warsaw - nemo initiative group zenon janas for search for neutrinoless double decay in nemo-3 and...
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Warsaw - NEMO initiative group
Zenon Janas
for
Search for neutrinoless double decay
in
NEMO-3 and SuperNEMO experiments
Warszawa, 03.07.2006
Warsaw - NEMO initiative group
W. Dominik, IFD UW
Z. Janas, IFD UW
T. Matulewicz, IFD UW
M. Pfutzner, IFD UW
E. Rondio, SINS........
Double beta decay
Main decay modes:
(A, Z) (A, Z+2) + 2e
2
0
(A, Z) (A, Z+2) + 2 e + 2 e
(A, Z)
(A, Z+1)
(A, Z+2)
L = 0
L = 2
Energy spectra of emitted electrons
arb
itra
ry u
nit
s
(Q ~ MeV)
220v0102/1 mMGT
Neutrinoless decay rate
Motivation of 0 decay studies
• neutrino nature: Dirac or Majorana ?
• absolute neutrino mass scale
• neutrino mass hierarchy
• Majoron emission ?
Tracking + calorimeter
Both techniques are complementary !!
only total energy measured
high energy resolution
good efficiency
compact detectors ( 10 m)
very pure crystals
source specific
Experimental approaches in decay studies
Calorimeter
HPGe – Te bolometers NEMO
individual electrons observed
modest energy resolution
small efficiency
large detector size ( 50 m)
background measured
universal
3 m
4 m
B (25 G)
20 sectors Location: Fréjus Underground Lab. 4800 m.w.e.
Source: 10 kg of isotopes (100Mo) cylindrical, S = 20 m2, 60 mg/cm2
Tracking detector: drift wire chamber operating in Geiger mode (6180 cells)Gas: He + 4% ethyl alcohol + 1% Ar + 0.1% H2O
Calorimeter: 1940 plastic scintillators coupled to low radioactivity PMTs
NEMO-3 detector
Ability to identify e, e, and © S. Julian, LAL
Criteria to select events• 2 tracks with charge < 0• 2 PMT, each > 200 keV• PMT-Track association • Common vertex
• Internal hypothesis (external event rejection)• No other isolated PMT ( rejection)• No delayed track (214Bi rejection)
Deposited energy: E1+E2= 2088 keVInternal hypothesis: (t)mes–(t)theo = 0.22 nsCommon vertex: (vertex) = 2.1 mm
Vertexemission
(vertex)// = 5.7 mm
Vertexemission
Transverse view Longitudinal view
Typical 2 event observed from 100Mo isotope
Trigger: at least 1 PMT > 150 keV
3 Geiger hits (2 neighbour layers + 1)
Trigger rate = 5.8 Hz
events: 1 event every 2.5 minutes
2 decay of 100Mo
T1/2(100Mo,2) = [ 7.11 ± 0.02 (stat) ± 0.54 (syst) ] 1018 yT1/2(100Mo,2) = [ 7.11 ± 0.02 (stat) ± 0.54 (syst) ] 1018 y
cos(ee)E1 + E2 (MeV)
219 000 evnts6914 g
389 days
219 000 evnts6914 g
389 days
2 sim.bgnd
Data
Sum Energy Spectrum Angular Distribution
2 sim.bgnd
Data
2.8 - 3.2 MeV range
Nobserved = 7 events
bgnd = 8.1 ± 1.3
0 decay of 100Mo
T1/2(100Mo,0) > 4.6 1023 y
<m> < 0.7 – 2.8 eV
T1/2(100Mo,0) > 4.6 1023 y
<m> < 0.7 – 2.8 eVR. Arnold et al., PRL 95 (2005) 182302
Plane geometry, 20 modules
Top view5 m
1 m
1 module: source: 34 m2 40 mg/m2 of enriched isotope
tracking volume: ~ 3000 drift chamber cells
calorimeter: ~ 1000 scintillators + PMTs
SuperNEMO - preliminary design
© S. Julian, NEMO-3 collaboration
NEMO-3 SuperNEMO
From NEMO-3 to SuperNEMO
7 kg 100 kg Mass of isotope
Efficiency () = 8 % () ~ 20 %
Isotope 100Mo
T1/2() = 7 x 1018 y
82SeT1/2() = 1020 y
~ 1 evt/ 100 kg / y ~ 1 evt / 7 kg / y
T1/2() > 2 x 1024 y
<m> < 0.3 – 1.3 eV
T1/2() > 2 x 1026 y
<m> < 0.04 – 0.1 eV
SENSITIVITYafter 5 years
Resolution~ 11 % at 3 MeV ~ 7 % at 3 MeV
208Tl and 214Bi background
Most promissing 0 projects
A.S. Barabash, arXiv:hep-ex/0602037
2005 - 2007 - R&D program
2008 - construction of the SuperNEMO module with 5 kg 82Se
2009 - 2011 - construction and installation of the 20 modules, start taking data with delivered modules
2012 - full SuperNEMO running with 100 kg of 82Se
Plans for SuperNEMO
SuperNEMO collaboration
Kurchatov Inst. Moscou, RussiaKarkhov UkraineManchester University, UKUCL London, UKINL Idaho Falls, USAMHC Massachusets , USASaga Univ., JapanTexas Univ. Austin, USA
CENBG Bordeaux, FranceIReS Strasbourg, FranceLAL Orsay, FranceLPC Caen, FranceLSCE Gif sur Yvette, FranceFNSPE Prague Univ., Czech Rep.ITEP Moscow, RussiaJINR Dubna, Russia
R&D tasks in the SuperNEMO collaboration
SuperNEMO R&D
Source
Enrichment
Purification
Foils prod.
Calorimeter
Scintillators
PMT
Drift Chamb
Prototype
Autom. wiring
Radiopurity
HPGe spectr
BiPo det.
Radon det.
MechanicsComputing
Simulation
Electronics
Calorimeter
Drift chamb
Trigger
© S. Julian, LAL
Possible contribution of Polish group:
- data analysis
• NEMO-3
- modeling and simulations
- main detector design and construction
- data analysis
- detector for purity control of drift chamber gas
• SuperNEMO
Detector for purity control of drift chamber gas
a possibility: Optical Time Projection Chamber
gas
CCD PMT
drift 1 s/cm
amp.
WLS
e
M. Ćwiok et al., IEEE TNS, 52 (2005) 2895
Performance of the OTPC
13O
p
K. Miernik et al.
Water shield ( 2 ktons)
Source foil
14 m
Needed cavity:
~60 x 15 x 15 m
Location: Modane, Gran Sasso …?
Full detector
3,75 m © S. Julian, LAL
20 modules: 100 kg of enriched isotope
100Mo 6.914 kg Q= 3034 keV
82Se 0.932 kg Q= 2995 keV
116Cd 405 g Q= 2805 keV
96Zr 9.4 g Q= 3350 keV
150Nd 37.0 g Q= 3367 keV
Cu 621 g
48Ca 7.0 g Q= 4272 keV
natTe 491 g
130Te 454 g Q= 2529 keV
measurement
External bkg measurement
search (all enriched isotopes produced in Russia)
100Mo purified in INL (USA) and ITEP (Russia)
sources in the NEMO-3 detector