Process for forming deposition film

Abstract: A process for forming a deposition film comprises introducing a gaseous starting material for forming a deposition film and a gaseous oxidizing agent having an oxidation action on the gaseous start­ ing material separately into a reaction space to chemically contact these two, thereby generating a plurality of precursors including precursor in an excited state, and utilizing at least one of the generated precursors as a supply source for film­ constituting members, thereby forming a deposition film on a substrate provided in a film-forming space, the deposition film being formed while supplying a bias energy to the substrate and changing the intensity of the bias energy.

Description: The present invention relates to a process for forming a deposition film particularly film useful for semiconductor devices, photosensitive devices for solar batteries and electrophotography, and electronic devices such as optical input sensors for optical image input-output devices. Heretofore, individually appropriate processes for forming deposition film have been used for forming crystal functional films such as semiconductor films, insulating films, photoconductive films, magnetic films or metal films, from the viewpoints of desired physical properties and applications. For example, in the formation of silicon crystal deposition films, a thermal CVD method, a hydrogen reduction method, a molecular beam epitaxial method (MBE), a sputtering method, a plasma CVD method, a photo CVD method etc. have been heretofore used. Among these methods, the thermal CVD method and the hydrogen reduction method have been already widely used in the semiconductor industry, but these two methods require so high a deposition temperature that they can fully meet neither a desired lowering temperature in the semiconductor process nor formation of crystalline deposition films on low melting point substrates such as glass. The molecular beam epitaxial method (MBE) is capable of forming crystal deposition films at a relatively low temperature, but owing to the deposition on substrates by a direct chemical absorption of coming raw material molecules, the deposition is readily influenced by contamination in the reaction chamber or impurities on the surfaces of substrates, so that an ultra high vacuum or a clear surface is required for the deposition. Thus, the MBE method is not always suitable for mass-production from the viewpoint of apparatus cost, maintenance or throughput. The plasma CVD method and the photo CVD method have been recently regarded as promising, and have been studied as processes for forming crystal deposition films of high quality at a lower temperature. However, for example, in the formation of silicon deposition films by a plasma CVD method or by a photo CVD method, so far widely studied, the reaction process is more complicated than that of the conventional CVD method, and its reaction mechanism has not been fully clarified yet. There are many deposition film formation parameters such as substrate temperature, flow rate of introduced gases and their ratios, pressure in the reaction space during the formation of deposition films, high frequency power, electrode structure for high frequency power input, structure of reaction chamber, venting rate from the reaction chamber, light intensity and wavelength, photoabsorbancy and heat conductivity of the substrate, etc. which are complicatedly interrelated with one another. Thus, the conditions for forming deposition films sometimes become unstable or it is sometimes substantially impossible to carry out the deposition while keeping all the parameters in a state set to the optimum conditions. Owing to these problems, the plasma CVD method and the photo CVD method are not always satisfactory as a method for forming good crystalline deposition films of large area with a good reproducibility and at a low cost. On the other hand, another process for forming good crystalline deposition films of large area at a low temperature with a good reproducibility, i.e., a process for forming a crystalline deposition film on a substrate by separately introducing gaseous starting materials for forming a deposition film and a gaseous oxidizing agent into a reaction space and then chemically contacting them, (which will be referred to as chemical deposition process below,) is disclosed in Japanese Patent Application Kokai (Laid-Open) No. 62-96675. In the above-mentioned process, the reaction to form a deposition film depends substantially on pressures and flow rate ratio of the gaseous starting material and the gaseous oxidizing agent, the substrate temperature, etc. That is, the process has less restrictions to the controllability of deposition process based on complicated deposition parameters of the conventional process for forming a crystalline deposition film at a low temperature, such as correlations between the flow rates of introduced gases or the pressure in the reaction space and the plasma state, the presence of side reaction by excitation of various chemical species, or correlation between the decomposition of gaseous starting materials by the wavelength or intensity of irradiation light and the reaction on the substrate surface, etc. in the above-mentioned plasma CVD process. Thus, the chemical deposition process can form a crystalline deposition film of large area with a good uniformity and a good reproducibility. However, in the above-mentioned chemical deposition process, such a range for conditions, i.e. pressure, flow rate ratio and temperature of a gaseous starting material and a gaseous oxidizing agent that the formed deposition film is in a crystalline form rather than in an amorphous form, is relatively