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Study of the emergence of collectivity in 131I and 133I isotopes in the vicinity of the doubly magic 132Sn nucleus

2 Sept 2026, 20:15
15m
Oral presentation Parallel Session 2 (Hall B)

Speaker

Katarzyna Gajewska (IFJ PAN/IJCLab)

Description

The emergence of collectivity can be explored by studying nuclei that differ from closed-shell configurations by a few particles or holes, involving both protons and neutrons. In this context, the regions around the doubly magic nuclei 208Pb and 132Sn provide ideal testing grounds for such investigations. This can be achieved by measuring the electric quadrupole moments associated with the first pure E2 excitations, as well as the E2 components of the first mixed M1 + E2 transitions.

In the 208Pb region, for the 209Po (2p–1h), 211Rn (4p–1h), and 213Ra (6p–1h) isotones, a systematic increase of the E2 transitions strength was found, originating from growing contributions of additional protons along the N=125 chain [1]. Similarly, in the 132Sn region, an increase of collectivity was observed in 129Sb for the states of the 2+(128Sn)⊗πg7/2 multiplet with respect to the 128Sn core [2]. Recently, the lifetime of the analogous 2+(130Sn)⊗πg7/2 state in 131Sb was measured by our collaboration [3]. The deduced probability of the E2 transition showed a value similar to that of the 130Sn core, in accordance with the weak-coupling limit, but in contrast with the 129Sb results. To shed more light on this behavior, in the present work the electric quadrupole transition probabilities were investigated in the 131I and 133I isotopes, which contain two additional protons compared with the 129Sb and 131Sb nuclei, respectively.

The 131I and 133I isotopes were produced during the thermal neutron induced fission of a 235U target at the Institut Laue-Langevin (ILL). The isotopes of interest were separated from all fission products using the LOHENGRIN spectrometer [4] according to their A/q and E/q mass-to-charge and energy-to-charge ratios. The 11/2+ and 5/2+ states, which decay via E2 and M1+E2 transitions, respectively, in 131,133I, were populated via the β-decay of 131,133Te isotopes. The lifetimes of the 11/2+ and 5/2+ levels were measured using the fast-timing technique [5] with two HPGe clover detectors and four LaBr3(Ce) scintillators.

The lifetimes of the low-lying states in the 133I isotope were measured for the first time in the present analysis. The corresponding states in 131I were remeasured with high precision. For both nuclei, a systematic increase in collectivity beyond the weak-coupling limit was observed. The experimental results will be supported by realistic shell-model calculations, providing deeper insight into the nature of the emergence of collectivity in the vicinity of the doubly magic 132Sn nucleus.

References:

[1] M. Gerathy et al., Phys. Lett. B 823, 136738 (2021).
[2] T. J. Gray et al., Phys. Rev. Lett. 124, 032502 (2020).
[3] S. Bottoni et at., Phys. Rev. C 107, 014322 (2023).
[4] P. Armbruster et al., Nucl. Instrum. Methods 139, 213 (1976).
[5] H. Mach, R. Gill, and M. Moszyński, Nucl. Instrum. Methods Phys. Res., Sect. A 280, 49 (1989).

Author

Katarzyna Gajewska (IFJ PAN/IJCLab)

Co-authors

Ł.W. Iskra (Institute of Nuclear Physics Polish Academy of Sciences, PL-31342 Krakow, Poland) Bogdan Fornal (IFJ PAN, Krakow) S. Bottoni (UNIMI and INFN-MI) E. Gamba (UNIMI and INFN-MI) S. Leoni (UNIMI and INFN-MI) F.C.L. Crespi (Università degli Studi di Milano e INFN sezione di Milano Via Celoria, 16, 20133 Milano, Italy) N. Cieplicka-Oryńczak (Institute of Nuclear Physics Polish Academy of Sciences, PL-31342 Krakow, Poland) Giacomo Colombi (University of Guelph) Y. H. Kim (Center for Exotic Nuclear Studies, Institute for Basic Science, Daejeon 34126, Republic of Korea) Ulli Köster (Institut Laue-Langevin, Grenoble) Caterina Michelagnoli (Institut Laue-Langevin, Grenoble) F. Dunkel (Universität zu Köln, Institut für Kernphysik) A. Esmaylzadeh (Institut für Kernphysik, Universität zu Köln) L. Gerhard (Universität zu Köln, Institut für Kernphysik) J. Jolie (Institut für Kernphysik, Universität zu Köln) L. Knafla (Universität zu Köln, Institut für Kernphysik) M. Ley (Institut für Kernphysik, Universität zu Köln, Zülpicher Straße 77, 50937 Köln, Germany) J. - M. Régis (Universität zu Köln, Institut für Kernphysik) K. Schomaker (Universität zu Köln, Institut für Kernphysik)

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