SOI SOI detectordetector SOI detector -...

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W.Kucewicz A Vertex Detector for the ILC; Ringberg Castle; May 28 - 31, 2006 1 SOI detector (SUCIMA project) SOI SOI detector detector (S (S UCIMA UCIMA project project ) ) Wojciech Kucewicz Wojciech Kucewicz AGH-Univ. of Science and Technology, On behalf of the SUCIMA Collaboration

Transcript of SOI SOI detectordetector SOI detector -...

W.Kucewicz A Vertex Detector for the ILC; Ringberg Castle; May 28 - 31, 2006 1

SOI detector(SUCIMA project)

SOI SOI detectordetector(S(SUCIMA UCIMA projectproject))

Wojciech KucewiczWojciech KucewiczAGH-Univ. of Science and Technology,

On behalf of the SUCIMA Collaboration

W.Kucewicz A Vertex Detector for the ILC; Ringberg Castle; May 28 - 31, 2006 2

OutlineOutlineOutline

Principle of the SOI sensor and Principle of the SOI sensor and technology sequencetechnology sequence

Preliminary test of the small area SOI Preliminary test of the small area SOI sensors on the high resistive substratessensors on the high resistive substrates

The full size SOI sensor The full size SOI sensor –– layout, layout, readout scheme and first measurementsreadout scheme and first measurements

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The main goal of the project was the

DEVELOPMENT OF AN ADVANCED IMAGING DEVELOPMENT OF AN ADVANCED IMAGING TECHNIQUETECHNIQUE OF EXTENDED RADIOACTIVE SOURCES USED IN OF EXTENDED RADIOACTIVE SOURCES USED IN

MEDICAL APPLICATIONSMEDICAL APPLICATIONS

Where “imaging” has be intended as the record of a dose map

Development & boundary conditions were defined by the specific end-user requirements:

BrachytherapyBrachytherapyHadrontherapyHadrontherapy

SUCIMASUCIMAThe collaboration The collaboration waswas made out of 9 Dept.made out of 9 Dept.’’s or Research Centers s or Research Centers and 2 companies from 5 EU countries.and 2 companies from 5 EU countries.

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Axial view

High activity seedMedium activity seedLow activity seed

Target

Online dose measurement inBrachytherapy

Online dose measurement inBrachytherapy

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Hadrontherapy:real-time beam monitoring

Hadrontherapy:Hadrontherapy:realreal--time time beam beam monitoringmonitoring

Basic principle:Basic principle: collection and imaging of secondary electrons emitted by thin Aluminum foils as the beam is delivered

vacuum chamber

HV

secondary emission foil

electron detector

PROFILE/CURRENT MEASUREMENT

beam

SLIMSLIM ≡ Secondary Emission for Low Interception Monitoring

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SOI Detector IdeaSOISOI DDetectoretector IdeaIdea

Readout electronicsReadout electronics

Silicon Silicon sensorsensor

On On the the same same waferwaferIs it possibleIs it possible??

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SOI Detector IdeaSOISOI DDetectoretector IdeaIdeaThe The wafer bondingwafer bonding techniques was chosen for SOI techniques was chosen for SOI

technologytechnology

Low resistivity

High resistivity

SIO2

SIO2

High resistivity

SIO2SIO2Thin low Thin low resistivityresistivity layer layer –– readout readout

electronics circuitelectronics circuit

High High resistivityresistivity support support –– sensitive areasensitive area

Termochemical bonding

11--1,5 1,5 μμmm

High resistivity

SIO2

Low resistivity

SIO2

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SOI Detector IdeaSOISOI DDetectoretector IdeaIdea

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SOI Detector SOISOI Detector Detector Advantages:Advantages:

•• The SOI sensor may merge the The SOI sensor may merge the advantages of the monolithic and advantages of the monolithic and hybrid detectorshybrid detectors

As a monolithic device eliminates bumpAs a monolithic device eliminates bump--bonding process and allows reductionbonding process and allows reductionof total sensor thickness of total sensor thickness reduction ofreduction of multiple scatteringmultiple scattering

