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

preprint1994arXivOpen access

Abstract

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), ab−ab-plane (ρabρ_{ab}) and c−c-axis (ρcρ_c) resistivity, and high resolution angle-resolved ultraviolet photoemission spectroscopy (ARUPS). TEM reveals that the modulation in the b−b-axis for Pb(0.4)−Pb(0.4)-doped Bi(Pb)−Bi(Pb)-2212 is dominantly of Pb−Pb-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 c−c-axis resistivity and a resistivity minimum at 80−13080-130K. He-annealed samples exhibit a much higher c−c-axis resistivity and dρc/dT<0dρ_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(π, π) along kx=kyk_x = k_y, and about 0.80(π,π)0.80(π, π) along kx=−kyk_x = - k_y, rather than (π,π)(π,π). The symmetry of the near-Fermi-energy dispersing states in the normal state changes between oxygen-annealed and He-annealed samples.

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