[819] | 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 | |
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| 28 | #include "globals.hh" |
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| 29 | #include "G4ios.hh" |
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| 30 | |
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| 31 | // |
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| 32 | // G4 Process: Gheisha High Energy Collision model. |
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| 33 | // This includes the high energy cascading model, the two-body-resonance model |
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| 34 | // and the low energy two-body model. Not included is the low energy stuff |
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| 35 | // like nuclear reactions, nuclear fission without any cascading and all |
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| 36 | // processes for particles at rest. |
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| 37 | // |
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| 38 | // H. Fesefeldt, RWTH-Aachen, 23-October-1996 |
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| 39 | // Last modified: 29-July-1998 |
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| 40 | // HPW, fixed bug in getting pdgencoding for nuclei |
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| 41 | // Hisaya, fixed HighEnergyCascading |
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| 42 | // Fesefeldt, fixed bug in TuningOfHighEnergyCascading, 23 June 2000 |
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| 43 | // Fesefeldt, fixed next bug in TuningOfHighEnergyCascading, 14 August 2000 |
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| 44 | // |
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| 45 | #include "G4HEInelastic.hh" |
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| 46 | #include "G4HEVector.hh" |
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| 47 | #include "G4ParticleDefinition.hh" |
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| 48 | #include "G4DynamicParticle.hh" |
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| 49 | #include "G4ParticleTable.hh" |
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| 50 | #include "G4KaonZero.hh" |
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| 51 | #include "G4AntiKaonZero.hh" |
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| 52 | #include "G4Deuteron.hh" |
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| 53 | #include "G4Triton.hh" |
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| 54 | #include "G4Alpha.hh" |
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| 55 | |
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[1347] | 56 | void G4HEInelastic::FillParticleChange(G4HEVector pv[], G4int aVecLength) |
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[819] | 57 | { |
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| 58 | theParticleChange.Clear(); |
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| 59 | for (G4int i=0; i<aVecLength; i++) |
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| 60 | { |
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| 61 | G4int pdgCode = pv[i].getCode(); |
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| 62 | G4ParticleDefinition * aDefinition=NULL; |
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| 63 | if(pdgCode == 0) |
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| 64 | { |
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| 65 | G4int bNumber = pv[i].getBaryonNumber(); |
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| 66 | if(bNumber==2) aDefinition = G4Deuteron::Deuteron(); |
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| 67 | if(bNumber==3) aDefinition = G4Triton::Triton(); |
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| 68 | if(bNumber==4) aDefinition = G4Alpha::Alpha(); |
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| 69 | } |
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| 70 | else |
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| 71 | { |
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| 72 | aDefinition = G4ParticleTable::GetParticleTable()->FindParticle(pdgCode); |
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| 73 | } |
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| 74 | G4DynamicParticle * aParticle = new G4DynamicParticle(); |
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| 75 | aParticle->SetDefinition(aDefinition); |
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| 76 | aParticle->SetMomentum(pv[i].getMomentum()*GeV); |
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| 77 | theParticleChange.AddSecondary(aParticle); |
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| 78 | } |
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| 79 | } |
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| 80 | |
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[1347] | 81 | void G4HEInelastic::SetParticles() |
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| 82 | { |
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| 83 | PionPlus.setDefinition("PionPlus"); |
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| 84 | PionZero.setDefinition("PionZero"); |
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| 85 | PionMinus.setDefinition("PionMinus"); |
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| 86 | KaonPlus.setDefinition("KaonPlus"); |
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| 87 | KaonZero.setDefinition("KaonZero"); |
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| 88 | AntiKaonZero.setDefinition("AntiKaonZero"); |
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| 89 | KaonMinus.setDefinition("KaonMinus"); |
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| 90 | KaonZeroShort.setDefinition("KaonZeroShort"); |
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| 91 | KaonZeroLong.setDefinition("KaonZeroLong"); |
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| 92 | Proton.setDefinition("Proton"); |
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| 93 | AntiProton.setDefinition("AntiProton"); |
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| 94 | Neutron.setDefinition("Neutron"); |
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| 95 | AntiNeutron.setDefinition("AntiNeutron"); |
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| 96 | Lambda.setDefinition("Lambda"); |
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| 97 | AntiLambda.setDefinition("AntiLambda"); |
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| 98 | SigmaPlus.setDefinition("SigmaPlus"); |
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| 99 | SigmaZero.setDefinition("SigmaZero"); |
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| 100 | SigmaMinus.setDefinition("SigmaMinus"); |
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| 101 | AntiSigmaPlus.setDefinition("AntiSigmaPlus"); |
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| 102 | AntiSigmaZero.setDefinition("AntiSigmaZero"); |
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| 103 | AntiSigmaMinus.setDefinition("AntiSigmaMinus"); |
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| 104 | XiZero.setDefinition("XiZero"); |
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| 105 | XiMinus.setDefinition("XiMinus"); |
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| 106 | AntiXiZero.setDefinition("AntiXiZero"); |
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| 107 | AntiXiMinus.setDefinition("AntiXiMinus"); |
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| 108 | OmegaMinus.setDefinition("OmegaMinus"); |
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| 109 | AntiOmegaMinus.setDefinition("AntiOmegaMinus"); |
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| 110 | Deuteron.setDefinition("Deuteron"); |
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| 111 | Triton.setDefinition("Triton"); |
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| 112 | Alpha.setDefinition("Alpha"); |
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| 113 | Gamma.setDefinition("Gamma"); |
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| 114 | return; |
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| 115 | } |
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[819] | 116 | |
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[1347] | 117 | G4double G4HEInelastic::Amin(G4double a, G4double b) |
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| 118 | { |
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| 119 | G4double c = a; |
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| 120 | if(b < a) c = b; |
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| 121 | return c; |
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| 122 | } |
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| 123 | |
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| 124 | G4double G4HEInelastic::Amax(G4double a, G4double b) |
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| 125 | { |
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| 126 | G4double c = a; |
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| 127 | if(b > a) c = b; |
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| 128 | return c; |
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| 129 | } |
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| 130 | |
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[819] | 131 | G4int |
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| 132 | G4HEInelastic::Imin(G4int a, G4int b) |
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| 133 | { |
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| 134 | G4int c = a; |
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| 135 | if(b < a) c = b; |
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| 136 | return c; |
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| 137 | } |
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| 138 | G4int |
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| 139 | G4HEInelastic::Imax(G4int a, G4int b) |
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| 140 | { |
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| 141 | G4int c = a; |
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| 142 | if(b > a) c = b; |
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| 143 | return c; |
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| 144 | } |
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| 145 | |
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| 146 | |
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| 147 | G4double |
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| 148 | G4HEInelastic::NuclearInelasticity(G4double incidentKineticEnergy, |
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| 149 | G4double atomicWeight, |
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| 150 | G4double /* atomicNumber*/) |
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| 151 | { |
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| 152 | G4double expu = std::log(MAXFLOAT); |
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| 153 | G4double expl = -expu; |
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| 154 | G4double ala = std::log(atomicWeight); |
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| 155 | G4double ale = std::log(incidentKineticEnergy); |
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| 156 | G4double sig1 = 0.5; |
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| 157 | G4double sig2 = 0.5; |
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| 158 | G4double em = Amin(0.239 + 0.0408*ala*ala, 1.); |
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| 159 | G4double cinem = Amin(0.0019*std::pow(ala,3.), 0.15); |
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| 160 | G4double sig = (ale > em) ? sig2 : sig1; |
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| 161 | G4double corr = Amin(Amax(-std::pow(ale-em,2.)/(2.*sig*sig),expl), expu); |
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| 162 | G4double dum1 = -(incidentKineticEnergy)*cinem; |
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| 163 | G4double dum2 = std::abs(dum1); |
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| 164 | G4double dum3 = std::exp(corr); |
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| 165 | G4double cinema = 0.; |
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| 166 | if (dum2 >= 1.) cinema = dum1*dum3; |
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| 167 | else if (dum3 > 1.e-10) cinema = dum1*dum3; |
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| 168 | cinema = - Amax(-incidentKineticEnergy, cinema); |
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| 169 | if(verboseLevel > 1) { |
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| 170 | G4cout << " NuclearInelasticity: " << ala << " " << ale << " " |
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| 171 | << em << " " << corr << " " << dum1 << " " << dum2 << " " |
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| 172 | << dum3 << " " << cinema << G4endl; |
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| 173 | } |
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| 174 | return cinema; |
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| 175 | } |
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| 176 | |
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| 177 | G4double |
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| 178 | G4HEInelastic::NuclearExcitation(G4double incidentKineticEnergy, |
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| 179 | G4double atomicWeight, |
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| 180 | G4double atomicNumber, |
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| 181 | G4double& excitationEnergyGPN, |
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| 182 | G4double& excitationEnergyDTA) |
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| 183 | { |
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| 184 | G4double neutronMass = Neutron.getMass(); |
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| 185 | G4double electronMass = 0.000511; |
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| 186 | G4double exnu = 0.; |
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| 187 | excitationEnergyGPN = 0.; |
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| 188 | excitationEnergyDTA = 0.; |
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| 189 | |
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| 190 | if (atomicWeight > (neutronMass + 2.*electronMass)) |
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| 191 | { |
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| 192 | G4int magic = ((G4int)(atomicNumber+0.1) == 82) ? 1 : 0; |
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| 193 | G4double ekin = Amin(Amax(incidentKineticEnergy, 0.1), 4.); |
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| 194 | G4double cfa = Amax(0.35 +((0.35 - 0.05)/2.3)*std::log(ekin), 0.15); |
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| 195 | exnu = 7.716*cfa*std::exp(-cfa); |
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| 196 | G4double atno = Amin(atomicWeight, 120.); |
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| 197 | cfa = ((atno - 1.)/120.) * std::exp(-(atno-1.)/120.); |
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| 198 | exnu = exnu * cfa; |
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| 199 | G4double fpdiv = Amax(1.-0.25*ekin*ekin, 0.5); |
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| 200 | G4double gfa = 2.*((atomicWeight-1.)/70.) |
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| 201 | * std::exp(-(atomicWeight-1.)/70.); |
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| 202 | |
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| 203 | excitationEnergyGPN = exnu * fpdiv; |
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| 204 | excitationEnergyDTA = exnu - excitationEnergyGPN; |
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| 205 | |
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| 206 | G4double ran1 = 0., ran2 = 0.; |
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| 207 | if (!magic) |
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| 208 | { ran1 = normal(); |
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| 209 | ran2 = normal(); |
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| 210 | } |
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| 211 | excitationEnergyGPN = Amax(excitationEnergyGPN*(1.+ran1*gfa),0.); |
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| 212 | excitationEnergyDTA = Amax(excitationEnergyDTA*(1.+ran2*gfa),0.); |
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| 213 | exnu = excitationEnergyGPN + excitationEnergyDTA; |
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| 214 | if(verboseLevel > 1) { |
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| 215 | G4cout << " NuclearExcitation: " << magic << " " << ekin |
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| 216 | << " " << cfa << " " << atno << " " << fpdiv << " " |
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| 217 | << gfa << " " << excitationEnergyGPN |
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| 218 | << " " << excitationEnergyDTA << G4endl; |
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| 219 | } |
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| 220 | |
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| 221 | while (exnu >= incidentKineticEnergy) |
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| 222 | { |
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| 223 | excitationEnergyGPN *= (1. - 0.5*normal()); |
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| 224 | excitationEnergyDTA *= (1. - 0.5*normal()); |
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| 225 | exnu = excitationEnergyGPN + excitationEnergyDTA; |
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| 226 | } |
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| 227 | } |
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| 228 | return exnu; |
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| 229 | } |
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| 230 | |
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| 231 | G4double |
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| 232 | G4HEInelastic::pmltpc(G4int np, G4int nm, G4int nz, G4int n, |
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| 233 | G4double b, G4double c) |
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| 234 | { |
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| 235 | G4double expxu = std::log(MAXFLOAT); |
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| 236 | G4double expxl = -expxu; |
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| 237 | G4int i; |
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| 238 | G4double npf = 0.0, nmf = 0.0, nzf = 0.0; |
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| 239 | for(i=2;i<=np;i++) npf += std::log((G4double)i); |
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| 240 | for(i=2;i<=nm;i++) nmf += std::log((G4double)i); |
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| 241 | for(i=2;i<=nz;i++) nzf += std::log((G4double)i); |
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| 242 | G4double r = Amin(expxu,Amax(expxl,-(np-nm+nz+b)*(np-nm+nz+b)/(2*c*c*n*n)-npf-nmf-nzf)); |
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| 243 | return std::exp(r); |
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| 244 | } |
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| 245 | |
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[962] | 246 | |
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[819] | 247 | G4int G4HEInelastic::Factorial(G4int n) |
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[962] | 248 | { |
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| 249 | G4int result = 1; |
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| 250 | if (n < 0) G4Exception("G4HEInelastic::Factorial()", "601", |
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| 251 | FatalException, "Negative factorial argument"); |
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| 252 | while (n > 1) result *= n--; |
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| 253 | return result; |
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| 254 | } |
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[819] | 255 | |
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[962] | 256 | |
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[819] | 257 | G4double G4HEInelastic::normal() |
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| 258 | { |
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| 259 | G4double ran = -6.0; |
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| 260 | for(G4int i=0; i<12; i++) ran += G4UniformRand(); |
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| 261 | return ran; |
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| 262 | } |
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| 263 | |
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| 264 | G4int G4HEInelastic::Poisson( G4double x ) |
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| 265 | { |
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| 266 | G4int i, iran = 0; |
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| 267 | G4double ran; |
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| 268 | if ( x > 9.9 ) |
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| 269 | { |
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| 270 | iran = G4int( Amax( 0.0, x + normal() * std::sqrt( x ) ) ); |
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| 271 | } |
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| 272 | else |
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| 273 | { |
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| 274 | G4int mm = G4int( 5.0 * x ); |
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| 275 | if ( mm <= 0 ) |
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| 276 | { |
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| 277 | G4double p1 = x * std::exp( -x ); |
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| 278 | G4double p2 = x * p1/2.; |
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| 279 | G4double p3 = x * p2/3.; |
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| 280 | ran = G4UniformRand(); |
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| 281 | if ( ran < p3 ) iran = 3; |
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| 282 | else if ( ran < p2 ) iran = 2; |
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| 283 | else if ( ran < p1 ) iran = 1; |
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| 284 | } |
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| 285 | else |
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| 286 | { G4double r = std::exp( -x ); |
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| 287 | ran = G4UniformRand(); |
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| 288 | if (ran > r) |
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| 289 | { |
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| 290 | G4double rrr; |
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| 291 | G4double rr = r; |
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| 292 | for (i=1; i <= mm; i++) |
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| 293 | { |
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| 294 | iran++; |
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| 295 | if ( i > 5 ) rrr = std::exp(i*std::log(x)-(i+0.5)*std::log((G4double)i)+i-0.9189385); |
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| 296 | else rrr = std::pow(x,i)*Factorial(i); |
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| 297 | rr += r * rrr; |
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| 298 | if (ran <= rr) break; |
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| 299 | } |
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| 300 | } |
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| 301 | } |
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| 302 | } |
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| 303 | return iran; |
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| 304 | } |
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| 305 | G4double |
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| 306 | G4HEInelastic::GammaRand( G4double avalue ) |
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| 307 | { |
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| 308 | G4double ga = avalue -1.; |
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| 309 | G4double la = std::sqrt(2.*avalue - 1.); |
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| 310 | G4double ep = 1.570796327 + std::atan(ga/la); |
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| 311 | G4double ro = 1.570796327 - ep; |
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| 312 | G4double y = 1.; |
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| 313 | G4double xtrial; |
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| 314 | repeat: |
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| 315 | xtrial = ga + la * std::tan(ep*G4UniformRand() + ro); |
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| 316 | if(xtrial == 0.) goto repeat; |
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| 317 | y = std::log(1.+sqr((xtrial-ga)/la))+ga*std::log(xtrial/ga)-xtrial+ga; |
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| 318 | if(std::log(G4UniformRand()) > y) goto repeat; |
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| 319 | return xtrial; |
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| 320 | } |
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| 321 | G4double |
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| 322 | G4HEInelastic::Erlang( G4int mvalue ) |
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| 323 | { |
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| 324 | G4double ran = G4UniformRand(); |
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| 325 | G4double xtrial = 0.62666*std::log((1.+ran)/(1.-ran)); |
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| 326 | if(G4UniformRand()<0.5) xtrial = -xtrial; |
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| 327 | return mvalue+xtrial*std::sqrt(G4double(mvalue)); |
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| 328 | } |
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| 329 | |
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| 330 | void |
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| 331 | G4HEInelastic::StrangeParticlePairProduction( |
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| 332 | const G4double availableEnergy, |
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| 333 | const G4double centerOfMassEnergy, |
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| 334 | G4HEVector pv[], |
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| 335 | G4int &vecLen, |
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[1347] | 336 | const G4HEVector& incidentParticle, |
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| 337 | const G4HEVector& targetParticle) |
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[819] | 338 | |
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| 339 | // Choose charge combinations K+ K-, K+ K0, K0 K0, K0 K-, |
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| 340 | // K+ Y0, K0 Y+, K0 Y- |
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| 341 | // For antibaryon induced reactions half of the cross sections KB YB |
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| 342 | // pairs are produced. Charge is not conserved, no experimental data |
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| 343 | // available for exclusive reactions, therefore some average behavior |
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| 344 | // assumed. The ratio L/SIGMA is taken as 3:1 (from experimental low |
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| 345 | // energy data) |
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| 346 | |
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| 347 | { |
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| 348 | static G4double avrs[] = {3.,4.,5.,6.,7.,8.,9.,10.,20.,30.,40.,50.}; |
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| 349 | static G4double avkkb[] = {0.0015,0.0050,0.0120,0.0285,0.0525,0.0750,0.0975, |
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| 350 | 0.1230,0.2800,0.3980,0.4950,0.5730}; |
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| 351 | static G4double kkb[] = {0.2500,0.3750,0.5000,0.5625,0.6250,0.6875,0.7500, |
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| 352 | 0.8750,1.0000}; |
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| 353 | static G4double ky[] = {0.2000,0.3000,0.4000,0.5500,0.6250,0.7000,0.8000, |
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| 354 | 0.8500,0.9000,0.9500,0.9750,1.0000}; |
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| 355 | static G4int ipakkb[] = {10,13,10,11,10,12,11,11,11,12,12,11,12,12, |
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| 356 | 11,13,12,13}; |
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| 357 | static G4int ipaky[] = {18,10,18,11,18,12,20,10,20,11,20,12,21,10, |
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| 358 | 21,11,21,12,22,10,22,11,22,12}; |
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| 359 | static G4int ipakyb[] = {19,13,19,12,19,11,23,13,23,12,23,11,24,13, |
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| 360 | 24,12,24,11,25,13,25,12,25,11}; |
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| 361 | static G4double avky[] = {0.0050,0.0300,0.0640,0.0950,0.1150,0.1300,0.1450, |
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| 362 | 0.1550,0.2000,0.2050,0.2100,0.2120}; |
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| 363 | static G4double avnnb[] ={0.00001,0.0001,0.0006,0.0025,0.0100,0.0200,0.0400, |
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| 364 | 0.0500,0.1200,0.1500,0.1800,0.2000}; |
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| 365 | |
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| 366 | G4int i, ibin, i3, i4; // misc. local variables |
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| 367 | G4double avk, avy, avn, ran; |
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| 368 | |
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| 369 | G4double protonMass = Proton.getMass(); |
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| 370 | G4double sigmaMinusMass = SigmaMinus.getMass(); |
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| 371 | G4int antiprotonCode = AntiProton.getCode(); |
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| 372 | G4int antineutronCode = AntiNeutron.getCode(); |
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| 373 | G4int antilambdaCode = AntiLambda.getCode(); |
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| 374 | |
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| 375 | G4double incidentMass = incidentParticle.getMass(); |
