Process for producing a defect-free photoelectric conversion device

Abstract: A process for producing a photoelectric conversion device comprising a substrate having a conductive surface, a semiconductor layer disposed on said conductive surface of substrate, a transparent and conductive layer disposed on said semiconductor layer and a collecting electrode disposed on said transparent and conductive layer, wherein one or more defective portions occurred at the semiconductor layer are repaired by means of electrolytic treatment using an electrolytic solution containing a material capable of providing an insulating material wherein the conductive surface of substrate is made to be an electrode, to thereby deposit an insulating material selectively at each of the defective portions.

Description: BACKGROUND OF THE INVENTION Field of the invention The present invention relates to a process for producing a defect-free photoelectric conversion device. More particularly, the present invention relates to an improved process for producing a defect-free photoelectric conversion device such as solar cell, photosensor, etc. while repairing a defective portion such as pinhole, hillock or the like occurred during the preparation thereof. Related background art In recent years, various studies have been made of large area photoelectric conversion devices such as solar cell, photosensor, electrophotographic photosensitive device, flat panel display, etc. The public attention has been focused on non-single crystal semiconductors such as amorphous silicon semiconductors to constitute those large area semiconductor devices mainly because of their reasonable production cost. For instance, there is known a pin junction type amorphous silicon solar cell as an example of such non-single crystal semiconductor device. In this solar cell, photocarriers are caused in its semiconductor layer comprising an amorphous silicon semiconductor thin film when light is impinged in the solar cell, those photocarriers migrate to its transparent electrode comprising a transparent conductive thin film situated on the side through which light is impinged and also to its conductive substrate situated opposite the transparent electrode by the action of an internal electric field, to thereby provide a photoelectromotive force. The conductive thin film to be the transparent electrode and the semiconductor thin film to be the semiconductor layer may be properly formed in a vacuum chamber in accordance with a plasma CVD method, a photo CVD method, a thermal CVD method, a vacuum evaporation method, or a sputtering method. In the preparation of such amorphous silicon solar cell, there is often found a problem that a short circuit is caused between the transparent electrode and the conductive substrate due to pinholes occurred at part of the semiconductor layer. There are various causes for such pinholes to be occurred. For instance, in one case, since the transparent electrode is usually of some hundreds angstrom (10 Å = 1 nm) in thickness and the semiconductor layer is usually of about 0.005 to some tens µm, minute dusts (some micrometer to some tens micrometer in size) are deposited on the surface of the conductive substrate or they are deposited on or contaminated into the semiconductor layer during film formation to cause removal of the conductive substrate or/and the semiconductor layer, whereby such pinholes are occurred at the semiconductor layer. In other case, such pinholes are occurred when part of the semiconductor layer is removed due to its internal stress or its insufficient adhesion with the transparent electrode to furnish the conductive substrate with a region not having a desired semiconductor layer. In this case, the transparent electrode situated on the side through which light is impinged and the conductive substrate situated opposite said electrode are connected with each other through said region to be in an electrically short-circuited state, and because of this, the resultant becomes extremely poor in the characteristics as a semiconductor device. The occurrence of pinholes causing a short circuit is a serious problem particularly in the case of a large area photoelectric conversion device such as solar cell, electrophotographic photosensitive device, etc. In any case, it is extremely difficult to obtain a large area photoelectric conversion device completely free of a short-circuited state region even under clean environment substantially free of minute dusts. In order to solve the above problem relative to occurrence of pinholes causing a short circuit, Japanese Laid-open patent application 62(1987)-53958 (hereinafter referred to as Literature 1) proposes a method of making the inside of each of pinholes occurred at the thin film semiconductor layer of a photosemiconductor to be in an electrically insulating state by perforating pinholes at its electrode layer and communicating the pinholes of the thin film semiconductor layer with the pinholes of the electrode layer. Similarly, Japanese Laid-open patent application No. 62(1987)-59901 (hereinafter referred to as Literature 2) proposes a method of reclaiming pinholes occurred at the thin film semiconductor layer of a semiconductor device by fusing the peripheries of the pinholes with radiation of energy beam. FIGs. 10(a) and 10(b) are schematic views respectively for explaining the method according to Literature 1. In FIGs. 10(a) and 10(b), numeral reference 1 stands for a translucent substrate, numeral reference 2 stands for a translucent electrode layer, numeral reference 3 stands for a semiconductor layer comprising a thin semiconductor film, numeral reference 4 stands for a back electrode layer, numeral reference 5 stands for a pinhole in a short-circuited state, numeral reference 6 stands for a pinhole provided at the back electrode layer, numeral reference 7 stands for laser beam, and numeral reference 8 stands for laser beam. The method according to Literature 1 will be explained with reference to FIGs. 10(a) and 10(b). That is, after a plurality of semiconductor devices having been prepared, the semiconductor devices defective in view of short circuit among them are sorted out. As for each of those defective semiconductor devices, beam plane-scanning is performed while irradiating laser beam 7 through other principal face of the translucent substrate 1 as shown in FIG. 10(a). When short circuit current is measured for the semiconductor device is measured at the time of performing the beam plane-scanning, short circuit current does not flow when the laser beam 7 is irradiated to the portion where a pinhole 5 in a short-circuited state is present. On the other hand, upon irradiating the laser beam 7 to other portion where such short-circuited state is not present, hole-electron pair are caused and they migrate in the semiconductor layer 3, whereby short circuit current flows. In view of this, the position where a pinhole 5 is present can be found for the semiconductor device by performing plane-scanning using the laser beam 7. As for the portion of the semiconductor layer where a pine hole 5 is present, laser beam outputted from YAG pulse laser of 5 x 10 6 W/cm 2 in peak outputting power is radiated through the back electrode layer 4 in the way as shown by an arrow 8 to thereby remove a short-circuited state region comprising the constituent of the back electrode layer 4 which is extended to the inside of the pinhole 5. Particularly, as shown in FIG. 10(b), a pinhole 6 is made at the back electrode layer 4 formed on the semiconductor layer 3 having the pinhole 5 occurred therethrough at the time of the formation thereof such that it is coaxially in communication with the pinhole 5, whereby the inside of the pinhole 5 and that of the pinhole 6 are made to be in an electrically insulating state. FIGs. 10(c), 10(d) and 10(e) are schematic views for explaining the method according to Literature 2. In FIGs. 10(c), 10(d) and 10(e), numeral reference 1 stands for a translucent substrate, numeral reference 2 stands for a translucent electrode layer, numeral reference 3 stands for a semiconductor layer comprising a thin semiconductor film, numeral reference 4 stands for a back electrode layer, numeral reference 5 stands for a pinhole in a short-circuited state, numeral reference 7 stands for laser beam, and numeral reference 9 stands for photosensor. The method according to Literature 2 will be explained with reference to FIGs. 10(c) through 10(e). That is, a translucent electrode 2 is formed on a translucent substrate 1 and then, a thin film semiconductor layer 3 is formed on the translucent electrode 2. As for the device thus obtained, plane-scanning is performed for the semiconductor layer 3 while irradiating laser beam 7 outputted from an Ar gas laser of an extremely low outputting power through the rear side of the semiconductor layer 3 and moving a photosensor 9 arranged on the side of the translucent substrate 1 and opposite the Ar gas laser in synchronism with the scanning of the laser beam 7 in the way as shown in FIG. 10(c), to thereby examine whether or not the semiconductor layer 3 is accompanied with a pinhole 5. In this case, if such pinhole 5 is not present at the portion of the semiconductor layer 3 where the laser beam 7 is irradiated, the laser beam 7 is absorbed by the semiconductor 3 and does not reach the photosensor 9. On the other hand, if such pinhole 5 is present at the portion of the semiconductor layer 3 where the laser beam 7 is irradiated, the laser beam 7 reaches the photosensor 9, and based on a signal outputted from the photosensor 9 at that time, the position where the pinhole 5 is present is detected. When the presence of the pinhole 5 is optically detected as above described, laser beam of about 2 to 3 W/cm 2 in power outputted from, for example, an Ar gas laser of 514.5 nm in oscillating wavelength