On-line Actinide Quantification with Extractive Scintillating Resins
Study of Neutrino-Electron Scattering with CsI(Tl) Scintillating Crystal Detector
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Transcript of Study of Neutrino-Electron Scattering with CsI(Tl) Scintillating Crystal Detector
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Study of Neutrino-Electron Scattering with CsI(Tl) Scintillating
Crystal Detector
TEXONO Physics Program on CsI(Tl) Detector
Shielding and CsI(Tl) Detector Design
Data Analysis Techniques
Cut Summary
Background Understanding and Suppression
Status and Plans
Muhammed Deniz1,2
1: METU, Ankara, Turkey2: IoP, Academia Sinica,
Taiwan
On behalf of TEXONO collaboration@ 2006 Workshop on the Underground Experiment –
Extension of KIMS + TEXONO Collaboration
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TEXONO Physics Program on CsI(Tl) detector
Region of Interest for e -ve scattering
CsI(Tl) (186 kg) : attempt a measurement of Standard Model (ee-)
sinw at MeV range
e + e- e + e-
Uncertainties in the low energy part of reactor neutrino for SMeehigher energies (T>2 MeV)
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KS Expt. : Detector Configuration
16 ch, 20 MHz, 8 bit
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10052031237020406
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CsI(Tl) crystal layout (93 cry. 186 kg)
40 cm-target crys.40 cm-veto crys.20+20 cm-veto crys.Plastic
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CsI(Tl) Array : Highlights
Period II Data Volume : Total ~ 110 / 50 days ON/OFF
186 kg mass ; 20+20 and 40 cm length (longest commercial prod.) CsI(Tl) crystals
Detector Threshold: 3 MeV
Energy: total light collection
z-position: the variation of the ratio
Energy & Z-position info:
10% FWHM @ 660 keV
Z-position resolution is
(z) = 2 cm @ 660 keV
(z) <2 cm @ higher energies
RL~ QQE
)/()( RLRL QQQQR
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a) Alpha Event Cut
• having fast decay time
Checking: Alphas are located around 2 MeV
Selection: Mean Time Method: tav vs. q and Double Charge Method: compare total charge with partial charge
Alpha Event Pulse
Normal Event Pulse
Data Analysing Techniques - Defining Cuts
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Narrow Pulse
Normal Pulse
0 cm 40 cm
40 cm long crystal No cut
Definition:
Selection: Both side peak means initially taken as 0 & 40.
Cut: 4 cm from both sides
)21/()21( QQQQZ
b) Z-position Cut:
Data Analysis Techniques - Defining Cuts
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Data Analysis Techniques - Defining Cuts
Veto cut: Reject Cosmic ray Single-hit cut: Anti Compton effectPSD cut : Alpha particleZ-pos cut : Both veto and S.H. effect
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Data Analysis Techniques - Calibration1) Z-POSITION CORRECTION:
BEFORE CORRECTION AFTER CORRECTION
2) SLOPE CORRECTION:
AFTER CORRECTION
BEFORE CORRECTION
3) ENERGY CORRECTION:
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ON spectrum 0.441/day/kg in Period II
OFF spectrum 0.423/day/kg in Period II
* 37 Crystals (40 cm) * Mass 59.2 kg* Basic cuts + Alpha cut + 4 cm Z-cut
ON and OFF Energy Spectra
208Tl (2614keV)
40K (1460 keV)
137Cs (662 keV)
OFF spectrum in all energy range
ON&OFF spectra in 3-8 MeV
energy range
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Two Type :1. Radioactive Contaminants
Decays of radioactive contaminants mainly 232Th and 238U chain produce background in the region of interest.
• Estimate the abundance of 137Cs, 238U and 232Th inside the detector.
• Figure out the contribution of 238U and 232Th chains to the background.
2. Environmental Background
Cosmic Ray muons, Products of cosmic ray muons, Spallation neutrons and some radioactive elements like 60Co, 208Tl• Estimate the background related to cosmic rays due to
inefficiency suppression.• Understand and suppress the contribution of 208Tl to the
background in region of 3-4 MeV.
Background Understanding
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Background Understanding
Radioactive Contaminants– IDEA: By monitoring the timing and position information related β-α
or α-α events can provide distinct signature to identify the decay process and the consistency of the isotopes involved.
Environmental Backgrounds– IDEA: multiple-hit analysis can give us very good understanding
especially Tl-208 and cosmic related background in the region of interest
• cosmic– By comparing cosmic and not-cosmic multiple-hit spectra. – By examining the pair-production phenomena in not-cosmic multiple-hit
spectra.
• Tl-208– By examining multiple-hit spectra as well as simulation of Tl-208 decay
chain energies to understand/suppress background in the region of 3-4 MeV.
