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252Cf自发裂变电荷分布研究——133mTe和133gTe分累计产额测定

CHARGE DISTRIBUTION IN THE SPONTANEOUS FISSION OF 252Cf——DETERMINATION OF FRACTIONAL CUMULATIVE YIELDS OF 133mTe AND133gTe

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【作者】 张艳玲; 李学良; 王方定; 郭景儒; 唐培家; 刘大鸣; 崔安智; 苏树新;

【Author】 Zhang Yanling Li Xueliang Wang Fangding Guo JingruTang Peijia Liu Darning Cui Anzhi Su Shuxin (INSTITUTE OF ATOMIC ENERGY, BEIJING, CHINA)

【机构】 中国原子能科学研究院; 中国原子能科学研究院 北京; 北京; 北京;

【摘要】 用放化法测定了252Cf自发裂变中133mTe和133gTe的分累计产额,其值分别为FCY(133mTe)=0.533±0.014,FCY(133gTe)=0.291±0.042。计算得到133mTe与133gTe分独立产额比R=3.5,由此导出133Te初始碎块均方根角动量为8.8h。FCY(133m+gTe)值与A.C.Wahl的电荷分布系统学预报值在误差范围内一致。N=82中子壳和质子对效应对A=131~141质量区电荷分布没呈现出明显影响。

【Abstract】 The fractional cumulative yields (FCY ) of 133mTe and I33gTe in the spontaneous fission of 2B2Cf have been determined by the radiochemical method.The values are 0.533?.014 and 0.291+0.042 respectively. The ratio of fractional indepeadeat yield of 133nTe to 133*Te was found to be /?=3.5 by using the measured fractional cumulative yields of 133lTe and 133gTe. From, these results the initial fragment angular momentum of root-mean-square of 13iTe, J,.m.,s=8-.(B>i ’bas been deduced. The FCF of i?n+玊e determined in this work is i’n good agreement with the expectation value derived from Wahl’s system-Sties of nuclear charge distribution in the fission. In the mass region of A = 131~141, there is no obvious effect of N = 82 neutron shell and proton pairing effects on the nuclear charge distribution.

【基金】 国家自然科学基金资助项目
  • 【文献出处】 中国核科技报告 ,China Nuclear Science and Technology Report , 编辑部邮箱 ,1990年00期
  • 【下载频次】9
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