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Resonant power transmission through a ridged circular aperture with variable aperture dimensions and its arrays

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초록

The transmission resonance characteristics of a single-ridged circular aperture (RCA) were analyzed using the finite-differ-ence time-domain method, and it was found that the transmission cross section (TCS) at the resonant frequency was quite similar to the theoretical TCS. The resonant frequency and corresponding TCS varied as the shape of the ridge changed because a change in the shape causes a change in the capacitance component. The maximum and minimum TCSs were investigated for cases wherein two RCAs were arranged collinearly and side by side. The resonance phenomenon did not differ significantly, even when the ridge width or gap was changed. Finally, the TCSs were compared with the gain ratios when two half-wavelength dipole antennas were arranged, and the duality between the resonant phenomena was satisfied.

Abstract

The transmission resonance characteristics of a single-ridged circular aperture (RCA) were analyzed using the finite-differ-ence time-domain method, and it was found that the transmission cross section (TCS) at the resonant frequency was quite similar to the theoretical TCS. The resonant frequency and corresponding TCS varied as the shape of the ridge changed because a change in the shape causes a change in the capacitance component. The maximum and minimum TCSs were investigated for cases wherein two RCAs were arranged collinearly and side by side. The resonance phenomenon did not differ significantly, even when the ridge width or gap was changed. Finally, the TCSs were compared with the gain ratios when two half-wavelength dipole antennas were arranged, and the duality between the resonant phenomena was satisfied.

참고문헌 (12)

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  2. R. F. Harrington, "Resonant behavior of a small aperture backed by a conducting body", IEEE Transactions on An-tennas & Propagation, 30(2), pp.205~212 (1982)
  3. X. Shi, "Ultrahigh light transmission through a C-shaped nanoaperture", Optics. Letters, 28(15), pp.1320~1322 (2003)
  4. F. M. Kong, "Propagation properties of the SPP modes in nanoscale narrow metallic gap, channel, and hole geometries", Progress in Electromagnetics Research, 76, pp.449~466 (2007)
  5. F. M. Kong, "Analysis of the surface magneto-plasmon modes in the semiconductor slit waveguide at te-rahertz frequencies", Progress in Electromagnetics Re-search, 82, pp.257~270 (2008)
  6. J. -E. Park, "Analysis of deep-subwavelength Au and Ag slit transmittances a terahertz frequencies", Journal of the Optical Society America B, 33(7), pp.1355~1364 (2016)
  7. J. -E. Park, "Resonant transmission of an electri-cally small aperture with a ridge", Journal of Electromag-netic Waves and Application, 23(14-15), pp.1981~1990 (2009)
  8. J. -E. Park, "Resonant power transmission through coupled subwavelength ridged circular apertures", Journal of ElectromagneticWaves Applications, 26(4), pp.423~435 (2012)
  9. J. -E. Park, "Comparison of mutual coupling phe-nomena in subwavelength ridged circular apertures and half-wavelength dipole antenna arrays", International Jour-nal of Antennas and Propagation, 2012, pp.129469~ (2012)
  10. A. Taflove, "Computational Electrody-namics: The Finite-Difference Time-Domain Method" (2005), Artech House
  11. L. Verslegers, "Temporal coupled-mode theory for resonant apertures", Journal of the Optical Society of America B, 27(10), pp.1947~1956 (2010)
  12. P. S. Carter, "Circuit relations in radiating systems and ap-plications to antenna problems", Proceedings of the Institute of Radio Engineers, 20(6), pp.1004~1041 (1932)

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