Dark Matter Search Results from the Silicon Detectors of the Cryogenic Dark Matter Search Experiment

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1 Dark Matter Search Results from the Silicon Detectors of the Cryogenic Dark Matter Search Experiment Kevin A. McCarthy Massachusetts Institute of Technology On behalf of the SuperCDMS and CDMS Collaborations

2 The SuperCDMS Collaboration "#$%&'()*+$,$-./$-0123$!456!

3 The CDMS-II Experiment ZIP Detectors Z-sensitive Ionization and Phonon mediated 230 g Ge or 106 g Si crystals (1 cm thick, 7.5 cm diameter) Photolithographically patterned to collect athermal phonons and ionization signals Direct xy-position imaging Surface (z) event rejection from pulse shapes and timing 30 detectors stacked into 5 towers of 6 detectors 3 (7.6 cm) 1 cm CDMS-II Exposure Oct Aug kg-days in 4 Si detectors Oct July kg-days in 6 Si detectors July Sep kg-days in 8 Si detectors

4 Background Estimate Active Muon Veto: Neutrons rejects events from cosmic rays Indistinguishable from WIMPs! Cosmogenic: active veto Radiogenic: passive shielding & materials screening <0.13 expected events SLAC, Dec. 17, Jodi Cooley, SMU, CDMS Collabora Surface events Optimize in 3 energy bins expected events estimated before unblinding Surface Events 0 20 Neutrons 40 Discriminate using phonon timing 2 n Peeling the Shielding Onion Recoil Energy (kev)

5 Exposure vs. Recoil Energy WIMP Exposure (kg days) Total +Raw Exposure +Good Nuclear Recoil +Fiducial Volume +Phonon Timing Recoil Energy (kev) WIMP efficiency

6 Unblinding Results - before timing cut

7 Unblinding Results - after timing cut Candidate 1 Candidate 2 Candidate 3

8 Three Events! Detector T4Z3 Candidate 1 Candidate 2 Candidate 3 Normalized Yield Surface Event Distribution Neutron Distribution Normalized Timing 25 Detector T5Z3 Normalized Yield Surface Event Distribution Neutron Distribution Normalized Timing

9 Post-Unblinding Checks After unblinding, the data quality was rechecked Checked energy in other detectors to verify events were single scatters 3 4 Surface event background fully estimated from the tails of three different NR sideband distributions Events were well-reconstructed Cf neutrons 5.5 WIMP search events below band Candidate events ( stat.) ( syst.) Checked for the possibility of recoils from 210Po decay, and limited this to be <0.08 events. 206Pb Phonon Delay (µs) 0.41 events 7 8 Stat only Stat + syst 3 PDFs Events occurred during high-quality data series Phonon Risetime (µs) 252 Candidate 1 Candidate 2 Candidate Expected leakage 1.5

10 Profile Likelihood Analysis Incorporated data-driven background models into a WIMP+background likelihood analysis. Monte Carlo simulations of the background-only model indicate the probability of a statistical fluctuation producing three or more events anywhere in our signal region is 5.4%. Tower 4, Detector 3 WIMP model Surface Leakage Neutrons Note: these are the Normalized Distributions! Pb recoils 0.7 expected events Surface + n + Pb

11 Profile Likelihood Analysis - cont. Testing our known background estimate against a WIMP+background hypothesis A likelihood ratio test favors a WIMP+background hypothesis over the known background estimate as the source of our signal at the 99.81% confidence level (~3σ). The maximum likelihood occurs at a WIMP mass of 8.6 GeV/c 2 and WIMP-nucleon cross section of 1.9x10-41 cm 2.

12 Confidence Intervals and Conclusions Analysis of a kg-day exposure of the CDMS-II Si detectors has been performed. Three events were seen in the signal region with a total expected background of <0.7 events. An optimal gap analysis sets a limit for the spinindependent WIMP-nucleon cross section of 2.4x10-41 cm 2 for a WIMP mass of 10 GeV/c 2. Monte Carlo simulations of the background-only model indicate that the probability of a statistical fluctuation producing three or more events anywhere in our signal region is 5.4%. A profile likelihood analysis favors a WIMP +background hypothesis over the known background estimate as the source of our signal at the 99.81% confidence level (~3σ). We do not believe this result rises to the level of a discovery, but does call for further investigation. The maximum likelihood occurs at a WIMP mass of 8.6 GeV/c 2 and WIMP-nucleon cross section of 1.9x10-41 cm 2. hep-ex: CDMSII c34+c58 Si

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