Interlayer Coupling and Floquet-Driven Topological Phases in Bilayer Haldane Lattices

TL;DR

This paper explores how Floquet driving and interlayer coupling in bilayer Haldane lattices induce and control various topological phases, including higher-Chern states, through tunable parameters and band structure engineering.

Contribution

It introduces a comprehensive analysis of Floquet-induced topological phase transitions in bilayer Haldane systems with tunable anisotropy and interlayer coupling, revealing new pathways for topological control.

Findings

Controlled transitions among Dirac, semi-Dirac, and higher-Chern phases.

Interlayer coupling induces valley-selective band inversions.

Higher-Chern phases stabilized by helicity-dependent band inversions.

Abstract

We investigate Floquet-driven topological phase transitions in an AB-stacked bilayer Haldane lattice with tunable intralayer hopping anisotropy. By combining interlayer hybridization, Haldane flux, and off-resonant circularly polarized light, we obtain controlled transitions among Dirac, semi-Dirac, and higher-Chern insulating phases. As the hopping anisotropy increases, the two inequivalent Dirac points move toward each other and merge at the Brillouin-zone $\mathbf{M}$ point, where a semi-Dirac dispersion emerges with linear and quadratic momentum dependence along orthogonal directions. In this regime, competition between the intrinsic Haldane mass and the Floquet-induced mass drives a sequence of sharp topological transitions with Chern numbers $C=0,\pm1,\pm2$. We further show that interlayer coupling qualitatively reshapes the Floquet band topology by inducing helicity-dependent and valley-selective band inversions at the K and K$'$ points, thereby stabilizing higher-Chern phases in the valence bands. These changes are accompanied by redistribution of the Berry curvature, bulk gap closings, and the collapse or sign reversal of quantized anomalous Hall plateaus. As the system approaches the semi-Dirac limit, the topological phase space narrows and disappears at the critical merger point, beyond which the system becomes topologically trivial even when it remains gapped. Overall, the bilayer geometry broadens the scope of Floquet topological control by enabling dynamically tunable higher-Chern phases and valley-dependent Hall responses governed by interlayer coupling and light helicity.