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# How good are Google's own "patch circuits" and "elided circuits" as a direct XEB approximation to full Sycamore circuits? | ||
# (Are they better than the 2019 Sycamore hardware?) | ||
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import math | ||
import random | ||
import statistics | ||
import sys | ||
import time | ||
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from pyqrack import QrackSimulator | ||
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def factor_width(width): | ||
col_len = math.floor(math.sqrt(width)) | ||
while (((width // col_len) * col_len) != width): | ||
col_len -= 1 | ||
row_len = width // col_len | ||
if col_len == 1: | ||
raise Exception("ERROR: Can't simulate prime number width!") | ||
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return (row_len, col_len) | ||
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def sqrt_x(sim, q): | ||
ONE_PLUS_I_DIV_2 = 0.5 + 0.5j | ||
ONE_MINUS_I_DIV_2 = 0.5 - 0.5j | ||
mtrx = [ ONE_PLUS_I_DIV_2, ONE_MINUS_I_DIV_2, ONE_MINUS_I_DIV_2, ONE_PLUS_I_DIV_2 ] | ||
sim.mtrx(mtrx, q); | ||
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def sqrt_y(sim, q): | ||
ONE_PLUS_I_DIV_2 = 0.5 + 0.5j | ||
ONE_PLUS_I_DIV_2_NEG = -0.5 - 0.5j | ||
mtrx = [ ONE_PLUS_I_DIV_2, ONE_PLUS_I_DIV_2_NEG, ONE_PLUS_I_DIV_2, ONE_PLUS_I_DIV_2 ] | ||
sim.mtrx(mtrx, q); | ||
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def sqrt_w(sim, q): | ||
diag = math.sqrt(0.5); | ||
m01 = -0.5 - 0.5j | ||
m10 = 0.5 - 0.5j | ||
mtrx = [ diag, m01, m10, diag ] | ||
sim.mtrx(mtrx, q); | ||
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def bench_qrack(width, depth): | ||
# This is a "nearest-neighbor" coupler random circuit. | ||
start = time.perf_counter() | ||
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dead_qubit = 3 if width == 54 else width | ||
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full_sim = QrackSimulator(width) | ||
patch_sim = QrackSimulator(width) | ||
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row_len, col_len = factor_width(width) | ||
row_bound = row_len >> 1 | ||
col_bound = col_len >> 1 | ||
lcv_range = range(width) | ||
last_gates = [] | ||
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# Nearest-neighbor couplers: | ||
gateSequence = [ 0, 3, 2, 1, 2, 1, 0, 3 ] | ||
one_bit_gates = [ sqrt_x, sqrt_y, sqrt_w ] | ||
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row_len, col_len = factor_width(width) | ||
patch_bound = (row_len + 1) >> 1 | ||
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for d in range(depth): | ||
# Single-qubit gates | ||
if d == 0: | ||
for i in lcv_range: | ||
g = random.choice(one_bit_gates) | ||
g(full_sim, i) | ||
g(patch_sim, i) | ||
last_gates.append(g) | ||
else: | ||
# Don't repeat the same gate on the next layer. | ||
for i in lcv_range: | ||
temp_gates = one_bit_gates.copy() | ||
temp_gates.remove(last_gates[i]) | ||
g = random.choice(one_bit_gates) | ||
g(full_sim, i) | ||
g(patch_sim, i) | ||
last_gates[i] = g | ||
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# Nearest-neighbor couplers: | ||
############################ | ||
gate = gateSequence.pop(0) | ||
gateSequence.append(gate) | ||
for row in range(1, row_len, 2): | ||
for col in range(col_len): | ||
temp_row = row | ||
temp_col = col | ||
temp_row = temp_row + (1 if (gate & 2) else -1); | ||
temp_col = temp_col + (1 if (gate & 1) else 0) | ||
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# Bounded: | ||
if (temp_row < 0) or (temp_col < 0) or (temp_row >= row_len) or (temp_col >= col_len): | ||
continue | ||
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b1 = row * row_len + col | ||
b2 = temp_row * row_len + temp_col | ||
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if (b1 >= width) or (b2 >= width) or (b1 == dead_qubit) or (b2 == dead_qubit): | ||
