| 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 | // G4AntiNeutronAnnihilationAtRest physics process
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| 27 | // Larry Felawka (TRIUMF), April 1998
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| 28 | //---------------------------------------------------------------------
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| 29 |
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| 30 | #include "G4AntiNeutronAnnihilationAtRest.hh"
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| 31 | #include "G4DynamicParticle.hh"
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| 32 | #include "G4ParticleTypes.hh"
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| 33 | #include "Randomize.hh"
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| 34 | #include <string.h>
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| 35 | #include <cmath>
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| 36 | #include <stdio.h>
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| 37 |
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| 38 | #define MAX_SECONDARIES 100
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| 39 |
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| 40 | // constructor
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| 41 |
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| 42 | G4AntiNeutronAnnihilationAtRest::G4AntiNeutronAnnihilationAtRest(const G4String& processName,
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| 43 | G4ProcessType aType) :
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| 44 | G4VRestProcess (processName, aType), // initialization
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| 45 | massPionMinus(G4PionMinus::PionMinus()->GetPDGMass()/GeV),
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| 46 | massPionZero(G4PionZero::PionZero()->GetPDGMass()/GeV),
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| 47 | massPionPlus(G4PionPlus::PionPlus()->GetPDGMass()/GeV),
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| 48 | massGamma(G4Gamma::Gamma()->GetPDGMass()/GeV),
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| 49 | massAntiNeutron(G4AntiNeutron::AntiNeutron()->GetPDGMass()/GeV),
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| 50 | massNeutron(G4Neutron::Neutron()->GetPDGMass()/GeV),
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| 51 | pdefGamma(G4Gamma::Gamma()),
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| 52 | pdefPionPlus(G4PionPlus::PionPlus()),
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| 53 | pdefPionZero(G4PionZero::PionZero()),
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| 54 | pdefPionMinus(G4PionMinus::PionMinus()),
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| 55 | pdefProton(G4Proton::Proton()),
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| 56 | pdefNeutron(G4Neutron::Neutron()),
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| 57 | pdefAntiNeutron(G4AntiNeutron::AntiNeutron()),
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| 58 | pdefDeuteron(G4Deuteron::Deuteron()),
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| 59 | pdefTriton(G4Triton::Triton()),
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| 60 | pdefAlpha(G4Alpha::Alpha())
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| 61 | {
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| 62 | if (verboseLevel>0) {
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| 63 | G4cout << GetProcessName() << " is created "<< G4endl;
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| 64 | }
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| 65 | SetProcessSubType(fHadronAtRest);
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| 66 | pv = new G4GHEKinematicsVector [MAX_SECONDARIES+1];
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| 67 | eve = new G4GHEKinematicsVector [MAX_SECONDARIES];
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| 68 | gkin = new G4GHEKinematicsVector [MAX_SECONDARIES];
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| 69 |
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| 70 | }
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| 71 |
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| 72 | // destructor
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| 73 |
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| 74 | G4AntiNeutronAnnihilationAtRest::~G4AntiNeutronAnnihilationAtRest()
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| 75 | {
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| 76 | delete [] pv;
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| 77 | delete [] eve;
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| 78 | delete [] gkin;
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| 79 | }
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| 80 |
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| 81 |
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| 82 | // methods.............................................................................
