Fission fragment anisotropies and mass distributions have been measured to high accuracy, over a wide range of angles, for the ${}_{}{}^{16}{}_{}{}^{}\mathrm{O}$ + ${}_{}{}^{238}{}_{}{}^{}\mathrm{U}$ reaction. The bombarding energies spanned the fusion barrier distribution, in steps of 1 MeV. Fission following transfer reactions was rejected by making use of the deduced velocity vectors of the fissioning nuclei. The resulting mass distributions for full momentum transfer fission show a small but significant skewness, which increases as the beam energy falls through the fusion barrier region, displaying a similar energy dependence as the fission fragment angular anisotropies. This is conclusive evidence for the interpretation that collisions with the tips of the deformed ${}_{}{}^{238}{}_{}{}^{}\mathrm{U}$ target nuclei lead to quasifission, while collisions with the sides result in fusion-fission. © 1996 The American Physical Society.

• Received 10 November 1995

DOI:https://doi.org/10.1103/PhysRevC.53.1290