J=32电子超导体的约瑟夫森效应

Dakyeong Kim, S. Kobayashi, Y. Asano
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引用次数: 3

摘要

在强自旋-轨道相互作用下,电子的角动量可以用$J=3/2$的赝自旋来表征。我们从理论上研究了超导体的约瑟夫森效应,其中这两个$J=3/2$电子形成一个库珀对。在偶宇称对称类中,可以存在$J=2$的伪自旋-五重配对态和$J=0$的伪自旋-单重态。我们特别关注这些偶宇称超导体中的约瑟夫森选择规则。我们发现五重态之间的选择规则比两个$S=1/2$电子形成的自旋三重态之间的选择规则更严格。讨论了伪自旋活性界面对选择规则的影响,以及由伪自旋相关带结构产生的奇频库珀对的影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Josephson effect of superconductors with J=32 electrons
The angular momentum of an electron is characterized well by pseudospin with $J=3/2$ in the presence of strong spin-orbit interactions. We study theoretically the Josephson effect of superconductors in which such two $J=3/2$ electrons form a Cooper pair. Within even-parity symmetry class, pseudospin-quintet pairing states with $J=2$ can exist as well as pseudospin-singlet state with $J=0$. We focus especially on the Josephson selection rule among these even-parity superconductors. We find that the selection rule between quintet states is severer than that between spin-triplet states formed by two $S=1/2$ electrons. The effects of a pseudospin-active interface on the selection rule are discussed as well as those of odd-frequency Cooper pairs generated by pseudospin dependent band structures.
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