| 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| 26 | //
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| 27 | // $Id: G4HELambdaInelastic.cc,v 1.15 2008/03/17 20:49:17 dennis Exp $
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| 28 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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| 29 | //
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| 30 | //
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| 31 |
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| 32 | #include "globals.hh"
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| 33 | #include "G4ios.hh"
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| 34 |
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| 35 | //
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| 36 | // G4 Process: Gheisha High Energy Collision model.
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| 37 | // This includes the high energy cascading model, the two-body-resonance model
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| 38 | // and the low energy two-body model. Not included are the low energy stuff like
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| 39 | // nuclear reactions, nuclear fission without any cascading and all processes for
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| 40 | // particles at rest.
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| 41 | // First work done by J.L.Chuma and F.W.Jones, TRIUMF, June 96.
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| 42 | // H. Fesefeldt, RWTH-Aachen, 23-October-1996
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| 43 | // Last modified: 29-July-1998
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| 44 |
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| 45 | #include "G4HELambdaInelastic.hh"
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| 46 |
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| 47 | G4HadFinalState * G4HELambdaInelastic::
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| 48 | ApplyYourself( const G4HadProjectile &aTrack, G4Nucleus &targetNucleus )
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| 49 | {
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| 50 | G4HEVector * pv = new G4HEVector[MAXPART];
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| 51 | const G4HadProjectile *aParticle = &aTrack;
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| 52 | // G4DynamicParticle *originalTarget = targetNucleus.ReturnTargetParticle();
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| 53 | const G4double A = targetNucleus.GetN();
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| 54 | const G4double Z = targetNucleus.GetZ();
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| 55 | G4HEVector incidentParticle(aParticle);
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| 56 |
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| 57 | G4double atomicNumber = Z;
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| 58 | G4double atomicWeight = A;
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| 59 |
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| 60 | G4int incidentCode = incidentParticle.getCode();
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| 61 | G4double incidentMass = incidentParticle.getMass();
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| 62 | G4double incidentTotalEnergy = incidentParticle.getEnergy();
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| 63 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum();
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| 64 | G4double incidentKineticEnergy = incidentTotalEnergy - incidentMass;
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| 65 |
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| 66 | if(incidentKineticEnergy < 1.)
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| 67 | {
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| 68 | G4cout << "GHELambdaInelastic: incident energy < 1 GeV" << G4endl;
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| 69 | }
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| 70 | if(verboseLevel > 1)
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| 71 | {
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| 72 | G4cout << "G4HELambdaInelastic::ApplyYourself" << G4endl;
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| 73 | G4cout << "incident particle " << incidentParticle.getName()
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| 74 | << "mass " << incidentMass
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| 75 | << "kinetic energy " << incidentKineticEnergy
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| 76 | << G4endl;
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| 77 | G4cout << "target material with (A,Z) = ("
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| 78 | << atomicWeight << "," << atomicNumber << ")" << G4endl;
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| 79 | }
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| 80 |
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| 81 | G4double inelasticity = NuclearInelasticity(incidentKineticEnergy,
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| 82 | atomicWeight, atomicNumber);
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| 83 | if(verboseLevel > 1)
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| 84 | G4cout << "nuclear inelasticity = " << inelasticity << G4endl;
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| 85 |
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| 86 | incidentKineticEnergy -= inelasticity;
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| 87 |
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| 88 | G4double excitationEnergyGNP = 0.;
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| 89 | G4double excitationEnergyDTA = 0.;
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| 90 |
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| 91 | G4double excitation = NuclearExcitation(incidentKineticEnergy,
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| 92 | atomicWeight, atomicNumber,
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| 93 | excitationEnergyGNP,
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| 94 | excitationEnergyDTA);
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| 95 | if(verboseLevel > 1)
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| 96 | G4cout << "nuclear excitation = " << excitation << excitationEnergyGNP
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| 97 | << excitationEnergyDTA << G4endl;
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| 98 |
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| 99 |
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| 100 | incidentKineticEnergy -= excitation;
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| 101 | incidentTotalEnergy = incidentKineticEnergy + incidentMass;
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| 102 | incidentTotalMomentum = std::sqrt( (incidentTotalEnergy-incidentMass)
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| 103 | *(incidentTotalEnergy+incidentMass));
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| 104 |
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| 105 |
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| 106 | G4HEVector targetParticle;
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| 107 | if(G4UniformRand() < atomicNumber/atomicWeight)
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| 108 | {
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| 109 | targetParticle.setDefinition("Proton");
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| 110 | }
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| 111 | else
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| 112 | {
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| 113 | targetParticle.setDefinition("Neutron");
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| 114 | }
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| 115 |
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| 116 | G4double targetMass = targetParticle.getMass();
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| 117 | G4double centerOfMassEnergy = std::sqrt( incidentMass*incidentMass + targetMass*targetMass
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| 118 | + 2.0*targetMass*incidentTotalEnergy);
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| 119 | G4double availableEnergy = centerOfMassEnergy - targetMass - incidentMass;
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| 120 |
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| 121 | // this was the meaning of inElastic in the
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| 122 | // original Gheisha stand-alone version.
