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geant4/source/processes/electromagnetic/lowenergy/src/G4LivermoreBremsstrahlungModel.cc
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Gabriele Cosmo 860a2b92bf Import Geant4 11.2.0 source tree
2023-12-08 10:43:34 +01:00

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//
// ********************************************************************
// * 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. *
// ********************************************************************
//
//
// -------------------------------------------------------------------
//
// GEANT4 Class file
//
//
// File name: G4LivermoreBremsstrahlungModel
//
// Author: Vladimir Ivanchenko use inheritance from Andreas Schaelicke
// base class implementing ultra relativistic bremsstrahlung
// model
//
// Creation date: 04.10.2011
//
// Modifications:
//
// -------------------------------------------------------------------
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#include "G4LivermoreBremsstrahlungModel.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4Electron.hh"
#include "G4Positron.hh"
#include "G4Gamma.hh"
#include "Randomize.hh"
#include "G4AutoLock.hh"
#include "G4Material.hh"
#include "G4Element.hh"
#include "G4ElementVector.hh"
#include "G4ProductionCutsTable.hh"
#include "G4ParticleChangeForLoss.hh"
#include "G4Generator2BS.hh"
#include "G4Physics2DVector.hh"
#include "G4Exp.hh"
#include "G4Log.hh"
#include "G4ios.hh"
#include <fstream>
#include <iomanip>
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
namespace { G4Mutex LivermoreBremsstrahlungModelMutex = G4MUTEX_INITIALIZER; }
using namespace std;
G4Physics2DVector* G4LivermoreBremsstrahlungModel::dataSB[] = {nullptr};
G4double G4LivermoreBremsstrahlungModel::ylimit[] = {0.0};
G4double G4LivermoreBremsstrahlungModel::expnumlim = -12.;
static const G4double emaxlog = 4*G4Log(10.);
static const G4double alpha = CLHEP::twopi*CLHEP::fine_structure_const;
static const G4double epeaklimit= 300*CLHEP::MeV;
static const G4double elowlimit = 20*CLHEP::keV;
G4LivermoreBremsstrahlungModel::G4LivermoreBremsstrahlungModel(
const G4ParticleDefinition* p, const G4String& nam)
: G4eBremsstrahlungRelModel(p,nam),useBicubicInterpolation(false)
{
SetLowEnergyLimit(10.0*eV);
SetAngularDistribution(new G4Generator2BS());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4LivermoreBremsstrahlungModel::~G4LivermoreBremsstrahlungModel()
{
if(IsMaster()) {
for(size_t i=0; i<101; ++i) {
if(dataSB[i]) {
delete dataSB[i];
dataSB[i] = nullptr;
}
}
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4LivermoreBremsstrahlungModel::Initialise(const G4ParticleDefinition* p,
const G4DataVector& cuts)
{
// Access to elements
if(IsMaster()) {
// check environment variable
// Build the complete string identifying the file with the data set
const char* path = G4FindDataDir("G4LEDATA");
const G4ElementTable* theElmTable = G4Element::GetElementTable();
size_t numOfElm = G4Element::GetNumberOfElements();
if(numOfElm > 0) {
for(size_t i=0; i<numOfElm; ++i) {
G4int Z = (*theElmTable)[i]->GetZasInt();
if(Z < 1) { Z = 1; }
else if(Z > 100) { Z = 100; }
//G4cout << "Z= " << Z << G4endl;
// Initialisation
if(!dataSB[Z]) { ReadData(Z, path); }
}
}
}
G4eBremsstrahlungRelModel::Initialise(p, cuts);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4String G4LivermoreBremsstrahlungModel::DirectoryPath() const
