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存在点上超导配对时的类 Fano 共振猝灭动力学。

Quench dynamics of Fano-like resonances in the presence of the on-dot superconducting pairing.

机构信息

Department of General Education, Polish Air Force University, ul. Dywizjonu 303 nr 35, 08521, Deblin, Poland.

Institute of Spintronics and Quantum Information, Faculty of Physics, Adam Mickiewicz University in Poznań, ul. Uniwersytetu Poznańskiego 2, 61614, Poznań, Poland.

出版信息

Sci Rep. 2023 May 11;13(1):7639. doi: 10.1038/s41598-023-34376-5.

Abstract

We explore the electron dynamics of a system composed of double quantum dot embedded between metallic and superconducting leads in a "T-shape" geometry. In nanoscopic systems, where electron transfer between electrodes can be realized via different paths, interference effects play an important role. For double quantum dot system in the chosen geometry, interference of electrons transferred between electrodes via the interfacial quantum dot and electrons scattered on the side dot gives rise to Fano-like interference. If such a system is additionally coupled to a superconducting electrode, together with the well-understood Fano resonance an additional resonance appears on the opposite side of the Fermi level. In the recent work (Barański et al. in Sci Rep 10:2881, 2020), we showed that this resonance occurs solely as a result of the local pairing of non-scattered electrons with scattered ones. In this work, considering the quench dynamics, we explore how much time is required for formation of each of these resonances. In particular, (i) we analyze the charge oscillations between subsystems; (ii) we estimate the time required for each resonance to achieve stable equilibrium upon an abrupt change of interdot connection; (iii) we discuss a typical energy and time scales for experiments on similar architectures.

摘要

我们研究了嵌入在金属和超导引线之间的“T 型”几何形状的双量子点系统的电子动力学。在纳米系统中,电极之间的电子转移可以通过不同的路径来实现,因此干涉效应起着重要的作用。对于所选几何形状中的双量子点系统,通过界面量子点和在侧点上散射的电子之间转移的电子的干涉会产生类 Fano 干涉。如果这样的系统另外与超导电极耦合,除了众所周知的 Fano 共振之外,在费米能级的另一侧还会出现另外一个共振。在最近的工作中(Barański 等人,在 Sci Rep 10:2881, 2020 中),我们表明,这种共振仅作为未散射电子与散射电子的局部配对的结果而出现。在这项工作中,考虑到淬火动力学,我们探讨了形成每个共振所需的时间。具体来说,(i)我们分析子系统之间的电荷振荡;(ii)我们估计在突然改变点间连接时,每个共振达到稳定平衡所需的时间;(iii)我们讨论了类似结构实验的典型能量和时间尺度。

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