Gabriele Cosmo
56 lines
2.1 KiB
Plaintext
56 lines
2.1 KiB
Plaintext
-------------------------------------------------------------------
|
|
|
|
|
|
G4IonBinaryCascadePhysics
|
|
-------------------------
|
|
Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
|
|
generic ion projectiles), with Glauber-Gribov cross section and
|
|
Binary Light Ion (BIC, with Precompound/de-excitation) and Fritiof (FTF)
|
|
string model (with Precompound/de-excitation) for the final state.
|
|
BIC is used for projectiles of kinetic energies below 6 GeV/nucleon, and
|
|
FTF above 3 GeV/nucleon.
|
|
|
|
G4IonINCLXXPhysics
|
|
------------------
|
|
Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
|
|
generic ion projectiles), with Glauber-Gribov cross section and
|
|
INCLXX and FTFP for the final state. INCLXX is used below 3 GeV/nucleon,
|
|
and FTF above 2.9 GeV/nucleon.
|
|
|
|
G4IonPhysics
|
|
------------
|
|
Currently equivalent to G4IonBinaryCascadePhysics.
|
|
|
|
G4IonPhysicsXS
|
|
--------------
|
|
As G4IonPhysics, except that for deuteron, triton, He3 and alpha
|
|
the corresponding G4ParticleInelasticXS cross section is used
|
|
(instead of G4ComponentGGNuclNuclXsc).
|
|
|
|
G4IonPhysicsPHP
|
|
---------------
|
|
Similar to G4IonBinaryCascadePhysics, except that ParticleHP (for both
|
|
cross sections and final states) is used below 200 MeV/n for deuteron,
|
|
triton, He3 and alpha (and BIC used above 190 MeV/n for these light ions).
|
|
|
|
G4IonQMDPhysics
|
|
---------------
|
|
Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
|
|
generic ion projectiles), with Glauber-Gribov cross section and
|
|
BIC, QMD and FTFP for the final state. These three final-state models
|
|
are used in the following intervals of projectile kinetic energy:
|
|
- BIC below 110 MeV/nucleon;
|
|
- QMD between 100 and 6'000 MeV/nucleon;
|
|
- FTF above 5990 MeV/nucleon.
|
|
|
|
G4IonLightIonQMDPhysics
|
|
-----------------------
|
|
A variant of G4IonQMDPhysics, in which G4LightIonQMDReaction is used
|
|
in the interval [30 MeV, 510 MeV].
|
|
These four final-state models are used in the following intervals of
|
|
projectile kinetic energy:
|
|
- BIC below 40 MeV/nucleon;
|
|
- LightIonQMD between 30 and 510 MeV/nucleon;
|
|
- QMD between 500 and 6'000 MeV/nucleon;
|
|
- FTF above 5990 MeV/nucleon.
|