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Quantum fluxes and Φ^2 for a nonminimally coupled scalar field: Ringdown and tail on approaching the polar Kerr inner horizon

Maria Alberti1,2,*, Noa Zilberman3,†, Marc Casals4,5,6,‡, and Adrian C. Ottewill5,§

  • *Contact author: mariaalberti@campus.technion.ac.il
  • Contact author: nz3745@princeton.edu
  • Contact author: marc.casals@uni-leipzig.de
  • §Contact author: adrian.ottewill@ucd.ie

Phys. Rev. D 114, 064039 – Published 14 September, 2026

DOI: https://doi.org/10.1103/t6ff-qsdf

Abstract

We compute Φ^2ren as well as the energy fluxes T^uuren and T^vvren (where u and v are the standard Eddington-Finkelstein coordinates) associated with a quantum massless real scalar field Φ^, with a general curvature coupling constant ξ, 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 Φ^2ren near the IH. State subtraction allows us to push the computation of Φ^2ren 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 Φ^2ren (a ξ-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 r* (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 r*23 (resembling Price’s law in the classical black hole exterior, upon replacement tr*). In particular, the sum over behaves as r*3 (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 T^uuren and T^vvren for general ξ at the IH vicinity. We find that the limiting IH values of T^uuren and T^vvren are independent of the coupling constant ξ. When translated to the Kruskal coordinate V (regular and vanishing at the Cauchy horizon), it implies that the prefactor C characterizing the divergence of the renormalized quantum stress-energy tensor appearing in T^VVrenCV2, is independent of the coupling to curvature in the case of polar Kerr.

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