monolithic pixel sensors

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inar at University of Geneva, November 6 th , 2013 1 Monolithic pixel sensors Ivan Perić

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Monolithic pixel sensors. Ivan Peri ć. Introduction – classification of CMOS sensors. Pixel type Simple pixels (no particle detection in pixel, analog output, rolling shutter readout) Intelligent pixels (particle detection in pixel, digital output, zero-suppressed readout) Technology - PowerPoint PPT Presentation

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Page 1: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 1

Monolithic pixel sensors

Ivan Perić

Page 2: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Introduction – classification of CMOS sensors

2

• Pixel type• Simple pixels (no particle detection in pixel, analog output, rolling shutter readout)• Intelligent pixels (particle detection in pixel, digital output, zero-suppressed readout)• Technology • Standard (CMOS, Opto- or HV-CMOS) or special technology (Hi-resistive CMOS, backside

depleted, SOI) • Bias voltage • Low (charge collection: diffusion based, sensor: epi layer)• High (charge collection: drift based, sensor: depleted layer)

Page 3: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Introduction – classification of CMOS sensors

3

• Simple pixels• CMOS pixel sensors• Standard MAPS• Intelligent pixels• INMPAS• TWELL MAPS• Depleted MAPS with intelligent pixels• HVCMOS (Hi-Res CMOS included)• Espros MAPS• T3 MAPS• SOI

LV MAPS(Epi Layer)

HV MAPS(Delpeted Layer)

Standard (HV-) or Opto-CMOS

Standard MAPS (“MIMOSA-type”)TWELL MAPS

HVCMOS,T3

Special technology INMAPS SOI,Espros

Page 4: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 4

Commercial CMOS monolithic pixel sensors

Page 5: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

CMOS monolithic sensors

• The original application of CMOS sensors – consumer electronics• Imaging sensors for digital cameras and mobile phones• Improvements are necessary for HEP

Phone with 41 M pixel sensor, 1.4um pixel size

Page 6: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Commercial imaging sensors

• Imaging sensors for digital cameras and mobile phones

Canon 120 M pixels CMOS, 2 µm pixel size

29 mm

Page 7: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

MOS technology

• MOS Technology – Integrated circuit technology based on Metal Oxide Semiconductor field effect transistors

Silicon p type

n type region “diffusion”

„Metal“ Electrode Insulator

Samsung 32nm process

Page 8: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

PN junction

• The simplest building element – PN junction• N-diffusion – potential minimum for electrons• P-substrate –potential barrier for electrons

Silicon n type Silicon p type

Free electrons

Page 9: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

PN junction

• Reversely biased – large depleted layer• Detector mode

Silicon n type Silicon p type

+

Depleted

Page 10: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

PN junction as sensor of radiation

• PN junction as sensor• 1. step - ionization

Atoms

Photons or particles

IonisationFree e-

Page 11: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

PN junction as sensor of radiation

• PN junction as sensor• 2. step – charge collection• Two possibilities for charge collection – drift (through E-force) and by diffusion (density gradient)

Atoms

Collection of electrons

Page 12: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

PN junction as sensor of radiation

• PN junction as sensor• 3. step – charge to voltage conversion• Collection of the charge signal leads to the potential change

AtomsPotential change

Page 13: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

CMOS pixel

• Pixel sensor in MOS technology

N-type regionDiffusion (shallow)

Or well (deep)

Sensor-junctionMOS FET

Sensor-junction

MOS FET

Gate

Page 14: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

CMOS pixel

• N in P diode acts as sensor element – signal collection electrode

N-type regionDiffusion (shallow)

Or well (deep)

Sensor-junctionMOS FET

Sensor-junction

MOS FET

Gate

Page 15: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

CMOS pixel

• Charge generated by ionization is collected by the N-diffusion• This leads to the potential change of the N-diffusion• The potential change is transferred to transistor gate – it modulates the transistor current

N-type regionDiffusion (shallow)

Or well (deep)

Sensor-junctionMOS FET

Sensor-junction

MOS FET

Gate

Page 16: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Rolling shutter readout

• Readout principle: Many pixels (usually one row) share one readout line• Additional MOSFET used as switch• The readout lines are connected to the electronics at the chip periphery that does signal

processing

A

AAAAA

SwitchSwitch

Pixel i+1Pixel iPeriphery of the chip

Page 17: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 17

CMOS monolithic pixel sensors for particle tracking

Page 18: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

CMOS sensors for particle tracking

• Can CMOS structure be used for detection of high energy particles in particle tracking?• Yes, but fill factor is an issue – ratio of the sensitive versus insensitive area

