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E1 and E2 cross sections of the ~(12)C(α,γ)~(16)Oreaction at E_(eff) ~ 1.2 MeV using pulsed a beams

机译:E1和E2〜(12)C(α,γ)〜(16)在E_(EFF)〜1.2MeV的横截面使用脉冲梁

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We have measured the γ-ray angular distribution of the ~(12)C(α,γ)~(16)O reaction at the 3.2 MV Pelletron accelerator laboratory at Tokyo Institute of Technology to accurately determine the E1 and E2 cross sections. In this experiment, we used high efficiency anti-Compton NaI(Tl) spectrometers to detect a γ-ray from the reaction with a large S/N ratio, intense pulsed α-beams to discriminate true events from background events due to neutrons from ~(13)C(α,n)~(16)O reaction with a time-of-flight method, and the monitoring system of target thickness. We succeeded in removing a background events due to neutrons and clearly detected the γ-ray from the ~(12)C(α,γ)~(16)O reaction with high statistics.
机译:在东京工业大学的3.2MV Pelletron加速器实验室在3.2MV Pelletron加速器实验室测量了γ射线角分布,在东京工业大学学院进行准确地确定E1和E2横截面。在该实验中,我们使用了高效抗康顿NAI(TL)光谱仪来检测与大的S / N比的反应中的γ射线,强烈的脉冲α光束,以判断由于中子的背景事件从背景事件中区分真实事件。 (13)C(α,N)〜(16)o与飞行时间方法的反应,以及目标厚度的监测系统。我们成功地移除了由于中子而导致的背景事件,并清楚地检测到来自〜(12)C(α,γ)〜(16)O与高统计反应的γ射线。

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