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now two seperate functions for Eye and NonEye

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This commit is contained in:
Felix Erben
2019-11-26 13:44:55 +00:00
parent 421a4395af
commit 5fd5c25114
3 changed files with 57 additions and 12 deletions
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61
Grid/qcd/utils/BaryonUtils.h
View File

@@ -131,7 +131,18 @@ public:
robj &result);
public:
template <class mobj>
static void Sigma_to_Nucleon(const PropagatorField &qq_xi,
static void Sigma_to_Nucleon_Eye(const PropagatorField &qq_loop,
const mobj &Du_spec,
const PropagatorField &qd_xf,
const PropagatorField &qs_xi,
const Gamma Gamma_H,
const Gamma GammaB_sigma,
const Gamma GammaB_nucl,
const int parity,
const std::string op,
SpinMatrixField &stn_corr);
template <class mobj>
static void Sigma_to_Nucleon_NonEye(const PropagatorField &qq_xi,
const PropagatorField &qq_xf,
const mobj &Du_spec,
const PropagatorField &qd_xf,
@@ -505,10 +516,48 @@ void BaryonUtils<FImpl>::Sigma_to_Nucleon_Q2_NonEye_site(const mobj &Du_xi,
}
}
template<class FImpl>
template <class mobj>
void BaryonUtils<FImpl>::Sigma_to_Nucleon_Eye(const PropagatorField &qq_loop,
const mobj &Du_spec,
const PropagatorField &qd_xf,
const PropagatorField &qs_xi,
const Gamma Gamma_H,
const Gamma GammaB_sigma,
const Gamma GammaB_nucl,
const int parity,
const std::string op,
SpinMatrixField &stn_corr)
{
assert(parity==1 || parity == -1 && "Parity must be +1 or -1");
GridBase *grid = qs_xi.Grid();
auto vcorr= stn_corr.View();
auto vq_loop = qq_loop.View();
auto vd_xf = qd_xf.View();
auto vs_xi = qs_xi.View();
// accelerator_for(ss, grid->oSites(), grid->Nsimd(), {
thread_for(ss,grid->oSites(),{
auto Dq_loop = vq_loop[ss];
auto Dd_xf = vd_xf[ss];
auto Ds_xi = vs_xi[ss];
sobj result=Zero();
if(op == "Q1"){
Sigma_to_Nucleon_Q1_Eye_site(Dq_loop,Du_spec,Dd_xf,Ds_xi,Gamma_H,GammaB_sigma,GammaB_nucl,parity,result);
} else if(op == "Q2"){
Sigma_to_Nucleon_Q2_Eye_site(Dq_loop,Du_spec,Dd_xf,Ds_xi,Gamma_H,GammaB_sigma,GammaB_nucl,parity,result);
} else {
assert(0 && "Weak Operator not correctly specified");
}
vcorr[ss] = result;
} );//end loop over lattice sites
}
template<class FImpl>
template <class mobj>
void BaryonUtils<FImpl>::Sigma_to_Nucleon(const PropagatorField &qq_xi,
void BaryonUtils<FImpl>::Sigma_to_Nucleon_NonEye(const PropagatorField &qq_xi,
const PropagatorField &qq_xf,
const mobj &Du_spec,
const PropagatorField &qd_xf,
@@ -537,14 +586,10 @@ void BaryonUtils<FImpl>::Sigma_to_Nucleon(const PropagatorField &qq_xi,
auto Dd_xf = vd_xf[ss];
auto Ds_xi = vs_xi[ss];
sobj result=Zero();
if(op == "Q1_NonEye"){
if(op == "Q1"){
Sigma_to_Nucleon_Q1_NonEye_site(Dq_xi,Dq_xf,Du_spec,Dd_xf,Ds_xi,Gamma_H,GammaB_sigma,GammaB_nucl,parity,result);
} else if(op == "Q1_Eye"){
Sigma_to_Nucleon_Q1_Eye_site(Dq_xi,Du_spec,Dd_xf,Ds_xi,Gamma_H,GammaB_sigma,GammaB_nucl,parity,result);
} else if(op == "Q2_NonEye"){
} else if(op == "Q2"){
Sigma_to_Nucleon_Q2_NonEye_site(Dq_xi,Dq_xf,Du_spec,Dd_xf,Ds_xi,Gamma_H,GammaB_sigma,GammaB_nucl,parity,result);
} else if(op == "Q2_Eye"){
Sigma_to_Nucleon_Q2_Eye_site(Dq_xi,Du_spec,Dd_xf,Ds_xi,Gamma_H,GammaB_sigma,GammaB_nucl,parity,result);
} else {
assert(0 && "Weak Operator not correctly specified");
}

