| 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| 26 | //
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| 27 | // $Id: G4ElasticHadrNucleusHE.cc,v 1.81 2009/09/22 16:21:46 vnivanch Exp $
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| 28 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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| 29 | //
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| 30 | //
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| 31 | // The generator of high energy hadron-nucleus elastic scattering
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| 32 | // The hadron kinetic energy T > 1 GeV
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| 33 | // N. Starkov 2003.
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| 34 | //
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| 35 | // 19.05.04 Variant for G4 6.1: The 'ApplyYourself' was changed
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| 36 | // 19.11.05 The HE elastic scattering on proton is added (N.Starkov)
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| 37 | // 16.11.06 The low energy boundary is shifted to T = 400 MeV (N.Starkov)
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| 38 | // 23.11.06 General cleanup, ONQ0=3, use pointer instead of particle name (VI)
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| 39 | // 02.05.07 Scale sampled t as p^2 (VI)
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| 40 | // 15.05.07 Redesign and cleanup (V.Ivanchenko)
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| 41 | // 17.05.07 cleanup (V.Grichine)
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| 42 | //
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| 43 |
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| 44 | #include "G4ElasticHadrNucleusHE.hh"
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| 45 | #include "Randomize.hh"
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| 46 | #include "G4ios.hh"
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| 47 | #include "G4ParticleTable.hh"
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| 48 | #include "G4IonTable.hh"
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| 49 | #include "G4Proton.hh"
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| 50 | #include "G4NistManager.hh"
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| 51 |
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| 52 | using namespace std;
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| 53 |
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| 54 | ///////////////////////////////////////////////////////////////
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| 55 | //
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| 56 | //
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| 57 |
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| 58 | G4ElasticData::G4ElasticData(const G4ParticleDefinition* p,
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| 59 | G4int Z, G4double AWeight, G4double* eGeV)
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| 60 | {
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| 61 | hadr = p;
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| 62 | massGeV = p->GetPDGMass()/GeV;
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| 63 | mass2GeV2= massGeV*massGeV;
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| 64 | AtomicWeight = G4int(AWeight + 0.5);
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| 65 |
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| 66 | DefineNucleusParameters(AWeight);
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| 67 |
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| 68 | limitQ2 = 35./(R1*R1); // (GeV/c)^2
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| 69 |
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| 70 | G4double dQ2 = limitQ2/(ONQ2 - 1.);
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| 71 |
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| 72 | TableQ2[0] = 0.0;
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| 73 |
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| 74 | for(G4int ii = 1; ii < ONQ2; ii++)
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| 75 | {
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| 76 | TableQ2[ii] = TableQ2[ii-1]+dQ2;
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| 77 | }
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| 78 |
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| 79 | massA = AWeight*amu_c2/GeV;
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| 80 | massA2 = massA*massA;
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| 81 |
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| 82 | for(G4int kk = 0; kk < NENERGY; kk++)
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| 83 | {
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| 84 | dnkE[kk] = 0;
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| 85 | G4double elab = eGeV[kk] + massGeV;
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| 86 | G4double plab2= eGeV[kk]*(eGeV[kk] + 2.0*massGeV);
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| 87 | G4double Q2m = 4.0*plab2*massA2/(mass2GeV2 + massA2 + 2.*massA2*elab);
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| 88 |
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| 89 | if(Z == 1 && p == G4Proton::Proton()) Q2m *= 0.5;
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| 90 |
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| 91 | maxQ2[kk] = std::min(limitQ2, Q2m);
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| 92 | TableCrossSec[ONQ2*kk] = 0.0;
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| 93 |
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| 94 | // G4cout<<" kk eGeV[kk] "<<kk<<" "<<eGeV[kk]<<G4endl;
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| 95 | }
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| 96 | }
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| 97 |
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| 98 | /////////////////////////////////////////////////////////////////////////
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| 99 | //
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| 100 | //
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| 101 |
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| 102 | void G4ElasticData::DefineNucleusParameters(G4double A)
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| 103 | {
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| 104 | switch (AtomicWeight)
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| 105 | {
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| 106 | case 207:
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| 107 | case 208:
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| 108 | R1 = 20.5;
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| 109 | // R1 = 17.5;
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| 110 | // R1 = 21.3;
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| 111 | R2 = 15.74;
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| 112 | // R2 = 10.74;
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| 113 |
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| 114 | Pnucl = 0.4;
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| 115 | Aeff = 0.7;
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| 116 | break;
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| 117 | case 237:
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| 118 | case 238:
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| 119 | R1 = 21.7;
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| 120 | R2 = 16.5;
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| 121 | Pnucl = 0.4;
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| 122 | Aeff = 0.7;
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| 123 | break;
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| 124 | case 90:
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| 125 | case 91:
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| 126 | R1 = 16.5*1.0;
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| 127 | R2 = 11.62;
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| 128 | Pnucl = 0.4;
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| 129 | Aeff = 0.7;
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| 130 | break;
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| 131 | case 58:
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| 132 | case 59:
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| 133 | R1 = 15.0*1.05;
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| 134 | R2 = 9.9;
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| 135 | Pnucl = 0.45;
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| 136 | Aeff = 0.85;
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| 137 | break;
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| 138 | case 48:
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| 139 | case 47:
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| 140 | R1 = 14.0;
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| 141 | R2 = 9.26;
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| 142 | Pnucl = 0.31;
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| 143 | Aeff = 0.75;
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| 144 | break;
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| 145 | case 40:
