\begin{document}$ 1d_{5/2} $\end{document} component largely enhances the couplings between the even-parity orbit \begin{document}$ 1/2_2^+ $\end{document} and the nuclear core to ensure an even-parity GS, whereas the \begin{document}$ 2s_{1/2} $\end{document} component therein dominates the halo formation in 11Be. Moreover, the deformed halo in 11Be is found to be stabilized by the attractive inherent correlations between the \begin{document}$ 1d_{5/2} $\end{document} and \begin{document}$ 2s_{1/2} $\end{document} components of the halo orbit \begin{document}$ 1/2_2^+ $\end{document}, instead of pairing correlations, which paves a new way for understanding the halo pictures in deformed unstable nuclei."> Unified mechanism behind the even-parity ground state and neutron halo of <sup>11</sup>Be -
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