Abstract
WAVELENGTH measurements, which are part of an accurate determination of the speed of light1, have been made on the radiation from a carbon dioxide laser, stabilised to the R(12) transition at 9.3 µm by saturated fluorescence in an external CO2 cell, which has a measured frequency2 reproducible to better than one part in 109. The problems of a direct intercomparison of infrared and visible wavelengths were avoided by mixing the CO2 radiation with light from a 10-mW He–Ne laser at 0.63 µm to give a difference frequency sideband at a wavelength of 0.68 µm. This mixing process, known as up-conversion, was performed in a cooled, single crystal of proustite3,4. The wavelength of the CO2 radiation was then determined using the relationship λ9.3 = λ0.63/(1—R), in which it is assumed that c is the same for the two visible radiations. The wavelength measurements were thus of the ratio R = λ0.63/λ0.68 and the value of λ0.63 with respect to the primary length standard.
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