| [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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| [921] | 27 | // $Id: G4ExcitedDeltaConstructor.cc,v 1.12 2008/09/18 08:37:27 kurasige Exp $
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| [1196] | 28 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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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 | //
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| 34 | // History: first implementation, based on object model of
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| 35 | // 10 oct 1998 H.Kurashige
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| 36 | // ---------------------------------------------------------------
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| 37 |
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| 38 |
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| 39 | #include "G4ExcitedDeltaConstructor.hh"
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| 40 |
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| 41 | #include "G4ParticleDefinition.hh"
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| 42 | #include "G4ParticleTable.hh"
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| 43 | #include "G4ShortLivedTable.hh"
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| 44 | #include "G4PhaseSpaceDecayChannel.hh"
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| 45 | #include "G4VDecayChannel.hh"
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| 46 | #include "G4DecayTable.hh"
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| 47 |
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| 48 |
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| 49 | G4ExcitedDeltaConstructor::G4ExcitedDeltaConstructor():
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| 50 | G4ExcitedBaryonConstructor(NStates, DeltaIsoSpin)
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| 51 | {
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| 52 |
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| 53 | }
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| 54 |
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| 55 | G4ExcitedDeltaConstructor::~G4ExcitedDeltaConstructor()
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| 56 | {
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| 57 | }
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| 58 |
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| 59 | G4int G4ExcitedDeltaConstructor::GetEncoding(G4int iIsoSpin3, G4int idxState)
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| 60 | {
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| 61 | G4int encoding;
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| 62 | // Delta has exceptinal encoding
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| 63 | if ((idxState==1)||(idxState==3)||(idxState==4)||(idxState==5)||(idxState==7)) {
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| 64 | encoding = GetEncodingOffset(idxState);
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| 65 | if ((iIsoSpin3==3)||(iIsoSpin3==-3)) {
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| 66 | // normal encoding
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| 67 | encoding += 1000*GetQuarkContents(0, iIsoSpin3);
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| 68 | encoding += 100*GetQuarkContents(1, iIsoSpin3);
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| 69 | encoding += 10*GetQuarkContents(2, iIsoSpin3);
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| 70 | } else if (iIsoSpin3== +1){
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| 71 | // 1st <--> 2nd quark
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| 72 | encoding += 1000*GetQuarkContents(0, iIsoSpin3);
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| 73 | encoding += 10*GetQuarkContents(1, iIsoSpin3);
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| 74 | encoding += 100*GetQuarkContents(2, iIsoSpin3);
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| 75 | } else if (iIsoSpin3== -1){
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| 76 | // 1st <--> 0th quark
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| 77 | encoding += 100*GetQuarkContents(0, iIsoSpin3);
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| 78 | encoding += 1000*GetQuarkContents(1, iIsoSpin3);
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| 79 | encoding += 10*GetQuarkContents(2, iIsoSpin3);
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| 80 | }
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| 81 | encoding += GetiSpin(idxState) +1;
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| 82 | } else {
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| 83 | encoding = G4ExcitedBaryonConstructor::GetEncoding(iIsoSpin3, idxState);
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| 84 | }
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| 85 | return encoding;
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| 86 | }
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| 87 | G4DecayTable* G4ExcitedDeltaConstructor::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][NRho]) >0.0) {
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| 106 | AddNRhoMode( decayTable, parentName, br, iIso3, fAnti);
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| 107 | }
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| 108 |
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| 109 | if ( (br=bRatio[iState][DeltaPi]) >0.0) {
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| 110 | AddDeltaPiMode( decayTable, parentName, br, iIso3, fAnti);
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| 111 | }
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| 112 |
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| 113 | if ( (br=bRatio[iState][NStarPi]) >0.0) {
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| 114 | AddNStarPiMode( decayTable, parentName, br, iIso3, fAnti);
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| 115 | }
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| 116 |
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| 117 | return decayTable;
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| 118 | }
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| 119 |
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| 120 | G4DecayTable* G4ExcitedDeltaConstructor::AddNGammaMode(
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| 121 | G4DecayTable* decayTable, const G4String& nameParent,
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| 122 | G4double br, G4int iIso3, G4bool fAnti)
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| 123 | {
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| 124 | G4VDecayChannel* mode;
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| 125 |
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| 126 | //
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| 127 | G4String daughterN;
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| 128 | if (iIso3 == +1) {
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| 129 | daughterN = "proton";
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| 130 | } else if (iIso3 == -1) {
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| 131 | daughterN = "neutron";
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| 132 | } else {
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| 133 | // can not decay into N+gamma
