#include <G4PenelopeComptonModel.hh>

Inheritance diagram for G4PenelopeComptonModel:

Public Member Functions
	G4PenelopeComptonModel (const G4ParticleDefinition *p=0, const G4String &processName="PenCompton")

virtual	~G4PenelopeComptonModel ()

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

virtual void	InitialiseLocal (const G4ParticleDefinition , G4VEmModel masterModel)

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

virtual G4double	ComputeCrossSectionPerAtom (const G4ParticleDefinition *, G4double, G4double, G4double, G4double, G4double)

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

void	SetVerbosityLevel (G4int lev)

G4int	GetVerbosityLevel ()

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 void	InitialiseLocal (const G4ParticleDefinition , G4VEmModel masterModel)

virtual void	InitialiseForMaterial (const G4ParticleDefinition , const G4Material )

virtual void	InitialiseForElement (const G4ParticleDefinition *, G4int Z)

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	GetPartialCrossSection (const G4Material , G4int level, const G4ParticleDefinition , G4double kineticEnergy)

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

virtual G4double	ComputeCrossSectionPerShell (const G4ParticleDefinition *, G4int Z, G4int shellIdx, G4double kinEnergy, 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 , G4double cut=0.0)

virtual G4double	MinEnergyCut (const G4ParticleDefinition , const G4MaterialCutsCouple )

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

virtual void	DefineForRegion (const G4Region *)

virtual void	ModelDescription (std::ostream &outFile) const

void	InitialiseElementSelectors (const G4ParticleDefinition *, const G4DataVector &)

std::vector< G4EmElementSelector * > *	GetElementSelectors ()

void	SetElementSelectors (std::vector< G4EmElementSelector * > *)

virtual 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)

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

const G4Element *	SelectTargetAtom (const G4MaterialCutsCouple , const G4ParticleDefinition , G4double kineticEnergy, G4double logKineticEnergy, 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)

G4int	SelectRandomAtomNumber (const G4Material *)

G4int	SelectIsotopeNumber (const G4Element *)

void	SetParticleChange (G4VParticleChange , G4VEmFluctuationModel f=nullptr)

void	SetCrossSectionTable (G4PhysicsTable *, G4bool isLocal)

G4ElementData *	GetElementData ()

G4PhysicsTable *	GetCrossSectionTable ()

G4VEmFluctuationModel *	GetModelOfFluctuations ()

G4VEmAngularDistribution *	GetAngularDistribution ()

G4VEmModel *	GetTripletModel ()

void	SetTripletModel (G4VEmModel *)

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

G4bool	UseAngularGeneratorFlag () const

void	SetAngularGeneratorFlag (G4bool)

void	SetHighEnergyLimit (G4double)

void	SetLowEnergyLimit (G4double)

void	SetActivationHighEnergyLimit (G4double)

void	SetActivationLowEnergyLimit (G4double)

G4bool	IsActive (G4double kinEnergy) const

void	SetPolarAngleLimit (G4double)

void	SetSecondaryThreshold (G4double)

void	SetLPMFlag (G4bool val)

void	SetDeexcitationFlag (G4bool val)

void	SetForceBuildTable (G4bool val)

void	SetFluctuationFlag (G4bool val)

void	SetMasterThread (G4bool val)

G4bool	IsMaster () const

void	SetUseBaseMaterials (G4bool val)

G4bool	UseBaseMaterials () const

G4double	MaxSecondaryKinEnergy (const G4DynamicParticle *dynParticle)

const G4String &	GetName () const

void	SetCurrentCouple (const G4MaterialCutsCouple *)

const G4Element *	GetCurrentElement () const

const G4Isotope *	GetCurrentIsotope () const

G4bool	IsLocked () const

void	SetLocked (G4bool)

G4VEmModel &	operator= (const G4VEmModel &right)=delete

	G4VEmModel (const G4VEmModel &)=delete

Protected Attributes
G4ParticleChangeForGamma *	fParticleChange

const G4ParticleDefinition *	fParticle

Protected Attributes inherited from G4VEmModel
G4ElementData *	fElementData

G4VParticleChange *	pParticleChange

G4PhysicsTable *	xSectionTable

const G4Material *	pBaseMaterial

const std::vector< G4double > *	theDensityFactor

const std::vector< G4int > *	theDensityIdx

size_t	idxTable

G4bool	lossFlucFlag

G4double	inveplus

G4double	pFactor

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 62 of file G4PenelopeComptonModel.hh.

