Superconducting material and process for producing the same

Abstract: Oxide materials of (L x A 1-x ) i MO y , (L x A 1-x ) i ­ M 1-z Cu z O y and (L x A 1-x ) i MO j-δ G k , wherein L is Sc, Y, lanthanides, etc.; A is Ba, Sr, Ca, etc.; M is V, Nb, Ta, Ti, Zr or Hf; 0 < x < 1; 0 < z < 1; i=1, 3/2 or 2; 0 < y ≦ 4; G is F, Cl or N; δ is oxygen defect, and having a perovskite-like crystal structure, show superconductivity at a temperature higher than the liquid nitrogen temperature.

Description: This invention relates to a superconducting material having a perovskite-like crystal structure and a superconducting part using the same, particularly to a superconducting material suitable for having a high superconducting transition temperature (Tc), and a process for producing the same. Heretofore, oxide series superconducting materials and their production have been discussed, for example, in Zeitschift für Physik B64 (1986), pp. 189-193; Science 235 (1987), pp. 567-569; Physical Review Letters 58 (1987), pp. 908-910, etc. According to the prior art technique, there have not been considered oxide superconducting materials having a Tc or 100 K or higher and production thereof. Thus, when these materials having low Tc were used in the superconducting state, there was a problem in that cooling at the level of liquid nitrogen temperature (78 K) was necessary. EPA-A-0280812 was published after the filing date of the present application and is thus prior art only under Article 54(3) EPC. It discloses superconductive square-planar oxide compound systems of Tc up to 100°K based on [L 1-x M x ] a A b O y where L is a rare earth element e.g. La or Y; M is a group II metal e.g. Ba or Sr; and A is one or more metals selected from a list including Cu and Nb. Objects of this invention are to provide a superconducting material having a high superconducting transition temperature (Tc), preferably Tc of 150 K or higher, a superconducting part using the same, and processes for producing the same. This invention provides a superconducting material represented by the formula [A]: (L x A 1-x ) i Nb 1-z Cu z O y [A] wherein (i) L=La, A=Sr or (ii) L=Y, A=Ba and wherein 0 < x < 1; 0 ≦ z < 1 and either i is 1 and 0 < y ≦ 3 or i is 3/2 or 2 and 0 < y ≦ 4. In a preferred type of embodiment, z = 0 so that the formula is (L x A 1-x ) i Nb O y Other preferred types of embodiment are (La x Sr 1-x ) i Nb 1-z Cu z O y and (Y x Ba 1-x ) i Nb 1-z Cu z O y This invention further provides a process for producing a superconducting material of the formula [A]: (L x A 1-x ) i Nb 1-z Cu z O y [A] as defined above but wherein 0 < z < 1, in the form of a film, which comprises depositing on a metal film of one element selected from L, A, Nb and Nb containing Cu, a mixture of the rest of the elements other than that of the metal film, and heat treating the metal film and the resulting deposited layer to carry out a diffusion reaction therebetween. The invention further provides a process for producing a superconducting material of the formula [A] as defined above where 0 < z < 1 in the form of a film which comprises: using as a target an oxide represented by the formula (L x A 1-x ) i Cu O y using as a substrate a film of Nb; passing an alternating electric current through the substrate so as to maintain the temperature of the substrate at 1000° to 1400°C; conducting sputtering by using a direct current magnetron sputtering apparatus in an argon atmosphere with a pressure of 0.1 to 0.8 Torr (1 Torr = 133.3 Pa) at a sputtering voltage of 200 to 400V and a sputtering electric current of 20 mA to 100 mA; and conducting a diffusion reaction between the substrate and the sputtered layer. The invention further provides a process for producing a superconducting material of the formula [A] as defined above where 0 < z < 1 in the form of a powder, which comprises depositing a film of pure metal of the element Nb on the outer surface of an oxide represented by the formula: (L x A 1-x ) i Cu O y (4) in vacuum; substituting the Cu of the oxide of the formula (4) with the Nb at 600° to 900°C by the diffusion of the element Nb; subjecting the resulting product to annealing in an oxidizing atmosphere, and pulverizing the resulting annealed product. The invention further provides a process for producing a superconducting material of the formula [A] wherein z = 0 so that the formula is (L x A 1-x ) i Nb O y in the form of a film, which comprises using as a substrate at least one material selected from silicon, aluminum oxide, silicon oxide, magnesium oxide and zirconium oxide, forming a metal thin film of the element Nb on the substrate, depositing a film of L x A 1-x on the metal thin film, and subjecting the resulting film to heat treatment to carry out a diffusion reaction of these elements; or a process which comprises depositing a film of L x A 1-x on a metal tape or a substrate of the element Nb and subjecting the resulting film to heat treatment to carry out a diffusion reaction of these elements. The invention further provides a process for producing a superconducting material of the formula (La x Sr 1-x ) i Nb 1-z Cu z O y or (Y x Ba 1-x ) i Nb 1-z Cu z O y in the form of a film, which comprises using a substrate made of at least one member selected from silicon, aluminum oxide, silicon oxide, magnesium oxide, and zirconium oxide, forming a metal thin film of the element Nb on the substrate, depositing an amorphous or polycrystalline film of (L x A 1-x ) i CuO y on the metal thin film, and subjecting the resulting film to heat treatment to diffuse the element Nb into the (L x A 1-x ) i CuO y film. The invention further provides a process for producing a film of La-Sr-Nb-0 oxide superconducting material which comprises using as a target a La-Sr-Cu-O₄ sintered body, and as a substrate a niobium material, passing an alternating electric current through the substrate so as to maintain the temperature of the substrate at 1000° to 1400°C, conducting sputtering in an argon atmosphere with a pressure of 0.1 to 0.8 Torr at a sputtering voltage of 200 to 400V and a sputtering electric current of 20 mA to 100 mA to form a film of La-Sr-Cu-O₄ on the niobium substrate surface, conducting a diffusion reaction between the substrate and the sputtered layer, and subjecting the resulting niobium substrate to heat treatment at 500° - 600°C for 10-30 minutes in a weakly oxidizing atmosphere. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a perspective view of a crystal structures of the materials of this invention. Fig. 2 is a graph showing EPMA (Electron Probe Micro Analyzer) analysis data of one example of the material of this invention. Figs. 3 to 5 are graphs showing a relationship between electric resistance and temperature. Figs. 6 and 7(a) to 7(c) show steps of processes of this invention. Figs. 8 and 9 are cross-sectional views of parts according to this invention. Figs. 10, 11 and 12 show individual steps according to the processes of this invention. Fig. 13 is a cross-sectional view of a direct current magnetron sputtering apparatus. Fig. 14 is a graph showing temperature change of the electric resistance of oxide superconducting material obtained in an example of Fig. 13. Fig. 15 is a graph showing the magnetization of the same material as used in Fig. 14. Fig. 16 shows the progress of substitution reaction according to one example of this invention. Fig. 17 is a schematic cross-sectional view of a laser using apparatus used in one example of this invention. Fig. 18 is a graph showing IMA (Ion Micro Analyzer) analysis of the thin film obtained by the apparatus of Fig. 17. DESCRIPTION OF THE PREFERRED EMBODIMENTS The superconducting materials of this invention have a perovskite-like crystal structure and are represented 1 by the formulae: (L x A 1-x ) i MO y (1) or (L x A 1-x ) i M 1-z Cu z O y (2) where M represents Nb. A superconducting part embodying this invention can be obtained by covering exposed portions of sintered body of a molded body of the above-mentioned superconducting materials with an oxygen preventing film (passivation film), or by laminating this superconducting material with other films of electrical insulating material. It is preferable to laminate a plurality of film-like layers alternatively, respectively. Further, it is preferable to use as an insulating material a perovskite-like ceramic of the same series. More in detail, the material represented by the formula (1) has a perovskite-like crystal structure in which M is positioned at the center of an octahedron formed by oxygen (0) and oxygen vacancies. Since this material has defect of oxygen, that is, one or more oxygen vacancies in the octahedron, it is expected to generate a mutual action of strong attraction necessary for forming a hole pair or electron pair showing a superconducting phenomenon at a temperature of 150 K or higher. The oxide superconducting material of this invention has the perovskite-like crystal structure as shown in Fig. 1. This drawing shows a unit lattice of the material represented by the formula: (L x A 1-x ) i Nb O y (1) As shown in Fig. 1, 6 oxygen atoms are arranged around the Nb in the formula (1) to form an octahedron. When one oxygen atom among the six oxygen atoms is deficient, there is formed a pyramid structure having Nb at the base, or when two oxygen atoms are deficient, there is formed a square of four oxygen atoms having Nb in its face center or a square of two oxygen atoms and two oxygen vacant holes having Nb in its face center, singly or in combination appearing regularly to form a plurality of layers, said pyramid or square being connected two-dimensionally in the crystal. With the generation of two-dimensionally connected pyramids or squares, mutual action of strong attraction necessary for forming hole pairs or electron pairs showing a superconducting phenomenon is generated. The thus generated hole pairs or electron pairs showing the superconducting phenomenon seem to pass along the pyramids or squares connected two-dimensionally. By containing Nb, the formation of defect of oxygen, that is, the formation of oxygen vacent holes, is accelerated to form continuous faces obtained by combining the pyramids or squares of Nb and oxygen as fundamental components. As mentioned above, since the octahedron formed by Nb and oxygen atoms or oxygen vacant holes (practically crystal structure of pyramid, square, etc.) seems to be essential for the superconductivity, the stable formation of such a structure seems to be sufficient. Suitable examples of the above-mentioned oxide superconducting materials are as follows: La x Sr 1-x Nb 1-z Cu z O 3-δ (La x Sr 1-x)2 Nb 1-z Cu z O 4-δ Y x Ba 1-x Nb 1-z Cu z O 3-δ In the above mentioned formulae, it is preferable to make x in the range of 0.4 ≦ x < 0.6, and more preferably x being about 0.5. In the next place, production of the superconducting materials represented by the formulae (1) and (2) is explained. The material represented by the formula (1) can be produced, for example, by mixing a powder of oxide of L element, a powder of carbonate of A element, and a powder of oxide of M element or pure metal of M element in the desired stoichiometric composition, reacting the mixed powders in vacuum, reducing, or oxidizing, preferably weakly oxidizing atmosphere at high temperatures with heating, and sintering the reaction mixture. Further, the superconducting material represented by the formula (1) can be obtained by substituting a part or whole of Cu in the oxide of the formula: (L x A 1-x ) i CuO y (4) wherein L, A, x, y and i are as defined above, with Nb. By the step of producing the oxide of the formula (4) and the step of substituting a part or whole of Cu in the formula (4) with at least one element selected from those of the group IVb and Vb, the total amount of the elements of the group IVb and Vb can exceed the amount of Cu. It is also possible to produce an oxide superconducting powder having a perovskite-like crystal structure containing M element mainly by mixing a powder of oxide material represented by (L x A 1-x ) i CuO y , wherein x is 0 < x < 1; i is 1, 3/2 or 2; and y is 0 < y ≦ 4, with pure Nb in a weight ratio of Cu:Nb = 1:1, carrying out substitution reaction between Cu and Nb in vacuum, and finally pulverizing the final reaction product. It is further possible to produce an oxide superconducting powder having a perovskite-like crystal structure and containing Nb mainly by depositing in vacuum a film of pure metal of Nb selected on an outer surface of an oxide ceramic containing Cu mainly represented by (L x A 1-x ) i CuO y , wherein x is 0 < x < 1; i is 1, 3/2 or 2; and y is 0 < y ≦ 4, diffusing the Nb at 600° to 900°C for several hours to substitute Cu with Nb; annealing the resulting product in an oxidizing atmosphere, and pulverizing the thus obtained ceramic. It is possible to subject an oxide material represented by the formula: (L x A 1-x ) i MO y (1), wherein x is 0 < x < 1; i is 1, 3/2 or 2; y is 0 < y ≦ 4, containing the M element mainly (M being Nb optionally to containing Cu) and having a perovskite-like crystal structure to annealing in an oxidizing atmosphere so as to have superconductivity. In the annealing step, it is effective to conduct the final heating step at 600 to 900°C for 12 to 48 hours. It is also possible to form an oxide film having the composition of the formula (1) by diffusion reaction on a substrate made of Nb by direct current magnetron sputtering using a sintered body of the formula (4) as a target in an argon atmosphere under conditions of the atmosphere pressure of 0.1 to 0.8 Torr, sputtering voltage of 200 to 400 V, sputtering electric current of 20 mA to 100 mA, while passing an alternating electric current directly through the substrate to maintain the substrate temperature at 1000° to 1400°C and forming the oxide of the formula (4) on the substrate surface. It is effective to subject the above-mentioned substrate obtained by the oxide film of the formula (1) formation step to the annealing step by heating at 500° to 600°C for 10 to 30 minutes in a weakly oxidizing atmosphere. An embodiment of the above-mentioned production comprises a step of using a niobium material as a substrate, passing an alternating electric current directly through the substrate to maintain at a temperature of 1000 to 1400°C, and forming on the niobium substrate surface an oxide of La-Sr-Cu-O₄ by direct current magnetron sputtering using La-Sr-Cu-O₄ sintered body as a target in an argon atmosphere under a pressure of 0.1 to 0.8 Torr at a sputtering voltage of 200 to 400 V and sputtering electric current of 20 mA to 100 mA, through which step a La-Sr-Nb-O oxide film is formed on the niobium substrate