Integration/Reliability Issues for Cu/low-k BEOL Interconnects
Transcript of Integration/Reliability Issues for Cu/low-k BEOL Interconnects
© 2007 IBM Corporation
IEEE Workshop on Microelectronics and Electron Devices, April 3, 2009, Boise
Integration/Reliability Issues for Cu/low-k BEOL Interconnects
Daniel C. EdelsteinIBM Fellow and Manager, BEOL Technology StrategyIBM T. J. Watson Research Center, Yorktown Hts., New [email protected]
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Outline
From an integration perspective, discuss scaling impacts on reliability of:
Metals
Insulators
Chip-Package Interaction (CPI)
Summarize for each– key issues, proposed solutions, key metrics, analytical techniques
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Via/line interface
Liner-seed and Cu fill
Cu electromigration
Cap reliability
Dielectric-Cap adhesion
Dielectric reliability
Outline
Vacuum (“Air-”) Gaps
90 nm45 nm
Technology Map
Underfill
Chip-Package
Crackstop
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SummaryMetals
– Issues: Cu gapfill, Cu grain growth, electromigration scaling, new materials in liner/seed– Proposed solutions: Noble-like metal in liner, selective metal cap, Cu-alloy seed– Critical Metrics: Via yields, Cu resistivity, defectivity, electromigration, stressmigration– Analytical: Cu/barrier interfacial diffusivity and Ea, Cu grainsize, metal interdiffusions, galvanic
potentials, TEM/EELS, tomography, other microprobes
Insulators– Issues: Low-k mechanical and dielectric strengths, process damage, damascene pattern integrity– Proposed solutions: Incremental k reduction, re-optimization of film properties, modify skeleton– Critical metrics: Patterning, wire C, I-V, Vbr, TDDB, tensile stress, modulus, chip-package reliability– Analytical: Electrical, mech. modeling, modulus/hardness, adhesion, fracture toughness, pore size,
porosity, plasma-induced damage
Chip-Package– Issues: TCE mismatches, tensile low-k, weak low-k and pkg. polymers, larger chips, Pb-free C4’s– Proposed solutions: Tough crackstop, maximized low-k strength and adhesion, “ideal” underfills,
chip-join thermal budgets, reduced-TCE laminates (cores), compliant leads, Si Carrier– Critical metrics: Deep thermal cycle reliability, T/H/B, etc., underfill toughness and fatigue– Analytical: Sonoscan, failure analyses techniques, polymer Kc and fatigue
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Acknowledgements
This work was done by countless colleagues from IBM and our R&D Alliance partners, at:– T. J. Watson Research Center, Yorktown Hts., NY
– Nanotechnology Center, Albany, NY
– Semiconductor and Packaging R&D Centers, E. Fishkill, NY
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Data Section
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Impact of Electron Scattering in Nanoscale Cu WiresExtracted Cu Resistivity vs. Wire Cross-Sectional Area
L. Gignac, AMC 2007
• Cu resistivity increases as Cu wire area decreases.• Cu grain size does not influence ρ greatly when grain size > electron mean free path.• In the above case, surface scattering is the major factor.• TCR method in literature overestimates ρ.
