{"title":"High Energy 10 fs Pulses by a New Pulse Compression Technique","authors":"M. Nisoli, S. De Silvestri, O. Svelto","doi":"10.1109/CLEOE.1996.562549","DOIUrl":null,"url":null,"abstract":"A well established method for the generation of ultrashort pulses is optical pulse compression, which consists in spectral broadening by self-phase modulation in a single-mode optical fiber followed by chirp compensation into suitable phase dispersive elements. In this way pulses as short as 6 fs have been obtained [1]. The use of single-mode fibers is limited to low energy (nanojoule) pulses due to both material damage and appearance of high-order nonlinearities. So far spectral broadening of high energy femtosecond pulses was achieved in bulk materials [2] where the non-uniform transverse intensity profile of the beam represents a limitation. A compression technique for high energy ultrashort pulses must have a large diameter single mode guiding element with sufficiently high damage threshold and very fast third order non-linear optical susceptibility.","PeriodicalId":11780,"journal":{"name":"EQEC'96. 1996 European Quantum Electronic Conference","volume":"15 1","pages":"211-211"},"PeriodicalIF":0.0000,"publicationDate":"2002-08-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"EQEC'96. 1996 European Quantum Electronic Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEOE.1996.562549","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
A well established method for the generation of ultrashort pulses is optical pulse compression, which consists in spectral broadening by self-phase modulation in a single-mode optical fiber followed by chirp compensation into suitable phase dispersive elements. In this way pulses as short as 6 fs have been obtained [1]. The use of single-mode fibers is limited to low energy (nanojoule) pulses due to both material damage and appearance of high-order nonlinearities. So far spectral broadening of high energy femtosecond pulses was achieved in bulk materials [2] where the non-uniform transverse intensity profile of the beam represents a limitation. A compression technique for high energy ultrashort pulses must have a large diameter single mode guiding element with sufficiently high damage threshold and very fast third order non-linear optical susceptibility.