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EE143 – Ali Javey Slide 5-1 Section 2: Lithography Jaeger Chapter 2

Section 2: Lithography Jaeger Chapter 2 EE143 Ali Javey

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The lithographic process EE143 – Ali Javey

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Page 1: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-1

Section 2: Lithography

Jaeger Chapter 2

Page 2: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-2

The lithographic process

Page 3: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-3

Photolithographic Process(a) Substrate covered with silicon dioxide

barrier layer(b) Positive photoresist applied to wafer surface(c) Mask in close proximity to surface(d) Substrate following resist exposure and

development(e) Substrate after etching of oxide layer(f) Oxide barrier on surface after resist removal(g) View of substrate with silicon dioxide

pattern on the surface

Page 4: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-4

Photomasks - CAD Layout

• Composite drawing of the masks for a simple integrated circuit using a four-mask process

• Drawn with computer layout system

• Complex state-of-the-art CMOS processes may use 25 masks or more

Page 5: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-5

Photo Masks

• Example of 10X reticle for the metal mask - this particular mask is ten times final size (10 m minimum feature size - huge!)

• Used in step-and-repeat operation

• One mask for each lithography level in process

Page 6: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-6

Lithographic Process

Page 7: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-7

Printing Techniques

• Contact printing damages the mask and the wafer and limits the number of times the mask can be used

• Proximity printing eliminates damage

• Projection printing can operate in reduction mode with direct step-on-wafer, eliminating the need for the reduction step presented earlier

Contact printing

Proximity printing

Projection printing

Page 8: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-8

Contact Printing

wafer

hv

photoresist

Resolution R < 0.5m

mask plate is easily damagedor accumulates defects

PhotoMaskPlate

Page 9: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-9

Proximity Printing

wafer

hv

g~20m

exposed

Photoresist

R is proportional to ( g ) 1/2

~ 1m for visible photons,much smaller for X-ray lithography

Page 10: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-10

Projection Printing

hv

lens

wafer

P.R.focal plane

~0.2 m resolution (deep UV photons)tradeoff: optics complicated and expensive

De-Magnification: nX

10X stepper4X stepper1X stepper

Page 11: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-11

Aerial Images formed by Contact Printing, Proximity Printing and Projection Printing

Page 12: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-12

Optical Stepper

wafer

scribe line

1 2

Imagefield

field size increaseswith future ICs

field size increaseswith future ICs

Translationalmotion

Page 13: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-13

Light is in pulses of 20 ns duration at a repetition rate of a few kHz.

About 50 pulses are used.

Excimer Laser Stepper

Page 14: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-14

Photon Sources

Page 15: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-15

Resolution limits in projection printing

Page 16: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-16

Resolution limits: Bragg condition

Page 17: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-17

Image Degradation by lens

waferplane

parallelopticalbeam

grating withspatial frequency 1/P

P P=2L

...,2,1,0sin

nnP

-1

-2

+1

+2Mask lens

L L

0

sin = NA of lens

Page 18: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-18

The /NA limit

x

x

Image on wafer optical system

Mask Intensity

Imax

O

The lens has to collect at least the n=1 diffracted beamsto show any spatially varying intensity on wafer.Therefore Pm ( = 2 lm) / NA

Page 19: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-19

n=0

n=0 + n=1

n=0 + n=1 + n=3

n=0 + n=1 + n=3 + n=5

Resolution and the need for higher order terms

Page 20: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-20

point

best

off

Depth of Focus (DOF)

Page 21: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-21

FieldOxide

Photo mask

Different photo images

Example of DOF problem

Page 22: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-22

( ) .

( )

1 0 6

22 2

lNA

want small l

DOFNA

want large DOF

m m

lm

(1) and (2) require a compromise between and NA !

Tradeoffs in projection lithography

Page 23: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-23

Sub-resolution exposure: Phase Shifting Masks

Pattern transfer of two closely spaced lines

(a) Conventional mask technology - lines not resolved

(b) Lines can be resolved with phase-shift technology

Page 24: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-24

•A liquid with index of refraction n>1 is introduced between theimaging optics and the wafer. Advantages

1) Resolution is improved proportionately to n. For water, the index of refraction at = 193 nm is 1.44, improving the resolution significantly, from 90 to 64 nm.

2) Increased depth of focus at larger features, even those that are printable with dry lithography.