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| 376 | G4int incidentCode = incidentParticle.getCode(); |
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| 377 | |
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| 378 | G4double targetMass = targetParticle.getMass(); |
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| 379 | |
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| 380 | // protection against annihilation processes like pbar p -> pi pi. |
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| 381 | |
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| 382 | if (vecLen <= 2) return; |
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| 383 | |
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| 384 | // determine the center of mass energy bin |
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| 385 | |
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| 386 | i = 1; |
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| 387 | while ( (i<12) && (centerOfMassEnergy > avrs[i]) )i++; |
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| 388 | if ( i == 12 ) ibin = 11; |
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| 389 | else ibin = i; |
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| 390 | |
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| 391 | // the fortran code chooses a random replacement of produced kaons |
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| 392 | // but does not take into account charge conservation |
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| 393 | |
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| 394 | if( vecLen == 3 ) { // we know that vecLen > 2 |
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| 395 | i3 = 2; |
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| 396 | i4 = 3; // note that we will be adding a new |
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| 397 | } // secondary particle in this case only |
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| 398 | else |
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| 399 | { // otherwise 2 <= i3,i4 <= vecLen |
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| 400 | i4 = i3 = 2 + G4int( (vecLen-2)*G4UniformRand() ); |
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| 401 | while ( i3 == i4 ) i4 = 2 + G4int( (vecLen-2)*G4UniformRand() ); |
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| 402 | } |
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| 403 | |
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| 404 | // use linear interpolation or extrapolation by y=centerofmassEnergy*x+b |
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| 405 | |
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| 406 | avk = (std::log(avkkb[ibin])-std::log(avkkb[ibin-1]))*(centerOfMassEnergy-avrs[ibin-1]) |
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| 407 | /(avrs[ibin]-avrs[ibin-1]) + std::log(avkkb[ibin-1]); |
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| 408 | avk = std::exp(avk); |
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| 409 | |
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| 410 | avy = (std::log(avky[ibin])-std::log(avky[ibin-1]))*(centerOfMassEnergy-avrs[ibin-1]) |
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| 411 | /(avrs[ibin]-avrs[ibin-1]) + std::log(avky[ibin-1]); |
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| 412 | avy = std::exp(avy); |
---|
| 413 | |
---|
| 414 | avn = (std::log(avnnb[ibin])-std::log(avnnb[ibin-1]))*(centerOfMassEnergy-avrs[ibin-1]) |
---|
| 415 | /(avrs[ibin]-avrs[ibin-1]) + std::log(avnnb[ibin-1]); |
---|
| 416 | avn = std::exp(avn); |
---|
| 417 | |
---|
| 418 | if ( avk+avy+avn <= 0.0 ) return; |
---|
| 419 | |
---|
| 420 | if ( incidentMass < protonMass ) avy /= 2.0; |
---|
| 421 | avy += avk+avn; |
---|
| 422 | avk += avn; |
---|
| 423 | |
---|
| 424 | ran = G4UniformRand(); |
---|
| 425 | if ( ran < avn ) |
---|
| 426 | { // p pbar && n nbar production |
---|
| 427 | if ( availableEnergy < 2.0) return; |
---|
| 428 | if ( vecLen == 3 ) |
---|
| 429 | { // add a new secondary |
---|
| 430 | if ( G4UniformRand() < 0.5 ) |
---|
| 431 | { |
---|
| 432 | pv[i3] = Neutron;; |
---|
| 433 | pv[vecLen++] = AntiNeutron; |
---|
| 434 | } |
---|
| 435 | else |
---|
| 436 | { |
---|
| 437 | pv[i3] = Proton; |
---|
| 438 | pv[vecLen++] = AntiProton; |
---|
| 439 | } |
---|
| 440 | } |
---|
| 441 | else |
---|
| 442 | { // replace two secondaries |
---|
| 443 | if ( G4UniformRand() < 0.5 ) |
---|
| 444 | { |
---|
| 445 | pv[i3] = Neutron; |
---|
| 446 | pv[i4] = AntiNeutron; |
---|
| 447 | } |
---|
| 448 | else |
---|
| 449 | { |
---|
| 450 | pv[i3] = Proton; |
---|
| 451 | pv[i4] = AntiProton; |
---|
| 452 | } |
---|
| 453 | } |
---|
| 454 | } |
---|
| 455 | else if ( ran < avk ) |
---|
| 456 | { // K Kbar production |
---|
| 457 | if ( availableEnergy < 1.0) return; |
---|
| 458 | G4double ran1 = G4UniformRand(); |
---|
| 459 | i = 0; |
---|
| 460 | while( (i<9) && (ran1>kkb[i]) )i++; |
---|
| 461 | if ( i == 9 ) return; |
---|
| 462 | |
---|
| 463 | // ipakkb[] = { 10,13, 10,11, 10,12, 11, 11, 11,12, 12,11, 12,12, 11,13, 12,13 }; |
---|
| 464 | // charge K+ K- K+ K0S K+ K0L K0S K0S K0S K0L K0LK0S K0LK0L K0S K- K0LK- |
---|
| 465 | |
---|
| 466 | switch( ipakkb[i*2] ) |
---|
| 467 | { |
---|
| 468 | case 10: pv[i3] = KaonPlus; break; |
---|
| 469 | case 11: pv[i3] = KaonZeroShort;break; |
---|
| 470 | case 12: pv[i3] = KaonZeroLong; break; |
---|
| 471 | case 13: pv[i3] = KaonMinus; break; |
---|
| 472 | } |
---|
| 473 | |
---|
| 474 | if( vecLen == 2 ) |
---|
| 475 | { // add a secondary |
---|
| 476 | switch( ipakkb[i*2+1] ) |
---|
| 477 | { |
---|
| 478 | case 10: pv[vecLen++] = KaonPlus; break; |
---|
| 479 | case 11: pv[vecLen++] = KaonZeroShort;break; |
---|
| 480 | case 12: pv[vecLen++] = KaonZeroLong; break; |
---|
| 481 | case 13: pv[vecLen++] = KaonMinus; break; |
---|
| 482 | } |
---|
| 483 | } |
---|
| 484 | else |
---|
| 485 | { // replace |
---|
| 486 | switch( ipakkb[i*2+1] ) |
---|
| 487 | { |
---|
| 488 | case 10: pv[i4] = KaonPlus; break; |
---|
| 489 | case 11: pv[i4] = KaonZeroShort;break; |
---|
| 490 | case 12: pv[i4] = KaonZeroLong; break; |
---|
| 491 | case 13: pv[i4] = KaonMinus; break; |
---|
| 492 | } |
---|
| 493 | } |
---|
| 494 | } |
---|
| 495 | else if ( ran < avy ) |
---|
| 496 | { // Lambda K && Sigma K |
---|
| 497 | if( availableEnergy < 1.6) return; |
---|
| 498 | G4double ran1 = G4UniformRand(); |
---|
| 499 | i = 0; |
---|
| 500 | while( (i<12) && (ran1>ky[i]) )i++; |
---|
| 501 | if ( i == 12 ) return; |
---|
| 502 | if ( (incidentMass<protonMass) || (G4UniformRand()<0.5) ) |
---|
| 503 | { |
---|
| 504 | |
---|
| 505 | // ipaky[] = { 18,10, 18,11, 18,12, 20,10, 20,11, 20,12, |
---|
| 506 | // L0 K+ L0 K0S L0 K0L S+ K+ S+ K0S S+ K0L |
---|
| 507 | // |
---|
| 508 | // 21,10, 21,11, 21,12, 22,10, 22,11, 22,12 } |
---|
| 509 | // S0 K+ S0 K0S S0 K0L S- K+ S- K0S S- K0L |
---|
| 510 | |
---|
| 511 | switch( ipaky[i*2] ) |
---|
| 512 | { |
---|
| 513 | case 18: pv[1] = Lambda; break; |
---|
| 514 | case 20: pv[1] = SigmaPlus; break; |
---|
| 515 | case 21: pv[1] = SigmaZero; break; |
---|
| 516 | case 22: pv[1] = SigmaMinus;break; |
---|
| 517 | } |
---|
| 518 | switch( ipaky[i*2+1] ) |
---|
| 519 | { |
---|
| 520 | case 10: pv[i3] = KaonPlus; break; |
---|
| 521 | case 11: pv[i3] = KaonZeroShort;break; |
---|
| 522 | case 12: pv[i3] = KaonZeroLong; break; |
---|
| 523 | } |
---|
| 524 | } |
---|
| 525 | else |
---|
| 526 | { // Lbar K && Sigmabar K production |
---|
| 527 | |
---|
| 528 | // ipakyb[] = { 19,13, 19,12, 19,11, 23,13, 23,12, 23,11, |
---|
| 529 | // Lb K- Lb K0L Lb K0S S+b K- S+b K0L S+b K0S |
---|
| 530 | // 24,13, 24,12, 24,11, 25,13, 25,12, 25,11 }; |
---|
| 531 | // S0b K- S0BK0L S0BK0S S-BK- S-B K0L S-BK0S |
---|
| 532 | |
---|
| 533 | if( (incidentCode==antiprotonCode) || (incidentCode==antineutronCode) || |
---|
| 534 | (incidentCode==antilambdaCode) || (incidentMass>sigmaMinusMass) ) |
---|
| 535 | { |
---|
| 536 | switch( ipakyb[i*2] ) |
---|
| 537 | { |
---|
| 538 | case 19:pv[0] = AntiLambda; break; |
---|
| 539 | case 23:pv[0] = AntiSigmaPlus; break; |
---|
| 540 | case 24:pv[0] = AntiSigmaZero; break; |
---|
| 541 | case 25:pv[0] = AntiSigmaMinus;break; |
---|
| 542 | } |
---|
| 543 | switch( ipakyb[i*2+1] ) |
---|
| 544 | { |
---|
| 545 | case 11:pv[i3] = KaonZeroShort;break; |
---|
| 546 | case 12:pv[i3] = KaonZeroLong; break; |
---|
| 547 | case 13:pv[i3] = KaonMinus; break; |
---|
| 548 | } |
---|
| 549 | } |
---|
| 550 | else |
---|
| 551 | { |
---|
| 552 | switch( ipaky[i*2] ) |
---|
| 553 | { |
---|
| 554 | case 18:pv[0] = Lambda; break; |
---|
| 555 | case 20:pv[0] = SigmaPlus; break; |
---|
| 556 | case 21:pv[0] = SigmaZero; break; |
---|
| 557 | case 22:pv[0] = SigmaMinus;break; |
---|
| 558 | } |
---|
| 559 | switch( ipaky[i*2+1] ) |
---|
| 560 | { |
---|
| 561 | case 10: pv[i3] = KaonPlus; break; |
---|
| 562 | case 11: pv[i3] = KaonZeroShort;break; |
---|
| 563 | case 12: pv[i3] = KaonZeroLong; break; |
---|
| 564 | } |
---|
| 565 | } |
---|
| 566 | } |
---|
| 567 | } |
---|
| 568 | else |
---|
| 569 | return; |
---|
| 570 | |
---|
| 571 | // check the available energy |
---|
| 572 | // if there is not enough energy for kkb/ky pair production |
---|
| 573 | // then reduce the number of secondary particles |
---|
| 574 | // NOTE: |
---|
| 575 | // the number of secondaries may have been changed |
---|
| 576 | // the incident and/or target particles may have changed |
---|
| 577 | // charge conservation is ignored (as well as strangness conservation) |
---|
| 578 | |
---|
| 579 | incidentMass = incidentParticle.getMass(); |
---|
| 580 | targetMass = targetParticle.getMass(); |
---|
| 581 | |
---|
| 582 | G4double energyCheck = centerOfMassEnergy-(incidentMass+targetMass); |
---|
| 583 | if (verboseLevel > 1) G4cout << "Particles produced: " ; |
---|
| 584 | |
---|
| 585 | for ( i=0; i < vecLen; i++ ) |
---|
| 586 | { |
---|
| 587 | energyCheck -= pv[i].getMass(); |
---|
| 588 | if (verboseLevel > 1) G4cout << pv[i].getCode() << " " ; |
---|
| 589 | if( energyCheck < 0.0 ) |
---|
| 590 | { |
---|
| 591 | if( i > 0 ) vecLen = --i; // chop off the secondary list |
---|
| 592 | return; |
---|
| 593 | } |
---|
| 594 | } |
---|
| 595 | if (verboseLevel > 1) G4cout << G4endl; |
---|
| 596 | return; |
---|
| 597 | } |
---|
| 598 | |
---|
| 599 | void |
---|
[1347] | 600 | G4HEInelastic::HighEnergyCascading(G4bool& successful, |
---|
[819] | 601 | G4HEVector pv[], |
---|
[1347] | 602 | G4int& vecLen, |
---|
| 603 | G4double& excitationEnergyGNP, |
---|
| 604 | G4double& excitationEnergyDTA, |
---|
| 605 | const G4HEVector& incidentParticle, |
---|
| 606 | const G4HEVector& targetParticle, |
---|
[819] | 607 | G4double atomicWeight, |
---|
| 608 | G4double atomicNumber) |
---|
[1347] | 609 | { |
---|
| 610 | // The multiplicity of particles produced in the first interaction has been |
---|
| 611 | // calculated in one of the FirstIntInNuc.... routines. The nuclear |
---|
| 612 | // cascading particles are parameterized from experimental data. |
---|
| 613 | // A simple single variable description E D3S/DP3= F(Q) with |
---|
| 614 | // Q^2 = (M*X)^2 + PT^2 is used. Final state kinematics are produced |
---|
| 615 | // by an FF-type iterative cascade method. |
---|
| 616 | // Nuclear evaporation particles are added at the end of the routine. |
---|
[819] | 617 | |
---|
[1347] | 618 | // All quantities in the G4HEVector Array pv are in GeV- units. |
---|
| 619 | // The method is a copy of MediumEnergyCascading with some special tuning |
---|
| 620 | // for high energy interactions. |
---|
[819] | 621 | |
---|
[1347] | 622 | G4int protonCode = Proton.getCode(); |
---|
| 623 | G4double protonMass = Proton.getMass(); |
---|
| 624 | G4int neutronCode = Neutron.getCode(); |
---|
| 625 | G4double neutronMass = Neutron.getMass(); |
---|
| 626 | G4double kaonPlusMass = KaonPlus.getMass(); |
---|
| 627 | G4int kaonPlusCode = KaonPlus.getCode(); |
---|
| 628 | G4int kaonMinusCode = KaonMinus.getCode(); |
---|
| 629 | G4int kaonZeroSCode = KaonZeroShort.getCode(); |
---|
| 630 | G4int kaonZeroLCode = KaonZeroLong.getCode(); |
---|
| 631 | G4int kaonZeroCode = KaonZero.getCode(); |
---|
| 632 | G4int antiKaonZeroCode = AntiKaonZero.getCode(); |
---|
| 633 | G4int pionPlusCode = PionPlus.getCode(); |
---|
| 634 | G4int pionZeroCode = PionZero.getCode(); |
---|
| 635 | G4int pionMinusCode = PionMinus.getCode(); |
---|
| 636 | G4String mesonType = PionPlus.getType(); |
---|
| 637 | G4String baryonType = Proton.getType(); |
---|
| 638 | G4String antiBaryonType = AntiProton.getType(); |
---|
[819] | 639 | |
---|
[1347] | 640 | G4double targetMass = targetParticle.getMass(); |
---|
[819] | 641 | |
---|
[1347] | 642 | G4int incidentCode = incidentParticle.getCode(); |
---|
| 643 | G4double incidentMass = incidentParticle.getMass(); |
---|
| 644 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); |
---|
| 645 | G4double incidentEnergy = incidentParticle.getEnergy(); |
---|
| 646 | G4double incidentKineticEnergy = incidentParticle.getKineticEnergy(); |
---|
| 647 | G4String incidentType = incidentParticle.getType(); |
---|
[819] | 648 | // G4double incidentTOF = incidentParticle.getTOF(); |
---|
[1347] | 649 | G4double incidentTOF = 0.; |
---|
[819] | 650 | |
---|
[1347] | 651 | // some local variables |
---|
[819] | 652 | |
---|
[1347] | 653 | G4int i, j, l; |
---|
[819] | 654 | |
---|
[1347] | 655 | if (verboseLevel > 1) G4cout << " G4HEInelastic::HighEnergyCascading " |
---|
| 656 | << G4endl; |
---|
| 657 | successful = false; |
---|
| 658 | if (incidentTotalMomentum < 25. + G4UniformRand()*25.) return; |
---|
[819] | 659 | |
---|
[1347] | 660 | // define annihilation channels. |
---|
[819] | 661 | |
---|
[1347] | 662 | G4bool annihilation = false; |
---|
| 663 | if (incidentCode < 0 && incidentType == antiBaryonType && |
---|
| 664 | pv[0].getType() != antiBaryonType && |
---|
| 665 | pv[1].getType() != antiBaryonType) { |
---|
| 666 | annihilation = true; |
---|
| 667 | } |
---|
[819] | 668 | |
---|
[1347] | 669 | G4double twsup[] = { 1., 1., 0.7, 0.5, 0.3, 0.2, 0.1, 0.0 }; |
---|
[819] | 670 | |
---|
[1347] | 671 | if (annihilation) goto start; |
---|
| 672 | if (vecLen >= 8) goto start; |
---|
| 673 | if( incidentKineticEnergy < 1.) return; |
---|
| 674 | if( ( incidentCode == kaonPlusCode || incidentCode == kaonMinusCode |
---|
| 675 | || incidentCode == kaonZeroCode || incidentCode == antiKaonZeroCode |
---|
| 676 | || incidentCode == kaonZeroSCode || incidentCode == kaonZeroLCode ) |
---|
| 677 | && ( G4UniformRand() < 0.5) ) goto start; |
---|
| 678 | if( G4UniformRand() > twsup[vecLen-1]) goto start; |
---|
| 679 | if( incidentKineticEnergy > (G4UniformRand()*200 + 50.) ) goto start; |
---|
| 680 | return; |
---|
[819] | 681 | |
---|
[1347] | 682 | start: |
---|
[819] | 683 | |
---|
[1347] | 684 | if (annihilation) { |
---|
| 685 | // do some corrections of incident particle kinematic |
---|
| 686 | G4double ekcor = Amax( 1., 1./incidentKineticEnergy); |
---|
| 687 | incidentKineticEnergy = 2*targetMass + incidentKineticEnergy*(1.+ekcor/atomicWeight); |
---|
| 688 | G4double excitation = NuclearExcitation(incidentKineticEnergy, |
---|
| 689 | atomicWeight, |
---|
| 690 | atomicNumber, |
---|
| 691 | excitationEnergyGNP, |
---|
| 692 | excitationEnergyDTA); |
---|
| 693 | incidentKineticEnergy -= excitation; |
---|
| 694 | if (incidentKineticEnergy < excitationEnergyDTA) incidentKineticEnergy = 0.; |
---|
| 695 | incidentEnergy = incidentKineticEnergy + incidentMass; |
---|
| 696 | incidentTotalMomentum = |
---|
| 697 | std::sqrt( Amax(0., incidentEnergy*incidentEnergy - incidentMass*incidentMass)); |
---|
| 698 | } |
---|
[819] | 699 | |
---|
[1347] | 700 | G4HEVector pTemp; |
---|
| 701 | for (i = 2; i < vecLen; i++) { |
---|
| 702 | j = Imin( vecLen-1, (G4int)(2. + G4UniformRand()*(vecLen - 2))); |
---|
| 703 | pTemp = pv[j]; |
---|
| 704 | pv[j] = pv[i]; |
---|
| 705 | pv[i] = pTemp; |
---|
| 706 | } |
---|
| 707 | // randomize the first two leading particles |
---|
| 708 | // for kaon induced reactions only |
---|
| 709 | // (need from experimental data) |
---|
[819] | 710 | |
---|
| 711 | if( (incidentCode==kaonPlusCode || incidentCode==kaonMinusCode || |
---|
| 712 | incidentCode==kaonZeroCode || incidentCode==antiKaonZeroCode || |
---|
| 713 | incidentCode==kaonZeroSCode || incidentCode==kaonZeroLCode) |
---|
| 714 | && (G4UniformRand() > 0.9) ) |
---|
| 715 | { |
---|
| 716 | pTemp = pv[1]; |
---|
| 717 | pv[1] = pv[0]; |
---|
| 718 | pv[0] = pTemp; |
---|
| 719 | } |
---|
| 720 | // mark leading particles for incident strange particles |
---|
| 721 | // and antibaryons, for all other we assume that the first |
---|
| 722 | // and second particle are the leading particles. |
---|
| 723 | // We need this later for kinematic aspects of strangeness |
---|
| 724 | // conservation. |
---|
| 725 | |
---|
| 726 | G4int lead = 0; |
---|
| 727 | G4HEVector leadParticle; |
---|
| 728 | if( (incidentMass >= kaonPlusMass-0.05) && (incidentCode != protonCode) |
---|
| 729 | && (incidentCode != neutronCode) ) |
---|
| 730 | { |
---|
| 731 | G4double pMass = pv[0].getMass(); |
---|
| 732 | G4int pCode = pv[0].getCode(); |
---|
| 733 | if( (pMass >= kaonPlusMass-0.05) && (pCode != protonCode) |
---|
| 734 | && (pCode != neutronCode) ) |
---|
| 735 | { |
---|
| 736 | lead = pCode; |
---|
| 737 | leadParticle = pv[0]; |
---|
| 738 | } |
---|
| 739 | else |
---|
| 740 | { |
---|
| 741 | pMass = pv[1].getMass(); |
---|
| 742 | pCode = pv[1].getCode(); |
---|
| 743 | if( (pMass >= kaonPlusMass-0.05) && (pCode != protonCode) |
---|
| 744 | && (pCode != neutronCode) ) |
---|
| 745 | { |
---|
| 746 | lead = pCode; |
---|
| 747 | leadParticle = pv[1]; |
---|
| 748 | } |
---|
| 749 | } |
---|
| 750 | } |
---|
| 751 | |
---|
[1347] | 752 | // Distribute particles in forward and backward hemispheres in center |
---|
| 753 | // of mass system. Incident particle goes in forward hemisphere. |
---|
[819] | 754 | |
---|
[1347] | 755 | G4HEVector pvI = incidentParticle; // for the incident particle |
---|
| 756 | pvI.setSide( 1 ); |
---|
[819] | 757 | |
---|
[1347] | 758 | G4HEVector pvT = targetParticle; // for the target particle |
---|
| 759 | pvT.setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 760 | pvT.setSide( -1 ); |
---|
| 761 | pvT.setTOF( -1.); |
---|
[819] | 762 | |
---|
[1347] | 763 | G4double centerOfMassEnergy = std::sqrt( sqr(incidentMass)+sqr(targetMass) |
---|
[819] | 764 | +2.0*targetMass*incidentEnergy ); |
---|
[1347] | 765 | // G4double availableEnergy = centerOfMassEnergy - ( targetMass + incidentMass ); |
---|
[819] | 766 | |
---|
[1347] | 767 | G4double tavai1 = centerOfMassEnergy/2.0 - incidentMass; |
---|
| 768 | G4double tavai2 = centerOfMassEnergy/2.0 - targetMass; |
---|
[819] | 769 | |
---|
[1347] | 770 | // define G4HEVector- array for kinematic manipulations, |
---|
| 771 | // with a one by one correspondence to the pv-Array. |
---|
[819] | 772 | |
---|
[1347] | 773 | G4int ntb = 1; |
---|
| 774 | for (i = 0; i < vecLen; i++) { |
---|
| 775 | if (i == 0) pv[i].setSide(1); |
---|
| 776 | else if (i == 1) pv[i].setSide(-1); |
---|
| 777 | else { |
---|
| 778 | if (G4UniformRand() < 0.5) { |
---|
| 779 | pv[i].setSide(-1); |
---|
| 780 | ntb++; |
---|
| 781 | } else { |
---|
| 782 | pv[i].setSide(1); |
---|
[819] | 783 | } |
---|
[1347] | 784 | } |
---|
| 785 | pv[i].setTOF(incidentTOF); |
---|
| 786 | } |
---|
[819] | 787 | |
---|
[1347] | 788 | G4double tb = 2. * ntb; |
---|
| 789 | if (centerOfMassEnergy < (2. + G4UniformRand())) |
---|
| 790 | tb = (2. * ntb + vecLen)/2.; |
---|
[819] | 791 | |
---|
[1347] | 792 | if (verboseLevel > 1) { |
---|
| 793 | G4cout << " pv Vector after Randomization " << vecLen << G4endl; |
---|
| 794 | pvI.Print(-1); |
---|
| 795 | pvT.Print(-1); |
---|
| 796 | for (i = 0; i < vecLen; i++) pv[i].Print(i); |
---|
| 797 | } |
---|
[819] | 798 | |
---|
[1347] | 799 | // Add particles from intranuclear cascade |
---|
| 800 | // nuclearCascadeCount = number of new secondaries produced by nuclear |
---|
| 801 | // cascading. |
---|
| 802 | // extraCount = number of nucleons within these new secondaries |
---|
| 803 | |
---|
[819] | 804 | G4double s, xtarg, ran; |
---|
| 805 | s = centerOfMassEnergy*centerOfMassEnergy; |
---|
| 806 | G4double afc; |
---|
| 807 | afc = Amin(0.5, 0.312 + 0.200 * std::log(std::log(s))+ std::pow(s,1.5)/6000.0); |
---|
| 808 | xtarg = Amax(0.01, afc * (std::pow(atomicWeight, 0.33) - 1.0) * tb); |
---|
| 809 | G4int nstran = Poisson( 0.03*xtarg); |
---|
| 810 | G4int momentumBin = 0; |
---|
| 811 | G4double nucsup[] = { 1.00, 0.7, 0.5, 0.4, 0.5, 0.5 }; |
---|
| 812 | G4double psup[] = { 3., 6., 20., 50., 100., 1000. }; |
---|
| 813 | while( (momentumBin < 6) && (incidentTotalMomentum > psup[momentumBin])) momentumBin++; |
---|
| 814 | momentumBin = Imin(5, momentumBin); |
---|
| 815 | G4double xpnhmf = Amax(0.01,xtarg*nucsup[momentumBin]); |
---|
| 816 | G4double xshhmf = Amax(0.01,xtarg - xpnhmf); |
---|
| 817 | G4double rshhmf = 0.25*xshhmf; |
---|
| 818 | G4double rpnhmf = 0.81*xpnhmf; |
---|
| 819 | G4double xhmf=0; |
---|
| 820 | if(verboseLevel > 1) |
---|
| 821 | G4cout << "xtarg= " << xtarg << " xpnhmf = " << xpnhmf << G4endl; |
---|
| 822 | |
---|
| 823 | G4int nshhmf, npnhmf; |
---|
| 824 | if (rshhmf > 1.1) |
---|
| 825 | { |
---|
| 826 | rshhmf = xshhmf/(rshhmf-1.); |
---|
| 827 | if (rshhmf <= 20.) |
---|
| 828 | xhmf = GammaRand( rshhmf ); |
---|
| 829 | else |
---|
| 830 | xhmf = Erlang( G4int(rshhmf+0.5) ); |
---|
| 831 | xshhmf *= xhmf/rshhmf; |
---|
| 832 | } |
---|
| 833 | nshhmf = Poisson( xshhmf ); |
---|
| 834 | if(verboseLevel > 1) |
---|
| 835 | G4cout << "xshhmf = " << xshhmf << " xhmf = " << xhmf |
---|
| 836 | << " rshhmf = " << rshhmf << G4endl; |
---|
| 837 | |
---|
| 838 | if (rpnhmf > 1.1) |
---|
| 839 | { |
---|
| 840 | rpnhmf = xpnhmf/(rpnhmf -1.); |
---|
| 841 | if (rpnhmf <= 20.) |
---|
| 842 | xhmf = GammaRand( rpnhmf ); |
---|
| 843 | else |
---|
| 844 | xhmf = Erlang( G4int(rpnhmf+0.5) ); |
---|
| 845 | xpnhmf *= xhmf/rpnhmf; |
---|
| 846 | } |
---|
| 847 | npnhmf = Poisson( xpnhmf ); |
---|
| 848 | if(verboseLevel > 1) |
---|
| 849 | G4cout << "nshhmf = " << nshhmf << " npnhmf = " << npnhmf |
---|
| 850 | << " nstran = " << nstran << G4endl; |
---|
| 851 | |
---|
| 852 | G4int ntarg = nshhmf + npnhmf + nstran; |
---|
| 853 | |
---|
| 854 | G4int targ = 0; |
---|
| 855 | |
---|
| 856 | while (npnhmf > 0) |
---|
| 857 | { |
---|
| 858 | if ( G4UniformRand() > (1. - atomicNumber/atomicWeight)) |
---|
| 859 | pv[vecLen] = Proton; |
---|
| 860 | else |
---|
| 861 | pv[vecLen] = Neutron; |
---|
| 862 | targ++; |
---|
| 863 | pv[vecLen].setSide( -2 ); |
---|
| 864 | pv[vecLen].setFlag( true ); |
---|
| 865 | pv[vecLen].setTOF( incidentTOF ); |
---|
| 866 | vecLen++; |
---|
| 867 | npnhmf--; |
---|
| 868 | } |
---|
| 869 | while (nstran > 0) |
---|
| 870 | { |
---|
| 871 | ran = G4UniformRand(); |
---|
| 872 | if (ran < 0.14) pv[vecLen] = Lambda; |
---|
| 873 | else if (ran < 0.20) pv[vecLen] = SigmaZero; |
---|
| 874 | else if (ran < 0.43) pv[vecLen] = KaonPlus; |
---|
| 875 | else if (ran < 0.66) pv[vecLen] = KaonZero; |
---|
| 876 | else if (ran < 0.89) pv[vecLen] = AntiKaonZero; |
---|
| 877 | else pv[vecLen] = KaonMinus; |
---|
| 878 | if (G4UniformRand() > 0.2) |
---|
| 879 | { |
---|
| 880 | pv[vecLen].setSide( -2 ); |
---|
| 881 | pv[vecLen].setFlag( true ); |
---|
| 882 | } |
---|
| 883 | else |
---|
| 884 | { |
---|
| 885 | pv[vecLen].setSide( 1 ); |
---|
| 886 | pv[vecLen].setFlag( false ); |
---|
| 887 | ntarg--; |
---|
| 888 | } |
---|
| 889 | pv[vecLen].setTOF( incidentTOF ); |
---|
| 890 | vecLen++; |
---|
| 891 | nstran--; |
---|
| 892 | } |
---|
| 893 | while (nshhmf > 0) |
---|
| 894 | { |
---|
| 895 | ran = G4UniformRand(); |
---|
| 896 | if( ran < 0.33333 ) |
---|
| 897 | pv[vecLen] = PionPlus; |
---|
| 898 | else if( ran < 0.66667 ) |
---|
| 899 | pv[vecLen] = PionZero; |
---|
| 900 | else |
---|
| 901 | pv[vecLen] = PionMinus; |
---|
| 902 | if (G4UniformRand() > 0.2) |
---|
| 903 | { |
---|
| 904 | pv[vecLen].setSide( -2 ); // backward cascade particles |
---|
| 905 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 906 | } |
---|
| 907 | else |
---|
| 908 | { |
---|
| 909 | pv[vecLen].setSide( 1 ); |
---|
| 910 | pv[vecLen].setFlag( false ); |
---|
| 911 | ntarg--; |
---|
| 912 | } |
---|
| 913 | pv[vecLen].setTOF( incidentTOF ); |
---|
| 914 | vecLen++; |
---|
| 915 | nshhmf--; |
---|
| 916 | } |
---|
| 917 | |
---|
[1347] | 918 | // assume conservation of kinetic energy |
---|
| 919 | // in forward & backward hemispheres |
---|
[819] | 920 | |
---|
[1347] | 921 | G4int is, iskip, iavai1; |
---|
| 922 | if (vecLen <= 1) return; |
---|
[819] | 923 | |
---|
[1347] | 924 | tavai1 = centerOfMassEnergy/2.; |
---|
| 925 | iavai1 = 0; |
---|
[819] | 926 | |
---|
[1347] | 927 | for (i = 0; i < vecLen; i++) |
---|
[819] | 928 | { |
---|
| 929 | if (pv[i].getSide() > 0) |
---|
| 930 | { |
---|
| 931 | tavai1 -= pv[i].getMass(); |
---|
| 932 | iavai1++; |
---|
| 933 | } |
---|
| 934 | } |
---|
[1347] | 935 | if ( iavai1 == 0) return; |
---|
[819] | 936 | |
---|
[1347] | 937 | while (tavai1 <= 0.0) { |
---|
| 938 | // must eliminate a particle from the forward side |
---|
| 939 | iskip = G4int(G4UniformRand()*iavai1) + 1; |
---|
| 940 | is = 0; |
---|
| 941 | for (i = vecLen-1; i >= 0; i--) { |
---|
| 942 | if (pv[i].getSide() > 0) { |
---|
| 943 | if (++is == iskip) { |
---|
| 944 | tavai1 += pv[i].getMass(); |
---|
| 945 | iavai1--; |
---|
| 946 | if (i != vecLen-1) { |
---|
| 947 | for (j = i; j < vecLen; j++) pv[j] = pv[j+1]; |
---|
| 948 | } |
---|
| 949 | if (--vecLen == 0) return; // all the secondaries except the |
---|
| 950 | break; // --+ |
---|
| 951 | } // | |
---|
| 952 | } // v |
---|
| 953 | } // break goes down to here |
---|
| 954 | } // to the end of the for- loop. |
---|
[819] | 955 | |
---|
[1347] | 956 | tavai2 = (targ+1)*centerOfMassEnergy/2.; |
---|
| 957 | G4int iavai2 = 0; |
---|
[819] | 958 | |
---|
| 959 | for (i = 0; i < vecLen; i++) |
---|
| 960 | { |
---|
| 961 | if (pv[i].getSide() < 0) |
---|
| 962 | { |
---|
| 963 | tavai2 -= pv[i].getMass(); |
---|
| 964 | iavai2++; |
---|
| 965 | } |
---|
| 966 | } |
---|
| 967 | if (iavai2 == 0) return; |
---|
| 968 | |
---|
| 969 | while( tavai2 <= 0.0 ) |
---|
| 970 | { // must eliminate a particle from the backward side |
---|
| 971 | iskip = G4int(G4UniformRand()*iavai2) + 1; |
---|
| 972 | is = 0; |
---|
| 973 | for( i = vecLen-1; i >= 0; i-- ) |
---|
| 974 | { |
---|
| 975 | if( pv[i].getSide() < 0 ) |
---|
| 976 | { |
---|
| 977 | if( ++is == iskip ) |
---|
| 978 | { |
---|
| 979 | tavai2 += pv[i].getMass(); |
---|
| 980 | iavai2--; |
---|
| 981 | if (pv[i].getSide() == -2) ntarg--; |
---|
| 982 | if (i != vecLen-1) |
---|
| 983 | { |
---|
| 984 | for( j=i; j<vecLen; j++) |
---|
| 985 | { |
---|
| 986 | pv[j] = pv[j+1]; |
---|
| 987 | } |
---|
| 988 | } |
---|
| 989 | if (--vecLen == 0) return; |
---|
| 990 | break; |
---|
| 991 | } |
---|
| 992 | } |
---|
| 993 | } |
---|
| 994 | } |
---|
| 995 | |
---|
[1347] | 996 | if (verboseLevel > 1) { |
---|
| 997 | G4cout << " pv Vector after Energy checks " |
---|
| 998 | << vecLen << " " << tavai1 << " " << iavai1 << " " << tavai2 |
---|
| 999 | << " " << iavai2 << " " << ntarg << G4endl; |
---|
| 1000 | pvI.Print(-1); |
---|
| 1001 | pvT.Print(-1); |
---|
| 1002 | for (i=0; i < vecLen ; i++) pv[i].Print(i); |
---|
| 1003 | } |
---|
[819] | 1004 | |
---|
[1347] | 1005 | // define some vectors for Lorentz transformations |
---|
[819] | 1006 | |
---|
[1347] | 1007 | G4HEVector* pvmx = new G4HEVector [10]; |
---|
[819] | 1008 | |
---|
[1347] | 1009 | pvmx[0].setMass( incidentMass ); |
---|
| 1010 | pvmx[0].setMomentumAndUpdate( 0.0, 0.0, incidentTotalMomentum ); |
---|
| 1011 | pvmx[1].setMass( protonMass); |
---|
| 1012 | pvmx[1].setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 1013 | pvmx[3].setMass( protonMass*(1+targ)); |
---|
| 1014 | pvmx[3].setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 1015 | pvmx[4].setZero(); |
---|
| 1016 | pvmx[5].setZero(); |
---|
| 1017 | pvmx[7].setZero(); |
---|
| 1018 | pvmx[8].setZero(); |
---|
| 1019 | pvmx[8].setMomentum( 1.0, 0.0 ); |
---|
| 1020 | pvmx[2].Add( pvmx[0], pvmx[1] ); |
---|
| 1021 | pvmx[3].Add( pvmx[3], pvmx[0] ); |
---|
| 1022 | pvmx[0].Lor( pvmx[0], pvmx[2] ); |
---|
| 1023 | pvmx[1].Lor( pvmx[1], pvmx[2] ); |
---|
[819] | 1024 | |
---|
[1347] | 1025 | if (verboseLevel > 1) { |
---|
| 1026 | G4cout << " General Vectors after Definition " << G4endl; |
---|
| 1027 | for (i=0; i<10; i++) pvmx[i].Print(i); |
---|
| 1028 | } |
---|
[819] | 1029 | |
---|
[1347] | 1030 | // Main loop for 4-momentum generation - see Pitha-report (Aachen) |
---|
| 1031 | // for a detailed description of the method. |
---|
| 1032 | // Process the secondary particles in reverse order. |
---|
[819] | 1033 | |
---|
[1347] | 1034 | G4double dndl[20]; |
---|
| 1035 | G4double binl[20]; |
---|
| 1036 | G4double pvMass(0), pvEnergy(0); |
---|
| 1037 | G4int pvCode; |
---|
| 1038 | G4double aspar, pt, phi, et, xval; |
---|
| 1039 | G4double ekin = 0.; |
---|
| 1040 | G4double ekin1 = 0.; |
---|
| 1041 | G4double ekin2 = 0.; |
---|
| 1042 | G4int npg = 0; |
---|
| 1043 | G4double rmg0 = 0.; |
---|
| 1044 | G4int targ1 = 0; // No fragmentation model for nucleons from |
---|
| 1045 | phi = G4UniformRand()*twopi; |
---|
| 1046 | |
---|
| 1047 | for (i = vecLen-1; i >= 0; i--) { |
---|
| 1048 | // Intranuclear cascade: mark them with -3 and leave the loop |
---|
[819] | 1049 | if( i == 1) |
---|
| 1050 | { |
---|
| 1051 | if ( (pv[i].getMass() > neutronMass + 0.05) && (G4UniformRand() < 0.2)) |
---|
| 1052 | { |
---|
| 1053 | if(++npg < 19) |
---|
| 1054 | { |
---|
| 1055 | pv[i].setSide(-3); |
---|
| 1056 | rmg0 += pv[i].getMass(); |
---|
| 1057 | targ++; |
---|
| 1058 | continue; |
---|
| 1059 | } |
---|
| 1060 | } |
---|
| 1061 | else if ( pv[i].getMass() > protonMass - 0.05) |
---|
| 1062 | { |
---|
| 1063 | if(++npg < 19) |
---|
| 1064 | { |
---|
| 1065 | pv[i].setSide(-3); |
---|
| 1066 | rmg0 += pv[i].getMass(); |
---|
| 1067 | targ++; |
---|
| 1068 | continue; |
---|
| 1069 | } |
---|
| 1070 | } |
---|
| 1071 | } |
---|
| 1072 | if( pv[i].getSide() == -2) |
---|
| 1073 | { |
---|
| 1074 | if ( pv[i].getName() == "Proton" || pv[i].getName() == "Neutron") |
---|
| 1075 | { |
---|
| 1076 | if( ++npg < 19 ) |
---|
| 1077 | { |
---|
| 1078 | pv[i].setSide( -3 ); |
---|
| 1079 | rmg0 += pv[i].getMass(); |
---|
| 1080 | targ1++; |
---|
| 1081 | continue; // leave the for loop !! |
---|
| 1082 | } |
---|
| 1083 | } |
---|
| 1084 | } |
---|
| 1085 | // Set pt and phi values - they are changed somewhat in the |
---|
| 1086 | // iteration loop. |
---|
| 1087 | // Set mass parameter for lambda fragmentation model |
---|
| 1088 | |
---|
| 1089 | G4double maspar[] = { 0.75, 0.70, 0.65, 0.60, 0.50, 0.40, 0.20, 0.10}; |
---|
| 1090 | G4double bp[] = { 4.00, 2.50, 2.20, 3.00, 3.00, 1.70, 3.50, 3.50}; |
---|
| 1091 | G4double ptex[] = { 1.70, 1.70, 1.50, 1.70, 1.40, 1.20, 1.70, 1.20}; |
---|
| 1092 | |
---|
| 1093 | // Set parameters for lambda simulation |
---|
| 1094 | // pt is the average transverse momentum |
---|
| 1095 | // aspar is average transverse mass |
---|
| 1096 | |
---|
| 1097 | pvMass = pv[i].getMass(); |
---|
| 1098 | j = 2; |
---|
| 1099 | if (pv[i].getType() == mesonType ) j = 1; |
---|
| 1100 | if ( pv[i].getMass() < 0.4 ) j = 0; |
---|
| 1101 | if ( i <= 1 ) j += 3; |
---|
| 1102 | if (pv[i].getSide() <= -2) j = 6; |
---|
