\begin{document}$\displaystyle\frac{13}{2}^{-}\left(\nu\displaystyle\frac{7}{2}^{+}[633]\otimes\nu\displaystyle\frac{1}{2}^{-}[521]\otimes\pi\displaystyle\frac{5}{2}^{+}[413]\right)$\end{document}. More low-lying multi-particle states are predicted in 163Eu. Due to its significant effect on the nuclear mean field, the high-order \begin{document}$\varepsilon_{6}$\end{document} deformation plays an important role in the energy and configuration assignment of the multi-particle states. Compared to its neighboring even-even nuclei 162Sm and 164Gd, there is a 10%~15% increase of \begin{document}$J^{(1)}$\end{document} of the one-particle ground-state band in 163Eu. This is explained by the pairing reduction due to the blocking of the nucleon on the proton \begin{document}$\pi\displaystyle\frac{5}{2}^{+}$\end{document}[413] orbital in 163Eu."> High-<i>K</i> isomer and the rotational properties in the odd-<i>Z</i> neutron-rich nucleus <inline-formula><tex-math id="Z-20190419053926-1">\begin{document}${{}^{\bf{163}} {\bf {Eu}}}$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/426bf2a7-693f-4dfe-b599-0f441a0608c1/CPC-2019-0075_Z-20190419053926-1.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/426bf2a7-693f-4dfe-b599-0f441a0608c1/CPC-2019-0075_Z-20190419053926-1.png"/></alternatives></inline-formula> -
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