[824] | 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: G4ExcitedNucleonConstructor.cc,v 1.11 2006/06/29 19:27:08 gunter Exp $ |
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[850] | 28 | // GEANT4 tag $Name: HEAD $ |
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[824] | 29 | // |
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| 30 | // |
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| 31 | // -------------------------------------------------------------- |
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| 32 | // GEANT 4 class implementation file |
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| 33 | // History: first implementation, based on object model of |
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| 34 | // 10 oct 1998 H.Kurashige |
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| 35 | // --------------------------------------------------------------- |
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| 36 | |
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| 37 | |
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| 38 | #include "G4ExcitedNucleonConstructor.hh" |
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| 39 | |
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| 40 | #include "G4ParticleDefinition.hh" |
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| 41 | #include "G4ParticleTable.hh" |
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| 42 | #include "G4ShortLivedTable.hh" |
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| 43 | #include "G4PhaseSpaceDecayChannel.hh" |
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| 44 | #include "G4VDecayChannel.hh" |
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| 45 | #include "G4DecayTable.hh" |
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| 46 | |
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| 47 | |
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| 48 | G4ExcitedNucleonConstructor::G4ExcitedNucleonConstructor(): |
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| 49 | G4ExcitedBaryonConstructor(NStates, NucleonIsoSpin) |
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| 50 | { |
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| 51 | |
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| 52 | } |
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| 53 | |
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| 54 | G4ExcitedNucleonConstructor::~G4ExcitedNucleonConstructor() |
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| 55 | { |
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| 56 | } |
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| 57 | |
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| 58 | G4int G4ExcitedNucleonConstructor::GetEncoding(G4int iIsoSpin3, G4int idxState) |
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| 59 | { |
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| 60 | G4int encoding; |
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| 61 | // Delta has exceptinal encoding |
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| 62 | if ((idxState==1)||(idxState==6)||(idxState==8)||(idxState==9)||(idxState==12) ) { |
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| 63 | encoding = GetEncodingOffset(idxState); |
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| 64 | if ((iIsoSpin3==3)||(iIsoSpin3==-3)) { |
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| 65 | // normal encoding |
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| 66 | encoding += 1000*GetQuarkContents(0, iIsoSpin3); |
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| 67 | encoding += 100*GetQuarkContents(1, iIsoSpin3); |
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| 68 | encoding += 10*GetQuarkContents(2, iIsoSpin3); |
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| 69 | } else if (iIsoSpin3== +1){ |
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| 70 | // 1st <--> 2nd quark |
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| 71 | encoding += 1000*GetQuarkContents(0, iIsoSpin3); |
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| 72 | encoding += 10*GetQuarkContents(1, iIsoSpin3); |
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| 73 | encoding += 100*GetQuarkContents(2, iIsoSpin3); |
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| 74 | } else if (iIsoSpin3== -1){ |
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| 75 | // 1st <--> 0th quark |
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| 76 | encoding += 100*GetQuarkContents(0, iIsoSpin3); |
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| 77 | encoding += 1000*GetQuarkContents(1, iIsoSpin3); |
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| 78 | encoding += 10*GetQuarkContents(2, iIsoSpin3); |
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| 79 | } |
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| 80 | encoding += GetiSpin(idxState) +1; |
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| 81 | } else { |
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| 82 | encoding = G4ExcitedBaryonConstructor::GetEncoding(iIsoSpin3, idxState); |
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| 83 | } |
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| 84 | return encoding; |
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| 85 | } |
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| 86 | |
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| 87 | G4DecayTable* G4ExcitedNucleonConstructor::CreateDecayTable( |
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| 88 | const G4String& parentName, |
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| 89 | G4int iIso3, |
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| 90 | G4int iState, |
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| 91 | G4bool fAnti) |
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| 92 | { |
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| 93 | // create decay table |
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| 94 | G4DecayTable* decayTable = new G4DecayTable(); |
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| 95 | |
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| 96 | G4double br; |
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| 97 | if ( (br=bRatio[iState][NGamma]) >0.0) { |
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| 98 | AddNGammaMode( decayTable, parentName, br, iIso3, fAnti); |
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| 99 | } |
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| 100 | |
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| 101 | if ( (br=bRatio[iState][NPi]) >0.0) { |
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| 102 | AddNPiMode( decayTable, parentName, br, iIso3, fAnti); |
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| 103 | } |
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| 104 | |
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| 105 | if ( (br=bRatio[iState][NEta]) >0.0) { |