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| 123 | // G4bool inElastic = InElasticCrossSectionInFirstInt
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| 124 | // (availableEnergy, incidentCode, incidentTotalMomentum);
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| 125 | // by unknown reasons, it has been replaced
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| 126 | // to the following code in Geant???
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| 127 | G4bool inElastic = true;
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| 128 | // if (G4UniformRand() < elasticCrossSection/totalCrossSection) inElastic = false;
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| 129 |
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| 130 | vecLength = 0;
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| 131 |
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| 132 | if(verboseLevel > 1)
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| 133 | G4cout << "ApplyYourself: CallFirstIntInCascade for particle "
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| 134 | << incidentCode << G4endl;
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| 135 |
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| 136 | G4bool successful = false;
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| 137 |
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| 138 | if(inElastic || (!inElastic && atomicWeight < 1.5))
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| 139 | {
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| 140 | FirstIntInCasLambda(inElastic, availableEnergy, pv, vecLength,
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| 141 | incidentParticle, targetParticle, atomicWeight);
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| 142 |
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| 143 | if(verboseLevel > 1)
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| 144 | G4cout << "ApplyYourself::StrangeParticlePairProduction" << G4endl;
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| 145 |
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| 146 |
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| 147 | if ((vecLength > 0) && (availableEnergy > 1.))
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| 148 | StrangeParticlePairProduction( availableEnergy, centerOfMassEnergy,
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| 149 | pv, vecLength,
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| 150 | incidentParticle, targetParticle);
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| 151 | HighEnergyCascading( successful, pv, vecLength,
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| 152 | excitationEnergyGNP, excitationEnergyDTA,
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| 153 | incidentParticle, targetParticle,
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| 154 | atomicWeight, atomicNumber);
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| 155 | if (!successful)
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| 156 | HighEnergyClusterProduction( successful, pv, vecLength,
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| 157 | excitationEnergyGNP, excitationEnergyDTA,
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| 158 | incidentParticle, targetParticle,
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| 159 | atomicWeight, atomicNumber);
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| 160 | if (!successful)
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| 161 | MediumEnergyCascading( successful, pv, vecLength,
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| 162 | excitationEnergyGNP, excitationEnergyDTA,
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| 163 | incidentParticle, targetParticle,
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| 164 | atomicWeight, atomicNumber);
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| 165 |
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| 166 | if (!successful)
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| 167 | MediumEnergyClusterProduction( successful, pv, vecLength,
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| 168 | excitationEnergyGNP, excitationEnergyDTA,
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| 169 | incidentParticle, targetParticle,
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| 170 | atomicWeight, atomicNumber);
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| 171 | if (!successful)
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| 172 | QuasiElasticScattering( successful, pv, vecLength,
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| 173 | excitationEnergyGNP, excitationEnergyDTA,
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| 174 | incidentParticle, targetParticle,
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| 175 | atomicWeight, atomicNumber);
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| 176 | }
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| 177 | if (!successful)
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| 178 | {
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| 179 | ElasticScattering( successful, pv, vecLength,
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| 180 | incidentParticle,
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| 181 | atomicWeight, atomicNumber);
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| 182 | }
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| 183 |
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| 184 | if (!successful)
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| 185 | {
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| 186 | G4cout << "GHEInelasticInteraction::ApplyYourself fails to produce final state particles" << G4endl;
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| 187 | }
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| 188 | FillParticleChange(pv, vecLength);
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| 189 | delete [] pv;
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| 190 | theParticleChange.SetStatusChange(stopAndKill);
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| 191 | return & theParticleChange;
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| 192 | }
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| 193 |
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| 194 | void
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| 195 | G4HELambdaInelastic::FirstIntInCasLambda( G4bool &inElastic,
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| 196 | const G4double availableEnergy,
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| 197 | G4HEVector pv[],
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| 198 | G4int &vecLen,
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| 199 | G4HEVector incidentParticle,
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| 200 | G4HEVector targetParticle,
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| 201 | const G4double atomicWeight)
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| 202 |
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| 203 | // Lambda undergoes interaction with nucleon within a nucleus. Check if it is
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| 204 | // energetically possible to produce pions/kaons. In not, assume nuclear
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| 205 | // excitation occurs and input particle is degraded in energy. No other
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| 206 | // particles are produced. If reaction is possible, find the correct number
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| 207 | // of pions/protons/neutrons produced using an interpolation to multiplicity
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| 208 | // data. Replace some pions or protons/neutrons by kaons or strange baryons
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| 209 | // according to the average multiplicity per inelastic reaction.
