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In case (1), this effect is important only if the decay channels are relativistic, thus adding a lot of entropy into the universe. In this project, we will consider the injection of neutrons, so we will not consider this effect. | In case (1), this effect is important only if the decay channels are relativistic, thus adding a lot of entropy into the universe. In this project, we will consider the injection of neutrons, so we will not consider this effect. | ||
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+ | It is thus the goal of this project to investigate the effect of the injection of non-thermal neutrons on the light element abundances. | ||
**Key parameters: ** | **Key parameters: ** | ||
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- The abundance of X. | - The abundance of X. | ||
- n interaction rates with every other nucleus. | - n interaction rates with every other nucleus. | ||
+ | - Mass of the WIMP. Chosen to be 100 GeV, based on the wikipedia WIMP entry, the font of all wisdom. | ||
+ | This figure: | ||
+ | {{::cdms_parameter_space_2004.png?600|}} | ||
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+ | from CDMS in 2004 suggests that this value isn't too far off. | ||
Reference Papers: | Reference Papers: | ||
- | Cyburt et. al. 2009 Nucleosynthesis Constraints on a Massive Gravitino in Neutralino Dark Matter Scenario [[http://arxiv.org/pdf/0907.5003v1.pdf]] | + | Cyburt et. al. 2009. Nucleosynthesis Constraints on a Massive Gravitino in Neutralino Dark Matter Scenario [[http://arxiv.org/pdf/0907.5003v1.pdf]] |
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+ | Kamionkowski 1994. Diffuse Gamma Rays from WIMP Decay and Annihilation [[http://arxiv.org/pdf/astro-ph/9404079v1.pdf]] | ||
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+ | Pierre Salati, 2014. Dark Matter Annihilation in the Universe [[http://arxiv.org/pdf/1403.4495.pdf]] | ||
**Logbook** | **Logbook** |