Allows using high resistive detector substrates and operation inAllows using high resistive detector substrates and operation in fully fully depleted region depleted region good detection efficiency, enables detection of particles good detection efficiency, enables detection of particles with limited range in the silicon without with limited range in the silicon without backthinningbackthinning processprocess))

Gives possibility to use both type of transistors in readout chaGives possibility to use both type of transistors in readout channels nnels increased flexibility of the design, design optimisation for difincreased flexibility of the design, design optimisation for different ferent applicationapplication

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SOI Detector SOISOI Detector Detector

Disadvantages:Disadvantages:•• Needs a new technology developmentNeeds a new technology development

•• Relatively small size sensor limited by technology limitsRelatively small size sensor limited by technology limits

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SOI Detector TechnologySOISOI DDetectoretector TechnologyTechnology

Etching of the cave forEtching of the cave for pnpn junctionjunction

NN typetype,, Low resistivityLow resistivitySiOSiO22

NN typetype,, High resistivityHigh resistivity

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SOI Detector TechnologySOISOI DDetectoretector TechnologyTechnology

P P well diffusionwell diffusion

PP wellwell

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SOI Detector TechnologySOISOI DDetectoretector TechnologyTechnology

P & N diffusion of channel stoppers to P well & substrateP & N diffusion of channel stoppers to P well & substrate

P+P+

N+N+

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SOI Detector TechnologySOISOI DDetectoretector TechnologyTechnology

PN PN junction diffusion junction diffusion

PN PN junctionjunction

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SOI Detector TechnologySOISOI DDetectoretector TechnologyTechnology

PolysiliconPolysilicon deposition deposition

PolysiliconPolysilicon

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SOI Detector TechnologySOISOI DDetectoretector TechnologyTechnology

Source Source & & drain implantationdrain implantation

NMOSNMOS

PMOSPMOS

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SOI Detector TechnologySOISOI DDetectoretector TechnologyTechnology

First First metal metal layerlayer

Metal 1Metal 1

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SOI Detector TechnologySOISOI DDetectoretector TechnologyTechnology

Second metal layer Second metal layer

Metal 2Metal 2

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Test structures of the SOI detector

Test structures of the SOI Test structures of the SOI detectordetector

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Test structures of the SOI detector

Test structures of the SOI Test structures of the SOI detectordetector

Small readout matrices (8x8) with associated detector diodes or input pads for external signal sources were fabricated on the SOI wafers at the IET, Warsaw

Two readout channel configurations – with NMOS transistor switch (cell dimensions 140x122 μm2) and with transmission gate (140x140 μm2)

Contact to the detector placed in the V-shape cavity.

Row selection signals led by two parallel lines with opposite polarization, body of the structure densely grounded →→ reduction of the cross-talk between the electronics and detector

VDET

VSS

VDD

IN

RES

N_ROW_SEL

ROW_SEL

COL

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Detector ReadoutDDetectoretector RReadouteadoutOperation in un-triggered mode (for imaging applications)Analogue serial readout organisationReadout sequence similar to rolling-shutter but double sampling performed for every pixelExternal subtraction of samples for CDSWell defined integration time and short dead time

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Readout pixel

Row

_sel

shi

ft re

gist

er a

nd re

set l

ogic

Analog Output

Column_sel shift register

Dummy pixel

Control block CLK RST

READ

Cur

rent

refe

renc

e

Row_sel<0>

Column_sel<0>

Column_sel<1>

Column_sel<31>

Reset_rowl<0>

Row_sel<1>

Row_sel<31>

Reset_rowl<1>

Reset_rowl<31>

Sample I-after reset

Sample II-after integration time

Charge integration

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SUCIMA Imager DAQ for the SOI DetectorSUCIMA Imager DAQ SUCIMA Imager DAQ for the SOI Detectorfor the SOI Detector

The DAQ is equipped with 4 independent 4 independent analogue inputanalogue input channels channels with 12 bit ADCs, 1MB fast static RAM, the FPGA Virtex II XC2V1000 chip for advanced algorithms and the high speed USB 2.0 portUSB 2.0 port for a fast data transfer to and from a PC computer.

