N. Bigler, J. Pupeikis, S. Hrisafov, L. Gallmann, C. Phillips, U. Keller
{"title":"大功率亚双周2.5 μm光参量啁啾脉冲放大系统","authors":"N. Bigler, J. Pupeikis, S. Hrisafov, L. Gallmann, C. Phillips, U. Keller","doi":"10.1109/CLEOE-EQEC.2019.8871538","DOIUrl":null,"url":null,"abstract":"Mid-infrared (mid-IR) laser sources with a high repetition rate and peak power are particularly interesting for strong-field and attosecond science, enabling fast measurements and shorter attosecond pulses via the high-harmonic cut-off [1]. Here we demonstrate our optical parametric chirped pulse amplification (OPCPA) system delivering pulses with 12.6 W average power and a pulse duration of 14.4 fs at 100 kHz with a center wavelength of 2.5 μm. This corresponds to a record-high mid-IR (above 2 μώ) peak power of 6.3 GW at 100 kHz repetition rate [2]. Moreover we present a new time-gated pulse shaping scheme which enables optimal compression of the high-power mid-IR pulses [3].","PeriodicalId":6714,"journal":{"name":"2019 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)","volume":"1 1","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2019-10-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"High-Power and Sub-Two-Cycle 2.5 μm Optical Parametric Chirped Pulse Amplification System\",\"authors\":\"N. Bigler, J. Pupeikis, S. Hrisafov, L. Gallmann, C. Phillips, U. Keller\",\"doi\":\"10.1109/CLEOE-EQEC.2019.8871538\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Mid-infrared (mid-IR) laser sources with a high repetition rate and peak power are particularly interesting for strong-field and attosecond science, enabling fast measurements and shorter attosecond pulses via the high-harmonic cut-off [1]. Here we demonstrate our optical parametric chirped pulse amplification (OPCPA) system delivering pulses with 12.6 W average power and a pulse duration of 14.4 fs at 100 kHz with a center wavelength of 2.5 μm. This corresponds to a record-high mid-IR (above 2 μώ) peak power of 6.3 GW at 100 kHz repetition rate [2]. Moreover we present a new time-gated pulse shaping scheme which enables optimal compression of the high-power mid-IR pulses [3].\",\"PeriodicalId\":6714,\"journal\":{\"name\":\"2019 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)\",\"volume\":\"1 1\",\"pages\":\"1-1\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-10-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2019 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CLEOE-EQEC.2019.8871538\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2019 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEOE-EQEC.2019.8871538","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
High-Power and Sub-Two-Cycle 2.5 μm Optical Parametric Chirped Pulse Amplification System
Mid-infrared (mid-IR) laser sources with a high repetition rate and peak power are particularly interesting for strong-field and attosecond science, enabling fast measurements and shorter attosecond pulses via the high-harmonic cut-off [1]. Here we demonstrate our optical parametric chirped pulse amplification (OPCPA) system delivering pulses with 12.6 W average power and a pulse duration of 14.4 fs at 100 kHz with a center wavelength of 2.5 μm. This corresponds to a record-high mid-IR (above 2 μώ) peak power of 6.3 GW at 100 kHz repetition rate [2]. Moreover we present a new time-gated pulse shaping scheme which enables optimal compression of the high-power mid-IR pulses [3].