Research progress on fiber laser spectral beam combining system and grating thermal analysis
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摘要: 受热效应、光学损伤与非线性效应等因素的限制,单纤的功率提高困难。因此通过光学元件将多束激光进行合束的光束合成技术应运而生。光谱合束方案具有结构简单,合束光束质量好等优点,逐渐成为了合束技术发展的主流。简要介绍了光纤激光光谱合束的几种常见合束方案,对比分析了几种合束技术的优缺点。对光谱合束中存在的光栅热畸变问题,从理论研究和实验研究两个方面进行了针对性的分析与讨论,并对光谱合束未来的发展趋势进行了展望。Abstract: The output power of single fiber is limited by the thermal effects, laser damage threshold, and nonlinear optical effects. Beam combining technology has been proposed to break through the limit of single fiber and achieve higher output power fiber laser. Spectral beam combining technology has the advantages of good beam quality and simple structure, which stands out among many beam combining technologies. We review several typical kinds of spectral beam combining technologies of fiber lasers, including their principles, current status, advantages and disadvantages. The recent progress of thermal distortion of the grating was introduced and discussed from the aspects of theoretical and experimental research, and the development trend of spectral beam combining technology are prospected.
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Key words:
- laser optics /
- spectral beam combining /
- thermal analysis /
- fiber laser /
- beam quality
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图 30 不同辐照功率密度,合成光束和单光束的光束强度分布。其中,图中心的光斑代表组合光束的强度分布,图右上角的光斑显示单光束的强度分布
Figure 30. Intensity distribution of the combined beams and that of a single emitter for different power densities,where the spots on the centers of the figures represent the intensity of the combined beams,and the spots on the upper right corners of the figures show the intensity of the beams from a single emitter
图 32 基板、薄膜和光栅浮雕的近场相位调制和远场强度分布。I/I0是归一化强度(波长为1064 nm)
Figure 32. Near-field phase modulation and far-field intensity distribution of A,B,and C,where A contains deformations of substrate,films,and grating reliefs,B contains substrate deformation only,and C is the circumstance without thermal deformation. I∕I0 is the normalization intensity (λ=1064 nm)
图 35 (a)不同功率激光辐照时光栅上表面最高温度实验与模拟结果对比图;(b)不同功率激光辐照时光栅背面实验与模拟的温度升温曲线图
Figure 35. (a) Simulation and experimental maximum MLD grating front surface temperature under different laser irradiation powers. (b) Maximum MLD grating back surface temperature as a function of the time and corresponding curves for different irradiation powers
表 1 组合光束质量变化
Table 1. Beam quality M2-Factors of the combined beams
power density/(kW·cm−2) M2 0 1.00 0.5 1.41 1 2.30 1.5 3.35 2 4.42 3 6.48 -
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