M. Dracos 1 Double Beta experiment with emulsions?

Slides:



Advertisements
Similar presentations
NEMO-III Status and prospects. 12 December 2005 HEP group Christmas meeting Vladimir Vasiliev.
Advertisements

SuperNEMO Thoughts about next generation NEMO experiment Ruben Saakyan UCL.
Double Beta Decay review
New results from the CHORUS Neutrino Oscillation Experiment Pasquale Migliozzi CERN XXIX International Conference on High Energy Physics UBC, Vancouver,
 NEMO-3 Detector  Preliminary results Performance of the detector  analysis for 100 Mo, 82 Se and 150 Nd  Background study for  research ( 208.
Neutrino Mass and Mixing David Sinclair Carleton University PIC2004.
OPERA experiment T.Toshito (Nagoya univ. Japan) for the OPERA collaboration Apr
Kouji Narita Nagoya University, Japan CHORUS collaboration Study of charm production in neutrino interactions.
NEMO-3 Experiment Neutrino Ettore Majorana Observatory
Comments on OPERA OPERA is going on. We will have good Tau neutrino interactions within years, if νμ - ντ oscillation is the real solution. New Techniques.
The SuperNEMO experiment A very low background experiment Jérémy ARGYRIADES, LAL Orsay.
Status of the OPERA experiment Yoshiaki Nonoyama Nagoya Univ.
M. Dracos, CEA, 10/04/ Double Beta experiment with emulsions?
Double Beta Decay Present and Future
First results from NEMO 3 Experiment V. Vasiliev (ITEP), H. Ohsumi (Saga) and Ch. Marquet Nara, Japan, June 2003 NEMO collaboration.
NEMO-3  experiment First Results and Future Prospects Ruben Saakyan, UCL UK HEP Neutrino Forum The Cosener’s House, Abingdon.
Warsaw - NEMO initiative group Zenon Janas for Search for neutrinoless double  decay in NEMO-3 and SuperNEMO experiments Warszawa,
NEMO-3 Double Beta Decay Experiment: Last Results A.S. Barabash ITEP, Moscow (On behalf of the NEMO Collaboration)
Status of R&D of the SuperNEMO experiment Gwénaëlle Broudin-Bay LAL Orsay GDR neutrino – Bordeaux – Oct
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,
SuperNEMO Simulations Darren Price University of Manchester July, 2005.
A screening facility for next generation low-background experiments Tom Shutt Laura Cadonati Princeton University.
Recent Results of the NEMO 3 Experiment Ladislav VÁLA Czech Technical University in Prague NOW2006, 9 th – 16 th September 2006, Conca Specchiulla, Italy.
Double beta decay and neutrino physics Osaka University M. Nomachi.
OPERA Experiment, Brick Finding Program A. Chukanov Joint Institute for Nuclear Research ISU, 12 th February, 2007.
Operation of and results from OPERA Ciro Pistillo LHEP Bern University CHIPP Plenary meeting Lausanne, EPFL-LPHE September
Neutrino Ettore Majorana Observatory
9-June-2003NDM2003 M. Nomachi M. Nomachi OSAKA University and MOON collaboration MOON (Mo Observatory Of Neutrinos) for double beta decay Photo by
OMC rates in Sm and Kr for 2  -decay V.G. Egorov, A.V. Klinskih, R.V. Vasiliev, M.V.Shirchenko, D.R. Zinatulina MEDEX’07 MEDEX’07.
Start Counter Collaboration Meeting September 2004 W. Boeglin FIU.
Development of metal-loaded liquid scintillators for the double beta decay experiment 연세대 : 황명진, 권영준 서울대 : 곽정원, 김상열, 김선기, 김승천, 김태연, 명성숙, 방형찬, 이명재, 이직,
