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Bulletin of the American Physical Society

BCS to BEC evolution for mixtures of fermions with unequal masses

Sá de Melo, A R Carlos

Published Mar 16, 2009• 0 citations
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We investigate the crossover from BCS pairing to molecular Bose-Einstein condensation (BEC) in an atomic gas with two fermion species with masses ${m}_{\ensuremath{\uparrow}}\ensuremath{\ne}{m}_{\ensuremath{\downarrow}}$ tuned through a Feshbach resonance. We present results for the $T=0$ equation of state as a function of the scattering length including the effects of Gaussian fluctuations about the mean field ground state. We compute the ground state energy as a function of ${m}_{\ensuremath{\uparrow}}/{m}_{\ensuremath{\downarrow}}$ at unitarity and find excellent agreement with the quantum Monte Carlo result for ${m}_{\ensuremath{\uparrow}}/{m}_{\ensuremath{\downarrow}}=6.67$ for a $^{40}\mathrm{K}$-$^{6}\mathrm{Li}$ mixture. We show that the dimer scattering length in the BEC limit as a function of ${m}_{\ensuremath{\uparrow}}/{m}_{\ensuremath{\downarrow}}$ compares well with the exact four-body results of Petrov et al. [J. Phys. B 38, S645 (2005)]. We also derive the condition for trapping frequencies to obtain an unpolarized gas in a harmonic trap.

arXiv:0906.4300•Physical Review A•Mar 15, 2010•19 citations
We analyze the phase diagram of superfluidity for two-species fermion mixtures from the Bardeen-Cooper-Schrieffer (BCS) to Bose-Einstein condensation (BEC) limit as a function of scattering parameter, population imbalance, and mass anisotropy. We identify regions corresponding to normal, or uniform or nonuniform superfluid phases, and discuss topological quantum phase transitions in the BCS, unitarity, and BEC limits. We derive the Ginzburg-Landau equation near the critical temperature, and show that it describes a dilute mixture of paired and unpaired fermions in the BEC limit. We also obtain the zero temperature low frequency and long wavelength collective excitation spectrum, and recover the Bogoliubov relation for weakly interacting dilute bosons in the BEC limit. Lastly, we discuss the effects of harmonic traps and the resulting density profiles in the BEC regime.
We investigate the crossover from BCS pairing to molecular Bose-Einstein condensation (BEC) in an atomic gas with two fermion species with masses ${m}_{\ensuremath{\uparrow}}\ensuremath{\ne}{m}_{\ensuremath{\downarrow}}$ tuned through a Feshbach resonance. We present results for the T=0T=0T=0 equation of state as a function of the scattering length including the effects of Gaussian fluctuations about the mean field ground state. We compute the ground state energy as a function of ${m}_{\ensuremath{\uparrow}}/{m}_{\ensuremath{\downarrow}}$ at unitarity and find excellent agreement with the quantum Monte Carlo result for ${m}_{\ensuremath{\uparrow}}/{m}_{\ensuremath{\downarrow}}=6.67$ for a 40K^{40}\mathrm{K}40K-6Li^{6}\mathrm{Li}6Li mixture. We show that the dimer scattering length in the BEC limit as a function of ${m}_{\ensuremath{\uparrow}}/{m}_{\ensuremath{\downarrow}}$ compares well with the exact four-body results of Petrov et al. [J. Phys. B 38, S645 (2005)]. We also derive the condition for trapping frequencies to obtain an unpolarized gas in a harmonic trap.