ASIC Development for the GLAST Trackerscipp.ucsc.edu/groups/fermi/publications/GTFE64_review.pdf ·...
Transcript of ASIC Development for the GLAST Trackerscipp.ucsc.edu/groups/fermi/publications/GTFE64_review.pdf ·...
November 24, 1997 Robert P. Johnson 1
ASIC Development for the GLAST TrackerRobert P. Johnson
Santa Cruz Institute for Particle Physics
University of California at Santa Cruz
• GLAST Instrument Concept• GLAST Tracker Electronics
Requirements• Analog Channel
• Preamplifier• Shaper• Comparator• Performance
• Readout Architecture
• Front-End Readout Chip• Architecture• Resistors• DACs• Command Decoder• Drivers and Receivers• Simulations• Layout and Verification
• Readout Controller Chip• Hybrids• Kapton Detector Interconnect• Flex Cables and Connectors
November 24, 1997 Robert P. Johnson 2
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
The GLAST Instrument Concept
175
cm
24 cm
24 cm
6 cm
6 cm
Preamps
236
um p
itch
Scintillator Veto
Con
vert
er (
.5 r
l)
Si Strip Detector
Conceptual Design of GLASTGamma Large Area Space Telescope
Cal
orim
eter
(
10 r
l)
8 x 8 ArrayCsI(Tl) XtalsDiode Readout
Com
plet
e G
LA
ST
One
Tow
er M
odul
e of
GL
AS
T
60 c
m
60 cm
7 x 7 Array of Towers
10 Layers of .05 rad length convertereach with xy silicon strips
2 Layers of XY silicon strips only
Gamma Ray
Electron Positron
Trigger and Computer Tray
GLAST conceptual design. (The currentbaseline design is for a 5×5 array of 32-cm square towers, each with 16 x,ylayers.)
An assembly ofidentical modules,each with a vetoshield, a silicon-striptracker, and acalorimeter.
The current trackerbaseline design callsfor 32 cm squaredetector planes, eachwith a 5×5 array of6.4-cm detectors.
November 24, 1997 Robert P. Johnson 3
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Electronics Requirements
• Power less than ≈250 µW/channel, including amplifiers and digital readout.
• Low noise occupancy (<0.05%) and good threshold uniformity.– Expected detector loading is about 1.2 pF/cm × 32 cm = 38 pF.
– Detector thickness is 400 µm, for about 5.3 fC/MIP.
– AC coupled detectors, with 194 µm pitch.
• Microsecond peaking time for the amplifiers.
• Sufficient redundancy to be immune to single-point failures.
• Self triggering.
• Radiation hard to 10 kRad with latch-up immunity.
• <1% dead-time at a 10 kHz trigger rate.
• Sparse readout and data formatting close to the front end.
Challenge: 1.3 million readout channels operating with high reliability ina space environment.
November 24, 1997 Robert P. Johnson 4
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Analog Channel
• A first 16-channel prototype was fabricated and tested one year ago.• Later, a 32-channel version was produced for the recent beam test at SLAC.
– Slightly reduced peaking time (1.3 µs, down from 1.6 µs).– Slightly reduced gain (125 mV/fC, down from 150 mV/fC).– OR gates for trigger output, rather than open drains.
• Extensive bench-top noise measurements have been done on several 16-channel chips.
• 71 32-channel chipswere runsuccessfully in thebeam, but the dataanalysis has onlybegun.
HP CMOS26G process(0.8 µm, 3-metal, N-well)
One beam test module.
November 24, 1997 Robert P. Johnson 5
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Preamplifier Design
• Standard folded cascodeamplifier with 2V bias for thefront end, to save power.
• ≈25 µA bias current set by anexternal resistor.
• Slow differential amplifierstabilizes the bias point andprovides a continuous reset.
• Input impedance ≈5 kΩ gives≈200 ns time constant withGLAST 38 pF detector load.
• Open loop gain: 64 dB at 0 Hz
• Power: ≈90 µW
Preamplifier schematic.
November 24, 1997 Robert P. Johnson 6
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Shaping Amplifier Design
• AC coupling from the preamplifier.
