The zeroth law of black hole thermodynamics in arbitrary higher derivative theories of gravity
arXiv:2205.01648 · doi:10.1007/JHEP10(2022)013
Abstract
We consider diffeomorphism invariant theories of gravity with arbitrary higher derivative terms in the Lagrangian as corrections to the leading two derivative theory of Einstein's general relativity. We construct a proof of the zeroth law of black hole thermodynamics in such theories. We assume that a stationary black hole solution in an arbitrary higher derivative theory can be obtained by starting with the corresponding stationary solution in general relativity and correcting it order by order in a perturbative expansion in the coupling constants of the higher derivative Lagrangian. We prove that surface gravity remains constant on its horizon when computed for such stationary black holes, which is the zeroth law. We argue that the constancy of surface gravity on the horizon is related to specific components of the equations of motion in such theories. We further use a specific boost symmetry of the near horizon space-time of the stationary black hole to constrain the off-shell structure of the equations of motion. Our proof for the zeroth law is valid up to arbitrary order in the expansion in the higher derivative couplings.
References added, Minor typos corrected
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- Entropy-current for dynamical black holes in Chern-Simons theories of gravity
- Iyer-Wald ambiguities and gauge covariance of Entropy current in Higher derivative theories of gravity
- Quasinormal Modes and Shadows of Black Holes in Infinite Derivative Theory of Gravity
- Generalized Second Law for Non-minimally Coupled Matter Theories
- Birkhoff's Theorem and Uniqueness: A Peek Beyond General Relativity
- Perturbative Renormalisation Group Improved Black Hole Solution and its Quasinormal Modes