Abstract:
The present invention provides an oxide superconductor which is mainly composed of bismuth, lead, strontium, calcium, magnesium, and copper and has the composition represented by the formula: 
     
       Bi.sub.1-A Pb.sub.A Sr.sub.1-B Mg.sub.B Ca.sub.1 Cu.sub.1.7±0.3 Ox 
     
     wherein A=0.15-0.35 and B=0.05-0.3 in which numerals represent atomic ratio and an oxide superconductor which is mainly composed of bismuth, lead, strontium, calcium, magnesium, barium and copper and has the composition represented by the formula: 
     
       Bi.sub.1-A Pb.sub.A Sr.sub.1-(B+C) (Mg.sub.B Ba.sub.C)Ca.sub.1 
     
      Cu 1 .7±0.3 Ox 
     wherein A=0.15-0.35, B=0.05-0.3 and C=0.02-0.2 in which numerals represent atomic ratio. Methods for producing these superconductors are also provided.

Description:
This application is a continuation of application Ser. No. 556,448, filed on Jul. 24, 1990 now abandoned. 
    
    
     BACKGROUND OF THE INVENTION 
     The present invention relates to oxide superconductors and process for production thereof. 
     As conventional oxide superconductors, generally known are Bi--Sr--Ca--Cu--O superconductors mainly composed of bismuth, strontium, calcium and copper which was found by Maeda, general research worker, and others of National Research Institute for Metals on Jan. 20, 1988, and Bi--Sr--Ca--Mg--Cu--O oxide superconductors mainly composed of bismuth, strontium, calcium, magnesium and copper, Bi--Pb--Sr--Ca--Cu--O oxide superconductors mainly composed of bismuth, lead, strontium, calcium and copper, and Bi--Pb--Sr--Ca--Ba--Cu--O oxide superconductors mainly composed of bismuth, lead, strontium, calcium, barium and copper which are obtained by substitution of elements of the above-mentioned Bi--Sr--Ca--Cu--O oxide superconductors. 
     However, the above Bi--Sr--Ca--Cu--O oxide superconductors suffer from the problems in that high temperature phase where critical temperature at which electrical resistance becomes zero (hereinafter referred to as &#34;T C   ZERO  &#34;) is about 110 K is formed with difficulty and intermediate temperature phase of T C   ZERO  being about 80 K and heterogeneous phases differing in crystal or composition are apt to be formed. Bi--Sr--Ca--Mg--Cu--O oxide superconductors comprising Bi--Sr--Ca--Cu--O to which Mg is added have a defect in that T C   ZERO  decreases with addition of Mg as shown, for example, in &#34;Japanese Journal of Applied Physics&#34;, Vol. 27, No. 12 (December, 1988), pages L2330-L2332. 
     In case of Bi--Pb--Sr--Ca--Cu--O oxide superconductors which comprise Bi--Sr--Ca--Cu--O to which Pb is added, high temperature phase is easily formed, but they have defects in that range of firing temperature for forming the high temperature phase is narrow and intermediate temperature phase tends to remain. In case of Bi--Pb--Sr--Ca--Ba--Cu--O oxide superconductors which comprise Bi--Pb--Sr--Ca--Cu--O to which Ba is added, T C   ZERO  rises with addition of Ba, but there is a defect in that heterogeneous phases such as BaCuO 2  and BaBiO 3  which are different from the desired high temperature phase are produced. 
     SUMMARY OF THE INVENTION 
     The object of the present invention is to provide an oxide superconductor in which high temperature phase can be readily formed and substantially no heterogeneous phases are formed and which has a high critical current density (Jc), and a process for producing it. 
     The present invention provides an oxide superconductor which comprises, as main components, bismuth, lead, strontium, calcium, magnesium and copper and has the composition represented by the formula (I): 
     
         Bi.sub.1-A Pb.sub.A Sr.sub.1-B Mg.sub.B Ca.sub.1 Cu.sub.1.7±0.3 Ox(I) 
    
     wherein A=0.15-0.35 and B=0.05-0.3, where numerals represent atomic ratio. 
     The present invention further provides a process for producing an oxide superconductor which comprises weighing starting materials containing bismuth, lead, strontium, calcium, magnesium and copper, respectively so as to obtain the composition shown by the above formula (I), primarily mixing the starting materials containing bismuth, strontium, calcium, magnesium and copper, calcining and grinding the mixture, adding a starting material containing lead to the ground product, secondarily mixing them, and firing the mixture. 
     The present invention further provides an oxide superconductor which comprises, as main components, bismuth, lead, strontium, calcium, magnesium, barium and copper and which has the composition represented by the formula (II): 
     
