Fission of <sup>205,207,209</sup>Bi Isotopes Using Proton-Bombardment of <sup>204,206,208</sup>Pb

ORAL

Abstract

Fission mass distributions for 205,207,209Bi nuclei at excitation energies close to their fission barriers were measured to determine how the mass distributions change with excitation energy and the neutron number of the compound nucleus1. Proton beams at various energies were delivered by the 14UD Tandem Electrostatic Accelerator at the Australian National University Heavy Ion Accelerator Facility. Fission fragments were measured using the CUBE fission spectrometer and fission fragment mass distributions were determined using a newly developed time difference analysis method. Measured mass distributions of all three Bi isotopes exhibit a component of mass-asymmetric fission at all energies studied. Comparisons between the three Bi isotopes at similar excitation energies hint at an increase in the mass-symmetric fission yield with increasing neutron number, which could be due to a decrease in the difference between the symmetric and asymmetric fission barriers.  The probability of mass-asymmetric fission decreases significantly with increasing excitation energy, from ~ 70% to ~ 40% over a 10 MeV range. The mass distributions were compared with GEF2 and PES3 semiempirical models.

  1. 1) B.M.A. Swinton-Bland, M.A. Stoyer, A.C. Berriman, et al., Phys. Rev. C 102, 054611 (2020).

    2) K.-H. Schmidt, B. Jurado, C. Amouroux, and C. Schmitt, Nucl. Data Sheets 131, 107 (2016).

    3) P. Möller and J. Randrup, Phys. Rev. C 91, 044316 (2015).

*This work performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07 NA27344. The authors acknowledge support from the Australian Research Council through Discovery Grants No. DP170102318, DP170102423, P190100256, and DP200100601.

Presenters

  • Mark A Stoyer

    • Lawrence Livermore National Laboratory
    • Lawrence Livermore Natl Lab

Authors

  • Mark A Stoyer

    • Lawrence Livermore National Laboratory
    • Lawrence Livermore Natl Lab
  • Ben M Swinton-Bland

    • Australian National University
  • David J Hinde

    • Australian National University
  • Annette C Berriman

    • Australian National University
  • C. Simenel

    • Australian National University
    • The Australian National University
    • Department of Theoretical Physics and Department of Nuclear Physics, Research School of Physics, The Australian National University, Canberra ACT 2601, Australia
  • J Buete

    • Australian National University
  • Kaushik Banerjee

    • VEEC
  • Lauren Bezzina

    • Australian National University
  • Ian P Carter

    • Australian National University
  • Kaitlin J Cook

    • Michigan State University
  • Mahananda Dasgupta

    • Australian National University
  • D Y Jeung

    • Australian National University
  • J Buete

    • Australian National University
  • Edward C Simpson

    • Australian National University
  • J Buete

    • Australian National University
  • Kirsten Vo-Phuoc

    • Australian National University