Gabriele Cosmo
178 lines
6.3 KiB
Plaintext
178 lines
6.3 KiB
Plaintext
// This code implementation is the intellectual property of
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// the GEANT4 collaboration.
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//
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// By copying, distributing or modifying the Program (or any work
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// based on the Program) you indicate your acceptance of this statement,
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// and all its terms.
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//
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// $Id: G4PhotoElectricEffect.icc,v 1.3 1999/12/15 14:51:48 gunter Exp $
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// GEANT4 tag $Name: geant4-03-00 $
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//
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//
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// ---------------------------------------------------------------
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// GEANT 4 class inlined methods file
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//
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// For information related to this code contact:
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// CERN, CN Division, ASD group
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// History: first implementation, based on object model of
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// 2nd December 1995, G.Cosmo
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// ------------ G4PhotoElectricEffect physics process ---------
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// by Michel Maire, April 1996
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// ***************************************************************
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// 12-06-96, update by M.Maire
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// 17-09-96, PartialSumSigma(i)
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// split ComputeBinbingEnergy(), M.Maire
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// 08-01-97, crossection table + meanfreepath table , M.Maire
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// 13-03-97, adapted for the new physics scheme, M.Maire
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// 20-11-97, change for lowest energy limit default action
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// 17-11-98, use table of atomic shells in PostStepDoIt, mma
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// 06-01-99, use Sandia crossSection, V.Grichine mma
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// ---------------------------------------------------------------
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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inline G4bool G4PhotoElectricEffect::IsApplicable(const G4ParticleDefinition& particle)
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{
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return ( &particle == G4Gamma::Gamma() );
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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inline G4double G4PhotoElectricEffect::GetCrossSectionPerAtom(
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const G4DynamicParticle* aDynamicGamma,
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G4Element* anElement)
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// gives the microscopic total cross section in GEANT4 internal units
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{
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G4double crossSection;
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G4double GammaEnergy = aDynamicGamma->GetKineticEnergy();
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G4double AtomicNumber = anElement->GetZ();
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G4bool isOutRange;
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if (GammaEnergy > HighestEnergyLimit)
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crossSection = 0.;
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else if (GammaEnergy > LowestEnergyLimit)
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crossSection = (*theCrossSectionTable)(anElement->GetIndex())->
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GetValue(GammaEnergy, isOutRange);
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else
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crossSection = ComputeSandiaCrossSection(GammaEnergy,AtomicNumber);
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return crossSection;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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inline G4double G4PhotoElectricEffect::GetMeanFreePath(const G4Track& aTrack,
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G4double,
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G4ForceCondition*)
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// returns the gamma mean free path in GEANT4 internal units
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// ( MeanFreePath is a private data member of the class)
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{
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const G4DynamicParticle* aDynamicGamma = aTrack.GetDynamicParticle();
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G4double GammaEnergy = aDynamicGamma->GetKineticEnergy();
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G4Material* aMaterial = aTrack.GetMaterial();
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G4bool isOutRange ;
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if (GammaEnergy > HighestEnergyLimit)
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MeanFreePath = DBL_MAX;
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else if (GammaEnergy > LowestEnergyLimit)
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MeanFreePath = (*theMeanFreePathTable)(aMaterial->GetIndex())->
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GetValue(GammaEnergy, isOutRange);
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else
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MeanFreePath = ComputeSandiaMeanFreePath(GammaEnergy, aMaterial);
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return MeanFreePath;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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inline G4double G4PhotoElectricEffect::ComputeMeanFreePath(G4double GammaEnergy,
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G4Material* aMaterial)
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// returns the gamma mean free path in GEANT4 internal units
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{
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const G4ElementVector* theElementVector = aMaterial->GetElementVector() ;
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const G4double* NbOfAtomsPerVolume = aMaterial->GetVecNbOfAtomsPerVolume();
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G4double SIGMA = 0 ;
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for ( G4int elm=0 ; elm < aMaterial->GetNumberOfElements() ; elm++ )
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{
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SIGMA += NbOfAtomsPerVolume[elm] *
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ComputeCrossSectionPerAtom(GammaEnergy,
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(*theElementVector)(elm)->GetZ());
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}
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return SIGMA > DBL_MIN ? 1./SIGMA : DBL_MAX ;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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inline
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G4double G4PhotoElectricEffect::ComputeSandiaMeanFreePath(G4double GammaEnergy,
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G4Material* aMaterial)
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{
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G4double energy2 = GammaEnergy*GammaEnergy, energy3 = GammaEnergy*energy2,
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energy4 = energy2*energy2;
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G4double* SandiaCof = aMaterial->GetSandiaTable()
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->GetSandiaCofForMaterial(GammaEnergy);
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G4double SIGMA = SandiaCof[0]/GammaEnergy + SandiaCof[1]/energy2 +
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SandiaCof[2]/energy3 + SandiaCof[3]/energy4;
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return SIGMA > DBL_MIN ? 1./SIGMA : DBL_MAX ;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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inline G4double G4PhotoElectricEffect::ComputeKBindingEnergy (G4double Z)
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// Calculates the binding energy of the K electronic shell, as a function
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// of the Atomic Number, from a parametrized formula of L. Urban.
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{
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const G4double
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aK (6.6644*eV), bK (2.2077e-1*eV), cK (-3.2552e-3*eV), dK (1.8199e-5*eV);
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return Z*Z*(aK + Z* (bK + Z* (cK + Z* dK)));
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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inline G4double G4PhotoElectricEffect::ComputeL1BindingEnergy (G4double Z)
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// Calculates the binding energy of the L1 electronic shell, as a function
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// of the Atomic Number, from a parametrized formula of L. Urban.
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{
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const G4double
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aL1(-2.9179e-1*eV), bL1(8.7983e-2*eV), cL1(-1.2589e-3*eV), dL1(6.9602e-6*eV);
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return Z*Z*(aL1 + Z* (bL1 + Z* (cL1 + Z* dL1)));
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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inline G4double G4PhotoElectricEffect::ComputeL2BindingEnergy (G4double Z)
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// Calculates the binding energy of the L2 electronic shell, as a function
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// of the Atomic Number, from a parametrized formula of L. Urban.
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{
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const G4double
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aL2(-6.8606e-1*eV), bL2(1.0078e-1*eV), cL2(-1.4496e-3*eV), dL2(7.8809e-6*eV);
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return Z*Z*(aL2 + Z* (bL2 + Z* (cL2 + Z* dL2)));
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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