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连接到不同马约拉纳纳米线的平行耦合双量子点中的约瑟夫森二极管效应。

Josephson Diode Effect in Parallel-Coupled Double-Quantum Dots Connected to Unalike Majorana Nanowires.

作者信息

Gao Yu-Mei, Xiao Hu, Jiang Mou-Hua, Chi Feng, Yi Zi-Chuan, Liu Li-Ming

机构信息

School of Electronic and Information Engineering, UEST of China, Zhongshan Institute, Zhongshan 528400, China.

Zhongshan Zhuoman Microelectronics Co., Ltd., Zhongshan 528400, China.

出版信息

Nanomaterials (Basel). 2024 Jul 25;14(15):1251. doi: 10.3390/nano14151251.

Abstract

We study theoretically the Josephson diode effect (JDE) when realized in a system composed of parallel-coupled double-quantum dots (DQDs) sandwiched between two semiconductor nanowires deposited on an s-wave superconductor surface. Due to the combined effects of proximity-induced superconductivity, strong Rashba spin-orbit interaction, and the Zeeman splitting inside the nanowires, a pair of Majorana bound states (MBSs) may possibly emerge at opposite ends of each nanowire. Different phase factors arising from the superconductor substrate can be generated in the coupling amplitudes between the DQDs and MBSs prepared at the left and right nanowires, and this will result in the Josephson current. We find that the critical Josephson currents in positive and negative directions are different from each other in amplitude within an oscillation period with respect to the magnetic flux penetrating through the system, a phenomenon known as the JDE. It arises from the quantum interference effect in this double-path device, and it can hardly occur in the system of one QD coupled to MBSs. Our results also show that the diode efficiency can reach up to 50%, but this depends on the overlap amplitude between the MBSs, as well as the energy levels of the DQDs adjustable by gate voltages. The present model is realizable within current nanofabrication technologies and may find practical use in the interdisciplinary field of Majorana and Josephson physics.

摘要

我们从理论上研究了约瑟夫森二极管效应(JDE),该效应是在一个由夹在沉积于s波超导体表面的两根半导体纳米线之间的平行耦合双量子点(DQDs)组成的系统中实现的。由于近邻诱导超导、强Rashba自旋轨道相互作用以及纳米线内部的塞曼分裂的综合作用,每根纳米线的两端可能会出现一对马约拉纳束缚态(MBSs)。在左右纳米线处制备的DQDs与MBSs之间的耦合振幅中,可以产生由超导衬底引起的不同相位因子,这将导致约瑟夫森电流。我们发现,在相对于穿透系统的磁通量的一个振荡周期内,正向和负向的临界约瑟夫森电流在幅度上彼此不同,这种现象被称为JDE。它源于这个双路径器件中的量子干涉效应,并且在一个量子点与MBSs耦合的系统中几乎不会出现。我们的结果还表明,二极管效率可以达到50%,但这取决于MBSs之间的重叠幅度,以及可通过栅极电压调节的DQDs的能级。本模型在当前的纳米制造技术范围内是可实现的,并且可能在马约拉纳和约瑟夫森物理学的跨学科领域中找到实际应用。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c52b/11314297/a9d90468d33d/nanomaterials-14-01251-g001.jpg

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