#include <G4LowEPComptonModel.hh>

Inheritance diagram for G4LowEPComptonModel:

Public Member Functions
	G4LowEPComptonModel (const G4ParticleDefinition *p=0, const G4String &nam="LowEPComptonModel")

virtual	~G4LowEPComptonModel ()

virtual void	Initialise (const G4ParticleDefinition *, const G4DataVector &)

virtual G4double	ComputeCrossSectionPerAtom (const G4ParticleDefinition *, G4double kinEnergy, G4double Z, G4double A=0, G4double cut=0, G4double emax=DBL_MAX)

virtual void	SampleSecondaries (std::vector< G4DynamicParticle * > , const G4MaterialCutsCouple , const G4DynamicParticle *, G4double tmin, G4double maxEnergy)

Public Member Functions inherited from G4VEmModel
	G4VEmModel (const G4String &nam)

virtual	~G4VEmModel ()

virtual void	Initialise (const G4ParticleDefinition *, const G4DataVector &)=0

virtual void	SampleSecondaries (std::vector< G4DynamicParticle * > , const G4MaterialCutsCouple , const G4DynamicParticle *, G4double tmin=0.0, G4double tmax=DBL_MAX)=0

virtual G4double	ComputeDEDXPerVolume (const G4Material , const G4ParticleDefinition , G4double kineticEnergy, G4double cutEnergy=DBL_MAX)

virtual G4double	CrossSectionPerVolume (const G4Material , const G4ParticleDefinition , G4double kineticEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)

virtual G4double	ComputeCrossSectionPerAtom (const G4ParticleDefinition *, G4double kinEnergy, G4double Z, G4double A=0., G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)

virtual G4double	ChargeSquareRatio (const G4Track &)

virtual G4double	GetChargeSquareRatio (const G4ParticleDefinition , const G4Material , G4double kineticEnergy)

virtual G4double	GetParticleCharge (const G4ParticleDefinition , const G4Material , G4double kineticEnergy)

virtual void	StartTracking (G4Track *)

virtual void	CorrectionsAlongStep (const G4MaterialCutsCouple , const G4DynamicParticle , G4double &eloss, G4double &niel, G4double length)

virtual G4double	Value (const G4MaterialCutsCouple , const G4ParticleDefinition , G4double kineticEnergy)

virtual G4double	MinPrimaryEnergy (const G4Material , const G4ParticleDefinition )

virtual void	SetupForMaterial (const G4ParticleDefinition , const G4Material , G4double kineticEnergy)

virtual void	DefineForRegion (const G4Region *)

void	InitialiseElementSelectors (const G4ParticleDefinition *, const G4DataVector &)

G4double	ComputeDEDX (const G4MaterialCutsCouple , const G4ParticleDefinition , G4double kineticEnergy, G4double cutEnergy=DBL_MAX)

G4double	CrossSection (const G4MaterialCutsCouple , const G4ParticleDefinition , G4double kineticEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)

G4double	ComputeMeanFreePath (const G4ParticleDefinition , G4double kineticEnergy, const G4Material , G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)

G4double	ComputeCrossSectionPerAtom (const G4ParticleDefinition , const G4Element , G4double kinEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)

G4int	SelectIsotopeNumber (const G4Element *)

const G4Element *	SelectRandomAtom (const G4MaterialCutsCouple , const G4ParticleDefinition , G4double kineticEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)

const G4Element *	SelectRandomAtom (const G4Material , const G4ParticleDefinition , G4double kineticEnergy, G4double cutEnergy=0.0, G4double maxEnergy=DBL_MAX)

void	SetParticleChange (G4VParticleChange , G4VEmFluctuationModel f=0)

void	SetCrossSectionTable (G4PhysicsTable *)

G4PhysicsTable *	GetCrossSectionTable ()

G4VEmFluctuationModel *	GetModelOfFluctuations ()

G4VEmAngularDistribution *	GetAngularDistribution ()

void	SetAngularDistribution (G4VEmAngularDistribution *)

