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Description  |
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BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention pertains to a method and apparatus for protecting the
conductive, typically metallic, portions of gas plasma process chambers
with a material which can be cleaned using gas plasma etching procedures.
2. Background of the Invention
The semiconductor industry relies on high throughput, single substrate
processing reactors which can be used for a variety of different processes
such as thermal chemical vapor deposition (CVD), plasma-enhanced CVD
(PECVD), plasma-assisted etching, and deposition topography modification
by sputtering. It is preferable to have such processing reactors be self
cleaning using plasma etching techniques to avoid labor-intensive manual
cleaning and loss of productivity which arise when the reactor must be
opened for cleaning.
The PECVD processing reactor chambers, which contain controlled gaseous
environments at reduced pressures, are generally constructed of aluminum,
although specialty alloys and materials such as quartz have been used at
times. Due to the broad experience of the semiconductor industry with
aluminum reaction chambers, an understanding of the effect of the presence
of the aluminum upon products produced in the reactors has been developed.
Thus, those working in the industry are comfortable with the use of
aluminum reaction chambers. However, as described in U.S. Pat. No.
4,563,367 to Sherman, plasma-assisted chemical vapor deposition processes
tend to form deposits on internal surfaces of the reaction chambers so
that the surface of the aluminum reaction chambers must be periodically
cleaned.
This periodic cleaning can be done by disassembling the chamber and
immersing the chamber parts in a wet chemical etchant bath or by
mechanically cleaning the chamber parts. However, these methods are time
consuming and may produce yield-decreasing particulates and contaminants.
An alternative to these methods is a self-cleaning reactor system, wherein
the reaction system plasma electrodes or coils are used to generate an
etching plasma which does the cleaning. Typically an etching plasma
generated from CF.sub.4 and O.sub.2 is used to clean the reactor chamber.
However, it has been discovered that after several plasma cleaning
sequences, reactor system performance frequently degrades to the point
that non-uniform depositions on semiconductor wafers occur. Investigation
of the possible causes of this performance degradation led to the
discovery that aluminum trifluoride (AlF.sub.3) crystallized on the bare
aluminum upper electrode of the reactor system during standard plasma
self-cleaning. One theory of causation was that the deposits resulted from
ion bombardment by active fluorine species in the high RF field which was
applied between the electrodes during the plasma self-cleaning process. It
was further theorized that the fluorine destroyed the natural oxide
protective coating on the bare aluminum of the upper electrode and that
the AlF.sub.3 deposits formed during the plasma self-cleaning cycles.
Sherman concluded that use of a small, enclosed plasma generation chamber
within a conventional semiconductor-processing vacuum chamber controlled
certain highly active species within the generation chamber, enabling the
use of increased RF power (higher plasma etching rates) without damage to
the conventional semiconductor-processing vacuum chamber. Thus, higher
semiconductor-processing etch rates should be possible without increasing
the required frequency of wet chemical cleaning of the conventional
processing vacuum chamber. The small, enclosed plasma generation chamber
is constructed from a ceramic material such as aluminum oxide. He said
that the conventional processing vacuum chamber could be constructed with
either metallic or ceramic walls, but he stated no preference. Another
attempt to reduce the formation of deposits on CVD reaction chamber walls
is described in U.S. Pat. No. 4,875,989 to Davis et al. Davis et al.
describe the use of a conical baffle which is in proximity to the wafer
face, to direct the stream of activated species. The conical baffle is
fabricated from aluminum which is anodized over its entire surface except
for its base.
