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[Keyword] superstrate(4hit)

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  • Effects of Finite Superstrate and Asymmetrical Ground on High Gain Superstrate Antenna

    Jae-Gon LEE  Taek-Sun KWON  Jeong-Hae LEE  

     
    PAPER-Antennas and Propagation

      Pubricized:
    2018/02/16
      Vol:
    E101-B No:8
      Page(s):
    1884-1890

    In this paper, we present the effects of finite superstrates and asymmetrical grounds on the performance of high gain superstrate antennas. First, when the source of a superstrate antenna is located at an edge of a ground plane, that is, an asymmetric ground plane, the gain of the superstrate antenna can be made to match the gain of the superstrate antenna with a symmetrical ground plane using the PEC (E-plane asymmetric) or the AMC wall (H-plane asymmetric) near the edge. Second, the gain of the superstrate antenna, which has a ground plane with dimensions sufficiently close to infinite, is found to be roughly proportional to the reflection magnitude of a partially reflective surface (PRS). It is found that when the square ground size has a finite dimension of two wavelengths or less, the reflection magnitude of the PRS should have the optimum value for achieving maximum gain. Finally, the gain of the superstrate antenna is studied when the ground plane differs from a PRS. For the above three cases, the performances of the superstrate antenna are verified and compared by analysis, full-wave simulation, and measurement.

  • Compact Controlled Reception Pattern Antenna (CRPA) Array Based on Mu-Zero Resonance (MZR) Antenna

    Jae-Gon LEE  Taek-Sun KWON  Bo-Hee CHOI  Jeong-Hae LEE  

     
    PAPER-Antennas and Propagation

      Pubricized:
    2017/12/20
      Vol:
    E101-B No:6
      Page(s):
    1427-1433

    In this paper, a compact controlled reception pattern antenna (CRPA) array based on a mu-zero resonance (MZR) antenna is proposed for a global positioning system (GPS). The MZR antenna can be minimized by designing structure based in mu-negative (MNG) transmission line. The MNG transmission line can be implemented by a gap structure for the series capacitance and a shorting via for a short-ended boundary condition. The CRPA array, which operates in L1 (1.57542GHz) and L2 (1.2276GHz) bands, is designed as a cylinder with a diameter and a height of 127mm (5 inches) and 20mm, respectively, and is composed of seven radiating elements. To design the compact CRPA array with high performance attributes such as an impedance matching (VSWR) value of less than 2, an isolation between array elements (<-12dB), an axial ratio (<5dB), and a circular polarization (CP) gain (>-1dBic: L1 band and >-3dBic: L2 band), we employ two orthogonal MZR antennas, a superstrate, and chip couplers. The performances of the CRPA antenna are verified and compared by an analytic analysis, a full-wave simulation, and measurements.

  • Radiation Pattern of the Rectangular Microstrip Antenna on Anisotropy Substrates with an Air Gap and Dielectric Superstrate

    Joong Han YOON  Hwa Choon LEE  Kyung Sup KWAK  

     
    LETTER-Electromagnetic Theory

      Vol:
    E86-C No:10
      Page(s):
    2145-2150

    This study investigate the rectangular microstrip patch antenna on anisotropy substrates with superstrate and air gap, based on rigorous full-wave analysis and Galerkin's moment method. Results show that radiation patterns with varying air gap, permittivity of the superstrate and substrate, and thickness of the superstrate can be determined and analyzed.

  • Resonant Frequency of Rectangular Microstrip Antennas on the Anisotropy Substrate with an Air Gap and Superstrate

    Joong Han YOON  Kyung Sup KWAK  

     
    LETTER-Microwaves, Millimeter-Waves

      Vol:
    E86-C No:2
      Page(s):
    244-249

    This study investigates the anisotropy substrate and dielectric cover effects of the rectangular microstrip patch antenna on anisotropy substrates with air gap, based on rigorous full-wave analysis and Galerkin's moment method. Results show that the resonant frequencies in the variation of air gap, patch length, and permittivity of superstrate can be determined and analyzed with varying dielectric cover thickness.