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geant4/source/processes/electromagnetic/utils/src/G4EmSaturation.cc
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//
// ********************************************************************
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//
// $Id: G4EmSaturation.cc,v 1.11 2010/10/25 17:23:01 vnivanch Exp $
// GEANT4 tag $Name: geant4-09-04 $
//
// -------------------------------------------------------------------
//
// GEANT4 Class file
//
//
// File name: G4EmSaturation
//
// Author: Vladimir Ivanchenko
//
// Creation date: 18.02.2008
//
// Modifications:
//
// -------------------------------------------------------------
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#include "G4EmSaturation.hh"
#include "G4LossTableManager.hh"
#include "G4NistManager.hh"
#include "G4Material.hh"
#include "G4MaterialCutsCouple.hh"
#include "G4Electron.hh"
#include "G4Proton.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4EmSaturation::G4EmSaturation()
{
verbose = 1;
manager = 0;
curMaterial = 0;
curBirks = 0.0;
curRatio = 1.0;
curChargeSq = 1.0;
nMaterials = 0;
electron = 0;
proton = 0;
nist = G4NistManager::Instance();
Initialise();
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4EmSaturation::~G4EmSaturation()
{}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4EmSaturation::VisibleEnergyDeposition(
const G4ParticleDefinition* p,
const G4MaterialCutsCouple* couple,
G4double length,
G4double edep,
G4double niel)
{
if(edep <= 0.0) { return 0.0; }
G4double evis = edep;
G4double bfactor = FindBirksCoefficient(couple->GetMaterial());
if(bfactor > 0.0) {
G4int pdgCode = p->GetPDGEncoding();
// atomic relaxations for gamma incident
if(22 == pdgCode) {
evis /= (1.0 + bfactor*edep/manager->GetRange(electron,edep,couple));
// energy loss
} else {
// protections
G4double nloss = niel;
if(nloss < 0.0) nloss = 0.0;
G4double eloss = edep - nloss;
// neutrons
if(2112 == pdgCode || eloss < 0.0 || length <= 0.0) {
nloss = edep;
eloss = 0.0;
}
// continues energy loss
if(eloss > 0.0) { eloss /= (1.0 + bfactor*eloss/length); }
// non-ionizing energy loss
if(nloss > 0.0) {
if(!proton) { proton = G4Proton::Proton(); }
G4double escaled = nloss*curRatio;
G4double s = manager->GetRange(proton,escaled,couple)/curChargeSq;
nloss /= (1.0 + bfactor*nloss/s);
}
evis = eloss + nloss;
}
}
return evis;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4EmSaturation::FindG4BirksCoefficient(const G4Material* mat)
{
G4String name = mat->GetName();
// is this material in the vector?
for(G4int j=0; j<nG4Birks; ++j) {
if(name == g4MatNames[j]) {
if(verbose > 0)
G4cout << "### G4EmSaturation::FindG4BirksCoefficient for "
<< name << " is " << g4MatData[j]*MeV/mm << " mm/MeV "
<< G4endl;
return g4MatData[j];
}
}
return FindBirksCoefficient(mat);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4EmSaturation::FindBirksCoefficient(const G4Material* mat)
{
// electron should exist in any case
if(!manager) {
manager = G4LossTableManager::Instance();
electron= G4Electron::Electron();
}
if(mat == curMaterial) { return curBirks; }
curMaterial = mat;
curBirks = 0.0;
curRatio = 1.0;
curChargeSq = 1.0;
// seach in the run-time list
