Induced interactions for ultracold Fermi gases in optical lattices
arXiv:0901.4769 · doi:10.1103/PhysRevLett.102.245301
Abstract
We investigate the effect of optical lattices on the BCS superfluidity by using the Gorkov--Melik-Barkhudarov (GMB) correction for a two-component Fermi gas. We find that the suppression of the order parameter is strongly enhanced by the lattice effects. The predictions made by the GMB corrections are in qualitative and, for the cases studied, quantitative agreement with previous quantum Monte Carlo results. We discuss how the GMB correction extends the validity of the mean-field theory to a wider range of tunable optical lattice systems in different dimensions.
arXiv comment4 pages, 4 figures
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Cited by in corpus (14)
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- Gap equation with pairing correlations beyond mean field and its equivalence to a Hugenholtz-Pines condition for fermion pairs
- Pseudogap phenomena in ultracold atomic Fermi gases
- Induced interactions and the superfluid transition temperature in a three-component Fermi gas
- Fulde-Ferrell--Larkin-Ovchinnikov state in the dimensional crossover between one- and three-dimensional lattices
- Finite Temperature Phase Diagram of Quasi-Two-Dimensional Imbalanced Fermi Gases Beyond Mean-Field
- Effect of the particle-hole channel on BCS--Bose-Einstein condensation crossover in atomic Fermi gases
- Induced interactions in the BCS-BEC crossover of two-dimensional Fermi gases with Rashba spin-orbit coupling
- Nesting and lifetime effects in the FFLO state of quasi-one-dimensional imbalanced Fermi gases
- Influence of Induced Interactions on Superfluid Properties of Quasi-Two Dimensional Dilute Fermi Gases With Spin-Orbit Coupling
- Crossovers in Unitary Fermi Systems
- The Gor'kov and Melik-Barkhudarov correction to an imbalanced Fermi gas in the presence of impurities
- The Gor'kov and Melik-Barkhudarov correction to the mean-field critical field transition to Fulde-Ferrell-Larkin-Ovchinnikov states
- Comment on Influence of induced interactions on superfluid properties of quasi-two-dimensional dilute Fermi gases with spin-orbit coupling