DarkSide-20k and the Darkside Program for Dark Matter Searches - - PowerPoint PPT Presentation

darkside 20k and the darkside program for dark matter
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DarkSide-20k and the Darkside Program for Dark Matter Searches - - PowerPoint PPT Presentation

DarkSide-20k and the Darkside Program for Dark Matter Searches Cristiano Galbiati Princeton University APC Paris Diderot GDR Neutrinos LPSC Grenoble June 6, 2016 DarkSide-20k Institutions 41 10 ] 2 ) 7 [cm 0 0 2 ( ) 5 P


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SLIDE 1

DarkSide-20k and the Darkside Program for Dark Matter Searches

Cristiano Galbiati Princeton University APC Paris Diderot GDR Neutrinos LPSC Grenoble June 6, 2016

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SLIDE 2

DarkSide-20k Institutions

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SLIDE 3

]

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[GeV/c

χ

M 10

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[cm σ

50 −

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49 −

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48 −

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47 −

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43 −

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42 −

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41 −

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D a r k S i d e

  • 5

( 2 1 5 ) D a r k S i d e

  • 5

( 3 y r p r

  • j

. ) D a r k S i d e

  • 2

k ( 1 t y r p r

  • j

. ) A r g

  • (

1 t y r p r

  • j

. ) W A R P ( 2 7 ) L U X ( 2 1 3 ) X E N O N 1 ( 2 1 2 ) P a n d a X

  • I

( 2 1 4 ) CDMS (2015) P I C O ( 2 1 5 )

10-1 t×yr 100 t×yr 101 t×yr 102 t×yr 103 t×yr 5 t×yr

LHC

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SLIDE 4

An Ambitious Discovery Program

  • Raising the bar: 0.1 ton×yr ⇒ 1000 ton×yr
  • Complementary to LHC and raising its energy scale:
  • 500 GeV ⇒ 1 TeV ⇒ 10 TeV ⇒ …
  • “Zero Background” absolutely necessary for a discovery program
  • Strong investment in 40Ar by INFN, NSF, and Fermilab
  • Ambitious program for discovery of heavy dark matter, potential

flagship program for LNGS

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SLIDE 5

The Root: DarkSide-50

  • The DarkSide-50 direct dark matter search:
  • A liquid argon TPC in stable operation having matched or

surpassed all basic requirements

  • The first dark matter detector operating with isotopically enhanced

target

  • Dark matter search operating in background-free mode
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SLIDE 6

Liquid Argon TPC 153 kg 39Ar-Depleted Underground Argon Target

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SLIDE 7

4 m Diameter 30 Tonnes Liquid Scintillator Neutron Veto

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SLIDE 8

10 m Height 11 m Diameter 1,000 Tonnes Water Cherenkov Muon Veto

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SLIDE 9

Liquid Argon TPC 153 kg 39Ar-Depleted Underground Argon Target 4 m Diameter 30 Tonnes Liquid Scintillator Neutron Veto 10 m Height 11 m Diameter 1,000 Tonnes Water Cherenkov Muon Veto

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SLIDE 10
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SLIDE 11

DarkSide-50 Milestones

  • Oct 2013: three detectors commissioned, cryostat filled with AAr
  • Oct 2014: WIMP search results with 1422 kg d AAr exposure
  • Fall 2014: Calibration campaign
  • Winter 2014: Refurbishment of LSV, 14C rate from 150 kHz to 0.3 kHz
  • Apr 2015: cryostat drained and filled with 153 kg of UAr
  • Oct 2015: WIMP search results with 2616 kg d UAr exposure
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SLIDE 12

S1 [PE]

2000 4000 6000 8000 10000 12000 14000 16000 18000 20000

s] × kg × Events / [50 PE

8 −

10

7 −

10

6 −

10

5 −

10

4 −

10

3 −

10

2 −

10

1 −

10

AAr Data UAr Data UAr MC Total Kr

85

MC Ar

39

MC

Bi

214

keV 609 (C+P) Co

60

MeV 1.17 (C+F) Co

60

MeV 1.33 (C+F) K

40

MeV 1.46 (P) Bi

214

MeV 1.77 (C+P) Tl

208

MeV 2.62 (P)

C: Cryostat P: PMTs F: Fused Silica

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SLIDE 13

β/γ nuclear recoils

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SLIDE 14

S1 [PE] 50 100 150 200 250 300 350 400 450

90

f 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 5000 10000 15000 20000 25000

50% 65% 80% 90% 95% 99%

]

nr

Energy [keV 20 40 60 80 100 120 140 160 180 200

1,422 kg d AAr - PLB 743, 456 (2015)

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SLIDE 15

S1 [PE] 50 100 150 200 250 300 350 400 450

90

f 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

50 100 150 200 250

50% 65% 80% 90% 95% 99%

]

nr

Energy [keV 20 40 60 80 100 120 140 160 180 200

2,616 kg d UAr - arXiv:1510.12345 (2015)

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SLIDE 16

S1 [PE] 50 100 150 200 250 300 350 400 450

90

f 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

10 20 30 40 50

50% 65% 80% 90% 95% 99%

]

nr

Energy [keV 20 40 60 80 100 120 140 160 180 200

2,616 kg d UAr - arXiv:1510.12345 (2015)

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SLIDE 17

Meeting Basic Requirements Pays Off

  • Light Yield: > 8 p.e./keV
  • Electron meanlife: >>5 ms
  • 39Ar contamination: 0.7 mBq/kg, factor 1,400 reduction res to

atmosphere

  • 222Rn contamination: <2 μBq/kg
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SLIDE 18

]

2

[GeV/c

χ

M 10

2

10

3

10

4

10 ]

