Adiabatic continuity in a partially reduced twisted Eguchi-Kawai model with one adjoint Dirac fermion

TL;DR

This study numerically investigates the persistence of the confined phase in a large-N SU(N) gauge theory with an adjoint Dirac fermion under spatial compactification, supporting an adiabatic continuity scenario.

Contribution

It provides numerical evidence that the confined phase remains stable under circle reduction in a partially reduced twisted Eguchi-Kawai model with specific boundary conditions.

Findings

Polyakov loop remains near zero with periodic boundary conditions as circle size decreases.

Volume-independence order parameters are consistent with zero, supporting reduced-model validity.

Deconfinement transition observed with antiperiodic boundary conditions.

Abstract

We numerically investigate whether the center-symmetric confined phase of large-$N$ $SU(N)$ gauge theory with one adjoint Dirac fermion persists under spatial compactification on $\mathbb{R}^3 \times S^1$. To this end, we employ a partially reduced twisted Eguchi-Kawai (TEK) model on a $1^3 \times L_4$ lattice with an adjoint Wilson fermion, and measure both the Polyakov loop around $S^1$ and order parameters for volume independence in the reduced directions. For $N=36$, $L_4=2$, $b=0.30\text{-}0.46$, and $\kappa=0.03\text{-}0.16$, we find that, with periodic boundary conditions, the Polyakov loop remains near zero in the light-fermion regime as the circle size is reduced. For the modified twist, the volume-independence order parameters are also consistent with zero in the explored region, supporting the validity of the partially reduced description. These results provide numerical evidence, within the reduced-model setup and parameter range studied, for an adiabatic-continuity scenario in which the confined phase is smoothly connected between large and small circles. By contrast, with antiperiodic boundary conditions, the Polyakov loop exhibits a clear deconfinement transition. We also discuss how this scenario is compatible with the anomaly constraints of the underlying four-dimensional theory. The symmetric twist is examined as a useful comparison, although its volume-independence properties appear less robust at the present value of $N$.