Neutrino Program in China

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Presentation transcript:

Neutrino Program in China Jun CAO Institute of High Energy Physics, Beijing Intl. Workshop on Physics Beyond the SM, TDLI, July 1, 2018

Programs in China/Outline Daya Bay Reactor Neutrino Experiment (2003-2011-2020) θ13 and Δm2ee, reactor ν spectrum, exotic searches JUNO (2008-2021-2050) 20 kton LS detector for mass hierarchy, precision measurements, Supernova, DSNB, solar, geo-ν, proton decay, etc. Participation of Super-K, EXO Planning Jinping Neutrino Experiment, for solar and geo-ν (next talk) 0νββ: JUNO-0νββ, PandaX-III, CDEX, GasTPC with SeF6, crystal bolometer. R&D on ν beam, Xsec measurements. Participation in intl. programs, e.g. nEXO, LBNF, etc.

Frontiers in Neutrino Physics Neutrino oscillation CP violation phase Mass Hierarchy Precision measurement Neutrino properties Direct measurement of mass Neutrinoless double beta decay Exotic searches: sterile, magnetic moment, NSI, … Neutrino astronomy High energy cosmic neutrino Supernova, Diffuse SN Background Solar neutrino Geo-neutrino Oscillation Parameters sin212, sin223, sin213 Δm221, Δm231 δCP

Daya Bay Daya Bay Reactor Neutrino Experiment for θ13. Proposed in 2003, immediately after oscillation established in 1998-2002. China: Civil construction + ~1/2 detector. US: ~1/2 detector. Russia, Czech, Hong Kong, and Taiwan all with significant contributions Dec.24, 2011 Collaboration 41 institutions, 193 collaborators China (22), US (16), Europe (2), Chile Aug.15, 2011

Oscillation Measurement Daya Bay announced the non-zero θ13 discovery in 2012 Released 5 results later on. Latest result: 3.4% uncertainty on sin22θ13 1958 d 3.9M ν

Reactor Neutrino Spectrum PRL2016, CPC2017 PRL2017 Found two deviations from models Flux 5% lower than model Large excess around 5 MeV (4σ) Precisely measured the spectrum Which one of the 4 isotopes contributes to the deviation? U-235, using fuel evolution To be understoodJUNO-ND

Sterile Neutrino Searches Best sensitivity in 0.001-0.1 eV2 Combined w/ MINOS, largely excluded the sterile neutrino Neutron yield measurement, PRD2018 Decoherence (wave packet), EPJC2017 Muon seasonal modulation, JCAP2018 LV and CPTV Other Studies PRL2014, PRL2016, PRL2016

Daya Bay Planning sin22θ13 Δm2ee Daya Bay will operate to the end of 2020, confirmed by the funding agency. Measure both sin22θ13 and Δm2ee to <3%. Most precise measurement on reactor neutrino spectrum. More exotic searches. Technical studies for JUNO with one Daya Bay detector: liquid scintillator optimization and low bkg studies sin22θ13 Stopped Δm2ee Stop Running to 2020

JUNO Jiangmen Underground Neutrino Observatory proposed in 2008 for mass hierarchy approved in Feb. 2013 ~ 300 M$ (+10% intl.) Data taking in 2021 20 kton LS detector 3% energy resolution 700 m underground Taishan NPP 9.2 + 9.2 GW Guang Zhou Daya Bay Hong Kong JUNO 53 km Dongguan Yangjiang NPP 17.4 GW

Stainless steel latticed shell: ID40.1m JUNO Detector Electronics Calibration Top Tracker Filling + Overflow Central detector SS latticed shell Acrylic Sphere: ID: 35.4m Thickness:120mm SSLS: ID: 40.1m OD: 41.1m Water pool ID: 43.5m Height: 44m Water Depth: 43.5m Acrylic sphere (20 kt LS) Acrylic sphere : ID35.4m Pool Depth: 44m 18000 20” PMT 25000 3’’ PMT Stainless steel latticed shell: ID40.1m Water Cherenkov ~2000 20’’ PMT Pool ID:43.5m

Neutrino Physics with JUNO Mass Hierarchy w/ reactor: 3-4σ in 6 years Large chance to be the 1st MH measurement at 3σ Precision w/ reactor: sin212, Δm221, Δm231 to <1% Supernova Burst: 5k events + Neutral current Diffuse SN Background: Discovery potential Geo-neutrino: Determine Geo-physics model Proton Decay: Best in K channel Solar Atmospheric Sterile Neutrino from Dark Matter Exotic searches JUNO Yellow book J. Phys. G 43, 030401 (2016)

Mass Hierarchy 3-4σ in 6 years, 5σ in 10 years NOvA: certain chance ORCA: 2022 (?) DUNE: 2026 Hyper-K: 2026 PINGU: 2025 (?) INO: ? M. Blennow et al.

Precision Measurements Probing UPMNS unitarity to ~1% more precise than CKM! Statistics +BG +1% b2b +1% EScale +1% EnonL sin2 θ12 0.54% 0.67% Δm221 0.24% 0.59% Δm2ee 0.27% 0.44% 0.16%0.24% 0.16%0.27% 0.39%0.54% E resolution Correlation among parameters

Supernova ν > 5k events for SN at 10kpc. Measure energy spectra & fluxes of almost all types of neutrinos with liquid scintillator detector.

