安德里耶夫光谱的相位不对称性来自库珀对动量
Abhishek Banerjee1, Max Geier1, Md Ahnaf Rahman1
1Center for Quantum Devices, Niels Bohr Institute, University of Copenhagen, Universitetsparken 5, 2100 Copenhagen, Denmark.
Physical review letters
|November 24, 2023
概括
研究人员在超导体-正常-超导体连接处展示了一种新的约瑟夫森二极管效应. 这种效应显示了安德里耶夫结合状态的非互惠反应,受磁场和拓相位过渡的影响.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 超导电性 超导电性 超导电性
- 量子电子学 量子电子学
背景情况:
- 约瑟夫森二极管表现出偏差不对称性,需要打破时间逆转和反转对称性.
- 最近的研究探讨了各种超导系统中的约瑟夫森二极管效应.
研究的目的:
- 在超导体-正常-超导体 (SNS) 约瑟夫森连接处演示双约瑟夫森二极管效应.
- 为了研究磁场对安德烈耶夫结合状态的非相互反应的影响.
主要方法:
- 制造表轴性InAs/Al异构的SNS约瑟夫森连接点.
- 在变化的平面内磁场下测量亚间隙安德里耶夫光谱及其相位不对称.
主要成果:
- 观察到安德里耶夫结合状态的非互惠反应,这是通常的约瑟夫森二极管效应的双重反应.
- 在没有磁场的情况下,相位不对称性是不存在的,在0.15 T横向场时最大化.
- 二极管效应的信号逆转发生在更高的磁场上,与光谱间隙重新开放和拓相位过渡相关.
结论:
- 阶段二极管效应归因于由轨道与磁场的合诱导的有限动量库珀配对.
- 信号反转与拓相位过渡有关,涉及Zeeman和旋转轨道相互作用以及轨道合.
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