XENON Collaboration Experiment Status “Highlights” Rick Gaitskell Brown University, Department of Physics see information and links at http://xenon.brown.edu/ Gaitskell Current XENON Collaboration Columbia University +PostDoc *Grad Elena Aprile (PI), Karl-Ludwig Giboni, Sharmila Kamat+, Pawel Majewski+, Kaixuan Ni*, Bhartendu Singh+ and Masaki Yamashita+ Brown University Richard Gaitskell, Peter Sorensen*, Luiz De Viveiros* University of Florida Laura Baudis, David Day* Lawrence Livermore National Laboratory Adam Bernstein, Chris Hagmann and Celeste Winant+ Princeton University (move CWRU Jan 2005->) Tom Shutt, John Kwong* Rice University Uwe Oberlack ,Omar Vargas* Yale University Daniel McKinsey, Richard Hasty+, Angel Manzur* Gaitskell Brown University XENON Collaboration September 2004 v05 <2> XENON10 Schematic of Detector and Shield Design Outer Poly (30cm) Inner Poly (20cm) Muon Veto (Plastic Scint.) not deployed for XENON10 @GS Pb (22.5cm inc 5 cm ancient liner) Stainless Steel Cryostat (62kg) PMTs (Hamamatsu R9288/8520/8778) Activity for R8778 used as baseline in simulations XENON10: 7 inner top PMTs +16 inner bottom PMTs or CsI Photocath. +16 outer veto PMTs Teflon Xenon Gas Liquid Xenon – Inner Region (ø17.5 cm, h 15 cm, 11 kg) Liquid Xenon – Veto Region (thickness 5cm, 50 kg) Copper (2.5cm) Gaitskell Brown University (parameters used in Monte Carlos) XENON Collaboration September 2004 v05 <3> Dark Matter Goals • Dark Matter Goals (labeled on figure) o XENON10 - Sensitivity curve corresponds to ~2 dm evts/10 kg/month • Equivalent CDMSII Goal for mass >100 GeV (Latest 2004 CDMSII result is x10 above this level) • With only 30 live-days x 10 kg fiducial - Zero events would reach XENON10 sensitivity goal (90% CL), but we would like to do physics! • Important goal of XENON10 prototype underground is to establish clear performance of systems o XENON100 - Sensitivity curve corresponds to ~20 dm evts/100 kg/year • Background Simulations for XENON10 indicate it could reach b/g suppression necessary to reach this goal sensitivity limit (would require some modest upgrabut with 10 kg target would only give ~2 dm evts/10kg/year no physics. Gaitskell Brown University XENON Collaboration September 2004 v05 <4> Additional Assumptions • Monte Carlo Inputs (stated here for the record, won’t discuss in detail) Assume threshold for full discrimination 16 keVr o Liquid Xe (3 regions) o • LXe Fiducial (after any x-y-z position cuts) majority of inner Xe / LXe Inner (surrounded by Teflon wall - low Kr content) / LXe Veto (Xe outer layer, 5 cm simulated) o Nuclear/Electron Recoil Quenching Factor Primary Light (QFprimary) • Zero Field (Conservative) QFp = 20% • High Field (5 keV/cm) QFp = 50% — Electron recoil primary light yield reduced to 38-36%@ 1-5 kV/cm, (vs zero field) due to ionization component no longer recombining — Nuclear recoil primary light yield ~90%@5 kV/cm (vs zero field) o Background Discrimination • • • • o Electron Recoil assumed 99.5% (1 in 200) above threshold of 8 keVee/16 keVr Monte Carlo results focus on rates for region 8-16 keVee (16-32 keVr) External 5 cm LXe veto (Assumed 50 keVee threshold) Multiple scatter cut within inner region (Dxy = 5cm, Dz = 1cm) Radioactivity of Components • Taken from direct measurements U/Th/K/Co (unless otherwise stated) Gaitskell Brown University XENON Collaboration September 2004 v05 <5> Progress & Some of Remaining Challenges 2002-2004 + + + + + + + PMTs operation in LXe ~1 meter e in LXe CsI photocathode immersed in LXe Operating ~few kV/cm electric field Electron extraction to gas phase Electron/Alpha recoil discrimination Efficient & Reliable Cryogenic System Achieved Achieved In progress Achieved Achieved Achieved Achieved Technology in place in 10 kg above ground Prototype + + + + + + + QF measurement with neutron beam Low Electron/Nuclear recoil discrimination Kr removal Background Simulations Materials Screening HV system for 15 cm drift ~5 kV/cm Alternatives to PMT (beyond XENON10) Gaitskell Brown University XENON Collaboration Done; analysis on-going In progress, move to 10kg