• Conventional cascode amplifierwith capacitive feedback.
• Slow differential amplifier in thefeedback provides the“differentiation” function andstabilizes the output bias point.(Ref.: I. Kipnis, LBNL)
• Open loop gain: 62 dB at 0 Hz
• Voltage gain: ≈26
• Peaking time: ≈1.3 µs
• Pulse shape: reset current sourcemakes a tail that is more linear thanexponential, except at the lowestpulse heights.
• Power: ≈35 µW
Shaping Amplifier Schematic
November 24, 1997 Robert P. Johnson 7
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Comparator Design
• 16-channel & 32-channelprototypes actually had NFETinputs. We need to go to PFETinputs (as shown here) toaccommodate better the biaslevel at the shaper output.
• Conventional two-stagecomparator, with DC couplingfrom the shaper output.
• No current in the second stagein the quiescent state (with noinput signals).
• Only 17µW of quiescent power.
“Old” Comparator Schematic
Old Design
November 24, 1997 Robert P. Johnson 8
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Comparator Design
New Design• Pavel preferred the symmetric design
shown here, and this is what is in thelayout at this time.
• Advantage: no coupling of the largeoutput swing into the common biasnetwork.
• Disadvantage: turn-on transition is notas abrupt as in the old design:
• Old: ∆Q<0.04 fC at preamp inputproduces a change at the comparatoroutput from 0 to 5V.
• New: ∆Q≈0.28 fC is needed to swingthe output from 0 to 5V.
• I would like to change the comparatorsin at least 1/2 of the channels back tothe old, proven design.
November 24, 1997 Robert P. Johnson 9
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Analog Channel Signal Shapes
• Top: preamp, shaper,and comparator outputsfor a 4 fC input charge.
• Bottom: 1 fC inputcharge.
• In both cases, the shaperbaseline and thethreshold (90 mV) areshown by solid blackhorizontal lines.
Spice Simulations
November 24, 1997 Robert P. Johnson 10
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Analog Channel Performance
• Gain (shaper output): ≈150 mV/fC in 16-ch chip, ≈125 mV/fC in 32-ch chip.
• Peaking time:≈1.6 µs in 16-ch chip,≈1.3-µs in 32-ch chip.
• Power consumption, including biascircuitry: 150 µW/channel
• Noise: ENC=174 + 32×C electrons, withC in pF, measured by several methods, asshown here, for the 16-ch chip.
ENC=204 + 30.3 C
0.0 5.0 10.0 15.0 20.0 25.0 30.0 35.0
C (pF)
Channel 14 Noise
0
200
400
600
800
1000
1200
1400
EN
C (
elec
tron
s)
Noise measured fromthreshold curves on 10channels.
Noisemeasured byprobe andspectrumanalyzer.
Noise measured from threshold curveson 16 channels connected to detectorstrips with 7 pF capacitance.
External Capacitors
External Capacitors
With Si Strip Detector Attached
0 2 4 6 8 10 12 14 160
100
200
300
400
500
RM
S N
oise
(el
ectr
ons)
Channel Number
Average ENC=407 electrons
0 10 20 30 40
External Capacitance (pF)
100
300
500
700
900
1100
1300
1500
RM
S N
oise
(el
ectr
ons)
ENC=174 + 32 C
November 24, 1997 Robert P. Johnson 11
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Threshold Matching
• Threshold matching from channelto channel across a given chipdepends primarily on the transistorpairs in the shaper feedback.
• Most chips meet the desired upperlimit of about 15 mV rmsthreshold variation (comparedwith the ≈32 mV rms noise level).
• Work is in progress to try toimprove this figure further in thenext prototypes.
• We plan always to have thecapability to set the thresholdindependently for each readoutchip, so chip-to-chip variationswon’t matter.
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18
RMS Offset (mV)
0
1
2
3
4
5
6
7
8
9
10
11
12
Num
ber
of C
hips
0 2 4 6 8 10 12 14 160
2000
4000
6000
8000
10000
12000
14000
Thr
esho
ld (
elec
tron
s)
Channel Number
RMS variation=325 electrons=6.5 mV
Results from threshold scans on asingle 16-channel prototypeconnected to a single detector.