surface by diffusion reaction, followed by heat treatment of the thus obtained niobium substrate in a weakly oxidizing atmosphere at 500°C to 600°C for 10 to 30 minutes. Still another embodiment of the production comprises vapor depositing a L-A-Cu-O film on a substrate made of Nb or alloy thereof and heated at high temperatures, and conducting substitution of Cu with Nb by the reaction between the substrate and the vapor deposited film. In the above-mentioned process, it is effective to conduct the vapor deposition by laser beam irradiation. The stabilization of the superconducting thin film thus obtained can desirably be conducted by rapidly cooling the thin film immediately after the vapor deposition. The oxide superconducting material represented by the formula (2) having a perovskite-like crystal structure can be produced by mixing a powder of oxide of L element, a powder of carbonate of A element, and cupric oxide (CuO) powder, heating the mixed powders at 900 to 1000°C in vacuum, reducing or oxidizing, preferably weakly oxidizing atmosphere, mixing the resulting reacted mixed powders with a powder of pure Nb metal in the desired stoichiometric amounts, heating again the resulting mixture in vacuum, reducing, or oxidizing, preferably weakly oxidizing atmosphere for reaction, and sintering the reaction mixture. Further, it is possible to form an oxide superconducting thin film represented by the formula (1) and having a perovskite-like crystal structure on a substrate of at least one of silicon (Si) single crystal, aluminum oxide (Al₂O₃) single crystal, silicon oxide (SiO₂) single crystal, magnesium oxide (MgO) single crystal and zirconium oxide (ZrO₂) single crystal by forming a metal thin film of Nb on the substrate, depositing a film of a mixture of the L element and A element (L x A 1-x film, and 0 < x < 1), and subjecting to heat treatment to react these elements. In addition, it is possible to obtain an oxide superconducting material represented by the formula (1) and having a perovskite-like crystal structure by depositing a film of a mixture of the L element and the A element (L x A 1-x film, and 0 < x < 1) on a metal tape or substrate of Nb, and heat treating to conduct the reaction of these elements. It is also effective to form an oxide superconducting film represented by the formula (2) and having a perovskite-like crystal structure by using as a substrate at least one of silicon (Si) single crystal, aluminum oxide (Al₂O₃) single crystal, silicon oxide (SiO₂) single crystal, magnesium oxide (MgO) single crystal, and zirconium oxide (ZrO₂) single crystal, forming a metal thin film of Nb on the substrate, depositing an amorphous or polycrystalline film containing the L element, A element, Cu and O [(L x A 1-x ) i CuO y ] on the metal thin film, and subjecting to heat treatment to diffuse the Nb into the film of (L x A 1-x ) i CuO y ). Polycrystalline or crystalline oxide superconducting materials represented by the formula (1) or (2) can be produced by heating a mixture containing the L element, A element and Nb in predetermined stoichiometric amounts at high temperatures in vacuum, reducing or oxidizing, preferably weakly oxidizing atmosphere to carry out the reaction, obtaining a powder of amorphous or polycrystalline oxide of the above-mentioned mixture, molding the powder and sintering the molded product. It is also possible to produce polycrystalline or crystalline oxide superconducting materials represented by the formula (1) or (2) by forming a film containing the L element, A element and Nb in predetermined stoichiometric compositional proportions on a tape or substrate, and heating the film in vacuum, reducing or oxidizing, preferably weakly oxidizing atmosphere to carry out the reaction. The elements belonging to the group Vb and IVb can take a plurality of valence numbers. Those having the higher valence number (e.g. Nb in Nb₂O₅ and the like having a higher oxygen element ratio) are generally stable. Element single bodies or low-oxygen-content compounds can generally be changed into those having the highest oxygen element ratio by heating in an oxidizing atmosphere. Therefore, a particularly preferable raw ceramics is NbO. By retaining those having a variety of valences in the perovskite-like molded product, the change of valence (e.g. valence 2 ( ↔ ) valence 5) takes place in the molded product to probably enhance the stability. It is preferable to make the valence of oxygen (y) equal to the total valences of L, A and Nb elements (p) in the range of ±0.5 (i.e., |p| = |y| ±0.5 ). The meaning of the value ± 0.5 is that slight excess and deficiency of oxygen defect is immaterial, and sufficient when becoming practically equal. The above-mentioned production processes are explained more in detail. For example, an oxide superconducting material represented by the formula (1) and having a perovskite-like crystal structure can be produced by reacting a powdery mixture of an oxide of L element, a carbonate of A element and CuO in the predetermined stoichiometric amounts, these elements being known to easily be reacted, at about 900°C in air or oxidizing atmosphere for several hours, press molding the resulting product, sintering at 950°C to 1100°C to give a powder or sintered body (ceramic) having a perovskite-like crystal structure containing Cu mainly, said Cu is easy in the production, and carrying out a substitution reaction of the Cu in the powder or sintered body with Nb in vacuum or oxidizing atmosphere with heating. Further, by annealing the resulting product in an oxidizing atmosphere, superconductivity can be obtained. A copper oxide of the formula (4) {(L x A 1-x ) i CuO y } having a perovskite-like crystal structure can easily be obtained stably in air or an oxidizing atmosphere. Thus, an oxide containing Nb mainly and represented by the formula (1) {(L x A 1-x ) i NbO y } having a perovskite-like crystal structure, which is difficult to be synthesized in an oxidizing atmosphere, can easily be produced by a previous step of forming the above-mentioned copper oxide which is used for determining the crystal structure and a later step of substituting the Cu element with Nb. On the other hand, it is thinkable to vapor deposite on a substrate such as sapphire, magnesia, strontium titanate, etc., and to make the vapor deposited film to have superconductivity by subjecting to the high temperature treatment after vapor deposition or maintaining the substrate at high temperatures during the vapor deposition. But it is well known that during the maintenance at high temperatures, the constituting elements of the substrate diffuse into the vapor deposited film to deteriorate superconducting properties. In order to prevent this, it is thinkable to conduct a thermal treatment at lower temperatures, or a low-temperature deposition as well as to previously deposit a diffusion preventing film on the substrate. According to this invention, the reaction between the substrate and the vapor deposited film is not prevented, but positively applied to produce a superconductive thin film. The materials typically represented by the formula (1) such as La-Sr-Nb-O series materials are known to have possibility to show superconductivity at higher temperature than the materials of Y-Ba-Cu-O and La-Ba-Cu-O series. According to this invention, a La-Sr-Cu-O film is vapor deposited on a niobium substrate to react the niobium of the substrate with the vapor deposited film. The niobium of the substrate diffuses into the vapor deposited film to substitute the copper in the film therewith to form a La-Sr-Nb-O film, while the substituted copper is liberated and vaporized from the film to deposit on a vacuum vessel wall or a cooling wall. Further, in a step of forming a La-Sr-Cu oxide film on a niobium substrate at a high temperature of 1000°C to 1400°C, the niobium substrate and the La-Sr-Cu-O₄ films are subjected to a diffusion reaction to form a La-Sr-Nb-O layer on the surface of the niobium substrate. In the thus formed layer, there is formed a compositional gradient of La and Sr, and thus a stable La-Sr-Nb-O series superconducting body can be formed in the layer with good reproducibility. In the superconducting material obtained by this invention, the positional relationship between the Cu corresponding portion (Nb) and the oxygen strongly influences the superconducting properties, and thus the La and Sr corresponding portion seems to contribute to the formation and maintenance of the predetermined chemical structure. In the next place, processes for producing the perovskite-like superconducting materials of this invention are explained concretely. Production of (La x Sr 1-x )₂NbOy by mixing starting material powders Lanthanum oxide (La₂O₃) powder, strontium carbonate (SrCO₃) powder and niobium oxide (NbO, NbO₂, Nb₂O₅) powder or pure metallic niobium (Nb) powder are weighed in predetermined stoichiometric amounts, and mixed to react at about 900° to 1500°C for several hours in an oxidizing atmosphere. When Nb₂O₅ is used, the temperature of 1300° to 1500°C is preferable. When Nb is used, the temperature of 900° to 1100°C is preferable. The resulting reaction mixture is pulverized, press molded into a suitable shape, and sintered at a temperature slightly higher than the above-mentioned reaction temperature to provide an oxide superconducting material having a desired shape. Production of (La x Sr 1-x )₂NbOy by sputtering La-Sr-Cu-O is used as a target. As a substrate, pure Nb plate of 15 µm thick is used. Sputtering is carried out at the substrate temperature of 1200°C. In this case, a substrate supporting plate is connected to a liquid nitrogen tank to rapidly cool the substrate to the liquid nitrogen temperature when a heater for the substrate is turned off. The sputtering is conducted in an argon atmosphere at a pressure of 0.5 to 0.7 Torr. After rapid cooling, the substrate is placed in an oxygen atmosphere of 2 Torr at 500°C for 5 minutes. By the sputtering at 1200°C, the Cu in the starting material is substituted with Nb. The thus obtained thin film can provide a sample of 15 µm thick. X-ray diffraction pattern of the thus produced sintered body of (La 0.5 Sr 0.5 )₂NbO₄ shows peaks of 2ϑ at 24.6°, 31.1°, 33.6°, 43.2°, 47.9°, 54.6°, 55.4° and 65.4°. The sintered body is crystallized and has a color of almost black. According to the present inventors' measurement, 2ϑ of the same series materials (i=2 in the formula (1), e.g. (L·A):M=2:1) is the same as 2ϑ of (La 0.5 Sr 0.5 )₂NbO₄. EPMA analysis of LaSrNbOy (y is estimated to be 4) thus obtained is shown in Fig. 2. The results of X-ray diffraction are the same as the above-mentioned 2ϑ data. From other properties and the analysis values of Fig. 2, this oxide has the above-mentioned composition and is identified as a superconducting material having a perovskite-like crystal structure. In Fig. 2, (1) is LaLβ 2.4583 Å, (2) is LaLα 2.6851 Å, (3) is LaLβ 2.4583 Å, (4) is NbLβ 5.4914 Å, (5) is NbLα 5.7235 Å, (6) is SrLβ 6.6234 Å, (7) is SrLα 6.8624 Å, and (8) is LaLα 2.6651 Å. Properties of LaSrNbO₄ immediately after sintering are shown in Fig. 3. Using the same sample that used for measuring the properties of Fig. 3 and lowering the sample temperature to 200 K, the electric resistance is measured again and shown in Fig. 4. As is clear from Fig. 4, the reproducibility is good and considerable stability is obtained. As shown in Fig. 4, the electric resistance of this material begins to down at 315 K and becomes zero at 300 K and completely zero at 255 K even if a slight noise region on measuring is removed. On the other hand, as shown in χ (%) in Figs. 3 and 4, Meissner effect is also admitted. χ means magnetization and represented by a ratio of magnetization compared with the complete superconducting standard (Nb at 4.2 K). When this ratio is negative, the Meissner effect is exhibited, and χ = -100% means complete superconductivity. The electric current condition in measuring resistance is 3 mA/cm². It is possible to obtain the desired superconductivity characteristics by subjecting to the above-mentioned temperature cycle. Further, it is possible to use an apparatus applying superconductivity by limiting the temperature range showing the desired properties. For example, if there is a region showing the complete zero of the resistance temporarily, for example at 300 K as shown in Fig. 4, the use of this region or the use as a switching material applying this region (due to the change in the resistance in the upper temperature region and the lower temperature region) becomes possible. Processes for producing the materials of this invention by substituting the Cu portion of so-called perovskite-like starting materials containing Cu by sputtering will be explained later. Production of Y x Ba 1-x NbOy Powders of Y₂O₃, BaCO₃ and Nb₂O₅ or pure metallic Nb as starting materials are weighed in predetermined amounts, mixed and subjected to heat treatment at high temperatures. The thus obtained reaction mixture powders are molded and sintered to give the desired oxide superconducting materials. The thus obtained sintered body {Y 0.4 Ba 0.6 NbO₃} has peaks of 2ϑ when measured by X-ray diffraction method at 22.7°, 32.7°, 38.5°, 40.3°, 46.6°, 47.5°, 58.2°, 58.9° and 68.8°. The sintered body is crystallized and has an almost black color. According to the present inventors' measurement, 2ϑ of the same series materials (i=1 in the formula (1)) is the same as that of the above-mentioned (Y x Ba 1-x )NbOy and shows peaks at 32.6°, 38.5°, 40.4°, 47.0°, 58.5°, etc. The sintered body is crystallized and has an almost black color. Temperature dependency of electric resistance of the sintered bodies thus obtained, i.e. (La x Sr 1-x )₂NbOy wherein 0 < y ≦ 4, x = 0.5, and Y x Ba 1-x NbOy wherein x = 0.5 and 0 < y ≦ 3, is shown in Fig. 5. Since these properties are changed greatly by the stoichiometric proportions, and heat treatment conditions (sintering temperature pattern, atmosphere at the time of sintering, annealing conditions, etc.), the data in Fig. 6 are only examples and not limited thereto. The electric resistance is lowered with a decrease of temperature and is rapidly lowered at about 280 K and becomes completely zero at about 250 K. That is, the superconducting state begins at about 280 K and is completely attained at about 250 K. In this case, the transition width is as large as 30 K, but this can be reduced remarkably by properly selecting the heat treatment conditions during the sintering, and annealing conditions after sintering. The reaction temperature of the starting material mixed powders and the heat treatment temperature at the time of sintering can be lowered by substituting by Cu as in the case of (L x A 1-x ) i Nb 1-z Cu z O y (0 < z < 1). In this case, there is no great deterioration in the superconductivity characteristics. Production of thin films of superconducting materials Oxide superconducting thin films of this invention with the desired shapes and thicknesses can directly be formed on a substrate of Si single cyrstal, Al₂O₃ single crystal, SiO₂ single crystal, MgO single crystal. ZrO₂ single crystal, or Al₂O₃ ceramic substrate by sputtering using the ceramics obtained by the sintering method as mentioned above as a target in an argon atmosphere or an oxidizing atmosphere with a suitable oxygen partial pressure. If fine film thickness adjustment and stoichiometric compositional ratio adjustment are necessary, it is preferable to deposit films by using, for example, a molecular beam epitaxy method. Needless to say, other conventionally known film forming methods such as physical methods, chemical methods, physicochemical methods can be used. Production of (L x A 1-x ) i Nb 1-z Cu z O y A process for producing materials containing Cu is explained referring to Fig. 6. An oxide powder of L element, a carbonate powder of A element, and CuO powder are weighed to give the desired compositions. The mixed powders are reacted at 900° to 1000°C in an oxidizing atmosphere with heating. With the reacted mixture powder, Nb metal powder is weighed and mixed. The resulting mixed powders are subjected to heat treatment again in vacuum, reducing or oxidizing, preferably weakly oxidizing atmosphere (in the latter case, the atmosphere is adjusted so as not to oxidize Nb(II)O to Nb₂(V)O₅) to give powder of (L x A 1-x ) i Nb i-z Cu z O y . The resulting powder is press molded and sintered to produce an oxide superconducting material having a suitable shape. Further, the reacted mixture powder obtained in the initial step or the final reaction powder can be packed in a tube of a metal such as copper or adhered to a metal tape as a film, followed by reaction and sintering to produce superconducting wires by using the oxide superconducting materials of this invention. After sintering, it is preferable to conduct annealing in an oxidizing atmosphere. Formation of thin films of oxide superconducting materials Oxide superconducting thin films of this invention with the desired shapes and thicknesses can directly be formed on Si single crystal, Al₂O₃ single crystal, SiO₂ single crystal, MgO single crystal, ZrO₂ single crystal or a substrate of these polycrystalline bodies by sputtering using the ceramics (bulk bodies) obtained by the above-mentioned sintering method in an argon atmosphere or in an argon atmosphere having a suitable oxygen partial pressure. If fine film thickness adjustment and stoichiometric compositional ratio adjustment are necessary, it is preferable to deposit films by using, for example, a molecular beam epitaxy method. Needless to say, other conventional known film forming methods such as physical methods, chemical methods, physiochemical methods can be used. In either case, by making the film growth conditions the most suitable, there can be obtained the superconductivity showing the same tendency as shown in Fig. 5. It is also possible to employ a method as shown in Fig. 7, wherein a metal thin film 2 of Nb element is grown on a substrate 1 of Al₂O₃ single crystal (Fig. 7(a)), a film 3 having a suitable stoichiometric compositional ratio of the L element and A element is deposited on the film 2 (Fig. 7(b)), then the metal thin film 2 and the film 3 are reacted by heat treatment to convert a part or whole of the portions of the films 2 and 3 into an oxide superconducting thin film 4 (Fig. 7(c)). In this case, it is possible to deposit the film 3 of the L element and A element first, and then to grow the Nb thin film 2, followed by the heat treatment to obtain the same effect. When a thin film of the superconducting material of this invention is used as an electrical wiring on a substrate, it is possible to form a film with the desired pattern on an electrical insulating ceramic substrate by screen printing, followed by firing. Similarly, it is also possible to produce a multi-layered wiring ceramic substrate. Production of tapes of oxide superconducting material On a metallic tape of Nb element, a film of L element (La or Y) and A element (Ba or, Sr) in a suitable stoichiometric composition (L x A 1-x , 0 < x < 1) (in the case of sputtering, a Cu-containing material such as LaSrCuO 3-δ or the like can be used as a target) is formed by a conventional film depositing method such as a sputtering method or a powder coating baking method, followed by heat treatment to subject a part or whole of the Nb metal tape to the substitution reaction, or diffusion reaction or both reactions in combination. Oxide superconducting wires can be produced by forming a film of L x A 1-x on the surface of a metallic wire made of copper, copper alloy or stainless steel as a base material, depositing a metallic film of Nb element, and subjecting to the heat treatment to carry out the reaction. In this case, a plurality of the L x A 1-x films and the Nb metallic films are laminated alternately, the reactivity at the time of heat treatment can be improved remarkably. Production of(L x A 1-x ) i Nb 1-z Cu z O y On a substrate such as Al₂O₃ single crystal, a metal film of Nb is first formed, and a film of (L x A 1-x ) i CuO y is deposited thereon in an inert atmosphere, followed by heat treatment in vacuum, reducing or oxidizing atmosphere to diffuse the Nb atoms and to substitute Nb Cu. In this case, when a plurality of the Nb metallic films and oxide films of (L x A 1-x ) i CuO y are laminated alternately, the substitution of Cu atom by Nb can be enhanced by the heat treatment. Further there can employ other processes such as forming an Nb metallic film on an oxide ceramic substrate made of (L x A 1-x ) i CuO y , followed by heat treatment. According to the above-mentioned illustrations, there can be easily obtained oxide superconducting materials having a Tc of 150 K or higher, those having a Tc of 200 K or higher, and those having a Tc of 250 K or higher as shown in Fig. 5. Influence of oxygen and prevention of oxygen infiltration In Fig. 6, the heat treatment is conducted in a non-oxidizing or weak oxidizing atmosphere, but it can be conducted in vacuum or in an oxidizing atmosphere. When the heat treatment is conducted in an oxidizing atmosphere, it is necessary to adjust the conditions so as not to enhance the oxidation number (valence number and oxygen content) of the oxidizing components in the Nb starting materials. As mentioned above, when the total valence number of oxygen and the total valence number of other elements are substantially balanced, there can be obtained stable (less deteriorating) materials. In this case, a slight excess and deficiency of oxygen defect is immaterial, and the difference between the total valence numbers in the range of ±0.5 causes no damages. In practice, valence numbers of the same element change mutually (e.g. in the case of Nb, valence 2 ↔ valence 5) in the perovskite-like materials, so that it is preferable to take the lower valence value (e.g. valence 2 in the case of Nb). The annealing can be conducted either in an oxidizing atmosphere or in a reducing atmosphere. In order to prevent deterioration of the thus