\begin{document}$ 3D $\end{document} multiplet within a nonrelativistic linear potential quark model. Furthermore, using the obtained wave functions, we also evaluate the strong decays of the strangeonium states with the \begin{document}$ ^3P_0 $\end{document} model. Based on our successful explanations of the well established states \begin{document}$ \phi(1020) $\end{document}, \begin{document}$ \phi(1680) $\end{document}, \begin{document}$ h_1(1415) $\end{document}, \begin{document}$ f'_2(1525) $\end{document}, and \begin{document}$ \phi_3(1850) $\end{document}, we further discuss the possible assignments of strangeonium-like states from experiments by combining our theoretical results with observations. It is found that some resonances, such as \begin{document}$ f_2(2010) $\end{document} and \begin{document}$ f_2(2150) $\end{document}, listed by the Particle Data Group, and \begin{document}$ X(2062) $\end{document} and \begin{document}$ X(2500) $\end{document}, newly observed by BESIII, may be interpreted as strangeonium states. The possibility of \begin{document}$ \phi(2170) $\end{document} as a candidate for \begin{document}$ \phi(3S) $\end{document} or \begin{document}$ \phi(2D) $\end{document} cannot be excluded. We expect our results to provide useful references for looking for the missing \begin{document}$ s\bar{s} $\end{document} states in future experiments."> Mass spectrum and strong decays of strangeonium in a constituent quark model -
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