Daya Bay Reactor Neutrino Experiment

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Daya Bay Reactor Neutrino Experiment Jun Cao caoj@ihep.ac.cn Institute of High Energy Physics Tsinghua University, HPGe workshop, Mar. 24, 2011

2 Past Reactor Neutrino Experiments Reactor anti-neutrino experiments have played a critical role in the 50- year-long history of neutrinos. The first neutrino observation in 1956 by Reines and Cowan. Determination of the upper limit of mixing angle theta13 to sin 2 2 13 <0.17 (Chooz, Palo Verde) The first observation of reactor anti-neutrino disappearance at KamLAND in 2003. Now reactor neutrino experiments become prominent again for measuring mixing angle 13 precisely.

3 Neutrino Oscillation Since 1998, we believe that neutrino can oscillate. non-zero mass + mixing Neutrino Mixing: PMNS Matrix i 1 0 0 cos13 0 e sin 13 cos1 2 sin12 0 0 cos23 sin2 3 0 1 0 sin12 cos1 2 0 i 0 sin23 cos 23 e sin13 0 cos 13 0 0 1 Atmospheric, K2K, MINOS, T2K, etc. 23 ~ 45º Reactor Accelerator 13 < 12º Solar KamLAND 12 ~ 30º Known: Dm 2 32, sin 2 2 23, Dm 2 21, sin 2 2 12 Unkown: sin 2 2 13, CP, Sign of Dm 2 32 Sterile Neutrino: Yes? No? Yes? Yes????

4 Measuring sin 2 2 13 to 0.01 If sin 2 2 13 <0.01, long baseline (LBL) experiments with conventional beam have little chance to determine the CP violation. Measuring sin 2 2 13 to 0.01 will provide a roadmap for the future LBL experiments. Planned Exp. We recommend, as a high priority,, An expeditiously deployed multi-detector reactor experiment with sensitivity to e disappearance down to sin 2 2 13 =0.01 ---- APS Neutrino Study, 2004

5 Proposals for measuring 13 at reactors RENO, Korea Braidwood, USA Krasnoyarsk, Russia 250 ton-gw th Proposed sin 2 2 13 ~0.02 Diablo Canyon, USA Double Chooz, France 85 ton-gw th Proposed sin 2 2 13 ~0.03 Daya Bay, China KASKA, Japan 1400 ton-gw th Proposed sin 2 2 13 ~0.01 Angra, Brazil 8 proposals 5 cancelled 3 in progress

6 Daya Bay collaboration Europe (3) JINR, Dubna, Russia Kurchatov Institute, Russia Charles University, Czech Republic North America (15) BNL, Caltech, LBNL, Iowa state, Illinois Inst. Tech., Princeton, RPI, Siena Coll. UC-Berkeley, UCLA, U- Cincinnati, U-Houston, U-Wisconsin, Virginia Tech., U-Illinois-Urbana- Champaign, Asia (19) IHEP, Beijing Normal Univ., Chengdu UST, CGNPG, CIAE, Dongguan Univ. of Tech., Nanjing Univ.,Nankai Univ., Shenzhen Univ., Shandong Univ.,Shanghai Jiaotong Univ., Tsinghua Univ., USTC, Zhongshan Univ., Hong Kong Univ., Chinese Hong Kong Univ., Taiwan Univ., Chiao Tung Univ., National United Univ. ~ 250 collaborators

7 Daya Bay and Ling Ao Nuclear Power Plant LingAo II NPP 2.9GW2 Under construction (2011) Daya Bay NPP 2.9GW2 LingAo NPP 2.9GW2

8 Layout Far site to LingAo cores 1615 m to Daya Bay cores 1985 m Overburden 350 m LingAo Near site to LingAo cores 500 m Overburden 112 m 3 experimental Hall connected with horizontal tunnel. 8 antineutrino Detectors (AD) Oscillation singal neutrino rate deficit energy spectrum distortion Daya Bay Near site To Daya Bay cores 363 m Overburden 98 m Near-far relative measurements Cancel reactor errors (3%) Identical ADs Cancel detector errors (2%) Enough Overburden reduce cosmogenic backgrounds Larger, better detector

9 Far Site Near Site Reactor

10 Signal and Backgrounds in detector e p e Prompt signal e e 2 n Peak at 4 MeV Capture on H or Gd, Delayed signal, 2.2, 8 MeV Capture on H Capture on Gd sin 2 2 13 =0.01

11 Past Results Chooz: R=1.012.8%(stat) 2.7%(syst), sin 2 2 13 <0.17 Chooz: bad Gd-LS Palo Verde: shallow site, large background Improve the precision by an order P ee 2 2 2 2 m31 L 4 2 2 m21 L 1 sin 213 sin D cos 13 sin 2 12 sin D 4E 4E

12 How to improve precision by an order? Large statistics (Powerful reactors, Large detector) Chooz: 14 t.gw.y, statistical error 3% Double Chooz: 214, RENO: 830, Daya Bay: 4176 Statistical error in 3 years: 0.2% Reduce backgrounds (Overburden, Low-background detectors) Chooz, Double Chooz: 300 mwe, 大亚湾 :940 mwe Reduce Systematic error Identical detectors, Near-far relative measurements Uncertainties Reactor Detector Backgrounds Chooz 3% 1.7%? Daya Bay 0.1% 0.4% <0.3%

