对剪切流稳定 Z 形夹缝中的中子能量各向同性进行时间分辨测量

R. A. Ryan, P. E. Tsai, A. R. Johansen, A. Youmans, D. P. Higginson, J. M. Mitrani, C. S. Adams, D. A. Sutherland, B. Levitt, U. Shumlak
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摘要

以前在运行聚变 Z 夹实验(FuZE)时使用快速塑料闪烁器对中子能量进行的测量,将产生产率的氘核束的能量限制在 4.65 keV 美元以下。此后,FuZE 的输入功率越来越大,导致等离子体电流增加,聚变中子产率提高。在这些情况下,对中子能量各向同性的详细实验研究对束靶聚变的可能贡献施加了更严格的限制。FuZE装置在$-25~kV$的充电电压下运行时,平均等离子体电流为370~kA$,每次放电的D-D聚变中子产率为4times10^7$。在这些运行条件下对中子能量各向同性的测量表明,氘核束的能量小于 7.4 \pm 5.6 ^\mathrm{(stat)} \pm3.7 ^\mathrm{(syst)}~keV$ 。探测器响应的特征描述减少了中子能量分布拟合中自由参数的数量,提高了正向拟合方法的可信度。对伽马背景进行了测量,并研究了这些贡献对各向同性结果的影响。此外,还首次解析了随时间变化的各向同性测量结果,表明在后期氘核束能量可能会增加。这表明在主辐射事件末期可能会出现 $m$=0 不稳定性的增长,但也证实了绝大多数中子产生表现出与热核起源一致的各向同性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Time-resolved measurement of neutron energy isotropy in a sheared-flow-stabilized Z pinch
Previous measurements of neutron energy using fast plastic scintillators while operating the Fusion Z Pinch Experiment (FuZE) constrained the energy of any yield-producing deuteron beams to less than $4.65 keV$. FuZE has since been operated at increasingly higher input power, resulting in increased plasma current and larger fusion neutron yields. A detailed experimental study of the neutron energy isotropy in these regimes applies more stringent limits to possible contributions from beam-target fusion. The FuZE device operated at $-25~kV$ charge voltage has resulted in average plasma currents of $370~kA$ and D-D fusion neutron yields of $4\times10^7$ neutrons per discharge. Measurements of the neutron energy isotropy under these operating conditions demonstrates the energy of deuteron beams is less than $7.4 \pm 5.6^\mathrm{(stat)} \pm 3.7^\mathrm{(syst)}~keV$. Characterization of the detector response has reduced the number of free parameters in the fit of the neutron energy distribution, improving the confidence in the forward-fit method. Gamma backgrounds have been measured and the impact of these contributions on the isotropy results have been studied. Additionally, a time dependent measurement of the isotropy has been resolved for the first time, indicating increases to possible deuteron beam energies at late times. This suggests the possible growth of $m$=0 instabilities at the end of the main radiation event but confirms that the majority of the neutron production exhibits isotropy consistent with thermonuclear origin.
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