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二维跳跃输运中库仑相互作用效应的数值研究。

A numerical study of Coulomb interaction effects on 2D hopping transport.

作者信息

Kinkhabwala Yusuf A, Sverdlov Viktor A, Likharev Konstantin K

机构信息

Department of Physics and Astronomy, Stony Brook University, Stony Brook, NY 11794-3800, USA.

出版信息

J Phys Condens Matter. 2006 Feb 15;18(6):2013-27. doi: 10.1088/0953-8984/18/6/016. Epub 2006 Jan 27.

Abstract

We have extended our supercomputer-enabled Monte Carlo simulations of hopping transport in completely disordered 2D conductors to the case of substantial electron-electron Coulomb interaction. Such interaction may not only suppress the average value of hopping current, but also affect its fluctuations rather substantially. In particular, the spectral density S(I)(f) of current fluctuations exhibits, at sufficiently low frequencies, a 1/f-like increase which approximately follows the Hooge scaling, even at vanishing temperature. At higher f, there is a crossover to a broad range of frequencies in which S(I)(f) is nearly constant, hence allowing characterization of the current noise by the effective Fano factor [Formula: see text]. For sufficiently large conductor samples and low temperatures, the Fano factor is suppressed below the Schottky value (F = 1), scaling with the length L of the conductor as F = (L(c)/L)(α). The exponent α is significantly affected by the Coulomb interaction effects, changing from α = 0.76 ± 0.08 when such effects are negligible to virtually unity when they are substantial. The scaling parameter L(c), interpreted as the average percolation cluster length along the electric field direction, scales as [Formula: see text] when Coulomb interaction effects are negligible and [Formula: see text] when such effects are substantial, in good agreement with estimates based on the theory of directed percolation.

摘要

我们已将基于超级计算机的、对完全无序二维导体中跳跃输运的蒙特卡罗模拟扩展到存在显著电子 - 电子库仑相互作用的情况。这种相互作用不仅可能抑制跳跃电流的平均值,还会相当大地影响其涨落。特别是,电流涨落的谱密度(S(I)(f))在足够低的频率下呈现出类似(1/f)的增长,即使在温度为零时也大致遵循胡格标度。在较高频率(f)时,会出现向一个较宽频率范围的转变,其中(S(I)(f))几乎恒定,因此可以通过有效法诺因子([公式:见正文])来表征电流噪声。对于足够大的导体样本和低温,法诺因子被抑制到低于肖特基值((F = 1)),并与导体长度(L)按(F = (L(c)/L)(α))标度。指数(α)受库仑相互作用效应的显著影响,当这种效应可忽略时(α = 0.76 ± 0.08),而当效应显著时(α)几乎变为(1)。标度参数(L(c)),被解释为沿电场方向的平均渗流团簇长度,当库仑相互作用效应可忽略时按([公式:见正文])标度,而当这种效应显著时按([公式:见正文])标度,这与基于定向渗流理论的估计结果吻合良好。

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