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| 83 |
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| 84 | G4bool G4AntiNeutronAnnihilationAtRest::IsApplicable(
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| 85 | const G4ParticleDefinition& particle
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| 86 | )
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| 87 | {
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| 88 | return ( &particle == pdefAntiNeutron );
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| 89 |
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| 90 | }
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| 91 |
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| 92 | // Warning - this method may be optimized away if made "inline"
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| 93 | G4int G4AntiNeutronAnnihilationAtRest::GetNumberOfSecondaries()
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| 94 | {
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| 95 | return ( ngkine );
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| 96 |
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| 97 | }
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| 98 |
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| 99 | // Warning - this method may be optimized away if made "inline"
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| 100 | G4GHEKinematicsVector* G4AntiNeutronAnnihilationAtRest::GetSecondaryKinematics()
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| 101 | {
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| 102 | return ( &gkin[0] );
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| 103 |
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| 104 | }
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| 105 |
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| 106 | G4double G4AntiNeutronAnnihilationAtRest::AtRestGetPhysicalInteractionLength(
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| 107 | const G4Track& track,
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| 108 | G4ForceCondition* condition
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| 109 | )
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| 110 | {
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| 111 | // beggining of tracking
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| 112 | ResetNumberOfInteractionLengthLeft();
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| 113 |
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| 114 | // condition is set to "Not Forced"
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| 115 | *condition = NotForced;
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| 116 |
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| 117 | // get mean life time
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| 118 | currentInteractionLength = GetMeanLifeTime(track, condition);
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| 119 |
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| 120 | if ((currentInteractionLength <0.0) || (verboseLevel>2)){
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| 121 | G4cout << "G4AntiNeutronAnnihilationAtRestProcess::AtRestGetPhysicalInteractionLength ";
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| 122 | G4cout << "[ " << GetProcessName() << "]" <<G4endl;
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| 123 | track.GetDynamicParticle()->DumpInfo();
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| 124 | G4cout << " in Material " << track.GetMaterial()->GetName() <<G4endl;
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| 125 | G4cout << "MeanLifeTime = " << currentInteractionLength/ns << "[ns]" <<G4endl;
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| 126 | }
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| 127 |
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| 128 | return theNumberOfInteractionLengthLeft * currentInteractionLength;
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| 129 |
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| 130 | }
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| 131 |
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| 132 | G4VParticleChange* G4AntiNeutronAnnihilationAtRest::AtRestDoIt(
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| 133 | const G4Track& track,
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| 134 | const G4Step&
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| 135 | )
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| 136 | //
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| 137 | // Handles AntiNeutrons at rest; an AntiNeutron can either create secondaries
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| 138 | // or do nothing (in which case it should be sent back to decay-handling
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| 139 | // section
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| 140 | //
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| 141 | {
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| 142 |
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| 143 | // Initialize ParticleChange
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| 144 | // all members of G4VParticleChange are set to equal to
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| 145 | // corresponding member in G4Track
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| 146 |
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| 147 | aParticleChange.Initialize(track);
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| 148 |
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| 149 | // Store some global quantities that depend on current material and particle
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| 150 |
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| 151 | globalTime = track.GetGlobalTime()/s;
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| 152 | G4Material * aMaterial = track.GetMaterial();
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| 153 | const G4int numberOfElements = aMaterial->GetNumberOfElements();
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| 154 | const G4ElementVector* theElementVector = aMaterial->GetElementVector();
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| 155 |
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| 156 | const G4double* theAtomicNumberDensity = aMaterial->GetAtomicNumDensityVector();
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| 157 | G4double normalization = 0;
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| 158 | for ( G4int i1=0; i1 < numberOfElements; i1++ )
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| 159 | {
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| 160 | normalization += theAtomicNumberDensity[i1] ; // change when nucleon specific
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| 161 | // probabilities are included.
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| 162 | }
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| 163 | G4double runningSum= 0.;
