[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 | // $Id: G4AtomicTransitionManager.cc,v 1.2 ???? |
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[991] | 28 | // GEANT4 tag $Name: geant4-09-02 $ |
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[819] | 29 | // |
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| 30 | // Authors: Elena Guardincerri (Elena.Guardincerri@ge.infn.it) |
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| 31 | // Alfonso Mantero (Alfonso.Mantero@ge.infn.it) |
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| 32 | // |
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| 33 | // History: |
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| 34 | // ----------- |
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| 35 | // 16 Sep 2001 E. Guardincerri First Committed to cvs |
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| 36 | // |
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| 37 | // ------------------------------------------------------------------- |
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| 38 | |
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| 39 | #include "G4AtomicTransitionManager.hh" |
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| 40 | |
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| 41 | G4AtomicTransitionManager::G4AtomicTransitionManager(G4int minZ, G4int maxZ, |
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| 42 | G4int limitInfTable,G4int limitSupTable) |
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| 43 | :zMin(minZ), |
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| 44 | zMax(maxZ), |
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| 45 | infTableLimit(limitInfTable), |
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| 46 | supTableLimit(limitSupTable) |
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| 47 | { |
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| 48 | // infTableLimit is initialized to 6 because EADL lacks data for Z<=5 |
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| 49 | G4ShellData* shellManager = new G4ShellData; |
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| 50 | |
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| 51 | // initialization of the data for auger effect |
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| 52 | |
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| 53 | augerData = new G4AugerData; |
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| 54 | |
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| 55 | shellManager->LoadData("/fluor/binding"); |
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| 56 | |
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| 57 | // Fills shellTable with the data from EADL, identities and binding |
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| 58 | // energies of shells |
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| 59 | for (G4int Z = zMin; Z<= zMax; Z++) |
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| 60 | { |
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| 61 | std::vector<G4AtomicShell*> vectorOfShells; |
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| 62 | size_t shellIndex = 0; |
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| 63 | |
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| 64 | size_t numberOfShells=shellManager->NumberOfShells(Z); |
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| 65 | for (shellIndex = 0; shellIndex<numberOfShells; shellIndex++) |
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| 66 | { |
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| 67 | G4int shellId = shellManager->ShellId(Z,shellIndex); |
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| 68 | G4double bindingEnergy = shellManager->BindingEnergy(Z,shellIndex); |
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| 69 | |
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| 70 | G4AtomicShell * shell = new G4AtomicShell(shellId,bindingEnergy); |
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| 71 | |
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| 72 | vectorOfShells.push_back(shell); |
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| 73 | } |
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| 74 | |
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| 75 | // shellTable.insert(std::make_pair(Z, vectorOfShells)); |
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| 76 | shellTable[Z] = vectorOfShells; |
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| 77 | } |
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| 78 | |
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| 79 | // Fills transitionTable with the data from EADL, identities, transition |
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| 80 | // energies and transition probabilities |
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| 81 | for (G4int Znum= infTableLimit; Znum<=supTableLimit; Znum++) |
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| 82 | { G4FluoData* fluoManager = new G4FluoData; |
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| 83 | std::vector<G4FluoTransition*> vectorOfTransitions; |
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| 84 | fluoManager->LoadData(Znum); |
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| 85 | |
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| 86 | size_t numberOfVacancies = fluoManager-> NumberOfVacancies(); |
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| 87 | |
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| 88 | for (size_t vacancyIndex = 0; vacancyIndex<numberOfVacancies; vacancyIndex++) |
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| 89 | |
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| 90 | { |
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| 91 | std::vector<G4int> vectorOfIds; |
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| 92 | G4DataVector vectorOfEnergies; |
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| 93 | G4DataVector vectorOfProbabilities; |
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| 94 | |
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| 95 | G4int finalShell = fluoManager->VacancyId(vacancyIndex); |
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| 96 | size_t numberOfTransitions = fluoManager->NumberOfTransitions(vacancyIndex); |
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| 97 | for (size_t origShellIndex = 0; origShellIndex < numberOfTransitions; |
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| 98 | origShellIndex++) |
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| 99 | |
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| 100 | { |
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| 101 | |
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| 102 | G4int originatingShellId = fluoManager->StartShellId(origShellIndex,vacancyIndex); |
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| 103 | |
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| 104 | vectorOfIds.push_back(originatingShellId); |
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| 105 | |
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| 106 | G4double transitionEnergy = fluoManager->StartShellEnergy(origShellIndex,vacancyIndex); |
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| 107 | vectorOfEnergies.push_back(transitionEnergy); |
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| 108 | G4double transitionProbability = fluoManager->StartShellProb(origShellIndex,vacancyIndex); |
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| 109 | vectorOfProbabilities.push_back(transitionProbability); |
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| 110 | } |
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| 111 | G4FluoTransition * transition = new G4FluoTransition (finalShell,vectorOfIds, |
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| 112 | vectorOfEnergies,vectorOfProbabilities); |
