Cargando…

Crystallization dynamics and interface stability of strontium titanate thin films on silicon

Different physical vapor deposition methods have been used to fabricate strontium titanate thin films. Within the binary phase diagram of SrO and TiO(2) the stoichiometry ranges from Ti rich to Sr rich, respectively. The crystallization of these amorphous SrTiO(3) layers is investigated by in situ g...

Descripción completa

Detalles Bibliográficos
Autores principales: Hanzig, Florian, Hanzig, Juliane, Mehner, Erik, Richter, Carsten, Veselý, Jozef, Stöcker, Hartmut, Abendroth, Barbara, Motylenko, Mykhaylo, Klemm, Volker, Novikov, Dmitri, Meyer, Dirk C.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4379435/
https://www.ncbi.nlm.nih.gov/pubmed/25844077
http://dx.doi.org/10.1107/S160057671500240X
Descripción
Sumario:Different physical vapor deposition methods have been used to fabricate strontium titanate thin films. Within the binary phase diagram of SrO and TiO(2) the stoichiometry ranges from Ti rich to Sr rich, respectively. The crystallization of these amorphous SrTiO(3) layers is investigated by in situ grazing-incidence X-ray diffraction using synchrotron radiation. The crystallization dynamics and evolution of the lattice constants as well as crystallite sizes of the SrTiO(3) layers were determined for temperatures up to 1223 K under atmospheric conditions applying different heating rates. At approximately 473 K, crystallization of perovskite-type SrTiO(3) is initiated for Sr-rich electron beam evaporated layers, whereas Sr-depleted sputter-deposited thin films crystallize at 739 K. During annealing, a significant diffusion of Si from the substrate into the SrTiO(3) layers occurs in the case of Sr-rich composition. This leads to the formation of secondary silicate phases which are observed by X-ray diffraction, transmission electron microscopy and X-ray photoelectron spectroscopy.