Dynamical Quantum Anomalous Hall Effect in Strong Optical Fields
arXiv:1703.00510 · doi:10.1103/PhysRevB.95.201411
Abstract
Topological insulators (TIs) are characterized by the quantum anomalous Hall effect (QAHE) on the topological surface states under time-reversal symmetry breaking. Motivated by recent experiments on the magneto-optical effects induced by the QAHE, we develop a theory for the dynamical Hall conductivity for subgap optical frequency and intense optical fields using the Keldysh-Floquet Green's function formalism. Our theory reveals a nonlinear regime in which the Hall conductivity remains close to at low frequencies. At higher optical fields, we find that the subsequent collapse of the half quantization is accompanied by coherent oscillations of the dynamical Hall conductivity as a function of field strength, triggered by the formation of Floquet subbands and the concomitant inter-subband transitions.
6 pages, 3 figures
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Cited by in corpus (12)
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- Photocontrol of magnetic structure in an itinerant magnet
- High-frequency breakdown of the integer QHE in GaAs/AlGaAs heterojunctions
- Photon-Induced Suppression of Interlayer Tunneling in Van Der Waals Heterostructures
- Impurity Screening and Friedel Oscillations in Floquet-driven Two-dimensional Metals
- Finite-Size Effects in the Dynamic Conductivity and Faraday Effect of Quantum Anomalous Hall Insulators
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- Photo-induced Non-collinear Interlayer RKKY Coupling in Bulk Rashba Semiconductors