Section 5: Thin Film Deposition Jaeger Chapter 6 Chemical Vapor ...
Section 5: Thin Film Deposition Jaeger Chapter 6 Chemical Vapor ...
Section 5: Thin Film Deposition Jaeger Chapter 6 Chemical Vapor ...
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<strong>Section</strong> 5: <strong>Thin</strong> <strong>Film</strong> <strong>Deposition</strong><br />
Part 2: <strong>Chemical</strong> Methods<br />
<strong>Jaeger</strong> <strong>Chapter</strong> 6<br />
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<strong>Chemical</strong> <strong>Vapor</strong> <strong>Deposition</strong> (CVD)<br />
substrate<br />
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source<br />
More conformal deposition vs. PVD<br />
Shown here<br />
is 100%<br />
conformal<br />
deposition<br />
t<br />
t<br />
chemical reaction<br />
film<br />
step
( a)<br />
SiO<br />
SiH<br />
+ O →SiO<br />
( b)<br />
PSG : phospho<br />
4PH3<br />
+ 5O<br />
→2P<br />
O<br />
SiH<br />
Si<br />
4<br />
4<br />
2<br />
+ O →SiO<br />
+ 2H<br />
+ 2H<br />
( OC H ) → SiO + C H O ↑<br />
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↑<br />
silicate<br />
+ 6H<br />
( c)<br />
TEOS : tetraethylene<br />
orthosilicate.<br />
2<br />
gas<br />
gas 350 o C-500 o C<br />
2<br />
2<br />
LPCVD Examples<br />
5<br />
2<br />
4<br />
( d ) Si<br />
3SiH<br />
( e)<br />
Poly<br />
(<br />
SiH<br />
f<br />
WF<br />
) W<br />
+<br />
N<br />
+<br />
solid<br />
2<br />
2<br />
2<br />
5<br />
2<br />
2<br />
2<br />
350 o C-500 o C<br />
−<br />
→<br />
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↑<br />
600 C<br />
⎯ ⎯ →Si<br />
3 H<br />
NH<br />
Si<br />
X<br />
→ Si<br />
W<br />
glass.<br />
LPCVD Examples<br />
6<br />
4<br />
3<br />
4<br />
4<br />
o<br />
2<br />
3<br />
2<br />
3<br />
+<br />
+<br />
Y<br />
N<br />
4<br />
Z<br />
2 H<br />
6 HF<br />
[ PO<br />
+ SiO ]<br />
2<br />
↑<br />
5<br />
+ 12 H<br />
2<br />
2<br />
2
1<br />
2<br />
surface<br />
diffusion<br />
CVD Mechanisms<br />
reactant<br />
substrate<br />
1 = Diffusion of reactant to surface<br />
2 = Absorption of reactant to surface<br />
3 = <strong>Chemical</strong> reaction<br />
4 = Desorption of gas by-products<br />
5 = Outdiffusion of by-product gas<br />
3<br />
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Example Poly-Si <strong>Deposition</strong><br />
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5<br />
4<br />
stagnant<br />
gas layer
F 1<br />
F<br />
F<br />
CVD <strong>Deposition</strong> Rate [Grove Model]<br />
1<br />
3<br />
=<br />
=<br />
F 3<br />
δ<br />
film<br />
D [ C G -C S ] / δ<br />
k S C S<br />
Si<br />
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G<br />
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D<br />
=<br />
δ<br />
k<br />
s<br />
=<br />
h<br />
k<br />
G<br />
o<br />
e<br />
−ΔE<br />
kT<br />
δ = thickness of stagnant layer<br />
s<br />
F =<br />
Grove model of CVD (cont’d)<br />
1<br />
∴F<br />
3 = ⋅CG<br />
1 1<br />
+<br />
h k<br />
<strong>Film</strong> growth rate = F 3 / N<br />
dx F3<br />
∴ = = contant with time<br />
dt N<br />
1<br />
F<br />
3<br />
N = atomic density<br />
of deposited film<br />
Note: This result is exactly the same as the Deal-Grove model<br />
or thermal oxidation with oxide thickness =0
[log scale] Rate<br />
0<br />
<strong>Deposition</strong> Rate versus Temp<br />
high T<br />
gas transport limited<br />
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R∝T 3 2<br />
surface-reaction<br />
limited<br />
low<br />
T<br />
1/T<br />
Growth Rate Dependence on Flow Velocity
LPCVD Features<br />
(1) More conformal deposition,<br />
if T is uniform<br />
(2) Inter-wafer and intra-wafer thickness uniformity less<br />
sensitive to gas flow patterns. (i.e. wafer placement).<br />
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Comments about LPCVD<br />
(1) Sensitivity to gas flow pattern<br />
(2) Mass depletion problem<br />
in<br />
more less<br />
wafers<br />
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Furnace tube<br />
out<br />
Wafer<br />
topography
Plasma Enhanced CVD<br />
• Ionized chemical species allows a lower process<br />
temperature to be used.<br />
• <strong>Film</strong> properties (e.g. mechanical stress) can be tailored<br />
by controllable ion bombardment with substrate bias voltage.<br />
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Atomic Layer <strong>Deposition</strong><br />
• The process involves two self-limiting half reactions that are repeated in cycles<br />
• Unlike CVD, in ALD pulses of precursors are introduced in each cycle<br />
• ALD is highly conformal and enables excellent thickness uniformity and control<br />
down to nm-scale<br />
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