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Understanding the nature of Ω(2012) in a coupled-channel approach

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arxiv 2212.02783 v2 pith:TCUG2IBE submitted 2022-12-06 hep-ph hep-exnucl-th

Understanding the nature of Ω(2012) in a coupled-channel approach

classification hep-ph hep-exnucl-th
keywords omegaresonancestateapproachbarechannelcoupled-channelmass
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We perform a systematic analysis of the mass and strong decays of the $\Omega(2012)$ resonance in a coupled-channel approach of a bare three-quark state and a composite meson-baryon state. Besides the coupling of the bare state and $\Xi^* \bar K$ channel, the effective meson-baryon interactions are also included. We find a pole with mass of $2008$ MeV by solving the Bethe-Salpeter equation. The calculated decay widths and its ratios of branching fractions $\mathcal {R}_{\Xi \bar K}^{\Xi \pi \bar K}$ agree well with the new experimental measurement by Belle Collaboration. Our results suggest that both three-quark core and $\Xi^* \bar K$ channel are essential for the description of the $\Omega(2012)$ resonance. We expect that present calculations can help us to better understand the nature of $\Omega(2012)$ resonance.

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Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Signatures of the $\Omega(2012)^{-}$ state in $\Xi^*\bar K$ Correlation Functions

    hep-ph 2026-03 accept novelty 6.5

    Ω(2012) is dynamically generated as a Ξ*K–Ωη molecule; its pole produces pronounced near-threshold structures in the Ξ*0K− correlation function that can be measured at the LHC.