KamLAND and Geoneutrinos Sanshiro Enomoto KamLAND Collaboration RCNS, Tohoku University 1. Review of Previous Results 2. Recent Improvements (Preliminary)

Slides:



Advertisements
Similar presentations
ISAPP 2004 International School on AstroParticle Physics - Laboratori Nazionali del Gran Sasso - 28 June 9 July 2004Lino Miramonti 1 ISAPP 2004 International.
Advertisements

Simulating Radioactive Decays in Next Generation Geoneutrino Detectors Megan Geen Wheaton College Advisor: Nikolai Tolich August 17, 2011.
The SNO+ Experiment: Overview and Status
Geoneutrinos Mark Chen Queen’s University
Sensitivity of the DANSS detector to short range neutrino oscillations
Neutrino emission =0.27 MeV E=0.39,0.86 MeV =6.74 MeV ppI loss: ~2% ppII loss: 4% note: /Q= 0.27/26.73 = 1% ppIII loss: 28% Total loss: 2.3%
Super-Kamiokande Introduction Contained events and upward muons Updated results Oscillation analysis with a 3D flux Multi-ring events  0 /  ratio 3 decay.
suekane 05 Erice School1 KamLAND F.Suekane Research Center for Neutrino Science Tohoku University Erice School
Lauren Hsu Lawrence Berkeley National Laboratory
Prospects for 7 Be Solar Neutrino Detection with KamLAND Stanford University Department of Physics Kazumi Ishii.
20 January 2005Steve Dye, HPU1 Neutrino Geophysics in Hawaii Presentation by Steve Dye Associate Professor of Physics Hawaii Pacific University January.
KamLand By Roy Lehn Omaha Roncalli. Means Kamioka Liquid scintillator Anti- Neutrino Detector.
Experimental Study of Geoneutrinos with KamLAND
Experimental Status of Geo-reactor Search with KamLAND Detector
Results and Future of the KamLAND Experiment
Results and plans of the KamLAND experiment
S. Dye /15/05 Neutrino Geophysics Workshop 1 Hawaii Anti-Neutrino Observatory For the Hanohano collaboration: Steve Dye University of Hawaii at Manoa.
Geoneutrino Overview 1.Review of Geoneutrino Physics (with KamLAND)
Exploring the Geo-reactor Hypothesis with Neutrinos Jelena Maričić KamLAND Collaboration March 24 th 2007 DOANOW Workshop University of Hawai’i.
Potassium Geo-neutrino Detection Mark Chen Queen’s University Neutrino Geophysics, Honolulu, Hawaii December 15, 2005.
Neutrino emission =0.27 MeV E=0.39,0.86 MeV =6.74 MeV ppI loss: ~2% ppII loss: 4% note: /Q= 0.27/26.73 = 1% ppIII loss: 28% Total loss: 2.3%
Measuring  13 with Reactors Stuart Freedman University of California at Berkeley SLAC Seminar September 29, 2003.
Lens ALens B Avg. Angular Resolution Best Angular Resolution (deg) Worst Angular Resolution (deg) Image Surface Area (mm 2 )
Low-energy neutrino physics with KamLAND Tadao Mitsui (Research Center for Neutrino Science, Tohoku U.) for the KamLAND collaboration Now2010, Grand Hotel.
1 The Daya Bay Reactor Electron Anti-neutrino Oscillation Experiment Jianglai Liu (for the Daya Bay Collaboration) California Institute of Technology APS.
KamLAND Experiment Kamioka Liquid scintillator Anti-Neutrino Detector - Largest low-energy anti-neutrino detector built so far - Located at the site of.
Geo Neutrino Detection at KamLAND F.Suekane RC S Tohoku University 5th Workshop on Applied Antineutrino Physics (AAP2009) Angra dos Reis, Brazil 20/03/2009.
Solar neutrino measurement at Super Kamiokande ICHEP'04 ICRR K.Ishihara for SK collaboration Super Kamiokande detector Result from SK-I Status of SK-II.
Lino MiramontiJune 9-14, 2003, Nara Japan 1st Yamada Symposium Neutrinos and Dark Matter in Nuclear Physics.
Requirement for photon-detectors at directional measurement of anti-neutorinos with KamLAND Mio Nakamura Research Center for Neutrino Science,Tohoku University.
Geo-neutrino Working Group Goals and Progress 10 December CIDER Workshop.
KamLAND : Studying Neutrinos from Reactor Atsuto Suzuki KamLAND Collaboration KEK : High Energy Accelerator Research Organization.
