Charged black holes in AdS spaces in 4D Einstein Gauss-Bonnet gravity

By Pedro G. S. Fernandes. Physics Letters B, 2020

253 citations recorded by the source corpus.

Abstract Recently a non-trivial 4-dimensional theory of gravity that claims to circumvent Lovelock's theorem and avoid Ostrogradsky instability was formulated in Glavan and Lin (2020) [1] . This theory, named “4D Einstein Gauss-Bonnet gravity”, presents several novel predictions for cosmology and black hole physics. In this paper, we generalize the vacuum black hole solution of Glavan & Lin to include electric charge in an anti-de Sitter space and explore some properties of this solution such as the asymptotics, properties of the horizons, the general relativity limit and thermodynamics.

Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics

View Paper: https://www.semanticscholar.org/paper/ae1f220a439f7b92552326a8d218c7bbe2a03173

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Citations in the corpus

The 4D Einstein–Gauss–Bonnet theory of gravity: a review (2022, background): “The temperature of this black hole can be computed to be [61]”
A note on the novel 4D Einstein–Gauss–Bonnet gravity (2020, background): “[19–51]), the dimensionalregularization prescription has not been justified with the matched rigor.”
Shadows and photon spheres with spherical accretions in the four-dimensional Gauss–Bonnet black hole (2020, background): “Many characteristics of the four-dimensional Gauss-Bonnet black hole have been investigated [23, 24, 25, 26, 27, 28, 29, 30, 31, 32].”
Derivation of regularized field equations for the Einstein-Gauss-Bonnet theory in four dimensions (2020, methodology): “[15] P.”
Gravitational lensing by black holes in the 4D Einstein-Gauss-Bonnet gravity (2020, background): “J C A P 0 9 ( 2 0 2 0 ) 0 3 0 the charged case [17]; this kind of solution for the Lovelock gravity has been obtained in refs.”
Extended thermodynamics and microstructures of four-dimensional charged Gauss-Bonnet black hole in AdS space (2020, methodology): “[30]: ds(2) = −f(r)dt(2) + 1 f(r) dr(2) + r(2)(dθ(2) + sin(2) θdφ(2)), (3)”