Observation of Electron Antineutrino Disappearance at Daya Bay
Observation of Electron Anti-neutrino Disappearance at Daya Bay Yifang Wang Institute of High Energy Physics CERN,March 20, 2012
Outline u u u u u Introduction Data set & quality control Calibration and Event reconstruction Event selection Backgrounds & uncertainties Efficiencies & systematic errors Expectation Results of neutrino oscillation Summary F. P. An et al. , Daya Bay Coll. , “ A side-by-side comparison of Daya Bay anti -neutrino detectors”, ar. Xiv: 1202. 6181[physics. ins-det], submitted to NIM F. P. An et al. , Daya Bay Coll. , “Observation of electron anti-neutrino disappearance at Daya Bay”, ar. Xiv: 1203. 1669[hep-ex], submitted to PRL 2020/9/25 2
Neutrinos & Neutrino Oscillation u Fundamental building blocks of matter: u Neutrino mass: the central issue of neutrino physics ð Tiny mass but huge amount ð Influence to Cosmology: evolution, large scale structure, … ð Only evidence beyond the Standard Model u Neutrino oscillation: a great method to probe the mass ne Oscillation probability: 2020/9/25 nm ne nm P(ne >nm) = sin 2(2 ) sin 2(1. 27 Dm 2 L/E) Oscillation amplitude Oscillation frequency 3
Daya Bay: for a New Type of Oscillation u Goal:search for a new oscillation 13 12 solar neutrino oscillation 23 atmospheric neutrino oscillation u n 1 n 2 n 3 13 ? Neutrino mixing matrix: Unknown mixing parameters: 13, d + 2 Majorana phases Need sizable 13 for the d measurement 2020/9/25 4
Two ways to measure 13 Reactor experiments: Pee 1 sin 22 13 sin 2 (1. 27 Dm 213 L/E) cos 4 13 sin 22 12 sin 2 (1. 27 Dm 212 L/E) Long baseline accelerator experiments: Small-amplitude oscillation due to 13 Pme ≈ sin 2 23 sin 22 13 sin 2(1. 27 Dm 223 L/E) + cos 2 23 sin 22 12 sin 2(1. 27 Dm 212 L/E) Large-amplitude A(r) cos 2 13 sin 13 sin(d) oscillation due to 12 At reactors: Ø Clean signal, no cross talk with d and matter effects Ø Relatively cheap compared to accelerator based experiments Ø Provides the direction to the future of neutrino physics 2020/9/25 5
Direct Searches in the Past Palo Verde & Chooz: no signal u Sin 22 13 < 0. 15 @ 90%C. L. if DM 223 = 0. 0024 e. V 2 T 2 K: 2. 5 s over bkg u 0. 03 < Sin 22 13 < 0. 28 @ 90%C. L. for NH 0. 04 < Sin 22 13 < 0. 34 @ 90%C. L. for IH Allowed region Minos: 1. 7 s over bkg u 0 < Sin 22 13 < 0. 12 @ 90%C. L. NH 0 < Sin 22 13 < 0. 19 @ 90%C. L. IH Double Chooz: 1. 7 s u sin 22θ 13 = 0. 086 ± 0. 041(stat) ± 0. 030(sys) 2020/9/25 6
Reactor Experiment: comparing observed/expected neutrinos Typical precision: 3 -6% Precision of past exp. u Reactor power: ~ 1% Spectrum: ~ 0. 3% Fission rate: 2% u Backgrounds: ~1 -3% u Target mass: ~1 -2% Efficiency: ~ 2 -3% u u u Our design goal:a precision of ~ 0. 4% 2020/9/25 7
Daya Bay Experiment: Layout Redundancy !!! u Relative measurement to cancel Corr. Syst. Err. ð 2 near sites, 1 far site u Multiple AD modules at each site to reduce Uncorr. Syst. Err. ð Far: 4 modules,near: 2 modules u Cross check; Reduce errors by 1/ N Multiple muon detectors to reduce veto eff. uncertainties ð Water Cherenkov: 2 layers ð RPC: 4 layers at the top + telescopes 2020/9/25 8
Underground Labs Overburden Rm Em ( (MWE) (Hz/m 2) Ge. V) 2020/9/25 D 1, 2 (m) L 3, 4 (m) EH 1 250 1. 27 57 364 857 1307 EH 2 265 0. 95 58 1348 480 528 EH 3 860 0. 056 137 1912 1540 1548 9
