2006
DOI: 10.1088/1126-6708/2006/04/010
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Smooth geometries with four charges in four dimensions

Abstract: A class of axially symmetric, rotating four-dimensional geometries carrying D1, D5, KK monopole and momentum charges is constructed. The geometries are found to be free of horizons and singularities, and are candidates to be the gravity duals of microstates of the (0,4) CFT. These geometries are constructed by performing singularity analysis on a suitably chosen class of solutions of six-dimensional minimal supergravity written over a Gibbons-Hawking base metric. The properties of the solutions raise some inte… Show more

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Cited by 70 publications
(90 citation statements)
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References 43 publications
(71 reference statements)
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“…In particular bubbling solutions for black holes and black rings, to be described below, were developed in [95,96,97,98,99,100,101,102,103,104]. Four charge solutions in four dimensions have been discussed in [105,106]. Non-supersymmetric solutions were found and their properties explored in [107,108,109].…”
Section: Horizon-less Limits Of Known Black Hole Solutionsmentioning
confidence: 99%
“…In particular bubbling solutions for black holes and black rings, to be described below, were developed in [95,96,97,98,99,100,101,102,103,104]. Four charge solutions in four dimensions have been discussed in [105,106]. Non-supersymmetric solutions were found and their properties explored in [107,108,109].…”
Section: Horizon-less Limits Of Known Black Hole Solutionsmentioning
confidence: 99%
“…These solutions are independent of the GH fiber coordinate, ψ [37,38,[40][41][42]. The fluxes, Θ j are harmonic and are given by expressions of the form (3.6):…”
Section: The "Classic" Solutionsmentioning
confidence: 99%
“…The standard, bubbled microstate geometries [5,35,[37][38][39]42] allow singularities at points in the R 3 defined by y. Indeed, near such a singular point, P , one has V ∼ qp rp while one also requires that the Z I are finite as r p → 0 and the bubble equations require that µ(r p ) = 0.…”
Section: Jhep10(2013)137mentioning
confidence: 99%
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“…According to this proposal, a black hole quantum state is not well approximated by its classical geometry near its horizon, but is rather defined as a sum of microstates that are themselves well approximated by globally hyperbolic smooth geometries. While the search for the possible smooth geometries has met with some success in the case of extremal black holes, especially in the presence of supersymmetry [3][4][5][6][7][8][9][10][11], less progress has been made for the non-extremal black holes, for which only a handful of special solutions are known [12][13][14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%