| 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 "G4HadronicProcessStore.hh"
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| 34 | #include "Randomize.hh"
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| 35 | #include <string.h>
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| 36 | #include <cmath>
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| 37 | #include <stdio.h>
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| 38 |
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| 39 | #define MAX_SECONDARIES 100
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| 40 |
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| 41 | // constructor
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| 42 |
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| 43 | G4AntiNeutronAnnihilationAtRest::G4AntiNeutronAnnihilationAtRest(const G4String& processName,
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| 44 | G4ProcessType aType) :
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| 45 | G4VRestProcess (processName, aType), // initialization
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| 46 | massPionMinus(G4PionMinus::PionMinus()->GetPDGMass()/GeV),
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| 47 | massPionZero(G4PionZero::PionZero()->GetPDGMass()/GeV),
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| 48 | massPionPlus(G4PionPlus::PionPlus()->GetPDGMass()/GeV),
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| 49 | massGamma(G4Gamma::Gamma()->GetPDGMass()/GeV),
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| 50 | massAntiNeutron(G4AntiNeutron::AntiNeutron()->GetPDGMass()/GeV),
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| 51 | massNeutron(G4Neutron::Neutron()->GetPDGMass()/GeV),
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| 52 | pdefGamma(G4Gamma::Gamma()),
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| 53 | pdefPionPlus(G4PionPlus::PionPlus()),
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| 54 | pdefPionZero(G4PionZero::PionZero()),
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| 55 | pdefPionMinus(G4PionMinus::PionMinus()),
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| 56 | pdefProton(G4Proton::Proton()),
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| 57 | pdefNeutron(G4Neutron::Neutron()),
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| 58 | pdefAntiNeutron(G4AntiNeutron::AntiNeutron()),
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| 59 | pdefDeuteron(G4Deuteron::Deuteron()),
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| 60 | pdefTriton(G4Triton::Triton()),
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| 61 | pdefAlpha(G4Alpha::Alpha())
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| 62 | {
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| 63 | if (verboseLevel>0) {
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| 64 | G4cout << GetProcessName() << " is created "<< G4endl;
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| 65 | }
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| 66 | SetProcessSubType(fHadronAtRest);
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| 67 | pv = new G4GHEKinematicsVector [MAX_SECONDARIES+1];
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| 68 | eve = new G4GHEKinematicsVector [MAX_SECONDARIES];
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| 69 | gkin = new G4GHEKinematicsVector [MAX_SECONDARIES];
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| 70 |
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| 71 | G4HadronicProcessStore::Instance()->RegisterExtraProcess(this);
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| 72 | }
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| 73 |
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| 74 | // destructor
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| 75 |
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| 76 | G4AntiNeutronAnnihilationAtRest::~G4AntiNeutronAnnihilationAtRest()
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| 77 | {
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| 78 | G4HadronicProcessStore::Instance()->DeRegisterExtraProcess(this);
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| 79 | delete [] pv;
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| 80 | delete [] eve;
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| 81 | delete [] gkin;
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| 82 | }
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| 83 |
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| 84 | void G4AntiNeutronAnnihilationAtRest::PreparePhysicsTable(const G4ParticleDefinition& p)
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| 85 | {
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| 86 | G4HadronicProcessStore::Instance()->RegisterParticleForExtraProcess(this, &p);
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| 87 | }
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| 88 |
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| 89 | void G4AntiNeutronAnnihilationAtRest::BuildPhysicsTable(const G4ParticleDefinition& p)
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| 90 | {
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| 91 | G4HadronicProcessStore::Instance()->PrintInfo(&p);
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| 92 | }
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| 93 |
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| 94 | // methods.............................................................................
