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This commit is contained in:
Gabriele Cosmo
2016-06-08 15:55:53 +02:00
parent e7d7193284
commit cfcb558cfe
3050 changed files with 91703 additions and 48310 deletions
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source/processes/hadronic/models/generator/de_excitation/include/G4AlphaCoulombBarrier.hh
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// and all its terms.
//
// $Id: G4AlphaCoulombBarrier.hh,v 1.1 2000/06/09 11:36:49 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Dec 1999)
source/processes/hadronic/models/generator/de_excitation/include/G4CoulombBarrier.hh
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// and all its terms.
//
// $Id: G4CoulombBarrier.hh,v 1.1 2000/06/09 11:36:52 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Dec 1999)
source/processes/hadronic/models/generator/de_excitation/include/G4DeuteronCoulombBarrier.hh
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// and all its terms.
//
// $Id: G4DeuteronCoulombBarrier.hh,v 1.1 2000/06/09 11:36:52 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Dec 1999)
source/processes/hadronic/models/generator/de_excitation/include/G4ExcitationHandler.hh
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// and all its terms.
//
// $Id: G4ExcitationHandler.hh,v 1.4 1999/12/15 14:52:15 gunter Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (May 1998)
source/processes/hadronic/models/generator/de_excitation/include/G4FissionBarrier.hh
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// and all its terms.
//
// $Id: G4FissionBarrier.hh,v 1.3 2000/06/09 11:36:52 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Oct 1998)
source/processes/hadronic/models/generator/de_excitation/include/G4He3CoulombBarrier.hh
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@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4He3CoulombBarrier.hh,v 1.1 2000/06/09 11:36:53 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Dec 1999)
source/processes/hadronic/models/generator/de_excitation/include/G4NeutronCoulombBarrier.hh
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@@ -6,7 +6,7 @@
// and all its terms.
//
// $Id: G4NeutronCoulombBarrier.hh,v 1.1 2000/06/09 11:36:53 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Dec 1999)
source/processes/hadronic/models/generator/de_excitation/include/G4ParaFissionModel.hh
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#ifndef G4ParaFissionModel_h
#define G4ParaFissionModel_h
#include "G4CompetitiveFission.hh"
#include "G4ExcitationHandler.hh"
#include "G4HadronicInteraction.hh"
#include "G4ParticleTable.hh"
// Class Description
// Final state production model for (based on evaluated data
// libraries) description of neutron induced fission below 60 MeV;
// In case you need the fission fragments, use this model.
// To be used in your physics list in case you need this physics.
// In this case you want to register an object of this class with
// the corresponding process.
// Class Description - End
class G4ParaFissionModel : public G4HadronicInteraction
{
public:
G4ParaFissionModel()
{
SetMinEnergy( 0.0 );
SetMaxEnergy( 60.*MeV );
}
virtual G4VParticleChange* ApplyYourself(const G4Track& aTrack,
G4Nucleus& theNucleus)
{
theParticleChange.Initialize(aTrack);
theParticleChange.SetStatusChange( fStopAndKill );
theParticleChange.SetEnergyChange( 0.0 );
// prepare the fragment
G4Fragment anInitialState;
G4int anA=theNucleus.GetN();
G4int aZ=theNucleus.GetZ();
G4double nucMass = G4ParticleTable::GetParticleTable()->GetIonTable()->GetIonMass(aZ ,anA);
anA += aTrack.GetDynamicParticle()->GetDefinition()->GetBaryonNumber();
aZ += aTrack.GetDynamicParticle()->GetDefinition()->GetPDGCharge();
G4int numberOfEx = aTrack.GetDynamicParticle()->GetDefinition()->GetBaryonNumber();
G4int numberOfCh = abs(aTrack.GetDynamicParticle()->GetDefinition()->GetPDGCharge());
G4int numberOfHoles = 0;
G4double exEnergy = 0;
G4ThreeVector exciton3Momentum = aTrack.GetMomentum();
G4double compoundMass = aTrack.GetTotalEnergy();
compoundMass += nucMass;
compoundMass = sqrt(compoundMass*compoundMass - exciton3Momentum*exciton3Momentum);
G4LorentzVector fragment4Momentum(exciton3Momentum,
sqrt(exciton3Momentum.mag2()+compoundMass*compoundMass));
anInitialState.SetA(anA);
anInitialState.SetZ(aZ);
anInitialState.SetNumberOfCharged(numberOfCh);
anInitialState.SetNumberOfHoles(numberOfHoles);
anInitialState.SetNumberOfExcitons(numberOfEx);
anInitialState.SetMomentum(fragment4Momentum);
// do the fission
G4FragmentVector * theFissionResult = theFission.BreakUp(anInitialState);
// deexcite the fission fragments and fill result
vector<G4DynamicParticle *> theResult;
G4int ll = theFissionResult->length();
for(G4int i=0; i<ll; i++)
{
G4ReactionProductVector * theExcitationResult = 0;
if(theFissionResult->at(i)->GetExcitationEnergy()>1.*eV)
{
G4Fragment * aFragment = theFissionResult->at(i);
G4double exenergy = aFragment->GetExcitationEnergy();
theExcitationResult = theHandler.BreakItUp(*(theFissionResult->at(i)));
// add secondaries
for(G4int j=0; j<theExcitationResult->length(); j++)
{
G4DynamicParticle* p0 = new G4DynamicParticle;
p0->SetDefinition( theExcitationResult->at(j)->GetDefinition() );
p0->SetMomentum( theExcitationResult->at(j)->GetMomentum() );
theResult.push_back(p0);
}
}
else
{
// add secondary
G4DynamicParticle* p0 = new G4DynamicParticle;
p0->SetDefinition(theFissionResult->at(i)->GetParticleDefinition());
p0->SetMomentum(theFissionResult->at(i)->GetMomentum().vect());
theResult.push_back(p0);
}
}
// fill particle change
for(G4int k=0; k<theResult.size(); k++)
{
theParticleChange.AddSecondary(theResult[k]);
}
// return
return &theParticleChange;
}
private:
G4CompetitiveFission theFission;
G4ExcitationHandler theHandler;
G4ParticleChange theParticleChange;
};
#endif
source/processes/hadronic/models/generator/de_excitation/include/G4ProtonCoulombBarrier.hh
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// and all its terms.
//
// $Id: G4ProtonCoulombBarrier.hh,v 1.1 2000/06/09 11:36:53 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Dec 1999)
source/processes/hadronic/models/generator/de_excitation/include/G4TritonCoulombBarrier.hh
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// and all its terms.
//
// $Id: G4TritonCoulombBarrier.hh,v 1.1 2000/06/09 11:36:53 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Dec 1999)
source/processes/hadronic/models/generator/de_excitation/include/G4VCoulombBarrier.hh
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// and all its terms.
//
// $Id: G4VCoulombBarrier.hh,v 1.1 2000/06/09 11:36:54 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Nov 1999)
source/processes/hadronic/models/generator/de_excitation/include/G4VFissionBarrier.hh
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// and all its terms.
//
// $Id: G4VFissionBarrier.hh,v 1.3 2000/06/09 11:36:54 larazb Exp $
// GEANT4 tag $Name: geant4-02-00 $
// GEANT4 tag $Name: geant4-03-00 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Oct 1998)