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Applying a SiPM response function to 7608 SiPMs of AHCAL physics prototype
CALICE meeting at Arlington TexasK. Kotera, DESY/Shinshu University
1
CLIC Workshop 2013CLIC Workshop 2013
new
15th September. 2016
2
Contents
1. Brief introduction to the response function using ScECAL case: up date version of Munich,
2. Applying to AHCAL SiPMs,
3
Motivation: Linear response after saturation
incident p.e.0 5000 10000 15000 20000
fired
pix
els
0
500
1000
1500
2000
tquenchPfourtquenchPfour
Often we see like red curve w/ fast recovery SiPMs
?
:the number of fired pixels,:photon detection efficiency (PDE),:the number of incident photons,:the number of pixels.
Equation plot of 1600 pixel SiPM, not data not completely saturating
conventional function
photonWe think this comes from reactivation of pixels in a few nano seconds after fired.
=LON
fire
= Npix
⇣1� e�✏N
in
/Npix
⌘
4
Motivation: Linear response after saturation
incident p.e.0 5000 10000 15000 20000
fired
pix
els
0
500
1000
1500
2000
tquenchPfourtquenchPfour
Often we see like red curve w/ fast recovery SiPMs
?
:the number of fired pixels,:photon detection efficiency (PDE),:the number of incident photons,:the number of pixels.
Equation plot of 1600 pixel SiPM, not data not completely saturating
conventional function
photonWe think this comes from reactivation of pixels in a few nano seconds after fired.
=LON
fire
= Npix
⇣1� e�✏N
in
/Npix
⌘
Adjustable parameter
Num
ber o
f fire
d pi
xels
d 0
1000
2000
3000
/NDF = 146 / 122χ
du 11± = 2260 effpixN
PMT response (ADC ch)0 50 100 150 200
dFu
nctio
n-da
ta
200−100−
0100200
5
Example of Npixeff (LO’)
PMT response (ADC ch)0 100 200 300 400
(p.e
./AD
C)
dG
radi
ent
10
210
- Calibration for ScECAL physics prototype.- 1600 pix was measured as 2260 pix (Npixeff).
applicable limit
6
Sample DATA (taken by W. Choi in Shinshu 2010)
72 channels of 30th layer of ScECAL prototype 30 layer-Physics proto. 30th layer (72 ch)
PMT
Laser
a. Scintillator, 3x10x45mm3,b. WLS,c. a hole on reflector,d. MPPC 25μm pitch, in 1x1mm2
e. half mirrorf. PMT,g. lens,h, i. polaroid.
LensPolaroid x 2
ScEcal layer
Half mirror
with 1600 pix MPPC
31ps,FWHM
Num
ber o
f fire
d pi
xels
d 0
1000
2000
3000
/NDF = 146 / 122χ
du 11± = 2260 effpixN
PMT response (ADC ch)0 50 100 150 200
dFu
nctio
n-da
ta
200−100−
0100200
7
Example of Npixeff (LO’)
PMT response (ADC ch)0 100 200 300 400
(p.e
./AD
C)
dG
radi
ent
10
210
- Calibration for ScECAL physics prototype.- 1600 pix was measured as 2260 pix (Npixeff).
applicable limit
Num
ber o
f fire
d pi
xels
d 0
1000
2000
3000
/NDF = 146 / 122χ
du 11± = 2260 effpixN
PMT response (ADC ch)0 50 100 150 200
dFu
nctio
n-da
ta
200−100−
0100200
8
Example of Npixeff (LO’)
PMT response (ADC ch)0 100 200 300 400
(p.e
./AD
C)
dG
radi
ent
10
210
- Calibration for ScECAL physics prototype.- 1600 pix was measured as 2260 pix (Npixeff).
