Non-equilibrium Fractional Hall Response After a Topological Quench
arXiv:1608.04395 · doi:10.1103/PhysRevA.94.053604
Abstract
We theoretically study the Hall response of a lattice system following a quench where the topology of a filled band is suddenly changed. In the limit where the physics is dominated by a single Dirac cone, we find that the change in the Hall conductivity is two-thirds of the quantum of conductivity. We explore this universal behavior in the Haldane model, and discuss cold-atom experiments for its observation. Beyond linear response, the Hall effect crosses over from fractional to integer values. We investigate finite-size effects, and the role of the harmonic confinement.
Updated reference list, minor revisions
References in corpus (5)
- Measuring the Chern number of Hofstadter bands with ultracold bosonic atoms
- Topological Quantum Matter with Ultracold Gases in Optical Lattices
- An Aharonov-Bohm interferometer for determining Bloch band topology
- Out of equilibrium electrons and the Hall conductance of a Floquet topological insulator
- Raman Coupling of Zeeman Sublevels in an Alkali Bose Condensate
Cited by in corpus (7)
- Topological Euler class as a dynamical observable in optical lattices
- Fate of fractional quantum Hall states in open quantum systems: characterization of correlated topological states for the full Liouvillian
- Tracing the nonequilibrium topological state of Chern insulators
- Synthetic Hall ladder with tunable magnetic flux
- Interband coherence induced correction to Thouless pumping: possible observation in cold-atom systems
- Digital Quantum Simulation of Floquet Topological Phases with a Solid-State Quantum Simulator
- Dynamical Geometry of the Haldane Model under a Quantum Quench