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| 164 | G4double random = G4UniformRand()*normalization;
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| 165 | for ( G4int i2=0; i2 < numberOfElements; i2++ )
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| 166 | {
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| 167 | runningSum += theAtomicNumberDensity[i2]; // change when nucleon specific
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| 168 | // probabilities are included.
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| 169 | if (random<=runningSum)
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| 170 | {
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| 171 | targetCharge = G4double( ((*theElementVector)[i2])->GetZ());
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| 172 | targetAtomicMass = (*theElementVector)[i2]->GetN();
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| 173 | }
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| 174 | }
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| 175 | if (random>runningSum)
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| 176 | {
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| 177 | targetCharge = G4double( ((*theElementVector)[numberOfElements-1])->GetZ());
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| 178 | targetAtomicMass = (*theElementVector)[numberOfElements-1]->GetN();
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| 179 | }
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| 180 |
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| 181 | if (verboseLevel>1) {
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| 182 | G4cout << "G4AntiNeutronAnnihilationAtRest::AtRestDoIt is invoked " <<G4endl;
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| 183 | }
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| 184 |
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| 185 | G4ParticleMomentum momentum;
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| 186 | G4float localtime;
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| 187 |
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| 188 | G4ThreeVector position = track.GetPosition();
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| 189 |
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| 190 | GenerateSecondaries(); // Generate secondaries
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| 191 |
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| 192 | aParticleChange.SetNumberOfSecondaries( ngkine );
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| 193 |
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| 194 | for ( G4int isec = 0; isec < ngkine; isec++ ) {
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| 195 | G4DynamicParticle* aNewParticle = new G4DynamicParticle;
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| 196 | aNewParticle->SetDefinition( gkin[isec].GetParticleDef() );
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| 197 | aNewParticle->SetMomentum( gkin[isec].GetMomentum() * GeV );
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| 198 |
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| 199 | localtime = globalTime + gkin[isec].GetTOF();
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| 200 |
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| 201 | G4Track* aNewTrack = new G4Track( aNewParticle, localtime*s, position );
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| 202 | aNewTrack->SetTouchableHandle(track.GetTouchableHandle());
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| 203 | aParticleChange.AddSecondary( aNewTrack );
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| 204 |
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| 205 | }
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| 206 |
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| 207 | aParticleChange.ProposeLocalEnergyDeposit( 0.0*GeV );
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| 208 |
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| 209 | aParticleChange.ProposeTrackStatus(fStopAndKill); // Kill the incident AntiNeutron
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| 210 |
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| 211 | // clear InteractionLengthLeft
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| 212 |
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| 213 | ResetNumberOfInteractionLengthLeft();
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| 214 |
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| 215 | return &aParticleChange;
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| 216 |
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| 217 | }
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| 218 |
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| 219 |
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| 220 | void G4AntiNeutronAnnihilationAtRest::GenerateSecondaries()
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| 221 | {
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| 222 | static G4int index;
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| 223 | static G4int l;
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| 224 | static G4int nopt;
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| 225 | static G4int i;
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| 226 | static G4ParticleDefinition* jnd;
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| 227 |
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| 228 | for (i = 1; i <= MAX_SECONDARIES; ++i) {
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| 229 | pv[i].SetZero();
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| 230 | }
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| 231 |
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| 232 |
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| 233 | ngkine = 0; // number of generated secondary particles
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| 234 | ntot = 0;
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| 235 | result.SetZero();
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| 236 | result.SetMass( massAntiNeutron );
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| 237 | result.SetKineticEnergyAndUpdate( 0. );
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| 238 | result.SetTOF( 0. );
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| 239 | result.SetParticleDef( pdefAntiNeutron );
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| 240 |
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| 241 | // *** SELECT PROCESS FOR CURRENT PARTICLE ***
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| 242 |
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| 243 | AntiNeutronAnnihilation(&nopt);
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| 244 |
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| 245 | // *** CHECK WHETHER THERE ARE NEW PARTICLES GENERATED ***
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| 246 | if (ntot != 0 || result.GetParticleDef() != pdefAntiNeutron) {
