Optimization of the JUNO liquid scintillator composition using a Daya Bay antineutrino detector
Fysiikka
Liquid scintillator
Physics - Instrumentation and Detectors
scintillation counter: liquid
hiukkasfysiikka
antineutrino: detector
Atomic
7. Clean energy
01 natural sciences
High Energy Physics - Experiment
neutrino
High Energy Physics - Experiment (hep-ex)
Particle and Plasma Physics
Daya Bay
[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]
neutrino oscillation
info:eu-repo/classification/ddc/530
physics.ins-det
JUNO
Ydin- ja kiihdytinfysiikan huippuyksikkö
Physics
Light yield; Liquid scintillator; Neutrino
neutriinot
Instrumentation and Detectors (physics.ins-det)
Nuclear and Plasma Physics
Nuclear & Particles Physics
Nuclear and plasma physics
Other Physical Sciences
antimateria
ilmaisimet
Physical Sciences
photon: yield
Astronomical and Space Sciences
organic compounds: admixture
330
[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]
light yield
tutkimuslaitteet
FOS: Physical sciences
model: optical
Centre of Excellence in Nuclear and Accelerator Based Physics
530
wavelength shifter
Light yield; Liquid scintillator; Neutrino;
Neutrino
0103 physical sciences
fluorine: admixture
Nuclear
[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]
liquid scintillator
ta114
hep-ex
Molecular
[PHYS.PHYS.PHYS-INS-DET] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]
Light yield
DOI:
10.1016/j.nima.2020.164823
Publication Date:
2020-11-06T07:13:56Z
AUTHORS (663)
ABSTRACT
To maximize the light yield of the liquid scintillator (LS) for the Jiangmen Underground Neutrino Observatory (JUNO), a 20 t LS sample was produced in a pilot plant at Daya Bay. The optical properties of the new LS in various compositions were studied by replacing the gadolinium-loaded LS in one antineutrino detector. The concentrations of the fluor, PPO, and the wavelength shifter, bis-MSB, were increased in 12 steps from 0.5 g/L and <0.01 mg/L to 4 g/L and 13 mg/L, respectively. The numbers of total detected photoelectrons suggest that, with the optically purified solvent, the bis-MSB concentration does not need to be more than 4 mg/L. To bridge the one order of magnitude in the detector size difference between Daya Bay and JUNO, the Daya Bay data were used to tune the parameters of a newly developed optical model. Then, the model and tuned parameters were used in the JUNO simulation. This enabled to determine the optimal composition for the JUNO LS: purified solvent LAB with 2.5 g/L PPO, and 1 to 4 mg/L bis-MSB.<br/>13 pages, 8 figures<br/>
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