• High Power Laser Science and Engineering
  • Vol. 1, Issue 1, 01000036 (2013)
Hongji Qi, Meipin Zhu, Ming Fang, Shuying Shao, Chaoyang Wei, Kui Yi, and and Jianda Shao*
Author Affiliations
  • Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
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    DOI: 10.1017/hpl.2013.6 Cite this Article Set citation alerts
    Hongji Qi, Meipin Zhu, Ming Fang, Shuying Shao, Chaoyang Wei, Kui Yi, and Jianda Shao. Development of high-power laser coatings[J]. High Power Laser Science and Engineering, 2013, 1(1): 01000036 Copy Citation Text show less
    Temperature and electric field distribution in a high-reflectance coating with and without interface absorption.
    Fig. 1. Temperature and electric field distribution in a high-reflectance coating with and without interface absorption.
    Designed and measured transmittance spectra of polarizer.
    Fig. 2. Designed and measured transmittance spectra of polarizer.
    Measured transmittance spectra of polarizer for three runs.
    Fig. 3. Measured transmittance spectra of polarizer for three runs.
    Surface morphology of fused silica before and after annealing treatment .
    Fig. 4. Surface morphology of fused silica before and after annealing treatment .
    Surface morphology of BK7 glass cleaned by different methods examined by an AFM: (a) manually swabbing with lint-free wipes, (b) ultrasonic cleaning, (c) acid solvent etching.
    Fig. 5. Surface morphology of BK7 glass cleaned by different methods examined by an AFM: (a) manually swabbing with lint-free wipes, (b) ultrasonic cleaning, (c) acid solvent etching.
    LIDT of antireflection coating with different cleaning methods (532 nm, , 10 ns).
    Fig. 6. LIDT of antireflection coating with different cleaning methods (532 nm, , 10 ns).
    Optimization of deposition process.
    Fig. 7. Optimization of deposition process.
    Measured LIDT of high-reflectance coating with different pre-melting processes.
    Fig. 8. Measured LIDT of high-reflectance coating with different pre-melting processes.
    Number of damage site and damage morphology without and with laser conditioning.
    Fig. 9. Number of damage site and damage morphology without and with laser conditioning.
    Absorption, defect density, and LIDT of coating with and without post-plasma treatment.
    Fig. 10. Absorption, defect density, and LIDT of coating with and without post-plasma treatment.
    Typical damage morphology with a fluence of (p-polarized wave), (p- and s-polarized waves).
    Fig. 11. Typical damage morphology with a fluence of (p-polarized wave), (p- and s-polarized waves).
    LIDT versus peak electric field for four kinds of polarizer: (a) p-polarized wave, (b) s-polarized wave.
    Fig. 12. LIDT versus peak electric field for four kinds of polarizer: (a) p-polarized wave, (b) s-polarized wave.
    LIDT of polarizer beam splitter for a p-polarized wave in the 2012 damage competition of XLIV Annual Boulder Damage Symposium[14].
    Fig. 13. LIDT of polarizer beam splitter for a p-polarized wave in the 2012 damage competition of XLIV Annual Boulder Damage Symposium[14].
    Dependence of residual stress of the coating on the deposition parameters.
    Fig. 14. Dependence of residual stress of the coating on the deposition parameters.
    Schematic diagram of the in situ stress measurement system.
    Fig. 15. Schematic diagram of the in situ stress measurement system.
    Typical stress evolution curve of and films recorded with the in situ stress measurement system.
    Fig. 16. Typical stress evolution curve of and films recorded with the in situ stress measurement system.
    Hongji Qi, Meipin Zhu, Ming Fang, Shuying Shao, Chaoyang Wei, Kui Yi, and Jianda Shao. Development of high-power laser coatings[J]. High Power Laser Science and Engineering, 2013, 1(1): 01000036
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