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| 95 |
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| 96 | G4bool G4AntiNeutronAnnihilationAtRest::IsApplicable(
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| 97 | const G4ParticleDefinition& particle
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| 98 | )
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| 99 | {
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| 100 | return ( &particle == pdefAntiNeutron );
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| 101 |
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| 102 | }
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| 103 |
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| 104 | // Warning - this method may be optimized away if made "inline"
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| 105 | G4int G4AntiNeutronAnnihilationAtRest::GetNumberOfSecondaries()
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| 106 | {
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| 107 | return ( ngkine );
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| 108 |
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| 109 | }
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| 110 |
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| 111 | // Warning - this method may be optimized away if made "inline"
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| 112 | G4GHEKinematicsVector* G4AntiNeutronAnnihilationAtRest::GetSecondaryKinematics()
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| 113 | {
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| 114 | return ( &gkin[0] );
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| 115 |
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| 116 | }
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| 117 |
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| 118 | G4double G4AntiNeutronAnnihilationAtRest::AtRestGetPhysicalInteractionLength(
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| 119 | const G4Track& track,
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| 120 | G4ForceCondition* condition
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| 121 | )
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| 122 | {
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| 123 | // beggining of tracking
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| 124 | ResetNumberOfInteractionLengthLeft();
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| 125 |
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| 126 | // condition is set to "Not Forced"
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| 127 | *condition = NotForced;
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| 128 |
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| 129 | // get mean life time
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| 130 | currentInteractionLength = GetMeanLifeTime(track, condition);
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| 131 |
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| 132 | if ((currentInteractionLength <0.0) || (verboseLevel>2)){
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| 133 | G4cout << "G4AntiNeutronAnnihilationAtRestProcess::AtRestGetPhysicalInteractionLength ";
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| 134 | G4cout << "[ " << GetProcessName() << "]" <<G4endl;
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| 135 | track.GetDynamicParticle()->DumpInfo();
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| 136 | G4cout << " in Material " << track.GetMaterial()->GetName() <<G4endl;
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| 137 | G4cout << "MeanLifeTime = " << currentInteractionLength/ns << "[ns]" <<G4endl;
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| 138 | }
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| 139 |
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| 140 | return theNumberOfInteractionLengthLeft * currentInteractionLength;
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| 141 |
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| 142 | }
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| 143 |
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| 144 | G4VParticleChange* G4AntiNeutronAnnihilationAtRest::AtRestDoIt(
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| 145 | const G4Track& track,
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| 146 | const G4Step&
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| 147 | )
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| 148 | //
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| 149 | // Handles AntiNeutrons at rest; an AntiNeutron can either create secondaries
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| 150 | // or do nothing (in which case it should be sent back to decay-handling
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| 151 | // section
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| 152 | //
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| 153 | {
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| 154 |
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| 155 | // Initialize ParticleChange
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| 156 | // all members of G4VParticleChange are set to equal to
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| 157 | // corresponding member in G4Track
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| 158 |
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| 159 | aParticleChange.Initialize(track);
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| 160 |
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| 161 | // Store some global quantities that depend on current material and particle
