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| United States Patent | 5436424 |
| Link to this page | http://www.wikipatents.com/5436424.html |
| Inventor(s) | Nakayama; Ichiro (Kadoma, JP);
Nomura; Noboru (Kyoto, JP);
Tamaki; Tokuhiko (Sakai, JP);
Okuni; Mitsuhiro (Higashiosaka, JP);
Kubota; Masafumi (Osaka, JP) |
| Abstract | A plasma generating apparatus includes a vacuum chamber having an insulated
inner surface, more than two electrodes arranged on the insulated inner
surface of the vacuum chamber, a high frequency applying device for
applying high frequencies having different phases in order of positions of
the electrodes, and a holder on which an object to be processed is placed.
In the apparatus, a magnetic field is produced under plural alternating
electric fields, so that electrons in a plasma generating portion are
rotated to generate high density plasma under a high vacuum when the high
frequencies are applied to the electrodes to generate the plasma and a
specified process such as etching, CVD, or doping is carried on the object
by reaction products generated at the portion. |
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Title Information  |
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Drawing from US Patent 5436424 |
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Plasma generating method and apparatus for generating rotating electrons
in the plasma |
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| Publication Date |
July 25, 1995 |
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| Filing Date |
June 24, 1993 |
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| Priority Data |
Jun 25, 1992[JP]4-167177 |
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Title Information  |
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Description  |
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BACKGROUND OF THE INVENTION
The present invention relates to a plasma generating method and apparatus
utilized in a process for manufacturing a semiconductor or a thin film
circuit.
Recently, fine processes using a plasma have become popular in processes
for manufacturing semiconductors or thin film circuits. More particularly,
in dry etching, CVD, a doping processes, and gas suitable for a desired
purpose is introduced into a vacuum chamber which has electrodes, and a
high frequency electric power is applied to the electrodes to relatively
simply carry out those processes. Thus, such fine processes using plasma
are used in many processes.
For example, in the dry etching process, it is indispensable to make
patterns fine, prevent ion scattering, and improve the directional
properties of ions. Therefore, it is effective to increase the degree of
vacuum and then to increase the mean free paths of the ions. Then, etching
is effected under a high degree of vacuum.
Generally, as the degree of vacuum increases, the generation of a high
frequency becomes more difficult. To prevent such a disadvantage, a method
in which a magnetic field is applied to a plasma chamber to make the
discharge easy, that is, a magnetron discharge or ECR (electron cyclotron
resonance) discharge has been developed.
FIG. 3 is a schematic diagram showing a conventional dry etching apparatus
using a magnetron discharge. In a vacuum chamber 29, a reactive gas is
introduced through a gas controller 30 to control the pressure to become
suitable by an exhaust system 31. An anode 32 is provided on the upper
portion of the chamber 29 and a sample table 33 as a cathode is provided
on the lower portion thereof. The table 33 is connected to an RF source 35
through an impedance matching circuit 34 to generate a high frequency
discharge between the holder 33 and the anode 32. In the chamber 29, a
magnetic field is applied thereto by an alternative electromagnet 36
provided on the side surface thereof to make the discharge easy in a high
degree of vacuum. The applied magnetic field allows the cycloid movement
of electrons to increase the ionization rate.
However, it is difficult to treat the magnetron discharge or ECR discharge
because of uneven plasma density. A sample to be processed is subjected to
any damage in such a discharge. For example, in a conventional magnetron
dry etching apparatus, there is local plasma bias in accordance with the
magnetic field to produce the local potential. Then, when the apparatus is
used for manufacturing MOS LSIs, the destruction of gate oxide films is
caused. Similarly, in the conventional ECR etching apparatus, the magnetic
field has distribution in a radial direction of the chamber to cause
uneven etching and to produce a local potential, on the basis of locally
uneven plasma degrees.
SUMMARY OF THE INVENTION
Accordingly, an object of the present invention is to provide a method and
an apparatus for generating a uniform high density plasma in a high degree
of vacuum.
In accomplishing these and other aspects, according to one aspect of the
present invention, there is provided a method for generating a plasma by
applying to more than two electrodes arranged on an insulated surface of a
vacuum chamber high frequencies having different phases in order of
positions of the electrodes, in which electrons are rotated in a portion
of the chamber where the plasma is generated when the high frequencies are
applied to the electrodes to generate the plasma.
