gem detector shoji uno kek. 2 wire chamber detector for charged tracks popular detector in the...
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![Page 1: GEM Detector Shoji Uno KEK. 2 Wire Chamber Detector for charged tracks Popular detector in the particle physics, like a Belle-CDC Simple structure using](https://reader035.vdocument.in/reader035/viewer/2022062409/56649cff5503460f949d13e7/html5/thumbnails/1.jpg)
GEM Detector
Shoji Uno
KEK
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2
Wire Chamber
• Detector for charged tracks
• Popular detector in the particle physics, like a Belle-CDC
• Simple structure using thin wires
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3
Gas amplification near anode wire• High electric field (>30kV/cm) can be
obtained easily due to using thin wire (diameter ~0.03mm)
• Energy of electron become higher for high electric field near wire.
• Electron can produce another electron for ionization.
• Number of electrons increases due to multi steps of this process.
(gas amplification 、 electric avalanche)
• Gas gain up to ~105 can be obtained easily.
Electron
Anode wire
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Recent gas chamber
• Requirement– High incident rate
• One wire covers wide region.
– Wire spacing > ~1mm
– Length >~10cm
Need more space
– Pure two-dimensional readout
– Wire has some limitation due to straight wire
LHC ATLAS
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Limitation of wire chamber
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New development
• Development MPGD ( Micro Pattern Gas detector)– Gas multiplication in high electric field
with other than wire – 3 types
• MSGC ( Micro Strip Gas Chamber )• MICROMEGAS ( Micromesh Gaseous
Detector )• GEM ( Gas Electron Multiplier )
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GEM (Gas Electron Multiplier)
Hole diameter 70mHole pitch 140mThickness 50mCu thickness 5m
Electric field
Developed by F.Sauli (CERN) in 1997.NIMA 386(1997)531
Double side flexible printed circuit board
GEM foil 50μm Kapton
3μm Cu
3μm Cu
Electrical field
Amplification
electrons
electron
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Flexible shape
Fabio Sauli
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Configuration for GEM detector
Readout
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Multi-layer
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High counting capability
ワイヤーチェンバー GEM
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Application of GEM
• Feature of GEM– Pure two-dimensional readout → Image
– Multi-layer structure
• Stable operation
• Multi-conversion-layer (Neutral Charged)
– High counting capability
• GEM can be applied for many other fields, not only high energy physics.
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TPC
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X-ray detector
X-ray absorption tomography
Crystal structure analysis using X-ray
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Photon sensor
• Same function for photomultiplier
• Usable in Magnetic field
• Fine segmentation in readout
• Cheap and Larger
• Key issue is photo-electric surface in gas volume.
• Under developement
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Basic property of GEM chamber
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Test Chamber
GAS Ar-CH4(90/10) (P-10) Ar-CO2(70/30)
2200pF
2200pF~ 2 mm
10 mm
GEM1
GEM2
GEM3~ 2 mm
~ 2 mm
55Fe (5.9 keV X-ray)
DRIFT
TRANSFER 1
TRANSFER 2
INDUCTIONPCB
36 = 6×6
1mm
□15mm×15mm
PCB
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Pulse shape
Signal from Readout pad
Signal from GEM foil
200ns
130mV
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Effective gas gain and resolution
Ar-CO2
P10
Num
ber
of e
vent
s
Sigma/Mean = 8.8%VGEM=325V
Edrift = 0.5kV/cm Etransfer = 1.6kV/cm Einduction= 3.3kV/cm
55Fe
ADC counts
Pedestal=104.6
Ar-CH4(90/10)
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Gas gain vs various parameters
P10
Ar-CO2
Ar-CO2
Ar-CO2
P10
P10
Ar-CO2
EDEI
ETEI
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ΔVGEM=360VET=1.6kV/cmEI=3.6kV/cm
ΔVGEM=360VET=1.6kV/cmEI=3.6kV/cm
Electric field dependence in drift region55Fe (5.9 keV X-ray)
EDDrift region
ED=3000V/cm
EI=1000V/cm
ED=500V/cm
EI=1000V/cm
In case of weak field In case of strong field
Δ VGEM=320VΔ VGEM=320V
Ionization occurs in drift region
Electrons enter into GEM holes.
