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Asymptotically hyperbolic black holes in Horava gravity
High Energy Physics - Theory · Submitted 6 Jan 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Both analytic and numeric solutions are studied which exhibit a causal boundary called the universal horizon, and are therefore black holes of the theory.
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The abstract, sentence by sentence
Solutions of Horava gravity that are asymptotically Lifshitz are explored. General near boundary expansions allow the calculation of the mass of these spacetimes via a Hamiltonian method. Both analytic and numeric solutions are studied which exhibit a causal boundary called the universal horizon, and are therefore black holes of the theory. The thermodynamics of an asymptotically Anti-de Sitter Horava black hole are verified.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Solutions of Horava gravity that are asymptotically Lifshitz are explored. | contribution 0.86 | 0.74 | 0.08 | asserted 0.90 |
| s1 | General near boundary expansions allow the calculation of the mass of these spacetimes via a Hamiltonian method. | method 0.97 | 0.79 | 0.09 | asserted 0.99 |
| s2 | Both analytic and numeric solutions are studied which exhibit a causal boundary called the universal horizon, and are therefore black holes of the theory. | result 0.74 | 0.86 | 0.46 | asserted 1.00 |
| s3 | The thermodynamics of an asymptotically Anti-de Sitter Horava black hole are verified. | result 0.88 | 0.83 | 0.17 | asserted 1.00 |
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The paper
Original abstract
Solutions of Horava gravity that are asymptotically Lifshitz are explored. General near boundary expansions allow the calculation of the mass of these spacetimes via a Hamiltonian method. Both analytic and numeric solutions are studied which exhibit a causal boundary called the universal horizon, and are therefore black holes of the theory. The thermodynamics of an asymptotically Anti-de Sitter Horava black hole are verified.
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References
How the literature uses it
17 arXiv papers cite this in 59 sentences
Papers citing it · 48 sentences without a confident label
Compares with it 3 papers
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But, in [ref] the khronon was considered as a part of the gravitational field, although in some cases their effects on the gravitational fields were assumed to be negligible.
Universal horizons and black holes in gravitational theories with broken Lorentz symmetry · Causal Structure of Gravitational Theories with Broken Lorentz Symmetry and Universal Horizons · 0.92
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This agrees with the value found by the on-shell Hamiltonian analysis in [ref] .
Horava-Lifshitz Black Hole Hydrodynamics · Equilibrium solution · 0.98
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The resulting solution will depend on one free parameter $ρ_0$ (similar to the Schwarzschild solution in GR, asymptotically flat Einstein-aether black holes in [ref] and finally the $z=1$ solution found in [ref] ).
New Asymptotically Lifshitz Black Holes in Horava gravity · Asymptotically Lifshitz Black Holes for $z ≠1$ · 0.89
Cites it as background 6 papers
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Asymptotically Lifshitz solutions were first studied in detail in [ref] in four-dimensional spacetime ($D=3$) by expanding the field equations in a power series around $r = 1/ρ= 0$.
New Asymptotically Lifshitz Black Holes in Horava gravity · Lifshitz Asymptotic Solutions · 0.95
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This has immediately attracted lot of attentions [ref] .
Universal horizons and black holes in gravitational theories with broken Lorentz symmetry · Introduction · 0.85
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So far, several exact black hole solutions with UH have been found in LV gravitational theories, including four-dimensional static asymptotically flat solutions of aether theory and Hořava gravity [ref] , four-dimensional static asymptotically (anti-) de sitter (Ads) solutions [ref] , three-dimensional fully rotating solution of infrared (IR) limit of Hořava gravity [ref] in the branch $c_14=0$, the black brane solutions with asymptotically Lifshitz property [ref] , charged static solutions in 3 and 4 dimensional [ref] , and the generalization to D dimensional static charged solutions [ref] .
Entropies and The First Laws of Black Hole Thermodynamics in Einstein-aether-Maxwell Theory · Introduction · 0.92
What it cites · 33 sentences without a confident label
Cites as support 3 papers
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Given that these spacetimes are vacuum solutions of Hořava gravity lends evidence to the proposal that this alternate theory of gravity is dual to generic NR QFTs [ref] .
Non-relativistic holography from Horava gravity · Discussion · 0.97
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Given that these spacetimes are vacuum solutions of Hořava gravity lends evidence to the proposal that this alternate theory of gravity is dual to generic NR QFTs [ref] .
String theory embeddings of non-relativistic field theories and their holographic Horava gravity duals · Discussion · 0.97
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Given that these spacetimes are vacuum solutions of Hořava gravity lends evidence to the proposal that this alternate theory of gravity is dual to generic NR QFTs [ref] .
Lifshitz Gravity for Lifshitz Holography · Discussion · 0.97
Cites as background 5 papers
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Hořava gravity is an alternate theory of gravity [ref] .
Quantum Gravity at a Lifshitz Point · Hořava gravity · 1.00
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The low energy action of Hořava gravity is expressed in terms of these fields as [ref] [Note that our coupling constants are not the same as [ref] , despite identical names.]: [equation] where $K_IJ≡1/2N(_̣t G_IJ-∇_I N_J-∇_J N_I)$ is the extrinsic curvature of the leaves of the foliation, $R$ is the Ricci scalar of the spatial metric $G_IJ$, $G$ is its determinant, and $Λ$ is the cosmological constant.
Lifshitz Gravity for Lifshitz Holography · Hořava gravity · 0.81
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This scalar field $ϕ$ is called the khronon [ref] and its level sets define the leaves of the foliation.
Models of non-relativistic quantum gravity: the good, the bad and the healthy · Khronon formalism · 0.85
Discussion
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