Asymptotically Lifshitz spacetimes with universal horizons in dimensions
arXiv:1601.03274 · doi:10.1103/PhysRevD.93.064072
Abstract
Horava gravity theory possesses global Lifshitz space as a solution and has been conjectured to provide a natural framework for Lifshitz holography. We derive the conditions on the two derivative Horava gravity Lagrangian that are necessary for static, asymptotically Lifshitz spacetimes with flat transverse dimensions to contain a universal horizon, which plays a similar thermodynamic role as the Killing horizon in general relativity. Specializing to z=2 in 1+2 dimensions, we then numerically construct such regular solutions over the whole spacetime. We calculate the mass for these solutions and show that, unlike the asymptotically anti-de Sitter case, the first law applied to the universal horizon is straightforwardly compatible with a thermodynamic interpretation.
12 pages, 4 figures
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Cited by in corpus (12)
- Hořava Gravity at a Lifshitz Point: A Progress Report
- Three-dimensional charged Einstein-aether black holes and Smarr formula
- Thermal fluctuations of (non)linearly charged BTZ black hole in massive gravity
- Static and rotating universal horizons and black holes in gravitational theories with broken Lorentz invariance
- Hawking Radiation from Universal Horizons
- On the first law of black holes with a universal horizon
- No static black hole hairs in gravitational theories of gravity with broken Lorentz invariance
- Constructing entanglement wedges for Lifshitz spacetimes with Lifshitz gravity
- New Asymptotically Lifshitz Black Holes in Horava gravity
- Energy-entropy relation for asymptotically Lifshitz spacetimes with universal horizons
- Asymptotic flatness and nonflat solutions in the critical 2+1 Horava theory
- Exact analytic solutions in 2+1 Hořava gravity with cosmological constant