| 1103 | if (j == 6 && (pv[i].getType() == baryonType || pv[i].getType() == antiBaryonType)) j = 7; |
---|
| 1104 | pt = std::sqrt(std::pow(-std::log(1.-G4UniformRand())/bp[j],ptex[j])); |
---|
| 1105 | if(pt<0.05) pt = Amax(0.001, 0.3*G4UniformRand()); |
---|
| 1106 | aspar = maspar[j]; |
---|
| 1107 | phi = G4UniformRand()*twopi; |
---|
| 1108 | pv[i].setMomentum( pt*std::cos(phi), pt*std::sin(phi) ); // set x- and y-momentum |
---|
| 1109 | |
---|
| 1110 | for( j=0; j<20; j++ ) binl[j] = j/(19.*pt); // set the lambda - bins. |
---|
| 1111 | |
---|
| 1112 | if( pv[i].getSide() > 0 ) |
---|
| 1113 | et = pvmx[0].getEnergy(); |
---|
| 1114 | else |
---|
| 1115 | et = pvmx[1].getEnergy(); |
---|
| 1116 | |
---|
| 1117 | dndl[0] = 0.0; |
---|
| 1118 | |
---|
| 1119 | // Start of outer iteration loop |
---|
| 1120 | |
---|
| 1121 | G4int outerCounter = 0, innerCounter = 0; // three times. |
---|
| 1122 | G4bool eliminateThisParticle = true; |
---|
| 1123 | G4bool resetEnergies = true; |
---|
| 1124 | while( ++outerCounter < 3 ) |
---|
| 1125 | { |
---|
| 1126 | for( l=1; l<20; l++ ) |
---|
| 1127 | { |
---|
| 1128 | xval = (binl[l]+binl[l-1])/2.; // x = lambda /GeV |
---|
| 1129 | if( xval > 1./pt ) |
---|
| 1130 | dndl[l] = dndl[l-1]; |
---|
| 1131 | else |
---|
| 1132 | dndl[l] = dndl[l-1] + |
---|
| 1133 | aspar/std::sqrt( std::pow((1.+aspar*xval*aspar*xval),3) ) * |
---|
| 1134 | (binl[l]-binl[l-1]) * et / |
---|
| 1135 | std::sqrt( pt*xval*et*pt*xval*et + pt*pt + pvMass*pvMass ); |
---|
| 1136 | } |
---|
| 1137 | |
---|
| 1138 | // Start of inner iteration loop |
---|
| 1139 | |
---|
| 1140 | innerCounter = 0; // try this not more than 7 times. |
---|
| 1141 | while( ++innerCounter < 7 ) |
---|
| 1142 | { |
---|
| 1143 | l = 1; |
---|
| 1144 | ran = G4UniformRand()*dndl[19]; |
---|
| 1145 | while( ( ran >= dndl[l] ) && ( l < 20 ) )l++; |
---|
| 1146 | l = Imin( 19, l ); |
---|
[962] | 1147 | xval = Amin( 1.0, pt*(binl[l-1] + G4UniformRand()*(binl[l]-binl[l-1]) ) ); |
---|
[819] | 1148 | if( pv[i].getSide() < 0 ) xval *= -1.; |
---|
| 1149 | pv[i].setMomentumAndUpdate( xval*et ); // Set the z-momentum |
---|
| 1150 | pvEnergy = pv[i].getEnergy(); |
---|
| 1151 | if( pv[i].getSide() > 0 ) // Forward side |
---|
| 1152 | { |
---|
| 1153 | if ( i < 2 ) |
---|
| 1154 | { |
---|
| 1155 | ekin = tavai1 - ekin1; |
---|
| 1156 | if (ekin < 0.) ekin = 0.04*std::fabs(normal()); |
---|
| 1157 | G4double pp1 = pv[i].Length(); |
---|
| 1158 | if (pp1 >= 1.e-6) |
---|
| 1159 | { |
---|
| 1160 | G4double pp = std::sqrt(ekin*(ekin+2*pvMass)); |
---|
| 1161 | pp = Amax(0., pp*pp - pt*pt); |
---|
| 1162 | pp = std::sqrt(pp)*pv[i].getSide()/std::fabs(G4double(pv[i].getSide())); // cast for aCC |
---|
| 1163 | pv[i].setMomentumAndUpdate( pp ); |
---|
| 1164 | } |
---|
| 1165 | else |
---|
| 1166 | { |
---|
| 1167 | pv[i].setMomentum(0.,0.,0.); |
---|
| 1168 | pv[i].setKineticEnergyAndUpdate( ekin); |
---|
| 1169 | } |
---|
| 1170 | pvmx[4].Add( pvmx[4], pv[i]); |
---|
| 1171 | outerCounter = 2; |
---|
| 1172 | resetEnergies = false; |
---|
| 1173 | eliminateThisParticle = false; |
---|
| 1174 | break; |
---|
| 1175 | } |
---|
| 1176 | else if( (ekin1+pvEnergy-pvMass) < 0.95*tavai1 ) |
---|
| 1177 | { |
---|
| 1178 | pvmx[4].Add( pvmx[4], pv[i] ); |
---|
| 1179 | ekin1 += pvEnergy - pvMass; |
---|
| 1180 | pvmx[6].Add( pvmx[4], pvmx[5] ); |
---|
| 1181 | pvmx[6].setMomentum( 0.0 ); |
---|
| 1182 | outerCounter = 2; // leave outer loop |
---|
| 1183 | eliminateThisParticle = false; // don't eliminate this particle |
---|
| 1184 | resetEnergies = false; |
---|
| 1185 | break; // next particle |
---|
| 1186 | } |
---|
| 1187 | if( innerCounter > 5 ) break; // leave inner loop |
---|
| 1188 | |
---|
| 1189 | if( tavai2 >= pvMass ) |
---|
| 1190 | { // switch sides |
---|
| 1191 | pv[i].setSide( -1 ); |
---|
| 1192 | tavai1 += pvMass; |
---|
| 1193 | tavai2 -= pvMass; |
---|
| 1194 | iavai2++; |
---|
| 1195 | } |
---|
| 1196 | } |
---|
| 1197 | else |
---|
| 1198 | { // backward side |
---|
| 1199 | xval = Amin(0.999,0.95+0.05*targ/20.0); |
---|
| 1200 | if( (ekin2+pvEnergy-pvMass) < xval*tavai2 ) |
---|
| 1201 | { |
---|
| 1202 | pvmx[5].Add( pvmx[5], pv[i] ); |
---|
| 1203 | ekin2 += pvEnergy - pvMass; |
---|
| 1204 | pvmx[6].Add( pvmx[4], pvmx[5] ); |
---|
| 1205 | pvmx[6].setMomentum( 0.0 ); // set z-momentum |
---|
| 1206 | outerCounter = 2; // leave outer iteration |
---|
| 1207 | eliminateThisParticle = false; // don't eliminate this particle |
---|
| 1208 | resetEnergies = false; |
---|
| 1209 | break; // leave inner iteration |
---|
| 1210 | } |
---|
| 1211 | if( innerCounter > 5 )break; // leave inner iteration |
---|
| 1212 | |
---|
| 1213 | if( tavai1 >= pvMass ) |
---|
| 1214 | { // switch sides |
---|
| 1215 | pv[i].setSide( 1 ); |
---|
| 1216 | tavai1 -= pvMass; |
---|
| 1217 | tavai2 += pvMass; |
---|
| 1218 | iavai2--; |
---|
| 1219 | } |
---|
| 1220 | } |
---|
| 1221 | pv[i].setMomentum( pv[i].getMomentum().x() * 0.9, |
---|
| 1222 | pv[i].getMomentum().y() * 0.9); |
---|
| 1223 | pt *= 0.9; |
---|
| 1224 | dndl[19] *= 0.9; |
---|
| 1225 | } // closes inner loop |
---|
| 1226 | |
---|
| 1227 | if (resetEnergies) |
---|
| 1228 | { |
---|
| 1229 | if (verboseLevel > 1) { |
---|
| 1230 | G4cout << " Reset energies for index " << i << " " |
---|
| 1231 | << ekin1 << " " << tavai1 << G4endl; |
---|
| 1232 | pv[i].Print(i); |
---|
| 1233 | } |
---|
| 1234 | ekin1 = 0.0; |
---|
| 1235 | ekin2 = 0.0; |
---|
| 1236 | pvmx[4].setZero(); |
---|
| 1237 | pvmx[5].setZero(); |
---|
| 1238 | |
---|
| 1239 | for( l=i+1; l < vecLen; l++ ) |
---|
| 1240 | { |
---|
| 1241 | if( (pv[l].getMass() < protonMass) || (pv[l].getSide() > 0) ) |
---|
| 1242 | { |
---|
| 1243 | pvEnergy = pv[l].getMass() + 0.95*pv[l].getKineticEnergy(); |
---|
| 1244 | pv[l].setEnergyAndUpdate( pvEnergy ); |
---|
| 1245 | if( pv[l].getSide() > 0) |
---|
| 1246 | { |
---|
| 1247 | ekin1 += pv[l].getKineticEnergy(); |
---|
| 1248 | pvmx[4].Add( pvmx[4], pv[l] ); |
---|
| 1249 | } |
---|
| 1250 | else |
---|
| 1251 | { |
---|
| 1252 | ekin2 += pv[l].getKineticEnergy(); |
---|
| 1253 | pvmx[5].Add( pvmx[5], pv[l] ); |
---|
| 1254 | } |
---|
| 1255 | } |
---|
| 1256 | } |
---|
| 1257 | } |
---|
| 1258 | } // closes outer iteration |
---|
| 1259 | |
---|
[1347] | 1260 | if (eliminateThisParticle) { |
---|
| 1261 | // Not enough energy - eliminate this particle |
---|
| 1262 | if (verboseLevel > 1) { |
---|
| 1263 | G4cout << " Eliminate particle index " << i << G4endl; |
---|
| 1264 | pv[i].Print(i); |
---|
| 1265 | } |
---|
| 1266 | if (i != vecLen-1) { |
---|
| 1267 | // shift down |
---|
| 1268 | for (j = i; j < vecLen-1; j++) pv[j] = pv[j+1]; |
---|
| 1269 | } |
---|
| 1270 | vecLen--; |
---|
[819] | 1271 | |
---|
[1347] | 1272 | if (vecLen < 2) { |
---|
| 1273 | delete [] pvmx; |
---|
| 1274 | return; |
---|
| 1275 | } |
---|
| 1276 | i++; |
---|
| 1277 | pvmx[6].Add( pvmx[4], pvmx[5] ); |
---|
| 1278 | pvmx[6].setMomentum( 0.0 ); // set z-momentum |
---|
| 1279 | } |
---|
| 1280 | } // closes main for loop |
---|
| 1281 | |
---|
| 1282 | if (verboseLevel > 1) { |
---|
| 1283 | G4cout << " pv Vector after lambda fragmentation " << vecLen << G4endl; |
---|
| 1284 | pvI.Print(-1); |
---|
| 1285 | pvT.Print(-1); |
---|
| 1286 | for (i=0; i < vecLen ; i++) pv[i].Print(i); |
---|
| 1287 | for (i=0; i < 10; i++) pvmx[i].Print(i); |
---|
| 1288 | } |
---|
| 1289 | |
---|
| 1290 | // Backward nucleons produced with a cluster model |
---|
| 1291 | |
---|
| 1292 | G4double gpar[] = {2.6, 2.6, 1.80, 1.30, 1.20}; |
---|
| 1293 | G4double cpar[] = {0.6, 0.6, 0.35, 0.15, 0.10}; |
---|
[819] | 1294 | |
---|
[1347] | 1295 | if (npg > 0) { |
---|
| 1296 | G4double rmg = rmg0; |
---|
| 1297 | if (npg > 1) { |
---|
| 1298 | G4int npg1 = npg-1; |
---|
| 1299 | if (npg1 >4) npg1 = 4; |
---|
| 1300 | rmg += std::pow( -std::log(1.-G4UniformRand()), cpar[npg1])/gpar[npg1]; |
---|
| 1301 | } |
---|
| 1302 | G4double ga = 1.2; |
---|
| 1303 | G4double ekit1 = 0.04, ekit2 = 0.6; |
---|
| 1304 | if (incidentKineticEnergy < 5.) { |
---|
| 1305 | ekit1 *= sqr(incidentKineticEnergy)/25.; |
---|
| 1306 | ekit2 *= sqr(incidentKineticEnergy)/25.; |
---|
| 1307 | } |
---|
| 1308 | G4double avalue = (1.-ga)/(std::pow(ekit2,1.-ga)-std::pow(ekit1,1.-ga)); |
---|
| 1309 | for (i = 0; i < vecLen; i++) { |
---|
| 1310 | if (pv[i].getSide() == -3) { |
---|
| 1311 | G4double ekit = std::pow(G4UniformRand()*(1.-ga)/avalue + std::pow(ekit1,1.-ga), 1./(1.-ga) ); |
---|
| 1312 | G4double cost = Amax(-1., Amin(1., std::log(2.23*G4UniformRand()+0.383)/0.96)); |
---|
| 1313 | G4double sint = std::sqrt(1. - cost*cost); |
---|
| 1314 | G4double phi = twopi*G4UniformRand(); |
---|
| 1315 | G4double pp = std::sqrt(ekit*(ekit+2*pv[i].getMass())); |
---|
| 1316 | pv[i].setMomentum(pp*sint*std::sin(phi), |
---|
| 1317 | pp*sint*std::cos(phi), |
---|
| 1318 | pp*cost); |
---|
| 1319 | pv[i].Lor( pv[i], pvmx[2] ); |
---|
| 1320 | pvmx[5].Add( pvmx[5], pv[i] ); |
---|
| 1321 | } |
---|
| 1322 | } |
---|
| 1323 | } |
---|
[819] | 1324 | |
---|
[1347] | 1325 | if (vecLen <= 2) { |
---|
| 1326 | successful = false; |
---|
| 1327 | delete [] pvmx; |
---|
| 1328 | return; |
---|
| 1329 | } |
---|
[819] | 1330 | |
---|
[1347] | 1331 | // Lorentz transformation in lab system |
---|
[819] | 1332 | |
---|
| 1333 | targ = 0; |
---|
| 1334 | for( i=0; i < vecLen; i++ ) |
---|
| 1335 | { |
---|
| 1336 | if( pv[i].getType() == baryonType )targ++; |
---|
| 1337 | if( pv[i].getType() == antiBaryonType )targ--; |
---|
| 1338 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 1339 | pv[i].Lor( pv[i], pvmx[1] ); |
---|
| 1340 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 1341 | } |
---|
| 1342 | if ( targ <1) targ = 1; |
---|
| 1343 | |
---|
| 1344 | G4bool dum=0; |
---|
| 1345 | if( lead ) |
---|
| 1346 | { |
---|
| 1347 | for( i=0; i<vecLen; i++ ) |
---|
| 1348 | { |
---|
| 1349 | if( pv[i].getCode() == lead ) |
---|
| 1350 | { |
---|
| 1351 | dum = false; |
---|
| 1352 | break; |
---|
| 1353 | } |
---|
| 1354 | } |
---|
| 1355 | if( dum ) |
---|
| 1356 | { |
---|
| 1357 | i = 0; |
---|
| 1358 | |
---|
| 1359 | if( ( (leadParticle.getType() == baryonType || |
---|
| 1360 | leadParticle.getType() == antiBaryonType) |
---|
| 1361 | && (pv[1].getType() == baryonType || |
---|
| 1362 | pv[1].getType() == antiBaryonType)) |
---|
| 1363 | || ( (leadParticle.getType() == mesonType) |
---|
| 1364 | && (pv[1].getType() == mesonType))) |
---|
| 1365 | { |
---|
| 1366 | i = 1; |
---|
| 1367 | } |
---|
| 1368 | ekin = pv[i].getKineticEnergy(); |
---|
| 1369 | pv[i] = leadParticle; |
---|
| 1370 | if( pv[i].getFlag() ) |
---|
| 1371 | pv[i].setTOF( -1.0 ); |
---|
| 1372 | else |
---|
| 1373 | pv[i].setTOF( 1.0 ); |
---|
| 1374 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 1375 | } |
---|
| 1376 | } |
---|
| 1377 | |
---|
[1347] | 1378 | pvmx[3].setMass( incidentMass); |
---|
| 1379 | pvmx[3].setMomentumAndUpdate( 0.0, 0.0, incidentTotalMomentum ); |
---|
[819] | 1380 | |
---|
[1347] | 1381 | G4double ekin0 = pvmx[3].getKineticEnergy(); |
---|
[819] | 1382 | |
---|
[1347] | 1383 | pvmx[4].setMass( protonMass * targ); |
---|
| 1384 | pvmx[4].setEnergy( protonMass * targ); |
---|
| 1385 | pvmx[4].setKineticEnergy(0.); |
---|
| 1386 | pvmx[4].setMomentum(0., 0., 0.); |
---|
| 1387 | ekin = pvmx[3].getEnergy() + pvmx[4].getEnergy(); |
---|
[819] | 1388 | |
---|
| 1389 | pvmx[5].Add( pvmx[3], pvmx[4] ); |
---|
| 1390 | pvmx[3].Lor( pvmx[3], pvmx[5] ); |
---|
| 1391 | pvmx[4].Lor( pvmx[4], pvmx[5] ); |
---|
| 1392 | |
---|
| 1393 | G4double tecm = pvmx[3].getEnergy() + pvmx[4].getEnergy(); |
---|
| 1394 | |
---|
| 1395 | pvmx[7].setZero(); |
---|
| 1396 | |
---|
| 1397 | ekin1 = 0.0; |
---|
| 1398 | G4double teta, wgt; |
---|
| 1399 | |
---|
| 1400 | for( i=0; i < vecLen; i++ ) |
---|
| 1401 | { |
---|
| 1402 | pvmx[7].Add( pvmx[7], pv[i] ); |
---|
| 1403 | ekin1 += pv[i].getKineticEnergy(); |
---|
| 1404 | ekin -= pv[i].getMass(); |
---|
| 1405 | } |
---|
| 1406 | |
---|
| 1407 | if( vecLen > 1 && vecLen < 19 ) |
---|
| 1408 | { |
---|
| 1409 | G4bool constantCrossSection = true; |
---|
| 1410 | G4HEVector pw[19]; |
---|
| 1411 | for(i=0; i<vecLen; i++) pw[i] = pv[i]; |
---|
| 1412 | wgt = NBodyPhaseSpace( tecm, constantCrossSection, pw, vecLen ); |
---|
| 1413 | ekin = 0.0; |
---|
| 1414 | for( i=0; i < vecLen; i++ ) |
---|
| 1415 | { |
---|
| 1416 | pvmx[6].setMass( pw[i].getMass()); |
---|
| 1417 | pvmx[6].setMomentum( pw[i].getMomentum() ); |
---|
| 1418 | pvmx[6].SmulAndUpdate( pvmx[6], 1. ); |
---|
| 1419 | pvmx[6].Lor( pvmx[6], pvmx[4] ); |
---|
| 1420 | ekin += pvmx[6].getKineticEnergy(); |
---|
| 1421 | } |
---|
| 1422 | teta = pvmx[7].Ang( pvmx[3] ); |
---|
| 1423 | if (verboseLevel > 1) |
---|
| 1424 | G4cout << " vecLen > 1 && vecLen < 19 " << teta << " " << ekin0 |
---|
| 1425 | << " " << ekin1 << " " << ekin << G4endl; |
---|
| 1426 | } |
---|
| 1427 | |
---|
| 1428 | if( ekin1 != 0.0 ) |
---|
| 1429 | { |
---|
| 1430 | pvmx[6].setZero(); |
---|
| 1431 | wgt = ekin/ekin1; |
---|
| 1432 | ekin1 = 0.; |
---|
| 1433 | for( i=0; i < vecLen; i++ ) |
---|
| 1434 | { |
---|
| 1435 | pvMass = pv[i].getMass(); |
---|
| 1436 | ekin = pv[i].getKineticEnergy() * wgt; |
---|
| 1437 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 1438 | ekin1 += ekin; |
---|
| 1439 | pvmx[6].Add( pvmx[6], pv[i] ); |
---|
| 1440 | } |
---|
| 1441 | teta = pvmx[6].Ang( pvmx[3] ); |
---|
| 1442 | if (verboseLevel > 1) { |
---|
| 1443 | G4cout << " ekin1 != 0 " << teta << " " << ekin0 << " " |
---|
| 1444 | << ekin1 << G4endl; |
---|
| 1445 | incidentParticle.Print(0); |
---|
| 1446 | targetParticle.Print(1); |
---|
| 1447 | for(i=0;i<vecLen;i++) pv[i].Print(i); |
---|
| 1448 | } |
---|
| 1449 | } |
---|
| 1450 | |
---|
[1347] | 1451 | // Do some smearing in the transverse direction due to Fermi motion |
---|
[819] | 1452 | |
---|
| 1453 | G4double ry = G4UniformRand(); |
---|
| 1454 | G4double rz = G4UniformRand(); |
---|
| 1455 | G4double rx = twopi*rz; |
---|
| 1456 | G4double a1 = std::sqrt(-2.0*std::log(ry)); |
---|
| 1457 | G4double rantarg1 = a1*std::cos(rx)*0.02*targ/G4double(vecLen); |
---|
| 1458 | G4double rantarg2 = a1*std::sin(rx)*0.02*targ/G4double(vecLen); |
---|
| 1459 | |
---|
| 1460 | for (i = 0; i < vecLen; i++) |
---|
| 1461 | pv[i].setMomentum( pv[i].getMomentum().x()+rantarg1, |
---|
| 1462 | pv[i].getMomentum().y()+rantarg2 ); |
---|
| 1463 | |
---|
| 1464 | if (verboseLevel > 1) { |
---|
| 1465 | pvmx[6].setZero(); |
---|
| 1466 | for (i = 0; i < vecLen; i++) pvmx[6].Add( pvmx[6], pv[i] ); |
---|
| 1467 | teta = pvmx[6].Ang( pvmx[3] ); |
---|
| 1468 | G4cout << " After smearing " << teta << G4endl; |
---|
| 1469 | } |
---|
| 1470 | |
---|
[1347] | 1471 | // Rotate in the direction of the primary particle momentum (z-axis). |
---|
| 1472 | // This does disturb our inclusive distributions somewhat, but it is |
---|
| 1473 | // necessary for momentum conservation |
---|
[819] | 1474 | |
---|
[1347] | 1475 | // Also subtract binding energies and make some further corrections |
---|
| 1476 | // if required |
---|
[819] | 1477 | |
---|
[1347] | 1478 | G4double dekin = 0.0; |
---|
| 1479 | G4int npions = 0; |
---|
| 1480 | G4double ek1 = 0.0; |
---|
| 1481 | G4double alekw, xxh; |
---|
| 1482 | G4double cfa = 0.025*((atomicWeight-1.)/120.)*std::exp(-(atomicWeight-1.)/120.); |
---|
| 1483 | G4double alem[] = {1.40, 2.30, 2.70, 3.00, 3.40, 4.60, 7.00, 10.00}; |
---|
| 1484 | G4double val0[] = {0.00, 0.40, 0.48, 0.51, 0.54, 0.60, 0.65, 0.70}; |
---|
[819] | 1485 | |
---|
[1347] | 1486 | if (verboseLevel > 1) |
---|
| 1487 | G4cout << " Rotation in Direction of primary particle (Defs1)" << G4endl; |
---|
[819] | 1488 | |
---|
[1347] | 1489 | for (i = 0; i < vecLen; i++) { |
---|
| 1490 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 1491 | pv[i].Defs1( pv[i], pvI ); |
---|
| 1492 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 1493 | if (atomicWeight > 1.5) { |
---|
| 1494 | ekin = Amax( 1.e-6,pv[i].getKineticEnergy() - cfa*( 1. + 0.5*normal())); |
---|
| 1495 | alekw = std::log( incidentKineticEnergy ); |
---|
| 1496 | xxh = 1.; |
---|
| 1497 | if (incidentCode == pionPlusCode || incidentCode == pionMinusCode) { |
---|
| 1498 | if (pv[i].getCode() == pionZeroCode) { |
---|
| 1499 | if (G4UniformRand() < std::log(atomicWeight)) { |
---|
| 1500 | if (alekw > alem[0]) { |
---|
| 1501 | G4int jmax = 1; |
---|
| 1502 | for (j = 1; j < 8; j++) { |
---|
| 1503 | if (alekw < alem[j]) { |
---|
| 1504 | jmax = j; |
---|
| 1505 | break; |
---|
[819] | 1506 | } |
---|
| 1507 | } |
---|
[1347] | 1508 | xxh = (val0[jmax]-val0[jmax-1])/(alem[jmax]-alem[jmax-1])*alekw |
---|
| 1509 | + val0[jmax-1] - (val0[jmax]-val0[jmax-1])/(alem[jmax]-alem[jmax-1])*alem[jmax-1]; |
---|
| 1510 | xxh = 1. - xxh; |
---|
| 1511 | } |
---|
| 1512 | } |
---|
| 1513 | } |
---|
[819] | 1514 | } |
---|
[1347] | 1515 | dekin += ekin*(1.-xxh); |
---|
| 1516 | ekin *= xxh; |
---|
| 1517 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 1518 | pvCode = pv[i].getCode(); |
---|
| 1519 | if ((pvCode == pionPlusCode) || |
---|
| 1520 | (pvCode == pionMinusCode) || |
---|
| 1521 | (pvCode == pionZeroCode)) { |
---|
| 1522 | npions += 1; |
---|
| 1523 | ek1 += ekin; |
---|
[819] | 1524 | } |
---|
[1347] | 1525 | } |
---|
| 1526 | } |
---|
[819] | 1527 | |
---|
[1347] | 1528 | if ( (ek1 > 0.0) && (npions > 0) ) { |
---|
| 1529 | dekin = 1.+dekin/ek1; |
---|
| 1530 | for (i = 0; i < vecLen; i++) { |
---|
| 1531 | pvCode = pv[i].getCode(); |
---|
| 1532 | if ((pvCode == pionPlusCode) || |
---|
| 1533 | (pvCode == pionMinusCode) || |
---|
| 1534 | (pvCode == pionZeroCode)) { |
---|
| 1535 | ekin = Amax(1.0e-6, pv[i].getKineticEnergy() * dekin); |
---|
| 1536 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 1537 | } |
---|
| 1538 | } |
---|
| 1539 | } |
---|
[819] | 1540 | |
---|
[1347] | 1541 | if (verboseLevel > 1) { |
---|
| 1542 | G4cout << " Lab-System " << ek1 << " " << npions << G4endl; |
---|
| 1543 | incidentParticle.Print(0); |
---|
| 1544 | targetParticle.Print(1); |
---|
| 1545 | for (i = 0; i < vecLen; i++) pv[i].Print(i); |
---|
| 1546 | } |
---|
| 1547 | |
---|
| 1548 | // Add black track particles |
---|
| 1549 | // the total number of particles produced is restricted to 198 |
---|
| 1550 | // this may have influence on very high energies |
---|
| 1551 | |
---|
[819] | 1552 | if (verboseLevel > 1) |
---|
| 1553 | G4cout << " Evaporation : " << atomicWeight << " " |
---|
| 1554 | << excitationEnergyGNP << " " << excitationEnergyDTA << G4endl; |
---|
| 1555 | |
---|
| 1556 | G4double sprob = 0.; |
---|
| 1557 | if (incidentKineticEnergy > 5.) |
---|
| 1558 | // sprob = Amin(1., (0.394-0.063*std::log(atomicWeight))*std::log(incidentKineticEnergy-4.) ); |
---|
| 1559 | sprob = Amin(1., 0.000314*atomicWeight*std::log(incidentKineticEnergy-4.)); |
---|
| 1560 | if( atomicWeight > 1.5 && G4UniformRand() > sprob ) |
---|
| 1561 | { |
---|
| 1562 | |
---|
| 1563 | G4double cost, sint, pp, eka; |
---|
| 1564 | G4int spall(0), nbl(0); |
---|
| 1565 | |
---|
| 1566 | // first add protons and neutrons |
---|
| 1567 | |
---|
| 1568 | if( excitationEnergyGNP >= 0.001 ) |
---|
| 1569 | { |
---|
| 1570 | // nbl = number of proton/neutron black track particles |
---|
| 1571 | // tex is their total kinetic energy (GeV) |
---|
| 1572 | |
---|
| 1573 | nbl = Poisson( (1.5+1.25*targ)*excitationEnergyGNP/ |
---|
| 1574 | (excitationEnergyGNP+excitationEnergyDTA)); |
---|
| 1575 | if( targ+nbl > atomicWeight ) nbl = (int)(atomicWeight - targ); |
---|
| 1576 | if (verboseLevel > 1) |
---|
| 1577 | G4cout << " evaporation " << targ << " " << nbl << " " |
---|
| 1578 | << sprob << G4endl; |
---|
| 1579 | spall = targ; |
---|
| 1580 | if( nbl > 0) |
---|
| 1581 | { |
---|
| 1582 | ekin = (excitationEnergyGNP)/nbl; |
---|
| 1583 | ekin2 = 0.0; |
---|
| 1584 | for( i=0; i<nbl; i++ ) |
---|
| 1585 | { |
---|
| 1586 | if( G4UniformRand() < sprob ) |
---|
| 1587 | { |
---|
| 1588 | if(verboseLevel > 1) G4cout << " Particle skipped " << G4endl; |
---|
| 1589 | continue; |
---|
| 1590 | } |
---|
| 1591 | if( ekin2 > excitationEnergyGNP) break; |
---|
| 1592 | ran = G4UniformRand(); |
---|
| 1593 | ekin1 = -ekin*std::log(ran) - cfa*(1.0+0.5*normal()); |
---|
| 1594 | if (ekin1 < 0) ekin1 = -0.010*std::log(ran); |
---|
| 1595 | ekin2 += ekin1; |
---|
| 1596 | if( ekin2 > excitationEnergyGNP) |
---|
| 1597 | ekin1 = Amax( 1.0e-6, excitationEnergyGNP-(ekin2-ekin1) ); |
---|
| 1598 | if( G4UniformRand() > (1.0-atomicNumber/(atomicWeight))) |
---|
| 1599 | pv[vecLen] = Proton; |
---|
| 1600 | else |
---|
| 1601 | pv[vecLen] = Neutron; |
---|
| 1602 | spall++; |
---|
| 1603 | cost = G4UniformRand() * 2.0 - 1.0; |
---|
| 1604 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 1605 | phi = twopi * G4UniformRand(); |
---|
| 1606 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 1607 | pv[vecLen].setSide( -4 ); |
---|
| 1608 | pv[vecLen].setTOF( 1.0 ); |
---|
| 1609 | pvMass = pv[vecLen].getMass(); |
---|
| 1610 | pvEnergy = ekin1 + pvMass; |
---|
| 1611 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 1612 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 1613 | pp*sint*std::cos(phi), |
---|
| 1614 | pp*cost ); |
---|
| 1615 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 1616 | vecLen++; |
---|
| 1617 | } |
---|
| 1618 | if( (atomicWeight >= 10.0 ) && (incidentKineticEnergy <= 2.0) ) |
---|
| 1619 | { |
---|
| 1620 | G4int ika, kk = 0; |
---|
| 1621 | eka = incidentKineticEnergy; |
---|
| 1622 | if( eka > 1.0 )eka *= eka; |
---|
| 1623 | eka = Amax( 0.1, eka ); |
---|
| 1624 | ika = G4int(3.6*std::exp((atomicNumber*atomicNumber |
---|
| 1625 | /atomicWeight-35.56)/6.45)/eka); |
---|
| 1626 | if( ika > 0 ) |
---|
| 1627 | { |
---|
| 1628 | for( i=(vecLen-1); i>=0; i-- ) |
---|
| 1629 | { |
---|
| 1630 | if( (pv[i].getCode() == protonCode) && pv[i].getFlag() ) |
---|
| 1631 | { |
---|
| 1632 | pTemp = pv[i]; |
---|
| 1633 | pv[i].setDefinition("Neutron"); |
---|
| 1634 | pv[i].setMomentumAndUpdate(pTemp.getMomentum()); |
---|
| 1635 | if (verboseLevel > 1) pv[i].Print(i); |
---|
| 1636 | if( ++kk > ika ) break; |
---|
| 1637 | } |
---|
| 1638 | } |
---|
| 1639 | } |
---|
| 1640 | } |
---|
| 1641 | } |
---|
| 1642 | } |
---|
| 1643 | |
---|
| 1644 | // finished adding proton/neutron black track particles |
---|
| 1645 | // now, try to add deuterons, tritons and alphas |
---|
| 1646 | |
---|
| 1647 | if( excitationEnergyDTA >= 0.001 ) |
---|
| 1648 | { |
---|
| 1649 | nbl = Poisson( (1.5+1.25*targ)*excitationEnergyDTA |
---|
| 1650 | /(excitationEnergyGNP+excitationEnergyDTA)); |
---|
| 1651 | |
---|
| 1652 | // nbl is the number of deutrons, tritons, and alphas produced |
---|
| 1653 | |
---|
| 1654 | if (verboseLevel > 1) |
---|
| 1655 | G4cout << " evaporation " << targ << " " << nbl << " " |
---|
| 1656 | << sprob << G4endl; |
---|
| 1657 | if( nbl > 0 ) |
---|
| 1658 | { |
---|
| 1659 | ekin = excitationEnergyDTA/nbl; |
---|
| 1660 | ekin2 = 0.0; |
---|
| 1661 | for( i=0; i<nbl; i++ ) |
---|
| 1662 | { |
---|
| 1663 | if( G4UniformRand() < sprob ) |
---|
| 1664 | { |
---|
| 1665 | if(verboseLevel > 1) G4cout << " Particle skipped " << G4endl; |
---|
| 1666 | continue; |
---|
| 1667 | } |
---|
| 1668 | if( ekin2 > excitationEnergyDTA) break; |
---|
| 1669 | ran = G4UniformRand(); |
---|
| 1670 | ekin1 = -ekin*std::log(ran)-cfa*(1.+0.5*normal()); |
---|
| 1671 | if( ekin1 < 0.0 ) ekin1 = -0.010*std::log(ran); |
---|
| 1672 | ekin2 += ekin1; |
---|
| 1673 | if( ekin2 > excitationEnergyDTA) |
---|
| 1674 | ekin1 = Amax( 1.0e-6, excitationEnergyDTA-(ekin2-ekin1)); |
---|
| 1675 | cost = G4UniformRand()*2.0 - 1.0; |
---|
| 1676 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 1677 | phi = twopi*G4UniformRand(); |
---|
| 1678 | ran = G4UniformRand(); |
---|
| 1679 | if( ran <= 0.60 ) |
---|
| 1680 | pv[vecLen] = Deuteron; |
---|
| 1681 | else if (ran <= 0.90) |
---|
| 1682 | pv[vecLen] = Triton; |
---|
| 1683 | else |
---|
| 1684 | pv[vecLen] = Alpha; |
---|
| 1685 | spall += (int)(pv[vecLen].getMass() * 1.066); |
---|
| 1686 | if( spall > atomicWeight ) break; |
---|
| 1687 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 1688 | pv[vecLen].setSide( -4 ); |
---|
| 1689 | pvMass = pv[vecLen].getMass(); |
---|
| 1690 | pv[vecLen].setTOF( 1.0 ); |
---|
| 1691 | pvEnergy = pvMass + ekin1; |
---|
| 1692 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 1693 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 1694 | pp*sint*std::cos(phi), |
---|
| 1695 | pp*cost ); |
---|
| 1696 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 1697 | vecLen++; |
---|
| 1698 | } |
---|
| 1699 | } |
---|
| 1700 | } |
---|
| 1701 | } |
---|
| 1702 | if( centerOfMassEnergy <= (4.0+G4UniformRand()) ) |
---|
| 1703 | { |
---|
| 1704 | for( i=0; i<vecLen; i++ ) |
---|
| 1705 | { |
---|
| 1706 | G4double etb = pv[i].getKineticEnergy(); |
---|
| 1707 | if( etb >= incidentKineticEnergy ) |
---|
| 1708 | pv[i].setKineticEnergyAndUpdate( incidentKineticEnergy ); |
---|
| 1709 | } |
---|
| 1710 | } |
---|
| 1711 | |
---|
| 1712 | if(verboseLevel > 1) |
---|
| 1713 | { G4cout << "Call TuningOfHighEnergyCacsading vecLen = " << vecLen << G4endl; |
---|
| 1714 | incidentParticle.Print(0); |
---|
| 1715 | targetParticle.Print(1); |
---|
| 1716 | for (i=0; i<vecLen; i++) pv[i].Print(i); |
---|
| 1717 | } |
---|
| 1718 | |
---|
| 1719 | TuningOfHighEnergyCascading( pv, vecLen, |
---|
| 1720 | incidentParticle, targetParticle, |
---|
| 1721 | atomicWeight, atomicNumber); |
---|
| 1722 | |
---|
| 1723 | if(verboseLevel > 1) |
---|
| 1724 | { G4cout << " After Tuning: " << G4endl; |
---|
| 1725 | for(i=0; i<vecLen; i++) pv[i].Print(i); |
---|
| 1726 | } |
---|
| 1727 | |
---|
| 1728 | // Calculate time delay for nuclear reactions |
---|
| 1729 | |
---|
| 1730 | G4double tof = incidentTOF; |
---|
| 1731 | if( (atomicWeight >= 1.5) && (atomicWeight <= 230.0) |
---|
| 1732 | && (incidentKineticEnergy <= 0.2) ) |
---|
| 1733 | tof -= 500.0 * std::exp(-incidentKineticEnergy /0.04) * std::log( G4UniformRand() ); |
---|
| 1734 | |
---|
| 1735 | for(i=0; i<vecLen; i++) |
---|
| 1736 | { |
---|
| 1737 | if(pv[i].getName() == "KaonZero" || pv[i].getName() == "AntiKaonZero") |
---|
| 1738 | { |
---|
| 1739 | pvmx[0] = pv[i]; |
---|
| 1740 | if(G4UniformRand() < 0.5) pv[i].setDefinition("KaonZeroShort"); |
---|
| 1741 | else pv[i].setDefinition("KaonZeroLong"); |
---|
| 1742 | pv[i].setMomentumAndUpdate(pvmx[0].getMomentum()); |
---|
| 1743 | } |
---|
| 1744 | } |
---|
| 1745 | |
---|
| 1746 | successful = true; |
---|
| 1747 | delete [] pvmx; |
---|
| 1748 | G4int testCurr=0; |
---|
| 1749 | G4double totKin=0; |
---|
| 1750 | for(testCurr=0; testCurr<vecLen; testCurr++) |
---|
| 1751 | { |
---|
| 1752 | totKin+=pv[testCurr].getKineticEnergy(); |
---|
| 1753 | if(totKin>incidentKineticEnergy*1.05) |
---|
| 1754 | { |
---|
| 1755 | vecLen = testCurr; |
---|
| 1756 | break; |
---|
| 1757 | } |
---|
| 1758 | } |
---|
| 1759 | |
---|
[1347] | 1760 | return; |
---|
| 1761 | } |
---|
[819] | 1762 | |
---|
| 1763 | void |
---|
[962] | 1764 | G4HEInelastic::TuningOfHighEnergyCascading(G4HEVector pv[], |
---|
[1347] | 1765 | G4int& vecLen, |
---|
| 1766 | const G4HEVector& incidentParticle, |
---|
| 1767 | const G4HEVector& targetParticle, |
---|
[962] | 1768 | G4double atomicWeight, |
---|
| 1769 | G4double atomicNumber) |
---|
| 1770 | { |
---|
| 1771 | G4int i,j; |
---|
| 1772 | G4double incidentKineticEnergy = incidentParticle.getKineticEnergy(); |
---|
| 1773 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); |
---|
| 1774 | G4double incidentCharge = incidentParticle.getCharge(); |
---|
| 1775 | G4double incidentMass = incidentParticle.getMass(); |
---|
| 1776 | G4double targetMass = targetParticle.getMass(); |
---|
| 1777 | G4int pionPlusCode = PionPlus.getCode(); |
---|
| 1778 | G4int pionMinusCode = PionMinus.getCode(); |
---|
| 1779 | G4int pionZeroCode = PionZero.getCode(); |
---|
| 1780 | G4int protonCode = Proton.getCode(); |
---|
| 1781 | G4int neutronCode = Neutron.getCode(); |
---|
| 1782 | G4HEVector *pvmx = new G4HEVector [10]; |
---|
| 1783 | G4double *reddec = new G4double [7]; |
---|
[819] | 1784 | |
---|
[962] | 1785 | if (incidentKineticEnergy > (25.+G4UniformRand()*75.) ) { |
---|
| 1786 | G4double reden = -0.7 + 0.29*std::log10(incidentKineticEnergy); |
---|
[819] | 1787 | // G4double redat = 1.0 - 0.40*std::log10(atomicWeight); |
---|
| 1788 | // G4double redat = 0.5 - 0.18*std::log10(atomicWeight); |
---|
[962] | 1789 | G4double redat = 0.722 - 0.278*std::log10(atomicWeight); |
---|
| 1790 | G4double pmax = -200.; |
---|
| 1791 | G4double pmapim = -200.; |
---|
| 1792 | G4double pmapi0 = -200.; |
---|
| 1793 | G4double pmapip = -200.; |
---|
| 1794 | G4int ipmax = 0; |
---|
| 1795 | G4int maxpim = 0; |
---|
| 1796 | G4int maxpi0 = 0; |
---|
| 1797 | G4int maxpip = 0; |
---|
| 1798 | G4int iphmf; |
---|
[819] | 1799 | if ( (G4UniformRand() > (atomicWeight/100.-0.28)) |
---|
| 1800 | && (std::fabs(incidentCharge) > 0.) ) |
---|
| 1801 | { |
---|
| 1802 | for (i=0; i < vecLen; i++) |
---|
| 1803 | { |
---|
| 1804 | iphmf = pv[i].getCode(); |
---|
| 1805 | G4double ppp = pv[i].Length(); |
---|
| 1806 | if ( ppp > pmax) |
---|
| 1807 | { |
---|
| 1808 | pmax = ppp; ipmax = i; |
---|
| 1809 | } |
---|
| 1810 | if (iphmf == pionPlusCode && ppp > pmapip ) |
---|
| 1811 | { |
---|
| 1812 | pmapip = ppp; maxpip = i; |
---|
| 1813 | } |
---|
| 1814 | else if (iphmf == pionZeroCode && ppp > pmapi0) |
---|
| 1815 | { |
---|
| 1816 | pmapi0 = ppp; maxpi0 = i; |
---|
| 1817 | } |
---|
| 1818 | else if (iphmf == pionMinusCode && ppp > pmapim) |
---|
| 1819 | { |
---|
| 1820 | pmapim = ppp; maxpim = i; |
---|
| 1821 | } |
---|
| 1822 | } |
---|
| 1823 | } |
---|
| 1824 | if(verboseLevel > 1) |
---|
| 1825 | { |
---|
| 1826 | G4cout << "ipmax, pmax " << ipmax << " " << pmax << G4endl; |
---|
| 1827 | G4cout << "maxpip,pmapip " << maxpip << " " << pmapip << G4endl; |
---|
| 1828 | G4cout << "maxpi0,pmapi0 " << maxpi0 << " " << pmapi0 << G4endl; |
---|
| 1829 | G4cout << "maxpim,pmapim " << maxpim << " " << pmapim << G4endl; |
---|
| 1830 | } |
---|
| 1831 | |
---|
| 1832 | if ( vecLen > 2) |
---|
| 1833 | { |
---|
| 1834 | for (i=2; i<vecLen; i++) |
---|
| 1835 | { |
---|
| 1836 | iphmf = pv[i].getCode(); |
---|
| 1837 | if ( ((iphmf==protonCode)||(iphmf==neutronCode)||(pv[i].getType()=="Nucleus")) |
---|
| 1838 | && (pv[i].Length()<1.5) |
---|
| 1839 | && ((G4UniformRand()<reden)||(G4UniformRand()<redat))) |
---|
| 1840 | { |
---|
| 1841 | pv[i].setMomentumAndUpdate( 0., 0., 0.); |
---|
| 1842 | if(verboseLevel > 1) |
---|
| 1843 | { |
---|
| 1844 | G4cout << "zero Momentum for particle " << G4endl; |
---|
| 1845 | pv[i].Print(i); |
---|
| 1846 | } |
---|
| 1847 | } |
---|
| 1848 | } |
---|
| 1849 | } |
---|
| 1850 | if (maxpi0 == ipmax) |
---|
| 1851 | { |
---|
| 1852 | if (G4UniformRand() < pmapi0/incidentTotalMomentum) |
---|
| 1853 | { |
---|
| 1854 | if ((incidentCharge > 0.5) && (maxpip != 0)) |
---|
| 1855 | { |
---|
| 1856 | G4ParticleMomentum mompi0 = pv[maxpi0].getMomentum(); |
---|
| 1857 | pv[maxpi0].setMomentumAndUpdate( pv[maxpip].getMomentum() ); |
---|
| 1858 | pv[maxpip].setMomentumAndUpdate( mompi0); |
---|
| 1859 | if(verboseLevel > 1) |
---|
| 1860 | { |
---|
| 1861 | G4cout << " exchange Momentum for " << maxpi0 << " and " << maxpip << G4endl; |
---|
| 1862 | } |
---|
| 1863 | } |
---|
| 1864 | else if ((incidentCharge < -0.5) && (maxpim != 0)) |
---|
| 1865 | { |
---|
| 1866 | G4ParticleMomentum mompi0 = pv[maxpi0].getMomentum(); |
---|
| 1867 | pv[maxpi0].setMomentumAndUpdate( pv[maxpim].getMomentum() ); |
---|
| 1868 | pv[maxpim].setMomentumAndUpdate( mompi0); |
---|
| 1869 | if(verboseLevel > 1) |
---|
| 1870 | { |
---|
