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Probing neutrino mass withSuperNEMO
Ruben Saakyan
Ulisse at LSM Workshop
30 June 2008
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 2
Outline
• The Concept
• The Detector
• Physics reach
• Status of design study
• Schedule
• Summary
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 3
Neutrinoless double beta decay ()
L = 2!
1 20 0 0 21/ 2 0(0 0 ) ( , )T G E Z M
Lepton number violation parameter
can be due to , V+A, Majoron, SUSY, H-- or a combination of them!
Need detectors which can probe different mechanisms (and different isotopes)
m
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 4
T0
2/1 > . . A
M . t
NBkg . Eln2 . N
kC.L.
(y)
SuperNEMO experimental technique
M: masse (g) : efficiencyKC.L.: Confidence levelN: Avogadro numbert: time (y)NBckg: Background events (keV-1.g-1.y-1)E: energy resolution (keV)
Focus on lowering Nbkg and open-minded search for any lepton violating process
Calorimetry + Tracking
• Build on NEMO3 experience • Reconstruct two electrons in the final state (E1+E2 = Q)• Measure several final state observables
• Individual electron energies• Electron trajectories and vertices • time of flight • Angular distribution between electrons
• Background rejection through particle ID: e-, e+, , • Sources separated from detector can measure different isotopes
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 5
From NEMO-3 to SuperNEMO
7 kg 100-200 kg isotope mass M
18 % ~ 30 %
isotope 100Mo
82Se or/and 150Nd
T1/2 () > ln 2 M Tobs
N90
NA
A
NEMO-3 SuperNEMO
internal contaminations 208Tl and 214Bi in the foil
208Tl: < 20 Bq/kg214Bi: < 300 Bq/kg
208Tl Bq/kg
if 82Se: 214Bi 10 Bq/kg
T1/2() > 2 x 1024 y<m> < 0.3 – 0.9 eV
T1/2() > (1-2) x 1026 y<m> < 0.04 - 0.11 eV
energy resolution (FWHM) 8% @ 3MeV 4% @ 3 MeV
efficiency
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 6
USAMHCINL
U Texas
JapanU Saga
KEKU Osaka
FranceCEN Bordeaux
IReS StrasbourgLAL ORSAY
LPC CaenLSCE Gif/Yvette
UKUCL
U ManchesterImperial College
FinlandU Jyvaskula
RussiaJINR DubnaITEP Mosow
Kurchatov Institute
UkraineINR Kiev
ISMA Kharkov
Czech RepublicCharles U PrahaIEAP Praha
MaroccoFes U
Slovakia(U. Bratislava)
~ 90 physicists, 12 countries, 27 laboratories
SpainU Valencia
U SaragossaU Barcelona
SuperNEMO Collaboration
PolandU Warsaw
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 7
SuperNEMO preliminary design
Planar geometry. 20 modules for 100+ kg
Top view Side view
Source (40 mg/cm2) 12m2, tracking volume (~2k Geiger channels). calorimeter (600 channels)
5 m
1 m
4 m
Total: ~ 40 Geiger channels for tracking ~ 12k PMTs (3k if scintillator bars design)
Single model (baseline design)
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 8
Single sub-module with ~5-7 kg of isotope
~20 sub-modules for 100+ kg of isotopesurrounded by water shielding
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 9
1,5m
1,5
m
4,1
m
7,7
5m
2,4m
1m 1,5
m
J.FORGET SuperNEMO general design june 2008
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 10
100m
10m 12m
Hestorage
15m
Radonless air and gazmixtures production
ISO6workshop
Heavy work surface24,5
m
62m
17,5
m
46m
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 11
Choice of Isotope
Criteria of choice:
- High Q value- Phase space G
- half-life- natural abundance- enrichment possibilities
• purification of 4kg of 82Se underway (INL, US)• enrichment of 150Nd possible
82Se obtained by centrifugationImpossible for 150Nd, only laserenrichment
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 12
SuperNEMO simulations
• Full detector simulation– Event generator GENBB ( + radioactivity)– Geant 4– Reconstruction
• Tracks reconstructed from tracker hits and fitted
– Cellular automation for track patterns– Kalman filter for fitting
• Even vertex found in the foil
• Track matched with calorimeter hits
• Charge sign measured from curvature
• Draws heavily from NEMO3 experience
Overall efficiency ~30% (conservative scenario: B-field on, module width 1m, reject “double hits” etc..)
