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Hydrogen motion in rutile TiO(2)

Uniaxial-stress experiments have been performed for the 3287- and 2445-cm(−1) local vibrational modes assigned to the positive charge state of interstitial hydrogen [Formula: see text] and deuterium [Formula: see text] , respectively, occurring in mono-crystalline rutile TiO2. The onset of the defec...

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Detalles Bibliográficos
Autores principales: Hupfer, A. J., Monakhov, E. V., Svensson, B. G., Chaplygin, I., Lavrov, E. V.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5719071/
https://www.ncbi.nlm.nih.gov/pubmed/29213050
http://dx.doi.org/10.1038/s41598-017-16660-3
Descripción
Sumario:Uniaxial-stress experiments have been performed for the 3287- and 2445-cm(−1) local vibrational modes assigned to the positive charge state of interstitial hydrogen [Formula: see text] and deuterium [Formula: see text] , respectively, occurring in mono-crystalline rutile TiO2. The onset of the defect alignment under the stress applied perpendicular to the [001] axis is detected at 165 K (185 K), which corresponds to the activation energy of 0.53 eV (0.58 eV) for interstitial hydrogen (deuterium). Based on these findings the diffusion constants of [Formula: see text] and [Formula: see text] along the [001] axis of TiO2 are determined. The experimental data are complemented by density-functional theory calculations and compared with the earlier results on the diffusion of [Formula: see text] /[Formula: see text] at elevated temperatures up to 700 °C. It is found that the activation energy value deduced from our low-temperature stress measurements yields a very good agreement with the high-temperature data, covering a dynamic range of 12 orders of magnitude.