.33 0.13113E-01 + 2807.0 105.24 0.21906E-01 + 2807.0 110.39 0.21231E-01 + 2807.0 115.39 0.19580E-010.23071E-02 + 2807.0 120.24 0.18737E-010.22078E-02 + 2807.0 125.09 0.18380E-010.32122E-02 + 2807.0 130.10 0.16951E-01 + 2807.0 145.03 0.94001E-020.13710E-02 + 2807.0 149.96 0.13875E-010.30385E-02 + 2807.0 154.85 0.25275E-01 + 2807.0 158.87 0.35910E-01 + 2807.0 159.93 0.36401E-010.32943E-02 + 2807.0 164.65 0.30395E-01 + 2807.0 168.76 0.26982E-01 + 2981.0 20.341 0.29208 0.46820E-01 + 2981.0 28.427 0.20078 0.32145E-01 + 2981.0 35.383 0.86074E-010.90822E-02 + 2981.0 60.513 0.34128E-010.40258E-02 + 2981.0 65.642 0.37442E-010.35332E-02 + 2981.0 70.703 0.25333E-010.23946E-02 + 2981.0 82.848 0.20302E-01 + 2981.0 85.721 0.20624E-010.24288E-02 + 2981.0 90.603 0.16389E-01 + 2981.0 100.62 0.32780E-01 + 2981.0 105.47 0.13507E-01 + 2981.0 120.48 0.11133E-010.14685E-02 + 2981.0 125.41 0.69916E-020.12205E-02 + 2981.0 130.29 0.56254E-020.90176E-03 + 2981.0 135.23 0.73395E-020.10717E-02 + 2981.0 150.18 0.89933E-020.10591E-02 + 2981.0 155.08 0.63140E-020.92194E-03 + 2981.0 159.00 0.71795E-020.84693E-03 + 2981.0 165.03 0.79834E-020.94176E-03 + 2981.0 168.85 0.65765E-020.62060E-03 + 3088.0 30.339 0.47439E-010.69189E-02 + 3088.0 35.393 0.33320E-010.11524E-01 + 3088.0 38.514 0.46708E-010.18533E-01 + 3088.0 40.426 0.26487E-010.54034E-02 + 3088.0 45.530 0.33704E-010.57155E-02 + 3088.0 50.432 0.23669E-010.70253E-02 + 3088.0 52.572 0.20964E-010.49092E-02 + 3088.0 55.573 0.24403E-010.42600E-02 + 3088.0 60.625 0.42314E-010.55749E-02 + 3088.0 65.634 0.15807E-010.32246E-02 + 3088.0 70.674 0.29521E-010.34785E-02 + 3088.0 72.657 0.26797E-010.35358E-02 + 3088.0 75.723 0.21254E-010.25044E-02 + 3088.0 80.809 0.30232E-010.39832E-02 + 3088.0 85.767 0.15200E-010.31008E-02 + 3088.0 90.754 0.15864E-010.20901E-02 + 3088.0 95.707 0.82777E-020.32864E-02 + 3088.0 100.62 0.12998E-010.15315E-02 + 3088.0 105.62 0.12752E-010.11516E-02 + 3088.0 110.49 0.10649E-010.12397E-02 + 3088.0 115.46 0.12894E-010.11669E-02 + 3088.0 120.47 0.11745E-010.74975E-03 + 3088.0 125.31 0.11520E-010.15178E-02 + 3088.0 130.34 0.95040E-020.11199E-02 + 3088.0 135.35 0.85503E-020.10075E-02 + 3088.0 140.15 0.45162E-020.85443E-03 + 3088.0 145.07 0.69180E-020.14127E-02 + 3088.0 158.99 0.17349E-010.25337E-02 + 3088.0 160.03 0.19416E-010.22878E-02 + 3088.0 164.94 0.12977E-010.17097E-02 + 3088.0 168.88 0.12252E-010.11088E-02 + 3287.0 20.319 0.12843 0.46602E-01 + 3287.0 25.372 0.91343E-010.17281E-01 + 3287.0 28.353 0.11887 0.24275E-01 + 3287.0 30.434 0.61828E-010.10793E-01 + 3287.0 35.527 0.83710E-010.87125E-02 + 3287.0 38.600 0.63981E-010.22129E-01 + 3287.0 40.441 0.55267E-010.57522E-02 + 3287.0 42.557 0.56093E-010.81808E-02 + 3287.0 45.570 0.60629E-010.79879E-02 + 3287.0 50.628 0.42067E-010.67270E-02 + 3287.0 52.584 0.44855E-010.59096E-02 + 3287.0 55.614 0.43912E-010.45788E-02 + 3287.0 60.637 0.37140E-010.48932E-02 + 3287.0 80.675 0.45210E-020.17172E-02 + 3287.0 90.839 0.93792E-020.15017E-02 + 3287.0 95.824 0.99124E-020.26278E-02 + 3287.0 100.69 0.86995E-020.13929E-02 + 3287.0 105.59 0.63413E-020.74843E-03 + 3287.0 110.54 0.32686E-020.76613E-03 + 3287.0 120.46 0.49135E-020.92958E-03 + 3287.0 125.28 0.55234E-020.16406E-02 + 3287.0 140.24 0.64398E-020.84844E-03 + 3287.0 145.17 0.38508E-020.10824E-02 + 3287.0 150.26 0.54109E-020.26294E-02 + 3287.0 155.11 0.20977E-020.10194E-02 + 3287.0 159.04 0.53326E-020.93197E-03 + 3287.0 160.06 0.66715E-020.10682E-02 + 3287.0 165.09 0.22576E-020.89578E-03 + 3287.0 168.93 0.38616E-020.67408E-03 + 3694.0 28.202 0.67717E-010.31995E-01 + 3694.0 30.480 0.98546E-010.11830E-01 + 3694.0 40.535 0.82098E-01 + 3694.0 42.440 0.10967 0.97600E-02 + 3694.0 45.645 0.10768 0.95608E-02 + 3694.0 50.493 0.92175E-010.92783E-02 + 3694.0 52.695 0.91382E-010.10276E-01 + 3694.0 55.669 0.98732E-01 + 3694.0 60.583 0.69027E-010.69623E-02 + 3694.0 65.900 0.88640E-01 + 3694.0 70.887 0.49545E-010.49772E-02 + 3694.0 72.730 0.43207E-010.39587E-02 + 3694.0 75.742 0.41518E-010.45925E-02 + 3694.0 80.735 0.42157E-01 + 3694.0 82.778 0.36770E-010.30049E-02 + 3694.0 86.007 0.33506E-010.43400E-02 + 3694.0 90.866 0.27780E-010.25406E-02 + 3694.0 100.85 0.15434E-010.14115E-02 + 3694.0 110.80 0.17702E-010.17819E-02 + 3694.0 115.44 0.15643E-010.23084E-02 + 3694.0 120.76 0.20087E-01 + 3694.0 135.54 0.11329E-010.17778E-02 + 3694.0 150.25 0.78241E-020.58038E-02 + 3694.0 155.03 0.82888E-020.13007E-02 + 3694.0 159.00 0.92550E-020.14508E-02 + 3694.0 160.12 0.11839E-010.13313E-02 + 3694.0 164.82 0.86357E-020.11172E-02 + 3694.0 168.76 0.10170E-010.10280E-02 +ENDDATA 368 +ENDSUBENT 385 +SUBENT F0506010 20050427 20050831 F021 +BIB 4 8 +REACTION (42-MO-100(P,INL)42-MO-100,PAR,DA) +SAMPLE Target thickness was 590 mu-g/cm2, target homogeneity + was 0.7%/mm, isotopic enrichment was 93.8%. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bars results from + peak-integrating procedure and is related to statistics +STATUS (CURVE)Fig.3c,6,10 +ENDBIB 8 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.1 0.1 +ENDCOMMON 3 +DATA 4 231 +E-LVL ANG-CM DATA-CM DATA-ERR +KEV ADEG MB/SR MB/SR + 535.00 12.462 3.3770 0.27380 + 535.00 15.003 6.4115 0.32610 + 535.00 17.589 11.181 0.56866 + 535.00 20.208 13.677 0.39328 + 535.00 22.780 18.346 0.39423 + 535.00 25.351 18.400 + 535.00 30.478 19.041 + 535.00 35.613 8.1205 + 535.00 40.519 4.0183 + 535.00 45.543 3.7916 + 535.00 50.634 4.2118 + 535.00 55.735 3.4246 + 535.00 60.859 2.6686 + 535.00 65.913 1.7789 + 535.00 70.911 1.7639 + 535.00 75.946 1.6294 + 535.00 80.827 1.5156 + 535.00 85.515 1.1393 + 535.00 90.447 0.71749 + 535.00 95.545 0.58754 0.83871E-02 + 535.00 100.63 0.66196 + 535.00 105.42 0.72472 + 535.00 110.63 0.64624 + 535.00 115.51 0.45264 0.16408E-01 + 535.00 120.53 0.31934 + 535.00 125.57 0.29083 + 535.00 130.50 0.32762 + 535.00 135.47 0.34625 + 535.00 140.53 0.30653 + 535.00 145.40 0.28714 + 535.00 150.39 0.28878 + 535.00 155.16 0.33698 + 535.00 158.17 0.34541 + 535.00 165.29 0.34333 + 535.00 168.12 0.27647 + 694.00 20.012 0.25312 0.83629E-01 + 694.00 30.167 0.11131 0.17836E-01 + 694.00 45.290 0.12940E-010.33230E-02 + 694.00 50.478 0.43698E-010.52770E-02 + 694.00 55.583 0.52184E-010.49916E-02 + 694.00 75.743 0.20483E-010.38312E-02 + 694.00 80.668 0.28048E-010.19890E-02 + 694.00 85.669 0.26651E-010.28846E-02 + 694.00 90.637 0.29713E-010.21071E-02 + 694.00 95.416 0.19362E-010.20957E-02 + 694.00 100.55 0.19932E-010.16586E-02 + 694.00 105.45 0.15418E-010.14748E-02 + 694.00 110.36 0.10639E-010.10198E-02 + 694.00 120.44 0.13845E-010.11494E-02 + 694.00 125.56 0.15263E-010.10824E-02 + 694.00 130.37 0.17407E-010.12344E-02 + 694.00 135.24 0.15267E-010.89995E-03 + 694.00 140.27 0.12649E-010.89945E-03 + 694.00 145.29 0.54030E-020.44961E-03 + 694.00 150.19 0.20352E-020.32612E-03 + 694.00 155.04 0.37932E-020.55706E-03 + 694.00 165.03 0.15291E-010.89842E-03 + 694.00 167.84 0.20648E-010.14642E-02 + 1063.0 15.124 0.71631 0.11469 + 1063.0 19.940 0.79868 0.86656E-01 + 1063.0 22.475 0.94020 0.72261E-01 + 1063.0 25.164 1.0944 + 1063.0 30.181 0.97120 + 1063.0 35.337 0.91268 + 1063.0 40.408 0.62991 + 1063.0 45.425 0.55899 + 1063.0 50.478 0.21053 + 1063.0 55.557 0.14041 + 1063.0 60.526 0.15481 + 1063.0 65.640 0.17666 + 1063.0 70.778 0.17984 + 1063.0 75.703 0.12129 + 1063.0 80.703 0.11660 + 1063.0 85.710 0.53941E-01 + 1063.0 90.581 0.46777E-01 + 1063.0 95.496 0.33025E-01 + 1063.0 100.43 0.42725E-01 + 1063.0 105.48 0.64875E-01 + 1063.0 110.48 0.63080E-01 + 1063.0 115.40 0.43528E-01 + 1063.0 120.48 0.28701E-01 + 1063.0 125.40 0.20263E-01 + 1063.0 130.44 0.15677E-01 + 1063.0 135.53 0.20286E-01 + 1063.0 140.48 0.24788E-01 + 1063.0 145.26 0.32064E-010.30686E-02 + 1063.0 150.49 0.42945E-01 + 1063.0 155.28 0.54295E-010.45203E-02 + 1063.0 158.15 0.53870E-010.58337E-02 + 1063.0 165.10 0.57533E-01 + 1063.0 167.89 0.40511E-01 + 1135.0 15.080 0.66914 0.11589 + 1135.0 20.055 0.36751 0.63736E-01 + 1135.0 22.535 0.28025 0.52381E-01 + 1135.0 25.080 0.31521 0.30163E-01 + 1135.0 30.272 0.25248 0.24107E-01 + 1135.0 35.254 0.26296 0.21891E-01 + 1135.0 40.302 0.20350 0.14437E-01 + 1135.0 50.419 0.21828 0.15486E-01 + 1135.0 60.650 0.14164 0.10019E-01 + 1135.0 65.608 0.16349 0.11598E-01 + 1135.0 70.644 0.13396 0.78739E-02 + 1135.0 75.749 0.80630E-010.57202E-02 + 1135.0 80.754 0.75772E-010.53755E-02 + 1135.0 85.771 0.67253E-010.39393E-02 + 1135.0 90.689 0.93197E-010.66117E-02 + 1135.0 95.445 0.68875E-010.57481E-02 + 1135.0 100.59 0.67765E-010.56412E-02 + 1135.0 105.46 0.60135E-010.42787E-02 + 1135.0 110.47 0.53987E-010.38301E-02 + 1135.0 115.37 0.42252E-010.29975E-02 + 1135.0 120.40 0.35420E-010.25128E-02 + 1135.0 125.36 0.39507E-010.28110E-02 + 1135.0 130.35 0.41147E-010.49793E-02 + 1135.0 135.31 0.45373E-010.26670E-02 + 1135.0 140.30 0.46720E-010.33145E-02 + 1135.0 145.32 0.40531E-010.33656E-02 + 1135.0 150.18 0.38081E-010.17009E-02 + 1135.0 155.21 0.31203E-010.22071E-02 + 1135.0 157.97 0.26991E-010.19204E-02 + 1908.0 17.534 2.2765 0.31048 + 1908.0 20.127 2.1878 0.16105 + 1908.0 22.608 2.6204 + 1908.0 25.205 3.3702 + 1908.0 30.351 4.5362 + 1908.0 35.411 5.3719 + 1908.0 40.596 4.9614 + 1908.0 45.436 3.7009 + 1908.0 50.650 2.3959 + 1908.0 55.698 1.5955 + 1908.0 60.743 1.4423 + 1908.0 65.878 1.4713 + 1908.0 71.049 1.3981 + 1908.0 76.130 1.5866 + 1908.0 80.717 1.0711 + 1908.0 85.618 0.95442 + 1908.0 90.627 0.68723 + 1908.0 95.484 0.49476 + 1908.0 100.44 0.39630 + 1908.0 105.38 0.32891 + 1908.0 110.68 0.32619 + 1908.0 115.52 0.32333 + 1908.0 120.55 0.30070 + 1908.0 125.48 0.25495 + 1908.0 130.43 0.20421 + 1908.0 135.50 0.13032 + 1908.0 140.52 0.93171E-01 + 1908.0 145.42 0.83020E-01 + 1908.0 150.34 0.95545E-01 + 1908.0 155.31 0.13610 + 1908.0 158.33 0.13753 + 1908.0 165.13 0.18678 + 1908.0 168.07 0.16489 + 2202.0 20.268 0.38297 0.12442 + 2202.0 22.947 0.21458 0.52755E-01 + 2202.0 30.442 0.12957 0.26049E-01 + 2202.0 35.653 0.11356 0.13194E-01 + 2202.0 40.665 0.11105 0.11344E-01 + 2202.0 45.756 0.90411E-010.80263E-02 + 2202.0 50.755 0.64329E-010.66326E-02 + 2202.0 55.722 0.49251E-010.64213E-02 + 2202.0 60.876 0.24592E-010.49565E-02 + 2202.0 65.974 0.27854E-010.43962E-02 + 2202.0 71.018 0.25313E-010.32879E-02 + 2202.0 85.799 0.10552E-010.22827E-02 + 2202.0 100.72 0.63511E-020.12801E-02 + 2202.0 110.78 0.39588E-020.85429E-03 + 2202.0 135.57 0.45720E-020.65734E-03 + 2202.0 155.37 0.73307E-020.85167E-03 + 2202.0 158.16 0.31783E-020.63894E-03 + 2371.0 20.111 0.41553E-010.12792E-01 + 2371.0 35.396 0.30811E-01 + 2371.0 40.600 0.38952E-01 + 2371.0 45.491 0.35379E-01 + 2371.0 50.754 0.27445E-01 + 2371.0 65.848 0.11044E-01 + 2371.0 75.866 0.10686E-01 + 2371.0 80.939 0.12860E-01 + 2371.0 90.575 0.10476E-01 + 2371.0 95.651 0.62085E-02 + 2371.0 100.58 0.36778E-02 + 2371.0 110.69 0.28224E-02 + 2371.0 115.84 0.40311E-02 + 2371.0 120.34 0.45566E-02 + 2371.0 125.42 0.38015E-02 + 2371.0 130.43 0.26081E-02 + 2371.0 135.26 0.27091E-02 + 2371.0 145.23 0.14583E-02 + 2371.0 150.16 0.17120E-02 + 2371.0 155.10 0.27951E-02 + 2371.0 165.15 0.35820E-02 + 2371.0 167.97 0.40795E-02 + 2658.0 30.238 0.82765E-010.22910E-01 + 2658.0 50.443 0.37288E-010.43442E-02 + 2658.0 60.686 0.30441E-010.52458E-02 + 2658.0 65.566 0.20131E-010.37587E-02 + 2658.0 80.573 0.20008E-010.31636E-02 + 2658.0 85.699 0.75501E-020.24449E-02 + 2658.0 95.520 0.16155E-010.23196E-02 + 2658.0 100.47 0.18066E-010.20961E-02 + 2658.0 115.52 0.11570E-010.19879E-02 + 2658.0 120.30 0.95295E-020.12408E-02 + 2658.0 130.27 0.74029E-020.85891E-03 + 2658.0 135.34 0.44424E-020.76330E-03 + 2658.0 140.26 0.76165E-020.67884E-03 + 2658.0 145.13 0.71773E-020.63970E-03 + 2658.0 150.18 0.91826E-020.70144E-03 + 2658.0 155.13 0.10269E-010.10525E-02 + 2658.0 165.06 0.86881E-020.89047E-03 + 2658.0 167.98 0.78489E-020.80446E-03 + 3050.0 22.543 0.22812 0.59513E-01 + 3050.0 30.186 0.13783 0.31768E-01 + 3050.0 35.363 0.18520 + 3050.0 40.322 0.20455 + 3050.0 55.559 0.16924 + 3050.0 60.691 0.12497 + 3050.0 65.676 0.12986 + 3050.0 80.764 0.52882E-01 + 3050.0 85.594 0.27377E-010.39455E-02 + 3050.0 90.542 0.30985E-010.31913E-02 + 3050.0 95.621 0.36837E-01 + 3050.0 105.62 0.25940E-010.26717E-02 + 3050.0 110.49 0.24738E-01 + 3050.0 115.62 0.18491E-01 + 3050.0 130.31 0.13355E-010.12419E-02 + 3050.0 135.34 0.87253E-020.91068E-03 + 3050.0 145.30 0.68574E-020.17890E-02 + 3050.0 150.23 0.11333E-01 + 3050.0 155.19 0.12671E-010.14554E-02 + 3050.0 158.13 0.10900E-010.14144E-02 + 3050.0 165.02 0.13346E-010.10925E-02 +ENDDATA 233 +ENDSUBENT 250 +ENDENTRY 10 diff --git a/exforall/F05/F0534.x4 b/exforall/F05/F0534.x4 new file mode 100644 index 000000000..50838f8a1 --- /dev/null +++ b/exforall/F05/F0534.x4 @@ -0,0 +1,1690 @@ +ENTRY F0534 20050511 20050831 F021 +SUBENT F0534001 20050511 20050831 F021 +BIB 11 26 +TITLE The 13C(p,a)10B reaction in the energy range between + 18 and 45 MeV. +AUTHOR (S.Abd El-Kariem,T.Rohwer,G.Staudt,W.Leitner) +INSTITUTE (2GERTUE) +REFERENCE (J,NP/A,487,353,1988) +FACILITY (ISOCY,2GERJUL) For momentum-analyzed proton beam with + energies of 22.5, 27.0, 31.0, 36.0, 41.0 and 45.0 MeV. + (CYCLO,2GERHAM)For proton beam with energies of 18.0 + and 22.5 MeV. +DETECTOR (TELES,SIBAR)Four detector telescopes,each employing a + 50 mu-m dE and a 1000 mu-m E silicon surface-barrier + detector,mounted in a 110cm diameter scattering chamber + (GELI)To provide a relative normalization between the + different measurements,elastic-scattering events were + recorded with a Ge(Li)detector in Julich. + (CSICR) CsI scintillation counter was used in Hamburg. +SAMPLE The targets consisted of enriched (82% 13C) carbon foil + with areal densities of 100 mu-g/cm2 typically. +METHOD (BCINT) + (EDE) +REL-REF (A,,D.L.Olberg+,J,PR/C,11,410,1975) + (A,,S.Micheletti+,J,PR/C,11,64,1975) +ERR-ANALYS (DATA-ERR)The resulting overall normalization + uncertainty in the cross sections. + (ERR-DIG)Digitizing error +HISTORY (20050201C) +ENDBIB 26 +COMMON 1 3 +DATA-ERR +PER-CENT + 20. +ENDCOMMON 3 +ENDSUBENT 33 +SUBENT F0534002 20050511 20050831 F021 +BIB 3 4 +REACTION (6-C-13(P,A)5-B-10,PAR,DA) +ERR-ANALYS (ANG-ERR-D)Digitizing error + (DATA-ERR1)Error from the graphic bars +STATUS (CURVE)Fig.3 +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.21 0.2 +ENDCOMMON 3 +DATA 5 347 +E-LVL EN ANG-CM DATA-CM DATA-ERR1 +MEV MEV ADEG MU-B/SR MU-B/SR + 0.0000 18.000 21.600 1190.1 + 0.0000 18.000 27.837 1369.3 + 0.0000 18.000 33.393 1416.2 + 0.0000 18.000 38.728 1338.3 59.491 + 0.0000 18.000 42.915 1165.0 + 0.0000 18.000 48.459 1329.4 + 0.0000 18.000 52.626 1363.4 48.461 + 0.0000 18.000 57.711 1493.2 31.042 + 0.0000 18.000 61.868 1662.2 + 0.0000 18.000 66.725 1761.7 + 0.0000 18.000 74.825 1883.4 57.728 + 0.0000 18.000 79.472 1694.3 29.864 + 0.0000 18.000 83.658 1487.0 + 0.0000 18.000 87.837 1382.1 + 0.0000 18.000 91.824 933.13 + 0.0000 18.000 96.931 853.35 + 0.0000 18.000 108.27 943.21 + 0.0000 18.000 114.70 1446.0 + 0.0000 18.000 118.38 1911.8 + 0.0000 18.000 123.22 2181.4 + 0.0000 18.000 128.99 2614.8 + 0.0000 18.000 133.18 2313.7 + 0.0000 18.000 137.80 2575.8 + 0.0000 18.000 146.39 2262.2 + 0.0000 18.000 153.78 2734.6 + 0.0000 18.000 158.40 2922.1 + 0.0000 18.000 162.08 3708.3 + 0.0000 18.000 166.93 3995.2 + 0.0000 18.000 170.85 4748.6 + 0.0000 22.500 8.7319 1643.5 + 0.0000 22.500 15.697 1448.4 + 0.0000 22.500 21.067 1021.3 + 0.0000 22.500 25.455 1142.3 + 0.0000 22.500 27.113 844.42 + 0.0000 22.500 33.384 738.22 30.815 + 0.0000 22.500 39.636 756.72 + 0.0000 22.500 45.700 537.88 + 0.0000 22.500 51.449 764.04 + 0.0000 22.500 57.673 994.40 32.373 + 0.0000 22.500 62.084 918.90 + 0.0000 22.500 68.089 1069.8 + 0.0000 22.500 73.871 1159.4 + 0.0000 22.500 84.819 697.73 + 0.0000 22.500 89.947 536.96 + 0.0000 22.500 95.300 436.93 + 0.0000 22.500 100.68 277.80 + 0.0000 22.500 106.00 293.93 + 0.0000 22.500 110.61 356.03 + 0.0000 22.500 115.47 370.73 + 0.0000 22.500 118.47 438.36 + 0.0000 22.500 120.08 449.05 + 0.0000 22.500 125.18 445.81 + 0.0000 22.500 130.03 498.70 + 0.0000 22.500 134.68 442.87 + 0.0000 22.500 138.64 371.95 + 0.0000 22.500 143.26 399.83 + 0.0000 22.500 147.20 419.62 + 0.0000 22.500 151.59 440.41 + 0.0000 22.500 155.98 504.53 + 0.0000 22.500 164.05 656.82 + 0.0000 22.500 168.91 706.07 + 0.0000 22.500 172.84 741.02 +0.72000 18.000 20.869 187.61 +0.72000 18.000 27.795 232.49 +0.72000 18.000 32.854 328.49 +0.72000 18.000 37.949 334.16 +0.72000 18.000 40.016 390.71 +0.72000 18.000 43.047 328.95 +0.72000 18.000 47.190 417.66 +0.72000 18.000 52.529 378.74 +0.72000 18.000 56.729 288.99 +0.72000 18.000 61.605 262.05 +0.72000 18.000 66.003 270.96 +0.72000 18.000 70.625 299.22 +0.72000 18.000 75.482 319.76 +0.72000 18.000 79.174 367.86 +0.72000 18.000 83.584 339.06 +0.72000 18.000 88.227 309.97 +0.72000 18.000 92.185 258.87 +0.72000 18.000 97.052 254.83 +0.72000 18.000 108.24 133.39 +0.72000 18.000 115.16 175.09 +0.72000 18.000 115.89 136.87 +0.72000 18.000 120.24 208.20 15.972 +0.72000 18.000 124.39 253.70 +0.72000 18.000 129.91 344.06 +0.72000 18.000 134.32 319.74 +0.72000 18.000 138.71 358.92 +0.72000 18.000 147.05 356.40 27.342 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7.0000 27.000 42.795 100.09 11.042 + 7.0000 27.000 49.089 120.55 12.226 + 7.0000 27.000 54.977 85.343 11.732 + 7.0000 27.000 60.678 39.752 11.680 + 7.0000 27.000 66.242 61.941 10.821 + 7.0000 27.000 71.883 48.688 10.855 + 7.0000 27.000 77.085 30.058 10.756 + 7.0000 27.000 83.121 44.630 10.391 + 7.0000 27.000 88.513 40.225 11.819 + 7.0000 27.000 93.408 46.904 10.457 + 7.0000 27.000 98.703 99.236 12.737 + 7.0000 27.000 103.65 73.131 16.304 + 7.0000 27.000 108.81 64.338 11.239 +ENDDATA 349 +ENDSUBENT 362 +SUBENT F0534003 20050511 20050831 F021 +BIB 3 3 +REACTION (6-C-13(P,A)5-B-10,PAR,DA) +ERR-ANALYS (ANG-ERR-D)Digitizing error +STATUS (CURVE)Fig.3 +ENDBIB 3 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.21 0.2 +ENDCOMMON 3 +DATA 5 64 +E-LVL-MIN E-LVL-MAX EN ANG-CM DATA-CM +MEV MEV MEV ADEG MU-B/SR + 5.1600 5.1800 18.000 27.181 943.62 + 5.1600 5.1800 18.000 33.706 1179.6 + 5.1600 5.1800 18.000 37.895 1450.1 + 5.1600 5.1800 18.000 39.554 1190.3 + 5.1600 5.1800 18.000 45.394 1282.9 + 5.1600 5.1800 18.000 48.448 1134.3 + 5.1600 5.1800 18.000 53.575 1349.3 + 5.1600 5.1800 18.000 59.423 1350.4 + 5.1600 5.1800 18.000 64.578 1244.5 + 5.1600 5.1800 18.000 69.028 1185.2 + 5.1600 5.1800 18.000 73.480 1101.2 + 5.1600 5.1800 18.000 77.932 1031.6 + 5.1600 5.1800 18.000 82.146 998.70 + 5.1600 5.1800 18.000 86.590 1007.6 + 5.1600 5.1800 18.000 90.569 983.48 + 5.1600 5.1800 18.000 94.077 992.08 + 5.1600 5.1800 18.000 98.293 937.03 + 5.1600 5.1800 18.000 103.42 1133.2 + 5.1600 5.1800 18.000 121.65 1264.3 + 5.1600 5.1800 18.000 126.57 1174.8 + 5.1600 5.1800 18.000 130.29 1444.1 + 5.1600 5.1800 18.000 135.20 1569.1 + 5.1600 5.1800 18.000 139.66 1299.1 + 5.1600 5.1800 22.500 13.546 200.26 + 5.1600 5.1800 22.500 20.268 356.74 + 5.1600 5.1800 22.500 26.550 488.23 + 5.1600 5.1800 22.500 32.842 610.32 + 5.1600 5.1800 22.500 39.144 691.15 + 5.1600 5.1800 22.500 44.753 726.70 + 5.1600 5.1800 22.500 57.174 582.78 + 5.1600 5.1800 22.500 62.802 515.44 + 5.1600 5.1800 22.500 68.922 362.02 + 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5.1600 5.1800 36.000 98.744 55.382 + 5.1600 5.1800 36.000 103.40 30.785 + 5.1600 5.1800 36.000 108.01 39.681 + 5.1600 5.1800 36.000 112.58 29.607 + 5.1600 5.1800 36.000 117.46 30.929 + 5.1600 5.1800 36.000 122.81 29.500 + 5.1600 5.1800 36.000 131.48 35.749 + 5.1600 5.1800 36.000 149.01 30.819 + 5.1600 5.1800 36.000 156.42 35.794 + 5.1600 5.1800 36.000 163.56 24.920 + 5.1600 5.1800 41.000 14.511 244.88 + 5.1600 5.1800 41.000 19.825 255.99 + 5.1600 5.1800 41.000 25.790 258.34 + 5.1600 5.1800 41.000 31.805 221.52 + 5.1600 5.1800 41.000 37.952 125.06 + 5.1600 5.1800 41.000 41.362 125.21 + 5.1600 5.1800 41.000 43.404 84.267 + 5.1600 5.1800 41.000 50.878 80.398 + 5.1600 5.1800 41.000 60.630 48.097 + 5.1600 5.1800 41.000 66.823 46.195 + 5.1600 5.1800 41.000 73.684 40.473 + 5.1600 5.1800 41.000 80.417 27.090 + 5.1600 5.1800 41.000 86.444 22.421 + 5.1600 5.1800 41.000 93.714 20.792 + 5.1600 5.1800 41.000 103.27 22.874 + 5.1600 5.1800 41.000 116.59 16.356 + 5.1600 5.1800 41.000 121.84 10.788 + 5.1600 5.1800 41.000 141.04 19.692 + 5.1600 5.1800 41.000 148.13 16.419 + 5.1600 5.1800 41.000 155.76 18.702 + 5.1600 5.1800 41.000 160.01 19.682 + 5.1600 5.1800 45.000 18.851 235.15 + 5.1600 5.1800 45.000 23.511 130.47 + 5.1600 5.1800 45.000 30.076 148.88 + 5.1600 5.1800 45.000 36.373 102.59 + 5.1600 5.1800 45.000 43.168 56.147 + 5.1600 5.1800 45.000 48.366 43.089 + 5.1600 5.1800 45.000 54.817 35.811 + 5.1600 5.1800 45.000 60.781 36.147 + 5.1600 5.1800 45.000 65.539 28.961 + 5.1600 5.1800 45.000 72.832 24.959 + 5.1600 5.1800 45.000 79.198 13.757 + 5.1600 5.1800 45.000 85.679 10.411 1.4835 + 5.1600 5.1800 45.000 93.368 9.8550 0.74932 + 5.1600 5.1800 45.000 126.78 11.602 + 5.1600 5.1800 45.000 135.14 9.9313 0.83181 + 5.1600 5.1800 45.000 148.09 11.359 1.0042 + 5.1600 5.1800 45.000 151.78 18.698 + 5.1600 5.1800 45.000 163.39 26.725 + 5.1600 5.1800 45.000 167.67 6.3358 2.6932 + 5.9200 6.0300 27.000 14.465 592.00 + 5.9200 6.0300 27.000 20.638 734.49 + 5.9200 6.0300 27.000 26.580 582.92 + 5.9200 6.0300 27.000 32.407 609.96 + 5.9200 6.0300 27.000 39.327 566.08 + 5.9200 6.0300 27.000 44.492 644.73 + 5.9200 6.0300 27.000 50.748 655.91 + 5.9200 6.0300 27.000 56.460 546.99 + 5.9200 6.0300 27.000 62.373 466.01 + 5.9200 6.0300 27.000 68.667 432.35 + 5.9200 6.0300 27.000 73.509 392.41 + 5.9200 6.0300 27.000 80.030 348.94 + 5.9200 6.0300 27.000 84.504 464.36 + 5.9200 6.0300 27.000 90.148 455.82 + 5.9200 6.0300 27.000 95.572 460.26 + 5.9200 6.0300 27.000 100.31 535.38 + 5.9200 6.0300 27.000 105.42 421.73 + 5.9200 6.0300 27.000 109.71 322.79 + 5.9200 6.0300 27.000 119.84 249.52 + 5.9200 6.0300 27.000 120.63 275.66 + 5.9200 6.0300 27.000 129.51 349.82 + 5.9200 6.0300 27.000 133.67 358.06 + 5.9200 6.0300 27.000 138.12 511.49 + 5.9200 6.0300 27.000 142.76 454.43 + 5.9200 6.0300 27.000 146.21 579.26 + 5.9200 6.0300 27.000 166.96 469.63 + 5.9200 6.0300 31.000 17.618 448.50 + 5.9200 6.0300 31.000 24.306 440.53 + 5.9200 6.0300 31.000 30.776 441.83 + 5.9200 6.0300 31.000 38.957 402.10 + 5.9200 6.0300 31.000 48.959 421.26 + 5.9200 6.0300 31.000 54.718 186.25 + 5.9200 6.0300 31.000 60.511 211.81 + 5.9200 6.0300 31.000 66.462 273.24 + 5.9200 6.0300 31.000 72.906 175.11 + 5.9200 6.0300 31.000 79.100 207.72 + 5.9200 6.0300 31.000 83.271 209.58 + 5.9200 6.0300 31.000 112.73 119.66 + 5.9200 6.0300 31.000 117.68 82.767 + 5.9200 6.0300 31.000 122.02 91.468 + 5.9200 6.0300 31.000 130.82 140.74 + 5.9200 6.0300 31.000 136.29 127.92 + 5.9200 6.0300 31.000 138.89 170.64 + 5.9200 6.0300 31.000 144.52 171.08 + 5.9200 6.0300 31.000 151.92 230.31 + 5.9200 6.0300 31.000 156.50 235.69 + 5.9200 6.0300 31.000 159.96 174.72 + 5.9200 6.0300 36.000 13.096 534.29 + 5.9200 6.0300 36.000 25.775 365.89 + 5.9200 6.0300 36.000 37.328 306.70 + 5.9200 6.0300 36.000 43.579 316.29 + 5.9200 6.0300 36.000 49.237 299.86 + 5.9200 6.0300 36.000 54.923 265.10 + 5.9200 6.0300 36.000 60.652 211.05 + 5.9200 6.0300 36.000 66.978 180.23 + 5.9200 6.0300 36.000 72.885 154.96 + 5.9200 6.0300 36.000 77.581 119.91 + 5.9200 6.0300 36.000 83.572 83.605 + 5.9200 6.0300 36.000 89.207 83.818 + 5.9200 6.0300 36.000 99.139 104.56 + 5.9200 6.0300 36.000 108.79 92.604 + 5.9200 6.0300 36.000 113.43 81.831 + 5.9200 6.0300 36.000 117.95 98.334 + 5.9200 6.0300 36.000 123.16 101.36 + 5.9200 6.0300 36.000 131.73 98.948 + 5.9200 6.0300 36.000 140.73 55.241 + 5.9200 6.0300 36.000 149.27 58.642 + 5.9200 6.0300 36.000 154.07 58.769 + 5.9200 6.0300 36.000 157.59 63.566 + 5.9200 6.0300 36.000 165.11 62.897 + 5.9200 6.0300 41.000 11.826 383.69 + 5.9200 6.0300 41.000 17.916 350.97 + 5.9200 6.0300 41.000 24.212 323.35 + 5.9200 6.0300 41.000 30.536 277.56 + 5.9200 6.0300 41.000 36.438 241.61 + 5.9200 6.0300 41.000 42.923 233.91 + 5.9200 6.0300 41.000 48.415 199.30 + 5.9200 6.0300 41.000 53.933 159.33 + 5.9200 6.0300 41.000 59.471 121.23 + 5.9200 6.0300 41.000 65.192 98.313 + 5.9200 6.0300 41.000 72.146 83.821 + 5.9200 6.0300 41.000 78.899 69.958 + 5.9200 6.0300 41.000 85.240 57.557 + 5.9200 6.0300 41.000 93.029 49.092 + 5.9200 6.0300 41.000 102.67 44.979 + 5.9200 6.0300 41.000 114.74 49.238 + 5.9200 6.0300 41.000 120.63 44.089 + 5.9200 6.0300 41.000 125.84 45.143 + 5.9200 6.0300 41.000 130.23 44.916 + 5.9200 6.0300 41.000 139.72 35.220 + 5.9200 6.0300 41.000 142.96 26.581 + 5.9200 6.0300 41.000 147.99 25.535 + 5.9200 6.0300 41.000 151.63 33.943 + 5.9200 6.0300 41.000 156.26 31.027 + 5.9200 6.0300 41.000 159.88 43.644 + 5.9200 6.0300 45.000 17.666 274.19 + 5.9200 6.0300 45.000 23.742 259.60 + 5.9200 6.0300 45.000 30.656 244.12 + 5.9200 6.0300 45.000 35.726 210.39 + 5.9200 6.0300 45.000 41.611 190.76 + 5.9200 6.0300 45.000 47.370 140.39 + 5.9200 6.0300 45.000 53.132 102.57 + 5.9200 6.0300 45.000 58.669 78.239 + 5.9200 6.0300 45.000 64.506 47.412 + 5.9200 6.0300 45.000 71.394 47.568 + 5.9200 6.0300 45.000 77.768 36.038 + 5.9200 6.0300 45.000 84.610 40.567 + 5.9200 6.0300 45.000 91.244 27.004 + 5.9200 6.0300 45.000 100.74 20.786 + 5.9200 6.0300 45.000 113.69 35.109 + 5.9200 6.0300 45.000 119.36 32.292 + 5.9200 6.0300 45.000 124.96 35.298 + 5.9200 6.0300 45.000 129.48 24.685 + 5.9200 6.0300 45.000 133.52 20.661 + 5.9200 6.0300 45.000 138.46 14.768 + 5.9200 6.0300 45.000 142.77 10.476 1.2854 + 5.9200 6.0300 45.000 147.05 13.700 1.0385 + 5.9200 6.0300 45.000 150.95 26.992 + 5.9200 6.0300 45.000 162.27 69.150 + 5.9200 6.0300 45.000 167.75 60.908 + 7.4800 7.5600 27.000 13.590 214.48 1.6935 + 7.4800 7.5600 27.000 19.115 336.31 + 7.4800 7.5600 27.000 25.580 272.74 + 7.4800 7.5600 27.000 37.194 311.74 + 7.4800 7.5600 27.000 43.549 321.77 + 7.4800 7.5600 27.000 49.191 390.84 + 7.4800 7.5600 27.000 55.695 291.09 + 7.4800 7.5600 27.000 61.167 203.28 + 7.4800 7.5600 27.000 66.235 215.71 + 7.4800 7.5600 27.000 72.645 197.35 + 7.4800 7.5600 27.000 78.891 162.31 + 7.4800 7.5600 27.000 83.668 204.18 + 7.4800 7.5600 27.000 88.896 153.05 1.5931 + 7.4800 7.5600 27.000 93.980 156.75 1.3726 + 7.4800 7.5600 27.000 98.822 171.11 1.7392 + 7.4800 7.5600 27.000 104.20 91.897 2.5826 + 7.4800 7.5600 31.000 19.025 374.19 + 7.4800 7.5600 31.000 25.408 362.45 + 7.4800 7.5600 31.000 30.815 290.50 + 7.4800 7.5600 31.000 37.819 182.39 + 7.4800 7.5600 31.000 49.203 135.75 + 7.4800 7.5600 31.000 54.651 62.158 + 7.4800 7.5600 31.000 60.845 91.619 + 7.4800 7.5600 31.000 66.490 110.98 + 7.4800 7.5600 31.000 73.271 71.151 + 7.4800 7.5600 31.000 83.405 80.539 + 7.4800 7.5600 31.000 88.176 103.13 + 7.4800 7.5600 31.000 93.694 40.486 + 7.4800 7.5600 31.000 116.54 48.094 + 7.4800 7.5600 31.000 121.49 41.621 + 7.4800 7.5500 41.000 19.500 194.60 + 7.4800 7.5500 41.000 26.275 202.36 + 7.4800 7.5500 41.000 36.163 94.676 + 7.4800 7.5500 41.000 42.545 56.780 + 7.4800 7.5500 41.000 55.042 60.497 + 7.4800 7.5500 41.000 60.886 46.912 + 7.4800 7.5500 41.000 66.726 36.639 + 7.4800 7.5500 41.000 73.277 39.200 + 7.4800 7.5500 41.000 80.223 27.717 + 7.4800 7.5500 41.000 86.036 23.084 + 7.4800 7.5500 41.000 93.166 17.408 1.1843 + 7.4800 7.5500 41.000 103.48 13.242 1.8371 + 7.4800 7.5500 41.000 115.40 19.875 + 7.4800 7.5500 41.000 120.48 20.503 + 7.4800 7.5500 41.000 125.95 22.723 + 7.4800 7.5500 41.000 130.57 25.717 1.7946 + 7.4800 7.5500 41.000 140.26 11.691 2.1895 + 7.4800 7.5500 41.000 149.33 13.261 2.3164 + 7.4800 7.5500 41.000 153.61 19.687 + 7.4800 7.5500 41.000 157.50 27.402 +ENDDATA 289 +ENDSUBENT 302 +SUBENT F0534006 20050511 20050831 F021 +BIB 3 3 +REACTION (6-C-13(P,A)5-B-10,PAR,IPA) +ERR-ANALYS (EN-ERR-DIG)Digitizing error +STATUS (CURVE)Fig.5 +ENDBIB 3 +COMMON 4 3 +EN-ERR-DIG ERR-DIG ANG-CM-MIN ANG-CM-MAX +MEV PER-CENT ADEG ADEG + 0.1 0.23 0. 90. +ENDCOMMON 3 +DATA 3 41 +E-LVL EN DATA-CM +MEV MEV MICRO-B + 0.0000 17.844 4470.8 + 0.0000 22.283 5487.3 + 0.0000 26.716 4240.6 + 0.0000 30.825 2827.7 + 0.0000 36.112 2358.7 + 0.0000 41.170 1540.6 + 0.0000 45.121 1236.2 +0.72000 17.770 1001.8 +0.72000 22.327 960.16 +0.72000 30.834 480.43 +0.72000 36.382 240.81 +0.72000 41.340 138.58 +0.72000 45.234 96.256 + 1.7400 17.672 1870.0 + 1.7400 22.284 1424.6 + 1.7400 26.649 1022.8 + 1.7400 30.829 599.15 + 1.7400 36.280 350.00 + 1.7400 41.220 236.82 + 1.7400 45.144 149.26 + 2.1500 17.647 1120.3 + 2.1500 22.253 833.59 + 2.1500 26.837 796.37 + 2.1500 30.832 529.46 + 2.1500 36.278 381.20 + 2.1500 41.188 212.37 + 2.1500 45.141 164.98 + 3.5900 17.673 1706.9 + 3.5900 22.228 1285.1 + 3.5900 26.980 569.32 + 3.5900 30.732 400.26 + 3.5900 36.361 160.87 + 3.5900 41.421 94.229 + 3.5900 45.125 76.278 + 4.7700 17.691 1223.8 + 4.7700 22.315 588.94 + 4.7700 26.849 396.33 + 4.7700 30.878 193.99 + 4.7700 36.465 98.679 + 4.7700 41.476 46.346 + 4.7700 45.377 38.753 +ENDDATA 43 +ENDSUBENT 55 +SUBENT F0534007 20050511 20050831 F021 +BIB 3 3 +REACTION (6-C-13(P,A)5-B-10,PAR,SIG) +ERR-ANALYS (EN-ERR-DIG)Digitizing error +STATUS (CURVE)Fig.5 +ENDBIB 3 +COMMON 2 3 +EN-ERR-DIG ERR-DIG +MEV PER-CENT + 0.1 0.22 +ENDCOMMON 3 +DATA 4 17 +E-LVL-MIN E-LVL-MAX EN DATA +MEV MEV MEV MICRO-B + 5.1600 5.1800 17.770 3491.1 + 5.1600 5.1800 22.217 2829.0 + 5.1600 5.1800 26.888 2135.5 + 5.1600 5.1800 30.813 1386.7 + 5.1600 5.1800 36.044 802.88 + 5.1600 5.1800 41.272 474.47 + 5.1600 5.1800 45.240 300.82 + 5.9200 6.0300 22.306 4209.9 + 5.9200 6.0300 26.790 3085.6 + 5.9200 6.0300 30.860 1839.7 + 5.9200 6.0300 36.092 1455.3 + 5.9200 6.0300 41.219 947.78 + 5.9200 6.0300 44.866 756.01 + 7.4800 7.5600 22.204 1755.8 + 7.4800 7.5600 26.645 1352.9 + 7.4800 7.5600 30.744 811.41 + 7.4800 7.5600 41.031 390.65 +ENDDATA 19 +ENDSUBENT 31 +ENDENTRY 7 diff --git a/exforall/F05/F0570.x4 b/exforall/F05/F0570.x4 new file mode 100644 index 000000000..728c80cf5 --- /dev/null +++ b/exforall/F05/F0570.x4 @@ -0,0 +1,1247 @@ +ENTRY F0570 20050527 20050831 F022 +SUBENT F0570001 20050527 20050831 F022 +BIB 8 18 +TITLE Energy spectra of particles with Z<=2 from the decay + of Ni60, Cu62 and Zn64 intermidiate systems. +AUTHOR (N.T.Burtebaev A.D.Dujsebaev,G.N.Ivanov, + V.I.Kanashevich,V.A.Lichman) +INSTITUTE (4KASKAZ) +REFERENCE (J,IZV,48,1006,1984) +FACILITY (ISOCY) +DETECTOR (SIBAR) + (CSICR) +ERR-ANALYS (E-ERR-DIG) Digitizing error + (ERR-DIG) Digitizing error + The accuracy of cross-section measurement was + determined by the errors of target thickness definition + (near 10%), integrator current calibration (near 3%), + solid angle of spectrometer (near 3%) and statistical + errors depending on the type and energy of particles + registered. +HISTORY (20030821C) +ENDBIB 18 +COMMON 1 3 +ERR-DIG +PER-CENT + 0.02 +ENDCOMMON 3 +ENDSUBENT 25 +SUBENT F0570002 20050527 20050831 F022 +BIB 4 5 +REACTION (26-FE-56(A,P)27-CO-59,,DA/DE) +SAMPLE Self-supported foils of Fe56(2.7 mg/cm2,99.7% enriched) +ERR-ANALYS Statistical errors are from 1% at the low + energy region to 10% at the high energy one. +STATUS (CURVE)Fig.1 +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 35.8 0.15 +ENDCOMMON 3 +DATA 3 116 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 30.000 4.6653 12.731 + 30.000 5.1932 12.464 + 30.000 5.5466 11.559 + 30.000 6.0175 10.605 + 30.000 6.4303 9.5217 + 30.000 6.7850 8.3657 + 30.000 7.1975 7.5927 + 30.000 7.4931 6.8163 + 30.000 7.9645 6.1202 + 30.000 8.4359 5.4952 + 30.000 8.8492 4.8283 + 30.000 9.2615 4.4298 + 30.000 9.6157 3.9770 + 30.000 10.088 3.4945 + 30.000 10.560 3.0049 + 30.000 11.090 2.7275 + 30.000 11.560 2.5296 + 30.000 12.149 2.2962 + 30.000 12.506 1.7913 + 30.000 13.151 1.7729 + 30.000 14.030 1.7742 + 30.000 14.388 1.3840 + 30.000 15.210 1.2840 + 30.000 15.622 1.2038 + 30.000 16.093 1.1045 + 30.000 16.797 1.0357 + 30.000 17.444 0.96072 + 30.000 17.855 0.92037 + 30.000 18.559 0.90119 + 30.000 19.146 0.85418 + 30.000 19.208 0.75030 + 30.000 19.328 0.66625 + 30.000 19.800 0.57912 + 30.000 20.563 0.55495 + 30.000 21.266 0.56741 + 30.000 21.677 0.53195 + 30.000 21.973 0.47756 + 30.000 22.152 0.41501 + 90.000 4.8146 8.6781 + 90.000 5.2281 7.7060 + 90.000 5.8764 6.7706 + 90.000 6.2900 6.0122 + 90.000 6.7621 5.3391 + 90.000 7.2935 4.6399 + 90.000 7.5315 4.0751 + 90.000 7.9451 3.6187 + 90.000 8.4178 3.1446 + 90.000 8.8323 2.7031 + 90.000 9.1298 2.2982 + 90.000 9.7775 2.0635 + 90.000 10.019 1.6262 + 90.000 10.375 1.3827 + 90.000 10.789 1.1758 + 90.000 11.146 0.97829 + 90.000 11.738 0.79672 + 90.000 12.270 0.67024 + 90.000 12.743 0.58879 + 90.000 13.335 0.47950 + 90.000 13.868 0.39048 + 90.000 14.400 0.33207 + 90.000 14.813 0.29170 + 90.000 15.345 0.25626 + 90.000 15.759 0.22028 + 90.000 16.583 0.19357 + 90.000 17.114 0.17191 + 90.000 17.878 0.15605 + 90.000 18.118 0.12843 + 90.000 18.998 0.12443 + 90.000 19.296 0.10352 + 90.000 19.945 0.90957E-01 + 90.000 20.416 0.83442E-01 + 90.000 20.655 0.70176E-01 + 90.000 21.241 0.70215E-01 + 90.000 21.596 0.62347E-01 + 90.000 22.069 0.53596E-01 + 90.000 22.425 0.46067E-01 + 90.000 22.786 0.32581E-01 + 90.000 23.603 0.37134E-01 + 120.00 4.7220 8.9329 + 120.00 5.3128 7.6940 + 120.00 5.8453 6.5559 + 120.00 6.2600 5.7064 + 120.00 6.9094 4.9153 + 120.00 7.3254 4.0989 + 120.00 7.7993 3.4924 + 120.00 8.2726 3.0401 + 120.00 8.8055 2.5628 + 120.00 9.4563 2.1149 + 120.00 9.9305 1.7828 + 120.00 10.115 1.3643 + 120.00 10.472 1.1499 + 120.00 10.886 1.0226 + 120.00 11.421 0.81709 + 120.00 11.777 0.69610 + 120.00 12.193 0.59306 + 120.00 12.788 0.43500 + 120.00 13.322 0.36281 + 120.00 13.795 0.31581 + 120.00 14.390 0.23666 + 120.00 14.865 0.19950 + 120.00 15.283 0.15601 + 120.00 15.755 0.13727 + 120.00 16.346 0.11950 + 120.00 16.878 0.10292 + 120.00 17.585 0.91552E-01 + 120.00 18.000 0.78000E-01 + 120.00 18.532 0.67901E-01 + 120.00 19.181 0.60397E-01 + 120.00 19.827 0.57288E-01 + 120.00 20.241 0.50401E-01 + 120.00 20.657 0.42941E-01 + 120.00 21.072 0.36978E-01 + 120.00 21.664 0.30189E-01 + 120.00 22.381 0.19685E-01 + 120.00 22.858 0.15069E-01 + 120.00 23.333 0.12567E-01 +ENDDATA 118 +ENDSUBENT 132 +SUBENT F0570003 20050527 20050831 F022 +BIB 4 5 +REACTION (26-FE-57(HE3,P)27-CO-59,,DA/DE) +SAMPLE Self-supported foils of Fe57(1.9mg/cm2, 99.5% enriched) +ERR-ANALYS Statistical errors are from 1% at the low + energy region to 10% at the high energy one. +STATUS (CURVE) Fig.1 +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 23. 0.15 +ENDCOMMON 3 +DATA 3 111 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 30.000 5.0383 14.108 + 30.000 5.6224 14.268 + 30.000 6.5002 13.677 + 30.000 7.2006 14.135 + 30.000 7.7298 12.560 + 30.000 8.4334 11.529 + 30.000 9.2507 11.917 + 30.000 9.7217 10.475 + 30.000 10.370 8.7256 + 30.000 10.951 9.7244 + 30.000 11.308 7.5906 + 30.000 12.070 7.1199 + 30.000 12.773 6.6064 + 30.000 12.954 5.3833 + 30.000 13.600 4.7326 + 30.000 14.073 3.8574 + 30.000 14.832 4.0302 + 30.000 15.012 3.3920 + 30.000 15.604 2.5093 + 30.000 16.365 2.4311 + 30.000 16.956 1.8777 + 30.000 17.489 1.4659 + 30.000 18.366 1.4204 + 30.000 18.546 1.1954 + 30.000 19.249 1.1457 + 30.000 19.722 0.91391 + 30.000 20.366 0.88533 + 30.000 20.899 0.67643 + 30.000 21.718 0.66967 + 30.000 22.367 0.52287 + 30.000 22.729 0.34718 + 90.000 4.9265 10.119 + 90.000 5.5113 10.015 + 90.000 6.0982 9.1873 + 90.000 6.6273 8.2461 + 90.000 7.2736 7.3223 + 90.000 7.8621 6.3618 + 90.000 8.3347 5.3496 + 90.000 8.8663 4.4020 + 90.000 9.5104 4.2175 + 90.000 10.041 3.6245 + 90.000 10.339 2.9177 + 90.000 11.103 2.5355 + 90.000 11.341 2.1783 + 90.000 11.990 1.7542 + 90.000 12.579 1.5076 + 90.000 13.109 1.3098 + 90.000 13.582 1.1134 + 90.000 14.053 0.97781 + 90.000 14.468 0.78723 + 90.000 14.999 0.66923 + 90.000 15.471 0.57510 + 90.000 15.943 0.48888 + 90.000 16.589 0.44364 + 90.000 17.119 0.37714 + 90.000 17.420 0.28137 + 90.000 18.182 0.25815 + 90.000 18.540 0.20336 + 90.000 18.838 0.16730 + 90.000 19.655 0.17487 + 90.000 20.185 0.14866 + 90.000 20.550 0.93223E-01 + 90.000 21.014 0.10510 + 90.000 21.487 0.84621E-01 + 90.000 22.186 0.93375E-01 + 90.000 22.663 0.68179E-01 + 90.000 22.912 0.40053E-01 + 90.000 23.611 0.43719E-01 + 90.000 24.200 0.36370E-01 + 90.000 24.380 0.31245E-01 + 90.000 25.198 0.31271E-01 + 90.000 25.568 0.15954E-01 + 120.00 5.5797 9.5424 + 120.00 6.1666 8.7655 + 120.00 6.7528 8.2257 + 120.00 7.2814 7.4753 + 120.00 7.7531 6.4396 + 120.00 8.3417 5.5480 + 120.00 8.6375 4.8817 + 120.00 9.1677 4.2056 + 120.00 9.8737 3.5471 + 120.00 10.171 2.9274 + 120.00 10.761 2.3909 + 120.00 11.116 2.0594 + 120.00 11.705 1.7554 + 120.00 12.236 1.4962 + 120.00 12.766 1.2617 + 120.00 13.123 1.0193 + 120.00 13.478 0.85944 + 120.00 14.126 0.72483 + 120.00 14.543 0.53763 + 120.00 15.016 0.44854 + 120.00 15.661 0.41204 + 120.00 16.191 0.35878 + 120.00 16.373 0.28368 + 120.00 17.139 0.22683 + 120.00 17.669 0.19541 + 120.00 18.084 0.15620 + 120.00 18.442 0.12352 + 120.00 19.145 0.11470 + 120.00 19.502 0.91676E-01 + 120.00 20.090 0.80689E-01 + 120.00 20.507 0.60493E-01 + 120.00 21.035 0.57374E-01 + 120.00 21.564 0.51038E-01 + 120.00 22.039 0.38676E-01 + 120.00 22.496 0.56842E-01 + 120.00 23.107 0.21512E-01 + 120.00 23.583 0.15957E-01 + 120.00 24.113 0.13747E-01 + 120.00 24.644 0.11593E-01 +ENDDATA 113 +ENDSUBENT 127 +SUBENT F0570004 20050527 20050831 F022 +BIB 4 5 +REACTION (27-CO-59(P,EL)27-CO-59,,DA/DE) +SAMPLE Self-supported foils of Co59(5.2 mg/cm2,99.8% enriched) +ERR-ANALYS Statistical errors are from 1% at the low + energy region to 10% at the high energy one. +STATUS (CURVE)Fig.1 +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 29.9 0.15 +ENDCOMMON 3 +DATA 3 137 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 30.000 5.0288 3.3872 + 30.000 5.4379 3.8570 + 30.000 5.9648 4.2063 + 30.000 6.7270 4.3463 + 30.000 7.3139 4.2544 + 30.000 8.0777 3.8611 + 30.000 8.9583 3.6593 + 30.000 9.6630 3.4305 + 30.000 10.720 3.2164 + 30.000 11.600 3.0483 + 30.000 11.953 2.7961 + 30.000 12.716 2.7669 + 30.000 13.420 2.6794 + 30.000 14.066 2.6801 + 30.000 14.770 2.5674 + 30.000 15.180 2.7998 + 30.000 15.884 2.7705 + 30.000 16.646 2.9570 + 30.000 17.116 2.7421 + 30.000 17.584 2.9903 + 30.000 18.113 2.6556 + 30.000 18.640 2.8650 + 30.000 19.227 2.7742 + 30.000 19.698 2.4372 + 30.000 20.286 2.2358 + 30.000 20.578 2.4913 + 30.000 20.987 2.8677 + 30.000 21.515 2.9310 + 30.000 22.160 2.9318 + 30.000 22.687 3.1973 + 30.000 23.391 3.1638 + 30.000 24.154 2.9983 + 30.000 24.740 3.2699 + 30.000 25.148 3.8462 + 30.000 25.912 3.5286 + 30.000 26.207 2.9685 + 30.000 26.913 2.5249 + 30.000 27.322 3.0348 + 30.000 27.730 3.8502 + 30.000 28.251 6.9039 + 30.000 28.832 10.302 + 30.000 29.005 13.068 + 30.000 29.827 12.793 + 30.000 30.420 7.2938 + 90.000 4.5820 2.2451 + 90.000 5.0478 2.5040 + 90.000 5.5140 2.7625 + 90.000 6.0392 3.0149 + 90.000 6.6872 2.7660 + 90.000 7.1589 2.5648 + 90.000 7.8063 2.4047 + 90.000 8.4553 2.1354 + 90.000 8.9860 1.9589 + 90.000 9.5764 1.7394 + 90.000 10.166 1.5785 + 90.000 10.757 1.3865 + 90.000 11.347 1.2582 + 90.000 11.819 1.1416 + 90.000 12.232 1.0471 + 90.000 12.822 0.93992 + 90.000 13.295 0.86215 + 90.000 14.057 0.87229 + 90.000 14.761 0.86353 + 90.000 15.406 0.86413 + 90.000 15.996 0.79273 + 90.000 16.469 0.69623 + 90.000 16.941 0.64559 + 90.000 17.238 0.57308 + 90.000 17.823 0.59891 + 90.000 18.410 0.59282 + 90.000 19.173 0.58690 + 90.000 19.820 0.55627 + 90.000 20.410 0.50480 + 90.000 20.934 0.56303 + 90.000 21.697 0.55741 + 90.000 22.462 0.52268 + 90.000 22.994 0.46409 + 90.000 23.695 0.50661 + 90.000 24.279 0.54697 + 90.000 25.041 0.55340 + 90.000 25.695 0.41756 + 90.000 26.110 0.36670 + 90.000 26.692 0.42719 + 90.000 27.209 0.59853 + 90.000 27.782 0.93484 + 90.000 28.126 1.2006 + 90.000 28.766 1.3836 + 90.000 29.242 1.1262 + 90.000 29.628 0.38446 + 120.00 4.8625 2.0562 + 120.00 5.1523 2.4430 + 120.00 5.7380 2.5514 + 120.00 6.4412 2.6364 + 120.00 7.1459 2.5539 + 120.00 7.7340 2.3696 + 120.00 8.3231 2.1060 + 120.00 8.9126 1.8319 + 120.00 9.3851 1.5762 + 120.00 9.9735 1.4468 + 120.00 10.328 1.2719 + 120.00 10.858 1.1549 + 120.00 11.271 1.0486 + 120.00 11.858 1.0049 + 120.00 12.272 0.86459 + 120.00 12.568 0.77656 + 120.00 12.981 0.69008 + 120.00 13.629 0.60027 + 120.00 14.333 0.60057 + 120.00 14.922 0.53375 + 120.00 15.277 0.45923 + 120.00 15.748 0.41252 + 120.00 16.395 0.38276 + 120.00 16.867 0.34015 + 120.00 17.158 0.37887 + 120.00 17.862 0.38315 + 120.00 18.392 0.35168 + 120.00 18.683 0.37927 + 120.00 19.328 0.39613 + 120.00 20.031 0.40061 + 120.00 20.328 0.33372 + 120.00 20.567 0.27798 + 120.00 21.270 0.28724 + 120.00 21.859 0.25804 + 120.00 22.562 0.26664 + 120.00 23.151 0.24475 + 120.00 23.915 0.22957 + 120.00 24.619 0.22479 + 120.00 25.327 0.18731 + 120.00 25.565 0.16114 + 120.00 26.038 0.13425 + 120.00 26.860 0.13006 + 120.00 27.206 0.17209 + 120.00 27.781 0.29167 + 120.00 28.242 0.43444 + 120.00 28.647 0.56868 + 120.00 29.238 0.47894 + 120.00 29.782 0.22080 +ENDDATA 139 +ENDSUBENT 153 +SUBENT F0570005 20050527 20050831 F022 +BIB 4 5 +REACTION (28-NI-60(D,P)28-NI-61,,DA/DE) +SAMPLE Self-supported foils of Ni60(4.9 mg/cm2,95.4% enriched) +ERR-ANALYS Statistical errors are from 1% at the low + energy region to 10% at the high energy one. +STATUS (CURVE)Fig.1(b) +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 24.7 0.15 +ENDCOMMON 3 +DATA 3 140 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 45.000 5.1382 6.1931 + 45.000 5.3093 7.2059 + 45.000 6.0057 7.0551 + 45.000 6.7609 6.6154 + 45.000 7.2844 6.1354 + 45.000 7.9823 5.5693 + 45.000 8.6209 5.3939 + 45.000 9.3158 5.6961 + 45.000 10.129 5.4581 + 45.000 10.706 6.2165 + 45.000 11.636 5.6437 + 45.000 12.160 5.0673 + 45.000 12.626 4.6995 + 45.000 13.151 4.0409 + 45.000 13.616 3.7476 + 45.000 14.081 3.6291 + 45.000 15.010 3.3306 + 45.000 15.708 3.0893 + 45.000 16.232 2.7439 + 45.000 16.756 2.4372 + 45.000 17.570 2.2608 + 45.000 18.153 1.9232 + 45.000 18.446 1.6714 + 45.000 19.202 1.5009 + 45.000 19.494 1.3044 + 45.000 19.962 1.0857 + 45.000 20.432 0.79382 + 45.000 21.068 0.87531 + 45.000 21.246 0.72063 + 45.000 22.173 0.75294 + 45.000 22.466 0.64036 + 45.000 22.934 0.53304 + 45.000 23.638 0.35364 + 45.000 24.099 0.41603 + 45.000 25.025 0.45882 + 45.000 25.318 0.39022 + 45.000 25.669 0.33550 + 45.000 26.187 0.40770 + 45.000 26.769 0.37005 + 45.000 27.237 0.29820 + 45.000 27.590 0.22764 + 45.000 28.176 0.17193 + 45.000 28.694 0.21582 + 45.000 29.328 0.25392 + 45.000 29.921 0.13424 + 90.000 4.8945 5.6487 + 90.000 5.5899 5.7170 + 90.000 6.1195 4.9186 + 90.000 6.6496 4.1861 + 90.000 7.1179 3.8424 + 90.000 7.3613 3.0633 + 90.000 7.9478 2.6934 + 90.000 8.5343 2.3681 + 90.000 9.0606 2.1739 + 90.000 9.4140 1.9523 + 90.000 10.058 1.7167 + 90.000 10.587 1.5092 + 90.000 11.290 1.2988 + 90.000 11.643 1.1919 + 90.000 12.230 1.0367 + 90.000 12.815 0.93144 + 90.000 13.400 0.84594 + 90.000 13.874 0.69693 + 90.000 14.458 0.64679 + 90.000 14.987 0.55646 + 90.000 15.458 0.48915 + 90.000 16.216 0.44439 + 90.000 17.036 0.38252 + 90.000 17.450 0.32549 + 90.000 18.037 0.28618 + 90.000 18.686 0.22831 + 90.000 19.102 0.18808 + 90.000 19.457 0.16176 + 90.000 20.095 0.16370 + 90.000 20.790 0.16748 + 90.000 20.985 0.10990 + 90.000 21.287 0.86683E-01 + 90.000 22.203 0.11013 + 90.000 22.616 0.94733E-01 + 90.000 23.259 0.86046E-01 + 90.000 24.414 0.95031E-01 + 90.000 24.545 0.70989E-01 + 90.000 24.976 0.43205E-01 + 90.000 25.847 0.42346E-01 + 90.000 26.182 0.54922E-01 + 90.000 26.694 0.66062E-01 + 90.000 27.440 0.77794E-01 + 90.000 27.764 0.39391E-01 + 90.000 28.064 0.32795E-01 + 90.000 28.477 0.28515E-01 + 90.000 29.009 0.23242E-01 + 90.000 29.634 0.29836E-01 + 90.000 30.296 0.18563E-01 + 135.00 5.7838 7.0723 + 135.00 6.4305 5.8536 + 135.00 6.7873 4.8428 + 135.00 7.4326 4.1373 + 135.00 7.8459 3.5333 + 135.00 8.4907 3.0507 + 135.00 9.1920 2.7190 + 135.00 9.5478 2.2975 + 135.00 9.9021 2.0038 + 135.00 10.491 1.6409 + 135.00 10.674 1.3572 + 135.00 11.261 1.1594 + 135.00 11.845 1.0777 + 135.00 12.138 1.0120 + 135.00 12.723 0.91137 + 135.00 12.961 0.78639 + 135.00 13.667 0.63733 + 135.00 14.252 0.57396 + 135.00 14.609 0.47484 + 135.00 15.196 0.40994 + 135.00 15.780 0.37310 + 135.00 15.963 0.30859 + 135.00 16.772 0.32573 + 135.00 17.011 0.27811 + 135.00 17.486 0.22294 + 135.00 18.130 0.19660 + 135.00 18.772 0.17707 + 135.00 19.356 0.16287 + 135.00 20.002 0.13768 + 135.00 20.475 0.11392 + 135.00 21.404 0.11053 + 135.00 21.538 0.75583E-01 + 135.00 22.465 0.76494E-01 + 135.00 22.763 0.65316E-01 + 135.00 23.001 0.56957E-01 + 135.00 23.982 0.63397E-01 + 135.00 24.629 0.52472E-01 + 135.00 25.098 0.46750E-01 + 135.00 25.572 0.37876E-01 + 135.00 26.225 0.27040E-01 + 135.00 26.805 0.27064E-01 + 135.00 27.317 0.33811E-01 + 135.00 27.715 0.40486E-01 + 135.00 28.187 0.34216E-01 + 135.00 29.110 0.37681E-01 + 135.00 29.588 0.27760E-01 + 135.00 30.192 0.16560E-01 +ENDDATA 142 +ENDSUBENT 156 +SUBENT F0570006 20050527 20050831 F022 +BIB 4 5 +REACTION (28-NI-61(P,EL)28-NI-61,,DA/DE) +SAMPLE Self-supported foils of Ni61(1.45 mg/cm2,98.1%enriched) +ERR-ANALYS Statistical errors are from 1% at the low + energy region to 10% at the high energy one. +STATUS (CURVE)Fig.1(b) +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 29.9 0.15 +ENDCOMMON 3 +DATA 3 137 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 45.000 4.8424 5.7334 + 45.000 5.3525 8.1961 + 45.000 5.8724 8.7507 + 45.000 6.8026 8.2994 + 45.000 7.5013 7.7009 + 45.000 8.0268 6.9912 + 45.000 8.7832 6.5580 + 45.000 9.3630 6.6338 + 45.000 10.472 5.4679 + 45.000 10.996 5.1834 + 45.000 11.579 4.8089 + 45.000 12.161 4.5590 + 45.000 12.972 4.6631 + 45.000 13.317 5.0864 + 45.000 13.837 5.5493 + 45.000 14.364 4.8247 + 45.000 14.948 4.2407 + 45.000 15.532 3.8501 + 45.000 15.817 4.3849 + 45.000 16.285 3.8954 + 45.000 16.811 3.4985 + 45.000 17.272 3.9000 + 45.000 17.732 4.3476 + 45.000 18.201 3.8207 + 45.000 18.720 4.1684 + 45.000 19.591 4.1279 + 45.000 20.580 3.7495 + 45.000 21.101 3.9602 + 45.000 21.736 4.3212 + 45.000 22.371 4.7663 + 45.000 23.122 5.2015 + 45.000 24.051 5.0958 + 45.000 24.518 4.6259 + 45.000 25.045 4.1098 + 45.000 25.739 4.3416 + 45.000 26.313 5.2211 + 45.000 27.057 7.1498 + 45.000 27.564 10.906 + 45.000 27.836 18.730 + 45.000 28.286 28.568 + 45.000 28.622 40.392 + 45.000 29.262 39.132 + 45.000 29.627 23.554 + 45.000 30.064 9.5039 + 90.000 4.4307 3.3282 + 90.000 4.9480 3.7918 + 90.000 5.4682 4.0051 + 90.000 5.9307 4.1846 + 90.000 7.4436 3.7227 + 90.000 7.9714 3.2021 + 90.000 8.4408 2.7839 + 90.000 9.0798 2.7267 + 90.000 9.5492 2.3706 + 90.000 10.017 2.1755 + 90.000 10.542 1.9967 + 90.000 11.010 1.7932 + 90.000 11.421 1.5930 + 90.000 12.122 1.4004 + 90.000 12.937 1.2858 + 90.000 13.577 1.2458 + 90.000 13.872 1.0712 + 90.000 14.508 1.1439 + 90.000 15.093 1.0055 + 90.000 15.554 1.1089 + 90.000 16.073 1.1969 + 90.000 16.485 1.0294 + 90.000 16.954 0.90468 + 90.000 17.653 0.83951 + 90.000 18.465 0.83136 + 90.000 19.159 0.89752 + 90.000 19.745 0.77205 + 90.000 20.496 0.83356 + 90.000 21.072 0.92941 + 90.000 21.312 0.74894 + 90.000 22.071 0.67286 + 90.000 22.704 0.75845 + 90.000 23.175 0.64531 + 90.000 23.870 0.66718 + 90.000 24.505 0.72022 + 90.000 25.141 0.76085 + 90.000 25.958 0.66899 + 90.000 26.253 0.59422 + 90.000 27.177 0.66285 + 90.000 27.744 0.94769 + 90.000 28.023 1.2694 + 90.000 28.363 1.5595 + 90.000 28.833 1.3413 + 90.000 29.619 0.57777 + 135.00 4.5880 3.4588 + 135.00 5.0469 4.0135 + 135.00 5.6241 4.3712 + 135.00 6.3214 4.2380 + 135.00 6.9057 3.7747 + 135.00 7.4327 3.2914 + 135.00 7.9578 3.0259 + 135.00 8.3684 2.6662 + 135.00 8.7778 2.4251 + 135.00 9.1308 2.1141 + 135.00 9.8869 2.0069 + 135.00 10.182 1.7310 + 135.00 10.884 1.4781 + 135.00 11.066 1.1712 + 135.00 11.762 1.1973 + 135.00 12.112 1.1122 + 135.00 12.754 1.0119 + 135.00 13.337 0.93034 + 135.00 13.576 0.76104 + 135.00 14.101 0.71464 + 135.00 14.798 0.69286 + 135.00 15.150 0.61045 + 135.00 15.618 0.54943 + 135.00 16.256 0.54984 + 135.00 16.899 0.48461 + 135.00 17.485 0.40938 + 135.00 17.887 0.46505 + 135.00 18.414 0.40551 + 135.00 18.885 0.32831 + 135.00 19.348 0.34634 + 135.00 20.280 0.30535 + 135.00 20.750 0.26066 + 135.00 21.275 0.24477 + 135.00 22.205 0.23240 + 135.00 22.675 0.19630 + 135.00 23.259 0.17670 + 135.00 23.718 0.20504 + 135.00 24.177 0.23294 + 135.00 24.708 0.18465 + 135.00 24.831 0.15103 + 135.00 25.585 0.14957 + 135.00 26.169 0.13607 + 135.00 26.636 0.12509 + 135.00 27.204 0.17751 + 135.00 27.597 0.25725 + 135.00 28.110 0.33897 + 135.00 28.809 0.30516 + 135.00 29.291 0.18762 + 135.00 29.603 0.99443E-01 +ENDDATA 139 +ENDSUBENT 153 +SUBENT F0570007 20050527 20050831 F022 +BIB 4 5 +REACTION (26-FE-56(A,D)27-CO-58,,DA/DE) +SAMPLE Self-supported foils of Fe56(2.7 mg/cm2,99.7% enriched) +ERR-ANALYS Statistical errors are from 7% at the low + energy region to 25% at the high energy one. +STATUS (CURVE)Fig.2(a) +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 35.8 0.07 +ENDCOMMON 3 +DATA 3 55 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 45.000 5.3249 0.33322 + 45.000 5.9560 0.32905 + 45.000 6.7584 0.32132 + 45.000 7.6728 0.30381 + 45.000 8.3009 0.29058 + 45.000 8.8054 0.25266 + 45.000 9.6068 0.24412 + 45.000 10.236 0.23599 + 45.000 10.580 0.23324 + 45.000 11.210 0.22788 + 45.000 11.774 0.20237 + 45.000 12.402 0.19356 + 45.000 13.268 0.20358 + 45.000 13.895 0.19062 + 45.000 14.473 0.19854 + 45.000 14.947 0.23254 + 45.000 15.443 0.18374 + 45.000 16.181 0.16659 + 45.000 16.895 0.11578 + 45.000 17.560 0.16587 + 45.000 18.135 0.16557 + 45.000 18.427 0.93148E-01 + 45.000 18.964 0.61420E-01 + 45.000 19.557 0.75035E-01 + 45.000 19.807 0.93739E-01 + 45.000 20.309 0.14944 + 45.000 21.106 0.13691 + 45.000 21.278 0.39011E-01 + 105.00 6.8852 0.25109 + 105.00 7.5070 0.22010 + 105.00 8.0713 0.19296 + 105.00 8.5757 0.16379 + 105.00 9.0834 0.14518 + 105.00 9.6469 0.12591 + 105.00 10.156 0.11282 + 105.00 10.885 0.89676E-01 + 105.00 11.790 0.75213E-01 + 105.00 12.010 0.66003E-01 + 105.00 12.758 0.66583E-01 + 105.00 12.971 0.54163E-01 + 105.00 13.191 0.47530E-01 + 105.00 13.411 0.41710E-01 + 105.00 13.939 0.47948E-01 + 105.00 14.799 0.46807E-01 + 105.00 15.596 0.42825E-01 + 105.00 16.342 0.41820E-01 + 105.00 17.263 0.20626E-01 + 105.00 17.565 0.24777E-01 + 105.00 17.993 0.34252E-01 + 105.00 18.471 0.20781E-01 + 105.00 18.836 0.13028E-01 + 105.00 19.478 0.70893E-02 + 105.00 19.905 0.96949E-02 + 105.00 20.337 0.14148E-01 + 105.00 21.135 0.62638E-02 +ENDDATA 57 +ENDSUBENT 71 +SUBENT F0570008 20050527 20050831 F022 +BIB 4 5 +REACTION (26-FE-57(HE3,D)27-CO-58,,DA/DE) +SAMPLE Self-supported foils of Fe57(1.9mg/cm2, 99.5% enriched) +ERR-ANALYS Statistical errors are from 7% at the low + energy region to 25% at the high energy one. +STATUS (CURVE)Fig.2(a) +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 23. 0.07 +ENDCOMMON 3 +DATA 3 28 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 45.000 5.9887 0.49809 + 45.000 6.2998 0.64840 + 45.000 6.7250 0.83490 + 45.000 7.5208 0.74923 + 45.000 7.9517 1.0280 + 45.000 8.5109 0.85721 + 45.000 9.0973 0.97161 + 45.000 9.1143 1.1755 + 45.000 9.9195 1.1727 + 45.000 10.340 1.4321 + 45.000 11.088 1.4289 + 45.000 11.895 1.4559 + 45.000 12.535 1.5815 + 45.000 12.859 1.2385 + 45.000 13.385 1.3602 + 45.000 14.196 1.4612 + 45.000 14.876 1.2979 + 45.000 15.612 1.1285 + 45.000 16.333 0.83722 + 45.000 16.950 0.69802 + 45.000 17.396 0.59473 + 45.000 17.871 0.70349 + 45.000 18.403 0.82325 + 45.000 18.836 0.61126 + 45.000 19.387 0.46341 + 45.000 20.032 0.53075 + 45.000 20.517 0.69790 + 45.000 20.992 0.43279 +ENDDATA 30 +ENDSUBENT 44 +SUBENT F0570009 20050527 20050831 F022 +BIB 4 5 +REACTION (27-CO-59(P,D)27-CO-58,,DA/DE) +SAMPLE Self-supported foils of Co59(5.2 mg/cm2,99.8% enriched) +ERR-ANALYS Statistical errors are from 7% at the low + energy region to 25% at the high energy one. +STATUS (CURVE)Fig.2(a) +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 29.9 0.07 +ENDCOMMON 3 +DATA 3 57 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 45.000 5.7088 0.25797 + 45.000 6.2363 0.28647 + 45.000 6.6910 0.26008 + 45.000 7.2675 0.25697 + 45.000 8.1358 0.26470 + 45.000 8.7740 0.27574 + 45.000 9.4628 0.26104 + 45.000 9.8021 0.23706 + 45.000 10.384 0.25228 + 45.000 11.197 0.26832 + 45.000 11.824 0.24093 + 45.000 12.451 0.21405 + 45.000 12.693 0.25083 + 45.000 13.325 0.24002 + 45.000 14.013 0.22483 + 45.000 14.323 0.29918 + 45.000 14.964 0.32516 + 45.000 15.245 0.29222 + 45.000 16.045 0.26228 + 45.000 16.343 0.29453 + 45.000 17.153 0.30344 + 45.000 17.579 0.40797 + 45.000 18.386 0.39860 + 45.000 18.636 0.23685 + 45.000 19.287 0.13476 + 45.000 19.717 0.19105 + 45.000 20.340 0.35296 + 45.000 20.922 0.37561 + 45.000 21.285 0.21614 + 105.00 6.7882 0.16447 + 105.00 7.4830 0.16964 + 105.00 7.8197 0.14565 + 105.00 8.3837 0.11840 + 105.00 8.7190 0.99484E-01 + 105.00 9.2838 0.81753E-01 + 105.00 9.7004 0.99264E-01 + 105.00 10.322 0.80682E-01 + 105.00 10.653 0.63524E-01 + 105.00 11.464 0.65502E-01 + 105.00 11.852 0.51010E-01 + 105.00 12.320 0.56787E-01 + 105.00 13.194 0.63848E-01 + 105.00 13.572 0.42725E-01 + 105.00 13.591 0.57240E-01 + 105.00 13.804 0.43167E-01 + 105.00 14.374 0.38268E-01 + 105.00 14.886 0.34299E-01 + 105.00 15.468 0.36953E-01 + 105.00 16.152 0.32048E-01 + 105.00 16.954 0.29018E-01 + 105.00 17.565 0.49276E-01 + 105.00 17.927 0.62488E-01 + 105.00 18.922 0.31505E-01 + 105.00 19.251 0.23753E-01 + 105.00 19.866 0.43044E-01 + 105.00 20.559 0.42976E-01 + 105.00 20.993 0.27835E-01 +ENDDATA 59 +ENDSUBENT 73 +SUBENT F0570010 20050527 20050831 F022 +BIB 4 5 +REACTION (26-FE-56(A,EL)26-FE-56,,DA/DE) +SAMPLE Self-supported foils of Fe56(2.7 mg/cm2,99.7% enriched) +ERR-ANALYS Statistical errors are from 3% at the low + energy region to 20% at the high energy one. +STATUS (CURVE)Fig.2(b) +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 35.8 0.07 +ENDCOMMON 3 +DATA 3 76 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 30.000 9.5637 4.0523 + 30.000 10.139 3.7161 + 30.000 10.773 3.4074 + 30.000 11.466 3.1912 + 30.000 12.455 3.2180 + 30.000 12.732 2.6545 + 30.000 13.190 2.4091 + 30.000 13.591 2.2101 + 30.000 14.643 2.3756 + 30.000 14.864 2.0235 + 30.000 15.677 1.9983 + 30.000 16.199 1.9538 + 30.000 16.595 1.6636 + 30.000 17.110 1.4777 + 30.000 17.869 1.5559 + 30.000 18.682 1.5365 + 30.000 19.492 1.4540 + 30.000 20.479 1.4201 + 30.000 21.407 1.3725 + 30.000 22.276 1.3266 + 30.000 23.212 1.4263 + 30.000 23.859 1.6013 + 30.000 24.216 1.7990 + 30.000 24.718 1.3333 + 30.000 25.216 2.1515 + 30.000 25.520 2.5771 + 30.000 26.029 2.1246 + 30.000 26.703 3.5009 + 30.000 27.286 0.66288 + 30.000 27.664 1.0144 + 30.000 28.172 1.8802 + 30.000 28.703 0.90004 + 30.000 29.383 0.70324 + 30.000 29.623 4.2128 + 30.000 29.946 6.8009 + 30.000 30.310 8.4098 + 30.000 31.228 3.0162 + 105.00 9.5682 2.3217 + 105.00 10.311 1.9294 + 105.00 10.709 1.6935 + 105.00 11.218 1.3781 + 105.00 11.902 1.1331 + 105.00 12.412 0.94214 + 105.00 12.922 0.77496 + 105.00 13.315 0.63079 + 105.00 14.127 0.61614 + 105.00 14.284 0.48061 + 105.00 14.969 0.39945 + 105.00 15.248 0.33592 + 105.00 15.875 0.28226 + 105.00 16.569 0.26700 + 105.00 16.673 0.22222 + 105.00 17.355 0.17881 + 105.00 18.221 0.16369 + 105.00 18.913 0.14992 + 105.00 19.481 0.12463 + 105.00 20.112 0.11053 + 105.00 20.627 0.96990E-01 + 105.00 21.082 0.84211E-01 + 105.00 21.896 0.84048E-01 + 105.00 22.232 0.70671E-01 + 105.00 22.925 0.66133E-01 + 105.00 23.916 0.68147E-01 + 105.00 24.252 0.56686E-01 + 105.00 24.590 0.48703E-01 + 105.00 25.347 0.49675E-01 + 105.00 25.712 0.62247E-01 + 105.00 26.407 0.60166E-01 + 105.00 26.728 0.40339E-01 + 105.00 27.269 0.22503E-01 + 105.00 27.769 0.16089E-01 + 105.00 28.436 0.23941E-01 + 105.00 29.054 0.17485E-01 + 105.00 30.061 0.23089E-01 + 105.00 30.528 0.54653E-01 + 105.00 30.836 0.70747E-01 +ENDDATA 78 +ENDSUBENT 92 +SUBENT F0570011 20050527 20050831 F022 +BIB 4 5 +REACTION (26-FE-57(HE3,A)26-FE-56,,DA/DE) +SAMPLE Self-supported foils of Fe57(1.9mg/cm2, 99.5% enriched) +ERR-ANALYS Statistical errors are from 3% at the low + energy region to 20% at the high energy one. +STATUS (CURVE)Fig.2(b) +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 23.0 0.07 +ENDCOMMON 3 +DATA 3 79 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 30.000 9.8305 2.7722 + 30.000 10.457 2.4358 + 30.000 10.912 2.1873 + 30.000 11.303 1.8430 + 30.000 11.743 1.3813 + 30.000 12.189 1.1153 + 30.000 12.867 0.90951 + 30.000 13.601 0.72598 + 30.000 14.708 0.77969 + 30.000 14.985 0.66421 + 30.000 15.375 0.55375 + 30.000 16.179 0.50745 + 30.000 16.885 0.57540 + 30.000 17.334 0.48476 + 30.000 17.925 0.55572 + 30.000 18.402 0.65792 + 30.000 18.915 0.59702 + 30.000 19.277 0.70705 + 30.000 19.784 0.59558 + 30.000 20.291 0.49637 + 30.000 20.889 0.62618 + 30.000 21.372 0.79018 + 30.000 21.824 0.68728 + 30.000 22.262 0.50427 + 30.000 23.131 0.50843 + 30.000 24.004 0.52924 + 30.000 24.444 0.40090 + 30.000 24.810 0.50071 + 30.000 25.523 0.61815 + 30.000 25.848 0.47341 + 30.000 26.283 0.33289 + 30.000 26.967 0.59003 + 30.000 27.454 0.38919 + 30.000 27.769 0.52932 + 30.000 28.377 0.74265 + 30.000 28.668 0.37570 + 30.000 29.283 0.28749 + 30.000 29.976 0.68276E-01 + 30.000 30.414 0.24829E-01 + 30.000 31.014 0.64553E-01 + 30.000 31.397 0.99729E-01 + 30.000 32.039 0.52036E-01 + 105.00 10.253 1.4156 + 105.00 10.761 1.1886 + 105.00 11.500 0.99735 + 105.00 12.005 0.81947 + 105.00 12.398 0.69579 + 105.00 13.130 0.53538 + 105.00 13.516 0.42138 + 105.00 13.965 0.35387 + 105.00 14.296 0.28777 + 105.00 15.206 0.23363 + 105.00 15.476 0.18197 + 105.00 15.981 0.14790 + 105.00 16.431 0.12556 + 105.00 16.879 0.10318 + 105.00 17.433 0.75246E-01 + 105.00 18.179 0.68855E-01 + 105.00 18.513 0.58472E-01 + 105.00 18.846 0.48591E-01 + 105.00 19.651 0.45430E-01 + 105.00 20.442 0.35331E-01 + 105.00 20.952 0.30645E-01 + 105.00 21.798 0.22819E-01 + 105.00 22.472 0.17561E-01 + 105.00 23.036 0.14584E-01 + 105.00 23.364 0.11480E-01 + 105.00 24.131 0.13624E-01 + 105.00 24.459 0.10609E-01 + 105.00 24.971 0.94038E-02 + 105.00 25.335 0.11667E-01 + 105.00 26.096 0.12834E-01 + 105.00 26.489 0.10897E-01 + 105.00 26.883 0.94552E-02 + 105.00 27.251 0.59279E-02 + 105.00 27.863 0.89319E-02 + 105.00 28.631 0.10715E-01 + 105.00 29.374 0.45929E-02 + 105.00 29.725 0.23439E-02 +ENDDATA 81 +ENDSUBENT 95 +SUBENT F0570012 20050527 20050831 F022 +BIB 4 5 +REACTION (27-CO-59(P,A)26-FE-56,,DA/DE) +SAMPLE Self-supported foils of Co59(5.2 mg/cm2,99.8% enriched) +ERR-ANALYS Statistical errors are from 3% at the low + energy region to 20% at the high energy one. +STATUS (CURVE)Fig.2(b) +ENDBIB 5 +COMMON 2 3 +EN E-ERR-DIG +MEV MEV + 29.9 0.07 +ENDCOMMON 3 +DATA 3 84 +ANG-CM E-CM DATA-CM +ADEG MEV MB/SR/MEV + 30.000 9.0843 1.0713 + 30.000 9.6206 1.3375 + 30.000 10.249 1.2395 + 30.000 10.994 1.1606 + 30.000 11.385 0.98843 + 30.000 11.779 0.86910 + 30.000 12.347 0.78024 + 30.000 12.794 0.65043 + 30.000 13.304 0.57784 + 30.000 13.580 0.49228 + 30.000 14.201 0.41457 + 30.000 14.823 0.35286 + 30.000 15.333 0.31348 + 30.000 15.901 0.28143 + 30.000 16.529 0.25805 + 30.000 17.099 0.23665 + 30.000 17.665 0.20578 + 30.000 18.117 0.18284 + 30.000 18.745 0.16765 + 30.000 19.489 0.15698 + 30.000 19.767 0.13661 + 30.000 20.394 0.12526 + 30.000 20.861 0.13335 + 30.000 21.365 0.10997 + 30.000 21.815 0.95657E-01 + 30.000 22.446 0.91521E-01 + 30.000 23.012 0.79584E-01 + 30.000 23.515 0.64937E-01 + 30.000 24.198 0.57664E-01 + 30.000 24.836 0.60069E-01 + 30.000 25.196 0.71904E-01 + 30.000 25.885 0.69520E-01 + 30.000 26.184 0.37887E-01 + 30.000 26.950 0.46773E-01 + 30.000 27.311 0.26878E-01 + 30.000 27.950 0.59577E-01 + 30.000 28.330 0.93031E-01 + 30.000 28.654 0.15737E-01 + 30.000 29.279 0.29425E-01 + 30.000 29.909 0.29851E-02 + 30.000 30.422 0.58258E-02 + 30.000 30.873 0.10669E-01 + 30.000 31.381 0.92786E-02 + 30.000 31.704 0.32694E-02 + 105.00 9.9895 0.42154 + 105.00 10.230 0.48492 + 105.00 10.919 0.46361 + 105.00 11.314 0.41119 + 105.00 11.874 0.32365 + 105.00 12.622 0.31275 + 105.00 13.073 0.26849 + 105.00 13.406 0.22320 + 105.00 13.741 0.18961 + 105.00 14.358 0.14762 + 105.00 14.981 0.12531 + 105.00 15.432 0.10875 + 105.00 15.885 0.95403E-01 + 105.00 16.165 0.84640E-01 + 105.00 16.998 0.53622E-01 + 105.00 17.468 0.60330E-01 + 105.00 17.791 0.43574E-01 + 105.00 18.287 0.31120E-01 + 105.00 18.978 0.30733E-01 + 105.00 19.232 0.18672E-01 + 105.00 19.683 0.16030E-01 + 105.00 20.251 0.14059E-01 + 105.00 21.001 0.14186E-01 + 105.00 21.276 0.11667E-01 + 105.00 21.670 0.10127E-01 + 105.00 22.534 0.99968E-02 + 105.00 22.864 0.78729E-02 + 105.00 23.333 0.88579E-02 + 105.00 23.841 0.75216E-02 + 105.00 24.113 0.59244E-02 + 105.00 24.892 0.39624E-02 + 105.00 25.249 0.46065E-02 + 105.00 25.845 0.60942E-02 + 105.00 26.335 0.39915E-02 + 105.00 26.831 0.28817E-02 + 105.00 27.381 0.19494E-02 + 105.00 28.062 0.16726E-02 + 105.00 28.498 0.11566E-02 + 105.00 28.995 0.19209E-02 + 105.00 29.616 0.69366E-03 +ENDDATA 86 +ENDSUBENT 100 +ENDENTRY 12 diff --git a/exforall/F05/F0578.x4 b/exforall/F05/F0578.x4 new file mode 100644 index 000000000..8634d3289 --- /dev/null +++ b/exforall/F05/F0578.x4 @@ -0,0 +1,433 @@ +ENTRY F0578 20050418 20050831 F021 +SUBENT F0578001 20050418 20050831 F021 +BIB 9 12 +TITLE The elastic scattering of protons with the energy of 15 + MeV by 24Mg nuclei. +AUTHOR (E.A.Romanovskij,T.I.Spasskaya,K.Kadim) +INSTITUTE (4RUSMOS) +REFERENCE (J,IZV,48,977,1984) +FACILITY Facility is not mentioned. +DETECTOR (SILI)Detectors with the thickness of sensitive level + of 700 mu-m were used. +METHOD Proton back-scattering on thick targets. +ERR-ANALYS (ERR-DIG)Digitizing error + (EN-ERR-DIG)Digitizing error +HISTORY (20041005C) +ENDBIB 12 +NOCOMMON 0 0 +ENDSUBENT 15 +SUBENT F0578002 20050418 20050831 F021 +BIB 2 2 +REACTION (12-MG-24(P,EL)12-MG-24,,DA) +STATUS (CURVE)Fig.5 +ENDBIB 2 +COMMON 2 3 +EN-ERR-DIG ERR-DIG +MEV MB/SR + 0.002 0.84 +ENDCOMMON 3 +DATA 3 256 +ANG-CM EN DATA-CM +ADEG MEV MB/SR + 92.400 5.7553 42.048 + 92.400 5.7911 44.751 + 92.400 5.8092 49.459 + 92.400 5.8378 47.706 + 92.400 5.8580 42.898 + 92.400 5.8795 36.408 + 92.400 5.9139 39.115 + 92.400 5.9391 48.000 + 92.400 5.9589 57.738 + 92.400 5.9881 64.375 + 92.400 6.0128 65.429 + 92.400 6.0332 63.697 + 92.400 6.0548 58.047 + 92.400 6.0858 50.693 + 92.400 6.1099 42.518 + 92.400 6.1342 36.301 + 92.400 6.1652 28.948 + 92.400 6.1981 29.701 + 92.400 6.2260 37.180 + 92.400 6.2555 49.969 + 92.400 6.2752 58.589 + 92.400 6.5969 57.467 + 92.400 6.6200 55.728 + 92.400 6.6476 58.174 + 92.400 6.6776 56.697 + 92.400 6.7071 46.550 + 92.400 6.7339 36.969 + 92.400 6.7622 31.021 + 92.400 6.7924 31.781 + 92.400 6.8220 45.969 + 92.400 6.8473 55.413 + 92.400 6.8792 61.763 + 92.400 6.9187 58.303 + 92.400 6.9410 42.861 + 92.400 6.9554 33.033 + 92.400 6.9782 24.862 + 92.400 7.0186 37.063 + 92.400 7.0699 46.719 + 92.400 7.1011 41.603 + 92.400 7.1295 36.494 + 92.400 7.1593 31.940 + 92.400 7.1947 28.211 + 92.400 7.2249 28.971 + 92.400 7.2553 33.367 + 92.400 7.2843 38.885 + 92.400 7.3187 40.194 + 92.400 7.3517 42.625 + 92.400 7.3833 44.780 + 92.400 7.4217 46.078 + 92.400 7.4556 41.514 + 92.400 7.4914 43.938 + 92.400 7.5150 49.470 + 92.400 7.5576 51.037 + 92.400 7.5954 43.665 + 112.30 5.6489 26.200 + 112.30 5.6735 25.297 + 112.30 5.6998 29.424 + 112.30 5.7269 25.437 + 112.30 5.7535 35.437 + 112.30 5.7825 38.438 + 112.30 5.8206 34.982 + 112.30 5.8741 36.520 + 112.30 5.8993 46.244 + 112.30 5.9238 42.824 + 112.30 5.9554 44.699 + 112.30 5.9832 52.178 + 112.30 6.0117 47.069 + 112.30 6.0400 40.003 + 112.30 6.0670 35.177 + 112.30 6.0955 30.907 + 112.30 6.1253 26.075 + 112.30 6.1637 26.254 + 112.30 6.2041 38.176 + 112.30 6.2308 47.896 + 112.30 6.2638 51.166 + 112.30 6.5089 51.924 + 112.30 6.5333 47.106 + 112.30 6.5712 41.133 + 112.30 6.6055 41.043 + 112.30 6.6412 42.908 + 112.30 6.6729 46.741 + 112.30 6.7170 51.381 + 112.30 6.7432 54.669 + 112.30 6.7746 53.748 + 112.30 6.8104 56.171 + 112.30 6.8421 60.284 + 112.30 6.8749 59.080 + 112.30 6.9047 53.128 + 112.30 6.9356 44.097 + 112.30 6.9791 39.229 + 112.30 7.0454 48.286 + 112.30 7.0893 49.290 + 112.30 7.1206 47.530 + 112.30 7.1612 38.753 + 112.30 7.1964 32.787 + 112.30 7.2292 31.583 + 112.30 7.2676 33.441 + 112.30 7.3088 35.571 + 112.30 7.3447 39.952 + 112.30 7.3752 45.746 + 112.30 7.4195 54.301 + 112.30 7.4492 47.511 + 112.30 7.4843 40.147 + 112.30 7.5271 45.070 + 112.30 7.5750 44.665 + 131.50 5.6561 36.060 + 131.50 5.6931 36.250 + 131.50 5.7207 40.495 + 131.50 5.7494 39.844 + 131.50 5.7743 42.944 + 131.50 5.8043 41.139 + 131.50 5.8384 39.035 + 131.50 5.8688 44.423 + 131.50 5.8941 55.868 + 131.50 5.9235 66.728 + 131.50 5.9619 66.627 + 131.50 5.9820 60.818 + 131.50 6.0105 56.426 + 131.50 6.0484 49.132 + 131.50 6.0825 45.877 + 131.50 6.1081 39.191 + 131.50 6.1377 31.342 + 131.50 6.1734 31.824 + 131.50 6.2082 42.669 + 131.50 6.2390 52.949 + 131.50 6.2736 60.053 + 131.50 6.5261 46.440 + 131.50 6.5573 42.617 + 131.50 6.5954 38.487 + 131.50 6.6282 36.387 + 131.50 6.6695 41.171 + 131.50 6.7101 56.030 + 131.50 6.7480 72.335 + 131.50 6.7812 77.428 + 131.50 6.8151 71.871 + 131.50 6.8526 58.534 + 131.50 6.8931 48.930 + 131.50 6.9615 47.024 + 131.50 6.9905 51.841 + 131.50 7.0113 56.966 + 131.50 7.0461 42.198 + 131.50 7.0703 35.515 + 131.50 7.1223 34.227 + 131.50 7.1595 38.159 + 131.50 7.1958 26.839 + 131.50 7.2309 19.265 + 131.50 7.2717 14.553 + 131.50 7.3125 9.8411 + 131.50 7.3521 9.1614 + 131.50 7.3907 13.377 + 131.50 7.4366 24.481 + 131.50 7.4739 30.714 + 131.50 7.5158 22.258 + 131.50 7.5567 18.122 + 131.50 7.6005 17.719 + 151.20 5.6441 40.308 + 151.20 5.6770 41.936 + 151.20 5.7081 35.569 + 151.20 5.7353 32.641 + 151.20 5.7599 30.862 + 151.20 5.7859 31.080 + 151.20 5.8188 32.137 + 151.20 5.8476 33.205 + 151.20 5.8755 42.276 + 151.20 5.9062 51.626 + 151.20 5.9356 61.836 + 151.20 5.9641 57.761 + 151.20 5.9900 56.551 + 151.20 6.0203 58.472 + 151.20 6.0571 55.805 + 151.20 6.0880 46.866 + 151.20 6.1109 39.949 + 151.20 6.1446 31.860 + 151.20 6.1766 39.206 + 151.20 6.2155 49.963 + 151.20 6.5022 58.359 + 151.20 6.5323 57.710 + 151.20 6.5652 58.767 + 151.20 6.5993 57.535 + 151.20 6.6321 56.306 + 151.20 6.6705 57.064 + 151.20 6.7108 66.388 + 151.20 6.7412 95.169 + 151.20 6.7832 110.78 + 151.20 6.8185 106.11 + 151.20 6.8592 76.860 + 151.20 6.8905 50.490 + 151.20 6.9311 42.669 + 151.20 6.9676 57.433 + 151.20 7.0110 73.035 + 151.20 7.0562 73.775 + 151.20 7.0994 40.230 + 151.20 7.1232 27.024 + 151.20 7.1631 29.206 + 151.20 7.1983 23.685 + 151.20 7.2337 19.307 + 151.20 7.2718 16.636 + 151.20 7.3142 15.383 + 151.20 7.3500 18.433 + 151.20 7.3848 28.343 + 151.20 7.4286 51.088 + 151.20 7.4677 63.845 + 151.20 7.5048 66.891 + 151.20 7.5476 49.635 + 151.20 7.5868 41.246 + 160.80 5.6869 44.757 + 160.80 5.7137 35.573 + 160.80 5.7392 28.325 + 160.80 5.7678 25.491 + 160.80 5.7967 27.076 + 160.80 5.8269 28.658 + 160.80 5.8531 31.631 + 160.80 5.8796 40.404 + 160.80 5.9132 52.199 + 160.80 5.9370 60.427 + 160.80 5.9643 58.977 + 160.80 5.9970 56.685 + 160.80 6.0246 59.378 + 160.80 6.0480 62.358 + 160.80 6.0810 64.485 + 160.80 6.1056 42.046 + 160.80 6.1364 31.194 + 160.80 6.1709 34.423 + 160.80 6.2033 49.536 + 160.80 6.2436 59.380 + 160.80 6.5137 65.331 + 160.80 6.5463 61.105 + 160.80 6.5754 66.834 + 160.80 6.6013 64.559 + 160.80 6.6431 77.438 + 160.80 6.6780 65.747 + 160.80 6.7181 71.724 + 160.80 6.7475 105.35 + 160.80 6.7888 130.67 + 160.80 6.8212 123.13 + 160.80 6.8535 92.103 + 160.80 6.8922 53.053 + 160.80 6.9281 37.215 + 160.80 6.9603 48.737 + 160.80 7.0005 78.197 + 160.80 7.0365 84.460 + 160.80 7.1033 58.600 + 160.80 7.1468 31.693 + 160.80 7.1738 25.547 + 160.80 7.2079 22.146 + 160.80 7.2405 18.749 + 160.80 7.2801 17.544 + 160.80 7.3173 20.766 + 160.80 7.3574 27.019 + 160.80 7.3860 47.391 + 160.80 7.4253 85.416 + 160.80 7.4662 125.65 + 160.80 7.5165 142.65 + 160.80 7.5475 113.29 + 160.80 7.5782 77.849 + 160.80 7.6300 52.579 +ENDDATA 258 +ENDSUBENT 269 +SUBENT F0578003 20050418 20050831 F021 +BIB 4 5 +REACTION (12-MG-24(P,EL)12-MG-24,,DA) +MONITOR Data were normalized on data of Rhoderick E.H. at + the angle of 20 degr. +MONIT-REF (,E.H.Rhoderick,J,PRS,201,348,1950) +STATUS (CURVE)Fig.6 +ENDBIB 5 +COMMON 2 3 +EN-ERR-DIG ERR-DIG +MEV MB/SR + 0.001 0.2 +ENDCOMMON 3 +DATA 3 102 +ANG-CM EN DATA-CM +ADEG MEV MB/SR + 92.400 4.3364 70.693 + 92.400 4.3498 68.589 + 92.400 4.3631 66.485 + 92.400 4.3784 64.983 + 92.400 4.3975 63.180 + 92.400 4.4147 61.677 + 92.400 4.4337 59.874 + 92.400 4.4547 57.771 + 92.400 4.4796 55.367 + 92.400 4.4986 51.459 + 92.400 4.5216 47.251 + 92.400 4.5483 41.840 + 92.400 4.5674 36.729 + 92.400 4.5884 32.220 + 92.400 4.6113 26.809 + 92.400 4.6285 21.698 + 92.400 4.6457 17.188 + 92.400 4.6705 12.379 + 92.400 4.6991 11.478 + 92.400 4.7144 15.389 + 92.400 4.7411 22.306 + 92.400 4.7659 28.623 + 92.400 4.8097 37.346 + 92.400 4.8326 38.550 + 92.400 4.8536 37.649 + 112.30 4.1855 69.768 + 112.30 4.2141 68.452 + 112.30 4.2408 66.146 + 112.30 4.2695 64.171 + 112.30 4.2867 56.917 + 112.30 4.3153 59.559 + 112.30 4.3382 58.572 + 112.30 4.3611 58.245 + 112.30 4.3878 56.929 + 112.30 4.4126 55.942 + 112.30 4.4355 54.956 + 112.30 4.4622 53.310 + 112.30 4.4852 51.663 + 112.30 4.5023 49.027 + 112.30 4.5272 45.402 + 112.30 4.5463 41.446 + 112.30 4.5711 35.182 + 112.30 4.5959 28.919 + 112.30 4.6150 23.644 + 112.30 4.6399 17.050 + 112.30 4.6666 9.4671 + 112.30 4.6972 6.8322 + 112.30 4.7277 9.4746 + 112.30 4.7544 15.085 + 112.30 4.7696 20.694 + 112.30 4.8039 28.944 + 112.30 4.8287 35.544 + 112.30 4.8593 35.877 + 131.80 4.2009 55.050 + 131.80 4.2295 54.344 + 131.80 4.2524 52.222 + 131.80 4.2830 48.685 + 131.80 4.3116 49.395 + 131.80 4.3383 50.812 + 131.80 4.3650 51.876 + 131.80 4.3898 53.647 + 131.80 4.4147 54.003 + 131.80 4.4376 51.527 + 131.80 4.4643 49.759 + 131.80 4.4948 48.346 + 131.80 4.5215 47.993 + 131.80 4.5521 46.580 + 131.80 4.5750 41.981 + 131.80 4.5979 34.550 + 131.80 4.6265 23.935 + 131.80 4.6437 17.920 + 131.80 4.6666 12.967 + 131.80 4.6895 8.7217 + 131.80 4.7163 7.6618 + 131.80 4.7525 9.4337 + 131.80 4.7792 12.975 + 131.80 4.8021 20.054 + 131.80 4.8307 21.826 + 131.80 4.8632 23.597 + 151.20 4.1971 52.900 + 151.20 4.2295 50.573 + 151.20 4.2601 45.528 + 151.20 4.2906 44.754 + 151.20 4.3154 47.087 + 151.20 4.3402 49.419 + 151.20 4.3650 52.140 + 151.20 4.4146 52.145 + 151.20 4.4375 50.206 + 151.20 4.4643 45.937 + 151.20 4.4948 44.775 + 151.20 4.5196 45.166 + 151.20 4.5463 46.333 + 151.20 4.5940 42.455 + 151.20 4.6208 35.467 + 151.20 4.6494 24.985 + 151.20 4.6723 17.997 + 151.20 4.6991 12.952 + 151.20 4.7449 7.5196 + 151.20 4.7697 9.4638 + 151.20 4.7926 14.126 + 151.20 4.8269 24.615 + 151.20 4.8536 31.608 +ENDDATA 104 +ENDSUBENT 118 +SUBENT F0578004 20050418 20050831 F021 +BIB 3 3 +REACTION (12-MG-24(P,EL)12-MG-24,,SIG) +ERR-ANALYS (DATA-ERR)Error from the graphic bars +STATUS (CURVE)Fig.8 +ENDBIB 3 +COMMON 2 3 +EN-ERR-DIG ERR-DIG +MEV MB + 0.1 2.61 +ENDCOMMON 3 +DATA 3 7 +EN DATA DATA-ERR +MEV MB MB + 4.8295 558.26 88.228 + 5.8256 694.63 113.96 + 6.1210 727.81 124.99 + 6.5642 775.76 139.71 + 7.3075 720.87 95.593 + 9.6050 747.39 80.863 + 12.607 774.16 110.30 +ENDDATA 9 +ENDSUBENT 21 +ENDENTRY 4 diff --git a/exforall/F05/F0579.x4 b/exforall/F05/F0579.x4 new file mode 100644 index 000000000..3c2be09cc --- /dev/null +++ b/exforall/F05/F0579.x4 @@ -0,0 +1,162 @@ +ENTRY F0579 20050623 20050831 F021 +SUBENT F0579001 20050623 20050831 F021 +BIB 12 25 +TITLE Total cross-sections of reactions induced by deutrons + with 13.6 MeV energy. +AUTHOR (L.V.Dubar,O.F.Nemets,L.I.Slyusarenko,V.V.Tokarevskij) +INSTITUTE (4UKRIJD) +REFERENCE (J,YF,20,624,1974) +FACILITY (CYCLO) R-7 cyclotron +INC-SOURCE Deutron beam with energy of 13.6 MeV was used. Size of + beam spot on target was 9.6 mm2. +DETECTOR Two Faraday Cups. +SAMPLE Target square was 314 mm2, diameter was 20 mm. + Target thickness measurement was carried out in two + ways: by weighting and by elastic scattering of 6.8 MeV + protons at small angles. +METHOD (BCINT) + The charge of incident particle beam and beam reduction + on the target was measured. It was propotional to the + charge collected on the target. +MONITOR Aperture of scattering chamber was determined by + measuring of 6.8 MeV proton beam reduction while + passing through platinum target. Total cross-section + of protons was 40790+-1230 mbr. +ERR-ANALYS (DATA-ERR) Error of total cross section. + Error of measurements due to uncertanties of target + thickness was 2%. +HISTORY (20041109C) +ENDBIB 25 +NOCOMMON 0 0 +ENDSUBENT 28 +SUBENT F0579002 20050623 20050831 F021 +BIB 3 3 +REACTION (13-AL-27(D,TOT),,SIG) +SAMPLE Target thickness was 8.12+-0.08 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.350 1204.0 27.000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0579003 20050623 20050831 F021 +BIB 3 3 +REACTION (26-FE-0(D,TOT),,SIG) +SAMPLE Target thickness was 10.38+-0.10 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.400 1577.0 68.000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0579004 20050623 20050831 F021 +BIB 3 3 +REACTION (27-CO-59(D,TOT),,SIG) +SAMPLE Target thickness was 9.94+-0.10 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.400 1609.0 41.000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0579005 20050623 20050831 F021 +BIB 3 3 +REACTION (28-NI-0(D,TOT),,SIG) +SAMPLE Target thickness was 17.98+-0.10 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.200 1457.0 33.000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0579006 20050623 20050831 F021 +BIB 3 3 +REACTION (28-NI-60(D,TOT),,SIG) +SAMPLE Target thickness was 5.51+-0.06 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.590 1536.0 125.00 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0579007 20050623 20050831 F021 +BIB 3 3 +REACTION (28-NI-64(D,TOT),,SIG) +SAMPLE Target thickness was 7.42+-0.15 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.460 1666.0 60.000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0579008 20050623 20050831 F021 +BIB 3 3 +REACTION (29-CU-63(D,TOT),,SIG) +SAMPLE Target thickness was 16.01+-0.32 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.310 1609.0 81.000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0579009 20050623 20050831 F021 +BIB 3 3 +REACTION (29-CU-65(D,TOT),,SIG) +SAMPLE Target thickness was 9.61+-0.19 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.420 1655.0 63.000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0579010 20050623 20050831 F021 +BIB 3 3 +REACTION (30-ZN-0(D,TOT),,SIG) +SAMPLE Target thickness was 8.79+-0.09 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.430 1562.0 46.000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0579011 20050623 20050831 F021 +BIB 3 3 +REACTION (47-AG-0(D,TOT),,SIG) +SAMPLE Target thickness was 5.78+-0.06 mg/cm2. +STATUS (TABLE) Table 1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN DATA DATA-ERR +MEV MB MB + 13.500 1644.0 101.00 +ENDDATA 3 +ENDSUBENT 11 +ENDENTRY 11 diff --git a/exforall/F05/F0581.x4 b/exforall/F05/F0581.x4 new file mode 100644 index 000000000..682c3e99f --- /dev/null +++ b/exforall/F05/F0581.x4 @@ -0,0 +1,64 @@ +ENTRY F0581 20050623 20050831 F021 +SUBENT F0581001 20050623 20050831 F021 +BIB 11 24 +TITLE 184m,gRe isomeric ratios in the reactions (a,n) + and (g,n). +AUTHOR (I.N.Vishnevskij,V.A.Zheltonozhskij,V.M.Mazur, + S.V.Reshit'ko) +INSTITUTE (4UKRIJD) +REFERENCE (J,IZV,53,(1),171,1989) +FACILITY (CYCLO) two cyclotrons U-120 and U-240. +SAMPLE The target assembly of pure tantalum foils was used. + The thickness of assembly used on U-120 was of such + value, that the energies of alpha particles were + decreased down to 0 MeV. The thicknesses of foils used + on U-240 were equal to 80 and 200 microns. The energies + of alpha particles were decreased from 100 MeV down to + 30 MeV. +METHOD (ACTIV) Isomeric ratios were determined by activation + technique. +DETECTOR (HPGE)Ge-spectrometer with germanium detector was used. +REL-REF (R,,I.N.Vishnevskiy+,J,YF,41,1435,1985)The calculation + technique was described in this work. +ERR-ANALYS (EN-ERR) Uncertanty was determined by special tables + and by experimental technique. + (DATA-ERR) Uncertanty was determined by statistic + accuracy. +HISTORY (20030806C) +ENDBIB 24 +NOCOMMON 0 0 +ENDSUBENT 27 +SUBENT F0581002 20050623 20050831 F021 +BIB 3 4 +REACTION (73-TA-181(A,N)75-RE-184-M/G,,SIG/RAT) +DECAY-DATA (75-RE-184-G,38.D,DG,903.) + (75-RE-184-M,165.D,DG,921.) +STATUS (TABLE) Table 1 +ENDBIB 4 +NOCOMMON 0 0 +DATA 4 20 +EN EN-ERR DATA DATA-ERR +MEV MEV NO-DIM NO-DIM + 13.200 0.30000 0.31000 0.30000E-01 + 15.600 0.30000 0.18000 0.20000E-01 + 17.700 0.30000 0.20000 0.10000E-01 + 19.800 0.30000 0.30000 0.20000E-01 + 21.600 0.30000 0.42000 0.20000E-01 + 23.400 0.30000 0.48000 0.20000E-01 + 25.200 0.30000 0.51000 0.30000E-01 + 26.800 0.30000 0.43000 0.40000E-01 + 31.000 1.0000 0.82000 0.40000E-01 + 35.000 1.0000 1.0100 0.50000E-01 + 39.000 1.0000 0.90000 0.90000E-01 + 43.000 1.0000 1.0500 0.50000E-01 + 46.000 1.0000 1.0300 0.50000E-01 + 49.000 1.0000 0.83000 0.40000E-01 + 57.000 1.0000 0.63000 0.40000E-01 + 65.000 1.0000 0.93000 0.90000E-01 + 72.000 1.0000 1.1000 0.10000 + 81.000 1.0000 2.0000 0.20000 + 90.000 1.0000 3.5000 0.40000 + 98.000 1.0000 4.3000 0.60000 +ENDDATA 22 +ENDSUBENT 31 +ENDENTRY 2 diff --git a/exforall/F05/F0586.x4 b/exforall/F05/F0586.x4 new file mode 100644 index 000000000..eaa30ee85 --- /dev/null +++ b/exforall/F05/F0586.x4 @@ -0,0 +1,591 @@ +ENTRY F0586 20050623 20050831 F021 +SUBENT F0586001 20050623 20050831 F021 +BIB 10 25 +TITLE Production of fragments of mass number 6<=A<=11 in 12C, + 14N and 16O spallation by alpha-particles at energies + near threshold. +AUTHOR (A.Vidal-Quadras, M.Ortega) +INSTITUTE (2SPNSPN) +REFERENCE (J,NC/A,49,235,1979) +FACILITY (SYNCY,2ZZZITU) +INC-SOURCE Alpha-particle beam.Cross sections represent an average + over the energy interval of 25-60 MeV and centred at + mean incident energy E=33.4 MeV. The mean energy of + incident alpha particles is found to be 33.4+-2.7, + 42.9+-2.9 and 50.6+-2.6 MeV for each of the three + energy regions of about 10 MeV width. + Incident angle was 45 degrees and approximate flux + 10**5 particles/cm2. +METHOD (EDE) +DETECTOR (PLATE) Semi-automic device TRICO was used. +ERR-ANALYS (DATA-ERR)Uncertanty of cross-section measurements. + Typical error of the residual range was between 5% and + 10%. Errors of momentum was between 4% and 8%. + The precision of polar and azimuthal angles was between + +-0.05 and 0.1 radians. + These errors increased considerably for very short + tracks of less than 5 microns residual range. +HISTORY (20040909C) +ENDBIB 25 +NOCOMMON 0 0 +ENDSUBENT 28 +SUBENT F0586002 20050623 20050831 F021 +BIB 3 3 +REACTION (6-C-12(A,P+A)5-B-11,,SIG,,AV) +PART-DET (5-B-11) +STATUS (TABLE) Table 1,2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 3 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 33.400 2.7000 127.00 33.000 + 42.900 2.9000 50.000 9.0000 + 50.600 2.6000 47.000 8.0000 +ENDDATA 5 +ENDSUBENT 13 +SUBENT F0586003 20050623 20050831 F021 +BIB 4 5 +REACTION (6-C-12(A,X)3-LI-6,IND,SIG,,AV) +PART-DET (3-LI-6) +FLAG (1.) Outgoing particle - D+2A + (2.) Outgoing particle - A+6Li +STATUS (TABLE) Table 2,3 +ENDBIB 5 +NOCOMMON 0 0 +DATA 5 3 +EN-MEAN EN-RSL DATA DATA-ERR FLAG +MEV MEV MB MB NO-DIM + 42.900 2.9000 1.0000 1.0000 + 50.600 2.6000 9.0000 4.0000 1.0000 + 50.600 2.6000 2.0000 2.0000 +ENDDATA 5 +ENDSUBENT 15 +SUBENT F0586004 20050623 20050831 F021 +BIB 3 3 +REACTION (6-C-12(A,P+3-LI-6)4-BE-9,,SIG,,AV) +PART-DET (3-LI-6) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 5.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586005 20050623 20050831 F021 +BIB 3 3 +REACTION (6-C-12(A,P+2A)3-LI-7,,SIG,,AV) +PART-DET (3-LI-7) +STATUS (TABLE) Table 2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 12.000 4.0000 + 50.600 2.6000 40.000 8.0000 +ENDDATA 4 +ENDSUBENT 12 +SUBENT F0586006 20050623 20050831 F021 +BIB 4 6 +REACTION (6-C-12(A,X)4-BE-9,IND,SIG,,AV) +PART-DET (4-BE-9) +FLAG (1.) Outgoing particle - 3He+A + (2.) Outgoing particle - P+D+A + (3.) Outgoing particle - P+6Li +STATUS (TABLE) Table 2,3 +ENDBIB 6 +NOCOMMON 0 0 +DATA 5 4 +EN-MEAN EN-RSL DATA DATA-ERR FLAG +MEV MEV MB MB NO-DIM + 42.900 2.9000 3.0000 1.0000 + 50.600 2.6000 9.0000 4.0000 1.0000 + 50.600 2.6000 8.0000 3.0000 2.0000 + 50.600 2.6000 6.0000 3.0000 3.0000 +ENDDATA 6 +ENDSUBENT 17 +SUBENT F0586007 20050623 20050831 F021 +BIB 3 3 +REACTION (6-C-12(A,2P+A)4-BE-10,,SIG,,AV) +PART-DET (4-BE-10) +STATUS (TABLE) Table 2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 8.0000 4.0000 + 50.600 2.6000 23.000 6.0000 +ENDDATA 4 +ENDSUBENT 12 +SUBENT F0586008 20050623 20050831 F021 +BIB 3 3 +REACTION (6-C-12(A,D+A)5-B-10,,SIG,,AV) +PART-DET (5-B-10) +STATUS (TABLE) Table 2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 15.000 5.0000 + 50.600 2.6000 29.000 7.0000 +ENDDATA 4 +ENDSUBENT 12 +SUBENT F0586009 20050623 20050831 F021 +BIB 3 3 +REACTION (6-C-12(A,D+T)6-C-11,,SIG,,AV) +PART-DET (6-C-11) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 2.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586010 20050623 20050831 F021 +BIB 4 4 +REACTION (7-N-14(A,3A)3-LI-6,,SIG,,AV) +SAMPLE 14N +PART-DET (3-LI-6) +STATUS (TABLE) Table 1,2,3 +ENDBIB 4 +NOCOMMON 0 0 +DATA 4 3 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 33.400 2.7000 64.000 24.000 + 42.900 2.9000 50.000 8.0000 + 50.600 2.6000 71.000 10.000 +ENDDATA 5 +ENDSUBENT 14 +SUBENT F0586011 20050623 20050831 F021 +BIB 3 3 +REACTION (7-N-14(A,P+3-LI-6)5-B-11,,SIG,,AV) +PART-DET (3-LI-6) +STATUS (TABLE) Table 2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 9.0000 4.0000 + 50.600 2.6000 14.000 4.0000 +ENDDATA 4 +ENDSUBENT 12 +SUBENT F0586012 20050623 20050831 F021 +BIB 3 3 +REACTION (7-N-14(A,D+3-LI-6)5-B-10,,SIG,,AV) +PART-DET (3-LI-6) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 1.