Topological phase transitions in Chern insulators within three-band models

TL;DR

This paper studies topological phase transitions in three-band Chern insulators on Lieb and kagome lattices, revealing how hopping parameters and interactions induce changes in topological invariants and fractional Chern insulator phases, with stable transitions confirmed in large systems.

Contribution

It demonstrates the occurrence of topological phase transitions driven by hopping and interactions in three-band models, analyzing entanglement spectra and entropy to characterize phases and transitions.

Findings

Chern number changes from 1 to -1 at phase transition

Fractional Chern insulator phases identified at 1/3 filling

Energy gap closure and entanglement entropy discontinuity at transitions

Abstract

We investigate topological phase transitions in Chern insulators within three-band models, focusing on the empty band and lowest band populated by spinless fermions. We consider Lieb and kagome lattices and notice phase transitions driven by the hopping integral between nearest-neighbors, which leads to the change of the lowest band Chern number from $C=1$ to $C=-1$. In the single-particle picture, different phases are examined by investigating corresponding entanglement spectra and the evolution of the entanglement entropy. Entanglement spectra reveal the spectral flow characteristic of topologically nontrivial systems before and after phase transitions. For the lowest band with $1/3$ filling, Fractional Chern insulator (FCI) phases are identified by examining the ground state momenta, the spectral flow, and counting of the entanglement energy levels below the gap in the entanglement spectrum. A quasilinear dependence of the entanglement entropy $\alpha(n_A)$ term is observed for FCI phase, similarly to linear behavior expected for Laughlin phase in the fractional quantum Hall effect. At the topological phase transition, for both empty and partially filled lowest bands, the energy gap closure and a discontinuity in the entanglement entropy are observed. This coincides with the divergence of a standard deviation of the Berry curvature. We notice also a phase transition driven by the nearest-neighbor interaction in the Lieb lattice, where the many-body energy gap closes. The phase transitions are shown to be stable for an arbitrary system size, thus predicted to be present in the thermodynamic limit. While our calculations are performed for an interaction energy far exceeding the gap between the two lowest energy bands, we note that the higher band does not affect the phase transitions, however destabilizes FCI phases.