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Interplay between global PT-symmetry and local PT-symmetry in coupled waveguide chain

机译:耦合波导链中全局PT对称与局部PT对称之间的相互作用

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Recently parity-time (PT) symmetric system in the field of optics attracts attention due to some intriguing phenomena, i.e., bifurcation and unidirectional light propagation. In presence of loss and gain, PT symmetric system become intrinsically non-Hermitian. Interestingly, in those non-Hermitian system all real eigenvalues still can exist in certain regime in the parameter space of non-Hermiticity. We study interplay between global PT-symmetry and local PT-symmetry in coupled waveguide chain with dimerized waveguide in presence of gain or losses. With assistance of SSH model and the concept of general coupled mode theory (GCMT) developed from first-principle of Maxwell's equation, we study the coupled waveguide chain which preserves the local PT-symmetry. Globally, the coupled waveguide chain can be either PT symmetric or PT-symmetry broken. The existence of edge states depends on Berry phase. If two coupled waveguide chains with different Berry phase are connected to form a new chain, it is likely to form an edge state. Surprisingly, the edge state exists in global PT symmetric system, and also in global PT-symmetry broken system. Moreover, the edge state is robust against non-Hermiticity, as confirmed by the existence of edge state regardless of variation of non-Hermiticity. It seems that there is no necessary to ensure PT symmetry in entire system for an edge state, but the local PT symmetry in each unit cell is needed.
机译:最近,由于一些有趣的现象,即分叉和单向光传播,光学领域的奇偶时间(PT)对称系统引起了人们的注意。在存在损耗和增益的情况下,PT对称系统本质上成为非Hermitian的系统。有趣的是,在那些非Hermitian系统中,所有非特征值仍然可以在非Hermiticity的参数空间中以某种形式存在。我们研究在存在增益或损耗的情况下,具有二聚化波导的耦合波导链中的全局PT对称性与局部PT对称性之间的相互作用。借助于SSH模型和麦克斯韦方程第一原理发展的通用耦合模式理论(GCMT)概念,我们研究了保留局部PT对称性的耦合波导链。总的来说,耦合的波导链可以是PT对称的或PT对称的。边缘状态的存在取决于Berry相。如果将两个具有不同贝里相位的耦合波导链连接起来以形成一条新链,则很可能会形成边缘状态。出人意料的是,边缘状态存在于整体PT对称系统中,也存在于整体PT对称破碎系统中。此外,边缘状态对非赫米蒂性具有鲁棒性,这由边缘状态的存在所证实,而与非赫米蒂性的变化无关。似乎没有必要在整个系统中确保边缘状态的PT对称性,但是需要每个单位单元中的局部PT对称性。

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