2006
DOI: 10.1103/physrevlett.96.090403
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Vortices in Superfluid Fermi Gases through the BEC to BCS Crossover

Abstract: We have analyzed a single vortex at T 0 in a 3D superfluid atomic Fermi gas across a Feshbach resonance. On the BCS side, the order parameter varies on two scales: k ÿ1 F and the coherence length , while only variation on the scale of is seen away from the BCS limit. The circulating current has a peak value j max which is a nonmonotonic function of 1=k F a s implying a maximum critical velocity v F at unitarity. The number of fermionic bound states in the core decreases as we move from the BCS to the BEC regim… Show more

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Cited by 118 publications
(219 citation statements)
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“…where in the last line we have made use of the BCS gap equation (11). The short-range behavior of g ↑↓ (ρ) which results from Eq.…”
Section: Bcs Cmentioning
confidence: 99%
“…where in the last line we have made use of the BCS gap equation (11). The short-range behavior of g ↑↓ (ρ) which results from Eq.…”
Section: Bcs Cmentioning
confidence: 99%
“…For Bose gases, the most common method is to employ the Gross-Pitaevskii (GP) equation 7,8 . Superfluid Fermi gases can however be studied by a variety of methods, the most common are: the GinzburgLandau (GL) formalism 9 , the Bogoliubov-De Gennes (BdG) theory [10][11][12][13][14][15][16] , superfluid density functional theory 17 , the density matrix renormalization group 18 and the coarse-grained BdG approximation 19 .…”
Section: Introduction: Vortices In the Bec-bcs Crossovermentioning
confidence: 99%
“…The problem with the BdG theory is however that the method is computationally fairly cumbersome. Consequently the use of the BdG theory is mainly limited to the consideration of zero-temperature properties of single-vortex states [10][11][12] . Because of this big computational cost of the BdG theory, there is a recent interest in the development of effective field theories [20][21][22][23][24][25][26] .…”
Section: Introduction: Vortices In the Bec-bcs Crossovermentioning
confidence: 99%
“…The Bogoliubov quasiparticles (the two branches being denoted by χ ↑ and χ ↓ ) can now be introduced as 10) where u k , v k are Bogoliubov amplitudes. For the lower branch quasiparticle field, which is simply denoted by χ (i.e, χ ≡ χ ↓ ), this becomes in real space…”
Section: A2 Galilean Transformation For Quasiparticlesmentioning
confidence: 99%
“…[7] In addition, several theoretical studies have analyzed the possible new properties of vortices across a Feshbach resonance from the BCS to the BEC side. [8,9,10,11] The physics of atomic Fermi gases is also of fundamental interest beyond the standard BCS/BEC physics, owing to the new tuning flexibility in the atomic gas systems. Under the condition of density imbalance (hence mismatched Fermi surfaces) between the spin-up and -down fermions, a modulated Larkin-Ovchinnikov-Fulde-Ferrell (LOFF) [12] superfluid phase, has long been theoretically anticipated.…”
Section: Introductionmentioning
confidence: 99%