Potential and Lim its of Texture Measurem ent Techniques for I nlaid Copper Process Optim ization
Holm Geisler, Inka Zienert, Hartmut Prinz, Moritz-Andreas Meyer, Ehrenfried Zschech AMD Saxony LLC & Co. KG, Dresden, Germany
Potential and Lim its of Texture Measurem ent Techniques for I nlaid - - PowerPoint PPT Presentation
Potential and Lim its of Texture Measurem ent Techniques for I nlaid Copper Process Optim ization Holm Geisler, Inka Zienert, Hartmut Prinz, Moritz-Andreas Meyer, Ehrenfried Zschech AMD Saxony LLC & Co. KG, Dresden, Germany Outline
Holm Geisler, Inka Zienert, Hartmut Prinz, Moritz-Andreas Meyer, Ehrenfried Zschech AMD Saxony LLC & Co. KG, Dresden, Germany
03/ 26/ 03 ICCM, March 24 - 28, 2003, Austin, Texas Holm Geisler 2
Outline
– X-ray micro-diffraction – OIM: EBSD & ACT
– Microstructure monitoring – ECD-filled inlaid structures with new ILDs, capping layers and barrier layers – Texture and stress – Orientation stereology, grain size, grain boundary distribution – Texture in ECD-filled via chains – Texture of barrier and seed layers before ECD filling
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Microstructure characterization of inlaid copper interconnects
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+ sidewalls + twins + engaged
Texture Al vs. inlaid Cu Al Al I nlaid Cu I nlaid Cu { 111} { 111} { 111} { 511} twins
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What is different ?
Inlaid Copper Interconnects Aluminum Interconnects Twins + Sidewall Bamboo + Columnar ???? Optimum EM Behaviour Large Anisotropy Small Anisotropy Electroplating Vapour Deposition Cu CMP Metal etch .... ....
E〈111〉 = 1 9 1 GPa E〈100〉 = 6 6 .7 GPa
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Texture, EM & defects Prevent grain boundaries along the trench direction! = Fast diffusion pathways Electromigration:
Sidewall-oriented grains? High-angle grain boundary?
Top view
void v > v
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Microstructure Characterization: General Concept
). , , ( / ) (
2 1
ϕ ϕ Φ = = f dg V dV g f
g
x1 x2 x3 g(x) x
Function: strain lattice defects, ns
phase ) ( ) ( ) ( ) ( = x D x g x i x G
g
dg
KB KA
H.J. Bunge (1999, 2001)
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Quantification: ODF approximation
[ K. Helming, http: / / www.texture.de/ ]
). , , ( / ) (
2 1
ϕ ϕ Φ = = f dg V dV g f
g
Euler angles ϕ1, Φ, ϕ2
KA: sample coordinates KB: cryst. coord. system
(111)+ (200)+ (220) e.g., ADC
χ
φ
( hkl) pole figure, P( χ,φ) OD, f( φ1, Φ, φ2)
dg f P hkl
Φ =
π
φ φ π φ χ
2 2 1 ) (
) , , ( 2 1 ) , (
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Evaluation of pole figures
– Harmonic Methods: computation in Fourier space – Discrete (Direct) Methods: computation in orientation space:
– based on ADC (Arbitrarily Defined Cells) – direct method, good for sharp textures – quantification of
– uncertainty in determination of random texture component (background, low signal-to-noise ratio)
(1991) U.F. Kocks et al. (1998)
] ) , , ( ) , [( 1 ) , (
2 1 1 i N i h
f N P φ φ φ χ φ χ Φ ⇐ = ∑
=
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Texture measurement techniques
– EBSD: Electron Backscatter Diffraction – ACT: Automated Crystallography for the TEM
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Texture measurement techniques for inlaid Cu interconnects: Overview ACT µ-XRD EBSD
ACT EBSD ?
nano- cryst.
EBSD µ-XRD ?