4
Hadrons/Modules/MContraction/SigmaToNucleonEye.hpp
View File

@@ -186,7 +186,7 @@ void TSigmaToNucleonEye<FImpl1, FImpl2, FImpl3, FImpl4>::execute(void)
r.info.gamma_H = G.g;
//Operator Q1, equivalent to the two-trace case in the rare-kaons module
c=Zero();
BaryonUtils<FIMPL>::Sigma_to_Nucleon(qq_loop,qq_loop,qut,qd_xf,qs_xi,G,GammaB,GammaB,parity,"Q1_Eye",c);
BaryonUtils<FIMPL>::Sigma_to_Nucleon_Eye(qq_loop,qut,qd_xf,qs_xi,G,GammaB,GammaB,parity,"Q1",c);
sliceSum(c,buf,Tp);
r.corr.clear();
for (unsigned int t = 0; t < buf.size(); ++t)
@@ -197,7 +197,7 @@ void TSigmaToNucleonEye<FImpl1, FImpl2, FImpl3, FImpl4>::execute(void)
result.push_back(r);
//Operator Q2, equivalent to the one-trace case in the rare-kaons module
c=Zero();
BaryonUtils<FIMPL>::Sigma_to_Nucleon(qq_loop,qq_loop,qut,qd_xf,qs_xi,G,GammaB,GammaB,parity,"Q2_Eye",c);
BaryonUtils<FIMPL>::Sigma_to_Nucleon_Eye(qq_loop,qut,qd_xf,qs_xi,G,GammaB,GammaB,parity,"Q2",c);
sliceSum(c,buf,Tp);
r.corr.clear();
for (unsigned int t = 0; t < buf.size(); ++t)

4
Hadrons/Modules/MContraction/SigmaToNucleonNonEye.hpp
View File

@@ -192,7 +192,7 @@ void TSigmaToNucleonNonEye<FImpl1, FImpl2, FImpl3, FImpl4>::execute(void)
r.info.gamma_H = G.g;
//Operator Q1, equivalent to the two-trace case in the rare-kaons module
c=Zero();
BaryonUtils<FIMPL>::Sigma_to_Nucleon(qu_xi,qu_xf,qut,qd_xf,qs_xi,G,GammaB,GammaB,parity,"Q1_NonEye",c);
BaryonUtils<FIMPL>::Sigma_to_Nucleon_NonEye(qu_xi,qu_xf,qut,qd_xf,qs_xi,G,GammaB,GammaB,parity,"Q1",c);
sliceSum(c,buf,Tp);
r.corr.clear();
for (unsigned int t = 0; t < buf.size(); ++t)
@@ -203,7 +203,7 @@ void TSigmaToNucleonNonEye<FImpl1, FImpl2, FImpl3, FImpl4>::execute(void)
result.push_back(r);
//Operator Q2, equivalent to the one-trace case in the rare-kaons module
c=Zero();
BaryonUtils<FIMPL>::Sigma_to_Nucleon(qu_xi,qu_xf,qut,qd_xf,qs_xi,G,GammaB,GammaB,parity,"Q2_NonEye",c);
BaryonUtils<FIMPL>::Sigma_to_Nucleon_NonEye(qu_xi,qu_xf,qut,qd_xf,qs_xi,G,GammaB,GammaB,parity,"Q2",c);
sliceSum(c,buf,Tp);
r.corr.clear();
for (unsigned int t = 0; t < buf.size(); ++t)