Abstract

The masses of ground and excited states of ${\mathrm{\ensuremath{\Omega}}}_{c}^{0}$, ${\mathrm{\ensuremath{\Omega}}}_{cc}^{+}$, and ${\mathrm{\ensuremath{\Omega}}}_{ccc}^{*++}$ baryons are calculated within the framework of Regge phenomenology. Here our attempt is to assign a possible spin parity to these obtained masses. Our calculated masses in the $(J,{M}^{2})$ plane with both natural (${J}^{P}=1/{2}^{+},3/{2}^{\ensuremath{-}},5/{2}^{+},\dots{}$) and unnatural (${J}^{P}=3/{2}^{+},5/{2}^{\ensuremath{-}},7/{2}^{+},\dots{}$) spin parities are in agreement with the experimental observations where available and reasonably close to other theoretical predictions. Further, we fix the slope and intercept of each Regge line in the $(n,{M}^{2})$ plane and estimate the masses of higher excited states of these baryons. The obtained mass relations and the mass value predictions could provide useful information in future experimental searches and the spin-parity assignment of these states.

Highlights

  • In 2017, the LHCb Collaboration observed five new narrow excited Ω0c states—Ωcð3000Þ0, Ωcð3050Þ0, Ωcð3066Þ0, Ωcð3090Þ0, and Ωcð3119Þ0—decaying into ΞþK− [1]

  • The masses of ground and excited states of Ω0c, Ωþcc, and ΩÃccþcþ baryons are calculated within the framework of Regge phenomenology

  • Our calculated masses in the ðJ; M2Þ plane with both natural (JP 1⁄4 1=2þ; 3=2−; 5=2þ; ...) and unnatural (JP 1⁄4 3=2þ; 5=2−; 7=2þ; ...) spin parities are in agreement with the experimental observations where available and reasonably close to other theoretical predictions

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Summary

INTRODUCTION

In 2017, the LHCb Collaboration observed five new narrow excited Ω0c states—Ωcð3000Þ0, Ωcð3050Þ0, Ωcð3066Þ0, Ωcð3090Þ0, and Ωcð3119Þ0—decaying into ΞþK− [1]. [22] a mass analysis was carried out for the newly excited Ωc=b baryons by proposing a new scheme of state classification called Jls mixing coupling, which goes beyond jj coupling This scheme successfully predict the spin parity of these states. We obtain relations between the intercept, slope ratios, and baryon masses in both the (J; M2) and (n; M2) planes Using these relations, we determine the mass spectra of the Ω0c baryons and try to assign a possible spin parity to these five recently observed baryonic states. We apply the same scheme for doubly and triply charmed omega baryons These baryons are yet to be observed by experiments and are not listed by the Particle Data Group (PDG) [17], which motivated us to study the mass spectra of Ω0c, Ωþcc, and ΩÃccþcþ baryons.

THEORETICAL FRAMEWORK
Masses of Ω0c baryons
ΞÃc ð28Þ
ΞÃcþ þ
Ωc ð1SÞ
AND DISCUSSION
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