| [819] | 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| 26 | // -------------------------------------------------------------------
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| 27 | //
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| 28 | // GEANT4 Class file
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| 29 | //
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| 30 | //
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| 31 | // File name: G4hShellCrossSectionExp.cc
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| 32 | //
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| 33 | // Author: Simona Saliceti (simona.saliceti@ge.infn.it)
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| 34 | //
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| 35 | // History:
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| 36 | // -----------
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| 37 | // From 23 Oct 2001 A. Mantero G4hShellCrossSection
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| 38 | // 30/03/2004 Simona Saliceti 1st implementation
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| 39 | // -------------------------------------------------------------------
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| 40 | // Class Description:
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| 41 | // Empiric Model for shell cross sections in proton ionisation
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| 42 | // -------------------------------------------------------------------
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| [961] | 43 | // $Id: G4hShellCrossSectionExp.cc,v 1.6 2008/05/02 19:23:38 pia Exp $
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| [1007] | 44 | // GEANT4 tag $Name: geant4-09-02 $
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| [819] | 45 |
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| 46 | #include "globals.hh"
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| 47 | #include <vector>
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| 48 | #include "G4hShellCrossSectionExp.hh"
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| 49 | #include "G4AtomicTransitionManager.hh"
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| 50 | #include "G4Electron.hh"
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| 51 | #include "G4hShellCrossSectionExpData.hh"
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| 52 | #include "G4Proton.hh"
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| 53 | #include "G4ParticleDefinition.hh"
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| 54 |
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| 55 | G4hShellCrossSectionExp::G4hShellCrossSectionExp()
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| 56 | {
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| 57 | kShellData = new G4hShellCrossSectionExpData();
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| 58 | }
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| 59 |
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| 60 | G4hShellCrossSectionExp::~G4hShellCrossSectionExp()
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| 61 | { }
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| 62 |
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| 63 | std::vector<G4double> G4hShellCrossSectionExp::GetCrossSection(G4int Z,
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| 64 | G4double incidentEnergy,
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| 65 | G4double mass,
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| 66 | G4double deltaEnergy,
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| 67 | G4bool testFlag) const
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| 68 | {
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| 69 | mass = 0.0;
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| 70 | deltaEnergy = 0.0;
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| 71 |
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| 72 | std::vector<G4double> aCrossSection;
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| 73 |
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| 74 | // Fill the vector of cross sections with the value just calculated
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| 75 | aCrossSection.push_back(GetCrossSectionExp(Z,incidentEnergy));
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| 76 |
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| 77 | if (testFlag)
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| 78 | {
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| 79 | G4cout <<"Element: " <<Z<<" Particle Energy: "<<incidentEnergy/MeV<<" MeV" <<G4endl;
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| 80 | G4cout <<"Cross Section: "<<aCrossSection[0]/barn<<" barns"<< G4endl;
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| 81 | }
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| 82 | return aCrossSection;
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| 83 | }
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| 84 |
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| 85 | //This function calculated the cross section with the Empiric model
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| 86 | G4double G4hShellCrossSectionExp::GetCrossSectionExp(G4int Z,
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| 87 | G4double incidentEnergy) const
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| 88 | {
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| 89 | // Vector that stores the calculated cross-sections for each shell:
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| 90 | G4double crossSectionsInBarn = 0.0;
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| 91 | G4double crossSections = 0.0;
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| 92 |
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| 93 | std::vector<G4double>* parVec = kShellData->GetParam(Z);
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| 94 | std::vector<G4double>::iterator i = (*parVec).begin();
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| 95 |
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| 96 | G4double a = *i;
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| 97 | G4double b = *(i+1);
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| 98 | G4double c = *(i+2);
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| 99 |
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| 100 | G4double incidentEnergyInMeV = incidentEnergy/MeV;
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| 101 |
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| 102 | if(Z<26 && Z>=6 && Z!=17)
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| 103 | {
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| 104 | crossSectionsInBarn = a*(std::pow(b,(1./incidentEnergyInMeV)))*(std::pow(incidentEnergyInMeV,c));
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| 105 | }
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| [961] | 106 | else if((Z<66 && Z>=26) || Z==17)
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| [819] | 107 | {
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| 108 | crossSectionsInBarn = std::exp(a+(b/incidentEnergyInMeV)+(c*std::log(incidentEnergyInMeV)));
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| 109 | }
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| 110 | else if(Z<=92 && Z>=66)
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| 111 | {
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| 112 | crossSectionsInBarn = (std::pow(incidentEnergyInMeV,a))*std::exp(b-(c*incidentEnergyInMeV));
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| 113 | }
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| 114 | else
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| 115 | {
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| 116 | G4cout << "Error: there is not that Z" << G4endl;
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| 117 | }
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| 118 |
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| 119 | crossSections = crossSectionsInBarn*barn;
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| 120 | return crossSections;
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| 121 | }
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| 122 |
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| 123 | // This function gives the atomic cross section of k shell only
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| 124 | void G4hShellCrossSectionExp::SetTotalCS(G4double value)
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| 125 | {
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| 126 | atomTotalCrossSection = value;
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| 127 | }
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| 128 |
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| 129 | //A new implementation of Probability to calculate the cross section probability for k shell only
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| 130 | std::vector<G4double> G4hShellCrossSectionExp::Probabilities(
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| 131 | G4int Z,
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| 132 | G4double incidentEnergy,
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| 133 | G4double hMass,
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| 134 | G4double deltaEnergy
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| 135 | ) const
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| 136 | {
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| 137 | hMass = 0.0;
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| 138 | deltaEnergy = 0.0;
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| 139 |
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| 140 | std::vector<G4double> kProbability;
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| 141 | kProbability.push_back(GetCrossSectionExp(Z,incidentEnergy)/atomTotalCrossSection);
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| 142 | // ---- MGP ---- Next line corrected to kProbability[0] instead of [1], which is not initialized!
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| 143 | kProbability.push_back(1 - kProbability[0]);
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| 144 |
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| 145 | return kProbability;
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| 146 | }
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| 147 |
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| 148 |
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| 149 |
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