• Acta Physica Sinica
  • Vol. 69, Issue 5, 054201-1 (2020)
Xiao-Lei Wang1, Jie-Hui Zhao1, Miao Li2, Guang-Ke Jiang1, Xiao-Xue Hu1, Nan Zhang1, Hong-Chen Zhai1, and Wei-Wei Liu1、*
Author Affiliations
  • 1Institute of Modern Optics, College of Electronic Information and Optical Engineering, Nankai University, Tianjin 300350, China
  • 2Key Laboratory of Optoelectronic Technology of Jiangsu Province, School of Physical Science and Technology, Nanjing Normal University, Nanjing 210023, China
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    DOI: 10.7498/aps.69.20191531 Cite this Article
    Xiao-Lei Wang, Jie-Hui Zhao, Miao Li, Guang-Ke Jiang, Xiao-Xue Hu, Nan Zhang, Hong-Chen Zhai, Wei-Wei Liu. Tight focus and field enhancement of terahertz waves using a probe based on spoof surface plasmons[J]. Acta Physica Sinica, 2020, 69(5): 054201-1 Copy Citation Text show less
    Thickness gradient silver plated strip probe schematic and the magnified schematic diagram of the structure at the tip in the different planes.
    Fig. 1. Thickness gradient silver plated strip probe schematic and the magnified schematic diagram of the structure at the tip in the different planes.
    Structure of the three probes and light field distribution in the y-z plane: (a) A Teflon probe structure; (b) light field distribution of a Teflon probe in the y-z plane; (c) a fully silver-plated probe structure; (d) light field distribution at the tip of a fully silver-plated probe in the y-z plane; (e) a thickness-graded silver-plated strip probe structure; (f) light field distribution of a thickness-graded silver-plated strip probe in the y-z plane.
    Fig. 2. Structure of the three probes and light field distribution in the y-z plane: (a) A Teflon probe structure; (b) light field distribution of a Teflon probe in the y-z plane; (c) a fully silver-plated probe structure; (d) light field distribution at the tip of a fully silver-plated probe in the y-z plane; (e) a thickness-graded silver-plated strip probe structure; (f) light field distribution of a thickness-graded silver-plated strip probe in the y-z plane.
    Peak electric field intensity distribution and normalized electric field intensity distribution curve along the probe centerline (y = 0) in the y-z plane: (a) The light field distribution at the tip of a thickness-graded silver-plated strip probe; (b) the normalized electric field intensity distribution curve.
    Fig. 3. Peak electric field intensity distribution and normalized electric field intensity distribution curve along the probe centerline (y = 0) in the y-z plane: (a) The light field distribution at the tip of a thickness-graded silver-plated strip probe; (b) the normalized electric field intensity distribution curve.
    Distribution of electric field intensity of three kinds of probes in x-y plane.
    Fig. 4. Distribution of electric field intensity of three kinds of probes in x-y plane.
    The electric field strength at the tip of the thickness-graded silver-plated strip probe is distributed in the x-y plane when the polarization directions of the incident terahertz waves are different. The first row to the fourth row are the tightly focused electric field intensity distributions of the incident wave along the y-axis polarization, the x-axis polarization, the left-hand circular polarization, and the right-hand circular polarization. The first to fourth columns are the Ex component, Ey component, Ez component, and Etotal of the tightly focused electric field, respectively.
    Fig. 5. The electric field strength at the tip of the thickness-graded silver-plated strip probe is distributed in the x-y plane when the polarization directions of the incident terahertz waves are different. The first row to the fourth row are the tightly focused electric field intensity distributions of the incident wave along the y-axis polarization, the x-axis polarization, the left-hand circular polarization, and the right-hand circular polarization. The first to fourth columns are the Ex component, Ey component, Ez component, and Etotal of the tightly focused electric field, respectively.
    Surface current and tightly focused electric field intensity curves of the thickness-graded silver-plated strip probe structure corresponding to different θ values. The first to fourth rows are the cases of θ = 30°, 45°, 60°, and 90°, respectively. The first to third columns are the probe structure, the surface current distribution, and the normalized electric field intensity of tightly focused light field in the x-y plane, respectively.
    Fig. 6. Surface current and tightly focused electric field intensity curves of the thickness-graded silver-plated strip probe structure corresponding to different θ values. The first to fourth rows are the cases of θ = 30°, 45°, 60°, and 90°, respectively. The first to third columns are the probe structure, the surface current distribution, and the normalized electric field intensity of tightly focused light field in the x-y plane, respectively.
    θ30º45º60º90º
    Emax/E0672.6744.7768849
    FWHMλ/150 (20 μm) λ/125 (24 μm) λ/115 (26 μm) λ/100 (30 μm)
    Table 1.

    Emax/E0 and FWHM corresponding to different θ values.

    不同θ值所对应的Emax/E0和FWHM

    Xiao-Lei Wang, Jie-Hui Zhao, Miao Li, Guang-Ke Jiang, Xiao-Xue Hu, Nan Zhang, Hong-Chen Zhai, Wei-Wei Liu. Tight focus and field enhancement of terahertz waves using a probe based on spoof surface plasmons[J]. Acta Physica Sinica, 2020, 69(5): 054201-1
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