narrow. That is, once a deposition film is formed under the crystallizable condition, the quality of the crystalline deposition film is invariably set. This fact shows that the chemical deposition process has a good controllability of deposition process by the pressure, flow rate ratios, temperature etc. of the gaseous starting material and the gaseous oxidizing agent, but a crystalline deposition film of required good quality cannot be always obtained in the condition range. An improvement of the chemical deposition process by introducing new deposition parameters has been in demand. The present invention is intended as a remedy. In accordance with a first aspect of the invention there is provided a process for forming a crystalline deposition film on a substrate in a reaction space which comprises: (i) separately introducing into said reaction space a gaseous starting material for forming a deposition film and a gaseous oxidizing agent capable of having an oxidation action on the gaseous starting material, (ii) chemically contacting said gaseous starting material and said oxidizing agent, thereby generating a plurality of precursors including a precursor in an excited state, and (iii) utilizing at least one of the generated precursors as a supply source of a film constituent, (iv) supplying to said substrate energy to vary the temperature of said substrate, and (v) varying the intensity of said energy, thereby forming a crystalline deposition film on said substrate in said reaction space. In accordance with a second aspect of the invention there is provided a process for forming a crystalline deposited film on a substrate in a reaction space which comprises: (i) separately introducing a gaseous starting material for forming a deposition film and a gaseous oxidizing agent capable of having an oxidation action on the gaseous starting material into said reaction space, (ii) chemically contacting said gaseous starting material and said oxidizing agent, thereby generating a plurality of precursors including a precursor in an excited state, and (iii) utilizing at least one of the generated precursors as a supply source of a film-constituting member, (iv) supplying to an area of said substrate an energy to vary the temperature of said substrate, and (v) changing the area on said substrate to which said energy is to be applied, thereby forming a crystalline deposition film on said substrate in said reaction space. Advantageously, a compact crystalline deposition film of large grain size can be uniformly formed over a larger area at a low temperature with less defects. Other advantages of this process include a reduction in apparatus cost and film-forming cost due to the lower film-forming temperature, an increase in the yield of a uniform crystalline deposition film of high quality over a large area and a simplification of maintenance which can be attained. In the drawings:- Fig. 1 is a schematic view showing one example of an apparatus for forming a deposition film suitable for the embodiment of the present invention. Fig. 2 is a diagram showing a relationship between a deposition rate of a deposition film and a substrate temperature by a chemical deposition process. Figs. 3A-3E are diagrams showing modulation patterns of bias energy supplied to a film-forming space in the present invention. To facilitate further understanding of this invention preferred embodiments thereof will now be described. The following description is given by way of example only. The principle of the present invention will be explained below, referring to a case using SiH₄ as a gaseous starting material and F₂ as a gaseous oxidizing agent as a preferred example. Fig. 1 is a schematic view showing a preferred example of an apparatus for forming a deposition film suitable for the embodiment of the present invention, where an inlet pipe 101 is provided for introducing a gaseous starting material (SiH₄) to a reactor chamber 103 and an inlet pipe 102 is provided for introducing a gaseous oxidizing agent (F₂) to the reactor chamber 103. The inlet pipes are not restricted to those shown in Fig. 1, but multiple concentric tubular conduits such as a double concentric pipe, a triple concentric pipe, etc. can be used as the inlet pipe, or gases may be introduced through spaces between the concentrically provided pipes. A substrate 104 is set to a support 106 including a heater 105 for heating the substrate 104. Before the formation of a deposition film, the reaction chamber 103 is evacuated to a predetermined background pressure by a vacuum pump 107. During the formation of a deposition film, the gaseous starting material and the gaseous oxidizing agent are evacuated at a predetermined rate by another vacuum pump 108. A window 109 is provided for irradiation of the substrate 104 with a bias light from a light source 110. The apparatus for forming a deposition film used for the embodiment of the present process for forming a deposition film is not restricted to the apparatus shown in Fig. 1. Any other apparatus can be used so long as it is provided with a means for separately introducing a gaseous starting material and a gaseous oxidizing agent to a reaction chamber, a support for supporting a substrate, which includes a heater for heating the substrate and is provided in the reaction chamber, and a means for applying energy to the substrate. Fig. 2 is a diagram showing a result of deposition tests of crystalline deposition film by a chemical deposition process in the apparatus shown in Fig. 1, where the curves show relationships between substrate temperature and deposition rate with respect to flow rate ratios of SiH₄ to F₂. Curve 201 shows a case of SiH₄/F₂ = 1/1, curve 202 a case of SiH₄/F₂ = 2/3 and curve 203 a