Patent Document

CROSS-REFERENCE TO RELATED APPLICATIONS 
     This application is based upon and claims the benefit of priority from the prior Japanese Patent Applications No. 2000-069044, filed Mar. 13, 2000; and No. 2000-085281, filed Mar. 24, 2000, the entire contents of which are incorporated herein by reference. 
     BACKGROUND OF THE INVENTION 
     The present invention relates to a discharge plasma generating method, discharge plasma generating apparatus, semiconductor device fabrication method, and semiconductor device fabrication apparatus used in the deposition of thin films of semiconductors such as amorphous silicon, nanocrystalline silicon, polycrystalline silicon, and silicon nitride for use in various electronic devices such as an amorphous Si-based solar cell, a thin-film polycrystalline Si-based solar cell, an LCD (liquid crystal display), a thin-film transistor of a flat panel display, a photosensitive body of a copying machine, and an information recording device, or used in the etching of thin films of semiconductor elements. 
     The surface processing technologies using a discharge plasma of a reactive gas are being more and more demanded to increase the area and processing speed in the fabrication of diverse electronic devices every year. To meet these needs, research and development are recently being extensively made, not only in the industrial world but also in learned societies, particularly for the use of plasma chemical vapor deposition (to be referred to as PCVD hereinafter) and a very-high-frequency (VHF) power supply having a frequency of 30 to 800 MHz. 
     Apparatuses and methods of generating a discharge plasma of a reactive gas are disclosed in Jpn. Pat. Appln. KOKAI Publication No. 8-325759 (to be referred to as reference  1  hereinafter) and L. Sansonnens et al., “A voltage uniformity study in large-area reactors for RF plasma deposition”, Plasma Source Sci. Technol. 6(1997), pp. 170-178 (to be referred to as reference  2  hereinafter). 
     Unfortunately, the conventional PCVD and plasma etching have the following problems. 
     (1) The first problem is an increased size of a substrate to be processed. Needs for large-sized solar cells and flat panel display LCDs are increasing. When an amorphous silicon film (to be referred to as an a-Si film hereinafter) is formed on a 50 cm×50 cm substrate by the conventional PCVD method, the film thickness distribution is, e.g., as shown in FIG.  6 A. Also, when an a-Si film is formed on a 100 cm×100 cm substrate by the conventional method, the film thickness distribution is, e.g., as shown in FIG.  6 B. As shown in FIGS. 6A and 6B, as the frequency of a high-frequency power supply increases, the film thickness distribution of an a-Si film increases, so the film thickness uniformity significantly lowers. In the field of LCDS, a film thickness distribution of ±5% is permitted. In the field of solar cells, a film thickness distribution of a maximum of ±20%, preferably ±10% is permitted. Accordingly, when such large-sized substrates are used in the conventional PCVD method, the only practical power-supply frequency is 13.56 MHz, and no VHFs in a frequency band exceeding this frequency are practical. 
     (2) The second problem is a method of increasing the surface processing speed (improving the productivity) and improving the film quality. To increase the speed of surface processing, the discharge plasma density must be increased. As a method of increasing the discharge plasma density, the use of a VHF in a frequency band exceeding a versatile power-supply frequency of 13.56 MHz is recommended. Also, to improve the film quality, ion damage to a film must be reduced. To this end, reducing the plasma potential related to the ion energy is effective. The use of a VHF which reduces the plasma potential is also recommended for this purpose. 
     As examples of needs for a high surface processing speed, low cost (a high film formation speed and a large area) and high quality (a low defect density and high crystallinity) are demanded in the formation of thin films for solar cells and thin-film transistors for flat panel displays. Mat. Res. Soc. Symp. Proc. Vol. 424, p. 9, 1997 (to be referred to as reference  3  hereinafter) disclosed a method of increasing the film formation speed and improving the quality of films by using a VHF power supply. A VHF is recently found to be suited to the high-speed, high-quality formation of particularly a thin nanocrystalline Si film which is attracting attention as a new thin film replacing an a-Si film. 
     When a VHF is used, however, a VHF progressive wave A 1  propagating in the forward direction on an electrode and a VHF reflected wave A 2  propagating in the opposite direction interfere with each other as shown in FIG. 2A, generating a standing wave A 3  as shown in FIG.  2 B. This standing wave A 3  promotes the spatial nonuniformity of the discharge plasma density, thereby increasing the film thickness distribution of a thin film formed on a substrate  804 . This is contrary to the need described in item (1) above. 
     Other causes which promote the film thickness nonuniformity resulting from this standing wave are as follows. 
     (a) The first cause is an increase and nonuniformity of the impedance of a propagation path resulting from the skin effect. When a VHF is supplied from a power supply  807  to an electrode  802  via feeding point (feeder distribution center)  809 ,  809   a , and  809   b  as shown in FIGS. 1A and 1B, the skin effect causes this VHF to propagate, along the surface portion of the electrode  802 , as the progressive wave A 1  in one direction and the progressive wave A 2  in the other direction on the electrode surface as shown in FIG.  2 A. This interference generates the standing wave as shown in FIG.  2 B. This skin effect appears more notably for a VHF than for a versatile frequency of 13.56 MHz as a high frequency. A surface depth δ at which a current flows by this skin effect is given by 
     
       
         δ=(3.14 ×f ·μ·σ) −0.5   
       
     
     where f is the frequency, μ is the permeability, and a is the conductivity. 
     When the electrode  802  is copper, for example, its surface depth is about 19 μm for a frequency of 13.56 MHz as a high frequency, about 10 μm for a VHF of 50 to 60 MHz, and about 5.8 μm for a VHF of 150 MHz. Therefore, in PCVD or plasma etching using a VHF, the impedance of a power-supply propagation path from a power supply to a discharge portion of a discharge electrode increases. This increases the impedance and makes voltage distribution nonuniform. Accordingly, the spatial uniformity of the discharge plasma density cannot be held any longer. 
     (b) The second cause is mutual interference between a plasma and VHF. When a VHF becomes nonuniform as described above, the plasma distribution becomes nonuniform accordingly, thereby producing a load distribution (the impedance lowers as the plasma density rises) to an electrode. This influences the VHF distribution. 
     As described above, the discharge plasma density becomes nonuniform owing to the generation of a standing wave by a reflected wave from the electrode end, the influence which the presence of the electrode impedance has on the voltage distribution, and the mutual interference between a plasma and VHF. Consequently, the film thickness uniformity suffers in large-area PCVD using a VHF. 
     For example, when the dimensions of a parallel plate electrode exceed 30 cm×30 cm or the VHF frequency exceeds 30 MHz, the influence of the standing wave A 3  becomes conspicuous. This makes it difficult to achieve the minimum necessary film thickness uniformity of semiconductor devices. 
     FIG. 3 is a graph showing a voltage distribution and an ion saturation current distribution by plotting the position (cm) on a discharge electrode on the abscissa and a voltage vpp (V) and ion saturation current on the ordinate. This data is obtained by the conventional method which uses a VHF of 100 MHz. Referring to FIG. 3, a characteristic curve B 1  indicates the voltage distribution, and a characteristic curve B 2  indicates the ion saturation current distribution. This ion saturation current distribution (B 2 ) is substantially equal to the electron density distribution and can be easily measured. Hence, the ion saturation current distribution is generally used as an index of the discharge plasma density distribution. The voltage distribution (B 1 ) shows that the standing wave A 3  is generated on the electrode and the ion saturation current distribution, i.e., the plasma distribution becomes nonuniform accordingly. 
     On the other hand, in Jpn. Pat. Appln. KOKAI Publication No. 11-111622 (a four-point feeding method: to be referred to as reference  4  hereinafter), the generation of the voltage distribution caused by the standing wave A 3  is suppressed by feeding power to four different portions of a ladder electrode. A ladder electrode is formed by assembling a plurality of parallel longitudinal electrode rods  304  and one or more pairs of parallel lateral electrode rods into the form of a lattice. This ladder electrode is assumed to be more uniform than a common parallel plate electrode. In the method of reference  4 , the standing wave generation suppressing means as described above is added to this ladder electrode. However, if the electrode dimensions exceed 30 cm×30 cm or the power-supply frequency exceeds 80 MHz, the effect of preventing the generation of a voltage distribution is substantially lost. This makes it difficult to form a film having a uniform thickness on a large-area substrate. 
     FIG. 4 is a graph showing voltage distributions by plotting the position (cm) on a ladder electrode on the abscissa and the voltage Vpp (V) on the ordinate. This data shows voltage distributions generated in a certain electrode rod on the ladder electrode when power is fed via four points by the conventional method by using VHFs of 60 and 100 MHz. Referring to FIG. 4, a characteristic curve C 1  indicates data obtained when a VHF of 60 MHz is used, and a characteristic curve C 2  indicates data obtained when a VHF of 100 MHz is used. Although a relatively uniform voltage distribution is obtained at a frequency of 60 MHz (the characteristic curve C 1 ), a nonuniform voltage distribution is obtained at a frequency of 100 MHz (the characteristic curve C 2 ). Also, in the method of this reference  4 , optimum positions of the four feeding points must be found by trial and error, and this requires much labor and time. Furthermore, if the film formation conditions such as the gas pressure and high-frequency power change, the optimum positions of the feeding points also change. 
     The above problems are also noted in learned societies. Mat. Res. Soc. Symp. Proc. Vol. 377, p. 27, 1995 (to be referred to as reference  5  hereinafter) has proposed a method in which a lossless reactance (coil) is connected to the side away from the feeding side of a parallel plate electrode. In the method of this reference  5 , the conditions of reflection of a progressive wave from the electrode end are changed to generate a portion in which the distribution is relatively flat in the waveform of the standing wave A 3 , e.g., an antinode portion (a portion near the peak of a sine wave) on the electrode, thereby decreasing the voltage distribution in the electrode. However, the method of reference  5  does not do away with the standing wave  3  all together but merely generates a flat portion of a sine wave on the electrode. Therefore, a uniform portion is obtained up to at most about ⅛ the wavelength (0.6 m for 60 MHz, and 0.4 m for 100 MHz). Uniformization within a range exceeding this is in principle impossible. The standing wave A 3  shown in FIG. 2B has four nodes and four antinodes. A standing wave like this cannot be uniformized. The method is effective only in a case as indicated by B 1  in FIG. 3, in which the length is equal to or smaller than a pair of one node and one antinode. 
     FIG. 5 is a graph showing a voltage distribution by plotting the position (cm) on a ladder electrode on the abscissa and the voltage Vpp (V) on the ordinate. Referring to FIG. 5, a characteristic curve D indicates data showing a voltage distribution when one end of a parallel plate electrode is terminated by a lossless reactance (coil) at a VHF of 100 MHz. As shown in FIG. 5, the voltage in a region from the end of the electrode to about 30 cm can be made substantially uniform. However, the voltage becomes nonuniform in a region larger than this, so this region cannot be used in film formation. 
     As described above, when a VHF is used in the conventional PCVD method, it is impossible to generate a uniform discharge plasma in a large area and perform uniform processing if a very large substrate exceeding 1 m×1 m is processed at 60 MHz or if a 30 cm×30 cm substrate is processed at a frequency exceeding 80 MHz. 
     M. Noisan, J. Pelletier, ed., “Microwave Excited Plasmas”, Technology, 4, second impression, p. 401, Elsevier Science B.V., 1999 (to be referred to as reference  6  hereinafter) disclosed a technique which supplies two different high-frequency waves to two discharge electrodes. This technique of reference  6  uses one high-frequency wave to generate a discharge plasma and the other high-frequency wave to control the surface bias voltage of a substrate, thereby controlling the amount of active ions flowing into the substrate and the amount of energy incident on the substrate. That is, the purpose of this technique is not to uniformize a plasma when a large-size substrate exceeding 1 m×1 m is processed. 
     BRIEF SUMMARY OF THE INVENTION 
     It is an object of the present invention to provide a discharge plasma generating method, discharge plasma generating apparatus, semiconductor device fabrication method, and semiconductor device fabrication apparatus which can generate a uniform discharge plasma in a large area by using a very high frequency (VHF) and can uniformly process a large substrate. 
     The first subject of the present invention is to eliminate the generation of a standing wave on an electrode in principle and uniformize the voltage distribution on the electrode while a plasma is generated, thereby improving the uniformity (in-plane uniformity) of the film formation rate or etching rate on the surface of a substrate. As described earlier, it is very difficult for the conventional method to make the voltage distribution uniform if the electrode size exceeds ⅛ of a high-frequency wavelength. For example, when a high frequency of 60 MHz is applied to an electrode having dimensions exceeding 1 m×1 m, a standing wave significantly appears to make the voltage distribution extremely nonuniform. Also, when a VHF exceeding 80 MHz is applied to a 30 cm×30 cm electrode, a standing wave significantly appears to make the voltage distribution very nonuniform. 
     The plasma density becomes nonuniform at a VHF probably by {circle around (1)} the generation of a standing wave on an electrode, {circle around (2)} the influence of the presence of floating impedance on the voltage distribution, and {circle around (3)} the mutual interference between a plasma and high-frequency wave. The present inventors made extensive studies on these problems and have found that {circle around (1)} the generation of a standing wave on an electrode is the main cause. On the basis of this knowledge, the present inventors have completed the present invention. 
     The present invention will be simply described below for the sake of easy understanding. 
     Assume that a phenomenon on two-dimensional electrode is simplified to a phenomenon on one-dimensional electrode and two frequencies are supplied from the two ends of one rod electrode (corresponding to one electrode rod of a ladder electrode). Assume also that the attenuation of the two high-frequency waves is neglected and the reflection at the electrode end is negligibly small. Under the simplified conditions, the high-frequency waves (voltages (φ(V))) supplied from the two ends of the rod electrode are given by 
     
