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狄拉克费米子的多次安德列夫反射的相位调谐以及Al-MoTe-Al结中的约瑟夫森超电流

Phase tuning of multiple Andreev reflections of Dirac fermions and the Josephson supercurrent in Al-MoTe-Al junctions.

作者信息

Zhu Zheyi, Kim Stephan, Lei Shiming, Schoop Leslie M, Cava R J, Ong N P

机构信息

Department of Physics, Princeton University, Princeton, NJ 08544.

Department of Electrical and Computer Engineering, Princeton University, Princeton, NJ 08544.

出版信息

Proc Natl Acad Sci U S A. 2022 Jul 12;119(28):e2204468119. doi: 10.1073/pnas.2204468119. Epub 2022 Jul 8.

DOI:10.1073/pnas.2204468119
PMID:35867759
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9282224/
Abstract

When an electron is incident on a superconductor from a metal, it is reflected as a hole in a process called Andreev reflection. If the metal is sandwiched between two superconductors in an junction, multiple Andreev reflections (MARs) occur. We have found that, in junctions with high transparency ([Formula: see text]) based on the Dirac semimetal MoTe, the MAR features are observed with exceptional resolution. By tuning the phase difference [Formula: see text] between the bracketing Al superconductors, we establish that the MARs coexist with a Josephson supercurrent [Formula: see text]. As we vary the junction voltage , the supercurrent amplitude [Formula: see text] varies in step with the MAR order , revealing a direct relation between them. Two successive Andreev reflections serve to shuttle a Cooper pair across the junction. If the pair is shuttled coherently, it contributes to [Formula: see text]. The experiment measures the fraction of pairs shuttled coherently vs. . Surprisingly, superconductivity in MoTe does not affect the MAR features.

摘要

当一个电子从金属入射到超导体上时,在一个称为安德列夫反射的过程中它会被反射为一个空穴。如果该金属夹在一个结中的两个超导体之间,就会发生多次安德列夫反射(MARs)。我们发现,在基于狄拉克半金属碲化钼(MoTe)的具有高透明度([公式:见正文])的结中,能以极高的分辨率观察到MAR特征。通过调节两侧铝超导体之间的相位差[公式:见正文],我们确定MARs与约瑟夫森超电流[公式:见正文]共存。当我们改变结电压时,超电流幅度[公式:见正文]随MAR阶数同步变化,揭示了它们之间的直接关系。两次连续的安德列夫反射用于将一个库珀对穿过结。如果该对是相干传输的,它会对[公式:见正文]有贡献。该实验测量了相干传输的对的比例与[具体变量]的关系。令人惊讶的是,碲化钼中的超导性并不影响MAR特征。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9ddd/9282224/a2dd7d2882e8/pnas.2204468119fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9ddd/9282224/ad9721bbb1b1/pnas.2204468119fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9ddd/9282224/1a3fb169c652/pnas.2204468119fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9ddd/9282224/6305f9b4e4ff/pnas.2204468119fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9ddd/9282224/a2dd7d2882e8/pnas.2204468119fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9ddd/9282224/ad9721bbb1b1/pnas.2204468119fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9ddd/9282224/1a3fb169c652/pnas.2204468119fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9ddd/9282224/6305f9b4e4ff/pnas.2204468119fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9ddd/9282224/a2dd7d2882e8/pnas.2204468119fig04.jpg

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