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An Analysis Technique for Active Neutron Multiplicity Measurements Based on First Principles

机译:基于第一性原理的主动中子多重测量分析技术

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Passive neutron multiplicity counting is commonly used to quantify the total mass of plutonium in asample, without prior knowledge of the sample geometry. However, passive neutron counting is lessapplicable to uranium measurements due to the low spontaneous fission rates of uranium. Activeneutron multiplicity measurements are therefore used to determine the ~(235)U mass in a sample.Unfortunately, there are still additional challenges to overcome for uranium measurements, such as thecoupling of the active source and the uranium sample. Techniques, such as the coupling method, havebeen developed to help reduce the dependence of calibration curves for active measurements onuranium samples; although, they still require similar geometry known standards. An advanced activeneutron multiplicity measurement method is being developed by Texas A&M University, in collaborationwith Los Alamos National Laboratory (LANL) in an attempt to overcome the calibration curverequirements. This method can be used to quantify the ~(235)U mass in a sample containing uraniumwithout using calibration curves. Furthermore, this method is based on existing detectors and nondestructiveassay (NDA) systems, such as the LANL Epithermal Neutron Multiplicity Counter (ENMC).This method uses an inexpensive boron carbide liner to shield the uranium sample from thermal andepithermal neutrons while allowing fast neutrons to reach the sample. Due to the relatively low andconstant fission and absorption energy dependent cross-sections at high neutron energies for uraniumisotopes, fast neutrons can penetrate the sample without significant attenuation. Fast neutroninterrogation therefore creates a homogeneous fission rate in the sample, allowing for first principlemethods to be used to determine the ~(235)U mass in the sample. This paper discusses the measurementmethod concept and development, including measurements and simulations performed to date, as wellas the potential limitations.
机译:被动中子多重计数通常用于量化样品中p的总质量。 无需事先了解样品几何形状的样品。但是,被动中子计数较少 由于铀的自发裂变率低,因此可用于铀测量。积极的 因此,使用中子多重性测量来确定样品中的〜(235)U质量。 不幸的是,铀的测量还需要克服其他挑战,例如 活性源与铀样品的耦合。诸如耦合方法之类的技术具有 旨在帮助减少校准曲线对主动测量的依赖性 铀样品尽管它们仍然需要类似的几何已知标准。先进的活动 德州农工大学正在合作开发中子多重性测量方法 与洛斯阿拉莫斯国家实验室(LANL)合作,试图克服校准曲线 要求。此方法可用于量化含铀样品中的〜(235)U质量 无需使用校准曲线。此外,该方法基于现有的检测器且无损 化验(NDA)系统,例如LANL超热中子多重计数器(ENMC)。 该方法使用廉价的碳化硼衬里来保护铀样品免受热和热的影响。 超热中子,同时允许快中子到达样品。由于相对较低 铀在中子高能量下恒定的取决于裂变和吸收能的截面 同位素,快中子可以穿透样品而没有明显的衰减。快中子 因此,询问会在样品中产生均一的裂变速率,从而允许第一个原理 测定样品中〜(235)U质量的方法本文讨论了测量 方法的概念和发展,包括迄今为止进行的测量和模拟 作为潜在的限制。

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