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Here we use a and K2 from Eqs. 15 18. We derived these equations assuming that the sample is Bose condensed which is not the case in a deep optical lattice. But a and K2 express only properties of two-body scattering processes. They are unaffected by the many-body state of the system.
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Here we use a and K2 from Eqs. 15 18. We derived these equations assuming that the sample is Bose condensed which is not the case in a deep optical lattice. But a and K2 express only properties of two-body scattering processes. They are unaffected by the many-body state of the system.
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