• Laser & Optoelectronics Progress
  • Vol. 57, Issue 11, 111403 (2020)
Yuedong Li, Weiyi Yin, and Ye Dai*
Author Affiliations
  • Department of Physics, Shanghai University, Shanghai 200444, China
  • show less
    DOI: 10.3788/LOP57.111403 Cite this Article Set citation alerts
    Yuedong Li, Weiyi Yin, Ye Dai. Research Progress on Spatio-Temporal Coupling of Femtosecond Pulse Laser for Direct-Writing Nanograting[J]. Laser & Optoelectronics Progress, 2020, 57(11): 111403 Copy Citation Text show less
    Introduction of AD and SC. (a) Prism; (b) grating
    Fig. 1. Introduction of AD and SC. (a) Prism; (b) grating
    Temporal chirp
    Fig. 2. Temporal chirp
    Two sources of pulse-front tilt. (a) Angular dispersion; (b) combination of spatial and temporal chirp[49]
    Fig. 3. Two sources of pulse-front tilt. (a) Angular dispersion; (b) combination of spatial and temporal chirp[49]
    Principle of femtosecond laser SSTF technology[56]
    Fig. 4. Principle of femtosecond laser SSTF technology[56]
    Comparison of nonlinear effect at different areas between common focusing and spatio-temporal focusing conditions. (a) Without spatially chirped pulses, self-focusing and supercontinuum generation result in a loss of intensity at the focus; (b) with spatially chirped pulses, self-focusing and continuum generation are suppressed[28]
    Fig. 5. Comparison of nonlinear effect at different areas between common focusing and spatio-temporal focusing conditions. (a) Without spatially chirped pulses, self-focusing and supercontinuum generation result in a loss of intensity at the focus; (b) with spatially chirped pulses, self-focusing and continuum generation are suppressed[28]
    Image of 2 mm height lion sculpture. (a) SEM image in the front view of sculpture; (b) front view of the original model; (c) SEM image of the head of fabricated lion; (d) head of the original model exhibited from the same angle of view[60]
    Fig. 6. Image of 2 mm height lion sculpture. (a) SEM image in the front view of sculpture; (b) front view of the original model; (c) SEM image of the head of fabricated lion; (d) head of the original model exhibited from the same angle of view[60]
    Schematic of four-dimensional optical shaping. (a) Optical experimental setup; (b) relationship between conventional focus and SSTF, as well as single focus and holographic 3D multiplexed[44]
    Fig. 7. Schematic of four-dimensional optical shaping. (a) Optical experimental setup; (b) relationship between conventional focus and SSTF, as well as single focus and holographic 3D multiplexed[44]
    Nonreciprocal direct writing phenomenon. (a) Orthogonal polarization and differential interference images of the lines written with orthogonal polarizations; (b) SEM images of cross sections of lines written with polarization perpendicular to writing direction[32]
    Fig. 8. Nonreciprocal direct writing phenomenon. (a) Orthogonal polarization and differential interference images of the lines written with orthogonal polarizations; (b) SEM images of cross sections of lines written with polarization perpendicular to writing direction[32]
    Glass modification under the influence of PFT. (a) Orientation of the pulse front tilt at the focal plane (dashed line);blue arrow is the writing direction, E is the polarization direction, in Fig. (b)-(d), each set of anti-parallel lines was imaged with bright field (top) and cross-polarized illumination (bottom); scale bar is 50 μm[33]
    Fig. 9. Glass modification under the influence of PFT. (a) Orientation of the pulse front tilt at the focal plane (dashed line);blue arrow is the writing direction, E is the polarization direction, in Fig. (b)-(d), each set of anti-parallel lines was imaged with bright field (top) and cross-polarized illumination (bottom); scale bar is 50 μm[33]
    Dependence of orientation of induced nanogating on PFT of femtosecond laser. (a) SEM images of self-organized nanogratings in transversal cross-section of the written lines with varied polarization plane azimuth(red curve highlights the varying trend for the longitudinal length of nanogratings); (b) SEM images of the written nanogratings in the transversal cross-section with two opposite scan directions; (c) schematic of 3D rotation of nanogratings[62]
    Fig. 10. Dependence of orientation of induced nanogating on PFT of femtosecond laser. (a) SEM images of self-organized nanogratings in transversal cross-section of the written lines with varied polarization plane azimuth(red curve highlights the varying trend for the longitudinal length of nanogratings); (b) SEM images of the written nanogratings in the transversal cross-section with two opposite scan directions; (c) schematic of 3D rotation of nanogratings[62]
    Asymmetric microstructures induced by spatially chirped pulse in fused silica. (a)(c) Optical images of transverse sections of the asymmetric microstructures with tilted heads induced by the laser pulses; corresponding to the processing diagram (b) without a Dove prism and (d) with a Dove prism[39]
    Fig. 11. Asymmetric microstructures induced by spatially chirped pulse in fused silica. (a)(c) Optical images of transverse sections of the asymmetric microstructures with tilted heads induced by the laser pulses; corresponding to the processing diagram (b) without a Dove prism and (d) with a Dove prism[39]
    Different laser fluence distributions at the focus with varied coupling parameters. (a)(c)(e) Coupling parameter, respectively p=(14+0.7i) fs/μm, p=(0.2+2i) fs/μm, and p=(-13.8-3.7i)fs/μm; (b)(d)(f) corresponding control group[52]
    Fig. 12. Different laser fluence distributions at the focus with varied coupling parameters. (a)(c)(e) Coupling parameter, respectively p=(14+0.7i) fs/μm, p=(0.2+2i) fs/μm, and p=(-13.8-3.7i)fs/μm; (b)(d)(f) corresponding control group[52]
    Yuedong Li, Weiyi Yin, Ye Dai. Research Progress on Spatio-Temporal Coupling of Femtosecond Pulse Laser for Direct-Writing Nanograting[J]. Laser & Optoelectronics Progress, 2020, 57(11): 111403
    Download Citation