Abstract

The SS-wave ΛΛΛΛ and NΞN Ξ interactions are studied on the basis of the (2+1)-flavor lattice QCD simulations close to the physical point (mπ≃146MeVm_π\simeq 146{\rm{MeV}} and mK≃525MeVm_K \simeq 525{\rm{MeV}}). Lattice QCD potentials in four different spin-isospin channels are extracted by using the coupled-channel HAL QCD method and are parametrized by analytic functions to calculate the scattering phase shifts. The ΛΛΛΛ interaction at low energies shows only a weak attraction, which does not provide a bound or resonant dihyperon. The NΞNΞ interaction in the spin-singlet and isospin-singlet channel is most attractive and lead the NΞNΞ system near unitarity. Relevance to the strangeness=−2-2 hypernuclei as well as to two-baryon correlations in proton-proton, proton-nucleus and nucleus-nucleus collisions is also discussed.

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