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A Korean Project of Neutrino Oscillations. Soo-Bong Kim Dept. of Physics & Astronomy Seoul National University April 15, 2009. 14 C b decay. Physics in trouble with b decay. Energy & momentum are not conserved. F. A. Scott, Phys. Rev. 48 , 391 (1935). Predicted discrete spectra.
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A Korean Project of Neutrino Oscillations Soo-Bong Kim Dept. of Physics & Astronomy Seoul National University April 15, 2009
14C bdecay Physics in trouble with bdecay Energy & momentum are not conserved F. A. Scott, Phys. Rev.48, 391 (1935) Predicted discrete spectra Observed continuous b spectra 14C 14N + e– spin 0 spin 1 spin 1/2 Birth of Neutrino Total spin is not conserved, either… Bohr: Energy and momentum may not be conserved inbdecay ?…
Neutrino Wolfgang Pauli’s introduction of an imaginary particle(1931) Neutrino :Undetectable massless neutral fermion (Weakly interacting)
Neutrino: Elementary Particles • Elementary particles with almost no interactions • Almost massless: impossible to measure its mass • Universe full of neutrinos
SM GUT Tiny Neutrino Masses mass E=mc2 10-36kg 10-30kg 10-27kg
Mixing Angles (12 , 23 , 13) Unmeasured yet Oscillating Neutrinos CKM Quark Mixing and CP Violation Discovery of Neutrino Oscillations (1998) • Three flavors of neutrinos repeat transformation among them as time goes by.
Properties of Neutrinos • Almost no interaction with matter(via weak interaction only) • Mass is too small to measure • Universe full of neutrinos(330 per 1cm3) • Elementary particles with three flavors(ne, nm, nt) • Transformation among the three flavors
Neutrino Oscillation andMass Window for New Physics ! Neutrinos are hot ! Why is the neutrino physics so improtant? Origin of Our Universe !!
n2 nt nm q n1 n1 2-Neutrino Oscillation n2 nt nt nt Neutrino Oscillation • neutrino oscillations due to wave property of neutrino Flavor states Mass states n1 n2 m1 m2
Neutrino trajectory Neutrino energy Oscillation Probability
Solar Neutrino(e) Oscillations (12측정) Nuclear fusion : 4p → 4He + 2e+ + 2e + thermal energy • Deficit of solar neutrinos→Evidence for oscillations - Homestake (Cℓ,1968~1993): first measurement - Kamiokande (H2O, 1986~1993): energy/directionality - SAGE & GALLEX/GNO (Ga, 1990~2001) - Super-Kamiokande (H2O, 1996~): precision exp. • Discovery of Solar Neutrino Oscillations - SNO (D2O, 2002): detect /(e → & ) • Confirmation of Solar Neutrino Oscillations - KamLAND (2002): reactor neutrino oscillation
Confirmation of atmospheric neutrino oscillations - K2K (2004) : accelerator beam(250km) - MINOSCNGS (2006) : ~700km Atmospheric Neutrino() Oscillations (23측정) Cosmic ray (p, He, …) + Atmosphere→ /K meson→ → e + • Discovery of atmospheric neutrino oscillations ( → ) - Super-Kamiokande (1998) - measurement of 23
23 13 12 • mass difference : Dm232 = 2.4(13% )10-3 eV2 ≈ Dm132 Dm122 = 7.9(5% )10-5 eV2 • mixing angles : sin212= 0.31(9%) sin213< 0.17 (90% C.L.) sin223= 0.44(+20–11% ) Summary of Neutrino Oscillation Parameters
CP : CP phase Ue3 reactor and accelerator atmospheric SK, K2K SNO, solar SK, KamLAND 0 23 = ~ 45° 13 = ? 12 ~ 32° ? Large and maximal mixing! (Solar neutrinos & reactor neutrinos) (atmospheric neutrinos & neutrino beams) Precision Measurementof Neutrino Oscillation Parameters (New field of particle physics open!)