Results fromthreshold scans on 5932-channel chips,with no detectorsattached.
November 24, 1997 Robert P. Johnson 12
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Readout Architecture
• 25 64-channel readout chips handle asingle detector layer.
• Data can shift out left or right, or in bothdirections, with a readout-controller chipat each end of the chain. (20 MHz clockfrequency.)
• Trigger-output (Fast-OR) signals alsomove left or right, or in both directions.
• Either readout controller chip canreprogram the readout direction of anyof the front-end readout chips, so asingle dead chip can be bypassedwithout losing data from any other chips.
• The readout controller chips pass datadown the tower in a token-controlledprotocol.
data
trigger
trigger
data
data
trigger
trigger
data
data
trigger
trigger
data
cmd
cloc
k
trg
ack
cmd clk
trg
ack
toke
n
data
data
data
cmd
clk
trg
ack
trg
ack
cloc
k
cmd
Controller
Controller
FE FE FE
data
trigger
trigger
data
data
trigger
trigger
data
data
trigger
trigger
data
cmd
cloc
k
trg
ack
toke
nda
ta
data
toke
n
trg
ack
cloc
k
cmd
Controller
Controller
FE FE FE
toke
n
data
To the Tower Controller
To the next layer
Trigger
Trigger
Tr i
gger
Tri
gger
Simplified block diagram of the readout of aGLAST tower, showing only 2 of 16 layersand only 3 of 25 readout chips on eachlayer.
November 24, 1997 Robert P. Johnson 13
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Front-End Readout Chip (GTFE64)
• The 64-channel chip currently beingdesigned has the followingadditional features:
– Calibration mask, to select anysubset of channels to be pulsed.
– Two 7 bit DACs, for settingcalibration and threshold levels.
– Separate masks for data and triggeroutput (Fast-OR).
– 8-deep FIFO event buffer.
– Dual redundant serial commanddecoders.
– Dual redundant output shiftregisters and trigger outputs.
– Bypasses to avoid clocking out datafrom empty chips.
– External communication via low-voltage-swing differential signals.
Cal
ibra
tion
Mas
k
64 in
put p
ads
Am
plif
iers
and
Dis
crim
inat
ors
FIFO
Buf
fer
(RA
M)
Shif
t Lef
t
Out
put R
egis
ter
Shif
t Rig
ht
Out
put R
egis
ter
ThresholdDAC
Cha
nnel
Mas
k
64inputOR
2inputOR
2inputOR
Fast-OR fromchip on left
Fast-OR fromchip on rightFast-OR to
chip on right
Fast-OR to chip on left
Command Receivers
Commands Clock Trigger
Dat
a In
Dat
a O
ut
Dat
a O
ut
Dat
a In
Controlregisteroutput
CalibrationDAC
Tri
gger
Mas
k
November 24, 1997 Robert P. Johnson 14
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Resistors
Resistors are used in several places in thedesign:
• The DACs
• Drivers and receivers (to reducedependency of the power consumptionon the supply voltage)
However, the CMOS26G process has noreally good way for making evenmoderately large resistors. Therefore, wehave resorted to using N-well structuresfor that purpose.
We made a test chip that includes somestructures for testing the method that weemploy to make large resistors in thisprocess (N-wells).
1 2 3 4 5V
-100
0
100
200
300
400
500
Cu
rre
nt
(uA
)
I17.24 kohm
The resistance is nearly a factor of twohigher than what we anticipated.
This is being corrected accordingly inthe layout.
Predicted value was4.6 kΩ.
November 24, 1997 Robert P. Johnson 15
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Threshold and Calibration DACs
• 6-bit linear DAC with 2 ranges.• Threshold DAC:
• 6 mV/step (≈0.05 fC).• or 24 mV/step (up to ≈12 fC).
• Calibration DAC (same voltage stepsinto a 42 fF calibration capacitor):
• 0.25 fC/step in low range.• 1 fC/step in high range (up to
about 12 MIPs).
• Functions by adding currents, the totalof which are converted to a voltage bya resistor (N-well structure).
