A. Kudlinski, B. Cumberland, J. Travers, G. Bouwmans, Y. Quiquempois, A. Mussot
{"title":"两个零色散波长光子晶体光纤中连续波超连续谱的产生","authors":"A. Kudlinski, B. Cumberland, J. Travers, G. Bouwmans, Y. Quiquempois, A. Mussot","doi":"10.1063/1.3002529","DOIUrl":null,"url":null,"abstract":"This study is devoted to supercontinuum generation in photonic crystal fibres using a continuous-wave pumping scheme. We demonstrate that the spectral broadening of a continuous-wave laser can be more efficiently achieved in a short piece of photonic crystal fibre with two zero-dispersion wavelengths rather than in a fibre with a single one. This is due to efficient self-frequency shift of the solitons initially created by modulation instability, because their peak power is kept high in fibres with two zero-dispersion wavelengths. We then focus on the dynamics of the supercontinuum evolution under continuous-wave pumping in a series of different photonic crystal fibres exhibiting two zero-dispersion wavelengths. Control of the supercontinuum spectral extension is demonstrated as well as the changing dynamics as the zero-dispersion wavelengths are brought closer together. For closest zero-dispersion wavelengths, the spectral broadening is mainly due to parametric processes. For increasing spectral separation between the two zero-dispersion wavelengths, the soliton self-frequency shift due to intrapulse Raman scattering becomes more important. The soliton self-frequency shift is canceled just before the second zero-dispersion wavelength and some energy is transferred to a phase-matched dispersive wave. We also pay particular attention to the effect of the water absorption band located around 1380 nm.","PeriodicalId":301956,"journal":{"name":"1st Workshop on Specialty Optical Fibers and Their Applications","volume":"102 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2008-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"12","resultStr":"{\"title\":\"CW Supercontinuum Generation in Photonic Crystal Fibres with Two Zero-Dispersion Wavelengths\",\"authors\":\"A. Kudlinski, B. Cumberland, J. Travers, G. Bouwmans, Y. Quiquempois, A. Mussot\",\"doi\":\"10.1063/1.3002529\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This study is devoted to supercontinuum generation in photonic crystal fibres using a continuous-wave pumping scheme. We demonstrate that the spectral broadening of a continuous-wave laser can be more efficiently achieved in a short piece of photonic crystal fibre with two zero-dispersion wavelengths rather than in a fibre with a single one. This is due to efficient self-frequency shift of the solitons initially created by modulation instability, because their peak power is kept high in fibres with two zero-dispersion wavelengths. We then focus on the dynamics of the supercontinuum evolution under continuous-wave pumping in a series of different photonic crystal fibres exhibiting two zero-dispersion wavelengths. Control of the supercontinuum spectral extension is demonstrated as well as the changing dynamics as the zero-dispersion wavelengths are brought closer together. For closest zero-dispersion wavelengths, the spectral broadening is mainly due to parametric processes. For increasing spectral separation between the two zero-dispersion wavelengths, the soliton self-frequency shift due to intrapulse Raman scattering becomes more important. The soliton self-frequency shift is canceled just before the second zero-dispersion wavelength and some energy is transferred to a phase-matched dispersive wave. We also pay particular attention to the effect of the water absorption band located around 1380 nm.\",\"PeriodicalId\":301956,\"journal\":{\"name\":\"1st Workshop on Specialty Optical Fibers and Their Applications\",\"volume\":\"102 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2008-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"12\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1st Workshop on Specialty Optical Fibers and Their Applications\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/1.3002529\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1st Workshop on Specialty Optical Fibers and Their Applications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.3002529","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
CW Supercontinuum Generation in Photonic Crystal Fibres with Two Zero-Dispersion Wavelengths
This study is devoted to supercontinuum generation in photonic crystal fibres using a continuous-wave pumping scheme. We demonstrate that the spectral broadening of a continuous-wave laser can be more efficiently achieved in a short piece of photonic crystal fibre with two zero-dispersion wavelengths rather than in a fibre with a single one. This is due to efficient self-frequency shift of the solitons initially created by modulation instability, because their peak power is kept high in fibres with two zero-dispersion wavelengths. We then focus on the dynamics of the supercontinuum evolution under continuous-wave pumping in a series of different photonic crystal fibres exhibiting two zero-dispersion wavelengths. Control of the supercontinuum spectral extension is demonstrated as well as the changing dynamics as the zero-dispersion wavelengths are brought closer together. For closest zero-dispersion wavelengths, the spectral broadening is mainly due to parametric processes. For increasing spectral separation between the two zero-dispersion wavelengths, the soliton self-frequency shift due to intrapulse Raman scattering becomes more important. The soliton self-frequency shift is canceled just before the second zero-dispersion wavelength and some energy is transferred to a phase-matched dispersive wave. We also pay particular attention to the effect of the water absorption band located around 1380 nm.