首页|应用于高能激光器的XY离焦像差校正方法

应用于高能激光器的XY离焦像差校正方法

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针对高能激光器出光过程中出现的大量离焦和 0°像散低阶像差现象,提出了基于哈特曼波前传感器和二维整形光路的XY离焦像差校正方法.首先,通过对Zernike多项式的离焦项和 0°像散项进行线性组合得到XY离焦像差的表达式,该XY离焦像差系数的大小可直接表征X离焦和Y离焦的波前PV值.同时,通过微调高能激光器中二维整形光路中的镜子间距,可实现激光器输出光束XY离焦波面的补偿.因此,首先利用哈特曼波前传感器提取出光束的XY离焦像差系数大小,而后再根据XY离焦像差系数的大小实时闭环微调二维整形光路中的镜子间距,从而实现XY离焦像差的校正,改善输出光束的光束质量.实验结果表明,该方法可有效地将高能激光器输出光束XY离焦量的PV值由5.2 μm和1.1 μm校正到0.5 μm以下,相应的光束质量β因子由3.1降到1.8,光束质量得到明显改善.
An XY defocus aberration correction method for high-energy lasers
A method for correcting XY defocus aberrations,based on Hartmann-Shack wavefront sensor and two-dimensional beam-shaping light path,was presented due to the large percentage of defocus and 0°astig-matism aberrations with large PV values in high-energy laser beam.The first step is to derive an expression for XY defocus aberrations by linearly combining the defocus and 0° astigmatism terms of Zernike polynomi-als.The coefficients directly characterize the wavefront peak-to-valley(PV)values of X and Y defocus.At the same time,compensation for XY defocus wavefronts of the laser beam can be achieved by fine-tuning the mirror spacing in the two-dimensional shaping optics of the high-energy laser.Therefore,the Hartmann wavefront sensor is used to extract the coefficients of XY defocus aberrations from the laser beam.The com-puter dynamically adjusts the mirror spacing in the two-dimensional shaping optics based on these coeffi-cient values to correct XY defocus aberrations and improve the beam quality of the output laser beam.The results of the experiment showcase a significant decrease in PV value of XY defocus aberrations from 5.2 μm and 1.1 μm to less than 0.5 μm,as well as a decrease in β factor from 3.1 to 1.8,resulting in substantial im-provement in beam quality.

high energy laserbeam qualityaberration correctionbeam shapingmatrix optics

冯亚飞、韦承甫、任晓明、郭建增、王杰

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中国船舶集团有限公司第七一八研究所,河北邯郸 056027

高能激光 光束质量 像差校正 光束整形 矩阵光学

国家高技术研究发展计划(863计划)

51326010201

2024

中国光学
中国科学院长春光学 精密机械与物理研究所 中国光学学会

中国光学

CSTPCD北大核心
影响因子:2.02
ISSN:2095-1531
年,卷(期):2024.17(2)
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