GUI – developed in LabVIEW environment, allows setting: the matrix size to be readout, readout frequency;It provides: the CDS or last frame readout mode, masking noisy pixels, subtracting pedestals, suppressing signals bellow threshold and writing data to the file.

VIRTEX IIXC2V1000

4FG456CES(324 I/O)

VIRTEX IIXC2V1000

4FG456CES(324 I/O)

40 MHz

BANK_7SE

NSO

R

SUCIMA_IMAGER

BANK_2 BANK_3

BA

NK

_5B

AN

K_4

BANK_6

BA

NK

_0B

AN

K_1

S RA

M

2x25

6Kx 1

6B

S RA

M

2x25

6Kx1

6B

USB

& 2

8 G

P IO

pi n

s

D32A18

D24

D16

.

JTA

G

A18

A18CLK

CTRL

328 USER’s I/O PADS

SEN

SOR

’S R

EPE

AT

ER

SRA

M

2x25

6Kx1

6B

S RA

M

2x25

6Kx1

6B XV18V04

EEPROM

DedicatedDedicated DAQ system calledDAQ system called„„SUCIMA imagerSUCIMA imager”” was was developeddeveloped for for

the SUCIMA projectthe SUCIMA project by INF by INF in Cracowin Cracow..

14 cm14 cm

9.5

cm9.

5 cm

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Stand Alone Detector Diodes and Electronics with Input PadsStand Alone DetectorStand Alone Detector Diodes Diodes

and Electronics withand Electronics with Input PadsInput Pads

Transfer characteristics were measured with external voltage pulse signal

with NMOS transistor switch → Measured DC output dynamic

range up to 1.0 Vwith transmission gate→ Measured DC output dynamic

range up to 1.6 V non-linearity at the middle range was reduced in the latest designs

Readout ElectronicsReadout Electronics

1.0E-12

1.0E-11

1.0E-10

1.0E-09

0 10 20 30 40 50 60Detector bias [V]

Leak

age

curr

ent

[A/m

m2 ]

e7 g8

1.0E-12

1.0E-11

1.0E-10

1.0E-09

0 10 20 30 40 50 60Detector bias [V]

Leak

age

curr

ent

[A/m

m2 ]

e7 g8

Pixel leakage current:→ From 200 nA down to 10 nA per

cm2 depending on the process Detector full depletion voltage:

→ 60 V down to 50 V for different iterations

Detector DiodesDetector Diodes

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Tests with the Laser LightTests Tests wwithith the Laser Lightthe Laser Light

Laser light not focused, shining from the backplane (biased by a metal mash)Wavelength = 850 nm4 μs wide light pulses – simulate particles passing through detector active volumeIntegration time = 1 msDetector polarization=60V10 000 events recorded and averagedInput signal scaled assuming the sensor gain of 11mV/MIP

GGood detector sensitivity for the ionising radiation and linear ood detector sensitivity for the ionising radiation and linear response as a function of the generated charge was observedresponse as a function of the generated charge was observed..

Linearity of Sensor ResponseLinearity of Sensor Response

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VDET

VSS

VDD

IN

RES

N_ROW_SEL

ROW_SEL

COL

tt

VinVin

RESRES

VinVin = (= (~ ~ leakage current leakage current + charge + charge collectioncollection))

„„pedestalpedestal””

ΔΔV ~charge V ~charge generatedgenerated by by particleparticle

Passing particlePassing particle

Output signal

Averaged pedestal

Output signal after pedestal subtraction

Resetsignal

Output signal

Averaged pedestal

Output signal after pedestal subtraction

Resetsignal

Tests with the 90 Sr Beta Source

Tests with theTests with the 90 90 SrSr Beta Beta SourceSource

26

Tests with the 90 Sr Beta SourceTests with theTests with the 90 90 SrSr Beta SourceBeta SourceSensor sensitivity tested with 90Sr beta sourceMeasurements conditions: complete depletion (Vdet= 60 V), integration time: Tint = 420 μs, source placed at the top of the sensor.Detector output signal amplified (4.5 ADC/mV) before digitalisationsOn-line CDS processing, off-line pedestal subtraction, common mode suppression and cluster search

