2019-09-16 17:20:54 +01:00
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/*************************************************************************************
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Grid physics library, www.github.com/paboyle/Grid
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Source file: ./tests/qdpxx/Test_qdpxx_wilson.cc
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Copyright (C) 2017
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2019-09-30 17:07:46 +01:00
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Author: Felix Erben <felix.erben@ed.ac.uk>
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2019-09-16 17:20:54 +01:00
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This program is free software; you can redistribute it and/or modify
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it under the terms of the GNU General Public License as published by
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the Free Software Foundation; either version 2 of the License, or
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(at your option) any later version.
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This program is distributed in the hope that it will be useful,
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but WITHOUT ANY WARRANTY; without even the implied warranty of
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MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
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GNU General Public License for more details.
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You should have received a copy of the GNU General Public License along
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with this program; if not, write to the Free Software Foundation, Inc.,
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51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
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See the full license in the file "LICENSE" in the top level distribution directory
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*************************************************************************************/
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/* END LEGAL */
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#include <chroma.h>
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#include <Grid/Grid.h>
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#include <Grid/qcd/utils/BaryonUtils.h>
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typedef Grid::LatticeGaugeField GaugeField;
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namespace Chroma
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{
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class ChromaWrapper
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{
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public:
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typedef multi1d<LatticeColorMatrix> U;
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typedef LatticeFermion T4;
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static void ImportGauge(GaugeField &gr,
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QDP::multi1d<QDP::LatticeColorMatrix> &ch)
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{
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Grid::LorentzColourMatrix LCM;
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Grid::Complex cc;
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QDP::ColorMatrix cm;
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QDP::Complex c;
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std::vector<int> x(4);
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QDP::multi1d<int> cx(4);
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Grid::Coordinate gd = gr.Grid()->GlobalDimensions();
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for (x[0] = 0; x[0] < gd[0]; x[0]++)
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{
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for (x[1] = 0; x[1] < gd[1]; x[1]++)
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{
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for (x[2] = 0; x[2] < gd[2]; x[2]++)
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{
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for (x[3] = 0; x[3] < gd[3]; x[3]++)
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{
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cx[0] = x[0];
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cx[1] = x[1];
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cx[2] = x[2];
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cx[3] = x[3];
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Grid::peekSite(LCM, gr, x);
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for (int mu = 0; mu < 4; mu++)
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{
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for (int i = 0; i < 3; i++)
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{
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for (int j = 0; j < 3; j++)
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{
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cc = LCM(mu)()(i, j);
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c = QDP::cmplx(QDP::Real(real(cc)), QDP::Real(imag(cc)));
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QDP::pokeColor(cm, c, i, j);
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}
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}
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QDP::pokeSite(ch[mu], cm, cx);
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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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static void ExportGauge(GaugeField &gr,
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QDP::multi1d<QDP::LatticeColorMatrix> &ch)
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{
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Grid::LorentzColourMatrix LCM;
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Grid::Complex cc;
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QDP::ColorMatrix cm;
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QDP::Complex c;
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std::vector<int> x(4);
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QDP::multi1d<int> cx(4);
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Grid::Coordinate gd = gr.Grid()->GlobalDimensions();
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for (x[0] = 0; x[0] < gd[0]; x[0]++)
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{
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for (x[1] = 0; x[1] < gd[1]; x[1]++)
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{
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for (x[2] = 0; x[2] < gd[2]; x[2]++)
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{
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for (x[3] = 0; x[3] < gd[3]; x[3]++)
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{
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cx[0] = x[0];
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cx[1] = x[1];
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cx[2] = x[2];
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cx[3] = x[3];
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for (int mu = 0; mu < 4; mu++)
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{
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for (int i = 0; i < 3; i++)
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{
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for (int j = 0; j < 3; j++)
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{
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cm = QDP::peekSite(ch[mu], cx);
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c = QDP::peekColor(cm, i, j);
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cc = Grid::Complex(toDouble(real(c)), toDouble(imag(c)));
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LCM(mu)
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()(i, j) = cc;
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}
