Time-reversal symmetry breaking in a square lattice
arXiv:2009.10001 · doi:10.1088/2399-6528/abf024
Abstract
The bulk conductivity of a two-dimensional system is studied assuming that quantum interference effects break time-reversal symmetry in the presence of strong spin-orbit interaction and strong lattice potential. The study is carried out by direct diagonalization in order to explore the nonlinear-response regime. The system displays a quantized conductivity that depends on the intensity of the electric field and under specific conditions the conductivity limit at zero electric field shows a nonvanishing value.
6 pages, 5 figures, comments or suggestions are welcome
References in corpus (9)
- Quantum Spin Hall Insulator State in HgTe Quantum Wells
- Experimental Observation of the Quantum Anomalous Hall Effect in a Magnetic Topological Insulator
- Quantized Anomalous Hall Effect in Magnetic Topological Insulators
- Topological Surface States Protected From Backscattering by Chiral Spin Texture
- High-precision realization of robust quantum anomalous Hall state in a hard ferromagnetic topological insulator
- Spin-orbit coupling in quantum gases
- Trajectory of Anomalous Hall Effect toward the Quantized State in a Ferromagnetic Topological Insulator
- Quantum anomalous Hall effect and related topological electronic states
- Thermodynamic signatures of an underlying quantum phase transition: A grand canonical approach