Abstract
In this work, we study the mass spectrum of the $\Omega_{ccc}$ and $\Omega_{bbb}$ baryons up to the $N=2$ shell within a nonrelativistic constituent quark model (NRCQM). The model parameters are adopted from the determinations by fitting the charmonium and bottomonium spectra in our previous works. The masses of the $\Omega_{ccc}$ and $\Omega_{bbb}$ baryon states predicted in present work reasonably agree with the results obtained with the Lattice QCD calculations. Furthermore, to provide more knowledge of the $\Omega_{ccc}$ and $\Omega_{bbb}$ states, we evaluate their radiative decays with the available masses and wave functions from the potential model.
Highlights
In the discovery of heavy baryons, the Large Hadron Collider (LHC) facility has shown its powerful abilities in recent years
Stimulated by the large discovery potentials of the heavy baryons at the LHC facility, in this work we carry out a systematic study of the triply heavy baryon spectra of Ωccc and Ωbbb within a nonrelativistic potential model
To provide more knowledge of the Ωccc and Ωbbb states, we evaluate their radiative decays with the available wave functions from our potential model calculations
Summary
In the discovery of heavy baryons, the Large Hadron Collider (LHC) facility has shown its powerful abilities in recent years. Stimulated by the large discovery potentials of the heavy baryons at the LHC facility, in this work we carry out a systematic study of the triply heavy baryon spectra of Ωccc and Ωbbb within a nonrelativistic potential model. With this model we have studied the spectra of the charmonium, bottomonium, Bc meson, Ω baryon, and fully heavy tetraquark states.
Sign-in/Register to view highlights & summary Sign-in/Register to access full text options 
Free) 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a call
