2. 2Microelectronics Processing Course - J. Salzman - Jan. 2002
Thin film deposition systemsThin film deposition systems
CVD
PVD
Spin-on
Electrolytic deposition
3. 3Microelectronics Processing Course - J. Salzman - Jan. 2002
CVD depositionCVD deposition
Chemical Vapor Deposition is the formation of a
non-volatile solid film on a substrate by the reaction
of vapor phase chemicals (reactants) that contain the
required constituents.
The reactant gases are introduced into a reaction
chamber and are decomposed and reacted at a heated
surface to form the thin film.
7. 7Microelectronics Processing Course - J. Salzman - Jan. 2002
Steps involved in a CVD processSteps involved in a CVD process
(schematic)(schematic)
8. 8Microelectronics Processing Course - J. Salzman - Jan. 2002
Steps involved in a CVD processSteps involved in a CVD process
(schematic)(schematic)
3. Adsorption of reactants on the wafer surface.
4. Surface processes, including chemical decomposition or
reaction, surface migration to attachment sites (such as atomic-
level ledges and kinks), site incorporation, and other surface
reactions.
5. Desorption of byproducts from the surface.
6. Transport of byproducts by diffusion through the boundary
layer and back to the main gas stream.
7. Transport of byproducts by forced convection away from the
deposition region.
1. Transport of reactants by
forced convection to the
deposition region.
2. Transport of reactants by
diffusion from the main gas
stream through the boundary
layer to the wafer surface.
9. 9Microelectronics Processing Course - J. Salzman - Jan. 2002
Steps involved in a CVD processSteps involved in a CVD process
(schematic)(schematic)
10. 10Microelectronics Processing Course - J. Salzman - Jan. 2002
Steps involved in a CVD processSteps involved in a CVD process
(schematic)(schematic)
11. 11Microelectronics Processing Course - J. Salzman - Jan. 2002
Steps involved in a CVD processSteps involved in a CVD process
(limiting processes)(limiting processes)
1. Gas phase process (mainly diffusion to substrate).
2. Surface process (mainly reaction)
12. 12Microelectronics Processing Course - J. Salzman - Jan. 2002
CVD kinetic growth modelCVD kinetic growth model
We approximate the flux Fl by the linear formula
F1
= hG
(CG
–CS
)
where CG
and CS
are the concentrations of the
SiCI4
(molecules per cubic centimeter) in the bulk
of the gas and at the surface, respectively, and hG
is the gas-phase mass-transfer coefficient.
The flux consumed by the chemical-reaction taking place at the surface of
the growing film F2
is approximated by the formula
F2
= kS
CS
where kS
is the chemical surface-reaction rate constant.
In steady state F1
= F2
= F. Using this condition, we get
GS
G
S
hk
C
C
/1+
=
13. 13Microelectronics Processing Course - J. Salzman - Jan. 2002
CVD kinetic growth model-IICVD kinetic growth model-II
We can now express the growth rate of the silicon film by writing
where N1
is the number of silicon atoms incorporated into a unit volume of the film.
Its value for silicon is 5.0×1022
cm-3
. Noting that CG
= YCT
where CT
is the total
number of molecules per cubic centimeter in the gas, we get the expression for the
growth rate,
11 N
C
hk
hk
N
F
v G
GS
GS
+
==
Y
N
C
hk
hk
N
F
v T
GS
GS
11 +
==
The growth rate at a given mole fraction is determined by the smaller of hG
or kS
. In
the limiting cases the growth rate will be given either by
[surface-reaction control]
or by
[mass-transfer control].Yk
N
C
v S
T
1
≅
Yk
N
C
v S
T
1
≅
hGY
14. 14Microelectronics Processing Course - J. Salzman - Jan. 2002
CVD growth model – Gas phase massCVD growth model – Gas phase mass
transfertransfer
The “Stagnant-film” model of
gas-phase mass-transfer
δ
SG
G
CC
DF
−
=1
δ
G
G
D
h =
Boundary layer theory: δ increases with
distance in the direction of gas flow
(from Newton’s second low).
DG – diffusivity of reactant species
δ - boundary layer thickness
15. 15Microelectronics Processing Course - J. Salzman - Jan. 2002
CVD growth model – Gas phase massCVD growth model – Gas phase mass
transfertransfer
The flow of reactants F is F ∝ DG
δ-1
16. 16Microelectronics Processing Course - J. Salzman - Jan. 2002
Tilted CVD susceptorTilted CVD susceptor
The susceptor in a horizontal epitaxial reactor is tilted so that
the cross-sectional area of the chamber is decreased,
increasing the gas velocity along the susceptor. This
compensates for both the boundary layer and depletion
effects.
17. 17Microelectronics Processing Course - J. Salzman - Jan. 2002
Áp suất cao, độ dài khuếch tán nhỏ, tốc độ phản ứng nhanh, tốc độ phát triển
màng bị giới hạn bởi sự truyền khí trong vùng biên. Dùng để kết tủa
những màng điện môi dày như silicon nitride, hạn chế của phương pháp
này là tạp.
