ANTI-NEUTRINOS- DIRAC OR MAJORANA

Slides:



Advertisements
Similar presentations
IS THE NEUTRINO A MAJORANA OR A DIRAC PARTICLE ? Ettore Fiorini, Bologna June or Lepton number conservation or violation Has neutrino a finite.
Advertisements

Proposal to join NEMO-3  decay experiment P. Adamson, R. Saakyan, J. Thomas UCL 27 January 2003.
Claudia Nones Physics of Massive Neutrinos - Blaubeuren, July 1 - 5, 2007 Status of Cuoricino and CUORE with some remarks on nuclear matrix elements Centre.
Double Beta Decay review
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.
COBRA Kai Zuber University of Sussex 5 th SNOLAB Workshop,
Experimental status of the Double Beta Decay Marisa Pedretti INFN Milano Bicocca.
Double Beta Decay review
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.
LNGS Capelli Silvia on behalf of CUORE Collaboration
Contents Lecture 1 General introduction What is measured in DBD ? Neutrino oscillations and DBD Other BSM physics and DBD Nuclear matrix elements Lecture.
Double beta decay Ruben Saakyan UCL 25 March 2004.
Double Beta Decay Present and Future
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.
Warsaw - NEMO initiative group Zenon Janas for Search for neutrinoless double  decay in NEMO-3 and SuperNEMO experiments Warszawa,
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.
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.
Present status of CUORE / CUORICINO Andrea Giuliani Università dell’Insubria and INFN Milano 3rd IDEA meeting, Orsay, April 14 – 15, 2005.
Operation of bare Ge-diodes in LN/LAr 1 st IDEA meeting Como, April 8 (2004) Stefan Schoenert.
The CUORE experiment Thomas Bloxham Lawrence Berkeley National Lab PHENO 2011 May 9th 2011.
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.
VIeme rencontres du Vietnam
M. Wójcik Instytut Fizyki, Uniwersytet Jagielloński Instytut Fizyki Doświadczalnej, Uniwersytet Warszawski Warszawa, 10 Marca 2006.
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.
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.
BACKGROUND REJECTION AND SENSITIVITY FOR NEW GENERATION Ge DETECTORS EXPERIMENTS. Héctor Gómez Maluenda University of Zaragoza (SPAIN)
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.
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.
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.
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.
1 DOUBLE BETA DECAY Double beta decay at the borderline between nuclear and subnuclear physics (no border in my opinion) Nucleus acting as a microlaboratory.
1 Study of 48 Ca Double Beta Decay by CANDLES T. Kishimoto Osaka Univ.
Proposal to join NEMO-3  decay experiment P. Adamson, R. Saakyan, J. Thomas UCL 27 January 2003.
M.Altmann, GERDA Status Report SNOLAB Workshop IV, Investigating Neutrinoless Double Beta Decay Status of the GERDA Experiment Michael Altmann.
Double Beta Decay - status and future Double beta decay basics Double beta decay basics Experimental challenges Experimental challenges Current experimental.
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
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.
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.
0νDBD Experimental Review and 136 Xe With HP Gas at CJPL 季向 东.
Probing neutrinos with  decay Ruben Saakyan UCLSwansea 31 January January 2006.
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 COBRA Experiment: Future Prospects
Experiments on Neutrino Nature and Mass
The search for neutrinoless double beta decay with Cuoricino and Cuore
Double Beta Decay - status and future
From Cuoricino to CUORE: approaching the inverted hierarchy region
Status and perspectives for Double Beta Decay measurements
Double beta decay and Majorana neutrinos
Presentation transcript:

ANTI-NEUTRINOS- DIRAC OR MAJORANA Ettore Fiorini, Venice February 10, 2006 n=n- or n  n- Lepton number conservation or violation Has neutrino a finite mass 100 % chirality n n-    

The Standard Model ne nm ne nt ne (n-e ) nm (n-m) nt(n-t) Flavor conservation or violation Neutrino oscillations need Dm2  0  ne nm ne nt

Oscillations have been found in solar, atmospheric and reactor neutrino experiments,but only only indicate that Dm n 2 0 to determine < m n > => neutrinoless double beta decay 1. (A,Z) => (A,Z+2) + 2 e- + 2 ne¯ 2. (A,Z) => (A,Z+2) + 2 e- + c ( …2,3 c) 3. (A,Z) => (A,Z+2) + 2 e-

