Double scaling limits in gauge theories and matrix models

Mar, 2006
38 pages
Published in:
  • JHEP 06 (2006) 045
e-Print:
Report number:
  • SWAT-06-459

Citations per year

20062011201620212025024681012
Abstract:
We show that N=1\N=1 gauge theories with an adjoint chiral multiplet admit a wide class of large-N double-scaling limits where NN 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. FF-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<1c<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 FF-terms in these cases satisfy the string equation of the KdV hierarchy.
  • large N limit
  • double-scaling limits
  • non-critical strings
  • matrix model
  • gauge field theory: Yang-Mills
  • scaling
  • supersymmetry
  • superpotential
  • expansion 1/N
  • bibliography