Comments on Neutrinoless Double Beta Decay Experiments

Slides:



Advertisements
Similar presentations
Cuoricino results for 2 decay to the first excited state 0 + Sergio Di Domizio for the Cuoricino Collaboration Università and INFN Genova Athens, June.
Advertisements

Results from CUORICINO and Prospects for CUORE (Cryogenic Underground Observatory for Rare Events) S. Cebrián, on behalf of the CUORE Collaboration Università
IS THE NEUTRINO A MAJORANA OR A DIRAC PARTICLE ? Ettore Fiorini, Bologna June or Lepton number conservation or violation Has neutrino a finite.
Proposal to join NEMO-3  decay experiment P. Adamson, R. Saakyan, J. Thomas UCL 27 January 2003.
Neutrinoless Double Beta Decay
Claudia Nones Physics of Massive Neutrinos - Blaubeuren, July 1 - 5, 2007 Status of Cuoricino and CUORE with some remarks on nuclear matrix elements Centre.
Recent Discoveries in Neutrino Physics: Understanding Neutrino Oscillations 2-3 neutrino detectors with variable baseline 1500 ft nuclear reactor Determining.
March 12, 2005Benasque Neutrinos Theory Neutrinos Theory Carlos Pena Garay IAS, Princeton ~
Double Beta Decay L=2 2: (A,Z)  (A,Z+2) + 2e- + 2ne
 decay and neutrino mass 35 isotopes in nature …and Mixing Neutrino Mass.. Imperial College/RAL Nottingham Nov 17 ’04 Dave Wark.
Experimental status of the Double Beta Decay Marisa Pedretti INFN Milano Bicocca.
GERDA: GERmanium Detector Array
Neutrino Mass and Mixing David Sinclair Carleton University PIC2004.
Determining the neutrino mass:
Charles Prescott - SLAC Neutrino Day - April 18, 2003 The Search for Neutrinoless Double Beta Decay - Physics Motivations - Limits from ν oscillations.
DBD matrix elements Welcome and aim of the workshop Experimental situation Outcome.
From CUORICINO to CUORE: To probe the inverted hierarchy region On behalf of the CUORE collaboration DUSL Meeting, Washington DC November 2,-4, 2007 Frank.
Daniel Lenz, University of Wisconsin, Madison 11/05/ APS DNP Cryogenic search for neutrinoless double beta decay Daniel Lenz on behalf of the CUORE.
No s is good s Sheffield Physoc 21/04/2005 Jeanne Wilson A historical introduction to neutrinoless double beta decay.
Daniele Pergolesi, Institut d’Astrophysique de Paris, Nov 14 th The MARE experiment on direct measurement of neutrino mass Daniele Pergolesi UNIVERSITY.
LNGS Capelli Silvia on behalf of CUORE Collaboration
Stefano Pirro LRT-2004 Sudbury December 13, 2004 Cleanliness backgrounds and surface contaminations in Cuore Stefano Pirro INFN-Milano.
Double beta decay Ruben Saakyan UCL 25 March 2004.
Double Beta Decay Present and Future
CUORE Cryogenic Underground Observatory for Rare Events
CUORICINO and CUORE Chiara Brofferio Università di Milano – Bicocca and INFN, Sez. di Milano NOW 2004 – Otranto 12 – 17 September 2004 On behalf of the.
First neutrinoless double beta decay results from CUORE-0
NEMO-3  experiment First Results and Future Prospects Ruben Saakyan, UCL UK HEP Neutrino Forum The Cosener’s House, Abingdon.
Massive neutrinos Dirac vs. Majorana
LUCIFER a potentially background-free approach to the search for 0  Claudia Nones CSNSM/CNRS-Orsay NOW2010 – September 4 th - 11 th, 2010 – Conca Specchiulla,
From Cuoricino to CUORE: towards the inverted hierarchy region Andrea Giuliani On behalf of the CUORE collaboration University of Insubria (Como) and INFN.
Double beta decay search with TeO 2 bolometers Andrea Giuliani on behalf of the CUORE collaboration University of Insubria (Como) and INFN Milano-Bicocca.
Stefano Pirro, IDEA Meeting -Zaragoza November 7, Nd Project High Temperature Thermistors News about NdGaO 3 Scintillating Bolometers Conclusions.
Andrea Giuliani University of Insubria (Como) and INFN Milano-Bicocca Italy Searches for Neutrinoless Double Beta Decay Epiphany Conference Krakow 6 th.
