Antisymmetric Treatment of Deuteron-Stripping Reaction Stripping and Heavy-Particle-Stripping Reactions

The deuteron stripping reaction is formulated using completely antisymmetric wave functions. The amplitude of the reaction is represented as a sum of "ordinary" stripping and heavy-particle-stripping amplitudes. Analogous to the case of the ordinary stripping, the amplitude of the heavyparticle- stripping can be represented in terms of three reduced width amplitudes of bound nucleons, e.g. those of the captured neutron and proton in the residual nucleus and that of the emitted proton in the target nucleus, or alternatively, in terms of two reduced width amplitudes of the emitted proton and captured deuteron in bound states. This formalism enables calculations of both angular distributions and "magnitudes" of heavy-particle-stripping cross sections. For simplicity, the cutoff Born approximation is employed, though its generalization can be performed easily, as is discussed.