corner
corner

Phys. Rev. D 51, 4302–4314 (1995)

Entropy, area, and black hole pairs

Download: PDF (550 kB) Buy this article Export: BibTeX or EndNote (RIS)

S. W. Hawking and Gary T. Horowitz
Isaac Newton Institute for Mathematical Sciences, University of Cambridge, 20 Clarkson Rd., Cambridge CB3 0EH, United Kingdom

Simon F. Ross
Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Silver St., Cambridge CB3 9EW, United Kingdom

Received 30 September 1994; published in the issue dated 15 April 1995

We clarify the relation between gravitational entropy and the area of horizons. We first show that the entropy of an extreme Reissner-Nordström black hole is zero, despite the fact that its horizon has nonzero area. Next, we consider the pair creation of extremal and nonextremal black holes. It is shown that the action which governs the rate of this pair creation is directly related to the area of the acceleration horizon and (in the nonextremal case) the area of the black hole event horizon. This provides a simple explanation of the result that the rate of pair creation of nonextreme black holes is enhanced by precisely the black hole entropy. Finally, we discuss black hole annihilation, and argue that Planck scale remnants are not sufficient to preserve unitarity in quantum gravity.

© 1995 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.51.4302
DOI:
10.1103/PhysRevD.51.4302
PACS:
04.70.Dy, 04.50.+h