• Chinese Optics Letters
  • Vol. 20, Issue 10, 103602 (2022)
Zhongwei Jin1、2, Guiyuan Cao3, Hongtao Wang2, Han Lin3、4, Baohua Jia3、4、5、*, and Cheng-Wei Qiu2、**
Author Affiliations
  • 1College of Optical and Electronic Technology, China Jiliang University, Hangzhou 310018, China
  • 2Department of Electrical and Computer Engineering, National University of Singapore, Singapore 117583, Singapore
  • 3Centre of Translational Atomaterials (CTAM), Faculty of Science, Engineering and Technology, Swinburne University of Technology, Hawthorn, VIC 3122, Australia
  • 4School of Science, RMIT University, Melbourne, VIC 3000, Australia
  • 5The Australian Research Council (ARC) Industrial Transformation Training Centre in Surface Engineering for Advanced Materials (SEAM), Swinburne University of Technology, Hawthorn, VIC 3122, Australia
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    DOI: 10.3788/COL202220.103602 Cite this Article Set citation alerts
    Zhongwei Jin, Guiyuan Cao, Hongtao Wang, Han Lin, Baohua Jia, Cheng-Wei Qiu. Broadband angular momentum cascade via a multifocal graphene vortex generator[J]. Chinese Optics Letters, 2022, 20(10): 103602 Copy Citation Text show less
    Concept and working principle of our rGO broadband multifocal vortex generator (BMVG). (a) Schematic of working principle of our BMVG. (b) Simulated intensity and phase profiles of continuous OAM patterns captured at corresponding focal planes. Scale bar, 4 µm.
    Fig. 1. Concept and working principle of our rGO broadband multifocal vortex generator (BMVG). (a) Schematic of working principle of our BMVG. (b) Simulated intensity and phase profiles of continuous OAM patterns captured at corresponding focal planes. Scale bar, 4 µm.
    Simulated light fields of our BMVG in the x–z plane. (a) Simulated intensity profile in the x–z plane of the light field generated by our BMVG. (b) Zoom-in simulated intensity profiles (x–z plane) of the non-diffracting regions of generated OAM modes from l=1 to l=10.
    Fig. 2. Simulated light fields of our BMVG in the x–z plane. (a) Simulated intensity profile in the x–z plane of the light field generated by our BMVG. (b) Zoom-in simulated intensity profiles (x–z plane) of the non-diffracting regions of generated OAM modes from l=1 to l=10.
    Fabricated sample and measured results of the BMVG. (a) The scanning electronic microscopy (SEM) image of the entire fabricated sample. (b) The topographic profile (top) of the rGO sample measured by an optical profiler and the cross-sectional profile (bottom) marked by the white dashed line in the top image of (b). (c) The interference patterns of the generated OAMs captured before and after the designed focal planes upon 633 nm illumination. Scale bar, 6 µm.
    Fig. 3. Fabricated sample and measured results of the BMVG. (a) The scanning electronic microscopy (SEM) image of the entire fabricated sample. (b) The topographic profile (top) of the rGO sample measured by an optical profiler and the cross-sectional profile (bottom) marked by the white dashed line in the top image of (b). (c) The interference patterns of the generated OAMs captured before and after the designed focal planes upon 633 nm illumination. Scale bar, 6 µm.
    Demonstration of wavelength tunability and focal distance tunability of our BMVG. (a) Simulated and measured interference patterns of generated OAMs captured before (left panel) and after (right panel) z = 450 µm under the incident light of 886 nm, 739 nm, and 633 nm. Scale bar, 6 µm. (b) The measured interference patterns of the generated OAMs under 633 nm (near z = 720 µm), 760 nm (near z = 600 µm), 800 nm (near z = 570 µm), 850 nm (near z = 536 µm), 886 nm (near z = 514 µm), 900 nm (near z = 506 µm), and 1000 nm (near z = 456 µm). Scale bar, 6 µm. (c) The measured interference patterns of the generated OAMs captured before and after the designed focal planes upon 900 nm illumination. Scale bar, 6 µm.
    Fig. 4. Demonstration of wavelength tunability and focal distance tunability of our BMVG. (a) Simulated and measured interference patterns of generated OAMs captured before (left panel) and after (right panel) z = 450 µm under the incident light of 886 nm, 739 nm, and 633 nm. Scale bar, 6 µm. (b) The measured interference patterns of the generated OAMs under 633 nm (near z = 720 µm), 760 nm (near z = 600 µm), 800 nm (near z = 570 µm), 850 nm (near z = 536 µm), 886 nm (near z = 514 µm), 900 nm (near z = 506 µm), and 1000 nm (near z = 456 µm). Scale bar, 6 µm. (c) The measured interference patterns of the generated OAMs captured before and after the designed focal planes upon 900 nm illumination. Scale bar, 6 µm.
    Zhongwei Jin, Guiyuan Cao, Hongtao Wang, Han Lin, Baohua Jia, Cheng-Wei Qiu. Broadband angular momentum cascade via a multifocal graphene vortex generator[J]. Chinese Optics Letters, 2022, 20(10): 103602
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