continue | ||
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full_sim.fsim(-math.pi / 2, math.pi / 6, b1, b2) | ||
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if ((row < row_bound) and (temp_row >= row_bound)) or ((temp_row < row_bound) and row >= row_bound) or ((col < col_bound) and (temp_col >= col_bound)) or ((temp_col < col_bound) and (col >= col_bound)): | ||
continue | ||
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patch_sim.fsim(-math.pi / 2, math.pi / 6, b1, b2) | ||
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ideal_probs = full_sim.out_probs() | ||
del full_sim | ||
patch_probs = patch_sim.out_probs() | ||
del patch_sim | ||
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return (ideal_probs, patch_probs, time.perf_counter() - start) | ||
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def calc_stats(ideal_probs, patch_probs, interval, depth): | ||
# For QV, we compare probabilities of (ideal) "heavy outputs." | ||
# If the probability is above 2/3, the protocol certifies/passes the qubit width. | ||
n_pow = len(ideal_probs) | ||
n = int(round(math.log2(n_pow))) | ||
threshold = statistics.median(ideal_probs) | ||
u_u = statistics.mean(ideal_probs) | ||
numer = 0 | ||
denom = 0 | ||
hog_prob = 0 | ||
for b in range(n_pow): | ||
ideal = ideal_probs[b] | ||
patch = patch_probs[b] | ||
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# XEB / EPLG | ||
ideal_centered = (ideal - u_u) | ||
denom += ideal_centered * ideal_centered | ||
numer += ideal_centered * (patch - u_u) | ||
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# QV / HOG | ||
if ideal > threshold: | ||
hog_prob += patch | ||
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xeb = numer / denom | ||
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return { | ||
'qubits': n, | ||
'depth': depth, | ||
'seconds': interval, | ||
'xeb': xeb, | ||
'hog_prob': hog_prob, | ||
'qv_pass': hog_prob >= 2 / 3, | ||
'eplg': (1 - (xeb ** (1 / depth))) if xeb < 1 else 0 | ||
} | ||
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def main(): | ||
if len(sys.argv) < 3: | ||
raise RuntimeError('Usage: python3 sycamore_2019_patch.py [width] [depth]') | ||
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width = int(sys.argv[1]) | ||
depth = int(sys.argv[2]) | ||
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# Run the benchmarks | ||
result = bench_qrack(width, depth) | ||
# Calc. and print the results | ||
print(calc_stats(result[0], result[1], result[2], depth)) | ||
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return 0 | ||
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if __name__ == '__main__': | ||
sys.exit(main()) |
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Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,128 @@ | ||
# How good are Google's own "patch circuits" and "elided circuits" as a direct XEB approximation to full Sycamore circuits? | ||
# (Are they better than the 2019 Sycamore hardware?) | ||
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import math | ||
import random | ||
import sys | ||
import time | ||
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from pyqrack import QrackSimulator | ||
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def factor_width(width): | ||
col_len = math.floor(math.sqrt(width)) | ||
while (((width // col_len) * col_len) != width): | ||
col_len -= 1 | ||
row_len = width // col_len | ||
if col_len == 1: | ||
raise Exception("ERROR: Can't simulate prime number width!") | ||
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return (row_len, col_len) | ||
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def sqrt_x(sim, q): | ||
ONE_PLUS_I_DIV_2 = 0.5 + 0.5j | ||
ONE_MINUS_I_DIV_2 = 0.5 - 0.5j | ||
mtrx = [ ONE_PLUS_I_DIV_2, ONE_MINUS_I_DIV_2, ONE_MINUS_I_DIV_2, ONE_PLUS_I_DIV_2 ] | ||
sim.mtrx(mtrx, q); | ||
