Title: Achievements
1Achievements Perspectives of MIMOSA Sensors
(MAPS) for Vertexing ApplicationsChristine
Hu-Guo (IPHC)on behalf of IPHC (Strasbourg)
IRFU (Saclay) collaboration
- Outline
- Achieved MAPS (Monolithic Active Pixel Sensors)
performances - RD for improving MAPS performances
- Increase readout speed ? Fast readout
architecture - Applications and perspectives
- Improve radiation tolerance
- Projection beyond present (2D sensors)
perspectives - Conclusion
2Development of MAPS for Charged Particle Tracking
- In 1999, the IPHC CMOS sensor group proposed the
first CMOS pixel sensor (MAPS) for future vertex
detectors (ILC) - Numerous other applications of MAPS have emerged
since then - 10-15 HEP groups in the USA Europe are
presently active in MAPS RD - Original aspect integrate sensitive volume (EPI
layer) and front-end readout electronics on the
same substrate - Charge created in EPI, excess carries propagate
thermally, collected by NWELL/PEPI , with help
of reflection on boundaries with P-well and
substrate (high doping) - Q 80 e-h / µm ? signal lt 1000 e-
- Compact, flexible
- EPI layer 1015 µm thick
- thinning to 3040 µm permitted
- Standard CMOS fabrication technology
- Cheap, fast multi-project run turn-around
- Room temperature operation
- Attractive balance between granularity, material
budget, radiation tolerance, read out speed and
power dissipation - BUT
- Very thin sensitive volume ? impacts signal
magnitude (mV!) - Sensitive volume almost un-depleted ? impacts
radiation tolerance speed - Commercial fabrication (parameters) ? impacts
sensing performances radiation tolerance
R.T.
3Achieved Performances with Analogue Readout
- MAPS provide excellent tracking performances
- Detection efficiency 100
- ENC 10-15 e-
- S/N gt 20-30 (MPV) at room temperature
- Single point resolution µm, a function of pixel
pitch - 1 µm (10 µm pitch), 3 µm (40 µm pitch)
4Radiation tolerance (preliminary)
- Ionising radiation tolerance
- O(1 M Rad) (MIMOSA15, test cond. 5 GeV e-, T
-20C, tint180 µs) - tint ltlt 1 ms, crucial at room temperature
- Non ionising radiation tolerance depends on
pixel pitch - 20 µm pitch 2x1012 neq /cm2 , (Mimosa15, tested
on DESY e- beams, T - 20C, tint 700 µs) - 5.81012neq/cm² values derived with standard and
with soft cuts - 10 µm pitch 1013 neq /cm2 , (MIMOSA18, tested at
CERN-SPS , T - 20C, tint 3 ms) - parasitic 12 kGy gas ? N ?
- Further studies needed
- Tolerance vs diode size, Readout speed, Digital
output, ... , Annealing ??
Integ. Dose Noise S/N (MPV) Detection Efficiency
0 9.0 1.1 27.8 0.5 100
1 Mrad 10.7 0.9 19.5 0.2 99.96 0.04
Fluence (1012neq/cm²) 0 0.47 2.1 5.8 (5/2) 5.8 (4/2)
S/N (MPV) 27.8 0.5 21.8 0.5 14.7 0.3 8.7 2. 7.5 2.
Det. Efficiency () 100. 99.9 0.1 99.3 0.2 77. 2. 84. 2.