III.1 APCVD (atmospheric pressure
CVD)
18. 18Microelectronics Processing Course - J. Salzman - Jan. 2002
• Giảm áp suất nhằm giảm các phản ứng ở pha khí không mong muốn làm cho
độ đòng đều màng tăng.
• Yêu cầu áp suất thấp chiều dài khuếch tán giảm , hgcao nên có thể điều khiển
được tốc độ phản ứng
• Có thể chế tạo màng bảo giác chất lượng tốt.
• Dùng cho điện môi và bán dẫn.
III.2 LPCVD (low pressure CVD)
Y
N
C
hk
hk
v T
GS
GS
1+
=
δ
G
G
D
h =
Recall that
and The key new point isThe key new point is total
G
P
D
1
∝
19. 19Microelectronics Processing Course - J. Salzman - Jan. 2002
Các ion khí hiếm được tăng cường bởi thế AC ( RF ) hay DC tới va
chạm với precuser tại bề mặt để tạo phản ứng.
Đưa plasma (năng lượng điện trường 1eV = 11600 K ) vào CVD để làm
ion phân ly trong plasma, dể dàng tạo phản ứng hóa học ở nhiệt độ thấp
PECVD ( đỉnh cao của CVD).
Thường dùng làm kết tủa lớp silicon nitride thụ động hóa.
III.3 PECVD (plasma-enhanced CVD)
20. 20Microelectronics Processing Course - J. Salzman - Jan. 2002
Ví dụ sử dụng quá trình CVD trong công nghệ sảnVí dụ sử dụng quá trình CVD trong công nghệ sản
xuất bán dẫn.xuất bán dẫn.
màng
Phương trình phản ứng Nhiệt độ (0
C)
SiO2
SiH4
+ O2
-> SiO2
+ 2H2
Si(OC2
H5
)4
-> SiO2
+ gas.RP
SiCl2
H2
+ N2
O -> SiO2
+ 2N2
+ 2HCl
SiH4
+ CO2
H2
-> SiO2
+ gas.RP
400-450
650-700
850-900
850-950
Si3
N4
3SiH2
Cl2
+ 4NH3
-> Si3
N4
+ 6HCl + 6H2 700-900
Polysilico
n
SiH4
-> Si + 2H2 600-650
Tungsten
2WF6
+ 3Si -> 2W + 3SiF4
WF6
+ SiH4
-> W + SiF4
+ 2HF + H2
300
400-450
22. 22Microelectronics Processing Course - J. Salzman - Jan. 2002
IV. Kiểu bình phản ứng CVD.
Bình phản ứng thành bình nóng.
Bình phản ứng thành bình lạnh.
Bình phản ứng liên tục.
Bình phản ứng CVD ghép điện plasma.
CVD bao gồm nhiều kiểu bình phản ứng và kiểu xử lý. Việc lựa chọn
kiểu bình phản ứng phụ thuộc vào ứng dụng thông qua các yêu cầu đối
với vật liệu đế, hình thái học lớp phủ độ dày và độ đồng đếu của lớp
màng.
23. 23Microelectronics Processing Course - J. Salzman - Jan. 2002
Advantages of CVD processesAdvantages of CVD processes
CVD processes are ideally suited for depositing thin layers of materials
on some substrate. In contrast to some other deposition processes
which we will encounter later, CVD layers always follow the contours of
the substrate: They are conformal to the substrate as shown below.
24. 24Microelectronics Processing Course - J. Salzman - Jan. 2002
Disadvantages of CVD processesDisadvantages of CVD processes
The two most important ones (and the only ones we will
address here) are:
1. They are not possible for some materials; there simply
is no suitable chemical reaction.
2. They are generally not suitable for mixtures of
materials.
25. 25Microelectronics Processing Course - J. Salzman - Jan. 2002
LP-CVDLP-CVD
Y
N
C
hk
hk
v T
GS
GS
1+
=
δ
G
G
D
h =
Recall that
and
The key new point isThe key new point is
total
G
P
D
1
∝
26. 26Microelectronics Processing Course - J. Salzman - Jan. 2002
Gas depletion in LPCVD reactorGas depletion in LPCVD reactor
In the surface reaction limited regime
T is critical (10
C). Ramping T compensates
depletion.
27. 27Microelectronics Processing Course - J. Salzman - Jan. 2002
Plasma enhanced CVD systemPlasma enhanced CVD system
(PECVD)(PECVD)
As the thermal budget gets more and more constrained while more
and more layers need to be added for multi-layer metallization, we
want to come down with the temperature for the oxide ( or other)
CVD processes.
One way for doing this is to supply the necessary energy for the
chemical reaction by ionizing the gas, thus forming a plasma.
28. 28Microelectronics Processing Course - J. Salzman - Jan. 2002
PECVD properties
Low substrate
temperature
Conformal film
Not stoichiometric film
By-products incorporated
Outgassing
Cracking
Peeling
29. 29Microelectronics Processing Course - J. Salzman - Jan. 2002
High Density Plasma CVD systemsHigh Density Plasma CVD systems
(HDP-CVD)(HDP-CVD)
• ECR
• ICP
A separate RF bias sputtering
planarization
30. 30Microelectronics Processing Course - J. Salzman - Jan. 2002
CVD of Si - EpitaxyCVD of Si - Epitaxy
When SiH4 gas is used in a CVD reactor, a Si layer
is deposited on the wafer surface. The size of the
crystallites depends on the deposition temperature.
