Double Scaling Limits in Gauge Theories and Matrix Models

TL;DR

This paper explores large-N double-scaling limits in $ ext{N}=1$ gauge theories with an adjoint chiral multiplet, revealing a decoupled sector with light states and connections to matrix models and two-dimensional gravity.

Contribution

It introduces a new class of double-scaling limits in gauge theories near Argyres-Douglas singularities, linking them to matrix models and 2D gravity descriptions.

Findings

Identification of a decoupled sector with fixed-mass light states at large N.

Connection of the double-scaling limit to the old matrix model and 2D gravity.

Validation of gravitational F-terms satisfying the string equation of the KdV hierarchy.

Abstract

We show that $\N=1$ gauge theories with an adjoint chiral multiplet admit a wide class of large-N double-scaling limits where $N$ is taken to infinity in a way coordinated with a tuning of the bare superpotential. The tuning is such that the theory is near an Argyres-Douglas-type singularity where a set of non-local dibaryons becomes massless in conjunction with a set of confining strings becoming tensionless. The doubly-scaled theory consists of two decoupled sectors, one whose spectrum and interactions follow the usual large-N scaling whilst the other has light states of fixed mass in the large-N limit which subvert the usual large-N scaling and lead to an interacting theory in the limit. $F$-term properties of this interacting sector can be calculated using a Dijkgraaf-Vafa matrix model and in this context the double-scaling limit is precisely the kind investigated in the "old matrix model'' to describe two-dimensional gravity coupled to $c<1$ conformal field theories. In particular, the old matrix model double-scaling limit describes a sector of a gauge theory with a mass gap and light meson-like composite states, the approximate Goldstone boson of superconformal invariance, with a mass which is fixed in the double-scaling limit. Consequently, the gravitational $F$-terms in these cases satisfy the string equation of the KdV hierarchy.