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Intrinsic 137Cs Level
137Cs contamination level in CsI was drived ==> (1.55 ± 0.02 ) X 10-17 g/g
31.3 kg-day of CsI(Tl) data was analysed.
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β
α
Data: The total of 40 crystals with data size of 1725 kg·day was analyzed.
i) 214Bi(-)→ 214Po(,164s) → 210Pb
Intrinsic U and Th Contamination Level
T1/2 = (163 ±8) s
238U abundance = 0.82 ± 0.02 x10-12 g/g
iii) 220Rn → 216Po0.15s) → 212Pb
T1/2 = (±s
232Th abundance2.23 ± 0.06 x 10-12 g/g
ii) 212Bi(-,64%) → 212Po(, 299ns) → 208PbSelection: - pulse followed by a large pulseSelection: 1st pulse is shaped &
2nd pulse shaped
Selection: two events with time delay less than 1s
β
α
T1/2 = (± 37 ns.
232Th abundance = 2.3 ± 0.1 x10-12 g/g
• Master Thesis results of Zhu Y. F. from Tsing Hua Univ. in Beijing (2006)
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510
1170 1330
2100 The Sources are external
Background Understanding via Multi Hit
• Co-60 contamination
• 1173.2 keV 99.86% accompanied with 1332.5 keV 99.98%
• Tl Pair Production: One escape peaks
• (~ 2105 + 511 keV)
The source is internal.
2614 keV 99.79 % accompanied with
583 keV 86%
510.8 keV 22.6%
860 keV with 12.4%
Combination of Tl gammas can affect up to around 4 MeV Cosmic induced neutrons can be captured by the target nuclei 133Cs.
The Source is external
600
800
Cs-134 (n + 133Cs 134Cs)
• 97.6% 605 keV;
• 85.5% 796 keV
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Background Understanding – Tl-208 and Cosmic Inefficiency
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Study on Background in Statistically
2&3 Hit Approach for 4 – 8 MeVTwo-Hit:
Expected to Single-Hit ratio:Exp/SH = 0.82 4cm z-cut
= 0.96 for no z-cut
Three-Hit:
Expected to Single-Hit ratio:Exp/SH = 0.98 for 4cm z-cut
= 1.15 for no z-cut
Pair Production Approach for 4 – 8 MeVFor no z-cut
Expected to Single-Hit ratio:
Exp/SH = 1.03
For 4cm z-cut
Expected to Single-Hit ratio:
Exp/SH = 0.90
• To understand the contribution of cosmic rays to the background,
~ 926 kg*day data was analyzed for cosmic and not-cosmic multi-hit as well as pair production.
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○○
There are two kinds of background events within our signal.
• one is matching well with reference -pulse (-)and
• the other is fast- falling ()…
Right side Right sideLeft side Left side
TYPE I TYPE II
2 Analysis
• Black – Recorded Pulse by FADC• Green – Reference pulse • Red - Reference pulse
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2 Analysis
Cutting at this point, suppression 66%(.248/.727)
-square function
Red – events
Black – events
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Preliminary Result of sin2W
g
The best fit of sin2W : 0.37 ± 0.13 at 3-8MeV
0.30 ± 0.22 at 3.5-8MeV
Ph.D. Thesis results of Dr. Lin Shin Ted (2006)
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Expected Accuracy of sin2W with data size
130
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Expected Result of Accuracy of e-e) and sin2W
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Characteristics of the previous and current neutrino-e scattering experiments
CsI(Tl) cry.CsI(Tl) cry.
186 kg186 kg
3.0 3.0
1.8 (expect)1.8 (expect)
0.10.1
<20% (goal<20% (goal)
CF4 gasCF4 gas
21 kg21 kg
0.9 0.9
1.771.77
0.20.2
50%50%
Si(Li)Si(Li)
37.5 kg37.5 kg
0.60.6
5.25.2
0.0080.008
49%49%
FluorocarbonFluorocarbon
103 kg103 kg
3.13.1
0.780.78
0.10.1
53%53%
Plastic scin.Plastic scin.
15.9 kg15.9 kg
1.51.5
1.21.2
0.180.18
29%29%**
TEXONOTEXONONUMUNUMURovnoRovnoKurtchatovKurtchatovSavannahSavannahExperimentsExperiments
TargetTarget
Fiducial MassFiducial Mass
Thr. (MeV)Thr. (MeV)
Signal Evt./DaySignal Evt./Day
S / BS / B
Accuracy ofAccuracy of
((eee)e)
TEXONO and World status !
“Our aim is to measure ((eee) e) with <20% <20% accuracy.”
Our aim is to measure Sin2W value with <8% accuracy.
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Thank you