[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 | // MODULES: G4NuclearDecayChannel.cc |
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| 29 | // |
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| 30 | // Version: 0.b.4 |
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| 31 | // Date: 14/04/00 |
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| 32 | // Author: F Lei & P R Truscott |
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| 33 | // Organisation: DERA UK |
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| 34 | // Customer: ESA/ESTEC, NOORDWIJK |
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| 35 | // Contract: 12115/96/JG/NL Work Order No. 3 |
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| 36 | // |
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| 37 | // %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 38 | // |
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| 39 | // CHANGE HISTORY |
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| 40 | // -------------- |
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| 41 | // |
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| 42 | // 29 February 2000, P R Truscott, DERA UK |
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| 43 | // 0.b.3 release. |
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| 44 | // |
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| 45 | // 18 October 2002, F Lei |
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| 46 | // modified link metheds in DecayIt() to G4PhotoEvaporation() in order to |
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| 47 | // use the new Internal Coversion feature. |
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| 48 | // 13 April 2000, F Lei, DERA UK |
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| 49 | // Changes made are: |
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| 50 | // 1) Use PhotonEvaporation instead of DiscreteGammaDeexcitation |
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| 51 | // 2) verbose control |
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| 52 | // |
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| 53 | // %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 54 | /////////////////////////////////////////////////////////////////////////////// |
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| 55 | // |
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| 56 | #include "G4NuclearLevelManager.hh" |
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| 57 | #include "G4NuclearLevelStore.hh" |
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| 58 | #include "G4NuclearDecayChannel.hh" |
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| 59 | #include "G4DynamicParticle.hh" |
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| 60 | #include "G4DecayProducts.hh" |
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| 61 | #include "G4DecayTable.hh" |
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| 62 | #include "G4PhysicsLogVector.hh" |
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| 63 | #include "G4ParticleChangeForRadDecay.hh" |
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| 64 | #include "G4IonTable.hh" |
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| 65 | |
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| 66 | #include "G4BetaFermiFunction.hh" |
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| 67 | #include "G4PhotonEvaporation.hh" |
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[962] | 68 | #include "G4AtomicTransitionManager.hh" |
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| 69 | #include "G4AtomicShell.hh" |
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[819] | 70 | #include "G4AtomicDeexcitation.hh" |
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| 71 | |
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| 72 | const G4double G4NuclearDecayChannel:: pTolerance = 0.001; |
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| 73 | const G4double G4NuclearDecayChannel:: levelTolerance = 2.0*keV; |
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| 74 | //const G4bool G4NuclearDecayChannel:: FermiOn = true; |
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| 75 | |
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| 76 | /////////////////////////////////////////////////////////////////////////////// |
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| 77 | // |
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| 78 | // |
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| 79 | // Constructor for one decay product (the nucleus). |
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| 80 | // |
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| 81 | G4NuclearDecayChannel::G4NuclearDecayChannel |
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| 82 | (const G4RadioactiveDecayMode &theMode, |
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| 83 | G4int Verbose, |
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| 84 | const G4ParticleDefinition *theParentNucleus, |
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| 85 | G4double theBR, |
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| 86 | G4double theQtransition, |
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| 87 | G4int A, |
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| 88 | G4int Z, |
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| 89 | G4double theDaughterExcitation) : |
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| 90 | G4GeneralPhaseSpaceDecay(Verbose), decayMode(theMode) |
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| 91 | { |
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| 92 | #ifdef G4VERBOSE |
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| 93 | if (GetVerboseLevel()>1) |
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| 94 | {G4cout <<"G4NuclearDecayChannel constructor for " <<G4int(theMode) <<G4endl;} |
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| 95 | #endif |
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| 96 | SetParent(theParentNucleus); |
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| 97 | FillParent(); |
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| 98 | parent_mass = theParentNucleus->GetPDGMass(); |
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| 99 | SetBR (theBR); |
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| 100 | SetNumberOfDaughters (1); |
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| 101 | FillDaughterNucleus (0, A, Z, theDaughterExcitation); |
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| 102 | Qtransition = theQtransition; |
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[1315] | 103 | halflifethreshold = 1e-6*second; |
