2012
DOI: 10.1088/1475-7516/2012/06/013
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WISPy cold dark matter

Abstract: Very weakly interacting slim particles (WISPs), such as axion-like particles (ALPs) or hidden photons (HPs), may be non-thermally produced via the misalignment mechanism in the early universe and survive as a cold dark matter population until today. We find that, both for ALPs and HPs whose dominant interactions with the standard model arise from couplings to photons, a huge region in the parameter spaces spanned by photon coupling and ALP or HP mass can give rise to the observed cold dark matter. Remarkabl… Show more

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Cited by 768 publications
(871 citation statements)
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References 178 publications
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“…Assuming that the ALP makes up all of the dark matter [10] the photon fluxes found in [1,2] correspond to lifetimes in the range 1 τ ϕ ∼ ð4 × 10 27 -4 × 10 28 Þ s: (2.3) Combining this with the energy of the photon line, we find the following parameters,…”
Section: A Simple Alp Explanationmentioning
confidence: 98%
“…Assuming that the ALP makes up all of the dark matter [10] the photon fluxes found in [1,2] correspond to lifetimes in the range 1 τ ϕ ∼ ð4 × 10 27 -4 × 10 28 Þ s: (2.3) Combining this with the energy of the photon line, we find the following parameters,…”
Section: A Simple Alp Explanationmentioning
confidence: 98%
“…The interest in homogeneous vector fields as cosmological fluids has been growing in the last years, see [58][59][60][61][62][63] for dark energy examples and [64,65] for inflation models based on vector fields. The possibility that a condensate of very light vector particles could play the role of DM was explored in [66] and a wide phenomenological study of this model was made in [67]. Such a condensate could be produced during inflation and its small mass could be generated by the Stückelberg mechanism.…”
Section: Jhep02(2017)064mentioning
confidence: 99%
“…Thus, our perturbative approach does not allow to explore this region. Fortunately, for the masses usually considered [67] this range is out of the cosmologically observable band. Notice for example that assuming for the preferred mass m = 10 −22 eV the limiting wave-number results k 10 −9 Mpc −1 h much smaller than the lowest wave number accessible today k > ∼ 2π/H 0 10 −4 Mpc −1 h, see figure 1.…”
Section: Jhep02(2017)064mentioning
confidence: 99%
“…(4.5) would give a negligible contribution to the dark matter density. Indeed the relics abundance is given by [40],…”
Section: Jhep05(2016)104mentioning
confidence: 99%