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| 146 | case 41:
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| 147 | R1 = 13.3;
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| 148 | R2 = 9.26;
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| 149 | Pnucl = 0.31;
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| 150 | Aeff = 0.75;
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| 151 | break;
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| 152 | case 28:
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| 153 | case 29:
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| 154 | R1 = 12.0;
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| 155 | R2 = 7.64;
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| 156 | Pnucl = 0.253;
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| 157 | Aeff = 0.8;
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| 158 | break;
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| 159 | case 16:
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| 160 | R1 = 10.50;
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| 161 | R2 = 5.5;
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| 162 | Pnucl = 0.7;
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| 163 | Aeff = 0.98;
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| 164 | break;
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| 165 | case 12:
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| 166 | R1 = 9.3936;
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| 167 | R2 = 4.63;
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| 168 | Pnucl = 0.7;
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| 169 | // Pnucl = 0.5397;
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| 170 | Aeff = 1.0;
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| 171 | break;
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| 172 | case 11:
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| 173 | R1 = 9.0;
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| 174 | R2 = 5.42;
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| 175 | Pnucl = 0.19;
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| 176 | // Pnucl = 0.5397;
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| 177 | Aeff = 0.9;
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| 178 | break;
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| 179 | case 9:
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| 180 | R1 = 9.9;
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| 181 | R2 = 6.5;
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| 182 | Pnucl = 0.690;
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| 183 | Aeff = 0.95;
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| 184 | break;
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| 185 | case 4:
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| 186 | R1 = 5.3;
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| 187 | R2 = 3.7;
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| 188 | Pnucl = 0.4;
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| 189 | Aeff = 0.75;
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| 190 | break;
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| 191 | case 1:
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| 192 | R1 = 4.5;
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| 193 | R2 = 2.3;
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| 194 | Pnucl = 0.177;
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| 195 | Aeff = 0.9;
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| 196 | break;
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| 197 | default:
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| 198 | R1 = 4.45*std::pow(A - 1.,0.309)*0.9;
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| 199 | R2 = 2.3 *std::pow(A, 0.36);
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| 200 |
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| 201 | if(A < 100 && A > 3) Pnucl = 0.176 + 0.00275*A;
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| 202 | else Pnucl = 0.4;
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| 203 |
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| 204 | //G4cout<<" Deault: A= "<<A<<" R1 R2 Aeff Pnucl "<<R1<<" "<<R2<<" "
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| 205 | // <<Aeff<<" "<<Pnucl<<G4endl;
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| 206 |
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| 207 | if(A >= 100) Aeff = 0.7;
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| 208 | else if(A < 100 && A > 75) Aeff = 1.5 - 0.008*A;
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| 209 | else Aeff = 0.9;
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| 210 | break;
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| 211 | }
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| 212 | //G4cout<<" Result: A= "<<A<<" R1 R2 Aeff Pnucl "<<R1<<" "<<R2<<" "
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| 213 | // <<Aeff<<" "<<Pnucl<<G4endl;
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| 214 | }
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| 215 |
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| 216 | ////////////////////////////////////////////////////////////////////
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| 217 | //
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| 218 | // The constructor for the generating of events
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| 219 | //
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| 220 |
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| 221 | G4ElasticHadrNucleusHE::G4ElasticHadrNucleusHE()
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| 222 | : G4VHadronElastic("hElasticGlauber")
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| 223 | // :G4HadronicInteraction("G4ElasticHadrNucleusHE")
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| 224 | {
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| 225 | verboseLevel = 0;
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| 226 | plabLowLimit = 20.0*MeV;
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| 227 | lowestEnergyLimit = 0.0;
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| 228 |
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| 229 | MbToGeV2 = 2.568;
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| 230 | sqMbToGeV = 1.602;
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| 231 | Fm2ToGeV2 = 25.68;
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| 232 | GeV2 = GeV*GeV;
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| 233 | protonM = proton_mass_c2/GeV;
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| 234 | protonM2 = protonM*protonM;
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| 235 |
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| 236 | BoundaryP[0]=9.0;BoundaryTG[0]=5.0;BoundaryTL[0]=0.;
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| 237 | BoundaryP[1]=20.0;BoundaryTG[1]=1.5;BoundaryTL[1]=0.;
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| 238 | BoundaryP[2]=5.0; BoundaryTG[2]=1.0;BoundaryTL[2]=1.5;
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| 239 | BoundaryP[3]=8.0; BoundaryTG[3]=3.0;BoundaryTL[3]=0.;
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| 240 | BoundaryP[4]=7.0; BoundaryTG[4]=3.0;BoundaryTL[4]=0.;
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| 241 | BoundaryP[5]=5.0; BoundaryTG[5]=2.0;BoundaryTL[5]=0.;
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| 242 | BoundaryP[6]=5.0; BoundaryTG[6]=1.5;BoundaryTL[6]=3.0;
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| 243 |
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| 244 | Binom();
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| 245 | // energy in GeV
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| 246 | Energy[0] = 0.4;
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| 247 | Energy[1] = 0.6;
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| 248 | Energy[2] = 0.8;
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| 249 | LowEdgeEnergy[0] = 0.0;
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| 250 | LowEdgeEnergy[1] = 0.5;
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| 251 | LowEdgeEnergy[2] = 0.7;
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| 252 | G4double e = 1.0;
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| 253 | G4double f = std::pow(10.,0.1);
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| 254 | for(G4int i=3; i<NENERGY; i++) {
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| 255 | Energy[i] = e;
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| 256 | LowEdgeEnergy[i] = e/f;
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| 257 | e *= f*f;
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| 258 | }
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| 259 | nistManager = G4NistManager::Instance();
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| 260 |
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| 261 | // PDG code for hadrons
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| 262 | G4int ic[NHADRONS] = {211,-211,2112,2212,321,-321,130,310,311,-311,
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| 263 | 3122,3222,3112,3212,3312,3322,3334,
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| 264 | -2212,-2112,-3122,-3222,-3112,-3212,-3312,-3322,-3334};
