Bat-El Pinchasik, Technion Israel
Bat-El Pinchasik, Technion Israel GEM detectors main element GEM - - PowerPoint PPT Presentation
Bat-El Pinchasik, Technion Israel GEM detectors main element GEM - - PowerPoint PPT Presentation
Bat-El Pinchasik, Technion Israel GEM detectors main element GEM foil Terminals 10 cm Kapton (polyimide) p (p y ) copper-clad on both sides CO2+ Argon CO2+ Argon CO2+ Argon CO2+ Argon GEM GEM DRIFT REGION INDUCTION REGION REGION
GEM detectors main element
GEM foil
Terminals
10 cm
Kapton (polyimide) p (p y ) copper-clad on both sides
CO2+ Argon CO2+ Argon GEM CO2+ Argon CO2+ Argon GEM
DRIFT REGION
INDUCTION REGION REGION
segmentation
Tracking, Triggering Etc..
Field lines
Drift field
Electrons follow the field lines
GEM foil
In the holes: high density of
500 volts 50μm
Induction
y field lines
Induction field
Electrons gain energy!
Si l ti Simulation:
Ions
CATHODE
Ions
Electron-Ion pair Drift field pa Drift field GEM
Top B
Electrons are shared between
Bottom
Induction field
between bottom GEM and anode Gain of the detector ANODE anode
Advantages Advantages
Detector Area Cost Rate Aging covered by a d (per area) capability g g process detector
GEM d
$$
Low aging
detector Wi
Gain loss and
Wire chamber
$
Gain loss and discharges increase
Silicon detectors
Noise and leakage t
detectors
current increase
72µm
40µm
- First invented in 1998
- Double conical geometry
Doub e co ca geo et y
- Used already in several
experiments e pe e s
- Easy to produce
98.9µm
copper
Easy to produce
- larger detectors
- low cost per area
42.5µm
kapton
low cost per area
µ
copper
Gl f b Glance from above
Internal & External External diameter 140 µm Larger diameter smaller diameter diameter diameter 140 µm
See the difference
Large conical GEM conical GEM foil
60 cm
10 X 10 cm
CO2+ Argon CO2+ Argon
Voltage
CO2+ Argon CO2+ Argon
Voltage
- ver the
GEM GEM
Drift field Induction
d
Induction field
Anode current
D ift fi ld Drift field scan
GEM voltage: 500 volts
1
conycal I anode (normalized) I anode (normalized) I anode (normalized) conical
g 5 E induction: 3 (kv/cm)
0.8
standard
0.6
Recombination
plateau
Electrons end
0.4
up in Top GEM
0.2
E drift (V lt / )
1000 2000 3000 4000 5000
(Volts/cm)
G i GEM lt Gain vs. GEM voltage
Gain Integration over Gain Integration over distance Townsend Field & gas
α
standard conical
Gain of the
coefficient g properties
α
500 conical
detector
Log
E induction:
50
scale
3kv/cm E drift: 2 kv/cm
50 5 300 350 400 450 500 550 600 650
Gem voltage (volt)
d i Induction scan
I d
Electrons distribution
1.1 conical
I anode (normalized)
0 8 0.9 1 standard 0.6 0.7 0.8
Higher
0.4 0.5
More electrons get to the anode Higher signal
0.2 0.3
Increasing induction field
0.1 1000 2000 3000 4000 5000 6000 7000 E induction (volt/cm)
C l i Conclusions
Results
- Conical GEM has similar performance as
standard GEM
- Low cost
Advantages
Low cost
- Larger area
- Easy to fabricate
C i l GEM i tt ti did t t
Conclusion
- Conical GEM is an attractive candidate to
future LHC upgrades
C t li ti Current applications
LHCB
TOTEM
COMPASS
LHCB muon