Acta Physica Sinica, Volume. 68, Issue 23, 234205-1(2019)
Fig. 1. Model of high energy system.高能激光系统模型
Fig. 2. Intensity distribution in near-field.近场光强分布
Fig. 3. Formation of atmospheric turbulence phase screen.大气湍流相位屏示意
Fig. 4. Distortion wavefront of atmospheric turbulence.大气湍流畸变波前
Fig. 5. Intensity distribution of two dimensions: (a) Before correcting tilt aberration; (b) after correcting tilt aberration.二维光强分布 (a) 倾斜像差校正前; (b) 倾斜像差校正后
Fig. 6. Intensity distribution of one dimension: (a) Central section in
Fig. 7. The beam quality at 2 km corresponding to different coherence lengths: (a) PIB; (b) SR.2 km处不同大气相干长度的激光光束质量 (a) PIB; (b) SR
Fig. 8. The beam quality at 3 km corresponding to different coherence lengths: (a) PIB; (b) SR3 km处不同大气相干长度的激光光束质量 (a) PIB; (b) SR
Fig. 9. Equipment at target.目标端设备实物
Fig. 10. Measurement results of beam quality analyzer: (a) Before correcting tilt aberration; (b) after correcting tilt aberration.光束质量分析仪测量结果 (a) 倾斜像差校正前; (b) 倾斜像差校正后
Coefficient of tilt aberration in each sub-wavefront.
子波前倾斜像差系数
Coefficient of tilt aberration in each sub-wavefront.
子波前倾斜像差系数
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Result of the beam quality in far-field.
激光远场光束质量计算结果
Result of the beam quality in far-field.
激光远场光束质量计算结果
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Wan-Tao Deng, Gang Zhao, Hui-Jun Xia, Mao Zhang, Yi-Fan Yang.
Received: Jun. 20, 2019
Accepted: --
Published Online: Sep. 17, 2020
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