Issue |
EPJ Web Conf.
Volume 306, 2024
FUSION23 – International Conference on Heavy-Ion Collisions at Near-Barrier Energies
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Article Number | 01026 | |
Number of page(s) | 5 | |
DOI | https://doi.org/10.1051/epjconf/202430601026 | |
Published online | 18 October 2024 |
https://doi.org/10.1051/epjconf/202430601026
Spontaneous fission half-life in Fm isotopes with nuclear energy density functional
Center for Computational Sciences, University of Tsukuba, Tsukuba, 305-8577, Japan
* e-mail: washiyama@nucl.ph.tsukuba.ac.jp
Published online: 18 October 2024
A microscopic description of fission dynamics is important to understand the decay properties of neutron-rich heavy nuclei that are relevant to r-process nucleosynthesis. To provide a reliable and efficient method to evaluate the spontaneous fission half-life, we develop a method, called the constrained Hartree– Fock–Bogoliubov (CHFB) plus local quasiparticle random-phase approximation (LQRPA), to include dynamical residual effects in the collective inertia. With the CHFB + LQRPA, we evaluate the collective potential and the collective inertia along a mass-symmetric fission path in Fm isotopes with the neutron numbers N = 158–164. The obtained LQRPA inertia is much larger than the cranking one that ignores dynamical residual effects and shows a remarkable variation along the fission path. We estimate the fission half-life of the Fm isotopes using the action integral with the obtained collective potential and inertia. A large difference between the fission half-lives obtained with the LQRPA inertia and with the cranking inertia is observed. This indicates the importance of evaluating the collective inertia for estimating the fission half-life.
© The Authors, published by EDP Sciences, 2024
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