Abstract

Experimental differential cross sections for the elastic scattering of $^{16}\mathrm{O}$ from $^{63}\mathrm{Cu}$ at ${E}_{\mathrm{lab}}=40, 42, \mathrm{and} 46$ MeV and $^{65}\mathrm{Cu}$ at ${E}_{\mathrm{lab}}=41 \mathrm{and} 46$ MeV are presented. The data are analyzed using a four parameter Woods-Saxon optical potential. Optical parameters are presented and it is verified that the experimental data are sensitive to the value of the real nuclear optical potential [$\mathrm{Re}{U}_{\mathrm{opt}}^{N}(r)$] and its slope near the strong absorption radius (${D}_{\frac{1}{2}}$). Fits to the data are also obtained using the real nuclear potentials given by two theoretical models\char22{}the adiabatic model of Nix and collaborators and a $G$-matrix double folding model. The potentials from the $G$-matrix model give a better description of the data than the potentials from the adiabatic model. The latter have too small a slope. A possible explanation for this deficiency is suggested.

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