Abstract

We study the holographic Dynamic AdS/QCD description of a SU($N_c$) non-abelian gauge theory with $N_f$ fermions in the fundamental representation which also have Nambu-Jona-Lasinio interactions included using Witten's multi-trace prescription. In particular here we study aspects of the dynamics in and near the conformal window of the gauge theory as described by the two loop running of the gauge theory. If the number of flavours is such that the IR fixed point lies with the anomalous dimension, $\gamma$, of the quark bilinear above one then chiral symmetry breaking occurs. Here we display a spiral in the mass - quark condensate plane describing a sequence of unstable excited states of the vacuum. An attractive NJL operator enhances the vacuum condensate but only an infinitely repulsive NJL interaction switches off the condensation completely. When $N_f$ changes so that the IR fixed point falls below one (the conformal window region) there is a numerical discontinuity in the phase structure with condensation only occurring with a super critical NJL interaction. In the conformal window, the running of $\gamma$ to a non-trivial IR fixed point is similar to walking dynamics, although chiral symmetry breaking is not triggered. In the "Ideal Walking" scenario, chiral symmetry is broken in that IR conformal regime by the NJL interaction, but the change in $\gamma$ enhances the UV condensate. That enhancement of the condensate is shown in an analytic model with a sharp change in $\gamma$ and we show equivalent numerical results for the case of the two loop running. In the model the $\sigma$ becomes massless as the gauge theory running becomes near conformal and we show it is possible to realize a light higgs-like state in Ideal Walking models.

Highlights

  • A holographic [1] description of the gauged Nambu–Jona-Lasino (NJL) model [2,3] was developed [4]

  • Our analysis of the gauge theory is based on the dynamic anti-de Sitter (AdS)/QCD model [5,6,7], which is motivated by top down holographic descriptions of chiral symmetry breaking [8,9]

  • If one takes the two-loop expressions for γ for Nc 1⁄4 3 and Nf 1⁄4 2 naively extended to the scale where γ 1⁄4 1, a very sensible description of QCD is obtained as we shown in Ref. [4]

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Summary

INTRODUCTION

A holographic [1] description of the gauged Nambu–Jona-Lasino (NJL) model [2,3] was developed [4]. Our analysis of the gauge theory is based on the dynamic anti-de Sitter (AdS)/QCD model [5,6,7], which is motivated by top down holographic descriptions of chiral symmetry breaking [8,9]. [15] to look at phenomenological models of electroweak symmetry breaking such as technicolor, extended technicolor, and top condensation This is the holographic description of the gauge theory we will again use here. There is interesting structure in the mass vs quark condensate plane—a spiral structure indicating the presence of excited states of the vacuum These structures have previously been observed in D3/D7 models of magnetic field induced chiral symmetry breaking [9], the alternative dual of the conformal window of Refs. We will work with κ 1⁄4 1 as a reference value—fπ grows as κ grows, but the phenomena we report on are qualitatively the same

NJL INTERACTIONS
CHIRALLY BROKEN PHASE
Simplified analysis
Two-loop runnings
Light σ
SUMMARY
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