mass hierarchy CP violation matter 13from Reactor and Accelerator Experiments * Reactor - Clean measurement of 13 - No matter effects * Accelerator - sin2213 is a missing key parameter for any measurement of CP
울진 영광 Reactor Neutrinos Reactor Neutrinos Nuclear Power Plants • 인체에 유해한 방사능(중성자, 알파선, 베타선, 감마선)은 원자로 내부에서 차폐됨 • 핵붕괴시 방출되는 중성미자는 물질과 거의 반응을 하지 않으므로 인체에 무해하며 원자로를 빠져 나와서 사방으로 끊임없이 퍼져 나감 (매초당 ~1017n/m2 방출) • 영광발전소는 열생산 최대용량이 17GW로서 세계 2위의 강력한 중성미자 방출원임
n captureenergy e+ energy (1) 0.7<Eprompot <9MeV (2) 5<Edelayed <11MeV Detection of Reactor Neutrinos
RENO (q13 ) Reactor Neutrino Experiments Chooz: q13<130 KamLAND (q12)
Find disappearance of nefluxes due to neutrino oscillation as a function of energy using multiple, identical detectors New Reactor NeutrinoExperiment (q13) • Detectors should be at underground to reduce the cosmic-ray backgrounds • Need identical detectors to reduce the systematic errors in 1% level
L~180km KamLAND: accurate Dm212 moderate q12 3s(RENO-q12) L~5km: Dm213 L~1.5km: pure sin22q13 L~50km: accurate sin22q12 Scope of RENO Project Oscillation Parameters from Reactor Neutrinos sin22q13=0.1, En=4MeV
Disappearance Reactor neutrino disappearance Prob. due to 13 with the allowed 2 range in m232 Reduction of Reactor Neutrinos due to Oscillations • sin22q13 > 0.01 with 10 t• 14GW• 3yr ~ 400 t•GW•yr (400 t•GW•yr: a 10(40) ton far detector and a 14(3.5) GW reactor in 3 years)
Double-CHOOZ (France) Double-Chooz Collaboration: France, US, Germany, Italy, Japan, England, Brasil, Spain & Russia * 2010년 근거리/원거리검출기 동시 가동 * Proposal (June 20, 2006) : hep-ex/0606025
Daya Bay (China) Daya Bay Collaboration: China, US, Czech Republic, Hong Kong, Russia & Taiwan * Proposal to DOE (Jan. 15, 2007): hep-ex/0701029
RENO Collaboration • Chonnam National University • Dongshin University • Gyeongsang National University • Kyungpook National University • Pusan National University • Sejong University • Seoul National University • Sungkyunkwan University • Institute of Nuclear Research RAS (Russia) • Institute of Physical Chemistry and Electrochemistry RAS (Russia) +++ http://neutrino.snu.ac.kr/RENO
200m high Near Detector Reactors 70m high 100m 300m 290m 1,380m Far Detector Schematic View of Underground Facility
Activities 2009 2006 2007 2008 12 12 12 12 3 3 3 3 6 6 6 6 9 9 9 9 Detector Design & Specification Geological Survey & Tunnel Design Detector Construction Tunnel excavation Detector construction Detector Commissioning Schedule for RENO Construction
Rock sampling (DaeWoo Engineering Co.) Rock samples from boring
Far detector site: • tunnel length : 272m • overburden • height : 168.1m Rock quality map • Near detector site: • tunnel length : 110m • overburden • height : 46.1m
Mixing & Supplying Liquid Scintillators • Data Acquisition System
Mockup Detector Event Display Real time display: Online monitoring tool Basic information on histograms PMT hit display
RENO Detector • RENO Detector Design and Specification
DAQ Electronics completed (’08. 11) • Use SK new electronics • 광센서의 신호를 초고속 처리하는 ASIC을 사용한 데이터 수집 장비
R&D of Gd Loaded Liquid Scintillator • Mixing for Liquid Scintillator : • LAB(Linear Alkyl Benzene) Properties: Light yield measurement CnH2n+1-C6H5 (n=10~14) PC100% LAB100% PC40% PC20% LAB100% PC20% N2 LAB60% LAB80% MO80% • 0.1% Gd compounds with CBX (Carboxylic acids; R-COOH) 합성 연구 : - CBX : TMHA (trimethylhexanoic acid), MVA (2-methylvaleric acid)
precipitation Synthesis of Gd-carboxylate Rinse with 18MΩ water Dryer
R&D with LAB CnH2n+1-C6H5 (n=10~14) PC와 Mineral oil/Dodecane 대용으로 사용할 수 있는 LAB(Linear Alkylbenzene)의 분자 구조식 Light yield measurement • High Light Yield : not likely Mineral oil(MO) • replace MO and even Pseudocume(PC) probably • Good transparency (better than PC) • High Flash point : 147oC (PC : 48oC) • Environmentally friendly (PC : toxic) • Components well known (MO : not well known) • Domestically available:Isu Chemical Ltd. (이수화학) PC100% LAB100% PC40% PC20% LAB100% PC20% N2 LAB60% LAB80% MO80%
LAB : (C6H5)CNH2N+1 C16H26 C17H28 C18H30 C19H32 7.17% 27.63% 34.97% 30.23% # of H [m-3] = 0.631 x 1029 H/C = 1.66 Measurement of LAB Components with GC-MS