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Axion Gegenschein: Probing Back-scattering of Astrophysical Radio Sources Induced by Dark Matter

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arxiv 2008.02729 v1 pith:4LZZOINV submitted 2020-08-06 astro-ph.CO hep-ph

classification astro-ph.COhep-ph
keywords axionradiodarkmatterdecayemissiongegenscheinhalo
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abstract

We investigate a novel technique for the astrophysical detection of axions or axion-like particles in the dark matter halo of the Milky Way based on stimulated decay of axions, which we call axion gegenschein emission. Photons from the brightest known radio sources with a frequency equal to half the axion mass stimulate axion decay while propagating through the dark matter halo, causing radio emission in a direction precisely opposite to the incoming photon in the axion rest-frame and creating a countersource for every radio source, with an image smoothed by the dark matter velocity dispersion. We calculate the flux of the axion gegenschein countersource of Cygnus A, the brightest extragalactic radio source, and the limits that can be set with SKA to the axion-photon coupling constant $g_{a\gamma}$. We find this method to be more powerful than previous proposals based on searching for radio emission from axion decay in nearby dwarf galaxies or the Milky Way. The forecasted limits remain considerably higher than predictions from QCD axion models, and limits that can be set with laboratory searches of radio waves generated in resonant cavities with strong magnetic fields similar to the ADMX experiment, although this observation would directly measure a column density of dark matter through the Galactic halo and is therefore not affected by possible substructure in the dark matter distribution.

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Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. OpenAlex reports about 8 citations worldwide. Full citation record

  1. Echoes in multi-ALP scenarios

    hep-ph 2025-07 conditional novelty 5.0 of 10

    In coherent multi-ALP models, axion echo power scales linearly with the number of ALPs, while incoherent (random-phase) models yield signals no stronger than the single-ALP case.

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