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Characterization of a Boron-Loaded Liquid Scintillator EJ-309:B5 for Neutron Energies Between 0.5 and 10 MeV

机译:硼负载液体闪烁体EJ-309:B5的中子能在0.5到10 MeV之间的表征

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Various neutron and gamma-ray detector types have been investigated for applications in fieldssuch as nuclear nonproliferation, nuclear safeguards, reactor instrumentation, and dosimetry.Recently, various capture-gated organic scintillation detectors have been studied with a focus ontheir neutron-spectroscopy capabilities. When compared to standard organic scintillators, thecapture-gated detectors contain an additional material with a high absorption cross section forthermal neutrons (B-10, Li-6, etc.). Therefore, fast neutrons can be thermalized and capturedwithin the detector, generating two separate pulses (scatter pulse followed by capture pulse) witha characteristic time delay. The data analysis is then used to ‘confirm’ the detection of a neutronand infer the incident neutron spectrum. One example of the capture-gated detector is EJ-309:B5(also known as EJ-339), which is a boron-loaded liquid scintillator manufactured by EljenTechnology, containing ~ 5wt% of natural boron. This detector was used in conjunction with aCf-252 source (neutron energies up to 10 MeV) to acquire its response. An optimized digitalpulse-shape discrimination method was used to separate captured neutrons from scatter neutronsand gamma rays, and to obtain the resulting pulse-height and time-to-capture distributions. Theknowledge of the detector response is especially important if the original neutron spectrum of thematerial under investigation needs to be acquired to identify/characterize the investigatedmaterial. The average pulse height of captured neutrons was estimated to be 98 keVee which isin a good agreement with the expected value. Approximately 0.25% of the measured pulses wereidentified as capture pulses and the ratio of capture and scatter neutron pulses was approximately0.62%.
机译:已经研究了各种类型的中子和伽马射线探测器以用于领域 例如核不扩散,核保障,反应堆仪器和剂量学。 最近,研究了各种捕获门控有机闪烁探测器,重点是 他们的中子光谱学能力。与标准有机闪烁体相比, 捕获门控检测器包含一种具有高吸收截面的附加材料,用于 热中子(B-10,Li-6等)。因此,快中子可以被热化并被捕获 在检测器中,产生两个独立的脉冲(散射脉冲,然后是捕获脉冲), 典型的时间延迟。然后使用数据分析来“确认”中子的检测 并推断入射中子谱。捕获门控检测器的一个示例是EJ-309:B5 (也称为EJ-339),这是由Eljen制造的硼加载液体闪烁器 技术,含有〜5wt%的天然硼。该检测器与 Cf-252源(中子能量高达10 MeV)获得其响应。优化的数字 脉冲形状鉴别方法用于将捕获的中子与散射中子分离 和伽马射线,并获得最终的脉冲高度和捕获时间分布。这 如果检测器的原始中子能谱知道检测器的响应就显得尤为重要。 需要获取被调查材料以识别/表征被调查者 材料。被捕获的中子的平均脉冲高度估计为98 keVee,这是 与预期价值保持良好的一致性。大约0.25%的测量脉冲为 识别为捕获脉冲,捕获中子脉冲与散射中子脉冲之比约为 0.62%。

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