2015
DOI: 10.1103/physrevd.92.055033
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Hidden dark matter sector, dark radiation, and the CMB

Abstract: We consider theories where dark matter is composed of a thermal relic of weak scale mass, whose couplings to the Standard Model (SM) are however too small to give rise to the observed abundance. Instead, the abundance is set by annihilation to light hidden sector states that carry no charges under the SM gauge interactions. In such a scenario the constraints from direct and indirect detection, and from collider searches for dark matter, can easily be satisfied. The masses of such light hidden states can be pro… Show more

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Cited by 89 publications
(103 citation statements)
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References 126 publications
(159 reference statements)
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“…Very light states (m eV) increase the radiation density at recombination, leaving an imprint on the CMB. This effect is usually expressed as an equivalent number of additional neutrino species [121][122][123][124][125], with measurements limiting ∆N CM B ef f < 0.30 [2]. More massive states can avoid the CMB bound, but can modify the expansion rate during BBN, with the limit for masses below m MeV given by ∆N BBN ef f 0.5 [126].…”
Section: Probing New Degrees Of Freedommentioning
confidence: 99%
“…Very light states (m eV) increase the radiation density at recombination, leaving an imprint on the CMB. This effect is usually expressed as an equivalent number of additional neutrino species [121][122][123][124][125], with measurements limiting ∆N CM B ef f < 0.30 [2]. More massive states can avoid the CMB bound, but can modify the expansion rate during BBN, with the limit for masses below m MeV given by ∆N BBN ef f 0.5 [126].…”
Section: Probing New Degrees Of Freedommentioning
confidence: 99%
“…In the very early time of our universe, shortly after the hot Big Bang, WIMP DM maintains in thermal equilibrium with the SM particles via rapid 2-to-2 annihilation (for variations such as annihilating into dark sector particles, see for instance, Refs. [7][8][9][10]. This annihilation rate is approximately Γ ann ∼ n eq χ σ ann v , where n eq χ is the number density of χ following the equilibrium distribution.…”
Section: Thermal History Of a Wimp-type Of Particlementioning
confidence: 96%
“…In calculating the relic abundance of χ, we follow the semi-analytic approach as detailed in Refs. [50] and [74],…”
Section: A Equilibrationmentioning
confidence: 99%