Small prototype studied Done on-going (SOLO) Testing on-going September 2004 v05 <6> XENON Event Discrimination: Electron or Nuclear Recoil? Within the xenon target: • Neutrons, WIMPs => Slow nuclear recoils => PMT Array (not all tubes shown) strong columnar recombination => Primary Scintillation (S1) preserved, but Ionization Time (S2) strongly suppressed • , e-, , (etc) => Fast electron recoils => Gas phase => Weaker S1, Stronger S2 Proportional Ionization signal from nuclear recoil too small to be directly detected => extract charges from liquid to gas and detect ~1 µs width much larger proportional scintillation signal => dual phase 0–150 µs depending on depth Simultaneously detect (array of UV PMTs) primary (S1) and proportional (S2) light => Primary Distinctly different S2 / S1 ratio for e / n recoils ~40 ns width provide basis for event-by-event discrimination. Challenge: ultra pure liquid and high drift field to preserve small electron signal (~20 electrons) ; efficient extraction into gas; efficient detection of small primary light signal (~ 200 photons) associated with 16 keVr Light Signal UV ~175 nm photons e-e- ee- Anode EAG e-e- eee-e- ee- Electron Drift ~2 mm/µs Liquid phase Liq. Surface Grid EGC Cathode EAG > EGC Interaction (WIMP or Electron) Gaitskell Addition of CsI Photocathode at base CsI is possible option being evaluated for prototype design A tertiary signal can be generated from absorbing primary photons by CsI photocathode in LXe: - No transmission loss - high QE 30% PMT Array (not all tubes shown) Time CsI Tertiary Gas phase Note: 16 keV nuclear recoil: ≈ 200 photons before applying efficiencies for geometry and PMT QE. Also ionization signal ≈ 7-20 electrons (assumes high field 8 kV/cm) Anode EAG 150 µs (if 30 cm chamber) Liq. Surface Grid EGC Primary ~40 ns width eLight Signal UV ~175 nm photons e- CsI Cathode EAG > EGC Interaction (WIMP or Electron) Gaitskell Available Signal in Liq. Xe (# of photons & electrons for 1 keV event) SUMMARY OF PARAMETERS FROM EXISTING MEASUREMENTS Zero Field High Field 0 V/cm 8 kV/cm GAMMA EVENT - 1 keV electron equivalent energy UV Photons 60-75 UV Electrons+Ions [60-75 elec] NUCLEAR RECOIL EVENT UV Photons Electrons+Ions 1 keV recoil energy 12-18 UV [12-18 elec] EFFECTIVE (NR/GAMMA) "QUENCHING FACTOR" UV Photons 20-25% Electrons+Ions [20-25%] 20-30 UV 50-60 elec 11.6 UV 0.4-1.2 elec 30-50% 0.8-2% • Summary The ranges shown reflect spread in existing experimental measurements o Note that the table considers signal from either 1 keV gamma or nuclear recoil event o 60 excitations / keV is equivalent to ~16 eV / excitation o Zero field electron-ion #’s in [ ] are inferred, but are signal is not measured (extracted) directly o Gaitskell Brown University XENON Collaboration September 2004 v05 <9> XENON R&D: Dual Phase 3D XeTPC Prototype XENON Set-up at Columbia Nevis Lab CsI PC in LXe. • Pulse Tube Refrigerator used to liquefy and maintain LXe at –95.1 ± 0.05 C • Array of 7 PMTs (Hamamatsu R9288) directly coupled to the Xe active volume • Fast and Slow digitizers for direct and proportional light waveforms • Drift Field > 1kV/cm; Extraction Field > 10 kV/cm '03 • Calibration with gamma (Co-57), alpha (Po-210) and neutron (AmBe)Sept. sources. Gaitskell Brown University XENON Collaboration September 2004 v05 <10> TPC and PMTs Details Gaitskell Brown University XENON Collaboration September 2004 v05 <11> Precise, Stable Cryogenics - Pulse Tube Cryocooler (Iwatani) - 100W Cooling Power @ 165 K - 3.5kW He compressor, water cooled -Used for pre-cooling (10W) and Xe liquefaction (45W) @ 5 slpm - 20W heat loss (insulation not yet optimized) Temperature Stability Feb 2-12, 2004 + Particularly Essential because PMT gain and Electroluminesence are T/P-dependant. + Safety: emergency recooperation of Xe demonstrated Gaitskell Brown University XENON Collaboration September 2004 v05 <12> XENON100:Cryogenic System and Xe Purification ~ 120 liters of LXe for target and shield. Pulse Tube Refrigerator with ~ 100 W cooling power (heat load on the XENON100 detector estimated at ~ 50W), used