ITRS65 nm nodeρ~2.5 µΩcm
1.5x103 104 105
2.0x10-6
2.2x10-6
2.4x10-6
2.6x10-6
2.8x10-6
3.0x10-6
3.2x10-6
3.4x10-6
3.6x10-6
3-4 TEMs per datapoint
Data fit to:ρ= ρo (1+Cλ/A)
ρo = 2.01 ± 0.02 E-6 Ω-cm
C = 580 ± 45 Ωcm. nmλ = 3 nm
M1
Cu
ρ( Ω
-cm
)
Line Area ( nm2 )
LRACu=ρ
Able to predict ρ for future technology nodes
ITRS45 nm nodeρ~3.0 µΩcm
ITRS32 nm nodeρ~3.9 µΩcm
a)
b)
c)
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IEEE WMEDExtendibility Problem: Electromigration Lifetime Reduction Scaling in Cu Damascene Lines
– Top Cu/cap interface dominates E-M diffusion for bamboo lines– Scaling trend is predictable by geometry, with no adjustable parameters– Lifetime drops as dimension shrinks – now dropping at 50%/generation– At the same time, chip current density requirements scale up– Cu lines at 45 nm node and beyond have reduced bamboo grains – further impact
0.0 0.2 0.4 0.6 0.8 1.0 1.2
0.01
0.1
1
Theory
t 50/t 50
(1.3
x0.9
)
∆Lcrxh (µm2)
e
Blocking material
liner Void Cu h
C-K. Hu, IRPS 2004 and IITC 200716 17 18 19
10 1
10 2
10 3 W f B w (µm ) Q E M(eV ) 1 .9 0 .93 0 .7 0 .96 0 .14 0 .95 0 .09 0 .84
t 50 (h
)1 /T (10 -4K -1)
Interfacial diffusion
Interfacial diffusion Ta
gb diffusion
SiCNH
surfa
ce
Void
Marker Velocity
Grain-boundary diffusion degrades Cu electromigration reliability in nanowires
Cu linewidth, grain size
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Bamboo (Cu grainsize solved) Non-Bamboo (Cu grains not solved)
Approaches to Recover Cu Electromigration Reliability vs. Scaling
Selective Metal Cap(Shut down top-surface Cu diffusivity)
e.g. electroless CoWPimpacts: leakage, TDDB,
manufacturability
Flash noble liner layer on TaN/Ta(Increase Cu grain growth?)
e.g. PVD (Ta)Ru, CVD-Ru or –Coimpacts: reduced Cu volume %, galvanic
corrosion potential, CMP difficulties
Doped Cu seed(Stuff small Cu grain boundaries)
e.g. Cu(Al)impacts: Cu resistivity, linewidth-dependence,
dilute alloy control in mfg.
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IEEE WMEDOne Solution to Cu Electromigration Scaling Problem: Selective Metal Caps
For “bamboo” lines:• Selective top metal cap can eliminate EM issue completely• Activation energy can reach to bulk Cu values• Current densities are then limited to much higher values by rms joule heating
For small-grained lines:• Grain boundary diffusion may still dominate electromigration lifetimes
Challenges:• Remedy insufficient Cu recrystallization or Cu grain boundary diffusion (e.g. by alloy)• Achieve manufacturable selective metal capping process with a uniform ~few nm cap, and no impact to shorts yield, line-line leakage, or dielectric breakdown reliability
C-K. Hu, IRPS 2004
example: electroless CoWP
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Selective CVD-Ru Metal Cap
Sele
ctiv
ity
Blanket Deposition Rates
Microanalysis
Test Chips
Performance
Opens and Shorts Yields
TDDB Reliability
Electromigration Reliability
C-C. Yang, et al. submitted to IITC 2009
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Another Approach - Cu-Alloy Seedlayer for E-M Enhancement
Pileup of Al dopant at Cu/cap interface reduces fast-path Cu E-M
S. Yokogawa, et al., IEEE IRPS 2007
Electromigration
Cu Resistivity
• Adding certain dopants to the Cu seedlayer can enhance E-M reliability…but at the expense of Cu resistivity…and linewidth-dependence…and other potential mfg. control issues
• Need to determine best dopant and its % in Cu for optimal R vs. E-M.Numerous candidates studied over the years, most rejectedAluminum has emerged as a good candidate
• Several companies have adopted Cu(≤ 1 at.% Al) in production since 65/45 nm
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Cu Metallization Gapfill Extendibility Problem
Via yield and reliability are based on liner/seed/plating process window…
…that is determined by Cu seed process window, comprised of:
• Reactive Ion Etch (RIE) patterning
• Liner pinch-off above, and continuity below
• Seed pinch-off above, and continuity below
• Plating (seed etching and superfill rates)