instead of the laser beam 7 is irradiated to the portion where the pinhole 5 is present, to thereby fuse the peripheries of the pinhole 5 with respect to the semiconductor layer 3, whereby the pinhole 5 is filled up with the constituent of the semiconductor layer 3 in such a state as shown in FIG. 10(d). The filled portion of the semiconductor layer 3 exhibits a fused state at the beginning but it is soon or later cooled, wherein the constituent of the filled portion is changed from amorphous state to polycrystalline state or the like and the junction state is eventually broken. Thus, the filled portion finally becomes to function substantially as an insulator. Finally, as shown in FIG. 10(e), an aluminum layer as a back electrode 4 is laminated on the semiconductor layer 3 having the above filled portion by a vacuum evaporation technique. The above mentioned two methods are effective in order to solve the foregoing problems relative to short circuit caused due to pinholes occurred at the semiconductor layer to a certain extent, but there still exist such problems as will be under mentioned, which are necessary to be solved. In the case of the method according to Literature 1, there is a problem that it takes a long period of time in order to detect a number of pinholes being present at the semiconductor layer of a large area by way of the laser beam scanning process. There is also other problem for the method according to Literature 1. That is, as apparent from what shown in FIGs. 10(a) and 10(b), the pinhole 6 is left as it is in any case. Such pinhole is necessary to be filled up in practice. Particularly, in the case of a semiconductor device in which the pinhole is left without being filled up, water, alkaline metal, or the like are apt to enter therethrough upon use. Once water or/and alkaline metal, etc. entered thereinto, the semiconductor device will be deteriorated shortly. However, in order to fill up such pinhole, not only a specific technique is required but also it takes time, and because of this, the resulting product becomes unavoidably costly. Likewise, there are problems also for the method according to Literature 2. That is, in the case of the method according to Literature 2, as apparent from what shown in FIGs. 10(c) through 10(e), the pinhole 5 is filled up by fusing the peripheries thereof, but this process is performed prior to forming the back electrode layer 4, and because of this, a pinhole which will be caused at the time of forming the back electrode layer on the semiconductor layer 3 having the filled portion is unavoidably left without being filled up. In addition to this, since to fill up the pinhole 5 is performed through the laser beam-irradiating process which takes time while exposing the semiconductor layer 3 to environmental atmosphere, the quality of the semiconductor 3 is apt to deteriorate during the filling up process. Further in addition, powdery materials are caused when the semiconductor layer 3 is liquefied or vaporized because of heat from the laser beam irradiated thereto wherein those powdery materials are scattered to deposit on the surface of the semiconductor layer and as a result, the resulting device becomes defective in the characteristics. As for the method according to Literature 2, there are disadvantages that it takes a long period of time in order to detect a number of pinholes being present at the semiconductor layer of a large area by way of the laser beam scanning process; and it is extremely difficult to fill up all such numerous pinholes uniformly by way of the laser beam fusing process. In view of the above, in the case of the method according to Literature 2, if a desirable semiconductor device should be obtained, it will be unavoidably costly. The term "defective potion" herein is meant to include a portion where a pinhole is present, a portion where a hillock extending from the conductive layer is present and a portion where a pinhole having said hillock therein is present, these portions being liable to cause short circuit. In the article "Improvement of amorphous silicon solar cells by electrochemical treatments" by M. Matsumura et al., J. Appl. Phys. 61(4), p 1648 (1987), a process for producing a photoelectric conversion device is disclosed, in which a semiconductor film is deposited on a substrate comprising a glass substrate and a transparent conductive layer such as an ITO layer. An insulation material is subsequently deposited on the transparent conductive layer at the position of a crack. Thereafter, an Al layer is deposited on the semiconductor film. Substrates suggested to be used in the above process are precoated substrates on which the transparent conductive layer (ITO) is already arranged. It is an object of the present invention to provide a process for producing a photoelectric conversion device capable of improving the repairing efficiency. This object is achieved by a process as claimed in claim 1. The present invention has been accomplished based on the following findings obtained as a result of experimental studies by the present inventor in order to attain the foregoing objects. That is, the present inventor employed electrolytic reduction etching treatment in order to repair a defective solar cell having one or more defective portions. Particularly, there were provided a plurality of solar cells of the configuration shown in FIG. 7. In FIG. 7, numeral reference 14 stands for a solar cell comprising a conductive substrate 10, an amorphous silicon semiconductor layer 11 formed on said conductive substrate, a transparent electrode layer 12 comprising ITO (In 2 O 3 + SnO 2 ) formed on said semiconductor layer and a collecting electrode 13 formed on said transparent electrode layer, wherein no defective portion is shown. Each of the solar cells thus provided was immersed in an aqueous solution of hydrochloric acid as an etching liquid contained in an electrolytic reduction etching treatment vessel as shown in FIG. 8. In FIG. 8, numeral reference 27 stands for said electrolytic etching treatment vessel and numeral reference 25 stands for said aqueous solution of hydrochloric acid. Likewise, numeral reference 24 stands for an anode and numeral reference 26 stands for a power source electrically connected to the anode 24. The power source 26 is also electrically connected to the conductive substrate 10 of the solar cell 14 immersed in the aqueous solution of hydrochloric acid 25 wherein the conductive substrate 10 serves as a cathode. Numeral reference 23 stands for a protective member disposed on the rear face of the conductive substrate 10 of the solar cell 14. The power source 26 was switched on to apply electric power between the anode 24 and the cathode (that is, the conductive substrate 10). In the case where the solar cell 14 was defective one that has one or more defective portions, current-flow was caused selectively at each of such defective portions through the conductive substrate 10 and the transparent electrode layer 12 comprising ITO, wherein etching was occurred only at the portion of the transparent electrode layer 12 where the short-circuited portion was present. The etching herein was considered to have been occurred due to the following chemical reactions. In 2 O 3 + 8H + + 2e - → 2In 3+ + 3H 2 O + H 2 SnO 2 + 4H + + 2e - → Sn 2+ + 2H 2 O In this case, such etching was not occurred at other portion of the transparent electrode layer where no defective portion was present since current-flow was not caused. The defective solar cell could be repaired in this way. The above procedures were repeated to thereby repair a plurality of defective solar cells having one or more defective portions. Each of the solar cells thus repaired was evaluated with respect to the photovoltaic characteristics including photoelectric conversion efficiency and durability. As a result, it was found that the solar cell repaired by the above electrolytic reduction etching treatment is superior to the solar cell repaired by the laser processing in the prior art with respect to the photovoltaic characteristics. However, it was found that the solar cells repaired by the above electrolytic reduction etching treatment are varied with respect to the photovoltaic characteristics. The present inventor experimentally investigated the reason for this. As a result, there was obtained a finding that there are various causes for the defective portion to be occurred in a solar cell and a certain defective potion cannot be repaired by the above electrolytic reduction etching treatment. This situation will be explained with reference to FIG. 9. FIG. 9 is a schematic cross section view illustrating an example of the solar cell repaired by the above electrolytic reduction etching treatment in which such defective portion still remains as unrepaired. Particularly, in the solar cell shown in FIG. 9, numeral reference 16 stands for a defective portion (pinhole) repaired by the electrolytic reduction etching treatment and numeral reference 15 stands for a defective portion (pinhole) which was not repaired by the electrolytic reduction etching treatment. As apparent from what shown in FIG. 9, it is understood that the defective portion situated below the collecting electrode 13 is left as not repaired by the electrolytic reduction etching treatment, whereas the defective portion situated at the position above which the collecting electrode 13 is not positioned is repaired. In addition to this finding, the present inventor also found that leakage of current at the defective portion situated under the collecting electrode is greater than that at other defective portion situated at the position above which the collecting electrode is not positioned. The present inventor then repeated experimental studies in order to find an appropriate means which enables to effectively repair all the defective portions of a