2021
DOI: 10.1103/physrevd.103.103017
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Gravity gradient noise from asteroids

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Cited by 21 publications
(50 citation statements)
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“…DM which can cool via emission of dark radiation will be more susceptible to collapse, and is likely to be more strongly constrained than models possessing only elastic cooling. Another particularly interesting case is electrically charged particles [67] or magnetic monopoles. Ultra-heavy monopoles and anti-monopoles could be captured in a WD and subsequently annihilate, igniting SN-we estimate that such a process can be used to place constraints on the flux of galactic monopoles ex-ceeding current limits [68].…”
Section: Discussionmentioning
confidence: 99%
“…DM which can cool via emission of dark radiation will be more susceptible to collapse, and is likely to be more strongly constrained than models possessing only elastic cooling. Another particularly interesting case is electrically charged particles [67] or magnetic monopoles. Ultra-heavy monopoles and anti-monopoles could be captured in a WD and subsequently annihilate, igniting SN-we estimate that such a process can be used to place constraints on the flux of galactic monopoles ex-ceeding current limits [68].…”
Section: Discussionmentioning
confidence: 99%
“…We also show the sensitivities to a stochastic background through power-law-integrated (PI) curves [39] as thicker solid lines, again indicating the impact of GGN on these predictions by thick dashed lines. In the case of AION-km, we see that the PI sensitivity is impacted at low frequencies 10 −6 by the estimated GGN from asteroids [36], but we emphasize that there may also be important sources of instrumental noise at low frequencies, as well as other sources of GGN.…”
Section: (A) a Terrestrial Project: Aionmentioning
confidence: 69%
“…The solid thick lines show the sensitivities to stochastic backgrounds with power-law-integrated (PI) curves while the impact of unmitigated GGN is again shown as a dashed curve. We also show the GGN generated by asteroids[36] at low frequencies, as well as the noise due to unresolved galactic and extragalactic binaries. (Online version in colour.…”
mentioning
confidence: 98%
“…−1 with θ = θ(t) the angle about the orbit from perihelion (which by Kepler's Third Law of course evolves non-trivially in time for an elliptical orbit; see, e.g., the discussion in Appendix A.4 of Ref. [56]). This means that we can take r = a with −e ≤ δr(t) ≤ +e, and with δr(t) having dominant frequency content near and around inner Solar System orbital frequencies ∼ 10 −8 Hz-10 −7 Hz (i.e.…”
Section: Physical Parametersmentioning
confidence: 99%
“…Proposals utilizing astrometric techniques on large-scale survey data (e.g., Gaia [47] and Roman Space Telescope [48] surveys) are also able to access this band (see, e.g., Refs. [49][50][51][52][53][54][55]), but existing projections indicate that the levels of strain sensitivity attainable are somewhat modest [55]; such approaches are however able to overcome some important noise sources [56] that limit all local-TM-based techniques operating in the inner Solar System below ∼ µHz frequencies. Recent work has also studied how orbital perturbations (of, e.g., binary millisecond pulsars, or the Moon) that arise specifically from a broadband stochastic GW background could access this band [57,58].…”
mentioning
confidence: 99%