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Extendibility of Cu Damascene Metallization: Add Noble Metal to Ta-Based Barrier
Retain ECD-Cu gapfill process window and Cu reliability with minimal integration disruptionRetain high-integrity PVD-Cu/barrier interface for electromigration (e.g. Ta/Cu, not Ta2O5/Cu)Increase thin Cu seed wettability and continuity in small, high a.r. featuresProvide good plating nucleation inside Cu-seed discontinuitiesMinimal impacts to plating (terminal effect), CMP, Cu fill volume (Cu line resistance)New concerns for galvanic corrosion, Cu/barrier adhesion and electromigration
PVD-TaNPVD-TaPVD Ta(Ru) or CVD-Ru
PVD-CuECD-Cu
TaN/Ta TaN/Ta0.3Ru0.7 TaN/Ta0.1Ru0.9
TaN/Ta TaN/Ta0.1Ru0.9 TaN/Ta/Ru
PVD
PVD/CVDPVDPVD
PVDPVD
BEOL: Yang et al., IITC 2006Cu contacts: Seo et al., AMC 2008
BEOL: Nogami et al., AMC 2008
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12
5
10
20
3040506070
80
90
95
9899
Cum
ulat
ive
Failu
re P
roba
bilit
y(%
)
Lifetime (au)
T = 300oC, I = 0.10 mA
V1 to M2
TaN/TaTaN/TaRu90%
TaN/Ta
TaN/TaRu90%
Cu Electromigration Performance with TaN/TaRu Barrier
More than 3X longer lifetimesRecovered normal reliability by fixing defective Cu gapfill
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Testing New Barrier Properties
TaRu90%
TaRuN90%
TaRuN70%
TaRu70%
Ta TaN
PVD TaRu(N) films do not fully block Cu+ or O2 diffusion.PVD TaN and/or Ta is required underneath TaRu.
Ta, TaN >> TaRu70% > TaRuN70% > TaRu90% > TaRuN90%
Cu+ Barrier Test(Triangular Voltage Sweep, 300C, 1 MV/cm
TaRuN90%/TaRu90%
No Cu oxidation
Cu is oxidized Cu is oxidized
TaRuN70%/TaRu70%
TaN/TaTaN/TaRu90%
No Cu oxidation
Oxidation Barrier Test(310C/8 days in air)
TaN/Ta = TaN/TaRu90% >> TaRuN/TaRu
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Extendibility of the Most Reliable Via/Line Contacts
max stress
low stress
stress gradient
max stress
low stress
stress gradient
max stress
low stress
stress gradient
max stress
low stress
stress gradient
max stress
low stress
stress gradient
A. Fischer, et al., IEEE IRPS (2007).
1 10 100 1000
Stress Failure Time (hrs.)
99.9
99959075502510
51
0.10.01
perc
entil
e
V2 -> M2; T50 = 215.3 hrs. σ = 0.1463
Cu is 500 X better than Al(Cu) at 300C
D. Edelstein, et al., IEEE IRPS (2004).
90 nm CMOS 45 nm CMOS65 nm CMOS ULK with new process
ULK with old process
C-C. Yang, et al., AMC (2008).
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Advanced Dielectrics Roadmap: current IBM status
Leading development and implementation of industry’s most advanced low-k and ultralow-k PECVD dielectrics
Technology nodes
AvailabilityImplementation
90nm 45nm65nm 32nm 22nmSiCOH k=3.0
pSiCOH k=2.4
15nm
SiCOH k=2.7
pSiCOH k=2.2
pSiCOH k=2.0
PECVD Films
A. Grill, AMC 2007 and MRS 2009
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IEEE WMEDLow-k and Ultralow-k Time-Dependent Dielectric Breakdown (TDDB)
• Low-k obeys root-E kinetics at least, and may be more robust• Cu reduces lifetimes and plays an important role• Moisture is bad• Line-edge roughness affects lifetimes J. Lloyd, AMC 2008
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channel crackingcohesive vs. adhesive failure
delamination
chip packaging interactionBEOL film fabrication
G: energy release rate G: fracture strengthstructure and geometryfilm stressthermal expansion and modulus
chemical bondinginteraction with environment
Methodology of Fracture Mechanicsexcerpts from X-H. Liu, MRS 2009 invited talk
ΓG <
X.H. Liu et al, IITC (2004) AMC (2004)Issue: Low-k C-doped SiOx glass films, the industry de facto standard, are unfortunately always tensile-stressed and have relatively low moduli and fracture toughnesses
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Strengthening Low-k and Ultralow-k SiCOH Interfacial RegionHistorically, chronically low SiCOH adhesion results
Typical pretreatments did not improve
Discovered weak nucleation layer at interface
Solution became clear – graded nucleation
Dramatic adhesion improvement, approaching
~bulk cohesive strength
Extendible to ultralow-k porous SiCOH (not trivial)
