Octupole correlations in the structure of 0(2)(+) bands in the N=88 nuclei Sm-150 and Gd-152

S. P. Bvumbi, J. F. Sharpey-Schafer,P. M. Jones,S. M. Mullins, B. M. Nyako,K. Juhasz,R. A. Bark,L. Bianco,D. M. Cullen,D. Curien,P. E. Garrett,P. T. Greenlees,J. Hirvonen,U. Jakobsson,J. Kau, F. Komati, R. Julin,S. Juutinen,S. Ketelhut, A. Korichi,E. A. Lawrie,J. J. Lawrie, M. Leino,T. E. Madiba,S. N. T. Majola, P. Maine, A. Minkova, N. J. Ncapayi, P. Nieminen,P. Peura, P. Rahkila,L. L. Riedinger,P. Ruotsalainen, J. Saren,C. Scholey, J. Sorri, S. Stolze, J. Timar,J. Uusitalo, P. A. Vymers

PHYSICAL REVIEW C(2013)

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摘要
Knowledge of the exact microscopic structure of the 0(1)(+) ground state and first excited 0(2)(+) state in Sm-150 is required to understand the branching of double beta decay to these states from Nd-150. The detailed spectroscopy of Sm-150 and Gd-152 has been studied using (alpha, xn) reactions and the gamma-ray arrays AFRODITE and JUROGAM II. Consistently strong E1 transitions are observed between the excited K-pi = 0(2)(+) bands and the lowest negative parity bands in both nuclei. These results are discussed in terms of the possible permanent octupole deformation in the first excited K-pi = 0(2)(+) band and also in terms of the "tidal wave" model of Frauendorf. DOI: 10.1103/PhysRevC.87.044333
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