Fluence (1012neq/cm²) 0 6 10
Q cluster (e-) 1026 680 560
S/N (MPV) 28.5 0.2 20.4 0.2 14.7 0.2
Det. Efficiency () 99.93 0.03 99.85 0.05 99.5 0.1
5System integration
- Industrial thinning (via STAR collaboration at
LBNL) - 50 µm, expected to 30-40 µm
- Ex. MIMOSA18 (5.55.5 mm² thinned to 50 µm)
- Development of ladder equipped with MIMOSA chips
(coll. with LBNL) - STAR ladder (lt 0.3 X0 ) ? ILC (lt0.2 X0 )
- Edgeless dicing / stitching ? alleviate material
budget of flex cable
6MAPS performance Improvement
RD organisation 4 (5) simultaneous prototyping
lines
- ?Architecture of pixel array organised in //
columns read out - Pre-amp and CDS in each pixel
- A/D 1 discriminator / column (offset
compensation) - Power vs Speed
- Power ? Readout in a rolling shutter mode
- Speed ? Pixels belonging to the same row are read
out simultaneously - MIMOSA8 (2004), MIMOSA16 (2006), MIMOSA22
(2007/08)
- ?Zero suppression circuit
- Reduce the raw data flow of MAPS
- Data compression factor ranging from 10 to 1000,
depending on the hit density per frame - SUZE-01 (2007)
- ?45 bits ADCs (103 ADC per sensor)
- Potentially replacing column-leveldiscriminators
- 5 bits ?sp 1.71.6 µm 4 bits ?sp lt 2 µm for
20 µm pitch - Next step integrate column-level ADC with pixel
array
- ?Serial link transmission with clock recovery
- Prototype (2008-2009)
?Voltage regulator DC-DC converter
7MIMOSA22 SUZE-01 Test Results
- MIMOSA22 (15 µm EPI) 136 x 576 pixels 128
column-level discriminators - SUZE-01
- Lab. test
- Laboratory test
- Temporal Noise 0.64 mV ? 12 e-
- FPN 0.22 mV ? 4 e-
- Beam test at CERN SPS (120 GeV pions)
- Threshold 4 mV ? 6 x s noise
- Detection Efficiency gt 99.5
- Single point resolution lt 4 µm
- Fake rate lt 10-4
8MIMOSA26 1st MAPS with Integrated Ø
CMOS 0.35 µm OPTO technology, Chip size 13.7 x
21.5 mm2
- Pixel array 576 x 1152, pitch 18.4 µm
- Active area 10.6 x 21.2 mm2
- In each pixel
- Amplification
- CDS (Correlated Double Sampling)
- Integration time 100 µs
- ? R.O. speed 10 k frames/s
- Hit density 106 particles/cm²/s
- Testability several test points implemented all
along readout path - Pixels out (analogue)
- Discriminators
- Zero suppression
- Signal transmission
- Row sequencer
- Width 350 µm
- 1152 column-level discriminators
- offset compensated high gain preamplifier
followedby latch
- Reference Voltages Buffering for 1152
discriminators
- I/O PadsPower supply PadsCircuit control
PadsLVDS Tx Rx
- Memory management
- Memory IP blocks
- Readout controller
- JTAG controller
9Test MIMOSA26 (Lab. beam test)
- Measured temporal noise 0.6-0.7 mV and FPN
0.3-0.4 mV for pixel array with its associated
discriminators. - These values are equivalent to those obtained
with Mimosa22. - It shows a good uniformity of the whole 576 x
1152 pixels with the 1152 discriminators - 30 MIMOSA26 chips are tested (only 1 "dead")
- The characterization of Mimosa26 is complemented
by the beam tests (Sept. 2009) - 6 MIMOSA26 chips running simultaneously at
nominal speed - Tracking successful
- data analysis is underway, preliminary results
show similar performances as MIMOSA22
10MIMOSA26 Final Sensor for EUDET Beam Telescope
- EUDET supported by the European Union in the 6th
Framework Programme - Provide to the scientific community an
infrastructure aiming to support the detector RD
for the ILC - JRA1 (Joint Research Activity) High resolution
pixel beam telescope (BT) - Two arms each equipped with three layers of pixel
sensors (MIMOSA) - DUT is located between these arms and moveable
via X-Y table -
-
- EUDET beam telescope specifications
- High extrapolated resolution lt 2 µm
- Large sensor area 2 cm2
- High read-out speed 10 k frame/s
- Hit density up to 106 hits/s/cm2
Pixel Sensor
MIMOSA26
13.7 mm
(DUT)
21.5 mm
Being Mounted on EUDET beam telescope
- Preliminary test results from the EUDET
collaboration - 3 MIMOSA26 chips mounted as DUT in BT
demonstrator in July - BT tracks reconstructed in the 3 planes ?
