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Abstract The real part of the interaction potential between two heavy ions is derived by folding the density distribution of one nucleus with the real part of the single nucleon potential of the other. In this study, the folowing two cases are considered: a)assuming the density distribution and single - nucleon optical potential to have Woods-Saxon form factors, with parameters adjusted to fit the experimental value of the critical angular momentum. b) adopting a density-dependent effective two body force with a Gaussian distribution and adjustable parameters to describe the densities. |