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}
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}
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Grid::pokeSite(LCM, gr, x);
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}
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}
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}
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}
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}
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// Specific for Wilson Fermions
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static void ImportPropagator(Grid::LatticePropagator &gr,
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QDP::LatticePropagator &ch)
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{
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Grid::LatticeSpinColourVector LF(gr.Grid());
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QDP::LatticeFermion cLF;
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int Nspin=4;
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int Ncolour=3;
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for (int is = 0; is < Nspin; is++){
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for (int ic = 0; ic < Ncolour; ic++){
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Grid::PropToFerm<Grid::WilsonImplR>(LF,gr,is,ic);
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ImportFermion(LF,cLF);
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Chroma::FermToProp(cLF,ch,ic,is);
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}
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}
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}
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static void ExportPropagator(Grid::LatticePropagator &gr,
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QDP::LatticePropagator &ch)
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{
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Grid::LatticeSpinColourVector LF(gr.Grid());
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QDP::LatticeFermion cLF;
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int Nspin=4;
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int Ncolour=3;
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for (int is = 0; is < Nspin; is++){
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for (int ic = 0; ic < Ncolour; ic++){
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Chroma::PropToFerm(ch,cLF,ic,is);
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ExportFermion(LF,cLF);
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Grid::FermToProp<Grid::WilsonImplR>(gr,LF,is,ic);
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}
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}
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}
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// Specific for Wilson Fermions
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static void ImportFermion(Grid::LatticeFermion &gr,
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QDP::LatticeFermion &ch)
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{
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Grid::SpinColourVector F;
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Grid::Complex c;
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QDP::Fermion cF;
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QDP::SpinVector cS;
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QDP::Complex cc;
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std::vector<int> x(4); // explicit 4d fermions in Grid
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QDP::multi1d<int> cx(4);
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Grid::Coordinate gd = gr.Grid()->GlobalDimensions();
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for (x[0] = 0; x[0] < gd[0]; x[0]++)
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{
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for (x[1] = 0; x[1] < gd[1]; x[1]++)
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{
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for (x[2] = 0; x[2] < gd[2]; x[2]++)
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{
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for (x[3] = 0; x[3] < gd[3]; x[3]++)
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{
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cx[0] = x[0];
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cx[1] = x[1];
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cx[2] = x[2];
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cx[3] = x[3];
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Grid::peekSite(F, gr, x);
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for (int j = 0; j < 3; j++)
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{
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for (int sp = 0; sp < 4; sp++)
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{
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c = F()(sp)(j);
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cc = QDP::cmplx(QDP::Real(real(c)), QDP::Real(imag(c)));
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QDP::pokeSpin(cS, cc, sp);
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}
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QDP::pokeColor(cF, cS, j);
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}
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QDP::pokeSite(ch, cF, cx);
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}
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}
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}
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}
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}
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// Specific for 4d Wilson fermions
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static void ExportFermion(Grid::LatticeFermion &gr,
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QDP::LatticeFermion &ch)
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{
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Grid::SpinColourVector F;
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Grid::Complex c;
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QDP::Fermion cF;
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QDP::SpinVector cS;
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QDP::Complex cc;
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std::vector<int> x(4); // 4d fermions
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QDP::multi1d<int> cx(4);
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Grid::Coordinate gd = gr.Grid()->GlobalDimensions();
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for (x[0] = 0; x[0] < gd[0]; x[0]++)
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{
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for (x[1] = 0; x[1] < gd[1]; x[1]++)
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{
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for (x[2] = 0; x[2] < gd[2]; x[2]++)
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{
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for (x[3] = 0; x[3] < gd[3]; x[3]++)
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{
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cx[0] = x[0];
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cx[1] = x[1];
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cx[2] = x[2];
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cx[3] = x[3];
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cF = QDP::peekSite(ch, cx);
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for (int sp = 0; sp < 4; sp++)
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{
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for (int j = 0; j < 3; j++)
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{
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cS = QDP::peekColor(cF, j);
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cc = QDP::peekSpin(cS, sp);
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c = Grid::Complex(QDP::toDouble(QDP::real(cc)),
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QDP::toDouble(QDP::imag(cc)));
