Enumerate ising.py
From Werner KRAUTH
(Difference between revisions)
Revision as of 21:39, 22 September 2015 Werner (Talk | contribs) ← Previous diff |
Current revision Werner (Talk | contribs) |
||
Line 1: | Line 1: | ||
- | This page presents the program markov_disks_box.py, a Markov-chain algorithm for four disks in a square box of sides 1. | + | This page presents the Python3 program enumerate_ising.py, an enumeration algorithm for the Ising model using the Gray code, on the two-dimensional L x L lattice with periodic boundary conditions. As it stands, the program is only really suited for L=2 and L=4. As Python is a bit slow, it will take a few hours to terminate for L=6. |
__FORCETOC__ | __FORCETOC__ | ||
Line 5: | Line 5: | ||
=Program= | =Program= | ||
- | |||
- | import random | ||
- | |||
- | L = [[0.25, 0.25], [0.75, 0.25], [0.25, 0.75], [0.75, 0.75]] | ||
- | sigma = 0.15 | ||
- | sigma_sq = sigma ** 2 | ||
- | delta = 0.1 | ||
- | n_steps = 1000 | ||
- | for steps in range(n_steps): | ||
- | a = random.choice(L) | ||
- | b = [a[0] + random.uniform(-delta, delta), a[1] + random.uniform(-delta, delta)] | ||
- | min_dist = min((b[0] - c[0]) ** 2 + (b[1] - c[1]) ** 2 for c in L if c != a) | ||
- | box_cond = min(b[0], b[1]) < sigma or max(b[0], b[1]) > 1.0 - sigma | ||
- | if not (box_cond or min_dist < 4.0 * sigma ** 2): | ||
- | a[:] = b | ||
- | print L | ||
- | |||
- | =Version= | ||
- | See history for version information. | ||
- | |||
- | [[Category:Python]] | ||
- | |||
- | |||
def gray_flip(t, N): | def gray_flip(t, N): | ||
k = t[0] | k = t[0] | ||
Line 50: | Line 27: | ||
E += 2 * h * S[k - 1] | E += 2 * h * S[k - 1] | ||
S[k - 1] *= -1 | S[k - 1] *= -1 | ||
- | print S, E | + | print(S, E) |
+ | |||
+ | =Version= | ||
+ | See history for version information. | ||
+ | |||
+ | [[Category:Python]] [[Category:Oxford_2024]] [[Category:MOOC_SMAC]] |
Current revision
This page presents the Python3 program enumerate_ising.py, an enumeration algorithm for the Ising model using the Gray code, on the two-dimensional L x L lattice with periodic boundary conditions. As it stands, the program is only really suited for L=2 and L=4. As Python is a bit slow, it will take a few hours to terminate for L=6.
Contents |
[edit]
Description
[edit]
Program
def gray_flip(t, N): k = t[0] if k > N: return t, k t[k - 1] = t[k] t[k] = k + 1 if k != 1: t[0] = 1 return t, k L = 4 N = L * L nbr = {i : ((i // L) * L + (i + 1) % L, (i + L) % N, (i // L) * L + (i - 1) % L, (i - L) % N) for i in range(N)} S = [-1] * N E = -2 * N print S, E tau = range(1, N + 2) for i in range(1, 2 ** N): tau, k = gray_flip(tau, N) h = sum(S[n] for n in nbr[k - 1]) E += 2 * h * S[k - 1] S[k - 1] *= -1 print(S, E)
[edit]
Version
See history for version information.