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solver.C
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solver.C
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/*
Developed by Sandeep Sharma and Garnet K.-L. Chan, 2012
Copyright (c) 2012, Garnet K.-L. Chan
This program is integrated in Molpro with the permission of
Sandeep Sharma and Garnet K.-L. Chan
*/
#include "solver.h"
#include "linear.h"
#include "davidson.h"
#include "guess_wavefunction.h"
#include "blas_calls.h"
#ifndef SERIAL
#include <boost/mpi.hpp>
#endif
#include "pario.h"
void SpinAdapted::Solver::solve_wavefunction(vector<Wavefunction>& solution, vector<double>& energies, SpinBlock& big, const double tol,
const guessWaveTypes& guesswavetype, const bool &onedot, const bool& dot_with_sys, const bool& warmUp,
double additional_noise, int currentRoot, std::vector<Wavefunction>& lowerStates)
{
const int nroots = solution.size();
DiagonalMatrix e;
bool useprecond = true;
e.ReSize(big.get_stateInfo().totalStates); e= 0;
p1out << "\t\t\t Building Diagonal Hamiltonian " << endl;
big.diagonalH(e);
p1out << "\t\t\t Done building diagonal hamiltonian "<<endl;
FORTINT m, n=1, nsize=e.Storage();
p2out << "\t\t\t Number of elements in wavefunction :: " << e.Ncols() << endl;
if (mpigetrank()==0) {
m = idamax_(nsize,e.Store(), n);
p3out << "\t\t\t highest diagonal value "<<m<<" "<<e(m)<<endl;
}
else
e.ReSize(0);
bool haveEnoughStates = (e.Ncols()< nroots) ? false : true;
#ifndef SERIAL
mpi::communicator world;
broadcast(world, haveEnoughStates, 0);
#endif
if (!haveEnoughStates) {
//sometimes when you need many roots and at the start of the sweep the hilbert space is not big
//enough to support all the roots
solution.resize(nroots);
if (dmrginp.calc_type() != RESPONSE) {
for (int i=0; i<nroots; i++) {
solution[i].initialise(dmrginp.effective_molecule_quantum_vec(), &big, onedot);
solution[i].Randomise();
Normalise(solution[i]);
}
}
else {
solution.resize(1);
GuessWave::guess_wavefunctions(solution[0], e, big, guesswavetype, onedot, currentRoot,
dot_with_sys, 0.0);
}
}
else {
if(dmrginp.solve_method() == DAVIDSON) {
solution.resize(nroots);
multiply_h davidson_f(big, onedot);
GuessWave::guess_wavefunctions(solution, e, big, guesswavetype, onedot, dot_with_sys, additional_noise, currentRoot);
if (mpigetrank() == 0) {
for (int istate=0; istate<lowerStates.size(); istate++) {
for (int jstate=istate+1; jstate<lowerStates.size(); jstate++) {
double overlap = DotProduct(lowerStates[istate], lowerStates[jstate]);
ScaleAdd(-overlap/DotProduct(lowerStates[istate], lowerStates[istate]), lowerStates[istate], lowerStates[jstate]);
}
}
}
if (nroots == 1 && currentRoot >= e.Ncols()) //state specific calculation
lowerStates.resize(0);
Linear::block_davidson(solution, e, tol, warmUp, davidson_f, useprecond, currentRoot, lowerStates);
}
else if (dmrginp.solve_method() == CONJUGATE_GRADIENT) {
solution.resize(1);
//SS PLEASE REMOVE THIS
//lowerStates.resize(2);
multiply_h davidson_f(big, onedot);
if (mpigetrank()!=0)
e.ReSize(0);
GuessWave::guess_wavefunctions(solution[0], e, big, guesswavetype, onedot, currentRoot,
dot_with_sys, 0.0);
if (guesswavetype == BASIC)
solution[0].Clear();
double functional = Linear::MinResMethod(solution[0], tol, davidson_f, lowerStates);
if (mpigetrank() == 0)
e(1) = functional;
}
else {
solution.resize(1);
multiply_h davidson_f(big, onedot);
GuessWave::guess_wavefunctions(solution, e, big, guesswavetype, onedot, dot_with_sys, additional_noise, currentRoot);
Linear::Lanczos(solution, e, tol, davidson_f, nroots);
}
}
solution.resize(nroots);
energies.resize(nroots);
if (haveEnoughStates) {
for (int i=0; i<nroots&& mpigetrank() == 0;i++) {
energies[i] = e(i+1);
//pout << "\t\t\t Energy of wavefunction "<<i<<" = "<<e(i+1)<<endl;
}
}
else {
for (int i=0; i<nroots&& mpigetrank() == 0;i++) {
if (dmrginp.calc_type() == RESPONSE)
energies[i] = 1.e10;
else
energies[i] = e(1);
}
}
#ifndef SERIAL
broadcast(world, energies, 0);
#endif
pout<<endl;
}