Abstract

We consider circular Wilson loops in a defect version of mathcal{N} = 4 super-Yang- Mills theory which is dual to the D3-D5 brane system with k units of flux. When the loops are parallel to the defect, we can construct both BPS and non-BPS operators, depending on the orientation of the scalar couplings in the R-symmetry directions. At strong ’t Hooft coupling we observe, in the non supersymmetric case, a Gross-Ooguri-like phase transition in the dual gravitational theory: the familiar disk solution dominates, as expected, when the operator is far from the defect while a cylindrical string worldsheet, connecting the boundary loop with the probe D5-brane, is favourite below a certain distance (or equivalently for large radii of the circles). In the BPS case, instead, the cylindrical solution does not exist for any choice of the physical parameters, suggesting that the exchange of light supergravity modes always saturate the expectation value at strong coupling. We study the double-scaling limit for large k and large ’t Hooft coupling, finding full consistency in the non-BPS case between the string solution and the one-loop perturbative result. Finally we discuss, in the BPS case, the failure of the double-scaling limit and the OPE expansion of the Wilson loop, finding consistency with the known results for the one-point functions of scalar composite operators.

Highlights

  • In the presence of a defect we expect that the structure of the operator product expansion (OPE) for the circular Wilson loop is unchanged, due to the fact that we are effectively probing the operator at infinite distance or, alternatively, because the ultraviolet properties of the theory are insensible to the boundary

  • While at level of correlation functions of local operators there has been a considerable amount of investigations in this field, much less attention has been devoted to the behavior of non-local operators: in this paper we tried to fill partially this gap, studying the fate of the circular Wilson loop in the defect N = 4 Super YangMills theory both at strong and weak coupling

  • The main result has been the discovery of a novel Gross-Ooguri type transition, separating a phase in which the dome solution, associated with the Wilson loop in absence of defect, dominates from a situation in which a cylindrical minimal surface attached to the defect D5 brane describes the non-local operator

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Summary

Prelude

The goal of the present paper is to study the vacuum expectation value of a circular Maldacena-Wilson loop in a four-dimensional dCFT given by N = 4 SYM theory with a co-dimension one hyperplane inserted at x3 = 0 as in [3, 5, 9]. An Higgsed N = 4 SYM lives in the x3 > 0 region, with gauge group SU (N ), where three scalar fields receive a x3-dependent VEV. The presence of the defect implies that fields living in the x3 > 0 region will have a non-trivial vacuum solution: by imposing that a part of the supersymmetry is preserved a specific profile is obtained for the scalars.

Setting-up the geometric description
General solution for the connected extremal surface
The distance from the defect
The area
Transition: connected solution vs dome
Perturbation theory: the non-BPS case
Comparing perturbative analysis with the strong coupling analysis
Perturbation theory: the BPS case
Operator product expansion of the Wilson loop
Wilson loop OPE and one-point functions
Conclusions and outlook
A Expression for the distance from the defect
E Connected solution as correlator between two circles of different radii
F Basis for chiral primary operators
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