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| 247 | // *** CURRENT PARTICLE IS NOT THE SAME AS IN THE BEGINNING OR/AND ***
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| 248 | // *** ONE OR MORE SECONDARIES HAVE BEEN GENERATED ***
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| 249 |
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| 250 | // --- INITIAL PARTICLE TYPE HAS BEEN CHANGED ==> PUT NEW TYPE ON ---
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| 251 | // --- THE GEANT TEMPORARY STACK ---
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| 252 |
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| 253 | // --- PUT PARTICLE ON THE STACK ---
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| 254 | gkin[0] = result;
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| 255 | gkin[0].SetTOF( result.GetTOF() * 5e-11 );
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| 256 | ngkine = 1;
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| 257 |
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| 258 | // --- ALL QUANTITIES ARE TAKEN FROM THE GHEISHA STACK WHERE THE ---
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| 259 | // --- CONVENTION IS THE FOLLOWING ---
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| 260 |
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| 261 | // --- ONE OR MORE SECONDARIES HAVE BEEN GENERATED ---
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| 262 | for (l = 1; l <= ntot; ++l) {
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| 263 | index = l - 1;
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| 264 | jnd = eve[index].GetParticleDef();
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| 265 |
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| 266 | // --- ADD PARTICLE TO THE STACK IF STACK NOT YET FULL ---
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| 267 | if (ngkine < MAX_SECONDARIES) {
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| 268 | gkin[ngkine] = eve[index];
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| 269 | gkin[ngkine].SetTOF( eve[index].GetTOF() * 5e-11 );
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| 270 | ++ngkine;
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| 271 | }
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| 272 | }
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| 273 | }
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| 274 | else {
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| 275 | // --- NO SECONDARIES GENERATED AND PARTICLE IS STILL THE SAME ---
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| 276 | // --- ==> COPY EVERYTHING BACK IN THE CURRENT GEANT STACK ---
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| 277 | ngkine = 0;
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| 278 | ntot = 0;
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| 279 | globalTime += result.GetTOF() * G4float(5e-11);
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| 280 | }
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| 281 |
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| 282 | // --- LIMIT THE VALUE OF NGKINE IN CASE OF OVERFLOW ---
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| 283 | ngkine = G4int(std::min(ngkine,G4int(MAX_SECONDARIES)));
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| 284 |
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| 285 | } // GenerateSecondaries
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| 286 |
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| 287 |
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| 288 | void G4AntiNeutronAnnihilationAtRest::Poisso(G4float xav, G4int *iran)
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| 289 | {
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| 290 | static G4int i;
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| 291 | static G4float r, p1, p2, p3;
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| 292 | static G4int mm;
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| 293 | static G4float rr, ran, rrr, ran1;
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| 294 |
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| 295 | // *** GENERATION OF POISSON DISTRIBUTION ***
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| 296 | // *** NVE 16-MAR-1988 CERN GENEVA ***
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| 297 | // ORIGIN : H.FESEFELDT (27-OCT-1983)
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| 298 |
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| 299 | // --- USE NORMAL DISTRIBUTION FOR <X> > 9.9 ---
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| 300 | if (xav > G4float(9.9)) {
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| 301 | // ** NORMAL DISTRIBUTION WITH SIGMA**2 = <X>
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| 302 | Normal(&ran1);
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| 303 | ran1 = xav + ran1 * std::sqrt(xav);
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| 304 | *iran = G4int(ran1);
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| 305 | if (*iran < 0) {
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| 306 | *iran = 0;
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| 307 | }
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| 308 | }
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| 309 | else {
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| 310 | mm = G4int(xav * G4float(5.));
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| 311 | *iran = 0;
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| 312 | if (mm > 0) {
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| 313 | r = std::exp(-G4double(xav));
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| 314 | ran1 = G4UniformRand();
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| 315 | if (ran1 > r) {
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| 316 | rr = r;
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| 317 | for (i = 1; i <= mm; ++i) {
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| 318 | ++(*iran);
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| 319 | if (i <= 5) {
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| 320 | rrr = std::pow(xav, G4float(i)) / NFac(i);
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| 321 | }
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| 322 | // ** STIRLING' S FORMULA FOR LARGE NUMBERS
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| 323 | if (i > 5) {
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| 324 | rrr = std::exp(i * std::log(xav) -
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| 325 | (i + G4float(.5)) * std::log(i * G4float(1.)) +
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| 326 | i - G4float(.9189385));
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| 327 | }
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| 328 | rr += r * rrr;
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| 329 | if (ran1 <= rr) {
