\begin{document}$ E_e=20\; {\rm GeV} $\end{document} and \begin{document}$ E_p=250\; {\rm GeV} $\end{document}, respectively. We can constrain the effective coupling strength between the ALP and photons to be \begin{document}$ 0.2\; {\rm TeV}^{-1} $\end{document} at the \begin{document}$ 2\sigma $\end{document} confidence level with an integrated luminosity of \begin{document}$ 300\; {\rm fb}^{-1} $\end{document} for the mass range \begin{document}$ m_a\in [5,40]\; {\rm GeV} $\end{document}. Such bounds may be significantly improved if we consider the nucleus beam at the EIC. We also demonstrate that the limits from the EIC can be stronger than the off Z-pole measurement at the LEP and light-by-light scattering with pp collisions at the LHC."> Searching for the axion-like particle at the EIC -
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