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KamLAND (Anti-Neutrino Status) The 10th International Conference on Topics in Astroparticle and Underground Physics Sep. 14, 2007 Itaru Shimizu (Tohoku Univ.) KamLAND Collaboration T. Ebihara,1 S. Enomoto,1 K. Furuno,1 Y. Gando,1 K. Ichimura,1


  1. KamLAND (Anti-Neutrino Status) The 10th International Conference on Topics in Astroparticle and Underground Physics Sep. 14, 2007 Itaru Shimizu (Tohoku Univ.)

  2. KamLAND Collaboration T. Ebihara,1 S. Enomoto,1 K. Furuno,1 Y. Gando,1 K. Ichimura,1 H. Ikeda,1 K. Inoue,1 Y. Kibe,1 Y. Kishimoto,1 M. Koga,1 Y. Konno,1 A. Kozlov,1 Y. Minekawa,1 T. Mitsui,1 K. Nakajima,1, K. Nakajima,1 K. Nakamura,1 K. Owada,1 I. Shimizu,1 J. Shirai,1 F. Suekane,1 A. Suzuki,1 K. Tamae,1 S. Yoshida,1 J. Busenitz,2 T. Classen,2 C. Grant,2 G. Keefer,2 D.S. Leonard,2 D. McKee,2 A. Piepke,2 M.P. Decowski,3 S.J. Freedman,3 B.K. Fujikawa,3 F. Gray,3, L. Hsu,3, R. Kadel,3 K.-B. Luk,3 H. Murayama,3 T. O’Donnell,3 H.M. Steiner,3 L.A. Winslow,3 D.A. Dwyer,4 C. Jillings,4, 、 C. Mauger,4 R.D. McKeown,4 C. Zhang,4 B.E. Berger,5 C.E. Lane,6 J. Maricic,6 T. Miletic,6 M. Batygov,7 J.G. Learned,7 S. Matsuno,7 S. Pakvasa,7 J. Foster,8 G.A. Horton-Smith,8 A. Tang,8 S. Dazeley,9, K. Downum,10 G. Gratta,10 K. Tolich,10 W. Bugg,11 Y. Efremenko,11 Y. Kamyshkov,11 O. Perevozchikov,11 H.J. Karwowski,12 D.M. Markoff,12 W. Tornow,12 K. M. Heeger,13 F. Piquemal,14 and J.-S. Ricol14 (KamLAND Collaboration) 1Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan 2Department of Physics and Astronomy, University of Alabama, Tuscaloosa, Alabama 35487, USA 3Physics Department, University of California at Berkeley and Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA 4W. K. Kellogg Radiation Laboratory, California Institute of Technology, Pasadena, California 91125, USA 5Department of Physics, Colorado State University, Fort Collins, Colorado 80523, USA 6Physics Department, Drexel University, Philadelphia, Pennsylvania 19104, USA 7Department of Physics and Astronomy, University of Hawaii at Manoa, Honolulu, Hawaii 96822, USA 8Department of Physics, Kansas State University, Manhattan, Kansas 66506, USA 9Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA 10Physics Department, Stanford University, Stanford, California 94305, USA 11Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA 12Triangle Universities Nuclear Laboratory, Durham, North Carolina 27708, USA and Physics Departments at Duke University, North Carolina State University, and the University of North Carolina at Chapel Hill 13Department of Physics, University of Wisconsin, 1150 University Avenue, Madison, WI 53706, USA 14CEN Bordeaux-Gradignan, IN2P3-CNRS and University Bordeaux I, F-33175 Gradignan Cedex, France

  3. KamLAND Kamioka Liquid Scintillator Anti-Neutrino Detector Inner tank 1,000 ton LS Outer water tank Kamioka ~ 180 km baseline 34% photo-coverage with 1325 17” and 554 20” PMTs 2 flavor neutrino oscillation most sensitive region ∆ m 2 = (1 / 1 . 27) · ( E [MeV] /L [ m ]) · ( π / 2) P ( ν e → ν e ) = 1 − sin 2 2 θ sin 2 (1 . 27 ∆ m 2 [eV 2 ] l [ m ] ) E [MeV] ∼ 3 × 10 − 5 eV 2 reactor neutrino : sensitive to LMA solution

