[824] | 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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[1315] | 27 | // $Id: G4NucleiProperties.cc,v 1.22 2010/05/20 01:01:07 kurasige Exp $ |
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| 28 | // GEANT4 tag $Name: geant4-09-04-beta-cand-01 $ |
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[824] | 29 | // |
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| 30 | // |
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| 31 | // ------------------------------------------------------------ |
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| 32 | // GEANT 4 class header file |
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| 33 | // |
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| 34 | // ------------------------------------------------------------ |
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| 35 | // |
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| 36 | // Hadronic Process: Nuclear De-excitations |
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| 37 | // by V. Lara (Oct 1998) |
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| 38 | // Migrate into particles category by H.Kurashige (17 Nov. 98) |
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| 39 | // Added Shell-Pairing corrections to the Cameron mass |
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| 40 | // excess formula by V.Lara (9 May 99) |
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[1196] | 41 | // 090331 Migrate to AME03 by Koi, Tatsumi |
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[824] | 42 | |
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| 43 | #include "G4NucleiProperties.hh" |
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| 44 | |
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| 45 | |
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[890] | 46 | G4double G4NucleiProperties::mass_proton = -1.; |
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| 47 | G4double G4NucleiProperties::mass_neutron = -1.; |
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| 48 | G4double G4NucleiProperties::mass_deuteron = -1.; |
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| 49 | G4double G4NucleiProperties::mass_triton = -1.; |
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| 50 | G4double G4NucleiProperties::mass_alpha = -1.; |
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| 51 | G4double G4NucleiProperties::mass_He3 = -1.; |
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[824] | 52 | |
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[1196] | 53 | G4double G4NucleiProperties::GetNuclearMass(const G4double A, const G4double Z) |
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[824] | 54 | { |
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[1196] | 55 | G4double mass=0.0; |
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[824] | 56 | |
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[1196] | 57 | if (std::fabs(A - G4int(A)) > 1.e-10) { |
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| 58 | mass = NuclearMass(A,Z); |
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| 59 | |
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| 60 | } else { |
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| 61 | // use mass table |
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| 62 | G4int iZ = G4int(Z); |
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| 63 | G4int iA = G4int(A); |
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| 64 | mass =GetNuclearMass(iA,iZ); |
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| 65 | } |
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| 66 | |
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| 67 | return mass; |
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[824] | 68 | } |
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| 69 | |
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[1315] | 70 | |
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[1196] | 71 | G4double G4NucleiProperties::GetNuclearMass(const G4int A, const G4int Z) |
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[824] | 72 | { |
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[1196] | 73 | if (mass_proton <= 0.0 ) { |
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[890] | 74 | G4ParticleDefinition * nucleus = 0; |
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| 75 | nucleus = G4ParticleTable::GetParticleTable()->FindParticle("proton"); // proton |
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| 76 | if (nucleus!=0) mass_proton = nucleus->GetPDGMass(); |
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| 77 | nucleus = G4ParticleTable::GetParticleTable()->FindParticle("neutron"); // neutron |
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| 78 | if (nucleus!=0) mass_neutron = nucleus->GetPDGMass(); |
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| 79 | nucleus = G4ParticleTable::GetParticleTable()->FindParticle("deuteron"); // deuteron |
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| 80 | if (nucleus!=0) mass_deuteron = nucleus->GetPDGMass(); |
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| 81 | nucleus = G4ParticleTable::GetParticleTable()->FindParticle("triton"); // triton |
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| 82 | if (nucleus!=0) mass_triton = nucleus->GetPDGMass(); |
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| 83 | nucleus = G4ParticleTable::GetParticleTable()->FindParticle("alpha"); // alpha |
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| 84 | if (nucleus!=0) mass_alpha = nucleus->GetPDGMass(); |
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| 85 | nucleus = G4ParticleTable::GetParticleTable()->FindParticle("He3"); // He3 |
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| 86 | if (nucleus!=0) mass_He3 = nucleus->GetPDGMass(); |
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| 87 | |
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| 88 | } |
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| 89 | |
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[824] | 90 | if (A < 1 || Z < 0 || Z > A) { |
