首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment >Observation of high-energy deuterium―tritium fusion gamma rays using gas Cherenkov detectors
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Observation of high-energy deuterium―tritium fusion gamma rays using gas Cherenkov detectors

机译:气体Cherenkov探测器观测高能氘-融合γ射线

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As fusion ignition conditions are approached using the National Ignition Facility (NIF), independent high-bandwidth gamma-ray fusion-burn measurements become essential complements to neutron-based methods. Time resolution ~20ps (10―30 GHz), energy discrimination, and significant stand off distance may be needed for credible burn history measurements. The 16.75 MeV gamma rays that accompany deuterium-tritium (d + t) fusion provide a high-bandwidth alternative to 14 MeV fusion neutrons for d + t burn-history measurements. A thresholding detector, based on the Cherenkov effect, resulting from Compton and pair production electron interactions in gaseous carbon dioxide, offers a means of separating the high-energy fusion gamma rays from other background sources. When coupled to appropriate streak camera recorders, a gas Cherenkov system response of 15 GHz is feasible. As a first step toward this goal, a gas Cherenkov system, employing a 1 GHz photodiode detector, was fielded at the Omega laser facility to demonstrate unambiguous detection of fusion gamma rays from high-yield d + t implosions. With the carbon dioxide Cherenkov production threshold at 12 MeV, the observed high-energy gamma-ray signal is proportional to the observed 14 MeV fusion neutron yield and independent of neutron-induced gamma rays.
机译:随着使用国家点火设施(NIF)达到聚变点火条件,独立的高带宽伽马射线聚变燃烧测量成为基于中子方法的必要补充。要进行可靠的燃烧历史测量,可能需要约20ps(10-30 GHz)的时间分辨率,能量辨别力和明显的隔离距离。氘-((d + t)聚变伴随的16.75 MeV伽马射线为d + t燃烧历史测量提供了14 MeV聚变中子的高带宽替代。一种基于切伦科夫效应的阈值检测器,是由气态二氧化碳中的康普顿和成对电子相互作用产生的,基于切伦科夫效应,提供了一种将高能聚变伽马射线与其他背景源分离的方法。当与适当的条纹摄像机配合使用时,15 GHz的气体Cherenkov系统响应是可行的。作为朝着这个目标迈出的第一步,在Omega激光设备上部署了采用1 GHz光电二极管检测器的气体Cherenkov系统,以演示对高产d + t内爆的融合伽马射线的明确检测。在二氧化碳切伦科夫生产阈值为12 MeV的情况下,观察到的高能伽马射线信号与观察到的14 MeV聚变中子产率成比例,并且与中子诱发的伽马射线无关。

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