Gabriele Cosmo
40 lines
1.5 KiB
Plaintext
40 lines
1.5 KiB
Plaintext
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G4IonBinaryCascadePhysics
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Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
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generic ion projectiles), with Glauber-Gribov cross section and
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Binary Light Ion (BIC, with Precompound/de-excitation) and Fritiof (FTF)
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string model (with Precompound/de-excitation) for the final state.
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BIC is used for projectiles of kinetic energies below 6 GeV/nucleon, and
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FTF above 3 GeV/nucleon.
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G4IonINCLXXPhysics
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Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
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generic ion projectiles), with Glauber-Gribov cross section and
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INCLXX and FTFP for the final state. INCLXX is used below 3 GeV/nucleon,
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and FTF above 2.9 GeV/nucleon.
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G4IonPhysics
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Currently equivalent to G4IonBinaryCascadePhysics.
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G4IonPhysicsPHP
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Similar to G4IonBinaryCascadePhysics, except that ParticleHP (for both
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cross sections and final states) is used below 200 MeV/n for deuteron,
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triton, He3 and alpha (and BIC used above 190 MeV/n for these light ions).
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G4IonQMDPhysic
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Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
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generic ion projectiles), with Glauber-Gribov cross section and
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BIC, QMD and FTFP for the final state. These three final-state models
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are used in the following intervals of projectile kinetic energy:
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- BIC below 110 MeV/nucleon;
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- QMD between 100 and 10'000 MeV/nucleon;
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- FTF above 9990 MeV/nucleon.
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