Method of manufacturing oxide superconductor

Abstract: A method of manufacturing an oxide superconductor by heating a raw material for an oxide superconductor composed of MBa₂Cu₃O 7-δ , where M represents at least a single element selected from a group of Y, Nd, Sm, Eu, Gd, Dy, Ho, Er, Tm, Yb and Lu, to a temperature higher than a peritectic reaction temperature for melting the same and thereafter reducing the temperature to the peritectic reaction temperature to crystallize the oxide superconductor by peritectic reaction. A method of forming a dispersion solution of powder of a raw material for an oxide superconductor and applying the same on a substrate to prepare a thick film. A method of dipping a single crystal of M₂BaCuO₅ in a molten solution of a mixture of BaCuO₂ and CuO to form a thin film of an oxide superconductor on the single crystal. A method of manufacturing a bulky oxide superconductor by dipping a porous sintered material of M₂BaCuO₅ in a molten solution of a mixture of BaCuO₂ and CuO.

Description: BACKGROUND OF THE INVENTION Field of the Invention The present invention relates to a method of manufacturing an oxide superconductor. Description of the Prior Art A superconductive material composed of YBa₂Cu₃O 7-δ , which shows superconductivity at a high temperature of about 90 K, is expected for various uses. For example, such a superconductive material can be applied to power transmission, in order to extremely reduce power loss of about 7 % caused by transmission. With respect to a use as an electromagnet, studied is application to nuclear fusion, SOR, an accelerator, a magnetic levitation train, NMR-CT, an electromagnetically driven ship or the like. In application to such usage, it is preferable to work the superconductive material having the aforementioned composition into the form of a bulk material, a wire rod, a tape or the like. In this case, a value generally obtained as critical current density Jc is about 10³ to 10⁴ A/cm² at the liquid nitrogen temperature of 77 K. However, it is said that critical current density Jc of at least 10⁶ A/cm² is required for practical use such as power transmission or application to an electromagnet. A bulk oxide superconductor has been mainly manufactured by a solid phase reaction method or a coprecipitation method. Powder of the aforementioned yttrium oxide superconductive material is generally synthesized by the solid phase reaction method. A YBa₂Cu₃O 7-δ material is prepared by the sintering method as follows: First, BaCO₃, Y₂O₃ and CuO are weighted as starting materials in the ratios Y:Ba:Cu = 1:2:3, and mixed in a mortar. Powder of such a mixture is heated/reacted within an alumina crucible in an oxygen flow or in the atmosphere at 930 to 950 o C for 8 to 12 hours. Then the powder is ground and pelletized, which is sintered in the air or in an oxygen flow of 900 to 950 o C for 12 to 24 hours, and then subjected to furnace cooling. In the coprecipitation method, reagents such as oxalate, carbonate and citrate are employed to synthesize YBa₂Cu₃O 7-δ through thermal decomposition of such reagents. Another oxide superconductor expressed as MBa₂Cu₃O 7-δ , where M represents at least a single element selected from a group of Nd, Sm, Eu, Gd, Dy, Ho, Er, Tm, Yb and Lu, is also prepared by a substantially similar synthesizing method. A vapor phase growth method has been conventionally reported as a method of preparing a thin film of an oxide superconductor. For example, there are reports that an oxide thin film has been formed by molecular beam epitaxy (MBE) to obtain a thin film having b and c axes oriented in surfaces, that a thin film of 1 µm in thickness has been grown on an SrTiO₃ substrate by a three-gun vapor deposition method, and the like. In the conventional solid phase reaction method, powder materials are mixed with each other in a mortar. However, the degree of such mixing is to about the size of the starting particles at the most, and homogenous dispersion is limited. Further, since solid phase reaction progresses only in the vicinity of contact points between particles, such reaction must be repeated in order to obtain a YBa₂Cu₃O 7-δ phase. In addition, the obtained sample is porous and its density is merely about 70 to 80 % of a theoretical value. In a conventional method of manufacturing an oxide superconductor by the vapor phase growth method, on