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| 265 | // internal index
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| 266 | G4int id[NHADRONS] = {2,3,6,0,4,5,4,4,4,5,
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| 267 | 0,0,0,0,0,0,0,
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| 268 | 1,7,1,1,1,1,1,1,1};
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| 269 |
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| 270 | G4int id1[NHADRONS] = {3,4,1,0,5,6,5,5,5,6,
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| 271 | 0,0,0,0,0,0,0,
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| 272 | 2,2,2,2,2,2,2,2,2};
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| 273 |
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| 274 | for(G4int j=0; j<NHADRONS; j++)
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| 275 | {
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| 276 | HadronCode[j] = ic[j];
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| 277 | HadronType[j] = id[j];
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| 278 | HadronType1[j] = id1[j];
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| 279 |
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| 280 | for(G4int k = 0; k < 93; k++) SetOfElasticData[j][k] = 0;
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| 281 | }
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| 282 | }
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| 283 |
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| 284 | ///////////////////////////////////////////////////////////////////
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| 285 | //
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| 286 | //
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| 287 |
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| 288 | G4ElasticHadrNucleusHE::~G4ElasticHadrNucleusHE()
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| 289 | {
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| 290 | for(G4int j = 0; j < NHADRONS; j++)
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| 291 | {
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| 292 | for(G4int k = 0; k < 93; k++)
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| 293 | {
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| 294 | if(SetOfElasticData[j][k]) delete SetOfElasticData[j][k];
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| 295 | }
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| 296 | }
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| 297 | }
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| 298 |
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| 299 | ////////////////////////////////////////////////////////////////////
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| 300 | //
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| 301 | //
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| 302 | /*
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| 303 | G4HadFinalState * G4ElasticHadrNucleusHE::ApplyYourself(
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| 304 | const G4HadProjectile &aTrack,
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| 305 | G4Nucleus &targetNucleus)
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| 306 | {
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| 307 | theParticleChange.Clear();
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| 308 |
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| 309 | const G4HadProjectile* aParticle = &aTrack;
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| 310 | G4double ekin = aParticle->GetKineticEnergy();
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| 311 |
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| 312 | if( ekin <= lowestEnergyLimit )
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| 313 | {
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| 314 | theParticleChange.SetEnergyChange(ekin);
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| 315 | theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
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| 316 | return &theParticleChange;
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| 317 | }
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| 318 |
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| 319 | G4double aTarget = targetNucleus.GetN();
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| 320 | G4double zTarget = targetNucleus.GetZ();
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| 321 |
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| 322 | G4double plab = aParticle->GetTotalMomentum();
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| 323 |
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| 324 | if (verboseLevel >1)
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| 325 | {
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| 326 | G4cout << "G4ElasticHadrNucleusHE: Incident particle plab="
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| 327 | << plab/GeV << " GeV/c "
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| 328 | << " ekin(MeV) = " << ekin/MeV << " "
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| 329 | << aParticle->GetDefinition()->GetParticleName() << G4endl;
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| 330 | }
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| 331 | // Scattered particle referred to axis of incident particle
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| 332 |
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| 333 | const G4ParticleDefinition* theParticle = aParticle->GetDefinition();
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| 334 | G4double m1 = theParticle->GetPDGMass();
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| 335 |
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| 336 | G4int Z = static_cast<G4int>(zTarget+0.5);
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| 337 | G4int A = static_cast<G4int>(aTarget+0.5);
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| 338 | G4int projPDG = theParticle->GetPDGEncoding();
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| 339 |
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| 340 | if (verboseLevel>1)
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| 341 | {
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| 342 | G4cout << "G4ElasticHadrNucleusHE for " << theParticle->GetParticleName()
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| 343 | << " PDGcode= " << projPDG << " on nucleus Z= " << Z
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| 344 | << " A= " << A
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| 345 | << G4endl;
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| 346 | }
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| 347 | G4ParticleDefinition * theDef = 0;
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| 348 |
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| 349 | if (Z == 1 && A == 1) theDef = G4Proton::Proton();
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| 350 | else if (Z == 1 && A == 2) theDef = G4Deuteron::Deuteron();
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| 351 | else if (Z == 1 && A == 3) theDef = G4Triton::Triton();
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| 352 | else if (Z == 2 && A == 3) theDef = G4He3::He3();
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| 353 | else if (Z == 2 && A == 4) theDef = G4Alpha::Alpha();
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| 354 | else theDef = G4ParticleTable::
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| 355 | GetParticleTable()->FindIon(Z,A,0,Z);
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| 356 |
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| 357 | G4double m2 = theDef->GetPDGMass();
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| 358 | G4LorentzVector lv1 = aParticle->Get4Momentum();
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| 359 | G4LorentzVector lv(0.0,0.0,0.0,m2);
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| 360 | lv += lv1;
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| 361 |
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| 362 | G4ThreeVector bst = lv.boostVector();
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| 363 | lv1.boost(-bst);
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| 364 |
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| 365 | G4ThreeVector p1 = lv1.vect();
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| 366 | G4double ptot = p1.mag();
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| 367 | G4double tmax = 4.0*ptot*ptot;
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| 368 | G4double t = 0.0;
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| 369 |
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| 370 | // Choose generator
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| 371 | G4bool swave = false;
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| 372 |
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| 373 | // S-wave for very low energy
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| 374 | if(plab < plabLowLimit) swave = true;
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| 375 |
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| 376 | // normal sampling
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| 377 | if(!swave) {
