Influence of Co, Ni and Zn substitution for Cu on the structural and superconducting properties of (Hg
暂无分享,去创建一个
[1] Y. Itoh,et al. Control of T c for Ni-substituted YBa 2 Cu 3 O 7-δ by annealing treatments , 2000 .
[2] M. Gupta,et al. Effect of nickel and zinc substitutions on the electronic charge-density redistribution in a YBa 2 Cu 3 O 7 superconductor , 1999 .
[3] Y. Tokunaga,et al. Novel relation between spin-fluctuation and superconductivity in Ni substituted high-Tc cuprate YBa2Cu3O7:Cu NQR study , 1997 .
[4] M. Hervieu,et al. On the crystal structure of the “1201” superconductors Hg0.5Bi0.5Sr2−xLaxCuO5−δ , 1996 .
[5] Wang,et al. Chromium clustering and ordering in Hg1-xCrxSr2CuO4+ delta. , 1995, Physical review. B, Condensed matter.
[6] T. Meen,et al. Structure, superconductivity and magnetism of YBa2(Cu1−xMx)4O8 (MFe, Co, Ni, Zn and Ga) , 1995 .
[7] T. Deng,et al. Synthesis and study of (Hg,Cr)-based 1201-type superconducting cuprate (Hg,Cr)Sr2CuO4+δ , 1995 .
[8] H. Alloul,et al. Macroscopic magnetic properties of Ni and Zn substituted YBa2Cu3Oχ , 1994 .
[9] Klein,et al. Comparison of the influence of Ni and Zn impurities on the electromagnetic properties of YBa2Cu3O6.95. , 1994, Physical review. B, Condensed matter.
[10] Hoffman,et al. X-ray-diffraction determination of the Ni-dopant site in single-crystal YBa2Cu3O7- delta. , 1994, Physical review. B, Condensed matter.
[11] K. Kitazawa,et al. A new mercury-based superconductor: (Hg, Cr)Sr2CuOy , 1994 .
[12] Pandey,et al. Tc depression in the YBa2Cu4-xMxO8 system for M=Fe, Ni, Zn, and Ga. , 1994, Physical review. B, Condensed matter.
[13] Y. Sun,et al. Synthesis of the high-temperature superconductors HgBa2CaCu2O6+δ and HgBa2Ca2Cu3O8+δ , 1993 .
[14] K. Ishida,et al. Cu NMR and NQR Studies of Impurities-Doped YBa2(Cu1-xMx)3O7 (M=Zn and Ni) , 1993 .
[15] G. Güntherodt,et al. Structural and superconducting properties of Bi2Sr2Ca(Cu1-yCoy)2O8+δ single crystals , 1992 .
[16] T. Nakadaira,et al. Effects of substitution of Fe and Co for Cu in Bi2Sr1.8Ca1.2Cu2Oy on electronic states studied by photoemission , 1991 .
[17] Chien,et al. Magnetic pair-breaking effects: Moment formation and critical doping level in superconducting La1.85Sr0.15Cu1-xAxO4 systems (A=Fe,Co,Ni,Zn,Ga,Al). , 1990, Physical review. B, Condensed matter.
[18] Tetsuro Nakamura,et al. Superconductivity, magnetism and oxygen nonstoichiometry of Ba2Y(Cu1−xMx)3Oy (M = Zn and Ni) , 1990 .
[19] Boyce,et al. Local structure about Ni atoms in Ni-substituted YBa2Cu3O7- delta. , 1990, Physical review. B, Condensed matter.
[20] P. Etchegoin,et al. Iron doping and Mössbauer spectroscopy in Bi-Sr-Ca-Cu ceramic superconductors , 1990 .
[21] Wang,et al. Magnetic versus nonmagnetic ion substitution effects on Tc in the La-Sr-Cu-O and Nd-Ce-Cu-O systems. , 1990, Physical review. B, Condensed matter.
[22] P. Wyder,et al. Superconductivity and microstructure in Fe-doped Bi-Sr-Ca-Cu-O compounds , 1990 .
[23] S. Kulkarni,et al. Superconductivity in Ni substituted Bi2Ca1Sr2Cu2−xNixOy , 1990 .
[24] S. Yamagata,et al. Effect of Ni or Zn substitution for Cu in NdCeCuO and BiSr(Ca,Y)CuO systems , 1990 .
[25] Yabe,et al. Substitution of 3d metals for Cu in Bi2(Sr0.6Ca0.4)3Cu2Oy. , 1989, Physical review. B, Condensed matter.
[26] R. D. Boss,et al. Substitutions of 3-d transition metal ions for copper in Bi2Sr2Can−1CunO2n+4 , 1989 .
[27] Islam Ms,et al. Atomistic simulation of dopant substitution in YBa2Cu3O7. , 1989 .
[28] Bach,et al. Influence of Ni, Fe, and Zn substitution on the superconducting and antiferromagnetic state of YBa2Cu3O7- delta. , 1989, Physical review. B, Condensed matter.
[29] Scott,et al. Determination of dopant site occupancies in Cu-substituted YBa2Cu3O7- delta by differential anomalous x-ray scattering. , 1989, Physical review. B, Condensed matter.
[30] Chien,et al. Correlation between superconductivity and normal-state properties in the La1.85Sr0.15 (Cu1-xZnx)O4 system. , 1989, Physical review. B, Condensed matter.
[31] Poon,et al. Synthesis and characterization of YBa2(Cu1-xMx)3O7- delta (M=Co,Ni): Crystal symmetry, superconductivity, and the role of oxygen. , 1988, Physical review. B, Condensed matter.
[32] Greene,et al. Structural and physical properties of the metal (M) substituted YBa2Cu3-xMxO7-y perovskite. , 1988, Physical review. B, Condensed matter.
[33] H. Adrian,et al. Effect of nickel impurities on superconductivity and electrical resistivity of the high-Tc superconductor Ba2YCu3O7 , 1988 .
[34] E. Takayama-Muromachi,et al. Superconductivity of YBa2Cu3-xMxOy (M = Co, Fe, Ni, Zn) , 1987 .
[35] Orlando,et al. 3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O. , 1987, Physical review. B, Condensed matter.
[36] Y. Maeno,et al. Substitution for copper in a high-Tc superconductor YBa2Cu3O7–δ , 1987, Nature.
[37] Chien,et al. Effect of transition-metal elements on the superconductivity of Y-Ba-Cu-O. , 1987, Physical review. B, Condensed matter.
[38] Y. Maeno,et al. Superconductivity in YBa2Cu3-yNiyO7-δ , 1987 .
[39] K. Kitazawa,et al. High Tc Superconductivity of (La1-xSrx)2CuO4 –Effect of Substitution of Foreign Ions for Cu and La on Superconductivity , 1987 .
[40] N. Morton,et al. Magnetic susceptibilities of some ternary molybdenum sulphides , 1975 .
[41] A. S. Cooper,et al. High-Temperature Superconductors, the First Ternary System , 1972, Science.