Materials Map

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The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

The dashboard provides detailed information about the selected scientist, e.g. publications. The dashboard can be filtered and shows the relationship to co-authors in different diagrams. In addition, a link is provided to find contact information.

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The Materials Map is still under development. In its current state, it is only based on one single data source and, thus, incomplete and contains duplicates. We are working on incorporating new open data sources like ORCID to improve the quality and the timeliness of our data. We will update Materials Map as soon as possible and kindly ask for your patience.

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Publications (1/1 displayed)

  • 2007Structural transformations during formation of quasi-amorphous BaTiO 322citations

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Ehre, David
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Lyahovitskaya, Vera
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2007

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  • Ehre, David
  • Lyahovitskaya, Vera
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article

Structural transformations during formation of quasi-amorphous BaTiO 3

  • Ehre, David
  • Lyahovitskaya, Vera
  • Tagantsev, Alexander
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>

Topics
  • perovskite
  • impedance spectroscopy
  • compound
  • amorphous
  • phase
  • thin film
  • x-ray photoelectron spectroscopy
  • anisotropic
  • void