1. Oto Cosmo Observatory 2. Detectors and Physics Results 3. Future Plans 4. Progress of Oto Lab. Oto Cosmo Observatory Present and Future Hiro Ejiri RCNP.

Slides:



Advertisements
Similar presentations
LRP2010 WG5 Fundamental Interactions Nathal Severijns ( K.U.Leuven) for WG5 Scoping workshop Frankfurt, October th 2009.
Advertisements

Masaki Yamashita XMASS at Kamioka Large Scale Cryogenic detector in the underground laboratory Masaki Yamashita Kamioka observatory, ICRR, Univ. Of Tokyo.
Hadron physics with GeV photons at SPring-8/LEPS II
Status of the XMASS experiment S. Moriyama for the XMASS collaboration Kamioka observatory, Institute for Cosmic Ray Research, Univ. of Tokyo, July 27,
Status of XMASS experiment Shigetaka Moriyama Institute for Cosmic Ray Research, University of Tokyo For the XMASS collaboration September 10 th, 2013.
Neutrino oscillations/mixing
March 12, 2005Benasque Neutrinos Theory Neutrinos Theory Carlos Pena Garay IAS, Princeton ~
DMSAG 14/8/06 Mark Boulay Towards Dark Matter with DEAP at SNOLAB Mark Boulay Canada Research Chair in Particle Astrophysics Queen’s University DEAP-1:
Report from Low Background Experiments Geant4 Collaboration Workshop 10 September 2012 Dennis Wright (SLAC)
COBRA Kai Zuber University of Sussex 5 th SNOLAB Workshop,
MOON Double beta decays for neutrinos and dark matter Hiro Ejiri Osaka /JASRI /ICU I. Neutrino studies by  and  II. MOON detector and MOON 1 for.
DBD matrix elements Welcome and aim of the workshop Experimental situation Outcome.
-Nucleus Interactions Double-beta Decay and Cristina VOLPE Institut de Physique Nucléaire Orsay, France.
Physics with Neutrinos ICU Nov.12 th, 2003 Hiro Ejiri RCNO Osaka University and JASRI Spring 8.
Solotvina Underground Laboratory
The XENON Project A 1 tonne Liquid Xenon experiment for a sensitive Dark Matter Search Elena Aprile Columbia University.
XXIV WWND South Padre, TX, April 08 W. Bauer Slide 1 Double  Decays, DUSEL, and the Standard Model Wolfgang Bauer Michigan State University.
P461 - particles VIII1 Neutrino Physics Three “active” neutrino flavors (from Z width measurements). Mass limit from beta decay Probably have non-zero.
Aldo IanniNNN05 April 8, Status and future prospects of Gran Sasso Aldo Ianni INFN Gran Sasso Laboratory NNN05 Aussois, April 7-9.
 APPEAL and Neutrinos Advanced Physics with Photons Electrons And Lasers -Leptons Hiro Ejiri RCNP Osaka JASRI Spring-8, ICU July 29, 05 A view from the.
Double Beta Decay in SNO+ Huaizhang Deng University of Pennsylvania.
Nuclear matrix elements 1 / T 1/2 = PS * NME 2 * (m / m e ) 2 measured quantityquantity of interest The big unknown Started worldwide effort for a coherent.
FIRST RESULTS OF THE NEMO 3 EXPERIMENT Laurent SIMARD LAL Orsay (France) HEP-EPS 2003 conference CENBG, IN2P3-CNRS et Université de Bordeaux, France CFR,
Double beta decay and neutrino physics Osaka University M. Nomachi.
2004/Dec/12 Low Radioactivity in CANDLES T. Kishimoto Osaka Univ.
Dark Matter Search with Direction Sensitive Scintillators NOON2004 Work Shop February 14, 2004, Odaiba H. Sekiya University of Tokyo M.Minowa, Y.Shimizu,
Neutron Monitoring Detector in KIMS Jungwon Kwak Seoul National University 2003 October 25 th KPS meeting.
Neutron scattering systems for calibration of dark matter search and low-energy neutrino detectors A.Bondar, A.Buzulutskov, A.Burdakov, E.Grishnjaev, A.Dolgov,
9-June-2003NDM2003 M. Nomachi M. Nomachi OSAKA University and MOON collaboration MOON (Mo Observatory Of Neutrinos) for double beta decay Photo by
2007/9/13N. Ishihara, TAUP2007, Sendai1 DCBA DCBA experiment for searching for Neutrinoless Double Beta Decay Nobuhiro Ishihara (KEK, Tsukuba) TAUP2007.
The Recent Status of KIMS Group and New Plan Li Xin (Tsinghua University) KIMS collaboration Aug. 28th, 2006.
A Study of Background Particles for the Implementation of a Neutron Veto into SuperCDMS Johanna-Laina Fischer 1, Dr. Lauren Hsu 2 1 Physics and Space Sciences.
K. Miuchi K. Miuchi July 10, 2008 Dark Matter and Dark Energy Direction-Sensitive Dark Matter Search --NEWAGE-- Kentaro Miuchi (Kyoto University) (New.
The Tokyo Dark Matter Experiment NDM03 13 Jun. 2003, Nara Hiroyuki Sekiya University of Tokyo.
