Mikio Kuzuya, H. Matsumoto, H. Sakanashi, Tomohiko Takemoto, O. Mikami
{"title":"Time and Spatially Resolved Spectrum Study of Laser-Induced Plasma in Reduced Pressure Atmospheres of Argon and Helium","authors":"Mikio Kuzuya, H. Matsumoto, H. Sakanashi, Tomohiko Takemoto, O. Mikami","doi":"10.5111/BUNKOU.43.80","DOIUrl":null,"url":null,"abstract":"In order to find the optimum conditions which give best line-to-background ratio as well as high spectral line intensity, the emission characteristics of a Nd: YAG laser-induced plasma were studied in argon and helium atmospheres at reduced pressures from 760 to 1 Torr by using a combination of space and time resolution. From the experimental results, the conditions of a 200 Torr argon, an observation position of about 1.5mm above the sample surface, and a gate delay time of 2μs measured after the initiation of the laser pulse were established as optimum.","PeriodicalId":199016,"journal":{"name":"Journal of the Spectroscopical Society of Japan","volume":"29 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1994-04-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of the Spectroscopical Society of Japan","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.5111/BUNKOU.43.80","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 order to find the optimum conditions which give best line-to-background ratio as well as high spectral line intensity, the emission characteristics of a Nd: YAG laser-induced plasma were studied in argon and helium atmospheres at reduced pressures from 760 to 1 Torr by using a combination of space and time resolution. From the experimental results, the conditions of a 200 Torr argon, an observation position of about 1.5mm above the sample surface, and a gate delay time of 2μs measured after the initiation of the laser pulse were established as optimum.