Files
geant4/source/processes/electromagnetic/lowenergy/src/G4PenelopeCompton.cc
T
2016-06-09 14:44:26 +02:00

756 lines
23 KiB
C++

//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4PenelopeCompton.cc,v 1.26 2006/06/29 19:40:41 gunter Exp $
// GEANT4 tag $Name: geant4-08-01 $
//
// Author: Luciano Pandola
//
// History:
// --------
// 12 Feb 2003 MG Pia const argument in SelectRandomAtomForCompton
// Migration to "cuts per region"
// 14 Feb 2003 MG Pia Corrected compilation errors and warnings
// from SUN
// Modified some variables to lowercase initial
// 10 Mar 2003 V.Ivanchenko Remove CutPerMaterial warning
// 13 Mar 2003 L.Pandola Code "cleaned"
// 20 Mar 2003 L.Pandola ReadData() changed (performance improved)
// 26 Mar 2003 L.Pandola Added fluorescence
// 24 May 2003 MGP Removed memory leak
// 09 Mar 2004 L.Pandola Bug fixed in the generation of final state
// (bug report # 585)
// 17 Mar 2004 L.Pandola Removed unnecessary calls to std::pow(a,b)
// 18 Mar 2004 L.Pandola Use of std::map (code review)
//
// -------------------------------------------------------------------
#include "G4PenelopeCompton.hh"
#include "Randomize.hh"
#include "G4ParticleDefinition.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4ForceCondition.hh"
#include "G4Gamma.hh"
#include "G4Electron.hh"
#include "G4DynamicParticle.hh"
#include "G4VParticleChange.hh"
#include "G4ThreeVector.hh"
#include "G4EnergyLossTables.hh"
#include "G4VCrossSectionHandler.hh"
#include "G4CrossSectionHandler.hh"
#include "G4VEMDataSet.hh"
#include "G4EMDataSet.hh"
#include "G4CompositeEMDataSet.hh"
#include "G4VDataSetAlgorithm.hh"
#include "G4LogLogInterpolation.hh"
#include "G4VRangeTest.hh"
#include "G4RangeTest.hh"
#include "G4ProductionCutsTable.hh"
#include "G4AtomicTransitionManager.hh"
#include "G4AtomicShell.hh"
#include "G4AtomicDeexcitation.hh"
#include "G4PenelopeIntegrator.hh"
#include "G4MaterialCutsCouple.hh"
G4PenelopeCompton::G4PenelopeCompton(const G4String& processName)
: G4VDiscreteProcess(processName),
lowEnergyLimit(250*eV),
highEnergyLimit(100*GeV),
intrinsicLowEnergyLimit(10*eV),
intrinsicHighEnergyLimit(100*GeV),
energyForIntegration(0.0),
ZForIntegration(1),
nBins(200),
cutForLowEnergySecondaryPhotons(250.0*eV)
{
if (lowEnergyLimit < intrinsicLowEnergyLimit ||
highEnergyLimit > intrinsicHighEnergyLimit)
{
G4Exception("G4PenelopeCompton::G4PenelopeCompton - energy outside intrinsic process validity range");
}
meanFreePathTable = 0;
ionizationEnergy = new std::map<G4int,G4DataVector*>;
hartreeFunction = new std::map<G4int,G4DataVector*>;
occupationNumber = new std::map<G4int,G4DataVector*>;
rangeTest = new G4RangeTest;
ReadData(); //Read data from file
if (verboseLevel > 0)
{
G4cout << GetProcessName() << " is created " << G4endl
