+ All Categories
Home > Documents > Lecture 17 - litho opticsweb.eecs.umich.edu/~peicheng/teaching/EECS598_06_Winter/Lecture … ·...

Lecture 17 - litho opticsweb.eecs.umich.edu/~peicheng/teaching/EECS598_06_Winter/Lecture … ·...

Date post: 20-Sep-2018
Category:
Upload: buiminh
View: 217 times
Download: 0 times
Share this document with a friend
23
Lecture 17 – Optical Lithography 2 - Optics EECS 598-002 Winter 2006 Nanophotonics and Nano-scale Fabrication P.C.Ku
Transcript

Lecture 17 –Optical Lithography 2 - Optics

EECS 598-002 Winter 2006Nanophotonics and Nano-scale Fabrication

P.C.Ku

2EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Fundamentals of lithographic optics

DiffractionPartial coherenceDepth of focusReflection and interferencePolarization dependence

3EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Image formation

Need to have at least the 0-th and the 1st diffraction orders being collected to recover the pitch information.

+1

-1

0

0

-1

Oblique incidence can improvethe minimum pitch but resultin a less image contrast.

Resolution limit (min pitch)= 2

2NA NAλ λ

× =

4EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Why not just use oblique incidence?

Because patterns on the mask are often random. Oblique illumination at a certain angle is only optimized for a specific structure (e.g. a line/space pattern at a certain pitch.)

5EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Incoherent illumination

0

-1

1

0

+1

-1

0

Some images may form.Some may not.

Resolution limit = 2NAλ

6EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Partial coherence

Illuminator Aperture

Entrance Pupil

Mask

Condenser

ab

optics)ion NA(projectator)NA(illumin

=≡abσ

7EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Depth of focus (DoF) for normal incidence

DoF

The optical path difference between the0-th order and the order coming from theedge of the lens needs to be smaller thanλ/4.

θ

( )

( )

2

2

DoF DoFcos4

NADoF

4 2

DoF2 NA

λ θ

λ

λ

= −

⇒ =

⇒ =

8EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

DoF for oblique incidence

0

-1

θ

( ) ( )2 2sin cos sin cos

2 cos 22cos sin

i x z i x z

y

i z

E Ae Ae

Ae x

π πθ θ θ θλ λ

π θλ π θ

λ

+ − += +

⎛ ⎞= ⎜ ⎟⎝ ⎠

z

x

If equal amplitudes:

independent of z!DoF = ∞

9EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Substrate reflection

resist

substrate

Reflection from the resist/substrate interfacecreate interference pattern perpendicularto the interface.

substrate

After exposure

1. Dose varies with depth.2. Dose varies with resist thickness.3. Focus must be maintained for at leasttwice the thickness of the resist thickness.

10EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Nonplanar substrates

The resist is spun on a non-flat substrate.

By R. R. Dammel et al., “Antireflection coating”

11EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Swing curve vs wavelength

Typical substrates exhibit a larger reflectivity at a shorter wavelength.

By R. R. Dammel et al., “Antireflection coating”

12EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Minimize the reflectivity problems

Very minimum we can do:Post exposure bake (PEB) to induce the diffusion of the photo generated compound to smooth out the interference profile.

Antireflection layer (AR):Can be inorganic or organic materials.Can be on top of or underneath the resist.Typically good to absorb the light before it reaches the substrate

Examples:Si(ON) (hardmask) – a good mask for metal etchBARC (bottom AR coating) Can be spun on just like resist itselfTARC (top AR coating)

13EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

BARC process (for non-developable organic BARC)

Spin coatBARC

Spin coatresist

14EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Advantages of organic BARC vs hardmask

Can be spin-coated. Can planarize the surface topologySome BARC’s can be developed at the same time as the resist. Save one etching step.BARC can be stripped at the same time with the resist while the hardmask can not be removed after it’s been deposited. This will improve the line yield.

15EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Polarization dependence

In general, the reflectivity of TE and TM components are different from each other.

As the feature size on the mask becomes comparable to the wavelength, a fully vectorial diffraction theory needs to be taken into account to accurately simulate the aerial image.

Mask

17EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Mask (reticle) design

pellicle

glass

chrome

Clear field Dark field

E-beam litho is typicallyused for mask making.

18EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Dose sensitivity

Comparison of clear and dark fields

1/3 intensitypasses throughdark field mask

Reaching reticle 20 mJ

Reaching wafer 15 mJ

60 mJ

15 mJ

24 mJ reach mask

18 mJ reach wfr

64 mJ reach mask

16 mJ reach wfr

Clear field Dark field

same variation of laser intensity

20% dose error for clear field6.7% dose error for dark field

19EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Mask Error Enhancement Factor

Line or Space on Mask

Line

or S

pace

on

Waf

erCD error on the mask translates to the CD error on the wafer.

MEEF = 1 when isolated features on the mask >> wavelength

When isolated features on the mask ~ wavelength Mask width determines the image intensity determines the CD of the resist

CDReduction MEEF

CDwafer

mask

∆= ×

For isolated features

20EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

MEEF for lines/spaces

0

0.2

0.4

0.6

0.8

1

1.2

0 0.2 0.4 0.6 0.8 1 1.2

Line/Pitch on Mask

Line

/Pitc

h on

Waf

er Non-linearity is generally worse than for isolated lines or spaces.

Light source

22EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Overview

Exposure wavelengthG-line (436 nm)I-line (365 nm)KrF (248 nm)ArF (193 nm)F2 (157 nm)EUV (13.4 nm)X-ray (~ 1 nm)

Minimum feature size:~ 500 nm~ 350 nm~ 120 nm~ 70 nm ?

???

DUV

23EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku

Excimer lasers and dose control

Excimer laser is a pulsed laserRepetition rate ~ 1 kHz

Excimer laserND filter

Moving waferScanning speed< 100 mm/sec

Adjust ND filter OD setting and the scanning speed to control the exposuredose (mJ/cm2)


Recommended