Lunar response to gravitational waves

It has been suggested to use seismic detectors on the Moon as a tool to search for gravitational waves in an intermediate frequency range between mHz and Hz. Employing three different spherically symmetric models for the lunar interior, we investigate the response of the Moon to gravitational waves in Einstein and Jordan-Brans-Dicke gravity. We find that the first eigenfrequencies of the different models depend only weakly on the model details, with the fundamental frequency ${\ensuremath{\nu}}_{1}$ close to 1 ms both for spheroidal and toroidal oscillations. In contrast, the resulting displacement varies up to a factor 5, being in the range $(3.6\ifmmode\times\else\texttimes\fi{}{10}^{12}--1.9\ifmmode\times\else\texttimes\fi{}{10}^{13})/{h}_{0}\text{ }\text{ }\mathrm{cm}$ for spheroidal oscillations with amplitude ${h}_{0}$ and assuming a quality factor ${Q}_{n}=3300$. Toroidal oscillations are suppressed by a factor $2\ensuremath{\pi}\ensuremath{\nu}R/c$, both in Einstein gravity and in general scalar-tensor theories.

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2024-09-10
DOI
https://doi.org/10.1103/physrevd.110.064034
Citations
7
Primary Topic
Pulsars and Gravitational Waves Research
Type
article
Field-Weighted Citation Impact
2.32
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article

Lunar response to gravitational waves

M. Kachelrieß, M. P. Nødtvedt
7 citations
Physical review. D/Physical review. D.
Pulsars and Gravitational Waves Research
2.32
article

Lunar response to gravitational waves

M. Kachelrieß, M. P. Nødtvedt
article en
7 citations

Abstract

It has been suggested to use seismic detectors on the Moon as a tool to search for gravitational waves in an intermediate frequency range between mHz and Hz. Employing three different spherically symmetric models for the lunar interior, we investigate the response of the Moon to gravitational waves in Einstein and Jordan-Brans-Dicke gravity. We find that the first eigenfrequencies of the different models depend only weakly on the model details, with the fundamental frequency ${\ensuremath{\nu}}_{1}$ close to 1 ms both for spheroidal and toroidal oscillations. In contrast, the resulting displacement varies up to a factor 5, being in the range $(3.6\ifmmode\times\else\texttimes\fi{}{10}^{12}--1.9\ifmmode\times\else\texttimes\fi{}{10}^{13})/{h}_{0}\text{ }\text{ }\mathrm{cm}$ for spheroidal oscillations with amplitude ${h}_{0}$ and assuming a quality factor ${Q}_{n}=3300$. Toroidal oscillations are suppressed by a factor $2\ensuremath{\pi}\ensuremath{\nu}R/c$, both in Einstein gravity and in general scalar-tensor theories.

Physical review. D/Physical review. D.Vol. 110(6)
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Pulsars and Gravitational Waves Research
2.32
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Lunar response to gravitational waves — M. Kachelrieß, M. P. Nødtvedt · Physical review. D/Physical review. D. (2024) | TGRS Research Map | TGRS