  4. 観測エネルギー (MeV) 1.0 2.6 8.5 0.4 太陽ニュートリノ 地球ニュートリノ 原子炉ニュートリノ 超新星ニュートリノ Physics Target in KamLAND observed energy (MeV) solar neutrino geo neutrino reactor neutrino supernova neutrino solar neutrino reactor neutrino γ ν x geo neutrino prompt e + p e - ¯ ν x ν e γ delayed e - mean capture time n γ ~ 200 µ sec on proton neutrino detection by electron scattering anti-neutrino detection by inverse beta-decay

  5. reaction accidental fast-neutron ¹⁶O* ¹²C* reactor neutrino (α, n) Reactor and Geo Neutrino Analysis S / B ratio map (energy v.s. radius) previous result S/N 5 m 5.5 m separated analysis 2 10 window for reactor 8 and geo neutrinos 10 7 Prompt Energy (MeV) 6 reactor neutrino 1 (2.6 - 8.5 MeV, R 5.5 m) 5 -1 10 4 -2 10 3 geo neutrino -3 10 2 (0.9 - 2.6 MeV, R 5.0 m) -4 1 10 0 0.2 0.4 0.6 0.8 1 3 (R/6.5m) large accidental B.G. Analysis improvement caused by external γ -rays (1) efficient accidental background rejection (2) combined analysis of reactor and geo neutrinos

  6. Anti-Neutrino Event Selection 2.2 < E prompt < 2.3 MeV (a) Accidental B.G. discrimination Events / Bin discriminator based on 5 parameters (E d , Δ R, Δ T, R p , R d ) accidental anti-neutrino 10 background (reactor, geo) L ratio = f ν / (f ν + f accidental ) 1 f : PDF generated by -1 10 S MC simulation Selection : Maximize “Figure of Merit” -2 10 √ S + B accidental (b) µ spallation cut -3 10 • Δ T µ > 2 s after showing µ ( Δ Q > 10 6 p.e.) -4 10 • Δ T µ > 2 s or Δ L > 3 m after non-showering µ -5 Detection efficiency 10 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Likelihood Ratio 100 10 Figure of Merit efficiency 8 90 9 Figure of Merit Efficiency 80 8 7.5 Figure of Merit 70 7 Figure of Merit 7 Efficiency (%) Figure of Merit 60 6 6.5 50 5 preliminary 6 40 4 5.5 maximum “Figure of Merit” 30 3 efficiency decrease L ratio > 0.967 5 20 2 caused by larger 4.5 accidental BG 10 1 0 0 4 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0 1 2 3 4 5 6 7 8 Likelihood Ratio E (MeV) prompt

  7. Systematic Uncertainty “full volume” calibration lowered the fiducial volume error (4.7% in previous analysis) preliminary Detector related Reactor related Fiducial volume 1.8% ν e spectra 2.4% Energy scale 1.5% Reactor power 2.1% L-selection eff. 0.6% Fuel composition 1.0% OD veto 0.2% Long-lived nuclei 0.3% Cross section 0.2% Time lag 0.01% 2.4% 3.4% Total systematic uncertainty : 4.1%

  8. Full Volume Calibration 5 event rate (arbitrary) Bias [cm] z-axis 60 60 Co Co 4 off-axis 3 2 1 z-axis 0 -1 off-axis -2 -3 bias < 3 cm -4 -5 0 100 200 300 400 500 600 R [cm] 5 Bias [cm] source deployment 68 Ge 68 Ge 4 off-axis 3 “4pi calibration” system for 2 the off-axis source deployment 1 z-axis 0 bias < 3 cm corresponds to -1 1.8% volume uncertainty -2 -3 bias < 3 cm cross-checked by -4 12 B/ 12 N uniformity -5 0 100 200 300 400 500 600 R [cm]

