| [819] | 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 | // $Id: G4AblaDataDefs.hh,v 1.6 2007/12/03 19:36:06 miheikki Exp $
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| 27 | // Translation of INCL4.2/ABLA V3
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| 28 | // Pekka Kaitaniemi, HIP (translation)
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| 29 | // Christelle Schmidt, IPNL (fission code)
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| 30 | // Alain Boudard, CEA (contact person INCL/ABLA)
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| 31 | // Aatos Heikkinen, HIP (project coordination)
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| 32 |
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| 33 | // Data structures needed by ABLA evaporation code.
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| 34 |
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| 35 | #ifndef G4AblaDataDefs_hh
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| 36 | #define G4AblaDataDefs_hh 1
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| 37 |
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| 38 | // ABLA
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| 39 |
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| 40 | class G4Nevent {
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| 41 | public:
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| 42 | G4Nevent() {};
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| 43 | ~G4Nevent() {};
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| 44 |
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| 45 | G4int ii;
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| 46 | };
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| 47 |
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| 48 | // ABLA
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| 49 | #define PACESIZEROWS 500
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| 50 | #define PACESIZECOLS 500
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| 51 | /**
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| 52 | * Masses.
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| 53 | */
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| 54 |
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| 55 | class G4Pace {
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| 56 |
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| 57 | public:
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| 58 | G4Pace() {};
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| 59 |
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| 60 | ~G4Pace() {};
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| 61 |
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| 62 | G4double dm[PACESIZEROWS][PACESIZECOLS];
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| 63 | };
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| 64 |
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| 65 | #define EC2SUBROWS 154
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| 66 | #define EC2SUBCOLS 99
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| 67 | /**
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| 68 | *
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| 69 | */
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| 70 |
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| 71 | class G4Ec2sub {
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| 72 | public:
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| 73 | G4Ec2sub() {};
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| 74 |
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| 75 | ~G4Ec2sub() {};
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| 76 |
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| 77 | G4double ecnz[EC2SUBROWS][EC2SUBCOLS];
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| 78 | };
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| 79 |
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| 80 | class G4Ald {
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| 81 | public:
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| 82 | /**
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| 83 | *
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| 84 | */
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| 85 | G4Ald() {};
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| 86 | ~G4Ald() {};
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| 87 |
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| 88 | G4double av,as,ak,optafan;
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| 89 | };
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| 90 |
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| 91 | class G4Ablamain {
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| 92 | public:
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| 93 | G4Ablamain() {};
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| 94 | ~G4Ablamain() {};
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| 95 |
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| 96 | G4double ap,zp,at,zt,eap,beta,bmaxnuc,crtot,crnuc,r_0, r_p,r_t,pi,bfpro,snpro,sppro,shell;
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| 97 | G4int imax, inum;
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| 98 | };
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| 99 |
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| 100 | #define ECLDROWS 154
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| 101 | #define ECLDCOLS 99
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| 102 | /**
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| 103 | * Shell corrections and deformations.
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| 104 | */
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| 105 |
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| 106 | class G4Ecld {
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| 107 |
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| 108 | public:
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| 109 | G4Ecld() {};
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| 110 | ~G4Ecld() {};
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| 111 |
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| 112 | /**
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| 113 | * Ground state shell correction frldm for a spherical ground state.
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| 114 | */
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| 115 | G4double ecgnz[ECLDROWS][ECLDCOLS];
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| 116 |
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| 117 | /**
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| 118 | * Shell correction for the saddle point (now: == 0).
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| 119 | */
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| 120 | G4double ecfnz[ECLDROWS][ECLDCOLS];
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| 121 |
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| 122 | /**
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| 123 | * Difference between deformed ground state and ldm value.
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| 124 | */
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| 125 | G4double vgsld[ECLDROWS][ECLDCOLS];
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| 126 |
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| 127 | /**
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| 128 | * Alpha ground state deformation (this is not beta2!)
