Method of preparing oxide superconducting film

Abstract: An oxide superconducting layer is formed on a base material of silver, whose single side is coated with MgO, or single-crystalline MgO for depositing a Bi₂Sr₂Ca₂Cu₃ phase in a crystallographically oriented state by sputtering, CVD or laser ablation, then metal lead or lead oxide is laid thereon by sputtering to obtain a two-layer structure, and the two-layer structure is heat treated in the atmospheric air. Thus, a bismuth oxide superconducting film, which is excellent in crystal orientation as well as denseness and thereby being increased in critical current density, is formed on the base material.

Description: BACKGROUND OF THE INVENTION Field of the Invention The present invention relates to a method of preparing an oxide superconducting film, and more particularly, it relates to a method of preparing an oxide superconducting film which is formed on a base material by a vapor phase method. Description of the Background Art In order to enable application of an oxide superconductive material to a conductor, an oxide superconducting film may be formed on a base material. When such base materials are made of single-crystalline materials, for example, it is possible to obtain various elements, provided with oxide superconducting films, which are employed in the field of electronics. When a base material is made of a flexible long material, it is possible to obtain an oxide superconducting wire. Among oxide superconductive materials, a BiSrCaCuO superconductive material is known by its high critical temperature of superconductivity. In order to obtain a BiSrCaCuO superconductor by a solid phase method, lead or a compound of lead is added to a BiSrCaCuO superconductive material, which in turn is heat treated, thereby effectively improving the critical temperature of superconductivity. In order to obtain a BiSrCaCuO superconductor by a vapor phase method, on the other hand, lead is added to a superconductive material for successfully preparing an oxide superconducting film having a high critical temperature, by: (1) a method of adding lead during film formation and heat treating the material; or (2) a method of depositing a Bi2Sr2Ca1Cu2 phase, which has a critical temperature of 80 K, in a crystallographically oriented state, thereafter laying lead on the same and heat treating the material, thereby converting the Bi₂Sr₂Ca₁Cu₂ phase to a Bi₂Sr₂Ca₂Cu₃ phase, which has a critical temperature of 110 K (1989 Heisei Gannen Dai 36 Kai Oyo Butsurigaku Kainkei Rengo Koen-Kai Koen Yoko-Shu, 4p-F-2, "BPSCCO Thin Films with a Zero-Resistance Critical Temperature of 110 K"). In the above method (1), c-axes of the Bi oxide superconductive material are perpendicularly oriented with respect to the base material by heat treatment. However, particles of the deposited film, which are grown along solid phase reaction, react at arbitrary growth rates in various sizes, whereby the film is significantly irregularized and deteriorated in smoothness and denseness. If an oxide superconductive material is thus deteriorated in denseness, it is impossible to improve critical current density. In the method (2), on the other hand, improvement of critical current density is limited since grain growth occurs during conversion from the Bi₂Sr₂Ca₁Cu₂ phase to the Bi₂Sr₂Ca₂Cu₃ phase, and a portion of unwanted film composition is caused by such change of phase, to develop a foreign phase. In the method (2), further, metal lead is laid on the Bi₂Sr₂Ca₁Cu₂ phase. Such metal lead heterogeneously reacts when the same is heated to a temperature exceeding its melting point of 327.4°C, to cause heterogeneous crystal grain growth. Improvement of critical current density is also limited by this. Thus, when a BiSrCaCuO superconducting film is prepared by a vapor phase method, it is difficult to obtain an oxide superconducting film having high critical current density of superconductivity, which is excellent in crystal orientation and denseness. SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a method of preparing an oxide superconducting film, which can obtain an oxide superconducting film having excellent crystal orientation and denseness as well as high critical current density, for preparing a film of an oxide superconductive material such as a BiSrCaCuO superconductive material, for example, by a vapor phase method. The present invention is directed to a method of preparing a Bi Sr Ca CuO superconducting film, which comprises a step of forming an oxide