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Lecture 20: On-Wafer Sensors Spanos EE290H F05 1 In-chamber and on-wafer sensors A Paradigm Shift

A Paradigm Shiftee290h/fa05... · Lecture 20: On-Wafer Sensors EE290H F05 Spanos 3 Thermocouples • operating principle Peltier-Seebeck effect, up to 3000o C T gradient along wires

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Page 1: A Paradigm Shiftee290h/fa05... · Lecture 20: On-Wafer Sensors EE290H F05 Spanos 3 Thermocouples • operating principle Peltier-Seebeck effect, up to 3000o C T gradient along wires

Lecture 20: On-Wafer Sensors

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In-chamber and on-wafer sensors

A Paradigm Shift

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Overview• Exact chamber environment control is relatively new• Various sensors (pressure, gas flow, gas composition,

temperature) are needed to accomplish it.• An interesting transition to “on-wafer” sensors holds

much promise...

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Thermocouples• operating principle

Peltier-Seebeck effect, up to 3000o CT gradient along wires of different materials develop different emfemf measures junction Tplatinum rhodium alloy, or silicon based sensitivity 100-200μV /oK

• problemsbig problems with shield designradiative effectslow signal -- need amplifiers or use thermopileinvasivegas T measurement is very hard, especially < 10-4 torr

• commentsinexpensive, low drift low bandwidth accuracy ~+/- 5oC at 800oC where do you want to measure T ?

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Acoustic Wave sensors

• operating principle – acoustic wave is transmitted through body– surface and internal waves propagate through body at

T dependent speed– interference with source gives beats – beat frequency determines T

• issues– implementation difficulty – invasive– calibration

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Pyrometry• operating principle

– hot objects radiate– radiation is wavelength dependent– radiation model for black bodies (Planck's Law)

λ in microns, T in oK, Rλ

– for non-black bodies need to account for emissivity• issues

– surface properties affect radiation– multiple internal reflections– emissivity is wavelength and geometry dependent– can change during processing– calibrations via thermocouples, difficult

)1(37418

/143885 −= Te

R λλ λ

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Pressure Sensors

• direct gauges– displacement of a solid or liquid surface– capacitance manometer, McLeod pressure transducer

• indirect gauges– measurement of a gas related property– momentum transfer, charge generation

• huge range of available sensors– cost– sensitivity– range

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Capacitance manometer

• basic idea– pressure differential causes

displacement of diaphragm– sense capacitance change

between diaphragm and fixed electrode

– resolution 10-2 %at 2 hertz and 10-3 torr

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Gas flow meters• differential pressure meters• thermal mass flow meters

– mass flow = K / (T1 - T2)– K depends on specific heat of gas etc.– must be calibrated for different gases– accuracy ~ 1 sccm at flows of 40 sccm– low bandwidth because of thermal inertia

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Mass Spectrometers

• two types– flux analyzers : sample gas through aperture– partial pressure sensors : analysis in exhaust stack

• issues– recombination in mass spec tube changes – indistinguishable species : (ex: CO, N2 and Si have

same amu (28))– pressure measurements are removed from

processing chamber

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RGA• basic idea

special kind of mass spectrometermeasures gas compositions works at low vacuum < 10-5 torrion beam is produced from gas sample by e-bombardmentbeam is collimated by electric fieldsq/m ratio of ions determines bending in B fielddetection of ions via a Faraday cup

• issuesquadrupole (magnetless design)very noisy !!good for diagnosticscan withstand 500 oCcan also be used at higher pressures with differential pumpsmass range 50 amu, resolution 2 amu,

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How about placing sensors on the wafer???

Sensarray products

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Calibration is an issue...

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Long Term Reliability also an Issue...

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On-Wafer Etch Rate by Resonant Structure

IEEE TRANSACTIONS ON SEMICONDUCTOR MANUFACTURING, VOL. 11, NO. 2, MAY 1998A Novel In Situ Monitoring Technique for Reactive Ion Etching Using a Surface Micromachined SensorMichael D. Baker, Frances R. Williams, Student Member, IEEE, and Gary S. May, Senior Member, IEEE

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Remote reading of resonant sensor

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Noise is the biggest problem...

