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Double Beta Decay - status and future

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Presentation on theme: "Double Beta Decay - status and future"— Presentation transcript:

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 Enrichment
“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

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
10’s 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
Discrimination through segmentation Increase in support materials GENIUS vs. Majorana Systematics checks Prototyping Direct scale-up of current technology won’t 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 (?) <1% 10kg Segmemtation Neutron background CUORE TeO2 Bolometer Cuoricino approved Not needed (34% natural) 0.2% Segmentation Materials close to target EXO LXe or Xe TPC Approved (Ba tag test, 100kg Lxe) <2% 10 tonne Co-location of daughter PSD Cost of enrichment Ba ion extraction GENIUS Naked HPGe Genius-TF approved G-TF: natural G: 86% enrichment 0.3% Use of LN Cosmogenics Majorana HPGe 1 Ge det under construction Needed (8% -> 86%) 420kg MOON Mo & Scintillator WLS/Scint/Mo testing 7% 3 tonne (34 tonnes nat. Mo) Localisation High Q (3.03MeV) NEMO Tracking chamber Scintillator NEMO-I/II Tracking Time of flight Magnetic field Radioisotopic impurity Scale-up? TGV CaCO3 foils TGV 1 (1g) Required (73%) ? 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: >10 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 b+b+ capability 124Xe (0.1% in nat. Xe) is one of seven known b+b+ emitters 2nb+ b+ gives 4x 511keV photon signal 2nb+EC gives X-ray (30keV) and 2x 511keV photon signal ( 2nECEC gives 2x X-ray (30keV) signal Current limits for 124Xe are T0.52n > 2x1014 years, T0.50n > 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 man’s background….


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