Oxide superconducting material and process for preparing the same

Abstract: Superconducting oxide material containing compound represented by the formula: (Tl (1-p-q) Bi p Pb q ) y γ z (α (1-r) β r ) s Cu v O w in which each of "α" and "γ" is an element selected in IIa group of the periodic table, "β" is an element selected from a group comprising Na, K, Rb and Cs, "y", "z", "v", "w", "p", "q", "r" and "s" are numbers each satisfying respective range of 0.5 ≦ y ≦ 3.0, 0.5 ≦ z ≦ 6.0, 1.0 ≦ v, 5.0 ≦ w, 0 ≦ p ≦ 1.0, 0 ≦ q ≦ 1.0, 0 ≦ r ≦ 1.0 and 0.5 ≦ s ≦ 3.0.

Description: Backgroud of the Invention Field of the Invention The present invention relates to superconducting oxide materials and processes for preparing the same. More particularly, it relates to thallium-containing superconducting oxide materials having high superconducting critical temperature (Tc) and higher superconducting critical current density (Jc) and processes for preparing the same. Description of the related art Discovery of new oxide type superconductor by Bednorz and Müller revealed the possibility of high temperature superconductors (Z. Phys. B64, 1986 p 189). The new type oxide superconductor discovered by Bednorz and Müller is represented by [La, Sr] 2 CuO 4 which is called the K 2 NiF 4 -type oxide having a crystal structure similar to known perovskite type oxides. The K 2 NiF 4 -type compound oxides show such higher Tc as 30 K which are extremely higher than known superconducting materials. C. W. Chu et al. reported another superconducting material of so-called YBCO type represented by YBa 2 Cu 3 O 7-x having the critical temperature of about 90 K (Physical Review letters, Vol. 58, No. 9, p 908). However, the critical temperature of this oxide superconductor is not so different from a boiling point 70 K of liquid nitrogen and hence the other oxide materials which have much higher critical temperature, in other words, which have larger temperature margin have been demanded. Maeda et al reported the other type new superconducting compound oxide of Bi-Sr-Ca-Cu-O system which show the critical temperature of mor than 100 k (Japanese Journal of Applied Physics. Vol. 27, No. 2, p 1209 to 1210). Thallium type compound oxides are also high Tc superconductors of more than 100 K. The present inventors disclosed several kinds of thallium type compound oxides superconductors in US patent application No. 223,634 filed on July 25, 1988 and Hermann et al. reported Tl-Ba-Ca-Cu-O system in Appl. Phys. Lett. 52 (20) p 1738. US patent No. 4,870.052 discloses a kind of thallium-containing oxide superconductor. Thallium type compound oxides have such a very important merit that superconductors which show such a high Tc as more than 100 K can be obtained without using rear earth elements as a material so that the production cost can be reduced. Although these known Tl-Ba-Ca-Cu-O system and Bi-Sr-Ca-Cu-O system oxide superconductors show very high Tco's at which the superconducting property is observed, their Tci's at which the apparent electrical resistance become zero or undetectable are such low as about 80 to 90 K which is not so different from that of the Y 1 Ba 2 Cu 3 O 7-x system because these compound oxide superconductors contain several different phases. Still more, their critical current density values (Jc) are inferior to that of the Y 1 Ba 2 Cu 3 O 7-x system. Still more, in the case of production of thallium type oxide superconductors, there