       
         φ 1 =cos(ω 1   t−k   1   z+θ   1 )  (1) 
       
     
     
       
         φ 2 =cos(ω 2   t−k   2   z+θ   2 )  (2) 
       
     
     where ω, k, t, z, and θ are the angular frequency (rad/sec), wave number (rad/m), time (sec), position (m), and phase angle (rad), respectively, of each wave. 
     The wave number k is represented using a phase velocity v (m/sec) and the angular frequency ω by 
     
       
           k   1 =ω 1   /v   1   , k   2 =ω 2   /v   2   (3) 
       
     
     A high-frequency voltage φ at each time in each point (portion) on the electrode is given as the sum of equations (1) and (2) by as follows: 
     
       
         φ=φ 1 +φ 2 =cos(ω 1   t−k   1   z+θ   1 )+cos(ω 2   t−k   2   z+θ   2 )=2cos(ω ave   t−k   mod   z+θ   ave )·cos(ω mod   t−k   ave   z+θ   mod )  (4) 
       
     
     The individual components in the equation are as follows: 
     
       
         ω ave =(ω 1 +ω 2 )/2, ω mod =(ω 1 −ω 2 )/2, 
       
     
     
       
           k   ave =( k   1   +k   2 )/2 , k   mod =( k   1   −k   2 )/2, 
       
     
     
       
         θ ave =(θ 1 +θ 2 )/2, θ mod =(θ 1 −θ 2 )/2, 
       
     
     In equation (4) above, the term cos(ω ave t−k mod z+θ ave ) corresponds to a carrier wave, and the term cos(ω mod t−k ave z+θ mod ) corresponds to an envelope. 
     An “envelope” is a curve formed by tracing and jointing the peaks of a modulated high-frequency wave. More specifically, when a high-frequency wave φ 1  shown in FIG. 7A and a high-frequency wave φ 2  shown in FIG. 7B are synthesized, a synthetic wave φ shown in FIG. 7C results. This synthetic wave φ is represented by equation (4) above, and its component cos(ω mod t−k ave z+θ mod ) is the envelope. 
     First, assume that ω 1 =ω 2  and θ mod  is constant with time (θ mod (t)=const.), i.e., assume that high-frequency waves having the same frequency and a phase difference which does not change with time are supplied from the two ends. This is equivalent to supplying high-frequency ω 1  power by dividing it into two portions from a single power supply or to operating a plurality of high-frequency power supplies in synchronism with each other by a high frequency from a single oscillator and supplying their outputs. That is, this case corresponds to the conventional method. When this is the case, the high-frequency voltage φ on the electrode is represented by 
     
       
         φ=2cos(ω 1   t+θ   ave )·cos(−ω 1   /v   1   ·z+θ   mod )(5) 
       
     
     This equation (5) shows that a high frequency having a carrier wave cos(ω 1 t+θ ave ) with the angular frequency ω 1  and an envelope cos(−ω 1 /v 1·z+θ   mod ) exist on the electrode. The carrier wave dominates a temporal change in the voltage at a certain point, and the envelope dominates the spatial distribution of the voltage. Since ω 1 =ω 2  and θ mod (t)=const, the envelope cos(−ω 1 /v 1 ·z+θ mod ) does not change with time and as a consequence becomes a standing wave. 
     This can be simply explained as follows. 
     FIG. 2A is a graph for explaining a standing wave generated when the two output high frequencies from a two-output phase-variable high-frequency oscillator are supplied to an electrode while the phase difference between the frequencies is held at a constant value (θ mod (t)=const). Referring to FIG. 2A, the waveform of a high frequency A 1  indicates a progressive wave of the first power, which is represented by equation (1), and a high frequency A 2  indicates a progressive wave of the second power, which is represented by equation (2). FIG. 2B is a graph showing the power distribution of a standing wave by plotting the position on the electrode surface on the abscissa and the square of the envelope term cos(−ω 1 /v 1 ·z+const.) of equation (5) on the ordinate. When the phase difference between the two output high-frequency power components is fixed to a constant value (θ mod (t)=const, e.g., 0°), these power components are synthesized to form a standing wave as shown in FIG.  2 B. This standing wave is the cause of a spatial voltage distribution, i.e., a plasma distribution, and a film deposition distribution in the conventional feeding method. 
     On the other hand, if the envelope does not stay as a standing wave but moves with time, the generation of a standing wave is suppressed. This is the gist of the present invention. Two examples will be presented below. 
     (a) When ω 1 ≠ω 2  (a method of supplying high-frequency waves of different frequencies) 
     When two frequencies are different (ω 1 ≠ω 2  ), a high-frequency voltage φ at each point at each time is calculated by 
     
       
         
               
               
               
               
             
           
               
                   
                   
               
             
             
               
                   
                 φ = 
                 2cos(ω ave t − k mod z + θ ave ) 
                   
               
               
                   
                   
                 ·cos(ω mod t − k ave z + θ mod ) 
                   ...  (6) 
               
               
                   
                   
               
             
          
         
       
     
     From equation (6) above, this high-frequency voltage φ contains a carrier wave cos(ω ave t−k mod z+θ ave ) having an angular frequency ω ave  and an envelope cos(ω mod t−k ave z+θ mod ) having an angular frequency ω mod  which is generally called “beat” or “hum”. Since the envelope includes a term ω mod t which changes with time, this envelope moves with the passing of time, so no standing wave is generated. This is the first best mode of the present invention. 
     (b) When ω 1 =ω 2  and θ mod (t)≠const. (a method of supplying high-frequency waves having the same frequency by temporally changing the phase difference) 
     When frequencies are the same (ω 1 =ω 2 ) and the phase difference θ mod  changes in a split second(at all times) (θ mod (t)≠const.), a high-frequency voltage φ at each point at each time is calculated by 
     
       
         φ=2cos(ω 1   t+θ   ave )cos(−ω 1   /v   1   ·z+θ   mod (t))  (7) 
       
     
     In equation (7) above, the envelope is cos(−ω 1 /v 1 ·z+θ mod (t)), i.e., includes a term θ mod (t) which changes with time. Accordingly, this envelope moves with the passing of time, and no standing wave is generated. This is the second best mode of the present invention. 
     When the envelope is in a split second (at all times) changed as indicated by items (a) and (b) above, no standing wave is generated on an electrode, so a uniform plasma can be generated. 
     Note that the conditions of ω 1 ≠ω 2  (the method of supplying high-frequency waves of different frequencies) and ω 1 =ω 2  and θ mod (t)≠const. (the method of supplying high-frequency waves having the same frequency by changing the phase difference) need not be intentionally made. These conditions can be simply realized by the use of two independent high-frequency oscillators. That is, even two high-frequency oscillators set to oscillate the same VHF, e.g., 100 MHz have characteristics unique to the individual oscillators. Hence, actual oscillation frequencies slightly deviate from the set frequency (100 MHz). For example, the first oscillation frequency is 100.001 MHz and the second oscillation frequency is 100.003 MHz, i.e., ω 1 ≠ω 2  holds in a strict sense. Also, frequencies change with temperature variation and the like, so the relationships between frequencies and between phases change at random. Therefore, when a plurality of independent high-frequency oscillators are used, the envelope moves with time, and no standing wave is generated. 
     Another method of changing the envelope is to change frequency with time (FM modulation: frequency modulation), perform chirp (frequency chirp), or change an amplitude with time (AM modulation: amplitude modulation). 
     In the formation of a large-area uniform film performed by a plasma by using a high-frequency wave on the basis of this principle, even when the electrode size exceeds ⅛ of the high-frequency wavelength, in which case uniformization is conventionally very difficult, i.e., even for an apparatus for processing a very large substrate exceeding 1 m×1 m at a high frequency of, e.g., 60 MHz, the present invention provides a method of feeding power to a discharge electrode, by which a high frequency is supplied to the electrode such that the envelope function of a high-frequency voltage φ on the electrode temporally changes, thereby performing high-speed, high-quality film formation as the characteristic of a high-frequency wave and at the same time generating a uniform plasma and forming a uniform film by suppressing the generation of a standing wave on the electrode. 
     This temporal change of the envelope function is realized by the use of a plurality of high-frequency power supplies. 
     First, case (a) in which ω 1 ≠ω 2  (the method of supplying high-frequency waves having different frequencies) will be explained. 
     As practical means of supplying two frequencies (ω 1 ≠ω 2 ) to an electrode, two independent high-frequency power supplies are used. For example, in two power supplies (containing high-frequency oscillators) having a rated frequency of 60 MHz, each oscillator has an oscillation frequency unique to the oscillator. In practice, therefore, a frequency difference of about a few hundred kHz exists between the two oscillators. This difference between the inherent oscillation frequencies allows ω 1 ≠ω 2  to hold in practice. 
     Alternatively, to avoid the contingency as described above, a plurality of power supplies having two oscillation frequencies positively made different from each other are used. 
     If the difference between the frequencies of these high-frequency power supplies is made too large and one frequency largely deviates from an optimum frequency, the properties of film formation and etching significantly lower from the properties of the optimum frequency. To prevent this, the frequency difference is set to 20% or less. 
     Case (b) described above in which ω 1 =ω 2  and θ mod (t)≠const. (the method of supplying high-frequency waves having the same frequency by temporally changing the phase difference) will be explained below. 
     In this method, power is fed to a discharge electrode via a plurality of feeding points, and the difference between a phase to one feeder distribution center and at least one phase to another is temporally changed. It is more preferable to use a phase shifter as a means for temporally changing the phase difference. This phase shifter is preferably inserted between an oscillator for determining the oscillation frequency of high-frequency power and an amplifier for amplifying the signal to necessary power. 
     To suppress a standing wave by using a plurality of power supplies, the one-dimensional modeling mentioned earlier must apply. As one practical condition, a plurality of feeding points of a discharge electrode are desirably arranged in symmetrical positions. 
     Also, when independent power supplies are used, the difference between VHFs does not stabilize to raise the problem of reproducibility in some cases. Therefore, it is desirable to ensure reproducibility by controlling the VHF difference to a constant value. 
     Furthermore, an isolator is preferably inserted between an impedance matching circuit and a power supply. This isolator reduces input power to the power supply from another power supply and thereby protects this power supply. The impedance matching circuit matches the impedances of a discharge electrode and the power supply. 
     The frequency band width of a practical isolator is about 4% for a high-frequency power of 1 kW or less and about 1% for a high-frequency power of about 2 kW. To build a system within this range, therefore, the difference between the frequencies of a plurality of high-frequency power supplies is preferably 4% or less, and more preferably, 1% or less of the average frequency. 
     Also, in accordance with the magnitude of input high-frequency power to each power supply from the discharge electrode side, the output from another power supply is restricted to reduce input power from this power supply. This prevents a VHF having a different frequency and/or phase from entering the former power supply and thereby prevents damage to the power supply. 
     To suppress a standing wave by using a plurality of power supplies, high-frequency waves having a plurality of frequencies are supplied from one feeder distribution center. This allows building a system more inexpensively than when the high-frequency waves are supplied from different feeding points. For this purpose, high-frequency power components from a plurality of high-frequency power supplies are mixed by a high-frequency mixer and supplied to a discharge electrode. 
     As a means for temporally changing the envelope function, different from the method using two frequencies or a temporally changing phase difference, it is possible to temporally change the voltage amplitude of high-frequency power (AM modulation), temporally change the frequency of high-frequency power (FM modulation), or perform frequency chirp. 
     It is favorable to previously measure at least one of a voltage distribution, plasma generation density distribution, radical generation density distribution, film formation distribution, etching distribution, and semiconductor film characteristic distribution with respect to the difference between a plurality of frequencies, the value of each frequency, the difference between phases, or the range of AM modulation, FM modulation, or frequency chirp, and obtain a necessary uniform distribution on the basis of the measurement result by using time average or time integral by adjusting at least one of the time, period, and frequency of power supply with respect to the difference between the specific frequencies, the value of each frequency, the difference between phases, or the range of AM modulation, FM modulation, or frequency chirp. 
     Since the envelope distribution of this system changes with time, nodes and antinodes move to turn on/off a plasma. This should not have any influence on the speed and quality of processing by the plasma as an object. Hence, the plasma must keep being ON in a pseudo manner. For this purpose, the cycle of plasma ON/OFF resulting from temporal change in the envelope distribution, i.e., a cycle equivalent to the reciprocal of the difference between the frequencies of a plurality of high-frequency power components, a cycle for changing the phase, or the cycle of AM modulation, FM modulation, or frequency chirp is made shorter than, preferably ½ or less the extinction life of an active atom, active molecule, or ion in a discharge plasma. This prevents the discharge plasma from uselessly repeating ON/OFF, so the speed and quality of processing are not influenced. 
     To keep the plasma ON state in a pseudo manner, the above cycle is determined as follows when a thin silicon film is to be formed by using silane. 
     Let τ denote the life of an SiH 3  active molecule calculated by 
     
