Konstantin Stefanov`s talk on LCFI at LCWS 2006
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Transcript Konstantin Stefanov`s talk on LCFI at LCWS 2006
LCFI Status Report: Sensors for the ILC
Konstantin Stefanov
CCLRC Rutherford Appleton Laboratory
LCSW06, Bangalore, India
Introduction
Sensor Development for the ILC
Column-Parallel CCDs
Readout and Drive Electronics
In-situ Storage Image Sensors
Summary and Plans
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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Introduction and Conceptual Design
Beam bunch structure at ILC
0.2 s
337 ns
2820x
0.95 ms
Multiple collisions
Main vertex detector parameters:
120 large sensors (e.g. CCDs) in 5 layers, 800
Mpixels (20 μm20 μm)
Excellent point resolution (3.5 μm), pixel size = 20 μm, close to IP
Low material budget ( <0.1% X0 per layer), low power dissipation
Readout:
Avoids excessive event overlap, occupancy << 1%
Inner layer effectively read out at 50 μs intervals during the 1 ms pulse train (20
readouts) – information may leave the sensor or be stored in pixel
Outer layers read out at 250 μs intervals
Moderate radiation hardness ( 20 krad/year)
Tolerates Electro-Magnetic Interference (EMI)
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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The Column Parallel CCD
Main detector work at LCFI
Every column has its own amplifier and ADC – requires readout chip
Readout time shortened by orders of magnitude
All image area clocked (> 5 nF/cm2)
Optimised for low voltage clocks to reduce power dissipation
M
M
N
N
“Classic CCD”
Readout time
NM/fout
Column Parallel
CCD
Readout time = N/fout
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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CPC1 Bump-bonded to CPR1
Hybrid assembly with Column-Parallel CCD (CPCCD) and CMOS ASIC
CPC1 : Two phase CCD, 400 (V) 750 (H)
pixels, 20 μm square;
CMOS readout chip (CPR1) designed by the
Microelectronics Group at RAL:
0.25 μm process
Charge and voltage amplifiers matching
the outputs of CPC1
Correlated double sampling
5-bit flash ADCs and 132-deep FIFO per
column
Everything on 20 μm pitch
Size : 6 mm 6.5 mm
Manufactured by IBM
Bump-bonded CPC1/CPR1 in a test PCB
Bump-bonded by VTT (Finland) using solder
bumps
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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CPC1/CPR1 Performance
5.9 keV X-ray hits, 1 MHz column-parallel readout
Voltage outputs, noninverting (negative
signals)
Charge outputs,
inverting (positive
signals)
Noise 60 e-
Noise 100 e-
First time e2V CCDs have been bump-bonded
High quality bumps, but assembly yield only 30% : mechanical
damage during compression suspected
Differential non-linearity in ADCs (100 mV full scale) : addressed
in CPR2
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
Bump bonds on CPC1
under microscope
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Next Generation CPCCD Readout Chip – CPR2
Bump bond pads
Voltage and charge amplifiers
125 channels each
Analogue test I/O
Digital test I/O
5-bit flash ADCs on 20 μm pitch
CPR1
Cluster finding logic (22
kernel)
CPR2
Sparse readout circuitry
FIFO
CPR2 designed for CPC2
Results from CPR1 taken into account
Numerous test features
Size : 6 mm 9.5 mm
Wire/Bump bond
pads
0.25 μm CMOS process (IBM)
Manufactured and delivered February 2005
Steve Thomas, RAL
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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CPR2 Test Results
Sparsified output
Test clusters in
Parallel cluster finder with 22
kernel
Global threshold
Upon exceeding the threshold,
49 pixels around the cluster are
flagged for readout
● Tests on the cluster finder: works!
