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作 者:范平[1] 袁大庆[1] 郑永男[1] 左翼[1] 张乔丽[1] 吴晓光[1] 李广生[1] 竺礼华[2] 许国基[1] 樊启文[1] 梁珺城 张锡珍[1] 朱升云[1]
机构地区:[1]中国原子能科学研究院,北京102413 [2]北京航空航天大学,北京100191
出 处:《核技术》2014年第10期29-32,共4页Nuclear Techniques
基 金:国家自然科学基金(No.10975189)资助
摘 要:在中国原子能科学研究院的HI-13串列加速器上,利用76Ge(37Cl,1p4n)108Cd重离子熔合蒸发反应布居了108Cd的yrast带高自旋态,采用瞬态场-离子注入扰动角分布(Transient-magnetic filed-ion implantation perturbed angular distribution,TMF-IMPAD)方法测量了108Cd的正宇称yrast带的g因子,测量得到2+、4+态g-因子分别为0.33(11)、0.18(6)。在10+态前后,发生h11/2中子顺排,g-因子值由正转负。从10+态到16+态,由于g7/2中子顺排,导致g-因子逐渐增大。测量得到反磁转动带带头16+态的g-因子为-0.09(3)。Background: The interplay between the collective rotation and the quasi-particle alignment is a significant feature of nuclear structure at high spins. The g-factors of intra-band high spin states of the ground rotational band can provide direct and unique information on quasi-particle alignment since the g-factors of the high-j proton and the high-j neutron are positively large and negatively small, respectively. Purpose: The present work was motivated to measure g-factors of the rotational states of the positive parity yrast band in ^108Cd and to study the quasi-particle alignment. Methods: High spin states of ^108Cd were populated by the fusion-evaporation reaction ^76Ge(^37Cl, 1p4n)^18Cd at beam energy of 135 MeV from the HI-13 tandem accelerator at China Institute of Atomic Energy, and the g-factors were determined by the transient-magnetic filed-ion implantation perturbed angular distribution (TMF-IMPAD) method. Results: The measured g-factors of 2^+, 4^+ state are 0.33(11), 0.18(6), respectively. The h11/2 neutrons align at the 10+ state, which leads to the decrement of the g-factors. And the g7/2 neutrons align gradually from 10^+ to 16^+, which makes the g-factors increase, Conclusion: The g-factor of the bend head of the anti-magnetic rotation band, 16^+ state, was measured and the value is -0.09(3).
关 键 词:g-因子 瞬态场-离子注入扰动角分布方法 ^108Cd
分 类 号:O571.22[理学—粒子物理与原子核物理]
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