Theory of the Normal/Superfluid interface in population imbalanced Fermi gases
arXiv:0901.2945 · doi:10.1103/PhysRevA.79.063628
Abstract
We present a series of theoretical studies of the boundary between a superfluid and normal region in a partially polarized gas of strongly interacting fermions. We present mean-field estimates of the surface energy in this boundary as a function of temperature and scattering length. We discuss the structure of the domain wall, and use a previously introduced phenomonological model to study its influence on experimental observables. Our microscopic mean-field calculations are not consistent with the magnitude of the surface tension found from our phenomonological modelling of data from the Rice experiments. We conclude that one must search for novel mechanisms to explain the experiments.
15 pages, 9 figures (13 subfigures) -- v2: minor changes
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Cited by in corpus (20)
- Imbalanced Feshbach-resonant Fermi gases
- The Fulde-Ferrell-Larkin-Ovchinnikov state for ultracold fermions in lattice and harmonic potentials: a review
- Repulsive Fermi gas in a harmonic trap: Ferromagnetism and spin textures
- Evaporative depolarization and spin transport in a unitary trapped Fermi gas
- Metastability in Spin-Polarized Fermi Gases
- Concomitant Modulated Superfluidity In Polarized Fermionic Gases
- Stability of Sarma phases in density imbalanced electron-hole bilayer systems
- Superfluidity in Two-Dimensional Imbalanced Fermi Gases
- Mean-field study of itinerant ferromagnetism in trapped ultracold Fermi gases: Beyond the local density approximation
- Fulde-Ferrell-Larkin-Ovchinnikov state in bilayer dipolar systems
- Quantum engineering of Majorana quasiparticles in one-dimensional optical lattices
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- Dependence of interface conductivity on relevant physical parameters in polarized Fermi mixtures
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- The Gor'kov and Melik-Barkhudarov correction to an imbalanced Fermi gas in the presence of impurities