thgem report
DESCRIPTION
THGEM report. Second part: starting since Mai; first part includes the period between January 2008 - April 2008. Elena Rocco. Induction and Drift scans summary for THGEM without rim. INDUCTION SCAN. DRIFT SCAN. ∆V=1.475 KV. ∆V=1.475 KV. ∆V=1.45 KV. ∆V=1.45 KV. ∆V=1.35 KV. ∆V=1.35 KV. - PowerPoint PPT PresentationTRANSCRIPT
THGEM report
Second part: starting since Mai;first part includes the period between January 2008 - April 2008.
1Elena Rocco
Induction and Drift scans summary for THGEM without rim
The fields conditions are the same for all measurements*: Einduction=3 KV/cm, Edrift=1.5KV/cm and e collimated X-Ray source (diam=1mm) has been used
with a rate about 1.7 KHz/mm2.
*for the treated THGEM the Edrift was 2 KV/cm .2
0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5
200
300
400
500
600
700
800
900
1000
1100
1200
1300
1400
Gai
n
Drift Field (KV/ cm)
THGEM 0 mm rim THGEM electro chem. polished Kapton THGEM
DRIFT SCAN
∆V=1.45 KV
∆V=1.475 KV
∆V=1.35 KV
1.0 1.5 2.0 2.5 3.0 3.5 4.0
200
400
600
800
1000
1200
1400
1600
1800
Gain
Induction Field (KV/ cm)
THGEM 0 mm rim THGEM electro chem. polished Kapton THGEM
INDUCTION SCAN
∆V=1.475 KV
∆V=1.45 KV
∆V=1.35 KV
Gain overview
33
1.3 1.4 1.5 1.6 1.7 1.8100
1000
Einduction
=3.5 KV/cm, Edrift
=1.5 KV/cm
Gain
Delta V (KV)
THGEM electro chem. polished THGEM 0 mm rim THGEM with 0.1 mm of rim THGEM made of kapton
∆V=1.35 KV, G~300
∆V=1.325 KV, G~205
∆V=1.3 KV, G~145
∆V=1.675 KV, G~860
∆V=1.725 KV, G~1880
∆V=1.7 KV, G~1350
∆V=1.75 KV, G~2800
∆V=1.775 KV, G~4170
∆V=1.8 KV, G~5580
∆V=1.375 KV, G~220
∆V=1.475 KV, G~1550
∆V=1.5 KV, G~2500
∆V=1.49 KV, G~2060
∆V=1.475 KV, G~1510
∆V=1.4 KV, G~390
∆V=1.45 KV, G~940
∆V=1.44 KV, G~790∆V=1.425 KV, G~600
∆V=1.415 KV, G~490
∆V=1.465 KV, G~1250
The gain of the electro-chem. polished THGEM is overlapped by the gain of the kapton THGEM
(Except for the THGEM with the asymm. rim)
Time stability measurements
4
0 2 4 6 8 10 12 14 16 18
0
2000
4000
6000
Gain
Time (hours)
THGEM 0 mm rim THGEM with 0.1 mm of rim THGEM with asymm. rim; rim (0.1 mm) face to the anode THGEM electro chem. polished
∆V=1.49 KV
∆V=1.775 KV
∆V=1.45 KV∆V=1.35 KV
Same working conditions: Einduction=3.5 KV/cm Edrift=1.5KV/cm; rate ~0.7-0.8 KHz collimated source
Remarks: the drift field is not optimized for these meas.
More about the THGEM in Kapton
Material structure;
Drift scan measuring the currents on all the electrodes.
