| Geant4 Cross Reference |
1 1
2 Geant4 extended examples - Hadronic pr 2 Geant4 extended examples - Hadronic processes
3 -------------------------------------- 3 ----------------------------------------------
4 4
5 Examples in this directory demonstrate specif 5 Examples in this directory demonstrate specific hadronic physics simulation
6 with histogramming. 6 with histogramming.
7 7
8 Hadr00 8 Hadr00
9 ------ 9 ------
10 10
11 This example demonstrates a usage of G4PhysLis 11 This example demonstrates a usage of G4PhysListFactory to build
12 Physics List and G4HadronicProcessStore to acc 12 Physics List and G4HadronicProcessStore to access cross sections.
13 13
14 Hadr01 14 Hadr01
15 ------ 15 ------
16 16
17 This example application is based on the appli 17 This example application is based on the application IION developed for
18 simulation of proton or ion beam interaction w 18 simulation of proton or ion beam interaction with a water target. Different
19 aspects of beam target interaction are demonst 19 aspects of beam target interaction are demonstrating in the example including
20 longitudinal profile of energy deposition, spe 20 longitudinal profile of energy deposition, spectra of secondary particles,
21 spectra of particles leaving the target. 21 spectra of particles leaving the target.
22 22
23 Hadr02 23 Hadr02
24 ------ 24 ------
25 25
26 This example application is providing simulati 26 This example application is providing simulation of ion beam interaction with different
27 targets. Hadronic aspects of beam target inter 27 targets. Hadronic aspects of beam target interaction are demonstrated in the example
28 including longitudinal profile of energy depos 28 including longitudinal profile of energy deposition, spectra of secondary particles,
29 isotope production spectra. 29 isotope production spectra.
30 30
31 Hadr03 31 Hadr03
32 ------ 32 ------
33 33
34 This example demonstrates how to compute total 34 This example demonstrates how to compute total cross section from the direct evaluation of the
35 mean free path ( see below, item Physics), how 35 mean free path ( see below, item Physics), how to identify nuclear reactions, how to plot
36 energy spectrum of secondary particles. 36 energy spectrum of secondary particles.
37 37
38 Hadr04 38 Hadr04
39 ------ 39 ------
40 40
41 This example is focused on neutronHP physics, 41 This example is focused on neutronHP physics, especially neutron transport,
42 including thermal scattering. 42 including thermal scattering.
43 See A.R. Garcia, E. Mendoza, D. Cano-Ott prese 43 See A.R. Garcia, E. Mendoza, D. Cano-Ott presentation at G4 Hadronic group
44 meeting (04/2013) and note on G4NeutronHP pack 44 meeting (04/2013) and note on G4NeutronHP package
45 45
46 Hadr05 <<
47 ------ <<
48 <<
49 Examples of hadronic calorimeters <<
50 <<
51 Hadr06 46 Hadr06
52 ------ 47 ------
53 48
54 This example demonstrates survey of energy dep 49 This example demonstrates survey of energy deposition and particle's flux from
55 a hadronic cascade. 50 a hadronic cascade.
56 51
57 Hadr07 52 Hadr07
58 ------ 53 ------
59 54
60 Survey energy deposition and particle's flux f 55 Survey energy deposition and particle's flux from an hadronic cascade.
61 Use PhysicsConstructor objects rather than pre 56 Use PhysicsConstructor objects rather than predefined G4 PhysicsLists.
62 Show how to plot a depth dose profile in a rec 57 Show how to plot a depth dose profile in a rectangular box.
63 58
64 Hadr08 <<
65 ------ <<
66 <<
67 This example shows how to get "hadronic model <<
68 biasing: in particular, it is shown how to use <<
69 while using the default "FTFP+BERT" in all oth <<
70 Notice that we use the generic biasing machine <<
71 of all tracks remain to the usual value (1.0) <<
72 case. <<
73 <<
74 Hadr09 <<
75 ------ <<
76 <<
77 This example shows how to use Geant4 as a gene <<
78 inelastic hadron-nuclear interactions. <<
79 Notice that the Geant4 run-manager is not used <<
80 <<
81 Hadr10 <<
82 ------ <<
83 <<
84 This example aims to test the treatment of dec <<
85 In particular, we want to test the decays of t <<
86 bottom hadrons, and the use of pre-assigned de <<
87 <<
88 FissionFragment 59 FissionFragment
89 --------------- 60 ---------------
90 This example demonstrates the Fission Fragment 61 This example demonstrates the Fission Fragment model as used within the
91 neutron_hp model. It will demostrate the capab 62 neutron_hp model. It will demostrate the capability for fission product
92 containmentby the cladding in a water moderate 63 containmentby the cladding in a water moderated sub-critical assembly. It could
93 also be further extended to calculate the effe 64 also be further extended to calculate the effective multiplication factor of
94 the subcritical assembly for various loading s 65 the subcritical assembly for various loading schemes.
95 66
96 FlukaCern <<
97 ------------- <<
98 A set of 2 examples, demonstrating how to make <<
99 the interface to `FLUKA` hadron-nucleus inelas <<
100 The examples are at the process (interaction) <<
101 (G4_HP_CernFLUKAHadronInelastic_PhysicsList) i <<
102 The interface to `FLUKA` itself is also includ <<
103 <<
104 NeutronSource 67 NeutronSource
105 ------------- 68 -------------
106 NeutronSource is an example of neutrons produc 69 NeutronSource is an example of neutrons production. It illustrates the cooperative work
107 of nuclear reactions and radioactive decay pro 70 of nuclear reactions and radioactive decay processes.
108 It survey energy deposition and particle's flu 71 It survey energy deposition and particle's flux.
109 It uses PhysicsConstructor objects. 72 It uses PhysicsConstructor objects.
110 73
111 ParticleFluence << 74 The example Hadr05, which demonstrated the usage of G4GenericPhysicsList to build
112 --------------- << 75 the concrete physics list at the run time, has been repleced in Geant4 10.4 by
113 This example aims to monitor the particle flue << 76 extended/physicslists/genericPL the generic physics list was demonstrated in the
114 and set-ups. The particle fluence at a given p << 77 extended/hadronic/Hadr05 example.
115 average number of particles crossing a unit su <<
116 (normalized per one incident primary). The par <<
117 estimated by summing the particles' track leng <<
118 and dividing for the cubic volume of such a sc <<