盛泉, 司汉英, 安建民, 张海伟, 张钧翔, 丁宇, 李升才, 史伟, 姚建铨. 高功率光纤激光器反向光放大和损伤特性数值分析[J]. 红外与激光工程, 2020, 49(10): 20200009. DOI: 10.3788/IRLA20200009
引用本文: 盛泉, 司汉英, 安建民, 张海伟, 张钧翔, 丁宇, 李升才, 史伟, 姚建铨. 高功率光纤激光器反向光放大和损伤特性数值分析[J]. 红外与激光工程, 2020, 49(10): 20200009. DOI: 10.3788/IRLA20200009
Sheng Quan, Si Hanying, An Jianmin, Zhang Haiwei, Zhang Junxiang, Ding Yu, Li Shengcai, Shi Wei, Yao Jianquan. Numerical analysis on backward light amplification and damage in high-power fiber laser[J]. Infrared and Laser Engineering, 2020, 49(10): 20200009. DOI: 10.3788/IRLA20200009
Citation: Sheng Quan, Si Hanying, An Jianmin, Zhang Haiwei, Zhang Junxiang, Ding Yu, Li Shengcai, Shi Wei, Yao Jianquan. Numerical analysis on backward light amplification and damage in high-power fiber laser[J]. Infrared and Laser Engineering, 2020, 49(10): 20200009. DOI: 10.3788/IRLA20200009

高功率光纤激光器反向光放大和损伤特性数值分析

Numerical analysis on backward light amplification and damage in high-power fiber laser

  • 摘要: 利用速率方程模型对主振荡−功率放大器结构的1 μm波段掺镱(Yb)高功率光纤激光器中存在连续波反向信号光时的功率特性进行了理论分析,结果显示反向信号光功率会被高功率激光放大器所明显放大,10 kW级的光纤激光器中,100 W的反向信号经过放大器后功率会被放大至kW量级;与此同时,反向信号放大过程对反转粒子数的消耗会导致激光器的正向输出功率的严重下降。另外,反向信号放大也会导致放大器输出端的激光功率过强,加剧泵浦吸收和受激发射过程,增加该处的热负载、导致温度大幅上升100 ℃以上,对稳定性产生潜在影响。反向信号导致振荡器提供的正向种子光功率波动和下降时,正向信号不能充分饱和有源光纤中的增益,会进一步加强反向信号在主放大级中的放大作用,进而对系统造成更严重的影响。提高正向种子光功率、增强正向信号对激光增益的饱和作用,有助于抑制反向信号的放大过程,但需综合考虑种子源稳定性、热负载、热致模式不稳定和受激拉曼散射等因素合理选择种子光功率。

     

    Abstract: The amplification of continuous-wave backward signal in 1 μm high-power master-oscillator-power-amplifier based Yb-doped fiber laser was investigated using rate equation model. The results show that the backward light power would be amplified significantly by the high-power amplifier. The 100 W backward signal from the output end of the fiber amplifier can be amplified to up to kW level. Meanwhile, the amplification of backward signal can consume the population inversion, saturate laser gain and thus decrease the laser output power seriously. Furthermore, the backward signal amplification would result in a much higher laser intensity at the incident end of the amplifier gain fiber, where the highest pump power existed. The temperature at the incident end of the fiber can be 100 ℃ higher than that without backward signal. The higher laser intensity at the incident end could break the pump absorption saturation, and enhance the rates of pump absorption and stimulated emission a lot, hence increased the thermal load and the temperature significantly. Since the backward signal gain was determined by the saturation of population inversion by the forward seed, the power fluctuation of oscillator caused by the amplified backward signal may aggravate the backward signal amplification, and further increase the risk of damage. Higher forward seed power resulted in stronger saturation of the laser gain in the active fiber, which could suppress the backward signal amplification effectively. However, higher seed power put forwards much complex requirements to laser oscillator, and the thermal load in the active fiber of the laser amplifier would be more concentrated, which made the thermal management more difficult. Furthermore, with higher seed power, the stimulated Raman scattering and thermal induced transverse mode instability are more likely to occur. Therefore, it is important to optimize the seed laser power based on a comprehensive consideration of the above issues, and to prevent the backward light from coupling into the fiber amplifier.

     

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