Shape polarization in the tin isotopes near N = 60 from precision g-factor measurements on short-lived 11/2− isomers

The g factors of 11/2− isomers in semimagic 109Sn and 111Sn (isomeric lifetimes τ=2.9(3) ns and τ=14.4(7) ns, respectively) were measured by an extension of the Time Differential Perturbed Angular Distribution technique, which uses LaBr3 detectors and the hyperfine fields of a gadolinium host to ach...

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Bibliographic Details
Main Authors: T.J. Gray, A.E. Stuchbery, J. Dobaczewski, A. Blazhev, H.A. Alshammari, L.J. Bignell, J. Bonnard, B.J. Coombes, J.T.H. Dowie, M.S.M. Gerathy, T. Kibédi, G.J. Lane, B.P. McCormick, A.J. Mitchell, C. Nicholls, J.G. Pope, P.-G. Reinhard, N.J. Spinks, Y. Zhong
Format: Article
Language:English
Published: Elsevier 2023-12-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269323006020
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Summary:The g factors of 11/2− isomers in semimagic 109Sn and 111Sn (isomeric lifetimes τ=2.9(3) ns and τ=14.4(7) ns, respectively) were measured by an extension of the Time Differential Perturbed Angular Distribution technique, which uses LaBr3 detectors and the hyperfine fields of a gadolinium host to achieve precise measurements in a new regime of short-lived isomers. The results, g(11/2−;109Sn)=−0.186(8) and g(11/2−;111Sn)=−0.214(4), are significantly lower in magnitude than those of the 11/2− isomers in the heavier isotopes and depart from the value expected for a near pure neutron h11/2 configuration. Broken-symmetry density functional theory calculations applied to the sequence of 11/2− states reproduce the magnitude and location of this deviation. The g(11/2−) values are affected by shape core polarization; the odd 0h11/2 neutron couples to Jπ=2+,4+,6+... configurations in the weakly-deformed effective core, causing a decrease in the g-factor magnitudes.
ISSN:0370-2693