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Grid/tests/Test_hmc_WilsonFermionGauge.cc
Peter Boyle 84a66476ab Rework/global edit to enforce type templating of fermion operators.
Allows multi-precision work and paves the way for alternate BC's and such like
allowing for example G-parity which is important for K pipi programme.
In particular, can drive an extra flavour index into the fermion fields
using template types.
2015-08-10 20:47:44 +01:00

58 lines
1.6 KiB
C++

#include "Grid.h"
using namespace std;
using namespace Grid;
using namespace Grid::QCD;
int main (int argc, char ** argv)
{
Grid_init(&argc,&argv);
std::vector<int> latt_size = GridDefaultLatt();
std::vector<int> simd_layout = GridDefaultSimd(4,vComplex::Nsimd());
std::vector<int> mpi_layout = GridDefaultMpi();
GridCartesian Fine(latt_size,simd_layout,mpi_layout);
GridRedBlackCartesian RBFine(latt_size,simd_layout,mpi_layout);
GridParallelRNG pRNG(&Fine);
pRNG.SeedRandomDevice();
LatticeLorentzColourMatrix U(&Fine);
SU3::HotConfiguration(pRNG, U);
// simplify template declaration? Strip the lorentz from the second template
WilsonGaugeAction<LatticeLorentzColourMatrix, LatticeColourMatrix> Waction(5.6);
Real mass=-0.77;
WilsonFermionR FermOp(U,Fine,RBFine,mass);
ConjugateGradient<LatticeFermion> CG(1.0e-8,10000);
ConjugateGradient<LatticeFermion> CGmd(1.0e-6,10000);
TwoFlavourPseudoFermionAction<WilsonImplR> WilsonNf2(FermOp,CG,CG);
//Collect actions
ActionLevel Level1;
Level1.push_back(&WilsonNf2);
ActionLevel Level2(3);
Level2.push_back(&Waction);
ActionSet FullSet;
FullSet.push_back(Level1);
FullSet.push_back(Level2);
// Create integrator
typedef MinimumNorm2 IntegratorAlgorithm;// change here to change the algorithm
// typedef LeapFrog IntegratorAlgorithm;// change here to change the algorithm
IntegratorParameters MDpar(12,20,1.0);
std::vector<int> rel ={1};
Integrator<IntegratorAlgorithm> MDynamics(&Fine,MDpar, FullSet);
// Create HMC
HMCparameters HMCpar;
HybridMonteCarlo<IntegratorAlgorithm> HMC(HMCpar, MDynamics);
HMC.evolve(U);
}