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    Systematic study of fusion-fission and quasifission in reactions using a Au197 target

    Shiva Prasad Nayak1,*, E. Prasad1,2,†, D. J. Hinde2, M. Dasgupta2, C. Simenel2,3, K. J. Cook2, E. C. Simpson2, J. Walshe2, D. Y. Jeung2 et al.

    C. Sengupta2,‡, K. Vo-Phuoc2,§, J. F. Smith2,∥, I. P. Carter2, H. Albers4, J. Khuyagbaatar4, and Ch. E. Düllmann4,5,6

    • *Contact author: nayakshiva011.spn@gmail.com
    • †Contact author: prasadenair@cukerala.ac.in
    • ‡Present address: Image X Institute, University of Sydney, Central Clinical School, Sydney, Australia.
    • §Present address: Airservices Australia, Alan Woods Building, 25 Constitution Ave, Canberra ACT 2600, Australia.
    • ∥Present address: Advanced Technology Institute, University of Surrey, Guildford, Surrey GU2 7XH, United Kingdom.

    Phys. Rev. C 113, 064605 – Published 11 June, 2026

    DOI: https://doi.org/10.1103/vmdx-klxv

    Abstract

    Background: Quasifission is a nonequilibrium phenomenon that strongly suppresses the formation of heavy nuclei in heavy-ion fusion reactions. This process shows a strong entrance channel dependence. Understanding quasifission is crucial for exploring potential avenues to synthesize new superheavy elements and their isotopes.

    Purpose: To study the interplay of fusion-fission and quasifission with increasing ZpZt for the reactions using Au197 as the target. To explore the variation of average sticking time in these reactions with a constant target deformation.

    Methods: The mass-angle distributions of fission and fission-like fragments were measured for seven reactions using Au197 as the target at energies near the Coulomb barrier. Negligible sequential fission is expected in these reactions; thus, the measured binary products represent the total quasifission yield. Pulsed beams of S32,36, Ca48, Ti50, Cr54, Fe58, and Ni64 were used in the study. A systematic analysis of mass ratio distributions and mass widths has been carried out. The experimental mass-angle distribution is simulated following a phenomenological approach. The average sticking time for the fast quasifission is extracted from the simulations.

    Results: Dominant mass-symmetric fission fragments with a slight mass-angle correlation are observed in the most mass-asymmetric (S32,36+Au197) reactions. In contrast, a U-shaped mass ratio distribution has been observed in the most symmetric (Ni64+Au197) reaction. A sharp decrease in fusion probability is inferred with increasing ZpZt. The width of the mass ratio distribution is found to increase exponentially with the increase in mean fissility for a fixed beam energy relative to the barrier. The average sticking time of fast quasifission is found to vary from approximately 14 to 15 zeptoseconds to approximately 4 to 5 zeptoseconds for the systems under study.

    Conclusion: The observed transition from a dominant symmetric mass split to an asymmetric mass split with mass-angle correlations indicates the increasing probability of fast quasifission and fusion suppression with increasing ZpZt. The observation is correlated with the sharp fall in the extracted average sticking time with increasing ZpZt from 1264 to 2212.

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