EUV mask imaging system based on the scanning reflective ...

20
2013 EUVL Symposium, Toyama Seong-Sue Kim, Donggun Lee, Jongju Park, Eokbong Kim, Chan-Uk Jeon, Hanku Cho, Byeonghwan Jeon, Changhoon choi (Samsung), Chris Anderson, Ryan Myakawa, and Patrick Naulleau (LBNL) October 9, 2013 EUV mask imaging system based on the scanning reflective microscopy

Transcript of EUV mask imaging system based on the scanning reflective ...

Page 1: EUV mask imaging system based on the scanning reflective ...

2013 EUVL Symposium, Toyama

Seong-Sue Kim, Donggun Lee, Jongju Park, Eokbong Kim, Chan-Uk Jeon, Hanku Cho, Byeonghwan Jeon, Changhoon choi (Samsung),

Chris Anderson, Ryan Myakawa, and Patrick Naulleau (LBNL)

October 9, 2013

EUV mask imaging system based on

the scanning reflective microscopy

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Introduction

In fabricating EUV mask, the printability review of the

phase defects is a necessary step and it’s possible only

by an actinic imaging tool.

Previously a timing gap was expected between the HVM

scanner and the commercialized mask imaging tool.

A bridge tool was developed to fill the gap based on

the scanning reflective microscopy using the high-

harmonic EUV source and the zone plate optics.

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Why zone plate?

The full field imaging system with a plasma source and

mirror optics is too expensive and needs a long lead time

for a bridge tool purpose.

The zone plate optics was considered to be an alternative

option.

I1

I2

I3

P1

P2

P3

CCD

Mask

Plasma source

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Why high harmonic EUV source?

In order to use a zone plate for full field imaging an

EUV source with extremely narrow spectral bandwidth is

needed.

The synchrotron beam filtered by a monochrometer

satisfies the spectral bandwidth spec., but for the manu-

facturing purposes a stand-alone source is required.

Among the available stand-alone EUV sources high

harmonic has the most narrow spectral bandwidth.

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Why scanning?

The high harmonic EUV source is both monochromatic

and stand-alone, but the spectral bandwidth is too large

to be used for a full field imaging and the power is too

small to be filtered by a monochrometer.

But in the scanning-type imaging system using on-axis

focused beam, the off-axis aberration can be mitigated

and consequently the spectral bandwidth requirement

can be reduced significantly.

Scanning EUV reflective microscopy

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Scanning EUV reflective microscopy(SERM)

Focused beam spot

(PSF of scanner)

Absorber defectReflectance Map

Mask pattern with

a phase defect

by SERM

Scanning(convolution)

Scanning EUV Reflection Microscopy(SERM)

“US8335038, by Dong-Gun Lee et al” by Scanner

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Outline of the tool development

Mask load-lock chamber

Main chamber & EUV optics

EUV source

IR drive laser

High harmonic EUV source

Zone plate Optics package

The zone plate optics was designed and fabricated by LBNL.

The high harmonic source was developed by Samsung and FST using

COHERENT Ti:Sapphire femtosecond laser( = 800nm, pulse width=

46fs) and the whole system was integrated by Samsung.

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Configuration of the high harmonic source

High Harmonic Generation Ti:Sapphire femtosecond drive laser(=800nm, 46fs)

Seed Laser

Stretcher Amplifier Compressor

in Air In Vacuum

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High harmonic EUV photon generation

High harmonics

Intense fs laser

Gas Cell

atom

electron

Laser

X-ray

• By the highly intense(1014 ~ 1015 W/cm2) IR femtosecond laser electrons are ionized, accelerated coherently, and recombined to generate the EUV light(59-th harmonic).

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Characteristics of the high harmonic source

124 126 128 130 132 134 136 138 140 142 144

0

20

40

60

80

100

Data: InterExtrap1_Book2C25

Model: Gauss

Chi^2 = 1.47946

R^2 = 0.99037

y0 3.88966 ±0.02803

xc 134.9984 ±0.00061

w 0.3972 ±0.00123

A 44.75471 ±0.12222

Sp

ec

tru

m (

arb

. u

nit

s)

Wavelength (Å )

EUV Power = 23.7nW

Bandwidth(/) = 1/280

Divergence = 0.195mrad

Wavefront error = /67

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Zone plate optics

1st order

radiation

A free-standing elliptical zone plate with NA = 0.35(4X) and f=533m

was fabricated.

All diffraction order radiations other than the 1st order are blocked

by the order sorting aperture(OSA) to enhance the contrast.

Zone plate optics with an OSA Elliptical zone plate with 6 CRA Optics package

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Characteristics of the zone plate

The wavefront error of the zone plate: /20

(illuminated by the high harmonic source and measured by the 2D

grating shear Interferometer)

Focused beam spot reconstructed from the wavefront: 84nm(FWHM)

diffraction limited

2D grating shear Interferogram Wavefront error Focused beam spot

84nm

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X/Y interferometer data

Scanning stage system

Hybrid scanning stage is applied to construct an aerial image from

the focused beam spot.

The position of the stage at each image acquisition point is

measured by an interferometer and used in the image reconstruction.

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EUV mask imaging system

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Results: Pattern image

25nm HP(1X) L/S pattern 30nm HP(1X) C/H pattern

The major sources of the LWR are the low source power(shot noise),

the mask LWR, and presumably mask surface roughness.

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Defect size (SEVD)

58nm 47nm 37nm 26nm 21nm

Defect image

Results: Phase defect images

Defocus -1.3m -0.7m 0m 0.7m 1.3m

Defect image

Phase defect imaging sensitivity(programmed pit defect)

Focus behavior of the phase defect(28nm-SEVD native bump defect)

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Results: Phase defect in a patterned mask

Wafer SEM Image Mask SEM Image Mask actinic Image

Phase defect printability on a wafer is reproduced

successfully in the actinic image by this tool.

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Application

This tool can be used for

Review of phase defect printability for both patterned mask and

ML blank

CD verification after repair of both pattern and phase defects

Studies on the surface roughness effect etc…

Once commercial EUV mask imaging tool is installed for

HVM, this tool can be upgraded to be a high-NA system,

which is possible by simply changing the zone plate and

the bending mirror.

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Summary

Using the concept of the scanning EUV reflective microscopy an

EUV mask aerial imaging system was developed.

An aberration-free(< /67) high harmonic EUV source was

developed using a femtosecond IR laser and a gas cell.

A free-standing elliptic zone plate optics was developed and a

diffraction-free beam spot was obtained.

Reviewing capability of the phase defects less than SEVD-21nm

were confirmed and the defect printability on the wafer pattern is

reproduced successfully.

This tool will be used for reviewing phase defect printability and

upgraded for high-NA EUV studies.

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Acknowledgement

I’d like to thank Prof. David Attwood who encouraged me

to apply the high harmonic EUV source in developing EUV

mask imaging system.