Using Reactor Anti-Neutrinos to Measure sin 2 2θ 13 Jonathan Link Columbia University Fermilab Long Range Planning Committee, Neutrino Session November.
RENO and the Last Result
1 A roadmap for geo-neutrinos: theory and experiment Ferrara University & INFN Gianni Fiorentini arXiv:
SNS2 Workshop August 28-29, 2003 Richard Talaga, Argonne1 Calibration of the OMNIS-LPC Supernova Neutrino Detector Outline –OMNIS Experiment and Detectors.
Yasuhiro Kishimoto for KamLAND collaboration RCNS, Tohoku Univ. September 12, 2007 TAUP 2007 in Sendai.
KamLAND, a culmination of half century of reactor neutrino studies. Petr Vogel, Caltech.
Present and future detectors for Geo-neutrinos: Borexino and LENA Applied Antineutrino Physics Workshop APC, Paris, Dec L. Oberauer, TU München.
Kr2Det: TWO - DETECTOR REACTOR NEUTRINO OSCILLATION EXPERIMENT AT KRASNOYARSK UNDERGROUND SITE L. Mikaelyan for KURCHATOV INSTITUTE NEUTRINO GROUP.
Geo-neutrino: Experiments Jelena Maricic Drexel University Neutrino Champagne – LowNu2009 October 20, 2009 BNO.
1 IDM2004 Edinburgh, 9 september 2004 Helenia Menghetti Bologna University and INFN Study of the muon-induced neutron background with the LVD detector.
New Results from the Salt Phase of SNO Kathryn Miknaitis Center for Experimental Nuclear Physics and Astrophysics, Univ. of Washington For the Sudbury.
Results from RENO Soo-Bong Kim (KNRC, Seoul National University) “17 th Lomosonov Conference on Elementary Particle Physics” Moscow. Russia, Aug ,
The Daya Bay Reactor Neutrino Experiment R. D. McKeown Caltech On Behalf of the Daya Bay Collaboration CIPANP 2009.
Performance Comparisons of Safeguard Detector Designs D. Reyna (Argonne National Laboratory) with help from R.W. McKeown (Drexel University)
Antineutrino Physics in KamLAND Atsuto Suzuki High Energy Accelerator Research Organization (KEK) 1. KamLAND Experiment 2. Reactor Antineutrino Oscillation.
Search for Sterile Neutrino Oscillations with MiniBooNE
Karsten Heeger Beijing, January 18, 2003 Design Considerations for a  13 Reactor Neutrino Experiment with Multiple Detectors Karsten M. Heeger Lawrence.
Double Chooz Near Detector Guillaume MENTION CEA Saclay, DAPNIA/SPP Workshop AAP 2007 Friday, December 14 th, 2007
Daya Bay Reactor Neutrino Experiment On behalf of the DayaBay collaboration Virginia Polytechnic Institute and State University Joseph ykHor YuenKeung,
1 Muon Veto System and Expected Backgrounds at Dayabay Hongshan (Kevin) Zhang, BNL DayaBay Collaboration DNP08, Oakland.
Current status of XMASS experiment 11 th International Workshop on Low Temperature Detectors (LTD-11) Takeda Hall, University of Tokyo, JAPAN 8/1, 2005.
Karsten Heeger, Univ. of Wisconsin Yale University, March 1, 2010  13 from Global Fits current best limit sin 2 2θ 13 < CL Fogli, et al., arXiv:0905:3549.
1 LTR 2004 Sudbury, December 2004 Helenia Menghetti, Marco Selvi Bologna University and INFN Large Volume Detector The Large Volume Detector (LVD)
Recent Results from RENO NUFACT2014 August. 25 to 30, 2014, Glasgow, Scotland, U.K. Hyunkwan Seo on behalf of the RENO Collaboration Seoul National University.
Solar Neutrino Results from SNO
5th June 2003, NuFact03 Kengo Nakamura1 Solar neutrino results, KamLAND & prospects Solar Neutrino History Solar.
1 Work report ( ) Haoqi Lu IHEP Neutrino group
Present and future of Geo-neutrinos Bill McDonough Geology, U Maryland.
Double Chooz Experiment Status Jelena Maricic, Drexel University (for the Double Chooz Collaboration) September, 27 th, SNAC11.
IBD Detection Efficiencies and Uncertainties
SoLid: Recent Results and Future Prospects
Simulation for DayaBay Detectors
Neutron backgrounds in KamLAND
KamLAND Update NuFact 05 Lauren Hsu June 21, 2005
Daya Bay Neutrino Experiment
Davide Franco for the Borexino Collaboration Milano University & INFN
Intae Yu Sungkyunkwan University (SKKU), Korea KNO 2nd KNU, Nov
Presentation transcript:

