2020
DOI: 10.48550/arxiv.2007.00214
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Spinning Black Holes Fall in Love

Alexandre Le Tiec,
Marc Casals

Abstract: The open question of whether a black hole can become tidally deformed by an external gravitational field has profound implications for fundamental physics, astrophysics and gravitational-wave astronomy. Love numbers characterize the tidal deformability of compact objects such as astrophysical (Kerr) black holes. We prove that all Love numbers vanish identically for a Kerr black hole in the nonspinning limit or for an axisymmetric tidal perturbation. In contrast to this result, we show that Love numbers are gen… Show more

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Cited by 18 publications
(29 citation statements)
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“…Conservation of P thus tells us this solution, when extended to the horizon, must approach a constant rather than the divergent logarithm. 13 It is worth emphasizing the vanishing of the Love number follows from two facts: (1) the purely decaying solution (∼ 1/r +1 at large r) is divergent at the horizon, and (2) the solution that is regular at the horizon is a finite polynomial going as 1 + r + • • • + r . The second fact by itself is not sufficient: it does not forbid us from adding to it a decaying tail that goes as 1/r +1 .…”
Section: Ladder In Schwarzschildmentioning
confidence: 99%
See 1 more Smart Citation
“…Conservation of P thus tells us this solution, when extended to the horizon, must approach a constant rather than the divergent logarithm. 13 It is worth emphasizing the vanishing of the Love number follows from two facts: (1) the purely decaying solution (∼ 1/r +1 at large r) is divergent at the horizon, and (2) the solution that is regular at the horizon is a finite polynomial going as 1 + r + • • • + r . The second fact by itself is not sufficient: it does not forbid us from adding to it a decaying tail that goes as 1/r +1 .…”
Section: Ladder In Schwarzschildmentioning
confidence: 99%
“…For black holes, though, such a polarizability, or tidal response, appears to be absent. Let us be more precise: under the influence of a weak static tidal field (spin 0, 1, or 2), black holes have vanishing Love numbers [2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18]. The Love numbers quantify the tidal response: suppose the external tidal field goes as r at large distance r ( is the multipole of interest), an object such as a star that gets tidally deformed would source a response field that goes as 1/r +1 far away.…”
Section: Introductionmentioning
confidence: 99%
“…What are the explicit finite transformations associated with 2 The case of the TNLs of the Kerr black hole has been the subject of debate recently as different claims have been made. See [16][17][18][19][20][21][22][23][24][25] for details. In this work, we shall only focus on the Schwarzschild black hole.…”
Section: Introductionmentioning
confidence: 99%
“…a source distribution that is deformed due to an external tidal field [14] or involve the application of black hole perturbation theory [8][9][10][11][12][13]. A limit of the compactness is then taken to deduce the corresponding Love numbers for black holes.…”
Section: Introductionmentioning
confidence: 99%