| Geant4 Cross Reference |
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3
4 G4IonBinaryCascadePhysics
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6 Inelastic ion-ion processes (for deuteron, tr
7 generic ion projectiles), with Glauber-Gribov
8 Binary Light Ion (BIC, with Precompound/de-ex
9 string model (with Precompound/de-excitation)
10 BIC is used for projectiles of kinetic energi
11 FTF above 3 GeV/nucleon.
12
13 G4IonINCLXXPhysics
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15 Inelastic ion-ion processes (for deuteron, tr
16 generic ion projectiles), with Glauber-Gribov
17 INCLXX and FTFP for the final state. INCLXX i
18 and FTF above 2.9 GeV/nucleon.
19
20 G4IonPhysics
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22 Currently equivalent to G4IonBinaryCascadePhy
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24 G4IonPhysicsXS
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26 As G4IonPhysics, except that for deuteron, tr
27 the corresponding G4ParticleInelasticXS cross
28 (instead of G4ComponentGGNuclNuclXsc).
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30 G4IonPhysicsPHP
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32 Similar to G4IonBinaryCascadePhysics, except
33 cross sections and final states) is used belo
34 triton, He3 and alpha (and BIC used above 190
35
36 G4IonQMDPhysics
37 ---------------
38 Inelastic ion-ion processes (for deuteron, tr
39 generic ion projectiles), with Glauber-Gribov
40 BIC, QMD and FTFP for the final state. These
41 are used in the following intervals of projec
42 - BIC below 110 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.