case of SiH₄/F₂ = 1/2, where the total pressure prevailing in the reaction chamber during the formation of deposition films was 66.7 Pa (500 m Torr). Glass No.7059, made by Corning Glass Works, USA was used for the substrate 104. In Fig. 2, an area 204 shows a condition range for forming an amorphous silicon film, an area 205 a condition range for forming a crystalline silicon film, and an area 206 a condition range for forming no deposition film at all due to etching action. The structural form of the thus formed deposition films was determined by X-ray diffraction. As is clear from Fig. 2, crystallization of the formed deposition films take place in the condition range very near the etching action-dominant area 206 in all the cases of curves 201 to 203, and the crystallization temperature increases with increasing flow rate ratio of SiH₄/F₂. This shows that a plurality of precursors including SiF n H m , a precursor for forming a deposition film, are formed by reaction of a gaseous starting material SiH₄ with a gaseous oxidizing agent F₂, and crystallization takes place only under such a condition that the action to deposit a silicon film on the substrate in the film-forming space by the precursors and an etching action by F₂ as an oxidizing agent are balanced. The higher the substrate temperature, the larger the grain size of the resulting crystal grain. For example, under the condition of point A on the curve 201, it was observed by a transmission type electron microscope that the grain size was about 600 nm. In order to obtain a crystalline deposition film of much larger grain size by the above-mentioned conventional chemical deposition process, it is necessary not only to increase the substrate temperature, but also to lower a flow rate ratio of SiH₄/F₂ and lower the reaction pressure during the deposition, because the film-forming rate can be lowered by lowering the flow rate ratio of SiH₄/F₂ and the reaction pressure. In the case of a lower film-forming rate the number of formed nuclei of crystals is decreased, as compared with the case of higher film-forming rate and consequently the grain size of grown crystals becomes larger. However, an increase in the substrate temperature deviates- from the proper object of the chemical deposition process, i.e., formation of a crystalline film at a lower temperature, and a decrease in the reaction pressure during the formation of a deposition film leads not only to a decrease in the deposition rate of the crystalline film, but also to a relative increase in partial pressures of impurity gases in the total reaction pressure and resulting inclusion of much more impurities into the crystalline film. The present invention has been accomplished in view of these situations and can form a crystalline deposition film of larger grain size with less impurities at a lower substrate temperature by a chemical deposition process. Herein, a deposition film is formed by changing the intensity of energy supplied to a substrate provided in the film-forming space or by changing the area on the substrate to be supplied with energy. That is, the deposition film can be formed by changing the film-forming conditions, thereby controlling a balance between the etching of the deposition film and the formation of the deposition film, and thus a crystalline deposition film having a distinguished crystal orientation, where the less etching-susceptive crystal face in a specific direction preferentially grows, can be formed. The substrate temperature can be elevated or lowered by varying the intensity of energy to be supplied to the substrate. As is obvious from Fig. 2, deposition of a crystalline film predominantly proceeds in a low substrate temperature phase (point A in Fig. 2), whereas etching of the deposition film takes place in a high substrate temperature phase (point B in Fig. 2). Under the condition of point B in Fig. 2, the deposition film is not uniformly etched, but parts of amorphous phase or crystal phases with many defects, or crystal grains with a readily etchable orientation are removed by etching with a relatively high speed. Thus, by repeatedly elevating and lowering the substrate temperature, a crystalline deposition film of high quality freed from the amorphous phases or crystal phases with many defects can be formed. At the same time, a balance between the deposition and the etching can be readily controlled by changing the application pattern of the energy, and thus a crystalline deposition film of larger grain size with less etching-susceptible crystal face preferentially grown in a specific direction can be formed by properly selecting the energy application conditions Furthermore, the above-mentioned effect can also be obtained by changing the area on the substrate to be supplied with energy, because the temperature in a specific area on the substrate surface can be varied by changing the area on the substrate surface to be supplied with energy. An alternative to this process for forming a crystalline deposition film of high quality will be explained below. In this case the temperature of substrate 104 is synchronized with periodically changing application of external energy and the flow rate ratio of gaseous oxidizing agent/gaseous starting material is also increased or decreased. In a phase of a higher substrate temperature and a lower flow rate ratio of gaseous oxidizing agent/gaseous starting material, the deposition of a crystalline film predominantly proceeds (point A in Fig. 2), whereas in a phase of a lower substrate temperature and a higher flow rate ratio of gaseous oxidizing agent/gaseous starting material, etching of the deposition film predominantly proceeds (point C in Fig. 2). In this process, the substrate temperature