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changed some naming conditions to resemble rare-kaons

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ferben
2019-12-05 16:56:54 +00:00
parent 1a5e562bde
commit 58b6a0d8d1
2 changed files with 47 additions and 47 deletions
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48
Hadrons/Modules/MContraction/SigmaToNucleonNonEye.hpp
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@ -44,7 +44,7 @@ BEGIN_HADRONS_NAMESPACE
* Sigma-to-Nucleon 3-pt diagrams, non-eye topologies.
*
* Schematic:
* qs_xi qu_xf | qs_xi qd_xf
* qsTi quTf | qsTi qdTf
* /-->--¬ /-->--¬ | /-->--¬ /-->--¬
* / \ / \ | / \ / \
* / \ / \ | / \ / \
@ -54,22 +54,22 @@ BEGIN_HADRONS_NAMESPACE
* | \ / \ /| | | \ / \ / |
* | \ / \ / | | | \ / \ / |
* | \ / \ / | | | \-->--/ \-->--/ |
* \ \-->--/ \-->--/ / | \ qu_xi qu_xf /
* \ qu_xi qd_xf / | \ /
* \ \-->--/ \-->--/ / | \ quTi quTf /
* \ quTi qdTf / | \ /
* \ / | \ /
* \--------->----------/ | \--------->-----------/
* qu_spec | qu_spec
* quSpec | quSpec
*
*
* analogously to the rare-kaon naming, the left diagram is named 'one-trace' and
* the diagram on the right 'two-trace'
*
* Propagators:
* * qu_xi, source at xi
* * qu_xf, source at xf
* * qu_spec, source at xi
* * qd_xf, source at xf
* * qs_xi, source at xi
* * quTi, source at ti
* * quTf, source at tf
* * quSpec, source at ti
* * qdTf, source at tf
* * qsTi, source at ti
*/
BEGIN_MODULE_NAMESPACE(MContraction)
@ -77,12 +77,12 @@ class SigmaToNucleonNonEyePar: Serializable
{
public:
GRID_SERIALIZABLE_CLASS_MEMBERS(SigmaToNucleonNonEyePar,
std::string, qu_xi,
std::string, qu_xf,
std::string, qu_spec,
std::string, qd_xf,
std::string, qs_xi,
unsigned int, xf,
std::string, quTi,
std::string, quTf,
std::string, quSpec,
std::string, qdTf,
std::string, qsTi,
unsigned int, tf,
std::string, sink,
std::string, output);
};
@ -139,7 +139,7 @@ TSigmaToNucleonNonEye<FImpl>::TSigmaToNucleonNonEye(const std::string name)
template <typename FImpl>
std::vector<std::string> TSigmaToNucleonNonEye<FImpl>::getInput(void)
{
std::vector<std::string> input = {par().qu_xi, par().qu_xf, par().qu_spec, par().qd_xf, par().qs_xi, par().sink};
std::vector<std::string> input = {par().quTi, par().quTf, par().quSpec, par().qdTf, par().qsTi, par().sink};
return input;
}
@ -180,18 +180,18 @@ void TSigmaToNucleonNonEye<FImpl>::execute(void)
r.info.gammaA_nucl = Id.g;
r.info.gammaB_nucl = GammaB.g;
auto &qu_xi = envGet(PropagatorField, par().qu_xi);
auto &qu_xf = envGet(PropagatorField, par().qu_xf);
auto &qu_spec = envGet(SlicedPropagator, par().qu_spec);
auto &qd_xf = envGet(PropagatorField, par().qd_xf);
auto &qs_xi = envGet(PropagatorField, par().qs_xi);
auto qut = qu_spec[par().xf];
auto &quTi = envGet(PropagatorField, par().quTi);
auto &quTf = envGet(PropagatorField, par().quTf);
auto &quSpec = envGet(SlicedPropagator, par().quSpec);
auto &qdTf = envGet(PropagatorField, par().qdTf);
auto &qsTi = envGet(PropagatorField, par().qsTi);
auto qut = quSpec[par().tf];
for (auto &G: Gamma::gall)
{
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_NonEye(qu_xi,qu_xf,qut,qd_xf,qs_xi,G,GammaB,GammaB,"Q1",c);
BaryonUtils<FIMPL>::Sigma_to_Nucleon_NonEye(quTi,quTf,qut,qdTf,qsTi,G,GammaB,GammaB,"Q1",c);
sliceSum(c,buf,Tp);
r.corr.clear();
for (unsigned int t = 0; t < buf.size(); ++t)
@ -202,7 +202,7 @@ void TSigmaToNucleonNonEye<FImpl>::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_NonEye(qu_xi,qu_xf,qut,qd_xf,qs_xi,G,GammaB,GammaB,"Q2",c);
BaryonUtils<FIMPL>::Sigma_to_Nucleon_NonEye(quTi,quTf,qut,qdTf,qsTi,G,GammaB,GammaB,"Q2",c);
sliceSum(c,buf,Tp);
r.corr.clear();
for (unsigned int t = 0; t < buf.size(); ++t)