superconducting layer on a base material in a crystallographically oriented state by a vapor phase method wherein said oriented state encompasses that the c axis of said super conducting layer is vertically oriented with respect to said base material. Thereafter a material containing lead is laid on the oxide superconducting layer to obtain a two-layer structure, and the two-layer structure is heat treated. When the present invention is applied to preparation of a BiSrCaCuO oxide superconducting film, the oxide superconducting layer, which is formed on the base material by a vapor phase method, is obtained by depositing a Bi₂Sr₂Ca₂Cu₃ phase in a crystallographically oriented state. According to the present invention, lead metal or a compound of lead such as lead oxide is preferably employed as the material containing a lead element. When the base material employed in the present invention is made of a single-crystalline material, it is possible to advantageously prepare an oxide superconducting film which is applicable to various elements employed in the field of electronics. MgO, SrTiO₃, ZrO, Si or the like may be employed as such a single-crystalline material. When a long flexible base material is used, it is possible to advantageously prepare an oxide superconducting wire, which comprises such a base material and an oxide superconducting film provided thereon. Such a flexible base material can be made of ceramics of partially stabilized zirconia, stabilized zirconia, alumina, yttria, silica or titania, or a metal material of platinum, gold, silver, aluminum, nickel, nickel alloy, copper, copper alloy, aluminum alloy or stainless steel. Further, this long flexible base material is prepared in the form of a tape or fiber. According to the present invention, a crystallographically oriented oxide superconducting layer is formed on a base material, and lead or a compound of lead such as lead oxide is laid thereon to obtain a two-layer structure, which in turn is heat treated. Thus, it is possible to prepare an oxide superconducting film having excellent crystal orientation and high critical current density after heat treatment. The present invention is also characterized in that surface smoothness of the oxide superconducting film is not significantly changed. If a film having a smooth surface, i.e., a dense film, is formed when the oxide superconducting layer is deposited on the base material, it is possible to maintain a relatively smooth state, i.e., a considerably dense state, after heat treatment. Thus, an oxide superconducting film having high critical current density can be readily prepared. Thus, according to the present invention, it is possible to easily prepare an oxide superconducting film which has excellent crystal orientation and denseness as well as high critical current density. Particularly when the present invention is applied to preparation of a BiSrCaCuO oxide superconducting film, it is possible to maximumly effectuate excellent properties of such an oxide superconductive material, which exhibits a critical temperature of 110 K at the maximum, thereby advantageously enabling application of such an oxide superconducting film to a conductor. According to the present invention, further, it is not necessary to particularly increase a film formation temperature in the step of laying lead or a compound of lead such as lead oxide, whereby the oxide superconducting film can be prepared through a simple apparatus in a short time. DESCRIPTION OF THE PREFERRED EMBODIMENTS Example 1 BiSrCaCuO oxide superconducting films were prepared through a sputtering device. First, base materials of silver, coated with MgO, and single-crystalline MgO were employed to form oxide superconducting layers under the following film forming conditions: Target: Bi₃Sr₂Ca₂Cu₃O x Film Forming Temperature: 650°C RF Power: 75 W Gas Pressure: 1.33 Pa (10 mTorr) Gas Composition: Ar/O₂ = 9/1 Film Forming Time: one hour The as-formed BiSrCaCuO oxide superconducting layers were examined in this stage, whereby the following facts were proved regardless of the types of the base materials: The surfaces of the oxide superconducting layers, observed with an electron microscope, were so smooth that it was impossible to discriminate boundaries between deposited particles. As to crystal orientation examined with an X-ray diffractometer, it was confirmed that c-axes of Bi₂Sr₂Ca₂Cu₃ phases were perpendicularly oriented with respect to the base materials. Parts of the oxide superconducting layers were cut