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| 91 | #ifdef G4VERBOSE |
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| 92 | if (G4ParticleTable::GetParticleTable()->GetVerboseLevel()>0) { |
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[1315] | 93 | G4cerr << "G4NucleiProperties::GetNuclearMass: Wrong values for A = " << A |
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[824] | 94 | << " and Z = " << Z << G4endl; |
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| 95 | } |
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| 96 | #endif |
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| 97 | return 0.0; |
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[1196] | 98 | } |
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| 99 | |
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| 100 | G4double mass= -1.; |
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| 101 | if ( (Z<=2) ) { |
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| 102 | // light nuclei |
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| 103 | if ( (Z==1)&&(A==1) ) { |
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| 104 | mass = mass_proton; |
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| 105 | } else if ( (Z==0)&&(A==1) ) { |
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| 106 | mass = mass_neutron; |
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| 107 | } else if ( (Z==1)&&(A==2) ) { |
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| 108 | mass = mass_deuteron; |
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| 109 | } else if ( (Z==1)&&(A==3) ) { |
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| 110 | mass = mass_triton; |
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| 111 | } else if ( (Z==2)&&(A==4) ) { |
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| 112 | mass = mass_alpha; |
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| 113 | } else if ( (Z==2)&&(A==3) ) { |
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| 114 | mass = mass_He3; |
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[824] | 115 | } |
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[1196] | 116 | } |
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| 117 | |
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| 118 | if (mass < 0.) { |
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| 119 | if (G4NucleiPropertiesTableAME03::IsInTable(Z,A)) { |
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| 120 | // AME 03 table |
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| 121 | mass = G4NucleiPropertiesTableAME03::GetNuclearMass(Z,A); |
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| 122 | } else if (G4NucleiPropertiesTheoreticalTable::IsInTable(Z,A)){ |
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| 123 | // Theoretical table |
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| 124 | mass = G4NucleiPropertiesTheoreticalTable::GetNuclearMass(Z,A); |
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| 125 | } else { |
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| 126 | mass = NuclearMass(G4double(A),G4double(Z)); |
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[824] | 127 | } |
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| 128 | } |
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[1196] | 129 | |
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| 130 | if (mass < 0.) mass = 0.0; |
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| 131 | return mass; |
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[824] | 132 | } |
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| 133 | |
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[890] | 134 | G4bool G4NucleiProperties::IsInStableTable(const G4double A, const G4double Z) |
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| 135 | { |
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[1196] | 136 | G4int iA = G4int(A); |
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| 137 | G4int iZ = G4int(Z); |
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| 138 | return IsInStableTable(iA, iZ); |
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| 139 | } |
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| 140 | |
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| 141 | G4bool G4NucleiProperties::IsInStableTable(const G4int A, const int Z) |
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| 142 | { |
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| 143 | if (A < 1 || Z < 0 || Z > A) { |
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[890] | 144 | #ifdef G4VERBOSE |
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| 145 | if (G4ParticleTable::GetParticleTable()->GetVerboseLevel()>0) { |
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[1315] | 146 | G4cerr << "G4NucleiProperties::IsInStableTable: Wrong values for A = " |
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[890] | 147 | << A << " and Z = " << Z << G4endl; |
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| 148 | } |
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| 149 | #endif |
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| 150 | return false; |
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[1196] | 151 | } |
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[824] | 152 | |
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[1196] | 153 | return G4NucleiPropertiesTableAME03::IsInTable(Z,A); |
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| 154 | |
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[890] | 155 | } |
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[824] | 156 | |
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[890] | 157 | G4double G4NucleiProperties::GetMassExcess(const G4double A, const G4double Z) |
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| 158 | { |
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| 159 | G4int iA = G4int(A); |
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| 160 | G4int iZ = G4int(Z); |
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| 161 | return GetMassExcess(iA,iZ); |