       
         τ≈(Δ x ) 2 /(2 D )  (8) 
       
     
     where D is a diffusion coefficient (D=2.5×10 3  (cm 2 s −1 )), and Δx is the distance (cm) from an electrode to a substrate. 
     The cycle described above is made shorter than one or both of the life τ and the life of 1.1×10 −4  sec of a hydrogen atom radical. More specifically, the cycle is preferably ½ or less the life τ or the life of 1.1×10 −4  of a hydrogen atom radical. 
     On the other hand, for an application in which active atoms, active molecules, or ions in a plasma start to be generated in an OFF time after the plasma is generated, e.g., for an application to etching, it is possible to delay the cycle to intentionally form a plasma OFF time to hold an enough OFF time to generate active atoms, active molecules, or ions in the plasma, turn on the next plasma before the active atoms, active molecules, or ions in the former plasma reduce, and turn off the latter plasma, thereby efficiently generating the active atoms, active molecules, or ions. To this end, the cycle of plasma ON/OFF caused by a temporal change in the envelope distribution is made longer than and 10 times or less, preferably 2 to 4 times the generation life of active atoms, active molecules, or ions in a plasma to be generated by the discharge electrode. 
     Also, the particle generation amount is reduced by setting the cycle to 1 sec or less, preferably 1 msec or less. 
     Alternatively, the particle generation amount is reduced by making the cycle longer than, preferably twice or more a discharge region dwell time t of a source gas calculated by 
     
       
           t ≈( S·Δx )/ Q   (9) 
       
     
     where S is the substrate area (cm 2 ) 
     Δx is the distance (cm) from the discharge electrode to the substrate 
     Q is the volume flow rate (cm 3 /sec) 
     One desirable practical condition by which the one-dimensional modeling described above simply applies is that the discharge electrode is a ladder electrode or a mesh electrode. 
     Furthermore, to supply to a substrate electrode high-frequency power which is one of two frequencies for maintaining uniformity and which adjusts the energy of ions incident on the substrate, high-frequency power components are supplied from two or more high-frequency power supplies to each of a discharge electrode having a substrate and a discharge electrode having no substrate. 
     The discharge electrode preferably has dimensions of 500×500 mm or more, more preferably in the range of 500×500 mm to 2,200×2,200 mm, and most preferably in the range of 500×500 mm to 1,600 to 1,600 mm. 
     A substrate to be processed can be made of a glass, metal, or resin material. When the substrate is made of glass, the substrate is preferably heated to the temperature of range between 80° C. and 350° C. in plasma processing. Examples of the glass include soda-lime glass and silica glass. When the substrate is made of a metal, the substrate is preferably heated to the temperature of range between 80° C. and 500° C. in plasma processing. Examples of the metal include various kinds of stainless steel, aluminum, and an aluminum alloy. When the substrate is made of a resin, the substrate is preferably heated to the temperature of range between 80° C. and 200° C. in plasma processing. Examples of the resin include polyimide and polyethylene terephthalate (PET). 
     Additional objects and advantages of the invention will be set forth in the description which follows, and in part will be obvious from the description, or may be learned by practice of the invention. The objects and advantages of the invention may be realized and obtained by means of the instrumentalities and combinations particularly pointed out hereinafter. 
    
