Topological nodal lines and hybrid Weyl nodes in YCoC2
Yuanfeng Xu,
Yueqiang Gu,
Tiantian Zhang,
Chen Fang,
Zhong Fang,
Xian-Lei Sheng,
Hongming Weng
Affiliations
Yuanfeng Xu
Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
Yueqiang Gu
Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
Tiantian Zhang
Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
Chen Fang
Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
Zhong Fang
Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
Xian-Lei Sheng
Department of Physics, Key Laboratory of Micro-nano Measurement-Manipulation and Physics (Ministry of Education), Beihang University, Beijing 100191, China
Hongming Weng
Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
Based on first-principles calculations and effective model analysis, we propose that the noncentrosymmetric superconductor YCoC2 in normal state is a topological semimetal. In the absence of spin-orbit coupling (SOC), it can host two intersecting nodal rings protected by two mirror planes, respectively. One ring is composed of type-I nodes, where the two crossing bands have opposite slope sign in their dispersions. The other ring consists of both type-I and type-II nodes (the slope signs of the two bands are the same in certain direction). In the presence of SOC, the former nodal ring is gapped totally while the latter one evolves into ten pairs of Weyl nodes, with two of them being type-I and eight being type-II. The type-II Weyl nodes are further classified into two kinds with different velocity matrices when described in Weyl equation near the nodes. Fermi arcs from topological surface states are observed in the surface projected energy dispersions. It is notable that YCoC2 has been reported as a superconductor with a critical temperature Tc of 4.2 K. This makes it very attractive since including superconducting into a topological semimetal state might result in topological superconductivity and be used to synthesize Majorana zero modes.