gerda and gedet project review 2010
play

GERDA and GeDet Project Review 2010 Fabiana Cossavella for GERDA - PowerPoint PPT Presentation

GERDA and GeDet Project Review 2010 Fabiana Cossavella for GERDA & GeDet groups Max-Planck Institut f ur Physik, M unchen 21 December 2010 Fabiana Cossavella GERDA and GeDet Project Review 2010 1/27 Director : Allen Caldwell Project


  1. GERDA and GeDet Project Review 2010 Fabiana Cossavella for GERDA & GeDet groups Max-Planck Institut f¨ ur Physik, M¨ unchen 21 December 2010 Fabiana Cossavella GERDA and GeDet Project Review 2010 1/27

  2. Director : Allen Caldwell Project leaders : B´ ela Majorovits (GERDA), Iris Abt (GeDet) Postdoc : Fabiana Cossavella, Josef Janicsko, Xiang Liu (03/10), Christopher O’Shaughnessy PhD : Neslihan Becerici-Schmidt, Sabine Dinter, Daniel Lenz (03/10), Oleksandr Volynets Diplomand : Hossein Aghaei-Khozani (11/10), Florian Faulstich, Sabine Hemmer (09/10), Annika Vauth (10/10) Group engineer : Hans Seitz, Franz Stelzer Engineering : Karlheinz Ackermann, Sven Vogt Many thanks to the Sonja Boisnel, Reinhard Sedlmeyer, Dominik Wamsler, Alex Wimmer, G¨ unter Winklm¨ uller and the colleagues from electronic & mechanic departments Fabiana Cossavella GERDA and GeDet Project Review 2010 2/27

  3. Search for 0 νββ decay Unknowns about Neutrinos: • Nature of the Neutrino (Dirac - Majorana?) • Absolute mass scale? Inverted/normal hierarchy? Evidence from Heidelberg- • CP phases? Moscow-Experiment n p 90% 90% degeneracy degeneracy F.Feruglio et al., Nucl. F.Feruglio et al., Nucl. CL CL L=2, w- Δ Phys. B 637(2002) Phys. B 637(2002) e - beyond SM Δm 32 < 0 eV Δm 32 < 0 eV e - Δm 32 > 0 eV Δm 32 > 0 eV w- n p If neutrinoless double beta-decay is observed: Neutrino is a Majorana particle Information on absolute mass scale |M nucl | 2 <m ee > 2 1/ τ = G(Q,Z) 0νββ Decay Phase space Matrix Effective Majorana rate factor element Neutrino mass Fabiana Cossavella GERDA and GeDet Project Review 2010 3/27

  4. Search for 0 νββ decay Signature: Sharp peak at Q-value of the decay (2039 keV for 76 Ge) Fabiana Cossavella GERDA and GeDet Project Review 2010 4/27

  5. The GERmanium Detector Array Clean-room Lock system Phase I: Water tank (steel) Use HdMo and Muon veto ( Č ) IGEX detectors (18kg) Cryostat (steel + Cu) Phase II: Liquid argon Use additional detectors from Detector array 37.5kg available enriched material Fabiana Cossavella GERDA and GeDet Project Review 2010 5/27

  6. Deployment of 1st string ◮ infrastructure completed in May 2010 ◮ 1st string of nat Ge installed in June 2010 background measurement ongoing since June 2010 Fabiana Cossavella GERDA and GeDet Project Review 2010 6/27

  7. Deployment of 1st string 4 10 GTF 45 4.4 keV FWHM Counts 2 10 0 10 0 500 1000 1500 2000 2500 3000 3500 Energy (keV) 4 10 GTF 32 4.0 keV FWHM Counts 2 10 0 10 0 500 1000 1500 2000 2500 3000 3500 Energy (keV) 4 10 GTF 112 4.2 keV FWHM Counts 2 10 0 10 0 500 1000 1500 2000 2500 3000 3500 Energy (keV) 228 Th calibration spectrum Fabiana Cossavella GERDA and GeDet Project Review 2010 7/27

  8. GERDA background Distinct peak at 1525 keV s o n r e c t e l m o f r d u n o g r c k a b u s u o n n t i o C ◮ background contributions due to 232 Th, 238 U: < 1 . 2 · 10 − 2 counts / ( kg keV y ) Fabiana Cossavella GERDA and GeDet Project Review 2010 8/27

  9. GERDA background Distinct peak at 1525 keV s o n t r e c e l m o f r d u n o g r c k b a s u u o n n t i o C ◮ 42 K + drift in the electric field ◮ Changing field configuration changes intensities → best background: 8 · 10 − 2 counts / ( kg keV y ) at Q ββ ◮ further studies ongoing Fabiana Cossavella GERDA and GeDet Project Review 2010 8/27

  10. GERDA enriched material Reduction in H 2 atmosphere enr GeO 2 powder enr Ge metal bars Zone refinement enr Ge 6N metal bars suitable for HP enr Ge crystal growth Reduction yield Zone refinement yield 98.5% 95.3% , overall 93.9% Material reduced and purified with yield > 80% (target) Fabiana Cossavella GERDA and GeDet Project Review 2010 9/27

  11. Crystal pulling for n-type HPGe detectors Pulling HPGe crystals is not trivial! Worlwide only three companies. Cooperation with IKZ, Berlin: Czochralski puller procured, Refurbrished and electropolished. Many crystals grown. One crystal with few 10 10 per cm 3 But most crystals with ~10 11 per cm 3 Still one order of magnitude too high 6N Material from PPM is already very clean Fabiana Cossavella GERDA and GeDet Project Review 2010 10/27

