锕系区的超变形和聚集

A. Krasznahorkay, D. Habs, M. Hunyadi, D. Gassmann, M. Csatlós, Y. Eisermann, T. Faestermann, G. Graw, J. Gulyás, R. Hertenberger, H. Maier, Z. Máté, A. Metz, J. Ott, P. Thirolf, S. Y. Werf
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引用次数: 2

摘要

用高能量分辨率研究了233U(d,pf)234U和235U(d,pf)236U反应。观察到的裂变共振被描述为具有超变形核形状特征的旋转参数的旋转带的成员。带的K值和带成员的J值的信息是由裂变碎片角分布测量得到的。将最强烈激发态的能级密度与后移费米-气体公式的预测进行了比较,并对234U的第三极小值基态的能量进行了估计。测量了236U超变形态的裂变碎片质量分布。与超变形带一致的质量分布宽度明显小于与共振上下背景区域一致的质量分布宽度,这表明236U在势垒的第三个井中呈梨形双核构型。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Hyperdeformation and clusterization in the actinide region
The 233U(d,pf)234U, and the 235U(d,pf)236U reactions have been studied with high energy resolution. The observed fission resonances were described as members of rotational bands with rotational parameters characteristic of hyperdeformed nuclear shapes. Information on the K values of the bands and for the J values of the band members has been obtained from fission fragment angular distribution measurements. The level density of the most strongly excited states has been compared to the prediction of the back-shifted Fermi-gas formula and the energy of the ground state in the third minimum has been estimated for 234U. The fission fragment mass distribution of the hyperdeformed states in 236U has also been measured. The width of the mass distribution, coincident with the hyperdeformed bands, is significantly smaller than the ones obtained in coincidence with background regions below and above the resonances, which suggests a pear-shaped di-nuclear configuration of 236U in the third well of the potential barrier.
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