    
     BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWING 
     The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate presently preferred embodiments of the invention, and together with the general description given above and the detailed description of the preferred embodiments given below, serve to explain the principles of the invention. 
     FIG. 1A is a schematic view for explaining the flow of a high-frequency current when power is fed to an electrode by a conventional method, and FIG. 1B is a schematic view for explaining the flow of a high-frequency current when power is fed to an electrode by another conventional method; 
     FIGS. 2A and 2B are graphs for explaining a standing wave generated when two output high frequencies from two-output variable-phase high-frequency oscillator are fed with a phase difference of 0° to an electrode by a conventional method; 
     FIG. 3 is a graph showing a voltage distribution and an ion saturation current distribution resulting from a standing wave generated when a high frequency of 100 MHZ is fed to one point of an electrode; 
     FIG. 4 is a graph showing voltage distributions formed on a ladder electrode when high frequencies of 60 and 100 MHz are fed to the electrode by using a conventional four-point feeding method; 
     FIG. 5 is a graph showing a voltage distribution formed on a parallel plate electrode when a high-frequency power of 100 MHz is fed to the electrode by a conventional feeding method with one end of the electrode terminated by a lossless reactance (coil); 
     FIG. 6A is a graph showing the correlation between a film thickness distribution and a power-supply frequency when a film is formed on a substrate (500 mm×500 mm) by using a conventional method, and FIG. 6B is a graph showing the correlation between a film thickness distribution and a power-supply frequency when a film is formed on a substrate (1,000 mm×1,000 mm) by using a conventional method; 
     FIG. 7A is a view showing the waveform of a high-frequency wave φ 1 , FIG. 7B is a view showing the waveform of a high-frequency wave φ 2 , and FIG. 7C is a view showing the waveform and envelope of a synthetic wave φ; 
     FIG. 8 is a plan block diagram showing a discharge plasma generating apparatus according to the first embodiment of the present invention; 
     FIG. 9 is a graph showing the result of measurement of the emission intensity distribution of a plasma generated by a method of the first embodiment; 
     FIGS. 10A to  10 C are tree-dimensional graphs each showing the distribution of the amplitude of a discharge electrode in the lateral and longitudinal directions of the electrode; 
     FIG. 11A is a graph showing the correlation between the distance from a feeder distribution center and a progressive wave voltage amplitude index and the correlation between the position from a reflection point and a reflected wave voltage amplitude index, FIG. 11B is a graph showing the correlation between the distance from a feeder distribution center and a standing wave voltage amplitude index, and FIG. 11C is a graph showing the correlation between the distance from one feeder distribution center, when power is supplied from the two ends of an electrode, and a synthetic wave voltage amplitude index; 
     FIG. 12 is a graph showing the correlation between a high frequency and the distance from a feeder distribution center before the high frequency attenuates to a certain value; 
     FIG. 13 is a graph showing the correlation between the difference between two high frequencies and a film thickness distribution (a film thickness variation); 
     FIG. 14 is a plan block diagram showing a discharge plasma generating apparatus according to the second embodiment (or the 13th embodiment) of the present invention; 
     FIG. 15 is a block diagram showing a feeder circuit of an apparatus used in a method of feeding power to a discharge electrode according to the third embodiment of the present invention; 
     FIG. 16 is an enlarged view of a portion where a feeding terminal is attached to an electrode; 
     FIG. 17 is a sectional block diagram showing, in an enlarged scale, the portion where the feeding terminal is attached to the electrode; 
     FIG. 18 is a three-dimensional view showing a film formation rate distribution with a phase difference of 0°; 
     FIG. 19 is a three-dimensional view showing a film formation rate distribution with a phase difference of 90°; 
     FIG. 20 is a timing chart showing the control pattern of a phase shifter phase difference for obtaining a uniform distribution; 
     FIG. 21 is a plan block diagram showing a discharge plasma generating apparatus according to the fourth embodiment of the present invention; 
     FIG. 22 is a plan block diagram showing a discharge plasma generating apparatus according to the fifth embodiment of the present invention; 
     FIG. 23 is a block diagram showing a feeder circuit of a discharge plasma generating apparatus according to the sixth embodiment of the present invention; 
     FIG. 24 is a block diagram showing a feeder circuit of a discharge plasma generating apparatus according to the seventh embodiment of the present invention; 
     FIG. 25 is a block diagram showing a feeder circuit of a discharge plasma generating apparatus according to the eighth embodiment of the present invention; 
     FIG. 26A is a graph showing an example of a frequency spectral distribution used to generate an arbitrary wavelength in implementing a method (a two-frequency method) of applying two or more high frequencies to the same electrode by using an arbitrary waveform generator, and FIG. 26B is a graph showing the envelope of a temporal change in the voltage generated by the arbitrary waveform generator, which is generated on the basis of the frequency spectral distribution; 
     FIG. 27 is a plan block diagram showing a discharge plasma generating apparatus according to the ninth embodiment of the present invention; 
     FIG. 28 is a plan block diagram showing a discharge plasma generating apparatus according to the 10th embodiment of the present invention; 
     FIG. 29 is a sectional block diagram showing the apparatus of the 10th embodiment; 
     FIG. 30 is a perspective block diagram showing the apparatus of the 10th embodiment; 
     FIG. 31 is a block diagram showing a feeder circuit of a discharge plasma generating apparatus according to the 11th embodiment of the present invention; 
     FIG. 32 is a plan block diagram showing a discharge plasma generating apparatus according to the 12th embodiment of the present invention; 
     FIG. 33 is a plan block diagram showing a discharge plasma generating apparatus according to the 14th embodiment of the present invention; 
     FIG. 34 is a perspective block diagram showing a feeder circuit of a discharge plasma generating apparatus according to the 15th embodiment of the present invention; 
     FIG. 35 is a sectional block diagram showing an outline of an apparatus used in a method of Comparative Example 1; 
     FIG. 36 is a sectional block diagram showing an outline of an apparatus used in a method of Comparative Example 2; 
     FIG. 37 is a perspective view showing a power distributor of the apparatus shown in FIG. 36; 
     FIG. 38 is a sectional block diagram showing an outline of an apparatus used in a method of Comparative Example 3; and 
     FIG. 39 is a plan view showing an outline of a discharge electrode of the apparatus shown in FIG. 38 and a feeding method. 
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     Various preferred embodiments of the present invention will be described below with reference to the accompanying drawings. 
     First Embodiment 
     In the first embodiment, a high-frequency plasma CVD apparatus  1 A shown in FIG. 8 is used. This apparatus  1 A includes a reaction vessel  2 , a ladder electrode (a discharge electrode)  303 , a ground electrode  3 , two high-frequency power supplies  5   a  and  5   b , a gas supply unit  71 , an exhaust unit  72 , and a controller  73 . The reaction vessel  2  is made airtight, and a gas supply pipe  17  and an exhaust pipe  18  open in appropriate portions of this vessel  2 . 
     The gas supply pipe  17  communicates with the gas supply unit  71 . The gas supply unit  71  incorporates a gas supply source and a mass-flow controller. The gas supply source contains process gases which contain film formation components. The process gases are, e.g., an Si-containing gas such as monosilane or disilane and an additive component gas such as hydrogen gas. The power switch of the mass-flow controller is connected to an output portion of the controller  73 . 
     The exhaust pipe  18  communicates with the exhaust unit  72 . The exhaust unit  72  houses a vacuum pump and a device for making toxic substances harmless. The power switch of the vacuum pump is connected to the output portion of the controller  73 . This vacuum pump can reduce the internal pressure of the reaction vessel  2  to less than about 1×10 −6  Torr. 
     The ground electrode  3  and the ladder electrode  303  are opposed with a clearance of, e.g., 20 mm between them. The ground electrode  3  includes a mechanism (not shown) for holding a glass substrate G to be processed and contains a heater (not shown) for heating this substrate G. When the dimensions of the substrate G are 2.0 m×1.4 m, the dimensions of the ground electrode  3  are 2.2 m×1.6 m. The gas supply pipe  17  preferably has a plurality of gas inlet ports. These gas inlet ports are desirably formed behind the ladder electrode  303  so as to form laminar flows of the process gases. 
     The ladder electrode  303  is formed by assembling a plurality of (e.g.,  17 ) parallel longitudinal rods  304  and one or more pairs of parallel lateral rods  305  into the form of a lattice. This ladder electrode  303  is opposed parallel to the substrate G which is held by the ground electrode  3 . The longitudinal rods  304  are arrayed at equal pitches in the Y-axis direction, and the lateral rods  305  are arrayed at equal pitches in the X-axis direction. The length in the X-axis direction of the ladder electrode  303  is about 2.2 m, and its length in the Y-axis direction is about 1.6 m. 
     The ladder electrode  303  has eight first feeding points  9   a  and eight second feeding points  9   b   1 . The first feeding points  9   a  are formed at nodes between the lateral rods  305  and the longitudinal rods  304  on one side. The second feeding points  9   b   1  are formed at nodes between the lateral rods  305  and the longitudinal rods  304  on the other side. These first and second feeding points  9   a  and  9   b   1  are formed at substantially equal pitches. 
     The first feeding points  9   a  are connected to a first distributor  26   a  by coaxial cables  8   b . To this first distributor  26   a , an impedance matching circuit  7   a , a power meter  6   a , and the first power supply  5   a  are connected in this order by a coaxial cable  8   a . The first power supply  5   a  contains a high-frequency oscillator whose frequency is set to 60 MHz, and supplies VHF power to the ladder electrode  303  via the eight first feeding points  9   a.    
     The second feeding points  9   b   1  are connected to a second distributor  26   b  via coaxial cables  8   b . To this second distributor  26   b , an impedance matching circuit  7   b , a power meter  6   b , and the second power supply  5   b  are connected in this order. The second power supply  5   b  is independent of the first power supply  5   a  and houses a high-frequency oscillator whose frequency is also set to 60 MHz. This second power supply  5   b  supplies VHF power to the ladder electrode  303  via the eight second feeding points  9   b   1 . 
     When the actual frequencies of these two power supplies were measured with a high-accuracy spectrum analyzer, the power supplies  5   a  and  5   b  output high frequencies of 59.8 MHz and 60.3 MHz, respectively. The actual oscillation frequency usually thus deviates from the set frequency, and this is because different oscillators have different characteristics. 
     Accordingly, different VHFs of 59.8 MHz and 60.3 Hz are supplied to the ladder electrode  303  from the two power supplies  5   a  and  5   b  via the first and second feeding points  9   a  and  9   b   1  facing each other. In the present invention, the difference (0.5 MHz) between the two VHFs is important. 
     In this embodiment, the first and second feeding points  9   a  and  9   b   1  were arranged symmetrically with respect to the central line of the ladder  303 , thereby generating a one-dimensional voltage distribution on each of the longitudinal rod  304 . This caused a phenomenon (to be described later) which moved an envelope at high speed. Consequently, it was possible to uniformize the longitudinal plasma generation distribution on the longitudinal rods  304  and the plasma generation distribution (a plasma distribution in the X-axis direction) between the longitudinal rods  304 . 
     In this embodiment, the number of each set of feeding points is eight (sixteen in total). However, the plasma generation distribution in the X-axis direction (the longitudinal direction of the electrode) can be further uniformized by increasing the number of feeding points to twelve (twenty four in total) or to sixteen (thirty two in total). The effects of the present invention are of course found even when the number of feeding points is decreased to six (twelve in total), five (ten in total), four (eight in total), three (six in total), two (four in total), and one (two in total). 
     Also, in this embodiment power components are fed to the different feeding points from the two power supplies. However, the discharge plasma density can be made more uniform by increasing the number of power supplies. For example, the uniformity of the discharge plasma density can be improved by supplying high-frequency power components having different frequencies from four power supplies to different feeding points. 
     FIG. 9 is a graph showing a characteristic curve E obtained by measuring, with a CCD camera, the emission intensity of a plasma generated by using the apparatus  1 A of this embodiment. In FIG. 9, a position index (an arbitrary value) on the ladder electrode is plotted on the abscissa, and an emission intensity index (an arbitrary value) is plotted on the ordinate. Referring to FIG. 9, three low-value portions inside the substrate size are behind structures of the apparatus, so the plasma in these portions cannot be seen. Therefore, these portions have no connection with the actual emission intensity distribution. This characteristic curve E shows that in the generation of a discharge plasma using the apparatus  1 A, a uniformity of ±7% (a maximum value of 127/a minimum value of 111) of an emission distribution, i.e., a plasma distribution can be achieved in a very large region of 2 m×1.4 m. 
