• Opto-Electronic Advances
  • Vol. 1, Issue 2, 170002 (2018)
Sicong Wang1, Xueying Ouyang1, Ziwei Feng1, Yaoyu Cao1, Min Gu2, and Xiangping Li1、*
Author Affiliations
  • 1Guangdong Provincial Key Laboratory of Optical Fiber Sensing and Communications, Institute of Photonics Technology, Jinan University, Guangzhou 510632, China
  • 2Laboratory of Artificial-Intelligence Nanophotonics and CUDOS (Centre for Ultrahigh bandwidth Devices for Optical Systems), School of Science, RMIT University, Melbourne, Victoria 3001, Australia
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    DOI: 10.29026/oea.2018.170002 Cite this Article
    Sicong Wang, Xueying Ouyang, Ziwei Feng, Yaoyu Cao, Min Gu, Xiangping Li. Diffractive photonic applications mediated by laser reduced graphene oxides[J]. Opto-Electronic Advances, 2018, 1(2): 170002 Copy Citation Text show less
    (a) The chemical structure of a monolayer graphene oxide adapted from the Lerf-Klinowski model18. (b) GO flakes prepared in water solution exhibit brown color before photoreduction and transform into dark color after photoreduction.
    Fig. 1. (a) The chemical structure of a monolayer graphene oxide adapted from the Lerf-Klinowski model18. (b) GO flakes prepared in water solution exhibit brown color before photoreduction and transform into dark color after photoreduction.
    (a) GO exhibits a broadband fluorescence emission ranging from 550 nm to 750 nm. rGO displays similar fluorescence emission but with a reduced intensity14. (b) Dispersion relations of refractive indices and extinction coefficients of GO and rGO films26. (c) Raman spectra of GO before and after reduction exhibit prominent peaks at D (1354 cm-1) and G (1599 cm-1) bands14. XPS spectra of GO before (d) and after reduction (e)15.
    Fig. 2. (a) GO exhibits a broadband fluorescence emission ranging from 550 nm to 750 nm. rGO displays similar fluorescence emission but with a reduced intensity14. (b) Dispersion relations of refractive indices and extinction coefficients of GO and rGO films26. (c) Raman spectra of GO before and after reduction exhibit prominent peaks at D (1354 cm-1) and G (1599 cm-1) bands14. XPS spectra of GO before (d) and after reduction (e)15.
    (a) Schematic illustration of photoreduction and patterning of GO through direct laser writing techniques. Optical microscopic images of patterned rGO samples by femtosecond-pulsed laser beams with a high repetition rate of 80 MHz (b)6 and highly spatially confined reduction by single femtosecond pulses (c).
    Fig. 3. (a) Schematic illustration of photoreduction and patterning of GO through direct laser writing techniques. Optical microscopic images of patterned rGO samples by femtosecond-pulsed laser beams with a high repetition rate of 80 MHz (b)6 and highly spatially confined reduction by single femtosecond pulses (c).
    (a) Retrieved fluorescence image of two patterns recorded through two-photon photoreduction in two layers in GO-polymer sample separated by a spacing of 20 μm. The scale bar is 10 μm14. (b) A complex grayscale photograph patterned through LightScribe methods35.
    Fig. 4. (a) Retrieved fluorescence image of two patterns recorded through two-photon photoreduction in two layers in GO-polymer sample separated by a spacing of 20 μm. The scale bar is 10 μm14. (b) A complex grayscale photograph patterned through LightScribe methods35.
    (a) Schematic illustration of the laser-patterned rGO planar lens13. (b) Topographic profile of the rGO planar lens prepared by direct laser writing methods13. (c) Simulated and experimental results of the intensity distributions of the focal field in the lateral and axial directions13.
    Fig. 5. (a) Schematic illustration of the laser-patterned rGO planar lens13. (b) Topographic profile of the rGO planar lens prepared by direct laser writing methods13. (c) Simulated and experimental results of the intensity distributions of the focal field in the lateral and axial directions13.
    (a) Schematic illustration of subwavelength scale and continuously tunable phase modulation in rGO holograms for full-color 3D displays achieved by exquisitely controllable photoreduction15. (b) Photograph of a rGO hologram recorded in a GO-dispersed sample15. (c) The optical image of the rGO holograms generated by laser reduction14. (d) CCD-captured images by focusing at different depths of reconstructed 3D objects, two teapots15. (e) Reconstructed color images of two balloons by rGO-polymer holograms through wavelength multiplexing15.
    Fig. 6. (a) Schematic illustration of subwavelength scale and continuously tunable phase modulation in rGO holograms for full-color 3D displays achieved by exquisitely controllable photoreduction15. (b) Photograph of a rGO hologram recorded in a GO-dispersed sample15. (c) The optical image of the rGO holograms generated by laser reduction14. (d) CCD-captured images by focusing at different depths of reconstructed 3D objects, two teapots15. (e) Reconstructed color images of two balloons by rGO-polymer holograms through wavelength multiplexing15.
    Sicong Wang, Xueying Ouyang, Ziwei Feng, Yaoyu Cao, Min Gu, Xiangping Li. Diffractive photonic applications mediated by laser reduced graphene oxides[J]. Opto-Electronic Advances, 2018, 1(2): 170002
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