2018-08-28 11:32:41 +01:00
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#ifndef Hadrons_MContraction_A2APionField_hpp_
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#define Hadrons_MContraction_A2APionField_hpp_
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#include <Grid/Hadrons/Global.hpp>
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#include <Grid/Hadrons/Module.hpp>
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#include <Grid/Hadrons/ModuleFactory.hpp>
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#include <Grid/Hadrons/AllToAllVectors.hpp>
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#include <unsupported/Eigen/CXX11/Tensor>
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BEGIN_HADRONS_NAMESPACE
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/******************************************************************************
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* A2APionField *
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******************************************************************************/
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BEGIN_MODULE_NAMESPACE(MContraction)
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typedef std::pair<Gamma::Algebra, Gamma::Algebra> GammaPair;
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class A2APionFieldPar : Serializable
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{
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public:
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GRID_SERIALIZABLE_CLASS_MEMBERS(A2APionFieldPar,
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int, cacheBlock,
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int, schurBlock,
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int, Nmom,
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std::string, A2A_i,
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std::string, A2A_j,
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std::string, output);
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};
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template <typename FImpl>
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class TA2APionField : public Module<A2APionFieldPar>
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{
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public:
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FERM_TYPE_ALIASES(FImpl, );
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SOLVER_TYPE_ALIASES(FImpl, );
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typedef A2AModesSchurDiagTwo<typename FImpl::FermionField, FMat, Solver> A2ABase;
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int d_unroll ;
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public:
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// constructor
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TA2APionField(const std::string name);
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// destructor
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virtual ~TA2APionField(void){};
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// dependency relation
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virtual std::vector<std::string> getInput(void);
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virtual std::vector<std::string> getOutput(void);
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// setup
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virtual void setup(void);
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// execution
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virtual void execute(void);
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virtual void DeltaFeq2(int dt_min,int dt_max,
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Eigen::Tensor<ComplexD,2> &dF2_fig8,
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Eigen::Tensor<ComplexD,2> &dF2_trtr,
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2018-08-28 14:11:03 +01:00
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Eigen::Tensor<ComplexD,1> &den0,
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Eigen::Tensor<ComplexD,1> &den1,
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2018-08-28 11:32:41 +01:00
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Eigen::Tensor<ComplexD,3> &WW_sd,
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const LatticeFermion *vs,
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const LatticeFermion *vd,
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int orthogdim);
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///////////////////////////////////////
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// Arithmetic help. Move to Grid??
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///////////////////////////////////////
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virtual void PionFieldXX(Eigen::Tensor<ComplexD,3> &mat,
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const LatticeFermion *wi,
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const LatticeFermion *vj,
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int orthogdim,
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int g5);
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///////////////////////////
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// Simple wrappers
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///////////////////////////
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virtual void PionFieldWVmom(Eigen::Tensor<ComplexD,4> &mat,
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const LatticeFermion *wi,
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const LatticeFermion *vj,
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const std::vector<LatticeComplex > &mom,
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int orthogdim);
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virtual void PionFieldWV(Eigen::Tensor<ComplexD,3> &mat,
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const LatticeFermion *wi,
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const LatticeFermion *vj,
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int orthogdim);
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virtual void PionFieldVV(Eigen::Tensor<ComplexD,3> &mat,
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const LatticeFermion *vi,
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const LatticeFermion *vj,
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int orthogdim);
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virtual void PionFieldWW(Eigen::Tensor<ComplexD,3> &mat,
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const LatticeFermion *wi,
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const LatticeFermion *wj,
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int orthogdim);
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};
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MODULE_REGISTER(A2APionField, ARG(TA2APionField<FIMPL>), MContraction);
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MODULE_REGISTER(ZA2APionField, ARG(TA2APionField<ZFIMPL>), MContraction);
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/******************************************************************************
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* TA2APionField implementation *
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******************************************************************************/
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// constructor /////////////////////////////////////////////////////////////////
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template <typename FImpl>
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TA2APionField<FImpl>::TA2APionField(const std::string name)
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: Module<A2APionFieldPar>(name)
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{
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}
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// dependencies/products ///////////////////////////////////////////////////////
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template <typename FImpl>
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std::vector<std::string> TA2APionField<FImpl>::getInput(void)
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{
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std::vector<std::string> in;
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in.push_back(par().A2A_i + "_class");
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in.push_back(par().A2A_i + "_w_high_4d");
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in.push_back(par().A2A_i + "_v_high_4d");
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in.push_back(par().A2A_j + "_class");
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in.push_back(par().A2A_j + "_w_high_4d");
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in.push_back(par().A2A_j + "_v_high_4d");
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return in;
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}
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template <typename FImpl>
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std::vector<std::string> TA2APionField<FImpl>::getOutput(void)
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{
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std::vector<std::string> out = {};
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return out;
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}
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// setup ///////////////////////////////////////////////////////////////////////
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template <typename FImpl>
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void TA2APionField<FImpl>::setup(void)
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{
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d_unroll = 32; // empirical default. Can be overridden if desired
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// Four D fields
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envTmp(std::vector<FermionField>, "wi", 1, par().schurBlock, FermionField(env().getGrid(1)));
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envTmp(std::vector<FermionField>, "vi", 1, par().schurBlock, FermionField(env().getGrid(1)));
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envTmp(std::vector<FermionField>, "wj", 1, par().schurBlock, FermionField(env().getGrid(1)));
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envTmp(std::vector<FermionField>, "vj", 1, par().schurBlock, FermionField(env().getGrid(1)));
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// 5D tmp
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int Ls_i = env().getObjectLs(par().A2A_i + "_class");
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envTmpLat(FermionField, "tmp_5d", Ls_i);
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int Ls_j= env().getObjectLs(par().A2A_j + "_class");
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assert ( Ls_i == Ls_j );
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}
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//////////////////////////////////////////////////////////////////////////////////
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// Cache blocked arithmetic routine
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// Could move to Grid ???
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//////////////////////////////////////////////////////////////////////////////////
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template <typename FImpl>
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void TA2APionField<FImpl>::PionFieldWVmom(Eigen::Tensor<ComplexD,4> &mat,
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const LatticeFermion *wi,
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const LatticeFermion *vj,
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const std::vector<LatticeComplex > &mom,
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int orthogdim)
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{
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double t0,t1,t2,t3; t0=t1=t2=t3= 0.0;
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typedef typename FImpl::SiteSpinor vobj;
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typedef typename vobj::scalar_object sobj;
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typedef typename vobj::scalar_type scalar_type;
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typedef typename vobj::vector_type vector_type;
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typedef iSpinMatrix<vector_type> SpinMatrix_v;
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typedef iSpinMatrix<scalar_type> SpinMatrix_s;
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int Lblock = mat.dimension(2);
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int Rblock = mat.dimension(3);
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GridBase *grid = wi[0]._grid;
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const int nd = grid->_ndimension;
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const int Nsimd = grid->Nsimd();
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int Nt = grid->GlobalDimensions()[orthogdim];
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int Nmom = mom.size();
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int fd=grid->_fdimensions[orthogdim];
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int ld=grid->_ldimensions[orthogdim];
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int rd=grid->_rdimensions[orthogdim];
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// will locally sum vectors first
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// sum across these down to scalars
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// splitting the SIMD
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int MFrvol = rd*Lblock*Rblock*Nmom;
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int MFlvol = ld*Lblock*Rblock*Nmom;
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Vector<vector_type > lvSum(MFrvol);
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parallel_for (int r = 0; r < MFrvol; r++){
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lvSum[r] = zero;
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}
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Vector<scalar_type > lsSum(MFlvol);
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parallel_for (int r = 0; r < MFlvol; r++){
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lsSum[r]=scalar_type(0.0);
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}
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int e1= grid->_slice_nblock[orthogdim];
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int e2= grid->_slice_block [orthogdim];
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int stride=grid->_slice_stride[orthogdim];
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t0-=usecond();
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parallel_for(int r=0;r<rd;r++){
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int so=r*grid->_ostride[orthogdim]; // base offset for start of plane
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for(int n=0;n<e1;n++){
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for(int b=0;b<e2;b++){
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int ss= so+n*stride+b;
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for(int i=0;i<Lblock;i++){
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auto w = conjugate(wi[i]._odata[ss]);
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for(int j=0;j<Rblock;j++){
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auto v = vj[j]._odata[ss];
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auto vv = w()(0)(0) * v()(0)(0)// Gamma5 Dirac basis explicitly written out
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+ w()(0)(1) * v()(0)(1)
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+ w()(0)(2) * v()(0)(2)
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+ w()(1)(0) * v()(1)(0)
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+ w()(1)(1) * v()(1)(1)
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+ w()(1)(2) * v()(1)(2)
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- w()(2)(0) * v()(2)(0)
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- w()(2)(1) * v()(2)(1)
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- w()(2)(2) * v()(2)(2)
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- w()(3)(0) * v()(3)(0)
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- w()(3)(1) * v()(3)(1)
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- w()(3)(2) * v()(3)(2);
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// After getting the sitewise product do the mom phase loop
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int base = Nmom*i+Nmom*Lblock*j+Nmom*Lblock*Rblock*r;
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for ( int m=0;m<Nmom;m++){
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int idx = m+base;
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auto phase = mom[m]._odata[ss];
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mac(&lvSum[idx],&vv,&phase()()());
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}
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}
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}
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}
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}
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}
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t0+=usecond();
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// Sum across simd lanes in the plane, breaking out orthog dir.