     The discharge plasma is thus uniformized because “hum (beat)” resulting from 0.5 MHZ as the difference between the first VHF (59.8 MHz) and the second VHF (60.3 MHz) suppresses the generation of a standing wave A 3  on the electrode. That is, as explained in item (a) in “BRIEF SUMMARY OF THE INVENTION”, an envelope is changed 0.5 million times for 1 sec, i.e., moved at high speed over the distance of 500,000 wavelengths. Therefore, although the envelope has a waveform similar to the standing wave A 3  for a very short time period, the amplitude of a voltage can be regarded as having a uniform distribution on time average. So, a plasma generated by this voltage has a substantially uniform distribution. The amplitude of a voltage is the maximum value of the voltage at a certain point. 
     This can also be considered as follows. Two high-frequency waves supplied to the electrode, i.e., a high-frequency wave (to be referred to as a high-frequency wave A hereinafter) supplied from the power supply  5   a  via the eight first feeding points  9   a  and a high-frequency wave (to be referred to as a high-frequency wave B hereinafter) supplied from the power supply  5   b  via the eight second feeding points  9   b   1  do not interfere with each other because they have different frequencies. Therefore, the amplitude distribution of the voltage of the high-frequency wave A and the amplitude distribution of the voltage of the high-frequency wave B are independent of each other. The actual voltage distribution is the superposition of the two. 
     Assuming that the attenuation of a high-frequency wave can be neglected and the reflection at the electrode end is negligibly small, the high-frequency waves A and B uniformly progress with no attenuation from the two ends of the longitudinal rods  304 , so the superposition of the two high-frequency waves forms a uniform distribution. This is the gist of this embodiment. 
     In practice, however, the phenomenon is slightly complicated because attenuation and reflection do occur, so these attenuation and reflection will be described below. First, attenuation will be explained. When attenuation occurs, the amplitude distribution of the voltage of the high-frequency wave A is indicated by R 1  shown in FIG.  10 A. Referring to FIG. 10A, the direction of the lateral rods  305  is the Y axis, the direction of the longitudinal rods  304  is the X axis, and the amplitude of the voltage is the Z axis. In the direction (the Y axis) of the lateral rods  305 , the voltage amplitude is substantially constant because the eight feeding points  9   a  are closely arranged. On the other hand, in the direction (the X axis) of the longitudinal rods  304 , the voltage amplitude attenuates from the feeding side, and this produces a distribution. As indicated by R 2  shown in FIG. 10B, the amplitude of the voltage of the high-frequency wave B also attenuates from the opposite feeding side. As indicated by R 3  in FIG. 10C, the distribution of the amplitude of the voltage formed by synthesizing the high-frequency waves A and B has high uniformity. Accordingly, a plasma having a substantially uniform distribution density is generated. 
     Since reflection at the electrode end cannot be neglected in practice, this reflection at the electrode end will also be explained in addition to the above attenuation. Referring to FIG. 11A, the distance (cm) from the feeding points in the direction of the longitudinal rods  304  is plotted on the abscissa, and the amplitude distribution of the voltage of the high-frequency wave A is plotted on the ordinate. FIG. 11A does not show the distribution in the direction of the lateral rods  305  because this distribution is substantially uniform as indicated by R 1  in FIG. 10A, and shows only one-dimensional distribution in the Y-axis direction of the longitudinal rods  304 . A progressive wave G 1  of the high-frequency wave A progresses toward the electrode end while attenuating from the feeding points. Since reflection occurs at the electrode end, the high-frequency wave A is reflected at the electrode end to form a reflected wave H, and this reflected wave H progresses to the feeding points. FIG. 11B shows the amplitude distribution of a voltage generated by the synthesis of the progressive wave G 1  and the reflected wave H. Since the progressive wave G 1  and the reflected wave H have the same frequency and interfere with each other, addition taking account of the phase is necessary. A synthetic wave G 2  does not monotonously attenuate and has a standing-wave-like distribution. FIG. 11B shows that a minimal point is generated near 120 cm. The high-frequency wave B also forms a similar distribution. Since the high-frequency waves A and B have different frequencies and hence do not interfere with each other, they can be simply synthesized by addition, and a substantially uniform distribution as shown in FIG. 11C is obtained. In this embodiment, a reflected wave H of a synthetic wave G 3  was small, resulting in a slight standing-wave-like distribution. Therefore, a substantially uniform voltage distribution was finally obtained, so a uniform plasma was generated. 
     As described above, in this embodiment a substantially uniform distribution was obtained because the reflected wave H was small and had little influence. However, if a high-frequency wave (e.g., the high-frequency wave A) fed from one end does not attenuate before reaching the other end, a reflected wave generated by the reflection of this high-frequency wave interferes with the progressive wave. Since this makes the standing wave appreciably large, no uniformity can be obtained any longer. Hence, a high-frequency wave preferably sufficiently attenuates before arriving at the other end. More specifically, when at the other end of the electrode the voltage of a progressive wave attenuates to about 50% of that at the feeding points, the reflected wave H generated there becomes about 25% (=50%×½) as shown in FIG. 11A, so a substantially uniform voltage distribution is obtained. If the voltage of a progressive wave attenuates to about 75%, the film thickness distribution is not substantially affected although a slight voltage distribution is formed. 
     Referring to FIG. 12, the abscissa indicates the VHF frequency (MHz), and the ordinate indicates the distance (cm) from the feeding points. A characteristic curve J shows the distance the progressive-wave voltage attenuates to about 50%, which is approximated by equation L=4×10 3 /f. A characteristic curve K shows the distance the progressive-wave voltage attenuates to about 75%, which is approximated by equation L=2×10 3 /f. Accordingly, the length L of the electrode from one end as a feeder distribution center (incident point) to the other end as a reflection point satisfies preferably inequality L≧2×10 3 /f, and more preferably, L≧4×10 3 /f. Within the range of equation L&gt;20×10 3 /f, attenuation is too large, and no uniformization is possible. Therefore, L≦20×10 3 /f is preferably met. 
     Symbol f represents a VHF (MHz). 
     The frequency difference between the high-frequency waves A and B will be described below by returning to the concept of high-speed movement of an envelope. The larger this frequency difference, the higher the speed at which an envelope is moved. However, to obtain a desired film formation rate and film formation quality, it is undesirable to use a high-frequency wave B with a frequency having a difference of 20% or more from that of the high-frequency wave A. Also, to allow an impedance matching circuit to function which is used to prevent incidence of VHF power to a power supply, the difference between the two VHFs is more preferably 1% or less. 
     In this embodiment, the difference between the two VHFs was about 0.8%. Therefore, the film formation rate and quality were high, and incidence of a high-frequency wave to the power supply could be suppressed to a low value, about 100 W. 
     The above apparatus  1 A was used to form a thin Si semiconductor film (an a-Si film or a nanocrystalline Si film) for a solar cell on a glass substrate following the procedures described below. 
     First, the temperature of the ground electrode  3  was set to 200° C. by heating by the heater. 2 m×1.4 m substrate G was placed on this ground electrode  3 . SiH 4  gas was supplied at a flow rate of 2,000 sccm from the gas supply unit  71  into the reaction vessel  2 . In the case of nanocrystalline Si film formation, hydrogen gas was supplied at, e.g., 50,000 sccm in addition to the SiH 4  gas. The operation of the exhaust unit  72  was controlled by the controller  3  to adjust the internal pressure of the reaction vessel  2  to 200 mTorr. 
     While the first and second impedance matching circuits  7   a  and  7   b  were so adjusted as to allow efficient supply of VHF power to a plasma, VHF power at a frequency of 59.8 MHz was supplied from the first power supply  5   a , and VHF power at a frequency of 60.3 MHz was supplied from the second power supply  5   b . These VHF power components were supplied to the ladder electrode  303  such that the total power from the two power supplies  5   a  and  5   b  was, e.g., 3,000 W, thereby generating a discharge plasma between the substrate G and the ladder electrode  303 . In this discharge plasma, SiH 4  decomposed to form an a-Si film or a nanocrystalline Si film on the surface of the substrate G. That is, a thin film having a desired film thickness was formed by performing film formation in this state for, e.g., about 10 min. The film thickness distribution of the formed film sample was measured, and the feeder distribution center positions were finely adjusted so that an optimum distribution was obtained. The film formation rate was as high as 1.0 nm/sec in the formation of a nanocrystalline film, and the uniformity was slightly over ±10%. That is, the uniformity necessary for an Si thin-film semiconductor of a solar cell was achieved. 
     In this arrangement, different VHFs are unintentionally supplied by using different power supplies. However, intentionally setting different frequencies is of course similarly effective. 
     FIG. 13 is a graph showing the correlation between the frequency difference (MHz) between two high-frequency waves and the film thickness distribution (%) of a film formed on a substrate, by plotting the frequency difference on the abscissa and the film thickness distribution on the ordinate. While the frequency of the high-frequency wave A was fixed to 60.0 MHz (a fundamental frequency), the frequency of the high-frequency wave B was changed to form a-Si films on 2.0 m×1.4 m rectangular glass substrates. As is apparent from a characteristics curve F, the film thickness distribution was 10% or less when the frequency difference between the two high-frequency waves A and B was 1.5 to 6.0 MHz. Also, the film thickness distribution was lower than 15% when the frequency difference was 1.0 to 10.0 MHz and lower than 20% when the frequency difference was 0.5 to 10.0 MHz. Furthermore, even when the frequency difference was only 0.1 MHz, the film thickness distribution exceeded 20% only slightly. 
     Furthermore, when the film thickness of a thin silicon film formed on a large-area substrate G (2 m×1.4 m) was measured by Raman spectroscopy, the peak ratio of a Raman spectrum exceeded 9:1. This proves that the film had high quality as a thin film for a solar cell. Also, the refractive index, spectral characteristics, and defect density of the thin film were measured. Consequently, the measured values were substantially equal to values measured when a film was formed on a small-area sample substrate (5 cm×5 cm) by using the same VHF (60 MHZ). 
     A high-quality thin film is formed on the large-area substrate G as described above because plasma ON/OFF caused by the high-speed movement of an envelope is much shorter than the life of active species (radicals). That is, in this embodiment the difference between the two VHFS is 0.5 MHz. Therefore, ON/OFF is repeated 500,000×2 times per second, and one OFF time is 1×10 −6  sec. This OFF time is much shorter than the extinction life ((τ=(2 (cm)) 2 /(2×2.5×10 3  (cm 2 /sec))=8×10 −4  sec) of an SiH 3  active molecule, and is much shorter than the extinction life (1.1×10 −4  sec) of a hydrogen atom radical. Accordingly, ON/OFF of the plasma is substantially negligible in the actual film formation. 
     Note that another effect obtained by this embodiment is the very small amount of particles produced during the film formation. This is presumably because, as described in “Silane Gas Decomposition by High-Frequency Modulation Discharge”, Discharge Research No. 138, pp. 27 to 36, 1992 (to be referred to as reference  7  hereinafter), substantially no particles are produced when the ON/OFF frequency is in the range of 0.5 Hz (inclusive) to 100 kHz (inclusive), i.e., the ON time is in the range of 0.01 msec (inclusive) to 1 sec (inclusive), and preferably when the ON/OFF frequency is 10 kHz or less, i.e., the ON time is 0.1 msec or more. That is, since the growth time of particles is about 1 sec, no particles increase for an ON time of 1 sec or less. However, when the ON/OFF frequency is 100 kHz or more, i.e., when the OFF time is 0.01 msec or less, a state in which plasma is not regarded to be off is set. That is, in this embodiment almost no particles were produced when the ON/OFF frequency was set to 10 kHz, i.e., when the ON time was set to 0.1 msec. 
     Furthermore, it is also possible to prevent an increase in particles by discharging particles over a sufficient time by prolonging the OFF time. That is, when a substrate area S is 200×200 cm 2 , a distance Δx from the discharge electrode to the substrate is 2 cm, and a volume flow rate Q is 4×10 5  cm 3 /sec, a discharge region dwell time t of a source gas is calculated to be 0.2 sec by substituting these values into equation (10) below. Therefore, by setting the OFF time to be longer than the time t, i.e., 0.2 sec or more, preferably twice the time t, i.e., 0.4 sec or more, it was possible to discharge particles from the plasma generation region and suppress an increase in particles in the reaction vessel. 
     
