Polarization jumps by breaking symmetries of two-dimensional Weyl semimetals

Abstract

The electric polarization as a bulk quantity is described by the modern theory of polarization in insulating systems and cannot be defined in conducting systems. Upon a gradual change of a parameter in the system, the polarization always varies smoothly as long as the gap remains open. In this paper, we focus on the two-dimensional Weyl semimetal, which hosts Weyl nodes protected by symmetries, and study the behavior of the polarization when a symmetry-breaking term $M$ is introduced and a gap opens. We show that there can be a jump between $M\to 0^{+}$ and $M\to 0^{-}$ limits. We find that the jump is universally described by the ``Weyl dipole" representing how the Weyl nodes with monopole charges are displaced in the reciprocal space. Our result is applicable to general two-dimensional Weyl semimetals.

8 pages, 5 figures

References in corpus (5)

• Quantum Spin Hall Effect and Topological Phase Transition in HgTe Quantum Wells
• Quantum Spin Hall Insulator State in HgTe Quantum Wells
• Photocurrents in Weyl semimetals
• Excess charges as a probe of one-dimensional topological crystalline insulating phases
• Tunable Topological Energy Bands in 2D Dialkali-Metal Monoxides

Cited by in corpus (6)

• Observation of 2D Weyl Fermion States in Epitaxial Bismuthene
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• Diverging shift current responses in the gapless limit of two-dimensional systems
• Polarization Jumps across Topological Phase Transitions in Two-dimensional Systems
• Polarization textures in crystal supercells with topological bands
• In-plane magnetization orientation driven topological phase transition in OsCl${}_3$ monolayer