KamLAND and Geoneutrinos Sanshiro Enomoto KamLAND Collaboration RCNS, Tohoku University 1. Review of Previous Results 2. Recent Improvements (Preliminary) 3. Future Prospects 4. Far Future Dreams Applied Antineutrino Physics 2007, APC Laboratory Paris, December

KamLAND Experiment observes low energy anti-neutrinos in the Kamioka Mine, Hida, Japan consists of 1000ton Liquid Scintillator, surrounded by 1845 PMT ’ s Reaction: 1000m Kamioka Mine 2002 Jan: Start data taking 2002 Dec: Evidence for reactor neutrino disappearance (145 days) 2005 Jan: Evidence of reactor neutrino spectral distortion (514 days) 2005 Jul: Investigation of geoneutrinos (749 days) 2007 Dec: 1491 day data accumulated

KamLAND Detector Yields light on ionization (8000 photons / MeV) Mainly consists of only C and H 20m Liquid Scintillator Liquid Scintillator 1000 ton Contained in plastic balloon 17-inch PMT inch 554 Detector Center Surrounded by (PMT : Photo Multiplier Tube, a photo sensor) PC: 20%dodecane: 20%PPO: 1.5 g/l

Antineutrino Detection Method time τ~210 μsec Two characteristic signals Clear event identification Great BG suppression

KamLAND Detector Japan Arc Kamioka Mine KamLAND Outer View KamLAND Inner View Photo Multiplier Tube Scintillator Container

Antineutrino Sources Nuclear Power ReactorsHPE (U/Th) in the Earth ~50% from surrounding crust ~25% from mantle

Reactor Neutrino Flux Calculation Example of Reactor Operation Data Neutrino Flux at KamLAND (no oscillation case) Japanese Reactors (95.5%): Operation data, including fuel burn-up, for each core are provided by operators. Korean Reactors (3.4%): Flux are calculated based on published electrical output Other Reactors (1.1%): Nominal power is assumed Total ~2% error (conservative)

Expected Geoneutrino Flux U-Series 2.3x10 6 [1/cm 2 /sec] Th-Series 2.0x10 6 [1/cm 2 /sec] Geoneutrino Flux Prediction BSE composition by [McDonough1999] Crustal composition by [Rudnick et al. 1995] Crustal thickness by CRUST 2.0 Uniform Mantle Model No U/Th in the Core With target protons, U-Series 32 events / year Th-Series 8 events / year Geoneutrino Origination Points Detectable at KamLAND (MC) South America Antarctic Australia KamLAND Greenland 50% within 500km 25% from Mantle [Earth.Plan.Sci.Lett, 258, 147 (2007)]

KamLAND Antineutrino Spectrum (expected) Neutrino Property Study Signature of Neutrino Oscillation Precision Measurement of Oscillation Parameters [Phys.Rev.Lett. 94, (2005)] Geoneutrinos: Neutrino Application Direct measurement of HPE in the Earth [Nature 436, 499 (2005)]

Geoneutrino Expected Rate and Spectrum Fiducial Volume: 408 ton Live-time: 749 days Efficiency: 68.7% Expected Geoneutrinos U-Series: 14.9 Th-Series:4.0 Backgrounds Reactor: 82.3±7.2 (α,n) : 42.4±11.1 Accidental:2.38±0.01 BG total: 127.4±13.3

First Geoneutrino Result Fiducial Volume: 408 ton Live-time: 749 days Efficiency: 68.7% Expected Geoneutrinos U-Series: 14.9 Th-Series:4.0 Backgrounds Reactor: 82.3±7.2 (α,n) : 42.4±11.1 Accidental:2.38±0.01 BG total: 127.4±13.3 Observed: 152 Number of Geoneutrinos: +19 -18 25 [Nature 436, 499 (2005)]

