{"title":"Fluorescence Excitation Spectra of 1-Methyl-, 2-Methyl-, and 2-Ethyl-Naphthalenes in a Supersonic Free Jet","authors":"T. Ichimura, A. Auty, Anita C Jones, D. Phillips","doi":"10.5111/BUNKOU.34.83","DOIUrl":null,"url":null,"abstract":"Fluorescence excitation spectra of 1-methyl-, 2-methyl- and 2-ethyl-naphthalenes have been observed with the excitation of a xenon lamp in a supersonic free jet. The excitation spectrum of 1-methylnaphthalene was much the same with that of naphthalene, while 2-methyl- and 2-ethyl-naphthalene molecules exhibited entirely different spectral profile from 1-methylnaphthalene. Methylation or ethylation on the position 2 of naphthalene ring caused an increase of the origin intensity and changes of vibronic band frequency, which can be explained by symmetry reduction and mode mixing.","PeriodicalId":199016,"journal":{"name":"Journal of the Spectroscopical Society of Japan","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1985-04-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of the Spectroscopical Society of Japan","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.5111/BUNKOU.34.83","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 4
Abstract
Fluorescence excitation spectra of 1-methyl-, 2-methyl- and 2-ethyl-naphthalenes have been observed with the excitation of a xenon lamp in a supersonic free jet. The excitation spectrum of 1-methylnaphthalene was much the same with that of naphthalene, while 2-methyl- and 2-ethyl-naphthalene molecules exhibited entirely different spectral profile from 1-methylnaphthalene. Methylation or ethylation on the position 2 of naphthalene ring caused an increase of the origin intensity and changes of vibronic band frequency, which can be explained by symmetry reduction and mode mixing.