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TRANSPORT AND NOISE IN MULTI-TERMINAL DIFFUSIVE CONDUCTORS

机译:多端子扩散导体中的传输和噪声

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Shot-noise induced by current or voltage fluctuations in electron transport is a striking manifestation of charge quantization (for a review, see). It serves as a sensitive tool to study correlations in conductors: while shot-noise assumes a maximum value (with Poissonian distribution) in the absence of correlations, it becomes suppressed when correlations set in as e.g. imposed by the Pauli principle. In diffusive mesoscopic two-terminal conductors where the inelastic scattering lengths exceed the system size the shot-noise suppression factor was predicted to be 1/3. The 1/3-suppression of shot-noise in diffusive conductors is now experimentally confirmed. While some derivations are based on a scattering matrix approach and thus a priori include quantum phase coherence, no such effects are included in the semiclassical Boltzmann-Langevin equation approach, which nevertheless leads to the same result. However, while in the quantum approach for a two-terminal conductor the factor 1/3 was even shown to be universal, the semiclassical derivations given so far are restricted to quasi-one-dimensional conductors. We present here the theory of transport and noise in multiterminal diffusive conductors. This problem has been recently addressed by Blanter and Buettiker in Ref. where they use the scattering matrix formulation followed by an impurity averaging procedure. Having the advantage of including quantum phase coherence, this approach is somewhat cumbersome to generalize to an arbitrary geometry and arbitrary disorder. In contrast to this, our approach is based on a semiclassical Boltzmann-Langevin equation, which greatly simplifies the calculations. In Section 2. we formulate hte problem and give a formal solution of it, while in Section 3. we present some applications of our theory.
机译:电子传输中电流或电压波动引起的散粒噪声是电荷量化的显着表现(有关综述,请参见)。它是研究导体中相关性的敏感工具:虽然散粒噪声在不存在相关性的情况下假设为最大值(具有泊松分布),但当相关性设置为例如保利原则规定的。在非弹性散射长度超过系统尺寸的扩散介观两端导体中,散粒噪声抑制因子预计为1/3。现在已通过实验证实了扩散导体中散粒噪声的1/3抑制。虽然某些推导是基于散射矩阵方法,因此先验包括量子相位相干性,但半经典的Boltzmann-Langevin方程方法中没有包含此类影响,但得出的结果相同。但是,尽管在使用二端导体的量子方法中,因子1/3甚至被证明是通用的,但到目前为止给出的半经典推导仅限于准一维导体。我们在此介绍多端子扩散导体中的传输和噪声理论。 Blanter和Buettiker最近在参考资料中解决了这个问题。他们使用散射矩阵公式,然后进行杂质平均程序。具有包括量子相位相干性的优点,该方法在将其推广到任意几何形状和任意无序方面有些麻烦。与此相反,我们的方法基于半经典的Boltzmann-Langevin方程,该方程大大简化了计算。在第2节中,我们提出了问题并给出了正式的解决方案,而在第3节中,我们提出了我们理论的一些应用。

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