is a special problem cause by such a fact that thallium is a very volatile element and toxic for human. In fact, it is difficult to obtain a thallium-containing oxide having a desired composition because the vapour pressure of thallium is relatively higher than the other elements. Further, the special attention must be paid to handle the material of the thallium-containing superconductor because thallium element is toxic for human. Article issued in Science, Vol. 242, N° 4876, 14th October 1988 pp. 249-252 discloses a superconducting oxide material having a composition given by (Tl 1-y Pb y )Sr 2 Ca 2 Cu 3 O 9 and a process for preparing a superconducting oxide material by mixing and sintering oxide powders at a temperature between 850 and 915°C for 12 hours in an oxygen gas atmosphere. Likewise, earlier European Patent Application n° 324 660 which is a document under Article 54(3) EPC discloses a superconducting oxide material having a composition given by Tl-R-Ba-Cu-O, wherein R is a 2A group element excluding Ba. An object or the present invention is to overcome the problems of the prior arts and to provide a thallium-containing superconductor which is relatively easy to be obtained as a single phase and also which has improved superconducting properties and a method for producing the same. Summary of the Invention This object is achieved by a superconducting oxide material according to claim 1. The present invention provides also a process for preparing the said superconducting oxide material. In operation, the material powder mixture is preferably wrapped with a metallic foil made of one of precious metals such as gold or their alloys. The sintering operation can be effected in an ordinary furnace. The interior of the furnace is preferably in the condition of oxygen-rich atmosphere. The oxygen gas is preferably fed continuously into the furnace during the sintering operation preferably at a rate of more than 0.1 liter per minute at 10 5 Pa(1 atm). Usual oxygen gas pressure is about 10 5 Pa (1 atm) but the sintering can be effected also at a higher oxygen pressure than 10 5 Pa (1 atm). According to the present invention, the sintering is effected at a temperature between 820 and 950 °C. When the sintering temperature is not higher than 820 °C, the resulting sintered mass becomes a mixture of different phases each having different critical temperature, so that the apparent Tc of the sintered mass become lower. To the contrary, if the sintering temperature is not lower than 950 °C, the evaporation of thallium increase excessively so that it is difficult to adjust the composition of the sintered mass to desired atomic ratios and also it increases precipitates which doesn't contribute the superconductivity. The sintering can be effected for a time duration between 6 to 100 hours. When the sintering time is not longer than 6 hours, the material powder mixture is not sintered satisfactorily so that a desired superconductor can not be obtained. Longer sintering time than 100 hours may not effective to improve the superconducting property. As is described hereinabove, the oxide superconductors according to the present invention exhibit very higher critical current density than the known oxide superconductors such as Bi-Sr-Ca-Cu-O system and Ti-Sr-Ca-Cu-O system while they exhibit the same or even higher critical temperature with respect to such known oxide superconductors. It is thought that such advantage