Dynamical competition between Quantum Hall and Quantum Spin Hall effects

TL;DR

This paper explores how circularly polarized light induces a transition from quantum spin Hall to quantum Hall phases in graphene with spin-orbit coupling, revealing new topological phases and photon resonance effects.

Contribution

It introduces a dynamical model combining spin-orbit coupling and light to study topological phase transitions in graphene, highlighting photon resonance-induced gaps and phase changes.

Findings

Photon resonances create additional spectral gaps at ω/2.

Increasing light intensity causes a transition from quantum spin Hall to quantum Hall phase.

Spectrum exhibits non-trivial gaps at zero energy and ω/2.

Abstract

In this paper we investigate the occurrence of quantum phase transitions in topological systems out of equi- librium. More specifically, we consider graphene with a sizable spin-orbit coupling, irradiated by circularly- polarized light. In the absence of light, the spin-orbit coupling drives a quantum spin Hall phase where edge currents with opposite spins counter-propagate. On the other hand, the light generates a time-dependent vector potential, which leads to a hopping parameter with staggered time-dependent phases around the benzene ring. The model is a dynamical version of the Haldane model, which considers a static staggered flux with zero total flux through each plaquette. Since the light breaks time-reversal symmetry, a quantum Hall phase protected by an integer topological invariant arises. By numerically solving the complete problem, with spin-orbit coupling and light, and investigating different values of the driving frequency {\omega}, we show that the spectrum exhibits non-trivial gaps not only at zero energy, but also at {\omega}/2. This additional gap is created by photon resonances between the valence and conduction band of graphene, and the symmetry of the spectrum forces it to lie at {\omega}/2. By increasing the intensity of the irradiation, the topological state in the zero energy gap undergoes a dynamical phase transition from a quantum spin Hall to a quantum Hall phase, whereas the gap around {\omega}/2 remains in the quantum Hall regime.