\begin{document}$ h_{11/2} $\end{document} orbit to the highest one. As the Fermi surface increases, notable transformations occur in the wobbling mode. Initially, the mode exhibits a transverse revolution around the short axis of the nucleus. However, as the Fermi surface continues to increase, the mode gradually shifts to a longitudinal revolution around the intermediate axis. Eventually, it transitions to a transverse revolution around the long axis. Notably, the stability of the long axis transverse mode diminishes relative to its counterpart along the short axis as the total angular momentum increases at \begin{document}$ \gamma=20^\circ $\end{document}."> Wobbling motion for a triaxial rotor plus a single quasiparticle -
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