solar cell regardless of their positions situated. As a result, it was found that when an electro-deposition process, an electrolytic polymerization process or an electrolytic process is employed in order to repair a defective solar cell having one or more defective portions, an insulating material is selectively deposited only at those defective portions, whereby the defective solar cell is repaired to be a practically usable solar cell. The electro-deposition process means a process of depositing an insulating material on an object by applying a voltage between opposite electrodes in an aqueous solution of a paint or a dispersion of a resin. The paint or the resin may be those capable of being negatively or positively charged. Specific examples are paints and resins having carboxyl group which can be negatively charged, and paints and resins having amino group which can be positively charged. In order to repair a defective solar cell having one or more defective portions by the electro-deposition process, the defective solar cell, which serves as an anode or cathode, is immersed in the foregoing aqueous solution or dispersion, in which a counter electrode is also immersed. A voltage, desirably of 5 to 50 V is then applied between the solar cell and the counter electrode to cause an electric field, desirably under the condition of 1 to 100 mA/cm 2 in current density, by which the paint or the resin is negatively or positively charged, and the charged paint or resin moves to cause selective deposition of an insulating material only at each of the defective portions of the solar cell so as to cover each of the defective portions in a state that no short circuit is caused. The electrolytic polymerization process means a process of depositing a polymer film on an object by applying a voltage of direct current (hereinafter referred to as direct current voltage) between the object as an anode and a counter electrode as a cathode in an electrolytic liquid comprising a solution or a dispersion of a monomer to thereby polymerize the monomer. In order to repair a defective solar cell having one or more of defective portions by the electrolytic polymerization process, the defective solar cell, which serves as the anode, is immersed in an electrolytic liquid comprising a solution or a dispersion of a given monomer, in which a counter electrode as the cathode is also immersed. A direct current voltage, desirably of 0.5 to 20 V is applied between the defective solar cell and the counter electrode, desirably under the condition of 0.1 to 100 mA/cm 2 in current density, wherein the monomer of the electrolytic solution in the vicinity of each of the defective portions of the defective solar cell is polymerized due to current-flow caused through the defective portion, whereby deposition of a polymer film is selectively caused only at each of the defective portions so as to cover each of the defective portions in a state that no short circuit is caused. Specifically, the electrolytic liquid used comprises an electrolyte and a monomer dissolved in a solvent. Specific examples of the electrolyte are acids such as H 2 SO 4 , HCl, HNO 3 etc., and salts comprising monovalent metal ions such as Li + , K + , Na + , Rb + , Ag + , etc. or tetraammonium ions such as TBS + (tetrabutylammonium ion), TEA + (tetraethylammonium ion), etc. and Lewis acid ions such as BF 4 P - , PF 6 - , AsF 6 - , ClO 4 - , etc. The electrolytic liquid may contain CuCl 2 or FeCl 3 other than such electrolyte. Specific examples of the solvent are water, alcohols, acetonitrile (CH 3 CN), benzonitrile (C 6 H 5 CN), propylene carbonate (PC), dimethylformamide (DMF), tetrahydrofuran (THF), nitrobenzene (C 6 H 5 NO 2 ), etc. Specific examples of the monomer are compounds having a conjugated double bond such as pyrrole, aniline, thiophene, benzene, furan, phenol, dimethoxyphenol, phenylsilanol, thiophenol, vinylcarbazole, pyridazine, selenophene, etc. Among these compounds, cyclic compounds are preferred and cyclic compounds containing oxygen atom (O) or silicon atom (Si) are the most preferred. Use of an organic solvent is desired in order for the resulting polymer film to be excelling in adhesion, dense in texture and free of pinhole. In order to improve the insulating property of the resulting polymer film, it is desired that the anions contained in the polymer film formed as a result of the electrolytic polymerization of the monomer are released therefrom by applying a voltage of a reverse polarity between the solar cell (as a cathode in this case) and a counter electrode (anode). The electrolytic process means a process of depositing an oxide film on an object by applying a direct current voltage between opposite electrodes in an electrolytic solution containing an inorganic compound. In order to repair a defective solar cell having one or more defective portions by the electrolytic process, the defective solar cell, which serves as an anode, is immersed in an electrolytic solution containing an inorganic compound, in which a counter electrode (cathode) is immersed. A direct current voltage, desirably of 0.5 to 50 V is then applied between the solar cell as the anode and the cathode, desirably under the condition of 1 to 1000 mA/cm 2 in current density, whereby deposition of an oxide film is selectively caused only at each of the defective portions so as to cover each of the defective portions in a state that no short circuit is caused. As the electrolytic solution, there can be used an aqueous solution of sulfuric acid, oxalic acid, phosphoric acid, boric acid or chromic acid. Specific examples of the inorganic compound are MnSO 4 , H 2 SiF 6 , etc. The electrolytic solution used in any of the electro-deposition process, the electrolytic polymerization process and the electrolytic process is desired to additionally contain an insulator in the form of a fine particle (hereinafter referred to as fine particle insulator) and one or more additives selected from surfactant, metal alkoxide, acetyacetone metal complex, metal octylate, metal naphthenate, phosphazene, etc. Specific examples of the fine particle insulator are alumina, silica, titanium oxide, tantalum oxide, zirconium oxide, glass, silicon carbide, silicon nitride, barium sulfate, fluorinated graphite, ethylene fluoride, polyvinyl chloride, epoxy resin, etc. The fine particle insulator is desired to be of 0.01 to 10 micrometers in the mean particle size. In the case of using such fine particle insulator in combination with an ionic surfactant in the electro-deposition process, the efficiency of electro-deposition is improved. As the metal alkoxide, there can be illustrated ethoxy or butoxy alkoxides of silicon, aluminum, titanium, tantalum, germanium, zirconium, etc. Specific examples are tetraethoxy silicon, tripropoxy silicon, tetrabutoxy silicon, triethoxy aluminium, tripropoxy aluminum, tributoxy aluminium, etc. Specific examples of the acetylacetone metal complex are acetylacetone aluminium complex, acetylacetone titanium complex, acetylacetone manganese complex, and acetyl acetone barium complex. Specific examples of the metal octylate are aluminium octylate, zirconium octylate, manganese octylate and barium octylate. Specific examples of the metal naphthenate are zirconium naphthenate and manganese naphthenate. The process according to the present invention makes it possible to efficiently produce a desirable defect-free photoelectric conversion device of a large area with an improved yield even in the case of using a conductive member accompanied by a plurality of minute protrusions such as stainless steel as the conductive substrate which is apt to cause defective portions, which lead to occurrence of short circuit, at the photoelectric conversion layer formed thereon. Particularly, those defective portions caused at the photoelectric conversion layer are repaired by an insulating material selectively deposited at each of those defective portions and because of this, the resulting photoelectric conversion device becomes to be such that is free of defective portions, which are liable to cause short circuit, that outputs a satisfactory electric current, and that is hardly deteriorated even upon repeated use over a long period of time. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a schematic cross section view illustrating the constitution of an example of a repaired photoelectric conversion device. FIG. 2 is a schematic cross section view illustrating the constitution of a repaired photoelectric conversion device in the present invention. FIGs. 3(a) through 3(c) are schematic explanatory views illustrating the steps of obtaining the repaired photoelectric conversion device shown in FIG. 1. FIG. 4 is a schematic diagram of an example of an electrolytic treatment apparatus employed in the present invention. FIGs. 5(a) through 5(c) are schematic explanatory views illustrating the steps of obtaining the repaired photoelectric conversion device shown in FIG. 2. FIG. 6 is a schematic diagram of an example of an electrolytic reduction etching apparatus employed in the present invention. FIGs. 7, 8 and 9 are schematic views for explaining the method of repairing a defective photoelectric conversion device by means of selectively etching techique. FIGs. 10(a), 10(b), 10(c), 10(d) and 10(e) are schematic views respectively for explaining a conventional method of repairing a defective semiconductor device. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The process for producing a defect-free photoelectric conversion device is characterized as including the step of repairing a defective portion liable to cause short circuit ,comprising a pinhole, hillock, pinhole having a hillock therein, or the like, occurred at the constituent elements of a photoelectric conversion device during the formation thereof by virtue of a method of selectively forming an insulating material utilizing an electro-deposition process, an electrolytic polymerization process or an electrolytic process. The process according to the present invention makes it possible to efficiently produce a defect-free large area photoelectric conversion device at an improved yield. The process according to the present invention is applicable not only in the production of a solar cell but also in the production of other photoelectric conversion devices such as photosensor, electrophotographic photosensitive member, etc. The process according to the present invention is particularly effective in the production of a solar cell. In the following, explanation will be made of the process according to the present invention in the case of producing a defect-free solar cell. Shown in FIG. 1 is a schematic cross section view of the constitution of an example of a repaired solar cell. Shown in FIG. 2 is a schematic cross section view of the constitution of a repaired solar cell produced by the process according to the present invention. In FIG. 1, numeral reference 100 stands for a conductive substrate. Numeral reference 101 stands for a conductive layer as a lower electrode disposed on the conductive substrate 100. Numeral reference 102 stands for a semiconductor later disposed on the lower electrode (conductive layer) 101. Numeral reference 103 stands for a transparent conductive layer as an upper electrode disposed on the semiconductor layer 102. Numeral reference 104 stands for a collecting electrode being disposed on the upper electrode (transparent conductive layer) 103. Numeral reference 105 stands for a defective portion comprising a hillock extending from the conductive layer occurred in the semiconductor layer 102 above which the collecting electrode 104 is not positioned. Numeral reference 105' stands for other defective portion comprising a pinhole containing a hillock extending from the conductive layer 101 occurred in the semiconductor layer 102 situated under the collecting electrode 104. Numeral reference 106 stands for an insulating film formed so as to cover the defective portion 105 in a state that no short circuit is caused. Numeral reference 106' stands for an insulating film formed so as to fill up the defective portion 105' in a state that no short circuit is caused. In FIG. 2, numeral reference 200 stands for a conductive substrate. Numeral reference 201 stands for a conductive layer as a lower electrode disposed on the conductive substrate 200. Numeral reference 202 stands for a semiconductor later disposed on the lower electrode (conductive layer) 201. Numeral reference 203 stands for a transparent conductive layer as an upper electrode disposed on the semiconductor layer 202. Numeral reference 204 stands for a collecting electrode being disposed on the upper electrode (transparent conductive layer) 203. Numeral reference 205 stands for a defective portion comprising a hillock extending from the conductive layer 201 occurred in the semiconductor layer 202 above which the collecting electrode 204 is not positioned. Numeral reference 205' stands for other defective portion comprising a pinhole containing a hillock extending from the conductive layer 201 occurred in the semiconductor layer 202 situated under the collecting electrode 204. Numeral reference 206 stands for an insulating film formed so as to cover the defective portion 205 while penetrating the upper electrode 203 in a state that no short circuit is caused. Numeral reference 206' stands for an insulating film formed so as to fill up the defective portion 205' while penetrating the upper electrode 203 in a state that no short circuit is caused. In the case of the repaired solar cell shown in FIG. 1, any of the defective portions 105 and 105' is covered or filled up by the insulating material 106 or 106' selectively deposited at the corresponding defective portion by virtue of the foregoing method of selectively forming an insulating material utilizing an electro-deposition process, an electrolytic polymerization process or an electrolytic process such that no current leakage is not occurred between the lower electrode 101 and the upper electrode 103. Likewise, in the case of the repaired solar cell shown in FIG. 2, any of the defective portions 205 and 205' is covered or filled up by the insulating material 206 or 206' selectively deposited at the corresponding defective portion by virtue of the foregoing method of selectively forming an insulating material utilizing an electro-deposition process, an electrolytic polymerization process or an electrolytic process such that no current leakage is not occurred between the lower electrode 201 and the upper electrode 203. The conductive substrate (100 or 200) is comprised of a metal member such as stainless steel, aluminium, copper, titanium, carbon sheet, galvanized sheet metal, etc. The conductive layer as the lower electrode (101 or 201) is comprised of a metallic material such as Ti, Cr, Mo, W, Al, Ag, Ni, etc. In an alternative, the conductive substrate (100 or 200) may be designed such that it serves also as the lower electrode (101 or 201). It is possible to dispose a diffusion preventive layer comprising an inorganic oxide such as ZnO, TiO 2 , SnO 2 , etc. on the conductive layer as the lower electrode (101 or 201) in case where necessary. The conductive layer as the lower electrode may be formed by a resistance heating evaporation method, an electron beam evaporation method, a sputtering method or a MO-CVD method. The semiconductor layer (102 or 202) is comprised of a non-single crystal material such as polycrystalline material, microcrystalline material or amorphous material. The semiconductor layer may be a pn junction layer, a pin junction layer or a hetero junction layer respectively comprising a plurality of semiconductor films being different in conduction type or band gap which are stacked. Specifically, the semiconductor layer is composed of a non-single crystal silicon-containing material such as non-single crystal silicon, non-single crystal silicon carbide, non-single crystal silicon germanium, and the like which may be formed by a plasma CVD method, a light CVD method, a thermal CVD method, a vacuum evaporation method or a sputtering method. In the case where the semiconductor layer is desired to be composed of an amorphous silicon material or a microcrystalline silicon material, the plasma CVD method is the most appropriate for the formation thereof. Other than the above film-forming methods, it is possible to employ a so-called casting method wherein fused silicon is firstly provided and the fused silicon is spread out in a sheet-like state while cooling, whereby a desired semiconductor layer is formed. This casting method is appropriate for the semiconductor later to be of a large area. The semiconductor layer (102 or 202) may be comprised of a compound semiconductor material such as CdS, CdTe, CuInSe 2 , ZnSe, ZnSeTe or the like which may be formed by an electron beam evaporation method, a sputtering method or an electro-deposition method. The transparent conductive layer as the upper electrode (103 or 203) is comprised of an inorganic oxide material such as In 2 O 3 , SnO 2 , ITO (In 2 O 3 + SnO 2 ), ZnO, TiO 2 , Cd 2 SnO 4 , etc. or a crystalline semiconductor film doped with an impurity at a high concentration. The transparent conductive layer as the upper electrode may be formed by a heat resistance evaporation method, an electron beam evaporation method, a sputtering method, a spray coating method, a chemical vapor deposition method or an impurity diffusion method. The collecting electrode (104 or 204) is comprised of a metallic material such as Ti, Cr, Mo, W, Al, Ag, Ni, Cu or Sn. Alternatively, the collecting electrode may be formed using a conductive paste such as Ag-paste or Ni-paste. The collecting electrode comprising such metallic material may be formed by an appropriate method such as a sputtering method wherein a mask pattern is used; a heat resistance evaporation method; a chemical vapor deposition method; a method wherein a metallic is firstly deposited on the entire area, followed by subjecting the resultant to patterning by means of etching; a method wherein a patterned collecting electrode is formed by means of light CVD technique; or a method wherein a negative pattern mask for the pattern of a collecting electrode is firstly formed, followed by subjecting the resultant to plating processing. The collecting electrode comprising the foregoing conductive paste may be formed by applying such conductive paste, for example, by means of screen printing technique. Explanation will be made of a process of producing a repaired photoelectric conversion device of the configuration similar to that shown in FIG. 1 with reference to FIGs. 3(a) through 3(c) and FIG. 4. FIG. 3(a) is a schematic cross section view illustrating the situation of a defective photoelectric conversion element having neither a transparent conductive layer as the upper electrode nor a collecting electrode in which defective portions are present; FIG. 3(b) is a schematic cross section view illustrating the situation of a photoelectric conversion element in which the defective portions shown in FIG. 3(a) are repaired by the electrolytic treatment; and FIG. 3(c) is a schematic cross section view illustrating the configuration of a finished photoelectric conversion device. FIG. 4 is a schematic diagram of an example of an apparatus suitable for practicing the electrolytic treatment according to the present invention. Now, there is firstly provided a conductive substrate 100 comprising the foregoing metal member. On the conductive substrate 100 are successively formed a conductive layer to be the lower electrode 101 comprising the foregoing metallic material and a semiconductor layer 102 comprising the foregoing semiconductor