\begin{document}$J/\psi$\end{document} and \begin{document}$\Upsilon (1S)$\end{document} via pentaquark \begin{document}$P_c$\end{document} and \begin{document}$P_b$\end{document} resonance channels in \begin{document}$e p \to e J/\psi p$\end{document} and \begin{document}$e p \to e \Upsilon(1S) p$\end{document} scattering processes at the proposed electron-ion colliders (EICs). The results obtained in this study are compared to those of non-resonance t-channels, which are described in the pomeron exchange model developed in our studies. Some pseudo-rapidity and rapidity distributions of \begin{document}$J/\psi$\end{document} and \begin{document}$\Upsilon(1S)$\end{document} are presented for the proposed EICs, including EicC and EIC-US. It is found that EicC is a good platform to identify \begin{document}$P_b$\end{document} states in the future."> Production of hidden-charm and hidden-bottom pentaquark states in electron-proton collisions -
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