1981
DOI: 10.1016/0030-3992(81)90035-9
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Single line CO laser operation

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Cited by 2 publications
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“…The usefulness of the effective multiline small signal gain (defined as the intensityweighted average of the individual single-line small signal gains) has been discussed previously and confirmed with a single-line laser (Smith and Murray 1981). A probe beam from a multiline low-power oscillator was passed through a 10 mm diameter, 1 m long, water-cooled sealed discharge tube (central cathode and anode at each end) filled with gas mixtures typical of those used in sealed-off cw lasers and the gain determined as described by Murray and Smith (1978).…”
Section: Measurements In Nitrogen and Hydrogen Mixturesmentioning
confidence: 70%
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“…The usefulness of the effective multiline small signal gain (defined as the intensityweighted average of the individual single-line small signal gains) has been discussed previously and confirmed with a single-line laser (Smith and Murray 1981). A probe beam from a multiline low-power oscillator was passed through a 10 mm diameter, 1 m long, water-cooled sealed discharge tube (central cathode and anode at each end) filled with gas mixtures typical of those used in sealed-off cw lasers and the gain determined as described by Murray and Smith (1978).…”
Section: Measurements In Nitrogen and Hydrogen Mixturesmentioning
confidence: 70%
“…The electron density was measured simultaneously with the gain and the discharge voltage in the same discharge tube; hence each set of measurements relates to identical plasma conditions. A microwave cavity (-9.1 GHz) method was used to measure the electron density (Murray and Smith 1981). From the difference in resonant frequency and cavity Q observed when the discharge is on and off the average electron density ne can be determined.…”
Section: Measurements In Nitrogen and Hydrogen Mixturesmentioning
confidence: 99%
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