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| 134 | return decayTable;
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| 135 | }
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| 136 |
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| 137 | if (fAnti) daughterN = "anti_" + daughterN;
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| 138 |
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| 139 | // create decay channel [parent BR #daughters]
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| 140 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2,
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| 141 | daughterN,"gamma");
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| 142 | // add decay table
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| 143 | decayTable->Insert(mode);
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| 144 |
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| 145 | return decayTable;
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| 146 | }
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| 147 |
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| 148 | G4DecayTable* G4ExcitedDeltaConstructor::AddNPiMode(
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| 149 | G4DecayTable* decayTable, const G4String& nameParent,
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| 150 | G4double br, G4int iIso3, G4bool fAnti)
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| 151 | {
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| 152 | G4VDecayChannel* mode;
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| 153 |
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| 154 | G4String daughterN;
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| 155 | G4String daughterPi;
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| 156 | G4double r = 0.;
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| 157 |
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| 158 | // ------------ N pi0 ------------
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| 159 | // determine daughters
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| 160 | if ((iIso3 == +1)||(iIso3 == -1)) {
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| 161 | if (iIso3 == +1) {
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| 162 | daughterN = "proton";
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| 163 | daughterPi = "pi0";
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| 164 | r = br*2./3.;
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| 165 | } else if (iIso3 == -1) {
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| 166 | daughterN = "neutron";
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| 167 | daughterPi = "pi0";
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| 168 | r = br/3.;
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| 169 | }
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| 170 | if (fAnti) daughterN = "anti_" + daughterN;
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| 171 | // create decay channel [parent BR #daughters]
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| 172 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 173 | daughterN,daughterPi);
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| 174 | // add decay table
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| 175 | decayTable->Insert(mode);
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| 176 | }
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| 177 |
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| 178 | // -------------N pi +/- --------------
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| 179 | // determine daughters
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| 180 | if (iIso3 == +3) {
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| 181 | daughterN = "proton";
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| 182 | if (!fAnti) {
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| 183 | daughterPi = "pi+";
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| 184 | } else {
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| 185 | daughterPi = "pi-";
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| 186 | }
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| 187 | r = br;
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| 188 | } else if (iIso3 == +1) {
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| 189 | daughterN = "neutron";
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| 190 | if (!fAnti) {
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| 191 | daughterPi = "pi+";
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| 192 | } else {
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| 193 | daughterPi = "pi-";
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| 194 | }
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| 195 | r = br/3.;
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| 196 | } else if (iIso3 == -1) {
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| 197 | daughterN = "proton";
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| 198 | if (!fAnti) {
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| 199 | daughterPi = "pi-";
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| 200 | } else {
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| 201 | daughterPi = "pi+";
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| 202 | }
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| 203 | r = br*2./3.;
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| 204 | } else if (iIso3 == -3) {
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| 205 | daughterN = "neutron";
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| 206 | if (!fAnti) {
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| 207 | daughterPi = "pi-";
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| 208 | } else {
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| 209 | daughterPi = "pi+";
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| 210 | }
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| 211 | r = br;
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| 212 | }
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| 213 | if (fAnti) daughterN = "anti_" + daughterN;
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| 214 |
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| 215 | // create decay channel [parent BR #daughters]
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| 216 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 217 | daughterN,daughterPi);
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| 218 | // add decay table
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| 219 | decayTable->Insert(mode);
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| 220 |
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| 221 | return decayTable;
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| 222 | }
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| 223 |
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| 224 |
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| 225 | G4DecayTable* G4ExcitedDeltaConstructor::AddNRhoMode(
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| 226 | G4DecayTable* decayTable, const G4String& nameParent,
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| 227 | G4double br, G4int iIso3, G4bool fAnti)
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| 228 | {
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| 229 | G4VDecayChannel* mode;
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| 230 |
