1994
DOI: 10.1117/12.184632
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<title>Continuous wave 200kW supersonic CO laser</title>

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Cited by 12 publications
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“…This approach has been used in the past, e.g. in high-power CO 2 [2] and CO [3] lasers, electrically excited oxygen-iodine laser [4], and a supersonic wind tunnel generating vibrationally nonequilibrium flows [5]. In most of these cases, the plasma was sustained by a combination of two fully overlapping discharges, (i) high peak voltage, high repetition rate, ns pulse discharge producing electron impact ionization, and (ii) subbreakdown DC discharge, which does not generate ionization by itself but couples additional energy to the pre-ionized flow.…”
Section: Introductionmentioning
confidence: 99%
“…This approach has been used in the past, e.g. in high-power CO 2 [2] and CO [3] lasers, electrically excited oxygen-iodine laser [4], and a supersonic wind tunnel generating vibrationally nonequilibrium flows [5]. In most of these cases, the plasma was sustained by a combination of two fully overlapping discharges, (i) high peak voltage, high repetition rate, ns pulse discharge producing electron impact ionization, and (ii) subbreakdown DC discharge, which does not generate ionization by itself but couples additional energy to the pre-ionized flow.…”
Section: Introductionmentioning
confidence: 99%
“…Since their first development by Patel [1] and by Osgood and Eppers [2], the highest performance has been achieved in gas systems excited by various electric discharge methods and with the gas cooled to cryogenic temperatures. Efficiencies as high as 50% were reported by Grigor'yan et al [3] and powers up to 200 kW have been obtained by Dymshits et al [4] in cw systems operating on the fundamental bands. Overtone cw lasing was also achieved in similar systems by Bergman and Rich [5], with efficiencies up to 5% reported by Utkin et al [6].…”
Section: Introductionmentioning
confidence: 90%
“…Electric discharge excited CO lasers emitting in midinfrared have demonstrated high power and efficiency, up to 200 kW [7] and 50% [8], with optimal performance achieved using electric discharges operated at cryogenic temperatures. Laser gain is obtained on rovibrational transitions of CO molecules initially populated by electron impact in the discharge, by rapid vibration-vibration (V-V) energy exchange resulting in a highly non-Boltzmann population distribution among CO vibrational levels in low-temperature environments [9,10].…”
Section: Introductionmentioning
confidence: 99%