applicable limit
linear behav
ior
9
= 1)∈Incident photons (
0 1000 2000 3000 4000 5000
Num
ber o
f fire
d pi
xels
0
1000
2000
3000
4000
5000
incide
nt
fired
not fi
red
Not fire photons can make the next contributions
NR = ✏Nin � LO
NNLOfire = LO + ↵NR
Idea: think which photons can hit a reactivated pixels
10
= 1)∈Incident photons (
0 1000 2000 3000 4000 5000
Num
ber o
f fire
d pi
xels
0
1000
2000
3000
4000
5000
incide
nt
fired
not fi
red
Not fire photons can make the next contributions
NR = ✏Nin � LO
NNLOfire = LO + ↵NR
Idea: think which photons can hit a reactivated pixels
waiting photon
waiting photons
11
= 1)∈Incident photons (
0 1000 2000 3000 4000 5000
Num
ber o
f fire
d pi
xels
0
1000
2000
3000
4000
5000
incide
nt
fired
not fi
red
Not fire photons can make the next contributions
Note: Linear of NR @ high light region̶after enough saturation
NR = ✏Nin � LO
NNLOfire = LO + ↵NR
Idea: think which photons can hit a reactivated pixels
waiting photon
waiting photons
Reason, why we see linear like behavior
12
Fitting with NLON
umbe
r of f
ired
pixe
lsd 0
1000
2000
3000
cable: 3, channel: 9
Npix: 2061.9 +- 8.6
’: 56.6 +- 0.2∈
: 0.0907 +- 0.0005α
/NDF = 28.22χ
PMT response (ADC ch)0 100 200 300 400
dFu
nctio
n-da
ta
200−100−
0100200
Fit region increased
However,Fitting is not enough wellboth- highly saturated region- small fired pixel region
Too simple
Limit of LO’
13
Consider Charge contribution by a photon
= 1)∈Incident photons (
0 1000 2000 3000 4000 5000
Num
ber o
f fire
d pi
xels
0
1000
2000
3000
4000
5000
incide
nt
fired
not fi
red
Not fire photons can make the next contributions
Charge contribution by a photon should be a function of #photon/pix.
NR = ✏Nin � LO
NNLOfire = LO + ↵NR
firednot fired
waiting photons
waiting photon
14
2 4 6 8 10
-1.2
-1.0
-0.8
-0.6
-0.4
-0.2
2 4 6 8 10
-1.2
-1.0
-0.8
-0.6
-0.4
-0.2
pulse shape ~ recovery of a pixel.
�t
V2nd
max
delayed photon
delayed photon comes before complete recharge
V 2nd
max
= 1� e��t/⌧R
Vmax
e�t/⌧R
⌧R = Rquench
Cpixel
charge by the second photon is :as is full charge case,
Q1Q0
Q1 = Q0(1� e��t/⌧R)
Consider Charge contribution by a photon (case multi-photons come)
15
0 2 4 6 8 10
2
4
6
8
10
12photons come from WLS fiber
dn
dt/ e�t/⌧s
2 4 6 8 10
-1.2
-1.0
-0.8
-0.6
-0.4
-0.2
Suppose: we have k photons waiting for...First: we have k candidate ➡ ⌧s/ksecond we have k-1; , then⌧s/(k � 1) ⌧s/(k � 2) · · · ⌧s
j th rate ; ⌧j = ⌧s/(k � j + 1)
Time distribution of photons ̶Charge by jth photon
note: we have photons coming later than .⌧s
D. Jeans arXiv:1511.06528
inverse proportion
16
Number of photons / pixel0 5 10 15
Cha
rge
cont
ribut
ion
/ pho
ton
0
0.2
0.4
0.6
0.8
1 = 0.5sτ/Rτ:
= 1.0sτ/Rτ:
= 2.0sτ/Rτ: Q0
h1 +
kX
j=2
�1� ⇣
⇣ + (k + 1� j)�1
i/k
Q(k)/k =
curve
h#photon/pixelfiredi = hki = ✏Nin
LO
h#photon/pixelfiredi = hki
Plot of Q(k)/k
=� + 1
� + k
NNLO0
fire = NNLOfire
� + 1
� + ✏Nin/LO
Num
ber o
f fire
d pi
xels
d 0
1000
2000
3000
4000
cable: 3, channel: 9 Npix: 1600.0 +- 0.0’: 61.5 +- 0.2∈ : 0.224 +- 0.003α : 17.7 +- 0.4β /NDF = 4.72χ
Fitting limit of LO’
PMT response (ADC ch)0 100 200 300 400
dFu
nctio
n-da
ta
100−
0100
17
Fitting with NLO’
Npix was fixed @ 1600only one additional free parameters to LO’
If Npix was free:= 1583±29
(72 sample)
high saturated region
small light region- modified
- good agreement
NNLO0
fire = NNLOfire
� + 1
� + ✏Nin/LO
hNpix
i
Num
ber o
f fire
d pi
xels
d 0
1000
2000
3000
4000
cable: 3, channel: 9 Npix: 1600.0 +- 0.0’: 56.8 +- 6.1∈ : 0.288 +- 0.015α : 12.8 +- 1.0β
cross talk ratio: 0.19 +- 0.08 after pulse ratio: -0.032 +- 0.04
/NDF = 2.52χ
Fitting limit of LO’
PMT response (ADC ch)0 100 200 300 400
dFu
nctio
n-da
ta
100−
0100
18
Considering Xtalk and After pulse
Npix was fixed @ 1600
NLO0C.A = NLO0 ⇥ (1 + PCe
�✏Nin
/Npix)(1 + PA)
<PC> = 0.22±0.02<PC>direct = 0.11±0.02
<PA> = 0.08±0.02<PA>direct = 0.1
High crosstalk ratio requires additional knowledge.