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| 104 | applyICM = true; |
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| 105 | applyARM = true; |
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[819] | 106 | } |
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| 107 | /////////////////////////////////////////////////////////////////////////////// |
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| 108 | // |
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| 109 | // |
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| 110 | // Constructor for a daughter nucleus and one other particle. |
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| 111 | // |
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| 112 | G4NuclearDecayChannel::G4NuclearDecayChannel |
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| 113 | (const G4RadioactiveDecayMode &theMode, |
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| 114 | G4int Verbose, |
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| 115 | const G4ParticleDefinition *theParentNucleus, |
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| 116 | G4double theBR, |
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| 117 | G4double theQtransition, |
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| 118 | G4int A, |
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| 119 | G4int Z, |
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| 120 | G4double theDaughterExcitation, |
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| 121 | const G4String theDaughterName1) : |
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| 122 | G4GeneralPhaseSpaceDecay(Verbose), decayMode(theMode) |
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| 123 | { |
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| 124 | #ifdef G4VERBOSE |
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| 125 | if (GetVerboseLevel()>1) |
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| 126 | {G4cout <<"G4NuclearDecayChannel constructor for " <<G4int(theMode) <<G4endl;} |
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| 127 | #endif |
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| 128 | SetParent (theParentNucleus); |
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| 129 | FillParent(); |
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| 130 | parent_mass = theParentNucleus->GetPDGMass(); |
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| 131 | SetBR (theBR); |
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| 132 | SetNumberOfDaughters (2); |
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| 133 | SetDaughter(0, theDaughterName1); |
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| 134 | FillDaughterNucleus (1, A, Z, theDaughterExcitation); |
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| 135 | Qtransition = theQtransition; |
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[1315] | 136 | halflifethreshold = 1e-6*second; |
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| 137 | applyICM = true; |
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| 138 | applyARM = true; |
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[819] | 139 | } |
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| 140 | /////////////////////////////////////////////////////////////////////////////// |
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| 141 | // |
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| 142 | // |
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| 143 | // Constructor for a daughter nucleus and two other particles. |
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| 144 | // |
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| 145 | G4NuclearDecayChannel::G4NuclearDecayChannel |
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| 146 | (const G4RadioactiveDecayMode &theMode, |
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| 147 | G4int Verbose, |
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| 148 | const G4ParticleDefinition *theParentNucleus, |
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| 149 | G4double theBR, |
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| 150 | G4double theFFN, |
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| 151 | G4bool betaS, |
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| 152 | CLHEP::RandGeneral* randBeta, |
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| 153 | G4double theQtransition, |
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| 154 | G4int A, |
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| 155 | G4int Z, |
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| 156 | G4double theDaughterExcitation, |
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| 157 | const G4String theDaughterName1, |
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| 158 | const G4String theDaughterName2) : |
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| 159 | G4GeneralPhaseSpaceDecay(Verbose), decayMode(theMode) |
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| 160 | //,BetaSimple(betaS), |
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| 161 | // RandomEnergy(randBeta), Qtransition(theQtransition),FermiFN(theFFN) |
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| 162 | { |
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| 163 | #ifdef G4VERBOSE |
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| 164 | if (GetVerboseLevel()>1) |
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| 165 | {G4cout <<"G4NuclearDecayChannel constructor for " <<G4int(theMode) <<G4endl;} |
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| 166 | #endif |
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| 167 | SetParent (theParentNucleus); |
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| 168 | FillParent(); |
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| 169 | parent_mass = theParentNucleus->GetPDGMass(); |
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| 170 | SetBR (theBR); |
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| 171 | SetNumberOfDaughters (3); |
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| 172 | SetDaughter(0, theDaughterName1); |
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| 173 | SetDaughter(2, theDaughterName2); |
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| 174 | FillDaughterNucleus(1, A, Z, theDaughterExcitation); |
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| 175 | BetaSimple = betaS; |
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| 176 | RandomEnergy = randBeta; |
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| 177 | Qtransition = theQtransition; |