• A reference current is derived fromthe 2V supply and a resistor (the tworesistor values cancel to 1st order).
• A test chip with this DAC wasreceived just last week from MOSIS.
0 10 20 30 40 50 60 70
Setting
0.0
0.1
0.2
0.3
0.4
0.5
Thr
esho
ld (
volts
)
MeasuredStep=5.77mVSimulatedStep=6.26mV
Measurement of the DAC performancein the low range, compared with aSpice simulation of the circuit. Theslope is close to expectations despitethe error in the resistor values.
The linearity is betterthan 0.5%.
November 24, 1997 Robert P. Johnson 16
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Threshold and Calibration DACs
Even though the DAC low range worksperfectly well, the high range does not.
-1 9 19 29 39 49 59 69Setting
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
Thr
esho
ld (
volts
)
DataSpiceLine Fit
10 30 50 70
Setting
30
80
130
180
Cur
rent
(uA
)
Measured6.18+25.4n
10 30 50 70
Setting
-3
-1
1
3
Res
idua
l
However, the high range is OK if thevoltage is held constant and the current ismeasured, as on the right ⇒
There is someclear nonlinearityhere, but it isworking.
Measuring current atthe DAC output, withthe voltage = 1.5 V.
November 24, 1997 Robert P. Johnson 17
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Threshold and Calibration DACs
0.0 1.0 2.0 3.0 4.0Voltage Across Resistor
-100
0
100
200
300
400
500
600
Cur
rent
(uA
)
ITHR-IREF7.29 kohm
Vref held constant at 1.28 V
All bits set to 0.
It appears that current is flowing out ofthe threshold output node by somemeans other than through the resistorwhen the voltage gets above about 2.6 V.
This mystery is being investigated.
With V-ref held constant, V-threshold isscanned from V-ref up to 5 V. Above acertain point there is more current flowinginto the threshold node than is flowing outthe opposite end of the resistor.
7.3 kohm
Threshold
V-ref=1.28 V
0.66 uA
0.66 uA
ITHR
IREF
November 24, 1997 Robert P. Johnson 18
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Command Decoder
The front-end chip is controlled by serial command strings delivered to either of 2 redundantcommand decoders. Either decoder can load the control register at any time, but all othercommands are accepted only if the decoder is selected by a bit in the control register.
• Command format:– Start bit.
– 3-bit command code.
– 5-bit chip address or 1F (for all chips).
– N-bits of data (load control register).
• Commands:– 000: no-op.
– 001: load control register.
– 010: read-event.
– 011: calibration strobe.
– 100: clear first event from FIFO.
– 101: reset chip (FIFO + cntrl. reg.).
– 110: reset FIFO.
– 111: end-read-event.
Control is by synchronous logic, with an11-bit state machine. The logic design wasdone by hand, using a schematic, but thelayout was made using DoD CMOSXstandard cells and Cadence automatic place-and-route.
The complete design was simulated inSpice, as well as in digital simulators(Viewsim and Verilog).
November 24, 1997 Robert P. Johnson 19
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Drivers and Receivers
• Controller chip to Readout Chips(clock, commands, trigger):
– Differential current drive, with 1 kΩtermination on the hybrid between thetwo lines.
– Maximum load is estimated to be 50 pF.
– Voltage swing is 0.7 V. Peak current is12 mA.
– Rise time is 5.4 ns (compared with 50nsclock period).
– Receiver power consumption is about150 µW each, with 5 operating at anygiven time on each chip.
• Data (chip-to-adjacent-chip):– 3V differential CMOS.
– Simplifies implementation of the 1600-element shift register across 25 chips.
– Experience with the 32-channel chipssuggests that this should not be aproblem for these very short distances.
• Fast-OR output (chip-to-adjacent-chip):– Small-voltage-swing differential.
– Local charge storage provides currentfor the fast edge; the charge is slowlyreplenished from VDD and GND.
– Therefore, in normal operation, withintermittent triggers, no spikes areintroduced into the supplies.
– Only one set of the redundant driversand receivers is turned on at a giventime, so save power.
