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首页> 外文期刊>EPJ Web of Conferences >A new analysis procedure to extract fusion excitation function with large beam energy dispersions: application to the 6Li+120Sn and 7Li+119Sn
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A new analysis procedure to extract fusion excitation function with large beam energy dispersions: application to the 6Li+120Sn and 7Li+119Sn

机译:一种提取具有大束能量色散的融合激励函数的新分析程序:在 6 Li + 120 Sn和 7 Li + 119中的应用 Sn

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摘要

In the present paper it is described an analysis procedure suited for experiments where cross-sections strongly varying with energy are measured using beams having large energy dispersion. These cross-sections are typically the sub-barrier fusion excitation function of reactions induced by radioactive beams. The large beam energy dispersion, typical of these experiments, can lead to ambiguities in the association of the effective beam energy to the reaction product yields and consequently to an error in the determination of the excitation function. As a test case, the approach is applied to the experiments ~(6)Li+~(120)Sn and ~(7)Li+~(119)Sn measured in the energy range 14 MeV ≤ E_(c.m.) ≤28 MeV. The complete fusion cross sections are deduced from activation measurements using the stacked target technique. The results of these experiments, that employ the two weakly-bound stable Li isotopes, show that the complete fusion cross sections above the barrier are suppressed of about 70% and 85% with respect to the Universal Fusion Function, used as a standard reference, in the ~(6)Li and ~(7)Li induced reactions respectively. Moreover, the excitation functions of the two systems at energies below the barrier, do not show significant differences, despite the two systems have different n -transfer Q_(value).
机译:在本文中,描述了一种适用于实验的分析程序,在该实验中,使用具有大能量色散的光束测量随能量而强烈变化的横截面。这些横截面通常是放射性束引起的反应的亚势垒融合激发函数。这些实验中典型的大束能量分散会导致有效束能量与反应产物收率之间的关联不明确,从而导致激发函数的确定错误。作为测试案例,该方法适用于在14 MeV≤E_(c.m。)≤28MeV的能量范围内测得的〜(6)Li +〜(120)Sn和〜(7)Li +〜(119)Sn。使用堆叠靶技术根据激活测量结果得出完整的融合截面。这些实验的结果使用了两个弱键合的稳定Li同位素,结果表明,相对于用作标准参考的通用聚变函数,势垒上方的完整聚变截面被抑制了约70%和85%。在〜(6)Li和〜(7)Li诱导的反应中。而且,尽管两个系统具有不同的n转移Q_(值),但是在势垒以下能量处的两个系统的激励函数没有显示出显着差异。

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