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| 178 | FermiFN = theFFN; |
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[1315] | 179 | halflifethreshold = 1e-6*second; |
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| 180 | applyICM = true; |
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| 181 | applyARM = true; |
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[819] | 182 | } |
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| 183 | |
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| 184 | //////////////////////////////////////////////////////////////////////////////// |
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| 185 | // |
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| 186 | // |
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| 187 | // |
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| 188 | // |
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| 189 | #include "G4HadTmpUtil.hh" |
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| 190 | |
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| 191 | void G4NuclearDecayChannel::FillDaughterNucleus (G4int index, G4int A, G4int Z, |
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| 192 | G4double theDaughterExcitation) |
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| 193 | { |
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| 194 | // |
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| 195 | // |
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| 196 | // Determine if the proposed daughter nucleus has a sensible A, Z and excitation |
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| 197 | // energy. |
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| 198 | // |
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| 199 | if (A<1 || Z<0 || theDaughterExcitation <0.0) |
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| 200 | { |
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| 201 | G4cerr <<"Error in G4NuclearDecayChannel::FillDaughterNucleus"; |
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| 202 | G4cerr <<"Inappropriate values of daughter A, Z or excitation" <<G4endl; |
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| 203 | G4cerr <<"A = " <<A <<" and Z = " <<Z; |
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| 204 | G4cerr <<" Ex = " <<theDaughterExcitation*MeV <<"MeV" <<G4endl; |
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| 205 | G4Exception(__FILE__, G4inttostring(__LINE__), FatalException, "G4NuclearDecayChannel::FillDaughterNucleus"); |
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| 206 | } |
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| 207 | // |
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| 208 | // |
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| 209 | // Save A and Z to local variables. Find the GROUND STATE of the daughter |
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| 210 | // nucleus and save this, as an ion, in the array of daughters. |
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| 211 | // |
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| 212 | daughterA = A; |
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| 213 | daughterZ = Z; |
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| 214 | if (Z == 1 && A == 1) { |
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| 215 | daughterNucleus = G4Proton::Definition(); |
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| 216 | } else if (Z == 0 && A == 1) { |
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| 217 | daughterNucleus = G4Neutron::Definition(); |
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| 218 | } else { |
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| 219 | G4IonTable *theIonTable = |
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| 220 | (G4IonTable*)(G4ParticleTable::GetParticleTable()->GetIonTable()); |
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| 221 | daughterNucleus = theIonTable->GetIon(daughterZ, daughterA, theDaughterExcitation*MeV); |
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| 222 | } |
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| 223 | daughterExcitation = theDaughterExcitation; |
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| 224 | SetDaughter(index, daughterNucleus); |
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| 225 | } |
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| 226 | |
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| 227 | /////////////////////////////////////////////////////////////////////////////// |
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| 228 | // |
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| 229 | // |
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| 230 | // |
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| 231 | // |
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| 232 | G4DecayProducts *G4NuclearDecayChannel::DecayIt (G4double theParentMass) |
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| 233 | { |
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| 234 | // |
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| 235 | // |
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| 236 | // Load-up the details of the parent and daughter particles if they have not |
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| 237 | // been defined properly. |
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| 238 | // |
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| 239 | if (parent == 0) FillParent(); |
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| 240 | if (daughters == 0) FillDaughters(); |
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| 241 | // |
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| 242 | // |
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| 243 | // We want to ensure that the difference between the total |
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| 244 | // parent and daughter masses equals the energy liberated by the transition. |
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| 245 | // |
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| 246 | theParentMass = 0.0; |
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| 247 | for( G4int index=0; index < numberOfDaughters; index++) |
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| 248 | {theParentMass += daughters[index]->GetPDGMass();} |
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| 249 | theParentMass += Qtransition ; |
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| 250 | // bug fix for beta+ decay (flei 25/09/01) |
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| 251 | if (decayMode == 2) theParentMass -= 2*0.511 * MeV; |
