G4AdjointBremsstrahlungModel.cc

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#include "G4AdjointBremsstrahlungModel.hh"
#include "G4AdjointCSManager.hh"
 
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
 
#include "G4Integrator.hh"
#include "G4TrackStatus.hh"
#include "G4ParticleChange.hh"
#include "G4AdjointElectron.hh"
#include "G4AdjointGamma.hh"
#include "G4Electron.hh"
#include "G4Timer.hh"
#include "G4SeltzerBergerModel.hh"
 
 
////////////////////////////////////////////////////////////////////////////////
//
G4AdjointBremsstrahlungModel::G4AdjointBremsstrahlungModel(G4VEmModel* aModel):
 G4VEmAdjointModel("AdjointeBremModel")
{ 
  SetUseMatrix(false);
  SetUseMatrixPerElement(false);
  
  theDirectStdBremModel = aModel;
  theDirectEMModel=theDirectStdBremModel;
  theEmModelManagerForFwdModels = new G4EmModelManager();
  isDirectModelInitialised = false;
  G4VEmFluctuationModel* f=0;
  G4Region* r=0;
  theEmModelManagerForFwdModels->AddEmModel(1, theDirectStdBremModel, f, r);
 
  SetApplyCutInRange(true);
  highKinEnergy= 1.*GeV;
  lowKinEnergy = 1.0*keV;
 
  lastCZ =0.;
 
  
  theAdjEquivOfDirectPrimPartDef =G4AdjointElectron::AdjointElectron();
  theAdjEquivOfDirectSecondPartDef=G4AdjointGamma::AdjointGamma();
  theDirectPrimaryPartDef=G4Electron::Electron();
  second_part_of_same_type=false;
 
  
  CS_biasing_factor =1.;
 
  
}
////////////////////////////////////////////////////////////////////////////////
//
G4AdjointBremsstrahlungModel::G4AdjointBremsstrahlungModel():
 G4VEmAdjointModel("AdjointeBremModel")
{
  SetUseMatrix(false);
  SetUseMatrixPerElement(false);
 
  theDirectStdBremModel = new G4SeltzerBergerModel();
  theDirectEMModel=theDirectStdBremModel;
  theEmModelManagerForFwdModels = new G4EmModelManager();
  isDirectModelInitialised = false;
  G4VEmFluctuationModel* f=0;
  G4Region* r=0;
  theEmModelManagerForFwdModels->AddEmModel(1, theDirectStdBremModel, f, r);
 // theDirectPenelopeBremModel =0;
  SetApplyCutInRange(true);
  highKinEnergy= 1.*GeV;
  lowKinEnergy = 1.0*keV;
  lastCZ =0.;
  theAdjEquivOfDirectPrimPartDef =G4AdjointElectron::AdjointElectron();
  theAdjEquivOfDirectSecondPartDef=G4AdjointGamma::AdjointGamma();
  theDirectPrimaryPartDef=G4Electron::Electron();
  second_part_of_same_type=false;
}
////////////////////////////////////////////////////////////////////////////////
//
G4AdjointBremsstrahlungModel::~G4AdjointBremsstrahlungModel()
{if (theDirectStdBremModel) delete theDirectStdBremModel;
 if (theEmModelManagerForFwdModels) delete theEmModelManagerForFwdModels;
}
 
////////////////////////////////////////////////////////////////////////////////
//
void G4AdjointBremsstrahlungModel::SampleSecondaries(const G4Track& aTrack,
                       G4bool IsScatProjToProjCase,
                   G4ParticleChange* fParticleChange)
{
 if (!UseMatrix) return RapidSampleSecondaries(aTrack,IsScatProjToProjCase,fParticleChange); 
 
 const G4DynamicParticle* theAdjointPrimary =aTrack.GetDynamicParticle();
 DefineCurrentMaterial(aTrack.GetMaterialCutsCouple());
 
