SILC: Silicon tracking for the International Linear Collider

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Transcript SILC: Silicon tracking for the International Linear Collider

SiLC (Silicon tracking for the
International Linear Collider)
http://silc.in2p3.fr
H.J.Kim (KyungPook National U.)
on behalf of the SILC R&D Collaboration
(major transpariencies from Aurore Savoy-Navarro)
Outline
The Collaboration
Goals
The R&D activities
¤ R&D on sensors
¤ R&D on electronics
¤ R&D on Mechanics
The tools
>> Alignment(s) & calibrations
>> Lab test benches
>> Test beams
>> Simulations
The SILC R&D Collaboration
U.S.A
Europe
Asia
IMB-CSIC, Barcelone (SP)
Kyungpook U. Taegu, Ko
Geneva U, Geneve (CH)
Korea U. Seoul, Ko
Helsinki U. (Fi)
Seoul Nat. U., Seoul, Ko
IEKP, Karlsuhe U. (D)
Close connections:
Tokyo U. (Japan)
Moscow St. U. , Moscou(Ru)
 FNAL (DOE prop 05)
HAMAMATSU (Japan)
Obninsk St. U., Obninsk (Ru)
UCSC, FNAL, LPNHE
LPNHE, Paris (Fr)
 SLAC (DOE prop 03:
INFN-Pisa, Pisa (It)
funded): UCSC, SLAC
Charles U. , Prague (CZ)
Michigan U, LPNHE
Roma 1, La Sapienza (It)
and meetings
IFCA, Santander(Sp)
Torino U., Torino (It)
IHEP, Academy Sci., Vienna (Au)
Michigan U.
SCIPP-UCSC
85 participants
Launched January 2002, Proposal to the PRC May 2003, Status Report May 2005
Several contracts of collaborations between Institutes, ex:
HPRN-CT-2002-00292, CICYT-IN2P3, IN2P3-Hamamatsu, DOE proposals,
EUDET
R&D Goals
SiLC is a generic R&D collaboration to develop the next generation of
large area Silicon Detectors for the ILC; It applies to all the detector
concepts and indeed gathers teams from all 3 detector concepts:
GLD
LDC
SiD
LDC
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Very high precision on momentum and spatial measurements
Full coverage
Low material budget
Robustness
Easy to build and to work with
Low cost
 In all 3 detector concepts Si tracking plays an essential role
 SILC R&D offers a unique framework to compare tracking performances
between the various detector concepts.
 Main difference between the detector concepts = tracking system
R&D on Sensors
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Silicon strips are the baseline with:
Larger size wafers
Thinner/Thinning
Smaller pitch
High yield
Eventually different shapes
Possibility to use new technos in some regions:
From ‘standard’ pixels of 50µ x 300µ to new Pixel
technos: FPCCD, DEPFET, MAPS/FAPS, SOI …
First Prototype on Si strips of different length
28cm x N=1,4
recto/verso
Built by Geneva U., ETH Zurich & Paris
with AMS technique
VA64_hdr
Tsh=3.7µs
Courtesy
G.Ambrosi
(Perrugia)
‘’Serpentine technique’’
Signal over noise as a function of strip length
sensor
to be measured
Signal spectrum is summed over a cluster
after pedestal and common mode subtraction.
The radioactive source is a
Sr90-Y90 beta source.
Results see next slide
The S/N measurements were achieved
on variable length strips with the prototype
at Paris test bench
Collaboration Paris-Prague
New
Results on S/N
L=28cm, S/N(MPV)=20
or S/N(Mean)=30
Noise
vs capa
L=56cm, S/N(MPV)=12
or S/N(Mean)=18
Cluster
size~2
Next steps: Change detector & FE prototypes
go to test beam
Some other S/N measurements and/or
computations
Curve computed
with the
known parameters
of VA_64hdr
Nomad experiment: results from beam tests
on S/N with same sensors and VA1 FE chips
These results and the ones we have obtained are confirming
that 30 cm long strips have S/N greater than 20,
and 60 cm long strips have S/N greater than 10.
Nota bene: These results are of course dependent of the
detector prototype and the associated F.E.E.
2) Development of fabrication line for new sensors
Ex1: 5’’ DSSD fab. line in Korean U.
Ex2: rad hard sensor techno at IMB-CNM
J.Lee’s
talk
Several Institutions in SILC
(also Helsinki U.) are developing new
sensor research lines
Such facilities are very usefull for developing
& testing new ideas and transfer to Industry.
For large production, high quality and
reliability: HAMAMATSU Monopoly
3) Process Quality Control and sensor characterization
(Vienna, Karlsruhe,
Korea, Helsinki,
Pisa ….)
Semi-automatic sensor
probe station for quality
Control: system overview
Process control scheme:
Test structure
Essential for
Developing new sensors
Test of production
Self-made chuck and
probe card support
Test of 10 Hamamatsu det.
S8743 (GLAST)
8.9500+/-20 x idem µm
Strip pitch: 228µm
Nb of strips: 384
(done @Vienna PQC set up )
Longer term prospects on the R&D on sensors
• To develop Si strip wafers single sided of at least 8’’, with readout pitch of
50µm, as thin as possible, and with high yield (>50%)
• To develop ‘’thinning’’ technique in order to get at least 2:1 reduction in
thickness (already underway)
• To develop double sided wafers of at least 6’’, and with high yield (>50%)
• Keep in mind some of the µvertex technologies for certain parts of the
Si tracking system.
• New way(s) to connect electronic on detector with strips (connectics)
Objectives:
To develop R&D sensors fab line in Research Laboratories in order to
develop ideas as listed above, and later on, to transfer technology to
Industrial firm(s).