Identifiable by TOF-SIMS profiles of thin samples
Adhesion StrengthControl - no optimization
G = 2.1 J/m2
With optimization
G = 5.0 J/m2
A. Grill et al., MRS Spring 2007.D. Restaino et al., AMC 2007.S. Molis et al., SIMS Workshop 2007.
Si
Bulk SiCOH
SiCHN “adhesion layer”
Low-k Insulators
3.53.52.7-3.42.0k=2.4
4.54.1n/a2.0k=2.7
6.05.03.0-4.02.0k=3.0
Cohesive Strength (J/m2)
Optimized Transition (J/m2)
Substrate Treatment (J/m2)
Bulk-only SiCOH (J/m2)
SiCOH Version
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Effect of Multilevel MetallizationX-H. Liu, MRS 2009 invited talk
0 5 10 15 200.0
0.5
1.0
1.5
2.0
Ene
rgy
Rel
ease
Rat
e N
orm
aliz
ed
Gap Width Normalized
thin wires
channel crack propagation
crack arrest on cap
fat wires
substrate
Single metal level
Multiple metal levels
Large enhancements in G possible with patterned metal under layers
J.M. Ambrico, E.E. Jones, and M.R. Begley, (2002) Int. J. Solids and Struct, 39, pp.1443
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•Cap layer acts like a springholding the metal pads together.•Strength of spring is proportional to the cap thickness X Cap Modulus
Effects of CapsX-H. Liu, MRS 2009 invited talk
Cap stiffness is important to prevent cracking.
0 2 4 6 8 1025
30
35
40
45
50
Gm
ax/G
0
varying modulus varying thickness
Modulus x Thickness (kNm)
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Spontaneous Cracking X-H. Liu, MRS 2009 invited talk
Spontaneous cracking observed in structures with a narrow gap. Tunneling cracks may form in the SiCN cap dielectric. Si SiO2
4 levels in SiCOH
4 Levels in pSiCOH
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Finite Element Modeling of ULK Films in BEOL StructuresTo optimize ULK mechanical properties and wiring groundrule limits, and compute maximum strain energy release rate before channel cracking
Energy release rate (crack driving force) increases with # levels in stackMost sensitive to (tensile) stress, somewhat sensitive to modulus
‚ Reduce ULK film stress and increase modulus to avoid cracking
X.Liu et al., ASME 200612
34
56
10
20
3040
5060
0
1
2
3
4
5
6
7
8
9
10
11
Film Stress Normalized
Ener
gy R
elea
se R
ate
Nor
mal
ized
Modulus Normalized
EB
B2
M31X
2X
4X
G=A σ2 h/E
Safe
Channel Cracking
Cohesive StrengthOf Dielectric
TE∆∆
−+= α
υσσ
1int
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Fundamental SiCOH Toughness
Goal: Exceed universal curve for tougher PECVD ULK pSiCOHReduce sensitivity to plasma-induced damage
Approach: Improve molecular skeleton with Si-C-Si bonding……but don’t go too far!
1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5 5.0Nominal Dielectric Constant, k
0.0
4.0
8.0
12.0
Coh
esiv
e St
reng
th, Γ
(J/m
2 )Universal curve determined by Si-O bond density
Current(O)SG Universal Trend
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DEMS
BCHD
SkeletonPrecursor 2
PECVD
300 mmProduction tool
UV cure
300 mmProduction tool
Ultralow-k Porous SiCOH Extendibility:Increase Cohesive Strength and Reduce Resistance to Plasma Damage
Skeleton 1: DEMS (diethoxymethylsiloxane), strong Si-O x-linking, efficient porogen incorp.Porogen: BCHD (bicycloheptadiene) incorporates very efficiently, widely tunable k.Skeleton 2: (proprietary), adds Si-CH2-Si bonding for smaller pores, reduced plasma damage, increased toughness.