At high enough temperature, the ad-atoms have
enough kinetic energy to move on the surface and
align themselves with the underlying Si.
This is an epitaxial layer, and the process is called
Epitaxy instead of CVD.
At lower deposition temperatures, the layer is
poly-crystalline Si (consisting of small crystallites)
31. 31Microelectronics Processing Course - J. Salzman - Jan. 2002
Si EpitaxySi Epitaxy
The chemical reaction that produces the
Si is fairly simple:
SiCl4(g)+2H2(g)=(1000-1200o
C)=Si(s)+4HCl(g)
Instead of SiCl4 you may want to
use SiHXCl4-X
33. 33Microelectronics Processing Course - J. Salzman - Jan. 2002
Effect of SiClEffect of SiCl44 concentration on Siconcentration on Si
depositiondeposition
Polysilicon deposition
occurs for growth rates
exceeding 2 μm/min.
Etching of the surface will
occur for mole fraction
concentrations exceeding
28%.
34. 34Microelectronics Processing Course - J. Salzman - Jan. 2002
CVD kinetic growth modelCVD kinetic growth model
Arrhenius plot of growth velocity
vs. 1/T for CVD process
Deposition rate vs. 1/T for Si deposited
by APCVD using various source gases.
Partial pressure of the reactant gas was
0.8 torr. H2 used as carrier gas for solid
curves. Using N2 as diluent shifts SiH4
curve to the right.
35. 35Microelectronics Processing Course - J. Salzman - Jan. 2002
Si epitaxy – controlling doping profilesSi epitaxy – controlling doping profiles
Epitaxy is definitely needed if a doping profile is
required where the resistivity in regions near the
surface is larger than in the bulk. By diffusion, you
can always lower the resistivity and even change the
doping type, but increasing the resistivity by diffusion
is not realistically possible.
36. 36Microelectronics Processing Course - J. Salzman - Jan. 2002
Examples for CVD Processes Used inExamples for CVD Processes Used in
Semiconductor ManufacturingSemiconductor Manufacturing
Layer Reaction equations Temperature (ºC)
SiO2
LTO
TEOS
HTO
SiH4
+ O2
-> SiO2
+ 2H2
Si(OC2
H5
)4
-> SiO2
+ gas.RP
SiCl2
H2
+ N2
O -> SiO2
+ 2N2
+ 2HCl
SiH4
+ CO2
H2
-> SiO2
+ gas.RP
400-450
650-700
850-900
850-950
Si3
N4
3SiH2
Cl2
+ 4NH3
-> Si3
N4
+ 6HCl + 6H2 700-900
Polysilico
n
SiH4
-> Si + 2H2 600-650
Tungsten
selective
blanket
2WF6
+ 3Si -> 2W + 3SiF4
WF6
+ SiH4
-> W + SiF4
+ 2HF + H2
300
400-450
37. 37Microelectronics Processing Course - J. Salzman - Jan. 2002
Oxide CVDOxide CVD
SiH2
CI2
+ 2NO2
= (900 °C) = SiO2
+ 2HCI + 2N2
There are several possibilities, one is
While this reaction was used until about 1985, a better reaction is offered by
the "TEOS" process.
Si(C2
H5
O)4
= (720 °C) = SiO2
+ 2H2
O + C2
H4
.
Si(C2
H5
O)4
has the chemical name Tetraethylorthosilicate
39. 39Microelectronics Processing Course - J. Salzman - Jan. 2002
SiSi33NN44 DepositionDeposition
•We don't "nitride" the Si, analogous to oxidations, by heating the Si in a N2
(actually we do - on occasion), because Si3
N4
is so impenetrable to almost
everything - including nitrogen - that the reaction stops after a few nm. There is
simply no way to grow a "thick" nitride layer thermally.
•Also, don't forget: Si3
N4
is always producing tremendous stress, and you don't want
to have it directly on the Si without a buffer oxide in between. In other words: We
need a CVD process for nitride.
Well, it becomes boring now:
•Take your CVD furnace from before, and use a suitable reaction, e.g.
3SiH2
Cl2
+ 4NH3
=(...o
C)= Si3
N4
+ 2HCl + 1,5 H2
.
40. 40Microelectronics Processing Course - J. Salzman - Jan. 2002
Tungsten (W) CVDTungsten (W) CVD
•Ironically, W-CVD comes straight form nuclear power technology: High
purity Uranium (chemical symbol U) is made by a CVD process using
UF6
as the gas that decomposes at high temperature.
•W is chemically very similar to U, so we use WF6
for W-CVD.
•A CVD furnace, however, is not good enough anymore. W-CVD needed
its own equipment, painfully (and expensively) developed a decade ago.
•We will not go into details, however. CVD methods, although quite
universally summarily described here, are all rather specialized and the
furnace type reactor referred to here, is more an exception than the rule.