| 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: G4ExcitedXiConstructor.cc,v 1.7 2006/06/29 19:27:12 gunter Exp $
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| 28 | // GEANT4 tag $Name: HEAD $
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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 | //
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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 "G4ExcitedXiConstructor.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 | G4ExcitedXiConstructor::G4ExcitedXiConstructor():
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| 49 | G4ExcitedBaryonConstructor(NStates, XiIsoSpin)
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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 | G4ExcitedXiConstructor::~G4ExcitedXiConstructor()
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| 55 | {
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| 56 | }
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| 57 |
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| 58 | G4DecayTable* G4ExcitedXiConstructor::CreateDecayTable(
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| 59 | const G4String& parentName,
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| 60 | G4int iIso3,
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| 61 | G4int iState,
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| 62 | G4bool fAnti)
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| 63 | {
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| 64 |
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| 65 | // create decay table
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| 66 | G4DecayTable* decayTable = new G4DecayTable();
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| 67 |
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| 68 | G4double br;
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| 69 | if ( (br=bRatio[iState][XiPi]) >0.0) {
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| 70 | AddXiPiMode( decayTable, parentName, br, iIso3, fAnti);
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| 71 | }
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| 72 |
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| 73 | if ( (br=bRatio[iState][XiGamma]) >0.0) {
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| 74 | AddXiGammaMode( decayTable, parentName, br, iIso3, fAnti);
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| 75 | }
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| 76 |
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| 77 | if ( (br=bRatio[iState][LambdaK]) >0.0) {
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| 78 | AddLambdaKMode( decayTable, parentName, br, iIso3, fAnti);
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| 79 | }
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| 80 |
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| 81 | if ( (br=bRatio[iState][SigmaK]) >0.0) {
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| 82 | AddSigmaKMode( decayTable, parentName, br, iIso3, fAnti);
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| 83 | }
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| 84 |
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| 85 | return decayTable;
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| 86 | }
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| 87 |
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| 88 | G4DecayTable* G4ExcitedXiConstructor::AddXiGammaMode(
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| 89 | G4DecayTable* decayTable, const G4String& nameParent,
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| 90 | G4double br, G4int iIso3, G4bool fAnti)
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| 91 | {
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| 92 | G4VDecayChannel* mode;
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| 93 | //
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| 94 | G4String daughterH;
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| 95 | if (iIso3== +1) {
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| 96 | daughterH = "xi0";
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| 97 | } else if (iIso3==-1) {
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| 98 | daughterH = "xi-";
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| 99 | }
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| 100 | if (fAnti) daughterH = "anti_" + daughterH;
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| 101 |
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| 102 | // create decay channel [parent BR #daughters]
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| 103 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2,
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| 104 | daughterH,"gamma");
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| 105 | // add decay table
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| 106 | decayTable->Insert(mode);
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| 107 |
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| 108 | return decayTable;
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| 109 | }
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| 110 |
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| 111 | G4DecayTable* G4ExcitedXiConstructor::AddLambdaKMode(
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| 112 | G4DecayTable* decayTable, const G4String& nameParent,
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| 113 | G4double br, G4int iIso3, G4bool fAnti)
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| 114 |
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| 115 |
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| 116 | {
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| 117 | G4VDecayChannel* mode;
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| 118 |
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| 119 | G4String lambda = "lambda";
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| 120 | G4String daughterK;
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| 121 | G4double r = 0.;
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| 122 |
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| 123 | // ------------ Lambda K- ------------
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| 124 | // determine daughters
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| 125 | if (iIso3 == +1) {
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| 126 | if (!fAnti) {
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| 127 | daughterK = "kaon0";
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| 128 | } else {
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| 129 | daughterK = "anti_kaon0";
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| 130 | }
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| 131 | r = br;
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| 132 | } else if (iIso3 == -1) {
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| 133 | if (!fAnti) {
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| 134 | daughterK = "kaon-";
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| 135 | } else {
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| 136 | daughterK = "kaon+";
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| 137 | }
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| 138 | r = br;
