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Formation Dirac point and the topological surface states for HgCdTe-QW and mixed 3D HgCdTe TI

机译:HgCdTe-QW和混合3D HgCdTe TI的形成狄拉克点和拓扑表面态

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In this paper the results of numerical calculations based on the finite difference method (FDM) for the 2D and 3D TI with and without uniaxial tensile strain for mixed Hg1-xCdxTe structures are presented. The numerical calculations were made using the 8×8 model for x from 0 up to 0.155 and for the wide range for the thickness from a few nm for 2D up to 150 nm for 3D TI as well as for different mismatch of the lattice constant and different barrier potential in the case of the QW. For the investigated region of the Cd composition (x value) the negative energy gap (Eg=Γ8-Γ6) in the Hg1-xCdxTe is smaller than in the case of pure HgTe which, as it turns out, has a significant influence on the topological surface states (TSS) and the position of the Dirac point for QW as well as for 3D TI. The results show that the strained gap and the position of the Dirac point against the Γ8 is a function of the x-Cd compounds in the case of the 3D TI as well as the critical width of the mixed Hg1-xCdxTe QW.
机译:本文提出了基于有限差分法(FDM)的2D和3D TI混合Hg1-xCdxTe结构具有和不具有单轴拉伸应变的数值计算结果。使用8×8模型对x从0到0.155进行了数值计算,对于从2D到几纳米的厚度到3D TI到150 nm的宽厚度以及不同的晶格常数和QW情况下势垒不同。对于研究的Cd组成区域(x值),Hg1-xCdxTe中的负能隙(Eg =Γ8-Γ6)小于纯HgTe的情形,事实证明,纯HgTe对Cd的影响很大。 QW和3D TI的拓扑表面状态(TSS)和Dirac点的位置。结果表明,在3D TI情况下,应变间隙和Dirac点相对于Γ8的位置是x-Cd化合物的函数以及Hg1-xCdxTe混合QW的临界宽度。

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