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| 162 |
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| 163 | globalTime = track.GetGlobalTime()/s;
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| 164 | G4Material * aMaterial = track.GetMaterial();
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| 165 | const G4int numberOfElements = aMaterial->GetNumberOfElements();
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| 166 | const G4ElementVector* theElementVector = aMaterial->GetElementVector();
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| 167 |
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| 168 | const G4double* theAtomicNumberDensity = aMaterial->GetAtomicNumDensityVector();
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| 169 | G4double normalization = 0;
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| 170 | for ( G4int i1=0; i1 < numberOfElements; i1++ )
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| 171 | {
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| 172 | normalization += theAtomicNumberDensity[i1] ; // change when nucleon specific
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| 173 | // probabilities are included.
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| 174 | }
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| 175 | G4double runningSum= 0.;
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| 176 | G4double random = G4UniformRand()*normalization;
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| 177 | for ( G4int i2=0; i2 < numberOfElements; i2++ )
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| 178 | {
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| 179 | runningSum += theAtomicNumberDensity[i2]; // change when nucleon specific
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| 180 | // probabilities are included.
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| 181 | if (random<=runningSum)
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| 182 | {
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| 183 | targetCharge = G4double( ((*theElementVector)[i2])->GetZ());
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| 184 | targetAtomicMass = (*theElementVector)[i2]->GetN();
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| 185 | }
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| 186 | }
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| 187 | if (random>runningSum)
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| 188 | {
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| 189 | targetCharge = G4double( ((*theElementVector)[numberOfElements-1])->GetZ());
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| 190 | targetAtomicMass = (*theElementVector)[numberOfElements-1]->GetN();
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| 191 | }
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| 192 |
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| 193 | if (verboseLevel>1) {
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| 194 | G4cout << "G4AntiNeutronAnnihilationAtRest::AtRestDoIt is invoked " <<G4endl;
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| 195 | }
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| 196 |
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| 197 | G4ParticleMomentum momentum;
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| 198 | G4float localtime;
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| 199 |
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| 200 | G4ThreeVector position = track.GetPosition();
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| 201 |
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| 202 | GenerateSecondaries(); // Generate secondaries
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| 203 |
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| 204 | aParticleChange.SetNumberOfSecondaries( ngkine );
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| 205 |
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| 206 | for ( G4int isec = 0; isec < ngkine; isec++ ) {
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| 207 | G4DynamicParticle* aNewParticle = new G4DynamicParticle;
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| 208 | aNewParticle->SetDefinition( gkin[isec].GetParticleDef() );
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| 209 | aNewParticle->SetMomentum( gkin[isec].GetMomentum() * GeV );
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| 210 |
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| 211 | localtime = globalTime + gkin[isec].GetTOF();
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| 212 |
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| 213 | G4Track* aNewTrack = new G4Track( aNewParticle, localtime*s, position );
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| 214 | aNewTrack->SetTouchableHandle(track.GetTouchableHandle());
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| 215 | aParticleChange.AddSecondary( aNewTrack );
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| 216 |
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| 217 | }
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| 218 |
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| 219 | aParticleChange.ProposeLocalEnergyDeposit( 0.0*GeV );
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| 220 |
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| 221 | aParticleChange.ProposeTrackStatus(fStopAndKill); // Kill the incident AntiNeutron
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| 222 |
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| 223 | // clear InteractionLengthLeft
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| 224 |
