The computer simulation of particles traversing an experimental setup has to take into account the interactions of those particles with the material of the detector. GEANT is able to simulate the dominant processes which can occur in the energy range from 10 keV to 10 TeV for electromagnetic interactions. As far as hadronic interactions are concerned, the range of validity is the one of the hadronic packages used, which usually does not extend below a few tens of MeV. For more information the user is invited to consult the relevant documentation [,,,,,].
Simulating a given process means:
Computation of total cross-section or energy losses | Generation of the final state particles | |
Processes involving the photon | ||
( ) pair conversion | PHYS 210 | PHYS 211 |
Compton collision | PHYS 220 | PHYS 221 |
Photoelectric effect | PHYS 230 | PHYS 231 |
Photo fission of heavy elements | PHYS 240 | PHYS 240 |
Rayleigh effect | PHYS 250 | PHYS 251 |
Processes involving | ||
Multiple scattering | PHYS 320or 325 or 328 | |
Ionisation and -rays production | PHYS 330 | PHYS 331or 332 |
Bremsstrahlung | PHYS 340 | PHYS 341 |
Annihilation of positron | PHYS 350 | PHYS 351 |
Generation of Cerenkov light | PHYS 260 | PHYS 260 |
Synchrotron radiation | PHYS 360 | |
Processes involving | ||
Decay in flight | CONS 310 | PHYS 400 |
Multiple scattering | PHYS 320or 325 | |
Ionisation and -rays production | PHYS 430 | PHYS 331or 332 |
Ionisation by heavy ions | PHYS 431 | |
Bremsstrahlung | PHYS 440 | PHYS 441 |
Direct ( ) pair production | PHYS 450 | PHYS 451 |
Nuclear interaction | PHYS 460 | PHYS 460 |
Generation of Cerenkov light | PHYS 260 | PHYS 260 |
Processes involving hadrons | ||
Decay in flight | CONS 310 | PHYS 400 |
Multiple scattering | PHYS 320or 325 | |
Ionisation and -rays production | PHYS 430 | PHYS 331or 332 |
Hadronic interactions | PHYS 500 or 510 | PHYS 500 or 510 |
Generation of Cerenkov light | PHYS 260 | PHYS 260 |
Table: Processes currently implemented in GEANT