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| 330 | break;
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| 331 | }
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| 332 | }
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| 333 | }
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| 334 | }
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| 335 | else {
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| 336 | // ** FOR VERY SMALL XAV TRY IRAN=1,2,3
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| 337 | p1 = xav * std::exp(-G4double(xav));
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| 338 | p2 = xav * p1 / G4float(2.);
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| 339 | p3 = xav * p2 / G4float(3.);
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| 340 | ran = G4UniformRand();
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| 341 | if (ran >= p3) {
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| 342 | if (ran >= p2) {
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| 343 | if (ran >= p1) {
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| 344 | *iran = 0;
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| 345 | }
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| 346 | else {
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| 347 | *iran = 1;
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| 348 | }
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| 349 | }
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| 350 | else {
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| 351 | *iran = 2;
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| 352 | }
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| 353 | }
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| 354 | else {
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| 355 | *iran = 3;
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| 356 | }
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| 357 | }
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| 358 | }
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| 359 |
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| 360 | } // Poisso
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| 361 |
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| 362 |
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| 363 | G4int G4AntiNeutronAnnihilationAtRest::NFac(G4int n)
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| 364 | {
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| 365 | G4int ret_val;
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| 366 |
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| 367 | static G4int i, m;
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| 368 |
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| 369 | // *** NVE 16-MAR-1988 CERN GENEVA ***
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| 370 | // ORIGIN : H.FESEFELDT (27-OCT-1983)
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| 371 |
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| 372 | ret_val = 1;
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| 373 | m = n;
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| 374 | if (m > 1) {
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| 375 | if (m > 10) {
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| 376 | m = 10;
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| 377 | }
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| 378 | for (i = 2; i <= m; ++i) {
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| 379 | ret_val *= i;
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| 380 | }
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| 381 | }
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| 382 | return ret_val;
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| 383 |
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| 384 | } // NFac
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| 385 |
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| 386 |
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| 387 | void G4AntiNeutronAnnihilationAtRest::Normal(G4float *ran)
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| 388 | {
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| 389 | static G4int i;
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| 390 |
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| 391 | // *** NVE 14-APR-1988 CERN GENEVA ***
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| 392 | // ORIGIN : H.FESEFELDT (27-OCT-1983)
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| 393 |
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| 394 | *ran = G4float(-6.);
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| 395 | for (i = 1; i <= 12; ++i) {
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| 396 | *ran += G4UniformRand();
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| 397 | }
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| 398 |
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| 399 | } // Normal
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| 400 |
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| 401 |
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| 402 | void G4AntiNeutronAnnihilationAtRest::AntiNeutronAnnihilation(G4int *nopt)
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| 403 | {
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| 404 | static G4float brr[3] = { G4float(.125),G4float(.25),G4float(.5) };
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| 405 |
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| 406 | G4float r__1;
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| 407 |
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| 408 | static G4int i, ii, kk;
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| 409 | static G4int nt;
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| 410 | static G4float cfa, eka;
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| 411 | static G4int ika, nbl;
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| 412 | static G4float ran, pcm;
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| 413 | static G4int isw;
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| 414 | static G4float tex;
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| 415 | static G4ParticleDefinition* ipa1;
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| 416 | static G4float ran1, ran2, ekin, tkin;
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| 417 | static G4float targ;
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| 418 | static G4ParticleDefinition* inve;
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| 419 | static G4float ekin1, ekin2, black;
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| 420 | static G4float pnrat, rmnve1, rmnve2;
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| 421 | static G4float ek, en;
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| 422 |
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| 423 | // *** ANTI NEUTRON ANNIHILATION AT REST ***
