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all the partial waves contribute with the same sign to the imaginary part of F(cos () = 1) and give rise to the diffraction peak in the forward direction. Then, one can easily suppose that the Pomeron term responsible for the forward peak involves significant contributions from all partial waves l<ka, where 7J1± and o1± are the absorption parameters and phase shifts, respectively, for the J = l ± i states, k is the center-of-mass momentum and a is the radius of interaction1l (a "'10-rscm).

Backward Amplitudes for Meson-Baryon Scattering and Average Radius of Interaction