Abstract

In order to elucidate the Stark structure of ${\mathrm{Tm}}^{3+}$ multiplets involved in the \ensuremath{\approxeq}2 \ensuremath{\mu}m emission of YAG:${\mathrm{Tm}}^{3+}$, and YAG:${\mathrm{Cr}}^{3+}$,${\mathrm{Tm}}^{3+}$, absorption and emission spectra have been measured over a wide range of concentrations. The ${\mathrm{Tm}}^{3+}$ spectra in YAG show, besides the main lines assigned to dodecahedral ${\mathit{D}}_{2}$ sites, a set of satellites associated with ${\mathrm{Tm}}^{3+}$ in perturbed sites. An attempt to correlate ${\mathrm{Tm}}^{3+}$ spectra with YAG structure and structural defects has been made. Using our data and an improved algorithm we have been able to identify Stark levels of ${\mathrm{Tm}}^{3+}$ in ${\mathit{D}}_{2}$ (${\mathrm{Y}}^{3+}$) sites, especially in the $^{3}$${\mathit{F}}_{4}$, $^{3}$${\mathit{H}}_{4}$, $^{3}$${\mathit{F}}_{3}$, and $^{3}$${\mathit{F}}_{2}$ multiplets. The spectra due to ${\mathrm{Tm}}^{3+}$ in perturbed sites, with a lower symmetry, were used to assign levels corresponding to forbidden transitions in the ${\mathit{D}}_{2}$ symmetry. Some of the identified levels in $^{3}$${\mathit{H}}_{4}$ can explain the luminescence data and the cross-relaxation mechanism that lead to the population of the $^{3}$${\mathit{F}}_{4}$ metastable level, while those in $^{3}$${\mathit{F}}_{3}$ seem to play an important role in ${\mathrm{Cr}}^{3+}$-${\mathrm{Tm}}^{3+}$ energy transfer. In ${\mathrm{Cr}}^{3+}$-codoped samples supplementary lines in both ${\mathrm{Cr}}^{3+}$ and ${\mathrm{Tm}}^{3+}$ spectra as well as a preferential energy transfer have been observed and explained in terms of structural data.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call