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| Main Authors: | , , |
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| Format: | Preprint |
| Published: |
2026
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| Subjects: | |
| Online Access: | https://arxiv.org/abs/2603.13721 |
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Table of Contents:
- We investigate the $1S$-, $1P$-, $2S$-, and $1D$-wave $Ω_c(css)$ spectroscopy through the non-leptonic decays of $Ω_b^-$ baryon within the constituent quark model. For the lowest-lying $1S$-wave $Ω_c$ state, we obtain the branching fractions ${\cal B}(Ω_b^- \to Ω_c^0 π^-,Ω_c^0 ρ^-)=(1.2,6.3) \times 10^{-3}$, which are consistent with existing model predictions. For $Ω_c(3000)$, $Ω_c(3050)$, $Ω_c(3065)$, and $Ω_c(3090)$, observed in the proton-proton and $e^+ e^-$ collisions and interpreted as members of the $1P$-wave multiplet (collectively denoted as $Ω_c^{**}$), we predict the branching fractions of $Ω_b^-\toΩ_c^{**}π^-,Ω_c^{**}ρ^-$ at the level of $10^{-3}$. Assigning the newly observed $Ω_c(3327)$ baryon to a $1D$-wave excitation with $J^P=5/2^+$ or $7/2^+$, we obtain ${\cal B}[Ω_b^-\to Ω_c(3327)^0π^-,Ω_c(3327)^0ρ^-] =(2.0,5.7)\times 10^{-3}$ or $(4.6,0.8)\times 10^{-3}$, respectively. The pronounced differences between these two scenarios provide a clear discriminant that can be tested in future measurements at LHCb.