Effects of Pb doping on the Raman spectrum of Bi2Sr2CuO6+δ
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[1] Klein,et al. Raman scattering from Ag and B1g phonons in Bi2Sr2Can-1CunO2n+4 (n=1,2). , 1992, Physical review. B, Condensed matter.
[2] Y. Idemoto,et al. Oxygen nonstoichiometry and high temperature conductivity of the 2201 phase of the BiSrCuO superconducting oxide , 1992 .
[3] R. Srinivasan,et al. Superconductivity of Bi-2201 (n=1) as influenced by the substitution of Pb and/or rare-earths (R=La, Nd and Pr) , 1991 .
[4] C. Torardi,et al. Lead-doped Bi2Sr2CuO6: a superconductor free of modulation and superstructure , 1991 .
[5] K. Kosuge,et al. OVER-DOPED METALLIC BEHAVIOR OF BI2SR2CUOY : SYNTHESIS OF BI-2201 WITH STOICHIOMETRIC CATION COMPOSITION , 1991 .
[6] F. Weill,et al. Preparation and electron diffraction study of Bi2Sr2CuO6 , 1991 .
[7] Scott,et al. Raman spectra of (Bi,Pb)2Sr2CaCu2O8+y single crystals and the role of lead substitution. , 1991, Physical Review B (Condensed Matter).
[8] J. Tarascon,et al. Superconductivity at 27 K in modulation-free Bi2−xPbxSr2−yLayCuO6 phases with x≅y+0.2 , 1990 .
[9] D. Sinclair,et al. Characterisation of Incommensurate Bi2+xSr2-xCuOz by X-Ray Powder Diffraction and Oxygen Content Determinations , 1990 .
[10] J. Ziaja,et al. Effect of PbO addition on crystal structure and resistivity of the 2201 type Bi-Sr-Cu-O superconductor , 1990 .
[11] S. Kemmler‐sack,et al. Structural and electric properties of the 2201 phase in the system Bi/Pb-Sr-Cu-O , 1990 .
[12] N. Krishnamurthy,et al. Lattice vibrations in high Tc Bi2(Sr1−xCax)2CuO6+β , 1990 .
[13] Hase,et al. Physical properties of Bi2Sr2Can-1CunOy (n=1,2,3). , 1990, Physical review. B, Condensed matter.
[14] D. Ginsberg. Physical properties of high temperature superconductors IV , 1990 .
[15] M. Takano,et al. Bi, PbSrCuO system including a modulation-free superconductor , 1990 .
[16] G. Lonzarich,et al. Characterisation and transport measurements on single crystals in the Bi-Sr-Cu-O system , 1989 .
[17] Chakoumakos,et al. Effects of oxygen and strontium vacancies on the superconductivity of single crystals of Bi2Sr2-xCuO6-y. , 1989, Physical review. B, Condensed matter.
[18] Y. Nakajima,et al. Tetragonal-to-Orthorhombic Transition and Disappearance of Superconductivity in the Pb-Doped Bi2Sr2CuOy System , 1989 .
[19] S. Yamazaki,et al. The Effect of Pb Substitution on the Bi–Sr–Cu–O Superconductor , 1989 .
[20] C. Chen,et al. Modulated structure of the superconducting compounds Bi2Sr2Can-1CunOy withn=1 and 2 , 1989 .
[21] Chandrashekhar,et al. Raman-active phonons in the high-temperature superconductors and results in Bi2Sr2CuO6. , 1989, Physical review. B, Condensed matter.
[22] I. Nakai,et al. Single Crystal X-Ray Structure Analysis of Bi2(Sr, Ca)2CuOx and Bi2(Sr, Ca)3Cu2Ox Superconductors , 1988 .
[23] C. Thomsen,et al. Phonon characterization of Bi2 (Sr1-xCax)2 CuO6+δ by infrared and Raman spectroscopy , 1988 .
[24] C. Thomsen,et al. Raman scattering on superconducting crystals of Bi2(Sr1−xCax)n+2Cun+10(6+2n)+δ (n = 0, 1) , 1988 .