R.J. Gambino, N.R. Stemple, et al.
Journal of Physics and Chemistry of Solids
Oxygen-deficient perovskites NdCuO3−δ (0 ≤ δ ≤ 0.5) were prepared for the first time at high pressures in a multianvil apparatus and characterized by X-ray and electron diffraction and by electron microprobe. Several new oxygen vacancy-order phases could be stabilized depending upon δ and synthetic conditions. The crystal structures of NdCuO3−δ are related to those previously observed in the LaCuO3−δ system, but are more highly distorted due to the smaller Nd cation size, leading to different symmetries, A-site coordination numbers and unit cell dimensions. Electron diffraction shows that NdCuO2.5 crystallizes in an orthorhombic √2ap × 2√2ap × ap subcell with a 6√2ap × 4√2ap × 2ap supercell, where ap is the simple cubic perovskite lattice parameter. NdCuO2.6 crystallizes in a monoclinic √5ap × √5ap × 2ap cell. In addition, two other phases with √10ap × √10ap × 2ap and √5ap × 2√5ap × 2ap have been observed for δ = 0.3–0.4, each exhibiting superstructures related to NdCuO2.6. Oxygen vacancy ordering models are proposed to interpret these results. An orthorhombic GdFe03-type phase with δ = 0–0.07, the first example of this structure-type in the rare earth cuprates, was found at the highest oxygen pressures investigated. The major structure-types, corresponding to δ = 0.07, 0.4, and 0.5, were refined by the Rietveld method. It was not possible to synthesize other LnCuO3−δ phases for rare earths smaller than Nd at pressures up to 150 kbar. Superconductivity was not observed in any of the new perovskites down to 4.2 K. © 1995, American Chemical Society. All rights reserved.
R.J. Gambino, N.R. Stemple, et al.
Journal of Physics and Chemistry of Solids
J. Paraszczak, J.M. Shaw, et al.
Micro and Nano Engineering
Elizabeth A. Sholler, Frederick M. Meyer, et al.
SPIE AeroSense 1997
A. Gangulee, F.M. D'Heurle
Thin Solid Films