Pixel readout electronics development for ALICE PIXEL VERTEX and LHCb RICH W. Snoeys, M. Campbell, E. Cantatore, V. Cencelli*, R. Dinapoli**, E.

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Presentation transcript:

Pixel readout electronics development for ALICE PIXEL VERTEX and LHCb RICH W. Snoeys, M. Campbell, E. Cantatore, V. Cencelli*, R. Dinapoli**, E. Heijne, P. Jarron, P. Lamanna**, A. Marchioro, D. Minervini**, V. Quiquempoix, D. San Segundo Bello***, B. van Koningsveld, K. Wyllie EP Division - CERN, Geneva *Rome III university **INFN and Politecnico Bari ***Nikhef Walter, how about alphabetical order, and underlining the name of the speaker ?

Outline Previous full readout chips Two testchips Omega2 Omega3/LHC1 Two testchips 0.5 mm CMOS 0.25 mm CMOS New chip for ALICE pixel and LHCb RICH Chip description Design for radiation tolerance Design for testability Design for uniformity Special issues Conclusions

Omega2 Binary position information Pixel 75x500 mm2, 64 rows by 16 columns Leakage current sensing cell at the bottom of each column Internal delay per pixel (current deprived invertors), dead for twice the trigger delay Shift register readout after level 1 trigger Limited testability : only one test row at the top Two metal layers only : no shielding between electronics and detector ~ 80 transistors/pixel (Self Aligned Contact 3 mm technology) Dies at < 50krad

Omega3/LHC1 Discriminator A Pixel 50x500 mm2, 128 rows by 16 columns Internal delay per pixel (current deprived invertors), front end reset after small fraction of the trigger delay Shift register readout after level 1 trigger All pixels can be tested electrically Third metal shield ~ 380 transistors/pixel (Self Aligned Contact 1 mm technology Dies at < 50krad Discriminator (see left) trade-off between threshold uniformity and speed Preamplifier feedback A Discriminator

Omega3 testability gave a wealth of information Top-down threshold variation due to resistive drop fixed in correction run

3 bit delay adjust on half plane (~ 50 000 channels) Before After

Omega2 and Omega3 worked well (CERN RD-19, WA97 and NA57) LHC1 : 2000 CMOS readout channels Pixel Ladders (6 chips) WA97 NA57 Experiment 1.2 M channels Half plane ~ 50 000 sensing elements

Two test chips in commercial submicron CMOS 2 columns of 64 pixels + 1 test pixel with analog outputs radiation tolerant layout 2 by 5 mm2 full mixed mode circuit LHC2TEST/ALICE1TEST 0.5 mm CMOS 25000 transistors ALICE2TEST 0.25 mm CMOS 50000 transistors

Iout to current comparator Changes in front end Preamplifier Shaper In Vbias Iout to current comparator Threshold setting IN Cfb OUT Vref DC level of input and output no longer coupled Leakage current compensation ref : F. Krummenacher, Nucl. Instr. and Meth., Vol. A305 (1991) 527-532 Change in discriminator for speed, went to current comparator

0.5 mm test chip Leakage current compensation works (for both signs of leakage) Timewalk LHC compatible

0.5 mm test chip : evolution of Threshold and Threshold Variation with Xray Dose Supply currents virtually unaffected during the irradiation ! Circuit dies around 1 Mrad because of transistor Vt-shifts which are still non-neglegible in 0.5 mm Confirmed for electrons, and for (cfr. F. Meddi et al.) gamma-rays and protons

0.5 mm test chip : conclusions Threshold dispersion too large : edgeless transistor show much larger mismatch (see left) => need other front end topology Motivations to go deeper submicron : Need more density Will get even higher radiation tolerance Need for further modeling of edgeless transistors Mismatch for edgeless transistors cfr. G. Anelli et al.

0.25 mm testchip Input structure Test FF Front end Delay 160 mm 420 mm 125 mm Mask FF + R/O mm 60 80 Eliminated the current mirror (cfr ISSCC 2000) and shrunk the front end from 260 mm to 125 mm Put synchronous delay (one column static, other dynamic) in the empty space and kept other logic identical to 0.5 mm version 50 mW per pixel Noise 220-250 e- rms Threshold dispersion 160 e- rms before 3 bit adjust, 25 e- rms after Used three metals only

Supply currents virtually unaffected during the irradiation ! 0.25 mm test chip : 10 keV X-ray Irradiation Pixel Threshold, Threshold Dispersion and Noise Vs Total Dose Supply currents virtually unaffected during the irradiation !