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| 378 | t = SampleT(theParticle,plab,Z,A);
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| 379 | if(t > tmax) swave = true;
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| 380 | }
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| 381 |
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| 382 | if(swave) t = G4UniformRand()*tmax;
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| 383 |
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| 384 | // Sampling in CM system
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| 385 | G4double phi = G4UniformRand()*twopi;
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| 386 | G4double cost = 1. - 2.0*t/tmax;
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| 387 | G4double sint;
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| 388 |
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| 389 | if( cost >= 1.0 )
|
|---|
| 390 | {
|
|---|
| 391 | cost = 1.0;
|
|---|
| 392 | sint = 0.0;
|
|---|
| 393 | }
|
|---|
| 394 | else if( cost <= -1.0)
|
|---|
| 395 | {
|
|---|
| 396 | cost = -1.0;
|
|---|
| 397 | sint = 0.0;
|
|---|
| 398 | }
|
|---|
| 399 | else
|
|---|
| 400 | {
|
|---|
| 401 | sint = std::sqrt((1.0-cost)*(1.0+cost));
|
|---|
| 402 | }
|
|---|
| 403 | if (verboseLevel>1)
|
|---|
| 404 | G4cout << "cos(t)=" << cost << " std::sin(t)=" << sint << G4endl;
|
|---|
| 405 |
|
|---|
| 406 | G4ThreeVector v1(sint*std::cos(phi),sint*std::sin(phi),cost);
|
|---|
| 407 | v1 *= ptot;
|
|---|
| 408 | G4LorentzVector nlv1( v1.x(), v1.y(), v1.z(), std::sqrt(ptot*ptot + m1*m1));
|
|---|
| 409 |
|
|---|
| 410 | nlv1.boost(bst);
|
|---|
| 411 |
|
|---|
| 412 | G4double eFinal = nlv1.e() - m1;
|
|---|
| 413 |
|
|---|
| 414 | if (verboseLevel > 1)
|
|---|
| 415 | {
|
|---|
| 416 | G4cout << "Scattered: "
|
|---|
| 417 | << nlv1<<" m= " << m1 << " ekin(MeV)= " << eFinal
|
|---|
| 418 | << " Proj: 4-mom " << lv1
|
|---|
| 419 | <<G4endl;
|
|---|
| 420 | }
|
|---|
| 421 | if( eFinal < 0.0 )
|
|---|
| 422 | {
|
|---|
| 423 | G4cout << "G4ElasticHadrNucleusHE WARNING ekin= " << eFinal
|
|---|
| 424 | << " after scattering of "
|
|---|
| 425 | << aParticle->GetDefinition()->GetParticleName()
|
|---|
| 426 | << " p(GeV/c)= " << plab
|
|---|
| 427 | << " on " << theDef->GetParticleName()
|
|---|
| 428 | << G4endl;
|
|---|
| 429 | eFinal = 0.0;
|
|---|
| 430 | nlv1.setE(m1);
|
|---|
| 431 | }
|
|---|
| 432 |
|
|---|
| 433 | theParticleChange.SetMomentumChange( nlv1.vect().unit() );
|
|---|
| 434 | theParticleChange.SetEnergyChange(eFinal);
|
|---|
| 435 |
|
|---|
| 436 | G4LorentzVector nlv0 = lv - nlv1;
|
|---|
| 437 | G4double erec = nlv0.e() - m2;
|
|---|
| 438 |
|
|---|
| 439 | if (verboseLevel > 1)
|
|---|
| 440 | {
|
|---|
| 441 | G4cout << "Recoil: "
|
|---|
| 442 | << nlv0<<" m= " << m2 << " ekin(MeV)= " << erec
|
|---|
| 443 | <<G4endl;
|
|---|
| 444 | }
|
|---|
| 445 | if(erec < 0.0)
|
|---|
| 446 | {
|
|---|
| 447 | G4cout << "G4ElasticHadrNucleusHE WARNING Erecoil(MeV)= " << erec
|
|---|
| 448 | << " after scattering of "
|
|---|
| 449 | << aParticle->GetDefinition()->GetParticleName()
|
|---|
| 450 | << " p(GeV/c)= " << plab
|
|---|
| 451 | << " on " << theDef->GetParticleName()
|
|---|
| 452 | << G4endl;
|
|---|
| 453 | nlv0.setE(m2);
|
|---|
| 454 | }
|
|---|
| 455 | G4DynamicParticle * aSec = new G4DynamicParticle(theDef, nlv0);
|
|---|
| 456 | theParticleChange.AddSecondary(aSec);
|
|---|
| 457 |
|
|---|
| 458 | return &theParticleChange;
|
|---|
| 459 | }
|
|---|
| 460 | */
|
|---|
| 461 | //////////////////////////////////////////////////////////////////////////
|
|---|
| 462 | //
|
|---|
| 463 | //
|
|---|
| 464 |
|
|---|
| 465 | G4double
|
|---|
| 466 | G4ElasticHadrNucleusHE::SampleInvariantT(const G4ParticleDefinition* p,
|
|---|
| 467 | G4double inLabMom,
|
|---|
| 468 | G4int Z, G4int N)
|
|---|
| 469 | {
|
|---|
| 470 | G4double plab = inLabMom/GeV; // (GeV/c)
|
|---|
| 471 | G4double Q2 = 0;
|
|---|
| 472 |
|
|---|
| 473 | iHadrCode = p->GetPDGEncoding();
|
|---|
| 474 |
|
|---|
| 475 | NumbN = N;
|
|---|
| 476 |
|
|---|
| 477 | if(verboseLevel > 1)
|
|---|
| 478 | {
|
|---|
| 479 | G4cout<< " G4ElasticHadrNucleusHE::SampleT: "
|
|---|
| 480 | << " for " << p->GetParticleName()
|
|---|
| 481 | << " at Z= " << Z << " A= " << N
|
|---|
| 482 | << " plab(GeV)= " << plab
|
|---|
| 483 | << G4endl;
|
|---|
| 484 | }
|
|---|
| 485 | G4int idx;
|
|---|
| 486 |
|
|---|
| 487 | for( idx = 0 ; idx < NHADRONS; idx++)
|
|---|
| 488 | {
|
|---|
| 489 | if(iHadrCode == HadronCode[idx]) break;
|
|---|
| 490 | }
|
|---|
| 491 |
|
|---|
| 492 | // Hadron is not in the list
|
|---|
| 493 |
|
|---|
| 494 | if( idx >= NHADRONS ) return Q2;
|
|---|
| 495 |
|
|---|
| 496 | iHadron = HadronType[idx];
|
|---|
| 497 | iHadrCode = HadronCode[idx];
|
|---|
| 498 |
|
|---|
| 499 | if(Z==1)
|
|---|
| 500 | {
|
|---|
| 501 | hMass = p->GetPDGMass()/GeV;
|
|---|
| 502 | hMass2 = hMass*hMass;
|
|---|
| 503 |
|
|---|
| 504 | G4double T = sqrt(plab*plab+hMass2)-hMass;
|
|---|
| 505 |
|
|---|
| 506 | if(T > 0.4) Q2 = HadronProtonQ2(p, plab);
|
|---|
| 507 |
|
|---|
| 508 | if (verboseLevel>1)
|
|---|
| 509 | G4cout<<" Proton : Q2 "<<Q2<<G4endl;
|
|---|
| 510 | }
|
|---|
| 511 | else
|
|---|
| 512 | {
|
|---|
| 513 | G4ElasticData* ElD1 = SetOfElasticData[idx][Z];
|
|---|
| 514 |
|
|---|
| 515 | // Construct elastic data
|
|---|
| 516 | if(!ElD1)
|
|---|
| 517 | {
|
|---|
| 518 | G4double AWeight = nistManager->GetAtomicMassAmu(Z);
|
|---|
| 519 | ElD1 = new G4ElasticData(p, Z, AWeight, Energy);
|
|---|
| 520 | SetOfElasticData[idx][Z] = ElD1;
|
|---|
| 521 |
|
|---|
| 522 | if(verboseLevel > 1)
|
|---|
| 523 | {
|
|---|
| 524 | G4cout<< " G4ElasticHadrNucleusHE::SampleT: new record " << idx
|
|---|
| 525 | << " for " << p->GetParticleName() << " Z= " << Z
|
|---|
| 526 | << G4endl;
|
|---|
| 527 | }
|
|---|
| 528 | }
|
|---|
| 529 | hMass = ElD1->massGeV;
|
|---|
| 530 | hMass2 = ElD1->mass2GeV2;
|
|---|
| 531 | G4double M = ElD1->massA;
|
|---|
| 532 | G4double M2 = ElD1->massA2;
|
|---|
| 533 | G4double plab2 = plab*plab;
|
|---|
| 534 | G4double Q2max = 4.*plab2*M2/
|
|---|
| 535 | (hMass2 + M2 + 2.*M*std::sqrt(plab2 + hMass2));
|
|---|
| 536 |
|
|---|
| 537 | // sample scattering
|
|---|
| 538 | G4double T = sqrt(plab2+hMass2)-hMass;
|
|---|
| 539 |
|
|---|
| 540 | if(T > 0.4) Q2 = HadronNucleusQ2_2(ElD1, Z, plab, Q2max);
|
|---|
| 541 |
|
|---|
| 542 | if(verboseLevel > 1)
|
|---|
| 543 | G4cout<<" SampleT: Q2(GeV^2)= "<<Q2<< " t/tmax= " << Q2/Q2max <<G4endl;
|
|---|
| 544 | }
|
|---|
| 545 | return Q2*GeV2;
|
|---|
| 546 | }
|
|---|
| 547 |
|
|---|
| 548 | //////////////////////////////////////////////////////////////////////////
|
|---|
| 549 | //
|
|---|
| 550 | //
|
|---|
| 551 |
|
|---|
| 552 | G4double
|
|---|
| 553 | G4ElasticHadrNucleusHE::SampleT(const G4ParticleDefinition* p,
|
|---|
| 554 | G4double inLabMom,
|
|---|
| 555 | G4int Z, G4int N)
|
|---|
| 556 | {
|
|---|
| 557 | return SampleInvariantT(p, inLabMom, Z, N);
|
|---|
| 558 | }
|
|---|
| 559 |
|
|---|
| 560 | //////////////////////////////////////////////////////////////////////////
|
|---|
| 561 | //
|
|---|
| 562 | //
|
|---|
| 563 |
|
|---|
| 564 | G4double G4ElasticHadrNucleusHE::
|
|---|
| 565 | HadronNucleusQ2_2(G4ElasticData* pElD, G4int Z,
|
|---|
| 566 | G4double plab, G4double tmax)
|
|---|
| 567 | {
|
|---|
| 568 | G4double LineFq2[ONQ2];
|
|---|
| 569 |
|
|---|
| 570 | G4double Rand = G4UniformRand();
|
|---|
| 571 |
|
|---|
| 572 | G4int iNumbQ2 = 0;
|
|---|
| 573 | G4double Q2 = 0.0;
|
|---|
| 574 |
|
|---|
| 575 | G4double ptot2 = plab*plab;
|
|---|
| 576 | G4double ekin = std::sqrt(hMass2 + ptot2) - hMass;
|
|---|
| 577 |
|
|---|
| 578 | if(verboseLevel > 1)
|
|---|
| 579 | G4cout<<"Q2_2: ekin plab "<<ekin<<" "<<plab<<" tmax "<<tmax<<G4endl;
|
|---|
| 580 |
|
|---|
| 581 | // Find closest energy bin
|
|---|
| 582 | G4int NumbOnE;
|
|---|
| 583 | for( NumbOnE = 0; NumbOnE < NENERGY-1; NumbOnE++ )
|
|---|
| 584 | {
|
|---|
| 585 | if( ekin <= LowEdgeEnergy[NumbOnE+1] ) break;
|
|---|
| 586 | }
|
|---|
| 587 | G4double* dNumbQ2 = pElD->TableQ2;
|
|---|
| 588 |
|
|---|
| 589 | G4int index = NumbOnE*ONQ2;
|
|---|
| 590 |
|
|---|
| 591 | // Select kinematics for node energy
|
|---|
| 592 | G4double T = Energy[NumbOnE];
|
|---|
| 593 | hLabMomentum2 = T*(T + 2.*hMass);
|
|---|
| 594 | G4double Q2max = pElD->maxQ2[NumbOnE];
|
|---|
| 595 | G4int length = pElD->dnkE[NumbOnE];
|
|---|
| 596 |
|
|---|
| 597 | // Build vector
|
|---|
| 598 | if(length == 0)
|
|---|
| 599 | {
|
|---|
| 600 | R1 = pElD->R1;
|
|---|
| 601 | R2 = pElD->R2;
|
|---|
| 602 | Aeff = pElD->Aeff;
|
|---|
| 603 | Pnucl = pElD->Pnucl;
|
|---|
| 604 | hLabMomentum = std::sqrt(hLabMomentum2);
|
|---|
| 605 |
|
|---|
| 606 | DefineHadronValues(Z);
|
|---|
| 607 |
|
|---|
| 608 | if(verboseLevel >0)
|
|---|
| 609 | {
|
|---|
| 610 | G4cout<<"1 plab T "<<plab<<" "<<T<<" sigTot B ReIm "
|
|---|
| 611 | <<HadrTot<<" "<<HadrSlope<<" "<<HadrReIm<<G4endl;
|
|---|
| 612 | G4cout<<" R1 R2 Aeff p "<<R1<<" "<<R2<<" "<<Aeff<<" "
|
|---|
| 613 | <<Pnucl<<G4endl;
|
|---|
| 614 | }
|
|---|
| 615 |
|
|---|
| 616 | pElD->CrossSecMaxQ2[NumbOnE] = 1.0;
|
|---|
| 617 |
|
|---|
| 618 | if(verboseLevel > 1)
|
|---|
| 619 | G4cout<<" HadrNucleusQ2_2: NumbOnE= " << NumbOnE
|
|---|
| 620 | << " length= " << length
|
|---|
| 621 | << " Q2max= " << Q2max
|
|---|
| 622 | << " ekin= " << ekin <<G4endl;
|
|---|
| 623 |
|
|---|
| 624 | pElD->TableCrossSec[index] = 0;
|
|---|
| 625 |
|
|---|
| 626 |
|
|---|