<< "Energy range: "
<< lowEnergyLimit / keV << " keV - "
<< highEnergyLimit / GeV << " GeV"
<< G4endl;
}
}
G4PenelopeCompton::~G4PenelopeCompton()
{
delete meanFreePathTable;
delete rangeTest;
for (size_t i1=0;i1<matCrossSections->size();i1++)
{
delete (*matCrossSections)[i1];
}
delete matCrossSections;
for (G4int Z=1;Z<100;Z++)
{
if (ionizationEnergy->count(Z)) delete (ionizationEnergy->find(Z)->second);
if (hartreeFunction->count(Z)) delete (hartreeFunction->find(Z)->second);
if (occupationNumber->count(Z)) delete (occupationNumber->find(Z)->second);
}
delete ionizationEnergy;
delete hartreeFunction;
delete occupationNumber;
}
void G4PenelopeCompton::BuildPhysicsTable(const G4ParticleDefinition& )
{
G4DataVector energyVector;
G4double dBin = std::log10(highEnergyLimit/lowEnergyLimit)/nBins;
G4int i;
for (i=0;i<nBins;i++)
{
energyVector.push_back(std::pow(10.,std::log10(lowEnergyLimit)+i*dBin));
}
const G4MaterialTable* materialTable = G4Material::GetMaterialTable();
G4int nMaterials = G4Material::GetNumberOfMaterials();
G4VDataSetAlgorithm* algo = new G4LogLogInterpolation();
size_t nOfBins = energyVector.size();
size_t bin=0;
G4DataVector* energies;
G4DataVector* data;
matCrossSections = new std::vector<G4VEMDataSet*>;
G4int m;
for (m=0; m<nMaterials; m++)
{
const G4Material* material= (*materialTable)[m];
G4int nElements = material->GetNumberOfElements();
const G4ElementVector* elementVector = material->GetElementVector();
const G4double* nAtomsPerVolume = material->GetAtomicNumDensityVector();
G4VEMDataSet* setForMat = new G4CompositeEMDataSet(algo,1.,1.);
for (i=0; i<nElements; i++) {
G4int Z = (G4int) (*elementVector)[i]->GetZ();
G4double density = nAtomsPerVolume[i];
G4double cross=0.0;
energies = new G4DataVector;
data = new G4DataVector;
for (bin=0; bin<nOfBins; bin++)
{
G4double e = energyVector[bin];
energies->push_back(e);
cross = density * CrossSection(e,Z);
data->push_back(cross);
}
G4VEMDataSet* elSet = new G4EMDataSet(i,energies,data,algo,1.,1.);
setForMat->AddComponent(elSet);
}
matCrossSections->push_back(setForMat);
}
//Build the mean free path table!
G4double matCS = 0.0;
G4VEMDataSet* matCrossSet = new G4CompositeEMDataSet(algo,1.,1.);
G4VEMDataSet* materialSet = new G4CompositeEMDataSet(algo,1.,1.);
for (m=0; m<nMaterials; m++)
{
energies = new G4DataVector;
data = new G4DataVector;
const G4Material* material= (*materialTable)[m];
material= (*materialTable)[m];
for (bin=0; bin<nOfBins; bin++)
{
G4double energy = energyVector[bin];
energies->push_back(energy);
matCrossSet = (*matCrossSections)[m];
matCS = 0.0;
G4int nElm = matCrossSet->NumberOfComponents();
for(G4int j=0; j<nElm; j++) {
matCS += matCrossSet->GetComponent(j)->FindValue(energy);
}
if (matCS > 0.)
