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Removal of Nano Particles on the Hard Mask Wafer Backside using Brush Cleaning Hyun-Tae Kim a *, Yeo-Ho Kim a , Nagendra Prasad Yerriboina b , Tae-Gon Kim c , KyuHwang Won d and Jin-Goo Park a, b, a Department of Bio-Nano Technology, b Materials Science and Chemical Engineering, c Smart Convergence Engineering, Hanyang University, Ansan, 15588, Korea d Samsung Electronics, Hwaseong, 18448, Korea (E-mail: *[email protected], [email protected]) As pattern nodes continue to scale down and become more complex, lithography technologies have required many solutions to create extremely small patterns. For a certain process such as, high aspect ratio trench patterning, the hard mask has been chosen for a high etch resistance and selectivity. Amorphous carbon and siloxane based materials were commonly used as hard mask materials which can be prepared by CVD or spin-on processes. During deposition process, the physical contacts of the wafer backside to pedestals such as chuck or lift pins are necessary to support and transfer the wafer. The electrostatic chuck (ESC) is widely utilized in deposition process because of its advantages in nonedge exclusion, wafer temperature control and particle defect reduction. However, the pin contact is the protrusion part on ESC that directly contacts wafer backside can make exfoliation of pre-existed backside film which results in the generation of particle defects. These backside particles may travel to the front side. These backside particles vary in size and materials because of backside particles which were crushed by the chucking pressure. It also greatly affects ESC chucking performance, adhesion uniformity and flatness stability. Especially, these backside particles were exposed to the thermal energy during the CVD process. It induces deformation of the particles, leading to an increase in adhesion to the substrate. This aging effect results in the reduction of particle removal efficiency. To solve these particle issues, an effective cleaning process is necessary to remove the contaminated particles on the backside. The adhesion and removal of these particles were first analyzed on backside surfaces. PVA brush cleaning, generally used for post CMP cleaning process, was applied to effectively remove the particles by physical cleaning in this study. Abstract Introduction Silicon wafer backside Electrostatic chuck Contact point Electrostatic chucking involves contact in many point between the ECS and backside of wafer Delamination of backside film (SiO 2 ) SEM images Crushed SiO 2 particles Research Objective Backside Particle Backside particles which were crushed by the chucking pressure - particle size : nm - 10 μm - composition : SiO 2 - process temp : - 550°C, hard mask coating process Brush Cleaning To remove these particles, Brush cleaning was applied with DIW Pin-type brush PVA brush Top view Parameters - Only DIW use - Pressure - Spin speed of brush - Spin speed of wafer How much force do we need to remove particles? Quantification of Cleaning force Quantification of Adhesion force Process was optimized by experiential approaching Optimization Backside cleaning condition Experimental Pre-treatment of silicon wafer 1.SC1 (NH 4 OH:H 2 O 2 :DIW=1:2:50) 10min. (dipping) particle removal 2.Rinse 5min. + Dry N 2 blowing 3.DHF (1:100) 3min. (dipping) native oxide removal 4.Rinse 5min. + Dry N 2 blowing Deposition of PSL particle on silicon surface (-3) Colloidal PSL solution (100-500ppm)+ DIW 1min. (dipping) Back side defect Lateral force analysis Brush cleaning Contamination particle Si wafer Particle counting (AFM / OM) Brush cleaning Particle counting (AFM / OM) Lab scale brush cleaning (Pin type) Parameters - z axis (pressure) ±30mm - brush rotation speed (500rpm) - wafer rotation speed (1000rpm) - DIW flow - brush type Quantification of adhesion force using AFM C-D signal (a+c)-(b+d) Torsional spring constant (k t ) = nN/rad Angle conversion factor () Force conversion factor (κ) Lateral force(F L ) Results SPCC 2019 | Portland, Oregon, USA | April 2-3, 2019 Lateral force (1.0-3.0) Back side particle (by ESC chucking) Standard particle (PSL particle) 10 20 30 40 50 60 70 80 90 100 110 0 5 10 15 20 25 30 35 40 Lateral force (nN) 10 20 30 40 50 60 70 80 90 100 110 0 5 10 15 20 25 30 35 40 Lateral force (20, 50, 100nm) Particle size (nm) Particle size (nm) 2.81nN 6.44nN 13.19nN 2.11nN 8.13nN 26.96nN 1day aging 7day aging A smaller than 100nm size of particle was sensitive to aging time Back side particle shows higher lateral force than standard particle Theoretical cal. 0 500 1000 1500 2000 2500 3000 -200 0 200 400 600 800 1000 1200 1400 1600 1800 2000 Lateral force(nN) Theorical calcuation Experimetal data Particle size (nm) Lateral force (nN) Experimental data <1000nm particle : JKR model >2000nm particle : DMT model Lateral force (0.1-3.0) Measuring of lateral force using AFM Brush cleaning optimization - with brush usage 30 60 90 120 150 180 210 60 65 70 75 80 85 90 95 100 105 PRE (%) Time of brush usage (sec.) Particle removal efficiency (%) Gap-distance : 0 Wafer rotation speed: 100 rpm Brush rotation speed: 105 rpm 600nm SiO 2 100 120 140 160 180 200 60 65 70 75 80 85 90 95 100 105 PRE (%) Brush rotation speed (RPM) - with brush rotation speed 600nm SiO 2 Gap-distance : 0 Wafer rotation speed: 100 rpm time: 20s Optimized condition : >90% removal efficiency (over 600nm SiO 2 particle) JKR model DMT model http://www.ntmdt.com/spm-basics/view/adhesion-forces 20 30 40 50 60 0 10 20 30 40 50 60 70 80 90 100 PRE(%) Process time (sec.) Gap-distance : 0 Wafer rotation speed: 100 rpm Brush rotation speed: 120 rpm - with process time 100nm SiO 2 Particle removal evaluation Before cleaning (O.M) After cleaning 1Kx 1Kx 20μm 20μm Particle removal efficiency (%) Aging effect 0 100 200 300 400 500 600 700 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 Temperature () Time (hr.) 71.6% 90.6% Aging condition : 600°C heating (6hr.) 100nm SiO 2 removal efficiency : 90.6% (60sec.) After aging process, removal efficiency is a 71.6% Conclusion Acknowledgment This research was supported by a Semiconductor Industry Collaborative Project between Hanyang University and Samsung Electronics Co. Ltd. To quantify the adhesion force of back side particle attached to the substrate, the lateral force was measured using the AFM Because of high temperature aging, back side particles (25.96nN) are harder to remove compared to the standard particle(13.19nN) Pin-type brush shows high removal efficiency of 100nm SiO 2 particle over 90%. However, after aging process, removal efficiency reduced to 19% decrease. Hence chemical forces are required to remove heat treated particle on backside Surface force acts only within the contact area Surface force acts only outside the contact area Attracting molecules Repulsing molecules Attracting molecules Repulsing molecules

