Occupation probabilities and current densities of bulk and edge states of a Floquet topological insulator

TL;DR

This paper investigates the occupation probabilities and current densities of bulk and edge states in a Floquet topological insulator modeled by irradiated graphene, revealing how different topological phases and laser parameters influence these properties.

Contribution

It provides a detailed analysis of occupation and current density profiles in various Floquet topological phases of irradiated graphene, highlighting the effects of laser frequency and symmetry breaking.

Findings

Edge states depend on laser frequency and topological phase.

Resonant processes lead to high effective temperature occupation of edge states.

Inversion symmetry breaking causes a net current density and charge imbalance.

Abstract

Results are presented for the occupation probabilities and current densities of bulk and edge states of half-filled graphene in a cylindrical geometry, and 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. Qualitative differences are found for the high frequency off-resonant and low frequency on-resonant laser with edge states arising due to resonant processes occupied with a high effective temperature on the one hand, while edge states arising due to off-resonant processes occupied with a low effective temperature on the other. 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, resulting in a net cylindrical sheet of current density at steady-state. Due to the underlying chirality of the system, this current density profile is associated with a net charge imbalance between the top and bottom of the cylinders.