{"title":"氩发射光谱法标准","authors":"J. Brault","doi":"10.1364/hrfts.1992.thb2","DOIUrl":null,"url":null,"abstract":"For over a decade, users of the FTS at the McMath Solar Telescope of the National Solar Observatory have had access to a simple but precise working wavenumber standard for absorption spectra in the form of a short sealed cell containing 10 or 20 Torr of N2O. Because of the high pressure, the observed wavenumbers are not those of the unperturbed molecule, but a direct calibration of the 0002 band at 4417 cm−1in this cell against the accurately known P(7) transition in CH4 yielded wavenumbers with a precision of the order of 0.000002 cm−1 and an accuracy thought to be at least 0.00001 cm−1 (Brault [1]). Some years later, this band was observed by Pollock, et al. [2] using laser heterodyne techniques, and when our cell values are corrected using the pressure shift which they observed, the absolute agreement is quite satisfactory: (NSO - Pollock, calculated) = 0.000035 ± .0000035 cm−1; note that the absolute uncertainty in Pollock, et al. is quoted as .000080 cm−1.","PeriodicalId":159025,"journal":{"name":"High Resolution Fourier Transform Spectroscopy","volume":"21 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Argon I Standards for Emission Spectrometry\",\"authors\":\"J. Brault\",\"doi\":\"10.1364/hrfts.1992.thb2\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"For over a decade, users of the FTS at the McMath Solar Telescope of the National Solar Observatory have had access to a simple but precise working wavenumber standard for absorption spectra in the form of a short sealed cell containing 10 or 20 Torr of N2O. Because of the high pressure, the observed wavenumbers are not those of the unperturbed molecule, but a direct calibration of the 0002 band at 4417 cm−1in this cell against the accurately known P(7) transition in CH4 yielded wavenumbers with a precision of the order of 0.000002 cm−1 and an accuracy thought to be at least 0.00001 cm−1 (Brault [1]). Some years later, this band was observed by Pollock, et al. [2] using laser heterodyne techniques, and when our cell values are corrected using the pressure shift which they observed, the absolute agreement is quite satisfactory: (NSO - Pollock, calculated) = 0.000035 ± .0000035 cm−1; note that the absolute uncertainty in Pollock, et al. is quoted as .000080 cm−1.\",\"PeriodicalId\":159025,\"journal\":{\"name\":\"High Resolution Fourier Transform Spectroscopy\",\"volume\":\"21 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"High Resolution Fourier Transform Spectroscopy\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/hrfts.1992.thb2\",\"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 Fourier Transform Spectroscopy","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/hrfts.1992.thb2","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
For over a decade, users of the FTS at the McMath Solar Telescope of the National Solar Observatory have had access to a simple but precise working wavenumber standard for absorption spectra in the form of a short sealed cell containing 10 or 20 Torr of N2O. Because of the high pressure, the observed wavenumbers are not those of the unperturbed molecule, but a direct calibration of the 0002 band at 4417 cm−1in this cell against the accurately known P(7) transition in CH4 yielded wavenumbers with a precision of the order of 0.000002 cm−1 and an accuracy thought to be at least 0.00001 cm−1 (Brault [1]). Some years later, this band was observed by Pollock, et al. [2] using laser heterodyne techniques, and when our cell values are corrected using the pressure shift which they observed, the absolute agreement is quite satisfactory: (NSO - Pollock, calculated) = 0.000035 ± .0000035 cm−1; note that the absolute uncertainty in Pollock, et al. is quoted as .000080 cm−1.