13 3 layers separated by Acrylic Vessels Detectors Mineral Oil: 50cm thick, shielding radioactivity from PMT and Steel 5.3m 20-ton Gd-LS Target Neutron RPC Water Cherenkov 192 PMTs LS: 45cm thick, improve neutron energy measurement. Water shields radioactivity and neutron Two layer water Cherenkov detector RPC Combined eff. 99.5%+-0.25%

14 Prototype studies Motivation Validate the design principle Test technical details of tanks Test Gd-LS Test calibration and Pu-C source Achievements Energy response & MC Comparison Reconstruction algorithm Neutron response & Pu-C source Effects of reflectors Gd-LS 137 Cs

15 Water detector: R&D with a prototype Compatibility tests of materials in water Established a water circulation model purification system design MC modeling for light transport & light collection

16 Backgrounds 9 Li/ 8 He (correlated background, B/S estimated to 0.3%) Cosmogenic long-lived isotopes, -n cascade, mimic neutrino signal "Fast Neutron" background (correlated background, B/S estimated to 0.1-0.2%) Cosmic produce high energy neutrons. Neutron recoil signal mimic the prompt signal. Thermalized neutron form the delayed signal. Neutron capture on C, O, etc, emit high energy neutron. Occidental coincidence background (B/S estimated 1%, error 0.1%) Prompt signal (single rate <50 Hz) Radioactivity (PMT, rock, steel tank, LS, etc) Cosmogenic isotopes Delayed signal (<200/day) single neutron: Cosmic produces neutrons, without recoil signal. cosmogenic long-lived isotopes (e.g. 12 B/ 12 N) Other events in 6-10 MeV (e.g. Michel s electron, corner-cutting muons)

17 Measuring He8/Li9 in-situ Time since last muon est 1 N 2 (1 R ) 1 L.J. Wen et. al. NIM A 564 (2006) 471 3 years data 0.36% error at DYB site 0.27% at LA near site 0.10% at the far site The unknown is 9 Li cross section. Combine DYB and LA site Measure to 0.2%, irrelevant to B/S ratio

18 Measuring fast neutron in-situ The most uncertain backgrounds. Simulation B/S ~ 0.1%. Depends on veto eff. DYB LA Far Fast neutron (/day/module) 0.6 0.4 0.04 Fast neutron/signal ~0.1% ~0.1% ~0.1% Tagged fast neutrons (by detecting the parent muons) will be 50 times of untagged ones. Can be used to determine the B/S d Distance from detector center to muon track Could be measured in-site to ~0.1%

19 Civil construction 3 2 4 Tunnel length: ~ 3100m Three experimental halls One assembly hall Water purification hall 5 1 All blasting safely completed, no one exceeded vibration limit (0.007g) Hall 1, 4, 5 completed last year Hall 2 completed last month Hall 3 to be completed this summer

20 Civil construction

21 Detector Component Production Stainless steel vessel 4m Acrylic vessel Reflector 3m acrylic vessel

22 Liquid Scintillator Production What we need: 185t Gd-LS, ~180t LS, ~320t oil Equipment designed, manufactured and tested at IHEP 4-ton Gd-LS test run successful: good quality up to now and aging test showing good stability Gd-LS production completed and stored in Hall 5 LS production almost finished AD Filling will start next month

23 AD assembly SSV Bottom reflector 4m AV Top reflector PMT 3m AV SSV lid Leak check ACU

24 Two completed ADs

25 AD Dry-run Complete test of assembled ADs with final electronics, trigger and DAQ Results show that: Both ADs are fully functional Their response to LED & cosmic-rays agrees with MC expectations Two ADs are identical Electronics, trigger, DAQ and offline software are all tested Double pulse signal Random coincidence

26 RPC production & assembly Each module consists of 4 layers of bare chambers made of bakelite without linseed oil(besiii-type) RPC bare chamber testing shows good performance Module assembly almost finished 2/3 modules shipped to Daya Bay

27 RPC supporting structure RPC installation Gas system RPC modules RPC module installation

28 Water Cerenkov detector installation PermeFlax Painting PMT supporting structure Tyvek barrier Completed pool

29

30 Muon Dry-run Test of all installed PMTs All PMTs and LEDs functional PMT performance within expectations No grounding problems Dark rate mostly low Single PE stable LED signal clean

31 Electronics, Trigger, and DAQ PMT FEE PMT readout electronics(ihep) Fully tested during dry run Ready for Hall 1 AD & muon-veto RPC readout electronics(ustc) All components ready for Hall 1 Testing with trigger & DAQ underway Trigger(Tsinghua) Fully tested with FEE DAQ software(ihep+many) Successful integration test with FEEs, trigger and DAQ Successful Online/offline integration test Ready for hall 1 data taking RPC FEC VME subsystem 1GHz FADC

32 32 Schedule 2011 Autumn Daya Bay near site only 2012 Autumn Full operation Full Operation

33 Thanks!