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https://github.com/triqs/dft_tools
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28140f14fb
Mainly on the python part. I had a quick browse through to check if the scripts were still working.
220 lines
5.9 KiB
ReStructuredText
220 lines
5.9 KiB
ReStructuredText
.. highlight:: c
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.. _ising_solution:
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The Ising chain in a magnetic field
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-----------------------------------
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Here is the a simple Monte-Carlo for a one-dimensional Ising chain. The
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problem is described in detail in this section about :ref:`the Ising model
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<isingex>`.
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The configuration
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*****************
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We start by defining a configuration class on which the move and measure
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classes will act. We write this class in a file :file:`configuration.hpp`::
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#ifndef configuration_hpp
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#define configuration_hpp
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// The configuration of the system
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struct configuration {
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// N is the length of the chain, M the total magnetization
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// beta the inverse temperature, J the coupling , field the magnetic field and energy the energy of the configuration
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// field the magnetic field and energy the energy of the configuration
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int N, M;
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double beta, J, field, energy;
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// the chain of spins: true means "up", false means "down"
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std::vector<bool> chain;
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// constructor
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configuration(int N_, double beta_, double J_, double field_):
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N(N_), M(-N), beta(beta_), J(J_), field(field_), energy(-N*(J-field)), chain(N,false) {}
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};
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#endif
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The move
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********
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The move class should have three methods: `attempt()`, `accept()` and `reject()`::
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#ifndef moves_hpp
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#define moves_hpp
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#include <triqs/mc_tools/random_generator.hpp>
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#include <vector>
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#include "configuration.hpp"
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// A move flipping a random spin
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struct flip {
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configuration * config;
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triqs::mc_tools::random_generator &RNG;
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int site;
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double delta_energy;
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// constructor
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flip(configuration & config_, triqs::mc_tools::random_generator & RNG_) :
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config(&config_), RNG(RNG_) {}
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double attempt() {
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// pick a random site
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site = RNG(config->N);
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// find the neighbors with periodicity
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int left = (site==0 ? config->N-1 : site-1);
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int right = (site==config->N-1 ? 0 : site+1);
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// compute energy difference from field
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delta_energy = (config->chain[site] ? 2 : -2) * config->field;
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// compute energy difference from J
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if(config->chain[left] == config->chain[right]) {
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delta_energy += (config->chain[left] == config->chain[site] ? 4 : -4) * config->J;
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}
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// return Metroplis ratio
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return std::exp(-config->beta * delta_energy);
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}
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// if move accepted just flip site and update energy and magnetization
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double accept() {
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config->M += (config->chain[site] ? -2 : 2);
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config->chain[site] = !config->chain[site];
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config->energy += delta_energy;
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return 1.0;
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}
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// nothing to do if the move is rejected
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void reject() {}
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};
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#endif
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Measure
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*******
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The measure class has two methods, `accumulate` and `collect_results`::
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#ifndef MEASURES_HPP
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#define MEASURES_HPP
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#include "configuration.hpp"
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// The measure of the magnetization
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struct compute_m {
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configuration * config;
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double Z, M;
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compute_m(configuration & config_) : config(&config_), Z(0), M(0) {}
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// accumulate Z and magnetization
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void accumulate(int sign) {
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Z += sign;
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M += config->M;
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}
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// get final answer M / (Z*N)
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void collect_results(boost::mpi::communicator const &c) {
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double sum_Z, sum_M;
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boost::mpi::reduce(c, Z, sum_Z, std::plus<double>(), 0);
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boost::mpi::reduce(c, M, sum_M, std::plus<double>(), 0);
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if (c.rank() == 0) {
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std::cout << "Magnetization: " << sum_M / (sum_Z*config->N) << std::endl << std::endl;
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}
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}
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};
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#endif
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Main program
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************
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The Monte-Carlo itself can now be written::
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#include <iostream>
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#include <boost/python.hpp>
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#include <triqs/mc_tools/mc_generic.hpp>
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#include <triqs/utility/callbacks.hpp>
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#include "moves.hpp"
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#include "configuration.hpp"
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#include "measures.hpp"
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int main(int argc, char* argv[]) {
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// initialize mpi
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boost::mpi::environment env(argc, argv);
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boost::mpi::communicator world;
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// greeting
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if (world.rank() == 0) std::cout << "Ising chain" << std::endl;
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// Prepare the MC parameters
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int n_cycles = 500000;
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int length_cycle = 50;
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int n_warmup_cycles = 100000;
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std::string random_name = "";
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int random_seed = 374982 + world.rank() * 273894;
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int verbosity = (world.rank() == 0 ? 2 : 0);
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// Construct a Monte Carlo loop
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triqs::mc_tools::mc_generic<double> IsingMC(n_cycles, length_cycle, n_warmup_cycles,
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random_name, random_seed, verbosity);
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// parameters of the model
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int length = 100;
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double J = -1.0;
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double field = 0.5;
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double beta = 0.5;
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// construct configuration
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configuration config(length, beta, J, field);
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// add moves and measures
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IsingMC.add_move(flip(config, IsingMC.rng()), "spin flip");
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IsingMC.add_measure(compute_m(config), "measure magnetization");
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// Run and collect results
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IsingMC.start(1.0, triqs::utility::clock_callback(-1));
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IsingMC.collect_results(world);
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return 0;
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}
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This yields::
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Ising chain
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1%; 2%; 3%; 4%; 5%; 6%; 7%; 8%; 9%; 10%; 11%; 12%; 13%; 14%; 15%; 16%; 17%;
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18%; 19%; 20%; 21%; 22%; 23%; 24%; 25%; 26%; 27%; 28%; 29%; 30%; 31%; 32%; 33%;
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34%; 35%; 36%; 37%; 38%; 39%; 40%; 41%; 42%; 43%; 44%; 45%; 46%; 47%; 48%; 49%;
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50%; 51%; 52%; 53%; 54%; 55%; 56%; 57%; 58%; 59%; 60%; 61%; 62%; 63%; 64%; 65%;
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66%; 67%; 68%; 69%; 70%; 71%; 72%; 73%; 74%; 75%; 76%; 77%; 78%; 79%; 80%; 81%;
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82%; 83%; 84%; 85%; 86%; 87%; 88%; 89%; 90%; 91%; 92%; 93%; 94%; 95%; 96%; 97%;
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98%; 99%; 100%;
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Total number of measures: 500000
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Average sign: 1
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Magnetization: 0.0927603
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