• High Power Laser Science and Engineering
  • Vol. 10, Issue 6, 06000e42 (2022)
Kun Shuai1、2, Xiaofeng Liu2, Yuanan Zhao2、*, Keqiang Qiu3, Dawei Li2, He Gong4, Jian Sun2, Li Zhou5, Youen Jiang5, Yaping Dai6, Jianda Shao2、7, and Zhilin Xia1
Author Affiliations
  • 1School of Materials Science and Engineering, Wuhan University of Technology, Wuhan, China
  • 2Laboratory of Thin Film Optics, Shanghai Institute of Optics and Fine Mechanics, Shanghai, China
  • 3National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei, China
  • 4School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai, China
  • 5National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, CAS, Shanghai, China
  • 6Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang, China
  • 7Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou, China
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    DOI: 10.1017/hpl.2022.34 Cite this Article Set citation alerts
    Kun Shuai, Xiaofeng Liu, Yuanan Zhao, Keqiang Qiu, Dawei Li, He Gong, Jian Sun, Li Zhou, Youen Jiang, Yaping Dai, Jianda Shao, Zhilin Xia. Multilayer dielectric grating pillar-removal damage induced by a picosecond laser[J]. High Power Laser Science and Engineering, 2022, 10(6): 06000e42 Copy Citation Text show less
    (a) Schematic representation of the MLDG and (b) the –1st-order diffraction efficiency of the MLDG; the inset shows an SEM image of the pristine cross-sectional morphology of the MLDG. The measured grating period T = 580 nm, mid-waist duty cycle ƒ = 0.38, groove depth D = 415 nm and base angle of the grating pillar θ = 87°.
    Fig. 1. (a) Schematic representation of the MLDG and (b) the –1st-order diffraction efficiency of the MLDG; the inset shows an SEM image of the pristine cross-sectional morphology of the MLDG. The measured grating period T = 580 nm, mid-waist duty cycle ƒ = 0.38, groove depth D = 415 nm and base angle of the grating pillar θ = 87°.
    Damage probability fitting curve of MLDGs under one-on-one test mode. The LIDT of the MLDGs was 2.2 J/cm2 irradiated by an 8.6 ps-pulsed laser with the wavelength of 1053 nm.
    Fig. 2. Damage probability fitting curve of MLDGs under one-on-one test mode. The LIDT of the MLDGs was 2.2 J/cm2 irradiated by an 8.6 ps-pulsed laser with the wavelength of 1053 nm.
    SEM images of typical damage morphology characteristics of the MLDGs. (a) Top-view image of the damage area irradiation by the ps-pulsed laser, and (b)–(d) are the local magnified views of the three black rectangular areas in (a). The test laser irradiated the surface from left to right with a fluence of 3.3 J/cm2.
    Fig. 3. SEM images of typical damage morphology characteristics of the MLDGs. (a) Top-view image of the damage area irradiation by the ps-pulsed laser, and (b)–(d) are the local magnified views of the three black rectangular areas in (a). The test laser irradiated the surface from left to right with a fluence of 3.3 J/cm2.
    Two-dimensional finite-element strain simulation model and calculation results. (a) Schematic representation of the eruptive impact process; the localized eruption of the left-hand pillar induced a rightward impact pressure on the right-hand pillar. (b), (c) Normal stress distributions along the y- and x-axis directions, and , of the right-hand pillar in (a), respectively. Positive values are tensile stresses and negative values are compressive stresses.
    Fig. 4. Two-dimensional finite-element strain simulation model and calculation results. (a) Schematic representation of the eruptive impact process; the localized eruption of the left-hand pillar induced a rightward impact pressure on the right-hand pillar. (b), (c) Normal stress distributions along the y- and x-axis directions, and , of the right-hand pillar in (a), respectively. Positive values are tensile stresses and negative values are compressive stresses.
    (a) Schematic representation of the electric field simulation model and (b) laser electric field distribution in MLDGs. The incident laser pulse is centered at 1053 nm, and its pulse width is 8.6 ps.
    Fig. 5. (a) Schematic representation of the electric field simulation model and (b) laser electric field distribution in MLDGs. The incident laser pulse is centered at 1053 nm, and its pulse width is 8.6 ps.
    Evolution of the electronic density in the conduction band. The rectangular, circular and triangular shapes represent the sampling point curves on the upper inset image. The calculation time is three times that of the laser pulse width.
    Fig. 6. Evolution of the electronic density in the conduction band. The rectangular, circular and triangular shapes represent the sampling point curves on the upper inset image. The calculation time is three times that of the laser pulse width.
    Calculation of the eruptive pressure in the MLDGs. The time step adopted was 10% that the pulse width. (a) Evolution of the eruptive pressure distribution on the right-hand side ridge and (b) distribution of the eruptive pressure in the grating when The red line in the inset image indicates the sampling boundary for eruptive pressure in (a).
    Fig. 7. Calculation of the eruptive pressure in the MLDGs. The time step adopted was 10% that the pulse width. (a) Evolution of the eruptive pressure distribution on the right-hand side ridge and (b) distribution of the eruptive pressure in the grating when The red line in the inset image indicates the sampling boundary for eruptive pressure in (a).
    LocationDamage characteristics
    Overall arrangementDamaged pillars arranged in the horizontal
    direction
    Groove‘Foggy’ region that spreads to the right
    Left-hand pillarIncomplete collapse toward the left
    Right-hand pillarFracture from the root
    Table 1. Morphological characteristics of the adjacent damaged pillars.
    VariablesMaterials
    SiO2HfO2

    ${n}_{\mathrm{e}0}\left({\mathrm{m}}^{-3}\right)^{\phantom{A^A}}$

    1 × 1010

    $e\;\left(\mathrm{C}\right)$

    1.6 × 10–19

    ${m}_{\mathrm{e}}\;\left(\mathrm{kg}\right)$

    9.1 × 10–31

    ${\tau}_{\mathrm{k}}\;\left(\mathrm{fs}\right)$

    4

    $n$

    1.421.86

    ${E}_{\mathrm{g}}\;\left(\mathrm{eV}\right)$

    8.55.5

    ${K}_{\mathrm{i}}(\mathrm{W}/\left(\mathrm{m} \cdot \mathrm{K}\right))$

    1.41.1

    ${C}_{\mathrm{i}}(\mathrm{J}/\left(\mathrm{kg} \cdot \mathrm{K}\right))$

    670120
    Density (

    $\mathrm{kg}/{\mathrm{m}}^3$

    )
    22009680
    Table 2. Material parameters used in the calculation[31].
    Kun Shuai, Xiaofeng Liu, Yuanan Zhao, Keqiang Qiu, Dawei Li, He Gong, Jian Sun, Li Zhou, Youen Jiang, Yaping Dai, Jianda Shao, Zhilin Xia. Multilayer dielectric grating pillar-removal damage induced by a picosecond laser[J]. High Power Laser Science and Engineering, 2022, 10(6): 06000e42
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