● Several minor problems, but chip is usable
● Design occupancy is 1%
● Cluster separation studies:
Errors as the distance between the
clusters decreases
Reveal dead time
Tim Woolliscroft, Liverpool U
Many of the findings have already been
input into the CPR2A design
Tim Woolliscroft, Liverpool U
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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Next Generation CPCCD : CPC2
No
connections
this side
Clock bus
Charge
injection
Three different chip sizes with
common design:
CPC2-70 : 92 mm 15 mm
image area
CPC2-40 : 53 mm long
Extra pads for clock
monitoring and
drive every 6.5 mm
Image area
Standard
Field-enhanced
Standard
Temperature
diode on
CCD
Four 2-stage SF in
adjacent columns
Four 1-stage and 2stage SF in adjacent
columns
Main clock
wire bonds
Main clock
wire bonds
CPR1
CPC2-10 : 13 mm long
Compatible with CPR1 and
CPR2
Two charge transport sections
Choice of epitaxial layers for
different depletion depth: 100
.cm (25 μm thick) and 1.5 k.cm
(50 μm thick)
CPR2
Baseline design allows few MHz
operation for the largest size
CPC2
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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CPC2 + ISIS1 Wafer
ISIS1
5” wafers
One CPC2-70 : 105 mm 17 mm
total chip size
Two CPC2-40 per wafer
6 CPC2-10 per wafer
CPC2-70
14 In-situ Storage Image Sensors
(ISIS1)
CPC2-40
3 wafers delivered
CPC2-10
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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CPC2-40 in MB4.0
Transformer
CPR1/CPR2 pads
Clock monitor pads
Transformer drive for CPC2
Johan Fopma, Oxford U
“Busline-free” CCD: the whole image area serves as a distributed busline
50 MHz achievable with suitable driver in CPC2-10 and CPC2-40 (L1 device)
First clocking tests have been done
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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Transformer Drive for CPC2
Requirements: 2 Vpk-pk at 50 MHz over 40 nF (half
CPC2-40);
Planar air core transformers on 10-layer PCB, 1
cm square
Operation from 1 MHz to > 70 MHz unloaded;
Parasitic inductance of bond wires is a major
effect – fully simulated;
Work on the reduction of the CCD capacitance
and clock voltage is continuing – range of test
devices under development.
Brian Hawes, Oxford U
Transformer is bulky;
IC driver could be a better solution;
Design of the first CPCCD driver chip (CPD1)
has started, manufacture in June
CPD1: 2-phase CMOS driver chip for 20 Amp
current load at 25 MHz (L2-L5 CCDs)
0.35 μm process, size 25 mm2
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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Radiation Damage Effects in CCDs: Simulations
Signal density of trapped electrons in 2D
● Full 2D simulation based on ISE-TCAD
developed
● Trapped signal electrons can be
counted
● CPU-intensive and time consuming
Simulation at 50 MHz
Operating
window
● Simpler analytical model also used,
compares well with the full simulation
● Window of low Charge Transfer
Inefficiency (CTI) between -40 C and 0 C
● Will be verified by measurements on
CPC2
L. Dehimi, K. Bekhouche (Biskra U); G. Davies, C. Bowdery,
A.Sopczak (Lancaster U)
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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In-situ Storage Image Sensor (ISIS)
Beam-related RF pickup is a concern for all sensors converting charge into
voltage during the bunch train;
The In-situ Storage Image Sensor (ISIS) eliminates this source of EMI:
Charge collected under a photogate;
Charge is transferred to 20-pixel storage CCD in situ, 20 times during the 1
ms-long train;
Conversion to voltage and readout in the 200 ms-long quiet period after the
train, RF pickup is avoided;
1 MHz column-parallel readout is sufficient;
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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In-situ Storage Image Sensor (ISIS)
5 μm
Global Photogate and Transfer gate
ROW 3: CCD clocks
On-chip logic
ROW 2: CCD clocks
On-chip switches
ROW 1: CCD clocks
ROW 1: RSEL
Additional ISIS advantages:
~100 times more radiation hard than
CCDs – less charge transfers
Easier to drive because of the low clock
frequency: 20 kHz during capture, 1 MHz
during readout
ISIS combines CCDs, active pixel transistors
and edge electronics in one device: specialised
process
Global RG, RD, OD
Development and design of ISIS is more
ambitious goal than CPCCD
RG RD
“Proof of principle” device (ISIS1) designed
and manufactured by e2V Technologies
OD RSEL
Column
transistor
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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The ISIS1 Cell
1616 array of ISIS cells with 5-pixel buried channel
CCD storage register each;
Cell pitch 40 μm 160 μm, no edge logic (pure CCD
process)
Chip size 6.5 mm 6.5 mm
Output and reset transistors
OG RG
OD
RSEL
Column
transistor
OUT
Photogate aperture (8 μm square)
CCD (56.75 μm pixels)
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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Tests of ISIS1
Tests with Fe-55 source
The top row and 2 side columns are not protected and collect diffusing charge
The bottom row is protected by the output circuitry
ISIS1 without p-well tested first and works OK
ISIS1 with p-well has very large transistor thresholds, permanently off
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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Conclusion and Plans
CPCCD program well advanced:
Main work at LCFI
Hybrid assembly with CPCCD and CMOS chips works OK
Detector-sized chips CPC2 have arrived, some tests have been done
Started to develop CPCCD drive system, lots of challenges
ISIS work will continue:
First ISIS prototype on CCD technology manufactured, first tests promising
Next-generation small pixel ISIS (CCD- or CMOS-based) will be actively
pursued
Immediate plans:
Evaluate CPC2 and CPC2/CPR2 bump-bonded
High speed external drive to CPC2-40 as demonstrator for the L1 vertex detector
Visit us at http://hepwww.rl.ac.uk/lcfi/
Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory
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