\begin{document}$ C\gamma_\alpha\otimes\stackrel{\leftrightarrow}{\partial}_\mu\otimes\gamma^\alpha C $\end{document} (or \begin{document}$ C\gamma_\alpha\otimes\stackrel{\leftrightarrow}D_\mu\otimes\gamma^\alpha C $\end{document}) type current with fully-strange quarks couples potentially to a tetraquark state with a mass \begin{document}$ 2.16 \pm 0.14 \,{\rm{GeV}} $\end{document}, which supports assigning \begin{document}$ Y(2175)/\phi(2170) $\end{document} as the diquark-antidiquark type tetraquark state with \begin{document}$J^{PC}=1^{--}$\end{document}. The \begin{document}$ qs\bar{q}\bar{s} $\end{document} and \begin{document}$ ss\bar{s}\bar{s} $\end{document} vector tetraquark states with the structure \begin{document}$ C\gamma_\mu\otimes \stackrel{\leftrightarrow}{\partial}_\alpha \otimes\gamma^\alpha C + C\gamma^\alpha \otimes\stackrel{\leftrightarrow}{\partial}_\alpha \otimes\gamma_\mu $\end{document} (or \begin{document}$ C\gamma_\mu\otimes \stackrel{\leftrightarrow}D_\alpha \otimes\gamma^\alpha C + C\gamma^\alpha \otimes\stackrel{\leftrightarrow}D_\alpha \otimes\gamma_\mu $\end{document}) are consistent with \begin{document}$ X(2200) $\end{document} and \begin{document}$ X(2400) $\end{document}, respectively, which lie in the region from \begin{document}$ 2.20 $\end{document} to \begin{document}$ 2.40\,{\rm{GeV}} $\end{document}. The central values of the masses of the fully-strange vector tetraquark states with an explicit P-wave are approximately \begin{document}$ 2.16-3.13\,{\rm{GeV}} $\end{document} (or \begin{document}$ 2.16-3.16\,{\rm{GeV}} $\end{document}). Predictions for other fully-light vector tetraquark states with and without hidden-strange are also presented."> Fully-light vector tetraquark states with explicit <i>P</i>-wave via QCD sum rules -
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