Cortés-Del Río Eva, Lado Jose Luis, Cherkez Vladimir, Mallet Pierre, Veuillen Jean-Yves, Cuevas Juan Carlos, Gómez-Rodríguez José María, Fernández-Rossier Joaquín, Brihuega Iván
Departamento Física de la Materia Condensada, Universidad Autónoma de Madrid, Madrid, E-28049, Spain.
Department of Applied Physics, Aalto University, Espoo, 02150, Finland.
Adv Mater. 2021 Jun;33(22):e2008113. doi: 10.1002/adma.202008113. Epub 2021 Apr 23.
When magnetic atoms are inserted inside a superconductor, the superconducting order is locally depleted as a result of the antagonistic nature of magnetism and superconductivity. Thereby, distinctive spectral features, known as Yu-Shiba-Rusinov states, appear inside the superconducting gap. The search for Yu-Shiba-Rusinov states in different materials is intense, as they can be used as building blocks to promote Majorana modes suitable for topological quantum computing. Here, the first observation of Yu-Shiba-Rusinov states in graphene, a non-superconducting 2D material, and without the participation of magnetic atoms, is reported. Superconductivity in graphene is induced by proximity effect brought by adsorbing nanometer-scale superconducting Pb islands. Using scanning tunneling microscopy and spectroscopy the superconducting proximity gap is measured in graphene, and Yu-Shiba-Rusinov states are visualized in graphene grain boundaries. The results reveal the very special nature of those Yu-Shiba-Rusinov states, which extends more than 20 nm away from the grain boundaries. These observations provide the long-sought experimental confirmation that graphene grain boundaries host local magnetic moments and constitute the first observation of Yu-Shiba-Rusinov states in a chemically pure system.
当磁性原子被插入到超导体内部时,由于磁性与超导性的对抗特性,超导序会在局部被耗尽。由此,被称为汤浅-芝-鲁西诺夫态(Yu-Shiba-Rusinov states)的独特光谱特征出现在超导能隙内。对不同材料中汤浅-芝-鲁西诺夫态的探索十分热烈,因为它们可被用作构建块来促进适用于拓扑量子计算的马约拉纳模式。在此,报道了在石墨烯(一种非超导二维材料)中首次观察到汤浅-芝-鲁西诺夫态,且该观察未涉及磁性原子的参与。石墨烯中的超导性是由吸附纳米尺度的超导铅岛所带来的近邻效应诱导产生的。利用扫描隧道显微镜和能谱技术,在石墨烯中测量了超导近邻能隙,并在石墨烯晶界处观察到了汤浅-芝-鲁西诺夫态。结果揭示了那些汤浅-芝-鲁西诺夫态的非常特殊的性质,它们从晶界延伸超过20纳米。这些观察结果提供了长期以来寻求的实验证实,即石墨烯晶界存在局部磁矩,并构成了在化学纯系统中首次观察到汤浅-芝-鲁西诺夫态。