might be obtained from such facts that the oxide superconducting materials according to the present invention have a novel layered crystal structure of tetragonal system having one layer of Tl-O, (Tl, Pb)-O, (Tl, Bi)-O or (Tl, Pb, Bi)-O and that the oxide superconducting materials according to the present invention are relatively easily obtained as a single phase. Brief Description of the drawings Fig. 1 to Fig. 5 are X-ray diffraction charts of five oxide superconductors (Sample No. 1 to 5) obtained in Example 1. Fig. 6 is a X-ray diffraction chart of an oxide superconductor (Sample No. 6) obtained in Example 3. Fig. 7 to 9 show respective temperature dependency of magnetic susceptibility of oxide superconductors (Sample No. 3 to 5) obtained in Example 1. Fig. 10 shows a temperature dependency of electric resistance of an oxide superconductor (Sample No. 1) obtained in Example 3. Fig. 11 and Fig. 12 show respective temperature dependency of electric resistance and of magnetic susceptibility of an oxide superconductor (Sample No. 6) obtained in Example 3. Now, the present invention will be described in more details by examples, but the scope of the present invention should not be limited to the following special examples. Example 1 (not part of the invention, technical information only) Oxide superconducting materials were prepared by the process according to the present invention. Powders of Ti 2 O 3 , PbO, CaO, BaO 2 and CuO used as materials were mixed in such proportions that the atomic ratios of Tl : Pb : Ca : Ba : Cu in each sample became as followings: (1) 0.8 : 0.2 : 3 : 1 : 3 (2) 0.75 : 0.25 : 3 : 1 : 3 (3) 0.8 : 0.2 : 3 : 1 : 3 (4) 0.95 : 0.05 : 3 : 1 : 3 (5) 0.95 : 0.05 : 3 : 1 : 3. Then, each of the resulting powder mixture was compacted under a pressure of about 100 kg/cm 2 into a pellet. Each pellet was wrapped with a gold foil of 50 micron thick and was sintered at a fixed temperature selected from a range between 850 °C and 900) °C for about 10 hours in a furnace into which O 2 gas is flown at a rate of 200 ml/mm to obtain an oxide supercondcutor according to the present invention. All of the resulting oxide superconductors were found that they contained compound oxide represented by the general formula: (Tl (1-q) Pb q ) y Ca z Ba s CU v O w in which each of "α" and "γ" is an element selected in IIa group of the periodic table, "y", "z", "v", "w", "q" and "s" are numbers each satisfying respective range of 0.5 ≤ y ≤ 3.0, 0.5 ≤ z ≤ 6.0, 2.0 ≤ v, 5.0 ≤ w, 0 ≤ q ≤ 1.0 and 0.5 ≤ s ≤ 3.0. Table. 1 shows the properties of each oxide superconducting material obtained and Fig. 1 to 5 show X-ray diffraction data thereof. Fig. 7 to 9 show the result of magnetic susceptibility measured on the samples No. 3, 4 and 5 respectively. In the composition shown in Table 1, there are such cases that the ratio of Tl to Pb and the ratio of Ca to Cu don't coincide with the theoretical values which are expected by the analysis of crystal structure because the values shown in Table 1 are measuered values and conain a tolerance. For a comparison, the corresponding properties of known superconducting materials represented by Tl 2 Ca 2 Ba 2 Cu 3 O 10 and (Bi, Pb) 2 Ca 2 Sr 2 Cu 3 O 10 are also shown in Table 1. From the Table 1, it is apparent that the oxide superconducting material show higher critical current density Jc than the known oxide superconducting materials while same or even higher critical temperature Tc