Fractional Chern Insulator phase at the transition between checkerboard and Lieb lattice
arXiv:1508.04399 · doi:10.1103/PhysRevB.92.245119
Abstract
The stability of Fractional Chern Insulator (FCI) phase is analysed on the example of checkerboard lattice undergoing a transition into Lieb lattice. The transition is performed by the addition of a second sublattice, whose coupling to the checkerboard sites is controlled by sublattice staggered potential. We investigate the influence of these sites on the many body energy gap between three lowest energy states and the fourth state. We consider cases with different complex phases acquired in hopping and a model with a flattened topologically nontrivial band. We find that an interaction with the additional sites either open the single-particle gap or enlarge the existing one, which translates into similar effect on the many-particle gap. Evidences of FCI phase for a region in a parameter space with larger energy gap are shown by looking at momenta of the three-fold degenerate ground state, spectral flow, and quasihole excitation spectrum.
7 pages, 7 figures
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- Desiging Artificial Lieb Lattice on Metal Surface
- Designer Flat Bands in Quasi-One-Dimensional Atomic Lattices
- Wigner crystallization in topological flat bands
- Experimental Realization of Two-Dimensional Buckled Lieb lattice
- Flat band transport and Josephson effect through a finite-size sawtooth lattice
- Characterization of quasiholes in two-component fractional quantum Hall states and fractional Chern insulators in flat bands
- Spontaneous particle-hole symmetry breaking of correlated fermions on the Lieb lattice
- Holstein polaron in a pseudospin- quantum spin Hall system: first and second order topological phase transitions
- Ground state spin and excitation energies in half-filled Lieb lattices
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- Topological Degeneracy Induced Flat Bands in two-Dimensional Holed Systems