G4AdjointhIonisationModel.cc

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// $Id: G4AdjointhIonisationModel.cc 66892 2013-01-17 10:57:59Z gunter $
//
#include "G4AdjointhIonisationModel.hh"

#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4AdjointCSManager.hh"
#include "G4Integrator.hh"
#include "G4TrackStatus.hh"
#include "G4ParticleChange.hh"
#include "G4AdjointElectron.hh"
#include "G4AdjointProton.hh"
#include "G4AdjointInterpolator.hh"
#include "G4BetheBlochModel.hh"
#include "G4BraggModel.hh"
#include "G4Proton.hh"
#include "G4NistManager.hh"

//
G4AdjointhIonisationModel::G4AdjointhIonisationModel(G4ParticleDefinition* projectileDefinition):
  G4VEmAdjointModel("Adjoint_hIonisation")
{ 



  UseMatrix =true;
  UseMatrixPerElement = true;
  ApplyCutInRange = true;
  UseOnlyOneMatrixForAllElements = true; 
  CS_biasing_factor =1.;
  second_part_of_same_type =false;
  
  //The direct EM Modfel is taken has BetheBloch it is only used for the computation 
  // of the differential cross section.
  //The Bragg model could be used  as an alternative as  it offers the same differential cross section
  
  theDirectEMModel = new G4BetheBlochModel(projectileDefinition);
  theBraggDirectEMModel = new G4BraggModel(projectileDefinition); 
  theAdjEquivOfDirectSecondPartDef=G4AdjointElectron::AdjointElectron();
  
  theDirectPrimaryPartDef = projectileDefinition;
  theAdjEquivOfDirectPrimPartDef = 0;
  if (projectileDefinition == G4Proton::Proton()) {
    theAdjEquivOfDirectPrimPartDef = G4AdjointProton::AdjointProton();
  
  }
  
  DefineProjectileProperty();
}
//
G4AdjointhIonisationModel::~G4AdjointhIonisationModel()
{;}


//
void G4AdjointhIonisationModel::SampleSecondaries(const G4Track& aTrack,
                                G4bool IsScatProjToProjCase,
        G4ParticleChange* fParticleChange)
{ 
 if (!UseMatrix) return RapidSampleSecondaries(aTrack,IsScatProjToProjCase,fParticleChange);
 
 const G4DynamicParticle* theAdjointPrimary =aTrack.GetDynamicParticle();
  
 //Elastic inverse scattering 
 //---------------------------------------------------------
 G4double adjointPrimKinEnergy = theAdjointPrimary->GetKineticEnergy();
 G4double adjointPrimP =theAdjointPrimary->GetTotalMomentum();

 if (adjointPrimKinEnergy>HighEnergyLimit*0.999){
  return;
 }
 
 //Sample secondary energy
 //-----------------------
 G4double projectileKinEnergy = SampleAdjSecEnergyFromCSMatrix(adjointPrimKinEnergy, IsScatProjToProjCase);
 CorrectPostStepWeight(fParticleChange, 
            aTrack.GetWeight(), 
            adjointPrimKinEnergy,
            projectileKinEnergy,
            IsScatProjToProjCase); //Caution !!!this weight correction should be always applied

     
 //Kinematic: 
 //we consider a two body elastic scattering for the forward processes where the projectile knock on an e- at rest  and gives
 // him part of its  energy
 //----------------------------------------------------------------------------------------
 
 G4double projectileM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass();
 G4double projectileTotalEnergy = projectileM0+projectileKinEnergy;
 G4double projectileP2 = projectileTotalEnergy*projectileTotalEnergy - projectileM0*projectileM0; 
 
 
 
 //Companion
 //-----------
 G4double companionM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass();
 if (IsScatProjToProjCase) {
    companionM0=theAdjEquivOfDirectSecondPartDef->GetPDGMass();
 } 
 G4double companionTotalEnergy =companionM0+ projectileKinEnergy-adjointPrimKinEnergy;
 G4double companionP2 = companionTotalEnergy*companionTotalEnergy - companionM0*companionM0;  
 