Neutrinoless double-beta decay and the SuperNEMO project. Darren Price University of Manchester 24 November, 2004.
Double Beta Decay Spectroscopy and Neutrino mass sensitivities Hiro Ejiri*, T. Shima RCNP Osaka Univ. *NIRS & CTU, Praha For the MOON collaboration Sendai.
1 GEMMA: experimental searches for neutrino magnetic moment JINR: V. Brudanin, V. Egorov, D. Medvedev, M. Shirchenko, E. Shevchik, I. Zhitnikov, V. Belov.
Double beta decays of 100 Mo and Molybdenum Observatory Of Neutrinos(MOON) Introduction Neutrino studied by 100 Mo ELEGANT V and Oto Cosmo Observatory.
Dark Matter Search with Direction Sensitive Scintillators The10th ICEPP Symposium February 16, 2004, Hakuba H. Sekiya University of Tokyo.
1 CANDLES for the study of 48 Ca double beta decay T. Kishimoto RCNP & Physics Dept. Osaka Univ.
28 May 2008NEMO-3 Neutrino081 NEMO-3 A search for double beta decay Robert L. Flack University College London On behalf of the NEMO-3 collaboration.
NEMO3 experiment: results G. Broudin-Bay LAL (CNRS/ Université Paris-Sud 11) for the NEMO collaboration Moriond EW conference La Thuile, March 2008.
Activities on double beta decay search experiments in Korea 1.Yangyang Underground laboratory 2.Double beta decay search with HPGe & CsI(Tl) 3.Metal Loaded.
Results of the NEMO-3 experiment (Summer 2009) Outline   The  decay  The NEMO-3 experiment  Measurement of the backgrounds   and  results.
Stefano Torre University College London for NEMO3 and SuperNEMO collaborations Half day IoP Meeting 12 Oct 2011 Outline 0νββ and 2νββ Observation technique.
Double Beta Decay Experiments Jeanne Wilson University of Sussex 29/06/05, RAL.
Large Format PMTs from Hamamatsu Photonics
. MOON MOON for  low E  solar ’s. Molybdenum Observatory Of Neutrinos for  low E  solar ’s. Molybdenum Observatory Of Neutrinos Hiro Ejiri.
Current status of XMASS experiment 11 th International Workshop on Low Temperature Detectors (LTD-11) Takeda Hall, University of Tokyo, JAPAN 8/1, 2005.
Solar Neutrinos By Wendi Wampler. What are Neutrinos? Neutrinos are chargeless, nearly massless particles Neutrinos are chargeless, nearly massless particles.
1 Study of 48 Ca Double Beta Decay by CANDLES T. Kishimoto Osaka Univ.
June INPC20071 Study of 48 Ca double beta decay with CANDLES OGAWA Izumi ( 小川 泉 ) Osaka Univ. ( 大阪大学 )
MOON for next-generation neutrino-less double beta decay experiment ; present status and perspective Outline of the MOON detector Background rejection.
1 Double Beta Decay of 150 Nd in the NEMO 3 Experiment Nasim Fatemi-Ghomi (On behalf of the NEMO 3 collaboration) The University of Manchester IOP HEPP.
Development of CaMoO 4 Scintillation Crystals for the 0-  decay search 1.Introduction 2.CaMoO4 Crystal R&D 3.YangYang underground laboratory for KIMS.
DPF-JPS 2006 Oct 31, Hawaii 1 CANDLES system for the study of 48-Ca double beta decay T. Kishimoto Osaka Univ.
Search for Neutrinoless Double Beta Decay with NEMO-3 Zornitza Daraktchieva University College London On behalf of the NEMO3 collaboration PANIC08, Eilat,
The NEMO3 Double Beta Decay Experiment Ruben Saakyan IoP meeting on Double Beta Decay Manchester 21 November 2007.
18-20 May 2015, Underground Science Conference, SDSM&T 1John Harton, Colorado State University Recent Results from the DRIFT Directional DM Experiment.
09/04/2006NDM061 CANDLES for the study of 48 Ca double beta decay OGAWA Izumi ( 小川 泉 ) Osaka Univ. ( 大阪大学 )
Search for Neutrinoless Double-Beta Decay Werner Tornow Duke University & Triangle Universities Nuclear Laboratory (TUNL) & Kavli-Tokyo Institute of the.
g beam test of the Liquid Xe calorimeter for the MEG experiment
Dark Matter Search With an Ultra-low Threshold Germanium Detector proposed by Tsinghua University Seoul National University Academia Sinica Qian Yue.
Double Beta Decay of 48Ca with CaF2(Eu) - ELEGANT VI -
Building ICECUBE A Neutrino Telescope at the South Pole
Dark Matter Search with Stilbene Scintillator
Institut de Physique Nucléaire Orsay, France
Search for Lepton-number Violating Processes
Welcome to Oto Cosmo Observatory
Dark Matter Detection,Models and Constraints
Presentation transcript:

1. Oto Cosmo Observatory 2. Detectors and Physics Results 3. Future Plans 4. Progress of Oto Lab. Oto Cosmo Observatory Present and Future Hiro Ejiri RCNP Osaka Univ., & JASRI Spring 8 For the ELEGANT Collaboration

RCNP Research Center for Nuclear Physics National Nuclear Physics Lab. Nucleon, Meson, and Quark Lepton Nuclear Physics. Ring Cycrotron lab GeV p, & light ions National and International users RCNP laboratory complex

RCNP & Physics Osaka Univ. Neutrinos and DM research programs. I. Oto Cosmo Observatory Underground Lab.  masses and natures by  with ELEGANT V & VI DM WIMPs search by nuclear scattering. II. Cyclotron Lab. Charge exchange spin flip reactions to study nuclear responses for charged weak currents. III. Laser Electron Photon Lab. at Spring 8. Nuclear responses for neutral weak currenta.

Osaka Univ. Oto Air port SK Oto Lab. is close to Osaka Univ. 100 km Kansai/Osaka Airport 40 km

Oto Cosmo Observatory Unused 5 km railway tunnel m we Lab.I, lab.II, lab.III New labs can be set in the center region of the 5 km tunnel. H. Ohsumi Proc. XI RCNP. Symp., World Scientific, (1996) Osaka-u.ac.jp/ Divisions/ np1-c/index.html  Lab.II Lab.I, III Nishiyoshino Oto To Osaka Lab.I. 33 m 2 ELEGANT VI  of 48 Ca and DM with CaF 2 Lab. II. 45 m 2 ELEGANT V,  of 100 Mo and DM with NaI 60 km south of Osaka, near Int. Airport

Experimental Roon I

Muon flux at underground labs. in the world  /m 2 /s Neutron /m 2 /s Rn 10 Bq/m 3 (Detector container 10 m Bq /m) Muon flux at underground labs. in the world  /m 2 /s Neutron /m 2 /s Rn 10 Bq/m 3 (Detector container 10 m Bq /m 3 ) Oto Cosmo Observatory 1400 m w.e

III. ELEGANT V ELEctron GAmma-ray Neutrino Telescope

ELEGANT V  f     Cd  -ray E&T PL  -ray by NaI DM –nucleus recoil E by NaI. H. Ejiri et al. NIM A

100 Mo 0  by ELEGANT V 100 M0 95% enriched kg. Most stringent limit by exclusive(  tracking) T  > 1.0 (0.55) y 68(90)%CL < 1.5 (2.1) eV < 9 (11) H.Ejiri, N.Kudomi, et al., Phys. Rev. C 63 ’01, 65501

Present

ELEGANT VI CaF 2 for 48 Ca  and 19 F Spin Coupled DM

ELEGANT IV CaF 2 for 48 Ca  and 19 F Spin Coupled DM CaF 2 (pure) as light guide & active shield against PMT CaF 2 (Eu) is not transparent for U.V. light.  DM signals  selected by role off ratio

Measurement of 48 Ca  at Oto 2  (sim) BG (sim) 0  window Isotope 48 Ca 76 Ge 82 Se 100 Mo 116 Cd 136 Xe 150 Nd Q-value (MeV) G 0v × (year -1 eV -2 )      y  CL   Ogawa et al., PANIC02, Nucl.Phys.2003 

ELEGANT VI CaF 2 ELEGANT VI CaF 2 19 F light mass and simple large spin matrix element I. Ogawa, et al. Nucl. Phys. 663(2000) 869c R. Hazama, NIM A482 (2002) 297

Results of ELEGANT’s Double beta decays EL III. Ge with NaI for  of 76 Ge : Limit of 1.9 eV (68% CL) on m and 1 st stringent limit on 0  to 2 + state. EL IV. 100 Mo with Si detector array and Nal. EL V. Drift chamber for  tracks, plastic scintillators for  and NaI for   st 2  lives for 100 Mo and 116 Cd.   Most stringent limits on o  100  m   eV(68% CL).  EL VI. Ca(F) 2 Crystals with CsI. Limit on 0  of 48 Ca: 7 eV  Dark matter  EL V. NaI 760 kg, annular modulation of WIMPS.  Most stringent limits at the low mass region.  EL VI. Ca(F) 2 Spin-coupled WIMPS.