Anti-neutrino Detector (AD) u Three zones modular structure: I. target: Gd-loaded scintillator II. -catcher: normal scintillator III. buffer shielding: oil u u 192 8” PMTs/module Two optical reflectors at the top and the bottom, Photocathode coverage increased from 5. 6% to 12% ~ 163 PE/Me. V Target: 20 t, 1. 6 m -catcher: 20 t, 45 cm Buffer: 40 t, 45 cm Total weight: ~110 t 2020/9/25 10
Neutrino Detection: Gd-loaded Liquid Scintillator t 28 ms(0. 1% Gd) n + p d + (2. 2 Me. V) n + Gd Gd* + (8 Me. V) Neutrino Event: coincidence in time, space and energy Neutrino energy: 10 -40 ke. V 2020/9/25 1. 8 Me. V: Threshold 11
Gd-loaded Liquid Scintillator u Liquid production, QA, storage and filling at Hall 5 u ð 185 t Gd-LS, ~180 t LS, ~320 t oil LAB+Gd (TMHA)3+PPO+Bis. MSB u Stable over time ð Light yield: ~163 PE/Me. V Stable Liquid 2020/9/25 Liquid hall:LS production and filling 12
Automatic Calibration System u Three Z axis: ð One at the center ü For time evolution, energy scale, nonlinearity… ð One at the edge ü For efficiency, space response ð One in the -catcher ü For efficiency, space response u 3 sources for each z axis: ð LED ü for T 0, gain and relative QE ð 68 Ge (2 0. 511 Me. V ’s) ü for positron threshold & non-linearity… ð 241 Am-13 C + 60 Co (1. 17+1. 33 Me. V ’s) ü For neutron capture time, … ü For energy scale, response function, … u Once every week: ð 3 axis, 5 points in Z, 3 sources 2020/9/25 13
Muon Veto Detector u RPCs ð 4 layers/module ð 54 modules/near hall, 81 modules/far hall ð 2 telescope modules/hall u Water Cerenkov detector ð Two layers, separated by Tyvek/PE/Tyvek film ð 288 8” PMTs for near halls; 384 8” PMTs for the far hall u Two active cosmic-muon veto’s Ø Ø Water Cerenkov: Eff. >97% RPC Muon tracker: Eff. > 88% 2020/9/25 Water processing ð High purity de-ionized water in pools also for shielding ð First stage water production in hall 4 ð Local water re-circulation & purification 14
Two ADs Installed in Hall 1 2020/9/25 15
Hall 1(two ADs) Started the Operation on Aug. 15, 2011 2020/9/25 16
One AD insalled in Hall 2 Physics Data Taking Started on Nov. 5, 2011 2020/9/25 17
Three ADs insalled in Hall 3 Physics Data Taking Started on Dec. 24, 2011 2020/9/25 18
Trigger Performance u Threshold for a hit: ð AD & pool: ¼ PE u Trigger thresholds: ð ð u AD: ~ NHIT=45, Etot= ~ 0. 4 Me. V Inner pool: NHIT=6 Outer pool: NHIT=7 (8 for far hall) RPC: 3/4 layers in each module Trigger rate(EH 1) ð AD singles rate: ü ü >0. 4 Me. V, ~ 280 Hz >0. 7 Me. V, ~ 60 Hz ð Inner pool rate: ~170 Hz ð Outer pool rate: ~ 230 Hz 2020/9/25 19
Data Set u u Dec. 24, 2011 - Feb. 17, 2012, 55 days Data volume: 15 TB DAQ eff. ~ 97% Eff. for physics: ~ 89% 2020/9/25 20
Flashers: Imperfect PMTs Neutrinos u u u Spontaneous light emission by PMT ~ 5% of PMT, 5% of event Rejection: pattern of fired PMTs ð 2020/9/25 Topology: a hot PMT + near-by PMTs and opposite PMTs Flashers Quadrant = Q 3/(Q 2+Q 4) Max. Q = max. Q/sum. Q Inefficiency to neutrinos: 0. 024% 0. 006%(stat) Contamination: < 0. 01% 21
Single Rate: Understood u u u Design: ~50 Hz above 1 Me. V Data: ~60 Hz above 0. 7 Me. V, ~40 Hz above 1 Me. V From sample purity and MC simulation, each of the following component contribute to singles ð ð u ~ 5 Hz from SSV ~ 10 Hz from LS ~ 25 Hz from PMT ~ 5 Hz from rock All numbers are consistent 2020/9/25 22
Event Reconstruction: PMT Calibration u PMT gains from low-intensity LED: ð PMT HV is set for a gain of 1 107 ð Gain stability depends on environments such as temperature All three halls are kept in a temperature within 1 o. C Fit to one PMT SPE distribution SPE peaks for AD 1/AD 2 2020/9/25 23