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| 252 | // |
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[962] | 253 | #ifdef G4VERBOSE |
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[819] | 254 | if (GetVerboseLevel()>1) { |
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[962] | 255 | G4cout << "G4NuclearDecayChannel::DecayIt "<< G4endl; |
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[819] | 256 | G4cout << "the decay mass = " << theParentMass << G4endl; |
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| 257 | } |
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[962] | 258 | #endif |
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[819] | 259 | |
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| 260 | SetParentMass (theParentMass); |
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| 261 | |
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| 262 | // |
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| 263 | // |
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| 264 | // Define a product vector. |
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| 265 | // |
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| 266 | G4DecayProducts *products = 0; |
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| 267 | // |
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| 268 | // |
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| 269 | // Depending upon the number of daughters, select the appropriate decay |
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| 270 | // kinematics scheme. |
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| 271 | // |
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| 272 | switch (numberOfDaughters) |
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| 273 | { |
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| 274 | case 0: |
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[962] | 275 | G4cerr << "G4NuclearDecayChannel::DecayIt "; |
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| 276 | G4cerr << " daughters not defined " <<G4endl; |
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[819] | 277 | break; |
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| 278 | case 1: |
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| 279 | products = OneBodyDecayIt(); |
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| 280 | break; |
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| 281 | case 2: |
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| 282 | products = TwoBodyDecayIt(); |
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| 283 | break; |
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| 284 | case 3: |
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| 285 | products = BetaDecayIt(); |
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| 286 | break; |
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| 287 | default: |
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| 288 | G4cerr <<"Error in G4NuclearDecayChannel::DecayIt" <<G4endl; |
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| 289 | G4cerr <<"Number of daughters in decay = " <<numberOfDaughters <<G4endl; |
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| 290 | G4Exception(__FILE__, G4inttostring(__LINE__), FatalException, "G4NuclearDecayChannel::DecayIt"); |
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| 291 | } |
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[962] | 292 | if (products == 0) { |
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[819] | 293 | G4cerr << "G4NuclearDecayChannel::DecayIt "; |
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| 294 | G4cerr << *parent_name << " can not decay " << G4endl; |
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| 295 | DumpInfo(); |
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| 296 | } |
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| 297 | // |
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| 298 | // If the decay is to an excited state of the daughter nuclide, we need |
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[1315] | 299 | // to apply the photo-evaporation process. This includes the IT decay mode itself. |
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[819] | 300 | // |
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[962] | 301 | // needed to hold the shell idex after ICM |
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| 302 | G4int shellIndex = -1; |
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| 303 | // |
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[1315] | 304 | if (daughterExcitation > 0.0) |
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[819] | 305 | { |
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| 306 | // |
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| 307 | // Pop the daughter nucleus off the product vector - we need to retain |
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| 308 | // the momentum of this particle. |
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| 309 | // |
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| 310 | dynamicDaughter = products->PopProducts(); |
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| 311 | G4LorentzVector daughterMomentum = dynamicDaughter->Get4Momentum(); |
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| 312 | G4ThreeVector const daughterMomentum1(static_cast<const G4LorentzVector> (daughterMomentum)); |
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| 313 | // |
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| 314 | // |
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| 315 | // Now define a G4Fragment with the correct A, Z and excitation, and declare and |
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[962] | 316 | // initialise a G4PhotonEvaporation object. |
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| 317 | // |
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[819] | 318 | G4Fragment nucleus(daughterA, daughterZ, daughterMomentum); |
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| 319 | G4PhotonEvaporation* deexcitation = new G4PhotonEvaporation; |
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| 320 | deexcitation->SetVerboseLevel(GetVerboseLevel()); |
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[962] | 321 | // switch on/off internal electron conversion |
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[1315] | 322 | deexcitation->SetICM(applyICM); |
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[962] | 323 | // set the maximum life-time for a level that will be treated. Level with life-time longer than this |
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| 324 | // will be outputed as meta-stable isotope |
