HV Problems - Istituto Nazionale di Fisica Nucleare

Download Report

Transcript HV Problems - Istituto Nazionale di Fisica Nucleare

D
DØSMT
DØ Silicon Microstrip Tracker for runIIa
Design
Production
Assembly
Readout
Installation
Commissioning
Conclusions
Eric Kajfasz (CPPM/FNAL) - Breese Quinn (FNAL)
Como, October 15, 2001
presented by Alice Bean (Kansas/FNAL)
RunIIa SMT Design
D
12 F Disks
4 H Disks
6 Barrels
4-layer barrel cross-section
72 ladders
12 cm long
Como2001, 10/15/01
SMT Statistics
Barrels
F-Disks
H-Disks
Channels
387072
258048
147456
Modules
432
144
96
Si Area
1.3 m2
0.4 m2
1.3 m2
Inner R
2.7 cm
2.6 cm
9.5 cm
Outer R
9.4 cm
10.5 cm
26 cm
E. Kajfasz/B. Quinn
6192 R/O chips = 792,576 channels
> 1.5 million wire bonds
2
D
Como2001, 10/15/01
RunIIa SMT Design
E. Kajfasz/B. Quinn
3
D
High Density Interconnect
Kapton based flex circuits with
0.2 mm pitch for chip mounting
Laminated to Beryllium substrate
and glued to Silicon sensor
Connects Sensor to SVXII chips
and SVXII chips to flex circuit via
wire bonds
(Al wedge bonding)
Connects to a Low Mass Cable
which carries the signals out of the
interaction region
Como2001, 10/15/01
SVXIIE chips
9-chip HDI for 20 sensor
Be substrate
E. Kajfasz/B. Quinn
Bus control and
power traces
4
SVXIIe chip
SVXIIFE
Como2001, 10/15/01
SVXIIBE
32 storage cells/channel
Analog section
E. Kajfasz/B. Quinn
ADC ramp
and counter
Digital section
To Readout System
128 channels
I/O
Sparsification FIFO
Analog Pipeline
ADC Comparators
Pipeline Control Logic
To Silicon Detector
1.2 um CMOS
amplifier/analog delay/ADC
chip fabricated in the UTMC
rad hard process
Designed by LBL/FNAL
Some features:
128 channels
32 cell pipeline/channel
8-bit Wilkinson ADC
Sparsification
53 MHz readout
106 MHz digitization
6.4 x 9.7 mm2
About 85,000 transistors
Integrators (128 channels)
D
5
D
SVXIIe chip
Externally programmed to
achieve optimal performance
for 132 or 396ns beam
crossings and detector
capacitances from 10 to 35pF
(preamp bandwidth
adjustment)
Chip noise
490e + 50e/pF
i.e. ~1200e ENC for C=15pF
1 MIP => ~4fC => ~25,000e
=> S/N ~ 20
Max dealy in analog pipeline:
32 x 132ns = 4.2us
Como2001, 10/15/01
E. Kajfasz/B. Quinn
6
D
Production: 3-chip ladders
72 single-sided axial
ladders
2 sensors/ladder
Located on 1st and
3rd layer of 2 outer
barrels
Be substrate, HDI
and rohacell
foam/carbon fiber
rails glued on Silicon
sensor
Como2001, 10/15/01
E. Kajfasz/B. Quinn
7
D
Production: 6-chip ladders
N-side
P-side
144 double-sided doublemetal axial/90° ladders
 1 sensor/ladder
 Located on 1st and 3rd layer of
4 inner barrels
Como2001, 10/15/01
Be substrate, HDI and
rohacell foam/carbon fiber
rails glued on Silicon sensor
E. Kajfasz/B. Quinn
8
D
Production: 9-chip ladders
N-side
P-side
216 double-sided axial/2° ladders
 2 sensors/ladder
 Located on 2nd and 4th layer all 6
barrels
Como2001, 10/15/01
Be substrate, HDI and
rohacell foam/carbon fiber
rails glued on Silicon sensor
E. Kajfasz/B. Quinn
9
D
Production: F-wedges
N-side
P-side
144 double-sided ±15° strips
 6 (n) and 8 (p) readout chips
 1 sensor/wedge
 Located on 12 F-disks
Como2001, 10/15/01
Silicon sensor glued on HDI
E. Kajfasz/B. Quinn
10
D
Production: H-wedges