Event Reconstruction: Energy Calibration u u PMT gain calibration No. of PEs in an AD 60 Co at the center raw energies, ð ð u time dependence corrected different for different ADs 60 Co at center 60 Co at different R & Z to obtain the correction function, ð ð space dependence corrected same for all the ADs ~% level residual non-uniformities 2020/9/25 24
Event Reconstruction: Energy Calibration u u Correct for energy non-linearity: normalize to neutron capture peak Energy uncertainty among 6 ADs (uncorrelated): ð Relative difference between ADs is better than 0. 5% ð Uncertainties from time-variation, non -linearity, non-uniformity… are also within 0. 5% Uniformity at different location 2020/9/25 Peak energy of different sources 25
An Alternative Method u u u Using spallation neutrons in each space grid to calibrate the energy response Neutrons from neutrinos can then be reconstructed correctly Consistent with methods within 0. 5% Uniformity of energy response Residual non-uniformities Energy of spallation neutron 2020/9/25 26
Event Signature and Backgrounds u Signature: ð Prompt: e+, 1 -10 Me. V, ð Delayed: n, 2. 2 Me. V@H, 8 Me. V @ Gd ð Capture time: 28 ms in 0. 1% Gd-LS u Backgrounds ð Uncorrelated: random coincidence of , n or nn from U/Th/K/Rn/Co… in LS, SS, PMT, Rock, … ü n from a-n, m-capture, m-spallation in LS, water & rock ü ð Correlated: Fast neutrons: prompt n scattering, delayed n capture 8 He/9 Li: prompt b decay, delayed n capture ü ü Am-C source: prompt rays, delayed n capture ü a-n: 13 C(α, n)16 O ü 2020/9/25 27
Neutrino Event Selection u Pre-selection ð Reject Flashers ð Reject Triggers within (-2 μs, 200 μs) to a tagged water pool muon u Neutrino event selection ð Multiplicity cut ü Prompt-delayed pairs within a time interval of 200 μs ü No triggers(E > 0. 7 Me. V) before the prompt signal and after the delayed signal by 200 μs ð Muon veto ü 1 s after an AD shower muon ü 1 ms after an AD muon ü 0. 6 ms after an WP muon ð 0. 7 Me. V < Eprompt < 12. 0 Me. V ð 6. 0 Me. V < Edelayed < 12. 0 Me. V ð 1μs < Δte+-n < 200μs 2020/9/25 28
Selected Signal Events:Good Agreement with MC Prompt energy Time between prompt-delayed 2020/9/25 Distance between prompt-delayed 29
Accidental Backgrounds Simple calculation: EH 1 -AD 1 EH 1 -AD 2 EH 2 -AD 1 EH 3 -AD 2 EH 3 -AD 3 Rate(/day) 9. 82± 0. 06 9. 88± 0. 06 7. 67± 0. 05 3. 29± 0. 03 3. 33± 0. 03 3. 12± 0. 03 B/S 1. 38% 1. 44% 4. 58% 4. 77% 4. 43% 2020/9/25 1. 37% 30
Cross Check: Outside the space and time window u u u Prompt-delayed distance distribution. Check the fraction of prompt-delayed pair with distance>2 m Off-window coincidence ‘measure’ the accidental background Results in agreement within 1%. EH 1 -AD 1 2020/9/25 EH 2 -AD 1 Uncertainty: < 1% EH 3 -AD 1 31
Fast Neutrons u Look at the prompt energy spectrum above 12 Me. V, to estimate backgrounds in the region of [0. 7 Me. V, 12 Me. V]: ð A fit to the spectrum in the region of [12 Me. V, 80 Me. V] extrapolate to [0. 7 Me. V, 12 Me. V] ð Difference of the fitting function, 0 th-order or 1 st-order polynomial, gives systematic uncertainties 2020/9/25 32
Cross Check: sum up all the sources u Fast neutrons from water pools ð Obtain the rate and energy spectrum of fast neutrons by tagged muons in water pool. Consistent with MC simulation. ð Estimate the untagged fast neutron by using water pool inefficiency u Fast neutrons from nearby rock ð Estimated based on MC simulation Fast neutron (event/day) Cross checks(event/day) AD 1 0. 84± 0. 28 0. 6± 0. 4 AD 2 0. 84± 0. 28 0. 6± 0. 4 AD 3 0. 74± 0. 44 0. 6± 0. 4 AD 4 0. 04± 0. 04 AD 5 0. 04± 0. 04 AD 6 0. 04± 0. 04 2020/9/25 Results are consistent 33