Constructor & Destructor Documentation

◆ G4PenelopeComptonModel()

G4PenelopeComptonModel::G4PenelopeComptonModel	(	const G4ParticleDefinition *	p = `0`,
		const G4String &	processName = `"PenCompton"`
	)

Definition at line 63 of file G4PenelopeComptonModel.cc.

  :G4VEmModel(nam),fParticleChange(0),fParticle(0),
   isInitialised(false),fAtomDeexcitation(0),
   oscManager(0)
{
  fIntrinsicLowEnergyLimit = 100.0*eV;
  fIntrinsicHighEnergyLimit = 100.0*GeV;
  SetHighEnergyLimit(fIntrinsicHighEnergyLimit);
  //
  oscManager = G4PenelopeOscillatorManager::GetOscillatorManager();
 
  if (part)
    SetParticle(part);
 
  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
 
  //Mark this model as "applicable" for atomic deexcitation
  SetDeexcitationFlag(true);
 
  fTransitionManager = G4AtomicTransitionManager::Instance();
}

◆ ~G4PenelopeComptonModel()

G4PenelopeComptonModel::~G4PenelopeComptonModel ( )

virtual

Definition at line 94 of file G4PenelopeComptonModel.cc.

95{;}

Member Function Documentation

◆ ComputeCrossSectionPerAtom()

G4double G4PenelopeComptonModel::ComputeCrossSectionPerAtom	(	const G4ParticleDefinition *	,
		G4double	,
		G4double	,
		G4double	,
		G4double	,
		G4double
	)

virtual

Reimplemented from G4VEmModel.

Definition at line 252 of file G4PenelopeComptonModel.cc.

{
  G4cout << "*** G4PenelopeComptonModel -- WARNING ***" << G4endl;
  G4cout << "Penelope Compton model v2008 does not calculate cross section _per atom_ " << G4endl;
  G4cout << "so the result is always zero. For physics values, please invoke " << G4endl;
  G4cout << "GetCrossSectionPerVolume() or GetMeanFreePath() via the G4EmCalculator" << G4endl;
  return 0;
}

◆ CrossSectionPerVolume()

G4double G4PenelopeComptonModel::CrossSectionPerVolume	(	const G4Material *	material,
		const G4ParticleDefinition *	p,
		G4double	kineticEnergy,
		G4double	cutEnergy = `0.0`,
		G4double	maxEnergy = `DBL_MAX`
	)

virtual

Reimplemented from G4VEmModel.

Definition at line 178 of file G4PenelopeComptonModel.cc.

{
  // Penelope model v2008 to calculate the Compton scattering cross section:
  // D. Brusa et al., Nucl. Instrum. Meth. A 379 (1996) 167
  //
  // The cross section for Compton scattering is calculated according to the Klein-Nishina
  // formula for energy > 5 MeV.
  // For E < 5 MeV it is used a parametrization for the differential cross-section dSigma/dOmega,
  // which is integrated numerically in cos(theta), G4PenelopeComptonModel::DifferentialCrossSection().
  // The parametrization includes the J(p)
  // distribution profiles for the atomic shells, that are tabulated from Hartree-Fock calculations
  // from F. Biggs et al., At. Data Nucl. Data Tables 16 (1975) 201
  //
  if (verboseLevel > 3)
    G4cout << "Calling CrossSectionPerVolume() of G4PenelopeComptonModel" << G4endl;
  SetupForMaterial(p, material, energy);
 
 
  G4double cs = 0;
  //Force null cross-section if below the low-energy edge of the table
  if (energy < LowEnergyLimit())
    return cs;
 
  //Retrieve the oscillator table for this material
  G4PenelopeOscillatorTable* theTable = oscManager->GetOscillatorTableCompton(material);
 
  if (energy < 5*MeV) //explicit calculation for E < 5 MeV
    {
      size_t numberOfOscillators = theTable->size();
      for (size_t i=0;i<numberOfOscillators;i++)
    {
      G4PenelopeOscillator* theOsc = (*theTable)[i];
      //sum contributions coming from each oscillator
      cs += OscillatorTotalCrossSection(energy,theOsc);
    }
    }
  else //use Klein-Nishina for E>5 MeV
    cs = KleinNishinaCrossSection(energy,material);
 
