Abstract

We study the color correlation between static quark and antiquark ($q\bar q$) in the confined phase via reduced density matrices $\rho$ defined in color space. We adopt the standard Wilson gauge action and perform quenched calculations with the Coulomb gauge condition for reduced density matrices. The spatial volumes are $L^3 = 8^3$, $16^3$, $32^3$ and $48^3$, with the gauge couplings $\beta = 5.7$, 5.8 and 6.0. Each element of the reduced density matrix in the sub space of quarks' color degrees of freedom of the $q\bar q$ pair is calculated from staples defined by link variables. As a result, we find that $\rho$ is well written by a linear combination of the strongly correlated $q\bar q$ pair state with the color-singlet component and the uncorrelated $q\bar q$ pair state with random color configurations. We compute the Renyi entropies $S^{\rm Renyi}$ from $\rho$ to investigate the $q\bar q$ distance dependence of the color correlation of the $q\bar q$ pair and find that the color correlation is quenched as the distance increases.

Highlights

  • Color confinement is one of the nonperturbative features of QCD, the fundamental theory of the strong interaction

  • We study the color correlation between the static quark and antiquark in the confined phase via reduced density matrices ρ defined in color space

  • The color charge first associated with a color-singlet qqpair flows into the interquark flux tube as the qqseparation is enlarged, keeping the total system color singlet [4,5]

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Summary

INTRODUCTION

Color confinement is one of the nonperturbative features of QCD, the fundamental theory of the strong interaction. The static interquark potential (qqpotential) in the confinement phase exhibits a linearly rising potential in the largeseparation limit giving the diverging energy, and quarks cannot be isolated. If the color charge of the qqpart and that of the gluon part are separately considered, this color transfer can be regarded as a color charge leak from the qqpart to the gluon part in association with the screening effect This color leak should depend on the qqdistance and would be observed as the distance dependence of the color correlation between the quark and antiquark. Such color correlation of the qqpair may be detected by entanglement entropy (EE) defined by the reduced density matrix.

Reduced two-body density matrix and qqcorrelation
Lattice QCD formalism
Ground-state dominance
Lattice QCD parameters
Finite volume effects
Entanglement entropy
CONCLUSIONS
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