is observed. sample No composition lattice constant Tci (K) Jc (A/cm 2 ) 1 (Tl,Pb) 1 Ca 1 Ba 2 Cu 2 O 7 a= 3.86x10 -10 m a = (3.86 Å) c = 12.95x10 -10 m c = (12.95 Å) 80 400 2 (Tl,Pb) 1 Ca 2 Ba 2 Cu 3 O 9 a = 3.86x10 -10 m a = (3.86 Å) c = 16.11x10 -10 m c (16.11 Å) 102 410 3 Tl 0.80 Pb 0.20 Ca 3.0 Ba 2.0 Cu 3.9 O x a =3.85x10 -10 m a = (3.85 Å) c = 19.36x10 -10 m c = (19.36 Å) 121 520 4 Tl 0.82 Pb 0.15 Ca 4.0 Ba 2.0 Cu 4.9 O y a = 3.85x10 -10 m a = (3.85 Å) c = 22.22x10 -10 m c = (22.22 Å) 113 470 5 Ti 0.90 Pb 0.16 Ca 5.0 Ba 2.0 Cu 5.8 O z a = 3.85x10 -10 m a = (3.85 Å) c = 25.97x10 -10 m c = (25.97 Å) 102 -- Comparative Tl 2 Ca 2 Ba 2 Cu 3 O 10 118 270 (Bi,Pb) 2 Ca 2 Sr 2 Cu 3 O 10 108 255 Example 2 (not part of the invention, technical information only) Oxide superconducting materials were prepared by the following process Powders of Tl 2 O 3 , Bi 2 O 3 , BaO 2 , CaO and CuO (purity is higher than 99.9 %) used as materials were weighted and mixed in the proportions shown in table 2 to prepare two samples of powder mixture. Then, the resulting powder mixtures were compacted into pellets, the resulting each pellet was wrapped with a gold foil and was sintered at a temperature of 870 °C for 12 hours. The resulting two samples of oxide superconductors were found that they contained compound oxide represented by the general formula: (Tl (1.p) Bi p ) y Ba s Ca z Cu v O w in which "y", "z", "v", "w", "p" and "s" are numbers each satisfying respective range of 0.5 ≤ y ≤ 3.0, 0.5 ≤ z ≤ 4.0, 1.0 ≤ v ≤ 5.0, 5 ≤ w ≤ 15.0, 0 ≤ p ≤ 1.0 and 0.5 ≤ s ≤ 3.0. On the resulting oxide superconductors, the critical temperature and the critical current density at liquid nitrogen temperature were measured and X-ray diffraction charts were obtained in order to check phases produced. For a comparison, a comparative superconducting material was prepared by sintering a powder mixture containing solely of Ti 2 O 3 , BaO 2 , CaO and CuO and the superconducting properties were determined by the same method as above. Table 2 shows the ratios of elements in the material powder mixture, the superconducting properties and the crystal structure (phase) determined by X-ray diffraction analysis including the value "y" in the general formula. From the Table 2, it is apparent that the oxide superconducting material show much higher critical current density Jc than the known oxide superconducting material while same or even higher critical temperature Tc is observed. Composition of the powder mixture Phase obtained y Tci (K) Jc (A/cm 2 ) Tl Bi Ba Ca Cu Example 1.4 0.6 2 2 3 a = 3.85x10 -10 m a = (3.85 Å) c = 15.8x10 -10 m c = (15.8 Å) tetragonal system same as above 2 110 400 1.6 0.4 2 2 3 2 115 450 Comparative 2 -- 2 2 3 a = 3.85x10 -10 m a = (3.85 Å) c = 35.8x10 -10 m c = (35.8 Å) -- 112 270 Note: Tci is a temperature where perfect zero resistance was observed Example 3 A plurality of oxide superconducting materials were prepared by the following process Powders of Tl 2 O 3 , Bi 2 O 3 , PbO, CaO, SrO and CuO (purity is higher than 99.9 %) used as materials were weighted and mixed in the proportions shown in Table 3, Table 4 and Table 5 to prepare powder mixture samples. Then, the resulting powder mixture samples were compacted into pellets. The resulting each pellet was wrapped with a gold foil and was sintered at a temperature of 870 °C for 12 hours. All of the resulting oxide superconductors were found that they contained compound oxide