 
 //Projectile momentum
 //--------------------
 G4double  P_parallel = (adjointPrimP*adjointPrimP +  projectileP2 - companionP2)/(2.*adjointPrimP);
 G4double  P_perp = std::sqrt( projectileP2 -  P_parallel*P_parallel);
 G4ThreeVector dir_parallel=theAdjointPrimary->GetMomentumDirection();
 G4double phi =G4UniformRand()*2.*3.1415926;
 G4ThreeVector projectileMomentum = G4ThreeVector(P_perp*std::cos(phi),P_perp*std::sin(phi),P_parallel);
 projectileMomentum.rotateUz(dir_parallel);
 
 
 
 if (!IsScatProjToProjCase ){ //kill the primary and add a secondary
  fParticleChange->ProposeTrackStatus(fStopAndKill);
  fParticleChange->AddSecondary(new G4DynamicParticle(theAdjEquivOfDirectPrimPartDef,projectileMomentum));
  //G4cout<<"projectileMomentum "<<projectileMomentum<<G4endl;
 }
 else {
  fParticleChange->ProposeEnergy(projectileKinEnergy);
  fParticleChange->ProposeMomentumDirection(projectileMomentum.unit());
 }  
      

  

}

//
void G4AdjointhIonisationModel::RapidSampleSecondaries(const G4Track& aTrack,
                       G4bool IsScatProjToProjCase,
                 G4ParticleChange* fParticleChange)
{ 

 const G4DynamicParticle* theAdjointPrimary =aTrack.GetDynamicParticle();
 DefineCurrentMaterial(aTrack.GetMaterialCutsCouple());
 
 
 G4double adjointPrimKinEnergy = theAdjointPrimary->GetKineticEnergy();
 G4double adjointPrimP =theAdjointPrimary->GetTotalMomentum();
 
 if (adjointPrimKinEnergy>HighEnergyLimit*0.999){
  return;
 }
  
 G4double projectileKinEnergy =0.;
 G4double eEnergy=0.;
 G4double newCS=currentMaterial->GetElectronDensity()*twopi_mc2_rcl2*mass;
 if (!IsScatProjToProjCase){//1/E^2 distribution
  
  eEnergy=adjointPrimKinEnergy;
  G4double Emax = GetSecondAdjEnergyMaxForProdToProjCase(adjointPrimKinEnergy);
        G4double Emin=  GetSecondAdjEnergyMinForProdToProjCase(adjointPrimKinEnergy);
  if (Emin>=Emax) return;
  G4double a=1./Emax;
  G4double b=1./Emin;
  newCS=newCS*(b-a)/eEnergy;
  
  projectileKinEnergy =1./(b- (b-a)*G4UniformRand()); 
  
  
 }
 else { G4double Emax = GetSecondAdjEnergyMaxForScatProjToProjCase(adjointPrimKinEnergy);
  G4double Emin = GetSecondAdjEnergyMinForScatProjToProjCase(adjointPrimKinEnergy,currentTcutForDirectSecond);
  if (Emin>=Emax) return;
  G4double diff1=Emin-adjointPrimKinEnergy;
  G4double diff2=Emax-adjointPrimKinEnergy;
  
  G4double t1=adjointPrimKinEnergy*(1./diff1-1./diff2);
  G4double t2=adjointPrimKinEnergy*(1./Emin-1./Emax);
  /*G4double f31=diff1/Emin;
  G4double f32=diff2/Emax/f31;*/
  G4double t3=2.*std::log(Emax/Emin);
  G4double sum_t=t1+t2+t3;
  newCS=newCS*sum_t/adjointPrimKinEnergy/adjointPrimKinEnergy;
  G4double t=G4UniformRand()*sum_t;
  if (t <=t1 ){
    G4double q= G4UniformRand()*t1/adjointPrimKinEnergy ;
    projectileKinEnergy =adjointPrimKinEnergy +1./(1./diff1-q);
    
  }
  else if (t <=t2 )  {
    G4double q= G4UniformRand()*t2/adjointPrimKinEnergy;
    projectileKinEnergy =1./(1./Emin-q);
  }
  else {  
    projectileKinEnergy=Emin*std::pow(Emax/Emin,G4UniformRand());
    