out, to confirm composition ratios of metal elements of Bi₂Sr₂Ca₂Cu₃. Then, lead oxide and lead were deposited on the BiSrCaCuO oxide superconducting layers, which were prepared in the aforementioned manner, by sputtering under the following conditions: (1) For Lead Oxide Layers: Target: PbO Film Forming Temperature: no heating RF Power: 100 W Gas Pressure: 1.33 Pa (10 mTorr) Gas Composition: Ar/O₂ = 9/1 Film Forming Time: 5 minutes (2) For Lead Layers: Target: Pb Film Forming Temperature: no heating RF Power: 100 W Gas Pressure: 1.33 Pa (10 mTorr) Gas Composition: Ar/O₂ = 9/1 Film Forming Time: one minute The as-formed two-layer films, which were provided with lead oxide layers under the conditions (1), were analyzed, to prove the following facts regardless of the types of the base materials: The surfaces of the films, observed with an electron microscope, were so smooth that it was impossible to discriminate boundaries between the particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of Bi₂Sr₂Ca₂Cu₃ phases were perpendicularly oriented with respect to the base materials substantially identically to the above results attained before deposition of lead oxide, and no diffraction peaks were newly caused by such deposition of lead oxide. Parts of the films were cut out, to confirm composition ratios of metal elements of Bi₂Pb 0.5 Sr₂Ca₂Cu₃. The other films, which were provided with lead layers under the conditions (2), exhibited surface states, crystal orientation properties and composition ratios substantially identical to those of the above films provided with the lead oxide layers under the conditions (1). The two-layer films thus provided with layers of lead oxide and lead respectively were heat treated under the following conditions: Atmosphere: atmospheric air Holding Temperature: 850°C Holding Time: one hour After the heat treatment, superconductive properties of the films were evaluated by a four-probe method. The results are as follows: A. As to Base Materials of Silver: (1) The film provided with the lead oxide layer exhibited a critical temperature of 108 K, and critical current density of 98 x 10⁴ A/cm² in liquid nitrogen. (2) The film provided with the lead layer exhibited a critical temperature of 108 K, and critical current density of 80 x 10⁴ A/cm² in liquid nitrogen. B. As to Base Materials of Single-Crystalline MgO: (1) The film provided with the lead oxide layer exhibited a critical temperature of 108 K, and critical current density of 156 x 10⁴ A/cm² in liquid nitrogen. (2) The film provided with the lead layer exhibited a critical temperature of 108 K, and critical current density of 130 x 10⁴ A/cm² in liquid nitrogen. Example 2 BiSrCaCuO oxide superconducting films were prepared by a CVD process. First, base materials of silver, whose single side was coated with MgO, and single-crystalline MgO were employed to form BiSrCaCuO oxide superconducting layers under the following film forming conditions: Film Forming Temperature: 700°C Gas: Bi(C₆H₅)₃, Sr(C₁₁H₉O₂)₂, Ca(C₁₁H₁₉O₂)₂, CU(C₁₁H₁₉O₂)₂ Carrier Gas: Ar + O₂ Gas Pressure: 1333 Pa 10 Torr Film Forming Time: one hour The as-formed oxide superconducting layers were examined in this stage, whereby the following facts were proved regardless of the types of the base materials: The surfaces of the oxide superconducting layers, observed with an electron microscope, were so smooth that it was impossible to discriminate boundaries between particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of Bi₂Sr₂Ca₂Cu₃ phases were perpendicularly oriented with respect to the base materials. Parts of the oxide superconducting layers were cut out, to confirm composition ratios of metal elements of Bi₂Sr₂Ca₂Cu₃. Then, lead oxide and lead were deposited on the BiSrCaCuO oxide superconducting layers, which were prepared in the aforementioned manner, by sputtering under the same conditions as Example 1. The as-formed two-layer films, which were provided with lead oxide films, were analyzed, to prove the following facts regardless of the types of the base materials: The surfaces of these films, observed with an electron microscope, were so smooth that it was impossible to discriminate boundaries between the particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of the Bi₂Sr₂Ca₂Cu₃ phases were perpendicularly oriented with respect to the base materials, substantially identically to the results attained before deposition of lead oxide, and no diffraction peaks were newly caused by such deposition of lead oxide. Parts of the