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    Shape evolution in neutron-rich odd-even Nb105–109 isotopes

    M. Abushawish1,*, E. H. Wang2,3,4,†, J. Dudouet1,‡, A. Navin5, E. Clément5, G. Duchêne6, J. H. Hamilton4, A. Lemasson5, C. Michelagnoli5,§ et al.

    O. Stezowski1, S. Bhattacharyya7,8, F. DidierJean6, B. Jacquot5, Y. H. Kim5,∥, Y. X. Luo9, A. V. Ramayya4, J. O. Rasmussen9, and S. J. Zhu10

    • *Present address: Grupo de Física Nuclear, Universidad Complutense de Madrid, CEI Moncloa, 28040 Madrid, Spain.
    • †Contact author: enWang9864@outlook.com
    • ‡Contact author: j.dudouet@ip2i.in2p3.fr
    • §Present address: Institut Laue-Langevin, F-38042 Grenoble Cedex, France.
    • ∥Present address: Center for Exotic Nuclear Studies, Institute for Basic Science, Daejeon 34126, Republic of Korea.

    Phys. Rev. C 113, 014308 – Published 9 January, 2026

    DOI: https://doi.org/10.1103/sj3y-qnzp

    Abstract

    Background: Neutron-rich nuclei around Z≈40 are well known for exhibiting multiple shape transitions. This region shows one of the sharpest shape transitions in the nuclear chart, evolving from a spherical vibrator at N=58 to a strongly deformed prolate shape at N=60. The largest deformations are observed for Sr38 and Zr40. This abrupt shape transition disappears at Z=36 and below, where a shape transition from spherical to oblate nuclei is predicted. On the other hand, for Z≥42 and N≥60, the shape is known to evolve from axial to triaxial. While the even-Z nuclei in this region have already been extensively studied, new insights can be gained from the studies of odd-Z isotopes for a better understanding of the underlying mechanisms driving these phenomena.

    Purpose: The Nb41 nuclei lie at the boundary between axially deformed Zr and triaxially deformed Mo nuclei. This work investigates the nuclear structure of very neutron-rich Nb nuclei up to N=68. The goal is to understand how the nuclear shape evolves as a function of isospin in this isotopic chain and provide new insights into the emergence of triaxial deformation.

    Methods: The structure of the neutron-rich Nb isotopes was investigated using state-of-the-art high-resolution γ-ray spectroscopy of fission fragments produced via two different fission reactions. The use of Be9(U238,f) inverse kinematics, with a detection system comprising AGATA, EXOGAM, and VAMOS++, enabled the measurement of prompt and delayed γ rays from isotopically identified fission fragments, and γ−γ−γ−γ highfold data were obtained from a spontaneous fission source of Cf252 using the Gammasphere array.

    Results: The level scheme of Nb105 has been significantly extended, with the addition of two negative-parity bands observed for the first time. A new level scheme is proposed for Nb107, which is not in agreement with an earlier measurement, and new levels and transitions have been added to the very neutron-rich Nb109. The degree of triaxiality of the new bands is discussed on the basis of signature splitting analysis. The recently reported level scheme of Nb99 has been revised.

    Conclusions: This systematic study on the Nb isotopic chain, compared to Zr and Mo, indicates that while the ground-state band exhibits a triaxial deformation, attributed to a proton hole coupled to a triaxially deformed Mo core, the negative-parity bands, based on isomeric bandheads, display an axially symmetric deformed structure, similar to that observed in the Zr isotopes, revealing the existence of a shape coexistence in the neutron-rich Nb nuclei.

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