5
Description of the structure of the THGEM made of Kapton
LF 110, Dupont 50 μm
LF 110, Dupont 50 μm
Copper
Polyimide: Apical, AV, Kareka
Kapton H, Dupont
Sheldhall G2300 17/50*
Sheldhall G2500 17/50*
LF 111, Dupont
*17/50 means 17 μm of copper and 50 μm of kapton
Epoxy acrylic
6
Section 1 Section 4
Directions of the cross sections
Drift scan measuring the currents on the THGEM made of Kapton
0.0 0.5 1.0 1.5 2.0 2.5 3.0
-30
-25
-20
-15
-10
-5
0
5
10
15
20
25
30
THGEm in Kapton; Einduction
=3.5 KV/ cm,Delta V=1.45 KV. High rate (> 100 KHz) collimator of 3mm of diameter.
Cu
rren
t (n
A)
Drift Field (KV/ cm)
Current on the Anode Current on the Bottom Current on the Top Current on the Drift
0.0 0.5 1.0 1.5 2.0 2.5 3.0
-30
-25
-20
-15
-10
-5
0
5
10
15
20
25
30
THGEm in Kapton; Einduction
=3.5 KV/ cm,Delta V=1.45 KV. High rate (> 100 KHz) collimator of 3mm of diameter.
Cu
rren
t (n
A)
Drift Field (KV/ cm)
Electrons Current Ions Current Currents Sum
THGEM
DRIFT
ANODE
6.5 mm
5mm Bottom side
Top side
Configuration inside the chamber
7
Currents measured on all the electrodes (anode, bottom THGEM, top THGEM, drift). The sensitivity for each devices used to read out the current is ± 1nA.
New systematic studies
8
1 2 3
4 5 6
7 8 9
d=0.5mm
d=0.5mm
d=0.5mm
d=0.4mm
d=0.4mm
d=0.4mm
d=0.3mm
d=0.3mm
d=0.3mm
p=0.9mm
p=0.8mm
p=0.7mm
p=0.6mm
p=0.7mm
p=0.8mm
p=0.6mm
p=0.7mm
p=0.5mm
Fixed diameter,Varying the difference pitch&diameter
Fig.2 .THGEMs labelling. Fig.3 .THGEMs geometry for fixed thickness and cleaning.In the increasing diameter direction there’s a
correspondent increasing of the breakdown voltage
The THGEM scheme on the “plaque”
9
Some pictures for looking in details the hole edges
G10_1_sideA
G10_1_sideB
G10_G_sideA
G10_G_sideB
10
Measurements planned and characterization procedure
Characterisation procedure:
1. Kept in the oven for 24h;2. Measurements of the maximum
voltage applied to the THGEM in Ar/CO2 (70/30);
3. Switching on voltage and setup of the electronics setting irradiating the chamber;
4. Time stability measurement for a night (~12 h);
5. Quick characterisation: induction & drift scans, voltage scans, currents measurements (for gain estimation too).
1 2 3
4 5 6
7 8 9
directions of THGEMs characterization
Rim constant: d=0.3 mm
Pitc
h co
nsta
nt: p
=0.7
mm
Voltage conditions: the idea is to keep the same voltage for all THGEMs.
11
G10 – sample #2
12
THGEM
DRIFT
ANODE
Thickness
6.5 mm
5mm
PARAMETERS:• Diameter = 0.3 mm• Pitch= 0.6 mm• Thickness = 0.6 mm• Rim = 0 mm• Gas: Ar/CO2 – 70/30
GEOMETRICAL CONFIGURATION
Side A Side B
Induction Scan
13
0 2 4500
600
700
800
900
1000
1100
1200
Peak Position Energy Resolution
Induction Field (KV/ Cm)
Peak
Pos
itio
n (
AD
C c
h.-
Ped.
Su
btr.
)
20
22
24
26
28
30
En
ergy Resolu
tion (%
)
∆V=1.77 KV collimated source rate~1.6 KHz/mm2
1 2 3 4500
600
700
800
900
1000
1100
1200
Pulse Height Current Measured
Induction Field (KV/ cm)Pe
ak P
osit
ion
(A
DC
ch
. -
Ped.
Su
btr.