On the bench... In the chamber...

When plasma is on...

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But it works! (almost)

Innovative

noisy

intrusive

may contaminate...

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Our VisionIn-situ sensor array, with integrated power and telemetry

Applications:process control, calibration, diagnostics & monitoring,process design

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Issues

• Sensor arrays– inexpensive, modular– environmentally isolated– transparent to wafer handling robotics– on-board power & communications

• Operating mode– no equipment modifications !!– Smart “dummy” wafer for in-situ metrology

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Test Case: Etch Rate

• Onboard etch-rate sensor for plasma etch– many sensor points on a wafer– accurate film thickness measurement– real-time data available– etch-friendly materials– wired power and communications (for now)

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Transduction Scheme - Etch Rate

Van der Pauw structure: ρπ

⎟⎠⎞

⎜⎝⎛⎟⎠⎞

⎜⎝⎛=

VIt 2ln

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Current Design

• Integrated Sensor Wafer Test Design• 57 etch-rate sensors on a 4” wafer• Full-wafer addressing of each sensor from a single die• Redundant interconnect to enhance yield• Four styles of sensor, selectable from a single die• On-board current-sourcing• Wired power and communications (at first)• Expandable to allow wireless power and communication

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Experimental Procedure

• Bond wires to wafer– solder wires to “strip header”– glue header to wafer edge– wire bond from header to wafer’s bond pads

• Verify operation on bench• Place wafer in XeF2 Chamber

– Measure film-thickness / etch-rate in real time– Calibrate using Nanospec thickness measurements

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Pictures

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Results

• 8 sensors (in a row) wired together in series• Everything works perfectly!• In-Situ XeF2 test performed

– XeF2 etch rate much too fast (~0.2μm/sec)– Sensor structure only 0.45 μm thick, gone in 2 sec– Sensors wired in series so when one etches through,

all measurements stop⇒ Data collected during etch, but no calibration

available

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Data - Etch #3

0 1 2 3 4 5 6 7 8 9 100

100 0

200 0

300 0

400 0

500 0P o ly s ilic on Th ic k ne s s vs . Tim e fo r E x pe rim en t #3

Tim e (s ec )

Mea

sure

d Th

ickn

ess

(A)

0 1 2 3 4 5 6 7 8 9 100

50 0

100 0

150 0

200 0P o ly s ilic on E tc h -R a te vs . Tim e fo r E x pe rim e n t #3

Tim e (s ec )

Filt

ered

Etc

h-R

ate

(A/s

ec)

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How about completely wireless???

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“Smart dummy” developed in 1998

• Developed and tested at the UC Berkeley Microfabrication Laboratory.

• 4 sensors, wafer covered with layer of epoxy• LED used for real-time, one-way transmission

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First Test results in plasma, 1999

13.56MHz, 100W, 0.76 Torr, O2

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An Update on OnWafer Sensors

• OnWafer technologies Inc, a Berkeley startup, was founded in 2000.

• Today OnWafer products are in use in all of the major fabs around the world, and by all the major tool makers (LAM, Applied, TEL, Nikon).

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Basic OnWafer System

IR DongleIR Dongle

Base StationBase Station

SensorWaferSensorWafer

ShipperShipper

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feedbackprocess control

processingequipment

data

OnWafer

base station

The Approach

wafers to be processed

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• 42 sensors/wafer, 1Hz• 0.5 °C accuracy• Rechargeable. • Functional up to 140 °C, several kW RF• Suitable for oxide/poly plasma etch• Non-contaminating, cleanable and reusable

PlasmaTemp SensorWafer

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Example - Process Monitoringof 200mm Poly Etching

Increased HeLow He

pre-etch

main etch

de-chuckover etch

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Cool chuck - 200mm Poly Etching

main etch

Temperature fluctuations during main etch

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Can see rotating magnetic field !

phase delay in temp fluctuationCan calculate B-field periodCan see rotation is clockwise

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Example - Gas flow trouble in TEL DRM Etcher

“before” data is hotter, further, the pre-etch step is significantly less uniform…“before” data is hotter, further, the pre-etch step is significantly less uniform…

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Example - Comparison between 8 PEB plates on a 193nm wafer track (+/- 0.1C accuracy)

11 12 13 14 21 22 23 24Best!

