[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: G4AtomicDeexcitation.cc,v 1.11 |
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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 | // |
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| 36 | // 16 Sept 2001 First committed to cvs |
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| 37 | // 12 Sep 2003 Bug in auger production fixed |
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| 38 | // |
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| 39 | // ------------------------------------------------------------------- |
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| 40 | |
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| 41 | #include "G4AtomicDeexcitation.hh" |
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| 42 | #include "Randomize.hh" |
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| 43 | #include "G4Gamma.hh" |
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| 44 | #include "G4Electron.hh" |
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| 45 | #include "G4AtomicTransitionManager.hh" |
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| 46 | #include "G4FluoTransition.hh" |
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| 47 | |
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| 48 | G4AtomicDeexcitation::G4AtomicDeexcitation(): |
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| 49 | minGammaEnergy(100.*eV), |
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| 50 | minElectronEnergy(100.*eV), |
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| 51 | fAuger(false) |
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| 52 | {} |
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| 53 | |
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| 54 | G4AtomicDeexcitation::~G4AtomicDeexcitation() |
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| 55 | {} |
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| 56 | |
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| 57 | std::vector<G4DynamicParticle*>* G4AtomicDeexcitation::GenerateParticles(G4int Z,G4int givenShellId) |
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| 58 | { |
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| 59 | |
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| 60 | std::vector<G4DynamicParticle*>* vectorOfParticles; |
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| 61 | |
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| 62 | vectorOfParticles = new std::vector<G4DynamicParticle*>; |
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| 63 | G4DynamicParticle* aParticle; |
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| 64 | G4int provShellId = 0; |
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| 65 | G4int counter = 0; |
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| 66 | |
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| 67 | // The aim of this loop is to generate more than one fluorecence photon |
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| 68 | // from the same ionizing event |
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| 69 | do |
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| 70 | { |
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| 71 | if (counter == 0) |
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| 72 | // First call to GenerateParticles(...): |
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| 73 | // givenShellId is given by the process |
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| 74 | { |
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| 75 | provShellId = SelectTypeOfTransition(Z, givenShellId); |
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| 76 | |
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| 77 | if ( provShellId >0) |
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| 78 | { |
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| 79 | aParticle = GenerateFluorescence(Z,givenShellId,provShellId); |
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| 80 | } |
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| 81 | else if ( provShellId == -1) |
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| 82 | { |
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| 83 | aParticle = GenerateAuger(Z, givenShellId); |
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| 84 | } |
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| 85 | else |
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| 86 | { |
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| 87 | G4Exception("G4AtomicDeexcitation: starting shell uncorrect: check it"); |
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| 88 | } |
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| 89 | } |
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| 90 | else |
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| 91 | // Following calls to GenerateParticles(...): |
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| 92 | // newShellId is given by GenerateFluorescence(...) |
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| 93 | { |
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| 94 | provShellId = SelectTypeOfTransition(Z,newShellId); |
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| 95 | if (provShellId >0) |
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| 96 | { |
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| 97 | aParticle = GenerateFluorescence(Z,newShellId,provShellId); |
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| 98 | } |
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| 99 | else if ( provShellId == -1) |
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| 100 | { |
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| 101 | aParticle = GenerateAuger(Z, newShellId); |
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| 102 | } |
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| 103 | else |
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| 104 | { |
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| 105 | G4Exception("G4AtomicDeexcitation: starting shell uncorrect: check it"); |
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| 106 | } |
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| 107 | } |
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| 108 | counter++; |
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| 109 | if (aParticle != 0) {vectorOfParticles->push_back(aParticle);} |
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| 110 | else {provShellId = -2;} |
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| 111 | } |
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| 112 | |
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| 113 | // Look this in a particular way: only one auger emitted! // |
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| 114 | while (provShellId > -2); |
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| 115 | |
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| 116 | return vectorOfParticles; |
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| 117 | } |
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| 118 | |
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| 119 | G4int G4AtomicDeexcitation::SelectTypeOfTransition(G4int Z, G4int shellId) |
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| 120 | { |
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| 121 | if (shellId <=0 ) |
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| 122 | {G4Exception("G4AtomicDeexcitation: zero or negative shellId");} |
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| 123 | |
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| 124 | G4bool fluoTransitionFoundFlag = false; |
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| 125 | |
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| 126 | const G4AtomicTransitionManager* transitionManager = |
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| 127 | G4AtomicTransitionManager::Instance(); |
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| 128 | G4int provShellId = -1; |
