Addressing issues in defining the Love numbers for black holes
arXiv:2306.13627 · doi:10.1103/PhysRevD.108.084013
Abstract
We present an analytic method for calculating the tidal response function of a nonrotating and a slowly rotating black hole from the Teukolsky equation in the small-frequency and near horizon limit. We point out that in the relativistic context, there can be two possible definitions of the tidal Love numbers and the dissipative part that arises from the tidal response function. Our results suggest that both of these definitions predict zero tidal Love numbers for a nonrotating black hole. On the other hand, for a slowly rotating black hole in a generic tidal environment, these two definitions of the tidal Love numbers do not coincide. While one procedure suggests zero tidal Love numbers, the other procedure gives purely imaginary tidal Love numbers. As expected, the dissipative terms differ as well. We emphasize that in our analysis, we keep all the terms linear in the frequency, unlike previous works in the literature. Following this, we propose a procedure to calculate the tidal response function -- and hence the Love numbers -- for an arbitrarily rotating black hole.
25 pages, 1 figure
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- Tidal Love numbers and approximate universal relations for fermion soliton stars
- Rotating black holes experience dynamical tides
- Scalar tidal response of a rotating BTZ black hole
- Systematic biases from ignoring environmental tidal effects in gravitational wave observations
- Dynamical Tidal Response of Non-rotating Black Holes: Connecting the MST Formalism and Worldline EFT
- Fermionic Love of Black Holes in General Relativity
- Response of a Kerr black hole to a generic tidal perturbation
- Tidal deformation of black holes in Lovelock gravity
- Ladder Symmetry: The Necessary and Sufficient Condition for Vanishing Love Numbers
- Highest-weight truncation, graded EFT structure, and renormalization of black hole Love numbers