Bound states and Cooper pairs of molecules in 2D optical lattices bilayer
arXiv:1511.06311 · doi:10.1002/andp.201500342
Abstract
We investigate the formation of Cooper pairs, bound dimers and the dimer-dimer elastic scattering of ultra- cold dipolar Fermi molecules confined in a 2D optical lattice bilayer configuration. While the energy and their associated bound states are determined in a variational way, the correlated two-molecule pair is addressed as in the original Cooper formulation. We demonstrate that the 2D lattice confinement favors the formation of zero center mass momentum bound states. Regarding the Cooper pairs binding energy, this depends on the molecule populations in each layer. Maximum binding energies occur for non-zero (zero) pair momentum when the Fermi system is polarized (unpolarized). We find an analytic expression for the dimer-dimer effective interaction in the deep BEC regime. The present analysis represents a route for addressing the BCS-BEC crossover superfluidity in dipolar Fermi gases confined in 2D optical lattices within the current experimental panorama.
7 pages, 8 figures
References in corpus (7)
- Ultracold Dipolar Gas of Fermionic NaK Molecules in their Absolute Ground State
- Two-particle states in the Hubbard model
- Interlayer superfluidity in bilayer systems of fermionic polar molecules
- Ultracold Dipolar Molecules Composed of Strongly Magnetic Atoms
- Density wave patterns for fermionic dipolar molecules on a square optical lattice: Mean-field-theory analysis
- Ultralong-range order in the Fermi-Hubbard model with long-range interactions
- Coexistence of density wave and superfluid order in a dipolar Fermi gas