obtained superconducting materials, it is necessary to take care of the selection of suitable stoichiometric compositional ratio of starting materials, ionic radii, and electrical neutrality. Fig. 8 a cross-sectional view of one example of superconducting parts according to this invention, wherein an oxygen prevention film 5 is used in order to solve the problem of being easily oxidizable. That is, whole exposed portions (sides and upper side) of the superconducting thin film 4 formed on a substrate 1 are covered with an oxygen preventing film 5. Examples of the oxygen preventing film 5 are films of copper, synthetic resins such as polyimides, silicon nitride, and polymer films obtained by using fluorinated hydrocarbon gases as starting materials but not limited thereto. The important thing is that the oxygen preventing film can prevent the oxidation of low-valence atom remained in the perovskite-like structure due to infiltration of oxygen from the outside. It is also possible to form an oxygen preventing film on a cladding material (the surface layer and the outer-side layer) in the case of wires of oxide superconducting materials of this invention. Fig. 9 is a cross-sectional view of another example of superconducting parts according to this invention. In Fig. 9, insulating sheets 7 are interposed between a plurality of thin films 4 of the superconducting materials of this invention. As the insulating sheet, it is preferable to use a material having a perovskite-like structure, since interface state can be improved due to having the same or similar lattice constants and crystal structures. The thickness of each sheet is preferably 10 to 20 Å. As the insulating sheet, there can be used SrTiO₃, LiNbO₃, and the like. When the superconducting material of this invention contains Nb, the use of LiNbO₃ is useful due to its affinity. Production of (L x A 1-x ) i NbO y by substitution of Cu with Nb The process is explained referring to Fig. 10, in which M signifies Nb. An oxide containing Cu mainly and represented by the formula: (L x A 1-x )CuO y is synthesized first. This can be produced by weighing powders of an oxide of L element, a carbonate of A element and CuO in the desired stoichiometric amounts as starting materials, mixing the starting materials, reacting the mixture at about 900°C for several hours in the air, pulverizing the reacted product, press molding the resulting powder, and sintering at 900°C to 1100°C for several hours in an oxidizing atmosphere such as air. By pulverizing the copper-containing oxide, there is obtained a superconducting powder. To the resulting powder, a pure metal powder of Nb is added and mixed to make Cu:Nb ≒ 1:1. The resulting mixture is press molded and reacted at 700° to 1000°C for several hours in vacuum to substitute the Cu atom with Nb, followed by sintering for several hours in a weakly oxidizing atmosphere to yield a ceramic. The resulting ceramic is annealed in an oxidizing atmosphere, followed by pulverization to yield a superconducting powder of (L x A 1-x ) i NbO y . Production of (L x A 1-x ) i NbO y by sputtering The process is explained referring to Fig. 11 in which M signifies Nb. The superconducting ceramic of (L x A 1-x ) i CuO y is synthesized in the same manner as mentioned above. On the outer surface of the thus obtained ceramic, a film of pure metal of M element (Nb) is coated by sputtering or vapor deposition method in vacuum. The resulting product is subjected to a diffusion-substitution reaction at 700° to 900°C in vacuum for several hours. The resulting ceramic of (L x A 1-x ) i NbO y is stable in the air. This ceramic is annealed at 500° to 900°C for several tens hours in an oxidizing atmosphere. The resulting product is pulverized to give a superconducting powder of (L x A 1-x ) i NbO y . A superconducting body with the desired shape can be produced by press molding the resulting ceramic powder into the desired shape, sintering the molded product at 900° to 1100°C for several hours in an oxidizing atmosphere, followed by annealing at 600° to 900°C for several tens hours in an oxidizing atmosphere. A superconducting wire can be produced by packing the above-mentioned ceramic powder in a metal tube made of Cu, Ag, etc., followed by heat treatment. Further, as shown in Fig. 12, a powder 5 of (L x A 1-x ) i CuO y is packed in a metal tube 6 made of Nb, which is then housed in a metal tube 7 and subjected to heat treatment at about 700°C for several hours to carry out a substitution reaction of the Cu atom in the powder 5 with the Nb of the metal tube 6 made to give a powder 8 of (L x A 1-x ) i NbO y . The inner side of the metal tube 6 becomes a metal tube 9 having waste Cu atoms produced by the substitution reaction. By subjecting this to heat treatment, sintering and annealing can be conducted. An apparatus usable for the above-mentioned illustration is explained referring to Fig. 13, which is a schematic cross-sectional view of an direct current magnetron sputtering apparatus. As a target 11, there is used a sintered body of a La-Sr-Cu-O 4-δ oxide. This oxide can be obtained by well mixing powders of La₂O₃, SrCO₃ and CuO, reacting the resulting mixture at 900°C for about 10 hours in the air with heating, press molding the reaction product powder into a circular plate, and sintering the circular plate at 1100°C for about 5 hours. The thus obtained target is placed on a cathode plate 12 made of copper. Numeral 13 denotes an electrical insulating part, and numeral 14 denotes a permanent magnet of samarium-cobalt series which is used for conducting magnetron sputtering discharge by forming a circular magnetic field distribution on the top face of the target 11 together with a magnetic circuit part 15 having high permeability. An earthed anode 16 is also used as a container for liquid nitrogen 17 and cooled to the liquid nitrogen temperature level. The bottom plate of said container is positioned between the electrical insulating part 13, the permanent magnet 14 and the magnetic circuit part 15 and is maintained at the liquid nitrogen temperature level. Numeral 18 denotes a part for holding the permanent magnet 14, the magnetic circuit part 15 and the anode 16. Numeral 19 denotes a lead wire for applying a negative direct current voltage to the anode plate 12. A niobium thin plate 20 which becomes a substrate for forming an oxide superconducting thin film is placed on a heater electrode 21. Argon is used as a sputtering atmosphere 22 and controlled in a pressure range of about 0.1 to 0.8 Torr during sputtering. The production of La-Sr-Nb-O series oxide superconducting material can be carried out as follows. A sputtering chamber is evacuated to about 1 x 10⁻⁶ Torr. Then, liquid nitrogen is charged into the container which becomes the anode 16. An argon gas is continuously flowed into the sputtering chamber so as to make the pressure 0.5 Torr. To the niobium thin plate 20 which becomes a substrate for forming the oxide superconducting film, an electric current is passed via the heater electrode 21 and set so as to make the niobium thin plate temperature 1100° to 1200°C. To the lead wire connected to the anode plate 12, a negative voltage of about 300 V which becomes the sputtering voltage is applied, and the magnetron sputtering discharge is started. At this stage, the sputtering current is about 250 mA. The