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| United States Patent | 5464476 |
| Link to this page | http://www.wikipatents.com/5464476.html |
| Inventor(s) | Gibb; Ian (Ruislip, GB2);
Allen; Philip (Feltham, GB2);
Barnes; Andrew (Hillingdon, GB2) |
| Abstract | A plasma processing device is described which is modular and can be scaled
up by assembly together with similar devices to provide a capability for
large area processing. The device includes a housing which contains an
array of RF coils and into which a process gas is fed. The article to be
processed is disposed close to the housing and egress of the process gas
from the housing to the process region is resisted so as to maintain a
positive pressure differential between the housing and the process region. |
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Title Information  |
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| Publication Date |
November 7, 1995 |
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| Filing Date |
October 17, 1994 |
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| Priority Data |
Oct 19, 1993[GB]9321489 |
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Title Information  |
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Description  |
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This invention relates to plasma processing and, more particularly, to a
module for mounting within a process chamber (equipped with a vacuum
system) for the purpose of plasma processing of insulating materials.
Plasma processing typically involves deposition of material onto substrate
surfaces or the etching/modification of those surfaces, but can involve
other operations either additionally to or alternatively to such
operations.
It is known, for example from U.S. Pat. No. 4,948,458, that a spiral
electrode mounted on the outside of an insulating wall of a vacuum system
is suitable for performing plasma etching through inductive coupling.
However, difficulties with the scale-up to larger processing areas have
been reported due to the size of the inductance required. This is in
addition to the usual scale-up problem of process parameters depending
strongly on chamber geometry due to the effects of walls, flow patterns of
reactive gases etc. An object of this invention is to address these
problems through the use of module(s) consisting of a number of small
coils; each module being optimised for uniform plasma generation and
containing an integral gas feed supply.
Another object of this invention is to provide a plasma processing device
utilising inductive coupling which has advantages over conventional
arrangements due to its inherent modularity which allows easy scale-up
from laboratory to commercial sizes. Each module consists of several coils
arranged for plasma uniformity, with power and gas feeds.
According to the invention there is provided a plasma processing device
comprising a housing with a wall member overlying a substrate to be
operated on by means of a plasma process but separated therefrom by a
discharge gap, the device comprising a plurality of inductive coils
distributed over said wall member, means for supplying RF energy to the
coils, means for introducing a process gas into said housing and causing
said gas to flow into the discharge gap, said wall member and/or said
housing being constructed to resist the flow of said gas so as to maintain
in said housing a higher pressure of said gas than exists in said
discharge gap.
BRIEF DESCRIPTION OF DRAWINGS
FIG. 1 shows schematically an arrangement for a processing module, and
FIGS. 2, 3 and 4 show a second embodiment of the invention.
Referring to FIG. 1, the module takes the form of a box 1 installed inside
a process chamber (vacuum system), which is not shown, the box 1 being
positioned, in this case, directly above a moving flat substrate 2 which
could be glass, a plastic or another insulating material. The top of the
module contains feeds 3, 4 respectively allowing the supply of RF power
(preferably though not exclusively at a frequency of 13.56 MHz) and
process gas e.g., methane for deposition of carbon films. The module
surface closest to the substrate, termed the bottom plate 5 in the figure,
is made from an insulating material and is perforated with many small
holes such as 6 (preferably in the range 10-100 .mu.m diameter) such that
process gas passes through with difficulty and a significant pressure
differential can thus be established between the gas feed and the process
chamber (the latter preferably in the region 0.5-10 mbar). Also on the
bottom plate (inside the module) is an arrangement of conducting coils
such as 7 to which the RF power is supplied. When sufficient power is
supplied, inductively coupled discharges form in the gap 8 between the
bottom plate 5 and substrate 2 allowing plasma modification (deposition in
this example) to take place. Discharges do not form inside the module due
to the much higher gas pressure and the use of suitable insulation (not
shown) around the coils. Since the feed gas is continually being
replenished close to the source, there is little risk of exhaustion of
reactive species even at very high powers. The geometrical arrangement of
coils, i.e., size, number and pattern, and their electrical
inter-connection can be worked out empirically or theoretically for
generation of plasma exhibiting a desired degree of uniformity over the
module bottom surface.