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| 231 | G4String daughterN;
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| 232 | G4String daughterRho;
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| 233 | G4double r = 0.;
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| 234 |
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| 235 | // ------------ N Rho0 ------------
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| 236 | // determine daughters
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| 237 | if ((iIso3 == +1)||(iIso3 == -1)) {
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| 238 | if (iIso3 == +1) {
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| 239 | daughterN = "proton";
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| 240 | daughterRho = "rho0";
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| 241 | r = br*2./3.;
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| 242 | } else if (iIso3 == -1) {
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| 243 | daughterN = "neutron";
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| 244 | daughterRho = "rho0";
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| 245 | r = br/3.;
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| 246 | }
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| 247 | if (fAnti) daughterN = "anti_" + daughterN;
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| 248 | // create decay channel [parent BR #daughters]
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| 249 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 250 | daughterN,daughterRho);
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| 251 | // add decay table
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| 252 | decayTable->Insert(mode);
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| 253 | }
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| 254 |
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| 255 | // -------------N Rho +/- --------------
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| 256 | // determine daughters
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| 257 | if (iIso3 == +3) {
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| 258 | daughterN = "proton";
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| 259 | if (!fAnti) {
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| 260 | daughterRho = "rho+";
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| 261 | } else {
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| 262 | daughterRho = "rho-";
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| 263 | }
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| 264 | r = br;
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| 265 | } else if (iIso3 == +1) {
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| 266 | daughterN = "neutron";
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| 267 | if (!fAnti) {
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| 268 | daughterRho = "rho+";
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| 269 | } else {
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| 270 | daughterRho = "rho-";
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| 271 | }
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| 272 | r = br/3.;
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| 273 | } else if (iIso3 == -1) {
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| 274 | daughterN = "proton";
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| 275 | if (!fAnti) {
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| 276 | daughterRho = "rho-";
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| 277 | } else {
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| 278 | daughterRho = "rho+";
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| 279 | }
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| 280 | r = br*2./3.;
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| 281 | } else if (iIso3 == -3) {
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| 282 | daughterN = "neutron";
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| 283 | if (!fAnti) {
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| 284 | daughterRho = "rho-";
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| 285 | } else {
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| 286 | daughterRho = "rho+";
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| 287 | }
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| 288 | r = br;
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| 289 | }
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| 290 | if (fAnti) daughterN = "anti_" + daughterN;
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| 291 |
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| 292 | // create decay channel [parent BR #daughters]
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| 293 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 294 | daughterN,daughterRho);
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| 295 | // add decay table
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| 296 | decayTable->Insert(mode);
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| 297 |
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| 298 | return decayTable;
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| 299 | }
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| 300 |
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| 301 | G4DecayTable* G4ExcitedDeltaConstructor::AddNStarPiMode(
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| 302 | G4DecayTable* decayTable, const G4String& nameParent,
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| 303 | G4double br, G4int iIso3, G4bool fAnti)
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| 304 | {
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| 305 | G4VDecayChannel* mode;
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| 306 |
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| 307 | G4String daughterN;
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| 308 | G4String daughterPi;
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| 309 | G4double r = 0.;
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| 310 |
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| 311 | // ------------ N pi0 ------------
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| 312 | // determine daughters
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| 313 | if ((iIso3 == +1)||(iIso3 == -1)) {
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| 314 | if (iIso3 == +1) {
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| 315 | daughterN = "N(1440)+";
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| 316 | daughterPi = "pi0";
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| 317 | r = br*2./3.;
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| 318 | } else if (iIso3 == -1) {
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| 319 | daughterN = "N(1440)0";
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| 320 | daughterPi = "pi0";
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| 321 | r = br/3.;
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| 322 | }
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| 323 | if (fAnti) daughterN = "anti_" + daughterN;
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| 324 | // create decay channel [parent BR #daughters]
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| 325 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 326 | daughterN,daughterPi);
