| 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: G4Abla.hh,v 1.7 2007/12/03 19:36:05 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 | #include "globals.hh"
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| 34 |
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| 35 | #include "G4AblaDataDefs.hh"
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| 36 | #include "G4InclDataDefs.hh"
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| 37 |
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| 38 | /**
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| 39 | * Class containing ABLA de-excitation code.
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| 40 | */
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| 41 |
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| 42 | class G4Abla {
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| 43 |
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| 44 | public:
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| 45 | /**
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| 46 | *
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| 47 | * We support Doxygen with JavaDoc style.
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| 48 | *
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| 49 | * \author{pekka.kaitaniemi@helsinki.fi}
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| 50 | */
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| 51 |
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| 52 | /**
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| 53 | * A constructor.
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| 54 | */
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| 55 | G4Abla();
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| 56 |
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| 57 | /**
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| 58 | * This constructor is used by standalone test driver and the Geant4 interface.
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| 59 | *
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| 60 | * @param aHazard random seeds
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| 61 | * @param aVolant data structure for ABLA output
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| 62 | * @param aVarNtp data structure for transfering ABLA output to Geant4 interface
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| 63 | */
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| 64 | G4Abla(G4Hazard *aHazard, G4Volant *aVolant, G4VarNtp *aVarntp);
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| 65 |
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| 66 | /**
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| 67 | *
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| 68 | */
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| 69 | G4Abla(G4Hazard *hazard, G4Volant *volant);
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| 70 |
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| 71 | /**
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| 72 | * A destructor.
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| 73 | * A more elaborate description of the destructor.
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| 74 | */
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| 75 | ~G4Abla();
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| 76 |
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| 77 | /**
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| 78 | *
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| 79 | */
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| 80 | void setVerboseLevel(G4int level);
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| 81 |
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| 82 | /**
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| 83 | * Main interface to the de-excitation code.
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| 84 | *
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| 85 | * @param nucleusA mass number of the nucleus
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| 86 | * @param nucleusZ charge number of the nucleus
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| 87 | * @param nucleusMass mass of the nucleus
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| 88 | * @param excitationEnergy excitation energy of the nucleus
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| 89 | * @param angularMomentum angular momentum of the nucleus (produced as output by INCL4)
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| 90 | * @param recoilEnergy recoil energy of the nucleus
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| 91 | * @param momX momentum x-component
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| 92 | * @param momY momentum y-component
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| 93 | * @param momZ momentum z-component
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| 94 | * @param eventnumber number of the event
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| 95 | */
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| 96 | void breakItUp(G4double nucleusA, G4double nucleusZ, G4double nucleusMass, G4double excitationEnergy,
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| 97 | G4double angularMomentum, G4double recoilEnergy, G4double momX, G4double momY, G4double momZ,
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| 98 | G4int eventnumber);
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| 99 |
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| 100 | // Evaporation
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| 101 | public:
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| 102 | /**
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| 103 | * Initialize ABLA evaporation code.
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| 104 | */
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| 105 | void initEvapora();
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| 106 |
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| 107 | /**
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| 108 | * qrot including damping
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| 109 | * Input: z,a,bet,sig,u
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| 110 | * Output: qr - collective enhancement factor
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| 111 | * See junghans et al., nucl. phys. a 629 (1998) 635
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| 112 | */
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| 113 | void qrot(G4double z, G4double a, G4double bet, G4double sig, G4double u, G4double *qr);
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| 114 |
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| 115 | /**
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| 116 | * Model de la goutte liquide de c. f. weizsacker.
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| 117 | * usually an obsolete option
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| 118 | */
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| 119 | void mglw(G4double a, G4double z, G4double *el);
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| 120 |
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| 121 | /**
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| 122 | * Mglms
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| 123 | */
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| 124 | void mglms(G4double a, G4double z, G4int refopt4, G4double *el);
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| 125 |
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| 126 | /**
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| 127 | *
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| 128 | */
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| 129 | // G4double spdef(G4int a, G4int z, G4int optxfis);
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| 130 |
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| 131 | /**
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| 132 | * Calculation of fissility parameter
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| 133 | */
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| 134 | // G4double fissility(int a,int z, int optxfis);
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| 135 |
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| 136 | /**
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| 137 | * Main evaporation routine.
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| 138 | */
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| 139 | void evapora(G4double zprf, G4double aprf, G4double ee, G4double jprf,
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| 140 | G4double *zf_par, G4double *af_par, G4double *mtota_par,
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| 141 | G4double *pleva_par, G4double *pxeva_par, G4double *pyeva_par,
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| 142 | G4int *ff_par, G4int *inttype_par, G4int *inum_par);
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| 143 |
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| 144 | /**
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| 145 | * Calculation of particle emission probabilities.
