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Edge state transmission, duality relation and its implication to measurements

机译:边缘状态传递,二元关系及其对蕴涵的启示   测量

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摘要

The duality in the Chalker-Coddington network model is examined. We are ableto write down a duality relation for the edge state transmission coefficient,but only for a specific symmetric Hall geometry. Looking for broaderimplication of the duality, we calculate the transmission coefficient $T$ interms of the conductivity $\sigma_{xx}$ and $\sigma_{xy}$ in the diffusivelimit. The edge state scattering problem is reduced to solving the diffusionequation with two boundary conditions$(\partial_y-(\sigma_{xy})/(\sigma_{xx})\partial_x)\phi=0$ and$[\partial_x+(\sigma_{xy}-\sigma_{xy}^{lead})/(\sigma_{xx}) \partial_y]\phi=0$.We find that the resistances in the geometry considered are not necessarilymeasures of the resistivity and $\rho_{xx}=L/W R/T h/e^2$ ($R=1-T$) holds onlywhen $\rho_{xy}$ is quantized. We conclude that duality alone is not sufficientto explain the experimental findings of Shahar et al and that Landauer-Buttikerargument does not render the additional condition, contrary to previousexpectation.
机译:检查了Chalker-Coddington网络模型中的对偶性。我们能够写下边缘状态传输系数的对偶关系,但仅针对特定的对称霍尔几何形状。寻找对偶的更广泛的含义,我们计算了扩散极限中电导率$ \ sigma_ {xx} $和$ \ sigma_ {xy} $的传输系数$ T $。边缘状态散射问题被简化为用两个边界条件$(\ partial_y-(\ sigma_ {xy})/(\ sigma_ {xx})\ partial_x)\ phi = 0 $和$ [\ partial_x +(\ sigma_ {xy}-\ sigma_ {xy} ^ {lead})/(\ sigma_ {xx})\ partial_y] \ phi = 0 $。我们发现所考虑的几何形状中的电阻不一定是电阻率和$ \的量度。仅当量化$ \ rho_ {xy} $时,rho_ {xx} = L / WR / T h / e ^ 2 $($ R = 1-T $)成立。我们得出的结论是,仅靠双重性不足以解释Shahar等人的实验发现,与先前的预期相反,Landauer-Buttikerarment并没有提供其他条件。

著录项

  • 作者

    Xiong, Shanhui;

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  • 年度 1998
  • 总页数
  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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