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| 113 | vectorOfTransitions.push_back(transition); |
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| 114 | } |
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| 115 | // transitionTable.insert(std::make_pair(Znum, vectorOfTransitions)); |
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| 116 | transitionTable[Znum] = vectorOfTransitions; |
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| 117 | |
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| 118 | delete fluoManager; |
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| 119 | } |
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| 120 | delete shellManager; |
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| 121 | } |
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| 122 | |
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| 123 | G4AtomicTransitionManager::~G4AtomicTransitionManager() |
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| 124 | |
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| 125 | { |
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| 126 | |
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| 127 | delete augerData; |
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| 128 | |
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| 129 | std::map<G4int,std::vector<G4AtomicShell*>,std::less<G4int> >::iterator pos; |
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| 130 | |
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| 131 | for (pos = shellTable.begin(); pos != shellTable.end(); pos++){ |
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| 132 | |
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| 133 | std::vector< G4AtomicShell*>vec = (*pos).second; |
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| 134 | |
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| 135 | G4int vecSize=vec.size(); |
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| 136 | |
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| 137 | for (G4int i=0; i< vecSize; i++){ |
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| 138 | G4AtomicShell* shell = vec[i]; |
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| 139 | delete shell; |
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| 140 | } |
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| 141 | |
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| 142 | } |
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| 143 | |
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| 144 | std::map<G4int,std::vector<G4FluoTransition*>,std::less<G4int> >::iterator ppos; |
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| 145 | |
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| 146 | for (ppos = transitionTable.begin(); ppos != transitionTable.end(); ppos++){ |
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| 147 | |
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| 148 | std::vector<G4FluoTransition*>vec = (*ppos).second; |
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| 149 | |
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| 150 | G4int vecSize=vec.size(); |
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| 151 | |
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| 152 | for (G4int i=0; i< vecSize; i++){ |
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| 153 | G4FluoTransition* transition = vec[i]; |
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| 154 | delete transition; |
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| 155 | } |
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| 156 | |
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| 157 | } |
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| 158 | |
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| 159 | } |
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| 160 | |
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| 161 | G4AtomicTransitionManager* G4AtomicTransitionManager::instance = 0; |
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| 162 | |
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| 163 | G4AtomicTransitionManager* G4AtomicTransitionManager::Instance() |
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| 164 | { |
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| 165 | if (instance == 0) |
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| 166 | { |
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| 167 | instance = new G4AtomicTransitionManager; |
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| 168 | |
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| 169 | } |
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| 170 | return instance; |
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| 171 | } |
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| 172 | |
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| 173 | |
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| 174 | G4AtomicShell* G4AtomicTransitionManager::Shell(G4int Z, size_t shellIndex) const |
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| 175 | { |
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| 176 | std::map<G4int,std::vector<G4AtomicShell*>,std::less<G4int> >::const_iterator pos; |
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| 177 | |
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| 178 | pos = shellTable.find(Z); |
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| 179 | |
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| 180 | if (pos!= shellTable.end()) |
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| 181 | { |
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| 182 | std::vector<G4AtomicShell*> v = (*pos).second; |
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| 183 | if (shellIndex<v.size()) |
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| 184 | { |
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| 185 | return(v[shellIndex]); |
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| 186 | } |
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| 187 | else |
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| 188 | { |
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| 189 | size_t lastShell = v.size(); |
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| 190 | G4cout << "G4AtomicTransitionManager::Shell - Z = " |
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| 191 | << Z << ", shellIndex = " << shellIndex |
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| 192 | << " not found; number of shells = " << lastShell << G4endl; |
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| 193 | // G4Exception("G4AtomicTransitionManager:shell not found"); |
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| 194 | if (lastShell > 0) |
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| 195 | { |
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| 196 | return v[lastShell - 1]; |
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| 197 | } |
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| 198 | else |
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| 199 | { |
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| 200 | return 0; |
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| 201 | } |
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| 202 | } |
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| 203 | } |
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| 204 | else |
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| 205 | { |
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| 206 | G4Exception("G4AtomicTransitionManager:Z not found"); |
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| 207 | return 0; |
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| 208 | } |
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| 209 | } |
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| 210 | |
