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应变光子菱形晶格中的能带演化与朗道-齐纳-布洛赫振荡

Band evolution and Landau-Zener Bloch oscillations in strained photonic rhombic lattices.

作者信息

Xia Shiqiang, Zhang Yingying, Li Zhixiang, Qin Lu, Yang Chunjie, Lu Hai, Zhang Jun, Zhao Xingdong, Zhu Zunlue

出版信息

Opt Express. 2021 Nov 8;29(23):37503-37514. doi: 10.1364/OE.441554.

Abstract

We investigate band evolution of chiral and non-chiral symmetric flatband photonic rhombic lattices by applying a strain along the diagonal direction, and thereby demonstrating Landau-Zener Bloch (LZB) oscillations in the presence of a refractive index gradient. The chiral and non-chiral symmetric rhombic lattices are obtained by adding a detuning to uniform lattices. For the chiral symmetric lattices, the middle flatband is perturbed due to the chiral symmetry breaking while a nearly flatband appears as the bottom band with the increase of strain-induced next-nearest-neighbor hopping. Consequently, LZB oscillations exhibit intriguing characteristics such as asymmetric energy transitions and almost complete suppression of the oscillations. Nevertheless, for the non-chiral symmetric lattices, flatband persists owing to the retained particle-hole symmetry and evolves into the bottom band. Remarkably, the band gap can be readily tuned, which allows controlling of the amplitude of Landau-Zener tunneling (LZT) rate and may lead to thorough LZT. Our analysis provides an alternative perspective on the generation of tunable flatband and may also bring insight to study the symmetry and topological characterization of the flatband.

摘要

我们通过沿对角线方向施加应变来研究手性和非手性对称平带光子菱形晶格的能带演化,从而在存在折射率梯度的情况下证明朗道 - 齐纳 - 布洛赫(LZB)振荡。手性和非手性对称菱形晶格是通过对均匀晶格添加失谐得到的。对于手性对称晶格,由于手性对称性破缺,中间平带受到扰动,而随着应变诱导的次近邻跳跃增加,底部能带出现一个近平带。因此,LZB振荡表现出有趣的特性,如不对称的能量跃迁和振荡几乎完全被抑制。然而,对于非手性对称晶格,由于保留的粒子 - 空穴对称性,平带持续存在并演变为底部能带。值得注意的是,带隙可以很容易地调节,这允许控制朗道 - 齐纳隧穿(LZT)速率的幅度,并可能导致完全的LZT。我们的分析为可调谐平带的产生提供了一个替代视角,也可能为研究平带的对称性和拓扑特性带来启示。

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