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Phys. Rev. B 39, 6667–6680 (1989)

Microstructure, lattice parameters, and superconductivity of YBa2(Cu1-xFex)3O7-δ for 0≤x≤0.33

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Youwen Xu, M. Suenaga, J. Tafto, R. L. Sabatini, and A. R. Moodenbaugh
Department of Applied Science, Brookhaven National Laboratory, Upton, New York 11973

P. Zolliker
Department of Physics, Brookhaven National Laboratory, Upton, New York 11973

Received 14 November 1988; published in the issue dated 1 April 1989

Iron was substituted for copper in YBa2(Cu1-xFex)3O7-δ for 0≤x≤0.33. Superconducting transition temperatures and lattice parameters have been determined as a function of Fe content. The orthorhombic distortion Δa0=2(b-a)/(a+b) decreased to zero near x=0.03. Beyond x=0.03 the structure appears tetragonal. For compositions 0≤x≤0.15 the superconducting critical temperature Tc decreased smoothly from Tc=90 K to below 4.2 K. Transmission electron microscopy (TEM) revealed that the spacing between the twin boundaries decreased from ∼200 nm for x=0 to ∼20 nm for x=0.02 before the twins disappeared for x>=0.03. The sharp streaks in TEM diffraction patterns were interpreted as due to the twin boundary layers whose thickness varied from ∼1 nm for the pure to ∼2 nm for the Fe (x=0.02) containing specimen. A tweed structure in the TEM image and associated diffuse streaks along the 〈110〉 directions in electron diffraction pattern appeared for x>0.015. This observation suggests that the structure consists of fine (<5 nm) orthorhombic domains, each domain having the twinlike crystallographic relation with its neighbors. Rietveld refinement of powder neutron diffraction for x=0.10 and 0.167 determined that Fe substituted primarily on the Cu ‘‘chain’’ site, and for every two atoms of Fe substituted, approximately one extra oxygen is incorporated in the Cu-O plane.

© 1989 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.39.6667
DOI:
10.1103/PhysRevB.39.6667
PACS:
74.70.Vy, 61.16.Di, 61.70.Ng, 61.60.+m