2019
DOI: 10.1007/jhep11(2019)019
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Little strings, long strings, and fuzzballs

Abstract: At high energy densities, fivebranes are populated by a Hagedorn phase of so-called little strings, whose statistical mechanics underlies black fivebrane thermodynamics. A particular limit of this phase yields BTZ black holes in AdS 3 , leading us to the idea that in this context fuzzballs and highly excited little strings are one and the same. We explore these ideas through an analysis of D-brane probes of fivebrane supertube backgrounds. String theory dynamics on these backgrounds is described by an exactly … Show more

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Cited by 52 publications
(120 citation statements)
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References 147 publications
(374 reference statements)
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“…In the geometrical description as a null-gauged sigma model on a Lunin-Mathur background, D-branes ending on the fivebranes localize the fivebranes at discrete (relative) positions determined by the quantization of worldvolume JHEP12(2020)135 flux. This phenomenon was first seen in our analysis of D-branes in the null-gauged WZW model in [22]; we verify that this structure continues to hold in the deformation of the circular fivebrane array to an elliptical array, and propose that it holds in general Lunin-Mathur geometries. On the Landau-Ginsburg side, the fivebrane locations are directly coded by the zeros of the holomorphic worldvolume superpotential; we exhibit a precise map between the parameters of the superpotential and those that determine the shape profile F I (v) of the supertube source in the supergravity description.…”
Section: Introductionsupporting
confidence: 78%
See 2 more Smart Citations
“…In the geometrical description as a null-gauged sigma model on a Lunin-Mathur background, D-branes ending on the fivebranes localize the fivebranes at discrete (relative) positions determined by the quantization of worldvolume JHEP12(2020)135 flux. This phenomenon was first seen in our analysis of D-branes in the null-gauged WZW model in [22]; we verify that this structure continues to hold in the deformation of the circular fivebrane array to an elliptical array, and propose that it holds in general Lunin-Mathur geometries. On the Landau-Ginsburg side, the fivebrane locations are directly coded by the zeros of the holomorphic worldvolume superpotential; we exhibit a precise map between the parameters of the superpotential and those that determine the shape profile F I (v) of the supertube source in the supergravity description.…”
Section: Introductionsupporting
confidence: 78%
“…Recent work on null-gauged sigma models for fivebrane backgrounds has focused on cosets where the "upstairs" (10+2)-dimensional spacetime contains global AdS 3 × S 3 [14,21,22]. The simplest example of the family of models that can be obtained in this way is the Coulomb branch circular array of fivebranes [11,12,14], where the isometry that is gauged corresponds to the Killing vectors in eq.…”
Section: Jhep12(2020)135mentioning
confidence: 99%
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“…Footnote a similar gap has recently been observed in[29] in a closely related context 6. The be precise, in one of the chambers that we consider we face a technical problem in the computation of the holomorphic Euler number via methods of algebraic topology, there we resort to the Abelianization technique of[11].…”
mentioning
confidence: 52%
“…[28], for a review), and which appear in the microstates entropy counting done in [29] and more recently in e.g. [30], in terms of strings living on the fivebrane.…”
Section: Jhep08(2020)020mentioning
confidence: 99%