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| 129 | * beta2 = std::sqrt(5/(4pi)) * alpha
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| 130 | */
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| 131 | G4double alpha[ECLDROWS][ECLDCOLS];
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| 132 | };
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| 133 |
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| 134 | class G4Fiss {
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| 135 | /**
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| 136 | * Options and parameters for fission channel.
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| 137 | */
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| 138 |
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| 139 | public:
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| 140 | G4Fiss() {};
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| 141 | ~G4Fiss() {};
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| 142 |
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| 143 | G4double akap,bet,homega,koeff,ifis;
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| 144 | G4int optshp, optxfis,optles,optcol;
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| 145 | };
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| 146 |
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| 147 | #define FBROWS 101
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| 148 | #define FBCOLS 161
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| 149 | /**
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| 150 | * Fission barriers.
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| 151 | */
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| 152 |
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| 153 | class G4Fb {
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| 154 |
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| 155 | public:
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| 156 | G4Fb() {};
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| 157 | ~G4Fb() {;}
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| 158 |
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| 159 | // G4double efa[FBROWS][FBCOLS];
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| 160 | G4double efa[FBCOLS][FBROWS];
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| 161 | };
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| 162 |
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| 163 | /**
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| 164 | * Options
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| 165 | */
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| 166 |
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| 167 | class G4Opt {
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| 168 |
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| 169 | public:
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| 170 | G4Opt() {};
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| 171 | ~G4Opt() {};
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| 172 |
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| 173 | G4int optemd,optcha;
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| 174 | G4double eefac;
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| 175 | };
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| 176 |
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| 177 | #define EENUCSIZE 2002
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| 178 | #define XHESIZE 50
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| 179 | class G4Eenuc {
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| 180 | public:
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| 181 | G4Eenuc() {};
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| 182 | ~G4Eenuc() {};
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| 183 |
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| 184 | G4double she[EENUCSIZE],xhe[XHESIZE][EENUCSIZE];
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| 185 | };
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| 186 |
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| 187 | #define EMDPARSIZE 1000
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| 188 | /**
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| 189 | * Energies widths and cross sections for em excitation.
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| 190 | */
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| 191 |
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| 192 | class G4Emdpar {
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| 193 |
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| 194 | public:
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| 195 | G4Emdpar() {};
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| 196 | ~G4Emdpar() {};
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| 197 |
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| 198 | G4double egdr,egqr,fwhmgdr,fwhmgqr,cremde1,cremde2;
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| 199 | G4double ae1[EMDPARSIZE],be1[EMDPARSIZE],ce1[EMDPARSIZE],ae2[EMDPARSIZE];
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| 200 | G4double be2[EMDPARSIZE],ce2[EMDPARSIZE],sre1[EMDPARSIZE],sre2[EMDPARSIZE];
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| 201 | G4double xre1[EMDPARSIZE],xre2[EMDPARSIZE],ds1,ds2;
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| 202 | };
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| 203 |
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| 204 | //#define VOLANTSIZE 200
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| 205 | #define VOLANTSIZE 2000
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| 206 | /**
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| 207 | * Evaporation and fission output data.
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| 208 | */
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| 209 |
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| 210 | class G4Volant {
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| 211 |
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| 212 | public:
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| 213 | G4Volant() {};
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| 214 | ~G4Volant() {};
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| 215 |
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| 216 | void dump()
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| 217 | {
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| 218 | G4cout <<"i \t ACV \t ZPCV \t PCV" << G4endl;
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| 219 | for(G4int i = 0; i <= iv; i++) {
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| 220 | G4cout << "volant" << i << "\t" << acv[i] << " \t " << zpcv[i] << " \t " << pcv[i] << G4endl;
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| 221 | }
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| 222 | }
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| 223 |
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| 224 | G4double acv[VOLANTSIZE],zpcv[VOLANTSIZE],pcv[VOLANTSIZE],xcv[VOLANTSIZE];
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| 225 | G4double ycv[VOLANTSIZE],zcv[VOLANTSIZE];
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| 226 | G4int iv;
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| 227 | };
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| 228 |
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| 229 | #endif
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