Collection Efficiency
Electric field (kV/cm)
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Charge distribution
AD
C c
ount
s
0 63Channel
One event
d X (各 strip - C.O.G)
σ = 359.7±0.4 μm
P10ΔVgem =330 V
Ed= 0.5 kV/cm
Et=1.65 kV/cmEi= 3.3 kV/cm
ΔVgem =330 V
Ed= 0.5 kV/cm
Et=1.65 kV/cmEi= 3.3 kV/cm
ADC
SUMADC
-1 0 1
Nor
mal
ized
AD
C c
ount
s
mm
ΔVgem =370 V
Ed= 0.5 kV/cm
Et=2.59kV/cmEi=5.18 kV/cm
ΔVgem =370 V
Ed= 0.5 kV/cm
Et=2.59kV/cmEi=5.18 kV/cm
σ = 181.2±0.3 μm
Ar-CO2
(70/30)
-1 0 1
Nor
mal
ized
AD
C c
ount
s
d X (各 strip - C.O.G)mm
dX (each strip – C.O.G)
dX (each strip – C.O.G)
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y = 0.2979x + 0.0016
y = 0.0668x + 0.0062
0
0.05
0.1
0.15
0.2
0.25
0 0.2 0.4 0.6 0.8
Total gap(cm)
(mm2 )
P10P10
Ar-CO2Ar-CO2
0.546mm/√cm0.546mm/√cm
0.258mm /√cm0.258mm /√cm
Charge spread
Diffusion is dominant factor.
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0 1 2 3 4
V/ cm)電場(k
σ2 (mm
2 )
P10P10
Ar-CO2Ar-CO2
MagBoltz
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Application of GEM
Shoji Uno (KEK-DTP)
Neutron detector X-ray detector
Soft X ray Hard X ray Light
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Application to Neutron Detector
Normal GEM
B10 coated GEMs
Readout board
Cathode plateWith B10
Ar-CO2
• Expensive 3He Gas is not necessary. – No pressure vessel
• Free readout pattern
• High resolution– Position and Time
• Insensitive against g-ray
• Capability against high counting rate
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Chamber structure
1 mm ( 0.5mm )
Readout strip
2 mm
1 mm
EI = 4.0kV/cm
GEM 2
ET = 2.2 kV/cm
ED = 1.5 kV/cm
Ar/CO2 = 70:30
GEM 1
1 mm
2 mm
B GEM 1
B GEM 2
ET = 1.5 kV/cm
ET = 1.5 kV/cm
Al - 10B cathode
150V (75V)
150V240V
240V150V400V
440V
370V
800V
X(120) +Y (120) strips0.8mm pitch
Thickness of Boron-10 : 4.4m2.0m + 0.6m ×48 mm
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Ethernet
GEMChamber
• I/F– One HV cable– Three LV cables– One Ethernet cable
• Electronics– 8 ASIC chips + 1 FPGA
• FE2009 ASIC : KEK-DTP• Data transfer and Control through
Ethernet– SiTCP by T. Uchida ( KE
K )– Using Note-PC
Present Detector System
Low Voltage
Electronics
Compact and Portable System T.Uchida et. al., "Prototype of a Compact Imaging System for GEMdetectors," was published on IEEE TNS 55(2008)2698.
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(Å)
11
Data samples
(Å)
L = 18789 mm ~ 18.8 m
L: distance from the source to the detector
The beam profile and its TOF distribution
An image of a cadmium slit and its TOF distribution
L = 18789 mm
27 mm
60 mm
The thickness of the slit ~0.5 mm
This image is produced with a wavelength cut.
Events from 1.5 Å to 8 Å are selected
Our system can obtain a 2D image and its TOF at the same time.
Cd cutoff
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Energy Selective Neutron Radiography
Bragg Edge region (Thermal and cold)
Resonance absorption region (E>1eV)
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Resonance absorption imaging By T. Kai (JAEA) et al. at BL10 in J-PARC
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One more demonstration
EURO coin
TEST Sample
gold coin
Ratio of ToF spectrums with/without sample
Imaging data with around 450sec ToF