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/* | ||
* MRCPP, a numerical library based on multiresolution analysis and | ||
* the multiwavelet basis which provide low-scaling algorithms as well as | ||
* rigorous error control in numerical computations. | ||
* Copyright (C) 2021 Stig Rune Jensen, Jonas Juselius, Luca Frediani and contributors. | ||
* | ||
* This file is part of MRCPP. | ||
* | ||
* MRCPP is free software: you can redistribute it and/or modify | ||
* it under the terms of the GNU Lesser General Public License as published by | ||
* the Free Software Foundation, either version 3 of the License, or | ||
* (at your option) any later version. | ||
* | ||
* MRCPP is distributed in the hope that it will be useful, | ||
* but WITHOUT ANY WARRANTY; without even the implied warranty of | ||
* MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the | ||
* GNU Lesser General Public License for more details. | ||
* | ||
* You should have received a copy of the GNU Lesser General Public License | ||
* along with MRCPP. If not, see <https://www.gnu.org/licenses/>. | ||
* | ||
* For information on the complete list of contributors to MRCPP, see: | ||
* <https://mrcpp.readthedocs.io/> | ||
*/ | ||
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#include "catch2/catch_all.hpp" | ||
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#include "factory_functions.h" | ||
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#include "functions/GaussFunc.h" | ||
#include "operators/MWOperator.h" | ||
#include "operators/PoissonKernel.h" | ||
#include "operators/PoissonOperator.h" | ||
#include "treebuilders/CrossCorrelationCalculator.h" | ||
#include "treebuilders/OperatorAdaptor.h" | ||
#include "treebuilders/TreeBuilder.h" | ||
#include "treebuilders/apply.h" | ||
#include "treebuilders/grid.h" | ||
#include "treebuilders/multiply.h" | ||
#include "treebuilders/project.h" | ||
#include "trees/BandWidth.h" | ||
#include "operators/TimeEvolutionOperator.h" | ||
#include "functions/special_functions.h" | ||
#include "treebuilders/complex_apply.h" | ||
#include "treebuilders/add.h" | ||
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//using namespace mrcpp; | ||
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namespace schrodinger_evolution_operator { | ||
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TEST_CASE("Apply Schrodinger's evolution operator", "[apply_schrodinger_evolution], [schrodinger_evolution_operator], [mw_operator]") { | ||
const auto min_scale = 0; | ||
const auto max_depth = 25; | ||
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const auto order = 4; | ||
const auto prec = 1.0e-7; | ||
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int finest_scale = 7; //for time evolution operator construction (not recommended to use more than 10) | ||
//int max_Jpower = 20; //the amount of J integrals to be used in construction (20 should be enough) | ||
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// Time moments: | ||
double t1 = 0.001; //initial time moment (not recommended to use more than 0.001) | ||
double delta_t = 0.03; //time step (not recommended to use less than 0.001) | ||
double t2 = delta_t + t1; //final time moment | ||
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// Initialize world in the unit cube [0,1] | ||
auto basis = mrcpp::LegendreBasis(order); | ||
auto world = mrcpp::BoundingBox<1>(min_scale); | ||
auto MRA = mrcpp::MultiResolutionAnalysis<1>(world, basis, max_depth); | ||
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// Time evolution operatror Exp(delta_t) | ||
mrcpp::TimeEvolutionOperator<1> ReExp(MRA, prec, delta_t, finest_scale, false); | ||
