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Quasi-Topological Lifshitz Black Holes
High Energy Physics - Theory · Submitted 18 Jan 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Furthermore, we examine black hole solutions and their thermodynamics in this situation and find that a negative quasi-topological term, just like a positive Gauss-Bonnet term, prevents instabilities in what are ordinarily unstable Einsteinian black holes.
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The abstract, sentence by sentence
We investigate the effects of including a quasi-topological cubic curvature term to the Gauss-Bonnet action to five dimensional Lifshitz gravity. We find that a new set of Lifshitz black hole solutions exist that are analogous to those obtained in third-order Lovelock gravity in higher dimensions. No additional matter fields are required to obtain solutions with asymptotic Lifshitz behaviour, though we also investigate solutions with matter. Furthermore, we examine black hole solutions and their thermodynamics in this situation and find that a negative quasi-topological term, just like a positive Gauss-Bonnet term, prevents instabilities in what are ordinarily unstable Einsteinian black holes.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate the effects of including a quasi-topological cubic curvature term to the Gauss-Bonnet action to five dimensional Lifshitz gravity. | contribution 0.98 | 0.92 | 0.07 | asserted 0.79 |
| s1 | We find that a new set of Lifshitz black hole solutions exist that are analogous to those obtained in third-order Lovelock gravity in higher dimensions. | result 1.00 | 0.96 | 0.40 | asserted 1.00 |
| s2 | No additional matter fields are required to obtain solutions with asymptotic Lifshitz behaviour, though we also investigate solutions with matter. | result 0.97 | 0.88 | 0.10 | asserted 1.00 |
| s3 | Furthermore, we examine black hole solutions and their thermodynamics in this situation and find that a negative quasi-topological term, just like a positive Gauss-Bonnet term, prevents instabilities in what are ordinarily unstable Einsteinian black holes. | result 0.99 | 0.95 | 0.47 | asserted 1.00 |
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The paper
Original abstract
We investigate the effects of including a quasi-topological cubic curvature term to the Gauss-Bonnet action to five dimensional Lifshitz gravity. We find that a new set of Lifshitz black hole solutions exist that are analogous to those obtained in third-order Lovelock gravity in higher dimensions. No additional matter fields are required to obtain solutions with asymptotic Lifshitz behaviour, though we also investigate solutions with matter. Furthermore, we examine black hole solutions and their thermodynamics in this situation and find that a negative quasi-topological term, just like a positive Gauss-Bonnet term, prevents instabilities in what are ordinarily unstable Einsteinian black holes.
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References
How the literature uses it
21 arXiv papers cite this in 27 sentences
Papers citing it · 10 sentences without a confident label
Builds on it 1 paper
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After the work of [ref] , the generalization to Lifshitz solution has been done in [ref] .
Hyperscaling-violating Lifshitz Solutions in Cubic Gravity · Black Hole Solution · 0.83
Compares with it 1 paper
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Similar to the effect of the quasi-topological term in numerical black hole solutions [ref] , the thermodynamic behaviour of the quasi-topological term closely follows Gauss-Bonnet thermodynamics for black holes beyond a certain radius (on the order of $r_h ∼1$).
Quasi-topological Reissner-Nordstr\"om Black Holes · RN Thermodynamics · 0.93
Cites it as background 14 papers
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Quasitopological gravity is one the most important modified gravities that has been studied in Refs. [ref] .
Thermodynamics of Rotating Lifshitz Dilaton Black Brane in Quartic Quasitopological gravity · Introduction · 0.94
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Attempts have been made to find analytic and numeric black hole/brane solutions which asymptotically admit Lifshitz geometry [ref] .
Asymptotically Lifshitz Brane-World Black Holes · Introduction · 0.88
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Until now, some investigations of the quasitopological black hole solutions have been done [ref] .
Yang-Mills black holes in Quasitopological gravity · Introduction · 0.97
What it cites · 21 sentences without a confident label
Uses the method or tool of 3 papers
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We are then able to write the equations of motion in the same manner as [ref] , obtaining the conserved quantity [equation] This derivation was performed using the form of the quasi-topological Lagrangian for $D$ dimensions, given by ([ref]), and the form of the conserved quantity was checked explicitly for $D$ from $7$ through $11$ to determine the dimensionally independent form given.
Thermodynamics of Lovelock-Lifshitz Black Branes · The conserved quantity along the radial coordinate $r$ · 0.94
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With these ODEs, initial conditions are chosen from the series solution (evaluated just beyond the horizon), and then the shooting method (explained in [ref] ) is used to obtain solutions.
Black holes in asymptotically Lifshitz spacetime · Numerical Solutions · 0.95
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With these ODEs, initial conditions are chosen from the series solution (evaluated just beyond the horizon), and then the shooting method (explained in [ref] ) is used to obtain solutions.
Lifshitz Topological Black Holes · Numerical Solutions · 0.95
Compares with 3 papers
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Although the asymptotic behaviour of our solution is different from Ref. [ref] and $f(r) ≠g(r)$, we obtain the same result: [equation] where $D$ is the number of dimensions and $A$ is the surface area of the black hole (since our metric is spherically symmetric, the surface area will be proportional to $r^D-2_0$).
Black Holes in Quasi-topological Gravity · Thermodynamics · 0.99
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This solution matches the form of one obtained in 3rd order Lovelock gravity for $D>6$ [ref] , as our field equations are of the same form.
Thermodynamic Instability of Black Holes of Third Order Lovelock Gravity · Matter-free Solutions · 0.99
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Due to the equivalence of our field equations, they match the values obtained in third order Lovelock gravity [ref] , once the substitutions $μL^4 =-α̂_3$ and $λL^2 =α̂_2$ are made.
Lovelock-Lifshitz Black Holes · Large $r$ Series Solutions · 1.00
Cites as background 11 papers
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Some new exact black hole solutions were obtained as well as a broad class of numerical solutions, and asymptotic Lifshitz solutions with curvature-squared terms in the action have also been investigated [ref] .
Analytic Lifshitz black holes in higher dimensions · Introduction · 0.80
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Some new exact black hole solutions were obtained as well as a broad class of numerical solutions, and asymptotic Lifshitz solutions with curvature-squared terms in the action have also been investigated [ref] .
A Lifshitz Black Hole in Four Dimensional R^2 Gravity · Introduction · 0.80
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Some new exact black hole solutions were obtained as well as a broad class of numerical solutions, and asymptotic Lifshitz solutions with curvature-squared terms in the action have also been investigated [ref] .
Lifshitz Black Hole in Three Dimensions · Introduction · 0.80
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