Proton irradiation in NA50 2mm Threshold and noise on hit column after proton irradiation and 4 hour anneal @ room temperature (Note: 1 mV = 100 e-) 2mm 3.6 x 1013 protons/4mm2 => 9 x 1014 protons/cm2

Proton irradiation in NA50 Conclusions Also withstands non-uniform irradiation Did not see any evidence of hard failure, i.e gate rupture... Threshold change and noise after proton irradiation and 20 hour anneal @ room temperature Note: 1 mV = 100 e-

Conclusions from test chips Challenges for full chip Speed, threshold uniformity and radiation tolerance (total ionizing dose and single event upset) proven Need to further characterize enclosed devices Challenges for full readout chip : Architecture for two different applications Large occupancy in LHCb, need to minimize dead time Readout (=digital activity) while being sensitive Large chip Large system : testability, uniformity Design for radiation tolerance : design implications revisited

Two applications : pixel for tracking/vertex finding in ALICE Half Stave ladder2 ladder1 10 chips of one half-stave read out sequentially in 400ms 120 half-staves read out in parallel Minimal mass, thin sensors => 12 000 e- most probable signal Spatial resolution of 12mm in r-f => 50 mm pixel pitch 1% average occupancy Level-1 trigger : latency of 5.5ms, few kHz rate, buffering on chip Full event readout in 400ms (deadtime about 10%), 10 MHz clock Radiation tolerant to ~ 500 krad

And… LHCb RICH : encapsulation of pixel chip-sensor assembly in HYBRID PHOTON DETECTOR for particle ID Single photons yield 5000e- signal with 20kV accelerating potential 2.5mm x 2.5mm channel size, 5 x demagnification => 500mm  500mm granularity 8% maximum occupancy 40 MHz event rate, also readout clock 1MHz average Level 0 trigger rate Buffering of Level-0 triggered events (latency of 4 ms) Readout of triggered event in 900ns (deadtime  1%)

New 8000 channel chip : pixel Shaper filter Comparator coinc logic 4-bit FIFO data FF delay Preamp 8 BCO Thres. strobe R W Cin 3 test FF th adj FFs mask FF Walter, is the text at the bottom of the picture necessary ? analog test input

Two applications : architectural solution ALICE mode of operation

Two applications : LHCb mode of operation

FRONT END Differential to reject substrate and supply noise Closed loop complex poles for fast return to zero to be immune to pile-up of subsequent signals

Pixel Cell : digital part Delay : stores a hit for duration of trigger latency latches the time-stamp of a hit from a periodic Gray-encoded pattern (modulo n) on an 8-bit bus FIFO : Read/write addressable by Gray encoded bus Risk of switching noise coupling into analog circuitry is reduced by: Gray encoding of patterns on busses Current starved logic cells

layout for radiation tolerance everywhere Pixel cell 125mm pre-amp (differential) shaper (differential) discriminator (+ fast-OR) 60mW static consumption 265mm two digital delay units trigger coincidence logic 4-event FIFO buffer readout logic 35mm 5 un-upsettable latches for configuration test input on/off pixel mask on/off 3 bits of threshold adjust 6 metal layers 1500 transistors/pixel layout for radiation tolerance everywhere

Periphery and I/O Periphery contains: Counters to generate timestamp Counters to address FIFO buffers 8-bit DACs to provide voltage and current references for analog circuitry and current-starved logic I/O pads :Single-ended : Gunning Tranceiver Logic (GTL) Low swing Slew rate control Separate supply for output buffers Multiple bonding pads for supply lines to reduce inductance and limit on-chip power supply bounce during switching

Design for testability Configuration of peripheral logic and pixel cells by means of JTAG serial interface - allows both write and read of configuration settings (test,mask….) reading back of analog levels (currents & voltages) generated by DACs connectivity tests of chips on stave using boundary scan allows detection of bad chips on stave Every pixel can be addressed individually for testing using analog input

Very important fine print Single event effects : Single event induced latch-up : radiation tolerant layout very effective also here Single event upset : special SEU hardened flip-flops Power distribution and voltage drops : Motivation for (late) decision to switch from 5 to 6 metal layers Local mirroring of sensitive biases to reduce sensitivity to on-chip resistive drops Digital to analog cross-talk : Slew rate control on all digital Differential frontend

Conclusions Experience from omega2 and omega3/LHC1, and from the two test chips Commercial deep submicron CMOS allows : High component density Radiation tolerance Good speed-power performance Full scale pixel readout chip designed One chip for Alice pixel vertex and LHCb RICH 8000 readout channels 13 M transistors in 14 by 16 mm2 6 metals Testability and system integration Uniformity Important fine print

Conclusions Basic building block in full readout chip : 8 pixels/12 000 transistors in 400 by 425 mm2