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Insight on the structure of 100Zr through lifetime measurements at GRIFFIN

2 Sept 2026, 13:00
15m
Oral presentation Parallel Session 1 (Hall B)

Speaker

Konstantin Stoychev (University of Guelph, Canada)

Description

The sudden onset of deformation in $A\approx100$ nuclei at $N=60$ has been described as a ground-state shape transition that has raised a lot of interest over the years from an experimental and theoretical point of view [1]. This transition is most pronounced in the Zr and Sr isotopic chains where the low-energy excited-state structure shows significant signs of deformation developing at $N=60$, as opposed to the spherical-like structure observed at $N\leq58$.

At present, the two most promising theoretical interpretations of this phenomenon are given by the Monte Carlo Shell Model (MCSM) [2] and the Interacting Boson Model with Configuration Mixing (IBM-CM) [3]. The MCSM calculations interpret the structure of $^{100}$Zr within a multiple-shape-coexistence scenario with several distinct deformed shapes predicted for the lowest $0^+$ states, with rotational bands built on top of them. In contrast, the IBM-CM calculations predict a weakly-deformed "intruder" ground-state configuration in $^{100}$Zr, with corresponding $\beta$ and $\gamma$ bands, and a low-lying spherical "normal" configuration.

In order to test these theoretical models an experiment was performed at the TRIUMF-ISAC facility to investigate the structure of $^{100}$Zr following the $\beta$ decay of $^{100}$Y by utilizing the GRIFFIN $\gamma$-ray spectrometer [4]. The 15 HPGe clover detectors of GRIFFIN were coupled with seven LaBr$_3$ detectors for fast-timing lifetime measurements using the Generalized Centroid Difference method [5].

Mainly low-spin excited states were populated in the $\beta$ decay of the $1^-$ state in $^{100}$Y. This allowed for the lifetimes of several key non-yrast excited states in $^{100}$Zr, including those of the $2^+_3$, and $0^+_3$ states, to be extracted for the first time in this study. These new results will be presented and compared to the MCSM and IBM-CM theoretical predictions.

[1] P.E. Garrett et al., Prog. Part. Nucl. Phys. 124 (2022) 103931.

[2] T. Togashi et al., Phys. Rev. Lett. 117 (2016) 172502.

[3] N. Gavrielov et al., Phys. Rev. C 99, 064324 (2019).

[4] A.B. Garnsworthy et al., Nucl. Instrum. Methods Phys. Res., Sect. A, 918 (2019).

[5] J.-M. Régis et al., Nucl. Instrum. Methods Phys. Res., Sect. A, 726 (2013).

Author

Konstantin Stoychev (University of Guelph, Canada)

Co-authors

Harris Bidaman (University of Guelph) Desislava Kalaydjieva (University of Guelph) Paul Garrett (University of Guelph) Vinzenz Bildstein (University of Guelph) Magda Zielinska (CEA Saclay) Marco Rocchini (INFN Firenze, Italy) Sangeet Pannu (University of Guelph) Wolfram Korten (CEA Saclay) Adam Garnsworthy (TRIUMF)

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