2005
DOI: 10.1002/prop.200410214
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New phases of thermal SYM and LST from Kaluza‐Klein black holes

Abstract: We review the recently found map that takes any static and neutral Kaluza-Klein black hole, i.e. any static and neutral black hole on Minkowski-space times a circle M d × S 1 , and maps it to a corresponding solution for a non-and near-extremal brane on a circle. This gives a precise connection between phases of Kaluza-Klein black holes and the thermodynamic behavior of the non-gravitational theories dual to near-extremal branes on a circle. In particular, for the thermodynamics of strongly-coupled supersymmet… Show more

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Cited by 16 publications
(34 citation statements)
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“…36 In this section we discuss gauge/gravity duals in which the gravity side exhibits a Gregory-Laflamme instability. The presence of this classical gravitational instability in the bulk has important consequences for the gauge theory on the boundary, which we review following [56,57,155,66,58]. Focusing on a set of examples that are closely connected to the material of this review we will consider first D-branes on a circle, where the relevant gauge theory is super-Yang-Mills theory on a circle.…”
Section: Holographic Implicationsmentioning
confidence: 99%
See 1 more Smart Citation
“…36 In this section we discuss gauge/gravity duals in which the gravity side exhibits a Gregory-Laflamme instability. The presence of this classical gravitational instability in the bulk has important consequences for the gauge theory on the boundary, which we review following [56,57,155,66,58]. Focusing on a set of examples that are closely connected to the material of this review we will consider first D-branes on a circle, where the relevant gauge theory is super-Yang-Mills theory on a circle.…”
Section: Holographic Implicationsmentioning
confidence: 99%
“…In this limit the dynamics of the theory is believed to reduce to a string theory without gravity called Little String Theory (LST), or more precisely (2, 0) LST of type A N −1 [166,167,168,169,170]. 45 In this subsection (see also [155,58]) we will consider the thermodynamics of the near-extremal NS5-brane in type IIA string theory using as a starting point the S-dual description as a near-extremal M5-brane on a transverse circle and the input of the phases obtained from six-dimensional neutral Kaluza-Klein black holes in Section 3. Other interesting work on the thermodynamics of LST can be found in [171,164,172,173,174,175,176,177,178,179,180].…”
Section: Little String Theorymentioning
confidence: 99%
“…In particular, for the strongly coupled region, the dual D1-brane system can be described by certain black holes in supergravity, with a compact spatial circle. Then arguments from the dual gravity model indicate a first order Gregory-Laflamme 82,83 phase transition between the black hole solutions localized on the circle and uniform black hole solutions which wrap the circle 80,81,84,85,86,87,88,89 . Translating back to the SYM, the dual gravity model predicts the parametric dependence of the transition temperature against dimensionless circle coupling -a dependence that seemingly cannot be deduced by simple SYM considerations.…”
Section: D1-brane Thermodynamics From Lattice Symmentioning
confidence: 99%
“…In this work, we wish to study how the compactness of extra dimensions changes the dynamics of such higher-dimensional gravity scenarios. There is considerable literature on Kaluza-Klein BHs and BHs on cylinders [19][20][21][22], but, to the best of our knowledge, the full non-linear dynamics of BHs on such spacetimes remains unexplored.…”
Section: Introductionmentioning
confidence: 99%