Examination of the lattice QCD-motivated strong attractive potentials in the system
arXiv:2504.04655 · doi:10.1103/mjg8-mxtg
Abstract
Within the framework of the Faddeev equations in configuration space, we examine the system, employing strongly attractive lattice HAL QCD and Yukawa-type meson exchange potentials for the interaction. Our formalism incorporates the attractive Coulomb force between the and proton, treating the system as three non-identical particle pairs (the model). In this study, we assess the impact of the Coulomb interaction on the system and compare our results with recent ( model) calculations obtained using various approaches. The model yields low-energy characteristics for the \(ΩNN\) system that differ from previous calculations. The Coulomb potential has a marginal perturbative effect on the system, shifting the three-body binding energy by the Coulomb energy of the two-body subsystem, but only slightly deviating the spatial configuration from isosceles triangle symmetry. These effects are primarily driven by the strong \(ΩN\) interaction. We demonstrate that the large binding energy of the system arises from the short-range behavior of the potentials.
arXiv comment13 pages, 4 figures
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