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| 327 | // add decay table
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| 328 | decayTable->Insert(mode);
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| 329 | }
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| 330 |
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| 331 | // -------------N pi +/- --------------
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| 332 | // determine daughters
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| 333 | if (iIso3 == +3) {
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| 334 | daughterN = "N(1440)+";
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| 335 | if (!fAnti) {
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| 336 | daughterPi = "pi+";
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| 337 | } else {
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| 338 | daughterPi = "pi-";
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| 339 | }
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| 340 | r = br;
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| 341 | } else if (iIso3 == +1) {
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| 342 | daughterN = "N(1440)0";
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| 343 | if (!fAnti) {
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| 344 | daughterPi = "pi+";
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| 345 | } else {
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| 346 | daughterPi = "pi-";
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| 347 | }
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| 348 | r = br/3.;
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| 349 | } else if (iIso3 == -1) {
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| 350 | daughterN = "N(1440)+";
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| 351 | if (!fAnti) {
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| 352 | daughterPi = "pi-";
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| 353 | } else {
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| 354 | daughterPi = "pi+";
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| 355 | }
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| 356 | r = br*2./3.;
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| 357 | } else if (iIso3 == -3) {
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| 358 | daughterN = "N(1440)0";
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| 359 | if (!fAnti) {
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| 360 | daughterPi = "pi-";
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| 361 | } else {
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| 362 | daughterPi = "pi+";
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| 363 | }
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| 364 | r = br;
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| 365 | }
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| 366 | if (fAnti) daughterN = "anti_" + daughterN;
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| 367 |
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| 368 | // create decay channel [parent BR #daughters]
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| 369 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 370 | daughterN,daughterPi);
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| 371 | // add decay table
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| 372 | decayTable->Insert(mode);
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| 373 |
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| 374 | return decayTable;
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| 375 | }
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| 376 |
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| 377 | G4DecayTable* G4ExcitedDeltaConstructor::AddDeltaPiMode(
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| 378 | G4DecayTable* decayTable, const G4String& nameParent,
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| 379 | G4double br, G4int iIso3, G4bool fAnti)
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| 380 | {
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| 381 | G4VDecayChannel* mode;
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| 382 |
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| 383 | G4String daughterDelta;
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| 384 | G4String daughterPi;
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| 385 | G4double r;
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| 386 |
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| 387 | // ------------ Delta pi +------------
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| 388 | // determine daughters
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| 389 | if (iIso3 == +3) {
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| 390 | daughterDelta = "delta+";
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| 391 | r = br*0.4;
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| 392 | } else if (iIso3 == +1) {
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| 393 | daughterDelta = "delta0";
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| 394 | r = br*8./15.0;
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| 395 | } else if (iIso3 == -1) {
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| 396 | daughterDelta = "delta-";
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| 397 | r = br*6./15.;
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| 398 | } else {
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| 399 | r = 0.;
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| 400 | }
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| 401 | if (!fAnti) {
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| 402 | daughterPi = "pi+";
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| 403 | } else {
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| 404 | daughterPi = "pi-";
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| 405 | }
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| 406 | if (fAnti) daughterDelta = "anti_" + daughterDelta;
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| 407 | if (r>0.0) {
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| 408 | // create decay channel [parent BR #daughters]
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| 409 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 410 | daughterDelta,daughterPi);
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| 411 | // add decay table
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| 412 | decayTable->Insert(mode);
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| 413 | }
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| 414 |
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| 415 | // ------------ Delta pi0 ------------
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| 416 | // determine daughters
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| 417 | if (iIso3 == +3) {
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| 418 | daughterDelta = "delta++";
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| 419 | r = br*0.6;
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| 420 | } else if (iIso3 == +1) {
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| 421 | daughterDelta = "delta+";
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| 422 | r = br*1./15.0;
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| 423 | } else if (iIso3 == -1) {
