2021
DOI: 10.1007/jhep12(2021)216
|View full text |Cite
|
Sign up to set email alerts
|

Resurrecting low-mass axion dark matter via a dynamical QCD scale

Abstract: In the framework where the strong coupling is dynamical, the QCD sector may confine at a much higher temperature than it would in the Standard Model, and the temperature-dependent mass of the QCD axion evolves in a non-trivial way. We find that, depending on the evolution of ΛQCD, the axion field may undergo multiple distinct phases of damping and oscillation leading generically to a suppression of its relic abundance. Such a suppression could therefore open up a wide range of parameter space, resurrecting in … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
8
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
5
2

Relationship

1
6

Authors

Journals

citations
Cited by 12 publications
(10 citation statements)
references
References 39 publications
2
8
0
Order By: Relevance
“…5, where region 3 for constant axion mass starts above the blue line T osc = T c . There, as found in our analysis, the relic density is independent of T eq and the smallest axion mass that can fulfil the whole DM density is, for β = 3 m a ∼ 10 −8 eV for T eq 10 4 GeV, (55) and for β = 2 m a ∼ 10 −10 eV for T eq 4 GeV. (56) Numerically in Fig.…”
Section: Constant Axion Masssupporting
confidence: 79%
See 1 more Smart Citation
“…5, where region 3 for constant axion mass starts above the blue line T osc = T c . There, as found in our analysis, the relic density is independent of T eq and the smallest axion mass that can fulfil the whole DM density is, for β = 3 m a ∼ 10 −8 eV for T eq 10 4 GeV, (55) and for β = 2 m a ∼ 10 −10 eV for T eq 4 GeV. (56) Numerically in Fig.…”
Section: Constant Axion Masssupporting
confidence: 79%
“…The most straightforward approach is to consider that in the case of the pre-inflationary scenario, there is a very small initial misalignment angle θ i , to compensate for a higher f a scale shifting it to be as high as ∼ 10 16 GeV, as allowed by bounds on isocurvature perturbations. Another way to open up the axion DM window to smaller masses or higher PQ scales invokes the coupling of the axion to some other field, for instance, to a hidden photon [50,51], or if the axion potential was much larger in the very early universe [52][53][54][55]. A different possibility to expand the range masses has been to consider a nonstandard cosmological (NSC) history in the early universe, such that entropy is injected into the thermal bath, diluting the axion energy density.…”
Section: Introductionmentioning
confidence: 99%
“…The QCD axion potential is well-known to be generated by non-perturbative effects around the QCD scale. At high temperature, the axion potential is unconstrained and can arise from a variety of PQ breaking effects [152,153,[165][166][167][168].…”
Section: Axion Model Realizations -Class a 6 Model A: An Axion-only R...mentioning
confidence: 99%
“…If the temperature is smaller than the fermion mass, T < y √ √, the heavy fermions are absent of the thermal plasma and must be integrated out. In that case, the scalar field can decay into gauge boson through a loop of fermions [165,167,168], cf. diagram c in Fig.…”
Section: G Radial Damping G1 Thermalizationmentioning
confidence: 99%
“…At this time, the Universe may deviate dramatically from our extrapolation based on the SM, due to unforeseen Physics beyond the Standard Model. Indeed, explorations of non-standard cosmological histories, including a period of early matter domination [8], late entropy injection [9], and modifications of fundamental parameters such as the strength of the SU(3) coupling [10,11] have all been shown to lead to dramatically different expectations in the mapping of WIMP parameter space onto its predicted abundance in the early Universe.…”
Section: Jhep02(2022)047mentioning
confidence: 99%