LD端泵浦Nd:YAG单晶光纤中泵浦分布的仿真与实验

Xiaotian Cai, Xiao Li, Guo-min Zhao
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摘要

基于MATLAB建立了泵浦分布模型,模拟了泵浦在端泵浦单晶光纤中的分布。仿真结果表明,杆状单晶光纤中的泵浦会再次收敛。通过改变晶体吸收系数可以发现,吸收系数越小,泵浦分布越均匀;当它较大时,泵将更严重地向泵端集中。在实验中建立端泵实验平台,晶体直径为1mm,长度为30mm, Nd3+掺杂浓度为1%。改变泵浦光聚焦在晶体中的位置,我们可以通过聚焦在晶体中的不同位置看到泵浦光的不同分布,发现当聚焦在晶体轴上且距离泵浦端面1mm时,泵浦光的分布最均匀。此时,泵的第二次收敛清晰可见。通过改变泵浦波长,晶体吸收系数发生变化。研究发现,在相同的泵功率下,吸光系数越大,泵向泵端集中的现象就越严重。晶体泵端温度升高,与仿真结果一致。结果表明,对于单晶光纤来说,吸收系数越高并不是越好,低的吸收系数导致泵浦分布均匀,在较长的单晶光纤中会有较好的吸收。而由于端面温度较低,端泵功率上限也会增大。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Simulation and experiment of pump distribution in LD end-pumped Nd:YAG single crystal fiber
The spread of the pump model, established based on MATLAB, simulates the distribution of the pump in End-Pumped single crystal fiber. Simulation results show that the pump in the rod single crystal fiber will converge again. By changing the crystal absorption coefficient, it can be found that smaller the absorption coefficient is, more uniform the pump distribution is; when it is greater, the pump will concentrate to the pump end more seriously. Establish End- Pumped Experimental platform in the experiment, the crystal is 1 mm in diameter and length of 30 mm, Nd3+ doping concentration is 1%. Change the position of the pump light's focus in the crystal, we can see different distribution of the pump light by different focus location in the crystal and find that the pump light has the most homogeneous distribution when the focus is on the crystal axis and has 1mm distance to the pump end face. At this time, the second convergence of the pump is clearly visible. By changing the pump wavelength, crystal absorption coefficient changes. It is found that under the same pump power, absorption coefficient is greater, the pump will concentrate to the pump end more seriously. And the temperature of crystal pump end rises, which is identical with the simulation results. The results indicate that for the single crystal fiber, the higher absorption coefficient is not better, low absorption coefficient leads to the uniform distribution of the pump, there will be a better absorption in a relatively long length of single crystal fiber. And due to the lower end face temperature, end pump power upper limit will also increase.
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