{
data->push_back(1./matCS);
}
else
{
data->push_back(DBL_MAX);
}
}
G4VEMDataSet* dataSet = new G4EMDataSet(m,energies,data,algo,1.,1.);
materialSet->AddComponent(dataSet);
}
meanFreePathTable = materialSet;
}
G4VParticleChange* G4PenelopeCompton::PostStepDoIt(const G4Track& aTrack,
const G4Step& aStep)
{
//Penelope model
aParticleChange.Initialize(aTrack);
// Dynamic particle quantities
const G4DynamicParticle* incidentPhoton = aTrack.GetDynamicParticle();
G4double photonEnergy0 = incidentPhoton->GetKineticEnergy();
if (photonEnergy0 <= lowEnergyLimit)
{
aParticleChange.ProposeTrackStatus(fStopAndKill);
aParticleChange.ProposeEnergy(0.);
aParticleChange.ProposeLocalEnergyDeposit(photonEnergy0);
return G4VDiscreteProcess::PostStepDoIt(aTrack,aStep);
}
G4ParticleMomentum photonDirection0 = incidentPhoton->GetMomentumDirection();
const G4MaterialCutsCouple* couple = aTrack.GetMaterialCutsCouple();
const G4Material* material = couple->GetMaterial();
G4int Z = SelectRandomAtomForCompton(material,photonEnergy0);
const G4int nmax = 64;
G4double rn[nmax],pac[nmax];
G4double ki,ki1,ki2,ki3,taumin,a1,a2;
G4double tau,TST;
G4double S=0.0;
G4double epsilon,cosTheta;
G4double harFunc = 0.0;
G4int occupNb= 0;
G4double ionEnergy=0.0;
G4int nosc = occupationNumber->find(Z)->second->size();
G4int iosc = nosc;
ki = photonEnergy0/electron_mass_c2;
ki2 = 2*ki+1.0;
ki3 = ki*ki;
ki1 = ki3-ki2-1.0;
taumin = 1.0/ki2;
a1 = std::log(ki2);
a2 = a1+2.0*ki*(1.0+ki)/(ki2*ki2);
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+tau*(ki1+tau*(ki2+tau*ki3)))/(ki3*tau*(1.0+tau*tau));
}while (G4UniformRand()> TST);
epsilon=tau;
cosTheta = 1.0 - (1.0-tau)/(ki*tau);
//Target shell electrons
TST = Z*G4UniformRand();
iosc = nosc;
S=0.0;
for (G4int j=0;j<nosc;j++)
{
occupNb = (G4int) (*(occupationNumber->find(Z)->second))[j];
S = S + occupNb;
if (S > TST) iosc = j;
if (S > TST) break;
}
ionEnergy = (*(ionizationEnergy->find(Z)->second))[iosc];
}while((epsilon*photonEnergy0-photonEnergy0+ionEnergy) >0);
}
else //photonEnergy0<5 MeV
{
//Incoherent scattering function for theta=PI
G4double s0=0.0;
G4double pzomc=0.0,rni=0.0;
G4double aux=0.0;
for (G4int i=0;i<nosc;i++){
ionEnergy = (*(ionizationEnergy->find(Z)->second))[i];
if (photonEnergy0 > ionEnergy)
{
G4double aux = photonEnergy0*(photonEnergy0-ionEnergy)*2.0;
harFunc = (*(hartreeFunction->find(Z)->second))[i]/fine_structure_const;
occupNb = (G4int) (*(occupationNumber->find(Z)->second))[i];
pzomc = harFunc*(aux-electron_mass_c2*ionEnergy)/
(electron_mass_c2*std::sqrt(2.0*aux+ionEnergy*ionEnergy));
if (pzomc > 0)
{
rni = 1.0-0.5*std::exp(0.5-(std::sqrt(0.5)+std::sqrt(2.0)*pzomc)*(std::sqrt(0.5)+std::sqrt(2.0)*pzomc));
}
else
{
rni = 0.5*std::exp(0.5-(std::sqrt(0.5)-std::sqrt(2.0)*pzomc)*(std::sqrt(0.5)-std::sqrt(2.0)*pzomc));
}
s0 = s0 + occupNb*rni;
}
}
//Sampling tau
G4double cdt1;
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)/(ki*tau);
S=0.0;
//Incoherent scattering function
for (G4int i=0;i<nosc;i++){
ionEnergy = (*(ionizationEnergy->find(Z)->second))[i];
if (photonEnergy0 > ionEnergy) //sum only on excitable levels
{
aux = photonEnergy0*(photonEnergy0-ionEnergy)*cdt1;
harFunc = (*(hartreeFunction->find(Z)->second))[i]/fine_structure_const;