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| 325 | // |
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[1315] | 326 | deexcitation->SetMaxHalfLife(halflifethreshold); |
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[962] | 327 | // but in IT mode, we need to force the transition |
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[819] | 328 | if (decayMode == 0) { |
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| 329 | deexcitation->RDMForced(true); |
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| 330 | } else { |
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| 331 | deexcitation->RDMForced(false); |
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| 332 | } |
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| 333 | // |
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[1315] | 334 | // Now apply the photo-evaporation |
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| 335 | // Use BreakUp() so limit to one transition at a time, if ICM is requested |
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| 336 | // this change is realted to bug#1001 (F.Lei 07/05/2010) |
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| 337 | G4FragmentVector* gammas = 0; |
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| 338 | if (applyICM) { |
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| 339 | gammas = deexcitation->BreakUp(nucleus); |
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| 340 | } else { |
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| 341 | gammas = deexcitation->BreakItUp(nucleus); |
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| 342 | } |
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| 343 | // the returned G4FragmentVector contains the residual nuclide |
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[819] | 344 | // as its last entry. |
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| 345 | G4int nGammas=gammas->size()-1; |
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| 346 | // |
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| 347 | // Go through each gamma/e- and add it to the decay product. The angular distribution |
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[962] | 348 | // of the gammas is isotropic, and the residual nucleus is assumed not to have suffered |
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[819] | 349 | // any recoil as a result of this de-excitation. |
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| 350 | // |
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| 351 | for (G4int ig=0; ig<nGammas; ig++) |
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| 352 | { |
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| 353 | G4DynamicParticle *theGammaRay = new |
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| 354 | G4DynamicParticle (gammas->operator[](ig)->GetParticleDefinition(), |
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| 355 | gammas->operator[](ig)->GetMomentum()); |
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| 356 | theGammaRay -> SetProperTime(gammas->operator[](ig)->GetCreationTime()); |
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| 357 | products->PushProducts (theGammaRay); |
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| 358 | } |
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| 359 | // |
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[1315] | 360 | // now the nucleus |
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[819] | 361 | G4double finalDaughterExcitation = gammas->operator[](nGammas)->GetExcitationEnergy(); |
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| 362 | // f.lei (03/01/03) this is needed to fix the crach in test18 |
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| 363 | if (finalDaughterExcitation <= 1.0*keV) finalDaughterExcitation = 0 ; |
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[962] | 364 | |
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[819] | 365 | // f.lei (07/03/05) added the delete to fix bug#711 |
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| 366 | if (dynamicDaughter) delete dynamicDaughter; |
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[962] | 367 | |
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| 368 | G4IonTable *theIonTable = (G4IonTable*)(G4ParticleTable::GetParticleTable()->GetIonTable()); |
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[819] | 369 | dynamicDaughter = new G4DynamicParticle |
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| 370 | (theIonTable->GetIon(daughterZ,daughterA,finalDaughterExcitation), |
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| 371 | daughterMomentum1); |
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| 372 | products->PushProducts (dynamicDaughter); |
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[1315] | 373 | |
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[962] | 374 | // retrive the ICM shell index |
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| 375 | shellIndex = deexcitation->GetVacantShellNumber(); |
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| 376 | |
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[819] | 377 | // |
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| 378 | // Delete/reset variables associated with the gammas. |
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| 379 | // |
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| 380 | while (!gammas->empty()) { |
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| 381 | delete *(gammas->end()-1); |
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| 382 | gammas->pop_back(); |
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| 383 | } |
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| 384 | // gammas->clearAndDestroy(); |
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| 385 | delete gammas; |
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| 386 | delete deexcitation; |
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| 387 | } |
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[962] | 388 | // |
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| 389 | // now we have to take care of the EC product which have to go through the ARM |
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| 390 | // |
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| 391 | G4int eShell = -1; |
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| 392 | if (decayMode == 3 || decayMode == 4 || decayMode == 5) { |
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| 393 | switch (decayMode) |
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| 394 | { |
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| 395 | case KshellEC: |
