Extended Haldane Model in The Dice Lattice: Multiple Flat‐Band‐Induced Topological Transitions Revealed
Résumé
ABSTRACT In this study, we examine the introduction of the Haldane model into the dice lattice by altering the flow between the next‐nearest‐neighbor sites. This breaks the lattice's inversion and time‐reversal symmetries. We demonstrate the presence of point‐charge particle symmetries at and and derive the analytical expression for quasi‐energies. We demonstrate that a gap closure occurs at these critical points, inducing a topological transition. This is confirmed by calculating the Berry curvature and orbital magnetic moment. A topological analysis shows that the Chern numbers of the valence band , the flat band and the conduction band depend strongly on the relationship between the fluxes and . When , the Chern numbers are in the region , and (0, 2, ‐2) in the region . Conversely, when , the topological invariants become for , and for . These variations reflect topological phase transitions at the critical points and , affecting all of the system's bands. Furthermore, the anomalous Hall conductivity exhibits a quantized plateau of 2, as well as an unquantized tilted plateau evolving from 1.50 to 1.25 at the same transition points. Controlling the flux allows topological transitions to be engineered and quantum transport in the dice lattice to be optimized, offering promising prospects for reconfigurable topological devices with low dissipation and robust quantum transport.
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