19
χ2/NDF
most channel < 10for both NLO’ NLO’C.A
NLO0C.A = NLO0 ⇥ (1 + PCe
�✏Nin
/Npix)(1 + PA)
/NDF2χ0 10 20 30 40 50
Entries
0
10
20
30
: w/ after pulse, crosstalk
: w/o after pulse, crosstalk
: w/ after pulse, crosstalk
: w/o after pulse, crosstalk
NLO0C.A
NLO0
NLO’ NLO’C.A
<χ2/q> 9.4±9.0(RMS) 6.9±7.9(RMS)
Uncertainty of each data point is statistical one.
Num
ber o
f fire
d pi
xels
d 0
500
1000
1500
2000
cable: 1, channel: 1 Npix: 1600.0 +- 0.0’: 71.6 +- 3.8∈ : 0.240 +- 0.021α : 6.9 +- 0.6β
cross talk ratio: 0.264 +- 0.04 after pulse ratio: -0.185 +- 0.02
/NDF = 13.82χ
PMT response (ADC ch)0 100 200 300 400
dFu
nctio
n-da
ta
100−
0100
20
Fast pulse inputNLO0
C.A = NLO0 ⇥ (1 + PCe�✏N
in
/Npix)(1 + PA): applied to scinti-MPPC w/o WLS fiber
WLS fiberWLS fiberw/ w/o
α 0.30 0.24
β 12 6.9
α: large small
smallβ: large
recovery
pulse width/recov.time
21
Applying to 7608 SiPM data of AHCAL physics prototype
ITEP SiPM 1156 pixels/(1.1×1.1mm2) Recovery time: 20ns (from CALICE JINST 5 P05004),LED UV light via Y11 WLS, at dV = 2V,Xtalk : < 35%, MPV~22%,
LED
SiPMs
WLS fibers
naked SiPM w/o scintillator
from CALICEJINST 5 P05004
22
Motivation
23
MotivationFelix’s (Eva Sicking’s) talked at LCWS Whistler: W-AHCAL
Rather artificial linear extrapolation
Num
ber o
f fire
d pi
xels
d 0200400600800
10001200
nch: 7301, SiPM: 23204 Npix: 1156.0 +- 0.0’: 2.8 +- 0.1∈ : 1.101 +- 0.006α : 5.4 +- 0.1β
cross talk ratio: 0.21 +- 0.00 after pulse ratio: 0.000 +- 0.00
/NDF = 6.32χ
Fitting limit of LO’
PMT response (ADC ch)0 500 1000 1500 2000 2500
dD
iff./f
unc.
0.02−0.01−
00.010.02
# photons in
1156N
umbe
r of f
ired
pixe
lsd 0
200400600800
10001200
nch: 7200, SiPM: 30756 Npix: 1156.0 +- 0.0’: 1.3 +- 0.0∈ : 0.685 +- 0.024α : 2.9 +- 0.1β
cross talk ratio: 0.17 +- 0.00 after pulse ratio: 0.000 +- 0.00
/NDF = 0.12χ
Fitting limit of LO’
PMT response (ADC ch)0 500 1000 1500 2000 2500
dD
iff./f
unc.
0.02−0.01−
00.010.02
24
ITEP SiPM in AHCAL physics prototypefitting example/7608, various fired/in
(# photons in: normalized at small number of fired pixels)
1156
Npix: fixed at 1156
Fitting: 7608 samples takes ~22min(0.17sec/ch)➡ light function
# photons in
Num
ber o
f fire
d pi
xels
d 0
200
400
600
800
nch: 7600, SiPM: 21222 Npix: 1156.0 +- 0.0’: 1.3 +- 0.0∈ : 0.456 +- 0.009α : 2.5 +- 0.1β
cross talk ratio: 0.17 +- 0.00 after pulse ratio: 0.000 +- 0.00
/NDF = 2.42χ
Fitting limit of LO’
PMT response (ADC ch)0 500 1000 1500 2000 2500
dD
iff./f
unc.
