Description of the evolution of mixed-symmetry states in the <I>N</I>=78 isotonic chain with IBM2

ZHANG Da-Li; YUAN Shu-Qing; DING Bin-Gang

doi:10.1088/1674-1137/39/7/074102

Chinese Physics C> 2015, Vol. 39> Issue(7) : 074102 DOI: 10.1088/1674-1137/39/7/074102

Description of the evolution of mixed-symmetry states in the N=78 isotonic chain with IBM2

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Abstract：
The characteristics of the lowest mixed-symmetry states 2ms+ and 1ms+ for 132Xe, 134Ba and 136Ce in the even-even N=78 isotones are investigated within the framework of the IBM2 model. The lowest mixed-symmetry state 2ms+ levels for both a single isolated state in 132Xe and 136Ce and a fragmented state in 134Ba are reproduced by the predictions. The agreement between the IBM2 calculation and the experimental values is good for the B(E2) and B(M1) transition probabilities both quantitatively and qualitatively. The predicted summed B(M1) strength follows the experimental data, remaining nearly constant as a function of proton number along the chain of the N=78 isotones.

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ZHANG Da-Li, YUAN Shu-Qing and DING Bin-Gang. Description of the evolution of mixed-symmetry states in the N=78 isotonic chain with IBM2[J]. Chinese Physics C, 2015, 39(7): 074102. doi: 10.1088/1674-1137/39/7/074102

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Received: 2014-11-20
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通讯作者: 陈斌, bchen63@163.com

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沈阳化工大学材料科学与工程学院沈阳 110142

Description of the evolution of mixed-symmetry states in the N=78 isotonic chain with IBM2

Corresponding author: ZHANG Da-Li,

Received Date: 2014-11-20

Accepted Date: 2015-01-19

Available Online: 2015-07-05

Abstract: The characteristics of the lowest mixed-symmetry states 2ms+ and 1ms+ for 132Xe, 134Ba and 136Ce in the even-even N=78 isotones are investigated within the framework of the IBM2 model. The lowest mixed-symmetry state 2ms+ levels for both a single isolated state in 132Xe and 136Ce and a fragmented state in 134Ba are reproduced by the predictions. The agreement between the IBM2 calculation and the experimental values is good for the B(E2) and B(M1) transition probabilities both quantitatively and qualitatively. The predicted summed B(M1) strength follows the experimental data, remaining nearly constant as a function of proton number along the chain of the N=78 isotones.

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Description of the evolution of mixed-symmetry states in the N=78 isotonic chain with IBM2

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Description of the evolution of mixed-symmetry states in the N=78 isotonic chain with IBM2

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