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586013 20050623 20050831 F021 +BIB 4 5 +REACTION (7-N-14(A,X)4-BE-9,IND,SIG,,AV) +PART-DET (4-BE-9) +FLAG (1.) Outgoing particle - P+2A + (2.) Outgoing particle - D+7Be +STATUS (TABLE) Table 1,2,3 +ENDBIB 5 +NOCOMMON 0 0 +DATA 5 4 +EN-MEAN EN-RSL DATA DATA-ERR FLAG +MEV MEV MB MB NO-DIM + 33.400 2.7000 96.000 29.000 1.0000 + 42.900 2.9000 54.000 9.0000 1.0000 + 50.600 2.6000 58.000 9.0000 1.0000 + 50.600 2.6000 1.0000 2.0000 +ENDDATA 6 +ENDSUBENT 16 +SUBENT F0586014 20050623 20050831 F021 +BIB 4 8 +REACTION (7-N-14(A,X)5-B-10,IND,SIG,,AV) +PART-DET (5-B-10) +FLAG (1.) Outgoing particle - 2A + (2.) Outgoing particle - P+T+A + (3.) Outgoing particle - P+7Li + (4.) Outgoing particle - D+6Li + (5.) Outgoing particle - 2D+A +STATUS (TABLE) Table 1,2,3 +ENDBIB 8 +NOCOMMON 0 0 +DATA 5 7 +EN-MEAN EN-RSL DATA DATA-ERR FLAG +MEV MEV MB MB NO-DIM + 33.400 2.7000 94.000 29.000 1.0000 + 42.900 2.9000 36.000 7.0000 1.0000 + 50.600 2.6000 18.000 5.0000 1.0000 + 50.600 2.6000 8.0000 3.0000 2.0000 + 50.600 2.6000 5.0000 3.0000 3.0000 + 50.600 2.6000 1.0000 4.0000 + 50.600 2.6000 1.0000 5.0000 +ENDDATA 9 +ENDSUBENT 22 +SUBENT F0586015 20050623 20050831 F021 +BIB 4 6 +REACTION (7-N-14(A,X)5-B-11,IND,SIG,,AV) +PART-DET (5-B-11) +FLAG (1.) Outgoing particle - 3He+A + (2.) Outgoing particle - P+6Li + (3.) Outgoing particle - P+D+A +STATUS (TABLE) Table 1,2,3 +ENDBIB 6 +NOCOMMON 0 0 +DATA 5 8 +EN-MEAN EN-RSL DATA DATA-ERR FLAG +MEV MEV MB MB NO-DIM + 33.400 2.7000 8.0000 1.0000 + 33.400 2.7000 1.0000 2.0000 + 42.900 2.9000 17.000 5.0000 3.0000 + 42.900 2.9000 12.000 4.0000 1.0000 + 42.900 2.9000 9.0000 4.0000 2.0000 + 50.600 2.6000 20.000 5.0000 3.0000 + 50.600 2.6000 13.000 4.0000 1.0000 + 50.600 2.6000 14.000 4.0000 2.0000 +ENDDATA 10 +ENDSUBENT 21 +SUBENT F0586016 20050623 20050831 F021 +BIB 4 5 +REACTION (7-N-14(A,X)6-C-11,IND,SIG,,AV) +PART-DET (6-C-11) +FLAG (1.) Outgoing particle - T+A + (2.) Outgoing particle - P+3He +STATUS (TABLE) Table 1,2,3 +ENDBIB 5 +NOCOMMON 0 0 +DATA 5 4 +EN-MEAN EN-RSL DATA DATA-ERR FLAG +MEV MEV MB MB NO-DIM + 33.400 2.7000 6.0000 1.0000 + 42.900 2.9000 17.000 5.0000 1.0000 + 50.600 2.6000 17.000 5.0000 1.0000 + 50.600 2.6000 7.0000 3.0000 2.0000 +ENDDATA 6 +ENDSUBENT 16 +SUBENT F0586017 20050623 20050831 F021 +BIB 3 3 +REACTION (7-N-14(A,P+2-HE-6)6-C-11,,SIG,,AV) +PART-DET (2-HE-6) +STATUS (TABLE) Table 2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 1.0000 + 50.600 2.6000 7.0000 3.0000 +ENDDATA 4 +ENDSUBENT 12 +SUBENT F0586018 20050623 20050831 F021 +BIB 3 3 +REACTION (7-N-14(A,A+3-LI-7)4-BE-7,,SIG,,AV) +PART-DET (3-LI-7) +STATUS (TABLE) Table 2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 2.0000 + 50.600 2.6000 5.0000 3.0000 +ENDDATA 4 +ENDSUBENT 12 +SUBENT F0586019 20050623 20050831 F021 +BIB 3 3 +REACTION (7-N-14(A,P+3-LI-7)5-B-10,,SIG,,AV) +PART-DET (3-LI-7) +STATUS (TABLE) Table 2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 1.0000 + 50.600 2.6000 5.0000 3.0000 +ENDDATA 4 +ENDSUBENT 12 +SUBENT F0586020 20050623 20050831 F021 +BIB 4 5 +REACTION (7-N-14(A,X)3-LI-7,IND,SIG,,AV) +PART-DET (3-LI-7) +FLAG (1.) Outgoing particle - 3He+2A + (2.) Outgoing particle - P+A+6Li +STATUS (TABLE) Table 3 +ENDBIB 5 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA FLAG +MEV MEV MB NO-DIM + 50.600 2.6000 3.0000 1.0000 + 50.600 2.6000 1.0000 2.0000 +ENDDATA 4 +ENDSUBENT 14 +SUBENT F0586021 20050623 20050831 F021 +BIB 4 5 +REACTION (7-N-14(A,X)4-BE-7,IND,SIG,,AV) +PART-DET (4-BE-7) +FLAG (1.) Outgoing particle - T+2A + (2.) Outgoing particle - A+7Li +STATUS (TABLE) Table 2,3 +ENDBIB 5 +NOCOMMON 0 0 +DATA 5 3 +EN-MEAN EN-RSL DATA DATA-ERR FLAG +MEV MEV MB MB NO-DIM + 42.900 2.9000 2.0000 2.0000 + 50.600 2.6000 8.0000 3.0000 1.0000 + 50.600 2.6000 5.0000 3.0000 2.0000 +ENDDATA 5 +ENDSUBENT 15 +SUBENT F0586022 20050623 20050831 F021 +BIB 3 3 +REACTION (7-N-14(A,D+4-BE-7)4-BE-9,,SIG,,AV) +PART-DET (4-BE-7) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 1.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586023 20050623 20050831 F021 +BIB 3 3 +REACTION (7-N-14(A,P+4-BE-7)4-BE-10,,SIG,,AV) +PART-DET (4-BE-7) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 1 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 50.600 2.6000 6.0000 3.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586024 20050623 20050831 F021 +BIB 4 5 +REACTION (7-N-14(A,X)4-BE-10,IND,SIG,,AV) +PART-DET (4-BE-10) +FLAG (1.) Outgoing particle - P+7BE + (2.) Outgoing particle - P+3He+A +STATUS (TABLE) Table 2,3 +ENDBIB 5 +NOCOMMON 0 0 +DATA 5 3 +EN-MEAN EN-RSL DATA DATA-ERR FLAG +MEV MEV MB MB NO-DIM + 42.900 2.9000 1.0000 1.0000 + 50.600 2.6000 6.0000 3.0000 1.0000 + 50.600 2.6000 4.0000 2.0000 +ENDDATA 5 +ENDSUBENT 15 +SUBENT F0586025 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,P+3-LI-7)6-C-12,,SIG,,AV) +PART-DET (3-LI-7) +STATUS (TABLE) Table 1,2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 3 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 33.400 2.7000 8.0000 + 42.900 2.9000 22.000 7.0000 + 50.600 2.6000 25.000 8.0000 +ENDDATA 5 +ENDSUBENT 13 +SUBENT F0586026 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,P+2A)5-B-11,,SIG,,AV) +PART-DET (5-B-11) +STATUS (TABLE) Table 1,2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 3 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 33.400 2.7000 3.0000 + 42.900 2.9000 17.000 6.0000 + 50.600 2.6000 26.000 8.0000 +ENDDATA 5 +ENDSUBENT 13 +SUBENT F0586027 20050623 20050831 F021 +BIB 2 2 +REACTION (8-O-16(A,P+2-HE-6)7-N-13,,SIG,,AV) +STATUS (TABLE) Table 2,3 +ENDBIB 2 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 2.0000 + 50.600 2.6000 10.000 5.0000 +ENDDATA 4 +ENDSUBENT 11 +SUBENT F0586028 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,2P+2-HE-6)6-C-12,,SIG,,AV) +PART-DET (2-HE-6) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 3.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586029 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,P+3-LI-6)6-C-13,,SIG,,AV) +PART-DET (3-LI-6) +STATUS (TABLE) Table 2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 10.000 5.0000 + 50.600 2.6000 12.000 5.0000 +ENDDATA 4 +ENDSUBENT 12 +SUBENT F0586030 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,D+3-LI-6)6-C-12,,SIG,,AV) +PART-DET (3-LI-6) +STATUS (TABLE) Table 2,3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA DATA-ERR +MEV MEV MB MB + 42.900 2.9000 4.0000 + 50.600 2.6000 8.0000 4.0000 +ENDDATA 4 +ENDSUBENT 12 +SUBENT F0586031 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,A+3-LI-6)5-B-10,,SIG,,AV) +PART-DET (3-LI-6) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 2.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586032 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,A+4-BE-7)4-BE-9,,SIG,,AV) +PART-DET (4-BE-7) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 4.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586033 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,D+4-BE-7)5-B-11,,SIG,,AV) +PART-DET (4-BE-7) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 1.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586034 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,P+4-BE-7)5-B-12,,SIG,,AV) +PART-DET (4-BE-7) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 1.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586035 20050623 20050831 F021 +BIB 4 5 +REACTION (8-O-16(A,X)4-BE-9,IND,SIG,,AV) +PART-DET (4-BE-9) +FLAG (1.) Outgoing particle - A+7BE + (2.) Outgoing particle - 3HE+A +STATUS (TABLE) Table 3 +ENDBIB 5 +NOCOMMON 0 0 +DATA 4 2 +EN-MEAN EN-RSL DATA FLAG +MEV MEV MB NO-DIM + 50.600 2.6000 4.0000 1.0000 + 50.600 2.6000 1.0000 2.0000 +ENDDATA 4 +ENDSUBENT 14 +SUBENT F0586036 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,P+4-BE-9)5-B-10,,SIG,,AV) +PART-DET (4-BE-9) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 3.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586037 20050623 20050831 F021 +BIB 3 3 +REACTION (8-O-16(A,2P+2A)4-BE-10,,SIG,,AV) +PART-DET (4-BE-10) +STATUS (TABLE) Table 3 +ENDBIB 3 +NOCOMMON 0 0 +DATA 3 1 +EN-MEAN EN-RSL DATA +MEV MEV MB + 50.600 2.6000 3.0000 +ENDDATA 3 +ENDSUBENT 11 +SUBENT F0586038 20050623 20050831 F021 +BIB 4 6 +REACTION (8-O-16(A,X)5-B-10,IND,SIG,,AV) +PART-DET (5-B-10) +FLAG (1.) Outgoing particle - D+2A + (2.) Outgoing particle - P+4BE + (3.) Outgoing particle - A+6LI +STATUS (TABLE) Table 3 +ENDBIB 6 +NOCOMMON 0 0 +DATA 4 3 +EN-MEAN EN-RSL DATA FLAG +MEV MEV MB NO-DIM + 50.600 2.6000 3.0000 1.0000 + 50.600 2.6000 3.0000 2.0000 + 50.600 2.6000 2.0000 3.0000 +ENDDATA 5 +ENDSUBENT 16 +ENDENTRY 38 diff --git a/exforall/F05/F0595.x4 b/exforall/F05/F0595.x4 new file mode 100644 index 000000000..ef7bb3b0f --- /dev/null +++ b/exforall/F05/F0595.x4 @@ -0,0 +1,706 @@ +ENTRY F0595 20050609 20050831 F022 +SUBENT F0595001 20050609 20050831 F022 +BIB 8 11 +TITLE The optical model and distorted-wave analysis of + cross-sections for the scattering of the 24-28 MeV + alpha particles from 28Si. +AUTHOR (L.Jarczyk,B.Maciuk,M.Siemaszko,W.Zipper) +INSTITUTE (3POLPOL) +REFERENCE (J,APP/B,7,531,1976) +FACILITY (CYCLO) U-120 +COMMENT No infromation about experiment technique. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error +HISTORY (20031104C) +ENDBIB 11 +NOCOMMON 0 0 +ENDSUBENT 14 +SUBENT F0595002 20050609 20050831 F022 +BIB 3 3 +REACTION (14-SI-28(A,EL)14-SI-28,,DA,,RTH) +ANALYSIS (WSP) +STATUS (CURVE)Fig.3 +ENDBIB 3 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.3 0.1 +ENDCOMMON 3 +DATA 3 369 +EN ANG-CM DATA-CM +MEV ADEG NO-DIM + 24.000 25.090 0.13660 + 24.000 26.450 0.63660E-01 + 24.000 29.130 0.13820 + 24.000 31.520 0.27220 + 24.000 34.210 0.26930 + 24.000 36.760 0.90840E-01 + 24.000 39.020 0.21720E-01 + 24.000 41.270 0.13970E-01 + 24.000 44.090 0.90870E-01 + 24.000 46.330 0.21490 + 24.000 48.720 0.26660 + 24.000 51.560 0.26660 + 24.000 53.810 0.15400 + 24.000 56.210 0.65130E-01 + 24.000 58.310 0.27540E-01 + 24.000 61.150 0.51970E-01 + 24.000 63.530 0.10350 + 24.000 66.070 0.12830 + 24.000 69.060 0.12700 + 24.000 71.160 0.92960E-01 + 24.000 73.560 0.48230E-01 + 24.000 76.110 0.21990E-01 + 24.000 78.650 0.22470E-01 + 24.000 81.040 0.30700E-01 + 24.000 83.730 0.54310E-01 + 24.000 86.270 0.73410E-01 + 24.000 88.660 0.92030E-01 + 24.000 91.650 0.91060E-01 + 24.000 93.450 0.73440E-01 + 24.000 96.140 0.34580E-01 + 24.000 98.390 0.27300E-01 + 24.000 101.10 0.48810E-01 + 24.000 103.50 0.10590 + 24.000 106.20 0.22500 + 24.000 108.40 0.18340 + 24.000 110.60 0.22020 + 24.000 113.20 0.14790 + 24.000 115.40 0.68170E-01 + 24.000 118.30 0.28830E-01 + 24.000 121.00 0.55580E-01 + 24.000 122.90 0.13290 + 24.000 125.70 0.27330 + 24.000 128.10 0.29790 + 24.000 130.50 0.28540 + 24.000 132.90 0.20670 + 24.000 135.20 0.10840 + 24.000 137.70 0.69730E-01 + 24.000 140.30 0.64670E-01 + 24.000 142.80 0.16850 + 24.000 144.90 0.28550 + 24.000 147.70 0.40730 + 24.000 150.30 0.31810 + 24.000 152.70 0.18570 + 24.000 155.20 0.56880E-01 + 24.000 157.80 0.32510E-01 + 24.000 160.10 0.18780 + 24.000 162.50 0.71320 + 24.000 165.10 1.4830 + 24.000 167.60 1.8990 + 24.000 171.60 2.4590 + 24.000 175.10 2.6810 + 25.000 24.030 0.19940 + 25.000 25.080 0.13610 + 25.000 26.440 0.75130E-01 + 25.000 28.830 0.95920E-01 + 25.000 31.210 0.24150 + 25.000 33.900 0.30180 + 25.000 36.740 0.25210 + 25.000 39.300 0.94990E-01 + 25.000 41.880 0.90100E-02 + 25.000 44.090 0.68390E-01 + 25.000 46.160 0.21740 + 25.000 48.850 0.31200 + 25.000 51.690 0.27770 + 25.000 53.940 0.19570 + 25.000 56.200 0.76120E-01 + 25.000 58.910 0.28990E-01 + 25.000 61.140 0.76150E-01 + 25.000 63.970 0.14700 + 25.000 66.360 0.16710 + 25.000 68.900 0.14710 + 25.000 71.460 0.70760E-01 + 25.000 73.860 0.29330E-01 + 25.000 76.560 0.30290E-01 + 25.000 78.640 0.57260E-01 + 25.000 81.330 0.64360E-01 + 25.000 83.870 0.63700E-01 + 25.000 86.560 0.65770E-01 + 25.000 88.800 0.87610E-01 + 25.000 91.340 0.87630E-01 + 25.000 93.580 0.16390 + 25.000 96.420 0.13550 + 25.000 98.370 0.96470E-01 + 25.000 106.40 0.89620E-01 + 25.000 108.50 0.21400 + 25.000 110.90 0.26180 + 25.000 113.60 0.33070 + 25.000 116.40 0.25640 + 25.000 118.70 0.19260 + 25.000 120.90 0.10300 + 25.000 124.00 0.25120E-01 + 25.000 125.90 0.43630E-01 + 25.000 128.10 0.12480 + 25.000 130.40 0.18480 + 25.000 133.20 0.25140 + 25.000 135.70 0.30440 + 25.000 138.40 0.21680 + 25.000 140.50 0.16280 + 25.000 143.10 0.13890 + 25.000 145.80 0.15610 + 25.000 148.00 0.20140 + 25.000 150.60 0.26830 + 25.000 153.40 0.26840 + 25.000 155.50 0.17940 + 25.000 158.10 0.77580E-01 + 25.000 160.80 0.29230E-01 + 25.000 163.00 0.13190 + 25.000 165.40 0.38530 + 25.000 167.60 0.71320 + 25.000 170.60 1.2390 + 25.000 173.00 1.4530 + 25.000 175.80 1.5650 + 26.000 27.090 0.28550 + 26.000 29.530 0.17600 + 26.000 31.850 0.55830E-01 + 26.000 34.390 0.13920 + 26.000 37.220 0.35120 + 26.000 39.620 0.40200 + 26.000 41.760 0.25070 + 26.000 44.210 0.70120E-01 + 26.000 46.430 0.12260E-01 + 26.000 49.210 0.12510 + 26.000 51.620 0.35000 + 26.000 54.160 0.39590 + 26.000 56.500 0.32140 + 26.000 58.600 0.15760 + 26.000 61.050 0.44080E-01 + 26.000 63.460 0.22110E-01 + 26.000 66.070 0.88200E-01 + 26.000 68.680 0.14070 + 26.000 71.220 0.15740 + 26.000 73.530 0.11010 + 26.000 76.030 0.39150E-01 + 26.000 78.180 0.10700E-01 + 26.000 80.920 0.38950E-01 + 26.000 83.440 0.86640E-01 + 26.000 86.000 0.11120 + 26.000 88.410 0.13630 + 26.000 90.790 0.13910 + 26.000 93.460 0.13870 + 26.000 96.120 0.13060 + 26.000 98.340 0.12450 + 26.000 101.00 0.12560 + 26.000 103.60 0.97350E-01 + 26.000 106.00 0.86600E-01 + 26.000 108.70 0.12320 + 26.000 111.30 0.15630 + 26.000 113.90 0.22230 + 26.000 116.30 0.27880 + 26.000 118.80 0.24520 + 26.000 121.40 0.17540 + 26.000 123.60 0.12270 + 26.000 125.60 0.43170E-01 + 26.000 128.40 0.43540E-01 + 26.000 131.20 0.15310 + 26.000 133.70 0.30710 + 26.000 136.10 0.43200 + 26.000 138.60 0.43580 + 26.000 140.90 0.30830 + 26.000 143.50 0.17540 + 26.000 145.80 0.96460E-01 + 26.000 148.40 0.12380 + 26.000 151.00 0.27210 + 26.000 153.50 0.48130 + 26.000 156.10 0.67690 + 26.000 158.90 0.53680 + 26.000 161.00 0.30550 + 26.000 163.10 0.75340E-01 + 26.000 165.90 0.12020 + 26.000 168.50 0.60280 + 26.000 171.20 1.7450 + 26.000 174.00 3.1200 + 26.000 176.50 4.8100 + 26.000 179.00 5.5680 + 26.000 181.50 5.6170 + 26.500 27.050 0.41330E-01 + 26.500 29.420 0.16710 + 26.500 32.260 0.26140 + 26.500 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28.000 119.10 0.18190E-01 + 28.000 121.70 0.31940E-01 + 28.000 124.40 0.61380E-01 + 28.000 127.10 0.85100E-01 + 28.000 129.40 0.10190 + 28.000 132.10 0.98540E-01 + 28.000 134.40 0.76070E-01 + 28.000 136.80 0.57420E-01 + 28.000 139.90 0.36610E-01 + 28.000 142.00 0.24970E-01 + 28.000 144.70 0.17610E-01 + 28.000 146.70 0.22830E-01 + 28.000 149.50 0.40540E-01 + 28.000 151.90 0.78790E-01 + 28.000 154.60 0.10210 + 28.000 157.00 0.11170 + 28.000 159.80 0.88230E-01 + 28.000 161.90 0.50820E-01 + 28.000 164.30 0.36260E-01 + 28.000 166.70 0.41980E-01 + 28.000 169.40 0.10940 + 28.000 172.50 0.16040 + 28.000 175.00 0.20550 +ENDDATA 371 +ENDSUBENT 383 +SUBENT F0595003 20050609 20050831 F022 +BIB 4 4 +REACTION (14-SI-28(A,INL)14-SI-28,PAR,DA) +ANALYSIS Distorted wave theory. +ERR-ANALYS (DATA-ERR) Errors from the graphic bars +STATUS (CURVE)Fig.8 +ENDBIB 4 +COMMON 3 3 +E-LVL ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT +1.78 0.6 0.15 +ENDCOMMON 3 +DATA 4 286 +EN ANG-CM DATA-CM DATA-ERR +MEV ADEG MB/SR MB/SR 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140.60 1.0370 0.65280E-01 + 26.000 142.60 0.73950 0.59750E-01 + 26.000 145.20 0.45640 0.31430E-01 + 26.000 147.10 0.47980 0.44550E-01 + 26.000 149.20 0.41540 0.23700E-01 + 26.000 151.50 0.63690 0.40090E-01 + 26.000 153.60 0.71570 0.45050E-01 + 26.000 155.50 0.84540 0.43290E-01 + 26.000 157.60 1.1280 0.77680E-01 + 26.000 159.50 1.1100 0.63320E-01 + 26.000 161.80 1.1930 + 26.000 164.00 1.1160 + 26.000 166.30 1.1480 + 26.000 168.40 1.0210 + 26.000 170.10 0.93480 + 26.000 172.70 0.81380 + 26.000 174.80 0.84610 + 26.000 176.00 1.1480 0.99650E-01 + 26.000 177.30 1.6650 0.95040E-01 + 27.000 28.310 7.3670 0.67420 + 27.000 31.190 11.800 0.93970 + 27.000 33.670 17.030 1.6610 + 27.000 36.490 11.490 0.71380 + 27.000 39.090 8.5050 0.52790 + 27.000 47.940 3.3210 0.34400 + 27.000 61.510 0.97580 + 27.000 64.230 1.2020 + 27.000 67.110 1.9250 + 27.000 69.820 2.4770 + 27.000 72.370 2.3590 + 27.000 75.430 1.3500 + 27.000 78.490 0.81170 + 27.000 83.350 0.89630 + 27.000 86.060 1.1040 + 27.000 88.600 1.1660 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0.68110 + 28.000 38.760 3.2100 0.25560 + 28.000 41.840 2.2870 0.23680 + 28.000 47.940 5.0650 0.58600 + 28.000 64.090 2.2360 + 28.000 67.040 2.4020 + 28.000 70.230 2.2640 + 28.000 72.450 1.6670 + 28.000 75.560 1.0420 + 28.000 78.280 0.59630 + 28.000 80.990 0.68410 0.38490E-01 + 28.000 83.430 0.96110 + 28.000 86.080 1.3280 0.67070E-01 + 28.000 88.810 1.4190 + 28.000 91.030 1.0560 0.59390E-01 + 28.000 93.770 0.55110 0.24670E-01 + 28.000 96.190 0.41480 0.30550E-01 + 28.000 99.010 0.66450 0.33530E-01 + 28.000 101.20 1.2070 + 28.000 103.60 1.4870 + 28.000 106.00 1.3710 + 28.000 108.80 1.1450 + 28.000 113.70 0.51540 + 28.000 115.80 0.58160 + 28.000 118.00 0.74440 + 28.000 120.80 0.78240 + 28.000 123.00 0.62200 + 28.000 125.00 0.45300 0.17670E-01 + 28.000 127.40 0.29730 0.21930E-01 + 28.000 129.80 0.30080 + 28.000 131.90 0.51740 0.35100E-01 + 28.000 134.40 0.70330 + 28.000 136.50 0.65890 + 28.000 138.90 0.52380 + 28.000 141.60 0.36120 + 28.000 143.50 0.33470 + 28.000 145.90 0.27050 0.15210E-01 + 28.000 148.00 0.28740 + 28.000 149.90 0.30370 0.17070E-01 + 28.000 152.50 0.25360 0.11340E-01 + 28.000 154.80 0.25240 0.18600E-01 + 28.000 156.60 0.42470 0.23890E-01 + 28.000 158.30 0.65830 + 28.000 160.80 0.95050 + 28.000 162.90 0.99890 + 28.000 164.80 0.95130 + 28.000 167.50 0.99990 + 28.000 169.10 1.3220 + 28.000 170.80 0.88220 + 28.000 170.80 0.83520 + 28.000 171.40 1.7390 + 28.000 171.80 0.92690 + 28.000 172.30 0.77380 + 28.000 173.10 2.8640 + 28.000 174.70 1.0070 + 28.000 175.60 4.1570 + 28.000 177.30 6.4790 +ENDDATA 288 +ENDSUBENT 301 +ENDENTRY 3 diff --git a/exforall/F05/F0597.x4 b/exforall/F05/F0597.x4 new file mode 100644 index 000000000..59e44db7a --- /dev/null +++ b/exforall/F05/F0597.x4 @@ -0,0 +1,501 @@ +ENTRY F0597 20050623 20050831 F022 +SUBENT F0597001 20050623 20050831 F022 +BIB 11 22 +TITLE Study of alpha-gamma correlation in the reaction plane + and the mechanism of the 28Si(a,ag)28Si reaction. +AUTHOR (K.Bodek,A.Budzanowski,L.Jarczyk,R.Kulessa,J.Majewski, + A.Strzalkowski,W.Walus,G.Willim) +INSTITUTE (3POLUJK,3POLIFJ) +REFERENCE (J,APP/B,13,767,1982) +FACILITY (CYCLO,3POLIFJ) U-120 cyclotron. +INC-SOURCE The beam with intensity 60 nA. +DETECTOR (SIBAR) A silicon surface barrier detector located in + the scattering chamber was used to detect alpha + particles. + (NAICR) Gamma rays were detected with 3*3 inches + 12S8/E-O Harshaw NaI(Ti) scintillation detector. Its + angular resolution was +-12 deg. The range of angles + accessible to the gamma detector was from 40 to 140 deg +METHOD (COINC) + (BCINT) +SAMPLE Self supporting silicon target of the thickness 150 + mu-g/cm2. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error +HISTORY (20031119C) +ENDBIB 22 +COMMON 1 3 +ANG-RSL +ADEG + 2. +ENDCOMMON 3 +ENDSUBENT 29 +SUBENT F0597002 20050623 20050831 F022 +BIB 5 10 +REACTION (14-SI-28(A,INL)14-SI-28,PAR,DA/DA,A/G,REL) + ANG1 is an angle of alpha particles detection. + ANG2 is an angle of gamma particles detection. +COMMENT The normalized correlation functions were calculated + from the measured number of coincidences Nc for the + random coincidences and the number of counts in the + corresponding peaks in single spectra N. +EN-SEC (E-LVL,14-SI-28) +ERR-ANALYS (DATA-ERR) Errors from the graphic bars +STATUS (CURVE)FIG.6,7,8,9 +ENDBIB 10 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG ARB-UNITS + 0.02 0.001 +ENDCOMMON 3 +DATA 6 216 +E-LVL EN ANG1 ANG2 DATA DATA-ERR +MEV MEV ADEG ADEG ARB-UNITS ARB-UNITS + 1.7800 27.500 31.400 39.134 0.54280 0.46832E-01 + 1.7800 27.500 31.400 39.470 0.48495 0.57851E-01 + 1.7800 27.500 31.400 49.333 0.84589 0.46832E-01 + 1.7800 27.500 31.400 59.033 0.98092 0.60606E-01 + 1.7800 27.500 31.400 69.067 1.1132 0.52342E-01 + 1.7800 27.500 31.400 78.610 0.75238 0.46832E-01 + 1.7800 27.500 31.400 89.320 0.54582 0.44077E-01 + 1.7800 27.500 31.400 99.363 0.26213 0.57851E-01 + 1.7800 27.500 31.400 108.56 0.20433 0.46832E-01 + 1.7800 27.500 31.400 118.93 0.34488 0.49587E-01 + 1.7800 27.500 31.400 128.30 0.60388 0.55096E-01 + 1.7800 27.500 31.400 138.50 0.89870 0.57851E-01 + 1.7800 27.500 45.500 50.188 0.28446 0.35714E-01 + 1.7800 27.500 45.500 59.752 0.40263 0.49451E-01 + 1.7800 27.500 45.500 59.753 0.39027 0.56319E-01 + 1.7800 27.500 45.500 69.482 0.54141 0.32967E-01 + 1.7800 27.500 45.500 78.882 0.59639 0.41209E-01 + 1.7800 27.500 45.500 89.127 0.56072 0.43956E-01 + 1.7800 27.500 45.500 99.546 0.41790 0.49451E-01 + 1.7800 27.500 45.500 109.46 0.28470 0.39835E-01 + 1.7800 27.500 45.500 119.20 0.21881 0.31593E-01 + 1.7800 27.500 45.500 129.62 0.17901 0.34341E-01 + 1.7800 27.500 45.500 139.85 0.32741 0.39835E-01 + 1.7800 27.500 52.100 40.601 0.33150 0.77348E-01 + 1.7800 27.500 52.100 50.921 0.66299 0.88398E-01 + 1.7800 27.500 52.100 60.902 1.0332 0.91160E-01 + 1.7800 27.500 52.100 70.375 1.2542 0.10773 + 1.7800 27.500 52.100 80.357 1.0221 0.99447E-01 + 1.7800 27.500 52.100 90.000 0.78730 0.82873E-01 + 1.7800 27.500 52.100 99.981 0.40609 0.71823E-01 + 1.7800 27.500 52.100 109.79 0.24035 0.69061E-01 + 1.7800 27.500 52.100 119.61 0.30388 0.58011E-01 + 1.7800 27.500 52.100 129.59 0.49449 0.71823E-01 + 1.7800 27.500 52.100 139.40 0.71825 0.10773 + 1.7800 27.500 72.700 43.802 0.39386 0.53073E-01 + 1.7800 27.500 72.700 48.593 0.54749 0.55866E-01 + 1.7800 27.500 72.700 58.517 0.78492 0.67039E-01 + 1.7800 27.500 72.700 64.334 0.94134 0.69832E-01 + 1.7800 27.500 72.700 69.125 1.2458 0.92179E-01 + 1.7800 27.500 72.700 79.049 1.3799 0.92179E-01 + 1.7800 27.500 72.700 84.353 1.5587 0.10615 + 1.7800 27.500 72.700 89.486 1.2095 0.72626E-01 + 1.7800 27.500 72.700 99.068 0.98325 0.83799E-01 + 1.7800 27.500 72.700 103.69 0.67040 0.81006E-01 + 1.7800 27.500 72.700 107.79 0.49721 0.53073E-01 + 1.7800 27.500 72.700 118.40 0.20113 0.53073E-01 + 1.7800 27.500 72.700 123.19 0.23185 0.47486E-01 + 1.7800 27.500 72.700 128.16 0.29051 0.41899E-01 + 1.7800 27.500 72.700 133.12 0.35476 0.61453E-01 + 1.7800 27.500 72.700 138.08 0.44414 0.55866E-01 + 4.6200 24.000 167.40 58.641 1.3981 0.22761 + 4.6200 24.000 167.40 78.176 1.0128 0.12506 + 4.6200 24.000 167.40 98.714 0.95009 0.13506 + 4.6200 24.000 167.40 118.77 0.94242 0.12256 + 4.6200 24.000 167.40 138.60 1.2749 0.14257 + 4.6200 26.000 162.30 37.148 1.0963 0.89370E-01 + 4.6200 26.000 162.30 47.475 1.1062 0.10427 + 4.6200 26.000 162.30 57.803 1.1310 0.91853E-01 + 4.6200 26.000 162.30 77.718 1.0044 0.81923E-01 + 4.6200 26.000 162.30 97.878 0.88024 0.69510E-01 + 4.6200 26.000 162.30 108.45 0.76603 0.79440E-01 + 4.6200 26.000 162.30 118.53 0.81567 0.49650E-01 + 4.6200 26.000 162.30 128.86 0.84793 0.69510E-01 + 4.6200 26.000 162.30 138.20 0.90998 0.81923E-01 + 4.6200 26.000 167.40 37.888 1.1214 0.84615E-01 + 4.6200 26.000 167.40 48.073 1.0417 0.10204 + 4.6200 26.000 167.40 57.778 1.0864 0.16674 + 4.6200 26.000 167.40 78.394 1.0042 0.94570E-01 + 4.6200 26.000 167.40 98.282 0.88221 0.67195E-01 + 4.6200 26.000 167.40 108.71 0.86226 0.67195E-01 + 4.6200 26.000 167.40 118.42 0.89209 0.62217E-01 + 4.6200 26.000 167.40 128.61 0.93435 0.69683E-01 + 4.6200 26.000 167.40 138.80 1.0587 0.77150E-01 + 4.6200 27.000 161.20 37.902 1.2231 0.82827E-01 + 4.6200 27.000 161.20 48.578 1.1202 0.77807E-01 + 4.6200 27.000 161.20 58.746 1.0172 0.62748E-01 + 4.6200 27.000 161.20 68.916 1.0574 0.65258E-01 + 4.6200 27.000 161.20 79.592 0.94944 0.60238E-01 + 4.6200 27.000 161.20 90.014 0.84401 0.67768E-01 + 4.6200 27.000 161.20 100.44 0.78626 0.57728E-01 + 4.6200 27.000 161.20 110.86 0.80633 0.67768E-01 + 4.6200 27.000 161.20 121.03 0.75862 0.60238E-01 + 4.6200 27.000 161.20 131.71 0.79374 0.55218E-01 + 4.6200 27.000 161.20 141.37 0.94181 0.62748E-01 + 4.6200 27.000 165.20 39.192 1.1287 0.56931E-01 + 4.6200 27.000 165.20 49.168 1.2177 0.56931E-01 + 4.6200 27.000 165.20 59.141 1.2078 0.54455E-01 + 4.6200 27.000 165.20 69.354 1.1162 0.71782E-01 + 4.6200 27.000 165.20 79.325 1.0345 0.61881E-01 + 4.6200 27.000 165.20 89.054 1.0221 0.59406E-01 + 4.6200 27.000 165.20 99.268 0.94038 0.64356E-01 + 4.6200 27.000 165.20 109.48 0.83639 0.51980E-01 + 4.6200 27.000 165.20 119.45 0.82151 0.37129E-01 + 4.6200 27.000 165.20 129.67 0.89574 0.47030E-01 + 4.6200 27.000 165.20 139.16 1.0219 0.54455E-01 + 4.6200 27.000 167.40 38.679 1.2155 0.63162E-01 + 4.6200 27.000 167.40 48.243 1.2054 0.58109E-01 + 4.6200 27.000 167.40 58.053 1.2862 0.58109E-01 + 4.6200 27.000 167.40 68.596 1.1548 0.68215E-01 + 4.6200 27.000 167.40 78.895 1.0563 0.65689E-01 + 4.6200 27.000 167.40 88.948 0.95772 0.63162E-01 + 4.6200 27.000 167.40 99.247 0.83644 0.58109E-01 + 4.6200 27.000 167.40 109.79 0.86421 0.55583E-01 + 4.6200 27.000 167.40 119.11 0.84399 0.55583E-01 + 4.6200 27.000 167.40 129.41 0.82882 0.65689E-01 + 4.6200 27.000 167.40 139.47 1.1143 0.60636E-01 + 6.2800 24.000 167.50 57.807 1.2442 0.22487 + 6.2800 24.000 167.50 78.708 0.67461 0.13742 + 6.2800 24.000 167.50 98.104 0.53975 0.17490 + 6.2800 24.000 167.50 118.98 0.72471 0.18240 + 6.2800 24.000 167.50 138.61 1.1545 0.24486 + 6.2800 26.000 162.40 38.272 1.2786 0.21391 + 6.2800 26.000 162.40 48.354 1.1915 0.25869 + 6.2800 26.000 162.40 58.436 1.1169 0.19899 + 6.2800 26.000 162.40 78.600 1.0746 0.14427 + 6.2800 26.000 162.40 99.012 0.80601 0.13681 + 6.2800 26.000 162.40 109.09 0.66922 0.11939 + 6.2800 26.000 162.40 119.67 0.56973 0.10944 + 6.2800 26.000 162.40 128.77 0.62446 0.11193 + 6.2800 26.000 162.40 139.09 0.72893 0.15670 + 6.2800 26.000 167.50 38.606 1.1845 0.24153 + 6.2800 26.000 167.50 48.934 1.2965 0.35109 + 6.2800 26.000 167.50 59.262 0.97783 0.16932 + 6.2800 26.000 167.50 79.180 0.92305 0.16683 + 6.2800 26.000 167.50 99.344 0.48980 0.92129E-01 + 6.2800 26.000 167.50 109.18 0.61430 0.10707 + 6.2800 26.000 167.50 119.51 0.56450 0.89639E-01 + 6.2800 26.000 167.50 129.10 0.83093 0.11205 + 6.2800 26.000 167.50 139.18 0.94048 0.15189 + 6.2800 27.000 161.20 38.456 1.2935 0.18528 + 6.2800 27.000 161.20 48.023 1.2022 0.19516 + 6.2800 27.000 161.20 58.321 1.2541 0.20504 + 6.2800 27.000 161.20 68.127 1.3307 0.17292 + 6.2800 27.000 161.20 78.187 1.1578 0.15069 + 6.2800 27.000 161.20 88.248 0.97999 0.13093 + 6.2800 27.000 161.20 98.305 0.90839 0.12846 + 6.2800 27.000 161.20 108.36 0.92325 0.14822 + 6.2800 27.000 161.20 118.42 0.67378 0.13093 + 6.2800 27.000 161.20 128.73 0.56018 0.12846 + 6.2800 27.000 161.20 139.02 0.75538 0.12846 + 6.2800 27.000 165.40 38.151 1.3870 0.16625 + 6.2800 27.000 165.40 48.692 1.2902 0.15136 + 6.2800 27.000 165.40 58.497 1.1810 0.16873 + 6.2800 27.000 165.40 78.356 1.0891 0.14392 + 6.2800 27.000 165.40 98.937 0.64234 0.10918 + 6.2800 27.000 165.40 119.05 0.69188 0.12903 + 6.2800 27.000 165.40 129.10 0.69184 0.11662 + 6.2800 27.000 165.40 138.92 0.83571 0.12655 + 6.2800 27.000 167.50 37.790 1.2779 0.21165 + 6.2800 27.000 167.50 47.735 1.3302 0.20169 + 6.2800 27.000 167.50 58.177 1.0712 0.19920 + 6.2800 27.000 167.50 67.873 1.1036 0.21912 + 6.2800 27.000 167.50 78.315 0.86454 0.19422 + 6.2800 27.000 167.50 88.508 0.76494 0.18426 + 6.2800 27.000 167.50 98.204 0.65787 0.16185 + 6.2800 27.000 167.50 108.90 0.65289 0.15687 + 6.2800 27.000 167.50 118.09 0.64293 0.17928 + 6.2800 27.000 167.50 128.54 0.81723 0.18675 + 6.2800 27.000 167.50 138.48 1.1509 0.23157 + 7.3800 27.000 161.30 39.397 1.3091 0.20916 + 7.3800 27.000 161.30 40.179 1.2100 0.25750 + 7.3800 27.000 161.30 49.323 1.0750 0.19671 + 7.3800 27.000 161.30 49.796 1.1750 0.27000 + 7.3800 27.000 161.30 59.241 1.0801 0.18177 + 7.3800 27.000 161.30 60.396 1.3700 0.27250 + 7.3800 27.000 161.30 68.921 0.99544 0.18426 + 7.3800 27.000 161.30 79.082 0.96559 0.15936 + 7.3800 27.000 161.30 80.369 1.3351 0.28500 + 7.3800 27.000 161.30 89.245 0.89093 0.14940 + 7.3800 27.000 161.30 89.742 1.0276 0.23000 + 7.3800 27.000 161.30 98.924 0.80630 0.12948 + 7.3800 27.000 161.30 100.34 1.0501 0.23000 + 7.3800 27.000 161.30 108.84 0.85613 0.15687 + 7.3800 27.000 161.30 109.71 1.0651 0.22250 + 7.3800 27.000 161.30 118.52 0.72171 0.15438 + 7.3800 27.000 161.30 120.07 1.0276 0.22250 + 7.3800 27.000 161.30 128.45 0.51756 0.13695 + 7.3800 27.000 161.30 130.18 1.0401 0.24500 + 7.3800 27.000 161.30 138.60 0.60724 0.14193 + 7.3800 27.000 161.30 141.03 1.1126 0.23000 + 7.3800 27.000 165.50 39.125 1.1192 0.15136 + 7.3800 27.000 165.50 39.224 1.5255 0.26757 + 7.3800 27.000 165.50 49.090 1.4685 0.26757 + 7.3800 27.000 165.50 49.342 1.0869 0.13399 + 7.3800 27.000 165.50 59.197 1.4164 0.24279 + 7.3800 27.000 165.50 59.310 1.2334 0.17121 + 7.3800 27.000 165.50 78.930 1.1761 0.22297 + 7.3800 27.000 165.50 79.512 0.86373 0.12655 + 7.3800 27.000 165.50 98.663 1.0845 0.21059 + 7.3800 27.000 165.50 99.461 0.74966 0.11662 + 7.3800 27.000 165.50 118.15 1.0027 0.19572 + 7.3800 27.000 165.50 119.41 0.66536 0.11166 + 7.3800 27.000 165.50 128.26 1.0993 0.19324 + 7.3800 27.000 165.50 129.38 0.75969 0.10670 + 7.3800 27.000 165.50 138.13 1.1291 0.20563 + 7.3800 27.000 165.50 139.35 0.89123 0.12903 + 7.3800 27.000 167.60 36.012 1.5043 0.24033 + 7.3800 27.000 167.60 39.736 1.2297 0.16191 + 7.3800 27.000 167.60 46.485 1.5711 0.22547 + 7.3800 27.000 167.60 49.846 1.2077 0.12266 + 7.3800 27.000 167.60 56.685 1.2762 0.22794 + 7.3800 27.000 167.60 59.716 1.0286 0.13493 + 7.3800 27.000 167.60 66.878 0.87479 0.18335 + 7.3800 27.000 167.60 69.583 0.89126 0.12512 + 7.3800 27.000 167.60 77.356 1.0135 0.19573 + 7.3800 27.000 167.60 79.698 0.74901 0.12266 + 7.3800 27.000 167.60 87.329 1.0630 0.21308 + 7.3800 27.000 167.60 89.564 0.66073 0.11530 + 7.3800 27.000 167.60 99.924 0.53810 0.10549 + 7.3800 27.000 167.60 108.02 1.1322 0.19821 + 7.3800 27.000 167.60 110.04 0.47436 0.95677E-01 + 7.3800 27.000 167.60 118.49 1.0850 0.23042 + 7.3800 27.000 167.60 119.89 0.65103 0.11285 + 7.3800 27.000 167.60 130.24 0.79091 0.12021 + 7.3800 27.000 167.60 138.92 1.0304 0.20812 + 7.3800 27.000 167.60 140.35 0.89153 0.14720 +ENDDATA 218 +ENDSUBENT 237 +SUBENT F0597003 20050623 20050831 F022 +BIB 2 2 +REACTION (14-SI-28(A,INL)14-SI-28,PAR,DA) +STATUS (CURVE)Fig.13 +ENDBIB 2 +COMMON 3 3 +E-LVL ANG-ERR-D ERR-DIG +MEV ADEG PER-CENT + 1.78 0.6 0.03 +ENDCOMMON 3 +DATA 3 214 +EN ANG DATA +MEV ADEG MB/SR + 24.000 33.890 13.379 + 24.000 37.228 16.579 + 24.000 39.394 10.621 + 24.000 45.446 4.7437 + 24.000 48.116 5.7003 + 24.000 51.081 6.3998 + 24.000 53.847 3.3686 + 24.000 62.004 0.71188 + 24.000 64.926 1.1584 + 24.000 67.172 1.9566 + 24.000 70.020 2.6345 + 24.000 72.600 2.9794 + 24.000 75.324 2.2557 + 24.000 78.058 1.5477 + 24.000 80.790 1.0863 + 24.000 83.398 0.97144 + 24.000 85.808 0.90901 + 24.000 88.409 0.86370 + 24.000 91.113 0.76663 + 24.000 93.814 0.70672 + 24.000 96.409 0.70271 + 24.000 98.575 1.0278 + 24.000 101.43 1.3124 + 24.000 104.60 1.3155 + 24.000 107.11 1.1586 + 24.000 109.55 0.85085 + 24.000 111.86 0.83946 + 24.000 113.84 1.1296 + 24.000 116.32 1.3167 + 24.000 118.43 1.4332 + 24.000 121.33 1.2066 + 24.000 123.94 1.0469 + 24.000 126.10 0.73448 + 24.000 128.52 0.61348 + 24.000 130.62 0.70415 + 24.000 132.96 1.1540 + 24.000 135.53 1.4402 + 24.000 139.27 1.5577 + 24.000 142.15 1.5609 + 24.000 143.82 1.2172 + 24.000 146.06 0.95676 + 24.000 149.13 0.95166 + 24.000 150.55 1.1777 + 24.000 152.75 1.3016 + 24.000 155.15 1.3138 + 24.000 157.46 1.3061 + 24.000 159.36 1.5567 + 24.000 161.56 1.6441 + 24.000 164.16 1.5740 + 24.000 165.88 1.7790 + 24.000 168.07 2.0421 + 24.000 170.28 2.0146 + 24.000 172.88 2.0338 + 26.000 33.935 16.216 + 26.000 36.665 11.862 + 26.000 39.692 8.0533 + 26.000 44.865 4.2448 + 26.000 47.996 5.8721 + 26.000 51.174 5.5438 + 26.000 56.202 2.0089 + 26.000 58.862 1.1825 + 26.000 61.771 0.96087 + 26.000 64.512 1.3899 + 26.000 67.136 2.3707 + 26.000 69.998 2.8015 + 26.000 72.899 2.4351 + 26.000 74.948 1.8905 + 26.000 78.061 1.3938 + 26.000 80.501 1.0348 + 26.000 83.101 0.99123 + 26.000 85.763 1.2529 + 26.000 88.530 1.4694 + 26.000 91.146 1.2300 + 26.000 93.491 0.90634 + 26.000 96.296 0.78187 + 26.000 99.044 1.0652 + 26.000 101.33 1.3063 + 26.000 104.59 1.2900 + 26.000 106.97 1.5586 + 26.000 109.96 1.4171 + 26.000 111.83 1.0675 + 26.000 113.97 0.82882 + 26.000 117.03 0.92955 + 26.000 119.42 1.0188 + 26.000 121.18 0.85229 + 26.000 123.40 0.72945 + 26.000 126.28 0.75328 + 26.000 128.60 0.68457 + 26.000 131.01 0.64592 + 26.000 133.50 0.68198 + 26.000 135.30 0.85502 + 26.000 137.50 0.93001 + 26.000 139.53 0.82622 + 26.000 141.79 0.55225 + 26.000 144.30 0.52111 + 26.000 146.55 0.38394 + 26.000 148.32 0.27443 + 26.000 150.99 0.33412 + 26.000 153.06 0.45158 + 26.000 155.04 0.64314 + 26.000 157.81 0.73203 + 26.000 159.91 0.79618 + 26.000 161.71 1.0133 + 26.000 164.11 1.0000 + 26.000 166.06 0.83042 + 26.000 168.83 0.91045 + 26.000 170.81 1.2678 + 26.000 173.55 1.8898 + 27.000 33.086 14.770 + 27.000 41.795 3.8083 + 27.000 44.429 6.2261 + 27.000 47.404 6.4831 + 27.000 55.597 2.2866 + 27.000 58.468 1.0993 + 27.000 61.726 1.1987 + 27.000 63.968 2.0828 + 27.000 66.632 2.6253 + 27.000 69.530 2.3101 + 27.000 72.252 1.7574 + 27.000 74.977 1.3066 + 27.000 77.620 0.85951 + 27.000 80.614 0.75635 + 27.000 83.170 1.0610 + 27.000 85.256 1.3471 + 27.000 88.234 1.3604 + 27.000 91.070 0.88819 + 27.000 92.863 0.51661 + 27.000 96.222 0.53808 + 27.000 98.259 1.0405 + 27.000 100.82 1.3730 + 27.000 103.79 1.5552 + 27.000 106.59 1.3476 + 27.000 109.11 1.1409 + 27.000 111.37 0.71662 + 27.000 114.27 0.64520 + 27.000 116.53 0.95471 + 27.000 118.70 1.3389 + 27.000 121.49 1.2620 + 27.000 123.75 0.83630 + 27.000 126.11 0.55001 + 27.000 128.45 0.38750 + 27.000 130.93 0.46290 + 27.000 133.46 0.78025 + 27.000 134.97 1.0209 + 27.000 137.53 1.3576 + 27.000 140.14 1.2220 + 27.000 142.23 0.68425 + 27.000 144.40 0.40735 + 27.000 146.75 0.28920 + 27.000 148.65 0.14436 + 27.000 151.41 0.18619 + 27.000 153.26 0.33605 + 27.000 154.96 0.46397 + 27.000 157.31 0.68659 + 27.000 159.52 0.72000 + 27.000 162.02 0.67850 + 27.000 163.54 0.79765 + 27.000 165.97 0.64007 + 27.000 168.46 0.70829 + 27.000 170.70 1.1755 + 27.000 172.85 2.1220 + 27.500 36.234 13.859 + 27.500 37.963 8.5556 + 27.500 43.497 2.1162 + 27.500 47.864 6.5827 + 27.500 49.704 7.2404 + 27.500 56.445 2.2500 + 27.500 60.031 1.3150 + 27.500 61.588 1.7179 + 27.500 64.360 2.6232 + 27.500 67.772 3.2807 + 27.500 70.879 2.7050 + 27.500 72.677 1.9726 + 27.500 75.727 1.2252 + 27.500 77.897 0.75231 + 27.500 80.824 0.64124 + 27.500 83.758 1.1127 + 27.500 85.650 1.6983 + 27.500 89.079 1.8182 + 27.500 91.244 1.1736 + 27.500 93.447 0.53689 + 27.500 95.956 0.37256 + 27.500 99.212 0.84873 + 27.500 101.12 1.1529 + 27.500 104.24 1.7316 + 27.500 106.56 1.3959 + 27.500 109.83 1.2303 + 27.500 111.81 0.86787 + 27.500 113.44 0.58226 + 27.500 116.52 0.65518 + 27.500 118.85 1.0114 + 27.500 121.75 1.0298 + 27.500 123.64 0.73449 + 27.500 125.80 0.49016 + 27.500 128.12 0.39076 + 27.500 130.29 0.52209 + 27.500 132.29 0.65617 + 27.500 134.55 0.85747 + 27.500 136.56 1.0252 + 27.500 139.39 0.93398 + 27.500 141.21 0.57979 + 27.500 143.78 0.50242 + 27.500 146.18 0.43053 + 27.500 149.71 0.18032 + 27.500 151.63 0.20967 + 27.500 153.81 0.27398 + 27.500 156.39 0.46230 + 27.500 158.93 0.53770 + 27.500 161.21 0.59483 + 27.500 163.14 0.64348 + 27.500 165.51 0.68095 + 27.500 167.63 0.66293 + 27.500 169.96 1.0522 + 27.500 172.79 2.0975 +ENDDATA 216 +ENDSUBENT 227 +ENDENTRY 3 diff --git a/exforall/F05/F0598.x4 b/exforall/F05/F0598.x4 new file mode 100644 index 000000000..fbbf3a8f9 --- /dev/null +++ b/exforall/F05/F0598.x4 @@ -0,0 +1,468 @@ +ENTRY F0598 20050609 20050831 F022 +SUBENT F0598001 20050609 20050831 F022 +BIB 13 51 +TITLE Elastic scattering of 27.5 MeV alpha particles on + 27Al, 28Si, 32S,Ti and 59Co nuclei and the r0 + discrete ambiguity of the optical potential. +AUTHOR (A.Bobrowska,A.Budzanowski,K.Grotowski,L.Jarczyk, + B.Kamys,S.Micek,M.Polok,A.Strzalkowski,Z.Wrobel) +INSTITUTE (3POLUJK,3POLIFJ) +REFERENCE (J,APP/B,3,533,1972) +FACILITY (CYCLO,3POLIFJ) U-120 +INC-SOURCE (KINDT) The energy of the incident beam was measured + by means of the differential absorption method. The + absolute reliability of this measurement was checked + by the kinematic method. +DETECTOR (SOLST) Thirteen semiconductor detectors were mounted + on four rotatable arms. Particles scaterred at extreme + backward angles up to 179 degrees were detected by + means of a special very narrow counter. Angular + resolution of the back scattering counter was about + +-0.1 degree while for the others was +-0.5 degree. + (SIBAR) Silicon surface barrier counters with the + thickness of the depletion layer of 0.5 mm were used. +SAMPLE A special arrangement was provided to prepare targets + by evaporation inside of the vacuum store. + The targets were located at the distance of about 12 m + from the cyclotron. The diameter of the targets was + about 30 mm. +METHOD (BCINT) +MONITOR During the cross-section measurements the thickness + of the target was checked by a special semiconductor + monitor viewing the target at a fixed angle of about + 30 degrees (lab). + The intensity of the alpha-particle beam was monitored + in two independent ways in order to ensure the proper + normalization of the cross-section. The total charge + in the Faraday cup was measured by a standart current + integrator. + In addition the beam intensity was monitored by two + semiconductor detectors counting alpha particles + scattered from a gold foil placed in the beam in front + of the Faraday cup. +ERR-ANALYS (EN-ERR) Accuracy of the absolute energy measurement + (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error of the absolute value of the cross- + section + The relative errors in the values of the experimental + differential cross-section vary from 1% to 10 % in deep + minima. +COMMENT Numerical results including realtive errors of + individual measurements are available in Report 624/PL + of the Institute of Nuclear Physics in Cracow. +HISTORY (20031105C) +ENDBIB 51 +COMMON 4 3 +EN EN-ERR EN-RSL-FW ERR-DIG +MEV KEV KEV PER-CENT + 27.5 100. 250. 