p x , y -orbital counterpart of graphene: Cold atoms in the honeycomb optical lattice
By Congjun Wu, D. Bergman. 2007
136 citations recorded by the source corpus.
We study the ground-state properties of the interacting spinless fermions in the ${p}_{x,y}$-orbital bands in the two-dimensional honeycomb optical lattice, which exhibit different features from those in the ${p}_{z}$-orbital system of graphene. In addition to two dispersive bands with Dirac cones, the tight-binding band structure exhibits another two completely flat bands over the entire Brillouin zone. With the realistic sinusoidal optical potential, the flat bands acquire a finite but much smaller bandwidth compared to the dispersive bands. The band flatness dramatically enhanced interaction effects giving rise to various charge and bond ordered states at commensurate fillings of $n=\frac{i}{6}(i=1\char21{}6)$. At $n=\frac{1}{6}$, the many-body ground states can be exactly solved as the close-packed hexagon states which can be stabilized even in the weakly interacting regime. The dimerization of bonding strength occurs at both $n=\frac{1}{2}$ and $\frac{5}{6}$, and the latter case is accompanied with the charge-density wave of holes. The trimerization of bonding strength and charge inhomogeneity appear at $n=\frac{1}{3},\frac{2}{3}$. These crystalline orders exhibit themselves in the noise correlations of the time-of-flight spectra.
Subfields: Atomic and Molecular Physics, and Optics, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/52b67c8c360e9ddf9754f26d556917f7f23ff8dd
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Citations in the corpus
- Graphene-based materials for tissue engineering (2016, background): “The electron confinement in the orbitals are localized to neighboring carbon atoms to create the covalent σ-bonds [41, 42].”
- Quantum phase transition to unconventional multi-orbital superfluidity in optical lattices (2011, background): “enables the emulation of graphene-like physics with ultracold atom”