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Development of Detectors for
Speckles – use of 3D-IC
Grzegorz (Gregory) Deptuch
Fermilab
Basic Energy Sciences Detector Workshop 2012
August 1-3, 2012
Outline
• Introduction:
• Motivation at Fermilab
• Collaboration benefits
• R&D on Intelligent pixels
• 3D-IC, introduction and program progress
• VIPIC1 and direction on VIPIC2
• Glance of SOI
• Comment on Future and Resources
• Conclusion
Basic Energy Sciences Detector Workshop 2012 2
• Activity of the ASIC Development Group at
Fermilab, whose role is to provide integrated circuits
for detectors to build experiments
• Primarily: advanced instrumentation for HEP;
• Secondarily: where synergies and where appropriate
- leverage technologies for other fields and work
through collaborations
Motivation at Fermilab
3 Basic Energy Sciences Detector Workshop 2012
Vertically Integrated Photon Imaging Chip
Detector: Si 500 mm thick sensors, soft X-rays
• Develop practices and techniques applicable later in devices for HEP
• Intelligent pixels (output of processed information, incl. inter-pixel communication)
• No device of targeted functionality available (2D autocorr. @~10ms or better)
• Immediate application in producing science on a light source
(DBI®) oxide-oxide bonding
Collaboration benefits • Collaborating institutions:
• BNL: Peter Siddons and Gabriella Carini (now SLAC)
• AGH-UST, Krakow Poland, Pawel Grybos
• and industrial partners: Tezzaron (IL), Ziptronix (NC) + …
4 Basic Energy Sciences Detector Workshop 2012
6”, 500mm thick sensor wafer for
ALL 3D pixel chips from Fermilab 1st 3D MPW
(designed at Fermilab masks and fabbing at BNL),
Fermilab and BNL partnered to develop 3D integrated No funds flow FermilabBNL
• Fermilab builds ASIC for XPCS
• BNL build sensors for XPCS and
Fermilab HEP projects
5 Basic Energy Sciences Detector Workshop 2012
• Through Silicon Vias (TSV): vertical wafer/chip connectivity
• Bonding: Oxide, polymer, metal, or adhesive strengthened (W-W, C-W, C-C) - not only for electronic chips but also for attaching detectors to readouts
• Wafer thinning: aggressive and precise
• Back-side: metallization and patterning
A chip in three-dimensional integrated circuit (3D-IC) technology
is composed of two or more layers of active electronic
components, integrated both V & H
MIT-LL
3D-IC process
FDSOI oxide-
oxide bonding
Face-Face
Back-Face
Face-Face
Tezzaron 3D-IC
bulk CMOS Cu-Cu
thermocompression
or DBI bonding TS Vias
(f=1mm)
3D-IC: definition
Basic Energy Sciences Detector Workshop 2012
3D-IC: benefits • Current fine-grained detector technologies has been facing serious
limitations; incremental improvements have proved inadequate
• 3D integration offers a transformational change to address current roadblocks to advance detectors in these areas
• 3D ROICs - complete separation of digital activity from low-noise
analog parts
• 3D ROICs - uniform distribution of power supply and I/O pads on
the back side
• ROICs can be integrated with sensors without bump-bonds
Strategic : 4 side buttable, dead-area-free detectors for use from X-ray, visible, IR imaging to classical tracking 6
Basic Energy Sciences Detector Workshop 2012
3D-IC status from Fermilab perspective
7
• Initially small efforts started with MIT-LL 3D
process in 2006 (DARPA 3-tier 3D run):
• stimulated great interest among the detector
community worldwide and move to Tezzaron/GF
• 3D-IC Consortium established in late 2008, now
17 members; 6 countries: USA, Italy, France, Germany,
Poland, Canada) + Tezzaron – various goals among members
• Fermilab organized first 3D-IC MPW run for HEP
• Designs in: 05/2009; Chartered (GF) 130nm
• Fermilab had a role of silicon broker
• Many challenges in working with cutting edge technology
• MPW frame accepted for fab in 03/2010
• 3D bonding did not yield for initial lot of wafer, • Fermilab MPW in fab in parallel with 2 other runs (DARPA
and SNL) – they were successful
• 3D bonding not successful on almost all wafer pairs from 1st lot
• 2nd lot is in bonding now
• 1st working chips obtained from 2 bonded
pairs of wafers in 06/2012
• 3D-IC MPWs
available now
from MOSIS
GF/Tezzaron wafer for 3D chips from
Fermilab MPW run before 3D bonding
Single mask set used to fabricate top and
bottom tier chips on the same wafer;
Bonding occurs by folding wafers over
symmetry line
• Main objectives of demonstration of 3D program has been achieved (Cu-Cu TC and Cu-Cu DBI bonding), but:
• limited number of available 3D dies
• need to make a connection to sensors
• Important
• Back-grinding down to TSVs’ tips and full back side processing to create Al pads!
