Lattice QCD study of the heavy-heavy-light quark potential

Abstract

We study the heavy-heavy-light quark ($QQq$) potential in SU(3) quenched lattice QCD, and discuss one of the roles of the finite-mass valence quark in the interquark potential. Monte Carlo simulations are performed with the standard gauge action on the ${16}^{4}$ lattice at $\ensuremath{\beta}=6.0$ and the $O(a)$-improved Wilson fermion action at four hopping parameters. For statistical improvement, the gauge configuration is fixed with the Coulomb gauge. We calculate the potential energy of $QQq$ systems as a function of the inter-heavy-quark distance $R$ in the range of $R\ensuremath{\le}0.8\text{ }\text{ }\mathrm{fm}$. The $QQq$ potential is well described with a Coulomb plus linear potential, and the effective string tension between the two heavy quarks is significantly smaller than the string tension $\ensuremath{\sigma}\ensuremath{\simeq}0.89\text{ }\text{ }\mathrm{GeV}/\mathrm{fm}$. It would generally hold that the effect of the finite-mass valence quark reduces the inter-two-quark confinement force in baryons.