Double Beta –Disintegration M Double Beta –Disintegration M.Goeppert-Mayer, The John Hopkins University (Received May, 20 , 1935) From the Fermi theory of b- disintegration the probability of simultameous emission of two electrons (and two neutrinos) has been calculated. The result is that this process occurs sufficiently rarely to allow an half-life of over 1017 years for a nucleus, even if its isobar of atomic number different by 2 were more stable by 20 times the electron mass Since the very beginning double beta decay was considered as a powerful tool to test lepton number conservation. Many experiments were carried out sometimes with later disproved evidences. First evidences in geochemical experiments and for the first time with a direct experiment by M.Moe et al “The cukoo sang in the Spring (Peter Rosen)”

Neutrinoless bb decay 0n - bb decay 2n - bb decay u e - d W n e - d u

1/t = G(Q,Z) |Mnucl|2 <mn>2 Solar, atmospheric and reactor neutrino oscillation experiments indicate that Dmn 2 finite=> need to determine the absolute neutrino mass Direct experiments on b decay => mn < 2.2 eV KATRIN .35-.2 Results of WMAP and 2dF Galaxy Redshift Survey = > S mn < 0.7 eV 1/t = G(Q,Z) |Mnucl|2 <mn>2 rate of DDB-0n Phase space Nuclear matrix elements EffectiveMajorana neutrino mass Need to search for neutrinoless DBD in various nuclei A pick could be due to some unforeseen background peak

Neutrinoless bb decay would imply a non zero effective majorana neutrino mass as indicated by oscillation experiments

Experimental approaches Source = detector (calorimetric) Geochemical experiments i82Se = > 82Kr, 96Zr = > 96Mo (?) , 128Te = > 128Xe (non confirmed), 130Te = > 130Te Radiochemical experiments 238U = > 238Pu (non confirmed) e- Direct experiments Source = detector (calorimetric) Source  detector e- source detector Source  Detector

Present experimental situation Nucleus Experiment % Qbb Enr Technique T0n (y) <mn) 48Ca Elegant IV 0.19 4271 scintillator >1.4x1022 7-45 76Ge Heidelberg-Moscow 7.8 2039 87 ionization >1.9x1025 .12 - 1 IGEX Ionization >1.6x1025 .14 – 1.2 Klapdor et al 1.2x1025 .44 82Se NEMO 3 9.2 2995 97 tracking >1.x1023 1.8-4.9 100Mo 9.6 3034 95-99 >4.6x1023 .7-2.8 116Cd Solotvina 7.5 83 >1.7x1023 1.7 - ? 128Te Bernatovitz 34 2529 geochem >7.7  1024 .1-4 130Te Cuoricino 33.8 bolometric >2x1024 .2-1. 136Xe DAMA 8.9 2476 69 >1.2x1024 1.1 -2.9 150Nd Irvine 5.6 3367 91 >1.2x1021 3 - ?

Cryogenic detectors heat bath Thermal sensor absorber crystal Incident particle absorber crystal

@ 2 MeV ~10 mk ~ 1 kg <10 eV ~ keV DE @ 5 keV ~100 mk ~ 1 mg <1 eV ~ 3 eV @ 2 MeV ~10 mk ~ 1 kg <10 eV ~ keV

Two new experiments NEMO III and CUORICINO Pluris est oculatus testis unus quam auditi decem: qui audiun audita vidunt, qui vident plane sciunt (Plautus)It is better a single witness who saw,then ten who heard: those who heard report whatr the heard, those who saw, fully know Two new experiments NEMO III and CUORICINO

Searches with thermal detectors CUORE R&D (Hall C) Cuoricino (Hall A) CUORE (Hall A) Cuoricino (Hall A)

Crescita della massa dei bolometri total mass [kg] year

Resolution of the 5x5x5 cm3 (~ 760 g ) crystals : 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 ever realized) Energy [keV] Counts 210Po a line

