Spin-orbital exchange of strongly interacting fermions on the $p$-band of a two-dimensional optical lattice

Abstract

Mott insulators with both spin and orbital degeneracy are pertinent to a large number of transition metal oxides. The intertwined spin and orbital fluctuations can lead to rather exotic phases such as quantum spin-orbital liquids. Here we consider two-component (spin 1/2) fermionic atoms with strong repulsive interactions on the $p$-band of the optical square lattice. We derive the spin-orbital exchange for quarter filling of the $p$-band when the density fluctuations are suppressed, and show it frustrates the development of long range spin order. Exact diagonalization indicates a spin-disordered ground state with ferro-orbital order. The system dynamically decouples into individual Heisenberg spin chains, each realizing a Luttinger liquid accessible at higher temperatures compared to atoms confined to the $s$-band.

revised

References in corpus (10)

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Cited by in corpus (2)

• Experimental realization of a high precision tunable hexagonal optical lattice
• Topological phases of spinless $p$-orbital fermions in zigzag optical lattices