2021
DOI: 10.48550/arxiv.2112.11431
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Asteroids for $μ$Hz gravitational-wave detection

Michael A. Fedderke,
Peter W. Graham,
Surjeet Rajendran

Abstract: A major challenge for gravitational-wave (GW) detection in the µHz band is engineering a test mass (TM) with sufficiently low acceleration noise. We propose a GW detection concept using asteroids located in the inner Solar System as TMs. Our main purpose is to evaluate the acceleration noise of asteroids in the µHz band. We show that a wide variety of environmental perturbations are small enough to enable an appropriate class of ∼ 10 km-diameter asteroids to be employed as TMs. This would allow a sensitive GW … Show more

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Cited by 16 publications
(35 citation statements)
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References 170 publications
(400 reference statements)
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“…We note also that timing measurements using atomic clocks located on asteroids have been proposed as a way to measure gravitational waves in the µHz range[244], in the gap between LISA and pulsar timing arrays 15. We comment in passing that radio astronomy would gain greatly from extending the Event Horizon Telescope[246] concept to a space mission with a much longer baseline, which would benefit from using atomic clocks for synchronization.…”
mentioning
confidence: 94%
“…We note also that timing measurements using atomic clocks located on asteroids have been proposed as a way to measure gravitational waves in the µHz range[244], in the gap between LISA and pulsar timing arrays 15. We comment in passing that radio astronomy would gain greatly from extending the Event Horizon Telescope[246] concept to a space mission with a much longer baseline, which would benefit from using atomic clocks for synchronization.…”
mentioning
confidence: 94%
“…Future clock development will provide further orders of magnitude of improvement for these experiments. Deployment of high-precision clocks in space will also open the door to new applications, including precision tests of gravity and relativity [210], searches for a dark-matter halo bound to the Sun [211], and gravitational wave detection in wavelength ranges inaccessible on Earth [212,213].…”
Section: Atomic Nuclear and Molecular Clocks And Precision Spectroscopymentioning
confidence: 99%
“…For M wd ∼ 0.6 M , this implies that the planetary body must have an orbital semi-major axis a around the star in the range 0.1 AU a 2 AU, in order for the fundamental orbital period to lie in the measurement band; higher harmonics of the orbital frequency will also enter for eccentric orbits, but are suppressed (see discussions in, e.g., Refs. [43,56]).…”
Section: B Planetsmentioning
confidence: 99%
“…These include pulsar timing arrays (PTAs) [6][7][8][15][16][17][18][19][20] that operate around nHz-µHz; the LISA constellation [21][22][23] that is aimed at 1-10 mHz; TianQin aimed at 0.01 Hz-1 Hz [24,25]; atomic-interferometry approaches such as MAGIS/MIGA/AION/AEDGE/ZAIGA [26][27][28][29][30][31][32][33][34][35][36][37] around 1 Hz; clock-based proposals [38] between mHz and Hz; DECIGO at 0.1-10 Hz [39,40]; and Cosmic Explorer [41] and the Einstein Telescope [42] above ∼ 10 Hz. Concepts have also been developed to detect gravitational waves in the µHz-mHz band using LISA-style constellations [11], using asteroids as test masses in a future space-based mission [43], studying orbital perturbations to various binary systems [44,45], and looking for low-frequency modulation of higher-frequency GWs [46]. Existing astrometric studies (e.g., Refs.…”
mentioning
confidence: 99%
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