Import Geant4 9.2.0 source tree

This commit is contained in:
Gabriele Cosmo
2016-06-09 15:58:43 +02:00
parent 96c8bcd0af
commit b79225fb37
7544 changed files with 245407 additions and 91099 deletions
@@ -23,8 +23,8 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eeToHadronsMultiModel.cc,v 1.4 2007/05/23 08:50:41 vnivanch Exp $
// GEANT4 tag $Name: geant4-09-01 $
// $Id: G4eeToHadronsMultiModel.cc,v 1.6 2008/07/11 17:49:11 vnivanch Exp $
// GEANT4 tag $Name: geant4-09-02 $
//
// -------------------------------------------------------------------
//
@@ -33,7 +33,7 @@
//
// File name: G4eeToHadronsMultiModel
//
// Author: Vladimir Ivanchenko on base of Michel Maire code
// Author: Vladimir Ivanchenko
//
// Creation date: 02.08.2004
//
@@ -50,7 +50,12 @@
#include "G4eeToHadronsMultiModel.hh"
#include "G4eeToTwoPiModel.hh"
#include "G4eeTo3PiModel.hh"
#include "G4eeToPGammaModel.hh"
#include "G4ee2KNeutralModel.hh"
#include "G4ee2KChargedModel.hh"
#include "G4eeCrossSections.hh"
#include "G4Vee2hadrons.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
@@ -79,33 +84,116 @@ G4eeToHadronsMultiModel::~G4eeToHadronsMultiModel()
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eeToHadronsMultiModel::Initialise(const G4ParticleDefinition* p, const G4DataVector& v)
void G4eeToHadronsMultiModel::Initialise(const G4ParticleDefinition*,
const G4DataVector&)
{
if(!isInitialised) {
isInitialised = true;
thKineticEnergy = DBL_MAX;
maxKineticEnergy = HighEnergyLimit();
thKineticEnergy = DBL_MAX;
maxKineticEnergy = 1.2*GeV;
cross = new G4eeCrossSections();
G4eeToHadronsModel* model =
new G4eeToHadronsModel(new G4eeToTwoPiModel(cross), verbose);
models.push_back(model);
model->SetHighEnergyLimit(maxKineticEnergy);
model->Initialise(p, v);
G4double emin = model->LowEnergyLimit();
if(emin < thKineticEnergy) thKineticEnergy = emin;
ekinMin.push_back(emin);
ekinMax.push_back(model->HighEnergyLimit());
ekinPeak.push_back(model->PeakEnergy());
cumSum.push_back(0.0);
nModels = 1;
if(pParticleChange)
G4eeToTwoPiModel* m2pi = new G4eeToTwoPiModel(cross);
m2pi->SetHighEnergy(maxKineticEnergy);
AddEEModel(m2pi);
G4eeTo3PiModel* m3pi1 = new G4eeTo3PiModel(cross);
m3pi1->SetHighEnergy(0.95*GeV);
AddEEModel(m3pi1);
G4eeTo3PiModel* m3pi2 = new G4eeTo3PiModel(cross);
m3pi2->SetLowEnergy(0.95*GeV);
m3pi2->SetHighEnergy(maxKineticEnergy);
AddEEModel(m3pi2);
G4ee2KChargedModel* m2kc = new G4ee2KChargedModel(cross);
m2kc->SetHighEnergy(maxKineticEnergy);
AddEEModel(m2kc);
G4ee2KNeutralModel* m2kn = new G4ee2KNeutralModel(cross);
m2kn->SetHighEnergy(maxKineticEnergy);
AddEEModel(m2kn);
G4eeToPGammaModel* mpg1 = new G4eeToPGammaModel(cross,"pi0");
mpg1->SetLowEnergy(0.7*GeV);
mpg1->SetHighEnergy(maxKineticEnergy);
AddEEModel(mpg1);
G4eeToPGammaModel* mpg2 = new G4eeToPGammaModel(cross,"eta");
mpg2->SetLowEnergy(0.7*GeV);
mpg2->SetHighEnergy(maxKineticEnergy);
AddEEModel(mpg2);
nModels = models.size();
if(pParticleChange) {
fParticleChange =
reinterpret_cast<G4ParticleChangeForGamma*>(pParticleChange);
else
} else {
fParticleChange = new G4ParticleChangeForGamma();
}
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eeToHadronsMultiModel::AddEEModel(G4Vee2hadrons* mod)
{
G4eeToHadronsModel* model = new G4eeToHadronsModel(mod, verbose);
model->SetLowEnergyLimit(LowEnergyLimit());
model->SetHighEnergyLimit(HighEnergyLimit());
models.push_back(model);
G4double elow = mod->ThresholdEnergy();
ekinMin.push_back(elow);
if(thKineticEnergy > elow) thKineticEnergy = elow;
ekinMax.push_back(mod->HighEnergy());
ekinPeak.push_back(mod->PeakEnergy());
cumSum.push_back(0.0);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4eeToHadronsMultiModel::CrossSectionPerVolume(
const G4Material* mat,
const G4ParticleDefinition* p,
G4double kineticEnergy,
G4double, G4double)
{
return mat->GetElectronDensity()*
ComputeCrossSectionPerElectron(p, kineticEnergy);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4eeToHadronsMultiModel::ComputeCrossSectionPerAtom(
const G4ParticleDefinition* p,
G4double kineticEnergy,
G4double Z, G4double,
G4double, G4double)
{
return Z*ComputeCrossSectionPerElectron(p, kineticEnergy);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4eeToHadronsMultiModel::SampleSecondaries(std::vector<G4DynamicParticle*>* newp,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* dp,
G4double, G4double)
{
G4double kinEnergy = dp->GetKineticEnergy();
if (kinEnergy > thKineticEnergy) {
G4double q = cumSum[nModels-1]*G4UniformRand();
for(G4int i=0; i<nModels; i++) {
if(q <= cumSum[i]) {
(models[i])->SampleSecondaries(newp, couple,dp);
if(newp->size() > 0) fParticleChange->ProposeTrackStatus(fStopAndKill);
break;
}
}
}
}
@@ -114,8 +202,12 @@ void G4eeToHadronsMultiModel::Initialise(const G4ParticleDefinition* p, const G4
void G4eeToHadronsMultiModel::PrintInfo()
{
if(verbose > 0) {
G4cout << " e+ annihilation into hadrons active above "
<< thKineticEnergy/GeV << " GeV"
G4double e1 = 0.5*thKineticEnergy*thKineticEnergy/electron_mass_c2
- 2.0*electron_mass_c2;
G4double e2 = 0.5*maxKineticEnergy*maxKineticEnergy/electron_mass_c2
- 2.0*electron_mass_c2;
G4cout << " e+ annihilation into hadrons active from "
<< e1/GeV << " GeV to " << e2/GeV << " GeV"
<< G4endl;
}
}
@@ -127,8 +219,8 @@ void G4eeToHadronsMultiModel::SetCrossSecFactor(G4double fac)
if(fac > 1.0) {
csFactor = fac;
if(verbose > 0)
G4cout << "### G4eeToHadronsMultiModel: The cross section for G4eeToHadronsMultiModel is "
<< "increased by the Factor= " << csFactor << G4endl;
G4cout << "### G4eeToHadronsMultiModel: The cross section for G4eeToHadronsMultiModel "
<< " is increased by the Factor= " << csFactor << G4endl;
}
}