  9. ( α , n) Background Estimation natural abundance cross section measurement 6.130MeV 3 - 1.1% 1 cross section [barn] Q = 2.2MeV 6.049MeV 0 + prompt -1 10 13 C( α , n) 16 O γ (6.1MeV) -2 10 or e + e - (6.0MeV) 16 O 13 C α 0 + recoil proton -3 10 16 O p delayed -4 n S. Harissopulos et al. 10 γ (2.22MeV) JENDL n -5 10 prompt 12 C d -6 10 (4.4MeV) γ 0 1 2 3 4 5 12 C(n, n γ ) 12 C alpha energy [MeV] neutron yield difference < 4% -6 10 � Po 13 C source calibration events/MeV/alpha ( α , n) background estimation ground state 6 163.3 ± 18.0 events for ground state 1st excited state 18.7 ± 3.7 events for excited state 4 2nd excitted state Estimation uncertainty 2 11% for ground state 0 1 2 3 4 5 6 7 8 20% for excited state visible energy [MeV]

  10. Rate Analysis above 2.6 MeV “Reactor” rate analysis period for “KamLAND 2004” updated 1.6 (2.6 MeV threshold) 515 days 976 days 1.4 1.2 events/day No osci. expected 1549 1 0.8 0.6 63 Background 0.4 total 1491 days 0.2 (see Poster Sessions : Ichimura and Minekawa et al.) 0 Observed events 985 2002 2003 2004 2005 2006 2007 1.6 Ratio = (obs. - B.G.) / No osci. preliminary e s 1.4 a c observed rate [events/day] n 0.594 ± 0.020(stat) ± 0.026(syst) o 1.2 i t a l l i c s 1 o 8.5 σ disappearance significance o n 0.8 n i d Fit constrained through B.G. expected e t 0.6 c e p x χ 2 / ndf = 3.1 / 4 e 0.4 Fit with a horizontal line 0.2 90% C.L. χ 2 / ndf = 11.8 / 4 0 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 (1.9% C.L.) expected rate in no oscillation [events/day]

  11. Energy Spectrum above 0.9 MeV exposure : 2881 ton-year (3.8 × 766 ton-year for “KamLAND 2004”) “Geo + Reactor” geo neutrinos previous result (above 2.6 MeV) 300 combined analysis KamLAND data No osci. expected 2178 no oscillation 250 best-fit oscillation Background 276 Events / 0.425 MeV accidental (w/o geo neutrino) 13 16 C( ,n) O ! 200 (Ichimura and Minekawa et al.) Expected Geo " e Observed events 1609 best-fit osci. + BG 150 + Expected Geo " best-fit e (tan 2 θ , Δ m 2 ) 100 = (0.56, 7.58 × 10 -5 eV 2 ) preliminary 50 free parameter : geo neutrinos (U, Th) = (39.3, 29.4) events 0 0 1 2 3 4 5 6 7 8 goodness of fit using equal probability bins E (MeV) prompt χ 2 / ndf = 21.0 / 16 (18.0% C.L.) best-fit χ 2 / ndf = 63.9 / 17 no osci. Scaled no oscillation spectrum is excluded at 5.2 σ

  12. L/E plot Ratio = (observed - B.G.) / (no osci. expected) w/o geo neutrino 1.4 KamLAND data best-fit osci. best-fit osci. + Expected Geo 1.2 ! e consistent with geo neutrino expectation 1 from an earth model Ratio 0.8 20% geo neutrino flux uncertainty 0.6 (a claim based on the geology) 0.4 preliminary 0.2 0 20 30 40 50 60 70 80 90 100 L /E (km/MeV) 0 ! e L 0 : a fixed baseline (180 km) Distortion effect is clearly illustrated by L/E plot

  13. Neutrino Oscillation previous result (above 2.6 MeV) 1.4 KamLAND data CHOOZ data short baseline best-fit osci. best-fit osci. + Expected Geo 1.2 ! experiment e 1 1st 2nd 3rd Ratio 0.8 0.6 0.4 preliminary 0.2 hypothetical single reactor 0 0 10 20 30 40 50 60 70 at 180 km L /E (km/MeV) 0 ! e KamLAND covers the 2nd and 3rd maximum characteristic of neutrino oscillation

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