Using the vector exchange interaction in the local hidden gauge approach, which in the light quark sector generates the chiral Lagrangians and has produced realistic results for \begin{document}$\Omega_c, \Xi_c, \Xi_b$\end{document}… Click to show full abstract
Using the vector exchange interaction in the local hidden gauge approach, which in the light quark sector generates the chiral Lagrangians and has produced realistic results for \begin{document}$\Omega_c, \Xi_c, \Xi_b$\end{document} and the hidden charm pentaquark states, we study the meson-baryon interactions in the coupled channels that lead to the \begin{document}$\Xi_{bb}$\end{document} and \begin{document}$\Omega_{bbb}$\end{document} excited states of the molecular type. We obtain seven states of the \begin{document}$\Xi_{bb}$\end{document} type with energies between \begin{document}$10408$\end{document} and \begin{document}$10869$\end{document} MeV, and one \begin{document}$\Omega_{bbb}$\end{document} state at \begin{document}$15212$\end{document} MeV.
               
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