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Page 1: Hyun-Tae Kim , Yeo-Ho Kim , Nagendra Prasad Yerriboina ... · 4/3/2019  · Removal of Nano Particles on the Hard Mask Wafer Backside using Brush Cleaning Hyun-Tae Kima*, Yeo-Ho Kima,

Removal of Nano Particles on the Hard Mask Wafer Backside using Brush Cleaning

Hyun-Tae Kima*, Yeo-Ho Kima, Nagendra Prasad Yerriboinab, Tae-Gon Kimc, KyuHwang Wond and Jin-Goo Parka, b, †

a Department of Bio-Nano Technology, b Materials Science and Chemical Engineering, c Smart Convergence Engineering, Hanyang University, Ansan, 15588, Korea

d Samsung Electronics, Hwaseong, 18448, Korea

(E-mail: *[email protected], †[email protected])

As pattern nodes continue to scale down and become more complex, lithography technologies have required many solutions to create extremely small patterns. For a certain process such as, high aspect ratio trench patterning, the hard mask has been chosen for a high etch resistance and selectivity.

Amorphous carbon and siloxane based materials were commonly used as hard mask materials which can be prepared by CVD or spin-on processes. During deposition process, the physical contacts of the wafer backside to pedestals such as chuck or lift pins are necessary to support and transfer the wafer.

The electrostatic chuck (ESC) is widely utilized in deposition process because of its advantages in nonedge exclusion, wafer temperature control and particle defect reduction. However, the pin contact is the protrusion part on ESC that directly contacts wafer backside can make exfoliation of pre-existed

backside film which results in the generation of particle defects. These backside particles may travel to the front side. These backside particles vary in size and materials because of backside particles which were crushed by the chucking pressure. It also greatly affects ESC chucking performance, adhesion

uniformity and flatness stability. Especially, these backside particles were exposed to the thermal energy during the CVD process. It induces deformation of the particles, leading to an increase in adhesion to the substrate. This aging effect results in the reduction of particle removal efficiency. To solve these

particle issues, an effective cleaning process is necessary to remove the contaminated particles on the backside. The adhesion and removal of these particles were first analyzed on backside surfaces. PVA brush cleaning, generally used for post CMP cleaning process, was applied to effectively remove the

particles by physical cleaning in this study.

Abstract

Introduction

Silicon wafer backside

Electrostatic chuck

Contact point

Electrostatic chucking involves contact in

many point between the ECS and backside

of wafer

Delamination of backside film (SiO2)

SEM images

Crushed SiO2 particles

Research Objective

Backside

Particle

Backside particles which were crushed by the chucking pressure

- particle size : nm - 10 µm

- composition : SiO2

- process temp : - 550°C, hard mask coating process

Brush

Cleaning

To remove these particles, Brush cleaning was applied with DIW

Pin-type brush

PVA

brush

Top view

Parameters

- Only DIW use

- Pressure

- Spin speed of brush

- Spin speed of wafer

How much force do we need to remove particles?