the other hand, manufacturing steps are complicated and the growth rate of a film is slow, leading to inferior productivity. In the conventional method, further, such a problem is particularly caused in density that a body obtained is considerably porous with density similar to that of a sintered material, and a critical current value is reduced as the result. Nature 328, 13 August, 1987, pp. 601-603, L.F.Schneemayer et al.; Adv. Ceramic Mat. 2, 20 July 1987, pp. 303-312, R.S.Roth et al.; and Jap.J.Appl.Phys., Vol.26, No.5, May 1987, pp. L825-L827, A.Ono and T.Tanaka disclose details on the BaO-CuO-Y₂O₃ ternary phase diagram. SUMMARY OF THE INVENTION An object of the present invention is to provide a method of manufacturing an oxide superconductor, which can manufacture a homogenously composed oxide superconductor being superior in density and crystallinity to the prior art through relatively simple steps. The present invention is directed to a method of manufacturing an oxide superconductor which is crystallized through peritectic reaction by heating a material therefor to a temperature higher than a peritectic reaction temperature for melting the same and then cooling the melt to the peritectic reaction temperature, thereby to crystallize the oxide superconductor thus obtained through peritectic reaction. According to the present invention, a material is temporarily heated to a temperature higher than the peritectic reaction temperature to be in a molten state, whereby rapid and homogenous reaction can be attained as compared with solid phase reaction which is caused only in grain boundaries. According to a first aspect of the present invention, the method comprises a step of heating a mixture of BaCuO₂ and CuO in an oxygen atmosphere for melting the same and a step of dipping a single crystal material composed of M₂BaCuo₅, where M represents at least a single element selected from the group of Y, Nd, Sm, Eu, Gd, Dy, Ho, Er, Tm, Yb and Lu, in a molten mixture to form a thin film of an oxide superconductor composed of MBa₂Cu₃O 7-δ on the surface of the single crystal material by peritectic reaction. In the first aspect of the present invention, it has been confirmed that MBa₂Cu₃O 7-δ is most rapidly generated when the mole composition ratio of BaCuO₂ to CuO contained in the raw material molten solution is 3:2. It has been also confirmed that superconductivity is improved by annealing the thin film formed on a substrate surface in an oxygen atmosphere of 850 to 900 o C for at least three hours. MBa₂Cu₃O 7-δ causes phase transition depending on density of oxygen, i.e., the value δ. It enters rhombic structure in a range of 0 ≦ δ ≾ 0.5, while entering tetragonal structure in a range of δ ≾ 0.5. A range of δ < 0.2 is preferable particularly in consideration of characteristics such as Tc, ΔTc , Jc and the like. The oxide superconductor composed of MBa₂Cu₃O 7-δ is heated to a high temperature, to cause decomposition/melting reaction as shown in the following formula I: 2MBa₂Cu₃O 7-δ (solid phase) = M₂BaCuO₅ (solid phase) + 3BaCuO₂ (liquid phase) + 2CuO (liquid phase) (I) The reaction system expressed in the formula (I) is peritectic reaction as hereinabove described, which reaction is caused at a temperature lower than that for melting a simple substance of CuO or BaCuO₂. According to the first aspect of the present invention, a substrate of a single crystal material of M₂BaCuO₅ is brought into contact with a raw material molten solution formed of a mixture of BaCuO₂ and CuO to facilitate leftward reaction in the above formula (I), thereby to form a dense thin film of MBa₂Cu₃O 7-δ on the single crystal surface of M₂BaCuO₅. This reaction is liquid-phase reaction, the growth rate of which is extremely high as compared with that of the conventional vapor phase growth method, while operation for such growth is simple. The thin film formed on the substrate, which is raised up from the raw material molten solution, can be further annealed in an oxygen atmosphere of 850 to 900 o C for at least three hours, thereby to improve superconductivity. Thus, according to the first aspect of the present invention, an oxide superconductor can be relatively easily manufactured at a high growth rate, to reduce the manufacturing cost. A thin film substrate manufactured by the method according to the present invention can be applied to a substrate