WIMP dark matter : direct detection · 2013-12-10 · WIMP signal in direct detection • Nuclear...
Transcript of WIMP dark matter : direct detection · 2013-12-10 · WIMP signal in direct detection • Nuclear...
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WIMP dark matter : direct detection
Eric Armengaud (CEA Saclay - IRFU/SPP)Workshop «News from the dark» - Montpellier - 06/12/2013
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• Principles of WIMP direct detection
• History of the detection techniques and sensitivities
• Focus on current sensitivity of XENON100/LUX for «standard» WIMPs
• Other channels
Refs :- L. Baudis review talk, SUSY 2013- Particle Data Group review...
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WIMPs : appealing and testable
3
χ
χ
q
q
Direct detection- observe the interaction of galactic WIMPs directly on a terrestrial detector- dedicated experiments, require a strong detector R&D + underground infrastructure
Indirect detection- observe WIMP annihilation products from astrophysical objects- many « observatories » involved- current strongest constraint from FERMI : m ≳ 10 GeV for standard WIMPs
Colliders- WIMP production, detection of some « missing energy »; monojet/photon events- a main goal of LHC, now that the SM is complete- if new particle discovered : does not prove that it is dark matter
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Direct proof of WIMP dark matter: direct detection
Interaction in a terrestrial detector
Galactic WIMP velocity v ~ 200 km/s local density ρ0 Energy deposition
Nuclear recoil Er
θr
€
Er =mχ
2v 2
#
$ %
&
' ( ×
4mNmχ
mN + mχ( )2 × cos
2ϑ r~ 1 - 100 keV
€
R ~ ρ0σ vmχ mN
~ 0.04 100A
%
& '
(
) * 100GeVmχ
%
& ' '
(
) * *
σ 0
10−8 pb%
& '
(
) *
ρ00.3GeV cm−3
%
& '
(
) *
v0230 km s−1%
& '
(
) * kg−1day−1
Low-threshold detectors (~ few keV) Ultra-low-background detectors
4
• Scaling with MWIMP : low recoil energies at low MWIMP
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WIMP signal in direct detection
• Nuclear recoil spectrum ~ exponential• Scaling with A : ~ A2 for spin-
independant (SI) coupling
• Directionnality of recoils (~100% modulation)
• Annual modulation 7% effect €
dRdEr
=σ 0 ρ02mχmr
2 F2(q) dv f1(v)
vvmin
∞
∫
Standard assumptions are used by expts to provide a reasonable comparison between sensitivities⇒ put constraints in the plane (MWIMP,σ0)Systematics :- ⍴0~0.3 (0.0 - 0.8) GeV/cm3 - f1(v) : may include non-maxwellian velocity structures, additional dark disk etc.- nuclear + hadronic physics parameters !!
New EW physics + hadron physics
Nuclear physics
Astrophysics (WIMP velocity distribution and local density)
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WIMP signal in direct detection
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WIMP detection is hard : signal vs backgrounds
WIMP signal• Nuclear recoils• Single scatters in the detector• Interactions uniformly distributed in
the detector volume• Exponential recoil spectrum• «A2» dependance• Annual modulation• Directionality
Backgrounds• External gammas• Internal gamma contamination• Beta radioactivity : internal and
surface• Alpha radioactivity• Neutrons from material radioactivity• Neutrons from cosmic muons• Neutrino (coherent) scattering
Massive target (kg … ton[s] )Low detection threshold ( ~ few keV)Background rejection :
passive rejection = underground detector, shields, vetos.. active rejection = smart detector design
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A wonderful playground for detector R&D
BPRS
ANAIS
NaIAD
DAMA
KIMSLIBRA
IGEXHDMS
TEXONO
CoGeNT
C4
CDMSEDELWEISS
CRESST
EDELWEISS-II
CDMS-II
ROSEBUD
SuperCDMSEURECA
GeoDMSIMPLE
PICASSO
COUPP
PICO
DRIFTDM-TPC
MiMac
DAMIC
EDELWEISS-III
ZEPLIN
ZEPLIN-II
ZEPLIN-IIIXENON-10
XENON-100
LUXXENON1tLZ
DARWINXMASS
WaRP
ArDM
CLEAN DEAP
DarkSide
DEAP3600
Panda-XCDEX
Newage
DM-Ice
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• Principles of WIMP direct detection
• History of the detection techniques and sensitivities
• Focus on current sensitivity of XENON100/LUX for «standard» WIMPs
• Other channels
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History of sensitivities
Oroville expt Phys. Rev. Lett. 61, 510 - 513
• Germanium detectors (ionization)• Measure low-energy background spectrum down to ~ few keV• No background discrimination (ERs)• Compare to expected WIMP signal
•NRs : take into account quenching factor signal(ENR) = Q x signal(EER)
• Ancestors of CoGeNT
ER scale
Cosmogenic activation lines
Compton plateau + surface radioactivity
expt threshold ~ 3 keVsensitivity close to threshold
depends more on details
WIM
P-G
e
nWIMP = ⍴/M
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History of sensitivities
DAMA limit 1996, Phys. Lett. B389, 757
• Low-threshold scintillating crystals (NaI, CsI...)• Goal exploit pulse shape discrimination to reduce the ER background
• Statistical discrimination only, and hard at low energy• Can reduce the bg intensity by factor ~ 1-10.
