Pseudogap and preformed pairs in the imbalanced Fermi gas in two dimensions

TL;DR

This paper develops a divergence-free path integral formalism to analyze the pseudogap state, preformed pairs, and superfluid transition temperatures in imbalanced two-dimensional Fermi gases, aligning theoretical predictions with experimental observations.

Contribution

It introduces a novel divergence-free approach for studying pairing and pseudogap phenomena in 2D Fermi gases, deriving key temperatures and phase diagrams.

Findings

Pseudogap temperature is suppressed by fluctuations compared to pair formation temperature.

The critical temperature for superfluidity aligns with the BKT transition.

Phase diagrams delineate superfluid, quasicondensate, and normal phases based on binding energy and imbalance.

Abstract

The physics of the pseudogap state is intimately linked with the pairing mechanism that gives rise to superfluidity in quantum gases and to superconductivity in high-Tc cuprates, and therefore, both in quantum gases and superconductors, the pseudogap state and preformed pairs have been under intensive experimental scrutiny. Here, we develop a path integral treatment that provides a divergence-free description of the paired state in two-dimensional Fermi gases. Within this formalism, we derive the pseudogap temperature and the pair fluctuation spectral function, and compare these results with the recent experimental measument of the pairing in the two-dimensional Fermi gas. The removal of the infrared divergence in the number equations is shown both numerically and analytically, through a study of the long-wavelength and low-energy limit of the pair fluctuation density. Besides the pseudogap temperature, also the pair formation temperature and the critical temperature for superfluidity are derived. The latter corresponds to the Berezinski-Kosterlitz-Thouless (BKT) temperature. The pseudogap temperature, which coincides with the pair formation temperature in mean field, is found to be suppressed with respect to the pair formation temperature by fluctuations. This suppression is strongest for large binding energies of the pairs. Finally, we investigate how the pair formation temperature, the pseudogap temperature and the BKT temperature behave as a function of both binding energy and imbalance between the pairing partners in the Fermi gas. This allows to set up phase diagrams for the two-dimensional Fermi gas, in which the superfluid phase, the phase-fluctuating quasicondensate, and the normal state can be identified.