for a superconducting device, for example. According to a second aspect of the present invention, the method comprises a step of heating a mixture of BaCuO₂ and CuO in an oxygen atmosphere for melting the same and a step of dipping a porous sintered material composed of M₂BaCuO₅, where M represents at least a single element selected from the group of Y, Nd, Sm, Eu, Gd, Dy, Ho, Er, Tm, Yb and Lu, in the said molten mixture to form an oxide superconductor having composition of MBa₂Cu₃O 7-δ through peritectic reaction. The sintered material of M₂BaCuO₅ can be obtained by pelletizing powder and thermally treating the same at a high temperature. This sintered material is obtained as a porous one, since it is impossible to obtain a completely dense material. Such a porous sintered material is so dipped in a molten mixture that the molten mixture is sucked up into the sintered material by a capillary phenomenon, to cause peritectic solidification reaction in the above reaction formula (I) over the entire region of the sintered material. Thus, the reaction smoothly progresses when powder forming the raw material for the sintered material has small particle size, while it is difficult to obtain a single phase of MBa₂Cu₃O 7-δ when the said particle size is large, since M₂BaCu₅ is left in MBa₂Cu₃O 7-δ . MBa₂Cu₃O 7-δ is grown from surfaces to interiors of M₂BaCuO₅ fine particles by peritectic reaction, while surrounding the liquid phase to be grown toward the outside. Thus, porosity of the sintered material of M₂BaCuO₅, serving as the raw material, is adjusted to be optimum so that adjacent particles of MBa₂Cu₃O 7-δ are completely adhered to each other upon completion of the peritectic reaction, to provide a bulky polycrystalline substance having dense structure. The sintered material of M₂BaCuO₅ is thus adjusted in particle size and porosity, to quickly obtain a dense bulky polycrystalline substance of MBa₂Cu₃O 7-δ . It has been clarified through the result of an experiment that the particle size is preferably not more than 0.5 µm and porosity is preferably within a range of 5 to 30 %. If the particle size is larger than 0.5 µm, M₂BaCuO₅ is left in the interior of MBa₂Cu₃O 7-δ to require a long time for obtaining a complete single phase, which may not be obtained as the case may be. If porosity is smaller than 5 %, a solid phase of M₂BaCuO₅ may be left and a single phase cannot be obtained after pores are completely filled up with progress of reaction. If porosity is larger than 30 %, on the other hand, pores filled with the molten solution of the mixture of BaCuO₂ and CuO may be left after completion of the reaction with disappearance of the phase of M₂BaCuO₅, to disable formation of a single phase. The mixing ratio of BaCuO₂ to CuO is preferably 3:2 in mole ratio. If the mixing ratio is not 3:2, the molten solution sucked up into the interior of the sintered material of M₂BaCuO₅ by the capillary phenomenon may not be completely removed through the leftward reaction in the above formula (I), i.e., peritectic solidification reaction, and hence excessive components with respect to the mole ratio 3:2 may be left to disable formation of a single phase. Thus, the mixing ratio of BaCuO₂ to CuO is preferably that corresponding to stoichiometric composition of the formula (I), i.e., 3:2. Strictly speaking, a temperature for retaining the molten mixture , in which the sintered material is dipped, is varied with elements. However, a peritectic solidification temperature is within a range of 1000 to 1100 o C for any element. The temperature for retaining the molten mixture, which is preferably lower by about 0 to 100 o C than the peritectic solidification temperature, is preferably 900 to 1100 o C. The time for dipping the sintered material in the molten solution and retaining the same is varied with the temperature for retaining the molten solution, the particle size of the sintered material and the like. However, the reaction can be generally completed in about five minutes to 10 hours. According to the second aspect of the present invention, an extremely dense bulky superconductive oxide having excellent characteristics can be manufactured through relatively simple steps. Further, a wire rod, a coil or the like can be obtained as a dense superconductor having high critical current density. Thus, the method according to the second aspect of the present invention is applicable in various fields to a transmission cable, a medical coil and the like. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 illustrates the result of differential thermal analysis of a YBa₂Cu₃O 7-δ sintered material; Fig. 2 is a sectional view showing an apparatus employed in Example according to a first aspect of the present invention; and Fig. 3 is a sectional view showing an apparatus employed in Example according to a second aspect of the present invention. DESCRIPTION OF THE PREFERRED EMBODIMENTS Example 1 The example is only for technical information and is not falling in the scope of the claims. An oxide superconductor was prepared from YBa₂Cu₃O 7-δ . The peritectic reaction temperature can be obtained by differential thermal analysis. For example, MBa₂Cu₃O 7-δ is decomposed by peritectic reaction into M₂BaCuO₅, CuO and BaCuO₂. The peritectic reaction temperature can be evaluated/decided by identifying a phase around a peak by differential thermal analysis. This peritectic reaction temperature is decided to be within a range of Tp ± 30 o C, assuming that Tp represents the rise temperature of the differential thermal peak. Fig. 1 illustrates the result of differential thermal analysis of YBa₂Cu₃O 7-δ . The leading edge of a temperature-up endothermic peak is 1030°C, and that of a temperature-down exothermic peak is also 1030°C. Example 2 Description is now made on Example 2 according to the first aspect of the present invention. Fig.2 is a sectional view showing an apparatus employed in Example 2 according to the first aspect of the present invention. Referring to Fig. 2, a substrate 1 is mounted on a second end of an upper shaft 3. A raw material molten solution 2 is contained in a platinum crucible 4, and a cylindrical platinum heater 5 is provided around the crucible 4 through a heat insulator 8. The heat insulator 8 is further extended to also enclose the platinum heater 5. These elements are contained in an alumina vessel 6, which is placed in a central portion of an airtight vessel 9. A high-frequency heating coil 11 is provided on the exterior of the airtight vessel 9. The cylindrical platinum heater 5 is provided in order to avoid direct heating of the platinum crucible 4. The airtight vessel 9 is provided with an oxygen inlet 10, which is adapted to supply oxygen. A thermocouple 7 is provided in the bottom portion of the platinum crucible 4. A ground mixture of BaCuO₂ and CuO is introduced into the platinum crucible 4 and oxygen is supplied into the airtight vessel 9 to maintain an oxygen atmosphere, while the high-frequency coil 11 is energized to melt the raw material mixture. Then it is confirmed that the raw material molten solution is retained at a prescribed temperature by the thermocouple 7, and thereafter the upper shaft 3 is downwardly moved to dip a substrate of an M₂BaCuO₅ single crystal in the raw material molten solution. This state is held for a constant period, and then the temperature of the raw material molten solution is gradually reduced to form a prescribed thin film. Thereafter the upper shaft 3 is raised up and the temperature is reduced to an annealing temperature, which in turn is retained for a constant period to form a superconducting oxide thin film of MBa₂Cu₃O 7-δ on the substrate. Example 2-1 The apparatus shown in Fig. 2 was employed to manufacture a thin film of YBa₂Cu₃O 7-δ . First, Y₂O₃, BaCO₃ and CuO were molten and mixed in mole ratios Y:Ba:Cu = 2:1:1 to be pelletized, sintered in the atmosphere at 900 o C for 12 hours, and ground. Powder thus obtained was introduced into an alumina crucible and heated up to 1400 o C to be molten, and then slowly cooled to the room temperature at a cooling rate of 5 o C/min., thereby to obtain a Y₂BaCuO₅ single crystal. It was confirmed by a powder X-ray diffraction method that the crystal was simply composed of Y₂BaCuO₅. A substrate of 2 mm x 2 mm x 5 mm in size was cut from this crystal. On the other hand, a raw material molten solution was prepared by mixing ground BaCO₃ and CuO in a mole ratio Ba:Cu = 3:5, pelletizing the mixture, sintering the same in the atmosphere at 890 o C for 12 hours and grinding the same. It was confirmed by a powder X-ray diffraction method that powder thus obtained was a mixture of BaCuO₂ and CuO. It may be considered that the mixing ratio of BaCuO₂ to CuO was about 3:2, since