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| 210 |
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| 211 | {
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| 212 | static const G4double expxu = std::log(MAXFLOAT); // upper bound for arg. of exp
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| 213 | static const G4double expxl = -expxu; // lower bound for arg. of exp
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| 214 |
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| 215 | static const G4double protb = 0.7;
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| 216 | static const G4double neutb = 0.7;
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| 217 | static const G4double c = 1.25;
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| 218 |
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| 219 | static const G4int numMul = 1200;
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| 220 | static const G4int numSec = 60;
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| 221 |
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| 222 | // G4int neutronCode = Neutron.getCode();
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| 223 | G4int protonCode = Proton.getCode();
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| 224 |
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| 225 | G4int targetCode = targetParticle.getCode();
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| 226 | // G4double incidentMass = incidentParticle.getMass();
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| 227 | // G4double incidentEnergy = incidentParticle.getEnergy();
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| 228 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum();
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| 229 |
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| 230 | static G4bool first = true;
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| 231 | static G4double protmul[numMul], protnorm[numSec]; // proton constants
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| 232 | static G4double neutmul[numMul], neutnorm[numSec]; // neutron constants
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| 233 |
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| 234 | // misc. local variables
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| 235 | // np = number of pi+, nm = number of pi-, nz = number of pi0
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| 236 |
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| 237 | G4int i, counter, nt, np, nm, nz;
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| 238 |
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| 239 | if( first )
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| 240 | { // compute normalization constants, this will only be done once
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| 241 | first = false;
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| 242 | for( i=0; i<numMul; i++ )protmul[i] = 0.0;
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| 243 | for( i=0; i<numSec; i++ )protnorm[i] = 0.0;
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| 244 | counter = -1;
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| 245 | for( np=0; np<(numSec/3); np++ )
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| 246 | {
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| 247 | for( nm=std::max(0,np-2); nm<=(np+1); nm++ )
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| 248 | {
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| 249 | for( nz=0; nz<numSec/3; nz++ )
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| 250 | {
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| 251 | if( ++counter < numMul )
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| 252 | {
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| 253 | nt = np+nm+nz;
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| 254 | if( (nt>0) && (nt<=numSec) )
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| 255 | {
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| 256 | protmul[counter] = pmltpc(np,nm,nz,nt,protb,c);
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| 257 | protnorm[nt-1] += protmul[counter];
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| 258 | }
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| 259 | }
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| 260 | }
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| 261 | }
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| 262 | }
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| 263 | for( i=0; i<numMul; i++ )neutmul[i] = 0.0;
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| 264 | for( i=0; i<numSec; i++ )neutnorm[i] = 0.0;
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| 265 | counter = -1;
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| 266 | for( np=0; np<numSec/3; np++ )
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| 267 | {
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| 268 | for( nm=std::max(0,np-1); nm<=(np+2); nm++ )
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| 269 | {
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| 270 | for( nz=0; nz<numSec/3; nz++ )
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| 271 | {
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| 272 | if( ++counter < numMul )
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| 273 | {
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| 274 | nt = np+nm+nz;
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| 275 | if( (nt>0) && (nt<=numSec) )
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| 276 | {
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| 277 | neutmul[counter] = pmltpc(np,nm,nz,nt,neutb,c);
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| 278 | neutnorm[nt-1] += neutmul[counter];
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| 279 | }
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| 280 | }
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| 281 | }
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| 282 | }
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| 283 | }
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| 284 | for( i=0; i<numSec; i++ )
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| 285 | {
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| 286 | if( protnorm[i] > 0.0 )protnorm[i] = 1.0/protnorm[i];
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| 287 | if( neutnorm[i] > 0.0 )neutnorm[i] = 1.0/neutnorm[i];
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| 288 | }
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| 289 | } // end of initialization
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| 290 |
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| 291 |
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| 292 | // initialize the first two places
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| 293 | // the same as beam and target
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| 294 | pv[0] = incidentParticle;
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| 295 | pv[1] = targetParticle;
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| 296 | vecLen = 2;
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| 297 |
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| 298 | if( !inElastic )
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| 299 | { // quasi-elastic scattering, no pions produced
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| 300 | G4double cech[] = {0.50, 0.45, 0.40, 0.35, 0.30, 0.25, 0.06, 0.04, 0.005, 0.};
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| 301 | G4int iplab = G4int( std::min( 9.0, incidentTotalMomentum*2.5 ) );
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| 302 | if( G4UniformRand() < cech[iplab]/std::pow(atomicWeight,0.42) )
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| 303 | {
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| 304 | G4double ran = G4UniformRand();
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| 305 | if( targetCode == protonCode)
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| 306 | {
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| 307 | if( ran < 0.2)
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| 308 | {
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| 309 | pv[0] = SigmaPlus;
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| 310 | pv[1] = Neutron;
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| 311 | }
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| 312 | else if(ran < 0.4)
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| 313 | {
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| 314 | pv[0] = SigmaZero;
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| 315 | }
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| 316 | else if(ran < 0.6)
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| 317 | {
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| 318 | pv[0] = Proton;
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| 319 | pv[1] = Lambda;
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| 320 | }
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| 321 | else if(ran < 0.8)
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| 322 | {
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| 323 | pv[0] = Proton;
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| 324 | pv[1] = SigmaZero;
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| 325 | }
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| 326 | else
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| 327 | {
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| 328 | pv[0] = Neutron;
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| 329 | pv[1] = SigmaPlus;
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| 330 | }
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| 331 | }
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| 332 | else
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| 333 | {
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| 334 | if(ran < 0.2)
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| 335 | {
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| 336 | pv[0] = SigmaZero;
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| 337 | }
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| 338 | else if(ran < 0.4)
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| 339 | {
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| 340 | pv[0] = SigmaMinus;
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| 341 | pv[1] = Proton;
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| 342 | }
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| 343 | else if(ran < 0.6)
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| 344 | {
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| 345 | pv[0] = Neutron;
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| 346 | pv[1] = Lambda;
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| 347 | }
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| 348 | else if(ran < 0.8)
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| 349 | {
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| 350 | pv[0] = Neutron;
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| 351 | pv[1] = SigmaZero;
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| 352 | }
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| 353 | else
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| 354 | {
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| 355 | pv[0] = Proton;
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| 356 | pv[1] = SigmaMinus;
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| 357 | }
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| 358 | }
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| 359 | }
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| 360 | return;
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| 361 | }
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| 362 | else if (availableEnergy <= PionPlus.getMass())
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| 363 | return;
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| 364 |
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| 365 | // inelastic scattering
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| 366 |
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| 367 | np = 0; nm = 0; nz = 0;
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| 368 |
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| 369 | // number of total particles vs. centre of mass Energy - 2*proton mass
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| 370 |
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| 371 | G4double aleab = std::log(availableEnergy);
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| 372 | G4double n = 3.62567+aleab*(0.665843+aleab*(0.336514
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| 373 | + aleab*(0.117712+0.0136912*aleab))) - 2.0;
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| 374 |
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| 375 | // normalization constant for kno-distribution.
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| 376 | // calculate first the sum of all constants, check for numerical problems.