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| 225 | ResetNumberOfInteractionLengthLeft();
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| 226 |
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| 227 | return &aParticleChange;
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| 228 |
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| 229 | }
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| 230 |
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| 231 |
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| 232 | void G4AntiNeutronAnnihilationAtRest::GenerateSecondaries()
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| 233 | {
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| 234 | static G4int index;
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| 235 | static G4int l;
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| 236 | static G4int nopt;
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| 237 | static G4int i;
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| 238 | static G4ParticleDefinition* jnd;
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| 239 |
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| 240 | for (i = 1; i <= MAX_SECONDARIES; ++i) {
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| 241 | pv[i].SetZero();
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| 242 | }
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| 243 |
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| 244 |
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| 245 | ngkine = 0; // number of generated secondary particles
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| 246 | ntot = 0;
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| 247 | result.SetZero();
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| 248 | result.SetMass( massAntiNeutron );
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| 249 | result.SetKineticEnergyAndUpdate( 0. );
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| 250 | result.SetTOF( 0. );
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| 251 | result.SetParticleDef( pdefAntiNeutron );
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| 252 |
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| 253 | // *** SELECT PROCESS FOR CURRENT PARTICLE ***
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| 254 |
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| 255 | AntiNeutronAnnihilation(&nopt);
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| 256 |
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| 257 | // *** CHECK WHETHER THERE ARE NEW PARTICLES GENERATED ***
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| 258 | if (ntot != 0 || result.GetParticleDef() != pdefAntiNeutron) {
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| 259 | // *** CURRENT PARTICLE IS NOT THE SAME AS IN THE BEGINNING OR/AND ***
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| 260 | // *** ONE OR MORE SECONDARIES HAVE BEEN GENERATED ***
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| 261 |
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| 262 | // --- INITIAL PARTICLE TYPE HAS BEEN CHANGED ==> PUT NEW TYPE ON ---
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| 263 | // --- THE GEANT TEMPORARY STACK ---
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| 264 |
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| 265 | // --- PUT PARTICLE ON THE STACK ---
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| 266 | gkin[0] = result;
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| 267 | gkin[0].SetTOF( result.GetTOF() * 5e-11 );
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| 268 | ngkine = 1;
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| 269 |
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| 270 | // --- ALL QUANTITIES ARE TAKEN FROM THE GHEISHA STACK WHERE THE ---
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| 271 | // --- CONVENTION IS THE FOLLOWING ---
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| 272 |
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| 273 | // --- ONE OR MORE SECONDARIES HAVE BEEN GENERATED ---
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| 274 | for (l = 1; l <= ntot; ++l) {
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| 275 | index = l - 1;
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| 276 | jnd = eve[index].GetParticleDef();
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| 277 |
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| 278 | // --- ADD PARTICLE TO THE STACK IF STACK NOT YET FULL ---
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| 279 | if (ngkine < MAX_SECONDARIES) {
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| 280 | gkin[ngkine] = eve[index];
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| 281 | gkin[ngkine].SetTOF( eve[index].GetTOF() * 5e-11 );
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| 282 | ++ngkine;
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| 283 | }
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| 284 | }
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| 285 | }
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| 286 | else {
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| 287 | // --- NO SECONDARIES GENERATED AND PARTICLE IS STILL THE SAME ---
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| 288 | // --- ==> COPY EVERYTHING BACK IN THE CURRENT GEANT STACK ---
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| 289 | ngkine = 0;
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| 290 | ntot = 0;
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| 291 | globalTime += result.GetTOF() * G4float(5e-11);
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| 292 | }