THE CUORE EXPERIMENT: A SEARCH FOR NEUTRINOLESS DOUBLE BETA DECAY Marco Andrea Carrettoni on behalf of the CUORE collaboration 2 nd International Conference.
Underground Crystal Growth Marisa Pedretti. Participants INFN (ITALY) LNGS Como Milano-Bicocca Contractor Lawrence Berkeley National Laboratory University.
Present status of CUORE / CUORICINO Andrea Giuliani Università dell’Insubria and INFN Milano 3rd IDEA meeting, Orsay, April 14 – 15, 2005.
Status of Surface Sensitive Bolometers University of Insubria – Como, Italy INFN – Milano, Italy Prague, Chiara Salvioni.
The CUORE experiment Thomas Bloxham Lawrence Berkeley National Lab PHENO 2011 May 9th 2011.
New era of neutrino physics 1.Atmospheric neutrino oscillations (in particular zenith angle dependence of the muon neutrino flux) 2. Solar neutrino deficit.
NWG 4/11/03 Executive Summary R.N. Cahn, W.C. Carithers, S.J. Freedman, K.M. Heeger, R.W. Kadel, V. Koch, K.T. Lesko, Z. Ligeti (deputy), K-B. Luk, H.
M. Wójcik for the GERDA Collaboration Institute of Physics, Jagellonian University Epiphany 2006, Kraków, Poland, 6-7 January 2006.
Neutrinoless double-beta decay and the SuperNEMO project. Darren Price University of Manchester 24 November, 2004.
Searches on neutrino physics with cryogenic detectors Ettore Fiorini, Columbia, May 16, 2008 The birth of the neutrino.
Production of Neutron Transmutation Doped Germanium Thermistors for CUORE Reina Maryama for the CUORE Collaboration University of Wisconsin, Madison APS.
M. Wójcik Instytut Fizyki, Uniwersytet Jagielloński Instytut Fizyki Doświadczalnej, Uniwersytet Warszawski Warszawa, 10 Marca 2006.
Reactor neutrinos, double beta and beta decays Experimental review Fabrice Piquemal Laboratoire Souterrain de Modane (CNRS/IN2P3 and CEA/IRFU) and Centre.
Stefano Pirro – NuMass 2010 Stefano Pirro Double beta decay searches with enriched and scintillating bolometers - Milano - Bicocca The Future of Neutrino.
May 19, 2005UAM-IFT, Madrid : Neutrino physics in underground labs Carlos Pena Garay IAS ~
NEMO3 experiment: results G. Broudin-Bay LAL (CNRS/ Université Paris-Sud 11) for the NEMO collaboration Moriond EW conference La Thuile, March 2008.
Double Beta Decay Experiments Jeanne Wilson University of Sussex 29/06/05, RAL.
Claudia Nones CEA/IRFU/SPP GDR Neutrino Meeting – Saclay – 4/11/15 The bolometric way towards the inverted hierarchy of the neutrino mass: CUORE-0 → CUORE.
Phase I: Use available 76 Ge diodes from Heidelberg- Moscow and IGEX experiments (~18 kg). Scrutinize with high siginificance current evidence. Phase II:
DOUBLE BETA DECAY EXPERIMENTS Yeongduk Kim Sejong University 2 nd Amore Meeting
From CUORICINO to CUORE The bolometric way to double beta decay on behalf of the CUORE collaboration PANIC08 EILAT November 2008 Maria Martinez INFN Milano-Bicocca.
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,
Neutrino physics: The future Gabriela Barenboim TAU04.
Double beta decay and Leptogenesis International workshop on double beta decay searches Oct SNU Sin Kyu Kang (Seoul National University of.
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.
ArchPbMoO4 scintillating bolometers as detectors to search for neutrinoless double beta decay of 100Mo Serge Nagorny INFN – Gran Sasso Science Institute,
The CUORE experiment Marisa Pedretti INFN Milano Bicocca.
The search for neutrinoless double beta decay with Cuoricino and Cuore
From Cuoricino to CUORE: approaching the inverted hierarchy region
Serge Nagorny – GSSI-INFN
Double beta decay and Majorana neutrinos
Huan Zhong Huang (黄焕中) Department of Physics and Astronomy
for the CUPID-0 collaboration
Search for Lepton-number Violating Processes
Presentation transcript:

