Effect of liquid phase mass for the production of single grain infiltration growth processed bulk YBa2Cu3Oy by YbBa2Cu3Oy+Liquid phase as a liquid source

被引:3
|
作者
Sushma, Miryala [1 ,2 ]
机构
[1] Shibaura Inst Technol, Dept Mat Sci & Engn, Superconducting Mat Lab, Koto Ku, 3-7-5 Toyosu, Tokyo 1358546, Japan
[2] Seisen Int Sch, Setagaya Ku, Chome 12-15 Yoga, Tokyo 1580097, Japan
关键词
Y-123; IG process; Yb-123+liquid (1:1.3); Critical current density; Trapped field; SUPERCONDUCTORS; FABRICATION; CEO2;
D O I
10.1016/j.matchemphys.2019.122477
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The efficient production of single grain YBa2Cu3O7-delta (Y-123) bulks via top-seeded infiltration growth (IG) process demands optimized liquid phase (in the given case a mixture of Y-123 and Ba3Cu5O8). This enables a smooth peritectic growth and results in high quality bulks. Recently, 1:1 mixture of Y-123 and Ba3Cu5O8 has been considered as an optimum. In the search for a further optimized mixture to attain a longer c-axis growth, we tested Yb-123 + Ba3Cu5O8 liquid mixture varying the liquid phase (LP) amount, i.e. Yb-123 + liquid (1:1; 1:1.2; and 1:1.3). Using these liquid phase concentrations, Y-123 blocks were isothermally grown at 995 degrees C for 50 h with following slow cooling. Single-grain Y-123 blocks of 20 mm diameter and 7 mm thickness were fabricated. We present detail properties of the bulk Y-123 prepared with the liquid source of Yb-123 +Ba3Cu5O8 (1:1.3). A sharp superconducting transition with T-c,(onset) at 90 K and critical current density (J(r)) at 77 K of around 40 kA/cm(2) and 13 kA/cm(2) in self-field and 2 T (H//c-axis), respectively, were observed. Trapped field showed a typical single cone profile with maximum value of 0.4 Tat 77 K, 0.3 mm above top centre of the bulk Y-123. It is more than triple value for the same size and a similar material reported so far for bulk Y-123 prepared with Yb-123 + Ba3Cu5O8 (1:1) as a liquid source.
引用
收藏
页数:8
相关论文
共 50 条
  • [41] Microwave magnetoabsorptions of YBa2Cu3Oy single crystal
    Tagaya, K
    Yokoo, T
    Fujita, T
    Fukuoka, N
    PHYSICA C, 1997, 281 (01): : 59 - 63
  • [43] Small angle grain boundary in YBa2Cu3Oy superconductor
    Chen, WM
    Huang, JW
    Jiang, SS
    Guo, YC
    Liu, HK
    Dou, SX
    INTERNATIONAL JOURNAL OF MODERN PHYSICS B, 1999, 13 (17): : 2285 - 2290
  • [44] QUADRUPOLE COUPLING IN SUPERCONDUCTING AND SEMICONDUCTING YBA2CU3OY AND GDBA2CU3OY
    LUTGEMEIER, H
    PIEPER, MW
    BOEHNER, W
    KOBLER, U
    HAUCK, J
    FISCHER, K
    ZUCHT, F
    RUPP, B
    EBERT, H
    PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 1988, 153 : 731 - 732
  • [45] Quadrupole coupling in superconducting and semiconducting YBa2Cu3Oy and GdBa2Cu3Oy
    Luetgemeier, H.
    Pieper, M.W.
    Boehner, W.
    Koebler, U.
    Hauck, J.
    Fischer, K.
    Zucht, F.
    Rupp, B.
    Ebert, K.
    Physica C: Superconductivity and its Applications, 1988, 153-55 (01): : 731 - 732
  • [46] Vortex phase diagram in untwinned YBa2Cu3Oy with columnar disorder
    Nishizaki, T.
    Kasuga, K.
    Takahashi, Y.
    Okayasu, S.
    Kobayashi, N.
    YAMADA CONFERENCE LX ON RESEARCH IN HIGH MAGNETIC FIELDS, 2006, 51 : 267 - +
  • [47] HARMONIC SUSCEPTIBILITIES OF A SINGLE-CRYSTAL YBA2CU3OY BULK SUPERCONDUCTOR
    YAMAMOTO, K
    MAZAKI, H
    YASUOKA, H
    TERASHIMA, T
    BANDO, Y
    JAPANESE JOURNAL OF APPLIED PHYSICS PART 1-REGULAR PAPERS SHORT NOTES & REVIEW PAPERS, 1992, 31 (03): : 770 - 774
  • [48] Phase diagram of interlayer Josephson vortices in underdoped YBa2Cu3Oy
    Nishizaki, Terukazu
    Takahashi, Yuki
    Kobayashi, Norio
    PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 2008, 468 (7-10): : 664 - 668
  • [49] Characterization of grain boundaries in YBa2Cu3Oy bicrystal junctions
    Yu, HW
    Chen, MJ
    Yang, HC
    Yang, SY
    Horng, HE
    IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, 1999, 9 (02) : 3101 - 3104
  • [50] OXYGEN ABSORPTION ISOTHERMS AND PHASE-DIAGRAM OF YBA2CU3OY
    KANEMATSU, K
    JAPANESE JOURNAL OF APPLIED PHYSICS PART 2-LETTERS, 1990, 29 (06): : L906 - L908