| 627 | dQ2 = pElD->TableQ2[1]-pElD->TableQ2[0];
|
|---|
| 628 |
|
|---|
| 629 | GetHeavyFq2(NumbN, LineFq2); // %%%%%%%%%%%%%%%%%%%%%%%%%
|
|---|
| 630 |
|
|---|
| 631 | for(G4int ii=0; ii<ONQ2; ii++)
|
|---|
| 632 | {
|
|---|
| 633 | //if(verboseLevel > 2)
|
|---|
| 634 | // G4cout<<" ii LineFq2 "<<ii<<" "<<LineFq2[ii]/LineFq2[ONQ2-1]
|
|---|
| 635 | // <<" dF(q2) "<<LineFq2[ii]-LineFq2[ii-1]<<G4endl;
|
|---|
| 636 |
|
|---|
| 637 | pElD->TableCrossSec[index+ii] = LineFq2[ii]/LineFq2[ONQ2-1];
|
|---|
| 638 | }
|
|---|
| 639 |
|
|---|
| 640 | pElD->dnkE[NumbOnE] = ONQ2;
|
|---|
| 641 | length = ONQ2;
|
|---|
| 642 | }
|
|---|
| 643 |
|
|---|
| 644 | G4double* dNumbFQ2 = &(pElD->TableCrossSec[index]);
|
|---|
| 645 |
|
|---|
| 646 | for( iNumbQ2 = 1; iNumbQ2<length; iNumbQ2++ )
|
|---|
| 647 | {
|
|---|
| 648 | if(Rand <= pElD->TableCrossSec[index+iNumbQ2]) break;
|
|---|
| 649 | }
|
|---|
| 650 | Q2 = GetQ2_2(iNumbQ2, dNumbQ2, dNumbFQ2, Rand);
|
|---|
| 651 |
|
|---|
| 652 | if(tmax < Q2max) Q2 *= tmax/Q2max;
|
|---|
| 653 |
|
|---|
| 654 | if(verboseLevel > 1)
|
|---|
| 655 | G4cout<<" HadrNucleusQ2_2(2): Q2= "<<Q2<<" iNumbQ2= " << iNumbQ2
|
|---|
| 656 | << " rand= " << Rand << G4endl;
|
|---|
| 657 |
|
|---|
| 658 | return Q2;
|
|---|
| 659 | }
|
|---|
| 660 |
|
|---|
| 661 | ///////////////////////////////////////////////////////////////////////
|
|---|
| 662 | //
|
|---|
| 663 | // The randomization of one dimensional array
|
|---|
| 664 | //
|
|---|
| 665 | G4double G4ElasticHadrNucleusHE::GetQ2_2(G4int kk, G4double * Q,
|
|---|
| 666 | G4double * F, G4double ranUni)
|
|---|
| 667 | {
|
|---|
| 668 | G4double ranQ2;
|
|---|
| 669 |
|
|---|
| 670 | G4double F1 = F[kk-2];
|
|---|
| 671 | G4double F2 = F[kk-1];
|
|---|
| 672 | G4double F3 = F[kk];
|
|---|
| 673 | G4double X1 = Q[kk-2];
|
|---|
| 674 | G4double X2 = Q[kk-1];
|
|---|
| 675 | G4double X3 = Q[kk];
|
|---|
| 676 |
|
|---|
| 677 | if(verboseLevel > 2)
|
|---|
| 678 | G4cout << "GetQ2_2 kk= " << kk << " X2= " << X2 << " X3= " << X3
|
|---|
| 679 | << " F2= " << F2 << " F3= " << F3 << " Rndm= " << ranUni << G4endl;
|
|---|
| 680 |
|
|---|
| 681 | if(kk == 1 || kk == 0)
|
|---|
| 682 | {
|
|---|
| 683 | F1 = F[0];
|
|---|
| 684 | F2 = F[1];
|
|---|
| 685 | F3 = F[2];
|
|---|
| 686 | X1 = Q[0];
|
|---|
| 687 | X2 = Q[1];
|
|---|
| 688 | X3 = Q[2];
|
|---|
| 689 | }
|
|---|
| 690 |
|
|---|
| 691 | G4double F12 = F1*F1;
|
|---|
| 692 | G4double F22 = F2*F2;
|
|---|
| 693 | G4double F32 = F3*F3;
|
|---|
| 694 |
|
|---|
| 695 | G4double D0 = F12*F2+F1*F32+F3*F22-F32*F2-F22*F1-F12*F3;
|
|---|
| 696 |
|
|---|
| 697 | if(verboseLevel > 2)
|
|---|
| 698 | G4cout << " X1= " << X1 << " F1= " << F1 << " D0= "
|
|---|
| 699 | << D0 << G4endl;
|
|---|
| 700 |
|
|---|
| 701 | if(std::abs(D0) < 0.00000001)
|
|---|
| 702 | {
|
|---|
| 703 | ranQ2 = X2 + (ranUni - F2)*(X3 - X2)/(F3 - F2);
|
|---|
| 704 | }
|
|---|
| 705 | else
|
|---|
| 706 | {
|
|---|
| 707 | G4double DA = X1*F2+X3*F1+X2*F3-X3*F2-X1*F3-X2*F1;
|
|---|
| 708 | G4double DB = X2*F12+X1*F32+X3*F22-X2*F32-X3*F12-X1*F22;
|
|---|
| 709 | G4double DC = X3*F2*F12+X2*F1*F32+X1*F3*F22
|
|---|
| 710 | -X1*F2*F32-X2*F3*F12-X3*F1*F22;
|
|---|
| 711 | ranQ2 = (DA*ranUni*ranUni + DB*ranUni + DC)/D0;
|
|---|
| 712 | }
|
|---|
| 713 | return ranQ2; // MeV^2
|
|---|
| 714 | }
|
|---|
| 715 |
|
|---|
| 716 | ////////////////////////////////////////////////////////////////////////
|
|---|
| 717 | //
|
|---|
| 718 | //
|
|---|
| 719 | G4double G4ElasticHadrNucleusHE::GetHeavyFq2(G4int Nucleus, G4double* LineF)
|
|---|
| 720 | {
|
|---|
| 721 | G4int ii, jj, aSimp;
|
|---|
| 722 | G4double curQ2, curSec;
|
|---|
| 723 | G4double curSum = 0.0;
|
|---|
| 724 | G4double totSum = 0.0;
|
|---|
| 725 |
|
|---|
| 726 | G4double ddQ2 = dQ2/20;
|
|---|
| 727 | G4double Q2l = 0;
|
|---|
| 728 |
|
|---|
| 729 | LineF[0] = 0;
|
|---|
| 730 | for(ii = 1; ii<ONQ2; ii++)
|
|---|
| 731 | {
|
|---|
| 732 | curSum = 0;
|
|---|
| 733 | aSimp = 4;
|
|---|
| 734 |
|
|---|
| 735 | for(jj = 0; jj<20; jj++)
|
|---|
| 736 | {
|
|---|
| 737 | curQ2 = Q2l+jj*ddQ2;
|
|---|
| 738 |
|
|---|
| 739 | curSec = HadrNucDifferCrSec(Nucleus, curQ2);
|
|---|
| 740 | curSum += curSec*aSimp;
|
|---|
| 741 |
|
|---|
| 742 | if(aSimp > 3) aSimp = 2;
|
|---|
| 743 | else aSimp = 4;
|
|---|
| 744 |
|
|---|
| 745 | if(jj == 0 && verboseLevel>2)
|
|---|
| 746 | G4cout<<" Q2 "<<curQ2<<" AIm "<<aAIm<<" DIm "<<aDIm
|
|---|
| 747 | <<" Diff "<<curSec<<" totSum "<<totSum<<G4endl;
|
|---|
| 748 | }
|
|---|
| 749 |
|
|---|
| 750 | Q2l += dQ2;
|
|---|
| 751 | curSum *= ddQ2/2.3; // $$$$$$$$$$$$$$$$$$$$$$$
|
|---|
| 752 | totSum += curSum;
|
|---|
| 753 |
|
|---|
| 754 | LineF[ii] = totSum;
|
|---|
| 755 |
|
|---|
| 756 | if (verboseLevel>2)
|
|---|
| 757 | G4cout<<" GetHeavy: Q2 dQ2 totSum "<<Q2l<<" "<<dQ2<<" "<<totSum
|
|---|
| 758 | <<" curSec "
|
|---|
| 759 | <<curSec<<" totSum "<< totSum<<" DTot "
|
|---|
| 760 | <<curSum<<G4endl;
|
|---|
| 761 | }
|
|---|
| 762 | return totSum;
|
|---|
| 763 | }
|
|---|
| 764 |
|
|---|
| 765 | ////////////////////////////////////////////////////////////////////////
|
|---|
| 766 | //
|
|---|
| 767 | //
|
|---|
| 768 |
|
|---|
| 769 | G4double G4ElasticHadrNucleusHE::GetLightFq2(G4int Z, G4int Nucleus,
|
|---|
| 770 | G4double Q2)
|
|---|
| 771 | {
|
|---|
| 772 | // Scattering of proton
|
|---|
| 773 | if(Z == 1)
|
|---|
| 774 | {
|
|---|
| 775 | G4double SqrQ2 = std::sqrt(Q2);
|
|---|
| 776 | G4double ConstU = 2.*(hMass2 + protonM2) - Q2;
|
|---|
| 777 |
|
|---|
| 778 | G4double y = (1.-Coeff1-Coeff0)/HadrSlope*(1.-std::exp(-HadrSlope*Q2))
|
|---|
| 779 | + Coeff0*(1.-std::exp(-Slope0*Q2))
|
|---|
| 780 | + Coeff2/Slope2*std::exp(Slope2*ConstU)*(std::exp(Slope2*Q2)-1.)
|
|---|
| 781 | + 2.*Coeff1/Slope1*(1./Slope1-(1./Slope1+SqrQ2)*std::exp(-Slope1*SqrQ2));
|
|---|
| 782 |
|
|---|
| 783 | return y;
|
|---|
| 784 | }
|
|---|
| 785 |
|
|---|
| 786 | // The preparing of probability function
|
|---|
| 787 |
|
|---|
| 788 | G4double prec = Nucleus > 208 ? 1.0e-7 : 1.0e-6;
|
|---|
| 789 |
|
|---|
| 790 | G4double Stot = HadrTot*MbToGeV2; // Gev^-2
|
|---|
| 791 | G4double Bhad = HadrSlope; // GeV^-2
|
|---|
| 792 | G4double Asq = 1+HadrReIm*HadrReIm;
|
|---|
| 793 | G4double Rho2 = std::sqrt(Asq);
|
|---|
| 794 |
|
|---|
| 795 | // if(verboseLevel >1)
|
|---|
| 796 | G4cout<<" Fq2 Before for i Tot B Im "<<HadrTot<<" "<<HadrSlope<<" "
|
|---|
| 797 | <<HadrReIm<<G4endl;
|
|---|
| 798 |
|
|---|
| 799 | if(verboseLevel > 1) {
|
|---|
| 800 | G4cout << "GetFq2: Stot= " << Stot << " Bhad= " << Bhad
|
|---|
| 801 | <<" Im "<<HadrReIm
|
|---|
| 802 | << " Asq= " << Asq << G4endl;
|
|---|
| 803 | G4cout << "R1= " << R1 << " R2= " << R2 << " Pnucl= " << Pnucl <<G4endl;
|
|---|
| 804 | }
|
|---|
| 805 | G4double R12 = R1*R1;
|
|---|
| 806 | G4double R22 = R2*R2;
|
|---|
| 807 | G4double R12B = R12+2*Bhad;
|
|---|
| 808 | G4double R22B = R22+2*Bhad;
|
|---|
| 809 |
|
|---|
| 810 | G4double Norm = (R12*R1-Pnucl*R22*R2); // HP->Aeff;
|
|---|
| 811 |
|
|---|
| 812 | G4double R13 = R12*R1/R12B;
|
|---|
| 813 | G4double R23 = Pnucl*R22*R2/R22B;
|
|---|
| 814 | G4double Unucl = Stot/twopi/Norm*R13;
|
|---|
| 815 | G4double UnucRho2 = -Unucl*Rho2;
|
|---|
| 816 |
|
|---|
| 817 | G4double FiH = std::asin(HadrReIm/Rho2);
|
|---|
| 818 | G4double NN2 = R23/R13;
|
|---|
| 819 |
|
|---|
| 820 | if(verboseLevel > 2)
|
|---|
| 821 | G4cout << "UnucRho2= " << UnucRho2 << " FiH= " << FiH << " NN2= " << NN2
|
|---|
| 822 | << " Norm= " << Norm << G4endl;
|
|---|
| 823 |
|
|---|
| 824 | G4double dddd;
|
|---|
| 825 |
|
|---|
| 826 | G4double Prod0 = 0;
|
|---|
| 827 | G4double N1 = -1.0;
|
|---|
| 828 | G4double Tot0 = 0;
|
|---|
| 829 | G4double exp1;
|
|---|
| 830 |
|
|---|
| 831 | G4double Prod3 ;
|
|---|
| 832 | G4double exp2 ;
|
|---|
| 833 | G4double N4, N5, N2, Prod1, Prod2;
|
|---|
| 834 | G4int i1, i2, m1, m2;
|
|---|
| 835 |
|
|---|
| 836 | for(i1 = 1; i1<= Nucleus; i1++) ////++++++++++ i1
|
|---|
| 837 | {
|
|---|
| 838 | N1 = -N1*Unucl*(Nucleus-i1+1)/i1*Rho2;
|
|---|
| 839 | Prod1 = 0;
|
|---|
| 840 | Tot0 = 0;
|
|---|
| 841 | N2 = -1;
|
|---|
| 842 |
|
|---|
| 843 | for(i2 = 1; i2<=Nucleus; i2++) ////+++++++++ i2
|
|---|
| 844 | {
|
|---|
| 845 | N2 = -N2*Unucl*(Nucleus-i2+1)/i2*Rho2;
|
|---|
| 846 | Prod2 = 0;
|
|---|
| 847 | N5 = -1/NN2;
|
|---|
| 848 | for(m2=0; m2<= i2; m2++) ////+++++++++ m2
|
|---|
| 849 | {
|
|---|
| 850 | Prod3 = 0;
|
|---|
| 851 | exp2 = 1/(m2/R22B+(i2-m2)/R12B);
|
|---|
| 852 | N5 = -N5*NN2;
|
|---|
| 853 | N4 = -1/NN2;
|
|---|
| 854 | for(m1=0; m1<=i1; m1++) ////++++++++ m1
|
|---|
| 855 | {
|
|---|
| 856 | exp1 = 1/(m1/R22B+(i1-m1)/R12B);
|
|---|
| 857 | dddd = exp1+exp2;
|
|---|
| 858 | N4 = -N4*NN2;
|
|---|
| 859 | Prod3 = Prod3+N4*exp1*exp2*
|
|---|
| 860 | (1-std::exp(-Q2*dddd/4))/dddd*4*SetBinom[i1][m1];
|
|---|
| 861 | } // m1
|
|---|
| 862 | Prod2 = Prod2 +Prod3*N5*SetBinom[i2][m2];
|
|---|
| 863 | } // m2
|
|---|
| 864 | Prod1 = Prod1 + Prod2*N2*std::cos(FiH*(i1-i2));
|
|---|
| 865 |
|
|---|
| 866 | if (std::fabs(Prod2*N2/Prod1)<prec) break;
|
|---|
| 867 | } // i2
|
|---|
| 868 | Prod0 = Prod0 + Prod1*N1;
|
|---|
| 869 | if(std::fabs(N1*Prod1/Prod0) < prec) break;
|
|---|
| 870 |
|
|---|
| 871 | } // i1
|
|---|
| 872 |
|
|---|
| 873 | Prod0 *= 0.25*pi/MbToGeV2; // This is in mb
|
|---|
| 874 |
|
|---|
| 875 | if(verboseLevel>1)
|
|---|
| 876 | G4cout << "GetLightFq2 Z= " << Z << " A= " << Nucleus
|
|---|
| 877 | <<" Q2= " << Q2 << " Res= " << Prod0 << G4endl;
|
|---|
| 878 | return Prod0;
|
|---|
| 879 | }
|
|---|