Gaussian distribution of the noise

Landau distribution of the measured signals

The most probably value of signal per MIP: 5151 ADCADCNoise for the seed pixels:1.1.,8,8 ADCADC (670 e(670 e--))

19200 e19200 e

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Simulated electrostatic potential inside SOI sensor

Simulated electrostatic Simulated electrostatic potential inside SOI sensorpotential inside SOI sensor

X

Y

0 100 200 300 400-300

-250

-200

-150

-100

-50

0 ElectrostaticPotential

6.9E+01

6.4E+01

6.0E+01

5.6E+01

5.1E+01

4.7E+01

4.3E+01

3.8E+01

3.4E+01

3.0E+01

2.5E+01

2.1E+01

1.7E+01

1.2E+01

8.2E+00

3.8E+00

-5.0E-01

PixelPixel 0V0V Well Well 0V0V

Sens

orSe

nsor

dept

hde

pth Potential distribution at Potential distribution at 5 5 μμmm depthdepth

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Tests with the Alpha ParticlesTests with theTests with the Alpha ParticlesAlpha Particles

Alpha source placed at the distance of 1 cm from the detector backplaneInitial energy of particles = 5.5 MeVDetector fully depleted (VD=70V), integration time 720 μsOn-line CDS processing, off-line pedestal subtraction, common mode suppression and cluster search

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Design of a full size detector layoutDesign of a full size detector layoutDesign of a full size detector layoutDimensions: 24x24 mm2

128 x 128 = 16 384 channels4 sub-segments with independent parallel analogue outputsCell dimensions: 150x150μm2

Possibility to extend to ladders with dimensions up to 72x24 mm2 and small dead areas

Row

_sel

Col_sel

ADC

10.24mm 12mm

<0-63>

<0-6

3>

10.2

4mm

12m

m

ADC

ADCADC

ADC ADC

ADCADC

ADC

24mm

24m

m

72mm

24m

m

a) b)

c)

PixelPixelcavitycavity

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Full size detectorFFullull size detectorsize detector

, , ,

SOI detector 128 x 128 channels with integrated control electronics

SOI detector 128 x 128SOI detector 128 x 128 channelschannels with with integrated integrated controlcontrol electronicselectronics

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Full size detector - Tests with thelaser light

FFullull size detectorsize detector -- Tests with theTests with thelaser laser lightlight

Visualization of the readout results obtained with the best fullVisualization of the readout results obtained with the best full size size SOI detector and laser pointer light shined on two different SOI detector and laser pointer light shined on two different

quarters of the readout matrixquarters of the readout matrix

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„Baby Detector”– backup solution of the SOI sensor

„„Baby DetectorBaby Detector””–– backup solution of the SOI sensorbackup solution of the SOI sensor

Smaller number of the transistors, simpler functionality: Smaller number of the transistors, simpler functionality: 48 x 48 readout channels, area 1.2 cm x 1.2 cm, no digital control blocks

Configuration of the analogue blockConfiguration of the analogue block isis the same as on the main detectorthe same as on the main detector..Two versions Two versions –– with dashed with dashed guardringguardring (like on the main chip) and continuous (like on the main chip) and continuous guardringguardring –– reliability and effectiveness of both solutions reliability and effectiveness of both solutions waswas compared.compared.Reset and Column/Row selection signal must be generated externalReset and Column/Row selection signal must be generated externallyly ((NRowNRow and and NCNColumnolumn signals are generated internallysignals are generated internally))

Dashed Dashed guardringguardring Continuous Continuous guardringguardring

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„Baby Detector”– backup solution of the SOI sensor

„„Baby DetectorBaby Detector””–– backup solution of the SOI sensorbackup solution of the SOI sensor

