Liquid Noble DM Detectors Hugh Lippincott Cosmic Science Working - - PowerPoint PPT Presentation

liquid noble dm detectors
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Liquid Noble DM Detectors Hugh Lippincott Cosmic Science Working - - PowerPoint PPT Presentation

Liquid Noble DM Detectors Hugh Lippincott Cosmic Science Working Group 20 April 2017 Current status DS-50 2.6 tonne-day exposure LAr, background free (50 kg fiducial, 50 days) Xenon100 17.6 tonne- day exposure LXe, ~5 events (30-40


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SLIDE 1

Hugh Lippincott Cosmic Science Working Group 20 April 2017

Liquid Noble DM Detectors

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SLIDE 2

Current status

4/20/17 Presenter | Presentation Title or Meeting Title 2

DS-50 – 2.6 tonne-day exposure LAr, background free (50 kg fiducial, 50 days) Xenon100 – 17.6 tonne- day exposure LXe, ~5 events (30-40 kg fiducial, ~500 days) PandaX-II – 33 tonne-day exposure, ~3 events (334 kg fiducial, ~100 days) LUX – 40 tonne-day exposure, ~3 events (100 kg fiducial, ~400 days)

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SLIDE 3

Very near future

4/20/17 Presenter | Presentation Title or Meeting Title 3

DS-50 – Still running, expect ~40-50 tonne-day exposure (half that in hand), after another 2 years (x20 improvement) DEAP-3600 – full since November, 500 tonne-days raw exposure so far (my guess would be ~100 tonne-days with fiducial cuts, maybe matches LUX)

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SLIDE 4

Very near future

4/20/17 Presenter | Presentation Title or Meeting Title 4

PandaX-II – still running, up to factor x3 improvement at this point? XENON1T – Running interrupted by earthquake in January, >=40 days in hand, supposedly 1 ton fiducial (would match LUX exposure)

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SLIDE 5

]

2

WIMP mass [GeV/c 10

2

10

3

10 ) [pb]

SI p

σ (

10

log

  • 12
  • 10
  • 8

]

2

[cm

SI p

σ

  • 49

10

  • 48

10

  • 47

10

  • 46

10

  • 45

10

  • 44

10

  • 43

10

scattering

  • N coherent

ν 1 e v e n t 1000 tonne-years significance σ 3 LZ projected Median Significance σ 5 Median Significance σ 3 90% CL Median (Baseline) XENON1T 90% CL

Near future

4/20/17 Presenter | Presentation Title or Meeting Title 5

LZ – 5.6 ton fiducial – begins 2020 (trying to advance) XENONnT – 86% LZ by mass – upgrade to begin in 2018 in parallel with XENON1T operation Nothing revolutionary in design

}

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SLIDE 6

Mid to long term future - Argon

4/20/17 Presenter | Presentation Title or Meeting Title 6

  • DarkSide-20K – “start operation

2021…”

– Merger of DS50, DEAP, MiniCLEAN, ArDM – 20 tonne argon, two phase TPC – Approved at INFN as of this month – SiPMs for light readout

  • SNR decreases with increasing surface

area

  • 5x5 cm tile demonstrated in March

– Low radioactivity (Ar39 depleted) argon

  • Aria – isotopic purification using

distillation column the size of Eiffel tower – under construction

  • Urania – underground argon at large

scale

  • Argo/DEAP-nT - mid 2020s

– Kton –year exposures – R&D starting now (e.g. digital SiPM array)

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SLIDE 7

]

2

WIMP mass [GeV/c ]

2

Cross Section [cm

  • 49

10

  • 48

10

  • 47

10

  • 46

10

  • 45

10

  • 44

10

  • 43

10

  • 42

10

  • 41

10 5 6 8 10 20 30 40 60 100 200 400 600 1000

PandaX y) × DARWIN (200 t XENON100 XENON1T XENONnT / LZ DarkSide-50 DEAP-3600 L U X

  • line (Billard)