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| 106 | AddNEtaMode( decayTable, parentName, br, iIso3, fAnti); |
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| 107 | } |
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| 108 | |
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| 109 | if ( (br=bRatio[iState][NOmega]) >0.0) { |
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| 110 | AddNOmegaMode( decayTable, parentName, br, iIso3, fAnti); |
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| 111 | } |
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| 112 | |
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| 113 | if ( (br=bRatio[iState][NRho]) >0.0) { |
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| 114 | AddNRhoMode( decayTable, parentName, br, iIso3, fAnti); |
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| 115 | } |
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| 116 | |
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| 117 | if ( (br=bRatio[iState][N2Pi]) >0.0) { |
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| 118 | AddN2PiMode( decayTable, parentName, br, iIso3, fAnti); |
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| 119 | } |
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| 120 | |
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| 121 | if ( (br=bRatio[iState][DeltaPi]) >0.0) { |
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| 122 | AddDeltaPiMode( decayTable, parentName, br, iIso3, fAnti); |
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| 123 | } |
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| 124 | |
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| 125 | if ( (br=bRatio[iState][NStarPi]) >0.0) { |
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| 126 | AddNStarPiMode( decayTable, parentName, br, iIso3, fAnti); |
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| 127 | } |
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| 128 | |
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| 129 | if ( (br=bRatio[iState][LambdaK]) >0.0) { |
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| 130 | AddLambdaKMode( decayTable, parentName, br, iIso3, fAnti); |
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| 131 | } |
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| 132 | |
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| 133 | return decayTable; |
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| 134 | } |
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| 135 | |
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| 136 | G4DecayTable* G4ExcitedNucleonConstructor::AddNGammaMode( |
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| 137 | G4DecayTable* decayTable, const G4String& nameParent, |
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| 138 | G4double br, G4int iIso3, G4bool fAnti) |
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| 139 | { |
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| 140 | G4VDecayChannel* mode; |
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| 141 | |
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| 142 | // |
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| 143 | G4String daughterN; |
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| 144 | if (iIso3 == +1) { |
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| 145 | daughterN = "proton"; |
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| 146 | } else { |
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| 147 | daughterN = "neutron"; |
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| 148 | } |
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| 149 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 150 | |
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| 151 | // create decay channel [parent BR #daughters] |
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| 152 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2, |
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| 153 | daughterN,"gamma"); |
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| 154 | // add decay table |
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| 155 | decayTable->Insert(mode); |
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| 156 | |
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| 157 | return decayTable; |
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| 158 | } |
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| 159 | |
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| 160 | G4DecayTable* G4ExcitedNucleonConstructor::AddNPiMode( |
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| 161 | G4DecayTable* decayTable, const G4String& nameParent, |
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| 162 | G4double br, G4int iIso3, G4bool fAnti) |
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| 163 | { |
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| 164 | G4VDecayChannel* mode; |
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| 165 | |
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| 166 | G4String daughterN; |
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| 167 | G4String daughterPi; |
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| 168 | |
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| 169 | // ------------ N pi0 ------------ |
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| 170 | // determine daughters |
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| 171 | if (iIso3 == +1) { |
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| 172 | daughterN = "proton"; |
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| 173 | daughterPi = "pi0"; |
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| 174 | } else { |
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| 175 | daughterN = "neutron"; |
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| 176 | daughterPi = "pi0"; |
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| 177 | } |
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| 178 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 179 | // create decay channel [parent BR #daughters] |
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| 180 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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| 181 | daughterN,daughterPi); |
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| 182 | // add decay table |
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| 183 | decayTable->Insert(mode); |
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| 184 | |
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| 185 | // -------------N pi +/- -------------- |
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| 186 | // determine daughters |
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| 187 | if (iIso3 == +1) { |
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| 188 | daughterN = "neutron"; |
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| 189 | if (!fAnti) { |
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| 190 | daughterPi = "pi+"; |
