Complete AM and residual PM noise measurements of an external cavity semiconductor laser hybridly modelocked at 10 GHz

T. Yilmaz, C. DePriest, P. Delfyett, J. Abeles, A. Braun
{"title":"Complete AM and residual PM noise measurements of an external cavity semiconductor laser hybridly modelocked at 10 GHz","authors":"T. Yilmaz, C. DePriest, P. Delfyett, J. Abeles, A. Braun","doi":"10.1109/LEOS.2001.969111","DOIUrl":null,"url":null,"abstract":"Modelocked semiconductor and fiber lasers have been shown to operate with very low noise levels making them suitable as sources of sampling pulses for applications in analog-to-digital converter (ADC) technologies. In spite of the need for long cavities in fiber lasers, obtaining multigigahertz sampling rates has been possible by harmonic modelocking at high integer multiples of the relatively low fundamental cavity frequencies. Semiconductor lasers, on the other hand, have the capability of operating in both regimes (cavities can be either long or short). For harmonically modelocked lasers, noise spurs will arise at harmonics of the cavity frequency, while fundamental modelocking has the ability to eliminate these spurs. At multigigahertz sampling rates, every doubling in the sampling frequency causes the ADC resolution to fall by /spl sim/1 bit due to phase modulation (PM) noise (timing jitter) in the sampler. Accurate evaluation of pulse train noise then becomes an important issue. Commonly, reported measurements of PM noise extend out to limited offset frequencies (several tens of megahertz or lower). To consider the noise characterization complete, however, sideband measurements should extend to the highest offset frequencies possible (i.e. the Nyquist frequency). For harmonically modelocked lasers, this offset range will include noise spurs arising from harmonic beating mechanisms. We report measurements of AM and residual PM noise out to the Nyquist offset frequency (5 GHz) of a hybridly modelocked external cavity semiconductor laser for fundamental cavity frequency modelocking as well as harmonic modelocking.","PeriodicalId":18008,"journal":{"name":"LEOS 2001. 14th Annual Meeting of the IEEE Lasers and Electro-Optics Society (Cat. No.01CH37242)","volume":"81 1","pages":"906-907 vol.2"},"PeriodicalIF":0.0000,"publicationDate":"2001-11-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"LEOS 2001. 14th Annual Meeting of the IEEE Lasers and Electro-Optics Society (Cat. No.01CH37242)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/LEOS.2001.969111","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

Modelocked semiconductor and fiber lasers have been shown to operate with very low noise levels making them suitable as sources of sampling pulses for applications in analog-to-digital converter (ADC) technologies. In spite of the need for long cavities in fiber lasers, obtaining multigigahertz sampling rates has been possible by harmonic modelocking at high integer multiples of the relatively low fundamental cavity frequencies. Semiconductor lasers, on the other hand, have the capability of operating in both regimes (cavities can be either long or short). For harmonically modelocked lasers, noise spurs will arise at harmonics of the cavity frequency, while fundamental modelocking has the ability to eliminate these spurs. At multigigahertz sampling rates, every doubling in the sampling frequency causes the ADC resolution to fall by /spl sim/1 bit due to phase modulation (PM) noise (timing jitter) in the sampler. Accurate evaluation of pulse train noise then becomes an important issue. Commonly, reported measurements of PM noise extend out to limited offset frequencies (several tens of megahertz or lower). To consider the noise characterization complete, however, sideband measurements should extend to the highest offset frequencies possible (i.e. the Nyquist frequency). For harmonically modelocked lasers, this offset range will include noise spurs arising from harmonic beating mechanisms. We report measurements of AM and residual PM noise out to the Nyquist offset frequency (5 GHz) of a hybridly modelocked external cavity semiconductor laser for fundamental cavity frequency modelocking as well as harmonic modelocking.
查看原文
分享 分享
微信好友 朋友圈 QQ好友 复制链接
本刊更多论文
完成在10ghz混合模型锁定的外腔半导体激光器的AM和残余PM噪声测量
锁模半导体和光纤激光器已被证明具有非常低的噪声水平,使其适合作为模数转换器(ADC)技术中应用的采样脉冲源。尽管光纤激光器需要长腔,但通过在相对较低的基腔频率的高整数倍处进行谐波模型锁定,可以获得多千兆赫的采样率。另一方面,半导体激光器具有在两种体制下工作的能力(空腔可以长也可以短)。对于谐波锁模激光器,噪声杂散会在谐振腔频率的谐波处产生,而基本锁模能够消除这些杂散。在多千兆赫的采样率下,采样频率每增加一倍,由于采样器中的相位调制(PM)噪声(时序抖动),导致ADC分辨率下降/spl sim/1位。因此,脉冲序列噪声的准确评估就成为一个重要的问题。通常,报道的PM噪声测量扩展到有限的偏移频率(几十兆赫兹或更低)。然而,为了考虑完整的噪声特性,边带测量应该扩展到可能的最高偏移频率(即奈奎斯特频率)。对于谐波锁模激光器,这个偏移范围将包括谐波加热机制引起的噪声杂散。本文报道了一种混合锁模外腔半导体激光器在基腔频率锁模和谐波锁模下,在奈奎斯特偏置频率(5 GHz)上的调幅和残余PM噪声测量结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 去求助
来源期刊
自引率
0.00%
发文量
0
期刊最新文献
Investigation of 2D-lattice distributed reflector lasers Comparison of numerical aperture increasing lens and standard subsurface microscopy Optical coherence tomography of living and fabricated microfluidic systems Periodically poling by chromophore molecule orientation control in cross-linked polymer film [for SHG] Widely tunable fiber ring laser with EDFA/SOA
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
现在去查看 取消
×
提示
确定
0
微信
客服QQ
Book学术公众号 扫码关注我们
反馈
×
意见反馈
请填写您的意见或建议
请填写您的手机或邮箱
已复制链接
已复制链接
快去分享给好友吧!
我知道了
×
扫码分享
扫码分享
Book学术官方微信
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术
文献互助 智能选刊 最新文献 互助须知 联系我们:info@booksci.cn
Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。
Copyright © 2023 Book学术 All rights reserved.
ghs 京公网安备 11010802042870号 京ICP备2023020795号-1