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Claims  |
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What is claimed is:
1. A plasma treating method comprising the steps of:
rendering a gas having a critical potential plasmic under a reduced
pressure, said critical potential being a potential at which an etching
action and a deposition action are in equilibrium with each other when a
sample is treated with the plasma which is generated by rendering a
certain kind of gas plasmic under a predetermined plasma condition and
applying an acceleration voltage to ions in said plasma so as to let them
be incident to said sample; and
changing said acceleration voltage for accelerating said ions in said
plasma towards said sample interposing said critical potential.
2. A plasma treating method according to claim 1, wherein said acceleration
voltage is provided by the combination of a D.C voltage and a radio
frequency voltage with a frequency having a half cycle time within the
time required by said ions in said plasma to pass through an ion sheath.
3. A plasma treating method according to claim 1, wherein said acceleration
voltage is provided by a radio frequency voltage with a frequency having a
half cycle time from 100 KHz to above the time required by said ions in
said plasma to pass through an ion sheath.
4. A plasma treating method according to claim 1, wherein said acceleration
voltage is provided by the combination of an A.C. voltage with a low
frequency and a radio frequency voltage with a frequency having a half
cycle time within the time required by said ions in said plasma to pass
through an ion sheath.
5. A plasma treating method according to claim 1, wherein said acceleration
voltage is provided by a D.C. voltage.
6. A plasma treating method according to claim 1, wherein said acceleration
voltage is a voltage to be applied to a sample table for said sample or a
voltage to be applied to a grid electrode disposed between said sample and
said plasma.
7. A plasma treating method according to claim 1, wherein said acceleration
voltage is changed in such a manner as to interpose said critical
potential and is changed, too, during the etching operation.
8. A plasma treating method comprising the steps of:
rending a gas having a critical potential plasmic under a reduced pressure,
said critical potential being a potential at which an etching action and a
deposition action are in equilibrium with each other when a sample is
treated with the plasma which is generated by rendering a certain kind of
gas plasmic under a predetermined plasma condition and applying an
acceleration voltage to ions in said plasma so as to let them be incident
to said sample; and
changing said acceleration voltage for accelerating ions in said plasma
towards said sample interposing said critical potential and stepwise
etching said sample in the direction of depth by carrying out alternately
said etching action and said deposition action.
9. A plasma treating method according to claim 8, wherein said etching
action takes place within the time at which undercut occurring on said
sample is within a range of allowable values and said deposition action
takes place within the time at which a film can be formed to a film
thickness sufficient to act as a protective film on side surfaces of said
sample.
10. A plasma treating method according to claim 8, wherein said gas is
either a single gas of C.sub.2 Cl.sub.3 F.sub.3, C.sub.2 Cl.sub.4 F.sub.2,
CCl.sub.4 or C.sub.4 F.sub.8 or its mixed gas with SF.sub.6 or NF.sub.3
when said sample is polysilicon, and said gas is either a single gas of
CCl.sub.4, CF.sub.4, C.sub.2 F.sub.6, C.sub.4 F.sub.8 or SiCl.sub.4 or its
mixed gas with Cl.sub.2 when said sample is aluminum.
11. A plasma treating apparatus comprising:
means for rending a gas having a critical potential plasmic under a reduced
pressure, said critical potential being a potential at which an etching
action and a deposition action are in equilibrium with each other when a
sample is treated with the plasma which is generated by rendering a
certain kind of gas plasmic under a predetermined plasma condition and
applying an acceleration voltage to ions in said plasma so as to let them
be incident to said sample; and
means for changing said acceleration voltage for accelerating said ions in
said plasma towards said sample interposing said critical potential.
12. A plasma treating apparatus according to claim 11, wherein said
acceleration voltage is provided by a D.C. power source and a radio
frequency power source with a frequency having a half cycle time within
the time required by said ions in said plasma to pass through an ion
sheath.
13. A plasma treating apparatus according to claim 11, wherein said
acceleration voltage is provided by a radio frequency power source with a
frequency having a half cycle time from 100 KHz to above the time required
by said ions in said plasma to pass through an ion sheath.
14. A plasma treating apparatus according to claim 11, wherein said
acceleration voltage is provided by an A.C. power supply with a low
frequency and a radio frequency power source with a frequency having a
half cycle time within the time required by said ions in said plasma to
pass through an ion sheath.
15. A plasma treating apparatus according to claim 11, wherein said
acceleration voltage is provided by a D.C. power source.