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| 424 | daughterDelta = "delta0";
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| 425 | r = br*1./15.;
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| 426 | } else {
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| 427 | daughterDelta = "delta-";
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| 428 | r = br*0.6;
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| 429 | }
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| 430 | daughterPi = "pi0";
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| 431 | if (fAnti) daughterDelta = "anti_" + daughterDelta;
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| 432 |
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| 433 | // create decay channel [parent BR #daughters]
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| 434 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 435 | daughterDelta,daughterPi);
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| 436 | // add decay table
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| 437 | decayTable->Insert(mode);
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| 438 |
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| 439 | // ------------ Delta pi - -------------
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| 440 | // determine daughters
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| 441 | if (iIso3 == +3) {
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| 442 | r= 0.;
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| 443 | } else if (iIso3 == +1) {
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| 444 | daughterDelta = "delta++";
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| 445 | r = br*6./15.0;
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| 446 | } else if (iIso3 == -1) {
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| 447 | daughterDelta = "delta+";
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| 448 | r = br*8./15.;
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| 449 | } else {
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| 450 | daughterDelta = "delta0";
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| 451 | r = br*0.4;
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| 452 | }
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| 453 | if (!fAnti) {
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| 454 | daughterPi = "pi-";
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| 455 | } else {
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| 456 | daughterPi = "pi+";
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| 457 | }
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| 458 | if (fAnti) daughterDelta = "anti_" + daughterDelta;
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| 459 | if (r>0.0) {
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| 460 | // create decay channel [parent BR #daughters]
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| 461 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 462 | daughterDelta,daughterPi);
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| 463 | // add decay table
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| 464 | decayTable->Insert(mode);
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| 465 | }
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| 466 |
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| 467 | return decayTable;
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| 468 | }
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| 469 |
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| 470 | const char* G4ExcitedDeltaConstructor::name[] =
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| 471 | {
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| 472 | "delta(1600)", "delta(1620)", "delta(1700)", "delta(1900)", "delta(1905)",
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| 473 | "delta(1910)", "delta(1920)", "delta(1930)", "delta(1950)"
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| 474 | };
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| 475 |
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| 476 | const G4double G4ExcitedDeltaConstructor::mass[] =
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| 477 | {
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|---|
| 478 | 1.600*GeV, 1.630*GeV, 1.700*GeV, 1.900*GeV, 1.890*GeV,
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| 479 | 1.910*GeV, 1.920*GeV, 1.960*GeV, 1.930*GeV
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| 480 | };
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|---|
| 481 |
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| 482 | const G4double G4ExcitedDeltaConstructor::width[] = {
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|---|
| 483 | 350.0*MeV, 145.0*MeV, 300.0*MeV, 200.0*MeV, 330.0*MeV,
|
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| [921] | 484 | 250.0*MeV, 200.0*MeV, 360.0*MeV, 290.0*MeV
|
|---|
| [824] | 485 | };
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|---|
| 486 |
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| 487 | const G4int G4ExcitedDeltaConstructor::iSpin[] =
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| 488 | {
|
|---|
| 489 | 3, 1, 3, 1, 5,
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|---|
| 490 | 1, 3, 5, 7
|
|---|
| 491 | };
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|---|
| 492 |
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|---|
| 493 | const G4int G4ExcitedDeltaConstructor::iParity[] = {
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|---|
| 494 | +1, -1, -1, -1, +1,
|
|---|
| 495 | +1, +1, -1, +1
|
|---|
| 496 | };
|
|---|
| 497 |
|
|---|
| 498 | const G4int G4ExcitedDeltaConstructor::encodingOffset[] = {
|
|---|
| 499 | 30000, 0, 10000, 10000, 0,
|
|---|
| 500 | 20000, 20000, 10000, 0
|
|---|
| 501 | };
|
|---|
| 502 |
|
|---|
| 503 | const G4double G4ExcitedDeltaConstructor::bRatio[ G4ExcitedDeltaConstructor::NStates ][ G4ExcitedDeltaConstructor::NumberOfDecayModes] =
|
|---|
| 504 | {
|
|---|
| 505 | // NGamma Npi NRho DeltaPi N*Pi
|
|---|
| 506 | { 0.0, 0.15, 0.0, 0.55, 0.30 },
|
|---|
| 507 | { 0.0, 0.25, 0.0, 0.60, 0.15 },
|
|---|
| 508 | { 0.0, 0.20, 0.10, 0.55, 0.15 },
|
|---|
| 509 | { 0.0, 0.30, 0.15, 0.30, 0.25 },
|
|---|
| 510 | { 0.0, 0.20, 0.60, 0.10, 0.10 },
|
|---|
| 511 | { 0.0, 0.35, 0.40, 0.15, 0.10 },
|
|---|
| 512 | { 0.0, 0.15, 0.30, 0.30, 0.25 },
|
|---|
| 513 | { 0.0, 0.20, 0.25, 0.25, 0.30 },
|
|---|
| 514 | { 0.01, 0.44, 0.15, 0.20, 0.20 }
|
|---|
| 515 | };
|
|---|
| 516 |
|
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| 517 |
|
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| 518 |
|
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| 519 |
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| 520 |
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| 521 |
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| 522 |
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| 523 |
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| 524 |
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| 525 |
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| 526 |
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| 527 |
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| 528 |
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| 529 |
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| 530 |
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| 531 |
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