Influence of space radiation on properties of high power Yb-doped fiber lasers and their recent progress
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摘要:
高功率掺镱光纤激光器在空间环境中的应用日益增多，但掺镱光纤材料在空间辐照条件下会产生色心效应，导致损耗增加，影响光纤器件以及激光器整机的性能，从而给高功率光纤激光器在空间环境的长期稳定工作带来隐患。从空间辐照对高功率光纤激光器性能的影响机理、抑制方法和研究进展等3个方面进行介绍。首先介绍了空间辐照对高功率掺镱光纤激光器中关键光学器件、放大级热负载、非线性效应等方面的影响分析，其次介绍了抑制辐照效应的典型方法及其在高功率掺镱光纤激光器中的可行性分析，最后介绍了国内外典型的高功率掺镱光纤激光器的辐照影响及抑制的研究成果，并展望了未来发展趋势。
Abstract:High power Yb-doped fiber lasers have gained increasing application in space environment. However, the space radiation will bring color centers in Yb-doped fiber materials, thus increasing the inherent loss of the fiber. As a result, the optical properties of typical fiber-based components and the fiber lasers will be deteriorated, which makes it difficult for high power fiber lasers to achieve long-term stable operation in space environment. In this paper, a detailed introduction from three main aspects is given. Firstly, the influence of space radiation on typical optical components, thermal loading and nonlinear effects in high power fiber laser are introduced. Next, the typical suppressing methods of space radiation and their feasibility in high power fiber laser system are discussed. In the end, the representative research progress on the influence of space radiation on high power Yb-doped fiber lasers and effective suppressing methods at home and abroad are introduced.
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Key words:
- fiber laser /
- color center /
- radiation-induced attenuation /
- thermal loading /
- nonlinear effects
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图 1 基于MOPA结构的高功率掺镱光纤激光器组成示意图
Figure 1. Construction of high power Yb-doped fiber laser based on MOPA structure
图 2 Yb3+掺杂光纤辐致色心形成模型
Figure 2. The model of radiation-induced color center of the Yb3+-doped fiber
图 3 载氢处理抑制光子暗化空穴相关色心的原理示意图
Figure 3. Illustration of suppressing the hole-related color center by H2 loading treatment
图 4 （a）光纤长度及（b）泵浦结构对EDFA 辐照性能的影响；（c）采用优化的光纤长度和泵浦结构与非优化参数的EDFA辐照性能对比
Figure 4. Influence of (a) doped fiber length and (b) pump structure on the EDFA’s radiation properties; (c) comparison of the EDFA’s radiation properties with and without the optimized parameters
图 5 不同掺杂光纤的增益随辐照总剂量的变化规律
Figure 5. Variation of gain versus total radiation dose of three different doping fibers
图 6 不同辐照剂量、不同系统参数下放大器性能变化规律
Figure 6. Variation trend of the amplifier under different dose and different system parameters
图 7 915 nm与976 nm泵浦下（a）输出激光功率及（b）单位长度光纤的辐致损耗随辐照剂量变化规律
Figure 7. (a) Output power and (b) irradiation loss vs irradiation dose under 915 nm and 976 nm pump
图 8 辐照前后（a）光纤合束器耦合效率与（b）包层光剥离器剥离度变化情况
Figure 8. Properties variation of (a) combiner and (b) cladding pump stripper before and after radiation
图 10 原始光纤、γ辐照光纤及532 nm漂白后光纤的输出功率和标准偏差随泵浦功率变化关系
Figure 10. Output power and STD versus pump power of pristine, γ irradiated and 532 nm bleached fibers
图 11 不同泵浦时光纤振荡器不同信号波长的输出功率
Figure 11. Output power of the fiber laser at different wavelength under diffevent pump
图 12 （a）TMI随辐照剂量变化关系以及（b）不同辐照剂量下输出功率分布和TMI区域
Figure 12. (a) Variation of TMI versus radiation dose and (b) the output power profile and TMI area under different radiation dose
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