| 1871 | G4cout << " exchange Momentum for " << maxpi0 << " and " << maxpip << G4endl; |
---|
| 1872 | } |
---|
| 1873 | } |
---|
| 1874 | } |
---|
| 1875 | } |
---|
| 1876 | G4double bntot = - incidentParticle.getBaryonNumber() - atomicWeight; |
---|
| 1877 | for (i=0; i<vecLen; i++) bntot += pv[i].getBaryonNumber(); |
---|
| 1878 | if(atomicWeight < 1.5) { bntot = 0.; } |
---|
| 1879 | else { bntot = 1. + bntot/atomicWeight; } |
---|
| 1880 | if(atomicWeight > (75.+G4UniformRand()*50.)) bntot = 0.; |
---|
| 1881 | if(verboseLevel > 1) |
---|
| 1882 | { |
---|
| 1883 | G4cout << " Calculated Baryon- Number " << bntot << G4endl; |
---|
| 1884 | } |
---|
| 1885 | |
---|
| 1886 | j = 0; |
---|
| 1887 | for (i=0; i<vecLen; i++) |
---|
| 1888 | { |
---|
| 1889 | G4double ppp = pv[i].Length(); |
---|
| 1890 | if ( ppp > 1.e-6) |
---|
| 1891 | { |
---|
| 1892 | iphmf = pv[i].getCode(); |
---|
| 1893 | if( (bntot > 0.3) |
---|
| 1894 | && ((iphmf == protonCode) || (iphmf == neutronCode) |
---|
| 1895 | || (pv[i].getType() == "Nucleus") ) |
---|
| 1896 | && (G4UniformRand() < 0.25) |
---|
| 1897 | && (ppp < 1.2) ) |
---|
| 1898 | { |
---|
| 1899 | if(verboseLevel > 1) |
---|
| 1900 | { |
---|
| 1901 | G4cout << " skip Baryon: " << G4endl; |
---|
| 1902 | pv[i].Print(i); |
---|
| 1903 | } |
---|
| 1904 | continue; |
---|
| 1905 | |
---|
| 1906 | } |
---|
| 1907 | if (j != i) |
---|
| 1908 | { |
---|
| 1909 | pv[j] = pv[i]; |
---|
| 1910 | } |
---|
| 1911 | j++; |
---|
| 1912 | } |
---|
| 1913 | } |
---|
| 1914 | vecLen = j; |
---|
[962] | 1915 | } |
---|
[819] | 1916 | |
---|
[962] | 1917 | pvmx[0] = incidentParticle; |
---|
| 1918 | pvmx[1] = targetParticle; |
---|
| 1919 | pvmx[8].setZero(); |
---|
| 1920 | pvmx[2].Add(pvmx[0], pvmx[1]); |
---|
| 1921 | pvmx[3].Lor(pvmx[0], pvmx[2]); |
---|
| 1922 | pvmx[4].Lor(pvmx[1], pvmx[2]); |
---|
[819] | 1923 | |
---|
[962] | 1924 | if (verboseLevel > 1) { |
---|
| 1925 | pvmx[0].Print(0); |
---|
| 1926 | incidentParticle.Print(0); |
---|
| 1927 | pvmx[1].Print(1); |
---|
| 1928 | targetParticle.Print(1); |
---|
| 1929 | pvmx[2].Print(2); |
---|
| 1930 | pvmx[3].Print(3); |
---|
| 1931 | pvmx[4].Print(4); |
---|
| 1932 | } |
---|
| 1933 | |
---|
| 1934 | // Calculate leading particle effect in which a single final state |
---|
| 1935 | // particle carries away nearly the maximum allowed momentum, while |
---|
| 1936 | // all other secondaries have reduced momentum. A secondary is |
---|
| 1937 | // proportionately less likely to be a leading particle as the |
---|
| 1938 | // difference of its quantum numbers with the primary increases. |
---|
[819] | 1939 | |
---|
[962] | 1940 | G4int ledpar = -1; |
---|
| 1941 | G4double redpar = 0.; |
---|
| 1942 | G4int incidentS = incidentParticle.getStrangenessNumber(); |
---|
| 1943 | if (incidentParticle.getName() == "KaonZeroShort" || |
---|
| 1944 | incidentParticle.getName() == "KaonZeroLong") { |
---|
| 1945 | if(G4UniformRand() < 0.5) { |
---|
| 1946 | incidentS = 1; |
---|
| 1947 | } else { |
---|
| 1948 | incidentS = -1; |
---|
| 1949 | } |
---|
| 1950 | } |
---|
[819] | 1951 | |
---|
[962] | 1952 | G4int incidentB = incidentParticle.getBaryonNumber(); |
---|
[819] | 1953 | |
---|
[962] | 1954 | for (i=0; i<vecLen; i++) { |
---|
| 1955 | G4int iphmf = pv[i].getCode(); |
---|
| 1956 | G4double ppp = pv[i].Length(); |
---|
[819] | 1957 | |
---|
[962] | 1958 | if (ppp > 1.e-3) { |
---|
| 1959 | pvmx[5].Lor( pv[i], pvmx[2] ); // secondary in CM frame |
---|
| 1960 | G4double cost = pvmx[3].CosAng( pvmx[5] ); |
---|
[819] | 1961 | |
---|
[962] | 1962 | // For each secondary, find the sum of the differences of its |
---|
| 1963 | // quantum numbers with that of the incident particle |
---|
| 1964 | // (dM + dQ + dS + dB) |
---|
[819] | 1965 | |
---|
[962] | 1966 | G4int particleS = pv[i].getStrangenessNumber(); |
---|
| 1967 | |
---|
| 1968 | if (pv[i].getName() == "KaonZeroShort" || |
---|
| 1969 | pv[i].getName() == "KaonZeroLong") { |
---|
| 1970 | if (G4UniformRand() < 0.5) { |
---|
| 1971 | particleS = 1; |
---|
| 1972 | } else { |
---|
| 1973 | particleS = -1; |
---|
| 1974 | } |
---|
| 1975 | } |
---|
| 1976 | G4int particleB = pv[i].getBaryonNumber(); |
---|
| 1977 | G4double hfmass; |
---|
| 1978 | if (cost > 0.) { |
---|
| 1979 | reddec[0] = std::fabs( incidentMass - pv[i].getMass() ); |
---|
| 1980 | reddec[1] = std::fabs( incidentCharge - pv[i].getCharge()); |
---|
| 1981 | reddec[2] = std::fabs( G4double(incidentS - particleS) ); // cast for aCC |
---|
| 1982 | reddec[3] = std::fabs( G4double(incidentB - particleB) ); // cast for aCC |
---|
| 1983 | hfmass = incidentMass; |
---|
| 1984 | |
---|
| 1985 | } else { |
---|
| 1986 | reddec[0] = std::fabs( targetMass - pv[i].getMass() ); |
---|
| 1987 | reddec[1] = std::fabs( atomicNumber/atomicWeight - pv[i].getCharge()); |
---|
| 1988 | reddec[2] = std::fabs( G4double(particleS) ); // cast for aCC |
---|
| 1989 | reddec[3] = std::fabs( 1. - particleB ); |
---|
| 1990 | hfmass = targetMass; |
---|
| 1991 | } |
---|
| 1992 | |
---|
| 1993 | reddec[5] = reddec[0]+reddec[1]+reddec[2]+reddec[3]; |
---|
| 1994 | G4double sbqwgt = reddec[5]; |
---|
| 1995 | if (hfmass < 0.2) { |
---|
| 1996 | sbqwgt = (sbqwgt-2.5)*0.10; |
---|
| 1997 | if(pv[i].getCode() == pionZeroCode) sbqwgt = 0.15; |
---|
| 1998 | } else if (hfmass < 0.6) { |
---|
| 1999 | sbqwgt = (sbqwgt-3.0)*0.10; |
---|
| 2000 | } else { |
---|
| 2001 | sbqwgt = (sbqwgt-2.0)*0.10; |
---|
| 2002 | if(pv[i].getCode() == pionZeroCode) sbqwgt = 0.15; |
---|
| 2003 | } |
---|
| 2004 | |
---|
| 2005 | ppp = pvmx[5].Length(); |
---|
| 2006 | |
---|
| 2007 | // Reduce the longitudinal momentum of the secondary by a factor |
---|
| 2008 | // which is a function of the sum of the differences |
---|
| 2009 | |
---|
| 2010 | if (sbqwgt > 0. && ppp > 1.e-6) { |
---|
| 2011 | G4double pthmf = ppp*std::sqrt(1.-cost*cost); |
---|
| 2012 | G4double plhmf = ppp*cost*(1.-sbqwgt); |
---|
| 2013 | pvmx[7].Cross( pvmx[3], pvmx[5] ); |
---|
| 2014 | pvmx[7].Cross( pvmx[7], pvmx[3] ); |
---|
| 2015 | |
---|
| 2016 | if (pvmx[3].Length() > 0.) |
---|
| 2017 | pvmx[6].SmulAndUpdate( pvmx[3], plhmf/pvmx[3].Length() ); |
---|
| 2018 | else if(verboseLevel > 1) |
---|
| 2019 | G4cout << "NaNQ in Tuning of High Energy Hadronic Interactions" << G4endl; |
---|
| 2020 | |
---|
| 2021 | if (pvmx[7].Length() > 0.) |
---|
| 2022 | pvmx[7].SmulAndUpdate( pvmx[7], pthmf/pvmx[7].Length() ); |
---|
| 2023 | else if(verboseLevel > 1) |
---|
| 2024 | G4cout << "NaNQ in Tuning of High Energy Hadronic Interactions" << G4endl; |
---|
| 2025 | |
---|
| 2026 | pvmx[5].Add3(pvmx[6], pvmx[7] ); |
---|
| 2027 | pvmx[5].setEnergy( std::sqrt(sqr(pvmx[5].Length()) + sqr(pv[i].getMass()))); |
---|
| 2028 | pv[i].Lor( pvmx[5], pvmx[4] ); |
---|
| 2029 | if (verboseLevel > 1) { |
---|
| 2030 | G4cout << " Particle Momentum changed to: " << G4endl; |
---|
| 2031 | pv[i].Print(i); |
---|
| 2032 | } |
---|
| 2033 | } |
---|
| 2034 | |
---|
| 2035 | // Choose leading particle |
---|
| 2036 | // Neither pi0s, backward nucleons from intra-nuclear cascade, |
---|
| 2037 | // nor evaporation fragments can be leading particles |
---|
| 2038 | |
---|
| 2039 | G4int ss = -3; |
---|
| 2040 | if (incidentS != 0) ss = 0; |
---|
| 2041 | if (iphmf != pionZeroCode && pv[i].getSide() > ss) { |
---|
| 2042 | pvmx[7].Sub3( incidentParticle, pv[i] ); |
---|
| 2043 | reddec[4] = pvmx[7].Length()/incidentTotalMomentum; |
---|
| 2044 | reddec[6] = reddec[4]*2./3. + reddec[5]/12.; |
---|
| 2045 | reddec[6] = Amax(0., 1. - reddec[6]); |
---|
| 2046 | if ( (reddec[5] <= 3.75) && (reddec[6] > redpar) ) { |
---|
| 2047 | ledpar = i; |
---|
| 2048 | redpar = reddec[6]; |
---|
| 2049 | } |
---|
| 2050 | } |
---|
| 2051 | } |
---|
| 2052 | pvmx[8].Add3(pvmx[8], pv[i] ); |
---|
| 2053 | } |
---|
| 2054 | |
---|
[819] | 2055 | if(false) if (ledpar >= 0) |
---|
| 2056 | { |
---|
| 2057 | if(verboseLevel > 1) |
---|
| 2058 | { |
---|
| 2059 | G4cout << " Leading Particle found : " << ledpar << G4endl; |
---|
| 2060 | pv[ledpar].Print(ledpar); |
---|
| 2061 | pvmx[8].Print(-2); |
---|
| 2062 | incidentParticle.Print(-1); |
---|
| 2063 | } |
---|
| 2064 | pvmx[4].Sub3(incidentParticle,pvmx[8]); |
---|
| 2065 | pvmx[5].Smul(incidentParticle, incidentParticle.CosAng(pvmx[4]) |
---|
| 2066 | *pvmx[4].Length()/incidentParticle.Length()); |
---|
| 2067 | pv[ledpar].Add3(pv[ledpar],pvmx[5]); |
---|
| 2068 | |
---|
| 2069 | pv[ledpar].SmulAndUpdate( pv[ledpar], 1.); |
---|
| 2070 | if(verboseLevel > 1) |
---|
| 2071 | { |
---|
| 2072 | pv[ledpar].Print(ledpar); |
---|
| 2073 | } |
---|
| 2074 | } |
---|
[962] | 2075 | |
---|
| 2076 | if (conserveEnergy) { |
---|
[819] | 2077 | G4double ekinhf = 0.; |
---|
[962] | 2078 | for (i=0; i<vecLen; i++) { |
---|
[819] | 2079 | ekinhf += pv[i].getKineticEnergy(); |
---|
| 2080 | if(pv[i].getMass() < 0.7) ekinhf += pv[i].getMass(); |
---|
| 2081 | } |
---|
| 2082 | if(incidentParticle.getMass() < 0.7) ekinhf -= incidentParticle.getMass(); |
---|
[962] | 2083 | |
---|
| 2084 | if(ledpar < 0) { // no leading particle chosen |
---|
[819] | 2085 | ekinhf = incidentParticle.getKineticEnergy()/ekinhf; |
---|
[962] | 2086 | for (i=0; i<vecLen; i++) |
---|
| 2087 | pv[i].setKineticEnergyAndUpdate(ekinhf*pv[i].getKineticEnergy()); |
---|
| 2088 | |
---|
| 2089 | } else { |
---|
| 2090 | // take the energy removed from non-leading particles and |
---|
| 2091 | // give it to the leading particle |
---|
[819] | 2092 | ekinhf = incidentParticle.getKineticEnergy() - ekinhf; |
---|
| 2093 | ekinhf += pv[ledpar].getKineticEnergy(); |
---|
| 2094 | if(ekinhf < 0.) ekinhf = 0.; |
---|
| 2095 | pv[ledpar].setKineticEnergyAndUpdate(ekinhf); |
---|
| 2096 | } |
---|
[962] | 2097 | } |
---|
| 2098 | |
---|
[819] | 2099 | delete [] reddec; |
---|
| 2100 | delete [] pvmx; |
---|
[962] | 2101 | |
---|
[819] | 2102 | return; |
---|
| 2103 | } |
---|
| 2104 | |
---|
| 2105 | void |
---|
[1347] | 2106 | G4HEInelastic::HighEnergyClusterProduction(G4bool& successful, |
---|
[819] | 2107 | G4HEVector pv[], |
---|
[1347] | 2108 | G4int& vecLen, |
---|
| 2109 | G4double& excitationEnergyGNP, |
---|
| 2110 | G4double& excitationEnergyDTA, |
---|
| 2111 | const G4HEVector& incidentParticle, |
---|
| 2112 | const G4HEVector& targetParticle, |
---|
[819] | 2113 | G4double atomicWeight, |
---|
| 2114 | G4double atomicNumber) |
---|
[1347] | 2115 | { |
---|
[819] | 2116 | // For low multiplicity in the first intranuclear interaction the cascading process |
---|
| 2117 | // as described in G4HEInelastic::MediumEnergyCascading does not work |
---|
| 2118 | // satisfactorily. From experimental data it is strongly suggested to use |
---|
| 2119 | // a two- body resonance model. |
---|
| 2120 | // |
---|
| 2121 | // All quantities on the G4HEVector Array pv are in GeV- units. |
---|
| 2122 | |
---|
[1347] | 2123 | G4int protonCode = Proton.getCode(); |
---|
| 2124 | G4double protonMass = Proton.getMass(); |
---|
| 2125 | G4int neutronCode = Neutron.getCode(); |
---|
| 2126 | G4double kaonPlusMass = KaonPlus.getMass(); |
---|
| 2127 | G4int pionPlusCode = PionPlus.getCode(); |
---|
| 2128 | G4int pionZeroCode = PionZero.getCode(); |
---|
| 2129 | G4int pionMinusCode = PionMinus.getCode(); |
---|
| 2130 | G4String mesonType = PionPlus.getType(); |
---|
| 2131 | G4String baryonType = Proton.getType(); |
---|
| 2132 | G4String antiBaryonType = AntiProton.getType(); |
---|
[819] | 2133 | |
---|
[1347] | 2134 | G4double targetMass = targetParticle.getMass(); |
---|
[819] | 2135 | |
---|
| 2136 | G4int incidentCode = incidentParticle.getCode(); |
---|
| 2137 | G4double incidentMass = incidentParticle.getMass(); |
---|
| 2138 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); |
---|
| 2139 | G4double incidentEnergy = incidentParticle.getEnergy(); |
---|
| 2140 | G4double incidentKineticEnergy = incidentParticle.getKineticEnergy(); |
---|
| 2141 | G4String incidentType = incidentParticle.getType(); |
---|
| 2142 | // G4double incidentTOF = incidentParticle.getTOF(); |
---|
| 2143 | G4double incidentTOF = 0.; |
---|
| 2144 | |
---|
[1347] | 2145 | // some local variables |
---|
| 2146 | G4int i, j; |
---|
[819] | 2147 | |
---|
[1347] | 2148 | if (verboseLevel > 1) |
---|
| 2149 | G4cout << " G4HEInelastic::HighEnergyClusterProduction " << G4endl; |
---|
[819] | 2150 | |
---|
[1347] | 2151 | successful = false; |
---|
| 2152 | if (incidentTotalMomentum < 25. + G4UniformRand()*25.) return; |
---|
[819] | 2153 | |
---|
[1347] | 2154 | G4double centerOfMassEnergy = std::sqrt( sqr(incidentMass) + sqr(targetMass) |
---|
| 2155 | +2.*targetMass*incidentEnergy); |
---|
[819] | 2156 | |
---|
[1347] | 2157 | G4HEVector pvI = incidentParticle; // for the incident particle |
---|
| 2158 | pvI.setSide(1); |
---|
[819] | 2159 | |
---|
[1347] | 2160 | G4HEVector pvT = targetParticle; // for the target particle |
---|
| 2161 | pvT.setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 2162 | pvT.setSide( -1 ); |
---|
| 2163 | pvT.setTOF( -1.); |
---|
| 2164 | // distribute particles in forward and backward |
---|
| 2165 | // hemispheres. Note that only low multiplicity |
---|
| 2166 | // events from FirstIntInNuc.... should go into |
---|
| 2167 | // this routine. |
---|
| 2168 | G4int targ = 0; |
---|
| 2169 | G4int ifor = 0; |
---|
| 2170 | G4int iback = 0; |
---|
| 2171 | G4int pvCode; |
---|
| 2172 | G4double pvMass, pvEnergy; |
---|
[819] | 2173 | |
---|
[1347] | 2174 | pv[0].setSide(1); |
---|
| 2175 | pv[1].setSide(-1); |
---|
| 2176 | for (i = 0; i < vecLen; i++) { |
---|
| 2177 | if (i > 1) { |
---|
| 2178 | if (G4UniformRand() < 0.5) { |
---|
| 2179 | pv[i].setSide( 1 ); |
---|
| 2180 | if (++ifor > 18) { |
---|
| 2181 | pv[i].setSide(-1); |
---|
| 2182 | ifor--; |
---|
| 2183 | iback++; |
---|
| 2184 | } |
---|
| 2185 | } else { |
---|
| 2186 | pv[i].setSide( -1 ); |
---|
| 2187 | if (++iback > 18) { |
---|
| 2188 | pv[i].setSide(1); |
---|
| 2189 | ifor++; |
---|
| 2190 | iback--; |
---|
| 2191 | } |
---|
| 2192 | } |
---|
| 2193 | } |
---|
[819] | 2194 | |
---|
[1347] | 2195 | pvCode = pv[i].getCode(); |
---|
[819] | 2196 | |
---|
[1347] | 2197 | if ( ( (incidentCode == protonCode) || (incidentCode == neutronCode) |
---|
| 2198 | || (incidentType == mesonType) ) |
---|
| 2199 | && ( (pvCode == pionPlusCode) || (pvCode == pionMinusCode) ) |
---|
| 2200 | && ( (G4UniformRand() < (10.-incidentTotalMomentum)/6.) ) |
---|
| 2201 | && ( (G4UniformRand() < atomicWeight/300.) ) ) { |
---|
| 2202 | if (G4UniformRand() > atomicNumber/atomicWeight) |
---|
| 2203 | pv[i].setDefinition("Neutron"); |
---|
| 2204 | else |
---|
| 2205 | pv[i].setDefinition("Proton"); |
---|
| 2206 | targ++; |
---|
| 2207 | } |
---|
| 2208 | pv[i].setTOF( incidentTOF ); |
---|
| 2209 | } |
---|
[819] | 2210 | |
---|
[1347] | 2211 | G4double tb = 2. * iback; |
---|
| 2212 | if (centerOfMassEnergy < (2+G4UniformRand())) tb = (2.*iback + vecLen)/2.; |
---|
| 2213 | |
---|
| 2214 | G4double nucsup[] = {1.0, 0.7, 0.5, 0.4, 0.35, 0.3}; |
---|
| 2215 | G4double psup[] = {3. , 6. , 20., 50., 100.,1000.}; |
---|
| 2216 | G4double s = centerOfMassEnergy*centerOfMassEnergy; |
---|
[819] | 2217 | |
---|
[1347] | 2218 | G4double xtarg = Amax(0.01, Amin(0.50, 0.312+0.2*std::log(std::log(s))+std::pow(s,1.5)/6000.) |
---|
[819] | 2219 | * (std::pow(atomicWeight,0.33)-1.) * tb); |
---|
[1347] | 2220 | G4int momentumBin = 0; |
---|
[819] | 2221 | while( (momentumBin < 6) && (incidentTotalMomentum > psup[momentumBin])) momentumBin++; |
---|
| 2222 | momentumBin = Imin(5, momentumBin); |
---|
| 2223 | G4double xpnhmf = Amax(0.01,xtarg*nucsup[momentumBin]); |
---|
| 2224 | G4double xshhmf = Amax(0.01,xtarg-xpnhmf); |
---|
| 2225 | G4double rshhmf = 0.25*xshhmf; |
---|
| 2226 | G4double rpnhmf = 0.81*xpnhmf; |
---|
| 2227 | G4double xhmf; |
---|
| 2228 | G4int nshhmf, npnhmf; |
---|
| 2229 | if (rshhmf > 1.1) |
---|
| 2230 | { |
---|
| 2231 | rshhmf = xshhmf/(rshhmf-1.); |
---|
| 2232 | if (rshhmf <= 20.) |
---|
| 2233 | xhmf = GammaRand( rshhmf ); |
---|
| 2234 | else |
---|
| 2235 | xhmf = Erlang( G4int(rshhmf+0.5) ); |
---|
| 2236 | xshhmf *= xhmf/rshhmf; |
---|
| 2237 | } |
---|
| 2238 | nshhmf = Poisson( xshhmf ); |
---|
| 2239 | if (rpnhmf > 1.1) |
---|
| 2240 | { |
---|
| 2241 | rpnhmf = xpnhmf/(rpnhmf -1.); |
---|
| 2242 | if (rpnhmf <= 20.) |
---|
| 2243 | xhmf = GammaRand( rpnhmf ); |
---|
| 2244 | else |
---|
| 2245 | xhmf = Erlang( G4int(rpnhmf+0.5) ); |
---|
| 2246 | xpnhmf *= xhmf/rpnhmf; |
---|
| 2247 | } |
---|
| 2248 | npnhmf = Poisson( xpnhmf ); |
---|
| 2249 | |
---|
| 2250 | while (npnhmf > 0) |
---|
| 2251 | { |
---|
| 2252 | if ( G4UniformRand() > (1. - atomicNumber/atomicWeight)) |
---|
| 2253 | pv[vecLen].setDefinition( "Proton" ); |
---|
| 2254 | else |
---|
| 2255 | pv[vecLen].setDefinition( "Neutron" ); |
---|
| 2256 | targ++; |
---|
| 2257 | pv[vecLen].setSide( -2 ); |
---|
| 2258 | pv[vecLen].setFlag( true ); |
---|
| 2259 | pv[vecLen].setTOF( incidentTOF ); |
---|
| 2260 | vecLen++; |
---|
| 2261 | npnhmf--; |
---|
| 2262 | } |
---|
| 2263 | while (nshhmf > 0) |
---|
| 2264 | { |
---|
| 2265 | G4double ran = G4UniformRand(); |
---|
| 2266 | if (ran < 0.333333 ) |
---|
| 2267 | pv[vecLen].setDefinition( "PionPlus" ); |
---|
| 2268 | else if (ran < 0.6667) |
---|
| 2269 | pv[vecLen].setDefinition( "PionZero" ); |
---|
| 2270 | else |
---|
| 2271 | pv[vecLen].setDefinition( "PionMinus" ); |
---|
| 2272 | pv[vecLen].setSide( -2 ); |
---|
| 2273 | pv[vecLen].setFlag( true ); |
---|
| 2274 | pv[vecLen].setTOF( incidentTOF ); |
---|
| 2275 | vecLen++; |
---|
| 2276 | nshhmf--; |
---|
| 2277 | } |
---|
| 2278 | |
---|
| 2279 | // Mark leading particles for incident strange particles |
---|
| 2280 | // and antibaryons, for all other we assume that the first |
---|
| 2281 | // and second particle are the leading particles. |
---|
| 2282 | // We need this later for kinematic aspects of strangeness conservation. |
---|
| 2283 | |
---|
| 2284 | G4int lead = 0; |
---|
| 2285 | G4HEVector leadParticle; |
---|
| 2286 | if( (incidentMass >= kaonPlusMass-0.05) && (incidentCode != protonCode) |
---|
| 2287 | && (incidentCode != neutronCode) ) |
---|
| 2288 | { |
---|
| 2289 | G4double pMass = pv[0].getMass(); |
---|
| 2290 | G4int pCode = pv[0].getCode(); |
---|
| 2291 | if( (pMass >= kaonPlusMass-0.05) && (pCode != protonCode) |
---|
| 2292 | && (pCode != neutronCode) ) |
---|
| 2293 | { |
---|
| 2294 | lead = pCode; |
---|
| 2295 | leadParticle = pv[0]; |
---|
| 2296 | } |
---|
| 2297 | else |
---|
| 2298 | { |
---|
| 2299 | pMass = pv[1].getMass(); |
---|
| 2300 | pCode = pv[1].getCode(); |
---|
| 2301 | if( (pMass >= kaonPlusMass-0.05) && (pCode != protonCode) |
---|
| 2302 | && (pCode != neutronCode) ) |
---|
| 2303 | { |
---|
| 2304 | lead = pCode; |
---|
| 2305 | leadParticle = pv[1]; |
---|
| 2306 | } |
---|
| 2307 | } |
---|
| 2308 | } |
---|
| 2309 | |
---|
| 2310 | if (verboseLevel > 1) |
---|
| 2311 | { G4cout << " pv Vector after initialization " << vecLen << G4endl; |
---|
| 2312 | pvI.Print(-1); |
---|
| 2313 | pvT.Print(-1); |
---|
| 2314 | for (i=0; i < vecLen ; i++) pv[i].Print(i); |
---|
| 2315 | } |
---|
| 2316 | |
---|
| 2317 | G4double tavai = 0.; |
---|
| 2318 | for(i=0;i<vecLen;i++) if(pv[i].getSide() != -2) tavai += pv[i].getMass(); |
---|
| 2319 | |
---|
| 2320 | while (tavai > centerOfMassEnergy) |
---|
| 2321 | { |
---|
| 2322 | for (i=vecLen-1; i >= 0; i--) |
---|
| 2323 | { |
---|
| 2324 | if (pv[i].getSide() != -2) |
---|
| 2325 | { |
---|
| 2326 | tavai -= pv[i].getMass(); |
---|
| 2327 | if( i != vecLen-1) |
---|
| 2328 | { |
---|
| 2329 | for (j=i; j < vecLen; j++) |
---|
| 2330 | { |
---|
| 2331 | pv[j] = pv[j+1]; |
---|
| 2332 | } |
---|
| 2333 | } |
---|
| 2334 | if ( --vecLen < 2) |
---|
| 2335 | { |
---|
| 2336 | successful = false; |
---|
| 2337 | return; |
---|
| 2338 | } |
---|
| 2339 | break; |
---|
| 2340 | } |
---|
| 2341 | } |
---|
| 2342 | } |
---|
| 2343 | |
---|
| 2344 | // Now produce 3 Clusters: |
---|
| 2345 | // 1. forward cluster |
---|
| 2346 | // 2. backward meson cluster |
---|
| 2347 | // 3. backward nucleon cluster |
---|
| 2348 | |
---|
| 2349 | G4double rmc0 = 0., rmd0 = 0., rme0 = 0.; |
---|
| 2350 | G4int ntc = 0, ntd = 0, nte = 0; |
---|
| 2351 | |
---|
| 2352 | for (i=0; i < vecLen; i++) |
---|
| 2353 | { |
---|
| 2354 | if(pv[i].getSide() > 0) |
---|
| 2355 | { |
---|
| 2356 | if(ntc < 17) |
---|
| 2357 | { |
---|
| 2358 | rmc0 += pv[i].getMass(); |
---|
| 2359 | ntc++; |
---|
| 2360 | } |
---|
| 2361 | else |
---|
| 2362 | { |
---|
| 2363 | if(ntd < 17) |
---|
| 2364 | { |
---|
| 2365 | pv[i].setSide(-1); |
---|
| 2366 | rmd0 += pv[i].getMass(); |
---|
| 2367 | ntd++; |
---|
| 2368 | } |
---|
| 2369 | else |
---|
| 2370 | { |
---|
| 2371 | pv[i].setSide(-2); |
---|
| 2372 | rme0 += pv[i].getMass(); |
---|
| 2373 | nte++; |
---|
| 2374 | } |
---|
| 2375 | } |
---|
| 2376 | } |
---|
| 2377 | else if (pv[i].getSide() == -1) |
---|
| 2378 | { |
---|
| 2379 | if(ntd < 17) |
---|
| 2380 | { |
---|
| 2381 | rmd0 += pv[i].getMass(); |
---|
| 2382 | ntd++; |
---|
| 2383 | } |
---|
| 2384 | else |
---|
| 2385 | { |
---|
| 2386 | pv[i].setSide(-2); |
---|
| 2387 | rme0 += pv[i].getMass(); |
---|
| 2388 | nte++; |
---|
| 2389 | } |
---|
| 2390 | } |
---|
| 2391 | else |
---|
| 2392 | { |
---|
| 2393 | rme0 += pv[i].getMass(); |
---|
| 2394 | nte++; |
---|
| 2395 | } |
---|
| 2396 | } |
---|
| 2397 | |
---|
| 2398 | G4double cpar[] = {0.6, 0.6, 0.35, 0.15, 0.10}; |
---|
| 2399 | G4double gpar[] = {2.6, 2.6, 1.80, 1.30, 1.20}; |
---|
| 2400 | |
---|
| 2401 | G4double rmc = rmc0, rmd = rmd0, rme = rme0; |
---|
| 2402 | G4int ntc1 = Imin(4,ntc-1); |
---|
| 2403 | G4int ntd1 = Imin(4,ntd-1); |
---|
| 2404 | G4int nte1 = Imin(4,nte-1); |
---|
| 2405 | if (ntc > 1) rmc = rmc0 + std::pow(-std::log(1.-G4UniformRand()),cpar[ntc1])/gpar[ntc1]; |
---|
| 2406 | if (ntd > 1) rmd = rmd0 + std::pow(-std::log(1.-G4UniformRand()),cpar[ntd1])/gpar[ntd1]; |
---|
| 2407 | if (nte > 1) rme = rme0 + std::pow(-std::log(1.-G4UniformRand()),cpar[nte1])/gpar[nte1]; |
---|
| 2408 | while( (rmc+rmd) > centerOfMassEnergy) |
---|
| 2409 | { |
---|
| 2410 | if ((rmc == rmc0) && (rmd == rmd0)) |
---|
| 2411 | { |
---|
| 2412 | rmd *= 0.999*centerOfMassEnergy/(rmc+rmd); |
---|
| 2413 | rmc *= 0.999*centerOfMassEnergy/(rmc+rmd); |
---|
| 2414 | } |
---|
| 2415 | else |
---|
| 2416 | { |
---|
| 2417 | rmc = 0.1*rmc0 + 0.9*rmc; |
---|
| 2418 | rmd = 0.1*rmd0 + 0.9*rmd; |
---|
| 2419 | } |
---|
| 2420 | } |
---|
| 2421 | if(verboseLevel > 1) |
---|
| 2422 | G4cout << " Cluster Masses: " << ntc << " " << rmc << " " << ntd |
---|
| 2423 | << " " << rmd << " " << nte << " " << rme << G4endl; |
---|
| 2424 | |
---|
| 2425 | G4HEVector* pvmx = new G4HEVector[11]; |
---|
| 2426 | |
---|
| 2427 | pvmx[1].setMass( incidentMass); |
---|
| 2428 | pvmx[1].setMomentumAndUpdate( 0., 0., incidentTotalMomentum); |
---|
| 2429 | pvmx[2].setMass( targetMass); |
---|
| 2430 | pvmx[2].setMomentumAndUpdate( 0., 0., 0.); |
---|
| 2431 | pvmx[0].Add( pvmx[1], pvmx[2] ); |
---|
| 2432 | pvmx[1].Lor( pvmx[1], pvmx[0] ); |
---|
| 2433 | pvmx[2].Lor( pvmx[2], pvmx[0] ); |
---|
| 2434 | |
---|
| 2435 | G4double pf = std::sqrt(Amax(0.0001, sqr(sqr(centerOfMassEnergy) + rmd*rmd -rmc*rmc) |
---|
| 2436 | - 4*sqr(centerOfMassEnergy)*rmd*rmd))/(2.*centerOfMassEnergy); |
---|
| 2437 | pvmx[3].setMass( rmc ); |
---|
| 2438 | pvmx[4].setMass( rmd ); |
---|
| 2439 | pvmx[3].setEnergy( std::sqrt(pf*pf + rmc*rmc) ); |
---|
| 2440 | pvmx[4].setEnergy( std::sqrt(pf*pf + rmd*rmd) ); |
---|
| 2441 | |
---|
| 2442 | G4double tvalue = -MAXFLOAT; |
---|
| 2443 | G4double bvalue = Amax(0.01, 4.0 + 1.6*std::log(incidentTotalMomentum)); |
---|
| 2444 | if (bvalue != 0.0) tvalue = std::log(G4UniformRand())/bvalue; |
---|
| 2445 | G4double pin = pvmx[1].Length(); |
---|
| 2446 | G4double tacmin = sqr( pvmx[1].getEnergy() - pvmx[3].getEnergy()) - sqr( pin - pf); |
---|
| 2447 | G4double ctet = Amax(-1., Amin(1., 1.+2.*(tvalue-tacmin)/Amax(1.e-10, 4.*pin*pf))); |
---|
| 2448 | G4double stet = std::sqrt(Amax(0., 1.0 - ctet*ctet)); |
---|
| 2449 | G4double phi = twopi * G4UniformRand(); |
---|
| 2450 | pvmx[3].setMomentum( pf * stet * std::sin(phi), |
---|
| 2451 | pf * stet * std::cos(phi), |
---|
| 2452 | pf * ctet ); |
---|
| 2453 | pvmx[4].Smul( pvmx[3], -1.); |
---|
| 2454 | |
---|
| 2455 | if (nte > 0) |
---|
| 2456 | { |
---|
| 2457 | G4double ekit1 = 0.04; |
---|
| 2458 | G4double ekit2 = 0.6; |
---|
| 2459 | G4double gaval = 1.2; |
---|
| 2460 | if (incidentKineticEnergy <= 5.) |
---|
| 2461 | { |
---|
| 2462 | ekit1 *= sqr(incidentKineticEnergy)/25.; |
---|
| 2463 | ekit2 *= sqr(incidentKineticEnergy)/25.; |
---|
| 2464 | } |
---|
| 2465 | G4double avalue = (1.-gaval)/(std::pow(ekit2, 1.-gaval)-std::pow(ekit1, 1.-gaval)); |
---|
| 2466 | for (i=0; i < vecLen; i++) |
---|
| 2467 | { |
---|
| 2468 | if (pv[i].getSide() == -2) |
---|
| 2469 | { |
---|
| 2470 | G4double ekit = std::pow(G4UniformRand()*(1.-gaval)/avalue +std::pow(ekit1, 1.-gaval), |
---|
| 2471 | 1./(1.-gaval)); |
---|
| 2472 | pv[i].setKineticEnergyAndUpdate( ekit ); |
---|
| 2473 | ctet = Amax(-1., Amin(1., std::log(2.23*G4UniformRand()+0.383)/0.96)); |
---|
| 2474 | stet = std::sqrt( Amax( 0.0, 1. - ctet*ctet )); |
---|
| 2475 | phi = G4UniformRand()*twopi; |
---|
| 2476 | G4double pp = pv[i].Length(); |
---|
| 2477 | pv[i].setMomentum( pp * stet * std::sin(phi), |
---|
| 2478 | pp * stet * std::cos(phi), |
---|
| 2479 | pp * ctet ); |
---|
| 2480 | pv[i].Lor( pv[i], pvmx[0] ); |
---|
| 2481 | } |
---|
| 2482 | } |
---|
| 2483 | } |
---|
| 2484 | // pvmx[1] = pvmx[3]; |
---|
| 2485 | // pvmx[2] = pvmx[4]; |
---|
| 2486 | pvmx[5].SmulAndUpdate( pvmx[3], -1.); |
---|
| 2487 | pvmx[6].SmulAndUpdate( pvmx[4], -1.); |
---|
| 2488 | |
---|
| 2489 | if (verboseLevel > 1) { |
---|
| 2490 | G4cout << " General vectors before Phase space Generation " << G4endl; |
---|
| 2491 | for (i=0; i<7; i++) pvmx[i].Print(i); |
---|
| 2492 | } |
---|
| 2493 | |
---|
| 2494 | G4HEVector* tempV = new G4HEVector[18]; |
---|
| 2495 | G4bool constantCrossSection = true; |
---|
| 2496 | G4double wgt; |
---|
| 2497 | G4int npg; |
---|
| 2498 | |
---|
| 2499 | if (ntc > 1) |
---|
| 2500 | { |
---|
| 2501 | npg = 0; |
---|
| 2502 | for (i=0; i < vecLen; i++) |
---|
| 2503 | { |
---|
| 2504 | if (pv[i].getSide() > 0) |
---|
| 2505 | { |
---|
| 2506 | tempV[npg++] = pv[i]; |
---|
| 2507 | } |
---|
| 2508 | } |
---|
| 2509 | wgt = NBodyPhaseSpace( pvmx[3].getMass(), constantCrossSection, tempV, npg); |
---|
| 2510 | |
---|
| 2511 | npg = 0; |
---|
| 2512 | for (i=0; i < vecLen; i++) |
---|
| 2513 | { |
---|
| 2514 | if (pv[i].getSide() > 0) |
---|
| 2515 | { |
---|
| 2516 | pv[i].setMomentum( tempV[npg++].getMomentum()); |
---|
| 2517 | pv[i].SmulAndUpdate( pv[i], 1. ); |
---|
| 2518 | pv[i].Lor( pv[i], pvmx[5] ); |
---|
| 2519 | } |
---|
| 2520 | } |
---|
| 2521 | } |
---|
| 2522 | else if(ntc == 1) |
---|
| 2523 | { |
---|
| 2524 | for(i=0; i<vecLen; i++) |
---|
| 2525 | { |
---|
| 2526 | if(pv[i].getSide() > 0) pv[i].setMomentumAndUpdate(pvmx[3].getMomentum()); |
---|
| 2527 | } |
---|
| 2528 | } |
---|
| 2529 | else |
---|
| 2530 | { |
---|
| 2531 | } |
---|
| 2532 | |
---|
| 2533 | if (ntd > 1) |
---|
| 2534 | { |
---|
| 2535 | npg = 0; |
---|
| 2536 | for (i=0; i < vecLen; i++) |
---|
| 2537 | { |
---|
| 2538 | if (pv[i].getSide() == -1) |
---|
| 2539 | { |
---|
| 2540 | tempV[npg++] = pv[i]; |
---|
| 2541 | } |
---|
| 2542 | } |
---|
| 2543 | wgt = NBodyPhaseSpace( pvmx[4].getMass(), constantCrossSection, tempV, npg); |
---|
| 2544 | |
---|
| 2545 | npg = 0; |
---|
| 2546 | for (i=0; i < vecLen; i++) |
---|
| 2547 | { |
---|
| 2548 | if (pv[i].getSide() == -1) |
---|
| 2549 | { |
---|
| 2550 | pv[i].setMomentum( tempV[npg++].getMomentum()); |
---|
| 2551 | pv[i].SmulAndUpdate( pv[i], 1.); |
---|
| 2552 | pv[i].Lor( pv[i], pvmx[6] ); |
---|
| 2553 | } |
---|
| 2554 | } |
---|
| 2555 | } |
---|
| 2556 | else if(ntd == 1) |
---|
| 2557 | { |
---|
| 2558 | for(i=0; i<vecLen; i++) |
---|
| 2559 | { |
---|
| 2560 | if(pv[i].getSide() == -1) pv[i].setMomentumAndUpdate(pvmx[4].getMomentum()); |
---|
| 2561 | } |
---|
| 2562 | } |
---|
| 2563 | else |
---|
| 2564 | { |
---|
| 2565 | } |
---|
| 2566 | |
---|
| 2567 | if(verboseLevel > 1) |
---|
| 2568 | { |
---|
| 2569 | G4cout << " Vectors after PhaseSpace generation " << G4endl; |
---|
| 2570 | for(i=0; i<vecLen; i++) pv[i].Print(i); |
---|
| 2571 | } |
---|
| 2572 | |
---|
| 2573 | // Lorentz transformation in lab system |
---|
| 2574 | |
---|
| 2575 | targ = 0; |
---|
| 2576 | for( i=0; i < vecLen; i++ ) |
---|
| 2577 | { |
---|
| 2578 | if( pv[i].getType() == baryonType )targ++; |
---|
| 2579 | if( pv[i].getType() == antiBaryonType )targ--; |
---|
| 2580 | pv[i].Lor( pv[i], pvmx[2] ); |
---|
| 2581 | } |
---|
| 2582 | if (targ<1) targ = 1; |
---|
| 2583 | |
---|
| 2584 | if(verboseLevel > 1) { |
---|
| 2585 | G4cout << " Transformation in Lab- System " << G4endl; |
---|
| 2586 | for(i=0; i<vecLen; i++) pv[i].Print(i); |
---|
| 2587 | } |
---|
| 2588 | |
---|
| 2589 | G4bool dum(0); |
---|
| 2590 | G4double ekin, teta; |
---|
| 2591 | |
---|
| 2592 | if( lead ) |
---|
| 2593 | { |
---|
| 2594 | for( i=0; i<vecLen; i++ ) |
---|
| 2595 | { |
---|
| 2596 | if( pv[i].getCode() == lead ) |
---|
| 2597 | { |
---|
| 2598 | dum = false; |
---|
| 2599 | break; |
---|
| 2600 | } |
---|
| 2601 | } |
---|
| 2602 | if( dum ) |
---|
| 2603 | { |
---|
| 2604 | i = 0; |
---|
| 2605 | |
---|
| 2606 | if( ( (leadParticle.getType() == baryonType || |
---|
| 2607 | leadParticle.getType() == antiBaryonType) |
---|
| 2608 | && (pv[1].getType() == baryonType || |
---|
| 2609 | pv[1].getType() == antiBaryonType)) |
---|
| 2610 | || ( (leadParticle.getType() == mesonType) |
---|
| 2611 | && (pv[1].getType() == mesonType))) |
---|
| 2612 | { |
---|
| 2613 | i = 1; |
---|
| 2614 | } |
---|
| 2615 | |
---|
| 2616 | ekin = pv[i].getKineticEnergy(); |
---|
| 2617 | pv[i] = leadParticle; |
---|
| 2618 | if( pv[i].getFlag() ) |
---|
| 2619 | pv[i].setTOF( -1.0 ); |
---|
| 2620 | else |
---|
| 2621 | pv[i].setTOF( 1.0 ); |
---|
| 2622 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 2623 | } |
---|
| 2624 | } |
---|
| 2625 | |
---|
| 2626 | pvmx[4].setMass( incidentMass); |
---|
| 2627 | pvmx[4].setMomentumAndUpdate( 0.0, 0.0, incidentTotalMomentum ); |
---|
| 2628 | |
---|
| 2629 | G4double ekin0 = pvmx[4].getKineticEnergy(); |
---|
| 2630 | |
---|
| 2631 | pvmx[5].setMass ( protonMass * targ); |
---|
| 2632 | pvmx[5].setEnergy( protonMass * targ); |
---|
| 2633 | pvmx[5].setKineticEnergy(0.); |
---|
| 2634 | pvmx[5].setMomentum( 0.0, 0.0, 0.0 ); |
---|
| 2635 | |
---|
| 2636 | ekin = pvmx[4].getEnergy() + pvmx[5].getEnergy(); |
---|
| 2637 | |
---|
| 2638 | pvmx[6].Add( pvmx[4], pvmx[5] ); |
---|
| 2639 | pvmx[4].Lor( pvmx[4], pvmx[6] ); |
---|
| 2640 | pvmx[5].Lor( pvmx[5], pvmx[6] ); |
---|
| 2641 | |
---|
| 2642 | G4double tecm = pvmx[4].getEnergy() + pvmx[5].getEnergy(); |
---|
| 2643 | |
---|
| 2644 | pvmx[8].setZero(); |
---|
| 2645 | |
---|
| 2646 | G4double ekin1 = 0.0; |
---|
| 2647 | |
---|
| 2648 | for( i=0; i < vecLen; i++ ) |
---|
| 2649 | { |
---|
| 2650 | pvmx[8].Add( pvmx[8], pv[i] ); |
---|
| 2651 | ekin1 += pv[i].getKineticEnergy(); |
---|
| 2652 | ekin -= pv[i].getMass(); |
---|
| 2653 | } |
---|
| 2654 | |
---|
| 2655 | if( vecLen > 1 && vecLen < 19 ) |
---|
| 2656 | { |
---|
| 2657 | constantCrossSection = true; |
---|
| 2658 | G4HEVector pw[18]; |
---|
| 2659 | for(i=0;i<vecLen;i++) pw[i] = pv[i]; |
---|
| 2660 | wgt = NBodyPhaseSpace( tecm, constantCrossSection, pw, vecLen ); |
---|
| 2661 | ekin = 0.0; |
---|
| 2662 | for( i=0; i < vecLen; i++ ) |
---|
| 2663 | { |
---|
| 2664 | pvmx[7].setMass( pw[i].getMass()); |
---|