mrcpp::TimeEvolutionOperator<1> ImExp(MRA, prec, delta_t, finest_scale, true); | ||
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// Analytical solution parameters for psi(x, t) | ||
double sigma = 0.001; | ||
double x0 = 0.5; | ||
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// Functions f(x) = psi(x, t1) and g(x) = psi(x, t2) | ||
auto Re_f = [sigma, x0, t=t1](const mrcpp::Coord<1> &r) -> double | ||
{ | ||
return mrcpp::free_particle_analytical_solution(r[0], x0, t, sigma).real(); | ||
}; | ||
auto Im_f = [sigma, x0, t=t1](const mrcpp::Coord<1> &r) -> double | ||
{ | ||
return mrcpp::free_particle_analytical_solution(r[0], x0, t, sigma).imag(); | ||
}; | ||
auto Re_g = [sigma, x0, t=t2](const mrcpp::Coord<1> &r) -> double | ||
{ | ||
return mrcpp::free_particle_analytical_solution(r[0], x0, t, sigma).real(); | ||
}; | ||
auto Im_g = [sigma, x0, t=t2](const mrcpp::Coord<1> &r) -> double | ||
{ | ||
return mrcpp::free_particle_analytical_solution(r[0], x0, t, sigma).imag(); | ||
}; | ||
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// Projecting functions | ||
mrcpp::FunctionTree<1> Re_f_tree(MRA); | ||
mrcpp::project<1>(prec, Re_f_tree, Re_f); | ||
mrcpp::FunctionTree<1> Im_f_tree(MRA); | ||
mrcpp::project<1>(prec, Im_f_tree, Im_f); | ||
mrcpp::FunctionTree<1> Re_g_tree(MRA); | ||
mrcpp::project<1>(prec, Re_g_tree, Re_g); | ||
mrcpp::FunctionTree<1> Im_g_tree(MRA); | ||
mrcpp::project<1>(prec, Im_g_tree, Im_g); | ||
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// Output function trees | ||
mrcpp::FunctionTree<1> Re_fout_tree(MRA); | ||
mrcpp::FunctionTree<1> Im_fout_tree(MRA); | ||
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// Complex objects for use in apply() | ||
mrcpp::ComplexObject< mrcpp::ConvolutionOperator<1> > E(ReExp, ImExp); | ||
mrcpp::ComplexObject< mrcpp::FunctionTree<1> > input(Re_f_tree, Im_f_tree); | ||
mrcpp::ComplexObject< mrcpp::FunctionTree<1> > output(Re_fout_tree, Im_fout_tree); | ||
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// Apply operator Exp(delta_t) f(x) | ||
mrcpp::apply(prec, output, E, input); | ||
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// Check g(x) = Exp(delta_t) f(x) | ||
mrcpp::FunctionTree<1> Re_error(MRA); // = Re_fout_tree - Re_g_tree | ||
mrcpp::FunctionTree<1> Im_error(MRA); // = Im_fout_tree - Im_g_tree | ||
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// Re_error = Re_fout_tree - Re_g_tree | ||
mrcpp::add(prec, Re_error, 1.0, Re_fout_tree, -1.0, Re_g_tree); | ||
auto Re_sq_norm = Re_error.getSquareNorm(); //6.2e-16 | ||
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// Im_error = Im_fout_tree - Im_g_tree | ||
mrcpp::add(prec, Im_error, 1.0, Im_fout_tree, -1.0, Im_g_tree); | ||
auto Im_sq_norm = Im_error.getSquareNorm(); //2.7e-16 | ||
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double tolerance = prec * prec / 10.0; //1.0e-15 | ||
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REQUIRE( Re_sq_norm < tolerance ); | ||
REQUIRE( Re_sq_norm > -tolerance ); | ||
REQUIRE( Im_sq_norm < tolerance ); | ||
REQUIRE( Im_sq_norm > -tolerance ); | ||
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//The following gives rise to FAILED | ||
/* | ||
std::cout << "Re_sq_norm : " << Re_sq_norm << std::endl; | ||
std::cout << "Im_sq_norm : " << Im_sq_norm << std::endl; | ||
std::cout << "prec^2 / 100.0 : " << prec * prec / 10.0 << std::endl; | ||
REQUIRE(Re_sq_norm == Catch::Approx(0.0).epsilon(tolerance)); | ||
REQUIRE(Im_sq_norm == Catch::Approx(0.0).epsilon(tolerance)); | ||
*/ | ||
} | ||
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} // namespace schrodinger_evolution_operator |