Classical and thermodynamic stability of black branes
By Harvey Reall. 2001
196 citations recorded by the source corpus.
It is argued that many nonextremal black branes exhibit a classical Gregory-Laflamme instability if, and only if, they are locally thermodynamically unstable. For some black branes, the Gregory-Laflamme instability must therefore disappear near extremality. For the black p-branes of the type II supergravity theories, the Gregory-Laflamme instability disappears near extremality for p=1,2,4 but persists all the way down to extremality for p=5,6 (the black D3-brane is not covered by the analysis of this paper). This implies that the instability also vanishes for the near-extremal black M2 and M5-brane solutions.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/ece9d121fe696907935ff5511d9f5e3d1497c8ef
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Citations in the corpus
- A Gravitational instability in higher dimensions (2002, methodology): “This should be contrasted with a similar embedding into a higher dimensional Ricci flat spacetime where the stability properties get worse due to negative Lichnerowicz modes in the initial spacetime [31], such as the Gregory-Laflamme instability of nonextremal black strings [32, 33, 25].”
- Topology change in general relativity, and the black-hole black-string transition (2002, methodology): “Other contributions include the realization of the connection between the GL instability and negative specific heat [8, 9], a discussion of the charged non-uniform black string [10], an attempt to use the Petrov classification to derive the metric of the non-uniform string [11], a numerical study of”
- Ricci solitons, Ricci flow and strongly coupled CFT in the Schwarzschild Unruh or Boulware vacua (2011, background): “There is of course no direct relationship between a Euclidean negative mode and a Lorentzian unstable mode as one cannot simply continue a time dependent mode and its boundary conditions between the two signatures, so a correspondence only holds for static perturbations [44].”
- The phase transition between caged black holes and black strings (2004, background): “ngth LGL = 2π/kGL ∼ r0/ √ d when it is quite “fat” (namely r0 ≫ LGL) and indicates that such a string would not decay into a black hole which would not “fit” inside the extra dimension. 7Footnote 4 of [38] explains “This relationship (eq. 2.11 - BK) was noted in [41], although the connection with cla”
- Stability of Black Holes and Black Branes (2012, background): “(9)Another argument in favor of the Gubser Mitra conjecture based on a “Wick rotation”, applicable to certain static black branes, has previously been given by [31].”
- A new approach to static numerical relativity and its application to Kaluza–Klein black holes (2009, methodology): “Reall showed that this is simply related to the usual four-dimensional Schwarzschild negative mode [56] with the Gregory–Laflamme zero mode of the uniform string with radius rc being given by Ac μν (r) e iωz.”
- Numerical methods for finding stationary gravitational solutions (2015, background): “[119] H.”
- On non-uniform black branes (2001, background): “Some evidence for this claim was presented in [8, 9], and further arguments have appeared in [10, 11].”
- Thermodynamics of Rotating Black Holes and Black Rings: Phase Transitions and Thermodynamic Volume (2014, unknown): “, [80–84].”
- Mimicking the QCD equation of state with a dual black hole (2008, background): “It was proposed in [13, 14] and further argued in [19] that, in the absence of conserved charges related to gauge symmetries, existence of a Gregory-Laflamme instability [20, 21]”
- GRAVITATIONAL PERTURBATIONS OF HIGHER DIMENSIONAL ROTATING BLACK HOLES (2006, background): “They admit a static zero mode [43] that signifies the onset of instability [44] and suggests the existence of a new family of solutions bifurcating from the known ones [45].”