| 2665 | pvmx[7].setMomentum( pw[i].getMomentum() ); |
---|
| 2666 | pvmx[7].SmulAndUpdate( pvmx[7], 1.); |
---|
| 2667 | pvmx[7].Lor( pvmx[7], pvmx[5] ); |
---|
| 2668 | ekin += pvmx[7].getKineticEnergy(); |
---|
| 2669 | } |
---|
| 2670 | teta = pvmx[8].Ang( pvmx[4] ); |
---|
| 2671 | if (verboseLevel > 1) |
---|
| 2672 | G4cout << " vecLen > 1 && vecLen < 19 " << teta << " " |
---|
| 2673 | << ekin0 << " " << ekin1 << " " << ekin << G4endl; |
---|
| 2674 | } |
---|
| 2675 | |
---|
| 2676 | if( ekin1 != 0.0 ) |
---|
| 2677 | { |
---|
| 2678 | pvmx[7].setZero(); |
---|
| 2679 | wgt = ekin/ekin1; |
---|
| 2680 | ekin1 = 0.; |
---|
| 2681 | for( i=0; i < vecLen; i++ ) |
---|
| 2682 | { |
---|
| 2683 | pvMass = pv[i].getMass(); |
---|
| 2684 | ekin = pv[i].getKineticEnergy() * wgt; |
---|
| 2685 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 2686 | ekin1 += ekin; |
---|
| 2687 | pvmx[7].Add( pvmx[7], pv[i] ); |
---|
| 2688 | } |
---|
| 2689 | teta = pvmx[7].Ang( pvmx[4] ); |
---|
| 2690 | if (verboseLevel > 1) |
---|
| 2691 | G4cout << " ekin1 != 0 " << teta << " " << ekin0 << " " |
---|
| 2692 | << ekin1 << G4endl; |
---|
| 2693 | } |
---|
| 2694 | |
---|
| 2695 | if(verboseLevel > 1) |
---|
| 2696 | { |
---|
| 2697 | G4cout << " After energy- correction " << G4endl; |
---|
| 2698 | for(i=0; i<vecLen; i++) pv[i].Print(i); |
---|
| 2699 | } |
---|
| 2700 | |
---|
[1347] | 2701 | // Do some smearing in the transverse direction due to Fermi motion |
---|
[819] | 2702 | |
---|
[1347] | 2703 | G4double ry = G4UniformRand(); |
---|
| 2704 | G4double rz = G4UniformRand(); |
---|
| 2705 | G4double rx = twopi*rz; |
---|
| 2706 | G4double a1 = std::sqrt(-2.0*std::log(ry)); |
---|
| 2707 | G4double rantarg1 = a1*std::cos(rx)*0.02*targ/G4double(vecLen); |
---|
| 2708 | G4double rantarg2 = a1*std::sin(rx)*0.02*targ/G4double(vecLen); |
---|
[819] | 2709 | |
---|
[1347] | 2710 | for (i = 0; i < vecLen; i++) |
---|
| 2711 | pv[i].setMomentum(pv[i].getMomentum().x()+rantarg1, |
---|
| 2712 | pv[i].getMomentum().y()+rantarg2); |
---|
[819] | 2713 | |
---|
[1347] | 2714 | if (verboseLevel > 1) { |
---|
| 2715 | pvmx[7].setZero(); |
---|
| 2716 | for (i = 0; i < vecLen; i++) pvmx[7].Add( pvmx[7], pv[i] ); |
---|
| 2717 | teta = pvmx[7].Ang( pvmx[4] ); |
---|
| 2718 | G4cout << " After smearing " << teta << G4endl; |
---|
| 2719 | } |
---|
[819] | 2720 | |
---|
[1347] | 2721 | // Rotate in the direction of the primary particle momentum (z-axis). |
---|
| 2722 | // This does disturb our inclusive distributions somewhat, but it is |
---|
| 2723 | // necessary for momentum conservation |
---|
[819] | 2724 | |
---|
[1347] | 2725 | // Also subtract binding energies and make some further corrections |
---|
| 2726 | // if required |
---|
[819] | 2727 | |
---|
[1347] | 2728 | G4double dekin = 0.0; |
---|
| 2729 | G4int npions = 0; |
---|
| 2730 | G4double ek1 = 0.0; |
---|
| 2731 | G4double alekw, xxh; |
---|
| 2732 | G4double cfa = 0.025*((atomicWeight-1.)/120.)*std::exp(-(atomicWeight-1.)/120.); |
---|
| 2733 | G4double alem[] = {1.40, 2.30, 2.70, 3.00, 3.40, 4.60, 7.00, 10.0}; |
---|
| 2734 | G4double val0[] = {0.00, 0.40, 0.48, 0.51, 0.54, 0.60, 0.65, 0.70}; |
---|
[819] | 2735 | |
---|
[1347] | 2736 | for (i = 0; i < vecLen; i++) { |
---|
| 2737 | pv[i].Defs1( pv[i], pvI ); |
---|
| 2738 | if (atomicWeight > 1.5) { |
---|
| 2739 | ekin = Amax( 1.e-6,pv[i].getKineticEnergy() - cfa*( 1. + 0.5*normal())); |
---|
| 2740 | alekw = std::log( incidentKineticEnergy ); |
---|
| 2741 | xxh = 1.; |
---|
| 2742 | if (incidentCode == pionPlusCode || incidentCode == pionMinusCode) { |
---|
| 2743 | if (pv[i].getCode() == pionZeroCode) { |
---|
| 2744 | if (G4UniformRand() < std::log(atomicWeight)) { |
---|
| 2745 | if (alekw > alem[0]) { |
---|
| 2746 | G4int jmax = 1; |
---|
| 2747 | for (j = 1; j < 8; j++) { |
---|
| 2748 | if (alekw < alem[j]) { |
---|
| 2749 | jmax = j; |
---|
| 2750 | break; |
---|
[819] | 2751 | } |
---|
[1347] | 2752 | } |
---|
| 2753 | xxh = (val0[jmax]-val0[jmax-1])/(alem[jmax]-alem[jmax-1])*alekw |
---|
| 2754 | + val0[jmax-1] - (val0[jmax]-val0[jmax-1])/(alem[jmax]-alem[jmax-1])*alem[jmax-1]; |
---|
| 2755 | xxh = 1. - xxh; |
---|
| 2756 | } |
---|
| 2757 | } |
---|
| 2758 | } |
---|
[819] | 2759 | } |
---|
[1347] | 2760 | dekin += ekin*(1.-xxh); |
---|
| 2761 | ekin *= xxh; |
---|
| 2762 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 2763 | pvCode = pv[i].getCode(); |
---|
| 2764 | if ((pvCode == pionPlusCode) || |
---|
| 2765 | (pvCode == pionMinusCode) || |
---|
| 2766 | (pvCode == pionZeroCode)) { |
---|
| 2767 | npions += 1; |
---|
| 2768 | ek1 += ekin; |
---|
| 2769 | } |
---|
| 2770 | } |
---|
| 2771 | } |
---|
| 2772 | |
---|
[819] | 2773 | if( (ek1 > 0.0) && (npions > 0) ) |
---|
| 2774 | { |
---|
| 2775 | dekin = 1.+dekin/ek1; |
---|
| 2776 | for (i = 0; i < vecLen; i++) |
---|
| 2777 | { |
---|
| 2778 | pvCode = pv[i].getCode(); |
---|
| 2779 | if((pvCode == pionPlusCode) || (pvCode == pionMinusCode) || (pvCode == pionZeroCode)) |
---|
| 2780 | { |
---|
| 2781 | ekin = Amax( 1.0e-6, pv[i].getKineticEnergy() * dekin ); |
---|
| 2782 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 2783 | } |
---|
| 2784 | } |
---|
| 2785 | } |
---|
| 2786 | if (verboseLevel > 1) |
---|
| 2787 | { G4cout << " Lab-System " << ek1 << " " << npions << G4endl; |
---|
| 2788 | for (i=0; i<vecLen; i++) pv[i].Print(i); |
---|
| 2789 | } |
---|
| 2790 | |
---|
| 2791 | // Add black track particles |
---|
| 2792 | // The total number of particles produced is restricted to 198 |
---|
| 2793 | // - this may have influence on very high energies |
---|
| 2794 | |
---|
| 2795 | if (verboseLevel > 1) |
---|
| 2796 | G4cout << " Evaporation " << atomicWeight << " " << excitationEnergyGNP |
---|
| 2797 | << " " << excitationEnergyDTA << G4endl; |
---|
| 2798 | |
---|
| 2799 | G4double sprob = 0.; |
---|
| 2800 | if (incidentKineticEnergy > 5. ) |
---|
| 2801 | // sprob = Amin( 1., (0.394-0.063*std::log(atomicWeight))*std::log(incidentKineticEnergy-4.) ); |
---|
| 2802 | sprob = Amin(1., 0.000314*atomicWeight*std::log(incidentKineticEnergy-4.)); |
---|
| 2803 | if( atomicWeight > 1.5 && G4UniformRand() > sprob) |
---|
| 2804 | { |
---|
| 2805 | |
---|
| 2806 | G4double cost, sint, ekin2, ran, pp, eka; |
---|
| 2807 | G4int spall(0), nbl(0); |
---|
| 2808 | |
---|
| 2809 | // first add protons and neutrons |
---|
| 2810 | |
---|
| 2811 | if( excitationEnergyGNP >= 0.001 ) |
---|
| 2812 | { |
---|
| 2813 | // nbl = number of proton/neutron black track particles |
---|
| 2814 | // tex is their total kinetic energy (GeV) |
---|
| 2815 | |
---|
| 2816 | nbl = Poisson( (1.5+1.25*targ)*excitationEnergyGNP/ |
---|
| 2817 | (excitationEnergyGNP+excitationEnergyDTA)); |
---|
| 2818 | if( targ+nbl > atomicWeight ) nbl = (int)(atomicWeight - targ); |
---|
| 2819 | if (verboseLevel > 1) |
---|
| 2820 | G4cout << " evaporation " << targ << " " << nbl << " " |
---|
| 2821 | << sprob << G4endl; |
---|
| 2822 | spall = targ; |
---|
| 2823 | if( nbl > 0) |
---|
| 2824 | { |
---|
| 2825 | ekin = excitationEnergyGNP/nbl; |
---|
| 2826 | ekin2 = 0.0; |
---|
| 2827 | for( i=0; i<nbl; i++ ) |
---|
| 2828 | { |
---|
| 2829 | if( G4UniformRand() < sprob ) continue; |
---|
| 2830 | if( ekin2 > excitationEnergyGNP) break; |
---|
| 2831 | ran = G4UniformRand(); |
---|
| 2832 | ekin1 = -ekin*std::log(ran) - cfa*(1.0+0.5*normal()); |
---|
| 2833 | if (ekin1 < 0) ekin1 = -0.010*std::log(ran); |
---|
| 2834 | ekin2 += ekin1; |
---|
| 2835 | if( ekin2 > excitationEnergyGNP) |
---|
| 2836 | ekin1 = Amax( 1.0e-6, excitationEnergyGNP-(ekin2-ekin1) ); |
---|
| 2837 | if( G4UniformRand() > (1.0-atomicNumber/(atomicWeight))) |
---|
| 2838 | pv[vecLen].setDefinition( "Proton"); |
---|
| 2839 | else |
---|
| 2840 | pv[vecLen].setDefinition( "Neutron" ); |
---|
| 2841 | spall++; |
---|
| 2842 | cost = G4UniformRand() * 2.0 - 1.0; |
---|
| 2843 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 2844 | phi = twopi * G4UniformRand(); |
---|
| 2845 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 2846 | pv[vecLen].setSide( -4 ); |
---|
| 2847 | pvMass = pv[vecLen].getMass(); |
---|
| 2848 | pv[vecLen].setTOF( 1.0 ); |
---|
| 2849 | pvEnergy = ekin1 + pvMass; |
---|
| 2850 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 2851 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 2852 | pp*sint*std::cos(phi), |
---|
| 2853 | pp*cost ); |
---|
| 2854 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 2855 | vecLen++; |
---|
| 2856 | } |
---|
| 2857 | if( (atomicWeight >= 10.0 ) && (incidentKineticEnergy <= 2.0) ) |
---|
| 2858 | { |
---|
| 2859 | G4int ika, kk = 0; |
---|
| 2860 | eka = incidentKineticEnergy; |
---|
| 2861 | if( eka > 1.0 )eka *= eka; |
---|
| 2862 | eka = Amax( 0.1, eka ); |
---|
| 2863 | ika = G4int(3.6*std::exp((atomicNumber*atomicNumber |
---|
| 2864 | /atomicWeight-35.56)/6.45)/eka); |
---|
| 2865 | if( ika > 0 ) |
---|
| 2866 | { |
---|
| 2867 | for( i=(vecLen-1); i>=0; i-- ) |
---|
| 2868 | { |
---|
| 2869 | if( (pv[i].getCode() == protonCode) && pv[i].getFlag() ) |
---|
| 2870 | { |
---|
| 2871 | G4HEVector pTemp = pv[i]; |
---|
| 2872 | pv[i].setDefinition( "Neutron" ); |
---|
| 2873 | pv[i].setMomentumAndUpdate(pTemp.getMomentum()); |
---|
| 2874 | if (verboseLevel > 1) pv[i].Print(i); |
---|
| 2875 | if( ++kk > ika ) break; |
---|
| 2876 | } |
---|
| 2877 | } |
---|
| 2878 | } |
---|
| 2879 | } |
---|
| 2880 | } |
---|
| 2881 | } |
---|
| 2882 | |
---|
| 2883 | // Finished adding proton/neutron black track particles |
---|
| 2884 | // now, try to add deuterons, tritons and alphas |
---|
| 2885 | |
---|
| 2886 | if( excitationEnergyDTA >= 0.001 ) |
---|
| 2887 | { |
---|
| 2888 | nbl = Poisson( (1.5+1.25*targ)*excitationEnergyDTA |
---|
| 2889 | /(excitationEnergyGNP+excitationEnergyDTA)); |
---|
| 2890 | |
---|
| 2891 | // nbl is the number of deutrons, tritons, and alphas produced |
---|
| 2892 | |
---|
| 2893 | if( nbl > 0 ) |
---|
| 2894 | { |
---|
| 2895 | ekin = excitationEnergyDTA/nbl; |
---|
| 2896 | ekin2 = 0.0; |
---|
| 2897 | for( i=0; i<nbl; i++ ) |
---|
| 2898 | { |
---|
| 2899 | if( G4UniformRand() < sprob ) continue; |
---|
| 2900 | if( ekin2 > excitationEnergyDTA) break; |
---|
| 2901 | ran = G4UniformRand(); |
---|
| 2902 | ekin1 = -ekin*std::log(ran)-cfa*(1.+0.5*normal()); |
---|
| 2903 | if( ekin1 < 0.0 ) ekin1 = -0.010*std::log(ran); |
---|
| 2904 | ekin2 += ekin1; |
---|
| 2905 | if( ekin2 > excitationEnergyDTA ) |
---|
| 2906 | ekin1 = Amax( 1.0e-6, excitationEnergyDTA-(ekin2-ekin1)); |
---|
| 2907 | cost = G4UniformRand()*2.0 - 1.0; |
---|
| 2908 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 2909 | phi = twopi*G4UniformRand(); |
---|
| 2910 | ran = G4UniformRand(); |
---|
| 2911 | if( ran <= 0.60 ) |
---|
| 2912 | pv[vecLen].setDefinition( "Deuteron"); |
---|
| 2913 | else if (ran <= 0.90) |
---|
| 2914 | pv[vecLen].setDefinition( "Triton" ); |
---|
| 2915 | else |
---|
| 2916 | pv[vecLen].setDefinition( "Alpha" ); |
---|
| 2917 | spall += (int)(pv[vecLen].getMass() * 1.066); |
---|
| 2918 | if( spall > atomicWeight ) break; |
---|
| 2919 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 2920 | pv[vecLen].setSide( -4 ); |
---|
| 2921 | pvMass = pv[vecLen].getMass(); |
---|
| 2922 | pv[vecLen].setTOF( 1.0 ); |
---|
| 2923 | pvEnergy = pvMass + ekin1; |
---|
| 2924 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 2925 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 2926 | pp*sint*std::cos(phi), |
---|
| 2927 | pp*cost ); |
---|
| 2928 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 2929 | vecLen++; |
---|
| 2930 | } |
---|
| 2931 | } |
---|
| 2932 | } |
---|
| 2933 | } |
---|
| 2934 | if( centerOfMassEnergy <= (4.0+G4UniformRand()) ) |
---|
| 2935 | { |
---|
| 2936 | for( i=0; i<vecLen; i++ ) |
---|
| 2937 | { |
---|
| 2938 | G4double etb = pv[i].getKineticEnergy(); |
---|
| 2939 | if( etb >= incidentKineticEnergy ) |
---|
| 2940 | pv[i].setKineticEnergyAndUpdate( incidentKineticEnergy ); |
---|
| 2941 | } |
---|
| 2942 | } |
---|
| 2943 | |
---|
| 2944 | TuningOfHighEnergyCascading( pv, vecLen, |
---|
| 2945 | incidentParticle, targetParticle, |
---|
| 2946 | atomicWeight, atomicNumber); |
---|
| 2947 | |
---|
| 2948 | // Calculate time delay for nuclear reactions |
---|
| 2949 | |
---|
| 2950 | G4double tof = incidentTOF; |
---|
| 2951 | if( (atomicWeight >= 1.5) && (atomicWeight <= 230.0) |
---|
| 2952 | && (incidentKineticEnergy <= 0.2) ) |
---|
| 2953 | tof -= 500.0 * std::exp(-incidentKineticEnergy /0.04) * std::log( G4UniformRand() ); |
---|
| 2954 | for ( i=0; i < vecLen; i++) |
---|
| 2955 | { |
---|
| 2956 | |
---|
| 2957 | pv[i].setTOF ( tof ); |
---|
| 2958 | // vec[i].SetTOF ( tof ); |
---|
| 2959 | } |
---|
| 2960 | |
---|
| 2961 | for(i=0; i<vecLen; i++) |
---|
| 2962 | { |
---|
| 2963 | if(pv[i].getName() == "KaonZero" || pv[i].getName() == "AntiKaonZero") |
---|
| 2964 | { |
---|
| 2965 | pvmx[0] = pv[i]; |
---|
| 2966 | if(G4UniformRand() < 0.5) pv[i].setDefinition("KaonZeroShort"); |
---|
| 2967 | else pv[i].setDefinition("KaonZeroLong"); |
---|
| 2968 | pv[i].setMomentumAndUpdate(pvmx[0].getMomentum()); |
---|
| 2969 | } |
---|
| 2970 | } |
---|
| 2971 | |
---|
[1347] | 2972 | successful = true; |
---|
| 2973 | delete [] pvmx; |
---|
| 2974 | delete [] tempV; |
---|
| 2975 | return; |
---|
| 2976 | } |
---|
[819] | 2977 | |
---|
| 2978 | void |
---|
[1347] | 2979 | G4HEInelastic::MediumEnergyCascading(G4bool& successful, |
---|
[819] | 2980 | G4HEVector pv[], |
---|
[1347] | 2981 | G4int& vecLen, |
---|
| 2982 | G4double& excitationEnergyGNP, |
---|
| 2983 | G4double& excitationEnergyDTA, |
---|
| 2984 | const G4HEVector& incidentParticle, |
---|
| 2985 | const G4HEVector& targetParticle, |
---|
[819] | 2986 | G4double atomicWeight, |
---|
| 2987 | G4double atomicNumber) |
---|
[1347] | 2988 | { |
---|
| 2989 | // The multiplicity of particles produced in the first interaction has been |
---|
| 2990 | // calculated in one of the FirstIntInNuc.... routines. The nuclear |
---|
| 2991 | // cascading particles are parametrized from experimental data. |
---|
| 2992 | // A simple single variable description E D3S/DP3= F(Q) with |
---|
| 2993 | // Q^2 = (M*X)^2 + PT^2 is used. Final state kinematic is produced |
---|
| 2994 | // by an FF-type iterative cascade method. |
---|
| 2995 | // Nuclear evaporation particles are added at the end of the routine. |
---|
[819] | 2996 | |
---|
[1347] | 2997 | // All quantities on the G4HEVector Array pv are in GeV- units. |
---|
[819] | 2998 | |
---|
[1347] | 2999 | G4int protonCode = Proton.getCode(); |
---|
| 3000 | G4double protonMass = Proton.getMass(); |
---|
| 3001 | G4int neutronCode = Neutron.getCode(); |
---|
| 3002 | G4double kaonPlusMass = KaonPlus.getMass(); |
---|
| 3003 | G4int kaonPlusCode = KaonPlus.getCode(); |
---|
| 3004 | G4int kaonMinusCode = KaonMinus.getCode(); |
---|
| 3005 | G4int kaonZeroSCode = KaonZeroShort.getCode(); |
---|
| 3006 | G4int kaonZeroLCode = KaonZeroLong.getCode(); |
---|
| 3007 | G4int kaonZeroCode = KaonZero.getCode(); |
---|
| 3008 | G4int antiKaonZeroCode = AntiKaonZero.getCode(); |
---|
| 3009 | G4int pionPlusCode = PionPlus.getCode(); |
---|
| 3010 | G4int pionZeroCode = PionZero.getCode(); |
---|
| 3011 | G4int pionMinusCode = PionMinus.getCode(); |
---|
| 3012 | G4String mesonType = PionPlus.getType(); |
---|
| 3013 | G4String baryonType = Proton.getType(); |
---|
| 3014 | G4String antiBaryonType = AntiProton.getType(); |
---|
[819] | 3015 | |
---|
[1347] | 3016 | G4double targetMass = targetParticle.getMass(); |
---|
[819] | 3017 | |
---|
[1347] | 3018 | G4int incidentCode = incidentParticle.getCode(); |
---|
| 3019 | G4double incidentMass = incidentParticle.getMass(); |
---|
| 3020 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); |
---|
| 3021 | G4double incidentEnergy = incidentParticle.getEnergy(); |
---|
| 3022 | G4double incidentKineticEnergy = incidentParticle.getKineticEnergy(); |
---|
| 3023 | G4String incidentType = incidentParticle.getType(); |
---|
| 3024 | // G4double incidentTOF = incidentParticle.getTOF(); |
---|
| 3025 | G4double incidentTOF = 0.; |
---|
[819] | 3026 | |
---|
[1347] | 3027 | // some local variables |
---|
[819] | 3028 | |
---|
[1347] | 3029 | G4int i, j, l; |
---|
[819] | 3030 | |
---|
[1347] | 3031 | if(verboseLevel > 1) |
---|
[819] | 3032 | G4cout << " G4HEInelastic::MediumEnergyCascading " << G4endl; |
---|
| 3033 | |
---|
[1347] | 3034 | // define annihilation channels. |
---|
[819] | 3035 | |
---|
[1347] | 3036 | G4bool annihilation = false; |
---|
| 3037 | if (incidentCode < 0 && incidentType == antiBaryonType && |
---|
| 3038 | pv[0].getType() != antiBaryonType && |
---|
| 3039 | pv[1].getType() != antiBaryonType) { |
---|
| 3040 | annihilation = true; |
---|
| 3041 | } |
---|
| 3042 | |
---|
| 3043 | successful = false; |
---|
[819] | 3044 | |
---|
[1347] | 3045 | G4double twsup[] = { 1., 1., 0.7, 0.5, 0.3, 0.2, 0.1, 0.0 }; |
---|
[819] | 3046 | |
---|
| 3047 | if(annihilation) goto start; |
---|
| 3048 | if(vecLen >= 8) goto start; |
---|
| 3049 | if(incidentKineticEnergy < 1.) return; |
---|
| 3050 | if( ( incidentCode == kaonPlusCode || incidentCode == kaonMinusCode |
---|
| 3051 | || incidentCode == kaonZeroCode || incidentCode == antiKaonZeroCode |
---|
| 3052 | || incidentCode == kaonZeroSCode || incidentCode == kaonZeroLCode ) |
---|
| 3053 | && ( G4UniformRand() < 0.5)) goto start; |
---|
| 3054 | if(G4UniformRand() > twsup[vecLen-1]) goto start; |
---|
| 3055 | return; |
---|
| 3056 | |
---|
| 3057 | start: |
---|
| 3058 | |
---|
| 3059 | if (annihilation) |
---|
| 3060 | { // do some corrections of incident particle kinematic |
---|
| 3061 | G4double ekcor = Amax( 1., 1./incidentKineticEnergy); |
---|
| 3062 | incidentKineticEnergy = 2*targetMass + incidentKineticEnergy*(1.+ekcor/atomicWeight); |
---|
| 3063 | G4double excitation = NuclearExcitation(incidentKineticEnergy, |
---|
| 3064 | atomicWeight, |
---|
| 3065 | atomicNumber, |
---|
| 3066 | excitationEnergyGNP, |
---|
| 3067 | excitationEnergyDTA); |
---|
| 3068 | incidentKineticEnergy -= excitation; |
---|
| 3069 | if (incidentKineticEnergy < excitationEnergyDTA) incidentKineticEnergy = 0.; |
---|
| 3070 | incidentEnergy = incidentKineticEnergy + incidentMass; |
---|
| 3071 | incidentTotalMomentum = |
---|
| 3072 | std::sqrt( Amax(0., incidentEnergy*incidentEnergy - incidentMass*incidentMass)); |
---|
| 3073 | } |
---|
| 3074 | |
---|
| 3075 | G4HEVector pTemp; |
---|
| 3076 | for(i = 2; i<vecLen; i++) |
---|
| 3077 | { |
---|
| 3078 | j = Imin(vecLen-1, (G4int)(2. + G4UniformRand()*(vecLen-2))); |
---|
| 3079 | pTemp = pv[j]; |
---|
| 3080 | pv[j] = pv[i]; |
---|
| 3081 | pv[i] = pTemp; |
---|
| 3082 | } |
---|
| 3083 | |
---|
| 3084 | // randomize the first two leading particles |
---|
| 3085 | // for kaon induced reactions only |
---|
| 3086 | // (need from experimental data) |
---|
| 3087 | |
---|
| 3088 | if( (incidentCode==kaonPlusCode || incidentCode==kaonMinusCode || |
---|
| 3089 | incidentCode==kaonZeroCode || incidentCode==antiKaonZeroCode || |
---|
| 3090 | incidentCode==kaonZeroSCode || incidentCode==kaonZeroLCode) |
---|
| 3091 | && (G4UniformRand()>0.7) ) |
---|
| 3092 | { |
---|
| 3093 | pTemp = pv[1]; |
---|
| 3094 | pv[1] = pv[0]; |
---|
| 3095 | pv[0] = pTemp; |
---|
| 3096 | } |
---|
| 3097 | |
---|
| 3098 | // mark leading particles for incident strange particles |
---|
| 3099 | // and antibaryons, for all other we assume that the first |
---|
| 3100 | // and second particle are the leading particles. |
---|
| 3101 | // We need this later for kinematic aspects of strangeness |
---|
| 3102 | // conservation. |
---|
| 3103 | |
---|
| 3104 | G4int lead = 0; |
---|
| 3105 | G4HEVector leadParticle; |
---|
| 3106 | if( (incidentMass >= kaonPlusMass-0.05) && (incidentCode != protonCode) |
---|
| 3107 | && (incidentCode != neutronCode) ) |
---|
| 3108 | { |
---|
| 3109 | G4double pMass = pv[0].getMass(); |
---|
| 3110 | G4int pCode = pv[0].getCode(); |
---|
| 3111 | if( (pMass >= kaonPlusMass-0.05) && (pCode != protonCode) |
---|
| 3112 | && (pCode != neutronCode) ) |
---|
| 3113 | { |
---|
| 3114 | lead = pCode; |
---|
| 3115 | leadParticle = pv[0]; |
---|
| 3116 | } |
---|
| 3117 | else |
---|
| 3118 | { |
---|
| 3119 | pMass = pv[1].getMass(); |
---|
| 3120 | pCode = pv[1].getCode(); |
---|
| 3121 | if( (pMass >= kaonPlusMass-0.05) && (pCode != protonCode) |
---|
| 3122 | && (pCode != neutronCode) ) |
---|
| 3123 | { |
---|
| 3124 | lead = pCode; |
---|
| 3125 | leadParticle = pv[1]; |
---|
| 3126 | } |
---|
| 3127 | } |
---|
| 3128 | } |
---|
| 3129 | |
---|
| 3130 | // Distribute particles in forward and backward hemispheres in center of |
---|
| 3131 | // mass system. Incident particle goes in forward hemisphere. |
---|
| 3132 | |
---|
| 3133 | G4HEVector pvI = incidentParticle; // for the incident particle |
---|
| 3134 | pvI.setSide( 1 ); |
---|
| 3135 | |
---|
| 3136 | G4HEVector pvT = targetParticle; // for the target particle |
---|
| 3137 | pvT.setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 3138 | pvT.setSide( -1 ); |
---|
| 3139 | pvT.setTOF( -1.); |
---|
| 3140 | |
---|
| 3141 | |
---|
| 3142 | G4double centerOfMassEnergy = std::sqrt( sqr(incidentMass)+sqr(targetMass) |
---|
| 3143 | +2.0*targetMass*incidentEnergy ); |
---|
| 3144 | // G4double availableEnergy = centerOfMassEnergy - ( targetMass + incidentMass ); |
---|
| 3145 | |
---|
| 3146 | G4double tavai1 = centerOfMassEnergy/2.0 - incidentMass; |
---|
| 3147 | G4double tavai2 = centerOfMassEnergy/2.0 - targetMass; |
---|
| 3148 | |
---|
| 3149 | G4int ntb = 1; |
---|
| 3150 | for( i=0; i < vecLen; i++ ) |
---|
| 3151 | { |
---|
| 3152 | if (i == 0) pv[i].setSide( 1 ); |
---|
| 3153 | else if (i == 1) pv[i].setSide( -1 ); |
---|
| 3154 | else |
---|
| 3155 | { if( G4UniformRand() < 0.5 ) |
---|
| 3156 | { |
---|
| 3157 | pv[i].setSide( -1 ); |
---|
| 3158 | ntb++; |
---|
| 3159 | } |
---|
| 3160 | else |
---|
| 3161 | pv[i].setSide( 1 ); |
---|
| 3162 | } |
---|
| 3163 | pv[i].setTOF( incidentTOF); |
---|
| 3164 | } |
---|
| 3165 | G4double tb = 2. * ntb; |
---|
| 3166 | if (centerOfMassEnergy < (2. + G4UniformRand())) |
---|
| 3167 | tb = (2. * ntb + vecLen)/2.; |
---|
| 3168 | |
---|
| 3169 | if (verboseLevel > 1) |
---|
| 3170 | { G4cout << " pv Vector after Randomization " << vecLen << G4endl; |
---|
| 3171 | pvI.Print(-1); |
---|
| 3172 | pvT.Print(-1); |
---|
| 3173 | for (i=0; i < vecLen ; i++) pv[i].Print(i); |
---|
| 3174 | } |
---|
| 3175 | |
---|
| 3176 | // Add particles from intranuclear cascade |
---|
| 3177 | // nuclearCascadeCount = number of new secondaries |
---|
| 3178 | // produced by nuclear cascading. |
---|
| 3179 | // extraCount = number of nucleons within these new secondaries |
---|
| 3180 | |
---|
| 3181 | G4double s, xtarg, ran; |
---|
| 3182 | s = centerOfMassEnergy*centerOfMassEnergy; |
---|
| 3183 | xtarg = Amax( 0.01, Amin( 0.75, 0.312 + 0.200 * std::log(std::log(s)) |
---|
| 3184 | + std::pow(s,1.5)/6000.0 ) |
---|
| 3185 | *(std::pow(atomicWeight, 0.33) - 1.0) * tb); |
---|
| 3186 | |
---|
| 3187 | G4int ntarg = Poisson( xtarg ); |
---|
| 3188 | G4int targ = 0; |
---|
| 3189 | |
---|
| 3190 | if( ntarg > 0 ) |
---|
| 3191 | { |
---|
| 3192 | G4double nucsup[] = { 1.00, 0.7, 0.5, 0.4, 0.35, 0.3 }; |
---|
| 3193 | G4double psup[] = { 3., 6., 20., 50., 100., 1000. }; |
---|
| 3194 | G4int momentumBin = 0; |
---|
| 3195 | while( (momentumBin < 6) && (incidentTotalMomentum > psup[momentumBin]) ) |
---|
| 3196 | momentumBin++; |
---|
| 3197 | momentumBin = Imin( 5, momentumBin ); |
---|
| 3198 | |
---|
| 3199 | // NOTE: in GENXPT, these new particles were given negative codes |
---|
| 3200 | // here I use flag = true instead |
---|
| 3201 | |
---|
| 3202 | for( i=0; i<ntarg; i++ ) |
---|
| 3203 | { |
---|
| 3204 | if( G4UniformRand() < nucsup[momentumBin] ) |
---|
| 3205 | { |
---|
| 3206 | if( G4UniformRand() > 1.0-atomicNumber/atomicWeight ) |
---|
| 3207 | pv[vecLen].setDefinition( "Proton" ); |
---|
| 3208 | else |
---|
| 3209 | pv[vecLen].setDefinition( "Neutron" ); |
---|
| 3210 | targ++; |
---|
| 3211 | } |
---|
| 3212 | else |
---|
| 3213 | { |
---|
| 3214 | ran = G4UniformRand(); |
---|
| 3215 | if( ran < 0.33333 ) |
---|
| 3216 | pv[vecLen].setDefinition( "PionPlus"); |
---|
| 3217 | else if( ran < 0.66667 ) |
---|
| 3218 | pv[vecLen].setDefinition( "PionZero"); |
---|
| 3219 | else |
---|
| 3220 | pv[vecLen].setDefinition( "PionMinus" ); |
---|
| 3221 | } |
---|
| 3222 | pv[vecLen].setSide( -2 ); // backward cascade particles |
---|
| 3223 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 3224 | pv[vecLen].setTOF( incidentTOF ); |
---|
| 3225 | vecLen++; |
---|
| 3226 | } |
---|
| 3227 | } |
---|
| 3228 | |
---|
| 3229 | // assume conservation of kinetic energy |
---|
| 3230 | // in forward & backward hemispheres |
---|
| 3231 | |
---|
| 3232 | G4int is, iskip; |
---|
| 3233 | tavai1 = centerOfMassEnergy/2.; |
---|
| 3234 | G4int iavai1 = 0; |
---|
| 3235 | |
---|
| 3236 | for (i = 0; i < vecLen; i++) |
---|
| 3237 | { |
---|
| 3238 | if (pv[i].getSide() > 0) |
---|
| 3239 | { |
---|
| 3240 | tavai1 -= pv[i].getMass(); |
---|
| 3241 | iavai1++; |
---|
| 3242 | } |
---|
| 3243 | } |
---|
| 3244 | if ( iavai1 == 0) return; |
---|
| 3245 | |
---|
| 3246 | while( tavai1 <= 0.0 ) |
---|
| 3247 | { // must eliminate a particle from the forward side |
---|
| 3248 | iskip = G4int(G4UniformRand()*iavai1) + 1; |
---|
| 3249 | is = 0; |
---|
| 3250 | for( i=vecLen-1; i>=0; i-- ) |
---|
| 3251 | { |
---|
| 3252 | if( pv[i].getSide() > 0 ) |
---|
| 3253 | { |
---|
| 3254 | if (++is == iskip) |
---|
| 3255 | { |
---|
| 3256 | tavai1 += pv[i].getMass(); |
---|
| 3257 | iavai1--; |
---|
| 3258 | if ( i != vecLen-1) |
---|
| 3259 | { |
---|
| 3260 | for( j=i; j<vecLen; j++ ) |
---|
| 3261 | { |
---|
| 3262 | pv[j] = pv[j+1]; |
---|
| 3263 | } |
---|
| 3264 | } |
---|
| 3265 | if( --vecLen == 0 ) return; // all the secondaries except of the |
---|
| 3266 | break; // --+ |
---|
| 3267 | } // | |
---|
| 3268 | } // v |
---|
| 3269 | } // break goes down to here |
---|
| 3270 | } // to the end of the for- loop. |
---|
| 3271 | |
---|
| 3272 | |
---|
| 3273 | tavai2 = (targ+1)*centerOfMassEnergy/2.; |
---|
| 3274 | G4int iavai2 = 0; |
---|
| 3275 | |
---|
| 3276 | for (i = 0; i < vecLen; i++) |
---|
| 3277 | { |
---|
| 3278 | if (pv[i].getSide() < 0) |
---|
| 3279 | { |
---|
| 3280 | tavai2 -= pv[i].getMass(); |
---|
| 3281 | iavai2++; |
---|
| 3282 | } |
---|
| 3283 | } |
---|
| 3284 | if (iavai2 == 0) return; |
---|
| 3285 | |
---|
| 3286 | while( tavai2 <= 0.0 ) |
---|
| 3287 | { // must eliminate a particle from the backward side |
---|
| 3288 | iskip = G4int(G4UniformRand()*iavai2) + 1; |
---|
| 3289 | is = 0; |
---|
| 3290 | for( i = vecLen-1; i >= 0; i-- ) |
---|
| 3291 | { |
---|
| 3292 | if( pv[i].getSide() < 0 ) |
---|
| 3293 | { |
---|
| 3294 | if( ++is == iskip ) |
---|
| 3295 | { |
---|
| 3296 | tavai2 += pv[i].getMass(); |
---|
| 3297 | iavai2--; |
---|
| 3298 | if (pv[i].getSide() == -2) ntarg--; |
---|
| 3299 | if (i != vecLen-1) |
---|
| 3300 | { |
---|
| 3301 | for( j=i; j<vecLen; j++) |
---|
| 3302 | { |
---|
| 3303 | pv[j] = pv[j+1]; |
---|
| 3304 | } |
---|
| 3305 | } |
---|
| 3306 | if (--vecLen == 0) return; |
---|
| 3307 | break; |
---|
| 3308 | } |
---|
| 3309 | } |
---|
| 3310 | } |
---|
| 3311 | } |
---|
| 3312 | |
---|
| 3313 | if (verboseLevel > 1) { |
---|
| 3314 | G4cout << " pv Vector after Energy checks " << vecLen << " " |
---|
| 3315 | << tavai1 << " " << iavai1 << " " << tavai2 << " " |
---|
| 3316 | << iavai2 << " " << ntarg << G4endl; |
---|
| 3317 | pvI.Print(-1); |
---|
| 3318 | pvT.Print(-1); |
---|
| 3319 | for (i=0; i < vecLen ; i++) pv[i].Print(i); |
---|
| 3320 | } |
---|
| 3321 | |
---|
| 3322 | // Define some vectors for Lorentz transformations |
---|
| 3323 | |
---|
| 3324 | G4HEVector* pvmx = new G4HEVector [10]; |
---|
| 3325 | |
---|
| 3326 | pvmx[0].setMass( incidentMass ); |
---|
| 3327 | pvmx[0].setMomentumAndUpdate( 0.0, 0.0, incidentTotalMomentum ); |
---|
| 3328 | pvmx[1].setMass( protonMass); |
---|
| 3329 | pvmx[1].setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 3330 | pvmx[3].setMass( protonMass*(1+targ)); |
---|
| 3331 | pvmx[3].setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 3332 | pvmx[4].setZero(); |
---|
| 3333 | pvmx[5].setZero(); |
---|
| 3334 | pvmx[7].setZero(); |
---|
| 3335 | pvmx[8].setZero(); |
---|
| 3336 | pvmx[8].setMomentum( 1.0, 0.0 ); |
---|
| 3337 | pvmx[2].Add( pvmx[0], pvmx[1] ); |
---|
| 3338 | pvmx[3].Add( pvmx[3], pvmx[0] ); |
---|
| 3339 | pvmx[0].Lor( pvmx[0], pvmx[2] ); |
---|
| 3340 | pvmx[1].Lor( pvmx[1], pvmx[2] ); |
---|
| 3341 | |
---|
| 3342 | if (verboseLevel > 1) { |
---|
| 3343 | G4cout << " General Vectors after Definition " << G4endl; |
---|
| 3344 | for (i=0; i<10; i++) pvmx[i].Print(i); |
---|
| 3345 | } |
---|
| 3346 | |
---|
| 3347 | // Main loop for 4-momentum generation - see Pitha-report (Aachen) |
---|
| 3348 | // for a detailed description of the method. |
---|
| 3349 | // Process the secondary particles in reverse order |
---|
| 3350 | |
---|
| 3351 | G4double dndl[20]; |
---|
| 3352 | G4double binl[20]; |
---|
| 3353 | G4double pvMass, pvEnergy; |
---|
| 3354 | G4int pvCode; |
---|
| 3355 | G4double aspar, pt, phi, et, xval; |
---|
| 3356 | G4double ekin = 0.; |
---|
| 3357 | G4double ekin1 = 0.; |
---|
| 3358 | G4double ekin2 = 0.; |
---|
| 3359 | phi = G4UniformRand()*twopi; |
---|
| 3360 | G4int npg = 0; |
---|
| 3361 | G4int targ1 = 0; // No fragmentation model for nucleons |
---|
| 3362 | for( i=vecLen-1; i>=0; i-- ) // from the intranuclear cascade. Mark |
---|
| 3363 | { // them with -3 and leave the loop. |
---|
| 3364 | if( (pv[i].getSide() == -2) || (i == 1) ) |
---|
| 3365 | { |
---|
| 3366 | if ( pv[i].getType() == baryonType || |
---|
| 3367 | pv[i].getType() == antiBaryonType) |
---|
| 3368 | { |
---|
| 3369 | if( ++npg < 19 ) |
---|
| 3370 | { |
---|
| 3371 | pv[i].setSide( -3 ); |
---|
| 3372 | targ1++; |
---|
| 3373 | continue; // leave the for loop !! |
---|
| 3374 | } |
---|
| 3375 | } |
---|
| 3376 | } |
---|
| 3377 | |
---|
| 3378 | // Set pt and phi values - they are changed somewhat in the |
---|
| 3379 | // iteration loop. |
---|
| 3380 | // Set mass parameter for lambda fragmentation model |
---|
| 3381 | |
---|
| 3382 | G4double maspar[] = { 0.75, 0.70, 0.65, 0.60, 0.50, 0.40, 0.75, 0.20}; |
---|
| 3383 | G4double bp[] = { 3.50, 3.50, 3.50, 6.00, 5.00, 4.00, 3.50, 3.50}; |
---|
| 3384 | G4double ptex[] = { 1.70, 1.70, 1.50, 1.70, 1.40, 1.20, 1.70, 1.20}; |
---|
| 3385 | // Set parameters for lambda simulation: |
---|
| 3386 | // pt is the average transverse momentum |
---|
| 3387 | // aspar the is average transverse mass |
---|
| 3388 | |
---|
| 3389 | pvMass = pv[i].getMass(); |
---|
| 3390 | j = 2; |
---|
| 3391 | if ( pv[i].getType() == mesonType ) j = 1; |
---|
| 3392 | if ( pv[i].getMass() < 0.4 ) j = 0; |
---|
| 3393 | if ( i <= 1 ) j += 3; |
---|
| 3394 | if (pv[i].getSide() <= -2) j = 6; |
---|
| 3395 | if (j == 6 && (pv[i].getType() == baryonType || pv[i].getType()==antiBaryonType) ) j = 7; |
---|
| 3396 | pt = Amax(0.001, std::sqrt(std::pow(-std::log(1.-G4UniformRand())/bp[j],ptex[j]))); |
---|
| 3397 | aspar = maspar[j]; |
---|
| 3398 | phi = G4UniformRand()*twopi; |
---|
| 3399 | pv[i].setMomentum( pt*std::cos(phi), pt*std::sin(phi) ); // set x- and y-momentum |
---|
| 3400 | |
---|
| 3401 | for( j=0; j<20; j++ ) binl[j] = j/(19.*pt); // set the lambda - bins. |
---|
| 3402 | |
---|
| 3403 | if( pv[i].getSide() > 0 ) |
---|
| 3404 | et = pvmx[0].getEnergy(); |
---|
| 3405 | else |
---|
| 3406 | et = pvmx[1].getEnergy(); |
---|
| 3407 | |
---|
| 3408 | dndl[0] = 0.0; |
---|
| 3409 | |
---|