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| 146 | */
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| 147 | void direct(G4double zprf,G4double a, G4double ee, G4double jprf,
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| 148 | G4double *probp_par, G4double *probn_par, G4double *proba_par,
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| 149 | G4double *probf_par, G4double *ptotl_par, G4double *sn_par, G4double *sbp_par, G4double *sba_par, G4double *ecn_par,
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| 150 | G4double *ecp_par,G4double *eca_par, G4double *bp_par, G4double *ba_par, G4int inttype, G4int inum, G4int itest);
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| 151 |
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| 152 | /**
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| 153 | * Level density parameters.
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| 154 | */
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| 155 | void densniv(G4double a, G4double z, G4double ee, G4double esous, G4double *dens, G4double bshell, G4double bs, G4double bk,
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| 156 | G4double *temp, G4int optshp, G4int optcol, G4double defbet);
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| 157 |
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| 158 | /**
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| 159 | * This subroutine calculates the fission barriers
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| 160 | * of the liquid-drop model of Myers and Swiatecki (1967).
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| 161 | * Analytic parameterization of Dahlinger 1982
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| 162 | * replaces tables. Barrier heights from Myers and Swiatecki
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| 163 | */
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| 164 | G4double bfms67(G4double zms, G4double ams);
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| 165 |
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| 166 | /**
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| 167 | * This subroutine calculates the ordinary legendre polynomials of
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| 168 | * order 0 to n-1 of argument x and stores them in the vector pl.
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| 169 | * They are calculated by recursion relation from the first two
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| 170 | * polynomials.
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| 171 | * Written by A.J.Sierk LANL t-9 February, 1984
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| 172 | */
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| 173 | void lpoly(G4double x, G4int n, G4double pl[]);
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| 174 |
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| 175 | /**
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| 176 | * This function will calculate the liquid-drop nuclear mass for spheri
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| 177 | * configuration according to the preprint NUCLEAR GROUND-STATE
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| 178 | * MASSES and DEFORMATIONS by P. Mo"ller et al. from August 16, 1993 p.
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| 179 | * All constants are taken from this publication for consistency.
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| 180 | */
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| 181 | G4double eflmac(G4int ia, G4int iz, G4int flag, G4int optshp);
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| 182 |
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| 183 | /**
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| 184 | * Procedure for calculating the pairing correction to the binding
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| 185 | * energy of a specific nucleus.
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| 186 | */
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| 187 | void appariem(G4double a, G4double z, G4double *del);
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| 188 |
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| 189 | /**
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| 190 | * PROCEDURE FOR CALCULATING THE PARITY OF THE NUMBER N.
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| 191 | * RETURNS -1 IF N IS ODD AND +1 IF N IS EVEN
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| 192 | */
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| 193 | void parite(G4double n, G4double *par);
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| 194 |
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| 195 | /**
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| 196 | * RISE TIME IN WHICH THE FISSION WIDTH HAS REACHED
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| 197 | * 90 PERCENT OF ITS FINAL VALUE
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| 198 | */
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| 199 | G4double tau(G4double bet, G4double homega, G4double ef, G4double t);
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| 200 |
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| 201 | /**
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| 202 | * KRAMERS FAKTOR - REDUCTION OF THE FISSION PROBABILITY
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| 203 | * INDEPENDENT OF EXCITATION ENERGY
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| 204 | */
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| 205 | G4double cram(G4double bet, G4double homega);
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| 206 |
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| 207 | /**
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| 208 | * CALCULATION OF THE SURFACE BS OR CURVATURE BK OF A NUCLEUS
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| 209 | * RELATIVE TO THE SPHERICAL CONFIGURATION
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| 210 | * BASED ON MYERS, DROPLET MODEL FOR ARBITRARY SHAPES
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| 211 | */
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| 212 | G4double bipol(int iflag, G4double y);
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| 213 |
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| 214 | /**
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| 215 | * THIS SUBROUTINE RETURNS THE BARRIER HEIGHT BFIS, THE
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| 216 | * GROUND-STATE ENERGY SEGS, IN MEV, AND THE ANGULAR MOMENTUM
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| 217 | * AT WHICH THE FISSION BARRIER DISAPPEARS, LMAX, IN UNITS OF
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| 218 | * H-BAR, WHEN CALLED WITH INTEGER AGUMENTS IZ, THE ATOMIC
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| 219 | * NUMBER, IA, THE ATOMIC MASS NUMBER, AND IL, THE ANGULAR
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| 220 | * MOMENTUM IN UNITS OF H-BAR. (PLANCK'S CONSTANT DIVIDED BY
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| 221 | * 2*PI).
