Abstract

We explore the interactions of two strangeness -3 baryons in multiple spin channels with lattice QCD. This system provides an ideal laboratory for exploring the interactions of multi-baryon systems with minimal dependence on light quark masses. Model calculations of the two-Ω−Ω^- system in two previous works have obtained conflicting results, which can be resolved by lattice QCD. The lattice calculations are performed using two different volumes with L∼2.5L\sim2.5 and 3.9 fm on anisotropic clover lattices at mπ∼390m_π\sim 390 MeV with a lattice spacing of as∼0.123a_s \sim 0.123 fm in the spatial direction and at∼as/3.5a_t\sim{a}_s/3.5 in the temporal direction. Using multiple interpolating operators from a non-displaced source, we present scattering information for two ground state Ω−Ω^- baryons in both the S=0 and S=2 channels. For S=0, kcot⁡δk\cotδ is extracted at two volumes, which lead to an extrapolated scattering length of aS=0ΩΩ=0.16±0.22 fma^{ΩΩ}_{S=0}=0.16 \pm 0.22 \ \text{fm}, indicating a weakly repulsive interaction. Additionally, for S=2, two separate highly repulsive states are observed. We also present results on the interactions of the excited strangeness -3, spin-1/2 states with the ground spin-3/2 states for the spin-1 and spin-2 channels. Results for these interactions are consistent with attractive behavior.

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