The ensemble-mean output (mean over ten independently seeded copies of a trained…

PHYSICS · Multi-part · Fermi University Physics · Computational Physics · High-performance and data-driven computational physics · High-performance and data-driven computational physics

Scientific Computing for Physicists, Ch Neural networks on physical data: backpropagation, convolution and symmetry

Problem

The ensemble-mean output Pˉ\bar P (mean over ten independently seeded copies of a trained convolutional classifier, each giving 1 for the ordered phase and 0 for the disordered phase) is measured on independent Monte Carlo configurations of a square Ising lattice of size L=32L=32 at several temperatures, reported as kBT/Jk_BT/J: The mean outputs Pˉ\bar P at kBT/J=2.15,2.20,2.25,2.30,2.35,2.40k_BT/J = 2.15, 2.20, 2.25, 2.30, 2.35, 2.40 are 0.93,0.81,0.62,0.38,0.19,0.080.93, 0.81, 0.62, 0.38, 0.19, 0.08 respectively. ((a)) Using linear interpolation between the two temperatures whose outputs bracket Pˉ=0.5\bar P=0.5, locate the half-crossing kBT×/Jk_BT_\times/J for L=32L=32. ((b)) Compute the difference between kBT×/Jk_BT_\times/J and Onsager's exact value kBTc/J=2.269185k_BT_c/J = 2.269185. ((c)) State, in one sentence, what else would be needed before this single number could be reported as the network's estimate of TcT_c rather than only as its L=32L=32 half-crossing.

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