• High Power Laser and Particle Beams
  • Vol. 32, Issue 1, 011020 (2020)
Yuzhen Liao, Deen Wang*, Xuewei Deng, Xin Zhang, Ying Yang, Yuyuan Guo, Shengheng Zheng, Qiang Yuan, and Dongxia Hu
Author Affiliations
  • Research Center of Laser Fusion, CAEP, P. O. Box 919-988, Mianyang 621900, China
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    DOI: 10.11884/HPLPB202032.190274 Cite this Article
    Yuzhen Liao, Deen Wang, Xuewei Deng, Xin Zhang, Ying Yang, Yuyuan Guo, Shengheng Zheng, Qiang Yuan, Dongxia Hu. Influence of structural surface roughness on self-excited oscillation of main amplification system of high power laser device[J]. High Power Laser and Particle Beams, 2020, 32(1): 011020 Copy Citation Text show less
    Amplifier optical path structure and self-oscillation time waveform in the back of cavity mirror
    Fig. 1. Amplifier optical path structure and self-oscillation time waveform in the back of cavity mirror
    Ablative trace near the aperture of the spatial filter
    Fig. 2. Ablative trace near the aperture of the spatial filter
    Two-dimensional Gaussian rough surface constructed by Monte-Carlo method
    Fig. 3. Two-dimensional Gaussian rough surface constructed by Monte-Carlo method
    Simulated circular light spot which is reflected by a Gaussian rough surface
    Fig. 4. Simulated circular light spot which is reflected by a Gaussian rough surface
    Resonant cavity between the orifice plate and the cavity mirror
    Fig. 5. Resonant cavity between the orifice plate and the cavity mirror
    Surface roughness comparison of samples prepared by shot blasting
    Fig. 6. Surface roughness comparison of samples prepared by shot blasting
    Relationship between aperture size, surface roughness and the proportion of reflected laser entering the main amplification system
    Fig. 7. Relationship between aperture size, surface roughness and the proportion of reflected laser entering the main amplification system
    Experiment procedure
    Fig. 8. Experiment procedure
    Spot image collected on CCD
    Fig. 9. Spot image collected on CCD
    Simulated spot image
    Fig. 10. Simulated spot image
    Statistical distribution of light intensity
    Fig. 11. Statistical distribution of light intensity
    Increasing the surface roughness of the structure
    Fig. 12. Increasing the surface roughness of the structure
    Self-oscillation waveform test before and after increasing the surface roughness of the structure
    Fig. 13. Self-oscillation waveform test before and after increasing the surface roughness of the structure
    geometric statisticstypical scattering characteristicsrepresentative surface
    subtle roughnessδs<0.1,lλspecular reflection with specular reflection peakmachine-finished surface, calm water surface
    slight roughness0.1<δs<0.3,lλnear diffuse reflection with peaks between mirror and normal direction ground surface, general machined surface
    strong roughness0.3<δs<1,l≈λdiffuse reflection with backward enhancement and significant depolarization effect artificial special surface
    extreme roughnessδs>1,l<λsimilar to an ideal reflectorunknown surface
    Table 1. Qualitative division of surface roughness
    σ/μm l/μm δs
    1#0.514.230.171
    2#0.955.720.235
    3#1.467.240.285
    4#1.958.780.314
    Table 2. Comparison of sample surface process statistics
    Yuzhen Liao, Deen Wang, Xuewei Deng, Xin Zhang, Ying Yang, Yuyuan Guo, Shengheng Zheng, Qiang Yuan, Dongxia Hu. Influence of structural surface roughness on self-excited oscillation of main amplification system of high power laser device[J]. High Power Laser and Particle Beams, 2020, 32(1): 011020
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