THE LZ OUTER DETECTORlz.lbl.gov/wp-content/uploads/sites/6/2019/09/UCLA_SShaw_LZOD.pdf · The LZ...
Transcript of THE LZ OUTER DETECTORlz.lbl.gov/wp-content/uploads/sites/6/2019/09/UCLA_SShaw_LZOD.pdf · The LZ...
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THE LZ OUTER DETECTOR
UCLA Dark Matter 23/02/2018 Sally Shaw
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7T active LXe
120 Veto PMTs
17 T gadolinium loaded liquid scintillator (GdLS)
2Tyvek reflector
water
60cmOptical fibres
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The LZ Outer Detector S. Shaw UCLA DM 20183
NR
𝝲
𝝲𝝲
𝝲Neutron emitted from PMTs
Gd
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The LZ Outer Detector S. Shaw UCLA DM 2018
Acrylic Tanks
43 bottom tanks
4 side tanks
plug (for when YBe
calibration source not in use) 2 top tanks
Test run with tank frame mock-up - transport tanks down shaft, through mine to Davis cavern
→ ICP-MS radioassay → UV transmission tested → radon exposure & dust monitored → strength & hardness tested
Fabrication almost complete - tanks are in the oven right now!
side tankSide tank panel
Segmented tanks - easier transport and installation underground
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The LZ Outer Detector S. Shaw UCLA DM 2018
Liquid Scintillator
5
Minfang Yeh leading GdLS product at Brookhaven → produced 185T for Daya Bay
Technique - chelation of Gd with TMHA in LAB → result 0.1% Gd by mass
Solvent - Linear Alkylbenzene (LAB)
wavelength (nm)300 350 400 450 500 550 600
0
0.001
0.002
0.003
0.004
0.005
Event.tracks.dWavelength_nm {Event.tracks.iParticleID==0}
Emission spectrum
Wavelength shifter: bis-MSBFluor: PPO
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The LZ Outer Detector S. Shaw UCLA DM 2018
Light Collection
6
Requirement: > 80 phe / MeV
120 Hamamatsu 8-inch PMTs procured, being tested at the
IBS, South Korea
Light collection map for uniform 152Gd 𝝰-decays
Building and testing PMT assemblies and holders
Developing optical calibration system consisting of 35 optical fibre assemblies
Enhancement from tyvek surrounding cryostat
photoelectrons
LZ cryostat
Top tanks
Bottom tanks
Side tanks
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The LZ Outer Detector S. Shaw UCLA DM 2018
3 low background
PMTs
Water buffer
Liquid scintillator
Thoron calibration tube
Reynolds acrylic
Screener lowered into LUX water tank
Tyvek
152Gd &147Sm 𝝰
14C
Other 𝝰
Prototype - LS Screener
7
14C/12C: ~20x10-6 ppt
Sensitive to 𝝰, β, 𝝲:
→ measure whole 238U & 232Th chains
→ 40K, 14C
→ 152Gd, 147Sm low energy 𝝰-particles
→ cavern background (z-scan)
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The LZ Outer Detector S. Shaw UCLA DM 2018
Cavern Backgrounds
8
Initial simulations suggested cavern was dominant background in OD at > 90 Hz,
but Davis cavern 𝝲-flux was uncertain. Background Rate (Hz)
Gd/Sm 𝝰-decays 36 (100 keV)
Internals (238U/232Th/40K/14C)
8-24 (100 keV) ~few (200 keV)
LZ Components 7 (100 keV)
Acrylic / dust <5 (100 keV)
Cavern 𝝲-rays 91 18 (200 keV)
0 500 1000 1500 2000 2500energy (keV)
4−10
3−10
2−10
1−10
1
Cou
nt R
ate
(Hz)
208Tl214Bi
40K
New measurements of 40K, 238U and 232Th concentrations in rock used to simulate
rate in OD - now 18 Hz
OD backgrounds & expected rates
Shielded & unshielded measurements taken with NaI detector in empty water tank
Oct 2017: Cavern flux measurement team
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The LZ Outer Detector S. Shaw UCLA DM 2018
LZ Backgrounds
9
With sim, can assess whether we meet requirements:
Veto >95% of neutrons that scatter in TPC
Veto >70% of 𝝲 -rays that scatter in TPC
Background Expected NR PMTs 0.027
TPC (field rings, PTFE) 0.022
Cryostat 0.018
Muon induced neutrons
0.06
Surface Contamination (ɑ,n)
0.23
Ion Misreconstruction
0.16
Neutrinos 0.51
neutrons backgrounds beaten down by OD
(post cuts, pre 50% acceptance)
No veto Skin+OD vetoes
See talk by J. Dobson on LZ sensitivity
Geant4 simulation - radioactivity placed in detector components
In simulation, veto an event if: energy deposit > 200 keV in
OD, within 500μs of S1 in TPC
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The LZ Outer Detector S. Shaw UCLA DM 2018
Neutron Capture on Gd
10
𝝲
Integration of DICEBOX 𝝲 -cascade code with LZ simulation → 25% increase in vetoing efficiency!
