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FE electronics for Micromégas Trackers eric.delagnes@cea.fr. Introduction: (Micro)Electronics for Micromégas @ Saclay. Several versions of FE cards using the Gassiplex chip from CERN => CAST…. FE of the COMPASS tracker (12K channels operating since 2000)
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Introduction: (Micro)Electronics for Micromégas @ Saclay. • Several versions of FE cards using the Gassiplex chip from CERN => CAST…. • FE of the COMPASS tracker (12K channels operating since 2000) • SFE 16 chip (ASD 16 channels) + F1-TDC. • Prototype of FE-boards for the upgrade of the COMPASS tracker: • Based on the APV chip from RAL. • FE of the T2K TPC (120 K channels operating since 2009) • AFTER chip (72 channels. Ampli Shaper + SCA). • FE for active target TPCs (for Nuclear Physics, 4x 20K channels): • AGET chip ( 64 channels ASD +SCA). Submitted in april 2010 • FE for the Micromégas CLAS12 tracker: 40 K channels
Lessons from few years working with MM (tracker for MIP) • Signal duration: 50-150ns depending on the gas and on the drift & multiplication gaps. • Detector capacitance always larger than what specified/foreseen. • For high rate operation and in practical conditions Gain limited to ~5000 because of sparks. • For detectors with long strips, the MIP signal is not so large => need for a low noise electronics. Can be very sensitive to common mode noise (as for all large detectors). Operating at very low threshold can become a nightmare. • Space required for spark protection networks is large (larger than chips). No success in fully integrating the protections (at least one external capa required). • Most of these limitations will disappear in case of success of the R&D on “resistive” Micromégas.
The CLAS12 tracker @ JLAB Clas12 detectors 3 Silicon views MM forward MM barrel Barrel: 3x2 (X,Y) cylindrical Micromégas Forward: 3x2 Disks Micromégas R=110to 240 mm / L =300 to 430 mm. R=200 mm Pitch ~ 300 µm Striplength >600mm . Total of ~5 m2 of Micromégas. Large Magnetic Field: 5T => Lorentz angle => decrease S/N No spaceinside the magnet: => Baseline :FE electronicsmovedaway (>0.8m flexcables).
Requirements for the CLAS12 MM electronics (1). • Use of standard (without resistive sheet) Micromegas assumed • ~40 K channels • Electronics moved away from detector using 0.8m Kapton cables • Particle rate < 20MHz • Hit Rate=> 48 kHz/strip (considering cluster size=4) • External trigger with Max Trigger Rate = 20 kHz, fixed latency =4.5µs • Inefficiency due to electronics ~ 2% • Ghost hits/trigger < 8/view. Noise hits rate negligible • Main functionalities (not necessary performed in this order): • Collect, amplify and filter the detector signal • Discriminate pulses • Timestamp pulses • Select pulses within a L1W ( = 100ns) window around the L1 accept signal • Measure signal charge (for centre of gravity calculation) • Many requirements very similar to those of COMPASS tracker
Requirements for the CLAS12 Micromegas electronics (2). • Channel Occupancy: • Tocc <250ns to keep occupancy < 1.2% • High order filtering (symmetrical shape). • Shaping peaking time must be • Large: • To avoid ballistic deficit . • To Minimize noise. • Small: • to limit occupancy • to be Compatible with L1W=100ns From calculations and experience from COMPASS: ~100ns peaking time should be ok => Tunable between 50-250ns.
Requirements for the CLAS12 Micromegas electronics (3). • Dynamic Range: • 600: 9-10 bit Max Signal over ENC required. - Max Charge = 10 MIP - Threshold = MIP/10 for efficiency - Threshold = 6 * Thresholds set to 6*ENC (for noise rejection). • Max range (and MIP) depends on the detector gain => Variable gain front-end: 4 ranges selectable by slow control: • i.e 160, 320, 640 fC for Micromegas. • ~ 40 fC range for Si detectors. Exemple: For the160fC range: => MIP = 100 Ke- => Th = 10 Ke – => ENC should be around 1500 e- rms (gives a S/N=60) Feasible with our large detectors (+ kapton cables) ?
What we can learn from the AFTER chip • AMS 0.35µm technology. • Designed for the TPC of T2K. • Slow Readout (incompatible with use in trackers) • But very versatile: • shaping time, dynamic range are ~matching with our needs. • Front-end part could be re-used nearly as it is associated with a custom back-end. • Modifications (50ns shaping) in progress for another experiment. • Noise deeply tested: a complete parameterization has been extracted: • Ability to predict the noise in other conditions. • 1Mrad radiation hardness demonstrated in another similar chip we designed using the same technology.
Power Supply Reference Voltage Reference Current x72(76) AFTER 1 channel 120fC<Cf<600fC BUFFER 76 to 1 FILTER SCA CSA ADC 511 cells 100ns<tpeak<2us Power On Reset SLOW CONTROL SCA MANAGER Asic Spy Mode TEST W / R CK In Test Serial Interface Mode CK CSA;CR;SCAin (N°1) AFTER ASIC design for T2K IEEE Trans. Nucl Sci, June 2008 • No zero suppress. • No auto triggering. • No selective readout. • AMS 0.35µm techno • 500000 transistors • Main features: • Input Current Polarity: positive or negative • 72 Analog Channels • 4 Gains: 120fC, 240fC, 360fC & 600fC • 16 Peaking Time values: (100ns to 2µs) • 511 analog memory cells / Channel: • Fwrite: 1MHz-50MHz; Fread: 20MHz • Optimized for 20-30pF detector capa • 12-bit dynamic range • Slow Control • Power on reset • Test modes • Spy mode on channel 1: • CSA, CR or filter out
Requirements for the CLAS12 Micromegas electronics (3). • Noise: • Must be minimized to be able to operate at low gain (if necessary to reduce spark rate). • Huge Flex + detector capacitance of 60-80 pF. • 1600-2000 ENC (for very low gain operation) seems feasible even with short shaping time: • From COMPASS experience. • From measurements on the AFTER chip. ENC versus input capacitance for different peaking times (120 fC range, ICSA=400 µA). Measured on the AFTER chip.