       
           t ≈( S·Δx )/ Q   (10) 
       
     
     In this embodiment, a ladder electrode was used as the electrode. When a mesh electrode reported in the reference  4  cited previously was used instead of the ladder electrode, a film thickness uniformity of 10% or less could be obtained. This electrode is a kind of a ladder electrode and has a large number of lateral electrode rods  305  according to this embodiment. 
     Also, this embodiment has been explained by taking the use of VHFs around 60 MHz as an example. However, analogous effects were obtained even when VHFs around 20, 200, and 700 MHz were used. 
     Second Embodiment 
     The second embodiment of the present invention will be described below with reference to FIG.  14 . An apparatus  1 B of this embodiment is obtained by partially changing the VHF feeder circuit of the apparatus  1 A of the first embodiment described above. This change in the feeder circuit permits the apparatus  1 B to have an operation condition range wider than that of the apparatus  1 A. Also in this embodiment, the apparatus is used to form a uniform film on a 2 m×1.4 m substrate by using VHFs, and the arrangements of a reaction vessel and the like except for a power-supply system are the same as in the first embodiment. So, an explanation of points common to the two embodiments will be omitted. 
     The apparatus  1 B of the second embodiment differs from the apparatus  1 A of the first embodiment in four points {circle around (1)} to {circle around (4)} below. 
     {circle around (1)} The oscillation frequencies of high-frequency power supplies. In the apparatus  1 A, two different frequencies are generated by using the uncertainty of the built-in quartz oscillators of the high-frequency power supplies  5   a  and  5   b . In the apparatus  1 B, a two-wave signal generator  20 B controls the frequency difference to a constant value. In the former apparatus (the apparatus  1 A), no arbitrary frequency difference can be selected. Accordingly, if the two oscillators have a frequency difference of only 10 Hz, the envelope distribution moves only 10 Hz, so a plasma turns on/off at this cycle to adversely affect film formation. Also, the oscillation frequency difference does not stabilize with time. This may result in low reproducibility. In contrast, the latter apparatus (the apparatus  1 B) can be operated with a fixed optimum frequency difference. 
     {circle around (2)} In the apparatus  1 A, protection circuits (not shown) of the two high-frequency power supplies  5   a  and  5   b  are also independent of each other. However, the apparatus  1 B has only one protection circuit  22 . Input power components to power supplies  5   a  and  5   b  are measured by power meters  6   a   1  and  6   b   2  and, if one of the two magnitudes exceeds a limiting value, the outputs from both the power supplies are restricted. In the former apparatus (the apparatus  1 A), if the input power (the sum of the reflected power and the input power from the second power supply  5   b ) to the first power supply  5   a  exceeds the tolerance of the first power supply  5   a  for some reason, the protection circuit of this first power supply suppresses the output from the first power supply  5   a . However, the excess input from the second power supply  5   b  is not suppressed at all and kept supplied. Hence, in the worst case the first power supply  5   a  is damaged. 
     In contrast, if the same even occurs in the latter apparatus (the apparatus  1 B), the excess input to the first power supply  5   a  activates the protection circuit  22  to suppress the outputs from both the first and second power supplies  5   a  and  5   b . Since the input power to the first power supply  5   a  is suppressed, this first power supply  5   a  is not damaged. While the input power is thus suppressed, an impedance matching circuit  7   b  is adjusted to remove the cause of the excess input from the second power supply  5   b . This makes it possible to again increase the outputs from the two power supplies  5   a  and  5   b  and supply desired power. 
     In the apparatus  1 B, isolators  24   a  and  24   b  are inserted into first and second feeder circuits to prevent excess input power components to the power supplies  5   a  and  5   b , respectively. Hence, no protection circuit is particularly necessary. However, if the reflected power exceeds the allowable power of the isolators  24   a  and  24   b  to make these isolators  24   a  and  24   b  inoperable, the protecting operation by this protection circuit  22  is required. 
     {circle around (3)} In the apparatus  1 A, the impedance matching circuit  7   a  is the only means for suppressing the input power (the sum of the reflected power and the input power from the second power supply  5   b ) to the first power supply  5   a . In the apparatus  1 B, however, the isolators  24   a  and  24   b  each comprising a circulator and load are inserted to eliminate the input power from the electrode  303  to the power supplies  5   a  and  5   b.    
     In the former apparatus (the apparatus  1 A), even when the power generated by reflecting the output from the first power supply  5   a  by the electrode  303  can be completely reduced to zero by the impedance matching circuit  7   a , the input power from the other power supply, i.e., the second power supply  5   b  via the electrode  303  and the impedance matching circuit  7   a  cannot be simultaneously reduced to zero, because the phases and frequencies are different. Therefore, if this power is large (the power transmitted through the electrode  303  varies, i.e., increases or decreases, in accordance with the generated state of a plasma), large power is input to the first power supply  5   a  to make the state of this first power supply  5   a  unstable. In the worst case, an excess input may destroy the first power supply  5   a . This situation readily occurs especially when there is no plasma load before plasma generation. 
     In contrast, in the latter apparatus (the apparatus  1 B) the isolators  24   a  and  24   b  are inserted into the feeder circuits. Accordingly, inputs to the power supplies  5   a  and  5   b  can be completely absorbed by the loads, and this prevents destruction of the power supplies  5   a  and  5   b  by an excess input. 
     The frequency band width of an isolator, especially the isolators  24   a  and  24   b  having kW-class high-frequency power as a rated value as used in this embodiment, is very narrow. That is, the frequency band width at a high-frequency power of 1 kW or less is about 4% of the frequency used, and that at a high-frequency power of about 2 kW is about 1% of the frequency used. Hence, the frequency difference between the first and second power supplies  5   a  and  5   b  must be decreased to these values. In this embodiment, the oscillation frequency of the first power supply  5   a  is set at 60.2 MHz, and the oscillation frequency of the second power supply  5   b  is set at 59.8 MHz. Consequently, the oscillation frequency difference between the two power supplies  5   a  and  5   b  is set to 0.6 MHz or less which corresponds to a frequency band width of 1% at a rated power of 2 kW. 
     {circle around (4)} In the apparatus  1 A, each system includes one of the two power meters  6   a  and  6   b  (two power meters in total). In the apparatus  1 B, one system includes the two power meters  6   a   1  and  6   a   2 , and another system also includes two power meters  6   b   1  and  6   b   2  (four power meters in total). Since the isolators  24   a  and  24   b  are inserted into the feeder circuits, input power components to the power supplies  5   a  and  5   b , i.e., the reflected power components in the power meters  6   a   1  and  6   a   2  are normally zero regardless of the impedance matching state. To optimize the impedance matching state, therefore, it is necessary to arrange the power meters  6   a   2  and  6   b   2  closer to the impedance matching circuits than the isolators  24   a  and  24   b  and measure the return power components from the impedance matching circuits  7   a  and  7 b .    
     Although the above improvements complicated the apparatus, a total input power of 4 kW was obtained. Hence, a high film formation rate of 1.5 nm/sec was obtained in, e.g., nanocrystalline film formation. The film thickness uniformity was ±10%. This clears the film thickness uniformity requirement necessary for an Si thin-film semiconductor of a solar cell. 
     Third Embodiment 
     The third embodiment of the present invention will be described below with reference to FIGS. 15 to  20 . 
     As shown in FIG. 15, a plasma CVD apparatus  1 C comprises a vacuum chamber  2 C for surrounding a substrate G, a ladder electrode  303  opposed to the substrate G in this vacuum chamber  2 C, and a feeder circuit  8 A for feeding power to this ladder electrode  303 . The vacuum chamber  2 C communicates with a vacuum pump via an exhaust passage (not shown) and is evacuated to about an internal pressure of 1×10 −3  to 1×10 −7  Torr. Also, a gas supply pipe (not shown) is placed behind the electrode  303  in the vacuum chamber  2 C. When silane or disilane is supplied as a film formation process gas from a gas supply source to the gas supply pipe, this process gas is supplied from a large number of inlet ports to a space between the electrode  303  and the substrate G. 
     The substrate G is held by a ground electrode  3  and heated to a predetermined temperature region by a built-in heater (not shown). AS this substrate G, a transparent glass substrate 1 mm thick, 460 mm wide, and 460 mm long was used. 
     The ladder electrode  303  as a discharge electrode is formed by assembling round rod electrode members at equal pitches into the form of a lattice. This ladder electrode  303  is connected to a feeder (central conductor)  6  of the circuit  8 A by four feeding points  9   a  and  9   b . The two feeding points  9   a  are formed in positions which divide the round rod electrode member placed at one end into three substantially equal parts. The other two feeding points  9   b  are formed in positions which divide the round rod electrode member placed at the other end into three substantially equal parts. The ladder electrode  303  has dimensions of, e.g., 520 mm×520 mm, and the round rod electrode member has a diameter of, e.g., 6 mm. 
     The feeder circuit  8 A includes a high-frequency oscillator  20 , a distributor  26 , a phase shifter  42 , a pair of amplifiers  41   a  and  41   b , and a pair of impedance matching circuits  7   a  and  7   b . The high-frequency oscillator  20  is connected to the amplifiers  41   a  and  41   b  via the distributor  26 . The amplifiers  41   a  and  41   b  are connected to the impedance matching circuits  7   a  and  7   b  which are connected to the feeding points  9   a  and  9   b , respectively. 
     An output circuit of the distributor  26  branches into two parts, and one of these branched circuits  8 A includes the phase shifter  42  driven and controlled by a computer  43 . Each branched circuit  8 A further branches into two circuits  8   a  and  8   b . These branched circuits  8   a  and  8   b  are connected to the electrode  303  via the feeding points  9   a  and  9   b , respectively. 
     A quartz oscillator having a rated frequency of 60 MHz was used as the high-frequency oscillator  20 . A full solid-state element type analog voltage-controlled phase shifter was used as the phase shifter  42 . The high-frequency oscillator  20  oscillates a very high frequency (VHF), and this VHF is distributed by the distributor  26  and fed to the electrode  303  via the amplifiers  41   a  and  41   b , the impedance matching circuits  7   a  and  7   b , and the feeding points  9   a  and  9   b . on the basis of a predetermined processing data signal transmitted from the computer  43 , the phase shifter  42  performs high-speed phase modulation for one distributed VHF at a repetition rate of a maximum of 100 kHz. 
     As shown in FIGS. 16 and 17, the feeder (central conductor)  6  is passed through a coaxial cable  61  and connected to the electrode  303  by the feeding points  9   a  and  9   b . An insulator  63  is mounted on the end portion of the coaxial cable  61  by a coupling  62 , thereby insulating the electrode  303  from the sheath of the cable  61 . A plurality of holes  64  are formed in side portions of the insulator  63 . A gas passage  66  in the coaxial cable  61  communicates with a gas supply source  68  and the holes  64  of the insulator. The gas supply source  68  contains industrially pure hydrogen gas H 2 . This hydrogen gas is supplied from the gas supply source  68 , passed through the gas passage  66  in the cable  61 , and blown off from the side holes  64  and an upper-end hole  65 , thereby blowing away a silane plasma existing at the feeding points  9   a  and  9   b  and its vicinity. Simultaneously, a plasma having a high hydrogen concentration etches unnecessary film formation components deposited on the insulator  63  and the like near the feeder distribution center. The blow of this hydrogen gas effectively prevents the deposition of unnecessary film formation components and the generation of particles near the feeding points  9   a  and  9   b  as an electric field concentrated portion. 
     In the above embodiment, the deposition of film formation components and the generation of particles are prevented by blowing pure hydrogen gas against each feeder distribution center. However, the present invention is not limited to this embodiment. That is, a similar effect can be obtained by blowing another gas such as argon gas against each feeder distribution center. 
     Furthermore, the method of the present invention is applicable not only to feeding points but also to parts where the deposition of unnecessary film formation components and the generation of particles are undesirable. For example, if a silicon film is deposited on an insulator pillar for supporting an electrode, the creeping insulation strength of the pillar lowers. In the worst case, a line-to-ground fault occurs. When a hydrogen local supply method analogous to the one described above was performed for this pillar, deposition was suppressed and no line-to-ground fault occurred. 
     The formation of a nanocrystalline Si film on a glass substrate using the plasma CVD film forming apparatus will be described below. 
     The film formation conditions were substrate dimensions of 46 cm×46 cm, a substrate temperature of 200° C., a reaction vessel internal pressure of 150 mTorr, a silane gas supply amount of 50 sccm, and a hydrogen gas supply amount of 1,500 sccm. 
     When the frequency of high-frequency power was set at 60 MHz and the distance between electrode and substrate was set at 10 mm in this apparatus, a standing wave was generated by the conventional feeding method, and no uniform film formation was possible. 
     FIGS. 18 and 19 are three-dimensional graphs showing film formation rate distributions when the phase difference is set to constant values of 0° and 90°, respectively, by a phase modulator. Referring to FIGS. 18 and 19, the positions on a substrate with respect to the discharge electrode are plotted on the X and Y axes, and the deposition rate (nm/sec) is plotted on the ordinate. As shown in FIGS. 18 and 19, with the fixed constant phase difference an envelope remains still as a standing wave to produce a deposition rate distribution. FIGS. 18 and 19 also reveal that the deposition rate distribution can be changed by changing the phase difference. This is principally because the change in the phase difference changes the envelope distribution (varies the nodes and antinodes of the standing wave distribution). 
     In this embodiment, therefore, high-frequency power components are supplied from two feeding systems, and the phase difference between them is changed with time, thereby moving the envelope and obtaining a uniform film thickness distribution by time quadrature. This is equivalent to case (b) (the method of supplying high-frequency waves having the same frequency while changing the phase difference with time) in “BRIEF SUMMARY OF THE INVENTION”. 
     If the above phase difference is slowly changed, active molecules or atoms in the plasma increase or decrease accordingly. Therefore, the arrival flux of these molecules or atoms with respect to the substrate varies with time, and this raises or lowers the deposition rate. In the worst case, a state equivalent to plasma OFF by which no film is formed appears. Additionally, the quality of deposited films temporally changes, and this change sometimes influences the quality of the film finally formed. This is a problem in a nanocrystalline type silicon thin-film solar cell in which delicate film quality is important. This makes the formation of a uniform, high-quality film on a large-area substrate difficult. 
     Also, if a mechanical phase modulator is used instead of a phase shifter, frequent maintenance is necessary because sliding portions wear. Additionally, high-speed phase modulation is impossible. 
     In the method of the present invention, however, the computer  43  rapidly and accurately controls the phase shifter  42 , and the high-speed phase modulation by this phase shifter  42  shifts the phase of high-frequency power supplied to one end of the electrode  303  from the phase of high-frequency power supplied to the other end. Hence, in a certain instant an envelope distribution is generated on the electrode  303  to produce local variations in the voltage amplitude distribution. In the whole processing time, however, the voltage amplitude distribution on the electrode  303  is averaged, and the density of a plasma generated between the electrode  303  and the substrate G is uniformized. 
     When this phase modulation circuit  8 A is used to rapidly modulate a high frequency at a maximum of 100 kHz, the envelope generated on the electrode moves at the same frequency. This movement is much shorter than the life of SiH 3  active molecules or H active atoms dominating film deposition. Therefore, the flux of these active molecules or atoms arriving at the substrate hardly changes with time. This allows the deposition of a film having a uniform film thickness and uniform film quality. 