  //cross sections are in units of pi*classic_electr_radius^2
  cs *= pi*classic_electr_radius*classic_electr_radius;
 
  //Now, cs is the cross section *per molecule*, let's calculate the
  //cross section per volume
 
  G4double atomDensity = material->GetTotNbOfAtomsPerVolume();
  G4double atPerMol =  oscManager->GetAtomsPerMolecule(material);
 
  if (verboseLevel > 3)
    G4cout << "Material " << material->GetName() << " has " << atPerMol <<
      "atoms per molecule" << G4endl;
 
  G4double moleculeDensity = 0.;
 
  if (atPerMol)
    moleculeDensity = atomDensity/atPerMol;
 
  G4double csvolume = cs*moleculeDensity;
 
  if (verboseLevel > 2)
    G4cout << "Compton mean free path at " << energy/keV << " keV for material " <<
            material->GetName() << " = " << (1./csvolume)/mm << " mm" << G4endl;
  return csvolume;
}

◆ GetVerbosityLevel()

G4int G4PenelopeComptonModel::GetVerbosityLevel ( )

inline

Definition at line 99 of file G4PenelopeComptonModel.hh.

99{return verboseLevel;};

◆ Initialise()

void G4PenelopeComptonModel::Initialise	(	const G4ParticleDefinition *	part,
		const G4DataVector &
	)

virtual

Implements G4VEmModel.

Definition at line 99 of file G4PenelopeComptonModel.cc.

{
  if (verboseLevel > 3)
    G4cout << "Calling G4PenelopeComptonModel::Initialise()" << G4endl;
 
  fAtomDeexcitation = G4LossTableManager::Instance()->AtomDeexcitation();
  //Issue warning if the AtomicDeexcitation has not been declared
  if (!fAtomDeexcitation)
    {
      G4cout << G4endl;
      G4cout << "WARNING from G4PenelopeComptonModel " << G4endl;
      G4cout << "Atomic de-excitation module is not instantiated, so there will not be ";
      G4cout << "any fluorescence/Auger emission." << G4endl;
      G4cout << "Please make sure this is intended" << G4endl;
    }
 
  SetParticle(part);
 
  if (IsMaster() && part == fParticle)
    {
 
      if (verboseLevel > 0)
    {
      G4cout << "Penelope Compton model v2008 is initialized " << G4endl
         << "Energy range: "
         << LowEnergyLimit() / keV << " keV - "
         << HighEnergyLimit() / GeV << " GeV";
    }
      //Issue a warning, if the model is going to be used down to a
      //energy which is outside the validity of the model itself
      if (LowEnergyLimit() < fIntrinsicLowEnergyLimit)
    {
      G4ExceptionDescription ed;
      ed << "Using the Penelope Compton model outside its intrinsic validity range. "
         << G4endl;
      ed << "-> LowEnergyLimit() in process = " << LowEnergyLimit()/keV << "keV " << G4endl;
      ed << "-> Instrinsic low-energy limit = " << fIntrinsicLowEnergyLimit/keV << "keV "
         << G4endl;
      ed << "Result of the simulation have to be taken with care" << G4endl;
      G4Exception("G4PenelopeComptonModel::Initialise()",
              "em2100",JustWarning,ed);
    }
    }
 
  if(isInitialised) return;
  fParticleChange = GetParticleChangeForGamma();
  isInitialised = true;
 
}

◆ InitialiseLocal()

void G4PenelopeComptonModel::InitialiseLocal	(	const G4ParticleDefinition *	part,
		G4VEmModel *	masterModel
	)

virtual

Reimplemented from G4VEmModel.

Definition at line 152 of file G4PenelopeComptonModel.cc.