| 880 | // +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
|
|---|
| 881 | G4double G4ElasticHadrNucleusHE::
|
|---|
| 882 | HadrNucDifferCrSec(G4int Nucleus, G4double aQ2)
|
|---|
| 883 | {
|
|---|
| 884 | // ------ All external kinematical variables are in MeV -------
|
|---|
| 885 | // ------ but internal in GeV !!!! ------
|
|---|
| 886 |
|
|---|
| 887 | G4double theQ2 = aQ2; ///GeV/GeV;
|
|---|
| 888 |
|
|---|
| 889 | // Scattering of proton
|
|---|
| 890 | if(Nucleus == 1)
|
|---|
| 891 | {
|
|---|
| 892 | G4double SqrQ2 = std::sqrt(aQ2);
|
|---|
| 893 | G4double ConstU = hMass2 + protonM2-2*protonM*HadrEnergy - aQ2;
|
|---|
| 894 |
|
|---|
| 895 | G4double MaxT = 4*MomentumCM*MomentumCM;
|
|---|
| 896 |
|
|---|
| 897 | BoundaryTL[0] = MaxT;
|
|---|
| 898 | BoundaryTL[1] = MaxT;
|
|---|
| 899 | BoundaryTL[3] = MaxT;
|
|---|
| 900 | BoundaryTL[4] = MaxT;
|
|---|
| 901 | BoundaryTL[5] = MaxT;
|
|---|
| 902 |
|
|---|
| 903 | G4double dSigPodT;
|
|---|
| 904 |
|
|---|
| 905 | dSigPodT = HadrTot*HadrTot*(1+HadrReIm*HadrReIm)*
|
|---|
| 906 | (
|
|---|
| 907 | Coeff1*std::exp(-Slope1*SqrQ2)+
|
|---|
| 908 | Coeff2*std::exp( Slope2*(ConstU)+aQ2)+
|
|---|
| 909 | (1-Coeff1-Coeff0)*std::exp(-HadrSlope*aQ2)+
|
|---|
| 910 | +Coeff0*std::exp(-Slope0*aQ2)
|
|---|
| 911 | // +0.1*(1-std::fabs(CosTh))
|
|---|
| 912 | )/16/3.1416*2.568;
|
|---|
| 913 |
|
|---|
| 914 | return dSigPodT;
|
|---|
| 915 | }
|
|---|
| 916 |
|
|---|
| 917 | G4double Stot = HadrTot*MbToGeV2;
|
|---|
| 918 | G4double Bhad = HadrSlope;
|
|---|
| 919 | G4double Asq = 1+HadrReIm*HadrReIm;
|
|---|
| 920 | G4double Rho2 = std::sqrt(Asq);
|
|---|
| 921 | G4double Pnuclp = 0.001;
|
|---|
| 922 | Pnuclp = Pnucl;
|
|---|
| 923 | G4double R12 = R1*R1;
|
|---|
| 924 | G4double R22 = R2*R2;
|
|---|
| 925 | G4double R12B = R12+2*Bhad;
|
|---|
| 926 | G4double R22B = R22+2*Bhad;
|
|---|
| 927 | G4double R12Ap = R12+20;
|
|---|
| 928 | G4double R22Ap = R22+20;
|
|---|
| 929 | G4double R13Ap = R12*R1/R12Ap;
|
|---|
| 930 | G4double R23Ap = R22*R2/R22Ap*Pnuclp;
|
|---|
| 931 | G4double R23dR13 = R23Ap/R13Ap;
|
|---|
| 932 | G4double R12Apd = 2/R12Ap;
|
|---|
| 933 | G4double R22Apd = 2/R22Ap;
|
|---|
| 934 | G4double R12ApdR22Ap = 0.5*(R12Apd+R22Apd);
|
|---|
| 935 |
|
|---|
| 936 | G4double DDSec1p = (DDSect2+DDSect3*std::log(1.06*2*HadrEnergy/R1/4));
|
|---|
| 937 | G4double DDSec2p = (DDSect2+DDSect3*std::log(1.06*2*HadrEnergy/
|
|---|
| 938 | std::sqrt((R12+R22)/2)/4));
|
|---|
| 939 | G4double DDSec3p = (DDSect2+DDSect3*std::log(1.06*2*HadrEnergy/R2/4));
|
|---|
| 940 |
|
|---|
| 941 | G4double Norm = (R12*R1-Pnucl*R22*R2)*Aeff;
|
|---|
| 942 | G4double Normp = (R12*R1-Pnuclp*R22*R2)*Aeff;
|
|---|
| 943 | G4double R13 = R12*R1/R12B;
|
|---|
| 944 | G4double R23 = Pnucl*R22*R2/R22B;
|
|---|
| 945 | G4double Unucl = Stot/twopi/Norm*R13;
|
|---|
| 946 | G4double UnuclScr = Stot/twopi/Normp*R13Ap;
|
|---|
| 947 | G4double SinFi = HadrReIm/Rho2;
|
|---|
| 948 | G4double FiH = std::asin(SinFi);
|
|---|
| 949 | G4double N = -1;
|
|---|
| 950 | G4double N2 = R23/R13;
|
|---|
| 951 |
|
|---|
| 952 | G4double ImElasticAmpl0 = 0;
|
|---|
| 953 | G4double ReElasticAmpl0 = 0;
|
|---|
| 954 |
|
|---|
| 955 | G4double exp1;
|
|---|
| 956 | G4double N4;
|
|---|
| 957 | G4double Prod1, Tot1=0, medTot, DTot1, DmedTot;
|
|---|
| 958 | G4int i;
|
|---|
| 959 |
|
|---|
| 960 | for( i=1; i<=Nucleus; i++)
|
|---|
| 961 | {
|
|---|
| 962 | N = -N*Unucl*(Nucleus-i+1)/i*Rho2;
|
|---|
| 963 | N4 = 1;
|
|---|
| 964 | Prod1 = std::exp(-theQ2/i*R12B/4)/i*R12B;
|
|---|
| 965 | medTot = R12B/i;
|
|---|
| 966 |
|
|---|
| 967 | for(G4int l=1; l<=i; l++)
|
|---|
| 968 | {
|
|---|
| 969 | exp1 = l/R22B+(i-l)/R12B;
|
|---|
| 970 | N4 = -N4*(i-l+1)/l*N2;
|
|---|
| 971 | Prod1 = Prod1+N4/exp1*std::exp(-theQ2/exp1/4);
|
|---|
| 972 | medTot = medTot+N4/exp1;
|
|---|
| 973 | } // end l
|
|---|
| 974 |
|
|---|
| 975 | ReElasticAmpl0 = ReElasticAmpl0+Prod1*N*std::sin(FiH*i);
|
|---|
| 976 | ImElasticAmpl0 = ImElasticAmpl0+Prod1*N*std::cos(FiH*i);
|
|---|
| 977 | Tot1 = Tot1+medTot*N*std::cos(FiH*i);
|
|---|
| 978 | if(std::fabs(Prod1*N/ImElasticAmpl0) < 0.000001) break;
|
|---|
| 979 | } // i
|
|---|
| 980 |
|
|---|
| 981 | ImElasticAmpl0 = ImElasticAmpl0*pi/2.568; // The amplitude in mB
|
|---|
| 982 | ReElasticAmpl0 = ReElasticAmpl0*pi/2.568; // The amplitude in mB
|
|---|
| 983 | Tot1 = Tot1*twopi/2.568;
|
|---|
| 984 |
|
|---|
| 985 | G4double C1 = R13Ap*R13Ap/2*DDSec1p;
|
|---|
| 986 | G4double C2 = 2*R23Ap*R13Ap/2*DDSec2p;
|
|---|
| 987 | G4double C3 = R23Ap*R23Ap/2*DDSec3p;
|
|---|
| 988 |
|
|---|
| 989 | G4double N1p = 1;
|
|---|
| 990 |
|
|---|
| 991 | G4double Din1 = 0.5;
|
|---|
| 992 |
|
|---|
| 993 | Din1 = 0.5*(C1*std::exp(-theQ2/8*R12Ap)/2*R12Ap-
|
|---|
| 994 | C2/R12ApdR22Ap*std::exp(-theQ2/4/R12ApdR22Ap)+
|
|---|
| 995 | C3*R22Ap/2*std::exp(-theQ2/8*R22Ap));
|
|---|
| 996 |
|
|---|
| 997 | DTot1 = 0.5*(C1/2*R12Ap-C2/R12ApdR22Ap+C3*R22Ap/2);
|
|---|
| 998 |
|
|---|
| 999 | G4double exp1p;
|
|---|
| 1000 | G4double exp2p;
|
|---|
| 1001 | G4double exp3p;
|
|---|
| 1002 | G4double N2p;
|
|---|
| 1003 | G4double Din2, BinCoeff;
|
|---|
| 1004 |
|
|---|
| 1005 | BinCoeff = 1;
|
|---|
| 1006 |
|
|---|
| 1007 | for( i = 1; i<= Nucleus-2; i++)
|
|---|
| 1008 | {
|
|---|
| 1009 | N1p = -N1p*UnuclScr*(Nucleus-i-1)/i*Rho2;
|
|---|
| 1010 | N2p = 1;
|
|---|
| 1011 | Din2 = 0;
|
|---|
| 1012 | DmedTot = 0;
|
|---|
| 1013 | for(G4int l = 0; l<=i; l++)
|
|---|
| 1014 | {
|
|---|
| 1015 | if(l == 0) BinCoeff = 1;
|
|---|
| 1016 | else if(l !=0 ) BinCoeff = BinCoeff*(i-l+1)/l;
|
|---|
| 1017 |
|
|---|
| 1018 | exp1 = l/R22B+(i-l)/R12B;
|
|---|
| 1019 | exp1p = exp1+R12Apd;
|
|---|
| 1020 | exp2p = exp1+R12ApdR22Ap;
|
|---|
| 1021 | exp3p = exp1+R22Apd;
|
|---|
| 1022 |
|
|---|
| 1023 | Din2 = Din2 + N2p*BinCoeff*
|
|---|
| 1024 | (C1/exp1p*std::exp(-theQ2/4/exp1p)-
|
|---|
| 1025 | C2/exp2p*std::exp(-theQ2/4/exp2p)+
|
|---|
| 1026 | C3/exp3p*std::exp(-theQ2/4/exp3p));
|
|---|
| 1027 |
|
|---|
| 1028 | DmedTot = DmedTot + N2p*BinCoeff*
|
|---|
| 1029 | (C1/exp1p-C2/exp2p+C3/exp3p);
|
|---|
| 1030 |
|
|---|
| 1031 | N2p = -N2p*R23dR13;
|
|---|
| 1032 | } // l
|
|---|
| 1033 |
|
|---|
| 1034 | Din1 = Din1+Din2*N1p/*Mnoj[i]*//(i+2)/(i+1)*std::cos(FiH*i);
|
|---|
| 1035 | DTot1 = DTot1+DmedTot*N1p/*Mnoj[i]*//(i+2)/(i+1)*std::cos(FiH*i);
|
|---|
| 1036 |
|
|---|
| 1037 | if(std::fabs(Din2*N1p/Din1) < 0.000001) break;
|
|---|
| 1038 | } // i
|
|---|
| 1039 |
|
|---|
| 1040 | Din1 = -Din1*Nucleus*(Nucleus-1)
|
|---|
| 1041 | /2/pi/Normp/2/pi/Normp*16*pi*pi;
|
|---|
| 1042 |
|
|---|
| 1043 | DTot1 = DTot1*Nucleus*(Nucleus-1)
|
|---|
| 1044 | /2/pi/Normp/2/pi/Normp*16*pi*pi;
|
|---|
| 1045 |
|
|---|
| 1046 | DTot1 *= 5; // $$$$$$$$$$$$$$$$$$$$$$$$
|
|---|
| 1047 | // Din1 *= 0.2; // %%%%%%%%%%%%%%%%%%%%%%% proton
|
|---|
| 1048 | // Din1 *= 0.05; // %%%%%%%%%%%%%%%%%%%%%%% pi+
|
|---|
| 1049 | // ---------------- dSigma/d|-t|, mb/(GeV/c)^-2 -----------------
|
|---|
| 1050 |
|
|---|
| 1051 | G4double DiffCrSec2 = (ReElasticAmpl0*ReElasticAmpl0+
|
|---|
| 1052 | (ImElasticAmpl0+Din1)*
|
|---|
| 1053 | (ImElasticAmpl0+Din1))*2/4/pi;
|
|---|
| 1054 |
|
|---|
| 1055 | Tot1 = Tot1-DTot1;
|
|---|
| 1056 | // Tott1 = Tot1*1.0;
|
|---|
| 1057 | Dtot11 = DTot1;
|
|---|
| 1058 | aAIm = ImElasticAmpl0;
|
|---|
| 1059 | aDIm = Din1;
|
|---|
| 1060 |
|
|---|
| 1061 | return DiffCrSec2*1.0; // dSig/d|-t|, mb/(GeV/c)^-2
|
|---|
| 1062 | } // function
|
|---|
| 1063 | // ##############################################
|
|---|
| 1064 |
|
|---|
| 1065 | ////////////////////////////////////////////////////////////////
|
|---|
| 1066 | //
|
|---|
| 1067 | //
|
|---|
| 1068 |
|
|---|
| 1069 | void G4ElasticHadrNucleusHE::DefineHadronValues(G4int Z)
|
|---|
| 1070 | {
|
|---|
| 1071 | HadrEnergy = std::sqrt(hMass2 + hLabMomentum2);
|
|---|
| 1072 |
|
|---|
| 1073 | G4double sHadr = 2.*HadrEnergy*protonM+protonM2+hMass2;
|
|---|
| 1074 | G4double sqrS = std::sqrt(sHadr);
|
|---|
| 1075 | G4double Ecm = 0.5*(sHadr-hMass2+protonM2)/sqrS;
|
|---|
| 1076 | MomentumCM = std::sqrt(Ecm*Ecm-protonM2);
|
|---|
| 1077 |
|
|---|
| 1078 | if(verboseLevel>2)
|
|---|
| 1079 | G4cout << "GetHadrVall.: Z= " << Z << " iHadr= " << iHadron
|
|---|
| 1080 | << " E(GeV)= " << HadrEnergy << " sqrS= " << sqrS
|
|---|
| 1081 | << " plab= " << hLabMomentum
|
|---|
| 1082 | <<" E - m "<<HadrEnergy - hMass<< G4endl;
|
|---|
| 1083 |
|
|---|
| 1084 | G4double TotN = 0.0;
|
|---|
| 1085 | G4double logE = std::log(HadrEnergy);
|
|---|
| 1086 | G4double logS = std::log(sHadr);
|
|---|
| 1087 | TotP = 0.0;
|
|---|
| 1088 |
|
|---|
| 1089 | switch (iHadron)
|
|---|
| 1090 | {
|
|---|
| 1091 | case 0: // proton, neutron
|
|---|
| 1092 | case 6:
|
|---|
| 1093 |
|
|---|
| 1094 | if(hLabMomentum > 10)
|
|---|
| 1095 | TotP = TotN = 7.5*logE - 40.12525 + 103*std::pow(sHadr,-0.165); // mb
|
|---|
| 1096 |
|
|---|
| 1097 | else
|
|---|
| 1098 | {
|
|---|
| 1099 | // ================== neutron ================
|
|---|
| 1100 |
|
|---|
| 1101 | //// if(iHadrCode == 2112)
|
|---|
| 1102 |
|
|---|
| 1103 |
|
|---|
| 1104 | if( hLabMomentum > 1.4 )
|
|---|
| 1105 | TotN = 33.3+15.2*(hLabMomentum2-1.35)/
|
|---|
| 1106 | (std::pow(hLabMomentum,2.37)+0.95);
|
|---|
| 1107 |
|
|---|
| 1108 | else if(hLabMomentum > 0.8)
|
|---|
| 1109 | {
|
|---|
| 1110 | G4double A0 = logE + 0.0513;
|
|---|
| 1111 | TotN = 33.0 + 25.5*A0*A0;
|
|---|
| 1112 | }
|
|---|
| 1113 | else
|
|---|
| 1114 | {
|
|---|
| 1115 | G4double A0 = logE - 0.2634; // log(1.3)
|
|---|
| 1116 | TotN = 33.0 + 30.*A0*A0*A0*A0;
|
|---|
| 1117 | }
|
|---|