U.S. Pat. No. 4,960,488 to Law et al., issued Oct. 2, 1990, describes a
process for cleaning a reactor chamber, both locally adjacent to the RF
electrodes and also throughout the chamber and exhaust system. Preferably,
a two-step continuous etch sequence is used in which the first step uses
relatively high pressure, close electrode spacing and fluorocarbon gas
chemistry.. The second step uses relatively lower pressure, farther
electrode spacing and fluoride gas chemistry. Typically, an etch gas
mixture of C.sub.2 F.sub.6 and O.sub.2 is used for the first cleaning
step, and NF.sub.3 is used as the etch gas for second cleaning step. To
avoid the formation of contaminant compounds, which occurs when
halogen-containing plasmas contact aluminum reactor chamber walls during
etch cleaning and to reduce the amount of etch cleaning necessary, the
reactor chamber is designed to have spacing between elements which reduces
the opportunity for active CVD species to deposit on chamber walls outside
the wafer area. In addition, particular surfaces inside the process
chamber are temperature controlled to reduce gas decomposition, or
condensation on chamber walls and the reactor is designed to have purging
gas flow to prevent deposition of CVD materials outside the wafer area.
In a further attempt to protect the aluminum reactor chamber from attack by
fluorine-containing gases, Lorimer et al. developed a method of forming a
corrosion-resistant protective coating on an aluminum substrate, as
described in U.S. Pat. No. 5,069,938. The protective coating is formed by
first forming a high purity aluminum oxide layer on an aluminum substrate
and then contacting the aluminum oxide layer with one or more high purity
fluorine-containing gases at elevated temperature. The aluminum oxide
layer may be either a thermally formed layer or an anodically formed layer
having a thickness from at least about 0.1 micrometer up to about 20
micrometers. The preferred fluorine-containing gases will comprise acid
vapors. Examples of fluorine-containing gases include gaseous HF, F.sub.2,
NF.sub.3, CF.sub.4, CHF.sub.3, and C.sub.2 F.sub.6. As is evidenced by the
process and the description of the finished coating, the
fluoride-containing gas penetrated the aluminum oxide (possibly to the
aluminum surface beneath) to form fluorine-containing compounds within.
The protective coating of Lorimer et al. is intended to protect the
chamber walls of the processing apparatus from the chemicals used in
chemical vapor deposition and etching processes. However, applicants have
determined that a thermal or anodized aluminum oxide coating of 20
micrometers or less on an aluminum surface does not prevent the gradual
build up of fluoride-containing compounds such as aluminum trifluoride
(AlF.sub.3), ammonium fluoride (NH.sub.4 F), and aluminum oxyfluorides
(AlO.sub.x F.sub.y) upon the outer surface of the coating. These compounds
eventually peel off from the surface of the coating and become a source of
particulate contamination.
As can be seen from the above descriptions, the semiconductor industry
would find it highly desirable to have a means of preventing the build up
of deposits on aluminum process reaction chambers. Build up must be
prevented even when the process reactor chamber is designed to limit
plasma operational areas to the minimum space possible within the reactor,
with a spacing between reactor elements which reduces the opportunity for
active CVD species to deposit on chamber walls outside the wafer area.
There has been heightened interest in liquid crystal displays in recent
years, in particular for flat panel displays such as computer display
screens, direct view and projection television screens, and navigation and
communication instruments. Such liquid crystal flat panel displays utilize
the kinds of materials and physical structures generally present in
semiconductor devices. Many of the processes required to fabricate the
liquid crystal displays are the same processes as those used to produce
semiconductor devices. Thus, semiconductor process equipment is presently
being modified for use in the production of such flat panel displays. For
many of the process steps, plasma-assisted CVD and plasma etching is
utilized. Typically the substrate to be processed is positioned on a
lower, grounded platen electrode, while the RF power is applied to the
upper electrode. The reactant gases are discharged in the region of the
upper electrode and a plasma forms between the two electrodes. Because the
rectangular flat panel display substrates are very large by comparison to
silicon wafers (up to 360.times.4.50 mm flat panels compared to 200 mm
maximum diameter for silicon wafers), it is impractical to make the
process reaction chamber very much larger than the plasma zone. The close
proximity of the reactor chamber walls to the plasma zone increases the
amount of deposition on the chamber walls and increases the possibility
for arcing between the platen electrode and the chamber walls.
