2020
DOI: 10.1088/1475-7516/2020/05/009
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Robust cosmological constraints on axion-like particles

Abstract: Axion-like particles with masses in the keV-GeV range have a profound impact on the cosmological evolution of our Universe, in particular on the abundance of light elements produced during Big Bang Nucleosynthesis. The resulting limits are complementary to searches in the laboratory and provide valuable additional information regarding the validity of a given point in parameter space. A potential drawback is that altering the cosmological history may potentially weaken or even fully invalidate these bounds. Th… Show more

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Cited by 106 publications
(107 citation statements)
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“…BBN represents a very stringent constraint on light species that were not in thermal equilibrium during BBN but that were still capable of modifying the expansion history of the early Universe. Relevant examples of these scenarios include axions [719,720], axion-like particles [721,722], majorons [723,724], and weakly coupled dark sectors [725,726].…”
Section: Bbn Constraints On Nonstandard Cosmologiesmentioning
confidence: 99%
“…BBN represents a very stringent constraint on light species that were not in thermal equilibrium during BBN but that were still capable of modifying the expansion history of the early Universe. Relevant examples of these scenarios include axions [719,720], axion-like particles [721,722], majorons [723,724], and weakly coupled dark sectors [725,726].…”
Section: Bbn Constraints On Nonstandard Cosmologiesmentioning
confidence: 99%
“…While originally motivated as a solution to the strong CP problem [18][19][20], they are ubiquitous in many high energy physics theories [21][22][23][24]. A variety of experimental efforts are underway to detect axions and axion-like particles (ALPs) in the laboratory [25][26][27][28] and through their unique astrophysical and cosmological signatures [29][30][31][32][33][34][35][36][37][38]. Many of these searches rely upon a coupling of the axion field φ(x, t) to electromagnetism via the interaction g aγ φE • B.…”
Section: Introductionmentioning
confidence: 99%
“…For the lowest masses we will consider (a few MeV), ALP and/or dark sector particle could remain in thermal equilibrium until the time of neutrinos decoupling and BBN, and this would yield additional constraints, see e.g. [61][62][63]. In this work, given that we do not specify the detailed structure of the dark sector, we will simply assume that a mechanism exists that allows to escape possible constraints from DM overabundance or from other cosmological arguments.…”
Section: Jhep06(2021)009mentioning
confidence: 99%