| 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| 26 | //
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| 27 | //080721 Create adjust_final_state method by T. Koi
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| 28 | //080801 Residual reconstruction with theNDLDataA,Z (A, Z, and momentum are adjusted) by T. Koi
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| 29 | //101110 Set lower limit for gamma energy(1keV) by T. Koi
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| 30 |
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| 31 | #include "G4NeutronHPFinalState.hh"
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| 32 |
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| 33 | #include "G4ParticleTable.hh"
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| 34 | #include "G4Gamma.hh"
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| 35 |
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| 36 |
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| 37 |
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| 38 | void G4NeutronHPFinalState::adjust_final_state ( G4LorentzVector init_4p_lab )
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| 39 | {
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| 40 |
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| 41 | G4double minimum_energy = 1*keV;
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| 42 |
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| 43 | if ( adjustResult != true ) return;
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| 44 |
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| 45 | G4int nSecondaries = theResult.GetNumberOfSecondaries();
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| 46 |
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| 47 | G4int sum_Z = 0;
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| 48 | G4int sum_A = 0;
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| 49 | G4int max_SecZ = 0;
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| 50 | G4int max_SecA = 0;
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| 51 | for ( int i = 0 ; i < nSecondaries ; i++ )
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| 52 | {
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| 53 | sum_Z += theResult.GetSecondary( i )->GetParticle()->GetDefinition()->GetAtomicNumber();
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| 54 | max_SecZ = std::max ( max_SecZ , theResult.GetSecondary( i )->GetParticle()->GetDefinition()->GetAtomicNumber() );
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| 55 | sum_A += theResult.GetSecondary( i )->GetParticle()->GetDefinition()->GetAtomicMass();
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| 56 | max_SecA = std::max ( max_SecA , theResult.GetSecondary( i )->GetParticle()->GetDefinition()->GetAtomicMass() );
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| 57 | }
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| 58 |
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| 59 | G4ParticleDefinition* resi_pd = NULL;
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| 60 | if ( (int)(theBaseZ - sum_Z) == 0 && (int)(theBaseA + 1 - sum_A) == 0 )
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| 61 | resi_pd = G4ParticleTable::GetParticleTable()->GetIon ( max_SecZ , max_SecA , 0.0 );
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| 62 | else
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| 63 | {
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| 64 | resi_pd = G4ParticleTable::GetParticleTable()->GetIon ( int(theBaseZ - sum_Z) , (int)(theBaseA + 1 - sum_A) , 0.0 );
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| 65 | if ( resi_pd == NULL )
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| 66 | {
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| 67 | // theNDLDataZ,A has the Z and A of used NDL file
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| 68 | if ( (int)(theNDLDataZ - sum_Z) == 0 && (int)(theNDLDataA + 1 - sum_A) == 0 )
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| 69 | {
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| 70 | G4int dif_Z = ( int ) ( theNDLDataZ - theBaseZ );
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| 71 | G4int dif_A = ( int ) ( theNDLDataA - theBaseA );
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| 72 | resi_pd = G4ParticleTable::GetParticleTable()->GetIon ( max_SecZ - dif_Z , max_SecA - dif_A , 0.0 );
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| 73 | for ( int i = 0 ; i < nSecondaries ; i++ )
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| 74 | {
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| 75 | if ( theResult.GetSecondary( i )->GetParticle()->GetDefinition()->GetAtomicNumber() == max_SecZ
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| 76 | && theResult.GetSecondary( i )->GetParticle()->GetDefinition()->GetAtomicMass() == max_SecA )
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| 77 | {
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| 78 | G4ThreeVector p = theResult.GetSecondary( i )->GetParticle()->GetMomentum();
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| 79 | p = p * resi_pd->GetPDGMass()/ G4ParticleTable::GetParticleTable()->GetIon ( max_SecZ , max_SecA , 0.0 )->GetPDGMass();
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| 80 | theResult.GetSecondary( i )->GetParticle()->SetDefinition( resi_pd );
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| 81 | theResult.GetSecondary( i )->GetParticle()->SetMomentum( p );
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| 82 | }
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| 83 | }
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| 84 | }
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| 85 | }
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| 86 | }
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| 87 |
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| 88 |
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| 89 | G4LorentzVector secs_4p_lab( 0.0 );
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| 90 |
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| 91 | G4int n_sec = theResult.GetNumberOfSecondaries();
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| 92 | G4double fast = 0;
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| 93 | G4double slow = 1;
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| 94 | G4int ifast = 0;
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| 95 | G4int islow = 0;
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| 96 | G4int ires = -1;
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| 97 |
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| 98 | for ( G4int i = 0 ; i < n_sec ; i++ )
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| 99 | {
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| 100 |
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| 101 | //G4cout << "HP_DB " << i
