Floquet topological phase transition in - lattice
arXiv:1901.10778 · doi:10.1103/PhysRevB.99.205429
Abstract
We investigate topological characteristics of the photon-dressed band structure of - lattice on being driven by off-resonant circularly polarized radiation. We obtain exact analytical expressions of the quasienergy bands over the first Brillouin zone. The broken time-reversal symmetry caused by the circularly polarized light lifts the triple point degeneracy completely at both the Dirac points. The gaps become unequal at and (except at and 1), which reveals the absence of inversion symmetry in the system. At , the gap between flat and valence bands closes at , while that between conduction and flat bands closes at , thereby restoring a semimetalic phase. At the gap closing point () which is independent of the radiation amplitude, there is a reappearance of low-energy Dirac cones around and points. Under the influence of the circularly polarized radiation, the - lattice is transformed from semimetal to a Haldane-like Chern insulator characterized by non-zero Chern number. The system undergoes a topological phase transition from to at , where is the Chern number of the valence (conduction) band. This sets an example of a multiband system having larger Chern number. These results are supported by the appearance of chiral edge states in irradiated - nanoribbon.
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