P. Colas for the LC TPC collaboration

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Presentation transcript:

P. Colas for the LC TPC collaboration PRC at DESY, Zeuthen P. Colas for the LC TPC collaboration

A TPC for the LC Higgs recoil ZH, Z->µµ Jets in a noisy environment d (1/PT) = 5. 10-5 GeV-1 Jets in a noisy environment Continuous 3D tracking High B required for vertex detector -> good for TPC Wires have disadvantages at high B: ExB Wires need to be tensioned -> MPGD ILD concept 14/10/2010 P. Colas - LC TPC

LC TPC gathers all the actors in R&D for a TPC at a LC 25/38 institutes from 12 countries have signed the MoU 7 institutes are observer. Most world specialists of TPCs, MPGD, front-end electronics, cooling, etc… are members 14/10/2010 P. Colas - LC TPC

The EUDET infrastructure at DESY Hamburg The prototypes www.lctpc.org After a decade of small prototype tests in various labs, all the member institutes joined their efforts and resources around the construction and exploitation of a beam test infrastructure in DESY, supported by the FP6 program EUDET. Links exist with RD51 (MPGD R&D). LC TPC created a speaker’s bureau in 2009 and started a new working group for TPC engineering and integration. Outline: The EUDET infrastructure at DESY Hamburg The prototypes Results of operation in 2008-2010 Future 14/10/2010 P. Colas - LC TPC

The EUDET facility at DESY Hamburg PCMAG: superconducting magnet, 1.2 T e- test beam @DESY (1GeV/c<p<6GeV/c) KEK Moving frame SiPM Cosmic Trigger Setup DESY Saclay LP : part of a TPC endplate 14/10/2010 P. Colas - LC TPC

The Large Prototype Field cage: extrapolable to LC L=61 cm, f=72 cm Endplate DESY Cornell Gas system DESY HV system DESY Slow control: T,P, O2, H2O Laser calibration U. Victoria Sharing infrastructure: - avoids duplication - favours communication 14/10/2010 P. Colas - LC TPC

Micromegas GEM a micromesh supported by 50-100 mm - high insulating pillars. Multiplication takes place between the anode and the mesh Two copper perforated foils separated by an insulator (50 mm). Multiplication takes place in the holes. Usually used in 2 or 3 stages. Very S1 S2 200 mm 14/10/2010 P. Colas - LC TPC

PLEASE ENTER… 14/10/2010 P. Colas - LC TPC

Beam tests at DESY Micromegas GEM Read out by T2K AFTER-based electronics (Saclay) Read out by ALTRO electronics (EUDET, Lund,CERN) From October 2008 to September 2010 several GEM and Micromegas modules were tested in beam at the LP 14/10/2010 P. Colas - LC TPC

5 Micromegas Modules for TPC Saclay CERN Carleton Resistive ink ~3 MΩ/□ Resistive Kapton ~5 MΩ/□ Standard 2 Resistive Kapton Bulk Micromegas: pillars hold the mesh on the whole surface: no need for frame Resistive bulk: continuous 2D RC network to spread the charge 14/10/2010 P. Colas - LC TPC 10

24 rows x 72 pads, 2.7-3.2 mm wide, 7 mm long 14/10/2010 P. Colas - LC TPC

Time issues with the resistive foils? Test at CERN (July 2010) at 180 kHz (5 x 2 cm² beam) showed no charging up and stable operation Peaking time of 200 ns is enough to obtain the best resolution -> 300 ns suffice to distinguish 2 tracks on the same pad 14/10/2010 P. Colas - LC TPC

Asian GEM Modules for TPC KEK Tsinghua Saga + other Japan Univ. 2-GEM (laser etched, with 100 µm gap, from SciEnergy, Japan), plus 1 gating grid (replaced by a field shaper in Sep. 2010 ) GEMs pegged down by the two arc-shaped stiffeners 14/10/2010 P. Colas - LC TPC

28 pad-rows of 176 -194 pads (pad size ~ 1.1 x 5.4 mm2 Total 5152 pads/modules 3 modules partially equipped (7616 channels) 14/10/2010 P. Colas - LC TPC

Drift velocity measurements Both GEM and Micromegas used T2K gas (Ar:CF4:iso=95:3:2). GEM T2K Gas: B=1T Micromegas, with P=1035 hPa, T=292 K, 35-50 ppm H20 Vdrift = 7.698 +- 0.040 cm/µs at E=230 V/cm (Magboltz : 7.583+-0.025(gas comp.)) GEM, with P=1013 hPa, T=290 K, 200 ppm H20 Vdrift = 7.563 +- 0.069 cm/µs at E=230 V/cm (Magboltz : 7.509+-0.024(gas comp.)) 14/10/2010 P. Colas - LC TPC

Velocity vs drift field with Micromegas s2 (pad resp.) vs drift distance with GEM CD = 95.4±0.1 µm/√cm Magboltz predicts 94.3 14/10/2010 P. Colas - LC TPC

Micromegas residual distributions Position residuals xrow-xtrack 14/10/2010 P. Colas - LC TPC