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t1-=usecond();
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parallel_for(int rt=0;rt<rd;rt++){
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std::vector<int> icoor(nd);
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iScalar<vector_type> temp;
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std::vector<iScalar<scalar_type> > extracted(Nsimd);
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// std::vector<scalar_type> extracted(Nsimd);
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for(int i=0;i<Lblock;i++){
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for(int j=0;j<Rblock;j++){
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for(int m=0;m<Nmom;m++){
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int ij_rdx = m+Nmom*i+Nmom*Lblock*j+Nmom*Lblock*Rblock*rt;
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temp._internal = lvSum[ij_rdx];
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extract(temp,extracted);
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for(int idx=0;idx<Nsimd;idx++){
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grid->iCoorFromIindex(icoor,idx);
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int ldx = rt+icoor[orthogdim]*rd;
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int ij_ldx = m+Nmom*i+Nmom*Lblock*j+Nmom*Lblock*Rblock*ldx;
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lsSum[ij_ldx]=lsSum[ij_ldx]+extracted[idx]._internal;
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}
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}}}
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}
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t1+=usecond();
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assert(mat.dimension(0) == Nmom);
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assert(mat.dimension(1) == Nt);
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t2-=usecond();
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// ld loop and local only??
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int pd = grid->_processors[orthogdim];
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int pc = grid->_processor_coor[orthogdim];
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parallel_for_nest2(int lt=0;lt<ld;lt++)
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{
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for(int pt=0;pt<pd;pt++){
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int t = lt + pt*ld;
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if (pt == pc){
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for(int i=0;i<Lblock;i++){
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for(int j=0;j<Rblock;j++){
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for(int m=0;m<Nmom;m++){
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int ij_dx = m+Nmom*i + Nmom*Lblock * j + Nmom*Lblock * Rblock * lt;
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mat(m,t,i,j) = lsSum[ij_dx];
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}
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}
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}
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} else {
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const scalar_type zz(0.0);
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for(int i=0;i<Lblock;i++){
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for(int j=0;j<Rblock;j++){
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for(int m=0;m<Nmom;m++){
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mat(m,t,i,j) =zz;
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}
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}
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}
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}
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}
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}
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t2+=usecond();
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t3-=usecond();
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grid->GlobalSumVector(&mat(0,0,0,0),Nmom*Nt*Lblock*Rblock);
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t3+=usecond();
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}
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///////////////////////////////////////////////////////////////////
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//Meson
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// Interested in
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//
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// sum_x,y Trace[ G S(x,tx,y,ty) G S(y,ty,x,tx) ]
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//
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// Conventional meson field:
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//
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// = sum_x,y Trace[ sum_j G |v_j(y,ty)> <w_j(x,tx)| G sum_i |v_i(x,tx) ><w_i(y,ty)| ]
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// = sum_ij sum_x,y < w_j(x,tx)| G |v_i(x,tx) > <w_i(y,ty) (x)|G| v_j(y,ty) >
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// = sum_ij PI_ji(tx) PI_ij(ty)
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//
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// G5-Hermiticity
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//
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// sum_x,y Trace[ G S(x,tx,y,ty) G S(y,ty,x,tx) ]
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// = sum_x,y Trace[ G S(x,tx,y,ty) G g5 S^dag(x,tx,y,ty) g5 ]
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// = sum_x,y Trace[ g5 G sum_j |v_j(y,ty)> <w_j(x,tx)| G g5 sum_i (|v_j(y,ty)> <w_i(x,tx)|)^dag ] -- (*)
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//
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// NB: Dag applies to internal indices spin,colour,complex
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//
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// = sum_ij sum_x,y Trace[ g5 G |v_j(y,ty)> <w_j(x,tx)| G g5 |w_i(x,tx)> <v_i(y,ty)| ]
|
|
|
|
// = sum_ij sum_x,y <v_i(y,ty)|g5 G |v_j(y,ty)> <w_j(x,tx)| G g5 |w_i(x,tx)>
|
|
|
|
// = sum_ij PionVV(ty) PionWW(tx)
|
|
|
|
//
|
|
|
|
// (*) is only correct estimator if w_i and w_j come from distinct noise sets to preserve the kronecker
|
|
|
|
// expectation value. Otherwise biased.
|
|
|
|
////////////////////////////////////////////////////////////////////
|
|
|
|
|
|
|
|
|
|
|
|
template <typename FImpl>
|
|
|
|
void TA2APionField<FImpl>::PionFieldXX(Eigen::Tensor<ComplexD,3> &mat,
|
|
|
|
const LatticeFermion *wi,
|
|
|
|
const LatticeFermion *vj,
|
|
|
|
int orthogdim,
|
|
|
|
int g5)
|
|
|
|
{
|
|
|
|
typedef typename FImpl::SiteSpinor vobj;
|
|
|
|
|
|
|
|
typedef typename vobj::scalar_object sobj;
|
|
|
|
typedef typename vobj::scalar_type scalar_type;
|
|
|
|
typedef typename vobj::vector_type vector_type;
|
|
|
|
|
|
|
|
typedef iSpinMatrix<vector_type> SpinMatrix_v;
|
|
|
|
typedef iSpinMatrix<scalar_type> SpinMatrix_s;
|
|
|
|
|
|
|
|
int Lblock = mat.dimension(1);
|
|
|
|
int Rblock = mat.dimension(2);
|
|
|
|
|
|
|
|
GridBase *grid = wi[0]._grid;
|
|
|
|
|
|
|
|
const int nd = grid->_ndimension;
|
|
|
|
const int Nsimd = grid->Nsimd();
|
|
|
|
|
|
|
|
int Nt = grid->GlobalDimensions()[orthogdim];
|
|
|
|
|
|
|
|
int fd=grid->_fdimensions[orthogdim];
|
|
|
|
int ld=grid->_ldimensions[orthogdim];
|
|
|
|
int rd=grid->_rdimensions[orthogdim];
|
|
|
|
|
|
|
|
// will locally sum vectors first
|
|
|
|
// sum across these down to scalars
|
|
|
|
// splitting the SIMD
|
|
|
|
int MFrvol = rd*Lblock*Rblock;
|
|
|
|
int MFlvol = ld*Lblock*Rblock;
|
|
|
|
|
|
|
|
Vector<vector_type > lvSum(MFrvol);
|
|
|
|
parallel_for (int r = 0; r < MFrvol; r++){
|
|
|
|
lvSum[r] = zero;
|
|
|
|
}
|
|
|
|
|
|
|
|
Vector<scalar_type > lsSum(MFlvol);
|
|
|
|
parallel_for (int r = 0; r < MFlvol; r++){
|
|
|
|
lsSum[r]=scalar_type(0.0);
|
|
|
|
}
|
|
|
|
|
|
|
|
int e1= grid->_slice_nblock[orthogdim];
|
|
|
|
int e2= grid->_slice_block [orthogdim];
|
|
|
|
int stride=grid->_slice_stride[orthogdim];
|
|
|
|
|
|
|
|
parallel_for(int r=0;r<rd;r++){
|
|
|
|
|
|
|
|
int so=r*grid->_ostride[orthogdim]; // base offset for start of plane
|
|
|
|
|
|
|
|
for(int n=0;n<e1;n++){
|
|
|
|
for(int b=0;b<e2;b++){
|
|
|
|
|
|
|
|
int ss= so+n*stride+b;
|
|
|
|
|
|
|
|
for(int i=0;i<Lblock;i++){
|
|
|
|
|
|
|
|
auto w = conjugate(wi[i]._odata[ss]);
|
|
|
|
|
|
|
|
for(int j=0;j<Rblock;j++){
|
|
|
|
|
|
|
|
auto v = vj[j]._odata[ss];
|
|
|
|
auto vv = v()(0)(0);
|
|
|
|
if (g5) {
|
|
|
|
vv = w()(0)(0) * v()(0)(0)// Gamma5 Dirac basis explicitly written out
|
|
|
|
+ w()(0)(1) * v()(0)(1)
|
|
|
|
+ w()(0)(2) * v()(0)(2)
|
|
|
|
+ w()(1)(0) * v()(1)(0)
|
|
|
|
+ w()(1)(1) * v()(1)(1)
|
|
|
|
+ w()(1)(2) * v()(1)(2)
|
|
|
|
- w()(2)(0) * v()(2)(0)
|
|
|
|
- w()(2)(1) * v()(2)(1)
|
|
|
|
- w()(2)(2) * v()(2)(2)
|
|
|
|
- w()(3)(0) * v()(3)(0)
|
|
|
|
- w()(3)(1) * v()(3)(1)
|
|
|
|
- w()(3)(2) * v()(3)(2);
|
|
|
|
} else {
|
|
|
|
vv = w()(0)(0) * v()(0)(0)// Gamma5 Dirac basis explicitly written out
|
|
|
|
+ w()(0)(1) * v()(0)(1)
|
|
|
|
+ w()(0)(2) * v()(0)(2)
|
|
|
|
+ w()(1)(0) * v()(1)(0)
|
|
|
|
+ w()(1)(1) * v()(1)(1)
|
|
|
|
+ w()(1)(2) * v()(1)(2)
|
|
|
|
+ w()(2)(0) * v()(2)(0)
|
|
|
|
+ w()(2)(1) * v()(2)(1)
|
|
|
|
+ w()(2)(2) * v()(2)(2)
|
|
|
|
+ w()(3)(0) * v()(3)(0)
|
|
|
|
+ w()(3)(1) * v()(3)(1)
|
|
|
|
+ w()(3)(2) * v()(3)(2);
|
|
|
|
}
|
|
|
|
|
|
|
|
int idx = i+Lblock*j+Lblock*Rblock*r;
|
|
|
|
lvSum[idx] = lvSum[idx]+vv;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
// Sum across simd lanes in the plane, breaking out orthog dir.
