micrOMEGAs 2.0.7: a program to calculate the relic density of dark matter in a generic model
By G. B'elanger, Fawzi Boudjema, Alexander Pukhov, A. Semenov. Computer Physics Communications, 2006
742 citations recorded by the source corpus.
micrOMEGAs2.0 is a code which calculates the relic density of a stable massive particle in an arbitrary model. The underlying assumption is that there is a conservation law like R-parity in supersymmetry which guarantees the stability of the lightest odd particle. The new physics model must be incorporated in the notation of CalcHEP, a package for the automatic generation of squared matrix elements. Once this is done, all annihilation and coannihilation channels are included automatically in any model. Cross-sections at v = 0, relevant for indirect detection of dark matter, are also computed automatically. The package includes three sample models: the minimal supersymmetric standard model (MSSM), the MSSM with complex phases and the NMSSM. Extension to other models, including non supersymmetric models, is described.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/948fcaaa18169b862752a02d1abeaebea4ecc199
How researchers see this paper
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In Astronomy and Astrophysics
- M. Raidal
- G. Arcadi
- Abdelhak Djouadi
- K. Kannike
- Igor P. Ivanov
- Alexander Pukhov
- G. B'elanger
- M. Maniatis
In Nuclear and High Energy Physics
- M. Raidal
- Igor P. Ivanov
- G. Arcadi
- Alexander Pukhov
- Abdelhak Djouadi
- G. B'elanger
- K. Kannike
- Fawzi Boudjema
Citations in the corpus
- Collider limits on new physics within micrOMEGAs4.3 (2016, positive): “The user can also implement his/her own model in micrOMEGAs, this requires creating model files in the CalcHEP format, see [8] for details.”
- micrOMEGAs_3: A program for calculating dark matter observables (2013, methodology): “y final states (full) and only 2-body final states (dash). 2.5 New functions and switches As in previous versions, the relic density computation is performed with the function darkOmega as described in [53], new features include the 3-body final state, which can be taken into account by specifying •VWd”