  }
  eEnergy=projectileKinEnergy-adjointPrimKinEnergy;
  
  
 }

 

 G4double diffCS_perAtom_Used=twopi_mc2_rcl2*mass*adjointPrimKinEnergy/projectileKinEnergy/projectileKinEnergy/eEnergy/eEnergy; 
  
  
                
 //Weight correction
 //-----------------------
 //First w_corr is set to the ratio between adjoint total CS and fwd total CS
 G4double w_corr=G4AdjointCSManager::GetAdjointCSManager()->GetPostStepWeightCorrection();
 
 //G4cout<<w_corr<<G4endl;
 w_corr*=newCS/lastCS;
 //G4cout<<w_corr<<G4endl;
 //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 numerical differentiation over Tcut of the direct CS
 
 G4double diffCS = DiffCrossSectionPerAtomPrimToSecond(projectileKinEnergy, eEnergy,1,1);
 w_corr*=diffCS/diffCS_perAtom_Used;
 //G4cout<<w_corr<<G4endl;
     
 G4double new_weight = aTrack.GetWeight()*w_corr;
 fParticleChange->SetParentWeightByProcess(false);
 fParticleChange->SetSecondaryWeightByProcess(false);
 fParticleChange->ProposeParentWeight(new_weight);
 
 
 
 
 //Kinematic: 
 //we consider a two body elastic scattering for the forward processes where the projectile knock on an e- at rest  and gives
 // him part of its  energy
 //----------------------------------------------------------------------------------------
 
 G4double projectileM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass();
 G4double projectileTotalEnergy = projectileM0+projectileKinEnergy;
 G4double projectileP2 = projectileTotalEnergy*projectileTotalEnergy - projectileM0*projectileM0; 
 
 
 
 //Companion
 //-----------
 G4double companionM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass();
 if (IsScatProjToProjCase) {
    companionM0=theAdjEquivOfDirectSecondPartDef->GetPDGMass();
 } 
 G4double companionTotalEnergy =companionM0+ projectileKinEnergy-adjointPrimKinEnergy;
 G4double companionP2 = companionTotalEnergy*companionTotalEnergy - companionM0*companionM0;  
 
 
 //Projectile momentum
 //--------------------
 G4double  P_parallel = (adjointPrimP*adjointPrimP +  projectileP2 - companionP2)/(2.*adjointPrimP);
 G4double  P_perp = std::sqrt( projectileP2 -  P_parallel*P_parallel);
 G4ThreeVector dir_parallel=theAdjointPrimary->GetMomentumDirection();
 G4double phi =G4UniformRand()*2.*3.1415926;
 G4ThreeVector projectileMomentum = G4ThreeVector(P_perp*std::cos(phi),P_perp*std::sin(phi),P_parallel);
 projectileMomentum.rotateUz(dir_parallel);
 
 
 
 if (!IsScatProjToProjCase ){ //kill the primary and add a secondary
  fParticleChange->ProposeTrackStatus(fStopAndKill);
  fParticleChange->AddSecondary(new G4DynamicParticle(theAdjEquivOfDirectPrimPartDef,projectileMomentum));
  //G4cout<<"projectileMomentum "<<projectileMomentum<<G4endl;
 }
 else {
  fParticleChange->ProposeEnergy(projectileKinEnergy);
  fParticleChange->ProposeMomentumDirection(projectileMomentum.unit());
 }  
      

 
 



} 
    
//
G4double G4AdjointhIonisationModel::DiffCrossSectionPerAtomPrimToSecond(
                                      G4double kinEnergyProj, 
                                      G4double kinEnergyProd,
              G4double Z, 
                                      G4double A)
{//Probably that here the Bragg Model should be also used for kinEnergyProj/nuc<2MeV
  