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| 102 | // << " " << theResult.GetSecondary( i )->GetParticle()->GetDefinition()->GetParticleName()
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| 103 | // << " 4p " << theResult.GetSecondary( i )->GetParticle()->Get4Momentum()
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| 104 | // << " ke " << theResult.GetSecondary( i )->GetParticle()->Get4Momentum().e() - theResult.GetSecondary( i )->GetParticle()->GetDefinition()->GetPDGMass()
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| 105 | // << G4endl;
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| 106 |
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| 107 | secs_4p_lab += theResult.GetSecondary( i )->GetParticle()->Get4Momentum();
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| 108 |
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| 109 | G4double beta = 0;
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| 110 | if ( theResult.GetSecondary( i )->GetParticle()->GetDefinition() != G4Gamma::Gamma() )
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| 111 | {
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| 112 | beta = theResult.GetSecondary( i )->GetParticle()->Get4Momentum().beta();
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| 113 | }
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| 114 | else
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| 115 | {
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| 116 | beta = 1;
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| 117 | }
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| 118 |
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| 119 | if ( theResult.GetSecondary( i )->GetParticle()->GetDefinition() == resi_pd ) ires = i;
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| 120 |
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| 121 | if ( slow > beta && beta != 0 )
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| 122 | {
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| 123 | slow = beta;
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| 124 | islow = i;
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| 125 | }
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| 126 |
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| 127 | if ( fast <= beta )
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| 128 | {
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| 129 | if ( fast != 1 )
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| 130 | {
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| 131 | fast = beta;
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| 132 | ifast = i;
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| 133 | }
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| 134 | else
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| 135 | {
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| 136 | // fast is already photon then check E
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| 137 | G4double e = theResult.GetSecondary( i )->GetParticle()->Get4Momentum().e();
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| 138 | if ( e > theResult.GetSecondary( ifast )->GetParticle()->Get4Momentum().e() )
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| 139 | {
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| 140 | // among photons, the highest E becomes the fastest
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| 141 | ifast = i;
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| 142 | }
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| 143 | }
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| 144 | }
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| 145 | }
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| 146 |
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| 147 |
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| 148 | G4LorentzVector dif_4p = init_4p_lab - secs_4p_lab;
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| 149 |
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| 150 | //G4cout << "HP_DB dif_4p " << init_4p_lab - secs_4p_lab << G4endl;
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| 151 | //G4cout << "HP_DB dif_3p mag " << ( dif_4p.v() ).mag() << G4endl;
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| 152 | //G4cout << "HP_DB dif_e " << dif_4p.e() - ( dif_4p.v() ).mag()<< G4endl;
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| 153 |
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| 154 | G4LorentzVector p4(0);
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| 155 | if ( ires == -1 )
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| 156 | {
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| 157 | // Create and Add Residual Nucleus
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| 158 | ires = nSecondaries;
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| 159 | nSecondaries += 1;
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| 160 |
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| 161 | G4DynamicParticle* res = new G4DynamicParticle ( resi_pd , dif_4p.v() );
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| 162 | theResult.AddSecondary ( res );
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| 163 |
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| 164 | p4 = res->Get4Momentum();
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| 165 | if ( slow > p4.beta() )
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| 166 | {
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| 167 | slow = p4.beta();
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| 168 | islow = ires;
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| 169 | }
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| 170 |
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| 171 | dif_4p = init_4p_lab - ( secs_4p_lab + p4 );
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| 172 | }
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| 173 |
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| 174 | //Which is bigger dif_p or dif_e
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| 175 |
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| 176 | if ( dif_4p.v().mag() < std::abs( dif_4p.e() ) )
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| 177 | {
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| 178 |
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| 179 | // Adjust p
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| 180 | //if ( dif_4p.v().mag() < 1*MeV )
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| 181 | if ( minimum_energy < dif_4p.v().mag() && dif_4p.v().mag() < 1*MeV )
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| 182 | {
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| 183 |
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| 184 | nSecondaries += 1;
