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geant4/source/processes/hadronic/models/theo_high_energy/src/G4QuasiElasticChannel.cc
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2020-06-26 10:23:25 +02:00

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//
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//
// Author : Gunter Folger March 2007
// Modified by Mikhail Kossov. Apr2009, E/M conservation: ResidualNucleus is added (ResNuc)
// Class Description
// Final state production model for theoretical models of hadron inelastic
// quasi elastic scattering in geant4;
// Class Description - End
//
// Modified:
// 20110805 M. Kelsey -- Follow change to G4V3DNucleus::GetNucleons()
// 20110808 M. Kelsey -- Move #includes from .hh, add many missing
#include "G4QuasiElasticChannel.hh"
#include "G4Fancy3DNucleus.hh"
#include "G4DynamicParticle.hh"
#include "G4HadTmpUtil.hh" /* lrint */
#include "G4KineticTrack.hh"
#include "G4KineticTrackVector.hh"
#include "G4LorentzVector.hh"
#include "G4Neutron.hh"
#include "G4Nucleon.hh"
#include "G4Nucleus.hh"
#include "G4ParticleDefinition.hh"
#include "G4ParticleTable.hh"
#include "G4IonTable.hh"
#include "G4QuasiElRatios.hh"
#include "globals.hh"
#include <vector>
//#define debug_scatter
G4QuasiElasticChannel::G4QuasiElasticChannel()
: G4HadronicInteraction("QuasiElastic"),
theQuasiElastic(new G4QuasiElRatios),
the3DNucleus(new G4Fancy3DNucleus) {
}
G4QuasiElasticChannel::~G4QuasiElasticChannel()
{
delete the3DNucleus;
delete theQuasiElastic;
}
G4double G4QuasiElasticChannel::GetFraction(G4Nucleus &theNucleus,
const G4DynamicParticle & thePrimary)
{
#ifdef debug_scatter
G4cout << "G4QuasiElasticChannel:: P=" << thePrimary.GetTotalMomentum()
<< ", pPDG=" << thePrimary.GetDefinition()->GetPDGEncoding()
<< ", Z = " << theNucleus.GetZ_asInt())
<< ", N = " << theNucleus.GetN_asInt())
<< ", A = " << theNucleus.GetA_asInt() << G4endl;
#endif
std::pair<G4double,G4double> ratios;
ratios=theQuasiElastic->GetRatios(thePrimary.GetTotalMomentum(),
thePrimary.GetDefinition()->GetPDGEncoding(),
theNucleus.GetZ_asInt(),
theNucleus.GetN_asInt());
#ifdef debug_scatter
G4cout << "G4QuasiElasticChannel::ratios " << ratios.first << " x " <<ratios.second
<< " = " << ratios.first*ratios.second << G4endl;
#endif
return ratios.first*ratios.second;
}
G4KineticTrackVector * G4QuasiElasticChannel::Scatter(G4Nucleus &theNucleus,
const G4DynamicParticle & thePrimary)
{
G4int A=theNucleus.GetA_asInt();
G4int Z=theNucleus.GetZ_asInt();
// build Nucleus and choose random nucleon to scatter with
the3DNucleus->Init(theNucleus.GetA_asInt(),theNucleus.GetZ_asInt());
const std::vector<G4Nucleon>& nucleons=the3DNucleus->GetNucleons();
G4double targetNucleusMass=the3DNucleus->GetMass();
G4LorentzVector targetNucleus4Mom(0.,0.,0.,targetNucleusMass);
G4int index;
do {
index=G4lrint((A-1)*G4UniformRand());
} while (index < 0 || index >= static_cast<G4int>(nucleons.size())); /* Loop checking, 07.08.2015, A.Ribon */
const G4ParticleDefinition * pDef= nucleons[index].GetDefinition();
G4int resA=A - 1;
G4int resZ=Z - static_cast<int>(pDef->GetPDGCharge());
const G4ParticleDefinition* resDef;
G4double residualNucleusMass;
if(resZ)
{
resDef=G4ParticleTable::GetParticleTable()->GetIonTable()->GetIon(resZ,resA,0);
residualNucleusMass=resDef->GetPDGMass();
}
else {
resDef=G4Neutron::Neutron();
residualNucleusMass=resA * G4Neutron::Neutron()->GetPDGMass();
}
#ifdef debug_scatter
G4cout<<"G4QElChan::Scatter: neutron - proton? A ="<<A<<", Z="<<Z<<", projName="
<<pDef->GetParticleName()<<G4endl;
#endif
G4LorentzVector pNucleon=nucleons[index].Get4Momentum();
G4double residualNucleusEnergy=std::sqrt(sqr(residualNucleusMass) +
pNucleon.vect().mag2());
pNucleon.setE(targetNucleusMass-residualNucleusEnergy);
G4LorentzVector residualNucleus4Mom=targetNucleus4Mom-pNucleon;
std::pair<G4LorentzVector,G4LorentzVector> result;
result=theQuasiElastic->Scatter(pDef->GetPDGEncoding(),pNucleon,
thePrimary.GetDefinition()->GetPDGEncoding(),
thePrimary.Get4Momentum());
G4LorentzVector scatteredHadron4Mom;
if (result.first.e() > 0.)
scatteredHadron4Mom=result.second;
else { //scatter failed
//G4cout << "Warning - G4QuasiElasticChannel::Scatter no scattering" << G4endl;
//return 0; //no scatter
scatteredHadron4Mom=thePrimary.Get4Momentum();
residualNucleus4Mom=G4LorentzVector(0.,0.,0.,targetNucleusMass);
resDef=G4ParticleTable::GetParticleTable()->GetIonTable()->GetIon(Z,A,0);
}
#ifdef debug_scatter
G4LorentzVector EpConservation=pNucleon+thePrimary.Get4Momentum()
- result.first - result.second;
if ( (EpConservation.vect().mag2() > .01*MeV*MeV )
|| (std::abs(EpConservation.e()) > 0.1 * MeV ) )
{
G4cout << "Warning - G4QuasiElasticChannel::Scatter E-p non conservation : "
<< EpConservation << G4endl;
}
#endif
G4KineticTrackVector * ktv = new G4KineticTrackVector();
G4KineticTrack * sPrim=new G4KineticTrack(thePrimary.GetDefinition(),
0.,G4ThreeVector(0), scatteredHadron4Mom);
ktv->push_back(sPrim);
if (result.first.e() > 0.)
{
G4KineticTrack * sNuc=new G4KineticTrack(pDef, 0.,G4ThreeVector(0), result.first);
ktv->push_back(sNuc);
}
if(resZ || resA==1) // For the only neutron or for tnuclei with Z>0
{
G4KineticTrack * rNuc=new G4KineticTrack(resDef,
0.,G4ThreeVector(0), residualNucleus4Mom);
ktv->push_back(rNuc);
}
else // The residual nucleus consists of only neutrons
{
residualNucleus4Mom/=resA; // Split 4-mom of A*n system equally
for(G4int in=0; in<resA; in++) // Loop over neutrons in A*n system.
{
G4KineticTrack* rNuc=new G4KineticTrack(resDef,
0.,G4ThreeVector(0), residualNucleus4Mom);
ktv->push_back(rNuc);
}
}
#ifdef debug_scatter
G4cout<<"G4QElC::Scat: Nucleon: "<<result.first <<" mass "<<result.first.mag() << G4endl;
G4cout<<"G4QElC::Scat: Project: "<<result.second<<" mass "<<result.second.mag()<< G4endl;
#endif
return ktv;
}