2015
DOI: 10.1088/1475-7516/2015/05/050
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Future cosmological sensitivity for hot dark matter axions

Abstract: We study the potential of a future, large-volume photometric survey to constrain the axion mass m a in the hot dark matter limit. Future surveys such as Euclid will have significantly more constraining power than current observations for hot dark matter. Nonetheless, the lowest accessible axion masses are limited by the fact that axions lighter than ∼ 0.15 eV decouple before the QCD epoch, assumed here to occur at a temperature T QCD ∼ 170 MeV; this leaves an axion population of such low density that its late-… Show more

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Cited by 48 publications
(41 citation statements)
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“…The phenomenology of axions and ALPs is determined by their low mass and very weak interactions. ALPs (and other WISPs) could affect stellar evolution [25,26] and cosmology [27] in a similar way to thermal neutrinos. These effects are responsible for the constraint f A 10 7 GeV mentioned above.…”
Section: Introductionmentioning
confidence: 99%
“…The phenomenology of axions and ALPs is determined by their low mass and very weak interactions. ALPs (and other WISPs) could affect stellar evolution [25,26] and cosmology [27] in a similar way to thermal neutrinos. These effects are responsible for the constraint f A 10 7 GeV mentioned above.…”
Section: Introductionmentioning
confidence: 99%
“…This regime is probed by measurements of N eff for m φ ≤ T rec and by warm dark matter constraints for m φ > T rec (see e.g. [34,35]), where T rec ≈ 0.26 eV is the temperature at recombination. We will discuss in turn the couplings to gauge bosons ( §2), to fermions ( §3) and to neutrinos ( §4).…”
Section: Introductionmentioning
confidence: 99%
“…with R = 0.553 ± 0.043, the up-to-down quark masses ratio, and f π = 93 MeV, the pion decay constant. Considering other values of R within the range 0.38 − 0.58 [73] does not affect in a significant way this relationship [74].…”
Section: Thermal Axionmentioning
confidence: 85%