Detected Not detected

Charge collection by drift

Absorbed by electronics

Page 19: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Fill-factor

• Partial signal collection in the regions without E-field

Page 20: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Fill-factor

• Partial signal collection in the regions without E-field

Recombination

Page 21: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Overview

• Partial signal collection in the regions without E-field

Recombination

Page 22: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Overview

• Partial signal collection in the regions without E-field

Charge collection by diffusion

Page 23: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Fill-factor

• Partial signal collection in the regions without E-field

Charge collection by diffusion

Page 24: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Fill-factor

• In the case visible light imaging, the insensitive regions do not impose a serious problem• Light can be focused by lenses• Exposure time can be increased• In the case of particle tracking, any insensitive region should be avoided

Page 25: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

CMOS pixel sensor with 100% fill factor

• MOS sensor with 100% fill-factor• Based on epi-layer• Monolithic active pixel sensor - “MAPS”

Lightly p-doped epi-layer

Heavily p-doped P-well

N-diffusion or N-well

MOS FETNMOS

Page 26: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

CMOS pixel sensor with 100% fill factor

• Ionization in the epi-layer• Charge collection by diffusion

N-diffusion or N-well

Particle

Page 27: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 27

MAPS

Page 28: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 28

CMOS pixel sensor with 100% fill factor - MAPS

MAPS

NMOS transistor in p-well N-well (collecting region)Pixel i

Charge collection (diffusion)

P-type epi-layer

P-type substrate Energy (e-)

Page 29: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

MAPS

• Many institutes are developing MAPS, for instance: IPHC Strasbourg (PICSEL group)• Family of MIMOSA chips• Applications:, STAR-detector (RHIC Brookhaven), Eudet beam-telescope and ALICE inner

tracker upgrade

http://www.iphc.cnrs.fr/Monolithic-Active-Pixel-Sensors.html

Page 30: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

MAPS

http://www.iphc.cnrs.fr/Monolithic-Active-Pixel-Sensors.html

Ultimate chip for STARMIMOSA 26 for Eudet telescope

• MIMOSAs are based on rolling shutter RO but use more complex pixel electronics• Continuous reset and double correlated sampling

Page 31: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Charge collection & technology studies – simple demonstrators

Production

MimoStar3

MimoTEL Imager10µ Imager12µ

Mimosa16 Mimosa16

Latchup ADC ADC MyMap

TestStruct

Real size prototype - yield studiesReticule 2x 2 cm 2006

Data compression - digitizationSara 2006Suze 2007

Final circuits – sub-blocs integration

Mimosa22

2008

Pixel Array

DiscriminatorsZero Suppression

Bias Readout

2007

1999

MAPS

Page 32: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 32

Advanced CMOS pixel sensors with intelligent pixels

Page 33: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 33

Frame readout

- Simple pixels- Signal and leakage current is

collected- No time information is attached to

hits- The whole frames are readout Small pixels Low power consumption Slow readout

Page 34: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 34

Sparse readout

6

9

9

3

6

9

9

3

- Intelligent pixels- FPN is tuned inside pixels- Leakage current is compensated- Hit detection on pixel level- Time information is attached to hits Larger pixels Larger power consumption Fast (trigger based) readout

Page 35: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 35

Intelligent pixel

LatchComparatorCR-RC

4-bit tune DACReadout bus

CSA

Bus driver

RAM

Page 36: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 36

Sparse readout

Sparse readout

Rolling shutter readout

Reset

Comp. out

Sensor

RO enable

Comp. out

Sensor

Page 37: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

CMOS electronics

• Two transistor types n-channel NMOS and p-channel PMOS are needed for the realization of complex circuits

Silicon p type

Silicon n type

„Metal“ ElectrodeInsulator

Silicon n type

Silicon p type

„Metal“ ElectrodeInsulator

NMOS PMOS

NMOS

PMOS

Free e-

Holes

Holes

Page 38: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

CMOS electronics

• Example: A good voltage amplifier can only be realized with CMOS

Silicon p type

Silicon n type

„Metal“ ElectrodeInsulator

Silicon n type

Silicon p type

„Metal“ ElectrodeInsulator

NMOS PMOS

NMOS

PMOS

Free e-

Holes

Page 39: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

MAPS structure with CMOS pixel electronics

• If PMOS transistors are introduced, signal loss can happen

NMOS transistor in p-well

N-well (collecting region)

Pixel i

P-type epi-layer

P-type substrate Energy (e-)

MAPS with a PMOS transistor in pixel

PMOS transistor in n-well

Signal collectionSignal loss

Page 40: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 40

Advanced structures: INMAPS

Page 41: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 41

INMAPS

NMOS shielded by a deep p-wellPMOS in a shallow p-well

N-well (collecting region)

Pixel

P-doped epi layer

INMPAS

• Deep P-layer is introduced to shield the PMOS transistors from epi layer• No charge loss occurs• This is not a CMOS standard process• Only one producer so far: Tower Jazz

Page 42: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Overview

• INMAPS Tower Jazz process is gaining popularity in particle physics community• /ALICE inner tracker)• It was originally developed by the foundry and the Detector Systems Centre, Rutherford Appleton