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F()
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(sp)(j) = c;
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}
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}
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Grid::pokeSite(F, gr, x);
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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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} // namespace Chroma
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void make_gauge(GaugeField &Umu, Grid::LatticePropagator &q1,Grid::LatticePropagator &q2,Grid::LatticePropagator &q3)
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{
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using namespace Grid;
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using namespace Grid::QCD;
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std::vector<int> seeds4({1, 2, 3, 4});
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Grid::GridCartesian *UGrid = (Grid::GridCartesian *)Umu.Grid();
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Grid::GridParallelRNG RNG4(UGrid);
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RNG4.SeedFixedIntegers(seeds4);
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Grid::SU3::HotConfiguration(RNG4, Umu);
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// Propagator
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Grid::gaussian(RNG4, q1);
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Grid::gaussian(RNG4, q2);
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Grid::gaussian(RNG4, q3);
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}
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void calc_chroma(GaugeField &lat, Grid::LatticePropagator &qU,Grid::LatticePropagator &qD,Grid::LatticePropagator &qS, std::vector<QDP::Complex> &res, std::string baryon)
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{
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QDP::multi1d<QDP::LatticeColorMatrix> u(4);
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Chroma::ChromaWrapper::ImportGauge(lat, u);
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QDP::LatticePropagator check;
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QDP::LatticePropagator result;
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QDP::LatticePropagator psiU;
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QDP::LatticePropagator psiD;
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QDP::LatticePropagator psiS;
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Chroma::ChromaWrapper::ImportPropagator(qU, psiU);
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Chroma::ChromaWrapper::ImportPropagator(qD, psiD);
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Chroma::ChromaWrapper::ImportPropagator(qS, psiS);
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if(0){
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std::cout << "Testing ImportPropagator(): " << std::endl;
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Grid::GridCartesian *UGrid = (Grid::GridCartesian *)lat.Grid();
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std::vector<Grid::TComplex> buf;
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Grid::LatticeComplex tmp(UGrid);
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tmp = Grid::trace(qU);
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Grid::sliceSum(tmp,buf,Grid::Nd-1);
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for (unsigned int t = 0; t < buf.size(); ++t)
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{
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std::cout << "Grid qU " << t << " " << Grid::TensorRemove(buf[t]) << std::endl;
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}
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QDP::LatticeComplex ctmp;
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ctmp = QDP::trace(psiU);
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Chroma::SftMom phases0(0,true,3); //How do I circumvent this? sliceSum equivalent?
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QDP::multi2d<DComplex> hsum0;
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hsum0 = phases0.sft(ctmp);
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for(int t = 0; t < phases0.numSubsets(); ++t){
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std::cout << "Chroma qU " << t << " " << hsum0[0][t] << std::endl;
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}
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}
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SpinMatrix C;
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SpinMatrix C_5;
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SpinMatrix C_4_5;
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SpinMatrix CG_1;
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SpinMatrix CG_2;
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SpinMatrix CG_3;
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SpinMatrix CG_4;
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SpinMatrix g_one = 1.0;
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//C = \gamma_2\gamma_4
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C = (Gamma(10)*g_one);
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//C_5 = C*gamma_5
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C_5 = (Gamma(5)*g_one);
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//C_4_5 = C*gamma_4*gamma_5
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C_4_5 = (Gamma(13)*g_one);
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//CG_1 = C*gamma_1
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CG_1 = (Gamma(11)*g_one);
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//CG_2 = C*gamma_2
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CG_2 = (Gamma(8)*g_one);
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//CG_3 = C*gamma_3
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CG_3 = (Gamma(14)*g_one);
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//CG_4 = C*gamma_4
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CG_4 = (Gamma(2)*g_one);
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// S_proj_unpol = (1/2)(1 + gamma_4)
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SpinMatrix S_proj_unpol = 0.5 * (g_one + (g_one * Gamma(8)));
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QDP::LatticeComplex b_prop;
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QDP::LatticePropagator di_quark;
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if(! baryon.compare("OmegaX")){
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// Omega_x - this esentially is degenerate (s C\gamma_1 s)s
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// C gamma_1 = Gamma(10) * Gamma(1) = Gamma(11)
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di_quark = QDP::quarkContract13(psiS * CG_1, CG_1 * psiS);
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b_prop = QDP::trace(S_proj_unpol * QDP::traceColor(psiS * QDP::traceSpin(di_quark)))
|
|
|
|
+ 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiS * di_quark));
|
|
|
|
} else if (! baryon.compare("OmegaY")){
|
|
|
|
// Omega_x - this esentially is degenerate (s C\gamma_3 s)s
|
|
|
|
// C gamma_1 = Gamma(10) * Gamma(2) = Gamma(8)
|
|
|
|
di_quark = QDP::quarkContract13(psiS * CG_2, CG_2 * psiS);
|
|
|
|
b_prop = QDP::trace(S_proj_unpol * QDP::traceColor(psiS * QDP::traceSpin(di_quark)))
|
|
|
|
+ 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiS * di_quark));
|
|
|
|
} else if (! baryon.compare("OmegaZ")){
|
|
|
|
// Omega_x - this esentially is degenerate (s C\gamma_3 s)s
|
|
|
|
// C gamma_1 = Gamma(10) * Gamma(4) = Gamma(14)
|
|
|
|
di_quark = QDP::quarkContract13(psiS * CG_3, CG_3 * psiS);
|
|
|
|
b_prop = QDP::trace(S_proj_unpol * QDP::traceColor(psiS * QDP::traceSpin(di_quark)))
|
|
|
|
+ 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiS * di_quark));
|
|
|
|
} else if (! baryon.compare("Proton")){
|
|
|
|
// Proton - this esentially is degenerate (d C\gamma_5 u)u
|
|
|
|
// This is how the UKHadron code is written - diquarks are swapped when compared to coment above code.
