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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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 haoxu blackholeevaporationinlovelockgravitywithdiversedimensions AT manhongyung blackholeevaporationinlovelockgravitywithdiversedimensions |
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