for keeping LXe at – 100 C within 0.1 degree. Pre-cooling (~1 day) and Xe liquefaction (~2 days) with same PTR. Hot Getter: Ba/Ti/V Pellets 350 degC - Remove H2O+O2, but not hot enough for more complex molecules. Ti Spark Purifier will be evaluated. September 2004 v05 <13> Gaitskell Brown University XENON Collaboration > 1m Drift Electron Attenuation Length XENON goal of 30 cm drift and ~few kV/cm E-field necessary for detection of ~ 20 e- signal (from 16 keV Xe recoil); requires purity < 1 ppb O2 equivalent. Have built & tested a dedicated Gas Purification System with continuous circulation through High-temp Getter. Gaitskell Brown University XENON Collaboration September 2004 v05 <14> Typical Light Waveforms from Dual Phase Chamber Localized ionization clouds liberated by alphas & 122 keV gammas Source below TPC --> photoelectric absorption events --> e- drift full LXe gap Gaitskell Brown University XENON Collaboration September 2004 v05 <15> Dual-Phase Discrimination Primary/Secondary Discrimination Gaitskell Brown University XENON Collaboration September 2004 v05 <16> R&D Milestone: Light Detection with UV PMTs in LXe 4.5kg Xe Circulation Gaitskell Brown University • Gridded Ionization Chamber (2 cm drift) viewed by 2 Hamamatsu R9288 with custom-developed HV divider also in LXe. • Demonstrated reliability of operation at –100 C and 3 atm. Measured single P.E. level. Gain calibration with blue LEDs. • Demonstrated compatibility of materials with high purity LXE requirement. Tested and optimized gas circulation performance and effectiveness. t~ 1ms. XENON Collaboration September 2004 v05 <18> Charge (Q amp) & Light Chamber in 3L chamber Best D E / E in LXE from light. Sensitivity Ideal for Quenching Factor Measurement with < 50 keV Neutron Recoils 57 Co (122keV) Best D E / E in LXe from simultaneous measurement of anticorrelated charge and light signals 137 Cs (662keV) Light σ/E = 8.8 % Light 3.5 p.e./keV Charge Charge +Light Gaitskell Brown University XENON Collaboration σ/E = 1.7 % September 2004 v05 <19> Hamamatsu PMT Selection Improvement in b/g’s of PMTs to ~20 mBq has been impressive (driven by XMASS). PMTs for XENON10/100 a realistic choice • Hamamatsu Low Background PMTs o The isotopes contribute differently to event rate in (8<E<16keVee) window. For inner PMTs the following concentrations (mBq/tube) of isotopes give the same event rates (238U/ 232Th/ 40K/ 60Co) — All Xe Events: — Xe Fiducial Anti-Coincident, Single Scatter Events: Model R6041 R9288 Photo (not same scales) Dimension & QE ø5 cm x 4 cm QE 5-8% ø5 cm x 4 cm QE 20% R8520 (2.5 QE >20% R8778 ø5 cm x 12 cm QE 26% Radioactive Background [mBq/tube] U Series Gaitskell Brown University Th Series 40K 360 90 5040 60Co 10 33.9 mBq – 238U equivalent (Use of Kovar for most of base) 10 10 120 3 0 5 23.7 mBq – 238U equivalent (expect further improvement) 13 4 60 XENON Collaboration Specifically designed for ops in LiqXe TPC Evolution of 6041 3 22.8 mBq – 238U equivalent 15 Base Components lower activity, than these #’s Comment 680 mBq – 238U equivalent (Dominated by glass seal at base) cm)2x3.5cm (good dyn optics) 10 / 6 / 319 / 23 mBq 10 / 10 / 461 / >80 mBq 3 Square/quad anode good fill factor (66.2%). Columbia tested at 150K/4 atm Designed for XMASS. Coverage Area: 49.7% Columbia tested at 150K/4 atm September 2004 v05 <20> The simulation is run with a source that simulates the emission lines of the 20 physical PMTs. For this simulated PMT, we used the Hammamatsu R8778 tube. 2D “Hitogram” – Energy vs. Depth Gaitskell Brown University XENON Collaboration September 2004 v05 <21> Inner Chamber PMT Gamma Background • Inner PMTs -- Hamamatsu 8778 (232Th/238U/40K/60Co): o Spatial Distribution and Energy Histogram for Events Detected in Inner Chamber XENON10 Target XENON10 Target x0.1 XE10/10 Gaitskell Brown University XENON Collaboration September 2004 v05 <23> Stainless Steel Gamma Background • Gamma Background from Stainless Steel Cryostat below XENON100 target - Liquid Xenon Veto provides excellent shield against radiation from Cryostat o Double-walled Cryostat, each wall 