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作 者:T. Hayakawa M. Oshima T. Toh T. Shizuma J. Katakura Y. Hatsukawa M. Matsuda H. Kusakari M. Sugawara
出 处:《Science China(Physics,Mechanics & Astronomy)》2004年第5期561-570,共10页中国科学:物理学、力学、天文学(英文版)
基 金:This work was supported by the National Natural Science Foundation of China(Grant No.10005012);the Major State Basic Research Development Program of China(Contract No.TG2000077402).
摘 要:High-spin states in 145Tb have been populated using the 118Sn (32S, 1p4n) reaction at beam energy of 165 MeV. The level scheme of 145Tb has been established up to Ex ≈7.4 MeV. The level scheme shows characteristics of a spherical or slightly oblate nucleus. Based on the systematic trends of the level structure in the neighboring N = 80 isotones, the level structure in 145Tb below 2 MeV excitation is well explained by coupling an h11/2valence proton to the even-even 144Gd core. Above 2 MeV excitation, most of the yrast levels are interpreted with multi-quasiparticle shell-model configurations.High-spin states in145Tb have been populated using the118Sn (32S, 1p4n) reaction at beam energy of 165 MeV. The level scheme of145Tb has been established up toEx≈7.4 MeV. The level scheme shows characteristics of a spherical or slightly oblate nucleus. Based on the systematic trends of the level structure in the neighboringN=80 isotones, the level structure in145Tb below 2 MeV excitation is well eplained by coupling anh 11/2 valence proton to the even-even144Gd core. Above 2 MeV excitation, most of the yrast levels are interpreted with multi-quasiparticle shell-model configurations.
关 键 词:HIGH-SPIN states LEVEL scheme multi-quasiparticle excitations.
分 类 号:O572.2[理学—粒子物理与原子核物理]
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