We employ radio-frequency spectroscopy on weakly bound 6 Li2 molecules to precisely determine the molecular binding energies and the energy splittings between molecular states for different magnetic fields. These measurements allow us to extract the interaction parameters of ultracold 6 Li atoms based on a multi-channel quantum scattering model. We determine the singlet and triplet scattering lengths to be as = 45.167(8)a0 and at = −2140(18)a0 (1 a0 = 0.0529177 nm), and the positions of the broad Feshbach resonances in the energetically lowest three s−wave scattering channels to be 83.41 (15) [2,3,4,5,6] and the studies of the crossover physics from a molecular Bose-Einstein condensate to atomic Cooper pairs in the Bardeen-CooperSchrieffer state (BEC-BCS crossover) [5,7,8]. These studies are of general importance in physics as the ultracold Fermi gas provides a unique model system for other strongly interacting fermionic systems [9].In spin mixtures of 6 Li atoms, a broad Feshbach resonance in the energetically lowest s-wave channel [10] allows for precise interaction tuning. This, together with the extraordinary stability of the system against inelastic decay [2,11], makes 6 Li the prime candidate for BEC-BCS crossover studies. Precise knowledge of the magnetic-field dependent scattering properties is crucial for a quantitative comparison of the experimental results with crossover theories. Of particular importance is the precise value of the magnetic field where the s−wave scattering diverges. At this unique point, the strongly interacting fermionic quantum gas is expected to exhibit universal properties [12]. Previous experiments explored the 6 Li resonance by measuring inelastic decay [13], elastic collisions [14,15], and the interaction energy [16], but could only locate the exact resonance point to within a range between 80 mT and 85 mT.An ultracold gas of weakly bound molecules is an excellent starting point to explore the molecular energy structure near threshold [17]. Improved knowledge on the exact 6 Li resonance position was recently obtained in an experiment that observed the controlled dissociation of weakly bound 6 Li 2 molecules induced by magnetic field ramps [18]. These measurements provided a lower bound of 82.2 mT for the resonance position. Studies of systematic effects suggested an upper bound of 83.4 mT. Within this range, however, we observe the physical behavior of the ultracold gas still exhibits a substantial dependence on the magnetic field [8]. In this Letter, we apply radiofrequency (rf) spectroscopy [17,19] on weakly bound molecules to precisely determine the interaction parameters of cold 6 Li atoms. Together with a multi-channel quantum scattering model, we obtain a full characterization of the two-body scattering properties, essential for BEC-BCS crossover physics.The relevant atomic states are the lowest three sublevels in the 6 Li ground state manifold, denoted by |1 , |2 and |3 . Within the magnetic field range investigated in this experiment, these levels form a triplet of st...
We report on precision measurements of the frequency of the radial compression mode in a strongly interacting, optically trapped Fermi gas of (6)Li atoms. Our results allow for a test of theoretical predictions for the equation of state in the BEC-BCS crossover. We confirm recent quantum Monte Carlo results and rule out simple mean-field BCS theory. Our results show the long-sought beyond-mean-field effects in the strongly interacting Bose-Einstein condensation (BEC) regime.
We present a joint theoretical and experimental study of the dynamical instability of a Bose-Einstein condensate at the band edge of a one-dimensional optical lattice. The instability manifests as rapid depletion of the condensate and conversion to a thermal cloud. We consider the collisional processes that can occur in such a system, and undertake a thorough theoretical study of the dynamical instability in systems of different dimensionality. We find spontaneous scattering is an important part of this process, and thus the GrossPitaevskii equation is unable to accurately predict the dynamics in this system. Our beyond mean-field approach, known as the truncated Wigner method, allows us to make quantitative predictions for the processes of parametric growth and heating that are observed in the laboratory, and we find good agreement with the experimental results.
We present the results of Bragg spectroscopy performed on an accelerating Bose-Einstein condensate. The Bose condensate undergoes circular micro-motion in a magnetic TOP trap and the effect of this motion on the Bragg spectrum is analyzed. A simple frequency modulation model is used to interpret the observed complex structure, and broadening effects are considered using numerical solutions to the Gross-Pitaevskii equation.Comment: 5 pages, 3 figures, to appear in PRA. Minor changes to text and fig
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