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Interdiffusion, Reactions, and Transformations
in Thin Film
Prepared by
Md Ataul Mamun
EE&CS Department, SDSU
1
•Impurity atom at position A must posses an energy EA to push
the host atoms away and move into the neighboring void at B
•EA is the activation energy
Diffusion of an impurity atom in a solid
2
Diffusion and diffusion length
d2 =4Dt
d= “distance” diffused after time t,
D = diffusion coefficient
D=
DO = constant
d
3
(a) Nucleation
(b) Growth
(c) Solidified polycrystalline solid
For simplicity cubes represent atoms.
Nuclei, Grain, and Grain Boundary
4
What is
Interdiffusion
?
Solid to solid diffusion
5
Interdiffusion facts for thin film
• Mass-transport differs from bulk to small scale
• Diffusions and corresponding reactions can alter the thin film
integrity
• May lead to device malfunction
• Capable of doing open and short circuits
6
How much Interdiffusion in thin film differs
from the bulk?
At 300C, Cu-Ni diffusion coefficient 3.8x10-24 cm2/s. For 0.1µm Ni film
what will be the Interdiffusion time?
d2 =4Dt
t=1/4(d2/D)
More than 200,000 years!!!
Experiment shows inter mixing happens in less than 1 hour!!!!
7
Considerable areas for diffusion
• Grain boundary (GB) Activation energy, EGB
• Dislocation (d)Activation energy, Ed
• Plain Surface (s)Activation energy, Es
8
Grain, Grain boundaries, and dislocations in
polycrystalline
• Grain-boundary slabs (δ) act as short circuit
diffusion path
• At dislocation cores (ꓕ), diffusion rate is
Just lower than grain-boundary
9
Dominant diffusion
regimes
TM =Melting point
From figure, as temperature rises
dominance goes from GB to L
However, for typical metal films with
a grain size of 1um or less, grain-
boundary diffusion dominates at all
practical temperature
Figure: Regimes of dominant diffusion mechanism in
FCC metal films as a function of temperature
10
T vs D
Figure: Diffusion coefficients (D) of various elements in Si
and GaAs as a function of temperature
D=
11
What should one do when diffusion parameters in
polycrystalline thin films must be estimated but
experimental data are lacking?
12
How to estimate
DGB/DL
• Draw horizontal line at T/TM
• Draw vertical line on grain size, log
d= log(2√DLt)
• Draw parallel line to beta through
intersection
Figure: Master Curves for estimating DGB/DL
13
Thin Film
Diffusion
couple
D=CADB+CBDA
CA and CB are respective concentrations
14
Effect of Infinite diffusion couple
• Consider O2 and Si wafer (They have an infinite
diffusion couple)
• SiO2 grows on surface and thickens with time
• The resulting amorphous SiO2 films serves critical
function of the gate oxide dielectric in FET
• Passivates the Si
• Allows a very low current leakage
• Leaves minimum dangling bonds
15
But not always great
• Difficult to solder on Al due to quick
oxidization
• Difficulty overcome by evaporated
Cr-Cu-Au thin film structure
• Solder joins with Cu easily, but Cu adheres
poorly with Al, so Cr is introduced
• To protect Cu, introduce Au
16
Interdiffusion in Miscible Alloy Systems
Figure: Palladium concentration profiles in a Au-Pd thin-film
Profile is symmetric when intrinsic
Atomic diffusivities are equal
ie, DA=DB
17
Grain Boundary
Diffusion in Thin-
Films
18
Intermetallic
compound formation
Figure: RBS spectrum showing formation of AuAl2 and
Au2Al Phases at 230C
Figure: Thickness relationship with time and temp
19
Compound Formation
in Films
End phases depend on whether
dAl>dAu or dAu>dAl
Figure: Compound formation sequence in Al-Au
thin film couples 20
Phase Transformation
in Thin Films
• Means changing state from one to another at
a fixed temperature
• Example: Amorphous CoSi2 to Crystalline
CoSi2
Figure: Transformed fraction of CoSi2 as a function of
time measured by change in resistivity
21
Metal-Semiconductor Reactions
22
Diffusion
Barriers
• Thin films used to separate materials from
coming into direct contact to prevent them
from reacting
• Similar to paint and electrodeposited layers to
protect underlying materials
23
Barrier
Requirements
Constitute a kinetic barrier to the traffic of A and B across
it (The diffusivity of A and B in X should be small)
Kinetic
barrier
Be thermodynamically stable with respect to A and B at
the highest temperature useStable
Have low contact resistance with A and B (and possess
high electrical and thermal conductivity)Low R
Be easy to deposit, adhere to the involved films, possess
low stress, and compatible with other processing
Easy to
deposit
Example: For Si-Al interconnection TiC, TiN
24
Silicides, Salicides,
Polycides
• Silicide: A silicide is a compound that has silicon
with (usually) more electropositive elements
(Example: Na2Si, TiSi2)
---Used in MOS/CMOS processes for ohmic
contacts of the source, drain, and poly-Si
gate
• Salicide: Self-Aligned silicide. Lithographic
patterning processes not required
• Polycide: Combination of a silicide and polysilicon
25
Salicides
26
Achieving Salicides
27
28

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Interdiffusion and thin film transformations

