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jasonlarkin edited this page Jan 13, 2013 · 11 revisions

##movies

each structrue is time-averaged over 100000 time steps (200 LJ units)

amorphous T=1K

https://github.com/jasonlarkin/disorder/blob/master/lj/amor/amor_1K.mp4

amorphous T=10K

https://github.com/jasonlarkin/disorder/blob/master/lj/amor/amor_10K.mp4

perfect T=10K

https://github.com/jasonlarkin/disorder/blob/master/lj/amor/per_10K.mp4

###urms

Eq. (30) refers to ~/Dropbox/ntpl-paper/internal/turney_prb09_aLD.pdf:

https://raw.github.com/jasonlarkin/disorder/master/lj/amor/m_lj_amor_x0_timeavg_compare_urms_t.png

The harmonic prediction works well for the perfect crystal, and also the amorphous phase at 1 K. However, for 5K and above the amorphous phase is more anharmonic. Even at T=1K, the amorphous phase has many meta-stable states, which contribute to larger fluctuations in the instantaneous values of <u^2>^{1/2}.

https://raw.github.com/jasonlarkin/disorder/master/lj/amor/m_lj_amor_x0_timeavg_compare_urmsmd_urms30.png

###lifetimes

https://raw.github.com/jasonlarkin/disorder/master/matlab/m_nmd_xcorr_fit_lj_plot_temperature.png

###book data

The meta-stability of the amorphous phase causes there to be negative correlation in the normal mode energies for the low frequency modes.

https://raw.github.com/jasonlarkin/disorder/master/matlab/m_nmd_xcorr_fit_lj_plot-2.png

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