|
|
|
|
//di_quark = QDP::quarkContract13(psiU * C_5, C_5 * psiD);
|
|
|
|
di_quark = QDP::quarkContract13(psiD * C_5, C_5 * psiU);
|
|
|
|
b_prop = QDP::trace(S_proj_unpol * QDP::traceColor(psiU * QDP::traceSpin(di_quark)))
|
|
|
|
+ QDP::trace(S_proj_unpol * QDP::traceColor(psiU * di_quark));
|
|
|
|
} else if (! baryon.compare("Lambda")){
|
|
|
|
// Lambda (octet) - This is the totally antisymmetric
|
|
|
|
// one from the middle of the octet
|
|
|
|
// Lambda - (d C\gamma_5 s)u - (u C\gamma_5 s)d
|
|
|
|
// This is given by:
|
|
|
|
// 1/3[ <us>d + <ds>u + 4<ud>s - (usd) - (dsu) + 2(sud) + 2(sdu) + 2(uds) + 2(dus) ]
|
|
|
|
|
|
|
|
/* This is how the UKHadron code is written - diquarks are swapped when compared to coments above code.
|
|
|
|
// This gives <us>d - (usd) -- yes
|
|
|
|
di_quark = QDP::quarkContract13(psiU * C_5, C_5 * psiS);
|
|
|
|
b_prop = QDP::trace(S_proj_unpol * QDP::traceColor(psiD * QDP::traceSpin(di_quark)))
|
|
|
|
- QDP::trace(S_proj_unpol * QDP::traceColor(psiD * di_quark));
|
|
|
|
|
|
|
|
// This gives <ds>u - (dsu) -- yes
|
|
|
|
di_quark = quarkContract13(psiD * C_5,C_5 * psiS);
|
|
|
|
b_prop += QDP::trace(S_proj_unpol * QDP::traceColor(psiU * QDP::traceSpin(di_quark)))
|
|
|
|
- QDP::trace(S_proj_unpol * QDP::traceColor(psiU * di_quark));
|
|
|
|
|
|
|
|
// This gives 4<ud>s -- yes
|
|
|
|
di_quark = quarkContract13(psiU * C_5,C_5 * psiD);
|
|
|
|
b_prop += 4.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiS * QDP::traceSpin(di_quark)));
|
|
|
|
|
|
|
|
//This gives 2(sud) -- yes
|
|
|
|
di_quark = quarkContract13(psiS * C_5,C_5 * psiU);
|
|
|
|
b_prop += 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiD * di_quark));
|
|
|
|
|
|
|
|
// This gives 2(sdu) -- yes
|
|
|
|
di_quark = quarkContract13(psiS * C_5,C_5 * psiD);
|
|
|
|
b_prop += 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiU * di_quark));
|
|
|
|
|
|
|
|
// This gives 2(uds) -- yes
|
|
|
|
di_quark = quarkContract13(psiU * C_5,C_5 * psiD);
|
|
|
|
b_prop += 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiS * di_quark));
|
|
|
|
|
|
|
|
// This gives 2(dus) -- yes
|
|
|
|
