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$$K^{pi}=8^{-}$$ isomers and $$K^{pi}=2^{-}$$ octupole vibrations in $$N=150$$ shell-stabilized isotones

Robinson, A. P.*; Khoo, T. L.*; Ahmad, I.*; Tandel, S. K.*; Kondev, F. G.*; Nakatsukasa, Takashi*; Seweryniak, D.*; Asai, Masato  ; Back, B. B.*; Carpenter, M. P.*; Chowdhury, P.*; Davids, C. N.*; Eeckhaudt, S.*; Greene, J. P.*; Greenlees, P. T.*; Gros, S.*; Heinz, A.*; Herzberg, R.-D.*; Janssens, R. V. F.*; Jones, G. D.*; Lauritsen, T.*; Lister, C. J.*; Peterson, D.*; Qian, J.*; Tandel, U. S.*; Wang, X.*; Zhu, S.*

Isomers have been identified in $$^{246}$$Cm and $$^{252}$$No with quantum number $$K^{pi}=8^{-}$$, which decay through $$K^{pi}=2^{-}$$ rotational bands built on octupole vibrational states. For $$N=150$$ isotones with atomic number $$Z=94$$$$sim$$102, the $$K^{pi}=8^{-}$$ and 2$$^{-}$$ states have remarkably stable energies, indicating neutron excitations. An exception is a singular minimum in the 2$$^{-}$$ energy at $$^{246}$$Cm, due to the additional role of proton configurations.

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Category:Physics, Nuclear

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