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| 211 | // This function gives, upon Z and the Index of the initial shell where te vacancy is, |
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| 212 | // the radiative transition that can happen (originating shell, energy, probability) |
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| 213 | |
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| 214 | const G4FluoTransition* G4AtomicTransitionManager::ReachableShell(G4int Z,size_t shellIndex) const |
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| 215 | { |
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| 216 | std::map<G4int,std::vector<G4FluoTransition*>,std::less<G4int> >::const_iterator pos; |
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| 217 | pos = transitionTable.find(Z); |
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| 218 | if (pos!= transitionTable.end()) |
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| 219 | { |
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| 220 | std::vector<G4FluoTransition*> v = (*pos).second; |
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| 221 | if (shellIndex < v.size()) return(v[shellIndex]); |
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| 222 | else { |
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| 223 | G4Exception("G4AtomicTransitionManager:reachable shell not found"); |
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| 224 | return 0; |
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| 225 | } |
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| 226 | } |
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| 227 | else{ |
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| 228 | G4cout << "G4AtomicTransitionMagare warning: No fluorescence or Auger for Z=" << Z << G4endl; |
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| 229 | G4cout << "Absorbed enrgy deposited locally" << G4endl; |
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| 230 | |
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| 231 | // G4Exception("G4AtomicTransitionManager:Z not found"); |
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| 232 | return 0; |
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| 233 | } |
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| 234 | } |
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| 235 | |
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| 236 | const G4AugerTransition* G4AtomicTransitionManager::ReachableAugerShell(G4int Z, G4int vacancyShellIndex) const |
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| 237 | { |
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| 238 | |
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| 239 | G4AugerTransition* augerTransition = augerData->GetAugerTransition(Z,vacancyShellIndex); |
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| 240 | return augerTransition; |
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| 241 | } |
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| 242 | |
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| 243 | |
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| 244 | |
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| 245 | G4int G4AtomicTransitionManager::NumberOfShells (G4int Z) const |
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| 246 | { |
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| 247 | |
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| 248 | std::map<G4int,std::vector<G4AtomicShell*>,std::less<G4int> >::const_iterator pos; |
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| 249 | |
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| 250 | pos = shellTable.find(Z); |
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| 251 | |
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| 252 | if (pos!= shellTable.end()){ |
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| 253 | |
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| 254 | std::vector<G4AtomicShell*> v = (*pos).second; |
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| 255 | |
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| 256 | return v.size(); |
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| 257 | } |
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| 258 | |
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| 259 | else{ |
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| 260 | G4cout << "G4AtomicTransitionMagare warning: No fluorescence or Auger for Z=" << Z << G4endl; |
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| 261 | G4cout << "Absorbed enrgy deposited locally" << G4endl; |
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| 262 | |
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| 263 | // G4Exception("G4AtomicTransitionManager:Z not found"); |
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| 264 | return 0; |
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| 265 | } |
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| 266 | } |
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| 267 | |
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| 268 | // This function returns the number of possible radiative transitions for the atom with atomic number Z |
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| 269 | // i.e. the number of shell in wich a vacancy can be filled with a radiative transition |
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| 270 | |
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| 271 | G4int G4AtomicTransitionManager::NumberOfReachableShells(G4int Z) const |
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| 272 | { |
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| 273 | std::map<G4int,std::vector<G4FluoTransition*>,std::less<G4int> >::const_iterator pos; |
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| 274 | |
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| 275 | pos = transitionTable.find(Z); |
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| 276 | |
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| 277 | if (pos!= transitionTable.end()) |
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| 278 | { |
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| 279 | std::vector<G4FluoTransition*> v = (*pos).second; |
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| 280 | return v.size(); |
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| 281 | } |
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| 282 | else |
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| 283 | { |
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| 284 | G4cout << "G4AtomicTransitionMagare warning: No fluorescence or Auger for Z=" << Z << G4endl; |
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| 285 | G4cout << "Absorbed enrgy deposited locally" << G4endl; |
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| 286 | |
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| 287 | // G4Exception("G4AtomicTransitionManager:Z not found"); |
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| 288 | return 0; |
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| 289 | } |
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| 290 | } |
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| 291 | |
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| 292 | // This function returns the number of possible NON-radiative transitions for the atom with atomic number Z |
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| 293 | // i.e. the number of shell in wich a vacancy can be filled with a NON-radiative transition |
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| 294 | |
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| 295 | G4int G4AtomicTransitionManager::NumberOfReachableAugerShells(G4int Z)const |
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| 296 | { |
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| 297 | G4int n = augerData->NumberOfVacancies(Z); |
