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i which may be considered as "instantaneous decay." Our experimental situation lies in between and the equation of motion cannot be written in such a simple form. Evaluation of the experimental data assuming the α=2 case (instead of α=7/5) leads to a modification of 20% in comparison of the loss rate to the theoretical result. The dynamics of the decay process is a interesting problem on its own and would go beyond the scope of this paper.
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85015737704
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note
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2 with an accuracy of 20%. The preparation asymmetry can be determined and compensated for each measurement regarding the actual asymmetry and assuming losses by pairs of F=2 and F=1 atoms. Nevertheless this procedure leads only to changes of 20% in initial loss rates and has negligible effects on position and width of the resonance.
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31
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85015748511
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note
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F is the imaginary part of the scattering length at the Feshbach resonance).
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