G. Baranov, A. A. Kuchinsky, P. Tomashevich, S. Kotov, A. Vasil’ev
{"title":"Laser amplifier for picosecond CO2 facilities of terawatt power level","authors":"G. Baranov, A. A. Kuchinsky, P. Tomashevich, S. Kotov, A. Vasil’ev","doi":"10.1080/10519990701859196","DOIUrl":null,"url":null,"abstract":"In this paper the design features and the results of studying an amplifier for a picosecond terawatt CO2-laser facility are given. The active medium of the amplifier (a CO2–N2–He gas mixture) is excited by a self-sustained volume discharge. The amplifier with an aperture of 0.1 m×0.1 m and with an active medium volume of 10 l provides the possibility for amplifying the 10 μ m radiation of a picosecond laser up to the terawatt power level. A volume discharge at a pressure of 10 atm and at a molecular gas content of 5% with a power input level of 80 J l−1 atm−1 was initiated. The optical gain constant of a small signal of the amplifier active medium was 0.027 cm−1 at a pressure of 8 atm, which confirms the possibility of high-pressure amplifier use as a final amplifier in picosecond CO2-laser facilities with a power output level of 1–10 TW.","PeriodicalId":54600,"journal":{"name":"Plasma Devices and Operations","volume":"27 1","pages":"45 - 59"},"PeriodicalIF":0.0000,"publicationDate":"2008-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Plasma Devices and Operations","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1080/10519990701859196","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
In this paper the design features and the results of studying an amplifier for a picosecond terawatt CO2-laser facility are given. The active medium of the amplifier (a CO2–N2–He gas mixture) is excited by a self-sustained volume discharge. The amplifier with an aperture of 0.1 m×0.1 m and with an active medium volume of 10 l provides the possibility for amplifying the 10 μ m radiation of a picosecond laser up to the terawatt power level. A volume discharge at a pressure of 10 atm and at a molecular gas content of 5% with a power input level of 80 J l−1 atm−1 was initiated. The optical gain constant of a small signal of the amplifier active medium was 0.027 cm−1 at a pressure of 8 atm, which confirms the possibility of high-pressure amplifier use as a final amplifier in picosecond CO2-laser facilities with a power output level of 1–10 TW.