tpc for lc
DESCRIPTION
RD51. TPC for LC. P. Colas. Lanzhou U., Saclay, Tsinghua U. T ime P rojection C hamber. t. electrons diffuse and drift due to the E-field. Ionizing Particle. electrons are separated from ions. E. B. A magnetic field reduces electron diffusion. y. x. - PowerPoint PPT PresentationTRANSCRIPT
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TPC for LCP. Colas
Lanzhou U., Saclay, Tsinghua U.
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E
Ionizing Particle
electrons are separated from ions
electrons diffuse and drift due to the E-field
Localization in time and x-y
B
t
x
y
A magnetic field reduces electron diffusion
MPGD TPC : the amplification is made by a MPGD
Time Projection Chamber
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TPC for ILCContinuous 3D tracking in a large gaseous volume with O(100) space points.
ILC-TPC (ILD concept)
Large prototype being tested at DESY
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LCTPC Collaboration
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DETECTION TECHNOLOGIES
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Micromegas and GEM
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11/05/2009, Orsay P. Colas, Micromegas TPC tests
S1
S2
• VeryVery
Two copper perforated foils separated by an insulator (50 m). Multiplication takes place in the holes.
Usually used in 2 or 3 stages.
a micromesh supported by 50-100 m - high insulating pillars. Multiplication takes place between the anode and the mesh
200 m
GEMMicromegas
6
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resistive anode
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D. Arogancia, K. Fujii et al., to appear in NIM A
LC-TPC goal is 200 measurement points on a track, with <130 micron resolution
With Micromegas, signal spread is equal to the avalanche size, 12-14 microns : not enough charge sharing at low diffusion even with 1mm pads.Need to share the charge between neighbouring pads to make a barycentre possible and improve resolution.
With GEMs, diffusion in the last transfert gap helps to spread the charge and good resolution is obtained with 1mm-wide pads.
Both solutions are studied in LC-TPC:Micromegas with resistive anode or GEMS with small standard pads.
Note that charge sharing saves number of channels ($, W, X°).
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resistive anode (2)
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One way to make charge sharing is to make a resistive anode (M.S.Dixit et.al., NIM A518 (2004) 721.) This corresponds to adding a continuous RC circuit on top of the pad plane. Charge density obeys 2D telegraph equation
t
1
RC
2r2
1
r
r
(r, t) RC
2t
r2RC
4 teM.S.Dixit and A. Rankin NIM A566 (2006) 281
SIMULATION
MEASUREMENT
Res. foil also provides anti-spark protection
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Small prototypes Micromegas
DESY 5T cosmic test, 200750 µm resolution with 2mm pads
KEK beam test, MP-TPC (2005)
Carleton TPC with res. anode
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Small prototypes
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GEM prototype built at Tsinghua to train and measure gas properties, with help from Japan.
Also work on MP-TPC cosmic-ray test at KEK.
Good operation with Ar-CF4-isobutane.
Tsinghua GEM
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THE LARGE PROTOTYPE
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LC-TPC project using the EUDET test facility at DESY
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The EUDET setupat DESY
PCMag magnet from KEKCosmic trigger hodoscope from Saclay-KEK-INRBeam trigger from NikhefDummy modules from BonnField cage, gas from DESYEndplate from Cornell
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Test one Micromegas module at a time
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About 3200 readout channelsALTRO-based electronics
(made at CERN)
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About 2000 readout channelsAFTER-based electronics
(made in Saclay)
GEMMicromegas
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DOUBLE GEMMicromegas
‘Bulk’ technology (CERN-Saclay) with resistive anode (Carleton)
New 100 micron GEM (plasma-etched in Japan) stretched from 2 sides.
Pad plane from Tsinghua
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DOUBLE GEMMicromegas
4-layer routing (CERN) and 6-layer routing (Saclay)24x72 pads, 2.7-3.2 mm x 7 mm
8-layer routing done at Tsinghua28x176-192 pads, 1.1 mm x 5.6 mm
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Double GEMMicromegas
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FIRST MICROMEGAS RESULTS
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0
1
2
3
4
5
6
7
8
0 100 200 300 400 500 600
Z (mm) arbitrary origin
Drif
t tim
e (µ
s)
Measured drift velocity (Edrift = 230 V/cm, 1002 mbar) : 7.56 ± 0.02 cm/µs
Magboltz : 7.548 ± 0.003 pour Ar:CF4:isobutane:H2O/95:3:2:100ppm
B=0 data
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y = 13,884x - 165,42
-200
-150
-100
-50
0
50
100
150
200
0 4 8 12 16 20 24Dis
plac
emen
t w
rt v
ertic
al s
trai
ght
line
(mic
rons
)
Pad line numberRms displacement: 9 microns
B=0 data
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Determination of the Pad Response Function(B=1T beam data)
Fraction of the row charge on a pad vs xpad – xtrack
(normalized to central pad charge)
Clearly shows charge spreading over 2-3 pads(use data with 500 ns shaping)
Then fit x(cluster) using this shape with a ² fit, and fit simultaneously all rows to a circle in the xy plane
xpad – xtrack (mm)
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RESIDUALS (z=10 cm)
Do not use lines 0-4 and 19-23 for the time being (non gaussian residuals, magnetic field inhomogeneous for some z positions?)
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Resolution 46±6 microns with 2.7-3.2 mm padsEffective number of electrons 23.3±2.0 consistent with expectations
eff
dx N
zC 2
20