Chinese Journal of Lasers, Volume. 50, Issue 12, 1202201(2023)

Picosecond Laser Ablation of Glass Surface by Dual‑Pulse Temporal Shaping

Wenfeng Liu1,2, Mingying Sun1、*, Yiqun Shi1,2, Yajing Guo1, Yingming Xu1,2, Zhaoyang Jiao1, Zijian Cui1, and Jianqiang Zhu1、**
Author Affiliations
  • 1National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
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    Figures & Tables(12)
    Schematic of picosecond dual-pulse laser ablation test platform (HWP: half wave-plate; QWP: quarter wave-plate; HR: high reflectance mirror; PBS: polarization beam splitter. The insert shows focal spot of dual-pulse recorded by beam analyzer)
    Variation of ablation morphology with increasing laser fluence under different shapes of dual-pulse radiation. (a0)-(d0) Dual-pulse train with various shape factors; (a1)-(a4) ablation morphology of glass under different laser fluences when η=0; (b1)-(b4) ablation morphology of glass under different laser fluence when η=0.33; (c1)-(c4) ablation morphology of glass under different laser fluences when η=0.50; (d1)-(d4) ablation morphology of glass under different laser fluences when η=0.67
    Optical microscopy images and SEM images of four types of representative ablation morphologies. (a1)-(d1) Optical microscopy images; (a2)-(d2) SEM images; (a3)-(d3) detail enlargement of SEM images
    Distribution of five kinds of dual-pulse ablation morphologies in different pump and probe fluences
    Size definition of typical dual-pulse ablation morphologies. (a) Ablation morphology for phase Ⅳ; (b) ablation morphology for phase Ⅴ
    Under dual-pulse irradiation with different shapes, Dcore2 and Douter2 as a function of laser fluence. (a)(d) Dcore2 and Douter2 as a function of pump fluence; (b)(e) Dcore2 and Douter2 as a function of probe fluence; (c)(f) Dcore2 and Douter2 as a function of train-pulse fluence
    Ablation size of core and outer rings as a function of train-pulse fluence with η=0.5
    Relation between ablation threshold and shape factor for dual-pulse train
    Relationship between ablation morphology and laser fluence for different pulse intervals of dual-pulse with η=0.50. (a) Pulse interval of 333 ps; (b) pulse interval of 667 ps
    Under dual-pulse with η=0.50, relationship between ablation size and laser fluence for different pulse intervals of dual-pulse. (a) Dcore2 as a function of pump fluence; (b) Douter2 as a function of train-pulse fluence
    Schematics of ablation process of K9 glass by picosecond dual-pulse. (a) Ablation morphologies for phases Ⅰ and Ⅱ; (b) ablation morphology for phase Ⅲ; (c) ablation morphology for phase Ⅳ; (d) ablation morphology for phase Ⅴ
    • Table 1. Focus spot radius and ablation threshold obtained according fitting curves

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      Table 1. Focus spot radius and ablation threshold obtained according fitting curves

      Fitting curveFocus spot radius ω0 /μmAblation threshold /(J·cm-2
      Dcore-F38.220.4
      Douter-F44.013.7
      Single pulse38.59.5
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    Wenfeng Liu, Mingying Sun, Yiqun Shi, Yajing Guo, Yingming Xu, Zhaoyang Jiao, Zijian Cui, Jianqiang Zhu. Picosecond Laser Ablation of Glass Surface by Dual‑Pulse Temporal Shaping[J]. Chinese Journal of Lasers, 2023, 50(12): 1202201

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    Paper Information

    Category: Laser Surface Machining

    Received: Sep. 13, 2022

    Accepted: Nov. 9, 2022

    Published Online: Jun. 6, 2023

    The Author Email: Sun Mingying (sunmy@siom.ac.cn), Zhu Jianqiang (jqzhu@siom.ac.cn)

    DOI:10.3788/CJL221235

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