2017
DOI: 10.1103/physrevd.95.106005
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Soft hairy horizons in three spacetime dimensions

Abstract: We discuss some aspects of soft hairy black holes and a new kind of "soft hairy cosmologies", including a detailed derivation of the metric formulation, results on flat space, and novel observations concerning the entropy. Remarkably, like in the case with negative cosmological constant, we find that the asymptotic symmetries for locally flat spacetimes with a horizon are governed by infinite copies of the Heisenberg algebra that generate soft hair descendants. It is also shown that the generators of the three… Show more

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Cited by 94 publications
(196 citation statements)
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References 93 publications
(248 reference statements)
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“…In this section we review material that appeared in [1,9], whose conventions and notations we use. We start with the near horizon expansion of non-extremal black holes (or cosmologies).…”
Section: Black Hole Entropy In Three Dimensionsmentioning
confidence: 99%
See 3 more Smart Citations
“…In this section we review material that appeared in [1,9], whose conventions and notations we use. We start with the near horizon expansion of non-extremal black holes (or cosmologies).…”
Section: Black Hole Entropy In Three Dimensionsmentioning
confidence: 99%
“…The near horizon boundary conditions of [1,9] allow for arbitrary variations of the horizon radius function γ and the rotation function ω but no variations of Rindler acceleration α, i.e., δγ 0 δω and δα = 0. For constant Rindler acceleration the equations of motion imply conservation of these functions in time, ∂ t γ = 0 = ∂ t ω, which are near horizon analogs of the holographic Ward identities ∂ ∓ T ±± = 0 for the usual Brown-Henneaux boundary conditions [20].…”
Section: Black Hole Entropy In Three Dimensionsmentioning
confidence: 99%
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“…We will study the fluid interpretation of 3d flat gravity in a companion paper [30]. In the future, it would be interesting to use the fluid perspective to understand the symmetry groups appearing at Rindler horizons [31], with negative cosmological constant [32,33], and in more general theories of gravity (e.g., [34,35]). The remainder of this paper is organized as follows.…”
Section: Jhep10(2017)049mentioning
confidence: 99%