New plasma processes for improved dimensional control and...
Transcript of New plasma processes for improved dimensional control and...
New plasma processes for improved dimensional control and LWR for a 28nm gate patterning
Onintza Ros a, Erwine Pargon b, Sebatien Barnola c, Pascal Gouraud a, Marc Fouchier b
a STMicroelectronics, 850 rue Jean Monnet, 38926 Crolles Cedex, France
b LTM, UMR 5129, Université Grenoble Alpes ; CNRS,
c CEA-Leti Minatec, 17 rue des Martyrs, F-38054 Grenoble Cedex.17 rue des Martyrs, 38054 Grenoble Cedex9, France
PESM 2014
Issue description 2
Local pattern distortion is observedafter gate patterning.
.
Planar deprocessing afterfull etch
Planar deprocessing afterfull etch
DesignDesignLocal OVL non-alignment of 11nm!
L1L2
L1>L2
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Gate Etch Process Partitioning3
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The cure step has been identified as a root cause for Gat e Shifting
POLY
Oxide HM
SoC
SiARC
PR
POLY
Oxide HM
SoC
SiARC
PR
POLY
Oxide HM
SoC
SiARC
PR
POLY
Oxide HM
SoC
POLY
Oxide HM
SoC
SoC
POLY POLYOxide
a) b) c) d) e) f) g)
Litho HBr Cure Trim SiARC Open SoC Open HM Open Full Etch
Cure HBrCure HBr
4Pattern shifting
New challenge � Pattern shifting
PR after lithography (50nm left)
PR after HBr cure (45nm left)
SEM Xsection (by LAM research)
Cure step leads to polymerdegradation and leads to an overall
resist flowing.
The resist reflow during HBr cure isresponsible of gate shifting.
LithographyLithography
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Pattern TransferSiARC etch without Cure
Cure step removal allows to maintain respectable Gate sh ifting but increases LWR
A compromise have to be found to control both Gate shif ting and LWR.
We will focus over SiARC etching process and subsequent pattern transfer steps
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With HBr CureWith HBr Cure Without HBr CureWithout HBr Cure
Low LWR~3.5nmHigh Gate Shift~4,5nm
High LWR~11,8nmLow Gate shift ~0,5nm
Pitch 1
Pitch 2
Pictures after SiARC open
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Metrology issue 6
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0
2
4
6
8
10
Pitch 1 Pitch 2 Pitch 3 Pitch 4
Pitch (nm) Pitch
Shift (nm)
Pitc
h sh
ift (
nm)
Pitch 4 remains stable after etch while Pitch 2 is incre ased. Pitch 2 shift is a signature of pattern shifting from initial design.
pitch1
pitch2
pitch3
pitch4
pitch1
pitch2
pitch3
pitch4
a) b) c)
LithographyLithography Full EtchFull EtchDesignDesign
Pitch = CD+Space
Two methods for LWR 7
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CD-SEMCD-SEM Tilted AFMTilted AFM
14µm
45°
� Top view observations
� LWR and LER
� Allows spectral analysis
Xi
LWR = 3 x stdev(CD)LWR = 3 x stdev(CD)
Line
y1
n
iyi
LER = 3 x stdev(y)LER = 3 x stdev(y)
� Only for LER
� Half profile scanning
� Estimation of LER all along the pattern height
Comparison of SiARC plasma etching processes 8
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CD = 44,8nm PR Th = 78nm CD = 44,8nm
PR Th = 78nm
Lithography
CD = 43nmPR Th = 99nm
CD = 43nmPR Th = 99nm
CF4 condition SF6 condition
CD = 47nm PR Th = 40nm
CD = 47nm PR Th = 40nm
CD = 44,8nm PR Th = 78nm
LithographyLithography
CD = 43nmPR Th = 99nm
CF4 conditionCF4 condition SF6 conditionSF6 condition
CD = 47nm PR Th = 40nm
PR SiARC
0.20.40.60.81.01.21.41.61.82.0
1.2
1.8
1.1
ER
(nm
/s)
CF4 SF6
0.6
SiARC ER is higher in CF4 due O depletion by Carbon
C1s O1s Si2p F1s05
10152025303540455055
At %
Ref CF4 SF6
XPS results over SiARC
80 70 60 50 40 30 20
0.3
0.4
0.5
0.6
0.7
0.8
F/C
Angle
CF4 SF6
A R XPS over Photoresist
A C-rich surface layer in CF4 decreasesPR ER and increases LWR.