represented by the general formula: (Tl (1-p) Bi p ) y Sr s Ca z Cu v O w in which "y", "z", "v", "w", "p" and "s" are numbers each satisfying respective range of 0.5 ≤ y ≤ 3.0, 0.5 ≤ z ≤ 4.0, 1.0 ≤ v ≤ 5.0, 5 ≤ w ≤ 15.0, 0 ≤ p ≤ 1.0 and 0.5 ≤ s ≤ 3.0, or compound oxide represented by the general formula: (Tl (1-P-q) Bi p Pb q ) y Sr s Ca z Cu v O w in which "y", "z", "v" "w" "p" "q" and "s" are numbers each satisfying respective range of 0.5 ≤ y ≤ 3.0, 0.5 ≤ z ≤ 4.5, 1.0 ≤ v ≤ 5.0, 5.0 ≤ w ≤ 15.0, 0 ≤ p ≤ 1.0, 0 ≤ q ≤ 0.6 and 0.5 ≤ s ≤ 3.0. On the resulting oxide superconductors, the critical temperature and the critical current density at liquid nitrogen temperature were measured and X-ray diffraction charts were obtained in order to check phases produced.' The value "y" in the general formula was also determined in several samples. From these experimental data, it was confirmed that a novel layered crystal structure of a tetragonal system having a mixed layer of Tl and Bi or a mixed layer of Tl and Pb was produced in the resulting oxide superconductor. From the analysis of the proportion of the phase obtained by X-ray diffraction chart, it was concluded that this novel phase contributes to a superconducting phase. For a comparison, the same test as above was repeated for comparative superconducting materials which were prepared by sintering a powder mixture containing solely of Bi 2 O 3 , SrO, CaO and CuO and a powder mixture containing solely of Bi 2 O 3 , SrO, CaO, CuO and PbO. The ratios in the material powder mixture and the results of tests are also summarized in Table 3, 4 and 5. Fig. 10 shows a temperature dependency of electric resistance measured on the sample No. 1. Fig. 6 shows a X-ray diffraction chart obtained from the sample No. 6. Fig. 11 and 12 show a temperature dependency of magnetic susceptibility and a temperature dependency of electric resistance obtained from the sample No. 6 respectively. All of the oxide superconducting materials show much higher critical current density Jc than the known oxide superconducting material while same or even higher critical temperature Tc is observed. Composition of the powder mixture Sample No Tl Bi Pb Sr Ca Cu Tci (K) Jc (A/cm 2 ) Example I (1) 0.8 0.2 -- 2 2 3 115 900 (2) 0.7 0.3 -- 2 2 3 100 450 (3) 0.6 0.4 -- 2 2 3 105 550 (4) 0.4 0.6 -- 2 2 3 100 500 (5) 0.2 0.8 -- 2 2 3 98 400 (6) 1 1 -- 2 2 3 105 780 (7) 0.6 0.3 0.1 2 2 3 108 650 (8) 0.56 0.24 0.2 2 2 3 110 700 (9) 0.42 0.18 0.4 2 2 3 113 750 (10) 0.35 0.15 0.5 2 2 3 110 680 (11) 0.28 0.12 0.6 2 2 3 108 650 (12) 0.21 0.09 0.7 2 2 3 80 90 Note: Tci is a temperature where perfect zero resistance was observed. The phase obtained was a tetragonal system having the lattice constant of a = 3.8x10 -10 m (3.8 Å) and c = 15.3x10 -10 m (15.3 Å) in all samples prepared. Composition of the powder mixture Sample No Tl Bi Pb Sr Ca Cu Tci (K) Jc (A/cm 2 ) Comparative Example I (13) 0.9 0.1 -- 2 2 3 78 10 (14) 0.1 0.9 -- 2 2 3 80 100 (15) 0 2 -- 2 2 3 80 90 (16) 1 0 -- 2 2 3 75 -- (17) 0 1.6 0.4 2 2 3 103 120 Note: Tci is a temperature where perfect zero resistance was observed Composition of the powder mixture Sample No Tl Bi Pb Sr Ca Cu Tci (K) Jc (A/cm 2 ) Example II (18) 0.7 0.3 -- 2 1 2 86 120 (19) 0.6 0.4 -- 2 1 2 90 150 (20) 0.4 0.6 -- 2 1 2 85 120 (21) 0.2 0.8 -- 2 1 2 85 120 (22) 0.6 0.3 0.1 2 1 2 95 300 Comparative Example II (23) 0.9 0.1 -- 2 1 2 78 10 (24) 0.1 0.9 -- 2 1 2 78 20 (25) 0 2 -- 2 1 2 78 