宇宙射线产生的中子和伽马射线对SNM的被动成像

K. Borozdin, C. Morris, A. Klimenko, R. Spaulding, J. Bacon
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引用次数: 3

摘要

我们提出了一种基于宇宙射线μ子跟踪与中子/伽马探测相结合的SNM成像系统的新概念。海平面上的宇宙射线通量约为1 μ子/平方公里。厘米/分钟。它由几乎相等数目的μ+和μ-组成。在之前的工作中,我们已经证明了这些μ子可以在相对较短的时间内通过测量它们在物体上的多次散射来成像核威胁。在这里,我们建议通过将μ子的跟踪与μ子在密集的潜在裂变材料中停止时产生的二次粒子的测量相结合来对核物体进行成像。我们使用多个漂移管平面来追踪入射的宇宙射线。塑料闪烁体充当出射中子和伽马射线的探测器。此外,同样的塑料闪烁体被用来估计入射宇宙射线的能量。我们利用n/伽马探测与初始宇宙射线触发的巧合来抑制背景。由停止的μ-产生的裂变链在几次(~ 5)次裂变后消失。每次裂变产生10个高能伽马射线和2.5个中子。虽然需要考虑自屏蔽,但很可能会有数十个中子和伽马射线从典型构型的物体中逃逸出来。对于具有相当大的立体角(~ 2秒)的探测器,在~ 100 ns内检测至少一种产物的效率可以接近100%。10分钟的数据应该在20kg的u中产生50个μ-停止的轨迹,这些数字可以缩放到其他大小的物体。我们的方法没有活动源,因此对人类是安全的,对被检查的物体没有影响。探测器是可扩展和便携式的。探测器的漂移管是密封的,不需要补充气体。通过自动重构算法实现对SNM的检测和定位,该算法可在标准计算机上运行。
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Passive imaging of SNM with cosmic-ray generated neutrons and gamma-rays
We present a novel concept of the SNM imaging system based on cosmic-ray muon tracking in coincidence with neutron/gamma detection. The cosmic-ray flux at sea level is about 1 muon/sq. cm/minute. It is composed of nearly equal numbers of μ+ and μ-. In previous work, we have demonstrated that these muons can be used to image nuclear threats in relatively short times by measuring their multiple scattering through objects. Here we propose to image nuclear objects by combining tracking of the muons into a scene with measurements of the secondary particles produced when the muons stop in dense potentially fissile materials. We use multiple drift tube planes to trace incoming cosmic rays. Plastic scintillator serves as a detector of outgoing neutrons and gamma-rays. Additionally, the same plastic scintillator is used to estimate the energy of incoming cosmic-rays. We use a coincidence of n/gamma detection with the initial cosmic-ray trigger to suppress the background. The fissions produced by the stopped μ-generate fission chains that die away after several (∼5) fissions. Each fission produces ∼10 energetic gamma rays and ∼2.5 neutrons. Although a self-shielding needs to be considered, it is likely that tens of neutrons and gamma rays will escape from the object of typical configuration. The efficiency of detecting at least one of the products within ∼100 ns could be close to 100% for a detector of reasonably large solid angle (∼2 ster). Ten minutes of data should produce 50 trajectories from μ-stopped in 20 kg of U. These numbers can be scaled for other size objects. Our approach has no active source, and therefore it is safe for humans and has no effect on the object under inspection. The detectors are scalable and portable. The drift tubes of the detectors are sealed and do not need the gas replenishment. Detection and localization of SNM is achieved with automatic reconstruction algorithm, which can be run at a standard computer.
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