\begin{document}$ (J,M^{2}) $\end{document} plane. We also preliminarily assign quantum numbers to the recently observed baryons, including \begin{document}$ \Xi_{c}(3055) $\end{document}, \begin{document}$ \Xi_{c}(3080) $\end{document}, \begin{document}$ \Xi_{c}(2930) $\end{document}, \begin{document}$ \Xi_{c}(2923) $\end{document}, \begin{document}$ \Xi_{c}(2939) $\end{document}, \begin{document}$ \Xi_{c}(2965) $\end{document}, \begin{document}$ \Xi_{c}(2970) $\end{document}, \begin{document}$ \Xi_{c}(3123) $\end{document}, \begin{document}$ \Xi_{b}(6100) $\end{document}, \begin{document}$ \Xi_{b}(6227) $\end{document}, \begin{document}$ \Xi_{b}(6327) $\end{document}, and \begin{document}$ \Xi_{b}(6333) $\end{document}. Finally, the spectral structure of strange single heavy baryons is discussed. Accordingly, we predict several new baryons that may be observed in forthcoming experiments."> Systematic analysis of strange single heavy baryons <inline-formula><tex-math id="M1">\begin{document}${ \boldsymbol\Xi_{\boldsymbol c} }$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/a9a777bb-53a6-4426-9c52-ef936db4c6ff/CPC-2023-0098_M1.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/a9a777bb-53a6-4426-9c52-ef936db4c6ff/CPC-2023-0098_M1.png"/></alternatives></inline-formula> and <inline-formula><tex-math id="M2">\begin{document}${\boldsymbol\Xi_{\boldsymbol b} }$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/a9a777bb-53a6-4426-9c52-ef936db4c6ff/CPC-2023-0098_M2.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/a9a777bb-53a6-4426-9c52-ef936db4c6ff/CPC-2023-0098_M2.png"/></alternatives></inline-formula> -
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