sematech defect printability studies - extreme ultraviolet

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Accelerating the next technology revolution Copyright ©2012 SEMATECH, Inc. SEMATECH, and the SEMATECH logo are registered servicemarks of SEMATECH, Inc. International SEMATECH Manufacturing Initiative, ISMI, Advanced Materials Research Center and AMRC are servicemarks of SEMATECH, Inc. All other servicemarks and trademarks are the property of their respective owners. SEMATECH Defect Printability Studies Il Yong Jang 1 , Jenah Harris-Jones 1 , Ranganath Teki 1 , Vibhu Jindal 1 , Frank Goodwin 1 Masaki Satake 2 , Ying Li 2 , Danping Peng 2 Sungmin Huh 3 , Seong-Sue Kim 3 1 SEMATECH 2 Luminescent Technologies 3 Samsung Electrinics

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Accelerating the next technology revolution

Copyright ©2012

SEMATECH, Inc. SEMATECH, and the SEMATECH logo are registered servicemarks of SEMATECH, Inc. International SEMATECH Manufacturing Initiative, ISMI, Advanced Materials Research Center

and AMRC are servicemarks of SEMATECH, Inc. All other servicemarks and trademarks are the property of their respective owners.

SEMATECH Defect Printability Studies

Il Yong Jang 1, Jenah Harris-Jones 1, Ranganath Teki 1,

Vibhu Jindal 1, Frank Goodwin 1

Masaki Satake 2, Ying Li 2, Danping Peng 2

Sungmin Huh3, Seong-Sue Kim3

1 SEMATECH 2 Luminescent Technologies 3 Samsung Electrinics

Outline

• Introduction

• Experimental procedure and conditions

• Experimental results – Multilayer Geometry

– CD error comparison

• Summary

2 2013 SPIE Advanced Lithography

Major show stopper

3

Since last 5 years, mask yield and defect inspection infra. has been the major show stopper.

Defect levels of EUV mask blanks require further improvement

2013 SPIE Advanced Lithography

Ref.) International EUVL Symposium Program Steering Committee

Recent report

22nm HP node is likely to be the real gateway for EUVL.

Defects of 23nm SEVD start to be printed at the 22nm HP node, however it is not easy to predict the real printability just with SEVD.

It is very important to know the printability of native defects having various dimension to understand phase defect printability.

Simulation work is very important for studying the defect printability.

SEMATECH had begun to study the printability of native defect using simulation and actinic exposure.

4 2013 SPIE Advanced Lithography

Experimental procedure

5

① Substrate Insp.& marking

② AFM analysis

⑥Absorber patterning

2013 SPIE Advanced Lithography

⑦ Wafer Exposure

③ ML deposition ④ AFM analysis

⑤ Absorber deposition

⑧ Analysis

*Images courtesy of www.tel.com, www.veeco.com

Absorber deposition at SEMATECH

6

Absorber deposition with SEMATECH’s IBD chamber

– Optical properties (n=0.9472, k=0.0304, measured@ CXRO, LBNL)

– Thickness : 59nm (3nm ARC + 56nm TaN)

Roughness, stress, chemical durability and defectivity of the absorber

film need to be verified as well.

n&k [email protected] TEM image

2013 SPIE Advanced Lithography

Absorber patterning

7

Absorber patterning at Samsung mask Shop

– Patterning with high-end EBW tool and EUV mask etcher

– Modified etch chemistry due to 1.5 times slower ER than commercial absorber

– Acquired excellent pattern quality and critical dimension SEM

2.8nm LWR

88degs

MTT:1.9nm

88nm 108nm 128nm

AFM

2013 SPIE Advanced Lithography

8

Simulation

– Defect : 24/30/36/42/48nm on substrate

– Absorber pattern : 27nm with 88degs of SWA

2013 SPIE Advanced Lithography

Exposure ML geometry CD Analysis

CD1

(CD1–CD2)x100 CD error =

Absorber Simulation

D P S

RCWA

Conventional Ill.

NA:0.25, σ:0.8

Conformal

Smoothed

Reconstructed

Position: X=0

9

ML Geometry

2013 SPIE Advanced Lithography

ML growth is dependent on the process and

configuration of H/W of ML deposition.