|
|
|
|
parallel_for(int rt=0;rt<rd;rt++){
|
|
|
|
|
|
|
|
std::vector<int> icoor(nd);
|
|
|
|
iScalar<vector_type> temp;
|
|
|
|
std::vector<iScalar<scalar_type> > extracted(Nsimd);
|
|
|
|
|
|
|
|
for(int i=0;i<Lblock;i++){
|
|
|
|
for(int j=0;j<Rblock;j++){
|
|
|
|
|
|
|
|
int ij_rdx = i+Lblock*j+Lblock*Rblock*rt;
|
|
|
|
|
|
|
|
temp._internal =lvSum[ij_rdx];
|
|
|
|
extract(temp,extracted);
|
|
|
|
|
|
|
|
for(int idx=0;idx<Nsimd;idx++){
|
|
|
|
|
|
|
|
grid->iCoorFromIindex(icoor,idx);
|
|
|
|
|
|
|
|
int ldx = rt+icoor[orthogdim]*rd;
|
|
|
|
|
|
|
|
int ij_ldx =i+Lblock*j+Lblock*Rblock*ldx;
|
|
|
|
|
|
|
|
lsSum[ij_ldx]=lsSum[ij_ldx]+extracted[idx]._internal;
|
|
|
|
|
|
|
|
}
|
|
|
|
}}
|
|
|
|
}
|
|
|
|
|
|
|
|
assert(mat.dimension(0) == Nt);
|
|
|
|
// ld loop and local only??
|
|
|
|
int pd = grid->_processors[orthogdim];
|
|
|
|
int pc = grid->_processor_coor[orthogdim];
|
|
|
|
parallel_for_nest2(int lt=0;lt<ld;lt++)
|
|
|
|
{
|
|
|
|
for(int pt=0;pt<pd;pt++){
|
|
|
|
int t = lt + pt*ld;
|
|
|
|
if (pt == pc){
|
|
|
|
for(int i=0;i<Lblock;i++){
|
|
|
|
for(int j=0;j<Rblock;j++){
|
|
|
|
int ij_dx = i + Lblock * j + Lblock * Rblock * lt;
|
|
|
|
mat(t,i,j) = lsSum[ij_dx];
|
|
|
|
}
|
|
|
|
}
|
|
|
|
} else {
|
|
|
|
const scalar_type zz(0.0);
|
|
|
|
for(int i=0;i<Lblock;i++){
|
|
|
|
for(int j=0;j<Rblock;j++){
|
|
|
|
mat(t,i,j) =zz;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
grid->GlobalSumVector(&mat(0,0,0),Nt*Lblock*Rblock);
|
|
|
|
}
|
|
|
|
|
|
|
|
template <typename FImpl>
|
|
|
|
void TA2APionField<FImpl>::PionFieldWV(Eigen::Tensor<ComplexD,3> &mat,
|
|
|
|
const LatticeFermion *wi,
|
|
|
|
const LatticeFermion *vj,
|
|
|
|
int orthogdim)
|
|
|
|
{
|
|
|
|
const int g5=1;
|
|
|
|
PionFieldXX(mat,wi,vj,orthogdim,g5);
|
|
|
|
}
|
|
|
|
template <typename FImpl>
|
|
|
|
void TA2APionField<FImpl>::PionFieldWW(Eigen::Tensor<ComplexD,3> &mat,
|
|
|
|
const LatticeFermion *wi,
|
|
|
|
const LatticeFermion *wj,
|
|
|
|
int orthogdim)
|
|
|
|
{
|
|
|
|
const int nog5=0;
|
|
|
|
PionFieldXX(mat,wi,wj,orthogdim,nog5);
|
|
|
|
}
|
|
|
|
template <typename FImpl>
|
|
|
|
void TA2APionField<FImpl>::PionFieldVV(Eigen::Tensor<ComplexD,3> &mat,
|
|
|
|
const LatticeFermion *vi,
|
|
|
|
const LatticeFermion *vj,
|
|
|
|
int orthogdim)
|
|
|
|
{
|
|
|
|
const int nog5=0;
|
|
|
|
PionFieldXX(mat,vi,vj,orthogdim,nog5);
|
|
|
|
}
|
|
|
|
|
|
|
|
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
// New dirac trace code needed for efficiency (I think).
|
|
|
|
// TODO: Ask Antonin to auto gen from Mathemetica
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
template<class vtype>
|
|
|
|
inline iScalar<vtype> traceGammaZ(const iMatrix<vtype, Ns> &rhs)
|
|
|
|
{
|
|
|
|
iScalar<vtype> ret;
|
|
|
|
ret() = timesI(rhs(2,0)) + timesMinusI(rhs(3,1)) + timesMinusI(rhs(0,2)) + timesI(rhs(1,3));
|
|
|
|
return ret;
|
|
|
|
};
|
|
|
|
template<class vtype>
|
|
|
|
inline iScalar<vtype> traceGammaZGamma5(const iMatrix<vtype, Ns> &rhs)
|
|
|
|
{
|
|
|
|
iScalar<vtype> ret;
|
|
|
|
ret() = timesMinusI(rhs(2,0)) + timesI(rhs(3,1)) + timesMinusI(rhs(0,2)) + timesI(rhs(1,3));
|
|
|
|
return ret;
|
|
|
|
};
|
|
|
|
template<class vtype>
|
|
|
|
inline iScalar<vtype> traceGammaY(const iMatrix<vtype, Ns> &rhs)
|
|
|
|
{
|
|
|
|
iScalar<vtype> ret;
|
|
|
|
ret() = -rhs(3,0) + rhs(2,1) + rhs(1,2) -rhs(0,3);
|
|
|
|
return ret;
|
|
|
|
};
|
|
|
|
template<class vtype>
|
|
|
|
inline iScalar<vtype> traceGammaYGamma5(const iMatrix<vtype, Ns> &rhs)
|
|
|
|
{
|
|
|
|
iScalar<vtype> ret;
|
|
|
|
ret() = rhs(3,0) - rhs(2,1) + rhs(1,2) -rhs(0,3);
|
|
|
|
return ret;
|
|
|
|
};
|
|
|
|
template<class vtype>
|
|
|
|
inline iScalar<vtype> traceGamma5(const iMatrix<vtype, Ns> &rhs)
|
|
|
|
{
|
|
|
|
iScalar<vtype> ret;
|
|
|
|
ret() = rhs(0, 0) + rhs(1, 1) - rhs(2, 2) - rhs(3,3);
|
|
|
|
return ret;
|
|
|
|
};
|
|
|
|
template<class vtype>
|
|
|
|
inline iScalar<vtype> traceGammaT(const iMatrix<vtype, Ns> &rhs)
|
|
|
|
{
|
|
|
|
iScalar<vtype> ret;
|
|
|
|
ret() = rhs(2, 0) + rhs(3, 1) + rhs(0, 2) + rhs(1,3);
|
|
|
|
return ret;
|
|
|
|
};
|
|
|
|
template<class vtype>
|
|
|
|
inline iScalar<vtype> traceGammaTGamma5(const iMatrix<vtype, Ns> &rhs)
|
|
|
|
{
|
|
|
|
iScalar<vtype> ret;
|
|
|
|
ret() = -rhs(2, 0) - rhs(3, 1) + rhs(0, 2) + rhs(1,3);
|
|
|
|
return ret;
|
|
|
|
};
|
|
|
|
template<class vtype>
|
|
|
|
inline iScalar<vtype> traceGammaX(const iMatrix<vtype, Ns> &rhs)
|
|
|
|
{
|
|
|
|
iScalar<vtype> ret;
|
|
|
|
ret() = timesMinusI(rhs(0, 3)) +timesMinusI(rhs(1, 2))
|
|
|
|
+ timesI(rhs(2, 1)) +timesI(rhs(3,0));
|
|
|
|
return ret;
|
|
|
|
};
|
|
|
|
template<class vtype>
|
|
|
|
inline iScalar<vtype> traceGammaXGamma5(const iMatrix<vtype, Ns> &rhs)
|
|
|
|
{
|
|
|
|
iScalar<vtype> ret;
|
|
|
|
ret() = timesMinusI(rhs(0, 3)) +timesMinusI(rhs(1, 2))
|
|
|
|
+ timesMinusI(rhs(2, 1)) +timesMinusI(rhs(3,0));
|
|
|
|
return ret;
|
|
|
|
};
|
|
|
|
|
|
|
|
|
|
|
|
////////////////////////////////////////////////////////////////////////
|
|
|
|
// DeltaF=2 contraction ; use exernal WW field for Kaon, anti Kaon sink
|
|
|
|
////////////////////////////////////////////////////////////////////////
|
|
|
|
//
|
|
|
|
// WW -- i vectors have adjoint, and j vectors not.
