{"title":"The measure of the isotopic and hyperfine structure of the radiation Hg 1849 Å by means of the magnetic scanning method","authors":"E. Leboucher, C. Bousquet, N. Bras","doi":"10.1088/0335-7368/5/2/308","DOIUrl":null,"url":null,"abstract":"The isotopic and hyperfine structure of the resonace radiation Hg 1 849 A was measured by means of the magnetic scanning method. Many difficulties were encountered: technical difficulties because of the field of wavelength of the far U-V radiation, difficulties due to the radiation itself (strong self-absorption effect, distortion of the scanning profile with the induction B). These last difficulties were overcome by using « the nodes » which do not depend on the scanning line profile, and by building theoretical models of the source profile and of the transmission curves. The splittings 198-200 and 200-202 were measured with great accuracy.","PeriodicalId":286899,"journal":{"name":"Nouvelle Revue D'optique","volume":"56 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1974-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"9","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nouvelle Revue D'optique","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/0335-7368/5/2/308","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 9
Abstract
The isotopic and hyperfine structure of the resonace radiation Hg 1 849 A was measured by means of the magnetic scanning method. Many difficulties were encountered: technical difficulties because of the field of wavelength of the far U-V radiation, difficulties due to the radiation itself (strong self-absorption effect, distortion of the scanning profile with the induction B). These last difficulties were overcome by using « the nodes » which do not depend on the scanning line profile, and by building theoretical models of the source profile and of the transmission curves. The splittings 198-200 and 200-202 were measured with great accuracy.