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lines changed Original file line number Diff line number Diff line change @@ -343,7 +343,7 @@ def main():
343343 # Additionally, this same mean-field exponent is the amplitude of time-dependent oscillation (also in the geometric series exponent).
344344 t = d * dt
345345 # Determine how to weight closed-form vs. conventional simulation contributions:
346- model = ( 1 - 1 / math .exp (t / t1 )) if (t1 > 0 ) and (( t / t1 ) < 709 ) else 1
346+ model = math .exp (- t / t1 ) if (t1 > 0 ) else 0
347347 d_magnetization = 0
348348 d_sqr_magnetization = 0
349349
@@ -392,9 +392,9 @@ def main():
392392 d_magnetization = - d_magnetization
393393
394394 # Mix in the initial state component.
395- bias = model * bias + ( 1 - model ) * bias_0
396- magnetization = model * d_magnetization + ( 1 - model ) * magnetization_0
397- sqr_magnetization = model * d_sqr_magnetization + ( 1 - model ) * sqr_magnetization_0
395+ bias = ( 1 - model ) * bias + model * bias_0
396+ magnetization = ( 1 - model ) * d_magnetization + model * magnetization_0
397+ sqr_magnetization = ( 1 - model ) * d_sqr_magnetization + model * sqr_magnetization_0
398398
399399 # The full 2^n marginal probabilities will be produced in the statistics calculation,
400400 # but notice that the global magnetization value only requires (n+1) dimensions of marginal probability,
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