Presently, HAMAMATSU is THE firm able to produce large amounts of
detectors in the most reliable way; Will this continue in the future?
R&D on Electronics
The Si tracking system:
a few 100m2, a few 106 strips
Events tagged every bunch (300ns) during the overall train (1 ms)
Data taking/pre-processing ~ 200 ms
Occupancy:
< a few %
Goals:
Low noise preamplifiers
Shaping time (from 0.5 to 5 µs,
depending the strip length)
Analogue sampling
Highly shared ADC
Digitization @ sparsification
Very low power dissipation
Power cycling
Compact and transparent
NEW!!
First LPNHE prototype
fulfills most of these
goals
Two designs
SCIPP-UCSC:
Double-comparator discrimination system
Improve spatial resolution (25%)
Next foundry: May 9.
LPNHE-Paris:
Analogue sampling+A/D,
including sparsification on
sums of 3 adjacent strips.
Deep sub micron CMOS techno.
First chip successfully submitted
and now under test
Next version: in progress
the chip (Feb 05)
the test board
1.6 mm
the layout: 16 +1 ch.(Nov 04)
3 mm
VERY ENCOURAGING FIRST RESULTS
Shaper:
simu vs measurement
LPNHE chip: layout results & tests
Lab test benches
Paris test bench
In most Labs:
LD & radioactiveSource (ex: Paris & Korea)
Dark reference
box
sensor
Pb
Pb
90Sr
source
sens
or
Korean test bench
S/N ~ 10.
sigma=14.4±0.2
J.Lee’s talk
Test beams: Goals
 To qualify in conditions closest to the real life:
prototypes of detectors (including New Si
technologies) and of the associated FE and readout
electronics.
 Detection efficiency vs operational parameters
 Spatial resolution, cluster size
 Signal/Bruit
 Effect of magnetic field (Lorenz angle determination)
 Angular scans, bias scans
 Integration with other sub-detectors
 Alignment
 Cooling (including power cycling)
 In the specific & new ILC conditions.
Foreseen beams
5T cosmiques,
laser
Bonn electron 3.5 GeV
Others:
CERN, FNAL,
KEK
(Korean
colleagues)
1T, 6 GeV
e- beam
Participants: All + FNAL
Using the test beam setup in Bonn
Szintillator
BAT 1
Si tracker
Prototype
2
3
4
Szintillator
3 x 3 mm²
beam
ATLAS Diamond
trigger
coincidence
T rigger
L ogic
U nit
busy
Collaboration with DEPFET
(under preparation)
Detector Prototypes:
Support mobile
Forward Prototype:
under CAD study
• Design (just started)
• Fabrication
• Assembling & Mounting
Module with 3 sensors
Module with 2 sensors
Second layer partly covering
the first one.
Total of 60 trapezoidal
sensors,
About 10 K readout channels
Ready by end 2006/beg. 2007
Other prototypes: Ladders of
different sizes and sensors
Schedule & Financing
Bonn
now
06
07
08
09
Preparations
tests Proto1
Beam tests:
elementary modules
construction proto
Forward
Chips 128 ch.
Construction barrel pototype
Tests (cont’d) also combined with
Other sub detectors
New foundry (>=512 ch + techno)
EUDET (I3 EU project) foresees for Si-tracking in JRA2, the financing of:
 Part of the chips (2 submissions) & large number of channels
 Protos large dimension: a part of the Si central & Si forward trackers
 Protos alignment
 Protos cooling
An R&D activity on a new scale is starting within SiLC when going
to test beams.
SiLC R&D proposal was presented to the PRC on May 2003
Goal: to develop the next generation of large area Si trackers suited for
performing very high precision measurements
in spatial position and momentum at the ILC,
All R&D aspects, on sensors, electronics and mechanics are addressed.
All needed tools: simulations, Lab test benches, test beams,
alignment and calibration are being developed
Highlights/important progress these last 2 years:
Work on sensors: characterization of strips of variable length,
development of fab lines
FE electronics in deep submicron CMOS techno
Developing Lab test bench for highly precise measurements
CAD of all the tracking components, for both LDC (Si Envelope) & SiD
Thermo mechanical studies
NOW:
Preparing for test beams and getting even closer to the real life conditions.
The collaboration is getting speed and established close contacts with all
3 detector concepts
Keeping synergy with LHC (SuperLHC).
Second Parigi prototype is underway
Next step: going to 128 channels
with analogue sampling included;
second chip prototype currently under
design, foreseen submission Fall 05.
Will equip the test beam prototypes
Longer term prospects for the FE readout chip
and processing of the Si-tracking information
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Higher multiplexing factor for A/D, at least 512:1, possibly 1024:1
Go to deeper DSM techno (90 nm)
Try SiGe techno for analogue part of the FE chip
Work out packaging, output of signal and cabling issues: following last
developments on those topics
Develop upper stages of the readout and of the data processing for the Sitrackers:
>> Clusterization to improve the position resolution
>> track reconstruction (track segments)
and their inclusion in the overall data flow architecture.
Study the time information provided by those detectors (shorter shaping time
possibility)
Stay in close contact with/participate to the new developments for the SLHC
tracking.
Tests prototypes on Lab test bench but also on more real life set ups= use
them for the readout of prototype detectors in test beams.
A systematic work is underway on an electronic test bench to fully characterize
the 40 first prototyped chips: amplifier gain, linearity, dynamic range, noise,
power dissipation; The power cycling will also be experienced.
All the results are compared with simulations performed before sending for
foundry as well as post simulations.
As an example here below the results on the noise
By courtesy of Jean Francois Genat