G4double	HighEnergyLimit () const

G4double	LowEnergyLimit () const

G4double	HighEnergyActivationLimit () const

G4double	LowEnergyActivationLimit () const

G4double	PolarAngleLimit () const

G4double	SecondaryThreshold () const

G4bool	LPMFlag () const

G4bool	DeexcitationFlag () const

G4bool	ForceBuildTableFlag () const

void	SetHighEnergyLimit (G4double)

void	SetLowEnergyLimit (G4double)

void	SetActivationHighEnergyLimit (G4double)

void	SetActivationLowEnergyLimit (G4double)

G4bool	IsActive (G4double kinEnergy)

void	SetPolarAngleLimit (G4double)

void	SetSecondaryThreshold (G4double)

void	SetLPMFlag (G4bool val)

void	SetDeexcitationFlag (G4bool val)

void	ForceBuildTable (G4bool val)

G4double	MaxSecondaryKinEnergy (const G4DynamicParticle *dynParticle)

const G4String &	GetName () const

void	SetCurrentCouple (const G4MaterialCutsCouple *)

const G4Element *	GetCurrentElement () const

Protected Attributes
G4ParticleChangeForGamma *	fParticleChange

Protected Attributes inherited from G4VEmModel
G4VParticleChange *	pParticleChange

G4PhysicsTable *	xSectionTable

const std::vector< G4double > *	theDensityFactor

const std::vector< G4int > *	theDensityIdx

Additional Inherited Members
Protected Member Functions inherited from G4VEmModel
G4ParticleChangeForLoss *	GetParticleChangeForLoss ()

G4ParticleChangeForGamma *	GetParticleChangeForGamma ()

virtual G4double	MaxSecondaryEnergy (const G4ParticleDefinition *, G4double kineticEnergy)

const G4MaterialCutsCouple *	CurrentCouple () const

void	SetCurrentElement (const G4Element *)

Detailed Description

Definition at line 78 of file G4LowEPComptonModel.hh.

Constructor & Destructor Documentation

◆ G4LowEPComptonModel()

G4LowEPComptonModel::G4LowEPComptonModel	(	const G4ParticleDefinition *	p = `0`,
		const G4String &	nam = `"LowEPComptonModel"`
	)

Definition at line 85 of file G4LowEPComptonModel.cc.

  :G4VEmModel(nam),fParticleChange(0),isInitialised(false),
   scatterFunctionData(0),crossSectionHandler(0),fAtomDeexcitation(0)
{
  lowEnergyLimit = 250 * eV; 
  highEnergyLimit = 100 * GeV;
 
  verboseLevel=0 ;
  // Verbosity scale:
  // 0 = nothing 
  // 1 = warning for energy non-conservation 
  // 2 = details of energy budget
  // 3 = calculation of cross sections, file openings, sampling of atoms
  // 4 = entering in methods
 
  if(  verboseLevel>0 ) { 
    G4cout << "Low energy photon Compton model is constructed " << G4endl
       << "Energy range: "
       << lowEnergyLimit / eV << " eV - "
       << highEnergyLimit / GeV << " GeV"
       << G4endl;
  }
 
  //Mark this model as "applicable" for atomic deexcitation
  SetDeexcitationFlag(true);
 
}

◆ ~G4LowEPComptonModel()

G4LowEPComptonModel::~G4LowEPComptonModel ( )

virtual

Definition at line 116 of file G4LowEPComptonModel.cc.

{  
  delete crossSectionHandler;
  delete scatterFunctionData;
}

Member Function Documentation

◆ ComputeCrossSectionPerAtom()

G4double G4LowEPComptonModel::ComputeCrossSectionPerAtom	(	const G4ParticleDefinition *	,
		G4double	kinEnergy,
		G4double	Z,
		G4double	A = `0`,
		G4double	cut = `0`,
		G4double	emax = `DBL_MAX`
	)

virtual

Reimplemented from G4VEmModel.

Definition at line 177 of file G4LowEPComptonModel.cc.

