// // ******************************************************************** // * 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, 507:11–19. // - S. Bakr et al (2018), NIMB B, 436: 285-291. // --------------------------------------------------------------------------------------- #include #include #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; }