Abstract

Using ab initio calculations based on density-functional theory and effective model analysis, we propose that the trigonal YH3 (Space Group: Pbar{{bf{3}}}c1) at ambient pressure is a node-line semimetal when spin-orbit coupling (SOC) is ignored. This trigonal YH3 has very clean electronic structure near Fermi level and its nodal lines locate very closely to the Fermi energy, which makes it a perfect system for model analysis. Symmetry analysis shows that the nodal ring in this compound is protected by the glide-plane symmetry, where the band inversion of |Y+, dxz〉 and |H1−, s〉 orbits at Γ point is responsible for the formation of the nodal lines. When SOC is included, the line nodes are prohibited by the glide-plane symmetry, and a small gap (≈5 meV) appears, which leads YH3 to be a strong topological insulator with Z2 indices (1,000). Thus the glide-plane symmetry plays an opposite role in the formation of the nodal lines in cases without and with SOC. As the SOC-induced gap is so small that can be neglected, this Pbar{{bf{3}}}c1 YH3 may be a good candidate for experimental explorations on the fundamental physics of topological node-line semimetals. We find the surface states of this Pbar{{bf{3}}}c1 phase are somehow unique and may be helpful to identify the real ground state of YH3 in the experiment.

Highlights

  • Topological semimetals (TSMs) have attracted great attention for both theoretical interests and experimental applications in recent years

  • Symmetries are important in classifying node-line semimetals (NLSMs), for instance, three types of NLSMs protected by different symmetries have been proposed: (a) mirror symmetry protected NLSMs8,14,16,40, (b) coexistence of time-reversal symmetry (TRS) and inversion symmetry (IS) protected NLSMs11–13,32 and (c) nonsymmorphic symmetry protected NLSMs15,32

  • Two of them are experimentally favoured with trigonal P3c1 and hexagonal P63cm symmetry[66,67,68,69,70,71], while the third candidate is in the space group of P63 which was predicted theoretically[72]

Read more

Summary

Methods

Calculations of the band structures are performed using the full-potential linearized augmented plane-wave (FP-LAPW) method[57,58] implemented in the WIEN2k59 package. We use 13 × 13 × 11 k-mesh for the BZ sampling and −7 for the plane wave cut-off parameter RMTKmax for the electronic structure calculation, where the RMT is the minimum muffin-tin radius and Kmax is the plane-wave vector cut-off parameter. SOC is taken into consideration by a second-variation method[60]. The tight-binding models are constructed with the maximally localized Wannier functions (MLWFs) method[61,62,63], the corresponding hopping parameters are determined from the projections of the bulk Bloch wave functions. The projected surface states are calculated using surface Green’s function in the semi-infinite system[64,65]

Results and Discussions
Bloch function
Additional Information
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call