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| 396 | // |
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| 397 | { |
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| 398 | eShell = 0; // --> 0 from 1 (f.lei 30/4/2008) |
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| 399 | } |
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| 400 | break; |
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| 401 | case LshellEC: |
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| 402 | // |
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| 403 | { |
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| 404 | eShell = G4int(G4UniformRand()*3)+1; |
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| 405 | } |
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| 406 | break; |
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| 407 | case MshellEC: |
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| 408 | // |
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| 409 | { |
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[1315] | 410 | // limit the shell index to 6 as specified by the ARM (F.Lei 06/05/2010) |
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| 411 | // eShell = G4int(G4UniformRand()*5)+4; |
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| 412 | eShell = G4int(G4UniformRand()*3)+4; |
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[962] | 413 | } |
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| 414 | break; |
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| 415 | case ERROR: |
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| 416 | default: |
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| 417 | G4Exception("G4NuclearDecayChannel::DecayIt()", "601", |
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| 418 | FatalException, "Error in decay mode selection"); |
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| 419 | } |
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| 420 | } |
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[1315] | 421 | // Also have to deal with the IT case where ICM may have been applied |
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[962] | 422 | // |
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| 423 | if (decayMode == 0) { |
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| 424 | eShell = shellIndex; |
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| 425 | } |
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| 426 | // |
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[1315] | 427 | // now apply ARM if it is requested and there is a vaccancy |
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| 428 | // |
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| 429 | if (applyARM && eShell != -1) { |
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[962] | 430 | G4int aZ = daughterZ; |
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| 431 | if (aZ > 5 && aZ < 100) { // only applies to 5< Z <100 |
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| 432 | // Retrieve the corresponding identifier and binding energy of the selected shell |
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| 433 | const G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance(); |
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| 434 | const G4AtomicShell* shell = transitionManager->Shell(aZ, eShell); |
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| 435 | G4double bindingEnergy = shell->BindingEnergy(); |
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| 436 | G4int shellId = shell->ShellId(); |
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| 437 | |
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| 438 | G4AtomicDeexcitation* atomDeex = new G4AtomicDeexcitation(); |
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| 439 | //the default is no Auger electron generation. |
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| 440 | // Switch it on/off here! |
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| 441 | atomDeex->ActivateAugerElectronProduction(true); |
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| 442 | std::vector<G4DynamicParticle*>* armProducts = atomDeex->GenerateParticles(aZ,shellId); |
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| 443 | |
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| 444 | // pop up the daughter before insertion; |
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| 445 | // f.lei (30/04/2008) check if the total kinetic energy is less than |
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| 446 | // the shell binding energy; if true add the difference to the daughter to conserve the energy |
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| 447 | dynamicDaughter = products->PopProducts(); |
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| 448 | G4double tARMEnergy = 0.0; |
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| 449 | for (size_t i = 0; i < armProducts->size(); i++) { |
---|
| 450 | products->PushProducts ((*armProducts)[i]); |
---|
| 451 | tARMEnergy += (*armProducts)[i]->GetKineticEnergy(); |
---|
| 452 | } |
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| 453 | if ((bindingEnergy - tARMEnergy) > 0.1*keV){ |
---|
| 454 | G4double dEnergy = dynamicDaughter->GetKineticEnergy() + (bindingEnergy - tARMEnergy); |
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| 455 | dynamicDaughter->SetKineticEnergy(dEnergy); |
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| 456 | } |
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| 457 | products->PushProducts(dynamicDaughter); |
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| 458 | |
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| 459 | #ifdef G4VERBOSE |
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| 460 | if (GetVerboseLevel()>0) |
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| 461 | { |
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| 462 | G4cout <<"G4NuclearDecayChannel::Selected shell number for ARM = " <<shellId <<G4endl; |
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| 463 | G4cout <<"G4NuclearDecayChannel::ARM products = " <<armProducts->size()<<G4endl; |
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| 464 | G4cout <<" The binding energy = " << bindingEnergy << G4endl; |
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| 465 | G4cout <<" Total ARM particle kinetic energy = " << tARMEnergy << G4endl; |
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| 466 | } |
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| 467 | #endif |
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| 468 | |
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| 469 | delete armProducts; |
