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“RENO/RENO-50” K.K. Joo Chonnam National University

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Presentation on theme: "“RENO/RENO-50” K.K. Joo Chonnam National University"— Presentation transcript:

1 “RENO/RENO-50” K.K. Joo Chonnam National University
(On behalf of RENO Collaboration) August 23, 2016 NuFact Quy Nhon, Vietnam

2 Neutrino Mixing Angles
SNO, Super-K; KamLAND Solar Neutrino Oscillation Atmospheric Neutrino Oscillation Reactor Neutrino Oscillation q12 q23 q13 9o (2012) Daya Bay, RENO Double Chooz ~45o (1998) Super-K; K2K 2015 Nobel Prize “Neutrino has mass” “Established three-flavor mixing framework”

3 RENO Collaboration Reactor Experiment for Neutrino Oscillation
9 institutions and 35 physicists in Korea Chonnam National University Dongshin University GIST Gyeongsang National University Kyungpook National University Sejong University Seoul National University Seoyeong University Sungkyunkwan University Total cost : $10M Start of project : 2006 The first experiment running with both near & far detectors since Aug. 2011 YongGwang (靈光) : New name: Hanbit Reactor Experiment for Neutrino Oscillation

4 YongGwang Nuclear Power Plant
100m 300m 70m high 200m high 1,380m 290m Far Detector Near Detector Reactors Google Satellite View of Experimental Site 16.5 GWth 120 m.w.e. 290m 6 reactors are lined up in roughly equal distances and span ~1.3 km Total average thermal output ~16.5GWth YongGwang Nuclear Power Plant 1380m

5 RENO Detector Target : 16.5 ton Gd-LS (R=1.4m, H=3.2m)
Gamma Catcher : 30 ton LS (R=2.0m, H=4.4m) Buffer : 65 ton mineral oil (MO) (R=2.7m, H=5.8m) Veto : 350 ton water (R=4.2m, H=8.8m) Inner PMTs: ” PMTs solid angle coverage = ~14% Outer PMTs: ~ 67 10” PMTs total ~460 tons

6 IBD signal: coincidence
Inverse beta decay (ve + p e+ + n) Prompt signal (S1) Delayed signal (S2) n-Gd IBD ~30 ms 8 MeV n-H IBD S1 S2 ~200 ms 2.2 MeV Sunny Seo

7 RENO Data-taking Status
Data taking began on Aug. 1, 2011 with both near and far detectors. (DAQ efficiency : ~95%) A B C D A (220 days) : First q13 result [11 Aug, 2011~26 Mar, 2012] PRL 108, (2012) B (403 days) : Improved q13 result [11 Aug, 2011~13 Oct, 2012] NuTel 2013, TAUP 2013, WIN 2013 C (~500 days) : New result Shape+rate analysis (q13 and |Dmee2 |) [11 Aug, 2011~21 Jan, 2013] PRL 116, (2016) D (~1400 days) : Absolute reactor flux and spectrum [11 Aug. 2011~ 30 Sep, 2015] Total ~ 1700 days

8 Observed Delayed Signal (n-Gd)
IBD (ve + p e+ + n) Delayed energy distribution (S2)

9 Measured Spectra of IBD Prompt Signal
Our DAQ Livetime is about 800 days And background is 3% on Far and 6 % on NEAR Near Live time = days # of IBD candidate = 290,775 # of background = 8,041 (2.8 %) Far Live time = days # of IBD candidate = 31,541 # of background = (4.9 %)

10 IBD Candidates & Backgrounds
Near Far DAQ live time (days) 458.49 489.93 IBD candidates 290755 31541 Total BKG rate (/day) 17.54± 0.83 3.14± 0.21 IBD rate (/day) after BKG subtraction 616.67± 1.44 61.24± 0.42

11 Observed Daily Averaged IBD Rate
preliminary Good agreement with observed rate and prediction Accurate measurement of thermal power by reactor neutrinos

12 The 5 MeV Excess is there ! In 2014, RENO showed that the 5 MeV excess
Double Chooz Daya Bay Neutrino 2014, Boston In 2014, RENO showed that the 5 MeV excess is from reactor neutrinos. Seon-Hee Seo, SNU Hawaii 2014

13 Observation of an excess at 5 MeV
(Preliminary) 1400 days of data (Aug – Sep 2015) Fraction of 5 MeV excess: ± 0.27 (%) ~3% ~2.5%

14 Correlation of 5 MeV Excess with Reactor Power
1400 days of data 5 MeV excess has a clear correlation with reactor thermal power ! two or three reactors are off All the six reactors are on The 5 MeV excess comes from reactors!

15 Measurement of Absolute Reactor Neutrino Flux
R (data/prediction) = (500 days) The flux prediction is with Huber + Mueller model Flux weighted baseline at near : 411 m Comparison with other experiments Preliminary Daya Bay *Prediction is corrected for three flavor neutrino oscillation

16 Reactor Neutrino Oscillations
Probability νe 1.0 flux before oscillation observed here Oscillations observed as a deficit of anti-neutrinos sin22θ13 the position of the minimum is defined by Δm2ee Distance 1200 to 1800 meters H. Nunokawa et al, PRD (2005)

17 Energy Calibration from g-ray Sources 12B Energy Spectrum (Near & Far)
Electron energy spectrum from β-decays from 12B and 12N, which are produced by cosmic-muon interactions Non-linear resonse of the scintillation energy is calibrated using γ-ray source Fit function : Evis/Etrue = a – b/(1 – exp(-cEtrue – d)) Deviation of all calibration data points with respect to the best-fit is within ~1% Good agreement between data and MC spectrum!

