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article
Structural transformations during formation of quasi-amorphous BaTiO 3
Abstract
<p>A model of structural transformations of amorphous into quasi-amorphous BaTiO<sub>3</sub> is suggested. The model is based on previously published data and on X-ray photoelectron spectroscopy data presented in the current report Both amorphous and quasi-amorphous phases of BaTiO<sub>3</sub> are made up of a network of slightly distorted TiO<sub>6</sub> octahedra connected in three different ways: by apices (akin to perovskite), edges, and faces. Ba ions in these phases are located in the voids between the octahedra, which is a nonperovskite environment. These data also suggest that Ba ions compensate electrical-charge imbalance incurred by randomly connected octahedra and, thereby, stabilize the TiO<sub>6</sub> network. Upon heating, the edge-to-edge and face-to-face connections between TiO<sub>6</sub> octahedra are severed and then reconnected via apices. Severing the connections between TiO<sub>6</sub> octahedra requires a volume increase, suppression of which keeps some of the edge-to-edge and face-to-face connections intact. Transformation of the amorphous thin films into the quasi-amorphous phase occurs during pulling through a steep temperature gradient. During this process, the volume increase is inhomogeneous and causes both highly anisotropic strain and a strain gradient. The strain gradient favors breaking those connections, which aligns the distorted TiO<sub>6</sub> octahedra along the direction of the gradient. As a result, the structure becomes not only anisotropic and non-centrosymmetric, but also acquires macroscopic polarization. Other compounds may also form a quasi-amorphous phase, providing that they satisfy the set of conditions derived from the suggested model.</p>