source: trunk/source/processes/hadronic/models/incl/include/G4Abla.hh @ 1350

Last change on this file since 1350 was 1347, checked in by garnier, 14 years ago

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26// $Id: G4Abla.hh,v 1.14 2010/11/17 20:19:09 kaitanie Exp $
27// Translation of INCL4.2/ABLA V3
28// Pekka Kaitaniemi, HIP (translation)
29// Christelle Schmidt, IPNL (fission code)
30// Alain Boudard, CEA (contact person INCL/ABLA)
31// Aatos Heikkinen, HIP (project coordination)
32
33#include "globals.hh"
34
35#include "G4VInclLogger.hh"
36#include "G4InclRandomNumbers.hh"
37#include "G4AblaDataDefs.hh"
38#include "G4InclDataDefs.hh"
39#include "G4AblaFissionBase.hh"
40
41#ifndef G4Abla_hh
42#define G4Abla_hh 1
43
44/**
45 *  Class containing ABLA de-excitation code.
46 */
47
48class G4Abla {
49
50public:
51  /**
52   * This constructor is used by standalone test driver and the Geant4 interface.
53   *
54   * @param aHazard random seeds
55   * @param aVolant data structure for ABLA output
56   * @param aVarNtp data structure for transfering ABLA output to Geant4 interface
57   */
58  G4Abla(G4Hazard *aHazard, G4Volant *aVolant, G4VarNtp *aVarntp);
59
60  /**
61   * Basic destructor.
62   */
63  ~G4Abla();
64
65  /**
66   * Register the INCL/ABLA internal variable logger.
67   */
68  void registerLogger(G4VInclLogger *theLogger);
69
70  /**
71   * Set verbosity level.
72   */
73  void setVerboseLevel(G4int level);
74
75  /**
76   * Get the internal output data structure pointer.
77   */
78  G4Volant* getVolant() {
79    return volant;
80  }
81
82  /**
83   * Main interface to the de-excitation code.
84   *
85   * @param nucleusA mass number of the nucleus
86   * @param nucleusZ charge number of the nucleus
87   * @param nucleusMass mass of the nucleus
88   * @param excitationEnergy excitation energy of the nucleus
89   * @param angularMomentum angular momentum of the nucleus (produced as output by INCL4)
90   * @param recoilEnergy recoil energy of the nucleus
91   * @param momX momentum x-component
92   * @param momY momentum y-component
93   * @param momZ momentum z-component
94   * @param eventnumber number of the event
95   */
96  void breakItUp(G4int nucleusA, G4int nucleusZ, G4double nucleusMass, G4double excitationEnergy,
97                 G4double angularMomentum, G4double recoilEnergy, G4double momX, G4double momY, G4double momZ,
98                 G4int eventnumber);
99
100  // Evaporation
101public:
102  /**
103   * Initialize ABLA evaporation code.
104   *
105   */
106  void initEvapora();
107
108  /**
109   * Coefficient of collective enhancement including damping                         
110   * Input: z,a,bet,sig,u                                                 
111   * Output: qr - collective enhancement factor                           
112   * See  junghans et al., nucl. phys. a 629 (1998) 635                   
113   * @param z charge number
114   * @param a mass number
115   * @param bet beta deformation
116   * @param sig perpendicular spin cut-off factor
117   * @param u Energy
118   * @return Coefficient of collective enhancement   
119   */
120  void qrot(G4double z, G4double a, G4double bet, G4double sig, G4double u, G4double *qr);
121
122  /**
123   * Model de la goutte liquide de c. f. weizsacker.
124   * usually an obsolete option
125   */
126  void mglw(G4double a, G4double z, G4double *el);
127
128  /**
129   * Mglms
130   */
131  void mglms(G4double a, G4double z, G4int refopt4, G4double *el);
132
133  /**
134   *
135   */
136  G4double spdef(G4int a, G4int z, G4int optxfis);
137
138  /**
139   * Calculation of fissility parameter
140   */
141  G4double fissility(int a,int z, int optxfis);
142
143  /**
144   * Main evaporation routine.
145   */
146  void evapora(G4double zprf, G4double aprf, G4double ee, G4double jprf, 
147               G4double *zf_par, G4double *af_par, G4double *mtota_par,
148               G4double *pleva_par, G4double *pxeva_par, G4double *pyeva_par,
149               G4int *ff_par, G4int *inttype_par, G4int *inum_par);
150
151  /**
152   * Calculation of particle emission probabilities.
153   */
154  void direct(G4double zprf,G4double a, G4double ee, G4double jprf, 
155              G4double *probp_par, G4double *probn_par, G4double *proba_par, 
156              G4double *probf_par, G4double *ptotl_par, G4double *sn_par, G4double *sbp_par, G4double *sba_par, G4double *ecn_par, 
157              G4double *ecp_par,G4double *eca_par, G4double *bp_par, G4double *ba_par, G4int, G4int inum, G4int itest);
158
159  /**
160   * Level density parameters.
161   */
162  void densniv(G4double a, G4double z, G4double ee, G4double esous, G4double *dens, G4double bshell, G4double bs, G4double bk, 
163               G4double *temp, G4int optshp, G4int optcol, G4double defbet);
164
165  /**
166   * This subroutine calculates the fission barriers                                                                 
167   * of the liquid-drop model of Myers and Swiatecki (1967).                                                                 
168   * Analytic parameterization of Dahlinger 1982
169   * replaces tables. Barrier heights from Myers and Swiatecki                                                               
170   */
171  G4double bfms67(G4double zms, G4double ams);
172
173  /**
174   * This subroutine calculates the ordinary legendre polynomials of   
175   * order 0 to n-1 of argument x and stores them in the vector pl.   
