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Quantum fluxes and for a nonminimally coupled scalar field: Ringdown and tail on approaching the polar Kerr inner horizon
Phys. Rev. D 114, 064039 – Published 14 September, 2026
DOI: https://doi.org/10.1103/t6ff-qsdf
Abstract
We compute as well as the energy fluxes and (where and are the standard Eddington-Finkelstein coordinates) associated with a quantum massless real scalar field , with a general curvature coupling constant , near the inner horizon (IH) of a Kerr black hole, along the axis of rotation. The quantum field is in the Unruh state, corresponding to an evaporating black hole. We renormalize these quantities by the state-subtraction method. We drop the assumption of minimal coupling to the curvature, thereby generalizing the results of [1] for the fluxes at the IH. This requires understanding the asymptotic behavior of near the IH. State subtraction allows us to push the computation of along the axis of rotation in the Kerr interior in [2] deeper into the near-IH region, exposing their final asymptotic behavior on approaching the IH. For (a -independent quantity in the Kerr case), we find that the approach to its finite asymptotic IH value is given, per -mode, by a ringdown phase (namely exponentially damped oscillations), followed by an inverse-power tail, both in the tortoise coordinate (which diverges at the IH). Interestingly, in the regime where the ringing dominates, the ringing’s complex frequencies are (numerically) found to match twice the well-known classical quasinormal-mode frequencies in Kerr, and the inverse-power tails are found to be (resembling Price’s law in the classical black hole exterior, upon replacement ). In particular, the sum over behaves as (with a prefactor obtained here analytically for the first time), resembling the known behavior of classical (axially symmetric) scalar perturbations on approaching the IH [3]. These results allow computing the flux components and for general at the IH vicinity. We find that the limiting IH values of and are independent of the coupling constant . When translated to the Kruskal coordinate (regular and vanishing at the Cauchy horizon), it implies that the prefactor characterizing the divergence of the renormalized quantum stress-energy tensor appearing in , is independent of the coupling to curvature in the case of polar Kerr.
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