| Geant4 Cross Reference |
1 ------------------------------------------------------------------- 2 3 4 G4HadronInelasticQBBC 5 --------------------- 6 Hadron nuclear inelastic processes for all hadrons: 7 - proton inelastic: 8 - cross section: G4ParticleInelasticXS 9 - final-state: Fritiof coupled with Precompound/de-excitation (FTFP) above 3 GeV; 10 Bertini (BERT) between 1 and 6 GeV; 11 Binary coupled with Precompound/de-excitation (BIC) below 1.5 GeV 12 - neutron inelastic: 13 - cross section: G4NeutronInelasticXS 14 - final-state: FTFP > 3 GeV; 1 GeV < BERT < 6 GeV; BIC < 1.5 GeV 15 neutron capture: 16 - cross section: G4NeutronCaptureXS 17 - final-state: G4NeutronRadCapture 18 - charged pions inelastic: 19 - cross section: Barashenkov-Glauber-Gribov 20 - final-state: FTFP > 3 GeV; 1 GeV < BERT < 12 GeV; BIC < 1.5 GeV 21 - kaons inelastic: 22 - cross section: Glauber-Gribov 23 - final-state: FTFP > 3 GeV; BERT < 6 GeV 24 - hyperons inelastic: 25 - cross section: Glauber-Gribov 26 - final-state: FTFP > 3 GeV; BERT < 6 GeV 27 - anti_proton, anti_neutron, anti_deuteron, anti_triton, anti_He3, anti_alpha inelastic: 28 - cross-section: Galoyan-Uzhinsky-Glauber-Gribov 29 - final-state: FTFP for all energies 30 - anti_hyperons inelastic: 31 - cross section: Glauber-Gribov 32 - final-state: FTFP for all energies 33 - charm and bottom hadrons inelastic: 34 - cross section: Glauber-Gribov 35 - final-state: FTFP for all energies 36 37 38 G4HadronInelasticQBBC_ABLA 39 -------------------------- 40 Similar to G4HadronInelasticQBBC, with the difference that for the final-state 41 of nuclear inelastic interactions of pion+, pion-, proton and neutron projectiles 42 the ABLA model (instead of the usual Precompound/de-excitation) is utilized for 43 nuclear de-excitation. 44 45 46 G4HadronPhysicsFTFP_BERT 47 ------------------------ 48 Hadron nuclear inelastic processes for all hadrons: 49 - proton inelastic: 50 - cross section: Barashenkov-Glauber-Gribov (G4BGGNucleonInelasticXS) 51 - final-state: FTFP > 3 GeV; BERT < 6 GeV 52 - neutron inelastic: 53 - cross section: G4NeutronInelasticXS 54 - final-state: FTFP > 3 GeV; BERT < 6 GeV 55 neutron capture: 56 - cross section: G4NeutronCaptureXS 57 - final-state: G4NeutronRadCapture 58 - charged pions inelastic: 59 - cross section: Barashenkov-Glauber-Gribov 60 - final-state: FTFP > 3 GeV; BERT < 6 GeV 61 - kaons inelastic: 62 - cross section: Glauber-Gribov 63 - final-state: FTFP > 3 GeV; BERT < 6 GeV 64 - hyperons inelastic: 65 - cross section: Glauber-Gribov 66 - final-state: FTFP > 3 GeV; BERT < 6 GeV 67 - anti_proton, anti_neutron, anti_deuteron, anti_triton, anti_He3, anti_alpha inelastic: 68 - cross-section: Galoyan-Uzhinsky-Glauber-Gribov 69 - final-state: FTFP for all energies 70 - anti_hyperons inelastic: 71 - cross section: Glauber-Gribov 72 - final-state: FTFP for all energies 73 - charm and bottom hadrons inelastic: 74 - cross section: Glauber-Gribov 75 - final-state: FTFP for all energies 76 - light hypernuclei inelastic: 77 - cross section: Glauber-Gribov 78 - final-state: FTFP for all energies 79 - light anti-hypernuclei inelastic: 80 - cross-section: Galoyan-Uzhinsky-Glauber-Gribov 81 - final-state: FTFP for all energies 82 83 84 G4HadronPhysicsFTFP_BERT_ATL 85 ---------------------------- 86 Similar to G4HadronPhysicsFTFP_BERT, with the difference that for proton, 87 neutron, pions and kaons, the FTFP is used above 9 GeV and BERT below 12 GeV 88 (i.e. transition between these two models is in the interval [9, 12] GeV 89 for the most frequent hadrons). 