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Double Beta Decay - status and future

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Title: Proposed Experiments Author: Nigel J.T. Smith Last modified by: Nigel J.T. Smith Created Date: 6/23/2002 11:15:58 AM Document presentation format – PowerPoint PPT presentation

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Title: Double Beta Decay - status and future


1
Double Beta Decay - status and future
  • Double beta decay basics
  • Experimental challenges
  • Current experimental status
  • HM(HKK) result
  • Future experimental programmes
  • Dark matter and bb0n

Based on talks at ApPEC Peer Review of bb0n,
Nu2002 (heavily) .and a night in the Lamb
with Kai Züber and Roland
2
Double Beta Decay
Cremonesi Nu2002
3
bb0n Rates
Cremonesi Nu2002
4
Why do bb0n?
Cremonesi Nu2002
5
Experimental Considerations
Measure this
Cremonesi Nu2002
6
Key Issues
  • Multi-isotopic targets
  • Redundancy, redundancy, redundancy (J. Bahcall)
  • Background removal by different peak positions
    (ie noise peak at Q)
  • Enrichment
  • Radio-isotopic backgrounds
  • Energy Resolution
  • Discrimination
  • Removal of gamma, beta, neutron backgrounds
  • bb(2n) background irremovable (separate peaks)
  • Co-location of daughter ion
  • Theory
  • Matrix elements
  • Analysis techniques
  • Esp. in light of H-M claim

7
Current Experimental Limits
Cremonesi Nu2002
8
Current Experimental Limits
Cremonesi Nu2002
9
Heidelberg Moscow Experiment
Cremonesi Nu2002
10
HM(HVKK) Result
Cremonesi Nu2002
11
HM(HVKK) Result
Cremonesi Nu2002
12
Comments on HM(HVKK)
Cremonesi Nu2002
13
Reply to the comments on HM(HVKK)
Cremonesi Nu2002
14
IGEX Canfranc
hep-ex 0202026
15
Thermal detectors - Milano DB
Cremonesi Nu2002
16
Milano DBD-II
Cremonesi Nu2002
17
MDBD-II Results
Cremonesi Nu2002
18
MDBD-II Background
Cremonesi Nu2002
19
Proposed Experiments
Cremonesi Nu2002
20
Proposed Experiments
  • Half life normalised to 5 years operation

10s kg scale
Tonne scale
  • Matrix element range. Half life for 50meV mass
    (in 1026y)

Elliott and Vogel Ann. Rev. Nucl. Part. Sci. 52
(2002)
21
Modularity and prototyping
  • Modularity
  • Discrimination through segmentation
  • Increase in support materials
  • GENIUS vs. Majorana
  • Systematics checks
  • Prototyping
  • Direct scale-up of current technology wont
    require prototyping - too expensive?
  • Prototype is first module
  • All experiments involved in prototyping
  • Handling scale up issues (cryostats, mass, etc)
  • Handling readout options (laser tag, WLS fibres)
  • Cross check against Monte Carlo

22
NEMO-III
Cremonesi Nu2002
23
NEMO-III
Cremonesi Nu2002
24
CUORE
Cremonesi Nu2002
25
CUORicino
Cremonesi Nu2002
26
EXO - Xenon
Cremonesi Nu2002
27
EXO - two approaches
Cremonesi Nu2002
28
Majorana
Cremonesi Nu2002
29
GENIUS
Cremonesi Nu2002
30
GENIUS-TF
Cremonesi Nu2002
31
GEM
Cremonesi Nu2002
32
DCBA/COBRA
Cremonesi Nu2002
33
Pros and Cons
Technique Prototyping MultiIsotope Enrichment Resolution Mass limit Discrimination Problems
CAMEO CdWO4 scintillator Use of B-CF 65kg array No Needed 10 1 tonne Active shield Enrichment costs
COBRA CdTe diodes Underway Yes No (?) lt1 10kg Segmemtation Neutron background
CUORE TeO2 Bolometer Cuoricino approved No Not needed (34 natural) 0.2 1 tonne Active shield Segmentation Materials close to target
EXO LXe or Xe TPC Approved (Ba tag test, 100kg Lxe) No Needed lt2 10 tonne Co-location of daughter PSD Cost of enrichment Ba ion extraction
GENIUS Naked HPGe Genius-TF approved No G-TF natural G 86 enrichment 0.3 1 tonne PSD Cost of enrichment Use of LN Cosmogenics
Majorana HPGe 1 Ge det under construction No Needed (8 -gt 86) 0.3 420kg Segmentation PSD Cost of enrichment
MOON Mo Scintillator WLS/Scint/Mo testing No Yes 7 3 tonne (34 tonnes nat. Mo) Localisation High Q (3.03MeV) Resolution
NEMO Tracking chamber Scintillator NEMO-I/II Yes Yes 10 10kg Tracking Time of flight Magnetic field Radioisotopic impurity Scale-up?
TGV HPGe CaCO3 foils TGV 1 (1g) No Required (73) 0.2 ? TGV-2 10g Enrichment from CaF2 Mass
34
bb0n and dark matter
  • Many common elements for rare event searches
  • Theoretically prejudice for max sensitivity
    required
  • DM 10-10pb covers most of SUSY models
  • bb gt10 meV from oscillations
  • Both require large mass targets (1 tonne)
  • Low backgrounds required
  • High radio-purity materials
  • Good shielding
  • Discrimination required
  • DM nuclear vs. electron recoil, spatial
  • bb spatial (co-location of daughter)
  • Good resolution/threshold (high light yield,
    etc.)
  • DM keV range - bite into DM spectrum
  • bb MeV range - separate peaks at Q
  • Can we do both in one detector?
  • Xenon is an obvious candidate to consider within
    U.K.

Beware!
35
Xenon experience in UK/RAL
Gotthard Xe TPC DB experiment (Roland)
ZEPLIN dark matter programme (RAL, IC, Shef)
36
ZEPLIN as bb0n experiment
  • Developing ideas for combining dark matter and
    bb0n experiments
  • Key issues are
  • Energy scales of interest
  • Primarily a DAQ issue, saturation of readouts,
    etc.
  • Discrimination of backgrounds
  • Can position sensitivity in ZEPLIN be improved to
    check co-locality in DB?
  • Resolution at MeV scales
  • Looks OK in second generation DM targets
  • There is also bb capability
  • 124Xe (0.1 in nat. Xe) is one of seven known
    bb emitters
  • 2nb b gives 4x 511keV photon signal
  • 2nbEC gives X-ray (30keV) and 2x 511keV photon
    signal (
  • 2nECEC gives 2x X-ray (30keV) signal
  • Current limits for 124Xe are T0.52n gt 2x1014
    years, T0.50n gt 4x1017 years

37
Conclusions
  • The bb0n decay search has the promise of
    illuminating
  • Absolute mass scale of neutrinos
  • (note this is effective mass, unlike beta end
    point KATRIN)
  • Lepton number violation
  • Majorana vs. Dirac description
  • Current limits/claims 300meV
  • H-M (HVKK) Claim contested
  • Oscillation results encourage meV searches
  • Several programmes suggested on Ge, Xe, Te, Mo
  • Need large scale, good resolution,
    discrimination, enrichment
  • Possibility of DM detectors as DB
  • ZEPLIN programme?
  • One mans background.
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