According to another aspect of the present invention, there is provided a
plasma generating apparatus comprising:
a vacuum chamber having an insulated inner surface;
more than two electrodes arranged on the insulated inner surface of the
vacuum chamber;
a high frequency applying device for applying high frequencies having
different phases in order of positions of the electrodes; and
a holder on which an object to be processed is placed;
wherein electrons, in a portion of the chamber where the plasma is
generated, are rotated when the high frequencies are applied to the
electrodes to generate the plasma and a specified process is carried out
onto the object by reaction products generated at the portion.
BRIEF DESCRIPTION OF THE DRAWINGS
These and other aspects and features of the present invention will become
clear from the following description taken in conjunction with the
preferred embodiments thereof with reference to the accompanying drawings,
in which:
FIG. 1 is a schematic diagram showing the construction of a plasma
generating apparatus for carrying out a plasma generating method,
according to first, second, and third embodiments of the present
invention;
FIG. 2 is a schematic diagram showing the construction of a plasma
generating apparatus for carrying out a plasma generating method,
according to a fourth embodiment of the present invention; and
FIG. 3 is a schematic diagram showing a conventional reactive ion-etching
apparatus using a magnetron discharge.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
Before the description of the present invention proceeds, it is to be noted
that like parts are designated by like reference numerals throughout the
accompanying drawings.
A first embodiment of the present invention which can be applied to an
etching process is described below with reference to FIG. 1.
A plasma generating apparatus for carrying out a plasma generating method,
according to the first embodiment is shown in FIG. 1. In FIG. 1, reference
numeral 1 denotes a chamber made of an insulating material such as quartz;
elements 2 and 3 are electrodes to which a high frequency electric power
is applied through respective matching circuits 6 and 7; and elements 4
and 5 are ground electrodes which respectively oppose the electrodes 2 and
3, respectively. The high frequency electric power which are the same as
each other are applied to the electrodes 2 and 3 from high frequency power
sources 8 and 9, respectively. The phase of the high frequency electric
power applied to the electrode 2 is shifted by approximately 90.degree.
from that of the high frequency electric power applied to the electrode 3
by a known phase-locked control mechanism 10.
According to the plasma generating apparatus, for example, an etching gas
such as SF.sub.6 of 5 sccm is introduced in the chamber 1 to control the
pressure therein to keep 1 Pa. In this condition, 100 w of electric power
is applied to each of the electrodes 2 and 3 from the power sources 8 and
9 at 50 MHz. An object 12 to be treated is placed on a sample table 11.
The object 12 is formed so that polysilicon is deposited on the surface
thereof and then a resist is patterned through a photolithographic
process. A 100 w of electric power is applied on the sample table 11
through a matching circuit 13 by a power source 14 at 800 KHz.
Then, the etching rate of polysilicon is 4000-5000 .ANG./min, the
uniformity is .+-.5% or less, which show excellent etching
characteristics. There is little side etching in the etching configuration
as compared with the conventional dry etching apparatus. There is little
local bias of the plasma, which causes little damage to devices such as
the destruction of gate oxide films in MOS LSIs.
Next, a second embodiment of the present invention which can be applied to
a CVD process is described below with reference to FIG. 1. A plasma
generating apparatus and a plasma generating method of the second
embodiment is the same as those of the first embodiment except for the
following operation.
According to the plasma generating apparatus, an etching gas such as
SiH.sub.4 (N.sub.2 20% dilution), and NH.sub.3 gas of 15 sccm and N.sub.2
gas of 34 sccm are introduced in the chamber 1 to control the pressure
therein to keep 1 Pa. In this condition, 200 w of electric power is
applied to each of the electrodes 2 and 3 from the power sources 8 and 9
at 50 MHz. The object 12 to be treated such as a silicon substrate is
placed on the sample table 11. The sample table 11 has a constant
temperature of 300.degree. C. 50 w of electric power is applied to the
sample table 11 through the matching circuit 13 by the power source of 800
KHz.
Then, the speed for forming a plasma silicon nitride thin film is 800
.ANG./min, the uniformity is .+-.3% or less, which show excellent etching
character.
Next, a third embodiment of the present invention which can be applied to a
doping process is described below with respect to FIG. 1. The plasma
generating apparatus and method of the third embodiment is the same as
those of the first embodiment except for the following operation.