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| 185 | theResult.AddSecondary ( new G4DynamicParticle ( G4Gamma::Gamma() , dif_4p.v() ) );
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| 186 |
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| 187 | }
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| 188 | else
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| 189 | {
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| 190 | //G4cout << "HP_DB Difference in dif_p is too large (>1MeV) or too small(<1keV) to adjust, so that give up tuning" << G4endl;
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| 191 | }
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| 192 |
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| 193 | }
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| 194 | else
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| 195 | {
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| 196 |
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| 197 | // dif_p > dif_e
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| 198 | // at first momentum
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| 199 | // Move residual momentum
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| 200 |
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| 201 | p4 = theResult.GetSecondary( ires )->GetParticle()->Get4Momentum();
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| 202 | theResult.GetSecondary( ires )->GetParticle()->SetMomentum( p4.v() + dif_4p.v() );
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| 203 | dif_4p = init_4p_lab - ( secs_4p_lab - p4 + theResult.GetSecondary( ires )->GetParticle()->Get4Momentum() );
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| 204 |
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| 205 | //G4cout << "HP_DB new residual kinetic energy " << theResult.GetSecondary( ires )->GetParticle()->GetKineticEnergy() << G4endl;
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| 206 |
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| 207 | }
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| 208 |
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| 209 | G4double dif_e = dif_4p.e() - ( dif_4p.v() ).mag();
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| 210 | //G4cout << "HP_DB dif_e " << dif_e << G4endl;
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| 211 |
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| 212 | if ( dif_e > 0 )
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| 213 | {
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| 214 |
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| 215 | // create 2 gamma
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| 216 |
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| 217 | nSecondaries += 2;
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| 218 | G4double e1 = ( dif_4p.e() -dif_4p.v().mag() ) / 2;
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| 219 |
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| 220 | if ( minimum_energy < e1 )
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| 221 | {
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| 222 | G4double costh = 2.*G4UniformRand()-1.;
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| 223 | G4double phi = twopi*G4UniformRand();
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| 224 | G4ThreeVector dir( std::sin(std::acos(costh))*std::cos(phi),
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| 225 | std::sin(std::acos(costh))*std::sin(phi),
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| 226 | costh);
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| 227 | theResult.AddSecondary ( new G4DynamicParticle ( G4Gamma::Gamma() , e1*dir ) );
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| 228 | theResult.AddSecondary ( new G4DynamicParticle ( G4Gamma::Gamma() , -e1*dir ) );
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| 229 | }
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| 230 | else
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| 231 | {
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| 232 | //G4cout << "HP_DB Difference is too small(<1keV) to adjust, so that neglect it" << G4endl;
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| 233 | }
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| 234 |
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| 235 | }
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| 236 | else //dif_e < 0
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| 237 | {
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| 238 |
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| 239 | // At first reduce KE of the fastest secondary;
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| 240 | G4double ke0 = theResult.GetSecondary( ifast )->GetParticle()->GetKineticEnergy();
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| 241 | G4ThreeVector p0 = theResult.GetSecondary( ifast )->GetParticle()->GetMomentum();
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| 242 | G4ThreeVector dir = ( theResult.GetSecondary( ifast )->GetParticle()->GetMomentum() ).unit();
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| 243 |
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| 244 | //G4cout << "HP_DB ifast " << ifast << " ke0 " << ke0 << G4endl;
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| 245 |
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| 246 | if ( ke0 + dif_e > 0 )
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| 247 | {
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| 248 | theResult.GetSecondary( ifast )->GetParticle()->SetKineticEnergy( ke0 + dif_e );
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| 249 | G4ThreeVector dp = p0 - theResult.GetSecondary( ifast )->GetParticle()->GetMomentum();
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| 250 |
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| 251 | G4ThreeVector p = theResult.GetSecondary( islow )->GetParticle()->GetMomentum();
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| 252 | //theResult.GetSecondary( islow )->GetParticle()->SetMomentum( p - dif_e*dir );
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| 253 | theResult.GetSecondary( islow )->GetParticle()->SetMomentum( p + dp );
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| 254 | }
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| 255 | else
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| 256 | {
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| 257 | //G4cout << "HP_DB Difference in dif_e too large ( <0MeV ) to adjust, so that give up tuning" << G4endl;
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| 258 | }
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| 259 |
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| 260 | }
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| 261 |
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| 262 | }
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