Abstract
If, during the early Universe epoch, the dark matter particle thermalizes in a hidden sector which does not thermalize with the Standard Model thermal bath, its relativistic thermal decoupling can easily lead to the observed relic density, even if the dark matter particle mass is many orders of magnitude heavier than the usual ∼ eV hot relic mass scale. This straightforward scenario simply requires that the temperature of the hidden sector thermal bath is one to five orders of magnitude cooler than the temperature of the Standard Model thermal bath. In this way the resulting relic density turns out to be determined only by the dark matter mass scale and the ratio of the temperatures of both sectors. In a model independent way we determine that this can work for a dark matter mass all the way from ∼1 keV to ∼30 PeV. We also show how this scenario works explicitly in the framework of two illustrative models. One of them can lead to a PeV neutrino flux from dark matter decay of the order of the one needed to account for the high energy neutrinos observed by IceCube.
Highlights
If, during the early Universe epoch, the dark matter particle thermalizes in a hidden sector which does not thermalize with the Standard Model thermal bath, its relativistic thermal decoupling can lead to the observed relic density, even if the dark matter particle mass is many orders of magnitude heavier than the usual ∼ eV hot relic mass scale
This scenario is quite different from the case of a relativistic dark matter (DM) decoupling, which leads to a suppressed enough relic density only if the DM mass is around a scale as low as the ∼ 10 eV scale
This Weakly Interacting Massive Particle (WIMP) miracle remains as of today the most straightforward, and in many ways the most attractive, possibility to account for the DM relic density
Summary
If, during the early Universe epoch, the dark matter particle thermalizes in a hidden sector which does not thermalize with the Standard Model thermal bath, its relativistic thermal decoupling can lead to the observed relic density, even if the dark matter particle mass is many orders of magnitude heavier than the usual ∼ eV hot relic mass scale. We show that relativistic or almost relativistic thermal decoupling within the hidden sector can straightforwardly lead to the observed relic density for DM masses much larger than in the ordinary freeze-out scenario with a single thermal bath.
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