is high in the phase of predominant deposition of a crystalline film (point A in Fig. 2) and crystals of high quality with less defects are liable to grow, whereas in the phase of predominant etching (point C in Fig. 2), the substrate temperature is low, and the etching reaction proceeds mildly and thus damage to the crystalline film is less. Thus, a crystalline film of higher quality can be formed. Since no plasma is generated in the reaction space for forming a crystalline film by the present process for forming a deposition film, the film is less susceptible to damages due to ions or radicals excited to a higher energy level, and thus it is needless to say from this point of view that a crystalline film of high quality can be formed. The gaseous starting material for use in the present process for forming a crystalline deposition film contains an element constituting the crystalline film to be deposited and is subjected an oxidation action through a chemical contact with the gaseous oxidizing agent and is appropriately selected in view of the speeds, characteristics and applications of a desired deposition film. For example, in the case of forming a silicon crystalline film or a germanium crystalline film, straight or branched chain silane compounds, cyclic silane compounds, chain germanium compounds, etc. can be used. More specifically, the straight chain silane compounds include those represented by the general formula: Si n H 2n+2 , where n is an integer of 1 to 8; branched chain silane compounds include SiH₃SiH(SiH₃)SiH₂SiH₃; the chain germanium compounds include those represented by the general formula: Ge m H 2m+2 , where m is an integer of 1 to 5. These starting materials can be used above or in combination of at least two thereof. The gaseous oxidizing agent for use in the present process for forming a crystalline deposition film is gasified when introduced into the reaction space and has an effective oxidation action on the gaseous starting material for forming the deposition film to be introduced into the reaction space at the same time only by chemical contact, and includes, for example, halogens such as F₂, Cl₂, gasified Br₂ and I₂, etc., halogenated carbons such as CF₄, C₂F₆, CCl₄, CBrF₃, CCl₂F₂, CCl₃F, CClF₃, C₂Cl₂F₄, etc., halogenated borons such as BCl₃, BF₃, etc., and other halides such as SF₅, NF₃, PF₅, etc., and radicals of these gases, such as F* , Cl* , etc. and ions of these gases such as CF₃⁺, CCl₃⁺, etc. These gases can be used alone or in combinations thereof, and other gases such as O₂, H₂, etc. can be added thereto to such an extent as not to give any influence on the film. In order to control the reaction between the gaseous starting material and the gaseous oxidizing agent, both or either of the gaseous starting material and the gaseous oxidizing agent can be diluted with such a gas as Ar, He, N₂, H₂, etc. A means of applying energy in the present process for forming a deposition film includes a halogen lamp, a laser, etc. as a photo energy, where a light beam having a relative long wavelength and such an energy level as not to generate an intense plasma in the film-forming space by irradiation, but to increase the substrate temperature is used and the wavelength of light beam for the irradiation is preferably 0.2 to 20 µm, and also includes heater heat, infrared heat, etc. as heat energy. The energy can be also supplied through a support that supports the substrate, where, for example, a plurality of heaters are provided in the support and the individual heaters are independently controlled to "on" or "off" to change the area on the substrate to be supplied with the energy. A means for periodic modulation of energy intensity includes modulation of intensity of energy source itself, or modulation by a chopper or an electrooptical device or an acoustic-optical device, etc. An optimum modulation of energy intensity is determined in view of the deposition rate, species of oxidizing agent, light intensity and wavelength, photo absorbancy and heat capacity of a substrate etc., and a preferable modulation of energy intensity is such as to make a change in the substrate surface temperature fall in a range of 10° to 80°C. The modulation pattern includes, for example, a sine wave pattern shown in Fig. 3A, a triangular shape pattern shown in Fig. 3B, a saw tooth shape pattern as shown in Fig. 3C and a pulse wave pattern as shown in Fig. 3D, or when energy is applied to the parts on a broad substrate by a narrow beam, raster scanning can be carried out, as shown in Fig. 3E. When the energy is applied in a pulse wave it is needless to say that the duty cycle can be changed, if required. When a crystalline film is deposited with photo-energy as the energy applied, the deposition rate is lowered only by increasing the light intensity, and thus the step of accelerating the deposition by light energy as in the ordinary photo CVD process is not substantially predominant. The irradiating photo-energy does not act to promote the formation of a deposition film. Furthermore, a decrease in the deposition rate takes place likewise even if the light wavelength is longer than that of the visible light, and thus is not due to direct photo-etching, but shows that the etching effect of the chemical deposition process is promoted basically by an increase in the substrate temperature. [Examples] The present invention will be explained in detail below, referring to Examples. Example 1 A polycrystalline silicon film was formed in an apparatus for forming a deposition film as shown in Fig. 1. That is, a polycrystalline silicon film was formed on a glass substrate 104 (# 7059, trademark of a product made by Corning Glass Works) by introducing SiH₄ gas through an inlet pipe 