PHASE-RELATIONS AND HOMOGENEITY REGION OF THE HIGH-TEMPERATURE SUPERCONDUCTING PHASE (BI,PB)(2)SR2CA2CU3O10+D

被引:19
作者
KAESCHE, S
MAJEWSKI, P
ALDINGER, F
机构
[1] Pulvermetallurgisches Laboratorium, Max-Planck-Institut für Metallforschung, Stuttgart, D-70569
关键词
BI-PB-SR-CA-CU-O; HIGH-T-C SUPERCONDUCTOR; PHASE RELATIONS;
D O I
10.1007/BF02652992
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
For the nominal composition of Bi2.27-xPbxSr2Ca2Cu3O10+d, the lead content was varied from x = 0.05 to 0.45. The compositions were examined between 800 and 890 degrees C which is supposed to be the temperatue range over which the so-called 2223 phase (Bi2Sr2Ca2Cu3O10+d) is stable. Only compositions between x = 0.18 to 0.36 could be synthezised in a single phase state. For x > 0.36, a lead-containing phase with a stoichiometry of Pb-4(Sr,Ca)(5)CuOd with a small solubiliy of Bi is formed, for x < 0.18 mainly Bi2Sr2CaCu2O8+d and cuprates are the equilibrium phases. The temperature range for the 2223 phase was found to be 800 to 890 degrees C but the 2223 phase has extremely varying cation ratios over this temperaure range. Former single phase 2223 samples turn to multiphase samples when annealed at slightly higher or lower temperaures. A decrease in the Pb solubility with increasing as well as decreasing temperature with a maximum at about 850 degrees C was found for the 2223 phase.
引用
收藏
页码:1829 / 1834
页数:6
相关论文
共 18 条
[1]   STUDIES OF OXYGEN-DEFICIENT BA2YCU3O7-DELTA AND SUPERCONDUCTIVITY BI(PB)-SR-CA-CU-O [J].
CAVA, RJ ;
BATLOGG, B ;
SUNSHINE, SA ;
SIEGRIST, T ;
FLEMING, RM ;
RABE, K ;
SCHNEEMEYER, LF ;
MURPHY, DW ;
VANDOVER, RB ;
GALLAGHER, PK ;
GLARUM, SH ;
NAKAHARA, S ;
FARROW, RC ;
KRAJEWSKI, JJ ;
ZAHURAK, SM ;
WASZCZAK, JV ;
MARSHALL, JH ;
MARSH, P ;
RUPP, LW ;
PECK, WF ;
RIETMAN, EA .
PHYSICA C, 1988, 153 :560-565
[2]   2223 PHASE FORMATION IN BI(PB)-SR-CA-CU-O .1. THE ROLE OF CHEMICAL-COMPOSITION [J].
CHEN, YL ;
STEVENS, R .
JOURNAL OF THE AMERICAN CERAMIC SOCIETY, 1992, 75 (05) :1142-1149
[3]   2223 PHASE FORMATION IN BI(PB)-SR-CA-CU-O .3. THE ROLE OF ATMOSPHERE [J].
CHEN, YL ;
STEVENS, R .
JOURNAL OF THE AMERICAN CERAMIC SOCIETY, 1992, 75 (05) :1160-1166
[4]   2223 PHASE FORMATION IN BI(PB)-SR-CA-CU-O .2. THE ROLE OF TEMPERATURE - REACTION-MECHANISM [J].
CHEN, YL ;
STEVEN, R .
JOURNAL OF THE AMERICAN CERAMIC SOCIETY, 1992, 75 (05) :1150-1159
[5]   COMPOSITION DEPENDENCE ON THE SUPERCONDUCTING PROPERTIES OF BI-PB-SR-CA-CU-O [J].
ENDO, U ;
KOYAMA, S ;
KAWAI, T .
JAPANESE JOURNAL OF APPLIED PHYSICS PART 2-LETTERS, 1989, 28 (02) :L190-L192
[6]   A NEW HIGH-TC OXIDE SUPERCONDUCTOR WITHOUT A RARE-EARTH ELEMENT [J].
MAEDA, H ;
TANAKA, Y ;
FUKUTOMI, M ;
ASANO, T .
JAPANESE JOURNAL OF APPLIED PHYSICS PART 2-LETTERS, 1988, 27 (02) :L209-L210
[7]   THE PB SOLUBILITY OF THE BI-BASED HIGH-TC SUPERCONDUCTORS BI2SR2CACU2O8 AND BI2SR2CA2CU3O10 AS A FUNCTION OF TEMPERATURE [J].
MAJEWSKI, P ;
KAESCHE, S ;
SU, HL ;
ALDINGER, F .
PHYSICA C, 1994, 221 (3-4) :295-298
[8]   BISRCACUO HIGH-TC SUPERCONDUCTORS [J].
MAJEWSKI, P .
ADVANCED MATERIALS, 1994, 6 (06) :460-469
[9]   THE PHASE-EQUILIBRIA OF BI2SR2CA2CU3O10 IN THE SYSTEM BI2O3-SRO-CAO-CUO [J].
MAJEWSKI, P ;
HETTICH, B ;
SCHULZE, K .
PHYSICA C, 1991, 185 :469-470
[10]   PREPARATION OF UNLEADED BI2SR2CA2CU3O10 [J].
MAJEWSKY, P ;
HETTICH, B ;
SCHULZE, K ;
PETZOW, G .
ADVANCED MATERIALS, 1991, 3 (10) :488-491