Export citation

Export citation

Choose format for download:

Download Citation

    Exact mobility line and mobility ring in the complex energy plane of a flat-band lattice with a non-Hermitian quasiperiodic potential

    Guang-Xin Pang1, Zhi Li2,3, Shan-Zhong Li2,3, Yan-Yang Zhang1, Jun-Feng Liu1, and Yi-Cai Zhang1,*

    • 1School of Physics and Materials Science, Guangzhou University, Guangzhou 510006, China
    • 2Key Laboratory of Atomic and Subatomic Structure and Quantum Control (Ministry of Education), Guangdong Basic Research Center of Excellence for Structure and Fundamental Interactions of Matter, School of Physics, South China Normal University, Guangzhou 510006, China
    • 3Guangdong Provincial Key Laboratory of Quantum Engineering and Quantum Materials, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Frontier Research Institute for Physics, South China Normal University, Guangzhou 510006, China

    • *Contact author: zhangyicai123456@163.com

    Phys. Rev. B 111, 214205 – Published 10 June, 2025

    DOI: https://doi.org/10.1103/z96m-ckm6

    Abstract

    In this study, we investigate the problem of Anderson localization in a one-dimensional flat band lattice with a non-Hermitian quasiperiodic on-site potential. First of all, we discuss the influences of non-Hermitian potentials on the existence of critical states. Our findings show that, unlike in Hermitian cases, the non-Hermiticity of the potential leads to the disappearance of critical states and critical regions. Furthermore, we are able to accurately determine the Lyapunov exponents and the mobility edges. Our results reveal that the mobility edges form mobility lines and mobility rings in the complex energy plane. Within the mobility rings, the eigenstates are extended, while the localized states are located outside the mobility rings. For mobility line cases, only when the eigenenergies lie on the mobility lines, their corresponding eigenstates are extended states. As the energy approaches the mobility edges, we observe that, differently from Hermitian cases, here the critical index of the localization length is not a constant, but rather varies depending on the positions of the mobility edges. In addition, we conducted a comprehensive study on the effects of different parameter changes on the phase diagram of the system. Finally, we find that the changes of parameters can lead to changes of the topological structure of the mobility rings.

    Physics Subject Headings (PhySH)

    Authorization Required

    We need you to provide your credentials before accessing this content.

    References (Subscription Required)

    Outline

    Information

    Sign In to Your Journals Account

    Filter

    Filter

    Article Lookup

    Enter a citation