| Geant4 Cross Reference |
1 ---------------------------------------------- 1 -------------------------------------------------------------------
2 2
3 3
4 G4IonBinaryCascadePhysics 4 G4IonBinaryCascadePhysics
5 ------------------------- 5 -------------------------
6 Inelastic ion-ion processes (for deuteron, tr 6 Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
7 generic ion projectiles), with Glauber-Gribov 7 generic ion projectiles), with Glauber-Gribov cross section and
8 Binary Light Ion (BIC, with Precompound/de-ex 8 Binary Light Ion (BIC, with Precompound/de-excitation) and Fritiof (FTF)
9 string model (with Precompound/de-excitation) 9 string model (with Precompound/de-excitation) for the final state.
10 BIC is used for projectiles of kinetic energi 10 BIC is used for projectiles of kinetic energies below 6 GeV/nucleon, and
11 FTF above 3 GeV/nucleon. 11 FTF above 3 GeV/nucleon.
12 12
13 G4IonINCLXXPhysics 13 G4IonINCLXXPhysics
14 ------------------ 14 ------------------
15 Inelastic ion-ion processes (for deuteron, tr 15 Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
16 generic ion projectiles), with Glauber-Gribov 16 generic ion projectiles), with Glauber-Gribov cross section and
17 INCLXX and FTFP for the final state. INCLXX i 17 INCLXX and FTFP for the final state. INCLXX is used below 3 GeV/nucleon,
18 and FTF above 2.9 GeV/nucleon. 18 and FTF above 2.9 GeV/nucleon.
19 19
20 G4IonPhysics 20 G4IonPhysics
21 ------------ 21 ------------
22 Currently equivalent to G4IonBinaryCascadePhy 22 Currently equivalent to G4IonBinaryCascadePhysics.
23 23
24 G4IonPhysicsXS 24 G4IonPhysicsXS
25 -------------- 25 --------------
26 As G4IonPhysics, except that for deuteron, tr 26 As G4IonPhysics, except that for deuteron, triton, He3 and alpha
27 the corresponding G4ParticleInelasticXS cross 27 the corresponding G4ParticleInelasticXS cross section is used
28 (instead of G4ComponentGGNuclNuclXsc). 28 (instead of G4ComponentGGNuclNuclXsc).
29 29
30 G4IonPhysicsPHP 30 G4IonPhysicsPHP
31 --------------- 31 ---------------
32 Similar to G4IonBinaryCascadePhysics, except 32 Similar to G4IonBinaryCascadePhysics, except that ParticleHP (for both
33 cross sections and final states) is used belo 33 cross sections and final states) is used below 200 MeV/n for deuteron,
34 triton, He3 and alpha (and BIC used above 190 34 triton, He3 and alpha (and BIC used above 190 MeV/n for these light ions).
35 35
36 G4IonQMDPhysics << 36 G4IonQMDPhysic
37 --------------- << 37 --------------
38 Inelastic ion-ion processes (for deuteron, tr 38 Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
39 generic ion projectiles), with Glauber-Gribov 39 generic ion projectiles), with Glauber-Gribov cross section and
40 BIC, QMD and FTFP for the final state. These 40 BIC, QMD and FTFP for the final state. These three final-state models
41 are used in the following intervals of projec 41 are used in the following intervals of projectile kinetic energy:
42 - BIC below 110 MeV/nucleon; 42 - BIC below 110 MeV/nucleon;
43 - QMD between 100 and 6'000 MeV/nucleon; 43 - QMD between 100 and 6'000 MeV/nucleon;
44 - FTF above 5990 MeV/nucleon. <<
45 <<
46 G4IonLightIonQMDPhysics <<
47 ----------------------- <<
48 A variant of G4IonQMDPhysics, in which G4Light <<
49 in the interval [30 MeV, 510 MeV]. <<
50 These four final-state models are used in the <<
51 projectile kinetic energy: <<
52 - BIC below 40 MeV/nucleon; <<
53 - LightIonQMD between 30 and 510 MeV/nucleon <<
54 - QMD between 500 and 6'000 MeV/nucleon; <<
55 - FTF above 5990 MeV/nucleon. 44 - FTF above 5990 MeV/nucleon.