Quantum fluxes at the inner horizon of a near-extremal spherical charged black hole
arXiv:2105.06521 · doi:10.1103/PhysRevD.104.024066
Abstract
We analyze and compute the semiclassical stress-energy flux components, the outflux and the influx ( and being the standard null Eddington coordinates), at the inner horizon (IH) of a Reissner-Nordström black hole (BH) of mass and charge , in the near-extremal domain in which approaches . We consider a minimally-coupled massless quantum scalar field, in both Hartle-Hawking () and Unruh () states, the latter corresponding to an evaporating BH. The near-extremal domain lends itself to an analytical treatment which sheds light on the behavior of various quantities on approaching extremality. We explore the behavior of the three near-IH flux quantities , , and , as a function of the small parameter (where the superscript "" refers to the IH value). We find that in the near-extremal domain behaves as . In contrast, behaves as , and we calculate the prefactor analytically. It therefore follows that the semiclassical fluxes at the IH neighborhood of an evaporating near-extremal spherical charged BH are dominated by the influx . In passing, we also find an analytical expression for the transmission coefficient outside a Reissner-Nordström BH to leading order in small frequencies (which turns out to be a crucial ingredient of our near-extremal analysis). Furthermore, we explicitly obtain the near-extremal Hawking-evaporation rate (), with an analytical expression for the prefactor (obtained here for the first time to the best of our knowledge). [Abridged]
17 pages, 2 figures. v2: sign error fixed in Eq. A30
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