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On Ω3cNN and Ω3c Ω3c N systems with HAL QCD potentials

2025/09/02 by Igor Filikhin, Roman Ya. Kezerashvili, Filikhin, Igor +3
Physics and Astronomy · #Cold Atom Physics and Bose-Einstein Condensates #FOS: Physical sciences #High Energy Physics - Lattice (hep-lat) #Nuclear Theory (nucl-th) #Nuclear physics research studies #Quantum Chromodynamics and Particle Interactions

paper · pdf · doi:10.48550/arxiv.2509.01902

openalex publication_date 2025/09/02 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

This study employs the Faddeev formalism in configuration space to investigate the Ω3cNN cluster containing a triply charmed Omega baryon (Ω3c). Using the recently reported HAL QCD S-wave Ω3cN potentials in the 3S1 and 5S2 channels, together with the MT-I--III nucleon--nucleon potential and neglecting the Coulomb force, we find no bound state for the Ω3cnp system. We predict near-threshold resonances in the Jπ=5/2+ (maximal total spin) and Jπ=1/2+ (minimal total spin) states, with resonance energies of 1.1~MeV below and 0.0~MeV at the three-body breakup threshold, respectively, at Euclidean time t/a = 16. A similar analysis of the Ω3cΩ3cN system likewise reveals no bound states, though a possible resonance is indicated. The short-distance behavior of the HAL QCD Ω3cN potential is also discussed.

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