Crystal growth of (Bi,Pb)2Sr2CaCu2Oz and their superconducting properties

[1]  M. Takano,et al.  Two-Phase Microstructures Generating Efficient Pinning Centers in the Heavily Pb-Substituted Bi2Sr2CaCu2O8+δSingle Crystals , 1998 .

[2]  H. Faqir,et al.  Growth of high-quality Bi_2Sr_2CaCu_2O_z crystal and characterization , 1997 .

[3]  T. Watanabe,et al.  Anisotropic Resistivities of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+δ: Systematic Study on “Spin Gap” Effect , 1997 .

[4]  Lei Shi,et al.  Variations of normal state resistivity and Cu2+ localized spin moment in the single crystal Bi2Sr2 CaCU2O8 + x , 1997 .

[5]  H. Faqir,et al.  Influence of the initial conditions on crystal growth of the Bi2Sr2CaCu2Oy superconductor , 1997 .

[6]  P. Fournier,et al.  Growth and annealing of (Bi1−xPbx)2Sr2CaCu2O8+δ single crystals , 1996 .

[7]  B. Mettout,et al.  Influence of lead substitution on the magnetic irreversibility line of 2212 superconducting single crystals , 1994 .

[8]  T. Yasuda,et al.  Effects of oxygen non-stoichiometry on the anisotropic resistivity in Bi2Sr2CaCu2O8+x , 1993 .

[9]  Fleming,et al.  Normal-state transport properties of Bi2+xSr2-yCuO6+ delta crystals. , 1990, Physical review. B, Condensed matter.

[10]  K. Ando,et al.  Structural modulation and superconducting properties in Bi2-xPbxSr2CaCu2O8+d and Bi2-yPbySr2YCu2O8+d , 1989 .

[11]  G. Tendeloo,et al.  Models for the modulation in A2B2CanCu1+nO6+2n, A, B=Bi, Sr OR Tl, Ba and n=0, 1, 2 , 1988 .

[12]  Wang,et al.  Out-of-plane conductivity in single-crystal YBa2Cu , 1988, Physical review. B, Condensed matter.

[13]  Zou,et al.  "Normal" tunneling and "normal" transport: Diagnostics for the resonating-valence-bond state. , 1988, Physical review letters.