  • 1. Interdiffusion, Reactions, and Transformations in Thin Film Prepared by Md Ataul Mamun EE&CS Department, SDSU 1
  • 2. •Impurity atom at position A must posses an energy EA to push the host atoms away and move into the neighboring void at B •EA is the activation energy Diffusion of an impurity atom in a solid 2
  • 3. Diffusion and diffusion length d2 =4Dt d= “distance” diffused after time t, D = diffusion coefficient D= DO = constant d 3
  • 4. (a) Nucleation (b) Growth (c) Solidified polycrystalline solid For simplicity cubes represent atoms. Nuclei, Grain, and Grain Boundary 4
  • 6. Interdiffusion facts for thin film • Mass-transport differs from bulk to small scale • Diffusions and corresponding reactions can alter the thin film integrity • May lead to device malfunction • Capable of doing open and short circuits 6
  • 7. How much Interdiffusion in thin film differs from the bulk? At 300C, Cu-Ni diffusion coefficient 3.8x10-24 cm2/s. For 0.1µm Ni film what will be the Interdiffusion time? d2 =4Dt t=1/4(d2/D) More than 200,000 years!!! Experiment shows inter mixing happens in less than 1 hour!!!! 7
  • 8. Considerable areas for diffusion • Grain boundary (GB) Activation energy, EGB • Dislocation (d)Activation energy, Ed • Plain Surface (s)Activation energy, Es 8
  • 9. Grain, Grain boundaries, and dislocations in polycrystalline • Grain-boundary slabs (δ) act as short circuit diffusion path • At dislocation cores (ꓕ), diffusion rate is Just lower than grain-boundary 9
  • 10. Dominant diffusion regimes TM =Melting point From figure, as temperature rises dominance goes from GB to L However, for typical metal films with a grain size of 1um or less, grain- boundary diffusion dominates at all practical temperature Figure: Regimes of dominant diffusion mechanism in FCC metal films as a function of temperature 10
  • 11. T vs D Figure: Diffusion coefficients (D) of various elements in Si and GaAs as a function of temperature D= 11
  • 12. What should one do when diffusion parameters in polycrystalline thin films must be estimated but experimental data are lacking? 12
  • 13. How to estimate DGB/DL • Draw horizontal line at T/TM • Draw vertical line on grain size, log d= log(2√DLt) • Draw parallel line to beta through intersection Figure: Master Curves for estimating DGB/DL 13
  • 14. Thin Film Diffusion couple D=CADB+CBDA CA and CB are respective concentrations 14
  • 15. Effect of Infinite diffusion couple • Consider O2 and Si wafer (They have an infinite diffusion couple) • SiO2 grows on surface and thickens with time • The resulting amorphous SiO2 films serves critical function of the gate oxide dielectric in FET • Passivates the Si • Allows a very low current leakage • Leaves minimum dangling bonds 15
  • 16. But not always great • Difficult to solder on Al due to quick oxidization • Difficulty overcome by evaporated Cr-Cu-Au thin film structure • Solder joins with Cu easily, but Cu adheres poorly with Al, so Cr is introduced • To protect Cu, introduce Au 16
  • 17. Interdiffusion in Miscible Alloy Systems Figure: Palladium concentration profiles in a Au-Pd thin-film Profile is symmetric when intrinsic Atomic diffusivities are equal ie, DA=DB 17
  • 18. Grain Boundary Diffusion in Thin- Films 18
  • 19. Intermetallic compound formation Figure: RBS spectrum showing formation of AuAl2 and Au2Al Phases at 230C Figure: Thickness relationship with time and temp 19
  • 20. Compound Formation in Films End phases depend on whether dAl>dAu or dAu>dAl Figure: Compound formation sequence in Al-Au thin film couples 20
  • 21. Phase Transformation in Thin Films • Means changing state from one to another at a fixed temperature • Example: Amorphous CoSi2 to Crystalline CoSi2 Figure: Transformed fraction of CoSi2 as a function of time measured by change in resistivity 21
  • 23. Diffusion Barriers • Thin films used to separate materials from coming into direct contact to prevent them from reacting • Similar to paint and electrodeposited layers to protect underlying materials 23
  • 24. Barrier Requirements Constitute a kinetic barrier to the traffic of A and B across it (The diffusivity of A and B in X should be small) Kinetic barrier Be thermodynamically stable with respect to A and B at the highest temperature useStable Have low contact resistance with A and B (and possess high electrical and thermal conductivity)Low R Be easy to deposit, adhere to the involved films, possess low stress, and compatible with other processing Easy to deposit Example: For Si-Al interconnection TiC, TiN 24
  • 25. Silicides, Salicides, Polycides • Silicide: A silicide is a compound that has silicon with (usually) more electropositive elements (Example: Na2Si, TiSi2) ---Used in MOS/CMOS processes for ohmic contacts of the source, drain, and poly-Si gate • Salicide: Self-Aligned silicide. Lithographic patterning processes not required • Polycide: Combination of a silicide and polysilicon 25
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