GROWTH AND SUPERCONDUCTIVITY OF BI2.USR1.9CA1.0(CU(1-Y)FE(Y))2O(X) SINGLE-CRYSTAL

被引:28
作者
GU, GD
TAKAMUKU, K
KOSHIZUKA, N
TANAKA, S
机构
[1] Superconductivity Research Laboratory, ISTEC, Koto-ku, Tokyo, 135, 10-13
关键词
D O I
10.1016/0022-0248(94)90986-5
中图分类号
O7 [晶体学];
学科分类号
0702 ; 070205 ; 0703 ; 080501 ;
摘要
Fe-substituted Bi-2212 single crystals in rods of Bi2.1Sr1.9Ca1.0(Cu(1-y)Fe(y))2O(x) with y less-than-or-equal-to 0.03 have been grown successfully by the floating zone method (FZM). Fe substitution in the rods depresses the growth stability of Bi-2212 crystals and consequently reduces the size of the crystals. The maximum thickness along the c-axis of the single crystals grown from a rod with y = 0 is as large as 2 mm, but only 0.4 mm for y = 0.03. The maximum Fe solubility limit of the as-grown crystals is less than 0.03 at%. Fe substitution in the crystals decreases sharply not only the superconducting transition temperature, but also the homogeneity of the superconducting phase. The rate of T(c) decrease with actual Fe-substituted content w in the crystals is as high as 16.7 K/(Fe/(Cu + Fe)) at% for the as-grown crystals of w = 0-0.01, but only 7.3 K/(Fe/(Cu + Fe)) at% for the as-grown crystals of w = 0.01-0.022 and the annealed crystals of w = 0-0.022.
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页码:472 / 478
页数:7
相关论文
共 17 条
[1]   STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA(CU1-YCOY)2O8+DELTA SINGLE-CRYSTALS [J].
BOEKHOLT, M ;
BOLLMEIER, T ;
BUSCHMANN, L ;
FLEUSTER, M ;
GUNTHERODT, G .
PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 1992, 198 (1-2) :33-41
[2]   STRUCTURAL AND MAGNETIC-PROPERTIES OF BI2SR2CACU2(1-X)FE2XO8+D [J].
CHAKRABARTY, JS ;
BHARGAVA, SC ;
JHANS, H ;
MALIK, SK .
SOLID STATE COMMUNICATIONS, 1992, 83 (09) :701-707
[3]  
CHILLIPEDDI S, 1988, PHYS REV B, V37, P7454
[4]   CRYSTAL-GROWTH AND ANNEALING EXPERIMENTS OF THE HIGH-TC SUPERCONDUCTOR BI2SR2CACU2O8+DELTA [J].
EMMEN, JHPM ;
LENCZOWSKI, SKJ ;
DALDEROP, JHJ ;
BRABERS, VAM .
JOURNAL OF CRYSTAL GROWTH, 1992, 118 (3-4) :477-482
[5]   SUBSTITUTION EFFECTS IN BI2SR2CACU2O8+DELTA [J].
FUJITA, T ;
TOMITA, T .
PHYSICA C, 1989, 162 :985-986
[6]   EFFECTS OF SUBSTITUTION OF FE AND CO FOR CU IN BI2SR1.8CA1.2CU2OY ON ELECTRONIC STATES STUDIED BY PHOTOEMISSION [J].
FUKUDA, Y ;
SANADA, N ;
NAKADAIRA, T ;
NAGOSHI, M ;
SYONO, Y ;
TACHIKI, M .
PHYSICA C, 1991, 190 (1-2) :73-74
[7]  
GINSBERG DM, 1989, PHYSICAL PROPERTIES, V1, P265
[8]   LARGE SINGLE-CRYSTAL BI-2212 ALONG THE C-AXIS PREPARED BY FLOATING ZONE METHOD [J].
GU, GD ;
TAKAMUKU, K ;
KOSHIZUKA, N ;
TANAKA, S .
JOURNAL OF CRYSTAL GROWTH, 1993, 130 (1-2) :325-329
[9]   SUPERCONDUCTIVITY IN NI SUBSTITUTED BI2CA1SR2CU2-XNIXOY [J].
KULKARNI, P ;
KULKARNI, SK ;
NIGAVEKAR, AS ;
AGARWAL, SK ;
AWANA, VPS ;
NARLIKAR, AV .
PHYSICA C, 1990, 166 (5-6) :530-534
[10]   SUBSTITUTION OF 3D METALS FOR CU IN BI2(SR0.6CA0.4)3CU2OY [J].
MAEDA, A ;
YABE, T ;
TAKEBAYASHI, S ;
HASE, M ;
UCHINOKURA, K .
PHYSICAL REVIEW B, 1990, 41 (07) :4112-4117