GeSparK α - β / γ符合探测器高效μ子否决系统的实现

IF 1.4 3区 物理与天体物理 Q3 INSTRUMENTS & INSTRUMENTATION Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment Pub Date : 2025-06-01 Epub Date: 2025-02-21 DOI:10.1016/j.nima.2025.170322
A. Barresi, D. Chiesa, M. Nastasi, E. Previtali, M. Sisti
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引用次数: 0

摘要

低背景高纯锗(HPGe)探测器的主要背景源之一是宇宙介子雨,它与探测器周围的铅和铜屏蔽层相互作用产生的介子雨可以诱导与放射性事件难以区分的信号。塑料闪烁体被广泛用于实施主动否决系统,以减少这种贡献,提高测量灵敏度。在这项工作中,我们提出了一种用于α - β / γ符合检测器的高效μ子否决系统的实现,称为GeSparK。该系统由六个塑料闪烁体探测器和液体闪烁体探测器组成,这些探测器精确地定位在HPGe和液体闪烁体探测器周围。最终的设计包括两个探测器在上面,四个探测器在铜层和铅层之间的被动屏蔽内。通过这种方式,与通常在铅屏蔽外实施的否决系统相比,我们可以限制它们的大小和外部放射性产生的事件率。一个专门的背景测量表明,实现的背景削减是略低于93%。
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Implementation of a high-efficiency muon veto system for the GeSparK alpha-beta/gamma coincidence detector
One of the main background sources of low background high purity germanium (HPGe) detectors is the cosmic muon showers produced in the interaction with the lead and copper shield surrounding the detector that can induce signals not distinguishable from radioactivity events. Plastic scintillators are widely used to implement active veto systems to reduce this contribution and increase the measurement sensitivity. In this work, we present the implementation of a high-efficiency muon veto system for the alpha-beta/gamma coincidence detector, called GeSparK. The veto system consists of six plastic scintillator detectors accurately positioned around the HPGe and liquid scintillator detectors. The final design includes two detectors above and four inside the passive shielding between the copper and lead layers. In this way, we can limit both their size and the event rate produced by external radioactivity, compared to the usual veto systems implemented outside the lead shielding. A dedicated background measurement showed that the achieved background reduction is a bit less than 93%.
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来源期刊
CiteScore
3.20
自引率
21.40%
发文量
787
审稿时长
1 months
期刊介绍: Section A of Nuclear Instruments and Methods in Physics Research publishes papers on design, manufacturing and performance of scientific instruments with an emphasis on large scale facilities. This includes the development of particle accelerators, ion sources, beam transport systems and target arrangements as well as the use of secondary phenomena such as synchrotron radiation and free electron lasers. It also includes all types of instrumentation for the detection and spectrometry of radiations from high energy processes and nuclear decays, as well as instrumentation for experiments at nuclear reactors. Specialized electronics for nuclear and other types of spectrometry as well as computerization of measurements and control systems in this area also find their place in the A section. Theoretical as well as experimental papers are accepted.
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