{"title":"高效大功率ch3f496 μm激光系统","authors":"T. Plant, T. Detemple","doi":"10.1364/cleos.1976.we4","DOIUrl":null,"url":null,"abstract":"Many different configurations, both cw and pulsed, have been reported for a 496-μm CH3F laser optically pumped with a CO2 laser; however, none as yet has both the high efficiency and good beam quality required for plasma diagnostics applications.1-4 Simple superradiant geometries using multimode TEA CO2 lasers have produced peak powers > 1 MW, but in pulses with subnanosecond structure.2 Complicated cavity geometries have yielded smooth pulses but only at lower powers, and both methods have a photon conversion efficiency (number of 496-μm quanta/number of CO2 quanta absorbed) of only ~5%.","PeriodicalId":301658,"journal":{"name":"Conference on Laser and Electrooptical Systems","volume":"3 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Efficient high-power CH3F 496-μm laser systems\",\"authors\":\"T. Plant, T. Detemple\",\"doi\":\"10.1364/cleos.1976.we4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Many different configurations, both cw and pulsed, have been reported for a 496-μm CH3F laser optically pumped with a CO2 laser; however, none as yet has both the high efficiency and good beam quality required for plasma diagnostics applications.1-4 Simple superradiant geometries using multimode TEA CO2 lasers have produced peak powers > 1 MW, but in pulses with subnanosecond structure.2 Complicated cavity geometries have yielded smooth pulses but only at lower powers, and both methods have a photon conversion efficiency (number of 496-μm quanta/number of CO2 quanta absorbed) of only ~5%.\",\"PeriodicalId\":301658,\"journal\":{\"name\":\"Conference on Laser and Electrooptical Systems\",\"volume\":\"3 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Conference on Laser and Electrooptical Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/cleos.1976.we4\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Conference on Laser and Electrooptical Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/cleos.1976.we4","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Many different configurations, both cw and pulsed, have been reported for a 496-μm CH3F laser optically pumped with a CO2 laser; however, none as yet has both the high efficiency and good beam quality required for plasma diagnostics applications.1-4 Simple superradiant geometries using multimode TEA CO2 lasers have produced peak powers > 1 MW, but in pulses with subnanosecond structure.2 Complicated cavity geometries have yielded smooth pulses but only at lower powers, and both methods have a photon conversion efficiency (number of 496-μm quanta/number of CO2 quanta absorbed) of only ~5%.