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Techniques: comparison
Classical Texture, ODF: f(g) = f(ϕ1, Φ, ϕ2) Phase: i Strain (Stress): Ds
Orientation Stereology: g(x) Grain Size Grain-boundary distribution
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Probed volume
X-rays: Penetration depth > > µm
Met n Met n+ 1
Vian ILD
Compared with EBSD: ≤ tens of nm
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Statistics
– Beam diameter d = 100µm A = π r2 = 7854 µm 2 – Test pattern: parallel trenches, w = 180nm, p = 360nm – Assumption: mean grain diameter = w
(one grain extends over the whole line width and depth)
– n = (L / w) / (2Lw) = 1 / (2w2) L: length of the line – n ∼ 15 grains / µm 2 – N = n A ∼ 118000 grains
– A = 3µm x 10µm = 30 µm 2 – N = n A ∼ 450 grains
X-ray EBSD { 1 1 1 } pole figures
RD TD
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X-ray
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Texture and stress measurements at inlaid test structures using X-ray micro-diffraction
sensitivity (80% quantum efficiency)
intensity
from 120 x 120 µm 2 up to 10 x 10 mm 2 Bruker AXS D8 micro-diffraction tool Huber goniometer with ¼ Eulerian cradle, PolyCap and area detector (GADDS) Video + laser for accurate height adjustment
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X-ray micro-diffraction on arrays of inlaid Cu lines
Copper lines Barrier Silicon Si(F)O, SiCOH SiN, SiCN
Narrow inlaid Cu lines Wide inlaid Cu lines
Inlaid structure > 120µm X-ray beam 80µm Ø
Metal 1
Video camera + laser beam alignment
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X-ray µ-diffraction on arrays of Cu lines and line segments geometry effects
Narrow Cu lines and line segments – width = 180nm
4.3µm x 4.3µm 10µm x 10µm 10µm x 10µm 10µm x 10µm 10µm x 10µm
.......
{ 111} { 111} { 111} { 111}
X-ray beam ~ 8 0 - 1 0 0 µm Ø
good good poor bad
I t should w ork on dense via arrays
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X-ray microstructure monitoring: Arrays of inlaid copper lines { 111} - narrow copper lines (180nm) { 111} - wide copper lines (1.8µm) Week
negligible
record TD RD RD TD
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Texture components in Cu lines
Si
SiO2
Cu
( 1 1 1 ) lattice planes Sym m etry equivalent, 7 0 .5 ° Sym m etry equivalent, 7 0 .5 °
Blanked
{111} {112} {110} {111} (-110) {111} (0-11) (-1-12)
Sketch of (111) Pole Figure
Trenches
Engaged ( 1 1 1 ) Fiber Texture
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Texture Components in copper lines
{111} {111} {111} {111} (-211) (-110) {111} (0-11) (-1-12) {111} {111} (-110) (-1-12) (-211) (0-11)
Sketch of { 1 1 1 } pole figure
Tilted sidewalls
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Texture Components in copper lines
{111} {111}
Superposition sidewall + fiber
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1st generation twins
{ 1 1 1 } pole figure { 111} center peak
Additional circles @ 38.9°, 56.2° and 70.5° in { 111} pole figure
{ 5 1 1 } : 1 st generation tw ins
{ 511} { 111} Twin
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2nd generation twins
Additional circles @ 22.19°, 56.25° and 65.95° in { 111} pole figure
{ 111} centre peak { 1 1 1 } pole figure
{ 5 7 1 3 } : 2 nd generation tw ins
{ 5 7 13} { 111} Twin
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Effect of different ILDs and etch stop layers on texture in copper lines
SiCOH + SiCN Si(F)O + SiN
{ 111} { 111}
TD RD RD TD RD TD
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Orientation spread: FWHM
1 2 3 4 5 6 7 8 9 10
1,0 1,5 2,0 2,5 3,0 3,5 4,0 4,5 5,0 5,5 6,0
Week
b)
w = 1.8µm
TD RD TD RD
ILD #2 ILD #1
TD RD
FWHM (111) [Deg.]
1,5 2,0 2,5 3,0 3,5 4,0 4,5 5,0 5,5 6,0
a)
w = 180nm
TD RD TD RD
ILD #2 ILD #1
TD RD
FWHM (111) [Deg.]