Features common to all FE solutions: Technology choices • Technology choices: • Use an existing chip: there are not a lot of available tracker chip adapted to both analog readout and large detector capacitances: the APV0.25 designed for CMS could be an option (under evaluation): + nearly a perfect chip + we already use it. • APV availability • APV not designed for high detector capacitance. • Large occupation time (RC-CR shaping). • New chip: • Using a well known technology (AMS CMOS 0.35µm): + very front-end part nearly already designed. • Chip size if integrates a lot of digital electronics. • Using a more recent technology: + long term availability. + prepare the future for our lab. + Less power consumption +? Less noisy. • more risky and longer development .
Features common to all FE Chip solutions • Packaging, modularity: • For Mmegas Prefer a QFN/QFP package (no bare die). • 32-64 channel/chip is the best modularity for integration on FE boards. • 128 channel/chip => big chip + package difficult to handle during test. • Power consumption • As we are outside the magnet, the requirements can be relaxed/ ~5 mW/ch for the FE Chip. • Configuration (Slow-control) Link: • To program test modes, peaking time, ranges, etc. • Test system: • Each Channel can be pulsed individually (or all together). • For test purpose and not absolute calibration. • Input Protections: • Designed to reduce the size (or even the need) of the external protections.
3 possible options for the FE chip architecture were proposed ONLY DEAD TIME-”FREE” solutions (with dual-port L1 buffers) are proposed • ASD + multihit TDC: • Similar to Micromegas COMPASS tracker readout. • Time Stamping + analog memory: • Trigerless Front-end. • Selective Readout. • Analog Memory L1-Buffer (APV-like): • Similar to GEM COMPASS tracker readout. • Solution selected: • Better noise rejection. • Minimum work for us : the only which could match with the schedule and the available manpower.
c510 c511 c0 c1 c. ci-2 ci+2 ci-1 ci+1 ci Analog Memory L1 buffer solution (APV-like solution) • A Switched Capacitor Array is used as a circular analogue buffer: • The analog signals of all the channels is continuously sampled at Fs in a Switched Capacitor Array (analogue memories). • When a L1-Trigger occurs it is sent to the chips with a FIXED LATENCY (TLAT): • 3-4 samples on all channels are kept (frozen) for each triggered event. • They are read and multiplexed towards an external ADC @ Fread. • Cells are rewritten after readout or if no trigger occurs during after TLAT. • Dead Time “Free” architecture: • No interruption of writing during readout of a triggered event. • several triggered events can be stored in the SCA waiting for readout. • No on-chip zero suppress: all channels are read for a trigger. Event Trigger latency Write pointer Read Pointer N cells Triggered cells
SCA: Key parameters Fs> 2/Tp (2 samples in the trailing edge) => Fs = 20 MHz for Tpeak =100ns SCA DEPTH = Latency + buffer + extra cells • 8 µs latency => 160 cells. • 10 events derandomizing buffer => 40 cells • SCA depth = 256 512 cells is feasible
Main advantages of this solution • Charge is directly measured. • Oscilloscope-like operation makes diagnostics easier. • The timing can be accurately calculated from the samples: • better than 1/Fs precision: In ATLAS LARG ECAL 1ns rms timing performed with FS=40 MHz (and tp=50ns) • Pile-up can be detected and even corrected. • Common mode noise can be calculated and subtracted. • Low frequency noise can be partially eliminated (by subtracting baseline samples). • Operations are performed before zero-suppress (discrimination)
L1 Accept Common mode Noise extract + subtraction FE CHIP Timing Extraction + filter Zero Suppress ADC Analog sampling solution (APV-like solution) • Data flow for the whole MM tracker~ 1600 MByte/s @ the ADC output. • Becomes 20 MByte/s after zero suppress. • Can be reduced by 3 if an online filtering on timing is performed. • For: • Simple & Proven • Very robust to bad grounding & pickup (common mode node correction) • Expertise of Saclay on SCAs • Against: • Need for high frequency ADC & FPGAs close to the very front-end. • Not self triggered • Need for a L1accept “fast” and synchronous.
Short term plans. • VFE part with 50ns shaping is currently designed for the AGET project. • No manpower in microelectronics for this project before April 2010. • Before summer 2010: Submission of a small size FE chip prototype : • 16 channels x 128 cells for lower prototype cost. • Test during the fall. • Check the possibility to use APV: • “successful test” with new large Micromégas of COMPASS last summer , but detailed analysis of beam data are required to check the efficiency).
CLAS12 & ATLAS Muon Chambers. • A lot of similar requirements. • Main difference: No auto-triggering/ need to provide fast signal for L1 trigger in the case of CLAS12. • We are open to collaborations => share expertise, cost & manpower. • As the real work on the CLAS12 chip has not really started, we can still change the selected option. • But CLAS12 tracker schedule is very tight.