Smaller number of the transistors, simpler functionality: Smaller number of the transistors, simpler functionality: 48 x 48 readout channels, area 1.2 cm x 1.2 cm, no digital control blocks

Configuration of the analogue blockConfiguration of the analogue block isis the same as on the main detectorthe same as on the main detector..Two versions Two versions –– with dashed with dashed guardringguardring (like on the main chip) and continuous (like on the main chip) and continuous guardringguardring –– reliability and effectiveness of both solutions reliability and effectiveness of both solutions waswas compared.compared.Reset and Column/Row selection signal must be generated externalReset and Column/Row selection signal must be generated externallyly ((NRowNRow and and NCNColumnolumn signals are generated internallysignals are generated internally))

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Light off

Light on

Light off

Light on

TThe output signal obtained for the detector exposed and not he output signal obtained for the detector exposed and not exposed to the red light from laser pointer.exposed to the red light from laser pointer.

„Baby Detector” – laser light„„Baby DetectorBaby Detector”” –– laser laser lightlight

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„Baby Detector”– Tests with Alpha Particles

„„Baby DetectorBaby Detector””–– Tests with Tests with Alpha ParticlesAlpha Particles

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„Baby Detector”– Tests with Beta Particles

„„Baby DetectorBaby Detector””–– Tests with Tests with BetaBeta ParticlesParticles

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ConclusionsConclusionsConclusionsFirst small area SOI pixel sensors have been fabricated.First small area SOI pixel sensors have been fabricated.The tests The tests results proveresults prove::

sensitivity of the test matrices for the MIP signals (measurements with 90Sr), wide dynamic range (measurements with laser spot and alpha particles), detector suitability for the detection of particles with limited range in silicon(measurements with alpha particles), effectiveness of the charge integration mechanism implemented in the readout circuit.

A larger and fully functional SOI sensor (128x128 readout channeA larger and fully functional SOI sensor (128x128 readout channels, active area of ls, active area of 2 cm x 2 cm, optimised for medical imaging applications) have be2 cm x 2 cm, optimised for medical imaging applications) have been designed and en designed and produced but only one produced but only one „„Baby detectorBaby detector”” was working.was working.

Next baNext batch tch of sensor with modified layout (smaller noof sensor with modified layout (smaller no polysiliconpolysilicon in the cave) will in the cave) will bebe applied soon.applied soon.

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Hybrids for SOI sensorsHybrids Hybrids for SOI for SOI sensorssensors

SOI SOI DetectorDetector 128x128 128x128 cells cells with driving circuits with driving circuits

SOI SOI DetectorDetector 48x48 48x48 cellscellswith external sequence electronicswith external sequence electronics

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Measurements setupMeasurements setupMeasurements setup

SOI test SOI test structurestructure

SOI SOI final final sensorsensor

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SimulationsSimulationsSimulations

The simulated devise structure, consisting of 1.2 μm thick silicon devise layer, 1 μm thick buried oxide 300 μm thick silicon detector substrate

The SOI sensor concept was validated in series of simulations and test structure measurements. The

simulations were performed with the DESSIS simulator from the ISE-TCAD package.

. In order to model the sensor operation 3 pixels with 20 μm width and 150 μm pitch were created in the detector substrate and several body ties and P-type wells were implemented in the devise layer of the sensor. The doping profiles for both detector and electronics part of the devise were provided by the silicon foundry. All the sensor electrodes were biased at nominal conditions.

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SimulationsSimulationsSimulationsSimulated charge collection for the particle hitting the SOI Simulated charge collection for the particle hitting the SOI

detector at the distance of 50 detector at the distance of 50 μμm from the central pixel. The hole m from the central pixel. The hole density presented at the impact time and 5 ns, 20 nsdensity presented at the impact time and 5 ns, 20 ns, , 100 ns later100 ns later

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SimulationsSimulationsSimulationsTotal current of the central pixel and two neighbour pixels Total current of the central pixel and two neighbour pixels