欠阻尼偏置电流拓扑约瑟夫森结绝缘状态的临界电流

A. Svetogorov, D. Loss, J. Klinovaja
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引用次数: 3

摘要

本文分析研究了欠阻尼电流偏置拓扑约瑟夫森结。首先,我们考虑了一个在零温度下的简化模型,其中由结上的马约兰纳束缚态(mbs)形成的非局域费米子态的宇称是固定的,并表明与非拓扑约瑟夫森结相比,在这种情况下,从绝缘到导电状态的转变是由单准粒子隧穿而不是库珀对隧穿控制的。这导致从绝缘到导电状态转变的临界电流显著降低。我们提出,如果系统的长度是有限的,从绝缘状态到导电状态的转变发生在指数级高的偏置电流下,这是由于位于结上的mbs和形成结的拓扑纳米线边缘的重叠导致具有不同对偶的状态的杂化。最后,我们讨论了如何通过测量不同外加磁场值下绝缘状态的临界电流来实验确定mbs的外观。
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Critical current for an insulating regime of an underdamped current-biased topological Josephson junction
We study analytically an underdamped current-biased topological Josephson junction. First, we consider a simplified model at zero temperature, where the parity of the non-local fermionic state formed by Majorana bound states (MBSs) localized on the junction is fixed, and show that a transition from insulating to conducting state in this case is governed by single-quasiparticle tunneling rather than by Cooper pair tunneling in contrast to a non-topological Josephson junction. This results in a significantly lower critical current for the transition from insulating to conducting state. We propose that, if the length of the system is finite, the transition from insulating to conducting state occurs at exponentially higher bias current due to hybridization of the states with different parities as a result of the overlap of MBSs localized on the junction and at the edges of the topological nanowire forming the junction. Finally, we discuss how the appearance of MBSs can be established experimentally by measuring the critical current for an insulating regime at different values of the applied magnetic field.
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