A CCD-based vertex detector Chris Damerell on behalf of the LCFI Collaboration • Project overview and design principles • R&D programme • Development of.
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Transcript A CCD-based vertex detector Chris Damerell on behalf of the LCFI Collaboration • Project overview and design principles • R&D programme • Development of.
A CCD-based vertex detector
Chris Damerell on behalf of the LCFI Collaboration
• Project overview and design principles
• R&D programme
• Development of novel CCDs and readout electronics
• Development of thinnest possible detector layers
• Physics studies
• Summary and future plans
July 14 2003
US LC Workshop Cornell U – Chris Damerell
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Project overview
• Linear Collider Flavour ID Collaboration: Bristol U, Lancaster U,
Liverpool U, Oxford U, QMUL and RAL
• R&D assumes up to 5 CCD development cycles at intervals of
~20 months
• Initially funded by PPARC for £2.3M for 3 yrs from April 2002
(£700K equipment, £1600K PPARC manpower)
• Synergy with recent PPARC plans to play a major part in the LC
BDS (beam delivery system)
• Working to develop closer ties between other regional VTX
activities. Our international phone conference at time of US
workshop at UT Arlington was a major success
• Looking forward to one international collaboration to build the
LC vertex detector, once prototype ladders have enabled the
technology choice to be made
• One major unknown in the decision process is the accelerator
technology
July 14 2003
US LC Workshop Cornell U – Chris Damerell
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Design principles
• 5 layers, inner layer at radius 12-15 mm
• 3-hit coverage to cosq = 0.96
• thin layers (<0.1% X0 ) for minimal mult scatt and g conversions
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US LC Workshop Cornell U – Chris Damerell
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• silicon pixels of size ~ 20 mm square for low cluster-merging in jets
• support structure with micron precision/stability (specially important
for oblique tracks near ladder ends)
• on-detector signal processing, so almost no external connections
• power dissipation measured in few tens of watts, so gas cooling
sufficient (
vital for low material budget)
• ‘adequate’ radiation hardness
• readout time ~ 5 ms for JLC/NLC (between bunch trains)
~ 50 ms for TESLA (20 frames/bunch train)
•
4
4
p sin3 / 2 q
• crucial for efficient charm ID (1-prong decays), vertex charge (Bs),
but quantitative physics examples still being worked on …
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US LC Workshop Cornell U – Chris Damerell
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Novel CCDs and readout electronics
• CCD sizes similar to SLD, but readout needs to be 20-2000 times faster
• eliminate bulky electronics which would degrade fwd tracking and
calorimetry
• total of 800 Mpixels, cf 307 Mpixels for SLD
• TESLA readout requirement stimulated concept of ‘column parallel’
operation
•
innovative CCD/CMOS hybrid. If successful, this architecture
may also be preferred for NLC/JLC. However, for this case, the
conventional architecture with a multiple-output linear register should
also be evaluated
July 14 2003
US LC Workshop Cornell U – Chris Damerell
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M
N
N
“Classic CCD”
Readout time NM/Fout
Column Parallel CCD
Readout time = N/Fout
• Max possible readout speed, for given noise performance
• Readout IC (amp+ADC on 20 mm pitch) only became available
with deep submicron CMOS technology
• TESLA requires parallel register clocking at 50 MHz: 1 MHz is
fine for NLC
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US LC Workshop Cornell U – Chris Damerell
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electronics only at the ends of the ladders
bump-bonded assembly between thinned CPCCD and readout chip
readout chip does all the signal processing, yielding sparsified digital data
CPCCD is driven with high frequency, low voltage clocks
low inductance layout required for clock delivery
July 14 2003
US LC Workshop Cornell U – Chris Damerell
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Standard 2-phase Field-enhanced 2-phase implant
implant
(high speed)
Features of our first CPCCD:
Metallised gates
(high speed)
• 2 different charge transfer regions
• 3 types of output circuitry
Source
followers
Direct
2-stage
source
followers
Readout
ASIC
Source
followers
Metallised gates
(high speed)
Direct
Readout
ASIC
To pre-amps
• Independent CPCCD and readout
chip testing possible:
•without readout chip - use
external wire bonded electronics
• without bump bonding - use
wire bonds to readout chip
• finally, bump-bonded
• Different readout concepts can be
tested (direct charge sensing, and
voltage sensing via source follower)
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US LC Workshop Cornell U – Chris Damerell
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CPC-1 delivered & under test
Direct connections and 2-stage source followers
1-stage source followers and direct connections on
20 μm pitch
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US LC Workshop Cornell U – Chris Damerell
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US LC Workshop Cornell U – Chris Damerell
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Single pixel events seen in one column of CPC-1
with 2 V peak-peak clocks
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US LC Workshop Cornell U – Chris Damerell
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Wire/bump bond pads
Charge Amplifiers
Voltage Amplifiers
250 5-bit flash ADCs
FIFO
Wire/bump bond pads
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US LC Workshop Cornell U – Chris Damerell
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US LC Workshop Cornell U – Chris Damerell
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Thinnest possible detector layers
3 approaches
•
Unsupported silicon
•
Semi-supported silicon
•
Supported silicon
Unsupported approach attractive – ‘like wires in a drift chamber’
Works beautifully along ladder length (sagitta stability around 2 microns)
However, processed thin CCD is not like a wire: it’s an inhomogeneous
membrane in which transverse stresses may lead to somewhat
uncontrollable shape
Also, we have concerns about handling issues, for attaching readout chips
etc
Not abandoned, but semi-supported approach may be more practicable
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US LC Workshop Cornell U – Chris Damerell
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Beryllium substrate with adhesive balls
Thinned CCD ( 20 μm)
CCD brought down
Shims
Assembly after shim removal and curing
Adhesive
0.2mm
Beryllium substrate (250 μm)
1 mm
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Physics studies
The design of the VXD should be driven by the physics requirements:
• 4 configurations, 5 layer single thickness and 4 layer double thickness,
and other combinations
• make single muon and pion tracks in Brahms for all momenta and
angles. Fit the distributions
• include the parametrizations in Simdet
• biggest effect comes from removal of the inner layer
• provide to physics groups
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US LC Workshop Cornell U – Chris Damerell
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5layers
•
•
4 layers,
double
Clear performance difference between configurations
Charm suffers most, B tagging is “easy”
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US LC Workshop Cornell U – Chris Damerell
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•
New procedure to attach track to
vertices
•
Charged B, up to 89% correct tag,
6-8% worse for 4 layer double
thickness configuration
•
Charged D, excellent purity, less
difference between configurations
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US LC Workshop Cornell U – Chris Damerell
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•
Neutral B: dipole
•
Maintain, develop and improve
tools
•
Provide them to the physics
community so we can get feedback on detector parameters from
various physics channels
•
Make a transition to Java/JAS
environment
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US LC Workshop Cornell U – Chris Damerell
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Summary and future plans
• Fast CCDs:
•
much to study with CPC-1
• tentative plan for design/production of CPC-2 (including detectorscale prototypes, 10x2 cm2) Oct 2003-June 2004
•
readout chips CPR-1 and CPR-2 all we need in medium term future
• Thin ladders:
• semi-supported assemblies with a well-behaved adhesive may be
fine, including satisfying the bump-bonding assembly requirements
• numerous alternative ideas, some (fortunately) being pursued by
other groups – notably the DEPFET collaboration
• Physics studies:
•
totally dependent on available effort, a small but dedicated team
• Major opportunities for wider collaboration in all areas, and
informally it is happening
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