Immersion Lithography

Page 25: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-25

Image Quality Metric: Contrast

Page 26: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-26

* simulated aerial image of an isolated line

Image Quality metric: Slope of image

Page 27: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-27

resistresist

substrate

resist

substrate

resist

Position x

Finitecontrast

Infinitecontrast

Optical image

The need for high contrast

Page 28: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-28

Resists for Lithography

• Resists– Positive– Negative

• Exposure Sources– Light– Electron beams– Xray sensitive

Page 29: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-29

Two Resist Types• Negative Resist

– Polymer (Molecular Weight (MW) ~65000)– Light Sensitive Additive Promotes Crosslinking– Volatile Solvents– Light breaks N-N => Crosslink Chains– Sensitive, hard, Swelling during Develop

• Positive Resist– Polymer (MW~5000)– Photoactive Inhibitor (20%)– Volatile Solvents– Inhibitor Looses N2 => Alkali Soluble Acid– Develops by “etching” - No Swelling.

Page 30: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-30

Positive P.R. Mechanism

Photons deactivatesensitizer

polymer +photosensitizer

less cross-linking

dissolvein developersolution

Page 31: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-31

=E resist sensitivity

Resist contrast

T

log

Positive Resisthv

mask

P.R.

100%

E1 ETexposurephotonenergy(log scale)

resist thickness remaining

(linearscale)

exposed part is removed

Page 32: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-32

Negative P.R. Mechanism

1

1log EET

hv => cross-linking => insoluble in developer solution.

hv

E1ET

remaining

photonenergy

after development

%

mask

Page 33: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-33

Positive vs. Negative Photoresists

• Positive P.R.: higher resolution aqueous-based solvents less sensitive

• Negative P.R.:more sensitive => higher exposure throughput relatively tolerant of developing conditions better chemical resistance => better mask material less expensive lower resolution organic-based solvents

Page 34: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-34

Overlay Errors

+

+

+

+

Alignmentmarksfrom previousmaskinglevel

wafer

alignmentmask

photomaskplate

Page 35: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-35

sisimm TTrR

T Tsi change of mask and wafer tempcoefficient of thermal expansion of

mask & Si

m

m si

, .,

run-out error

waferradius

Thermal Run-in/Run-out errors

Page 36: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-36

(2) Translational Error

referrer

image

n+

Al

p

Rotational / Translational Errors

(3) Rotational Error

Page 37: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-37

Overlay implications: Contacts

n+

SiO2 SiO2

Al“ideal”

p-Si

SiO2 SiO2

Al

p-Sin+ “short”, ohmic contact

Alignment error

SiO2

n+

SiO2

Al

Solution: Design n+ region larger than contact hole

Page 38: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-38

Overlay implications: Gate edgeFox“Ideal”

poly-gate

S/D implantn+ Electrical

short

“With alignment error”

Solution: Make poly gate longer to overlap the FOX

Page 39: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-39

Total Overlay Tolerance

2 2total i

i

i = std. deviation of overlay error for ith masking step

total = std. deviation for total overlay error

Layout design-rule specification should be > total

Page 40: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-40

Standing Waves

substrate

PositivePhotoresist

hv

substrate

After developmentPositivePhotoresist.After developmentPositivePhotoresist.

Higher Intensity

Lower Intensity

Faster Development rate

Slower Development rate

Page 41: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-41

P.R.

Intensity = minimum whenn

mdx2

x d

m = 0, 1, 2,...

Intensity = maximum whenn

mdx4

m = 1, 3, 5,...

n = refractive index of resist

SiO2/Si substrate

Standing waves in photoresists

Page 42: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-42

Proximity Scattering

Page 43: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-43

Approaches for Reducing Substrate Effects• Use absorption dyes in photoresist• Use anti-reflection coating (ARC)• Use multi-layer resist process

1: thin planar layer for high-resolution imaging2: thin develop-stop layer, used for pattern transfer to 33: thick layer of hardened resist

(imaging layer)

(etch stop)(planarization layer)

Page 44: Section 2: Lithography Jaeger Chapter 2 EE143  Ali Javey

EE143 – Ali Javey Slide 5-44

Electron-Beam Lithography

V312.

Angstroms

for V in Volts

Example: 30 kV e-beam => = 0.07 Angstroms

NA = 0.002 – 0.005Resolution < 1 nm

But beam current needs to be 10’s of mA for a throughput of more than 10 wafers an hour.

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EE143 – Ali Javey Slide 5-45

Types of Ebeam Systems

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EE143 – Ali Javey Slide 5-46

Resolution limits in e-beam lithography

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EE143 – Ali Javey Slide 5-47

The Proximity Effect