• DAMA : then turned to annual modulation search (without PSD)
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History of sensitivities• Low-temperature bolometers• Combine phonon (heat) with ionization or scintillation measurement
• Event by event discrimination of ERs vs NRs• Orders of magnitude improvement in sensitivity
EDELWEISS-II neutron calibration
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History of sensitivities• Dual-phase Xenon TPCs• XENON10 - XENON100 - LUX - XENON1t• Discriminate ERs vs NRs with scintillation + ionization measurement
• Not as splendid as in bolometers, but decent enough, especially and remarkably at low E
• Scale to large volume (self-shieding) + radiopurity of Xenon : very low intrinsic bg• By far the leading technology as of 2013
LUX - spatial distribution of background
XENON10
0 (20
11)
XENON10
0 (20
12)
LUX (2013)
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• Principles of WIMP direct detection
• History of the detection techniques and sensitivities
• Focus on current sensitivity of XENON100/LUX for «standard» WIMPs
• Other channels
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Dual-phase Xenon TPC
« S1 » = direct light, scintillation« S2 » = light emitted when electrons are accelerated in the gas phase, ionization
Discrimination between ER and NRStrong self-shielding
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ER vs NR in practice for Xenon
• Discrimination works even at low energy! BUT event populations overlap• Cut on Δlog(S2/S1) to reject most ERs
⇒ typical rejection power > 99% for an efficiency loss 50%
First generation: Xenon10, ZEPLIN
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Low-energy calibration of Xenon
Scintillation signal :
Ionization signal :
Example of Leff measurementPlante et al., arXiv:1104.2587
Neutron diffusion exptScan over θ ! recoil energyFit data to low-energy MC
90% trigger efficiency
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XENON100 : global fit of NR responseAmBe calibration compared to (MC+absolute source flux measurement)
arxiv:1304.1427
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XENON100 WIMP search
• z position : from electron drift time• r position : from PMT signal pattern
- first «long run» : ~ 100 live days, fiducial Kr bckgd start to be limiting- reduced Kr → new run : 224 live days with expected bg ~ 1 event- Fiducial volume in the TPC : 34 kg (self-shielding against external radioactivity - PMTs ...)- « 2 events » : may belong to single electron tail ?