16. A plasma treating apparatus according to claim 11, wherein said
acceleration voltage is provided by a power source applied to a sample
table of said sample or a power source applied to a grid electrode
disposed between said sample and said plasma.
17. A plasma treating apparatus according to claim 11, wherein said
acceleration voltage is changed in such a manner as to interpose said
critical potential and is changed, too, during the etching operation.
18. A plasma treating apparatus comprising:
means for rendering a gas having a critical potential plasmic under a
reduced pressure, said critical potential being a potential at which an
etching action and a deposition action are in equilibrium with each other
when a sample is treated with the plasma which is generated by rendering a
certain kind of gas plasmic under a predetermined plasma condition and
applying an acceleration voltage to ions in said plasma so as to let them
be incident to said sample; and
means for changing said acceleration voltage for accelerating ions in said
plasma towards said sample interposing said critical potential and
carrying out alternately said etching action and said deposition action.
19. A plasma treating apparatus according to claim 18, wherein said gas is
either a single gas of C.sub.2 Cl.sub.3 F.sub.3, C.sub.2 Cl.sub.4 F.sub.2,
CCl.sub.4 or C.sub.4 F.sub.8 or its mixed gas with SF.sub.6 or NF.sub.3
when said sample is polysilicon, and said gas is either a single gas of
CCl.sub.4, CF.sub.4, C.sub.2 F.sub.6, C.sub.4 F.sub.8 or SiCl.sub.4 or its
mixed gas with Cl.sub.2 when said sample is aluminum.
20. A plasma treating apparatus comprising:
means for rendering a gas having a critical potential plasmic under a
reduced pressure by use of the action of an electric field by microwaves
and the action of a magnetic field by magnetic field generation means,
said critical potential being a potential at which an etching action and a
deposition action are in equilibrium with each other when a sample is
treated with the plasma which is generated by rendering a certain kind of
gas plasmic under a predetermined plasma condition and applying an
acceleration voltage to ions in said plasma so as to let thm be incident
to said sample;
means for applying said acceleration voltage to a sample table on which
said sample is placed; and
means for changing said acceleration voltage interposing said critical
potential.
21. A plasma treating apparatus comprising:
a vacuum treating vessel having a discharge tube disposed at an upper
opening thereof;
a discharge space within said discharge tube;
a waveguide disposed so as to encircle said discharge tube, said waveguide
including a magnetron for generating microwaves;
an electromagnetic coil disposed around the outer periphery of said
discharge tube through said waveguide;
an electrode including a sample table disposed within said vacuum treating
vessel so as to allow support of a sample to be treated in said discharge
space;
a ground electrode disposed around the outer periphery of said electrode
and electrically insulated therefrom;
means to introduce gas into said discharge space, said gas having a
critical potential at which an etching action and a deposition action of
said gas are in equilibrium; and
means to control an acceleration voltage connected to said electrode, for
accelerating ions in a plasma of said gas, so as to alternately etch and
deposit said sample.
22. A plasma treating apparatus according to claim 21, wherein said means
to control an acceleration voltage, comprises:
a radio frequency power source for supplying radio frequency voltage to
said electrode, connected to said electrode through a matching box;
a D.C. power source for supplying D.C. voltage to said electrode, connected
to said electrode through a lower pass filter;
an output voltage controller connected to said D.C. power source; and
an output waveform controller connected to said output voltage controller.
23. A plasma treating apparatus according to claim 21, wherein said means
to control an acceleration voltage, comprises:
a radio frequency power source connected to said electrode through a
matching box; and
an output voltage control means connected to said radio frequency power
source.
24. A plasma treating apparatus according to claim 21, wherein said means
to control an acceleration voltage, comprises:
a radio frequency power source connected to said electrode through a
synthesizer;
an A.C. waveform generator connected to said synthesizer; and
an output waveform controller connected to said A.C. waveform generator.
25. A plasma treating apparatus comprising:
a vacuum treating vessel having a discharge tube disposed at an upper
opening thereof;
a discharge space within said discharge tube;
a waveguide disposed so as to encircle said discharge tube, said waveguide
including a magnetron for generating microwaves;
an electromagnetic coil disposed around the outer periphery of said
discharge tube through said waveguide;
an electrode including a sample table disposed within said vacuum treating
vessel so as to allow support of a sample to be treated in said discharge
space;
means to introduce gas into said discharge space, said gas having a
critical potential at which at etching action and a deposition action of
said gas are in equilibrium;
means to control an acceleration voltage for accelerating ions in a plasma
of said gas, so as to alternately etch and deposit said sample;
said means to control acceleration voltage including a grid electrode
disposed in said discharge space above said sample, D.C. power source
connected to said grid electrode, an output voltage controller connected
to said D.C. power source, and an output waveform controller connected to
said output voltage controller.
