Angular distributions of fragments emitted in the reaction ${}_{}{}^{19}{}_{}{}^{}\mathrm{F}$${+}^{63}$Cu measured in the range ${\mathrm{\theta }}_{\mathrm{lab}}$=10° to 120° at incident energy between 100 to 108 MeV (lab) have been analyzed according to available models for deep inelastic collisions with the aim to evidence different mechanisms contributing to such reactions. The analysis was performed in the framework of Strutinsky model taking into account both the development of Kun and of Abul-Magd and Simbel. To determine the interaction times, previously published excitation functions were also analyzed in the framework of Kun’s model of cross section statistical fluctuations and near-side and far-side scattering were taken into account separately. It was pointed out that the rotational energy dissipation occurs in a limited angular range around the grazing angle. The presence of two distinct reaction mechanisms, each of them characterized by an interaction time, was also evidenced by comparing the energy averaged angular distributions to the Abul-Magd and Simbel model for dissipative collisions.

• Received 30 November 1989

DOI:https://doi.org/10.1103/PhysRevC.41.2062