Coexistence of superconductivity and ferromagnetism in 1212-Ru1-xMxSr2GdCu2O8 (M=Ti, V, Nb)

被引:15
|
作者
Malo, S
Ko, DG
Rijssenbeek, JT
Maignan, A [1 ]
Pelloquin, D
Dravid, VP
Poeppelmeier, KR
机构
[1] Univ Caen, ISMRA, Lab CRISMAT, UMR 6508, F-14032 Caen, France
[2] Northwestern Univ, Sci & Technol Ctr Superconduct, Evanston, IL 60208 USA
[3] Northwestern Univ, Dept Chem, Evanston, IL 60208 USA
[4] Northwestern Univ, Dept Mat Sci & Engn, Evanston, IL 60208 USA
[5] Northwestern Univ, Ctr Mat Res, Evanston, IL 60208 USA
来源
基金
美国国家科学基金会;
关键词
superconductivity; ferromagnetism; cuprates; ruthenium;
D O I
10.1016/S1466-6049(00)00075-1
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
The coexistence of superconductivity and ferromagnetism in 1212-RuSr2GdCu2O8 is unique among high-T-c materials. Samples of Ru1-xMxSr2GdCu2O8, with M=Ti, V and Nb; and 0 less than or equal tox less than or equal to1, were prepared to elucidate the role of the RuO2 planes in this interesting layered 1212 cuprate. The solubility ranges of M =Ti and V are limited to x<0.15 whereas that of Nb extends to full substitution. In all cases superconductivity is lost at higher substitution levels (x>0.2), however with vanadium substitution the T-c increases from 20 K to 25 K. The ferromagnetism of the RuO2 layers is dramatically affected by the electronic configuration of the substituting ion, weakened for M=Ti and Nb and enhanced for M=V. These results indicate that the superconductivity and ferromagnetism are intimately linked to the layered architecture of this 1212 structure. (C) 2000 Elsevier Science Ltd. All rights reserved.
引用
收藏
页码:601 / 608
页数:8
相关论文
共 50 条
  • [1] Electrical and magnetic properties of Ru1-xMxSr2GdCu2O8 (M = Ti, V and Nb)
    Rijssenbeek, JT
    Mansourian-Hadavi, N
    Malo, S
    Ko, D
    Washburn, C
    Maignan, A
    Pelloquin, D
    Mason, TO
    Poeppelmeier, KR
    PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 2000, 341 (341-348): : 481 - 482
  • [2] On the coexistence in RuSr2GdCu2O8 of superconductivity and ferromagnetism
    Weht, R
    Shick, AB
    Pickett, WE
    HIGH TEMPERATURE SUPERCONDUCTIVITY, 1999, 483 : 141 - 146
  • [3] Pressure effects on the superconductivity and magnetization in (Ru1-xMx)Sr2GdCu2O8 (M = Nb, V)
    Yamada, Yuh
    Hamada, H.
    Shimada, M.
    Kubo, S.
    Matsushita, A.
    JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS, 2004, 272 : E173 - E174
  • [4] Coexistence of ferromagnetism and superconductivity in EuSr2Ru1-xNbxCu2O8
    Feng, MB
    Fang, MH
    Xu, Z
    Jiao, ZK
    CHINESE PHYSICS LETTERS, 2001, 18 (07) : 963 - 966
  • [5] Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0≤x≤0.2)
    Hassen, A
    Hemberger, J
    Loidl, A
    Krimmel, A
    PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 2003, 400 (1-2): : 71 - 80
  • [6] Coexistence of ferromagnetism with superconductivity in RuSr2GdCu2O8 from ESR measurements
    Yoshida, K
    Nakamura, M
    Higashi, N
    Shimizu, H
    EPR IN THE 21ST CENTURY: BASICS AND APPLICATIONS TO MATERIAL, LIFE AND EARTH SCIENCES, 2002, : 151 - 156
  • [7] Superconductivity and magnetism in Ru1-xIrxSr2GdCu2O8 compounds
    Torikachvili, MS
    Bossi, I
    O'Brien, JR
    Fonseca, FC
    Muccillo, R
    Jardim, RF
    PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 2004, 408 : 195 - 196
  • [8] Chemical tuning of ferromagnetism and superconductivity in RuSr2GdCu2O8
    Mclaughlin, AC
    Janowitz, V
    McAllister, JA
    Attfield, JP
    CHEMICAL COMMUNICATIONS, 2000, (14) : 1331 - 1332
  • [9] Ferromagnetism and superconductivity in pure and doped RuSr2GdCu2O8
    Hemberger, J
    Hassen, A
    Krimmel, A
    Mandal, P
    Loidl, A
    PHYSICA B-CONDENSED MATTER, 2002, 312 : 805 - 807
  • [10] NMR study of ferromagnetism and superconductivity of RuSr2GdCu2O8
    Furukawa, Y
    Takada, S
    Yamanaka, A
    Kumagai, K
    PHYSICA C, 2000, 341 : 453 - 454