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| 139 | }
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| 140 | if (fAnti) lambda = "anti_" + lambda;
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| 141 | if (r>0.) {
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| 142 | // create decay channel [parent BR #daughters]
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| 143 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 144 | lambda,daughterK);
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| 145 | // add decay table
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| 146 | decayTable->Insert(mode);
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| 147 | }
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| 148 |
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| 149 | return decayTable;
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| 150 | }
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| 151 |
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| 152 | G4DecayTable* G4ExcitedXiConstructor::AddSigmaKMode(
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| 153 | G4DecayTable* decayTable, const G4String& nameParent,
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| 154 | G4double br, G4int iIso3, G4bool fAnti)
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| 155 | {
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| 156 | G4VDecayChannel* mode;
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| 157 |
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| 158 | G4String daughterH;
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| 159 | G4String daughterK;
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| 160 | G4double r = 0.;
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| 161 |
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| 162 | // ------------ Sigma K- ------------
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| 163 | // determine daughters
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| 164 | if (iIso3== +1) {
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| 165 | daughterH = "sigma+";
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| 166 | r= br/2.;
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| 167 | } else if (iIso3== -1) {
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| 168 | daughterH = "sigma0";
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| 169 | r = br/2.;
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| 170 | }
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| 171 | if (!fAnti) {
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| 172 | daughterK = "kaon-";
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| 173 | } else {
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| 174 | daughterK = "kaon+";
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| 175 | }
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| 176 | if (fAnti) daughterH = "anti_" + daughterH;
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| 177 | if (r>0.) {
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| 178 | // create decay channel [parent BR #daughters]
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| 179 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 180 | daughterH,daughterK);
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| 181 | // add decay table
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| 182 | decayTable->Insert(mode);
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| 183 | }
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| 184 |
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| 185 | // ------------ Sigma K0 ------------
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| 186 | // determine daughters
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| 187 | if (iIso3 == +1) {
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| 188 | daughterH = "sigma0";
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| 189 | r= br/2.;
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| 190 | } else if (iIso3 == -1) {
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| 191 | daughterH = "sigma-";
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| 192 | r = br/2.;
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| 193 | }
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| 194 | if (!fAnti) {
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| 195 | daughterK = "anti_kaon0";
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| 196 | } else {
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| 197 | daughterK = "kaon0";
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| 198 | }
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| 199 | if (fAnti) daughterH = "anti_" + daughterH;
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| 200 | if (r>0.) {
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| 201 | // create decay channel [parent BR #daughters]
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| 202 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 203 | daughterH,daughterK);
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| 204 | // add decay table
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| 205 | decayTable->Insert(mode);
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| 206 | }
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| 207 |
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| 208 | return decayTable;
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| 209 | }
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| 210 |
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| 211 | G4DecayTable* G4ExcitedXiConstructor::AddXiPiMode(
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| 212 | G4DecayTable* decayTable, const G4String& nameParent,
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| 213 | G4double br, G4int iIso3, G4bool fAnti)
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| 214 | {
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| 215 | G4VDecayChannel* mode;
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| 216 |
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| 217 | G4String daughterXi;
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| 218 | G4String daughterPi;
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| 219 | G4double r = 0.;
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| 220 |
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| 221 | // ------------ Xi pi- ------------
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| 222 | // determine daughters
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| 223 | if (iIso3== +1) {
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| 224 | r = 0.;
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| 225 | } else if (iIso3 == -1) {
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| 226 | daughterXi = "xi0";
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| 227 | r = br/2.;
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| 228 | }
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| 229 | if (!fAnti) {
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| 230 | daughterPi = "pi-";
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| 231 | } else {
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| 232 | daughterPi = "pi+";
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| 233 | }