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| 162 | } |
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[824] | 163 | |
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| 164 | G4double G4NucleiProperties::GetMassExcess(const G4int A, const G4int Z) |
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| 165 | { |
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| 166 | if (A < 1 || Z < 0 || Z > A) { |
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| 167 | #ifdef G4VERBOSE |
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| 168 | if (G4ParticleTable::GetParticleTable()->GetVerboseLevel()>0) { |
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[1315] | 169 | G4cerr << "G4NucleiProperties::GetMassExccess: Wrong values for A = " |
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[824] | 170 | << A << " and Z = " << Z << G4endl; |
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| 171 | } |
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| 172 | #endif |
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| 173 | return 0.0; |
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| 174 | |
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| 175 | } else { |
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| 176 | |
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[1196] | 177 | if (G4NucleiPropertiesTableAME03::IsInTable(Z,A)){ |
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| 178 | return G4NucleiPropertiesTableAME03::GetMassExcess(Z,A); |
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[824] | 179 | } else if (G4NucleiPropertiesTheoreticalTable::IsInTable(Z,A)){ |
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| 180 | return G4NucleiPropertiesTheoreticalTable::GetMassExcess(Z,A); |
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| 181 | } else { |
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| 182 | return MassExcess(A,Z); |
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| 183 | } |
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| 184 | } |
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| 185 | |
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| 186 | } |
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| 187 | |
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| 188 | |
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| 189 | G4double G4NucleiProperties::GetAtomicMass(const G4double A, const G4double Z) |
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| 190 | { |
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[1196] | 191 | if (A < 1 || Z < 0 || Z > A) { |
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[824] | 192 | #ifdef G4VERBOSE |
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| 193 | if (G4ParticleTable::GetParticleTable()->GetVerboseLevel()>0) { |
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[1315] | 194 | G4cerr << "G4NucleiProperties::GetAtomicMass: Wrong values for A = " |
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[824] | 195 | << A << " and Z = " << Z << G4endl; |
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| 196 | } |
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| 197 | #endif |
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| 198 | return 0.0; |
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| 199 | |
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[1196] | 200 | } else if (std::fabs(A - G4int(A)) > 1.e-10) { |
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[824] | 201 | return AtomicMass(A,Z); |
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| 202 | |
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| 203 | } else { |
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| 204 | G4int iA = G4int(A); |
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| 205 | G4int iZ = G4int(Z); |
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[1196] | 206 | if (G4NucleiPropertiesTableAME03::IsInTable(iZ,iA)) { |
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| 207 | return G4NucleiPropertiesTableAME03::GetAtomicMass(iZ,iA); |
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[824] | 208 | } else if (G4NucleiPropertiesTheoreticalTable::IsInTable(iZ,iA)){ |
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| 209 | return G4NucleiPropertiesTheoreticalTable::GetAtomicMass(iZ,iA); |
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| 210 | } else { |
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| 211 | return AtomicMass(A,Z); |
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| 212 | } |
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| 213 | } |
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| 214 | } |
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| 215 | |
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[890] | 216 | G4double G4NucleiProperties::GetBindingEnergy(const G4double A, const G4double Z) |
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| 217 | { |
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| 218 | G4int iA = G4int(A); |
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| 219 | G4int iZ = G4int(Z); |
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| 220 | return GetBindingEnergy(iA,iZ); |
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| 221 | } |
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| 222 | |
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[824] | 223 | G4double G4NucleiProperties::GetBindingEnergy(const G4int A, const G4int Z) |
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| 224 | { |
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| 225 | if (A < 1 || Z < 0 || Z > A) { |
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| 226 | #ifdef G4VERBOSE |
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| 227 | if (G4ParticleTable::GetParticleTable()->GetVerboseLevel()>0) { |
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[1315] | 228 | G4cerr << "G4NucleiProperties::GetMassExccess: Wrong values for A = " |
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[824] | 229 | << A << " and Z = " << Z << G4endl; |
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| 230 | } |