Bias inside a row vs track position Bias before correction Bias after correction ±50µm ±50µm Bias after Bias due to non-uniformity can be easily corrected. 14/10/2010 P. Colas - LC TPC

Uniformity (B = 0T) from cosmic-ray tracks Preliminary Time of pulse max Preliminary Total charge by row using cosmic-ray events 14/10/2010 P. Colas - LC TPC

Uniformity MEAN RESIDUAL vs ROW number Z-independent distortions Z=5cm MEAN RESIDUAL vs ROW number Z-independent distortions Distortions up to 50 microns for resistive ink (blue points) Rms 7 microns for CLK film (red points) Z=35cm Z=50cm Carbon loaded kapton is much more uniform than resistive ink 14/10/2010 P. Colas - LC TPC

Micromegas results (B = 0T & 1T) Carbon-loaded kapton resistive foil B=0 T Cd = 315.1 µm/√cm (Magboltz) B=1 T Cd = 94.2 µm/√cm (Magboltz) χ2/Ndof = 10.6/10 χ2/Ndof = 29.1/11 Module 4 Module 3 Averaging B=0T data and B=1T data (excluding ink module): Neff = 38.0±0.2(stat) ±0.8 (Cd syst) σ0= 59 ± 3 µm 80 µm resolution at 2m in B=3.5 T ! 14/10/2010 P. Colas - LC TPC

Resolution with GEMs 3 modules allow a momentum measurement : 1/PT resolution extrapolated to z=0 obtained 0.083 GeV-1 (expected 0.081 GeV-1 ) Using MarlinTPC software 14/10/2010 P. Colas - LC TPC

Micromegas+pixels, GridPix Nikhef Saclay Bonn CERN TimePix chip : 65 000 digital pixels (55 µm x 55 µm) with time and TOT measurement Single electron capability Octopuce : 8 chips bounded on a LP panel. Next steps within AIDA e- content and width of the escape peak Single electron efficiency vs gain determined by counting electrons from a source, assuming some analytic form for avalanche fluctuations 14/10/2010 P. Colas - LC TPC

GEM + Pixels 2 TimePix quads topped by 3 GEMs /cm 14/10/2010 P. Colas - LC TPC

SOFTWARE DESY, KEK, Bonn, Tsinghua, Victoria, Carleton… LC TPC developped a common software for reconstruction and simulation of test data: MarlinTPC (based on the ILC software). This provides input for ILD design and benchmark studies It includes reconstruction up to hit level (treatment of charge-spreading by resistive anodes to come) Packages are available for track finding and fitting (Kalman filter, Hough transform, c2 and likelihood) Calibration and correction methods (alignment, inhomogeneous fields) tools are being set up with the ILD collaboration 14/10/2010 P. Colas - LC TPC

DESY GEM module Present GEMs need improved flatness: a design with a thin ceramic support structure is under construction. The GEMs are stretchless in this design, minimizing the dead space and flattening the gaps. This also allows to reach the dE/dx goal and provides robustness. Previous studies with MediTPC showed that the ceramic grid (1 mm x 1 mm mullions) has a negligeable effect on single-point resolution. 14/10/2010 P. Colas - LC TPC

7-module electronics for Micromegas LP test Effort to integrate the electronics flat behind the modules : cards with naked wire-bonded chips, special high density flat connectors, tailored protection Expect noise reduction Air cooling “Power-pulsing ready” Status: Backend and 2 prototype module cards operational, FECs under fabrication. Test of 1 module soon, construc-tion in 2011 and full tests in 2012 Saclay Carleton 14/10/2010 P. Colas - LC TPC

S-Altro electronics Until now used PCA16 preamp and ALTRO filter+ADC Full chain new S-ALTRO16 chip prototype submitted Will be mounted on Multi-Channel Modules Towards new chip 64 channels CO2 Cooling and power pulsing foreseen (to be tested in a 5T magnet) The final electronics (could be SALTRO 64) will be usable for both GEM and Micromegas 14/10/2010 P. Colas - LC TPC

Mechanical engineered design New Endplate under study at Cornell: hybrid Al (for surfaces) and composite (for rigidity) Or light space frame Mechanical studies for the ILD TPC within AIDA (DESY-Saclay) Deflexion O(150 µm) @ 3 mbar 14/10/2010 P. Colas - LC TPC

Space charge Study of effects of primary ionisation (curlers and ‘snow’, mainly due to micro-curlers and X rays has started Also effect of the ‘ion disk’ flowing back in the drift volume at each train crossing will be assessed Gating is problematic : 50% transmission of gating GEM Work at low gain, wire grid? Background from 150 bunch crossings overlapped with a ttbar event 14/10/2010 P. Colas - LC TPC

Towards the Detailed Baseline The next milestone of LC TPC is to converge towards a Detailed Baseline Document answering all the open questions New endplate and field cage designs with reduced material budget S-ALTRO 16 chip in production Add He compressors to PCMAG (AIDA-DESY + KEK-TOSHIBA) lowers operation cost and makes the magnet movable Cooling and power pulsing will be tested (need 5T magnet) Software developments towards corrections for space charge and field inhomogeneity TimePix 2 and its readout 14/10/2010 P. Colas - LC TPC