Mean field self consistency single site.py
From Werner KRAUTH
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| - | The program performs a most basic iteration (searching self-consistency) of the m = tanh(q beta m) loop. | + | The program performs a most basic iteration (searching self-consistency) of the m = tanh(q beta m) loop. If you run this program, you will notice the appearance of a self-consistent solution with m different from zero at temperatures below T=4. |
| =Program= | =Program= | ||
Current revision
This page presents the Python2 program Mean_field_self_consistency_single_site.py, that obtains the most basic self-consistency solution for the Ising model.
Contents |
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Reference
This program is discussed in Lecture 08 of my 2019 ICFP lecture on Statistical physics: "Mean-field theory: The three pillars".
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Description
The program performs a most basic iteration (searching self-consistency) of the m = tanh(q beta m) loop. If you run this program, you will notice the appearance of a self-consistent solution with m different from zero at temperatures below T=4.
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Program
import random, math, pylab
dim = 2
q = 2.0 * dim
Tc = 2.0 * dim
m_vec = [1.0]
T_vec = [0]
for iter in range(-1000, 1000):
t = iter / float(1100.0)
beta = (t * Tc + Tc) ** (-1)
T_vec.append(1.0 / beta)
m = 0.1
for iter2 in range(1000):
m = math.tanh(beta * q * m)
m_vec.append(m)
pylab.plot(T_vec, m_vec)
pylab.title('Weiss self-consistency for the Ising model
in $d$ = ' + str(dim) + ' dimensions')
pylab.xlabel('$T$ (Temperature)', fontsize=18)
pylab.ylabel('$m$ (magnetization per site)', fontsize=18)
pylab.savefig('mean_field_self_consistency_Ising.png')
pylab.show()
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Version
See history for version information.
Categories: Python | ICFP
