25–29 sept. 2023
Soustons
Fuseau horaire Europe/Paris

Evolution of the N=50 shell gap: new insights from spectroscopic data on 82Ge

28 sept. 2023, 09:50
20m
Oral Presentation Nuclear Structure Shell evolution

Orateur

Dr THISSE, Damien (CEA)

Description

The evolution of the N = 50 single-particle gap size from β stability towards the exotic 78Ni, at the origin of the magic nature of the N = 50 isotones, is still poorly understood. Experimental data indicate that the size of the effective N = 50 gap continuously decreases from stability down to Z = 32 [1]. This reduction must certainly be followed by a stabilization around Z = 30, a phenomenon that has still not received any theoretical explanation.

In 2018, the ν-Ball campaign took place at the ALTO facility of Orsay [2]. The γ-spectrometer was made of 34 HPGe detectors to perform high resolution γ-spectroscopy, coupled to 20 LaBr3 scintillators enabling the realization of fast-timing measurements. During this campaign, medium-spin yrast and near-yrast states of neutron-rich nuclei were successfully populated in the fission of a 232Th target exposed to the quasi-mono-energetic fast-neutron flux generated by LICORNE. Among all the reaction products, the N = 50 nucleus 82Ge have been identified. In this presentation, I will show results focusing on the new spectroscopic data obtained for the nucleus 82Ge [3]. Indeed, using double and triple γ coincidences in the HPGe of ν-Ball, we were able to add two new transitions and one excited state in its level scheme. The latter is interpreted as the 7+ state originating from the N = 50 core-breaking configuration ν(1g$_{9/2}$)$^{−1}$ν(2d$_{5/2}$)$^1$, and we discuss the relationship between its observed excitation energy and the effective N = 50 shell gap amplitude at Z = 32. This new information is used to quantify the evolution of the N = 50 gap from Z = 38 down to Z = 32. According to our analysis, the gap slope is almost three times as high as the one obtained in Ref. [1]. We propose for the first time to explain this
evolution by the effect of the isospin asymmetry of the pseudo-spin symmetry in this region [4].

In the future, at GANIL, there will be the opportunity to study N = 50 isotones on the neutron deficient side at the DESIR facility. The possibility to study nuclei close the N = Z line, near the doubly magic 100Sn nucleus, will allow to further study the role of the isospin asymmetry of the pseudo-spin symmetry in the evolution of the nuclear orbitals.

Références
[1] M.-G. Porquet and O. Sorlin, Evolution of the N = 50 gap from Z = 30 to Z = 38 and extrapolation toward 78Ni., Phys. Rev. C 85, 014307 (2012)
[2] M. Lebois et al., The ν-ball γ- spectrometer, NIM A 960, 163580 (2020)
[3] D. Thisse et al., Article submitted to EPJ A in January 2023
[4] H. Liang et al., Hidden pseudospin and spin symmetries and their origins in atomic nuclei, Phys. Rep. 570, 1-84 (2015)

Auteur principal

Co-auteurs

LEBOIS, Matthieu (Institut de Physique Nucléaire d'Orsay) VERNEY, David (IPN Orsay) Dr WILSON, Jonathan (IJC Lab, Orsay, France)

Documents de présentation