         Bi.sub.1-A Pb.sub.A Sr.sub.1-(B+C) (Mg.sub.B Ba.sub.C)Ca.sub.1 Cu.sub.1.7±0.3 Ox                                      (II) 
    
     wherein A=0.15-0.35, B=0.05-0.3, and C=0.02-0.2, where the numerals represent atomic ratio. 
     The present invention additionally provides a process for producing an oxide superconductor which comprises weighing starting materials containing bismuth, lead, strontium, calcium, magnesium, barium and copper, respectively so as to obtain the composition represented by the above formula (II), then primarity mixing the starting materials containing bismuth, strontium, calcium, magnesium, barium and copper, respectively, calcining and grinding the mixture, adding a starting material containing lead to the ground product, secondarily mixing them and firing the mixture. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a graph which shows relation between diffraction peak intensity ratio and firing temperature and 
     FIG. 2 shows relation between superconductor content at 77 K and firing temperature. 
    
    
     DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     There are no limitations in starting materials containing bismuth, lead, strontium, calcium, magnesium, and copper which are main components constituting the oxide superconductor of the present invention and starting material containing barium and, for example, at least one of oxide, carbonate, nitrate, and oxalate is used. 
     In the formula: 
     
         Bi.sub.1-A Pb.sub.A Sr.sub.1-B Mg.sub.B Ca.sub.1 Cu.sub.1.7±0.3 Ox(I) 
    
     subscript A is atomic ratio and is within the range of 0.15-0.35. When the atomic ratio is less than 0.15, intermediate temperature phase is readily formed to result in reduction of amount of high temperature phase formed and when it is more than 0.35, heterogeneous phase such as oxide of lead and calcium (Ca 2  PbO 4 ) is formed in a large amount and critical temperature decreases. 
     Subscript B is atomic ratio and is within the range of 0.05-0.3. When the atomic ratio is less than 0.05, range of firing condition for formation of high temperature phase is narrow and besides, it is difficult to make electrical resistance stably zero at about 110 K and when it is more than 0.3, heterogeneous phase such as crystals other than superconductor and glass tend to be formed and T C   ZERO  decreases. 
     In the formula: 
     
         Bi.sub.1-A Pb.sub.A Sr.sub.1-(B+C) (Mg.sub.B Ba.sub.C)Ca.sub.1 Cu.sub.1.7±0.3 Ox                                      (II) 
    
