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>
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
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