• Acta Photonica Sinica
  • Vol. 51, Issue 1, 0151104 (2022)
Peng LI*, Xinhao FAN, Yu LI, Sheng LIU, Bingyan WEI, and Jianlin ZHAO
Author Affiliations
  • Shaanxi Key Laboratory of Optical Information Technology,School of Physical Science and Technology,Northwestern Polytechnical University,Xi'an 710129,China
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    DOI: 10.3788/gzxb20225101.0151104 Cite this Article
    Peng LI, Xinhao FAN, Yu LI, Sheng LIU, Bingyan WEI, Jianlin ZHAO. Progress on Longitudinal Modulation of Light Field(Invited)[J]. Acta Photonica Sinica, 2022, 51(1): 0151104 Copy Citation Text show less
    Intensity distributions of Frozen waves with uniform(left)and sinusoidal(right)profiles along propagation direction. Lines:radial and longitudinal intensity profiles[75]
    Fig. 1. Intensity distributions of Frozen waves with uniform(left)and sinusoidal(right)profiles along propagation direction. Lines:radial and longitudinal intensity profiles75
    Longitudinal intensity modulation based on optical metasurface realized by our group[76]
    Fig. 2. Longitudinal intensity modulation based on optical metasurface realized by our group76
    Caustic principle[88]
    Fig. 3. Caustic principle88
    Schematic principle of rays emitted from expanding circles on the input plane intersect on the specified focal curve,and self-accelerating Bessel-like beams[91]
    Fig. 4. Schematic principle of rays emitted from expanding circles on the input plane intersect on the specified focal curve,and self-accelerating Bessel-like beams91
    Illustration showing the accelerative behavior of Airy and radially self-accelerating beams[99]
    Fig. 5. Illustration showing the accelerative behavior of Airy and radially self-accelerating beams99
    Spirally propagating light fields with non-equidistant period produced by the superposition of nonlinear vortex beams[100]
    Fig. 6. Spirally propagating light fields with non-equidistant period produced by the superposition of nonlinear vortex beams100
    Spirally propagating light fields with radially and longitudinally modulated rotations
    Fig. 7. Spirally propagating light fields with radially and longitudinally modulated rotations
    Evolutions of polarization distribution of light fields with the modulation of PB phases[105]
    Fig. 8. Evolutions of polarization distribution of light fields with the modulation of PB phases105
    Longitudinally manipulating the polarization structures of non-diffractive beams
    Fig. 9. Longitudinally manipulating the polarization structures of non-diffractive beams
    Tightly focusing fields of radially polarized light fields with radial binary phase and amplitude modulation
    Fig. 10. Tightly focusing fields of radially polarized light fields with radial binary phase and amplitude modulation
    Generation of light 'cage' and light 'chain' based on the tight focusing of cylindirally polarized beams with modulated polarization and phase
    Fig. 11. Generation of light 'cage' and light 'chain' based on the tight focusing of cylindirally polarized beams with modulated polarization and phase
    Generation of light 'needle' from the tightly focusing of radially polarized Bessel-Gaussian beam[160]
    Fig. 12. Generation of light 'needle' from the tightly focusing of radially polarized Bessel-Gaussian beam160
    Peng LI, Xinhao FAN, Yu LI, Sheng LIU, Bingyan WEI, Jianlin ZHAO. Progress on Longitudinal Modulation of Light Field(Invited)[J]. Acta Photonica Sinica, 2022, 51(1): 0151104
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