• Controller chip to and from adjacentlayers and to and from the towerreadout electronics:
– Some form of low-voltage-swingdifferential transmission will be used.
– Probably it will be similar to thecommunication from controller chips toreadout chips, but it has not yet beenstudied and designed.
November 24, 1997 Robert P. Johnson 20
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
GTFE64 Simulations
• All of the subcircuits designed by Pavelwere simulated thoroughly by him inSPICE (memory, shift registers, drivers,receivers, DACs, etc.).
• The complete analog channel has beenthoroughly simulated in SPICE (usingBSIM models).
• An 8-channel model of the completeoutput stage (FIFO plus shift registers)was simulated in SPICE (includingadditional load to account for themissing 56 channels).
• The command decoder was simulatedin SPICE as a single unit, as well as inVerilog, using the CMOSX standard-cell Verilog models.
• Logic simulations have been carried outon the complete chip and on a set ofthree chips connected together:
– each primitive cell was simulated inSPICE and analog timing diagramswere made.
– A VHDL model was written for eachcell and then executed to produce adigital timing diagram.
– Delays were introduced into the VHDLmodels to give a good match betweenthe digital and analog timing diagrams.
– Dummy VHDL models were made forthe analog components for which adigital simulation is meaningless (suchas the DACs).
– The entire schematic was thensimulated at 20 MHz and 40 MHz byViewsim, using Viewsim built-inmodels for the logic gates and inverters(with nominal 0.5 ns delays).
November 24, 1997 Robert P. Johnson 21
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Layout and Verification
• All layout but that for the commanddecoder has been drawn manually usingthe Mentor Graphics IC-Station andMOSIS SCMOS design rules. Thisincludes all I/O pads, with ESDprotection. This has all passed LVSand DRC within Mentor Graphics.
• The command decoder layout was doneby automatic place-and-route inCadence using CMOSX design rules.
• The Mentor layout has been transferredinto Cadence by way of GDS2, and thetwo command decoders will be insertedand connected within Cadence. Thefinal LVS and DRC will be done inCadence before submission, aftertransferring the schematics fromPower-View to Cadence (using EDIF).
• Test-pads have been, or are being,added as follows:
– Reset pad, to force a reset of thecommand decoder, if necessary.
– External calibration pulse input, incase the internal system doesn’twork or is insufficient for testing.
– All analog channel bias points.
– All preamp and shaper outputs.
– All receiver CMOS outputs anddriver CMOS inputs.
– DAC outputs.
– All clock and control outputs fromthe command decoders.
November 24, 1997 Robert P. Johnson 22
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Layout
11.5
20.1
DRIN
DRIP
TA
CK
LN
CT
RL
RE
G
A1
A3
A2
A4
A0
TA
CK
RN
AV
DD
DLOP
DLON
DROP
DRON
DLIP
DLINQV
DD
AV
DD
2
AG
ND
CL
KL
P
CL
KL
N
TA
CK
LP
CM
DL
N
CM
DL
P
DG
ND
R
DV
DD
R
CM
DR
P
CM
DR
N
CL
KR
P
CL
KR
N
TA
CK
RP
AG
ND
R
AV
DD
R
I1VIR
AV
DD
2R
0.2 0.25 0.30.2
0.70.95
1.05
TLON TLIN
DV
DD
DG
ND
TRIP
TRIN
TLOP
TRON
TROP
TLIP
• The chip is designed to match the 195 micron detector strip pitch.
• Analog power and ground pads are doubled, with one of each at each end ofthe chip.
• Analog power must pass over the chip-to-chip digital signals. One of themetal layers is used as a shield between them where they cross.
• Analog and digital circuitry are separated by a well structure, but both analogand digital grounds are tied solidly everywhere to the substrate, to avoid latch-up problems.
November 24, 1997 Robert P. Johnson 23
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Readout Controller Chip (GTRC)
• Control initialization, calibration,and readout of the front-end readoutchips.
• Sparse readout—build list of hit-strip addresses.
• Calculate the time-over-threshold ofthe prompt trigger output.
• Build events and coordinate thereadout with neighboring layers viaa serial data line and a token.
• External communication via low-voltage-swing differential lines.