films were cut out, to confirm composition ratios of metal elements of Bi₂Pb 0.5 Sr₂Ca₂Cu₃. The surface states, crystal orientation properties and composition ratios of the other two-layer films, which were provided with lead layers, were substantially identical to those of the above films provided with the lead oxide layers. The two-layer films, which were provided with the layers of lead oxide and lead, were heat treated under conditions similar to those of Example 1. After the heat treatment, superconductive properties of the films were evaluated by a four-probe method. The results are as follows: A. As to Base Materials of Silver: (1) The film provided with the lead oxide layer exhibited a critical temperature of 107 K, and critical current density of 77 x 10⁴ A/cm² in liquid nitrogen. (2) The film provided with the lead layer exhibited a critical temperature of 107 K, and critical current density of 64 x 10⁴ A/cm² in liquid nitrogen. B: As to Base Materials of Single-Crystalline MgO: (1) The film provided with the lead oxide layer exhibited a critical temperature of 107 K, and critical current density of 145 x 10⁴ A/cm² in liquid nitrogen. (2) The film provided with the lead layer exhibited a critical temperature of 107 K, and critical current density of 118 x 10⁴ A/cm² in liquid nitrogen. Example 3 BiSrCaCuO oxide superconducting films were prepared by laser ablation. First, base materials of silver, whose single side was coated with MgO, and single-crystalline MgO were employed to form BiSrCaCuO oxide superconducting layers under the following film forming conditions: Laser Beam: ArF (193 nm) Energy Density of Laser Beam: 1 J/cm² Frequency of Laser Beam: 10 Hz Film Forming Temperature: 630°C Target: Bi₂Sr₂Ca₂Cu₃O x Gas: oxygen Gas pressure: 13.33 Pa (100 mTorr) The as-formed BiSrCaCuO oxide superconducting layers were examined, whereby the following facts were proved regardless of the types of the base materials: The surfaces of the oxide superconducting layers, observed with an electron microscope, were so smooth that it was impossible to discriminate boundaries between particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of Bi₂Sr₂Ca₂Cu₃ phases were perpendicularly oriented with respect to the base materials. Parts of the oxide superconducting layers were cut out, to confirm composition ratios of metal elements of Bi₂Sr₂Ca₂Cu₃. Then, lead oxide and lead were deposited on the BiSrCaCuO superconducting layers, which were prepared in the aforementioned manner, by sputtering under the same conditions as Example 1. The two-layer films which were provided with lead oxide layers were analyzed, to prove the following facts regardless of the types of the base materials: The surfaces of the films, observed with an electron microscope, were so smooth that it was impossible to discriminate boundaries between the particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of the Bi₂Sr₂Ca₂Cu₃ phases were perpendicularly oriented with respect to the base materials substantially identically to the result attained before deposition of lead oxide, and no diffraction peaks were newly caused by such deposition of lead oxide. Parts of the films were cut out, to confirm composition ratios of metal elements of Bi₂Pb 0.5 Sr₂Ca₂Cu₃. The surface states, crystal orientation properties and composition ratios of the other two-layer films, which were provided with lead layers, were substantially identical to those of the above films provided with the lead oxide layers. The two-layer films, which were provided with the lead oxide and lead layers, were heat treated under conditions similar to those of Example 1. After the heat treatment, superconductive properties of the films were evaluated by a four-probe method. The results are as follows: A. As to Base Materials of Silver: (1) The film provided with the lead oxide layer exhibited a critical temperature of 106 K, and critical current density of 94 x 10⁴ A/cm² in liquid nitrogen. (2) The film provided with the lead layer exhibited a critical temperature of 106 K, and critical current density of 78 x 10⁴ A/cm² in liquid nitrogen. B: As to Base Materials of Single-Crystalline MgO: (I) The film provided with the lead oxide layer exhibited a critical temperature of 106 K, and critical current density of 176 x 10⁴ A/cm² in liquid nitrogen. (2) The film provided with the lead layer exhibited a critical temperature of 106 K, and critical current density of 148 x 10⁴ A/cm² in liquid nitrogen. Reference Example 1 BiSrCaCuO oxide superconducting