中国电子科技集团公司第十一研究所固体激光技术重点实验室,北京,100015
纸质出版:2025
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张利明, 张昆, 张雪霞, 等. 2.5 kW线偏振窄线宽全光纤激光器[J]. 航空制造技术, 2025,68(19).
ZHANG Liming, ZHANG Kun, ZHANG Xuexia, et al. 2.5 kW Linearly Polarized Narrow Linewidth All-Fiber Laser[J]. Aeronautical Manufacturing Technology, 2025, 68(19).
张利明, 张昆, 张雪霞, 等. 2.5 kW线偏振窄线宽全光纤激光器[J]. 航空制造技术, 2025,68(19). DOI: 10.16080/j.issn1671-833x.2025.19.092.
ZHANG Liming, ZHANG Kun, ZHANG Xuexia, et al. 2.5 kW Linearly Polarized Narrow Linewidth All-Fiber Laser[J]. Aeronautical Manufacturing Technology, 2025, 68(19). DOI: 10.16080/j.issn1671-833x.2025.19.092.
高功率线偏振窄线宽光纤激光器在功率光谱合成、相干探测等领域具有广泛的应用前景。在高功率线偏振窄线宽光纤激光器中,模式不稳定(Transverse mode instability,TMI)效应是限制其功率提升的主要因素之一。本文分析了 TMI 效应对其输出功率的限制机制,提出基于多波长泵浦技术的 TMI 抑制方案。试验采用多波长泵浦技术,以输出功率 100 mW 的单频激光器为种子源,通过相位调制器将种子源线宽展宽至 23 GHz,经三级放大后,最终实现了功率 2.54 kW、线宽 23 GHz、中心波长 1064 nm 的线偏振激光输出,消光比达 98%,光束质量 M
x
2
= 1.21,M
y
2
= 1.23。进一步分析了泵浦波长对 TMI 效应的影响:由于光纤纤芯直径较小(20 μm),增益光纤对泵浦光的吸收系数较高(1.8 dB/m@976 nm),导致纤芯温度升高;加之泵浦光量子亏损引入的热量,使得纤芯折射率发生变化,导致激光器在较低功率下发生 TMI 效应。当泵浦波长向长波偏移时,泵浦光的量子亏损降低,同时泵浦吸收系数也减小,光纤整体及单位长度上的热分布均显著降低,从而提高了 TMI 阈值,有效提升了线偏振窄线宽光纤激光器的输出功率。
High-power linearly polarized narrow linewidth fiber lasers hold broad application prospects in wavelength beam combining
coherent detection
and other fields. In such lasers
transverse mode instability (TMI) is one of the main factors limiting their power scaling. In this paper
the influence of the TMI effect on the output power of high-power linearly polarized narrow linewidth fiber lasers is analyzed
and a TMI suppression method is proposed. The experiment employs multi-wavelength pumping technology
using 100 mW single-frequency laser as the seed
source. The linewidth of the seed source is broadened to 23 GHz via a phase modulator
and after three-stage amplification
a linearly polarized narrow linewidth laser output is finally achieved with the following parameters: power of 2.54 kW
linewidth of 23 GHz
central wavelength of 1064 nm
extinction ratio of 98%
and beam quality factors M
x
2
= 1.21 and M
y
2
= 1.23. The influence of pump wavelength on the TMI effect is further analyzed. Due to the small core diameter of the fiber (20 μm) and the high absorption coefficient of the gain fiber for pump light (1.8 dB/m@976 nm)
the core temperature increases significantly. Additionally
the heat introduced by the pump photon quantum defect causes a variation in the refractive index of the fiber core
leading to the occurrence of TMI at relatively low power levels. When the pump wavelength is shifted to longer wavelengths
both the quantum defect of the pump light and the pump absorption coefficient decrease
resulting in reduced heat distribution across the entire fiber length as well as per unit length. This thus increases the TMI threshold and effectively improves the output power of the linearly polarized narrow linewidth fiber laser.
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