The semiclassical Einstein equations are solved to first order in ϵ=ℏ/M2 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<∣Q∣,
with Q the charge of the black hole. It is further shown that no black hole
solutions with rh<∣Q∣ can be obtained by solving the semiclassical
Einstein equations perturbatively.Comment: 7 pages, to appear in the Proceedings of the Ninth Marcel Grossmann
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