occupNb = (G4int) (*(occupationNumber->find(Z)->second))[i];
pzomc = harFunc*(aux-electron_mass_c2*ionEnergy)/
(electron_mass_c2*std::sqrt(2.0*aux+ionEnergy*ionEnergy));
if (pzomc > 0)
{
rn[i] = 1.0-0.5*std::exp(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*std::exp(0.5-(std::sqrt(0.5)-std::sqrt(2.0)*pzomc)*(std::sqrt(0.5)-std::sqrt(2.0)*pzomc));
}
S = S + occupNb*rn[i];
pac[i] = S;
}
else
{
pac[i] = S-(1e-06);
}
}
//Rejection function
TST = S*(1.0+tau*(ki1+tau*(ki2+tau*ki3)))/(ki3*tau*(1.0+tau*tau));
}while ((G4UniformRand()*s0) > TST);
//Target electron shell
cosTheta = 1.0 - cdt1;
G4double fpzmax=0.0,fpz=0.0;
G4double A=0.0;
do
{
do
{
TST =S*G4UniformRand();
iosc=nosc;
for (G4int i=0;i<nosc;i++){
if (pac[i]>TST) iosc = i;
if (pac[i]>TST) break;
}
A = G4UniformRand()*rn[iosc];
harFunc = (*(hartreeFunction->find(Z)->second))[iosc]/fine_structure_const;
occupNb = (G4int) (*(occupationNumber->find(Z)->second))[iosc];
if (A < 0.5) {
pzomc = (std::sqrt(0.5)-std::sqrt(0.5-std::log(2.0*A)))/
(std::sqrt(2.0)*harFunc);
}
else
{
pzomc = (std::sqrt(0.5-std::log(2.0-2.0*A))-std::sqrt(0.5))/
(std::sqrt(2.0)*harFunc);
}
} 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))));
}
}
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);
aParticleChange.ProposeMomentumDirection(photonDirection1) ;
G4double photonEnergy1 = epsilon * photonEnergy0;
if (photonEnergy1 > 0.)
{
aParticleChange.ProposeEnergy(photonEnergy1) ;
}
else
{
aParticleChange.ProposeEnergy(0.) ;
aParticleChange.ProposeTrackStatus(fStopAndKill);
}
// Kinematics of the scattered electron
G4double diffEnergy = photonEnergy0*(1-epsilon);
ionEnergy = (*(ionizationEnergy->find(Z)->second))[iosc];
//G4double eKineticEnergy = diffEnergy - ionEnergy;
G4double Q2 = photonEnergy0*photonEnergy0+photonEnergy1*(photonEnergy1-2.0*photonEnergy0*cosTheta);
G4double cosThetaE; //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);
const G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance();
const G4AtomicShell* shell = transitionManager->Shell(Z,iosc);
G4double bindingEnergy = shell->BindingEnergy();
G4int shellId = shell->ShellId();
//G4cout << bindingEnergy/keV << " " << ionEnergy/keV << " keV" << G4endl;
ionEnergy = std::max(bindingEnergy,ionEnergy); //protection against energy non-conservation
G4double eKineticEnergy = diffEnergy - ionEnergy;
size_t nTotPhotons=0;
G4int nPhotons=0;
const G4ProductionCutsTable* theCoupleTable=
G4ProductionCutsTable::GetProductionCutsTable();
size_t indx = couple->GetIndex();
G4double cutg = (*(theCoupleTable->GetEnergyCutsVector(0)))[indx];
cutg = std::min(cutForLowEnergySecondaryPhotons,cutg);
G4double cute = (*(theCoupleTable->GetEnergyCutsVector(1)))[indx];
cute = std::min(cutForLowEnergySecondaryPhotons,cute);
std::vector<G4DynamicParticle*>* photonVector=0;
G4DynamicParticle* aPhoton;
G4AtomicDeexcitation deexcitationManager;
if (Z>5 && (ionEnergy > cutg || ionEnergy > cute))
{
photonVector = deexcitationManager.GenerateParticles(Z,shellId);
nTotPhotons = photonVector->size();
for (size_t k=0;k<nTotPhotons;k++){
aPhoton = (*photonVector)[k];
if (aPhoton)
{
G4double itsCut = cutg;
if (aPhoton->GetDefinition() == G4Electron::Electron()) itsCut = cute;