di_quark = quarkContract13(psiD * C_5,C_5 * psiU);
|
|
|
|
b_prop += 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiS * di_quark));*/
|
|
|
|
|
|
|
|
// This gives <us>d - (usd) -- yes
|
|
|
|
di_quark = QDP::quarkContract13(psiS * C_5, C_5 * psiU);
|
|
|
|
b_prop = QDP::trace(S_proj_unpol * QDP::traceColor(psiD * QDP::traceSpin(di_quark)))
|
|
|
|
- QDP::trace(S_proj_unpol * QDP::traceColor(psiD * di_quark));
|
|
|
|
|
|
|
|
// This gives <ds>u - (dsu) -- yes
|
|
|
|
di_quark = quarkContract13(psiS * C_5,C_5 * psiD);
|
|
|
|
b_prop += QDP::trace(S_proj_unpol * QDP::traceColor(psiU * QDP::traceSpin(di_quark)))
|
|
|
|
- QDP::trace(S_proj_unpol * QDP::traceColor(psiU * di_quark));
|
|
|
|
|
|
|
|
// This gives 4<ud>s -- yes
|
|
|
|
di_quark = quarkContract13(psiD * C_5,C_5 * psiU);
|
|
|
|
b_prop += 4.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiS * QDP::traceSpin(di_quark)));
|
|
|
|
|
|
|
|
//This gives 2(sud) -- yes
|
|
|
|
di_quark = quarkContract13(psiU * C_5,C_5 * psiS);
|
|
|
|
b_prop += 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiD * di_quark));
|
|
|
|
|
|
|
|
// This gives 2(sdu) -- yes
|
|
|
|
di_quark = quarkContract13(psiD * C_5,C_5 * psiS);
|
|
|
|
b_prop += 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiU * di_quark));
|
|
|
|
|
|
|
|
// This gives 2(uds) -- yes
|
|
|
|
di_quark = quarkContract13(psiD * C_5,C_5 * psiU);
|
|
|
|
b_prop += 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiS * di_quark));
|
|
|
|
|
|
|
|
// This gives 2(dus) -- yes
|
|
|
|
di_quark = quarkContract13(psiU * C_5,C_5 * psiD);
|
|
|
|
b_prop += 2.0 * QDP::trace(S_proj_unpol * QDP::traceColor(psiS * di_quark));
|
|
|
|
} else {
|
|
|
|
std::cout << "baryon not part of test " << std::endl;
|
|
|
|
return;
|
|
|
|
}
|
|
|
|
std::cout<< "Chroma computing " << baryon << std::endl;
|
|
|
|
|
|
|
|
Chroma::SftMom phases(0,true,3); //How do I circumvent this? sliceSum equivalent?
|
|
|
|
QDP::multi2d<DComplex> hsum;
|
|
|
|
hsum = phases.sft(b_prop);
|
|
|
|
int length = phases.numSubsets();
|
|
|
|
res.resize(length);
|
|
|
|
for(int t = 0; t < length; ++t){
|
|
|
|
res[t] = hsum[0][t]; //Should I test momentum?