Worst!

Data collection in two 10-minute cassette-to-cassette missionsData collection in two 10-minute cassette-to-cassette missions

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On-Wafer PEB / CD Analysis

P6P6P5P5P4P4P3P3P2P2P1P1

Six TEL ACT 8 plates used for 90nm CD lines (193nm Lithography)Six TEL ACT 8 plates used for 90nm CD lines (193nm Lithography)

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Much more than you ever wanted to know about Post Exposure Bake

Overshoot

Cooling

Steady

Heating

Chill

200mm ArF90nm

130oC 60sec

Courtesy OnWafer Technologies

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PEB Evolved from a Single Zone to Multi-Zone Control System Why?

Multi-Zone Control

Single Zone Control

10 Years of Product

Evolution

Post Exposure Bake Track Equipment Complexity is Increasing

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PEB Hotplate Thermal Profile Optimization System

Baseline Thermal Profile

Condition

Offset Generator

Engine

Plate Type Specific Thermal Profile Modeling

Engine

Offset ValuesOptimized for Both Within-Plate and

Plate-to-Plate Thermal Profile

Uniformities

Output

Input

BakeTemp™& OnView™

AutoCal™

Input

Courtesy OnWafer Technologies

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PEB Temp Control

16 plates, 120 ºC Target

2.700oC

Target = 120oC

0.175oC

Before After

Courtesy OnWafer Technologies

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Spatial PEB/CD Distribution Correlation

• Plotting both the bake plate temperature trajectory and R2

from temperature-CD correlation against bake time:

Max R2 during the transient heating period

Continued high R2

during steady state due to poor temperature control in single-zone plate design

• Plotting both the bake plate temperature trajectory and R2

from temperature-CD correlation against bake time:

Max R2 during the transient heating period

Continued high R2

during steady state due to poor temperature control in single-zone plate design

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PEB Hotplate Critical Dimension Optimization System

Baseline Thermal Profile

Condition

Offset Generator

Engine

Plate Type Specific Thermal Profile Modeling

Engine

Offset ValuesOptimized for Both Within-Plate and

Plate-to-Plate Critical Dimensions

Uniformities

Output

Input

BakeTemp™& OnView™

AutoCal™

Input

Input

Resist & Litho Cell Specific CD

Modeling Engine

AutoCD™

Baseline CD Profiles per Plate Customer

Provided

Input

Courtesy OnWafer Technologies

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CDU Improvement

AcrossPlate Plate to

Plate

AutoCD

AutoCalPOR

0

0.5

1

1.5

2

2.5

3

3.5

AutoCDAutoCalPOR

Courtesy OnWafer Technologies

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The New Problem

How can we improve the across-wafer CDU? How much can we improve CDU?

Poor Across-Wafer CD Uniformity

Processing Tool

EtchEtch

Wafer

LithoLitho

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Supervisory Control with Wireless Metrology

Compensate for systematic spatial non-uniformities across the litho-etch sequence using all available control authority:

– Exposure step: die to die dose

– PEB step: temperature of multi-zone bake plate

– Etch: backside pressure of dual-zone He chuck

Exposure PEB /Develop Etch

Wafer-levelCD MetrologyOptimizer

Scatterometry/CDSEM

dose temperature He pressure

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Next Step: Zero-Footprint Metrology Wafer

Prototyping a zero-footprint metrology wafer with optical detection unit and encapsulated power source.

