TY - JOUR
T1 - Signature splitting inversion and backbending in 80Rb
AU - He, Chuangye
AU - Shen, Shuifa
AU - Wen, Shuxian
AU - Zhu, Lihua
AU - Wu, Xiaoguang
AU - Li, Guangsheng
AU - Zhao, Yue
AU - Yan, Yupeng
AU - Bai, Zhijun
AU - Wu, Yican
AU - Li, Yazhou
AU - Li, Gui
AU - Yan, Shiwei
AU - Oshima, M.
AU - Toh, Y.
AU - Osa, A.
AU - Koizumi, M.
AU - Hatsukawa, Y.
AU - Matsuda, M.
AU - Hagakawa, T.
PY - 2013/3/22
Y1 - 2013/3/22
N2 - High-spin states of 80Rb are studied via the fusion-evaporation reactions 65Cu+19F, 66Zn+18O, and 68Zn+16O with the beam energies of 75 MeV, 76 MeV, and 80 MeV, respectively. Twenty-three states with twenty-eight γ transitions are added to the previously proposed level scheme, where the second negative-parity band is significantly pushed up to spins of 22- and 15- and two sidebands are built on the known first negative-parity band. Two successive band crossings with frequencies 0.51 MeV and 0.61 MeV in the α = 0 branch as well as another one in the α = 1 branch of the second negative-parity band are observed. Signature inversions occur in the positive-parity and first negative-parity bands at the spins of 11 and 16, respectively. The signature splitting is seen obviously in the second negative-parity band, but the signature inversion is not observed. It is also found that the structure of the two negative-parity bands is similar to that of its isotone 82Y. Signature inversion in the positive-parity yrast band with configuration πg9/2⊠- νg9/2 in this nucleus is discussed using the projected shell model.
AB - High-spin states of 80Rb are studied via the fusion-evaporation reactions 65Cu+19F, 66Zn+18O, and 68Zn+16O with the beam energies of 75 MeV, 76 MeV, and 80 MeV, respectively. Twenty-three states with twenty-eight γ transitions are added to the previously proposed level scheme, where the second negative-parity band is significantly pushed up to spins of 22- and 15- and two sidebands are built on the known first negative-parity band. Two successive band crossings with frequencies 0.51 MeV and 0.61 MeV in the α = 0 branch as well as another one in the α = 1 branch of the second negative-parity band are observed. Signature inversions occur in the positive-parity and first negative-parity bands at the spins of 11 and 16, respectively. The signature splitting is seen obviously in the second negative-parity band, but the signature inversion is not observed. It is also found that the structure of the two negative-parity bands is similar to that of its isotone 82Y. Signature inversion in the positive-parity yrast band with configuration πg9/2⊠- νg9/2 in this nucleus is discussed using the projected shell model.
UR - https://www.scopus.com/pages/publications/84875968801
U2 - 10.1103/PhysRevC.87.034320
DO - 10.1103/PhysRevC.87.034320
M3 - 文章
AN - SCOPUS:84875968801
SN - 0556-2813
VL - 87
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 3
M1 - 034320
ER -