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放大自发辐射辅助泵浦的L波段扩展掺铒光纤放大器

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近年来,L波段扩展的掺铒光纤放大器(LE-EDFA)由于能增加光纤传输带宽而成为研究热点,但该放大器所需增益光纤较长,普遍存在泵浦转换效率低、增益水平不高等问题.将反向放大自发辐射(ASE)辅助泵浦技术应用于LE-EDFA增益提升研究,发现反向ASE在泵浦功率较低或铒镱共掺光纤(EYDF)较长的情况下,可以大幅度提高LE-EDFA的增益水平,提高量可达5.1 dB~16.7 dB.采用反向ASE辅助泵浦结合预放大技术,在550 mW的较低总泵浦功率情况下,实现了 1570~1610 nm范围内高于 20 dB的增益、低于 6 dB的噪声系数,并且 1620 nm处的增益尚达13.7 dB.与其他已报道LE-EDFA相比,反向ASE辅助泵浦的LE-EDFA在较低的泵浦功率情况下实现了等同的增益水平,具有泵浦转换效率高、制备成本低等优势,有望广泛应用于高容量光纤传输系统.
L-Band Extended EDFA Co-Pumped by Backward ASE
L-band extended erbium-doped fiber amplifiers(LE-EDFA)have been studied in recent years for their extended gain bandwidths.However,the pump conversion efficiency and gain level are generally low due to the relatively long gain fiber required for this amplifier.In this paper,we improve the gain level of LE-EDFA by employing the backward amplified spontaneous emission(ASE)co-pumping technique.It is found that gain level improvement up to 5.1 dB‒16.7 dB can be achieved in the wavelength range of 1570‒1620 nm when the pump power is relatedly low or the Er/Yb co-doped fiber(EYDF)is relatively long.We then use the backward ASE co-pumping technique in a pre-amplified LE-EDFA and achieve a 20 dB gain bandwidth covering 1570‒1610 nm and noise figure less than 6.0 dB at a relatively low pump power of 550 mW.And the gain at 1620 nm is 13.7 dB.Compared with other reported LE-EDFAs,the L-band extended EDFA co-pumped by backward ASE achieves the same high gain level at the lowest pump power.The extended gain bandwidth,high pump conversion efficiency and low cost make it very prospective in high-capacity optical transmission systems.

L-band extended erbium-doped fiber amplifierEr/Yb co-doped fiberamplified spontaneous emission

林漫冰、阮继宇、劳浩贤、钟力、汪松、董新永

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广东工业大学信息工程学院先进光子技术研究院,广东 广州 510006

长飞光纤光缆股份有限公司光纤光缆先进制造与应用技术全国重点实验室,湖北 武汉 430073

广东工业大学通感融合光子技术教育部重点实验室,广东 广州 510006

广东工业大学广东省信息光子技术重点实验室,广东 广州 510006

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L波段扩展掺铒光纤放大器 铒镱共掺光纤 放大自发辐射

国家重点研发计划项目广东省引进创新创业团队项目

2020YFB18058042019ZT08X340

2024

激光与光电子学进展
中国科学院上海光学精密机械研究所

激光与光电子学进展

CSTPCD北大核心
影响因子:1.153
ISSN:1006-4125
年,卷(期):2024.61(13)