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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
FissionFragment Example
B.Wendt brycen.linn.wendt@cern.ch

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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
HADR00
V.Ivanchenko CERN, Geneva, Switzerland

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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
HADR01
A.Bagulya, I.Gudowska, V.Ivanchenko, N.Starkov CERN, Geneva, Switzerland Karolinska Institute & Hospital, Stockholm, Sweden Lebedev Physical Institute, Moscow, Russia

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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
HADR02
Example and DMJET: V.Ivanchenko, A.Ivanchenko, UrQMD: Kh Abdel-Waged et al, A. Dotti CRMC: A. Ribon (with contributions by T. Pierog and A. Tykhonov) CERN, Geneva, Switzerland Geant4 Associate International University of Bordeaux, CENBG/IN2P3/CNRS (ESA contract 22712/09/NL/AT)

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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
Hadr03
How to compute total cross section from the direct evaluation of the mean free path ( see below, item Physics). How to identify nuclear reactions. How to plot energy spectrum of secondary particles.

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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
Hadr04
This example is focused on neutronHP physics, especially neutron transport, including thermal scattering. See A.R. Garcia, E. Mendoza, D. Cano-Ott presentation at G4 Hadronic group meeting (04/2013) and note on G4NeutronHP package

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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
Hadr05
How to collect energy deposition in a sampling calorimeter. How to survey energy flow. Hadr05 is the hadronic equivalent of TestEm3.

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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
Hadr06
Survey energy deposition and particle's flux from an hadronic cascade. Use PhysicsConstructor objects rather than predefined G4 PhysicsLists.
1- MATERIALS AND GEOMETRY DEFINITION

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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
Hadr07
Survey energy deposition and particle's flux from an hadronic cascade. Use PhysicsConstructor objects rather than predefined G4 PhysicsLists. Show how to plot a depth dose profile in a rectangular box.

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This is an example of how to use "generic biasing" to get the following functionality which is currently not available directly in the Geant4 hadronic framework.
We want to use the physics list FTFP_BERT everywhere in our detector, except that in one (or more) logical volume(s) we want to use a different combination of hadronic models, e.g. FTFP + INCLXX (instead of the default FTFP + BERT), for the final-state generation.

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This example shows how to use Geant4 as a generator for simulating inelastic hadron-nuclear interactions.
The class HadronicGenerator is the "generator". The main hadronic models (FTFP, QGSP, BERT, BIC, IonBIC, INCL) and some combinations of two of them - in a transition energy region, similarly to what happens in physics lists - are available. See include/HadronicGenerator.hh for more detailed information.

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This is an example that aims to test the treatment of decays in Geant4. In particular, we want to test the decays of the tau lepton, charmed and bottom hadrons, and the use of pre-assigned decays.
Note that pre-assigned decays are decays that are usually specified by Monte Carlo event generators. For simplicity, and to avoid dependencies on external code, in this test we don't use any MC generator, and we pre-assign decays by hand (using the Geant4 decay table: this is done in the method SteppingAction::UserSteppingAction). But this does not change anything regarding the testing of the pre-assignment mechanism of Geant4.

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Geant4 - an Object-Oriented Toolkit for Simulation in HEP
NeutronSource
NeutronSource is an example of neutrons production. It illustrates the cooperative work of nuclear reactions and radioactive decay processes. It survey energy deposition and particle's flux. It uses PhysicsConstructor objects.

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ParticleFluence set-ups
Sphere
This set-up consists of a full solid target sphere - whose radius and material can be set via UI commands. The primary particle is shot from the center of the target sphere (along the z-axis direction by default). As scoring volume, we use a thin spherical shell outside the target sphere. The particle fluences are evaluated in the forward and backward hemispheres (with respect to the primary particle direction).

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