Deviation: changed ILD + capping layer Process of record stable Wide lines: no influence
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Monitoring: Quantification
10 20 30 40 50 10 9 8
{111} total {111} {111}[0 1 -1] {111}[1 0 -1] Volume Fraction [%]
Week
{511} {611} {5 7 13}
(180nm)
Si(F)O / SiN
SiCOH / SiCN
With LaboTex (ADC)
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Influence of barrier layers on final Cu texture in inlaid copper lines
Ta Std Ta resputter TaN resputter Ta/ TaN/ TiSiN/ Ta
T a S t d T a / T a N / T i S i N / T a T a N / T a T a / T a N / T a T a r e s p u t t e r T a N r e s p u t t e r T a T E O S
1 2 3 4 5 6 7 8 9 10 FWHM(RD) FWHM(TD)
FWHM {111} [Deg.]
Barrier Layer
5 10 15 20 25 30 35 40 45 50 55
{511} {611} {5 7 13}
Volume Fraction [% ]
{111} total {111} {111}[0 1 -1] {111}[1 0 -1]
b) a) Barrier Layer RD TD changed EM behaviour
!
ILD = SiCOH
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Texture: explanation process (b)
{111}
RD TD
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GADDS Texture & Stress
texture on stress values
Anisotropy & shear stresses
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GADDS 2D stress analysis (triaxial) Bruker AXS (311)
180nm inlaid copper lines
GADDS
shear
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X-ray: in-line application
Why? Time critical issues (e.g., recrystallization) In-line process monitoring (also 300mm) How? Nondestructive, relatively fast X-ray See this conference:
Mapping on 200/ 300mm Patterned Wafers“, K. J. Kozaczek, et al.
During Damascene Copper Processing“, K. J. Kozaczek, et al.
al.
Interconnects“, K. Mirpuri, et al.
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X-ray summary:
X-ray micro-diffraction suitable for texture (and stress) analysis on arrays of ECD-filled inlaid copper lines, line segments, and vias (?) Nondestructive ( also in-line) X-ray lim its: Inlaid structures with barrier only or barrier and seed only (intensity!) Does not provide g(x), grain-boundary distribution and in- plane grain size
X-ray OIM
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EBSD: principle 70° sample tilt Kikuchi patterns Depth ∼ tens of nm SEM
Here: LEO 1 5 5 0 + therm . FEG, EBSD: TexSem Lab. ( TSL)
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EBSD on copper lines & via chains
I nverse pole figure m aps ( a) 2 0 0 nm lines ( b) via1 , via3 , via5 twin boundary
a)
Grain size monitoring
g(x)
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Limits of EBSD: passivation H= 27nm H= 34nm Narrow lines Cu Pad Narrow lines Cu Pad (200nm)
(Thickness of Passivation)
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Limits of EBSD: passivation Lines Cu pad
IQ= 93 IQ= 143
EBSD Analysis
H= 3 0
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EBSD: perspectives
Sequential FIB + EBSD 3D orientation image (e.g., via cross-section)
which grains & grain boundaries are critical ? locally resolved since g(x) is measured
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Barrier & Seed: X-ray, EBSD ACT
copper seed layers (∼30-50nm) EBSD not possible for nanocrystalline barriers and seed inside inlaid structures
ACT needed for barriers and seed in inlaid structures
ACT – Automated Crystallography for the TEM
[ TSL]
Multiple dark field images are collected by rotating the beam
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ACT on Cu seed in inlaid structures
Courtesy of Holger Saage, Hans-Jürgen Engelm ann
AMD Saxony, Dresden, Germ any
Grain size distribution of Cu seed inside inlaid structures Grain orientation map not possible yet in this case Compare seed grain sizes inside the structures with seed grain sizes on top and in the ECD-filled metal layer underneath !!
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Summary
X-ray micro-diffraction & EBSD process monitoring, texture, grain size, grain boundary distribution, trenches and vias
structures
ACT needed
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Trademark Attribution
AMD, the AMD Arrow Logo and combinations thereof are trademarks of Advanced Micro Devices, Inc. Other product names used in this presentation are for identification purposes