Diffuse Supernova Neutrino DSNB: Past core-collapse events Cosmic star-formation rate Core-collapse neutrino spectrum Rate of failed SNe 10 Years’ sensitivity

Geo-neutrino JUNO 20 kton Jinping 3 kton Zhe’s talk JUNO will measure the geo-ν flux and U/Th ratio. So far KamLAND and Borexino measured ~100 geo-ν, limited by statistics, JUNO will have 400/year Radioactive heat: different BSE models. Mantle convection, earth magnetic Jinping 3 kton Zhe’s talk

JUNO: solar and reactor Solar Neutrino Borexino (500 ton) JUNO (20 kton), Jinping (3 kton), SNO+ (1 kton) Solar Standard Model: CNO cycle; Metallicity Vacuum oscillation to MSW Exotic searches JUNO: solar and reactor Jinping

Takaaki Kajita, Neutrino2018 Proton Decay Proton decay: physics at very high energy scale, where neutrino mass/mixing might be related with. Hyper-K: ~1035 years for eπ0 JUNO: ~21034 years for νK+ Takaaki Kajita, Neutrino2018

JUNO Collaboration 72 institutions, 580 collaborators China (30), Taiwan(3), Thailand (3), Pakistan, Armenia Italy (8), Germany (7), France (5), Russia (3), Belgium, Czech, Finland, Latvia, Slovakia Brazil (2), Chile (2), USA (2)

Civil Construction Progress Finish the above-floor part of EH in 2018. Finish all civil in 2019.

State-of-Art LS Detector Daya Bay BOREXINO KamLAND JUNO Target Mass ~20 t ~300 t ~1 kt ~20 kt Photoelectron Yield (PE/MeV) ~160 ~500 ~250 ~1200 Photocathode Coverage ~12% ~34% ~78% Energy Resolution ~7.5%/√E ~5%/√E ~6%/√E <3%/√E Energy Non-linearity ~1.5% ~1% ~2% <1% Titanic detector Unprecedented energy resolution (3%) PMT Coverage 78% PMT DE > 27% LS attenuation length > 20 m Minimize the optical loss due to detector material. Calibration Low background (e.g. 1 ppt for acrylic, 10-15 or 10-17 for LS)

Major Breakthroughs – MCP-PMT New type of 20-inch PMT based on MCP Started PMT R&D in 2008, chose MCP-PMT in 2009 (Patented by Y.F.Wang, S. Qian, T.C.Zhao, J. Cao in China, US, Russia, Japan, EU) 2013: 8” prototypes 2014: 20” prototype, PDE 15% 2015: Prototype PDE 26%, tender: 15k MCP, 5k Dynode 2016: Production line 2017: Batch average PDE 25% in March, 27% in April. 3.6k produced 2018: 6k produced. Recent batch of 300 PMTs average PDE 30% First 1300 tested at JUNO Type # PMTs PDE MCP 1354 27.3% Dynode 1229 28.6%

Key Progress – Acrylic, LS 35.4-m Acrylic Vessel Solved all technical problems: No standards for construction, high precision curved sheet, anti-seismic, low bkg, fast bonding Tender in 2017. Intl. reviews. The most transparent Liquid Scintillator (attn. >20 m) Al2O3 filtration Distillation (Italy) Gas tripping (Italy) Water extraction 3x8x0.12m sheet 20 ton pilot plant at DYB LAB (solvent) LS (0.5g/L) LS (3g/L) Attn len 25 m 23.8 m 20.5 m Fast bonding test

Key Progress - Energy Calibration Sources γ: 40K, 54Mn, 60Co, 137Cs e+:22Na, 68Ge n: 241Am-Be, 241Am- 13C or 241Pu- 13C, 252Cf All 4 subsystems prototyped and tested

JUNO-0νββ A possible upgrade: neutrinoless double beta decay w/ JUNO detector after MH determination (e.g. 2026) Load 5 to 50-ton Xenon in LS (also R&D on other isotopes) Starting R&D on Xenon enrichment w/ a company, aiming at 100 kg/year CPC41, 053001 (2017) Xe

Charge Readout Tile Prototype 0νββ Experiments EXO is one of the most sensitivity 0νββ experiments. IHEP participate in EXO since 2012. nEXO R&D by IHEP Charge readout, Ultra-UV reflective cathode Low temp. ASIC electronics (noise 200 e) ICP-MS low bkg measurement Detector simulation & design optimization Other 0νββ experiments (see Huanzhong’s talk) Charge Readout Tile Prototype Test at Stanford ICP-MS Analog multiplexing readout

Other R&D MOMENT: emerging scenarios, R&D on key tech. (Target) Participating LBNF in US, working on target, magnets, etc. Gas TPC prototype for neutrino scattering JUNO-Near Detector w/ SiPM  Best possible energy resolution Neutrinos from muon decay Proton LINAC for ADS ~15 MW Ideal energy: 300 MeV/150 km Good Energy resolution & track Reactor ν spectrum, mag. Moment, θw

Thanks! Summary Daya Bay will take data until 2020 sin2213 and m2ee to < 3% precision, best in future 20y? Most precise reactor ν spectrum, exotic searches JUNO aims at data taking in 2021. Mass Hierarchy, precision measurements World-leading neutrino astrophysics New experiments JUNO-ND, Jingping, likely Xsec meas. etc Many 0νββ proposals and R&Ds Thanks!