| 3410 | // Start of outer iteration loop |
---|
| 3411 | |
---|
| 3412 | G4int outerCounter = 0, innerCounter = 0; // three times. |
---|
| 3413 | G4bool eliminateThisParticle = true; |
---|
| 3414 | G4bool resetEnergies = true; |
---|
| 3415 | while( ++outerCounter < 3 ) |
---|
| 3416 | { |
---|
| 3417 | for( l=1; l<20; l++ ) |
---|
| 3418 | { |
---|
| 3419 | xval = (binl[l]+binl[l-1])/2.; // x = lambda /GeV |
---|
| 3420 | if( xval > 1./pt ) |
---|
| 3421 | dndl[l] = dndl[l-1]; |
---|
| 3422 | else |
---|
| 3423 | dndl[l] = dndl[l-1] + |
---|
| 3424 | aspar/std::sqrt( std::pow((1.+aspar*xval*aspar*xval),3) ) * |
---|
| 3425 | (binl[l]-binl[l-1]) * et / |
---|
| 3426 | std::sqrt( pt*xval*et*pt*xval*et + pt*pt + pvMass*pvMass ); |
---|
| 3427 | } |
---|
| 3428 | |
---|
| 3429 | // Start of inner iteration loop |
---|
| 3430 | |
---|
| 3431 | innerCounter = 0; // try this not more than 7 times. |
---|
| 3432 | while( ++innerCounter < 7 ) |
---|
| 3433 | { |
---|
| 3434 | l = 1; |
---|
| 3435 | ran = G4UniformRand()*dndl[19]; |
---|
| 3436 | while( ( ran >= dndl[l] ) && ( l < 20 ) )l++; |
---|
| 3437 | l = Imin( 19, l ); |
---|
[962] | 3438 | xval = Amin( 1.0, pt*(binl[l-1] + G4UniformRand()*(binl[l]-binl[l-1]) ) ); |
---|
[819] | 3439 | if( pv[i].getSide() < 0 ) xval *= -1.; |
---|
| 3440 | pv[i].setMomentumAndUpdate( xval*et ); // set the z-momentum |
---|
| 3441 | pvEnergy = pv[i].getEnergy(); |
---|
| 3442 | if( pv[i].getSide() > 0 ) // forward side |
---|
| 3443 | { |
---|
| 3444 | if ( i < 2 ) |
---|
| 3445 | { |
---|
| 3446 | ekin = tavai1 - ekin1; |
---|
| 3447 | if (ekin < 0.) ekin = 0.04*std::fabs(normal()); |
---|
| 3448 | G4double pp1 = pv[i].Length(); |
---|
| 3449 | if (pp1 >= 1.e-6) |
---|
| 3450 | { |
---|
| 3451 | G4double pp = std::sqrt(ekin*(ekin+2*pvMass)); |
---|
| 3452 | pp = Amax(0.,pp*pp-pt*pt); |
---|
| 3453 | pp = std::sqrt(pp)*pv[i].getSide()/std::fabs(G4double(pv[i].getSide())); |
---|
| 3454 | pv[i].setMomentumAndUpdate( pp ); |
---|
| 3455 | } |
---|
| 3456 | else |
---|
| 3457 | { |
---|
| 3458 | pv[i].setMomentum(0.,0.,0.); |
---|
| 3459 | pv[i].setKineticEnergyAndUpdate( ekin); |
---|
| 3460 | } |
---|
| 3461 | pvmx[4].Add( pvmx[4], pv[i]); |
---|
| 3462 | outerCounter = 2; |
---|
| 3463 | resetEnergies = false; |
---|
| 3464 | eliminateThisParticle = false; |
---|
| 3465 | break; |
---|
| 3466 | } |
---|
| 3467 | else if( (ekin1+pvEnergy-pvMass) < 0.95*tavai1 ) |
---|
| 3468 | { |
---|
| 3469 | pvmx[4].Add( pvmx[4], pv[i] ); |
---|
| 3470 | ekin1 += pvEnergy - pvMass; |
---|
| 3471 | pvmx[6].Add( pvmx[4], pvmx[5] ); |
---|
| 3472 | pvmx[6].setMomentum( 0.0 ); |
---|
| 3473 | outerCounter = 2; // leave outer loop |
---|
| 3474 | eliminateThisParticle = false; // don't eliminate this particle |
---|
| 3475 | resetEnergies = false; |
---|
| 3476 | break; // next particle |
---|
| 3477 | } |
---|
| 3478 | if( innerCounter > 5 ) break; // leave inner loop |
---|
| 3479 | |
---|
| 3480 | if( tavai2 >= pvMass ) |
---|
| 3481 | { // switch sides |
---|
| 3482 | pv[i].setSide( -1 ); |
---|
| 3483 | tavai1 += pvMass; |
---|
| 3484 | tavai2 -= pvMass; |
---|
| 3485 | iavai2++; |
---|
| 3486 | } |
---|
| 3487 | } |
---|
| 3488 | else |
---|
| 3489 | { // backward side |
---|
| 3490 | xval = Amin(0.999,0.95+0.05*targ/20.0); |
---|
| 3491 | if( (ekin2+pvEnergy-pvMass) < xval*tavai2 ) |
---|
| 3492 | { |
---|
| 3493 | pvmx[5].Add( pvmx[5], pv[i] ); |
---|
| 3494 | ekin2 += pvEnergy - pvMass; |
---|
| 3495 | pvmx[6].Add( pvmx[4], pvmx[5] ); |
---|
| 3496 | pvmx[6].setMomentum( 0.0 ); // set z-momentum |
---|
| 3497 | outerCounter = 2; // leave outer iteration |
---|
| 3498 | eliminateThisParticle = false; // don't eliminate this particle |
---|
| 3499 | resetEnergies = false; |
---|
| 3500 | break; // leave inner iteration |
---|
| 3501 | } |
---|
| 3502 | if( innerCounter > 5 )break; // leave inner iteration |
---|
| 3503 | |
---|
| 3504 | if( tavai1 >= pvMass ) |
---|
| 3505 | { // switch sides |
---|
| 3506 | pv[i].setSide( 1 ); |
---|
| 3507 | tavai1 -= pvMass; |
---|
| 3508 | tavai2 += pvMass; |
---|
| 3509 | iavai2--; |
---|
| 3510 | } |
---|
| 3511 | } |
---|
| 3512 | pv[i].setMomentum( pv[i].getMomentum().x() * 0.9, |
---|
| 3513 | pv[i].getMomentum().y() * 0.9); |
---|
| 3514 | pt *= 0.9; |
---|
| 3515 | dndl[19] *= 0.9; |
---|
| 3516 | } // closes inner loop |
---|
| 3517 | |
---|
| 3518 | if (resetEnergies) |
---|
| 3519 | { |
---|
| 3520 | ekin1 = 0.0; |
---|
| 3521 | ekin2 = 0.0; |
---|
| 3522 | pvmx[4].setZero(); |
---|
| 3523 | pvmx[5].setZero(); |
---|
| 3524 | if (verboseLevel > 1) |
---|
| 3525 | G4cout << " Reset energies for index " << i << G4endl; |
---|
| 3526 | for( l=i+1; l < vecLen; l++ ) |
---|
| 3527 | { |
---|
| 3528 | if( (pv[l].getMass() < protonMass) || (pv[l].getSide() > 0) ) |
---|
| 3529 | { |
---|
| 3530 | pvEnergy = Amax( pv[l].getMass(), 0.95*pv[l].getEnergy() |
---|
| 3531 | + 0.05*pv[l].getMass() ); |
---|
| 3532 | pv[l].setEnergyAndUpdate( pvEnergy ); |
---|
| 3533 | if( pv[l].getSide() > 0) |
---|
| 3534 | { |
---|
| 3535 | ekin1 += pv[l].getKineticEnergy(); |
---|
| 3536 | pvmx[4].Add( pvmx[4], pv[l] ); |
---|
| 3537 | } |
---|
| 3538 | else |
---|
| 3539 | { |
---|
| 3540 | ekin2 += pv[l].getKineticEnergy(); |
---|
| 3541 | pvmx[5].Add( pvmx[5], pv[l] ); |
---|
| 3542 | } |
---|
| 3543 | } |
---|
| 3544 | } |
---|
| 3545 | } |
---|
| 3546 | } // closes outer iteration |
---|
| 3547 | |
---|
| 3548 | if( eliminateThisParticle ) // not enough energy, |
---|
| 3549 | { // eliminate this particle |
---|
| 3550 | if (verboseLevel > 1) |
---|
| 3551 | { |
---|
| 3552 | G4cout << " Eliminate particle with index " << i << G4endl; |
---|
| 3553 | pv[i].Print(i); |
---|
| 3554 | } |
---|
| 3555 | for( j=i; j < vecLen; j++ ) |
---|
| 3556 | { // shift down |
---|
| 3557 | pv[j] = pv[j+1]; |
---|
| 3558 | } |
---|
| 3559 | vecLen--; |
---|
[1347] | 3560 | if (vecLen < 2) { |
---|
| 3561 | delete [] pvmx; |
---|
| 3562 | return; |
---|
| 3563 | } |
---|
[819] | 3564 | i++; |
---|
| 3565 | pvmx[6].Add( pvmx[4], pvmx[5] ); |
---|
| 3566 | pvmx[6].setMomentum( 0.0 ); // set z-momentum |
---|
| 3567 | } |
---|
| 3568 | } // closes main for loop |
---|
| 3569 | if (verboseLevel > 1) |
---|
| 3570 | { G4cout << " pv Vector after lambda fragmentation " << vecLen << G4endl; |
---|
| 3571 | pvI.Print(-1); |
---|
| 3572 | pvT.Print(-1); |
---|
| 3573 | for (i=0; i < vecLen ; i++) pv[i].Print(i); |
---|
| 3574 | for (i=0; i < 10; i++) pvmx[i].Print(i); |
---|
| 3575 | } |
---|
| 3576 | |
---|
| 3577 | // Backward nucleons produced with a cluster model |
---|
| 3578 | |
---|
| 3579 | pvmx[6].Lor( pvmx[3], pvmx[2] ); |
---|
| 3580 | pvmx[6].Sub( pvmx[6], pvmx[4] ); |
---|
| 3581 | pvmx[6].Sub( pvmx[6], pvmx[5] ); |
---|
| 3582 | if (verboseLevel > 1) pvmx[6].Print(6); |
---|
| 3583 | |
---|
| 3584 | npg = 0; |
---|
| 3585 | G4double rmb0 = 0.; |
---|
| 3586 | G4double rmb; |
---|
| 3587 | G4double wgt; |
---|
| 3588 | G4bool constantCrossSection = true; |
---|
| 3589 | for (i = 0; i < vecLen; i++) |
---|
| 3590 | { |
---|
| 3591 | if(pv[i].getSide() == -3) |
---|
| 3592 | { |
---|
| 3593 | npg++; |
---|
| 3594 | rmb0 += pv[i].getMass(); |
---|
| 3595 | } |
---|
| 3596 | } |
---|
| 3597 | if( targ1 == 1 || npg < 2) |
---|
| 3598 | { // target particle is the only backward nucleon |
---|
| 3599 | ekin = Amin( tavai2-ekin2, centerOfMassEnergy/2.0-protonMass ); |
---|
| 3600 | if( ekin < 0.04 ) ekin = 0.04 * std::fabs( normal() ); |
---|
| 3601 | G4double pp = std::sqrt(ekin*(ekin+2*pv[1].getMass())); |
---|
| 3602 | G4double pp1 = pvmx[6].Length(); |
---|
| 3603 | if(pp1 < 1.e-6) |
---|
| 3604 | { |
---|
| 3605 | pv[1].setKineticEnergyAndUpdate(ekin); |
---|
| 3606 | } |
---|
| 3607 | else |
---|
| 3608 | { |
---|
| 3609 | pv[1].setMomentum(pvmx[6].getMomentum()); |
---|
| 3610 | pv[1].SmulAndUpdate(pv[1],pp/pp1); |
---|
| 3611 | } |
---|
| 3612 | pvmx[5].Add( pvmx[5], pv[1] ); |
---|
| 3613 | } |
---|
| 3614 | else |
---|
| 3615 | { |
---|
| 3616 | G4double cpar[] = { 0.6, 0.6, 0.35, 0.15, 0.10 }; |
---|
| 3617 | G4double gpar[] = { 2.6, 2.6, 1.80, 1.30, 1.20 }; |
---|
| 3618 | |
---|
| 3619 | G4int tempCount = Imin( 5, targ1 ) - 1; |
---|
| 3620 | |
---|
| 3621 | rmb = rmb0 + std::pow(-std::log(1.0-G4UniformRand()), cpar[tempCount])/gpar[tempCount]; |
---|
| 3622 | pvEnergy = pvmx[6].getEnergy(); |
---|
| 3623 | if ( rmb > pvEnergy ) rmb = pvEnergy; |
---|
| 3624 | pvmx[6].setMass( rmb ); |
---|
| 3625 | pvmx[6].setEnergyAndUpdate( pvEnergy ); |
---|
| 3626 | pvmx[6].Smul( pvmx[6], -1. ); |
---|
| 3627 | if (verboseLevel > 1) { |
---|
| 3628 | G4cout << " General Vectors before input to NBodyPhaseSpace " |
---|
| 3629 | << targ1 << " " << tempCount << " " << rmb0 << " " |
---|
| 3630 | << rmb << " " << pvEnergy << G4endl; |
---|
| 3631 | for (i=0; i<10; i++) pvmx[i].Print(i); |
---|
| 3632 | } |
---|
| 3633 | |
---|
| 3634 | // tempV contains the backward nucleons |
---|
| 3635 | |
---|
| 3636 | G4HEVector* tempV = new G4HEVector[18]; |
---|
| 3637 | npg = 0; |
---|
| 3638 | for( i=0; i < vecLen; i++ ) |
---|
| 3639 | { |
---|
| 3640 | if( pv[i].getSide() == -3 ) tempV[npg++] = pv[i]; |
---|
| 3641 | } |
---|
| 3642 | |
---|
| 3643 | wgt = NBodyPhaseSpace( pvmx[6].getMass(), constantCrossSection, tempV, npg ); |
---|
| 3644 | |
---|
| 3645 | npg = 0; |
---|
| 3646 | for( i=0; i < vecLen; i++ ) |
---|
| 3647 | { |
---|
| 3648 | if( pv[i].getSide() == -3 ) |
---|
| 3649 | { |
---|
| 3650 | pv[i].setMomentum( tempV[npg++].getMomentum()); |
---|
| 3651 | pv[i].SmulAndUpdate( pv[i], 1.); |
---|
| 3652 | pv[i].Lor( pv[i], pvmx[6] ); |
---|
| 3653 | pvmx[5].Add( pvmx[5], pv[i] ); |
---|
| 3654 | } |
---|
| 3655 | } |
---|
| 3656 | delete [] tempV; |
---|
| 3657 | } |
---|
| 3658 | if( vecLen <= 2 ) |
---|
| 3659 | { |
---|
| 3660 | successful = false; |
---|
| 3661 | return; |
---|
| 3662 | } |
---|
| 3663 | |
---|
| 3664 | // Lorentz transformation in lab system |
---|
| 3665 | |
---|
| 3666 | targ = 0; |
---|
| 3667 | for( i=0; i < vecLen; i++ ) |
---|
| 3668 | { |
---|
| 3669 | if( pv[i].getType() == baryonType )targ++; |
---|
| 3670 | if( pv[i].getType() == antiBaryonType )targ++; |
---|
| 3671 | pv[i].Lor( pv[i], pvmx[1] ); |
---|
| 3672 | } |
---|
| 3673 | targ = Imax( 1, targ ); |
---|
| 3674 | |
---|
| 3675 | G4bool dum(0); |
---|
| 3676 | if( lead ) |
---|
| 3677 | { |
---|
| 3678 | for( i=0; i<vecLen; i++ ) |
---|
| 3679 | { |
---|
| 3680 | if( pv[i].getCode() == lead ) |
---|
| 3681 | { |
---|
| 3682 | dum = false; |
---|
| 3683 | break; |
---|
| 3684 | } |
---|
| 3685 | } |
---|
| 3686 | if( dum ) |
---|
| 3687 | { |
---|
| 3688 | i = 0; |
---|
| 3689 | |
---|
| 3690 | if( ( (leadParticle.getType() == baryonType || |
---|
| 3691 | leadParticle.getType() == antiBaryonType) |
---|
| 3692 | && (pv[1].getType() == baryonType || |
---|
| 3693 | pv[1].getType() == antiBaryonType)) |
---|
| 3694 | || ( (leadParticle.getType() == mesonType) |
---|
| 3695 | && (pv[1].getType() == mesonType))) |
---|
| 3696 | { |
---|
| 3697 | i = 1; |
---|
| 3698 | } |
---|
| 3699 | ekin = pv[i].getKineticEnergy(); |
---|
| 3700 | pv[i] = leadParticle; |
---|
| 3701 | if( pv[i].getFlag() ) |
---|
| 3702 | pv[i].setTOF( -1.0 ); |
---|
| 3703 | else |
---|
| 3704 | pv[i].setTOF( 1.0 ); |
---|
| 3705 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 3706 | } |
---|
| 3707 | } |
---|
| 3708 | |
---|
| 3709 | pvmx[3].setMass( incidentMass); |
---|
| 3710 | pvmx[3].setMomentumAndUpdate( 0.0, 0.0, incidentTotalMomentum ); |
---|
| 3711 | |
---|
| 3712 | G4double ekin0 = pvmx[3].getKineticEnergy(); |
---|
| 3713 | |
---|
| 3714 | pvmx[4].setMass ( protonMass * targ); |
---|
| 3715 | pvmx[4].setEnergy( protonMass * targ); |
---|
| 3716 | pvmx[4].setMomentum(0.,0.,0.); |
---|
| 3717 | pvmx[4].setKineticEnergy(0.); |
---|
| 3718 | |
---|
| 3719 | ekin = pvmx[3].getEnergy() + pvmx[4].getEnergy(); |
---|
| 3720 | |
---|
| 3721 | pvmx[5].Add( pvmx[3], pvmx[4] ); |
---|
| 3722 | pvmx[3].Lor( pvmx[3], pvmx[5] ); |
---|
| 3723 | pvmx[4].Lor( pvmx[4], pvmx[5] ); |
---|
| 3724 | |
---|
| 3725 | G4double tecm = pvmx[3].getEnergy() + pvmx[4].getEnergy(); |
---|
| 3726 | |
---|
| 3727 | pvmx[7].setZero(); |
---|
| 3728 | |
---|
| 3729 | ekin1 = 0.0; |
---|
| 3730 | G4double teta; |
---|
| 3731 | |
---|
| 3732 | for( i=0; i < vecLen; i++ ) |
---|
| 3733 | { |
---|
| 3734 | pvmx[7].Add( pvmx[7], pv[i] ); |
---|
| 3735 | ekin1 += pv[i].getKineticEnergy(); |
---|
| 3736 | ekin -= pv[i].getMass(); |
---|
| 3737 | } |
---|
| 3738 | |
---|
| 3739 | if( vecLen > 1 && vecLen < 19 ) |
---|
| 3740 | { |
---|
| 3741 | constantCrossSection = true; |
---|
| 3742 | G4HEVector pw[18]; |
---|
| 3743 | for(i=0;i<vecLen;i++) pw[i] = pv[i]; |
---|
| 3744 | wgt = NBodyPhaseSpace( tecm, constantCrossSection, pw, vecLen ); |
---|
| 3745 | ekin = 0.0; |
---|
| 3746 | for( i=0; i < vecLen; i++ ) |
---|
| 3747 | { |
---|
| 3748 | pvmx[6].setMass( pw[i].getMass()); |
---|
| 3749 | pvmx[6].setMomentum( pw[i].getMomentum() ); |
---|
| 3750 | pvmx[6].SmulAndUpdate( pvmx[6], 1.); |
---|
| 3751 | pvmx[6].Lor( pvmx[6], pvmx[4] ); |
---|
| 3752 | ekin += pvmx[6].getKineticEnergy(); |
---|
| 3753 | } |
---|
| 3754 | teta = pvmx[7].Ang( pvmx[3] ); |
---|
| 3755 | if (verboseLevel > 1) |
---|
| 3756 | G4cout << " vecLen > 1 && vecLen < 19 " << teta << " " << ekin0 |
---|
| 3757 | << " " << ekin1 << " " << ekin << G4endl; |
---|
| 3758 | } |
---|
| 3759 | |
---|
| 3760 | if( ekin1 != 0.0 ) |
---|
| 3761 | { |
---|
| 3762 | pvmx[6].setZero(); |
---|
| 3763 | wgt = ekin/ekin1; |
---|
| 3764 | ekin1 = 0.; |
---|
| 3765 | for( i=0; i < vecLen; i++ ) |
---|
| 3766 | { |
---|
| 3767 | pvMass = pv[i].getMass(); |
---|
| 3768 | ekin = pv[i].getKineticEnergy() * wgt; |
---|
| 3769 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 3770 | ekin1 += ekin; |
---|
| 3771 | pvmx[6].Add( pvmx[6], pv[i] ); |
---|
| 3772 | } |
---|
| 3773 | teta = pvmx[6].Ang( pvmx[3] ); |
---|
| 3774 | if (verboseLevel > 1) |
---|
| 3775 | G4cout << " ekin1 != 0 " << teta << " " << ekin0 << " " |
---|
| 3776 | << ekin1 << G4endl; |
---|
| 3777 | } |
---|
| 3778 | |
---|
| 3779 | // Do some smearing in the transverse direction due to Fermi motion. |
---|
| 3780 | |
---|
| 3781 | G4double ry = G4UniformRand(); |
---|
| 3782 | G4double rz = G4UniformRand(); |
---|
| 3783 | G4double rx = twopi*rz; |
---|
| 3784 | G4double a1 = std::sqrt(-2.0*std::log(ry)); |
---|
| 3785 | G4double rantarg1 = a1*std::cos(rx)*0.02*targ/G4double(vecLen); |
---|
| 3786 | G4double rantarg2 = a1*std::sin(rx)*0.02*targ/G4double(vecLen); |
---|
| 3787 | |
---|
| 3788 | for (i = 0; i < vecLen; i++) |
---|
| 3789 | pv[i].setMomentum( pv[i].getMomentum().x()+rantarg1, |
---|
| 3790 | pv[i].getMomentum().y()+rantarg2 ); |
---|
| 3791 | |
---|
| 3792 | if (verboseLevel > 1) { |
---|
| 3793 | pvmx[6].setZero(); |
---|
| 3794 | for (i = 0; i < vecLen; i++) pvmx[6].Add( pvmx[6], pv[i] ); |
---|
| 3795 | teta = pvmx[6].Ang( pvmx[3] ); |
---|
| 3796 | G4cout << " After smearing " << teta << G4endl; |
---|
| 3797 | } |
---|
| 3798 | |
---|
[1347] | 3799 | // Rotate in the direction of the primary particle momentum (z-axis). |
---|
| 3800 | // This does disturb our inclusive distributions somewhat, but it is |
---|
| 3801 | // necessary for momentum conservation. |
---|
[819] | 3802 | |
---|
[1347] | 3803 | // Also subtract binding energies and make some further corrections |
---|
| 3804 | // if required. |
---|
[819] | 3805 | |
---|
[1347] | 3806 | G4double dekin = 0.0; |
---|
| 3807 | G4int npions = 0; |
---|
| 3808 | G4double ek1 = 0.0; |
---|
| 3809 | G4double alekw, xxh; |
---|
| 3810 | G4double cfa = 0.025*((atomicWeight-1.)/120.)*std::exp(-(atomicWeight-1.)/120.); |
---|
| 3811 | G4double alem[] = {1.40, 2.30, 2.70, 3.00, 3.40, 4.60, 7.00, 10.00}; |
---|
| 3812 | G4double val0[] = {0.00, 0.40, 0.48, 0.51, 0.54, 0.60, 0.65, 0.70}; |
---|
[819] | 3813 | |
---|
[1347] | 3814 | for (i = 0; i < vecLen; i++) { |
---|
| 3815 | pv[i].Defs1( pv[i], pvI ); |
---|
| 3816 | if (atomicWeight > 1.5) { |
---|
| 3817 | ekin = Amax( 1.e-6,pv[i].getKineticEnergy() - cfa*( 1. + 0.5*normal())); |
---|
| 3818 | alekw = std::log( incidentKineticEnergy ); |
---|
| 3819 | xxh = 1.; |
---|
| 3820 | if (incidentCode == pionPlusCode || incidentCode == pionMinusCode) { |
---|
| 3821 | if (pv[i].getCode() == pionZeroCode) { |
---|
| 3822 | if (G4UniformRand() < std::log(atomicWeight)) { |
---|
| 3823 | if (alekw > alem[0]) { |
---|
| 3824 | G4int jmax = 1; |
---|
| 3825 | for (j = 1; j < 8; j++) { |
---|
| 3826 | if (alekw < alem[j]) { |
---|
| 3827 | jmax = j; |
---|
| 3828 | break; |
---|
[819] | 3829 | } |
---|
[1347] | 3830 | } |
---|
| 3831 | xxh = (val0[jmax] - val0[jmax-1])/(alem[jmax]-alem[jmax-1])*alekw |
---|
| 3832 | + val0[jmax-1] - (val0[jmax]-val0[jmax-1])/(alem[jmax]-alem[jmax-1])*alem[jmax-1]; |
---|
| 3833 | xxh = 1. - xxh; |
---|
| 3834 | } |
---|
| 3835 | } |
---|
| 3836 | } |
---|
| 3837 | } |
---|
| 3838 | dekin += ekin*(1.-xxh); |
---|
| 3839 | ekin *= xxh; |
---|
| 3840 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 3841 | pvCode = pv[i].getCode(); |
---|
| 3842 | if ((pvCode == pionPlusCode) || |
---|
| 3843 | (pvCode == pionMinusCode) || |
---|
| 3844 | (pvCode == pionZeroCode)) { |
---|
| 3845 | npions += 1; |
---|
| 3846 | ek1 += ekin; |
---|
[819] | 3847 | } |
---|
[1347] | 3848 | } |
---|
| 3849 | } |
---|
| 3850 | |
---|
[819] | 3851 | if( (ek1 > 0.0) && (npions > 0) ) |
---|
| 3852 | { |
---|
| 3853 | dekin = 1.+dekin/ek1; |
---|
| 3854 | for (i = 0; i < vecLen; i++) |
---|
| 3855 | { |
---|
| 3856 | pvCode = pv[i].getCode(); |
---|
| 3857 | if((pvCode == pionPlusCode) || (pvCode == pionMinusCode) || (pvCode == pionZeroCode)) |
---|
| 3858 | { |
---|
| 3859 | ekin = Amax( 1.0e-6, pv[i].getKineticEnergy() * dekin ); |
---|
| 3860 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 3861 | } |
---|
| 3862 | } |
---|
| 3863 | } |
---|
| 3864 | if (verboseLevel > 1) |
---|
| 3865 | { G4cout << " Lab-System " << ek1 << " " << npions << G4endl; |
---|
| 3866 | for (i=0; i<vecLen; i++) pv[i].Print(i); |
---|
| 3867 | } |
---|
| 3868 | |
---|
| 3869 | // Add black track particles |
---|
| 3870 | // The total number of particles produced is restricted to 198 |
---|
| 3871 | // this may have influence on very high energies |
---|
| 3872 | |
---|
| 3873 | if (verboseLevel > 1) G4cout << " Evaporation " << atomicWeight << " " << |
---|
| 3874 | excitationEnergyGNP << " " << excitationEnergyDTA << G4endl; |
---|
| 3875 | |
---|
| 3876 | if( atomicWeight > 1.5 ) |
---|
| 3877 | { |
---|
| 3878 | |
---|
| 3879 | G4double sprob, cost, sint, pp, eka; |
---|
| 3880 | G4int spall(0), nbl(0); |
---|
| 3881 | // sprob is the probability of self-absorption in heavy molecules |
---|
| 3882 | |
---|
| 3883 | if( incidentKineticEnergy < 5.0 ) |
---|
| 3884 | sprob = 0.0; |
---|
| 3885 | else |
---|
| 3886 | // sprob = Amin( 1.0, 0.6*std::log(incidentKineticEnergy-4.0) ); |
---|
| 3887 | sprob = Amin(1., 0.000314*atomicWeight*std::log(incidentKineticEnergy-4.)); |
---|
| 3888 | |
---|
| 3889 | // First add protons and neutrons |
---|
| 3890 | |
---|
| 3891 | if( excitationEnergyGNP >= 0.001 ) |
---|
| 3892 | { |
---|
| 3893 | // nbl = number of proton/neutron black track particles |
---|
| 3894 | // tex is their total kinetic energy (GeV) |
---|
| 3895 | |
---|
| 3896 | nbl = Poisson( (1.5+1.25*targ)*excitationEnergyGNP/ |
---|
| 3897 | (excitationEnergyGNP+excitationEnergyDTA)); |
---|
| 3898 | if( targ+nbl > atomicWeight ) nbl = (int)(atomicWeight - targ); |
---|
| 3899 | if (verboseLevel > 1) |
---|
| 3900 | G4cout << " evaporation " << targ << " " << nbl << " " |
---|
| 3901 | << sprob << G4endl; |
---|
| 3902 | spall = targ; |
---|
| 3903 | if( nbl > 0) |
---|
| 3904 | { |
---|
| 3905 | ekin = excitationEnergyGNP/nbl; |
---|
| 3906 | ekin2 = 0.0; |
---|
| 3907 | for( i=0; i<nbl; i++ ) |
---|
| 3908 | { |
---|
| 3909 | if( G4UniformRand() < sprob ) continue; |
---|
| 3910 | if( ekin2 > excitationEnergyGNP) break; |
---|
| 3911 | ran = G4UniformRand(); |
---|
| 3912 | ekin1 = -ekin*std::log(ran) - cfa*(1.0+0.5*normal()); |
---|
| 3913 | if (ekin1 < 0) ekin1 = -0.010*std::log(ran); |
---|
| 3914 | ekin2 += ekin1; |
---|
| 3915 | if( ekin2 > excitationEnergyGNP) |
---|
| 3916 | ekin1 = Amax( 1.0e-6, excitationEnergyGNP-(ekin2-ekin1) ); |
---|
| 3917 | if( G4UniformRand() > (1.0-atomicNumber/(atomicWeight))) |
---|
| 3918 | pv[vecLen].setDefinition( "Proton"); |
---|
| 3919 | else |
---|
| 3920 | pv[vecLen].setDefinition( "Neutron"); |
---|
| 3921 | spall++; |
---|
| 3922 | cost = G4UniformRand() * 2.0 - 1.0; |
---|
| 3923 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 3924 | phi = twopi * G4UniformRand(); |
---|
| 3925 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 3926 | pv[vecLen].setSide( -4 ); |
---|
| 3927 | pvMass = pv[vecLen].getMass(); |
---|
| 3928 | pv[vecLen].setTOF( 1.0 ); |
---|
| 3929 | pvEnergy = ekin1 + pvMass; |
---|
| 3930 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 3931 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 3932 | pp*sint*std::cos(phi), |
---|
| 3933 | pp*cost ); |
---|
| 3934 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 3935 | vecLen++; |
---|
| 3936 | } |
---|
| 3937 | if( (atomicWeight >= 10.0 ) && (incidentKineticEnergy <= 2.0) ) |
---|
| 3938 | { |
---|
| 3939 | G4int ika, kk = 0; |
---|
| 3940 | eka = incidentKineticEnergy; |
---|
| 3941 | if( eka > 1.0 )eka *= eka; |
---|
| 3942 | eka = Amax( 0.1, eka ); |
---|
| 3943 | ika = G4int(3.6*std::exp((atomicNumber*atomicNumber |
---|
| 3944 | /atomicWeight-35.56)/6.45)/eka); |
---|
| 3945 | if( ika > 0 ) |
---|
| 3946 | { |
---|
| 3947 | for( i=(vecLen-1); i>=0; i-- ) |
---|
| 3948 | { |
---|
| 3949 | if( (pv[i].getCode() == protonCode) && pv[i].getFlag() ) |
---|
| 3950 | { |
---|
| 3951 | pTemp = pv[i]; |
---|
| 3952 | pv[i].setDefinition( "Neutron"); |
---|
| 3953 | pv[i].setMomentumAndUpdate(pTemp.getMomentum()); |
---|
| 3954 | if (verboseLevel > 1) pv[i].Print(i); |
---|
| 3955 | if( ++kk > ika ) break; |
---|
| 3956 | } |
---|
| 3957 | } |
---|
| 3958 | } |
---|
| 3959 | } |
---|
| 3960 | } |
---|
| 3961 | } |
---|
| 3962 | |
---|
| 3963 | // Finished adding proton/neutron black track particles |
---|
| 3964 | // now, try to add deuterons, tritons and alphas |
---|
| 3965 | |
---|
| 3966 | if( excitationEnergyDTA >= 0.001 ) |
---|
| 3967 | { |
---|
| 3968 | nbl = Poisson( (1.5+1.25*targ)*excitationEnergyDTA |
---|
| 3969 | /(excitationEnergyGNP+excitationEnergyDTA)); |
---|
| 3970 | |
---|
| 3971 | // nbl is the number of deutrons, tritons, and alphas produced |
---|
| 3972 | |
---|
| 3973 | if( nbl > 0 ) |
---|
| 3974 | { |
---|
| 3975 | ekin = excitationEnergyDTA/nbl; |
---|
| 3976 | ekin2 = 0.0; |
---|
| 3977 | for( i=0; i<nbl; i++ ) |
---|
| 3978 | { |
---|
| 3979 | if( G4UniformRand() < sprob ) continue; |
---|
| 3980 | if( ekin2 > excitationEnergyDTA) break; |
---|
| 3981 | ran = G4UniformRand(); |
---|
| 3982 | ekin1 = -ekin*std::log(ran)-cfa*(1.+0.5*normal()); |
---|
| 3983 | if( ekin1 < 0.0 ) ekin1 = -0.010*std::log(ran); |
---|
| 3984 | ekin2 += ekin1; |
---|
| 3985 | if( ekin2 > excitationEnergyDTA) |
---|
| 3986 | ekin1 = Amax( 1.0e-6, excitationEnergyDTA-(ekin2-ekin1)); |
---|
| 3987 | cost = G4UniformRand()*2.0 - 1.0; |
---|
| 3988 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 3989 | phi = twopi*G4UniformRand(); |
---|
| 3990 | ran = G4UniformRand(); |
---|
| 3991 | if( ran <= 0.60 ) |
---|
| 3992 | pv[vecLen].setDefinition( "Deuteron"); |
---|
| 3993 | else if (ran <= 0.90) |
---|
| 3994 | pv[vecLen].setDefinition( "Triton"); |
---|
| 3995 | else |
---|
| 3996 | pv[vecLen].setDefinition( "Alpha"); |
---|
| 3997 | spall += (int)(pv[vecLen].getMass() * 1.066); |
---|
| 3998 | if( spall > atomicWeight ) break; |
---|
| 3999 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 4000 | pv[vecLen].setSide( -4 ); |
---|
| 4001 | pvMass = pv[vecLen].getMass(); |
---|
| 4002 | pv[vecLen].setSide( pv[vecLen].getCode()); |
---|
| 4003 | pv[vecLen].setTOF( 1.0 ); |
---|
| 4004 | pvEnergy = pvMass + ekin1; |
---|
| 4005 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 4006 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 4007 | pp*sint*std::cos(phi), |
---|
| 4008 | pp*cost ); |
---|
| 4009 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 4010 | vecLen++; |
---|
| 4011 | } |
---|
| 4012 | } |
---|
| 4013 | } |
---|
| 4014 | } |
---|
| 4015 | if( centerOfMassEnergy <= (4.0+G4UniformRand()) ) |
---|
| 4016 | { |
---|
| 4017 | for( i=0; i<vecLen; i++ ) |
---|
| 4018 | { |
---|
| 4019 | G4double etb = pv[i].getKineticEnergy(); |
---|
| 4020 | if( etb >= incidentKineticEnergy ) |
---|
| 4021 | pv[i].setKineticEnergyAndUpdate( incidentKineticEnergy ); |
---|
| 4022 | } |
---|
| 4023 | } |
---|
| 4024 | |
---|
| 4025 | // Calculate time delay for nuclear reactions |
---|
| 4026 | |
---|
| 4027 | G4double tof = incidentTOF; |
---|
| 4028 | if( (atomicWeight >= 1.5) && (atomicWeight <= 230.0) |
---|
| 4029 | && (incidentKineticEnergy <= 0.2) ) |
---|
| 4030 | tof -= 500.0 * std::exp(-incidentKineticEnergy /0.04) * std::log( G4UniformRand() ); |
---|
| 4031 | for ( i=0; i < vecLen; i++) |
---|
| 4032 | { |
---|
| 4033 | |
---|
| 4034 | pv[i].setTOF ( tof ); |
---|
| 4035 | // vec[i].SetTOF ( tof ); |
---|
| 4036 | } |
---|
| 4037 | |
---|
| 4038 | for(i=0; i<vecLen; i++) |
---|
| 4039 | { |
---|
| 4040 | if(pv[i].getName() == "KaonZero" || pv[i].getName() == "AntiKaonZero") |
---|
| 4041 | { |
---|
| 4042 | pvmx[0] = pv[i]; |
---|
| 4043 | if(G4UniformRand() < 0.5) pv[i].setDefinition("KaonZeroShort"); |
---|
| 4044 | else pv[i].setDefinition("KaonZeroLong"); |
---|
| 4045 | pv[i].setMomentumAndUpdate(pvmx[0].getMomentum()); |
---|
| 4046 | } |
---|
| 4047 | } |
---|
| 4048 | |
---|
| 4049 | successful = true; |
---|
| 4050 | delete [] pvmx; |
---|
| 4051 | return; |
---|
| 4052 | } |
---|
| 4053 | |
---|
| 4054 | void |
---|
[1347] | 4055 | G4HEInelastic::MediumEnergyClusterProduction(G4bool& successful, |
---|
[819] | 4056 | G4HEVector pv[], |
---|
[1347] | 4057 | G4int& vecLen, |
---|
| 4058 | G4double& excitationEnergyGNP, |
---|
| 4059 | G4double& excitationEnergyDTA, |
---|
| 4060 | const G4HEVector& incidentParticle, |
---|
| 4061 | const G4HEVector& targetParticle, |
---|
[819] | 4062 | G4double atomicWeight, |
---|
| 4063 | G4double atomicNumber) |
---|
[1347] | 4064 | { |
---|
[819] | 4065 | // For low multiplicity in the first intranuclear interaction the cascading |
---|
| 4066 | // process as described in G4HEInelastic::MediumEnergyCascading does not work |
---|
| 4067 | // satisfactorily. From experimental data it is strongly suggested to use |
---|
| 4068 | // a two- body resonance model. |
---|
| 4069 | // |
---|
| 4070 | // All quantities on the G4HEVector Array pv are in GeV- units. |
---|
| 4071 | |
---|
[1347] | 4072 | G4int protonCode = Proton.getCode(); |
---|
| 4073 | G4double protonMass = Proton.getMass(); |
---|
| 4074 | G4int neutronCode = Neutron.getCode(); |
---|
| 4075 | G4double kaonPlusMass = KaonPlus.getMass(); |
---|
| 4076 | G4int pionPlusCode = PionPlus.getCode(); |
---|
| 4077 | G4int pionZeroCode = PionZero.getCode(); |
---|
| 4078 | G4int pionMinusCode = PionMinus.getCode(); |
---|
| 4079 | G4String mesonType = PionPlus.getType(); |
---|
| 4080 | G4String baryonType = Proton.getType(); |
---|
| 4081 | G4String antiBaryonType = AntiProton.getType(); |
---|
[819] | 4082 | |
---|
[1347] | 4083 | G4double targetMass = targetParticle.getMass(); |
---|
[819] | 4084 | |
---|
[1347] | 4085 | G4int incidentCode = incidentParticle.getCode(); |
---|
| 4086 | G4double incidentMass = incidentParticle.getMass(); |
---|
| 4087 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); |
---|
| 4088 | G4double incidentEnergy = incidentParticle.getEnergy(); |
---|
| 4089 | G4double incidentKineticEnergy = incidentParticle.getKineticEnergy(); |
---|
| 4090 | G4String incidentType = incidentParticle.getType(); |
---|
[819] | 4091 | // G4double incidentTOF = incidentParticle.getTOF(); |
---|
[1347] | 4092 | G4double incidentTOF = 0.; |
---|
[819] | 4093 | |
---|
[1347] | 4094 | // some local variables |
---|
[819] | 4095 | |
---|
[1347] | 4096 | G4int i, j; |
---|
[819] | 4097 | |
---|
[1347] | 4098 | if (verboseLevel > 1) |
---|
| 4099 | G4cout << " G4HEInelastic::MediumEnergyClusterProduction " << G4endl; |
---|
[819] | 4100 | |
---|
[1347] | 4101 | if (incidentTotalMomentum < 0.01) { |
---|
| 4102 | successful = false; |
---|
| 4103 | return; |
---|
| 4104 | } |
---|
| 4105 | G4double centerOfMassEnergy = std::sqrt( sqr(incidentMass) + sqr(targetMass) |
---|
| 4106 | +2.*targetMass*incidentEnergy); |
---|
[819] | 4107 | |
---|
[1347] | 4108 | G4HEVector pvI = incidentParticle; // for the incident particle |
---|
| 4109 | pvI.setSide( 1 ); |
---|
[819] | 4110 | |
---|
[1347] | 4111 | G4HEVector pvT = targetParticle; // for the target particle |
---|
| 4112 | pvT.setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 4113 | pvT.setSide( -1 ); |
---|
| 4114 | pvT.setTOF( -1.); |
---|
[819] | 4115 | |
---|
[1347] | 4116 | // Distribute particles in forward and backward hemispheres. Note that |
---|
| 4117 | // only low multiplicity events from FirstIntInNuc.... should go into |
---|
| 4118 | // this routine. |
---|
[819] | 4119 | |
---|
[1347] | 4120 | G4int targ = 0; |
---|
| 4121 | G4int ifor = 0; |
---|
| 4122 | G4int iback = 0; |
---|
| 4123 | G4int pvCode; |
---|
| 4124 | G4double pvMass, pvEnergy; |
---|
[819] | 4125 | |
---|
| 4126 | pv[0].setSide( 1 ); |
---|
| 4127 | pv[1].setSide( -1 ); |
---|
| 4128 | for(i = 0; i < vecLen; i++) |
---|
| 4129 | { |
---|
| 4130 | if (i > 1) |
---|
| 4131 | { |
---|
| 4132 | if( G4UniformRand() < 0.5) |
---|
| 4133 | { |
---|
| 4134 | pv[i].setSide( 1 ); |
---|
| 4135 | if (++ifor > 18) |
---|
| 4136 | { |
---|
| 4137 | pv[i].setSide( -1 ); |
---|
| 4138 | ifor--; |
---|
| 4139 | iback++; |
---|
| 4140 | } |
---|
| 4141 | } |
---|
| 4142 | else |
---|
| 4143 | { |
---|
| 4144 | pv[i].setSide( -1 ); |
---|
| 4145 | if (++iback > 18) |
---|
| 4146 | { |
---|
| 4147 | pv[i].setSide( 1 ); |
---|
| 4148 | ifor++; |
---|
| 4149 | iback--; |
---|
| 4150 | } |
---|
| 4151 | } |
---|
| 4152 | } |
---|
| 4153 | |
---|
| 4154 | pvCode = pv[i].getCode(); |
---|
| 4155 | |
---|
| 4156 | if ( ( (incidentCode == protonCode) || (incidentCode == neutronCode) |
---|
| 4157 | || (incidentType == mesonType) ) |
---|
| 4158 | && ( (pvCode == pionPlusCode) || (pvCode == pionMinusCode) ) |
---|
| 4159 | && ( (G4UniformRand() < (10.-incidentTotalMomentum)/6.) ) |
---|
| 4160 | && ( (G4UniformRand() < atomicWeight/300.) ) ) |
---|
| 4161 | { |
---|
| 4162 | if (G4UniformRand() > atomicNumber/atomicWeight) |
---|
| 4163 | pv[i].setDefinition( "Neutron"); |
---|
| 4164 | else |
---|
| 4165 | pv[i].setDefinition( "Proton"); |
---|
| 4166 | targ++; |
---|
| 4167 | } |
---|
| 4168 | pv[i].setTOF( incidentTOF ); |
---|
| 4169 | } |
---|
| 4170 | G4double tb = 2. * iback; |
---|
| 4171 | if (centerOfMassEnergy < (2+G4UniformRand())) tb = (2.*iback + vecLen)/2.; |
---|
| 4172 | |
---|
| 4173 | G4double nucsup[] = { 1.0, 0.8, 0.6, 0.5, 0.4}; |
---|
| 4174 | |
---|
[1347] | 4175 | G4double xtarg = Amax(0.01, (0.312+0.2*std::log(std::log(centerOfMassEnergy*centerOfMassEnergy))) |
---|
[819] | 4176 | * (std::pow(atomicWeight,0.33)-1.) * tb); |
---|
| 4177 | G4int ntarg = Poisson(xtarg); |
---|
| 4178 | if (ntarg > 0) |
---|
| 4179 | { |
---|
| 4180 | G4int ipx = Imin(4, (G4int)(incidentTotalMomentum/3.)); |
---|
| 4181 | for (i=0; i < ntarg; i++) |
---|
| 4182 | { |
---|
| 4183 | if (G4UniformRand() < nucsup[ipx] ) |
---|
| 4184 | { |
---|
| 4185 | if (G4UniformRand() < (1.- atomicNumber/atomicWeight)) |
---|
| 4186 | pv[vecLen].setDefinition( "Neutron"); |
---|
| 4187 | else |