an X-ray diffraction peak shows only phases of BaCuO₂ and CuO but no other phase, while both of Ba and Cu are substantially non-volatile. The powder was introduced into the platinum crucible, which was placed in the airtight vessel of Pyrex. Oxygen was introduced into the airtight vessel at a flow rate of 1 ℓ/min. to maintain an oxygen atmosphere, and the high-frequency heating coil was energized to heat the raw material. It was observed that the surface of the raw material was completely molten when the thermocouple pointed a temperature of 1025 o C. It has been confirmed through other experiments such as thermal analysis and X-ray diffraction that the raw material molten solution in this state was a mixed molten solution of BaCuO₂ and CuO. The upper shaft was downwardly moved while retaining the temperature of the thermocouple at 1025 o C to hold the substrate in a position immediately above the raw material molten solution with a space of 3 mm and to sufficiently heat the same, thereby to reduce temperature difference between the raw material molten solution and the substrate. Then, the upper shaft was further downwardly moved by 4 mm, to dip the substrate in the raw material molten solution. This state was maintained for 30 minutes, and then the raw material molten solution was cooled to 1005 o C at a temperature-down rate of 10 o C/h. Thereafter the substrate was gradually raised up to be held in a position immediately above the raw material molten solution with a space of 20 mm, and the temperature was reduced until the thermocouple pointed a temperature of 880 o C, which temperature was stabilized and retained for five hours, thereby to anneal the substrate in the oxygen atmosphere. Supply of oxygen during this operation was 1 ℓ/min. Thereafter the substrate was cooled to the room temperature at a cooling rate of 150 o C/h. and then taken out from the apparatus. The color of the substrate was green in correspondence to the composition of Y₂BaCuO₅ before dipping in the raw material molten solution. However, the surface of the substrate was coated with a black thin film after annealing. This black thin film was subjected to structure analysis by X-ray diffraction, to confirm that the same was a polycrystal layer of YBa₂Cu₃O 7-δ . Then, temperature dependence of electrical resistivity was measured by a general four-terminal method, to confirm superconductivity of Tc = 82 K and Jc = 600 A/cm² at 4.2 K. Further, the section was observed through an optical microscope, to confirm that a thin film of 5.3 ± 0.8 µm in thickness was formed over the entire surface of the substrate of 2 mm x 5 mm. The surface was observed through an electron microscope, to confirm that the film was formed by an extremely dense aggregate of fine polycrystals of 20 to 30 µm in particle size. It was confirmed from the result of weight change of DTA/TG measurement that the thin film of YBa₂Cu₃O 7-δ was of high quality with oxygen concentration of δ ≒ 0.1. Example 2-2 An experiment similar to that in Example 2-1 was made by employing Er in place of Y. As the result, a dense polycrystal thin film of ErBa₂Cu₃O 7-δ was formed on a single crystal substrate of Er₂BaCuO₅. In this thin film, Tc was 80 K and Jc was 550 A/cm² at 4.2 K. Example 3 Description is now made on Example 3 according to the second aspect of the present invention. Example 3-1 Fig. 3 is a sectional view showing an apparatus for illustrating Example according to the second aspect of the present invention. Referring to Fig. 3, a sintered material 21 is mounted on a lower end of an upper shaft 23. A raw material molten solution 22 is contained in a platinum crucible 24, and a platinum heater 25 is provided around the platinum crucible 24 through a heat insulator 28. The heat insulator 28 is further extended to also enclose the platinum heater 25. These elements are contained in an alumina vessel 26, which is entirely placed in an airtight vessel 29. A high-frequency heating coil 31 is provided around the airtight vessel 29. The airtight vessel 29 is provided with an oxygen inlet 30, which is adapted to supply oxygen. A thermocouple 27 is provided on the bottom portion of the platinum crucible 24. In this Example, the raw material molten solution 22 was prepared by mixing ground raw materials of BaCO₃ and CuO, pressing the mixture, sintering the same in the atmosphere at 890 o C for 