residues compatible with ssp 3.5-4 µm
11Extension of MIMOSA-26 to STAR
- Final HFT (Heavy Flavour Tracker) - PIXEL sensor
- MIMOSA-26 with active surface 1.7
- 1088 col. of 1024 pixels ? 1.1 million pixels
- Pitch 18.4 µm ? (20.0 x 18.8 mm²)
- Integration time 200 µs
- Design from now ? fab. Feb. 2010
- 1st physics data expected in 2011/12
- Critical points
- Reduction of power consumption
- Radiation tolerance improvement
- Also
- Integrated voltage reference
- High speed transmission
Pixel Vx Detector
22.4 mm
Inner Layer 10 ladders
Outer Layer 30 ladders 10 sensors / ladder
20.4 mm
STAR Detector Upgrade
12Extension of MIMOSA-26 to CBM/FAIR ILC
- Micro Vertex Detector (MVD) of the CBM H.I. fixed
target expt - 2 double-sided stations equipped with MIMOSA
sensors - MIMOSA-26 with double-sided read-out ? readout
speed ! - Active surface 2 x 1152 columns of 256 pixels
- 21.2 x 9.4 mm2
- tint. 40 µs
- lt 25 µs in lt 0.18 µm techno.
- Prototyping until 2012 ? start of physics in
2013/14 (?) - Vertex detector of the ILC
- tint. 25 µs (innermost layer) ? double-sided
readout - tint. 100 µs (outer layer) ? Single-sided
readout - 2 µm (4-bit ADC, 20 µm) lt ?sp lt 3 µm (discri. 14
µm pitch) - Pdiss lt 0.11 W/cm² 1/50 duty cycle
-
ILD design 2 options
- Critical points
- Power pulsing
- Design for the innermost layer
- Small pixel pitch
- Faster readout speed
3 double layers
5 single layers
13Radiation Tolerance Improvement
- Ionising radiation tolerance 1. Special layout
- Diode level (already realized) Remove thick
oxide surrounding N-well diode by replacing with
thin-oxide? without design rule violation!! - Pixel circuit level ELT for the transistors
connected to the detection diode - 2. Minimise integration time ? Increase readout
speed - Minimise leakage current
14Radiation Tolerance Improvement
- Non ionising radiation toleranceHigh resistivity
sensitive volume ? faster charge collection - Exploration of a VDSM technology with depleted
(partially 30 µm) substrate - Project "LePix" driven by CERN for SLHC trackers
(attractive for CBM, ILC and CLIC Vx Det.) - Exploration of a technology with high resistivity
thin epitaxial layer - XFAB 0.6 µm techno 15 µm EPI (? O(103)?.cm),
Vdd 5 V (MIMOSA25) - ? Benefit from the need of industry for
improvement of the photo-sensing elements
embedded into CMOS chip
TCAD Simulation 15 µm high resistivity EPI
compared to 15 µm standard EPI
For comparison standard CMOS technology, low
resistivity P-epi
high resistivity P-epi size of depletion zone
size is comparable to the P-epi thickness!
15MIMOSA25 in a high resistivity epitaxial layer
MIMOSA25
saturation -gt gt90 of charge is collected is 3
pixels -gt very low charge spread for depleted
substrate
16x96 Pitch 20µm
To compare standard non-depleted EPI
substrate MIMOSA15 Pitch20µm, before and after
5.8x1012 neq/cm2
- 20 µm pitch, 20C, self-bias diode _at_ 4.5 V, 160
µs read-out time - Fluence (0.3 / 1.3 / 3)1013 neq/cm2
- Tolerance improved by gt 1 order of mag.