• Currently being designed for the HP0.8 µm process using the CMOSXstandard cells. The logic design issynthesized from Verilog code.
I/O ControlGlobal Control Comand Decoding
FIFO for TOT
TOT CounterHit Counter
Event buffer
1
Event buffer
2
Gate
tokendata tokendata
Previous Layer
Next Layer
Data from Front End Chips
Tri
gger
Ack
now
ledg
e
Clo
ck
Com
man
ds
To Front End Chips
Trigger Out Triggers from the Front-End Chips
Commands
Clock
Trigger Acknowledge
Simplified block diagram of thereadout controller chip.
November 24, 1997 Robert P. Johnson 24
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Hybrids
To minimize dead area, the hybrid circuits holdingthe readout chips and controller chips must be mountedon the sides of the detector trays.
A Kapton flex circuit brings the signals around thecorner of the tray.
The hybrid is divided into 5 pieces, each the widthof one detector wafer and each holding 5 readout chips.They are connected by wire bonds. The two end pieceseach hold a controller chip and connector.
November 24, 1997 Robert P. Johnson 25
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Hybrids
• The hybrid circuits include– bypass capacitors for each readout chip and the detector bias,
– resistors to set the front-end bias current, and termination resistors for the digitalsignal lines.
– Power supply filtering and fuses.
– Temperature monitors.
• Eight layers are used in the layout, including entire planes for power, ground,analog 2V, and detector bias. The central type has already been fabricated.
Left-Hand Hybrid: All analog signals pass alongplanes beneath the digital signal planes and areseparated from them by power and ground planes.Detectors and readout chips have wide low-inductance paths to the decoupling capacitors.
November 24, 1997 Robert P. Johnson 26
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Flex-Circuit Detector Interconnect• Top layer of conductors for bias
(120 V), ground, and signals.
• Bottom layer is a shield plane toisolate detectors from the trays.
• 3 pads to supply bias to the backsof each of 25 detectors.
• 5 traces to bond to the bias-voltage strips to each of the 5hybrid circuits.
• 6 traces to bring the ground of thehybrids around the tray corner tothe detectors.
• 1600 traces to bring the signalsfrom the detectors around the traycorner to the readout chips.
• Alignment mark at the corner ofeach detector.
Status:• Manufacture of 5 prototype pieces is in progress.• 3-week turn-around.
November 24, 1997 Robert P. Johnson 27
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Cabling and Connectors
• The connectors must lie flat on the hybrid tominimize dead space at the tower edge.
• Nanonics space-qualified 25-pin “Dualobe” 25-milpitch connectors appear to fit the requirements well.
• The cable must include connections from layer toadjacent layer, as well as from each layer to the towerbase. A Kapton circuit provides the best flexibility indesign and allows us to build in shielding.
• The design concept shown below will give goodaccess to the connectors and is manufacturable.
0.9
PC
Boa
rd
Chi
ps
Flex
Cir
cuit
Nanonics Connector
Analog power and ground, plus detector bias.
A connector forevery other tray.
Tower Base Digital Traces, surrounded by digital power and groun
November 24, 1997 Robert P. Johnson 28
Santa CruzInstitute forParticle Physics
ASIC Development for the GLAST Tracker
Conclusion
• The near-term goal is to have allelectronics and detectors necessaryto begin assembly of anengineering prototype tower nextautumn.
– Submit GTFE64 chip for 1stprototype production by December10, 1997. Begin testing inFebruary, 1998.
– Submit GTRC chip for 1stprototype production in January orFebruary, 1998.
– Produce at least 10 wafers ofGTFE64 chips in July, 1998.
– Test 1st full readout section insummer 1998.
• Final loose ends of the GTFE64 layoutand verification must be tied up soon.
• Controller-chip simulations must becarried out together with the readout-chip digital model.
• I/O design of the controller chip mustbe finalized and layout done.
• Controller chip layout and verificationmust be done.
• End hybrid design needs to beprototyped, after some possiblemodifications (more terminationresistors?).
• Cables need to be prototyped.
• More interfacing to DAQ at Stanfordand mechanical work at SLAC.
• Lots of testing!