12 hours and grinding the same. The materials were mixed in a mole ratio Ba:Cu = 3:5 (BaCuO₂:CuO = 3:2), and it was confirmed by a powder X-ray diffraction method that powder obtained through the grinding step was a mixture of BaCuO₂ and CuO. The sintered material 21 was prepared by the following process. The mixture of Y₂O₃, BaCO₃ and CuO in mole ratios Y:Ba:Cu = 2:1:1, are pelletized and sintered in the atmosphere at 900 o C for 12 hours, and grinding. Thereafter the powder are pelletized into a column of 10 mm in diameter and 25 mm in length and further sintering the column in the atmosphere at 1080 o C for five hours. It was confirmed by a powder X-ray diffraction method that the sintered material 21 was simply composed of M₂BaCuO₅. The sintered material 21 and the raw material molten solution 22 prepared in the aforementioned manner were employed to manufacture a superconducting oxide in the apparatus shown in Fig. 3. The raw material powder was introduced into the platinum crucible 24 and heated by the high-frequency coil 31. The cylindrical platinum heater 25 is provided to avoid direct heating of the platinum crucible 24. Oxygen was introduced into the airtight vessel 29 of Pyrex from the oxygen inlet 30 at a flow rate of 1 ℓ/min., to provide an oxygen atmosphere in the airtight vessel 29. The raw material contained in the platinum crucible 24 was heated in such an oxygen atmosphere. It was observed that the surface of the raw material contained in the platinum crucible 24 was completely liquefied when the thermocouple 27 pointed a temperature of 1025 o C. It has been clarified by other experiments such as thermal analysis, X-ray diffraction and the like that this state is attained by melting of BaCuO₂ and CuO into liquid phases. The upper shaft 23 was downwardly moved while retaining the thermocouple 27 at the temperature of 1025 o C, and the sintered material 21 was held in a position immediately above the raw material molten solution 22 with a space of 3 mm for 20 minutes and sufficiently heated to reduce temperature difference between the raw material molten solution 22 and the sintered material 21. The sintered material 21 was held in this state for 30 minutes and then gradually raised up to be held in a position immediately above the raw material molten solution 22 with a space of 20 mm. Then the temperature was reduced at a cooling rate of 10 o C/h. until the thermocouple 27 pointed a temperature of 880 o C, which temperature was then stabilized. The sintered material 21 was held in this state for five hours, to be annealed in the oxygen atmosphere. Thereafter the sintered material 21 was cooled to the room temperature at a cooling rate of 150 o C/h. to be taken out from the apparatus. Supply of oxygen during this operation was maintained at a flow rate of 1 ℓ/min. Before dipping in the raw material molten solution 22, the sintered material 21 was a green substance having composition of Y₂BaCuO₅. However, it was changed into a black substance through the aforementioned process. It was confirmed through structure analysis by an X-ray diffraction method that the black substance was a superconductive oxide of YBa₂Cu₃O 7-δ . Temperature dependency of electrical resistivity was measured by a general four-terminal method, to observe superconductivity of Tc = 82 K and Jc = 1050 A/cm² at 4.2 K. The section was polished for observation through an electron microscope, to confirm that the superconducting oxide was extremely densely filled with fine crystals of 30 to 70 µm in particle size. Element composition ratios analyzed by EDX were Y:Ba:Cu = 1:2:3, and it was confirmed that this substance was composed of YBa₂Cu₃O 7-δ . Example 3-2 A superconducting oxide was manufactured in a similar manner to Example 3-1 by a similar apparatus, except for that a sintered material was prepared from a wire rod of 2 mm in diameter and 80 mm in length in place of the cylindrical sintered material. The raw material molten solution, the composition of the sintered material and the like were identical to those of Example 3-1. It was confirmed through an X-ray diffraction method that the wire rod obtained in this Example was changed into a superconductive oxide of YBa₂Cu₃O 7-δ . Temperature dependence of electrical resistivity was measured by a four-terminal method, to confirm superconductivity of Tc = 80 K and Jc = 780 A/cm² at 4.2 k.

