14mev中子发生器作为TFTR原位校准源的性能

A. Roquemore, D. Jassby, L. C. Johnson, J. Strachan, C. Barnes
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引用次数: 5

摘要

随着氚的引入,TFTR将很快进入D-T阶段。这将导致产生14 MeV能量的中子,这比D-D操作期间遇到的2.5 MeV中子要大得多。为了准备D-T阶段,使用14-MeV中子发生器对四个中子探测系统进行了校准,产生速度为10/sup 8/ n/sec。为了考虑环形等离子体的空间范围和从周围结构散射的中子,探测器的响应被确定为源位于真空容器内的许多位置。在该发生器用作标定源之前,对其总产率和角发射特性进行了表征。铝活化法测定的总产率在/spl + usmn/6%以内,而正反锥沿发生器轴方向的角发射呈各向异性。表征完成后,发生器被安装在真空容器内的可移动轨道上,在那里它可以在每个探测器的视野范围内远程移动。本文详细介绍了源表征的方法和结果,以及容器内D-T中子校准的初步结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Performance of a 14-MeV neutron generator as an in situ calibration source for TFTR
TFTR will soon enter its D-T phase with the introduction of tritium. This will result in the production of neutrons having 14 MeV energy which is significantly greater than the 2.5-MeV neutrons encountered during D-D operation. In preparation for the D-T phase, a calibration of the four neutron detection systems was performed using a 14-MeV neutron generator producing 10/sup 8/ n/sec. To account for the spatial extent of the toroidally shaped plasma and for neutrons scattered from surrounding structures, detector responses were determined with the source positioned at many locations inside the vacuum vessel. Before the generator could be used as a calibration source, a characterization of its total yield and angular emission properties was obtained. The total yield was determined by aluminum activation methods to within /spl plusmn/6%, while the angular emission was found to be anisotropic in the forward and reverse cones along the generator axis. After the characterization was performed, the generator was mounted on a moveable track inside the vacuum vessel, where it could be remotely moved across the view of each detector. This paper presents details of the methods and results of the source characterization, together with initial results of the in-vessel D-T neutron calibration.
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