     the atomic ratios of A and B are the same as above and subscript C is atomic ratio and within the range of 0.02-0.2. When the atomic ratio of C is less than 0.02, conspicuous effect cannot be obtained and when it is more than 0.2, heterogeneous phases such as BaCuO 2  and BaBiO 3  are readily formed. 
     Mixing method has no special limitation and preferred is one which comprises charging balls coated with synthetic resin, a solvent such as ethanol, methanol or the like and the starting materials in a ball mill made of synthetic resin and carrying out wet mixing. 
     After other starting materials than the starting material containing lead have been primarily mixed, calcined and ground, the starting material containing lead is added to the ground product and secondarily mixed. If the starting material containing lead is primarily mixed together with other starting materials and then the mixture is calcined, a part of lead is evaporated to result in deviation in composition and oxide superconductor of high temperature phase cannot be obtained. 
     Regarding the calcination conditions, calcination temperature is optionally chosen depending on mixing ratio of the starting materials and preferably is 780°-830° C. Calcination atmosphere is not critical and may be air atmosphere, oxygen atmosphere, vacuum atmosphere, reducing atmosphere, and the like. 
     Grinding is preferably carried out by rough grinding in an alumina mortar and then wet grinding to fine powders. Balls used for grinding have no special limitation, but preferred are those which have a large specific gravity and are excellent in wear resistance such as zirconia balls and super hard balls. 
     Regarding firing conditions, firing temperature can be optionally chosen depending on mixing ratio of the starting materials and preferably is 820°-870° C. and firing atmosphere is preferably air atmosphere, air stream, low oxygen pressure atmosphere (oxygen content: 1-20 vol %, preferably 2-10 vol %), or the like. 
     With reference to crystalline phase, the high temperature phase is one which has a crystalline phase which shows a T C   ZERO  of about 110 K and the intermediate temperature phase is one which has a crystalline phase which shows a T C   ZERO  of about 80 K. 
     In the composition of the present invention, amount of O (oxygen) determines depending on amount of Pb, amount of Cu and oxidation state of Cu. However, the oxidation state cannot severely and accurately be measured and so amount of O is expressed by x. 
     The present invention will be explained by the following examples. 
     EXAMPLE 1 
     Bismuth trioxide (purity: 99.9%, manufactured by Kojundo Kagaku Kenkyusho Co.), strontium carbonate (purity: 99.9%, manufactured by Rare Metallic Co.), magnesium oxide (purity: 99.9%, manufactured by Kojundo Kagaku Kenkyusho Co.), calcium carbonate (purity: 99.99%, manufactured by Kojundo Kagaku Kenkyusho Co.), and cupric oxide (purity: 99.9%, manufactured by Kojundo Kagaku Kenkyusho Co.) were weighed so as to obtain the atomic ratio of bismuth, strontium, magnesium, calcium, and copper as shown in the composition in Table 1. These were used as starting materials. 
     The starting materials were charged in a ball mill made of a synthetic resin together with steel balls covered with a synthetic resin and methanol and wet mixed and ground at 50 rpm for 60 hours. After drying, the resulting ground product was put on an aluminum fired plate and calcined at 800° C. for 12 hours in the air atmosphere using an electric furnace and roughly ground in a mortar. Then, the roughly ground product, zirconia balls, methanol, and lead monoxide (yellow) (special grade: manufactured by Wako Pure Chemical Industries, Ltd.) weighed so as to obtain the atomic rate as shown in the composition in Table 1 were charged in a ball mill of a synthetic resin and wet ground at 50 rpm for 24 hours and then, the ground product was dried to obtain a composition for oxide superconductor. This composition was press molded in a mold under a pressure of 147 MPa. Thereafter, Sample Nos. 1-3 were fired in the air for 80 hours at a firing temperature shown in Table 1 and Sample Nos. 4-20 were fired in a low oxygen pressure atmosphere of O 2  :N 2  =1:10 in volume ratio for 80 hours at a firing temperature shown in Table 1 to obtain oxide superconductors of 1 mm thick. 
     The resulting oxide superconductors were processed into rectangular parallelopipeds of 20 mm length×3 mm width×1 mm thickness. Change of electrical resistance with temperature was measured by four terminal method and T C   ZERO  was obtained. The results are shown in Table 1. 
     Each of the oxide superconductors was ground in a mortar into powders and rate of change of inductance was measured and content of superconductor at 77 K was obtained. The results are shown in Table 1. 
     Separately, each of oxide superconductors of Sample Nos. 4, 5, 18 and 20 was again ground in a mortar and then press molded in a mold under a pressure of 196 MPa and subsequently, the resulting molded product was refired for 24 hours at firing temperature shown in Table 1 in the same low oxygen pressure atmosphere as used above to obtain again oxide superconductor. This was processed into a rectangular parallelopiped and critical current density (Jc) was measured at the temperature of liquid nitrogen (77.3 K) by four terminal method. The results are shown in Table 2. 
     