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| 377 | G4double test, dum, anpn = 0.0;
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| 378 |
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| 379 | for (nt=1; nt<=numSec; nt++) {
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| 380 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
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| 381 | dum = pi*nt/(2.0*n*n);
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| 382 | if (std::fabs(dum) < 1.0) {
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| 383 | if( test >= 1.0e-10 )anpn += dum*test;
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| 384 | } else {
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| 385 | anpn += dum*test;
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| 386 | }
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| 387 | }
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| 388 |
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| 389 | G4double ran = G4UniformRand();
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| 390 | G4double excs = 0.0;
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| 391 | if( targetCode == protonCode )
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| 392 | {
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| 393 | counter = -1;
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| 394 | for (np=0; np<numSec/3; np++) {
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| 395 | for (nm=std::max(0,np-2); nm<=(np+1); nm++) {
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| 396 | for (nz=0; nz<numSec/3; nz++) {
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|---|
| 397 | if (++counter < numMul) {
|
|---|
| 398 | nt = np+nm+nz;
|
|---|
| 399 | if ( (nt>0) && (nt<=numSec) ) {
|
|---|
| 400 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
|
|---|
| 401 | dum = (pi/anpn)*nt*protmul[counter]*protnorm[nt-1]/(2.0*n*n);
|
|---|
| 402 | if (std::fabs(dum) < 1.0) {
|
|---|
| 403 | if( test >= 1.0e-10 )excs += dum*test;
|
|---|
| 404 | } else {
|
|---|
| 405 | excs += dum*test;
|
|---|
| 406 | }
|
|---|
| 407 | if (ran < excs) goto outOfLoop; //--------------------->
|
|---|
| 408 | }
|
|---|
| 409 | }
|
|---|
| 410 | }
|
|---|
| 411 | }
|
|---|
| 412 | }
|
|---|
| 413 | // 3 previous loops continued to the end
|
|---|
| 414 |
|
|---|
| 415 | inElastic = false; // quasi-elastic scattering
|
|---|
| 416 | return;
|
|---|
| 417 | }
|
|---|
| 418 | else
|
|---|
| 419 | { // target must be a neutron
|
|---|
| 420 | counter = -1;
|
|---|
| 421 | for (np=0; np<numSec/3; np++) {
|
|---|
| 422 | for (nm=std::max(0,np-1); nm<=(np+2); nm++) {
|
|---|
| 423 | for (nz=0; nz<numSec/3; nz++) {
|
|---|
| 424 | if (++counter < numMul) {
|
|---|
| 425 | nt = np+nm+nz;
|
|---|
| 426 | if ( (nt>=1) && (nt<=numSec) ) {
|
|---|
| 427 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
|
|---|
| 428 | dum = (pi/anpn)*nt*neutmul[counter]*neutnorm[nt-1]/(2.0*n*n);
|
|---|
| 429 | if (std::fabs(dum) < 1.0) {
|
|---|
| 430 | if( test >= 1.0e-10 )excs += dum*test;
|
|---|
| 431 | } else {
|
|---|
| 432 | excs += dum*test;
|
|---|
| 433 | }
|
|---|
| 434 | if (ran < excs) goto outOfLoop; // ------------->
|
|---|
| 435 | }
|
|---|
| 436 | }
|
|---|
| 437 | }
|
|---|
| 438 | }
|
|---|
| 439 | }
|
|---|
| 440 | // 3 previous loops continued to the end
|
|---|
| 441 | inElastic = false; // quasi-elastic scattering.
|
|---|
| 442 | return;
|
|---|
| 443 | }
|
|---|
| 444 |
|
|---|
