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Chinese Physics C> 2008, Vol. 32> Issue(S2) : 134-137 

Level scheme in 160Tm towards complete high-spin structure

  • High-spin states of 160Tm have been studied through the 146Nd(19F, 5n) reaction at a beam energy of 102 MeV. The previously known πh11/2⊙νi13/2 yrast band and πh11/2⊙νh9/2 side band are confirmed, and several low-lying levels are observed. A 4-quasiparticle band feeding into the yrast band based on the πg7/2⊙νh9/2⊙νi13/22 is suggested. Other two bands are observed and assigned to be based on the πd3/2⊙νi13/2 and πg7/2⊙νi13/2 configurations, respectively.
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    [1] . Espino J M et al. Nucl. Phys. A, 1998, 640: 1632. Reviol W et al. Phys. Rev. C, 1999, 59: 13513. Cardona M A et al. Phys. Rev. C, 2002, 66: 0443084. André S et al. Z. Phys. A, 1989, 333: 2475. Lagergren K et al. Phys. Rev. C, 2005, 72: 0573036. Singh B et al. Phys. Rev. C, 1983, 28: 21187. Simpson J et al. Eur. Phys. A, 1998, 1: 2678. Reich C W, Helmer R G. Nucl. Data Sheets, 2000, 90: 6459. Helmer R G. Nucl. Data Sheets, 2003, 99: 48310. Warburton S J et al. Nucl. Phys. A, 1995, 591: 323

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SUN Liang, LU Jing-Bin, YANG Dong, WANG Lie-Lin, LIU Yun-Zuo, ZHU Li-Hua, WU Xiao-Guang and LI Guang-Sheng. Level scheme in 160Tm towards complete high-spin structure[J]. Chinese Physics C, 2008, 32(S2): 134-137.
SUN Liang, LU Jing-Bin, YANG Dong, WANG Lie-Lin, LIU Yun-Zuo, ZHU Li-Hua, WU Xiao-Guang and LI Guang-Sheng. Level scheme in 160Tm towards complete high-spin structure[J]. Chinese Physics C, 2008, 32(S2): 134-137. shu
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Received: 2008-07-17
Revised: 1900-01-01
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Level scheme in 160Tm towards complete high-spin structure

    Corresponding author: SUN Liang,
  • Received Date: 2008-07-17
  • Accepted Date: 1900-01-01
  • Available Online: 2008-01-03

Abstract: High-spin states of 160Tm have been studied through the 146Nd(19F, 5n) reaction at a beam energy of 102 MeV. The previously known πh11/2⊙νi13/2 yrast band and πh11/2⊙νh9/2 side band are confirmed, and several low-lying levels are observed. A 4-quasiparticle band feeding into the yrast band based on the πg7/2⊙νh9/2⊙νi13/22 is suggested. Other two bands are observed and assigned to be based on the πd3/2⊙νi13/2 and πg7/2⊙νi13/2 configurations, respectively.

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