Unidirectional microstructure formation of Sm-Ba-Cu-O superconductor on melting via peritectic reaction

被引:1
|
作者
Sumida, M [1 ]
Shiohara, Y [1 ]
Umeda, T [1 ]
机构
[1] ISTEC, SUPERCONDUCT RES LAB, DIV 4, TOKYO 135, JAPAN
关键词
Sm1Ba2Cu3O7-d; Sm2Ba1Cu1O5; oxide superconductor; microstructure control; unidirectional melting; partial molten mixture;
D O I
10.2320/jinstmet1952.61.9_956
中图分类号
TF [冶金工业];
学科分类号
0806 ;
摘要
In this paper, solidification microstructure control of a partial molten mixture is discussed. Since finely dispersed non-superconductive high temperature stable phase (Sm2Ba1Cu1O5, Sm211) particles in the superconductive Sm1Ba2Cu3O7-d (Sm123) can act as effective pinning centers and grain boundaries play as weak-links of electric transport, single crystalline Sm123 with finely dispersed Sm211 particles is required to improve the critical current density (J(c)). To obtain the bulk single crystalline Sm123 with fine Sm211 particles by floating-zone partial melting and the solidification method, the microstructure of the partial molten mixture (Sm211 particles and liquid) is to be controlled, because the solidification microstructure of Sm123/211 is mainly determined by that of the mixture. During unidirectional melting, the mean diameter, d(211), (or spacing, lambda) of rod-likely aligned Sm211 particles after decomposition of the precursor Sm123 decreased with increasing growth rate, R. The mean diameter d(211) became larger under P-O2=1 kPa atomsphere than that at atomspheric pressure. Based upon the experimental results, a simple model for the formation of aligned Sm211 particles via peritectic decomposition was proposed, and prediction from the model was compared with the experimental results. Effects of melting conditions on the microstructure formation of the partial molten mixture were discussed.
引用
收藏
页码:956 / 962
页数:7
相关论文
共 50 条
  • [1] HIGH-TEMPERATURE ANOMALIES IN SM-BA-CU-O SUPERCONDUCTOR
    HAJKO, V
    HUDAK, O
    MOLOKAC, S
    SEMAN, M
    TIMKO, M
    ZENTKO, A
    FIZIKA NIZKIKH TEMPERATUR, 1988, 14 (02): : 215 - 217
  • [2] Magnetic flux distribution of Sm-Ba-Cu-O bulk superconductor
    Inoue, K
    Hirabayashi, I
    Murakami, M
    PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 2004, 412 : 521 - 525
  • [3] Fabrication of Sm-Ba-Cu-O superconducting rods for current leads by unidirectional solidification
    Hayashi, A
    Kurachi, K
    Seiki, S
    Izumi, T
    Shiohara, Y
    PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 2003, 392 : 970 - 974
  • [4] Trapped field distribution within a cylindrical hole in Sm-Ba-Cu-O bulk superconductor
    Masuzawa, Mika
    Egawa, Kazumi
    Tsuchiya, Kiyosumi
    IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, 2006, 16 (02) : 1031 - 1034
  • [5] Thermodynamic study on the Sm-Ba-Cu-O system
    Xing, XR
    Qiao, ZY
    Wei, SK
    Chen, XL
    Liang, JK
    Rao, GH
    ACTA PHYSICA SINICA-OVERSEAS EDITION, 1996, 5 (11): : 857 - 862
  • [6] Partial melting in filamentary Sm-Ba-Cu-O superconductors under various oxygen atmospheres
    Ban, E
    Goto, T
    Matsuoka, Y
    PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 2003, 388 : 411 - 412
  • [7] MEASUREMENT OF INVERSE AC JOSEPHSON EFFECT IN HIGH-TC SM-BA-CU-O SUPERCONDUCTOR
    RAO, VV
    SREEKUMAR, N
    PRADHAN, AK
    MALLICK, AK
    INDIAN JOURNAL OF PURE & APPLIED PHYSICS, 1990, 28 (04) : 192 - 193
  • [8] Thermodynamic characteristics of compounds in the Sm-Ba-Cu-O system
    Matskevich, NI
    Krabbes, G
    Berasteguie, P
    THERMOCHIMICA ACTA, 2003, 397 (1-2) : 97 - 101
  • [9] Trapped field distribution on Sm-Ba-Cu-O bulk superconductor by pulsed-field magnetization
    Yanagi, Y
    Itoh, Y
    Yoshikawa, M
    Oka, T
    Hosokawa, T
    Ishihara, H
    Ikuta, H
    Mizutani, U
    ADVANCES IN SUPERCONDUCTIVITY XII, 2000, : 470 - 472
  • [10] THERMAL-PROPERTIES OF THE SUPERCONDUCTIVE SM-BA-CU-O
    MOLOKAC, S
    FLACHBART, K
    BISCHOF, J
    BELLING, A
    PHYSICA B-CONDENSED MATTER, 1990, 165 : 1205 - 1206