{"title":"Laser‐induced breakdown of UF6 and its application to flow diagnostics","authors":"S. W. Allison, M. Cates, B. Noel","doi":"10.1063/1.35825","DOIUrl":null,"url":null,"abstract":"Breakdown of gaseous UF6 can be produced with relatively low fluence (approximately 106 W/cm2) near‐uv pulsed laser light. A broad spectrum is produced consisting of hundred of atomic (U1 and U11) lines. Following breakdown, particles are formed from the dissociation/ionization products and the sample volume remains ionized for a long time. This sample volume is elevated in temperature, and a shock wave is produced. Other pertinent details are presented. A schlieren technique is described for observing the motion, hence velocity, of the temperature defect and shock wave. Also given is a flow visualization method based on imaging a long‐lived emission component with a gated (≥10‐ns) image intensifier system. These and other methods are prospective ways to perform flow diagnostics in gas centrifuges.","PeriodicalId":298672,"journal":{"name":"Advances in Laser Science-I","volume":"35 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2008-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in Laser Science-I","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.35825","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Breakdown of gaseous UF6 can be produced with relatively low fluence (approximately 106 W/cm2) near‐uv pulsed laser light. A broad spectrum is produced consisting of hundred of atomic (U1 and U11) lines. Following breakdown, particles are formed from the dissociation/ionization products and the sample volume remains ionized for a long time. This sample volume is elevated in temperature, and a shock wave is produced. Other pertinent details are presented. A schlieren technique is described for observing the motion, hence velocity, of the temperature defect and shock wave. Also given is a flow visualization method based on imaging a long‐lived emission component with a gated (≥10‐ns) image intensifier system. These and other methods are prospective ways to perform flow diagnostics in gas centrifuges.