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| 293 |
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| 294 | // --- LIMIT THE VALUE OF NGKINE IN CASE OF OVERFLOW ---
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| 295 | ngkine = G4int(std::min(ngkine,G4int(MAX_SECONDARIES)));
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| 296 |
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| 297 | } // GenerateSecondaries
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| 298 |
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| 299 |
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| 300 | void G4AntiNeutronAnnihilationAtRest::Poisso(G4float xav, G4int *iran)
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| 301 | {
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| 302 | static G4int i;
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| 303 | static G4float r, p1, p2, p3;
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| 304 | static G4int mm;
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| 305 | static G4float rr, ran, rrr, ran1;
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| 306 |
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| 307 | // *** GENERATION OF POISSON DISTRIBUTION ***
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| 308 | // *** NVE 16-MAR-1988 CERN GENEVA ***
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| 309 | // ORIGIN : H.FESEFELDT (27-OCT-1983)
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| 310 |
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| 311 | // --- USE NORMAL DISTRIBUTION FOR <X> > 9.9 ---
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| 312 | if (xav > G4float(9.9)) {
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| 313 | // ** NORMAL DISTRIBUTION WITH SIGMA**2 = <X>
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| 314 | Normal(&ran1);
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| 315 | ran1 = xav + ran1 * std::sqrt(xav);
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| 316 | *iran = G4int(ran1);
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| 317 | if (*iran < 0) {
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| 318 | *iran = 0;
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| 319 | }
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| 320 | }
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| 321 | else {
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| 322 | mm = G4int(xav * G4float(5.));
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| 323 | *iran = 0;
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| 324 | if (mm > 0) {
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| 325 | r = std::exp(-G4double(xav));
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| 326 | ran1 = G4UniformRand();
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| 327 | if (ran1 > r) {
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| 328 | rr = r;
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| 329 | for (i = 1; i <= mm; ++i) {
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| 330 | ++(*iran);
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| 331 | if (i <= 5) {
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| 332 | rrr = std::pow(xav, G4float(i)) / NFac(i);
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| 333 | }
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| 334 | // ** STIRLING' S FORMULA FOR LARGE NUMBERS
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| 335 | if (i > 5) {
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| 336 | rrr = std::exp(i * std::log(xav) -
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| 337 | (i + G4float(.5)) * std::log(i * G4float(1.)) +
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| 338 | i - G4float(.9189385));
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| 339 | }
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| 340 | rr += r * rrr;
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| 341 | if (ran1 <= rr) {
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| 342 | break;
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| 343 | }
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| 344 | }
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| 345 | }
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| 346 | }
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| 347 | else {
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| 348 | // ** FOR VERY SMALL XAV TRY IRAN=1,2,3
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| 349 | p1 = xav * std::exp(-G4double(xav));
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| 350 | p2 = xav * p1 / G4float(2.);
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| 351 | p3 = xav * p2 / G4float(3.);
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| 352 | ran = G4UniformRand();
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| 353 | if (ran >= p3) {
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| 354 | if (ran >= p2) {
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| 355 | if (ran >= p1) {
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| 356 | *iran = 0;
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| 357 | }
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| 358 | else {
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| 359 | *iran = 1;
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| 360 | }
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| 361 | }
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| 362 | else {
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| 363 | *iran = 2;
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| 364 | }
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| 365 | }