{
  if (verboseLevel > 3) {
    G4cout << "Calling ComputeCrossSectionPerAtom() of G4LowEPComptonModel" << G4endl;
  }
  if (GammaEnergy < lowEnergyLimit || GammaEnergy > highEnergyLimit) { return 0.0; }
    
  G4double cs = crossSectionHandler->FindValue(G4int(Z), GammaEnergy);  
  return cs;
}

◆ Initialise()

void G4LowEPComptonModel::Initialise	(	const G4ParticleDefinition *	particle,
		const G4DataVector &	cuts
	)

virtual

Implements G4VEmModel.

Definition at line 124 of file G4LowEPComptonModel.cc.

{
  if (verboseLevel > 2) {
    G4cout << "Calling G4LowEPComptonModel::Initialise()" << G4endl;
  }
 
  if (crossSectionHandler)
  {
    crossSectionHandler->Clear();
    delete crossSectionHandler;
  }
  delete scatterFunctionData;
 
  // Reading of data files - all materials are read  
  crossSectionHandler = new G4CrossSectionHandler;
  G4String crossSectionFile = "comp/ce-cs-";
  crossSectionHandler->LoadData(crossSectionFile);
 
  G4VDataSetAlgorithm* scatterInterpolation = new G4LogLogInterpolation;
  G4String scatterFile = "comp/ce-sf-";
  scatterFunctionData = new G4CompositeEMDataSet(scatterInterpolation, 1., 1.);
  scatterFunctionData->LoadData(scatterFile);
 
  // For Doppler broadening
  shellData.SetOccupancyData();
  G4String file = "/doppler/shell-doppler";
  shellData.LoadData(file);
 
  InitialiseElementSelectors(particle,cuts);
 
  if (verboseLevel > 2) {
    G4cout << "Loaded cross section files for low energy photon Compton model" << G4endl;
  }
 
  if(isInitialised) { return; }
  isInitialised = true;
 
  fParticleChange = GetParticleChangeForGamma();
 
  fAtomDeexcitation  = G4LossTableManager::Instance()->AtomDeexcitation();
 
  if(  verboseLevel>0 ) { 
    G4cout << "Low energy photon Compton model is initialized " << G4endl
       << "Energy range: "
       << LowEnergyLimit() / eV << " eV - "
       << HighEnergyLimit() / GeV << " GeV"
       << G4endl;
  }  
}

◆ SampleSecondaries()

void G4LowEPComptonModel::SampleSecondaries	(	std::vector< G4DynamicParticle * > *	fvect,
		const G4MaterialCutsCouple *	couple,
		const G4DynamicParticle *	aDynamicGamma,
		G4double	tmin,
		G4double	maxEnergy
	)

virtual

Implements G4VEmModel.

Definition at line 199 of file G4LowEPComptonModel.cc.

{
 
  // The scattered gamma energy is sampled according to Klein - Nishina formula.
  // then accepted or rejected depending on the Scattering Function multiplied
  // by factor from Klein - Nishina formula.
  // Expression of the angular distribution as Klein Nishina
  // angular and energy distribution and Scattering fuctions is taken from
  // D. E. Cullen "A simple model of photon transport" Nucl. Instr. Meth.
  // Phys. Res. B 101 (1995). Method of sampling with form factors is different
  // data are interpolated while in the article they are fitted.
  // Reference to the article is from J. Stepanek New Photon, Positron
  // and Electron Interaction Data for GEANT in Energy Range from 1 eV to 10
  // TeV (draft).
  // The random number techniques of Butcher & Messel are used
  // (Nucl Phys 20(1960),15).
 