{
return "/livermore/brem/br";
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4LivermoreBremsstrahlungModel::ReadData(G4int Z, const char* path)
{
if(dataSB[Z]) { return; }
const char* datadir = path;
if(nullptr == datadir) {
datadir = G4FindDataDir("G4LEDATA");
if(!datadir) {
G4Exception("G4LivermoreBremsstrahlungModel::ReadData()","em0006",
FatalException,"Environment variable G4LEDATA not defined");
return;
}
}
std::ostringstream ost;
ost << datadir << DirectoryPath() << Z;
std::ifstream fin(ost.str().c_str());
if( !fin.is_open()) {
G4ExceptionDescription ed;
ed << "Bremsstrahlung data file <" << ost.str().c_str()
<< "> is not opened!";
G4Exception("G4LivermoreBremsstrahlungModel::ReadData()","em0003",
FatalException,ed,
"G4LEDATA version should be G4EMLOW8.0 or later.");
return;
}
//G4cout << "G4LivermoreBremsstrahlungModel read from <" << ost.str().c_str()
// << ">" << G4endl;
G4Physics2DVector* v = new G4Physics2DVector();
if(v->Retrieve(fin)) {
if(useBicubicInterpolation) { v->SetBicubicInterpolation(true); }
dataSB[Z] = v;
ylimit[Z] = v->Value(0.97, emaxlog, idx, idy);
} else {
G4ExceptionDescription ed;
ed << "Bremsstrahlung data file <" << ost.str().c_str()
<< "> is not retrieved!";
G4Exception("G4LivermoreBremsstrahlungModel::ReadData()","em0005",
FatalException,ed,
"G4LEDATA version should be G4EMLOW8.0 or later.");
delete v;
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double
G4LivermoreBremsstrahlungModel::ComputeDXSectionPerAtom(G4double gammaEnergy)
{
if(gammaEnergy < 0.0 || fPrimaryKinEnergy <= 0.0) { return 0.0; }
G4double x = gammaEnergy/fPrimaryKinEnergy;
G4double y = G4Log(fPrimaryKinEnergy/MeV);
G4int Z = fCurrentIZ;
//G4cout << "G4LivermoreBremsstrahlungModel::ComputeDXSectionPerAtom Z= " << Z
// << " x= " << x << " y= " << y << " " << dataSB[Z] << G4endl;
if(!dataSB[Z]) { InitialiseForElement(0, Z); }
G4double invb2 = fPrimaryTotalEnergy*fPrimaryTotalEnergy/(fPrimaryKinEnergy
*(fPrimaryKinEnergy + 2.*fPrimaryParticleMass));
G4double cross = dataSB[Z]->Value(x,y,idx,idy)*invb2*millibarn/gBremFactor;
if(!fIsElectron) {
G4double invbeta1 = sqrt(invb2);
G4double e2 = fPrimaryKinEnergy - gammaEnergy;
if(e2 > 0.0) {
G4double invbeta2 = (e2 + fPrimaryParticleMass)
/sqrt(e2*(e2 + 2.*fPrimaryParticleMass));
G4double xxx = alpha*fCurrentIZ*(invbeta1 - invbeta2);
if(xxx < expnumlim) { cross = 0.0; }
else { cross *= G4Exp(xxx); }
} else {
cross = 0.0;
}
}
return cross;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void
G4LivermoreBremsstrahlungModel::SampleSecondaries(
std::vector<G4DynamicParticle*>* vdp,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* dp,
G4double cutEnergy,
G4double maxEnergy)
{
G4double kineticEnergy = dp->GetKineticEnergy();
G4double cut = std::min(cutEnergy, kineticEnergy);
G4double emax = std::min(maxEnergy, kineticEnergy);
if(cut >= emax) { return; }
// sets total energy, kinetic energy and density correction
SetupForMaterial(fPrimaryParticle, couple->GetMaterial(), kineticEnergy);
const G4Element* elm =
SelectRandomAtom(couple,fPrimaryParticle,kineticEnergy,cut,emax);
fCurrentIZ = elm->GetZasInt();
G4int Z = fCurrentIZ;
G4double totMomentum = sqrt(kineticEnergy*(fPrimaryTotalEnergy+electron_mass_c2));
/*
G4cout << "G4LivermoreBremsstrahlungModel::SampleSecondaries E(MeV)= "
<< kineticEnergy/MeV
