{"title":"相位扰动引起的单模激光不稳定性","authors":"J. C. Englund","doi":"10.1364/idlnos.1985.tub4","DOIUrl":null,"url":null,"abstract":"I have recently discovered that phase perturbations may destabilize the steady-state operation of gas lasers described by a single, standing- wave mode in resonance with a tuned cavity. The threshold of this instability may lie above or below that arising from amplitude perturbations1,2; furthermore, it coincides with a bifurcation of the steady-state field intensity ℐ and frequency ν. Neither the instability nor the bifurcation is experienced by running-wave modes.","PeriodicalId":262701,"journal":{"name":"International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems","volume":"34 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Single-mode Laser Instability Induced by Phase Perturbations\",\"authors\":\"J. C. Englund\",\"doi\":\"10.1364/idlnos.1985.tub4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"I have recently discovered that phase perturbations may destabilize the steady-state operation of gas lasers described by a single, standing- wave mode in resonance with a tuned cavity. The threshold of this instability may lie above or below that arising from amplitude perturbations1,2; furthermore, it coincides with a bifurcation of the steady-state field intensity ℐ and frequency ν. Neither the instability nor the bifurcation is experienced by running-wave modes.\",\"PeriodicalId\":262701,\"journal\":{\"name\":\"International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems\",\"volume\":\"34 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\":\"International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/idlnos.1985.tub4\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/idlnos.1985.tub4","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Single-mode Laser Instability Induced by Phase Perturbations
I have recently discovered that phase perturbations may destabilize the steady-state operation of gas lasers described by a single, standing- wave mode in resonance with a tuned cavity. The threshold of this instability may lie above or below that arising from amplitude perturbations1,2; furthermore, it coincides with a bifurcation of the steady-state field intensity ℐ and frequency ν. Neither the instability nor the bifurcation is experienced by running-wave modes.