---|
| 4188 | pv[vecLen].setDefinition( "Proton"); |
---|
| 4189 | targ++; |
---|
| 4190 | } |
---|
| 4191 | else |
---|
| 4192 | { |
---|
| 4193 | G4double ran = G4UniformRand(); |
---|
| 4194 | if (ran < 0.3333 ) |
---|
| 4195 | pv[vecLen].setDefinition( "PionPlus"); |
---|
| 4196 | else if (ran < 0.6666) |
---|
| 4197 | pv[vecLen].setDefinition( "PionZero"); |
---|
| 4198 | else |
---|
| 4199 | pv[vecLen].setDefinition( "PionMinus"); |
---|
| 4200 | } |
---|
| 4201 | pv[vecLen].setSide( -2 ); |
---|
| 4202 | pv[vecLen].setFlag( true ); |
---|
| 4203 | pv[vecLen].setTOF( incidentTOF ); |
---|
| 4204 | vecLen++; |
---|
| 4205 | } |
---|
| 4206 | } |
---|
| 4207 | |
---|
| 4208 | // Mark leading particles for incident strange particles and antibaryons, |
---|
| 4209 | // for all other we assume that the first and second particle are the |
---|
| 4210 | // leading particles. |
---|
| 4211 | // We need this later for kinematic aspects of strangeness conservation. |
---|
| 4212 | |
---|
| 4213 | G4int lead = 0; |
---|
| 4214 | G4HEVector leadParticle; |
---|
| 4215 | if( (incidentMass >= kaonPlusMass-0.05) && (incidentCode != protonCode) |
---|
| 4216 | && (incidentCode != neutronCode) ) |
---|
| 4217 | { |
---|
| 4218 | G4double pMass = pv[0].getMass(); |
---|
| 4219 | G4int pCode = pv[0].getCode(); |
---|
| 4220 | if( (pMass >= kaonPlusMass-0.05) && (pCode != protonCode) |
---|
| 4221 | && (pCode != neutronCode) ) |
---|
| 4222 | { |
---|
| 4223 | lead = pCode; |
---|
| 4224 | leadParticle = pv[0]; |
---|
| 4225 | } |
---|
| 4226 | else |
---|
| 4227 | { |
---|
| 4228 | pMass = pv[1].getMass(); |
---|
| 4229 | pCode = pv[1].getCode(); |
---|
| 4230 | if( (pMass >= kaonPlusMass-0.05) && (pCode != protonCode) |
---|
| 4231 | && (pCode != neutronCode) ) |
---|
| 4232 | { |
---|
| 4233 | lead = pCode; |
---|
| 4234 | leadParticle = pv[1]; |
---|
| 4235 | } |
---|
| 4236 | } |
---|
| 4237 | } |
---|
| 4238 | |
---|
| 4239 | if (verboseLevel > 1) { |
---|
| 4240 | G4cout << " pv Vector after initialization " << vecLen << G4endl; |
---|
| 4241 | pvI.Print(-1); |
---|
| 4242 | pvT.Print(-1); |
---|
| 4243 | for (i=0; i < vecLen ; i++) pv[i].Print(i); |
---|
| 4244 | } |
---|
| 4245 | |
---|
| 4246 | G4double tavai = 0.; |
---|
| 4247 | for(i=0;i<vecLen;i++) if(pv[i].getSide() != -2) tavai += pv[i].getMass(); |
---|
| 4248 | |
---|
| 4249 | while (tavai > centerOfMassEnergy) |
---|
| 4250 | { |
---|
| 4251 | for (i=vecLen-1; i >= 0; i--) |
---|
| 4252 | { |
---|
| 4253 | if (pv[i].getSide() != -2) |
---|
| 4254 | { |
---|
| 4255 | tavai -= pv[i].getMass(); |
---|
| 4256 | if( i != vecLen-1) |
---|
| 4257 | { |
---|
| 4258 | for (j=i; j < vecLen; j++) |
---|
| 4259 | { |
---|
| 4260 | pv[j] = pv[j+1]; |
---|
| 4261 | } |
---|
| 4262 | } |
---|
| 4263 | if ( --vecLen < 2) |
---|
| 4264 | { |
---|
| 4265 | successful = false; |
---|
| 4266 | return; |
---|
| 4267 | } |
---|
| 4268 | break; |
---|
| 4269 | } |
---|
| 4270 | } |
---|
| 4271 | } |
---|
| 4272 | |
---|
| 4273 | // Now produce 3 Clusters: |
---|
| 4274 | // 1. forward cluster |
---|
| 4275 | // 2. backward meson cluster |
---|
| 4276 | // 3. backward nucleon cluster |
---|
| 4277 | |
---|
| 4278 | G4double rmc0 = 0., rmd0 = 0., rme0 = 0.; |
---|
| 4279 | G4int ntc = 0, ntd = 0, nte = 0; |
---|
| 4280 | |
---|
| 4281 | for (i=0; i < vecLen; i++) |
---|
| 4282 | { |
---|
| 4283 | if(pv[i].getSide() > 0) |
---|
| 4284 | { |
---|
| 4285 | if(ntc < 17) |
---|
| 4286 | { |
---|
| 4287 | rmc0 += pv[i].getMass(); |
---|
| 4288 | ntc++; |
---|
| 4289 | } |
---|
| 4290 | else |
---|
| 4291 | { |
---|
| 4292 | if(ntd < 17) |
---|
| 4293 | { |
---|
| 4294 | pv[i].setSide(-1); |
---|
| 4295 | rmd0 += pv[i].getMass(); |
---|
| 4296 | ntd++; |
---|
| 4297 | } |
---|
| 4298 | else |
---|
| 4299 | { |
---|
| 4300 | pv[i].setSide(-2); |
---|
| 4301 | rme0 += pv[i].getMass(); |
---|
| 4302 | nte++; |
---|
| 4303 | } |
---|
| 4304 | } |
---|
| 4305 | } |
---|
| 4306 | else if (pv[i].getSide() == -1) |
---|
| 4307 | { |
---|
| 4308 | if(ntd < 17) |
---|
| 4309 | { |
---|
| 4310 | rmd0 += pv[i].getMass(); |
---|
| 4311 | ntd++; |
---|
| 4312 | } |
---|
| 4313 | else |
---|
| 4314 | { |
---|
| 4315 | pv[i].setSide(-2); |
---|
| 4316 | rme0 += pv[i].getMass(); |
---|
| 4317 | nte++; |
---|
| 4318 | } |
---|
| 4319 | } |
---|
| 4320 | else |
---|
| 4321 | { |
---|
| 4322 | rme0 += pv[i].getMass(); |
---|
| 4323 | nte++; |
---|
| 4324 | } |
---|
| 4325 | } |
---|
| 4326 | |
---|
| 4327 | G4double cpar[] = {0.6, 0.6, 0.35, 0.15, 0.10}; |
---|
| 4328 | G4double gpar[] = {2.6, 2.6, 1.80, 1.30, 1.20}; |
---|
| 4329 | |
---|
| 4330 | G4double rmc = rmc0, rmd = rmd0, rme = rme0; |
---|
| 4331 | G4int ntc1 = Imin(4,ntc-1); |
---|
| 4332 | G4int ntd1 = Imin(4,ntd-1); |
---|
| 4333 | G4int nte1 = Imin(4,nte-1); |
---|
| 4334 | if (ntc > 1) rmc = rmc0 + std::pow(-std::log(1.-G4UniformRand()),cpar[ntc1])/gpar[ntc1]; |
---|
| 4335 | if (ntd > 1) rmd = rmd0 + std::pow(-std::log(1.-G4UniformRand()),cpar[ntd1])/gpar[ntd1]; |
---|
| 4336 | if (nte > 1) rme = rme0 + std::pow(-std::log(1.-G4UniformRand()),cpar[nte1])/gpar[nte1]; |
---|
| 4337 | while( (rmc+rmd) > centerOfMassEnergy) |
---|
| 4338 | { |
---|
| 4339 | if ((rmc == rmc0) && (rmd == rmd0)) |
---|
| 4340 | { |
---|
| 4341 | rmd *= 0.999*centerOfMassEnergy/(rmc+rmd); |
---|
| 4342 | rmc *= 0.999*centerOfMassEnergy/(rmc+rmd); |
---|
| 4343 | } |
---|
| 4344 | else |
---|
| 4345 | { |
---|
| 4346 | rmc = 0.1*rmc0 + 0.9*rmc; |
---|
| 4347 | rmd = 0.1*rmd0 + 0.9*rmd; |
---|
| 4348 | } |
---|
| 4349 | } |
---|
| 4350 | if(verboseLevel > 1) |
---|
| 4351 | G4cout << " Cluster Masses: " << ntc << " " << rmc << " " << ntd << " " |
---|
| 4352 | << rmd << " " << nte << " " << rme << G4endl; |
---|
| 4353 | |
---|
| 4354 | |
---|
| 4355 | G4HEVector* pvmx = new G4HEVector[11]; |
---|
| 4356 | |
---|
| 4357 | pvmx[1].setMass( incidentMass); |
---|
| 4358 | pvmx[1].setMomentumAndUpdate( 0., 0., incidentTotalMomentum); |
---|
| 4359 | pvmx[2].setMass( targetMass); |
---|
| 4360 | pvmx[2].setMomentumAndUpdate( 0., 0., 0.); |
---|
| 4361 | pvmx[0].Add( pvmx[1], pvmx[2] ); |
---|
| 4362 | pvmx[1].Lor( pvmx[1], pvmx[0] ); |
---|
| 4363 | pvmx[2].Lor( pvmx[2], pvmx[0] ); |
---|
| 4364 | |
---|
| 4365 | G4double pf = std::sqrt(Amax(0.0001, sqr(sqr(centerOfMassEnergy) + rmd*rmd -rmc*rmc) |
---|
| 4366 | - 4*sqr(centerOfMassEnergy)*rmd*rmd))/(2.*centerOfMassEnergy); |
---|
| 4367 | pvmx[3].setMass( rmc ); |
---|
| 4368 | pvmx[4].setMass( rmd ); |
---|
| 4369 | pvmx[3].setEnergy( std::sqrt(pf*pf + rmc*rmc) ); |
---|
| 4370 | pvmx[4].setEnergy( std::sqrt(pf*pf + rmd*rmd) ); |
---|
| 4371 | |
---|
| 4372 | G4double tvalue = -MAXFLOAT; |
---|
| 4373 | G4double bvalue = Amax(0.01, 4.0 + 1.6*std::log(incidentTotalMomentum)); |
---|
| 4374 | if (bvalue != 0.0) tvalue = std::log(G4UniformRand())/bvalue; |
---|
| 4375 | G4double pin = pvmx[1].Length(); |
---|
| 4376 | G4double tacmin = sqr( pvmx[1].getEnergy() - pvmx[3].getEnergy()) - sqr( pin - pf); |
---|
| 4377 | G4double ctet = Amax(-1., Amin(1., 1.+2.*(tvalue-tacmin)/Amax(1.e-10, 4.*pin*pf))); |
---|
| 4378 | G4double stet = std::sqrt(Amax(0., 1.0 - ctet*ctet)); |
---|
| 4379 | G4double phi = twopi * G4UniformRand(); |
---|
| 4380 | pvmx[3].setMomentum( pf * stet * std::sin(phi), |
---|
| 4381 | pf * stet * std::cos(phi), |
---|
| 4382 | pf * ctet ); |
---|
| 4383 | pvmx[4].Smul( pvmx[3], -1.); |
---|
| 4384 | |
---|
| 4385 | if (nte > 0) |
---|
| 4386 | { |
---|
| 4387 | G4double ekit1 = 0.04; |
---|
| 4388 | G4double ekit2 = 0.6; |
---|
| 4389 | G4double gaval = 1.2; |
---|
| 4390 | if (incidentKineticEnergy <= 5.) |
---|
| 4391 | { |
---|
| 4392 | ekit1 *= sqr(incidentKineticEnergy)/25.; |
---|
| 4393 | ekit2 *= sqr(incidentKineticEnergy)/25.; |
---|
| 4394 | } |
---|
| 4395 | G4double avalue = (1.-gaval)/(std::pow(ekit2, 1.-gaval)-std::pow(ekit1, 1.-gaval)); |
---|
| 4396 | for (i=0; i < vecLen; i++) |
---|
| 4397 | { |
---|
| 4398 | if (pv[i].getSide() == -2) |
---|
| 4399 | { |
---|
| 4400 | G4double ekit = std::pow(G4UniformRand()*(1.-gaval)/avalue +std::pow(ekit1, 1.-gaval), |
---|
| 4401 | 1./(1.-gaval)); |
---|
| 4402 | pv[i].setKineticEnergyAndUpdate( ekit ); |
---|
| 4403 | ctet = Amax(-1., Amin(1., std::log(2.23*G4UniformRand()+0.383)/0.96)); |
---|
| 4404 | stet = std::sqrt( Amax( 0.0, 1. - ctet*ctet )); |
---|
| 4405 | phi = G4UniformRand()*twopi; |
---|
| 4406 | G4double pp = pv[i].Length(); |
---|
| 4407 | pv[i].setMomentum( pp * stet * std::sin(phi), |
---|
| 4408 | pp * stet * std::cos(phi), |
---|
| 4409 | pp * ctet ); |
---|
| 4410 | pv[i].Lor( pv[i], pvmx[0] ); |
---|
| 4411 | } |
---|
| 4412 | } |
---|
| 4413 | } |
---|
| 4414 | // pvmx[1] = pvmx[3]; |
---|
| 4415 | // pvmx[2] = pvmx[4]; |
---|
| 4416 | pvmx[5].SmulAndUpdate( pvmx[3], -1.); |
---|
| 4417 | pvmx[6].SmulAndUpdate( pvmx[4], -1.); |
---|
| 4418 | |
---|
| 4419 | if (verboseLevel > 1) { |
---|
| 4420 | G4cout << " General vectors before Phase space Generation " << G4endl; |
---|
| 4421 | for (i=0; i<7; i++) pvmx[i].Print(i); |
---|
| 4422 | } |
---|
| 4423 | |
---|
| 4424 | |
---|
| 4425 | G4HEVector* tempV = new G4HEVector[18]; |
---|
| 4426 | G4bool constantCrossSection = true; |
---|
| 4427 | G4double wgt; |
---|
| 4428 | G4int npg; |
---|
| 4429 | |
---|
| 4430 | if (ntc > 1) |
---|
| 4431 | { |
---|
| 4432 | npg = 0; |
---|
| 4433 | for (i=0; i < vecLen; i++) |
---|
| 4434 | { |
---|
| 4435 | if (pv[i].getSide() > 0) |
---|
| 4436 | { |
---|
| 4437 | tempV[npg++] = pv[i]; |
---|
| 4438 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 4439 | } |
---|
| 4440 | } |
---|
| 4441 | wgt = NBodyPhaseSpace( pvmx[3].getMass(), constantCrossSection, tempV, npg); |
---|
| 4442 | |
---|
| 4443 | npg = 0; |
---|
| 4444 | for (i=0; i < vecLen; i++) |
---|
| 4445 | { |
---|
| 4446 | if (pv[i].getSide() > 0) |
---|
| 4447 | { |
---|
| 4448 | pv[i].setMomentum( tempV[npg++].getMomentum()); |
---|
| 4449 | pv[i].SmulAndUpdate( pv[i], 1. ); |
---|
| 4450 | pv[i].Lor( pv[i], pvmx[5] ); |
---|
| 4451 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 4452 | } |
---|
| 4453 | } |
---|
| 4454 | } |
---|
| 4455 | else if(ntc == 1) |
---|
| 4456 | { |
---|
| 4457 | for(i=0; i<vecLen; i++) |
---|
| 4458 | { |
---|
| 4459 | if(pv[i].getSide() > 0) pv[i].setMomentumAndUpdate(pvmx[3].getMomentum()); |
---|
| 4460 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 4461 | } |
---|
| 4462 | } |
---|
| 4463 | else |
---|
| 4464 | { |
---|
| 4465 | } |
---|
| 4466 | |
---|
| 4467 | if (ntd > 1) |
---|
| 4468 | { |
---|
| 4469 | npg = 0; |
---|
| 4470 | for (i=0; i < vecLen; i++) |
---|
| 4471 | { |
---|
| 4472 | if (pv[i].getSide() == -1) |
---|
| 4473 | { |
---|
| 4474 | tempV[npg++] = pv[i]; |
---|
| 4475 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 4476 | } |
---|
| 4477 | } |
---|
| 4478 | wgt = NBodyPhaseSpace( pvmx[4].getMass(), constantCrossSection, tempV, npg); |
---|
| 4479 | |
---|
| 4480 | npg = 0; |
---|
| 4481 | for (i=0; i < vecLen; i++) |
---|
| 4482 | { |
---|
| 4483 | if (pv[i].getSide() == -1) |
---|
| 4484 | { |
---|
| 4485 | pv[i].setMomentum( tempV[npg++].getMomentum()); |
---|
| 4486 | pv[i].SmulAndUpdate( pv[i], 1.); |
---|
| 4487 | pv[i].Lor( pv[i], pvmx[6] ); |
---|
| 4488 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 4489 | } |
---|
| 4490 | } |
---|
| 4491 | } |
---|
| 4492 | else if(ntd == 1) |
---|
| 4493 | { |
---|
| 4494 | for(i=0; i<vecLen; i++) |
---|
| 4495 | { |
---|
| 4496 | if(pv[i].getSide() == -1) pv[i].setMomentumAndUpdate(pvmx[4].getMomentum()); |
---|
| 4497 | if(verboseLevel > 1) pv[i].Print(i); |
---|
| 4498 | } |
---|
| 4499 | } |
---|
| 4500 | else |
---|
| 4501 | { |
---|
| 4502 | } |
---|
| 4503 | |
---|
| 4504 | if(verboseLevel > 1) |
---|
| 4505 | { |
---|
| 4506 | G4cout << " Vectors after PhaseSpace generation " << G4endl; |
---|
| 4507 | for(i=0;i<vecLen; i++) pv[i].Print(i); |
---|
| 4508 | } |
---|
| 4509 | |
---|
| 4510 | // Lorentz transformation in lab system |
---|
| 4511 | |
---|
| 4512 | targ = 0; |
---|
| 4513 | for( i=0; i < vecLen; i++ ) |
---|
| 4514 | { |
---|
| 4515 | if( pv[i].getType() == baryonType )targ++; |
---|
| 4516 | if( pv[i].getType() == antiBaryonType )targ++; |
---|
| 4517 | pv[i].Lor( pv[i], pvmx[2] ); |
---|
| 4518 | } |
---|
| 4519 | if (targ <1) targ =1; |
---|
| 4520 | |
---|
| 4521 | if(verboseLevel > 1) { |
---|
| 4522 | G4cout << " Transformation in Lab- System " << G4endl; |
---|
| 4523 | for(i=0; i<vecLen; i++) pv[i].Print(i); |
---|
| 4524 | } |
---|
| 4525 | |
---|
[1347] | 4526 | G4bool dum(0); |
---|
| 4527 | G4double ekin, teta; |
---|
[819] | 4528 | |
---|
[1347] | 4529 | if (lead) { |
---|
| 4530 | for (i = 0; i < vecLen; i++) { |
---|
| 4531 | if (pv[i].getCode() == lead) { |
---|
| 4532 | dum = false; |
---|
| 4533 | break; |
---|
| 4534 | } |
---|
| 4535 | } |
---|
| 4536 | // At this point dum is always false, so the following code |
---|
| 4537 | // cannot be executed. For now, comment it out. |
---|
| 4538 | /* |
---|
| 4539 | if (dum) { |
---|
| 4540 | i = 0; |
---|
[819] | 4541 | |
---|
[1347] | 4542 | if ( ( (leadParticle.getType() == baryonType || |
---|
| 4543 | leadParticle.getType() == antiBaryonType) |
---|
| 4544 | && (pv[1].getType() == baryonType || |
---|
| 4545 | pv[1].getType() == antiBaryonType)) |
---|
| 4546 | || ( (leadParticle.getType() == mesonType) |
---|
| 4547 | && (pv[1].getType() == mesonType))) { |
---|
| 4548 | i = 1; |
---|
| 4549 | } |
---|
[819] | 4550 | |
---|
[1347] | 4551 | ekin = pv[i].getKineticEnergy(); |
---|
| 4552 | pv[i] = leadParticle; |
---|
| 4553 | if (pv[i].getFlag() ) |
---|
| 4554 | pv[i].setTOF( -1.0 ); |
---|
| 4555 | else |
---|
| 4556 | pv[i].setTOF( 1.0 ); |
---|
| 4557 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 4558 | } |
---|
| 4559 | */ |
---|
| 4560 | } |
---|
[819] | 4561 | |
---|
| 4562 | pvmx[4].setMass( incidentMass); |
---|
| 4563 | pvmx[4].setMomentumAndUpdate( 0.0, 0.0, incidentTotalMomentum ); |
---|
| 4564 | |
---|
| 4565 | G4double ekin0 = pvmx[4].getKineticEnergy(); |
---|
| 4566 | |
---|
| 4567 | pvmx[5].setMass ( protonMass * targ); |
---|
| 4568 | pvmx[5].setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 4569 | |
---|
| 4570 | ekin = pvmx[4].getEnergy() + pvmx[5].getEnergy(); |
---|
| 4571 | |
---|
| 4572 | pvmx[6].Add( pvmx[4], pvmx[5] ); |
---|
| 4573 | pvmx[4].Lor( pvmx[4], pvmx[6] ); |
---|
| 4574 | pvmx[5].Lor( pvmx[5], pvmx[6] ); |
---|
| 4575 | |
---|
| 4576 | G4double tecm = pvmx[4].getEnergy() + pvmx[5].getEnergy(); |
---|
| 4577 | |
---|
| 4578 | pvmx[8].setZero(); |
---|
| 4579 | |
---|
| 4580 | G4double ekin1 = 0.0; |
---|
| 4581 | |
---|
| 4582 | for( i=0; i < vecLen; i++ ) |
---|
| 4583 | { |
---|
| 4584 | pvmx[8].Add( pvmx[8], pv[i] ); |
---|
| 4585 | ekin1 += pv[i].getKineticEnergy(); |
---|
| 4586 | ekin -= pv[i].getMass(); |
---|
| 4587 | } |
---|
| 4588 | |
---|
| 4589 | if( vecLen > 1 && vecLen < 19 ) |
---|
| 4590 | { |
---|
| 4591 | constantCrossSection = true; |
---|
| 4592 | G4HEVector pw[18]; |
---|
| 4593 | for(i=0;i<vecLen;i++) pw[i] = pv[i]; |
---|
| 4594 | wgt = NBodyPhaseSpace( tecm, constantCrossSection, pw, vecLen ); |
---|
| 4595 | ekin = 0.0; |
---|
| 4596 | for( i=0; i < vecLen; i++ ) |
---|
| 4597 | { |
---|
| 4598 | pvmx[7].setMass( pw[i].getMass()); |
---|
| 4599 | pvmx[7].setMomentum( pw[i].getMomentum() ); |
---|
| 4600 | pvmx[7].SmulAndUpdate( pvmx[7], 1.); |
---|
| 4601 | pvmx[7].Lor( pvmx[7], pvmx[5] ); |
---|
| 4602 | ekin += pvmx[7].getKineticEnergy(); |
---|
| 4603 | } |
---|
| 4604 | teta = pvmx[8].Ang( pvmx[4] ); |
---|
| 4605 | if (verboseLevel > 1) |
---|
| 4606 | G4cout << " vecLen > 1 && vecLen < 19 " << teta << " " << ekin0 |
---|
| 4607 | << " " << ekin1 << " " << ekin << G4endl; |
---|
| 4608 | } |
---|
| 4609 | |
---|
| 4610 | if( ekin1 != 0.0 ) |
---|
| 4611 | { |
---|
| 4612 | pvmx[7].setZero(); |
---|
| 4613 | wgt = ekin/ekin1; |
---|
| 4614 | ekin1 = 0.; |
---|
| 4615 | for( i=0; i < vecLen; i++ ) |
---|
| 4616 | { |
---|
| 4617 | pvMass = pv[i].getMass(); |
---|
| 4618 | ekin = pv[i].getKineticEnergy() * wgt; |
---|
| 4619 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 4620 | ekin1 += ekin; |
---|
| 4621 | pvmx[7].Add( pvmx[7], pv[i] ); |
---|
| 4622 | } |
---|
| 4623 | teta = pvmx[7].Ang( pvmx[4] ); |
---|
| 4624 | if (verboseLevel > 1) |
---|
| 4625 | G4cout << " ekin1 != 0 " << teta << " " << ekin0 << " " |
---|
| 4626 | << ekin1 << G4endl; |
---|
| 4627 | } |
---|
| 4628 | |
---|
| 4629 | // Do some smearing in the transverse direction due to Fermi motion. |
---|
| 4630 | |
---|
| 4631 | G4double ry = G4UniformRand(); |
---|
| 4632 | G4double rz = G4UniformRand(); |
---|
| 4633 | G4double rx = twopi*rz; |
---|
| 4634 | G4double a1 = std::sqrt(-2.0*std::log(ry)); |
---|
| 4635 | G4double rantarg1 = a1*std::cos(rx)*0.02*targ/G4double(vecLen); |
---|
| 4636 | G4double rantarg2 = a1*std::sin(rx)*0.02*targ/G4double(vecLen); |
---|
| 4637 | |
---|
| 4638 | for (i = 0; i < vecLen; i++) |
---|
| 4639 | pv[i].setMomentum( pv[i].getMomentum().x()+rantarg1, |
---|
| 4640 | pv[i].getMomentum().y()+rantarg2 ); |
---|
| 4641 | |
---|
| 4642 | if (verboseLevel > 1) { |
---|
| 4643 | pvmx[7].setZero(); |
---|
| 4644 | for (i = 0; i < vecLen; i++) pvmx[7].Add( pvmx[7], pv[i] ); |
---|
| 4645 | teta = pvmx[7].Ang( pvmx[4] ); |
---|
| 4646 | G4cout << " After smearing " << teta << G4endl; |
---|
| 4647 | } |
---|
| 4648 | |
---|
[1347] | 4649 | // Rotate in the direction of the primary particle momentum (z-axis). |
---|
| 4650 | // This does disturb our inclusive distributions somewhat, but it is |
---|
| 4651 | // necessary for momentum conservation. |
---|
[819] | 4652 | |
---|
[1347] | 4653 | // Also subtract binding energies and make some further corrections |
---|
| 4654 | // if required. |
---|
[819] | 4655 | |
---|
[1347] | 4656 | G4double dekin = 0.0; |
---|
| 4657 | G4int npions = 0; |
---|
| 4658 | G4double ek1 = 0.0; |
---|
| 4659 | G4double alekw, xxh; |
---|
| 4660 | G4double cfa = 0.025*((atomicWeight-1.)/120.)*std::exp(-(atomicWeight-1.)/120.); |
---|
| 4661 | G4double alem[] = {1.40, 2.30, 2.70, 3.00, 3.40, 4.60, 7.00}; |
---|
| 4662 | G4double val0[] = {0.00, 0.40, 0.48, 0.51, 0.54, 0.60, 0.65}; |
---|
[819] | 4663 | |
---|
[1347] | 4664 | for (i = 0; i < vecLen; i++) { |
---|
| 4665 | pv[i].Defs1( pv[i], pvI ); |
---|
| 4666 | if (atomicWeight > 1.5) { |
---|
| 4667 | ekin = Amax( 1.e-6,pv[i].getKineticEnergy() - cfa*( 1. + 0.5*normal())); |
---|
| 4668 | alekw = std::log( incidentKineticEnergy ); |
---|
| 4669 | xxh = 1.; |
---|
| 4670 | xxh = 1.; |
---|
| 4671 | if (incidentCode == pionPlusCode || incidentCode == pionMinusCode) { |
---|
| 4672 | if (pv[i].getCode() == pionZeroCode) { |
---|
| 4673 | if (G4UniformRand() < std::log(atomicWeight)) { |
---|
| 4674 | if (alekw > alem[0]) { |
---|
| 4675 | G4int jmax = 1; |
---|
| 4676 | for (j = 1; j < 8; j++) { |
---|
| 4677 | if (alekw < alem[j]) { |
---|
| 4678 | jmax = j; |
---|
| 4679 | break; |
---|
[819] | 4680 | } |
---|
[1347] | 4681 | } |
---|
| 4682 | xxh = (val0[jmax]-val0[jmax-1])/(alem[jmax]-alem[jmax-1])*alekw |
---|
| 4683 | + val0[jmax-1] - (val0[jmax]-val0[jmax-1])/(alem[jmax]-alem[jmax-1])*alem[jmax-1]; |
---|
| 4684 | xxh = 1. - xxh; |
---|
| 4685 | } |
---|
| 4686 | } |
---|
| 4687 | } |
---|
| 4688 | } |
---|
| 4689 | dekin += ekin*(1.-xxh); |
---|
| 4690 | ekin *= xxh; |
---|
| 4691 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 4692 | pvCode = pv[i].getCode(); |
---|
| 4693 | if ((pvCode == pionPlusCode) || |
---|
| 4694 | (pvCode == pionMinusCode) || |
---|
| 4695 | (pvCode == pionZeroCode)) { |
---|
| 4696 | npions += 1; |
---|
| 4697 | ek1 += ekin; |
---|
[819] | 4698 | } |
---|
[1347] | 4699 | } |
---|
| 4700 | } |
---|
| 4701 | |
---|
[819] | 4702 | if( (ek1 > 0.0) && (npions > 0) ) |
---|
| 4703 | { |
---|
| 4704 | dekin = 1.+dekin/ek1; |
---|
| 4705 | for (i = 0; i < vecLen; i++) |
---|
| 4706 | { |
---|
| 4707 | pvCode = pv[i].getCode(); |
---|
| 4708 | if((pvCode == pionPlusCode) || (pvCode == pionMinusCode) || (pvCode == pionZeroCode)) |
---|
| 4709 | { |
---|
| 4710 | ekin = Amax( 1.0e-6, pv[i].getKineticEnergy() * dekin ); |
---|
| 4711 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
| 4712 | } |
---|
| 4713 | } |
---|
| 4714 | } |
---|
| 4715 | if (verboseLevel > 1) |
---|
| 4716 | { G4cout << " Lab-System " << ek1 << " " << npions << G4endl; |
---|
| 4717 | for (i=0; i<vecLen; i++) pv[i].Print(i); |
---|
| 4718 | } |
---|
| 4719 | |
---|
| 4720 | // Add black track particles |
---|
| 4721 | // The total number of particles produced is restricted to 198 |
---|
| 4722 | // this may have influence on very high energies |
---|
| 4723 | |
---|
| 4724 | if (verboseLevel > 1) |
---|
| 4725 | G4cout << " Evaporation " << atomicWeight << " " |
---|
| 4726 | << excitationEnergyGNP << " " << excitationEnergyDTA << G4endl; |
---|
| 4727 | |
---|
| 4728 | if( atomicWeight > 1.5 ) |
---|
| 4729 | { |
---|
| 4730 | |
---|
| 4731 | G4double sprob, cost, sint, ekin2, ran, pp, eka; |
---|
| 4732 | G4int spall(0), nbl(0); |
---|
| 4733 | // sprob is the probability of self-absorption in heavy molecules |
---|
| 4734 | |
---|
| 4735 | if( incidentKineticEnergy < 5.0 ) |
---|
| 4736 | sprob = 0.0; |
---|
| 4737 | else |
---|
| 4738 | // sprob = Amin( 1.0, 0.6*std::log(incidentKineticEnergy-4.0) ); |
---|
| 4739 | sprob = Amin(1., 0.000314*atomicWeight*std::log(incidentKineticEnergy-4.)); |
---|
| 4740 | // First add protons and neutrons |
---|
| 4741 | |
---|
| 4742 | if( excitationEnergyGNP >= 0.001 ) |
---|
| 4743 | { |
---|
| 4744 | // nbl = number of proton/neutron black track particles |
---|
| 4745 | // tex is their total kinetic energy (GeV) |
---|
| 4746 | |
---|
| 4747 | nbl = Poisson( (1.5+1.25*targ)*excitationEnergyGNP/ |
---|
| 4748 | (excitationEnergyGNP+excitationEnergyDTA)); |
---|
| 4749 | if( targ+nbl > atomicWeight ) nbl = (int)(atomicWeight - targ); |
---|
| 4750 | if (verboseLevel > 1) |
---|
| 4751 | G4cout << " evaporation " << targ << " " << nbl << " " |
---|
| 4752 | << sprob << G4endl; |
---|
| 4753 | spall = targ; |
---|
| 4754 | if( nbl > 0) |
---|
| 4755 | { |
---|
| 4756 | ekin = excitationEnergyGNP/nbl; |
---|
| 4757 | ekin2 = 0.0; |
---|
| 4758 | for( i=0; i<nbl; i++ ) |
---|
| 4759 | { |
---|
| 4760 | if( G4UniformRand() < sprob ) continue; |
---|
| 4761 | if( ekin2 > excitationEnergyGNP) break; |
---|
| 4762 | ran = G4UniformRand(); |
---|
| 4763 | ekin1 = -ekin*std::log(ran) - cfa*(1.0+0.5*normal()); |
---|
| 4764 | if (ekin1 < 0) ekin1 = -0.010*std::log(ran); |
---|
| 4765 | ekin2 += ekin1; |
---|
| 4766 | if( ekin2 > excitationEnergyGNP ) |
---|
| 4767 | ekin1 = Amax( 1.0e-6, excitationEnergyGNP-(ekin2-ekin1) ); |
---|
| 4768 | if( G4UniformRand() > (1.0-atomicNumber/(atomicWeight))) |
---|
| 4769 | pv[vecLen].setDefinition( "Proton"); |
---|
| 4770 | else |
---|
| 4771 | pv[vecLen].setDefinition( "Neutron"); |
---|
| 4772 | spall++; |
---|
| 4773 | cost = G4UniformRand() * 2.0 - 1.0; |
---|
| 4774 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 4775 | phi = twopi * G4UniformRand(); |
---|
| 4776 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 4777 | pv[vecLen].setSide( -4 ); |
---|
| 4778 | pvMass = pv[vecLen].getMass(); |
---|
| 4779 | pv[vecLen].setTOF( 1.0 ); |
---|
| 4780 | pvEnergy = ekin1 + pvMass; |
---|
| 4781 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 4782 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 4783 | pp*sint*std::cos(phi), |
---|
| 4784 | pp*cost ); |
---|
| 4785 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 4786 | vecLen++; |
---|
| 4787 | } |
---|
| 4788 | if( (atomicWeight >= 10.0 ) && (incidentKineticEnergy <= 2.0) ) |
---|
| 4789 | { |
---|
| 4790 | G4int ika, kk = 0; |
---|
| 4791 | eka = incidentKineticEnergy; |
---|
| 4792 | if( eka > 1.0 )eka *= eka; |
---|
| 4793 | eka = Amax( 0.1, eka ); |
---|
| 4794 | ika = G4int(3.6*std::exp((atomicNumber*atomicNumber |
---|
| 4795 | /atomicWeight-35.56)/6.45)/eka); |
---|
| 4796 | if( ika > 0 ) |
---|
| 4797 | { |
---|
| 4798 | for( i=(vecLen-1); i>=0; i-- ) |
---|
| 4799 | { |
---|
| 4800 | if( (pv[i].getCode() == protonCode) && pv[i].getFlag() ) |
---|
| 4801 | { |
---|
| 4802 | G4HEVector pTemp = pv[i]; |
---|
| 4803 | pv[i].setDefinition( "Neutron"); |
---|
| 4804 | pv[i].setMomentumAndUpdate(pTemp.getMomentum()); |
---|
| 4805 | if (verboseLevel > 1) pv[i].Print(i); |
---|
| 4806 | if( ++kk > ika ) break; |
---|
| 4807 | } |
---|
| 4808 | } |
---|
| 4809 | } |
---|
| 4810 | } |
---|
| 4811 | } |
---|
| 4812 | } |
---|
| 4813 | |
---|
| 4814 | // Finished adding proton/neutron black track particles |
---|
| 4815 | // now, try to add deuterons, tritons and alphas |
---|
| 4816 | |
---|
| 4817 | if( excitationEnergyDTA >= 0.001 ) |
---|
| 4818 | { |
---|
| 4819 | nbl = Poisson( (1.5+1.25*targ)*excitationEnergyDTA |
---|
| 4820 | /(excitationEnergyGNP+excitationEnergyDTA)); |
---|
| 4821 | |
---|
| 4822 | // nbl is the number of deutrons, tritons, and alphas produced |
---|
| 4823 | |
---|
| 4824 | if( nbl > 0 ) |
---|
| 4825 | { |
---|
| 4826 | ekin = excitationEnergyDTA/nbl; |
---|
| 4827 | ekin2 = 0.0; |
---|
| 4828 | for( i=0; i<nbl; i++ ) |
---|
| 4829 | { |
---|
| 4830 | if( G4UniformRand() < sprob ) continue; |
---|
| 4831 | if( ekin2 > excitationEnergyDTA) break; |
---|
| 4832 | ran = G4UniformRand(); |
---|
| 4833 | ekin1 = -ekin*std::log(ran)-cfa*(1.+0.5*normal()); |
---|
| 4834 | if( ekin1 < 0.0 ) ekin1 = -0.010*std::log(ran); |
---|
| 4835 | ekin2 += ekin1; |
---|
| 4836 | if( ekin2 > excitationEnergyDTA) |
---|
| 4837 | ekin1 = Amax( 1.0e-6, excitationEnergyDTA-(ekin2-ekin1)); |
---|
| 4838 | cost = G4UniformRand()*2.0 - 1.0; |
---|
| 4839 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 4840 | phi = twopi*G4UniformRand(); |
---|
| 4841 | ran = G4UniformRand(); |
---|
| 4842 | if( ran <= 0.60 ) |
---|
| 4843 | pv[vecLen].setDefinition( "Deuteron"); |
---|
| 4844 | else if (ran <= 0.90) |
---|
| 4845 | pv[vecLen].setDefinition( "Triton"); |
---|
| 4846 | else |
---|
| 4847 | pv[vecLen].setDefinition( "Alpha"); |
---|
| 4848 | spall += (int)(pv[vecLen].getMass() * 1.066); |
---|
| 4849 | if( spall > atomicWeight ) break; |
---|
| 4850 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 4851 | pv[vecLen].setSide( -4 ); |
---|
| 4852 | pvMass = pv[vecLen].getMass(); |
---|
| 4853 | pv[vecLen].setTOF( 1.0 ); |
---|
| 4854 | pvEnergy = pvMass + ekin1; |
---|
| 4855 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 4856 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 4857 | pp*sint*std::cos(phi), |
---|
| 4858 | pp*cost ); |
---|
| 4859 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 4860 | vecLen++; |
---|
| 4861 | } |
---|
| 4862 | } |
---|
| 4863 | } |
---|
| 4864 | } |
---|
| 4865 | if( centerOfMassEnergy <= (4.0+G4UniformRand()) ) |
---|
| 4866 | { |
---|
| 4867 | for( i=0; i<vecLen; i++ ) |
---|
| 4868 | { |
---|
| 4869 | G4double etb = pv[i].getKineticEnergy(); |
---|
| 4870 | if( etb >= incidentKineticEnergy ) |
---|
| 4871 | pv[i].setKineticEnergyAndUpdate( incidentKineticEnergy ); |
---|
| 4872 | } |
---|
| 4873 | } |
---|
| 4874 | |
---|
| 4875 | // Calculate time delay for nuclear reactions |
---|
| 4876 | |
---|
| 4877 | G4double tof = incidentTOF; |
---|
| 4878 | if( (atomicWeight >= 1.5) && (atomicWeight <= 230.0) |
---|
| 4879 | && (incidentKineticEnergy <= 0.2) ) |
---|
| 4880 | tof -= 500.0 * std::exp(-incidentKineticEnergy /0.04) * std::log( G4UniformRand() ); |
---|
| 4881 | for ( i=0; i < vecLen; i++) |
---|
| 4882 | { |
---|
| 4883 | |
---|
| 4884 | pv[i].setTOF ( tof ); |
---|
| 4885 | // vec[i].SetTOF ( tof ); |
---|
| 4886 | } |
---|
| 4887 | |
---|
| 4888 | for(i=0; i<vecLen; i++) |
---|
| 4889 | { |
---|
| 4890 | if(pv[i].getName() == "KaonZero" || pv[i].getName() == "AntiKaonZero") |
---|
| 4891 | { |
---|
| 4892 | pvmx[0] = pv[i]; |
---|
| 4893 | if(G4UniformRand() < 0.5) pv[i].setDefinition("KaonZeroShort"); |
---|
| 4894 | else pv[i].setDefinition("KaonZeroLong"); |
---|
| 4895 | pv[i].setMomentumAndUpdate(pvmx[0].getMomentum()); |
---|
| 4896 | } |
---|
| 4897 | } |
---|
| 4898 | |
---|
| 4899 | successful = true; |
---|
| 4900 | delete [] pvmx; |
---|
| 4901 | delete [] tempV; |
---|
| 4902 | return; |
---|
| 4903 | } |
---|
| 4904 | |
---|
| 4905 | void |
---|
[1347] | 4906 | G4HEInelastic::QuasiElasticScattering(G4bool& successful, |
---|
| 4907 | G4HEVector pv[], |
---|
| 4908 | G4int& vecLen, |
---|
| 4909 | G4double& excitationEnergyGNP, |
---|
| 4910 | G4double& excitationEnergyDTA, |
---|
| 4911 | const G4HEVector& incidentParticle, |
---|
| 4912 | const G4HEVector& targetParticle, |
---|
| 4913 | G4double atomicWeight, |
---|
| 4914 | G4double atomicNumber) |
---|
| 4915 | { |
---|
| 4916 | // if the Cascading or Resonance - model fails, we try this, |
---|
| 4917 | // QuasiElasticScattering. |
---|
| 4918 | // |
---|
| 4919 | // All quantities on the G4HEVector Array pv are in GeV- units. |
---|
[819] | 4920 | |
---|
[1347] | 4921 | G4int protonCode = Proton.getCode(); |
---|
| 4922 | G4String mesonType = PionPlus.getType(); |
---|
| 4923 | G4String baryonType = Proton.getType(); |
---|
| 4924 | G4String antiBaryonType = AntiProton.getType(); |
---|
[819] | 4925 | |
---|
[1347] | 4926 | G4double targetMass = targetParticle.getMass(); |
---|
| 4927 | G4double incidentMass = incidentParticle.getMass(); |
---|
| 4928 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); |
---|
| 4929 | G4double incidentEnergy = incidentParticle.getEnergy(); |
---|
| 4930 | G4double incidentKineticEnergy = incidentParticle.getKineticEnergy(); |
---|
| 4931 | G4String incidentType = incidentParticle.getType(); |
---|
[819] | 4932 | // G4double incidentTOF = incidentParticle.getTOF(); |
---|
[1347] | 4933 | G4double incidentTOF = 0.; |
---|
[819] | 4934 | |
---|
[1347] | 4935 | // some local variables |
---|
| 4936 | G4int i; |
---|
[819] | 4937 | |
---|
[1347] | 4938 | if (verboseLevel > 1) |
---|
| 4939 | G4cout << " G4HEInelastic::QuasiElasticScattering " << G4endl; |
---|
[819] | 4940 | |
---|
[1347] | 4941 | if (incidentTotalMomentum < 0.01 || vecLen < 2) { |
---|
| 4942 | successful = false; |
---|
| 4943 | return; |
---|
| 4944 | } |
---|
[819] | 4945 | |
---|
[1347] | 4946 | G4double centerOfMassEnergy = std::sqrt( sqr(incidentMass) + sqr(targetMass) |
---|
| 4947 | +2.*targetMass*incidentEnergy); |
---|
[819] | 4948 | |
---|
[1347] | 4949 | G4HEVector pvI = incidentParticle; // for the incident particle |
---|
| 4950 | pvI.setSide( 1 ); |
---|
[819] | 4951 | |
---|
[1347] | 4952 | G4HEVector pvT = targetParticle; // for the target particle |
---|
| 4953 | pvT.setMomentumAndUpdate( 0.0, 0.0, 0.0 ); |
---|
| 4954 | pvT.setSide( -1 ); |
---|
| 4955 | pvT.setTOF( -1.); |
---|
[819] | 4956 | |
---|
[1347] | 4957 | G4HEVector* pvmx = new G4HEVector[3]; |
---|
[819] | 4958 | |
---|
[1347] | 4959 | if (atomicWeight > 1.5) { |
---|
| 4960 | // for the following case better use ElasticScattering |
---|
| 4961 | if ( (pvI.getCode() == pv[0].getCode() ) |
---|
| 4962 | && (pvT.getCode() == pv[1].getCode() ) |
---|
| 4963 | && (excitationEnergyGNP < 0.001) |
---|
| 4964 | && (excitationEnergyDTA < 0.001) ) { |
---|
| 4965 | successful = false; |
---|
| 4966 | delete [] pvmx; |
---|
| 4967 | return; |
---|
| 4968 | } |
---|
| 4969 | } |
---|
[819] | 4970 | |
---|
[1347] | 4971 | pv[0].setSide( 1 ); |
---|
| 4972 | pv[0].setFlag( false ); |
---|
| 4973 | pv[0].setTOF( incidentTOF); |
---|
| 4974 | pv[0].setMomentumAndUpdate( incidentParticle.getMomentum() ); |
---|
| 4975 | pv[1].setSide( -1 ); |
---|
| 4976 | pv[1].setFlag( false ); |
---|
| 4977 | pv[1].setTOF( incidentTOF); |
---|
| 4978 | pv[1].setMomentumAndUpdate(targetParticle.getMomentum() ); |
---|
| 4979 | |
---|