)
12
14
16
18
20
22
24
26
28
30
Cu
rrent (n
A)
Comparison between the pulse height measurement and the current measurement*
*For current measurement I used different rate
Same curve
Drift field not optimized ED=1.5 KV/cm Drift field optimized ED=1.5 KV/cm
Drift scans
14
0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5400
500
600
700
800
900
1000
1100
1200
1300
1400
Pea
k P
osit
ion
(A
DC
ch
.- P
ed.
Su
btr
.)
Drift Field (KV/ cm)
Einduction
=3 KV/ cm E
induction=3.5 KV/ cm
Einduction
=4 KV/ cm
0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5
20
25
30
35
40
45
50
En
ergy
Res
olu
tion
(%
)
Drift Field (KV/ cm)
Einduction
=3 KV/ cm E
induction=3.5 KV/ cm
Einduction
=4 KV/ cm
∆V=1.77 KV collimated source rate~1.6 KHz/mm2
0 1 2 3400
500
600
700
800
900
1000
1100
1200
Pulse Height Current measured
Drift Field (KV/ cm)
Pea
k P
osit
ion
(A
DC
ch
.- P
ed S
ubtr
.)
18
20
22
24
26
Cu
rrent (n
A)Comparison between
the pulse height measurement and the current measurement*
Same curve
*For current measurement I used different rate
∆V=1.77 KV collimated source rate~1.6 KHz/mm2
Gain estimation from current measurement
15
REMARKS: @ the same voltage there’s almost the same gain but different geometry!!!
1.3 1.4 1.5 1.6 1.7 1.8100
1000
Gain
Delta V (KV)
THGEM electro-chem. polished without rim THGEM without rim THGEM with rim=0.1mm THGEM made of kapton THGEM with different geometry
1.66 1.68 1.70 1.72 1.74 1.76 1.78
1000
Collimated source 1 mm of diameter,E
induction=3.5 KV/ cm and E
drift=1 KV/ cm (optimized).
Gain
Delta V (KV)
Gain
∆V=1.675 KV G~620
∆V=1.77 KV G~3420
Currents behaviour
16
0.0 0.5 1.0 1.5 2.0 2.5 3.0
-30
-20
-10
0
10
20
30
40
Cu
rren
t (n
A)
Drift Field (KV/ cm)
Anode Current Bottom THGEM Current Top THGEM Current Drift Current
Drift Scan
1.0 1.5 2.0 2.5 3.0 3.5 4.0-40
-30
-20
-10
0
10
20
30
40
Cu
rren
t (n
A)
Induction Filed (KV/ cm)
Anode Current Bottom THGEM Current Top THGEM Current Drift Current
Induction Scan
Time Stability Measurement
17
0 2 4 6 8 10 12 14 16 18 20 22 24
1200
1500
1800
2100
2400
2700
3000
3300
3600
3900
4200
4500
4800
Gain
Time (hours)
Energy Spectrum
V=1.77KV, Einduction=3.5 KV/cm, Edrift=1.5 KV/cm (not optimized), rate=0.8 KHz, collimated source
Problems with the fit due to the low statistics for the first quick acquisition
0 500 1000 1500 2000-10
0
10
20
30
40
50
60
70Data: RUN1200_BModel: Gauss Chi^2/DoF = 7.64017R^2 = 0.89543 y0 0 ±0xc1 42.06558 ±2.35413w1 32.76208 ±4.74061A1 207.53534 ±25.88851xc2 670.33861 ±7.23481w2 215.11112 ±15.54975A2 1263.27492 ±76.27703xc3 1052.18048 ±1.05339w3 203.21437 ±2.24038A3 7994.77666 ±74.42436
Cou
nts
ADC channels
Energy Spectrum
Good statistics
0 500 1000 1500 2000
0
2
4
6
8
10
12Data: RUN0900_BModel: Gauss Chi^2/DoF = 0.52652R^2 = 0.53932 y0 0 ±0xc 1080.10429 ±2.71053w 222.14204 ±5.42106A 834.39498 ±17.6342
Cou
nts
ADC channels
B Gauss fit of RUN0900_B
Bad statistics