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| 366 | else {
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| 367 | *iran = 3;
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| 368 | }
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| 369 | }
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| 370 | }
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| 371 |
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| 372 | } // Poisso
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| 373 |
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| 374 |
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| 375 | G4int G4AntiNeutronAnnihilationAtRest::NFac(G4int n)
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| 376 | {
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| 377 | G4int ret_val;
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| 378 |
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| 379 | static G4int i, m;
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| 380 |
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| 381 | // *** NVE 16-MAR-1988 CERN GENEVA ***
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| 382 | // ORIGIN : H.FESEFELDT (27-OCT-1983)
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| 383 |
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| 384 | ret_val = 1;
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| 385 | m = n;
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| 386 | if (m > 1) {
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| 387 | if (m > 10) {
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| 388 | m = 10;
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| 389 | }
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| 390 | for (i = 2; i <= m; ++i) {
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| 391 | ret_val *= i;
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| 392 | }
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| 393 | }
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| 394 | return ret_val;
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| 395 |
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| 396 | } // NFac
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| 397 |
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| 398 |
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| 399 | void G4AntiNeutronAnnihilationAtRest::Normal(G4float *ran)
|
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| 400 | {
|
|---|
| 401 | static G4int i;
|
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| 402 |
|
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| 403 | // *** NVE 14-APR-1988 CERN GENEVA ***
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| 404 | // ORIGIN : H.FESEFELDT (27-OCT-1983)
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| 405 |
|
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| 406 | *ran = G4float(-6.);
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| 407 | for (i = 1; i <= 12; ++i) {
|
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| 408 | *ran += G4UniformRand();
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| 409 | }
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| 410 |
|
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| 411 | } // Normal
|
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| 412 |
|
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| 413 |
|
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| 414 | void G4AntiNeutronAnnihilationAtRest::AntiNeutronAnnihilation(G4int *nopt)
|
|---|
| 415 | {
|
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| 416 | static G4float brr[3] = { G4float(.125),G4float(.25),G4float(.5) };
|
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| 417 |
|
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| 418 | G4float r__1;
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| 419 |
|
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| 420 | static G4int i, ii, kk;
|
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| 421 | static G4int nt;
|
|---|
| 422 | static G4float cfa, eka;
|
|---|
| 423 | static G4int ika, nbl;
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|---|
| 424 | static G4float ran, pcm;
|
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| 425 | static G4int isw;
|
|---|
| 426 | static G4float tex;
|
|---|
| 427 | static G4ParticleDefinition* ipa1;
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|---|
| 428 | static G4float ran1, ran2, ekin, tkin;
|
|---|
| 429 | static G4float targ;
|
|---|
| 430 | static G4ParticleDefinition* inve;
|
|---|
| 431 | static G4float ekin1, ekin2, black;
|
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| 432 | static G4float pnrat, rmnve1, rmnve2;
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|---|
| 433 | static G4float ek, en;
|
|---|
| 434 |
|
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| 435 | // *** ANTI NEUTRON ANNIHILATION AT REST ***
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| 436 | // *** NVE 04-MAR-1988 CERN GENEVA ***
|
|---|
| 437 | // ORIGIN : H.FESEFELDT (09-JULY-1987)
|
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| 438 |
|
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| 439 | // NOPT=0 NO ANNIHILATION
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| 440 | // NOPT=1 ANNIH.IN PI+ PI-
|
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| 441 | // NOPT=2 ANNIH.IN PI0 PI0
|
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| 442 | // NOPT=3 ANNIH.IN PI+ PI0
|
|---|
| 443 | // NOPT=4 ANNIH.IN GAMMA GAMMA
|
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| 444 |
|
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| 445 | pv[1].SetZero();
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|---|