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| 129 | G4int shellNum = 0; |
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| 130 | G4int maxNumOfShells = transitionManager->NumberOfReachableShells(Z); |
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| 131 | |
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| 132 | const G4FluoTransition* refShell = transitionManager->ReachableShell(Z,maxNumOfShells-1); |
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| 133 | |
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| 134 | // This loop gives shellNum the value of the index of shellId |
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| 135 | // in the vector storing the list of the shells reachable through |
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| 136 | // a radiative transition |
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| 137 | if ( shellId <= refShell->FinalShellId()) |
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| 138 | { |
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| 139 | while (shellId != transitionManager->ReachableShell(Z,shellNum)->FinalShellId()) |
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| 140 | { |
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| 141 | if(shellNum ==maxNumOfShells-1) |
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| 142 | { |
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| 143 | break; |
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| 144 | } |
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| 145 | shellNum++; |
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| 146 | } |
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| 147 | G4int transProb = 0; //AM change 29/6/07 was 1 |
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| 148 | |
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| 149 | G4double partialProb = G4UniformRand(); |
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| 150 | G4double partSum = 0; |
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| 151 | const G4FluoTransition* aShell = transitionManager->ReachableShell(Z,shellNum); |
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| 152 | G4int trSize = (aShell->TransitionProbabilities()).size(); |
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| 153 | |
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| 154 | // Loop over the shells wich can provide an electron for a |
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| 155 | // radiative transition towards shellId: |
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| 156 | // in every loop the partial sum of the first transProb shells |
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| 157 | // is calculated and compared with a random number [0,1]. |
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| 158 | // If the partial sum is greater, the shell whose index is transProb |
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| 159 | // is chosen as the starting shell for a radiative transition |
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| 160 | // and its identity is returned |
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| 161 | // Else, terminateded the loop, -1 is returned |
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| 162 | while(transProb < trSize){ |
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| 163 | |
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| 164 | partSum += aShell->TransitionProbability(transProb); |
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| 165 | |
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| 166 | if(partialProb <= partSum) |
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| 167 | { |
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| 168 | provShellId = aShell->OriginatingShellId(transProb); |
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| 169 | fluoTransitionFoundFlag = true; |
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| 170 | |
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| 171 | break; |
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| 172 | } |
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| 173 | transProb++; |
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| 174 | } |
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| 175 | |
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| 176 | // here provShellId is the right one or is -1. |
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| 177 | // if -1, the control is passed to the Auger generation part of the package |
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| 178 | } |
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| 179 | |
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| 180 | |
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| 181 | |
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| 182 | else |
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| 183 | { |
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| 184 | |
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| 185 | provShellId = -1; |
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| 186 | |
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| 187 | } |
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| 188 | return provShellId; |
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| 189 | } |
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| 190 | |
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| 191 | G4DynamicParticle* G4AtomicDeexcitation::GenerateFluorescence(G4int Z, |
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| 192 | G4int shellId, |
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| 193 | G4int provShellId ) |
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| 194 | { |
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| 195 | |
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| 196 | |
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| 197 | const G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance(); |
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| 198 | // G4int provenienceShell = provShellId; |
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| 199 | |
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| 200 | //isotropic angular distribution for the outcoming photon |
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| 201 | G4double newcosTh = 1.-2.*G4UniformRand(); |
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| 202 | G4double newsinTh = std::sqrt(1.-newcosTh*newcosTh); |
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| 203 | G4double newPhi = twopi*G4UniformRand(); |
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| 204 | |
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| 205 | G4double xDir = newsinTh*std::sin(newPhi); |
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| 206 | G4double yDir = newsinTh*std::cos(newPhi); |
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| 207 | G4double zDir = newcosTh; |
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| 208 | |
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| 209 | G4ThreeVector newGammaDirection(xDir,yDir,zDir); |
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| 210 | |
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| 211 | G4int shellNum = 0; |
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| 212 | G4int maxNumOfShells = transitionManager->NumberOfReachableShells(Z); |
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| 213 | |
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| 214 | // find the index of the shell named shellId |
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| 215 | while (shellId != transitionManager-> |
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| 216 | ReachableShell(Z,shellNum)->FinalShellId()) |
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| 217 | { |
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| 218 | if(shellNum == maxNumOfShells-1) |
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| 219 | { |
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| 220 | break; |