                                           TABLE 1__________________________________________________________________________                                           Firing SuperconductorSample                     Crystalline phase identified                                           temperature                                                  contentNo. Composition       T .sub.c.sup.zero  (K)                      X-ray diffraction peak                                           (°C.)                                                  at 77K (vol__________________________________________________________________________                                                  %)*1  Bi.sub.1 Sr.sub.1 Ca.sub.1 Cu.sub.1.5 Ox                  72  Intermediate temperature phase, Ca.sub.2                      CuO.sub.3,           875     0                      high temperature phase*2  Bi.sub.1 S.sub.0.9 Mg.sub.0.1 Ca.sub.1 Cu.sub.1.5 Ox                  70  Intermediate temperature phase,                                           875     0*3  Bi.sub.1 Sr.sub.0.7 Mg.sub.0.3 Ca.sub.1 Cu.sub.2 Ox                  62  Intermediate temperature phase,                                           875,    0                      unidentifiable peak*4  Bi.sub.0.5 Pb.sub.0.2 Sr.sub.1 Ca.sub.1 Cu.sub.1.8 Ox                 106  High temperature phase, intermediate                                           845    63                      temperature phase*5  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.1 Ca.sub.1 Cu.sub.1.4 Ox                 105  High temperature phase, intermediate                                           845    62                      temperature phase, Ca.sub.2 PbO.sub.4*6  Bi.sub.0.8 Pb.sub.0.2 Sr.sub.1 Ca.sub.1 Cu.sub.2 Ox                 106  High temperature phase, intermediate                                           850    59                      temperature phase*7  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.7 Ba.sub.0.3 Ca.sub.1 Cu.sub.1.6                 103  High temperature phase, BaCuO.sub.2,                      BaBiO.sub.3,         825    57                      unidentifiable peak*8  Bi.sub.0.75 Pb.sub.0.25 Sr.sub.0.75 Ba.sub.0.25 Ca.sub.1 Cu.sub.1.8    Ox                106  High temperature phase, BaCuO.sub.2,                      BaBiO.sub.3          830    61 9  Bi.sub.0.85 Pb.sub.0.15 Sr.sub.0.9 Mg.sub.0.1 Ca.sub.1 Cu.sub.1.8                 108  High temperature phase                                           835    9010  Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.55 Mg.sub.0.15 Ca.sub.1 Cu.sub.2                 109  High temperature phase                                           830    8511  Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.7 Mg.sub.0.3 Ca.sub.1 Cu.sub.2                 108  High temperature phase                                           820    83*12 Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.65 Mg.sub.0.35 Ca.sub.1 Cu.sub.2                  84  Intermediate temperature phase,                                           820h   39                      temperature phase, unidentifiable peak*13 Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.97 Mg.sub.0.03 Ca.sub.1 Cu.sub.2                 106  High temperature phase, intermediate                                           840    61                      temperature phase14  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.9 Mg.sub.0.1 Ca.sub.1 Cu.sub.1.6                 109  High temperature phase                                           840    8915  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.75 Mg.sub.0.25 Ca.sub.1 Cu.sub.1.6                 110  High temperature phase                                           830    92*16 Bi.sub.0.9 Pb.sub.0.1 Sr.sub.0.9 Mg.sub.0.1 Ca.sub.1 Cu.sub.1.6                  88  Intermediate temperature phase                                           840    17*17 Bi.sub.0.6 Pb.sub.0.4 Sr.sub.0.9 Mg.sub.0.1 Ca.sub.1 Cu.sub.1.6                  63  Intermediate temperature phase, Ca.sub.2                      PbO.sub.4,           830    42                      Unidentifiable peak, High temperature phase18  Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.8 Mg.sub.0.2 Ca.sub.1 Cu.sub.1.8                 110  High temperature phase                                           830    8419  Bi.sub.0.75 Pb.sub.0.25 Sr.sub.0.8 Mg.sub.0.2 Ca.sub.1 Cu.sub.1.8                 109  High temperature phase                                           825    8220  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.8 Mg.sub.0.2 Ca.sub.1 Cu.sub.1.8                 110  High temperature phase                                           820    80__________________________________________________________________________ Mark * means samples which are not covered by the present invention. &#34;Unidentifiable peak&#34; shows that there exists indefinite crystalline phase. 
    
     
                       TABLE 2______________________________________      Sample No.      *4   *5         18     20______________________________________Jc (A/cm.sup.2)        620    430        1810 1630______________________________________ Mark * means samples which are not covered by the present invention. 
    
