Recent Results and Prospects from Kam LAND Nikolai

  • Slides: 22
Download presentation
Recent Results and Prospects from Kam. LAND Nikolai Tolich August 16, 2004 PASCOS '04

Recent Results and Prospects from Kam. LAND Nikolai Tolich August 16, 2004 PASCOS '04

Kam. LAND Collaboration T. Araki 1, K. Eguchi 1, S. Enomoto 1, K. Furuno

Kam. LAND Collaboration T. Araki 1, K. Eguchi 1, S. Enomoto 1, K. Furuno 1, K. Ichimura 1, H. Ikeda 1, K. Inoue 1, K. Ishihara 1, T. Iwamoto 1, T. Kawashima 1, Y. Kishimoto 1, M. Koga 1, Y. Koseki 1, T. Maeda 1, T. Mitsui 1, M. Motoki 1, K. Nakajima 1, H. Ogawa 1, K. Owada 1, J. -S. Ricol 1, I. Shimizu 1, J. Shirai 1, F. Suekane 1, A. Suzuki 1, K. Tada 1, O. Tajima 1, K. Tamae 1, Y. Tsuda 1, H. Watanabe 1, J. Busenitz 2, T. Classen 2, Z. Djurcic 2, G. Keefer 2, K. Mc. Kinny 2, D-M. Mei 2, A. Piepke 2, E. Yakushev 2, B. E. Berger 3, Y. D. Chan 3, M. P. Decowski 3, D. A. Dwyer 3, S. J. Freedman 3, Y. Fu 3, B. K. Fujikawa 3, J. Goldman 3, F. Gray 3, K. M. Heeger 3, K. T. Lesko 3, K. -B. Luk 3, H. Murayama 3, A. W. P. Poon 3, H. M. Steiner 3, L. A. Winslow 3, G. A. Horton-Smith 4, C. Mauger 4, R. D. Mc. Keown 4, P. Vogel 4, C. E. Lane 5, T. Miletic 5, P. W. Gorham 6, G. Guillian 6, J. G. Learned 6, J. Maricic 6, S. Matsuno 6, S. Pakvasa 6, S. Dazeley 7, S. Hatakeyama 7, A. Rojas 7, R. Svoboda 7, B. D. Dieterle 8, J. Detwiler 9, G. Gratta 9, K. Ishii 9, N. Tolich 9, Y. Uchida 9, M. Batygov 10, W. Bugg 10, Y. Efremenko 10, Y. Kamyshkov 10, A. Kozlov 10, Y. Nakamura 10, H. J. Karwowski 11, D. M. Markoff 11, J. A. Messimore 11, K. Nakamura 11, R. M. Rohm 11, W. Tornow 11, R. Wendell 11, A. R. Young 11, M. -J. Chen 12, Y. -F. Wang 12, and F. Piquemal 13 1 Research Center for Neutrino Science, Tohoku University, Sendai 980 -8578, Japan of Physics and Astronomy, University of Alabama, Tuscaloosa, Alabama 35487, USA 3 Physics Department, University of California at Berkeley and Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA 4 W. K. Kellogg Radiation Laboratory, California Institute of Technology, Pasadena, California 91125, USA 5 Physics Department, Drexel University, Philadelphia, Pennsylvania 19104, USA 6 Department of Physics and Astronomy, University of Hawaii at Manoa, Honolulu, Hawaii 96822, USA 7 Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA 8 Physics Department, University of New Mexico, Albuquerque, New Mexico 87131, USA 9 Physics Department, Stanford University, Stanford, California 94305, USA 10 Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA 11 Triangle 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 12 Institute of High Energy Physics, Beijing 100039, People's Republic of China 13 CEN Bordeaux-Gradignan, IN 2 P 3 -CNRS and University Boreaux I, F-33175 Gradignan Cedex, France 2 Department August 16, 2004 PASCOS '04 2

Introduction to reactor measurement Kam. LAND ne Nuclear Reactor August 16, 2004 L PASCOS

Introduction to reactor measurement Kam. LAND ne Nuclear Reactor August 16, 2004 L PASCOS '04 3

Kam. LAND Situated to Detect Reactor Anti-neutrinos Kashiwazaki Kam. LAND Takahama Ohi August 16,

Kam. LAND Situated to Detect Reactor Anti-neutrinos Kashiwazaki Kam. LAND Takahama Ohi August 16, 2004 PASCOS '04 4

Detecting Anti-neutrinos at Kam. LAND • Kam. LAND (Kamioka Liquid scintillator Anti. Neutrino Detector)

Detecting Anti-neutrinos at Kam. LAND • Kam. LAND (Kamioka Liquid scintillator Anti. Neutrino Detector) • Inverse beta decay ne + p → e + + n Prompt 0. 5 Me. V e 0. 5 Me. V Delayed 2. 2 Me. V e+ n p p d ne • The positron losses its energy then annihilates with an electron • The neutron first thermalizes then captures on a proton with a mean capture time of ~200 ms August 16, 2004 PASCOS '04 5 g

