We investigate an unconventional topological phase transition that occurs in quantum spin Hall (QSH) systems when applying an external in-plane magnetic field. We show that this transition between QSH and trivial insulator phases is separated by a stable topological gapless phase, which is protected by the combination of particle-hole and reflection symmetries, and thus, we dub it as crystalline Weyl semimetal. We explore the stability of this new phase when particle-hole symmetry breaking terms are present. Especially, we predict a robust unconventional topological phase transition to be visible for materials described by Kane and Mele model even if particle-hole symmetry is significantly broken.
Cited by 1
Guo et al., Zeeman Field-Induced Two-Dimensional Weyl Semimetal Phase in Cadmium Arsenide
Phys. Rev. Lett. 131, 046601 (2023) [Crossref]
Authors / Affiliations: mappings to Contributors and OrganizationsSee all Organizations.
- 1 2 Fernando Dominguez,
- 1 2 Benedikt Scharf,
- 1 2 Ewelina Hankiewicz
- 1 Julius-Maximilians-Universität Würzburg / University of Würzburg
- 2 Würzburg-Dresden Cluster of Excellence [ct.qmat]