|
|
|
|
// -- Think of "i" as the strange quark, forward prop from 0
|
|
|
|
// -- Think of "j" as the anti-down quark.
|
|
|
|
//
|
|
|
|
// WW_sd are w^dag_s w_d
|
|
|
|
//
|
|
|
|
// Hence VV vectors correspondingly are v^dag_d, v_s from t=0
|
|
|
|
// and v^dag_d, v_s from t=dT
|
|
|
|
//
|
|
|
|
// There is an implicit g5 associated with each v^dag_d from use of g5 Hermiticity.
|
|
|
|
// The other gamma_5 lies in the WW external meson operator.
|
|
|
|
//
|
|
|
|
// From UKhadron wallbag.cc:
|
|
|
|
//
|
|
|
|
// LatticePropagator anti_d0 = adj( Gamma(G5) * Qd0 * Gamma(G5));
|
|
|
|
// LatticePropagator anti_d1 = adj( Gamma(G5) * Qd1 * Gamma(G5));
|
|
|
|
//
|
|
|
|
// PR1 = Qs0 * Gamma(G5) * anti_d0;
|
|
|
|
// PR2 = Qs1 * Gamma(G5) * anti_d1;
|
|
|
|
//
|
|
|
|
// TR1 = trace( PR1 * G1 );
|
|
|
|
// TR2 = trace( PR2 * G2 );
|
|
|
|
// Wick1 = TR1 * TR2;
|
|
|
|
//
|
|
|
|
// Wick2 = trace( PR1* G1 * PR2 * G2 );
|
|
|
|
// // was Wick2 = trace( Qs0 * Gamma(G5) * anti_d0 * G1 * Qs1 * Gamma(G5) * anti_d1 * G2 );
|
|
|
|
//
|
|
|
|
// TR TR(tx) = Wick1 = sum_x WW[t0]_sd < v^_d |g5 G| v_s> WW[t1]_s'd' < v^_d' |g5 G| v_s'> |_{x,tx)
|
|
|
|
// = sum_x [ Trace(WW[t0] VgV(t,x) ) x Trace( WW_[t1] VgV(t,x) ) ]
|
|
|
|
//
|
|
|
|
//
|
|
|
|
// Calc all Nt Trace(WW VV) products at once, take Nt^2 products of these.
|
|
|
|
//
|
|
|
|
// Fig8(tx) = Wick2 = sum_x WW[t0]_sd WW[t1]_s'd' < v^_d |g5 G| v_s'> < v^_d' |g5 G| v_s> |_{x,tx}
|
|
|
|
//
|
|
|
|
// = sum_x Trace( WW[t0] VV[t,x] WW[t1] VV[t,x] )
|
|
|
|
//
|
|
|
|
///////////////////////////////////////////////////////////////////////////////
|
2018-08-28 14:11:03 +01:00
|
|
|
//
|
2018-08-28 11:32:41 +01:00
|
|
|
// WW is w_s^dag (x) w_d (G5 implicitly absorbed)
|
|
|
|
//
|
|
|
|
// WWVV will have spin-col (x) spin-col tensor.
|
|
|
|
//
|
|
|
|
// Want this to look like a strange fwd prop, anti-d prop.
|
|
|
|
//
|
|
|
|
// Take WW_sd v^dag_d (x) v_s
|
|
|
|
//
|
|
|
|
//
|
|
|
|
|
|
|
|
template <typename FImpl>
|
2018-08-28 14:11:03 +01:00
|
|
|
void TA2APionField<FImpl>::DeltaFeq2(int dt_min,int dt_max,
|
|
|
|
Eigen::Tensor<ComplexD,2> &dF2_fig8,
|
|
|
|
Eigen::Tensor<ComplexD,2> &dF2_trtr,
|
|
|
|
Eigen::Tensor<ComplexD,1> &den0,
|
|
|
|
Eigen::Tensor<ComplexD,1> &den1,
|
|
|
|
Eigen::Tensor<ComplexD,3> &WW_sd,
|
|
|
|
const LatticeFermion *vs,
|
|
|
|
const LatticeFermion *vd,
|
|
|
|
int orthogdim)
|
2018-08-28 11:32:41 +01:00
|
|
|
{
|
|
|
|
LOG(Message) << "Computing A2A DeltaF=2 graph" << std::endl;
|
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2018-08-28 14:11:03 +01:00
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int dt = dt_min;
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2018-08-28 11:32:41 +01:00
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auto G5 = Gamma(Gamma::Algebra::Gamma5);
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typedef typename FImpl::SiteSpinor vobj;
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typedef typename vobj::scalar_object sobj;
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typedef typename vobj::scalar_type scalar_type;
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typedef typename vobj::vector_type vector_type;
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typedef iSpinMatrix<vector_type> SpinMatrix_v;
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typedef iSpinMatrix<scalar_type> SpinMatrix_s;
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typedef iSinglet<vector_type> Scalar_v;
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typedef iSinglet<scalar_type> Scalar_s;
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int N_s = WW_sd.dimension(1);
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int N_d = WW_sd.dimension(2);
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GridBase *grid = vs[0]._grid;
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const int nd = grid->_ndimension;
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const int Nsimd = grid->Nsimd();
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int N_t = grid->GlobalDimensions()[orthogdim];
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double vol = 1.0;
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for(int dim=0;dim<nd;dim++){
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vol = vol * grid->GlobalDimensions()[dim];
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}
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double nodes = grid->NodeCount();
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dF2_trtr.resize(N_t,16);
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dF2_fig8.resize(N_t,16);
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den0.resize(N_t);
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den1.resize(N_t);
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for(int t=0;t<N_t;t++){
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for(int g=0;g<dF2_trtr.dimension(1);g++) dF2_trtr(t,g)= ComplexD(0.0);
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for(int g=0;g<dF2_fig8.dimension(1);g++) dF2_fig8(t,g)= ComplexD(0.0);
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den0(t) =ComplexD(0.0);
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den1(t) =ComplexD(0.0);
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}
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LatticeComplex D0(grid); // <P|A0> correlator from each wall
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LatticeComplex D1(grid);
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LatticeComplex O1_trtr(grid);
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LatticeComplex O2_trtr(grid);
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LatticeComplex O3_trtr(grid);
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LatticeComplex O4_trtr(grid);
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LatticeComplex O5_trtr(grid);
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LatticeComplex O1_fig8(grid);
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LatticeComplex O2_fig8(grid);
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LatticeComplex O3_fig8(grid);
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LatticeComplex O4_fig8(grid);
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LatticeComplex O5_fig8(grid);
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O1_trtr = zero;
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O2_trtr = zero;
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O3_trtr = zero;
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O4_trtr = zero;
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O5_trtr = zero;
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O1_fig8 = zero;
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O2_fig8 = zero;
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O3_fig8 = zero;
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O4_fig8 = zero;
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O5_fig8 = zero;
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D0 = zero;
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D1 = zero;
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double t_tot = -usecond();
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std::vector<LatticePropagator> WWVV (N_t,grid);
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for(int t=0;t<N_t;t++){
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WWVV[t] = zero;
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}
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2018-08-28 14:11:03 +01:00
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//////////////////////////////////////////////////////////////////
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// Method-5 - wrap this assembly in a distinct routine for reuse
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//////////////////////////////////////////////////////////////////
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2018-08-28 11:32:41 +01:00
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double t_outer= -usecond();
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parallel_for(int ss=0;ss<grid->oSites();ss++){
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for(int d_o=0;d_o<N_d;d_o+=d_unroll){
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for(int t=0;t<N_t;t++){
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for(int s=0;s<N_s;s++){
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auto tmp1 = vs[s]._odata[ss];
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vobj tmp2 = zero;
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2018-08-28 14:11:03 +01:00
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////////////////////////////////////////
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// Surprisingly slow with d_unroll = 32