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| 191 | } else { |
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| 192 | daughterPi = "pi-"; |
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| 193 | } |
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| 194 | } else { |
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| 195 | daughterN = "proton"; |
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| 196 | if (!fAnti) { |
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| 197 | daughterPi = "pi-"; |
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| 198 | } else { |
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| 199 | daughterPi = "pi+"; |
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| 200 | } |
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| 201 | } |
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| 202 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 203 | |
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| 204 | // create decay channel [parent BR #daughters] |
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| 205 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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| 206 | daughterN,daughterPi); |
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| 207 | // add decay table |
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| 208 | decayTable->Insert(mode); |
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| 209 | |
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| 210 | return decayTable; |
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| 211 | } |
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| 212 | |
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| 213 | G4DecayTable* G4ExcitedNucleonConstructor::AddNEtaMode( |
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| 214 | G4DecayTable* decayTable, const G4String& nameParent, |
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| 215 | G4double br, G4int iIso3, G4bool fAnti) |
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| 216 | { |
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| 217 | G4VDecayChannel* mode; |
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| 218 | |
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| 219 | G4String daughterN; |
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| 220 | |
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| 221 | // ------------ N eta------------ |
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| 222 | // determine daughters |
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| 223 | if (iIso3 == +1) { |
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| 224 | daughterN = "proton"; |
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| 225 | } else { |
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| 226 | daughterN = "neutron"; |
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| 227 | } |
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| 228 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 229 | // create decay channel [parent BR #daughters] |
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| 230 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2, |
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| 231 | daughterN, "eta"); |
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| 232 | // add decay table |
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| 233 | decayTable->Insert(mode); |
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| 234 | |
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| 235 | return decayTable; |
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| 236 | } |
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| 237 | |
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| 238 | G4DecayTable* G4ExcitedNucleonConstructor::AddNOmegaMode( |
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| 239 | G4DecayTable* decayTable, const G4String& nameParent, |
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| 240 | G4double br, G4int iIso3, G4bool fAnti) |
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| 241 | { |
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| 242 | G4VDecayChannel* mode; |
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| 243 | |
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| 244 | G4String daughterN; |
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| 245 | |
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| 246 | // ------------ N omega------------ |
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| 247 | // determine daughters |
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| 248 | if (iIso3 == +1) { |
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| 249 | daughterN = "proton"; |
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| 250 | } else { |
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| 251 | daughterN = "neutron"; |
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| 252 | } |
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| 253 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 254 | // create decay channel [parent BR #daughters] |
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| 255 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2, |
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| 256 | daughterN, "omega"); |
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| 257 | // add decay table |
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| 258 | decayTable->Insert(mode); |
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| 259 | |
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| 260 | return decayTable; |
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| 261 | } |
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| 262 | |
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| 263 | G4DecayTable* G4ExcitedNucleonConstructor::AddNRhoMode( |
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| 264 | G4DecayTable* decayTable, const G4String& nameParent, |
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| 265 | G4double br, G4int iIso3, G4bool fAnti) |
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| 266 | { |
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| 267 | G4VDecayChannel* mode; |
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| 268 | |
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| 269 | G4String daughterN; |
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| 270 | G4String daughterRho; |
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| 271 | |
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| 272 | // ------------ N rho0 ------------ |
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| 273 | // determine daughters |
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| 274 | if (iIso3 == +1) { |
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| 275 | daughterN = "proton"; |
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| 276 | daughterRho = "rho0"; |
