• Chinese Physics B
  • Vol. 29, Issue 8, (2020)
Guodong Zhu1, Yangzhe Guo1, Bin Dong2、†, and Yurui Fang1
Author Affiliations
  • 1Key Laboratory of Materials Modification by Laser, Electron, and Ion Beams (Ministry of Education); School of Physics, Dalian University of Technology, Dalian 6024, China
  • 2Key Laboratory of New Energy and Rare Earth Resource Utilization of State Ethnic Affairs Commission, Key Laboratory of Photosensitive Materials & Devices of Liaoning Province, School of Physics and Materials Engineering, Dalian Nationalities University, Dalian 116600, China
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    DOI: 10.1088/1674-1056/ab9698 Cite this Article
    Guodong Zhu, Yangzhe Guo, Bin Dong, Yurui Fang. Quantization of electromagnetic modes and angular momentum on plasmonic nanowires[J]. Chinese Physics B, 2020, 29(8): Copy Citation Text show less
    Schematic illustration of SPPs propagating on a plasmonic cylindrical waveguide, km≡k∥,m=0⋅ρ^+mkϕϕ^+kz,mz^.
    Fig. 1. Schematic illustration of SPPs propagating on a plasmonic cylindrical waveguide, kmk,m=0ρ^+mkϕϕ^+kz,mz^.
    Schematic illustration of the plasmonic cylindrical wire excited by light at one terminal for lower order modes. The light goes along y direction and the polarization is at 45° with the z axis which can be decomposed into x and z components.
    Fig. 2. Schematic illustration of the plasmonic cylindrical wire excited by light at one terminal for lower order modes. The light goes along y direction and the polarization is at 45° with the z axis which can be decomposed into x and z components.
    (a) Schematic illustration of the superposed m = 0 mode and m > 0 modes, which is similar to the vortex waves with l = 1,2,3. The red lines represent the maximum of the beats waves; the lighter lines indicate the beats behind the wire and the darker ones indicate the beats on the reader’s side. (b) The scheme of electric field distributions on plasmonic cylindrical nanowires excited by focusing light on one left terminals with polarization at + 45°(AL), –45°(AR) and 0°(A0) directions to z axis.
    Fig. 3. (a) Schematic illustration of the superposed m = 0 mode and m > 0 modes, which is similar to the vortex waves with l = 1,2,3. The red lines represent the maximum of the beats waves; the lighter lines indicate the beats behind the wire and the darker ones indicate the beats on the reader’s side. (b) The scheme of electric field distributions on plasmonic cylindrical nanowires excited by focusing light on one left terminals with polarization at + 45°(AL), –45°(AR) and 0°(A0) directions to z axis.
    The scheme of electric field distributions on plasmonic cylindrical nanowires excited by focused LCP (ALCP) and RCP (ARCP) light on left ends. The insets show the cross section at the wires at positions i and ii.
    Fig. 4. The scheme of electric field distributions on plasmonic cylindrical nanowires excited by focused LCP (ALCP) and RCP (ARCP) light on left ends. The insets show the cross section at the wires at positions i and ii.
    Guodong Zhu, Yangzhe Guo, Bin Dong, Yurui Fang. Quantization of electromagnetic modes and angular momentum on plasmonic nanowires[J]. Chinese Physics B, 2020, 29(8):
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