{"title":"具有乘性彩色噪声的染料激光模型","authors":"P. Jung, H. Risken","doi":"10.1364/idlnos.1985.thc4","DOIUrl":null,"url":null,"abstract":"A single mode laser model with fluctuating pump parameter is in use to describe the statistical properties of the light intensity of a Dye laser [1-4]. The normalized Langevin equation with multiplicative colored noise read where ϵ represents exponential correlated noise with the noise strength D and the relaxation time γ-4[5-7]. The equivalent two variable Fokker-Planck equation has the form [5,8,9]","PeriodicalId":262701,"journal":{"name":"International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Dye Laser Model with Multiplicative Colored Noise\",\"authors\":\"P. Jung, H. Risken\",\"doi\":\"10.1364/idlnos.1985.thc4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A single mode laser model with fluctuating pump parameter is in use to describe the statistical properties of the light intensity of a Dye laser [1-4]. The normalized Langevin equation with multiplicative colored noise read where ϵ represents exponential correlated noise with the noise strength D and the relaxation time γ-4[5-7]. The equivalent two variable Fokker-Planck equation has the form [5,8,9]\",\"PeriodicalId\":262701,\"journal\":{\"name\":\"International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems\",\"volume\":\"1 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.thc4\",\"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.thc4","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A single mode laser model with fluctuating pump parameter is in use to describe the statistical properties of the light intensity of a Dye laser [1-4]. The normalized Langevin equation with multiplicative colored noise read where ϵ represents exponential correlated noise with the noise strength D and the relaxation time γ-4[5-7]. The equivalent two variable Fokker-Planck equation has the form [5,8,9]