|
- Timestamp:
-
Feb 23, 2020, 3:11:52 PM (5 years ago)
- Author:
-
mosel
- Comment:
-
--
Legend:
- Unmodified
- Added
- Removed
- Modified
-
v382
|
v383
|
|
15 | 15 | using the same physics input and code. The GiBUU code provides a full dynamical description of the reaction and delivers the complete final state of an event; it can thus be used as an '''event generator'''. The code is freely available. |
16 | 16 | |
17 | | For all the reactions, the flow of particles is modelled within a [wiki:physicsInput Boltzmann-Uehling-Uhlenbeck (BUU) framework]. |
18 | | The relevant degrees of freedom are '''mesons''' and '''baryons''', which propagate in mean fields and scatter according to cross sections which are applicable to the energy range of a few 10 MeV to about 40 GeV. In the higher energy regimes the concept of '''pre-hadronic''' interactions is implemented in order to realize ''color transparancy'' and ''formation time'' effects. For a general overview of the model, its theoretical basis as well as many practical details, refer to the review paper: |
| 17 | For all the reactions, the flow of particles is modeled within a [wiki:physicsInput Boltzmann-Uehling-Uhlenbeck (BUU) framework]. |
| 18 | The relevant degrees of freedom are '''mesons''' and '''baryons''', which propagate in mean fields and scatter according to cross sections which are applicable to the energy range of a few 10 MeV to about 40 GeV. In the higher energy regimes the concept of '''pre-hadronic''' interactions is implemented in order to realize ''color transparency'' and ''formation time'' effects. For a general overview of the model, its theoretical basis as well as many practical details, refer to the review paper: |
19 | 19 | |
20 | 20 | '''Transport-theoretical Description of Nuclear Reactions'''[[br]] |
|