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////////////////////////////////////////
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2018-08-28 11:32:41 +01:00
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for(int d=d_o;d<MIN(d_o+d_unroll,N_d);d++){
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Scalar_v coeff = WW_sd(t,s,d);
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mac(&tmp2 ,& coeff, & vd[d]._odata[ss]);
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}
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2018-08-28 14:11:03 +01:00
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//////////////////////////
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// Fast outer product of tmp1 with a sum of terms suppressed by d_unroll
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//////////////////////////
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2018-08-28 11:32:41 +01:00
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tmp2 = conjugate(tmp2);
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for(int s1=0;s1<Ns;s1++){
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for(int s2=0;s2<Ns;s2++){
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WWVV[t]._odata[ss]()(s1,s2)(0,0) += tmp1()(s1)(0)*tmp2()(s2)(0);
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WWVV[t]._odata[ss]()(s1,s2)(0,1) += tmp1()(s1)(0)*tmp2()(s2)(1);
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WWVV[t]._odata[ss]()(s1,s2)(0,2) += tmp1()(s1)(0)*tmp2()(s2)(2);
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WWVV[t]._odata[ss]()(s1,s2)(1,0) += tmp1()(s1)(1)*tmp2()(s2)(0);
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WWVV[t]._odata[ss]()(s1,s2)(1,1) += tmp1()(s1)(1)*tmp2()(s2)(1);
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WWVV[t]._odata[ss]()(s1,s2)(1,2) += tmp1()(s1)(1)*tmp2()(s2)(2);
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WWVV[t]._odata[ss]()(s1,s2)(2,0) += tmp1()(s1)(2)*tmp2()(s2)(0);
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WWVV[t]._odata[ss]()(s1,s2)(2,1) += tmp1()(s1)(2)*tmp2()(s2)(1);
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WWVV[t]._odata[ss]()(s1,s2)(2,2) += tmp1()(s1)(2)*tmp2()(s2)(2);
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}}
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}}
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}
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}
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t_outer+=usecond();
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//////////////////////////////
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// Implicit gamma-5
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//////////////////////////////
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for(int t=0;t<N_t;t++){
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WWVV[t] = WWVV[t]* G5 ;
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}
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//////////////////////////////////////////////////
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// Used to store appropriate correlation funcs
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//////////////////////////////////////////////////
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std::vector<TComplex> C1;
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std::vector<TComplex> C2;
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std::vector<TComplex> C3;
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std::vector<TComplex> C4;
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std::vector<TComplex> C5;
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//////////////////////////////////////////////////////////
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// Could do AA, VV, SS, PP, TT and form linear combinations later.
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// Almost 2x. but for many modes, the above loop dominates.
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//////////////////////////////////////////////////////////
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double t_contr= -usecond();
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for(int t0=0;t0<N_t;t0++){
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// No loop over t1
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// Cost is trivial to add given cost of outer product
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{
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int t1 = (t0+dt)%N_t;
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parallel_for(int ss=0;ss<grid->oSites();ss++){
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auto VV0= WWVV[t0]._odata[ss];
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auto VV1= WWVV[t1]._odata[ss];
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// Tr Tr Wick contraction
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auto VX = Gamma(Gamma::Algebra::GammaX);
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auto VY = Gamma(Gamma::Algebra::GammaY);
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auto VZ = Gamma(Gamma::Algebra::GammaZ);
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auto VT = Gamma(Gamma::Algebra::GammaT);
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auto AX = Gamma(Gamma::Algebra::GammaXGamma5);
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auto AY = Gamma(Gamma::Algebra::GammaYGamma5);
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auto AZ = Gamma(Gamma::Algebra::GammaZGamma5);
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auto AT = Gamma(Gamma::Algebra::GammaTGamma5);
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auto S = Gamma(Gamma::Algebra::Identity);
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auto P = Gamma(Gamma::Algebra::Gamma5);
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auto T0 = Gamma(Gamma::Algebra::SigmaXY);
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auto T1 = Gamma(Gamma::Algebra::SigmaXZ);
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auto T2 = Gamma(Gamma::Algebra::SigmaXT);
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auto T3 = Gamma(Gamma::Algebra::SigmaYZ);
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auto T4 = Gamma(Gamma::Algebra::SigmaYT);
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auto T5 = Gamma(Gamma::Algebra::SigmaZT);
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O1_trtr._odata[ss] = trace(VX*VV0) * trace(VX*VV1)
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+ trace(VY*VV0) * trace(VY*VV1)
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+ trace(VZ*VV0) * trace(VZ*VV1)
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+ trace(VT*VV0) * trace(VT*VV1)
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+ trace(AX*VV0) * trace(AX*VV1)
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+ trace(AY*VV0) * trace(AY*VV1)
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+ trace(AZ*VV0) * trace(AZ*VV1)
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+ trace(AT*VV0) * trace(AT*VV1);
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O2_trtr._odata[ss] = trace(VX*VV0) * trace(VX*VV1)
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+ trace(VY*VV0) * trace(VY*VV1)
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+ trace(VZ*VV0) * trace(VZ*VV1)
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+ trace(VT*VV0) * trace(VT*VV1)
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- trace(AX*VV0) * trace(AX*VV1)
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- trace(AY*VV0) * trace(AY*VV1)
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- trace(AZ*VV0) * trace(AZ*VV1)
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- trace(AT*VV0) * trace(AT*VV1);
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O3_trtr._odata[ss] = trace(S*VV0) * trace(S*VV1)
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+ trace(P*VV0) * trace(P*VV1);
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O4_trtr._odata[ss] = trace(S*VV0) * trace(S*VV1)
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- trace(P*VV0) * trace(P*VV1);
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O5_trtr._odata[ss] = trace(T0*VV0) * trace(T0*VV1)
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+ trace(T1*VV0) * trace(T1*VV1)
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+ trace(T2*VV0) * trace(T2*VV1)
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+ trace(T3*VV0) * trace(T3*VV1)
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+ trace(T4*VV0) * trace(T4*VV1)
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+ trace(T5*VV0) * trace(T5*VV1);
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////////////////////////////////////
