Pixelized gaseous detectors

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Pixelized gaseous detectors Motivation Pixel chips Production Applications Y. Bilevych, H. Blank, C. Brezina, K. Desch, J. Kaminski, C. Krieger, M. Lupberger, W. Ockenfels, F. Müller (Bonn) in collaboration with: O. Ehrmann, T. Fritzsch, M. Töpper (IZM Berlin) N. van Bakel, H. van der Graaf, J. Rövekamp (NIKHEF) J. Schmitz (Twente) TRD2011 Bari, Italy – 15/09/2011 Klaus Desch University of Bonn K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 Motivation Micro-structuring of semiconductor detectors led to breakthrough in charged particle tracking  silicon strip + pixel detector Q: Can gaseous detectors also benefit from extremely fine-grained readout? A1: (for thin planar drift detectors) diffusion of drifting electrons limits spatial resolution  typical diffusion coefficient D ~ o(100) μm/√cm  o(30) μm for single electron after 1 mm drift + average over o(10) electrons for a single tracklet  o(10) μm single point for a thin planar detector K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 Motivation Q: Can gaseous detectors also benefit from extremely fine-grained readout? A2: (for long drift distances, e.g. TPC)  to first order no advantage over pad-based r/o for p-resolution but - identify (and remove) short δ-tracks for track reconstruction - clearly superior for double track resolution (dense jets...) - lower occupancy  BG tolerance - dE/dx by cluster counting - (potentially simpler readout) A3: (for x-ray photon identification, BG suppression, rare event searches, TR)  clear distinction of photons / m.i.p.s / alphas / ...  reconstruction of photoelectron „tracks“ ~2 mm K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Detector Technologies Clearly, micro-structured readout needs micro-structured gas-amplification MPGDs (GEMs, Micromegas) Pioneering example: Bellazini et al (X-ray polarimeter using „special“ GEM + dedicated CMOS pixel chip) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 Timepix derived from Medipix-2 chip (X-ray imaging) 256x256 pixels each with - CSA - Time (~20 ns) or TOT measurement 1.4 x 1.4 cm2 active area frame-based (rather slow) readout Next generation: Timepix-3 to be submitted end 2011 fast, sparse readout, ~ 2.5 Gbps output LHC compatible ultrafast (1.4 ns) timing on-pixel measure charge (TOT) + time simultaneously Si through via (STV) capability (backside connection) (Medipix-3 collaboration) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Detector Technologies First „large area“ ( 2.8 x 5.6 cm2, 500k „channels“) tracking devices (EUDET): 3-GEM 8 Timepix InGrid 8 Timepix NIKHEF Saclay Twente Bonn Freiburg K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Detector Technologies 3-GEM 8 (2x4) Timepix InGrid 8 Timepix „Octopuce“ underneath a 3-GEM stack NIKHEF Saclay Twente Bonn Freiburg K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Detector Technologies Both GEMs and InGrids work nicely Major GEM advantage: amplification field(s) seperated from CMOS electronics Major GEM disadvantage: diffusion in GEM stack spreads charge over o (100) pixels  need (very) high gain Look at InGrids = a micromegas grid produced through postprocessing on a CMOS substrate (so far, the Timepix chip) pioneered by NIKHEF + Twente U. (Mesa+) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 How is it done? 1. Preliminary analysis and cleaning of chip surface 7. Development of SU-8 Chip 2. Deposition of protection layer (aSi or SixNy) 3. Deposition (spin coating) of SU-8 (50 μm polymer photoresist) 4. Exposition and baking of SU-8 5. Deposition of thin Al film (critical) 6. Patterning of Al to form the Grid K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Protection of CMOS chip potential showstopper: sparks, large signals, HV breakdowns can kill input stage of CSA of CMOS pixel chip  protection on chip? on detector: SiProt Amorphous Si or SixNy Structuring (bond pads!) through shadow mask (high T process) 7 μm protection layer - finite (but large) resistivity (1011-1014 Ωcm) reduce local E-field charge-up at high rate  reduction of signal vital for stable operation (unprotected Ingrids typically die after few h from α-induced discharges) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Single chips / 3x3 chip squares at Twente Facilities at Twente U can (at most) handle 4 inch wafers practically at most 3x3 chips can be handled at once several days of processing (+working) time for one run Try to find a place which can manufacture Ingrids on a 8 inch wafer scale (Berlin) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 IZM Ingrids transfer original „Twente“ process to 8´´ very successful 1st attempt on dummy wafers development after dicing IZM+Y.Bilevych,Bonn extremely regular... K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 IZM Ingrids first 8“ Timepix wafer completed in August (55Fe signals seen last week) some problems: SiN deposition (done at Twente U) partially covers wire bonding pads Last (additional) cleaning step partially peeled off grid (solutions known for next iteration) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Radiation damage and ageing? „Sensor“: No radiation damage of gas (can be replaced) CMOS: same as for Si pixels (go to small feature sizes) Ageing of amplification structure? In general, planar structures more robust than wires (no 1/r dependence of E-field) Preliminary tests done at NIKHEF: Irradiation with 8 keV X-rays: No rate effects up to anode current density of 0.2 μA / mm2  very fast track counting possible! After 0.3 Coulomb/mm2 (eq. 3.7 x 1016 MIPs/cm2) deposit of carbon polymer on anode is clearly visible. Micromegas is clean (?!) Little deposit on cathode, and…… chamber still worked! H. van der Graaf, NIKHEF K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Alternate road at IZM: „GEMGrids“ Technically simpler – BCB can be etched Avoid cross-linking of photo-resist during Al sputtering K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Alternate road at IZM: „GEMGrids“ K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

