{"title":"分布式双稳光学系统中的准孤子","authors":"G. Surdutovich","doi":"10.1364/nldos.1990.ob223","DOIUrl":null,"url":null,"abstract":"In an arbitrary bistable distributed system -e.g. passive ring resonator with nonlinear medium and stationary input signal - spatially limited solitary initial perturbation (seed pulse) of a sufficiently large amplitude and arbitrary form turns into an asymtotically rectangular pulse with exponentially small instability increment (quasisoliton). The properties of the quasisoliton are analized within the frames of a different dispersion models. Such a quasisoliton regime was realized experimentally in acousto-electronic model system and in the system with bicompound injection laser and external cavity.","PeriodicalId":441335,"journal":{"name":"Nonlinear Dynamics in Optical Systems","volume":"39 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Quasi-Soliton Within a Distributed Bistable Optical System\",\"authors\":\"G. Surdutovich\",\"doi\":\"10.1364/nldos.1990.ob223\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In an arbitrary bistable distributed system -e.g. passive ring resonator with nonlinear medium and stationary input signal - spatially limited solitary initial perturbation (seed pulse) of a sufficiently large amplitude and arbitrary form turns into an asymtotically rectangular pulse with exponentially small instability increment (quasisoliton). The properties of the quasisoliton are analized within the frames of a different dispersion models. Such a quasisoliton regime was realized experimentally in acousto-electronic model system and in the system with bicompound injection laser and external cavity.\",\"PeriodicalId\":441335,\"journal\":{\"name\":\"Nonlinear Dynamics in Optical Systems\",\"volume\":\"39 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\":\"Nonlinear Dynamics in Optical Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/nldos.1990.ob223\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nonlinear Dynamics in Optical Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/nldos.1990.ob223","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Quasi-Soliton Within a Distributed Bistable Optical System
In an arbitrary bistable distributed system -e.g. passive ring resonator with nonlinear medium and stationary input signal - spatially limited solitary initial perturbation (seed pulse) of a sufficiently large amplitude and arbitrary form turns into an asymtotically rectangular pulse with exponentially small instability increment (quasisoliton). The properties of the quasisoliton are analized within the frames of a different dispersion models. Such a quasisoliton regime was realized experimentally in acousto-electronic model system and in the system with bicompound injection laser and external cavity.