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XENON100 results
Limit derived from likelihood analysisLow-mass sensitivity may be disputed
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LUX : first WIMP search
• Run Apr-Jul 2013 @ Sanford lab, 4300 mwe
• 370 kg LXe TPC (118 kg fiducial), 2x61 PMTs, very similar to Xenon• Drift field ~180V/cm• Light yield ~ 8 phe/keV ⇒better
low energy response than XENON100
• Remarkable low-energy ER «calibration»
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LUX results
85 live days- Neutron bg ~ 0.06 evt- ER bg in fiducial volume 3.1x10-3 evts/kgd/keV
in particular only 4ppt 85Kr99.6% ER discrimination in 50% NR band : 0.6 evt
- Analysis window [2-30] photoelectrons- Likelihood analysis based on S1,S2 and position
Does NOT include «astrophysical uncertainties, nor calibration uncertainties (use NEST model)
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Example of COUPP (but also PICASSO, SIMPLE)• CF3I chamber with cameras + piezo-acoustic sensors• Thermodynamical parameters well choosen: see NR above a given threshold, don’t measure a spectrum !• Alpha bckgd : rejected with acoustic signal (alpha «louder» than NR)• COUPP-4 also has bckgd correlated with activity at the water/CF3I boundary
- Mostly competitive for SD, but project to compete on the SI channel- COUPP-4 (4kg) done - COUPP-60 : under installation at SNOlab- Ton-scale projected (PICASSO joining)
COUPP-60
Other techniques (1) : bubble chambers
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Other techniques (2) : Argon detectors• Production of singlet and triplet states with very different livetimes → Pulse
Shape Discrimination between NR and ER • Proven above ~50keV
• Very strong 39Ar electron recoil background• Need to use depleted Ar, found recently in deep underground site («UAr»)
+ dedicated method to extract and purify
- Single phase detectors (rely only on PSD)DEAP/CLEAN- Dual phase detectorsDarkSide
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• Principles of WIMP direct detection
• History of the detection techniques and sensitivities
• Focus on current sensitivity of XENON100/LUX for «standard» WIMPs
• Other channels
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Other channels
• Search for different couplings or signatures
• Other form factors / isospin violating / inelastic scattering ... : specific spectral analysis, multi-target
• Spin-dependent couplings : light nuclei targets
• Directionnality : low-energy trace reconstruction
• Annual modulation : high exposure
• Take advantage of detector developments to perform other physics searches than «standard WIMPs»
• Low-mass WIMPs (1 - 10 GeV) : lower threshold
• Very-low mass WIMPs (down to MeV) : low threshold and search ERs
• Axion searches : search ERs
• Other «exotics»...
• Neutrinos : eg. coherent scattering from solar neutrinos, reachable with multi-ton detectors and low thresholds
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Inelastic scattering
-Designed in light of DAMA results-Signal globally reduced and suppressed at low recoil energies-Heavier target preffered-Annual modulation enhanced
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Isospin-violating DM
�SI ⇠ µ2
M�[Z fp + (A� Z) fn]
2
Effective couplings to proton and neutron may differ
Need multi-target approach
arXiv:1307.1758
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Spin-dependent couplings
�SD ⇠ µ2 JN + 1
JN(aphSpi+ anhSni)2
Use several (light) targetsIn practice Xe is now sensitive enough to be the leading technology
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Measuring the WIMP-induced NR direction
• Strong WIMP signature, allows «WIMP astronomy»• Difficulty : reconstruct tracks@ low E, using a
large mass of gaz ⇒ R&D efforts
• DRIFT : TPC with MWPC wire readout (Boulby)• DMTPC : TPC with light (CCD) and charge readout• NewAge (Japan)• MIMAC : micro-TPC, low-pressure (~50mbar), using micromegas
Map of recoils in galactic coordinates : ~100%
feature !
€
dRdErdcosϕ
∝exp −ve cosϕ − vmin( )2
v02
%
& ' '
(
) * *
MiMAC : Eion~40keV recoil of F (CF4)
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Annual modulation of the event rate in DAMA
• NaI scintillating crystals (no rejection of ER bckgd)• 1.2 ton-yr (0.29 DAMA + 0.87 DAMA/LIBRA)• Search exclusively an annual modulation of the raw single interaction rate
• Large statistical significance, the signal is «as it should be»
• VERY low threshold• Efficiency close to threshold ?• ER bckgd in this energy range ?• Phase ~ modulation of muon flux @ LNGS (LVD) ?
→ «Environmental» effect?
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How to check DAMA’s claim?
• DAMA upgrade (PMTs, more cycles)
• Direct tests : DM-Ice• 17kg of NAIAD crystals @
IceCube - South Pole• Continuous running since June
2011• Which threshold.. ?
• Indirect tests :• NR hypothesis : now quite well
checked (high-mass, low-mass, SD, SI, inelastic...)
