2006
DOI: 10.1016/j.tsf.2006.02.016
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Crystallinity and electrical properties of neodymium-substituted bismuth titanate thin films

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Cited by 10 publications
(5 citation statements)
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“…However, no obvious mode shift is observed in this region, showing that Nd additive stays mainly inside the perovskite units and does not incorporate into the fluorite-like layers [19,20]. Meanwhile, significant changes can be indexed at modes from 268 to 853 cm −1 with the increase of Nd doping concentration, such as the shift of the mode at 268 cm −1 , the broadening and softening of the modes at 268, 552, and 853 cm −1 , indicating the tilting and distortion in TiO 6 octahedral and more difficulties in achieving perovskite phase upon increased Nd content [17,19]. Such variation tendency would be involved to explain the retardation in crystallization as the increase of Nd content as shown in the XRD analysis.…”
Section: Tuning the Structural And Optical Properties Of Bismuth Titamentioning
confidence: 94%
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“…However, no obvious mode shift is observed in this region, showing that Nd additive stays mainly inside the perovskite units and does not incorporate into the fluorite-like layers [19,20]. Meanwhile, significant changes can be indexed at modes from 268 to 853 cm −1 with the increase of Nd doping concentration, such as the shift of the mode at 268 cm −1 , the broadening and softening of the modes at 268, 552, and 853 cm −1 , indicating the tilting and distortion in TiO 6 octahedral and more difficulties in achieving perovskite phase upon increased Nd content [17,19]. Such variation tendency would be involved to explain the retardation in crystallization as the increase of Nd content as shown in the XRD analysis.…”
Section: Tuning the Structural And Optical Properties Of Bismuth Titamentioning
confidence: 94%
“…However, only 8 Raman modes can be indexed, which can be attributed to the symmetry breaking, TiO 6 octahedron distortion, vibration modes overlap, and weak feature of some Raman peaks [16][17][18]. Raman active modes locating at 60, 90, and 121 cm −1 originate from the bismuth displacement in the pseudo-perovskite slab and (Bi 2 O 2 ) 2+ fluorite-like layers, and the modes from 268 to 853 cm −1 can be classified as internal vibration modes of TiO 6 octahedral of perovskite unit [17,19]. Moreover, the internal modes of 268 and 329 cm −1 can be attributed to the O-Ti-O bending, while the mode at 853 cm −1 is caused by the Ti-O symmetric stretching of TiO 6 octahedral, and the Raman mode at 552 and 627 cm −1 can be ascribed as the combination of bending and stretching of TiO 6 octahedral.…”
Section: Tuning the Structural And Optical Properties Of Bismuth Titamentioning
confidence: 99%
“…BNdTx thin films are sometimes reported to show optimized electrical properties, especially a larger P r value, with an intermediate x, e.g. x = 0.46, 0.75 or 0.85 [18,26,27]. We argue that this may be a compromise between the decreased P r and the simultaneously suppressed leakage current.…”
Section: Resultsmentioning
confidence: 77%
“…It is important to note that the desert flower shape is mainly constituted by the connection between plates. Chen et al showed in Bi 4−x Nd x Ti 3 O 12 films the formation of plate‐like grains that tend to elongate with the increase in Nd, becoming a rod‐like shape. Li et al showed, for Bi 2 Ti 2 O 7 crystals prepared by co‐precipitation, the formation of micro‐size ball‐like particles (ie, spheres) with irregular surface shapes, very similar to the ones observed in our samples A and B.…”
Section: Resultsmentioning
confidence: 99%