26. A plasma treating apparatus comprising:
a vacuum treating vessel having a gas injection port;
an upper electrode disposed in an upper portion of said vacuum treating
vessel;
a lower electrode for supporting a sample to be treated, disposed in a
lower portion of said vacuum treating vessel so as to face said upper
electrode, said lower electrode being insulated from said vacuum treating
vessel;
means to introduce gas into said vacuum treating vessel through said
injection port, said gas having a critical potential at which an etching
action and a deposition action of said gas are in equilibrium; and
means to control an acceleration voltage connected to said lower electrode
for accelerating ions in a plasma of said gas, so as to alternately etch
and deposit said sample.
27. A plasma treating apparatus according to claim 26, wherein said means
to control an acceleration voltage, comprises:
a radio frequency power for supplying radio frequency voltage to said lower
electrode, connected to said lower electrode through a matching box;
a D.C. power source for supplying D.C. voltage to said lower electrode,
connected to said lower electrode through a low-pass filter;
an output voltage controller connected to said D.C. power source; and
an output waveform controller connected to said output voltage controller.
28. A plasma treating apparatus according to claim 25, wherein said means
to control an acceleration voltage, comprises:
a radio frequency power connected to said lower electrode through a
matching box; and
an output voltage control means connected to said radio frequency power
source.
29. A plasma treating apparatus according to claim 26, wherein said means
to control an acceleration voltage, comprises:
a radio frequency power source connected to said lower electrode through a
synthesizer;
an A.C. waveform generator connected to said synthesizer; and
an output waveform controller connected to said A.C. waveform generator.
30. A plasma treating apparatus according to claim 26, wherein said means
to control an acceleration voltage, comprises:
a radio frequency power source connected to said lower electrode through a
matching box and a capacitor; and
an output voltage control means connected to said radio frequency power
source.
31. A plasma treating apparatus according to claim 26, wherein said means
to introduce gas includes a discharge tube connected to said injection
port and a coil wound around a periphery of said discharge tube and
connected to a radio frequency power source.
32. A plasma treating apparatus comprising:
a vacuum treating vessel having a gas injection port;
an upper electrode disposed in an upper portion of said vacuum treating
vessel;
a lower electrode for supporting a sample to be treated, disposed in a
lower portion of said vacuum treating vessel so as to face said upper
electrode, said lower electrode being insulated from said vacuum treating
vessel;
means to introduce gas into said vacuum treating vessel through said
injection port, said gas having a critical potential at which an etching
action and a deposition action of said gas are in equilibrium; and
means to control an acceleration voltage for accelerating ions in a plasma
of said gas, so as to alternately etch and deposit said sample, said means
to control an acceleration voltage including a grid electrode disposed in
said vacuum treating vessel above said sample, a D.C. power source
connected to said grid electrode, an output voltage controller connected
to said D.C. power source, an output waveform controller connected to said
output voltage controller, and a radio frequency power source connected to
said lower electrode through a matching box. |
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Claims  |
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Description  |
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BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates to a plasma treating method and apparatus therefor,
and more particularly to a plasma treating method and apparatus therefor
which will be suitable for carrying out the treatment by effecting
alternately etching and deposition.
2. Description of the Prior Art
With a progress in miniaturization of semiconductor devices, dimensional
machining accuracy of circuit patterns and a low damage machining method
have become more and more important. Particularly in devices of a
submicron range, the device structure has become three-dimensional owing
to limitation to a chip area. For this reason, it has become necessary to
form a film having a large ratio of a machining depth to a machining
width, that is, an aspect ratio, with high dimensional accuracy.
An example of prior art techniques for satisfying such a requirement is
disclosed in Japanese Patent Laid-Open No. 50923/1985, for example. This
prior art technique uses a mixed gas consisting of an SF.sub.6 gas which
contributes to etching, an N.sub.2 gas which contributes to the formation
of a protective film of silicon nitride and other gases as an etching gas
for etching poly-Si, and changes periodically the composition and
concentration of the treating gas during the etching treatment. In this
manner, this prior art technique carries out etching at a high speed and
with high dimensional accuracy by repeating alternately the etching step
and the formation step of the silicon nitride protective film.
