1990
DOI: 10.1103/physrevd.41.1142
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Evolution of charged evaporating black holes

Abstract: The evaporative evolution of charged nonrotating black holes is studied by numerically integrating a set of coupled differential equations describing the charge and mass as functions of time. We find that large charged black holes will evolve through a region (in the black-hole configuration space) of positive specific heat, undergoing two phase transitions as they evaporate. The region is approximately bounded by a < ( Q / M )~ < 1 and M > 2.03X 1 0 '~~. Unlike rotating black holes (which always evolve toward… Show more

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Cited by 118 publications
(167 citation statements)
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“…This shows that the loss of charge process of the hole is described by Schwinger effect, as in ordinary flat-space quantum eletrodynamics. This result can be understood by noting that in the large radius hypothesis adopted above, the event horizon of the hole is much larger than the Compton wavelength of the emitted particles, and the radiated pairs can be viewed as being produced by the electic field of the hole, and not by the gravitational field [7]. Our result is compatible with the usual rate of electron-positron pair creation; indeed, remember that we obtained it in a reduced 1+1 dimensional spacetime.…”
Section: Functional Integral and Transition Ratiosupporting
confidence: 81%
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“…This shows that the loss of charge process of the hole is described by Schwinger effect, as in ordinary flat-space quantum eletrodynamics. This result can be understood by noting that in the large radius hypothesis adopted above, the event horizon of the hole is much larger than the Compton wavelength of the emitted particles, and the radiated pairs can be viewed as being produced by the electic field of the hole, and not by the gravitational field [7]. Our result is compatible with the usual rate of electron-positron pair creation; indeed, remember that we obtained it in a reduced 1+1 dimensional spacetime.…”
Section: Functional Integral and Transition Ratiosupporting
confidence: 81%
“…They spontaneously radiate their own charge and, once they are neutralized, continue to evaporate according to the usual Hawking process. On the other hand, for the same Q/M ratio charge, the holes more massive lose mass by the Hawking process, while they conserve the same electric charge (the most massive even become "extreme"), before that the neutralization process really happens [7].…”
Section: Functional Integral and Transition Ratiomentioning
confidence: 99%
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“…Hiscock and Weems [19] considered the loss of charge and mass for the exteriors of charged black holes of large initial mass. They assumed adiabatic evolution, so that the spacetime could be described by a sequence of Reissner-Nordström metrics with the mass and charge of the black hole being slowly varying functions of time.…”
Section: Introductionmentioning
confidence: 99%
“…Specifically, any charged black hole with mass less than approximately 10 5 M ⊙ will rapidly lose any initial electric charge [4,5]. Furthermore, unless there are a large number of undiscovered massless scalar fields in nature [6], black holes will quickly spin down, with their specific angular momentum a = J/M decreasing at roughly twice the rate their mass decreases [3].…”
mentioning
confidence: 99%