The ABC model for the Ω−np system with lattice HAL QCD and Yukawa potentials produces low-energy characteristics differing from prior AAC calculations, with the Coulomb force exerting only marginal perturbative effects and binding driven by short-range ΩN behavior.
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Folding the central HAL QCD Ω-N potential with alpha density produces a Woods-Saxon Ω-α potential whose cluster-model binding energy matches prior results.
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Examination of the lattice QCD-motivated strong attractive $\Omega N$ potentials in the $\Omega^- n p$ system
The ABC model for the Ω−np system with lattice HAL QCD and Yukawa potentials produces low-energy characteristics differing from prior AAC calculations, with the Coulomb force exerting only marginal perturbative effects and binding driven by short-range ΩN behavior.
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Folding procedure for $\Omega$-$\alpha$ potential
Folding the central HAL QCD Ω-N potential with alpha density produces a Woods-Saxon Ω-α potential whose cluster-model binding energy matches prior results.