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拓扑半金属中库珀对动量产生的约瑟夫森二极管效应。

Josephson diode effect from Cooper pair momentum in a topological semimetal.

作者信息

Pal Banabir, Chakraborty Anirban, Sivakumar Pranava K, Davydova Margarita, Gopi Ajesh K, Pandeya Avanindra K, Krieger Jonas A, Zhang Yang, Date Mihir, Ju Sailong, Yuan Noah, Schröter Niels B M, Fu Liang, Parkin Stuart S P

机构信息

Max Planck Institute of Microstructure Physics, Halle (Saale), Germany.

Department of Physics, Massachusetts Institute of Technology, Cambridge, MA USA.

出版信息

Nat Phys. 2022;18(10):1228-1233. doi: 10.1038/s41567-022-01699-5. Epub 2022 Aug 15.

DOI:10.1038/s41567-022-01699-5
PMID:36217362
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9537108/
Abstract

Cooper pairs in non-centrosymmetric superconductors can acquire finite centre-of-mass momentum in the presence of an external magnetic field. Recent theory predicts that such finite-momentum pairing can lead to an asymmetric critical current, where a dissipationless supercurrent can flow along one direction but not in the opposite one. Here we report the discovery of a giant Josephson diode effect in Josephson junctions formed from a type-II Dirac semimetal, NiTe. A distinguishing feature is that the asymmetry in the critical current depends sensitively on the magnitude and direction of an applied magnetic field and achieves its maximum value when the magnetic field is perpendicular to the current and is of the order of just 10 mT. Moreover, the asymmetry changes sign several times with an increasing field. These characteristic features are accounted for by a model based on finite-momentum Cooper pairing that largely originates from the Zeeman shift of spin-helical topological surface states. The finite pairing momentum is further established, and its value determined, from the evolution of the interference pattern under an in-plane magnetic field. The observed giant magnitude of the asymmetry in critical current and the clear exposition of its underlying mechanism paves the way to build novel superconducting computing devices using the Josephson diode effect.

摘要

在存在外部磁场的情况下,非中心对称超导体中的库珀对可以获得有限的质心动量。最近的理论预测,这种有限动量配对会导致不对称的临界电流,即无耗散超电流可以沿一个方向流动,但不能沿相反方向流动。在此,我们报告了在由II型狄拉克半金属NiTe形成的约瑟夫森结中发现的巨大约瑟夫森二极管效应。一个显著特征是临界电流的不对称性敏感地取决于外加磁场的大小和方向,当磁场垂直于电流且仅为10 mT量级时达到最大值。此外,随着磁场增加,不对称性会多次改变符号。这些特征由基于有限动量库珀配对的模型解释,该配对主要源于自旋螺旋拓扑表面态的塞曼位移。通过面内磁场下干涉图案的演变,进一步确定了有限配对动量及其值。所观察到的临界电流不对称性的巨大幅度及其潜在机制的清晰阐述,为利用约瑟夫森二极管效应构建新型超导计算设备铺平了道路。

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本文引用的文献

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Universal Josephson diode effect.通用约瑟夫森二极管效应。
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