Black holes and black branes in Lifshitz spacetimes
By J. Tarrío, S. Vandoren. 2011
189 citations recorded by the source corpus.
We construct analytic solutions describing black holes and black branes in asymptotically Lifshitz spacetimes with arbitrary dynamical exponent z and for arbitrary number of dimensions. The model considered consists of Einstein gravity with negative cosmological constant, a scalar, and N U(1) gauge fields with dilatonic-like couplings. We study the phase diagrams and thermodynamic instabilities of the solution, and find qualitative differences between the cases with 1 ≤ z < 2, z = 2 and z > 2.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/36fa4c3a2f3785ddac220cf17f1116bfcd4e11dd
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In Astronomy and Astrophysics
- J. Hartong
- N. Obers
- E. Kiritsis
- Marika Taylor
- Blaise Goutéraux
- B. Rollier
- M. Christensen
- Eric Bergshoeff
In Nuclear and High Energy Physics
- J. Hartong
- Marika Taylor
- N. Obers
- E. Kiritsis
- Blaise Goutéraux
- B. Rollier
- M. Christensen
- Aristomenis Donos
In Statistical and Nonlinear Physics
- J. Hartong
- N. Obers
- Marika Taylor
- E. Kiritsis
- B. Rollier
- Blaise Goutéraux
- M. Christensen
- Eric Bergshoeff
Citations in the corpus
- Lifshitz holography (2015, background): “Numerical solutions for Lifshitz black holes and branes have been found in [91, 75, 76, 92, 93, 94, 95, 96].”
- Boundary stress-energy tensor and Newton-Cartan geometry in Lifshitz holography (2013, background): “This gives a rationale for why one usually separates out one Maxwell field from the others in solutions of charged Lifshitz black holes as in [26, 28].”
- Generalized holographic quantum criticality at finite density (2011, methodology): “Note that this procedure could be repeated to generate new EMD solutions, for instance starting from the solutions uncovered in [58], which consider non-planar as well as multiple U(1) charge solutions.”