Axion pulsarscope

Electromagnetic fields surrounding pulsars may source coherent ultralight axion signals at the known rotational frequencies of the neutron stars, which can be detected by laboratory experiments (e.g., pulsarscopes). As a promising case study, we model axion emission from the well-studied Crab pulsar, which would yield a prominent signal at <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mi>f</a:mi><a:mo>≈</a:mo><a:mn>29.6</a:mn><a:mtext> </a:mtext><a:mtext> </a:mtext><a:mi>Hz</a:mi></a:mrow></a:math> regardless of whether the axion contributes to the dark matter abundance. We estimate the relevant sensitivity of future axion dark matter detection experiments such as DMRadio-GUT, Dark SRF, and CASPEr, assuming different magnetosphere models to bracket the uncertainty in astrophysical modeling. For example, depending on final experimental parameters, the Dark SRF experiment could probe axions with any mass <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msub><c:mi>m</c:mi><c:mi>a</c:mi></c:msub><c:mo>≪</c:mo><c:msup><c:mn>10</c:mn><c:mrow><c:mo>−</c:mo><c:mn>13</c:mn></c:mrow></c:msup><c:mtext> </c:mtext><c:mtext> </c:mtext><c:mi>eV</c:mi></c:math> down to <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mrow><e:msub><e:mrow><e:mi>g</e:mi></e:mrow><e:mrow><e:mi>a</e:mi><e:mi>γ</e:mi><e:mi>γ</e:mi></e:mrow></e:msub><e:mo>∼</e:mo><e:mn>3</e:mn><e:mo>×</e:mo><e:msup><e:mrow><e:mn>10</e:mn></e:mrow><e:mrow><e:mo>−</e:mo><e:mn>13</e:mn></e:mrow></e:msup><e:mtext> </e:mtext><e:mtext> </e:mtext><e:mrow><e:msup><e:mrow><e:mi>GeV</e:mi></e:mrow><e:mrow><e:mo>−</e:mo><e:mn>1</e:mn></e:mrow></e:msup></e:mrow></e:mrow></e:math> with one year of data and assuming the vacuum magnetosphere model. These projected sensitivities may be degraded depending on the extent to which the magnetosphere is screened by charge-filled plasma. The promise of pulsar-sourced axions as a clean target for direct detection experiments motivates dedicated simulations of axion production in pulsar magnetospheres.

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2025-04-17
DOI
https://doi.org/10.1103/physrevd.111.083027
Citations
3
Primary Topic
Dark Matter and Cosmic Phenomena
Type
article
Field-Weighted Citation Impact
5.61

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Axion pulsarscope

Mariangela Lisanti, Anirudh Prabhu, Benjamin R. Safdi, Mariia Khelashvili
3 citations
Physical review. D/Physical review. D.
Dark Matter and Cosmic Phenomena
5.61
article

Axion pulsarscope

Mariangela Lisanti, Anirudh Prabhu, Benjamin R. Safdi, Mariia Khelashvili
article en
3 citations

Abstract

Electromagnetic fields surrounding pulsars may source coherent ultralight axion signals at the known rotational frequencies of the neutron stars, which can be detected by laboratory experiments (e.g., pulsarscopes). As a promising case study, we model axion emission from the well-studied Crab pulsar, which would yield a prominent signal at <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mi>f</a:mi><a:mo>≈</a:mo><a:mn>29.6</a:mn><a:mtext> </a:mtext><a:mtext> </a:mtext><a:mi>Hz</a:mi></a:mrow></a:math> regardless of whether the axion contributes to the dark matter abundance. We estimate the relevant sensitivity of future axion dark matter detection experiments such as DMRadio-GUT, Dark SRF, and CASPEr, assuming different magnetosphere models to bracket the uncertainty in astrophysical modeling. For example, depending on final experimental parameters, the Dark SRF experiment could probe axions with any mass <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msub><c:mi>m</c:mi><c:mi>a</c:mi></c:msub><c:mo>≪</c:mo><c:msup><c:mn>10</c:mn><c:mrow><c:mo>−</c:mo><c:mn>13</c:mn></c:mrow></c:msup><c:mtext> </c:mtext><c:mtext> </c:mtext><c:mi>eV</c:mi></c:math> down to <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mrow><e:msub><e:mrow><e:mi>g</e:mi></e:mrow><e:mrow><e:mi>a</e:mi><e:mi>γ</e:mi><e:mi>γ</e:mi></e:mrow></e:msub><e:mo>∼</e:mo><e:mn>3</e:mn><e:mo>×</e:mo><e:msup><e:mrow><e:mn>10</e:mn></e:mrow><e:mrow><e:mo>−</e:mo><e:mn>13</e:mn></e:mrow></e:msup><e:mtext> </e:mtext><e:mtext> </e:mtext><e:mrow><e:msup><e:mrow><e:mi>GeV</e:mi></e:mrow><e:mrow><e:mo>−</e:mo><e:mn>1</e:mn></e:mrow></e:msup></e:mrow></e:mrow></e:math> with one year of data and assuming the vacuum magnetosphere model. These projected sensitivities may be degraded depending on the extent to which the magnetosphere is screened by charge-filled plasma. The promise of pulsar-sourced axions as a clean target for direct detection experiments motivates dedicated simulations of axion production in pulsar magnetospheres.

Physical review. D/Physical review. D.Vol. 111(8)
Goethe University Frankfurt (DE), Goethe-Institute United Kingdom (GB), Lawrence Berkeley National Laboratory (US), Princeton University (US), Flatiron Health (United States) (US), Bogolyubov Institute for Theoretical Physics (UA), Flatiron Institute (US), University of California, Berkeley (US)
U.S. Department of Energy, Simons Foundation, Princeton University
Openalex Percentile: Top 5%
Dark Matter and Cosmic Phenomena
5.61
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