Most Strange Dibaryon from Lattice QCD

The $\mathrm{\Omega }\mathrm{\Omega }$ system in the ${}^1{S}_0$ channel (the most strange dibaryon) is studied on the basis of the ($2+1$)-flavor lattice QCD simulations with a large volume $(8.1\mathrm{fm}{)}^3$ and nearly physical pion mass $m_{\pi }\simeq 146\mathrm{MeV}$ at a lattice spacing of $a\simeq 0.0846\mathrm{fm}$. We show that lattice QCD data analysis by the HAL QCD method leads to the scattering length $a_0=4.6(6){(}_{-0.5}^{+1.2})\mathrm{fm}$, the effective range $r_{\mathrm{eff}}=1.27(3){(}_{-0.03}^{+0.06})\mathrm{fm}$, and the binding energy $B_{\mathrm{\Omega }\mathrm{\Omega }}=1.6(6){(}_{-0.6}^{+0.7})\mathrm{MeV}$. These results indicate that the $\mathrm{\Omega }\mathrm{\Omega }$ system has an overall attraction and is located near the unitary regime. Such a system can be best searched experimentally by the pair-momentum correlation in relativistic heavy-ion collisions.