https://doi.org/10.1140/epja/s10050-026-01859-8
Code Paper
QMFTMD a code for fission mass distribution within quantum mechanical fragmentation theory-application to Hg isotopes
Department of Physics, Bharathiar University, 641046, Coimbatore, Tamil Nadu, India
a
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Received:
10
January
2026
Accepted:
9
April
2026
Published online:
12
May
2026
Abstract
Experimental investigations using (p,f) and (
,f) reactions on nuclei near the
-stability line in the mass range A = 190–200 have revealed symmetric fission fragment distributions. However, the experimental observation of an asymmetric mass distribution in the
-delayed fission of excited
Tl has triggered renewed theoretical and experimental interest in understanding the fission dynamics within the pre-actinide region. We investigate the mass distribution of neutron-deficient to neutron-rich even-mass Hg isotopes in the mass range from 178 to 200 within the framework of the quantum mechanical fragmentation theory (QMFT) based on the two-centre shell model. A dedicated Python code QMFTMD has been developed to numerically evaluate fission fragment mass yield distributions. Without temperature and deformation effect,
Hg–
Hg show symmetric mass distributions, which become asymmetric from
Hg to
Hg. Introducing deformation (at
MeV) yields asymmetric distributions from
Hg–
Hg and symmetric ones from
Hg onward. With both deformation and temperature (
MeV), a similar trend persists with magnitude changes. The inclusion of nuclear deformation alone is sufficient to drive the transition from asymmetric to symmetric fission fragment mass distributions across the even-mass Hg isotopes. The results are compared with experimental data and GEF calculations for
Hg and
Hg. Overall, the obtained results successfully capture the qualitative features of the experimental trends in the pre-actinide region, providing an understanding of the mechanisms governing fission in neutron-deficient and neutron-rich mercury isotopes.
Copyright comment Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.
Communicated by Denis Lacroix.
© The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2026
Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.

