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cc63078de5
Tested by doubling lattice in t-direction.
299 lines
11 KiB
C++
299 lines
11 KiB
C++
#ifndef GRID_QCD_FERMION_OPERATOR_H
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#define GRID_QCD_FERMION_OPERATOR_H
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namespace Grid {
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namespace QCD {
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////////////////////////////////////////////////////////////////
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// Hardwire to four spinors, allow to select
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// between gauge representation rank bc's, flavours etc.
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// and single/double precision.
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////////////////////////////////////////////////////////////////
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template<class S,int Nrepresentation=Nc>
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class WilsonImpl {
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public:
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typedef S Simd;
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template<typename vtype> using iImplSpinor = iScalar<iVector<iVector<vtype, Nrepresentation>, Ns> >;
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template<typename vtype> using iImplHalfSpinor = iScalar<iVector<iVector<vtype, Nrepresentation>, Nhs> >;
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template<typename vtype> using iImplGaugeLink = iScalar<iScalar<iMatrix<vtype, Nrepresentation> > >;
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template<typename vtype> using iImplGaugeField = iVector<iScalar<iMatrix<vtype, Nrepresentation> >, Nd >;
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template<typename vtype> using iImplDoubledGaugeField = iVector<iScalar<iMatrix<vtype, Nrepresentation> >, Nds >;
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typedef iImplSpinor <Simd> SiteSpinor;
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typedef iImplHalfSpinor<Simd> SiteHalfSpinor;
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typedef iImplGaugeLink <Simd> SiteGaugeLink;
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typedef iImplGaugeField<Simd> SiteGaugeField;
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typedef iImplDoubledGaugeField<Simd> SiteDoubledGaugeField;
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typedef Lattice<SiteSpinor> FermionField;
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typedef Lattice<SiteGaugeLink> GaugeLinkField; // bit ugly naming; polarised gauge field, lorentz... all ugly
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typedef Lattice<SiteGaugeField> GaugeField;
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typedef Lattice<SiteDoubledGaugeField> DoubledGaugeField;
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typedef WilsonCompressor<SiteHalfSpinor,SiteSpinor> Compressor;
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static inline void multLink(SiteHalfSpinor &phi,const SiteDoubledGaugeField &U,const SiteHalfSpinor &chi,int mu,StencilEntry *SE,CartesianStencil &St){
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mult(&phi(),&U(mu),&chi());
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}
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static inline void DoubleStore(GridBase *GaugeGrid,DoubledGaugeField &Uds,const GaugeField &Umu)
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{
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conformable(Uds._grid,GaugeGrid);
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conformable(Umu._grid,GaugeGrid);
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GaugeLinkField U(GaugeGrid);
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for(int mu=0;mu<Nd;mu++){
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U = PeekIndex<LorentzIndex>(Umu,mu);
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PokeIndex<LorentzIndex>(Uds,U,mu);
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U = adj(Cshift(U,mu,-1));
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PokeIndex<LorentzIndex>(Uds,U,mu+4);
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}
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}
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static inline void InsertForce(GaugeField &mat,const FermionField &Btilde,const FermionField &A,int mu){
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GaugeLinkField link(mat._grid);
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link = TraceIndex<SpinIndex>(outerProduct(Btilde,A));
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PokeIndex<LorentzIndex>(mat,link,mu);
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}
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};
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typedef WilsonImpl<vComplex,Nc> WilsonImplR; // Real.. whichever prec
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typedef WilsonImpl<vComplexF,Nc> WilsonImplF; // Float
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typedef WilsonImpl<vComplexD,Nc> WilsonImplD; // Double
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template<class S,int Nrepresentation=Nc>
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class GparityWilsonImpl {
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public:
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typedef S Simd;
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template<typename vtype> using iImplSpinor = iVector<iVector<iVector<vtype, Nrepresentation>, Ns>, Ngp >;
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template<typename vtype> using iImplHalfSpinor = iVector<iVector<iVector<vtype, Nrepresentation>, Nhs>, Ngp >;
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template<typename vtype> using iImplGaugeField = iVector<iScalar<iMatrix<vtype, Nrepresentation> >, Nd >;
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template<typename vtype> using iImplGaugeLink = iScalar<iScalar<iMatrix<vtype, Nrepresentation> > >;
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template<typename vtype> using iImplDoubledGaugeField = iVector<iVector<iScalar<iMatrix<vtype, Nrepresentation> >, Nds >, Ngp >;
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typedef iImplSpinor <Simd> SiteSpinor;
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typedef iImplHalfSpinor<Simd> SiteHalfSpinor;
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typedef iImplGaugeLink <Simd> SiteGaugeLink;
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typedef iImplGaugeField<Simd> SiteGaugeField;
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typedef iImplDoubledGaugeField<Simd> SiteDoubledGaugeField;
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typedef Lattice<SiteSpinor> FermionField;
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typedef Lattice<SiteGaugeLink> GaugeLinkField; // bit ugly naming; polarised gauge field, lorentz... all ugly
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typedef Lattice<SiteGaugeField> GaugeField;
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typedef Lattice<SiteDoubledGaugeField> DoubledGaugeField;
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// typedef GparityWilsonCompressor<SiteHalfSpinor,SiteSpinor> Compressor;
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typedef WilsonCompressor<SiteHalfSpinor,SiteSpinor> Compressor;
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// provide the multiply by link that is differentiated between Gparity (with flavour index) and
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// non-Gparity
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static inline void multLink(SiteHalfSpinor &phi,const SiteDoubledGaugeField &U,const SiteHalfSpinor &chi,int mu,StencilEntry *SE,CartesianStencil &St){
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// FIXME; need to be more careful. If this is a simd direction we are still stuffed
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// Need access to _simd_layout[mu]. mu is not necessarily dim.
