Ultraviolet asymptotics of glueball propagators

TL;DR

This paper explores the constraints imposed by perturbation theory and the renormalization group on the structure of large-N glueball propagators in confining gauge theories, testing various theoretical models against these constraints.

Contribution

It demonstrates that the AdS string/large-N gauge theory models do not satisfy the RG-imposed constraints, while a Topological Field Theory does, highlighting differences in their ultraviolet behavior.

Findings

AdS models fail to meet RG constraints in the UV

Topological Field Theory satisfies asymptotic freedom constraints

Three-loop computations support the RG analysis

Abstract

We point out that perturbation theory in conjunction with the renormalization group (RG) puts a severe constraint on the structure of the large-N non-perturbative glueball propagators in SU(N) pure YM, in QCD and in n=1 SUSY QCD with massless quarks, or in any confining asymptotically-free gauge theory massless in perturbation theory. For the scalar and pseudoscalar glueball propagators in pure YM and QCD with massless quarks we check in detail the RG-improved estimate to the order of the leading and next-to-leading logarithms by means of a remarkable three-loop computation by Chetyrkin et al. We investigate as to whether the aforementioned constraint is satisfied by any of the scalar or pseudoscalar glueball propagators computed in the framework of the AdS String/ large-N Gauge Theory correspondence and of a recent proposal based on a Topological Field Theory underlying the large-N limit of YM. We find that none of the proposals for the scalar or the pseudoscalar glueball propagators based on the AdS String/ large-N Gauge Theory correspondence satisfies the constraint, actually as expected, since the gravity side of the correspondence is in fact strongly coupled in the ultraviolet. On the contrary, the Topological Field Theory satisfies the constraint that follows by the asymptotic freedom.