Abstract

We present arguments for the existence of five-dimensional rotating black holes with equal magnitude angular momenta in Einstein–Gauss–Bonnet theory with negative cosmological constant. These solutions posses a regular horizon of spherical topology and approach asymptotically an anti-de Sitter spacetime background. We discuss the general properties of these solutions and, using an adapted counterterm prescription, we compute their entropy and conserved charges.

Highlights

  • The most general theory of gravity leading to second order field equations for the metric is the so called Einstein-Gauss-Bonnet (EGB) theory, which contains quadratic powers of the curvature

  • The study of black holes with higher derivative curvature in Anti-de Sitter (AdS) spaces has been considered by many authors in the recent years

  • Static AdS black hole solutions in EGB gravity are known in closed form, presenting a number of interesting features

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Summary

Introduction

The most general theory of gravity leading to second order field equations for the metric is the so called Einstein-Gauss-Bonnet (EGB) theory, which contains quadratic powers of the curvature. The main purpose of this work is to present numerical evidence for the existence of a different class of rotating solutions in d = 4 + 1 EGB theory with negative cosmological constant, approaching asymptotically an AdS spacetime background. These solutions are found within a nonperturbative approach, by directly solving the EGB equations with suitable boundary conditions. They posses a regular horizon of spherical topology and have two equal magnitude angular momenta. The same approach has been employed recently to construct Einstein-Maxwell rotating black hole solutions in higher dimensions [8, 9]

The action and boundary counterterms
The metric ansatz and known limits
Black hole properties
The global charges and entropy of solutions
Numerical results
Further remarks
Full Text
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