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The progresses in the experimental sector have been the harbinger of theobservations of many new hadrons. Very recently, LHCb Collaboration announcedthe observation of two new $\Sigma_b(6097)^{\pm}$ states in the$\Lambda^0_b\pi^{\pm}$ invariant mass distribution, which are considered as theexcited states of the ground state $\Sigma^{(*)}_b$ baryon. Though, almost allof the ground state baryons have been observed, having a limited number ofexcited states observed so far makes them intriguing. Understanding theproperties of the excited baryons improve our knowledge on the stronginteraction as well as the nature and internal structures of these baryons. Tospecify the quantum numbers of the $\Sigma_b(6097)^{\pm}$ an analysis on theirstrong decays to $\Lambda_b^0$ and $\pi^{\pm}$ is performed within the lightcone QCD sum rule formalism. To this end, they are considered as possible $1P$or $2S$ excitation of either the ground state $\Sigma_b$ baryon with$J=\frac{1}{2}$ or $\Sigma_b^{*}$ baryon with $J=\frac{3}{2}$. Thecorresponding masses are also calculated considering the same scenarios fortheir quantum numbers. The results of the analyses indicate that the$\Sigma_b(6097)^{\pm}$ baryons are excited $1P$ baryons having quantum numbers$J^P=\frac{3}{2}^-$.

Determination of the quantum numbers of $\Sigma_b(6097)^{\pm}$ via their strong decays