Stability of hexaquarks in the string limit of confinement

The stability of systems containing six quarks or antiquarks is studied within a simple string model inspired by the strong-coupling regime of quantum chromodynamics and used previously for tetraquarks and pentaquarks. We discuss both six-quark $(q^6)$ and three-quark–three-antiquark $(q^3\bar{q}{}^3)$ states. The quarks are assumed to be distinguishable and thus not submitted to antisymmetrization. It is found that the ground state of $(q^6)$ is stable against dissociation into two isolated baryons. For the case of $ (q^3\bar q{}^3)$, our results indicate the existence of a bound state very close to the threshold. The investigations are extended to $(q^3{Q}^3)$ and $(Q^3{\bar{q}}^3)$ systems with two different constituent masses, and their stability is discussed as a function of the mass ratio.