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typedef SiteHalfSpinor vobj;
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typedef typename SiteHalfSpinor::scalar_object sobj;
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vobj vtmp;
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sobj stmp;
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std::vector<int> gpbc({0,0,0,1,0,0,0,1});
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GridBase *grid = St._grid;
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const int Nsimd = grid->Nsimd();
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int direction = St._directions[mu];
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int distance = St._distances[mu];
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int ptype = St._permute_type[mu];
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int sl = St._grid->_simd_layout[direction];
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// assert our assumptions
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assert((distance==1)||(distance==-1)); // nearest neighbour stencil hard code
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assert((sl==1)||(sl==2));
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std::vector<int> icoor;
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if ( SE->_around_the_world && gpbc[mu] ) {
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if ( sl == 2 ) {
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// std::cout << "multLink for mu= "<<mu<<" simd length "<<sl<<std::endl;
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std::vector<sobj> vals(Nsimd);
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extract(chi,vals);
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for(int s=0;s<Nsimd;s++){
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grid->iCoorFromIindex(icoor,s);
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assert((icoor[direction]==0)||(icoor[direction]==1));
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int permute_lane;
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if ( distance == 1) {
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permute_lane = icoor[direction]?1:0;
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} else {
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permute_lane = icoor[direction]?0:1;
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}
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if ( permute_lane ) {
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stmp(0) = vals[s](1);
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stmp(1) = vals[s](0);
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vals[s] = stmp;
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}
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}
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merge(vtmp,vals);
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} else {
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vtmp(0) = chi(1);
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vtmp(1) = chi(0);
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}
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mult(&phi(0),&U(0)(mu),&vtmp(0));
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mult(&phi(1),&U(1)(mu),&vtmp(1));
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} else {
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mult(&phi(0),&U(0)(mu),&chi(0));
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mult(&phi(1),&U(1)(mu),&chi(1));
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}
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}
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static inline void InsertForce(GaugeField &mat,const FermionField &Btilde,const FermionField &A,int mu){
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// Fixme
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return;
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}
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static inline void DoubleStore(GridBase *GaugeGrid,DoubledGaugeField &Uds,const GaugeField &Umu)
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{
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conformable(Uds._grid,GaugeGrid);
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conformable(Umu._grid,GaugeGrid);
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GaugeLinkField Utmp(GaugeGrid);
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GaugeLinkField U(GaugeGrid);
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GaugeLinkField Uconj(GaugeGrid);
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Lattice<iScalar<vInteger> > coor(GaugeGrid);
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std::vector<int> gpdirs({0,0,0,1});
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for(int mu=0;mu<Nd;mu++){
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LatticeCoordinate(coor,mu);
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U = PeekIndex<LorentzIndex>(Umu,mu);
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Uconj = conjugate(U);
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int neglink = GaugeGrid->GlobalDimensions()[mu]-1;
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if ( gpdirs[mu] ) {
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Uconj = where(coor==neglink,-Uconj,Uconj);
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}
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PARALLEL_FOR_LOOP
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for(auto ss=U.begin();ss<U.end();ss++){
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Uds[ss](0)(mu) = U[ss]();
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Uds[ss](1)(mu) = Uconj[ss]();
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}
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U = adj(Cshift(U ,mu,-1)); // correct except for spanning the boundary
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Uconj = adj(Cshift(Uconj,mu,-1));
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Utmp = U;
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if ( gpdirs[mu] ) {
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Utmp = where(coor==0,Uconj,Utmp);
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}
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PARALLEL_FOR_LOOP
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for(auto ss=U.begin();ss<U.end();ss++){
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Uds[ss](0)(mu+4) = Utmp[ss]();
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}
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Utmp = Uconj;
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if ( gpdirs[mu] ) {
