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FULL COUNTING STATISTICS OF SUPERCONDUCTOR--NORMAL-METAL HETEROSTRUCTURES

机译:超导体的全计数统计-规范金属异质结构

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In 1918 Schottky discovered that the fluctuations in vacuum diodes can be related to the discrete nature of the charge carriers. His observation was that the power spectrum of the current fluctuations gave direct access to the charge e of the discrete carriers responsible for the current. From his theoretical considerations he found a relation between the noise power of the current fluctuations S_I and the average current I, S_I = 2eI,(1) a result nowadays known as the Schottky formula. Its consequence is, that the current noise provides information on the transport process, which is not accessible through conductance measurements only. Studies of the noise properties of tunnel-junctions renewed the interest in noise later. Since about ten years the investigation of transport in quantum coherent structures has boosted the interest in the theory of current noise in mesoscopic structures. Correlations in the transport of fermions have lead to a number of interesting predictions. For example, the noise of a single channel quantum contact of transparency T at zero temperature has the form S_I =2eI(1-T). The noise is thus suppressed below the Schottky value, Eq. (1). The suppression is a direct consequence of the Pauli principle, and is therefore specific to electrons. Particles with bosonic statistics or classical particles show a different behaviour, e. g. for Bosons the noise is enhanced by a factor 1 + T. A convenient measure of the deviation from the Schottky result is the so-called Fano factor F = S_I/2eI.
机译:1918年,肖特基发现真空二极管的波动可能与电荷载流子的离散特性有关。他的观察是,电流波动的功率谱可以直接获取负责电流的离散载波的电荷e。从他的理论考虑,他发现了电流波动S_I的噪声功率与平均电流I之间的关系,S_I = 2eI,(1)如今被称为肖特基公式。其结果是,当前噪声提供了有关传输过程的信息,仅通过电导测量无法获得这些信息。对隧道结噪声特性的研究后来重新引起人们对噪声的关注。大约十年以来,对量子相干结构中的输运的研究引起了人们对介观结构中电流噪声理论的兴趣。费米子运输中的相关性导致了许多有趣的预测。例如,在零温度下透明性T的单通道量子接触的噪声具有S_I = 2eI(1-T)的形式。因此,噪声被抑制在肖特基值Eq以下。 (1)。抑制是保利原理的直接结果,因此特定于电子。具有Bosonic统计量的粒子或经典粒子显示出不同的行为,例如。 G。对于玻色子而言,噪声增加了1 + T倍。肖特基结果偏差的一种简便度量是所谓的Fano因子F = S_I / 2eI。

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