European Physical Journal C: Particles and Fields (Dec 2022)

Calibration strategy of the JUNO-TAO experiment

  • Hangkun Xu,
  • Angel Abusleme,
  • Nikolay V. Anfimov,
  • Stéphane Callier,
  • Agustin Campeny,
  • Guofu Cao,
  • Jun Cao,
  • Cedric Cerna,
  • Yu Chen,
  • Alexander Chepurnov,
  • Yayun Ding,
  • Frederic Druillole,
  • Andrea Fabbri,
  • Zhengyong Fei,
  • Maxim Gromov,
  • Miao He,
  • Wei He,
  • Yuanqiang He,
  • Joseph Y. K. Hor,
  • Shaojing Hou,
  • Jianrun Hu,
  • Jun Hu,
  • Cédric Huss,
  • Xiaolu Ji,
  • Tao Jiang,
  • Xiaoshan Jiang,
  • Cécile Jolliet,
  • Daozheng Li,
  • Min Li,
  • Ruhui Li,
  • Yichen Li,
  • Caimei Liu,
  • Mengchao Liu,
  • Yunzhe Liu,
  • Claudio Lombardo,
  • Selma Conforti Di Lorenzo,
  • Peizhi Lu,
  • Guang Luo,
  • Stefano M. Mari,
  • Xiaoyan Ma,
  • Paolo Montini,
  • Juan Pedro Ochoa-Ricoux,
  • Yatian Pei,
  • Frédéric Perrot,
  • Fabrizio Petrucci,
  • Xiaohui Qian,
  • Abdel Rebii,
  • Bedr̆ich Roskovec,
  • Arsenij Rybnikov,
  • Hans Steiger,
  • Xilei Sun,
  • Pablo Walker,
  • Derun Wang,
  • Meifen Wang,
  • Wei Wang,
  • Wei Wang,
  • Zhimin Wang,
  • Diru Wu,
  • Xiang Xiao,
  • Yuguang Xie,
  • Zhangquan Xie,
  • Wenqi Yan,
  • Huan Yang,
  • Haifeng Yao,
  • Mei Ye,
  • Chengzhuo Yuan,
  • Kirill Zamogilnyi,
  • Liang Zhan,
  • Jie Zhang,
  • Shuihan Zhang,
  • Rong Zhao

DOI
https://doi.org/10.1140/epjc/s10052-022-11069-3
Journal volume & issue
Vol. 82, no. 12
pp. 1 – 14

Abstract

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Abstract The Taishan Antineutrino Observatory (TAO or JUNO-TAO) is a satellite experiment of the Jiangmen Underground Neutrino Observatory (JUNO). Located near a reactor of the Taishan Nuclear Power Plant, TAO will measure the reactor antineutrino energy spectrum with an unprecedented energy resolution of $$<2\%$$ < 2 % at 1 MeV. Energy calibration is critical to achieve such a high energy resolution. Using the Automated Calibration Unit (ACU) and the Cable Loop System (CLS), multiple radioactive sources are deployed to various positions in the TAO detector for energy calibration. The residual non-uniformity can be controlled within 0.2%. The energy resolution degradation and energy bias caused by the residual non-uniformity can be controlled within 0.05% and 0.3%, respectively. The uncertainty of the non-linear energy response can be controlled within 0.6% with the radioactive sources of various energies, and could be further improved with cosmogenic $$^{12}{\textrm{B}}$$ 12 B which is produced by the interaction of cosmic muon in the liquid scintillator. The stability of other detector parameters, e.g., the gain of each Silicon Photo-multiplier, will be monitored with an ultraviolet LED calibration system.