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[en] The angular distribution functions for the cascades p bar p → 3D2 → XJγ1 → (ψγ2)γ1 → ([e+e-]γ2)γ1 with J=0, 1, 2, are computed in terms of the angular momentum helicity amplitudes. A measurement of each of these distribution functions would yield enough information to determine both the real and imaginary parts of the individual amplitudes of the various steps of the cascades
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