     Furthermore, deposition rate distributions with several phase differences were previously measured as shown in FIGS. 18 and 19 and input to the computer  43 . On the basis of this data, deposition time ratios corresponding to the individual phase differences necessary to achieve a uniform distribution were calculated to form phase difference change patterns M 1 , M 2 , and M 3  as shown in FIG.  20 . When the phase shifter  42  was controlled by using these phase difference change patterns M 1 , M 2 , and M 3 , film formation was possible by which both the film thickness distribution and the film quality fell within the ranges of ±5% of their respective target values. 
     When the apparatus was operated by setting the maximum value of high-frequency power to about 800 W which is limited by the rating of the maximum power of the high-frequency amplifier, an average deposition rate of about 2 nm/sec was obtained. Also, as described above, the film thickness distribution of the deposited films cleared ±5% or less necessary for solar cells and thin-film TFTs. 
     The substrate dimensions used in this embodiment were 46 cm×46 cm. However, even when substrates having the same dimensions of 2.0×1.4 m as in the first embodiment were used, a uniformity of 10% or less could be obtained by a similar method. 
     Fourth Embodiment 
     The fourth embodiment of the present invention will be described below with reference to FIG.  21 . An apparatus  1 D of this embodiment is obtained by partially changing the VHF feeder circuit of the apparatus  1 B of the second embodiment described earlier. 
     A feeder circuit of this apparatus  1 D includes two independent high-frequency power supplies  5   a  and  5   b , an oscillator  20 D, phase detectors  30   a  and  30   b , a phase-shifting device  33 , and a function generator  34 . The two power supplies  5   a  and  5   b  incorporate amplifiers and independently feed very-high-frequency (VHF) power components having the same frequency of 60 MHz. The phase-shifting device  33  is inserted between the oscillator  20 D and the second power supply  5   b  and shifts the phase of the high frequency fed from the second power supply  5   b . Consequently, the high frequency fed from the second power supply  5   b  to an electrode  303  is so controlled as to have a certain phase difference from the high frequency fed from the first power supply  5   a  to the electrode  303 . The function generator  34  transmits an arbitrary waveform signal to the phase-shifting device  33  and controls a temporal change in the phase difference. 
     When the oscillator  20 D oscillates a VHF wave having a frequency of 60 MHz, one system (a signal S 1 ) of the oscillation signal is directly amplified by the first power supply  5   a  and input to the first phase detector  30   a  via a power meter  6   a   1 , an isolator  24   a , a power meter  6   a   2 , and an impedance matching circuit  7   a . The phase detector  30   a  detects the phase of the signal S 1 , and this signal S 1  is supplied to the electrode  303  via a distributor  26   a.    
     The phase of the other system (a signal S 2 ) of the oscillation signal is shifted by the phase-shifting device  33 . After that, the signal S 2  is amplified by the second power supply  5   b  and input to the second phase detector  30   b  via a power meter  6   b   1 , an isolator  24   b , a power meter  6   b   2 , and an impedance matching circuit  7   b . The second phase detector  30   b  detects the phase of the signal S 2 , and this signal S 2  is supplied to the electrode  303  via a distributor  26   b.    
     The phase-shifting device  33  performs feedback control such that the difference between the phase of the signal S 1  detected by the first phase detector and the phase of the signal S 2  detected by the second phase detector temporally changes in accordance with the phase difference control signal generated by the function generator  34 . That is, a temporal change in the phase difference is controlled by the phase-shifting device  33  in accordance with the arbitrary waveform signal generated by the function generator  34 . The phase detectors  30   a  and  30   b  detect the phase difference between the signals S 1  and S 2  immediately before the distributors  26   a  and  26   b , respectively. This phase detection signal is supplied to the phase-shifting device  33  to control the phase-shifting operation by feedback. 
     In this embodiment, if the apparatus is operated with a fixed constant phase difference, an envelope spatially stops to generate a standing wave, and this makes a plasma nonuniform. In contrast, by moving the envelope by changing the phase difference with time, it is possible to suppress a standing wave and obtain a uniform plasma and a uniform film thickness distribution by time average within the film formation time. Note that the isolators  24   a  and  24   b  and a protection circuit  22  contribute to stabilization of the power supplies  5   a  and  5   b  when they are operated, as in the apparatus  1 B described previously. 
     If the phase difference is modulated too rapidly, the frequency band of a VHF widens to exceed the frequency band width of the isolators  24   a  and  24   b . This may damage these isolators  24   a  and  24   b . Therefore, a spectrum analyzer (not shown) was connected to the phase detectors  30   a  and  30   b  to determine the modulation rate such that the band width was 1% or less of the rated frequency. 
     In this embodiment, the band width did not exceed 1% when modulation was performed by setting the frequency of the phase control signal from the function generator 34 to 10 kHz. 
     In the present embodiment, the uniformity of deposition rate was within ±8% when the function generator adjusted the modulation width was adjusted to ±110% while the modulation frequency of the phase shifting device was set at 10 kHz. 
     Fifth Embodiment 
     The fifth embodiment will be described below with reference to FIG.  22 . In this embodiment, a description of the same portions as in the above embodiment will be omitted to avoid duplication. 
     A high-frequency power supply  5  of a plasma CVD film forming apparatus  1 E is connected to a feeder circuit  8 B via an impedance matching circuit  44 . This feeder circuit  8 B branches into two circuits. One branched circuit  8 B further branches into two branched circuits  8   a  which are connected to a ladder electrode  303  via two feeding points  9   a . The other branched circuit  8 B has a phase modulation device  45 . This branched circuit  8 B also further branches into two branched circuits  8   b  which are connected to the ladder electrode  303  via two feeding points  9   b . A mechanically driven device having a vacuum capacitor was used as the phase modulation device  45 . The same device as in the third embodiment was used as the high-frequency power supply  5 . 
     In this embodiment, feeding points of a multi-point feeding system are divided into two groups. A difference is produced between the phases of high-frequency power components supplied to feeding points of each group, and the high-frequency power components are applied to the ladder electrode  303  via these feeding points. In this manner, the position of an envelope distribution can be controlled. 
     The apparatus  1 E of this embodiment was used to form a-Si films on glass substrates G. The film formation conditions of this embodiment were as follows. 
     Substrate dimensions: 460 mm×460 mm×1 mm 
     Substrate temperature: 200° C. 
     Pressure: 150 mTorr 
     Process gas: monosilane(SiH 4 )+hydrogen(H 2 ) 
     Gas flow rate: 50 sccm SiH 4 +1,500 sccm H 2    
     Electrode-to-substrate distance: 10 mm 
     Electrode dimensions: 520 mm×520 mm×6 mm 
     Electrode material: stainless steel (JIS SUS304) 
     Power-supply frequency: 60 MHz 
     Target film thickness: 1,000 nm 
     Even under the above conditions, film formation rate distributions analogous to those shown in FIGS. 18 and 19 were obtained with phase differences of 0° and 90°. However, the absolute value of the film formation rate was about ⅕. 
     Films were formed by setting the total film formation time to 6 min and manually controlling the phase difference at 0° for the first three minutes and 90° for the last three minutes. In this embodiment, an average deposition rate of about 0.4 nm/sec was obtained when the apparatus was operated by setting the high-frequency power to about 200 W that was limited by the rating of the phase modulation device. Also, the obtained film thickness distribution was ±15%. These results show that the method of this embodiment can be used in the manufacture of low-cost versatile solar cells. 
     Sixth Embodiment 
     The sixth embodiment of the present invention will be described below with reference to FIG.  23 . An apparatus  1 F of this embodiment is obtained by partially changing the VHF feeder circuit of the apparatus  1 A of the first embodiment. 
     A feeder circuit of this apparatus  1 F comprises two independent power supplies  5   a  and  5   b , two independent power meters  6   a  and  6   b , a mixer  40 , an impedance matching circuit  7 , and a distributor  26 . The independent power supplies  5   a  and  5   b  output VHF power components having different frequencies. The mixer  40  mixes these VHF power components, and the mixed VHF power is supplied to a ladder electrode  303  via the impedance matching circuit  7  and the distributor. 
     In this embodiment, a film thickness uniformity of ±10% or less could be obtained regardless of the simplicity of the feeder circuit. Note that in this embodiment the maximum value of power is limited to 2 kW by the rating of the mixer  40 . 
     Seventh Embodiment 
     The seventh embodiment of the present invention will be described below with reference to FIG.  24 . An apparatus  1 G of this embodiment is obtained by partially changing the VHF feeder circuit of the apparatus  1 F of the above sixth embodiment. 
     A feeder circuit of this apparatus  1 G comprises two independent high-frequency generators  20 G 1  and  20 G 2 , a mixer  40 , a high-frequency amplifier  41 , a power meter  6 , an impedance matching circuit  7 , and a distributor  26 . The independent high-frequency oscillators  20 G 1  and  20 G 2  oscillate different VHFS. These VHFs are mixed by the mixer  40 , amplified by the amplifier  41 , and supplied to a ladder electrode  303  via the power meter  6 , the impedance matching circuit  7 , and the distributor  26 . 
     Also in this embodiment, a film thickness uniformity of ±10% or less could be obtained regardless of the simplicity of the feeder circuit. The arrangement of feeding points in this embodiment could be the same as in the sixth embodiment. On the other hand, in this embodiment the maximum value of power was not restricted by the rating of the mixer  40 , and film deposition was possible at 4 kW. 
     Eighth Embodiment 
     The eighth embodiment of the present invention will be described below with reference to FIG.  25 . An apparatus  1 H of this embodiment is obtained by partially changing the VHF feeder circuit of the apparatus  1 G of the above seventh embodiment. In the seventh embodiment, the mixer  40  mixes two signals having different frequencies oscillated by the two high-frequency oscillators, thereby generating a multiple high frequency which is a mixture of plurality of frequencies. In this embodiment, the same effect can be obtained by using one arbitrary waveform generator  20 H. 
     FIG. 26A is a graph of a frequency spectral waveform showing a multiple high frequency in a frequency band of 59 to 61 MHZ. In FIG. 26A, the frequency (MHz) is plotted on the abscissa, and the amplitude is plotted on the ordinate. First, this frequency spectrum was converted into a temporally changing waveform by performing inverse Fourier transform by using a computer (not shown). The result is shown in FIG.  26 B. That is, FIG. 26B is a graph showing the waveform obtained by performing inverse Fourier transform for the multiple high frequency shown in FIG.  26 A. In FIG. 26B, the time elapsed (×10 −6  sec) from the beginning of VHF oscillation is plotted on the abscissa, and the voltage (V) on the electrode is plotted on the ordinate. FIG. 26B shows an envelope which contains a wave of about 60 MHz, although details of the waveform are not shown. That is, this waveform contains waves at different frequencies of 59 to 61 MHz. This waveform is stored in the arbitrary waveform generator  20 H and repetitively generated from it. Consequently, a multiple high-frequency wave containing frequencies of 59 to 61 MHz is continuously supplied to a high-frequency amplifier  41 . This high-frequency wave is then supplied to a ladder electrode  303  via a power meter  6 , an impedance matching circuit  7 , and a distributor  26 . Also in this embodiment, a film thickness uniformity of ±10% or less could be obtained as in the seventh embodiment described above. 
     Ninth Embodiment 
     The ninth embodiment of the present invention will be described below with reference to FIG.  27 . An apparatus  1 J of this embodiment includes a circular parallel plate electrode  313  in a vacuum chamber  2 J. Six VHF feeder circuits are connected to this parallel plate electrode  313  via six feeding points  9   a . The six feeding points  9   a  are connected to the circular parallel plate electrode  313  by point symmetry. The six VHF feeder circuits are independent of one another. The first VHF feeder circuit includes a high-frequency power supply  5   a , a power meter  6   a , and an impedance matching circuit  7   a . Analogously, the second to sixth VHF feeder circuits include high-frequency power supplies  5   b  to  5   f , power meters  6   b  to  6   f , and impedance matching circuits  7   b  to  7   f , respectively. 
     In this embodiment, a plasma on the parallel plate electrode  313  could be uniformized by supplying high-frequency waves having different frequencies from the six independent feeder circuits. A film thickness uniformity of ±10% or less could be obtained by adjusting the VHF power and the electrode spacing. However, the range of uniformization conditions of the circular parallel plate electrode  313  is narrower than that of the ladder electrode  303 . In this embodiment, the aforementioned uniformity could be obtained only at a power of 2.0 to 2.2 kW and an electrode spacing of 25 to 30 mm. 
     10th Embodiment 
     The 10th embodiment of the present invention will be described below with reference to FIGS. 28,  29 , and  30 . FIG. 28 is a plan block diagram showing an apparatus of this embodiment. FIG. 32 is a sectional block diagram showing the apparatus of this embodiment. FIG. 33 is a perspective block diagram showing the external appearance of the apparatus of this embodiment. An apparatus  1 K of this embodiment includes a shower type parallel plate electrode  323 , instead of the ladder electrode  303  of the apparatus  1 A of the first embodiment. A gas supply pipe  17  is connected to the upper surface of this electrode  323 . This gas supply pipe  17  communicates with a hollow portion  324  in the electrode via a port  321 . The hollow portion  324  communicates with a discharge plasma generation space  330  via a plurality of pores  325 . 
     The electrode  323  is held on the side walls of a chamber  2 K by insulating members  336  and  338 . Coaxial cables  8   b  of two feeder circuits  341  and  342  are introduced into the chamber  2 K and connected to the electrode  323  via a plurality of feeding points  9   a  and a plurality of feeding points  9   b   1 , respectively. Insulating members  340  insulate portions where the cables  8   b  extend through the walls of the chamber  2 K. 
     The feeder circuit  341  includes a high-frequency power supply  5   a , a power meter  6   a , an impedance matching circuit  7   a , and a distributor  26   a . The distributor  26   a  feeds power to the feeding points  9   a  via the eight branched cables  8   b . The feeder circuit  342  includes a high-frequency power supply  5   b , a power meter  6   b , an impedance matching circuit  7   b , and a distributor  26   b . The distributor  26   b  feeds power to the feeding points  9   b   1  via the eight branched cables  8   b.    
     A ground electrode  3  is supported by a plurality of columns  331  so as to oppose parallel to the shower electrode  323 . A pair of gate valves  334  are formed in the side surfaces of the chamber  2 K to allow a substrate G to be loaded/unloaded into/from the chamber  2 K. When the gate valves  334  are opened, a loader (not shown) loads the substrate G into the chamber  2 K and places the substrate G on the ground electrode  3 . A heater  3   a  connected to a power supply  332  is embedded in the ground electrode  3  and heats the substrate G. 
     An exhaust pipe  18  communicates with an appropriate portion of the chamber  2 K. An evacuation device  72  evacuates the chamber  2 K to a high vacuum degree. 
     The apparatus  1 K of this embodiment was used to form films on the substrates G under the same conditions as in the first embodiment. Consequently, in this embodiment a film thickness uniformity of ±12% or less could be obtained. In the apparatus  1 K of this embodiment, when the arrangement of the feeding points was changed, the film thickness uniformity largely changed accordingly. Therefore, it was necessary to optimize the feeder distribution center arrangement. 
     11th Embodiment 
     The 11th embodiment of the present invention will be described below with reference to FIG.  31 . An apparatus  1 L of this embodiment is obtained by partially changing the very-high-frequency (VHF) feeder circuit of the apparatus  1 A of the first embodiment shown in FIG.  8 . 
     This apparatus  1 L comprises an AM modulation oscillator  50 , an amplifier  41 , a power meter  6 , an impedance matching circuit  7 , and a distributor  26 . A high-frequency wave from the AM modulation oscillator  50  was amplified by the amplifier  41  to generate an AM-modulated high-frequency wave having a carrier frequency of 60 MHz, a modulation frequency of 30 MHz, and a modulation amplitude range from 100% to 20%. This AM-modulated high-frequency wave was fed to a ladder electrode  303  via the power meter  6 , the impedance matching circuit  7 , and the distributor  26 . 
     In this embodiment, a film thickness distribution of ±15% could be obtained regardless of the simplicity of the circuit. 
     12th Embodiment 
     The 12th embodiment will be described below with reference to FIG.  32 . In this embodiment, a description of the same portions as in the above embodiments will be omitted to avoid duplication. 