The build up of deposition on reaction chamber walls is critically
important since flat panel displays are as sensitive to particulate
contamination because they include semiconductor devices with submicron
geometries. The flat panel design geometries, that is, lateral dimension,
are typically large, in the range of 5 to 20 .mu.m. However, the device
layers, that is, vertical dimension, are thin, in the range of 0.03 to 0.3
.mu.m, so the presence of small particles can cause electrical leakage
currents which can cause a pixel or row of pixels to fail. Also,
considering that a display may have 1,000.times.1,000 lines, there are one
million pixels being controlled by active semiconductor transistors.
Further, since the substrate for liquid crystal display panels is typically
glass, an insulating material, there is an increased tendency for the
plasma to expand toward the chamber walls and for arcing to occur between
the platen electrode (suceptor) on which the glass substrate is supported
and the aluminum walls of the process reactor chamber.
Thus, it is important in the production of semiconductor substrates, and
particularly flat panel liquid crystal displays, to develop means for: 1)
confining plasma exposure boundaries, thereby reducing the formation of
deposits on the reactor chamber walls; 2) cleaning the reactor walls in a
manner which does not cause a gradual build up of contaminants on the
reactor walls; and 3) preventing arcing from the plasma-generating
electrodes to conductive reactor chamber surfaces.
SUMMARY OF THE INVENTION
In accordance with the present invention, a ceramic barrier material is
used to protect conductive, typically metallic, surfaces of a process
reactor chamber which have the potential of becoming contaminated during
plasma processing. The ceramic barrier material is selected to be a good
insulator, so that a charge builds up on the surface of the ceramic
barrier material. This charge build up is approximately equal to the
plasma potential which is typically, for example, less than about 20
volts. This charge build up helps repel the plasma away from the surface
of the ceramic barrier material, thereby confining the plasma and greatly
reducing deposits formed on the reactor chamber walls. In addition, it has
further been discovered that such a ceramic barrier material can be
cleaned using fluoride-containing etch gases without the build up of
contaminants upon the ceramic which can later become a source of
particulate contamination.
Further, it is well established that process chambers should be as small in
volume as possible in order to minimize the time required to change
pressure and thereby maximize productivity. Therefore the chamber walls
should be as close to the electrodes as possible. Because the chamber is
only slightly larger than the susceptor, the ceramic barrier material
prevents arcing (or intense discharges) between the susceptor and the
nearby conductive surfaces of the reactor chamber.
The ceramic barrier material need not shield the entire inner surface of
the process reactor chamber, but it should protect rector chamber surfaces
surrounding the area in which plasma will be generated. In addition, it is
preferred that the ceramic liner protect reactor chamber surfaces likely
to be exposed to plasma etch cleaning processing.
The ceramic barrier material typically comprises aluminum oxide since this
is relatively inexpensive and readily available. The aluminum oxide must
be sufficiently pure that it does not "out-gas" or include contaminants
that could be sputtered onto the substrate during process operation, and
it must be chemically stable when exposed to the particular etching
processes contemplated. The aluminum oxide or other metal-oxide ceramic
can be a single crystal oxide, polycrystalline oxide, or amorphous oxide.
Flame sprayed or plasma sprayed aluminum oxide can also be used to form
the ceramic barrier.
Other materials which can be used to form the ceramic liner include by way
of illustration., but are not limited to, the oxide and fluoride forms of
aluminum, magnesium, and tantalum.
The thickness of the ceramic barrier material is typically at least about
0.005 inches (130 micrometers), and preferably ranges from about 0.01
inches (250 micrometers) to about 0.25 inches (6.4 millimeters).
BRIEF DESCRIPTION OF THE DRAWINGS
FIGS. 1A & 1B illustrate a widely used prior art combined CVD and
plasma-enhanced CVD (PECVD) semiconductor processing reactor. FIG. 1A
shows a vertical cross-section of the reactor, partly in schematic. This
cross-sectional view makes the relative structural locations of the
various reactor elements clear. FIG. 1B shows the top plan view of the
same reactor, shown with the cover open. These illustrations, from U.S.