| 4980 | if ((incidentTotalMomentum > 0.1) && (centerOfMassEnergy > 0.01) ) { |
---|
| 4981 | if (pv[1].getType() == mesonType) { |
---|
| 4982 | if (G4UniformRand() < 0.5) |
---|
| 4983 | pv[1].setDefinition( "Proton"); |
---|
| 4984 | else |
---|
| 4985 | pv[1].setDefinition( "Neutron"); |
---|
| 4986 | } |
---|
| 4987 | pvmx[0].Add( pvI, pvT ); |
---|
| 4988 | pvmx[1].Lor( pvI, pvmx[0] ); |
---|
| 4989 | pvmx[2].Lor( pvT, pvmx[0] ); |
---|
| 4990 | G4double pin = pvmx[1].Length(); |
---|
| 4991 | G4double bvalue = Amax(0.01 , 4.225+1.795*std::log(incidentTotalMomentum)); |
---|
| 4992 | G4double pf = sqr(sqr(centerOfMassEnergy) + sqr(pv[1].getMass()) - sqr(pv[0].getMass())) |
---|
| 4993 | - 4 * sqr(centerOfMassEnergy) * sqr(pv[1].getMass()); |
---|
| 4994 | |
---|
| 4995 | if (pf < 0.001) { |
---|
| 4996 | successful = false; |
---|
| 4997 | delete [] pvmx; |
---|
| 4998 | return; |
---|
| 4999 | } |
---|
| 5000 | pf = std::sqrt(pf)/(2.*centerOfMassEnergy); |
---|
| 5001 | G4double btrang = 4. * bvalue * pin * pf; |
---|
| 5002 | G4double exindt = -1.; |
---|
| 5003 | if (btrang < 46.) exindt += std::exp(-btrang); |
---|
| 5004 | G4double tdn = std::log(1. + G4UniformRand()*exindt)/btrang; |
---|
| 5005 | G4double ctet = Amax( -1., Amin(1., 1. + 2.*tdn)); |
---|
| 5006 | G4double stet = std::sqrt((1.-ctet)*(1.+ctet)); |
---|
| 5007 | G4double phi = twopi * G4UniformRand(); |
---|
| 5008 | pv[0].setMomentumAndUpdate( pf*stet*std::sin(phi), |
---|
| 5009 | pf*stet*std::cos(phi), |
---|
| 5010 | pf*ctet ); |
---|
| 5011 | pv[1].SmulAndUpdate( pv[0], -1.); |
---|
| 5012 | for (i = 0; i < 2; i++) { |
---|
| 5013 | // ** pv[i].Lor( pv[i], pvmx[4] ); |
---|
| 5014 | // ** DHW 1 Dec 2010 : index 4 out of range : use 0 |
---|
| 5015 | pv[i].Lor(pv[i], pvmx[0]); |
---|
| 5016 | pv[i].Defs1(pv[i], pvI); |
---|
| 5017 | if (atomicWeight > 1.5) { |
---|
| 5018 | G4double ekin = pv[i].getKineticEnergy() |
---|
| 5019 | - 0.025*((atomicWeight-1.)/120.)*std::exp(-(atomicWeight-1.)/120.) |
---|
| 5020 | *(1. + 0.5*normal()); |
---|
| 5021 | ekin = Amax(0.0001, ekin); |
---|
| 5022 | pv[i].setKineticEnergyAndUpdate( ekin ); |
---|
[819] | 5023 | } |
---|
[1347] | 5024 | } |
---|
| 5025 | } |
---|
| 5026 | vecLen = 2; |
---|
[819] | 5027 | |
---|
[1347] | 5028 | // add black track particles |
---|
| 5029 | // the total number of particles produced is restricted to 198 |
---|
| 5030 | // this may have influence on very high energies |
---|
[819] | 5031 | |
---|
[1347] | 5032 | if (verboseLevel > 1) |
---|
| 5033 | G4cout << " Evaporation " << atomicWeight << " " |
---|
| 5034 | << excitationEnergyGNP << " " << excitationEnergyDTA << G4endl; |
---|
[819] | 5035 | |
---|
| 5036 | if( atomicWeight > 1.5 ) |
---|
| 5037 | { |
---|
| 5038 | |
---|
| 5039 | G4double sprob, cost, sint, ekin2, ran, pp, eka; |
---|
| 5040 | G4double ekin, cfa, ekin1, phi, pvMass, pvEnergy; |
---|
| 5041 | G4int spall(0), nbl(0); |
---|
| 5042 | // sprob is the probability of self-absorption in heavy molecules |
---|
| 5043 | |
---|
| 5044 | sprob = 0.; |
---|
| 5045 | cfa = 0.025*((atomicWeight-1.)/120.)*std::exp(-(atomicWeight-1.)/120.); |
---|
| 5046 | // first add protons and neutrons |
---|
| 5047 | |
---|
| 5048 | if( excitationEnergyGNP >= 0.001 ) |
---|
| 5049 | { |
---|
| 5050 | // nbl = number of proton/neutron black track particles |
---|
| 5051 | // tex is their total kinetic energy (GeV) |
---|
| 5052 | |
---|
| 5053 | nbl = Poisson( excitationEnergyGNP/0.02); |
---|
| 5054 | if( nbl > atomicWeight ) nbl = (int)(atomicWeight); |
---|
| 5055 | if (verboseLevel > 1) |
---|
| 5056 | G4cout << " evaporation " << nbl << " " << sprob << G4endl; |
---|
| 5057 | spall = 0; |
---|
| 5058 | if( nbl > 0) |
---|
| 5059 | { |
---|
| 5060 | ekin = excitationEnergyGNP/nbl; |
---|
| 5061 | ekin2 = 0.0; |
---|
| 5062 | for( i=0; i<nbl; i++ ) |
---|
| 5063 | { |
---|
| 5064 | if( G4UniformRand() < sprob ) continue; |
---|
| 5065 | if( ekin2 > excitationEnergyGNP) break; |
---|
| 5066 | ran = G4UniformRand(); |
---|
| 5067 | ekin1 = -ekin*std::log(ran) - cfa*(1.0+0.5*normal()); |
---|
| 5068 | if (ekin1 < 0) ekin1 = -0.010*std::log(ran); |
---|
| 5069 | ekin2 += ekin1; |
---|
| 5070 | if( ekin2 > excitationEnergyGNP) |
---|
| 5071 | ekin1 = Amax( 1.0e-6, excitationEnergyGNP-(ekin2-ekin1) ); |
---|
| 5072 | if( G4UniformRand() > (1.0-atomicNumber/(atomicWeight))) |
---|
| 5073 | pv[vecLen].setDefinition( "Proton"); |
---|
| 5074 | else |
---|
| 5075 | pv[vecLen].setDefinition( "Neutron"); |
---|
| 5076 | spall++; |
---|
| 5077 | cost = G4UniformRand() * 2.0 - 1.0; |
---|
| 5078 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 5079 | phi = twopi * G4UniformRand(); |
---|
| 5080 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 5081 | pv[vecLen].setSide( -4 ); |
---|
| 5082 | pvMass = pv[vecLen].getMass(); |
---|
| 5083 | pv[vecLen].setTOF( 1.0 ); |
---|
| 5084 | pvEnergy = ekin1 + pvMass; |
---|
| 5085 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 5086 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 5087 | pp*sint*std::cos(phi), |
---|
| 5088 | pp*cost ); |
---|
| 5089 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 5090 | vecLen++; |
---|
| 5091 | } |
---|
| 5092 | if( (atomicWeight >= 10.0 ) && (incidentKineticEnergy <= 2.0) ) |
---|
| 5093 | { |
---|
| 5094 | G4int ika, kk = 0; |
---|
| 5095 | eka = incidentKineticEnergy; |
---|
| 5096 | if( eka > 1.0 )eka *= eka; |
---|
| 5097 | eka = Amax( 0.1, eka ); |
---|
| 5098 | ika = G4int(3.6*std::exp((atomicNumber*atomicNumber |
---|
| 5099 | /atomicWeight-35.56)/6.45)/eka); |
---|
| 5100 | if( ika > 0 ) |
---|
| 5101 | { |
---|
| 5102 | for( i=(vecLen-1); i>=0; i-- ) |
---|
| 5103 | { |
---|
| 5104 | if( (pv[i].getCode() == protonCode) && pv[i].getFlag() ) |
---|
| 5105 | { |
---|
| 5106 | pv[i].setDefinition( "Neutron" ); |
---|
| 5107 | if (verboseLevel > 1) pv[i].Print(i); |
---|
| 5108 | if( ++kk > ika ) break; |
---|
| 5109 | } |
---|
| 5110 | } |
---|
| 5111 | } |
---|
| 5112 | } |
---|
| 5113 | } |
---|
| 5114 | } |
---|
| 5115 | |
---|
| 5116 | // finished adding proton/neutron black track particles |
---|
| 5117 | // now, try to add deuterons, tritons and alphas |
---|
| 5118 | |
---|
| 5119 | if( excitationEnergyDTA >= 0.001 ) |
---|
| 5120 | { |
---|
| 5121 | nbl = (G4int)(2.*std::log(atomicWeight)); |
---|
| 5122 | |
---|
| 5123 | // nbl is the number of deutrons, tritons, and alphas produced |
---|
| 5124 | |
---|
| 5125 | if( nbl > 0 ) |
---|
| 5126 | { |
---|
| 5127 | ekin = excitationEnergyDTA/nbl; |
---|
| 5128 | ekin2 = 0.0; |
---|
| 5129 | for( i=0; i<nbl; i++ ) |
---|
| 5130 | { |
---|
| 5131 | if( G4UniformRand() < sprob ) continue; |
---|
| 5132 | if( ekin2 > excitationEnergyDTA) break; |
---|
| 5133 | ran = G4UniformRand(); |
---|
| 5134 | ekin1 = -ekin*std::log(ran)-cfa*(1.+0.5*normal()); |
---|
| 5135 | if( ekin1 < 0.0 ) ekin1 = -0.010*std::log(ran); |
---|
| 5136 | ekin2 += ekin1; |
---|
| 5137 | if( ekin2 > excitationEnergyDTA) |
---|
| 5138 | ekin1 = Amax( 1.0e-6, excitationEnergyDTA-(ekin2-ekin1)); |
---|
| 5139 | cost = G4UniformRand()*2.0 - 1.0; |
---|
| 5140 | sint = std::sqrt(std::fabs(1.0-cost*cost)); |
---|
| 5141 | phi = twopi*G4UniformRand(); |
---|
| 5142 | ran = G4UniformRand(); |
---|
| 5143 | if( ran <= 0.60 ) |
---|
| 5144 | pv[vecLen].setDefinition( "Deuteron"); |
---|
| 5145 | else if (ran <= 0.90) |
---|
| 5146 | pv[vecLen].setDefinition( "Triton"); |
---|
| 5147 | else |
---|
| 5148 | pv[vecLen].setDefinition( "Alpha"); |
---|
| 5149 | spall += (int)(pv[vecLen].getMass() * 1.066); |
---|
| 5150 | if( spall > atomicWeight ) break; |
---|
| 5151 | pv[vecLen].setFlag( true ); // true is the same as IPA(i)<0 |
---|
| 5152 | pv[vecLen].setSide( -4 ); |
---|
| 5153 | pvMass = pv[vecLen].getMass(); |
---|
| 5154 | pv[vecLen].setTOF( 1.0 ); |
---|
| 5155 | pvEnergy = pvMass + ekin1; |
---|
| 5156 | pp = std::sqrt( std::fabs( pvEnergy*pvEnergy - pvMass*pvMass ) ); |
---|
| 5157 | pv[vecLen].setMomentumAndUpdate( pp*sint*std::sin(phi), |
---|
| 5158 | pp*sint*std::cos(phi), |
---|
| 5159 | pp*cost ); |
---|
| 5160 | if (verboseLevel > 1) pv[vecLen].Print(vecLen); |
---|
| 5161 | vecLen++; |
---|
| 5162 | } |
---|
| 5163 | } |
---|
| 5164 | } |
---|
| 5165 | } |
---|
| 5166 | |
---|
| 5167 | // Calculate time delay for nuclear reactions |
---|
| 5168 | |
---|
| 5169 | G4double tof = incidentTOF; |
---|
| 5170 | if( (atomicWeight >= 1.5) && (atomicWeight <= 230.0) |
---|
| 5171 | && (incidentKineticEnergy <= 0.2) ) |
---|
| 5172 | tof -= 500.0 * std::exp(-incidentKineticEnergy /0.04) * std::log( G4UniformRand() ); |
---|
| 5173 | for ( i=0; i < vecLen; i++) |
---|
| 5174 | { |
---|
| 5175 | |
---|
| 5176 | pv[i].setTOF ( tof ); |
---|
| 5177 | // vec[i].SetTOF ( tof ); |
---|
| 5178 | } |
---|
| 5179 | |
---|
| 5180 | for(i=0; i<vecLen; i++) |
---|
| 5181 | { |
---|
| 5182 | if(pv[i].getName() == "KaonZero" || pv[i].getName() == "AntiKaonZero") |
---|
| 5183 | { |
---|
| 5184 | pvmx[0] = pv[i]; |
---|
| 5185 | if(G4UniformRand() < 0.5) pv[i].setDefinition("KaonZeroShort"); |
---|
| 5186 | else pv[i].setDefinition("KaonZeroLong"); |
---|
| 5187 | pv[i].setMomentumAndUpdate(pvmx[0].getMomentum()); |
---|
| 5188 | } |
---|
| 5189 | } |
---|
| 5190 | |
---|
[1347] | 5191 | successful = true; |
---|
| 5192 | delete [] pvmx; |
---|
| 5193 | return; |
---|
| 5194 | } |
---|
[819] | 5195 | |
---|
| 5196 | void |
---|
[1347] | 5197 | G4HEInelastic::ElasticScattering(G4bool& successful, |
---|
[819] | 5198 | G4HEVector pv[], |
---|
[1347] | 5199 | G4int& vecLen, |
---|
| 5200 | const G4HEVector& incidentParticle, |
---|
[819] | 5201 | G4double atomicWeight, |
---|
| 5202 | G4double /* atomicNumber*/) |
---|
[1347] | 5203 | { |
---|
| 5204 | if (verboseLevel > 1) |
---|
| 5205 | G4cout << " G4HEInelastic::ElasticScattering " << G4endl; |
---|
[819] | 5206 | |
---|
[1347] | 5207 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); |
---|
| 5208 | if (verboseLevel > 1) |
---|
| 5209 | G4cout << "DoIt: Incident particle momentum=" |
---|
| 5210 | << incidentTotalMomentum << " GeV" << G4endl; |
---|
| 5211 | if (incidentTotalMomentum < 0.01) { |
---|
| 5212 | successful = false; |
---|
| 5213 | return; |
---|
| 5214 | } |
---|
| 5215 | |
---|
[819] | 5216 | if (atomicWeight < 0.5) |
---|
| 5217 | { |
---|
| 5218 | successful = false; |
---|
| 5219 | return; |
---|
| 5220 | } |
---|
| 5221 | pv[0] = incidentParticle; |
---|
| 5222 | vecLen = 1; |
---|
| 5223 | |
---|
| 5224 | G4double aa, bb, cc, dd, rr; |
---|
| 5225 | if (atomicWeight <= 62.) |
---|
| 5226 | { |
---|
| 5227 | aa = std::pow(atomicWeight, 1.63); |
---|
| 5228 | bb = 14.5*std::pow(atomicWeight, 0.66); |
---|
| 5229 | cc = 1.4*std::pow(atomicWeight, 0.33); |
---|
| 5230 | dd = 10.; |
---|
| 5231 | } |
---|
| 5232 | else |
---|
| 5233 | { |
---|
| 5234 | aa = std::pow(atomicWeight, 1.33); |
---|
| 5235 | bb = 60.*std::pow(atomicWeight, 0.33); |
---|
| 5236 | cc = 0.4*std::pow(atomicWeight, 0.40); |
---|
| 5237 | dd = 10.; |
---|
| 5238 | } |
---|
| 5239 | aa = aa/bb; |
---|
| 5240 | cc = cc/dd; |
---|
| 5241 | G4double ran = G4UniformRand(); |
---|
| 5242 | rr = (aa + cc)*ran; |
---|
| 5243 | if (verboseLevel > 1) |
---|
| 5244 | { |
---|
| 5245 | G4cout << "ElasticScattering: aa,bb,cc,dd,rr" << G4endl; |
---|
| 5246 | G4cout << aa << " " << bb << " " << cc << " " << dd << " " |
---|
| 5247 | << rr << G4endl; |
---|
| 5248 | } |
---|
| 5249 | G4double t1 = -std::log(ran)/bb; |
---|
| 5250 | G4double t2 = -std::log(ran)/dd; |
---|
| 5251 | if (verboseLevel > 1) { |
---|
| 5252 | G4cout << "t1,fctcos " << t1 << " " << fctcos(t1, aa, bb, cc, dd, rr) |
---|
| 5253 | << G4endl; |
---|
| 5254 | G4cout << "t2,fctcos " << t2 << " " << fctcos(t2, aa, bb, cc, dd, rr) |
---|
| 5255 | << G4endl; |
---|
| 5256 | } |
---|
| 5257 | G4double eps = 0.001; |
---|
| 5258 | G4int ind1 = 10; |
---|
| 5259 | G4double t; |
---|
| 5260 | G4int ier1; |
---|
| 5261 | ier1 = rtmi(&t, t1, t2, eps, ind1, aa, bb, cc, dd, rr); |
---|
| 5262 | if (verboseLevel > 1) { |
---|
| 5263 | G4cout << "From rtmi, ier1=" << ier1 << G4endl; |
---|
| 5264 | G4cout << "t, fctcos " << t << " " << fctcos(t, aa, bb, cc, dd, rr) |
---|
| 5265 | << G4endl; |
---|
| 5266 | } |
---|
| 5267 | if (ier1 != 0) t = 0.25*(3.*t1 + t2); |
---|
| 5268 | if (verboseLevel > 1) |
---|
| 5269 | G4cout << "t, fctcos " << t << " " << fctcos(t, aa, bb, cc, dd, rr) |
---|
| 5270 | << G4endl; |
---|
| 5271 | |
---|
| 5272 | G4double phi = G4UniformRand()*twopi; |
---|
| 5273 | rr = 0.5*t/sqr(incidentTotalMomentum); |
---|
| 5274 | if (rr > 1.) rr = 0.; |
---|
| 5275 | if (verboseLevel > 1) |
---|
| 5276 | G4cout << "rr=" << rr << G4endl; |
---|
| 5277 | G4double cost = 1. - rr; |
---|
| 5278 | G4double sint = std::sqrt(Amax(rr*(2. - rr), 0.)); |
---|
| 5279 | if (verboseLevel > 1) |
---|
| 5280 | G4cout << "cos(t)=" << cost << " std::sin(t)=" << sint << G4endl; |
---|
| 5281 | // Scattered particle referred to axis of incident particle |
---|
| 5282 | G4HEVector pv0; |
---|
| 5283 | G4HEVector pvI; |
---|
| 5284 | pvI.setMass( incidentParticle.getMass() ); |
---|
| 5285 | pvI.setMomentum( incidentParticle.getMomentum() ); |
---|
| 5286 | pvI.SmulAndUpdate( pvI, 1. ); |
---|
| 5287 | pv0.setMass( pvI.getMass() ); |
---|
| 5288 | |
---|
| 5289 | pv0.setMomentumAndUpdate( incidentTotalMomentum * sint * std::sin(phi), |
---|
| 5290 | incidentTotalMomentum * sint * std::cos(phi), |
---|
| 5291 | incidentTotalMomentum * cost ); |
---|
| 5292 | pv0.Defs1( pv0, pvI ); |
---|
| 5293 | |
---|
| 5294 | successful = true; |
---|
| 5295 | return; |
---|
| 5296 | } |
---|
| 5297 | |
---|
| 5298 | |
---|
| 5299 | G4int |
---|
| 5300 | G4HEInelastic::rtmi(G4double *x, G4double xli, G4double xri, G4double eps, |
---|
| 5301 | G4int iend, |
---|
| 5302 | G4double aa, G4double bb, G4double cc, G4double dd, |
---|
| 5303 | G4double rr) |
---|
| 5304 | { |
---|
| 5305 | G4int ier = 0; |
---|
| 5306 | G4double xl = xli; |
---|
| 5307 | G4double xr = xri; |
---|
| 5308 | *x = xl; |
---|
| 5309 | G4double tol = *x; |
---|
| 5310 | G4double f = fctcos(tol, aa, bb, cc, dd, rr); |
---|
| 5311 | if (f == 0.) return ier; |
---|
| 5312 | G4double fl, fr; |
---|
| 5313 | fl = f; |
---|
| 5314 | *x = xr; |
---|
| 5315 | tol = *x; |
---|
| 5316 | f = fctcos(tol, aa, bb, cc, dd, rr); |
---|
| 5317 | if (f == 0.) return ier; |
---|
| 5318 | fr = f; |
---|
| 5319 | |
---|
| 5320 | // Error return in case of wrong input data |
---|
| 5321 | if (fl*fr >= 0.) |
---|
| 5322 | { |
---|
| 5323 | ier = 2; |
---|
| 5324 | return ier; |
---|
| 5325 | } |
---|
| 5326 | |
---|
| 5327 | // Basic assumption fl*fr less than 0 is satisfied. |
---|
| 5328 | // Generate tolerance for function values. |
---|
| 5329 | G4int i = 0; |
---|
| 5330 | G4double tolf = 100.*eps; |
---|
| 5331 | |
---|
| 5332 | // Start iteration loop |
---|
| 5333 | |
---|
| 5334 | label4: // <------------- |
---|
| 5335 | i++; |
---|
| 5336 | |
---|
| 5337 | // Start bisection loop |
---|
| 5338 | |
---|
| 5339 | for (G4int k = 1; k <= iend; k++) |
---|
| 5340 | { |
---|
| 5341 | *x = 0.5*(xl + xr); |
---|
| 5342 | tol = *x; |
---|
| 5343 | f = fctcos(tol, aa, bb, cc, dd, rr); |
---|
| 5344 | if (f == 0.) return 0; |
---|
| 5345 | if (f*fr < 0.) |
---|
| 5346 | { // Interchange xl and xr in order to get the |
---|
| 5347 | tol = xl; // same sign in f and fr |
---|
| 5348 | xl = xr; |
---|
| 5349 | xr = tol; |
---|
| 5350 | tol = fl; |
---|
| 5351 | fl = fr; |
---|
| 5352 | fr = tol; |
---|
| 5353 | } |
---|
| 5354 | tol = f - fl; |
---|
| 5355 | G4double a = f*tol; |
---|
| 5356 | a = a + a; |
---|
| 5357 | if (a < fr*(fr - fl) && i <= iend) goto label17; |
---|
| 5358 | xr = *x; |
---|
| 5359 | fr = f; |
---|
| 5360 | |
---|
| 5361 | // Test on satisfactory accuracy in bisection loop |
---|
| 5362 | tol = eps; |
---|
| 5363 | a = std::fabs(xr); |
---|
| 5364 | if (a > 1.) tol = tol*a; |
---|
| 5365 | if (std::fabs(xr - xl) <= tol && std::fabs(fr - fl) <= tolf) goto label14; |
---|
| 5366 | } |
---|
| 5367 | // End of bisection loop |
---|
| 5368 | |
---|
| 5369 | // No convergence after iend iteration steps followed by iend |
---|
| 5370 | // successive steps of bisection or steadily increasing function |
---|
| 5371 | // values at right bounds. Error return. |
---|
| 5372 | ier = 1; |
---|
| 5373 | |
---|
| 5374 | label14: // <--------------- |
---|
| 5375 | if (std::fabs(fr) > std::fabs(fl)) |
---|
| 5376 | { |
---|
| 5377 | *x = xl; |
---|
| 5378 | f = fl; |
---|
| 5379 | } |
---|
| 5380 | return ier; |
---|
| 5381 | |
---|
| 5382 | // Computation of iterated x-value by inverse parabolic interp |
---|
| 5383 | label17: // <--------------- |
---|
| 5384 | G4double a = fr - f; |
---|
| 5385 | G4double dx = (*x - xl)*fl*(1. + f*(a - tol)/(a*(fr - fl)))/tol; |
---|
| 5386 | G4double xm = *x; |
---|
| 5387 | G4double fm = f; |
---|
| 5388 | *x = xl - dx; |
---|
| 5389 | tol = *x; |
---|
| 5390 | f = fctcos(tol, aa, bb, cc, dd, rr); |
---|
| 5391 | if (f == 0.) return ier; |
---|
| 5392 | |
---|
| 5393 | // Test on satisfactory accuracy in iteration loop |
---|
| 5394 | tol = eps; |
---|
| 5395 | a = std::fabs(*x); |
---|
| 5396 | if (a > 1) tol = tol*a; |
---|
| 5397 | if (std::fabs(dx) <= tol && std::fabs(f) <= tolf) return ier; |
---|
| 5398 | |
---|
| 5399 | // Preparation of next bisection loop |
---|
| 5400 | if (f*fl < 0.) |
---|
| 5401 | { |
---|
| 5402 | xr = *x; |
---|
| 5403 | fr = f; |
---|
| 5404 | } |
---|
| 5405 | else |
---|
| 5406 | { |
---|
| 5407 | xl = *x; |
---|
| 5408 | fl = f; |
---|
| 5409 | xr = xm; |
---|
| 5410 | fr = fm; |
---|
| 5411 | } |
---|
| 5412 | goto label4; |
---|
| 5413 | } |
---|
| 5414 | |
---|
| 5415 | |
---|
| 5416 | // Test function for root-finder |
---|
| 5417 | |
---|
| 5418 | G4double |
---|
| 5419 | G4HEInelastic::fctcos(G4double t, G4double aa, G4double bb, G4double cc, |
---|
| 5420 | G4double dd, G4double rr) |
---|
| 5421 | { |
---|
| 5422 | const G4double expxl = -82.; |
---|
| 5423 | const G4double expxu = 82.; |
---|
| 5424 | |
---|
| 5425 | G4double test1 = -bb*t; |
---|
| 5426 | if (test1 > expxu) test1 = expxu; |
---|
| 5427 | if (test1 < expxl) test1 = expxl; |
---|
| 5428 | |
---|
| 5429 | G4double test2 = -dd*t; |
---|
| 5430 | if (test2 > expxu) test2 = expxu; |
---|
| 5431 | if (test2 < expxl) test2 = expxl; |
---|
| 5432 | |
---|
| 5433 | return aa*std::exp(test1) + cc*std::exp(test2) - rr; |
---|
| 5434 | } |
---|
| 5435 | |
---|
| 5436 | G4double G4HEInelastic::NBodyPhaseSpace |
---|
| 5437 | ( const G4double totalEnergy, // MeV |
---|
| 5438 | const G4bool constantCrossSection, |
---|
| 5439 | G4HEVector vec[], |
---|
| 5440 | G4int& vecLen ) |
---|
| 5441 | { |
---|
| 5442 | // derived from original FORTRAN code PHASP by H. Fesefeldt (02-Dec-1986) |
---|
| 5443 | // Returns the weight of the event |
---|
| 5444 | |
---|
| 5445 | G4int i; |
---|
| 5446 | |
---|
| 5447 | const G4double expxu = std::log(FLT_MAX); // upper bound for arg. of exp |
---|
| 5448 | const G4double expxl = -expxu; // lower bound for arg. of exp |
---|
| 5449 | |
---|
| 5450 | if( vecLen < 2 ) { |
---|
| 5451 | G4cerr << "*** Error in G4HEInelastic::GenerateNBodyEvent" << G4endl; |
---|
| 5452 | G4cerr << " number of particles < 2" << G4endl; |
---|
| 5453 | G4cerr << "totalEnergy = " << totalEnergy << ", vecLen = " |
---|
| 5454 | << vecLen << G4endl; |
---|
| 5455 | return -1.0; |
---|
| 5456 | } |
---|
| 5457 | |
---|
| 5458 | G4double* mass = new G4double [vecLen]; // mass of each particle |
---|
| 5459 | G4double* energy = new G4double [vecLen]; // total energy of each particle |
---|
| 5460 | G4double** pcm; // pcm is an array with 3 rows and vecLen columns |
---|
| 5461 | pcm = new G4double* [3]; |
---|
| 5462 | for( i=0; i<3; ++i )pcm[i] = new G4double [vecLen]; |
---|
| 5463 | |
---|
| 5464 | G4double totalMass = 0.0; |
---|
| 5465 | G4double* sm = new G4double [vecLen]; |
---|
| 5466 | |
---|
| 5467 | for( i=0; i<vecLen; ++i ) { |
---|
| 5468 | mass[i] = vec[i].getMass(); |
---|
| 5469 | vec[i].setMomentum( 0.0, 0.0, 0.0 ); |
---|
| 5470 | pcm[0][i] = 0.0; // x-momentum of i-th particle |
---|
| 5471 | pcm[1][i] = 0.0; // y-momentum of i-th particle |
---|
| 5472 | pcm[2][i] = 0.0; // z-momentum of i-th particle |
---|
| 5473 | energy[i] = mass[i]; // total energy of i-th particle |
---|
| 5474 | totalMass += mass[i]; |
---|
| 5475 | sm[i] = totalMass; |
---|
| 5476 | } |
---|
[962] | 5477 | |
---|
[819] | 5478 | if( totalMass >= totalEnergy ) { |
---|
[962] | 5479 | if (verboseLevel > 1) { |
---|
| 5480 | G4cout << "*** Error in G4HEInelastic::GenerateNBodyEvent" << G4endl; |
---|
| 5481 | G4cout << " total mass (" << totalMass << ") >= total energy (" |
---|
| 5482 | << totalEnergy << ")" << G4endl; |
---|
| 5483 | } |
---|
[819] | 5484 | delete [] mass; |
---|
| 5485 | delete [] energy; |
---|
| 5486 | for( i=0; i<3; ++i )delete [] pcm[i]; |
---|
| 5487 | delete [] pcm; |
---|
| 5488 | delete [] sm; |
---|
| 5489 | return -1.0; |
---|
| 5490 | } |
---|
[962] | 5491 | |
---|
[819] | 5492 | G4double kineticEnergy = totalEnergy - totalMass; |
---|
| 5493 | G4double* emm = new G4double [vecLen]; |
---|
| 5494 | emm[0] = mass[0]; |
---|
| 5495 | if( vecLen > 3 ) { // the random numbers are sorted |
---|
| 5496 | G4double* ran = new G4double [vecLen]; |
---|
| 5497 | for( i=0; i<vecLen; ++i )ran[i] = G4UniformRand(); |
---|
| 5498 | for( i=0; i<vecLen-1; ++i ) { |
---|
| 5499 | for( G4int j=vecLen-1; j > i; --j ) { |
---|
| 5500 | if( ran[i] > ran[j] ) { |
---|
| 5501 | G4double temp = ran[i]; |
---|
| 5502 | ran[i] = ran[j]; |
---|
| 5503 | ran[j] = temp; |
---|
| 5504 | } |
---|
| 5505 | } |
---|
| 5506 | } |
---|
| 5507 | for( i=1; i<vecLen; ++i )emm[i] = ran[i-1]*kineticEnergy + sm[i]; |
---|
| 5508 | delete [] ran; |
---|
| 5509 | } else { |
---|
| 5510 | emm[1] = G4UniformRand()*kineticEnergy + sm[1]; |
---|
| 5511 | } |
---|
| 5512 | emm[vecLen-1] = totalEnergy; |
---|
| 5513 | |
---|
| 5514 | // Weight is the sum of logarithms of terms instead of the product of terms |
---|
| 5515 | |
---|
| 5516 | G4bool lzero = true; |
---|
| 5517 | G4double wtmax = 0.0; |
---|
| 5518 | if( constantCrossSection ) { // this is KGENEV=1 in PHASP |
---|
| 5519 | G4double emmax = kineticEnergy + mass[0]; |
---|
| 5520 | G4double emmin = 0.0; |
---|
| 5521 | for( i=1; i<vecLen; ++i ) { |
---|
| 5522 | emmin += mass[i-1]; |
---|
| 5523 | emmax += mass[i]; |
---|
| 5524 | G4double wtfc = 0.0; |
---|
| 5525 | if( emmax*emmax > 0.0 ) { |
---|
| 5526 | G4double arg = emmax*emmax |
---|
| 5527 | + (emmin*emmin-mass[i]*mass[i])*(emmin*emmin-mass[i]*mass[i])/(emmax*emmax) |
---|
| 5528 | - 2.0*(emmin*emmin+mass[i]*mass[i]); |
---|
| 5529 | if( arg > 0.0 )wtfc = 0.5*std::sqrt( arg ); |
---|
| 5530 | } |
---|
| 5531 | if( wtfc == 0.0 ) { |
---|
| 5532 | lzero = false; |
---|
| 5533 | break; |
---|
| 5534 | } |
---|
| 5535 | wtmax += std::log( wtfc ); |
---|
| 5536 | } |
---|
| 5537 | if( lzero ) |
---|
| 5538 | wtmax = -wtmax; |
---|
| 5539 | else |
---|
| 5540 | wtmax = expxu; |
---|
| 5541 | } else { |
---|
| 5542 | wtmax = std::log( std::pow( kineticEnergy, vecLen-2 ) * |
---|
| 5543 | pi * std::pow( twopi, vecLen-2 ) / Factorial(vecLen-2) ); |
---|
| 5544 | } |
---|
| 5545 | lzero = true; |
---|
| 5546 | G4double* pd = new G4double [vecLen-1]; |
---|
| 5547 | for( i=0; i<vecLen-1; ++i ) { |
---|
| 5548 | pd[i] = 0.0; |
---|
| 5549 | if( emm[i+1]*emm[i+1] > 0.0 ) { |
---|
| 5550 | G4double arg = emm[i+1]*emm[i+1] |
---|
| 5551 | + (emm[i]*emm[i]-mass[i+1]*mass[i+1])*(emm[i]*emm[i]-mass[i+1]*mass[i+1]) |
---|
| 5552 | /(emm[i+1]*emm[i+1]) |
---|
| 5553 | - 2.0*(emm[i]*emm[i]+mass[i+1]*mass[i+1]); |
---|
| 5554 | if( arg > 0.0 )pd[i] = 0.5*std::sqrt( arg ); |
---|
| 5555 | } |
---|
| 5556 | if( pd[i] == 0.0 ) |
---|
| 5557 | lzero = false; |
---|
| 5558 | else |
---|
| 5559 | wtmax += std::log( pd[i] ); |
---|
| 5560 | } |
---|
| 5561 | G4double weight = 0.0; // weight is returned by GenerateNBodyEvent |
---|
| 5562 | if( lzero )weight = std::exp( Amax(Amin(wtmax,expxu),expxl) ); |
---|
| 5563 | |
---|
| 5564 | G4double bang, cb, sb, s0, s1, s2, c, s, esys, a, b, gama, beta; |
---|
| 5565 | pcm[0][0] = 0.0; |
---|
| 5566 | pcm[1][0] = pd[0]; |
---|
| 5567 | pcm[2][0] = 0.0; |
---|
| 5568 | for( i=1; i<vecLen; ++i ) { |
---|
| 5569 | pcm[0][i] = 0.0; |
---|
| 5570 | pcm[1][i] = -pd[i-1]; |
---|
| 5571 | pcm[2][i] = 0.0; |
---|
| 5572 | bang = twopi*G4UniformRand(); |
---|
| 5573 | cb = std::cos(bang); |
---|
| 5574 | sb = std::sin(bang); |
---|
| 5575 | c = 2.0*G4UniformRand() - 1.0; |
---|
| 5576 | s = std::sqrt( std::fabs( 1.0-c*c ) ); |
---|
| 5577 | if( i < vecLen-1 ) { |
---|
| 5578 | esys = std::sqrt(pd[i]*pd[i] + emm[i]*emm[i]); |
---|
| 5579 | beta = pd[i]/esys; |
---|
| 5580 | gama = esys/emm[i]; |
---|
| 5581 | for( G4int j=0; j<=i; ++j ) { |
---|
| 5582 | s0 = pcm[0][j]; |
---|
| 5583 | s1 = pcm[1][j]; |
---|
| 5584 | s2 = pcm[2][j]; |
---|
| 5585 | energy[j] = std::sqrt( s0*s0 + s1*s1 + s2*s2 + mass[j]*mass[j] ); |
---|
| 5586 | a = s0*c - s1*s; // rotation |
---|
| 5587 | pcm[1][j] = s0*s + s1*c; |
---|
| 5588 | b = pcm[2][j]; |
---|
| 5589 | pcm[0][j] = a*cb - b*sb; |
---|
| 5590 | pcm[2][j] = a*sb + b*cb; |
---|
| 5591 | pcm[1][j] = gama*(pcm[1][j] + beta*energy[j]); |
---|
| 5592 | } |
---|
| 5593 | } else { |
---|
| 5594 | for( G4int j=0; j<=i; ++j ) { |
---|
| 5595 | s0 = pcm[0][j]; |
---|
| 5596 | s1 = pcm[1][j]; |
---|
| 5597 | s2 = pcm[2][j]; |
---|
| 5598 | energy[j] = std::sqrt( s0*s0 + s1*s1 + s2*s2 + mass[j]*mass[j] ); |
---|
| 5599 | a = s0*c - s1*s; // rotation |
---|
| 5600 | pcm[1][j] = s0*s + s1*c; |
---|
| 5601 | b = pcm[2][j]; |
---|
| 5602 | pcm[0][j] = a*cb - b*sb; |
---|
| 5603 | pcm[2][j] = a*sb + b*cb; |
---|
| 5604 | } |
---|
| 5605 | } |
---|
| 5606 | } |
---|
| 5607 | G4double pModule; |
---|
| 5608 | for( i=0; i<vecLen; ++i ) { |
---|
| 5609 | kineticEnergy = energy[i] - mass[i]; |
---|
| 5610 | pModule = std::sqrt( sqr(kineticEnergy) + 2*kineticEnergy*mass[i] ); |
---|
| 5611 | vec[i].setMomentum( pcm[0][i]/pModule, |
---|
| 5612 | pcm[1][i]/pModule, |
---|
| 5613 | pcm[2][i]/pModule ); |
---|
| 5614 | vec[i].setKineticEnergyAndUpdate( kineticEnergy ); |
---|
| 5615 | } |
---|
| 5616 | delete [] mass; |
---|
| 5617 | delete [] energy; |
---|
| 5618 | for( i=0; i<3; ++i )delete [] pcm[i]; |
---|
| 5619 | delete [] pcm; |
---|
| 5620 | delete [] emm; |
---|
| 5621 | delete [] sm; |
---|
| 5622 | delete [] pd; |
---|
| 5623 | return weight; |
---|
| 5624 | } |
---|
| 5625 | |
---|
| 5626 | G4double |
---|
| 5627 | G4HEInelastic::gpdk( G4double a, G4double b, G4double c ) |
---|
| 5628 | { |
---|
| 5629 | if( a == 0.0 ) |
---|
| 5630 | { |
---|
| 5631 | return 0.0; |
---|
| 5632 | } |
---|
| 5633 | else |
---|
| 5634 | { |
---|
| 5635 | G4double arg = a*a+(b*b-c*c)*(b*b-c*c)/(a*a)-2.0*(b*b+c*c); |
---|
| 5636 | if( arg <= 0.0 ) |
---|
| 5637 | { |
---|
| 5638 | return 0.0; |
---|
| 5639 | } |
---|
| 5640 | else |
---|
| 5641 | { |
---|
| 5642 | return 0.5*std::sqrt(std::fabs(arg)); |
---|
| 5643 | } |
---|
| 5644 | } |
---|
| 5645 | } |
---|
| 5646 | |
---|
| 5647 | |
---|
| 5648 | G4double |
---|
| 5649 | G4HEInelastic::NBodyPhaseSpace(G4int npart, G4HEVector pv[], |
---|
| 5650 | G4double wmax, G4double wfcn, |
---|
| 5651 | G4int maxtrial, G4int ntrial) |
---|
| 5652 | { ntrial = 0; |
---|
| 5653 | G4double wps(0); |
---|
| 5654 | while ( ntrial < maxtrial) |
---|
| 5655 | { ntrial++; |
---|
| 5656 | G4int i, j; |
---|
| 5657 | G4int nrn = 3*(npart-2)-4; |
---|
| 5658 | G4double *ranarr = new G4double[nrn]; |
---|
| 5659 | for (i=0;i<nrn;i++) ranarr[i]=G4UniformRand(); |
---|
| 5660 | G4int nrnp = npart-4; |
---|
| 5661 | if(nrnp > 1) QuickSort( ranarr, 0 , nrnp-1 ); |
---|
| 5662 | G4HEVector pvcms; |
---|
| 5663 | pvcms.Add(pv[0],pv[1]); |
---|
| 5664 | pvcms.Smul( pvcms, -1.); |
---|
| 5665 | G4double rm = 0.; |
---|
| 5666 | for (i=2;i<npart;i++) rm += pv[i].getMass(); |
---|
| 5667 | G4double rm1 = pvcms.getMass() - rm; |
---|
| 5668 | rm -= pv[2].getMass(); |
---|
| 5669 | wps = (npart-3)*std::pow(rm1/sqr(twopi), npart-4)/(4*pi*pvcms.getMass()); |
---|
| 5670 | for (i=3; (i=npart-1);i++) wps /= i-2; // @@@@@@@@@@ bug @@@@@@@@@ |
---|
| 5671 | G4double xxx = rm1/sqr(twopi); |
---|
| 5672 | for (i=1; (i=npart-4); i++) wps /= xxx/i; // @@@@@@@@@@ bug @@@@@@@@@ |
---|
| 5673 | wps /= (4*pi*pvcms.getMass()); |
---|
| 5674 | G4double p2,cost,sint,phi; |
---|
| 5675 | j = 1; |
---|
| 5676 | while (j) |
---|
| 5677 | { j++; |
---|
| 5678 | rm -= pv[j+1].getMass(); |
---|
| 5679 | if(j == npart-2) break; |
---|
| 5680 | G4double rmass = rm + rm1*ranarr[npart-j-1]; |
---|
| 5681 | p2 = Alam(sqr(pvcms.getMass()), sqr(pv[j].getMass()), |
---|
| 5682 | sqr(rmass))/(4.*sqr(pvcms.getMass())); |
---|
| 5683 | cost = 1. - 2.*ranarr[npart+2*j-9]; |
---|
| 5684 | sint = std::sqrt(1.-cost*cost); |
---|
| 5685 | phi = twopi*ranarr[npart+2*j-8]; |
---|
| 5686 | p2 = std::sqrt( Amax(0., p2)); |
---|
| 5687 | wps *= p2; |
---|
| 5688 | pv[j].setMomentumAndUpdate( p2*sint*std::sin(phi), p2*sint*std::cos(phi),p2*cost); |
---|
| 5689 | pv[j].Lor(pv[j], pvcms); |
---|
| 5690 | pvcms.Add3( pvcms, pv[j] ); |
---|
| 5691 | pvcms.setEnergy(pvcms.getEnergy()-pv[j].getEnergy()); |
---|
| 5692 | pvcms.setMass( std::sqrt(sqr(pvcms.getEnergy()) - sqr(pvcms.Length()))); |
---|
| 5693 | } |
---|
| 5694 | p2 = Alam(sqr(pvcms.getMass()), sqr(pv[j].getMass()), |
---|
| 5695 | sqr(rm))/(4.*sqr(pvcms.getMass())); |
---|
| 5696 | cost = 1. - 2.*ranarr[npart+2*j-9]; |
---|
| 5697 | sint = std::sqrt(1.-cost*cost); |
---|
| 5698 | phi = twopi*ranarr[npart+2*j-8]; |
---|
| 5699 | p2 = std::sqrt( Amax(0. , p2)); |
---|
| 5700 | wps *= p2; |
---|
| 5701 | pv[j].setMomentumAndUpdate( p2*sint*std::sin(phi), p2*sint*std::cos(phi), p2*cost); |
---|
| 5702 | pv[j+1].setMomentumAndUpdate( -p2*sint*std::sin(phi), -p2*sint*std::cos(phi), -p2*cost); |
---|
| 5703 | pv[j].Lor( pv[j], pvcms ); |
---|
| 5704 | pv[j+1].Lor( pv[j+1], pvcms ); |
---|
| 5705 | wfcn = CalculatePhaseSpaceWeight( npart ); |
---|
| 5706 | G4double wt = wps * wfcn; |
---|
| 5707 | if (wt > wmax) |
---|
| 5708 | { wmax = wt; |
---|
| 5709 | G4cout << "maximum weight changed to " << wmax << G4endl; |
---|
| 5710 | } |
---|
| 5711 | wt = wt/wmax; |
---|
| 5712 | if (G4UniformRand() < wt) break; |
---|
| 5713 | } |
---|
| 5714 | return wps; |
---|
| 5715 | } |
---|
| 5716 | |
---|
| 5717 | |
---|
| 5718 | void |
---|
| 5719 | G4HEInelastic::QuickSort(G4double arr[], const G4int lidx, const G4int ridx) |
---|
| 5720 | { // sorts the Array arr[] in ascending order |
---|
| 5721 | G4double buffer; |
---|
| 5722 | G4int k, e, mid; |
---|
| 5723 | if(lidx>=ridx) return; |
---|
| 5724 | mid = (int)((lidx+ridx)/2.); |
---|
| 5725 | buffer = arr[lidx]; |
---|
| 5726 | arr[lidx]= arr[mid]; |
---|
| 5727 | arr[mid] = buffer; |
---|
| 5728 | e = lidx; |
---|
| 5729 | for (k=lidx+1;k<=ridx;k++) |
---|
| 5730 | if (arr[k] < arr[lidx]) |
---|
| 5731 | { e++; |
---|
| 5732 | buffer = arr[e]; |
---|
| 5733 | arr[e] = arr[k]; |
---|
| 5734 | arr[k] = buffer; |
---|
| 5735 | } |
---|
| 5736 | buffer = arr[lidx]; |
---|
| 5737 | arr[lidx]= arr[e]; |
---|
| 5738 | arr[e] = buffer; |
---|
| 5739 | QuickSort(arr, lidx, e-1); |
---|
| 5740 | QuickSort(arr, e+1 , ridx); |
---|
| 5741 | return; |
---|
| 5742 | } |
---|
| 5743 | |
---|
| 5744 | G4double |
---|
| 5745 | G4HEInelastic::Alam( G4double a, G4double b, G4double c) |
---|
| 5746 | { return a*a + b*b + c*c - 2.*a*b - 2.*a*c -2.*b*c; |
---|
| 5747 | } |
---|
| 5748 | |
---|
| 5749 | G4double |
---|
| 5750 | G4HEInelastic::CalculatePhaseSpaceWeight( G4int /* npart */) |
---|
| 5751 | { G4double wfcn = 1.; |
---|
| 5752 | return wfcn; |
---|
| 5753 | } |
---|
| 5754 | |
---|
| 5755 | |
---|
| 5756 | |
---|
| 5757 | |
---|
| 5758 | |
---|
| 5759 | |
---|
| 5760 | |
---|