Backgrounds – 8 He/9 Li u Cosmic m produced 9 Li/8 He in LS ð b-decay + neutron emitter ð t(8 He/9 Li ) = 171. 7 ms/257. 2 ms ð 8 He/9 Li, Br(n) = 12%/48%, 9 Li dominant ð Production rate follow Em 0. 74 power law u Measurement: ð Time-since-last-muon fit 9 Li yield ð Improve the precision by reducing the muon rate: Select only muons with an energy deposit >1. 8 Me. V within a [10 us, 200 us] window ü Issue: possible inefficiency of 9 Li ü ð Results w/ and w/o the reduction is studied 2020/9/25 Error follows NIM A 564 (2006)471 34
Measurement in EH 1+EH 2 & Prediction in EH 3 u u Measurement in EH 1/EH 2 with good precision, but EH 3 suffers from poor statistics Results w/ and w/o the muon reduction consistent within 10% Correlated 9 Li production (Em 0. 74 power law) allow us to further constraint 9 Li yield in EH 3 Cross check: Energy spectrum consistent with expectation EH 1 9 Li yield Uncertainty : 50% EH 2 9 Li yield Uncertainty : 60% EH 3 9 Li yield Uncertainty : 70% 2020/9/25 35
241 Am-13 C Backgrounds Uncorrelated backgrounds: R = 50 Hz 200 ms Rn-like (events/day/AD) u ð Rn-like Measured to be ~230/day/AD, in consistent with MC Simulation ð R is not a negligible amount, particularly at the far site (B/S ~ 3. 17%) ð Measured precisely together with all the other uncorrelated backgrounds u Correlated backgrounds: ð Neutron inelastic scattering with 56 Fe + neutron capture on 57 Fe ð Simulation shows that correlated background is 0. 2 events/day/AD, corresponding to a B/S ratio of 0. 03% at near site, 0. 3% at far site 2020/9/25 Uncertainty: 100% 36
Backgrounds from 13 C(α, n)16 O Identify α sources: 238 U, 232 Th, 227 Ac, 210 Po, … u Determine α rate from cascade decays u Calculate backgrounds from α rate + (a, n) cross sections u D F B E A G C Components Total α rate Region A Acc. Coincidence of 210 Po & 210 Po: Region B Acc. Coincidence of 210 Po & 40 K Region C Acc. Coincidence of 40 K & 210 Po Region D Acc. Coincidence of 208 Tl & 210 Po 10 Hz at EH 1 8 Hz at EH 2 6 Hz at EH 3 Region E Cascade decay in 227 Ac chain 1. 4 Bq 0. 01/day Region F Cascade decay in 238 U chain 0. 07 Bq 0. 001/day Region G Cascade decay in 232 Th chain 1. 2 Bq 0. 01/day 2020/9/25 Uncertainty: 50% BG rate 0. 02/day at EH 1 0. 015/day at EH 2 0. 01/day at EH 3 37
Signals and Backgrounds Neutrino candidates DAQ live time (day) AD 1 AD 2 AD 3 AD 4 AD 5 AD 6 28935 28975 22466 3528 3436 3452 49. 5530 49. 4971 48. 9473 Veto time (day) 8. 7418 8. 9109 7. 0389 0. 8785 0. 8800 0. 8952 Efficiency em*em 0. 8019 0. 7989 0. 8363 0. 9547 0. 9543 0. 9538 Accidentals (/day) 9. 82± 0. 06 9. 88± 0. 06 7. 67± 0. 05 3. 29± 0. 03 3. 33± 0. 03 3. 12± 0. 03 Fast neutron (/day) 0. 84± 0. 28 0. 74± 0. 44 0. 04± 0. 04 8 He/9 Li (/day) 3. 1± 1. 6 1. 8± 1. 1 Am-C corr. (/day) 13 C(α, 0. 16± 0. 11 0. 2± 0. 2 n)16 O background (/day) 0. 04 ± 0. 02 0. 035 ± 0. 02 0. 03 ± 0. 02 Neutrino rate (/day) 714. 17 ± 4. 58 717. 86 ± 4. 60 532. 29 ± 3. 82 71. 78 ± 1. 29 69. 80 ± 1. 28 70. 39 ± 1. 28 2020/9/25 38
Signal+Backgound Spectrum EH 1 EH 2 57910 signal candidates 22466 signal candidates B/S @EH 1/2 B/S @EH 3 10416 signal candidates 2020/9/25 Accidentals ~1. 4% ~4. 5% Fast neutrons ~0. 1% ~0. 06% 8 He/9 Li ~0. 4% ~0. 2% Am-C ~0. 03% ~0. 3% a-n ~0. 01% ~0. 04% Sum 1. 5% 4. 7% 39