ν DarkSide-20k

Mid to long term future - Xenon

4/20/17 Presenter | Presentation Title or Meeting Title 7

  • LZ – not currently working on G3

– Can break 1e-48 barrier if hit targets – Expecting 0.5 neutrino events in 1000 days (2020-2023)

  • DARWIN – successor to XENON

– 40ton active (~$100M in xenon, worlds annual production) – Not that much bigger than LZ/XENONnT – Proposed project start in 2019-2020

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SLIDE 8

Xenon-Argon ~100 GeV WIMP considerations

4/20/17 Presenter | Presentation Title or Meeting Title 8

  • Xenon is a better target for the most part

– At high mass, 3.2x better sensitivity per unit mass – At low mass, >>3.2x better sensitivity (lower threshold) – More flexible physics

  • Spin dependent couplings, double beta decay, axion searches, electron interaction searches,

etc

– Denser (better self-shielding, smaller detectors/unit mass) – Not as cryogenic – 165K vs 85K (may have been a factor in PMT operation)

  • Two major exceptions

– Cost – raw material is much more expensive

  • Although the effort needed to find low radioactivity argon is significant. Unclear how this

scales, probably argon still comes out way ahead for ~100 tonne scales, assuming it works

– Electron recoil rejection

  • Rn/pp solar neutrinos are the biggest backgrounds in LZ/XENONnT. Because ER rejection is
  • nly ~1e-3-1e-4, you need to do really well at radon mitigation. Argon does not have this

problem (~1e-8 or better)

  • How important is the last decade to the neutrino floor?

– LZ expects 0.5 neutrinos, so diminishing returns starts then – ~x50 increase in exposure gives ~x10 sensitivity

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SLIDE 9

Reach thermal DM production parameter space in <1 year!

plots from Essig et al, cf. arXiv:1703:00910 Xe 3 events 1 kg-year The only existing limits on dark sector DM are from liquid xenon targets Xe 3 events 1 kg-year

8

Other ideas

4/20/17 Presenter | Presentation Title or Meeting Title 9

  • Xenon

– Doping with He/Ne for low mass sensitivity – use existing detector, extend reach down to 1 GeV or below in optimistic scenario (my EC proposal from 2015)

  • Not competitive with dedicated detector like SuperCDMS, but not too bad either

– Single electron counting – P. Sorensen at CV workshop

  • Optimize on S2, forget about S1
  • R&D on eliminating electron backgrounds observed in LUX/XENON100
  • Proposal for 10 kg scale, could then scale up and observe freeze-in/freeze-out regions
  • [/]
  • []
  • []
  • ν

ν

LZ Neon LZ Helium LZ Helium S2-only

LZ Xe

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SLIDE 10

Superfluid helium detector (Hertel, McKinsey, etc)

4/20/17 Presenter | Presentation Title or Meeting Title 10

  • Aiming for 1 MeV to 1 GeV dark matter

– Detection of either He recoils (100 MeV dm masses) or electron recoils (<100 MeV)

  • Excitations in superfluid He

– Excimers (He2* molecules, created with eV-scale excitations) – Photons, rotons, at meV scale

  • Demonstration of excimer detection

using TES sensors in He (1605.00694)

  • Rotons are “high-momentum phonons”

– Difficult to detect, but many ideas (HERON, quantum evaporation)

101 102 103 104 105

Recoil Energy [eV]

0.2 0.4 0.6 0.8 1

Energy Fraction Nuclear Recoil

101 102 103 104 105

Recoil Energy [eV]

0.2 0.4 0.6 0.8 1

Energy Fraction Electron Recoil

Singlet Excimers Triplet Excimers IR photons Phonons/R-/R+

  • und up.

: partitioning

George Seidel, unpub.

23

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SLIDE 11

Superfluid helium detector (Hertel, McKinsey, etc)

4/20/17 Presenter | Presentation Title or Meeting Title 11

  • Backgrounds

– Standard radioactivity, neutrinos, gammas (LHe is radiopure) – Alan’s gamma-NR background – Arguments for low dark rate

  • Can do ER discrimination

using excimers at 20 eV and above

1 kg-y, superCDMS bg levels, 5eV calorimeter, some assumptions on roton detection