Abstract LaxSr1−xCoO3(LSCO) (0<x<0·5) has attracted much attention recently because of its applications as electrodes for fuel cells and for ferroelectric memories. In this paper, the microstructure of LSCO grown on MgO(001) by metal-organic chemical vapour deposition has been analysed by transmission electron microscopy. The LSCO film is dominated by an ordered anisotropic perovskite-type structure, denoted as new La0·5Sr0·5CoO3 (n-LSCO). This structure is the result of lattice substitution between La and Sr. The atomic model of the structure is determined for the first time. The LSCO film is composed of domains exhibiting a [001], [010] and/or [100] directional anisotropic n-LSCO structure. Numerous stacking faults with displacement vector of 1/4[011] have been observed. The stacking faults are confined in the (100) and (010) planes and are produced by the [100] and [010] steps respectively on the MgO(001) substrate. The (010) and (100) interplanar distances in LSCO are constrained owing to lattice mismatch between LSCO and MgO and the presence of (010) and (100) planar stacking faults.
Thermal treatment of self-assembled FePt nanoparticles reduces the interparticle distances, resulting in dramatic changes in the type and strength of interparticle interactions. Consequently, magnetic properties such as the hysteresis and magnetization reversal mechanisms are strongly affected. It is suggested that controlled annealing of self-assembled nanoparticles may offer a novel approach for producing hard magnetic nanocomposites.
An effective approach is demonstrated for growing large-area, hexagonally patterned, aligned ZnO nanorods. The synthesis uses a catalyst template produced by a self-assembled monolayer of submicron spheres and guided vapor-liquid-solid (VLS) growth on a single crystal alumina substrate. The ZnO nanorods have uniform shape and length, align vertically on the substrate, and are distributed according to the pattern defined by the catalyst template. The nanorods grow along [0001] with side surfaces defined by {21̄1̄0}. This approach opens the possibility of creating patterned one-dimensional nanostructures for applications as sensor arrays, piezoelectric antenna arrays, optoelectronic devices, and interconnects.