# Microsecond Isomer at the N=20 Island of Shape Inversion Observed at   FRIB

**Authors:** T. J. Gray, J. M. Allmond, Z. Xu, T. T. King, R. S. Lubna, H. L., Crawford, V. Tripathi, B. P. Crider, R. Grzywacz, S. N. Liddick, A. O., Macchiavelli, T. Miyagi, A. Poves, A. Andalib, E. Argo, C. Benetti, S., Bhattacharya, C. M. Campbell, M. P. Carpenter, J. Chan, A. Chester, J., Christie, B. R. Clark, I. Cox, A. A. Doetsch, J. Dopfer, J. G. Duarte, P., Fallon, A. Frotscher, T. Gaballah, J. T. Harke, J. Heideman, H. Huegen, J. D., Holt, R. Jain, N. Kitamura, K. Kolos, F. G. Kondev, A. Laminack, B., Longfellow, S. Luitel, M. Madurga, R. Mahajan, M. J. Mogannam, C. Morse, S., Neupane, A. Nowicki, T. H. Ogunbeku, W.-J. Ong, C. Porzio, C. J. Prokop, B., C. Rasco, E. K. Ronning, E. Rubino, T. J. Ruland, K. P. Rykaczewski, L., Schaedig, D. Seweryniak, K. Siegl, M. Singh, A. E. Stuchbery, S. L. Tabor, T., L. Tang, T. Wheeler, J. A. Winger, J. L. Wood

arXiv: 2302.11607 · 2023-06-28

## TL;DR

This paper reports the first observation of a microsecond isomer at the N=20 island of shape inversion at FRIB, providing insights into nuclear shape coexistence and the underlying structure of $^{32}$Na and $^{32}$Mg.

## Contribution

It presents the discovery of a unique microsecond isomer in $^{32}$Na, linking experimental data with shape coexistence and theoretical models of nuclear deformation.

## Key findings

- Observed a 24(2)-μs isomer in $^{32}$Na
- Identified the isomer as related to shape coexistence in $^{32}$Mg
- Supports deformation-dominated low-lying states in this region

## Abstract

Excited-state spectroscopy from the first Facility for Rare Isotope Beams (FRIB) experiment is reported. A 24(2)-$\mu$s isomer was observed with the FRIB Decay Station initiator (FDSi) through a cascade of 224- and 401-keV $\gamma$ rays in coincidence with $^{32}\textrm{Na}$ nuclei. This is the only known microsecond isomer ($1{\text{ }\mu\text{s}}\leq T_{1/2} < 1\text{ ms}$) in the region. This nucleus is at the heart of the $N=20$ island of shape inversion and is at the crossroads of spherical shell-model, deformed shell-model, and ab initio theories. It can be represented as the coupling of a proton hole and neutron particle to $^{32}\textrm{Mg}$, $^{32}\textrm{Mg}+\pi^{-1} + \nu^{+1}$. This odd-odd coupling and isomer formation provides a sensitive measure of the underlying shape degrees of freedom of $^{32}\textrm{Mg}$, where the onset of spherical-to-deformed shape inversion begins with a low-lying deformed $2^+$ state at 885 keV and a low-lying shape-coexisting $0_2^+$ state at 1058 keV. We suggest two possible explanations for the 625-keV isomer in $^{32}$Na: a $6^-$ spherical shape isomer that decays by $E2$ or a $0^+$ deformed spin isomer that decays by $M2$. The present results and calculations are most consistent with the latter, indicating that the low-lying states are dominated by deformation.

## Full text

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## Figures

5 figures with captions in the complete paper: https://tomesphere.com/paper/2302.11607/full.md

## References

70 references — full list in the complete paper: https://tomesphere.com/paper/2302.11607/full.md

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Source: https://tomesphere.com/paper/2302.11607