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arXiv 2005.11848cond-mat.mes-hallcond-mat.supr-con
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拓扑约瑟夫森结中的量子点宇称效应

Quantum-Dot Parity Effects in Trivial and Topological Josephson Junctions

D. Razmadze, E. C. T. O'Farrell, P. Krogstrup, C. M. Marcus

摘要:

约瑟夫森结中的奇占据量子点可以翻转传输相位,产生π结。当结耦合拓扑超导体时,预期没有相位翻转。我们在一个全壳层混合干涉仪中研究了这一点和相关的影响,使用栅极电压来控制点结宇称和轴向磁通量来控制从平凡到拓扑超导的过渡。增强的零偏压电导和奇宇称的拓扑相位的临界电流反映了杂交的限制自旋与零能量模式的领导。

英文摘要:

An odd-occupied quantum dot in a Josephson junction can flip transmission phase, creating a π-junction. When the junction couples topological superconductors, no phase flip is expected. We investigate this and related effects in a full-shell hybrid interferometer, using gate voltage to control dot-junction parity and axial magnetic flux to control the transition from trivial to topological superconductivity. Enhanced zero-bias conductance and critical current for odd parity in the topological phase reflects hybridization of the confined spin with zero-energy modes in the leads.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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