SNOVA
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 13
SuperNEMO simulations and physics reach
Se82 Nd150
“Con
serv
ativ
e” s
cena
rio
82Se:T1/2() =(1-2) 1026 yr depending on final mass, background and efficiency<m> 0.06 – 0.1 eV (includes uncertainty in T1/2) – MEDEX’07 NME150Nd:T1/2() =5 1025 yr <m> 0.045 eV (but deformation not taken into account)
Sensitivity
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 14
2006 – 2009
• Approved in UK, France and Spain. Smaller but vital contributions from US, Russia, Czech Republic, Japan.
• Main tasks and deliverables– R&D on critical components
• Calorimeter energy resolution of 4% (FWHM) at 3 MeV• Optimisation of tracking detector and construction
(robot)• Better background rejection (e.g. extra veto counters)• Ultra-pure source production and purity control • Simulations and geometry optimisation.
– Technical Design report in 2010– Experimental site selection (Frejus, Canfranc, Gran Sasso,
Boulby)
SuperNEMO Design Study
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 15
Calorimeter R&D
• Energy resolution is a combination of energy losses in foil and calorimeter E/E
• Goal: 7-8%/√E 4% at 3 MeV (82Se Q)
• Studies:– Material: plastic (PST, PVT) or liquid – Geometry and shape (blocks, bars)– Size– Reflective coating– PMT
• High QE• Ultra-low background
Factor of 2 compared to NEMO3!
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 16
Calorimeter R&D.
scintillator
Hamamatsu high-QE
PMT
207Bi
E/E = 6.5% E/E = 6.5% at 1 MeVat 1 MeV
3.8% at 3 MeV3.8% at 3 MeV
Scint. Block in
dark box
90Sr (370 MBq) e- beam
& trigger
DAQ
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 17
Scint Dimensions
(solid)
FWHM @ 1 MeV
PMT Size and Make
52 x 2 cm BC404 6.5 % 3in Ham-SBA
92 x 2 cm BC408 10.1 % 8in Ham-SBA w/ LG
142 x 2 cm BC404 9.2 % 8in ETL w/ LG
152 x 2 cm BC408 10.3 % 8in Ham-SBA w/ LG
20(hex) x 2 cm BC408 11.2 % 8in Ham-SBA w/ LG
** 202 x 2 cm PST (cast) 7.0 % 8in Photonis XP1886
** 202 x 10 cm PST (cast) 7.7 % 8in Photonis XP1886
Solid Scint. Results
** preliminary
Calorimeter R&D. Results so far.
Baseline design target!
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 18
Calorimeter R&D. Results so far.
Liquid Scint. Results
Scint Dimensions
(liquid)
FWHM @ 976 keV
PMT Size and Make
7.6 x 5 cm 7.6 % 3in Photonis XP5312
7.6 x 10 cm 8.0 % 3in Photonis XP5312
8.4 x 9.2 cm 7.3 % 5in Photonis XP2412
20.3 x 20 cm 11.3 % 8in Photonis XP1886
23(hex) x 9.2 cm 10.8 % 5in ETL 9390
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 19
Calorimeter R&D. Status.
• Four routes pursued– 8” PMT + plastic block– 8” PMT + liquid scintillator– 8” PMT + hybrid (liquid + plastic) scintillator– 2m scint. bar with 3” or 5” PMTs
• Target resolution 7-8% at 1 MeV (~4% FWHM at 3 MeV) reached for individual large baseline design blocks.
