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    Theoretical analysis of monopole-mode damping in a nearly spherical unitary Fermi gas

    Jing Min1 and Shi-Guo Peng2,3,4,*

    • 1State Key Laboratory for Mesoscopic Physics, School of Physics, Frontiers Science Center for Nano-optoelectronics, Collaborative Innovation Center of Quantum Matter, Peking University, Beijing 100871, China
    • 2Center for Theoretical Physics, Hainan University, Haikou 570228, China
    • 3School of Physics and Optoelectronic Engineering, Hainan University, Haikou 570228, China
    • 4State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, Innovation Academy for Precision Measurement Science and Technology, Chinese Academy of Sciences, Wuhan 430071, China

    • *Contact author: pengshiguo@wipm.ac.cn

    Phys. Rev. A 113, 013303 – Published 2 January, 2026

    DOI: https://doi.org/10.1103/5ykf-zzrr

    Abstract

    We present a comprehensive theoretical investigation of the damping of the monopole mode in strongly interacting Fermi gases confined close to spherical symmetry. Within a hydrodynamic scaling framework, we systematically account for deviations from ideal conditions, including trap anisotropy, anharmonicity, and finite detuning from unitarity. By treating these effects perturbatively, we derive analytical expressions for frequency shifts and damping rates of collective modes. Our analysis reveals that trap-induced symmetry breaking and interaction-induced corrections constitute the primary damping mechanisms, arising from mode coupling between monopole and quadrupole excitations. The results establish a unified theoretical framework that quantitatively captures recent observations of long-lived breathing oscillations and clarify the roles of geometry and interactions in shaping collective dynamics of strongly correlated quantum gases.

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