Since each module has its own separate power and gas feed, it can be
readily perceived that many modules can be run together with little
interaction. Scale-up of any plasma process can thus be achieved by
tessellation of the appropriate number of modules. This could be a 1
dimensional (1-D) array for treating a moving sheet of any width, or a 2-D
array for a stationary object of any size. In the former case, a further
development would be the use of a 2-D array which could allow longer
exposure to the plasma (e.g., larger deposited film thickness or etch
depth) or differing processes to be carried out in series (e.g., different
materials deposited, or etching followed by deposition). Individual
control of modules allows the possibility of spatial and/or temporal
gradation in deposited film characteristics such as composition or
structure.
Other embodiments of the invention may use a bottom plate constructed of,
or including, one or more regions of a material which is inherently gas
permeable. Any RF drive circuitry or impedance matching circuits, as
understood by those skilled in the art, may also be incorporated within
the module, such that only a supply of DC or mains electricity is
necessary. Further, the box structure need not be rectangular but it may
take any convenient shape to conform with the required processing
operation.
In another embodiment, the box structure may contain baffles which resist
the flow of gas to a desired extent but do not significantly impede the
distribution of RF energy to the inductive coils such as 7. In that case
larger apertures can be used in the bottom plate 5 of the box 1.
Those skilled in the art will readily perceive various modifications to the
device shown in the drawing and described herein, and it is intended that
such modifications shall be within the scope of the present invention.
FIG. 2 shows, in cross sectional view, a large area reactor built in
accordance with the principles described previously. The plasma treatment
takes place in a vacuum chamber 11 connected, in known manner, with a
vacuum system (not shown) of a kind that will operate with a high
throughput of gas at the pressures of interest. Typically, such systems
will utilise throttled-back diffusion pumps or Roots pumps.
Multiple spiral coils 12 are positioned in an array, as described
previously, within a dielectric enclosure 13. Typically, the enclosure 13
is constructed of ceramic, glass ceramic, fused silica or quartz, although
other materials may be used.
The spiral coils 12 are supported by insulative feedthrough devices 14 and
may be cooled by means of a fluid, a typical direction of flow of which is
indicated by the arrows 15. Typical cooling fluids suitable for use in
this application are air, inert gases, water or an insulative medium such
as fluorocarbon.
Underlying each of the coils 12 and screening its radial electric fields is
a spoke like conductor configuration 16 (seen in more detail in FIG. 3).
The configurations 16 are provided in order to avoid sputtering of the
enclosure 13 which could otherwise arise as a result of ions being
accelerated by the radial fields. The conductor configurations 16 are
separated from their respective coils by dielectric sheet material 17.
Instead of the conductor configuration 16, the radial fields may be
screened by means of a structure such as that shown in FIG. 4 at 18. This
comprises a conductive material with a meandering slot to form an
interdigitated conductor arrangement. It is fitted to the underside of the
base 20 of the enclosure 13 and held at a fixed, positive potential with
respect to the plasma.
The base 20 is fitted with inserts 21 which allow a working gas, applied as
shown by the arrow 22, into the reactor chamber 11. The inserts 21 may be
formed with microscopic holes or be of a porous material such as low
density ceramic. Alternatively, as mentioned previously, the entire base
20 (or certain sections of it) may be perforated with microscopic holes.
For ease of maintenance, the enclosure 13 is demountable and sealed with a
gasket 23.
Gas is fed into the enclosure 13 via an inlet tube 24 from a gas handling
system, the line being equipped with a by-pass valve 25 to evacuate the
enclosure during the pump-down of the main reactor chamber.
The coils are supplied with radio frequency power from power
supply/matching network modules 26 which use similar techniques to
induction heaters to separate RF power and cooling fluids. Adjustment of
the power in individual coils is used to compensate for edge effects
giving an improvement in uniformity of coating or surface treatment over
the prior art.
In certain applications the reactor is fitted with a substrate platen 27
which may be cooled by fluid 28: the platen may share cooling fluids with
the coils. To enable RF or DC bias to be applied, the platen is supported
on insulators 29. A power supply 30 is used to apply RF or DC bias.
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Description  |
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