Since the prior art technique carries out the etching treatment by changing
the gas composition and concentration, however, the condition of plasma
changes whenever the gas composition and concentration are changed. When
the gas composition and concentration are changed, a previous plasma
condition is changed to a new plasma condition. In other words, any
remaining ions and radicals must be exhausted rapidly. Since a treating
vessel has a certain inner capacity, a certain period of time is necessary
before the plasma condition is changed over so that the overall treating
time becomes elongated. If this problem is to be somewhat alleviated, an
exhaust device becomes greater in size to reduce the exhaust time. In
addition, it becomes necessary to control the exhaust quantity during the
treatment and the exhaust quantity at the time of change-over so that a
controller and control technique become complicated.
On the other hand, a technique which changes the voltage to be impressed
upon an electrode is disclosed in Japanese Patent Publication No.
41132/1986, Japanese Patent Laid-open No. 13625/1986, and the like. These
prior arts carry out the plasma treatment by changing the voltage to be
applied to the electrode, and merely improve plasma characteristics such
as an etching rate, a selection ratio, and the like, by controlling the
incidence energy of ions in the plasma.
SUMMARY OF THE INVENTION
It is therefore an object of the present invention to provide a plasma
treating method and apparatus therefor which carries out alternately the
etching step and the film formation step and can shorten the plasma
treating time without changing over the treating gas.
As a result of intensive studies and experiments, the inventors of the
present invention have found out for the first time the following
observation as the basis of the present invention. A certain kind of
component gas is rendered plasmic under a predetermined plasma condition.
An acceleration voltage is applied to ions inside this plasma and arranged
in such a manner that the ions are incident to a sample. The present
invention treats the sample by use of such a plasma. The inventors of the
invention have found out that if the value of the acceleration voltage is
changed in this case, there exist a voltage at which the etching action
occurs preferentially and a voltage at which the deposition action occurs
preferentially. It has been found also that there is a voltage at which
the etching action is in equilibrium with the deposition action.
Hereinafter, this equilibrium voltage will be referred to as a "critical
potential".
Namely, the present invention provides an apparatus comprising means for
rendering plasmic a gas having a critical potential under a reduced
pressure and means for changing an acceleration voltage for accelerating
ions in the plasma towards a sample while interposing the critical
potential, and a treating method including a step of rendering plasmic a
gas having a critical potential under a reduced pressure and a step of
changing an acceleration voltage for accelerating ions in the plasma
towards a sample interposing the critical potential. Thus, the present
invention can shorten the plasma treating time by alternately carrying out
the etching step and the film formation step without changing over the
treating gas.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a structural view showing a plasma treating apparatus in
accordance with one embodiment of the present invention;
FIG. 2 is a diagram showing the relationship between a bias voltage in a
treating gas and an etching speed or a deposition speed;
FIG. 3 is a diagram showing the impressing pattern of an acceleration
voltage in the apparatus shown in FIG. 1;
FIG. 4 is a schematic view showing the etching state when a bias voltage is
not changed;
FIGS. 5 and 6 are schematic views showing the etching state in accordance
with the present invention;
FIG. 7 is a structural view showing a plasma treating apparatus in
accordance with the second embodiment of the present invention;
FIG. 8 is a diagram showing the impressing pattern of an acceleration
voltage in the apparatus shown in FIG. 7;
FIG. 9 is a structural view showing the plasma treating apparatus in
accordance with the third embodiment of the present invention;
FIG. 10 is a diagram showing the impressing pattern of an acceleration
voltage in the apparatus shown in FIG. 9;
FIG. 11 is a structural view showing the plasma treating apparatus in
accordance wihh the fourth embodiment of the present invention;
FIG. 12 is a diagram showing the impressing pattern of an acceleration
voltage in the apparatus shown in FIG. 11;
FIG. 13 is a structural view of the plasma treating apparatus in accordance
with the fifth embodiment of the present invention;
FIG. 14 is a structural view showing the plasma treating apparatus in
accordance with the sixth embodiment of the present invention;
FIG. 15 is a structural view showing the plasma treating apparatus in
accordance with the seventh embodiment of the present invention;
FIG. 16 is a structural view showing the plasma treating apparatus in
accordance with the eighth embodiment of the present invention;
FIG. 17 is a diagram showing the impressing pattern of an acceleration
voltage in the apparatus shown in FIG. 16;
FIG. 18 is a structural view showing the plasma treating apparatus in
accordance with the ninth embodiment of the present invention; and
FIG. 19 is a structural view showing the plasma treating apparatus in
accordacce with the tenth embodiment of the present invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
First of all, the first embodiment of the present invention will be
described with reference to FIGS. 1 to 6.
