thermal laser stimulation (tls / obirch / tiva) · 3 microelectronics tls principles laser λ = 1,3...
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MICROELECTRONICS
FAILURE ANALYSIS LABORATORYTHALES Microelectronics S.A.
THERMAL LASER STIMULATION(TLS / OBIRCH / TIVA)
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TLS in the FA flowI.C. FA flow
Electrical diagnostic
Defect localization
Physical analysis
Current related defects
Emission microscopy
Thermal Laser Stimulation
– Ileakage metallic shorts
– Ileakage junctions– Ileakage oxides
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TLS PrinciplesLASER
λ = 1,3 µm• Heating• No e-h pair
generation
High absorption in:– Metals– Polysilicon– Highly doped silicon
16Aluminium cm10x1,1 −=α
Valence band
Conduction band
Ephoton < Eb.g.
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Laser Heating of Metals
Electric current density :
↑ T° → Current variation∇ T°→ Additional current
( )[ ]TQ ∇−+≅ Ej σ
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A. Resistance Variation
( ) TSLR TTCR ∆−=∆ δαρ 20
αTCR → Temperature Coefficient of Resistivity
δT → Coefficient of Thermal linear dilatation
Aluminium
αTCR = 4,29x10-3
δT = 2,36x10-5 ( )V RRI 2∆−=∆
Current Source (TIVA)
IRV ⋅∆=∆Voltage Source (OBIRCH)
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B. Electromotive Force Generation
T > T0
T0
Laser
T0 M 1 M 2
Q → Thermoelectric power orSeebeck coefficient
Q12 → Relative Thermoelectric power
( )( ) ( )01202112 TTQTTQQV −=−−=
Materials Q12 (µV/oC)
Al / W 7,0
-121
Al / n+ Si(1020cm-3) -105
Al / n+ Poly
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TLS Model
Length = 120µm
Model: 1µm Al line, Gaussien Laser
2 cases:- Transversal- Longitudinal
1µm0.5µm1µm
AlSiO2
Silicon
1µm
4µm
10µm
Parameters:Tini: 25oCPlaser: 100mWRlaser: 0,65µmVfast: 1,23m/sVslow: 0,00768m/s
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A. Transversal Case• Rapid thermal equilibrium and heat dissipation• Hottest temperature occurs at laser spot
Slowest scanning speed
253545556575
0 1 2 3 4 5 6 7 8 9 10 11 12 13Position (µm) Elapsed time (µs)
T (°
C)
transversal slowtransversal fast
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B. Longitudinal Case
• Thermal equilibrium reached after 10µs
Slowest scanning speed
25
35
45
55
65
75
0,0E+00 5,0E-06 1,0E-05 1,5E-05 2,0E-05Time (s)
T (°C
) longitudinal slowlongitudinal fast
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Temperature CalculationAt thermal
equilibrium:
Thermal spreading limited to ~ 30µm
Temperature varies linearly with laser
power
∆Tmax = 0.55oC/mW
25
35
45
55
65
75
-20 -10 0 10 20Position from the laser center (µm)
T (°C)trans. slowtrans. fastlong. slowlong. fast
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Resistance Calculation
Laser Power(mW)0 20 40 60 80 100
Res
ista
nce
Varia
tion
(Ω)
0,00
0,05
0,10
0,15
0,20∆R = 0,17Ω
∆Rmax = 1,7 mΩ/mW
( )0MoyTCR0 TTS
LR −αρ
=∆
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Model Conclusion
Precise localizationThermal diffusion < 30µm
Tmax at center of line and laser beam
Localization of defects and lines submitted to Ileakage∆R 1/∝ Section∆V ∝ Ileakage
Localization of junctions and interface defectsQ12 or ∆T
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TLS System Requirements• Laser scanning microscope (LSM)
– Gaussian laser of λ > 1,1µm• Acquisition and imaging system• Biasing and amplification scheme :
Techniques Inventor Bias
OBIRCHCC-OBIRCH
TIVATBIPXIVA
NikawaNikawa
Cole
PalaniappanFalk
V
I
V
SEI Cole
Amplifier
I / None
I
V
V
V
TLS
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Configurations
I.C.
AMPLIV / V
I.C.
AMPLII / V
OBIRCH
I.C.
AMPLIV / V
TIVA• Other configurations:
– Inductance (TBIP / XIVA)– No bias (SEI)
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TLS on Test StructuresAl line
Poly line
N+ resistance
No bias (SEI)
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TLS Case Study #1• Failed CMOS IC
– I ~ 2mA @ 5V• No emission• Front-side
Metal short (M1-M2)
TLS 200X
TLS 5X
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TLS Case Study #2• Failed BICMOS IC
– I > 100 µA (I/O)• Backside
– 4 metal levels
TLS (20x)
W short (Drain-Source)EMMI (20x)
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TLS Case Study #3• Failed CMOS IC
– I ~ 2 mA @ 3V • Front-side
TLS (20x)
TLS (20x)
Metal short (M2-M3)
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TLS Case Study #4• ESD failed commercial ICs
– HBM and MM stressed• Front-side
– No bias applied (SEI)SEI (200x)
SEI (50x)
Molten Si/Al filament
Molten Sispike
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TLS Case Study #5• GaAs failed ASICS
– I ~ 50 µA @ 3V • Front-side
TLS (100x) Gold filament
Defects induced by CDM type ESD stress
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Conclusion : TLS Application Field
Thermal Laser
StimulationSignature Defect type Material
Current lines Shorts
ESD defects Voids
No Bias
Ileakage >1µA
All circuits Comparison
Bias
ESD defects Interface defects
AI, W, Au, PolySi,
Doped Si, Amorph. Si
Metal / Metal Metal / Si
Metal / Poly SiMelted Si / Si