2 research outputs found

    Luminescence and Location of Gd<sup>3+</sup> or Tb<sup>3+</sup> Ions in Perovskite-Type LaScO<sub>3</sub>

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    The luminescence properties of Gd<sup>3+</sup> or Tb<sup>3+</sup> ions at La and Sc sites were investigated in LaScO<sub>3</sub> with a distorted perovskite-type structure (ABO<sub>3</sub>). Although the luminescence of lanthanide ions located at B sites is not common and has not been examined in detail, Gd<sup>3+</sup> or Tb<sup>3+</sup> luminescence from B sites and A sites is clearly observed in Gd<sup>3+</sup>- or Tb<sup>3+</sup>-doped LaScO<sub>3</sub>. The differences in the luminescence characteristics concern peak positions, peak shapes, and decay time, which are all influenced by the crystal field and the site symmetry. The UV luminescence of Gd<sup>3+</sup> at B sites shows a red shift compared to Gd<sup>3+</sup> at A sites, and the green luminescence of Tb<sup>3+</sup> at B sites contrasts with the blue-violet and green luminescence of Tb<sup>3+</sup> at A sites. The decay time of the luminescence from B sites is systematically longer than that from A sites in both the Gd<sup>3+</sup> and Tb<sup>3+</sup> cases

    Luminescence and Valence of Tb Ions in Alkaline Earth Stannates and Zirconates Examined by X‑ray Absorption Fine Structures

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    The difference in Tb<sup>3+</sup> green luminescence intensities in doped perovskite­(ABO<sub>3</sub>)-type alkaline earth stannates, AeSnO<sub>3</sub> (Ae = Ca, Sr, Ba), and the Mg codoping effect on the luminescence intensities in doped CaMO<sub>3</sub> (M = Sn, Zr) were investigated utilizing the X-ray absorption fine structures (XAFS) of the Tb L<sub>III</sub> absorption edge. It is considered that the local symmetry at A sites is responsible for the different Tb<sup>3+</sup> luminescence intensities in AeSnO<sub>3</sub> (Ae = Ca, Sr, Ba) doped with Tb ions at A sites. However, it was found from the XAFS spectra that some Tb ions are unintentionally stabilized at B sites as Tb<sup>4+</sup>, especially in BaSnO<sub>3</sub>. Not only the central symmetry for Tb<sup>3+</sup> at A sites but also the presence of Tb<sup>4+</sup> at B sites were considered to bring about the absence of Tb<sup>3+</sup> luminescence in doped cubic BaSnO<sub>3</sub>. No obvious changes in the Tb<sup>3+</sup> local structure at A sites were detected between Tb single doped and Tb–Mg codoped CaMO<sub>3</sub> (M = Sn, Zr) from the extended XAFS oscillation, but the trace of Tb<sup>4+</sup> at B sites in the Tb single doped sample was observed in the X-ray absorption near edge structures. It is, therefore, considered that the Tb<sup>3+</sup> luminescence enhancement by Mg codoping is primarily attributed to the charge compensation rather than the changes in the local structure around Tb<sup>3+</sup> at A sites
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