| [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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| 27 | // $Id: G4NucleiPropertiesTheoreticalTableA.cc,v 1.8 2006/06/29 19:25:46 gunter Exp $
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| [1196] | 28 | // GEANT4 tag $Name: geant4-09-03-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 implementation file
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| 33 | //
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| 34 | // ------------------------------------------------------------
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| 35 | // Remove "theInstance" by H.Kurashige (12 Dec. 03)
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| 36 |
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| 37 | #include "G4NucleiPropertiesTheoreticalTable.hh"
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| 38 |
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| 39 | // Determine the table index for a Nuclide with Z protons and A nucleons
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| 40 | G4int G4NucleiPropertiesTheoreticalTable::GetIndex(G4int Z, G4int A)
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| 41 | {
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| 42 |
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| 43 | if(A>339) {
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| 44 | G4Exception("G4NucleiPropertiesTheoreticalTable::GetIndex",
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| 45 | "Illegal arguemnt",
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| 46 | EventMustBeAborted,"Nucleon number larger than 339!");
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| 47 | } else if(A<16) {
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| 48 | G4Exception("G4NucleiPropertiesTheoreticalTable::GetIndex",
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| 49 | "Illegal arguemnt",
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| 50 | EventMustBeAborted," Nucleon number smaller than 16!");
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| 51 | } else if(Z>136) {
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| 52 | G4Exception("G4NucleiPropertiesTheoreticalTable::GetIndex",
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| 53 | "Illegal arguemnt",
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| 54 | EventMustBeAborted, "Proton number larger than 136!");
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| 55 | } else if(Z<8) {
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| 56 | G4Exception("G4NucleiPropertiesTheoreticalTable::GetIndex",
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| 57 | "Illegal arguemnt",
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| 58 | EventMustBeAborted, "Proton number smaller than 8!");
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| 59 | } else if(Z>A) {
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| 60 | G4Exception("G4NucleiPropertiesTheoreticalTable::GetIndex",
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| 61 | "Illegal arguemnt",
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| 62 | EventMustBeAborted, "Nucleon number smaller than Z!");
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| 63 | }
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| 64 |
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| 65 | G4int i = shortTable[Z-8];
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| 66 | while ( i < shortTable[Z-8+1] ) {
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| 67 | if (indexArray[1][i] != A ) i++;
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| 68 | else return i;
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| 69 | }
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| 70 |
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| 71 | return -1;
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| 72 | }
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| 73 |
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| 74 |
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| 75 |
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| 76 | G4double G4NucleiPropertiesTheoreticalTable::GetMassExcess(G4int Z, G4int A)
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| 77 | {
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| 78 | G4int i=GetIndex(Z, A);
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| 79 | if (i >= 0) {
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| 80 | return AtomicMassExcess[i]*MeV;
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| 81 | } else {
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| 82 | return 0.0;
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| 83 | }
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| 84 | }
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| 85 |
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| 86 | G4double G4NucleiPropertiesTheoreticalTable::GetBindingEnergy(G4int Z, G4int A)
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| 87 | {
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| 88 | G4int i=GetIndex(Z, A);
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| 89 | if (i >= 0){
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| 90 | const G4double Mh = 7.289034*MeV; // hydrogen atom mass excess
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| 91 | const G4double Mn = 8.071431*MeV; // neutron mass excess
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| 92 | return G4double(Z)*Mh + G4double(A-Z)*Mn - AtomicMassExcess[i]*MeV;
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| 93 | } else {
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| 94 | return 0.0;
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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 | G4double G4NucleiPropertiesTheoreticalTable::GetAtomicMass(G4int Z, G4int A)
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| 101 | {
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| 102 | G4int i=GetIndex(Z, A);
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| 103 | if (i >= 0) {
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| 104 | return AtomicMassExcess[i]*MeV + A*amu_c2;
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| 105 | } else {
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| 106 | return 0.0;
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| 107 | }
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| 108 | }
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| 109 |
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| 110 |
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| 111 |
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| 112 | G4double G4NucleiPropertiesTheoreticalTable::GetNuclearMass(G4int Z, G4int A)
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| 113 | {
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| 114 | G4int i=GetIndex(Z, A);
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| 115 | if (i >= 0) {
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| 116 | return GetAtomicMass(Z,A) - G4double(Z)*electron_mass_c2 + ElectronicBindingEnergy(Z);
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| 117 | } else {
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| 118 | return 0.0;
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| 119 | }
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| 120 | }
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| 121 |
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| 122 | G4double G4NucleiPropertiesTheoreticalTable::ElectronicBindingEnergy(G4int Z) {
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| 123 | const G4double ael = 1.433e-5*MeV; // electronic-binding constant
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| 124 | return ael*std::pow(G4double(Z),2.39);
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| 125 | }
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| 126 |
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| 127 | G4bool G4NucleiPropertiesTheoreticalTable::IsInTable(G4int Z, G4int A)
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| 128 | {
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| 129 | return (Z <= A && A >= 16 && A <= 339 && Z <= 136 && Z >= 8 && GetIndex(Z, A) >= 0);
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| 130 | }
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| 131 |
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| 132 |
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| 133 |
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| 134 |
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| 135 |
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| 136 |
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| 137 |
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| 138 |
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