• Acta Optica Sinica
  • Vol. 40, Issue 20, 2014001 (2020)
Peng Hu* and Jianzhu Zhang
Author Affiliations
  • Institute of Applied Physics and Computational Mathematics, Beijing 100088, China
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    DOI: 10.3788/AOS202040.2014001 Cite this Article Set citation alerts
    Peng Hu, Jianzhu Zhang. Analysis of Spatio-Temporal Characters of Thermal Effects of Optical Components in Laser System[J]. Acta Optica Sinica, 2020, 40(20): 2014001 Copy Citation Text show less
    Temperature increase distribution of Si reflective mirror. (a) Maximal temperature increase change with time; (b) radial distribution of surface temperature increase
    Fig. 1. Temperature increase distribution of Si reflective mirror. (a) Maximal temperature increase change with time; (b) radial distribution of surface temperature increase
    RMS of thermal aberration of Si reflective mirror change with time
    Fig. 2. RMS of thermal aberration of Si reflective mirror change with time
    Temperature increase distribution of SiO2 window mirror at different moments. (a) Face absorption; (b) body absorption
    Fig. 3. Temperature increase distribution of SiO2 window mirror at different moments. (a) Face absorption; (b) body absorption
    Thermal effect of SiO2 window mirror change with time. (a) Maximal temperature increase; (b) RMS of thermal aberration
    Fig. 4. Thermal effect of SiO2 window mirror change with time. (a) Maximal temperature increase; (b) RMS of thermal aberration
    Adaptive correction simulation optical path of thermal effect. (a) Reflective mirrors Si; (b) window mirror SiO2
    Fig. 5. Adaptive correction simulation optical path of thermal effect. (a) Reflective mirrors Si; (b) window mirror SiO2
    RMS of thermal aberration under uniform intensity laser irradiation change with time
    Fig. 6. RMS of thermal aberration under uniform intensity laser irradiation change with time
    Normalized peak intensity of far-field under uniform laser irradiation change with time. (a) AO open; (b) AO closed
    Fig. 7. Normalized peak intensity of far-field under uniform laser irradiation change with time. (a) AO open; (b) AO closed
    Laser intensity distribution in experiment
    Fig. 8. Laser intensity distribution in experiment
    Distribution of thermal aberration at 20 s. (a) Reflective mirrors Si; (b) window mirror SiO2
    Fig. 9. Distribution of thermal aberration at 20 s. (a) Reflective mirrors Si; (b) window mirror SiO2
    RMS of thermal aberration under experimental laser irradiation change with time
    Fig. 10. RMS of thermal aberration under experimental laser irradiation change with time
    Normalized peak intensity of far-field under experimental laser irradiation change with time before and after correction. (a) AO open; (b) AO closed
    Fig. 11. Normalized peak intensity of far-field under experimental laser irradiation change with time before and after correction. (a) AO open; (b) AO closed
    MaterialDensity /(kg·m-3)Heat capacity /(J·K-1·kg-1)Thermal conductivity /(W·m-1·K-1)Young's modulus /GPaPoisson ratioThermal expansion /K-1Thermal optic coefficient /K-1
    Si23296951531900.264.68×10-6-
    SiO222007531.4730.170.42×10-61.10×10-5
    Table 1. Physical parameters of the materials
    Peng Hu, Jianzhu Zhang. Analysis of Spatio-Temporal Characters of Thermal Effects of Optical Components in Laser System[J]. Acta Optica Sinica, 2020, 40(20): 2014001
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