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// Fig8 Wick contraction
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////////////////////////////////////
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// was (UKhadron) Wick2 = trace( Qs0 * Gamma(G5) * anti_d0 * G * Qs1 * Gamma(G5) * anti_d1 * G );
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//
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// = trace( [ Vs WW_sd'[t0] Vd'^dag ] G [ Vs' WW_s'd[t1] Vd^dag ] G )
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// = trace( WWVV * G * WWVV * G )
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//
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// Can do VV and AA seperately and then add/sub later cheaper
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O1_fig8._odata[ss] = trace (VV0 * VX * VV1 * VX)
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+ trace (VV0 * VY * VV1 * VY)
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+ trace (VV0 * VZ * VV1 * VZ)
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+ trace (VV0 * VT * VV1 * VT)
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+ trace (VV0 * AX * VV1 * AX)
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+ trace (VV0 * AY * VV1 * AY)
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+ trace (VV0 * AZ * VV1 * AZ)
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+ trace (VV0 * AT * VV1 * AT);
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O2_fig8._odata[ss] = trace (VV0 * VX * VV1 * VX)
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+ trace (VV0 * VY * VV1 * VY)
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+ trace (VV0 * VZ * VV1 * VZ)
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+ trace (VV0 * VT * VV1 * VT)
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- trace (VV0 * AX * VV1 * AX)
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- trace (VV0 * AY * VV1 * AY)
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- trace (VV0 * AZ * VV1 * AZ)
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- trace (VV0 * AT * VV1 * AT);
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O3_fig8._odata[ss] = trace (VV0 * S * VV1 * S)
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+ trace (VV0 * P * VV1 * P);
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O4_fig8._odata[ss] = trace (VV0 * S * VV1 * S)
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- trace (VV0 * P * VV1 * P);
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O5_fig8._odata[ss] = trace (VV0 * T0 * VV1 * T0)
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+ trace (VV0 * T1 * VV1 * T1)
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+ trace (VV0 * T2 * VV1 * T2)
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+ trace (VV0 * T3 * VV1 * T3)
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+ trace (VV0 * T4 * VV1 * T4)
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+ trace (VV0 * T5 * VV1 * T5);
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// Hack force PP correlator
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// D0._odata[ss] = trace(P*VV0); // These match signed off
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// D1._odata[ss] = trace(P*VV1);
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D0._odata[ss] = trace(AT*VV0);
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|
D1._odata[ss] = trace(AT*VV1);
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}
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|
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sliceSum(O1_trtr,C1, orthogdim);
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sliceSum(O2_trtr,C2, orthogdim);
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|
sliceSum(O3_trtr,C3, orthogdim);
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|
sliceSum(O4_trtr,C4, orthogdim);
|
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|
|
sliceSum(O5_trtr,C5, orthogdim);
|
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|
|
|
|
|
|
for(int t=0;t<N_t;t++){// 2x from Wick contraction reordering
|
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|
|
dF2_trtr(t,0)+= 2.0*C1[(t+t0)%N_t]()()()/vol;
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|
|
dF2_trtr(t,1)+= 2.0*C2[(t+t0)%N_t]()()()/vol;
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|
|
dF2_trtr(t,2)+= 2.0*C3[(t+t0)%N_t]()()()/vol;
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|
|
dF2_trtr(t,3)+= 2.0*C4[(t+t0)%N_t]()()()/vol;
|
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|
|
dF2_trtr(t,4)+= 2.0*C5[(t+t0)%N_t]()()()/vol;
|
|
|
|
}
|
|
|
|
|
|
|
|
sliceSum(O1_fig8,C1, orthogdim);
|
|
|
|
sliceSum(O2_fig8,C2, orthogdim);
|
|
|
|
sliceSum(O3_fig8,C3, orthogdim);
|
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|
|
sliceSum(O4_fig8,C4, orthogdim);
|
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|
|
sliceSum(O5_fig8,C5, orthogdim);
|
|
|
|
|
|
|
|
for(int t=0;t<N_t;t++){
|
|
|
|
dF2_fig8(t,0)= 2.0*C1[(t+t0)%N_t]()()()/vol;
|
|
|
|
dF2_fig8(t,1)= 2.0*C2[(t+t0)%N_t]()()()/vol;
|
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|
|
dF2_fig8(t,2)= 2.0*C3[(t+t0)%N_t]()()()/vol;
|
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|
|
dF2_fig8(t,3)= 2.0*C4[(t+t0)%N_t]()()()/vol;
|
|
|
|
dF2_fig8(t,4)= 2.0*C5[(t+t0)%N_t]()()()/vol;
|
|
|
|
}
|
|
|
|
|
|
|
|
sliceSum(D0,C1, orthogdim);
|
|
|
|
sliceSum(D1,C2, orthogdim);
|
|
|
|
for(int t=0;t<N_t;t++){
|
|
|
|
den0(t)+=C1[(t+t0)%N_t]()()()/vol;
|
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|
|
den1(t)+=C2[(t+t0)%N_t]()()()/vol;
|
|
|
|
}
|
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|
|
|
|
|
|
}
|
|
|
|
}
|
|
|
|
t_contr +=usecond();
|
|
|
|
|
|
|
|
t_tot+=usecond();
|
|
|
|
double million=1.0e6;
|
|
|
|
LOG(Message) << "Computing A2A DeltaF=2 graph t_tot " << t_tot /million << " s "<< std::endl;
|
|
|
|
LOG(Message) << "Computing A2A DeltaF=2 graph t_outer " << t_outer /million << " s "<< std::endl;
|
|
|
|
LOG(Message) << "Computing A2A DeltaF=2 graph t_contr " << t_contr /million << " s "<< std::endl;
|
|
|
|
|
|
|
|
}
|
|
|
|
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|
|
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|
|
|
|
|
|
|
|
// execution ///////////////////////////////////////////////////////////////////
|
|
|
|
template <typename FImpl>
|
|
|
|
void TA2APionField<FImpl>::execute(void)
|
|
|
|
{
|
|
|
|
LOG(Message) << "Computing A2A Pion fields" << std::endl;
|
|
|
|
|
|
|
|
auto &a2a_i = envGet(A2ABase, par().A2A_i + "_class");
|
|
|
|
auto &a2a_j = envGet(A2ABase, par().A2A_j + "_class");
|
|
|
|
|
|
|
|
///////////////////////////////////////////////
|
|
|
|
// Square assumption for now Nl = Nr = N
|
|
|
|
///////////////////////////////////////////////
|
|
|
|
int nt = env().getDim(Tp);
|
|
|
|
int nx = env().getDim(Xp);
|
|
|
|
int ny = env().getDim(Yp);
|
|
|
|
int nz = env().getDim(Zp);
|
|
|
|
|
|
|
|
// int N_i = a2a_i.par().N;
|
|
|
|
// int N_j = a2a_j.par().N;
|
|
|
|
int N_i = a2a_i.getN();
|
|
|
|
int N_j = a2a_j.getN();
|
|
|
|
|
|
|
|
int nmom=par().Nmom;
|
|
|
|
|
|
|
|
int schurBlock = par().schurBlock;
|
|
|
|
int cacheBlock = par().cacheBlock;
|
|
|
|
|
|
|
|
|
|
|
|
///////////////////////////////////////////////
|
|
|
|
// Momentum setup
|
|
|
|
///////////////////////////////////////////////
|
|
|
|
GridBase *grid = env().getGrid(1);
|
|
|
|
std::vector<LatticeComplex> phases(nmom,grid);
|
|
|
|
for(int m=0;m<nmom;m++){
|
|
|
|
phases[m] = Complex(1.0); // All zero momentum for now
|
|
|
|
}
|
|
|
|
|
|
|
|
///////////////////////////////////////////////////////////////////////
|
|
|
|
// i and j represent different flavours, hits, with different ranks.
|
|
|
|
// in general non-square case.
|
|
|
|
///////////////////////////////////////////////////////////////////////
|
|
|
|
Eigen::Tensor<ComplexD,4> pionFieldWVmom_ij (nmom,nt,N_i,N_j);
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldWV_ij (nt,N_i,N_j);
|
|
|
|
|
|
|
|
Eigen::Tensor<ComplexD,4> pionFieldWVmom_ji (nmom,nt,N_j,N_i);
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldWV_ji (nt,N_j,N_i);
|
|
|
|
|
|
|
|
|
|
|
|
LOG(Message) << "Rank for A2A PionField is " << N_i << " x "<<N_j << std::endl;
|
|
|
|
|
|
|
|
envGetTmp(std::vector<FermionField>, wi);
|
|
|
|
envGetTmp(std::vector<FermionField>, vi);
|
|
|
|
|
|
|
|
envGetTmp(std::vector<FermionField>, wj);
|
|
|
|
envGetTmp(std::vector<FermionField>, vj);
|
|
|
|
envGetTmp(FermionField, tmp_5d);
|
|
|
|
|
|
|
|
LOG(Message) << "Finding v and w vectors " << std::endl;
|
|
|
|
|
|
|
|
//////////////////////////////////////////////////////////////////////////
|
|
|
|
// i,j is first loop over SchurBlock factors reusing 5D matrices
|
|
|
|
// ii,jj is second loop over cacheBlock factors for high perf contractoin
|
|
|
|
// iii,jjj are loops within cacheBlock
|
|
|
|
// Total index is sum of these i+ii+iii etc...
