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Absorption of Axion Dark Matter in a Magnetized Medium

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arxiv 2305.05681 v1 pith:PAOT6OHB submitted 2023-05-09 hep-ph astro-ph.COcond-mat.mtrl-scihep-ex

classification hep-phastro-ph.COcond-mat.mtrl-scihep-ex
keywords textaxiondarkmatterabsorptionexcitationsin-mediumnoise
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

Detection of axion dark matter heavier than a meV is hindered by its small wavelength, which limits the useful volume of traditional experiments. This problem can be avoided by directly detecting in-medium excitations, whose $\sim \text{meV} - \text{eV}$ energies are decoupled from the detector size. We show that for any target inside a magnetic field, the absorption rate of electromagnetically-coupled axions into in-medium excitations is determined by the dielectric function. As a result, the plethora of candidate targets previously identified for sub-GeV dark matter searches can be repurposed as broadband axion detectors. We find that a $\text{kg} \cdot \text{yr}$ exposure with noise levels comparable to recent measurements is sufficient to probe parameter space currently unexplored by laboratory tests. Noise reduction by only a few orders of magnitude can enable sensitivity to the QCD axion in the $\sim 10 \ \text{meV} - 10 \ \text{eV}$ mass range.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Resonant axion and dark photon production in magnetic white dwarfs

    hep-ph 2025-09 conditional novelty 7.0 of 10

    Magnetic fields broaden the resonant conversion of photons to axions and dark photons inside magnetic white dwarfs, enabling emission where none occurred before.

  2. Probing the axion-electron coupling at cavity experiments

    hep-ph 2025-07 conditional novelty 6.0 of 10

    Cavity walls radiate microwave photons when axion dark matter generates a chiral magnetic current at the conductor surface, turning existing haloscope data into a bound on the axion-electron coupling g_ae ≲ 10^-5.

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