|
|
|
|
}
|
|
|
|
|
|
|
|
}
|
|
|
|
|
|
|
|
|
|
|
|
void calc_grid(Grid::LatticeGaugeField &Umu, Grid::LatticePropagator &qU, Grid::LatticePropagator &qD, Grid::LatticePropagator &qS, std::vector<Grid::Complex> &res, std::string baryon)
|
|
|
|
{
|
|
|
|
using namespace Grid;
|
|
|
|
using namespace Grid::QCD;
|
|
|
|
|
|
|
|
Grid::GridCartesian *UGrid = (Grid::GridCartesian *)Umu.Grid();
|
|
|
|
|
|
|
|
Grid::Gamma G_A = Grid::Gamma(Grid::Gamma::Algebra::Identity);
|
|
|
|
Grid::Gamma G_B = Grid::Gamma(Grid::Gamma::Algebra::GammaZGamma5); // OmegaX: C*GammaX = i* GammaZ*Gamma5
|
|
|
|
|
|
|
|
Grid::LatticeComplex c(UGrid);
|
|
|
|
Grid::LatticeComplex c1(UGrid);
|
|
|
|
|
|
|
|
if(! baryon.compare("OmegaX")){
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qS,qS,qS,G_A,G_B,G_A,G_B,"sss","sss",1,c);
|
2019-09-16 17:20:54 +01:00
|
|
|
c*=0.5;
|
|
|
|
std::cout << "Grid-Omega factor 2 larger than Chroma-Omega!!!" << std::endl;
|
|
|
|
} else if (! baryon.compare("OmegaY")){
|
|
|
|
G_B = Grid::Gamma(Grid::Gamma::Algebra::GammaT);
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qS,qS,qS,G_A,G_B,G_A,G_B,"sss","sss",1,c);
|
2019-09-16 17:20:54 +01:00
|
|
|
c*=0.5;
|
|
|
|
std::cout << "Grid-Omega factor 2 larger than Chroma-Omega!!!" << std::endl;
|
|
|
|
} else if (! baryon.compare("OmegaZ")){
|
|
|
|
G_B = Grid::Gamma(Grid::Gamma::Algebra::GammaXGamma5);
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qS,qS,qS,G_A,G_B,G_A,G_B,"sss","sss",1,c);
|
2019-09-16 17:20:54 +01:00
|
|
|
c*=0.5;
|
|
|
|
std::cout << "Grid-Omega factor 2 larger than Chroma-Omega!!!" << std::endl;
|
|
|
|
} else if (! baryon.compare("Proton")){
|
|
|
|
G_B = Grid::Gamma(Grid::Gamma::Algebra::SigmaXZ);
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qU,qD,qU,G_A,G_B,G_A,G_B,"udu","udu",1,c);
|
2019-09-16 17:20:54 +01:00
|
|
|
std::cout << "UKHadron-Proton has flipped diquarks in original code." << std::endl;
|
|
|
|
} else if (! baryon.compare("Lambda")){
|
|
|
|
G_B = Grid::Gamma(Grid::Gamma::Algebra::SigmaXZ);
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qS,qU,qD,G_A,G_B,G_A,G_B,"sud","sud",1,c1); //<ud>s
|
2019-09-16 17:20:54 +01:00
|
|
|
c = 4.*c1;
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qD,qU,qS,G_A,G_B,G_A,G_B,"dus","dus",1,c1); //<us>d
|
2019-09-16 17:20:54 +01:00
|
|
|
c += c1;
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qU,qD,qS,G_A,G_B,G_A,G_B,"uds","uds",1,c1); //<ds>u
|
2019-09-16 17:20:54 +01:00
|
|
|
c += c1;
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qD,qU,qS,G_A,G_B,G_A,G_B,"dus","sud",1,c1); //(sud)
|
2019-09-16 17:20:54 +01:00
|
|
|
c += 2.*c1;
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qU,qD,qS,G_A,G_B,G_A,G_B,"uds","sud",1,c1); //(sdu)
|
2019-09-16 17:20:54 +01:00
|
|
|
c -= 2.*c1;
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qS,qU,qD,G_A,G_B,G_A,G_B,"sud","dus",1,c1); //(dus)
|
2019-09-16 17:20:54 +01:00
|
|
|
c += 2.*c1;
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qU,qD,qS,G_A,G_B,G_A,G_B,"uds","dus",1,c1); //-(dsu)
|
2019-09-16 17:20:54 +01:00
|
|
|
c -= c1;
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qS,qU,qD,G_A,G_B,G_A,G_B,"sud","uds",1,c1); //(uds)
|
2019-09-16 17:20:54 +01:00
