392 lines
14 KiB
C++
392 lines
14 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: G4LivermoreBremsstrahlungModel.cc,v 1.6 2009/06/11 15:47:08 mantero Exp $
|
|
// GEANT4 tag $Name: geant4-09-03 $
|
|
//
|
|
// Author: Luciano Pandola
|
|
//
|
|
// History:
|
|
// --------
|
|
// 03 Mar 2009 L Pandola Migration from process to model
|
|
// 12 Apr 2009 V Ivanchenko Cleanup initialisation and generation of secondaries:
|
|
// - apply internal high-energy limit only in constructor
|
|
// - do not apply low-energy limit (default is 0)
|
|
// - added MinEnergyCut method
|
|
// - do not change track status
|
|
// - do not initialize element selectors
|
|
// - use cut value from the interface
|
|
// - fixed bug in sampling of angles between keV and MeV
|
|
// 19 May 2009 L Pandola Explicitely set to zero pointers deleted in
|
|
// Initialise(), since they might be checked later on
|
|
//
|
|
|
|
#include "G4LivermoreBremsstrahlungModel.hh"
|
|
#include "G4ParticleDefinition.hh"
|
|
#include "G4MaterialCutsCouple.hh"
|
|
|
|
#include "G4DynamicParticle.hh"
|
|
#include "G4Element.hh"
|
|
#include "G4Gamma.hh"
|
|
#include "G4Electron.hh"
|
|
#include "G4SemiLogInterpolation.hh"
|
|
//
|
|
#include "G4VBremAngularDistribution.hh"
|
|
#include "G4ModifiedTsai.hh"
|
|
#include "G4Generator2BS.hh"
|
|
#include "G4Generator2BN.hh"
|
|
//
|
|
#include "G4BremsstrahlungCrossSectionHandler.hh"
|
|
//
|
|
#include "G4VEnergySpectrum.hh"
|
|
#include "G4eBremsstrahlungSpectrum.hh"
|
|
|
|
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|
|
|
|
|
G4LivermoreBremsstrahlungModel::G4LivermoreBremsstrahlungModel(const G4ParticleDefinition*,
|
|
const G4String& nam)
|
|
:G4VEmModel(nam),isInitialised(false),crossSectionHandler(0),
|
|
energySpectrum(0)
|
|
{
|
|
fIntrinsicLowEnergyLimit = 10.0*eV;
|
|
fIntrinsicHighEnergyLimit = 100.0*GeV;
|
|
fNBinEnergyLoss = 360;
|
|
// SetLowEnergyLimit(fIntrinsicLowEnergyLimit);
|
|
SetHighEnergyLimit(fIntrinsicHighEnergyLimit);
|
|
//
|
|
verboseLevel = 0;
|
|
//
|
|
generatorName = "tsai";
|
|
angularDistribution = new G4ModifiedTsai("TsaiGenerator"); //default generator
|
|
//
|
|
TsaiAngularDistribution = new G4ModifiedTsai("TsaiGenerator");
|
|
//
|
|
}
|
|
|
|
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|
|
|
G4LivermoreBremsstrahlungModel::~G4LivermoreBremsstrahlungModel()
|
|
{
|
|
if (crossSectionHandler) delete crossSectionHandler;
|
|
if (energySpectrum) delete energySpectrum;
|
|
energyBins.clear();
|
|
delete angularDistribution;
|
|
delete TsaiAngularDistribution;
|
|
}
|
|
|
|
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|
|
|
void G4LivermoreBremsstrahlungModel::Initialise(const G4ParticleDefinition* particle,
|
|
const G4DataVector& cuts)
|
|
{
|
|
//Check that the Livermore Bremsstrahlung is NOT attached to e+
|
|
if (particle != G4Electron::Electron())
|
|
{
|
|
G4cout << "ERROR: Livermore Bremsstrahlung Model is applicable only to electrons"
|
|
<< G4endl;
|
|
G4cout << "It cannot be registered to " << particle->GetParticleName() << G4endl;
