Reanalysis of the most strange dibaryon within constituent quark models

Abstract

The most strange dibaryon $\Omega \Omega$ with quantum numbers $S=-6$, $I=0$, and $J^P=0^{+},1^{-},2^{+},3^{-}$ is reanalyzed in the framework of quark delocalization color screening model (QDCSM) and chiral quark model (ChQM). The $\Omega \Omega$ dibaryon with $J^P=0^{+}$ is bound, and the one with other quantum numbers $J^P=1^{-},2^{+},3^{-}$ are all unbound in our calculation. The low-energy scattering phase shifts, the scattering length, and the effective range of the $\Omega \Omega$ dibaryon with $J^P=0^{+}$ also support the existence of such strange dibaryon. This dibaryon is showed to be a shallow bound state in QDCSM, while the binding energy becomes much larger in the ChQM by including the effect of the hidden-color channel coupling. And the scalar nonet meson-exchange in the ChQM also provides more attraction for the $\Omega \Omega$ system. Experimental search for such most strange dibaryon will provide much information for understanding the hadron-hadron interactions in different quark models.

Comments: 8 pages, 3 figures. arXiv admin note: text overlap with arXiv:1507.07124