• Acta Optica Sinica
  • Vol. 40, Issue 1, 0111016 (2020)
Qiongyao Li, Bamao Zhaxi, Ziyang Chen, and Jixiong Pu*
Author Affiliations
  • Fujian Province Key Laboratory of Light Propagation and Transformation, College of Information Science and Engineering, Huaqiao University, Xiamen, Fujian 361021, China
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    DOI: 10.3788/AOS202040.0111016 Cite this Article Set citation alerts
    Qiongyao Li, Bamao Zhaxi, Ziyang Chen, Jixiong Pu. Focusing of Laser Through Strong Scattering Media with Different Thicknesses[J]. Acta Optica Sinica, 2020, 40(1): 0111016 Copy Citation Text show less
    Schematics of focusing of incident laser after passing through scattering medium by modulating wavefront. (a) Random speckle formed by plane wave passing through scattering medium; (b) focal spot formed at specific position by modulated incident laser passing through scattering medium
    Fig. 1. Schematics of focusing of incident laser after passing through scattering medium by modulating wavefront. (a) Random speckle formed by plane wave passing through scattering medium; (b) focal spot formed at specific position by modulated incident laser passing through scattering medium
    Flow chart of unit phase modulation using continuous sequential algorithm. M represents segment under modulating, O represents segment without phase modulation, and B represents segment after optimization
    Fig. 2. Flow chart of unit phase modulation using continuous sequential algorithm. M represents segment under modulating, O represents segment without phase modulation, and B represents segment after optimization
    Schematic of experimental setup
    Fig. 3. Schematic of experimental setup
    Scattering medium samples with different thicknesses
    Fig. 4. Scattering medium samples with different thicknesses
    Images of random speckles formed by unmodulated incident laser passing through scattering media with different thicknesses. (a) 50 μm; (b) 100 μm; (c) 150 μm; (d) 200 μm; (e) 250 μm
    Fig. 5. Images of random speckles formed by unmodulated incident laser passing through scattering media with different thicknesses. (a) 50 μm; (b) 100 μm; (c) 150 μm; (d) 200 μm; (e) 250 μm
    Focused spots produced by phase-modulated laser passing through scattering media with different thicknesses. (a) 50 μm; (b) 100 μm; (c) 150 μm; (d) 200 μm; (e) 250 μm
    Fig. 6. Focused spots produced by phase-modulated laser passing through scattering media with different thicknesses. (a) 50 μm; (b) 100 μm; (c) 150 μm; (d) 200 μm; (e) 250 μm
    Phase patterns of incident laser wavefront used for generating focal spots which are shown in Fig. 6(a)-(e). (a) 50 μm; (b) 100 μm; (c) 150 μm; (d) 200 μm; (e) 250 μm
    Fig. 7. Phase patterns of incident laser wavefront used for generating focal spots which are shown in Fig. 6(a)-(e). (a) 50 μm; (b) 100 μm; (c) 150 μm; (d) 200 μm; (e) 250 μm
    Enhancement factor of intensity at focal point as a function of thickness of scattering medium
    Fig. 8. Enhancement factor of intensity at focal point as a function of thickness of scattering medium
    Qiongyao Li, Bamao Zhaxi, Ziyang Chen, Jixiong Pu. Focusing of Laser Through Strong Scattering Media with Different Thicknesses[J]. Acta Optica Sinica, 2020, 40(1): 0111016
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