176   * They are calculated by recursion relation from the first two     
177   * polynomials.                                                     
178   * Written by A.J.Sierk  LANL  t-9  February, 1984                   
179   */
180  void lpoly(G4double x, G4int n, G4double pl[]);
181
182  /**
183   * This function will calculate the liquid-drop nuclear mass for spheri
184   * configuration according to the preprint NUCLEAR GROUND-STATE       
185   * MASSES and DEFORMATIONS by P. Mo"ller et al. from August 16, 1993 p.
186   * All constants are taken from this publication for consistency.     
187   */
188  G4double eflmac(G4int ia, G4int iz, G4int flag, G4int optshp);
189
190  /**
191   * Procedure for calculating the pairing correction to the binding   
192   * energy of a specific nucleus.
193   */
194  void appariem(G4double a, G4double z, G4double *del);
195
196  /**
197   * PROCEDURE FOR CALCULATING THE PARITY OF THE NUMBER N.             
198   * RETURNS -1 IF N IS ODD AND +1 IF N IS EVEN                       
199   */
200  void parite(G4double n, G4double *par);
201
202  /**
203   * RISE TIME IN WHICH THE FISSION WIDTH HAS REACHED     
204   * 90 PERCENT OF ITS FINAL VALUE
205   */
206  G4double tau(G4double bet, G4double homega, G4double ef, G4double t);
207
208  /**
209   * KRAMERS FAKTOR  - REDUCTION OF THE FISSION PROBABILITY       
210   * INDEPENDENT OF EXCITATION ENERGY
211   */
212  G4double cram(G4double bet, G4double homega);
213
214  /**
215   * CALCULATION OF THE SURFACE BS OR CURVATURE BK OF A NUCLEUS       
216   * RELATIVE TO THE SPHERICAL CONFIGURATION                           
217   * BASED ON  MYERS, DROPLET MODEL FOR ARBITRARY SHAPES               
218   */
219  G4double bipol(int iflag, G4double y);
220
221  /**
222   * THIS SUBROUTINE RETURNS THE BARRIER HEIGHT BFIS, THE             
223   * GROUND-STATE ENERGY SEGS, IN MEV, AND THE ANGULAR MOMENTUM       
224   * AT WHICH THE FISSION BARRIER DISAPPEARS, LMAX, IN UNITS OF       
225   * H-BAR, WHEN CALLED WITH INTEGER AGUMENTS IZ, THE ATOMIC           
226   * NUMBER, IA, THE ATOMIC MASS NUMBER, AND IL, THE ANGULAR           
227   * MOMENTUM IN UNITS OF H-BAR. (PLANCK'S CONSTANT DIVIDED BY         
228   * 2*PI).                                                           
229   */
230  void barfit(G4int iz, G4int ia, G4int il, G4double *sbfis, G4double *segs, G4double *selmax);
231
232  /**
233   * Random numbers.
234   */
235  G4double haz(G4int k);
236  void standardRandom(G4double *rndm, G4long *seed);
237
238  /**
239   * TIRAGE ALEATOIRE DANS UNE EXPONENTIELLLE : Y=EXP(-X/T)
240   */ 
241  G4double expohaz(G4int k, G4double T);
242
243  /**
244   * DISTRIBUTION DE MAXWELL
245   */
246  G4double fd(G4double E);
247
248  /**
249   *FONCTION INTEGRALE DE FD(E)
250   */
251  G4double f(G4double E);
252
253  /**
254   * tirage aleatoire dans une maxwellienne
255   */
256  G4double fmaxhaz(G4double T);
257
258  /**
259   *
260   */
261  G4double pace2(G4double a, G4double z);
262
263  /**
264   *
265   */
266  void guet(G4double *x_par, G4double *z_par, G4double *find_par);
267   
268public:
269  // Coordinate system transformations:
270  void lorab(G4double gam, G4double eta, G4double ein, G4double pin[],
271             G4double *eout, G4double pout[]);
272
273  void translab(G4double gamrem, G4double etrem, G4double csrem[4], G4int nopart, G4int ndec);
274  void translabpf(G4double masse1, G4double t1, G4double p1, G4double ctet1,
275                  G4double phi1, G4double gamrem, G4double etrem, G4double R[][4],
276                  G4double *plab1, G4double *gam1, G4double *eta1, G4double csdir[]);
277
278  void rotab(G4double R[4][4], G4double pin[4], G4double pout[4]);
279
280  // Utils
281  G4int min(G4int a, G4int b);
282  G4double min(G4double a, G4double b);
283  G4int max(G4int a, G4int b);
284  G4double max(G4double a, G4double b);
285
286  G4int nint(G4double number);
287  G4int secnds(G4int x);
288  G4int mod(G4int a, G4int b);
289  G4double dmod(G4double a, G4double b);
290  G4double dint(G4double a);
291  G4int idint(G4double a);
292  G4int idnint(G4double value);
293  G4double utilabs(G4double a);
294  G4double dmin1(G4double a, G4double b, G4double c);
295  G4Ec2sub* getFrldmTable() {
296    return ec2sub;
297  }
298
299private:
300  G4int verboseLevel;
301  G4int ilast;
302
303  G4AblaFissionBase *fissionModel;
304  G4InclRandomInterface *randomGenerator;
305  G4Pace *pace;
306  G4Hazard *hazard;
307  G4Ald *ald;
308  G4Eenuc *eenuc;
309  G4Ec2sub *ec2sub;
310  G4Ecld *ecld; 
311  G4Fb *fb;
312  G4Fiss *fiss;
313  G4Opt *opt;
314  G4Volant *volant;
315  G4VarNtp *varntp; 
316
317  G4VInclLogger *theLogger;
318};
319
320#endif
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