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1 // 2 // ******************************************************************** 3 // * License and Disclaimer * 4 // * * 5 // * The Geant4 software is copyright of the Copyright Holders of * 6 // * the Geant4 Collaboration. It is provided under the terms and * 7 // * conditions of the Geant4 Software License, included in the file * 8 // * LICENSE and available at http://cern.ch/geant4/license . These * 9 // * include a list of copyright holders. * 10 // * * 11 // * Neither the authors of this software system, nor their employing * 12 // * institutes,nor the agencies providing financial support for this * 13 // * work make any representation or warranty, express or implied, * 14 // * regarding this software system or assume any liability for its * 15 // * use. Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitation of liability. * 17 // * * 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************************************** 25 // 26 // INCL++ intra-nuclear cascade model 27 // Alain Boudard, CEA-Saclay, France 28 // Joseph Cugnon, University of Liege, Belgium 29 // Jean-Christophe David, CEA-Saclay, France 30 // Pekka Kaitaniemi, CEA-Saclay, France, and Helsinki Institute of Physics, Finland 31 // Sylvie Leray, CEA-Saclay, France 32 // Davide Mancusi, CEA-Saclay, France 33 // 34 #define INCLXX_IN_GEANT4_MODE 1 35 36 #include "globals.hh" 37 38 #include "G4INCLNpiToSKpiChannel.hh" 39 #include "G4INCLKinematicsUtils.hh" 40 #include "G4INCLBinaryCollisionAvatar.hh" 41 #include "G4INCLRandom.hh" 42 #include "G4INCLGlobals.hh" 43 #include "G4INCLLogger.hh" 44 #include <algorithm> 45 #include "G4INCLPhaseSpaceGenerator.hh" 46 47 namespace G4INCL { 48 49 const G4double NpiToSKpiChannel::angularSlope = 6.; // What is the exact effect? Sould be check 50 51 NpiToSKpiChannel::NpiToSKpiChannel(Particle *p1, Particle *p2) 52 : particle1(p1), particle2(p2) 53 {} 54 55 NpiToSKpiChannel::~NpiToSKpiChannel(){} 56 57 void NpiToSKpiChannel::fillFinalState(FinalState *fs) { 58 59 // p pi+ -> S+ pi+ K0 (5/4) 60 // p pi+ -> S+ pi0 K+ (3/4) 61 // p pi+ -> S0 pi+ K+ (1/4) 62 // 63 // p pi0 -> S+ pi0 K0 (1/2) 64 // p pi0 -> S+ pi- K+ (1/2) 65 // p pi0 -> S0 pi+ K0 (3/4) 66 // p pi0 -> S0 pi0 K+ (3/8) 67 // p pi0 -> S- pi+ K+ (1/2) 68 // 69 // p pi- -> S+ pi- K0 (3/8) 70 // p pi- -> S0 pi0 K0 (5/8) 71 // p pi- -> S0 pi- K+ (5/8) 72 // p pi- -> S- pi+ K0 (1) 73 // p pi- -> S- pi0 K+ (3/8) 74 75 Particle *nucleon; 76 Particle *pion; 77 78 79 if(particle1->isNucleon()){ 80 nucleon = particle1; 81 pion = particle2; 82 } 83 else{ 84 nucleon = particle2; 85 pion = particle1; 86 } 87 88 const G4double sqrtS = KinematicsUtils::totalEnergyInCM(nucleon, pion); 89 90 const G4int iso = ParticleTable::getIsospin(nucleon->getType()) + ParticleTable::getIsospin(pion->getType()); 91 G4double rdm = Random::shoot(); 92 93 ParticleType KaonType; 94 95 if(iso == 3 || iso == -3){ 96 if(rdm*9. < 5.){ 97 KaonType = ParticleTable::getKaonType(-iso/3); 98 nucleon->setType(ParticleTable::getSigmaType(iso/3*2)); 99 } 100 else if(rdm*9. < 8.){ 101 KaonType = ParticleTable::getKaonType(iso/3); 102 pion->setType(PiZero); 103 nucleon->setType(ParticleTable::getSigmaType(iso/3*2)); 104 } 105 else{ 106 KaonType = ParticleTable::getKaonType(iso/3); 107 nucleon->setType(SigmaZero); 108 } 109 } 110 else if(pion->getType() == PiZero){ 111 if(rdm*21. < 4.){ 112 KaonType = ParticleTable::getKaonType(-iso); 113 nucleon->setType(ParticleTable::getSigmaType(iso*2)); 114 } 115 else if(rdm*21. < 8.){ 116 KaonType = ParticleTable::getKaonType(iso); 117 pion->setType(ParticleTable::getPionType(-2*iso)); 118 nucleon->setType(ParticleTable::getSigmaType(iso*2)); 119 } 120 else if(rdm*21. < 14.){ 121 KaonType = ParticleTable::getKaonType(-iso); 122 pion->setType(ParticleTable::getPionType(2*iso)); 123 nucleon->setType(SigmaZero); 124 } 125 else if(rdm*21. < 17.){ 126 KaonType = ParticleTable::getKaonType(iso); 127 nucleon->setType(SigmaZero); 128 } 129 else{ 130 KaonType = ParticleTable::getKaonType(iso); 131 pion->setType(ParticleTable::getPionType(2*iso)); 132 nucleon->setType(ParticleTable::getSigmaType(-iso*2)); 133 } 134 } 135 else{ 136 if(rdm*24. < 3.){ 137 KaonType = ParticleTable::getKaonType(iso); 138 nucleon->setType(ParticleTable::getSigmaType(-iso*2)); 139 } 140 else if(rdm*24. < 8.){ 141 KaonType = ParticleTable::getKaonType(iso); 142 pion->setType(PiZero); 143 nucleon->setType(SigmaZero); 144 } 145 else if(rdm*24. < 13.){ 146 KaonType = ParticleTable::getKaonType(-iso); 147 nucleon->setType(SigmaZero); 148 } 149 else if(rdm*24. < 21.){ 150 KaonType = ParticleTable::getKaonType(iso); 151 pion->setType(ParticleTable::getPionType(-2*iso)); 152 nucleon->setType(ParticleTable::getSigmaType(iso*2)); 153 } 154 else{ 155 KaonType = ParticleTable::getKaonType(-iso); 156 pion->setType(PiZero); 157 nucleon->setType(ParticleTable::getSigmaType(iso*2)); 158 } 159 } 160 161 #ifdef INCLXX_IN_GEANT4_MODE 162 // Erase the parent resonance information of the nucleon and pion 163 nucleon->setParentResonancePDGCode(0); 164 nucleon->setParentResonanceID(0); 165 pion->setParentResonancePDGCode(0); 166 pion->setParentResonanceID(0); 167 #endif 168 169 ParticleList list; 170 list.push_back(nucleon); 171 list.push_back(pion); 172 const ThreeVector &rcol = nucleon->getPosition(); 173 const ThreeVector zero; 174 Particle *kaon = new Particle(KaonType,zero,rcol); 175 list.push_back(kaon); 176 177 PhaseSpaceGenerator::generateBiased(sqrtS, list, 0, angularSlope); 178 179 INCL_DEBUG("NpiToSKpi " << (kaon->getMomentum().theta()) * 180. / G4INCL::Math::pi << '\n'); 180 181 fs->addModifiedParticle(nucleon); 182 fs->addModifiedParticle(pion); 183 fs->addCreatedParticle(kaon); 184 185 } 186 } 187