 
 G4double dSigmadEprod=0;
 G4double Emax_proj = GetSecondAdjEnergyMaxForProdToProjCase(kinEnergyProd);
 G4double Emin_proj = GetSecondAdjEnergyMinForProdToProjCase(kinEnergyProd);
 
 
 if (kinEnergyProj>Emin_proj && kinEnergyProj<=Emax_proj){ //the produced particle should have a kinetic energy smaller than the projectile 
  G4double Tmax=kinEnergyProj;
  
        G4double E1=kinEnergyProd;
  G4double E2=kinEnergyProd*1.000001;
  G4double dE=(E2-E1);
  G4double sigma1,sigma2;
  if (kinEnergyProj >2.*MeV){
      sigma1=theDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,Z,A ,E1,1.e20);
      sigma2=theDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,Z,A ,E2,1.e20);
        }
  else {
      sigma1=theBraggDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,Z,A ,E1,1.e20);
      sigma2=theBraggDirectEMModel->ComputeCrossSectionPerAtom(theDirectPrimaryPartDef,kinEnergyProj,Z,A ,E2,1.e20);
  }
  
  
  dSigmadEprod=(sigma1-sigma2)/dE;
  if (dSigmadEprod>1.) {
    G4cout<<"sigma1 "<<kinEnergyProj/MeV<<'\t'<<kinEnergyProd/MeV<<'\t'<<sigma1<<G4endl;
    G4cout<<"sigma2 "<<kinEnergyProj/MeV<<'\t'<<kinEnergyProd/MeV<<'\t'<<sigma2<<G4endl;
    G4cout<<"dsigma "<<kinEnergyProj/MeV<<'\t'<<kinEnergyProd/MeV<<'\t'<<dSigmadEprod<<G4endl;
    
  }
  
   
  
   //correction of differential cross section at high energy to correct for the suppression of particle at secondary at high
   //energy used in the Bethe Bloch Model. This correction consist to multiply by g the probability function used
   //to test the rejection of a secondary
   //-------------------------
   
   //Source code taken from    G4BetheBlochModel::SampleSecondaries
   
   G4double deltaKinEnergy = kinEnergyProd;
   
   //Part of the taken code
   //----------------------
   
   
   
   // projectile formfactor - suppresion of high energy
         // delta-electron production at high energy
   G4double x = formfact*deltaKinEnergy;
          if(x > 1.e-6) {
    
    
    G4double totEnergy     = kinEnergyProj + mass;
          G4double etot2         = totEnergy*totEnergy;
    G4double beta2 = kinEnergyProj*(kinEnergyProj + 2.0*mass)/etot2;
    G4double f;
    G4double f1 = 0.0;
    f = 1.0 - beta2*deltaKinEnergy/Tmax;
        if( 0.5 == spin ) {
            f1 = 0.5*deltaKinEnergy*deltaKinEnergy/etot2;
            f += f1;
        }
    G4double x1 = 1.0 + x;
        G4double gg  = 1.0/(x1*x1);
        if( 0.5 == spin ) {
            G4double x2 = 0.5*electron_mass_c2*deltaKinEnergy/(mass*mass);
            gg *= (1.0 + magMoment2*(x2 - f1/f)/(1.0 + x2));
        }
        if(gg > 1.0) {
            G4cout << "### G4BetheBlochModel in Adjoint Sim WARNING: g= " << g
            << G4endl;
      gg=1.;
    }
    //G4cout<<"gg"<<gg<<G4endl;
    dSigmadEprod*=gg;   
       }
   
  }

 return dSigmadEprod; 
}



//
void G4AdjointhIonisationModel::DefineProjectileProperty()
{   
    //Slightly modified code taken from G4BetheBlochModel::SetParticle
    //------------------------------------------------
    G4String pname = theDirectPrimaryPartDef->GetParticleName();
    if (theDirectPrimaryPartDef->GetParticleType() == "nucleus" &&
  pname != "deuteron" && pname != "triton") {
      isIon = true;
    }
    