According to the apparatus, a doping gas such as B.sub.2 H.sub.6 of 5 sccm
is introduced in the chamber 1 to control the pressure therein to keep 0.3
Pa. In this condition, 100 w of electric power is applied to each of the
electrodes 2 and 3 from the power sources 8 and 9 at 50 MHz. The object 12
to be treated such as a silicon substrate is placed on the sample table
11. 500 w of electric power is applied onto the sample table 11 through
the matching circuit 13 by the power source 14 of 800 KHz.
Then, after discharging for one minute, the boron density fin the vicinity
of the surface of the silicon substrate 12 is analyzed by SIMS (secondary
ion mass spectroscopy), which indicate the doping density to be
2.times.10.sup.21 in number, thus showing excellent doping results.
Next, a fourth embodiment of the present invention which can be applied to
a doping process is described below with respect to FIG. 2. The plasma
generating apparatus and method of the fourth embodiment is the same as
the apparatus shown in FIG. 1 except for a grid 27 and a DC power source
28 and the following operation.
According to the apparatus, a doping gas such as B.sub.2 H.sub.6 of 5 sccm
is introduced in the chamber 1 to control the pressure therein to keep 0.3
Pa. In this condition, 100 w of electric power is applied to each of the
electrodes 2 and 3 from the power sources 8 and 9 at 50 MHz. The object 12
to be treated such as a silicon substrate is placed on the sample table
11. There is a potential of 2 KV between the sample table 11 and the grid
27 by the DC power source 28.
Then, after discharging for two minutes, the boron density in the vicinity
of the surface of the silicon substrate 12 is analyzed by SIMS, which
indicate the doping density to be 5.times.10.sup.21 in number, which shows
excellent doping results.
According to the embodiments, more than three electrodes, that is, the four
electrodes 2,3,4,5 are arranged in the chamber 1 on the insulating
material, and the high frequencies which are different from each other in
phase in order of the positions of the electrodes are applied to the
electrodes to generate a plasma to rotate electrons in the plasma
generating portion. That is, the application of the high frequencies to
the electrodes causes a magnetic field which allows the oscillation and
rotation of electrons. Thus, under even a high vacuum, a high ionization
efficiency can be obtained to make the discharge easy. As compared with
the conventional magnetron discharge or ECR discharge, the apparatus
according to each embodiment can produce the uniform electric field to
obtain a plasma with excellent uniformity and make it easy to design a
large scale apparatus. There is little local bias of the plasma, which
causes little damage to an object to be processed. The insulating material
of the chamber prevents the electrons from flowing out of the chamber. In
the embodiments, preferably, the surface of the holder where the object is
placed is substantially the same as the electrodes to increase the
processing rate for etching, CVD, or doping because the electrodes are
located at portions where the plasma density is high. Furthermore, in
order to obtain the same effects as above, the electrodes may be located
on the same circle.
Although the present invention is described using the etching, CVD, and
doping apparatuses in the embodiments, the present invention can be
applied to a sputtering, an ion source for an ion implantation device, and
any apparatus which requires a high vacuum plasma. And, though the
embodiments are described in the case where the constant phase difference
of the high frequency is 90 degree, the phase difference may vary like a
time function. Although the description is directed to four electrodes,
the number of electrodes may be N (N is any integer more than 2) as long
as the phase difference is 360/N, thus obtaining the same effects as
above. The high frequencies may be different from each other in phase by
120.degree. in order of the positions of the electrodes, for example.
Instead of the chamber comprised of the insulating material, only the
inner surface of the electrically conductive chamber may be made of
insulating material, thus obtaining the same effects as above.
As described above, according to the embodiments, the rotation of electrons
under a plurality of appropriate alternating electric fields, a high
density plasma is generated in high vacuum. Furthermore, the present
invention can have excellent fine processability and high mass
productivity, and can considerably reduce the damage to devices such as
the destruction of gate oxide films, realizing such a plasma process.
Although the present invention has been fully described in connection with
the preferred embodiments thereof with reference to the accompanying
drawings, it is to be noted that various changes and modifications are
apparent to those skilled in the art. Such changes and modifications are
to be understood as being included within the scope of the present
invention as defined by the appended claims unless they depart therefrom.
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Description  |
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