Comments on Neutrinoless Double Beta Decay Experiments Huan Zhong Huang (黄焕中) Department of Physics and Astronomy University of California, Los Angeles 90095 huang@physics.ucla.edu OCPA Underground Sciences Workshop Hong Kong, July 21-23 2008 Thanks to F. Avignone, S.J. Freedman, E. Fiorini, R. Maruyama

Neutrino Physics Program Critical Questions for Future Neutrino Physics Program 1) Are neutrinos their own anti-particles? Dirac or Majorana neutrinos 2) What are the scale of neutrino masses and the hierarchy of the neutrino mass ordering? 3) What is the remaining neutrino mixing angle q13? 4) Do neutrinos violate the CP symmetry and contribute to the matter-antimatter asymmetry?

Massive Neutrinos: Majorana or Dirac? Lorentz Invariance: massive particle velocity < speed of light c spin Left-handed nLH Momentum (Lab) Right-handed nRH (Speed-of-light Frame) Majorana Neutrino Neutrino=anti-neutrino Dirac Neutrino Neutrino and anti-neut distinct Boost Boost nLH nRH nLH nRH CPT CPT CPT

Double Beta Decay (A,Z+1) 2 (A,Z) bb (A,Z+2) e– 1935 Even-even nucleus 2 2nbb: T1/2 ≥ 1018y e– (A,Z) (A,Z+2) W 1935 M. Goeppert-Mayer (A,Z)  (A,Z+2) + 2e– + 2ne

Dirac or Majorana Neutrinos? 0 1937 n e e– (A,Z) (A,Z+2) W (A,Z)  (A,Z+2) + 2e– 0nbb: T1/2 ≥ 1025y Majorana  neutrino = anti-neutrino Lepton Number violation !

Measuring Neutrino Masses Direct Measurement tritium decays E0 = 18.6 keV <mb> = 2) Effective Majorana Mass <mbb> = ei – CP phase for neutrinos 3) Precise Cosmological Measurement <mS> =

The actual range of mbb depends on the NME ! There is no clear issue identified regarding the experimental data.

The Cuoricino experiment 62 TeO2 bolometers Total detector mass: M ~ 11 kg 130Te ~ 5x1025 130Te nuclides Deep underground in the Gran Sasso Laboratory (Italy) (3500 m.w.e.) Started in 2003, currently the largest operated bolometric experiment

Cuoricino Results Neither Support Nor Rule Out Heidelberg-Moscow Claim Background in bb region 0.18  0.01 c/keV/kg/y Average resolution @ 2615keV ~ 8keV PRELIMINARY Updated Aug 2007 Tot exposure = 15.53 kg y 130Te bb0n 60Co Results for 0nbb half life and Majorana mass (90% c.l.): T1/20n (130Te) > 3.1 x 1024 y mbb < 200 - 680 meV (*) (*) using NME from Rodin et al, Nucl. Phys. A 776 (2006) and erratum arXiv::nucl-th/0706.4304 Cuoricino demonstrates the feasibility of a large scale bolometric detector with good energy resolution Background reduction is being worked on for scaled up CUORE