0.1 +ENDCOMMON 3 +ENDSUBENT 58 +SUBENT F0598002 20050609 20050831 F022 +BIB 3 4 +REACTION (13-AL-27(A,EL)13-AL-27,,DA,,RTH) +SAMPLE The target of Al prepared by evaporation was used. + The thickness of the target was 1.05 mg/cm2. +STATUS (CURVE)Fig.5a +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D DATA-ERR +ADEG PER-CENT + 0.6 5.2 +ENDCOMMON 3 +DATA 2 66 +ANG-CM DATA-CM +ADEG NO-DIM + 12.490 0.61270 + 14.790 0.47780 + 17.450 0.21910 + 20.540 0.19910 + 23.360 0.35880 + 27.040 0.47380 + 29.260 0.33090 + 32.030 0.10200 + 35.290 0.69490E-01 + 37.590 0.29030 + 40.670 0.45800 + 44.170 0.45400 + 46.200 0.23290 + 49.010 0.13320 + 51.110 0.76270E-01 + 55.110 0.29690 + 57.120 0.44940 + 59.860 0.40860 + 63.120 0.27850 + 65.380 0.11700 + 67.810 0.64090E-01 + 70.170 0.96930E-01 + 73.360 0.31690 + 76.300 0.22590 + 79.750 0.20960 + 81.280 0.14660 + 83.930 0.11430 + 86.820 0.76230E-01 + 89.270 0.13160 + 91.040 0.23780 + 93.320 0.31510 + 96.490 0.32670 + 98.740 0.23850 + 101.40 0.19000 + 103.00 0.14520 + 105.80 0.16100 + 108.40 0.17870 + 111.20 0.19810 + 113.60 0.18430 + 116.20 0.20450 + 119.00 0.22680 + 120.50 0.26960 + 123.40 0.30560 + 125.40 0.26630 + 127.70 0.20770 + 130.00 0.95340E-01 + 133.20 0.98860E-01 + 135.10 0.12540 + 137.00 0.16270 + 139.20 0.18890 + 142.10 0.20940 + 144.50 0.18640 + 146.10 0.93640E-01 + 149.00 0.97180E-01 + 150.60 0.13480 + 152.80 0.15650 + 155.00 0.19840 + 157.50 0.20610 + 159.90 0.19600 + 161.20 0.16370 + 164.40 0.17350 + 165.90 0.21090 + 170.10 0.39590 + 172.00 0.50240 + 175.30 0.56900 + 178.20 0.70440 +ENDDATA 68 +ENDSUBENT 81 +SUBENT F0598003 20050609 20050831 F022 +BIB 3 4 +REACTION (14-SI-28(A,EL)14-SI-28,,DA,,RTH) +SAMPLE The target was SiO2 blowed. The thickness of the target + was 0.542 mg/cm2. +STATUS (CURVE)Fig.5b +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D DATA-ERR +ADEG PER-CENT + 0.5 7.5 +ENDCOMMON 3 +DATA 2 61 +ANG-CM DATA-CM +ADEG NO-DIM + 31.060 0.93410E-01 + 33.660 0.74470E-01 + 36.250 0.31720 + 38.620 0.53830 + 41.670 0.52300 + 44.440 0.23850 + 46.580 0.32230E-01 + 50.310 0.89690E-01 + 52.990 0.29380 + 56.400 0.45240 + 59.970 0.41180 + 61.630 0.26050 + 63.930 0.10760 + 65.770 0.38940E-01 + 70.350 0.35500E-01 + 72.510 0.12010 + 73.930 0.16710 + 77.450 0.17930 + 79.580 0.12940 + 82.320 0.65140E-01 + 85.190 0.22110E-01 + 87.390 0.63450E-01 + 90.650 0.15990 + 92.990 0.29950 + 96.000 0.33180 + 98.110 0.24750 + 99.860 0.12040 + 102.20 0.45060E-01 + 105.60 0.71700E-01 + 107.30 0.21970 + 111.70 0.35000 + 113.10 0.44130 + 115.20 0.35160 + 118.00 0.17700 + 119.20 0.94930E-01 + 122.10 0.12810 + 125.10 0.17860 + 126.40 0.30270 + 129.50 0.29410 + 130.60 0.20520 + 133.30 0.11780 + 135.40 0.87860E-01 + 138.20 0.19400 + 141.10 0.35190 + 142.00 0.42910 + 144.50 0.50730 + 146.20 0.28140 + 148.60 0.89370E-01 + 151.40 0.31340E-01 + 154.40 0.23350 + 156.10 0.60700 + 157.50 0.96340 + 160.40 1.1400 + 161.00 0.90630 + 163.80 0.36250 + 167.40 0.61750E-01 + 168.40 0.30940 + 170.60 1.1940 + 171.30 2.6290 + 173.70 4.1780 + 175.10 6.2080 +ENDDATA 63 +ENDSUBENT 76 +SUBENT F0598004 20050609 20050831 F022 +BIB 3 4 +REACTION (16-S-32(A,EL)16-S-32,,DA,,RTH) +SAMPLE The target of S evaporated on C backing was used. The + thickness of the target was 2.64 mg/cm2. +STATUS (CURVE)Fig.5c +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D DATA-ERR +ADEG PER-CENT + 0.6 8.7 +ENDCOMMON 3 +DATA 2 64 +ANG-CM DATA-CM +ADEG NO-DIM + 25.730 0.34540 + 28.440 0.20430 + 31.260 0.79270E-01 + 34.170 0.12450 + 37.370 0.32270 + 40.310 0.43250 + 43.020 0.26270 + 45.480 0.78260E-01 + 48.050 0.14890E-01 + 50.470 0.16030 + 52.880 0.31060 + 56.320 0.32000 + 59.010 0.21040 + 60.960 0.85950E-01 + 63.490 0.19160E-01 + 65.800 0.56620E-01 + 69.030 0.13210 + 71.610 0.13240 + 73.830 0.10460 + 77.340 0.80660E-01 + 79.220 0.42900E-01 + 81.750 0.53110E-01 + 84.980 0.12390 + 87.030 0.18930 + 89.110 0.25360 + 92.990 0.24790 + 95.180 0.21770 + 96.580 0.13920 + 100.50 0.10180 + 102.20 0.12270 + 104.70 0.17790 + 106.30 0.25770 + 108.90 0.28710 + 111.90 0.25910 + 114.10 0.21030 + 116.80 0.12440 + 119.00 0.10640 + 121.60 0.10670 + 123.80 0.10970 + 125.60 0.66590E-01 + 127.30 0.86830E-01 + 130.70 0.11040 + 132.80 0.12630 + 135.30 0.14070 + 137.60 0.11120 + 139.70 0.95100E-01 + 142.10 0.39910E-01 + 144.90 0.15480E-01 + 146.90 0.31620E-01 + 148.90 0.66300E-01 + 151.30 0.10680 + 154.00 0.84480E-01 + 155.80 0.52640E-01 + 158.20 0.18860E-01 + 160.10 0.50140E-01 + 161.80 0.76580E-01 + 164.80 0.69110E-01 + 167.20 0.24120E-01 + 169.20 0.86370E-02 + 171.10 0.10890 + 173.00 0.39720 + 174.90 1.1430 + 176.60 0.95180 + 178.30 1.1770 +ENDDATA 66 +ENDSUBENT 79 +SUBENT F0598005 20050609 20050831 F022 +BIB 3 4 +REACTION (22-TI-0(A,EL)22-TI-0,,DA,,RTH) +SAMPLE The target of Ti prepared by evaporation was used. The + thickness of the target was 0.244 mg/cm2. +STATUS (CURVE)Fig.5f +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D DATA-ERR +ADEG PER-CENT + 0.3 9.7 +ENDCOMMON 3 +DATA 2 65 +ANG-CM DATA-CM +ADEG NO-DIM + 18.150 0.29030 + 21.530 0.38250 + 24.550 0.31560 + 27.540 0.18520 + 29.870 0.11840 + 32.910 0.14950 + 35.300 0.22870 + 38.320 0.20990 + 40.950 0.87640E-01 + 44.290 0.59700E-01 + 46.010 0.10600 + 49.070 0.14890 + 52.090 0.13370 + 55.070 0.66210E-01 + 56.950 0.89530E-02 + 59.770 0.54600E-01 + 61.830 0.10110 + 65.190 0.10110 + 67.860 0.71850E-01 + 70.490 0.26980E-01 + 72.020 0.28260E-02 + 74.140 0.13070E-01 + 77.240 0.37050E-01 + 79.620 0.50950E-01 + 82.630 0.40290E-01 + 84.920 0.15130E-01 + 86.850 0.41280E-02 + 89.570 0.60510E-02 + 91.350 0.26260E-01 + 94.720 0.28570E-01 + 97.430 0.34570E-01 + 99.770 0.27340E-01 + 102.70 0.88440E-02 + 103.70 0.40230E-02 + 106.80 0.10470E-01 + 108.80 0.27860E-01 + 111.60 0.31630E-01 + 113.90 0.36690E-01 + 116.90 0.31590E-01 + 118.60 0.19350E-01 + 121.90 0.89880E-02 + 123.60 0.13460E-01 + 126.60 0.93670E-02 + 128.30 0.16280E-01 + 131.40 0.14940E-01 + 132.70 0.21900E-01 + 135.80 0.21430E-01 + 137.80 0.19250E-01 + 140.10 0.15890E-01 + 142.80 0.78660E-02 + 146.10 0.55910E-02 + 148.50 0.76890E-02 + 149.90 0.11520E-01 + 152.60 0.14240E-01 + 154.30 0.20430E-01 + 156.60 0.14840E-01 + 158.60 0.10780E-01 + 161.60 0.11240E-01 + 164.30 0.11720E-01 + 165.30 0.88830E-02 + 168.00 0.60520E-02 + 170.00 0.73260E-02 + 173.10 0.19480E-01 + 174.50 0.54080E-01 + 178.30 0.98040E-01 +ENDDATA 67 +ENDSUBENT 80 +SUBENT F0598006 20050609 20050831 F022 +BIB 3 4 +REACTION (27-CO-59(A,EL)27-CO-59,,DA,,RTH) +SAMPLE The target of Co was used (rolled). The thickness of + the target was 1.81 mg/cm2. +STATUS (CURVE)Fig.5g +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D DATA-ERR +ADEG PER-CENT + 0.2 11.1 +ENDCOMMON 3 +DATA 2 65 +ANG-CM DATA-CM +ADEG NO-DIM + 16.600 0.87650 + 19.700 0.78180 + 22.160 0.75310 + 25.250 0.72570 + 26.520 0.51310 + 32.120 0.29980 + 35.800 0.35040 + 37.680 0.27830 + 39.570 0.18220 + 43.330 0.10640 + 45.150 0.13420 + 47.590 0.16290 + 50.060 0.15100 + 53.220 0.75520E-01 + 56.380 0.37770E-01 + 57.570 0.53480E-01 + 59.970 0.91870E-01 + 64.900 0.92080E-01 + 66.780 0.67690E-01 + 68.740 0.26850E-01 + 71.900 0.13430E-01 + 73.660 0.27970E-01 + 75.440 0.48030E-01 + 78.520 0.48100E-01 + 81.030 0.34030E-01 + 83.570 0.17020E-01 + 86.750 0.75820E-02 + 89.170 0.10330E-01 + 91.570 0.17750E-01 + 94.000 0.23280E-01 + 95.920 0.13070E-01 + 100.30 0.96150E-02 + 101.60 0.56070E-02 + 105.20 0.58370E-02 + 106.40 0.10420E-01 + 108.80 0.14750E-01 + 112.50 0.15960E-01 + 115.00 0.12680E-01 + 116.30 0.73950E-02 + 119.40 0.52340E-02 + 121.30 0.39990E-02 + 123.10 0.77090E-02 + 126.10 0.11350E-01 + 128.50 0.14890E-01 + 133.50 0.14360E-01 + 136.00 0.94050E-02 + 139.10 0.54890E-02 + 141.00 0.38820E-02 + 144.10 0.55010E-02 + 145.90 0.87460E-02 + 147.70 0.11920E-01 + 150.70 0.12400E-01 + 153.20 0.10640E-01 + 155.70 0.78260E-02 + 158.80 0.53290E-02 + 160.70 0.64680E-02 + 163.10 0.75550E-02 + 166.20 0.78640E-02 + 167.50 0.40840E-02 + 170.00 0.32440E-02 + 173.00 0.39400E-02 + 173.50 0.20690E-01 + 174.60 0.54300E-01 + 177.00 0.63430E-01 + 178.80 0.76980E-01 +ENDDATA 67 +ENDSUBENT 80 +ENDENTRY 6 diff --git a/exforall/F06/F0608.x4 b/exforall/F06/F0608.x4 new file mode 100644 index 000000000..570a329d5 --- /dev/null +++ b/exforall/F06/F0608.x4 @@ -0,0 +1,706 @@ +ENTRY F0608 20050415 20050831 F021 +SUBENT F0608001 20050415 20050831 F021 +BIB 11 29 +TITLE Narrow a+ 28Si elastic-scattering states at high + excitation in 32S. +AUTHOR (K.-M.Kallman,M.Brenner,V.Z.Goldberg,T.Lonnroth, + P.Manngard,A.E.Pakhomov,V.V.Pankratov) +INSTITUTE (2SF ABA) + (4RUSKUR) +REFERENCE (J,EPJ/A,16,159,2003) +FACILITY (ISOCY,2SF ABA) K-20 isochronous cyclotron in the + particle energy range 12.0-19.6 MeV. + (VDGT,2SWDUPP) in the range of 6.5-12.8 MeV beam + energy. + (CYCLO,2NOROSL) K-35 cyclotron in the energy range + 19-30 MeV. +SAMPLE Target was 10 micron thick plate of natural silicon. + Isotope abundances are 28Si 92.2, 29Si 4.7 and 30Si + 3.1% respectively. +DETECTOR 105 degree analyzing magnet at K-20 cyclotron, 90 + degree magnet at accelerator, 50 degree analyzing + magnet at K-35 cyclotron were used for beam energies + analyzing. + The exitation functions were measured with a set of + seven detectors in three settings, giving 21 angular- + distribution points in the angle range 107-173 degrees. + No information about the detector type used is given. +METHOD Backscattering technique on a thick target. +CORRECTION Partial spectra were corrected for energy loss in + the target and matched by normalizing the intensity. +ERR-ANALYS Intrinsic detector resolution was about 20 keV. +HISTORY (20040901C) +ENDBIB 29 +NOCOMMON 0 0 +ENDSUBENT 32 +SUBENT F0608002 20050415 20050831 F021 +BIB 3 4 +REACTION (14-SI-28(A,EL)14-SI-28,,DA,,REL) +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error +STATUS (CURVE)Fig.4 +ENDBIB 4 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.2 0.1 +ENDCOMMON 3 +DATA 3 124 +EN-CM ANG-CM DATA-CM +MEV ADEG ARB-UNITS + 8.7000 114.36 0.39187E-01 + 8.7000 117.25 0.58361E-01 + 8.7000 120.37 0.79871E-01 + 8.7000 123.92 0.12956 + 8.7000 126.83 0.14963 + 8.7000 129.51 0.15874 + 8.7000 133.11 0.13446 + 8.7000 136.03 0.11382 + 8.7000 138.73 0.99084E-01 + 8.7000 142.33 0.68870E-01 + 8.7000 145.04 0.52057E-01 + 8.7000 147.51 0.46606E-01 + 8.7000 151.29 0.71461E-01 + 8.7000 153.95 0.11581 + 8.7000 156.61 0.18246 + 8.7000 160.17 0.27971 + 8.7000 162.61 0.40479 + 8.7000 165.06 0.53820 + 8.7000 168.63 0.65816 + 8.7000 171.32 0.71824 + 8.7000 173.77 0.85293 + 9.8300 114.53 0.11654 + 9.8300 117.24 0.90583E-01 + 9.8300 120.17 0.64700E-01 + 9.8300 124.20 0.66786E-01 + 9.8300 126.88 0.70832E-01 + 9.8300 129.56 0.94174E-01 + 9.8300 133.13 0.12181 + 9.8300 135.80 0.14880 + 9.8300 138.49 0.16233 + 9.8300 142.07 0.16284 + 9.8300 144.99 0.14174 + 9.8300 147.70 0.10412 + 9.8300 151.31 0.62811E-01 + 9.8300 154.01 0.48822E-01 + 9.8300 156.69 0.64911E-01 + 9.8300 159.99 0.17499 + 9.8300 162.66 0.27562 + 9.8300 165.32 0.41029 + 9.8300 168.67 0.57754 + 9.8300 171.12 0.68568 + 9.8300 173.80 0.81423 + 11.350 114.81 0.37145E-01 + 11.350 117.50 0.36215E-01 + 11.350 120.42 0.31587E-01 + 11.350 124.24 0.26076E-01 + 11.350 126.94 0.21504E-01 + 11.350 129.87 0.17737E-01 + 11.350 133.44 0.21638E-01 + 11.350 136.11 0.31181E-01 + 11.350 138.99 0.48867E-01 + 11.350 142.32 0.78786E-01 + 11.350 145.22 0.96050E-01 + 11.350 147.91 0.96297E-01 + 11.350 151.50 0.96627E-01 + 11.350 153.98 0.65530E-01 + 11.350 156.73 0.27659E-01 + 11.350 160.36 0.13064E-01 + 11.350 162.73 0.59100E-01 + 11.350 165.57 0.17114 + 11.350 168.89 0.38568 + 11.350 171.56 0.52561 + 11.350 174.00 0.77868 + 12.680 206.00 0.36930E-01 + 12.680 208.47 0.47758E-01 + 12.680 211.64 0.53667E-01 + 12.680 215.03 0.73511E-01 + 12.680 217.75 0.73742E-01 + 12.680 220.71 0.66088E-01 + 12.680 224.38 0.42233E-01 + 12.680 227.16 0.20326E-01 + 12.680 229.95 0.87373E-02 + 12.680 233.55 0.13787E-01 + 12.680 236.20 0.38237E-01 + 12.680 238.65 0.65588E-01 + 12.680 242.26 0.92439E-01 + 12.680 244.99 0.92730E-01 + 12.680 247.50 0.74186E-01 + 12.680 251.17 0.46088E-01 + 12.680 253.89 0.50322E-01 + 12.680 256.33 0.10226 + 12.680 259.90 0.26830 + 12.680 262.35 0.46022 + 12.680 264.82 0.72526 + 14.070 205.77 0.80497E-01 + 14.070 208.52 0.57398E-01 + 14.070 211.50 0.37591E-01 + 14.070 215.13 0.39945E-01 + 14.070 217.82 0.66827E-01 + 14.070 220.54 0.67022E-01 + 14.070 224.15 0.94635E-01 + 14.070 226.90 0.67480E-01 + 14.070 229.87 0.48128E-01 + 14.070 233.56 0.21797E-01 + 14.070 236.48 0.35453E-01 + 14.070 238.71 0.70308E-01 + 14.070 242.29 0.13572 + 14.070 245.01 0.14823 + 14.070 247.52 0.12181 + 14.070 250.99 0.52108E-01 + 14.070 253.76 0.26416E-01 + 14.070 256.44 0.49516E-01 + 14.070 259.99 0.18909 + 14.070 262.44 0.37509 + 14.070 264.90 0.64545 + 17.550 114.73 0.40590E-01 + 17.550 117.67 0.50924E-01 + 17.550 120.40 0.49686E-01 + 17.550 123.86 0.25536E-01 + 17.550 133.37 0.33207E-01 + 17.550 136.28 0.58232E-01 + 17.550 138.78 0.55238E-01 + 17.550 142.68 0.35510E-01 + 17.550 145.24 0.15856E-01 + 17.550 147.96 0.16821E-01 + 17.550 151.26 0.62699E-01 + 17.550 153.94 0.11952 + 17.550 156.64 0.14991 + 17.550 160.30 0.11390 + 17.550 162.85 0.58476E-01 + 17.550 165.68 0.14947E-01 + 17.550 168.97 0.65867E-01 + 17.550 171.37 0.24525 + 17.550 173.79 0.60081 +ENDDATA 126 +ENDSUBENT 139 +SUBENT F0608003 20050415 20050831 F021 +BIB 3 4 +REACTION (14-SI-28(A,EL)14-SI-28,,DA) +ERR-ANALYS (EN-ERR-DIG) Digitizing error + (ERR-DIG) Digitizing error +STATUS (CURVE)Fig.5 +ENDBIB 4 +COMMON 3 3 +ANG EN-ERR-DIG ERR-DIG +ADEG MEV MB/SR + 173.0 0.01 0.7 +ENDCOMMON 3 +DATA 2 407 +EN DATA +MEV MB/SR + 6.3906 26.809 + 6.4161 20.278 + 6.4411 26.932 + 6.4580 24.776 + 6.4832 27.034 + 6.5085 24.899 + 6.5250 35.927 + 6.5422 24.980 + 6.5509 18.409 + 6.5844 22.886 + 6.5898 106.41 + 6.5926 29.498 + 6.6141 135.04 + 6.6348 27.403 + 6.6682 34.078 + 6.6931 45.126 + 6.7177 62.767 + 6.7253 84.762 + 6.7327 113.35 + 6.7489 133.17 + 6.7646 163.97 + 6.7723 185.97 + 6.7905 146.45 + 6.7919 106.90 + 6.8145 181.68 + 6.8308 197.10 + 6.8401 172.95 + 6.8500 131.22 + 6.8601 82.893 + 6.8678 104.89 + 6.8777 63.157 + 6.9037 41.244 + 6.9296 23.726 + 6.9543 39.169 + 6.9792 50.218 + 6.9965 37.074 + 7.0041 61.267 + 7.0381 52.559 + 7.0468 43.790 + 7.0723 37.259 + 7.0894 30.707 + 7.1064 26.354 + 7.1230 32.987 + 7.1482 33.048 + 7.1642 57.261 + 7.1804 77.079 + 7.2058 72.746 + 7.2316 57.425 + 7.2405 44.261 + 7.2660 35.533 + 7.2825 46.561 + 7.2903 64.161 + 7.3150 79.605 + 7.3229 92.810 + 7.3309 106.01 + 7.3493 62.107 + 7.3501 40.132 + 7.3591 22.573 + 7.3764 11.627 + 7.3924 33.643 + 7.4255 51.304 + 7.4332 71.102 + 7.4485 115.09 + 7.4646 134.91 + 7.4982 137.19 + 7.5311 159.25 + 7.5723 183.52 + 7.5801 203.32 + 7.5991 141.83 + 7.6084 117.68 + 7.6325 148.50 + 7.6401 172.70 + 7.6732 188.16 + 7.7045 254.17 + 7.7241 177.30 + 7.7286 52.042 + 7.7381 21.298 + 7.7708 49.947 + 7.7777 91.719 + 7.7931 133.51 + 7.8327 439.08 + 7.8794 74.385 + 7.9010 175.53 + 7.9021 146.96 + 7.9270 155.81 + 7.9443 142.67 + 7.9656 19.654 + 8.0246 17.600 + 8.0809 92.457 + 8.1390 349.72 + 8.1538 171.75 + 8.1831 59.741 + 8.1876 167.44 + 8.1954 185.04 + 8.2146 121.35 + 8.2385 158.77 + 8.2671 299.49 + 8.2955 213.85 + 8.3188 266.65 + 8.3855 51.443 + 8.4483 179.06 + 8.4734 183.51 + 8.5065 436.32 + 8.5193 313.29 + 8.5488 429.83 + 8.5804 251.90 + 8.6047 280.53 + 8.6241 208.06 + 8.6930 399.42 + 8.7105 381.88 + 8.7636 74.339 + 8.7873 118.35 + 8.7983 45.855 + 8.9046 369.17 + 8.9719 136.38 + 9.0178 501.30 + 9.0536 206.90 + 9.0691 244.30 + 9.0921 72.941 + 9.1019 33.408 + 9.1094 59.798 + 9.1926 86.372 + 9.2078 132.56 + 9.2426 337.02 + 9.2652 176.65 + 9.2913 154.74 + 9.3014 106.42 + 9.3486 198.83 + 9.3686 110.97 + 9.3791 53.861 + 9.4120 73.720 + 9.4375 69.387 + 9.4776 124.43 + 9.5037 100.31 + 9.5289 102.57 + 9.5545 93.845 + 9.5843 201.60 + 9.6083 236.82 + 9.6260 212.69 + 9.6270 186.32 + 9.6572 283.09 + 9.6717 111.71 + 9.6828 274.36 + 9.7083 502.98 + 9.7725 118.55 + 9.8155 329.63 + 9.8901 127.63 + 9.9301 659.55 + 9.9745 123.44 + 9.9966 211.40 + 10.033 138.96 + 10.070 275.31 + 10.110 88.605 + 10.163 268.94 + 10.169 334.88 + 10.198 238.26 + 10.215 236.10 + 10.227 374.58 + 10.240 240.56 + 10.262 75.790 + 10.294 363.76 + 10.310 155.02 + 10.336 152.88 + 10.371 104.62 + 10.401 205.79 + 10.492 27.999 + 10.524 61.043 + 10.558 63.322 + 10.573 102.92 + 10.591 74.391 + 10.595 195.27 + 10.620 208.52 + 10.674 96.571 + 10.704 206.53 + 10.736 252.75 + 10.755 211.04 + 10.763 200.08 + 10.786 270.46 + 10.788 226.51 + 10.815 178.22 + 10.852 66.237 + 10.880 244.31 + 10.912 286.15 + 10.985 110.51 + 11.043 372.17 + 11.089 288.77 + 11.122 293.25 + 11.155 84.554 + 11.196 335.19 + 11.223 302.29 + 11.224 280.31 + 11.249 273.78 + 11.287 163.99 + 11.335 476.17 + 11.364 111.44 + 11.388 170.83 + 11.425 54.446 + 11.456 149.02 + 11.490 133.72 + 11.517 72.251 + 11.577 278.97 + 11.624 140.64 + 11.697 217.73 + 11.753 778.27 + 11.769 802.48 + 11.831 237.84 + 11.882 237.96 + 11.936 383.14 + 11.974 31.606 + 12.007 33.885 + 12.063 106.54 + 12.096 126.40 + 12.106 100.05 + 12.156 104.57 + 12.191 62.903 + 12.237 212.45 + 12.254 192.72 + 12.270 216.93 + 12.290 129.07 + 12.323 140.14 + 12.342 94.036 + 12.374 375.41 + 12.434 111.84 + 12.474 171.27 + 12.500 155.95 + 12.549 191.24 + 12.578 96.807 + 12.593 128.46 + 12.668 268.92 + 12.728 124.68 + 12.740 98.360 + 12.761 82.778 + 12.839 185.22 + 12.867 191.09 + 12.904 88.748 + 12.946 45.883 + 13.036 127.86 + 13.099 59.661 + 13.137 74.317 + 13.166 71.416 + 13.186 62.658 + 13.246 157.28 + 13.300 79.328 + 13.329 193.42 + 13.382 254.89 + 13.419 152.55 + 13.429 147.68 + 13.458 151.61 + 13.480 111.65 + 13.501 95.095 + 13.519 105.83 + 13.561 70.770 + 13.595 122.47 + 13.650 39.645 + 13.703 97.213 + 13.738 145.02 + 13.760 104.09 + 13.776 34.875 + 13.815 29.057 + 13.868 86.626 + 13.915 93.490 + 13.955 82.798 + 13.994 76.981 + 14.040 95.544 + 14.143 18.606 + 14.170 43.978 + 14.171 28.379 + 14.200 32.303 + 14.270 113.29 + 14.314 48.973 + 14.352 49.005 + 14.390 62.686 + 14.419 59.786 + 14.503 323.10 + 14.574 51.140 + 14.601 67.737 + 14.630 73.611 + 14.660 60.961 + 14.718 51.260 + 14.748 34.711 + 14.797 31.826 + 14.827 12.352 + 14.959 168.46 + 15.057 29.118 + 15.124 38.923 + 15.197 78.959 + 15.207 73.118 + 15.235 90.690 + 15.279 28.328 + 15.336 145.37 + 15.400 69.379 + 15.402 48.905 + 15.422 43.072 + 15.450 47.971 + 15.488 59.702 + 15.529 27.562 + 15.588 13.961 + 15.626 21.792 + 15.665 15.975 + 15.708 71.585 + 15.737 76.484 + 15.785 72.624 + 15.805 66.791 + 15.825 57.058 + 15.871 85.371 + 15.933 38.623 + 15.994 108.87 + 16.024 94.273 + 16.079 18.270 + 16.108 13.419 + 16.127 17.335 + 16.155 26.134 + 16.156 19.309 + 16.193 29.090 + 16.223 26.190 + 16.242 21.331 + 16.279 42.811 + 16.317 47.718 + 16.358 13.628 + 16.407 6.8439 + 16.446 7.8509 + 16.474 18.599 + 16.492 22.515 + 16.521 28.388 + 16.550 20.613 + 16.579 22.587 + 16.589 19.670 + 16.628 10.928 + 16.694 34.382 + 16.734 11.991 + 16.783 8.1319 + 16.811 11.081 + 16.839 24.754 + 16.887 27.719 + 16.912 72.589 + 16.964 143.81 + 17.023 8.3326 + 17.043 5.4239 + 17.071 9.3476 + 17.119 11.338 + 17.138 15.253 + 17.173 60.132 + 17.206 12.385 + 17.245 8.5172 + 17.283 11.474 + 17.338 44.669 + 17.397 36.918 + 17.443 55.482 + 17.473 49.656 + 17.520 63.345 + 17.547 87.742 + 17.567 72.160 + 17.606 71.217 + 17.619 25.404 + 17.647 33.227 + 17.677 25.452 + 17.697 15.719 + 17.736 10.876 + 17.774 10.909 + 17.820 39.221 + 17.861 15.855 + 17.889 15.879 + 17.977 118.33 + 17.996 123.22 + 18.061 38.447 + 18.090 31.647 + 18.100 26.780 + 18.139 26.812 + 18.158 29.753 + 18.178 24.895 + 18.188 12.229 + 18.218 8.3531 + 18.256 6.4354 + 18.265 14.243 + 18.294 19.141 + 18.323 19.165 + 18.323 12.341 + 18.352 10.415 + 18.381 13.364 + 18.410 14.363 + 18.459 4.6541 + 18.497 4.6862 + 18.534 20.317 + 18.553 24.233 + 18.591 31.089 + 18.620 29.163 + 18.630 25.272 + 18.649 29.188 + 18.658 35.045 + 18.677 37.986 + 18.708 19.487 + 18.728 13.653 + 18.757 10.752 + 18.805 10.793 + 18.834 12.767 + 18.852 18.632 + 18.871 24.498 + 18.890 29.388 + 18.919 29.412 + 18.929 25.521 + 18.948 22.612 + 18.967 25.553 + 18.987 22.644 + 18.997 15.828 + 19.027 7.0776 + 19.065 12.959 + 19.074 11.017 +ENDDATA 409 +ENDSUBENT 422 +SUBENT F0608004 20050415 20050831 F021 +BIB 4 12 +REACTION 1(14-SI-28(A,0),,EN) + 2(14-SI-28(A,TOT),,WID) + 3(14-SI-28(A,EL),,WID) +ANALYSIS Individual measured spectra for different angles + were energy shifted and merged into two-dimensional + Ecm x ANGcm matrices. Excitation function was analyzed + by fitting individual peaks with individual widths + together with background in the 173 degree spectrum. In + this manner resonance energies and widths were + extracted. +ERR-ANALYS (DATA-ERR) Uncertainty in resonance width. +STATUS (TABLE) Table 1 +ENDBIB 12 +NOCOMMON 0 0 +DATA 5 84 +DATA 1DATA 2DATA-ERR 2DATA 3DATA-ERR 3 +MEV KEV KEV KEV KEV + 6.8340 29.000 5.0000 16.000 10.000 + 7.0120 26.000 7.0000 6.0000 4.0000 + 7.2200 49.000 3.0000 17.900 1.2000 + 7.3370 28.800 1.3000 12.800 0.80000 + 7.4740 54.000 5.0000 28.000 3.0000 + 7.5860 18.000 4.0000 8.0000 2.0000 + 7.6630 74.000 2.0000 50.000 2.0000 + 7.7100 23.600 0.90000 12.300 0.60000 + 7.8360 47.400 0.80000 27.900 1.0000 + 7.9080 22.000 1.1000 11.000 0.60000 + 7.9380 22.400 1.0000 8.8000 0.50000 + 8.1370 29.600 0.70000 27.300 0.80000 + 8.2070 15.200 0.60000 6.6000 0.30000 + 8.2590 42.000 1.1000 25.400 1.1000 + 8.3240 89.000 2.0000 69.000 2.0000 + 8.5470 40.000 2.0000 41.000 2.0000 + 8.6760 84.500 1.1000 66.000 2.0000 + 8.7800 7.0000 0.90000 2.0000 0.30000 + 9.0080 37.500 0.50000 33.200 0.60000 + 9.0600 25.500 0.70000 14.800 0.50000 + 9.2290 30.500 1.1000 21.000 2.0000 + 9.3320 36.000 2.0000 15.800 1.4000 + 9.4630 18.000 2.0000 5.1000 0.70000 + 9.5930 45.900 1.0000 23.000 0.70000 + 9.6400 24.500 0.60000 13.600 0.40000 + 9.7040 34.300 0.30000 24.700 0.50000 + 9.8020 46.800 1.3000 24.800 0.90000 + 9.9210 29.900 0.30000 27.900 0.40000 + 9.9840 35.900 1.0000 16.700 0.70000 + 10.066 41.000 0.90000 20.000 0.60000 + 10.168 47.000 2.0000 33.000 2.0000 + 10.222 28.000 0.80000 18.500 0.70000 + 10.291 21.600 0.50000 14.400 0.40000 + 10.402 54.000 2.0000 28.000 2.0000 + 10.620 41.300 0.80000 18.800 0.50000 + 10.732 86.000 2.0000 47.100 1.4000 + 10.908 64.000 3.0000 39.000 3.0000 + 11.046 60.000 2.0000 38.000 2.0000 + 11.132 23.000 2.0000 12.000 3.0000 + 11.197 45.000 2.0000 23.000 3.0000 + 11.251 76.000 6.0000 41.000 3.0000 + 11.333 38.100 0.60000 27.800 0.60000 + 11.394 35.000 0.80000 14.400 0.50000 + 11.461 47.000 3.0000 18.000 2.0000 + 11.577 58.000 1.4000 32.500 1.3000 + 11.771 92.000 14.000 96.000 27.000 + 11.935 35.000 6.0000 20.000 17.000 + 12.235 36.000 2.0000 16.400 0.80000 + 12.272 26.000 2.0000 10.800 1.0000 + 12.478 82.000 7.0000 35.000 3.0000 + 12.553 48.000 4.0000 20.000 2.0000 + 12.677 44.000 2.0000 26.400 1.2000 + 12.872 76.000 7.0000 28.000 7.0000 + 13.152 66.000 5.0000 15.200 1.2000 + 13.262 73.600 1.4000 28.300 0.70000 + 13.383 74.000 5.0000 38.000 3.0000 + 13.470 75.000 6.0000 29.000 2.0000 + 13.546 46.000 3.0000 12.900 1.0000 + 13.755 34.000 2.0000 11.900 1.0000 + 13.907 84.000 7.0000 23.000 4.0000 + 14.055 54.000 10.000 15.000 3.0000 + 14.276 72.000 2.0000 25.400 0.70000 + 14.401 75.000 18.000 18.000 4.0000 + 14.518 54.000 2.0000 31.600 1.1000 + 14.625 79.000 9.0000 20.000 3.0000 + 15.228 44.000 4.0000 15.100 1.0000 + 15.350 72.000 17.000 24.000 10.000 + 15.468 84.000 4.0000 20.800 1.1000 + 15.718 37.000 4.0000 6.7000 1.0000 + 15.869 59.000 2.0000 16.500 0.80000 + 16.299 69.000 3.0000 15.000 0.80000 + 16.509 70.000 5.0000 11.200 0.80000 + 16.579 45.000 4.0000 6.2000 0.70000 + 16.665 39.000 10.000 6.0000 2.0000 + 16.952 53.000 2.0000 22.400 0.80000 + 17.354 74.000 4.0000 14.900 1.1000 + 17.434 54.000 9.0000 12.000 4.0000 + 17.552 47.000 14.000 10.000 7.0000 + 17.606 24.000 5.0000 4.6000 1.3000 + 18.167 51.000 5.0000 8.3000 1.1000 + 18.395 58.000 3.0000 8.1000 0.60000 + 18.601 74.000 16.000 14.000 3.0000 + 18.681 52.000 7.0000 10.000 2.0000 + 18.906 93.000 12.000 17.000 2.0000 +ENDDATA 86 +ENDSUBENT 103 +ENDENTRY 4 diff --git a/exforall/F06/F0618.x4 b/exforall/F06/F0618.x4 new file mode 100644 index 000000000..e298f8e14 --- /dev/null +++ b/exforall/F06/F0618.x4 @@ -0,0 +1,146 @@ +ENTRY F0618 20050615 20050831 F022 +SUBENT F0618001 20050615 20050831 F022 +BIB 13 35 +TITLE Charged particle activation analysis of phosphorus in + biological materials. +AUTHOR (K.Masumoto,M.Yagi) +INSTITUTE (2JPNTOH) +REFERENCE (J,JRC,78,233,1983) +FACILITY (ISOCY) +INC-SOURCE 1 mu-A beam of alphas. +DETECTOR (GELI)Detector with a useful volume of 80 cm3,relative + efficiency of 15%,and resolution of 2.10 keV at 1333.0 + keV. +SAMPLE Potassium dihydrogen phosphate,sulfur and sodium + chloride were used as the targets to determine the + thick-target yields of 34mCl on phosphorus,sulfur and + chlorine. All irradiation samples were pressed into + smooth-surfaced pellets of 1 cm in diameter by using an + oil pressure press of 10 tons. The thickness of each + pellett was thick enough to stop the incident alpha + particles. All pellets prepared were wrapped with + 10 mu-m aluminium foil of more than 99.99% purity. +METHOD (ACTIV) + (BCINT) + (EDEG) +MONITOR The calibration standards of phosphorus in biological + samples were prepared by using co-polymerization + reaction of a homogeneous acrylamide solution + containing known amounts of potassium dihydrogen + phosphate. +MONIT-REF (,K.Masumoto+,J,RRL,42,99,1980) +ERR-ANALYS (ERR-T)The overall error in the absolute value of the + above thick-target yield.It is mainly due to errors in + the counting statistics,detector efficiencies and decay + scheme data. + (EN-ERR-DIG)Digitizing error + (ERR-DIG)Digitizing error +HISTORY (20040202C) +ENDBIB 35 +COMMON 3 3 +ERR-T EN-ERR-DIG ERR-DIG +PER-CENT MEV PER-CENT + 10.0 0.1 0.2 +ENDCOMMON 3 +ENDSUBENT 42 +SUBENT F0618002 20050615 20050831 F022 +BIB 3 3 +REACTION (15-P-31(A,N)17-CL-34-M,,TTY,,DT) +DECAY-DATA (17-CL-34-M,32.2MIN) +STATUS (CURVE)Fig.1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 2 30 +EN DATA +MEV MCI/MUAHR + 8.8979 0.15171 + 10.385 0.38085 + 10.887 0.47409 + 11.435 0.48580 + 12.206 0.65570 + 12.575 0.94155 + 13.126 0.93220 + 13.876 1.1092 + 14.218 1.0247 + 14.623 1.3738 + 15.519 1.7820 + 15.982 2.4872 + 16.147 2.1075 + 16.780 2.3673 + 17.172 2.5095 + 17.536 2.5998 + 17.867 2.7714 + 18.655 3.0091 + 20.000 2.9516 + 20.901 3.5949 + 21.810 3.9496 + 23.612 3.9236 + 23.942 4.2065 + 25.163 4.2446 + 26.474 4.3834 + 26.873 4.2398 + 29.131 4.3646 + 31.207 4.3640 + 33.374 4.4401 + 36.823 4.5592 +ENDDATA 32 +ENDSUBENT 40 +SUBENT F0618003 20050615 20050831 F022 +BIB 3 3 +REACTION (16-S-32(A,N+P)17-CL-34-M,,TTY,,DT) +DECAY-DATA (17-CL-34-M,32.2MIN) +STATUS (CURVE)Fig.1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 2 18 +EN DATA +MEV MCI/MUAHR + 17.151 0.16331E-02 + 17.508 0.18226E-02 + 18.370 0.14666E-01 + 19.869 0.86813E-01 + 20.621 0.14232 + 21.067 0.23713 + 22.382 0.68612 + 23.438 0.79411 + 23.570 1.0160 + 24.520 1.3957 + 25.479 1.7397 + 26.166 2.0815 + 26.617 2.2711 + 29.023 3.4932 + 31.034 5.3360 + 33.093 6.5591 + 35.418 8.8932 + 37.483 10.206 +ENDDATA 20 +ENDSUBENT 28 +SUBENT F0618004 20050615 20050831 F022 +BIB 3 3 +REACTION (17-CL-35(A,N+A)17-CL-34-M,,TTY,,DT) +DECAY-DATA (17-CL-34-M,32.2MIN) +STATUS (CURVE)Fig.1 +ENDBIB 3 +NOCOMMON 0 0 +DATA 2 16 +EN DATA +MEV MCI/MUAHR + 19.812 0.15635E-02 + 20.433 0.40726E-02 + 20.729 0.65540E-02 + 21.122 0.98501E-02 + 22.380 0.39034E-01 + 23.475 0.83821E-01 + 23.545 0.75634E-01 + 24.505 0.13289 + 25.536 0.20827 + 26.292 0.32616 + 26.803 0.35797 + 28.953 0.63843 + 31.013 1.1126 + 33.182 1.5874 + 35.535 2.2277 + 37.357 2.5402 +ENDDATA 18 +ENDSUBENT 26 +ENDENTRY 4 diff --git a/exforall/F06/F0629.x4 b/exforall/F06/F0629.x4 new file mode 100644 index 000000000..073af0089 --- /dev/null +++ b/exforall/F06/F0629.x4 @@ -0,0 +1,629 @@ +ENTRY F0629 20050615 20050831 F022 +SUBENT F0629001 20050615 20050831 F022 +BIB 10 24 +TITLE Anomalies in alpha-scattering and (3He,alpha) reactions + on 40,41Ca and the effect of cluster exchange. +AUTHOR (H.J.Apell,W.Gemeinhardt,R.Stock,R.R.Betts,O.Hansen, + A.Sperduto,H.Fuchs,R.Santo) +INSTITUTE (2GERMBG,2DENNBI,2GERBER,2GERMST) +REFERENCE (J,NP/A,246,477,1975) +FACILITY (VDGT,2DENNBI) +SAMPLE The target was evaporated from CaCO3 onto a thin carbon + foil and had a Ca thickness of about 20 mu-g/cm2 with + an isotopic abundance of 81% 41Ca and 18% 40Ca. +DETECTOR (SOLST)Scattering chamber was equipped with four cooled + solid state detectors. +MONITOR The data for the angles more than 75 deg. were + normalized to the 41Ca target abundance and matched to + the 41Ca data at larger angles. + The absolute cross section scale was established a) by + Rutherford scattering determination of the total Ca + thickness of the target, and b) by matching the elastic + 3He and alpha scattering yields to optical model + calculations. +ERR-ANALYS (ANG-ERR-D) Digitizing error + (ERR-DIG) Digitizing error + (DATA-ERR) Error from the graphic bars +HISTORY (20031003C) +ENDBIB 24 +NOCOMMON 0 0 +ENDSUBENT 27 +SUBENT F0629002 20050615 20050831 F022 +BIB 2 2 +REACTION (20-CA-40(A,EL)20-CA-40,,DA,,RTH) +STATUS (CURVE)Fig.1,2 +ENDBIB 2 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.6 0.03 +ENDCOMMON 3 +DATA 4 96 +EN ANG-CM DATA-CM DATA-ERR +MEV ADEG NO-DIM NO-DIM + 19.000 83.543 0.15701 + 19.000 85.955 0.98408E-01 + 19.000 87.829 0.41856E-01 + 19.000 90.179 0.94444E-02 + 19.000 92.932 0.87220E-02 + 19.000 96.125 0.24871E-01 + 19.000 98.357 0.61580E-01 + 19.000 100.56 0.87653E-01 + 19.000 103.64 0.13257 + 19.000 106.15 0.18310 0.14363E-01 + 19.000 108.60 0.18051 + 19.000 111.24 0.18435 + 19.000 113.62 0.14711 + 19.000 115.89 0.12596 + 19.000 118.32 0.71389E-01 + 19.000 120.74 0.42334E-01 + 19.000 122.49 0.10145E-01 + 19.000 124.74 0.10677E-01 + 19.000 127.48 0.47880E-01 + 19.000 132.46 0.24370 + 19.000 134.90 0.26039 0.21824E-01 + 19.000 137.03 0.30766 + 19.000 139.61 0.24307 + 19.000 141.51 0.17894 + 19.000 143.29 0.75344E-01 + 19.000 145.67 0.27422E-01 + 19.000 147.66 0.21770E-01 + 19.000 150.16 0.68982E-01 + 19.000 152.59 0.15919 + 19.000 157.23 0.25205 + 19.000 159.84 0.16531 + 19.000 161.47 0.99493E-01 + 19.000 163.52 0.49217E-01 + 24.100 83.454 0.13110E-01 + 24.100 86.280 0.11018E-02 + 24.100 88.847 0.15859E-01 + 24.100 90.737 0.47017E-01 + 24.100 93.499 0.40710E-01 + 24.100 98.598 0.11958E-01 + 24.100 100.92 0.19207E-01 + 24.100 103.51 0.53378E-01 + 24.100 106.35 0.60491E-01 + 24.100 108.80 0.64569E-01 + 24.100 110.89 0.47898E-01 + 24.100 113.56 0.34661E-01 + 24.100 115.06 0.63054E-02 + 24.100 120.24 0.38723E-01 + 24.100 122.82 0.10870 + 24.100 125.34 0.17634 0.22416E-01 + 24.100 127.60 0.17730 + 24.100 129.69 0.12084 + 24.100 132.47 0.83608E-01 + 24.100 134.74 0.76465E-01 + 24.100 137.00 0.81210E-01 + 24.100 139.73 0.11012 + 24.100 141.49 0.12415 + 24.100 143.72 0.18783 + 24.100 148.38 0.25734E-01 + 24.100 150.83 0.12312 + 24.100 153.22 0.29027 + 24.100 155.75 0.43483 + 24.100 157.51 0.55252 + 24.100 160.45 0.60772 0.70433E-01 + 24.100 162.63 0.42677 + 24.100 164.91 0.32948 + 26.500 83.094 0.47536E-01 + 26.500 93.119 0.13067E-01 + 26.500 95.418 0.47290E-01 + 26.500 98.717 0.96922E-01 + 26.500 101.10 0.94897E-01 + 26.500 103.68 0.93375E-01 + 26.500 106.14 0.14446 + 26.500 108.71 0.13518 + 26.500 110.83 0.15943 + 26.500 113.54 0.18705 0.22921E-01 + 26.500 115.71 0.97695E-01 + 26.500 117.70 0.29204E-01 + 26.500 120.43 0.12921 + 26.500 122.52 0.23840 + 26.500 125.05 0.32200 + 26.500 127.61 0.27523 + 26.500 129.58 0.23650 + 26.500 131.79 0.83871E-01 + 26.500 134.50 0.28279E-01 + 26.500 136.58 0.92557E-01 + 26.500 138.79 0.10971 + 26.500 141.29 0.21825 + 26.500 143.55 0.18103 + 26.500 145.65 0.19602 + 26.500 148.05 0.34555E-01 + 26.500 150.70 0.53457E-01 + 26.500 151.99 0.17154 + 26.500 156.95 0.29911 + 26.500 159.05 0.32226 0.48698E-01 + 26.500 161.58 0.23570 + 26.500 164.58 0.26162 +ENDDATA 98 +ENDSUBENT 109 +SUBENT F0629003 20050615 20050831 F022 +BIB 2 2 +REACTION (20-CA-41(A,EL)20-CA-41,,DA,,RTH) +STATUS (CURVE)Fig.1,2 +ENDBIB 2 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.6 0.03 +ENDCOMMON 3 +DATA 4 154 +EN ANG-CM DATA-CM DATA-ERR +MEV ADEG NO-DIM NO-DIM + 19.000 18.486 0.82030 + 19.000 24.339 0.46781 + 19.000 29.258 0.39491 + 19.000 34.554 0.37621 + 19.000 39.776 0.13985 + 19.000 45.125 0.18759 + 19.000 50.205 0.20782 + 19.000 55.286 0.10714 + 19.000 58.181 0.70629E-01 + 19.000 60.739 0.64895E-100.50906E-02 + 19.000 65.698 0.85736E-01 + 19.000 71.076 0.43543E-01 + 19.000 76.224 0.60500E-01 + 19.000 78.457 0.70413E-01 + 19.000 80.884 0.82786E-01 + 19.000 83.319 0.91629E-01 + 19.000 86.291 0.71318E-01 + 19.000 88.345 0.34230E-01 + 19.000 88.622 0.39216E-01 + 19.000 90.035 0.13432E-01 + 19.000 92.500 0.56004E-02 + 19.000 95.563 0.96544E-02 + 19.000 97.956 0.31212E-01 + 19.000 100.43 0.53795E-01 + 19.000 103.23 0.71737E-01 + 19.000 105.47 0.79394E-100.62250E-02 + 19.000 107.63 0.77479E-01 + 19.000 110.39 0.68730E-01 + 19.000 113.05 0.62520E-01 + 19.000 115.70 0.59506E-01 + 19.000 118.01 0.37483E-01 + 19.000 120.19 0.15238E-01 + 19.000 122.17 0.12722E-01 + 19.000 124.54 0.22259E-01 + 19.000 127.23 0.70536E-01 + 19.000 129.72 0.11502 + 19.000 132.33 0.14956 + 19.000 134.18 0.16140 + 19.000 136.03 0.16898 0.16967E-01 + 19.000 138.69 0.15217 + 19.000 140.79 0.11259 + 19.000 143.31 0.63176E-01 + 19.000 145.23 0.19472E-01 + 19.000 150.19 0.51780E-01 + 19.000 152.27 0.91505E-01 + 19.000 155.26 0.13563 + 19.000 156.71 0.15390 + 19.000 159.36 0.15404 + 19.000 161.43 0.13188 + 19.000 164.00 0.11236 + 24.100 19.918 0.37468 + 24.100 22.386 0.31958 + 24.100 27.587 0.36233 + 24.100 33.650 0.13793 + 24.100 41.019 0.14590 + 24.100 43.497 0.10716 + 24.100 45.989 0.65785E-01 + 24.100 48.859 0.49543E-01 + 24.100 52.055 0.98119E-01 + 24.100 57.137 0.15076 + 24.100 59.446 0.75067E-01 + 24.100 61.812 0.16671E-01 + 24.100 64.483 0.13000E-01 + 24.100 67.499 0.83887E-01 + 24.100 70.425 0.11604 + 24.100 73.085 0.10613 + 24.100 75.661 0.79132E-01 + 24.100 77.057 0.59876E-01 + 24.100 79.775 0.23826E-01 + 24.100 82.775 0.27823E-02 + 24.100 85.531 0.10798E-01 + 24.100 87.333 0.27844E-01 + 24.100 92.641 0.28009E-01 + 24.100 95.362 0.10551E-01 + 24.100 97.946 0.70497E-02 + 24.100 100.70 0.67438E-02 + 24.100 103.11 0.14463E-01 + 24.100 105.52 0.27383E-01 + 24.100 108.76 0.27536E-01 + 24.100 110.47 0.17328E-01 + 24.100 112.83 0.40651E-02 + 24.100 115.66 0.56232E-02 + 24.100 120.47 0.24000E-01 + 24.100 123.37 0.49958E-01 + 24.100 125.31 0.67730E-01 + 24.100 128.23 0.10560 0.99106E-02 + 24.100 130.13 0.67789E-01 + 24.100 132.11 0.53920E-01 + 24.100 134.60 0.31648E-01 + 24.100 136.76 0.33612E-01 + 24.100 139.47 0.66231E-01 + 24.100 141.61 0.89796E-01 + 24.100 144.15 0.11758 + 24.100 146.22 0.10385 + 24.100 148.52 0.57698E-01 + 24.100 150.87 0.70106E-01 + 24.100 153.00 0.10141 + 24.100 155.62 0.16784 + 24.100 157.46 0.25015 + 24.100 160.30 0.29649 0.37665E-01 + 24.100 162.46 0.29220 + 24.100 165.04 0.20624 + 26.500 19.803 0.33827 + 26.500 22.574 0.31333 + 26.500 27.956 0.34396 + 26.500 32.919 0.98148E-01 + 26.500 40.576 0.10032 + 26.500 42.866 0.30595E-100.27327E-02 + 26.500 45.836 0.28480E-01 + 26.500 48.757 0.12103 + 26.500 52.318 0.19880 + 26.500 55.162 0.15756 + 26.500 57.056 0.89198E-01 + 26.500 59.700 0.20836E-01 + 26.500 61.819 0.75395E-02 + 26.500 64.752 0.62847E-01 + 26.500 67.943 0.12311 + 26.500 70.692 0.99561E-01 + 26.500 75.306 0.20909E-01 + 26.500 76.577 0.54861E-02 + 26.500 79.910 0.13887E-01 + 26.500 82.623 0.30392E-01 + 26.500 83.457 0.38481E-01 + 26.500 85.397 0.28868E-01 + 26.500 88.051 0.13161E-01 + 26.500 88.178 0.15536E-01 + 26.500 89.488 0.51628E-02 + 26.500 91.495 0.10587E-01 + 26.500 95.554 0.32269E-01 + 26.500 98.847 0.63850E-01 + 26.500 103.93 0.69051E-01 + 26.500 105.88 0.55024E-01 + 26.500 108.62 0.75823E-01 + 26.500 111.05 0.99374E-100.13304E-01 + 26.500 113.08 0.73064E-01 + 26.500 115.69 0.83596E-01 + 26.500 118.01 0.31330E-01 + 26.500 120.80 0.10565 + 26.500 123.11 0.12649 + 26.500 125.49 0.21533 + 26.500 127.85 0.19356 + 26.500 130.18 0.13600 + 26.500 132.04 0.62649E-01 + 26.500 134.31 0.57174E-01 + 26.500 136.71 0.60364E-01 + 26.500 139.06 0.93395E-01 + 26.500 141.54 0.16139 + 26.500 146.40 0.15240 + 26.500 148.19 0.83295E-01 + 26.500 152.22 0.64346E-01 + 26.500 157.65 0.16521 + 26.500 159.88 0.21438 0.29927E-01 + 26.500 162.06 0.21204 + 26.500 164.23 0.10270 +ENDDATA 156 +ENDSUBENT 167 +SUBENT F0629004 20050615 20050831 F022 +BIB 2 2 +REACTION (20-CA-41(HE3,A)20-CA-40,PAR,DA) +STATUS (CURVE)Fig.3,4 +ENDBIB 2 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.1 0.02 +ENDCOMMON 3 +DATA 5 192 +E-LVL EN ANG-CM DATA-CM DATA-ERR +MEV MEV ADEG MB/SR MB/SR + 0.0000 16.000 16.529 0.28226 0.48681E-01 + 0.0000 16.000 22.305 0.18752 0.18713E-01 + 0.0000 16.000 27.678 0.20000 0.21836E-01 + 0.0000 16.000 33.374 0.17192 0.18775E-01 + 0.0000 17.000 16.736 0.33218 0.46949E-01 + 0.0000 17.000 22.300 0.15766 0.16483E-01 + 0.0000 17.000 27.836 0.23049 0.21894E-01 + 0.0000 17.000 33.478 0.17836 0.19478E-01 + 0.0000 18.000 16.651 0.38306 0.38145E-01 + 0.0000 18.000 22.407 0.18114 0.22265E-01 + 0.0000 18.000 27.973 0.19725 0.17763E-01 + 0.0000 18.000 33.476 0.16611 0.20413E-01 + 0.0000 19.000 16.791 0.48826 0.53267E-01 + 0.0000 19.000 22.465 0.27878 0.22464E-01 + 0.0000 19.000 27.873 0.23604 0.20157E-01 + 0.0000 19.000 33.577 0.23514 0.34257E-01 + 0.0000 20.000 16.767 0.51191 0.55952E-01 + 0.0000 20.000 22.489 0.29652 0.26782E-01 + 0.0000 20.000 27.897 0.25360 0.26534E-01 + 0.0000 20.000 33.496 0.21346 0.18275E-01 + 0.0000 21.000 16.687 0.53298 0.45347E-01 + 0.0000 21.000 22.412 0.33145 0.26599E-01 + 0.0000 21.000 27.912 0.26502 0.23806E-01 + 0.0000 21.000 33.498 0.17923 0.20317E-01 + 0.0000 22.000 16.579 0.63265 0.62882E-01 + 0.0000 22.000 22.479 0.35133 0.28221E-01 + 0.0000 22.000 28.034 0.29343 0.33325E-01 + 0.0000 22.000 33.384 0.18366 0.15648E-01 + 0.0000 23.000 16.639 0.92502 0.78811E-01 + 0.0000 23.000 22.366 0.43657 0.37165E-01 + 0.0000 23.000 27.940 0.31488 0.28333E-01 + 0.0000 23.000 33.622 0.20780 0.20668E-01 + 0.0000 24.000 16.767 0.73819 0.93738E-01 + 0.0000 24.000 22.465 0.30495 0.31664E-01 + 0.0000 24.000 27.960 0.27562 0.29885E-01 + 0.0000 24.000 33.597 0.17932 0.16082E-01 + 0.0000 25.000 16.997 0.86774 0.86516E-01 + 0.0000 25.000 22.537 0.39438 0.46638E-01 + 0.0000 25.000 28.120 0.26705 0.30378E-01 + 0.0000 25.000 33.657 0.17706 0.24191E-01 + 0.0000 26.000 16.672 0.84721 0.10861 + 0.0000 26.000 22.501 0.38964 0.49979E-01 + 0.0000 26.000 27.928 0.28488 0.40421E-01 + 0.0000 26.000 33.449 0.14942 0.20503E-01 + 0.0000 27.000 16.753 0.79473 0.12287 + 0.0000 27.000 22.518 0.40763 0.46370E-01 + 0.0000 27.000 27.973 0.24204 0.26405E-01 + 0.0000 27.000 33.675 0.19902 0.21699E-01 + 3.7300 16.000 16.506 0.16237 0.42341E-01 + 3.7300 16.000 22.104 0.16848 0.21688E-01 + 3.7300 16.000 27.841 0.99690E-010.15999E-01 + 3.7300 16.000 33.379 0.63856E-010.39372E-02 + 3.7300 17.000 16.635 0.13837 0.30323E-01 + 3.7300 17.000 22.210 0.10413 0.10895E-01 + 3.7300 17.000 27.765 0.10088 0.20856E-01 + 3.7300 17.000 33.462 0.54493E-010.30651E-02 + 3.7300 18.000 16.598 0.17284 0.30740E-01 + 3.7300 18.000 22.312 0.13986 0.16031E-01 + 3.7300 18.000 27.931 0.11021 0.20556E-01 + 3.7300 18.000 33.503 0.86387 0.99015E-02 + 3.7300 19.000 16.822 0.37058 0.40956E-01 + 3.7300 19.000 22.437 0.16321 0.21864E-01 + 3.7300 19.000 27.817 0.12503 0.20700E-01 + 3.7300 19.000 33.390 0.95790E-010.11937E-01 + 3.7300 20.000 16.790 0.24628 0.37386E-01 + 3.7300 20.000 22.365 0.18483 0.22988E-01 + 3.7300 20.000 27.990 0.13365 0.17855E-01 + 3.7300 20.000 33.527 0.86439E-010.99395E-02 + 3.7300 21.000 16.708 0.29896 0.41322E-01 + 3.7300 21.000 22.152 0.18529 0.19570E-01 + 3.7300 21.000 27.770 0.14743 0.13448E-01 + 3.7300 21.000 33.180 0.75470E-010.93869E-02 + 3.7300 22.000 16.847 0.33713 0.38781E-01 + 3.7300 22.000 22.475 0.19476 0.20563E-01 + 3.7300 22.000 28.154 0.13196 0.16415E-01 + 3.7300 22.000 33.637 0.78288E-010.97390E-02 + 3.7300 23.000 16.843 0.30820 0.40954E-01 + 3.7300 23.000 22.373 0.16332 0.17145E-01 + 3.7300 23.000 27.915 0.16225 0.17798E-01 + 3.7300 23.000 33.539 0.79008E-010.94054E-02 + 3.7300 24.000 16.892 0.32500 0.50957E-01 + 3.7300 24.000 22.519 0.17867 0.20613E-01 + 3.7300 24.000 27.961 0.14190 0.18362E-01 + 3.7300 24.000 33.640 0.99153E-010.16433E-01 + 3.7300 25.000 16.798 0.32005 0.38725E-01 + 3.7300 25.000 22.476 0.20134 0.19544E-01 + 3.7300 25.000 28.156 0.13953 0.18842E-01 + 3.7300 25.000 33.686 0.75114E-010.10143E-01 + 3.7300 26.000 16.864 0.36889 0.35410E-01 + 3.7300 26.000 22.389 0.16783 0.16109E-01 + 3.7300 26.000 27.927 0.13990 0.22492E-01 + 3.7300 26.000 33.360 0.77062E-010.92231E-02 + 3.7300 27.000 16.859 0.31708 0.40896E-01 + 3.7300 27.000 22.386 0.15213 0.18917E-01 + 3.7300 27.000 27.974 0.14028 0.18739E-01 + 3.7300 27.000 33.500 0.65537E-010.10828E-01 + 4.4900 16.000 16.567 0.25940 0.48145E-01 + 4.4900 16.000 22.196 0.18940 0.18927E-01 + 4.4900 16.000 27.608 0.11566 0.16897E-01 + 4.4900 16.000 33.151 0.13076 0.13684E-01 + 4.4900 17.000 16.546 0.38826 0.38780E-01 + 4.4900 17.000 22.077 0.19723 0.17822E-01 + 4.4900 17.000 27.568 0.15106 0.22077E-01 + 4.4900 17.000 33.091 0.14583 0.19312E-01 + 4.4900 18.000 16.605 0.37738 0.42785E-01 + 4.4900 18.000 22.287 0.19959 0.16971E-01 + 4.4900 18.000 27.781 0.15634 0.18448E-01 + 4.4900 18.000 33.167 0.15995 0.15891E-01 + 4.4900 19.000 16.673 0.35733 0.43603E-01 + 4.4900 19.000 22.272 0.20927 0.16733E-01 + 4.4900 19.000 27.728 0.17653 0.19942E-01 + 4.4900 19.000 33.287 0.15685 0.18431E-01 + 4.4900 20.000 16.676 0.41125 0.55748E-01 + 4.4900 20.000 22.236 0.25920 0.26826E-01 + 4.4900 20.000 27.587 0.20547 0.19339E-01 + 4.4900 20.000 33.182 0.11791 0.18602E-01 + 4.4900 21.000 16.626 0.48956 0.39137E-01 + 4.4900 21.000 22.324 0.14506 0.17018E-01 + 4.4900 21.000 27.760 0.21468 0.19207E-01 + 4.4900 21.000 33.167 0.12649 0.21604E-01 + 4.4900 22.000 16.835 0.37546 0.26803E-01 + 4.4900 22.000 22.496 0.24209 0.18488E-01 + 4.4900 22.000 27.857 0.20028 0.17226E-01 + 4.4900 22.000 33.424 0.95026E-010.12655E-01 + 4.4900 23.000 16.679 0.33493 0.34912E-01 + 4.4900 23.000 22.369 0.26326 0.21163E-01 + 4.4900 23.000 27.873 0.21586 0.20447E-01 + 4.4900 23.000 33.249 0.76158E-010.11074E-01 + 4.4900 24.000 16.971 0.47378 0.51509E-01 + 4.4900 24.000 22.406 0.24775 0.19914E-01 + 4.4900 24.000 27.826 0.22094 0.17742E-01 + 4.4900 24.000 33.429 0.98719E-010.84009E-02 + 4.4900 25.000 16.972 0.48617 0.55020E-01 + 4.4900 25.000 22.535 0.23149 0.19678E-01 + 4.4900 25.000 27.976 0.23525 0.21120E-01 + 4.4900 25.000 33.532 0.78918E-010.10385E-01 + 4.4900 26.000 16.917 0.40861 0.46227E-01 + 4.4900 26.000 22.559 0.23620 0.21183E-01 + 4.4900 26.000 28.033 