2013
DOI: 10.1088/1475-7516/2013/08/041
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A lower bound on the mass of cold thermal dark matter from Planck

Abstract: We show that the new measurement of the effective number of neutrinos (N eff ) by the Planck satellite can be used to set a robust lower bound on the mass of cold thermal dark matter of O(MeV). Our limit applies if the dark matter remains in thermal equilibrium by coupling to electrons and photons or through interactions with neutrinos, and applies regardless of whether the dark matter annihilation cross-section is s-wave or p-wave. To illustrate our bounds we apply them to a model of a supersymmetric neutrali… Show more

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Cited by 217 publications
(123 citation statements)
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References 137 publications
(226 reference statements)
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“…Figure 11 shows a plot of the m χ − ϵ parameter space of this model with several relevant constraints. Sufficiently light millicharged DM remains in thermal equilibrium with electrons and photons until after neutrinos decouple from the SM, altering the N eff measurement from the CMB power spectrum [51]. Since the irreducible annihilation to e þ e − heats the baryons, by requiring T m ðz ¼ 17.2Þ ≤ 4 K, 2 we can set an upper limit of ϵ ≲ 5 × 10 −5 , cutting the remaining parameter space down to a narrow window between m χ ∼10-100MeV and ϵ ∼ 5 × 10 −6 to 5 × 10 −5 .…”
Section: F Millicharged Dmmentioning
confidence: 99%
“…Figure 11 shows a plot of the m χ − ϵ parameter space of this model with several relevant constraints. Sufficiently light millicharged DM remains in thermal equilibrium with electrons and photons until after neutrinos decouple from the SM, altering the N eff measurement from the CMB power spectrum [51]. Since the irreducible annihilation to e þ e − heats the baryons, by requiring T m ðz ¼ 17.2Þ ≤ 4 K, 2 we can set an upper limit of ϵ ≲ 5 × 10 −5 , cutting the remaining parameter space down to a narrow window between m χ ∼10-100MeV and ϵ ∼ 5 × 10 −6 to 5 × 10 −5 .…”
Section: F Millicharged Dmmentioning
confidence: 99%
“…When ϕ becomes nonrelativistic and decays, its entropy is dumped either into some hidden sector bath (which would heat that bath relative to the SM bath) or into the SM bath, heating it further. If m ϕ ≳ 5 MeV when it decays to the SM (whether to electrons or neutrinos), there is little effect on BBN or cosmic microwave background (CMB) measurements of the number of relativistic degrees of freedom, N eff [11]; if, on the other hand, m ϕ ≲ 5 MeV and the decay is to neutrinos or to additional radiation in the dark sector, there may be observable signals in next-generation CMB experiments, depending on the decoupling temperature of the dark sector from the SM. In this paper we take an agnostic view towards the exact dynamics that determines the ratio of temperatures, but note that in many plausible scenarios,…”
Section: B Synthesis Temperaturementioning
confidence: 99%
“…This dark acoustic oscillation (DAO) feature generically arises in any model where DM is coupled to relativistic particles until relatively late times. For instance, they occur if DM couples to neutrinos [41,[48][49][50][51][52][53][54] or photons [55][56][57][58], if DM interacts with a dark Uð1Þ D gauge boson [36,37,47,59,60], if DM couples to a light scalar field [61], or in the case of the so-called cannibal DM model [62][63][64]. We emphasize for the reader unfamiliar with the above body of work that if the DM sector couples purely gravitationally to the visible sector, some of these scenarios are surprisingly unconstrained.…”
Section: Introductionmentioning
confidence: 99%