Geant4
9.6.p02
|
#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.