layers were deposited on base materials under the same conditions as Example 1. The surface states, crystal orientation properties and composition ratios of these oxide superconducting layers were substantially identical to those of Example 1. These oxide superconducting layers were heat treated under the same conditions as Example 1, with no deposition of lead oxide or lead. After the heat treatment, superconductive properties of the films were evaluated by a four-probe method. As to critical current density in liquid nitrogen, the film comprising a base material of silver exhibited 800 A/cm² and that comprising a base material of single-crystalline MgO exhibited 5000 A/cm², while both films exhibited critical temperatures of 87 K. When similar films were evaluated with no heat treatment, the critical temperatures remained at 75 K regardless of the types of the base materials. Reference Example 2 BiSrCaCuO oxide superconducting layers were deposited on base materials under the same conditions as Example 2. The surface states, crystal orientation properties and composition ratios of these oxide superconducting layers were substantially identical to those of Example 2. These oxide superconducting layers were heat treated under the same conditions as Example 1, with no deposition of lead oxide or lead. After the heat treatment, superconductive properties of the films were evaluated by a four-probe method. As to critical current density in liquid nitrogen, the film comprising a base material of silver exhibited 700 A/cm² and that comprising a base material of single-crystalline MgO exhibited 4000 A/cm², while both films exhibited critical temperatures of 88 K. When similar films were evaluated with no heat treatment, the critical temperatures remained at 74 K regardless of the types of the base materials. Reference Example 3 BiSrCaCuO oxide superconducting layers were deposited on base materials under the same conditions as Example 3. The surface states, crystal orientation properties and composition ratios of these oxide superconducting layers were substantially identical to those of Example 3. These oxide superconducting layers were heat treated under the same conditions as Example 1, with no deposition of lead oxide or lead. After the heat treatment, superconductive properties of the films were evaluated by a four-probe method. As to critical current density in liquid nitrogen, the film comprising a base material of silver exhibited 800 A/cm² and that comprising a base material of single-crystalline MgO exhibited 6000 A/cm², while both films exhibited critical temperatures of 89 K. When similar films were evaluated with no heat treatment, the critical temperatures remained at 76 K regardless of the types of the base materials. Example 4 A BiSrCaCuO oxide superconducting film was prepared through a sputtering device. First, a base material of silver coated with MgO was employed to form an oxide superconducting layer under the following film forming conditions: Target: Bi₃Sr₂Ca₁Cu₂O x Film Forming Temperature: 620°C RF Power: 75 W Gas Pressure: 1.33 Pa (10 mTorr) Gas Composition: Ar/O₂ = 9/1 Film Forming Time: one hour The as-formed BiSrCaCuO oxide superconducting layer was examined in this stage, to prove the following facts: The surface of the oxide superconducting layer, observed with an electron microscope, was so smooth that it was impossible to discriminate boundaries between deposited particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of a Bi₂Sr₂Ca₁Cu₂ phase were perpendicularly oriented with respect to the base material. A part of the oxide superconducting layer was cut out, to confirm composition ratios of metal elements of Bi₂Sr₂Ca₁Cu₂. Then, lead oxide was deposited on the BiSrCaCuO oxide superconducting layer, which was prepared in the aforementioned manner, by sputtering under the following conditions: Target: PbO Film Forming Temperature: no heating RF Power: 100 W Gas Pressure: 1.33 Pa (10 mTorr) Gas Composition: Ar/O₂ = 9/1 Film Forming Time: 5 minutes The two-layer film provided with a lead oxide layer was analyzed, to prove the following facts: The surface of the film, observed with an electron microscope, was so smooth that it was impossible to discriminate boundaries between the particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of the Bi₂Sr₂Ca₁Cu₂ phase were perpendicularly oriented with respect to the base material substantially identically to the result attained before deposition of lead oxide, and no diffraction peak was newly caused by