6533b855fe1ef96bd12b144e
RESEARCH PRODUCT
Microscopic theory for the light-induced anomalous Hall effect in graphene
Andrea CavalleriMichael A. SentefShunsuke A. SatoShunsuke A. SatoMarlon NuskeLudwig MatheyGregor JotzuHannes HübenerJames MciverU. De GiovanniniB. SchultePeizhe TangAngel Rubiosubject
Dirac (software)PopulationFOS: Physical sciences02 engineering and technology01 natural sciencesSettore FIS/03 - Fisica Della Materialaw.inventionlawHall effect0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)010306 general physicseducationQuantumPhysicseducation.field_of_studyCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsGrapheneRelaxation (NMR)dissipation021001 nanoscience & nanotechnologyCondensed Matter::Mesoscopic Systems and Quantum Hall EffectFloquet topologyBerry connection and curvatureMicroscopic theory0210 nano-technologyPhysics - OpticsOptics (physics.optics)description
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.
year | journal | country | edition | language |
---|---|---|---|---|
2019-05-11 | Physical Review B |