Data Transmission

Photo-/RF Transmitter

Data Processing, Storage Unit

Dielectric Layer

Si

BatteryData Acquisition Unit

500μm

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Self-contained wireless transmitter

+ -Power

+ -

Power Management & RF Transmission Unit

Measurement Units

Integrated excitation/detection Unit

Power Unit Thin film Battery

Proposed Architecture

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3 x 3 Pixels Optical Metrology Prototype

Bottom Wafer with LEDPhotodetector integrated

Top Wafer

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Feasibility Test: Thickness Measurement

LEDPD

Si

Packaging Substrate

Glass Slide

Test Coating

Filter

5mm

Green LED

Blue LED

1500 1600 1700 1800 1900 2000 2100 2200-16

-14

-12

-10

-8

-6

-4

-2

Ref

lect

ion

Inte

nsity

(a.u

.)

PR Thickness (nm)

Excitation λ=525nm

Theoretical Curve

1500 1600 1700 1800 1900 2000 2100 2200-16

-14

-12

-10

-8

-6

-4

-2

Ref

lect

ion

Inte

nsity

(a.u

.)

PR Thickness (nm)

Excitation λ=525nm

Theoretical Curve

Shipley S1818 PRon Glass Slide

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Wireless Aerial Image Metrology

Mask

light

Image system

Wafer

NAPartial coherenceIllumination aberrationsDefocusmagnification

Aerial image

Latent image

Resist image

Mask image

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An Integrated Aerial Image Sensor

How can a μm detector retrieve nanometer-scale resolution of the aerial image?

How can a μm detector retrieve nanometer-scale resolution of the aerial image?

Dark contact mask forms a “moving” aperture to capture incident electromagnetic field.

Poly-silicon mask

Substrate

Photo-detector

Mask aperture

Φ1 Φ2 Φ3 Φ1 Φ2 Φ3

p-Si

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Moiré Patterns for Spatial Frequency Shift

Patterns Overlap Pattern rotates 4o Pattern rotates 8o Pattern rotates 16o

Nar

row

CD

Wid

e C

D

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Aperture pattern shift testing

Image pattern

Detect pattern

4.4

2.2

2

4.4

d

Detector mask layout design

Mask layout

-40 -20 0 20 40 60 80 100 120 140 16035000

40000

45000

50000

55000

60000

-20 0 20 40 60 80 100 120 140 160

60000

70000

80000

90000

100000

110000

120000

image pattern

inte

nsity

x(pixel)

Measurement result

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Near-Field Optical Simulation

Intensity at the center of the simulation domainm

ask

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Spin

HMDS

PA Bake

Exposure

PEB

Develop

PD Bake

Photoresist Removal

ELMELM

Poly Etch System

ADIADI AEIAEI

Etch

Etch

Etch

Present Status of “Active” CD Control

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On-wafer and in-line metrology in pattern transfer

Spin

HMDS

PA Bake

Exposure

PEB

Develop

PD Bake

Photoresist Removal

ELMELM

Poly Etch SystemEtch

Etch

Etch

T (t, x, y)T (t, x, y)

T (t, x, y)V (t, x, y)E (t, x, y)…

T (t, x, y)V (t, x, y)E (t, x, y)…

I (x, y)I (x, y)

OCDOCD

Thin FilmThin Film

OCDOCD OCDOCD

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CDU control has to incorporate many strategies

Spin

HMDS

PA Bake

Exposure

PEB

Develop

PD Bake

Photoresist Removal

ELMELM

Poly Etch SystemEtch

Etch

Etch

T (t, x, y)FF control

T (t, x, y)FF control

T (t, x, y)V (t, x, y)E (t, x, y)FF/FB Control, chuck diagnostics

T (t, x, y)V (t, x, y)E (t, x, y)FF/FB Control, chuck diagnostics

I (x, y)Optimal Pattern Design

I (x, y)Optimal Pattern Design

OCDProfile Inversion

FB Control

OCDProfile Inversion

FB Control

Thin FilmFB/FF Control

Thin FilmFB/FF Control

OCDFB Control

OCDFB Control

OCDFB/FF Control

OCDFB/FF Control