STRUCTURE OF THE INFRARED "ATMOSPHERIC" BANDS IN LIQUID OXYGEN
dc.creator | Cho, C. W. | en_US |
dc.creator | Allin, Elizabeth J. | en_US |
dc.creator | Welsh, H. L. | en_US |
dc.date.accessioned | 2006-06-15T12:47:30Z | |
dc.date.available | 2006-06-15T12:47:30Z | |
dc.date.issued | 1956 | en_US |
dc.identifier | 1956-H-4 | en_US |
dc.identifier.uri | http://hdl.handle.net/1811/7498 | |
dc.description | Author Institution: Department of Physics, University of Toronto | en_US |
dc.description.abstract | The $0-0, 1-0$, and 2-0 bands of the $^{1}\Delta_{g}-^{3}\Sigma_{g}$ electronic transition have been studied in liquid $O_{2}$ and in liquid $O_{2}-N_{2}$ and $O_{2}- A$ mixtures. Two cryostats were used; one enabled absorption to be observed for any path length up to 60 cm., the other for a fixed path length of 300 cm. In pure $O_{2}$ the bands are broad with their intensities degraded towards higher frequencies. On dilution of the oxygen they become sharper and the $1-0$ and $2-0$ bands show two well defined components, the stronger of which is at the band origin, $\nu_{o}$, as calculated from the constants for the free molecule. The frequency difference between the two components indicates that the weaker is due to simultaneous transitions in two oxygen molecules; one molecule makes the electronic transition together with the $0-0$ or $1-0$ vibrational transition and the other molecule makes only the 1-0 vibrational transition of the ground electronic state. The integrated absorption coefficient of the bands varies in a complex way with increasing dilution. The behaviour of the bands in the gas phase at high pressures will also be discussed. | en_US |
dc.format.extent | 103510 bytes | |
dc.format.mimetype | image/jpeg | |
dc.language.iso | en | en_US |
dc.publisher | Ohio State University | en_US |
dc.title | STRUCTURE OF THE INFRARED "ATMOSPHERIC" BANDS IN LIQUID OXYGEN | en_US |
dc.type | article | en_US |
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