1/8” thick, total 50kg o Activity (per kg): 60Co: 23mBq / 238U: 3.5mBq / 232Th: 2.7mBq Inner Chamber Events (8 < E < 28 keV) Energy Histogram Anti-Coincident Inner Events (8 < E < 100keV) Spatial Distribution XENON10 Target XENON10 Target / 10 XE10/10 XE10/10 Gaitskell Brown University XENON Collaboration September 2004 v05 <24> XENON10 – Gamma/Electron Background Event Rates • Gamma Background Event Rates (8 < E < 16keVee) for XENON10 Module XENON10 Goal is 160 mdru gammas before electron recoil rejection o XENON100 Goal (16 mdru) can also be achieved using anti-coin. LXe Veto and multiple scatters cut o All rates quoted before assumed 99.5% electron recoil rejection vs nuclear recoil signal o Source Inner Event Rate (only z cut) (8 < E <16 keVee) [ mdru ] Inner Event Rate with extra cuts: Anti-Coincid. with LXe outer + single scatter cut (8 < E <16 keVee) [ mdru ] 7 Inner PMTs 38 3.5 16 Outer PMTs 8.3 <0.1 HV Shaping Ring Resistors 6.8 1.6 Stainless Steel Cryostat 33 5.7 6 6 Lead - - (PMT Neutrons) ( 10-5 ) ( 10-6 ) Total 92 mdru 16.8 mdru 85Kr (@ 0.1 ppb) Event Rate Tables for External Neutrons are dealt with in Appendix Gaitskell Brown University XENON Collaboration mdru = 10-3 evts/keVee/kg/day September 2004 v05 <25> R&D Milestone: Primary Light QF Measurement Existing published data are inconsistent & do not extend to the low-energy (~10-30 keV) region, of interest to next-generation DM searches: LXe Recoil (keV) Measured QF Authors 40 - 70 0.22 ± 0.01 Akimov, et. al. 2002 45 - 110 ~ 0.2 Arneodo, et. al. 2000 35 - 70 0.45 ± 0.10 Bernabei, et. al. 2001 CU RARAF 2.2 MeV neutrons p(t,3He)n Borated Polyethylene Lead LXe L ~ 20 cm BC501A scintillator tags recoil events: Gaitskell Brown University XENON Collaboration BC501A Using pulse shape discrimination and time of flight to BC501A to identify neutron recoils September 2004 v05 <26> Preliminary Results: Low Energy Quenching Factor (Zero Applied Field) 56.5 keV NR 15.5 keV NR Aprile et al., analysis on-going (current plots not to be considered definitive) - Electron equivalent Energy scale calibrated with 57Co spectrum & compared with MC - Multiple scattering makes low-E data more difficult to interpret Gaitskell Brown University XENON Collaboration September 2004 v05 <29> Field Dependence of Primary Nuclear Recoil Scintillation ~90% light yield at high field, similar to alpha recoil… Aprile et al., in preparation Gaitskell Brown University XENON Collaboration September 2004 v05 <31> Burle Industries MicroChannel Plate (MCP 85006) MCP similar gain to PMT / better form factor / BG similar Fast 1 ns electronic pulse width 30% QE of Photocathode best performance of ANY photo sensor we have tested. Pulse Area Spectrum from 207Bi ~80 keV x-rays 1000 160 ~100 phe pulse ~750 phe / 80 keV 100 80 ~30 keV x-rays! mV cts 0 10 1000 Gaitskell Brown University 3000 5000 phe XENON Collaboration 5x5 cm enclosure - MCP removed, leaving 4 separate anodes visible. 0 50 100 ns September 2004 v05 <32> Summary: XENON R&D Goals and Status • XENON Above Ground R&D Program: Goals achieved > 1 meter electron drift attenuation length in LXe o Reliable Operation of UV PMTs in LXe o LXe Cryogenics System with Pulse Tube Refrigerator o Dual Phase Operation with 7PMTs 100 % Electron Extraction o Novel HV Distribution to PMTs Array in LXe o Detector Simulations of E-Fields / Light Collection/ 3D TPC o Low Radioactivity PMTs (with ~10-100 mBq/2” tube) o MC Background Simulations o Xe Nuclear Recoils (10 –100 keV) Scintillation Efficiency and its Field Dependence ‡ (paper in preparation) o • R&D Goals Underway: Xe Nuclear Recoils (10 –100 keV) Ionization Efficiency and its Field Dependence o Demonstrate Electron / Nuclear Recoil Discrimination down to 16 keVr with PMTs coverage on bottom (~2.3-2.6 p.e./keV) o Combine Xe gas purification with Kr separation system ( < 0.1 ppb ) o Finalize Materials Screening and selection for XENON10 o • Construction of Underground Infrastructure/Shield Jul 05 –> • Operate 10 kg system underground Jan 06 –> Gaitskell Brown University XENON Collaboration September 2004 v05 <34>