\begin{document}$ d_{N\Omega} $\end{document} dibaryon production in the \begin{document}$ K^- p \rightarrow d_{N\Omega} \bar{\Xi}^0 $\end{document} process by utilizing a kaon beam with a typical momentum of approximately 10 GeV, which may be available at COMPASS, OKA@U-70, and SPS@CERN. The cross sections for \begin{document}$ K^- p \rightarrow d_{N\Omega} \bar{\Xi}^0 $\end{document} are estimated, and in particular, the magnitude of the cross sections is evaluated to be several hundred nanobarns at \begin{document}$ P_K=20 $\end{document} GeV. Considering that the \begin{document}$ d_{N\Omega} $\end{document} dibaryon dominantly decays into \begin{document}$ \Xi \Lambda $\end{document} and \begin{document}$ \Xi \Sigma $\end{document}, we also estimate the cross sections for \begin{document}$ K^- p \to \Xi^0 \Lambda \bar{\Xi}^0 $\end{document} and \begin{document}$ K^- p \to $\end{document}\begin{document}$ \Xi^- \Sigma^+ \bar{\Xi}^0 $\end{document}, where the \begin{document}$ d_{N\Omega} $\end{document} dibaryon can be observed in the invariant mass distributions of \begin{document}$ \Xi^0 \Lambda $\end{document} and \begin{document}$ \Xi^- \Sigma^+ $\end{document}, respectively."> Production of <inline-formula><tex-math id="M1">\begin{document}$ {\boldsymbol{d}_{\boldsymbol{N\Omega}}} $\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/a374c2f7-3dae-4c41-afce-c5331f286abb/CPC-2022-0592_M1.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/a374c2f7-3dae-4c41-afce-c5331f286abb/CPC-2022-0592_M1.png"/></alternatives></inline-formula> dibaryon in kaon induced reactions -
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