An experimental study of laser-induced collisional energy transfer in a mixture of europium and strontium vapors is reported. The profile of the excitation spectrum in the static wing has been measured with high accuracy and compared with available calculations, demonstrating that simple two-level models are inadequate to describe the transfer process. A comparison with the predictions of a three-level model assuming dipole-dipole interaction, recently developed by Bambini and Berman, shows for the first time agreement between theory and experiment.
Quenching and excitation-transfer processes involving the
32P and
32D states of the Li atom are studied in a temperature-controlled heat-pipe oven with the use of two-step laser excitation of the
42S state followed by radiative cascade towards the
32P state. Numerical identification of the collision-induced $3^{2}D\ensuremath{\rightarrow}2^{2}P$ fluorescence with a three-level model allows the determination of radiative coefficients and collisional rate coefficients.
42S,
32D, and
32P radiative lifetimes are found to be in agreement with accepted values. Quenching and excitation transfer strongly depend on the colliding atoms. Rate coefficients for the $3^{2}D\ensuremath{\rightarrow}3^{2}P$ excitation processes induced by Li, He, and Ne ground-state atoms are measured in the ratio 1.05: 0.23: 0.02 expressed in ${10}^{\ensuremath{-}9}$ ${\mathrm{sec}}^{\ensuremath{-}1}$
cm3.
We discuss a scheme suitable for the study of strong-field effects on the excitation spectrum of the laser-induced collisional energy-transfer process. The use of a weak radiation field, to induce the interatomic transition, and a strong radiation field, to modify the energy-level position, is found to give rise to a splitting of the resonance peak. The position and the relative intensity of the two spectral components are strongly dependent on the intensity and detuning of the strong field. Line-shape calculations performed for the Eu-Sr system show that the effect is expected to be detectable even for moderate intensities of the strong field.