Abstract

Class-S theories are four-dimensional N=2 supersymmetric field theories constructed by the reduction of a (2,0) six-dimensional theory on a punctured Riemann surface C (called the UV curve). A basic degeneration limit of the surface C is when several punctures are brought close to each other. As this happens, a long tube appears in C and a weakly coupled gauge group emerges. When the corresponding gauge coupling is turned off, we are left with two surfaces. This decoupling leads to a unique result. We explain how to fix the gauge group that becomes weakly coupled and the resulting two theories, in terms of the types of punctures on the surface C. Each of the resulting theories is given in terms of a class-S theory (plus possibly additional free hypermultiplets). Many other more complicated degeneration limits can be described by repeatedly using this specification. For questions about weak coupling limits in such theories, it is useful to consider the set of punctures that can appear at the end of a tube. These are the punctures that are created in the resulting surfaces when the gauge coupling is taken to be extremely weak. Not any puncture can be formed in a decoupling process, and this set is described. Each such puncture can be found diagrammatically in terms of the other punctures on C in a particular decoupling limit. The relation of the gauge group to the symmetry associated with this puncture is discussed. We discuss the relation of such degeneration limits of large N theories, through the AdS/CFT correspondence, to decoupled field theories on AdS_5.

Highlights

  • Consider the Coulomb branch of N 1⁄4 2 superconformal field theories in four dimensions

  • In the low energy effective action, the gauge coupling constants matrix is promoted to τijðaÞ

  • Linear quivers of SUðkiÞ gauge groups with N 1⁄4 2 supersymmetry were constructed through the decoupling limit of configurations of NS5 and D4 branes in type-IIA

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Summary

INTRODUCTION

Consider the Coulomb branch of N 1⁄4 2 superconformal field theories in four dimensions. Linear quivers of SUðkiÞ gauge groups with N 1⁄4 2 supersymmetry were constructed through the decoupling limit of configurations of NS5 and D4 branes in type-IIA superstring These configurations have singularities, but when interpreted in M theory, could be described by a single M5 brane. As is manifest in the brane constructions mentioned above, the structure of the SW curve as a branched covering of C identifies the four-dimensional theory. The pole structure of regular (untwisted) punctures in a superconformal class-S AN−1 theory is restricted. In other words, gauging a diagonal subgroup of the symmetry associated with a regular puncture and of a global symmetry from an additional theory, what are the possibilities for that additional theory that will result in a SCFT? V and the conclusions of the other sections can be applied in this context

WEAK COUPLING LIMITS OF A CLASS-S THEORY
Maximal gauge group along a tube
Decoupling on a sphere using the curve
Þ þ n ðPjÞ
Relation to previous works
Punctures appearing at the end of a tube
Classification of PRPs
Diagrammatic construction of the decoupling
Irregular punctures
A GIVEN THEORY
Gauging a puncture
The possible gauge groups GT
The embedding of GT in a PRP
A bound on the rank of the symmetry of a PRP
LARGE N AND FIELD THEORIES ON AdS5
Large N
Decoupled field theories in the large N limit
Nonsingular weakly curved gravitational duals
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