0.21852 0.20650E-01 + 4.4900 26.000 33.374 0.45896E-010.97972E-02 + 4.4900 27.000 16.842 0.38785 0.34751E-01 + 4.4900 27.000 22.453 0.25020 0.16415E-01 + 4.4900 27.000 27.956 0.20526 0.17413E-01 + 4.4900 27.000 33.261 0.86792E-010.11008E-01 + 5.6100 16.000 16.620 0.36853 0.50257E-01 + 5.6100 16.000 22.098 0.20751 0.20610E-01 + 5.6100 16.000 27.800 0.14475 0.19698E-01 + 5.6100 16.000 33.226 0.15431 0.13128E-01 + 5.6100 17.000 16.540 0.41341 0.53342E-01 + 5.6100 17.000 22.188 0.19567 0.15938E-01 + 5.6100 17.000 27.719 0.15839 0.18929E-01 + 5.6100 17.000 33.262 0.13958 0.14064E-01 + 5.6100 18.000 16.640 0.49526 0.58936E-01 + 5.6100 18.000 22.080 0.20730 0.18830E-01 + 5.6100 18.000 27.698 0.15600 0.16390E-01 + 5.6100 18.000 33.206 0.15133 0.15888E-01 + 5.6100 19.000 16.722 0.50645 0.62593E-01 + 5.6100 19.000 22.412 0.22857 0.20699E-01 + 5.6100 19.000 27.926 0.16328 0.15579E-01 + 5.6100 19.000 33.415 0.13882 0.18433E-01 + 5.6100 20.000 16.822 0.64082 0.58350E-01 + 5.6100 20.000 22.309 0.27308 0.27484E-01 + 5.6100 20.000 27.947 0.16866 0.17765E-01 + 5.6100 20.000 33.306 0.11345 0.15145E-01 + 5.6100 21.000 16.798 0.51018 0.33992E-01 + 5.6100 21.000 22.346 0.23664 0.20386E-01 + 5.6100 21.000 27.733 0.19267 0.21206E-01 + 5.6100 21.000 33.348 0.14252 0.19006E-01 + 5.6100 22.000 16.856 0.44226 0.46680E-01 + 5.6100 22.000 22.192 0.24587 0.18825E-01 + 5.6100 22.000 27.800 0.20147 0.15425E-01 + 5.6100 22.000 33.324 0.12066 0.86422E-02 + 5.6100 23.000 16.773 0.43660 0.41874E-01 + 5.6100 23.000 22.343 0.28640 0.23308E-01 + 5.6100 23.000 27.867 0.18006 0.12889E-01 + 5.6100 23.000 33.536 0.10851 0.83004E-02 + 5.6100 24.000 16.721 0.53586 0.43551E-01 + 5.6100 24.000 22.162 0.24395 0.21016E-01 + 5.6100 24.000 27.818 0.20214 0.16438E-01 + 5.6100 24.000 33.451 0.91547E-010.78868E-02 + 5.6100 25.000 16.869 0.45148 0.47633E-01 + 5.6100 25.000 22.355 0.21521 0.15423E-01 + 5.6100 25.000 27.920 0.16114 0.14689E-01 + 5.6100 25.000 33.514 0.58277E-010.88486E-02 + 5.6100 26.000 16.619 0.48801 0.44437E-01 + 5.6100 26.000 22.450 0.19138 0.16505E-01 + 5.6100 26.000 28.095 0.20673 0.16824E-01 + 5.6100 26.000 33.496 0.78514E-010.86512E-02 + 5.6100 27.000 16.768 0.39692 0.43708E-01 + 5.6100 27.000 22.113 0.19039 0.15495E-01 + 5.6100 27.000 27.760 0.19924 0.14258E-01 + 5.6100 27.000 33.069 0.71384E-010.85344E-02 +ENDDATA 194 +ENDSUBENT 205 +SUBENT F0629005 20050615 20050831 F022 +BIB 2 2 +REACTION (20-CA-40(HE3,A)20-CA-39,PAR,DA) +STATUS (CURVE)Fig.5 +ENDBIB 2 +COMMON 2 3 +ANG-ERR-D ERR-DIG +ADEG PER-CENT + 0.04 0.004 +ENDCOMMON 3 +DATA 5 96 +E-LVL EN ANG-CM DATA-CM DATA-ERR +MEV MEV ADEG MB/SR MB/SR + 0.0000 16.000 16.875 7.1070 0.55697 + 0.0000 16.000 22.381 2.5131 0.18341 + 0.0000 16.000 28.165 1.5192 0.11087 + 0.0000 16.000 33.491 1.6262 0.14479 + 0.0000 17.000 16.697 5.8648 0.54879 + 0.0000 17.000 22.212 2.9432 0.27531 + 0.0000 17.000 27.940 1.5557 0.12916 + 0.0000 17.000 33.424 1.7032 0.14140 + 0.0000 18.000 16.811 6.4010 0.56387 + 0.0000 18.000 22.211 2.4399 0.21493 + 0.0000 18.000 27.952 2.0600 0.18147 + 0.0000 18.000 33.485 1.9631 0.12060 + 0.0000 19.000 16.840 7.2231 0.52205 + 0.0000 19.000 22.346 2.7500 0.24255 + 0.0000 19.000 28.086 2.2426 0.20952 + 0.0000 19.000 33.620 2.1620 0.15619 + 0.0000 20.000 16.767 7.2470 0.48311 + 0.0000 20.000 22.329 2.9163 0.25630 + 0.0000 20.000 28.170 2.0853 0.20497 + 0.0000 20.000 33.552 2.4876 0.16579 + 0.0000 21.000 16.808 7.0348 0.58263 + 0.0000 21.000 22.265 2.9922 0.27922 + 0.0000 21.000 27.953 2.4691 0.21751 + 0.0000 21.000 33.483 2.0851 0.20547 + 0.0000 22.000 16.689 7.5635 0.59180 + 0.0000 22.000 22.445 2.7140 0.25563 + 0.0000 22.000 28.156 2.4002 0.20064 + 0.0000 22.000 33.547 2.0860 0.17437 + 0.0000 23.000 16.719 8.6723 0.72253 + 0.0000 23.000 22.208 3.1592 0.32964 + 0.0000 23.000 27.972 2.3900 0.23693 + 0.0000 23.000 33.520 1.5370 0.16037 + 0.0000 24.000 16.814 7.9399 0.78429 + 0.0000 24.000 22.461 2.4696 0.21805 + 0.0000 24.000 28.120 2.3292 0.24217 + 0.0000 24.000 33.557 1.1239 0.12266 + 0.0000 25.000 16.905 7.3835 0.87422 + 0.0000 25.000 22.552 2.6463 0.18989 + 0.0000 25.000 28.210 2.3580 0.21876 + 0.0000 25.000 33.752 1.0327 0.10648 + 0.0000 26.000 16.973 6.3539 0.69258 + 0.0000 26.000 22.516 2.6412 0.20498 + 0.0000 26.000 28.228 2.4066 0.18678 + 0.0000 26.000 33.505 0.99463 0.98132E-01 + 0.0000 27.000 16.781 5.7124 0.53827 + 0.0000 27.000 22.220 2.3294 0.19479 + 0.0000 27.000 28.040 2.3147 0.16871 + 0.0000 27.000 33.638 0.80654 0.71737E-01 + 2.4700 16.000 16.626 6.1813 0.80676 + 2.4700 16.000 22.251 4.2891 0.28964 + 2.4700 16.000 27.665 2.3710 0.13417 + 2.4700 16.000 33.540 0.40167 0.22734E-01 + 2.4700 17.000 16.481 4.7586 0.73480 + 2.4700 17.000 22.153 4.1528 0.26487 + 2.4700 17.000 27.464 1.8524 0.10772 + 2.4700 17.000 33.388 0.35084 0.20403E-01 + 2.4700 18.000 16.498 6.0098 0.96437 + 2.4700 18.000 22.178 4.1454 0.25754 + 2.4700 18.000 27.607 1.3875 0.86200E-01 + 2.4700 18.000 33.466 0.50396 0.31309E-01 + 2.4700 19.000 16.471 5.9981 0.78487 + 2.4700 19.000 22.144 5.2240 0.32532 + 2.4700 19.000 27.647 1.1122 0.69260E-01 + 2.4700 19.000 33.387 0.67028 0.41741E-01 + 2.4700 20.000 16.238 5.0644 0.66320 + 2.4700 20.000 21.969 3.9692 0.24730 + 2.4700 20.000 27.646 0.47874 0.29828E-01 + 2.4700 20.000 33.085 0.78390 0.48842E-01 + 2.4700 21.000 16.455 6.4555 1.0102 + 2.4700 21.000 22.256 2.9816 0.18643 + 2.4700 21.000 27.543 0.61262 0.38295E-01 + 2.4700 21.000 33.354 1.1707 0.73180E-01 + 2.4700 22.000 16.710 6.7459 + 2.4700 22.000 22.597 2.0645 + 2.4700 22.000 28.002 0.52420 + 2.4700 22.000 33.668 1.1259 + 2.4700 23.000 16.950 5.3525 0.65911 + 2.4700 23.000 22.891 2.2388 0.12981 + 2.4700 23.000 28.084 0.90339 0.57450E-01 + 2.4700 23.000 33.698 0.99442 0.57664E-01 + 2.4700 24.000 17.032 5.8367 0.73824 + 2.4700 24.000 22.495 0.98891 0.56468E-01 + 2.4700 24.000 27.897 0.72865 0.45634E-01 + 2.4700 24.000 33.669 1.5023 0.94084E-01 + 2.4700 25.000 16.902 6.0678 0.80072 + 2.4700 25.000 22.683 0.77509 0.52951E-01 + 2.4700 25.000 28.190 1.0472 0.65770E-01 + 2.4700 25.000 33.857 1.4066 0.80543E-01 + 2.4700 26.000 16.846 4.7042 0.49220 + 2.4700 26.000 22.579 0.35979 0.22300E-01 + 2.4700 26.000 27.814 1.2351 0.83271E-01 + 2.4700 26.000 33.696 1.2070 0.74812E-01 + 2.4700 27.000 16.899 5.0448 0.66466 + 2.4700 27.000 22.429 0.18904 0.10807E-01 + 2.4700 27.000 27.816 1.5196 0.95273E-01 + 2.4700 27.000 33.486 1.1194 0.70184E-01 +ENDDATA 98 +ENDSUBENT 109 +ENDENTRY 5 diff --git a/exforall/F06/F0655.x4 b/exforall/F06/F0655.x4 new file mode 100644 index 000000000..a8a3822bf --- /dev/null +++ b/exforall/F06/F0655.x4 @@ -0,0 +1,959 @@ +ENTRY F0655 20050609 20050831 F022 +SUBENT F0655001 20050609 20050831 F022 +BIB 10 26 +TITLE Investigation of the 28Si(a,p)31P and 28Si(a,d)30P + reactions at Ea=26 MeV. +AUTHOR (K.Jankowski,A.Grzeszczuk,M.Siemaszko,A.Surowiec, + W.Zipper,A.Budzanowski,E.Kozik) +INSTITUTE (3POLPOL,3POLIFJ) +REFERENCE (J,NP/A,426,1,1984) +FACILITY (CYCLO,3POLIFJ) +DETECTOR (TELES)The standard dE-E telescope consisting of + silicon surface-barrier detectors with the following + thicknesses:dE, 40.7 mu-m; E, 4700 mu-m. + (SIBAR)The elastically scattered alpha-particles + were detected by a 1500 mu-m thick surface-barrier + silicon detector placed in the reaction plane on the + side of the beam opposite to the telescope. +MONITOR The absolute values of the cross sections have been + determined by normalization to the known value of the + elastic cross section at the laboratory angle of 35 + degrees taken from the reference of W.Zipper, thesis, + Jagellonian University,Cracow,1973,unpublished. +METHOD (EDE) +ERR-ANALYS (DATA-ERR1) Experimental error of the absolute + value of cross section + (ANG-ERR-D)Digitizing error + (ERR-DIG)Digitizing error + (DATA-ERR2)Error from the graphic bars +HISTORY (20040220C) +ENDBIB 26 +COMMON 4 3 +EN EN-RSL DATA-ERR1 ERR-DIG +MEV KEV PER-CENT PER-CENT + 26. 150.0 10.0 0.2 +ENDCOMMON 3 +ENDSUBENT 33 +SUBENT F0655002 20050609 20050831 F022 +BIB 3 4 +REACTION (14-SI-28(A,P)15-P-31,PAR,DA) +COMMENT Angular distribution for the continuous part of proton + energy spectra averaged over energy bins 1 MeV is given +STATUS (CURVE)Fig.2(a) +ENDBIB 4 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.65 +ENDCOMMON 3 +DATA 4 85 +E-CM ANG-CM DATA-CM DATA-ERR2 +MEV ADEG MB/SR MB/SR + 11.000 19.777 0.86098 0.13069 + 11.000 25.162 0.31466 0.63291E-01 + 11.000 36.467 0.19670 0.22221E-01 + 11.000 41.795 0.19918 0.22467E-01 + 11.000 47.932 0.19566 0.14089E-01 + 11.000 53.659 0.19224 0.19175E-01 + 11.000 56.867 0.15798 0.13583E-01 + 11.000 63.040 0.17235 0.17161E-01 + 11.000 67.938 0.16440 0.11866E-01 + 11.000 72.857 0.16650 0.14345E-01 + 11.000 79.035 0.18439 0.18392E-01 + 11.000 83.493 0.16079 0.16010E-01 + 11.000 89.236 0.16524 0.18639E-01 + 11.000 93.626 0.11859 0.13397E-01 + 11.000 99.348 0.11478 0.98692E-02 + 11.000 102.61 0.10957 0.94021E-02 + 11.000 107.14 0.11785 0.10112E-01 + 11.000 112.88 0.12111 0.13702E-01 + 11.000 118.95 0.96461E-010.10880E-01 + 11.000 123.96 0.12987 0.12932E-01 + 11.000 127.67 0.13974 0.10086E-01 + 11.000 132.21 0.15256 0.13144E-01 + 11.000 141.98 0.12879 0.11051E-01 + 11.000 146.56 0.16091 0.24478E-01 + 11.000 151.53 0.18650 0.21099E-01 + 11.000 154.72 0.14873 0.12788E-01 + 11.000 160.04 0.14399 0.16241E-01 + 11.000 165.29 0.11645 0.10013E-01 + 12.000 17.746 8.6872 0.99178 + 12.000 19.592 3.3931 0.56416 + 12.000 24.831 2.2847 0.26107 + 12.000 34.656 2.2438 0.22606 + 12.000 41.078 1.2216 0.15561 + 12.000 46.395 1.1832 0.13509 + 12.000 51.777 1.5519 0.23811 + 12.000 57.481 1.3518 0.11733 + 12.000 61.963 1.2141 0.88589E-01 + 12.000 66.870 1.1762 0.10196 + 12.000 73.006 1.1390 0.98989E-01 + 12.000 78.304 1.0074 0.73506E-01 + 12.000 83.676 1.2625 0.73966E-01 + 12.000 88.606 1.3599 0.17337 + 12.000 93.023 0.90210 0.90690E-01 + 12.000 98.698 0.68560 0.59584E-01 + 12.000 102.78 0.65434 0.29080E-01 + 12.000 108.12 0.70474 0.61248E-01 + 12.000 113.03 0.69315 0.60316E-01 + 12.000 122.05 0.70187 0.80055E-01 + 12.000 127.78 0.69016 0.50358E-01 + 12.000 132.31 0.80202 0.91648E-01 + 12.000 136.86 0.97535 0.57363E-01 + 12.000 146.75 1.2775 0.93074E-01 + 12.000 151.27 1.3763 0.13865 + 12.000 155.32 1.1118 0.14175 + 12.000 160.64 1.1101 0.14152 + 12.000 164.75 1.1781 0.15031 + 13.000 21.061 3.6906 0.60611 + 13.000 26.095 1.2554 0.17433 + 13.000 38.340 1.0763 0.10695 + 13.000 43.278 1.1753 0.10083 + 13.000 47.786 1.1910 0.13426 + 13.000 53.507 1.1365 0.11307 + 13.000 58.794 0.99150 0.98648E-01 + 13.000 63.218 0.73406 0.63078E-01 + 13.000 69.312 0.61216 0.52521E-01 + 13.000 75.049 0.62010 0.53203E-01 + 13.000 79.565 0.64750 0.55553E-01 + 13.000 86.048 0.50101 0.42850E-01 + 13.000 90.549 0.49277 0.68429E-01 + 13.000 94.150 0.35952 0.30797E-01 + 13.000 100.71 0.37513 0.32235E-01 + 13.000 105.70 0.49011 0.42115E-01 + 13.000 110.67 0.61223 0.77076E-01 + 13.000 115.19 0.62980 0.45448E-01 + 13.000 120.38 0.38958 0.43917E-01 + 13.000 125.36 0.50143 0.56525E-01 + 13.000 129.47 0.52367 0.44929E-01 + 13.000 133.58 0.55512 0.55231E-01 + 13.000 141.79 0.60544 0.43690E-01 + 13.000 148.80 0.72261 0.71800E-01 + 13.000 152.49 0.73252 0.52860E-01 + 13.000 154.99 0.84990 0.84560E-01 + 13.000 160.68 0.71954 0.71399E-01 + 13.000 163.55 0.74061 0.73785E-01 + 13.000 166.42 0.75100 0.64433E-01 +ENDDATA 87 +ENDSUBENT 100 +SUBENT F0655003 20050609 20050831 F022 +BIB 3 4 +REACTION (14-SI-28(A,D)15-P-30,PAR,DA) +COMMENT Angular distribution for the continuous part of proton + energy spectra averaged over energy bins 1 MeV is given +STATUS (CURVE)Fig.2(b) +ENDBIB 4 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.39 +ENDCOMMON 3 +DATA 4 81 +E-CM ANG-CM DATA-CM DATA-ERR2 +MEV ADEG MB/SR MB/SR + 5.0000 43.328 0.61378 0.74079E-01 + 5.0000 48.838 0.47358 0.67628E-01 + 5.0000 54.419 0.47260 0.67593E-01 + 5.0000 59.901 0.32899 0.39707E-01 + 5.0000 65.446 0.28869 0.47572E-01 + 5.0000 70.907 0.18604 0.26566E-01 + 5.0000 76.382 0.12622 0.12342E-01 + 5.0000 81.990 0.13961 0.19967E-01 + 5.0000 87.620 0.16681 0.16310E-01 + 5.0000 92.700 0.34217 0.49014E-01 + 5.0000 99.097 0.52862 0.39133E-01 + 5.0000 103.24 0.45231 0.33593E-01 + 5.0000 108.09 0.39700 0.38819E-01 + 5.0000 112.26 0.37651 0.36815E-01 + 5.0000 117.82 0.34782 0.25833E-01 + 5.0000 121.91 0.24226 0.17992E-01 + 5.0000 126.85 0.30481 0.29804E-01 + 5.0000 131.04 0.30434 0.36662E-01 + 5.0000 135.90 0.28122 0.27498E-01 + 5.0000 140.02 0.22276 0.11170E-01 + 5.0000 144.29 0.30284 0.29612E-01 + 5.0000 148.50 0.33514 0.24891E-01 + 5.0000 152.70 0.35229 0.34446E-01 + 5.0000 156.93 0.41044 0.30286E-01 + 5.0000 161.79 0.37927 0.28168E-01 + 5.0000 164.65 0.49002 0.36393E-01 + 5.0000 166.76 0.51549 0.50404E-01 + 5.0000 170.25 0.51482 0.38235E-01 + 6.0000 43.087 0.38096 0.44667E-01 + 6.0000 49.372 0.39816 0.38086E-01 + 6.0000 54.219 0.27665 0.27744E-01 + 6.0000 59.097 0.26221 0.19980E-01 + 6.0000 64.663 0.22955 0.23044E-01 + 6.0000 70.953 0.25488 0.25561E-01 + 6.0000 77.166 0.14239 0.14265E-01 + 6.0000 82.047 0.13857 0.17160E-01 + 6.0000 86.277 0.20581 0.15683E-01 + 6.0000 91.894 0.28233 0.21543E-01 + 6.0000 96.080 0.28214 0.28266E-01 + 6.0000 102.32 0.20528 0.20607E-01 + 6.0000 107.90 0.20509 0.10556E-01 + 6.0000 112.79 0.21042 0.21102E-01 + 6.0000 117.00 0.25976 0.19794E-01 + 6.0000 121.15 0.19412 0.19467E-01 + 6.0000 128.87 0.29588 0.29672E-01 + 6.0000 132.36 0.28049 0.28101E-01 + 6.0000 136.54 0.28030 0.28110E-01 + 6.0000 139.38 0.41643 0.41803E-01 + 6.0000 144.27 0.43867 0.54283E-01 + 6.0000 148.45 0.41581 0.41700E-01 + 6.0000 156.84 0.48658 0.48846E-01 + 6.0000 161.03 0.51263 0.51357E-01 + 6.0000 163.81 0.46102 0.23776E-01 + 6.0000 167.99 0.47304 0.36045E-01 + 6.0000 170.78 0.44849 0.34174E-01 + 7.0000 42.086 0.69498 0.85675E-01 + 7.0000 48.357 0.66852 0.96173E-01 + 7.0000 51.737 0.30681 0.44845E-01 + 7.0000 58.653 0.20110 0.20090E-01 + 7.0000 64.182 0.13898 0.13867E-01 + 7.0000 68.338 0.11250 0.13883E-01 + 7.0000 73.856 0.71847E-010.88659E-02 + 7.0000 80.160 0.86268E-010.10635E-01 + 7.0000 85.047 0.88481E-010.88506E-02 + 7.0000 90.665 0.11498 0.58946E-02 + 7.0000 96.246 0.11486 0.87178E-02 + 7.0000 101.10 0.95440E-010.72566E-02 + 7.0000 106.70 0.10316 0.78304E-02 + 7.0000 111.58 0.10581 0.80175E-02 + 7.0000 116.49 0.12378 0.93956E-02 + 7.0000 121.35 0.10560 0.80155E-02 + 7.0000 124.87 0.13373 0.10150E-01 + 7.0000 129.07 0.14844 0.11267E-01 + 7.0000 134.66 0.15629 0.15613E-01 + 7.0000 138.86 0.16898 0.16860E-01 + 7.0000 143.06 0.19772 0.19752E-01 + 7.0000 147.25 0.19242 0.19223E-01 + 7.0000 155.63 0.20787 0.20741E-01 + 7.0000 161.23 0.23684 0.23630E-01 + 7.0000 164.71 0.23052 0.23059E-01 + 7.0000 169.63 0.28426 0.28397E-01 +ENDDATA 83 +ENDSUBENT 96 +SUBENT F0655004 20050609 20050831 F022 +BIB 3 4 +REACTION (14-SI-28(A,EL)14-SI-28,PAR,DA) +COMMENT Angular distribution for the continuous part of proton + energy spectra averaged over energy bins 1 MeV is given +STATUS (CURVE)Fig.2(c) +ENDBIB 4 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.74 +ENDCOMMON 3 +DATA 4 86 +E-CM ANG-CM DATA-CM DATA-ERR2 +MEV ADEG MB/SR MB/SR + 15.000 24.314 0.75756 0.73734E-01 + 15.000 25.785 16.761 2.3856 + 15.000 29.157 1.2637 0.17991 + 15.000 31.289 10.846 1.0551 + 15.000 44.359 3.5153 0.34198 + 15.000 47.801 2.8641 0.21167 + 15.000 54.033 6.8357 0.82109 + 15.000 61.634 11.401 0.84233 + 15.000 65.054 4.4222 0.53129 + 15.000 71.210 0.79583 0.77440E-01 + 15.000 77.419 0.83741 0.10059 + 15.000 81.552 0.71809 0.53070E-01 + 15.000 86.379 0.71795 0.53042E-01 + 15.000 91.901 0.83692 0.81439E-01 + 15.000 96.733 1.0009 0.12023 + 15.000 102.98 3.3320 0.32431 + 15.000 109.18 2.6458 0.19561 + 15.000 113.97 0.75481 0.73448E-01 + 15.000 118.11 1.0526 0.10242 + 15.000 122.93 0.77409 0.38626E-01 + 15.000 125.71 1.3592 0.16326 + 15.000 128.46 1.1656 0.11345 + 15.000 133.98 1.2909 0.12558 + 15.000 137.43 1.4669 0.10842 + 15.000 144.33 1.4665 0.10839 + 15.000 149.15 1.2901 0.95348E-01 + 15.000 152.61 1.5830 0.15404 + 15.000 156.76 2.3837 0.11894 + 15.000 158.15 3.4991 0.17460 + 15.000 163.66 3.4099 0.33181 + 15.000 167.11 3.5885 0.34919 + 15.000 169.86 2.7779 0.20530 + 17.000 42.134 1.0691 0.13228 + 17.000 46.416 0.55305 0.80961E-01 + 17.000 52.703 0.38283 0.38389E-01 + 17.000 58.208 0.40431 0.68260E-01 + 17.000 63.817 0.26541 0.26615E-01 + 17.000 69.270 0.35554 0.52182E-01 + 17.000 75.448 0.40655 0.50305E-01 + 17.000 79.958 1.7410 0.21508 + 17.000 83.253 0.14935 0.21892E-01 + 17.000 85.119 0.37674 0.46689E-01 + 17.000 91.360 0.32216 0.32305E-01 + 17.000 93.755 1.7031 0.17078 + 17.000 100.80 0.88182 0.45381E-01 + 17.000 105.95 0.20118 0.24892E-01 + 17.000 112.03 0.36045 0.27390E-01 + 17.000 115.82 1.7152 0.13069 + 17.000 121.16 3.8971 0.39001 + 17.000 125.31 3.6049 0.36149 + 17.000 128.98 1.3579 0.69884E-01 + 17.000 134.91 0.19776 0.15068E-01 + 17.000 139.68 0.25795 0.13275E-01 + 17.000 147.22 0.32798 0.85508E-02 + 17.000 150.64 0.36494 0.18781E-01 + 17.000 157.49 0.45182 0.34333E-01 + 17.000 162.32 0.44072 0.33579E-01 + 17.000 165.76 0.46514 0.23938E-01 + 17.000 169.88 0.50417 0.25946E-01 + 17.000 174.05 0.44238 0.22766E-01 + 19.000 28.317 1.8865 0.22881 + 19.000 39.391 1.1553 0.86204E-01 + 19.000 44.949 0.70706 0.69523E-01 + 19.000 51.121 1.0705 0.12991 + 19.000 56.608 1.5388 0.15153 + 19.000 64.834 2.7930 0.27463 + 19.000 68.458 0.33478 0.32917E-01 + 19.000 75.949 1.0462 0.78139E-01 + 19.000 78.748 0.64006 0.62889E-01 + 19.000 92.687 0.11035 0.13391E-01 + 19.000 97.525 0.97009E-010.95315E-02 + 19.000 105.78 0.12257 0.12052E-01 + 19.000 109.27 0.73079E-010.88688E-02 + 19.000 115.43 0.13261 0.13039E-01 + 19.000 118.23 0.75073E-010.56017E-02 + 19.000 123.71 0.12282 0.14897E-01 + 19.000 128.55 0.99913E-010.98241E-02 + 19.000 132.70 0.94920E-010.24246E-02 + 19.000 137.51 0.11988 0.89538E-02 + 19.000 141.64 0.12308 0.62076E-02 + 19.000 147.82 0.17242 0.16941E-01 + 19.000 151.26 0.18165 0.91618E-02 + 19.000 156.08 0.19643 0.99069E-02 + 19.000 160.20 0.25456 0.19013E-01 + 19.000 164.33 0.27524 0.27064E-01 + 19.000 169.15 0.29002 0.28496E-01 +ENDDATA 88 +ENDSUBENT 101 +SUBENT F0655005 20050609 20050831 F022 +BIB 2 2 +REACTION (14-SI-28(A,D)15-P-30,PAR,DA) +STATUS (CURVE)Fig.5(a,b,c) +ENDBIB 2 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.85 +ENDCOMMON 3 +DATA 4 271 +E-LVL ANG-CM DATA-CM DATA-ERR2 +MEV ADEG MB/SR MB/SR + 0.0000 28.116 0.74893E-010.95395E-02 + 0.0000 39.682 0.74937E-010.11303E-01 + 0.0000 45.448 0.11913 0.12302E-01 + 0.0000 51.952 0.12584 0.24649E-01 + 0.0000 57.016 0.11288 0.14377E-01 + 0.0000 62.094 0.69134E-010.71394E-02 + 0.0000 67.180 0.33134E-010.42205E-02 + 0.0000 72.965 0.31386E-010.47340E-02 + 0.0000 78.013 0.43537E-010.44961E-02 + 0.0000 83.817 0.24574E-010.37057E-02 + 0.0000 88.870 0.29746E-010.30718E-02 + 0.0000 93.211 0.26680E-010.27552E-02 + 0.0000 99.738 0.15059E-010.22714E-02 + 0.0000 104.78 0.24600E-010.42728E-02 + 0.0000 109.13 0.19254E-010.24525E-02 + 0.0000 113.47 0.16354E-010.16888E-02 + 0.0000 118.53 0.16358E-010.16892E-02 + 0.0000 122.85 0.26720E-010.27594E-02 + 0.0000 128.64 0.18755E-010.14722E-02 + 0.0000 132.99 0.15930E-010.16445E-02 + 0.0000 137.33 0.12812E-010.13227E-02 + 0.0000 142.38 0.19287E-010.19917E-02 + 0.0000 146.72 0.17777E-010.18352E-02 + 0.0000 152.48 0.34199E-010.26845E-02 + 0.0000 155.37 0.32390E-010.48843E-02 + 0.0000 158.99 0.27509E-010.35031E-02 + 0.0000 166.20 0.42559E-010.64193E-02 +0.70900 25.810 0.83621E-010.12408E-01 +0.70900 35.928 0.73134E-010.14099E-01 +0.70900 43.153 0.51634E-010.88231E-02 +0.70900 49.663 0.73119E-010.91601E-02 +0.70900 53.998 0.63955E-010.80114E-02 +0.70900 59.781 0.65684E-010.97458E-02 +0.70900 63.391 0.41668E-010.52204E-02 +0.70900 71.344 0.51612E-010.64663E-02 +0.70900 77.112 0.12490E-010.18531E-02 +0.70900 81.445 0.88183E-020.15068E-02 +0.70900 86.511 0.15062E-010.29035E-02 +0.70900 92.302 0.31868E-010.54455E-02 +0.70900 96.636 0.23111E-010.39489E-02 +0.70900 100.97 0.20214E-010.34543E-02 +0.70900 106.75 0.14659E-010.21752E-02 +0.70900 111.81 0.14271E-010.30555E-02 +0.70900 117.59 0.92983E-020.13797E-02 +0.70900 121.20 0.10349E-010.19950E-02 +0.70900 124.81 0.71137E-020.10556E-02 +0.70900 129.88 0.77080E-020.16503E-02 +0.70900 134.22 0.15879E-010.19892E-02 +0.70900 144.34 0.15049E-010.22329E-02 +0.70900 148.68 0.16748E-010.28618E-02 +0.70900 152.29 0.12476E-010.15629E-02 + 1.4540 38.800 0.64302E-010.16273E-01 + 1.4540 43.860 0.59383E-010.10063E-01 + 1.4540 47.474 0.40962E-010.69414E-02 + 1.4540 53.257 0.38845E-010.65827E-02 + 1.4540 59.039 0.15351E-010.44772E-02 + 1.4540 65.545 0.21104E-010.31052E-02 + 1.4540 70.604 0.97787E-020.20768E-02 + 1.4540 75.664 0.13444E-010.19781E-02 + 1.4540 81.447 0.12415E-010.15421E-02 + 1.4540 87.230 0.23466E-010.39765E-02 + 1.4540 90.844 0.18979E-010.23574E-02 + 1.4540 95.904 0.12415E-010.18267E-02 + 1.4540 100.96 0.13443E-010.19780E-02 + 1.4540 105.30 0.95223E-020.16137E-02 + 1.4540 111.08 0.22851E-010.38723E-02 + 1.4540 116.14 0.20550E-010.25526E-02 + 1.4540 121.20 0.13091E-010.27802E-02 + 1.4540 124.82 0.10041E-010.21324E-02 + 1.4540 129.16 0.13091E-010.13178E-02 + 1.4540 132.77 0.10311E-010.17473E-02 + 1.4540 139.28 0.13443E-010.16697E-02 + 1.4540 143.61 0.14947E-010.21993E-02 + 1.4540 148.67 0.18481E-010.27192E-02 + 1.4540 153.01 0.28251E-010.41568E-02 + 1.4540 156.62 0.30591E-010.37998E-02 + 1.4540 160.24 0.42057E-010.61881E-02 + 1.4540 165.30 0.51999E-010.64588E-02 + 1.9740 27.243 0.14705 0.24998E-01 + 1.9740 43.867 0.64433E-010.10953E-01 + 1.9740 48.203 0.38857E-010.48419E-02 + 1.9740 54.710 0.59486E-010.10112E-01 + 1.9740 65.552 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2.5380 62.477 0.20336E-010.34948E-02 + 2.5380 68.223 0.25942E-010.32699E-02 + 2.5380 73.271 0.28153E-010.35450E-02 + 2.5380 78.360 0.23343E-010.29393E-02 + 2.5380 83.416 0.24005E-010.30195E-02 + 2.5380 89.223 0.20450E-010.25750E-02 + 2.5380 100.03 0.26827E-010.33779E-02 + 2.5380 104.42 0.18923E-010.19315E-02 + 2.5380 109.41 0.29140E-010.36691E-02 + 2.5380 114.50 0.24820E-010.31253E-02 + 2.5380 119.52 0.31657E-010.47209E-02 + 2.5380 123.81 0.42603E-010.73161E-02 + 2.5380 128.21 0.27721E-010.34869E-02 + 2.5380 134.04 0.21205E-010.21644E-02 + 2.5380 138.38 0.20660E-010.30811E-02 + 2.5380 142.00 0.19072E-010.24014E-02 + 2.5380 147.83 0.14201E-010.21178E-02 + 2.5380 151.36 0.25693E-010.38317E-02 + 2.5380 155.66 0.32766E-010.33488E-02 + 2.5380 160.60 0.73546E-010.75070E-02 + 2.5380 164.94 0.69755E-010.71199E-02 + 2.5380 169.28 0.71723E-010.90405E-02 + 2.7200 26.860 0.40970E-010.60203E-02 + 2.7200 39.578 0.55023E-010.68160E-02 + 2.7200 43.294 0.36079E-010.60980E-02 + 2.7200 49.755 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2.8400 78.181 0.17934E-010.34319E-02 + 2.8400 83.309 0.13064E-010.19221E-02 + 2.8400 88.318 0.16610E-010.28146E-02 + 2.8400 93.905 0.42099E-010.52288E-02 + 2.8400 99.111 0.21154E-010.26236E-02 + 2.8400 104.18 0.20090E-010.24989E-02 + 2.8400 108.43 0.30749E-010.45240E-02 + 2.8400 112.89 0.17177E-010.29106E-02 + 2.8400 119.33 0.23658E-010.40129E-02 + 2.8400 123.00 0.17689E-010.21971E-02 + 2.8400 128.02 0.21329E-010.26491E-02 + 2.8400 132.27 0.32645E-010.40546E-02 + 2.8400 141.11 0.15165E-010.25723E-02 + 2.8400 144.77 0.12278E-010.23474E-02 + 2.8400 149.72 0.20900E-010.30786E-02 + 2.8400 154.76 0.22070E-010.46904E-02 + 2.8400 158.40 0.19869E-010.15197E-02 + 2.8400 162.03 0.18862E-010.36062E-02 + 2.8400 165.51 0.35685E-010.52440E-02 + 3.0200 26.535 0.64366E-010.11117E-01 + 3.0200 33.259 0.29419E-010.44128E-02 + 3.0200 38.929 0.44264E-010.66290E-02 + 3.0200 44.704 0.45582E-010.78834E-02 + 3.0200 49.215 0.24489E-010.36734E-02 + 3.0200 53.514 0.28088E-010.83368E-02 + 3.0200 61.571 0.19284E-010.64313E-02 + 3.0200 66.646 0.18303E-010.57728E-02 + 3.0200 73.302 0.10675E-010.27527E-02 + 3.0200 77.790 0.62204E-020.19631E-02 + 3.0200 82.729 0.96138E-020.14397E-02 + 3.0200 86.998 0.12289E-010.23913E-02 + 3.0200 92.661 0.18997E-010.28450E-02 + 3.0200 97.977 0.75787E-020.16396E-02 + 3.0200 103.07 0.66319E-020.20917E-02 + 3.0200 107.38 0.74033E-020.11087E-02 + 3.0200 113.73 0.13109E-010.22641E-02 + 3.0200 118.19 0.85130E-020.12769E-02 + 3.0200 122.49 0.95033E-020.16413E-02 + 3.0200 127.53 0.10328E-010.13082E-02 + 3.0200 133.37 0.85636E-020.10868E-02 + 3.0200 134.87 0.68992E-020.87215E-03 + 3.0200 141.32 0.85903E-020.10881E-02 + 3.0200 146.94 0.15206E-010.22846E-02 + 3.0200 154.22 0.12615E-010.24578E-02 + 3.0200 158.59 0.11339E-010.17009E-02 + 3.0200 163.62 0.12662E-010.16006E-02 + 3.0200 167.93 0.13757E-010.26833E-02 + 3.8300 25.504 0.20119 0.45478E-01 + 3.8300 38.435 0.67538E-010.16066E-01 + 3.8300 44.585 0.55377E-010.15035E-01 + 3.8300 56.092 0.42021E-010.95090E-02 + 3.8300 67.347 0.13089E-010.26500E-02 + 3.8300 76.819 0.11216E-010.17185E-02 + 3.8300 82.611 0.11191E-010.18538E-02 + 3.8300 94.474 0.30170E-010.46147E-02 + 3.8300 105.45 0.15234E-010.28975E-02 + 3.8300 109.90 0.10587E-010.14844E-02 + 3.8300 112.55 0.19343E-010.21999E-02 + 3.8300 116.96 0.11560E-010.19134E-02 + 3.8300 127.28 0.10841E-010.13768E-02 + 3.8300 133.02 0.87569E-020.16678E-02 + 3.8300 137.40 0.21300E-010.37944E-02 + 3.8300 139.15 0.29669E-010.33782E-02 + 3.8300 145.69 0.22217E-010.36773E-02 + 3.8300 150.51 0.13275E-010.28478E-02 + 3.8300 155.55 0.17651E-010.29238E-02 + 3.8300 156.90 0.26120E-010.29777E-02 + 3.8300 162.89 0.12070E-010.21517E-02 + 3.8300 167.20 0.22039E-010.41974E-02 + 4.6200 29.703 0.45131E-010.80109E-02 + 4.6200 39.028 0.24261E-010.46044E-02 + 4.6200 51.937 0.82923E-020.17751E-02 + 4.6200 58.226 0.10844E-010.21892E-02 + 4.6200 74.079 0.16668E-010.31634E-02 + 4.6200 86.099 0.17883E-010.36103E-02 + 4.6200 97.009 0.76663E-020.14560E-02 + 4.6200 111.98 0.99899E-020.11328E-02 + 4.6200 122.14 0.54499E-020.90172E-03 + 4.6200 126.22 0.17331E-010.24207E-02 + 4.6200 131.55 0.14878E-010.22692E-02 + 4.6200 135.87 0.26707E-010.57135E-02 + 4.6200 147.77 0.19378E-010.29528E-02 + 4.6200 152.12 0.10282E-010.19528E-02 + 4.6200 156.89 0.20504E-010.31272E-02 + 4.6200 161.08 0.24519E-010.27767E-02 + 4.6200 169.25 0.17551E-010.31202E-02 + 5.4200 25.848 0.78539E-010.13262E-01 + 5.4200 37.677 0.49166E-010.76758E-02 + 5.4200 42.311 0.61813E-010.11997E-01 + 5.4200 51.294 0.44518E-010.86327E-02 + 5.4200 56.455 0.24339E-010.50239E-02 + 5.4200 61.213 0.13727E-010.30044E-02 + 5.4200 68.664 0.13888E-010.21682E-02 + 5.4200 73.908 0.95680E-020.17340E-02 + 5.4200 84.315 0.35835E-010.73908E-02 + 5.4200 89.592 0.27080E-010.38632E-02 + 5.4200 94.265 0.37925E-010.54170E-02 + 5.4200 114.89 0.10124E-010.13113E-02 + 5.4200 120.13 0.21826E-010.33960E-02 + 5.4200 124.62 0.18380E-010.28727E-02 + 5.4200 129.31 0.27377E-010.42646E-02 + 5.4200 131.85 0.10039E-010.13020E-02 + 5.4200 140.73 0.17142E-010.26702E-02 + 5.4200 149.87 0.19303E-010.30069E-02 + 7.2000 30.215 0.81346 0.12599 + 7.2000 38.858 0.66498 0.11153 + 7.2000 47.884 0.47362 0.73459E-01 + 7.2000 54.062 0.41827 0.53801E-01 + 7.2000 59.839 0.39274 0.50475E-01 + 7.2000 65.204 0.36882 0.47441E-01 + 7.2000 70.544 0.31118 0.40062E-01 + 7.2000 76.284 0.24694 0.31791E-01 +ENDDATA 273 +ENDSUBENT 284 +SUBENT F0655006 20050609 20050831 F022 +BIB 2 2 +REACTION (14-SI-28(A,P)15-P-31,PAR,DA) +STATUS (CURVE)Fig.6(a,b,c,d,e) +ENDBIB 2 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.69 +ENDCOMMON 3 +DATA 4 318 +E-LVL ANG-CM DATA-CM DATA-ERR2 +MEV ADEG MB/SR MB/SR + 0.0000 29.176 0.11442 0.11178E-01 + 0.0000 34.772 0.86192E-010.12318E-01 + 0.0000 41.036 0.37834E-010.62305E-02 + 0.0000 43.792 0.16612E-010.34305E-02 + 0.0000 49.342 0.59367E-020.18999E-02 + 0.0000 53.564 0.71049E-020.17501E-02 + 0.0000 59.160 0.53520E-020.17130E-02 + 0.0000 64.779 0.57785E-020.16422E-02 + 0.0000 69.718 0.89430E-020.16628E-02 + 0.0000 74.598 0.53451E-020.99407E-03 + 0.0000 79.528 0.70896E-020.16075E-02 + 0.0000 90.012 0.36299E-020.10314E-02 + 0.0000 106.12 0.22240E-020.50406E-03 + 0.0000 110.32 0.19054E-020.46941E-03 + 0.0000 115.26 0.28739E-020.34672E-03 + 0.0000 120.84 0.17624E-020.59435E-03 + 0.0000 128.55 0.14338E-020.23625E-03 + 0.0000 134.17 0.15883E-020.26172E-03 + 0.0000 148.20 0.15462E-020.46744E-03 + 0.0000 169.28 0.22699E-020.55904E-03 + 1.2660 26.429 0.64128E-010.97867E-02 + 1.2660 31.384 0.81161E-010.13994E-01 + 1.2660 35.521 0.54239E-010.10395E-01 + 1.2660 41.737 0.31437E-010.60361E-02 + 1.2660 47.351 0.31400E-010.66186E-02 + 1.2660 52.843 0.16172E-010.39967E-02 + 1.2660 57.682 0.10806E-010.26706E-02 + 1.2660 61.970 0.16528E-010.34818E-02 + 1.2660 66.799 0.10533E-010.18187E-02 + 1.2660 84.355 0.11267E-010.25815E-02 + 1.2660 88.487 0.73535E-020.18174E-02 + 1.2660 92.624 0.49142E-020.11259E-02 + 1.2660 103.06 0.30551E-020.46625E-03 + 1.2660 108.89 0.99591E-020.11110E-02 + 1.2660 113.17 0.14189E-010.24448E-02 + 1.2660 117.39 0.15219E-010.23226E-02 + 1.2660 123.71 0.15563E-010.20594E-02 + 1.2660 129.23 0.92377E-020.14098E-02 + 1.2660 134.73 0.48715E-020.74284E-03 + 1.2660 138.89 0.38419E-020.58631E-03 + 1.2660 145.89 0.34899E-020.80000E-03 + 1.2660 152.30 0.57279E-020.12054E-02 + 1.2660 157.31 0.96290E-020.16603E-02 + 1.2660 162.20 0.85461E-020.95337E-03 + 1.2660 167.11 0.85374E-020.11308E-02 + 2.2340 26.168 0.23515E-010.53291E-02 + 2.2340 32.481 0.22900E-010.65028E-02 + 2.2340 35.929 0.12037E-010.31960E-02 + 2.2340 41.533 0.10853E-010.32812E-02 + 2.2340 47.094 0.61606E-020.21815E-02 + 2.2340 54.055 0.34076E-020.14718E-02 + 2.2340 59.035 0.69951E-020.18568E-02 + 2.2340 64.003 0.12627E-010.26091E-02 + 2.2340 68.864 0.73550E-020.15187E-02 + 2.2340 73.798 0.92639E-020.21001E-02 + 2.2340 84.314 0.83475E-020.15511E-02 + 2.2340 94.803 0.56690E-020.93364E-03 + 2.2340 100.37 0.35664E-020.58736E-03 + 2.2340 104.64 0.62752E-020.12962E-02 + 2.2340 109.58 0.83209E-020.20496E-02 + 2.2340 114.48 0.75031E-020.12357E-02 + 2.2340 118.01 0.92123E-020.17132E-02 + 2.2340 125.01 0.83047E-020.11871E-02 + 2.2340 129.19 0.59422E-020.71675E-03 + 2.2340 134.80 0.56404E-020.11651E-02 + 2.2340 138.28 0.39338E-020.64786E-03 + 2.2340 144.64 0.64061E-020.13237E-02 + 2.2340 149.55 0.62396E-020.11599E-02 + 2.2340 153.77 0.72764E-020.11984E-02 + 2.2340 158.67 0.60743E-020.10004E-02 + 2.2340 162.88 0.62291E-020.11579E-02 + 2.2340 167.77 0.52000E-020.96664E-03 + 3.1340 23.118 0.17248E-010.31987E-02 + 3.1340 40.497 0.51521E-020.17333E-02 + 3.1340 53.135 0.54107E-020.13292E-02 + 3.1340 60.780 0.31536E-020.83524E-03 + 3.1340 66.481 0.59807E-020.98262E-03 + 3.1340 113.39 0.28191E-020.69229E-03 + 3.1340 122.51 0.27432E-020.56503E-03 + 3.1340 128.16 0.35414E-020.87000E-03 + 3.1340 132.27 0.16823E-020.38050E-03 + 3.1340 137.15 0.13691E-020.33634E-03 + 3.1340 142.09 0.16368E-020.57831E-03 + 3.1340 150.66 0.47977E-020.68412E-03 + 3.1340 155.60 0.58848E-020.96687E-03 + 3.1340 159.89 0.10605E-010.12761E-02 + 3.1340 165.45 0.70292E-020.14485E-02 + 3.2950 27.388 0.18395E-010.33530E-02 + 3.2950 37.043 0.18377E-010.33508E-02 + 3.2950 47.415 0.26110E-010.47593E-02 + 3.2950 57.717 0.14994E-010.27331E-02 + 3.2950 63.149 0.49524E-020.16414E-02 + 3.2950 66.642 0.88311E-020.14268E-02 + 3.2950 71.524 0.17856E-010.28849E-02 + 3.2950 78.305 0.40431E-020.11278E-02 + 3.2950 82.506 0.90414E-020.21861E-02 + 3.2950 86.003 0.16955E-010.34369E-02 + 3.2950 107.20 0.15493E-020.72341E-03 + 3.2950 122.46 0.49222E-020.12832E-02 + 3.2950 127.96 0.40224E-020.89488E-03 + 3.2950 132.76 0.26879E-020.49012E-03 + 3.2950 136.91 0.32043E-020.64919E-03 + 3.2950 143.14 0.42234E-020.77010E-03 + 3.2950 149.37 0.60032E-020.96953E-03 + 3.2950 155.63 0.11254E-010.22807E-02 + 3.2950 165.28 0.11243E-010.22785E-02 + 3.4150 24.721 0.24478E-010.49851E-02 + 3.4150 35.751 0.27793E-010.50930E-02 + 3.4150 53.688 0.23301E-010.47464E-02 + 3.4150 57.838 0.16354E-010.26545E-02 + 3.4150 61.305 0.93741E-020.27962E-02 + 3.4150 66.834 0.65795E-020.14709E-02 + 3.4150 77.865 0.72839E-020.14836E-02 + 3.4150 81.311 0.78596E-020.16006E-02 + 3.4150 86.131 0.98717E-020.13904E-02 + 3.4150 101.33 0.39728E-020.96519E-03 + 3.4150 105.47 0.37775E-020.84454E-03 + 3.4150 110.99 0.41808E-020.10157E-02 + 3.4150 126.13 0.91666E-020.16797E-02 + 3.4150 130.27 0.89392E-020.18203E-02 + 3.4150 136.47 0.12743E-010.25951E-02 + 3.4150 140.60 0.16004E-010.32590E-02 + 3.4150 144.75 0.11233E-010.20586E-02 + 3.4150 151.63 0.17718E-010.32467E-02 + 3.4150 155.78 0.12435E-010.25321E-02 + 3.5060 25.778 0.33949E-010.70524E-02 + 3.5060 42.940 0.88317E-020.16509E-02 + 3.5060 51.948 0.18208E-010.34045E-02 + 3.5060 56.724 0.75535E-020.10859E-02 + 3.5060 62.907 0.49909E-020.82661E-03 + 3.5060 66.369 0.62974E-020.13079E-02 + 3.5060 78.084 0.53869E-020.10070E-02 + 3.5060 83.601 0.53845E-020.10065E-02 + 3.5060 93.934 0.43742E-020.62883E-03 + 3.5060 102.91 0.55168E-020.11458E-02 + 3.5060 109.82 0.61147E-020.10127E-02 + 3.5060 116.71 0.56549E-020.81294E-03 + 3.5060 129.14 0.73168E-020.10522E-02 + 3.5060 135.34 0.71263E-020.13321E-02 + 3.5060 143.61 0.59420E-020.85421E-03 + 3.5060 148.42 0.44687E-020.11925E-02 + 3.5060 158.82 0.12244E-010.27903E-02 + 3.5060 165.04 0.13928E-010.26042E-02 + 4.4310 39.500 0.13473 0.32121E-01 + 4.4310 44.896 0.11614 0.16033E-01 + 4.4310 49.611 0.14515 0.26084E-01 + 4.4310 55.008 0.11617 0.10954E-01 + 4.4310 59.729 0.10523 0.18910E-01 + 4.4310 65.795 0.10788 0.19386E-01 + 4.4310 69.843 0.93001E-010.12840E-01 + 4.4310 73.222 0.58106E-010.80205E-02 + 4.4310 79.286 0.67422E-010.13467E-01 + 4.4310 84.007 0.61071E-010.10974E-01 + 4.4310 89.410 0.36315E-010.65249E-02 + 4.4310 93.458 0.29064E-010.40122E-02 + 4.4310 98.859 0.19082E-010.30358E-02 + 4.4310 108.96 0.32906E-010.52367E-02 + 4.4310 119.75 0.23273E-010.32128E-02 + 4.4310 123.79 0.29814E-010.41158E-02 + 4.4310 129.86 0.30566E-010.35591E-02 + 4.4310 139.29 0.37270E-010.51445E-02 + 4.4310 144.69 0.42187E-010.49129E-02 + 4.4310 148.73 0.45444E-010.52909E-02 + 4.6340 25.650 0.33786E-010.55629E-02 + 4.6340 36.440 0.41486E-010.59298E-02 + 4.6340 42.491 0.19681E-010.48480E-02 + 4.6340 47.223 0.35544E-010.42865E-02 + 4.6340 51.261 0.26785E-010.38286E-02 + 4.6340 57.316 0.14826E-010.21189E-02 + 4.6340 61.369 0.22367E-010.31971E-02 + 4.6340 65.413 0.21243E-010.34985E-02 + 4.6340 70.123 0.14444E-010.23790E-02 + 4.6340 76.202 0.24149E-010.44894E-02 + 4.6340 81.593 0.22353E-010.36808E-02 + 4.6340 86.986 0.22349E-010.31940E-02 + 4.6340 132.82 0.14049E-010.26116E-02 + 4.6340 148.33 0.19615E-010.36458E-02 + 4.6340 150.34 0.14407E-010.26784E-02 + 4.6340 159.78 0.15558E-010.28920E-02 + 4.6340 165.18 0.19604E-010.36438E-02 + 4.7830 28.303 0.30930E-010.80299E-02 + 4.7830 37.059 0.59332E-010.13147E-01 + 4.7830 62.026 0.80018E-020.20773E-02 + 4.7830 76.863 0.47298E-020.13146E-02 + 4.7830 91.006 0.15355E-010.36981E-02 + 4.7830 97.071 0.17847E-010.39544E-02 + 4.7830 102.47 0.14246E-010.28753E-02 + 4.7830 107.19 0.12570E-010.25373E-02 + 4.7830 111.25 0.36839E-020.81625E-03 + 4.7830 126.07 0.56410E-020.90718E-03 + 4.7830 131.46 0.90800E-020.16488E-02 + 4.7830 137.53 0.80120E-020.14549E-02 + 4.7830 140.89 0.13902E-010.16366E-02 + 4.7830 148.31 0.11379E-010.15880E-02 + 4.7830 149.65 0.22947E-010.21875E-02 + 4.7830 159.09 0.19260E-010.26877E-02 + 4.7830 165.17 0.10043E-010.20269E-02 + 5.3430 40.088 0.32430E-010.83353E-02 + 5.3430 49.521 0.30082E-010.71703E-02 + 5.3430 60.337 0.46927E-010.11187E-01 + 5.3430 63.675 0.29309E-010.64291E-02 + 5.3430 69.073 0.31553E-010.43556E-02 + 5.3430 75.757 0.13589E-010.21623E-02 + 5.3430 81.194 0.25855E-010.61626E-02 + 5.3430 87.247 0.21197E-010.38066E-02 + 5.3430 93.319 0.22819E-010.45568E-02 + 5.3430 97.336 0.14974E-010.35706E-02 + 5.3430 104.04 0.91209E-020.20003E-02 + 5.3430 116.87 0.12569E-010.27572E-02 + 5.3430 124.30 0.14937E-010.23776E-02 + 5.3430 129.01 0.12870E-010.23125E-02 + 5.3430 133.73 0.12550E-010.22550E-02 + 5.3430 143.18 0.15669E-010.24932E-02 + 5.3430 147.20 0.11929E-010.18981E-02 + 5.3430 153.98 0.20553E-010.23942E-02 + 5.3430 160.71 0.16850E-010.40162E-02 + 5.7730 42.153 0.25158E-010.58869E-02 + 5.7730 56.930 0.16226E-010.34933E-02 + 5.7730 62.413 0.33540E-010.72209E-02 + 5.7730 81.981 0.38667E-010.83215E-02 + 5.7730 93.411 0.30290E-010.59355E-02 + 5.7730 97.387 0.17336E-010.33972E-02 + 5.7730 106.85 0.21529E-010.33610E-02 + 5.7730 113.48 0.89880E-020.14024E-02 + 5.7730 123.63 0.12002E-010.18715E-02 + 5.7730 128.40 0.17250E-010.26899E-02 + 5.7730 133.04 0.96355E-020.18881E-02 + 5.7730 143.20 0.13837E-010.29766E-02 + 5.7730 147.88 0.98483E-020.23053E-02 + 5.7730 160.10 0.19848E-010.38911E-02 + 5.7730 164.87 0.31431E-010.61592E-02 + 6.2330 29.251 0.46377E-010.10419E-01 + 6.2330 35.331 0.49985E-010.10237E-01 + 6.2330 40.659 0.34072E-010.76634E-02 + 6.2330 56.838 0.33938E-010.62546E-02 + 6.2330 70.164 0.13526E-010.30406E-02 + 6.2330 80.372 0.23626E-010.53139E-02 + 6.2330 91.075 0.14526E-010.29749E-02 + 6.2330 100.44 0.94007E-020.22976E-02 + 6.2330 105.95 0.18201E-010.29715E-02 + 6.2330 111.89 0.86851E-020.15994E-02 + 6.2330 125.46 0.15158E-010.39925E-02 + 6.2330 130.78 0.93317E-020.20989E-02 + 6.2330 136.19 0.10585E-010.27880E-02 + 6.2330 145.78 0.26410E-010.54054E-02 + 6.9320 35.903 0.23686 0.38255E-01 + 6.9320 41.285 0.16649 0.30359E-01 + 6.9320 46.671 0.13271 0.29526E-01 + 6.9320 50.695 0.68974E-010.13979E-01 + 6.9320 60.828 0.13263 0.21421E-01 + 6.9320 65.546 0.12931 0.15288E-01 + 6.9320 81.034 0.76176E-010.13893E-01 + 6.9320 86.442 0.11980 0.16785E-01 + 6.9320 91.122 0.34900E-010.48910E-02 + 6.9320 95.177 0.48398E-010.78181E-02 + 6.9320 100.57 0.43753E-010.88674E-02 + 6.9320 105.96 0.48375E-010.67795E-02 + 6.9320 110.69 0.63790E-010.89397E-02 + 6.9320 120.81 0.76043E-010.89887E-02 + 6.9320 125.53 0.97783E-010.15793E-01 + 6.9320 130.92 0.76010E-010.12276E-01 + 6.9320 140.36 0.86166E-010.10187E-01 + 6.9320 145.08 0.77898E-010.10917E-01 + 6.9320 149.13 0.92887E-010.88972E-02 + 6.9320 153.16 0.70414E-010.98680E-02 + 6.9320 157.22 0.88296E-010.10439E-01 + 6.9320 163.29 0.95195E-010.91183E-02 + 7.2140 37.807 0.32149E-010.75421E-02 + 7.2140 42.420 0.58999E-010.12487E-01 + 7.2140 47.577 0.45735E-010.91343E-02 + 7.2140 52.552 0.73417E-010.15529E-01 + 7.2140 62.106 0.51198E-010.10232E-01 + 7.2140 76.993 0.13167E-010.39483E-02 + 7.2140 90.427 0.21379E-010.50155E-02 + 7.2140 95.714 0.25495E-010.38430E-02 + 7.2140 106.75 0.11722E-010.23396E-02 + 7.2140 128.70 0.23005E-010.43192E-02 + 7.2140 143.29 0.32180E-010.60461E-02 + 7.2140 148.43 0.23506E-010.35432E-02 + 7.2140 152.14 0.30665E-010.38371E-02 + 7.2140 156.20 0.34993E-010.48249E-02 + 7.2140 161.41 0.31940E-010.35832E-02 + 7.2140 166.19 0.27072E-010.40807E-02 + 8.0320 36.817 0.17323 0.28161E-01 + 8.0320 47.034 0.98311E-010.17167E-01 + 8.0320 57.464 0.22314 0.41660E-01 + 8.0320 67.317 0.13838 0.22383E-01 + 8.0320 85.335 0.44630E-010.77667E-02 + 8.0320 90.568 0.44491E-010.72146E-02 + 8.0320 95.329 0.15342E-010.40852E-02 + 8.0320 123.02 0.31085E-010.42613E-02 + 8.0320 128.25 0.30988E-010.42480E-02 + 8.0320 133.31 0.20747E-010.45919E-02 + 8.0320 142.89 0.42492E-010.47368E-02 + 8.0320 147.79 0.49101E-010.79523E-02 + 8.0320 156.79 0.68560E-010.11118E-01 + 8.0320 160.36 0.59910E-010.89694E-02 + 8.0320 166.23 0.10303 0.26348E-01 + 8.8400 38.621 0.69666 0.78389E-01 + 8.8400 42.476 0.39482 0.79026E-01 + 8.8400 47.710 0.39397 0.78804E-01 + 8.8400 52.008 0.25527 0.48133E-01 + 8.8400 57.563 0.19477 0.31890E-01 + 8.8400 62.551 0.85637E-010.11855E-01 + 8.8400 68.200 0.89344E-010.18940E-01 + 8.8400 74.127 0.61405E-010.10054E-01 + 8.8400 79.226 0.39186E-010.49179E-02 + 8.8400 83.739 0.51915E-010.51576E-02 + 8.8400 109.83 0.39866E-010.70095E-02 + 8.8400 117.70 0.21893E-010.35907E-02 + 8.8400 122.00 0.54242E-010.10213E-01 + 8.8400 126.70 0.35141E-010.48747E-02 + 8.8400 132.51 0.61760E-010.12354E-01 + 8.8400 137.25 0.45076E-010.73805E-02 + 8.8400 142.10 0.49194E-010.86631E-02 + 8.8400 147.56 0.27449E-010.44905E-02 + 8.8400 152.66 0.66978E-010.83962E-02 + 8.8400 154.88 0.34221E-010.60264E-02 +ENDDATA 320 +ENDSUBENT 331 +ENDENTRY 6 diff --git a/exforall/F06/F0658.x4 b/exforall/F06/F0658.x4 new file mode 100644 index 000000000..9e5f4ac09 --- /dev/null +++ b/exforall/F06/F0658.x4 @@ -0,0 +1,494 @@ +ENTRY F0658 20050617 20050831 F022 +SUBENT F0658001 20050617 20050831 F022 +BIB 10 30 +TITLE Resonances in low energy elastic scattering of alpha + particles from 28Si. +AUTHOR (J.J.Lawrie,A.A.Cowley,D.M.Whittal,S.J.Mills, + W.R.McMurray) +INSTITUTE (3SAFITH) +REFERENCE (J,ZP/A,325,175,1986) +FACILITY (VDG) 6 MV +DETECTOR (SI) The 100 mu silicon detectors mounted on + rotatable arms, with an angular accuracy of 0.1 degr. + Circular detector collimators subtended a solid angle + of 0.5 msr with an angular acceptance of 0.8 degr. +SAMPLE The target consisted of 250 mu-g/cm2 natural silicon + evaporated onto a backing consisting of a 40 mu-g/cm2 + gold layer on a KAPTON film. +MONITOR Forward angle elastic scattering from a thin gold + target, measured on both sides of the beam, was used to + determine the angular offset