101 and F₂ gas diluted with a He gas to 10 % through an inlet pipe 102 into a reaction chamber 103 under a total pressure of 66.7 Pa (500 m Torr) during the formation of deposition film. The flow rate of the SiH₄ gas was in a range of 15 to 30 sccm and that of the F₂ gas was 30 sccm. As energy source, an Ar gas laser beam of maximum output of 6 W with continuous oscillation was used. Specifically, the laser beam was focussed to a spot, about 1 mm in diameter on the glass substrate and subjected to raster scanning over an area, 3 cm x 2 cm, on the glass substrate by an optical system based on a pair of galvano mirrors, where the repeating frequency of raster scanning was 1 Hz. At that time, the substrate temperatures were 250 °C, 300 °C and 400 °C without laser beam irradiation and when the substrate was irradiated with the laser beam under the above-mentioned conditions, the temperature in given five regions in the substrate was elevated and lowered with a period of 1 Hz, and the peak value was higher by about 40° to 80°C than that without the laser beam irradiation. The measurement of temperatures on the substrate was carried out with a plurality of thermocouples, 0.2 mm in diameter, embedded in the glass substrate. The deposition was continued under the above-mentioned conditions for about 10 to 20 minutes, whereby a polycrystalline film having an average film thickness of about 1.2 µm was obtained (Sample A). Besides the sample A prepared under the above-mentioned conditions, two samples were prepared for comparison at the same time. A first comparative sample (Sample B) was prepared under the same conditions as in the case of Sample A except that laser beam irradiation was not effected and that the film-forming time was adjusted. That is, the film-forming time was adjusted so as to make an average film thickness of about 1.2 µm. A second comparative sample (Sample C) was prepared under the same condition as in the case of Sample A except that the laser beam was subjected to a high speed raster scanning of 100 Hz or more and the temperature of the entire substrate was constantly maintained at a temperature higher by about 40° to 80°C than the temperature without the laser beam irradiation. Results of determining the average grain size of these samples by the peak on (111) plane by X-ray diffraction are shown in Table 1. As is obvious from Table 1, a polycrystalline silicon film of larger grain size can be formed by irradiation of the substrate with a laser beam of periodically modulated intensity in the chemical deposition process, and no deposition of film is obtained in Sample C. It is seen from this fact that it is important to periodically modulate the intensity of laser beam. Example 2 A polycrystalline silicon thin film was formed in an apparatus for forming a deposition film as shown in Fig. 1 in the same manner as in Example 1. That is, a polycrystalline silicon film was formed on a glass substrate 104 (# 7059, trademark of a product by Corning Glass Works) with an area of 15 cm x 15 cm under a total pressure of about 66.7 Pa (500 m Torr) during the formation of the deposition film by introducing SiH₄ gas through an inlet pipe 101 and F₂ gas diluted with He gas to 10 % into a reaction chamber 103, where the flow rate of the F₂ gas was 30 sccm. The substrate was irradiated with energy by switching a halogen lamp beam to "on" or "off" by a chopper at a period of about 2 seconds. The irradiation energy of the halogen lamp used had an energy irradiation density of 1 W/cm² on average on the substrate surface. The substrate temperature without irradiation with the halogen lamp light was about 250°C and the substrate temperature with the irradiation was about 300°C. At the time, the flow rate of the SiH₄ gas was 20 sccm, and an actual flow rate of the F₂ gas was changed to about 50 sccm when not irradiated with the halogen lamp light and to about 30 sccm when irradiated in a synchronized manner. Temperature determination of the substrate was carried out with thermocouples in the same manner as in Example 1. When the deposition was continued for about 10 minutes under the above-mentioned conditions, a polycrystalline deposition film having an average film thickness of about 0.5 µm was obtained (Sample D). The average grain sizes of these samples were determined by the peak on (111) plane by X-ray diffraction. Furthermore, etching rates of these samples were determined in an etching solution, which was a mixture of 49 % fluoric acid solution, a 70 % nitric acid solution and 90 % acetic acid solution in a mixing ratio of 1 : 25 : 25. The results are shown in Table 2 together with results of Sample A at a substrate temperature of 250°C and Sample B at a substrate temperature of 300 °C. As is obvious from the results of etching rates shown in Table 2, the crystalline film according to Example 1 of the present invention (Sample A) is more compact, less in defects and higher in quality than the crystalline film prepared by the conventional chemical deposition process (Sample B), and furthermore the crystalline film according to Example 2 of the present invention (Sample D) is much more compact, much less in defects and much higher in quality than the crystalline film according to Example 1 of the present invention (Sample A). The results of etching rates reveal that the quality of crystalline film of Sample D is most uniform throughout the entire substrate surface. It is evident from the foregoing detailed explanation and Examples that a compact crystalline thin film of larger grain size with less defects can be uniformly formed over a larger area at a low temperature such as about 200° to about 400°C according to the present process for forming a crystalline deposition film.

