BCS-BEC crossover at finite temperature in spin-orbit coupled Fermi gases
arXiv:1303.4136 · doi:10.1103/PhysRevA.87.053616
Abstract
By adopting a -matrix-based method within the approximation for the pair susceptibility, we study the effects of the pairing fluctuation on the three-dimensional spin-orbit coupled Fermi gases at finite temperature. The critical temperatures of the superfluid/normal phase transition are determined for three different types of spin-orbit coupling (SOC): (1) the extreme oblate (EO) or Rashba SOC, (2) the extreme prolate (EP) or equal Rashba-Dresselhaus SOC, and (3) the spherical (S) SOC. For EO- and S-type SOC, the SOC dependence of the critical temperature signals a crossover from BCS to BEC state; at strong SOC limit, the critical temperature recover those of ideal BEC of rashbons. The pairing fluctuation induces a pseudogap in the fermionic excitation spectrum in both superfluid and normal phases. We find that, for EO- and S-type SOC, even at weak coupling, sufficiently strong SOC can induce sizable pseudogap. Our research suggests that the spin-orbit coupled Fermi gases may open new means to the study of the pseudogap formation in fermionic systems.
V2: 13 pages, 8 figures, more discussions added, matches published version
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- Quantum Geometric Contributions to the BKT Transition: Beyond Mean Field Theory
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- Thermodynamic Properties of Rashba Spin-Orbit-Coupled Fermi Gas
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- Fluctuation Theory of Rashba Fermi Gases
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- Interaction-Range Effects and Universality in the BCS-BEC Crossover of Spin-Orbit Coupled Fermi Gases