FIG. 1 shows a microwave plasma treating apparatus using ECR discharge,
which is an etching apparatus in this case. A discharge tube 1 made of
silica is disposed at an upper opening of a vacuum treating vessel 4. An
exhaust portion 3 which is connected to a vacuum exhaust device, not
shown, is disposed at the lower part of the vacuum treating vessel 4. An
electrode 5 having a sample table 5a, on which a wafer 6 as a sample is
placed, is disposed inside the vacuum treating vessel 4. A discharge space
7 is formed above the sample table 5a inside the discharge tube 1.
A waveguide 9 is disposed above the discharge tube 1 and encircles the tube
1. A magnetron 8 which generates a 2.45 GHz microwave in this case is
disposed at the end portion of the waveguide 9. An electromagnetic coil 10
is disposed around the outer periphery of the discharge tube 1 through the
waveguide 9.
A gas introduction portion 2 for supplying an etching gas into the
discharge space 7 is disposed sideways of the vacuum treating vessel 4 and
communicated with a gas source, not shown, through a mass flow controller
18.
A ground electrode 11 is disposed around the outer periphery of the
electrode 5 and electrically insulated therefrom. One end of this ground
electrode 11 is positioned near the sample table 5a while the other end is
grounded. A radio frequency power source 13 which oscillates a 13.56 MHz
radio frequency in this case is connected to the electrode 5 through a
matching box 12 while a D.C. power source 15 is connected to the electrode
5 through a low-pass filter 14. The other ends of the radio frequency
power source 13 and the D.C. power source 15 are each grounded. A voltage
controller 16 is connected to the D.C. power source 15 and an output
waveform controller 17 is connected to the output voltage controller 16.
The matching box 12 consists of capacitor coupling in this case. The
low-pass filter 14 is to cut off the radio frequency voltage from the
radio frequency power source 13.
The mass flow controller 18 controls the etching gas from the gas source,
not shown, to a predetermined flow rate and sends the etching gas into the
discharge space 7. The inside of the discharge space 7 is evacuated to a
reduced pressure by an exhaust device, not shown, and held at a
predetermined pressure.
In this case, a means for rendering plasmic the etching gas introduced into
the discharge space consists of the magnetron 8 and the electromagnetic
coil 10. The etching gas inside the discharge space 7 is rendered palsmic
by the ECR discharge resulting from the action of the electromagnetic
field provided by the magnetron 8 and the electromagnetic coil 10.
A means for applying incident energy to the wafer 6 to the ions in the
plasma, that is, a means for generating an acceleration voltage in the
sample table 5a in this case, consists of the radio frequency power source
13 and the D.C. power source 15. The radio frequency voltage from the
radio frequency power source 13 and the D.C. voltage from the D.C. power
source 15 are applied to the sample table 5a on which the wafer 6 is
placed. When the radio frequency voltage is applied to the sample table 5a
through the matching box 12 consisting of the capacitor coupling, the
radio frequency voltage is given D.C.-wise and floatingly so that a D.C.
bias voltage occurs. This D.C. bias voltage attracts the ions in the
plasma towards the sample table 5a, that is, towards the wafer 6. The
wafer 6 is sputter-etched by the incidence energy of the ions at this
time. Since the D.C. voltage is applied to the sample table 5a, the value
of the D.C. bias voltage occurring on the sample table 5a is adjusted. In
this case, this D.C. bias voltage becomes the acceleration voltage for
accelerating the ions.
Furthermore, a means for changing the value of the acceleration voltage
generated on the sample table 5a interposing the critical potential
consists of the voltage controller 16 and the output waveform controller
17, and the output voltage controller 16 controls the D.C. voltage value
of the D.C. power source 15. The output waveform controller 17 controls
the timing for changing the D.C. voltage value which the output voltage
controller 16 controls. The timing is controlled periodically in this
case.
The wafer 6 in this case is produced by depositing a poly-Si layer that is
a wiring forming material on a Si substrate. The etching apparatus of this
embodiment uses a mixed gas of sulfur hexafluoride (SF.sub.6) and
trichlorotrifluoroethane (C.sub.2 Cl.sub.3 F.sub.3 : "Flon - 113",
tradename) as the etching gas and etches the poly-Si layer of the wafer 6.