Nuclear Track Emulsion Workshop Romania Nuclear emulsion with molybdenum filling for 2  -decay observation V.D.Ashitkov, A.S.Barabash, V.J.Bradnova,
Neutrinoless double-beta decay and the SuperNEMO project. Darren Price University of Manchester 24 November, 2004.
VIeme rencontres du Vietnam
Tracking (wire chamber) Shield radon, neutron,  Source foil (40 mg/cm 2 ) Scintillator + PMT 2 modules 2  3 m 2 → 12 m 2 Background < 1 event / month.
IOP HEPP Matthew Kauer Double beta decay of Zr96 using NEMO- 3 and calorimeter R&D for SuperNEMO IOP HEPP April Matthew Kauer UCL London.
NEMO3 analysis and SuperNEMO development Benjamin Richards D14.
1 NuFact’01 WG1 : Neutrino Oscillation Physics May 24-30, 2001 An appearance experiment to search for  -  oscillations in the CNGS beam CNGS1 O scillation.
Telescope Germanium Vertical Telescope Germanium Vertical JINR Dubna, Russia CSNSM Orsay, France CTU Prague, Czech Republic RRC - Kurchatov Institute Moscow,
DOUBLE BETA DECAY TO THE EXCITED STATES (EXPERIMENTAL REVIEW) A.S. BARABASH ITEP, MOSCOW.
Neutrino Ettore Majorana Observatory
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.
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.
1st Year Talk1 PEP Violation Analysis with NEMO3 and Calorimeter R&D for SuperNEMO Anastasia Freshville.
By Matthew Kauer First Year Report – 15 June 07 Measurement of 2b2ν Half-Life of Zr96 and Lightguide Studies for SuperNEMO Calorimeter Matthew Kauer UCL.
A screening facility for next generation low-background experiments Tom Shutt Case Western Reserve University.
OPERA Experiment, Brick Finding Program A. Chukanov Joint Institute for Nuclear Research Dubna, 25 th January, 2007.
BENE MECC detector Pasquale Migliozzi INFN – Napoli.
Proposal to join NEMO-3  decay experiment P. Adamson, R. Saakyan, J. Thomas UCL 27 January 2003.
Second Workshop on large TPC for low energy rare event detection, Paris, December 21 st, 2004.
Nasim Fatemi-Ghomi, Group Christmass Meeting December Nasim Fatemi-Ghomi Double Beta Decay Study of 150 Nd at NEMO3 (The magic isotope!!)
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.
Scintillating Bolometers – Rejection of background due to standard two-neutrino double beta decay D.M. Chernyak 1,2, F.A. Danevich 2, A. Giuliani 1, M.
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.
Neutrinoless double beta decay (0  ) CdTe Semico nductor Band gap (eV) Electron mobility (cm 2 /V/s) Hole mobility (cm 2 /V/s) Density (g/cm 3.
V. Egorov. JINR + LSM V. Egorov = The love story 1991 Orsay S.Jullian and D.Lalanne proposed to bring our 2β-spectrometer to Modane 1993 TGV.
Yuri Shitov Imperial College London On behalf of the NEMO Collaboration A search for neutrinoless double beta decay: from NEMO-3 to SuperNEMO Moriond EW.
Search for Neutrinoless Double-Beta Decay Werner Tornow Duke University & Triangle Universities Nuclear Laboratory (TUNL) & Kavli-Tokyo Institute of the.
Double Beta experiment using nuclear emulsions?
Status of 100Mo based DBD experiment
Status of the OPERA experiment
Preliminary Study of 214Bi Background in 100Mo foils
• • • Ge measurements for SuperNEMO
The 0-neutrino double beta decay search
Double Beta experiment using nuclear emulsions?
Double Beta experiment with emulsions?
Presentation transcript:

M. Dracos 1 Double Beta experiment with emulsions?

M. Dracos 2 Double Beta Decay ? T 1/2 ~ years ! Observed for: Mo 100, Ge 76, Se 82, Cd 116, Te 130, Zr 96, Ca 48, Nd 150 allowed double beta double beta without neutrino Isotope Q   (keV) 116 Cd  116 Sn  Se  82 Kr  Mo  100 Ru  Zr  96 Mo  Nd  150 Sm  Ca  48 Ti  4.1 The NEMO3 experiment

M. Dracos 3 The NEMO3 detector Sources : 10 kg, 20 m 2 wire chamber (Geiger) 3m energy and time of flight measurements plastic scintillator blocks 2 electron tracks + photomultipliers (Hamamatsu 3", 5") expected sensitivity up to m ~0.3 eV

M. Dracos 4 Event Examples

M. Dracos 5Results 932 g 389 days 2750 even. S/B = 4 82 Se 82 Se T 1/2 = 9.6  0.3 (stat)  1.0 (syst)  y 116 Cd T 1/2 = 2.8  0.1 (stat)  0.3 (syst)  y 150 Nd T 1/2 = 9.7  0.7 (stat)  1.0 (syst)  y 96 Zr T 1/2 = 2.0  0.3 (stat)  0.2 (syst)  y 48 Ca T 1/2 = 3.9  0.7 (stat)  0.6 (syst)  y 48 Ca background subtracted Phase I + II 693 days T 1/2 (  ) > (90 % C.L.)  < eV Expected in 2009 T 1/2 (  ) > (90 % C.L.)  < eV 100 Mo ( 7 kg )

M. Dracos 6 Super NEMO Improvements: –Energy resolution 15%   E/E = 3 MeV –Efficiency 15%  MeV –Source x10 larger 7kg  kg Most promising isotopes – 82 Se (baseline) or perhaps – 150 Nd Aim: T 1/2 > 2 x y   M   < meV R&D up to 2009, construction between 2010 and 2013 source sheet

M. Dracos 7 e e 2  with emulsions "veto" emulsion, if needed (~50  m like in OPERA?) plastic base "2  " emulsion thick enough to detect up to 4 MeV electrons (density?) beta source (~50  m inNEMO could be less for emulsions) 1 MeV e- 2 MeV e- (Akitaka Ariga)

M. Dracos 8 2  with emulsions NEMO3 surface: 20 m 2 Super-NEMO surface: 10x20 m 2 To cover the same isotope source surface with emulsions (both sides to detect the 2 electrons) we need an emulsion surface: 2x200=400 m 2. Just for comparison, one OPERA emulsion has about m 2 and one brick m 2. So 400 m 2 is about the equivalent of 600 OPERA bricks (but not with the same thickness of course…). Use the same envelops like the OPERA changeable sheets by introducing at the middle of the two emulsions a double beta source sheet, or use longer emulsion sheets easier to handle by microscopes. Keep all these envelops for some time (e.g months depending on fading) in the experiment and after this period start scanning them one after the other. They could be replaced by new envelops during 5 years in order to accumulate something equivalent to what Super-NEMO could do:  400*5 year*m 2

M. Dracos cm 2 / h TS(1994)NTS(1996)UTS(1998)SUTS(2006)SUTS(2007-) Scanning Power Roadmap 1stage facility CHORUSDONUTOPERA 2  with emulsions How much time is needed to make a full scan of 2000 m 2 (is a full scan in all volume really needed?)? If the Japanese S-UTS scanning system is used with a speed of 50 cm 2 /hour (be careful with thickness…), for one scanning table: 25 m 2 /year (200 working days/year). By using 16 tables and extracting 100 m 2 /3 months (1 year exposure at the beginning and putting back new emulsions with the same isotopes), this finally will take less than 5 years (as Super-NEMO). Probably the emulsion thickness needed to detect these electrons will need more scanning time and the speed would be significantly less than 50 cm 2 /h. On the other hand, scanning speed increases with time… Nakamura san Nufact07

M. Dracos 10 Pending questions Energy resolution for NEMO: 15% for 3 MeV electrons Required for Super-NEMO: lower than 7% (goal 4%) Emulsion experiment resolution: ??? (monoenergetic 1 MeV 207 Bi electrons could be used to have a good estimate of this resolution) Reconstruction efficiency for NEMO: 15% Required for Super-NEMO: 40% Emulsion experiment efficiency: ?? Afforded background? Could magnetic field help? Possibility to take thinner isotope sheets (60 mm for NEMO3) and have better energy resolution (but also more scanning for the same isotope mass).

M. Dracos 11 Extra Ideas e e decreasing density (25 mm layers) to minimize the emulsion thickness e e emitter in powder better vertex and energy reconstruction ?

M. Dracos 12 END

M. Dracos 13 2  with emulsions for 400 m 2 /year and 400 m 2 isotopes available isotope block number time (years)surface (m 2 )exposure time (years) surface*time (m 2 *years) total