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| 277 | } else { |
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| 278 | daughterN = "neutron"; |
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| 279 | daughterRho = "rho0"; |
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| 280 | } |
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| 281 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 282 | // create decay channel [parent BR #daughters] |
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| 283 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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| 284 | daughterN,daughterRho); |
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| 285 | // add decay table |
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| 286 | decayTable->Insert(mode); |
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| 287 | |
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| 288 | // -------------N rho+/- -------------- |
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| 289 | // determine daughters |
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| 290 | if (iIso3 == +1) { |
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| 291 | daughterN = "neutron"; |
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| 292 | if (!fAnti) { |
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| 293 | daughterRho = "rho+"; |
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| 294 | } else { |
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| 295 | daughterRho = "rho-"; |
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| 296 | } |
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| 297 | } else { |
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| 298 | daughterN = "proton"; |
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| 299 | if (!fAnti) { |
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| 300 | daughterRho = "rho-"; |
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| 301 | } else { |
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| 302 | daughterRho = "rho+"; |
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| 303 | } |
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| 304 | } |
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| 305 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 306 | |
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| 307 | // create decay channel [parent BR #daughters] |
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| 308 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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| 309 | daughterN,daughterRho); |
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| 310 | // add decay table |
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| 311 | decayTable->Insert(mode); |
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| 312 | |
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| 313 | return decayTable; |
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| 314 | } |
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| 315 | |
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| 316 | G4DecayTable* G4ExcitedNucleonConstructor::AddN2PiMode( |
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| 317 | G4DecayTable* decayTable, const G4String& nameParent, |
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| 318 | G4double br, G4int iIso3, G4bool fAnti) |
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| 319 | { |
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| 320 | // Decay Modes |
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| 321 | // N* --> N + pi + pi |
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| 322 | // Only I=0 states are included for 2-pi system |
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| 323 | |
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| 324 | G4VDecayChannel* mode; |
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| 325 | |
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| 326 | G4String daughterN; |
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| 327 | G4String daughterPi1; |
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| 328 | G4String daughterPi2; |
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| 329 | |
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| 330 | // -------------N pi+ pi- -------------- |
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| 331 | // determine daughters |
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| 332 | if (iIso3 == +1) { |
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| 333 | daughterN = "proton"; |
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| 334 | daughterPi1 = "pi+"; |
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| 335 | daughterPi2 = "pi-"; |
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| 336 | } else { |
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| 337 | daughterN = "neutron"; |
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| 338 | daughterPi1 = "pi+"; |
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| 339 | daughterPi2 = "pi-"; |
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| 340 | } |
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| 341 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 342 | |
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| 343 | // create decay channel [parent BR #daughters] |
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| 344 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 3, |
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| 345 | daughterN,daughterPi1,daughterPi2); |
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| 346 | // add decay table |
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| 347 | decayTable->Insert(mode); |
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| 348 | |
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| 349 | // -------------N pi0 pi0 -------------- |
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| 350 | // determine daughters |
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| 351 | if (iIso3 == +1) { |
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| 352 | daughterN = "proton"; |
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| 353 | daughterPi1 = "pi0"; |
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| 354 | daughterPi2 = "pi0"; |
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| 355 | } else { |
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| 356 | daughterN = "neutron"; |
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| 357 | daughterPi1 = "pi0"; |
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| 358 | daughterPi2 = "pi0"; |
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| 359 | } |
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| 360 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 361 | |
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| 362 | // create decay channel [parent BR #daughters] |
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| 363 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 3, |