{
  if (verboseLevel > 3)
    G4cout << "Calling  G4PenelopeComptonModel::InitialiseLocal()" << G4endl;
 
  //
  //Check that particle matches: one might have multiple master models (e.g.
  //for e+ and e-).
  //
  if (part == fParticle)
    {
      //Get the const table pointers from the master to the workers
      const G4PenelopeComptonModel* theModel =
        static_cast<G4PenelopeComptonModel*> (masterModel);
 
      //Same verbosity for all workers, as the master
      verboseLevel = theModel->verboseLevel;
    }
 
  return;
}

◆ SampleSecondaries()

void G4PenelopeComptonModel::SampleSecondaries	(	std::vector< G4DynamicParticle * > *	fvect,
		const G4MaterialCutsCouple *	couple,
		const G4DynamicParticle *	aDynamicGamma,
		G4double	tmin,
		G4double	maxEnergy
	)

virtual

Implements G4VEmModel.

Definition at line 268 of file G4PenelopeComptonModel.cc.

{
 
  // Penelope model v2008 to sample the Compton scattering final state.
  // D. Brusa et al., Nucl. Instrum. Meth. A 379 (1996) 167
  // The model determines also the original shell from which the electron is expelled,
  // in order to produce fluorescence de-excitation (from G4DeexcitationManager)
  //
  // The final state for Compton scattering is calculated according to the Klein-Nishina
  // formula for energy > 5 MeV. In this case, the Doppler broadening is negligible and
  // one can assume that the target electron is at rest.
  // For E < 5 MeV it is used the parametrization for the differential cross-section dSigma/dOmega,
  // to sample the scattering angle and the energy of the emerging electron, which is
  // G4PenelopeComptonModel::DifferentialCrossSection(). The rejection method is
  // used to sample cos(theta). The efficiency increases monotonically with photon energy and is
  // nearly independent on the Z; typical values are 35%, 80% and 95% for 1 keV, 1 MeV and 10 MeV,
  // respectively.
  // The parametrization includes the J(p) distribution profiles for the atomic shells, that are
  // tabulated
  // from Hartree-Fock calculations from F. Biggs et al., At. Data Nucl. Data Tables 16 (1975) 201.
  // Doppler broadening is included.
  //
 
  if (verboseLevel > 3)
    G4cout << "Calling SampleSecondaries() of G4PenelopeComptonModel" << G4endl;
 
  G4double photonEnergy0 = aDynamicGamma->GetKineticEnergy();
 
  // do nothing below the threshold
  // should never get here because the XS is zero below the limit
  if(photonEnergy0 < LowEnergyLimit())
    return;
 
  G4ParticleMomentum photonDirection0 = aDynamicGamma->GetMomentumDirection();
  const G4Material* material = couple->GetMaterial();
 
  G4PenelopeOscillatorTable* theTable = oscManager->GetOscillatorTableCompton(material);
 
  const G4int nmax = 64;
  G4double rn[nmax]={0.0};
  G4double pac[nmax]={0.0};
 
  G4double S=0.0;
  G4double epsilon = 0.0;
  G4double cosTheta = 1.0;
  G4double hartreeFunc = 0.0;
  G4double oscStren = 0.0;
  size_t numberOfOscillators = theTable->size();
  size_t targetOscillator = 0;
  G4double ionEnergy = 0.0*eV;
 
  G4double ek = photonEnergy0/electron_mass_c2;
  G4double ek2 = 2.*ek+1.0;
  G4double eks = ek*ek;
  G4double ek1 = eks-ek2-1.0;
 
  G4double taumin = 1.0/ek2;
  G4double a1 = G4Log(ek2);
  G4double a2 = a1+2.0*ek*(1.0+ek)/(ek2*ek2);
 
  G4double TST = 0;
  G4double tau = 0.;
 
  //If the incoming photon is above 5 MeV, the quicker approach based on the
  //pure Klein-Nishina formula is used
  if (photonEnergy0 > 5*MeV)
    {
      do{
    do{
      if ((a2*G4UniformRand()) < a1)
        tau = std::pow(taumin,G4UniformRand());
      else
        tau = std::sqrt(1.0+G4UniformRand()*(taumin*taumin-1.0));
      //rejection function
      TST = (1.0+tau*(ek1+tau*(ek2+tau*eks)))/(eks*tau*(1.0+tau*tau));
    }while (G4UniformRand()> TST);
    epsilon=tau;
    cosTheta = 1.0 - (1.0-tau)/(ek*tau);
 