Next, the experiment wherein both components of the etching gas described
above, that is, SF.sub.6 and C.sub.2 Cl.sub.3 F.sub.3, are rendered
palsmic under the same plasma formation condition (microwave power: 400 W,
gas flow rate: 70 sccm, pressure: 0.01 Torr, radio frequency power: 100W)
in the etching apparatus described above and the D.C. bias voltage applied
to the sample table 5a is changed will be explained with reference to FIG.
2.
In the graph of FIG. 2, the etching speed is plotted at the upper part of
the ordinate while the deposition speed is plotted at its lower part. The
D.C. bias voltage is plotted on the abscissa.
As is obvious from FIG. 2, SF.sub.6 always causes the etching phenomenon
irrespective of the magnitude of the D.C. bias voltage and the etching
speed increases with an increasing D.C. bias voltage.
On the other hand, C.sub.2 Cl.sub.3 F.sub.3 causes the deposition
phenomenon within the range where the D.C. bias voltage is small and the
etching phenomenon within the range where D.C. bias is great. Furthermore,
it can be seen from the diagram that C.sub.2 Cl.sub.3 F.sub.3 has a
critical potential (Vo) exactly at its boundary where neither etching nor
deposition occur.
Incidentally, the term "critical potential" used hereby means the potential
at which the deposition phenomenon and the etching phenomenon reverse each
other when the gas is rendered palsmic and the D.C. bias voltage is
changed, and is found out for the first time through the experiments
conducted by the inventors of the present invention.
This means the following: When C.sub.2 Cl.sub.3 F.sub.3 is rendered
plasmic, the deposition action and the etching action occur concurrently.
At this time, if the D.C. bias voltage applied to the sample table 5a is
smaller than the critical potential, the deposition action occurs
preferentially. If the D.C. bias voltage applied to the sample table 5a is
increased within the range where it is smaller than the critical
potential, the ions in the plasma are accelerated with the increase of the
D.C. bias voltage, the etching action becomes gradually stronger and
priority of the deposition action decays gradually. If the D.C. bias
voltage increases beyond the critical potential, the ions in the plasma
are further accelerated and the etching action occurs more preferentially
than the deposition action so that the etching action becomes gradually
stronger. If the D.C. bias voltage is equal to the critical potential, the
deposition action and the etching action are in equilibrium with each
other.
A similar experiment was carried out by use of a mixed gas of SF.sub.6 not
having the critical potential described above and C.sub.2 Cl.sub.3 F.sub.3
having the critical potential (1: 9 mixture). The result is represented
by dash line curve in FIG. 2. As is obvious from this dash line curve, the
critical potential Vo' exists in this mixed gas, the deposition action
occurs preferentially at a D.C. bias voltage lower than the critical
potential Vo' and the etching action occurs preferentially at a D.C. bias
voltage greater than the critical potential Vo'. Moreover, when this mixed
gas is used, the etching speed depends more greatly on the D.C. bias
voltage than when C.sub.2 Cl.sub.3 F.sub.3 is used alone, as is obvious
from the diagram. It is found out therefore that this mixed gas can be
used as an etchant whose etching speed has high bias voltage dependence.
Next, the etching treatment using the mixed gas having such characteristics
will be described with reference to FIGS. 2 to 6.
First of all, when a poly-Si film having a high aspect ratio is etched at a
bias voltage value V1' higher than the critical potential Vo', an undercut
C becomes greater as shown in FIG. 4 and dimensional accuracy cannot be
secured. Here, reference numeral 19 represents a photoresist, 20 is
polysilicon and 21 is the Si substrate.
Accordingly, the D.C. voltage which is to be superposed with the radio
frequency voltage which floats D.C.-wise is controlled by the output
voltage controller 16 and the output waveform controller 17 and the D.C.
bias voltage is set to V.sub.1 (negative potential) greater than the
critical potential Vo' of the mixed gas for t.sub.1 seconds and to V.sub.2
(negative potential) smaller than the critical potential Vo' for t.sub.2
second and changed periodically.
Since the D.C. bias voltage is great for the time t.sub.1 seconds, etching
can be made while accelerating the ions in the plasma towards the wafer 6
so that relatively anisotropic etching can be carried out. However, an
undercut C.sub.0 occurs somewhat due partially to the influences of free
radicals. The size of this undercut C.sub.0 is substantially from 1/5 to
1/10 of the etching depth d in the vertical direction. The time t.sub.1 is
set within the range which does not exceed the allowance of the undercut
C.sub.0.
