\begin{document}$d^*(2380)$\end{document} resonance. Several selected exclusive processes at high energies for the production of \begin{document}$d^*$\end{document} are discussed. Results of two structural scenarios for \begin{document}$d^*(2380)$\end{document}, a hexaquark dominant compact system in the quark degrees of freedom, and a \begin{document}$\pi N\Delta$\end{document} three-body bound state in the hadronic degrees of freedom, are analyzed and compared. A rather remarkable difference between the results of these two scenarios for the mentioned processes are addressed."> Constituent counting rule and the production of <inline-formula><tex-math id="M1">\begin{document}${{d^*(2380)}}$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/41ce8927-90e5-47a0-a570-e690de4091e4/CPC-2019-0044_M1.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/41ce8927-90e5-47a0-a570-e690de4091e4/CPC-2019-0044_M1.png"/></alternatives></inline-formula> at high energies -
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