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| 424 | // *** NVE 04-MAR-1988 CERN GENEVA ***
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| 425 | // ORIGIN : H.FESEFELDT (09-JULY-1987)
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| 426 |
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| 427 | // NOPT=0 NO ANNIHILATION
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| 428 | // NOPT=1 ANNIH.IN PI+ PI-
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| 429 | // NOPT=2 ANNIH.IN PI0 PI0
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| 430 | // NOPT=3 ANNIH.IN PI+ PI0
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| 431 | // NOPT=4 ANNIH.IN GAMMA GAMMA
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| 432 |
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| 433 | pv[1].SetZero();
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| 434 | pv[1].SetMass( massAntiNeutron );
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| 435 | pv[1].SetKineticEnergyAndUpdate( 0. );
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| 436 | pv[1].SetTOF( result.GetTOF() );
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| 437 | pv[1].SetParticleDef( result.GetParticleDef() );
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| 438 | isw = 1;
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| 439 | ran = G4UniformRand();
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| 440 | if (ran > brr[0]) {
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| 441 | isw = 2;
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| 442 | }
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| 443 | if (ran > brr[1]) {
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| 444 | isw = 3;
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| 445 | }
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| 446 | if (ran > brr[2]) {
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| 447 | isw = 4;
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| 448 | }
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| 449 | *nopt = isw;
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| 450 | // **
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| 451 | // ** EVAPORATION
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| 452 | // **
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| 453 | rmnve1 = massPionPlus;
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| 454 | rmnve2 = massPionMinus;
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| 455 | if (isw == 2) {
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| 456 | rmnve1 = massPionZero;
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| 457 | }
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| 458 | if (isw == 2) {
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| 459 | rmnve2 = massPionZero;
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| 460 | }
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| 461 | if (isw == 3) {
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| 462 | rmnve2 = massPionZero;
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| 463 | }
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| 464 | if (isw == 4) {
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| 465 | rmnve1 = massGamma;
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| 466 | }
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| 467 | if (isw == 4) {
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| 468 | rmnve2 = massGamma;
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| 469 | }
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| 470 | ek = massNeutron + massAntiNeutron - rmnve1 - rmnve2;
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| 471 | tkin = ExNu(ek);
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| 472 | ek -= tkin;
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| 473 | if (ek < G4float(1e-4)) {
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| 474 | ek = G4float(1e-4);
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| 475 | }
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| 476 | ek /= G4float(2.);
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| 477 | en = ek + (rmnve1 + rmnve2) / G4float(2.);
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| 478 | r__1 = en * en - rmnve1 * rmnve2;
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| 479 | pcm = r__1 > 0 ? std::sqrt(r__1) : 0;
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| 480 | pv[2].SetZero();
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| 481 | pv[2].SetMass( rmnve1 );
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| 482 | pv[3].SetZero();
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| 483 | pv[3].SetMass( rmnve2 );
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| 484 | if (isw > 3) {
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| 485 | pv[2].SetMass( 0. );
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| 486 | pv[3].SetMass( 0. );
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| 487 | }
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| 488 | pv[2].SetEnergyAndUpdate( std::sqrt(pv[2].GetMass()*pv[2].GetMass()+pcm*pcm) );
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| 489 | pv[2].SetTOF( result.GetTOF() );
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| 490 | pv[3].SetEnergy( std::sqrt(pv[3].GetMass()*pv[3].GetMass()+pcm*pcm) );
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| 491 | pv[3].SetMomentumAndUpdate( -pv[2].GetMomentum().x(), -pv[2].GetMomentum().y(), -pv[2].GetMomentum().z() );
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| 492 | pv[3].SetTOF( result.GetTOF() );
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| 493 | switch ((int)isw) {
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| 494 | case 1:
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| 495 | pv[2].SetParticleDef( pdefPionPlus );
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| 496 | pv[3].SetParticleDef( pdefPionMinus );
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| 497 | break;
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| 498 | case 2:
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| 499 | pv[2].SetParticleDef( pdefPionZero );
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| 500 | pv[3].SetParticleDef( pdefPionZero );
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| 501 | break;
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| 502 | case 3:
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| 503 | pv[2].SetParticleDef( pdefPionPlus );
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| 504 | pv[3].SetParticleDef( pdefPionZero );
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| 505 | break;
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| 506 | case 4:
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| 507 | pv[2].SetParticleDef( pdefGamma );
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| 508 | pv[3].SetParticleDef( pdefGamma );
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| 509 | break;