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Utmp = where(coor==0,U,Utmp);
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}
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PARALLEL_FOR_LOOP
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for(auto ss=U.begin();ss<U.end();ss++){
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Uds[ss](1)(mu+4) = Utmp[ss]();
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}
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}
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}
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};
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typedef GparityWilsonImpl<vComplex,Nc> GparityWilsonImplR; // Real.. whichever prec
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typedef GparityWilsonImpl<vComplexF,Nc> GparityWilsonImplF; // Float
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typedef GparityWilsonImpl<vComplexD,Nc> GparityWilsonImplD; // Double
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//////////////////////////////////////////////////////////////////////////////
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// Four component fermions
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// Should type template the vector and gauge types
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// Think about multiple representations
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//////////////////////////////////////////////////////////////////////////////
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template<class Impl>
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class FermionOperator : public CheckerBoardedSparseMatrixBase<typename Impl::FermionField>
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{
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public:
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#include <qcd/action/fermion/FermionImplTypedefs.h>
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public:
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GridBase * Grid(void) { return FermionGrid(); }; // this is all the linalg routines need to know
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GridBase * RedBlackGrid(void) { return FermionRedBlackGrid(); };
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virtual GridBase *FermionGrid(void) =0;
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virtual GridBase *FermionRedBlackGrid(void) =0;
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virtual GridBase *GaugeGrid(void) =0;
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virtual GridBase *GaugeRedBlackGrid(void) =0;
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// override multiply
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virtual RealD M (const FermionField &in, FermionField &out)=0;
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virtual RealD Mdag (const FermionField &in, FermionField &out)=0;
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// half checkerboard operaions
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virtual void Meooe (const FermionField &in, FermionField &out)=0;
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virtual void MeooeDag (const FermionField &in, FermionField &out)=0;
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virtual void Mooee (const FermionField &in, FermionField &out)=0;
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virtual void MooeeDag (const FermionField &in, FermionField &out)=0;
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virtual void MooeeInv (const FermionField &in, FermionField &out)=0;
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virtual void MooeeInvDag (const FermionField &in, FermionField &out)=0;
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// non-hermitian hopping term; half cb or both
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virtual void Dhop (const FermionField &in, FermionField &out,int dag)=0;
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virtual void DhopOE(const FermionField &in, FermionField &out,int dag)=0;
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virtual void DhopEO(const FermionField &in, FermionField &out,int dag)=0;
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virtual void DhopDir(const FermionField &in, FermionField &out,int dir,int disp)=0; // implemented by WilsonFermion and WilsonFermion5D
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// force terms; five routines; default to Dhop on diagonal
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virtual void MDeriv (GaugeField &mat,const FermionField &U,const FermionField &V,int dag){DhopDeriv(mat,U,V,dag);};
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virtual void MoeDeriv(GaugeField &mat,const FermionField &U,const FermionField &V,int dag){DhopDerivOE(mat,U,V,dag);};
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virtual void MeoDeriv(GaugeField &mat,const FermionField &U,const FermionField &V,int dag){DhopDerivEO(mat,U,V,dag);};
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virtual void MooDeriv(GaugeField &mat,const FermionField &U,const FermionField &V,int dag){mat=zero;};
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virtual void MeeDeriv(GaugeField &mat,const FermionField &U,const FermionField &V,int dag){mat=zero;};
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virtual void DhopDeriv (GaugeField &mat,const FermionField &U,const FermionField &V,int dag)=0;
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virtual void DhopDerivEO(GaugeField &mat,const FermionField &U,const FermionField &V,int dag)=0;
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virtual void DhopDerivOE(GaugeField &mat,const FermionField &U,const FermionField &V,int dag)=0;
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virtual void Mdiag (const FermionField &in, FermionField &out) { Mooee(in,out);}; // Same as Mooee applied to both CB's
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virtual void Mdir (const FermionField &in, FermionField &out,int dir,int disp)=0; // case by case Wilson, Clover, Cayley, ContFrac, PartFrac
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///////////////////////////////////////////////
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// Updates gauge field during HMC
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///////////////////////////////////////////////
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virtual void ImportGauge(const GaugeField & _U)=0;
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};
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}
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}
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#endif
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