    //Target shell electrons
    TST = oscManager->GetTotalZ(material)*G4UniformRand();
    targetOscillator = numberOfOscillators-1; //last level
    S=0.0;
    G4bool levelFound = false;
    for (size_t j=0;j<numberOfOscillators && !levelFound; j++)
      {
        S += (*theTable)[j]->GetOscillatorStrength();
        if (S > TST)
          {
        targetOscillator = j;
        levelFound = true;
          }
      }
    //check whether the level is valid
    ionEnergy = (*theTable)[targetOscillator]->GetIonisationEnergy();
      }while((epsilon*photonEnergy0-photonEnergy0+ionEnergy) >0);
    }
  else //photonEnergy0 < 5 MeV
    {
      //Incoherent scattering function for theta=PI
      G4double s0=0.0;
      G4double pzomc=0.0;
      G4double rni=0.0;
      G4double aux=0.0;
      for (size_t i=0;i<numberOfOscillators;i++)
    {
      ionEnergy = (*theTable)[i]->GetIonisationEnergy();
      if (photonEnergy0 > ionEnergy)
        {
          G4double aux2 = photonEnergy0*(photonEnergy0-ionEnergy)*2.0;
          hartreeFunc = (*theTable)[i]->GetHartreeFactor();
          oscStren = (*theTable)[i]->GetOscillatorStrength();
          pzomc = hartreeFunc*(aux2-electron_mass_c2*ionEnergy)/
        (electron_mass_c2*std::sqrt(2.0*aux2+ionEnergy*ionEnergy));
          if (pzomc > 0)
        rni = 1.0-0.5*G4Exp(0.5-(std::sqrt(0.5)+std::sqrt(2.0)*pzomc)*
                       (std::sqrt(0.5)+std::sqrt(2.0)*pzomc));
          else
        rni = 0.5*G4Exp(0.5-(std::sqrt(0.5)-std::sqrt(2.0)*pzomc)*
                   (std::sqrt(0.5)-std::sqrt(2.0)*pzomc));
          s0 += oscStren*rni;
        }
    }
      //Sampling tau
      G4double cdt1 = 0.;
      do
    {
      if ((G4UniformRand()*a2) < a1)
        tau = std::pow(taumin,G4UniformRand());
      else
        tau = std::sqrt(1.0+G4UniformRand()*(taumin*taumin-1.0));
      cdt1 = (1.0-tau)/(ek*tau);
      //Incoherent scattering function
      S = 0.;
      for (size_t i=0;i<numberOfOscillators;i++)
        {
          ionEnergy = (*theTable)[i]->GetIonisationEnergy();
          if (photonEnergy0 > ionEnergy) //sum only on excitable levels
        {
          aux = photonEnergy0*(photonEnergy0-ionEnergy)*cdt1;
          hartreeFunc = (*theTable)[i]->GetHartreeFactor();
          oscStren = (*theTable)[i]->GetOscillatorStrength();
          pzomc = hartreeFunc*(aux-electron_mass_c2*ionEnergy)/
            (electron_mass_c2*std::sqrt(2.0*aux+ionEnergy*ionEnergy));
          if (pzomc > 0)
            rn[i] = 1.0-0.5*G4Exp(0.5-(std::sqrt(0.5)+std::sqrt(2.0)*pzomc)*
                         (std::sqrt(0.5)+std::sqrt(2.0)*pzomc));
          else
            rn[i] = 0.5*G4Exp(0.5-(std::sqrt(0.5)-std::sqrt(2.0)*pzomc)*
                     (std::sqrt(0.5)-std::sqrt(2.0)*pzomc));
          S += oscStren*rn[i];
          pac[i] = S;
        }
          else
        pac[i] = S-1e-6;
        }
      //Rejection function
      TST = S*(1.0+tau*(ek1+tau*(ek2+tau*eks)))/(eks*tau*(1.0+tau*tau));
    }while ((G4UniformRand()*s0) > TST);
 