• PMTs– Working closely with manufacturers: Hamamatsu,
Photonis, ETL– Real breakthrough in high-QE PMTs from Hamamatsu and
Photonis: 43% QE.– Deep involvement in ultra-low background PMT
development (especially Photonis)
• Decision on calorimeter design in early 2009
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 20
Optimize length, wire material and diameter, read-out, gas mixture etcSeveral 1-cell and two 9-cell prototypes built and tested90-cell prototype being built
Tracker R&D
9-cell prototype in Manchester
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 21
Tracker studies. 1-cell prototypes.
370 cm
Plasma propagation timesAnode and cathode ring signals from ionization event
- Transverse position from electron drift times- Longitudinal position from plasma propagation times
- Wire diameter studies- Anode vs cathode rings only readoutfor longitudinal position reconstruction (anode readout feasible)- Electron drift times measured with laser - Cell diameter studies
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 22
Tracker studies. 9- and 90-cell prototypes.
12 wires per cell8 wires per cell
9-cell:End-cap design optimized for wiring robot feasible8-12 wires per cell workGeiger plateau > 200 VPlasma propagation efficiency ~100%
90-cellWill be built and wired by AugustTracking efficiency, cross-talk, ageing etcFinal SuperNEMO tracker design in early 2009.
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 23
Pair of end fittings
Anode wire feed mechanism
Clamp mechanism
Actuator mechanism
Tracker fully automated wiring.
Up to ~500,000 wires to be strung, crimped, terminatedWiring robot being developed in collaboration with Mullard Space Science Lab (UCL)
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 24
BiPo detector
• To measure contaminations of 208Tl and 214Bi in source foils before installation in SuperNEMO
• Goal: ~5kg of foil (12m2 , 40mg/cm2) in one month with a sensitivity of– 208Tl < 2 Bq/kg– 214Bi < 10Bq/kg
• BiPo-1 to measure scintillator surface contamination• Installed and commissioned in Canfranc in October’07• Temporarily relocated to Modane until Canfranc reopens• Extrapolated sensitivity from BiPo-1 first results:~1-10 Bq/kg • BiPo-2 results expected end 2008.
Background < 1 event/month!
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 25
SuperNEMO SuperNEMO Design StudyDesign Study
Schedule Summary2007 2008 2009 2010 2011 2012 2013
NEMO3 Running NEMO3 Running
Running full detector in 2014Running full detector in 2014
Target sensitivity (0.05-0.1 eV) in 2016/17Target sensitivity (0.05-0.1 eV) in 2016/17
construction of construction of 20 modules 20 modules
Installation Installation at new LSM at new LSM
Preparation of new Preparation of new LSM siteLSM site
BiPoBiPoinstallatioinstallatio
nn
BiPo1BiPo1Canfranc/LSMCanfranc/LSM
BiPoBiPoconstructionconstruction
BiPo BiPo running @ Canfrancrunning @ Canfranc
1-4 SuperNEMO modules1-4 SuperNEMO modules running at Canfrancrunning at Canfranc
SuperNEMO 1SuperNEMO 1stst module module
constructionconstruction
2014
30-Jun-2008 R. Saakyan: Ulisse at LSM Workshop. 26
• SuperNEMO: a chance to see a “smoking gun” evidence for 0 and directly disentangle underlying physics mechanism (V+A, Majoron, etc)
• Design Study addresses most critical issues– Energy resolution– Tracker optimization– Radiopurity
• Based on design study results full proposal for 100+ kg detector in 2010.– 82Se – baseline, 150Nd possible. – “Last minute” isotope change if e.g. CUORE sees the signal in 130Te.
• Start-up in stages due to modular approach– First module 2010/11– All 20 modules ~2013
• Target sensitivity: 50-100 meV by 2016/17
Summary