Como2001, 10/15/01
E. Kajfasz/B. Quinn
96x2 back to back
single-sided, ±7.5°
strip angles
6-chip readout per
side
2 sensors/wedge
Be substrate and
HDI glued on Silicon
sensor
Located on 4 H-disks
11
D
Production: Sensor problems
Sensor lithography defects
A silicon manufacturing problem
produced p-stop isolation defects
in the 90° stereo ladders. This
resulted in a 30% yield from the
manufacturer.
Micro-discharge effect
With negative p-side bias on double-sided detectors, we observed microdischarges producing large leakage currents and noise above a certain
breakdown voltage.
The effect occurs along the edges of the p implants, where large field
distortions and charge accumulations result from misalignment of electrodes
with implants.
Como2001, 10/15/01
E. Kajfasz/B. Quinn
12
D
Production: Testing
Fail
Functionality Test
Debug bad strips (broken capacitors),
bonds, chips, etc.
Determine the V-I characteristics of the
sensors
Measure V-max p-side breakdown voltage
(micro-discharge effect)
V-max
Burn-in
Bias the ladder or wedge and test the
readout for 72 hours
Measure pedestals, noise, gain and
check sparse readout
Laser
Expose biased detectors to a narrow
laser scan
Measure the depletion voltage and
leakage currents and identify dead
channels
Readout tested again after the detector
is mounted on a barrel or disk
Como2001, 10/15/01
E. Kajfasz/B. Quinn
13
D
Production: Vop
L6
L3
Vop (V)
L9
Como2001, 10/15/01
Vop (V)
FW
Vop (V)
E. Kajfasz/B. Quinn
Vop (V)
14
D
Production: V-max
L6
|V-max| (V)
L9
|V-max| (V)
FW
|V-max| (V)
Como2001, 10/15/01
E. Kajfasz/B. Quinn
15
D
Production: dead channels
L3
% dead strips
L6-p
% dead strips
L9-p
% dead strips
FW-p
% dead strips
Como2001, 10/15/01
E. Kajfasz/B. Quinn
L6-n
% dead strips
L9-n
% dead strips
FW-n
% dead strips
16
D
Production: Rates
Production mainly paced by problems with HDIs and Silicon sensors
(yields, delivery delays …)
300
250
200
L3
150
L6
L9
100
FW
HW
50
0
11/1/98
2/9/99
5/20/99
8/28/99
12/6/99
3/15/00
6/23/00
10/1/00
1/9/01
-50
Como2001, 10/15/01
E. Kajfasz/B. Quinn
17
D
Production: Detector Quality
Detector classification:
Dead channel: < 40 ADC count response to laser
Noisy channel: > 6 ADC count pedestal width
Grade A: less than 2.6% dead/noisy channels
Grade B: less than 5.2% dead/noisy channels
Only used mechanically OK Grade A and B detectors
Channel Fractions (%)
Dead Noisy
Barrel
Como2001, 10/15/01
1
1.5
0.6
2
1.6
0.5
3
1.0
0.3
4
1.3
0.3
5
1.2
0.4
6
2.0
0.2
F Disks 0.5
0.3
E. Kajfasz/B. Quinn
18
D
Assembly: Barrel alignment
Ladders placed
on barrels using
an insertion
fixture
Internal
alignment done
using a CMM
(touch probe)
Como2001, 10/15/01
E. Kajfasz/B. Quinn
19
D
Barrel2 alignment - rotations
In the plane of the ladder
Around ladder short axis
10um
48um

s() =10um induces a 3um error
48um
(mm)
(mm)
s() =48um induces a 3um error

 (mm)

