Output power and intensity distribution of a transverse-flow CO2 laser
We have measured the intensity distribution of a transverse-flow CO2 laser along the flow direction and the dependence of its output power on the cavity width. The experiments were performed with a transverse-flow CO2:N2 laser chemically excited by the reaction of nitric oxide with atomic nitrogen....
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Veröffentlicht in: | Journal of applied physics 1977-07, Vol.48 (7), p.2718-2722, Article 7 |
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container_title | Journal of applied physics |
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creator | Eidelman, O. Bin-Nun, E. Rokni, M. |
description | We have measured the intensity distribution of a transverse-flow CO2 laser along the flow direction and the dependence of its output power on the cavity width. The experiments were performed with a transverse-flow CO2:N2 laser chemically excited by the reaction of nitric oxide with atomic nitrogen. The intensity distribution is found to be of a multimode structure, fairly symmetrical about the optical axis. The overall output power for a given flow velocity and gas mixture is found to increase with increasing cavity width, up to a maximum value, and then it diminishes with any further increase of the cavity width. These results do not agree with those expected from a simple geometric-ray model. On the ohter hand, our results conform qualitatively with those expected from a coupled multimode approach. The main differences between the two approaches are discussed, and simple arguments are presented to illustrate the limitations of these two approaches. |
doi_str_mv | 10.1063/1.324123 |
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The experiments were performed with a transverse-flow CO2:N2 laser chemically excited by the reaction of nitric oxide with atomic nitrogen. The intensity distribution is found to be of a multimode structure, fairly symmetrical about the optical axis. The overall output power for a given flow velocity and gas mixture is found to increase with increasing cavity width, up to a maximum value, and then it diminishes with any further increase of the cavity width. These results do not agree with those expected from a simple geometric-ray model. On the ohter hand, our results conform qualitatively with those expected from a coupled multimode approach. The main differences between the two approaches are discussed, and simple arguments are presented to illustrate the limitations of these two approaches.</abstract><doi>10.1063/1.324123</doi><tpages>5</tpages></addata></record> |
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title | Output power and intensity distribution of a transverse-flow CO2 laser |
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