Abstract
We study the effects of modifying the expansions history of the Universe on Dark Matter freezeout. We derived a modified Boltzmann equation for freeze-out for an arbitrary energy density in the early Universe and provide an analytic approach using some approximations. We then look at the required thermally averaged cross sections needed to obtain the correct relic density for the specific case where the energy density consists of radiation plus one extra component which cools faster. We compare our analytic approximation to a numerical solutions. We find that it gives reasonable results for most of the parameter space explored, being at most a factor of order one away from the measured value. We find that if the new contribution to the energy density is comparable to the radiation density, then a much smaller cross section for Dark Matter annihilation is required. This would lead to weak scale Dark Matter being much more difficult to detect and opens up the possibility that much heavier Dark Matter could undergo freezeout without violating perturbative unitarity.
Highlights
Dark matter is still one of the biggest unsolved puzzles in modern physics
If one wishes to construct a particle physics model which can explain dark matter, they must ensure that its interactions are quite weak to avoid all these constraints
The dark matter starts in thermal equilibrium with the Standard Model at an early time but eventually decouples once the rate of the reactions maintaining chemical equilibrium become comparable to the expansion rate of the Universe [1,2,3,4,5,6,8]
Summary
Dark matter is still one of the biggest unsolved puzzles in modern physics. It continues to escape detection in both direct and indirect detection experiments while collider experiments have yet to be able to identify a statistically significant dark matter signal. A popular production mechanism that has been studied is freeze-out In this scenario, the dark matter starts in thermal equilibrium with the Standard Model at an early time but eventually decouples once the rate of the reactions maintaining chemical equilibrium become comparable to the expansion rate of the Universe [1,2,3,4,5,6,8]. ALEXANDRE POULIN decay away [28,29,30,31] All these models have a different expansion rate from the standard ΛCMD model and some previous work has been done to understand the physics in these scenarios [32,33,34,35].
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