Zero temperature black holes in semiclassical gravity

The semiclassical Einstein equations are solved to first order in \(\epsilon = \hbar/M^2\) 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,...

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Veröffentlicht in:arXiv.org 2001-03
Hauptverfasser: Anderson, Paul R, Hiscock, William A, Taylor, Brett E
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description The semiclassical Einstein equations are solved to first order in \(\epsilon = \hbar/M^2\) 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 \(r_h < |Q|\), with \(Q\) the charge of the black hole. It is further shown that no black hole solutions with \(r_h < |Q|\) can be obtained by solving the semiclassical Einstein equations perturbatively.
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subjects Black holes
Einstein equations
Event horizon
Mathematical analysis
Quantum theory
title Zero temperature black holes in semiclassical gravity
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