The high-precision detector of the JUNO-TAO experiment

IF 1.5 3区 物理与天体物理 Q3 INSTRUMENTS & INSTRUMENTATION
Zhimin Wang, JUNO collaboration
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引用次数: 0

Abstract

The Taishan Antineutrino Observatory (TAO) is a proposed ton scale liquid scintillator (LS) detector designed to precisely measure the reactor neutrino energy spectrum with the highest possible energy resolution. This will provide a reference spectrum for Jiangmen Underground Neutrino Observatory (JUNO) and a benchmark to verify the nuclear database. As a satellite experiment of JUNO, TAO will be installed near the reactor core at a distance of 30 m. The detector uses 2.8 m3 of Gd-doped liquid scintillator (1 ton fiducial volume, Gd-LS) contained in a spherical acrylic vessel. To maximize the photon collection efficiency in the detector, a 10 m2 SiPM array is proposed to fully cover the acrylic vessel and collect as many scintillation photon as possible. The photon detection efficiency of SiPMs should be larger than 50%, in order to achieve the desired energy resolution (1.5%/E, photon statistical resolution). Additionally, the SiPMs will be operated at low temperature (−50 °C or lower) to reduce dark noise. Meanwhile, a shield and muon veto system will be located outside of the neutrino detector to control the environmental background. An overview of the JUNO-TAO experiment and its current progress are discussed.
JUNO-TAO 实验的高精度探测器
台山反中微子观测站(TAO)是一个拟建的吨级液体闪烁体(LS)探测器,旨在以尽可能高的能量分辨率精确测量反应堆中微子能谱。这将为江门地下中微子观测站(JUNO)提供参考能谱,并为验证核数据库提供基准。作为 JUNO 的卫星实验,TAO 将安装在反应堆堆芯附近,距离约 30 米。为了最大限度地提高探测器的光子收集效率,建议使用一个 10 平方米的 SiPM 阵列来完全覆盖丙烯酸容器,尽可能多地收集闪烁光子。SiPM 的光子探测效率应大于 50%,以达到所需的能量分辨率(1.5%/E,光子统计分辨率)。此外,SiPM 将在低温(-50 °C 或更低)下运行,以减少暗噪。同时,将在中微子探测器外部安装屏蔽和μ介子否决系统,以控制环境背景。本文讨论了 JUNO-TAO 实验的概况及其目前的进展情况。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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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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