Abstract

We calculate the pair susceptibility of an attractive spin-polarized Fermi gas in the normal phase, as a function of the pair momentum. Close to unitarity, we find a strong enhancement of Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) pairing fluctuations over an extended region of the temperature-polarization phase diagram, which manifests itself as a pronounced peak in the pair-momentum distribution at a finite pair momentum. This peak should be amenable to experimental observation at achievable temperatures in a box-like trapping potential, as a fingerprint of FFLO pairing. Our calculations rest on a self-consistent t-matrix approach which, for the unitary balanced Fermi gas, has been validated against experimental data for several thermodynamic quantities.

Highlights

  • One of the main motivations that some time ago [1,2] initiated a vibrant experimental and theoretical research activity on ultracold polarized attractive Fermi gases [3], was the search for exotic superfluid phases, like the FFLO phase predicted many years before by Fulde and Ferrell [4] and Larkin and Ovchinnikov [5] for superconductors in a strong magnetic field

  • We find a strong enhancement of Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) pairing fluctuations over an extended region of the temperature-polarization phase diagram, which manifests itself as a pronounced peak in the pair-momentum distribution at a finite pair momentum

  • Close to unitarity [15], we find that the pair susceptibility is considerably enhanced at a finite value Q0(r) proportional to χpair (Q0) of Q(= |Q|) over an extended region of the temperature-polarization phase diagram, such that it should be possible to observe this strong tendency towards FFLO ordering at experimentally achievable temperatures in the normal phase

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Summary

Introduction

One of the main motivations that some time ago [1,2] initiated a vibrant experimental and theoretical research activity on ultracold polarized attractive Fermi gases [3], was the search for exotic superfluid phases, like the FFLO phase predicted many years before by Fulde and Ferrell [4] and Larkin and Ovchinnikov [5] for superconductors in a strong magnetic field. This phase is characterized by pairing at finite center-of-mass momentum of the pairs, with spatially dependent gap parameter (r) = Q0 eiQ0·r for the Fulde-Ferrell (FF) and (r) = Q0 cos(Q0 · r) for the Larkin-Ovchinnikov (LO) solutions.

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