Tanaka, T.Hinde, DavidDasgupta, M.Williams, E.Vo-Phuoc, K.Simenel, C.Simpson, E. C.Jeung, D. Y.P. Carter, I.Cook, K. J.Lobanov, N. R.Luong, D. H.Palshetkar, C.Rafferty, D. C.Ramachandran, K.2024-07-262024-07-262469-9985https://hdl.handle.net/1885/733714207Background: Mass and angle distribution measurements have illuminated many aspects of the physical variables controlling quasifission. However, mapping from detection angle to reaction time is clouded by the wide range of contributing angular momenta L h̄, ranging from 0h̄ to the maximum of the reaction ( 100h̄), which complicates the mapping, and thus limits our understanding of the reaction dynamics. Purpose: To investigate the angular momentum dependence of the reaction dynamics in quasifission and determine the fission fragment mass evolutions in the reaction. Method: The mass and angular distributions of products of the reactions 52 Cr + 198 Pt and 54 Cr + 196 Pt were measured. The distributions were compared with quasifission simulation results. Results: Mass angle distributions are reproduced by utilizing a new quasifission mass evolution model, and including a mass-symmetric component associated with low L. The latter increases in yield at higher beam energy. Conclusions: The symmetric component represents the total of slow quasifission and fusion-fission. The increase in contribution with energy above the Coulomb barrier suggests that an extra-push energy is required to achieve fusion.The authors acknowledge the Australian Research Council for support through Discovery Grants No. DP200100601, No. DP190100256, No. DP190101442, No. DP170102318, and No. DE140100784. Financial support from the NCRIS HIA capability for operation of the Heavy Ion Accelerator Facility is acknowledged. The authors thank T. Kibédi for his key role in operation of the Linacapplication/pdfen-AU© 2023 American Physical SocietyNuclear physics202310.1103/PhysRevC.107.054601