sputtering is conducted for about 1 hour. A La-Sr-Cu-O oxide film adhered to the A and B portions of the niobium thin plate which is also used as a heater is subjected to a diffusion reaction with the niobium substrate 20 and a substitution reaction of Cu with Nb in the course of the film formation to finally form a La-Sr-Nb-O film layer of about 5 µm thick on the niobium substrate 20. After the sputtering, the temperature of the niobium substrate is lowered to about 500°C in about 10 minutes. Then, the liquid nitrogen is removed, and oxygen is introduced into the argon atmosphere until the pressure of about 2 Torr is obtained to subject the niobium substrate surface to oxidation treatment for about 10 minutes. Subsequently, the temperature of the niobium substrate is lowered to about 100°C in about 5 minutes. Under this state, oxygen is further introduced into the argon atmosphere to make the pressure about 100 Torr, and allowed to stand for 24 hours. The thus obtained niobium substrate is cut into a suitable size and subjected to the measurement of electric resistance and magnetization by varying temperatures. A sample of the A portion shown in Fig. 13 does not show a superconducting state at about 4 K or higher. On the other hand, a sample of the B portion lowers its electric resistance rapidly at about 300 K as shown in Fig. 14 and becomes zero in the electric resistance at about 270 K. Further, the magnetization of this sample is decreased to the negative side at about 300 K corresponding to the temperature change of electric resistance, and becomes an almost constant value at about 250 K as shown in Fig. 15. From the above-mentioned two facts, it is estimated that the sample of B portion is transferred to the superconducting state at about 270 K. According to the above illustration, since La-Sr-Nb-O oxide superconducting material can be produced stably with good reproducibility, it is effective to produce oxide superconducting materials having a Tc of about 270 K. Another illustration is explained referring to Figs. 16 to 18. Fig. 16 is a schematic flow chart showing the production of La-Sr-Cu-O series superconducting thin film by the reaction between a substrate and a vapor deposited film. Fig. 17 is a schematic cross-sectional view showing another apparatus for producing a superconducting thin film according to this invention. Fig. 18 is a graph showing the results of analysis of element distribution in a thin film by using an ion microanalyzer. A principle of the process of this invention is explained referring to Fig. 16. On a niobium substrate 31, a La-Sr-Cu-O film 32 is vapor deposited. Copper atoms 33 in the vapor deposited La-Sr-Cu-O film 32 are substituted with niobium atoms 34 diffused from the substrate 31. In order to bring about the substitution reaction rapidly, it is necessary to heat the niobium substrate 31 at sufficiently high temperatures and to make the diffusion rate of the niobium atoms 34 fast into the La-Sr-Cu-O film 32. As a result of the substitution reaction, a La-Sr-Nb-O film 35 is formed on the niobium substrate 31. The librated copper atoms 36 are vaporized. Fig. 17 is a schematic cross-sectional view of an apparatus used for producing thin films of this invention. The niobium substrate 31 shown in Fig. 16 is introduced into a vacuum container 37 and installed. The vacuum container 37 can be maintained at ultrahigh vacuum of the order of 10⁻¹⁰ Torr by evacuating by a turbo-molecular pump 39. It is also possible to introduce gases such as oxygen, argon, etc. through a gas introducing valve 45. When the pressure becomes 10⁻³ Torr or higher, the turbo-molcular pump 39 is separated by a gate valve 38. The niobium substrate 31 is heated by directly passing an electric current from a constant electric current source 48 through an electric current introducing terminal 42. A La-Sr-Cu-O target 46 for vapor deposition is fixed to a revolving, linear introducing mechanism 43, and irradiated by a Nd:YAG laser light 44 in pulse state to vaporize La-Sr-Cu-O and to vapor deposit on the niobium substrate 31. On the niobium substrate 31, the substitution reaction of copper atoms with niobium atoms takes place as explained in Fig. 16 to form a La-Sr-Nb-O film on the niobium substrate 31. In order to maintain the formed crystal structure showing superconductivity at room temperature, the niobium substrate 31 is rapidly cooled immediately after stopping the electric current passing after completion of the vapor deposition. This rapid cooling is carried out via a copper wire mesh 47 insulated electrically from a cooling shroud 40 installed so as to surround the niobium substrate, and the niobium substrate 31 but thermally connected to the cooling shroud 40. In order to monitor the composition of vapor deposited molecules at the time of vapor deposition, a mass filter 41 is attached via a gate valve 38. A La-Sr-Nb-O thin film showing superconductivity at near room temperature can be produced by using the apparatus shown in Fig. 17. As the niobium substrate 31, there is used a niobium foil of 5 mm wide and 50 µm thick. The niobium substrate 31 is attached to the electric current introducing terminal 42. The vacuum container 37 is evacuated by the turbo-molecular pump 39 to the pressure of the order of 10⁻⁷ Torr. Then, the cooling shroud 40 is filled with liquid nitrogen and the niobium substrate 31 is heated by passing an electric current from the constant electric current source 48. The temperature of the niobium substrate is maintained at 1100°C. After separating the turbo-molecular pump 39 with the gate valve 38, an argan gas is introduced from the gas introducing valve 45 to make the pressure 0.5 Torr. Then, the LaSrCuO₄ target 46 of 100 mm in diameter and 5 mm in thickness attached to the revolving linear introducing mechanism 43 is irradiated with a Nd:YAG laser light 44 having a wavelength of 1064 nm, a maximum intensity of 10⁷ Watt/cm², a pulse width of 0.12 ms, and a repeating rate of 10 Hz. The distance between the niobium substrate 31 and the LaSrCuO₄ target 46 is 4 cm. The angle of incidence of the Nd:YAG laser light 44 to the target 46 is made 25°. Under such conditions, a vapor deposition rate of about 1 nm/s can be obtained. When the film thickness of the vapor deposited film becomes 2 µm, the constant electric current source 48 for heating by passing an electric current is turned off. The vapor deposited film is rapidly cooled by heat conduction via the copper wire mesh 47 to the cooling shroud 40 to the liquid nitrogen temperature within several minutes. The resulting film shows the presence of copper atoms in a very small amount and the substitution of copper atoms with niobium atoms as shown in Fig. 20. The resulting thin film shows diamagnetism in 1/3 of superconducting niobium near room temperature. As the vapor deposition method, a sputtering method, and electron beam vapor deposition can also be used in place of the laser light. According to the above-mentioned illustration, Sa-Sr-Nb-O thin films showing superconductivity near room temperature can easily be produced stably. As mentioned above, according to this invention, oxide superconducting materials having a Tc of 150 K or higher can be produced easily. Thus, the liquid nitrogen temperature level for maintaining superconductivity is not necessary according to this invention.