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| 470 | delete atomDeex; |
---|
| 471 | } |
---|
| 472 | } |
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| 473 | |
---|
[819] | 474 | return products; |
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| 475 | } |
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| 476 | //////////////////////////////////////////////////////////////////////////////// |
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| 477 | // |
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| 478 | |
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| 479 | G4DecayProducts *G4NuclearDecayChannel::BetaDecayIt() |
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| 480 | |
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| 481 | { |
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| 482 | if (GetVerboseLevel()>1) G4cout << "G4Decay::BetaDecayIt()"<<G4endl; |
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| 483 | |
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| 484 | //daughters'mass |
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| 485 | G4double daughtermass[3]; |
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| 486 | G4double sumofdaughtermass = 0.0; |
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| 487 | G4double pmass = GetParentMass(); |
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| 488 | for (G4int index=0; index<3; index++) |
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| 489 | { |
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| 490 | daughtermass[index] = daughters[index]->GetPDGMass(); |
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| 491 | sumofdaughtermass += daughtermass[index]; |
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| 492 | } |
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| 493 | |
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| 494 | //create parent G4DynamicParticle at rest |
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| 495 | G4ParticleMomentum dummy; |
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| 496 | G4DynamicParticle * parentparticle = new G4DynamicParticle( parent, dummy, 0.0); |
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| 497 | |
---|
| 498 | //create G4Decayproducts |
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| 499 | G4DecayProducts *products = new G4DecayProducts(*parentparticle); |
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| 500 | delete parentparticle; |
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| 501 | |
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| 502 | G4double Q = pmass - sumofdaughtermass; |
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| 503 | |
---|
| 504 | // 09/11/2004 flei |
---|
| 505 | // All Beta decays are now treated with the improved 3 body decay algorithm. No more slow/fast modes |
---|
| 506 | /* |
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| 507 | if (BetaSimple == true) { |
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| 508 | |
---|
| 509 | // Use the histogramed distribution to generate the beta energy |
---|
| 510 | G4double daughtermomentum[2]; |
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| 511 | G4double daughterenergy[2]; |
---|
| 512 | daughterenergy[0] = RandomEnergy->shoot() * Q; |
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| 513 | daughtermomentum[0] = std::sqrt(daughterenergy[0]*daughterenergy[0] + |
---|
| 514 | 2.0*daughterenergy[0] * daughtermass[0]); |
---|
| 515 | // the recoil neuleus is asummed to have a maximum energy of Q/daughterA/1000. |
---|
| 516 | daughterenergy[1] = G4UniformRand() * Q/(1000.*daughterA); |
---|
| 517 | G4double recoilmomentumsquared = daughterenergy[1]*daughterenergy[1] + |
---|
| 518 | 2.0*daughterenergy[1] * daughtermass[1]; |
---|
| 519 | if (recoilmomentumsquared < 0.0) recoilmomentumsquared = 0.0; |
---|
| 520 | daughtermomentum[1] = std::sqrt(recoilmomentumsquared); |
---|
| 521 | // |
---|
| 522 | //create daughter G4DynamicParticle |
---|
| 523 | G4double costheta, sintheta, phi, sinphi, cosphi; |
---|
| 524 | // G4double costhetan, sinthetan, phin, sinphin, cosphin; |
---|
| 525 | costheta = 2.*G4UniformRand()-1.0; |
---|
| 526 | sintheta = std::sqrt((1.0-costheta)*(1.0+costheta)); |
---|
| 527 | phi = twopi*G4UniformRand()*rad; |
---|
| 528 | sinphi = std::sin(phi); |
---|
| 529 | cosphi = std::cos(phi); |
---|
| 530 | G4ParticleMomentum direction0(sintheta*cosphi,sintheta*sinphi,costheta); |
---|
| 531 | G4DynamicParticle * daughterparticle |
---|
| 532 | = new G4DynamicParticle( daughters[0], direction0*daughtermomentum[0]); |
---|
| 533 | products->PushProducts(daughterparticle); |
---|
| 534 | // The two products are independent in directions |
---|
| 535 | costheta = 2.*G4UniformRand()-1.0; |
---|
| 536 | sintheta = std::sqrt((1.0-costheta)*(1.0+costheta)); |
---|
| 537 | phi = twopi*G4UniformRand()*rad; |
---|
| 538 | sinphi = std::sin(phi); |
---|
| 539 | cosphi = std::cos(phi); |
---|
| 540 | G4ParticleMomentum direction1(sintheta*cosphi,sintheta*sinphi,costheta); |
---|
| 541 | daughterparticle |
---|
| 542 | = new G4DynamicParticle( daughters[1], direction1*daughtermomentum[1]); |
---|
| 543 | products->PushProducts(daughterparticle); |
---|
| 544 | |
---|
| 545 | // the neutrino is igored in this case |
---|
| 546 | |
---|
| 547 | } else { |
---|
| 548 | */ |
---|
| 549 | /* original slow method |
---|
| 550 | //calculate daughter momentum |
---|
| 551 | // Generate two |
---|
| 552 | G4double rd1, rd2; |
---|
| 553 | G4double daughtermomentum[3]; |
---|
| 554 | G4double daughterenergy[3]; |
---|
| 555 | G4double momentummax=0.0, momentumsum = 0.0; |
---|
| 556 | G4double fermif; |
---|
| 557 | G4BetaFermiFunction* aBetaFermiFunction; |
---|
| 558 | if (decayMode == 1) { |
---|
| 559 | // beta-decay |
---|
| 560 | aBetaFermiFunction = new G4BetaFermiFunction (daughterA, daughterZ); |
---|
| 561 | } else { |
---|
| 562 | // beta+decay |
---|
| 563 | aBetaFermiFunction = new G4BetaFermiFunction (daughterA, -daughterZ); |
---|
| 564 | } |
---|
| 565 | if (GetVerboseLevel()>1) { |
---|
| 566 | G4cout<< " Q = " <<Q<<G4endl; |
---|
| 567 | G4cout<< " daughterA = " <<daughterA<<G4endl; |
---|
| 568 | G4cout<< " daughterZ = " <<daughterZ<<G4endl; |
---|
| 569 | G4cout<< " decayMode = " <<static_cast<G4int>(decayMode) << G4endl; |
---|
| 570 | G4cout<< " FermiFN = " <<FermiFN<<G4endl; |
---|
| 571 | } |
---|
| 572 | do |
---|
| 573 | { |
---|
| 574 | rd1 = G4UniformRand(); |
---|
| 575 | rd2 = G4UniformRand(); |
---|
| 576 | |
---|
| 577 | momentummax = 0.0; |
---|
| 578 | momentumsum = 0.0; |
---|
| 579 | |
---|
| 580 | // daughter 0 |
---|
| 581 | |
---|
| 582 | // energy = rd2*(pmass - sumofdaughtermass); |
---|