| 1118 | // ================= proton ===============
|
|---|
| 1119 | // else if(iHadrCode == 2212)
|
|---|
| 1120 | {
|
|---|
| 1121 | if(hLabMomentum >= 1.05)
|
|---|
| 1122 | {
|
|---|
| 1123 | TotP = 39.0+75.*(hLabMomentum-1.2)/
|
|---|
| 1124 | (hLabMomentum2*hLabMomentum+0.15);
|
|---|
| 1125 | }
|
|---|
| 1126 |
|
|---|
| 1127 | else if(hLabMomentum >= 0.7)
|
|---|
| 1128 | {
|
|---|
| 1129 | G4double A0 = logE + 0.3147;
|
|---|
| 1130 | TotP = 23.0 + 40.*A0*A0;
|
|---|
| 1131 | }
|
|---|
| 1132 | else
|
|---|
| 1133 | {
|
|---|
| 1134 | TotP = 23.+50.*std::pow(std::log(0.73/hLabMomentum),3.5);
|
|---|
| 1135 | }
|
|---|
| 1136 | }
|
|---|
| 1137 | }
|
|---|
| 1138 |
|
|---|
| 1139 | // HadrTot = 0.5*(82*TotP+126*TotN)/104; // $$$$$$$$$$$$$$$$$$
|
|---|
| 1140 | HadrTot = 0.5*(TotP+TotN);
|
|---|
| 1141 | // ...................................................
|
|---|
| 1142 | // Proton slope
|
|---|
| 1143 | if(hLabMomentum >= 2.) HadrSlope = 5.44 + 0.88*logS;
|
|---|
| 1144 |
|
|---|
| 1145 | else if(hLabMomentum >= 0.5) HadrSlope = 3.73*hLabMomentum-0.37;
|
|---|
| 1146 |
|
|---|
| 1147 | else HadrSlope = 1.5;
|
|---|
| 1148 |
|
|---|
| 1149 | // ...................................................
|
|---|
| 1150 | if(hLabMomentum >= 1.2)
|
|---|
| 1151 | HadrReIm = 0.13*(logS - 5.8579332)*std::pow(sHadr,-0.18);
|
|---|
| 1152 |
|
|---|
| 1153 | else if(hLabMomentum >= 0.6)
|
|---|
| 1154 | HadrReIm = -75.5*(std::pow(hLabMomentum,0.25)-0.95)/
|
|---|
| 1155 | (std::pow(3*hLabMomentum,2.2)+1);
|
|---|
| 1156 |
|
|---|
| 1157 | else
|
|---|
| 1158 | HadrReIm = 15.5*hLabMomentum/(27*hLabMomentum2*hLabMomentum+2);
|
|---|
| 1159 | // ...................................................
|
|---|
| 1160 | DDSect2 = 2.2; //mb*GeV-2
|
|---|
| 1161 | DDSect3 = 0.6; //mb*GeV-2
|
|---|
| 1162 | // ================== lambda ==================
|
|---|
| 1163 | if( iHadrCode == 3122)
|
|---|
| 1164 | {
|
|---|
| 1165 | HadrTot *= 0.88;
|
|---|
| 1166 | HadrSlope *=0.85;
|
|---|
| 1167 | }
|
|---|
| 1168 | // ================== sigma + ==================
|
|---|
| 1169 | else if( iHadrCode == 3222)
|
|---|
| 1170 | {
|
|---|
| 1171 | HadrTot *=0.81;
|
|---|
| 1172 | HadrSlope *=0.85;
|
|---|
| 1173 | }
|
|---|
| 1174 | // ================== sigma 0,- ==================
|
|---|
| 1175 | else if(iHadrCode == 3112 || iHadrCode == 3212 )
|
|---|
| 1176 | {
|
|---|
| 1177 | HadrTot *=0.88;
|
|---|
| 1178 | HadrSlope *=0.85;
|
|---|
| 1179 | }
|
|---|
| 1180 | // =================== xi =================
|
|---|
| 1181 | else if( iHadrCode == 3312 || iHadrCode == 3322 )
|
|---|
| 1182 | {
|
|---|
| 1183 | HadrTot *=0.77;
|
|---|
| 1184 | HadrSlope *=0.75;
|
|---|
| 1185 | }
|
|---|
| 1186 | // ================= omega =================
|
|---|
| 1187 | else if( iHadrCode == 3334)
|
|---|
| 1188 | {
|
|---|
| 1189 | HadrTot *=0.78;
|
|---|
| 1190 | HadrSlope *=0.7;
|
|---|
| 1191 | }
|
|---|
| 1192 |
|
|---|
| 1193 | break;
|
|---|
| 1194 | // ===========================================================
|
|---|
| 1195 | case 1: // antiproton
|
|---|
| 1196 | case 7: // antineutron
|
|---|
| 1197 |
|
|---|
| 1198 | HadrTot = 5.2+5.2*logE + 123.2/sqrS; // mb
|
|---|
| 1199 | HadrSlope = 8.32+0.57*logS; //(GeV/c)^-2
|
|---|
| 1200 |
|
|---|
| 1201 | if( HadrEnergy < 1000 )
|
|---|
| 1202 | HadrReIm = 0.06*(sqrS-2.236)*(sqrS-14.14)*std::pow(sHadr,-0.8);
|
|---|
| 1203 | else
|
|---|
| 1204 | HadrReIm = 0.6*(logS - 5.8579332)*std::pow(sHadr,-0.25);
|
|---|
| 1205 |
|
|---|
| 1206 | DDSect2 = 11; //mb*(GeV/c)^-2
|
|---|
| 1207 | DDSect3 = 3; //mb*(GeV/c)^-2
|
|---|
| 1208 | // ================== lambda ==================
|
|---|
| 1209 | if( iHadrCode == -3122)
|
|---|
| 1210 | {
|
|---|
| 1211 | HadrTot *= 0.88;
|
|---|
| 1212 | HadrSlope *=0.85;
|
|---|
| 1213 | }
|
|---|
| 1214 | // ================== sigma + ==================
|
|---|
| 1215 | else if( iHadrCode == -3222)
|
|---|
| 1216 | {
|
|---|
| 1217 | HadrTot *=0.81;
|
|---|
| 1218 | HadrSlope *=0.85;
|
|---|
| 1219 | }
|
|---|
| 1220 | // ================== sigma 0,- ==================
|
|---|
| 1221 | else if(iHadrCode == -3112 || iHadrCode == -3212 )
|
|---|
| 1222 | {
|
|---|
| 1223 | HadrTot *=0.88;
|
|---|
| 1224 | HadrSlope *=0.85;
|
|---|
| 1225 | }
|
|---|
| 1226 | // =================== xi =================
|
|---|
| 1227 | else if( iHadrCode == -3312 || iHadrCode == -3322 )
|
|---|
| 1228 | {
|
|---|
| 1229 | HadrTot *=0.77;
|
|---|
| 1230 | HadrSlope *=0.75;
|
|---|
| 1231 | }
|
|---|
| 1232 | // ================= omega =================
|
|---|
| 1233 | else if( iHadrCode == -3334)
|
|---|
| 1234 | {
|
|---|
| 1235 | HadrTot *=0.78;
|
|---|
| 1236 | HadrSlope *=0.7;
|
|---|
| 1237 | }
|
|---|
| 1238 |
|
|---|
| 1239 | break;
|
|---|
| 1240 | // -------------------------------------------
|
|---|
| 1241 | case 2: // pi plus, pi minus
|
|---|
| 1242 | case 3:
|
|---|
| 1243 |
|
|---|
| 1244 | if(hLabMomentum >= 3.5)
|
|---|
| 1245 | TotP = 10.6+2.*logE + 25.*std::pow(HadrEnergy,-0.43); // mb
|
|---|
| 1246 | // =========================================
|
|---|
| 1247 | else if(hLabMomentum >= 1.15)
|
|---|
| 1248 | {
|
|---|
| 1249 | G4double x = (hLabMomentum - 2.55)/0.55;
|
|---|
| 1250 | G4double y = (hLabMomentum - 1.47)/0.225;
|
|---|
| 1251 | TotP = 3.2*std::exp(-x*x) + 12.*std::exp(-y*y) + 27.5;
|
|---|
| 1252 | }
|
|---|
| 1253 | // =========================================
|
|---|
| 1254 | else if(hLabMomentum >= 0.4)
|
|---|
| 1255 | {
|
|---|
| 1256 | TotP = 88*(logE+0.2877)*(logE+0.2877)+14.0;
|
|---|
| 1257 | }
|
|---|
| 1258 | // =========================================
|
|---|
| 1259 | else
|
|---|
| 1260 | {
|
|---|
| 1261 | G4double x = (hLabMomentum - 0.29)/0.085;
|
|---|
| 1262 | TotP = 20. + 180.*std::exp(-x*x);
|
|---|
| 1263 | }
|
|---|
| 1264 | // -------------------------------------------
|
|---|
| 1265 |
|
|---|
| 1266 | if(hLabMomentum >= 3.0 )
|
|---|
| 1267 | TotN = 10.6 + 2.*logE + 30.*std::pow(HadrEnergy,-0.43); // mb
|
|---|
| 1268 |
|
|---|
| 1269 | else if(hLabMomentum >= 1.3)
|
|---|
| 1270 | {
|
|---|
| 1271 | G4double x = (hLabMomentum - 2.1)/0.4;
|
|---|
| 1272 | G4double y = (hLabMomentum - 1.4)/0.12;
|
|---|
| 1273 | TotN = 36.1+0.079 - 4.313*logE + 3.*std::exp(-x*x) +
|
|---|
| 1274 | 1.5*std::exp(-y*y);
|
|---|
| 1275 | }
|
|---|
| 1276 | else if(hLabMomentum >= 0.65)
|
|---|
| 1277 | {
|
|---|
| 1278 | G4double x = (hLabMomentum - 0.72)/0.06;
|
|---|
| 1279 | G4double y = (hLabMomentum - 1.015)/0.075;
|
|---|
| 1280 | TotN = 36.1 + 10.*std::exp(-x*x) + 24*std::exp(-y*y);
|
|---|
| 1281 | }
|
|---|
| 1282 | else if(hLabMomentum >= 0.37)
|
|---|
| 1283 | {
|
|---|
| 1284 | G4double x = std::log(hLabMomentum/0.48);
|
|---|
| 1285 | TotN = 26. + 110.*x*x;
|
|---|
| 1286 | }
|
|---|
| 1287 | else
|
|---|
| 1288 | {
|
|---|
| 1289 | G4double x = (hLabMomentum - 0.29)/0.07;
|
|---|
| 1290 | TotN = 28.0 + 40.*std::exp(-x*x);
|
|---|
| 1291 | }
|
|---|
| 1292 | HadrTot = (TotP+TotN)/2;
|
|---|
| 1293 | // ........................................
|
|---|
| 1294 | HadrSlope = 7.28+0.245*logS; // GeV-2
|
|---|
| 1295 | HadrReIm = 0.2*(logS - 4.6051702)*std::pow(sHadr,-0.15);
|
|---|
| 1296 |
|
|---|
| 1297 | DDSect2 = 0.7; //mb*GeV-2
|
|---|
| 1298 | DDSect3 = 0.27; //mb*GeV-2
|
|---|
| 1299 |
|
|---|
| 1300 | break;
|
|---|
| 1301 | // ==========================================================
|
|---|
| 1302 | case 4: // K plus
|
|---|
| 1303 |
|
|---|
| 1304 | HadrTot = 10.6+1.8*logE + 9.0*std::pow(HadrEnergy,-0.55); // mb
|
|---|
| 1305 | if(HadrEnergy>100) HadrSlope = 15.0;
|
|---|
| 1306 | else HadrSlope = 1.0+1.76*logS - 2.84/sqrS; // GeV-2
|
|---|
| 1307 |
|
|---|
| 1308 | HadrReIm = 0.4*(sHadr-20)*(sHadr-150)*std::pow(sHadr+50,-2.1);
|
|---|
| 1309 | DDSect2 = 0.7; //mb*GeV-2
|
|---|
| 1310 | DDSect3 = 0.21; //mb*GeV-2
|
|---|
| 1311 | break;
|
|---|
| 1312 | // =========================================================
|
|---|
| 1313 | case 5: // K minus
|
|---|
| 1314 |
|
|---|
| 1315 | HadrTot = 10+1.8*logE + 25./sqrS; // mb
|
|---|
| 1316 | HadrSlope = 6.98+0.127*logS; // GeV-2
|
|---|
| 1317 | HadrReIm = 0.4*(sHadr-20)*(sHadr-20)*std::pow(sHadr+50,-2.1);
|
|---|
| 1318 | DDSect2 = 0.7; //mb*GeV-2
|
|---|
| 1319 | DDSect3 = 0.27; //mb*GeV-2
|
|---|
| 1320 | break;
|
|---|
| 1321 | }
|
|---|
| 1322 | // =========================================================
|
|---|
| 1323 | if(verboseLevel>2)
|
|---|
| 1324 | G4cout << "HadrTot= " << HadrTot << " HadrSlope= " << HadrSlope
|
|---|
| 1325 | << " HadrReIm= " << HadrReIm << " DDSect2= " << DDSect2
|
|---|
| 1326 | << " DDSect3= " << DDSect3 << G4endl;
|
|---|
| 1327 |
|
|---|
| 1328 | if(Z != 1) return;
|
|---|
| 1329 |
|
|---|
| 1330 | // Scattering of protons
|
|---|
| 1331 |
|
|---|
| 1332 | Coeff0 = Coeff1 = Coeff2 = 0.0;
|
|---|
| 1333 | Slope0 = Slope1 = 1.0;
|
|---|
| 1334 | Slope2 = 5.0;
|
|---|
| 1335 |
|
|---|
| 1336 | // data for iHadron=0
|
|---|
| 1337 | static const G4double EnP0[6]={1.5,3.0,5.0,9.0,14.0,19.0};
|
|---|
| 1338 | static const G4double C0P0[6]={0.15,0.02,0.06,0.08,0.0003,0.0002};
|
|---|
| 1339 | static const G4double C1P0[6]={0.05,0.02,0.03,0.025,0.0,0.0};
|
|---|
| 1340 | static const G4double B0P0[6]={1.5,2.5,3.0,4.5,1.4,1.25};
|
|---|
| 1341 | static const G4double B1P0[6]={5.0,1.0,3.5,4.0,4.8,4.8};
|
|---|
| 1342 |
|
|---|
| 1343 | // data for iHadron=6,7
|
|---|
| 1344 | static const G4double EnN[5]={1.5,5.0,10.0,14.0,20.0};
|
|---|
| 1345 | static const G4double C0N[5]={0.0,0.0,0.02,0.02,0.01};
|
|---|
| 1346 | static const G4double C1N[5]={0.06,0.008,0.0015,0.001,0.0003};
