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

Triaxial shape in 129Ce

  • 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 Qt 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 Qt and collective moments of inertia JRR.
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    [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.
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. shu
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Received: 2008-07-17
Revised: 1900-01-01
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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 Qt 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 Qt and collective moments of inertia JRR.

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