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Dark Matter Detection with Liquid Xenon

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Title: Dark Matter Detection with Liquid Xenon


1
Dark Matter Detectionwith Liquid Xenon
  • Masahiro Morii
  • Harvard University
  • Laboratory for Particle Physics and Cosmology

2
Dark Matter
  • Existence of Dark Matter is well establishedfrom
    its gravitational effects
  • Coma cluster Zwicky, Galaxy rotation curve
    Rubin
  • Weak gravitational lensing, Bullet cluster
  • Amount of Dark Matter is inferred from
    cosmological data
  • 22 of the energy of the Universe
  • Local density 0.3 GeV/cm3
  • Identity of Dark Matter is unknown
  • Majority must be cold and non-baryonic
  • i.e. made of particles that are not a part of the
    SM
  • Dark Matter is a particle physics problemas much
    as a cosmology problem

3
WIMP Dark Matter
  • No shortage of candidates, but
  • WIMPs are the front runners
  • 100 GeV new particles with weak(and
    gravitational) interactions
  • Such a particle would naturally havethe right
    thermal relic density
  • Predicted in many BSM theories(e.g. the LSP)
  • Since the annihilation cross section
    is constrained by therelic density, we can
    predict

Direct detection
Production at colliders
4
Direct WIMP Detection
  • Best limits on the WIMP-nucleoncross section are
    5x10-44 cm2
  • CDMS Ge and Si crystals at 10 mK, 121 kg-day
    exposure
  • XENON10 liquid Xe, 136 kg-day
  • For LSPs, the interesting region is around 10-44
    cm2
  • Smaller cross sections possible, but increasingly
    difficult to reconcile with the flavor problem
  • Next generation of experiments aim for lt10-45 cm2

5
Liquid Xenon
  • WIMP-nucleus cross section ? A2
  • Xe (A 131.3) gives high signal rate
  • 100 kg-year exposure can probes(WIMP-p) lt 10-45
    cm2
  • Key liquid Xe properties
  • High density 3 g/cm3
  • High boiling point 165K
  • Good scintillator 42 photons/keV
  • ? 175 nm easy to detect with PMTs
  • High ionization yield W 15.6 eV
  • High electron mobility, low diffusion
  • No long-lived radioactive isotopes besides
    double-beta decays
  • 85Kr must be removed by charcoal chromatography

6
Two-Phase Xe Detector
  • PMTs collect prompt (S1) and proportional (S2)
    light signals
  • S1-S2 delay ? Drift length
  • S2 light pattern ? Horizontal location
  • S2/S1 ratio differs markedly between electron and
    nuclear recoil
  • gt98.5 rejection of EM backgrounds
  • Good scaling to larger masses
  • 1 m3 holds 3 tonnes
  • Instrumentation ? (mass)2/3
  • Backgrounds improve with size due to self
    shielding

7
LUX Experiment
  • LUX is a 350 kg (100 kg fiducial) liquid Xe
    experiment
  • Located in the Davis cavern, Sanford Underground
    Lab in Homestake, SD
  • XENON10 technology has beenimproved to achieve
    lt1 bkgd. in100 kg-year
  • Xe purification system has 300 kg/day throughput
    using a heat exchanger
  • Ultra-low activity Ti vacuum vessel replaces SS
    Cu
  • PMTs have low activity (9/3 mBq of U/Th per tube)
    and high QE (27)
  • 183 m3 purified water tank shields the detector
    from neutrons
  • Recoil energy threshold lt5 keV ? s(WIMP-p)
    5x10-46 cm2

8
LUX Collaboration
  • Brown, Case Western, LBNL, Harvard, LLNL,
    Maryland, Texas AM, Rochester, South Dakota,
    Yale
  • Funded by DOE NSF

9
Harvard Group
  • Harvard joined LUX in June 2009
  • Morii (50) is the PI
  • Took up a critical-path item post-amplifier
  • 120 channels of receiver-amplifier-shaper for the
    PMT signals
  • Full system is needed in November
  • Harvard took over production from UC Davis
  • Oliver and Morii improved the LLNL design
  • New LPPC engineer, Meghna Kundoor, working on
    testing
  • Components in hand. PC boards in fabrication
  • On track for November delivery
  • Recruiting a postdoc and 12 graduate students
  • Will take part in detector integration,
    commissioning
  • Develop analysis software framework

10
LUX Status and Schedule
  • Prototype LUX0.1 is operating at Case
  • 1 liter of liquid Xe viewed by 4 PMTs
  • Test cryogenics and Xe purification system
  • gt1 m electron drift achieved in 3 days
  • Assembly of LUX in Sanford surfacebuilding will
    start in November
  • All major components are in hand
  • Building is being fitted out
  • Fully-assembled LUX lowered to Davis cavern
    (4,850 ft) in Spring 2010
  • Dark Matter search will start!

11
LZ Proposal
  • LZ LUX scaled up to 1500 kg (1200 kg fiducial)
  • Joint collaboration of LUX and ZEPLIN-III
  • LUX infrastructure designed to accommodate LZ
  • s(WIMP-p) 2x10-47 cm2 in 2 years
  • 2000-fold improvement over current limits
  • Cost of liquid Xe 1000/kg
  • Maximize the fiducial/total mass ratio by
    rejecting single-scatter ?-ray background with
    liquid scintillator
  • Harvard will assume larger responsibilities
  • Development of low radioactivity, high-QE PMT
  • Complete analog electronics chain (pre postamp)
  • MRI-R2 proposal submitted this month
  • 3-year construction ? Data taking in 2013

12
Summary and Prospect
  • Exciting time for Dark Matter detection
  • Cosmology points us to compelling particle
    physics
  • Liquid Xe technology has the potential for first
    observation
  • Harvard is entering DM hunting with strong
    commitment
  • Producing critical component for the LUX
    experiment
  • PMTs and analog electronics for the proposed LZ
    experiment
  • Discovery potential of LUX is excellent
  • s(WIMP-p) 5x10-46 cm2 covers the SUSY-favored
    region
  • Dark Matter search run will start in 2010
  • LZ will push the sensitivity to 2x10-47 cm2 by
    2015
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