• ER hypothesis : XENON100 (but need calibration)
G. Gerbier
DM-Ice spectrum
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Low-mass WIMPs (1-10 GeV)
• Reported signals :• DAMA, CoGeNT, CRESST, CDMS• Unconvincing !!
• Reported constraints : • XENON10, XENON100, LUX,
EDELWEISS, CoGeNT, CDMS ...• Rely on assumptions• Threshold effect: less reliability when the
sensitivity curves «shoots to the stars»
• WIMP safe mass : protected against resolution effect; and require the expt sensitivity to > 1% of total WIMP spectrum
• eg. impact of escape velocity• ~12 GeV for XENON100 • ~9 GeV for LUX
CDMS 2013
Schwetz, arXiv:1011.5432
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CoGeNT spectrum and annual modulation
• Germanium, ionization only• PPC diode : achieve very low threshold
• Clear exponential rise of bgckd spectrum• Efficiency of PSD rejection near threshold?
• Annual modulation signal (~2.5σ), mostly at energy > exponential rise
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CRESST WIMP search
• Bolometers, reject ER using scintillation signal• Can choose target material• CaWO4 : Oxygen recoils sensitive to low-mass WIMPs
• Many residual bckgd, under control ?
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CDMS - Si target
140 kg.d, Si lower mass than Ge3 evts vs 0.7 bgVery near threshold (both ionization and phonon timing)Best fit 8.6 GeV, 1.9x10-42 cm2
Also a limit is set based on another Si dataset (why not combined?)
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Ex. of low WIMP-safe mass : «S2-only» XENON10
• No gamma rejection, poor position reconstruction
• XENON10 hardware trigger: S2, single electron
• 1.2kg, 15 kg.d
• WIMP-safe mass ~ 5 GeV
See also:- DAMIC (CCDs)- Heat-only bolometer measurements (CDMSlite, EDW0)
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Examples : DM ∈ dark sector U(1)D, DM interacts with ordinary matter through dark photon-photon kinetic mixing
- For sub-GeV DM, kinematics prefers direct detection using ER- Need ultra-low threshold detectors (eV scale)
- XENON10 single e- spectrum study- Ge detectors promissing
INTEGRAL 511keV signal
Sub-GeV dark matter
XE10
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Axion searches with DM detectors : EDELWEISS
• Constraint couplings of axions or axion-like particles to SM particles using the low-energy ER spectrum : need low bg, low threshold, good resolution
• 4 channels were explored:
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Bounds on axion couplings with EDELWEISSSolar Primakoff axion
Solar Compton-Bremsstrahlung axions
DM axion hypothesis (DAMA)
Solar axions from 57Fe (bound on gaexgaN)
Exclude 0.91 eV < mA < 80 keV for DFSZ axions with a single direct detection expt
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Neutrino physics
- «Classical» low energy ERs- NRs: coherent scattering vN → vN
ERs from pp solar neutrinos : oscillations, precision solar physics
NRs :- observe neutrino coherent scattering- irreducible background for WIMP search
8B solar neutrinos atm. + supernovae neutrinos
NB: DM detectors are also 0vBB detectors (test of Majorana/Dirac nature of neutrinos) - But difficult to be competitive in both channels with a single detector
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Backup
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Xenon response to ERsStill major uncertaintiesNeeded for:- ER interpretation of DAMA annual modulation- axion / sub-GeV WIMP searches
Baudis et al. 2013
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Germanium bolometers : EDELWEISS-CDMS
• Energy deposition E0 in the absorber ! ΔT=E0/C
• Working point ~ 20 mK (EDW) : C(T)~T3 ! large sensitivity
• Thermometer : various technologies• EDW : NTD sensor, thermal phonons• CDMS : TES, sensitive to out-of-equilibrium phonons
• Ionization readout (electrodes)• Measure the ionization yield for each event : discrimination between nuclear and electron recoils
EDELWEISSAbsorber ~ 400gNTD thermometer
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An example of setup : EDELWEISS-II (2006-2012)
