297 lines
8.8 KiB
C++
Executable File
297 lines
8.8 KiB
C++
Executable File
//
|
|
// ********************************************************************
|
|
// * 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: 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....
|