Symmetry conditions of a nodal superconductor for generating robust flat-band Andreev bound states at its dirty surface

被引:8
|
作者
Ikegaya, Satoshi [1 ]
Kobayashi, Shingo [2 ,3 ]
Asano, Yasuhiro [1 ,4 ,5 ]
机构
[1] Hokkaido Univ, Dept Appl Phys, Sapporo, Hokkaido 0608628, Japan
[2] Nagoya Univ, Dept Appl Phys, Nagoya, Aichi 4648603, Japan
[3] Nagoya Univ, Inst Adv Res, Nagoya, Aichi 4648601, Japan
[4] Hokkaido Univ, Ctr Topol Sci & Technol, Sapporo, Hokkaido 0608628, Japan
[5] Moscow Inst Phys & Technol, Dolgoprudnyi 141700, Russia
基金
日本科学技术振兴机构; 日本学术振兴会;
关键词
D-WAVE SUPERCONDUCTORS; HIGH-TEMPERATURE SUPERCONDUCTORS; TOPOLOGICAL INSULATORS; P-WAVE;
D O I
10.1103/PhysRevB.97.174501
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We discuss the symmetry property of a nodal superconductor that hosts robust flat-band zero-energy states at its surface under potential disorder. Such robust zero-energy states are known to induce the anomalous proximity effect in a dirty normal metal attached to a superconductor. A recent study has shown that a topological index N-ZES describes the number of zero-energy states at the dirty surface of a p-wave superconductor. We generalize the theory to clarify the conditions required for a superconductor that enables N-ZES not equal 0. Our results show that N-ZES not equal 0 is realized in a topological material that belongs to either the BDI or CII class. We also present two realistic Hamiltonians that result in N-ZES not equal 0.
引用
收藏
页数:9
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