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Zero temperature black holes in semiclassical gravity

Abstract

The semiclassical Einstein equations are solved to first order in ϵ=/M2\epsilon = \hbar/M^2 for the case of an extreme or nearly extreme Reissner-Nordstr\"{o}m black hole perturbed by the vacuum stress-energy of quantized free fields. It is shown that, for realistic fields of spin 0, 1/2, or 1, any zero temperature black hole solution to the equations must have an event horizon at rh<Qr_h < |Q|, with QQ the charge of the black hole. It is further shown that no black hole solutions with rh<Qr_h < |Q| can be obtained by solving the semiclassical Einstein equations perturbatively.Comment: 7 pages, to appear in the Proceedings of the Ninth Marcel Grossmann Meeting, change in titl

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