Claims: A process for forming a crystalline deposition film on a substrate in a reaction space which comprises: (i) separately introducing into said reaction space a gaseous starting material for forming a deposition film and a gaseous oxidizing agent capable of having an oxidation action on the gaseous starting material, (ii) chemically contacting said gaseous starting material and said oxidizing agent, thereby generating a plurality of precursors including a precursor in an excited state, and (iii) utilizing at least one of the generated precursors as a supply source of a film constituent, (iv) supplying to said substrate energy to vary the temperature of said substrate, and (v) varying the intensity of said energy, thereby forming a crystalline deposition film on said substrate in said reaction space. A process according to claim 1, wherein said substrate temperature is changed by varying said energy supplied to said substrate to selectively reduce or increase said substrate temperature such that said substrate temperature is synchronized with the flow ratio of the gaseous oxidizing agent to the gaseous starting material, thereby controlling deposition and etching during the forming of a deposition film on said substrate. A process according to either of claims 1 or 2, wherein said energy is a photo energy. A process according to claim 1, wherein the gaseous starting material is a chain silane compound. A process according to claim 4, wherein the chain silane compound is represented by the general formula: Si n H 2n+2 where n is an integer of 1 to 8. A process according to any one of claims 1 to 5, wherein the gaseous oxidizing agent is a halogen compound. A process according to claim 6, wherein the halogen compound is a fluorine compound. A process according to claim 7, wherein the fluorine compound is a fluorine gas. A process according to any one of claims 1 to 8, wherein a part or the whole of the substrate surface on which a deposition film is formed is composed of an amorphous material. A process according to any one of claims 1 to 9, wherein said energy supplied to the substrate is periodically varied. A process according to claim 2, wherein the substrate temperature is changed in a range of 10°C to 80°C by supply of said energy. A process according to claim 1, wherein said energy is supplied through a support that supports the substrate. A process for forming a crystalline deposited film on a substrate in a reaction space which comprises: (i) separately introducing a gaseous starting material for forming a deposition film and a gaseous oxidizing agent capable of having an oxidation action on the gaseous starting material into said reaction space, (ii) chemically contacting said gaseous starting material and said oxidizing agent, thereby generating a plurality of precursors including a precursor in an excited state, and (iii) utilizing at least one of the generated precursors as a supply source of a film-constituting member, (iv) supplying to an area of said substrate an energy to vary the temperature of said substrate, and (v) changing the area on said substrate to which said energy is to be applied, thereby forming a crystalline deposition film on said substrate in said reaction space. A process according to claim 13, wherein the temperature of a specified region on the substrate surface is changed by changing the area to be supplied with said energy on the substrate. A process according to claim 13 or 14, wherein said energy is a photo energy. A process according to claim 13, wherein the gaseous starting material is a chain silane compound. A process according to claim 16, wherein the chain silane compound is represented by the general formula: Si n H 2n+2 where n is an integer of 1 to 8. A process according to any one of claims 13 to 17, wherein the gaseous oxidizing agent is a halogen compound. A process according to claim 18, wherein the halogen compound is a fluorine compound. A process according to claim 19, wherein the fluorine compound is a fluorine gas. A process according to any one of claims 13 to 20, wherein a part or the whole of the substrate surface on which a deposition film is formed is composed of an amorphous material. A process according to claim 13, wherein said energy is supplied through a support that supports the substrate.

Inventors: HANNA JUN-ICHI, OSADA YOSHIYUKI, HANNA, JUN-ICHI, OSADA, YOSHIYUKI
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1990
Main classification: C23C16
IPC codes: C23C16, H01L21, C30B25