Effective theory for the Goldstone field in the BCS-BEC crossover at T=0
arXiv:0810.3797 · doi:10.1016/j.aop.2009.01.003
Abstract
We perform a detailed study of the effective Lagrangian for the Goldstone mode of a superfluid Fermi gas at zero temperature in the whole BCS-BEC crossover. By using a derivative expansion of the response functions, we derive the most general form of this Lagrangian at the next to leading order in the momentum expansion in terms of four coefficient functions. This involves the elimination of all the higher order time derivatives by careful use of the leading order field equations. In the infinite scattering length limit where conformal invariance is realized, we show that the effective Lagrangian must contain an unnoticed invariant combination of higher spatial gradients of the Goldstone mode, while explicit couplings to spatial gradients of the trapping potential are absent. Across the whole crossover, we determine all the coefficient functions at the one-loop level, taking into account the dependence of the gap parameter on the chemical potential in the mean-field approximation. These results are analytically expressed in terms of elliptic integrals of the first and second kind. We discuss the form of these coefficients in the extreme BCS and BEC regimes and around the unitary limit, and compare with recent work by other authors.
arXiv comment27 pages. 4 references added, typos corrected, expanded Section III B
References in corpus (21)
- Theory of ultracold Fermi gases
- Observation of resonance condensation of fermionic atom pairs
- Condensation of Pairs of Fermionic Atoms Near a Feshbach Resonance
- Experimental Study of the BEC-BCS Crossover Region in Lithium 6
- Evidence for Superfluidity in a Resonantly Interacting Fermi Gas
- Crossover from a molecular Bose-Einstein condensate to a degenerate Fermi gas
- General coordinate invariance and conformal invariance in nonrelativistic physics: Unitary Fermi gas
- Quantum Fluctuations in the Superfluid State of the BCS-BEC Crossover
- Epsilon expansion for a Fermi gas at infinite scattering length
- Evolution from BCS Superconductivity to Bose Condensation: Analytic Results for the crossover in three dimensions
- BCS-BEC crossover at finite temperature in the broken-symmetry phase
- Conformal Invariance for Non-Relativistic Field Theory
- Effective Lagrangians for BCS Superconductors at T=0
- Effective action for Superconductors and BCS-Bose crossover
- The low-energy phase-only action in a superconductor: a comparison with the XY model
- Universality in Phase Transitions for Ultracold Fermionic Atoms
- Functional Integral for Ultracold Fermionic Atoms
- Effective Field Theory for Dilute Fermions with Pairing
- Derivation of hydrodynamics for the gapless mode in the BEC-BCS crossover from the exact one-loop effective action
- Effective theory of excitations in a Feshbach resonant superfluid
- Effective action for superfluid Fermi systems in the strong-coupling limit
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- Derivation of the effective action of a dilute Fermi gas in the unitary limit of the BCS-BEC crossover
- Phonon contribution to the shear viscosity of a superfluid Fermi gas in the unitarity limit
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- Numerical study of unitary fermions in one spatial dimension
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