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We calculate the tidal response of a rotating black hole from the Teukolsky equation in the near-horizon and small-frequency regime. While the static tidal Love number of an arbitrarily rotating black hole is still zero, the dynamical tidal Love number is not; rather, it is proportional to the angular velocity of the black hole -- in the linear order of frequency -- and to the square of the angular velocity of the black hole -- in the zeroth order. Intriguingly, the zero-frequency limit of the dynamical tidal response function is not equal to the static tidal response function. We demonstrate that these results hold true for an extremal rotating black hole as well, with the dynamical tidal Love numbers being non-zero. This shows that Kerr black holes experience dynamical tides.
Bhatt et al. (Thu,) studied this question.