|
|
G4Exception();
|
|
}
|
|
//Prepare energy spectrum
|
|
if (energySpectrum)
|
|
{
|
|
delete energySpectrum;
|
|
energySpectrum = 0;
|
|
}
|
|
|
|
energyBins.clear();
|
|
for(size_t i=0; i<15; i++)
|
|
{
|
|
G4double x = 0.1*((G4double)i);
|
|
if(i == 0) x = 0.01;
|
|
if(i == 10) x = 0.95;
|
|
if(i == 11) x = 0.97;
|
|
if(i == 12) x = 0.99;
|
|
if(i == 13) x = 0.995;
|
|
if(i == 14) x = 1.0;
|
|
energyBins.push_back(x);
|
|
}
|
|
const G4String dataName("/brem/br-sp.dat");
|
|
energySpectrum = new G4eBremsstrahlungSpectrum(energyBins,dataName);
|
|
|
|
if (verboseLevel > 0)
|
|
G4cout << "G4eBremsstrahlungSpectrum is initialized" << G4endl;
|
|
|
|
//Initialize cross section handler
|
|
if (crossSectionHandler)
|
|
{
|
|
delete crossSectionHandler;
|
|
crossSectionHandler = 0;
|
|
}
|
|
G4VDataSetAlgorithm* interpolation = new G4SemiLogInterpolation();
|
|
crossSectionHandler = new G4BremsstrahlungCrossSectionHandler(energySpectrum,interpolation);
|
|
crossSectionHandler->Initialise(0,LowEnergyLimit(),HighEnergyLimit(),
|
|
fNBinEnergyLoss);
|
|
crossSectionHandler->Clear();
|
|
crossSectionHandler->LoadShellData("brem/br-cs-");
|
|
//This is used to retrieve cross section values later on
|
|
crossSectionHandler->BuildMeanFreePathForMaterials(&cuts);
|
|
|
|
if (verboseLevel > 0)
|
|
{
|
|
G4cout << "Livermore Bremsstrahlung model is initialized " << G4endl
|
|
<< "Energy range: "
|
|
<< LowEnergyLimit() / keV << " keV - "
|
|
<< HighEnergyLimit() / GeV << " GeV"
|
|
<< G4endl;
|
|
}
|
|
|
|
if (verboseLevel > 1)
|
|
{
|
|
G4cout << "Cross section data: " << G4endl;
|
|
crossSectionHandler->PrintData();
|
|
G4cout << "Parameters: " << G4endl;
|
|
energySpectrum->PrintData();
|
|
}
|
|
|
|
if(isInitialised) return;
|
|
fParticleChange = GetParticleChangeForLoss();
|
|
isInitialised = true;
|
|
}
|
|
|
|
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|
|
|
G4double G4LivermoreBremsstrahlungModel::MinEnergyCut(const G4ParticleDefinition*,
|
|
const G4MaterialCutsCouple*)
|
|
{
|
|
return 250.*eV;
|
|
}
|
|
|
|
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|
|
|
G4double
|
|
G4LivermoreBremsstrahlungModel::ComputeCrossSectionPerAtom(const G4ParticleDefinition*,
|
|
G4double energy,
|
|
G4double Z, G4double,
|
|
G4double cutEnergy,
|
|
G4double)
|
|
{
|
|
G4int iZ = (G4int) Z;
|
|
if (!crossSectionHandler)
|
|
{
|
|
G4cout << "G4LivermoreBremsstrahlungModel::ComputeCrossSectionPerAtom" << G4endl;
|
|
G4cout << "The cross section handler is not correctly initialized" << G4endl;
|
|
G4Exception();
|
|
}
|
|
|
|
//The cut is already included in the crossSectionHandler
|
|
G4double cs =
|
|
crossSectionHandler->GetCrossSectionAboveThresholdForElement(energy,cutEnergy,iZ);
|
|
|
|
if (verboseLevel > 1)
|
|
{
|
|
G4cout << "G4LivermoreBremsstrahlungModel " << G4endl;
|
|
G4cout << "Cross section for gamma emission > " << cutEnergy/keV << " keV at " <<
|
|
energy/keV << " keV and Z = " << iZ << " --> " << cs/barn << " barn" << G4endl;
|
|
}
|
|
return cs;
|
|
}
|
|
|
|
