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Edge-state-transmission duality relation and its implication for measurements

机译:边缘状态传输对偶关系及其对测量的意义

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The duality in the Chalker-Coddington network model is examined. We are able to write down a duality relation for the edge-state-transmission coefficient, but only for a specific symmetric Hall geometry. Looking for broader implication of the duality, we calculate the transmission coefficient T in terms of the conductivity sigma(xx) and sigma(xy) in the diffusive limit. The edge-state scattering problem is reduced to solving the diffusion equation with two boundary conditions [partial derivative(y)-(sigma(xy)/sigma(xx))]partial derivative(x) phi=0 and {partial derivative(x)+[(sigma(xy)-sigma(xy)(lead))/sigma(xx)]partial derivative(y)}phi=0. We find that the resistances in the geometry considered are not necessarily measures of the resistivity and rho(xx), =(W/L)(R/T)hle(2)(R=1-T) holds only when p(xy) is quantized. We conclude that duality alone is not sufficient to explain the experimental findings of Shahar et al. and that Landauer-Buttiker argument does not render the additional condition, contrary to previous expectation. [S0163-1829(98)06015-9]. [References: 39]
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。为了寻找对偶性的更广泛含义,我们根据扩散极限中的电导率sigma(xx)和sigma(xy)计算透射系数T。边缘状态散射问题被简化为具有两个边界条件[偏导数(y)-(sigma(xy)/ sigma(xx))]偏导数(x)phi = 0和{偏导数(x )+ [((sigma(xy)-sigma(xy)(lead))/ sigma(xx)]偏导数(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的量度,rho(xx),=(W / L)(R / T)hle(2)(R = 1-T)仅在p(xy )被量化。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。而且,Landauer-Buttiker的论点没有提供额外的条件,这与先前的预期相反。 [S0163-1829(98)06015-9]。 [参考:39]

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