of the angle + determinations. + Rutherford scattering from the thin gold layer + sandwiched between the silicon target material and the + KAPTON backing, was used to monitor the total incident + flux. +ERR-ANALYS (ERR-S)Statistical error + (ERR-SYS)Systematic error in the measured cross section + values, which is mainly due to uncertainties in the + silicon and gold target thicknesses. + (DATA-ERR)The experimental error bars represent + statistical errors only. + (ERR-DIG)Digitizing error +HISTORY (20040309C) +ENDBIB 30 +COMMON 3 3 +ERR-S ERR-SYS ERR-DIG +PER-CENT PER-CENT NO-DIM + 5.0 10.0 0.01 +ENDCOMMON 3 +ENDSUBENT 37 +SUBENT F0658002 20050617 20050831 F022 +BIB 3 3 +REACTION (14-SI-28(A,EL)14-SI-28,,DA,,RTH) +ERR-ANALYS (EN-ERR-DIG)Digitizing error +STATUS (CURVE)Fig.2 +ENDBIB 3 +COMMON 1 3 +EN-ERR-DIG +MEV + 0.02 +ENDCOMMON 3 +DATA 4 284 +ANG-CM EN-CM DATA-CM DATA-ERR +ADEG MEV NO-DIM NO-DIM + 78.000 4.3879 1.0732 0.60799E-01 + 78.000 4.4666 1.0884 0.60799E-01 + 78.000 4.5612 1.0885 0.55724E-01 + 78.000 4.6402 1.0581 0.55724E-01 + 78.000 4.7348 1.0633 0.65855E-01 + 78.000 4.8295 1.0430 0.45592E-01 + 78.000 4.9081 1.0735 0.50658E-01 + 78.000 5.0025 1.1039 0.65855E-01 + 78.000 5.0973 1.0787 0.55724E-01 + 78.000 5.1760 1.0990 0.55733E-01 + 78.000 5.2396 1.0028 0.55724E-01 + 78.000 5.3342 1.0079 0.55714E-01 + 78.000 5.4275 1.2156 0.75987E-01 + 78.000 5.5222 1.2106 0.65855E-01 + 78.000 5.6022 1.0131 0.55724E-01 + 78.000 5.7123 1.0537 0.60809E-01 + 78.000 5.8068 1.0740 0.75997E-01 + 78.000 5.8717 0.74987 0.40526E-01 + 78.000 5.9680 0.47131 0.30395E-01 + 78.000 6.0461 0.59293 0.30395E-01 + 78.000 6.1548 0.87162 0.60799E-01 + 78.000 6.2330 0.97805 0.60799E-01 + 78.000 6.3278 0.94265 0.50668E-01 + 78.000 6.3924 0.68433 0.45583E-01 + 78.000 6.4855 0.93768 0.50668E-01 + 78.000 6.5807 0.84149 0.45592E-01 + 78.000 6.6458 0.49199 0.40517E-01 + 78.000 6.7404 0.49204 0.35461E-01 + 78.000 6.8510 0.45665 0.25339E-01 + 78.000 6.9148 0.31991 0.30395E-01 + 78.000 7.0085 0.48208 0.35461E-01 + 78.000 7.1027 0.54293 0.30395E-01 + 78.000 7.1805 0.72028 0.35470E-01 + 78.000 7.2750 0.73047 0.45592E-01 + 78.000 7.3533 0.81157 0.45592E-01 + 78.000 7.4654 0.52288 0.30395E-01 + 78.000 7.5444 0.49254 0.35451E-01 + 78.000 7.6082 0.38113 0.25329E-01 + 78.000 7.7168 0.66488 0.30395E-01 + 78.000 7.7966 0.49776 0.35451E-01 + 78.000 7.8915 0.45222 0.30395E-01 + 78.000 7.9854 0.57386 0.30395E-01 + 78.000 8.0654 0.36621 0.25339E-01 + 78.000 8.1442 0.37133 0.20254E-01 + 78.000 8.2391 0.32579 0.15207E-01 + 78.000 8.3173 0.42716 0.25329E-01 + 78.000 8.4284 0.31578 0.20273E-01 + 78.000 8.5219 0.48807 0.30404E-01 + 78.000 8.5864 0.25508 0.20273E-01 + 78.000 8.6801 0.39698 0.20254E-01 + 78.000 8.7738 0.55915 0.35461E-01 + 78.000 8.8544 0.26031 0.15207E-01 + 78.000 8.9495 0.16919 0.10132E-01 + 78.000 9.0423 0.46813 0.35470E-01 + 78.000 9.1209 0.50364 0.30385E-01 + 78.000 9.2321 0.37199 0.25339E-01 + 78.000 9.2960 0.22512 0.15188E-01 + 78.000 9.3595 0.15931 0.10132E-01 + 78.000 9.4678 0.49878 0.25329E-01 + 78.000 9.5621 0.54950 0.20263E-01 + 78.000 9.6572 0.45837 0.30395E-01 + 78.000 9.7519 0.43817 0.30404E-01 + 78.000 9.8160 0.27610 0.25329E-01 + 78.000 9.9111 0.17991 0.15207E-01 + 78.000 9.9736 0.28126 0.25329E-01 + 78.000 10.084 0.19015 0.15197E-01 + 78.000 10.148 0.12433 0.15197E-01 + 78.000 10.256 0.51447 0.30395E-01 + 78.000 10.320 0.27135 0.20263E-01 + 78.000 10.416 0.11943 0.20273E-01 + 78.000 10.507 0.70205 0.45592E-01 + 98.000 4.4113 0.99896 0.54259E-01 + 98.000 4.4747 1.0260 0.74627E-01 + 98.000 4.5854 1.0056 0.67813E-01 + 98.000 4.6644 0.97837 0.74627E-01 + 98.000 4.7432 0.92403 0.40706E-01 + 98.000 4.8229 1.0325 0.67857E-01 + 98.000 4.9179 1.0392 0.61058E-01 + 98.000 4.9963 0.90344 0.61073E-01 + 98.000 5.1067 0.82193 0.47490E-01 + 98.000 5.2015 0.80148 0.47475E-01 + 98.000 5.2649 0.81499 0.40706E-01 + 98.000 5.3609 1.0184 0.54289E-01 + 98.000 5.4396 0.93017 0.54274E-01 + 98.000 5.5335 0.71976 0.61058E-01 + 98.000 5.6121 0.61793 0.40720E-01 + 98.000 5.7075 0.70603 0.40706E-01 + 98.000 5.7853 0.44816 0.33921E-01 + 98.000 5.8635 0.27169 0.33907E-01 + 98.000 5.9762 0.65151 0.47475E-01 + 98.000 6.0734 1.0992 0.67828E-01 + 98.000 6.1520 0.99735 0.61058E-01 + 98.000 6.2476 1.1262 0.54274E-01 + 98.000 6.3240 0.57656 0.33907E-01 + 98.000 6.4204 0.87498 0.47490E-01 + 98.000 6.4835 0.82065 0.47475E-01 + 98.000 6.5600 0.30497 0.20353E-01 + 98.000 6.6564 0.58982 0.40706E-01 + 98.000 6.7671 0.58972 0.40691E-01 + 98.000 6.8458 0.49467 0.33921E-01 + 98.000 6.9251 0.53530 0.33921E-01 + 98.000 7.0208 0.67768 0.33921E-01 + 98.000 7.0990 0.50800 0.40706E-01 + 98.000 7.1619 0.42653 0.27152E-01 + 98.000 7.2569 0.43323 0.40706E-01 + 98.000 7.3513 0.31780 0.27152E-01 + 98.000 7.4463 0.32450 0.27137E-01 + 98.000 7.5407 0.21586 0.67842E-02 + 98.000 7.6364 0.37181 0.20353E-01 + 98.000 7.7160 0.45994 0.33907E-01 + 98.000 7.7941 0.26312 0.13554E-01 + 98.000 7.8907 0.58189 0.40720E-01 + 98.000 8.0019 0.67677 0.47475E-01 + 98.000 8.0809 0.65634 0.33907E-01 + 98.000 8.1594 0.52737 0.33921E-01 + 98.000 8.2386 0.53408 0.27122E-01 + 98.000 8.3491 0.47970 0.33921E-01 + 98.000 8.4278 0.39822 0.27122E-01 + 98.000 8.5249 0.82554 0.40691E-01 + 98.000 8.5859 0.37093 0.33921E-01 + 98.000 8.6803 0.26908 0.20353E-01 + 98.000 8.7760 0.40468 0.33921E-01 + 98.000 8.8719 0.60812 0.33921E-01 + 98.000 8.9840 0.86582 0.54259E-01 + 98.000 9.0481 1.0286 0.54289E-01 + 98.000 9.1432 1.0556 0.61058E-01 + 98.000 9.2216 0.91309 0.47519E-01 + 98.000 9.3163 0.86551 0.47490E-01 + 98.000 9.3937 0.52622 0.27122E-01 + 98.000 9.4556 0.23444 0.13569E-01 + 98.000 9.5688 0.72281 0.40706E-01 + 98.000 9.6466 0.45815 0.33936E-01 + 98.000 9.7251 0.34274 0.20368E-01 + 98.000 9.8205 0.42406 0.33921E-01 + 98.000 9.9007 0.64787 0.33921E-01 + 98.000 9.9810 0.86489 0.33936E-01 + 98.000 10.091 0.72232 0.27137E-01 + 98.000 10.205 1.3260 0.74612E-01 + 98.000 10.266 0.84428 0.54274E-01 + 98.000 10.344 0.74244 0.54274E-01 + 98.000 10.441 1.0544 0.67828E-01 + 98.000 10.553 1.2579 0.61029E-01 + 133.00 4.3683 1.1554 0.67839E-01 + 133.00 4.4484 1.1549 0.67839E-01 + 133.00 4.5444 1.1408 0.81316E-01 + 133.00 4.6243 1.1268 0.81407E-01 + 133.00 4.7200 1.0720 0.81407E-01 + 133.00 4.7994 0.99010 0.67839E-01 + 133.00 4.8955 0.98955 0.54181E-01 + 133.00 4.9761 1.0569 0.67839E-01 + 133.00 5.0722 1.0564 0.67748E-01 + 133.00 5.1681 1.0423 0.54181E-01 + 133.00 5.2311 0.90624 0.67839E-01 + 133.00 5.3287 1.0956 0.81407E-01 + 133.00 5.4077 0.95951 0.54181E-01 + 133.00 5.4873 0.90478 0.40704E-01 + 133.00 5.5851 1.1213 0.81407E-01 + 133.00 5.6805 1.0258 0.81316E-01 + 133.00 5.7756 0.90315 0.40613E-01 + 133.00 5.8408 1.0520 0.67839E-01 + 133.00 5.9496 0.63079 0.40613E-01 + 133.00 6.0451 0.56241 0.27045E-01 + 133.00 6.1265 0.72477 0.40613E-01 + 133.00 6.1911 0.79224 0.54271E-01 + 133.00 6.2879 0.88667 0.54271E-01 + 133.00 6.3978 0.60111 0.40704E-01 + 133.00 6.4601 0.38366 0.40704E-01 + 133.00 6.5567 0.45096 0.27045E-01 + 133.00 6.6367 0.43694 0.27136E-01 + 133.00 6.7328 0.43639 0.27136E-01 + 133.00 6.8307 0.66650 0.40704E-01 + 133.00 6.9124 0.88313 0.54272E-01 + 133.00 6.9925 0.88268 0.54272E-01 + 133.00 7.0909 1.1806 0.67839E-01 + 133.00 7.1758 1.7907 0.94975E-01 + 133.00 7.2399 1.7904 0.12220 + 133.00 7.3430 0.65002 0.54271E-01 + 133.00 7.4377 0.47310 0.27136E-01 + 133.00 7.5189 0.62189 0.27136E-01 + 133.00 7.6001 0.75711 0.27136E-01 + 133.00 7.6773 2.4256 0.14925 + 133.00 7.7945 1.0409 0.81407E-01 + 133.00 7.8881 0.72834 0.40704E-01 + 133.00 7.9512 0.60587 0.40704E-01 + 133.00 8.0455 0.38824 0.27136E-01 + 133.00 8.1591 0.57755 0.40704E-01 + 133.00 8.2126 1.2692 0.94975E-01 + 133.00 8.3044 0.72598 0.40704E-01 + 133.00 8.4148 0.50826 0.40613E-01 + 133.00 8.4886 1.7426 0.94884E-01 + 133.00 8.5664 1.4572 0.95066E-01 + 133.00 8.6507 1.9859 0.13559 + 133.00 8.7521 0.62846 0.40704E-01 + 133.00 8.8497 0.81787 0.67748E-01 + 133.00 8.9349 1.4687 0.10854 + 133.00 9.0104 0.89836 0.67930E-01 + 133.00 9.1068 0.93852 0.54181E-01 + 133.00 9.2002 0.59878 0.54272E-01 + 133.00 9.3022 1.3445 0.94975E-01 + 133.00 9.3724 2.1175 0.13568 + 133.00 9.4760 1.0450 0.54272E-01 + 133.00 9.5704 0.82734 0.67839E-01 + 133.00 9.6522 1.0440 0.81498E-01 + 133.00 9.7286 0.58221 0.54181E-01 + 133.00 9.8063 0.28327 0.27136E-01 + 133.00 9.9202 0.51328 0.54272E-01 + 133.00 9.9895 1.1777 0.81316E-01 + 133.00 10.079 0.32243 0.40704E-01 + 133.00 10.165 1.0818 0.10854 + 133.00 10.258 0.66062 0.40704E-01 + 133.00 10.329 1.5829 0.54271E-01 + 133.00 10.436 0.97168 0.54181E-01 + 133.00 10.498 2.6538 0.16281 + 170.00 4.3529 1.2105 + 170.00 4.4487 1.3435 + 170.00 4.5286 1.4769 + 170.00 4.6242 1.2034 + 170.00 4.7044 2.2854 + 170.00 4.7840 1.8768 + 170.00 4.8795 1.3323 + 170.00 4.9912 1.3294 + 170.00 5.0551 1.4633 + 170.00 5.1508 1.1898 + 170.00 5.2308 2.0008 + 170.00 5.3268 2.5403 + 170.00 5.4063 1.7252 + 170.00 5.4858 1.1811 + 170.00 5.5656 1.1791 + 170.00 5.6773 1.0407 + 170.00 5.7731 1.3092 + 170.00 5.8372 1.9850 + 170.00 5.9496 3.8792 0.54242 + 170.00 6.0460 5.9092 0.81219 + 170.00 6.1085 2.1135 + 170.00 6.2043 2.3820 + 170.00 6.2839 1.7025 + 170.00 6.3799 2.5130 + 170.00 6.4756 2.5105 + 170.00 6.5557 3.1860 + 170.00 6.6531 7.7906 0.54159 + 170.00 6.7489 8.0591 0.81343 + 170.00 6.8281 6.5665 0.67710 + 170.00 6.9092 10.087 0.67751 + 170.00 6.9870 4.5298 + 170.00 7.0819 2.3593 + 170.00 7.1798 8.3189 0.81301 + 170.00 7.2597 8.5879 0.81301 + 170.00 7.3401 10.347 0.67792 + 170.00 7.4354 8.9898 0.67751 + 170.00 7.5343 17.930 1.0844 + 170.00 7.6141 17.928 1.2195 + 170.00 7.7077 12.099 0.94893 + 170.00 7.8026 9.6578 0.94810 + 170.00 7.9011 17.379 0.94810 + 170.00 7.9637 13.854 0.94851 + 170.00 8.0558 3.8246 + 170.00 8.1534 8.9712 0.67751 + 170.00 8.2159 5.3110 + 170.00 8.3115 4.9020 + 170.00 8.4236 6.1186 0.81219 + 170.00 8.4896 12.079 0.94851 + 170.00 8.6023 14.786 0.81301 + 170.00 8.6806 10.584 0.94852 + 170.00 8.7619 15.053 0.94851 + 170.00 8.8556 9.2240 0.54242 + 170.00 8.9521 11.390 0.94851 + 170.00 9.0485 13.284 0.81260 + 170.00 9.1102 7.1849 0.40692 + 170.00 9.2217 6.6400 + 170.00 9.3161 3.1145 + 170.00 9.3815 7.3134 + 170.00 9.4786 11.240 0.67792 + 170.00 9.5738 9.7474 0.81343 + 170.00 9.6712 14.217 0.81301 + 170.00 9.7662 12.317 0.94810 + 170.00 9.8145 13.400 0.94852 + 170.00 9.9428 15.158 0.94769 + 170.00 10.022 13.936 0.81260 + 170.00 10.084 7.2952 0.81343 + 170.00 10.179 7.4282 + 170.00 10.276 11.084 0.67751 + 170.00 10.349 34.660 2.1680 + 170.00 10.442 27.611 1.7611 + 170.00 10.533 15.007 0.94851 +ENDDATA 286 +ENDSUBENT 298 +SUBENT F0658003 20050617 20050831 F022 +BIB 3 3 +REACTION (14-SI-28(A,EL)14-SI-28,,DA,,RTH) +ERR-ANALYS (ANG-ERR-D)Digitizing error +STATUS (CURVE)Fig.3,4,5 +ENDBIB 3 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.15 +ENDCOMMON 3 +DATA 4 137 +EN-CM ANG-CM DATA-CM DATA-ERR +MEV ADEG NO-DIM NO-DIM + 5.8000 77.906 1.0794 0.54566E-01 + 5.8000 83.051 0.88447 0.46213E-01 + 5.8000 88.201 0.69792 0.58817E-01 + 5.8000 93.213 0.54923 0.33610E-01 + 5.8000 98.554 0.45086 0.29408E-01 + 5.8000 103.46 0.41985 0.29358E-01 + 5.8000 108.23 0.42251 0.42062E-01 + 5.8000 113.02 0.47137 0.33610E-01 + 5.8000 117.82 0.53704 0.33560E-01 + 5.8000 122.48 0.63218 0.37811E-01 + 5.8000 125.44 0.72785 0.33560E-01 + 5.8000 127.31 0.78607 0.37761E-01 + 5.8000 127.75 0.72711 0.37861E-01 + 5.8000 132.45 0.91046 0.46263E-01 + 5.8000 137.09 0.98459 0.54566E-01 + 5.8000 141.25 0.98324 0.58867E-01 + 5.8000 145.84 0.93553 0.46213E-01 + 5.8000 150.41 0.83320 0.50464E-01 + 5.8000 154.86 0.81075 0.50414E-01 + 5.8000 159.02 0.83041 0.50364E-01 + 5.8000 163.40 0.97605 0.63068E-01 + 5.8000 166.07 1.1180 0.67119E-01 + 5.8000 169.75 1.4362 0.88225E-01 + 6.0000 77.654 0.45811 + 6.0000 83.041 0.34574 + 6.0000 88.411 0.30635 + 6.0000 93.745 0.42751 + 6.0000 98.812 0.65064 + 6.0000 103.87 0.91755 0.72977E-01 + 6.0000 108.70 1.1113 0.72977E-01 + 6.0000 113.54 1.2320 0.87772E-01 + 6.0000 118.42 1.2360 0.73177E-01 + 6.0000 122.85 1.0353 0.72777E-01 + 6.0000 126.04 0.92113 0.72977E-01 + 6.0000 127.52 0.87855 + 6.0000 128.50 0.82096 + 6.0000 132.93 0.63482 + 6.0000 137.58 0.56564 + 6.0000 141.96 0.59842 + 6.0000 146.28 0.89393 0.72777E-01 + 6.0000 151.06 1.3212 0.11696 + 6.0000 155.32 1.8502 0.10217 + 6.0000 159.58 2.4230 0.16055 + 6.0000 163.77 3.2586 0.21893 + 6.0000 166.63 3.5383 0.17534 + 6.0000 170.67 3.9941 0.24832 + 6.3000 77.660 0.83361 0.73086E-01 + 6.3000 83.046 0.70584 0.87875E-01 + 6.3000 88.189 0.57789 + 6.3000 93.323 0.49379 + 6.3000 98.440 0.49740 + 6.3000 103.31 0.50084 + 6.3000 108.66 0.57770 + 6.3000 113.27 0.68329 + 6.3000 118.13 0.75981 + 6.3000 122.99 0.80710 + 6.3000 125.43 0.80881 0.87704E-01 + 6.3000 127.86 0.83977 0.87875E-01 + 6.3000 132.50 0.79918 0.58469E-01 + 6.3000 137.14 0.75859 + 6.3000 141.53 0.73245 + 6.3000 145.93 0.63322 + 6.3000 150.58 0.56340 + 6.3000 154.72 0.58094 + 6.3000 159.08 0.70097 + 6.3000 163.64 1.0550 0.72914E-01 + 6.3000 166.27 1.3347 0.11694 + 6.3000 170.33 1.7322 0.87875E-01 + 7.5000 77.677 0.23226 + 7.5000 83.116 0.35177 + 7.5000 87.953 0.25268 + 7.5000 93.192 0.15440 + 7.5000 98.431 0.27350 + 7.5000 103.27 0.39180 + 7.5000 108.50 0.40221 + 7.5000 113.14 0.62881 + 7.5000 117.97 0.63841 + 7.5000 122.81 0.86541 + 7.5000 125.43 0.76192 + 7.5000 127.04 0.76512 + 7.5000 128.25 0.87622 + 7.5000 132.48 0.66724 + 7.5000 137.32 0.35078 + 7.5000 141.55 0.25049 + 7.5000 146.18 0.80316 + 7.5000 150.81 1.7906 + 7.5000 155.23 3.9732 + 7.5000 159.44 6.5902 0.43477 + 7.5000 163.64 11.490 0.76084 + 7.5000 166.24 13.886 0.76084 + 7.5000 170.25 17.698 1.0869 + 7.7000 77.067 0.56871 + 7.7000 82.507 0.68939 + 7.7000 87.545 0.58715 + 7.7000 92.582 0.59601 + 7.7000 97.621 0.38266 + 7.7000 102.66 0.39152 + 7.7000 107.49 0.40003 + 7.7000 112.33 0.29743 + 7.7000 117.16 0.63926 + 7.7000 122.40 1.3151 + 7.7000 124.82 1.6527 + 7.7000 126.22 1.8774 + 7.7000 127.23 2.1014 + 7.7000 132.06 2.4432 + 7.7000 136.70 2.6736 + 7.7000 141.13 2.0147 + 7.7000 145.57 1.5781 + 7.7000 150.01 1.1415 + 7.7000 154.44 1.3715 + 7.7000 158.86 3.2681 0.55589 + 7.7000 162.87 5.8307 0.77740 + 7.7000 165.68 8.2800 0.77775 + 7.7000 169.49 12.287 1.5551 + 7.8000 77.271 0.54476 + 7.8000 82.511 0.44438 + 7.8000 87.548 0.45352 + 7.8000 92.989 0.35350 + 7.8000 98.026 0.36264 + 7.8000 103.06 0.48166 + 7.8000 107.69 0.92959 + 7.8000 112.73 1.0486 + 7.8000 117.77 1.0577 + 7.8000 122.60 1.1764 + 7.8000 125.43 1.0716 + 7.8000 127.04 1.0746 + 7.8000 127.84 1.1859 + 7.8000 132.48 1.0844 + 7.8000 136.91 1.0925 + 7.8000 141.34 0.99063 + 7.8000 145.78 0.88879 + 7.8000 150.41 1.1170 + 7.8000 154.44 1.7836 + 7.8000 158.86 3.1102 + 7.8000 163.28 5.3159 0.33001 + 7.8000 165.89 6.8589 0.54904 + 7.8000 169.70 9.2833 0.54941 +ENDDATA 139 +ENDSUBENT 151 +ENDENTRY 3 diff --git a/exforall/F06/F0678.x4 b/exforall/F06/F0678.x4 new file mode 100644 index 000000000..43721cfeb --- /dev/null +++ b/exforall/F06/F0678.x4 @@ -0,0 +1,101 @@ +ENTRY F0678 20050421 20050831 F021 +SUBENT F0678001 20050421 20050831 F021 +BIB 10 14 +TITLE Study of (d5/2)2 5+ configuration for 22Na and 24Na(*). +AUTHOR (E.Labie,P.Leleux,P.C.Macq) +INSTITUTE (2BLGPCL) +REFERENCE (J,JPR/L,1,1,1974) +FACILITY (CYCLO) +SAMPLE Gas target consists of natural Ne under pressure of + 380+-1 mm Hg and 22Ne enriched to 98.95% under pressure + of 137+- mm Hg. +DETECTOR (TELES,SIBAR) +METHOD (EDE) +ERR-ANALYS (ERR-DIG)Digitizing error + (ANG-ERR-D)Digitizing error + (DATA-ERR)Error from the graphic bars +HISTORY (20031218C) +ENDBIB 14 +COMMON 4 3 +ANG-RSL EN-RSL ERR-DIG ANG-ERR-D +ADEG KEV PER-CENT ADEG + 1.7 290. 0.2 0.1 +ENDCOMMON 3 +ENDSUBENT 21 +SUBENT F0678002 20050421 20050831 F021 +BIB 3 3 +REACTION (10-NE-20(A,D)11-NA-22,PAR,DA) +LEVEL-PROP (11-NA-22,E-LVL=1.529,SPIN=5.,PARITY=+1.) +STATUS (CURVE)Fig.2 +ENDBIB 3 +COMMON 2 3 +EN E-LVL +MEV MEV + 21.4 1.529 +ENDCOMMON 3 +DATA 3 25 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR MB/SR + 16.799 0.54351 0.13027E-01 + 19.975 0.62111 0.22063E-01 + 20.175 0.69572 0.14903E-01 + 26.487 0.59915 0.14361E-01 + 32.650 0.59998 0.12087E-01 + 32.654 0.57008 0.20242E-01 + 36.186 0.56307 0.14214E-01 + 39.509 0.57303 0.15198E-01 + 45.474 0.49780 0.10661E-01 + 45.476 0.48676 0.21942E-01 + 48.669 0.43513 0.12098E-01 + 51.645 0.44949 0.12498E-01 + 54.838 0.40332 0.17987E-01 + 57.667 0.46321 0.17652E-01 + 57.670 0.44676 0.14788E-01 + 63.427 0.39103 0.10873E-01 + 66.548 0.36605 0.22089E-01 + 69.518 0.40548 0.13358E-01 + 75.400 0.42840 0.16325E-01 + 80.800 0.43600 0.12323E-01 + 80.866 0.45715 0.11541E-01 + 84.136 0.37265 0.11797E-01 + 86.691 0.40716 0.12366E-01 + 92.166 0.38596 0.12715E-01 + 97.706 0.38649 0.14228E-01 +ENDDATA 27 +ENDSUBENT 39 +SUBENT F0678003 20050421 20050831 F021 +BIB 3 3 +REACTION (10-NE-22(A,D)11-NA-24,PAR,DA) +LEVEL-PROP (11-NA-24,E-LVL=1.5,SPIN=5.,PARITY=+1.) +STATUS (CURVE)Fig.2 +ENDBIB 3 +COMMON 2 3 +EN E-LVL +MEV MEV + 21.7 1.5 +ENDCOMMON 3 +DATA 3 19 +ANG-CM DATA-CM DATA-ERR +ADEG MB/SR MB/SR + 18.076 0.65052 0.21329E-01 + 18.333 0.81535 0.34077E-01 + 21.039 0.76351 0.27976E-01 + 24.223 0.78374 0.33770E-01 + 27.205 0.74678 0.38976E-01 + 30.385 0.79071 0.25925E-01 + 30.389 0.75149 0.35502E-01 + 41.961 0.69349 0.20964E-01 + 47.927 0.61267 0.23236E-01 + 53.634 0.44823 0.19895E-01 + 58.974 0.40644 0.17515E-01 + 64.535 0.32393 0.17752E-01 + 70.214 0.32078 0.16324E-01 + 75.848 0.24177 0.15795E-01 + 78.473 0.26048 0.13936E-01 + 81.384 0.25161 0.14449E-01 + 86.916 0.27551 0.16544E-01 + 92.106 0.28813 0.18823E-01 + 97.016 0.30814 0.16082E-01 +ENDDATA 21 +ENDSUBENT 33 +ENDENTRY 3 diff --git a/exforall/F06/F0686.x4 b/exforall/F06/F0686.x4 index 5a8e48d47..5012fecb0 100644 --- a/exforall/F06/F0686.x4 +++ b/exforall/F06/F0686.x4 @@ -1,6 +1,6 @@ -ENTRY F0686 20050405 20050610 F020 -SUBENT F0686001 20050405 20050610 F020 -BIB 11 52 +ENTRY F0686 20050620 20050831 F022 +SUBENT F0686001 20050620 20050831 F022 +BIB 11 54 TITLE High spin negative parity states in 35Cl. AUTHOR (P.R.G.Lornie,E.M.Jayasinghe,G.D.Jones,H.G.Price, M.F.Thomas,P.J.Twin,P.J.Nolan) @@ -53,51 +53,60 @@ LEVEL-PROP (17-CL-35,E-LVL=4.348,SPIN=4.5,PARITY=-1.) (17-CL-35,E-LVL=5.408,SPIN=5.5,PARITY=-1.) (17-CL-35,E-LVL=6.088,SPIN=6.5,PARITY=-1.) HISTORY (20040520C) -ENDBIB 52 + (20050601A) Subent 002 was separated into two + subentries. +ENDBIB 54 NOCOMMON 0 0 -ENDSUBENT 55 -SUBENT F0686002 20050405 20050610 F020 -BIB 3 6 -REACTION 1(16-S-32(A,P)17-CL-35,PAR,DA,G,LEG/RSD) - 2(16-S-32(A,P)17-CL-35,,POL/DA) -ERR-ANALYS Error of 25% is included in the time scale. - 1(DATA-ERR) Error of Legendre coefficients - 2(DATA-ERR) Error of polarization +ENDSUBENT 57 +SUBENT F0686002 20050620 20050831 F022 +BIB 3 4 +REACTION (16-S-32(A,P)17-CL-35,PAR,DA,G,LEG/RS) +ERR-ANALYS (DATA-ERR) Error of Legendre coefficients + Error of 25% is included in the time scale. STATUS (TABLE) Table 1 -ENDBIB 6 +ENDBIB 4 +COMMON 2 3 +EN-MIN EN-MAX +MEV MEV + 11. 12. +ENDCOMMON 3 +DATA 4 10 +E-LVL NUMBER DATA DATA-ERR +KEV NO-DIM NO-DIM NO-DIM + 4348.0 2.0000 -.95000 0.30000E-01 + 4348.0 2.0000 -.34000 0.50000E-01 + 4348.0 4.0000 0.40000E-010.50000E-01 + 4348.0 4.0000 0.80000E-010.30000E-01 + 5408.0 2.0000 0.19000 0.11000 + 5408.0 2.0000 0.44000 0.30000E-01 + 5408.0 4.0000 -.10000E-010.13000 + 5408.0 4.0000 -.19000 0.30000E-01 + 6088.0 2.0000 -.22000 0.10000E-01 + 6088.0 4.0000 0.50000E-020.15000E-01 +ENDDATA 12 +ENDSUBENT 25 +SUBENT F0686003 20050620 20050831 F022 +BIB 3 4 +REACTION (16-S-32(A,P)17-CL-35,PAR,POL/DA) +ERR-ANALYS (DATA-ERR) Error of polarization + Error of 25% is included in the time scale. +STATUS (TABLE) Table 1 +ENDBIB 4 COMMON 3 3 ANG EN-MIN EN-MAX ADEG MEV MEV 90. 11. 12. ENDCOMMON 3 -DATA 7 10 -E-LVL E NUMBER DATA 1DATA-ERR 1DATA 2 -DATA-ERR -KEV KEV NO-DIM NO-DIM NO-DIM NO-DIM -NO-DIM - 4348.0 1185.0 2.0000 -.95000 0.30000E-01-.50000E-02 -0.40000E-01 - 4348.0 1185.0 4.0000 0.80000E-010.30000E-01-.50000E-02 -0.40000E-01 - 4348.0 1702.0 2.0000 -.34000 0.50000E-010.36000 -0.70000E-01 - 4348.0 1702.0 4.0000 0.40000E-010.50000E-010.36000 -0.70000E-01 - 5408.0 1060.0 2.0000 0.19000 0.11000 -.40000 -0.14000 - 5408.0 1060.0 4.0000 -.10000E-010.13000 -.40000 -0.14000 - 5408.0 2245.0 2.0000 0.44000 0.30000E-01 - - 5408.0 2245.0 4.0000 -.19000 0.30000E-01 - - 6088.0 680.00 2.0000 -.22000 0.10000E-01-.45000 -0.50000E-01 - 6088.0 680.00 4.0000 0.50000E-020.15000E-01-.45000 -0.50000E-01 -ENDDATA 24 -ENDSUBENT 39 -SUBENT F0686003 20050405 20050610 F020 +DATA 3 4 +E-LVL DATA DATA-ERR +KEV NO-DIM NO-DIM + 4348.0 -.50000 20.400 + 4348.0 0.36000 0.70000 + 5408.0 -.40000 0.14000 + 6088.0 -.45000 0.50000 +ENDDATA 6 +ENDSUBENT 19 +SUBENT F0686004 20050620 20050831 F022 BIB 5 12 REACTION (16-S-32(A,P)17-CL-35,PAR,DA/DA,P/G,REL) ANG1 is an angle of proton detection. @@ -138,4 +147,4 @@ KEV KEV NO-DIM ARB-UNITS ARB-UNITS NO-DIM 6088.0 680.00 0.99903 1.9925 0.58554E-010.99806 ENDDATA 18 ENDSUBENT 39 -ENDENTRY 3 +ENDENTRY 4 diff --git a/exforall/F06/F0694.x4 b/exforall/F06/F0694.x4 new file mode 100644 index 000000000..070e7e164 --- /dev/null +++ b/exforall/F06/F0694.x4 @@ -0,0 +1,59 @@ +ENTRY F0694 20050524 20050831 F021 +SUBENT F0694001 20050524 20050831 F021 +BIB 14 26 +TITLE Energy-dependent coherence width of 28Si at excitation + energies between 22 and 33 MeV. +AUTHOR (J.D.A.Roeders,L.W.Put,A.G.Drentje,A. Van Der Woude) +INSTITUTE (2NEDGRN) + (1USAORL) +REFERENCE (J,NCL,2,209,1969) +REL-REF (R,,L.W.Put,J,NP/A,112,561,1968) Experimental + arrangement was described. +FACILITY (ISOCY,2NEDGRN)Philips prototype 30 MeV AVF-cyclotron. +SAMPLE Target of MG-24 was used. +INC-SOURCE Alpha-particle beam. +INC-SPECT Energy of alpha particles is in the range from 18 MeV + to 27 MeV. +DETECTOR (SIBAR) Detectors were placed at eight angles between + 80 degrees and 164 degrees (lab.) +ANALYSIS Excitation functions were obtained in steps of + 35, 40 and 100 keV. Statistical analysis was applied to + 56 measured excitation functions. +CORRECTION The values of resonance width Gamma(n) were corrected + for energy resolution and finite range of data effects. + Half-widths of Gamma(g) needed extra correction for + "damping" of excitation functions. Values of resonance + width Gamma(p) were corrected for energy resolution, + step size and counting statistics. +ERR-ANALYS (DATA-ERR) Uncertainty in resonance width. +HISTORY (20040810C) +ENDBIB 26 +COMMON 1 3 +EN-RSL +KEV + 30. +ENDCOMMON 3 +ENDSUBENT 33 +SUBENT F0694002 20050524 20050831 F021 +BIB 3 9 +REACTION 1(12-MG-24(A,0),,EN) + 2(12-MG-24(A,INL),,WID) +COMMENT DATA2 is a mean value of an averaged value of width + from normal autocorrelation functions,an averaged value + of width from autocorrelation functions of + trend-reduced excitation functions and an averaged + value from a number of maxima in the excitation + functions. +STATUS (TABLE) Table 1 +ENDBIB 9 +NOCOMMON 0 0 +DATA 4 4 +DATA-MIN 1DATA-MAX 1DATA 2DATA-ERR 2 +MEV MEV KEV KEV + 17.700 20.400 81.000 14.000 + 19.000 23.700 96.000 15.000 + 22.900 25.200 97.000 17.000 + 23.000 27.000 116.00 29.000 +ENDDATA 6 +ENDSUBENT 20 +ENDENTRY 2 diff --git a/exforall/F06/F0696.x4 b/exforall/F06/F0696.x4 new file mode 100644 index 000000000..96cf578fa --- /dev/null +++ b/exforall/F06/F0696.x4 @@ -0,0 +1,686 @@ +ENTRY F0696 20041207 20050831 F021 +SUBENT F0696001 20041207 20050831 F021 +BIB 11 18 +TITLE Investigation of the 28Si(3He,p)30P reaction. +AUTHOR (Yu.V.Nikitenko,G.M.Osetinskij,Son Von Nam,M.A.Faruk) +INSTITUTE (4ZZZDUB) +REFERENCE (J,YF,18,954,1973) +FACILITY (VDG) +SAMPLE Thin self-supporting 28Si target with the thickness + of 28 mu-g/cm2. +METHOD (BCINT) +DETECTOR (SIBAR) Five surface barrier detectors with lithium + drift. One of them was used as a monitor and it was + set at 90 degr. The others were mounted on a mobile + corbel providing measurements at the angles 0-160 degr. +MONITOR (3-LI-7(P,N)4-BE-7,,SIG) The scale of electrostatic + generator was calibrated. +ERR-ANALYS (ERR-DIG) Digitizing error. + (DATA-ERR1) Mean square error. + (DATA-ERR2) Error from the graphic bars. +HISTORY (20041018C) +ENDBIB 18 +NOCOMMON 0 0 +ENDSUBENT 21 +SUBENT F0696002 20041207 20050831 F021 +BIB 3 3 +REACTION (14-SI-28(HE3,P)15-P-30,PAR,DA) +ERR-ANALYS (EN-ERR-DIG) Digitizing error +STATUS (CURVE)Fig.2 +ENDBIB 3 +COMMON 3 3 +DATA-ERR1 EN-ERR-DIG ERR-DIG +PER-CENT MEV MU-B/SR + 9. 0.001 0.13 +ENDCOMMON 3 +DATA 5 284 +E-LVL ANG EN DATA DATA-ERR2 +MEV ADEG MEV MU-B/SR MU-B/SR + 0.0000 45.000 2.9569 6.6243 3.7917 + 0.0000 45.000 2.9718 7.1302 3.5389 + 0.0000 45.000 3.0002 7.8893 3.5389 + 0.0000 45.000 3.0200 7.8897 3.5389 + 0.0000 45.000 3.0497 8.9016 3.2861 + 0.0000 45.000 3.0968 11.178 3.5389 + 0.0000 45.000 3.1451 12.948 3.2861 + 0.0000 45.000 3.1946 13.708 3.2861 + 0.0000 45.000 3.2478 19.270 3.0334 + 0.0000 45.000 3.2998 27.866 3.0334 + 0.0000 45.000 3.3506 21.800 3.2861 + 0.0000 45.000 3.4013 25.846 3.2861 + 0.0000 45.000 3.4471 33.178 3.2861 + 0.0000 45.000 3.4991 44.554 3.7917 + 0.0000 45.000 3.5511 31.664 3.0334 + 0.0000 45.000 3.5969 28.126 4.0445 + 0.0000 45.000 3.6440 27.369 3.0334 + 0.0000 45.000 3.6935 27.875 3.0334 + 0.0000 45.000 3.7442 29.899 3.7917 + 0.0000 45.000 3.7962 32.681 3.0334 + 0.0000 45.000 3.8965 45.069 4.2973 + 0.0000 45.000 3.9485 81.976 3.5389 + 0.0000 45.000 4.0029 96.133 3.7917 + 0.0000 45.000 4.0413 97.145 6.3195 + 0.0000 45.000 4.0958 88.805 3.2861 + 0.0000 45.000 4.1466 91.587 6.5723 + 0.0000 45.000 4.1985 112.06 3.0333 + 0.0000 45.000 4.2468 122.43 7.3306 + 0.0000 90.000 2.9564 2.9702 3.2581 + 0.0000 90.000 3.0033 5.4808 3.2581 + 0.0000 90.000 3.0489 5.2344 3.5088 + 0.0000 90.000 3.0983 5.7402 3.0075 + 0.0000 90.000 3.1464 6.7471 3.2581 + 0.0000 90.000 3.1970 7.5037 3.2581 + 0.0000 90.000 3.2476 9.0121 3.5088 + 0.0000 90.000 3.2982 10.771 3.5088 + 0.0000 90.000 3.3513 12.530 3.0075 + 0.0000 90.000 3.3994 15.793 3.7594 + 0.0000 90.000 3.4463 25.572 3.5088 + 0.0000 90.000 3.4932 35.601 4.0100 + 0.0000 90.000 3.5512 16.058 3.0075 + 0.0000 90.000 3.5932 13.054 5.0125 + 0.0000 90.000 3.6487 16.067 3.5088 + 0.0000 90.000 3.6944 20.331 3.5088 + 0.0000 90.000 3.7475 27.354 3.0075 + 0.0000 90.000 3.7907 27.859 4.2606 + 0.0000 90.000 3.8437 25.107 3.2581 + 0.0000 90.000 3.8881 37.893 3.5088 + 0.0000 90.000 3.9424 54.690 3.2581 + 0.0000 90.000 3.9967 56.199 3.0075 + 0.0000 90.000 4.0461 53.697 3.2581 + 0.0000 90.000 4.0917 54.203 4.0100 + 0.0000 90.000 4.1473 67.741 3.2581 + 0.0000 90.000 4.1978 74.764 3.2581 + 0.0000 90.000 4.2447 76.272 4.2606 + 0.0000 135.00 2.9646 2.7968 3.4947 + 0.0000 135.00 3.0015 4.2946 3.4947 + 0.0000 135.00 3.0618 6.0421 3.4947 + 0.0000 135.00 3.1036 6.5415 3.2451 + 0.0000 135.00 3.1529 8.2890 2.9955 + 0.0000 135.00 3.1996 10.036 3.2451 + 0.0000 135.00 3.2513 15.778 3.4947 + 0.0000 135.00 3.3005 12.783 3.4947 + 0.0000 135.00 3.3583 18.274 3.4947 + 0.0000 135.00 3.4001 21.020 3.2451 + 0.0000 135.00 3.4481 22.518 3.7443 + 0.0000 135.00 3.5465 17.027 2.9955 + 0.0000 135.00 3.6007 24.516 3.2451 + 0.0000 135.00 3.6486 35.499 4.2436 + 0.0000 135.00 3.6966 48.729 3.4947 + 0.0000 135.00 3.7471 49.728 3.4947 + 0.0000 135.00 3.7938 50.976 3.9940 + 0.0000 135.00 3.8479 55.470 2.9955 + 0.0000 135.00 3.8934 64.955 3.7443 + 0.0000 135.00 3.9427 82.429 4.4932 + 0.0000 135.00 3.9992 46.234 5.7413 + 0.0000 135.00 4.0472 55.221 6.7398 + 0.0000 135.00 4.0903 83.178 6.4902 + 0.0000 135.00 4.1432 100.65 3.4947 + 0.0000 135.00 4.1936 152.32 5.7413 + 0.0000 135.00 4.2428 139.84 4.7428 + 0.0000 160.00 3.0959 5.7783 3.5750 + 0.0000 160.00 3.1440 6.0288 3.8304 + 0.0000 160.00 3.1947 8.5774 3.3197 + 0.0000 160.00 3.2390 13.425 3.5750 + 0.0000 160.00 3.2922 22.868 5.1072 + 0.0000 160.00 3.3504 36.396 3.5750 + 0.0000 160.00 3.3935 51.969 4.5965 + 0.0000 160.00 3.4378 50.688 3.3197 + 0.0000 160.00 3.4909 37.404 4.0858 + 0.0000 160.00 3.5542 20.799 3.8304 + 0.0000 160.00 3.5960 29.988 3.5750 + 0.0000 160.00 3.6492 51.177 3.5750 + 0.0000 160.00 3.6948 61.643 4.8518 + 0.0000 160.00 3.7479 54.487 4.0858 + 0.0000 160.00 3.7986 73.379 3.8304 + 0.0000 160.00 3.8556 77.714 4.3411 + 0.0000 160.00 3.9011 58.047 5.1072 + 0.0000 160.00 3.9518 86.642 5.8733 + 0.0000 160.00 4.0086 34.799 5.3626 + 0.0000 160.00 4.0554 31.219 3.5750 + 0.0000 160.00 4.1011 90.713 8.9376 + 0.0000 160.00 4.1481 142.80 3.5750 + 0.0000 160.00 4.2039 172.67 4.8518 + 0.0000 160.00 4.2570 157.35 4.0858 + 1.4500 45.000 2.9616 1.7348 0.74257 + 1.4500 45.000 3.0164 3.1234 0.69307 + 1.4500 45.000 3.0639 4.4127 0.69307 + 1.4500 45.000 3.1017 5.1074 0.69307 + 1.4500 45.000 3.1504 5.2581 0.69307 + 1.4500 45.000 3.2028 8.0822 0.69307 + 1.4500 45.000 3.2528 6.6488 0.69307 + 1.4500 45.000 3.3016 5.2153 0.69307 + 1.4500 45.000 3.3528 4.7720 0.64356 + 1.4500 45.000 3.4076 6.1111 0.69307 + 1.4500 45.000 3.4514 8.3408 0.74257 + 1.4500 45.000 3.5085 16.066 0.74257 + 1.4500 45.000 3.5560 16.860 0.69307 + 1.4500 45.000 3.6011 16.318 0.69307 + 1.4500 45.000 3.6499 15.379 0.74257 + 1.4500 45.000 3.6974 17.164 0.74257 + 1.4500 45.000 3.7511 14.097 0.59406 + 1.4500 45.000 3.7985 18.653 0.59406 + 1.4500 45.000 3.8509 20.141 0.74257 + 1.4500 45.000 3.8947 23.955 0.64356 + 1.4500 45.000 3.9421 28.264 0.84158 + 1.4500 45.000 3.9958 24.504 0.74257 + 1.4500 45.000 4.0493 30.051 0.69307 + 1.4500 45.000 4.0969 29.409 0.64356 + 1.4500 45.000 4.1396 27.084 0.69307 + 1.4500 45.000 4.1922 20.354 0.74257 + 1.4500 45.000 4.2420 27.089 0.89109 + 1.4500 90.000 2.9508 9.0234 3.7276 + 1.4500 90.000 3.0491 13.998 3.7276 + 1.4500 90.000 3.0976 12.509 3.7276 + 1.4500 90.000 3.1486 11.020 3.4791 + 1.4500 90.000 3.1971 14.998 3.4791 + 1.4500 90.000 3.2494 14.006 3.4791 + 1.4500 90.000 3.2991 15.499 3.7276 + 1.4500 90.000 3.3539 13.265 3.4791 + 1.4500 90.000 3.4036 14.261 3.4791 + 1.4500 90.000 3.4596 16.500 3.4791 + 1.4500 90.000 3.5006 26.939 3.4791 + 1.4500 90.000 3.5554 23.959 3.4791 + 1.4500 90.000 3.6076 23.216 3.4791 + 1.4500 90.000 3.6549 30.922 3.2306 + 1.4500 90.000 3.7009 32.663 3.4791 + 1.4500 90.000 3.7519 33.659 3.2306 + 1.4500 90.000 3.8029 39.874 7.4552 + 1.4500 90.000 3.8502 37.391 3.4791 + 1.4500 90.000 3.9061 46.588 5.7157 + 1.4500 90.000 3.9546 65.974 4.7216 + 1.4500 90.000 4.0069 57.527 5.2186 + 1.4500 90.000 4.0516 68.463 4.9701 + 1.4500 90.000 4.1039 51.318 5.9642 + 1.4500 90.000 4.1561 80.396 3.9761 + 1.4500 90.000 4.2021 115.44 4.4731 + 1.4500 90.000 4.2531 111.71 3.4791 + 1.4500 135.00 2.9491 4.0663 3.4878 + 1.4500 135.00 2.9969 4.5691 3.7369 + 1.4500 135.00 3.0484 5.8196 3.7369 + 1.4500 135.00 3.0924 8.0659 3.7369 + 1.4500 135.00 3.1426 10.064 3.4878 + 1.4500 135.00 3.1904 10.816 3.4878 + 1.4500 135.00 3.2431 11.817 3.4878 + 1.4500 135.00 3.2997 11.324 3.4878 + 1.4500 135.00 3.3499 10.582 3.4878 + 1.4500 135.00 3.3977 10.835 3.4878 + 1.4500 135.00 3.4479 13.581 3.7369 + 1.4500 135.00 3.5032 30.028 3.7369 + 1.4500 135.00 3.5534 26.545 3.4878 + 1.4500 135.00 3.5999 20.072 3.4878 + 1.4500 135.00 3.6514 23.316 3.2386 + 1.4500 135.00 3.7042 25.314 3.9860 + 1.4500 135.00 3.7532 36.031 3.4878 + 1.4500 135.00 3.8034 39.773 4.7334 + 1.4500 135.00 3.8549 41.770 3.7369 + 1.4500 135.00 3.9014 57.968 3.7369 + 1.4500 135.00 3.9542 53.489 3.4878 + 1.4500 135.00 4.0031 62.960 8.7194 + 1.4500 135.00 4.0509 77.663 3.2386 + 1.4500 135.00 4.1037 59.233 3.4878 + 1.4500 135.00 4.1589 89.382 5.4808 + 1.4500 135.00 4.2078 141.70 6.4773 + 1.4500 135.00 4.2568 108.57 3.2386 + 1.4500 160.00 3.1007 9.5535 3.2679 + 1.4500 160.00 3.1513 13.066 3.5193 + 1.4500 160.00 3.2019 13.814 3.5193 + 1.4500 160.00 3.2487 12.049 3.2679 + 1.4500 160.00 3.3043 14.807 3.5193 + 1.4500 160.00 3.3511 14.298 3.2679 + 1.4500 160.00 3.4017 10.521 3.5193 + 1.4500 160.00 3.4535 10.766 3.7706 + 1.4500 160.00 3.5054 25.088 3.5193 + 1.4500 160.00 3.5534 21.814 5.2789 + 1.4500 160.00 3.6040 12.004 4.2734 + 1.4500 160.00 3.6546 14.512 3.2679 + 1.4500 160.00 3.7001 12.746 3.5193 + 1.4500 160.00 3.7469 20.784 3.5193 + 1.4500 160.00 3.8013 24.548 4.5248 + 1.4500 160.00 3.8518 19.766 3.5193 + 1.4500 160.00 3.9012 29.563 3.2679 + 1.4500 160.00 3.9543 27.043 6.2844 + 1.4500 160.00 4.0049 63.737 9.5523 + 1.4500 160.00 4.0569 84.595 3.2679 + 1.4500 160.00 4.1099 61.965 4.2734 + 1.4500 160.00 4.1605 90.615 5.5303 + 1.4500 160.00 4.2088 153.45 5.0275 + 1.4500 160.00 4.2554 107.45 5.5303 + 1.9700 90.000 2.9475 3.0002 1.7500 + 1.9700 90.000 3.0004 3.5004 3.2500 + 1.9700 90.000 3.0509 6.3756 1.7500 + 1.9700 90.000 3.0977 4.7508 1.8750 + 1.9700 90.000 3.1519 5.2510 1.8750 + 1.9700 90.000 3.2036 6.7512 1.7500 + 1.9700 90.000 3.2492 5.2514 1.7500 + 1.9700 90.000 3.3021 4.3766 1.8750 + 1.9700 90.000 3.3539 6.8768 1.8750 + 1.9700 90.000 3.3957 7.8769 1.8750 + 1.9700 90.000 3.4499 10.002 1.7500 + 1.9700 90.000 3.5016 12.127 1.7500 + 1.9700 90.000 3.5546 14.253 1.7500 + 1.9700 90.000 3.6039 15.503 1.7500 + 1.9700 90.000 3.6531 16.878 1.8750 + 1.9700 90.000 3.7036 24.753 1.8750 + 1.9700 90.000 3.7553 27.628 3.0000 + 1.9700 90.000 3.8095 44.254 2.5000 + 1.9700 90.000 3.9068 35.629 2.6250 + 1.9700 90.000 3.9548 41.629 2.1250 + 1.9700 90.000 4.0041 23.879 1.8750 + 1.9700 90.000 4.0546 28.379 1.7500 + 1.9700 90.000 4.1063 37.380 1.7500 + 1.9700 90.000 4.1506 32.880 2.7500 + 1.9700 90.000 4.2036 34.255 2.1250 + 1.9700 90.000 4.2504 39.880 2.7500 + 1.9700 135.00 2.9960 9.6819 1.7526 + 1.9700 135.00 3.0497 11.812 1.7526 + 1.9700 135.00 3.0958 13.066 1.6274 + 1.9700 135.00 3.1495 14.069 1.7526 + 1.9700 135.00 3.1994 11.567 1.7526 + 1.9700 135.00 3.2469 10.568 1.7526 + 1.9700 135.00 3.2980 11.947 1.7526 + 1.9700 135.00 3.3517 14.202 1.7526 + 1.9700 135.00 3.3991 15.080 1.7526 + 1.9700 135.00 3.4503 14.206 1.7526 + 1.9700 135.00 3.5065 18.464 1.7526 + 1.9700 135.00 3.5626 20.970 1.6274 + 1.9700 135.00 3.6612 28.610 2.1281 + 1.9700 135.00 3.7061 33.744 1.7526 + 1.9700 135.00 3.7598 40.005 2.3785 + 1.9700 135.00 3.8134 45.515 1.7526 + 1.9700 135.00 3.8621 41.010 1.8778 + 1.9700 135.00 3.9120 47.397 1.6274 + 1.9700 135.00 3.9532 41.264 1.6274 + 1.9700 135.00 4.0094 34.882 1.7526 + 1.9700 135.00 4.0556 45.274 1.8778 + 1.9700 135.00 4.1129 56.918 1.6274 + 1.9700 135.00 4.1566 51.537 1.6274 + 1.9700 135.00 4.2041 51.539 1.6274 + 1.9700 135.00 4.2602 60.429 3.6303 + 1.9700 160.00 3.0971 9.8646 1.7676 + 1.9700 160.00 3.1497 10.247 1.6414 + 1.9700 160.00 3.1997 11.640 1.7676 + 1.9700 160.00 3.2522 9.8764 1.7676 + 1.9700 160.00 3.3035 14.173 1.7676 + 1.9700 160.00 3.3548 10.768 1.6414 + 1.9700 160.00 3.4010 12.539 1.7676 + 1.9700 160.00 3.4510 11.407 1.6414 + 1.9700 160.00 3.5035 18.481 1.8939 + 1.9700 160.00 3.5560 19.243 2.3989 + 1.9700 160.00 3.6049 13.565 1.6414 + 1.9700 160.00 3.6536 20.639 1.7676 + 1.9700 160.00 3.7011 16.223 1.7676 + 1.9700 160.00 3.7498 28.727 1.6414 + 1.9700 160.00 3.7999 21.281 2.1464 + 1.9700 160.00 3.8512 20.654 1.7676 + 1.9700 160.00 3.8986 29.496 1.7676 + 1.9700 160.00 3.9511 33.793 2.7777 + 1.9700 160.00 4.0036 35.185 1.7676 + 1.9700 160.00 4.0512 33.295 1.6414 + 1.9700 160.00 4.1037 36.329 2.2727 + 1.9700 160.00 4.1549 44.035 2.2727 + 1.9700 160.00 4.2024 45.428 2.9040 + 1.9700 160.00 4.2598 65.507 2.1464 +ENDDATA 286 +ENDSUBENT 298 +SUBENT F0696003 20041207 20050831 F021 +BIB 3 3 +REACTION (14-SI-28(HE3,P)15-P-30,PAR,DA) +ERR-ANALYS (EN-ERR-DIG) Digitizing error +STATUS (CURVE)Fig.2 +ENDBIB 3 +COMMON 5 3 +E-LVL-MIN E-LVL-MAX DATA-ERR1 EN-ERR-DIG ERR-DIG +MEV MEV PER-CENT MEV MU-B/SR + 0.68 0.71 9. 0.0001 0.1 +ENDCOMMON 3 +DATA 4 99 +ANG EN DATA DATA-ERR2 +ADEG MEV MU-B/SR MU-B/SR + 45.000 2.9588 6.1953 3.2176 + 45.000 3.0012 6.9409 3.4651 + 45.000 3.0460 7.9342 3.2176 + 45.000 3.0956 6.2052 3.2176 + 45.000 3.1453 5.9613 3.2176 + 45.000 3.1973 6.7075 2.9701 + 45.000 3.2482 8.9388 3.2176 + 45.000 3.2942 11.912 2.7226 + 45.000 3.3523 13.649 2.9701 + 45.000 3.3995 11.425 3.7126 + 45.000 3.4382 11.428 3.2176 + 45.000 3.4915 13.906 3.2176 + 45.000 3.5448 15.643 3.2176 + 45.000 3.5920 16.636 4.7026 + 45.000 3.6489 28.273 3.2176 + 45.000 3.6936 32.484 3.9601 + 45.000 3.7493 30.013 2.9701 + 45.000 3.7966 25.561 4.9501 + 45.000 3.8389 29.277 2.9701 + 45.000 3.8910 26.806 3.9601 + 45.000 3.9358 35.224 3.2176 + 45.000 3.9890 44.881 4.4551 + 45.000 4.0302 55.279 3.4651 + 45.000 4.0822 67.658 4.2076 + 45.000 4.1319 58.256 3.7126 + 45.000 4.1791 65.685 5.9402 + 45.000 4.2275 78.064 4.4551 + 90.000 2.9502 6.1565 3.1785 + 90.000 2.9992 8.6046 3.1785 + 90.000 3.0984 10.078 3.1785 + 90.000 3.1928 10.084 2.9340 + 90.000 3.2504 12.777 3.1785 + 90.000 3.3006 10.824 2.9340 + 90.000 3.3497 12.050 2.9340 + 90.000 3.3999 13.765 3.1785 + 90.000 3.4501 14.257 3.1785 + 90.000 3.5053 20.617 3.4230 + 90.000 3.5555 21.598 3.1785 + 90.000 3.6021 16.467 3.4230 + 90.000 3.6560 23.316 3.1785 + 90.000 3.7062 26.009 3.1785 + 90.000 3.7553 31.880 3.1785 + 90.000 3.8521 39.710 3.4230 + 90.000 3.8998 47.537 3.6675 + 90.000 3.9476 57.076 3.4230 + 90.000 4.0003 60.502 3.9120 + 90.000 4.0457 58.060 3.4230 + 90.000 4.0959 65.642 3.4230 + 90.000 4.1474 62.956 3.6675 + 90.000 4.1976 73.473 3.1785 + 90.000 4.2393 75.920 4.6455 + 135.00 2.9473 5.5576 3.2386 + 135.00 3.0002 6.8031 3.7368 + 135.00 3.0937 10.540 3.4877 + 135.00 3.1466 11.785 3.2386 + 135.00 3.2007 10.539 3.2386 + 135.00 3.2499 8.7954 3.4877 + 135.00 3.2991 10.290 3.4877 + 135.00 3.3520 15.770 3.2386 + 135.00 3.4012 14.027 3.2386 + 135.00 3.4541 19.258 3.7368 + 135.00 3.5070 33.458 4.2350 + 135.00 3.5513 27.479 2.9894 + 135.00 3.6017 18.759 4.7333 + 135.00 3.6509 20.752 3.2386 + 135.00 3.7025 24.987 3.2386 + 135.00 3.7530 23.243 3.2386 + 135.00 3.8022 33.208 4.4842 + 135.00 3.8526 39.685 3.7368 + 135.00 3.9006 58.867 4.4842 + 135.00 3.9424 82.284 3.4877 + 135.00 3.9953 119.40 5.2315 + 135.00 4.0371 120.15 3.4877 + 135.00 4.0925 72.319 6.2280 + 135.00 4.1503 92.248 3.4877 + 135.00 4.1921 141.08 3.7368 + 135.00 4.2401 133.10 4.2350 + 160.00 3.0973 9.4204 3.6649 + 160.00 3.1995 7.8478 3.4031 + 160.00 3.2512 5.4908 3.4031 + 160.00 3.2980 9.4166 3.6649 + 160.00 3.3535 15.960 3.6649 + 160.00 3.4052 12.032 3.4031 + 160.00 3.4471 20.147 3.6649 + 160.00 3.4963 43.968 3.6649 + 160.00 3.5530 27.998 3.1414 + 160.00 3.5998 17.526 3.4031 + 160.00 3.6478 19.881 3.6649 + 160.00 3.6958 38.728 4.1885 + 160.00 3.7451 35.848 3.4031 + 160.00 3.7919 44.224 3.4031 + 160.00 3.8436 58.883 5.2356 + 160.00 3.8941 85.060 3.9267 + 160.00 3.9372 118.04 3.4031 + 160.00 3.9976 170.66 6.2827 + 160.00 4.0875 88.197 5.2356 + 160.00 4.1466 158.88 3.9267 + 160.00 4.1885 206.78 7.8534 + 160.00 4.2328 206.00 3.1414 +ENDDATA 101 +ENDSUBENT 113 +SUBENT F0696004 20041207 20050831 F021 +BIB 3 3 +REACTION (14-SI-28(HE3,P)15-P-30,PAR,DA) +ERR-ANALYS (ANG-ERR-D) Digitizing error +STATUS (CURVE)Fig.3 +ENDBIB 3 +COMMON 3 3 +DATA-ERR1 ANG-ERR-D ERR-DIG +PER-CENT ADEG MU-B/SR + 10. 