Quantification of

Cleaning force

Quantification of

Adhesion force

Process was optimized by

experiential approaching

Optimization

Backside cleaning

condition

Experimental

• Pre-treatment of silicon wafer

1.SC1 (NH4OH:H2O2:DIW=1:2:50) 10min. (dipping) – particle removal

2.Rinse 5min. + Dry N2 blowing

3.DHF (1:100) 3min. (dipping) – native oxide removal

4.Rinse 5min. + Dry N2 blowing

•Deposition of PSL particle on silicon surface (-3㎛)

Colloidal PSL solution (100-500ppm)+ DIW 1min. (dipping)

Back side defect Lateral force analysis

Brush cleaning

① Contamination

particle

Si wafer

② Particle counting

(AFM / OM)③ Brush cleaning ④ Particle counting

(AFM / OM)

• Lab scale brush cleaning (Pin type)

Parameters

- z axis (pressure) ±30mm

- brush rotation speed (500rpm)

- wafer rotation speed (1000rpm)

- DIW flow

- brush type

Quantification of adhesion force using AFM

• C-D signal (a+c)-(b+d)

• Torsional spring constant (kt) = nN/rad

• Angle conversion factor (𝜂)

• Force conversion factor (κ)

• Lateral force(FL)

Results

SPCC 2019 | Portland, Oregon, USA | April 2-3, 2019

• Lateral force (1.0-3.0㎛)

Back side particle

(by ESC chucking)

Standard particle

(PSL particle)

10 20 30 40 50 60 70 80 90 100 1100

5

10

15

20

25

30

35

40

Late

ral fo

rce (

nN

)

Particle size (nm)

10 20 30 40 50 60 70 80 90 100 110

0

5

10

15

20

25

30

35

40

Particle size(nm)

• Lateral force (20, 50, 100nm)

Particle size (nm) Particle size (nm)

2.81nN

6.44nN

13.19nN

2.11nN

8.13nN

26.96nN1day aging 7day aging

A smaller than 100nm size of particle was sensitive to aging time

Back side particle shows higher lateral force than standard particle

Theoretical cal.

0 500 1000 1500 2000 2500 3000

-200

0

200

400

600

800

1000

1200

1400

1600

1800

2000

La

tera

l fo

rce

(nN

)

Particle size (nm)

Theorical calcuation

Experimetal data

Particle size (nm)

Late

ral fo

rce (

nN

)

Experimental data

<1000nm particle : JKR model

>2000nm particle : DMT model

• Lateral force (0.1-3.0㎛)

Measuring of lateral force

using AFM

• Brush cleaning optimization

- with brush usage

30 60 90 120 150 180 21060

65

70

75

80

85

90

95

100

105

PR

E (

%)

Cleaning time (s)Time of brush usage (sec.)

Part

icle

rem

oval effic

iency (

%)

Gap-distance : 0

Wafer rotation speed: 100 rpm

Brush rotation speed: 105 rpm

600nm SiO2

100 120 140 160 180 20060

65

70

75

80

85

90

95

100

105

PR

E (

%)

Brush rotation speed (rpm)Brush rotation speed (RPM)

- with brush rotation speed

600nm SiO2

Gap-distance : 0

Wafer rotation speed: 100 rpm

time: 20s

Optimized condition : >90% removal efficiency (over 600nm SiO2 particle)

JKR model DMT model

http://www.ntmdt.com/spm-basics/view/adhesion-forces

20 30 40 50 600

10

20

30

40

50

60

70

80

90

100

PR

E(%

)

Process time (sec.)Process time (sec.)

Gap-distance : 0

Wafer rotation speed: 100 rpm

Brush rotation speed: 120 rpm

- with process time100nm SiO2

• Particle removal evaluation

Before cleaning (O.M)

After cleaning

1Kx

1Kx20μm

20μm

Part

icle

rem

oval effic

iency (

%)

• Aging effect

0

100

200

300

400

500

600

700

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19

Tem

pera

ture

(℃

)

Time (hr.)

71.6%90.6%Aging condition : 600°C heating (6hr.)

100nm SiO2 removal efficiency : 90.6% (60sec.)

After aging process, removal efficiency is a 71.6%

Conclusion Acknowledgment

This research was supported by a Semiconductor Industry Collaborative Project

between Hanyang University and Samsung Electronics Co. Ltd.

• To quantify the adhesion force of back side particle attached to the substrate, the lateral force was measured using the AFM

• Because of high temperature aging, back side particles (25.96nN) are harder to remove compared to the standard particle(13.19nN)

• Pin-type brush shows high removal efficiency of 100nm SiO2 particle over 90%. However, after aging process, removal efficiency reduced to

19% decrease. Hence chemical forces are required to remove heat treated particle on backside

Surface force

acts only within

the contact area

Surface force

acts only outside

the contact area

Attracting molecules

Repulsing molecules

Attracting molecules

Repulsing molecules