{ "id": "1601.05732", "version": "v1", "published": "2016-01-21T18:09:38.000Z", "updated": "2016-01-21T18:09:38.000Z", "title": "Occupation probabilities and current densities of bulk and edge states of a Floquet topological insulator", "authors": [ "Hossein Dehghani", "Aditi Mitra" ], "comment": "12 pages, 9 figures", "categories": [ "cond-mat.mes-hall" ], "abstract": "Results are presented for the occupation probabilities and current densities of bulk and edge states of half-filled graphene irradiated by a circularly polarized laser. It is assumed that the system is closed, and that the laser has been switched on as a quench. Laser parameters corresponding to some representative topological phases are studied: one where the Chern number of the Floquet bands equals the number of chiral edge modes, a second where anomalous edge states appear in the Floquet Brillouin zone boundaries, and a third where the Chern number is zero, yet topological edge states appear at the center and boundaries of the Floquet Brillouin zone. For an ideal half-filled system where only one of the bands in the Floquet Brillouin zone is occupied and the other empty, particle-hole and inversion symmetry of the Floquet Hamiltonian implies zero current density. However the laser switch-on protocol breaks the inversion symmetry, creating a nonequilibrium occupation of the Floquet bands, which results in a net current density at steady-state. A study of how the current density is distributed among the edge and bulk states is presented, and qualitative differences are found for the high frequency off-resonant and low frequency on-resonant laser.", "revisions": [ { "version": "v1", "updated": "2016-01-21T18:09:38.000Z" } ], "analyses": { "keywords": [ "floquet topological insulator", "occupation probabilities", "floquet brillouin zone", "implies zero current density", "hamiltonian implies zero current" ], "note": { "typesetting": "TeX", "pages": 12, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2016arXiv160105732D" } } }