Results from the LUX Experiment
Sally Shaw DMUK Meeting UCL, 18th January 2016
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Results from the LUX Experiment Sally Shaw DMUK Meeting UCL, 18th - - PowerPoint PPT Presentation
Results from the LUX Experiment Sally Shaw DMUK Meeting UCL, 18th January 2016 1 Large Underground Xenon Detector 2 The LUX Collaboration 3 The Black Hills 4 Sanford Lab, South Dakota 5 Direct Detection of WIMPs WIMP-nucleon
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Need a medium that produces something detectable after a nuclear recoil, and if possible a way to discriminate between signal (DM) and background (𝛿,e-,n) Need a low background environment, well shielded from cosmic rays and with minimal radioactivity
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cylindrical, distance between ions much shorter than e- thermalisation length → S2/S1 higher
Nuclear recoil (NR) tracks: dense, high recombination, low extraction → S2/S1 lower
32.2 keV 9.4 keV
83Kr 83mKr 83Rb
T1/2 = 1.83 h E = 32.2 keV T1/2 = 154.4 ns E = 9.4 keV T1/2 = 86.2 d J = 5/2-
83mKr → position reconstruction, S1 & S2 corrections, field mapping
CH3T injected via gas system distributes uniformly within LXe
Emax = 18.6 keV <E> = 5.9 KeV
performed every 3 months rubidium source left to decay, then build-up of krypton injected into LUX performed weekly
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arXiv:1512.03133
Neutrons pass through an air-filled acrylic conduit, collimated to 1°
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Beam aligned 15.5 cm below the liquid level within the LUX active region (maximise double scatters)
neutrons are within 4% of 2.45 MeV and are well constructed
Monte Carlo
arXiv:1608.05381
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NR band characterised with much better statistics than previously Results confirmed validity of past NR calibrations (AmBe,
252Cf)
arXiv:1608.05381
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2016 (Feb): spin-dependent limits arXiv:1602.03489 arXiv:1310.8214 arXiv:1512.03506 2006 2008 2012 2013 (April) 2013 (Nov) 2014 (Jan) 2014 (Sept) 2015 (Dec) 2016 (May) 2016 (July) 2016 (Sep) 2016 (Oct)
collaboration founded LUX funded LUX moved underground 1st science run starts 85-day limit published grid conditioning 2nd science run starts 2nd science run ends reanalysis limit published (95-day) 332-day limit published LUX decommissioned 427-day limit published
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Effects of grid conditioning between 1st and 2nd science run:
~49% to >70%
charge on PTFE wall 2006 2008 2012 2013 (April) 2013 (Nov) 2014 (Jan) 2014 (Sept) 2015 (Dec) 2016 (May) 2016 (July) 2016 (Sep) 2016 (Oct)
collaboration founded LUX funded LUX moved underground 1st science run starts 85-day limit published grid conditioning 2nd science run starts 2nd science run ends reanalysis limit published (95-day) 332-day limit published LUX decommissioned 427-day limit published
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4 bins in time, 4 bins in z Treat each bin as a separate detector, with its own calibration and model!
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2006 2008 2012 2013 (April) 2013 (Nov) 2014 (Jan) 2014 (Sept) 2015 (Dec) 2016 (May) 2016 (July) 2016 (Sep) 2016 (Oct)
collaboration founded LUX funded LUX moved underground 1st science run starts 83-day limit published grid conditioning 2nd science run starts 2nd science run ends reanalysis limit published (93-day) 332-day limit published LUX decommissioned 427-day limit published
arXiv:1608.07648
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2006 2008 2012 2013 (April) 2013 (Nov) 2014 (Jan) 2014 (Sept) 2015 (Dec) 2016 (May) 2016 (July) 2016 (Sep) 2016 (Oct)
collaboration founded LUX funded LUX moved underground 1st science run starts 85-day limit published grid conditioning 2nd science run starts 2nd science run ends reanalysis limit published (95-day) 332-day limit published LUX decommissioned 427-day limit published
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FV no longer a simple cylinder - calculate using acceptance of uniform 83mKr events and multiply by total LXe mass for each time bin Decayed away by the start of the 2nd run (half life ~36 days)
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arXiv:1608.07648 2006 2008 2012 2013 (April) 2013 (Nov) 2014 (Jan) 2014 (Sept) 2015 (Dec) 2016 (May) 2016 (July) 2016 (Sep) 2016 (Oct)
collaboration founded LUX funded LUX moved underground 1st science run starts 85-day limit published grid conditioning 2nd science run starts 2nd science run ends reanalysis limit published (95-day) 332-day limit published LUX decommissioned 427-day limit published
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2006 2008 2012 2013 (April) 2013 (Nov) 2014 (Jan) 2014 (Sept) 2015 (Dec) 2016 (May) 2016 (July) 2016 (Sep) 2016 (Oct)
collaboration founded LUX funded LUX moved underground 1st science run starts 83-day limit published grid conditioning 2nd science run starts 2nd science run ends reanalysis limit published (93-day) 332-day limit published LUX decommissioned 427-day limit published
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131Xe - 23.7%) for spin-dependent sensitivity
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Triplet 27ns Singlet 3ns
recombination
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Quantisation at low S1 is due to digital spike counting of photons
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data at 180 V/cm data at 105 V/cm NEST at 180 V/cm NEST at 105 V/cm bands are 1σ
Ly relative to 32.1 keV 83mKr decay
Aprile et al (zero field) Baudis et al (zero field) Baudis et al (450 V/m)
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10-4 10-3 10-2 10-1 1 2 3 4 5 6 7 8 9 10 probability energy [MeV] Spectra for spontaneous Cf252 fission 1 neutron emitted 2 neutron emitted 3 neutron emitted 4 neutron emitted 5 neutron emitted 6 neutron emitted 7 neutron emitted 8 neutron emitted
log10(S2b/S1) xyz corrected
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Qy determination: Calculate ne using S2 size, extraction efficiency and single electron size Bin in keVnr (0.7-24.2 keVnr) and fit signal model to each bin Unbinned extended maximum likelihood (resolution effects as nuisance parameter)
Ly determination: Model S1 and S2 distributions of single scatters using NEST with measured Qy Bin data in S2s, compare S1 distribution to model Ly measurement used S2s of 50 - 900 phd (900+ used for normalisatioin), corresponds to ~0-20 keV Fit each bins ith maximum-likelihood optimisation of the simulated S1 spectrum, extract nᵧ
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effect of 2 phe emission
Run 3 threshold: 3 keV Reanalysis threshold: 1.1 keV
better background model → upper S1 threshold increased from 30 photoelectrons to 50
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emission per photon at the photocathode in a PMT (VUV effect)
improved
events”
data (low rates can still be used for WIMP search as is high energy)
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