Abstract

The total cross sections for excitation transfer between the 62P1/2and 62P3/2levels in cesium, induced by collisions of the second kind between cesium and inert gas atoms, have been determined using methods of sensitized fluorescence. The experiments were carried out at a cesium vapor pressure of 1 × 10−6 mm Hg, at which there is no trapping of resonance radiation, and over a range of inert gas pressures extending from 1 to 300 mm Hg. The cross sections Q1(2P1/2 → P3/2) and Q2(2P1/2 ← 2P3/2) are as follows: Cs–He: 5.7 × 10−21and 3.9 × 10−20 cm2; Cs–Ne: 1.9 × 10−21and 3.1 × 10−20 cm2; Cs–A: 1.6 × 10−21and 5.2 × 10−20 cm2; Cs–Kr: 8.3 × 10−21and 18.4 × 10−20 cm2; Cs–Xe: 7.2 × 10−21and 27.4 × 10−20 cm2. A mechanism for the excitation transfer is suggested, which involves an interaction between the inert gas atoms and the 62P electron in cesium, behaving as a free particle.

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