| 445 | outOfLoop: // <--------------------------------------------
|
|---|
| 446 |
|
|---|
| 447 | ran = G4UniformRand();
|
|---|
| 448 | if( targetCode == protonCode)
|
|---|
| 449 | {
|
|---|
| 450 | if( np == nm)
|
|---|
| 451 | {
|
|---|
| 452 | if (ran < 0.25)
|
|---|
| 453 | {
|
|---|
| 454 | }
|
|---|
| 455 | else if(ran < 0.5)
|
|---|
| 456 | {
|
|---|
| 457 | pv[0] = SigmaZero;
|
|---|
| 458 | }
|
|---|
| 459 | else
|
|---|
| 460 | {
|
|---|
| 461 | pv[0] = SigmaPlus;
|
|---|
| 462 | pv[1] = Neutron;
|
|---|
| 463 | }
|
|---|
| 464 | }
|
|---|
| 465 | else if (np == (nm+1))
|
|---|
| 466 | {
|
|---|
| 467 | if( G4UniformRand() < 0.25)
|
|---|
| 468 | {
|
|---|
| 469 | pv[1] = Neutron;
|
|---|
| 470 | }
|
|---|
| 471 | else if(ran < 0.5)
|
|---|
| 472 | {
|
|---|
| 473 | pv[0] = SigmaZero;
|
|---|
| 474 | pv[1] = Neutron;
|
|---|
| 475 | }
|
|---|
| 476 | else
|
|---|
| 477 | {
|
|---|
| 478 | pv[0] = SigmaMinus;
|
|---|
| 479 | }
|
|---|
| 480 | }
|
|---|
| 481 | else if (np == (nm-1))
|
|---|
| 482 | {
|
|---|
| 483 | pv[0] = SigmaPlus;
|
|---|
| 484 | }
|
|---|
| 485 | else
|
|---|
| 486 | {
|
|---|
| 487 | pv[0] = SigmaMinus;
|
|---|
| 488 | pv[1] = Neutron;
|
|---|
| 489 | }
|
|---|
| 490 | }
|
|---|
| 491 | else
|
|---|
| 492 | {
|
|---|
| 493 | if (np == nm)
|
|---|
| 494 | {
|
|---|
| 495 | if(ran < 0.5)
|
|---|
| 496 | {
|
|---|
| 497 | }
|
|---|
| 498 | else
|
|---|
| 499 | {
|
|---|
| 500 | pv[0] = SigmaMinus;
|
|---|
| 501 | pv[1] = Proton;
|
|---|
| 502 | }
|
|---|
| 503 | }
|
|---|
| 504 | else if (np == (nm-1))
|
|---|
| 505 | {
|
|---|
| 506 | if( ran < 0.25)
|
|---|
| 507 | {
|
|---|
| 508 | pv[1] = Proton;
|
|---|
| 509 | }
|
|---|
| 510 | else if(ran < 0.5)
|
|---|
| 511 | {
|
|---|
| 512 | pv[0] = SigmaZero;
|
|---|
| 513 | pv[1] = Proton;
|
|---|
| 514 | }
|
|---|
| 515 | else
|
|---|
| 516 | {
|
|---|
| 517 | pv[1] = SigmaPlus;
|
|---|
| 518 | }
|
|---|
| 519 | }
|
|---|
| 520 | else if (np == (1+nm))
|
|---|
| 521 | {
|
|---|
| 522 | pv[0] = SigmaMinus;
|
|---|
| 523 | }
|
|---|
| 524 | else
|
|---|
| 525 | {
|
|---|
| 526 | pv[0] = SigmaPlus;
|
|---|
| 527 | pv[1] = Proton;
|
|---|
| 528 | }
|
|---|
| 529 | }
|
|---|
| 530 |
|
|---|
| 531 |
|
|---|
| 532 | nt = np + nm + nz;
|
|---|
| 533 | while ( nt > 0)
|
|---|
| 534 | {
|
|---|
| 535 | G4double ran = G4UniformRand();
|
|---|
| 536 | if ( ran < (G4double)np/nt)
|
|---|
| 537 | {
|
|---|
| 538 | if( np > 0 )
|
|---|
| 539 | { pv[vecLen++] = PionPlus;
|
|---|
| 540 | np--;
|
|---|
| 541 | }
|
|---|
| 542 | }
|
|---|
| 543 | else if ( ran < (G4double)(np+nm)/nt)
|
|---|
| 544 | {
|
|---|
| 545 | if( nm > 0 )
|
|---|
| 546 | {
|
|---|
| 547 | pv[vecLen++] = PionMinus;
|
|---|
| 548 | nm--;
|
|---|
| 549 | }
|
|---|
| 550 | }
|
|---|
| 551 | else
|
|---|
| 552 | {
|
|---|
| 553 | if( nz > 0 )
|
|---|
| 554 | {
|
|---|
| 555 | pv[vecLen++] = PionZero;
|
|---|
| 556 | nz--;
|
|---|
| 557 | }
|
|---|
| 558 | }
|
|---|
| 559 | nt = np + nm + nz;
|
|---|
| 560 | }
|
|---|
| 561 | if (verboseLevel > 1)
|
|---|
| 562 | {
|
|---|
| 563 | G4cout << "Particles produced: " ;
|
|---|
| 564 | G4cout << pv[0].getName() << " " ;
|
|---|
| 565 | G4cout << pv[1].getName() << " " ;
|
|---|
| 566 | for (i=2; i < vecLen; i++)
|
|---|
| 567 | {
|
|---|
| 568 | G4cout << pv[i].getName() << " " ;
|
|---|
| 569 | }
|
|---|
| 570 | G4cout << G4endl;
|
|---|
| 571 | }
|
|---|
| 572 | return;
|
|---|
| 573 | }
|
|---|
| 574 |
|
|---|
| 575 |
|
|---|
| 576 |
|
|---|
| 577 |
|
|---|
| 578 |
|
|---|
| 579 |
|
|---|
| 580 |
|
|---|
| 581 |
|
|---|
| 582 |
|
|---|
| 583 |
|
|---|