<< " Z= " << Z << " cut(MeV)= " << cut/MeV
<< " emax(MeV)= " << emax/MeV << " corr= " << fDensityCorr << G4endl;
*/
G4double xmin = G4Log(cut*cut + fDensityCorr);
G4double xmax = G4Log(emax*emax + fDensityCorr);
G4double y = G4Log(kineticEnergy/MeV);
G4double gammaEnergy, v;
// majoranta
G4double x0 = cut/kineticEnergy;
G4double vmax = dataSB[Z]->Value(x0, y, idx, idy)*1.02;
// majoranta corrected for e-
if(fIsElectron && x0 < 0.97 &&
((kineticEnergy > epeaklimit) || (kineticEnergy < elowlimit))) {
G4double ylim = std::min(ylimit[Z],1.1*dataSB[Z]->Value(0.97,y,idx,idy));
if(ylim > vmax) { vmax = ylim; }
}
if(x0 < 0.05) { vmax *= 1.2; }
do {
//++ncount;
G4double x = G4Exp(xmin + G4UniformRand()*(xmax - xmin)) - fDensityCorr;
if(x < 0.0) { x = 0.0; }
gammaEnergy = sqrt(x);
G4double x1 = gammaEnergy/kineticEnergy;
v = dataSB[Z]->Value(x1, y, idx, idy);
// correction for positrons
if(!fIsElectron) {
G4double e1 = kineticEnergy - cut;
G4double invbeta1 = (e1 + fPrimaryParticleMass)
/sqrt(e1*(e1 + 2*fPrimaryParticleMass));
G4double e2 = kineticEnergy - gammaEnergy;
G4double invbeta2 = (e2 + fPrimaryParticleMass)
/sqrt(e2*(e2 + 2*fPrimaryParticleMass));
G4double xxx = twopi*fine_structure_const*fCurrentIZ*(invbeta1 - invbeta2);
if(xxx < expnumlim) { v = 0.0; }
else { v *= G4Exp(xxx); }
}
if (v > 1.05*vmax && nwarn < 5) {
++nwarn;
G4ExceptionDescription ed;
ed << "### G4LivermoreBremsstrahlungModel Warning: Majoranta exceeded! "
<< v << " > " << vmax << " by " << v/vmax
<< " Egamma(MeV)= " << gammaEnergy
<< " Ee(MeV)= " << kineticEnergy
<< " Z= " << Z << " " << fPrimaryParticle->GetParticleName();
if ( 20 == nwarn ) {
ed << "\n ### G4LivermoreBremsstrahlungModel Warnings stopped";
}
G4Exception("G4LivermoreBremsstrahlungModel::SampleScattering","em0044",
JustWarning, ed,"");
}
} while (v < vmax*G4UniformRand());
//
// angles of the emitted gamma. ( Z - axis along the parent particle)
// use general interface
//
G4ThreeVector gammaDirection =
GetAngularDistribution()->SampleDirection(dp,fPrimaryTotalEnergy-gammaEnergy,
Z, couple->GetMaterial());
// create G4DynamicParticle object for the Gamma
G4DynamicParticle* gamma =
new G4DynamicParticle(fGammaParticle,gammaDirection,gammaEnergy);
vdp->push_back(gamma);
G4ThreeVector direction = (totMomentum*dp->GetMomentumDirection()
- gammaEnergy*gammaDirection).unit();
/*
G4cout << "### G4SBModel: v= "
<< " Eg(MeV)= " << gammaEnergy
<< " Ee(MeV)= " << kineticEnergy
<< " DirE " << direction << " DirG " << gammaDirection
<< G4endl;
*/
// energy of primary
G4double finalE = kineticEnergy - gammaEnergy;
// stop tracking and create new secondary instead of primary
if(gammaEnergy > SecondaryThreshold()) {
fParticleChange->ProposeTrackStatus(fStopAndKill);
fParticleChange->SetProposedKineticEnergy(0.0);
G4DynamicParticle* el =
new G4DynamicParticle(const_cast<G4ParticleDefinition*>(fPrimaryParticle),
direction, finalE);
vdp->push_back(el);
// continue tracking
} else {
fParticleChange->SetProposedMomentumDirection(direction);
fParticleChange->SetProposedKineticEnergy(finalE);
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
void G4LivermoreBremsstrahlungModel::InitialiseForElement(
const G4ParticleDefinition*,
G4int Z)
{
G4AutoLock l(&LivermoreBremsstrahlungModelMutex);
if(!dataSB[Z]) { ReadData(Z); }
l.unlock();
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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