High Power Laser Science and Engineering, Volume. 13, Issue 4, 04000e64(2025)

Pulse-length dependence of the laser-induced damage behavior of a fused-silica antireflective metasurface

Kyle R. P. Kafka, Brittany Hoffman, Hu Huang, Alexei Kozlov, Marek Stehlik, and Stavros G. Demos
Author Affiliations
  • Laboratory for Laser Energetics, https://ror.org/022kthw22University of Rochester, Rochester, NY, USA
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    Figures & Tables(9)
    Scanning electron micrographs of the RAR metasurface without laser exposure, showing (a) side view at 60° from normal and (b) top view. Note that the bulbous appearance of the tips of the structures is an artifact of the platinum coating process required for imaging and that the actual features are more pointed.
    SEM images of an example site formed by 1.4-ns pulse duration, at 24 J/cm2. (a) Overview of the entire damage site, (b) zoom-in as indicated in yellow, (c) further zoom-in as indicated in the white dashed region showing the modified nanostructure, as compared with (d) the pristine location on the same scale. (e) Further zoom-in, as indicated in green, showing elongated features in the crater.
    Images of a damage site formed by 10-ps pulse duration, at 2.6 J/cm2. (a) DIC microscope image overview, (b) SE-SEM image of a region showing two types of damages, which are further magnified to show the (c) larger type in the solid-line region and (d) smaller type in the dashed line region. Both (c) and (d) are BSE-SEM images.
    Images of a damage site formed by 0.8-ps pulse duration, at 2.4 J/cm2. (a) DIC image overview, (b) SE-SEM image near the center of the site and (c) BSE-SEM image of the solid-line region, magnifying the shallow damage pits.
    Images of a damage site formed by 100 pulses of 20-fs duration, at 1.1 J/cm2, collected via (a) in situ dark-field microscopy, (b) DIC microscopy and (c) SEM. The rectangle in (a) corresponds to the imaged region of (b) and (c), indicating detected modifications not observed in DIC and SEM images.
    Fluorescence microscopy images of 20-fs, 100-on-1 damage sites on an RAR silica sample, organized by femtosecond-laser fluence (horizontal) and excitation wavelength of the microscope (vertical). The fluorescence signal was integrated for wavelengths of more than 400 nm.
    Experimental LIDT results. (a) All measured LIDT values as a function of pulse duration. (b) Ratio of LIDT values from multipulse tests (R-on-1 or 100-on-1) divided by those of single-pulse tests (1-on-1). (c) Ratio of LIDT values of the RAR samples divided by those of the untextured samples. Additional data points for 20-fs duration correspond to an additional sample.
    Simulated metasurface shape and example cross-sectional color maps of EFI distribution. (a) Perspective view of the structure. (b) Example side-view cross-section, with the top (black) showing the structure and the bottom (color) mapping the EFI, with laser polarization directed into the page. (c) Example top-view cross-section mapping the EFI at a height in the middle of the nanopillars, with laser polarization oriented vertically. Black indicates the location of air/vacuum.
    • Table 1. Summary of parameters used in the three laser-induced damage-testing systems.

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      Table 1. Summary of parameters used in the three laser-induced damage-testing systems.

      WavelengthAngle ofTest
      System(nm)incidenceambiencePulse durationTest protocols
      ns1053Air1.4 ns1-on-1, R-on-1
      ps1053Vacuum10 ps, 0.8 ps1-on-1, R-on-1
      fs900Vacuum20 fs1-on-1, 100-on-1
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    Kyle R. P. Kafka, Brittany Hoffman, Hu Huang, Alexei Kozlov, Marek Stehlik, Stavros G. Demos. Pulse-length dependence of the laser-induced damage behavior of a fused-silica antireflective metasurface[J]. High Power Laser Science and Engineering, 2025, 13(4): 04000e64

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    Paper Information

    Category: Research Articles

    Received: Mar. 8, 2025

    Accepted: May. 15, 2025

    Published Online: Sep. 23, 2025

    The Author Email:

    DOI:10.1017/hpl.2025.10036

    CSTR:32185.14.hpl.2025.10036

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