for(G4int i=0; i<nMaterials; ++i) {
if(mat == matPointers[i]) {
curBirks = mat->GetIonisation()->GetBirksConstant();
curRatio = massFactors[i];
curChargeSq = effCharges[i];
return curBirks;
}
}
G4String name = mat->GetName();
curBirks = mat->GetIonisation()->GetBirksConstant();
// material has no Birks coeffitient defined
// seach in the Geant4 list
if(curBirks == 0.0) {
for(G4int j=0; j<nG4Birks; ++j) {
if(name == g4MatNames[j]) {
mat->GetIonisation()->SetBirksConstant(g4MatData[j]);
curBirks = g4MatData[j];
break;
}
}
}
if(curBirks == 0.0 && verbose > 0) {
G4cout << "### G4EmSaturation::FindBirksCoefficient fails "
" for material " << name << G4endl;
}
// compute mean mass ratio
curRatio = 0.0;
curChargeSq = 0.0;
G4double norm = 0.0;
const G4ElementVector* theElementVector = mat->GetElementVector();
const G4double* theAtomNumDensityVector = mat->GetVecNbOfAtomsPerVolume();
size_t nelm = mat->GetNumberOfElements();
for (size_t i=0; i<nelm; ++i) {
const G4Element* elm = (*theElementVector)[i];
G4double Z = elm->GetZ();
G4double w = Z*Z*theAtomNumDensityVector[i];
curRatio += w/nist->GetAtomicMassAmu(G4int(Z));
curChargeSq = Z*Z*w;
norm += w;
}
curRatio *= proton_mass_c2/norm;
curChargeSq /= norm;
// store results
matPointers.push_back(mat);
matNames.push_back(name);
massFactors.push_back(curRatio);
effCharges.push_back(curChargeSq);
nMaterials++;
if(curBirks > 0.0 && verbose > 0) {
G4cout << "### G4EmSaturation::FindBirksCoefficient Birks coefficient for "
<< name << " " << curBirks*MeV/mm << " mm/MeV" << G4endl;
}
return curBirks;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4EmSaturation::DumpBirksCoefficients()
{
if(nMaterials > 0) {
G4cout << "### Birks coeffitients used in run time" << G4endl;
for(G4int i=0; i<nMaterials; ++i) {
G4double br = matPointers[i]->GetIonisation()->GetBirksConstant();
G4cout << " " << matNames[i] << " "
<< br*MeV/mm << " mm/MeV" << " "
<< br*matPointers[i]->GetDensity()*MeV*cm2/g
<< " g/cm^2/MeV"
<< G4endl;
}
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4EmSaturation::DumpG4BirksCoefficients()
{
if(nG4Birks > 0) {
G4cout << "### Birks coeffitients for Geant4 materials" << G4endl;
for(G4int i=0; i<nG4Birks; ++i) {
G4cout << " " << g4MatNames[i] << " "
<< g4MatData[i]*MeV/mm << " mm/MeV" << G4endl;
}
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4EmSaturation::Initialise()
{
// M.Hirschberg et al., IEEE Trans. Nuc. Sci. 39 (1992) 511
// SCSN-38 kB = 0.00842 g/cm^2/MeV; rho = 1.06 g/cm^3
g4MatNames.push_back("G4_POLYSTYRENE");
g4MatData.push_back(0.07943*mm/MeV);
// C.Fabjan (private communication)
// kB = 0.006 g/cm^2/MeV; rho = 7.13 g/cm^3
g4MatNames.push_back("G4_BGO");
g4MatData.push_back(0.008415*mm/MeV);
// A.Ribon analysis of publications
// Scallettar et al., Phys. Rev. A25 (1982) 2419.
// NIM A 523 (2004) 275.
// kB = 0.022 g/cm^2/MeV; rho = 1.396 g/cm^3;
// ATLAS Efield = 10 kV/cm provide the strongest effect
g4MatNames.push_back("G4_lAr");
g4MatData.push_back(0.1576*mm/MeV);
//G4_BARIUM_FLUORIDE
//G4_CESIUM_IODIDE
//G4_GEL_PHOTO_EMULSION
//G4_PHOTO_EMULSION
//G4_PLASTIC_SC_VINYLTOLUENE
//G4_SODIUM_IODIDE
//G4_STILBENE
//G4_lAr
//G4_PbWO4
//G4_Lucite
nG4Birks = g4MatData.size();
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....