首页> 外文OA文献 >Analysis of the ground-state band and a closely related intercalated band of ^(235)_(92)U_(143) by the two-revolving-cluster model with consideration of symmetric and antisymmetric resonance of the two dissimilar clusters
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Analysis of the ground-state band and a closely related intercalated band of ^(235)_(92)U_(143) by the two-revolving-cluster model with consideration of symmetric and antisymmetric resonance of the two dissimilar clusters

机译:考虑两个异种簇对称和非对称共振的二次旋转模型分析^(235)_(92)U_(143)的基态带和紧密相关的嵌入带

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摘要

The reported ground-state band of ^(235)_(92)U_(143) extending from J = 7/2- to 51/2- is found to be two intercalated bands, one beginning with 7/2- and the other with 9/2-, each with ΔJ = 2. Analysis by the two-resonating-cluster model leads to 3875 Da.fm^2 for the moment of inertia for the first few levels, then increasing by centrifugal stretching. This value is interpreted by the structure p^(70)n^(112) for the central sphere with clusters p^(11)n^(16) and p^(11)n^(15) with radius of revolution R = 8.55 fm. The major principal axis of the Poinsot ellipsoid is taken to be determined by an unquantized number K, with vector intermediate in orientation between L and J. The values of K are found by empirical analysis to equal L + 0.28, with the theory of rotation of the ellipsoid giving L + 0.28 for 7/2-, slowly decreasing to L + 0.251 for 51/2-. The 7/2- band is based on odd values of L (negative parity) and the 9/2- band on even values (positive parity). Negative parity for both bands is achieved by symmetric resonance of the two dissimilar clusters in the 7/2- band and antisymmetric resonance in the 9/2- band.
机译:发现报告的从J = 7 / 2-扩展到51 / 2-的^(235)_(92)U_(143)的基态带是两个插层带,一个从7 / 2-开始,另一个对于9 / 2-,每一个的ΔJ=2。通过两个共振群集模型的分析得出,在最初几个水平上,惯性矩为3875 Da.fm ^ 2,然后通过离心拉伸进行增加。该值由中心球体的结构p ^(70)n ^(112)解释,其簇半径为p ^(11)n ^(16)和p ^(11)n ^(15),旋转半径R = 8.55分。 Poinsot椭球的主轴线是由一个未量化的数字K确定的,矢量的方向在L和J之间。通过经验分析得出K的值等于L + 0.28,根据旋转理论椭圆形的L / 2为7 / 2-时为0.28,逐渐减小为51 / 2-的L + 0.251。 7/2频段基于L的奇数值(负奇偶校验),而9/2频段基于偶数值(正奇偶校验)。两个波段的负奇偶性是通过7/2波段中两个不同簇的对称共振和9/2波段中的反对称共振来实现的。

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    Pauling Linus; Kamb Barclay;

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  • 年度 1993
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