Files
geant4/source/processes/electromagnetic/utils/src/G4ElectronIonPair.cc
2022-12-09 14:43:28 +01:00

248 lines
7.4 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. *
// ********************************************************************
//
//
// -------------------------------------------------------------------
//
// GEANT4 Class file
//
//
// File name: G4ElectronIonPair
//
// Author: Vladimir Ivanchenko
//
// Creation date: 08.07.2008
//
// Modifications:
//
// -------------------------------------------------------------
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#include "G4ElectronIonPair.hh"
#include "G4SystemOfUnits.hh"
#include "G4Material.hh"
#include "G4MaterialTable.hh"
#include "G4StepPoint.hh"
#include "G4VProcess.hh"
#include "G4ProcessType.hh"
#include "G4Track.hh"
#include "Randomize.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4ElectronIonPair::G4ElectronIonPair(G4int verb)
{
verbose = verb;
curMaterial = nullptr;
curMeanEnergy = 0.0;
nMaterials = 0;
invFanoFactor = 1.0/0.2;
Initialise();
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4ElectronIonPair::~G4ElectronIonPair() = default;
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double G4ElectronIonPair::MeanNumberOfIonsAlongStep(
const G4ParticleDefinition* part,
const G4Material* material,
G4double edep,
G4double niel)
{
G4double nion = 0.0;
// NIEL does not provide ionisation clusters
if(edep > niel) {
// neutral particles do not produce ionisation along step
if(part->GetPDGCharge() != 0.0) {
// select material
if(material != curMaterial) {
curMaterial = material;
curMeanEnergy = material->GetIonisation()->GetMeanEnergyPerIonPair();
// if mean energy is not defined then look into G4 DB
if(0.0 == curMeanEnergy) {
curMeanEnergy = FindG4MeanEnergyPerIonPair(material);
}
}
if(curMeanEnergy > 0.0) { nion = (edep - niel)/curMeanEnergy; }
}
}
return nion;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
std::vector<G4ThreeVector>*
G4ElectronIonPair::SampleIonsAlongStep(const G4Step* step)
{
std::vector<G4ThreeVector>* v = nullptr;
G4int nion = SampleNumberOfIonsAlongStep(step);
// sample ionisation along step
if(nion > 0) {
v = new std::vector<G4ThreeVector>;
G4ThreeVector prePos = step->GetPreStepPoint()->GetPosition();
G4ThreeVector deltaPos = step->GetPostStepPoint()->GetPosition() - prePos;
for(G4int i=0; i<nion; ++i) {
v->push_back( prePos + deltaPos*G4UniformRand() );
}
if(verbose > 1 ) {
G4cout << "### G4ElectronIonPair::SampleIonisationPoints: "
<< v->size() << " ion pairs are added" << G4endl;
}
}
return v;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4int
G4ElectronIonPair::ResidualeChargePostStep(const G4ParticleDefinition*,
const G4TrackVector*,
G4int subType) const
{
G4int nholes = 0;
if(2 == subType || 12 == subType || 13 == subType) { nholes = 1; }
return nholes;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
G4double
G4ElectronIonPair::FindG4MeanEnergyPerIonPair(const G4Material* mat) const
{
G4String name = mat->GetName();
G4double res = 0.0;
// is this material in the vector?
for(G4int j=0; j<nMaterials; ++j) {
if(name == g4MatNames[j]) {
res = g4MatData[j];
mat->GetIonisation()->SetMeanEnergyPerIonPair(res);
if(verbose > 0) {
G4cout << "### G4ElectronIonPair::FindG4MeanEnergyPerIonPair for "
<< name << " Epair= " << res/eV << " eV is set"
<< G4endl;
}
break;
}
}
return res;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4ElectronIonPair:: DumpMeanEnergyPerIonPair() const
{
std::size_t nmat = G4Material::GetNumberOfMaterials();
const G4MaterialTable* mtable = G4Material::GetMaterialTable();
if(nmat > 0) {
G4cout << "### G4ElectronIonPair: mean energy per ion pair available:"
<< G4endl;
for(std::size_t i=0; i<nmat; ++i) {
const G4Material* mat = (*mtable)[i];
G4double x = mat->GetIonisation()->GetMeanEnergyPerIonPair();
if(x > 0.0) {
G4cout << " " << mat->GetName() << " Epair= "
<< x/eV << " eV" << G4endl;
}
}
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4ElectronIonPair::DumpG4MeanEnergyPerIonPair() const
{
if(nMaterials > 0) {
G4cout << "### G4ElectronIonPair: mean energy per ion pair "
<< " for Geant4 materials" << G4endl;
for(G4int i=0; i<nMaterials; ++i) {
G4cout << " " << g4MatNames[i] << " Epair= "
<< g4MatData[i]/eV << " eV" << G4endl;
}
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
void G4ElectronIonPair::Initialise()
{
// ICRU Report 31, 1979
g4MatNames.push_back("G4_Si");
g4MatData.push_back(3.62*eV);
g4MatNames.push_back("G4_Ge");
g4MatData.push_back(2.97*eV);
g4MatNames.push_back("G4_He");
g4MatData.push_back(44.4*eV);
g4MatNames.push_back("G4_N");
g4MatData.push_back(36.4*eV);
g4MatNames.push_back("G4_O");
g4MatData.push_back(32.3*eV);
g4MatNames.push_back("G4_Ne");
g4MatData.push_back(36.8*eV);
g4MatNames.push_back("G4_Ar");
g4MatData.push_back(26.34*eV);
g4MatNames.push_back("G4_Kr");
g4MatData.push_back(24.1*eV);
g4MatNames.push_back("G4_Xe");
g4MatData.push_back(21.6*eV);
g4MatNames.push_back("G4_lAr");
g4MatData.push_back(23.6*eV);
g4MatNames.push_back("G4_lKr");
g4MatData.push_back(20.5*eV);
g4MatNames.push_back("G4_lXe");
g4MatData.push_back(15.6*eV);
g4MatNames.push_back("G4_AIR");
g4MatData.push_back(35.1*eV);
nMaterials = (G4int)g4MatData.size();
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....