Basic Energy Sciences Detector Workshop 2012
3D-IC: post foundry
8
TSVs
Aluminum oxide
Back-thinned
Cu TC Bond at EVG with 1st good 3D chips!
chips with pads
to a sensor DBI
or
Au stud bonding
chips with pads
distributed on
whole back
surface
3D-IC: it works
Basic Energy Sciences Detector Workshop 2012 9
Long strip tier
threshold
noise
• VICTR chip (track-triggering in HL-CMS) shown operational
• VIPIC tests - underway, communication with chip workings – so far good!
Analog
signals
Top detector
Amp/disc cluster
and stub formation
Interposer
Long (1 cm) strips
Short (1.25 mm) strips
Basic Energy Sciences Detector Workshop 2012
VIPIC1 and future direction
10
time Standard XPCS analysis: multi-tau
correlator Probes correlations between intensity
fluctuations at times 0 and 0+t with 2D
resolution
Ultimately, every pixel outputting sequences of
correlation coefficients, in meantime:
LP and LN (low threshold), time-of arrival, max
DQE by charge sharing correction, fast-
-continuous output device
Intelligent pixels:
• Exchange information/data with neighbors
• Perform in-situ processing
• Detector outputs smaller quantity of digested
results – not always image in the strict sense
Set of XPCS methods is one of customer who
needs pixel detectors w. 2D+ hidden dimensions
To approach dreams:
• A lot of transistors / pixel is
required, which is becoming
enabled by nm processes,
3D-IC or both!
1000 Mpixels; 1μm pitch;
1ns frame rate; no dead time;
100% efficiency at all energies;
100 bit dynamic range;
cost free
Basic Energy Sciences Detector Workshop 2012
VIPIC1: architecture
11
Architecture of VIPIC1 oriented on XPCS
How it works:
• Continuously, in
dead-time-less way
outputs hits on 16
parallel outputs
from 64×64 matrix
of pixels using
priority encoder
based sparsification
method
• 5 bit long content of
pixel counters
followed by 8 bit
long address of hit
pixel
• Die size:
5.5×6.3mm2
Basic Energy Sciences Detector Workshop 2012
VIPIC 1: Pixel architecture and layouts
12
Digital:1400 transistors / pixel Analog: 280 transistors / pixel
Pix
el
80x80 m
m2
• Pseudo-differential CSA-shaping filter-discriminator
• shaping time tp=250 ns, power ~25 mW / analog pixel,
noise <150 e- ENC, optimized for 8 keV
• 12 bit/pixel DAC adjustments
•
• 2 dead-time-less modes:
• timed readout address and hit count st=~ 10ms
• imaging – counting of events
• 2 5 bit-long counters / pixel (counting limited by
duration of analog signals), RO with sparsification but
clamping addresses: tread= (fclk)-1×(3+5) bits×4×64<20ms
• ‘Set’ + ‘Kill’ bits/pixel
Basic Energy Sciences Detector Workshop 2012
VIPIC 1: Pixel analog details
13
Analog tier
Digital tier
Basic Energy Sciences Detector Workshop 2012
VIPIC 1: Pixel digital details
14
Part of config. shift register;
Pixel permanently reset (no
hits) or set (always hit)
During Dtn hits from Dtn+1
go to ‘waiting room’
rising edge of TS_Clk shifts
hits to ‘service room’ where
they are ready for readout
Read acknowledge
from priority encoder
Prevents counting hits
twice (requests dis_in ‘LOW’
after rising edge of TS_Clk )
Ambiguous: discriminator
being high at the boundary
of adjacent time slices
Global RStrobe removes
hit from read-out queue
Basic Energy Sciences Detector Workshop 2012
VIPIC 1: 4 side-buttable detector
15
Fan-out on the detector; detector attached
on the back of analog tier, pads bonded to
the traces on the detector and redistributed
outside of the chip contour for bonding
2 steps to demonstrate 4-side buttable
detectors,
2 bonding options and placement of I/O,
power supply and bias pads: One side bonded to the detector - opposite
side bonded to the PCB board; all I/Os,
power and bias connection transferred to
the digital tier
Basic Energy Sciences Detector Workshop 2012
VIPIC 2: Intelligent pixels
16
Maybe still intelligence of a bacteria, but at
least direction is on evolution …
Central hit no charge sharing
Side hit max charge sharing
defeat charge sharing (degrades DQE,
amplitude and timing spectroscopic
performances) in X-ray detectors dynamic
cluster reconstruction in tracking detectors
100×100mm2, 130nm GF, 2k transistors / pixel
New algorithm for full event charge
• Each pixel is an asynchronous processor
(machinery), exchanging data with
