• Laser & Optoelectronics Progress
  • Vol. 58, Issue 3, 3140021 (2021)
Lin Yuhan, Shi Hui, and Jia Tianqing*
Author Affiliations
  • State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200241, China
  • show less
    DOI: 10.3788/LOP202158.0314002 Cite this Article Set citation alerts
    Lin Yuhan, Shi Hui, Jia Tianqing. Distortion and Light Intensity Correction for Spatiotemporal-Interference-Based Spatial Shaping[J]. Laser & Optoelectronics Progress, 2021, 58(3): 3140021 Copy Citation Text show less
    Experimental setup of spatiotemporal-interference-based femtosecond laser shaping
    Fig. 1. Experimental setup of spatiotemporal-interference-based femtosecond laser shaping
    Simulation results. (a) Relative distortion fitting curve of l-q(l); (b)(c) gridded phase holograms before and after distortion correction, respectively; (d)(e) distribution of irradiance at the simulated sample when Figs. (b) and (c) are loaded on SLM
    Fig. 2. Simulation results. (a) Relative distortion fitting curve of l-q(l); (b)(c) gridded phase holograms before and after distortion correction, respectively; (d)(e) distribution of irradiance at the simulated sample when Figs. (b) and (c) are loaded on SLM
    Gauss Amp fitting curve for relative light intensity distribution of circular light field after the contraction
    Fig. 3. Gauss Amp fitting curve for relative light intensity distribution of circular light field after the contraction
    Simulation results. (a)(d) Circular phase holograms before and after light-intensity correction; (b)(c) two-dimensional and one-dimensional simulated light intensity distributions when loading Fig. (a) on SLM, total power is 1.619×10-1 W; (e)(f) two-dimensional and one-dimensional simulated light intensity distributions when loading Fig. (d) on SLM, total power is 1.352×10-1 W
    Fig. 4. Simulation results. (a)(d) Circular phase holograms before and after light-intensity correction; (b)(c) two-dimensional and one-dimensional simulated light intensity distributions when loading Fig. (a) on SLM, total power is 1.619×10-1 W; (e)(f) two-dimensional and one-dimensional simulated light intensity distributions when loading Fig. (d) on SLM, total power is 1.352×10-1 W
    Simulation result. (a)(d) Striped phase holograms before and after distortion and light-intensity correction; (b)(c) two-dimensional and one-dimensional simulated light intensity distributions when loading Fig. (a) on SLM, total power is 6.995×10-2 W; (e)(f) two-dimensional and one-dimensional simulated light intensity distributions when loading Fig. (d) on SLM, total power is 5.073×10-2 W; (g)(h) stainless steel surface processing images,when loading Fig. (a) or (d)
    Fig. 5. Simulation result. (a)(d) Striped phase holograms before and after distortion and light-intensity correction; (b)(c) two-dimensional and one-dimensional simulated light intensity distributions when loading Fig. (a) on SLM, total power is 6.995×10-2 W; (e)(f) two-dimensional and one-dimensional simulated light intensity distributions when loading Fig. (d) on SLM, total power is 5.073×10-2 W; (g)(h) stainless steel surface processing images,when loading Fig. (a) or (d)
    Edge images of laser processing results before and after correction. (a)Before correction; (b)after correction
    Fig. 6. Edge images of laser processing results before and after correction. (a)Before correction; (b)after correction
    Long stripe structure on a 500 μm thick silicon formed by stitching
    Fig. 7. Long stripe structure on a 500 μm thick silicon formed by stitching
    Simulation results. (a)(b) Two phase holograms when processing a single pixel of a QR code; (c) two-dimensional simulated light intensity distributions when loading Fig. (a) on SLM, peak irradiance is 2.077×103 W/cm2; (d) QR code structure on stainless steel surface; (e) zoom in the view of the QR code structure
    Fig. 8. Simulation results. (a)(b) Two phase holograms when processing a single pixel of a QR code; (c) two-dimensional simulated light intensity distributions when loading Fig. (a) on SLM, peak irradiance is 2.077×103 W/cm2; (d) QR code structure on stainless steel surface; (e) zoom in the view of the QR code structure
    Observation results. (a)LIPSS image inside QR code structure; (b)legend for measuring the LIPSS cycle
    Fig. 9. Observation results. (a)LIPSS image inside QR code structure; (b)legend for measuring the LIPSS cycle
    Schematic of observation method for the QR code structural color
    Fig. 10. Schematic of observation method for the QR code structural color
    Images obtained from the structure on the stainless steel surface of different α varied from large to small
    Fig. 11. Images obtained from the structure on the stainless steel surface of different α varied from large to small
    ItemValueStandard deviation
    I00.3361.66×10-3
    w42.1099.17×10-2
    A0.6581.57×10-3
    Table 1. Gauss Amp fitting solution and its standard deviation for relative light intensity distribution of circular light field after the contraction
    Lin Yuhan, Shi Hui, Jia Tianqing. Distortion and Light Intensity Correction for Spatiotemporal-Interference-Based Spatial Shaping[J]. Laser & Optoelectronics Progress, 2021, 58(3): 3140021
    Download Citation