|
|
|
c -= 2.*c1;
|
2019-10-09 14:52:33 +01:00
|
|
|
BaryonUtils<Grid::WilsonImplR>::ContractBaryons(qD,qU,qS,G_A,G_B,G_A,G_B,"dus","uds",1,c1); //-(usd)
|
2019-09-16 17:20:54 +01:00
|
|
|
c -= c1;
|
|
|
|
std::cout << "UKHadron-Lambda has flipped diquarks in original code." << std::endl;
|
|
|
|
} else {
|
|
|
|
std::cout << "baryon not part of test " << std::endl;
|
|
|
|
return;
|
|
|
|
}
|
|
|
|
std::cout<< "Grid computing " << baryon << std::endl;
|
|
|
|
|
|
|
|
std::vector<Grid::TComplex> buf;
|
|
|
|
Grid::sliceSum(c,buf,Grid::Nd-1);
|
|
|
|
res.resize(buf.size());
|
|
|
|
for (unsigned int t = 0; t < buf.size(); ++t)
|
|
|
|
{
|
|
|
|
res[t]=Grid::TensorRemove(buf[t]);
|
|
|
|
}
|
|
|
|
|
|
|
|
}
|
|
|
|
|
|
|
|
int main(int argc, char **argv)
|
|
|
|
{
|
|
|
|
|
|
|
|
/********************************************************
|
|
|
|
* Setup QDP
|
|
|
|
*********************************************************/
|
|
|
|
Chroma::initialize(&argc, &argv);
|
|
|
|
Chroma::WilsonTypeFermActs4DEnv::registerAll();
|
|
|
|
|
|
|
|
/********************************************************
|
|
|
|
* Setup Grid
|
|
|
|
*********************************************************/
|
|
|
|
Grid::Grid_init(&argc, &argv);
|
|
|
|
Grid::GridCartesian *UGrid = Grid::SpaceTimeGrid::makeFourDimGrid(Grid::GridDefaultLatt(),
|
|
|
|
Grid::GridDefaultSimd(Grid::Nd, Grid::vComplex::Nsimd()),
|
|
|
|
Grid::GridDefaultMpi());
|
|
|
|
|
|
|
|
Grid::Coordinate gd = UGrid->GlobalDimensions();
|
|
|
|
QDP::multi1d<int> nrow(QDP::Nd);
|
|
|
|
for (int mu = 0; mu < 4; mu++)
|
|
|
|
nrow[mu] = gd[mu];
|
|
|
|
|
|
|
|
QDP::Layout::setLattSize(nrow);
|
|
|
|
QDP::Layout::create();
|
|
|
|
|
|
|
|
GaugeField Ug(UGrid);
|
|
|
|
typedef Grid::LatticePropagator PropagatorField;
|
|
|
|
PropagatorField up(UGrid);
|
|
|
|
PropagatorField down(UGrid);
|
|
|
|
PropagatorField strange(UGrid);
|
|
|
|
std::vector<ComplexD> res_chroma;
|
|
|
|
std::vector<Grid::Complex> res_grid;
|
2019-10-10 11:07:20 +01:00
|
|
|
Grid::Complex res_chroma_g;
|
2019-09-16 17:20:54 +01:00
|
|
|
|
|
|
|
std::vector<std::string> baryons({"OmegaX","OmegaY","OmegaZ","Proton","Lambda"});
|
|
|
|
int nBaryon=baryons.size();
|
|
|
|
|
|
|
|
for (int iB = 0; iB < nBaryon; iB++)
|
|
|
|
{
|
|
|
|
make_gauge(Ug, up, down, strange); // fills the gauge field and the propagator with random numbers
|
|
|
|
|
|
|
|
calc_chroma(Ug, up, down, strange, res_chroma,baryons[iB]);
|
|
|
|
|
|
|
|
for(int t=0;t<res_chroma.size();t++){
|
|
|
|
std::cout << " Chroma baryon "<<t<<" "<< res_chroma[t] << std::endl;
|
|
|
|
}
|
|
|
|
|
|
|
|
calc_grid(Ug, up, down, strange, res_grid,baryons[iB]);
|
|
|
|
|
|
|
|
for(int t=0;t<res_chroma.size();t++){
|
|
|
|
std::cout << " Grid baryon "<<t<<" "<< res_grid[t] << std::endl;
|
|
|
|
}
|
2019-10-10 11:07:20 +01:00
|
|
|
for(int t=0;t<res_chroma.size();t++){
|
|
|
|
res_chroma_g = Grid::Complex(toDouble(real(res_chroma[t])), toDouble(imag(res_chroma[t])));
|
|
|
|
std::cout << " Difference "<<t<<" "<< res_chroma_g - res_grid[t] << std::endl;
|
|
|
|
}
|
2019-09-16 17:20:54 +01:00
|
|
|
|
|
|
|
std::cout << "Finished test " << std::endl;
|
|
|
|
|
|
|
|
}
|
|
|
|
Chroma::finalize();
|
|
|
|
}
|