Claims: A superconducting material represented by the formula (L x A 1-x ) i Nb 1-z Cu z O y wherein (i) L=La, A=Sr or (ii) L=Y, A=Ba and wherein 0 < x < 1; 0 ≦ z < 1 and either i is 1 and 0 < y ≦ 3 or i is 3/2 or 2 and 0 < y ≦ 4. A material according to claim 1 wherein z = 0 so that the formula is (L x A 1-x ) i Nb O y A material according to claim 2 of the formula (La x Sr 1-x ) i NbO y A material according to claim 2 of the formula (La 0.5 Sr 0.5 )₂ NbO y wherein y is 4. A material according to claim 2 of the formula (Y x Ba 1-x ) i NbO y A material according to claim 1 wherein 0 < z < 1, L=La and A=Sr, so that the formula is (La x Sr 1-x ) i Nb 1-z Cu z O y A material according to claim 1 wherein 0 < z < 1, L=Y and A=Ba, so that the formula is (Y x Ba 1-x ) i Nb 1-z Cu z Oy A process for providing a superconducting material according to claim 1 wherein 0 < z < 1 in the form of a film, which comprises depositing, on a metal film of one element selected from the elements L,A, as defined in claim 1 and Nb or Nb containing Cu, a mixture of the rest of the elements other than that of the metal film, and heat treating the metal film and the resulting deposited layer to carry out a diffusion reaction therebetween. A process according to claim 8 wherein a concentration gradient of the constituting metal elements is formed by the diffusion reaction in the film in the thickness direction. A process for producing a superconducting material according to claim 1 wherein 0 < z < 1 in the form of a film which comprises: using as a target an oxide represented by the formula (L x A 1-x ) i Cu O y using as a substrate a film of Nb; passing an alternating electric current through the substrate so as to maintain the temperature of the substrate at 1000° to 1400°C; conducting sputtering by using a direct current magnetron sputtering apparatus in an argon atmosphere with a pressure of 13.3 - 106.7 Pa (0.1 to 0.8 Torr) at a sputtering voltage of 200 to 400V and a sputtering electric current of 20 mA to 100 mA; and conducting a diffusion reaction between the substrate and the sputtered layer. A process according to claim 10 which further comprises subjecting the resulting film-coated substrate to heat treatment at 500° to 600° C for 10 to 30 minutes in a weakly oxidizing atmosphere. A process for producing a superconducting material according to claim 1 wherein 0 < z < 1 in the form of a powder, which comprises depositing a film of pure metal of the element Nb on the outer surface of an oxide represented by the formula: (L x A 1-x ) i Cu O y (4) in vacuum; substituting the Cu of the oxide of the formula (4) with the Nb at 600° to 900°C by the diffusion of the element Nb; subjecting the resulting product to annealing in an oxidizing atmosphere, and pulverizing the resulting annealed product. A process for producing a superconducting material according to claim 2 in the form of a film, which comprises using as a substrate at least one material selected from silicon, aluminum oxide, silicon oxide, magnesium oxide and zirconium oxide, forming a metal thin film of the element Nb on the substrate, depositing a film of L x A 1-x on the metal thin film, and subjecting the resulting film to heat treatment to carry out a diffusion reaction of these elements. A process according to claim 13 wherein a plurality of the metal thin films of the element Nb and a plurality of the L x A 1-x films are laminated alternately on the substrate before the heat treatment. A process for producing a superconducting material according to claim 2 which comprises depositing a film of L x A 1-x , on a metal tape or a substrate of the element Nb and subjecting the resulting film to heat treatment to carry out a diffusion reaction of these elements. A process according to claim 15 wherein the deposition of L x A 1-x film is carried out by a sputtering method or a molecular beam epitaxy method. A process for producing a superconducting material according to claim 6 or claim 7 in the form of a film, which comprises using a substrate made of at least one member selected from silicon, aluminum oxide, silicon oxide, magnesium oxide, and zirconium oxide, forming a metal thin film of the element Nb on the substrate, depositing an amorphous or polycrystalline film of (L x A 1-x ) i CuO y on the metal thin film, and subjecting the resulting film to heat treatment to diffuse the element Nb into the (L x A 1-x ) i CuO y film. A process for producing a film of La-Sr-Nb-0 oxide superconducting material which comprises using as a target a La-Sr-Cu-O₄ sintered body, and as a substrate a niobium material, passing an alternating electric current through the substrate so as to maintain the temperature of the substrate at 1000° to 1400°C, conducting sputtering in an argon atmosphere with a pressure of 13.3 - 106.7 Pa (0.1 to 0.8 Torr) at a sputtering voltage of 200 to 400V and a sputtering electric current of 20 mA to 100 mA to form a film of La-Sr-Cu-O₄ on the niobium substrate surface, conducting a diffusion reaction between the substrate and the sputtered layer, and subjecting the resulting niobium substrate to heat treatment at 500° - 600°C for 10-30 minutes in a weakly oxidizing atmosphere.

Inventors: HAKURAKU YOSHINORI, OGATA HISANAO HITACHI TSUKUBA, OGUSHI TETSUYA, HAKURAKU, YOSHINORI, OGATA, HISANAO HITACHI TSUKUBA HAUSU 8-4-4, OGUSHI, TETSUYA
Applicants: HITACHI LTD, HITACHI, LTD.
Application year: 1988
Main classification: H01L29
IPC codes: H01L39