0.02−0.01−
00.010.02
# photons in
25
ITEP SiPM in AHCAL physics prototype some parameters
0 5 10 15 200
500
1000
1500
2000
redchiredchi
0
200
400
600
800
1000scale:aftP
0.5− 0 0.5 10
1
2
3
4
scale:aftP
0.12 0.14 0.16 0.18 0.2 0.22 0.240
500
1000
1500
2000
crosstalk ratiocrosstalk ratio
χ2/NDF < 20 7425ch/7608ch
χ2/NDF crosstalk ratio
mean 0.17 ± 0.01
after pulse ratio
ε
✏ =0.88
1.02 + afterPulse
NLO0C.A = NLO0 ⇥ (1 + PCe
�✏Nin
/Npix)(1 + PA)
in our simple model, P_afterpulse is a scale factor in N_fired (no effect on shape).
negative peak (-0.28) indicates some systematics.
:
26
ITEP SiPM in AHCAL physics prototype some parameters
0 5 10 15 200
500
1000
1500
2000
redchiredchi
0
200
400
600
800
1000scale:aftP
0.5− 0 0.5 10
1
2
3
4
scale:aftP
0.12 0.14 0.16 0.18 0.2 0.22 0.240
500
1000
1500
2000
crosstalk ratiocrosstalk ratio
χ2/NDF < 20 7425ch/7608ch
χ2/NDF crosstalk ratio
mean 0.17 ± 0.01
after pulse ratio
ε
✏ =0.88
1.02 + afterPulse
NLO0C.A = NLO0 ⇥ (1 + PCe
�✏Nin
/Npix)(1 + PA)
in our simple model, P_afterpulse is a scale factor in N_fired (no effect on shape).
negative peak (-0.28) indicates some systematics.
:Our function works well for also ITEP SiPMs in AHCAL
27
α vs. β
020406080100120140160180200220
0 0.2 0.4 0.6 0.8 1 1.20
5
10
15alpha:beta {alpha<15}alpha:beta {alpha<15}
β
α
α and β have a relation with each other.However, a clear peak indicates that those both have meanings of existences respectively.
NNLOfire = LO + ↵NR
NNLO0
fire = NNLOfire
� + 1
� + ✏Nin/LO
LO = Npix
⇣1� e�✏N
in
/Npix
⌘
28
crosstalk ratio vs. β
020406080100120140160180200220
0 0.2 0.4 0.6 0.8 1 1.20
5
10
15alpha:beta {alpha<15}alpha:beta {alpha<15}
β
α
020406080100120140
0 0.5 10.14
0.16
0.18
0.2xtalk:beta {0.14<xtalk&&xtalk<0.2}xtalk:beta {0.14<xtalk&&xtalk<0.2}
β
cros
stalk ratio
- Correlation between cross-talk ratio and β has a clear peak and no clear correlation (only small amount of large β has correlation.
- without crosstalk correction, fitting results are very much degrading
β and crosstalk individually affect on the shape of function
Three parameters α,β,and crasstalk ratio are individually required.
29
Summary- We developed functions having high performance to represent SiPM behavior in wide ranges.
- Light function (0.17sec/fit).- The function models reactivating pixels in a event more carefully than taking the number of effective pixels;•the number of photons fire reactivated pixels,•charge contribution par one photon is implemented by an approximation of the first principle method.
- Crosstalk and after pulse models improves fitting performance, whereas it did not work with LO’(Npixeff).
- The function successfully worked on 7608 SiPM for AHCAL physics prototype.
Next- Understand detail effects of individual parameters.- Usage in calibration procedure.
