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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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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author 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
author_facet 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
author_sort T.J. Gray
collection DOAJ
description 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.
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spelling doaj.art-a3db4bfb25e94067873e389ef92978402023-11-26T05:11:21ZengElsevierPhysics Letters B0370-26932023-12-01847138268Shape polarization in the tin isotopes near N = 60 from precision g-factor measurements on short-lived 11/2− isomersT.J. Gray0A.E. Stuchbery1J. Dobaczewski2A. Blazhev3H.A. Alshammari4L.J. Bignell5J. Bonnard6B.J. Coombes7J.T.H. Dowie8M.S.M. Gerathy9T. Kibédi10G.J. Lane11B.P. McCormick12A.J. Mitchell13C. Nicholls14J.G. Pope15P.-G. Reinhard16N.J. Spinks17Y. Zhong18Department of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, Australia; Physics Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA; Corresponding author.Department of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaSchool of Physics, Engineering and Technology, University of York, York YO10 5DD, United Kingdom; Institute of Theoretical Physics, Faculty of Physics, University of Warsaw, PL-02-093 Warsaw, PolandInstitut für Kernphysik, Universität zu Köln, Zülpicher Sraße 77, D-50937, Köln, GermanyDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, Australia; College of Science and Arts in Turaif, Physics Department, Northern Border University, Saudi ArabiaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaSchool of Physics, Engineering and Technology, University of York, York YO10 5DD, United Kingdom; Université de Lyon, Institut de Physique des 2 Infinis de Lyon, IN2P3-CNRS-UCBL, 4 rue Enrico Fermi, 69622 Villeurbanne, FranceDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaInstitut für Theoretische Physik II, Universität Erlangen-Nürnberg, 91058 Erlangen, GermanyDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaDepartment of Nuclear Physics and Accelerator Applications, Research School of Physics, Australian National University, Canberra, ACT 2601, AustraliaThe 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.http://www.sciencedirect.com/science/article/pii/S0370269323006020
spellingShingle 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
Shape polarization in the tin isotopes near N = 60 from precision g-factor measurements on short-lived 11/2− isomers
Physics Letters B
title Shape polarization in the tin isotopes near N = 60 from precision g-factor measurements on short-lived 11/2− isomers
title_full Shape polarization in the tin isotopes near N = 60 from precision g-factor measurements on short-lived 11/2− isomers
title_fullStr Shape polarization in the tin isotopes near N = 60 from precision g-factor measurements on short-lived 11/2− isomers
title_full_unstemmed Shape polarization in the tin isotopes near N = 60 from precision g-factor measurements on short-lived 11/2− isomers
title_short Shape polarization in the tin isotopes near N = 60 from precision g-factor measurements on short-lived 11/2− isomers
title_sort shape polarization in the tin isotopes near n   60 from precision g factor measurements on short lived 11 2 isomers
url http://www.sciencedirect.com/science/article/pii/S0370269323006020
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