Strain-tunable topological quantum phase transition in buckled honeycomb lattices

Abstract

Low-buckled silicene is a prototypical quantum spin Hall insulator with the topological quantum phase transition controlled by an out-of-plane electric field. We show that this field-induced electronic transition can be further tuned by an in-plane hydrostatic biaxial strain $\epsilon$, owing to the curvature-dependent spin-orbit coupling (SOC): There is a $Z_2$ = 1 topological insulator phase for biaxial strain $|\epsilon |$ smaller than 0.07, and the band gap can be tuned from 0.7 meV for $\epsilon =+0.07$ up to a fourfold 3.0 meV for $\epsilon =-0.07$. First-principles calculations also show that the critical field strength $E_c$ can be tuned by more than 113\%, with the absolute values nearly 10 times stronger than the theoretical predictions based on a tight-binding model. The buckling structure of the honeycomb lattice thus enhances the tunability of both the quantum phase transition and the SOC-induced band gap, which are crucial for the design of topological field-effect transistors based on two-dimensional materials.

arXiv comment5 pages, 4 figures

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Cited by in corpus (5)

• Electronic and optical properties of strained graphene and other strained 2D materials: a review
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• Electronic and optical conductivity of kekulé-patterned graphene: Intravalley and intervalley transport
• Controlling plasmon modes and damping in buckled two-dimensional material open systems
• Antiferromagnetic Chern insulator with large charge gap in heavy transition-metal compounds