k 2.4 pore size distributions from EP
0
2
4
6
8
10
12
1 1.5 2 2.5 3 3.5 4 4.5 5Pore diameter (nm)
dV/d
(ln R
)
V1.0 Film 2
Property V1 V2 V1 V2
Modulus [Gpa] 4.5 3.8 2.7 2.3
Stress [Mpa] 47 51 38 40
Interface strength [J/m2] 4.0 4.0 3.5 4.0
Porosity (%) 30 29 37 33
k 2.4 k 2.2
S. Gates, et al., AMC (2008).
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Effects of adding Si-C-Si bonding to Si-O-Si matrixLess pore connectivity, more Si-C bonds to break for damage less plasma-induced damage
Average line width reducedTrench bottoms improvedLeakage current reducedNet reduction in line capacitance for same k of film
K 2.2, V1
K 2.2, V2
K 2.2, V2Advanced Porous SiCOH, K=2.2, at 32 nm Node 1x Dimensions
S. Gates, et al., AMC (2008).
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Advanced Bilayer Low-k Cap Film
Passes O2 Barrier test
Cu
Adv. SiCNy
SiCNx
0 0.5 1 1.5 2 2.5 3 3.5 4 4.50
10
20
30
40
50
60
70
80
90
100
Sputter Time (min)
Rel
ativ
e C
once
ntra
tion
(%)
N1.ls1C1.ls1
Si2.ls1
O1.ls1
Cu1.ls1Air barrier properties confirmed
G. Bonilla, et al., AMC (2008).
10 100 100012
5
10
20304050607080
90
95
98 302oC
Cum
ulat
ive
Failu
re P
roba
bilit
y (%
)
τ (h)
256oC331oC 218oC
SiCNxLow-k Adv barrier
350oC
Passes E-M, S-M, and TDDB tests
-5%
Achieves required keff reduction
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Multilevel Airgap Wiring Demonstration on Advanced 65 nm Production Microprocessor
Airgap process schemes applied to all Cu wiring levels above M1.Lithographic slots on larger (2x and above) levelsSelf-assembly sublithographic patterning for minimum (1x) levels
No changes to standard Cu wiring process flow, fab tooling, or materials.Yield, performance, reliability, and modeling predictions demonstrated.
8x
4x
2x
8x
4x
2x1x
1x
Airgap Technology
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Capacitance modeling– C reduction can be optimized to -40%
CPU tuned performance estimates – ~10% Fmax, ~15% active pwr
Capacitance modeling– C reduction can be optimized to -40%
CPU tuned performance estimates – ~10% Fmax, ~15% active pwr
Mechanical modeling – Gap calculations find low cracking risk
Capacitance modeling– C reduction can be optimized to -40%
CPU tuned performance estimates – ~10% Fmax, ~15% active pwr
Mechanical modeling – Gap calculations find low cracking risk
Thermal modeling sets current limits – very small gap impact is calculated
Capacitance modeling– C reduction can be optimized to -40%
CPU tuned performance estimates – ~10% Fmax, ~15% active pwr
Mechanical modeling – Gap calculations find low cracking risk
Thermal modeling sets current limits – very small gap impact is calculated
Electromigration– good preliminary results
Capacitance modeling– C reduction can be optimized to -40%
CPU tuned performance estimates – ~10% Fmax, ~15% active pwr
Mechanical modeling – Gap calculations find low cracking risk
Thermal modeling sets current limits – very small gap impact is calculated
Electromigration– good preliminary results
Time-dependent dielectric breakdown– good preliminary results
1.00E-3 1.000.01 0.10 1.00 10.00 100.00 1000.00 10000.00 100000.001000000.001.00
5.00
10.00
50.00
90.00
99.00
Time [hrs]C
DF
(%)
Ungapped (Green)
Gapped (Red)
Capacitance modeling– C reduction can be optimized to -40%
CPU tuned performance estimates – ~10% Fmax, ~15% active pwr
Mechanical modeling – Gap calculations find low cracking risk
Thermal modeling sets current limits – very small gap impact is calculated
Electromigration– good preliminary results
Time-dependent dielectric breakdown– good preliminary results
Chip-package reliability stressing– no issues in preliminary tests
We have seen some good preliminary indicators for manufacturabilityNeed more extensive data, models, process windows for qualification
Comprehensive Airgap Performance/Reliability Assessment
Sonoscan after 1000 deep thermal cycles shows no fails
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1. Corner Underfill Delam./Crack 2. C4/BEOL Delam.
