الفهرس 
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Abstract
between two nuclei whosB mass numbers satisfying the ·1/31/1 condition CA1 . + A2) ~ 8.12. For very heavy nuclei or ·1/3 1/3 for nuclei with(A1 + A2) 8.12 the folding model produces weaker potentials at the Coulomb barrier. approximated by the product of a geometr.ic~l· factor, depending on the shapes of the interacting nuclei, and