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| 510 | default:
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| 511 | break;
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| 512 | }
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| 513 | nt = 3;
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| 514 | if (targetAtomicMass >= G4float(1.5)) {
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| 515 | cfa = (targetAtomicMass - G4float(1.)) / G4float(120.) *
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| 516 | G4float(.025) * std::exp(-G4double(targetAtomicMass - G4float(1.)) /
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| 517 | G4float(120.));
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| 518 | targ = G4float(1.);
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| 519 | tex = evapEnergy1;
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| 520 | if (tex >= G4float(.001)) {
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| 521 | black = (targ * G4float(1.25) +
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| 522 | G4float(1.5)) * evapEnergy1 / (evapEnergy1 + evapEnergy3);
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| 523 | Poisso(black, &nbl);
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| 524 | if (G4float(G4int(targ) + nbl) > targetAtomicMass) {
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| 525 | nbl = G4int(targetAtomicMass - targ);
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| 526 | }
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| 527 | if (nt + nbl > (MAX_SECONDARIES - 2)) {
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| 528 | nbl = (MAX_SECONDARIES - 2) - nt;
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| 529 | }
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| 530 | if (nbl > 0) {
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| 531 | ekin = tex / nbl;
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| 532 | ekin2 = G4float(0.);
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| 533 | for (i = 1; i <= nbl; ++i) {
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| 534 | if (nt == (MAX_SECONDARIES - 2)) {
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| 535 | continue;
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| 536 | }
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| 537 | if (ekin2 > tex) {
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| 538 | break;
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| 539 | }
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| 540 | ran1 = G4UniformRand();
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| 541 | Normal(&ran2);
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| 542 | ekin1 = -G4double(ekin) * std::log(ran1) -
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| 543 | cfa * (ran2 * G4float(.5) + G4float(1.));
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| 544 | if (ekin1 < G4float(0.)) {
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| 545 | ekin1 = std::log(ran1) * G4float(-.01);
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| 546 | }
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| 547 | ekin1 *= G4float(1.);
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| 548 | ekin2 += ekin1;
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| 549 | if (ekin2 > tex) {
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| 550 | ekin1 = tex - (ekin2 - ekin1);
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| 551 | }
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| 552 | if (ekin1 < G4float(0.)) {
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| 553 | ekin1 = G4float(.001);
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| 554 | }
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| 555 | ipa1 = pdefNeutron;
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| 556 | pnrat = G4float(1.) - targetCharge / targetAtomicMass;
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| 557 | if (G4UniformRand() > pnrat) {
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| 558 | ipa1 = pdefProton;
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| 559 | }
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| 560 | ++nt;
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| 561 | pv[nt].SetZero();
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| 562 | pv[nt].SetMass( ipa1->GetPDGMass()/GeV );
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| 563 | pv[nt].SetKineticEnergyAndUpdate( ekin1 );
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| 564 | pv[nt].SetTOF( result.GetTOF() );
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| 565 | pv[nt].SetParticleDef( ipa1 );
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| 566 | }
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| 567 | if (targetAtomicMass >= G4float(230.) && ek <= G4float(2.)) {
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| 568 | ii = nt + 1;
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| 569 | kk = 0;
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| 570 | eka = ek;
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| 571 | if (eka > G4float(1.)) {
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| 572 | eka *= eka;
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| 573 | }
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| 574 | if (eka < G4float(.1)) {
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| 575 | eka = G4float(.1);
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| 576 | }
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| 577 | ika = G4int(G4float(3.6) / eka);
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| 578 | for (i = 1; i <= nt; ++i) {
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| 579 | --ii;
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| 580 | if (pv[ii].GetParticleDef() != pdefProton) {
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| 581 | continue;
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| 582 | }
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| 583 | ipa1 = pdefNeutron;
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| 584 | pv[ii].SetMass( ipa1->GetPDGMass()/GeV );
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| 585 | pv[ii].SetParticleDef( ipa1 );
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| 586 | ++kk;
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| 587 | if (kk > ika) {
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| 588 | break;
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| 589 | }
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| 590 | }
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| 591 | }
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| 592 | }
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| 593 | }
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| 594 | // **
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| 595 | // ** THEN ALSO DEUTERONS, TRITONS AND ALPHAS
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| 596 | // **
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| 597 | tex = evapEnergy3;