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| 298 | return n; |
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| 299 | } |
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| 300 | |
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| 301 | |
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| 302 | |
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| 303 | G4double G4AtomicTransitionManager::TotalRadiativeTransitionProbability(G4int Z, |
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| 304 | size_t shellIndex) |
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| 305 | |
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| 306 | { |
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| 307 | std::map<G4int,std::vector<G4FluoTransition*>,std::less<G4int> >::iterator pos; |
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| 308 | |
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| 309 | pos = transitionTable.find(Z); |
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| 310 | |
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| 311 | if (pos!= transitionTable.end()) |
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| 312 | { |
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| 313 | std::vector<G4FluoTransition*> v = (*pos).second; |
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| 314 | |
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| 315 | if (shellIndex < v.size()) |
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| 316 | { |
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| 317 | G4FluoTransition* transition = v[shellIndex]; |
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| 318 | G4DataVector transProb = transition->TransitionProbabilities(); |
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| 319 | G4double totalRadTransProb = 0; |
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| 320 | |
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[961] | 321 | for (size_t j = 0; j<transProb.size(); j++) // AM -- corrected, it was 1 |
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[819] | 322 | { |
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| 323 | totalRadTransProb = totalRadTransProb + transProb[j]; |
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| 324 | } |
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| 325 | return totalRadTransProb; |
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| 326 | |
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| 327 | } |
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| 328 | else { |
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| 329 | G4Exception( "G4AtomicTransitionManager: shell not found" ); |
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| 330 | return 0; |
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| 331 | |
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| 332 | } |
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| 333 | } |
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| 334 | else{ |
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| 335 | G4cout << "G4AtomicTransitionMagare warning: No fluorescence or Auger for Z=" << Z << G4endl; |
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| 336 | G4cout << "Absorbed enrgy deposited locally" << G4endl; |
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| 337 | |
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| 338 | // G4Exception("G4AtomicTransitionManager:Z not found"); |
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| 339 | |
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| 340 | return 0; |
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| 341 | } |
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| 342 | } |
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| 343 | |
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| 344 | G4double G4AtomicTransitionManager::TotalNonRadiativeTransitionProbability(G4int Z, size_t shellIndex) |
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| 345 | |
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| 346 | { |
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| 347 | |
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| 348 | std::map<G4int,std::vector<G4FluoTransition*>,std::less<G4int> >::iterator pos; |
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| 349 | |
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| 350 | pos = transitionTable.find(Z); |
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| 351 | |
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| 352 | if (pos!= transitionTable.end()){ |
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| 353 | |
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| 354 | std::vector<G4FluoTransition*> v = (*pos).second; |
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| 355 | |
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| 356 | |
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| 357 | if (shellIndex<v.size()){ |
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| 358 | |
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| 359 | G4FluoTransition* transition=v[shellIndex]; |
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| 360 | G4DataVector transProb = transition->TransitionProbabilities(); |
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| 361 | G4double totalRadTransProb = 0; |
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| 362 | |
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[961] | 363 | for(size_t j = 0; j<transProb.size(); j++) // AM -- Corrected, was 1 |
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[819] | 364 | { |
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| 365 | totalRadTransProb = totalRadTransProb + transProb[j]; |
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| 366 | } |
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| 367 | |
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| 368 | G4double totalNonRadTransProb= (1 - totalRadTransProb); |
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| 369 | |
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| 370 | return totalNonRadTransProb; } |
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| 371 | |
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| 372 | else { |
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| 373 | G4Exception( "shell not found"); |
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| 374 | return 0; |
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| 375 | } |
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| 376 | } |
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| 377 | else{ |
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| 378 | G4cout << "G4AtomicTransitionMagare warning: No fluorescence or Auger for Z=" << Z << G4endl; |
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| 379 | G4cout << "Absorbed enrgy deposited locally" << G4endl; |
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| 380 | |
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| 381 | // G4Exception("G4AtomicTransitionManager:Z not found"); |
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| 382 | return 0; |
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| 383 | } |
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| 384 | } |
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| 385 | |
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| 386 | |
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| 387 | |
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| 388 | |
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| 389 | |
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| 390 | |
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| 391 | |
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| 392 | |
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| 393 | |
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| 394 | |
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