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Topological black holes in Hořava-Lifshitz gravity

Rong-Gen CaiKey Laboratory of Frontiers in Theoretical Physics, Institute of Theoretical Physics, Chinese Academy of Sciences, P.O. Box 2735, Beijing 100190, China and Kavli Institute for Theoretical Physics China (KITPC), Chinese Academy of Sciences, P.O. Box 2735, Beijing 100190, ChinaLi-Ming CaoAsia Pacific Center for Theoretical Physics, Pohang, Gyeongbuk 790-784, KoreaNobuyoshi OhtaDepartment of Physics, Kinki University, Higashi-Osaka, Osaka 577-8502, Japan
2009en
ABI

Abstract

We find topological (charged) black holes whose horizon has an arbitrary constant scalar curvature $2k$ in Ho\ifmmode \check{r}\else \v{r}\fi{}ava-Lifshitz theory. Without loss of generality, one may take $k=1$, 0, and $\ensuremath{-}1$. The black hole solution is asymptotically anti--de Sitter with a nonstandard asymptotic behavior. Using the Hamiltonian approach, we define a finite mass associated with the solution. We discuss the thermodynamics of the topological black holes and find that the black hole entropy has a logarithmic term in addition to an area term. We find a duality in Hawking temperature between topological black holes in Ho\ifmmode \check{r}\else \v{r}\fi{}ava-Lifshitz theory and Einstein's general relativity: the temperature behaviors of black holes with $k=1$, 0, and $\ensuremath{-}1$ in Ho\ifmmode \check{r}\else \v{r}\fi{}ava-Lifshitz theory are, respectively, dual to those of topological black holes with $k=\ensuremath{-}1$, 0, and 1 in Einstein's general relativity. The topological black holes in Ho\ifmmode \check{r}\else \v{r}\fi{}ava-Lifshitz theory are thermodynamically stable.

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