\begin{document}$^{93}$\end{document}Mo are investigated using Large Scale Shell Model calculations, and reasonable agreement is obtained between the experimental and calculated values. The calculated results show that the lower-lying states are mainly dominated by proton excitations from the \begin{document}$1f_{5/2}$\end{document}, \begin{document}$2p_{3/2}$\end{document}, and \begin{document}$2p_{1/2}$\end{document} orbitals into the higher orbitals across the Z = 38 or Z = 40 subshell closure. For the higher-spin states, multi-particle excitations, including the excitation of \begin{document}$2d_{5/2}$\end{document} neutrons across the N = 56 subshell closure into the high-j intruder \begin{document}$1h_{11/2}$\end{document} orbital, are essential. Moreover, the previously unknown spin-parity assignments of the six higher excited states in \begin{document}$^{93}$\end{document}Mo are inferred from the shell model calculations."> Multi-quasiparticle excitations and the impact of the high-<i>j</i> intruder orbital in the <i>N</i> = 51 <sup>93</sup>Mo nucleus -
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