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| 222 | */
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| 223 | void barfit(G4int iz, G4int ia, G4int il, G4double *sbfis, G4double *segs, G4double *selmax);
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| 224 |
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| 225 | /**
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| 226 | * TIRAGE ALEATOIRE DANS UNE EXPONENTIELLLE : Y=EXP(-X/T)
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| 227 | */
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| 228 | G4double expohaz(G4int k, G4double T);
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| 229 |
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| 230 | /**
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| 231 | * DISTRIBUTION DE MAXWELL
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| 232 | */
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| 233 | G4double fd(G4double E);
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| 234 |
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| 235 | /**
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| 236 | *FONCTION INTEGRALE DE FD(E)
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| 237 | */
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| 238 | G4double f(G4double E);
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| 239 |
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| 240 | /**
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| 241 | * tirage aleatoire dans une maxwellienne
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| 242 | */
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| 243 | G4double fmaxhaz(G4double T);
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| 244 |
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| 245 | /**
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| 246 | *
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| 247 | */
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| 248 | G4double pace2(G4double a, G4double z);
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| 249 |
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| 250 | /**
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| 251 | *
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| 252 | */
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| 253 | void guet(G4double *x_par, G4double *z_par, G4double *find_par);
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| 254 |
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| 255 | // Fission
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| 256 | public:
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| 257 | /**
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| 258 | *
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| 259 | */
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| 260 | G4double spdef(G4int a, G4int z, G4int optxfis);
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| 261 |
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| 262 | /**
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| 263 | *
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| 264 | */
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| 265 | G4double fissility(G4int a, G4int z, G4int optxfis);
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| 266 |
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| 267 | // void evapora(G4double zprf, G4double aprf, G4double ee, G4double jprf,
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| 268 | // G4double *zf_par, G4double *af_par, G4double *mtota_par,
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| 269 | // G4double *pleva_par, G4double *pxeva_par);
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| 270 | // G4double bfms67(G4double zms, G4double ams);
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| 271 | // void lpoly(G4double x, G4int n, G4double pl[]);
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| 272 | // G4double expohaz(G4int k, G4double T);
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| 273 | // G4double fd(G4double E);
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| 274 | // G4double f(G4double E);
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| 275 | // G4double fmaxhaz(G4double k, G4double T);
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| 276 | void even_odd(G4double r_origin,G4double r_even_odd,G4int &i_out);
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| 277 | G4double umass(G4double z,G4double n,G4double beta);
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| 278 | G4double ecoul(G4double z1,G4double n1,G4double beta1,G4double z2,G4double n2,G4double beta2,G4double d);
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| 279 | void fissionDistri(G4double &a,G4double &z,G4double &e,
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| 280 | G4double &a1,G4double &z1,G4double &e1,G4double &v1,
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| 281 | G4double &a2,G4double &z2,G4double &e2,G4double &v2);
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| 282 | void standardRandom(G4double *rndm, G4long *seed);
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| 283 | G4double haz(G4int k);
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| 284 | G4double gausshaz(int k, double xmoy, double sig);
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| 285 |
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| 286 |
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| 287 | public:
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| 288 | // Coordinate system transformations:
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| 289 | void lorab(G4double gam, G4double eta, G4double ein, G4double pin[],
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| 290 | G4double *eout, G4double pout[]);
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| 291 |
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| 292 | void translab(G4double gamrem, G4double etrem, G4double csrem[4], G4int nopart, G4int ndec);
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| 293 | void translabpf(G4double masse1, G4double t1, G4double p1, G4double ctet1,
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| 294 | G4double phi1, G4double gamrem, G4double etrem, G4double R[][4],
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| 295 | G4double *plab1, G4double *gam1, G4double *eta1, G4double csdir[]);
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| 296 |
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| 297 | void rotab(G4double R[4][4], G4double pin[4], G4double pout[4]);
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| 298 |
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| 299 | // Utils
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| 300 | G4int min(G4int a, G4int b);
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| 301 | G4double min(G4double a, G4double b);
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| 302 | G4int max(G4int a, G4int b);
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| 303 | G4double max(G4double a, G4double b);
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| 304 |
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| 305 | G4int nint(G4double number);
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| 306 | G4int secnds(G4int x);
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| 307 | G4int mod(G4int a, G4int b);
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| 308 | G4double dmod(G4double a, G4double b);
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| 309 | G4double dint(G4double a);
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| 310 | G4int idint(G4double a);
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| 311 | G4int idnint(G4double value);
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| 312 | G4double utilabs(G4double a);
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| 313 | G4double dmin1(G4double a, G4double b, G4double c);
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| 314 |
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| 315 | private:
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| 316 | G4int verboseLevel;
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| 317 |
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| 318 | G4Pace *pace;
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| 319 | G4Hazard *hazard;
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| 320 | G4Ald *ald;
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| 321 | G4Ablamain *ablamain;
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| 322 | G4Emdpar *emdpar;
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| 323 | G4Eenuc *eenuc;
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| 324 | G4Ec2sub *ec2sub;
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| 325 | G4Ecld *ecld;
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| 326 | G4Fb *fb;
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| 327 | G4Fiss *fiss;
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| 328 | G4Opt *opt;
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| 329 | G4Volant *volant;
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| 330 | G4VarNtp *varntp;
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| 331 | };
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