Abstract

Topological insulators (TIs) are considered as ideal platforms for generating large spin Hall conductivity (SHC), however, the bulk carrier problem, which is unavoidable in TIs, hinders their practical applications. Recently, topological semimetals (TSMs) have been proposed to achieve large SHC to replace TIs. However, the ideal TSM candidates with large SHC are still lacking. In terms of first-principles calculations, we predict that Ta3As family compounds exhibit complex crossing nodal-lines (CNL) properties in absence of the spin-orbit coupling (SOC). However, they transfer to Dirac TSMs under the influence of strong SOC, and present large SHC around Fermi level in particular. Remarkably, the SHC value of Ta3Y (Y = As, Sb, Bi) is around 1500–1700 (hbar /e)({mathrm{{Omega}}} cdot {mathrm{cm}})^{ - 1}, which is comparable to noble metal Pt and much larger than TIs, Weyl TSMs, and 4d/5d transition metals. Our work not only suggests a kind of TSM family with interesting Dirac CNL around Fermi level, but also paves the way for searching large intrinsic SHC materials in complex CNL TSM systems.

Highlights

  • The spin Hall effect (SHE) is a phenomenon that a transverse pure spin current appears if a longitudinal electric field is applied[1,2,3,4]

  • In this article, using first-principles calculations, we propose that the X3Y (X = Ta, Nb; Y = As, Sb, Bi) compounds are a family of CNL semimetals (CNLSMs)

  • Previous studies mainly focused on the Ta3Y compounds with the Ti3P-type (A15 phase, space group 223) structure[34,35], instead of the Pm3m phase

Read more

Summary

Introduction

The spin Hall effect (SHE) is a phenomenon that a transverse pure spin current appears if a longitudinal electric field is applied[1,2,3,4]. The SHC is around 1500 ðh=eÞðΩ Á cmÞÀ1 in stable Ta3As compound, which is attributed to its large SOC band splitting.

Results
Conclusion

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

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.