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    Axially deformed proton-neutron relativistic quasiparticle finite amplitude method for charge-exchange transitions

    Chen Chen (陈晨)1,2, Zhengzheng Li (李征征)3, Yinu Zhang (张一怒)4, and Yifei Niu (牛一斐)1,2,*

    • 1Frontiers Science Center for Rare isotope, Lanzhou University, Lanzhou 730000, China
    • 2School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China
    • 3State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, China
    • 4Sino-French Institute of Nuclear Engineering and Technology, Sun Yat-sen University, Zhuhai 519082, China

    • *Contact author: niuyf@lzu.edu.cn

    Phys. Rev. C 112, 064332 – Published 29 December, 2025

    DOI: https://doi.org/10.1103/qsbz-q1q6

    Abstract

    The quasiparticle finite amplitude method is extended to describe charge-exchange transitions based on the relativistic Hartree-Bogoliubov model, adopting the point-coupling energy density functional DD-PC1 and a finite-range separable pairing force. After validation through comparison with relativistic quasiparticle random-phase approximation results in spherical nuclei, the deformation effects on isobaric analog resonances and Gamow-Teller (GT) transitions in Zn isotopes are investigated. The GT strength exhibits significant fragmentation in deformed nuclei. The analysis of summed strengths and centroid energies in GT resonance region between the K=0 and K=1 components reveals that prolate configurations exhibit stronger K=1 strength and lower K=1 centroid energy, while oblate shapes show an opposite behavior, with stronger K=0 strength and lower K=0 energy. The effects of isoscalar pairing on GT strength distributions for different shape configurations are also examined.

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