|
|
|
|
//////////////////////////////////////////////////////////////////////////
|
|
|
|
|
|
|
|
double flops = 0.0;
|
|
|
|
double bytes = 0.0;
|
|
|
|
double vol = nx*ny*nz*nt;
|
|
|
|
double vol3 = nx*ny*nz;
|
|
|
|
double t_schur=0;
|
|
|
|
double t_contr_vwm=0;
|
|
|
|
double t_contr_vw=0;
|
|
|
|
double t_contr_ww=0;
|
|
|
|
double t_contr_vv=0;
|
|
|
|
|
|
|
|
double tt0 = usecond();
|
|
|
|
for(int i=0;i<N_i;i+=schurBlock){ //loop over SchurBlocking to suppress 5D matrix overhead
|
|
|
|
for(int j=0;j<N_j;j+=schurBlock){
|
|
|
|
|
|
|
|
///////////////////////////////////////////////////////////////
|
|
|
|
// Get the W and V vectors for this schurBlock^2 set of terms
|
|
|
|
///////////////////////////////////////////////////////////////
|
|
|
|
int N_ii = MIN(N_i-i,schurBlock);
|
|
|
|
int N_jj = MIN(N_j-j,schurBlock);
|
|
|
|
|
|
|
|
t_schur-=usecond();
|
|
|
|
for(int ii =0;ii < N_ii;ii++) a2a_i.return_w(i+ii, tmp_5d, wi[ii]);
|
|
|
|
for(int jj =0;jj < N_jj;jj++) a2a_j.return_w(j+jj, tmp_5d, wj[jj]);
|
|
|
|
|
|
|
|
for(int ii =0;ii < N_ii;ii++) a2a_i.return_v(i+ii, tmp_5d, vi[ii]);
|
|
|
|
for(int jj =0;jj < N_jj;jj++) a2a_j.return_v(j+jj, tmp_5d, vj[jj]);
|
|
|
|
t_schur+=usecond();
|
|
|
|
|
|
|
|
LOG(Message) << "Found i w&v vectors " << i <<" .. " << i+N_ii-1 << std::endl;
|
|
|
|
LOG(Message) << "Found j w&v vectors " << j <<" .. " << j+N_jj-1 << std::endl;
|
|
|
|
|
|
|
|
///////////////////////////////////////////////////////////////
|
|
|
|
// Series of cache blocked chunks of the contractions within this SchurBlock
|
|
|
|
///////////////////////////////////////////////////////////////
|
|
|
|
for(int ii=0;ii<N_ii;ii+=cacheBlock){
|
|
|
|
for(int jj=0;jj<N_jj;jj+=cacheBlock){
|
|
|
|
|
|
|
|
int N_iii = MIN(N_ii-ii,cacheBlock);
|
|
|
|
int N_jjj = MIN(N_jj-jj,cacheBlock);
|
|
|
|
|
|
|
|
Eigen::Tensor<ComplexD,4> pionFieldWVmomB_ij(nmom,nt,N_iii,N_jjj);
|
|
|
|
Eigen::Tensor<ComplexD,4> pionFieldWVmomB_ji(nmom,nt,N_jjj,N_iii);
|
|
|
|
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldWVB_ij(nt,N_iii,N_jjj);
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldWVB_ji(nt,N_jjj,N_iii);
|
|
|
|
|
|
|
|
t_contr_vwm-=usecond();
|
|
|
|
PionFieldWVmom(pionFieldWVmomB_ij, &wi[ii], &vj[jj], phases,Tp);
|
|
|
|
PionFieldWVmom(pionFieldWVmomB_ji, &wj[jj], &vi[ii], phases,Tp);
|
|
|
|
t_contr_vwm+=usecond();
|
|
|
|
|
|
|
|
t_contr_vw-=usecond();
|
|
|
|
PionFieldWV(pionFieldWVB_ij, &wi[ii], &vj[jj],Tp);
|
|
|
|
PionFieldWV(pionFieldWVB_ji, &wj[jj], &vi[ii],Tp);
|
|
|
|
t_contr_vw+=usecond();
|
|
|
|
|
|
|
|
|
|
|
|
flops += vol * ( 2 * 8.0 + 6.0 + 8.0*nmom) * N_iii*N_jjj;
|
|
|
|
|
|
|
|
bytes += vol * (12.0 * sizeof(Complex) ) * N_iii*N_jjj
|
|
|
|
+ vol * ( 2.0 * sizeof(Complex) *nmom ) * N_iii*N_jjj;
|
|
|
|
|
|
|
|
///////////////////////////////////////////////////////////////
|
|
|
|
// Copy back to full meson field tensor
|
|
|
|
///////////////////////////////////////////////////////////////
|
|
|
|
parallel_for_nest2(int iii=0;iii< N_iii;iii++) {
|
|
|
|
for(int jjj=0;jjj< N_jjj;jjj++) {
|
|
|
|
|
|
|
|
for(int m =0;m< nmom;m++) {
|
|
|
|
for(int t =0;t< nt;t++) {
|
|
|
|
pionFieldWVmom_ij(m,t,i+ii+iii,j+jj+jjj) = pionFieldWVmomB_ij(m,t,iii,jjj);
|
|
|
|
pionFieldWVmom_ji(m,t,j+jj+jjj,i+ii+iii) = pionFieldWVmomB_ji(m,t,jjj,iii);
|
|
|
|
}}
|
|
|
|
|
|
|
|
for(int t =0;t< nt;t++) {
|
|
|
|
pionFieldWV_ij(t,i+ii+iii,j+jj+jjj) = pionFieldWVB_ij(t,iii,jjj);
|
|
|
|
pionFieldWV_ji(t,j+jj+jjj,i+ii+iii) = pionFieldWVB_ji(t,jjj,iii);
|
|
|
|
}
|
|
|
|
|
|
|
|
|
|
|
|
}}
|
|
|
|
}}
|
|
|
|
}}
|
|
|
|
|
|
|
|
double nodes=grid->NodeCount();
|
|
|
|
double tt1 = usecond();
|
|
|
|
LOG(Message) << " Contraction of PionFields took "<<(tt1-tt0)/1.0e6<< " seconds " << std::endl;
|
|
|
|
LOG(Message) << " Schur "<<(t_schur)/1.0e6<< " seconds " << std::endl;
|
|
|
|
LOG(Message) << " Contr WVmom "<<(t_contr_vwm)/1.0e6<< " seconds " << std::endl;
|
|
|
|
LOG(Message) << " Contr WV "<<(t_contr_vw)/1.0e6<< " seconds " << std::endl;
|
|
|
|
|
|
|
|
double t_kernel = t_contr_vwm;
|
|
|
|
LOG(Message) << " Arith "<<flops/(t_kernel)/1.0e3/nodes<< " Gflop/s / node " << std::endl;
|
|
|
|
LOG(Message) << " Arith "<<bytes/(t_kernel)/1.0e3/nodes<< " GB/s /node " << std::endl;
|
|
|
|
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
// Test: Build the pion correlator (two end)
|
|
|
|
// < PI_ij(t0) PI_ji (t0+t) >
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
std::vector<ComplexD> corrMom(nt,ComplexD(0.0));
|
|
|
|
|
|
|
|
for(int i=0;i<N_i;i++){
|
|
|
|
for(int j=0;j<N_j;j++){
|
|
|
|
int m=0; // first momentum
|
|
|
|
for(int t0=0;t0<nt;t0++){
|
|
|
|
for(int t=0;t<nt;t++){
|
|
|
|
int tt = (t0+t)%nt;
|
|
|
|
corrMom[t] += pionFieldWVmom_ij(m,t0,i,j)* pionFieldWVmom_ji(m,tt,j,i);
|
|
|
|
}}
|
|
|
|
}}
|
|
|
|
for(int t=0;t<nt;t++) corrMom[t] = corrMom[t]/ (double)nt;
|
|
|
|
|
|
|
|
for(int t=0;t<nt;t++) LOG(Message) << " C_vwm " << t << " " << corrMom[t]<<std::endl;
|
|
|
|
|
|
|
|
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
// Test: Build the pion correlator (two end) from zero mom contraction
|
|
|
|
// < PI_ij(t0) PI_ji (t0+t) >
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
std::vector<ComplexD> corr(nt,ComplexD(0.0));
|
|
|
|
|
|
|
|
for(int i=0;i<N_i;i++){
|
|
|
|
for(int j=0;j<N_j;j++){
|
|
|
|
for(int t0=0;t0<nt;t0++){
|
|
|
|
for(int t=0;t<nt;t++){
|
|
|
|
int tt = (t0+t)%nt;
|
|
|
|
corr[t] += pionFieldWV_ij(t0,i,j)* pionFieldWV_ji(tt,j,i);
|
|
|
|
}}
|
|
|
|
}}
|
|
|
|
for(int t=0;t<nt;t++) corr[t] = corr[t]/ (double)nt;
|
|
|
|
|
|
|
|
for(int t=0;t<nt;t++) LOG(Message) << " C_vw " << t << " " << corr[t]<<std::endl;
|
|
|
|
|
|
|
|
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
// Test: Build the pion correlator from zero mom contraction with revers
|
|
|
|
// charge flow
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
std::vector<ComplexD> corr_wwvv(nt,ComplexD(0.0));
|
|
|
|
|
|
|
|
wi.resize(N_i,grid);
|
|
|
|
vi.resize(N_i,grid);
|
|
|
|
wj.resize(N_j,grid);
|
|
|
|
vj.resize(N_j,grid);
|
|
|
|
|
|
|
|
for(int i =0;i < N_i;i++) a2a_i.return_v(i, tmp_5d, vi[i]);
|
|
|
|
for(int i =0;i < N_i;i++) a2a_i.return_w(i, tmp_5d, wi[i]);
|
|
|
|
for(int j =0;j < N_j;j++) a2a_j.return_v(j, tmp_5d, vj[j]);
|
|
|
|
for(int j =0;j < N_j;j++) a2a_j.return_w(j, tmp_5d, wj[j]);
|
|
|
|
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldWW_ij (nt,N_i,N_j);
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldVV_ji (nt,N_j,N_i);
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldWW_ji (nt,N_j,N_i);
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldVV_ij (nt,N_i,N_j);
|
|
|
|
|
|
|
|
PionFieldWW(pionFieldWW_ij, &wi[0], &wj[0],Tp);
|
|
|
|
PionFieldVV(pionFieldVV_ji, &vj[0], &vi[0],Tp);
|
|
|
|
PionFieldWW(pionFieldWW_ji, &wj[0], &wi[0],Tp);
|
|
|
|
PionFieldVV(pionFieldVV_ij, &vi[0], &vj[0],Tp);
|
|
|
|
|
|
|
|
|
|
|
|
for(int i=0;i<N_i;i++){
|
|
|
|
for(int j=0;j<N_j;j++){
|
|
|
|
for(int t0=0;t0<nt;t0++){
|
|
|
|
for(int t=0;t<nt;t++){
|
|
|
|
int tt = (t0+t)%nt;
|
|
|
|
corr_wwvv[t] += pionFieldWW_ij(t0,i,j)* pionFieldVV_ji(tt,j,i);
|
|
|
|
corr_wwvv[t] += pionFieldWW_ji(t0,j,i)* pionFieldVV_ij(tt,i,j);
|
|
|
|
}}
|
|
|
|
}}
|
|
|
|
for(int t=0;t<nt;t++) corr_wwvv[t] = corr_wwvv[t] / vol /2.0 ; // (ij+ji noise contribs if i!=j ).