• Located at Laboratoire Souterrain de Modane (1700m rock overburden)
• Clean room• Deradonized air circulation• Pb shield against gammas
• Archeological lead near detectors• Polyethylene shield against
neutrons : slows down fast neutrons from the rock or cosmic rays
• Muon veto : tag residual muons coming inside the PE shield
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Electron vs nuclear recoils in Ge bolometers
«EDELWEISS-I» detector design
(S. Scorza PhD thesis)
electron recoils
inelastic neutron scattering
neutron-induced nuclear recoils
FULL separation between ER and NR
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Surface events in Ge bolometers
• Local radioactivity : betas from 210Pb (from Radon in the air)
• Hard to control• Surface β interaction: ER but interaction depth ~
few microns $ incomplete charge collectionCannot discriminate clearly against NRs
210Po
206Pb α
5.3 MeV100 keV
210Bi
210Pbe- 61 keV max
γ 46.5 keV (4%)
22 yr
WIMP search - Edelweiss 2003Sensitivity limited by betas
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Rejecting surface events with «ID» bolometers‘a’ electrodes (+4V)
collecting‘b’ electrodes (-1.5V)
field shapping
‘c’ (-4V) ‘d’ (+1.5V)
fiducialvolume
• Same thermometer as EDELWEISS-I• Change the E field close to the surface using «interleaved» electrodes• Use ‘b’ and ‘d’ signals as a veto
• R&D started 2007, validation 2008• Physics run 2009-2010
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WIMP search with EDELWEISS-II
• 10 ID detectors, all working (redundancy between channels)• Each detector : 400g → 160g after fiducial cut• Stable cryogenics @ 20 mK for 14 months• 380 kg.d after all cuts, 98% efficiency @ 20keV threshold
NR signal region : 5 «WIMP candidates»Expected bg : 3 (mostly neutrons + «anomalous gammas»)
Phys. Lett. B702 (2011) 329-335
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Rejecting surface events with phonons : CDMS-II
• TES measure thermal and athermal phonons, with a complex division into cells ⇒ partial reconstruction of the interaction position (athermal phonon faster for near-surface interactions)• Reject betas, loosing ~50% WIMP efficiency
gammas
betas
neutrons
Phys. Rev. D 84, 011102 (2011).
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EDW-CDMS : low-threshold analysis
Heat energy (keV, NR scale)4 6 8 10 12 14 16 18 20
Fid
uc
ial
ion
iza
tio
n (
ke
Vee
)
2
4
6
8
10
Dedicated analysis to gain WIMP sensitivity at low energy (→ low-mass WIMPs)- using less exposure (best detector resolutions)- potentially less bckgd rejection- calibration and efficiency well controlled
CDMS: best threshold, EDW: best bg rejection
CDMS, Phys.Rev.Lett.106:131302,2011
EDW, PHYSICAL REVIEW D 86, 051701(R), 2012
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EDELWEISS-CDMS : current statusEDELWEISS-III • 40 FID (Full Interdigit) bolometers
with better fiducial volume and background rejection : 24 kg (~XENON100)
• Upgraded EDW-II infrastructure, in commissionning
Super-CDMS @ Soudan• Switched to «iZIP» technology : use
the ID concept for surface event rejection
• 15 detectors running
$ Both aim at ~ XENON100 sensitivity soon
FID800
SuperCDMS
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EDELWEISS-CDMS : (joint) future
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PandaX
PandaX @ CJPL:- Stage Ia in installation- Light yield 4-5 pe/keVee (low mass WIMPs)
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DEAP-3600 / MiniCLEAN, DarkSide, ArDM ...
• DEAP/CLEAN @ SNOlab : single phase• CLEAN: also Neon.• MiniCLEAN: 150 kg fid (360
total), achieve PSD demonstration• DEAP-3600: 1t fid (3.6 total), start
2014• DarkSide (~ WARP) : dual-phase
• 50kg active mass of UAr, construction/commissionning
• Within the Borexino CTF tank as a muon veto
• Prototype for future detector• Also ArDM @ Canfranc DarkSide
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XENON1t, XMASS
XMASS @ Kamioka:- sphere, ~900kg Xenon, water shielkd- rely only on fiducialization + low radioactivity- running but currently strongly background limited
XENON-1t @ LNGS- construction started, physics > 2015