Abstract

From the momentum space Faddeev equations we derive approximate expressions which describe the Coulomb-nuclear interference in the three-body elastic scattering, rearrangement, and breakup problems and apply the formalism to $p\ensuremath{-}d$ elastic scattering. The approximations treat the Coulomb interference as mainly a two-body effect, but we allow for the charge distribution of the deuteron in the $p\ensuremath{-}d$ calculations. Real and imaginary parts of the Coulomb correction to the elastic scattering phase shifts are described in terms of on-shell quantities only. In the case of pure Coulomb breakup we recover the distorted-wave Born approximation result. Comparing the derived approximation with the full Faddeev $p\ensuremath{-}d$ elastic scattering calculation, which includes the Coulomb force, we obtain good qualitative agreement in $S$ and $P$ waves, but disagreement in repulsive higher partial waves. The on-shell approximation investigated is found to be superior to other current approximations. The calculated differential cross sections at 10 MeV raise the question of whether there is a significant Coulomb-nuclear interference at backward angles.NUCLEAR STRUCTURE Coulomb effects, approximation formulas; three-body elastic scattering, rearrangement, breakup; applied to $p\ensuremath{-}d$ scattering.

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