| 446 | pv[1].SetMass( massAntiNeutron );
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|---|
| 447 | pv[1].SetKineticEnergyAndUpdate( 0. );
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|---|
| 448 | pv[1].SetTOF( result.GetTOF() );
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|---|
| 449 | pv[1].SetParticleDef( result.GetParticleDef() );
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|---|
| 450 | isw = 1;
|
|---|
| 451 | ran = G4UniformRand();
|
|---|
| 452 | if (ran > brr[0]) {
|
|---|
| 453 | isw = 2;
|
|---|
| 454 | }
|
|---|
| 455 | if (ran > brr[1]) {
|
|---|
| 456 | isw = 3;
|
|---|
| 457 | }
|
|---|
| 458 | if (ran > brr[2]) {
|
|---|
| 459 | isw = 4;
|
|---|
| 460 | }
|
|---|
| 461 | *nopt = isw;
|
|---|
| 462 | // **
|
|---|
| 463 | // ** EVAPORATION
|
|---|
| 464 | // **
|
|---|
| 465 | rmnve1 = massPionPlus;
|
|---|
| 466 | rmnve2 = massPionMinus;
|
|---|
| 467 | if (isw == 2) {
|
|---|
| 468 | rmnve1 = massPionZero;
|
|---|
| 469 | }
|
|---|
| 470 | if (isw == 2) {
|
|---|
| 471 | rmnve2 = massPionZero;
|
|---|
| 472 | }
|
|---|
| 473 | if (isw == 3) {
|
|---|
| 474 | rmnve2 = massPionZero;
|
|---|
| 475 | }
|
|---|
| 476 | if (isw == 4) {
|
|---|
| 477 | rmnve1 = massGamma;
|
|---|
| 478 | }
|
|---|
| 479 | if (isw == 4) {
|
|---|
| 480 | rmnve2 = massGamma;
|
|---|
| 481 | }
|
|---|
| 482 | ek = massNeutron + massAntiNeutron - rmnve1 - rmnve2;
|
|---|
| 483 | tkin = ExNu(ek);
|
|---|
| 484 | ek -= tkin;
|
|---|
| 485 | if (ek < G4float(1e-4)) {
|
|---|
| 486 | ek = G4float(1e-4);
|
|---|
| 487 | }
|
|---|
| 488 | ek /= G4float(2.);
|
|---|
| 489 | en = ek + (rmnve1 + rmnve2) / G4float(2.);
|
|---|
| 490 | r__1 = en * en - rmnve1 * rmnve2;
|
|---|
| 491 | pcm = r__1 > 0 ? std::sqrt(r__1) : 0;
|
|---|
| 492 | pv[2].SetZero();
|
|---|
| 493 | pv[2].SetMass( rmnve1 );
|
|---|
| 494 | pv[3].SetZero();
|
|---|
| 495 | pv[3].SetMass( rmnve2 );
|
|---|
| 496 | if (isw > 3) {
|
|---|
| 497 | pv[2].SetMass( 0. );
|
|---|
| 498 | pv[3].SetMass( 0. );
|
|---|
| 499 | }
|
|---|
| 500 | pv[2].SetEnergyAndUpdate( std::sqrt(pv[2].GetMass()*pv[2].GetMass()+pcm*pcm) );
|
|---|
| 501 | pv[2].SetTOF( result.GetTOF() );
|
|---|
| 502 | pv[3].SetEnergy( std::sqrt(pv[3].GetMass()*pv[3].GetMass()+pcm*pcm) );
|
|---|
| 503 | pv[3].SetMomentumAndUpdate( -pv[2].GetMomentum().x(), -pv[2].GetMomentum().y(), -pv[2].GetMomentum().z() );
|
|---|
| 504 | pv[3].SetTOF( result.GetTOF() );
|
|---|
| 505 | switch ((int)isw) {
|
|---|
| 506 | case 1:
|
|---|
| 507 | pv[2].SetParticleDef( pdefPionPlus );
|
|---|
| 508 | pv[3].SetParticleDef( pdefPionMinus );
|
|---|
| 509 | break;
|
|---|
| 510 | case 2:
|
|---|
| 511 | pv[2].SetParticleDef( pdefPionZero );
|
|---|
| 512 | pv[3].SetParticleDef( pdefPionZero );
|
|---|
| 513 | break;
|
|---|
| 514 | case 3:
|
|---|
| 515 | pv[2].SetParticleDef( pdefPionPlus );
|
|---|
| 516 | pv[3].SetParticleDef( pdefPionZero );
|
|---|
| 517 | break;
|
|---|
| 518 | case 4:
|
|---|
| 519 | pv[2].SetParticleDef( pdefGamma );
|
|---|
| 520 | pv[3].SetParticleDef( pdefGamma );
|
|---|
| 521 | break;
|
|---|
| 522 | default:
|
|---|
| 523 | break;
|
|---|
| 524 | }
|
|---|
| 525 | nt = 3;
|
|---|
| 526 | if (targetAtomicMass >= G4float(1.5)) {
|
|---|
| 527 | cfa = (targetAtomicMass - G4float(1.)) / G4float(120.) *
|
|---|
| 528 | G4float(.025) * std::exp(-G4double(targetAtomicMass - G4float(1.)) /
|
|---|
| 529 | G4float(120.));
|
|---|
| 530 | targ = G4float(1.);
|
|---|
| 531 | tex = evapEnergy1;
|
|---|
| 532 | if (tex >= G4float(.001)) {
|
|---|
| 533 | black = (targ * G4float(1.25) +
|
|---|
| 534 | G4float(1.5)) * evapEnergy1 / (evapEnergy1 + evapEnergy3);
|
|---|
| 535 | Poisso(black, &nbl);
|
|---|
| 536 | if (G4float(G4int(targ) + nbl) > targetAtomicMass) {
|
|---|
| 537 | nbl = G4int(targetAtomicMass - targ);
|
|---|
| 538 | }
|
|---|
| 539 | if (nt + nbl > (MAX_SECONDARIES - 2)) {
|
|---|
| 540 | nbl = (MAX_SECONDARIES - 2) - nt;
|
|---|
| 541 | }
|
|---|
| 542 | if (nbl > 0) {
|
|---|
| 543 | ekin = tex / nbl;
|
|---|
| 544 | ekin2 = G4float(0.);
|
|---|
| 545 | for (i = 1; i <= nbl; ++i) {
|
|---|
| 546 | if (nt == (MAX_SECONDARIES - 2)) {
|
|---|
| 547 | continue;
|
|---|
| 548 | }
|
|---|
| 549 | if (ekin2 > tex) {
|
|---|
| 550 | break;
|
|---|
| 551 | }
|
|---|
| 552 | ran1 = G4UniformRand();
|
|---|
| 553 | Normal(&ran2);
|
|---|
| 554 | ekin1 = -G4double(ekin) * std::log(ran1) -
|
|---|
| 555 | cfa * (ran2 * G4float(.5) + G4float(1.));
|
|---|
| 556 | if (ekin1 < G4float(0.)) {
|
|---|
| 557 | ekin1 = std::log(ran1) * G4float(-.01);
|
|---|
| 558 | }
|
|---|
| 559 | ekin1 *= G4float(1.);
|
|---|
| 560 | ekin2 += ekin1;
|
|---|
| 561 | if (ekin2 > tex) {
|
|---|
| 562 | ekin1 = tex - (ekin2 - ekin1);
|
|---|
| 563 | }
|
|---|
| 564 | if (ekin1 < G4float(0.)) {
|
|---|
| 565 | ekin1 = G4float(.001);
|
|---|
| 566 | }
|
|---|
| 567 | ipa1 = pdefNeutron;
|
|---|
| 568 | pnrat = G4float(1.) - targetCharge / targetAtomicMass;
|
|---|
| 569 | if (G4UniformRand() > pnrat) {
|
|---|
| 570 | ipa1 = pdefProton;
|
|---|
| 571 | }
|
|---|
| 572 | ++nt;
|
|---|
| 573 | pv[nt].SetZero();
|
|---|
| 574 | pv[nt].SetMass( ipa1->GetPDGMass()/GeV );
|
|---|
| 575 | pv[nt].SetKineticEnergyAndUpdate( ekin1 );
|
|---|
| 576 | pv[nt].SetTOF( result.GetTOF() );
|
|---|
| 577 | pv[nt].SetParticleDef( ipa1 );
|
|---|
| 578 | }
|
|---|
| 579 | if (targetAtomicMass >= G4float(230.) && ek <= G4float(2.)) {
|
|---|
| 580 | ii = nt + 1;
|
|---|
| 581 | kk = 0;
|
|---|
| 582 | eka = ek;
|
|---|
| 583 | if (eka > G4float(1.)) {
|
|---|
| 584 | eka *= eka;
|
|---|
| 585 | }
|
|---|
| 586 | if (eka < G4float(.1)) {
|
|---|
| 587 | eka = G4float(.1);
|
|---|
| 588 | }
|
|---|
| 589 | ika = G4int(G4float(3.6) / eka);
|
|---|
| 590 | for (i = 1; i <= nt; ++i) {
|
|---|
| 591 | --ii;