such deposition of lead oxide. A part of the film was cut out, to confirm composition ratios of metal elements of Bi₂Pb 0.5 Sr₂Ca₁Cu₂. The two-layer film thus provided with the lead oxide layer was heat treated under the following conditions: Atmosphere: atmospheric air Holding Temperature: 850°C Holding Time: one hour After the heat treatment, superconductive properties of the film were evaluated by a four-probe method. The film exhibited a critical temperature of 108 K, and critical current density of 35 x 10⁴ A/cm² in liquid nitrogen. Example 5 A BiSrCaCuO oxide superconducting film was prepared by a CVD process. First, a base material of silver whose single side was coated with MgO was employed to form a BiSrCaCuO oxide superconducting layer under the following film forming conditions: Film Forming Temperature: 650°C Gas: Bi(C₆H₅)₃, Sr(C₁₁H₁₉O₂)₂, Ca(C₁₁H₁₉O₂)₂, CU(C₁₁H₁₉O₂)₂ Carrier Gas: Ar + O₂ Gas Pressure: 1333 Pa (10 Torr) Film Forming Time: one hour The as-formed oxide superconducting layer was examined in this stage, to prove the following facts: The surface of the oxide superconducting layer, observed with an electron microscope, was so smooth that it was impossible to discriminate boundaries between particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of a Bi₂Sr₂Ca₁Cu₂ phase were perpendicularly oriented with respect to the base material. A part of the oxide superconducting layer was cut out, to confirm composition ratios of metal elements of Bi₂Sr₂Ca₁Cu₂. Then, lead oxide was deposited on the BiSrCaCuO oxide superconducting layer prepared in the aforementioned manner, under the same conditions as Example 4. The two-layer film which was provided with a lead oxide layer was analyzed, to prove the following facts: The surface of this film, observed with an electron microscope, was so smooth that it was impossible to discriminate boundaries between the particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of the Bi₂Sr₂Ca₁Cu₂ phase were perpendicularly oriented with respect to the base material substantially identically to the result attained before deposition of lead oxide, and no diffraction peak was newly caused by such deposition of lead oxide. A part of this film was cut out, to confirm composition ratios of metal elements of Bi₂Pb 0.5 Sr₂Ca₁Cu₂. Then, the two-layer film provided with the lead oxide layer was heat treated under conditions similar to those of Example 4. After the heat treatment, superconductive properties of this film was evaluated by a four-probe method. As the result, the film exhibited a critical temperature of 107 K, and critical current density of 30 x 10⁴ A/cm² in liquid nitrogen. Example 6 A BiSrCaCuO oxide superconducting film was prepared by laser ablation. A base material of silver whose single side was coated with MgO was employed to form a BiSrCaCuO oxide superconducting layer under the following film forming conditions: Laser Beam: ArF (193 nm) Energy Density of Laser Beam: 1 J/cm² Frequency of Laser Beam: 10 Hz Film Forming Temperature: 600°C Target: Bi₂Sr₂Ca₁Cu₂O x Gas: oxygen Gas Pressure: 13.33 Pa (100 mTorr) The as-formed BiSrCaCuO oxide superconducting layer was examined, to prove the following facts: The surface of the oxide superconducting layer, observed with an electron microscope, was so smooth that it was impossible to discriminate boundaries between particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of a Bi₂Sr₂Ca₁Cu₂ phase were perpendicularly oriented with respect to the base material. A part of this oxide superconducting layer was cut out, to confirm composition ratios of metal elements of Bi₂Sr₂Ca₁Cu₂. Then, lead oxide was deposited on the BiSrCaCuO superconducting layer which was prepared in the aforementioned manner, by sputtering under the same conditions as Example 4. The two-layer film which was provided with a lead oxide layer was analyzed, to prove the following facts: The surface of this film, observed with an electron microscope, was so smooth that it was impossible to discriminate boundaries between the particles. As to crystal orientation examined with an X-ray diffractometer, c-axes of the Bi₂Sr₂Ca₁Cu₂ phase were perpendicularly oriented with respect to the base material substantially identically to the result attained before deposition of lead oxide, and no diffraction peak was newly caused by such deposition of lead oxide. A part of this film was cut out, to confirm composition ratios of metal elements of Bi₂Pb 0.5 Sr₂Ca₁Cu₂. Then, the two-layer film provided with the lead oxide