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Bulletin of the American Physical Society

P-wave Paired Ground state Structure of Two-component Population Imbalanced Fermi Systems with Unequal Mass

Florentin Popescu, Renyuan Liao, Khandker Quader

Published Mar 13, 2008• 0 citations
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We study $p$-wave pairing in a two-component Fermi system with unequal population across weak-coupling BCS to strong-coupling BEC regimes. We find a rich ${m}_{s}=0$ spin triplet $p$-wave superfluid (SF) ground state (GS) structure as a function of population imbalance. Under a phase stability condition, the ``global'' energy minimum is given by a multitude of ``mixed'' SF states formed of linear combinations of $m=\ifmmode\pm\else\textpm\fi{}1,0$ substates of the $\ensuremath{\ell}=1$ orbital angular momentum state. Except for the ``pure'' SF states ($\ensuremath{\ell}=1,m=\ifmmode\pm\else\textpm\fi{}1$), other states exhibit oscillation in energy with the relative phase between the constituent gap amplitudes. We also find states with ``local'' energy minimum that can be stable at higher polarizations, suggesting a quantum phase transition between the ``global'' and ``local'' minima phases driven by polarization. We relate the local and global minimum states to Morse and non-Morse critical points. We calculate the variations of the ground state energy with a relative phase angle, coupling, and polarization, and discuss possible consequences for experiments.

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We investigate two-component attractive Fermi gases with imbalanced spin populations in trapped one-dimensional configurations. The ground state properties are determined with the local density approximation, starting from the exact Bethe-ansatz equations for the homogeneous case. We predict that the atoms are distributed according to a two-shell structure: a partially polarized phase in the center of the trap and either a fully paired or a fully polarized phase in the wings. The partially polarized core is expected to be a superfluid of the Fulde-Ferrell-Larkin-Ovchinnikov type. The size of the cloud as well as the critical spin polarization needed to suppress the fully paired shell are calculated as a function of the coupling strength.
We present an exact quantum Monte Carlo study of the effect of unequal masses on pair formation in fermionic systems with population imbalance loaded into optical lattices. We have considered three forms of the attractive interaction and find in all cases that the system is unstable and collapses as the mass difference increases and that the ground state becomes an inhomogeneous collapsed state. We also address the question of canonical vs. grand canonical ensemble and its role, if any, in stabilizing certain phases.
We study ppp-wave pairing in a two-component Fermi system with unequal population across weak-coupling BCS to strong-coupling BEC regimes. We find a rich ms=0{m}_{s}=0ms​=0 spin triplet ppp-wave superfluid (SF) ground state (GS) structure as a function of population imbalance. Under a phase stability condition, the ``global'' energy minimum is given by a multitude of ``mixed'' SF states formed of linear combinations of $m=\ifmmode\pm\else\textpm\fi{}1,0$ substates of the $\ensuremath{\ell}=1$ orbital angular momentum state. Except for the ``pure'' SF states ($\ensuremath{\ell}=1,m=\ifmmode\pm\else\textpm\fi{}1$), other states exhibit oscillation in energy with the relative phase between the constituent gap amplitudes. We also find states with ``local'' energy minimum that can be stable at higher polarizations, suggesting a quantum phase transition between the ``global'' and ``local'' minima phases driven by polarization. We relate the local and global minimum states to Morse and non-Morse critical points. We calculate the variations of the ground state energy with a relative phase angle, coupling, and polarization, and discuss possible consequences for experiments.