 
 G4double adjointPrimKinEnergy = theAdjointPrimary->GetKineticEnergy();
 G4double adjointPrimTotalEnergy = theAdjointPrimary->GetTotalEnergy();
 
 if (adjointPrimKinEnergy>HighEnergyLimit*0.999){
    return;
 }
  
  G4double projectileKinEnergy = SampleAdjSecEnergyFromCSMatrix(adjointPrimKinEnergy,
                            IsScatProjToProjCase);
 //Weight correction
 //-----------------------                     
 CorrectPostStepWeight(fParticleChange, 
               aTrack.GetWeight(), 
               adjointPrimKinEnergy,
               projectileKinEnergy,
               IsScatProjToProjCase);   
 
 
 //Kinematic
 //---------
 G4double projectileM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass();
 G4double projectileTotalEnergy = projectileM0+projectileKinEnergy;
 G4double projectileP2 = projectileTotalEnergy*projectileTotalEnergy - projectileM0*projectileM0;   
 G4double projectileP = std::sqrt(projectileP2);
 
 
 //Angle of the gamma direction with the projectile taken from G4eBremsstrahlungModel
 //------------------------------------------------
  G4double u;
  const G4double a1 = 0.625 , a2 = 3.*a1 , d = 27. ;
 
  if (9./(9.+d) > G4UniformRand()) u = - std::log(G4UniformRand()*G4UniformRand())/a1;
     else                          u = - std::log(G4UniformRand()*G4UniformRand())/a2;
 
  G4double theta = u*electron_mass_c2/projectileTotalEnergy;
 
  G4double sint = std::sin(theta);
  G4double cost = std::cos(theta);
 
  G4double phi = twopi * G4UniformRand() ;
  
  G4ThreeVector projectileMomentum;
  projectileMomentum=G4ThreeVector(std::cos(phi)*sint,std::sin(phi)*sint,cost)*projectileP; //gamma frame
  if (IsScatProjToProjCase) {//the adjoint primary is the scattered e-
    G4ThreeVector gammaMomentum = (projectileTotalEnergy-adjointPrimTotalEnergy)*G4ThreeVector(0.,0.,1.);
    G4ThreeVector dirProd=projectileMomentum-gammaMomentum;
    G4double cost1 = std::cos(dirProd.angle(projectileMomentum));
    G4double sint1 =  std::sqrt(1.-cost1*cost1);
    projectileMomentum=G4ThreeVector(std::cos(phi)*sint1,std::sin(phi)*sint1,cost1)*projectileP;
  
  }
  
  projectileMomentum.rotateUz(theAdjointPrimary->GetMomentumDirection());
 
 
 
  if (!IsScatProjToProjCase ){ //kill the primary and add a secondary
    fParticleChange->ProposeTrackStatus(fStopAndKill);
    fParticleChange->AddSecondary(new G4DynamicParticle(theAdjEquivOfDirectPrimPartDef,projectileMomentum));
  }
  else {
    fParticleChange->ProposeEnergy(projectileKinEnergy);
    fParticleChange->ProposeMomentumDirection(projectileMomentum.unit());
    
  } 
} 
////////////////////////////////////////////////////////////////////////////////
//
void G4AdjointBremsstrahlungModel::RapidSampleSecondaries(const G4Track& aTrack,
                       G4bool IsScatProjToProjCase,
                   G4ParticleChange* fParticleChange)
{ 
 
 const G4DynamicParticle* theAdjointPrimary =aTrack.GetDynamicParticle();
 DefineCurrentMaterial(aTrack.GetMaterialCutsCouple());
 
 
 G4double adjointPrimKinEnergy = theAdjointPrimary->GetKineticEnergy();
 G4double adjointPrimTotalEnergy = theAdjointPrimary->GetTotalEnergy();
 
 if (adjointPrimKinEnergy>HighEnergyLimit*0.999){
    return;
 }
  
 G4double projectileKinEnergy =0.;
 G4double gammaEnergy=0.;
 G4double diffCSUsed=0.; 
 if (!IsScatProjToProjCase){
    gammaEnergy=adjointPrimKinEnergy;
    G4double Emax = GetSecondAdjEnergyMaxForProdToProjCase(adjointPrimKinEnergy);
        G4double Emin=  GetSecondAdjEnergyMinForProdToProjCase(adjointPrimKinEnergy);;
    if (Emin>=Emax) return;
    projectileKinEnergy=Emin*std::pow(Emax/Emin,G4UniformRand());
    diffCSUsed=CS_biasing_factor*lastCZ/projectileKinEnergy;
    
 }
 else { G4double Emax = GetSecondAdjEnergyMaxForScatProjToProjCase(adjointPrimKinEnergy);
    G4double Emin = GetSecondAdjEnergyMinForScatProjToProjCase(adjointPrimKinEnergy,currentTcutForDirectSecond);
    if (Emin>=Emax) return;
    G4double f1=(Emin-adjointPrimKinEnergy)/Emin;
    G4double f2=(Emax-adjointPrimKinEnergy)/Emax/f1;
    projectileKinEnergy=adjointPrimKinEnergy/(1.-f1*std::pow(f2,G4UniformRand()));
    gammaEnergy=projectileKinEnergy-adjointPrimKinEnergy;
    diffCSUsed=lastCZ*adjointPrimKinEnergy/projectileKinEnergy/gammaEnergy;
    
 }
  
  
  
                            
 //Weight correction
 //-----------------------
 //First w_corr is set to the ratio between adjoint total CS and fwd total CS
 //if this has to be done in the model
 //For the case of forced interaction this will be done in the PostStepDoIt of the
 //forced interaction
 //It is important to set the weight before the vreation of the  secondary
 //
 G4double w_corr=additional_weight_correction_factor_for_post_step_outside_model;
 if (correct_weight_for_post_step_in_model) {
     w_corr=G4AdjointCSManager::GetAdjointCSManager()->GetPostStepWeightCorrection();
 }
 //G4cout<<"Correction factor start in brem model "<<w_corr<<std::endl;
 
 
 //Then another correction is needed due to the fact that a biaised differential CS has been used rather than the one consistent with the direct model
 //Here we consider the true  diffCS as the one obtained by the numericla differentiation over Tcut of the direct CS, corrected by the Migdal term.
 //Basically any other differential CS   diffCS could be used here (example Penelope). 
 
 G4double diffCS = DiffCrossSectionPerVolumePrimToSecond(currentMaterial, projectileKinEnergy, gammaEnergy);
 /*G4cout<<"diffCS "<<diffCS <<std::endl;
 G4cout<<"diffCS_Used "<<diffCSUsed <<std::endl;*/
 w_corr*=diffCS/diffCSUsed;
 
 
 G4double new_weight = aTrack.GetWeight()*w_corr;
 /*G4cout<<"New weight brem "<<new_weight<<std::endl;
 G4cout<<"Weight correction brem "<<w_corr<<std::endl;*/
 fParticleChange->SetParentWeightByProcess(false);
 fParticleChange->SetSecondaryWeightByProcess(false);
 fParticleChange->ProposeParentWeight(new_weight);
 
 //Kinematic
 //---------
 G4double projectileM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass();
 G4double projectileTotalEnergy = projectileM0+projectileKinEnergy;
 G4double projectileP2 = projectileTotalEnergy*projectileTotalEnergy - projectileM0*projectileM0;   
 G4double projectileP = std::sqrt(projectileP2);
 
 
 //Use the angular model of the forward model to generate the gamma direction
 //---------------------------------------------------------------------------
//Dum dynamic particle to use the model
 G4DynamicParticle * aDynPart = new G4DynamicParticle(G4Electron::Electron(),G4ThreeVector(0.,0.,1.)*projectileP);
 
 //Get the element from the direct model
 const G4Element* elm = theDirectEMModel->SelectRandomAtom(currentCouple,G4Electron::Electron(),
                                                        projectileKinEnergy,currentTcutForDirectSecond);
 G4int Z=elm->GetZasInt();
 G4double energy = aDynPart->GetTotalEnergy()-gammaEnergy;
 G4ThreeVector projectileMomentum =
   theDirectEMModel->GetAngularDistribution()->SampleDirection(aDynPart,energy,Z,currentMaterial)*projectileP;
  G4double phi = projectileMomentum.getPhi();
 
