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Grodner, E; Srebrny, J; Droste, Ch; Próchniak, L; Rohoziński, S G; Kowalczyk, M; Ionescu-Bujor, M; Ur, C A; Starosta, K; Ahn, T; Kisieliński, M; Marchlewski, T; Aydin, S; Recchia, F; Georgiev, G; Lozeva, R; Fiori, E; Zielińska, M; Chen, Q B; Zhang, S Q; Yu, L F; Zhao, P W; Meng, J
Physical review letters, 2018-Jan-12, Letnik: 120, Številka: 2Journal Article
The g factor of the 56 ns half-life isomeric state in ^{128}Cs 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 ^{128}Cs demonstrated in previous works by characteristic patterns of electromagnetic transitions appears only above some value of the total nuclear spin.
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