Abstract

Confinement remains one the most interesting and challenging nonperturbative phenomenon in non-Abelian gauge theories. Recent semiclassical [for $SU(2)$] and lattice (for QCD) studies have suggested that confinement arises from interactions of statistical ensembles of instanton dyons with the Polyakov loop. We extend studies of a semiclassical ensemble of dyons to the $SU(3)$ Yang-Mills theory. We find that such interactions do generate the expected first-order deconfinement phase transition. The properties of the ensemble, including correlations and topological susceptibility, are studied over a range of temperatures above and below ${T}_{c}$. Additionally, the dyon ensemble is studied in the Yang-Mills theory containing an extra trace-deformation term. It is shown that such a term can cause the theory to remain confined and even retain the same topological observables at high temperatures.

Highlights

  • Quantum chromodynamics (QCD) is the quantum field theory describing the fundamental particles and forces that make up nuclear physics

  • While QCD is remarkably successful in describing nuclear physics, many phenomena remain beyond the scope of what can be studied analytically

  • In this work we study pure gauge theory rather than QCD-like theories with light quarks, let us mention that the instanton-dyon ensemble describes the breaking of chiral symmetry

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Summary

Introduction

Quantum chromodynamics (QCD) is the quantum field theory describing the fundamental particles and forces that make up nuclear physics. While QCD is remarkably successful in describing nuclear physics, many phenomena remain beyond the scope of what can be studied analytically. Nonperturbative phenomena such as confinement—the disappearance of quarks and gluons from the physical spectrum—is not completely understood. At T < Tc the chromoelectrically charged quarks and gluons are connected by QCD flux tubes, dual to magnetic flux tubes in superconductor. The profile of the QCD flux tubes [4] was found to agree well with the dual superconductor model.

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