Journal
MATERIALS
Volume 16, Issue 18, Pages -Publisher
MDPI
DOI: 10.3390/ma16186207
Keywords
STO; ultrathin films; Raman calculations; DFT; dependence on thickness
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This study used DFT methods to model the Raman spectra of ultra-thin strontium titanate (STO) films, revealing differences in features compared to bulk crystals and frequency shifts with increasing film thickness.
While the bulk strontium titanate (STO) crystal characteristics are relatively well known, ultrathin perovskites' nanostructure, chemical composition, and crystallinity are quite complex and challenging to understand in detail. In our study, the DFT methods were used for modelling the Raman spectra of the STO bulk (space group I4/mcm) and 5-21-layer thin films (layer group p4/mbm) in tetragonal phase with different thicknesses ranging from similar to 0.8 to 3.9 nm. Our calculations revealed features in the Raman spectra of the films that were absent in the bulk spectra. Out of the seven Raman-active modes associated with bulk STO, the frequencies of five modes (2E(g), A(1g), B-2g, and B-1g) decreased as the film thickness increased, while the low-frequency B-2g and higher-frequency E-g modes frequencies increased. The modes in the films exhibited vibrations with different amplitudes in the central or surface parts of the films compared to the bulk, resulting in frequency shifts. Some peaks related to bulk vibrations were too weak (compared to the new modes related to films) to distinguish in the Raman spectra. However, as the film thickness increased, the Raman modes approached the frequencies of the bulk, and their intensities became higher, making them more noticeable in the Raman spectrum. Our results could help to explain inconsistencies in the experimental data for thin STO films, providing insights into the behavior of Raman modes and their relationship with film thickness.
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