90 91 92 G4HadronPhysicsFTFP_BERT_HP 93 -------------------------- 94 Similar to G4HadronPhysicsFTFP_BERT, but with a different treatment of 95 low-energy neutrons: 96 - neutron inelastic: use NeutronHP (for both cross section and final state) 97 below 20 MeV; above G4NeutronCaptureXS cross section; 98 final-state: BERT between 19.9 MeV and 6 GeV, 99 FTFP above 3 GeV. 100 - neutron capture: use NeutronHP (for both cross section and final state) 101 below 20 MeV; above G4NeutronCaptureXS cross section 102 and G4NeutronRadCapture final-state. 103 - neutron fission: use NeutronHP (for both cross section and final state) 104 below 20 MeV; above Gheisha (cross section and final state). 105 Moreover, RadioactiveDecay is activated (as in all the physics lists that use HP). 106 107 108 G4HadronPhysicsFTFP_BERT_TRV 109 ---------------------------- 110 The same as G4HadronPhysicsFTFP_BERT. 111 112 113 G4HadronPhysicsFTF_BIC 114 ---------------------- 115 Similar to G4HadronPhysicsFTFP_BERT, with the following differences: 116 - For proton and neutron, BIC is used (instead of BERT) below 6 GeV 117 - For pions, BIC is used below 1.5 GeV, whereas BERT is used in the 118 interval 1 GeV < BERT < 6 GeV 119 - FTF is coupled with BIC (instead of directly to Precompound/de-excitation). 120 121 122 G4HadronPhysicsQGS_BIC 123 ---------------------- 124 Similar to G4HadronPhysicsFTP_BIC, except that QGSP is used above 12 GeV 125 and FTFP below 25 GeV. 126 127 128 G4HadronPhysicsFTFQGSP_BERT 129 --------------------------- 130 Similar to G4HadronPhysicsFTFP_BERT, but with QGS fragmentation of strings 131 (instead of the Lund string fragmentation). 132 133 134 G4HadronPhysicsINCLXX 135 --------------------- 136 Similar to QGSP_BERT except for: 137 - proton inelastic: 138 - cross section: Barashenkov-Glauber-Gribov (G4BGGNucleonInelasticXS) 139 - final-state: QGSP > 15 GeV; 1 MeV < INCLXX < 20 GeV; Preco < 2 MeV 140 - neutron inelastic: 141 - cross section: G4NeutronInelasticXS 142 - final-state: QGSP > 15 GeV; 1 MeV < INCLXX < 20 GeV; Preco < 2 MeV 143 - charged pions inelastic: 144 - cross section: Barashenkov-Glauber-Gribov 145 - final-state: QGSP > 15 GeV; 1 MeV < INCLXX < 20 GeV; Preco < 2 MeV 146 - kaons inelastic: 147 - cross section: Glauber-Gribov 148 - final-state: QGSP > 14 GeV; BERT < 15 GeV 149 - light hypernuclei inelastic: 150 - cross section: Glauber-Gribov 151 - final-state: FTFP > 15 GeV; 1 MeV < INCLXX < 20 GeV; Preco < 2 MeV 152 - light anti-hypernuclei inelastic: 153 - cross-section: Galoyan-Uzhinsky-Glauber-Gribov 154 - final-state: FTFP for all energies 155 Note: it is possible to specify in the constructor the use of FTFP 156 instead of QGSP; 157 moreover, NeutronHP can also be activated in the constructor, 158 in which case inelastic, capture and fission below 20 MeV are 159 taken from NeutronHP (both cross section and final-state). 