Water-based Liquid Scintillator and Isotope Loadings
Minfang Yeh
Neutrino and Nuclear Chemistry, Brookhaven National Laboratory
Future Solar Neutrino Detector at JinPing
Water-based Liquid Scintillator and Isotope Loadings Minfang Yeh - - PowerPoint PPT Presentation
Water-based Liquid Scintillator and Isotope Loadings Minfang Yeh Neutrino and Nuclear Chemistry, Brookhaven National Laboratory Future Solar Neutrino Detector at JinPing Water-based Liquid Scintillator 12000 Optical Photons per MeV LAB in
Neutrino and Nuclear Chemistry, Brookhaven National Laboratory
Future Solar Neutrino Detector at JinPing
2000 4000 6000 8000 10000 12000 50 100
Optical Photons per MeV LS%
utilizing nonlinear light-yield as a function
property of water for physics below Cerenkov or low-energy neutrino detection
be absorbed and re-emitted to give isotropic light.
detector (directionality).
reconstruction to separate the directional Cherenkov (fast) and isotropic scintillation (slow, controllable)
electrons neutrons LSND rejects neutrons by a factor of 100 at ¼ Cherenkov & ¾ Scintillation light (NIM A388, 149, 1997). 20%LS give ~50% light as a pure LS Minfang Yeh, BNL 6/17/2014 2 LAB in cyclohexane
scintillation in conventional scintillators
directionality
scintillation is ~1:1
Cherenkov
separation could discriminate low-energy , e-, e+ and
suppression, larger detector fiducial volume
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4
Cerenkov (e.g. SK, SNO) Scintillator (e.g. SNO+, Daya Bay)
Oil-like
technology for hydrophilic elements
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Water-based Liquid Scintillator
Water-like
Scintillation
(water‐based and metal‐doped) detectors for particle physics experiments.
emission, light‐yield coinc. PMT, 2‐m system, low bkg. counting, etc. (access to ICP‐MS at SBU) for detector R&Ds and prototype tests.
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K+ μ+ e+ μ+ e+
Hit Time (Time of Flight Corrected) [ns] Number of PE
10 102 103 104 50 10 15
p → K+ + ν e+ + νμ + νe _ μ+ + νμ 12 ns 2.2 μs
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Good Attenuation Length Fast Timing
need 104 optical purification
H2O
below and above Cerenkov
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WbLS Detectors
NSRL @BNL
210 MeV dE/dx ~ K+ from PDK 475 MeV Cerenkov threshold 2 GeV MIP
3 low Intensity Proton Beams
Water pure water WbLS 1 0.4% LS WbLS 2 0.99% LS LS pure LS
4 Material Samples
Tub 1 PTFE (highly reflective white Teflon) Tub 2 Aluminum coated with black Teflon
2 Detectors
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below Č threshold
8
475MeV and below
*
1 2 3 4 5 6 7 8 9 10 100 1000 10000 Charge (PE/MeV) Beam Energy (MeV)
T1 (white Teflon) Charge (in PE/MeV)
Water Sample WbLS1 Sample WbLS2 Sample LS Sample /30
0.001 0.01 0.1 1 10 0.1 1 10 100 Sample/LS Ratio LS Concentration (%)
Ratio to LS at 475-MeV
T1 Data T2 Data
linear or nonlinear?
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Reactor Solar Others
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Lead-doped scintillator calorimeter
Lithium-doped scintillator detector
11 Conventional loading is no good for hydrophilic ions (i.e. Te)
complexing ligands has been successfully applied to reactor ̅ detection (e.g. Gd-LS)
8-MeV ’s (Gd) vs. ,T (6Li) Neutron Tagging
Tellurium-doped scintillator detector
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7Li + e7Be + e-
115In + e 115Sn + e- + (τ =4.76 µs) 2 γ (LENS)
208Pb + e 208Bi* + e- & 208Pb + x 208Pb* + x (HALO)
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Minfang Yeh, BNL
Daya Bay PROSPECT
BNL + Yale PSD enhancement for 0.1% Gd-doped LS (compatible with plastics) over 6 months; and further improvement can be achieved 6/17/2014
A stable 0.1% Li-LS at ~5000 ph/MeV
than commercial product) for PROSPECT
sites
applicable to Li-LS
0.01 0.02 0.03 0.04 0.05 200 700 Absorbance Wavelength (nm)
51213 71913 90813 103113
500 1000 1500 2000 2500 3000 3500 4000 1000 Counts (AU) ADC Channel
0.1% Li - 2nd formulation 0.1% Li Commercial Product LAB + PPO + MSB
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additional high-priority activities, to complement the LBNF liquid argon detector, unifying the global long-baseline neutrino community to take full advantage of the world’s highest intensity neutrino beam. The placement of the water and liquid argon detectors would be optimized for complementarity. This approach would be an excellent example of global cooperation and planning” – P5 (scenario C)
http://underground.physics. berkeley.edu/WbLS/slides/
UCLA, U. Hawaii
0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08 0.09 0.1 200 300 400 500 600 Absorption Length (1/m) Wavelength (nm)
WbLS-2014 (extinction coefficient) WbLS-2012 SK-water
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purification
material
cost and labor-consuming
to measure its effect
component (successfully predict LS)
flour/shifter; need to be optimized
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WbLS non-purified
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loading
transmission
and LS% (up to ~15%)
scintillator
than WbLS-2012
16
1 10 100 1000 0.1 1 10 100
Compton Edge, AU
LS % in Water
WbLS 2014 WbLS 2012
1 10 100 1000 10000 1 10 100 1000 Counts (AU) ADC Channels
WbLS 1% WbLS 4.7% WbLS 8.14% WbLS 10.1% WbLS 13.9% LS H2O WbLS 1% (NSRL 2012)
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0.01 0.02 0.03 0.04 0.05 200 400 600 800 Abs Wavelength (nm)
3/7/2014 3/13/2014 3/24/2014 3/31/2014
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Atomic force microscopy (AFM) high-resolution scanning (acrylic in EtOH) 0.5 1 1.5 750 1750 2750 3750 AU Wavelength (nm)
1 5 4 2
FT-IR Microscope (acrylic in EtOH)
BNL-NSLS
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extensive studies by environmental researches in academia and industry
inhibits bacteria growth
for 2+ years for WbLS-2012 and 6 months for WbLS-2014
circulation if careful selection of vessel and material-in-contact
circulation (e.g. SNO+, PROSPECT)
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Common features between detectors unique requirement for individual detector
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SNO+
WbLS (90%+) doped with 3%Te (130) 0ββ isotope
PROSPECT
WbLS (70%+) doped with 0.1% Gd or 6Li with high PSD
WATCHMAN
WbLS (1%) doped with 0.1%Gd
T2K
WbLS (10%)
Medical Applications
WbLS (1-5%) for QA phantom or doped with high Z element (~10%) for TOF-PET
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the current developments focus on ongoing and newly proposed experiments (every detector has different requirements); 1-ton prototype is under construction
cosmogenic background for solar neutrino and other rare-event Physics
limited for water or scintillator detectors
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