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| 364 | daughterN,daughterPi1,daughterPi2); |
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| 365 | // add decay table |
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| 366 | decayTable->Insert(mode); |
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| 367 | |
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| 368 | return decayTable; |
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| 369 | } |
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| 370 | |
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| 371 | G4DecayTable* G4ExcitedNucleonConstructor::AddNStarPiMode( |
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| 372 | G4DecayTable* decayTable, const G4String& nameParent, |
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| 373 | G4double br, G4int iIso3, G4bool fAnti) |
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| 374 | { |
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| 375 | G4VDecayChannel* mode; |
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| 376 | |
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| 377 | G4String daughterN; |
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| 378 | G4String daughterPi; |
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| 379 | |
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| 380 | // ------------ N pi0 ------------ |
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| 381 | // determine daughters |
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| 382 | if (iIso3 == +1) { |
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| 383 | daughterN = "N(1440)+"; |
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| 384 | daughterPi = "pi0"; |
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| 385 | } else { |
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| 386 | daughterN = "N(1440)0"; |
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| 387 | daughterPi = "pi0"; |
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| 388 | } |
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| 389 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 390 | // create decay channel [parent BR #daughters] |
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| 391 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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| 392 | daughterN,daughterPi); |
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| 393 | // add decay table |
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| 394 | decayTable->Insert(mode); |
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| 395 | |
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| 396 | // -------------N pi +/- -------------- |
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| 397 | // determine daughters |
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| 398 | if (iIso3 == +1) { |
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| 399 | daughterN = "N(1440)0"; |
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| 400 | if (!fAnti) { |
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| 401 | daughterPi = "pi+"; |
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| 402 | } else { |
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| 403 | daughterPi = "pi-"; |
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| 404 | } |
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| 405 | } else { |
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| 406 | daughterN = "N(1440)+"; |
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| 407 | if (!fAnti) { |
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| 408 | daughterPi = "pi-"; |
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| 409 | } else { |
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| 410 | daughterPi = "pi+"; |
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| 411 | } |
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| 412 | } |
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| 413 | if (fAnti) daughterN = "anti_" + daughterN; |
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| 414 | |
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| 415 | // create decay channel [parent BR #daughters] |
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| 416 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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| 417 | daughterN,daughterPi); |
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| 418 | // add decay table |
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| 419 | decayTable->Insert(mode); |
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| 420 | |
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| 421 | return decayTable; |
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| 422 | } |
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| 423 | |
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| 424 | G4DecayTable* G4ExcitedNucleonConstructor::AddDeltaPiMode( |
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| 425 | G4DecayTable* decayTable, const G4String& nameParent, |
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| 426 | G4double br, G4int iIso3, G4bool fAnti) |
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| 427 | { |
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| 428 | G4VDecayChannel* mode; |
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| 429 | |
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| 430 | G4String daughterDelta; |
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| 431 | G4String daughterPi; |
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| 432 | G4double r; |
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| 433 | |
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| 434 | // ------------ Delta pi+/- ------------ |
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| 435 | // determine daughters |
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| 436 | if (iIso3 == +1) { |
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| 437 | daughterDelta = "delta0"; |
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| 438 | if (!fAnti) { |
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| 439 | daughterPi = "pi+"; |
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| 440 | } else { |
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| 441 | daughterPi = "pi-"; |
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| 442 | } |
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| 443 | r = br/6.0; |
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| 444 | } else { |
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| 445 | daughterDelta = "delta+"; |
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| 446 | if (!fAnti) { |
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| 447 | daughterPi = "pi-"; |
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| 448 | } else { |
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| 449 | daughterPi = "pi+"; |