s() =48um induces
a 2um error


Como2001, 10/15/01
Around ladder long axis
Active
BH
Passive
BH
E. Kajfasz/B. Quinn
20
D
Como2001, 10/15/01
Assembly: Barrel-Fdisk mating
E. Kajfasz/B. Quinn
21
D
Como2001, 10/15/01
Assembly: End Fdisks mating
E. Kajfasz/B. Quinn
22
D
Como2001, 10/15/01
Assembly: Hdisk
E. Kajfasz/B. Quinn
23
D
Como2001, 10/15/01
Assembly: Radiation monitors
E. Kajfasz/B. Quinn
24
D
Assembly: ½-cylinder
HDI connection to low-mass cable
South Half Cylinder
Como2001, 10/15/01
E. Kajfasz/B. Quinn
25
SMT Readout: Data Flow
D
HV / LV
8’ Low Mass
Cable
I,V,T Monitoring
~19’-30’ High Mass Cable
(3M/80 conductor)
25’ High Mass Cable
(3M/50 conductor)
3/6/8/9 Chip HDI
KSU
CLKs
CLKs
Adapter Card
Interface
Board
Sensor
Optical Link
1Gb/s
SEQ
Controller
S
E
Q
S
E
Q
S
E
Q
Detector volume
Platform
Serial Command
Link
VRB
VME
Controller
Counting House
Como2001, 10/15/01
Pwr
PC
V
R
B
V
R
B
V
R
B
V
B
D
VRC
1
5
5
3
L3
SDAQ
E. Kajfasz/B. Quinn
26
D
SMT Readout: Electronics
Interface Boards
8 crates (144 boards)
located inside the
detector volume
Regenerates signals
SVX monitoring and
power management
Bias voltage
distribution
Como2001, 10/15/01
SEQuencers
6 crates (120 boards)
located on the
detector platform
Use SVX control lines
to actuate acquisition,
digitization and
readout
Convert SVX data to
optical signals
E. Kajfasz/B. Quinn
VRBs (VME Readout
Buffers)
12 crates (120
boards) located in
counting house
Data buffer pending
L2 trigger decision
Input @ 5-10 kHz L1
accept rate ~ 50
Mb/s/channel
Output @ 1 kHz L2
accept rate ~ 50 Mb/s
27
Installation
D
Fiber Tracker
Cylinder installation was
completed on 12/20/00
A ½ cylinder of 3 barrels and
6 F disks was inserted into
each end of the CFT bore
H Disk installation was
completed on 2/6/01
Calorimeter
Low Mass Cables
The cabling (~15,000
connections) and
electronics installation was
completed in May 2001
SMT
High Mass
Cables
Interface Boards
Como2001, 10/15/01
E. Kajfasz/B. Quinn
28
Commissioning: Status
D
The entire detector has been
connected and powered
The 30% glycol + water coolant is
refrigerated at –10 degC (=>
detectors run between –5 and 0
degC)
~15% of the devices are not in the
readout:
10% ladders, 18% F wedges, 20%
H wedges
Problems could be with boards,
cables, connectors, chips, etc. We
will debug each of them during
the October/November shutdown,
and expect to recover at least half
of them.
Currently collecting calibration,
alignment and commissioning
data
Como2001, 10/15/01
E. Kajfasz/B. Quinn
29
D
Commissioning; Event Display
Online SMT event display
Como2001, 10/15/01
E. Kajfasz/B. Quinn
30
D
Commissioning: Monitoring
Online event monitoring program
Como2001, 10/15/01
E. Kajfasz/B. Quinn
31
D
Commissioning: Charge Collection
A cluster is defined as a
contiguous sequence of
strips with
Each strip  6 ADC
counts
Cluster  12 ADC counts
1 MIP ~ 25 ADC counts
One can play on:
Timing settings, i.e. the
delay of the integration
window w.r.t. the beam
crossing
Preamp bandwith (pabw)
Como2001, 10/15/01
E. Kajfasz/B. Quinn
32
D
Commissioning: Timing and S/N
Higher preamp
bandwith does not
significantly
reduce noise on nside
= 4x132ns + 1x18ns + 0x2ns
Highest value  smallest bandwith
Como2001, 10/15/01
E. Kajfasz/B. Quinn
33
D
Commissioning: Calibrations
SMT pedestal, noise and gain
measurements are taken using
SDAQ.
Pedestal and noise measurements
are used to calculate the threshold
per chip to be used in sparse read
out
Como2001, 10/15/01
E. Kajfasz/B. Quinn
34
D
Barrel cluster charge vs eta
MC
data
Como2001, 10/15/01
E. Kajfasz/B. Quinn
35
D
Como2001, 10/15/01
6-chip ladder n-side cluster
size fraction vs eta
E. Kajfasz/B. Quinn
36
D
SMT & CFT Track Matching
Tracks were found
separately in the SMT and
the Central Fiber Tracker
(CFT)
SMT tracks were
extrapolated to the CFT at
which point the track
offsets were measured
Magnet off data
r = -3  36 m
Como2001, 10/15/01
E. Kajfasz/B. Quinn
37
D
Como2001, 10/15/01
SMT-CFT primary tracks
E. Kajfasz/B. Quinn
38
Conclusions
D
Design/Production
Experience with double-sided detectors has led to the decision to use
single-sided silicon for the upgrade.
Should work towards simpler designs in the future. For example,
using 6 different sensor types resulted in extensive logistical
complications.
Had to overcome numerous vendor related problems for HDIs,
Silicon Sensors, jumpers, low mass cables …
Assembly/Installation
First alignment results show that the DØ SMT was assembled and
installed very well.
The installation in the D0 detector went rather smoothly. The biggest
challenge to overcome was the lack of real estate. The D0 detector,
when first designed, was unfortunately not designed with a Silicon
detector in mind
Como2001, 10/15/01
E. Kajfasz/B. Quinn
39
Conclusions
D
Commissioning
The SMT was the first major DØ Upgrade detector system fully operational
for Run 2a. More than 85% of the channels were available for readout on
startup, and most of the remaining channels will be debugged and recovered
by November.
Calibrations and first look at physics show that we understand our detector.
The offline software is debugged at the same time as the hardware. Now that
they are both reasonably stable, we can start systematic studies.
The detector should be commissioned by the end of the year.
We are eager to start doing good physics with it.
General
Construction and commissioning of the SMT has been an adventure full of
challenges. But thanks to the relentless efforts of many physicists, engineers
and technicians, D0 has now a vertex detector to play with.
We had so much fun building this detector for run 2a that we are already
planning to build a completely new Silicon Microstrip detector for run 2b
(see Alice’s talk)
Como2001, 10/15/01
E. Kajfasz/B. Quinn
40