精确输运方程下二维Anderson局部化的自洽理论

Y. Yamane, M. Itoh
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引用次数: 0

摘要

在本文作者(YI)导出的精确输运方程和电导率表达式的基础上,建立了二维非相互作用电子的安德森局域化自一致理论。该方程采用Vollhardt和Wolfle的不可约散射顶点(VW),通过爱因斯坦关系自洽地确定散射顶点的扩散系数。它预测的定位长度与VW得到的相似,但表明随着系统尺寸接近定位长度,由Kubo公式评估的电导率呈指数衰减。结果与大众的预测相反,大众的预测显示了与我们的电导率等效的扩散系数的不同行为。我们的计算还表明,局部化可以与费米液体的朗道-西林理论一起描述。
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Self-Consistent Theory of Anderson Localization in Two Dimensions in View of Exact Transport Equation
Self-consistent theory of Anderson localization of two-dimensional non-interacting electrons is formulated in the context of the exact transport equation and conductivity expression derived by the present authors (YI). The irreducible scattering vertex by Vollhardt and Wolfle (VW) is used in this equation, determining the diffusion coefficient in the scattering vertex self-consistently, through Einstein relation. It predicts a similar localization length to that obtained by VW, but shows that the conductivity evaluated by the Kubo formula decays exponentially, as the system size approaches the localization length. The result is opposed to the prediction by VW, who showed different behaviour of the diffusion coefficient that is equivalent to our conductivity. Our calculation also implies that the localization may be described along with the Landau-Silin theory of Fermi liquid.
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Progress of Theoretical Physics
Progress of Theoretical Physics 物理-物理:综合
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