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The shift and the broadening of Ag λλ3280 and 3382 produced by argon and helium for pressures up to 83.3 atmospheres at about 950^∘{}C were determined. The shift of Pb 2833 was also measured under the same conditions. Argon produces a red shift and a slight red asymmetry, while helium produces a violet shift and a very slight violet asymmetry for all these lines. The ²P1/2 component of silver resonance lines is shifted more than the ²P3/2 component. The relative difference in the shift is much more pronounced for helium than for argon. For helium the ²P1/2 component is shifted about six times greater than the ²P3/2 component.Both the shift and the broadening appear to be linear with the relative density for argon or helium. The ²P1/2 component produces a shift of 0.289 cm^-1 (red) per unit relative density of argon, and of 0.131 cm^-1 (violet) per unit relative density of helium. The corresponding figures for the ²P3/2 component are 0.248 cm^-1 (red) and 0.023 cm^-1 (violet) per unit r.d. Shifts for Pb 2833 are respectively 0.388 cm^-1 (red) and 0.188 cm^-1 (violet) per unit r.d. for argon and helium.There is no significant difference between the half-widths of the doublet components of the silver lines for helium. They are broadened 0.466 cm^-1 per unit r.d. For argon the ²P3/2 component is broadened slightly more than the ²P1/2 component. The ²P1/2 and the ²P3/2 components are broadened respectively 0.468 cm^-1 and 0.560 cm^-1 per unit r.d. The optical collision diameters as calculated from the half-widths turn out to be 6.50A for He-Ag and 11.3A for A-Ag.
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Clayton et al. (1952) studied this question.
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