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| 234 | if (fAnti) daughterXi = "anti_" + daughterXi;
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| 235 | if (r>0.) {
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| 236 | // create decay channel [parent BR #daughters]
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| 237 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 238 | daughterXi,daughterPi);
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| 239 | // add decay table
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| 240 | decayTable->Insert(mode);
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| 241 | }
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| 242 | // ------------ Xi Pi0 ------------
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| 243 | // determine daughters
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| 244 | if (iIso3== +1) {
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| 245 | daughterXi = "xi0";
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| 246 | r = br/2.;
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| 247 | } else if (iIso3 == -1) {
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| 248 | daughterXi = "xi-";
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| 249 | r = br/2.;
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| 250 | }
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| 251 | daughterPi = "pi0";
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| 252 | if (fAnti) daughterXi = "anti_" + daughterXi;
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| 253 | if (r>0.) {
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| 254 | // create decay channel [parent BR #daughters]
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| 255 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 256 | daughterXi,daughterPi);
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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 |
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| 261 | // ------------ XI pi + ------------
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| 262 | // determine daughters
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| 263 | if (iIso3== +1) {
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| 264 | daughterXi = "xi-";
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| 265 | r = br/2.;
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| 266 | } else if (iIso3==-1) {
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| 267 | r = 0.;
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| 268 | }
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| 269 | if (!fAnti) {
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| 270 | daughterPi = "pi+";
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| 271 | } else {
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| 272 | daughterPi = "pi-";
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| 273 | }
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| 274 | if (fAnti) daughterXi = "anti_" + daughterXi;
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| 275 | if (r>0.) {
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| 276 | // create decay channel [parent BR #daughters]
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| 277 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2,
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| 278 | daughterXi,daughterPi);
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| 279 | // add decay table
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| 280 | decayTable->Insert(mode);
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| 281 | }
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| 282 |
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| 283 | return decayTable;
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| 284 | }
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| 285 |
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| 286 |
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| 287 | const char* G4ExcitedXiConstructor::name[] = {
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| 288 | "xi(1530)", "xi(1690)", "xi(1820)", "xi(1950)", "xi(2030)"
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| 289 | };
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| 290 |
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| 291 | const G4double G4ExcitedXiConstructor::mass[] = {
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| 292 | 1.5318*GeV, 1.690*GeV, 1.823*GeV, 1.950*GeV, 2.025*GeV
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| 293 | };
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| 294 |
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| 295 | const G4double G4ExcitedXiConstructor::width[] = {
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| 296 | 9.1*MeV, 50.0*MeV, 24.0*MeV, 60.0*MeV, 20.0*MeV
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| 297 | };
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| 298 |
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| 299 | const G4int G4ExcitedXiConstructor::iSpin[] = {
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| 300 | 3, 3, 3, 3, 5
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| 301 | };
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| 302 |
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| 303 | const G4int G4ExcitedXiConstructor::iParity[] = {
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| 304 | +1, +1, -1, -1, +1
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| 305 | };
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| 306 |
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| 307 |
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| 308 | const G4int G4ExcitedXiConstructor::encodingOffset[] = {
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| 309 | 0, 20000, 10000, 30000, 10000
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| 310 | };
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| 311 |
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| 312 | const G4double G4ExcitedXiConstructor::bRatio[ G4ExcitedXiConstructor::NStates ][ G4ExcitedXiConstructor::NumberOfDecayModes] =
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| 313 | {
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| 314 | { 0.98, 0.02, 0.0, 0.0},
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| 315 | { 0.10, 0.0, 0.70, 0.20},
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| 316 | { 0.15, 0.0, 0.70, 0.15},
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| 317 | { 0.25, 0.0, 0.50, 0.25},
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| 318 | { 0.10, 0.0, 0.20, 0.70}
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| 319 | };
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| 320 |
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| 321 |
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| 322 |
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| 323 |
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| 324 |
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| 325 |
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| 326 |
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| 327 |
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| 328 |
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| 329 |
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| 330 |
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