The Constraint from Cosmology Competitive Model Dependent ! G.L. Fogli et al, hep-ph/0805.2517 Cosmological Data Set S (at 2s) CMB < 1.19 eV CMB+HST+SN-Ia < 0.75 eV CMB+HST+SN-Ia+BAO < 0.60 eV CMB+HST+SN-Ia+BAO+Lya < 0.19 eV CMB – WMAP 5-year, ACBAR, VSA, CBI, BOOMERANG HST – Hubble Space Telescope h=0.75+-0.07 SN-Ia – SNLA (The SuperNova Legacy Survey) BAO – Baryonic Acoustic Oscillation (WMAP) Lya – Small Scale Primordial Spec from Lyman-a forest coulds

Candidate for Double beta Decays Q (MeV) Abund.(%) 48Ca48Ti 4.271 0.187 76Ge76Se 2.040 7.8 82Se82Kr 2.995 9.2 96Zr96Mo 3.350 2.8 100Mo100Ru 3.034 9.6 110Pd110Cd 2.013 11.8 116Cd116Sn 2.802 7.5 124Sn124Te 2.228 5.64 130Te130Xe 2.533 34.5 136Xe136Ba 2.479 8.9 150Nd150Sm 3.367 5.6

Major 0nbb Experiments (scalable to ~1 ton now or planned) -- CUORE 130Te -- MAJORANA/GERDA 76Ge -- EXO 136Xe Essential to Measure 0nbb for Several Elements !!

Underground National Laboratory US-Italy Collaboration CUORE @ LNGS CUORE R&D (Hall C) Underground National Laboratory of Gran Sasso L'Aquila – ITALY 3500 m.w.e. CUORICINO - CUORE (Hall A)

19 CUORICINO-like towers with 13 planes of 4 crystals each CUORE CUORE: Cryogenic Underground Observatory for Rare Events will be a tightly packed array of 988 Bolometers - M ~ 200 kg of 130Te 80 cm 19 CUORICINO-like towers with 13 planes of 4 crystals each Operated at Gran Sasso laboratory Special cryostat built w/ selected materials Cryogen-free dilution refrigerator Shielded by several lead shields

Bolometer TeO2 Bolometer: Source = Detector Heat sink: ~8-10 mK Thermal coupling: Teflon Thermometer: NTD Ge thermistor Absorber: TeO2 crystal TeO2 Bolometer: Source = Detector

Signal from NTD Ge Thermistor

Energy resolution of a TeO2 crystal of 5x5x5 cm3 (~ 760 g ) Energy [keV] Counts 210Po a line 0.8 keV FWHM @ 46 keV 1.4 keV FWHM @ 0.351 MeV 2.1 keV FWHM @ 0.911 MeV 2.6 keV FWHM @ 2.615 MeV 3.2 keV FWHM @ 5.407 MeV the best a spectrometer so far

Scaling CUORE from CUORICINO

Background Reduction is the Key CUORICINO – Surface Related Background CUORE -- Crystal Production -- TeO2 Material QA for Crystal Production -- Crystal Processing QA -- Improved Surface Cleaning Procedure Crystal Support Structure (Cu) -- New/Improved Surface Cleaning Procedure Note – CUORICINO/CUORE Has Excellent Shielding (Roman Lead)

Expected Sensitivity of the CUORE Experiment APS Neutrino Study 2004

General Comments CUORE-- 130Te -- Excellent Energy Resolution (FWHM 0.3%) -- Cost Effective -- Background Elimination Challenging -- Data-Taking Early 2011 GERDA/MAJORANA -- 76Ge -- Ultra-Low Background Possible -- Detector Segmentation and Pulse Shape Analysis Possible -- Very Costly ! EXO -- 136Xe -- Easy to Scale Up -- Ba+ Tagging Challenging / FWHM ~3.4%

Interdisciplinary Sciences Three Overarching Themes -- APS multidivisional neutrino study Neutrino Matrix – physics/0411216 Neutrinos and the New Paradigm -- neutrino masses, Dirac/Majorana and CP violation beyond the Standard Model 2) Neutrinos and the Unexpected -- Many discoveries in recent years, what surprises and extraordinary properties ahead? 3) Neutrinos and Cosmos -- # of neutrinos, neutrino masses – large structures CP violation – matter/anti-matter asymmetry