|
|---|
| 592 | if (pv[ii].GetParticleDef() != pdefProton) {
|
|---|
| 593 | continue;
|
|---|
| 594 | }
|
|---|
| 595 | ipa1 = pdefNeutron;
|
|---|
| 596 | pv[ii].SetMass( ipa1->GetPDGMass()/GeV );
|
|---|
| 597 | pv[ii].SetParticleDef( ipa1 );
|
|---|
| 598 | ++kk;
|
|---|
| 599 | if (kk > ika) {
|
|---|
| 600 | break;
|
|---|
| 601 | }
|
|---|
| 602 | }
|
|---|
| 603 | }
|
|---|
| 604 | }
|
|---|
| 605 | }
|
|---|
| 606 | // **
|
|---|
| 607 | // ** THEN ALSO DEUTERONS, TRITONS AND ALPHAS
|
|---|
| 608 | // **
|
|---|
| 609 | tex = evapEnergy3;
|
|---|
| 610 | if (tex >= G4float(.001)) {
|
|---|
| 611 | black = (targ * G4float(1.25) + G4float(1.5)) * evapEnergy3 /
|
|---|
| 612 | (evapEnergy1 + evapEnergy3);
|
|---|
| 613 | Poisso(black, &nbl);
|
|---|
| 614 | if (nt + nbl > (MAX_SECONDARIES - 2)) {
|
|---|
| 615 | nbl = (MAX_SECONDARIES - 2) - nt;
|
|---|
| 616 | }
|
|---|
| 617 | if (nbl > 0) {
|
|---|
| 618 | ekin = tex / nbl;
|
|---|
| 619 | ekin2 = G4float(0.);
|
|---|
| 620 | for (i = 1; i <= nbl; ++i) {
|
|---|
| 621 | if (nt == (MAX_SECONDARIES - 2)) {
|
|---|
| 622 | continue;
|
|---|
| 623 | }
|
|---|
| 624 | if (ekin2 > tex) {
|
|---|
| 625 | break;
|
|---|
| 626 | }
|
|---|
| 627 | ran1 = G4UniformRand();
|
|---|
| 628 | Normal(&ran2);
|
|---|
| 629 | ekin1 = -G4double(ekin) * std::log(ran1) -
|
|---|
| 630 | cfa * (ran2 * G4float(.5) + G4float(1.));
|
|---|
| 631 | if (ekin1 < G4float(0.)) {
|
|---|
| 632 | ekin1 = std::log(ran1) * G4float(-.01);
|
|---|
| 633 | }
|
|---|
| 634 | ekin1 *= G4float(1.);
|
|---|
| 635 | ekin2 += ekin1;
|
|---|
| 636 | if (ekin2 > tex) {
|
|---|
| 637 | ekin1 = tex - (ekin2 - ekin1);
|
|---|
| 638 | }
|
|---|
| 639 | if (ekin1 < G4float(0.)) {
|
|---|
| 640 | ekin1 = G4float(.001);
|
|---|
| 641 | }
|
|---|
| 642 | ran = G4UniformRand();
|
|---|
| 643 | inve = pdefDeuteron;
|
|---|
| 644 | if (ran > G4float(.6)) {
|
|---|
| 645 | inve = pdefTriton;
|
|---|
| 646 | }
|
|---|
| 647 | if (ran > G4float(.9)) {
|
|---|
| 648 | inve = pdefAlpha;
|
|---|
| 649 | }
|
|---|
| 650 | ++nt;
|
|---|
| 651 | pv[nt].SetZero();
|
|---|
| 652 | pv[nt].SetMass( inve->GetPDGMass()/GeV );
|
|---|
| 653 | pv[nt].SetKineticEnergyAndUpdate( ekin1 );
|
|---|
| 654 | pv[nt].SetTOF( result.GetTOF() );
|
|---|
| 655 | pv[nt].SetParticleDef( inve );
|
|---|
| 656 | }
|
|---|
| 657 | }
|
|---|
| 658 | }
|
|---|
| 659 | }
|
|---|
| 660 | result = pv[2];
|
|---|
| 661 | if (nt == 2) {
|
|---|
| 662 | return;
|
|---|
| 663 | }
|
|---|
| 664 | for (i = 3; i <= nt; ++i) {
|
|---|
| 665 | if (ntot >= MAX_SECONDARIES) {
|
|---|
| 666 | return;
|
|---|
| 667 | }
|
|---|
| 668 | eve[ntot++] = pv[i];
|
|---|
| 669 | }
|
|---|
| 670 |
|
|---|
| 671 | } // AntiNeutronAnnihilation
|
|---|
| 672 |
|
|---|
| 673 |
|
|---|
| 674 | G4double G4AntiNeutronAnnihilationAtRest::ExNu(G4float ek1)
|
|---|
| 675 | {
|
|---|
| 676 | G4float ret_val, r__1;
|
|---|
| 677 |
|
|---|
| 678 | static G4float cfa, gfa, ran1, ran2, ekin1, atno3;
|
|---|
| 679 | static G4int magic;
|
|---|
| 680 | static G4float fpdiv;
|
|---|
| 681 |
|
|---|
| 682 | // *** NUCLEAR EVAPORATION AS FUNCTION OF ATOMIC NUMBER ATNO ***
|
|---|
| 683 | // *** AND KINETIC ENERGY EKIN OF PRIMARY PARTICLE ***
|
|---|
| 684 | // *** NVE 04-MAR-1988 CERN GENEVA ***
|
|---|
| 685 | // ORIGIN : H.FESEFELDT (10-DEC-1986)
|
|---|
| 686 |
|
|---|
| 687 | ret_val = G4float(0.);
|
|---|
| 688 | if (targetAtomicMass >= G4float(1.5)) {
|
|---|
| 689 | magic = 0;
|
|---|
| 690 | if (G4int(targetCharge + G4float(.1)) == 82) {
|
|---|
| 691 | magic = 1;
|
|---|
| 692 | }
|
|---|
| 693 | ekin1 = ek1;
|
|---|
| 694 | if (ekin1 < G4float(.1)) {
|
|---|
| 695 | ekin1 = G4float(.1);
|
|---|
| 696 | }
|
|---|
| 697 | if (ekin1 > G4float(4.)) {
|
|---|
| 698 | ekin1 = G4float(4.);
|
|---|
| 699 | }
|
|---|
| 700 | // ** 0.35 VALUE AT 1 GEV
|
|---|
| 701 | // ** 0.05 VALUE AT 0.1 GEV
|
|---|
| 702 | cfa = G4float(.13043478260869565);
|
|---|
| 703 | cfa = cfa * std::log(ekin1) + G4float(.35);
|
|---|
| 704 | if (cfa < G4float(.15)) {
|
|---|
| 705 | cfa = G4float(.15);
|
|---|
| 706 | }
|
|---|
| 707 | ret_val = cfa * G4float(7.716) * std::exp(-G4double(cfa));
|
|---|
| 708 | atno3 = targetAtomicMass;
|
|---|
| 709 | if (atno3 > G4float(120.)) {
|
|---|
| 710 | atno3 = G4float(120.);
|
|---|
| 711 | }
|
|---|
| 712 | cfa = (atno3 - G4float(1.)) /
|
|---|
| 713 | G4float(120.) * std::exp(-G4double(atno3 - G4float(1.)) / G4float(120.));
|
|---|
| 714 | ret_val *= cfa;
|
|---|
| 715 | r__1 = ekin1;
|
|---|
| 716 | fpdiv = G4float(1.) - r__1 * r__1 * G4float(.25);
|
|---|
| 717 | if (fpdiv < G4float(.5)) {
|
|---|
| 718 | fpdiv = G4float(.5);
|
|---|
| 719 | }
|
|---|
| 720 | gfa = (targetAtomicMass - G4float(1.)) /
|
|---|
| 721 | G4float(70.) * G4float(2.) *
|
|---|
| 722 | std::exp(-G4double(targetAtomicMass - G4float(1.)) / G4float(70.));
|
|---|
| 723 | evapEnergy1 = ret_val * fpdiv;
|
|---|
| 724 | evapEnergy3 = ret_val - evapEnergy1;
|
|---|
| 725 | Normal(&ran1);
|
|---|
| 726 | Normal(&ran2);
|
|---|
| 727 | if (magic == 1) {
|
|---|
| 728 | ran1 = G4float(0.);
|
|---|
| 729 | ran2 = G4float(0.);
|
|---|
| 730 | }
|
|---|
| 731 | evapEnergy1 *= ran1 * gfa + G4float(1.);
|
|---|
| 732 | if (evapEnergy1 < G4float(0.)) {
|
|---|
| 733 | evapEnergy1 = G4float(0.);
|
|---|
| 734 | }
|
|---|
| 735 | evapEnergy3 *= ran2 * gfa + G4float(1.);
|
|---|
| 736 | if (evapEnergy3 < G4float(0.)) {
|
|---|
| 737 | evapEnergy3 = G4float(0.);
|
|---|
| 738 | }
|
|---|
| 739 | while ((ret_val = evapEnergy1 + evapEnergy3) >= ek1) {
|
|---|
| 740 | evapEnergy1 *= G4float(1.) - G4UniformRand() * G4float(.5);
|
|---|
| 741 | evapEnergy3 *= G4float(1.) - G4UniformRand() * G4float(.5);
|
|---|
| 742 | }
|
|---|
| 743 | }
|
|---|
| 744 | return ret_val;
|
|---|
| 745 |
|
|---|
| 746 | } // ExNu
|
|---|