  G4double photonEnergy0 = aDynamicGamma->GetKineticEnergy()/MeV;
 
  if (verboseLevel > 3) {
    G4cout << "G4LowEPComptonModel::SampleSecondaries() E(MeV)= " 
       << photonEnergy0/MeV << " in " << couple->GetMaterial()->GetName() 
       << G4endl;
  }
  
  // low-energy gamma is absorpted by this process
  if (photonEnergy0 <= lowEnergyLimit) 
    {
      fParticleChange->ProposeTrackStatus(fStopAndKill);
      fParticleChange->SetProposedKineticEnergy(0.);
      fParticleChange->ProposeLocalEnergyDeposit(photonEnergy0);
      return ;
    }
 
  G4double e0m = photonEnergy0 / electron_mass_c2 ;
  G4ParticleMomentum photonDirection0 = aDynamicGamma->GetMomentumDirection();
 
  // Select randomly one element in the current material
  const G4ParticleDefinition* particle =  aDynamicGamma->GetDefinition();
  const G4Element* elm = SelectRandomAtom(couple,particle,photonEnergy0);
  G4int Z = (G4int)elm->GetZ();
 
  G4double LowEPCepsilon0 = 1. / (1. + 2. * e0m);
  G4double LowEPCepsilon0Sq = LowEPCepsilon0 * LowEPCepsilon0;
  G4double alpha1 = -std::log(LowEPCepsilon0);
  G4double alpha2 = 0.5 * (1. - LowEPCepsilon0Sq);
 
  G4double wlPhoton = h_Planck*c_light/photonEnergy0;
 
  // Sample the energy of the scattered photon
  G4double LowEPCepsilon;
  G4double LowEPCepsilonSq;
  G4double oneCosT;
  G4double sinT2;
  G4double gReject;
 
  do
    {
      if ( alpha1/(alpha1+alpha2) > G4UniformRand())
    {
      LowEPCepsilon = std::exp(-alpha1 * G4UniformRand());  
      LowEPCepsilonSq = LowEPCepsilon * LowEPCepsilon;
    }
      else
    {
      LowEPCepsilonSq = LowEPCepsilon0Sq + (1. - LowEPCepsilon0Sq) * G4UniformRand();
      LowEPCepsilon = std::sqrt(LowEPCepsilonSq);
    }
 
      oneCosT = (1. - LowEPCepsilon) / ( LowEPCepsilon * e0m);
      sinT2 = oneCosT * (2. - oneCosT);
      G4double x = std::sqrt(oneCosT/2.) / (wlPhoton/cm);
      G4double scatteringFunction = scatterFunctionData->FindValue(x,Z-1);
      gReject = (1. - LowEPCepsilon * sinT2 / (1. + LowEPCepsilonSq)) * scatteringFunction;
 
    } while(gReject < G4UniformRand()*Z); 
 
  G4double cosTheta = 1. - oneCosT;
  G4double sinTheta = std::sqrt(sinT2);
  G4double phi = twopi * G4UniformRand();
  G4double dirx = sinTheta * std::cos(phi);
  G4double diry = sinTheta * std::sin(phi);
  G4double dirz = cosTheta ;
 
  
  // Scatter photon energy and Compton electron direction - Method based on:
  // J. M. C. Brown, M. R. Dimmock, J. E. Gillam and D. M. Paganin'
  // "A low energy bound atomic electron Compton scattering model for Geant4"
  // TNS ISSUE, PG, 2012
  
  // Set constants and initialize scattering parameters
 
  G4double vel_c = 299792458;
  G4double momentum_au_to_nat = (pi/2.0)*1.992851740*std::pow(10.,-24.);
  G4double e_mass_kg = 9.10938188 * std::pow(10.,-31.);
    
  G4int maxDopplerIterations = 1000;  
  G4double bindingE = 0.; 
  G4double pEIncident = photonEnergy0 ;
  G4double pERecoil =  -1.;
  G4double eERecoil = -1.;
  G4double e_alpha =0.;
  G4double e_beta = 0.;
 
  G4double CE_emission_flag = 0.;
  G4double ePAU = -1;
  //G4double Alpha=0;
  G4int shellIdx = 0;
  G4double u_temp = 0;
  G4double cosPhiE =0;
  G4double sinThetaE =0;
  G4double cosThetaE =0;
  G4int iteration = 0; 
  do{
    