neighbors
• Applied directly in X-ray science, but may
be ported to cluster reconstruction in HEP
Basic Energy Sciences Detector Workshop 2012
VIPIC 2: comparison of signals
17
System challenge: must be asynchronous and self organized
Circuit challenge: must use feature of signal given least ambiguity
a) TOT, b) amplitude
We concluded:
for equal noise comparison of
amplitude of two signals
should provide better
performance
amp1
amp2
tot1
tot2
Basic Energy Sciences Detector Workshop 2012
VIPIC 2: C8P1 algorithm
18
C8P1 algorithm:
• Continuous summing of signals from neighbors in every pixel,
• Triggering on S>threshold (fast shaper) and performing all way comparisons
(slow shaper) and latching one winning pixel (seed of cluster)
• miniVIPIC2 is 2D in preparation for 3D “clock” generated
from fast shaping filter that
gets summed ‘on wire’ signals
from all 4 neighbors; duration
of fast signal is chosen to
latch;
Comparators are auto-0’ed, reset
when fast shaping filter is below
threshold
Basic Energy Sciences Detector Workshop 2012 19
ToA measurement with C8P1 algorithm:
• Every pixel has TDC (triggered by fast shaper discriminator):
• 10 bit counter with external clock reference in prototype
• 10 bit counter with local (per pixel) oscillator in final chip
• TDC performs precise measurement within alternating time slots
VIPIC 2: C8P1 algorithm c’d
summing, fast shaper, discriminator all directions comparisons
Basic Energy Sciences Detector Workshop 2012 20
Analog chain of the C8P1 algorithm:
• AC coupling CSA- to- shaping filters,
• Signals summed in charge domain (less sensitive to systematic)
VIPIC 2: C8P1 algorithm c’d
miniVipic2 chip (prototype before next
3D run) submitted in 02/2012 – tests
has just been started
Basic Energy Sciences Detector Workshop 2012
Silicon On Insulator (SOI) pixels
21
• Collaboration established with KEK and under a Japan-US agreement (MoU
2007) on monolithic SOI devices + OKI/LAPIS (industrial partner).
• also domestically with ASI through SBIR
process was a slightly modified version of a commercial FD SOI process at the beginning
Suffering from strong back-gating and generally coupling between sensor and electronics
Electronics
+
sensor
Unity, without
post-foundry bonding
Basic Energy Sciences Detector Workshop 2012
SOI pixels: Fermilab process improvement
22
– Triple role of shielding between the SOI electronics and detector layer:
• to avoid back-gating in transistors (DC potential underneath the BOX shifts threshold of transistors),
• to avoid injection of parasitic charges (from the SOI electronics to detector),
• to avoid strong electric field in BOX (that results in accelerated radiation damage).
This well separates digital circuits
from sensor substrate and
prevents back gating effects
This well collects
the charge carriers
SILVACO
process simulatiom
• Simulation with Silvaco
• Feature introduced in the
design kit together with
scientist from KEK and
engineers from OKI/LAPIS
improvement proposed
by Fermilab
109Cd source (22keV X-rays) with MAMBO 5 – submission cost
covered by US-Japan funds Basic Energy Sciences Detector Workshop 2012
SOI pixels: Results
23
First images obtained with counting (150ns) SOI pixel detector PCB
(1.9×1.9mm2) square W mask flat field
– Started in 2006, a sequence of counting MAMBO chips developed:
• gradually improve circuitry and understand better the technology
24
• Development of pixel detectors in the USA has been significantly less dynamic
than for example in Europe
• It is money hungry
• It is resource hungry
• It is technology hungry
• ……. but enables science
• For Fermilab (known to be uni-purpose HEP lab) pixels for XPCS are an
interesting R&D projects with the challenges, where the 3D-IC technology
shows its claws,
• Intelligent pixels = direction for much higher level of in-situ processing
• Intensified work at Fermilab on selected directions, ex.:
• 3D-IC technology for a wide spectrum of scientific uses
• and pixels: HL-CMS pixels upgrade and tracking-triggering, lepton collider, etc.
• Leveraging of Fermilab developments in pixels would mutually be beneficial – some level of funding for SR should be assured
Conclusions
Basic Energy Sciences Detector Workshop 2012