用于μ+→e+γ的有源转换对谱仪的研制

IF 1.4 3区 物理与天体物理 Q3 INSTRUMENTS & INSTRUMENTATION
R. Sakakibara , S. Ban , L. Gerritzen , F. Ikeda , T. Iwamoto , A. Matsushita , K. Matsuoka , T. Mori , H. Nishiguchi , A. Ochi , W. Ootani , A. Oya , Y. Uchiyama , K. Yamamoto , R. Yokota
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引用次数: 0

摘要

在目前的MEG II实验之后,未来寻找μ+→e+γ的实验计划正在进行中。为了达到比MEG II高一个数量级的灵敏度,需要进一步提高探测器的分辨率,特别是对伽马射线的分辨率。为了解决这个问题,我们引入了一个由转换层(将伽马射线转换成电子-正电子对)和跟踪层(测量它们的动量)组成的对光谱仪。此外,我们计划在转换层中使用活性材料,使其能够测量转换粒子的能量沉积和时间。作为有源变换器的原型,我们开发了尺寸为3×5×50mm3的LYSO晶体,在两边加上硅光电倍增管。我们用3gev电子束测试了它们的光产率和时间分辨率。结果表明,该器件具有25 ~ 30 ps的时间分辨率和5000 ~ 7000个光电子的光产率,满足未来μ+→e+γ实验的要求。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Development of an active converter pair spectrometer for the future search for μ+→e+γ
Plans for a future experiment to search for μ+e+γafter the current MEG II experiment are underway. To achieve an order of magnitude higher sensitivity than the MEG II, further improvements in detector resolution, particularly for gamma-rays, are required. To address this, we introduce a pair spectrometer consisting of a converter layer, which converts gamma-ray into electron–positron pairs, and a tracker layer, which measures their momenta. Additionally, we plan to use active material for the converter layer, allowing it to measure both the energy deposition and timing of the converted particles.
As a prototype of the active converter, we developed LYSO crystals with dimensions of 3×5×50mm3, coupled with silicon photomultipliers on both edges. We evaluated their light yield and timing resolution using a 3 GeV electron test beam. The results demonstrated an excellent timing resolution of 25–30 ps and a sufficient light yield of 5000–7000 photoelectrons, meeting the requirements for the future μ+e+γexperiment.
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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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