/*
 //Angle of the gamma direction with the projectile taken from G4eBremsstrahlungModel
 //------------------------------------------------
  G4double u;
  const G4double a1 = 0.625 , a2 = 3.*a1 , d = 27. ;
 
  if (9./(9.+d) > G4UniformRand()) u = - std::log(G4UniformRand()*G4UniformRand())/a1;
     else                          u = - std::log(G4UniformRand()*G4UniformRand())/a2;
 
  G4double theta = u*electron_mass_c2/projectileTotalEnergy;
 
  G4double sint = std::sin(theta);
  G4double cost = std::cos(theta);
 
  G4double phi = twopi * G4UniformRand() ;
  G4ThreeVector projectileMomentum;
  projectileMomentum=G4ThreeVector(std::cos(phi)*sint,std::sin(phi)*sint,cost)*projectileP; //gamma frame
*/
  if (IsScatProjToProjCase) {//the adjoint primary is the scattered e-
    G4ThreeVector gammaMomentum = (projectileTotalEnergy-adjointPrimTotalEnergy)*G4ThreeVector(0.,0.,1.);
    G4ThreeVector dirProd=projectileMomentum-gammaMomentum;
    G4double cost1 = std::cos(dirProd.angle(projectileMomentum));
    G4double sint1 =  std::sqrt(1.-cost1*cost1);
    projectileMomentum=G4ThreeVector(std::cos(phi)*sint1,std::sin(phi)*sint1,cost1)*projectileP;
  }
 
  projectileMomentum.rotateUz(theAdjointPrimary->GetMomentumDirection());
 
  if (!IsScatProjToProjCase ){ //kill the primary and add a secondary
    fParticleChange->ProposeTrackStatus(fStopAndKill);
    fParticleChange->AddSecondary(new G4DynamicParticle(theAdjEquivOfDirectPrimPartDef,projectileMomentum));
  }
  else {
    fParticleChange->ProposeEnergy(projectileKinEnergy);
    fParticleChange->ProposeMomentumDirection(projectileMomentum.unit());
  } 
} 
////////////////////////////////////////////////////////////////////////////////
//
G4double G4AdjointBremsstrahlungModel::DiffCrossSectionPerVolumePrimToSecond(const G4Material* aMaterial,
                                      G4double kinEnergyProj,  // kinetic energy of the primary particle before the interaction 
                                      G4double kinEnergyProd // kinetic energy of the secondary particle 
                      )
{if (!isDirectModelInitialised) {
    theEmModelManagerForFwdModels->Initialise(G4Electron::Electron(),G4Gamma::Gamma(),1.,0);
    isDirectModelInitialised =true;
 }
/*
 return  DiffCrossSectionPerVolumePrimToSecondApproximated2(aMaterial,
                                                         kinEnergyProj, 
                                                         kinEnergyProd);
*/
return G4VEmAdjointModel::DiffCrossSectionPerVolumePrimToSecond(aMaterial,
                                                         kinEnergyProj, 
                                                         kinEnergyProd);                                                                 
}                     
 
////////////////////////////////////////////////////////////////////////////////
//
G4double G4AdjointBremsstrahlungModel::DiffCrossSectionPerVolumePrimToSecondApproximated1(
                      const G4Material* aMaterial,
                                      G4double kinEnergyProj,  // kinetic energy of the primary particle before the interaction 
                                      G4double kinEnergyProd // kinetic energy of the secondary particle 
                      )
{
 G4double dCrossEprod=0.;
 G4double Emax_proj = GetSecondAdjEnergyMaxForProdToProjCase(kinEnergyProd);
 G4double Emin_proj = GetSecondAdjEnergyMinForProdToProjCase(kinEnergyProd);
 
 
 //In this approximation we consider that the secondary gammas are sampled with 1/Egamma energy distribution
 //This is what is applied in the discrete standard model before the  rejection test  that make a correction
 //The application of the same rejection function is not possible here.
 //The differentiation of the CS over Ecut does not produce neither a good differential CS. That is due to the 
 // fact that in the discrete model the differential CS and the integrated CS are both fitted but separatly and 
 // therefore do not allow a correct numerical differentiation of the integrated CS to get the differential one. 
 // In the future we plan to use the brem secondary spectra from the G4Penelope implementation 
 
 if (kinEnergyProj>Emin_proj && kinEnergyProj<=Emax_proj){
    G4double sigma=theDirectEMModel->CrossSectionPerVolume(aMaterial,theDirectPrimaryPartDef,kinEnergyProj,1.*keV);
    dCrossEprod=sigma/kinEnergyProd/std::log(kinEnergyProj/keV);
 }
 return dCrossEprod;
  
