设计和控制 Kane-Mele 纳米带中的拓扑法诺共振以实现传感应用

S. Jalilvand, M. Soltani, Z. Noorinejad, M. Amini, E. Ghanbari-Adivi
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引用次数: 0

摘要

拓扑法诺共振的概念以超锐利的非对称线形为特征,由于其对外部参数的敏感性和对结构紊乱的免疫性,它是稳健传感应用的一个很有前途的候选概念。在这项研究中,我们沿着一条横跨纳米带宽度的之字形链,以一定的距离引入了几个特意制造的现场空位,从而研究了由六边形晶格和扶手椅边组成的纳米带中空位诱导的拓扑法诺共振。现场空位的存在会在电子能带结构中产生局部能态,导致杂质带的形成,并通过在色带两条扶手边的边缘模式之间形成导电通道而产生法诺共振现象。因此,我们提出了一种源自石墨烯基纳米机械声波晶体的超小型可调片上集成拓扑法诺共振。法诺共振源于纳米带结构中三维绝缘体和非三维绝缘体界面上拓扑保护的偶边和奇边模式之间的干涉,受描述六方晶格中量子自旋霍尔效应的 Kane-Mele 模型支配。拓扑法诺共振的模拟是利用李普曼-施温格散射公式进行分析的。本研究的优势之一是通过分析进行相关计算,除了简单直接之外,还在定量和定性方面很好地再现了通过 Landauer-BÄuttiker 公式得到的结果。研究结果为设计高灵敏度和高精确度的鲁棒传感器提供了可能性,这种传感器可用于检测极其微小的力、质量和空间位置。
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Design and Control of Topological Fano Resonance in Kane-Mele Nanoribbons for Sensing Applications
The concept of topological Fano resonance, characterized by an ultrasharp asymmetric line shape, is a promising candidate for robust sensing applications due to its sensitivity to external parameters and immunity to structural disorder. In this study, the vacancy-induced topological Fano resonance in a nanoribbon made up of a hexagonal lattice with armchair sides is examined by introducing several on-site vacancies, which are deliberately created at regular distances, along a zigzag chain that stretches across the width of the ribbon. The presence of the on-site vacancies can create localized energy states within the electronic band structure, leading to the formation of an impurity band, which can result in Fano resonance phenomena by forming a conductivity channel between the edge modes on both armchair sides of the ribbon. Consequently, an ultracompact tunable on-chip integrated topological Fano resonance derived from the graphene-based nanomechanical phononic crystals is proposed. The Fano resonance arises from the interference between topologically protected even and odd edge modes at the interface between trivial and nontrivial insulators in a nanoribbon structure governed by the Kane-Mele model describing the quantum spin Hall e®ect in hexagonal lattices. The simulation of the topological Fano resonance is performed analytically using the Lippmann-Schwinger scattering formulation. One of the advantages of the present study is that the related calculations are carried out analytically, and in addition to the simplicity and directness, it reproduces the results obtained from the Landauer-BÄuttiker formulation very well both quantitatively and qualitatively. The ¯ndings open up possibilities for the design of highly sensitive and accurate robust sensors for detecting extremely tiny forces, masses, and spatial positions.
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