Hierarchy of Floquet gaps and edge states for driven honeycomb lattices

TL;DR

This paper explores the complex hierarchy of Floquet gaps and edge states in driven honeycomb lattices across different frequencies and intensities, combining analytical and numerical methods to classify topological phases.

Contribution

It introduces a hierarchical classification of Floquet gaps and edge states in driven honeycomb lattices, using effective Hamiltonians and topological invariants for different driving regimes.

Findings

Hierarchy of Floquet edge states resembles a nesting doll.

Effective Hamiltonians reveal the topological character of gaps.

Numerical calculations map topological phase transitions.

Abstract

Electromagnetic driving in a honeycomb lattice can induce gaps and topological edge states with a structure of increasing complexity as the frequency of the driving lowers. While the high frequency case is the most simple to analyze we focus on the multiple photon processes allowed in the low frequency regime to unveil the hierarchy of Floquet edge-states. In the case of low intensities an analytical approach allows us to derive effective Hamiltonians and address the topological character of each gap in a constructive manner. At high intensities we obtain the net number of edge states, given by the winding number, with a numerical calculation of the Chern numbers of each Floquet band. Using these methods, we find a hierarchy that resembles that of a Russian nesting doll. This hierarchy classifies the gaps and the associated edge states in different orders according to the electron-photon coupling strength. For large driving intensities, we rely on the numerical calculation of the winding number, illustrated in a map of topological phase transitions. The hierarchy unveiled with the low energy effective Hamiltonians, alongside with the map of topological phase transitions discloses the complexity of the Floquet band structure in the low frequency regime. The proposed method for obtaining the effective Hamiltonian can be easily adapted to other Dirac Hamiltonians of two dimensional materials and even the surface of a 3D topological insulator.