Claims: A method of manufacturing an oxide superconductor comprising the steps of: heating a mixture of BaCuO₂ and CuO in an oxygen atmosphere for melting the same; and dipping a single crystal composed of M₂BaCuO₅, where M represents at least a single element selected from the group of Y, Nd, Sm, Eu, Gd, Dy, Ho, Er, Tm, Yb and Lu, in said molten mixture to form a thin film of an oxide superconductor composed of MBa₂Cu₃O 7-δ on the surface of said single crystal member by peritectic reaction. A method of manufacturing an oxide superconductor in accordance with claim 1, further comprising a step of annealing said thin film in an oxygen atmosphere at a temperature of 850 to 900°C for at least three hours. A method of manufacturing an oxide superconductor comprising the steps of: heating a mixture of BaCuO₂ and CuO in an oxygen atmosphere for melting the same; and dipping a porous sintered material composed of M₂BaCuO₅, where M represents at least a single element selected from the group of Y, Nd, Sm, Eu, Gd, Dy, Ho, Er, Tm, Yb and Lu, in said molten mixture to form an oxide superconductor composed of MBa₂Cu₃O 7-δ by peritectic reaction. A method of manufacturing an oxide superconductor in accordance with any of claims 1 to 3, wherein said melting step comprises a step of employing a mixture obtained by mixing BaCuO₂ and CuO in a mole ratio 3:2. A method of manufacturing an oxide superconductor in accordance with claim 3, wherein said sintered material is formed by particles of not more than 0.5 µm in particle size. A method of manufacturing an oxide superconductor in accordance with claim 3 and/or 5, wherein said sintered material has porosity of 5 to 30 %. A method of manufacturing an oxide superconductor in accordance with any of claims 3, 5 and/or 6, wherein said superconductor forming step comprises a step of dipping said sintered material in said molten mixture which is retained at 900 to 1100°C. A method of manufacturing an oxide superconductor in accordance with any of claims 3, 5 to 7, wherein said superconductor forming step comprises a step of dipping said sintered material in said molten mixture and retaining the same for five minutes to 10 hours. A method of manufacturing an oxide superconductor in accordance with any of claims 3, 5 to 8, further comprising a step of cooling said superconductor at a cooling rate of 5 to 110°C/h. after said superconductor forming step.

Inventors: NAMIKAWA YASUO C O OSAKA WORKS, TATSUMI MASAMI C O OSAKA WORKS, TORII YASUKO C O OSAKA WORKS, NAMIKAWA, YASUO C/O OSAKA WORKS, TATSUMI, MASAMI C/O OSAKA WORKS, TORII, YASUKO C/O OSAKA WORKS
Applicants: SUMITOMO ELECTRIC INDUSTRIES, SUMITOMO ELECTRIC INDUSTRIES LIMITED
Application year: 1988
Main classification: H01L39
IPC codes: C04B41, H01L39, C01B13, C04B35, C01G1, H01B13, C01G3