|
|
|
|
|
|
|
|
for(int t=0;t<nt;t++) LOG(Message) << " C_wwvv " << t << " " << corr_wwvv[t]<<std::endl;
|
|
|
|
|
|
|
|
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
// This is only correct if there are NO low modes
|
|
|
|
// Use the "ii" case to construct possible Z wall source one end trick
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
std::vector<ComplexD> corr_z2(nt,ComplexD(0.0));
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldWW (nt,N_i,N_i);
|
|
|
|
Eigen::Tensor<ComplexD,3> pionFieldVV (nt,N_i,N_i);
|
|
|
|
|
|
|
|
|
|
|
|
PionFieldWW(pionFieldWW, &wi[0], &wi[0],Tp);
|
|
|
|
PionFieldVV(pionFieldVV, &vi[0], &vi[0],Tp);
|
|
|
|
for(int i=0;i<N_i;i++){
|
|
|
|
for(int t0=0;t0<nt;t0++){
|
|
|
|
for(int t=0;t<nt;t++){
|
|
|
|
int tt = (t0+t)%nt;
|
|
|
|
corr_z2[t] += pionFieldWW(t0,i,i) * pionFieldVV(tt,i,i) /vol ;
|
|
|
|
}}
|
|
|
|
}
|
|
|
|
|
|
|
|
LOG(Message) << " C_z2 WARNING only correct if Nl == 0 "<<std::endl;
|
|
|
|
for(int t=0;t<nt;t++) LOG(Message) << " C_z2 " << t << " " << corr_z2[t]<<std::endl;
|
|
|
|
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
// Test: Build a bag contraction
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
Eigen::Tensor<ComplexD,2> DeltaF2_fig8 (nt,16);
|
|
|
|
Eigen::Tensor<ComplexD,2> DeltaF2_trtr (nt,16);
|
|
|
|
Eigen::Tensor<ComplexD,1> denom0 (nt);
|
|
|
|
Eigen::Tensor<ComplexD,1> denom1 (nt);
|
|
|
|
|
|
|
|
const int dT=16;
|
|
|
|
|
2018-08-28 14:11:03 +01:00
|
|
|
DeltaFeq2 (dT,dT,DeltaF2_fig8,DeltaF2_trtr,
|
|
|
|
denom0,denom1,
|
|
|
|
pionFieldWW_ij,&vi[0],&vj[0],Tp);
|
|
|
|
|
|
|
|
{
|
|
|
|
int g=0; // O_{VV+AA}
|
2018-08-28 11:32:41 +01:00
|
|
|
for(int t=0;t<nt;t++)
|
|
|
|
LOG(Message) << " Bag [" << t << ","<<g<<"] "
|
|
|
|
<< (DeltaF2_fig8(t,g)+DeltaF2_trtr(t,g))
|
|
|
|
/ ( 8.0/3.0 * denom0[t]*denom1[t])
|
|
|
|
<<std::endl;
|
|
|
|
}
|
|
|
|
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
// Test: Build a bag contraction the Z2 way
|
|
|
|
// Build a wall bag comparison assuming no low modes
|
|
|
|
/////////////////////////////////////////////////////////////////////////
|
|
|
|
LOG(Message) << " Bag_z2 WARNING only correct if Nl == 0 "<<std::endl;
|
|
|
|
|
|
|
|
int t0=0;
|
|
|
|
int t1=dT;
|
|
|
|
int Nl=0;
|
|
|
|
LatticePropagator Qd0(grid);
|
|
|
|
LatticePropagator Qd1(grid);
|
|
|
|
LatticePropagator Qs0(grid);
|
|
|
|
LatticePropagator Qs1(grid);
|
|
|
|
for(int s=0;s<4;s++){
|
|
|
|
for(int c=0;c<3;c++){
|
|
|
|
int idx0 = Nl+t0*12+s*3+c;
|
|
|
|
int idx1 = Nl+t1*12+s*3+c;
|
|
|
|
FermToProp<FImpl>(Qd0, vi[idx0], s, c);
|
|
|
|
FermToProp<FImpl>(Qd1, vi[idx1], s, c);
|
|
|
|
FermToProp<FImpl>(Qs0, vj[idx0], s, c);
|
|
|
|
FermToProp<FImpl>(Qs1, vj[idx1], s, c);
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
std::vector<Gamma::Algebra> gammas ( {
|
|
|
|
Gamma::Algebra::GammaX,
|
|
|
|
Gamma::Algebra::GammaY,
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Gamma::Algebra::GammaZ,
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Gamma::Algebra::GammaT,
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Gamma::Algebra::GammaXGamma5,
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Gamma::Algebra::GammaYGamma5,
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Gamma::Algebra::GammaZGamma5,
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Gamma::Algebra::GammaTGamma5,
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Gamma::Algebra::Identity,
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Gamma::Algebra::Gamma5,
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Gamma::Algebra::SigmaXY,
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Gamma::Algebra::SigmaXZ,
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Gamma::Algebra::SigmaXT,
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Gamma::Algebra::SigmaYZ,
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Gamma::Algebra::SigmaYT,
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Gamma::Algebra::SigmaZT
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});
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auto G5 = Gamma::Algebra::Gamma5;
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LatticePropagator anti_d0 = adj( Gamma(G5) * Qd0 * Gamma(G5));
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LatticePropagator anti_d1 = adj( Gamma(G5) * Qd1 * Gamma(G5));
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LatticeComplex TR1(grid);
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LatticeComplex TR2(grid);
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LatticeComplex Wick1(grid);
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LatticeComplex Wick2(grid);
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LatticePropagator PR1(grid);
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LatticePropagator PR2(grid);
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PR1 = Qs0 * Gamma(G5) * anti_d0;
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PR2 = Qs1 * Gamma(G5) * anti_d1;
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for(int g=0;g<Nd*Nd;g++){
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auto g1 = gammas[g];
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Gamma G1 (g1);
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TR1 = trace( PR1 * G1 );
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TR2 = trace( PR2 * G1 );
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Wick1 = TR1*TR2;
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Wick2 = trace( PR1* G1 * PR2 * G1 );
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std::vector<TComplex> C1;
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std::vector<TComplex> C2;
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std::vector<TComplex> C3;
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sliceSum(Wick1,C1, Tp);
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sliceSum(Wick2,C2, Tp);
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sliceSum(TR1 ,C3, Tp);
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if(g<5){
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for(int t=0;t<C1.size();t++){
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LOG(Message) << " Wick1["<<g<<","<<t<< "] "<< C1[t]<<std::endl;
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}
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for(int t=0;t<C2.size();t++){
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LOG(Message) << " Wick2["<<g<<","<<t<< "] "<< C2[t]<<std::endl;
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}
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}
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2018-08-28 14:11:03 +01:00
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if( (g==9) || (g==7) ){ // P and At in above ordering
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2018-08-28 11:32:41 +01:00
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for(int t=0;t<C3.size();t++){
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LOG(Message) << " <G|P>["<<g<<","<<t<< "] "<< C3[t]<<std::endl;
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}
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}
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}
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}
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END_MODULE_NAMESPACE
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END_HADRONS_NAMESPACE
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#endif // Hadrons_MContraction_A2APionField_hpp_
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