Advanced Photonics Nexus, Volume. 3, Issue 2, 026003(2024)

Generation of subwavelength inverted pin beam via fiber end integrated plasma structure On the Cover

Zhengchuan Cai1,2、†, Zhiqiang Quan3,4, Libo Yuan1,2, Jian Wang3,4、*, and Houquan Liu1,2、*
Author Affiliations
  • 1Guilin University of Electronic Technology, Photonics Research Center, School of Optoelectronic Engineering, Guilin, China
  • 2Guilin University of Electronic Technology, Guangxi Key Laboratory of Optoelectronic Information Processing, Guilin, China
  • 3Huazhong University of Science and Technology, Wuhan National Laboratory for Optoelectronics and School of Optical and Electronic Information, Wuhan, China
  • 4Optics Valley Laboratory, Wuhan, China
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    Figures & Tables(7)
    (a) 3D schematic diagram of the all-fiber far-field IPB generator. SMF is a single-mode fiber and MMF is a graded index multimode fiber. r1 and r2 in the inset are the inner and external radii of the nanoring slot plasma structures, respectively, and the white circular region denotes the area of the gold film that has been etched. (b) Measurement system for observing the far field of the IPB generated by the fiber-integrated plasma structure.
    Normalized intensity distributions of the output optical field simulated via the analytic equation. (a) Normalized intensity distribution in the x−z plane. (b1)–(b4) Normalized intensity distributions on the x−y plane with different transmission distances of 4, 5, 6, and 7 μm, respectively. (c1)–(c4) Normalized intensity distributions on the x axis extracted from the results of (b1)–(b4), respectively.
    Normalized intensity distributions of the optical field of the MMF. (a) Normalized intensity distribution on the x−z plane. (b) Normalized intensity distribution on the x−y plane after being expanded by 250 μm MMF. (c) Normalized simulation and experimental intensity distributions on the x axis after being expanded by 250 μm MMF.
    Sample characterization. (a) 3D morphology measurement result of the polished fiber end surface. (b) Morphology measurement results along the x axis of the polished fiber end surface. (c) SEM images of the fiber end surface and the nanoring slot.
    (a1)–(a4) Observed intensity distributions of the output light on the x−y plane at z=4, 5, 6, and 7 μm, respectively. (b1)–(b4) Comparison of the simulation and experimental results of the normalized light-intensity distributions along the x axis of z=4, 5, 6, and 7 μm planes. (c) Experimental result of the intensity distribution of the output light on the x−z plane. (d) Variation of the FWHM of the IPB’s main lobe with the propagation distance in different environments. (e) Normalized intensity distributions on the center axis of the IPB in a blood serum environment with different absorption losses.
    (a) Schematic of the nanopetal structure etched on the fiber end surface. (b) SEM image of the nanopetal plasma structure. (c) and (d) Simulation and experimental results of the optical intensity distribution with a propagation distance of 6 μm, respectively.
    Normalized intensity distributions along the x axis of the nanopetal plasma structure with different transmission distances. (a) 4 μm, (b) 5 μm, (c) 6 μm, and (d) 7 μm, respectively. (e) and (f) Comparison of the sidelobe suppression effect of the nanoring slot and nanopetal plasma structures. The proportional value is defined as the ratio of the maximum light intensity of the first-order sidelobe to that of the main lobe.
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    Zhengchuan Cai, Zhiqiang Quan, Libo Yuan, Jian Wang, Houquan Liu. Generation of subwavelength inverted pin beam via fiber end integrated plasma structure[J]. Advanced Photonics Nexus, 2024, 3(2): 026003

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    Paper Information

    Category: Research Articles

    Received: Oct. 7, 2023

    Accepted: Jan. 12, 2024

    Published Online: Feb. 23, 2024

    The Author Email: Wang Jian (jwang@hust.edu.cn), Liu Houquan (houquanliu@163.com)

    DOI:10.1117/1.APN.3.2.026003

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