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| 221 | } |
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| 222 | shellNum++; |
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| 223 | } |
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| 224 | // number of shell from wich an electron can reach shellId |
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| 225 | size_t transitionSize = transitionManager-> |
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| 226 | ReachableShell(Z,shellNum)->OriginatingShellIds().size(); |
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| 227 | |
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| 228 | size_t index = 0; |
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| 229 | |
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| 230 | // find the index of the shell named provShellId in the vector |
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| 231 | // storing the shells from which shellId can be reached |
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| 232 | while (provShellId != transitionManager-> |
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| 233 | ReachableShell(Z,shellNum)->OriginatingShellId(index)) |
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| 234 | { |
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| 235 | if(index == transitionSize-1) |
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| 236 | { |
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| 237 | break; |
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| 238 | } |
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| 239 | index++; |
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| 240 | } |
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| 241 | // energy of the gamma leaving provShellId for shellId |
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| 242 | G4double transitionEnergy = transitionManager-> |
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| 243 | ReachableShell(Z,shellNum)->TransitionEnergy(index); |
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| 244 | |
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| 245 | // This is the shell where the new vacancy is: it is the same |
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| 246 | // shell where the electron came from |
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| 247 | newShellId = transitionManager-> |
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| 248 | ReachableShell(Z,shellNum)->OriginatingShellId(index); |
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| 249 | |
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| 250 | |
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| 251 | G4DynamicParticle* newPart = new G4DynamicParticle(G4Gamma::Gamma(), |
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| 252 | newGammaDirection, |
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| 253 | transitionEnergy); |
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| 254 | return newPart; |
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| 255 | } |
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| 256 | |
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| 257 | G4DynamicParticle* G4AtomicDeexcitation::GenerateAuger(G4int Z, G4int shellId) |
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| 258 | { |
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| 259 | if(!fAuger) return 0; |
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| 260 | |
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| 261 | |
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| 262 | const G4AtomicTransitionManager* transitionManager = |
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| 263 | G4AtomicTransitionManager::Instance(); |
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| 264 | |
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| 265 | |
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| 266 | |
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| 267 | if (shellId <=0 ) |
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| 268 | {G4Exception("G4AtomicDeexcitation: zero or negative shellId");} |
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| 269 | |
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| 270 | // G4int provShellId = -1; |
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| 271 | G4int maxNumOfShells = transitionManager->NumberOfReachableAugerShells(Z); |
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| 272 | |
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| 273 | const G4AugerTransition* refAugerTransition = |
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| 274 | transitionManager->ReachableAugerShell(Z,maxNumOfShells-1); |
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| 275 | |
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| 276 | |
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| 277 | // This loop gives to shellNum the value of the index of shellId |
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| 278 | // in the vector storing the list of the vacancies in the variuos shells |
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| 279 | // that can originate a NON-radiative transition |
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| 280 | |
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| 281 | // ---- MGP ---- Next line commented out to remove compilation warning |
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| 282 | // G4int p = refAugerTransition->FinalShellId(); |
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| 283 | |
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| 284 | G4int shellNum = 0; |
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| 285 | |
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| 286 | |
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| 287 | if ( shellId <= refAugerTransition->FinalShellId() ) |
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| 288 | //"FinalShellId" is final from the point of view of the elctron who makes the transition, |
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| 289 | // being the Id of the shell in which there is a vacancy |
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| 290 | { |
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| 291 | G4int pippo = transitionManager->ReachableAugerShell(Z,shellNum)->FinalShellId(); |
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| 292 | if (shellId != pippo ) { |
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| 293 | do { |
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| 294 | shellNum++; |
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| 295 | if(shellNum == maxNumOfShells) |
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| 296 | { |
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| 297 | // G4cout << "G4AtomicDeexcitation warning: No Auger transition found" << G4endl; |
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| 298 | // G4cout << "Absorbed enrgy deposited locally" << G4endl; |
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| 299 | return 0; |
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| 300 | // // G4Exception("G4AtomicDeexcitation: No Auger transition found"); |
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| 301 | } |
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| 302 | } |
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| 303 | while (shellId != (transitionManager->ReachableAugerShell(Z,shellNum)->FinalShellId()) ) ; |
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| 304 | } |
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| 305 | /* { |
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| 306 | |
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| 307 | if(shellNum == maxNumOfShells-1) |
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| 308 | { |
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| 309 | G4Exception("G4AtomicDeexcitation: No Auger tramsition found"); |
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| 310 | } |
