在Nb3Cl8中的效率调节的无场约瑟夫森二极管效应 基于范德瓦尔斯交叉点
Si Li Wu1,2, Zhi-Hui Ren1,2, Liu Yang1,2
1Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing 100081, China.
Nano letters
|December 12, 2025
概括
我们在范德瓦尔斯异构结构中演示了一个可调节的无磁场的约瑟夫森二极管效应 (JDE). 调节屏障厚度和电场通过调节内在电极化来控制二极管效率.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
- 量子设备 量子设备
背景情况:
- 约瑟夫森二极管效应 (JDE) 允许超导器件中的非反向电流流.
- 了解无现场JDE的微观起源和控制机制对于设备应用至关重要.
- 范德瓦尔斯 (vdW) 的异构结构提供可调节的电子特性.
研究的目的:
- 展示和控制一个可调节的,无磁场的约瑟夫森二极管效应 (JDE).
- 为了研究内在电极化在无电场JDE中的作用.
- 探索VDW异构结构对于非互通超导装置的潜力.
主要方法:
- 制造具有不同屏障厚度的NbSe2/Nb3Cl8/NbSe2 vdW约瑟夫森接口.
- 电传输测量以表征约瑟夫森二极管效应.
- 应用平面外电场来调节节点特性.
主要成果:
- 通过降低Nb3Cl8屏障厚度 (1.75%至20.88%) 显著提高无现场JDE效率.
- 可调节的二极管效率通过外平面电场,表明内在的电极化.
- 极化强度,屏障厚度和JDE的电场调制之间的相关性.
结论:
- 本质的电极化是实现可调节的关键,在VDW异构结构中实现无场的JDE.
- 这些结点的JDE对自发的时间逆转对称性破坏敏感.
- 这项工作为设计先进的非互惠超导装置提供了一条途径.
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