2018
DOI: 10.1103/physrevd.97.123001
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Radio telescope search for the resonant conversion of cold dark matter axions from the magnetized astrophysical sources

Abstract: We study the conditions for the adiabatic resonant conversion of the cold dark matter (CDM) axions into photons in the astrophysically sourced strong magnetic fields such as those in the neutron star magnetosphere. We demonstrate the possibility that the forthcoming radio telescopes such as the SKA (Square Kilometre Array) can probe those photon signals from the CDM axions.

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Cited by 127 publications
(95 citation statements)
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“…Observations of galaxies with SKA can potentially reach sensitivity comparable to ALPS-II for m a ∈ ½4 × 10 −7 ; 3 × 10 −4 eV by searching for stimulated decay of relic ALPs in galactic magnetic fields [108,109]. Dark matter ALPs can also convert to radio photons in the magnetospheres of neutron stars, leading to constraints in the μeV mass-range [110,111]. We show the limits from Ref.…”
Section: Fig 4 Theoretical Targets (Colored Bands)mentioning
confidence: 83%
“…Observations of galaxies with SKA can potentially reach sensitivity comparable to ALPS-II for m a ∈ ½4 × 10 −7 ; 3 × 10 −4 eV by searching for stimulated decay of relic ALPs in galactic magnetic fields [108,109]. Dark matter ALPs can also convert to radio photons in the magnetospheres of neutron stars, leading to constraints in the μeV mass-range [110,111]. We show the limits from Ref.…”
Section: Fig 4 Theoretical Targets (Colored Bands)mentioning
confidence: 83%
“…Due to the new coupling and the possible oscillations among the three light bosons, the radio flux from the neutron star may be different from the benchmark value in Ref. [36], since it is determined by many sources, such as the property of the mass matrix, the properties of the external (dark) magnetic field, the axion dark matter density and so on.…”
Section: Summary and Discussionmentioning
confidence: 85%
“…For example, often we have m 2 plasma = ω 2 plasma near pulsars. In some special position, this plasma mass can be equal to the axion mass [36].…”
Section: Photon-dark Photon-axion Oscillationsmentioning
confidence: 99%
“…As such, a signal in the range 98 GHz ≤ ω/2π ≤ 137 GHz might be expected for the conditions of the experiment proposed in Refs. [34,53], based on axion dark matter conversion (notice that in our case we do not need a dark matter background). At this stage, however, we can not commit whether or not the axions produced via streaming instability can be detected within the sensitivity of telescopes such as CAST or the Arecibo Telescope for the typical observation periods (this would involve a more detailed calculation of the beam injection rates, intensity, energies etc.…”
mentioning
confidence: 99%