      
      // ******************************************
      // |     Determine scatter photon energy    |
      // ******************************************      
   
  do
    {
      iteration++;
      
      
      // ********************************************
      // |     Sample bound electron information    |
      // ********************************************
      
      // Select shell based on shell occupancy
      
      shellIdx = shellData.SelectRandomShell(Z);
      bindingE = shellData.BindingEnergy(Z,shellIdx)/MeV; 
      
      //G4cout << "New sample" << G4endl;
      
      // Randomly sample bound electron momentum (memento: the data set is in Atomic Units)
      ePAU = profileData.RandomSelectMomentum(Z,shellIdx);  
 
      // Convert to SI units
      
      G4double ePSI = ePAU * momentum_au_to_nat;
      
      //Calculate bound electron velocity and normalise to natural units
      
      u_temp = sqrt( ((ePSI*ePSI)*(vel_c*vel_c)) / ((e_mass_kg*e_mass_kg)*(vel_c*vel_c)+(ePSI*ePSI)))/vel_c;  
      
      // Sample incident electron direction, amorphous material, to scattering photon scattering plane      
      
      e_alpha = pi*G4UniformRand();
      e_beta = twopi*G4UniformRand();   
      
      // Total energy of system  
      
      G4double eEIncident = electron_mass_c2 / sqrt( 1 - (u_temp*u_temp));
      G4double systemE = eEIncident + pEIncident;
 
 
      G4double gamma_temp = 1.0 / sqrt( 1 - (u_temp*u_temp));
      G4double numerator = gamma_temp*electron_mass_c2*(1 - u_temp * std::cos(e_alpha));
      G4double subdenom1 =  u_temp*cosTheta*std::cos(e_alpha);
      G4double subdenom2 = u_temp*sinTheta*std::sin(e_alpha)*std::cos(e_beta);
      G4double denominator = (1.0 - cosTheta) +  (gamma_temp*electron_mass_c2*(1 - subdenom1 - subdenom2) / pEIncident);
      pERecoil = (numerator/denominator);
      eERecoil = systemE - pERecoil; 
      CE_emission_flag = pEIncident - pERecoil;
    } while ( (iteration <= maxDopplerIterations) && (CE_emission_flag < bindingE));      
    
    
   
  // End of recalculation of photon energy with Doppler broadening
 
 
 
   // *******************************************************
   // |     Determine ejected Compton electron direction    |
   // *******************************************************      
      
      // Calculate velocity of ejected Compton electron   
      
      G4double a_temp = eERecoil / electron_mass_c2;
      G4double u_p_temp = sqrt(1 - (1 / (a_temp*a_temp)));
 
      // Coefficients and terms from simulatenous equations     
     
      G4double sinAlpha = std::sin(e_alpha);
      G4double cosAlpha = std::cos(e_alpha);
      G4double sinBeta = std::sin(e_beta);
      G4double cosBeta = std::cos(e_beta);
      
      G4double gamma = 1.0 / sqrt(1 - (u_temp*u_temp));
      G4double gamma_p = 1.0 / sqrt(1 - (u_p_temp*u_p_temp));
      
      G4double var_A = pERecoil*u_p_temp*sinTheta;
      G4double var_B = u_p_temp* (pERecoil*cosTheta-pEIncident);
      G4double var_C = (pERecoil-pEIncident) - ( (pERecoil*pEIncident) / (gamma_p*electron_mass_c2))*(1 - cosTheta);
 
      G4double var_D1 = gamma*electron_mass_c2*pERecoil;
      G4double var_D2 = (1 - (u_temp*cosTheta*cosAlpha) - (u_temp*sinTheta*cosBeta*sinAlpha));
      G4double var_D3 = ((electron_mass_c2*electron_mass_c2)*(gamma*gamma_p - 1)) - (gamma_p*electron_mass_c2*pERecoil);
      G4double var_D = var_D1*var_D2 + var_D3;     
 