}
 
////////////////////////////////////////////////////////////////////////////////
//
G4double G4AdjointBremsstrahlungModel::DiffCrossSectionPerVolumePrimToSecondApproximated2(
                      const G4Material* material,
                                      G4double kinEnergyProj,  // kinetic energy of the primary particle before the interaction 
                                      G4double kinEnergyProd // kinetic energy of the secondary particle 
                      )
{
 //In this approximation we derive the direct cross section over Tcut=gamma energy, en after apply the Migdla correction factor 
  //used in the direct model
 
 G4double dCrossEprod=0.;
 
 const G4ElementVector* theElementVector = material->GetElementVector();
 const double* theAtomNumDensityVector = material->GetAtomicNumDensityVector();
 G4double dum=0.;
 G4double E1=kinEnergyProd,E2=kinEnergyProd*1.001;
 G4double dE=E2-E1;
 for (size_t i=0; i<material->GetNumberOfElements(); i++) { 
    G4double C1=theDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,(*theElementVector)[i]->GetZ(),dum ,E1);
    G4double C2=theDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,(*theElementVector)[i]->GetZ(),dum,E2);
    dCrossEprod += theAtomNumDensityVector[i] * (C1-C2)/dE;
 }
 
 return dCrossEprod;
  
}
////////////////////////////////////////////////////////////////////////////////
//
G4double G4AdjointBremsstrahlungModel::AdjointCrossSection(const G4MaterialCutsCouple* aCouple,
                             G4double primEnergy,
                             G4bool IsScatProjToProjCase)
{ if (!isDirectModelInitialised) {
    theEmModelManagerForFwdModels->Initialise(G4Electron::Electron(),G4Gamma::Gamma(),1.,0);
    isDirectModelInitialised =true;
  }
  if (UseMatrix) return G4VEmAdjointModel::AdjointCrossSection(aCouple,primEnergy,IsScatProjToProjCase);
  DefineCurrentMaterial(aCouple);
  G4double Cross=0.;
  lastCZ=theDirectEMModel->CrossSectionPerVolume(aCouple->GetMaterial(),theDirectPrimaryPartDef,100.*MeV,100.*MeV/std::exp(1.));//this give the constant above
  
  if (!IsScatProjToProjCase ){
    G4double Emax_proj = GetSecondAdjEnergyMaxForProdToProjCase(primEnergy);
    G4double Emin_proj = GetSecondAdjEnergyMinForProdToProjCase(primEnergy);
    if (Emax_proj>Emin_proj && primEnergy > currentTcutForDirectSecond) Cross= CS_biasing_factor*lastCZ*std::log(Emax_proj/Emin_proj);
  }
  else {
    G4double Emax_proj = GetSecondAdjEnergyMaxForScatProjToProjCase(primEnergy);
    G4double Emin_proj = GetSecondAdjEnergyMinForScatProjToProjCase(primEnergy,currentTcutForDirectSecond);
    if (Emax_proj>Emin_proj) Cross= lastCZ*std::log((Emax_proj-primEnergy)*Emin_proj/Emax_proj/(Emin_proj-primEnergy));
    
  }
  return Cross; 
}                        
 
G4double G4AdjointBremsstrahlungModel::GetAdjointCrossSection(const G4MaterialCutsCouple* aCouple,
                             G4double primEnergy,
                             G4bool IsScatProjToProjCase)
{ 
  return AdjointCrossSection(aCouple, primEnergy,IsScatProjToProjCase);
  lastCZ=theDirectEMModel->CrossSectionPerVolume(aCouple->GetMaterial(),theDirectPrimaryPartDef,100.*MeV,100.*MeV/std::exp(1.));//this give the constant above
  return G4VEmAdjointModel::GetAdjointCrossSection(aCouple, primEnergy,IsScatProjToProjCase);
    
}