论文标题

量子线和量子线与量子旋转厅绝缘子的边缘状态的散射

Scattering in quantum wires and junctions of quantum wires with edge states of quantum spin Hall insulators

论文作者

Soori, Abhiram

论文摘要

连续量子系统中散射理论计算的组成部分涉及识别适当的边界条件,除了写下正确的汉密尔顿人。在一维晶格中散射的最简单问题中,由于现场电位和散射而导致的散射(在否则翻译为不变的晶格中)引起的散射给出了不同的结果。虽然可以将连续体和晶格模型中的散射问题相互映射以散射由于现场电位,但由于不相等的键,用于散射的等效连续模型。我们在连续模型的边界条件下引入了一个新的参数$ c $,这等同于由于晶格上的不平等键而引起的散射。此外,我们使用参数$ c $研究了常规金属量子线和连续性中量子旋转厅绝缘子(QSHI)之间的连接。在普通金属量子线和QSHI边缘之间的连接处,我们确定允许最大传输的边界条件。此外,我们使用晶格模型解决了量子线和QSHI的连接之间的散射问题,并将其映射到连续模型结果。跨四个通道的正常金属量子线和两个QSHI边缘的两个通道之间的运输问题不是明确的。我们通过用QSHI的无限边缘的半无限正常金属量子线的连接来纠正这种情况,从而通过Zeeman场来散布QSHI边缘的一个半无限段,并在交界处施加适当的边界条件。我们通过分析计算散射幅度。

An integral part of scattering theory calculations in continuum quantum systems involves identifying appropriate boundary conditions in addition to writing down the correct Hamiltonian. In the simplest problem of scattering in one dimensional lattice, scattering due to an on-site potential and scattering due to an unequal bond (in otherwise translationally invariant lattice) give different results for scattering amplitudes. While the scattering problems in the continuum and the lattice models can be mapped to one another for scattering due to on-site potential, the equivalent continuum model for scattering due to an unequal bond is missing. We introduce a new parameter $c$ in the boundary condition of the continuum model that is equivalent to scattering due to an unequal bond on the lattice. Further, we study a junction between a normal metal quantum wire and a one dimensional edge of quantum spin Hall insulator (QSHI) in continuum using the parameter $c$. In the case of a junction between a normal metal quantum wire and the edge of QSHI, we identify the boundary condition that permits maximum transmission. Further, we solve the scattering problem between the junction of quantum wire and QSHI using a lattice model and map it to continuum model results. The problem of transport between four channels of spinful normal metal quantum wire and two channels of QSHI edge is not well-defined. We rectify this situation by formulating the scattering problem in terms of a junction of a semi-infinite normal metal quantum wire with an infinite edge of QSHI, gapping out one semi-infinite section of the QSHI edge by a Zeeman field and applying an appropriate boundary condition at the junction. We calculate the scattering amplitudes analytically.

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