      G4double var_E1 = ((gamma*gamma_p)*(electron_mass_c2*electron_mass_c2)*(u_temp*u_p_temp)*cosAlpha);
      G4double var_E2 = gamma_p*electron_mass_c2*pERecoil*u_p_temp*cosTheta;
      G4double var_E = var_E1 - var_E2;
      
      G4double var_F1 = ((gamma*gamma_p)*(electron_mass_c2*electron_mass_c2)*(u_temp*u_p_temp)*cosBeta*sinAlpha);
      G4double var_F2 = (gamma_p*electron_mass_c2*pERecoil*u_p_temp*sinTheta);
      G4double var_F = var_F1 - var_F2;
      
      G4double var_G = (gamma*gamma_p)*(electron_mass_c2*electron_mass_c2)*(u_temp*u_p_temp)*sinBeta*sinAlpha;
      
      // Two equations form a quadratic form of Wx^2 + Yx + Z = 0
      // Coefficents and solution to quadratic
      
      G4double var_W1 = (var_F*var_B - var_E*var_A)*(var_F*var_B - var_E*var_A);
      G4double var_W2 = (var_G*var_G)*(var_A*var_A) + (var_G*var_G)*(var_B*var_B);
      G4double var_W = var_W1 + var_W2;
      
      G4double var_Y = 2.0*(((var_A*var_D-var_F*var_C)*(var_F*var_B-var_E*var_A)) - ((var_G*var_G)*var_B*var_C));
      
      G4double var_Z1 = (var_A*var_D - var_F*var_C)*(var_A*var_D - var_F*var_C);
      G4double var_Z2 = (var_G*var_G)*(var_C*var_C) - (var_G*var_G)*(var_A*var_A);
      G4double var_Z = var_Z1 + var_Z2;
      
      G4double diff = ((var_Y*var_Y)-4*var_W*var_Z);
      
      
     // Check if diff has FPE, if so set var_Y*var_Y and 4*var_W*var_Z to six significant figures to fix
     if (diff < 0.0)    
     {
 
      G4double funorder = 0.0;
      G4double sf = 6.0;
      
      G4double diff1 = var_Y*var_Y;
      funorder = abs(G4lrint(std::log10(static_cast<double>(abs(diff1)))+std::numeric_limits<double>::epsilon()))+sf;      
      diff1 = G4lrint(diff1*std::pow(10.0,funorder))/(1.0*std::pow(10.0,funorder));
      
      G4double diff2 = 4*var_W*var_Z;
      funorder = abs(G4lrint(std::log10(static_cast<double>(abs(diff2)))+std::numeric_limits<double>::epsilon()))+sf;      
      diff2 = G4lrint(diff2*std::pow(10.0,funorder))/(1.0*std::pow(10.0,funorder));     
      
      diff = diff1 -diff2; 
 
     }
 
  
      // Plus and minus of quadratic
      
      G4double X_p = (-var_Y + sqrt (diff))/(2*var_W);
      G4double X_m = (-var_Y - sqrt (diff))/(2*var_W);
 
 
      // Randomly sample one of the two possible solutions and determin theta angle of ejected Compton electron
      G4double ThetaE = 0.;
      G4double sol_select = G4UniformRand();
      
      if (sol_select < 0.5)
      {
          ThetaE = std::acos(X_p);
      }
      if (sol_select > 0.5)
      {
          ThetaE = std::acos(X_m);
      }
      
      cosThetaE = std::cos(ThetaE);
      sinThetaE = std::sin(ThetaE);
      G4double Theta = std::acos(cosTheta);
      
      //Calculate electron Phi
      G4double iSinThetaE = std::sqrt(1+std::tan((pi/2.0)-ThetaE)*std::tan((pi/2.0)-ThetaE));
      G4double iSinTheta = std::sqrt(1+std::tan((pi/2.0)-Theta)*std::tan((pi/2.0)-Theta)); 
      G4double ivar_A = iSinTheta/ (pERecoil*u_p_temp);
      // Trigs
      cosPhiE = (var_C - var_B*cosThetaE)*(ivar_A*iSinThetaE); 
      