18 Energy Dependent Disappearance L/E Dependent Disappearance
PRL 116, , 2016 Clear energy-dependent disappearance of reactor antineutrinos

19 Summary of New Oscillation Results
Rate Only ± 0.011(total) Rate + Shape ± 0.26 (total) 10 % precision ± 0.010(total) 12 % precision arXiv: v2 PRL 116, (2016)

20 Projected Sensitivity of q13 & |Dmee2|
(±12%) (5 years of data) (±6 %) (±10%) (~500 days) (6 % precision) (sensitivity goal of q13 ) CERN

21 n-H IBD Event Vertex Distribution
n-H IBD Analysis Motivation: 1. Independent measurement of q13 value. 2. Consistency and systematic check on reactor neutrinos. n-H IBD Event Vertex Distribution target g-catcher Seon-Hee Seo, SNU

22 q13 Measurement with n-H Preliminary rate only analysis results is
Uncertainty Detection efficiency 0.59% Thermal power 0.5 % Isotope fraction 0.7 % Background Near : 0.2% Far : 0.8% Data set : 2011/08 ~ 2013/01 (~500 days) Preliminary rate only analysis results is

23 Summary (1st part) ± 0.26(total) ± 0.010(total)
New measurement of q13 by rate-only analysis Observed an excess at 5 MeV in reactor neutrino spectrum Observation of energy dependent disappearance of reactor neutrinos and our first measurement of Dmee2 ± 0.26(total) 10 % precision ± 0.010(total) 12 % precision RENO (goal): sin(2q13) to 6% accuracy Dmee2 to 0.15×10-3 eV2 (6%) for final sensitivity

24 Overview of RENO-50 RENO-50 : An underground detector consisting of 18 kton ultra- low-radioactivity liquid scintillator & 15,000 20” PMTs, at 50 km away from the Hanbit(Yonggwang) nuclear power plant Goals : - Determination of neutrino mass hierarchy High-precision measurement of q12, Dm221 and Dm2ee Supernova neutrinos, Geo neutrinos, Sterile neutrino search, …. Budget : $ 100M for 6 year construction (Civil engineering: $ 15M, Detector: $ 85M) Schedule : ~ 2021 : Facility and detector construction ~ : Operation and experiment

25 RENO-50 18 kton LS Detector ~47 km from YG reactors
Far Detector Near Detector RENO-50 18 kton LS Detector ~47 km from YG reactors Mt. Guemseong (450 m) ~900 m.w.e. overburden Courtesy by YoshitaroTakaesu (Tokyo) (NEAR Detector) (FAR Detector)

26 RENO-50 Candidate Site Dongshin University RENO-50 Candidate Site
Mt. GuemSeong Altitude : 450 m Dongshin University RENO-50 Candidate Site City of Naju

27 Geological Survey for Underground Facility
Conceptual Design of RENO-50 Detector 39 m LS (18 kton) ” PMTs Water, ” PMTs RENO-50 detector (MC) Cost estimation for RENO-50 underground facility (in progress)  Geological survey for design of tunnel and experimental hall  Cost estimation to be obtained soon

28 RENO-50 R&D Status in Progress
(1) Development of DAQ electronics is on-going (2) Develop techniques of LS purification is on-going (3) Mechanical design of detector is on-going (4) Measurement of radioactivity for the detector materials is on-going (5) Upgrade of measurement device for absolute LS attenuation length is on-going Current status An R&D funding (US $2M for 3 years of ) is given by the Samsung Science & Technology Foundation. Efforts on obtaining a full construction fund

29 T2HKK (Korea option) The T2K n beam will come to Korea. (2nd osc. maximum) Hyper-K Give T2K the capability to provide n mass ordering sensitivity T2HKK session @KPS (Oct. 22) HK members are welcome 2.5 deg. off axis 2.5 deg. off axis ~1100km 2.5deg.off-axis beam @Kamioka JPARC see hep-ph/ ) Off-axis angle

30 Summary of RENO/RENO-50 Independent measurement of q13 with n-H
New results are presented Clear observation of 5 MeV excess Absolute antineutrino flux measurement (R = ) Independent measurement of q13 with n-H RENO-50: various R&D in progress In addition, T2HKK option will be considered seriously

31

32 Correlation of 5 MeV excess with 235U isotope fraction
(Preliminary) 235U fraction corresponds to freshness of reactor fuel Fit function χ2 y = p0 1.407 y = p0 + p1*x 0.233 Δχ2 = 1.174 P-value = 0.240 (End of reactor cycle) (Beginning of reactor cycle)

33 Energy Scale Difference between Near & Far
Energy scale difference < 0.15% for Ep = 1~8 MeV

34 Delayed spectrum and capture time
Delayed signal peak: ~2.2 MeV Mean coincidence time: ~ 200 ms Capture time (n-H) Far and near data match very well 34

35 Light Sterile Neutrino Search Results
All 500 days of RENO data Consistent with standard 3-flavor neutrino oscillation model Able to set stringent limits in the region (Preliminary) eV2 full curves assumes

36 Various Physics with RENO-50
Determination of neutrino mass ordering - 3s sensitivity with 10 years of data Precise (~0.5%) measurement of q12, Dm221 and Dm2ee - An interesting test for unitarity & essential for the future discoveries Neutrino burst from a Supernova in our Galaxy - Study the core collapsing mechanism with neutrino cooling Geo-neutrinos : ~ 1,500 geo-neutrinos for 5 years - Study the heat generation mechanism inside the Earth Solar neutrinos - MSW effect on neutrino oscillation Sterile neutrino search : reactor / radioactive sources / IsoDAR Detection of J-PARC beam : ~200 events/year


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