CUORE Collaboration Universita’ di Milano-Bicocca5 C. Arnaboldi, C. Brofferio, S. Capelli, M. Carrettoni, M. Clemenza, E. Fiorini, S. Kraft, C. Maiano, C. Nones, A. Nucciotti, M. Pavan, D. Schaeffer, M. Sisti, L. Zanotti Sezione di Milano dell’INFN F. Alessandria, L. Carbone, O. Cremonesi, L. Gironi, G. Pessina, S. Pirro, E. Previtali Politecnico di Milano R. Ardito, G. Maier Laboratori Nazionali del Gran Sasso M. Balata, C. Bucci, P. Gorla, S. Nisi, E. L. Tatananni, C. Tomei, C. Zarra Universita’ di Firenze and Sezione di Firenze dell’INFN M. Barucci, L. Risegari, G. Ventura Universita’ dell’Insubria5 E. Andreotti, L. Foggetta, A. Giuliani, M. Pedretti, C. Salvioni Universita di Genova S. Didomizio6, A. Giachero7, P. Ottonello6, M. Pallavicini6 Laboratori Nazionali di Legnaro G. Keppel, P. Menegatti, V. Palmieri, V. Rampazzo Universita di Roma La Sapienza and Sezione di Roma dell’INFN F. Bellini, C. Cosmelli, I. Dafinei, R. Faccini, F. Ferroni, C. Gargiulo, E. Longo, S. Morganti, M. Olcese, M. Vignati Universita’ di Bologna and Sezione di Bologna dell’INFN M. M. Deninno, N. Moggi, F. Rimondi, S. Zucchelli University of Zaragoza M. Martinez Kammerling Onnes Laboratory, Leiden University A. de Waard, G. Frossati Shanghai Institute of Applied Physics (Chinese Academy of Sciences) X. Cai, D. Fang, Y. Ma, W. Tian, H. Wang 5also Sezione di Milano dell’INFN 6also Sezione di Genova dell’INFN 7also LNGS University of California at Berkeley A. Bryant2, M.P. Decowski2 , M.J. Dolinski3 , S.J. Freedman2, E.E. Haller2, L. Kogler2, Yu.G. Kolomensky2 University of South Carolina F.T. Avignone III, I. Bandac, R. J. Creswick, H.A. Farach, C. Martinez, L. Mizouni, C. Rosenfeld Lawrence Berkeley National Laboratory J. Beeman, E. Guardincerri, R.W. Kadel, A.R. Smith, N. Xu Lawrence Livermore National Laboratory K. Kazkaz, E.B. Norman4, N. Scielzo University of California, Los Angeles H. Z. Huang, S. Trentalange, C. Whitten Jr. University of Wisconsin, Madison L.M. Ejzak, K.M. Heeger, R.H. Maruyama, S. Sangiorgio California Polytechnic State University T.D. Gutierrez 2also LBNL 3also LLNL 4also UC Berkeley

Full estimated range of M0n within QRPA framework and comparison with NSM (higher order currents now included in NSM) – P. Vogel

Double Beta Decay Candidates Normal beta-decay is energetically forbidden, while double beta-decay from (A,Z)  (A, Z+2) is energetically allowed: (A=even, Z=even) A, Z+1 A, Z+3 0+ A, Z bb 0+ A, Z+2 Some candidates: 48Ca, 70Zn, 76Ge, 80Se, 86Kr, 96Zr, 100Mo, 116Cd, 130Te, 136Xe, 150Nd

CUORE Array of 988 TeO2 crystals 19 Cuoricino-like “towers” 13 levels, 4 crystals each 5x5x5 cm3 (750 g each) Low conductance Teflon insulators OFHC Cu structure Crystals equipped with NTDs Suspended from cold stage Mechanically isolated OGHC-Oxygen Free High Conductivity NTD-Neutron Transmutation Doped

Neutrino Masses and Hierarchy Normal Inverted

Cosmogenic Co from Te