      
      // Check if cosPhiE has FPE, if so set to four significant figures to fix
      if (abs(cosPhiE) > 1.0)
      {
      G4double funorder = 0.0;
      G4double sf = 4.0;
      funorder = abs(G4lrint(std::log10(static_cast<double>(abs(cosPhiE)))+std::numeric_limits<double>::epsilon()))+sf;      
      cosPhiE = G4lrint(cosPhiE*std::pow(10.0,funorder))/(1.0*std::pow(10.0,funorder));
 
      }
     // End of calculation of ejection Compton electron direction
     
      //Fix for floating point errors
 
    } while ( (iteration <= maxDopplerIterations) && (abs(cosPhiE) > 1));        
      
   // Revert to original if maximum number of iterations threshold has been reached     
      
  
  if (iteration >= maxDopplerIterations)
    {
      pERecoil = photonEnergy0 ;
      bindingE = 0.;
      dirx=0.0;
      diry=0.0;
      dirz=1.0;
    }
  
  // Set "scattered" photon direction and energy
  
  G4ThreeVector photonDirection1(dirx,diry,dirz);
  photonDirection1.rotateUz(photonDirection0);
  fParticleChange->ProposeMomentumDirection(photonDirection1) ;
 
  if (pERecoil > 0.)
    {
     fParticleChange->SetProposedKineticEnergy(pERecoil) ;
 
     // Set ejected Compton electron direction and energy
     G4double PhiE = std::acos(cosPhiE);
     G4double eDirX = sinThetaE * std::cos(phi+PhiE);
     G4double eDirY = sinThetaE * std::sin(phi+PhiE);
     G4double eDirZ = cosThetaE;
  
     G4double eKineticEnergy = pEIncident - pERecoil - bindingE;  
  
     G4ThreeVector eDirection(eDirX,eDirY,eDirZ);
     eDirection.rotateUz(photonDirection0);
     G4DynamicParticle* dp = new G4DynamicParticle (G4Electron::Electron(),
                           eDirection,eKineticEnergy) ;
     fvect->push_back(dp);
 
    }
  else
    {
      fParticleChange->SetProposedKineticEnergy(0.);
      fParticleChange->ProposeTrackStatus(fStopAndKill);   
    }
      
 
 
 
  // sample deexcitation
  
  if(fAtomDeexcitation && iteration < maxDopplerIterations) {
    G4int index = couple->GetIndex();
    if(fAtomDeexcitation->CheckDeexcitationActiveRegion(index)) {
      size_t nbefore = fvect->size();
      G4AtomicShellEnumerator as = G4AtomicShellEnumerator(shellIdx);
      const G4AtomicShell* shell = fAtomDeexcitation->GetAtomicShell(Z, as);
      fAtomDeexcitation->GenerateParticles(fvect, shell, Z, index);
      size_t nafter = fvect->size();
      if(nafter > nbefore) {
    for (size_t i=nbefore; i<nafter; ++i) {
      bindingE -= ((*fvect)[i])->GetKineticEnergy();
    } 
      }
    }
  }
  if(bindingE < 0.0) { bindingE = 0.0; }
  fParticleChange->ProposeLocalEnergyDeposit(bindingE);
  
}

Member Data Documentation

◆ fParticleChange

G4ParticleChangeForGamma* G4LowEPComptonModel::fParticleChange

protected

Definition at line 105 of file G4LowEPComptonModel.hh.

Referenced by Initialise(), and SampleSecondaries().

The documentation for this class was generated from the following files:

Public Member Functions

Protected Attributes

Additional Inherited Members

Detailed Description

Constructor & Destructor Documentation

◆ G4LowEPComptonModel()

◆ ~G4LowEPComptonModel()

Member Function Documentation

◆ ComputeCrossSectionPerAtom()

◆ Initialise()

◆ SampleSecondaries()

Member Data Documentation

◆ fParticleChange