Pat. No. 4,960,488, to Law et al. are presented to provide an improved
understanding of the structural relationship between the plasma processing
areas of the reactor and the reactor chamber walls which can be
contaminated by active species from the plasma.
FIGS. 2A and 2B illustrate a preferred embodiment of the present invention
as employed in a CVD and PECVD semiconductor processing reactor. FIG. 2A
shows a simplified schematic of a vertical cross section of a combined
CVD/PECVD reactor of the kind used to fabricate flat panel liquid crystal
displays. FIG. 2B shows a top plan view of a combined CVD/PECVD reactor.
The reactor is shown with the cover open.
DETAILED DESCRIPTION OF THE PRESENT INVENTION
In accordance with the present invention, a method and apparatus are
provided for use in CVD, PECVD, and other types of process chambers which:
1) confine plasma exposure boundaries, thereby reducing the formation of
deposits on process chamber walls;
2) enable etch cleaning of reactor walls in a manner which does not cause a
gradual build up of contaminants on process chamber walls; and
3) prevent arcing from plasma-generating electrodes within the CVD process
chamber to conductive reaction chamber surfaces.
In particular, this method and apparatus enable the operation of
plasma-enhanced chemical vapor deposition processes within the reactor
chamber with reduced film deposition upon reactor chamber walls. Further,
the reactor chamber can be periodically cleaned using halogen-containing
(typically fluorine-containing) gas and plasma etching techniques, without
a film residue forming upon reactor chamber walls.
In accordance with the present invention, CVD and/or PECVD process chamber
walls which are significantly exposed to active species during plasma
processing or cleaning operations are lined with a relatively thick,
electrically insulating ceramic barrier material.
A prior art combined CVD and PECVD semiconductor processing reactor is
shown in FIGS. 1A & 1B. A vertical cross-sectional schematic of the
processing reactor is shown in FIG. 1A, with a top plan view shown in FIG.
1B. The top plan view is shown with the cover open. The reactor system 10
comprises a housing 12 (also termed a "chamber"), typically made of
aluminum, which defines an inner vacuum chamber 13 that has a plasma
processing region 14.
The reactor system 10 includes a wafer-holding susceptor 16, wafer support
fingers 20, and a wafer transport system 18 which cooperates with an
external robotic blade 24. The reactor system 10 further comprises a gas
manifold (not shown), which applies process gas and purging gas from a
distribution system 32 present within housing cover 80. An RF power supply
and matching network 28 create and sustain a process gas plasma from the
inlet gas while a lamp heating system 30, passes radiation through quartz
window 70 and heats the susceptor 16 and wafer 15 positioned thereon, to
effect deposition of active species from the plasma onto the wafer 15.
The plasma processing region 14 is significantly limited in area.
Preferably in addition, a second purge gas manifold 112 is positioned
beneath the wafer processing area to provide purge gas flow 103 upwardly
across the bottom of the susceptor 16. Such purge gas flow 103, in
combination with gas flow 105 from the distribution system 32 (including
apertured manifold face plate 92) is used to help prevent depositions from
the plasma from accumulating in general on surfaces in reactor chamber 13
and particularly on surfaces beneath the susceptor 16.
Despite the actions taken to prevent CVD accumulations upon chamber walls
of the process reactor, problems with such depositions have not been
eliminated, and reactor cleaning must be conducted periodically.
Plasma-assisted etching is the preferred method of cleaning, since this
reduces the danger of particles contaminating the reactor. Since the
reactor chamber walls are typically aluminum, which is directly attacked
by chlorine gas plasmas comprising, fluorine gas plasmas are commonly used
for plasma-assisted etch cleaning. However, as previously described, this
results in the gradual build up of on the aluminum walls of aluminum
trifluoride deposits, which can flake off, providing particulate
contaminants within the process reactor chamber.