- Need to confirm ?det (uniformity !) with beam
tests
16Using 3DIT to improve MAPS performances
- 3DIT are expected to be particularly beneficial
for MAPS - Combine different fabrication processes
- Resorb most limitations specific to 2D MAPS
- Split signal collection and processing
functionalities, use best suited technology for
each Tier - Tier-1 charge collection system ? Epitaxy
(depleted or not), deep N-well ? ? ultra thin
layer? X0 ? - Tier-2 analogue signal processing? analogue, low
Ileak, process (number of metal layers) - Tier-3 mixed and digital signal processing
- Tier-4 data formatting (electro-optical
conversion ?) - Run in Chartered - Tezzaron technology
- 130 nm, 2-Tier run with "high"-res substrate
(allows m.i.p. detection) - Tier A to tier B bond? Cu-Cu bond
- 3 D consortium coordinated by FermiLab
- FermiLab
- INFN
- IN2P3-IRFU
- Univ. of Bonn
- CMP
17IPHC IRFU 3D MAPS
- Delayed R.O. Architecture for the ILC Vertex
Detector - Try 3D architecture based on small pixel pitch,
motivated by - Single point resolution lt 3 µm with binary output
- Probability of gt 1 hit per train ltlt 10
- 12 µm pitch
- ?sp 2.5 µm
- Probability of gt 1 hit/train lt 5
- Split signal collection and processing
functionalities - Tier-1 A sensing diode amplifier, B shaper
discriminator - Tier-2 time stamp (5 bits) overflow bit
delayed readout - ? Architecture prepares for 3-Tier perspectives
12 µm - Tier-1 CMOS process adapted to charge collection
- Tier-2 CMOS process adapted to analogue mixed
signal processing - Tier-3 digital process (ltlt 100 nm ????)
18IPHC 3D MAPS Self Triggering Pixel Strip-like
Tracker (STriPSeT)
- Combine Tezzaron/Chartered 2-tiers process with
XFAB high resistivity EPI process - Tier-1 XFAB, 15 µm depleted epitaxy ? ultra thin
sensor!!! - Fully depleted ? Fast charge collection (5ns) ?
should be radiation tolerant - For small pitch, charge contained in less than
two pixels - Sufficient (rather good) S/N ratio defined by the
first stage - charge amplification ( gtx10) by capacitive
coupling to the second stage - Tier-2 Shaperless front-end (Pavia Bergamo)
- Single stage, high gain, folded cascode based
charge amplifier, with a current source in the
feedback loop ? Shaping time of 200 ns very
convenient good time resolution - Low offset, continuous discriminator
- Tier-3 Digital Data driven (self-triggering),
sparsified binary readout, X and Y projection of
hit pixels pattern - Matrix 256x256 ? 2 µs readout time
- DBI Direct Bond Interconnect, low temperature
CMOS compatible direct oxide bonding with
scalable interconnect for highest density 3D
interconnections (lt 1 µm Pitch, gt 108/cm /cm²
Possible)
19IRFU IPHC 3D MAPS RSBPix
- FAST R.O. architecture aiming to minimise power
consumption - Subdivide sensitive area in small matrices
running INDIVIDUALLY in rolling shutter mode - Adapt the number of raws to required frame r.o.
time - ? few µs r.o. time may be reached (???)
- Planned also to connect this 2 tier circuit to
XFAB detector tier
20Conclusion
- 2D MAPS have reached necessary prototyping
maturity for real scale applications - Beam telescopes allowing for ?sp few µm 106
particles/cm²/s - Vertex detectors requiring high resolution very
low material budget - The emergence of fabrication processes with
depleted epitaxy / substrate opens the door to - Substantial improvements in read-out speed and
non-ionising radiation tolerance - "Large pitch" applications ? trackers (e.g. Super
LHC ) - Translation to 3D integration technology
- Resorb most limitations specific to 2D MAPS
- T type density, peripheral insensitive zone,
combination of different CMOS processes - Offer an improved read-out speed O(µs) !
- Many difficulties to overcome (ex. heat, power)
- RD in progress ? 2009/10 important step for
validation of this promising technology