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A Study of 2H + 3He Elastic Scattering and the Reaction 2H( 3He, 4He)1H Between 17.5 and 44.1 MeV

机译:2H + 3He弹性散射和17.5至44.1 MeV之间的2H(3He,4He)1H反应的研究

摘要

An investigation of 2H + 3He elastic scattering and the reaction 2H ( 3He , 4He) 1H has been conducted at bombarding energies between 17.5 and 44.1 MeV to determine whether any states in 5Li, with appreciable widths for decay into two-body final states, exist in the region of excitation from 23.4 to 34 MeV in 5Li. An excitation function for 2H + 3He elastic scattering was measured at three laboratory scattering angles, and for 2H ( 3He, 4He) 1H at four laboratory scattering angles. No evidence was found for virtual states of the nucleus 5Li having appreciable two-body decay widths between 23.4 and 30.4 MeV excitation. Any such states have widths less than 200 keV between 23.4 and 25 MeV, less than 1.4 MeV between 25 and 30.4 MeV, less than 100 keV between 30.4 and 31 MeV, and less than 1 MeV between 31 and 34 MeV excitation in 5Li. Complete angular distributions for 2H + 3He elastic scattering and the reaction 2H( 3He , 3He) 1H were taken at several bombarding energies between 18.5 and 44.1 MeV. A partial-wave decomposition of the elastic scattering angular distributions has been performed. No anomalous behavior is observed. The angular distributions were also fitted with a linear Legendre polynomial series. Finally, the angular distributions have been compared to the predictions of two simple direct-reaction theories: the Butler stripping theory and the diffraction theory. The fits to the Butler theory are satisfactory, and the fits to the diffraction theory are remarkably good. Absolute differential cross sections were measured to an accuracy of 3%. At bombarding energies below 21.6 MeV they supplement existing data of comparable accuracy. Between 34.8 and 40.5 MeV bombarding energy, existing data are sparse, and of only moderate (14%) accuracy. The present work extends the data in this region, and improves the absolute accuracy by a factor of five. The differential cross sections measured above 40 MeV in the present, work are the only data in this energy region.
机译:研究了2H + 3He弹性散射和2H(3He,4He)1H反应,轰击能量在17.5和44.1 MeV之间,以确定在5Li中是否存在任何可衰减到两体最终状态的宽度的可观状态。在5Li中从23.4到34 MeV的激发范围内在三个实验室散射角下测量2H + 3He弹性散射的激发函数,并在四个实验室散射角下测量2H(3He,4He)1H的激发函数。没有证据表明原子核5Li的虚拟状态在23.4和30.4 MeV激发之间具有可观的两体衰减宽度。在5Li中,任何这种状态的宽度在23.4和25 MeV之间小于200 keV,在25和30.4 MeV之间小于1.4 keV,在30.4和31 MeV之间小于100 keV,在31和34 MeV之间小于1 MeV。在18.5和44.1 MeV之间的几个轰击能量下,获得了2H + 3He弹性散射的完整角分布和2H(3He,3He)1H反应。已经对弹性散射角分布进行了部分波分解。没有观察到异常行为。角度分布也符合线性勒让德多项式级数。最后,将角分布与两种简单的直接反应理论(巴特勒汽提理论和衍射理论)的预测结果进行了比较。巴特勒理论的拟合令人满意,衍射理论的拟合非常好。绝对差分横截面的测量精度为3%。在轰击低于21.6 MeV的能量时,它们补充了可比精度的现有数据。在34.8和40.5 MeV的轰击能量之间,现有数据稀疏,并且准确度仅为中等(14%)。目前的工作扩展了该区域中的数据,并将绝对精度提高了五倍。目前,在40 MeV以上测量的微分横截面是该能量区域中的唯一数据。

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    King Thomas Richard;

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  • 年度 1941
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