A. Wada, T. Sakai, D. Tanaka, T. Nozawa, R. Yamauchi
{"title":"High-Efficiency Erbium-Doped Fiber Amplifier using Mode Field Diameter Adjusting Technique","authors":"A. Wada, T. Sakai, D. Tanaka, T. Nozawa, R. Yamauchi","doi":"10.1364/oaa.1991.fd3","DOIUrl":null,"url":null,"abstract":"For efficient operation of an Er-doped fiber amplifier (EDFA) at 1.55 µm band it is essential to maximize the pump intensity in the Er-doped region because of the three level system [1], A high NA structure of EDF is effective to reduce the mode field diameter (MFD) of the pump and to achieve strong pump intensity [2], and has resulted in excellent gain performance [3],[4], In practical use, however, such small MFD fibers have a connection/splicing problem due to the mode field diameter mismatching. For example, approximately 1 dB splice loss is expected between an EDF with a 5 µm MFD and a conventional dispersion shifted fiber (DSF) with a 8 µm MFD. The smaller MFD of EDF, the higher splice loss. The increase of splicing loss causes noise figure degradation in pre-amplifiers and decreasing of conversion efficiency in booster amplifiers.","PeriodicalId":308628,"journal":{"name":"Optical Amplifiers and Their Applications","volume":"50 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1992-05-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Optical Amplifiers and Their Applications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/oaa.1991.fd3","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
For efficient operation of an Er-doped fiber amplifier (EDFA) at 1.55 µm band it is essential to maximize the pump intensity in the Er-doped region because of the three level system [1], A high NA structure of EDF is effective to reduce the mode field diameter (MFD) of the pump and to achieve strong pump intensity [2], and has resulted in excellent gain performance [3],[4], In practical use, however, such small MFD fibers have a connection/splicing problem due to the mode field diameter mismatching. For example, approximately 1 dB splice loss is expected between an EDF with a 5 µm MFD and a conventional dispersion shifted fiber (DSF) with a 8 µm MFD. The smaller MFD of EDF, the higher splice loss. The increase of splicing loss causes noise figure degradation in pre-amplifiers and decreasing of conversion efficiency in booster amplifiers.
为了使掺铒光纤放大器(EDFA)在1.55µm波段高效工作,由于是三能级系统[1],必须使掺铒区域的泵浦光强最大化。EDFA的高NA结构可以有效降低泵浦光强的模场直径(MFD)[2],从而获得优异的增益性能[3],[4]。然而,在实际应用中,由于模场直径不匹配,这种小的MFD光纤存在连接/拼接问题。例如,具有5 μ m MFD的EDF和具有8 μ m MFD的传统色散移位光纤(DSF)之间的拼接损耗约为1 dB。EDF的MFD越小,剪接损失越大。拼接损耗的增加导致前置放大器的噪声系数下降,升压放大器的转换效率下降。