  12. The final lock system Outer Lock Cable Feedthrough Inner Lock Motor Feedthrough assembly starts after delivery of the 3-string arm of c-lock Fabiana Cossavella GERDA and GeDet Project Review 2010 11/27

  13. GeDet Project Development of segmented n-type Germaniun detectors for future applications 1 Ton initiative Properties of Ge detectors ◮ push further down sensitivity ◮ study of surface events ◮ normal or inverted hierarchy? induced by α and β ◮ 1 Ton of enr Ge ◮ study of pulse shape details to ◮ background index = 10 − 5 cts identify surface events and multiple interaction → keV − 1 kg − 1 y − 1 background reduction Fabiana Cossavella GERDA and GeDet Project Review 2010 12/27

  14. Test Stands: detector characterization K1 test stand: detector operated in vacuum cryostat (T from 90 K to 120 K), γ scans only task completed → prototype detector for a GERDA scale experiment “Characterization of the first true coaxial 18-fold segmented n-type prototype detector for the GERDA project”, Iris Abt et al., Nucl.Instrum.Meth. A 577 (2007) 574 Fabiana Cossavella GERDA and GeDet Project Review 2010 13/27

  15. Test Stands: detector characterization Gerdalinchen II ◮ able to handle 3 HPGe detectors in LN 2 or LAr ◮ operation at 77 K ”Operation of an 18-fold segmented n-type HPGe detector in liquid nitrogen”, Iris Abt et al., J. Instrum. 4 (2009) p11008 Fabiana Cossavella GERDA and GeDet Project Review 2010 14/27

  16. Pulse Shape simulation Development of a complete package to simulate pulses. Shape of a pulse strongly influenced by: impurity of the crystal ◮ impurities are not homogenous ◮ each crystal is individual ◮ uncertainty ∼ 20% − 30% mobility ◮ e − reasonably well known ◮ holes → available measurements differ inside a factor 2 Fabiana Cossavella GERDA and GeDet Project Review 2010 15/27

  17. Pulse Shape simulation h, outward drift [degree] 10 (a) <100> <110> <100> 40 〈 〉 010 0 0 5 〉 1 110 〉 〈 30 〈 0 20 5 10 10 y [mm] 〈 110 〉 0 120 140 160 180 200 220 240 260 280 -10 -20 -30 (b) -40 -40 -30 -20 -10 0 10 20 30 40 x [mm] ◮ trajectories are bent due to the crystal structure ◮ charge carries slower in the < 110 > than in the < 100 > direction → very clear for the holes trajectories Fabiana Cossavella GERDA and GeDet Project Review 2010 16/27

  18. Pulse Shape simulation 40 1 electron (a) γ hole B 30 20 C A -1 10 10 y [mm] 0 -10 -2 10 -20 -30 -3 -40 10 -40 -30 -20 -10 0 10 20 30 40 x [mm] ◮ electric signals induced on the electrodes by cumulative influence of moving electrons and holes ◮ pulse in segment B + mirror pulses in segments A and C ◮ kinks in core and segment B pulse when e − reach the core Fabiana Cossavella GERDA and GeDet Project Review 2010 17/27

  19. Pulse Shape simulation Data Fitted Simulated Pulse Time scale factor = 0.90 ± 0.01 χ ² /dof = 184/146 ◮ simulated core pulses fitted to measured pulses → simulation describe the general shape very well ◮ overall length of simulated pulse to be adjusted → ρ imp , T, µ Fabiana Cossavella GERDA and GeDet Project Review 2010 18/27

  20. Pulse lenght: T dependence Expectation 550 Rise time [ns] o Core, 0 , <110> axis ◮ if E ∼ const. → DS1, T=77.4 K 500 DS2 shifted for 8.5 K t r ∝ µ eff − 1 DS3 shifted for 10.0 K Fit p +p exp(-p /T) 0 1 2 450 Theoretical calculation ◮ µ eff ∝ T − 3 / 2 400 DS3 Data 350 ◮ Boltzmann-like law: DS2 300 t r ∝ e − k / T DS1 ◮ is something else 250 80 90 100 110 120 130 Temperature [K] T-dependent? ◮ t r core = 290ns, simulation T dependence will be included → in PS simulation package! ◮ t r core = 287ns, data Fabiana Cossavella GERDA and GeDet Project Review 2010 19/27

  21. GALATEA ◮ analysis of surface effects with coaxial Ge detectors ◮ direct irradiation with α and β particles and IR laser Fabiana Cossavella GERDA and GeDet Project Review 2010 20/27

  22. GALATEA first measurements ◮ 60 Co and 228 Th on top of the tank to test functionality ◮ alpha-( 241 Am), beta-( 90 Sr) and gamma sources inside the tank for precision measurements Fabiana Cossavella GERDA and GeDet Project Review 2010 21/27

  23. GALATEA first measurements Th spectrum of segment 7 with background number of events 600 Th228 500 400 FWHM @ 2.6MeV = 3.75 keV 300 200 K40 100 0 500 1000 1500 2000 2500 3000 energy in keV Fabiana Cossavella GERDA and GeDet Project Review 2010 22/27

  24. Background reduction R&D ◮ singly Compton scattered γ s escaping detector → same event topology as signal-like events ◮ use scintillation light to identify event as background ◮ normal PMTs contribute to radioactive background! Fabiana Cossavella GERDA and GeDet Project Review 2010 23/27

  25. Background reduction R&D ◮ 12 SiPMs + 15 m wavelength shifting fibers ◮ successfully operated in anticoincidence with 6-fold segmented HPGe detector ◮ detection efficiency ≈ 90 p.e./MeV energy deposit Fabiana Cossavella GERDA and GeDet Project Review 2010 24/27

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend