• Laser & Optoelectronics Progress
  • Vol. 61, Issue 5, 0500004 (2024)
Luoxian Zhou, Chengyu Zhu*, Hang Yuan, and Lü Zhiwei
Author Affiliations
  • National Key Laboratory of Science and Technology on Tunable Laser, Harbin Institute of Technology, Harbin 150080, Heilongjiang , China
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    DOI: 10.3788/LOP230783 Cite this Article Set citation alerts
    Luoxian Zhou, Chengyu Zhu, Hang Yuan, Lü Zhiwei. Laser Parameters in Laser Shock Processing:Research Progress and Prospect[J]. Laser & Optoelectronics Progress, 2024, 61(5): 0500004 Copy Citation Text show less
    Schematic diagram of basic structure of laser shock processing
    Fig. 1. Schematic diagram of basic structure of laser shock processing
    Pulse-width dependence of damage threshold of a gold grating and a gold mirror [30]
    Fig. 2. Pulse-width dependence of damage threshold of a gold grating and a gold mirror [30]
    Dependence of reflectivity of titanium on wavelength[44]
    Fig. 3. Dependence of reflectivity of titanium on wavelength[44]
    Dependence of optical properties of aluminum on wavelength[47]. (a) Extinction coefficient kM; (b) skin depth δ
    Fig. 4. Dependence of optical properties of aluminum on wavelength[47]. (a) Extinction coefficient kM; (b) skin depth δ
    Dependences of ratio of plasma thermal energy to laser energy α′on power density and pulse width[16]
    Fig. 5. Dependences of ratio of plasma thermal energy to laser energy α′on power density and pulse width[16]
    Effect of wavelength on the curve of maximum pressure and power density (pulse width is 25‒30 ns) [23]
    Fig. 6. Effect of wavelength on the curve of maximum pressure and power density (pulse width is 25‒30 ns) [23]
    Absorbed energy from only first-pulse, only second-pulse, and total-pulses in 100 mJ+100 mJ laser double-pulse[73]
    Fig. 7. Absorbed energy from only first-pulse, only second-pulse, and total-pulses in 100 mJ+100 mJ laser double-pulse[73]
    Maximum pressure of the shock waves caused by combined double-pulse changes with time delay[75]
    Fig. 8. Maximum pressure of the shock waves caused by combined double-pulse changes with time delay[75]
    Year20212009201120201990199920202004
    Pulse width100 fs191 fs200 fs2 ps150 ps600 ps5 ns10 ns
    Intensity /(TW/cm28×10312‒55796371.72.42.5×10-35.5×10-3
    Spot size /μm2940×80122.8101003×1034×1037×103
    Wavelength /μm0.80.80.7550.81.061.0541.0641.06
    Ebergy /mJ0.07‒0.340.61201051.6×1034×104
    Matrrial typeANSI 304 stainless steelSUS 304 stainless steelLow carbon steel

    316 steel,

    316L steel

    Maraging steelLow carbon steel316L steelRolling steel 100Cr6
    Constrained environmentWaterWaterWaterVacuumWater
    Hardness improvement /%2020‒1009.3024,188010
    Influence depth /μm8050100652400
    Reference3637383940414243
    Table 1. Effect of laser parameters on stainless steel in LSP
    Luoxian Zhou, Chengyu Zhu, Hang Yuan, Lü Zhiwei. Laser Parameters in Laser Shock Processing:Research Progress and Prospect[J]. Laser & Optoelectronics Progress, 2024, 61(5): 0500004
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