Since the D.C. bias voltage value is smaller than the critical potential
for the period t.sub.2, deposition can be generated so that regression of
etching stops, the plasma polymerization products start depositing on the
entire surface of the wafer 6 and the protective film is formed on the
wall surface on the pattern side of polysilicon 20.
After the protective film is formed, a large D.C. bias voltage V.sub.1 is
applied again to the sample table 5a to effect etching. The ions in the
plasma accelerated by this large D.C. bias voltage V.sub.1 are incident
perpendicularly to the wafer 6. Accordingly, the protective film deposited
at the pattern bottom of the polysilicon 20 formed by the photoresist 19
is removed rapidly by the sputter action of the ions and etching proceeds
while the pattern bottom of polysilicon 20 is exposed. The protective film
deposited on the wall surface on the pattern side of polysilicon 20 is
attacked by free radicals having extremely small physical energy and
removed gradually by the chemical reaction between the free radicals and
the components of the composition of the protective film. The deposition
time t.sub.2 of the protective film is set so that the protective film
deposited on the wall surface on the pattern side of polysilicon 20
remains even when etching is effected for the period t.sub.1.
Incidentally, the time t.sub.1 and t.sub.2 thus set are stored in advance
in the output waveform controller 17 and automatically changed over.
The polysilicon film having a high aspect ratio shown in FIG. 6 can be
machined with high dimensional accuracy by alternately repeating the
etching step and the deposition step, that is, the film formation step, in
the manner described above.
Incidentally, the value of the large D.C. bias voltage V.sub.1 is set to be
smaller than 1/2 of the total amplitude value V.sub.pp of the radio
frequency voltage in order to prevent charge-up of the ions to the sample.
For there is a limitation to the D.C. voltage to be superposed with the
radio frequency voltage in order to obtain a high etching speed and
moreover to effect etching without applying any damage to the device
formed on the sample.
Namely, if the D.C. bias voltage value (negative potential) is increased to
be greater than 1/2 of the total amplitude value V.sub.pp of the radio
frequency voltage, the sample is always at a negative potential, only the
positive ions are attracted to the sample surface and the sample is
charged. Accordingly, the positive ions (reactive ions) in the plasma
become finally repulsive and do not reach the sample, resulting in a
drastic drop of the etching speed of the sample: If the charge potential
is great at this time, degradation and breakdown of the gate portion of
the device formed on the sample will occur.
Therefore, this embodiment applies a negative D.C. voltage smaller than 1/2
of the total amplitude value V.sub.pp of the radio frequency voltage to
the sample table 5a so that part of the waveform of the radio frequency
voltage remains as the positive potential and this positive potential
portion entraps the electrons in the plasma, thereby neutralizing the
positive ions charged to the sample.
Furthermore, in order to solve this problem of charge-up, the transmission
frequency of the radio frequency voltage must be increased above about 100
KHz, as described in detail in Japanese Patent Publication No. 37311/1981.
Though there is no limitation, in particular, to the upper limit of the
transmission frequency, an oscillation frequency of up to about 27 MHz
will be suitable if oscillators that are commercially available on the
market are used.
In accordance with the first embodiment of the invention described above,
the radio frequency voltage is applied to the electrode 5 by the radio
frequency power source 13 in such a manner as to superpose the D.C.
voltage from the D.C. power source 15 with the D.C. bias voltage generated
in the sample table 5a by the application of the radio frequency voltage
and the D.C. bias voltage having superposed the D.C. voltage therewith is
changed in such a manner as to interpose the critical potential by the
output voltage controller 16 as well as the output waveform controller 17.
In this manner, etching and deposition, that is, film formation, can be
effected alternately to the wafer without changing the plasma generated in
the discharge portion 7, that is, without supplying the gas by changing it
over. Accordingly, in comparison with the conventional technique which
changes over the kind of gases and etches the sample by effecting
alternately etching and deposition, the present invention eliminates the
gas replacement time and can shorten the treating time effectively by at
least the elimination of this gas replacement time. For instance, an about
10 seconds time is necessary when a gas of 70 SCCM is supplied to a vacuum
treating vessel having a capacity similar to the capacity (20,000
cm.sup.3) of the vacuum treating vessel of this embodiment by use of an
exhaust device having an exhaust capacity of 500 l/sec, and the state
described above is established by changing over the kind of gases from the
state where the pressure is kept at 0.01 Torr. As the number of times of
gas switching increases, the effect of the present invention becomes more
remarkable. In other words, since it is not necessary in the present
invention to change over the gas at a high speed as required by the prior
art, the exhaust device can be made compact in size. Since the pressure
control and the change-over control for the change-over of the gas kind
become unnecessary in accordance with the present invention, the
apparatuses and control techniques required therefor become simplified.
