Large-Frequency-Ratio <i>X</i> / <i>Ka</i> Dual-Band Transmitarray Antenna Exploiting Effective Operating Size Differences of Huygens’ Elements

A dual-band orthogonally polarized transmitarray antenna (TA) aperture design scheme featuring a large frequency ratio (FR) is presented. The proposed aperture is implemented by employing two thin Huygens’ elements: glide bilayer-dipole-pair (GBDP) and parallel bilayer-dipole-pairs (PBDP) elements, which exhibit widely varying electrical sizes. Initially, we investigate the effective operating sizes of these two types of Huygens’ elements and observe significant disparities in their operating sizes due to variations in their magneto-electric degeneracy mechanisms. Subsequently, by exploiting the disparity in elements’ effective operating sizes, we arrange the two elements orthogonally within a single aperture, thereby achieving dual-band functionality with a significantly large FR. Furthermore, we design an <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">X</i>/<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">Ka</i> dual-band orthogonal linearly polarized TA prototype to verify the advantages offered by our proposed strategy. The GBDP element is employed to modulate the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</i>-polarized waves in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">Ka</i> band, with an electrical size of 0.6<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_h \times $</tex-math></inline-formula> 0.6<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_h \times $</tex-math></inline-formula> 0.18<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_h$</tex-math></inline-formula>. Concurrently, the PBDP element is utilized to modulate the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">y</i>-polarized waves in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">X</i> band with an electrical size of 0.4<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_l \times $</tex-math></inline-formula> 0.4<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_l \times $</tex-math></inline-formula> 0.06<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_l$</tex-math></inline-formula>. Here, <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${{{\bm{\lambda }}}_h}$</tex-math></inline-formula> and <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${{{\bm{\lambda }}}_l}$</tex-math></inline-formula> denote the wavelengths corresponding to 30 and 10 GHz, respectively. Measurements indicate that the FR of the dual-band prototype reaches 3, with a 3 dB/1 dB gain bandwidth of 12.6%/4% in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">X</i> band and 8.1%/4.7% in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">Ka</i> band. The peak gain of the prototype is 22.56/29.73 dBi in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">X</i>/<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">Ka</i> bands, respectively.

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Journal
IEEE Antennas and Wireless Propagation Letters
Published
2024-12-23
DOI
https://doi.org/10.1109/lawp.2024.3521672
Citations
2
Primary Topic
Advanced Antenna and Metasurface Technologies
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article
Field-Weighted Citation Impact
2.60
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article

Large-Frequency-Ratio X / Ka Dual-Band Transmitarray Antenna Exploiting Effective Operating Size Differences of Huygens’ Elements

Bing‐Zhong Wang, Xue‐Song Yang, Zi‐Hao Fu
2 citations
IEEE Antennas and Wireless Propagation Letters
Advanced Antenna and Metasurface Technologies
2.60
article

Large-Frequency-Ratio X / Ka Dual-Band Transmitarray Antenna Exploiting Effective Operating Size Differences of Huygens’ Elements

Bing‐Zhong Wang, Xue‐Song Yang, Zi‐Hao Fu
article en
2 citations

Abstract

A dual-band orthogonally polarized transmitarray antenna (TA) aperture design scheme featuring a large frequency ratio (FR) is presented. The proposed aperture is implemented by employing two thin Huygens’ elements: glide bilayer-dipole-pair (GBDP) and parallel bilayer-dipole-pairs (PBDP) elements, which exhibit widely varying electrical sizes. Initially, we investigate the effective operating sizes of these two types of Huygens’ elements and observe significant disparities in their operating sizes due to variations in their magneto-electric degeneracy mechanisms. Subsequently, by exploiting the disparity in elements’ effective operating sizes, we arrange the two elements orthogonally within a single aperture, thereby achieving dual-band functionality with a significantly large FR. Furthermore, we design an <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">X</i>/<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">Ka</i> dual-band orthogonal linearly polarized TA prototype to verify the advantages offered by our proposed strategy. The GBDP element is employed to modulate the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</i>-polarized waves in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">Ka</i> band, with an electrical size of 0.6<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_h \times $</tex-math></inline-formula> 0.6<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_h \times $</tex-math></inline-formula> 0.18<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_h$</tex-math></inline-formula>. Concurrently, the PBDP element is utilized to modulate the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">y</i>-polarized waves in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">X</i> band with an electrical size of 0.4<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_l \times $</tex-math></inline-formula> 0.4<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_l \times $</tex-math></inline-formula> 0.06<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\bm{\lambda }}_l$</tex-math></inline-formula>. Here, <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${{{\bm{\lambda }}}_h}$</tex-math></inline-formula> and <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${{{\bm{\lambda }}}_l}$</tex-math></inline-formula> denote the wavelengths corresponding to 30 and 10 GHz, respectively. Measurements indicate that the FR of the dual-band prototype reaches 3, with a 3 dB/1 dB gain bandwidth of 12.6%/4% in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">X</i> band and 8.1%/4.7% in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">Ka</i> band. The peak gain of the prototype is 22.56/29.73 dBi in <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">X</i>/<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">Ka</i> bands, respectively.

IEEE Antennas and Wireless Propagation LettersVol. 24(4)
University of Electronic Science and Technology of China (CN)
Affordable and clean energy
Openalex Percentile: Top 8%
Advanced Antenna and Metasurface Technologies
2.60
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