paper

Optically Controlled Topological Phases in the Deformed Lattice

arXiv:2503.22146 · doi:10.1016/j.aop.2025.170203

Abstract

Haldane's tight-binding model, which describes a Chern insulator in a two-dimensional hexagonal lattice, exhibits quantum Hall conductivity without an external magnetic field. Here, we explore an lattice subjected to circularly polarized off-resonance light. This lattice, composed of two sublattices (A and B) and a central site (C) per unit cell, undergoes deformation by varying the hopping parameter while keeping = = . Analytical expressions for quasi-energies in the first Brillouin zone reveal significant effects of symmetry breaking. Circularly polarized light lifts the degeneracy of Dirac points, shifting the cones from M. This deformation evolves with , breaking symmetry at , as observed in Berry curvature diagrams. In the standard case (), particle-hole and inversion symmetries are preserved for and . The system transitions from a semi-metal to a Chern insulator, with band-specific Chern numbers: , , and for shifting to , , and when For , the system enters a trivial insulating phase. These transitions, confirmed via Wannier charge centers, are accompanied by a diminishing Hall conductivity. Our findings highlight tunable topological phases in lattices, driven by light and structural deformation, with promising implications for quantum materials.

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