160 161 162 G4HadronPhysicsNuBeam 163 --------------------- 164 Similar to FTFP_BERT, except for the final-state models of proton: 165 - proton : QGSP with Lund string fragmentation > 100 GeV; 166 3 GeV < FTFP < 101 GeV; BERT < 6 GeV 167 168 169 G4HadronPhysicsQGSP_BERT 170 ------------------------ 171 Hadron nuclear inelastic processes for all hadrons: 172 - proton inelastic: 173 - cross section: Barashenkov-Glauber-Gribov (G4BGGNucleonInelasticXS) 174 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BERT < 6 GeV 175 - neutron inelastic: 176 - cross section: G4NeutronInelasticXS 177 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BERT < 6 GeV 178 neutron capture: 179 - cross section: G4NeutronCaptureXS 180 - final-state: G4NeutronRadCapture 181 - charged pions inelastic: 182 - cross section: Barashenkov-Glauber-Gribov 183 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BERT < 6 GeV 184 - kaons inelastic: 185 - cross section: Glauber-Gribov 186 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BERT < 6 GeV 187 - hyperons inelastic: 188 - cross section: Glauber-Gribov 189 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BERT < 6 GeV 190 - anti_proton and anti_neutron inelastic: 191 - cross-section: Galoyan-Uzhinsky-Glauber-Gribov 192 - final-state: QGSP > 12 GeV; FTFP < 25 GeV 193 - anti_deuteron, anti_triton, anti_He3, and anti_alpha inelastic: 194 - cross-section: Galoyan-Uzhinsky-Glauber-Gribov 195 - final-state: FTFP for all energies 196 - anti_hyperons inelastic: 197 - cross section: Glauber-Gribov 198 - final-state: QGSP > 12 GeV; FTFP < 25 GeV 199 - charm and bottom hadrons inelastic: 200 - cross section: Glauber-Gribov 201 - final-state: QGSP > 12 GeV; FTFP < 25 GeV 202 203 204 G4HadronPhysicsQGSP_FTFP_BERT 205 ----------------------------- 206 Currently it is the same as QGSP_BERT (this was not the case before G4 10.6). 207 It might be removed in future versions of Geant4. 208 209 210 G4HadronPhysicsQGSP_BERT_HP 211 --------------------------- 212 Similar to G4HadronPhysicsQGSP_BERT, but with a different treatment of 213 low-energy neutrons: 214 - neutron inelastic: for cross section, use G4NeutronHPInelasticXS 215 below 20 MeV, and G4NeutronInelasticXS above; 216 for final-state model, use G4NeutronHPInelasticVI 217 below 20 MeV, BERT between 19.9 MeV and 6 GeV, 218 FTFP between 3 and 25 GeV, QGSP above 12 GeV. 219 - neutron capture: use G4NeutronHPCaptureXS cross section and 220 G4NeutronRadCaptureHP final-state model 221 (Note: if NuDEX is enabled (by default it is not), 222 then G4NuDEXNeutronCaptureModel final-state 223 model is used instead of G4NeutronRadCaptureHP). 224 - neutron fission: use G4NeutronHPFissionXS cross section and 225 G4NeutronFissionVI final-state model. 226 Moreover, RadioactiveDecay is activated (as in all the physics lists that use HP) 227 Important warning: since G4 11.2, this constructor is different than all 228 other HP-based constructors for the treatment of neutrons 229 below 20 MeV : new "experimental" cross sections and 230 final-state models - which are different from the HP ones - 231 are utilised for testing, and therefore we recommend to 232 not using them for physics studies. 233 234 G4HadronPhysicsQGSP_BIC 235 ----------------------- 236 Hadron nuclear inelastic processes for all hadrons: 237 - proton inelastic: 238 - cross section: Barashenkov-Glauber-Gribov (G4BGGNucleonInelasticXS) 239 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BIC < 6 GeV 240 - neutron inelastic: 241 - cross section: G4NeutronInelasticXS 242 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BIC < 6 GeV 243 neutron capture: 244 - cross section: G4NeutronCaptureXS 245 - final-state: G4NeutronRadCapture 246 - charged pions inelastic: 247 - cross section: Barashenkov-Glauber-Gribov 248 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BERT < 6 GeV 249 - kaons inelastic: 250 - cross section: Glauber-Gribov 251 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BERT < 6 GeV 252 - hyperons inelastic: 253 - cross section: Glauber-Gribov 254 - final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; BERT < 6 GeV 255 - anti_proton and anti_neutron inelastic: 256 - cross-section: Galoyan-Uzhinsky-Glauber-Gribov 257 - final-state: QGSP > 12 GeV; FTFP < 25 GeV 258 - anti_deuteron, anti_triton, anti_He3, and anti_alpha inelastic: 259 - cross-section: Galoyan-Uzhinsky-Glauber-Gribov 260 - final-state: FTFP for all energies 261 - anti_hyperons inelastic: 262 - cross section: Glauber-Gribov 263 - final-state: QGSP > 12 GeV; FTFP < 25 GeV 264 265 266 G4HadronPhysicsQGSP_BIC_HP 267 -------------------------- 268 Similar to G4HadronPhysicsQGSP_BIC, but with a different treatment of 269 low-energy neutrons: 270 - neutron inelastic: use NeutronHP (for both cross section and final state) 271 below 20 MeV; above G4NeutronCaptureXS cross section; 272 final-state: BIC between 19.9 MeV and 6 GeV, 273 FTFP between 3 and 25 GeV, QGSP above 12 GeV. 274 - neutron capture: use NeutronHP (for both cross section and final state) 275 below 20 MeV; above G4NeutronCaptureXS cross section 276 and G4NeutronRadCapture final-state. 277 - neutron fission: use NeutronHP (for both cross section and final state) 278 below 20 MeV; above Gheisha (cross section and final state). 279 Moreover, RadioactiveDecay is activated (as in all the physics lists that use HP). 280 281 282 G4HadronPhysicsQGSP_BIC_AllHP 283 ----------------------------- 284 Similar to G4HadronPhysicsQGSP_BIC_HP, but with a different treatment of 285 low-energy protons: 286 ParticleHP is used (for both cross section and final state) below 200 MeV; 287 above it: Barashenkov-Glauber-Gribov inelastic cross section; 288 final-state: QGSP > 12 GeV; 3 GeV < FTFP < 25 GeV; 190 MeV < BIC < 6 GeV. 289 290 291 G4HadronPhysicsShielding 292 ------------------------ 293 Similar to G4HadronPhysicsFTFP_BERT_HP except for using 294 JENDLHEInelasticCrossSection for the neutron inelastic cross section 295 above 20 MeV. 296 Note: the variant "M" of the Shielding physics list has a transition region 297 between FTFP and BERT for pions between 9.5 and 9.9 GeV 298 (instead of 3-6 GeV). 299 300 301 G4HadronPhysicsShieldingLEND 302 ---------------------------- 303 Similar to G4HadronPhysicsShielding, except that LEND is used for neutrons 304 below 20 MeV instead of NeutronHP. 305 306 307 G4VHadronPhysics 308 ---------------- 309 Utility class which provides useful methods. 310 311 312 G4URRNeutrons 313 ------------- 314 Physics list constructor that can be applied on top of any _HP or _HPT based 315 physics list, to enable the special Unresolved Resonance Region (URR) treatment 316 of low-energy neutrons based on Particle Table (PT). 317 Notes: 318 - If this constructor is applied on top of a non-HP based physics list, 319 then nothing changes and a warning is printed out. 320 - If this constructor is applied on top of a HP-based physics list, 321 and the thermal scattering is applied after G4URRNeutrons, then 322 there will be a problem of full overlappings between models. 323 Therefore, if you need thermal scattering, activate it (e.g. by 324 using a HPT-based physics list) before applying G4URRNeutrons.