Finite Temperature Phase Diagram of Quasi-Two-Dimensional Imbalanced Fermi Gases Beyond Mean-Field
arXiv:1209.1838 · doi:10.1103/PhysRevA.86.033603
Abstract
We investigate the superfluid transition temperature of quasi-two-dimensional imbalanced Fermi gases beyond the mean-field approximation, through the second-order (or induced) interaction effects. For a balanced Fermi system the transition temperature is suppressed by a factor . For imbalanced Fermi systems, the polarization and transition temperature of the tricritical point are significantly reduced as the two-body binding energy increases.
6 pages, 3 figures
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Cited by in corpus (13)
- Quantum fluctuations in the BCS-BEC crossover of two-dimensional Fermi gases
- Spin-Imbalanced Quasi-Two-Dimensional Fermi Gases
- Entanglement between pairing and screening in the Gorkov-Melik-Barkhudarov correction to the critical temperature throughout the BCS-BEC crossover
- Mechanism for enhancement of superconductivity in multi-band systems with odd parity hybridization
- 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
- Two-dimensional spin-imbalanced Fermi gases at non-zero temperature: Phase separation of a non-condensate
- Toward precision Fermi liquid theory in two dimensions
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- Induced p-wave Superfluidity in Imbalanced Fermi Gases in a Synthetic Gauge Field
- Temporal fluctuation induced order in conventional superconductors