Defect shape changes the ML geometry

No universal ML growth model could give

versatility in defect printability simulation

It is very important to select the optimum ML

geometry to increase simulation accuracy

Used the AFM data measured from substrate

and surface of ML to make a new ML geometry.

10

Smoothed Geometry (for 35nm defect)

2013 SPIE Advanced Lithography

ML pairs ↑ → Defect dimension ↑

Good for any type of defect ?

35nm

Smoothed ML Geometry

11

Conformal Geometry

2013 SPIE Advanced Lithography

Which model should we use for simulation ?

Need to find out the optimum ML geometry for each defect

75nm

Conformal ML Geometry

12

Normalized Dimension

2013 SPIE Advanced Lithography

Surface

β

Substrate

α

Normalized dimension : Surf. dimension β / Sub. dimension α

Measured and got the all normalized dimension from 24nm,

30nm, 36nm, 42nm and 48nm defects

13

Fitting ML geometry

2013 SPIE Advanced Lithography

14

Reconstructed ML geometry

2013 SPIE Advanced Lithography

Defined each defect’s

dimension based on the

fitting curve.

Created “Reconstructed

ML geometry”

Compared the CD error

simulated by three types of

ML geometry.

(Conformal vs Smoothed

vs Reconstructed ML)

15

CD error with defect dimension

2013 SPIE Advanced Lithography

Simul. image

Wafer image

Position : X=0

NA=0.25, sigma=0.8

0 100 200 300 400 500 6000

50

100

150

200

250

300

350

X Mask Distance (nm)

Z M

ask H

eig

ht

(nm

)

EUV Mask Geometry Cutline Through Center of DefectBump

Illumination Defocus

Focus = 0nm

16

CD error with defect dimension

2013 SPIE Advanced Lithography

Simul. image

Wafer image

Position : X=0

NA=0.25, sigma=0.8

Pit

Illumination Defocus

Focus = 0nm

0 100 200 300 400 500 6000

50

100

150

200

250

300

350

X Mask Distance (nm)

Z M

ask H

eig

ht

(nm

)

EUV Mask Geometry Cutline Through Center of Defect

CD error with defocus

2013 SPIE Advanced Lithography

Simul. image

Wafer image

Position : X=0

NA=0.25, sigma=0.8

0 100 200 300 400 500 6000

50

100

150

200

250

300

350

X Mask Distance (nm)

Z M

ask H

eig

ht

(nm

)

EUV Mask Geometry Cutline Through Center of DefectBump

Illumination Defect dim.

24nm

CD error with defocus

2013 SPIE Advanced Lithography

Simul. image

Wafer image

Position : X=0

NA=0.25, sigma=0.8

Pit

Illumination Defect dim.

24nm

0 100 200 300 400 500 6000

50

100

150

200

250

300

350

X Mask Distance (nm)

Z M

ask H

eig

ht

(nm

)

EUV Mask Geometry Cutline Through Center of Defect

DPS performance

2013 SPIE Advanced Lithography

CD error from DPS, RCWA and wafer are within 2% range

DPS S/W developed by Luminescent Technologies shows good

simulation accuracy while taking less calculation time than that of

RCWA simulation.

Summary

2013 SPIE Advanced Lithography

Analyzed defect dimensions measured on the

substrate and the ML surface and found correlation

between defect dimension and ML geometry

The reconstructed ML geometry predicts the CD error

better than conventional conformal ML geometry.

24nm bump and pit defects on substrate occurs 7.6%

and 17% of wafer CD error showing that the Teron can

detect the most of defects which could be printed on

wafer for 27nmHP node L&S pattern.

DPS shows good accuracy and faster calculation time

than RCWA simulator.

Acknowledgements

2013 SPIE Advanced Lithography

. Dr. Tsukasa Abe and Naoya Hayashi, DNP for discussing mask manufacturing . Dr. Eric Gullikson from LBNL for providing metrology to measure the optical properties of SEMATECH’s absorber . Gregg Inderhees from KLA-Tencor for providing blank inspection . Dr. Tae-Geun Kim and Dr. Sang-Hyun Kim from Samsung for supporting the defect analysis for this study.