0.2 0.06 +ENDCOMMON 3 +DATA 5 148 +E-LVL EN ANG-CM DATA-CM DATA-ERR2 +MEV MEV ADEG MU-B/SR MU-B/SR + 0.0000 3.5600 7.2629 18.160 1.7964 + 0.0000 3.5600 16.965 20.312 1.7964 + 0.0000 3.5600 26.903 22.583 2.0359 + 0.0000 3.5600 36.134 26.171 1.9161 + 0.0000 3.5600 46.071 27.724 1.7964 + 0.0000 3.5600 51.038 27.482 1.9161 + 0.0000 3.5600 61.445 27.358 2.6347 + 0.0000 3.5600 81.296 16.930 2.0359 + 0.0000 3.5600 92.168 12.015 1.7964 + 0.0000 3.5600 105.88 9.4938 1.7964 + 0.0000 3.5600 117.47 8.1712 1.6766 + 0.0000 3.5600 129.55 15.950 2.1557 + 0.0000 3.5600 149.67 24.803 1.7964 + 0.0000 3.5600 163.62 25.037 1.7964 + 0.0000 3.5600 170.24 22.399 1.7964 + 0.0000 3.7000 16.099 16.650 1.8149 + 0.0000 3.7000 26.663 15.441 2.0569 + 0.0000 3.7000 36.052 16.531 1.8149 + 0.0000 3.7000 47.318 20.645 2.2988 + 0.0000 3.7000 52.482 21.614 1.5729 + 0.0000 3.7000 61.635 27.301 1.6939 + 0.0000 3.7000 71.493 28.149 1.6939 + 0.0000 3.7000 82.292 25.004 1.6939 + 0.0000 3.7000 93.093 17.383 1.6939 + 0.0000 3.7000 97.553 17.262 2.5408 + 0.0000 3.7000 106.71 20.772 1.6939 + 0.0000 3.7000 116.33 27.548 2.0569 + 0.0000 3.7000 131.58 47.634 1.6939 + 0.0000 3.7000 140.26 51.386 2.2988 + 0.0000 3.7000 149.65 56.710 1.5729 + 0.0000 3.7000 160.45 67.479 3.0248 + 0.0000 3.7000 164.90 70.383 1.8149 + 0.0000 3.7000 169.60 72.320 1.8149 + 0.0000 3.8600 0.25133 26.192 1.6843 + 0.0000 3.8600 16.575 27.991 1.6843 + 0.0000 3.8600 26.293 30.755 1.8046 + 0.0000 3.8600 35.773 32.076 1.8046 + 0.0000 3.8600 45.726 31.953 2.1655 + 0.0000 3.8600 52.596 31.109 1.8046 + 0.0000 3.8600 61.127 30.745 1.6843 + 0.0000 3.8600 71.784 25.809 2.0452 + 0.0000 3.8600 92.157 20.510 2.1655 + 0.0000 3.8600 106.62 29.889 1.5640 + 0.0000 3.8600 117.29 36.864 1.9249 + 0.0000 3.8600 126.07 45.283 1.8046 + 0.0000 3.8600 131.29 47.447 1.5640 + 0.0000 3.8600 136.04 57.190 1.6843 + 0.0000 3.8600 140.78 59.956 2.5264 + 0.0000 3.8600 151.46 75.713 1.6843 + 0.0000 3.8600 161.67 91.591 3.3686 + 0.0000 4.0100 11.649 57.607 1.8030 + 0.0000 4.0100 24.024 64.818 1.6828 + 0.0000 4.0100 34.736 74.192 2.8847 + 0.0000 4.0100 43.781 83.567 1.6828 + 0.0000 4.0100 49.969 88.254 2.7645 + 0.0000 4.0100 60.440 90.777 2.7645 + 0.0000 4.0100 70.667 79.117 1.6828 + 0.0000 4.0100 81.369 62.889 2.4039 + 0.0000 4.0100 89.456 55.917 1.6828 + 0.0000 4.0100 95.404 53.392 2.4039 + 0.0000 4.0100 106.35 59.161 1.5626 + 0.0000 4.0100 115.87 60.482 2.5241 + 0.0000 4.0100 131.33 55.072 1.5626 + 0.0000 4.0100 136.33 55.672 1.5626 + 0.0000 4.0100 139.90 51.345 2.2837 + 0.0000 4.0100 150.36 41.127 1.5626 + 0.0000 4.0100 160.12 29.828 2.2837 + 0.0000 4.0100 166.06 27.543 1.5626 + 0.0000 4.0100 169.63 20.692 1.6828 + 0.0000 4.0900 6.2720 38.350 1.7433 + 0.0000 4.0900 16.306 45.197 1.7433 + 0.0000 4.0900 25.388 56.651 1.6187 + 0.0000 4.0900 35.194 79.062 3.1130 + 0.0000 4.0900 44.271 83.793 1.8678 + 0.0000 4.0900 60.987 83.416 4.3582 + 0.0000 4.0900 71.486 70.713 1.7433 + 0.0000 4.0900 81.271 61.746 3.6110 + 0.0000 4.0900 91.051 45.681 1.7433 + 0.0000 4.0900 97.022 47.050 3.2375 + 0.0000 4.0900 106.82 52.154 1.7433 + 0.0000 4.0900 117.09 56.012 1.7433 + 0.0000 4.0900 131.19 71.450 1.7433 + 0.0000 4.0900 136.20 72.943 3.8601 + 0.0000 4.0900 140.27 86.017 1.7433 + 0.0000 4.0900 150.31 95.354 3.9846 + 0.0000 4.0900 158.90 94.730 1.6187 + 1.4500 3.7000 25.489 9.8879 2.4998 + 1.4500 3.7000 34.945 8.6383 1.3635 + 1.4500 3.7000 45.582 14.093 1.5908 + 1.4500 3.7000 51.018 20.456 1.5908 + 1.4500 3.7000 62.365 21.024 1.9316 + 1.4500 3.7000 73.002 25.456 1.9316 + 1.4500 3.7000 82.457 25.342 1.4771 + 1.4500 3.7000 90.967 27.729 1.4771 + 1.4500 3.7000 96.640 29.206 1.9316 + 1.4500 3.7000 116.97 31.479 1.5908 + 1.4500 3.7000 131.39 24.434 1.9316 + 1.4500 3.7000 135.64 26.821 1.7044 + 1.4500 3.7000 139.66 22.503 1.5908 + 1.4500 3.7000 150.77 17.276 2.0453 + 1.4500 3.7000 159.99 12.845 1.5908 + 1.4500 3.7000 165.43 13.754 1.5908 + 1.4500 3.8600 16.634 7.5897 1.7878 + 1.4500 3.8600 26.406 14.262 1.7878 + 1.4500 3.8600 36.410 20.101 2.9797 + 1.4500 3.8600 45.014 19.980 1.7878 + 1.4500 3.8600 52.457 21.886 2.2646 + 1.4500 3.8600 61.768 34.637 4.1716 + 1.4500 3.8600 71.769 35.589 1.5494 + 1.4500 3.8600 91.774 42.856 2.5029 + 1.4500 3.8600 96.665 53.939 2.5029 + 1.4500 3.8600 105.97 52.746 1.6686 + 1.4500 3.8600 115.27 50.241 1.7878 + 1.4500 3.8600 132.00 39.988 2.3838 + 1.4500 3.8600 139.67 32.001 2.9797 + 1.4500 3.8600 149.44 29.496 1.6686 + 1.4500 3.8600 159.90 19.840 1.6686 + 1.4500 4.0100 26.241 14.632 1.6898 + 1.4500 4.0100 36.097 21.272 1.6898 + 1.4500 4.0100 45.954 23.566 2.2933 + 1.4500 4.0100 52.526 25.378 1.6898 + 1.4500 4.0100 62.614 36.362 1.5691 + 1.4500 4.0100 72.938 45.778 2.4140 + 1.4500 4.0100 82.794 52.176 1.6898 + 1.4500 4.0100 92.651 54.833 2.8968 + 1.4500 4.0100 97.343 60.023 1.6898 + 1.4500 4.0100 117.06 63.164 1.5691 + 1.4500 4.0100 132.31 71.735 2.5347 + 1.4500 4.0100 137.24 77.167 1.5691 + 1.4500 4.0100 142.17 77.409 1.5691 + 1.4500 4.0100 150.62 79.462 3.6209 + 1.4500 4.0100 160.01 82.963 1.6898 + 1.4500 4.0100 165.40 81.033 1.4484 + 1.4500 4.0900 26.626 21.740 1.6906 + 1.4500 4.0900 36.117 24.758 1.6906 + 1.4500 4.0900 48.931 31.881 2.5359 + 1.4500 4.0900 72.897 45.404 1.6906 + 1.4500 4.0900 82.626 50.595 3.2604 + 1.4500 4.0900 92.592 55.787 1.9321 + 1.4500 4.0900 97.813 59.168 1.8113 + 1.4500 4.0900 112.76 71.000 1.8113 + 1.4500 4.0900 117.98 67.740 2.2943 + 1.4500 4.0900 127.00 65.324 1.5698 + 1.4500 4.0900 133.16 63.995 1.6906 + 1.4500 4.0900 137.20 63.632 1.6906 + 1.4500 4.0900 142.18 62.787 3.1396 + 1.4500 4.0900 159.50 67.495 1.5698 + 1.4500 4.0900 166.38 73.652 4.4679 +ENDDATA 150 +ENDSUBENT 162 +SUBENT F0696005 20041207 20050831 F021 +BIB 3 3 +REACTION (14-SI-28(HE3,P)15-P-30,PAR,DA) +ERR-ANALYS (ANG-ERR-D) Digitizing error +STATUS (CURVE)Fig.3 +ENDBIB 3 +COMMON 5 3 +E-LVL-MIN E-LVL-MAX DATA-ERR1 ANG-ERR-D ERR-DIG +MEV MEV PER-CENT ADEG MU-B/SR + 0.68 0.71 10. 0.1 0.1 +ENDCOMMON 3 +DATA 4 66 +EN ANG-CM DATA-CM DATA-ERR2 +MEV ADEG MU-B/SR MU-B/SR + 3.7000 0.60146 16.534 1.7140 + 3.7000 15.787 19.849 1.5997 + 3.7000 26.298 25.449 1.9425 + 3.7000 35.644 26.022 1.5997 + 3.7000 46.156 29.222 1.9425 + 3.7000 60.408 30.023 1.8283 + 3.7000 71.858 27.853 1.9425 + 3.7000 81.672 25.455 1.8283 + 3.7000 91.018 23.285 1.4855 + 3.7000 96.858 26.485 2.0568 + 3.7000 106.44 28.085 1.7140 + 3.7000 116.25 27.858 2.1711 + 3.7000 131.21 21.003 2.1711 + 3.7000 135.88 22.946 1.5997 + 3.7000 141.02 25.346 2.0568 + 3.7000 149.66 32.660 1.7140 + 3.7000 160.64 36.661 2.0568 + 3.7000 169.75 42.603 1.5997 + 3.8600 5.9885 14.879 1.7942 + 3.8600 16.481 17.746 2.5119 + 3.8600 34.898 20.252 1.9139 + 3.8600 46.093 25.512 2.5119 + 3.8600 62.889 36.511 1.6746 + 3.8600 71.517 39.858 3.1100 + 3.8600 91.796 39.732 1.7942 + 3.8600 96.921 36.501 2.2727 + 3.8600 106.25 37.096 1.6746 + 3.8600 117.44 42.834 1.7942 + 3.8600 127.70 42.233 2.2727 + 3.8600 130.96 47.136 1.6746 + 3.8600 135.39 44.981 1.5550 + 3.8600 140.76 50.482 2.8708 + 3.8600 151.26 57.297 1.6746 + 3.8600 161.05 61.002 2.6316 + 3.8600 170.84 64.109 1.7942 + 4.0100 6.7305 29.337 3.3566 + 4.0100 14.925 33.178 3.3566 + 4.0100 26.165 35.102 3.1168 + 4.0100 35.062 40.621 3.3566 + 4.0100 45.833 43.025 3.3566 + 4.0100 60.352 45.430 3.5963 + 4.0100 70.419 51.669 3.5963 + 4.0100 81.658 55.751 2.8771 + 4.0100 90.317 66.305 3.3566 + 4.0100 106.46 91.489 4.5554 + 4.0100 117.00 99.886 3.5964 + 4.0100 131.04 115.00 3.3566 + 4.0100 140.87 132.27 4.5554 + 4.0100 151.16 148.57 3.5963 + 4.0100 160.06 163.68 3.5963 + 4.0100 165.90 177.83 5.5144 + 4.0900 6.0541 27.617 1.6797 + 4.0900 16.631 32.775 1.4397 + 4.0900 26.272 47.891 2.0396 + 4.0900 35.676 57.608 1.5597 + 4.0900 46.725 65.525 1.5597 + 4.0900 50.958 72.484 3.1194 + 4.0900 71.640 77.641 3.4793 + 4.0900 81.746 78.479 1.6797 + 4.0900 90.906 65.281 1.5597 + 4.0900 97.485 61.441 3.8392 + 4.0900 117.23 64.319 1.6797 + 4.0900 132.74 68.516 3.3593 + 4.0900 140.97 78.953 1.6797 + 4.0900 161.42 90.349 2.1596 + 4.0900 169.88 94.548 1.4397 +ENDDATA 68 +ENDSUBENT 80 +ENDENTRY 5 diff --git a/exforall/F06/F0697.x4 b/exforall/F06/F0697.x4 new file mode 100644 index 000000000..697200223 --- /dev/null +++ b/exforall/F06/F0697.x4 @@ -0,0 +1,417 @@ +ENTRY F0697 20050606 20050831 F022 +SUBENT F0697001 20050606 20050831 F022 +BIB 13 31 +TITLE Backscattering of alpha-particles at C12 and C13. +AUTHOR (B.I.Kuznetsov,I.P.Chernov,R.E.Ovsyannikova) +INSTITUTE (4RUSTPI) Institute of nuclear physics, electronics and + automatics. +REFERENCE (J,YF,18,950,1973) +FACILITY (CYCLO) +INC-SOURCE Alpha-particle beam was focused with a pair of + quadrupole lenses and was deflected by turning the + magnet to the target under study. Before this it passed + through two quadrupole lenses and several collimating + splits. +INC-SPECT Beam divergency was less than 0.02 degree. +DETECTOR (SCIN) Two scintillation spectrometers with thin + crystals were placed under constant angles of 45-50 + degrees to an incident beam to measure the beam current + Faraday cup with current integrator was used. + (SIBAR) +METHOD (BCINT) +MONITOR (6-C-12(A,EL)6-C-12,,DA) Energy of incident alpha + particles was determined by comparison of the energy + of scattered particles at 176 degrees with the energy + of alpha-particles of reference spectrometric source. +SAMPLE Carbon foils of 0.28mg/cm2 thickness were used as a + target.They were enriched on C13 up to 80%. The target + was placed in the center of scatterring chamber with + a diameter of 1.5 m. +ERR-ANALYS (ANG-ERR) Error of a scattering angle measurement. + (ERR-DIG) Digitizing error + Errors of relative meauserements were 3-5 %, errors of + absolute measurements were 15 %. +HISTORY (20050131C) +ENDBIB 31 +COMMON 4 3 +EN-RSL ANG-RSL ANG-ERR ERR-DIG +PER-CENT ADEG ADEG PER-CENT + 1. 0.2 0.2 0.1 +ENDCOMMON 3 +ENDSUBENT 38 +SUBENT F0697002 20050606 20050831 F022 +BIB 3 3 +REACTION (6-C-12(A,EL)6-C-12,,DA) +ERR-ANALYS (ANG-ERR-D) Digitizing error +STATUS (CURVE)Fig.1 +ENDBIB 3 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.04 +ENDCOMMON 3 +DATA 3 155 +EN ANG-CM DATA-CM +MEV ADEG MB/SR + 18.000 111.90 3.9880 + 18.000 115.40 19.750 + 18.000 118.40 41.040 + 18.000 121.40 59.850 + 18.000 124.40 71.050 + 18.000 127.40 67.110 + 18.000 129.60 55.910 + 18.000 131.60 30.870 + 18.000 132.10 24.280 + 18.000 134.80 6.4540 + 18.000 136.80 2.0830 + 18.000 138.80 8.4920 + 18.000 139.50 24.580 + 18.000 142.50 59.930 + 18.000 144.80 95.750 + 18.000 147.30 123.10 + 18.000 149.80 133.40 + 18.000 152.30 126.00 + 18.000 154.10 100.30 + 18.000 156.30 57.300 + 18.000 158.00 19.810 + 18.000 160.10 3.9110 + 18.000 162.20 14.390 + 18.000 162.50 25.760 + 18.000 164.90 94.790 + 18.000 167.00 175.70 + 18.000 169.00 360.90 + 18.000 171.00 617.60 + 18.000 173.40 870.20 + 18.000 175.40 1033.0 + 18.000 177.00 1172.0 + 18.000 179.00 1328.0 + 19.000 123.10 63.080 + 19.000 125.80 47.510 + 19.000 128.30 36.640 + 19.000 131.10 20.790 + 19.000 133.00 5.8770 + 19.000 135.10 0.82780 + 19.000 139.00 7.7100 + 19.000 140.80 23.390 + 19.000 143.50 46.950 + 19.000 146.00 70.140 + 19.000 148.40 89.870 + 19.000 150.90 97.610 + 19.000 155.20 66.890 + 19.000 156.70 31.420 + 19.000 158.60 5.0990 + 19.000 160.60 1.4760 + 19.000 163.20 18.690 + 19.000 165.80 63.800 + 19.000 167.90 140.70 + 19.000 170.10 225.70 + 19.000 174.10 402.50 + 19.000 176.60 486.10 + 19.000 178.60 553.50 + 22.000 117.40 3.9460 + 22.000 120.10 5.7270 + 22.000 121.70 6.5860 + 22.000 123.20 7.1450 + 22.000 125.30 7.4830 + 22.000 127.30 6.7360 + 22.000 128.30 5.3340 + 22.000 131.00 3.9380 + 22.000 137.40 4.2690 + 22.000 140.20 5.9140 + 22.000 143.90 7.6390 + 22.000 145.90 9.7560 + 22.000 147.40 10.340 + 22.000 149.10 10.960 + 22.000 150.80 8.9850 + 22.000 152.60 5.7670 + 22.000 155.20 2.0910 + 22.000 157.10 1.8390 + 22.000 159.40 2.7970 + 22.000 160.90 5.9660 + 22.000 163.50 23.600 + 22.000 165.70 43.770 + 22.000 167.90 73.080 + 22.000 170.10 112.50 + 22.000 171.70 143.60 + 22.000 173.90 194.40 + 22.000 176.10 231.50 + 22.000 177.80 285.50 + 24.000 118.10 9.3630 + 24.000 120.60 10.150 + 24.000 123.40 13.040 + 24.000 126.10 15.300 + 24.000 128.80 14.300 + 24.000 130.90 11.920 + 24.000 134.30 8.9770 + 24.000 136.50 8.0140 + 24.000 138.60 5.6980 + 24.000 141.50 3.8280 + 24.000 144.30 4.4920 + 24.000 146.20 5.2700 + 24.000 148.50 6.1830 + 24.000 151.00 7.0120 + 24.000 155.70 8.1380 + 24.000 157.80 7.3490 + 24.000 160.20 6.9460 + 24.000 162.50 5.8580 + 24.000 166.50 10.240 + 24.000 168.70 13.620 + 24.000 170.80 18.320 + 24.000 171.80 27.610 + 24.000 172.80 32.020 + 24.000 174.60 35.080 + 24.000 176.80 35.910 + 24.000 178.30 36.750 + 25.000 123.50 8.6670 + 25.000 126.30 9.7470 + 25.000 129.20 10.110 + 25.000 131.70 10.240 + 25.000 134.80 9.6740 + 25.000 136.90 8.6230 + 25.000 138.00 7.5070 + 25.000 139.70 6.7680 + 25.000 142.00 7.9700 + 25.000 144.40 8.3580 + 25.000 149.20 7.2050 + 25.000 151.40 4.8620 + 25.000 153.30 3.3190 + 25.000 155.50 2.2920 + 25.000 158.10 1.8620 + 25.000 159.70 1.8210 + 25.000 162.10 1.6810 + 25.000 164.00 5.0640 + 25.000 164.60 7.2580 + 25.000 166.90 12.250 + 25.000 169.00 19.720 + 25.000 170.90 32.130 + 25.000 173.20 47.170 + 25.000 175.20 56.850 + 25.000 177.40 68.510 + 25.000 178.70 106.50 + 26.600 119.70 6.9720 + 26.600 122.80 6.8190 + 26.600 125.70 5.3660 + 26.600 128.00 4.8640 + 26.600 131.20 4.5050 + 26.600 134.70 3.7430 + 26.600 137.80 3.9500 + 26.600 140.70 6.0350 + 26.600 143.60 8.5440 + 26.600 146.20 8.2670 + 26.600 149.70 6.1600 + 26.600 153.20 4.2080 + 26.600 155.70 3.1020 + 26.600 159.00 1.0340 + 26.600 162.40 2.6910 + 26.600 164.90 6.8530 + 26.600 167.90 13.160 + 26.600 171.00 24.980 + 26.600 173.60 38.580 + 26.600 176.80 48.460 +ENDDATA 157 +ENDSUBENT 169 +SUBENT F0697003 20050606 20050831 F022 +BIB 3 3 +REACTION (6-C-13(A,EL)6-C-13,,DA) +ERR-ANALYS (ANG-ERR-D) Digitizing error +STATUS (CURVE)Fig.1 +ENDBIB 3 +COMMON 1 3 +ANG-ERR-D +ADEG + 0.04 +ENDCOMMON 3 +DATA 3 142 +EN ANG-CM DATA-CM +MEV ADEG MB/SR + 18.000 111.20 4.7340 + 18.000 113.90 3.5180 + 18.000 117.20 3.5590 + 18.000 119.60 4.3720 + 18.000 122.40 6.1610 + 18.000 125.30 7.3140 + 18.000 127.90 7.3150 + 18.000 130.80 5.0760 + 18.000 133.10 3.9040 + 18.000 136.00 3.5230 + 18.000 138.80 8.4920 + 18.000 141.00 12.100 + 18.000 143.60 17.850 + 18.000 148.50 27.570 + 18.000 151.00 27.890 + 18.000 153.50 24.040 + 18.000 155.40 18.920 + 18.000 157.50 13.280 + 18.000 159.90 9.3180 + 18.000 164.00 28.890 + 18.000 166.20 65.770 + 18.000 168.50 102.70 + 18.000 170.50 138.20 + 18.000 172.90 186.10 + 18.000 174.90 220.90 + 18.000 177.20 256.30 + 18.000 178.60 259.30 + 19.000 121.30 4.2230 + 19.000 123.80 4.4270 + 19.000 127.00 5.0410 + 19.000 129.50 5.1610 + 19.000 131.80 3.3340 + 19.000 134.50 1.8920 + 19.000 137.00 1.3120 + 19.000 139.70 3.1060 + 19.000 141.70 4.3230 + 19.000 144.20 7.0980 + 19.000 146.50 10.600 + 19.000 149.90 14.240 + 19.000 152.40 14.080 + 19.000 156.20 9.5340 + 19.000 158.70 7.2670 + 19.000 160.60 6.1600 + 19.000 162.90 8.1770 + 19.000 165.10 15.470 + 19.000 167.30 29.610 + 19.000 169.90 57.370 + 19.000 171.60 72.640 + 19.000 174.00 101.10 + 19.000 176.00 129.60 + 19.000 178.30 151.00 + 22.000 116.50 7.5810 + 22.000 118.60 6.8240 + 22.000 125.80 6.6590 + 22.000 130.00 7.8350 + 22.000 132.90 7.1350 + 22.000 135.20 6.1290 + 22.000 137.50 5.9170 + 22.000 140.20 5.9140 + 22.000 145.10 7.2900 + 22.000 149.60 12.450 + 22.000 152.30 13.830 + 22.000 154.40 12.300 + 22.000 158.80 7.1910 + 22.000 160.90 5.9660 + 22.000 163.10 6.8590 + 22.000 165.00 12.570 + 22.000 166.50 24.430 + 22.000 169.50 43.740 + 22.000 171.60 66.540 + 22.000 173.70 95.470 + 22.000 175.60 115.00 + 22.000 177.30 135.40 + 24.000 115.90 11.360 + 24.000 118.90 11.360 + 24.000 121.60 8.8520 + 24.000 124.30 4.9560 + 24.000 126.80 2.5910 + 24.000 129.50 1.9500 + 24.000 132.20 2.8410 + 24.000 134.80 5.1980 + 24.000 137.50 7.4020 + 24.000 140.00 8.3940 + 24.000 142.30 7.4090 + 24.000 144.80 5.9710 + 24.000 149.70 1.8090 + 24.000 152.10 0.68750 + 24.000 153.90 1.0130 + 24.000 156.20 2.1730 + 24.000 158.60 2.8570 + 24.000 160.90 3.6300 + 24.000 165.10 3.5920 + 24.000 166.90 2.8950 + 24.000 169.60 2.0120 + 24.000 172.10 1.8380 + 24.000 174.20 2.1560 + 24.000 177.70 2.8680 + 25.000 122.50 13.150 + 25.000 127.40 6.3490 + 25.000 129.80 3.6420 + 25.000 132.60 2.4870 + 25.000 135.30 4.1010 + 25.000 140.70 10.050 + 25.000 142.80 11.560 + 25.000 145.40 11.310 + 25.000 147.90 8.8720 + 25.000 150.10 5.3930 + 25.000 152.50 2.7880 + 25.000 153.90 1.2970 + 25.000 154.20 1.1690 + 25.000 156.40 1.1170 + 25.000 158.90 2.1660 + 25.000 161.20 3.4090 + 25.000 167.20 7.7910 + 25.000 170.40 7.4500 + 25.000 172.60 5.7780 + 25.000 176.70 2.3160 + 25.000 177.30 1.4900 + 26.600 113.50 3.7950 + 26.600 116.20 5.7350 + 26.600 118.80 6.2540 + 26.600 121.80 5.6690 + 26.600 127.20 2.8860 + 26.600 129.60 1.9080 + 26.600 132.50 1.9710 + 26.600 135.00 2.7300 + 26.600 140.00 5.1270 + 26.600 142.70 5.0700 + 26.600 144.70 4.1670 + 26.600 147.30 1.4040 + 26.600 151.90 0.33390 + 26.600 154.30 0.30260 + 26.600 156.30 0.73810 + 26.600 160.50 1.2170 + 26.600 162.70 1.0220 + 26.600 164.80 0.73720 + 26.600 167.20 0.67550 + 26.600 169.70 1.1760 + 26.600 171.20 1.6650 + 26.600 173.60 2.7750 + 26.600 175.90 4.6260 + 26.600 177.90 6.0690 +ENDDATA 144 +ENDSUBENT 156 +SUBENT F0697004 20050606 20050831 F022 +BIB 3 3 +REACTION (6-C-12(A,EL)6-C-12,,DA) +ERR-ANALYS (EN-ERR-DIG) Digitizing error +STATUS (CURVE)Fig.2 +ENDBIB 3 +COMMON 2 3 +ANG EN-ERR-DIG +ADEG MEV + 176. 0.02 +ENDCOMMON 3 +DATA 2 7 +EN DATA +MEV MB/SR + 17.950 3560.0 + 19.040 530.20 + 19.980 28.830 + 21.950 252.90 + 23.960 30.470 + 25.030 90.210 + 26.690 89.680 +ENDDATA 9 +ENDSUBENT 21 +SUBENT F0697005 20050606 20050831 F022 +BIB 3 3 +REACTION (6-C-13(A,EL)6-C-13,,DA) +ERR-ANALYS (EN-ERR-DIG) Digitizing error +STATUS (CURVE)Fig.2 +ENDBIB 3 +COMMON 2 3 +ANG EN-ERR-DIG +ADEG MEV + 176. 0.02 +ENDCOMMON 3 +DATA 2 7 +EN DATA +MEV MB/SR + 17.980 274.90 + 19.040 144.80 + 20.030 154.70 + 21.960 123.30 + 23.930 2.4940 + 24.990 1.1970 + 26.780 7.0050 +ENDDATA 9 +ENDSUBENT 21 +ENDENTRY 5 diff --git a/exforall/F06/F0699.x4 b/exforall/F06/F0699.x4 new file mode 100644 index 000000000..bf6a2b1fd --- /dev/null +++ b/exforall/F06/F0699.x4 @@ -0,0 +1,123 @@ +ENTRY F0699 20050415 20050831 F021 +SUBENT F0699001 20050415 20050831 F021 +BIB 10 27 +TITLE Polarization measurement of fast neutrons from the + 9Be(a,n)12C and the 13C(a,n)16O reaction using a + high-pressure 4He-polarimeter in a new design. +AUTHOR (W.Weiss,W.Grum,J.W.Hammer,M.Koch,G.Schreder) +INSTITUTE (2GERIFS) +REFERENCE (J,NIM/A,292,359,1990) +FACILITY (DYNAM) Stuttgart neutron scattering facility SCORPION. +DETECTOR Four shielded neutron detectors (NE 213) were + positioned and the range of the accessible reaction + angles was between 21 and 124 degr. with a symmetric + position of left and right detector. The minimum + angular distance between two detectors was limited by + the extension of the detector shielding to 42 degr. + Two detectors were at a forward scattering angle + of 50 degr and two detectors under a backscattering + angle of 124 degr. +METHOD (TOF) +COMMENT All measurements were performed using high-pressure + 4He polarimeters. +ERR-ANALYS (DATA-ERR) Definition error + Energetic resolution varied between 12% (13C, 5.4 MeV) + and 10% (9Be, 8.5 MeV). + The errors of the present experiment could be kept + small because of the use of the SCORPION facility + favouring small systematic errors and the fourfold + redundant measurement. +HISTORY (20030716C) +ENDBIB 27 +NOCOMMON 0 0 +ENDSUBENT 30 +SUBENT F0699002 20050415 20050831 F021 +BIB 2 2 +REACTION (4-BE-9(A,N)6-C-12,,POL/DA) +STATUS (TABLE)Table 1 +ENDBIB 2 +COMMON 1 3 +EN +MEV + 2.6 +ENDCOMMON 3 +DATA 3 5 +ANG DATA DATA-ERR +ADEG NO-DIM NO-DIM + 0.0000 0.0000 0.31000E-01 + 32.730 0.40400 0.24000E-01 + 54.180 0.60200 0.25000E-01 + 64.730 0.54100 0.26000E-01 + 74.100 0.36600 0.25000E-01 +ENDDATA 7 +ENDSUBENT 18 +SUBENT F0699003 20050415 20050831 F021 +BIB 2 2 +REACTION (4-BE-9(A,N)6-C-12,,POL/DA) +STATUS (TABLE)Table 2 +ENDBIB 2 +NOCOMMON 0 0 +DATA 4 10 +EN ANG DATA DATA-ERR +MEV ADEG NO-DIM NO-DIM + 1.9000 50.000 -.38000E-010.39000E-01 + 2.0600 50.000 -.27000E-010.27000E-01 + 2.2100 50.000 0.17600 0.26000E-01 + 2.3700 50.000 0.36100 0.26000E-01 + 2.5200 50.000 0.62700 0.29000E-01 + 2.6000 50.000 0.60200 0.25000E-01 + 2.7200 60.000 0.50000 0.30000E-01 + 2.7200 70.000 0.45200 0.39000E-01 + 2.8300 50.000 0.52500 0.32000E-01 + 3.0300 50.000 0.50800 0.33000E-01 +ENDDATA 12 +ENDSUBENT 19 +SUBENT F0699004 20050415 20050831 F021 +BIB 2 2 +REACTION (6-C-13(A,N)8-O-16,,POL/DA) +STATUS (TABLE)Table 3 +ENDBIB 2 +COMMON 1 3 +EN +MEV + 2.406 +ENDCOMMON 3 +DATA 3 8 +ANG DATA DATA-ERR +ADEG NO-DIM NO-DIM + 0.0000 0.0000 0.38000E-01 + 10.940 0.30000E-020.28000E-01 + 27.280 0.68000E-010.27000E-01 + 43.470 0.80000E-010.28000E-01 + 54.140 0.55000E-010.40000E-01 + 59.420 -.16100 0.47000E-01 + 68.850 -.34900 0.79000E-01 + 75.080 -.41300 0.47000E-01 +ENDDATA 10 +ENDSUBENT 21 +SUBENT F0699005 20050415 20050831 F021 +BIB 2 2 +REACTION (6-C-13(A,N)8-O-16,,POL/DA) +STATUS (TABLE)Table 4 +ENDBIB 2 +COMMON 1 3 +EN +MEV + 3.308 +ENDCOMMON 3 +DATA 3 10 +ANG DATA DATA-ERR +ADEG NO-DIM NO-DIM + 0.0000 0.0000 0.34000E-01 + 11.020 -.11500 0.27000E-01 + 22.000 -.16900 0.25000E-01 + 27.470 -.16700 0.44000E-01 + 35.100 -.14500 0.23000E-01 + 43.760 -.13000E-010.27000E-01 + 51.280 0.15100 0.24000E-01 + 59.800 0.16500 0.30000E-01 + 67.170 0.10300 0.34000E-01 + 75.510 -.16100 0.26000E-01 +ENDDATA 12 +ENDSUBENT 23 +ENDENTRY 5 diff --git a/exforall/F07/F0700.x4 b/exforall/F07/F0700.x4 new file mode 100644 index 000000000..e8b0577a8 --- /dev/null +++ b/exforall/F07/F0700.x4 @@ -0,0 +1,1460 @@ +ENTRY F0700 20050621 20050831 F022 +SUBENT F0700001 20050621 20050831 F022 +BIB 15 41 +TITLE Measurements of the elastic scattering cross-section of + alpha particles of the heavy and medium weight nuclei + in the vicinity of the Coulomb barrier in a wide + angular range. +AUTHOR (W.Karcz,I.Kluska,Z.Sanok,J.Szmider,J.Szymakowski, + S.Wiktor,R.Wolski) +INSTITUTE (3POLITJ) +REFERENCE (J,APP/B,3,525,1972) +FACILITY (CYCLO) +INC-SOURCE Collimated beam of alpha particles. +INC-SPECT The exact energies of the incident alpha particles at + half target thickness are given. +SAMPLE Nb, Pd, Ag, In, Sn, Ta, Pt, Am, Pb, Bi self-supporting + targets were made of natural elements. +DETECTOR (SIBAR) Three silicon surface barrier counters were + mounted on a rotatable arm inside the scattering + chamber. + After passing the target the beam was collected in + the Faraday cup connected with the current integrator. +MONITOR (83-BI-209(A,2N)85-AT-211,,DA) The energy measurements + were verified kinematically, determining the angle at + which the alpha peaks from two independent sources + coincided. + The intensity of the beam was monitored by + semiconductor counter viewing the target at a fixed + angle of 20 degrees. +METHOD (BCINT) +COMMENT The absolute values of cross-sections for all targets + except the lightest ones were determined by + normalization of the experimental data, taken at + relative small angles, to the Rutherford cross-section. +CORRECTION Corrections were node for energy loss in the targets. +ERR-ANALYS (ANG-ERR) The accuracy of the angle setting + (DATA-ERR1) Data error from table + (DATA-ERR2) Error of absolute value of cross-section + The error of the absolute value of the cross-section + was evaluated individually taking into account the + possible energy fluctuation of the beam. + The accuracy of the measurement of the absolute energy + value was estimated to be +-150 keV. +HISTORY (20050425C) +ENDBIB 41 +COMMON 2 3 +EN-RSL ANG-ERR +KEV ADEG + 350. 0.1 +ENDCOMMON 3 +ENDSUBENT 48 +SUBENT F0700002 20050621 20050831 F022 +BIB 4 8 +REACTION (41-NB-93(A,EL)41-NB-93,,DA) +SAMPLE 41Nb target (rolled) was used. The Nb target was + contaminated by a small percentage of tantalium. This + contamination was determined by chemical analysis. +CORRECTION For angles smaller than 90 degrees the contribution of + alpha particles scattered on tantalium was calculated + and subtracted. +STATUS (CURVE)Table 2 +ENDBIB 8 +COMMON 1 3 +THICKNESS +G/CM-SQ + 0.0037 +ENDCOMMON 3 +DATA 5 100 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 +MEV ADEG MB/SR MB/SR PER-CENT + 23.100 10.430 0.26400E+06 10000. 5.5000 + 23.100 13.030 0.10400E+06 3000.0 5.5000 + 23.100 15.640 52800. 1700.0 5.5000 + 23.100 18.240 30800. 1100.0 5.5000 + 23.100 20.840 20400. 1000.0 5.5000 + 23.100 23.450 12300. 400.00 5.5000 + 23.100 26.040 8120.0 410.00 5.5000 + 23.100 28.640 5230.0 260.00 5.5000 + 23.100 31.230 3330.0 170.00 5.5000 + 23.100 33.830 2050.0 100.00 5.5000 + 23.100 36.420 1390.0 70.000 5.5000 + 23.100 39.000 958.00 48.000 5.5000 + 23.100 41.590 627.00 32.000 5.5000 + 23.100 44.170 407.00 20.000 5.5000 + 23.100 46.750 274.00 14.000 5.5000 + 23.100 49.320 198.00 10.000 5.5000 + 23.100 51.890 150.00 8.0000 5.5000 + 23.100 54.460 110.00 6.0000 5.5000 + 23.100 57.020 78.900 3.9000 5.5000 + 23.100 59.580 52.700 2.6000 5.5000 + 23.100 62.140 38.500 1.9000 5.5000 + 23.100 64.690 31.500 1.6000 5.5000 + 23.100 67.240 25.200 1.3000 5.5000 + 23.100 69.780 19.700 1.0000 5.5000 + 23.100 72.320 13.900 0.70000 5.5000 + 23.100 74.860 9.7100 0.49000 5.5000 + 23.100 77.390 7.6700 0.38000 5.5000 + 23.100 79.910 6.9200 0.59000 5.5000 + 23.100 82.430 5.5900 0.48000 5.5000 + 23.100 84.950 4.3900 0.37000 5.5000 + 23.100 87.460 3.5400 0.30000 5.5000 + 23.100 89.970 2.7200 0.23000 5.5000 + 23.100 92.470 2.0800 0.18000 5.5000 + 23.100 94.970 1.6600 0.14000 5.5000 + 23.100 97.460 1.5700 0.13000 5.5000 + 23.100 99.950 1.4200 0.12000 5.5000 + 23.100 102.43 1.1500 0.10000 5.5000 + 23.100 104.91 0.85900 0.73000E-01 5.5000 + 23.100 107.39 0.81300 0.69000E-01 5.5000 + 23.100 109.86 0.59100 0.50000E-01 5.5000 + 23.100 112.32 0.56700 0.48000E-01 5.5000 + 23.100 114.78 0.48900 0.42000E-01 5.5000 + 23.100 117.24 0.49900 0.42000E-01 5.5000 + 23.100 119.69 0.38200 0.33000E-01 5.5000 + 23.100 122.14 0.30600 0.26000E-01 5.5000 + 23.100 124.58 0.24500 0.21000E-01 5.5000 + 23.100 127.02 0.29200 0.25000E-01 5.5000 + 23.100 129.46 0.24500 0.21000E-01 5.5000 + 23.100 131.89 0.21700 0.18000E-01 5.5000 + 23.100 134.32 0.21000 0.18000E-01 5.5000 + 23.100 136.75 0.17700 0.15000E-01 5.5000 + 23.100 139.17 0.12300 0.10000E-01 5.5000 + 23.100 141.59 0.13000 0.11000E-01 5.5000 + 27.300 10.430 0.17300E+06 9000.0 7.0000 + 27.300 13.030 71100. 3000.0 7.0000 + 27.300 15.640 38900. 1600.0 7.0000 + 27.300 18.240 21300. 600.00 7.0000 + 27.300 20.840 12100. 300.00 7.0000 + 27.300 23.450 7110.0 180.00 7.0000 + 27.300 26.040 4160.0 80.000 7.0000 + 27.300 28.640 2200.0 40.000 7.0000 + 27.300 31.230 1310.0 30.000 7.0000 + 27.300 33.830 873.00 13.000 7.0000 + 27.300 36.420 561.00 16.000 7.0000 + 27.300 39.000 323.00 6.0000 7.0000 + 27.300 41.590 187.00 9.0000 7.0000 + 27.300 44.170 147.00 4.0000 7.0000 + 27.300 46.750 108.00 3.0000 7.0000 + 27.300 49.320 67.600 1.8000 7.0000 + 27.300 51.890 42.800 1.4000 7.0000 + 27.300 54.460 29.100 1.1000 7.0000 + 27.300 57.020 24.800 1.0000 7.0000 + 27.300 59.580 19.500 0.80000 7.0000 + 27.300 62.140 13.700 0.40000 7.0000 + 27.300 64.690 8.1400 0.42000 7.0000 + 27.300 67.240 5.7200 0.30000 7.0000 + 27.300 69.780 5.3700 0.23000 7.0000 + 27.300 72.320 4.4400 0.17000 7.0000 + 27.300 74.860 3.2500 0.13000 7.0000 + 27.300 77.390 2.0100 0.15000 7.0000 + 27.300 79.910 1.4200 0.90000E-01 7.0000 + 27.300 82.430 1.1500 0.70000E-01 7.0000 + 27.300 84.950 1.1900 0.50000E-01 7.0000 + 27.300 87.460 1.1500 0.40000E-01 7.0000 + 27.300 89.970 0.86500 0.66000E-01 7.0000 + 27.300 92.470 0.48400 0.25000E-01 7.0000 + 27.300 94.970 0.32300 0.21000E-01 7.0000 + 27.300 97.460 0.30300 0.24000E-01 7.0000 + 27.300 99.950 0.32300 0.24000E-01 7.0000 + 27.300 102.43 0.32000 0.24000E-01 7.0000 + 27.300 104.91 0.26500 0.20000E-01 7.0000 + 27.300 107.39 0.18900 0.14000E-01 7.0000 + 27.300 109.86 0.11800 0.90000E-02 7.0000 + 27.300 112.32 0.83800E-010.60000E-02 7.0000 + 27.300 114.78 0.96100E-010.80000E-02 7.0000 + 27.300 117.24 0.11000 0.90000E-02 7.0000 + 27.300 119.69 0.11100 0.90000E-02 7.0000 + 27.300 122.14 0.89400E-010.72000E-02 7.0000 + 27.300 124.58 0.80400E-010.85000E-02 7.0000 + 27.300 127.02 0.46300E-010.38000E-02 7.0000 +ENDDATA 102 +ENDSUBENT 119 +SUBENT F0700003 20050621 20050831 F022 +BIB 3 3 +REACTION (46-PD-0(A,EL)46-PD-0,,DA) +SAMPLE Pd target : rolled +STATUS (CURVE)Table 2 +ENDBIB 3 +COMMON 1 3 +THICKNESS +G/CM-SQ + 0.004 +ENDCOMMON 3 +DATA 5 117 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 +MEV ADEG MB/SR MB/SR PER-CENT + 23.100 10.370 0.32100E+06 11000. 4.0000 + 23.100 11.600 0.24600E+06 8000.0 4.0000 + 23.100 12.960 0.13700E+06 4000.0 4.0000 + 23.100 15.560 63000. 1800.0 4.0000 + 23.100 16.850 53000. 1500.0 4.0000 + 23.100 18.150 34400. 900.00 4.0000 + 23.100 20.730 21900. 600.00 4.0000 + 23.100 22.000 19800. 600.00 4.0000 + 23.100 23.320 14600. 400.00 4.0000 + 23.100 25.910 9900.0 240.00 4.0000 + 23.100 28.490 7190.0 170.00 4.0000 + 23.100 31.070 4850.0 120.00 4.0000 + 23.100 33.650 3340.0 80.000 4.0000 + 23.100 36.230 2340.0 60.000 4.0000 + 23.100 38.810 1640.0 20.000 4.0000 + 23.100 41.380 1170.0 30.000 4.0000 + 23.100 43.950 821.00 12.000 4.0000 + 23.100 46.520 560.00 14.000 4.0000 + 23.100 49.080 388.00 6.0000 4.0000 + 23.100 51.650 298.00 5.0000 4.0000 + 23.100 54.210 229.00 4.0000 4.0000 + 23.100 56.760 165.00 3.0000 4.0000 + 23.100 59.310 124.00 2.0000 4.0000 + 23.100 61.860 84.600 2.1000 4.0000 + 23.100 64.410 70.600 1.4000 4.0000 + 23.100 66.950 54.200 0.60000 4.0000 + 23.100 69.490 41.000 0.50000 4.0000 + 23.100 72.020 31.600 0.40000 4.0000 + 23.100 74.550 24.200 0.40000 4.0000 + 23.100 77.080 19.100 0.30000 4.0000 + 23.100 79.600 15.100 0.30000 4.0000 + 23.100 82.120 12.200 0.20000 4.0000 + 23.100 84.630 9.5100 0.16000 4.0000 + 23.100 87.140 7.6200 0.15000 4.0000 + 23.100 89.650 6.4200 0.13000 4.0000 + 23.100 92.150 5.1500 0.12000 4.0000 + 23.100 94.650 4.3600 0.11000 4.0000 + 23.100 97.140 3.5600 0.10000 4.0000 + 23.100 99.630 2.9900 0.60000E-01 4.0000 + 23.100 102.12 2.4000 0.80000E-01 4.0000 + 23.100 104.60 2.1100 0.50000E-01 4.0000 + 23.100 107.08 1.8300 0.70000E-01 4.0000 + 23.100 109.55 1.5700 0.60000E-01 4.0000 + 23.100 112.02 1.3300 0.50000E-01 4.0000 + 23.100 114.49 1.1500 0.30000E-01 4.0000 + 23.100 116.35 0.97100 0.42000E-01 4.0000 + 23.100 119.41 0.92800 0.26000E-01 4.0000 + 23.100 121.86 0.68500 0.34000E-01 4.0000 + 23.100 124.31 0.71800 0.23000E-01 4.0000 + 23.100 126.76 0.65100 0.23000E-01 4.0000 + 23.100 129.21 0.60700 0.26000E-01 4.0000 + 23.100 131.65 0.52000 0.21000E-01 4.0000 + 23.100 134.08 0.45700 0.23000E-01 4.0000 + 23.100 136.52 0.44300 0.19000E-01 4.0000 + 23.100 138.95 0.38700 0.20000E-01 4.0000 + 23.100 141.38 0.39000 0.27000E-01 4.0000 + 23.100 146.23 0.31500 0.25000E-01 4.0000 + 23.100 151.07 0.25700 0.22000E-01 4.0000 + 27.300 10.370 0.24100E+06 14000. 6.0000 + 27.300 12.960 94900. 2600.0 6.0000 + 27.300 15.560 47800. 1800.0 6.0000 + 27.300 18.150 26400. 2500.0 6.0000 + 27.300 20.730 17600. 700.00 6.0000 + 27.300 23.320 10700. 200.00 6.0000 + 27.300 25.910 6640.0 180.00 6.0000 + 27.300 28.490 3900.0 110.00 6.0000 + 27.300 31.070 2390.0 40.000 6.0000 + 27.300 33.650 1560.0 50.000 6.0000 + 27.300 36.230 965.00 37.000 6.0000 + 27.300 38.810 617.00 22.000 6.0000 + 27.300 41.380 374.00 8.0000 6.0000 + 27.300 43.950 260.00 3.0000 6.0000 + 27.300 46.520 179.00 8.0000 6.0000 + 27.300 49.080 118.00 2.0000 6.0000 + 27.300 51.650 76.600 5.1000 6.0000 + 27.300 54.210 59.600 1.0000 6.0000 + 27.300 56.760 44.600 1.3000 6.0000 + 27.300 59.310 32.000 0.80000 6.0000 + 27.300 61.860 21.900 0.60000 6.0000 + 27.300 64.410 14.900 0.30000 6.0000 + 27.300 66.950 11.400 0.40000 6.0000 + 27.300 69.490 9.5400 0.25000 6.0000 + 27.300 72.020 7.5400 0.15000 6.0000 + 27.300 74.550 5.4100 0.80000E-01 6.0000 + 27.300 77.080 3.9400 0.90000E-01 6.0000 + 27.300 79.600 3.0200 0.50000E-01 6.0000 + 27.300 82.120 2.4600 0.90000E-01 6.0000 + 27.300 84.630 2.1400 0.70000E-01 6.0000 + 27.300 87.140 1.6000 0.30000E-01 6.0000 + 27.300 89.650 1.2900 0.30000E-01 6.0000 + 27.300 92.150 0.93100 0.48000E-01 6.0000 + 27.300 94.650 0.73400 0.10000E-01 6.0000 + 27.300 97.140 0.61500 0.28000E-01 6.0000 + 27.300 99.630 0.54800 0.80000E-02 6.0000 + 27.300 102.12 0.46400 0.12000E-01 6.0000 + 27.300 104.60 0.40200 0.60000E-02 6.0000 + 27.300 107.08 0.31600 0.80000E-02 6.0000 + 27.300 109.55 0.25300 0.11000E-01 6.0000 + 27.300 112.02 0.21300 0.30000E-02 6.0000 + 27.300 114.49 0.20000 0.12000E-01 6.0000 + 27.300 116.35 0.17000 0.40000E-02 6.0000 + 27.300 119.41 0.13500 0.50000E-02 6.0000 + 27.300 121.86 0.12800 0.30000E-02 6.0000 + 27.300 124.31 0.10700 0.60000E-02 6.0000 + 27.300 126.76 0.99400E-010.26000E-02 6.0000 + 27.300 129.21 0.91300E-010.46000E-02 6.0000 + 27.300 131.65 0.75900E-010.48000E-02 6.0000 + 27.300 134.08 0.64400E-010.45000E-02 6.0000 + 27.300 136.52 0.57500E-010.43000E-02 6.0000 + 27.300 138.95 0.47400E-010.39000E-02 6.0000 + 27.300 141.38 0.38400E-010.34000E-02 6.0000 + 27.300 143.81 0.39100E-010.34000E-02 6.0000 + 27.300 146.23 0.43400E-010.32000E-02 6.0000 + 27.300 148.66 0.33300E-010.28000E-02 6.0000 + 27.300 151.07 0.45400E-010.33000E-02 6.0000 + 27.300 153.49 0.40500E-010.31000E-02 6.0000 + 27.300 155.91 0.31100E-010.29000E-02 6.0000 +ENDDATA 119 +ENDSUBENT 131 +SUBENT F0700004 20050621 20050831 F022 +BIB 3 3 +REACTION (47-AG-0(A,EL)47-AG-0,,DA) +SAMPLE 47Ag target : evaporated +STATUS (CURVE)Table 2 +ENDBIB 3 +NOCOMMON 0 0 +DATA 6 113 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 THICKNESS +MEV ADEG MB/SR MB/SR PER-CENT G/CM-SQ + 23.200 10.370 0.34500E+06 9000.0 5.0000 0.17000E-02 + 23.200 12.960 0.14500E+06 4000.0 5.0000 0.17000E-02 + 23.200 15.550 67300. 1600.0 5.0000 0.17000E-02 + 23.200 18.140 36400. 2400.0 5.0000 0.17000E-02 + 23.200 20.730 22900. 800.00 5.0000 0.17000E-02 + 23.200 23.310 14400. 1000.0 5.0000 0.17000E-02 + 23.200 25.900 10300. 200.00 5.0000 0.17000E-02 + 23.200 28.480 7220.0 170.00 5.0000 0.17000E-02 + 23.200 31.060 5120.0 50.000 5.0000 0.17000E-02 + 23.200 33.640 3650.0 230.00 5.0000 0.17000E-02 + 23.200 36.220 2400.0 40.000 5.0000 0.17000E-02 + 23.200 38.790 1810.0 100.00 5.0000 0.17000E-02 + 23.200 41.370 1250.0 60.000 5.0000 0.17000E-02 + 23.200 43.940 873.00 61.000 5.0000 0.17000E-02 + 23.200 46.500 673.00 57.000 5.0000 0.17000E-02 + 23.200 49.070 468.00 28.000 5.0000 0.17000E-02 + 23.200 51.630 347.00 26.000 5.0000 0.17000E-02 + 23.200 54.190 251.00 17.000 5.0000 0.17000E-02 + 23.200 56.740 186.00 16.000 5.0000 0.17000E-02 + 23.200 59.290 136.00 12.000 5.0000 0.17000E-02 + 23.200 61.840 98.400 6.2000 5.0000 0.17000E-02 + 23.200 64.390 82.600 5.2000 5.0000 0.17000E-02 + 23.200 66.930 55.700 4.3000 5.0000 0.17000E-02 + 23.200 69.470 46.500 0.50000 5.0000 0.17000E-02 + 23.200 72.000 36.200 0.50000 5.0000 0.17000E-02 + 23.200 74.530 28.400 0.40000 5.0000 0.17000E-02 + 23.200 77.050 21.000 0.40000 5.0000 0.17000E-02 + 23.200 79.580 17.100 0.30000 5.0000 0.17000E-02 + 23.200 82.090 13.800 0.20000 5.0000 0.17000E-02 + 23.200 84.610 10.600 0.20000 5.0000 0.17000E-02 + 23.200 87.120 9.2200 0.17000 5.0000 0.17000E-02 + 23.200 89.620 7.2300 0.15000 5.0000 0.17000E-02 + 23.200 92.130 5.9900 0.13000 5.0000 0.17000E-02 + 23.200 94.620 4.9100 0.12000 5.0000 0.17000E-02 + 23.200 97.120 3.9100 0.90000E-01 5.0000 0.17000E-02 + 23.200 99.610 3.3500 0.10000 5.0000 0.17000E-02 + 23.200 102.09 2.7600 0.70000E-01 5.0000 0.17000E-02 + 23.200 104.58 2.3300 0.60000E-01 5.0000 0.17000E-02 + 23.200 107.05 2.0100 0.60000E-01 5.0000 0.17000E-02 + 23.200 109.53 1.7300 0.50000E-01 5.0000 0.17000E-02 + 23.200 112.02 1.4300 0.40000E-01 5.0000 0.17000E-02 + 23.200 114.47 1.3000 0.70000E-01 5.0000 0.17000E-02 + 23.200 116.93 1.1100 0.60000E-01 5.0000 0.17000E-02 + 23.200 119.39 0.96800 0.48000 5.0000 0.17000E-02 + 23.200 121.84 0.85500 0.43000 5.0000 0.17000E-02 + 23.200 124.29 0.70000 0.35000 5.0000 0.17000E-02 + 23.200 126.74 0.62000 0.31000 5.0000 0.17000E-02 + 23.200 129.19 0.56000 0.28000 5.0000 0.17000E-02 + 23.200 131.63 0.52200 0.26000 5.0000 0.17000E-02 + 23.200 134.07 0.47100 0.24000 5.0000 0.17000E-02 + 23.200 136.50 0.40000 0.20000 5.0000 0.17000E-02 + 23.200 138.94 0.39300 0.20000 5.0000 0.17000E-02 + 23.200 141.37 0.36900 0.19000 5.0000 0.17000E-02 + 23.200 143.79 0.34200 0.17000 5.0000 0.17000E-02 + 23.200 146.22 0.30000 0.15000 5.0000 0.17000E-02 + 23.200 148.64 0.26600 0.13000 5.0000 0.17000E-02 + 23.200 151.06 0.25900 0.13000 5.0000 0.17000E-02 + 23.200 153.48 0.22000 0.11000 5.0000 0.17000E-02 + 23.200 155.90 0.24300 0.12000 5.0000 0.17000E-02 + 23.200 158.31 0.24100 0.12000 5.0000 0.17000E-02 + 23.200 160.73 0.22900 0.12000 5.0000 0.17000E-02 + 23.200 163.14 0.21400 0.11000 5.0000 0.17000E-02 + 23.200 165.55 0.20600 0.10000 5.0000 0.17000E-02 + 23.200 167.96 0.21000 0.10000 5.0000 0.17000E-02 + 27.500 10.370 0.24500E+06 11000. 4.5000 0.13000E-02 + 27.500 12.960 96900. 3100.0 4.5000 0.13000E-02 + 27.500 15.550 46200. 2100.0 4.5000 0.13000E-02 + 27.500 18.140 27800. 1000.0 4.5000 0.13000E-02 + 27.500 20.730 16800. 800.00 4.5000 0.13000E-02 + 27.500 23.310 10400. 400.00 4.5000 0.13000E-02 + 27.500 25.900 6930.0 110.00 4.5000 0.13000E-02 + 27.500 28.480 4040.0 40.000 4.5000 0.13000E-02 + 27.500 31.060 2490.0 50.000 4.5000 0.13000E-02 + 27.500 33.640 1530.0 20.000 4.5000 0.13000E-02 + 27.500 36.220 1010.0 10.000 4.5000 0.13000E-02 + 27.500 38.790 608.00 21.000 4.5000 0.13000E-02 + 27.500 41.370 393.00 9.0000 4.5000 0.13000E-02 + 27.500 43.940 268.00 3.0000 4.5000 0.13000E-02 + 27.500 46.500 191.00 2.0000 4.5000 0.13000E-02 + 27.500 49.070 119.00 3.0000 4.5000 0.13000E-02 + 27.500 51.630 83.800 0.80000 4.5000 0.13000E-02 + 27.500 54.190 59.300 0.10000 4.5000 0.13000E-02 + 27.500 56.740 42.900 0.40000 4.5000 0.13000E-02 + 27.500 59.290 30.600 0.70000 4.5000 0.13000E-02 + 27.500 61.840 22.100 0.80000 4.5000 0.13000E-02 + 27.500 64.390 15.000 0.20000 4.5000 0.13000E-02 + 27.500 66.930 11.400 0.20000 4.5000 0.13000E-02 + 27.500 69.470 9.0700 0.20000 4.5000 0.13000E-02 + 27.500 72.000 7.0100 0.11000 4.5000 0.13000E-02 + 27.500 74.530 5.0400 0.14000 4.5000 0.13000E-02 + 27.500 77.050 3.5800 0.70000E-01 4.5000 0.13000E-02 + 27.500 79.580 2.7000 0.60000E-01 4.5000 0.13000E-02 + 27.500 82.090 2.2300 0.50000E-01 4.5000 0.13000E-02 + 27.500 84.610 1.9200 0.30000E-01 4.5000 0.13000E-02 + 27.500 87.120 1.5900 0.40000E-01 4.5000 0.13000E-02 + 27.500 89.620 1.1500 0.20000E-01 4.5000 0.13000E-02 + 27.500 92.130 0.82700 0.14000E-01 4.5000 0.13000E-02 + 27.500 94.620 0.65900 0.37000E-01 4.5000 0.13000E-02 + 27.500 97.120 0.55600 0.12000E-01 4.5000 0.13000E-02 + 27.500 99.610 0.49500 0.80000E-02 4.5000 0.13000E-02 + 27.500 102.09 0.42400 0.12000E-01 4.5000 0.13000E-02 + 27.500 104.58 0.32800 0.24000E-01 4.5000 0.13000E-02 + 27.500 107.05 0.26800 0.70000E-02 4.5000 0.13000E-02 + 27.500 109.53 0.21100 0.70000E-02 4.5000 0.13000E-02 + 27.500 112.02 0.18400 0.60000E-02 4.5000 0.13000E-02 + 27.500 114.47 0.14600 0.90000E-02 4.5000 0.13000E-02 + 27.500 116.93 0.12500 0.40000E-02 4.5000 0.13000E-02 + 27.500 119.39 0.11800 0.11000E-01 4.5000 0.13000E-02 + 27.500 121.84 0.11000 0.40000E-02 4.5000 0.13000E-02 + 27.500 124.29 0.90600E-010.36000E-02 4.5000 0.13000E-02 + 27.500 126.74 0.77000E-010.25000E-02 4.5000 0.13000E-02 + 27.500 129.19 0.65100E-010.36000E-02 4.5000 0.13000E-02 + 27.500 131.63 0.57800E-010.27000E-02 4.5000 0.13000E-02 +ENDDATA 115 +ENDSUBENT 123 +SUBENT F0700005 20050621 20050831 F022 +BIB 3 3 +REACTION (49-IN-0(A,EL)49-IN-0,,DA) +SAMPLE 49In target : evaporated +STATUS (CURVE)Table 2 +ENDBIB 3 +COMMON 1 3 +THICKNESS +G/CM-SQ + 0.0014 +ENDCOMMON 3 +DATA 5 136 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 +MEV ADEG MB/SR MB/SR PER-CENT + 23.500 10.350 0.35900E+06 15000. 4.0000 + 23.500 12.930 0.15900E+06 6000.0 4.0000 + 23.500 15.920 73000. 2600.0 4.0000 + 23.500 18.100 38800. 1500.0 4.0000 + 23.500 20.680 22400. 800.00 4.0000 + 23.500 23.260 15300. 500.00 4.0000 + 23.500 25.840 10100. 300.00 4.0000 + 23.500 28.420 7780.0 150.00 4.0000 + 23.500 31.000 5210.0 110.00 4.0000 + 23.500 33.570 3940.0 170.00 4.0000 + 23.500 36.150 2580.0 50.000 4.0000 + 23.500 38.720 1960.0 60.000 4.0000 + 23.500 41.280 1320.0 10.000 4.0000 + 23.500 43.850 909.00 7.0000 4.0000 + 23.500 46.410 646.00 5.0000 4.0000 + 23.500 48.970 441.00 3.0000 4.0000 + 23.500 51.530 335.00 3.0000 4.0000 + 23.500 54.080 241.00 3.0000 4.0000 + 23.500 56.640 188.00 4.0000 4.0000 + 23.500 59.190 136.00 6.0000 4.0000 + 23.500 61.730 102.00 4.0000 4.0000 + 23.500 64.270 73.900 3.2000 4.0000 + 23.500 66.810 59.400 0.70000 4.0000 + 23.500 69.350 44.400 0.70000 4.0000 + 23.500 71.880 33.200 1.5000 4.0000 + 23.500 74.410 25.400 0.80000 4.0000 + 23.500 76.930 19.500 0.80000 4.0000 + 23.500 79.450 15.500 0.30000 4.0000 + 23.500 81.970 12.500 0.50000 4.0000 + 23.500 84.480 10.100 0.30000 4.0000 + 23.500 86.990 7.6000 0.27000 4.0000 + 23.500 89.500 6.3100 0.20000 4.0000 + 23.500 92.000 5.0300 0.22000 4.0000 + 23.500 94.500 4.1500 0.60000E-01 4.0000 + 23.500 96.990 3.3400 0.14000 4.0000 + 23.500 99.480 2.8500 0.60000E-01 4.0000 + 23.500 101.97 2.4900 0.80000E-01 4.0000 + 23.500 104.45 1.9800 0.10000 4.0000 + 23.500 106.93 1.8000 0.70000E-01 4.0000 + 23.500 109.40 1.4200 0.60000E-01 4.0000 + 23.500 111.88 1.2500 0.40000E-01 4.0000 + 23.500 114.35 0.96500 0.29000E-01 4.0000 + 23.500 116.81 0.85400 0.26000E-01 4.0000 + 23.500 119.27 0.71800 0.29000E-01 4.0000 + 23.500 121.73 0.63900 0.19000E-01 4.0000 + 23.500 124.19 0.54100 0.22000E-01 4.0000 + 23.500 126.64 0.48100 0.15000E-01 4.0000 + 23.500 129.09 0.46000 0.18000E-01 4.0000 + 23.500 131.53 0.38600 0.12000E-01 4.0000 + 23.500 133.97 0.32200 0.80000E-02 4.0000 + 23.500 136.41 0.31700 0.13000E-01 4.0000 + 23.500 138.85 0.26200 0.70000E-02 4.0000 + 23.500 141.28 0.21900 0.60000E-02 4.0000 + 23.500 143.72 0.19900 0.10000E-01 4.0000 + 23.500 146.15 0.18700 0.60000E-02 4.0000 + 23.500 148.57 0.18250 0.73000E-01 4.0000 + 23.500 151.00 0.17400 0.90000E-02 4.0000 + 23.500 153.42 0.16900 0.50000E-02 4.0000 + 23.500 155.84 0.17300 0.52000E-01 4.0000 + 23.500 158.26 0.17300 0.70000E-02 4.0000 + 23.500 160.68 0.17200 0.90000E-02 4.0000 + 23.500 163.10 0.14500 0.70000E-02 4.0000 + 23.500 165.52 0.13400 0.40000E-02 4.0000 + 23.500 167.93 0.12000 0.40000E-02 4.0000 + 23.500 170.35 0.11300 0.30000E-02 4.0000 + 23.500 172.76 0.99300E-010.40000E-02 4.0000 + 23.500 175.17 0.99100E-010.60000E-02 4.0000 + 23.500 177.58 0.95400E-010.85000E-02 4.0000 + 27.640 10.350 0.25000E+06 9000.0 5.0000 + 27.640 12.930 0.10200E+06 3000.0 5.0000 + 27.640 15.520 47200. 1600.0 5.0000 + 27.640 18.100 29100. 900.00 5.0000 + 27.640 20.680 17600. 