Flatband发电机

W. Maimaiti
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引用次数: 3

摘要

平带(FBs)是平动不变紧结合网络单粒子谱中的无色散能带。由于相消干涉的发生,导致宏观简并特征态存在于有限数量的单元胞中,称为紧定局域态(CLSs)。这种宏观简并通常对摄动高度敏感,即使是轻微的摄动也会解除简并并导致各种有趣的物理现象。在本文中,我们开发了一种在一维、二维厄米和一维非厄米系统中识别和构造FB哈密顿量的方法。首先,我们根据FB格的CLS性质对它们进行了系统的分类,并提出了一种生成具有给定CLS性质的FB格的紧密结合哈密顿子的方案——FB生成器。将该FB发生器应用于一维系统,我们识别了具有任意频带数和CLS大小的一维晶格的所有可能的FB哈密顿量。扩展一维方法,我们建立了二维FB哈密顿子的FB生成器,其中cls在$2\times2$斑块中最多占用四个单元格。利用这种方法,我们实现了一维双波段非厄米格的FB发生器。最后,我们运用我们的方法提出了一个紧密结合的模型来解释微波光子晶体的光谱特性。本文的研究结果和方法进一步加深了我们对FB晶格及其类结构性质的理解,为实验中设计FB晶格提供了更大的灵活性,并为未来的研究开辟了新的途径。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flatband generators
Flatbands (FBs) are dispersionless energy bands in the single-particle spectrum of a translational invariant tight-binding network. The FBs occur due to destructive interference, resulting in macroscopically degenerate eigenstates living in a finite number of unit cells, which are called compact localized states (CLSs). Such macroscopic degeneracy is in general highly sensitive to perturbations, such that even slight perturbation lifts the degeneracy and leads to various interesting physical phenomena. In this thesis, we develop an approach to identify and construct FB Hamiltonians in 1D, 2D Hermitian, and 1D non-Hermitian systems. First, we introduce a systematic classification of FB lattices by their CLS properties, and propose a scheme to generate tight-binding Hamiltonians having FBs with given CLS properties---a FB generator. Applying this FB generator to a 1D system, we identify all possible FB Hamiltonians of 1D lattices with arbitrary numbers of bands and CLS sizes. Extending the 1D approach, we establish a FB generator for 2D FB Hamiltonians that have CLSs occupying a maximum of four unit cells in a $2\times2$ plaquette. Employing this approach in the non-Hermitiaon regime, we realize a FB generator for a 1D non-Hermitian lattice with two bands. Ultimately, we apply our methods to propose a tight-binding model that explains the spectral properties of a microwave photonic crystal. Our results and methods in this thesis further our understanding of the properties of FB lattices and their CLSs, provide more flexibility to design FB lattices in experiments, and open new avenues for future research.
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