\begin{document}$\Lambda$\end{document} with strangeness S = −1 and isospin I = 0, \begin{document}$\Sigma$\end{document} with S = −1 and I = 1, and \begin{document}$\Xi$\end{document} baryon with S = −2 and \begin{document}$I=\dfrac{1}{2}$\end{document}. In this study, the hypercentral constituent quark model with linear confining potential has been employed along with a first order correction term to obtain the resonance masses up to approximately 4 GeV. The calculated states include 1S-5S, 1P-4P, 1D-3D, 1F-2F, and 1G (in a few cases) along with all possible spin-parity assignments. Regge trajectories have been explored for the linearity of the calculated masses for \begin{document}$(n,M^{2})$\end{document} and \begin{document}$(J,M^{2})$\end{document}. Magnetic moments have been intensively studied for ground state spin \begin{document}$\dfrac{1}{2}$\end{document} and \begin{document}$\dfrac{3}{2}$\end{document}, in addition to the configuration mixing of the first negative parity state for \begin{document}$\Xi$\end{document}. Lastly, the transition magnetic moments and radiative decay widths have been presented."> Spectroscopic investigation of light strange <i>S</i> = −1 Λ and Σ and <i>S</i> = −2 Ξ baryons -
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