4.4 Review

JUNO physics and detector

Journal

PROGRESS IN PARTICLE AND NUCLEAR PHYSICS
Volume 123, Issue -, Pages -

Publisher

ELSEVIER
DOI: 10.1016/j.ppnp.2021.103927

Keywords

JUNO; neutrino physics; neutrino detector

Funding

  1. Chinese Academy of Sciences
  2. National Key R&D Program of China
  3. CAS Center for Excellence in Particle Physics, Australia
  4. Tsung-Dao Lee Institute of Shanghai Jiao Tong University in China
  5. Institut National de Physique Nucleaire et de Physique de Particules (IN2P3) in France
  6. Istituto Nazionale di Fisica Nucleare (INFN) in Italy
  7. Italian-Chinese collaborative research program MAECI-NSFC
  8. Fond de la Recherche Scientifique (F.R.S-FNRS) , Belgium
  9. FWO under the Excellence of Science - EOSin Belgium
  10. Conselho Nacional de Desenvolvimento Cientifico e Tecnolgico in Brazil
  11. Agencia Nacional de Investigacion y Desarrollo in Chile
  12. Charles University Research Centre in Czech Republic
  13. Ministry of Education, Youth, and Sports in Czech Republic
  14. Deutsche Forschungsgemeinschaft (DFG) , Germany
  15. Helmholtz Association in Germany
  16. Cluster of Excellence PRISMA+ in Germany
  17. Joint Institute of Nuclear Research (JINR) , Russia
  18. Lomonosov Moscow State University in Russia
  19. Russian Science Foundation (RSF)
  20. National Natural Science Foundation of China (NSFC)
  21. MOST in Taiwan
  22. MOE in Taiwan
  23. Chulalongkorn University in Thailand
  24. Suranaree University of Technology in Thailand
  25. University of California at Irvine in USA
  26. Wuyi University, China

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The Jiangmen Underground Neutrino Observatory (JUNO) is a 20 kton liquid scintillator detector located 700 meters underground, with excellent energy resolution and a large fiducial volume. It offers exciting opportunities for studying neutrino and astro-particle physics. The construction and design of JUNO are challenging, but it provides potential for significant scientific research.
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20 kton liquid scintillator detector in a laboratory at 700-m underground. An excellent energy resolution and a large fiducial volume offer exciting opportunities for addressing many important topics in neutrino and astro-particle physics. With six years of data, the neutrino mass ordering can be determined at a 3-4 sigma significance and the neutrino oscillation parameters sin(2 )theta(12), Delta m(21)(2), and vertical bar Delta m(32)(2)vertical bar can be measured to a precision of 0.6% or better, by detecting reactor antineutrinos from the Taishan and Yangjiang nuclear power plants. With ten years of data, neutrinos from all past core-collapse supernovae could be observed at a 3 sigma significance; a lower limit of the proton lifetime, 8.34 x 10(33) years (90% C.L.), can be set by searching for p -> (nu) over barK(+); detection of solar neutrinos would shed new light on the solar metallicity problem and examine the vacuum-matter transition region. A typical core-collapse supernova at a distance of 10 kpc would lead to similar to 5000 inverse-beta-decay events and similar to 2000 (300) all-flavor neutrino-proton (electron) elastic scattering events in JUNO. Geo-neutrinos can be detected with a rate of similar to 400 events per year. Construction of the detector is very challenging. In this review, we summarize the final design of the JUNO detector and the key R&D achievements, following the Conceptual Design Report in 2015 (Djurcic et al., 2015). All 20-inch PMTS have been procured and tested. The average photon detection efficiency is 28.9% for the 15,000 MCP PMTS and 28.1% for the 5000 dynode PMTS, higher than the JUNO requirement of 27%. Together with the >20 m attenuation length of the liquid scintillator achieved in a 20-ton pilot purification test and the >96% transparency of the acrylic panel, we expect a yield of 1345 photoelectrons per MeV and an effective relative energy resolution of 3.02%/root E(MeV) in simulations (Abusleme et al., 2021). To maintain the high performance, the underwater electronics is designed to have a loss rate <0.5% in six years. With degassing membranes and a micro-bubble system, the radon concentration in the 35 kton water pool could be lowered to <10 mBq/m(3). Acrylic panels of radiopurity <0.5 ppt U/Th for the 35.4-m diameter liquid scintillator vessel are produced with a dedicated production line. The 20 kton liquid scintillator will be purified onsite with Alumina filtration, distillation, water extraction, and gas stripping. Together with other low background handling, singles in the fiducial volume can be controlled to similar to 10 Hz. The JUNO experiment also features a double calorimeter system with 25,600 3-inch PMTS, a liquid scintillator testing facility OSIRIS, and a near detector TAO. (C) 2021 Elsevier B.V. All rights reserved.

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