12 research outputs found

    Pb0.4Bi1.6Sr2Ca1Cu2O8+xPb_{0.4}Bi_{1.6}Sr_{2}Ca_{1}Cu_{2}O_{8+x} and Oxygen Stoichiometry: Structure, Resistivity, Fermi Surface Topology and Normal State Properties

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    Pb0.4Bi1.6Sr2CaCu2O8+xPb_{0.4}Bi_{1.6}Sr_2CaCu_2O_{8+x} (Bi(Pb)Bi(Pb)-2212) single crystal samples were studied using transmission electron microscopy (TEM), abab-plane (ρab\rho_{ab}) and cc-axis (ρc\rho_c) resistivity, and high resolution angle-resolved ultraviolet photoemission spectroscopy (ARUPS). TEM reveals that the modulation in the bb-axis for Pb(0.4)Pb(0.4)-doped Bi(Pb)Bi(Pb)-2212 is dominantly of PbPb-type that is not sensitive to the oxygen content of the system, and the system clearly shows a structure of orthorhombic symmetry. Oxygen annealed samples exhibit a much lower cc-axis resistivity and a resistivity minimum at 8013080-130K. He-annealed samples exhibit a much higher cc-axis resistivity and dρc/dT<0d\rho_c/dT<0 behavior below 300K. The Fermi surface (FS) of oxygen annealed Bi(Pb)Bi(Pb)-2212 mapped out by ARUPS has a pocket in the FS around the Mˉ\bar{M} point and exhibits orthorhombic symmetry. There are flat, parallel sections of the FS, about 60\% of the maximum possible along kx=kyk_x = k_y, and about 30\% along kx=kyk_x = - k_y. The wavevectors connecting the flat sections are about 0.72(π,π)0.72(\pi, \pi) along kx=kyk_x = k_y, and about 0.80(π,π)0.80(\pi, \pi) along kx=kyk_x = - k_y, rather than (π,π)(\pi,\pi). The symmetry of the near-Fermi-energy dispersing states in the normal state changes between oxygen-annealed and He-annealed samples.Comment: APS_REVTEX 3.0, 49 pages, including 11 figures, available upon request. Submitted to Phys. Rev. B
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