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| 598 | if (tex >= G4float(.001)) {
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| 599 | black = (targ * G4float(1.25) + G4float(1.5)) * evapEnergy3 /
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| 600 | (evapEnergy1 + evapEnergy3);
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| 601 | Poisso(black, &nbl);
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| 602 | if (nt + nbl > (MAX_SECONDARIES - 2)) {
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| 603 | nbl = (MAX_SECONDARIES - 2) - nt;
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| 604 | }
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| 605 | if (nbl > 0) {
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| 606 | ekin = tex / nbl;
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| 607 | ekin2 = G4float(0.);
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| 608 | for (i = 1; i <= nbl; ++i) {
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| 609 | if (nt == (MAX_SECONDARIES - 2)) {
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| 610 | continue;
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| 611 | }
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| 612 | if (ekin2 > tex) {
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| 613 | break;
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| 614 | }
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|---|
| 615 | ran1 = G4UniformRand();
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| 616 | Normal(&ran2);
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| 617 | ekin1 = -G4double(ekin) * std::log(ran1) -
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| 618 | cfa * (ran2 * G4float(.5) + G4float(1.));
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| 619 | if (ekin1 < G4float(0.)) {
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| 620 | ekin1 = std::log(ran1) * G4float(-.01);
|
|---|
| 621 | }
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|---|
| 622 | ekin1 *= G4float(1.);
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| 623 | ekin2 += ekin1;
|
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| 624 | if (ekin2 > tex) {
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| 625 | ekin1 = tex - (ekin2 - ekin1);
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| 626 | }
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|---|
| 627 | if (ekin1 < G4float(0.)) {
|
|---|
| 628 | ekin1 = G4float(.001);
|
|---|
| 629 | }
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|---|
| 630 | ran = G4UniformRand();
|
|---|
| 631 | inve = pdefDeuteron;
|
|---|
| 632 | if (ran > G4float(.6)) {
|
|---|
| 633 | inve = pdefTriton;
|
|---|
| 634 | }
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|---|
| 635 | if (ran > G4float(.9)) {
|
|---|
| 636 | inve = pdefAlpha;
|
|---|
| 637 | }
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|---|
| 638 | ++nt;
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|---|
| 639 | pv[nt].SetZero();
|
|---|
| 640 | pv[nt].SetMass( inve->GetPDGMass()/GeV );
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|---|
| 641 | pv[nt].SetKineticEnergyAndUpdate( ekin1 );
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|---|
| 642 | pv[nt].SetTOF( result.GetTOF() );
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|---|
| 643 | pv[nt].SetParticleDef( inve );
|
|---|
| 644 | }
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|---|
| 645 | }
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|---|
| 646 | }
|
|---|
| 647 | }
|
|---|
| 648 | result = pv[2];
|
|---|
| 649 | if (nt == 2) {
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| 650 | return;
|
|---|
| 651 | }
|
|---|
| 652 | for (i = 3; i <= nt; ++i) {
|
|---|
| 653 | if (ntot >= MAX_SECONDARIES) {
|
|---|
| 654 | return;
|
|---|
| 655 | }
|
|---|
| 656 | eve[ntot++] = pv[i];
|
|---|
| 657 | }
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|---|
| 658 |
|
|---|
| 659 | } // AntiNeutronAnnihilation
|
|---|
| 660 |
|
|---|
| 661 |
|
|---|
| 662 | G4double G4AntiNeutronAnnihilationAtRest::ExNu(G4float ek1)
|
|---|
| 663 | {
|
|---|
| 664 | G4float ret_val, r__1;
|
|---|
| 665 |
|
|---|
| 666 | static G4float cfa, gfa, ran1, ran2, ekin1, atno3;
|
|---|
| 667 | static G4int magic;
|
|---|
| 668 | static G4float fpdiv;
|
|---|
| 669 |
|
|---|
| 670 | // *** NUCLEAR EVAPORATION AS FUNCTION OF ATOMIC NUMBER ATNO ***
|
|---|
| 671 | // *** AND KINETIC ENERGY EKIN OF PRIMARY PARTICLE ***
|
|---|
| 672 | // *** NVE 04-MAR-1988 CERN GENEVA ***
|
|---|
| 673 | // ORIGIN : H.FESEFELDT (10-DEC-1986)
|
|---|
| 674 |
|
|---|
| 675 | ret_val = G4float(0.);
|
|---|
| 676 | if (targetAtomicMass >= G4float(1.5)) {
|
|---|
| 677 | magic = 0;
|
|---|
| 678 | if (G4int(targetCharge + G4float(.1)) == 82) {
|
|---|
| 679 | magic = 1;
|
|---|
| 680 | }
|
|---|
| 681 | ekin1 = ek1;
|
|---|
| 682 | if (ekin1 < G4float(.1)) {
|
|---|
| 683 | ekin1 = G4float(.1);
|
|---|
| 684 | }
|
|---|
| 685 | if (ekin1 > G4float(4.)) {
|
|---|
| 686 | ekin1 = G4float(4.);
|
|---|
| 687 | }
|
|---|
| 688 | // ** 0.35 VALUE AT 1 GEV
|
|---|
| 689 | // ** 0.05 VALUE AT 0.1 GEV
|
|---|
| 690 | cfa = G4float(.13043478260869565);
|
|---|
| 691 | cfa = cfa * std::log(ekin1) + G4float(.35);
|
|---|
| 692 | if (cfa < G4float(.15)) {
|
|---|
| 693 | cfa = G4float(.15);
|
|---|
| 694 | }
|
|---|
| 695 | ret_val = cfa * G4float(7.716) * std::exp(-G4double(cfa));
|
|---|
| 696 | atno3 = targetAtomicMass;
|
|---|
| 697 | if (atno3 > G4float(120.)) {
|
|---|
| 698 | atno3 = G4float(120.);
|
|---|
| 699 | }
|
|---|
| 700 | cfa = (atno3 - G4float(1.)) /
|
|---|
| 701 | G4float(120.) * std::exp(-G4double(atno3 - G4float(1.)) / G4float(120.));
|
|---|
| 702 | ret_val *= cfa;
|
|---|
| 703 | r__1 = ekin1;
|
|---|
| 704 | fpdiv = G4float(1.) - r__1 * r__1 * G4float(.25);
|
|---|
| 705 | if (fpdiv < G4float(.5)) {
|
|---|
| 706 | fpdiv = G4float(.5);
|
|---|
| 707 | }
|
|---|
| 708 | gfa = (targetAtomicMass - G4float(1.)) /
|
|---|
| 709 | G4float(70.) * G4float(2.) *
|
|---|
| 710 | std::exp(-G4double(targetAtomicMass - G4float(1.)) / G4float(70.));
|
|---|
| 711 | evapEnergy1 = ret_val * fpdiv;
|
|---|
| 712 | evapEnergy3 = ret_val - evapEnergy1;
|
|---|
| 713 | Normal(&ran1);
|
|---|
| 714 | Normal(&ran2);
|
|---|
| 715 | if (magic == 1) {
|
|---|
| 716 | ran1 = G4float(0.);
|
|---|
| 717 | ran2 = G4float(0.);
|
|---|
| 718 | }
|
|---|
| 719 | evapEnergy1 *= ran1 * gfa + G4float(1.);
|
|---|
| 720 | if (evapEnergy1 < G4float(0.)) {
|
|---|
| 721 | evapEnergy1 = G4float(0.);
|
|---|
| 722 | }
|
|---|
| 723 | evapEnergy3 *= ran2 * gfa + G4float(1.);
|
|---|
| 724 | if (evapEnergy3 < G4float(0.)) {
|
|---|
| 725 | evapEnergy3 = G4float(0.);
|
|---|
| 726 | }
|
|---|
| 727 | while ((ret_val = evapEnergy1 + evapEnergy3) >= ek1) {
|
|---|
| 728 | evapEnergy1 *= G4float(1.) - G4UniformRand() * G4float(.5);
|
|---|
| 729 | evapEnergy3 *= G4float(1.) - G4UniformRand() * G4float(.5);
|
|---|
| 730 | }
|
|---|
| 731 | }
|
|---|
| 732 | return ret_val;
|
|---|
| 733 |
|
|---|
| 734 | } // ExNu
|
|---|