    mass = theDirectPrimaryPartDef->GetPDGMass();
    mass_ratio_projectile = proton_mass_c2/theDirectPrimaryPartDef->GetPDGMass();;
    spin = theDirectPrimaryPartDef->GetPDGSpin();
    G4double q = theDirectPrimaryPartDef->GetPDGCharge()/eplus;
    chargeSquare = q*q;
    ratio = electron_mass_c2/mass;
    ratio2 = ratio*ratio;
    one_plus_ratio_2=(1+ratio)*(1+ratio);
    one_minus_ratio_2=(1-ratio)*(1-ratio);
    G4double magmom = theDirectPrimaryPartDef->GetPDGMagneticMoment()
      *mass/(0.5*eplus*hbar_Planck*c_squared);
    magMoment2 = magmom*magmom - 1.0;
    formfact = 0.0;
    if(theDirectPrimaryPartDef->GetLeptonNumber() == 0) {
      G4double x = 0.8426*GeV;
      if(spin == 0.0 && mass < GeV) {x = 0.736*GeV;}
      else if(mass > GeV) {
        x /= G4NistManager::Instance()->GetZ13(mass/proton_mass_c2);
  //  tlimit = 51.2*GeV*A13[iz]*A13[iz];
      }
      formfact = 2.0*electron_mass_c2/(x*x);
      tlimit   = 2.0/formfact;
   }
}

//
G4double G4AdjointhIonisationModel::AdjointCrossSection(const G4MaterialCutsCouple* aCouple,
                     G4double primEnergy,
                     G4bool IsScatProjToProjCase)
{ 
  if (UseMatrix) return G4VEmAdjointModel::AdjointCrossSection(aCouple,primEnergy,IsScatProjToProjCase);
  DefineCurrentMaterial(aCouple);
    
  
  G4double Cross=currentMaterial->GetElectronDensity()*twopi_mc2_rcl2*mass;
  
  if (!IsScatProjToProjCase ){
    G4double Emax_proj = GetSecondAdjEnergyMaxForProdToProjCase(primEnergy);
    G4double Emin_proj = GetSecondAdjEnergyMinForProdToProjCase(primEnergy);
  if (Emax_proj>Emin_proj && primEnergy > currentTcutForDirectSecond) {
    Cross*=(1./Emin_proj -1./Emax_proj)/primEnergy;
  } 
  else Cross=0.;
    
  

  
  
  
  }
  else {
    G4double Emax_proj = GetSecondAdjEnergyMaxForScatProjToProjCase(primEnergy);
  G4double Emin_proj = GetSecondAdjEnergyMinForScatProjToProjCase(primEnergy,currentTcutForDirectSecond);
  G4double diff1=Emin_proj-primEnergy;
  G4double diff2=Emax_proj-primEnergy;
  G4double t1=(1./diff1+1./Emin_proj-1./diff2-1./Emax_proj)/primEnergy;
  //G4double t2=2.*std::log(diff2*Emin_proj/Emax_proj/diff1)/primEnergy/primEnergy;
  G4double t2=2.*std::log(Emax_proj/Emin_proj)/primEnergy/primEnergy;
  Cross*=(t1+t2);

    
  }
  lastCS =Cross;
  return Cross; 
}
//
G4double G4AdjointhIonisationModel::GetSecondAdjEnergyMaxForScatProjToProjCase(G4double PrimAdjEnergy)
{ 
  G4double Tmax=PrimAdjEnergy*one_plus_ratio_2/(one_minus_ratio_2-2.*ratio*PrimAdjEnergy/mass);
  return Tmax;
}
//
G4double G4AdjointhIonisationModel::GetSecondAdjEnergyMinForScatProjToProjCase(G4double PrimAdjEnergy,G4double Tcut)
{ return PrimAdjEnergy+Tcut;
}
//        
G4double G4AdjointhIonisationModel::GetSecondAdjEnergyMaxForProdToProjCase(G4double )
{ return HighEnergyLimit;
}
//
G4double G4AdjointhIonisationModel::GetSecondAdjEnergyMinForProdToProjCase(G4double PrimAdjEnergy)
{  G4double Tmin= (2*PrimAdjEnergy-4*mass + std::sqrt(4.*PrimAdjEnergy*PrimAdjEnergy +16.*mass*mass + 8.*PrimAdjEnergy*mass*(1/ratio +ratio)))/4.;
   return Tmin;
}