EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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EE143 – Ali Javey Slide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader
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Transcript of EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

Page 1: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-1

Section 2: Lithography

Jaeger Chapter 2

Litho Reader

Page 2: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-2

The lithographic process

Page 3: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-6

Lithographic Process

Page 7: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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

Contact printing

Proximity printing

Projection printing

Page 8: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

Diffraction

EE143 – Ali Javey Slide 5-11

Page 12: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-12

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

Page 13: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-13

Photon Sources

Page 14: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

14

Optical Projection Printing Modules Optical System:

illumination and lens

Mask: transmission and diffraction

Resist: exposure, post-exposure bake and dissolution

Wafer Topography: scattering

Alignment:

Page 15: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-15

Optical Stepper

wafer

scribe line

1 2

Imagefield

field size increaseswith future ICs

field size increaseswith future ICs

Translationalmotion

Page 16: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

16

Resolution in Projection Printing

Minimum separation of a star to be visible.

f = focal distanced = lens diameter

Page 17: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-17

Resolution limits in projection printing

Page 18: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-18

point

Depth of Focus (DOF)

Page 19: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-19

Page 20: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-20

FieldOxide

Photo mask

Different photo images

Example of DOF problem

Page 21: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-21

( ) .

( )

1 0 6

22 2

lNA

want small l

DOFNA

want large DOF

m m

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

Tradeoffs in projection lithography

Page 22: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-22

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 23: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-23

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

Advantages1) 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 24: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-24

Image Quality Metric: Contrast

Contrast is also sometimes referred as the Modulation Transfer Function (MTF)

Page 25: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

Questions:

EE143 – Ali Javey Slide 5-25

How does contrast change as a function of feature size?

How does contrast change for coherent vs. partially coherent light?

Page 26: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-26

* simulated aerial image of an isolated line

Image Quality metric: Slope of image

Page 27: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-27

resistresist

substrate

resist

substrate

resist

Position x

Finitecontrast

Infinitecontrast

Optical image

The need for high contrast

Page 28: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-28

Resists for Lithography

• Resists– Positive

– Negative

• Exposure Sources– Light

– Electron beams

– Xray sensitive

Page 29: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-29

Two Resist Types• Negative Resist

– Composition:• Polymer (Molecular Weight (MW) ~65000)

• Light Sensitive Additive: Promotes Crosslinking

• Volatile Solvents

– Light breaks N-N in light sensitive additive => Crosslink Chains

– Sensitive, hard, Swelling during Develop

• Positive Resist– Composition

• Polymer (MW~5000)

• Photoactive Dissolution Inhibitor (20%)

• Volatile Solvents

– Inhibitor Looses N2 => Alkali Soluble Acid

– Develops by “etching” - No Swelling.

Page 30: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-30

Positive P.R. Mechanism

Photons deactivatesensitizer

polymer +photosensitizer

dissolvein developersolution

Page 31: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-31

Resist contrastQf

log

Positive Resisthv

mask

P.R.

100%

E1 ETexposurephotonenergy(log scale)

resist thickness remaining

(linearscale)

exposed part is removed

Q

Qf

Q0

Page 32: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-32

Negative P.R. Mechanism

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

hv

E1ET

remaining

photonenergy

after development

%

mask

Q0

Qf

Page 33: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-34

Overlay Errors

+

+

+

+

Alignmentmarksfrom previousmaskinglevel

wafer

alignmentmask

photomaskplate

Page 35: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-35

sisimm TTrR

T Tsi change of mask and wafer temp

coefficient of thermal expansion of

mask & Si

m

m si

, .

,

run-out error

waferradius

(1) Thermal Run-in/Run-out errors

Page 36: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-36

(2) Translational Error

referrer

image

n+

Al

p

Rotational / Translational Errors

(3) Rotational Error

Page 37: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-37

Overlay implications: Contacts

n+

SiO2 SiO2

Al“ideal”

p-Si

SiO2 SiO2

Al

p-Si

n+ “short”, ohmic contactAlignment error

SiO2

n+

SiO2

Al

Solution: Design n+ region larger than contact hole

Page 38: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-38

Overlay implications: Gate edge

Fox“Ideal”

poly-gate

S/D implantn+ Electrical

short

“With alignment error”

Solution: Make poly gate longer to overlap the FOX

Page 39: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-42

Proximity Scattering

Page 43: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

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: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-44

Electron-Beam Lithography

V

312.

Angstroms

for V in Volts

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

NA = 0.002 – 0.005

Resolution < 1 nm

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

Page 45: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-45

Types of Ebeam Systems

Page 46: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-46

Resolution limits in e-beam lithography

Page 47: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

EE143 – Ali Javey Slide 5-47

The Proximity Effect

Page 48: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.
Page 49: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

Richard Feynman

Page 50: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.
Page 51: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.
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Page 53: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.
Page 54: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

Dip Pen Nanolithography

Dip-Pen Nanolithography: Transport of molecules to the surface via water meniscus.

Page 55: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

Dip-pen Lithography, Chad Mirkin, NWU

Page 56: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.
Page 57: EE143 – Ali JaveySlide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader.

Patterning of individual Xe atoms on Ni, by Eigler (IBM)