|
|
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|
|
|
G4double G4LivermoreBremsstrahlungModel::ComputeDEDXPerVolume(const G4Material* material,
|
|
const G4ParticleDefinition* ,
|
|
G4double kineticEnergy,
|
|
G4double cutEnergy)
|
|
{
|
|
G4double sPower = 0.0;
|
|
|
|
const G4ElementVector* theElementVector = material->GetElementVector();
|
|
size_t NumberOfElements = material->GetNumberOfElements() ;
|
|
const G4double* theAtomicNumDensityVector =
|
|
material->GetAtomicNumDensityVector();
|
|
|
|
// loop for elements in the material
|
|
for (size_t iel=0; iel<NumberOfElements; iel++ )
|
|
{
|
|
G4int iZ = (G4int)((*theElementVector)[iel]->GetZ());
|
|
G4double e = energySpectrum->AverageEnergy(iZ, 0.0,cutEnergy,
|
|
kineticEnergy);
|
|
G4double cs= crossSectionHandler->FindValue(iZ,kineticEnergy);
|
|
sPower += e * cs * theAtomicNumDensityVector[iel];
|
|
}
|
|
|
|
if (verboseLevel > 2)
|
|
{
|
|
G4cout << "G4LivermoreBremsstrahlungModel " << G4endl;
|
|
G4cout << "Stopping power < " << cutEnergy/keV << " keV at " <<
|
|
kineticEnergy/keV << " keV = " << sPower/(keV/mm) << " keV/mm" << G4endl;
|
|
}
|
|
|
|
return sPower;
|
|
}
|
|
|
|
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|
|
|
void G4LivermoreBremsstrahlungModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
|
|
const G4MaterialCutsCouple* couple,
|
|
const G4DynamicParticle* aDynamicParticle,
|
|
G4double energyCut,
|
|
G4double)
|
|
{
|
|
|
|
G4double kineticEnergy = aDynamicParticle->GetKineticEnergy();
|
|
|
|
// this is neede for pathalogical cases of no ionisation
|
|
if (kineticEnergy <= fIntrinsicLowEnergyLimit)
|
|
{
|
|
fParticleChange->SetProposedKineticEnergy(0.);
|
|
fParticleChange->ProposeLocalEnergyDeposit(kineticEnergy);
|
|
return;
|
|
}
|
|
|
|
//Sample material
|
|
G4int Z = crossSectionHandler->SelectRandomAtom(couple, kineticEnergy);
|
|
|
|
//Sample gamma energy
|
|
G4double tGamma = energySpectrum->SampleEnergy(Z, energyCut, kineticEnergy, kineticEnergy);
|
|
G4double totalEnergy = kineticEnergy + electron_mass_c2;
|
|
G4double finalEnergy = kineticEnergy - tGamma; // electron final energy
|
|
G4double theta = 0;
|
|
|
|
if (tGamma == 0.) //nothing happens
|
|
return;
|
|
|
|
//Sample gamma direction
|
|
//Use alternative algorithms, if it is the case.
|
|
if((kineticEnergy < MeV && kineticEnergy > keV))
|
|
{
|
|
theta = angularDistribution->PolarAngle(kineticEnergy,finalEnergy,Z);
|
|
}
|
|
else
|
|
//Otherwise, use tsai
|
|
{
|
|
theta = TsaiAngularDistribution->PolarAngle(kineticEnergy,finalEnergy,Z);
|
|
}
|
|
|
|
G4double phi = twopi * G4UniformRand();
|
|
G4double dirZ = std::cos(theta);
|
|
G4double sinTheta = std::sqrt(1. - dirZ*dirZ);
|
|
G4double dirX = sinTheta*std::cos(phi);
|
|
G4double dirY = sinTheta*std::sin(phi);
|
|
|
|
G4ThreeVector gammaDirection (dirX, dirY, dirZ);
|
|
G4ThreeVector electronDirection = aDynamicParticle->GetMomentumDirection();
|
|
|
|
//Update the incident particle
|
|
gammaDirection.rotateUz(electronDirection);
|
|
|
|
if (finalEnergy < 0.)
