Title: Results from MPGDs with Protected Pixel Sensors as Active Anode MP33
1Results from MPGDs with Protected Pixel Sensors
asActive AnodeMP3-3
- Harry van der Graaf
- Nikhef, Amsterdam
- on behalf of the
- GridPix group
- IEEE-NSS Honolulu 2007
2Overview
- GridPix chambers
- InGrid the Integrated Grid
- SiProt the amorphous Si Protection layer
- Chamber results
- GridPix TimePix SiProt InGrid/Micromegas
- PSI-46 Pixel FE chip SiProt Micromegas
- TimePix SiProt Micromegas _at_ CEA/Saclay
- All-Gas detectors for trackers
3GridPix chamber principle
cathode
Micromegas or InGrid
Pixel chip
4Wafer post-processingInGrid
Hex / Pillars
- InGrid an Integrated Grid on Si (wafers or
chips) - perfect alignment of grid holes and pixel pads
- small pillars Ø, hidden pillars, full pixel area
coverage - Sub-micron precision homogeneity
5New Ingrid developments and results
- Process improvement grids much flatter
- Extremely good (record?) energy resolution
- 13.6 FWHM with 55Fe in P10
- Removal of Kß 6.5 keV line
- 11.7 _at_ 5.9 keV in P10
- New wafer masks
- hole pitches down to 20 µm
- with various diameters and gaps
- Investigate Micromegas geometry
- Test of the ion backflow theory
- Until now 1 µm thin Al
- but can now be increased to 5 µm by electrolysis
- Expect less damaged from sparks
Ka escape
Kß escape
13.6 FWHM
Gap 50 µm Hole picth 32 µm,Ø 14 µm
Kß-filtered spectrum with Cr foil
11.7 FWHM
6Full post-processing of a TimePix
- Timepix chip Micromegas mesh
Moiré effects pillars
CERN
- Timepix chip SiProt Ingrid
Uniform
MESA
IMT Neuchatel
Charge mode
7A scratch occurred during the construction of
Ingrid Loose parts removed. Ingrid working!
8- SiProt protection against
- hot spark plasma
- Too large charge in pixel circuitry Principle
of RPCs - local reduction of E-field quenching
- widening discharge funnel signal dilution
- increased distance of influention
SiProt a low T deposited hydrogenated amorphous
silicon (aSiH) layer Up to 50 µm thick films,
1011 O.cm
9TimePix SiProt results
10setup
Next-1,2
11Status of Timepix application at Nikhef
- 13 dec. B05 with 3 µm SiProt Micromegas in He
20 iC4H10 - 24 jan. Switch to Ar 20 iC4H10, chip died after
2 days - 20 mar. MediPix2 with 3 µm SiProt InGrid
operated 4 days in He - 17 apr. C08 with 3 µm SiProt Micromegas
- guard electrode (G.E.) in He
- 25 jul. Stop C08 after 3 months of continuous
operation in He - E09 with 20 µm SiProt InGrid placed
- in NEXT-1 chamber in He
- 22 aug. A06 with 20 µm SiProt Micromegas placed
- in NEXT-2 chamber in He
- 04 sep. Flush NEXT-2 (A06) with Ar, stable
operation for 2 weeks - 23 sep. Flush NEXT-1 (E09) with Ar, same nice
results
12Fully sensitive detector
A long cosmic track
Timepix 20 µm thick Siprot Ingrid
Stable operation in He iC4H10
13Stable operation in Argon too!
Time mode
After 2 weeks of cosmic event recording, it was
time for a definitive assessment whether 20 µm
SiProt is enough to protect against discharges
14Final assessment spark-proofness
- Provoke discharges by introducing small amount of
Thorium in the Ar gas - Thorium decays to Radon 222 which emits 2 alphas
of 6.3 6.8 MeV - Depose on average 2.5.105 2.7.105 e- in
Ar/iC4H10 80/20 - at -420 V on the grid, likely to trigger
discharges
Charge mode
Since 1 week, some 5.104 alpha events recorded in
1 of which
15 discharges are observed !
- For the 1st time image of discharges are being
recorded - Round-shaped pattern of some 100 overflow pixels
- Perturbations in the concerned column pixels
- Threshold?
- Power?
- Chip keeps working
16Discharge signals on grid directly measured on
scope
17proportional signals from alfas
discharges
18Qmax 1 2 fC Chip may die if Qmax gt 10 fQ
19GOSSIP-Brico PSI-46
First prototype of GOSSIP on a PSI46 is
working 30µm layer of SiProt 1.2 mm Drift
gap Uses MicroMegas MicroMegas grid used as
trigger We can see tracks
replacement of (vertex) tracking detectors..
20GOSSIP Basics (PSI-46 Brico specific)
Use Pixel chip for readout, use gas layer for
detecting MIPs
50µm high support pillars
Gas 1.2 mm as detection medium 99 chance to
have at least 1 e- Gas amplification 25,000 in
90/10 Ar/CH4 Single electron sensitive All
signals arrive within 18 ns
21We can see tracks!
(Frame 17 is really great)
7.8mm
8mm
Animated GIF of 100 hits on the PSI46 brico, 30µm
SiProt. (if this does not animate, drop the
picture into a web browser)
22(No Transcript)
23Since last week TimePix SiProt
Micromegas works in CEA/Saclay Paul Colas et
al.
55Fe events, enlarged
55Fe events
24Tracking of charged particles principle
Measurement of time and place of a charge signal
from detection material
- Gas compared with Si as detector material
- cheap
- exchangeable therefore no radiation damage
- readout requires much less power thus
detector mass - no bias current
- low source capacity
- low mass
- electron multiplication
- light
- but
- discharges now solved!
- chamber ageing
- Consequences for future experiments
- ILC
- LHC Upgrade (Super LHC)
- All Gas detectors, followed by calorimeters
25Conclusions Plans
- InGrid is now a proven technology
- With a 20 µm SiProt layer, a chip in GridPix is
spark proof - GridPix has shown to work with Medipix-2, TimePix
and PSI-46 - Next steps
- High-Resistive InGrid
- Build a larger area detector
- Chip tiling, wafer thinning through-via
bounding, fast Gbit/s readout - Build beam telescope and vertex detectors from
PSI-46 chip - More tests to quantify the detector performances
- Beam tests for spatial and time resolution
measurements - GridPix as Transition Radiation Tracker
- Tests in magnetic field for measurements of dE/dx
and gas diffusion - Gas ageing studies testing Si containing
compounds (SiO2, SiH4, SiCnHm) - Absence of ageing measured up to 5 x 1015
MIPs/cm2 - Extreme large rates and gas gains up to 500 k are
possible, maintaining the proportional mode
26- NIKHEF
- Harry van der Graaf, Max Chefdeville, Fred
Hartjes, Jan Timmermans, Jan Visschers, Marten
Bosma, Martin Fransen, Yevgen Bilevych, - Wim Gotink, Joop Rovekamp
- University of Twente
- Cora Salm, Joost Melai, Jurriaan Schmitz, Sander
Smits, - Victor Blanco Carballo
- University of Nijmegen
- Michael Rogers, Thei Wijnen, Adriaan Konig,
Jan Dijkema, - Nicolo de Groot
- CEA/DAPNIA Saclay
- D. Attié, P. Colas, I. Giomataris
- CERN
- M. Campbell, X. Llopart
- University of Neuchatel/MTI