Tunable topologically driven Fermi arc van Hove singularities

物理 螺旋面 范霍夫奇点 拓扑(电路) 费米面 引力奇点 凝聚态物理 电荷密度波 态密度 费米能级 电子 量子力学 几何学 超导电性 数学 组合数学
作者
Daniel S. Sanchez,Tyler A. Cochran,Ilya Belopolski,Zi‐Jia Cheng,Xiàn Yáng,Yiyuan Liu,Tao Hou,Xitong Xu,Kaustuv Manna,Chandra Shekhar,Jia‐Xin Yin,Horst Borrmann,Alla Chikina,Jonathan D. Denlinger,Vladimir N. Strocov,Weiwei Xie,Claudia Felser,Shuang Jia,Guoqing Chang,M. Zahid Hasan
出处
期刊:Nature Physics [Nature Portfolio]
卷期号:19 (5): 682-688 被引量:11
标识
DOI:10.1038/s41567-022-01892-6
摘要

The classification scheme of electronic phases uses two prominent paradigms: correlations and topology. Electron correlations give rise to superconductivity and charge density waves, while the quantum geometric Berry phase gives rise to electronic topology. The intersection of these two paradigms has initiated an effort to discover electronic instabilities at or near the Fermi level of topological materials. Here we identify the electronic topology of chiral fermions as the driving mechanism for creating van Hove singularities that host electronic instabilities in the surface band structure. We observe that the chiral fermion conductors RhSi and CoSi possess two types of helicoid arc van Hove singularities that we call type I and type II. In RhSi, the type I variety drives a switching of the connectivity of the helicoid arcs at different energies. In CoSi, we measure a type II intra-helicoid arc van Hove singularity near the Fermi level. Chemical engineering methods are able to tune the energy of these singularities. Finally, electronic susceptibility calculations allow us to visualize the dominant Fermi surface nesting vectors of the helicoid arc singularities, consistent with recent observations of surface charge density wave ordering in CoSi. This suggests a connection between helicoid arc singularities and surface charge density waves. Strong correlations between electrons in topological surface states drive the formation of surface van Hove singularities. These may be linked to charge density waves in the surface states.
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