     The results shown in Tables 1 and 2 show that in the oxide superconductors in examples of the present invention, heterogeneous phases are not formed and they are higher in T C   ZERO  and Jc than those of comparative examples and besides, in the superconductors of the present invention, much high temperature phase is formed and content of superconductor at 77 K is high. 
     EXAMPLE 2 
     Bismuth trioxide (purity: 99.9%, manufactured by Kojundo Kagaku Kenkyusho Co.), strontium carbonate (purity: 99.9%, manufactured by Rare Metallic Co.), magnesium oxide (purity: 99.9%, manufactured by Kojundo Kagaku Kenkyusho Co.), barium carbonate (purity: 99.9%, manufactured by Wako Pure Chemical Industries, Ltd.), calcium carbonate (purity: 99.99%, manufactured by Kojundo Kagaku Kenkyusho Co.), and cupric oxide (purity: 99.9%, manufactured by Kojundo Kagaku Kenkyusho Co.) were weighed so as to obtain the atomic ratio of bismuth, strontium, magnesium, barium, calcium, and copper as shown in the composition in Table 3. These were used as starting materials. 
     Thereafter, compositions for oxide superconductor were obtained in the same manner as in Example 1 except that lead was added in such as amount as giving the atomic ratio as shown in Table 3. 
     Each of the resulting compositions was press molded in a mold under a pressure of 147 MPa. Thereafter, Sample Nos. 1-3 were fired in the air for 80 hours at the firing temperature as shown in Table 3 and Sample Nos. 4-22 were fired in a low oxygen pressure atmosphere of O 2  :N 2  =1:10 in volume ratio for 80 hours at the firing temperature as shown in Table 3 to obtain oxide superconductors of 1 mm thick. 
     The resulting oxide superconductors were processed into rectangular parallelopipeds of the same size as in Example 1 and then, T C   ZERO  was obtained in the same manner as in Example 1. The results are shown in Table 3. 
     Each of the oxide superconductors was ground in a mortar into powders and rate of change of inductance was measured and content of superconductor at 77 K was obtained. The results are shown in Table 3. 
     Separately, each of oxide superconductors of Sample Nos. 4, 5, 7, and 11 was again ground in a mortar and then press molded in a mold under a pressure of 196 MPa and subsequently, the resulting molded product was refired for 24 hours at the firing temperature as shown in Table 3 in the same low oxygen pressure atmosphere as used above to obtain again oxide superconductor. This was processed into a rectangular parallelopiped of the same size as in Example 1 and critical current density (Jc) was measured at the temperature of liquid nitrogen (77.3 K) by four terminal method. The results are shown in Table 4. 
     
