{"title":"同位素质量差(16O, 18O)对CO2激光振荡光谱影响的研究","authors":"Yasuyuki Saito","doi":"10.1364/hrs.1993.pd10","DOIUrl":null,"url":null,"abstract":"It is difficult to explain continuity between12C16O2−12C16O2−12C18O2 laser oscillation spectra due to only oxygen isotope–mass–difference (16O, 18O) effect on rotation energy level of fine structure for 00°1 to 10°0 of transition of CO2 molecules. In order to explain fine structure interval of CO2 laser oscillation spectra, it is necessary to consider CO2 molecule shape of smaller O=C bond length (this means smaller rotation inertia moment of a CO2 molecule) through nuclear characteristics (for example, gravity center, shape, spin) in a CO2 molecule.","PeriodicalId":109383,"journal":{"name":"High Resolution Spectroscopy","volume":"10 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Study on isotope mass difference (16O, 18O) effect on CO2 laser oscillation spectra\",\"authors\":\"Yasuyuki Saito\",\"doi\":\"10.1364/hrs.1993.pd10\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"It is difficult to explain continuity between12C16O2−12C16O2−12C18O2 laser oscillation spectra due to only oxygen isotope–mass–difference (16O, 18O) effect on rotation energy level of fine structure for 00°1 to 10°0 of transition of CO2 molecules. In order to explain fine structure interval of CO2 laser oscillation spectra, it is necessary to consider CO2 molecule shape of smaller O=C bond length (this means smaller rotation inertia moment of a CO2 molecule) through nuclear characteristics (for example, gravity center, shape, spin) in a CO2 molecule.\",\"PeriodicalId\":109383,\"journal\":{\"name\":\"High Resolution Spectroscopy\",\"volume\":\"10 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"High Resolution Spectroscopy\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/hrs.1993.pd10\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"High Resolution Spectroscopy","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/hrs.1993.pd10","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Study on isotope mass difference (16O, 18O) effect on CO2 laser oscillation spectra
It is difficult to explain continuity between12C16O2−12C16O2−12C18O2 laser oscillation spectra due to only oxygen isotope–mass–difference (16O, 18O) effect on rotation energy level of fine structure for 00°1 to 10°0 of transition of CO2 molecules. In order to explain fine structure interval of CO2 laser oscillation spectra, it is necessary to consider CO2 molecule shape of smaller O=C bond length (this means smaller rotation inertia moment of a CO2 molecule) through nuclear characteristics (for example, gravity center, shape, spin) in a CO2 molecule.
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