20 (26) 1 0 -- 2 1 2 75 -- (27) 0 1.6 0.4 2 1 2 90 180 Note: Tci is a temperature where perfect zero resistance was observed Composition of the powder mixture -- Sample No Bi Tl Pb Sr Ca Cu Lattice constant (Å) (10 -10 m) y Tci (K) Jc (A/cm 2 ) Example III (28) 1.2 0.8 -- 2 2 3 a = 3.8 a = (3.8 Å) c = 15.3 c = (15.3 Å) tetragonal 2 100 450 (29) 0.8 1.2 -- 2 2 3 same as above 2 105 550 (30) 1.0 0.6 0.4 2 2 3 a = 3.8 a = (3.8 Å) c = 15.8 c = (15.8 Å) 2 110 500 Comparative Example III (31) 2 -- -- 2 2 3 a = 5.41 a = (5.41 Å) c = 36.8 c = (36.8 Å) -- 78 10 (32) 1.6 0.4 -- 2 2 3 a = 5.41 a = (5.41 Å) c = 36.8 c = (36.8 Å) -- 103 120 Note: Tci is a temperature where perfect zero resistance was observed Example 4 (not part of the invention, technical information only). Oxide superconducting materials according to the present invention were prepared by the process according to the present invention. Powders of Tl 2 O 3 , CaO, BaO 2 , Cs 2 CO 3 and CuO (purity is higher than 99.9 %) used as materials were weighted and mixed in the proportions shown in Table 6 to prepare five samples of powder mixture. Then, the resulting powder mixtures were compacted into pellets. The resulting each pellet was wrapped with a gold foil and was sintered at a temperature of 850 °C for 12 hours in oxygen gas stream. For a comparison, a comparative superconducting material was prepared by sintering a powder mixture containing the same materials except Cs 2 CO 3 . The resulting all samples of oxide superconductors were found that they contained compound oxide represented by the general formula: Tl y Ca z (Ba (1-r) Cs r ) s Cu v O w in which "y", "z", "v", "w", "r" and "s" are numbers each satisfying respective range of 0.5 ≤ y ≤ 3.0, 0.5 ≤ z ≤ 4.0, 2.0 ≤ v ≤ 5.0, 5.0 ≤ w ≤ 15.0, 0 ≤ r ≤ 0.8 and 0.5 < s ≤ 3.0. On the resulting oxide superconductors, the critical temperature Tc and the critical current density Jc at liquid nitrogen temperature were measured. The results are summarized in Table 6. All of the oxide superconducting materials according to the present invention show much higher critical current density Jc than known oxide superconducting material while same or even higher critical temperature Tc is observed. Composition of the powder mixture Sample No Tl Ca Ba Cs Cu Tci (K) Jc (A/cm 2 ) Comparative 2 2 2.0 -- 3 110 300 (1) 2 2 1.95 0.05 3 113 280 (2) 2 2 1.8 0.2 3 116 350 (3) 2 2 1.0 1.0 3 116 400 (4) 2 2 0.4 1.6 3 117 450 (5) 2 2 0.2 1.8 3 -- -- Example 5 (not part of the invention, technical information only) Oxide superconducting materials according to the present invention were prepared by the same process as Example 4 except that Bi 2 O 3 and PbO were added additionally. The resulting oxide superconductor was evaluated by the same method as Example 4. Table 7 shows the composition of the material powder and the properties of the resulting oxide superconductor. The resulting oxide superconducting material was found that it contained compound oxide represented by the general formula: (Tl (1-p-q) Bi p Pb q ) y Ca z (Ba (1-r) Cs r ) s Cu v O w in which "y", "z", "v", "w", "p", "q", "r" and "s" are numbers each satisfying respective range of 0.5 ≤ y ≤ 3.0, 0.5 ≤ z ≤ 4.0, 2.0 ≤ v ≤ 5.0, 5.0 ≤ w ≤ 15.0, 0 ≤ p ≤ 0.5, 0 ≤ q ≤ 0.5, 0 ≤ r ≤ 0.8 and 0.5 ≤ s ≤ 3.0. This oxide superconducting material according to the present invention shows much higher critical current density Jc than known oxide superconducting material while same or even higher critical temperature Tc is observed. Composition of the powder mixture Sample No Tl Bi Pb Ca Ba Cs Cu Tci (K) Jc (A/cm 2 ) (6) 1.6 0.2 0.2 2 1 1 3 116 350 Example 6 (not part of the invention, technical information only) Oxide superconducting materials according to the present invention were prepared by the same process as Example 4 except that BaO 2 is replaced by SrO 2 . The resulting oxide superconductor was evaluated by the same method as Example 4. Table. 