We present optical linewidth and line-shape studies of transitions of $4f$ impurity ions in doubly doped systems and show that interactions which involve excitation transfer between the impurity systems produce homogeneous broadening and line-shape changes in the optical transitions. In particular, we have studied the behavior of the 5985-Å line of ${\mathrm{Pr}}^{3+}$ in doubly doped La${\mathrm{F}}_3$: ${\mathrm{Pr}}^{3+}$, ${\mathrm{Nd}}^{3+}$ as a function of ${\mathrm{Nd}}^{3+}$ concentration. The 5985-Å ${\mathrm{Pr}}^{3+}$ transition at 4.2°K involves two long-lived electronic states of the ${\mathrm{Pr}}^{3+}$ ion; it follows that in the singly doped La${\mathrm{F}}_3$: ${\mathrm{Pr}}^{3+}$ the transition shows a Gaussian shape which is characteristic of inhomogeneous strain and imperfection broadening. As ${\mathrm{Nd}}^{3+}$ is added to the system, a broader Lorentzian component begins to appear in the 5985-Å ${\mathrm{Pr}}^{3+}$ transition and eventually (at ${\mathrm{Nd}}^{3+}$ concentrations of ∼1% or above) completely dominates the width and shape of the transition. The Lorentzian component of the transition line shape was successfully separated using a Fourier-transform technique and the width of this component was studied as a function of the ${\mathrm{Nd}}^{3+}$ concentration. The width is found to increase linearly with increasing ${\mathrm{Nd}}^{3+}$ concentration up to concentrations of 2%; at higher concentrations, the linewidth saturates and approaches an asymptotic value of ∼2 ${\mathrm{cm}}^{-1\mathrm{}}$. We construe this homogeneous component to be evidence of a rapid short-range energy transfer mechanism between the ${\mathrm{Pr}}^{3+}$ and ${\mathrm{Nd}}^{3+}$ systems at the terminating ${\left({}_{}{}^3{}_{}{}^{}H_6^{}{}_{}{}^{}\right)}_1$ level of the 5985-Å ${\mathrm{Pr}}^{3+}$ transition. Various mechanisms are investigated as causes of the energy transfer process; it is concluded that the spin-exchange interaction is the most probable cause for the transfer. Results of other spectroscopic measurements on the doubly doped La${\mathrm{F}}_3$: ${\mathrm{Pr}}^{3+}$, ${\mathrm{Nd}}^{3+}$ system are also presented.

Close

PrevNext

View figure in article