30
Backup
31
0 2 4 6 8 10
2
4
6
8
10
12photons come from WLS fiber
dn
dt/ e�t/⌧s
2 4 6 8 10
-1.2
-1.0
-0.8
-0.6
-0.4
-0.2
Suppose: we have k photons waiting for...First: we have k candidate ➡ ⌧s/ksecond we have k-1; , then⌧s/(k � 1) ⌧s/(k � 2) · · · ⌧s
j th rate ; ⌧j = ⌧s/(k � j + 1)
Time distribution of photons ̶Charge by jth photon
note: we have photons coming later than .⌧s
Incorrect: no effect in .⌧s < ⌧R
by D. Jeans
32
charge by the jth photon
Qj = Q0
Z 1
0dt
1
⌧je�t/⌧j (1� e�t/⌧R)
⌧j = ⌧s/(k � j + 1)
= Q0
⇣1� ⌧R
⌧R + ⌧j
⌘
= Q0
⇣1� ⇣
⇣ + (k � j + 1)�1
⌘
⇣ = ⌧R/⌧scharge by ks photons
Q(k) = Q0
n
1 +k
X
j=2
⇣
1� ⇣
⇣ + (k � j � 1)�1
⌘o
Charge by ks photons on a cell
D. Jeans arXiv:1511.06528
33
Hamamatsu MPPC (2008)Hamamatsu MPPC: corresponding to S10362-11-25P1600pixels/(1×1mm2) Recovery time: 4ns,at dV = 3V,crosstalk : 11% measured in lab,after pulse : 10% from some references.
408nm 31ps (FWHM) Laser via Scintillator + Y11 WLS, Y11 decay time: 11ns
34
Purpose of developing functions
Practical usage in experiments using SiPMs in wide range of number of photons,
based on much reasonable̶detail̶model of SiPM phenomena than current others.
- detector calibration,- simulation of detector responses
35
DataCALICE DATA base we can access it using CaliceSoft.
each data (7608) has:one SiPM ID20 data of # photons injected,20 data of fired pixels corresponding,no uncertainty information.
- Wrote a processor to read and create a TTree.
Applying our function to # of fired pix. as a function of # of photons injected.
Num
ber o
f fire
d pi
xels
d 0
200
400
600
800
nch: 7600, SiPM: 21222 Npix: 1156.0 +- 0.0’: 1.8 +- 0.1∈ : 0.616 +- 0.179α : 2.4 +- 0.8β
cross talk ratio: 0.08 +- 0.07 after pulse ratio: -0.491 +- 0.05
/NDF = 0.02χ
Fitting limit of LO’
PMT response (ADC ch)0 500 1000 1500 2000 2500
dD
iff./f
unc.
0.05−
00.05
36
Some example of fittingN
umbe
r of f
ired
pixe
lsd 0
200400600800
10001200
nch: 7200, SiPM: 30756 Npix: 1156.0 +- 0.0’: 1.3 +- 0.1∈ : 0.504 +- 0.139α : 4.7 +- 1.7β
cross talk ratio: 0.08 +- 0.04 after pulse ratio: -0.294 +- 0.07
/NDF = 0.02χ
Fitting limit of LO’
PMT response (ADC ch)0 500 1000 1500 2000 2500
dD
iff./f
unc.
0.05−
00.05
Num
ber o
f fire
d pi
xels
d 0200400600800
100012001400
nch: 7300, SiPM: 21156 Npix: 1156.0 +- 0.0’: 2.0 +- 0.2∈ : 1.025 +- 0.038α : 4.2 +- 0.7β
cross talk ratio: 0.19 +- 0.03 after pulse ratio: -0.584 +- 0.03
/NDF = 0.02χ
Fitting limit of LO’
PMT response (ADC ch)0 500 1000 1500 2000 2500
dD
iff./f
unc.
0.05−
00.05
Fine fitting result.Too large error estimation :(
net # of pix. 1156net # of pix. 1156
# photon arrived?
# photon arrived?
# photon arrived?
Each error #photons × 0.01
Evaluation of fitting (good)
37
0 0.5 1 1.5 2 2.5 30
200
400
600
800
1000’∈’∈
#photon arrived was already normalized at small p.e. response. (linear pixels? )
~1
PMT, PDE scale factor: ✏example
38
Error estimation trial (sqrt)N
umbe
r of f
ired
pixe
lsd 0
200400600800
10001200
nch: 7200, SiPM: 30756 Npix: 1156.0 +- 0.0’: 1.1 +- 0.0∈ : 0.461 +- 0.006α : 4.7 +- 0.1β
cross talk ratio: 0.12 +- 0.00 after pulse ratio: -0.221 +- 0.01
/NDF = 4.12χ
Fitting limit of LO’
PMT response (ADC ch)0 500 1000 1500 2000 2500
dD
iff./f
unc.
