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Geant4
9.6.p02
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#include <G4Abla.hh>
| G4Abla::G4Abla | ( | G4Hazard * | aHazard, |
| G4Volant * | aVolant, | ||
| G4VarNtp * | aVarntp | ||
| ) |
| G4Abla::G4Abla | ( | G4Hazard * | hazard, |
| G4Volant * | volant | ||
| ) |
| void G4Abla::barfit | ( | G4int | iz, |
| G4int | ia, | ||
| G4int | il, | ||
| G4double * | sbfis, | ||
| G4double * | segs, | ||
| G4double * | selmax | ||
| ) |
THIS SUBROUTINE RETURNS THE BARRIER HEIGHT BFIS, THE GROUND-STATE ENERGY SEGS, IN MEV, AND THE ANGULAR MOMENTUM AT WHICH THE FISSION BARRIER DISAPPEARS, LMAX, IN UNITS OF H-BAR, WHEN CALLED WITH INTEGER AGUMENTS IZ, THE ATOMIC NUMBER, IA, THE ATOMIC MASS NUMBER, AND IL, THE ANGULAR MOMENTUM IN UNITS OF H-BAR. (PLANCK'S CONSTANT DIVIDED BY 2*PI).
Definition at line 2870 of file G4Abla.cc.


| void G4Abla::breakItUp | ( | G4double | nucleusA, |
| G4double | nucleusZ, | ||
| G4double | nucleusMass, | ||
| G4double | excitationEnergy, | ||
| G4double | angularMomentum, | ||
| G4double | recoilEnergy, | ||
| G4double | momX, | ||
| G4double | momY, | ||
| G4double | momZ, | ||
| G4int | eventnumber | ||
| ) |
Main interface to the de-excitation code.
| nucleusA | mass number of the nucleus |
| nucleusZ | charge number of the nucleus |
| nucleusMass | mass of the nucleus |
| excitationEnergy | excitation energy of the nucleus |
| angularMomentum | angular momentum of the nucleus (produced as output by INCL4) |
| recoilEnergy | recoil energy of the nucleus |
| momX | momentum x-component |
| momY | momentum y-component |
| momZ | momentum z-component |
| eventnumber | number of the event |
Definition at line 109 of file G4Abla.cc.


| void G4Abla::direct | ( | G4double | zprf, |
| G4double | a, | ||
| G4double | ee, | ||
| G4double | jprf, | ||
| G4double * | probp_par, | ||
| G4double * | probn_par, | ||
| G4double * | proba_par, | ||
| G4double * | probf_par, | ||
| G4double * | ptotl_par, | ||
| G4double * | sn_par, | ||
| G4double * | sbp_par, | ||
| G4double * | sba_par, | ||
| G4double * | ecn_par, | ||
| G4double * | ecp_par, | ||
| G4double * | eca_par, | ||
| G4double * | bp_par, | ||
| G4double * | ba_par, | ||
| G4int | inttype, | ||
| G4int | inum, | ||
| G4int | itest | ||
| ) |
This function will calculate the liquid-drop nuclear mass for spheri configuration according to the preprint NUCLEAR GROUND-STATE MASSES and DEFORMATIONS by P. Mo"ller et al. from August 16, 1993 p. All constants are taken from this publication for consistency.
Definition at line 2542 of file G4Abla.cc.


| void G4Abla::fissionDistri | ( | G4double & | a, |
| G4double & | z, | ||
| G4double & | e, | ||
| G4double & | a1, | ||
| G4double & | z1, | ||
| G4double & | e1, | ||
| G4double & | v1, | ||
| G4double & | a2, | ||
| G4double & | z2, | ||
| G4double & | e2, | ||
| G4double & | v2 | ||
| ) |
/* Eexc at scission */
/* 1. fragment is spherical */
/* 2. fragment is spherical */
/* N appr. 86 */
/* 2. fragment is spherical */
/* 1. fragment is spherical */
/* When(3) */
Definition at line 3512 of file G4Abla.cc.


| void G4Abla::initEvapora | ( | ) |
This subroutine calculates the ordinary legendre polynomials of order 0 to n-1 of argument x and stores them in the vector pl. They are calculated by recursion relation from the first two polynomials. Written by A.J.Sierk LANL t-9 February, 1984
Definition at line 2524 of file G4Abla.cc.

Coefficient of collective enhancement including damping Input: z,a,bet,sig,u Output: qr - collective enhancement factor See junghans et al., nucl. phys. a 629 (1998) 635
| z | charge number |
| a | mass number |
| bet | beta deformation |
| sig | perpendicular spin cut-off factor |
| u | Energy |
Definition at line 974 of file G4Abla.cc.

1.8.4