Geant4 Cross Reference

Cross-Referencing   Geant4
Geant4/physics_lists/constructors/ions/README

Version: [ ReleaseNotes ] [ 1.0 ] [ 1.1 ] [ 2.0 ] [ 3.0 ] [ 3.1 ] [ 3.2 ] [ 4.0 ] [ 4.0.p1 ] [ 4.0.p2 ] [ 4.1 ] [ 4.1.p1 ] [ 5.0 ] [ 5.0.p1 ] [ 5.1 ] [ 5.1.p1 ] [ 5.2 ] [ 5.2.p1 ] [ 5.2.p2 ] [ 6.0 ] [ 6.0.p1 ] [ 6.1 ] [ 6.2 ] [ 6.2.p1 ] [ 6.2.p2 ] [ 7.0 ] [ 7.0.p1 ] [ 7.1 ] [ 7.1.p1 ] [ 8.0 ] [ 8.0.p1 ] [ 8.1 ] [ 8.1.p1 ] [ 8.1.p2 ] [ 8.2 ] [ 8.2.p1 ] [ 8.3 ] [ 8.3.p1 ] [ 8.3.p2 ] [ 9.0 ] [ 9.0.p1 ] [ 9.0.p2 ] [ 9.1 ] [ 9.1.p1 ] [ 9.1.p2 ] [ 9.1.p3 ] [ 9.2 ] [ 9.2.p1 ] [ 9.2.p2 ] [ 9.2.p3 ] [ 9.2.p4 ] [ 9.3 ] [ 9.3.p1 ] [ 9.3.p2 ] [ 9.4 ] [ 9.4.p1 ] [ 9.4.p2 ] [ 9.4.p3 ] [ 9.4.p4 ] [ 9.5 ] [ 9.5.p1 ] [ 9.5.p2 ] [ 9.6 ] [ 9.6.p1 ] [ 9.6.p2 ] [ 9.6.p3 ] [ 9.6.p4 ] [ 10.0 ] [ 10.0.p1 ] [ 10.0.p2 ] [ 10.0.p3 ] [ 10.0.p4 ] [ 10.1 ] [ 10.1.p1 ] [ 10.1.p2 ] [ 10.1.p3 ] [ 10.2 ] [ 10.2.p1 ] [ 10.2.p2 ] [ 10.2.p3 ] [ 10.3 ] [ 10.3.p1 ] [ 10.3.p2 ] [ 10.3.p3 ] [ 10.4 ] [ 10.4.p1 ] [ 10.4.p2 ] [ 10.4.p3 ] [ 10.5 ] [ 10.5.p1 ] [ 10.6 ] [ 10.6.p1 ] [ 10.6.p2 ] [ 10.6.p3 ] [ 10.7 ] [ 10.7.p1 ] [ 10.7.p2 ] [ 10.7.p3 ] [ 10.7.p4 ] [ 11.0 ] [ 11.0.p1 ] [ 11.0.p2 ] [ 11.0.p3, ] [ 11.0.p4 ] [ 11.1 ] [ 11.1.1 ] [ 11.1.2 ] [ 11.1.3 ] [ 11.2 ] [ 11.2.1 ] [ 11.2.2 ] [ 11.3.0 ] 

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  2 
  3 
  4  G4IonBinaryCascadePhysics
  5  -------------------------
  6  Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
  7  generic ion projectiles), with Glauber-Gribov cross section and
  8  Binary Light Ion (BIC, with Precompound/de-excitation) and Fritiof (FTF)
  9  string model (with Precompound/de-excitation) for the final state.
 10  BIC is used for projectiles of kinetic energies below 6 GeV/nucleon, and
 11  FTF above 3 GeV/nucleon.
 12  
 13  G4IonINCLXXPhysics
 14  ------------------
 15  Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
 16  generic ion projectiles), with Glauber-Gribov cross section and
 17  INCLXX and FTFP for the final state. INCLXX is used below 3 GeV/nucleon,
 18  and FTF above 2.9 GeV/nucleon.
 19  
 20  G4IonPhysics
 21  ------------
 22  Currently equivalent to G4IonBinaryCascadePhysics.
 23 
 24  G4IonPhysicsXS
 25  --------------
 26  As G4IonPhysics, except that for deuteron, triton, He3 and alpha
 27  the corresponding G4ParticleInelasticXS cross section is used
 28  (instead of G4ComponentGGNuclNuclXsc).
 29 
 30  G4IonPhysicsPHP
 31  ---------------
 32  Similar to G4IonBinaryCascadePhysics, except that ParticleHP (for both
 33  cross sections and final states) is used below 200 MeV/n for deuteron,
 34  triton, He3 and alpha (and BIC used above 190 MeV/n for these light ions).
 35 
 36  G4IonQMDPhysics
 37  ---------------
 38  Inelastic ion-ion processes (for deuteron, triton, He3, alpha and
 39  generic ion projectiles), with Glauber-Gribov cross section and
 40  BIC, QMD and FTFP for the final state. These three final-state models
 41  are used in the following intervals of projectile kinetic energy:
 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 G4LightIonQMDReaction is used
 49 in the interval [30 MeV, 510 MeV].
 50 These four final-state models are used in the following intervals of
 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.