The three-quark potential and perfect Abelian dominance in SU(3) lattice QCD

TL;DR

This study demonstrates that the three-quark potential in SU(3) lattice QCD is well described by a Y-shaped linear potential and reveals perfect Abelian dominance in quark confinement, supporting the dual superconductor model.

Contribution

It provides high-statistics evidence that the 3Q potential follows the Y-ansatz and shows perfect Abelian dominance in quark confinement within SU(3) lattice QCD.

Findings

3Q potential fits Y-ansatz across distances

Quark confinement in Qar{Q} and 3Q systems exhibits perfect Abelian dominance

Abelian variables suffice to describe quark confinement phenomena

Abstract

We study the static three-quark (3Q) potential for more than 300 different patterns of 3Q systems with high statistics, i.e., 1000-2000 gauge configurations, in SU(3) lattice QCD at the quenched level. For all the distances, the 3Q potential is found to be well described by the Y-ansatz, i.e., one-gluon-exchange (OGE) Coulomb plus Y-type linear potential. Also, we investigate Abelian projection of quark confinement in the context of the dual superconductor picture proposed by Yoichiro~Nambu~{\it et al.} in SU(3) lattice QCD. Remarkably, quark confinement forces in both Q$\bar{\rm Q}$ and 3Q systems can be described only with Abelian variables in the maximally Abelian gauge, i.e., $\sigma_{\rm Q \bar Q} \simeq \sigma_{\rm Q \bar Q}^{\rm Abel} \simeq \sigma_{\rm 3Q} \simeq \sigma_{\rm 3Q}^{\rm Abel}$, which we call ``perfect Abelian dominance'' of quark confinement.