G4double itsEnergy = aPhoton->GetKineticEnergy();
if (itsEnergy > itsCut && itsEnergy <= ionEnergy)
{
nPhotons++;
ionEnergy -= itsEnergy;
}
else
{
delete aPhoton;
(*photonVector)[k]=0;
}
}
}
}
G4double energyDeposit =ionEnergy; //il deposito locale e' quello che rimane
G4int nbOfSecondaries=nPhotons;
// Generate the electron only if with large enough range w.r.t. cuts and safety
G4double safety = aStep.GetPostStepPoint()->GetSafety();
G4DynamicParticle* electron = 0;
if (rangeTest->Escape(G4Electron::Electron(),couple,eKineticEnergy,safety))
{
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) ;
nbOfSecondaries++;
}
else
{
energyDeposit += eKineticEnergy;
}
aParticleChange.SetNumberOfSecondaries(nbOfSecondaries);
if (electron) aParticleChange.AddSecondary(electron);
for (size_t ll=0;ll<nTotPhotons;ll++)
{
aPhoton = (*photonVector)[ll];
if (aPhoton) aParticleChange.AddSecondary(aPhoton);
}
delete photonVector;
if (energyDeposit < 0)
{
G4cout << "WARNING-"
<< "G4PenelopeCompton::PostStepDoIt - Negative energy deposit"
<< G4endl;
energyDeposit=0;
}
aParticleChange.ProposeLocalEnergyDeposit(energyDeposit);
return G4VDiscreteProcess::PostStepDoIt( aTrack, aStep);
}
G4bool G4PenelopeCompton::IsApplicable(const G4ParticleDefinition& particle)
{
return ( &particle == G4Gamma::Gamma() );
}
G4double G4PenelopeCompton::GetMeanFreePath(const G4Track& track,
G4double, // previousStepSize
G4ForceCondition*)
{
const G4DynamicParticle* photon = track.GetDynamicParticle();
G4double energy = photon->GetKineticEnergy();
G4Material* material = track.GetMaterial();
size_t materialIndex = material->GetIndex();
G4double meanFreePath;
if (energy > highEnergyLimit) meanFreePath = meanFreePathTable->FindValue(highEnergyLimit,materialIndex);
else if (energy < lowEnergyLimit) meanFreePath = DBL_MAX;
else meanFreePath = meanFreePathTable->FindValue(energy,materialIndex);
return meanFreePath;
}
void G4PenelopeCompton::ReadData()
{
char* path = getenv("G4LEDATA");
if (!path)
{
G4String excep = "G4PenelopeCompton - G4LEDATA environment variable not set!";
G4Exception(excep);
}
G4String pathString(path);
G4String pathFile = pathString + "/penelope/compton-pen.dat";
std::ifstream file(pathFile);
std::filebuf* lsdp = file.rdbuf();
if (!(lsdp->is_open()))
{
G4String excep = "G4PenelopeCompton - data file " + pathFile + " not found!";
G4Exception(excep);
}
G4int k1,test,test1;
G4double a1,a2;
G4int Z=1,nLevels=0;
G4DataVector* f;
G4DataVector* u;
G4DataVector* j;
do{
f = new G4DataVector;
u = new G4DataVector;
j = new G4DataVector;
file >> Z >> nLevels;
for (G4int h=0;h<nLevels;h++){
file >> k1 >> a1 >> a2;
f->push_back((G4double) k1);
u->push_back(a1);
j->push_back(a2);
}
ionizationEnergy->insert(std::make_pair(Z,u));
hartreeFunction->insert(std::make_pair(Z,j));
occupationNumber->insert(std::make_pair(Z,f));
file >> test >> test1; //-1 -1 close the data for each Z
if (test > 0) {
G4String excep = "G4PenelopeCompton - data file corrupted!";
G4Exception(excep);
}
}while (test != -2); //the very last Z is closed with -2 instead of -1
}
G4double G4PenelopeCompton::CrossSection(G4double energy,G4int Z)
{
G4double cs=0.0;
energyForIntegration=energy;
