\begin{document}$\Omega\Omega$\end{document} dibaryon states with \begin{document}$J^P=0^+$\end{document} and \begin{document}$2^+$\end{document} in a molecular picture. We construct a tensor \begin{document}$\Omega$\end{document}\begin{document}$\Omega$\end{document} molecular interpolating current and calculate the two-point correlation function within the method of QCD sum rules. Our calculations indicate that the masses of the scalar and tensor dibaryon states are \begin{document}$m_{\Omega\Omega, \, 0^+} = $\end{document} \begin{document}$ (3.33\pm 0.51) \,{\rm{GeV}}$\end{document} and \begin{document}$m_{\Omega\Omega,\, 2^+}=(3.15\pm0.33)\, {\rm{GeV}}$\end{document}, respectively, which are below the \begin{document}$2m_\Omega$\end{document} threshold. Within error, these results do not negate the existence of loosely bound molecular \begin{document}$\Omega\Omega$\end{document} dibaryon states. These exotic strangeness \begin{document}$S=-6$\end{document} and doubly-charged \begin{document}$\Omega\Omega$\end{document} dibaryons, if they exist, may be identified in heavy-ion collision processes in the future."> Exotic ΩΩ dibaryon states in a molecular picture -
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