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    Measurement and analysis of the incomplete fusion strength function in the C12(Elab=4A–7A MeV)+Te130 system to probe entrance-channel dependence

    Subham Kumar1,*, Amanjot1, Priyanka1, Malika Kaushik1,†, Rupinderjeet Kaur1, Rudra N. Sahoo1,‡, Manoj K. Sharma2, Yashraj Jangid3, and Pushpendra P. Singh1,§

    • *Contact author: subham.19phz0013@iitrpr.ac.in
    • †Present address: Università degli Studi di Napoli Federico II, Naples, Campania, Italy.
    • ‡Present address: Institute of Physics, Bhubaneswar, Odisha 751005, India.
    • §Contact author: pps@iitrpr.ac.in

    Phys. Rev. C 114, 044619 – Published 15 October, 2026

    DOI: https://doi.org/10.1103/rxbt-rh1p

    Abstract

    To investigate low-energy incomplete fusion (ICF) dynamics, the excitation functions (EFs) of different evaporation residues (ERs) produced in C12+Te130 system were measured in the 4–7 MeV/nucleon energy range using the recoil-catcher activation technique followed by off-line γ-ray spectroscopy and analyzed in the framework of statistical model code pace4. It has been found that cross sections for xn channels were well reproduced by the code, suggesting that they originate from complete fusion (CF) reactions. In contrast, the α-emitting channels display a marked enhancement over theoretical predictions, pointing to the contribution of incomplete fusion (ICF) processes arising from projectile breakup. To quantify these effects, the ICF fraction (FICF) has been deduced and analyzed as a function of projectile energy, mass asymmetry, Coulomb factor ZPZT, deformation parameter β2, and the α-separation energy of the projectile Qα. The results show that FICF increases with projectile energy and shows systematic dependence on mass asymmetry and ZPZT. However, comparisons with earlier studies reveal that these parameters alone are insufficient to fully account for the observed strength of ICF, underscoring the role of projectile structure and Qα. Additionally, the angular-momentum distributions calculated using ccfull indicate that, at the studied energies, both CF and ICF contributions arise from partial waves with ℓ<ℓcrit, suggesting a diffused angular-momentum boundary rather than a sharp cutoff for the onset of ICF.

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