Since the output voltage controller 16 is controlled in such a manner as to
apply the D.C. bias voltage greater than the critical potential to the
sample table 5a, the wafer 6 is etched and if the D.C. bias voltage
smaller than the critical potential is applied to the sample table 5a, the
protective film is deposited on the wafer 6. Furthermore, the output
waveform controller 17 is controlled in order to alternately change over
the timings at which the D.C. bias voltage is changed, interposing the
critical potential between them. Accordingly, etching can be made
step-wise while protecting the etching side surface of the wafer 6 by the
protective film and a material to be etched, which has a depth or height
greater than the pattern dimensional width can be machined.
Since the embodiment utilizes the treatment by the microwave plasma using
ECR discharge, the plasma can be generated at a pressure as low as
10.sup.-2 Torr, and since the ions in the plasma can be attracted by a
small acceleration voltage to the wafer 6, anisotropic etching with less
damage can be practised and a material to be etched, which has a delicate
pattern, can be machined. In other words, the material to be etched having
a delicate pattern and a great aspect ratio can be machined in cooperation
with the effects described above.
The change-over timing of the etching action and the deposition action is
set by the output waveform controller in such a manner that the undercut
of the material to be etched is within the allowance at the time of
etching and the protective film on the etching side surface remains till
next etching at the time of deposition. Accordingly, machining can be made
with high dimensional accuracy.
Since the plasma generation means utilizing the electromagnetic action is
independent of the D.C. bias voltage application means provided by the
radio frequency voltage and the D.C. voltage, that is, the acceleration
voltage application means, the state of generation of the plasma, that is,
the state of the electrons, ions and free radicals in the plasma, does not
change even if the D.C. bias voltage is changed, so that etching can be
made while light emission intensity is stable, and the end point of
etching can be easily judged by light emission spectroscopy.
Moreover, the radio frequency power source 13 is connected to the sample
table 5a to apply the radio frequency voltage and the D.C. voltage of the
D.C. power source 15 is controlled so as to set the D.C. bias voltage to
be below 1/2 of the total amplitude of the radio frequency voltage
generated from the radio frequency power source 13. Accordingly, even if
the sample has an insulating material or an insulating film, no charge is
built up in the sample and etching can be made without the drop of the
etching speed and degradation and breakdown of the gate portion of the
device. If a device of a device structure having an MOS gate in a lower
layer is etched by the etching method of the first embodiment of the
invention, degradation of breakdown voltage and damage of the gate portion
do not occur.
Incidentally, the ion sheath width is generally about 0.1 mm in microwave
plasma treating apparatuses which cause discharge by the ECR system by
utilizing the microwave as in the present embodiment. The time necessary
for the ions to pass through this ion sheath (t.sub.i) varies somewhat
depending upon the kind of ions but is generally from about 1 to
4.times.10.sup.-7 sec. In contrast, the half cycle time (t.sub.RF) of the
voltage waveform of the 13.56 MHz radio frequency that is generally used
for industrial applications is 3.7.times.10.sup.-8 sec. For this reason,
in the 13.56 MHz radio frequency voltage, the ions cannot follow while
passing through the ion sheath. Therefore, the ions can be accelerated by
generating the negative D.C. bias voltage as in the present embodiment.
The method which utilizes the D.C. bias voltage is particularly effective
when treating a sample which can establish conduction with the electrode
5, such as a Si or a metal film. The method of using the D.C. bias voltage
becomes effective when the half cycle time t.sub.RF of the voltage
waveform of the radio frequency and the ion sheath passage time of ions
t.sub.i have the following relation:
t.sub.RF <t.sub.i
Accordingly, the lower limit of the frequency of the radio frequency power
source 13 is about 2 MHz (t.sub.RF =2.5.times.10.sup.-7 sec). If the
frequency is lower than this value, the ions follow up the A.C. voltage
waveform and are accelerated so that the effect of superposition of the
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