      cosTheta = 1.0 - cdt1;
      G4double fpzmax=0.0,fpz=0.0;
      G4double A=0.0;
      //Target electron shell
      do
    {
      do
        {
          TST = S*G4UniformRand();
          targetOscillator = numberOfOscillators-1; //last level
          G4bool levelFound = false;
          for (size_t i=0;i<numberOfOscillators && !levelFound;i++)
        {
          if (pac[i]>TST)
            {
              targetOscillator = i;
              levelFound = true;
            }
        }
          A = G4UniformRand()*rn[targetOscillator];
          hartreeFunc = (*theTable)[targetOscillator]->GetHartreeFactor();
          oscStren = (*theTable)[targetOscillator]->GetOscillatorStrength();
          if (A < 0.5)
        pzomc = (std::sqrt(0.5)-std::sqrt(0.5-G4Log(2.0*A)))/
          (std::sqrt(2.0)*hartreeFunc);
          else
        pzomc = (std::sqrt(0.5-G4Log(2.0-2.0*A))-std::sqrt(0.5))/
          (std::sqrt(2.0)*hartreeFunc);
        } while (pzomc < -1);
 
      // F(EP) rejection
      G4double XQC = 1.0+tau*(tau-2.0*cosTheta);
      G4double AF = std::sqrt(XQC)*(1.0+tau*(tau-cosTheta)/XQC);
      if (AF > 0)
        fpzmax = 1.0+AF*0.2;
      else
        fpzmax = 1.0-AF*0.2;
      fpz = 1.0+AF*std::max(std::min(pzomc,0.2),-0.2);
    }while ((fpzmax*G4UniformRand())>fpz);
 
      //Energy of the scattered photon
      G4double T = pzomc*pzomc;
      G4double b1 = 1.0-T*tau*tau;
      G4double b2 = 1.0-T*tau*cosTheta;
      if (pzomc > 0.0)
    epsilon = (tau/b1)*(b2+std::sqrt(std::abs(b2*b2-b1*(1.0-T))));
      else
    epsilon = (tau/b1)*(b2-std::sqrt(std::abs(b2*b2-b1*(1.0-T))));
    } //energy < 5 MeV
 
  //Ok, the kinematics has been calculated.
  G4double sinTheta = std::sqrt(1-cosTheta*cosTheta);
  G4double phi = twopi * G4UniformRand() ;
  G4double dirx = sinTheta * std::cos(phi);
  G4double diry = sinTheta * std::sin(phi);
  G4double dirz = cosTheta ;
 
  // Update G4VParticleChange for the scattered photon
  G4ThreeVector photonDirection1(dirx,diry,dirz);
  photonDirection1.rotateUz(photonDirection0);
  fParticleChange->ProposeMomentumDirection(photonDirection1) ;
 
  G4double photonEnergy1 = epsilon * photonEnergy0;
 
  if (photonEnergy1 > 0.)
    fParticleChange->SetProposedKineticEnergy(photonEnergy1) ;
  else
  {
    fParticleChange->SetProposedKineticEnergy(0.) ;
    fParticleChange->ProposeTrackStatus(fStopAndKill);
  }
 
  //Create scattered electron
  G4double diffEnergy = photonEnergy0*(1-epsilon);
  ionEnergy = (*theTable)[targetOscillator]->GetIonisationEnergy();
 
  G4double Q2 =
    photonEnergy0*photonEnergy0+photonEnergy1*(photonEnergy1-2.0*photonEnergy0*cosTheta);
  G4double cosThetaE = 0.; //scattering angle for the electron
 
  if (Q2 > 1.0e-12)
    cosThetaE = (photonEnergy0-photonEnergy1*cosTheta)/std::sqrt(Q2);
  else
    cosThetaE = 1.0;
  G4double sinThetaE = std::sqrt(1-cosThetaE*cosThetaE);
 
  //Now, try to handle fluorescence
  //Notice: merged levels are indicated with Z=0 and flag=30
  G4int shFlag = (*theTable)[targetOscillator]->GetShellFlag();
  G4int Z = (G4int) (*theTable)[targetOscillator]->GetParentZ();
 
  //initialize here, then check photons created by Atomic-Deexcitation, and the final state e-
  G4double bindingEnergy = 0.*eV;
  const G4AtomicShell* shell = 0;
 