| 583 | daughtermomentum[0] = std::sqrt(rd2) * std::sqrt((Q + 2.0*daughtermass[0])*Q); |
---|
| 584 | daughterenergy[0] = std::sqrt(daughtermomentum[0]*daughtermomentum[0] + |
---|
| 585 | daughtermass[0] * daughtermass[0]) - daughtermass[0]; |
---|
| 586 | if ( daughtermomentum[0] >momentummax )momentummax = daughtermomentum[0]; |
---|
| 587 | momentumsum += daughtermomentum[0]; |
---|
| 588 | |
---|
| 589 | // daughter 2 |
---|
| 590 | // energy = (1.-rd1)*(pmass - sumofdaughtermass); |
---|
| 591 | daughtermomentum[2] = std::sqrt(rd1)*std::sqrt((Q + 2.0*daughtermass[2])*Q); |
---|
| 592 | daughterenergy[2] = std::sqrt(daughtermomentum[2]*daughtermomentum[2] + |
---|
| 593 | daughtermass[2] * daughtermass[2]) - daughtermass[2]; |
---|
| 594 | if ( daughtermomentum[2] >momentummax )momentummax = daughtermomentum[2]; |
---|
| 595 | momentumsum += daughtermomentum[2]; |
---|
| 596 | |
---|
| 597 | // daughter 1 |
---|
| 598 | |
---|
| 599 | daughterenergy[1] = Q - daughterenergy[0] - daughterenergy[2]; |
---|
| 600 | if (daughterenergy[1] > 0.0) { |
---|
| 601 | daughtermomentum[1] = std::sqrt(daughterenergy[1]*daughterenergy[1] + |
---|
| 602 | 2.0*daughterenergy[1] * daughtermass[1]); |
---|
| 603 | if ( daughtermomentum[1] >momentummax ) momentummax = |
---|
| 604 | daughtermomentum[1]; |
---|
| 605 | momentumsum += daughtermomentum[1]; |
---|
| 606 | } else { |
---|
| 607 | momentummax = momentumsum = Q; |
---|
| 608 | } |
---|
| 609 | // beta particles is sampled with no coulomb effects applied above. Now |
---|
| 610 | // apply the Fermi function using rejection method. |
---|
| 611 | daughterenergy[0] = daughterenergy[0]*MeV/0.511; |
---|
| 612 | fermif = aBetaFermiFunction->GetFF(daughterenergy[0])/FermiFN; |
---|
| 613 | // fermif: normalised Fermi factor |
---|
| 614 | if (G4UniformRand() > fermif) momentummax = momentumsum = Q; |
---|
| 615 | // rejection method |
---|
| 616 | } while (momentummax > momentumsum - momentummax ); |
---|
| 617 | delete aBetaFermiFunction; |
---|
| 618 | |
---|
| 619 | // output message |
---|
| 620 | if (GetVerboseLevel()>1) { |
---|
| 621 | G4cout <<" daughter 0:" <<daughtermomentum[0]/GeV <<"[GeV/c]" <<G4endl; |
---|
| 622 | G4cout <<" daughter 1:" <<daughtermomentum[1]/GeV <<"[GeV/c]" <<G4endl; |
---|
| 623 | G4cout <<" daughter 2:" <<daughtermomentum[2]/GeV <<"[GeV/c]" <<G4endl; |
---|
| 624 | G4cout <<" momentum sum:" <<momentumsum/GeV <<"[GeV/c]" <<G4endl; |
---|
| 625 | } |
---|
| 626 | */ |
---|
| 627 | // faster method as suggested by Dirk Kruecker of FZ-Julich |
---|
| 628 | G4double daughtermomentum[3]; |
---|
| 629 | G4double daughterenergy[3]; |
---|
| 630 | // Use the histogramed distribution to generate the beta energy |
---|
| 631 | daughterenergy[0] = RandomEnergy->shoot() * Q; |
---|
| 632 | daughtermomentum[0] = std::sqrt(daughterenergy[0]*daughterenergy[0] + |
---|
| 633 | 2.0*daughterenergy[0] * daughtermass[0]); |
---|
| 634 | |
---|
| 635 | //neutrino energy distribution is flat within the kinematical limits |
---|
| 636 | G4double rd = 2*G4UniformRand()-1; |
---|
| 637 | // limits |
---|
| 638 | G4double Mme=pmass-daughtermass[0]; |
---|
| 639 | G4double K=0.5-daughtermass[1]*daughtermass[1]/(2*Mme*Mme-4*pmass*daughterenergy[0]); |
---|
| 640 | |
---|
| 641 | daughterenergy[2]=K*(Mme-daughterenergy[0]+rd*daughtermomentum[0]); |
---|
| 642 | daughtermomentum[2] = daughterenergy[2] ; |
---|
| 643 | |
---|
| 644 | // the recoil neuleus |
---|
| 645 | daughterenergy[1] = Q-daughterenergy[0]-daughterenergy[2]; |
---|
| 646 | G4double recoilmomentumsquared = daughterenergy[1]*daughterenergy[1] + |
---|
| 647 | 2.0*daughterenergy[1] * daughtermass[1]; |
---|
| 648 | if (recoilmomentumsquared < 0.0) recoilmomentumsquared = 0.0; |
---|
| 649 | daughtermomentum[1] = std::sqrt(recoilmomentumsquared); |
---|
| 650 | |
---|
| 651 | // output message |
---|
| 652 | if (GetVerboseLevel()>1) { |
---|
| 653 | G4cout <<" daughter 0:" <<daughtermomentum[0]/GeV <<"[GeV/c]" <<G4endl; |
---|
| 654 | G4cout <<" daughter 1:" <<daughtermomentum[1]/GeV <<"[GeV/c]" <<G4endl; |
---|
| 655 | G4cout <<" daughter 2:" <<daughtermomentum[2]/GeV <<"[GeV/c]" <<G4endl; |
---|
| 656 | } |
---|
| 657 | //create daughter G4DynamicParticle |
---|
| 658 | G4double costheta, sintheta, phi, sinphi, cosphi; |
---|
| 659 | G4double costhetan, sinthetan, phin, sinphin, cosphin; |
---|
| 660 | costheta = 2.*G4UniformRand()-1.0; |
---|
| 661 | sintheta = std::sqrt((1.0-costheta)*(1.0+costheta)); |
---|
| 662 | phi = twopi*G4UniformRand()*rad; |
---|
| 663 | sinphi = std::sin(phi); |
---|
| 664 | cosphi = std::cos(phi); |
---|
| 665 | G4ParticleMomentum direction0(sintheta*cosphi,sintheta*sinphi,costheta); |
---|
| 666 | G4DynamicParticle * daughterparticle |
---|
| 667 | = new G4DynamicParticle( daughters[0], direction0*daughtermomentum[0]); |
---|
| 668 | products->PushProducts(daughterparticle); |
---|
| 669 | |
---|
| 670 | costhetan = (daughtermomentum[1]*daughtermomentum[1]- |
---|
| 671 | daughtermomentum[2]*daughtermomentum[2]- |
---|
| 672 | daughtermomentum[0]*daughtermomentum[0])/ |
---|
| 673 | (2.0*daughtermomentum[2]*daughtermomentum[0]); |
---|
| 674 | // added the following test to avoid rounding erros. A problem |
---|
| 675 | // reported bye Ben Morgan of Uni.Warwick |
---|
| 676 | if (costhetan > 1.) costhetan = 1.; |
---|
| 677 | if (costhetan < -1.) costhetan = -1.; |
---|
| 678 | sinthetan = std::sqrt((1.0-costhetan)*(1.0+costhetan)); |
---|
| 679 | phin = twopi*G4UniformRand()*rad; |
---|
| 680 | sinphin = std::sin(phin); |
---|
| 681 | cosphin = std::cos(phin); |
---|
| 682 | G4ParticleMomentum direction2; |
---|
| 683 | direction2.setX( sinthetan*cosphin*costheta*cosphi - |
---|
| 684 | sinthetan*sinphin*sinphi + costhetan*sintheta*cosphi); |
---|
| 685 | direction2.setY( sinthetan*cosphin*costheta*sinphi + |
---|
| 686 | sinthetan*sinphin*cosphi + costhetan*sintheta*sinphi); |
---|
| 687 | direction2.setZ( -sinthetan*cosphin*sintheta + |
---|
| 688 | costhetan*costheta); |
---|
| 689 | daughterparticle = new G4DynamicParticle |
---|
| 690 | ( daughters[2], direction2*(daughtermomentum[2]/direction2.mag())); |
---|
| 691 | products->PushProducts(daughterparticle); |
---|
| 692 | |
---|
| 693 | daughterparticle = |
---|
| 694 | new G4DynamicParticle (daughters[1], |
---|
| 695 | (direction0*daughtermomentum[0] + |
---|
| 696 | direction2*(daughtermomentum[2]/direction2.mag()))*(-1.0)); |
---|
| 697 | products->PushProducts(daughterparticle); |
---|
| 698 | // } |
---|
| 699 | // delete daughterparticle; |
---|
| 700 | |
---|
| 701 | if (GetVerboseLevel()>1) { |
---|
| 702 | G4cout << "G4NuclearDecayChannel::BetaDecayIt "; |
---|
| 703 | G4cout << " create decay products in rest frame " <<G4endl; |
---|
| 704 | products->DumpInfo(); |
---|
| 705 | } |
---|
| 706 | return products; |
---|
| 707 | } |
---|