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| 450 | } |
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| 451 | r = br/6.0; |
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| 452 | } |
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| 453 | if (fAnti) daughterDelta = "anti_" + daughterDelta; |
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| 454 | // create decay channel [parent BR #daughters] |
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| 455 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2, |
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| 456 | daughterDelta,daughterPi); |
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| 457 | // add decay table |
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| 458 | decayTable->Insert(mode); |
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| 459 | |
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| 460 | // ------------ Delta pi+/- ------------ |
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| 461 | // determine daughters |
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| 462 | if (iIso3 == +1) { |
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| 463 | daughterDelta = "delta++"; |
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| 464 | if (!fAnti) { |
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| 465 | daughterPi = "pi-"; |
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| 466 | } else { |
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| 467 | daughterPi = "pi+"; |
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| 468 | } |
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| 469 | r = br/2.0; |
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| 470 | } else { |
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| 471 | daughterDelta = "delta-"; |
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| 472 | if (!fAnti) { |
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| 473 | daughterPi = "pi+"; |
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| 474 | } else { |
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| 475 | daughterPi = "pi-"; |
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| 476 | } |
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| 477 | r = br/2.0; |
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| 478 | } |
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| 479 | if (fAnti) daughterDelta = "anti_" + daughterDelta; |
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| 480 | // create decay channel [parent BR #daughters] |
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| 481 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2, |
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| 482 | daughterDelta,daughterPi); |
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| 483 | // add decay table |
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| 484 | decayTable->Insert(mode); |
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| 485 | |
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| 486 | // ------------ Delta pi0 ------------ |
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| 487 | // determine daughters |
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| 488 | if (iIso3 == +1) { |
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| 489 | daughterDelta = "delta+"; |
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| 490 | daughterPi = "pi0"; |
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| 491 | r = br/3.0; |
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| 492 | } else { |
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| 493 | daughterDelta = "delta0"; |
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| 494 | daughterPi = "pi0"; |
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| 495 | r = br/3.0; |
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| 496 | } |
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| 497 | if (fAnti) daughterDelta = "anti_" + daughterDelta; |
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| 498 | // create decay channel [parent BR #daughters] |
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| 499 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2, |
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| 500 | daughterDelta,daughterPi); |
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| 501 | // add decay table |
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| 502 | decayTable->Insert(mode); |
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| 503 | |
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| 504 | |
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| 505 | return decayTable; |
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| 506 | } |
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| 507 | |
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| 508 | G4DecayTable* G4ExcitedNucleonConstructor::AddLambdaKMode( |
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| 509 | G4DecayTable* decayTable, const G4String& nameParent, |
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| 510 | G4double br, G4int iIso3, G4bool fAnti) |
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| 511 | { |
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| 512 | G4VDecayChannel* mode; |
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| 513 | |
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| 514 | G4String lambda = "lambda"; |
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| 515 | G4String daughterK; |
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| 516 | |
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| 517 | // ------------ N pi0 ------------ |
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| 518 | // determine daughters |
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| 519 | if (iIso3 == +1) { |
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| 520 | if (!fAnti) { |
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| 521 | daughterK = "kaon+"; |
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| 522 | } else { |
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| 523 | daughterK = "kaon-"; |
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| 524 | } |
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| 525 | } else { |
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| 526 | if (!fAnti) { |
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| 527 | daughterK = "kaon0"; |
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| 528 | } else { |
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| 529 | daughterK = "anti_kaon0"; |
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| 530 | } |
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| 531 | } |
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| 532 | if (fAnti) lambda = "anti_" + lambda; |
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| 533 | // create decay channel [parent BR #daughters] |
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| 534 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2, |
