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Physical Review A

Pairing and coherence order parameters in a three-component ultracold Fermi gas

Chun Kit Chung, C. K. Law

Published Sep 29, 2010• 3 citations
Publisher

Abstract

We investigate the mean-field ground state of a homogeneous three-component attractive Fermi gas at zero temperature. This is achieved by deriving a set of Bogoliubov--de Gennes (BdG) equations of the three-component system, including pairing both order parameters ${\ensuremath{\Delta}}_{\mathit{ij}}$ and coherence order parameters $\ensuremath{\langle}{\ensuremath{\psi}}_{i}^{\ifmmode\dagger\else\textdagger\fi{}}{\ensuremath{\psi}}_{j}\ensuremath{\rangle}$ ($i\ensuremath{\ne}j$), where ${\ensuremath{\psi}}_{j}$ is the field operator for spin level $j$. Ward-Takahashi identities are obtained to constrain these order parameters. In addition, we present an explicit analytic mean-field solution for symmetric systems and verify that the quasiparticle excitations consist of both gapped and gapless spectra, which correspond to the excitations of paired and unpaired atoms. We further point out that the omission of $\ensuremath{\langle}{\ensuremath{\psi}}_{i}^{\ifmmode\dagger\else\textdagger\fi{}}{\ensuremath{\psi}}_{j}\ensuremath{\rangle}$ in BdG equations could lead to an overestimation of ${\ensuremath{\Delta}}_{\mathit{ij}}$ in the strong coupling regime.

DOI
10.1103/physreva.82.033620

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We investigate the mean-field ground state of a homogeneous three-component attractive Fermi gas at zero temperature. This is achieved by deriving a set of Bogoliubov--de Gennes (BdG) equations of the three-component system, including pairing both order parameters \ensuremathΔij{\ensuremath{\Delta}}_{\mathit{ij}}\ensuremathΔij​ and coherence order parameters \ensuremath⟨\ensuremathψi\ifmmode†\else\textdagger\fi\ensuremathψj\ensuremath⟩\ensuremath{\langle}{\ensuremath{\psi}}_{i}^{\ifmmode\dagger\else\textdagger\fi{}}{\ensuremath{\psi}}_{j}\ensuremath{\rangle}\ensuremath⟨\ensuremathψi\ifmmode†\else\textdagger\fi​\ensuremathψj​\ensuremath⟩ (i\ensuremath≠ji\ensuremath{\ne}ji\ensuremath=j), where \ensuremathψj{\ensuremath{\psi}}_{j}\ensuremathψj​ is the field operator for spin level jjj. Ward-Takahashi identities are obtained to constrain these order parameters. In addition, we present an explicit analytic mean-field solution for symmetric systems and verify that the quasiparticle excitations consist of both gapped and gapless spectra, which correspond to the excitations of paired and unpaired atoms. We further point out that the omission of \ensuremath⟨\ensuremathψi\ifmmode†\else\textdagger\fi\ensuremathψj\ensuremath⟩\ensuremath{\langle}{\ensuremath{\psi}}_{i}^{\ifmmode\dagger\else\textdagger\fi{}}{\ensuremath{\psi}}_{j}\ensuremath{\rangle}\ensuremath⟨\ensuremathψi\ifmmode†\else\textdagger\fi​\ensuremathψj​\ensuremath⟩ in BdG equations could lead to an overestimation of \ensuremathΔij{\ensuremath{\Delta}}_{\mathit{ij}}\ensuremathΔij​ in the strong coupling regime.
We provide a general methodology to directly determine the validity of the meanfield Bogoliubov-de Gennes equation. In particular we apply this methodology to the case of two component interacting ultracold Fermi gases. As an example, we consider the case of population imbalance, between the two components, in the strongly attractive interacting regime, where meanfield results predict Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) states. For these states we find at finite temperatures that the assumptions used to derive the Bogoliubov-de Gennes equation are invalid.
Ultracold three-component atomic Fermi gases in one dimension are expected to exhibit rich physics due to the presence of trions and different pairing states. Quantum phase transitions from the trion state into a paired phase and a normal Fermi liquid occur at zero temperature. We derive the analytical thermodynamics of strongly attractive three-component one-dimensional fermions with SU(3) symmetry via the thermodynamic Bethe ansatz method in unequal Zeeman splitting fields H1{H}_{1}H1​ and H2{H}_{2}H2​. We find explicitly that for low temperature the system acts like either a two-component or a three-component Tomonaga-Luttinger liquid dependent on the system parameters. The phase diagrams for the chemical potential and specific heat are presented for illustrative values of the Zeeman splitting. We also demonstrate that crossover between different Tomonaga-Luttinger-liquid phases exhibit singular behavior in specific heat and entropy as the temperature tends to zero. Beyond Tomonaga-Luttinger-liquid physics, we obtain the equation of state which provides a precise description of universal thermodynamics and quantum criticality in three-component, strongly attractive Fermi gases.
We investigate the formation of Bose-Einstein condensation and a population imbalance in a three-component Fermi superfluid by increasing the U(3) invariant attractive interaction. We consider the system at zero temperature in three dimensions as well as in two dimensions. Within mean-field theory, we derive explicit formulas for the number densities, the gap order parameter, the condensate density, and the condensate fraction of the uniform system and analyze them in the crossover from the Bardeen-Cooper-Schrieffer (BCS) state of Cooper pairs to the Bose-Einstein condensate (BEC) of strongly bound molecular dimers. In addition we study this Fermi mixture trapped by a harmonic potential: We calculate the density profiles of the three components and the condensate density profile of Cooper pairs in the BCS-BEC crossover.
We study the ground-state properties of a two-component ultracold superfluid Fermi gas with Rashba spin-orbit coupling at zero temperature in two-dimensional.The gap-order parameter and number densities are found analytically throught the thermodynamic potential at saddle point by using the functional and integral method.We obtain the phase diagram by solve the self-consistent equations.Under the influence of spin orbit couping,and we construct the phase diagram by comparing the thermodynamic potential of superfluid and phase-separated states.The balance of pairing will be broken due to the unequal chemical potentials in the two-component ultracold Fermi gas in two-dimensional with spin orbit coupling.
We consider imbalanced Fermi gases with strong attractive interactions, for which Cooper-pair formation plays an important role. The two-component mix-tures consist either of identical fermionic atoms in two different hyperfine states, or of two different atomic species both occupying only a single hyperfine state. In both cases, the number of atoms for each component is allowed to be differ-ent, which leads to a spin imbalance, or spin polarization. Two different atomic species also lead to a mass imbalance. Imbalanced Fermi gases are relevant to condensed-matter physics, nuclear physics and astroparticle physics. They have been studied intensively in recent years, following their experimental realization in ultracold atomic Fermi gases. The experimental control in such a system allows for a systematic study of the equation of state and the phase diagram as a function of temperature, spin polarization and interaction strength. In this re-view, we discuss the progress in understanding strongly-interacting imbalanced Fermi gases, where a main goal is to describe the results of the highly controlled experiments. We start by discussing Feshbach resonances, after which we treat the imbalanced Fermi gas in mean-field theory to give an introduction to the relevant physics. We encounter several unusual superfluid phases, including phase-separation, gapless Sarma superfluidity, and supersolidity. To obtain a more quantitative description of the experiments, we review also more sophisti-cated techniques, such as diagrammatic methods and the renormalization-group theory. We end the review by discussing two theoretical approaches to treat the inhomogeneous imbalanced Fermi gas, namely the Landau-Ginzburg theory and the Bogoliubov-de Gennes approach. Key words: