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    Octupole rotational band in Zn67

    S. Y. Zhang1, D. W. Luo1, R. Han2, C. Xu1,*, H. Y. Wu1,3,†, H. Hua1,‡, J. Z. Li3, Y. Zheng3, Y. D. Fang4 et al.

    Z. H. Li1, X. Q. Li1, C. Y. Guo1, Z. X. Zhou1, J. Lin1, J. Z. Zhang1, L. Ni1, C. B. Li3, T. X. Li3, X. G. Wu3, Z. Y. He3, R. Hong3, Y. Q. Li3, M. Zheng3, Z. H. Zhao3, W. Q. Zhang4, J. H. Xu4, J. H. Li4, Z. H. Jia4, and C. X. Jia4

    • *Contact author: chuan@pku.edu.cn
    • †Contact author: wuhongyi@pku.edu.cn
    • ‡Contact author: hhua@pku.edu.cn

    Phys. Rev. C 112, 054313 – Published 17 November, 2025

    DOI: https://doi.org/10.1103/mxw2-7mfw

    Abstract

    The spectroscopy of Zn67 has been investigated via the fusion-evaporation reaction Ni64(C12, 2α1n)Zn67. Three collective bands are established. The observation of strong E1 transitions and the well-behaved rotational sequence suggest the new negative-parity band built on the 15/2− state is an octupole rotational band. The octupole characteristics of Zn67 is well described by the newly developed semimicroscopic cluster model. Systematics of the excitation energies of the 3− state in even-even Zn isotopes and observation of an octupole rotational band in odd-A Zn67 indicate that the strong octupole effects occur around neutron number 38 in Zn isotopes.

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