The fate of Schwarzschild–de Sitter black holes in f(R) gravity

Author:

Addazi Andrea12,Capozziello Salvatore345ORCID

Affiliation:

1. Dipartimento di Fisica, Università di L’Aquila, 67010 Coppito AQ, Italy

2. Laboratori Nazionali del Gran Sasso (INFN), 67010 Assergi AQ, Italy

3. Dipartimento di Fisica, Università di Napoli “Federico II”, Complesso Universitario di Monte S. Angelo, Edificio G, Via Cinthia, I-80126, Napoli, Italy

4. Istituto Nazionale di Fisica Nucleare (INFN) Sez. di Napoli, Complesso Universitario di Monte S. Angelo, Edificio G, Via Cinthia, I-80126, Napoli, Italy

5. Gran Sasso Science Institute (INFN), Viale F. Crispi, 7, I-67100, L’Aquila, Italy

Abstract

The semiclassical effects of anti-evaporating black holes can be discussed in the framework of f(R) gravity. In particular, the Bousso–Hawking–Nojiri–Odinstov anti-evaporation instability of degenerate Schwarzschild–de Sitter black holes (the so-called Nariai spacetime) leads to a dynamical increasing of black hole horizon in f(R) gravity. This phenomenon causes the following transition: emitting marginally trapped surfaces (TS) become space-like surfaces before the effective Bekenstein–Hawking emission time. As a consequence, Bousso–Hawking thermal radiation cannot be emitted in an anti-evaporating Nariai black hole. Possible implications in cosmology and black hole physics are also discussed.

Publisher

World Scientific Pub Co Pte Lt

Subject

General Physics and Astronomy,Astronomy and Astrophysics,Nuclear and High Energy Physics

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