ZForIntegration = Z;
if (energy< 5*MeV)
{
G4PenelopeIntegrator<G4PenelopeCompton,G4double (G4PenelopeCompton::*)(G4double)> theIntegrator;
cs = theIntegrator.Calculate(this,&G4PenelopeCompton::DifferentialCrossSection,-1.0,1.0,1e-05);
}
else
{
G4double ki=energy/electron_mass_c2;
G4double ki3=ki*ki;
G4double ki2=1.0+2*ki;
G4double ki1=ki3-ki2-1.0;
G4double t0=1.0/(ki2);
G4double csl = 0.5*ki3*t0*t0+ki2*t0+ki1*std::log(t0)-(1.0/t0);
G4int nosc = occupationNumber->find(Z)->second->size();
for (G4int i=0;i<nosc;i++)
{
G4double ionEnergy = (*(ionizationEnergy->find(Z)->second))[i];
G4double tau=(energy-ionEnergy)/energy;
if (tau > t0)
{
G4double csu = 0.5*ki3*tau*tau+ki2*tau+ki1*std::log(tau)-(1.0/tau);
G4int f = (G4int) (*(occupationNumber->find(Z)->second))[i];
cs = cs + f*(csu-csl);
}
}
cs=pi*classic_electr_radius*classic_electr_radius*cs/(ki*ki3);
}
return cs;
}
G4double G4PenelopeCompton::DifferentialCrossSection(G4double cosTheta)
{
const G4double k2 = std::sqrt(2.0);
const G4double k1 = std::sqrt(0.5);
const G4double k12 = 0.5;
G4double cdt1 = 1.0-cosTheta;
G4double energy = energyForIntegration;
G4int Z = ZForIntegration;
G4double ionEnergy=0.0,Pzimax=0.0,XKN=0.0;
G4double diffCS=0.0;
G4double x=0.0,siap=0.0;
G4double harFunc=0.0;
G4int occupNb;
//energy of Compton line;
G4double EOEC = 1.0+(energy/electron_mass_c2)*cdt1;
G4double ECOE = 1.0/EOEC;
//Incoherent scattering function (analytical profile)
G4double sia = 0.0;
G4int nosc = occupationNumber->find(Z)->second->size();
for (G4int i=0;i<nosc;i++){
ionEnergy = (*(ionizationEnergy->find(Z)->second))[i];
//Sum only of those shells for which E>Eion
if (energy > ionEnergy)
{
G4double aux = energy * (energy-ionEnergy)*cdt1;
Pzimax = (aux - electron_mass_c2*ionEnergy)/(electron_mass_c2*std::sqrt(2*aux+ionEnergy*ionEnergy));
harFunc = (*(hartreeFunction->find(Z)->second))[i]/fine_structure_const;
occupNb = (G4int) (*(occupationNumber->find(Z)->second))[i];
x = harFunc*Pzimax;
if (x > 0)
{
siap = 1.0-0.5*std::exp(k12-(k1+k2*x)*(k1+k2*x));
}
else
{
siap = 0.5*std::exp(k12-(k1-k2*x)*(k1-k2*x));
}
sia = sia + occupNb*siap; //sum of all contributions;
}
}
XKN = EOEC+ECOE-1+cosTheta*cosTheta;
diffCS = pi*classic_electr_radius*classic_electr_radius*ECOE*ECOE*XKN*sia;
return diffCS;
}
G4int G4PenelopeCompton::SelectRandomAtomForCompton(const G4Material* material,G4double energy) const
{
G4int nElements = material->GetNumberOfElements();
//Special case: the material consists of one element
if (nElements == 1)
{
G4int Z = (G4int) material->GetZ();
return Z;
}
//Composite material
const G4ElementVector* elementVector = material->GetElementVector();
size_t materialIndex = material->GetIndex();
G4VEMDataSet* materialSet = (*matCrossSections)[materialIndex];
G4double materialCrossSection0 = 0.0;
G4DataVector cross;
cross.clear();
G4int i;
for (i=0;i<nElements;i++)
{
G4double cr = (materialSet->GetComponent(i))->FindValue(energy);
materialCrossSection0 += cr;
cross.push_back(materialCrossSection0); //cumulative cross section
}
G4double random = G4UniformRand()*materialCrossSection0;
for (i=0;i<nElements;i++)
{
if (random <= cross[i]) return (G4int) (*elementVector)[i]->GetZ();
}
//It should never get here
return 0;
}