F-rich surface layer in SF6 increases PR ER and trims PR smoothing the surface.
Surface Bulk
POR CF4 SF60
2
4
6
8
10
12
14
4.8nm
11.8nm
LWR
(nm
)
LWR after SiARC open
3.5nm
Pattern TransferSiARC etch without Cure
New process in SF6 was proved to improve Gate Shifting an d LWR
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PORPOR CF4 conditionCF4 condition SF6 conditionSF6 condition
Pitch 1
Pitch 2
Pictures after SiARC open
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POR CF4 SF60123456789
10
0.5nm1.3nm
Gat
e S
hifti
ng (
nm)
GS in SiARC
6.5nm
Study of Roughness over Photoresist 10
LithographyLithography
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LER PR 4.5nm 15.2nm 2.7nm
LER SiARC - 10.9nm 2.8nm
In CF4 photoresist LWR is degraded during process and partially transfered into SiARC.
In SF6, F rich surface layer will trim the photoresist and smooth it during transfer.
Resulting LER is better in SF6 plasmas
LER ~3.7nm
CF4 conditionCF4 condition
LER ~12.5nm
SF6 conditionSF6 condition
LER ~3.7nm
CD-SEM Measures
0 5 10 15 20 25 30 35 40 450
20
40
60
80
100
120
140
Hei
ght (
nm)
LER (nm)
Reference
SiARC
PR
0 5 10 15 20 25 30 35 40 450
20
40
60
80
100
120
140
Hei
ght (
nm)
LER (nm)
Reference
CF4
SiARC
PR
0 5 10 15 20 25 30 35 40 450
20
40
60
80
100
120
140
Hei
ght (
nm)
LER (nm)
Reference
CF4
SF6
SiARC
PR
POR
CF4 SF6
0
1
2
3
4
5
6
7
8
3.9nm
5.1nm
6.3nm
LWR
(nm
)
LWR in Silicon
Roughness transfer into Silicon 11
1
10
100
1E-3 0.01 0.1
1
10
PS
D (
nm)
Lithography SiARC Silicon
Spectral analysis after pattern transfer
PS
D (
nm)
Wavenumber (Kn, nm -1)
Lithography SiARC Silicon
CF4
SF6
In CF4 all roughness frequencies are increased but during pattern transfer just low frequencies are transferred, lead ing to high LWR.
Spectral analysis of LWR in SF6 does not show rough ness improvements since lithography value is underestima ted. Despite subsequent gate etch steps degrade LWR.
After transfer to Silicon, SF6 plasma is the best o ption for LWR and GS decrease
POR
CF4 SF6
0123456789
10
0.5nm1.3nm
G
ate
Shi
fting
(nm
)
GS in Silicon
6.5nm
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How to improve LWR? 12
LithographyLithography
LWR = 4.9nm
TrimTrim
LWR = 3.7nm
HBr CureHBr Cure
LWR = 4.1nm
GS 1.0nm 6.0nm 1.4nm
LER 4.4nm 3.0nm 2.2nm
Photoresist trim has been identified as a good option to limit LWR without Gate Shifting.
Litho Trim
Measures over Photoresist
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Trim steps to correct LWR 13
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LithographyLithography
LWR = 4.9nm
Trim – SF 6Trim – SF 6
LWR = 4.0nm
LWR measures taken over SiARC show a big roughness improvement with Trim step addition.
