Microscopic theory for the light-induced anomalous Hall effect in graphene
arXiv:1905.04508 · doi:10.1103/PhysRevB.99.214302
Abstract
We employ a quantum Liouville equation with relaxation to model the recently observed anomalous Hall effect in graphene irradiated by an ultrafast pulse of circularly polarized light. In the weak-field regime, we demonstrate that the Hall effect originates from an asymmetric population of photocarriers in the Dirac bands. By contrast, in the strong-field regime, the system is driven into a non-equilibrium steady state that is well-described by topologically non-trivial Floquet-Bloch bands. Here, the anomalous Hall current originates from the combination of a population imbalance in these dressed bands together with a smaller anomalous velocity contribution arising from their Berry curvature. This robust and general finding enables the simulation of electrical transport from light-induced Floquet-Bloch bands in an experimentally relevant parameter regime and creates a pathway to designing ultrafast quantum devices with Floquet-engineered transport properties.
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Cited by in corpus (7)
- Cavity Quantum-Electrodynamical Chern Insulator: Route Towards Light-Induced Quantized Anomalous Hall Effect in Graphene
- Floquet engineering of twisted double bilayer graphene
- Light-induced bound electron states in two-dimensional systems: Contribution to electron transport
- Robustness of quantized transport through edge states of finite length: Imaging current density in Floquet topological vs. quantum spin and anomalous Hall insulators
- Quantum Hall effective action for anisotropic Dirac semi-metal
- Floquet boundary states in AB-stacked graphite
- Photovoltaic Effect from the Viewpoint of Time-reversal Symmetry