{"title":"Reverse dark resonance in Rb excited by a diode laser","authors":"J. Alnis, M. Auzinsh","doi":"10.1088/0953-4075/34/20/302","DOIUrl":null,"url":null,"abstract":"The origin of recently discovered reverse (opposite-sign) dark resonances has been explained theoretically and verified experimentally. It is shown that the reason for these resonances is a specific optical pumping of the ground state magnetic sublevel in a transition when the ground state angular momentum is smaller than the excited state momentum. An experiment was conducted on 85Rb atoms in a cell, when a diode laser using the ground state hyperfine level Fg = 3 simultaneously excites spectrally unresolved hyperfine levels with total angular momentum quantum numbers Fe = 2,3 and 4. It is shown that due to differences in the transition probabilities the dominant role in total absorption and fluorescence signals is played by absorption on a transition Fg = 3→Fe = 4.","PeriodicalId":16799,"journal":{"name":"Journal of Physics B","volume":"23 1","pages":"3889-3898"},"PeriodicalIF":0.0000,"publicationDate":"2000-11-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"11","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics B","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/0953-4075/34/20/302","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 11
Abstract
The origin of recently discovered reverse (opposite-sign) dark resonances has been explained theoretically and verified experimentally. It is shown that the reason for these resonances is a specific optical pumping of the ground state magnetic sublevel in a transition when the ground state angular momentum is smaller than the excited state momentum. An experiment was conducted on 85Rb atoms in a cell, when a diode laser using the ground state hyperfine level Fg = 3 simultaneously excites spectrally unresolved hyperfine levels with total angular momentum quantum numbers Fe = 2,3 and 4. It is shown that due to differences in the transition probabilities the dominant role in total absorption and fluorescence signals is played by absorption on a transition Fg = 3→Fe = 4.