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G4HadronElasticPhysics
----------------------
Hadron nuclear elastic process for all hadrons:
- proton
- cross section: Barashenkov-Glauber-Gribov
- final-state: Chips
- neutron:
- cross section: G4NeutronElasticXS
- final-state: Chips
- charged pions:
- cross section: Barashenkov-Glauber-Gribov
- final-state: Starkov's model (G4ElasticHadrNucleusHE) for all energies
- kaons, hyperons, anti-hyperons
- cross section: Glauber-Gribov
- final-state: Gheisha
- deuteron, triton, He3, alpha
- cross section: Glauber-Gribov
- final-state: Gheisha
- anti_proton, anti_neutron, anti_deuteron, anti_triton, anti_He3,
anti_alpha
- cross-section: Galoyan-Uzhinsky-Glauber-Gribov
- final-state: Galoyan-Uzhinsky model above 100 MeV/nucleon,
Gheisha below.
G4HadronElasticPhysicsHP
------------------------
As G4HadronElasticPhysics, with the only difference that for neutrons
below 20 MeV, NeutronHP elastic is used (for both cross section and
final-state model).
G4HadronElasticPhysicsLEND
--------------------------
As G4HadronElasticPhysics, with the only difference that for neutrons
below 20 MeV, LEND elastic is used (for both cross section and
final-state model).
G4HadronElasticPhysicsXS
------------------------
Now exactly as G4HadronElasticPhysics.
G4HadronHElasticPhysics
-----------------------
- proton
- cross section: Barashenkov-Glauber-Gribov
- final-state: Diffuse model, except for Hydrogen where Chips is used
- neutron:
- cross section: G4NeutronElasticXS
- final-state: Diffuse model, except for Hydrogen where Chips is used
- charged pions:
- cross section: Barashenkov-Glauber-Gribov
- final-state: Diffuse model, except for Hydrogen where Chips is used
- kaons, hyperons, anti-hyperons
- cross section: Glauber-Gribov
- final-state: Chips
- deuteron, triton, He3, alpha
- cross section: Glauber-Gribov
- final-state: Gheisha
- anti_proton, anti_neutron
- cross section: Galoyan-Uzhinsky-Glauber-Gribov
- final-state: Galoyan-Uzhinsky model above 100 MeV/nucleon,
Chips below.
- anti_deuteron, anti_triton, anti_He3, anti_alpha
- cross-section: Galoyan-Uzhinsky-Glauber-Gribov
- final-state: Galoyan-Uzhinsky model above 100 MeV/nucleon,
Gheisha below.
G4IonElasticPhysics
-------------------
As G4HadronElasticPhysics, with the addition of elastic process for
generic ion:
- cross section: Glauber-Gribov
- final-state: Diffuse model
G4HadronDElasticPhysics
-----------------------
Hadron nuclear elastic process for all hadrons:
- proton and charged pions:
- cross section: Barashenkov-Glauber-Gribov
- final-state: Diffuse model where applicable, else Gheisha
- neutron:
- cross section: G4NeutronElasticXS
- final-state: Diffuse model where applicable, else Gheisha
- kaons
- cross section: Glauber-Gribov
- final-state: Diffuse model where applicable, else Gheisha
- hyperons, anti-hyperons, deuteron, triton, He3, alpha
- cross section: Glauber-Gribov
- final-state: Gheisha
- anti_proton, anti_neutron, anti_deuteron, anti_triton, anti_He3,
anti_alpha
- cross-section: Galoyan-Uzhinsky-Glauber-Gribov
- final-state: Galoyan-Uzhinsky model above 100 MeV/nucleon,
Gheisha below.
G4ChargeExchangePhysics
-----------------------
Hadron nuclear coherent charge exchange, used in this constructor
only for nucleons and charged pions.