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Status of EDELWEISS-II. Outline. EDELWEISS experiment EDELWEISS-I limits EDELWEISS-II setup EDELWEISS-II preliminary results. *Expérience pour DEtecter Les WIMPs En SIte Souterrain (Underground experiment to detect WIMP). The EDELWEISS collaboration. CEA Saclay CSNSM Orsay
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Outline • EDELWEISS experiment • EDELWEISS-I limits • EDELWEISS-II setup • EDELWEISS-II preliminary results SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
*Expérience pour DEtecter Les WIMPs En SIte Souterrain (Underground experiment to detect WIMP) The EDELWEISS collaboration • CEA Saclay • CSNSM Orsay • IPN Lyon • Institut Néel Grenoble • FZ/ Universität Karlsruhe • JINR Dubna SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
EDELWEISS @ LSM (Laboratoire Souterrain de Modane) SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Ionization threshold Neutrons 73Ge(n,n',) Gammas Heat and Ionization Ge detectors Heat Reference electrode Center electrode Guard ring Amorphous (Ge or Si) ~ 60 nm Thermometer (Ge NTD) Fiducial volume(≈ 57%) Ge crystal Guard Electrodes Center electrode Ionization guard 7 cm • Simultaneous measurement of • Heat @ 17 mK with Ge/NTD sensor • Ionization @ few V/cm with Al electrodes • Different charge/heat ratio for nuclear recoils (WIMP, neutrons) and electron recoils (, ) • EI/ER = 0.3 for nuclear recoils • EI/ER = 1 for electronic recoils • Event-by-event discrimination of electron recoils (main background) m=320g Ionization center SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
EDELWEISS-I (V.S. et al., PRD 71, 122002 (2005)) • 62 kg.d with 3 detectors • Best sensitivity up to 2003, but • Background • Neutrons : 1 n-n coincidence observed (2 singles expected by MC) • Surface electron recoils • Miscollected charge events at low energy • Leak of events down to the nuclear recoil band not visible in coincidence events • Rate compatible with 210Pb contamination ( rate ~ 5 / kg.d) SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
EDELWEISS-II setup • Cryogenic installation (~ 20 mK) • Reversed geometry cryostat • Dilution refrigerator + pulse tube • Room for up to 120 detectors • Shielding • Clean room + deradonized air (15 mB/m3) • 20 cm Pb • 50 cm PE • Active veto (> 98% coverage) • Facilities • Remotely controlled sources for calibrations and regenerations • Remote operations (cryogeny, acquisition, …) • Detector storage and repair within the clean room • 9 cool-downs since January 2006 SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
EDELWEISS-II setup • Cryogenic installation (~ 20 mK) • Reversed geometry cryostat • Dilution refrigerator + pulse tube • Room for up to 120 detectors • Shielding • Clean room + deradonized air (15 mB/m3) • 20 cm Pb • 50 cm PE • Active veto (> 98% coverage) • Facilities • Remotely controlled sources for calibrations and regenerations • Remote operations (cryogeny, acquisition, …) • Detector storage and repair within the clean room • 9 cool-downs since January 2006 SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
EDELWEISS-II detectors • “standard” Ge/NTD bolometers (320 g) as for EDELWEISS-I • Ge/NbSi bolometers (400 g) • “interdigit” Ge/NTD bolometers (200-400 g) SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Results from “standard” NTD detectors • Commissioning background run (spring 2007) ~ 19 kg.d • 8 lowest threshold detectors selected • Only « pure center » events selected for better Ei resolution • Reduction of factor 3 of and background Ionization/Recoil Ratio Ionization/Recoil Ratio Recoil energy threshold (20-35 keV) SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Results from “standard” NTD detectors • Commissioning background run (spring 2007) ~ 19 kg.d • 8 lowest threshold detectors selected • Only « pure center » events selected for better Ei resolution • Reduction of factor 3 of and background Ionization/Recoil Ratio Recoil energy threshold (20-35 keV) SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Results from “standard” NTD detectors • Significant reduction of the background • Calibration with source (210Pb) to study the detector’s response to surface events • ~ 100 kg.d of fiducial exposure accumulated after quality cuts (analysis still underway) SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Results from Ge/NbSi detectors • Developed @ CSNSM since 2003 • Goal : active identification of surface events using athermal phonon measurement with NbSi thin film thermometers • Each signal = thermal + athermal component • For surface events, athermal higher in corresponding thermometer • Thermal signals proportional to the deposited energy • Discrimination parameter = asymetry of athermal part of signals from the two surfaces • Surface rejection ok, some problems in 2007 with film contacts / leak currents • Resolutions hasn’t reached Ge/NTD performances SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Results from Ge/NbSi detectors • Developed @ CSNSM since 2003 • Goal : active identification of surface events using athermal phonon measurement with NbSi thin film thermometers • Each signal = thermal + athermal component • For surface events, athermal higher in corresponding thermometer • Thermal signals proportional to the deposited energy • Discrimination parameter = asymetry of athermal part of signals from the two surfaces • Surface rejection ok, some problems in 2007 with film contacts / leak currents • Resolutions hasn’t reached Ge/NTD performances Data taken with 1 NbSi detector May & June 2007 ~ 1,5 kg.d fiducial SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Results from Ge/Interdigit detector • Keep the standard phonon detector • Modify the E field near surfaces with interleaved electrodes (6 ionization channels) • Use B and D signals as vetos against surface events • From preliminary sea-level measurements • Surface event rejection > 95 % • Fiducial volume ~ 50 % A electrodes : + 2V B electrodes + 1V Z (cm) guard electrode G : + 1V A & B Near surface event A , B & C Event in low-field area Electrons trajectories A & C Bulk event holes trajectories guard electrode H : - 1V Radial coordinate (cm) C electrodes : - 2V D electrodes : - 1V SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Results from Ge/Interdigit detector • Few kg.d of background runs @ LSM with a 200g detector • Performance as expected (resolutions, threshold, …) • Currently • 3 new 400g detectors • Precise measurement of rejection • A promising detector with a simple design calibration EDELWEISS-II ID-201 EDELWEISS-II ID-201 Neutron calibration SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Results from Ge/Interdigit detector • Few kg.d of background runs @ LSM with a 200g detector • Performance as expected (resolutions, threshold, …) • Currently • 3 new 400g detectors • Precise measurement of rejection • A promising detector with a simple design EDELWEISS-II ID-201 (4 kg.d) ER threshold < 20 keV No event below Q=0.5 SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Current run (May 2008 - …) • Instrumented detectors: • 23 “standard” Ge/NTD bolometers • 5 “NbSi” bolometers • 4 “Interdigit” bolometers ~ 10 kg of Ge SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
Conclusion • “standard” Ge/NTD detectors • Improved background understanding : significant reduction of , and backgrounds • 100 kg.d recorded and in analysis • Ge/NbSi detectors • Surface rejection ok • Resolution improvements needed • Ge/Interdigit detectors • December 2008 : 9 additional detectors • July 2009 : 120 kg.d fiducial exposure with threshold < 20 keV • Up to 35x320g Ge crystals available for reconfiguration as Ge/Interdigit SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th
EDELWEISS prospects • 1st Goal : • 4x10-8 pb in 2010 • Acquire physics data with 32 Ge/ID • 2nd Goal : • Few 10-9 pb in 2012 • ~ 70 detectors Ge/ID • EURECA (see H. Kraus’s talk next session) SANGLARD V., « Dark Energy and Dark Matter », Lyon, 2008 July 10th