material. Thus, there is obtained a photoelectric conversion element comprising the conductive layer as the lower electrode 101 and the semiconductor layer 102 being disposed in this order on the conductive substrate 100. However, during the formation of this element, there are often occurred defective portions: a pinhole 105" due to deposition or release of foreign matter such dust, etc., a hillock 105 grown from the conductive layer as the lower electrode due to heat, and another pinhole 105" having a hillock 105' extending from the conductive layer as the lower electrode, as shown in FIG. 3(a). These defective portions present in the defective photoelectric conversion element are repaired by subjecting the defective photoelectric conversion element to the electrolytic treatment according to the present invention using the apparatus shown in FIG. 4 to deposit an insulating material 106 selectively at each of the defective portions, whereby the pinhole 105" is filled up with the insulating material, the hillock 105 is covered by the insulating film, and the pinhole 105" containing the hillock 105' is filled up with the insulating material respectively as shown in FIG. 3(b), respectively in a state that no short circuit is caused. Then, on the surface of the semiconductor layer 102 of the repaired photoelectric conversion element are successively formed a transparent conductive layer as the upper electrode 103 comprising the foregoing inorganic oxide material or the foregoing impurity-doped crystalline semiconductor film and a collecting electrode 104 comprising the foregoing metallic material as shown in FIG. 3(c). As a result, there is obtained a finished photoelectric conversion device in which the defective portion situated under the collecting electrode is sufficiently repaired in a desirable state and which is free of occurrence of short circuit. Explanation will be made of the above step of repairing the defective photoelectric conversion element by subjecting it to the electrolytic treatment according to the present invention using the apparatus shown in FIG. 4. As above described, FIG. 4 is a schematic diagram of an example of an apparatus suitable for practicing the electrolytic treatment according to the present invention. Any of the foregoing electro-deposition process, the foregoing electrolytic polymerization process and the foregoing electrolytic process can be optionally employed for practicing the electrolytic treatment. And any of these processes can be practiced in the apparatus shown in FIG. 4. In FIG. 4, numeral reference 511 stands for an electrolysis vessel in which an electrolytic solution 507 is contained. Numeral reference 508 stands for a counter electrode immersed in the electrolytic solution 507. The counter electrode 508 is electrically connected to a D.C. power source 509. The D.C. power source is electrically connected to a defective photoelectric conversion element to be repaired which is immersed in the electrolytic solution 507. The photoelectric conversion element shown in FIG. 4 is in a repaired state corresponding to the repaired photoelectric conversion element shown in FIG. 3(b). The photoelectric conversion element comprises a conductive layer 501 as the lower electrode and a semiconductor layer 502 being disposed in this order on a conductive substrate 500. Numeral reference 510 stands for a protective member, which is disposed such that it covers not only the entire rear surface but also the opposite side faces of the conductive substrate 500. The protective member 510 serves not only to prevent the conductive substrate 500 from contacting the electrolytic solution 507 but also prevent the electrolytic reaction caused from being reduced in terms of efficiency. The conductive substrate 500 or the lower electrode 501 serves an electrode to oppose the counter electrode 508. Numeral reference 505 stands for a defective portion comprising a hillock extending from the conductive layer as the lower electrode 501, numeral reference 505' stands for other defective portion comprising a pinhole, and numeral reference 505" stands for a further defective portion comprising a pinhole containing a hillock extending from the conductive layer as the lower electrode 501. The counter electrode 508 is made of a corrosion resistance material such as platinum, carbon, nickel or stainless steel. The protective member 510 is comprised of an insulating film of acetylcellulose or magnetic rubber. Under this situation, the foregoing electro-deposition process, the foregoing electrolytic polymerization process or the foregoing electrolytic process is performed to deposit an insulating material 506 selectively at each of the defective portions, whereby the pinhole 505' is filled up with the insulating material, the hillock 505 is covered by the insulating film, and the pinhole 105" containing the hillock is filled up with the insulating material respectively as shown in FIG. 4, respectively in a state that no short circuit is caused. Explanation will be made of the process of producing a repaired photoelectric conversion device of the configuration similar to that shown in FIG. 2 according to the present invention with reference to FIGs. 5(a) through 5(c) and FIG. 6. FIG. 5(a) is a schematic cross section view illustrating the situation of a defective photoelectric conversion element not having a collecting electrode in which defective portions are present; FIG. 5(b) is a schematic cross section view illustrating the situation of a photoelectric conversion element in which the defective portions shown in FIG. 5(a) are repaired by the electrolytic treatment according to the present invention; and FIG. 5(c) is a schematic cross section view illustrating the configuration of a finished photoelectric conversion device. FIG. 6 is a schematic diagram of an electrolytic etching apparatus. Now, there is firstly provided a conductive substrate 200 comprising the foregoing metal member. On the conductive substrate 200 are successively formed a conductive layer to be the lower electrode 201 comprising the foregoing metallic material, a semiconductor layer 202 comprising the foregoing semiconductor material, and a transparent conductive layer to be the upper electrode 203 comprising the foregoing inorganic oxide material or the foregoing crystalline semiconductor film. Thus, there is obtained a photoelectric conversion element comprising the conductive layer as the lower electrode 201, the semiconductor layer 202 and the transparent conductive layer as the upper electrode 203 being disposed in this order on the conductive substrate 200. However, during the formation of this element, there are often occurred defective portions: a pinhole due to deposition or release of foreign matter such dust, etc., a hillock 205 grown from the conductive layer as the lower electrode due to heat, and another pinhole having a hillock 205 extending from the conductive layer as the lower electrode, as shown in FIG. 5(a). According to the invention prior to subjecting the defective photoelectric conversion element to the repairing treatment by the electrolytic technique, the corresponding portions of the transparent conductive layer 203 under which the defective portions are present are removed by subjecting the defective photoelectric conversion element to electrolytic etching treatment using the electrolytic etching apparatus shown in FIG. 6. The electrolytic etching apparatus shown in FIG. 6 is of the same constitution as that of the apparatus shown in FIG. 4, except that the electrolytic solution 507 in FIG. 4 is replaced by an electrolytic etching solution 507'. As the electrolytic etching solution 507', there is used, for example, an electrolytic solution containing hydrogen ion and/or hydronium ion. The conductive substrate 500 or the conductive layer as the lower electrode 501 of the defective photoelectric element immersed in the electrolytic etching solution 507' is made as a cathode, and the counter electrode 508 is made as an anode. Then, the D.C. power source 509 is switched on to apply a predetermined voltage with a predetermined current density between the two electrodes, wherein the corresponding portions of the transparent conductive layer 203 under which the defective portions are present are selectively reduced and dissolved into the electrolytic etching solution 507'. As a result, there is afforded a defective photoelectric conversion element of which defective portions being exposed through the transparent conductive layer as the upper electrode as shown in FIG. 5 (b). The defective photoelectric conversion element thus obtained is then subjected to the same electrolytic repair treatment as in the above embodiment using the apparatus shown in FIG. 4 to deposit an insulating material 206 selectively at each of the defective portions, whereby the pinhole is filled up with the insulating material, the hillock is covered by the insulating film, and the pinhole containing the hillock is filled up with the insulating material respectively as shown in FIG. 5(c), respectively in a state that no short circuit is caused. Then, on the surface of the transparent conductive layer as the upper electrode of the repaired photoelectric conversion element is formed a collecting electrode 204 comprising the foregoing metallic material as shown in FIG. 5(c). As a result, there is obtained a finished photoelectric conversion device in which the defective portion situated under the collecting electrode is sufficiently repaired in a desirable state and which is free of occurrence of short circuit. Since a consistent dry process is continued up to the formation of the transparent conductive layer as the upper electrode and because of this, there is not occasion for the semiconductor layer to absorb water wherein the characteristics of the semiconductor layer are stably maintained. Although the electrolytic etching step is additionally performed, that step is simpler in comparison with a conventional repairing method and therefore, the influence of this step to the production cost of a product is slight. EXAMPLE 1 In this example, there was prepared a defect-free amorphous silicon solar cell of the configuration shown in FIG. 2. Firstly, there was provided a stainless steel plate as the conductive substrate 200. This stainless steel plate was well cleaned in a cleaning vessel. On the cleaned stainless steel plate was formed a conductive layer as the lower electrode 201 comprising a 500 Å (10 Å = 1 nm) thick Al film containing 1 % by weight of Si and a 1.5 um thick ZnO film being laminated in this order from the side of the conductive substrate 200 by a sputtering method. On the conductive layer 201 was then formed a 4300 Å thick nip junction amorphous silicon semiconductor layer as the semiconductor layer 202 comprising a 200 Å thick n-type semiconductor film, a 4000 Å thick i-type semiconductor film and a 100 Å thick p-type semiconductor film being laminated in this order from the side of the conductive substrate 200 by a plasma CVD method using SiH 4 gas, PH 3 gas, B 2 H 6 gas and H 2 gas. Then, on the nip junction amorphous silicon semiconductor layer 202 thus formed was formed a 800 Å thick ITO transparent conductive layer as the upper electrode 203 by a heat resistance evaporation method. The solar cell element thus obtained was immersed in the electrolytic etching solution 507' comprising an aqueous solution of AlCl 3 contained in the electrolytic vessel 511 shown in FIG. 6, in which a platinum electrode as the counter electrode was immersed. The conductive substrate 200 comprising the stainless steel plate of the solar cell element was made to be a cathode, whereas the platinum electrode was made to be an anode. Then, the D.C. power source 509 was switched on to apply a direct current voltage of 3 V between the two electrodes, wherein the corresponding portions of the transparent conductive layer as the upper electrode 203 under which defective portions are present were reduced to dissolve into the electrolytic etching solution 507'. A magnetic rubber member was disposed to the the etched solar cell element such that it covered not only the rear surface but also the opposite side faces of the conductive substrate. The resultant was immersed in the electrolytic solution 507 comprising an electrolytic solution obtained by dissolving 0.1 mole/liter of furan into 0.5 mole/liter of a solution of tetrabutylammonium perchlorate contained in the electrolytic vessel 511 shown in FIG. 4, in which a platinum electrode as the counter electrode 508 was immersed. The conductive substrate 200 was made to be an anode, whereas the platinum electrode was made to be a cathode. The D.C. power source 509 was switched on to apply a direct current voltage of 5.0 V with a current density of 5 mA/cm 2 between the two electrode, wherein a polymer film was deposited selectively at each of the defective portions. Then, the conductive substrate 200 was made to be a cathode, whereas the platinum counter electrode 508 was made to be an anode, wherein the D.C. power source was switched on to apply a direct current voltage of 2.0 V between the two electrodes to thereby release anions from the respective polymer films deposited. The solar cell element thus treated was taken out from the apparatus shown in FIG. 4, followed by drying. On the transparent conductive layer as the upper electrode 203 of the solar cell element was formed a negative pattern mask comprising a photosensitive resin film for the formation of a collecting electrode. The resultant was immersed in an sulfuric acid-containing aqueous solution of copper sulfate, wherein the upper electrode 203 was made to be a cathode and a phosphorus-containing copper plate was made to be an anode, and the collecting electrode pattern was subjected to Ni/Cu plating to thereby form the collecting electrode 204. Thus, there was obtained a repaired solar cell. Separately, there was prepared a comparative solar cell by repeating the above procedures, except for not performing the electrolytic polymerization process. Each of the resultant solar cells was evaluated with respect to short circuit current outputted. As a result, it was found that the repaired solar cell is surpassing the comparative solar cell by about 20 %. In addition, as for the solar cell obtained in this example, whether or not it is accompanied by defective portions was observed by a so-called Cu-decoration method. The Cu-decoration method is to observe the presence of a defective portion in a semiconductor device such as photoelectric conversion device, etc. by immersing a semiconductor device to be observed in an aqueous solution of copper sulfate contained in an electrolytic vessel having a counter electrode therein and applying a predetermined voltage between the semiconductor device and the counter electrode in the aqueous solution of copper sulfate, wherein if one or more defective portions are present in the semiconductor device, copper is deposited selectively at each defective portion. The solar cell obtained in this example was subjected to treatment by this Cu-decoration method. The above comparative cell was also subjected to treatment by this Cu-decoration method. And, as for each of the two resultants, the situation of the presence of defective portions deposited with copper was observed using a microscope. As a result, it was found that the number of defective portions of the solar cell obtained in this example is 1/10000 over that of the comparative solar cell. Example 2 In this example, there was prepared a defect-free solar cell of the configuration shown in FIG. 1. Firstly, there was provided a stainless steel plate as the conductive substrate 100. This stainless steel plate was well cleaned in a cleaning vessel. On the cleaned stainless steel plate was formed a conductive layer as the lower electrode 101 comprising a 5000 Å thick Mo-film by a sputtering method. Then, there were successively formed a 2000 Å thick Cu-film and a 4000 Å thick In-film on the Mo-film as the lower electrode 101 by a sputtering method, followed by exposing the resultant to H 2 Se vapor, and subjecting it to heat treatment in an nitrogen gas atmosphere maintained at 400 °C, whereby forming a CuInSe 2 layer on the conductive layer as the lower electrode 101. Successively, there was formed a 6000 Å thick ZnCd film on the CuInSe 2 layer by a sputtering method. Thus, a multilayered semiconductor layer to be the semiconductor layer 102, comprising the CuInSe 2 layer and the ZnCd layer being laminated in this order from the side of the conductive substrate 100, was formed on the conductive layer as the lower electrode 101. An acetylcellulose film was disposed to the resultant solar cell element such that it covered not only the rear surface but also the opposite side faces of the solar cell element. The resultant was immersed in the electrolytic solution 507 comprising an aqueous solution containing a water soluble carboxylic paint dissolved therein contained in the electrolytic vessel 511 shown in FIG. 4, in which a platinum electrode as the counter electrode 508 was immersed. The conductive substrate 100 of the solar cell element was made to be an anode, whereas the platinum electrode was made to be a cathode. Then, the D.C. power source 509 was switched on to apply a direct current voltage of 40 V between the two electrodes, wherein an insulating paint was deposited selectively at each of the defective portions of the solar cell element. On the semiconductor layer 102 of the solar cell element thus repaired was formed a 700 Å thick ZnO film to be the transparent conductive layer 103 by a sputtering method. Finally, on the transparent conductive layer 103 was applied an Ag-paste by means of screen printing technique to thereby form a collecting electrode 104. Thus, there was obtained a repaired copper indium selenide solar cell. Separately, there was prepared a comparative solar cell by repeating the above procedures, except for not performing the electrolytic process of depositing the insulating paint. Each of the resultant solar cells was evaluated with respect to short circuit current outputted. As a result, it was found that the solar cell obtained in this example is surpassing the comparative solar cell by about 18 %. In addition, as for each of the solar cell obtained in this example and the comparative solar cell, whether or not it is accompanied by defective portions was observed in the same manner as in Example 1. As a result, it was found that the number of defective portions of the solar cell obtained in this example is 1/12000 over that of the comparative solar cell. Example 3 In this example, there was prepared a defect-free amorphous silicon solar cell of the configuration shown in FIG. 1. Firstly, there was provided a titanium plate as the conductive substrate 100. This titanium plate was well cleaned in a cleaning vessel. On the cleaned titanium plate was formed a conductive layer as the lower electrode 101 comprising a 5000 Å thick aluminum film by a sputtering method. Then, on the conductive later 101 was formed a nip junction semiconductor layer to be the semiconductor layer 102 by a plasma CVD method. A magnetic rubber member was disposed to the the resultant solar cell element such that it covered not only the rear surface but also the opposite side faces of the conductive substrate 100. The resultant was immersed in the electrolytic solution 507 comprising an aqueous solution of 0.5 mole/liter sulfuric acid, containing 0.3 mole/liter of MnSO 4 contained in the electrolytic vessel 511 shown in FIG. 4, in which a carbon electrode as the counter electrode 508 was immersed. The conductive substrate 100 of the solar cell element was made to be an anode, whereas the carbon electrode was made to be a cathode. Then, the D.C. power source 509 was switched on to apply a direct current voltage of 10 V with a current density of 5 mA/cm 2 between the two electrodes, wherein an insulating material of MnO 2 was deposited selectively at each of the defective portions of the solar cell element. The repaired solar cell element was subjected to heat treatment at 200 °C for an hour. On the semiconductor layer 102 of the solar cell element was then formed a 800 Å thick In 2 O 3 film to be the transparent conductive layer 103 by an electron beam evaporation method. On the transparent conductive layer 103 was formed a negative pattern mask comprising a photosensitive resin for the formation of a collecting electrode, followed by forming a 400 Å thick Cr-film, a 10000 Å thick Ag-film and a 200 Å thick Cr-film to be the collecting electrode 104 by an electron beam evaporation method. Thus, there was obtained a repaired amorphous silicon solar cell. Separately, there was prepared a comparative solar cell by repeating the above procedures, except for not performing the electrolytic process of depositing the MnO 2 insulating material. Each of the resultant solar cells was evaluated with respect to short circuit current outputted. As a result, it was found that the solar cell obtained in this example is surpassing the comparative solar cell by about 18 %. In addition, as for each of the solar cell obtained in this example and the comparative solar cell, whether or not it is accompanied by defective portions was observed in the same manner as in Example 1. As a result, it was found that the number of defective portions of the solar cell obtained in this example is 1/6000 over that of the comparative solar cell. From the results obtained in Examples 1 to 3, it was found that the process according to the present invention makes it possible to efficiently produce a defect-free photoelectric conversion device which exhibits desirable characteristics desired therefor without causing short circuit. Example 4 In this example, there was prepared a defect-free nip junction amorphous silicon germanium solar cell device of the configuration shown in FIG. 2. Firstly, there was provided a stainless steel plate of 100 mm x 100 mm in size and 1.0 mm in thickness as the conductive substrate 200. This stainless steel plate was well cleaned in a cleaning vessel. On the cleaned stainless steel plate as the conductive substrate 200 was formed an about 0.5 µm thick aluminium film to be the conductive layer as the lower electrode 201 by a sputtering method. Successively, an about 0.4 µm thick nip junction amorphous silicon germanium semiconductor layer to be the semiconductor layer 202 was formed on the previously formed conductive layer as the lower electrode 201 by a plasma CVD method. Then, on the nip junction amorphous silicon germanium semiconductor layer thus formed was formed an about 0.07 µm thick ITO transparent and conductive thin film to be the upper electrode 203 by a vacuum evaporation method. In this way, there were prepared a plurality of nip junction amorphous silicon germanium solar cell elements. As for each of the resultant nip junction amorphous silicon germanium solar cell elements, its current/voltage characteristics in a dark state were examined by a conventional method. As a result, more than twenty of the nip junction amorphous silicon germanium solar cell elements thus obtained did not exhibit diode characteristics as expected. From this result, it was found that these nip junction amorphous silicon germanium solar cell elements are such that have one or more defective portions as shown in FIG. 5(a). Thus, twenty of those defective nip junction amorphous silicon germanium solar cell elements were randomly selected. Each of them was subjected to repairing treatment in the same manner as in Example 1. That is, the defective nip junction amorphous silicon germanium solar element was immersed in the electrolytic etching solution 507' comprising an aqueous solution of ALCl 3 contained in the electrolytic vessel shown in FIG. 6, in which a platinum electrode as the counter electrode 508 was immersed. The conductive substrate 200 was made to be a cathode, whereas the platinum electrode was made to be an anode. The D.C. power source was switched on to apply a direct current voltage of 3 V between the two electrodes, wherein the corresponding portions of the transparent and conductive layer 203 under which defective portions were present were reduced to dissolve into the electrolytic etching solution 507' (see, FIG. 5(b)). Thereafter, a magnetic rubber was disposed to the resultant etched solar cell element such that it covered not only the rear face but also the opposite side faces of the conductive substrate 200. The resultant was immersed in the electrolytic solution 507 comprising a solution of tetrabutylammonium perchlorate in acetonitrile contained in the electrolytic vessel 511 shown in FIG. 4, in which a platinum electrode as the counter electrode 508 was immersed. The conductive substrate 200 was made to be an anode, whereas the platinum electrode was made to be a cathode. The D.C. power source was switched on to apply a direct current voltage of 5.0 V with a current density of 5 mA/cm 2 between the two electrodes, wherein a polymer film was deposited selectively at each of the defective portions. Then, the conductive substrate 200 was made to be a cathode, whereas the platinum electrode was made to be an anode, wherein the D.C. power source was switched on to apply a direct current between the two electrodes to thereby release anions from the respective polymer films deposited. The twenty defective nip junction amorphous silicon germanium solar cell elements were thus repaired. As for each of the resultant twenty nip junction amorphous silicon germanium solar cell elements thus repaired, its current/voltage characteristics in a dark state were examined. As a result, it was found that any of the twenty repaired nip junction amorphous silicon germanium solar cell elements exhibits desirable diode characteristics as expected. And each of the twenty repaired nip junction amorphous silicon solar cell elements was found to have been repaired in a desirable state. On the ITO conductive and transparent layer as the upper electrode 203 of each of the twenty repaired nip junction amorphous silicon germanium solar cell elements was formed an about 1.0 µm thick Ag-film to be the collecting electrode 204 by a vacuum evaporation method, to thereby obtain twenty nip junction amorphous silicon solar cell devices. Each of the resultant twenty nip junction amorphous silicon solar cell devices was found to have been repaired in a desirable state as shown in FIG. 5(c). As for each of the resultants, its current/voltage characteristics in a dark state were examined. As a result, it was found that any of the resultant twenty nip junction amorphous silicon germanium solar cell devices are satisfactory in current/voltage characteristics. Further, each of the resultant twenty nip junction amorphous silicon germanium solar cell devices was allowed to stand outdoors for two months. And its current/voltage characteristics in a dark state were examined. As a result, nineteen of the twenty solar cell devices were still satisfactory in current/voltage characteristics. As for each of the twenty nip junction amorphous silicon germanium solar cell devices, it was subjected to measurement of photoelectric conversion efficiency under irradiation of AM 1.5 light. As a result, it was found that the foregoing nineteen nip junction amorphous silicon solar cell devices provide a satisfactory photoelectric conversion efficiency of more than 10 %. Example 5 In this example, there was prepared a defect-free nip junction amorphous silicon germanium solar cell device of the configuration shown in FIG. 1. Firstly, there was provided a stainless steel plate of 100 mm x 100 mm in size and 1.0 mm in thickness as the conductive substrate 100. This stainless steel plate was well cleaned in a cleaning vessel. On the cleaned stainless steel plate as the conductive substrate 100 was formed an about 5000 Å thick Mo-film to be the conductive layer as the lower electrode 101 by a sputtering method. Successively, an about 4000 Å thick nip junction amorphous silicon germanium semiconductor film to be the semiconductor layer 102 was formed on the previously formed conductive layer as the lower electrode 101 by a plasma CVD method. In this way, there were prepared a plurality of partially fabricated nip junction amorphous silicon germanium solar cell elements. As for each of the resultant partially fabricated nip junction amorphous silicon germanium solar cell elements, its surface potential was observed by a conventional noncontact surface-potential measuring method using an electrostatic surface voltmeter. As a result, as for more than twenty of the partially fabricated nip junction amorphous silicon germanium solar cell elements, their surface potential could not be measured. From this result, it was found that these partially fabricated nip junction amorphous silicon germanium solar cell elements are such that have one or more defective portions as shown in FIG. 3(a). Thus, twenty of those defective partially fabricated pin junction amorphous silicon germanium solar cell elements were randomly selected. The twenty defective partially fabricated pin junction amorphous silicon germanium solar cell elements were repaired in the same manner as in Example 2. That is, as for each of them, an acetylcellulose film was disposed such that it covered not only the rear face but also the opposite side faces of the conductive substrate 100. Each of the resultants was immersed in the electrolytic solution 507 comprising an aqueous solution of a water soluble carboxylic paint contained in the electrolytic vessel 511, in which a platinum electrode as the counter electrode 508 was immersed. The Mo-lower electrode 101 was made to be an anode, whereas the platinum electrode was made to be a cathode. The D.C. power source was switched on to apply a direct current voltage of 40 V between the two electrodes, wherein an insulating paint was deposited selectively at each of the defective portions (see, FIG. 3(b)). The twenty partially fabricated defective nip junction amorphous silicon germanium solar cell elements were thus repaired. As for each of the resultant twenty nip junction amorphous silicon germanium solar cell elements thus repaired, a 700 Å thick ZnO transparent and conductive film to be the upper electrode 103 was formed on the nip junction semiconductor layer 102. Thus, there were obtained twenty repaired nip junction amorphous silicon germanium solar cell elements. On the ZnO conductive and transparent layer as the upper electrode 103 of each of the twenty repaired nip junction amorphous silicon germanium solar cell elements was applied an As-paste by means of screen printing technique to thereby form a collecting electrode 104 as shown in FIG. 3(c), to thereby obtain twenty nip junction amorphous silicon germanium solar cell devices. Each of the resultant twenty nip junction amorphous silicon germanium solar cell devices was found to have been repaired in a desirable state as shown in FIG. 3(c). As for each of the resultants, its current/voltage characteristics in a dark state were examined. As a result, it was found that any of the resultant twenty nip junction amorphous silicon germanium solar cell devices are satisfactory in current/voltage characteristics. Further, each of the resultant twenty nip junction amorphous silicon germanium solar cell devices was allowed to stand outdoors for two months. And its current/voltage characteristics in a dark state were examined. As a result, nineteen of the twenty solar cell devices were still satisfactory in current/voltage characteristics. As for each of the twenty nip junction amorphous silicon germanium solar cell devices, it was subjected to measurement of photoelectric conversion efficiency under irradiation of AM 1.5 light. As a result, it was found that the foregoing nineteen nip junction amorphous silicon solar cell devices provide a satisfactory photoelectric conversion efficiency of more than 10 %. Example 6 In this example, there was prepared a defect-free nip junction amorphous silicon germanium solar cell device of the configuration shown in FIG. 2. Firstly, there was provided a stainless steel plate of 100 mm x 100 mm in size and 1.0 mm in thickness as the conductive substrate 200. This stainless steel plate was well cleaned in a cleaning vessel. On the cleaned stainless steel plate as the conductive substrate 200 was formed an about 5000 Å thick Mo-film to be the conductive layer as the lower electrode 201 by a sputtering method. Successively, an about 4000 Å thick nip junction amorphous silicon germanium semiconductor film to be the semiconductor layer 202 was formed on the previously formed conductive layer as the lower electrode 201 by a plasma CVD method. Then, on the nip junction amorphous silicon germanium semiconductor layer thus formed was formed an about 700 Å thick ZnO transparent and conductive thin film to be the upper electrode 203 by a sputtering method. In this way, there were prepared a plurality of nip junction amorphous silicon germanium solar cell elements. As for each of the resultant nip junction amorphous silicon germanium solar cell elements, its current/voltage characteristics in a dark state were examined by a conventional method. As a result, more than twenty of the nip junction amorphous silicon germanium solar cell elements thus obtained did not exhibit diode characteristics as expected. From this result, it was found that these nip junction amorphous silicon germanium solar cell elements are such that have one or more defective portions as shown in FIG. 5(a). Thus, twenty of those defective nip junction amorphous silicon germanium solar cell elements were randomly selected. Each of them was subjected to repairing treatment in the same manner as in Example 1. That is, the defective nip junction amorphous silicon germanium solar element was immersed in the electrolytic etching solution 507' comprising an aqueous solution of ALCl 3 contained in the electrolytic vessel 511 shown in FIG. 6, in which a platinum electrode as the counter electrode 508 was immersed. The conductive substrate 200 was made to be a cathode, whereas the platinum electrode was made to be an anode. The D.C. power source was switched on to apply a direct current voltage of 3 V between the two electrodes, wherein the corresponding portions of the transparent and conductive layer 203 under which defective portions were present were reduced to dissolve into the electrolytic etching solution 507' (see, FIG. 5(b)). Thereafter, a magnetic rubber was disposed to the resultant etched solar cell element such that it covered not only the rear face but also the opposite side faces of the conductive substrate 200. The resultant was immersed in the electrolytic solution 507 comprising an aqueous solution of a water soluble carboxylic paint contained in the electrolytic vessel 511 shown in FIG. 4, in which a platinum electrode as the counter electrode 508 was immersed. The Mo lower electrode 201 was made to be an anode, whereas the platinum electrode was made to be a cathode. The D.C. power source was switched on to apply a direct current voltage of 4.0 V between the two electrodes, wherein an insulating paint was deposited selectively at each of the defective portions. The twenty defective pin junction amorphous silicon germanium solar cell elements were thus repaired. As for each of the resultant twenty pin junction amorphous silicon germanium solar cell elements thus repaired, its current/voltage characteristics in a dark state were examined. As a result, it was found that any of the twenty repaired pin junction amorphous silicon germanium solar cell elements exhibits desirable diode characteristics as expected. And each of the twenty repaired nip junction amorphous silicon germanium solar cell elements was found to have been repaired in a desirable state. On the ZnO conductive and transparent layer as the upper electrode 203 of each of the twenty repaired nip junction amorphous silicon germanium solar cell elements was formed a collecting electrode 204 by applying an Ag-paste by means of screen printing technique. Thus, there were obtained twenty pin junction amorphous silicon germanium solar cell devices. Each of the resultant twenty nip junction amorphous silicon germanium solar cell devices was found to have been repaired in a desirable state as shown in FIG. 5(c). As for each of the resultants, its current/voltage characteristics in a dark state were examined. As a result, it was found that any of the resultant twenty pin junction amorphous silicon germanium solar cell devices are satisfactory in current/voltage characteristics. Further, each of the resultant twenty nip junction amorphous silicon germanium solar cell devices was allowed to stand outdoors for two months. And its current/voltage characteristics in a dark state were examined. As a result, nineteen of the twenty solar cell devices were still satisfactory in current/voltage characteristics. As for each of the twenty nip junction amorphous silicon germanium solar cell devices, it was subjected to measurement of photoelectric conversion efficiency under irradiation of AM 1.5 light. As a result, it was found that the foregoing nineteen nip junction amorphous silicon germanium solar cell devices provide a satisfactory photoelectric conversion efficiency of more than 10 %.

Claims: A process for producing a photoelectric conversion device comprising the sequence of steps of: a) forming a semiconductor layer (502) on a conductive metallic surface (501) of a substrate (500) and using said conductive metallic surface (501) as a back electrode of said photoelectric conversion device; b) forming a transparent and conductive layer (103) on said semiconductor layer (502) ; and c) repairing defective portions (505) of said semiconductor layer (502) by subjecting said transparent and conductive layer (103) to an electrolytic etching treatment in an electrolytic etching solution (507') wherein said conductive metallic surface (501) of said substrate (500) is used as an electrode such that those parts of said transparent and conductive layer (103) are removed under which said defective portions (505) of said semiconductor layer (502) are present so as to obtain a patially etched product, and subjecting said partially etched product to an electrolytic treatment which comprises the steps of immersing said semiconductor layer (502) in an electrolytic liquid (507) and applying a voltage between a counter electrode (508) and said conductive metallic surface (501) which thus acts as an electrode in order to selectively deposit an insulation material (506) obtained from said electrolytic liquid (507) on each of said defective portions (505) ; and d) forming a collecting electrode (104) on said transparent and conductive layer (103) . A process according to claim 1, wherein said electrolytic treatment is an electro-deposition processing. A process according to claim 1, wherein said electrolytic treatment is an electrolytic polymerization processing. A process according to claim 2, wherein the electro-deposition processing uses a liquid containing a paint or a resin. A process according to claim 4, wherein the liquid contains a surfactant.

Inventors: KAWAKAMI SOICHIRO, KAWAKAMI, SOICHIRO, KAWAKAMI, SOICHIRO, C/O CANON KABUSHIKI KAISHA
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1992
Main classification: H01L31
IPC codes: H01L31, H01L27