The process reactor used in fabrication of liquid-crystal, flat-panel
displays has many features common to the semiconductor processing reactor
described above. However, the flat-panel displays are generally
rectangular so that the top plan view of the reactor, with the cover open,
would appear as shown in FIG. 2B. With reference to FIGS. 2A and 2B, which
show a reactor system 200, a rectangular flat-panel display glass
substrate 215 sits upon a raised step of a rectangular suceptor 216. A
display-panel substrate transport system 218 cooperates with a normally
external robotic arm 224 to move glass substrates 215 into and out of an
inner vacuum chamber 213 of the reactor 200. The inner vacuum chamber 213
is encompassed by reactor housing (or chamber) 212 including a hinged lid.
The reactor system 200 further comprises a gas manifold within the lid
which applies process gas and purging gas from a distribution system 232
above the substrate 215. A rectangular face plate 292 having hundreds of
orifices 293 applies process gas and purge gas to the substrate 215. An RF
power supply and matching network 228 create and sustain a process gas
plasma from the inlet gas issuing from the face plate 292. This process
gas plasma is principally contained in a plasma processing region 214
above the substrate 215. However, due to the size of the insulating glass
substrate 215 relative to the reactor housing 212, there would, without
benefit of the present invention, be a tendency for the plasma to migrate
toward the reactor housing 212. There would also be a tendency for the
plasma to form in the space beneath the susceptor 216 and for arcing to
occur between the susceptor 216 and the lower side walls of the reactor
housing 212. These last effects arise because the susceptor 216 is
imperfectly grounded through its sliding shaft 230 to the reactor housing
212.
Without the method and apparatus of the present invention, the plasma
formed in the plasma processing region 214 migrates towards the aluminum
reactor housing 212, leaving deposits on the walls of this process/reactor
chamber which would otherwise need to be periodically cleaned using
fluoride gas plasma etching. As previously discussed, this results in the
reactor chamber walls having film residue made of aluminum fluoride and
other compounds which build up and flake off, causing particulate
contamination within the reactor chamber.
Those skilled in the art have used ceramic components for particular
elements within semiconductor processing reactors for a number of years. A
ceramic is a metal oxide that is typically electrically insulating and the
crystallinity of which varies among amorphous, glassy, microcrystalline,
and singly crystalline, dependent on material and its processing.
Applicants, for example, have used an alumina baffle to deflect active
species from the electrode plate of a plasma-assisted CVD reactor, in an
attempt to avoid the formation of deposits upon the electrode plate.
Sherman has used a small, enclosed plasma generation chamber of aluminum
oxide, as previously discussed.
Anodized aluminum has been widely used for baffles and elements in the area
of the electrodes of the plasma generator. However, an anodized surface of
aluminum is electrically leaky permitting current leakage to a conductive
aluminum beneath and, therefore, attraction of plasma toward the anodized
aluminum surface. Thus, anodized aluminum does not significantly act to
confine the plasma and does not sufficiently aid in reducing arcing from a
plasma-generating electrode toward the anodized aluminum surface. In all
of the known art cases it was still necessary to clean deposit build-up
off the aluminum walls of the reaction chamber and such cleaning resulted
in the formation of aluminum-comprising deposits which eventually
contributed a source of particulates to the reaction chamber.
The characteristic that distinguishes anodized aluminum from ceramic
alumina for this application is the two layer structure of the anodized
aluminum compared to the nearly homogenous structure for bulk or deposited
alumina. The top layer of anodized aluminum is porous and has poor
electrical insulation properties. This layer has a high degree of
contamination (H.sub.2 O, SO.sub.3, Cr or other species) from the
anodizing process and reacts chemically differently from the pure
material. Channels extend vertically through the top layer to within a few
hundred angstroms of the underlying aluminum affording passage for an
electrically conductive plasma so that only the bottom layer of 200
angstroms or so acts as an electrical barrier to the plasma. The bottom
layer is the barrier layer which is a good electrical insulator and is a
more dense, pure aluminum oxide. Typically anodized aluminum total
thickness is limited to less than 0.005 inches (approximately 130
micrometers) of which only a few hundred angstroms (hundredths of
micrometers) are the barrier layer.