3. BEOL Edge Delam. 4. Chip Fracture
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1. Corner Underfill Delam/Crack 2. C4/BEOL Delam.
3. Edge BEOL Delamination Chip Fracture
– Worst for ultra-large chips on organic laminates– Increases with chip-size– Cracks circumvent chip crackstop– Fatal, independent of BEOL materials– Limitations on available underfills, laminates– Mitigation strategies required
– Chip-size, dicing, and BEOL low-k, ULK dependent– Solved by tough crackstop and optimized dicing– Crackstop toughness >> ULK, Si, SiO2, etc.– Low-k and ULK optimized for adhesion/cohesion
– Flat vs. chip size above ~0.5 cm– Worse for Pb-free C4– Can fail at weakest BEOL interface– Mitigation strategies required
– Primarily when chips are thinned– Dicing and handling defects + stress– Increases with chip size– Fatal, independent of BEOL materials– Mitigation strategies required
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Crackstop Problem OverviewX-H. Liu, MRS 2009 invited talk
Si
G, Γ
Interfacial adhesion (limited by ILD cohesive strength)
Crackstop toughness
position
Energy of dicing cracks during dicing process
Maximum energy of delamination during DTC
Si toughness
(After Robert Cook 1994)
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molding compound
Silicon substrate
oxide
ILD
Method to Improve Crackstop ToughnessX-H. Liu, MRS 2009 invited talk
fibre toughening
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Measurement of Crackstop Effective Toughness
Produce chip with large areas of crackstop structure
Mask designs includes multiple isolated crackstop designs
4 point bend test gives toughness of individual designs
Load for failure of crack stop used to determine optimum design
0 1000 2000 30000
2
4
6
Load
(lbs
)
Time (Secs)
8-10 J/m2
4 J/m2
Delamination traveling
In the unreinforced area
Delamination hits
Crack stops
Delamination pinned
at loading points
Delamination
initiates
Load Displacement for Multilevel ULK Build
T. Shaw et al., IITC 2007
Notch position
Crackstops
Isolated widths of crackstop structure
4-pt. bend load cell
Fracture Energy Calculation:
32
222
16)1(21hEb
LPG cν−=
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IEEE WMEDSolving Cu/Low-k and Ultralow-k Chip-Package Interaction (CPI) Reliabilityexample: 45 nm CMOS with low-k and ultralow-k wiring levels
Fundamental mechanical solutions enable ULK (k=2.4) to pass comprehensive CPI:Extensive finite-element modelingOptimized dicingImproved crackstop toughness Improved ULK adhesion S. Sankaran et.al., IEEE IEDM (2006).
C4
Si
BEOL
Delaminationsobserved
No Delaminationsobserved after dicing optimization
Delaminationsobserved
No Delaminationsobserved after dicing optimization
0 CPI fails after 1000 cycles of -55/+125C
EPBGAWirebond
0 fails after 1800 cycles of -40/+125C stress.
FCPBGA
0 fails after 1000 cycles of -55/+125C stress.
MLC-LGAFlip chip
Deep thermal cycle stress
PackagingTest chip
0 CPI fails after 1000 cycles of -55/+125C
EPBGAWirebond
0 fails after 1800 cycles of -40/+125C stress.
FCPBGA
0 fails after 1000 cycles of -55/+125C stress.
MLC-LGAFlip chip
Deep thermal cycle stress
PackagingTest chip
SiMold
MoldOxide
SiSiCOH
BPSG
X25 Crackstop Toughness
Interface CS1 CS20
1
2
3
4
5
6
7
8
9
10
Rel
ativ
e To
ughn
ess
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Crack dives into BEOL structuredamage found on multiple layers
Examples of Chip-Corner/Underfill Fail Mode
Modeling is well understood for corner stresses, but not underfill fatigue