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The Scintillator ECAL Beam Test at FNAL
K. Kotera, Shinshu-u, 1st October 2009CALICE Scintillator ECAL group;
Kobe University, Kyungpook University, the University of Tsukuba,
1
Requirements for ILD Electromagnetic calorimeter
• performance• from a standpoint of particle flow
algorithm for the jet energy resolution• energy resolution• linearity• uniformity• granularity
• Robustness• Low cost• Magnetic field tolerance
5x5~10x10 mm2
(~1%) (~15%)
2
Requirements for ILD Electromagnetic calorimeter
• performance• from a standpoint of particle flow
algorithm for the jet energy resolution• energy resolution• linearity• uniformity• granularity
• Robustness• Low cost• Magnetic field tolerance
Strip scintillator/PPD
Wave length shift fiber
Strip scintillator/PPD
2
Our challengeMPPC
WLS fiber
Kyungpook National University (Korea)
Extrude method→low cost, it can make hole for WLS fiber simultaneously
4 mm
3 m
m
Hamamatsu 1600 pixel 1 x 1 mm PPD
= MPPC in Plastic package
• plastic scintillator 10mm x 45 mm x 3mm
• 1mmΦ WLS fiber
3
First prototype1- 6 GeV e+ beam @ DESY 2007
9 cm
9 c
m26 layer = 18.5 X0
Nice linearity for 1 - 6 GeV
0.2
4
First prototype1- 6 GeV e+ beam @ DESY 2007
9 cm
9 c
m26 layer = 18.5 X0
Nice linearity for 1 - 6 GeV
σ/E
00.2
0.1
0.7 0.70 1/√E(GeV)
4
σstoch ~ 14%, :-)σconst = 2.0% w/high unif.
still larger than 1%,by leakage?
low unif. strips
First prototype
9 cm
9 c
m26 layer = 18.5 X0
Nice linearity for 1 - 6 GeV
Uniform region
σ/E
00.2
0.1
0.7 0.70 1/√E(GeV)σstoch ~ 14%, :-)σconst = 2.0% w/high unif.
still larger than 1%,by leakage?
Beam position
Sensitivity of low unif.
strips
beam
beam
Uniform region
Central region 4
1- 6 GeV e+ beam @ DESY 2007
low unif. strips
First prototype
9 cm
9 c
m26 layer = 18.5 X0
Nice linearity for 1 - 6 GeV
high unif.strips
Uniform region
σ/E
00.2
0.1
0.7 0.70 1/√E(GeV)
Central region
low unif. strips
large σconst by non-unif strips
low unif. strips
Beam position
Sensitivity of low unif.
strips
beam
beam
Uniform region
Central region 4
σstoch ~ 14%, :-)σconst = 2.0% w/high unif.
still larger than 1%,by leakage?
1- 6 GeV e+ beam @ DESY 2007
30 layer21.3 X0
18x4 strips
18 cm
18 c
m
w/ Modified uniformity of response of strips
2160 channel
5
2nd prototype,
2nd prototype, tested at FNAL, Sep 2008 and May 2009
• Study of performance combinedwith AScHCAL and T-Cacher,
• First comprehensive study of performance of ScECAL,
• Linearity of energy response for 1- 32 GeV,
• Energy resolution for 1 - 32 GeV,
• Effect of incident angle of particles,
• Position dependence of response.
• Observation of π0 events - separation 2γ
• Establish LED gain monitoring system
30 layer21.3 X0
18x4 strips
18 cm
18 c
m
w/ Modified uniformity of response of strips
2160 channel
5
pu
rpose
2nd prototype of ScECAL9 MPPCs on a flat cable
In front of AHCAL
Hole to inlet LED light for Gain monitoring
Holding W absorber (3.5 mmT) behind the strip scintillators
6
18 x 4 strips
2nd prototype of ScECAL
Holding W absorber behind the strip scintillators
9 MPPCs on a flat cable
In front of AHCAL
- LED lights are distributed by clear fibers,then fibers distribute the light through notches on them. - MPPC can separate peaks of p.e.
Distance between them gives us absolute gain of MPPC.
- a clear fiber lying along the holes
cover sheet
7
MPPC saturation correctionFor each event of each channel, MPPC saturation correction was made.
1 3 6 12 16 25 32 GeV
Electron energy spectra
PMT response
new value of response
≈≈ççPMT response
2 4 6 4 8 10 1214 16 18 20x10 (ADC)
0
4
8
12
14 x102 (ADC)
Fitting result
# of photons from each channel
MPPC
resp
on
se
8
Bench test using 400 nm psLaser pulse
Reverse function of fitting result of this function was used to make saturation correction
Output of correction
Input for correction
result of fitting:
Calibration of each strip scintillator channel
- We use muon beam runs made with iron shutter put upstream of exp site.
A typical MIP (muon) event in the online monitor
ADC count distribution of MIP event for a channel.( 1st layer, 46th channel )
x102
Cou
nts
5
10
15
x 10(ADC count)10 12 14 16
9
Event selections and spectra
Selection; - Cerenkov, - Layer having maximum (L_Max) energy in ECAL < 20th, - Energy in L_Max > 10 - 150 MIP depending on beam mom., - Energy in L_Max of HCAL < 20MIP, - Energy in last layer of HCAL < 0.4 MIP, - Abs(gravitational center of energy in x(y) axis of ECAL) < 4 cm.
32 G
eV
Effects of cuts After all cuts
Spectra, before any selection cut but Celenkov ^
^
10
Each cut variation was investigated to make sure that the cut did not induce a bias.
Sep 2008, linearity
good linearity
Calice Preliminary
11
Sep 2008, linearity
good linearity but ...
Calice Preliminary
11
Sep 2008, linearity
Deviation from linear< 6%
Candidates to correct residual deviation; - correct with more detail MPPC saturation correction, - investigate some energy leakage (maybe small), - apply temperature correction,
good linearity but ... not enough
Calice Preliminary
Calice Preliminary
only statistic errors
11
Sep 2008, energy resolution
constant term 1.41±0.02%
stochastic term 15.15±0.03%
Calice Preliminary
Calice Preliminary
only statistic errors
* only statistic errors
13
π0 RunSep.2008,
π- :16,25,32 GeVπ+: 60 GeV(2009)
π 0 peak
- reconstructed mass was well done (Rather small invariant mass than Mπ0 so far ).
Calice Preliminary
14
Summary
• ScECAL group of CALICE made 18 cm x 18 cm 2nd prototype, quad surface of 1st prototype.
• Beam test at FNAL Sep.2008, May 2009,
• Sep.2008 data were analyzed;
• good linearity but need more brash up,
• Constant term of resolution was modified → uniformity was modified (2.7%→1.4%)
• π0 is reconstructed ( still small Mπ0 )
• and more detail anelysis is ongoing
15
extrude
Plan
• Linearity and resolution,
• do temperature correction,
• do more detail study for MPPC saturation,
• remove the influence of pion contamination,
• estimate any systematic uncertainty.
• brash up π0,
• to study the performance of combination with AScHCAL and Tail Catcher.
• to study the influence of incident angle,
• to study the detailed position dependence.
16
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