Energy Cuts Efficiency and Systematics u Delayed energy cut En > 6 Me. V ð Energy scale uncertainty 0. 5% ð Efficiency uncertainty ~ 0. 12% u Prompt energy cut Ep > 0. 7 Me. V ð Energy scale uncertainty 2 % ð Efficiency uncertainty ~ 0. 01% The inefficiency mainly comes from edges Eff. Delayed energy cut 90. 9% Prompt energy cut 2020/9/25 Corr. Un-corr. 0. 6% 0. 12% 99. 88% 0. 10% 0. 01% 40
Spill-in effect and Systematics u u u Neutrons generated in acrylic and LS can spill into Gd-LS and be captured on Gd. Simulation shows that Gd capture is increased by 5%. The relative differences in acrylic vessel thickness, acrylic density and liquid density are modeled in MC Eff. Spill-in 105. 0% Corr. Un-corr. 1. 5% 0. 02% Acrylic vessel Low H density Gd. LS 2020/9/25 LS 41
Muon Veto and Multiplicity Cut u Muon veto ð Total veto time is the sum of all the veto time windows ð Temporal overlap is taken into account u Multiplicity cut ð Efficiency = e 1 e 2 e 3 u Total efficiency 1 s after an AD shower mu 1 ms after an AD mu 0. 6 ms after an WP mu Prompt-delayed pairs within 200 μs No triggers before the prompt and after the delayed signal by 200 μs ð Uncertainty coming mainly from the average neutron capture time. It is correlated. Multiplicity cut Corr. Un-corr. 0. 02% < 0. 01% e 1 e 3 200μs γ e+ n 1μs< Δe+-n<200μs 2020/9/25 Efficiency is AD dependent, see page 38 e 2 γ t 42
Gd Capture Fraction: H/Gd and Systematics Gd capture Neutron capture time from Am-C H capture u u u Uncertainty is large if takes simply the ratio of area Relative Gd content variation 0. 1% evaluated from neutron capture time Geometry effect on spill-in/out 0. 02% relative differences in acrylic thickness, acrylic density and liquid density are modeled in MC 2020/9/25 Eff. Gd capture ratio 83. 8% Corr. Un-corr. 0. 8% <0. 1% 43
Time Correlation Cut: 1μs < Δte -n < 200μs + u Uncertainty comes from Gd concentration difference and possible trigger time walk effect (assuming 20 ns) Uncertainty: ~0. 02% Capture time cut 2020/9/25 Eff. Corr. Un-corr. 98. 6% 0. 12% 0. 01% 44
Livetime u Synchronization of 3 Halls ð Divide data taking time into one-hour slices ð Discard data in a whole slice if not all 3 halls are running u Uncertainty ð Comes from the case when electronics buffer is full. ð This estimated to be less than 0. 0025%, by either blocked trigger ratio or accumulating all buffer full periods. Eff. Livetime 100% 2020/9/25 Corr. Un-corr. 0. 002% < 0. 01% 45
Alternative Analysis u u Using an alternative energy calibration algorithm based on spallation neutron peak Different neutrino selection criteria ð Muon cut: 0. 4 s after an AD shower muon (different shower muon threshold), 1. 4 ms after an AD muon, 0. 6 ms after a WP muon ð A different multiplicity cut u 2020/9/25 Results: consistent within statistical errors 46
Side-by-side Comparison u Expected ratio of neutrino events: R(AD 1/AD 2) = 0. 981 ð The ratio is not 1 because of target mass, baseline, etc. u Measured ratio: 0. 987 0. 008(stat) 0. 003(syst) This final check shows that systematic errors are under control 2020/9/25 47
Predictions u u u 2020/9/25 Baseline Target mass Reactor neutrino flux These three predictions are blinded before we fix our analysis cuts and procedures They are opened on Feb. 29, 2012 The physics paper is submitted to PRL on March 7, 2012 48
