Abstract
We studied the decay of self-trapped excitons (STE's) in ${\mathrm{BaF}}_{2},$ ${\mathrm{SrF}}_{2},$ and ${\mathrm{CaF}}_{2}$ excited at room temperature by two-photon absorption of femtosecond laser pulses by recording time-resolved triplet-luminescence spectra. For ${\mathrm{BaF}}_{2}$ we detected significant spectral changes as a function of decay time but this effect was much less pronounced for ${\mathrm{SrF}}_{2}$ and barely to be identified in ${\mathrm{CaF}}_{2}.$ A careful analysis of ${\mathrm{BaF}}_{2}$ data revealed two principal decay times of 0.6 \ensuremath{\mu}s and approximately 4 \ensuremath{\mu}s, respectively, where the latter is actually a range of decay times correlating with photon energy within the luminescence band. We attribute this spectral characteristic to a superposition of contributions from several relaxed STE configurations while the two principal decay times are believed to result from the zero-field splitting of the ${}^{3}{\ensuremath{\Sigma}}_{u}^{+}$ state of the STE.
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