Abstract
The volume part of the phenomenological optical potential is interpreted in terms of the microscopic theory of nuclear matter. The latter is based on the Brueckner-Hartree-Fock approach with a new version of three-body force, reproducing the empirical saturation properties of nuclear matter. The self-energy is calculated and its on-shell matrix elements are related to the volume part of the optical potential. A comparison is made with a recent parametrization of the optical model potential fitting the experimental nucleon-nucleus elastic scattering. The isospin effects and Coulomb corrections are emphasized.
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