| 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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| 28 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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| 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);
|
|---|
| 420 |
|
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| 421 | return decayTable;
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| 422 | }
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|---|
| 423 |
|
|---|
| 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 | {
|
|---|
| 428 | G4VDecayChannel* mode;
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|---|
| 429 |
|
|---|
| 430 | G4String daughterDelta;
|
|---|
| 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-";
|
|---|
| 442 | }
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|---|
| 443 | r = br/6.0;
|
|---|
| 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 {
|
|---|
| 449 | daughterPi = "pi+";
|
|---|
| 450 | }
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|---|
| 451 | r = br/6.0;
|
|---|
| 452 | }
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|---|
| 453 | if (fAnti) daughterDelta = "anti_" + daughterDelta;
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|---|
| 454 | // create decay channel [parent BR #daughters]
|
|---|
| 455 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
|
|---|
| 456 | daughterDelta,daughterPi);
|
|---|
| 457 | // add decay table
|
|---|
| 458 | decayTable->Insert(mode);
|
|---|
| 459 |
|
|---|
| 460 | // ------------ Delta pi+/- ------------
|
|---|
| 461 | // determine daughters
|
|---|
| 462 | if (iIso3 == +1) {
|
|---|
| 463 | daughterDelta = "delta++";
|
|---|
| 464 | if (!fAnti) {
|
|---|
| 465 | daughterPi = "pi-";
|
|---|
| 466 | } else {
|
|---|
| 467 | daughterPi = "pi+";
|
|---|
| 468 | }
|
|---|
| 469 | r = br/2.0;
|
|---|
| 470 | } else {
|
|---|
| 471 | daughterDelta = "delta-";
|
|---|
| 472 | if (!fAnti) {
|
|---|
| 473 | daughterPi = "pi+";
|
|---|
| 474 | } else {
|
|---|
| 475 | daughterPi = "pi-";
|
|---|
| 476 | }
|
|---|
| 477 | r = br/2.0;
|
|---|
| 478 | }
|
|---|
| 479 | if (fAnti) daughterDelta = "anti_" + daughterDelta;
|
|---|
| 480 | // create decay channel [parent BR #daughters]
|
|---|
| 481 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
|
|---|
| 482 | daughterDelta,daughterPi);
|
|---|
| 483 | // add decay table
|
|---|
| 484 | decayTable->Insert(mode);
|
|---|
| 485 |
|
|---|
| 486 | // ------------ Delta pi0 ------------
|
|---|
| 487 | // determine daughters
|
|---|
| 488 | if (iIso3 == +1) {
|
|---|
| 489 | daughterDelta = "delta+";
|
|---|
| 490 | daughterPi = "pi0";
|
|---|
| 491 | r = br/3.0;
|
|---|
| 492 | } else {
|
|---|
| 493 | daughterDelta = "delta0";
|
|---|
| 494 | daughterPi = "pi0";
|
|---|
| 495 | r = br/3.0;
|
|---|
| 496 | }
|
|---|
| 497 | if (fAnti) daughterDelta = "anti_" + daughterDelta;
|
|---|
| 498 | // create decay channel [parent BR #daughters]
|
|---|
| 499 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
|
|---|
| 500 | daughterDelta,daughterPi);
|
|---|
| 501 | // add decay table
|
|---|
| 502 | decayTable->Insert(mode);
|
|---|
| 503 |
|
|---|
| 504 |
|
|---|
| 505 | return decayTable;
|
|---|
| 506 | }
|
|---|
| 507 |
|
|---|
| 508 | G4DecayTable* G4ExcitedNucleonConstructor::AddLambdaKMode(
|
|---|
| 509 | G4DecayTable* decayTable, const G4String& nameParent,
|
|---|
| 510 | G4double br, G4int iIso3, G4bool fAnti)
|
|---|
| 511 | {
|
|---|
| 512 | G4VDecayChannel* mode;
|
|---|
| 513 |
|
|---|
| 514 | G4String lambda = "lambda";
|
|---|
| 515 | G4String daughterK;
|
|---|
| 516 |
|
|---|
| 517 | // ------------ N pi0 ------------
|
|---|
| 518 | // determine daughters
|
|---|
| 519 | if (iIso3 == +1) {