     A plasma CVD apparatus  1 M has a high-frequency oscillator  20 M with an FM modulation function as a power supply. An arbitrary waveform generator was used as this high-frequency oscillator  20 M. An amplifier  41  and an impedance matching circuit  7  are connected in series to the high-frequency oscillator  20 M. An output circuit of the impedance matching circuit  7  branches into two circuits, and each branched circuit  8 M further branches into two circuits. These branched circuits  8 a and  8   b  are connected to an electrode  303  via a pair of feeding points  9   a  and a pair of feeding points  9   b , respectively. 
     In this embodiment, the use of FM modulation made it possible to simplify the feeder circuit and uniformize the film thickness as in the above embodiments. That is, a film thickness uniformity of ±10% or less was obtained on a 10 cm×10 cm square substrate by setting the oscillation frequency to 200 MHz, the modulation frequency to 1 MHz, and the maximum deviation amount to 20%. This film thickness uniformity was much superior to a film thickness uniformity of ±50% obtained by the conventional method. 
     Similar effects were also obtained by frequency chirp. That is, the film thickness uniformity was ±12% when the chirp frequency was 10 MHz and the maximum deviation amount was 20%. 
     13th Embodiment 
     A thin semiconductor film, thin metal film, or insulating film of a semiconductor element can be etched by generating a plasma by using a halogen-based gas, e.g., a chlorine-based gas, thereby generating negative chlorine ions (C 1   − ). In this case, as described in S. Samukawa, “Role of Negative Ions in High-Performance Etching Using Pulse-Time-Modulated Plasma”, Extended Abstract of 4th International Conference on Reactive Plasma, SR 1.04, p. 415, 1998 (to be referred to as reference  8  hereinafter), a plasma is conventionally generated and extinguished by turning on/off electric power generated from a high-frequency power supply, thereby generating a large amount of negative chlorine ions by the electron adhesion effect when the plasma disappears. In addition to this effect, the rate and quality of etching are increased by using the effect of disappearance of the wall electric charge generated on the substrate surface. In this embodiment, a plasma is turned on/off by moving the nodes and antinodes of an envelope. 
     The apparatus  1 B of the second embodiment shown in FIG. 14 was used. Two different frequencies of 750.000 and 750.004 MHz were used to set the frequency difference at 4 kHz, and the electrode dimensions were set to 33 cm×33 cm. In addition, a halogen-based gas, e.g., a chlorine-based gas was used to generate a plasma to generate negative chlorine ions (C 1   − ), thereby etching a thin Au film on the substrate surface. In this state, the plasma was ON in the antinodes of an envelope distribution and OFF in its nodes. Therefore, etching could be performed at high rate by efficiently and simply generating a large amount of negative chlorine ions by rapidly moving the envelope. 
     Since the frequency difference was 4 kHz, the changing cycle of the envelope was set to about 250 μsec so that the cycle was longer than, i.e., twice to four times, a negative chlorine ion generation time of about 100 μsec described in reference  10 . That is, the plasma turns on/off at a cycle equivalent to the reciprocal of the frequency difference between a plurality of high frequencies. Accordingly, the plasma OFF time was about 125 μsec, so sufficient negative ions are generated. 
     The etching conditions of this embodiment were as follows. 
     Substrate dimensions: 300 mm×300 mm×0.5 mm 
     Substrate temperature: 80° C. 
     Pressure: 2 mTorr 
     Etching gas: Cl 2    
     Gas flow rate: 50 sccm 
     Electrode-to-substrate distance: 20 mm 
     Electrode dimensions: 330 mm×330 mm×5 mm 
     Electrode material: stainless steel (JIS SUS304) 
     Power-supply frequencies: 750.000 MHz, 750.004 MHz 
     Target etching rate: 3 nm/sec 
     Since 750 MHz was used as the frequency of a high-frequency wave, the plasma density became higher than when 13.56 MHz of the conventional method was used, and simultaneously the thickness of the plasma sheath decreased. Consequently, a large amount of negative chlorine ions generated in the plasma efficiently flowed into the substrate surface, and this further raised the etching rate. 
     In this embodiment, it was possible to obtain an etching rate about 40 times that obtained when a conventional single frequency of 13.56 MHz was used. 
     The method of this embodiment is also applicable to so-called self-cleaning which removes foreign matter (thin silicon-based films) sticking to the chamber inner walls of a PCVD apparatus by using a discharge plasma. 
     The effect of this embodiment is obtained by moving an envelope by using the frequency difference between two frequencies. However, the same effect can naturally be obtained by another envelope moving method, e.g., a phase difference change, AM modulation, or FM modulation. 
     14th Embodiment 
     The 14th embodiment of the present invention will be described below with reference to FIG.  33 . 
     An apparatus  1 N of this embodiment is obtained by changing the feeding points and high frequencies of the apparatus  1 A of the first embodiment. 
     This apparatus  1 N includes first and second high-frequency power supplies  5   a  and  5   b , two feeding points  9   a  attached to a ladder electrode  303 , and two feeding points  9   b   2  attached to a ground electrode  3 . The first power supply  5   a  supplies high-frequency power at a frequency of 60.00 MHz to the ladder electrode  303  via the feeding points  9   a . The second power supply  5   b  supplies high-frequency power at a frequency of 13.56 MHz to the ground electrode  3  via the feeding points  9   b   2 . 
     This embodiment was applied to silicon film etching using halogen-based gas NF 3 . Consequently, a high etching rate (about 10 nm/sec) was uniformly obtained in a large area of 1 m×1 m by the high density resulting from a very high frequency of 60 MHz, by the substrate bias effect obtained by 13.56 MHz, and by the effect of suppressing a standing wave obtained by the difference between the two frequencies. 
     This embodiment can also be applied to a surface treatment method such as plasma cleaning of a reaction vessel used in the formation of a thin silicon film, i.e., so-called self-cleaning. 
     15th Embodiment 
     The 15th embodiment of the present invention will be described below with reference to FIG.  34 . An apparatus  1 Q of this embodiment includes upper and lower discharge electrodes  323   a  and  323   b  in place of the ground electrode  3  of the apparatus  1 K of the 10th embodiment described earlier. These upper and lower electrodes  323   a  and  323   b  are flat plates having substantially the same size and arranged parallel to each other. Four first feeding points  9   a  are formed in a side portion of the upper electrode  323   a . An impedance matching circuit  7   a , a power meter  6   a , and a high-frequency power supply  5   a  are connected to these four first feeding points  9   a  via a coaxial cable  8   a  and a T-shaped branched connector  27   a . Four second feeding points  9   b  are formed in a side portion of the lower electrode  323   b . An impedance matching circuit  7   b , a power meter  6   b , and a high-frequency power supply  5   b  are connected to these four second feeding points  9   a  via a coaxial cable  8   b  and a T-shaped branched connector  27   b . The four first feeding points  9   a  are attached at substantially equal intervals to a short edge on one side of the upper electrode  323   a . The four second feeding points  9   b  are attached at substantially equal intervals to a short edge on the other side of the lower electrode  323   b . Accordingly, the four second feeding points  9   b  are symmetrically positioned on the side far away from the four first feeding points  9   a.    
     In the apparatus  1 Q of this embodiment, when a VHF is fed from the power supply  5   b  to the lower electrode  323   b  via the four second feeding points  9   b , the lower electrode  323   b  generates a voltage similar to the voltage distribution R 1  shown in FIG. 10A in the first embodiment. When a VHF is fed from the power supply  5   a  to the upper electrode  323   a  via the four first feeding points  9   a , the upper electrode  323   a  generates a voltage similar to the voltage distribution R 2  shown in FIG.  10 B. Therefore, on a substrate G a voltage distribution analogous to the synthetic voltage distribution R 3  of the two voltage distributions R 1  and R 2  is generated. This synthetic voltage distribution R 3  is highly uniform and generates a plasma having a substantially uniform distribution density, so the uniformity of the film thickness improves. A high film formation rate of 0.9 nm/sec was obtained in nanocrystalline film formation, and the uniformity was about ±10%. That is, the uniformity necessary for S 1  thin-film semiconductors for solar cells was achieved. 
     Comparative examples in which amorphous silicon films (a-Si films) were formed on substrates by using conventional feeding methods will be described below. 
     Comparative Example 1 
     In Comparative Example 1, a parallel plate plasma CVD apparatus  400  shown in FIG. 35 was used. This apparatus  400  is known by the reference  1  cited previously. Upper and lower electrodes  402  and  404  are opposed in a vacuum vessel  401 . The upper electrode  402  is mounted on the upper portion of the vacuum vessel  401  via an insulator  405 . This upper electrode  402  is connected to an impedance matching circuit  406  and a high-frequency power supply  407  via a coaxial cable  408 . The power-supply frequency is 13.56 MHz. The cable  408  is connected to the upper electrode  402  by a feeder distribution center  409 . This feeder distribution center  409  is formed on the surface (outer surface) exposed to the atmosphere of the upper electrode  402  so as not to be exposed in a plasma generation space  410 . 
     The lower electrode  404  houses a heater  403  for heating a substrate G. A heater power supply is controlled by a controller (not shown). The substrate G is placed on the lower electrode  404  and heated to a predetermined temperature by the heater  403 . Note that the lower electrode  404  is grounded. 
     A gas supply pipe  411  is open in the upper portion of the vacuum vessel  401 . This gas supply pipe  411  communicates with a gas supply source (not shown) via a flow rate control valve  416 . The gas supply source contains monosilane (SiH 4 ). An exhaust pipe  412  is open in the lower portion of the vacuum vessel  401 . This exhaust pipe  412  communicates with a vacuum pump  413 . 
     The above apparatus  400  was used to form a-Si films on glass substrates. The film formation conditions of Comparative Example 1 were as follows. 
     Substrate dimensions: 1,200 mm×1,000 mm×1 mm 
     Substrate temperature: 200° C. 
     Pressure: 0.05 to 0.5 Torr 
     Process gas: monosilane (SiH 4 ) 
     Gas flow rate: 100 sccm 
     Electrode-to-substrate distance: 30 mm 
     Electrode dimensions: 1,300 mm×1,100 mm×50 mm 
     Electrode material: stainless steel (JIS SUS304) 
     Power-supply frequency: 13.56 MHz 
     Target film thickness: 1,000 nm 
     As a consequence, a-Si films having a variation of ±18% with respect to the target film thickness were obtained. The average film formation rate was 0.13 nm/sec. 
     Comparative Example 2 
     In Comparative Example 2, a parallel plate plasma CVD apparatus  500  shown in FIGS. 36 and 37 was used. This apparatus  500  is known by the reference  1  cited previously. 
     As Comparative Example 2, the second apparatus described in reference  1  will be explained with reference to FIGS. 36 and 37. In this Comparative Example 2, a description of the same portions as in Comparative Example 1 described above will be omitted to avoid duplication. 
     Reference numeral  521  denotes a gate valve formed in a side wall of a vacuum vessel  501 . A substrate G is loaded/unloaded through this gate valve  521 . A hollow non-grounded electrode  502  is placed inside an insulator  505  which is positioned in the upper portion of the vacuum vessel  501 . A large number of gas supply holes  502   b  about 0.5 mm in diameter are formed in a lower surface (front surface)  502   a  of this non-grounded electrode  502  at intervals of 10 to 15 mm to face a plasma generation space  510 . An opening  502   c  for a discharge gas is formed in the upper surface of the non-grounded electrode  502 . A discharge gas supply pipe  511   b  is connected to this opening  502   c  of the non-grounded electrode  502  via a connecting member  523 . This discharge gas supply pipe  511   b  supplies, e.g., monosilane gas (SiH 4 ) into the non-grounded electrode  502 . A power distributor  525  for branching the output from a high-frequency power supply into a plurality of portions is placed on the non-grounded electrode  502 . 
     A glow discharge plasma is generated in the vacuum vessel  501  by the non-grounded electrode  502  and a grounded electrode  504 . The non-grounded electrode  502  is a rectangular or square plate-like member (about 500 mm×500 mm to about 1,000 mm×1,000 mm and 60 mm in thickness) and made of stainless steel. This non-grounded electrode  502  is supplied with necessary power by a power supply system composed of a high-frequency power supply  507 , an impedance matching circuit  506 , and the power distributor  525  described above. 
     As shown in FIG. 37, the power distributor  525  is composed of a columnar connection port  526  placed in the center, four band-like branched ports  527  radially extending from the connection port  526 , and four columnar members  528   a ,  528   b ,  528   c , and  528   d . Reference numerals  509   a ,  509   b ,  509   c , and  509   d  in FIG. 37 denote power supply portions. A gas in the vacuum vessel  501  is exhausted through the exhaust pipe  512  by the vacuum pump  513 . A substrate  514  is placed on the grounded electrode  504  by opening the gate valve  521  and heated to a predetermined temperature by a substrate heater  503  and a substrate heater power supply  515 . 
     The above apparatus  500  was used to form a-Si films on glass substrates. The film formation conditions of Comparative Example 2 were as follows. 
     Substrate dimensions: 350 mm×450 mm×1 mm 
     Substrate temperature: 200° C. 
     Pressure: 0.2 Torr 
     Process gas: monosilane (SiH 4 ) 
     Gas flow rate: 100 sccm 
     Electrode-to-substrate distance: 20 mm 
     Electrode dimensions: 500 mm×500 mm×50 mm 
     Electrode material: stainless steel (JIS SUS304) 
     Power-supply frequency: 70 MHz 
     Target film thickness: 1,000 nm 
     As a consequence, a-Si films having a variation of ±50% with respect to the target film thickness were obtained. 
     First, the gate valve  521  was opened to place the substrate G on the grounded electrode  504 , and the gate valve  521  was closed. The vacuum pump  513  was driven to evacuate the vacuum vessel  501  to an internal pressure of about 1×10 −7  Torr. While the power supply amount from the power supply  515  was controlled, the substrate G was heated to a predetermined target temperature by the heater  503 . A predetermined amount of monosilane gas was supplied through the discharge gas supply pipes  511   a  and  511   b , and the internal pressure of the vacuum vessel was held at 0.05 to 0.5 Torr. A high-frequency voltage was applied to the non-grounded electrode  502  by the power supply  507 , thereby generating a glow discharge plasma between the non-grounded electrode  502  and the grounded electrode  504 . 
     When the monosilane gas was formed into a plasma, radicals such as SiH 3 , SiH 2 , and SiH existing in the plasma diffused by a diffusion phenomenon. These radicals were adsorbed in and deposited on the surface of the substrate G to form an a-Si film. 
     Comparative Example 3 
     In Comparative Example 3, a parallel plate plasma CVD apparatus  600  shown in FIGS. 38 and 39 was used. This apparatus  600  is known by reference  2  cited previously. 
     As Comparative Example 3, the apparatus described in reference  2  will be explained below with reference to FIGS. 38 and 39. 
     A high-frequency oscillator  631  is connected to an impedance matching circuit  606  via a high-frequency power amplifier  632 . The high-frequency oscillator  631  and the high-frequency amplifier  632  constitute a high-frequency power supply. A vacuum current supply terminal  633  is formed on a wall surface  634  of a vacuum vessel  601 . A coaxial cable  608  extending through this supply terminal  633  connects a non-grounded electrode  602  and the impedance matching circuit  606 . The wall surface  634  of the vacuum vessel  601  is grounded. A substrate G is placed on the wall surface  634 . When a gas is supplied into the vacuum vessel  601  and a high frequency is applied between the electrode  502  and the wall surface  634 , a glow discharge plasma is generated between them. The non-grounded electrode is supplied with high-frequency power from the power supply  631  via the vacuum current supply terminal  633 , the coaxial cable  608 , and the impedance matching circuit  606 . The frequency of the high-frequency wave oscillated by the power supply  631  is 70 MHz. 
     As shown in FIG. 39, an H-shaped feeder  635  is formed on the rear surface (the surface not in contact with the plasma generation space) of the electrode  602 . Feeding points  609   a ,  609   b ,  609   c , and  609   d  are formed at the four corners of this feeder  635 . 
     The above apparatus  600  was used to form a-Si films on glass substrates. The film formation conditions of Comparative Example 3 were as follows. 
     Substrate dimensions: 350 mm×450 mm×1 mm 
     Substrate temperature: 200° C. 
     Pressure: 0.2 Torr 
     Process gas: monosilane (SiH 4 ) 
     Gas flow rate: 100 sccm 
     Electrode dimensions: 470 mm×570 mm 
     Electrode material: stainless steel (JIS SUS304) 
     Power-supply frequency: 70 MHz 
     Target film thickness: 1,000 nm 
     As a consequence, a-Si films having a variation of ±18% with respect to the target film thickness were obtained. 
     Additional advantages and modifications will readily occur to those skilled in the art. Therefore, the invention in its broader aspects is not limited to the specific details and representative embodiments shown and described herein. Accordingly, various modifications may be made without departing from the spirit or scope of the general inventive concept as defined by the appended claims and their equivalents.

Technology Category: 5