0.02−0.01−
00.010.02
net # of pix. 1156net # of pix. 1156
Error = √(N_fired) × 0.01
- a bit reasonable error- S structure .... 0 5 10 15 20
0
500
1000
1500
2000
redchiredchi
0 0.01 0.02 0.03 0.040
1000
2000
3000
redchiredchiχ2/ndf
χ2/ndf
rea
sona
ble
適当
Parameters with error∝√(#photon)
39
0 0.5 1 1.5 2 2.5 30
500
1000
1500
’∈’∈
0 0.5 1 1.5 2 2.5 30
200
400
600
800
1000’∈’∈
0 0.5 1 1.5 20
200
400
600
αα
0 5 10 15 200
200
400
600
800
1000
1200ββ
0 0.5 1 1.5 20
200
400
600
800
1000
αα
0 5 10 15 200
200
400
600
800
ββ
Error = sqrt(N_fired) × 0.01 makes parameter distributions to be narrower ➡ better estimation
εPMT, PDE scale factor αRecovery parameter β# photons/cell effect
√(#photon)× 0.01 or 0.005?
40
0 5 10 15 20
200
400
600
800
1000
1200
1400redchiredchi
0 5 10 15 200
500
1000
1500
2000
redchiredchiχ2/NDF with × 0.01 χ2/NDF with × 0.005
Too small error estimation makes fits.
χ2/NDF < 20: 7178channels χ2/NDF < 20: 4918ch
Num
ber o
f fire
d pi
xels
d 0200400600800
10001200
nch: 7200, SiPM: 30756 Npix: 798.0 +- 15.1’: 0.8 +- 0.0∈ : 0.727 +- 0.017α : 2.6 +- 0.0β
cross talk ratio: 0.22 +- 0.00 after pulse ratio: 0.000 +- 0.00
/NDF = 0.22χ
Fitting limit of LO’
PMT response (ADC ch)0 500 1000 1500 2000 2500
dD
iff./f
unc.
0.02−0.01−
00.010.02
Example of fitting results
41
Num
ber o
f fire
d pi
xels
d 0200400600800
10001200
nch: 7200, SiPM: 30756 Npix: 1156.0 +- 0.0’: 1.1 +- 0.0∈ : 0.461 +- 0.006α : 4.7 +- 0.1β
cross talk ratio: 0.12 +- 0.00 after pulse ratio: -0.221 +- 0.01
/NDF = 4.12χ
Fitting limit of LO’
PMT response (ADC ch)0 500 1000 1500 2000 2500
dD
iff./f
unc.
0.02−0.01−
00.010.02
net # of pix. net # of pix. net # of pix.
Current best fitting
apply to calibration?Next step
Fixed Npix at 1156
Free Npix
42
Motivation: Linear response after saturation
incident p.e.0 5000 10000 15000 20000
fired
pix
els
0
500
1000
1500
2000
tquenchPfourtquenchPfour ?
:the number of fired pixels,:scale factor of horizontal direction,:the number of incident photons,:the number of pixels.
Equation plot of 1600 pixel SiPM, not data not completely saturating
conventional function
photonWe think this comes from reactivation of pixels in a few nano seconds after fired.
To date, we take
for such a case.
Often we see like red courve especially w/ MPPC
43
Motivation: Linear response after saturation
incident p.e.0 5000 10000 15000 20000
fired
pix
els
0
500
1000
1500
2000
tquenchPfourtquenchPfour
Often we see like red courve especially w/ MPPC
?
:the number of fired pixels,:photon detection efficiency (PDE),:the number of incident photons,:the number of pixels.
Equation plot of 1600 pixel SiPM, not data not completely saturating
conventional function
photonWe think this comes from reactivation of pixels in a few nano seconds after fired.
=LO
44
Sample DATA (taken by W. Choi in Shinshu 2010)
72 channels of 30th layer of ScECAL prototype 30 layer-Physics proto. 30th layer (72 ch)
PMT
Laser
a. Scintillator, 3x10x45mm3,b. WLS,c. a hole on reflector,d. MPPC 25μm pitch, in 1x1mm2
e. half mirrorf. PMT,g. lens,h, i. polaroid.
LensPolaroid x 2
ScEcal layer
Half mirror
with 1600 pix MPPC
31ps,FWHM
45
Some remind of ScECAL response curve
Hamamatsu MPPC1600pixels/(1×1mm2) Recovery time: 4ns,408nm 31ps Laser via Scintillator + Y11 WLS, at dV = 3V,crosstalk : 11% measured in lab,after pulse : 10% from some references.
46
Contents
1. Brief introduction to the response function using ScECAL case,
2. Applying to AHCAL data,
3. Discussion on parameters and fitting conditions.