{"title":"无限时间维非线性环形空腔混沌的非feigenbaum路径","authors":"M. Le Berre, E. Ressayre, A. Tallet, H. Gibbs","doi":"10.1364/idlnos.1985.wd32","DOIUrl":null,"url":null,"abstract":"The equations of motion for a ring cavity containing a cell of two-level atoms are where E0 and ε(t) are the cw input and intracavity electric field amplitudes at the input mirror. The phase difference {ϕ(t) - ϕ(0)} gives a measure of the amount of energy absorbed by the atoms and χϕ(t) is proportional to the instantaneous complex nonlinear refractive index. Other parameters in Eqs. (1) and (2) are the reflectivity factor R = 1 - T, γ-1 the inversion relaxation time for an atom, and τR the round-trip time.","PeriodicalId":262701,"journal":{"name":"International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems","volume":"367 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Non-Feigenbaum Route to Chaos of a Nonlinear Ring Cavity with Infinite Temporal Dimension\",\"authors\":\"M. Le Berre, E. Ressayre, A. Tallet, H. Gibbs\",\"doi\":\"10.1364/idlnos.1985.wd32\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The equations of motion for a ring cavity containing a cell of two-level atoms are where E0 and ε(t) are the cw input and intracavity electric field amplitudes at the input mirror. The phase difference {ϕ(t) - ϕ(0)} gives a measure of the amount of energy absorbed by the atoms and χϕ(t) is proportional to the instantaneous complex nonlinear refractive index. Other parameters in Eqs. (1) and (2) are the reflectivity factor R = 1 - T, γ-1 the inversion relaxation time for an atom, and τR the round-trip time.\",\"PeriodicalId\":262701,\"journal\":{\"name\":\"International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems\",\"volume\":\"367 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\":\"International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/idlnos.1985.wd32\",\"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.wd32","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Non-Feigenbaum Route to Chaos of a Nonlinear Ring Cavity with Infinite Temporal Dimension
The equations of motion for a ring cavity containing a cell of two-level atoms are where E0 and ε(t) are the cw input and intracavity electric field amplitudes at the input mirror. The phase difference {ϕ(t) - ϕ(0)} gives a measure of the amount of energy absorbed by the atoms and χϕ(t) is proportional to the instantaneous complex nonlinear refractive index. Other parameters in Eqs. (1) and (2) are the reflectivity factor R = 1 - T, γ-1 the inversion relaxation time for an atom, and τR the round-trip time.