Thermal neutron capture cross sections: 157Gd: 254,000 barns 155Gd: 61,000 barns
Very complex 𝝲-cascade - not
modelled well by Geant4
Capture time in GdLS/LS
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The LZ Outer Detector S. Shaw UCLA DM 2018
Performance
11
0 100 200 300 400 500 600 700 800 900 1000s)µod veto window (
1
1.5
2
2.5
3
3.5
4
4.5
5
5.5
6
inef
ficie
ncy
(%)
OD Threshold
0 keV
100 keV
200 keV
At 200 keV threshold, 500μs window, the OD is only 3.5% inefficient!→96.5 % of neutrons that single scatter within the region of interest in the TPC
(mimicking a WIMP) are vetoed
May be possible to go to 100 keV threshold, reaching < 3% inefficiency
No veto: 12.31 counts/1000 days
OD + Skin veto: 1.24 counts/1000 days
~3.3 T fiducial
5.6 T fiducial
Time between S1 in TPC & signal in OD (μs)
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The LZ Outer Detector S. Shaw UCLA DM 2018
Summary
12
• Construction of LZ veto detector well underway • Tanks almost complete, arriving at SURF in next couple of months • Liquid scintillator production starting July
• Analysis of prototype (LS screener) data ongoing, but already learnt a lot about contaminants and LS handling
• 14C measurement, light yield, quenching • Unexpected backgrounds - 147Sm, 176Lu, 7Be … • Data used to test LZ data analysis framework
• Analysis of NaI measurements of cavern 𝝲-rays also ongoing, but so far suggests 5x lower background rate in OD than first thought
• Performance of OD in simulation so far meeting all goals - vetoes 97.5% of WIMP search background neutrons
• Commission and calibration in 2020 - exciting physics to come!
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The LZ Outer Detector S. Shaw UCLA DM 201813
Thanks!
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The LZ Outer Detector S. Shaw UCLA DM 2018
Backup
14
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The LZ Outer Detector S. Shaw UCLA DM 201815
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The LZ Outer Detector S. Shaw UCLA DM 201816
Non-linearity of scintillator Daya Bay - Phys. Rev. D 95, 072006 (2017)
Pulse shape discrimination in the LS Screener
Proton light response Krosigk et al, Eur. Phys. J. C
External rate in the LS Screener
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The LZ Outer Detector S. Shaw UCLA DM 201817
OD Threshold (keV)0 100 200 300 400 500
Veto
Inef
ficie
ncy
0.02
0.03
0.04
0.05
0.06
0.07
DICEBOX
Geant4-FS
Full Sims, 100 keV Skin Threshold
6 7 8 9 10 11 1210-2
10-1
1
10
102
10
102
103
104
0 1 2 3 4 5 6
10-2
10-1
1
10
1
10
102
103
104
100 200 300 400 500 600 700 800 900 1000 1100 1200 1300 1400
102
103
104
¤ 6420
6672
6750
6914
7858
80
,89
256
278
@60
6
780
871
8982
998
1097
1108
,111
911
4112
31 1263
1323
1438
1517
4925
5582
5903
80
89 199
256 2
7829
7
@
606
768
780
871
915,
917,
918
944
9
6297
7
998
,100
4 1
010
1065 10
97
11
0811
17,1
119
1154
,115
9
1
180,
1184
1220
1231
1
260,
1263
1279 13
23,1
327
1373
=
=
Cou
nt/M
ass/
Flue
nce
×106
Energy (MeV)
182,
199
Sample: Gd2O3 (Gd)Holder: Teflon bagMass: 11 mg (9 mg)Live time: 6,620 sBeam: thermalFlux: 2.3×106 cm-2s-1
Eff. flux: 1×106 cm-2s-1
Vacuum: noCount rate: 3,101 cpsTotal counts: 20,530,263
64:Gd
1186
,118
72
1141
8982
182X
Gd(n,𝝲) spectrum (G. L. Molnar, ed., Handbook of Prompt Gamma Activation Analysis)
Gd neutron capture cross sections
Veto inefficiency (DICEBOX vs default Geant4)