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具有周期性跳跃调制的非厄米Su-Schrieffer-Heeger链中的拓扑与PT对称性。

Topology andPTsymmetry in a non-Hermitian Su-Schrieffer-Heeger chain with periodic hopping modulation.

作者信息

Mandal Surajit, Kar Satyaki

机构信息

Department of Physics, Jadavpur University, Kolkata 700032, West Bengal, India.

Department of Physics, AKPC Mahavidyalaya, Bengai, West Bengal 712611, India.

出版信息

J Phys Condens Matter. 2024 Dec 27;37(9). doi: 10.1088/1361-648X/ad9f08.

Abstract

We study the effect of periodic hopping modulation in a Su-Schrieffer-Heeger (SSH) chain with an additional onsite staggered imaginary potential (of strength). Such dissipative, non-Hermitian (NH) extension amply modifies the features of the topological trivial phase (TTP) and the topological nontrivial phase (TNP) of the SSH chain, more so with the periodic hopping distribution. Generally a weak NH potential can respect the parity-time (PT) symmetry keeping the energy eigenvalues real, while a strong potential breaksPTconservation leading to imaginary edge state and complex bulk state energies in the system. We find that the non-zero energy in-gap states, that appear due to periodic hopping modulations even in the = 0 limit, take purely real or purely imaginary eigenvalues depending on the strength of bothand Δ (dimerization parameter). The localization of topological edge states (in-gap states) at the boundaries are investigated that reveals extended nature not only near topological transitions (further away from|Δ/t|=1) but also near the unmodulated limit ofΔ=0. Moreover, localization of the bulk states is observed at the maximally dimerized limit of|Δ/t|=1, which increases further with. These dissipative features can offer additional tunability in modulating the gain-loss contrast in optical systems or in designing various quantum information processing and storage devices.

摘要

我们研究了在具有额外在位交错虚势(强度为 )的Su-Schrieffer-Heeger(SSH)链中周期性跳跃调制的影响。这种耗散的非厄米(NH)扩展极大地改变了SSH链的拓扑平凡相(TTP)和拓扑非平凡相(TNP)的特征,在周期性跳跃分布的情况下更是如此。一般来说,弱NH势可以保持宇称时间(PT)对称性,使能量本征值为实数,而强势会破坏PT守恒,导致系统中的虚边缘态和复体态能量。我们发现,即使在 = 0极限下由于周期性跳跃调制而出现的非零能隙态,其本征值根据 和Δ(二聚化参数)的强度取纯实数或纯虚数。研究了拓扑边缘态(能隙态)在边界处的局域化,结果表明不仅在拓扑转变附近(远离|Δ/t| = 1),而且在Δ = 0的未调制极限附近,它们都具有扩展性质。此外,在|Δ/t| = 1的最大二聚化极限处观察到体态的局域化,并且随着 进一步增加。这些耗散特性可以在调制光学系统中的增益-损耗对比度或设计各种量子信息处理和存储设备时提供额外的可调性。

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