600.00 5.0000 + 27.640 23.260 11800. 400.00 5.0000 + 27.640 25.840 7830.0 150.00 5.0000 + 27.640 28.420 4880.0 100.00 5.0000 + 27.640 31.000 2900.0 50.000 5.0000 + 27.640 33.570 1980.0 30.000 5.0000 + 27.640 36.150 1230.0 20.000 5.0000 + 27.640 38.720 750.00 12.000 5.0000 + 27.640 41.280 474.00 8.0000 5.0000 + 27.640 43.850 330.00 6.0000 5.0000 + 27.640 46.410 252.00 4.0000 5.0000 + 27.640 48.970 152.00 3.0000 5.0000 + 27.640 51.530 97.200 1.7000 5.0000 + 27.640 54.080 70.500 1.5000 5.0000 + 27.640 56.640 47.800 0.80000 5.0000 + 27.640 59.190 38.500 0.80000 5.0000 + 27.640 61.730 25.200 0.60000 5.0000 + 27.640 64.270 17.800 0.40000 5.0000 + 27.640 66.810 13.600 0.30000 5.0000 + 27.640 69.350 11.600 0.30000 5.0000 + 27.640 71.880 8.2700 0.20000 5.0000 + 27.640 74.410 5.4600 0.14000 5.0000 + 27.640 76.930 3.9400 0.11000 5.0000 + 27.640 79.450 3.1100 0.90000E-01 5.0000 + 27.640 81.970 2.8100 0.80000E-01 5.0000 + 27.640 84.480 2.2100 0.50000E-01 5.0000 + 27.640 86.990 1.7600 0.40000E-01 5.0000 + 27.640 89.500 1.2200 0.30000E-01 5.0000 + 27.640 92.000 0.83000 0.29000E-01 5.0000 + 27.640 94.500 0.71400 0.24000E-01 5.0000 + 27.640 96.990 0.64700 0.22000E-01 5.0000 + 27.640 99.480 0.60600 0.24000E-01 5.0000 + 27.640 101.97 0.51300 0.18000E-01 5.0000 + 27.640 104.45 0.34900 0.14000E-01 5.0000 + 27.640 106.93 0.22900 0.12000E-01 5.0000 + 27.640 109.40 0.21800 0.90000E-02 5.0000 + 27.640 111.88 0.18800 0.10000E-01 5.0000 + 27.640 114.35 0.16600 0.60000E-02 5.0000 + 27.640 116.81 0.15600 0.60000E-02 5.0000 + 27.640 119.27 0.13100 0.50000E-02 5.0000 + 27.640 121.73 0.11450 0.50000E-01 5.0000 + 27.640 124.19 0.86200E-010.42000E-02 5.0000 + 27.640 126.64 0.78400E-010.49000E-02 5.0000 + 27.640 129.09 0.60600E-010.38000E-02 5.0000 + 27.640 131.53 0.55050E-010.36000E-02 5.0000 + 27.640 133.97 0.47800E-010.34000E-02 5.0000 + 27.640 136.41 0.45900E-010.41000E-02 5.0000 + 27.640 138.85 0.43500E-010.32000E-02 5.0000 + 27.640 141.28 0.37300E-010.28000E-02 5.0000 + 27.640 143.72 0.36400E-010.22000E-02 5.0000 + 27.640 146.15 0.32000E-010.22000E-02 5.0000 + 27.640 148.57 0.30200E-010.36000E-02 5.0000 + 27.640 151.00 0.27000E-010.20000E-02 5.0000 + 27.640 153.42 0.22900E-010.21000E-02 5.0000 + 27.640 155.84 0.23600E-010.19000E-02 5.0000 + 27.640 158.26 0.23000E-010.17000E-02 5.0000 + 27.640 160.68 0.22100E-010.16000E-02 5.0000 + 27.640 163.10 0.29600E-010.19000E-02 5.0000 + 27.640 165.52 0.27200E-010.20000E-02 5.0000 + 27.640 167.93 0.26300E-010.20000E-02 5.0000 + 27.640 170.35 0.23600E-010.20000E-02 5.0000 + 27.640 172.76 0.17200E-010.16000E-02 5.0000 + 27.640 175.17 0.13000E-010.14000E-02 5.0000 + 27.640 177.58 0.10800E-010.12000E-02 5.0000 +ENDDATA 138 +ENDSUBENT 150 +SUBENT F0700006 20050621 20050831 F022 +BIB 3 3 +REACTION (50-SN-0(A,EL)50-SN-0,,DA) +SAMPLE 50Sn target : evaporated +STATUS (CURVE)Table 2 +ENDBIB 3 +NOCOMMON 0 0 +DATA 6 135 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 THICKNESS +MEV ADEG MB/SR MB/SR PER-CENT G/CM-SQ + 23.300 10.340 0.37800E+06 11000. 3.5000 0.14000E-02 + 23.300 12.920 0.16100E+06 4000.0 3.5000 0.14000E-02 + 23.300 15.500 79400. 1700.0 3.5000 0.14000E-02 + 23.300 18.080 41500. 800.00 3.5000 0.14000E-02 + 23.300 20.660 23900. 500.00 3.5000 0.14000E-02 + 23.300 23.240 15900. 300.00 3.5000 0.14000E-02 + 23.300 25.820 10900. 200.00 3.5000 0.14000E-02 + 23.300 28.390 7460.0 180.00 3.5000 0.14000E-02 + 23.300 30.970 5880.0 120.00 3.5000 0.14000E-02 + 23.300 33.540 4140.0 60.000 3.5000 0.14000E-02 + 23.300 36.110 3040.0 40.000 3.5000 0.14000E-02 + 23.300 38.680 2170.0 40.000 3.5000 0.14000E-02 + 23.300 41.240 1540.0 20.000 3.5000 0.14000E-02 + 23.300 43.810 1045.0 14.000 3.5000 0.14000E-02 + 23.300 46.370 753.00 11.000 3.5000 0.14000E-02 + 23.300 48.930 529.00 9.0000 3.5000 0.14000E-02 + 23.300 51.480 393.00 8.0000 3.5000 0.14000E-02 + 23.300 54.030 279.00 6.0000 3.5000 0.14000E-02 + 23.300 56.580 192.00 2.0000 3.5000 0.14000E-02 + 23.300 59.130 144.00 2.0000 3.5000 0.14000E-02 + 23.300 61.670 103.00 2.0000 3.5000 0.14000E-02 + 23.300 64.210 79.300 0.60000 3.5000 0.14000E-02 + 23.300 66.750 59.500 0.60000 3.5000 0.14000E-02 + 23.300 69.290 47.400 0.40000 3.5000 0.14000E-02 + 23.300 71.820 36.500 0.30000 3.5000 0.14000E-02 + 23.300 74.340 27.900 0.30000 3.5000 0.14000E-02 + 23.300 76.870 22.200 0.30000 3.5000 0.14000E-02 + 23.300 79.390 16.800 0.20000 3.5000 0.14000E-02 + 23.300 81.900 13.800 0.20000 3.5000 0.14000E-02 + 23.300 84.420 12.700 0.20000 3.5000 0.14000E-02 + 23.300 86.930 8.9400 0.12000 3.5000 0.14000E-02 + 23.300 89.430 7.3200 0.12000 3.5000 0.14000E-02 + 23.300 91.930 5.4500 0.90000E-01 3.5000 0.14000E-02 + 23.300 94.430 4.7400 0.10000 3.5000 0.14000E-02 + 23.300 96.930 3.5700 0.70000E-01 3.5000 0.14000E-02 + 23.300 99.420 3.1800 0.80000E-01 3.5000 0.14000E-02 + 23.300 101.90 2.5600 0.60000E-01 3.5000 0.14000E-02 + 23.300 104.39 2.1900 0.50000E-01 3.5000 0.14000E-02 + 23.300 106.87 1.8100 0.40000E-01 3.5000 0.14000E-02 + 23.300 109.34 1.6100 0.40000E-01 3.5000 0.14000E-02 + 23.300 111.83 1.2950 0.34000E-01 3.5000 0.14000E-02 + 23.300 114.29 1.1300 0.40000E-01 3.5000 0.14000E-02 + 23.300 116.75 0.96000 0.32000E-01 3.5000 0.14000E-02 + 23.300 119.21 0.78300 0.20000E-01 3.5000 0.14000E-02 + 23.300 121.67 0.67800 0.20000E-01 3.5000 0.14000E-02 + 23.300 124.13 0.60200 0.18000E-01 3.5000 0.14000E-02 + 23.300 126.58 0.54500 0.17000E-01 3.5000 0.14000E-02 + 23.300 129.03 0.46100 0.16000E-01 3.5000 0.14000E-02 + 23.300 131.48 0.42200 0.15000E-01 3.5000 0.14000E-02 + 23.300 133.93 0.39000 0.14000E-01 3.5000 0.14000E-02 + 23.300 136.37 0.34100 0.14000E-01 3.5000 0.14000E-02 + 23.300 138.81 0.29400 0.29000E-01 3.5000 0.14000E-02 + 23.300 141.24 0.27500 0.12000E-01 3.5000 0.14000E-02 + 23.300 143.68 0.24600 0.12000E-01 3.5000 0.14000E-02 + 23.300 146.11 0.23100 0.12000E-01 3.5000 0.14000E-02 + 23.300 148.54 0.20800 0.80000E-02 3.5000 0.14000E-02 + 23.300 150.97 0.21300 0.11000E-01 3.5000 0.14000E-02 + 23.300 153.39 0.19800 0.16000E-01 3.5000 0.14000E-02 + 23.300 155.82 0.21500 0.70000E-02 3.5000 0.14000E-02 + 23.300 158.24 0.23100 0.10000E-01 3.5000 0.14000E-02 + 23.300 160.06 0.20000 0.80000E-02 3.5000 0.14000E-02 + 23.300 163.03 0.19000 0.80000E-02 3.5000 0.14000E-02 + 23.300 165.50 0.17700 0.90000E-02 3.5000 0.14000E-02 + 23.300 167.92 0.17400 0.70000E-02 3.5000 0.14000E-02 + 23.300 170.34 0.13300 0.60000E-02 3.5000 0.14000E-02 + 23.300 172.75 0.13800 0.12000E-01 3.5000 0.14000E-02 + 23.300 175.17 0.12700 0.64000E-01 3.5000 0.14000E-02 + 27.700 10.340 0.26500E+06 11000. 5.0000 0.90000E-03 + 27.700 12.920 0.10050E+06 3800.0 5.0000 0.90000E-03 + 27.700 15.500 49600. 1300.0 5.0000 0.90000E-03 + 27.700 18.080 28600. 700.00 5.0000 0.90000E-03 + 27.700 20.660 18800. 300.00 5.0000 0.90000E-03 + 27.700 23.240 12000. 200.00 5.0000 0.90000E-03 + 27.700 25.820 8180.0 110.00 5.0000 0.90000E-03 + 27.700 28.390 5010.0 90.000 5.0000 0.90000E-03 + 27.700 30.970 3140.0 50.000 5.0000 0.90000E-03 + 27.700 33.540 2090.0 40.000 5.0000 0.90000E-03 + 27.700 36.110 1360.0 20.000 5.0000 0.90000E-03 + 27.700 38.680 880.00 22.000 5.0000 0.90000E-03 + 27.700 41.240 536.00 11.000 5.0000 0.90000E-03 + 27.700 43.810 350.00 4.0000 5.0000 0.90000E-03 + 27.700 46.370 252.00 4.0000 5.0000 0.90000E-03 + 27.700 48.930 169.00 2.0000 5.0000 0.90000E-03 + 27.700 51.480 112.00 1.0000 5.0000 0.90000E-03 + 27.700 54.030 75.900 1.3000 5.0000 0.90000E-03 + 27.700 56.580 58.200 0.40000 5.0000 0.90000E-03 + 27.700 59.130 41.800 0.80000 5.0000 0.90000E-03 + 27.700 61.670 29.600 0.30000 5.0000 0.90000E-03 + 27.700 64.210 20.600 0.40000 5.0000 0.90000E-03 + 27.700 66.750 15.200 0.10000 5.0000 0.90000E-03 + 27.700 69.290 12.450 0.30000 5.0000 0.90000E-03 + 27.700 71.820 9.4100 0.90000E-01 5.0000 0.90000E-03 + 27.700 74.340 6.9600 0.10000 5.0000 0.90000E-03 + 27.700 76.870 4.7250 0.71000E-01 5.0000 0.90000E-03 + 27.700 79.390 3.7300 0.80000E-01 5.0000 0.90000E-03 + 27.700 81.900 3.1200 0.40000E-01 5.0000 0.90000E-03 + 27.700 84.420 2.6900 0.70000E-01 5.0000 0.90000E-03 + 27.700 86.930 2.0800 0.30000E-01 5.0000 0.90000E-03 + 27.700 89.430 1.4600 0.30000E-01 5.0000 0.90000E-03 + 27.700 91.930 1.0800 0.20000E-01 5.0000 0.90000E-03 + 27.700 94.430 0.84150 0.19000E-01 5.0000 0.90000E-03 + 27.700 96.930 0.71800 0.18000E-01 5.0000 0.90000E-03 + 27.700 99.420 0.69000 0.17000E-01 5.0000 0.90000E-03 + 27.700 101.90 0.56200 0.16000E-01 5.0000 0.90000E-03 + 27.700 104.39 0.40500 0.13000E-01 5.0000 0.90000E-03 + 27.700 106.87 0.29900 0.12000E-01 5.0000 0.90000E-03 + 27.700 109.34 0.25100 0.11000E-01 5.0000 0.90000E-03 + 27.700 111.83 0.19750 0.95000E-02 5.0000 0.90000E-03 + 27.700 114.29 0.19850 0.95000E-02 5.0000 0.90000E-03 + 27.700 116.75 0.18400 0.90000E-02 5.0000 0.90000E-03 + 27.700 119.21 0.15400 0.80000E-02 5.0000 0.90000E-03 + 27.700 121.67 0.12750 0.76000E-02 5.0000 0.90000E-03 + 27.700 124.13 0.11200 0.70000E-02 5.0000 0.90000E-03 + 27.700 126.58 0.83900E-010.38000E-02 5.0000 0.90000E-03 + 27.700 129.03 0.74200E-010.58000E-02 5.0000 0.90000E-03 + 27.700 131.48 0.59900E-010.32000E-02 5.0000 0.90000E-03 + 27.700 133.93 0.58600E-010.42000E-02 5.0000 0.90000E-03 + 27.700 136.37 0.57300E-010.32000E-02 5.0000 0.90000E-03 + 27.700 138.81 0.58900E-010.43000E-02 5.0000 0.90000E-03 + 27.700 141.24 0.44000E-010.32000E-02 5.0000 0.90000E-03 + 27.700 143.68 0.38400E-010.21000E-02 5.0000 0.90000E-03 + 27.700 146.11 0.28100E-010.15000E-02 5.0000 0.90000E-03 + 27.700 148.54 0.27500E-010.18000E-02 5.0000 0.90000E-03 + 27.700 150.97 0.22700E-010.11000E-02 5.0000 0.90000E-03 + 27.700 153.39 0.21000E-010.80000E-03 5.0000 0.90000E-03 + 27.700 155.82 0.22000E-010.80000E-03 5.0000 0.90000E-03 + 27.700 158.24 0.27100E-010.80000E-03 5.0000 0.90000E-03 + 27.700 160.06 0.31200E-010.14000E-02 5.0000 0.90000E-03 + 27.700 163.03 0.32300E-010.14000E-02 5.0000 0.90000E-03 + 27.700 165.50 0.33000E-010.10000E-02 5.0000 0.90000E-03 + 27.700 167.92 0.29550E-010.65000E-03 5.0000 0.90000E-03 + 27.700 170.34 0.19900E-010.50000E-03 5.0000 0.90000E-03 + 27.700 172.75 0.12600E-010.60000E-03 5.0000 0.90000E-03 + 27.700 175.17 0.88200E-020.55000E-03 5.0000 0.90000E-03 + 27.700 177.08 0.56700E-020.67000E-03 5.0000 0.90000E-03 +ENDDATA 137 +ENDSUBENT 145 +SUBENT F0700007 20050621 20050831 F022 +BIB 3 3 +REACTION (73-TA-0(A,EL)73-TA-0,,DA) +SAMPLE 73Ta target : rolled +STATUS (CURVE)Table 2 +ENDBIB 3 +COMMON 1 3 +THICKNESS +G/CM-SQ + 0.0067 +ENDCOMMON 3 +DATA 5 134 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 +MEV ADEG MB/SR MB/SR PER-CENT + 23.500 10.220 0.83600E+06 29000. 1.7000 + 23.500 12.770 0.35600E+06 11000. 1.7000 + 23.500 15.330 0.16100E+06 39000. 1.7000 + 23.500 17.880 91000. 1900.0 1.7000 + 23.500 20.430 51700. 1100.0 1.7000 + 23.500 22.990 33600. 700.00 1.7000 + 23.500 25.540 22100. 400.00 1.7000 + 23.500 28.090 15400. 200.00 1.7000 + 23.500 30.630 10900. 100.00 1.7000 + 23.500 33.180 7900.0 80.000 1.7000 + 23.500 35.730 5860.0 60.000 1.7000 + 23.500 38.270 4450.0 50.000 1.7000 + 23.500 40.820 3420.0 40.000 1.7000 + 23.500 43.360 2710.0 30.000 1.7000 + 23.500 45.900 2280.0 30.000 1.7000 + 23.500 48.740 1910.0 20.000 1.7000 + 23.500 50.970 1620.0 20.000 1.7000 + 23.500 53.510 1360.0 20.000 1.7000 + 23.500 56.040 1160.0 10.000 1.7000 + 23.500 58.570 974.00 26.000 1.7000 + 23.500 61.100 837.00 10.000 1.7000 + 23.500 63.630 690.00 19.000 1.7000 + 23.500 66.150 574.00 9.0000 1.7000 + 23.500 68.670 485.00 16.000 1.7000 + 23.500 71.190 434.00 4.0000 1.7000 + 23.500 73.710 369.00 4.0000 1.7000 + 23.500 76.230 308.00 3.0000 1.7000 + 23.500 78.740 262.00 3.0000 1.7000 + 23.500 81.250 213.00 2.0000 1.7000 + 23.500 83.760 182.00 2.0000 1.7000 + 23.500 86.260 156.00 2.0000 1.7000 + 23.500 88.770 131.00 2.0000 1.7000 + 23.500 91.270 112.00 2.0000 1.7000 + 23.500 93.770 95.500 1.4000 1.7000 + 23.500 96.260 80.200 1.5000 1.7000 + 23.500 98.760 68.100 1.2000 1.7000 + 23.500 101.25 57.000 1.0000 1.7000 + 23.500 103.74 48.700 0.80000 1.7000 + 23.500 106.22 43.100 0.80000 1.7000 + 23.500 108.71 37.100 0.70000 1.7000 + 23.500 111.19 33.200 0.70000 1.7000 + 23.500 113.67 28.400 0.60000 1.7000 + 23.500 116.15 24.700 1.1000 1.7000 + 23.500 118.63 20.900 0.40000 1.7000 + 23.500 121.10 18.300 0.50000 1.7000 + 23.500 123.57 16.400 0.80000 1.7000 + 23.500 126.04 13.600 0.50000 1.7000 + 23.500 128.51 13.000 0.60000 1.7000 + 23.500 130.97 11.400 0.50000 1.7000 + 23.500 133.44 10.600 0.50000 1.7000 + 23.500 135.90 9.4200 0.45000 1.7000 + 23.500 138.36 9.0400 0.40000 1.7000 + 23.500 140.82 8.1700 0.38000 1.7000 + 23.500 143.27 7.4400 0.34000 1.7000 + 23.500 145.72 6.4800 0.31000 1.7000 + 23.500 148.18 5.9600 0.28000 1.7000 + 23.500 150.63 6.0700 0.32000 1.7000 + 23.500 153.09 5.1800 0.28000 1.7000 + 23.500 155.54 4.7900 0.23000 1.7000 + 23.500 157.99 4.8100 0.21000 1.7000 + 23.500 160.43 4.3400 0.21000 1.7000 + 23.500 162.88 3.5700 0.18000 1.7000 + 23.500 165.33 3.7500 0.19000 1.7000 + 23.500 167.77 3.4700 0.12000 1.7000 + 23.500 170.22 3.5500 0.15000 1.7000 + 23.500 172.67 3.4500 0.16000 1.7000 + 23.500 175.11 3.1200 0.12000 1.7000 + 27.200 10.220 0.57200E+06 19000. 2.2000 + 27.200 12.770 0.24900E+06 7000.0 2.2000 + 27.200 15.330 0.11900E+06 3000.0 2.2000 + 27.200 17.880 67700. 1200.0 2.2000 + 27.200 20.430 40200. 700.00 2.2000 + 27.200 22.990 25900. 600.00 2.2000 + 27.200 25.540 16200. 400.00 2.2000 + 27.200 28.090 11200. 200.00 2.2000 + 27.200 30.630 8020.0 160.00 2.2000 + 27.200 33.180 6340.0 120.00 2.2000 + 27.200 35.730 4940.0 70.000 2.2000 + 27.200 38.270 4010.0 30.000 2.2000 + 27.200 40.820 3050.0 30.000 2.2000 + 27.200 43.360 2450.0 50.000 2.2000 + 27.200 45.900 1830.0 20.000 2.2000 + 27.200 48.740 1480.0 20.000 2.2000 + 27.200 50.970 1070.0 30.000 2.2000 + 27.200 53.510 846.00 9.0000 2.2000 + 27.200 56.040 649.00 15.000 2.2000 + 27.200 58.570 500.00 16.000 2.2000 + 27.200 61.100 370.00 3.0000 2.2000 + 27.200 63.630 302.00 2.0000 2.2000 + 27.200 66.150 234.00 2.0000 2.2000 + 27.200 68.670 180.00 4.0000 2.2000 + 27.200 71.190 140.00 3.0000 2.2000 + 27.200 73.710 107.00 3.0000 2.2000 + 27.200 76.230 82.800 2.1000 2.2000 + 27.200 78.740 65.300 2.2000 2.2000 + 27.200 81.250 49.900 1.3000 2.2000 + 27.200 83.760 39.700 0.80000 2.2000 + 27.200 86.260 30.100 1.2000 2.2000 + 27.200 88.770 25.800 0.50000 2.2000 + 27.200 91.270 20.300 0.30000 2.2000 + 27.200 93.770 16.800 0.40000 2.2000 + 27.200 96.260 13.500 0.20000 2.2000 + 27.200 98.760 11.200 0.20000 2.2000 + 27.200 101.25 9.4200 0.24000 2.2000 + 27.200 103.74 7.5300 0.17000 2.2000 + 27.200 106.22 5.9400 0.12000 2.2000 + 27.200 108.71 5.1300 0.12000 2.2000 + 27.200 111.19 4.4100 0.13000 2.2000 + 27.200 113.67 3.5000 0.40000E-01 2.2000 + 27.200 116.15 3.1600 0.90000E-01 2.2000 + 27.200 118.63 2.7300 0.11000 2.2000 + 27.200 121.10 2.4300 0.70000E-01 2.2000 + 27.200 123.57 1.8500 0.50000E-01 2.2000 + 27.200 126.04 1.7200 0.70000E-01 2.2000 + 27.200 128.51 1.4400 0.50000E-01 2.2000 + 27.200 130.97 1.2600 0.30000E-01 2.2000 + 27.200 133.44 1.1400 0.20000E-01 2.2000 + 27.200 135.90 1.0600 0.20000E-01 2.2000 + 27.200 138.36 0.89700 0.28000E-01 2.2000 + 27.200 140.82 0.84300 0.20000E-01 2.2000 + 27.200 143.27 0.77000 0.18000E-01 2.2000 + 27.200 145.72 0.71500 0.19000E-01 2.2000 + 27.200 148.18 0.66200 0.26000E-01 2.2000 + 27.200 150.63 0.59200 0.18000E-01 2.2000 + 27.200 153.09 0.55400 0.33000E-01 2.2000 + 27.200 155.54 0.50000 0.10000E-01 2.2000 + 27.200 157.99 0.49500 0.11000E-01 2.2000 + 27.200 160.43 0.49600 0.17000E-01 2.2000 + 27.200 162.88 0.46300 0.10000E-01 2.2000 + 27.200 165.33 0.45300 0.11000E-01 2.2000 + 27.200 167.77 0.44200 0.80000E-02 2.2000 + 27.200 170.22 0.42500 0.90000E-02 2.2000 + 27.200 172.67 0.40100 0.16000E-01 2.2000 + 27.200 175.11 0.39300 0.14000E-01 2.2000 +ENDDATA 136 +ENDSUBENT 148 +SUBENT F0700008 20050621 20050831 F022 +BIB 3 3 +REACTION (78-PT-0(A,EL)78-PT-0,,DA) +SAMPLE 78Pt target : rolled +STATUS (CURVE)Table 2 +ENDBIB 3 +COMMON 1 3 +THICKNESS +G/CM-SQ + 0.0045 +ENDCOMMON 3 +DATA 5 134 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 +MEV ADEG MB/SR MB/SR PER-CENT + 23.350 10.200 0.96500E+06 39000. 1.6000 + 23.350 12.750 0.40300E+06 13000. 1.6000 + 23.350 15.300 0.18800E+06 7000.0 1.6000 + 23.350 17.850 0.10400E+06 3000.0 1.6000 + 23.350 20.400 60000. 2100.0 1.6000 + 23.350 22.900 39400. 1100.0 1.6000 + 23.350 25.500 25200. 300.00 1.6000 + 23.350 28.040 17800. 300.00 1.6000 + 23.350 30.590 12300. 200.00 1.6000 + 23.350 33.130 9130.0 130.00 1.6000 + 23.350 35.670 6870.0 70.000 1.6000 + 23.350 38.220 5300.0 70.000 1.6000 + 23.350 40.760 4080.0 50.000 1.6000 + 23.350 43.290 3160.0 30.000 1.6000 + 23.350 45.830 2610.0 30.000 1.6000 + 23.350 48.370 2170.0 30.000 1.6000 + 23.350 50.960 1830.0 20.000 1.6000 + 23.350 53.430 1530.0 40.000 1.6000 + 23.350 55.960 1370.0 50.000 1.6000 + 23.350 58.490 1170.0 10.000 1.6000 + 23.350 61.020 1010.0 10.000 1.6000 + 23.350 63.540 874.00 9.0000 1.6000 + 23.350 66.070 751.00 8.0000 1.6000 + 23.350 68.590 646.00 7.0000 1.6000 + 23.350 71.100 567.00 5.0000 1.6000 + 23.350 73.620 459.00 7.0000 1.6000 + 23.350 76.140 416.00 5.0000 1.6000 + 23.350 78.650 363.00 4.0000 1.6000 + 23.350 81.160 310.00 4.0000 1.6000 + 23.350 83.670 259.00 3.0000 1.6000 + 23.350 86.170 222.00 3.0000 1.6000 + 23.350 88.670 191.00 3.0000 1.6000 + 23.350 91.180 167.00 2.0000 1.6000 + 23.350 93.670 146.00 2.0000 1.6000 + 23.350 96.170 123.00 2.0000 1.6000 + 23.350 98.670 106.00 1.0000 1.6000 + 23.350 101.16 91.600 0.10000 1.6000 + 23.350 103.65 79.100 0.10000 1.6000 + 23.350 106.14 66.800 0.90000 1.6000 + 23.350 108.62 59.900 0.70000 1.6000 + 23.350 111.10 51.200 0.70000 1.6000 + 23.350 113.59 46.000 0.60000 1.6000 + 23.350 116.07 39.300 0.60000 1.6000 + 23.350 118.54 35.200 0.60000 1.6000 + 23.350 121.02 30.900 0.50000 1.6000 + 23.350 123.49 27.400 0.40000 1.6000 + 23.350 125.96 24.100 0.50000 1.6000 + 23.350 128.43 23.100 0.40000 1.6000 + 23.350 130.90 20.100 0.40000 1.6000 + 23.350 133.37 18.200 0.30000 1.6000 + 23.350 135.81 16.500 0.30000 1.6000 + 23.350 138.29 14.900 0.30000 1.6000 + 23.350 140.76 13.400 0.30000 1.6000 + 23.350 143.22 13.000 0.30000 1.6000 + 23.350 145.67 12.100 0.30000 1.6000 + 23.350 148.13 11.500 0.20000 1.6000 + 23.350 150.59 10.300 0.20000 1.6000 + 23.350 153.04 9.9300 0.40000 1.6000 + 23.350 155.50 9.3800 0.24000 1.6000 + 23.350 157.95 8.9800 0.22000 1.6000 + 23.350 160.40 8.6600 0.23000 1.6000 + 23.350 162.85 8.4000 0.50000 1.6000 + 23.350 165.30 8.1500 0.21000 1.6000 + 23.350 167.75 8.0200 0.32000 1.6000 + 23.350 170.20 7.7600 0.27000 1.6000 + 23.350 172.65 7.5800 0.30000 1.6000 + 23.350 175.10 7.5300 0.26000 1.6000 + 27.700 10.200 0.69500E+06 51000. 1.8000 + 27.700 12.750 0.28600E+06 22000. 1.8000 + 27.700 15.300 0.13800E+06 11000. 1.8000 + 27.700 17.850 71900. 5600.0 1.8000 + 27.700 20.400 44400. 3600.0 1.8000 + 27.700 22.950 27100. 2300.0 1.8000 + 27.700 25.500 17500. 300.00 1.8000 + 27.700 28.040 11800. 200.00 1.8000 + 27.700 30.590 8100.0 180.00 1.8000 + 27.700 33.130 5920.0 140.00 1.8000 + 27.700 35.670 4730.0 110.00 1.8000 + 27.700 38.220 3820.0 100.00 1.8000 + 27.700 40.760 3060.0 40.000 1.8000 + 27.700 43.290 2610.0 70.000 1.8000 + 27.700 45.830 2050.0 20.000 1.8000 + 27.700 48.370 1660.0 40.000 1.8000 + 27.700 50.960 1290.0 10.000 1.8000 + 27.700 53.430 1040.0 20.000 1.8000 + 27.700 55.960 760.00 10.000 1.8000 + 27.700 58.490 614.00 8.0000 1.8000 + 27.700 61.020 461.00 5.0000 1.8000 + 27.700 63.540 364.00 5.0000 1.8000 + 27.700 66.070 270.00 5.0000 1.8000 + 27.700 68.590 203.00 6.0000 1.8000 + 27.700 71.100 169.00 2.0000 1.8000 + 27.700 73.620 133.00 4.0000 1.8000 + 27.700 76.140 105.00 2.0000 1.8000 + 27.700 78.650 81.700 3.3000 1.8000 + 27.700 81.160 64.900 0.70000 1.8000 + 27.700 83.670 51.500 1.2000 1.8000 + 27.700 86.170 40.800 1.4000 1.8000 + 27.700 88.670 34.200 0.80000 1.8000 + 27.700 91.180 26.900 0.40000 1.8000 + 27.700 93.670 22.100 0.30000 1.8000 + 27.700 96.170 18.300 0.30000 1.8000 + 27.700 98.670 15.100 0.30000 1.8000 + 27.700 101.16 12.300 0.50000 1.8000 + 27.700 103.65 10.400 0.20000 1.8000 + 27.700 106.14 8.8200 0.16000 1.8000 + 27.700 108.62 7.2300 0.33000 1.8000 + 27.700 111.10 6.3600 0.10000 1.8000 + 27.700 113.59 5.3700 0.17000 1.8000 + 27.700 116.07 4.0300 0.80000E-01 1.8000 + 27.700 118.54 3.6300 0.60000E-01 1.8000 + 27.700 121.02 3.0600 0.70000E-01 1.8000 + 27.700 123.49 2.7500 0.70000E-01 1.8000 + 27.700 125.96 2.4000 0.60000E-01 1.8000 + 27.700 128.43 2.0900 0.70000E-01 1.8000 + 27.700 130.90 1.8700 0.50000E-01 1.8000 + 27.700 133.37 1.5500 0.40000E-01 1.8000 + 27.700 135.81 1.3900 0.40000E-01 1.8000 + 27.700 138.29 1.3000 0.40000E-01 1.8000 + 27.700 140.76 1.2000 0.60000E-01 1.8000 + 27.700 143.22 1.1200 0.50000E-01 1.8000 + 27.700 145.67 0.95600 0.32000E-01 1.8000 + 27.700 148.13 0.87800 0.25000E-01 1.8000 + 27.700 150.59 0.82400 0.25000E-01 1.8000 + 27.700 153.04 0.78300 0.23000E-01 1.8000 + 27.700 155.50 0.70500 0.23000E-01 1.8000 + 27.700 157.95 0.66100 0.21000E-01 1.8000 + 27.700 160.40 0.65900 0.57000E-01 1.8000 + 27.700 162.85 0.62400 0.30000E-01 1.8000 + 27.700 165.30 0.61400 0.35000E-01 1.8000 + 27.700 167.75 0.59900 0.29000E-01 1.8000 + 27.700 170.20 0.58700 0.28000E-01 1.8000 + 27.700 172.65 0.61400 0.30000E-01 1.8000 + 27.700 175.10 0.58900 0.37000E-01 1.8000 +ENDDATA 136 +ENDSUBENT 148 +SUBENT F0700009 20050621 20050831 F022 +BIB 3 3 +REACTION (79-AU-197(A,EL)79-AU-197,,DA) +SAMPLE Au target : evaporated +STATUS (CURVE)Table 2 +ENDBIB 3 +NOCOMMON 0 0 +DATA 6 121 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 THICKNESS +MEV ADEG MB/SR MB/SR PER-CENT G/CM-SQ + 23.650 10.200 0.92200E+06 41000. 2.5000 0.90000E-03 + 23.650 12.750 0.39600E+06 14000. 2.5000 0.90000E-03 + 23.650 15.300 0.19800E+06 15000. 2.5000 0.90000E-03 + 23.650 17.850 0.10700E+06 1000.0 2.5000 0.90000E-03 + 23.650 20.400 59300. 600.00 2.5000 0.90000E-03 + 23.650 22.950 39600. 500.00 2.5000 0.90000E-03 + 23.650 25.490 25800. 200.00 2.5000 0.90000E-03 + 23.650 28.040 17200. 100.00 2.5000 0.90000E-03 + 23.650 30.580 12300. 100.00 2.5000 0.90000E-03 + 23.650 33.130 8960.0 30.000 2.5000 0.90000E-03 + 23.650 35.670 7060.0 30.000 2.5000 0.90000E-03 + 23.650 38.210 5110.0 20.000 2.5000 0.90000E-03 + 23.650 40.750 4380.0 30.000 2.5000 0.90000E-03 + 23.650 43.290 3200.0 10.000 2.5000 0.90000E-03 + 23.650 45.820 2770.0 100.00 2.5000 0.90000E-03 + 23.650 48.360 2140.0 10.000 2.5000 0.90000E-03 + 23.650 50.890 1900.0 10.000 2.5000 0.90000E-03 + 23.650 53.420 1550.0 10.000 2.5000 0.90000E-03 + 23.650 55.950 1380.0 10.000 2.5000 0.90000E-03 + 23.650 61.010 1050.0 10.000 2.5000 0.90000E-03 + 23.650 66.050 792.00 2.0000 2.5000 0.90000E-03 + 23.650 71.090 592.00 2.0000 2.5000 0.90000E-03 + 23.650 76.120 440.00 2.0000 2.5000 0.90000E-03 + 23.650 81.150 323.00 1.0000 2.5000 0.90000E-03 + 23.650 86.160 237.00 1.0000 2.5000 0.90000E-03 + 23.650 91.160 174.00 1.0000 2.5000 0.90000E-03 + 23.650 96.160 125.00 1.0000 2.5000 0.90000E-03 + 23.650 101.15 92.600 0.10000 2.5000 0.90000E-03 + 23.650 106.12 70.200 0.30000 2.5000 0.90000E-03 + 23.650 111.09 52.800 0.30000 2.5000 0.90000E-03 + 23.650 116.05 41.300 0.40000 2.5000 0.90000E-03 + 23.650 121.01 33.700 0.40000 2.5000 0.90000E-03 + 23.650 123.48 29.300 0.30000 2.5000 0.90000E-03 + 23.650 125.95 26.000 0.30000 2.5000 0.90000E-03 + 23.650 128.42 23.300 0.60000 2.5000 0.90000E-03 + 23.650 130.89 20.700 0.40000 2.5000 0.90000E-03 + 23.650 133.36 19.000 0.60000 2.5000 0.90000E-03 + 23.650 135.82 17.700 0.30000 2.5000 0.90000E-03 + 23.650 138.29 16.400 0.20000 2.5000 0.90000E-03 + 23.650 140.75 15.100 0.20000 2.5000 0.90000E-03 + 23.650 143.21 14.000 0.20000 2.5000 0.90000E-03 + 23.650 145.67 13.000 0.20000 2.5000 0.90000E-03 + 23.650 148.13 11.700 0.20000 2.5000 0.90000E-03 + 23.650 150.58 11.200 0.20000 2.5000 0.90000E-03 + 23.650 153.04 10.100 0.10000 2.5000 0.90000E-03 + 23.650 155.49 9.4900 0.16000 2.5000 0.90000E-03 + 23.650 157.95 9.1500 0.13000 2.5000 0.90000E-03 + 23.650 160.40 9.0600 0.16000 2.5000 0.90000E-03 + 23.650 162.85 8.4900 0.10000 2.5000 0.90000E-03 + 23.650 165.30 8.0600 0.10000 2.5000 0.90000E-03 + 23.650 167.75 8.0000 0.13000 2.5000 0.90000E-03 + 23.650 170.20 7.8700 0.11000 2.5000 0.90000E-03 + 23.650 172.65 8.0000 0.13000 2.5000 0.90000E-03 + 23.650 175.10 7.2000 0.12000 2.5000 0.90000E-03 + 27.950 10.200 0.65100E+06 16000. 2.0000 0.21000E-02 + 27.950 12.750 0.27800E+06 7000.0 2.0000 0.21000E-02 + 27.950 15.300 0.13700E+06 4000.0 2.0000 0.21000E-02 + 27.950 17.850 76400. 2800.0 2.0000 0.21000E-02 + 27.950 20.400 44900. 1600.0 2.0000 0.21000E-02 + 27.950 22.950 29200. 1200.0 2.0000 0.21000E-02 + 27.950 25.490 19100. 1100.0 2.0000 0.21000E-02 + 27.950 28.040 13000. 900.00 2.0000 0.21000E-02 + 27.950 30.580 8990.0 720.00 2.0000 0.21000E-02 + 27.950 33.130 6670.0 10.000 2.0000 0.21000E-02 + 27.950 35.670 5190.0 60.000 2.0000 0.21000E-02 + 27.950 38.210 4280.0 40.000 2.0000 0.21000E-02 + 27.950 40.750 3480.0 30.000 2.0000 0.21000E-02 + 27.950 43.290 2790.0 30.000 2.0000 0.21000E-02 + 27.950 45.820 2330.0 20.000 2.0000 0.21000E-02 + 27.950 48.360 1860.0 40.000 2.0000 0.21000E-02 + 27.950 50.890 1640.0 10.000 2.0000 0.21000E-02 + 27.950 53.420 1150.0 10.000 2.0000 0.21000E-02 + 27.950 55.950 934.00 6.0000 2.0000 0.21000E-02 + 27.950 58.480 721.00 5.0000 2.0000 0.21000E-02 + 27.950 61.010 570.00 5.0000 2.0000 0.21000E-02 + 27.950 63.530 426.00 4.0000 2.0000 0.21000E-02 + 27.950 66.050 322.00 6.0000 2.0000 0.21000E-02 + 27.950 68.580 246.00 3.0000 2.0000 0.21000E-02 + 27.950 71.090 185.00 5.0000 2.0000 0.21000E-02 + 27.950 73.610 149.00 4.0000 2.0000 0.21000E-02 + 27.950 76.120 111.00 4.0000 2.0000 0.21000E-02 + 27.950 78.640 83.900 3.3000 2.0000 0.21000E-02 + 27.950 81.150 65.700 2.0000 2.0000 0.21000E-02 + 27.950 83.650 53.700 1.9000 2.0000 0.21000E-02 + 27.950 86.160 39.400 1.6000 2.0000 0.21000E-02 + 27.950 88.660 31.900 1.4000 2.0000 0.21000E-02 + 27.950 91.160 26.600 1.3000 2.0000 0.21000E-02 + 27.950 93.660 21.000 1.2000 2.0000 0.21000E-02 + 27.950 96.160 17.700 0.30000 2.0000 0.21000E-02 + 27.950 98.650 14.300 0.40000 2.0000 0.21000E-02 + 27.950 101.15 11.700 0.30000 2.0000 0.21000E-02 + 27.950 103.64 10.200 0.50000 2.0000 0.21000E-02 + 27.950 106.12 7.2600 0.22000 2.0000 0.21000E-02 + 27.950 108.61 6.4200 0.29000 2.0000 0.21000E-02 + 27.950 111.09 5.0300 0.18000 2.0000 0.21000E-02 + 27.950 113.58 4.2600 0.36000 2.0000 0.21000E-02 + 27.950 116.05 3.7300 0.18000 2.0000 0.21000E-02 + 27.950 118.53 3.3600 0.31000 2.0000 0.21000E-02 + 27.950 121.01 3.0600 0.11000 2.0000 0.21000E-02 + 27.950 123.48 2.7900 0.14000 2.0000 0.21000E-02 + 27.950 125.95 2.4100 0.60000E-01 2.0000 0.21000E-02 + 27.950 128.42 2.1500 0.21000 2.0000 0.21000E-02 + 27.950 130.89 1.9600 0.80000E-01 2.0000 0.21000E-02 + 27.950 133.36 1.7900 0.11000 2.0000 0.21000E-02 + 27.950 135.82 1.5500 0.70000E-01 2.0000 0.21000E-02 + 27.950 138.29 1.5300 0.60000E-01 2.0000 0.21000E-02 + 27.950 140.75 1.3700 0.30000E-01 2.0000 0.21000E-02 + 27.950 143.21 1.3200 0.50000E-01 2.0000 0.21000E-02 + 27.950 145.67 1.2000 0.30000E-01 2.0000 0.21000E-02 + 27.950 148.13 1.0600 0.20000E-01 2.0000 0.21000E-02 + 27.950 150.58 0.96000 0.40000E-01 2.0000 0.21000E-02 + 27.950 153.04 0.93100 0.40000E-01 2.0000 0.21000E-02 + 27.950 155.49 0.81300 0.33000E-01 2.0000 0.21000E-02 + 27.950 157.95 0.77200 0.19000E-01 2.0000 0.21000E-02 + 27.950 160.40 0.77700 0.23000E-01 2.0000 0.21000E-02 + 27.950 162.85 0.72900 0.24000E-01 2.0000 0.21000E-02 + 27.950 165.30 0.70500 0.37000E-01 2.0000 0.21000E-02 + 27.950 167.75 0.70200 0.24000E-01 2.0000 0.21000E-02 + 27.950 170.20 0.66400 0.39000E-01 2.0000 0.21000E-02 + 27.950 172.65 0.64800 0.22000E-01 2.0000 0.21000E-02 + 27.950 175.10 0.61500 0.35000E-01 2.0000 0.21000E-02 +ENDDATA 123 +ENDSUBENT 131 +SUBENT F0700010 20050621 20050831 F022 +BIB 3 3 +REACTION (82-PB-208(A,EL)82-PB-208,,DA) +SAMPLE Pb target : evaporated +STATUS (CURVE)Table 2 +ENDBIB 3 +NOCOMMON 0 0 +DATA 6 134 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 THICKNESS +MEV ADEG MB/SR MB/SR PER-CENT G/CM-SQ + 23.600 10.190 0.10300E+07 50000. 1.5000 0.12000E-02 + 23.600 12.740 0.44800E+06 23000. 1.5000 0.12000E-02 + 23.600 15.290 0.20100E+06 9000.0 1.5000 0.12000E-02 + 23.600 17.830 0.11200E+06 4000.0 1.5000 0.12000E-02 + 23.600 20.380 74600. 3400.0 1.5000 0.12000E-02 + 23.600 22.920 42300. 1400.0 1.5000 0.12000E-02 + 23.600 25.470 27300. 600.00 1.5000 0.12000E-02 + 23.600 28.010 18700. 500.00 1.5000 0.12000E-02 + 23.600 30.550 13400. 300.00 1.5000 0.12000E-02 + 23.600 33.100 9930.0 210.00 1.5000 0.12000E-02 + 23.600 35.640 7450.0 160.00 1.5000 0.12000E-02 + 23.600 38.170 5930.0 110.00 1.5000 0.12000E-02 + 23.600 40.710 4540.0 80.000 1.5000 0.12000E-02 + 23.600 43.250 3510.0 70.000 1.5000 0.12000E-02 + 23.600 45.780 2790.0 70.000 1.5000 0.12000E-02 + 23.600 48.320 2320.0 40.000 1.5000 0.12000E-02 + 23.600 50.850 1900.0 40.000 1.5000 0.12000E-02 + 23.600 53.380 1630.0 30.000 1.5000 0.12000E-02 + 23.600 55.910 1400.0 40.000 1.5000 0.12000E-02 + 23.600 58.430 1230.0 20.000 1.5000 0.12000E-02 + 23.600 60.600 1070.0 30.000 1.5000 0.12000E-02 + 23.600 63.480 943.00 20.000 1.5000 0.12000E-02 + 23.600 66.000 841.00 13.000 1.5000 0.12000E-02 + 23.600 68.520 720.00 13.000 1.5000 0.12000E-02 + 23.600 71.040 617.00 23.000 1.5000 0.12000E-02 + 23.600 73.560 533.00 9.0000 1.5000 0.12000E-02 + 23.600 76.070 462.00 25.000 1.5000 0.12000E-02 + 23.600 78.580 391.00 10.000 1.5000 0.12000E-02 + 23.600 81.090 343.00 10.000 1.5000 0.12000E-02 + 23.600 83.600 296.00 8.0000 1.5000 0.12000E-02 + 23.600 86.100 253.00 6.0000 1.5000 0.12000E-02 + 23.600 88.610 219.00 5.0000 1.5000 0.12000E-02 + 23.600 91.110 182.00 5.0000 1.5000 0.12000E-02 + 23.600 93.610 159.00 2.0000 1.5000 0.12000E-02 + 23.600 96.100 136.00 2.0000 1.5000 0.12000E-02 + 23.600 98.600 118.00 1.0000 1.5000 0.12000E-02 + 23.600 101.09 106.00 3.0000 1.5000 0.12000E-02 + 23.600 103.58 89.100 1.3000 1.5000 0.12000E-02 + 23.600 106.07 80.000 3.0000 1.5000 0.12000E-02 + 23.600 108.56 69.500 1.0000 1.5000 0.12000E-02 + 23.600 111.04 61.700 1.9000 1.5000 0.12000E-02 + 23.600 113.52 52.000 1.1000 1.5000 0.12000E-02 + 23.600 116.00 45.600 3.2000 1.5000 0.12000E-02 + 23.600 118.42 39.000 0.60000 1.5000 0.12000E-02 + 23.600 120.96 33.200 0.50000 1.5000 0.12000E-02 + 23.600 123.43 30.900 0.60000 1.5000 0.12000E-02 + 23.600 125.91 28.400 1.0000 1.5000 0.12000E-02 + 23.600 128.38 24.400 0.40000 1.5000 0.12000E-02 + 23.600 130.85 21.000 0.30000 1.5000 0.12000E-02 + 23.600 133.32 19.500 0.30000 1.5000 0.12000E-02 + 23.600 135.78 17.900 0.30000 1.5000 0.12000E-02 + 23.600 138.25 15.900 0.30000 1.5000 0.12000E-02 + 23.600 140.71 15.000 0.30000 1.5000 0.12000E-02 + 23.600 143.17 13.100 0.30000 1.5000 0.12000E-02 + 23.600 145.64 12.300 0.60000 1.5000 0.12000E-02 + 23.600 148.10 11.200 0.30000 1.5000 0.12000E-02 + 23.600 150.55 11.000 0.30000 1.5000 0.12000E-02 + 23.600 153.01 10.400 0.20000 1.5000 0.12000E-02 + 23.600 155.47 9.8700 0.22000 1.5000 0.12000E-02 + 23.600 157.92 9.2600 0.25000 1.5000 0.12000E-02 + 23.600 160.38 8.5900 0.23000 1.5000 0.12000E-02 + 23.600 162.83 8.5600 0.23000 1.5000 0.12000E-02 + 23.600 165.29 8.4600 0.23000 1.5000 0.12000E-02 + 23.600 167.74 8.1300 0.22000 1.5000 0.12000E-02 + 23.600 170.19 7.7800 0.21000 1.5000 0.12000E-02 + 23.600 172.64 7.8300 0.21000 1.5000 0.12000E-02 + 23.600 175.10 7.9600 0.22000 1.5000 0.12000E-02 + 27.600 10.190 0.73900E+06 28000. 1.7000 0.80000E-03 + 27.600 12.740 0.29900E+06 15000. 1.7000 0.80000E-03 + 27.600 15.290 0.15100E+06 5000.0 1.7000 0.80000E-03 + 27.600 17.830 81100. 2900.0 1.7000 0.80000E-03 + 27.600 20.380 49600. 2500.0 1.7000 0.80000E-03 + 27.600 22.920 29600. 1100.0 1.7000 0.80000E-03 + 27.600 25.470 21500. 400.00 1.7000 0.80000E-03 + 27.600 28.010 14700. 200.00 1.7000 0.80000E-03 + 27.600 30.550 9880.0 160.00 1.7000 0.80000E-03 + 27.600 33.100 7170.0 110.00 1.7000 0.80000E-03 + 27.600 35.640 5440.0 100.00 1.7000 0.80000E-03 + 27.600 38.170 4180.0 80.000 1.7000 0.80000E-03 + 27.600 40.710 3590.0 20.000 1.7000 0.80000E-03 + 27.600 43.250 2860.0 10.000 1.7000 0.80000E-03 + 27.600 45.780 2450.0 20.000 1.7000 0.80000E-03 + 27.600 48.320 1960.0 10.000 1.7000 0.80000E-03 + 27.600 50.850 1640.0 20.000 1.7000 0.80000E-03 + 27.600 53.380 1280.0 80.000 1.7000 0.80000E-03 + 27.600 55.910 1060.0 10.000 1.7000 0.80000E-03 + 27.600 58.430 834.00 6.0000 1.7000 0.80000E-03 + 27.600 60.600 649.00 6.0000 1.7000 0.80000E-03 + 27.600 63.480 516.00 5.0000 1.7000 0.80000E-03 + 27.600 66.000 399.00 5.0000 1.7000 0.80000E-03 + 27.600 68.520 315.00 4.0000 1.7000 0.80000E-03 + 27.600 71.040 247.00 2.0000 1.7000 0.80000E-03 + 27.600 73.560 191.00 2.0000 1.7000 0.80000E-03 + 27.600 76.070 149.00 2.0000 1.7000 0.80000E-03 + 27.600 78.580 117.00 1.0000 1.7000 0.80000E-03 + 27.600 81.090 94.200 1.2000 1.7000 0.80000E-03 + 27.600 83.600 74.800 0.90000 1.7000 0.80000E-03 + 27.600 86.100 59.500 0.60000 1.7000 0.80000E-03 + 27.600 88.610 47.700 0.50000 1.7000 0.80000E-03 + 27.600 91.110 38.200 0.50000 1.7000 0.80000E-03 + 27.600 93.610 31.400 0.40000 1.7000 0.80000E-03 + 27.600 96.100 25.700 0.40000 1.7000 0.80000E-03 + 27.600 98.600 22.200 1.0000 1.7000 0.80000E-03 + 27.600 101.09 17.200 0.30000 1.7000 0.80000E-03 + 27.600 103.58 14.900 0.50000 1.7000 0.80000E-03 + 27.600 106.07 12.600 0.70000 1.7000 0.80000E-03 + 27.600 108.56 10.100 0.50000 1.7000 0.80000E-03 + 27.600 111.04 8.7100 0.37000 1.7000 0.80000E-03 + 27.600 113.52 7.5100 0.21000 1.7000 0.80000E-03 + 27.600 116.52 6.1800 0.30000 1.7000 0.80000E-03 + 27.600 118.42 5.6900 0.45000 1.7000 0.80000E-03 + 27.600 120.96 4.6300 0.36000 1.7000 0.80000E-03 + 27.600 123.43 4.3200 0.34000 1.7000 0.80000E-03 + 27.600 125.91 3.6600 0.36000 1.7000 0.80000E-03 + 27.600 128.38 3.4600 0.19000 1.7000 0.80000E-03 + 27.600 130.85 2.9500 0.11000 1.7000 0.80000E-03 + 27.600 133.32 2.5500 0.11000 1.7000 0.80000E-03 + 27.600 135.78 2.2800 0.50000E-01 1.7000 0.80000E-03 + 27.600 138.25 2.0100 0.50000E-01 1.7000 0.80000E-03 + 27.600 140.71 1.8300 0.40000E-01 1.7000 0.80000E-03 + 27.600 143.17 1.6700 0.80000E-01 1.7000 0.80000E-03 + 27.600 145.64 1.6200 0.40000E-01 1.7000 0.80000E-03 + 27.600 148.10 1.4800 0.40000E-01 1.7000 0.80000E-03 + 27.600 150.55 1.4100 0.40000E-01 1.7000 0.80000E-03 + 27.600 153.01 1.2800 0.11000 1.7000 0.80000E-03 + 27.600 155.47 1.1900 0.30000E-01 1.7000 0.80000E-03 + 27.600 157.92 1.0200 0.30000E-01 1.7000 0.80000E-03 + 27.600 160.38 1.0300 0.30000E-01 1.7000 0.80000E-03 + 27.600 162.83 1.0200 0.30000E-01 1.7000 0.80000E-03 + 27.600 165.29 0.96600 0.22000E-01 1.7000 0.80000E-03 + 27.600 167.74 0.99100 0.29000E-01 1.7000 0.80000E-03 + 27.600 170.19 0.91800 0.48000E-01 1.7000 0.80000E-03 + 27.600 172.64 0.94500 0.34000E-01 1.7000 0.80000E-03 + 27.600 175.10 0.91500 0.27000E-01 1.7000 0.80000E-03 +ENDDATA 136 +ENDSUBENT 144 +SUBENT F0700011 20050621 20050831 F022 +BIB 3 3 +REACTION (83-BI-209(A,EL)83-BI-209,,DA) +SAMPLE Bi target : evaporated +STATUS (CURVE)Table 2 +ENDBIB 3 +COMMON 1 3 +THICKNESS +G/CM-SQ + 0.001 +ENDCOMMON 3 +DATA 5 135 +EN ANG-CM DATA-CM DATA-ERR1 DATA-ERR2 +MEV ADEG MB/SR MB/SR PER-CENT + 23.650 10.190 0.10300E+07 30000. 1.5000 + 23.650 12.740 0.43400E+06 11000. 1.5000 + 23.650 15.280 0.20900E+06 2000.0 1.5000 + 23.650 17.830 0.12000E+06 1000.0 1.5000 + 23.650 20.380 68200. 700.00 1.5000 + 23.650 22.920 42900. 700.00 1.5000 + 23.650 25.460 28100. 300.00 1.5000 + 23.650 28.010 19100. 200.00 1.5000 + 23.650 30.550 13900. 100.00 1.5000 + 23.650 33.090 10000. 100.00 1.5000 + 23.650 35.630 7490.0 100.00 1.5000 + 23.650 38.170 5720.0 70.000 1.5000 + 23.650 40.710 4680.0 40.000 1.5000 + 23.650 43.240 3680.0 30.000 1.5000 + 23.650 45.780 2980.0 30.000 1.5000 + 23.650 48.310 2380.0 20.000 1.5000 + 23.650 50.840 1980.0 30.000 1.5000 + 23.650 53.370 1700.0 20.000 1.5000 + 23.650 55.900 1450.0 10.000 1.5000 + 23.650 58.430 1280.0 10.000 1.5000 + 23.650 60.950 1080.0 10.000 1.5000 + 23.650 63.470 967.00 9.0000 1.5000 + 23.650 66.000 876.00 10.000 1.5000 + 23.650 68.510 764.00 9.0000 1.5000 + 23.650 71.030 682.00 6.0000 1.5000 + 23.650 73.550 594.00 4.0000 1.5000 + 23.650 76.060 524.00 5.0000 1.5000 + 23.650 78.570 449.00 5.0000 1.5000 + 23.650 81.080 393.00 5.0000 1.5000 + 23.650 83.590 351.00 4.0000 1.5000 + 23.650 86.090 310.00 4.0000 1.5000 + 23.650 88.600 274.00 3.0000 1.5000 + 23.650 91.100 234.00 3.0000 1.5000 + 23.650 93.600 210.00 3.0000 1.5000 + 23.650 96.090 179.00 3.0000 1.5000 + 23.650 98.590 156.00 2.0000 1.5000 + 23.650 101.08 139.00 2.0000 1.5000 + 23.650 103.57 119.00 2.0000 1.5000 + 23.650 106.06 105.00 2.0000 1.5000 + 23.650 108.55 91.700 1.3000 1.5000 + 23.650 111.03 80.300 1.6000 1.5000 + 23.650 113.51 71.900 1.2000 1.5000 + 23.650 116.00 62.800 0.50000 1.5000 + 23.650 118.47 57.400 0.70000 1.5000 + 23.650 120.95 50.600 0.40000 1.5000 + 23.650 123.43 45.200 0.70000 1.5000 + 23.650 125.90 40.900 0.90000 1.5000 + 23.650 128.37 35.800 0.60000 1.5000 + 23.650 130.84 32.800 0.40000 1.5000 + 23.650 133.31 29.800 0.40000 1.5000 + 23.650 135.78 26.800 0.40000 1.5000 + 23.650 138.24 24.800 0.30000 1.5000 + 23.650 140.71 22.700 0.30000 1.5000 + 23.650 143.17 21.200 0.30000 1.5000 + 23.650 145.63 20.400 0.20000 1.5000 + 23.650 148.09 18.300 0.30000 1.5000 + 23.650 150.55 17.500 0.20000 1.5000 + 23.650 153.01 15.900 0.20000 1.5000 + 23.650 155.46 15.600 0.20000 1.5000 + 23.650 157.92 14.300 0.10000 1.5000 + 23.650 160.38 13.700 0.20000 1.5000 + 23.650 162.83 13.400 0.10000 1.5000 + 23.650 165.28 12.900 0.10000 1.5000 + 23.650 167.74 12.500 0.20000 1.5000 + 23.650 170.19 12.300 0.20000 1.5000 + 23.650 172.64 12.100 0.20000 1.5000 + 23.650 175.10 12.300 0.20000 1.5000 + 27.500 10.190 0.76400E+06 31000. 1.5000 + 27.500 12.740 0.33100E+06 10000. 1.5000 + 27.500 15.280 0.15400E+06 5000.0 1.5000 + 27.500 17.830 86400. 2400.0 1.5000 + 27.500 20.380 48900. 1000.0 1.5000 + 27.500 22.920 31800. 600.00 1.5000 + 27.500 25.460 21400. 300.00 1.5000 + 27.500 28.010 14800. 200.00 1.5000 + 27.500 30.550 10500. 200.00 1.5000 + 27.500 33.090 7260.0 90.000 1.5000 + 27.500 35.630 5570.0 70.000 1.5000 + 27.500 38.170 4280.0 50.000 1.5000 + 27.500 40.710 3250.0 20.000 1.5000 + 27.500 43.240 2770.0 20.000 1.5000 + 27.500 45.780 2300.0 10.000 1.5000 + 27.500 48.310 1950.0 10.000 1.5000 + 27.500 50.840 1610.0 10.000 1.5000 + 27.500 53.370 1290.0 10.000 1.5000 + 27.500 55.900 1050.0 10.000 1.5000 + 27.500 58.430 838.00 4.0000 1.5000 + 27.500 60.950 673.00 3.0000 1.5000 + 27.500 63.470 541.00 3.0000 1.5000 + 27.500 66.000 413.00 2.0000 1.5000 + 27.500 68.510 335.00 2.0000 1.5000 + 27.500 71.030 267.00 2.0000 1.5000 + 27.500 73.550 208.00 1.0000 1.5000 + 27.500 76.060 163.00 1.0000 1.5000 + 27.500 78.570 131.00 1.0000 1.5000 + 27.500 81.080 99.800 1.1000 1.5000 + 27.500 83.590 83.700 1.0000 1.5000 + 27.500 86.090 64.300 0.80000 1.5000 + 27.500 88.600 52.200 0.70000 1.5000 + 27.500 91.100 42.400 0.60000 1.5000 + 27.500 93.600 34.800 0.50000 1.5000 + 27.500 96.090 28.300 0.50000 1.5000 + 27.500 98.590 23.600 0.40000 1.5000 + 27.500 101.08 18.900 0.30000 1.5000 + 27.500 103.57 15.300 0.40000 1.5000 + 27.500 106.06 12.600 0.30000 1.5000 + 27.500 108.55 11.000 0.20000 1.5000 + 27.500 111.03 8.9100 0.23000 1.5000 + 27.500 113.51 7.8300 0.21000 1.5000 + 27.500 116.00 6.3200 0.10000 1.5000 + 27.500 118.47 5.6100 0.13000 1.5000 + 27.500 120.95 4.7300 0.70000E-01 1.5000 + 27.500 123.43 4.1400 0.80000E-01 1.5000 + 27.500 125.90 3.7500 0.14000 1.5000 + 27.500 128.37 3.2300 0.70000E-01 1.5000 + 27.500 130.84 2.8600 0.60000E-01 1.5000 + 27.500 133.31 2.4000 0.70000E-01 1.5000 + 27.500 135.78 2.2500 0.60000E-01 1.5000 + 27.500 138.24 2.0300 0.60000E-01 1.5000 + 27.500 140.71 1.8000 0.60000E-01 1.5000 + 27.500 143.17 1.7200 0.40000E-01 1.5000 + 27.500 145.63 1.6000 0.40000E-01 1.5000 + 27.500 148.09 1.4500 0.40000E-01 1.5000 + 27.500 150.55 1.4000 0.40000E-01 1.5000 + 27.500 153.01 1.2900 0.50000E-01 1.5000 + 27.500 155.46 1.2200 0.50000E-01 1.5000 + 27.500 157.92 1.0400 0.20000E-01 1.5000 + 27.500 160.38 0.93800 0.19000E-01 1.5000 + 27.500 162.83 0.90000 0.27000E-01 1.5000 + 27.500 165.28 0.86100 0.93000E-01 1.5000 + 27.500 167.74 0.78200 0.85000E-01 1.5000 + 27.500 170.19 0.76600 0.61000E-01 1.5000 + 27.500 172.64 0.75200 0.56000E-01 1.5000 + 27.500 175.10 0.78600 0.63000E-01 1.5000 + 27.500 177.55 0.81800 0.62000E-01 1.5000 +ENDDATA 137 +ENDSUBENT 149 +ENDENTRY 11 diff --git a/exforall/F07/F0703.x4 b/exforall/F07/F0703.x4 new file mode 100644 index 000000000..08c437eed --- /dev/null +++ b/exforall/F07/F0703.x4 @@ -0,0 +1,208 @@ +ENTRY F0703 20050608 20050831 F022 +SUBENT F0703001 20050608 20050831 F022 +BIB 12 20 +TITLE Analytical possibilities of medium energy tritium beams + (3