Measures after transfer to Silicon prove that Gate shifting will not be degraded during gate etch but LWR can be degrade d due to
subsequent etch steps.
Std Process SF6 Trim-SF60
1
2
3
4
5
6
4.5nm5nm
LWR
(nm
)
LWR measure over Silicon
4nm
Std Process SF6 Trim SF60
2
4
6
8
10
1nm0.5nm
Gat
e S
hift
(nm
)
Gate Shifting measured over Silicon
6.6nm
85%
SF6SF6
LWR = 4.8nm
Measures over SiARC
Conclusion 14
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CF4 conditionCF4 condition SF6 conditionSF6 condition
� Cure steps improve LWR but distort gate patterns.
� Cure step removal requires new plasma processing for gate patterning.
�A new SiARC etching process in SF6 has been compared to the standard process in CF4
�SiARC etching in CF4 leads to C-rich hard surficiallayers that increase LWR
�SiARC etching in SF6 leads to F-rich reactive layers triming photoresist and resulting in lower LWR.
� AFM gate profile analysis shows that LER is lower i n SiARC than in Photoresist.
�Spectral analysis of LWR transfer for these two pla smas shows a degradation of LWR during gate etch processing.
�Addition of Trim steps has been proved to reduce initial LWR
� New process Trim-SF6 allows GateShiftingimprovement of a 85%
Std Process SF6 Trim SF60
2
4
6
8
10
1nm0.5nm
Gat
e S
hift
(nm
)
Gate Shifting measured over Silicon
6.6nm
85%
Thank you for your attention
How to solve it? 16
Gate shifting has an impact on the
electrical performance of the device.
LITHOLITHO CURECURE Trim PR+SiARCTrim PR+SiARC
The cure step is mandatory to ensure minimized gate LWR but it is the
main contributor to pattern shifting.
SiARC woCURE, wo TRIM
SiARC woCURE, wo TRIM
New strategies have to be implemented to fulfill the requirements of the 20nm
technological node in terms of LWR and gate shifting:
1. Optimization of the hard mask opening steps (Si ARC etching and trim, SOC
and TEOS etching)
2. Optimization of the cure step
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Study of Roughness over Photoresist 17
LithographyLithography
CF4 conditionCF4 condition
SF6 conditionSF6 condition
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0102030405060708090
100110120130
0 5 10 15 20 25 30 35 40 45
SF6 CF4 Reference
LER (nm)
Hei
ght (
nm)
SiARC
PR
LER PR 4.5nm 15.2nm 2.7nm
LER SiARC - 10.9nm 2.8nm
In CF4 initial PR roughness is partially transferred into SiARC sidewalls.
In SF6, initial PR roughness is smoothed during SiARC opening.
Resulting LER is better in SF6 plasmas
Comparison of SiARC plasma etchingprocesses
18
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CF4 conditionCF4 condition SF6 conditionSF6 condition
CD = 44,8nm PR Th = 78nm
CD = 47nm PR Th = 40nm
A C-rich hard surface layer is deposed in CF4 plasmas thatprevents photoresist etching and increases LWR.
In SF6 plasmas a F-rich surface layer increases photo resistetch rate and LWR is not impacted.
SiARC ER is higher in CF4 due to a higher C and F conte nt that will increase Oxygen depletion and Si Etch
LithographyLithography
CD = 43nmPR Th = 99nm
2530354045
80 70 60 50 40 30 20
0.30.40.50.60.7
At (
%)
F1s CF4 F1s SF6
AR XPS Measures over photoresist
F/C
Angle
CF4 SF6
SF6 70V CF4 600V0.00.40.81.21.62.0
Etc
h R
ate
(nm
/s)
ERPR ERSiARC
XPS & ER Measures over SiARC
C1s O1s F1s0
10203040
At %
CF4 SF6