ATMOSPHERIC TRANSMISSION OF $N_{2}O$ LASER ENERGY.

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1969

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Ohio State University

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The $N_{2}O$ laser operates in the atmospheric window occurring in the wave-length region around 10 microns. Since the amount of $N_{2}O$ in the atmosphere is very small, very little absorption of this radiant energy is expected over long atmospheric paths. A detailed study of the rotational lines of the $00^{\circ}1-10^{\circ}0$ band of $N_{2}O$ was undertaken in order to study the effect of atmospheric absorption. The laser tube containing $N_{2}O$ was placed in a cavity in which one mirror was replaced by a grating.$^{1}$ By turning the grating 65 rotational lines appeared whose frequencies were determined. Absorption of this energy by $N_{2}O$ was observed by use of a 10 m long absorption cell filled with $N_{2}O$. When the absorption cell was filled with $CO_{2}$ strong absorption was observed at R(10), R(12), R(14) and P(7) of the studied band of $N_{2}O$. This absorption occurs since these lines coincide in frequency with lines of the $00^{\circ}1-10^{\circ}0$ band of $CO_{2}$. It follows that the strongest lines of $N_{2}O$ occurring around P(19), are not obstructed by $CO_{2}$ in the atmosphere. This research was sponsored by the Air Force Office of Scientific Research under Grant EOOAR 69 0053, through the European Office of Aerospace Research (OAR), U.S. Air Force.

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$^{1}$ U.P. Oppenheim and A. D. Devir, J. Opt. Soc. Am. 58, 585 (1968).
Author Institution: Department of Physics, Technion, Israel Institute of Technology

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