欢迎登录材料期刊网

材料期刊网

高级检索

A series of oxygen-doped RE2CuO4 (RE=Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm) was synthesized using high-pressure/oxygen-doped technique. The structures and low temperature magnetic properties were investigated. The XRD patterns indicate that the structures of high oxygen pressure RE2CuO4 (only for RE=Sm, Eu) samples are pure T' phase, but when RE= Gd, Tb, Dy, Ho, Er, Tm, the structures turn to disorder. The magnetic anomalies that occurred at T~30 K are observed in high oxygen pressure RE2CuO4. It is found that the transition temperatures of weak ferromagnetic anomalies are nearly independent of the rare-earth components. Thus, the O-doping plays an important role in anomalous magnetic properties of RE2CuO4+δ. The magnetic anomalies in RE2CuO4 are considered to be due to ferromagnetic clusters formed in the Cu-O plane after the oxygen doping.

参考文献

[1] Tokura Y;Fujimori A;Matsubara H et al.Electron and hole doping in Nd-based cuprates with single-layer CuO2 sheets: Role of doped Ce ions and 30-K superconductivity[J].Physical Review B,1989,39:9704.
[2] Tokura Y;Takagi, H;Watabe H et al.New family of layered copper oxide compounds with ordered cations: Prospective high-temperature superconductors[J].Physical Review B,1989,40:2568.
[3] Hundley M F;Thompson J D;Cheong S W et al.Bulk superconductivity above 30 K in T·-phase compounds[J].Physical Review B,1989,40:5251.
[4] Sutjahja IM.;Diantoro M.;Tjia MO.;Gelders H.;Menovsky AA. Franse JJM.;Nugroho AA. .Single crystal growth of T*-phase SmLa0.8Sr0.2CuO4[J].Physica, C. Superconductivity and its applications,2001(1):25-30.
[5] Fisk Z;Cheong S W;Thompson J D et al.T·-phase superconductivity[J].PHYSICA C,1989,162-164:1681.
[6] Cheong S W;Fisk Z;Thompson J D et al.Systematics of new T·-phase superconductivity[J].PHYSICA C,1989,159:407.
[7] Tokura Y;Takagi H;Uchida S .A superconducting copper oxide compound with electrons as the charge carriers[J].Nature,1989,337:345.
[8] Adelmann P;Ahrens R;Czjzek G et al.Structure and rare-earth magnetism in (Nd1-xGdx)2CuO4[J].Physical Review B,1992,46:3619.
[9] Tovar M;Obradors X;Pérez F et al.Weak ferromagnetism and spin-glass-like behavior in the rare-earth cuprates R2CuO4 (R=Tb, Dy, Ho, Er, Tm, and Y)[J].Physical Review B,1992,45:4729.
[10] Bordet P;Capponi J J;Chailout C et al.High pressure synthesis and structural study of R2CuO4 compounds with R=Y, Tb, Dy, Ho, Er, Tm[J].PHYSICA C,1991,185-189:539.
[11] Laguna M L;Sanjuán M.L;Butera A et al.Raman study of T'-phase distortion in R2CuO4 compounds (R=Nd, Sm, Eu, Gd)[J].Physical Review B,1993,48:7565.
[12] Steren L B;Tovar M;Oseroff S B .Boundary for weak ferromagnetism in Sm2-xGdxCuO4 solid solutions[J].Physical Review B,1992,46:2874.
[13] Luo HM.;Lin BN.;Chi YP.;Lee TJ.;Ku HC.;Hsu YY. .Correlation between weak ferromagnetism and crystal symmetry in Gd2CuO4-type cuprates[J].Physical Review.B.Condensed Matter,1999(18):13119-13124.
[14] Meen TH. .Structural and magnetic properties of (R1-xYx)(1.85)Ce0.15CuO4 (R = Pr, Nd, Sm and Eu)[J].Japanese journal of applied physics,2000(6A):3366-3370.
[15] Luo HM.;Hsu YY.;Lin BN.;Ku HC.;Ding SY. .Weak ferromagnetism in distorted T '-phase cuprates[J].Physica, C. Superconductivity and its applications,2001(2):91-96.
[16] Zhigadlo ND.;Kimoto K.;Isobe M.;Matsui Y.;Takayama-Muromachi E. .High-pressure synthesis, crystal structure and magnetic properties of a new cuprate (Nd,Ce)2+xCaCu(2)O6+y[J].International Journal of Quantum Chemistry,2003(1):24-29.
[17] Yang H D;Meen T H;Chen Y C .Occurrence of weak ferromagnetism in T'-(R1-xYx)2CuO4 (R=Sm and Eu)[J].Physical Review B,1993,48:7720.
[18] Zakharov AA.;Parfionov OE.;Nikonov AA. .Phase separation and weak ferromagnetism in lightly-oxygen-doped La2CuO4+x single crystals in low magnetic fields[J].Physical Review.B.Condensed Matter,1998(6):R3233-R3236.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%