  //Real level
  if (Z > 0 && shFlag<30)
    {
      shell = fTransitionManager->Shell(Z,shFlag-1);
      bindingEnergy = shell->BindingEnergy();
    }
 
  G4double ionEnergyInPenelopeDatabase = ionEnergy;
  //protection against energy non-conservation
  ionEnergy = std::max(bindingEnergy,ionEnergyInPenelopeDatabase);
 
  //subtract the excitation energy. If not emitted by fluorescence
  //the ionization energy is deposited as local energy deposition
  G4double eKineticEnergy = diffEnergy - ionEnergy;
  G4double localEnergyDeposit = ionEnergy;
  G4double energyInFluorescence = 0.; //testing purposes only
  G4double energyInAuger = 0; //testing purposes
 
  if (eKineticEnergy < 0)
    {
      //It means that there was some problem/mismatch between the two databases.
      //Try to make it work
      //In this case available Energy (diffEnergy) < ionEnergy
      //Full residual energy is deposited locally
      localEnergyDeposit = diffEnergy;
      eKineticEnergy = 0.0;
    }
 
  //the local energy deposit is what remains: part of this may be spent for fluorescence.
  //Notice: shell might be nullptr (invalid!) if shFlag=30. Must be protected
  //Now, take care of fluorescence, if required
  if (fAtomDeexcitation && shell)
    {
      G4int index = couple->GetIndex();
      if (fAtomDeexcitation->CheckDeexcitationActiveRegion(index))
    {
      size_t nBefore = fvect->size();
      fAtomDeexcitation->GenerateParticles(fvect,shell,Z,index);
      size_t nAfter = fvect->size();
 
      if (nAfter > nBefore) //actual production of fluorescence
        {
          for (size_t j=nBefore;j<nAfter;j++) //loop on products
        {
          G4double itsEnergy = ((*fvect)[j])->GetKineticEnergy();
          if (itsEnergy < localEnergyDeposit) // valid secondary, generate it
            {
              localEnergyDeposit -= itsEnergy;
              if (((*fvect)[j])->GetParticleDefinition() == G4Gamma::Definition())
            energyInFluorescence += itsEnergy;
              else if (((*fvect)[j])->GetParticleDefinition() == 
                   G4Electron::Definition())
            energyInAuger += itsEnergy;
            }
          else //invalid secondary: takes more than the available energy: delete it
            {
              delete (*fvect)[j];
              (*fvect)[j] = nullptr;
            }
        }
        }
      
    }
    }
 
 
  /*
  if(DeexcitationFlag() && Z > 5 && shellId>0) {
 
    const G4ProductionCutsTable* theCoupleTable=
      G4ProductionCutsTable::GetProductionCutsTable();
 
    size_t index = couple->GetIndex();
    G4double cutg = (*(theCoupleTable->GetEnergyCutsVector(0)))[index];
    G4double cute = (*(theCoupleTable->GetEnergyCutsVector(1)))[index];
 
    // Generation of fluorescence
    // Data in EADL are available only for Z > 5
    // Protection to avoid generating photons in the unphysical case of
    // shell binding energy > photon energy
    if (localEnergyDeposit > cutg || localEnergyDeposit > cute)
      {
    G4DynamicParticle* aPhoton;
    deexcitationManager.SetCutForSecondaryPhotons(cutg);
    deexcitationManager.SetCutForAugerElectrons(cute);
 
    photonVector = deexcitationManager.GenerateParticles(Z,shellId);
    if(photonVector)
      {
        size_t nPhotons = photonVector->size();
        for (size_t k=0; k<nPhotons; k++)
          {
        aPhoton = (*photonVector)[k];
        if (aPhoton)
          {
            G4double itsEnergy = aPhoton->GetKineticEnergy();
            G4bool keepIt = false;
            if (itsEnergy <= localEnergyDeposit)
              {
            //check if good!
            if(aPhoton->GetDefinition() == G4Gamma::Gamma()
               && itsEnergy >= cutg)
              {
                keepIt = true;
                energyInFluorescence += itsEnergy;
              }
            if (aPhoton->GetDefinition() == G4Electron::Electron() &&
                itsEnergy >= cute)
              {
                energyInAuger += itsEnergy;
                keepIt = true;
              }
              }
            //good secondary, register it
            if (keepIt)
              {
            localEnergyDeposit -= itsEnergy;
            fvect->push_back(aPhoton);
              }
            else
              {
            delete aPhoton;
            (*photonVector)[k] = 0;
              }
          }
          }
        delete photonVector;
      }
      }
  }
  */
 