|
|---|
| 520 | if (!fAnti) {
|
|---|
| 521 | daughterK = "kaon+";
|
|---|
| 522 | } else {
|
|---|
| 523 | daughterK = "kaon-";
|
|---|
| 524 | }
|
|---|
| 525 | } else {
|
|---|
| 526 | if (!fAnti) {
|
|---|
| 527 | daughterK = "kaon0";
|
|---|
| 528 | } else {
|
|---|
| 529 | daughterK = "anti_kaon0";
|
|---|
| 530 | }
|
|---|
| 531 | }
|
|---|
| 532 | if (fAnti) lambda = "anti_" + lambda;
|
|---|
| 533 | // create decay channel [parent BR #daughters]
|
|---|
| 534 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2,
|
|---|
| 535 | lambda, daughterK);
|
|---|
| 536 | // add decay table
|
|---|
| 537 | decayTable->Insert(mode);
|
|---|
| 538 |
|
|---|
| 539 | return decayTable;
|
|---|
| 540 | }
|
|---|
| 541 |
|
|---|
| 542 | // PDG2005
|
|---|
| 543 | // N(2090) is renamed to N(2080)
|
|---|
| 544 | // but keep unchanged temporalily Apr 06
|
|---|
| 545 |
|
|---|
| 546 | const char* G4ExcitedNucleonConstructor::name[] = {
|
|---|
| 547 | "N(1440)", "N(1520)", "N(1535)", "N(1650)", "N(1675)",
|
|---|
| 548 | "N(1680)", "N(1700)", "N(1710)", "N(1720)", "N(1900)",
|
|---|
| 549 | "N(1990)", "N(2090)", "N(2190)", "N(2220)", "N(2250)"
|
|---|
| 550 | };
|
|---|
| 551 |
|
|---|
| 552 | const G4double G4ExcitedNucleonConstructor::mass[] = {
|
|---|
| 553 | 1.440*GeV, 1.520*GeV, 1.535*GeV, 1.655*GeV, 1.675*GeV,
|
|---|
| 554 | 1.685*GeV, 1.700*GeV, 1.710*GeV, 1.720*GeV, 1.900*GeV,
|
|---|
| 555 | 1.950*GeV, 2.080*GeV, 2.190*GeV, 2.250*GeV, 2.275*GeV
|
|---|
| 556 | };
|
|---|
| 557 |
|
|---|
| 558 | const G4double G4ExcitedNucleonConstructor::width[] = {
|
|---|
| 559 | 300.0*MeV, 115.0*MeV, 150.0*MeV, 165.0*MeV, 150.0*MeV,
|
|---|
| 560 | 130.0*MeV, 100.0*MeV, 100.0*MeV, 200.0*MeV, 500.0*MeV,
|
|---|
| 561 | 555.0*MeV, 350.0*MeV, 500.0*MeV, 400.0*MeV, 500.0*MeV
|
|---|
| 562 | };
|
|---|
| 563 |
|
|---|
| 564 | const G4int G4ExcitedNucleonConstructor::iSpin[] = {
|
|---|
| 565 | 1, 3, 1, 1, 5,
|
|---|
| 566 | 5, 3, 1, 3, 3,
|
|---|
| 567 | 7, 3, 7, 9, 9
|
|---|
| 568 | };
|
|---|
| 569 |
|
|---|
| 570 | const G4int G4ExcitedNucleonConstructor::iParity[] = {
|
|---|
| 571 | +1, -1, -1, -1, -1,
|
|---|
| 572 | +1, -1, +1, +1, +1,
|
|---|
| 573 | +1, -1, +1, -1, -1
|
|---|
| 574 | };
|
|---|
| 575 |
|
|---|
| 576 | const G4int G4ExcitedNucleonConstructor::encodingOffset[] = {
|
|---|
| 577 | 10000, 0, 20000, 30000, 0,
|
|---|
| 578 | 10000, 20000, 40000, 30000, 40000,
|
|---|
| 579 | 10000, 50000, 0, 0, 10000
|
|---|
| 580 | };
|
|---|
| 581 |
|
|---|
| 582 | const G4double G4ExcitedNucleonConstructor::bRatio[ G4ExcitedNucleonConstructor::NStates ][ G4ExcitedNucleonConstructor::NumberOfDecayModes] =
|
|---|
| 583 | {
|
|---|
| 584 | { 0.0, 0.70, 0.0, 0.0, 0.0, 0.05, 0.25, 0.0, 0.0},
|
|---|
| 585 | { 0.0, 0.60, 0.0, 0.0, 0.0, 0.15, 0.25, 0.0, 0.0},
|
|---|
| 586 | {0.001, 0.55, 0.35, 0.0, 0.0, 0.05, 0.00, 0.05, 0.0},
|
|---|
| 587 | { 0.0, 0.65, 0.05, 0.0, 0.0, 0.05, 0.10, 0.05, 0.10},
|
|---|
| 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},
|
|---|
| 590 | { 0.0, 0.10, 0.05, 0.0, 0.05, 0.45, 0.35, 0.0, 0.0},
|
|---|
| 591 | { 0.0, 0.15, 0.20, 0.0, 0.05, 0.20, 0.20, 0.10, 0.10},
|
|---|
| 592 | { 0.0, 0.15, 0.00, 0.0, 0.25, 0.45, 0.10, 0.00, 0.05},
|
|---|
| 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},
|
|---|
| 595 | { 0.0, 0.60, 0.05, 0.0, 0.25, 0.05, 0.05, 0.0, 0.0},
|
|---|
| 596 | { 0.0, 0.35, 0.0, 0.00, 0.30, 0.15, 0.15, 0.05, 0.0},
|
|---|
| 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 | };
|
|---|
| 600 |
|
|---|
| 601 |
|
|---|
| 602 |
|
|---|
| 603 |
|
|---|
| 604 |
|
|---|
| 605 |
|
|---|
| 606 |
|
|---|
| 607 |
|
|---|
| 608 |
|
|---|
| 609 |
|
|---|
| 610 |
|
|---|
| 611 |
|
|---|
| 612 |
|
|---|
| 613 |
|
|---|
| 614 |
|
|---|
| 615 |
|
|---|