首页|非厄米准周期系统中的二次局域体态和局域-扩展的边缘态

非厄米准周期系统中的二次局域体态和局域-扩展的边缘态

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局域化是物理学中一个基础且极具潜力的研究领域。基于广义Su-Schrieffer-Heeger模型,本文针对其非厄米项以准周期、非对角形式出现的特点,提出了一种新的分析框架,旨在分别探讨体态与边缘态的局域化特性。对于体态,它可以经历由准无序诱导的扩展-共存-局域-共存-局域的转变,或者是由非厄米特性引起的共存-局域-共存-局域的转变。同时边缘态可以被破坏和恢复,且其拓扑相变与局域化转变完全同步。最后,发现在局域化转变点处归一化参与率的导数展现出明显的不连续性。本文的结果不仅展示了体态和边缘态局域化性质的多样性,而且为局域化研究开辟了一个新的研究视角。
Reentrant localized bulk and localized-extended edge in quasiperiodic non-Hermitian systems
The localization is one of the active and fundamental research areas in topology physics.In this field,a comprehensive understanding of how wave functions distribute within a system is crucial.This work delves into this topic by proposing a novel systematic method based on a generalized Su-Schrieffer-Heeger(SSH)model.This model incorporates a quasiperiodic non-Hermitian term that appears at an off-diagonal position,adding a layer of complexity to the traditional SSH framework.By utilizing this model,we analyze the localization behaviors of both bulk state and edge state.For the bulk states,the analysis reveals a fascinating transition sequence.Specifically,the bulk states can undergo an extended-coexisting-localized-coexisting-localized transition,which is induced by the introduction of quasidisorder.This transition is not arbitrary but is rather conformed by the inverse participation ratio(IPR),a metric that quantifies the degree of localization of a wave function.As quasidisorder increases,the bulk states initially remain extended,but gradually,some states begin to be localized.A coexistence region appears where both extended and localized states are present.Further increase in quasidisorder leads to a complete localization of all bulk states.However,remarkably,within a certain range of quasidisorder strengths,the localized states can once again transition back to an extended state,creating another coexistence region.This complex behavior demonstrates the rich and diverse localization properties of the bulk states in non-Hermitian quasiperiodic systems.In addition to the IPR,other metrics such as the normalized participation ratio(NPR)and the fractal dimension of the eigenstates also play important roles in characterizing the localization behavior.These metrics provide a more in-depth understanding of the transition process and help to confirm the existence of the coexistence regions.Overall,we comprehensively analyze the localization behaviors of bulk and edge states in non-Hermitian quasiperiodic systems based on a generalized SSH model.The proposed systematic method present new insights into the complex interplay between quasidisorder,non-Hermiticity,and localization properties in topological physics.

non-Hermitianquasidisorderreentrant-localizedtopological phase transition

郭刚峰、包茜茜、谭磊、刘伍明

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宿迁学院数理学院,宿迁 223800

兰州大学,兰州理论物理中心,甘肃省理论重点实验室,兰州 730000

中国科学院物理研究所,北京凝聚态物理国家研究中心,北京 100190

非厄米 准无序 二次局域 拓扑相变

2025

物理学报
中国物理学会,中国科学院物理研究所

物理学报

北大核心
影响因子:1.038
ISSN:1000-3290
年,卷(期):2025.74(1)