Abstract

Thin films of bismuth-layered perovskites such as SrBi2Ta2O9, Bi4Ti3O12 ,a ndBaBi4Ti4O15 with preferred orientations were grown by pulsed laser deposition on epitax- ial conducting LaNiO3 electrodes on single-crystalline (100) SrTiO3 or on top of epitaxial buffer layers on (100) sil- icon. A morphology and structure investigation by X-ray diffraction analysis, scanning probe microscopy, and scan- ning and transmission electron microscopy showed that the films consisted of both c-axis-oriented regions and mixed (110)-, (100)-, and (001)-oriented regions. The regions with mixed orientation featured rectangular as well as equiaxed crystalline grains protruding out of a smooth c-oriented back- ground. A closer examination revealed that the regions with mixed orientation actually consisted of a c-axis-oriented sub- layer growing directly on the epitaxial LaNiO3 electrode, on top of which the growth of either (110)-, (100)-, or (001)- oriented grains took place. Macroscopic as well as micro- scopic measurements of the ferroelectric properties of regions with pure c-orientation and of regions with mixed orienta- tions showed a clear relationship between their ferroelectric properties and their morphology and crystallographic orien- tation. In the regions with mixed orientation, the films exhib- ited saturated ferroelectric hysteresis loops with well-defined remnant polarisation Pr and coercive field Ec. The regions having c-axis orientation with a smooth surface morphology in contrast exhibited a linear P E curve with no hysteretic behaviour for SrBi2Ta2O9 and BaBi4Ti4O15 and a weak fer- roelectric behaviour for Bi4Ti3O12. This clearly showed that the ferroelectric properties of bismuth-layered ferroelectric oxides depended on the crystalline orientation of the film and that the observed ferroelectric hysteresis loops in SrBi2Ta2O9 and BaBi4Ti4O15 films were solely due to the (100)- and (110)-oriented grains. The size of the (110)- and (100)- oriented grains being of the order of 100 nm and spontaneous polarisation having been observed and switched in a con- trolled manner is a demonstration that ferroelectricity can exist in structures of submicrometer size. These results might have a technological impact due to the relevance of bismuth- layered ferroelectric oxides for the fabrication of non-volatile FeRAM memories.

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