|
|
{
|
|
// Kinematic problem
|
|
tGamma = kineticEnergy;
|
|
fParticleChange->SetProposedKineticEnergy(0.);
|
|
}
|
|
else
|
|
{
|
|
G4double momentum = std::sqrt((totalEnergy + electron_mass_c2)*kineticEnergy);
|
|
G4double finalX = momentum*electronDirection.x() - tGamma*gammaDirection.x();
|
|
G4double finalY = momentum*electronDirection.y() - tGamma*gammaDirection.y();
|
|
G4double finalZ = momentum*electronDirection.z() - tGamma*gammaDirection.z();
|
|
G4double norm = 1./std::sqrt(finalX*finalX + finalY*finalY + finalZ*finalZ);
|
|
|
|
fParticleChange->ProposeMomentumDirection(finalX*norm, finalY*norm, finalZ*norm);
|
|
fParticleChange->SetProposedKineticEnergy(finalEnergy);
|
|
}
|
|
|
|
//Generate the bremsstrahlung gamma
|
|
G4DynamicParticle* aGamma= new G4DynamicParticle (G4Gamma::Gamma(),
|
|
gammaDirection, tGamma);
|
|
fvect->push_back(aGamma);
|
|
|
|
if (verboseLevel > 1)
|
|
{
|
|
G4cout << "-----------------------------------------------------------" << G4endl;
|
|
G4cout << "Energy balance from G4LivermoreBremsstrahlung" << G4endl;
|
|
G4cout << "Incoming primary energy: " << kineticEnergy/keV << " keV" << G4endl;
|
|
G4cout << "-----------------------------------------------------------" << G4endl;
|
|
G4cout << "Outgoing primary energy: " << finalEnergy/keV << " keV" << G4endl;
|
|
G4cout << "Gamma ray " << tGamma/keV << " keV" << G4endl;
|
|
G4cout << "Total final state: " << (finalEnergy+tGamma)/keV << " keV" << G4endl;
|
|
G4cout << "-----------------------------------------------------------" << G4endl;
|
|
}
|
|
if (verboseLevel > 0)
|
|
{
|
|
G4double energyDiff = std::fabs(finalEnergy+tGamma-kineticEnergy);
|
|
if (energyDiff > 0.05*keV)
|
|
G4cout << "G4LivermoreBremsstrahlung WARNING: problem with energy conservation: "
|
|
<< (finalEnergy+tGamma)/keV << " keV (final) vs. "
|
|
<< kineticEnergy/keV << " keV (initial)" << G4endl;
|
|
}
|
|
return;
|
|
}
|
|
|
|
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|
|
|
void
|
|
G4LivermoreBremsstrahlungModel::SetAngularGenerator(G4VBremAngularDistribution* distribution)
|
|
{
|
|
if(angularDistribution == distribution) return;
|
|
if(angularDistribution) delete angularDistribution;
|
|
angularDistribution = distribution;
|
|
angularDistribution->PrintGeneratorInformation();
|
|
}
|
|
|
|
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|
|
|
void G4LivermoreBremsstrahlungModel::SetAngularGenerator(const G4String& name)
|
|
{
|
|
if(name == generatorName) return;
|
|
if (name == "tsai")
|
|
{
|
|
delete angularDistribution;
|
|
angularDistribution = new G4ModifiedTsai("TsaiGenerator");
|
|
generatorName = name;
|
|
}
|
|
else if (name == "2bn")
|
|
{
|
|
delete angularDistribution;
|
|
angularDistribution = new G4Generator2BN("2BNGenerator");
|
|
generatorName = name;
|
|
}
|
|
else if (name == "2bs")
|
|
{
|
|
delete angularDistribution;
|
|
angularDistribution = new G4Generator2BS("2BSGenerator");
|
|
generatorName = name;
|
|
}
|
|
else
|
|
{
|
|
G4cout << "### G4LivermoreBremsstrahlungModel::SetAngularGenerator WARNING:"
|
|
<< " generator <" << name << "> is not known" << G4endl;
|
|
return;
|
|
|
|
}
|
|
|
|
angularDistribution->PrintGeneratorInformation();
|
|
}
|