Abstract
Positions of satellite bands near the atomic lines of alkali metals in the presence of heavy noble gases together with the assumption of a Lennard-Jones (6-12) interaction potential and knowledge of the attractive force constant ${C}_{6}$ are used to determine the repulsive force constant ${C}_{12}$ for excited states of the alkali atoms. The formula commonly used for ${C}_{6}$ is modified and leads to an improved agreement of the calculated values for this constant with experimental measurements. The constant ${C}_{12}$, derived from satellite-band measurements, is found to rapidly increase with excitation of the alkali atom and to be nearly independent of the noblegas. The values of ${C}_{12}$ found for 82 excited states of Li, Na, K, Rb, and Cs in the presence of Kr and Xe are represented by a simple power law in the effective principal quantum number of the excited state. The expression appears to have general utility when one atom is a noble gas and the other has one or two excited electrons.
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