Universality of shell effects in fusion-fission mass distributions

We present the results of a broad, systematic study of heavy-ion induced fission mass distributions for every even-Z compound nucleus ( Z CN ) from 144 Gd to 212 Th. We find systematic evidence of shell-driven structure in every fission mass distribution. The change in shape of the mass distributions with Z CN is consistent with the results of quantitative simultaneous fitting in mass and total kinetic energy, demonstrating that fragment proton shell gaps at Z FF = 34 , 36 and Z FF = 44 , 46 are both major drivers of fission mass distributions below the actinide region. The mass distributions show enhanced yields at mass symmetry for values of Z CN equal to two times these favoured Z FF values. Thus, the same shell gaps that are drivers of mass-asymmetric fission also affect mass distributions at and near mass-symmetry. For all systems a second, more mass-asymmetric, fission mode is required to fit the fission mass distributions. If driven by a single shell gap, it appears to be in the light fragment around Z FF = 28 , 30 .

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Publication Details

Journal
Physics Letters B
Published
2025-04-08
DOI
https://doi.org/10.1016/j.physletb.2025.139459
Citations
4
Primary Topic
Nuclear physics research studies
Type
article
Field-Weighted Citation Impact
7.48
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article

Universality of shell effects in fusion-fission mass distributions

K. Banerjee, I.P. Carter, M. Dasgupta, D. J. Hinde et al.
4 citations
Physics Letters B
Nuclear physics research studies
7.48
article

Universality of shell effects in fusion-fission mass distributions

K. Banerjee, I.P. Carter, M. Dasgupta, D. J. Hinde, L. T. Bezzina, B. M. A. Swinton-Bland, C. Sengupta, J. Buete, K. J. Cook, D. Y. Jeung, A. C. Berriman, C. Simenel, E. C. Simpson
article en
4 citations

Abstract

We present the results of a broad, systematic study of heavy-ion induced fission mass distributions for every even-Z compound nucleus ( Z CN ) from 144 Gd to 212 Th. We find systematic evidence of shell-driven structure in every fission mass distribution. The change in shape of the mass distributions with Z CN is consistent with the results of quantitative simultaneous fitting in mass and total kinetic energy, demonstrating that fragment proton shell gaps at Z FF = 34 , 36 and Z FF = 44 , 46 are both major drivers of fission mass distributions below the actinide region. The mass distributions show enhanced yields at mass symmetry for values of Z CN equal to two times these favoured Z FF values. Thus, the same shell gaps that are drivers of mass-asymmetric fission also affect mass distributions at and near mass-symmetry. For all systems a second, more mass-asymmetric, fission mode is required to fit the fission mass distributions. If driven by a single shell gap, it appears to be in the light fragment around Z FF = 28 , 30 .

Physics Letters BVol. 865
Australian National University (AU), Michigan State University (US)
Openalex Percentile: Top 4%
Nuclear physics research studies
7.48
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