Baseline u Survey: ð Methods: GPS, Total Station, laser tracker, level instruments, … ð Results are compared with design values, and NPP coordinates ð Data processed by three independent software u u Results: sum of all the difference less than 28 mm Uncertainty of the fission center from reactor simulation: ð 2 cm horizontally ð 20 cm vertically The combined baseline error is 35 mm, corresponding to a negligible reactor flux uncertainty (<0. 02%) u 2020/9/25 By Total station By GPS 49
Target Mass & No. of Protons Target mass during the filling measured by bellows the load cell, precision ~ 3 kg 0. 015% u Checked by Coriolis flow meters, precision ~ 0. 1% u Actually target mass: Mtarget = Mfill – Moverflow - Mbellow u Moverflow and Mbellows are determined by geometry u Moverflow is monitored by sensors Overflow tank u 2020/9/25 One batch LAB Quantity Relative Absolute Free protons/Kg neg. 0. 47% Density neg. 0. 0002% Total mass 0. 015% Bellows 0. 0025% 0. 0025 Overflow tank 0. 02% Total 0. 03% 0. 47% 50
Reactor Neutrinos u Reactor neutrino spectrum u Thermal power, Wth, measured by KIT system, calibrated by KME method Fission fraction, fi, determined by reactor core simulation Neutrino spectrum of fission isotopes Si(En) from measurements Energy released per fission ei u u u Kopeikin et al, Physics of Atomic Nuclei, Vol. 67, No. 10, 1892 (2004) 2020/9/25 Relative measurement independent from the neutrino spectrum prediction 51
Daily Rate u u Three halls taking data synchronously allows near-far cancellation of reactor related uncertainties Rate changes reflect the reactor on/off. Predictions are absolute, multiplied by a normalization factor from the fitting 2020/9/25 52
Complete Efficiency and Systematics TDR:(0. 18 - 0. 38) % 2020/9/25 53
Electron Anti-neutrino Disappearence Using near to predict far: Determination of α, β: 1) Set R=1 if no oscillation 2) Minimize the residual reactor uncertainty Observed: 9901 neutrinos at far site, Prediction: 10530 neutrinos if no oscillation R = 0. 940 ± 0. 011 (stat) ± 0. 004 (syst) 2020/9/25 Spectral distortion Consistent with oscillation 54
c 2 Analysis Sin 22 13 = 0. 092 0. 016(stat) 0. 005(syst) No constrain on absolute c 2/NDF = 4. 26/4 normalization. Fit on the nearfar relative measurement. 5. 2 σ for non-zero θ 13 2020/9/25 55
Future plan u u u Assembly of AD 7 and AD 8 is underway now, to be completed before summer Current data taking will continue until the summer Summer activities: ð Installation of AD 7 & AD 8 ð Detector calibration u 2020/9/25 Re-start data taking after summer 56
The Daya Bay Collaboration Europe (2) JINR, Dubna, Russia Charles University, Czech Republic North America (16) BNL, Caltech, LBNL, Iowa State Univ. , Illinois Inst. Tech. , Princeton, RPI, UC-Berkeley, UCLA, Univ. of Cincinnati, Univ. of Houston, Univ. of Wisconsin, William & Mary, Virginia Tech. , Univ. of Illinois-Urbana-Champaign, Siena ~250 Collaborators 2020/9/25 Asia (20) IHEP, Beijing Normal Univ. , Chengdu Univ. of Sci. and Tech. , CGNPG, CIAE, Dongguan Polytech. Univ. , Nanjing Univ. , Nankai Univ. , NCEPU, Shandong Univ. , Shanghai Jiao tong Univ. , Shenzhen Univ. , Tsinghua Univ. , USTC, Zhongshan Univ. , Univ. of Hong Kong, Chinese Univ. of Hong Kong, National Taiwan Univ. , National Chiao Tung Univ. , National United Univ. 57
Summary u Electron anti-neutrino disappearance is observed at Daya Bay, R = 0. 940 ± 0. 011 (stat) ± 0. 004 (syst), together with a spectral distortion u A new type of neutrino oscillation is thus discovered Sin 22 13=0. 092 0. 016 (stat) 0. 005(syst) c 2/NDF = 4. 26/4 5. 2 σ for non-zero θ 13 2020/9/25 58
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