Abstract
We present a consistent nonequilibrium theory for the production of molecular dimers from a two-component quantum-degenerate atomic Fermi gas, via a linear downward sweep of a magnetic field across a Feshbach resonance. This problem raises interest because it is presently unclear as to why deviations from the universal Landau–Zener formula for the transition probability at two-level crossing are observed in the experimentally measured production efficiencies. We show that the molecular conversion efficiency is represented by a power series in terms of a dimensionless parameter which, in the zero-temperature limit, depends solely on the initial gas density and the Landau–Zener parameter. Our result reveals a hindrance of the canonical Landau–Zener transition probability due to many-body effects, and presents an explanation for the experimentally observed deviations [K.E. Strecker, et al., Phys. Rev. Lett. 91 (2003) 080406].
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