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486nm blue laser operating at 500kHz pulse repetition frequency

机译:486 nm蓝色激光,脉冲重复频率为500 kHz

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Compact, high power blue light in the 470-490nm region is difficult to generate due to the lack of laser sources which are easily convertible (through parametric processes) to those wavelengths. By using a pulsed Tm-doped fiber laser as a pump source for a 2-stage second harmonic generation (SHG) scheme, we have generated ~2W of 486.5nm light at 500kHz pulse repetition frequency (PRF). To our knowledge, this is the highest PRF and output power achieved in the blue region based on a frequency converted, monolithic fiber laser. This pump laser is a pulsed Tm-doped fiber laser/amplifier which generates 12.8W of 1946nm power at 500kHz PRF with diffraction-limited output from a purely single-mode fiber. The output from this laser is converted to 973nm through second harmonic generation (SHG). The 973nm is then converted to 486.5nm via another SHG stage. This architecture operates with very low peak power, which can be challenging from a nonlinear conversion standpoint. However, the low peak power enables the use of a single-mode monolithic fiber amplifier without undergoing nonlinear effects in the fiber. This also eliminates the need for novel fiber designs, large-mode area fiber, or free-space coupling to rod-type amplifiers, improving reliability and robustness of the laser source. Higher power and conversion efficiency are possible through the addition of Tm-doped fiber amplification stages as well as optimization of the nonlinear conversion process and nonlinear materials. In this paper, we discuss the laser layout, results, and challenges with generating blue light using a low peak power approach.
机译:由于缺少易于转换(通过参数过程)转换为那些波长的激光源,因此难以在470-490nm区域产生紧凑的高功率蓝光。通过使用掺有Tm的脉冲光纤激光器作为泵浦光源,进行二级二次谐波(SHG)方案,我们以500kHz脉冲重复频率(PRF)产生了约2W的486.5nm光。据我们所知,这是基于频率转换的单片光纤激光器在蓝色区域实现的最高PRF和输出功率。该泵浦激光器是脉冲Tm掺杂光纤激光器/放大器,它在500kHz PRF时产生12.8W的功率,功率为1946nm,纯单模光纤的衍射极限输出。该激光器的输出通过二次谐波(SHG)转换为973nm。然后,通过另一个SHG平台将973nm转换为486.5nm。这种架构的峰值功率非常低,从非线性转换的角度来看,这可能是一个挑战。然而,低峰值功率使得能够使用单模单片光纤放大器,而不会在光纤中遭受非线性影响。这也消除了对新颖光纤设计,大模面积光纤或自由空间耦合到棒型放大器的需求,从而提高了激光源的可靠性和耐用性。通过添加掺有Tm的光纤放大级以及优化非线性转换过程和非线性材料,可以实现更高的功率和转换效率。在本文中,我们讨论了使用低峰值功率方法产生蓝光的激光器布局,结果和挑战。

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