V. Future Experiments A. MOON Molybdenum Observatory Of Neutrinos for  and low energy solar ’s. MOON 1 Proto - type MOON and R&D. B. CANDLES CA lcium fluoride for studies of Neutrinos and Dark Matters by Low Energy Spectrometers

V. Future Experiments I MOON. Molybdenum Observatory Of Neutrinos for  and low energy  solar and supernova ’s. MOON collaboration : Interenational collaboration RCNP/ Physics, Osaka Univ. General Arts Tokushima Univ. Phys. ICU. Tokyo, Phys. CENPA, Univ. Washington, LANL Univ. North Carolina. FNAL Phys. Charles Univ. CERN High Energy Physics, Protvino. JINR VNIIEF Contact persons Hiro Ejiri and Hamish Robertson

MOON Objectives. MOON Objectives.  studies in 100 Mo : large responses for  & low E e ’s. Double beta (  ) decays with m ~0.03 eV. Low E solar and SN e. Two charged particle (  ) spectroscopy with high localization in time & space. MOON, a super module of ~1 ton 100 Mo & scintillators with modest volume and realistic purity. H.Ejiri,, Phys, Rev. Lett.,85 (2000) 2917

MOON Hybrid Detector MOON Hybrid Detector  o film Super modules of fiber-plate scintillators with 100 Mo films. 1. Position read-out Fibers (x-y)  m - 2 mm mm 2. Energy read-out Plate scintillator with  E ~  ~ 2 % 3. Modest volume with enriched Mo 4. Enriched Mo 85 % in 100 Mo Centrifuges MoF 6 gas Laser MOON 1. Proto type 100 Mo 1 kg. M ~0.3 eV MOON 2. 1 unit : 100 Mo 0.25 ton 2m – 2m – 1.7 m, M ~0.05 eV MOON 3. 4 units: 100 Mo 1 ton. 2m – 2m -- 7 m, M ~0.02eV Fiber x

EL VI ---CANDLES 48 Ca for  large Q   4.27 MeV, small 0.19% 48 Ca 7.7 g (EL VI) to O(10kg) & Enrichment  of 1  l crystals of CaF 2 in iiquid scintillator 3.1 kg of 48 Ca in 3.2 ton n CaF 2 Goal 0.1 eV sensitivity. R & D Osaka Univ.Physics. Future Experiments Future Experiments II CANDLES

VII. Progress & Grants I. ELEGANTs at Kamoka Start  and project at Osaka ELEGANT I, II, Ge with NaI at Osaka 1982 –1984 ELEGANT III. Ge wih NaI Grant A. B 1982 – 1985 ELEGANT IV. Mo with Si. Toray Science Award 1984 EL III Starts at Kamioka Grant A – 1990 ELEGANT V Mo Cd Drift Chamber & NaI Grant Special Project 1990 – EL V Starts run – 1995 EL VI CaF 2 with CsI Construction Grant Basic Research

Oto Underground Lab New underground lab. & DM project start – 1995 survey of new underground lab Select Oto and proposal Start construction Grant COE lab Commencement of Oto Lab. Improve EL V and set at Oto EL V starts run at Oto 1999 EL IV starts run at Oto MOON 2000 MOON project, MOON R&D Yamada award 2001, 2003 MOON 1 Proto-type Government Grant A. CANDLES 2002 R&D and Government Grant A.

References Nuclear responses for neutrinos. Review H.Ejiri, Phys. Rep. 338 (2000) 265. GR and , solar & sn ’s  H.Ejiri, Nucl. Phys. A 687 (2001) 350c LI reactions. 3 He H.Ejiri, et al. PLB 433 (1998) B, 11 Li H. Ejiri, K. Takahisa, et al., 1997, Double beta decays and neutrinos.  L V  H.Ejiri, N.Kudomi, et al., Phys. Rev. C 63 (2001) Review H.Ejiri, Nucl. Phys.B 91 (2001) 255, v2000 proc MOON  and solar  H.Ejiri, J.Engel, G.Hazama, P.Krastev, N.Kudomi, R.G.H.Robertson, Phys, Rev. Lett.,85 (2000) 2917 Supernova  H.Ejiri, J.Engel, N.Kudomi, PL B530 (2002) 27

We would express our cordial thanks to Oto & Nishiyoshino villages & the chiefs, Mr T. Kitamura & Mr S . Nakagaki, for the great and timely support for construction of the new lab. National Railway Corporation for transfer of the tunnel to the two villages to be used for our underground lab. Japanese people for their great contributions. Toray, Takeda, and Yamada S.F.for their timely awards/suports.

Thank you for attension.

Here we would like to express our cordial thanks to The distinguished chief of Oto, Mr. Toshihiro. Kitamura for great, timely, & crucial supports for our science projects.