18 crystals 3x3x6 cm3 + 44 crystals 5x5x5 cm3 = 40.7 kg of TeO2 Search for the 2b|on in 130Te (Q=2529 keV) and other rare events At Hall A in the Laboratori Nazionali del Gran Sasso (LNGS) 18 crystals 3x3x6 cm3 + 44 crystals 5x5x5 cm3 = 40.7 kg of TeO2 Operation started in the beginning of 2003 => ~ 4 months Background .18±.01 c /kev/ kg/ a T 1/2 0n (130Te) > 2x 1024 y <mn> .2 -1. Klapdor 0.1 – 0.9 2 modules, 9 detector each, crystal dimension 3x3x6 cm3 crystal mass 330 g 9 x 2 x 0.33 = 5.94 kg of TeO2 11 modules, 4 detector each, crystal dimension 5x5x5 cm3 crystal mass 790 g 4 x 11 x 0.79 = 34.76 kg of TeO2

Tower assembling

DBD and Neutrino Masses Present Cuoricino region Arnaboldi et al., submitted to PRL, hep-ex/0501034 (2005). Possible evidence (best value 0.39 eV) H.V. Klapdor-Kleingrothaus et al., Nucl.Instrum.and Meth. ,522, 367 (2004). With the same matrix elements the Cuoricino limit is 0.53 eV “quasi” degeneracy m1 m2  m3 Inverse hierarchy m212= m2atm Direct hierarchy m212= m2sol Cosmological disfavoured region (WMAP) Feruglio F. , Strumia A. , Vissani F. hep-ph/0201291

Next generation experiments Name % Qbb % E B c/y T (year) Tech <m> CUORE 130Te 34 2533 90 3.5 1.8x1027 Bolometric 9-57 GERDA 76Ge 7.8 2039 3.85 2x1027 Ionization 29-94 Majorana .6 4x1027 21-67 GENIUS .4 1x1028 13-42 Supernemo 82Se 8.7 2995 1 21026 Tracking 54-167 EXO 136Xe 8.9 2476 65 .55 1.3x1028 12-31 Moon-3 100Mo 9.6 3034 85 3.8 1.7x1027 13-48 DCBA-2 150Nd 5.6 3367 80 1x1026 16-22 Candles 48Ca .19 4271 - .35 3x1027 Scintillation 29-54 CARVEL 50-94 GSO 160Gd 22 1730 200 65-? COBRA 115Cd 7.5 2805 SNOLAB+

GERDA Approved by LNGS S.C. site: Hall A northern wing IONIZATION GERDA goal: analise HM evidence in a short time using existing 76Ge enriched detectors (HM, Igex) approach similar to GENIUS but less LN2 naked Ge crystals in LN2 or LAr more compact than GENIUS 1.5 m LN2(LAr) + 10 cm Pb + 2 m water 2-3 orders of magnitude better bkg than present Status-of-the-Art active shielding with LAr scintillation 3 phases experiment Phase I: radioactivity tests ≈20 kg 76Ge from HM and Igex expected bkg 0.01 c/keV/kg/y (intrinsic) check at 5s HM evidence 15 kg×y 6±1 bb events on 0.5 bkg events Phase II: add new enriched segmented detectors with special care for activation expected background ≈0.001 c/keV/kg/y 2×1026 y with 100 kg×y <m> 0.09 ÷ 0.29 eV Phase III: => 0.01 eV with 1 ton Ge worldwide collaboration Approved by LNGS S.C. site: Hall A northern wing funded 40 kg enriched 76Ge for phase II aggressive time schedule

Majorana concept: cosmogenics main background source (IGEX) White paper nucl-ex/0311013 concept: cosmogenics main background source (IGEX) 500 kg Ge crystals in ultra low background cryostats segmentation and PSD to reduce bkg 2 experimental phases: 180 kg → 500 kg Phase I: 180 kg 86% 76Ge (centrifugation) Modules with 57 crystals each ( 40 cm x 40 cm Cryostat) Three modules for 180 kg Eight modules for 500 kg (phase II) Maximal use of copper electroformed underground Background rejection methods Granularity Pulse Shape Discrimination Single Site Time Correlation Detector Segmentation Underground Lab 6000 mwe Class 1000 FULL EXPERIMENT (9 years from start in 2006) expected bkg 1.21 c/ton/y in ROI mainly Th from Cu structure 1/2  4 1026 y in 3 years 〈m〉  0.07 ÷ 0.21 eV

Scintillation X-MASS

Scintillation Nd dissolved in SNO => tons of material; 0n: 1000 events per year with 1% natural Nd-loaded liquid scintillator in SNO++ by Alex Wright simulation: one year of data maximum likelihood statistical test of the shape to extract 0n and 2n components…~240 units of Dc2 significance after only 1 year!