8 shows the composition of the material powder and the properties of the resulting oxide superconductor. All of the resulting oxide superconducting materials were found that they contained compound oxide represented by the general formula: Tl y Ca z (Sr (1-r) Cs r ) s Cu v O w in which "y", "z", "v", "w", "r" and "s" are numbers each satisfying respective range of 0.5 ≤ y ≤ 3.0, 0.5 ≤ z ≤ 4.0, 2.0 ≤ v ≤ 5.0, 5.0 ≤ w ≤ 15.0, 0 ≤ r ≤ 0.8 and 0.5 ≤ s ≤ 3.0. These oxide superconducting materials according to the present invention show much higher critical current density Jc than known oxide superconducting material while same or even higher critical temperature Tc is observed. Composition of the powder mixture Sample No Tl Ca Sr Cs Cu Tci (K) Jc (A/cm 2 ) Comparative 2 2 2.0 -- 3 70 -- (7) 2 2 1.95 0.05 3 72 -- (8) 2 2 1.8 0.2 3 100 280 (9) 2 2 1.0 1.0 3 105 400 (10) 2 2 0.4 1.6 3 103 350 (11) 2 2 0.2 1.8 3 -- -- Example 7 (not part of the invention, technical information only) Oxide superconducting material according to the present invention was prepared by the same process as Example 6 except that Bi 2 O 3 and PbO were added additionally. The resulting oxide superconductor was evaluated by the same method as Example 6. Table. 9 shows the composition of the material powder and the properties of the resulting oxide superconductor. The resulting oxide superconducting material was found that it contained compound oxide represented by the general formula: (Tl (1-p-q) Bi p Pb q ) y Ca z (Sr (1-r) Cs r ) s Cu v O w in which "y", "z", "v", "w", "p", "q", "r" and "s" are numbers each satisfying respective range of 0.5 ≤ y ≤ 3.0, 0.5 ≤ z ≤ 4.0, 2.0 ≤ v ≤ 5.0, 5.0 ≤ w ≤ 15.0, 0 ≤ p ≤ 0.5, 0 ≤ q ≤ 0.5, 0 ≤ r ≤ 0.8 and 0.5 ≤ s ≤ 3.0. The oxide superconducting material according to the present invention show much higher critical current density Jc than known oxide superconducting material while same or even higher critical temperature Tc is observed. Sample No Composition of the powder mixture Tci (K) Jc (A/cm 2 ) Tl Bi Pb Ca Sr Cs Cu (12) 1.6 0.2 0.2 2 1 1 3 108 380

Claims: Superconducting oxide material, characterized in that it contains compound oxide having a composition represented by the formula : (Tl (1-p-q) Bi p Pb q ) 1 Sr 2 Ca 2 Cu 3 O w in which "p" , "q" and "w" are numbers each satisfying 0.12 ≤ p ≤ 0.3 ; 0.1 ≤ q ≤ 0.6 ; and 5 ≤ w ≤ 15. A process for preparing the superconducting oxide material set forth in claim 1, characterized by the step of mixing powders containing Tl, Bi, Pb, Sr, Ca and Cu in proportions of Tl : Bi : Pb : Ca : Sr : Cu = h : i : j : k : l : n in which "h", "i", "j", "k", "l", and "n" are numbers each satisfying 0 < h < 3.0 ; 0 < i < 3.0 ; 0 < j < 3.0 ; 0.5 ≤k ≤4.0; 0.5 ≤1 ≤3.0 and 2.0 ≤n.

Inventors: KUSUHARA HIROYOKI, TORRI YASUKO, KUSUHARA, HIROYOKI, TORRI, YASUKO
Applicants: SUMITOMO ELECTRIC INDUSTRIES, SUMITOMO ELECTRIC INDUSTRIES, LTD.
Application year: 1989
Main classification: H01L39
IPC codes: H01L39, C04B35