Goorden M C, Jacquod Ph, Weiss J
Département de Physique Théorique, Université de Genève, CH-1211 Genève 4, Switzerland.
Nanotechnology. 2008 Apr 2;19(13):135401. doi: 10.1088/0957-4484/19/13/135401. Epub 2008 Feb 15.
We investigate the conductance through and the spectrum of ballistic chaotic quantum dots attached to two s-wave superconductors, as a function of the phase difference phi between the two order parameters. A combination of analytical techniques-random matrix theory, Nazarov's circuit theory and the trajectory-based semiclassical theory-allows us to explore the quantum-to-classical crossover in detail. When the superconductors are not phase-biased, phi = 0, we recover known results that the spectrum of the quantum dot exhibits an excitation gap, while the conductance across two normal leads carrying N(N) channels and connected to the dot via tunnel contacts of transparency Gamma(N) is [Formula: see text]. In contrast, when phi = pi, the excitation gap closes and the conductance becomes [Formula: see text] in the universal regime. For [Formula: see text], we observe an order-of-magnitude enhancement of the conductance towards [Formula: see text] in the short-wavelength limit. We relate this enhancement to resonant tunnelling through a macroscopic number of levels close to the Fermi energy. Our predictions are corroborated by numerical simulations.
我们研究了连接到两个s波超导体的弹道混沌量子点的电导及其能谱,作为两个序参量之间相位差φ的函数。解析技术的组合——随机矩阵理论、纳扎罗夫电路理论和基于轨迹的半经典理论——使我们能够详细探索量子到经典的转变。当超导体没有相位偏置时,即φ = 0,我们得到已知结果,量子点的能谱表现出激发能隙,而通过携带N(N)个通道并通过透明度为Gamma(N)的隧道接触连接到量子点的两个正常引线的电导为[公式:见正文]。相反,当φ = π时,激发能隙关闭,在普适区域电导变为[公式:见正文]。对于[公式:见正文],我们在短波长极限下观察到电导朝着[公式:见正文]增强了一个数量级。我们将这种增强与通过靠近费米能的大量能级的共振隧穿联系起来。我们的预测得到了数值模拟的证实。