2

[cm σ

50 −

10

49 −

10

48 −

10

47 −

10

46 −

10

45 −

10

44 −

10

43 −

10

42 −

10

41 −

10

D a r k S i d e

  • 5

( 2 1 5 ) D a r k S i d e

  • 5

( 3 y r p r

  • j

. ) D a r k S i d e

  • 2

k ( 1 t y r p r

  • j

. ) A r g

  • (

1 t y r p r

  • j

. ) W A R P ( 2 7 ) L U X ( 2 1 3 ) X E N O N 1 ( 2 1 2 ) P a n d a X

  • I

( 2 1 4 ) CDMS (2015) P I C O ( 2 1 5 )

10-1 t×yr 100 t×yr 101 t×yr 102 t×yr 103 t×yr 5 t×yr

LHC

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SLIDE 19

“Zero Background” condition (<0.1 background events) necessary to conduct discovery program

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SLIDE 20

What are the backgrounds for large scale, high mass dark matter searches?

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SLIDE 21

Scatters of pp solar neutrinos

  • n electrons

Radioactive noble gases (39Ar)

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SLIDE 22

Elastic Scatters

  • f pp Solar Neutrinos on Electrons
  • 200 events/tonne×yr in ROI
  • 200,000 background events @neutrino floor
  • Defeated in argon thanks to β/γ rejection better than 1÷1.6×107
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SLIDE 23

39Ar Rejection

1,422 kg×day (@AAr) 5.5 tonne×yr (UAr) 1,000 tonne×yr (UAr/DAr) additional active isotopic depletion and higher light yield x1400 (39Ar AAr/39Ar UAr)

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SLIDE 24

Based on what we know today, can a depleted argon experiment be background free at the scale of 1000 tonnes×yr?

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SLIDE 25

Yes

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SLIDE 26

Strategic Issues

  • Strong cooperation with Sardegna and Abruzzo on key associated

programs

  • Aria, Urania, SiPM, EBW
  • 1-ton technical prototype proposed @CERN
  • Exploring a possible directional effect
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SLIDE 27

Drift electric field [V/cm] 200 400 600 800 1000 S1 yield relative to 0 field 0.7 0.75 0.8 0.85 0.9 0.95 1 1.05 1.1 1.15 57.2 keV

d

ε Parallel to

d

ε Perpendicular to

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SLIDE 28

Impact of Basic Research on Industry

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SLIDE 29

Cryogenic Distillation Column at Fermilab

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SLIDE 30

Goals of Future Program

  • Procurement of 30 tonnes by 2020 in support of DarkSide-20k
  • 100 tonne×yr background free exposure for dark matter
  • Procurement of 300 tonnes by 2030 in support of Argo
  • 1000 tonne×yr background free exposure for dark matter
  • Precision solar neutrino measurements
  • Possible procurement of larger quantities … maybe to enable solar

and supernova relic neutrino physics in DUNE?

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SLIDE 31

Argon Purification Unit

  • A set of elemental process units:
  • The first cryogenic column removes the bulk of CO2 and CH4
  • The Pressure Swing Adsorption columns removes the traces of

CO2 and CH4

  • The second cryogenic column removes N2 and He
  • The third cryogenic column refines the argon-rich stream detector-

grade argon

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SLIDE 32
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SLIDE 33

Urania to Aria to LNGS

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SLIDE 34

Aria

  • The purpose of Aria is the reduction of 39Ar in the target of the

DarkSide detectors

  • The method of isotopic separation is cryogenic distillation
  • The project is supported by INFN, US NSF, and Regione Autonoma

della Sardegna

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SLIDE 35

Seruci Wells

Seruci in Sardinia an excellent location

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SLIDE 36

A Very Tall Column

10 20 30 40 50 60 70 80 90 100 110 120 130 140 150 160 170 180 190 200 210 220 230 240 250 260 270 280 290 300 310 320 330 340 350 360 370 380 390 400 410 420 430 440 450 460 470 480 490 500 510 520 530 540 550 560 570 580 590 600 10 20 30 40 50 60 70 80 90 100 110 120 130 140 150 160 170 180 190 200 210 220 230 240 250 260 270 280 290 300 310 320 330 340 350 360 370 380 390 400 410 420 430 440 450 460 470 480 490 500 510 520 530 540 550 560 570 580 590 600

Production Column 150 cm diameter 350 m height R&D Column 30 cm diameter 350 m height

325 m

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SLIDE 37

DarkSide-20k

20-tonnes fiducial dark matter detector start of operations at LNGS within 2020 100 tonne×year background-free search for dark matter

Argo

300-tonnes depleted argon detector start of operations at LNGS within 2025 1,000 tonne×year background-free search for dark matter precision measurement of solar neutrinos 20- 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 DS-20k ARGO

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SLIDE 38
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SLIDE 39

Photosensors for LAr Detectors

  • A new program of FBK/TIFPA and LFoundry under the guidance of INFN

and Princeton: complete replacement of Hamamatsu cryogenic PMTs

  • Much lower radioactivity
  • Light yield increase by 50%
  • Greater stability
  • Ten-fold reduction of costs per unit area vs. R11065-xx
  • Capability of large-scale production at LFoundry
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SLIDE 40

SiPM Requirements

  • PDE larger than 40% at 420 nm, signicant improvement over the 34% QE of the

photocathode of the Hamamatsu R11065 PMTs used in DarkSide-50

  • Dark count rate (DCR) lower than 1 Hz/mm2, as higher rates would impact both the

trigger efficiency and the pulse shape discrimination power

  • Total correlated noise probability (TCNP) (crosstalk + afterpulsing) lower than 40%
  • Inactive gap between devices smaller than 200 μm to maximize the tiling efficiency
  • Photo-electron gain larger than 1M and a signal duration of less than 300 ns
  • Overall surface 14 m2
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SLIDE 41
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SLIDE 42

The End