Spectrum Analysis Number of Geoneutrinos: % C.L. upper limit:70.7 events Significance 95.3% (1.99-sigmas) +15.6 -14.6 Parameters N U, N Th : Number of Geoneutrinos sin 2 2θ, Δm 2 : Neutrino Oscillation α 1, α 2 : Backgrounds Uncertainties KamLAND is insensitive to U/Th ratio → adopt U/Th ~ 3.9 from Earth science Discrimination of U and Th Total Number of U and Th Earth Model Prediction

Flux Prediction from Earth Models Scale Bulk Composition Fix Crustal Composition, Parameterize Mantle U+Th Mass [kg] Geoneutrino Flux [1/cm 2 /sec]

Comparison with Earth Model Predictions Consistent with BSE model predictions 99%C.L. upper limit too large to be converted to heat production (No Earth models applicable) U+Th Mass [kg] Geoneutrino Flux [1/cm 2 /sec] Earth Model Prediction KamLAND 1-σ Range KamLAND 99% Limit Total Terrestrial Heat Flow (44TW)

KamLAND Problem: Overwhelming Backgrounds Reactor Neutrino BG (α,n) BG 206 Pb 210 Bi 210 Po 210 Pb d 22.3 y stable d 222 Rn 3.8 d 13 C (α,n) 16 O n + p → n + p 210 Po decay rate error 14% Cross-section error: 20% Quenting factor error: 10%

Improvements New (α,n) Cross section data available Vertex reconstruction improved (for 210 Po decay rate) Proton quenching factor measured 210 Po- 13 C source calibration performed ⇒ (α,n) error reduced from ~26% to ~11% (α,n) Background error reduced Po-C Calibration (MC/Data)P quenching measurement

Improved Results (Preliminary) More statistics accumulated: 749 day to 1491 day (α,n) error reduced: ~26% to ~11% Reconstruction improved (off-axis calibration) Analysis improved: – Fiducial volume increased – Time variation included – Optimal event selection with figure-of-merit basis Preliminary

Geophysics with Improved Results (Preliminary) Earth Model Prediction KamLAND 1-σ Range KamLAND 99% Limit Error is reduced from 56% to 36% Consistent with BSE model predictions 99%C.L. upper limit is approaching to the total terrestrial heat Preliminary

Future Prospects LS Distillation in Progress ⇒ removes radioactivity by we remove these distilled scintillator Preliminary

Future Prospects If combined with the current 1491 day data, Error is reduced:from 36% to 25% (error is dominated by reactor neutrinos) Significance: % (3.96 sigmas) BEFORE AFTER we remove these Assuming: reduction of 210 Pb Enlarged fiducial volume (5.5m) Improved selection criteria 749 days livetime

Future Prospects 25% uncertainty 749 days after purification, combined with current 1491 day data Measurement error is comparable with Earth model predictions 99%C.L. limit can exclude some “ upper limit ” models 99% upper limit 1.6 times above BSE

Far Future Dreams: Directional Sensitivity Directional information provides: ・Rejection of backgrounds ・Separation of crust and mantle ・Earth tomography by multiple detectors Good News: ・Recoiled neutron remembers direction Bad News: ・Thermalization blurs the info ・Gamma diffusion spoils the info ・Reconstruction resolution is too poor Wish List: ・large neutron capture cross-section ・(heavy) charged particle emission and ・good resolution detector (~1cm)

Towards Directional Sensitivity 1 Neutron Capture Position (MC) Delayed Event Position (MC) 6 Li loading helps preserving directional information Large neutron capture cross-section: 940 barn 6 Li + n → α + T : no gamma-ray emission Natural abundance 7.59% Various chemical forms for Li loading are being tested …

Towards Directional Sensitivity 2 ~1M pixel imaging can achieve 1 cm resolution LS lends image intensifier 10cm CCD lens LS image intensifier CCD Fresnel lens Proper optics need to be implemented Sensitivity to 1 p.e. and high-speed readout required First step for LS imaging, just started … Muon Event ??? Isotope Decay Event ??? (Bis-MSB added)

Summary KamLAND, low-energy antineutrino detector, – determined oscillation parameters precisely – made first experimental investigation on geoneutrinos Recent updates with more stat. and less syst. err., – reduced geoneutrino measurement error from 54% to 36% – Upper limit is comparable with Earth model limits Further LS purification is in progress – will reduce error to ~25% – Measurement error will be comparable with Earth models R&D for directional sensitivity underway