Triaxial shape in <SUP>129</SUP>Ce

LIU Ying; WU Xiao-Guang; ZHU Li-Hua; LI Guang-Sheng; HE Chuang-Ye; LI Xue-Qin; PAN Bo; HAO Xin; LI Li-Hua; WANG Zhi-Min; LI Zhong-Yu; XU Qiang; WANG Jian-Guo; DING Huai-Bo; ZHAI Jian

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《中国物理C》（英文）编辑部

2024年10月30日

Chinese Physics C> 2008, Vol. 32> Issue(S2) : 141-142

Triaxial shape in ¹²⁹Ce

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Abstract：
The high spin states of ¹²⁹Ce have been populated via heavy-ion fusion evaporation reaction ⁹⁶Mo (³⁷Cl, 1p3n) ¹²⁹Ce. The comparison between the signature- and B(M1)-staggering defined by Hagemann and Hamamoto have been showed in the negative-parity band of ¹²⁹Ce. The lifetimes and quadrupole moments Q_t of the high spin states of ¹²⁹Ce have been extracted from the line shape analyses using Doppler shift attenuation method (DSAM). The deformation parameters extracted through the solution of equations for quadrupole transition moments Q_t and collective moments of inertia J_RR.

References

[1]	. Aryaeinejad R et al. J. Phys. G: Nucl. Phys., 1984, 102. Price H G et al. Phys. Rev. Letters, 1983, 51: 18423. Hagemann G B et al. Phys. Rev. C, 1989, 40: 2862

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LIU Ying, WU Xiao-Guang, ZHU Li-Hua, LI Guang-Sheng, HE Chuang-Ye, LI Xue-Qin, PAN Bo, HAO Xin, LI Li-Hua, WANG Zhi-Min, LI Zhong-Yu, XU Qiang, WANG Jian-Guo, DING Huai-Bo and ZHAI Jian. Triaxial shape in ¹²⁹Ce[J]. Chinese Physics C, 2008, 32(S2): 141-142.

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Received: 2008-07-17
Revised: 1900-01-01

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沈阳化工大学材料科学与工程学院沈阳 110142

Triaxial shape in ¹²⁹Ce

Corresponding author: LIU Ying,

Received Date: 2008-07-17
Accepted Date: 1900-01-01
Available Online: 2008-01-03

Abstract: The high spin states of ¹²⁹Ce have been populated via heavy-ion fusion evaporation reaction ⁹⁶Mo (³⁷Cl, 1p3n) ¹²⁹Ce. The comparison between the signature- and B(M1)-staggering defined by Hagemann and Hamamoto have been showed in the negative-parity band of ¹²⁹Ce. The lifetimes and quadrupole moments Q_t of the high spin states of ¹²⁹Ce have been extracted from the line shape analyses using Doppler shift attenuation method (DSAM). The deformation parameters extracted through the solution of equations for quadrupole transition moments Q_t and collective moments of inertia J_RR.