2007
DOI: 10.1088/1126-6708/2007/06/025
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Bubbling surface operators and S-duality

Abstract: We construct smooth asymptotically AdS 5 ×S 5 solutions of Type IIB supergravity corresponding to all the half-BPS surface operators in N = 4 SYM. All the parameters labeling a half-BPS surface operator are identified in the corresponding bubbling geometry. We use the supergravity description of surface operators to study the action of the SL(2, Z) duality group of N = 4 SYM on the parameters of the surface operator, and find that it coincides with the recent proposal by Gukov and Witten in the framework of th… Show more

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Cited by 106 publications
(180 citation statements)
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References 29 publications
(89 reference statements)
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“…Thermal properties and Wilson loops in the CFT dual to these geometries were studied in [127,128] while in [129,130,131] 1/2 BPS geometries corresponding to defects in the CFT were considered. In [132] the relation between phase space densities in the fermion formulation of the theory and generalized Young tableaux is studied.…”
Section: I-the 1/2 Bps Casementioning
confidence: 99%
“…Thermal properties and Wilson loops in the CFT dual to these geometries were studied in [127,128] while in [129,130,131] 1/2 BPS geometries corresponding to defects in the CFT were considered. In [132] the relation between phase space densities in the fermion formulation of the theory and generalized Young tableaux is studied.…”
Section: I-the 1/2 Bps Casementioning
confidence: 99%
“…This led to a natural gauge theory description of the tame case of the geometric Langlands correspondence. For an elegant supergravity analysis of the relevant family of surface operators, see [17].…”
Section: Introductionmentioning
confidence: 99%
“…Restricting to systems with large amounts of supersymmetry, large classes of geometries have been explicitly constructed. These include geometries describing Wilson lines [6,7], surface operators [8], defect theories [9,10] and theories with boundaries [11]. These explicit geometries have been used to provide non-trivial checks of the AdS/CFT correspondence [12,13].…”
Section: Jhep10(2014)103mentioning
confidence: 99%
“…We note that the metric is regular in string frame, although the coupling still diverges. 8 Next we examine the solution near A = 0. Assuming A ∼ 0 and eliminating G in favor of a second order equation for A, we obtain the approximate equation 2A + ∂ h A − ∂ 2 h A = 0, whose general solution is given by A ∼ C 3 e −h + C 4 e 2h .…”
Section: Jhep10(2014)103mentioning
confidence: 99%