We use a phenomenological nucleus-nucleus optical potential constructed in the light of a potential developed by Ginocchio[1] to study the elastic angular distributions of different nuclear systems near Coulomb barrier. The differential cross section ratios of elastic to Rutherford are studied for systems 14 N+ 56 Fe and 14 N+ 90 Zr for several colliding energies. Our theoretical predictions are well competitive with the experimental data, and the significantly small imaginary part of the potential explains the elastic scattering cross section and threshold anomaly in both systems.

A phenomenological optical potential is used to study the elastic angular distributions for the 19 F + 208 Pb system close to the Coulomb barrier. This potential is constructed by taking into account the flexible potential developed by Ginocchio. The fluctuations in the real and imaginary parts of the optical model potential follow the trends of the threshold anomaly. The set of optical potential parameters needed to analyze the fusion cross sections of the same system are obtained through analysis of the scattering cross sections. Theoretical fusion cross sections and results from four different experimental groups well agree for a range of energies. Several fluorine (F) isotopes are used as projectiles in this study of fusion cross sections by slightly altering the radial parameter. It was found that the fusion process occurs unfettered in the 19 F + 208 Pb system below the Coulomb barrier but is seriously hindered in the case of its isotopic projectiles.