Black hole evaporation in Lovelock gravity with diverse dimensions

We investigate the black hole evaporation process in Lovelock gravity with diverse dimensions. By selecting the appropriate coefficients, the space-time solutions can possess a unique AdS vacuum with a fixed cosmological constant Λ=−(d−1)(d−2)2ℓ2. The black hole solutions can be divided into two cas...

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Main Authors: Hao Xu, Man-Hong Yung
Format: Article
Language:English
Published: Elsevier 2019-07-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269319303429
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spelling doaj-49ac2c38386a4dcb8e409b31b9b5325e2020-11-25T00:27:31ZengElsevierPhysics Letters B0370-26932019-07-017947782Black hole evaporation in Lovelock gravity with diverse dimensionsHao Xu0Man-Hong Yung1Institute for Quantum Science and Engineering, Department of Physics, Southern University of Science and Technology, Shenzhen 518055, China; Department of Physics, University of Science and Technology of China, Hefei 230026, China; Corresponding author.Institute for Quantum Science and Engineering, Department of Physics, Southern University of Science and Technology, Shenzhen 518055, China; Shenzhen Key Laboratory of Quantum Science and Engineering, Shenzhen, 518055, ChinaWe investigate the black hole evaporation process in Lovelock gravity with diverse dimensions. By selecting the appropriate coefficients, the space-time solutions can possess a unique AdS vacuum with a fixed cosmological constant Λ=−(d−1)(d−2)2ℓ2. The black hole solutions can be divided into two cases: d>2k+1 and d=2k+1. In the case of d>2k+1, the black hole is in an analogy with the Schwarzschild AdS black hole, and the life time is bounded by a time of the order of ℓd−2k+1, which reduces Page's result on the Einstein gravity in k=1. In the case of d=2k+1, the black hole resembles the three dimensional black hole. The black hole vacuum corresponds to T=0, so the black hole will take infinite time to evaporate away for any initial states, which obeys the third law of thermodynamics. In the asymptotically flat limit ℓ→∞, the system reduces to the pure Lovelock gravity that only possesses the highest k-th order term. For an initial mass M0, the life time of the black hole is in the order of M0d−2k+1d−2k−1.http://www.sciencedirect.com/science/article/pii/S0370269319303429
collection DOAJ
language English
format Article
sources DOAJ
author Hao Xu
Man-Hong Yung
spellingShingle Hao Xu
Man-Hong Yung
Black hole evaporation in Lovelock gravity with diverse dimensions
Physics Letters B
author_facet Hao Xu
Man-Hong Yung
author_sort Hao Xu
title Black hole evaporation in Lovelock gravity with diverse dimensions
title_short Black hole evaporation in Lovelock gravity with diverse dimensions
title_full Black hole evaporation in Lovelock gravity with diverse dimensions
title_fullStr Black hole evaporation in Lovelock gravity with diverse dimensions
title_full_unstemmed Black hole evaporation in Lovelock gravity with diverse dimensions
title_sort black hole evaporation in lovelock gravity with diverse dimensions
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2019-07-01
description We investigate the black hole evaporation process in Lovelock gravity with diverse dimensions. By selecting the appropriate coefficients, the space-time solutions can possess a unique AdS vacuum with a fixed cosmological constant Λ=−(d−1)(d−2)2ℓ2. The black hole solutions can be divided into two cases: d>2k+1 and d=2k+1. In the case of d>2k+1, the black hole is in an analogy with the Schwarzschild AdS black hole, and the life time is bounded by a time of the order of ℓd−2k+1, which reduces Page's result on the Einstein gravity in k=1. In the case of d=2k+1, the black hole resembles the three dimensional black hole. The black hole vacuum corresponds to T=0, so the black hole will take infinite time to evaporate away for any initial states, which obeys the third law of thermodynamics. In the asymptotically flat limit ℓ→∞, the system reduces to the pure Lovelock gravity that only possesses the highest k-th order term. For an initial mass M0, the life time of the black hole is in the order of M0d−2k+1d−2k−1.
url http://www.sciencedirect.com/science/article/pii/S0370269319303429
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AT manhongyung blackholeevaporationinlovelockgravitywithdiversedimensions
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