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| 535 | lambda, daughterK); |
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| 536 | // add decay table |
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| 537 | decayTable->Insert(mode); |
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| 538 | |
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| 539 | return decayTable; |
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| 540 | } |
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| 541 | |
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| 542 | // PDG2005 |
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| 543 | // N(2090) is renamed to N(2080) |
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| 544 | // but keep unchanged temporalily Apr 06 |
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| 545 | |
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| 546 | const char* G4ExcitedNucleonConstructor::name[] = { |
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| 547 | "N(1440)", "N(1520)", "N(1535)", "N(1650)", "N(1675)", |
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| 548 | "N(1680)", "N(1700)", "N(1710)", "N(1720)", "N(1900)", |
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| 549 | "N(1990)", "N(2090)", "N(2190)", "N(2220)", "N(2250)" |
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| 550 | }; |
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| 551 | |
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| 552 | const G4double G4ExcitedNucleonConstructor::mass[] = { |
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| 553 | 1.440*GeV, 1.520*GeV, 1.535*GeV, 1.655*GeV, 1.675*GeV, |
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| 554 | 1.685*GeV, 1.700*GeV, 1.710*GeV, 1.720*GeV, 1.900*GeV, |
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| 555 | 1.950*GeV, 2.080*GeV, 2.190*GeV, 2.250*GeV, 2.275*GeV |
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| 556 | }; |
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| 557 | |
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| 558 | const G4double G4ExcitedNucleonConstructor::width[] = { |
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| 559 | 300.0*MeV, 115.0*MeV, 150.0*MeV, 165.0*MeV, 150.0*MeV, |
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| 560 | 130.0*MeV, 100.0*MeV, 100.0*MeV, 200.0*MeV, 500.0*MeV, |
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| 561 | 555.0*MeV, 350.0*MeV, 500.0*MeV, 400.0*MeV, 500.0*MeV |
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| 562 | }; |
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| 563 | |
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| 564 | const G4int G4ExcitedNucleonConstructor::iSpin[] = { |
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| 565 | 1, 3, 1, 1, 5, |
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| 566 | 5, 3, 1, 3, 3, |
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| 567 | 7, 3, 7, 9, 9 |
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| 568 | }; |
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| 569 | |
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| 570 | const G4int G4ExcitedNucleonConstructor::iParity[] = { |
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| 571 | +1, -1, -1, -1, -1, |
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| 572 | +1, -1, +1, +1, +1, |
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| 573 | +1, -1, +1, -1, -1 |
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| 574 | }; |
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| 575 | |
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| 576 | const G4int G4ExcitedNucleonConstructor::encodingOffset[] = { |
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| 577 | 10000, 0, 20000, 30000, 0, |
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| 578 | 10000, 20000, 40000, 30000, 40000, |
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| 579 | 10000, 50000, 0, 0, 10000 |
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| 580 | }; |
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| 581 | |
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| 582 | const G4double G4ExcitedNucleonConstructor::bRatio[ G4ExcitedNucleonConstructor::NStates ][ G4ExcitedNucleonConstructor::NumberOfDecayModes] = |
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| 583 | { |
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| 584 | { 0.0, 0.70, 0.0, 0.0, 0.0, 0.05, 0.25, 0.0, 0.0}, |
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| 585 | { 0.0, 0.60, 0.0, 0.0, 0.0, 0.15, 0.25, 0.0, 0.0}, |
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| 586 | {0.001, 0.55, 0.35, 0.0, 0.0, 0.05, 0.00, 0.05, 0.0}, |
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| 587 | { 0.0, 0.65, 0.05, 0.0, 0.0, 0.05, 0.10, 0.05, 0.10}, |
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| 588 | { 0.0, 0.45, 0.0, 0.0, 0.0, 0.00, 0.55, 0.0, 0.0}, |
---|
| 589 | { 0.0, 0.65, 0.0, 0.0, 0.0, 0.20, 0.15, 0.0, 0.0}, |
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| 590 | { 0.0, 0.10, 0.05, 0.0, 0.05, 0.45, 0.35, 0.0, 0.0}, |
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| 591 | { 0.0, 0.15, 0.20, 0.0, 0.05, 0.20, 0.20, 0.10, 0.10}, |
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| 592 | { 0.0, 0.15, 0.00, 0.0, 0.25, 0.45, 0.10, 0.00, 0.05}, |
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| 593 | { 0.0, 0.35, 0.0, 0.55, 0.05, 0.00, 0.05, 0.0, 0.0}, |
---|
| 594 | { 0.0, 0.05, 0.0, 0.0, 0.15, 0.25, 0.30, 0.15, 0.10}, |
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| 595 | { 0.0, 0.60, 0.05, 0.0, 0.25, 0.05, 0.05, 0.0, 0.0}, |
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| 596 | { 0.0, 0.35, 0.0, 0.00, 0.30, 0.15, 0.15, 0.05, 0.0}, |
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| 597 | { 0.0, 0.35, 0.0, 0.0, 0.25, 0.20, 0.20, 0.0, 0.0}, |
---|
| 598 | { 0.0, 0.30, 0.0, 0.00, 0.25, 0.20, 0.20, 0.05, 0.0} |
---|
| 599 | }; |
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| 600 | |
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| 601 | |
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| 602 | |
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| 603 | |
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| 604 | |
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| 605 | |
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| 606 | |
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| 607 | |
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| 608 | |
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| 609 | |
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| 610 | |
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| 611 | |
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| 612 | |
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| 613 | |
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| 614 | |
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| 615 | |
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