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| 311 | shellNum++; |
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| 312 | }*/ |
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| 313 | |
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| 314 | |
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| 315 | |
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| 316 | |
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| 317 | // Now we have that shellnum is the shellIndex of the shell named ShellId |
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| 318 | |
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| 319 | // G4cout << " the index of the shell is: "<<shellNum<<G4endl; |
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| 320 | |
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| 321 | // But we have now to select two shells: one for the transition, |
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| 322 | // and another for the auger emission. |
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| 323 | |
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| 324 | G4int transitionLoopShellIndex = 0; |
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| 325 | G4double partSum = 0; |
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| 326 | const G4AugerTransition* anAugerTransition = |
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| 327 | transitionManager->ReachableAugerShell(Z,shellNum); |
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| 328 | |
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| 329 | // G4cout << " corresponding to the ID: "<< anAugerTransition->FinalShellId() << G4endl; |
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| 330 | |
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| 331 | |
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| 332 | G4int transitionSize = |
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| 333 | (anAugerTransition->TransitionOriginatingShellIds())->size(); |
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| 334 | while (transitionLoopShellIndex < transitionSize) { |
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| 335 | |
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| 336 | std::vector<G4int>::const_iterator pos = |
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| 337 | anAugerTransition->TransitionOriginatingShellIds()->begin(); |
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| 338 | |
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| 339 | G4int transitionLoopShellId = *(pos+transitionLoopShellIndex); |
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| 340 | G4int numberOfPossibleAuger = |
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| 341 | (anAugerTransition->AugerTransitionProbabilities(transitionLoopShellId))->size(); |
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| 342 | G4int augerIndex = 0; |
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| 343 | // G4int partSum2 = 0; |
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| 344 | |
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| 345 | |
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| 346 | if (augerIndex < numberOfPossibleAuger) { |
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| 347 | |
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| 348 | do |
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| 349 | { |
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| 350 | G4double thisProb = anAugerTransition->AugerTransitionProbability(augerIndex, |
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| 351 | transitionLoopShellId); |
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| 352 | partSum += thisProb; |
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| 353 | augerIndex++; |
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| 354 | |
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| 355 | } while (augerIndex < numberOfPossibleAuger); |
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| 356 | } |
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| 357 | transitionLoopShellIndex++; |
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| 358 | } |
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| 359 | |
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| 360 | |
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| 361 | |
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| 362 | // Now we have the entire probability of an auger transition for the vacancy |
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| 363 | // located in shellNum (index of shellId) |
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| 364 | |
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| 365 | // AM *********************** F I X E D **************************** AM |
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| 366 | // Here we duplicate the previous loop, this time looking to the sum of the probabilities |
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| 367 | // to be under the random number shoot by G4 UniformRdandom. This could have been done in the |
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| 368 | // previuos loop, while integrating the probabilities. There is a bug that will be fixed |
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| 369 | // 5 minutes from now: a line: |
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| 370 | // G4int numberOfPossibleAuger = (anAugerTransition-> |
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| 371 | // AugerTransitionProbabilities(transitionLoopShellId))->size(); |
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| 372 | // to be inserted. |
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| 373 | // AM *********************** F I X E D **************************** AM |
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| 374 | |
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| 375 | // Remains to get the same result with a single loop. |
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| 376 | |
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| 377 | // AM *********************** F I X E D **************************** AM |
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| 378 | // Another Bug: in EADL Auger Transition are normalized to all the transitions deriving from |
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| 379 | // a vacancy in one shell, but not all of these are present in data tables. So if a transition |
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| 380 | // doesn't occur in the main one a local energy deposition must occur, instead of (like now) |
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| 381 | // generating the last transition present in EADL data. |
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| 382 | // AM *********************** F I X E D **************************** AM |
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| 383 | |
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| 384 | |
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| 385 | G4double totalVacancyAugerProbability = partSum; |
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| 386 | |
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| 387 | |
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| 388 | //And now we start to select the right auger transition and emission |
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| 389 | G4int transitionRandomShellIndex = 0; |
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| 390 | G4int transitionRandomShellId = 1; |
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| 391 | G4int augerIndex = 0; |
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| 392 | partSum = 0; |
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| 393 | G4double partialProb = G4UniformRand(); |
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| 394 | // G4int augerOriginatingShellId = 0; |
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| 395 | |
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| 396 | G4int numberOfPossibleAuger = |