Laboratory

2 Megapixels, large area sensorDesigned for high-dynamic range X-ray imaging40 µm pixel pitch1350 x 1350 active pixels in focal planeAnalogue readoutRegion-of-Reset setting140 dB dynamic range20 frames per second

FORTIS chip

http://dsc.stfc.ac.uk/Capabilities/CMOS+Sensors+Design/Follow+us/19816.aspx

Page 43: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Overview

• Detector Systems Centre, Rutherford Appleton Laboratory – some examples

http://dsc.stfc.ac.uk/Capabilities/CMOS+Sensors+Design/Follow+us/19816.aspx

Wafer scale 120 x 145 mm chip for medical imaging

Page 44: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 44

TWELL - MAPS

Page 45: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 45

TWELL MAPS

Triple-well MAPS

Deep n-well 2. n-wellP-well

NMOS PMOS

Pixel

Epi-layer Diffusion

Energy (e-)

Signal lossSignal collection

• Collection electrode is a deep n-well• To avoid crosstalk, secondary n-well is used for digital electronics• Rely on diffusion, implemented in low voltage CMOS processes• Collaboration: INFN Pisa, Pavia, Trieste, Padova, Torino, Bologna

Page 46: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 46

TWELL MAPS• APSEL Chips for B-factories

The APSEL4D MAPS chip bonded to the chip carrier.

Schematic drawing of the full Layer0 made of 8 pixel modules mounted around the beam pipe with a pinwheel arrangement.

“Thin pixel development for the SuperB silicon vertex tracker”, NIMA vol. 650, 2011

Page 47: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 47

Fast CMOS detectors based on drift charge collection:detectors in HVCMOS-processes and the CMOS

processes with a high resistive wafer

Page 48: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 48

Drift based detector: HVMAPS• HVMAPS rely on the charge collection by drift• Fast charge collection – high radiation tolerance• The key is the use of a high voltage n-well in a relatively highly doped substrate• Pixel electronics is embedded in the n-well• Two concepts:• High Ohmic Monolithic Pixels - LePIX – relies on a special CMOS process with high resistive

substrate (CERN, Geneve)• HVCMOS (or smart diode arrays - SDAs) – use a commercial HVCMOS process

Page 49: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 49

HVCMOS detectors (smart diode arrays)

Page 50: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 50

P-Substrate

Depleted

“Smart” Diode

n-Well

Pixel

“Smart diode” Detector

Drift Energy (e-)

• Smart diode array

SDA

Page 51: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

SDA

• Collected charge causes a voltage change in the n-well.• This signal is sensed by the amplifier – placed in the n-well.

PMOS

N-well

NMOS

DS

G

holes

electrons

P-well

P-substrate

Page 52: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

SDA

• Collected charge causes a voltage change in the n-well.• This signal is sensed by the amplifier – placed in the n-well.

P-substrate

Page 53: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

SDA

P-substrate

• Collected charge causes a voltage change in the n-well.• This signal is sensed by the amplifier – placed in the n-well.

Page 54: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 54

Intelligent pixel

ComparatorCR-RC

CSA

N-well

AC coupling

3.3 V

-50 V

P-substrate

Page 55: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 55

Intelligent pixel

ComparatorCR-RC

CSA

N-well

AC coupling

3.3 V

-50 V

P-substrate

Page 56: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 56

Intelligent pixel

ComparatorCR-RC

CSA

N-well

AC coupling

3.3 V

-50 V

P-substrate

Page 57: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 57

Intelligent pixel

ComparatorCR-RC

CSA

N-well

AC coupling

3.3 V

-50 V

P-substrate

Page 58: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 58

Intelligent pixel

ComparatorCR-RC

CSA

N-well

AC coupling

3.3 V

-50 V

P-substrate

Page 59: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 59

Intelligent pixel

ComparatorCR-RC

CSA

N-well

AC coupling

3.3 V

-50 V

P-substrate

Page 60: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 60

Intelligent pixel

ComparatorCR-RC

CSA

N-well

AC coupling

3.3 V

-50 V

P-substrate

Page 61: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

3D layout of a “smart diode”

40 µm

3D layout generated by GDS2POV software

Page 62: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Applications

• Mu3e experiment at PSI and ATLAS upgrade option

5 m

m

62

Mu3e prototype chip

4.4m

m

ATLAS prototype chip

Page 63: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 63

Special monolithic technologies

Page 64: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Espros

64

N-type

P-diffusion

Depleted

Ohmic connection

P-wellN-well

• Espros – semiconductor company in Switzerland

Page 65: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Espros

65

HV

N-type depleted

N-well

P-diffusion

No ohmic connection

P-well

Page 66: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

Espros

66

P-wellN-well

HV

N-type depleted

P-diffusion

Page 67: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013

T3-MAPS

67

P-well

T3-well

P-substrate

• T3-MAPS rely on a special option in IBM 130nm technology

Page 68: Monolithic pixel sensors

Seminar at University of Geneva, November 6 th, 2013 68

• Thank you!