 
  //Always produce explicitly the electron
  G4DynamicParticle* electron = 0;
 
  G4double xEl = sinThetaE * std::cos(phi+pi);
  G4double yEl = sinThetaE * std::sin(phi+pi);
  G4double zEl = cosThetaE;
  G4ThreeVector eDirection(xEl,yEl,zEl); //electron direction
  eDirection.rotateUz(photonDirection0);
  electron = new G4DynamicParticle (G4Electron::Electron(),
                    eDirection,eKineticEnergy) ;
  fvect->push_back(electron);
 
 
  if (localEnergyDeposit < 0) //Should not be: issue a G4Exception (warning)
    {
      G4Exception("G4PenelopeComptonModel::SampleSecondaries()",
           "em2099",JustWarning,"WARNING: Negative local energy deposit");
      localEnergyDeposit=0.;
    }
  fParticleChange->ProposeLocalEnergyDeposit(localEnergyDeposit);
 
  G4double electronEnergy = 0.;
  if (electron)
    electronEnergy = eKineticEnergy;
  if (verboseLevel > 1)
    {
      G4cout << "-----------------------------------------------------------" << G4endl;
      G4cout << "Energy balance from G4PenelopeCompton" << G4endl;
      G4cout << "Incoming photon energy: " << photonEnergy0/keV << " keV" << G4endl;
      G4cout << "-----------------------------------------------------------" << G4endl;
      G4cout << "Scattered photon: " << photonEnergy1/keV << " keV" << G4endl;
      G4cout << "Scattered electron " << electronEnergy/keV << " keV" << G4endl;
      if (energyInFluorescence)
    G4cout << "Fluorescence x-rays: " << energyInFluorescence/keV << " keV" << G4endl;
      if (energyInAuger)
    G4cout << "Auger electrons: " << energyInAuger/keV << " keV" << G4endl;
      G4cout << "Local energy deposit " << localEnergyDeposit/keV << " keV" << G4endl;
      G4cout << "Total final state: " << (photonEnergy1+electronEnergy+energyInFluorescence+
                      localEnergyDeposit+energyInAuger)/keV <<
    " keV" << G4endl;
      G4cout << "-----------------------------------------------------------" << G4endl;
    }
  if (verboseLevel > 0)
    {
      G4double energyDiff = std::fabs(photonEnergy1+
                      electronEnergy+energyInFluorescence+
                      localEnergyDeposit+energyInAuger-photonEnergy0);
      if (energyDiff > 0.05*keV)
    G4cout << "Warning from G4PenelopeCompton: problem with energy conservation: " <<
      (photonEnergy1+electronEnergy+energyInFluorescence+energyInAuger+localEnergyDeposit)/keV <<
      " keV (final) vs. " <<
      photonEnergy0/keV << " keV (initial)" << G4endl;
    }
}

◆ SetVerbosityLevel()

void G4PenelopeComptonModel::SetVerbosityLevel ( G4int lev )

inline

Definition at line 98 of file G4PenelopeComptonModel.hh.

98{verboseLevel = lev;};

Member Data Documentation

◆ fParticle

const G4ParticleDefinition* G4PenelopeComptonModel::fParticle

protected

Definition at line 104 of file G4PenelopeComptonModel.hh.

Referenced by Initialise(), and InitialiseLocal().

◆ fParticleChange

G4ParticleChangeForGamma* G4PenelopeComptonModel::fParticleChange

protected

Definition at line 103 of file G4PenelopeComptonModel.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

◆ G4PenelopeComptonModel()

◆ ~G4PenelopeComptonModel()

Member Function Documentation

◆ ComputeCrossSectionPerAtom()

◆ CrossSectionPerVolume()

◆ GetVerbosityLevel()

◆ Initialise()

◆ InitialiseLocal()

◆ SampleSecondaries()

◆ SetVerbosityLevel()

Member Data Documentation

◆ fParticle

◆ fParticleChange