                                           TABLE 3__________________________________________________________________________                                           Firing SuperconductorSample                      Crystalline phase identified                                           temperature                                                  contentNo. Composition        T .sub.c.sup.zero  (K)                       X-ray diffraction peak                                           (°C.)                                                  at 77K (vol__________________________________________________________________________                                                  %)*1  BiSr.sub.1 Ca.sub.1 Cu.sub.1.5 Ox                   72  Intermediate temperature phase,                                           875     0                       Ca.sub.2 CuO.sub.3, high temperature phase*2  Bi.sub.1 S.sub.0.9 Mg.sub.0.1 Ca.sub.1 Cu.sub.1.5 Ox                   70  Intermediate temperature phase,                                           875     0*3  Bi.sub.1 Sr.sub.0.7 Mg.sub.0.3 Ca.sub.1 Cu.sub.2 Ox                   62  Intermediate temperature phase,                                           875,    0                       unidentifiable peak*4  Bi.sub.0.8 Pb.sub.0.2 Sr.sub.1 Ca.sub.1 Cu.sub.1.8 Ox                  106  High temperature, phase intermediate                                           845    63                       temperature phase*5  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.1 Ca.sub.1 Cu.sub.1.4 Ox                  105  High temperature phase, intermediate                                           845    62                       temperature phase, Ca.sub.2 PbO.sub.4*6  Bi.sub.0.9 Pb.sub.0.1 Sr.sub.0.8 Mg.sub.0.1 Ba.sub.0.1 Ca.sub.1    Cu.sub.1.8 Ox       88  High temperature phase, intermediate                                           835    52                       temperature phase 7  Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.8 Mg.sub.0.1 Ba.sub.0.1 Ca.sub.1    Cu.sub.1.8 Ox      110  High temperature phase                                           830    86 8  Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.8 Mg.sub.0.05 Ba.sub.0.15 Ca.sub.1    Cu.sub.1.8 Ox      108  High temperature phase                                           830    83*9  Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.6 Mg.sub.0.1 Ba.sub.0.3 Ca.sub.1    Cu.sub.1.8 Ox      105  High temperature phase, BaCuO.sub.2,                       BaBiO.sub.3         830    60*10 Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.55 Mg.sub.0.4 Ba.sub.0.05 Ca.sub.1    Cu.sub.1.8 Ox       95  High temperature phase, intermediate                                           830    52                       temperature phase, unidentifiable peak11  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.85 Mg.sub.0.1 Ba.sub.0.05 Ca.sub.1    Cu.sub.1.8 Ox      109  High temperature phase                                           830    8212  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.9 Mg.sub.0.05 Ba.sub.0.05 Ca.sub.1    Cu.sub.1.8 Ox      109  High temperature phase                                           835    85*13 Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.7 Ba.sub.0.3 Ca.sub.1 Cu.sub.1.6                  103  High temperature phase, BaCuO.sub.2,                                           825    62                       BaBiO.sub.3, Unidentifiable peak14  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.7 Mg.sub.0.2 Ba.sub.0.1 Ca.sub.1    Cu.sub. 1.6 Ox     110  High temperature phase                                           825    8915  Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.6 Mg.sub.0.3 Ba.sub.0.1 Ca.sub.1    Cu.sub.1.6 Ox      107  High temperature phase                                           825    9116  Bi.sub.0.8 Pb.sub.0.2 Sr.sub.0.9 Mg.sub.0.05 Ba.sub.0.05 Ca.sub.1    Cu.sub.1.8 Ox      109  High temperature phase                                           835    84*17 Bi.sub.0.7 Pb.sub.0.3 Sr.sub.0.6 Mg.sub.0.35 Ba.sub.0.05 Ca.sub.1    Cu.sub.1.8 Ox       90  High temperature phase, Intermediate                                           825    59                       temperature phase, Unidentifiable peak18  Bi.sub.0.75 Pb.sub.0.25 Sr.sub.0.93 Mg.sub.0.05 Ba.sub.0.02 Ca.sub.1    Cu.sub.1.8 Ox      108  High temperature phase                                           840    87*19 Bi.sub.0.75 Pb.sub.0.25 Sr.sub.0.75 Ba.sub.0.25 Ca.sub.1 Cu.sub.1.8    Ox                 106  High temperature phase, BaCuO.sub.2,                       BaBiO.sub.3         830    6120  Bi.sub.0.75 Pb.sub.0.28 Sr.sub.0.8 Mg.sub.0.15 Ba.sub.0.05 Ca.sub.1    Cu.sub.1.8 Ox      110  High temperature phase                                           830    88*21 Bi.sub.0.6 Pb.sub.0.4 Sr.sub.0.8 Mg.sub.0.1 Ba.sub.0.1 Ca.sub.1    Cu.sub.1.8 Ox       65  Intermediate temperature phase,                                           830    53                       Ca.sub.2 PbO.sub.4, unidentifiable peak*22 Bi.sub.0.8 Pb.sub.0.2 Sr.sub.1 Ca.sub.1 Cu.sub.2 Ox                  106  High temperature phase, intermediate                                           850    59                       temperature phase__________________________________________________________________________ Mark * means samples which are not covered by the present invention. &#34;Unidentifiable peak&#34; shows that there exists indefinite crystalline phase. 
    
     
                       TABLE 4______________________________________      Sample No.      *4   *5         7      11______________________________________Jc (A/cm.sup.2)        620    432        1840 1690______________________________________ Mark * means samples which are not covered by the present invention. 
    
     The results shown in Table 3 and 4 show that in the oxide superconductors obtained in examples of the present invention, heterogeneous phases are not formed and they are higher in T C   ZERO  and Jc than those of comparative examples and besides, in the superconductors of the present invention, much high temperature phase is formed and content of superconductor at 77 K is high. 
     EXAMPLE 3 
     Each of the oxide superconductors of Sample Nos. 4 and 18 obtained in Example 1 and Sample No. 7 obtained in Example 2 was ground in a mortar to obtain Samples A, B and C in the form of powder. 
     Samples A, B and C were subjected to powder X-ray diffraction and diffraction peak intensity ratio was obtained using the following formula: ##EQU1## Relation between diffraction peak intensity ratio and firing temperature is shown in FIG. 1. 
     Furthermore, rate of change of inductance of the above Samples A, B and C was measured and content of superconductor at 77 K was obtained. The results are shown in FIG. 2. 
     FIGS. 1 and 2 show that Samples B and C obtained using the oxide superconductors according to the examples of the present invention contain much high temperature phase and range of firing temperature for obtaining much high temperature phase is broad. 
     In the oxide superconductor of the present invention, high temperature phase is readily formed and range of firing temperature for forming much high temperature phase is broad, and substantially no heterogeneous phase is formed. Thus, this superconductor is high in T C   ZERO  and Jc and is industrially very suitable.