Title: CDMS Run 21
1CDMS Run 21
Ray Bunker CDMS Collaboration Meeting Feb. 11th
, 2005
2Outline
- Run 21 Overview
- Review of R21 results to date
- Motivation for a low threshold analysis
- Analysis Strategy
- Backgrounds Noise
- Plans and Expectations
3Run 21 Overview
- Run Description
- Final background exposure at the shallow
Stanford Underground Facility - 17 mwe overburden (muon flux reduced by 5x)
- Relatively low gamma background
- 1st Tower of CDMS II ZIP technology detectors
- Four 250 gram Germanium (Z1, 2, 3 5)
- Two 100 gram Silicon (Z4 Z6)
- 118 live days taken during the first half of
2002 - 66 live days with 3V charge bias published,
hep-ex/0306001 - 52 live days with 6V charge bias unpublished
- Goals Achieved
- Confirmed CDMS I results candidate events
consistent with neutron background - Measured the muon anti-coincident flux at SUF
simultaneously with Si Ge ZIPs - Tested and confirmed Monte Carlo predictions of
neutron suppression rates due to addition of
internal polyethylene - Quantified gamma beta rejection
4Review of Results to Date
Run 21 Combined 3V 6V Background Exposure 49
kg-d after cuts
10-42 cm2 ?
5Motivation for Low Mass WIMPs
Bottino et al. hep-ph/0307303
New (2003) SUSY calculations make DAMA appear
more plausible
10-42 cm2 ?
Relax GUT scale gaugino mass unification
assumption
LEP2 chargino mass bound does not give a
neutralino mass lower limit
10-42 cm2 ?
6WIMP Detection Rates
- Consider a 100 GeV WIMP
- with a WIMP-nucleon cross
- section of 10-42 cm2
- Now consider a 10 GeV WIMP
- with a WIMP-nucleon cross
- section of 10-42 cm2
- Detection threshold is everything!!!
mc 10 GeV
Silicon ? 0 1.2 2.5
3.7 4.9 6.1 Germanium ?
0 0.46 0.93 1.4
1.9 2.3 Xenon ? 0
0.28 0.56 0.85 1.1
1.4 Visible Energy keV
7Run 21 Recoil Thresholds
Germanium Detectors Z2, Z3 Z5 Very Low, Stable
Thresholds lt 1 keV !
Silicon Detectors Z4 Z6 Low, Stable
Thresholds lt 2 keV !
8The Analysis
- Extend analysis threshold to include lowest
possible recoil energies - Understanding of backgrounds noise environment
critical! - Search both Germanium Silicon data for low
mass WIMPs - Use Germanium detector Z1 as veto only
threshold backgrounds are too high to be
sensitive to recoils from low mass WIMPs - Select events that pass
- Data quality cuts selects good pulse
chi-squares, remove multiple pulses data known
to be of poor quality - Muon veto anticoincidence cut selects events
with no veto activity 50 ms before trigger
(larger window for - recoils less than 3.5 keV)
- Qinner cut selects events for which the Qouter
charge signal is consistent with noise (no Qinner
Threshold cut) - Single scatters cut selects events for which
only 1 detector has phonon energy over its 6-s
threshold
9R21 Germanium Recoil Spectra 1st Pass
Z2 141 3V singles 3142 6V singles !?
Z3 114 3V singles 265 6V singles ?
Z5 148 3V singles 209 6V singles ?
10R21 Germanium 6V y Plots - Backgrounds
Large Z2 Candidate Excess Near Threshold Noise
Events?
1 keV Charge Feature New Background Source
Shallow Site Neutron Background
10.4 keV x-rays from 71Ge Decays
11The 1.3 keV Background
- Detector activation due to neutron calibration
Thermal Neutron Activation Decays via EC
n 70Ge ? 71Ge ? 70Ga
(stable) 21 Natural Abundance 11.4 day
half life
- 71Ge typically decays via Electron Capture
- from the K shell resulting in a 70Ga nucleus
- with a hole in its K shell
- The hole radiates outward releasing 10.4 keV
- in x-rays
- The decay may also proceed via EC from the
- L shell EC(L shell)/EC(K shell) 0.12
- Ga L shell binding energy 1.3 keV
Neutron Calibration (Activation!)
Beginning of Run 21
End of Run 21
12The Z2 Near-Threshold Excess
- Large noise-like excess of
- candidates near threshold
- Event rate vs. time sporadic
- probably not a true physics
- process
- Clear bursts of events throughout
- these runs many occur directly
- after LED flashing times
-
13Cutting the Near-Threshold Excess
Phonon Pulses
Elevated phonon pre-pulse baseline during event
bursts
Percentage of events with average baseline gt mean
2-s provides an excellent discriminant against
these event bursts
14(No Transcript)
15Event Burst Cut Optimization
Maximize S2/B
?
16Event Burst Cut Performance
Raw Exposure (days) Before Cut
After Cut 51.7
? 22.3
Candidate Event Count Before Cut
After Cut 3142
? 121 !!!
Taking correlations into account should result
in a greater exposure similar discrimination
17Event Bursts In Other Z?
Worst Z2 SeriesNumber in 6V data
EventTime histograms show no indications of event
bursts for Z3, Z4, Z5 or Z6 in 6V data
No event bursts for any Z in the 3V data
18R21 Silicon 6V y Plots
Low yield band likely leaking events into
signal region. Fixing should significantly clean
up the Silicon data.
19Plans and Expectations
- Remaining analysis for low mass WIMP search
- Finalize event bursts cut for Z2 6V cut
Qouter-like events in Silicon data - Recalculate exposure effienciences recoil
spectra - Subtract 1.3 keV background estimate gamma
leakage into nuclear recoil band - Compare remaining candidate events with
predicted neutron background (MC) - Calculate Limts
- Expectations
- Set NEW world best limits on the
spin-independent WIMP-nucleon cross section for - WIMP mass less than 10 GeV ???
- Publish Si Ge results in PRL