„GEMGrids“ – work (in principle) first signals seen in Bonn setup with 55-Fe source challenges / problems limited yield (~ 1 / 6 structures working so far...) sparking at the edges limited HV  limited efficiency to be understood T. Krautscheid, Bonn K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 Example Applications TPC prototype X Ray detector for low rate experiment (CAST, ...) Gridpix tracker proposal for ATLAS  A. Romaniouk (tomorrow) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 Applications 1: TPC example track 25cm drift TPC – cosmic test stand He/CO2 (70/30) endplate with single Ingrid several weeks of stable data taking K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 Applications 1: TPC He/CO2 (70/30) expect 25/cm close to 100% single-electron efficiency at moderate gas gain (~1000)  low (few 100 e threshold of Timepix) some attachment seen K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 Applications 1: TPC hit map  less hits on edges  field distortions reaching diffusion limit in central region single point resolution K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Applications 2: X-Rays (e.g. CAST Axion search) Test detector with 2 cm drift Single Ingrid Ar/Iso (95/5) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Applications 2: X-Rays (e.g. CAST Axion search) 5.9 keV photon can count electrons! 55Fe spectrum just from hit counting! topolgical background suppression „easy“ background K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Applications 2: X-Rays (e.g. CAST Axion search) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Applications 2: X-Rays (e.g. CAST Axion search) ~ 1week of data Test detector operated for many weeks with same chip (still alive...) 520995 acquisitions (1 s)  37109 non-empty events After background rejection: 707 candidate events Background rate: 5 x 10-5 cm-2 keV-1 s-1 (= 1 photon cand. in 6h in 1 keV window) Xe run still t.b.d. K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Applications 3: GridPix Tracker for ATLAS? K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 Ideas for ATLAS: GridPix Tracker A. Romaniouk Can do fast in-situ reconstruction of 3D tracklets  L1 fast track trigger ! K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Applications 3: GridPix TR-Tracker for ATLAS? L=30 mm Testbeam Nov 5 – 12, 2007 PS/T9: electrons and pions, 1 – 15 GeV/c V0 V1 f Transition Radiator 0.05 mm Anatoli Romaniouk, Serguei Morozov, Serguei Konovalov Martin Fransen, Fred Hartjes, Max Chefdeville, Victor Blanco Carballo K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

Particle Identification pion (6 GeV/c) electron (6 GeV/c) K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 Summary and Outlook Pixelized gaseous detector are still in their infancy Fascinating potential - TPCs - planar vertex / tracking detectors - TR (identification of single TR photons along with the track) - X ray polarimetry / WIMP searches / UV photon detection ... Proofs of principle done Lots of work ahead – first full Timepix/Ingrid wafer back  „mass production“ allows for systematic tests + real projects Timepix3 submission by end of 2012 Synergy with aspects of Si-pixels (thinning, STV, common ASICs, ...) Lots of fun ahead... K. Desch - Pixelized Gaseous Detectors - Bari TRD2011

K. Desch - Pixelized Gaseous Detectors - Bari TRD2011 A Quiz... 2 cosmic tracks from our TPC with 3GEM + Timepix readout Blobs = single electrons after amplification K. Desch - Pixelized Gaseous Detectors - Bari TRD2011