Research PaperNo Access

Spectroscopy of $Ω_{c c c}$ $Ω_{c c c}$ and $Ω_{b b b}$ $Ω_{b b b}$ baryons

Amee Kakadiya

Department of Physics, Sardar Vallabhbhai National Institute of Technology, Ichchhanath, Surat 395007, Gujarat, India

E-mail Address: ameekakadiya@gmail.com

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Zalak Shah

Department of Physics, Sardar Vallabhbhai National Institute of Technology, Ichchhanath, Surat 395007, Gujarat, India

E-mail Address: zalak.physics@gmail.com

Corresponding author.

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, and

Ajay Kumar Rai

Department of Physics, Sardar Vallabhbhai National Institute of Technology, Ichchhanath, Surat 395007, Gujarat, India

E-mail Address: raiajayk@gmail.com

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https://doi.org/10.1142/S0217751X22502256Cited by:15 (Source: Crossref)

Abstract

In this paper, we study the properties of triply charm and triply bottom baryon. The mass spectra of these baryons are calculated in nonrelativistic constituent quark model with Coulomb plus screened potential. Several states $S$ $S$ , $P$ $P$ , $D$ $D$ and $F$ $F$ of the $Ω_{c c c}$ $Ω_{c c c}$ and $Ω_{b b b}$ $Ω_{b b b}$ baryons with quantum number $J^{P} = {\frac{1}{2}}^{\pm}$ $J^{P} = {\frac{1}{2}}^{\pm}$ , ${\frac{3}{2}}^{\pm}$ ${\frac{3}{2}}^{\pm}$ , ${\frac{5}{2}}^{\pm}$ ${\frac{5}{2}}^{\pm}$ , ${\frac{7}{2}}^{\pm}$ ${\frac{7}{2}}^{\pm}$ are determined. Regge trajectories are also plotted to determine the quantum number of baryons. Moreover, the magnetic moments are calculated for $J^{P} = {\frac{3}{2}}^{+}$ $J^{P} = {\frac{3}{2}}^{+}$ .

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