Tracking SuperNemo Planar geometry source (40 mg/cm2): 12m2 tracking volume: ~3000 channels calorimeter: ~1000 PMT Modular: ~5 kg of enriched isotope/module 100 kg: 20 modules ~ 60 000 channels for drift chamber ~ 20 000 PMT energy resolution E = 2.6% @ 3 MeV efficiency: 40% LNGS/LSM concept: scale NEMO setup tracking calorimeter already tested technology (NEMO) event topology (Detection of the 2 electrons) single and sum energy + angular correlation particle identification Background control source purification background level measurement external background reduction (Rn) No strong theoritical criteria for isotope selection: 82Se transition energy: 2 995 keV natural i.a.: 8.7% 2006-2008: R&D 2009: first module 2011: all modules 2016: final results 3 years R&D aiming at a 50 meV <mn> sensitivity: accepted by IN2P3 s.c. 5 kg of 82Se funded by ILIAS (Europe) Enrichment: 1 kg of 82Se in 2005 2 kg of 82Se in 2006 5 kg of 82Se in 2007 Enrichment of 100 kg of 82Se is possible in 3 years at ECP (Zelenogorsk)

EXO concept: scale Gotthard experiment adding Ba tagging to suppress background (136Xe136Ba+2e) single Ba detected by optical spectroscopy two options with 63% enriched Xe High pressure Xe TPC LXe TPC + scintillation calorimetry + tracking expected bkg only by -2 energy resolution E = 2% Present R&D Ba+ spectroscopy in HP Xe / Ba+ extraction energy resolution in LXe (ion.+scint.): OK Prototype scale: 200 kg enriched L136Xe without tagging all EXO functionality except Ba id operate in WIPP for ~two years Protorype goals: Test all technical aspects of EXO (except Ba id) Measure 2n mode Set decent limit for 0n mode (probe Heidelberg- Moscow) 2P1/2 4D3/2 2S1/2 493 nm 650 nm metastable 47s LXe TPC Full scale experiment at WIPP or SNOLAB 10 t (for LXe ⇒ 3 m3) b = 4×10-3 c/keV/ton/y 1/2  1.3×1028 y in 5 years 〈m〉  0.013 ÷ 0.037 eV

Tracking

The CUORE project (approved by the S. C The CUORE project (approved by the S.C. of Gran Sasso Laboratory and by INFN) CUORE is an array of 988 bolometers grouped in 19 colums with 13 flours of 4 crystals 750 kg TeO2 => 600 kg Te => 203 kg 130Te Crystals are separated by a few mm, only, with little material among them

CUORE expected sensitivity disfavoured by cosmology In 5 years: Strumia A. and Vissani F. hep-ph/0503246

Other possible candidates for neutrinoless DBD Compound Isotopic abundance Transition energy 48CaF2 .0187 % keV 76Ge 7.44 " 2038.7 " 100MoPbO4 9.63 " 3034 " 116CdWO4 7.49 " 2804 " 130TeO2 34 " 2528 " 150NdF3 150NdGaO3 5.64 " 3368 " 130Te has high transition energy and 34% isotopic abundance => enrichment non needed and/or very cheap. Any future extensions are possible Performance of CUORE, amply tested with CUORICINO - CUORE has been approved and has already an underground location Dilution refrigerator already funded

CONCLUSIONS Neutrino oscillations have been discovered and Dm2 is finite We need to determine the Majorana nature of the neutrino and the absolute value of <mn > Neutrinoless double beta decay would indicate not only lepton number violation , but also <mn >finite This process has been indicated by an experiment (Klapdor) with a value of ~0.44 eV but not yet confirmed Future experiments on neutrinoless double beta decay will allow to reach the sensitivity predicted by oscillations Their peculiar multidisciplinarity involves nuclear and e subnuclear physics , astrophysics , radioactivity, material science, geochronology etc There are more things in Earth and Heaven, Polonius, that can be dream’t of by our philosophy (Hamlet)