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def sqrt_y(sim, q): | ||
ONE_PLUS_I_DIV_2 = 0.5 + 0.5j | ||
ONE_PLUS_I_DIV_2_NEG = -0.5 - 0.5j | ||
mtrx = [ ONE_PLUS_I_DIV_2, ONE_PLUS_I_DIV_2_NEG, ONE_PLUS_I_DIV_2, ONE_PLUS_I_DIV_2 ] | ||
sim.mtrx(mtrx, q); | ||
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def sqrt_w(sim, q): | ||
diag = math.sqrt(0.5); | ||
m01 = -0.5 - 0.5j | ||
m10 = 0.5 - 0.5j | ||
mtrx = [ diag, m01, m10, diag ] | ||
sim.mtrx(mtrx, q); | ||
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def bench_qrack(width, depth): | ||
# This is a "nearest-neighbor" coupler random circuit. | ||
start = time.perf_counter() | ||
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dead_qubit = 3 if width == 54 else width | ||
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patch_sim = QrackSimulator(width) | ||
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patch_bound = (width + 1) >> 1 | ||
lcv_range = range(width) | ||
all_bits = list(lcv_range) | ||
last_gates = [] | ||
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# Nearest-neighbor couplers: | ||
gateSequence = [ 0, 3, 2, 1, 2, 1, 0, 3 ] | ||
one_bit_gates = [ sqrt_x, sqrt_y, sqrt_w ] | ||
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row_len, col_len = factor_width(width) | ||
patch_bound = (row_len + 1) >> 1 | ||
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for d in range(depth): | ||
# Single-qubit gates | ||
if d == 0: | ||
for i in lcv_range: | ||
g = random.choice(one_bit_gates) | ||
g(patch_sim, i) | ||
last_gates.append(g) | ||
else: | ||
# Don't repeat the same gate on the next layer. | ||
for i in lcv_range: | ||
temp_gates = one_bit_gates.copy() | ||
temp_gates.remove(last_gates[i]) | ||
g = random.choice(one_bit_gates) | ||
g(patch_sim, i) | ||
last_gates[i] = g | ||
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# Nearest-neighbor couplers: | ||
############################ | ||
gate = gateSequence.pop(0) | ||
gateSequence.append(gate) | ||
for row in range(1, row_len, 2): | ||
for col in range(col_len): | ||
temp_row = row | ||
temp_col = col | ||
temp_row = temp_row + (1 if (gate & 2) else -1); | ||
temp_col = temp_col + (1 if (gate & 1) else 0) | ||
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# Bounded: | ||
if (temp_row < 0) or (temp_col < 0) or (temp_row >= row_len) or (temp_col >= col_len): | ||
continue | ||
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b1 = row * row_len + col | ||
b2 = temp_row * row_len + temp_col | ||
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if (b1 >= width) or (b2 >= width) or (b1 == dead_qubit) or (b2 == dead_qubit): | ||
continue | ||
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if ((b1 < patch_bound) and (b2 >= patch_bound)) or ((b2 < patch_bound) and (b1 >= patch_bound)): | ||
continue | ||
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patch_sim.fsim(-math.pi / 2, math.pi / 6, b1, b2) | ||
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# Terminal measurement | ||
patch_probs = patch_sim.m_all() | ||
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return time.perf_counter() - start | ||
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def main(): | ||
if len(sys.argv) < 3: | ||
raise RuntimeError('Usage: python3 sycamore_2019_patch.py [width] [depth]') | ||
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width = int(sys.argv[1]) | ||
depth = int(sys.argv[2]) | ||
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# Run the benchmarks | ||
result = bench_qrack(width, depth) | ||
# Calc. and print the results | ||
print("Width=" + str(width) + ", Depth=" + str(depth) + ", Seconds=" + str(result)) | ||
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return 0 | ||
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if __name__ == '__main__': | ||
sys.exit(main()) |
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