layer was heat treated under conditions similar to those in Example 4. After the heat treatment, superconductive properties of the film were evaluated by a four-probe method. As the result, the film exhibited a critical temperature of 106 K, and critical current density of 40 x 10⁴ A/cm². Reference Example 4 A BiSrCaCUO oxide superconducting layer was deposited on a base material under the same conditions as Example 4. The surface state, crystal orientation and composition of this oxide superconducting layer were substantially identical to those of Example 4. This oxide superconducting layer was heat treated under the same conditions as Example 4, with no deposition of lead oxide. After the heat treatment, superconductive properties of the film were evaluated by a four-probe method. As the result, the film exhibited a critical temperature of 93 K, and critical current density of 800 A/cm². When a similar film was evaluated with no heat treatment, the critical temperature remained at 75 K. Reference Example 5 A BiSrCaCuO oxide superconducting layer was deposited under the same conditions as Example 5. The surface state, crystal orientation and composition of this oxide superconducting layer were substantially identical to those of Example 5. The oxide superconducting layer was heat treated under the same conditions as Example 4, with no deposition of lead oxide. After the heat treatment, superconductive properties of this film was evaluated. As the result, the film exhibited a critical temperature of 89 K, and critical current density of 700 A/cm² in liquid nitrogen. When a similar film was evaluated with no heat treatment, the critical temperature remained at 74 K. Reference Example 6 A BiSrCaCuO oxide superconducting layer was deposited under the same conditions as Example 6. The surface state, crystal orientation and composition of this oxide superconducting layer were substantially identical to those of Example 6. Then, the oxide superconducting layer was heat treated under the same conditions as Example 4, with no deposition of lead oxide. After the heat treatment, superconductive properties of this film were evaluated by a four-probe method. As the result, the film exhibited a critical temperature of 87 K, and critical current density of 800 A/cm² in liquid nitrogen. When a similar oxide superconducting film was evaluated with no heat treatment, the critical temperature remained at 76 K.

Claims: A method of preparing a BiSrCaCuO superconducting film, comprising in the following sequence the steps of: forming an oxide superconducting layer on a base material in a crystallographically oriented state by a vapor phase method wherein said oriented state encompasses that the c axis of said superconducting layer is vertically oriented with respect to said base material; depositing a layer containing lead on said oxide superconducting layer to obtain a two-layer structure; and heat treating said two-layer structure. A method of preparing an oxide superconducting film in accordance with claim 1, being applied to preparation of a BiSrCaCuO oxide superconducting film, wherein said oxide superconducting layer is obtained by depositing a Bi₂Sr₂Ca₂Cu₃ phase in a crystallographically oriented state. A method of preparing an oxide superconducting film in accordance with claim 1, wherein said material containing lead is metallic lead. A method of preparing an oxide superconducting film in accordance with claim 1, wherein said material containing lead is a compound of lead. A method of preparing an oxide superconducting film in accordance with claim 4, wherein said compound of lead is lead oxide. A method of preparing an oxide superconducting film in accordance with claim 1, wherein said vapor phase method is any one selected from a group of sputtering, CVD and laser ablation. A method of preparing an oxide superconducting film in accordance with claim 1, wherein said step of laying a material containing a lead element on said oxide superconducting layer is carried out by sputtering. A method of preparing an oxide superconducting film in accordance with claim 1, wherein said base material is formed of a long flexible material.

Inventors: HAYASHI NORIKI OSAKA WORKS OF, TAKANO SATOSHI OSAKA WORKS OF, HAYASHI, NORIKI, OSAKA WORKS OF SUMITOMO, TAKANO, SATOSHI, OSAKA WORKS OF SUMITOMO
Applicants: KANSAI ELECTRIC POWER CO, SUMITOMO ELECTRIC INDUSTRIES, SUMITOMO ELECTRIC INDUSTRIES, LTD., THE KANSAI ELECTRIC POWER CO., INC.
Application year: 1991
Main classification: H01L39
IPC codes: H01L39