|
|---|
| 1347 | static const G4double B0N[5]={1.5,2.5,3.8,3.8,3.5};
|
|---|
| 1348 | static const G4double B1N[5]={1.5,2.2,3.6,4.5,4.8};
|
|---|
| 1349 |
|
|---|
| 1350 | // data for iHadron=1
|
|---|
| 1351 | static const G4double EnP[2]={1.5,4.0};
|
|---|
| 1352 | static const G4double C0P[2]={0.001,0.0005};
|
|---|
| 1353 | static const G4double C1P[2]={0.003,0.001};
|
|---|
| 1354 | static const G4double B0P[2]={2.5,4.5};
|
|---|
| 1355 | static const G4double B1P[2]={1.0,4.0};
|
|---|
| 1356 |
|
|---|
| 1357 | // data for iHadron=2
|
|---|
| 1358 | static const G4double EnPP[4]={1.0,2.0,3.0,4.0};
|
|---|
| 1359 | static const G4double C0PP[4]={0.0,0.0,0.0,0.0};
|
|---|
| 1360 | static const G4double C1PP[4]={0.15,0.08,0.02,0.01};
|
|---|
| 1361 | static const G4double B0PP[4]={1.5,2.8,3.8,3.8};
|
|---|
| 1362 | static const G4double B1PP[4]={0.8,1.6,3.6,4.6};
|
|---|
| 1363 |
|
|---|
| 1364 | // data for iHadron=3
|
|---|
| 1365 | static const G4double EnPPN[4]={1.0,2.0,3.0,4.0};
|
|---|
| 1366 | static const G4double C0PPN[4]={0.0,0.0,0.0,0.0};
|
|---|
| 1367 | static const G4double C1PPN[4]={0.0,0.0,0.0,0.0};
|
|---|
| 1368 | static const G4double B0PPN[4]={1.5,2.8,3.8,3.8};
|
|---|
| 1369 | static const G4double B1PPN[4]={0.8,1.6,3.6,4.6};
|
|---|
| 1370 |
|
|---|
| 1371 | // data for iHadron=4
|
|---|
| 1372 | static const G4double EnK[4]={1.4,2.33,3.0,5.0};
|
|---|
| 1373 | static const G4double C0K[4]={0.0,0.0,0.0,0.0};
|
|---|
| 1374 | static const G4double C1K[4]={0.01,0.007,0.005,0.003};
|
|---|
| 1375 | static const G4double B0K[4]={1.5,2.0,3.8,3.8};
|
|---|
| 1376 | static const G4double B1K[4]={1.6,1.6,1.6,1.6};
|
|---|
| 1377 |
|
|---|
| 1378 | // data for iHadron=5
|
|---|
| 1379 | static const G4double EnKM[2]={1.4,4.0};
|
|---|
| 1380 | static const G4double C0KM[2]={0.006,0.002};
|
|---|
| 1381 | static const G4double C1KM[2]={0.00,0.00};
|
|---|
| 1382 | static const G4double B0KM[2]={2.5,3.5};
|
|---|
| 1383 | static const G4double B1KM[2]={1.6,1.6};
|
|---|
| 1384 |
|
|---|
| 1385 | switch(iHadron)
|
|---|
| 1386 | {
|
|---|
| 1387 | case 0 :
|
|---|
| 1388 |
|
|---|
| 1389 | if(hLabMomentum <BoundaryP[0])
|
|---|
| 1390 | InterpolateHN(6,EnP0,C0P0,C1P0,B0P0,B1P0);
|
|---|
| 1391 |
|
|---|
| 1392 | Coeff2 = 0.8/hLabMomentum/hLabMomentum;
|
|---|
| 1393 | break;
|
|---|
| 1394 |
|
|---|
| 1395 | case 6 :
|
|---|
| 1396 |
|
|---|
| 1397 | if(hLabMomentum < BoundaryP[1])
|
|---|
| 1398 | InterpolateHN(5,EnN,C0N,C1N,B0N,B1N);
|
|---|
| 1399 |
|
|---|
| 1400 | Coeff2 = 0.8/hLabMomentum/hLabMomentum;
|
|---|
| 1401 | break;
|
|---|
| 1402 |
|
|---|
| 1403 | case 1 :
|
|---|
| 1404 | case 7 :
|
|---|
| 1405 | if(hLabMomentum < BoundaryP[2])
|
|---|
| 1406 | InterpolateHN(2,EnP,C0P,C1P,B0P,B1P);
|
|---|
| 1407 | break;
|
|---|
| 1408 |
|
|---|
| 1409 | case 2 :
|
|---|
| 1410 |
|
|---|
| 1411 | if(hLabMomentum < BoundaryP[3])
|
|---|
| 1412 | InterpolateHN(4,EnPP,C0PP,C1PP,B0PP,B1PP);
|
|---|
| 1413 |
|
|---|
| 1414 | Coeff2 = 0.02/hLabMomentum;
|
|---|
| 1415 | break;
|
|---|
| 1416 |
|
|---|
| 1417 | case 3 :
|
|---|
| 1418 |
|
|---|
| 1419 | if(hLabMomentum < BoundaryP[4])
|
|---|
| 1420 | InterpolateHN(4,EnPPN,C0PPN,C1PPN,B0PPN,B1PPN);
|
|---|
| 1421 |
|
|---|
| 1422 | Coeff2 = 0.02/hLabMomentum;
|
|---|
| 1423 | break;
|
|---|
| 1424 |
|
|---|
| 1425 | case 4 :
|
|---|
| 1426 |
|
|---|
| 1427 | if(hLabMomentum < BoundaryP[5])
|
|---|
| 1428 | InterpolateHN(4,EnK,C0K,C1K,B0K,B1K);
|
|---|
| 1429 |
|
|---|
| 1430 | if(hLabMomentum < 1) Coeff2 = 0.34;
|
|---|
| 1431 | else Coeff2 = 0.34/hLabMomentum2/hLabMomentum;
|
|---|
| 1432 | break;
|
|---|
| 1433 |
|
|---|
| 1434 | case 5 :
|
|---|
| 1435 | if(hLabMomentum < BoundaryP[6])
|
|---|
| 1436 | InterpolateHN(2,EnKM,C0KM,C1KM,B0KM,B1KM);
|
|---|
| 1437 |
|
|---|
| 1438 | if(hLabMomentum < 1) Coeff2 = 0.01;
|
|---|
| 1439 | else Coeff2 = 0.01/hLabMomentum2/hLabMomentum;
|
|---|
| 1440 | break;
|
|---|
| 1441 | }
|
|---|
| 1442 |
|
|---|
| 1443 | if(verboseLevel > 2)
|
|---|
| 1444 | G4cout<<" HadrVal : Plasb "<<hLabMomentum
|
|---|
| 1445 | <<" iHadron "<<iHadron<<" HadrTot "<<HadrTot<<G4endl;
|
|---|
| 1446 | }
|
|---|
| 1447 |
|
|---|
| 1448 | // =====================================================
|
|---|
| 1449 | void G4ElasticHadrNucleusHE::
|
|---|
| 1450 | GetKinematics(const G4ParticleDefinition * aHadron,
|
|---|
| 1451 | G4double MomentumH)
|
|---|
| 1452 | {
|
|---|
| 1453 | if (verboseLevel>1)
|
|---|
| 1454 | G4cout<<"1 GetKin.: HadronName MomentumH "
|
|---|
| 1455 | <<aHadron->GetParticleName()<<" "<<MomentumH<<G4endl;
|
|---|
| 1456 |
|
|---|
| 1457 | DefineHadronValues(1);
|
|---|
| 1458 |
|
|---|
| 1459 | G4double Sh = 2.0*protonM*HadrEnergy+protonM2+hMass2; // GeV
|
|---|
| 1460 |
|
|---|
| 1461 | ConstU = 2*protonM2+2*hMass2-Sh;
|
|---|
| 1462 |
|
|---|
| 1463 | G4double MaxT = 4*MomentumCM*MomentumCM;
|
|---|
| 1464 |
|
|---|
| 1465 | BoundaryTL[0] = MaxT; //2.0;
|
|---|
| 1466 | BoundaryTL[1] = MaxT;
|
|---|
| 1467 | BoundaryTL[3] = MaxT;
|
|---|
| 1468 | BoundaryTL[4] = MaxT;
|
|---|
| 1469 | BoundaryTL[5] = MaxT;
|
|---|
| 1470 |
|
|---|
| 1471 | G4int NumberH=0;
|
|---|
| 1472 |
|
|---|
| 1473 | while(iHadrCode!=HadronCode[NumberH]) NumberH++;
|
|---|
| 1474 |
|
|---|
| 1475 | NumberH = HadronType1[NumberH];
|
|---|
| 1476 |
|
|---|
| 1477 | if(MomentumH<BoundaryP[NumberH]) MaxTR = BoundaryTL[NumberH];
|
|---|
| 1478 | else MaxTR = BoundaryTG[NumberH];
|
|---|
| 1479 |
|
|---|
| 1480 | if (verboseLevel>1)
|
|---|
| 1481 | G4cout<<"3 GetKin. : NumberH "<<NumberH
|
|---|
| 1482 | <<" Bound.P[NumberH] "<<BoundaryP[NumberH]
|
|---|
| 1483 | <<" Bound.TL[NumberH] "<<BoundaryTL[NumberH]
|
|---|
| 1484 | <<" Bound.TG[NumberH] "<<BoundaryTG[NumberH]
|
|---|
| 1485 | <<" MaxT MaxTR "<<MaxT<<" "<<MaxTR<<G4endl;
|
|---|
| 1486 |
|
|---|
| 1487 | // GetParametersHP(aHadron, MomentumH);
|
|---|
| 1488 | }
|
|---|
| 1489 | // ============================================================
|
|---|
| 1490 | G4double G4ElasticHadrNucleusHE::GetFt(G4double Q2)
|
|---|
| 1491 | {
|
|---|
| 1492 | G4double Fdistr=0;
|
|---|
| 1493 | G4double SqrQ2 = std::sqrt(Q2);
|
|---|
| 1494 |
|
|---|
| 1495 | Fdistr = (1-Coeff1-Coeff0) //-0.0*Coeff2*std::exp(ConstU))
|
|---|
| 1496 | /HadrSlope*(1-std::exp(-HadrSlope*Q2))
|
|---|
| 1497 | + Coeff0*(1-std::exp(-Slope0*Q2))
|
|---|
| 1498 | + Coeff2/Slope2*std::exp(Slope2*ConstU)*(std::exp(Slope2*Q2)-1)
|
|---|
| 1499 | + 2*Coeff1/Slope1*(1/Slope1-(1/Slope1+SqrQ2)*std::exp(-Slope1*SqrQ2));
|
|---|
| 1500 |
|
|---|
| 1501 | if (verboseLevel>1)
|
|---|
| 1502 | G4cout<<"Old: Coeff0 Coeff1 Coeff2 "<<Coeff0<<" "
|
|---|
| 1503 | <<Coeff1<<" "<<Coeff2<<" Slope Slope0 Slope1 Slope2 "
|
|---|
| 1504 | <<HadrSlope<<" "<<Slope0<<" "<<Slope1<<" "<<Slope2
|
|---|
| 1505 | <<" Fdistr "<<Fdistr<<G4endl;
|
|---|
| 1506 | return Fdistr;
|
|---|
| 1507 | }
|
|---|
| 1508 | // +++++++++++++++++++++++++++++++++++++++
|
|---|
| 1509 | G4double G4ElasticHadrNucleusHE::GetQ2(G4double Ran)
|
|---|
| 1510 | {
|
|---|
| 1511 | G4double DDD0=MaxTR*0.5, DDD1=0.0, DDD2=MaxTR, delta;
|
|---|
| 1512 | G4double Q2=0;
|
|---|
| 1513 |
|
|---|
| 1514 | FmaxT = GetFt(MaxTR);
|
|---|
| 1515 | delta = GetDistrFun(DDD0)-Ran;
|
|---|
| 1516 |
|
|---|
| 1517 | while(std::fabs(delta) > 0.0001)
|
|---|
| 1518 | {
|
|---|
| 1519 | if(delta>0)
|
|---|
| 1520 | {
|
|---|
| 1521 | DDD2 = DDD0;
|
|---|
| 1522 | DDD0 = (DDD0+DDD1)*0.5;
|
|---|
| 1523 | }
|
|---|
| 1524 | else if(delta<0)
|
|---|
| 1525 | {
|
|---|
| 1526 | DDD1 = DDD0;
|
|---|
| 1527 | DDD0 = (DDD0+DDD2)*0.5;
|
|---|
| 1528 | }
|
|---|
| 1529 | delta = GetDistrFun(DDD0)-Ran;
|
|---|
| 1530 | }
|
|---|
| 1531 |
|
|---|
| 1532 | Q2 = DDD0;
|
|---|
| 1533 |
|
|---|
| 1534 | return Q2;
|
|---|
| 1535 | }
|
|---|
| 1536 | // ++++++++++++++++++++++++++++++++++++++++++
|
|---|
| 1537 | G4double G4ElasticHadrNucleusHE::
|
|---|
| 1538 | HadronProtonQ2(const G4ParticleDefinition * p,
|
|---|
| 1539 | G4double inLabMom)
|
|---|
| 1540 | {
|
|---|
| 1541 |
|
|---|
| 1542 | hMass = p->GetPDGMass()/GeV;
|
|---|
| 1543 | hMass2 = hMass*hMass;
|
|---|
| 1544 | hLabMomentum = inLabMom;
|
|---|
| 1545 | hLabMomentum2 = hLabMomentum*hLabMomentum;
|
|---|
| 1546 | HadrEnergy = sqrt(hLabMomentum2+hMass2);
|
|---|
| 1547 |
|
|---|
| 1548 | G4double Rand = G4UniformRand();
|
|---|
| 1549 |
|
|---|
| 1550 | GetKinematics(p, inLabMom);
|
|---|
| 1551 |
|
|---|
| 1552 | G4double Q2 = GetQ2(Rand);
|
|---|
| 1553 |
|
|---|
| 1554 | return Q2;
|
|---|
| 1555 | }
|
|---|
| 1556 |
|
|---|
| 1557 | // ===========================================
|
|---|
| 1558 |
|
|---|
| 1559 | ///////////////////////////////////////////////////////////////////
|
|---|
| 1560 | //
|
|---|
| 1561 | //
|
|---|
| 1562 |
|
|---|
| 1563 | void G4ElasticHadrNucleusHE::Binom()
|
|---|
| 1564 | {
|
|---|
| 1565 | G4int N, M;
|
|---|
| 1566 | G4double Fact1, J;
|
|---|
| 1567 |
|
|---|
| 1568 | for(N = 0; N < 240; N++)
|
|---|
| 1569 | {
|
|---|
| 1570 | J = 1;
|
|---|
| 1571 |
|
|---|
| 1572 | for( M = 0; M <= N; M++ )
|
|---|
| 1573 | {
|
|---|
| 1574 | Fact1 = 1;
|
|---|
| 1575 |
|
|---|
| 1576 | if ( ( N > 0 ) && ( N > M ) && M > 0 )
|
|---|
| 1577 | {
|
|---|
| 1578 | J *= G4double(N-M+1)/G4double(M);
|
|---|
| 1579 | Fact1 = J;
|
|---|
| 1580 | }
|
|---|
| 1581 | SetBinom[N][M] = Fact1;
|
|---|
| 1582 | }
|
|---|
| 1583 | }
|
|---|
| 1584 | return;
|
|---|
| 1585 | }
|
|---|
| 1586 |
|
|---|
| 1587 |
|
|---|
| 1588 | //
|
|---|
| 1589 | //
|
|---|
| 1590 | ///////////////////////////////////////////////////////////
|
|---|
| 1591 |
|
|---|