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The scattering length can be replaced by a function of the relative momentum in order to get an advanced energy dependence of the scattering phase shift. In case of a constant a, one accounts for a trivial energy dependence δ (k) =arctan ka, which is valid for broad Feshbach resonances and nonresonant scattering.
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The scattering length can be replaced by a function of the relative momentum in order to get an advanced energy dependence of the scattering phase shift. In case of a constant a, one accounts for a trivial energy dependence δ (k) =arctan ka, which is valid for broad Feshbach resonances and nonresonant scattering.
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