Simulating the Galactic population of axion clouds around stellar-origin black holes: Gravitational wave signals in the 10–100 kHz band

Ultralight scalar fields can experience runaway ``superradiant'' amplification near spinning black holes, resulting in a macroscopic ``axion cloud,'' which slowly dissipates via continuous monochromatic gravitational waves. For a particular range of boson masses, $\mathcal{O}({10}^{\ensuremath{-}11}--{10}^{\ensuremath{-}10})\text{ }\text{ }\mathrm{eV}$, an axion cloud will radiate in the 10--100 kHz band of the levitated sensor detector (LSD). Using fiducial models of the mass, spin, and age distributions of stellar-origin black holes, we simulate the present-day Milky Way population of these hypothetical objects. As a first step toward assessing the LSD's sensitivity to the resultant ensemble of gravitational wave signals, we compute the corresponding signal-to-noise ratios which build up over a nominal integration time of ${10}^{7}\text{ }\text{ }\mathrm{s}$, assuming the projected sensitivity of the 1 m LSD prototype currently under construction, as well as for future 10 m and 100 m concepts. For a 100 m cryogenic instrument, hundreds of resolvable signals could be expected if the boson mass $\ensuremath{\mu}$ is around $3\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}\text{ }\text{ }\mathrm{eV}$, and this number diminishes with increasing $\ensuremath{\mu}$ up to $\ensuremath{\approx}5.5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}\text{ }\text{ }\mathrm{eV}$. The much larger population of unresolved sources will produce a confusion foreground which could be detectable by a 10-m instrument if $\ensuremath{\mu}\ensuremath{\in}(3--4.5)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}\text{ }\text{ }\mathrm{eV}$ or by a 100-m instrument if $\ensuremath{\mu}\ensuremath{\in}(3--6)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}\text{ }\text{ }\mathrm{eV}$.

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2024-12-18
DOI
https://doi.org/10.1103/physrevd.110.123025
Citations
3
Primary Topic
Cosmology and Gravitation Theories
Type
article
Field-Weighted Citation Impact
0.99

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article

Simulating the Galactic population of axion clouds around stellar-origin black holes: Gravitational wave signals in the 10–100 kHz band

Shane L. Larson, Shelby Klomp, George Winstone, Andrew A. Geraci et al.
3 citations
Physical review. D/Physical review. D.
Cosmology and Gravitation Theories
0.99
article

Simulating the Galactic population of axion clouds around stellar-origin black holes: Gravitational wave signals in the 10–100 kHz band

Shane L. Larson, Shelby Klomp, George Winstone, Andrew A. Geraci, Andrew Laeuger, Jacob Sprague, Zhiyuan Wang, N. Aggarwal, Vicky Kalogera
article en
3 citations

Abstract

Ultralight scalar fields can experience runaway ``superradiant'' amplification near spinning black holes, resulting in a macroscopic ``axion cloud,'' which slowly dissipates via continuous monochromatic gravitational waves. For a particular range of boson masses, $\mathcal{O}({10}^{\ensuremath{-}11}--{10}^{\ensuremath{-}10})\text{ }\text{ }\mathrm{eV}$, an axion cloud will radiate in the 10--100 kHz band of the levitated sensor detector (LSD). Using fiducial models of the mass, spin, and age distributions of stellar-origin black holes, we simulate the present-day Milky Way population of these hypothetical objects. As a first step toward assessing the LSD's sensitivity to the resultant ensemble of gravitational wave signals, we compute the corresponding signal-to-noise ratios which build up over a nominal integration time of ${10}^{7}\text{ }\text{ }\mathrm{s}$, assuming the projected sensitivity of the 1 m LSD prototype currently under construction, as well as for future 10 m and 100 m concepts. For a 100 m cryogenic instrument, hundreds of resolvable signals could be expected if the boson mass $\ensuremath{\mu}$ is around $3\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}\text{ }\text{ }\mathrm{eV}$, and this number diminishes with increasing $\ensuremath{\mu}$ up to $\ensuremath{\approx}5.5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}\text{ }\text{ }\mathrm{eV}$. The much larger population of unresolved sources will produce a confusion foreground which could be detectable by a 10-m instrument if $\ensuremath{\mu}\ensuremath{\in}(3--4.5)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}\text{ }\text{ }\mathrm{eV}$ or by a 100-m instrument if $\ensuremath{\mu}\ensuremath{\in}(3--6)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}\text{ }\text{ }\mathrm{eV}$.

Physical review. D/Physical review. D.Vol. 110(12)
California Institute of Technology (US), University of California, Davis (US)
National Science Foundation, W. M. Keck Foundation, John Templeton Foundation, Hertz Foundation, Heising-Simons Foundation, Engineering and Physical Sciences Research Council, Office of Naval Research
Openalex Percentile: Top 22%
Cosmology and Gravitation Theories
0.99
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