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| 231 | #endif |
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| 232 | return 0.0; |
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| 233 | |
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| 234 | } else { |
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[1196] | 235 | if (G4NucleiPropertiesTableAME03::IsInTable(Z,A)) { |
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| 236 | return G4NucleiPropertiesTableAME03::GetBindingEnergy(Z,A); |
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[824] | 237 | } else if (G4NucleiPropertiesTheoreticalTable::IsInTable(Z,A)) { |
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| 238 | return G4NucleiPropertiesTheoreticalTable::GetBindingEnergy(Z,A); |
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| 239 | }else { |
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| 240 | return BindingEnergy(A,Z); |
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| 241 | } |
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| 242 | |
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| 243 | } |
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| 244 | } |
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| 245 | |
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| 246 | |
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| 247 | G4double G4NucleiProperties::MassExcess(G4double A, G4double Z) |
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| 248 | { |
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| 249 | return GetAtomicMass(A,Z) - A*amu_c2; |
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| 250 | } |
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[1196] | 251 | |
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| 252 | G4double G4NucleiProperties::AtomicMass(G4double A, G4double Z) |
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| 253 | { |
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| 254 | const G4double hydrogen_mass_excess = G4NucleiPropertiesTableAME03::GetMassExcess(1,1); |
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| 255 | const G4double neutron_mass_excess = G4NucleiPropertiesTableAME03::GetMassExcess(0,1); |
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| 256 | |
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| 257 | G4double mass = |
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| 258 | (A-Z)*neutron_mass_excess + Z*hydrogen_mass_excess - BindingEnergy(A,Z) + A*amu_c2; |
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| 259 | |
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| 260 | return mass; |
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| 261 | } |
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| 262 | |
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| 263 | G4double G4NucleiProperties::NuclearMass(G4double A, G4double Z) |
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| 264 | { |
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| 265 | if (A < 1 || Z < 0 || Z > A) { |
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| 266 | #ifdef G4VERBOSE |
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| 267 | if (G4ParticleTable::GetParticleTable()->GetVerboseLevel()>0) { |
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[1315] | 268 | G4cerr << "G4NucleiProperties::NuclearMass: Wrong values for A = " |
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[1196] | 269 | << A << " and Z = " << Z << G4endl; |
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| 270 | } |
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| 271 | #endif |
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| 272 | return 0.0; |
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| 273 | } |
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| 274 | |
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| 275 | G4double mass = AtomicMass(A,Z); |
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| 276 | // atomic mass is converted to nuclear mass according formula in AME03 |
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| 277 | mass -= Z*electron_mass_c2; |
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| 278 | mass += ( 14.4381*std::pow ( Z , 2.39 ) + 1.55468*1e-6*std::pow ( Z , 5.35 ) )*eV; |
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| 279 | |
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| 280 | return mass; |
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| 281 | } |
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| 282 | |
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| 283 | G4double G4NucleiProperties::BindingEnergy(G4double A, G4double Z) |
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| 284 | { |
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| 285 | // |
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| 286 | // Weitzsaecker's Mass formula |
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| 287 | // |
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| 288 | G4int Npairing = G4int(A-Z)%2; // pairing |
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| 289 | G4int Zpairing = G4int(Z)%2; |
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| 290 | G4double binding = |
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| 291 | - 15.67*A // nuclear volume |
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| 292 | + 17.23*std::pow(A,2./3.) // surface energy |
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| 293 | + 93.15*((A/2.-Z)*(A/2.-Z))/A // asymmetry |
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| 294 | + 0.6984523*Z*Z*std::pow(A,-1./3.); // coulomb |
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| 295 | if( Npairing == Zpairing ) binding += (Npairing+Zpairing-1) * 12.0 / std::sqrt(A); // pairing |
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| 296 | |
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| 297 | return -binding*MeV; |
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| 298 | } |
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| 299 | |
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