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    Fission and quasifission studies in the Si30+Au197 reaction

    B. Ashna1,*, M. Shareef1,2, A. Shamlath1,3, P. V. Laveen1,4, A. C. Visakh1, A. Jhingan5, A. K. Nasirov6,7, E. D. Khusanov7,8, Jhilam Sadhukhan9 et al.

    N. Saneesh5, K. S. Golda5, Mohit Kumar5, S. K. Duggi10, Shiva Prasad Nayak1, S. Ramakrishna Reddy11, K. Prameela11, S. Appannababu11, P. V. Madhusudhana Rao11, A. M. Vinodkumar12, P. Sugathan5, and E. Prasad1,†

    • *Contact author: ashna.pph072205@cukerala.ac.in
    • †Contact author: prasadenair@cukerala.ac.in

    Phys. Rev. C 113, 034606 – Published 12 March, 2026

    DOI: https://doi.org/10.1103/js52-tnp5

    Abstract

    Background: Quasifission substantially hinders the formation of the compound nucleus in heavy ion fusion reactions. It poses a major obstacle to superheavy element formation. This process has a strong entrance channel dependence.

    Purpose: To study the interplay between fission and quasifission in Si30+Au197 reaction at energies around the Coulomb barrier.

    Methods: Binary fragments from Si30+Au197 reaction were measured in coincidence using a pair of large area multiwire proportional counters. The mass-ratio and mass angle distributions of the fragments were obtained using the kinematic re-construction method. Experimental results are interpreted using different theoretical methods. Further, the results of present reaction have been compared with that of Si28+Au197 reaction available in literature.

    Results: Broadened mass ratio distributions have been observed in the range of energy studied compared to the theoretical calculations assuming compound nucleus formation. No mass angle correlation is observed. Fission fragment mass distribution of the present reaction is compared with that of other neptunium isotopes at low excitation energies. A fast transition from asymmetric fission to symmetric fission is observed with decrease of N/Z along the isotopic chain of neptunium. The difference between the asymmetric and symmetric fission barrier is higher for the Np238 at all temperatures, compared to Np225,227 resulting in asymmetric mass division in the fission of Np238 and symmetric split at low excitation energies in Np225,227. Calculated quasifission yields in the mass range 80≤A≤150 show significant dependence on collision energy for both Si28,30+Au197 reactions.

    Conclusions: Measured fragment mass distribution has significant contribution from slow quasifission in Si30+Au197 reaction. 40–60% fusion probability is obtained for the Si28,30+Au197 reactions. Quasifission yields show strong dependence on energy and angular momentum.

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