The ceramic material of the present invention is a non-porous, homogeneous
material. It is a good electrical insulator, and because it can be made in
a relatively pure form (approximately 99% or better) it has a low degree
of chemical reactivity in the plasma environment. The bulk, free standing
ceramic material typically :has a thickness of at least 0.005 inches
(approximately 127 micrometers) and preferably has a thickness ranging
between 0.01 inches (approximately 250 micrometers) and 0.25 inches (6,350
micrometers).
Applicants have discovered that when ceramic such as aluminum oxide is
cleaned with etch plasmas formed from fluoride-containing gas, no build up
of aluminum trifluoride occurs. Thus, a reactor of aluminum oxide can be
cleaned using standard etch plasma techniques without the formation of
particulates. However, aluminum oxide being impractical as a reactor
fabrication material in itself, applicants prefer to use this material as
a barrier material, typically a liner, to protect a metallic reactor wall.
Applicants discovered that it is preferable to have an aluminum oxide
thickness of at least 0,005 inches (approximately equals to 130
micrometers) to confine the deposition plasma and to prevent the
fluoride-comprising plasma etch gas from penetrating the ceramic barrier
to the aluminum surface being protected beneath. Thus, a coating of lesser
thickness may not enable the satisfactory cleaning of plasma process
chambers using known plasma etching procedures.
As shown for the embodiment of FIG. 2A, a set of ceramic liners 220, 221,
and 222 are placed adjacent to the aluminum housing 212. These liners 220,
221, and 222 are machined from solid alumina of high purity (99%) and
hence are highly insulating, whether at DC, RF, or in the presence of a
plasma. The importance of high purity aluminum oxide is discussed by
Lorimer et. al. Since they are machined into :free standing form, they
should have a minimum thickness of 130 micrometers (0,005 inch). Such a
thickness more than adequately provides the desired resistance. A
similarly sized and insulative ceramic annulus 223 is attached to the
periphery of the face plate 292. Such an annulus 223 has been previously
used to provide electrical insulation and support for the face plate 292,
which is electrically connected to the RF source 228, and to protect a
Teflon insulator 294 at its back; however, it additionally provides many
of the same advantages as the ceramic liners 220, 221, and 222. The bottom
surface of the face plate 292 is typically anodized.
The insulative upper ceramic liners 221 and 222 and ceramic annulus 217
repel a plasma and thus confine the processing plasma to a processing
region more closely adjacent to the substrate 215, thereby decreasing
deposits on the walls of the chamber housing 212 and also increasing
processing efficiency. The lower ceramic liner 220 electrically isolates
the susceptor 216, which is partially floating electrically, from the
grounded chamber housing 212. It prevents arcing between the periphery of
the susceptor 216 and the chamber housing 212 and also prevents the
formation of a plasma beneath the susceptor 216. Although it might be
preferable to additionally cover the bottom of the inner vacuum chamber
213 with another alumina liner, this appears to be unnecessary because the
disc forming the major part of the transport system 218 is a bulk ceramic
and because the primarily aluminum susceptor 216 is supported on its
bottom by another ceramic disc.
The ceramic liners 220, 221, and 222 and ceramic annulus 223 prevent the
build up of deposits upon the surface of the chamber housing 212 during
general PECVD processing. Deposits which do build up on these ceramic
members 220-222 as well as on the anodized bottom surface of the face
plate 292 can be cleaned off using standard plasma etching techniques
without the need for wet chemical cleaning, which causes the formation of
compounds the particulates of which contaminate the inner vacuum chamber
213.
Although free-standing liners have been described above, ceramic layers
which are deposited without consuming the underlying aluminum may be made
having sufficient thickness and resistivity so as to provide the
advantages of bulk alumina without the disadvantages of anodized aluminum
surfaces. For example, | | |