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First Measurement of the g Factor in the Chiral Band: The Case of the Cs 128 Isomeric State

  • E. Grodner
  • , J. Srebrny
  • , Ch Droste
  • , L. Próchniak
  • , S. G. Rohoziński
  • , M. Kowalczyk
  • , M. Ionescu-Bujor
  • , C. A. Ur
  • , K. Starosta
  • , T. Ahn
  • , M. Kisieliński
  • , T. Marchlewski
  • , S. Aydin
  • , F. Recchia
  • , G. Georgiev
  • , R. Lozeva
  • , E. Fiori
  • , M. Zielińska
  • , Q. B. Chen
  • , S. Q. Zhang
  • L. F. Yu, P. W. Zhao, J. Meng
  • National Centre for Nuclear Research
  • Faculty of Physics
  • University of Warsaw
  • Horia Hulubei National Institute of Physics and Nuclear Engineering
  • Extreme Light Infrastructure
  • Simon Fraser University
  • Department of Physics
  • University of Notre Dame
  • Laboratori Nazionali di Legnaro
  • Department of Physics
  • Aksaray University
  • University of Padua
  • Université Paris-Saclay
  • Peking University
  • Kyoto University

科研成果: 期刊稿件 › 文章 › 同行评审

摘要

The g factor of the 56 ns half-life isomeric state in Cs128 has been measured using the time-differential perturbed angular distribution method. This state is the bandhead of the positive-parity chiral rotational band, which emerges when an unpaired proton, an unpaired neutron hole, and an even-even core are coupled such that their angular momentum vectors are aplanar (chiral configuration). g-factor measurements can give important information on the relative orientation of the three angular momentum vectors. The measured g factor g=+0.59(1) shows that there is an important contribution of the core rotation in the total angular momentum of the isomeric state. Moreover, a quantitative theoretical analysis supports the conclusion that the three angular momentum vectors lie almost in one plane, which suggests that the chiral configuration in Cs128 demonstrated in previous works by characteristic patterns of electromagnetic transitions appears only above some value of the total nuclear spin.

源语言英语
期刊论文编号022502
期刊Physical Review Letters
卷120
期2
DOI
出版状态已出版 - 12 1月 2018
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