1 km Overburden The Detector Electronics Hut Steel Sphere PMTs 1325 17” 554 20”

1 km Overburden The Detector Electronics Hut Steel Sphere PMTs 1325 17” 554 20” 34% coverage 1 kton liquidscintillator Water Cherenkov outer detector 225 PMTs August 16, 2004 PASCOS '04 6

Inside the Detector August 16, 2004 PASCOS '04 7

Inside the Detector August 16, 2004 PASCOS '04 7

Determining the Event Vertex (2. 5 Me. V) (1. 1 Me. V) (1. 0

Determining the Event Vertex (2. 5 Me. V) (1. 1 Me. V) (1. 0 Me. V) August 16, 2004 PASCOS '04 8

Tagged Cosmogenics used as Calibration Device 12 B τ=29. 1 ms Q=13. 4 Me.

Tagged Cosmogenics used as Calibration Device 12 B τ=29. 1 ms Q=13. 4 Me. V 12 N τ=15. 9 ms Q=17. 3 Me. V μ August 16, 2004 PASCOS '04 9

Fraction of volume used verified using μ-produced 12 B/12 N and n Neutrons 12

Fraction of volume used verified using μ-produced 12 B/12 N and n Neutrons 12 B/12 N August 16, 2004 PASCOS '04 10

Energy Calibration Using g Sources and 12 B/12 N n-p 68 Ge n-12 C

Energy Calibration Using g Sources and 12 B/12 N n-p 68 Ge n-12 C 60 Co 65 Zn • Includes Birks law, Cherenkov light to obtain constants for γ and e–type depositions August 16, 2004 PASCOS '04 11

Selecting Electron Anti-neutrinos • Rprompt, Rdelayed < 5. 5 m • ΔR < 2

Selecting Electron Anti-neutrinos • Rprompt, Rdelayed < 5. 5 m • ΔR < 2 m • 0. 5μs < ΔT < 1 ms • 1. 8 Me. V < Edelayed < 2. 6 Me. V • 2. 6 Me. V < Eprompt < 8. 5 Me. V • • 89. 8% tagging efficiency 33% increase in volume Delayed Prompt 0. 5 Me. V August 16, 2004 PASCOS '04 2. 2 Me. V e+ 12 g

Japan Nuclear Reactor Scandal August 16, 2004 PASCOS '04 13

Japan Nuclear Reactor Scandal August 16, 2004 PASCOS '04 13

2003 saw a substantial dip in reactor anti-neutrino flux August 16, 2004 PASCOS '04

2003 saw a substantial dip in reactor anti-neutrino flux August 16, 2004 PASCOS '04 14

Fit constrained through known background c 2/dof=2. 1/4 N o os ci lla tio

Fit constrained through known background c 2/dof=2. 1/4 N o os ci lla tio n ex pe ct ed Good correlation with reactor flux 90% CL August 16, 2004 PASCOS '04 15

Energy spectrum shows distortion • Best fit c 2/dof=18. 3/18 (goodness of fit is

Energy spectrum shows distortion • Best fit c 2/dof=18. 3/18 (goodness of fit is 42%) • Fit to rescaled reactor spectrum c 2/dof=43. 4/19 (excluded at 99. 89% CL) August 16, 2004 PASCOS '04 16

Oscillations with L/E Kam. LAND sees reactor neutrinos from different distances Hypothetical oscillation curve

Oscillations with L/E Kam. LAND sees reactor neutrinos from different distances Hypothetical oscillation curve for single reactor distance August 16, 2004 PASCOS '04 17

Alternative neutrino propagation models • Decay* excluded at 95% CL • Decoherence† excluded at

Alternative neutrino propagation models • Decay* excluded at 95% CL • Decoherence† excluded at 94% CL *V. Barger et al. Phys. Rev. Lett. , 82 (1999) 2640 †E. Lisi et al. Phys. Rev. Lett. , 85 (2000) 1166 August 16, 2004 PASCOS '04 18

Two flavor rate and shape analysis • LMA 2 excluded at 99. 6% CL

Two flavor rate and shape analysis • LMA 2 excluded at 99. 6% CL • Best fit Dm 2=8. 3× 10 -5 e. V 2 sin 22 q=0. 83 • LMA 0 excluded at 94% CL August 16, 2004 PASCOS '04 19

Improvement since first result New Result August 16, 2004 Previous Result PASCOS '04 20

Improvement since first result New Result August 16, 2004 Previous Result PASCOS '04 20

Combined solar and Kam. LAND two flavor result August 16, 2004 PASCOS '04 21

Combined solar and Kam. LAND two flavor result August 16, 2004 PASCOS '04 21

Prospects Geo Signal Reactor Signal August 16, 2004 • Measure the global concentration of

Prospects Geo Signal Reactor Signal August 16, 2004 • Measure the global concentration of U and Th in the Earth • Solar anti-neutrinos • Solar neutrinos • Exotic nucleon decay modes • Observe supernova neutrinos PASCOS '04 22