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1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory 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

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Page 1: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

1Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

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

Page 2: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

2Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

Main vertex detector parameters:

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)

337 ns

2820x

0.2 s

0.95 ms

Beam bunch structure at ILC

Multiple collisions

Introduction and Conceptual Design

120 large sensors (e.g. CCDs) in 5 layers, 800 Mpixels (20 μm20 μm)

Page 3: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

3Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

“Classic CCD”Readout time

NM/fout

N

M

N

Column Parallel CCD

Readout time = N/fout

M

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

The Column Parallel CCD

Page 4: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

4Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

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 by VTT (Finland) using solder bumps

Hybrid assembly with Column-Parallel CCD (CPCCD) and CMOS ASIC

Bump-bonded CPC1/CPR1 in a test PCB

CPC1 Bump-bonded to CPR1

Page 5: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

5Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

5.9 keV X-ray hits, 1 MHz column-parallel readout

Voltage outputs, non-inverting (negative signals)

Noise 60 e-Charge outputs, inverting (positive signals)

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 Bump bonds on CPC1

under microscope

CPC1/CPR1 Performance

Page 6: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

6Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

CPR2 designed for CPC2

Results from CPR1 taken into account

Numerous test features

Size : 6 mm 9.5 mm

0.25 μm CMOS process (IBM)

Manufactured and delivered February 2005

Bump bond pads

Wire/Bump bond pads

CPR1

CPR2

Voltage and charge amplifiers 125 channels each

Analogue test I/O

Digital test I/O

5-bit flash ADCs on 20 μm pitch

Cluster finding logic (22 kernel)

Sparse readout circuitry

FIFO

Next Generation CPCCD Readout Chip – CPR2

Steve Thomas, RAL

Page 7: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

7Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

CPR2 Test Results

Tim Woolliscroft, Liverpool U

● 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

Many of the findings have already been input into the CPR2A design

Tim Woolliscroft, Liverpool U

Parallel cluster finder with 22 kernel

Global threshold

Upon exceeding the threshold, 49 pixels around the cluster are flagged for readout

Test clusters in Sparsified output

Page 8: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

8Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

Clock bus

Main clock wire bonds

Main clock wire bonds

CPR1 CPR2

Temperature diode on

CCD

Charge injection

Four 1-stage and 2-stage SF in adjacent

columns

Four 2-stage SF in adjacent columns

Standard Field-enhanced Standard

No connections

this side

Image area

Extra pads for clock monitoring and

drive every 6.5 mm

Next Generation CPCCD : CPC2

Three different chip sizes with common design:

CPC2-70 : 92 mm 15 mm image area

CPC2-40 : 53 mm long

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)

Baseline design allows few MHz operation for the largest size CPC2

Page 9: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

9Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

CPC2 + ISIS1 Wafer

ISIS1

CPC2-70

CPC2-40

CPC2-10

5” wafers

One CPC2-70 : 105 mm 17 mm total chip size

Two CPC2-40 per wafer

6 CPC2-10 per wafer

14 In-situ Storage Image Sensors (ISIS1)

3 wafers delivered

Page 10: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

10Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

Clock monitor pads

CPR1/CPR2 pads

CPC2-40 in MB4.0

Johan Fopma, Oxford U Transformer drive for CPC2

“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

Transformer

Page 11: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

11Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

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.

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

Brian Hawes, Oxford U

Page 12: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

12Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

Radiation Damage Effects in CCDs: Simulations

Simulation at 50 MHz

Operating window

L. Dehimi, K. Bekhouche (Biskra U); G. Davies, C. Bowdery, A.Sopczak (Lancaster U)

● Full 2D simulation based on ISE-TCAD developed

● Trapped signal electrons can be counted

● CPU-intensive and time consuming

● 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

Signal density of trapped electrons in 2D

Page 13: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

13Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

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;

Page 14: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

14Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

In-situ Storage Image Sensor (ISIS)

RG RD OD RSEL

Column transistor

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

Development and design of ISIS is more ambitious goal than CPCCD

“Proof of principle” device (ISIS1) designed and manufactured by e2V Technologies

On-

chip

logi

c

On-

chip

sw

itche

s

Global Photogate and Transfer gate

ROW 1: CCD clocks

ROW 2: CCD clocks

ROW 3: CCD clocks

ROW 1: RSEL

Global RG, RD, OD

5 μm

Page 15: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

15Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

Output and reset transistors

Photogate aperture (8 μm square)

CCD (56.75 μm pixels)

The ISIS1 Cell

OG RG OD RSEL

OUT

Column transistor

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

Page 16: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

16Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

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

Page 17: 1 Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory LCFI Status Report: Sensors for the ILC Konstantin Stefanov CCLRC Rutherford Appleton Laboratory

17Konstantin Stefanov, CCLRC Rutherford Appleton Laboratory

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/