论文标题

一维非甲状化晶体的本地化过渡,频谱结构和绕组数

Localization transition, spectrum structure and winding numbers for one-dimensional non-Hermitian quasicrystals

论文作者

Liu, Yanxia, Zhou, Qi, Chen, Shu

论文摘要

通过分析Lyapunov指数(LE),我们开发了一种严格的,基本的方案,用于研究具有复杂相位因子和非重生跳跃的一般非热晶晶体。特别是,本地化 - 范围化过渡点,$ \ Mathcal {pt} $ - 对称点 - 破坏点和绕组的数字过渡点由其双重Hermitian模型的LES确定。该分析基于阿维拉的全球理论,我们发现绕组数与LE的加速度直接相关,而加速度的量化是Avila全球理论的关键成分。该结果也适用于具有较高绕组的模型,不仅是最简单的Aubry-André模型。作为典型示例,我们在整个参数空间中获得了非Hermitian Aubry-André模型的定位过渡的分析相边界,并且可以直接确定完整的相图。对于一个高缠绕模型的非热式Soukoulis-Economou模型,我们展示了定位过渡和绕组数转变的相位边界与其双重遗产模型的LES有关。此外,我们发现了鲁棒频谱的一个有趣功能,即,如果一个分别处于扩展状态或本地化的状态(分别是扩展的状态或本地化的状态),则在更改复杂相位参数$ h $ $ h $ $ h $ $ h $ $ h $ $ h $或非重点参数$ g $时保持不变的功能。

By analyzing the Lyapunov exponent (LE), we develop a rigorous, fundamental scheme for the study of general non-Hermitian quasicrystals with both complex phase factor and non-reciprocal hopping. Specially, the localization-delocalization transition point, $\mathcal{PT}$-symmetry-breaking point and the winding number transition points are determined by LEs of its dual Hermitian model. The analysis was based on Avila's global theory, and we found that winding number is directly related to the acceleration, the slope of the LE, while quantization of acceleration is the crucial ingredient of Avila's global theory. This result applies as well to the models with higher winding, not only the simplest Aubry-André model. As typical examples, we obtain the analytical phase boundaries of localization transition for non-Hermitian Aubry-André model in the whole parameter space, and the complete phase diagram is straightforwardly determined. For the non-Hermitian Soukoulis-Economou model, a high winding model, we show how the phase boundaries of localization transition and winding number transitions relate to the LEs of its dual Hermitian model. Moreover, we discover an intriguing feature of robust spectrum, i.e., the spectrum keeps invariant when one changes the complex phase parameter $h$ or non-reciprocal parameter $g$ in the region of $h<|h_c|$ or $g<|g_c|$ if the system is in the extended or localized state, respectively.

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