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| 397 | (anAugerTransition->AugerTransitionProbabilities(transitionRandomShellId))->size(); |
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| 398 | G4bool foundFlag = false; |
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| 399 | |
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| 400 | while (transitionRandomShellIndex < transitionSize) { |
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| 401 | |
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| 402 | std::vector<G4int>::const_iterator pos = |
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| 403 | anAugerTransition->TransitionOriginatingShellIds()->begin(); |
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| 404 | |
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| 405 | transitionRandomShellId = *(pos+transitionRandomShellIndex); |
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| 406 | |
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| 407 | augerIndex = 0; |
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| 408 | numberOfPossibleAuger = (anAugerTransition-> |
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| 409 | AugerTransitionProbabilities(transitionRandomShellId))->size(); |
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| 410 | |
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| 411 | while (augerIndex < numberOfPossibleAuger) { |
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| 412 | G4double thisProb =anAugerTransition->AugerTransitionProbability(augerIndex, |
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| 413 | transitionRandomShellId); |
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| 414 | |
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| 415 | partSum += thisProb; |
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| 416 | |
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| 417 | if (partSum >= (partialProb*totalVacancyAugerProbability) ) { // was / |
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| 418 | foundFlag = true; |
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| 419 | break; |
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| 420 | } |
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| 421 | augerIndex++; |
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| 422 | } |
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| 423 | if (partSum >= (partialProb*totalVacancyAugerProbability) ) {break;} // was / |
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| 424 | transitionRandomShellIndex++; |
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| 425 | } |
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| 426 | |
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| 427 | // Now we have the index of the shell from wich comes the auger electron (augerIndex), |
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| 428 | // and the id of the shell, from which the transition e- come (transitionRandomShellid) |
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| 429 | // If no Transition has been found, 0 is returned. |
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| 430 | |
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| 431 | if (!foundFlag) {return 0;} |
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| 432 | |
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| 433 | // Isotropic angular distribution for the outcoming e- |
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| 434 | G4double newcosTh = 1.-2.*G4UniformRand(); |
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| 435 | G4double newsinTh = std::sqrt(1.-newcosTh*newcosTh); |
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| 436 | G4double newPhi = twopi*G4UniformRand(); |
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| 437 | |
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| 438 | G4double xDir = newsinTh*std::sin(newPhi); |
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| 439 | G4double yDir = newsinTh*std::cos(newPhi); |
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| 440 | G4double zDir = newcosTh; |
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| 441 | |
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| 442 | G4ThreeVector newElectronDirection(xDir,yDir,zDir); |
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| 443 | |
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| 444 | // energy of the auger electron emitted |
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| 445 | |
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| 446 | |
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| 447 | G4double transitionEnergy = anAugerTransition->AugerTransitionEnergy(augerIndex, transitionRandomShellId); |
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| 448 | /* |
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| 449 | G4cout << "AUger TransitionId " << anAugerTransition->FinalShellId() << G4endl; |
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| 450 | G4cout << "augerIndex: " << augerIndex << G4endl; |
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| 451 | G4cout << "transitionShellId: " << transitionRandomShellId << G4endl; |
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| 452 | */ |
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| 453 | |
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| 454 | // This is the shell where the new vacancy is: it is the same |
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| 455 | // shell where the electron came from |
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| 456 | newShellId = transitionRandomShellId; |
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| 457 | |
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| 458 | |
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| 459 | G4DynamicParticle* newPart = new G4DynamicParticle(G4Electron::Electron(), |
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| 460 | newElectronDirection, |
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| 461 | transitionEnergy); |
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| 462 | return newPart; |
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| 463 | |
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| 464 | } |
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| 465 | else |
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| 466 | { |
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| 467 | //G4Exception("G4AtomicDeexcitation: no auger transition found"); |
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| 468 | return 0; |
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| 469 | } |
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| 470 | |
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| 471 | } |
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| 472 | |
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| 473 | void G4AtomicDeexcitation::SetCutForSecondaryPhotons(G4double cut) |
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| 474 | { |
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| 475 | minGammaEnergy = cut; |
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| 476 | } |
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| 477 | |
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| 478 | void G4AtomicDeexcitation::SetCutForAugerElectrons(G4double cut) |
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| 479 | { |
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| 480 | minElectronEnergy = cut; |
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| 481 | } |
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| 482 | |
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| 483 | void G4AtomicDeexcitation::ActivateAugerElectronProduction(G4bool val) |
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| 484 | { |
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| 485 | fAuger = val; |
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| 486 | } |
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| 487 | |
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