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geant4/source/processes/electromagnetic/lowenergy/src/G4ANSTOecpssrKxsModel.cc
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2021-12-10 16:15:15 +00:00

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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. *
// ********************************************************************
//
// History:
// -----------
// 10 Nov 2021 S. Guatelli & S. Bakr, Wollongong University - 1st implementation
//
// Class description
// ----------------
// Computation of K, L & M shell ECPSSR ionisation cross sections for protons and alphas
// Based on the work of
// - S. Bakr et al. (2021) NIM B, 507:1119.
// - S. Bakr et al (2018), NIMB B, 436: 285-291.
// ---------------------------------------------------------------------------------------
#include <fstream>
#include <iomanip>
#include "G4ANSTOecpssrKxsModel.hh"
#include "globals.hh"
#include "G4SystemOfUnits.hh"
#include "G4ios.hh"
#include "G4EMDataSet.hh"
#include "G4LogLogInterpolation.hh"
#include "G4Proton.hh"
#include "G4Alpha.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4ANSTOecpssrKxsModel::G4ANSTOecpssrKxsModel()
{
G4cout << "Using ANSTO K Cross Sections! "<< G4endl;
interpolation = new G4LogLogInterpolation();
for (G4int i=6; i<93; i++)
{
protonDataSetMap[i] = new G4EMDataSet(i,interpolation);
protonDataSetMap[i]->LoadData("pixe_ANSTO/proton/k-");
}
for (G4int i=6; i<93; i++)
{
alphaDataSetMap[i] = new G4EMDataSet(i,interpolation);
alphaDataSetMap[i]->LoadData("pixe_ANSTO/alpha/k-");
}
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4ANSTOecpssrKxsModel::~G4ANSTOecpssrKxsModel()
{
protonDataSetMap.clear();
alphaDataSetMap.clear();
delete interpolation;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4ANSTOecpssrKxsModel::CalculateCrossSection(G4int zTarget,G4double massIncident, G4double energyIncident)
{
G4Proton* aProton = G4Proton::Proton();
G4Alpha* aAlpha = G4Alpha::Alpha();
G4double sigma = 0;
if (massIncident == aProton->GetPDGMass())
{
if (energyIncident > 0.2*MeV && energyIncident < 5.*MeV && zTarget < 93 && zTarget > 5) {
sigma = protonDataSetMap[zTarget]->FindValue(energyIncident/MeV);
if (sigma !=0 && energyIncident > protonDataSetMap[zTarget]->GetEnergies(0).back()*MeV) return 0.;
}
}
else if (massIncident == aAlpha->GetPDGMass())
{
if (energyIncident > 0.2*MeV && energyIncident < 40.*MeV && zTarget < 93 && zTarget > 5) {
sigma = alphaDataSetMap[zTarget]->FindValue(energyIncident/MeV);
if (sigma !=0 && energyIncident > alphaDataSetMap[zTarget]->GetEnergies(0).back()*MeV) return 0.;
}
}
else
{
sigma = 0.;
}
// sigma is in internal units: it has been converted from
// the input file in barns bt the EmDataset
return sigma;
}