4.7 Article

An Equivalent Circuit/System by Design Approach to the Design of Reflection-Type Dual-Band Circular Polarizers

期刊

IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION
卷 70, 期 3, 页码 2364-2369

出版社

IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
DOI: 10.1109/TAP.2021.3111511

关键词

Circular polarization (CP); dual-frequency; frequency selective surfaces (FSSs); polarization conversion

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A dual-band, wide-bandwidth and wide-angle scanning circular polarizer is designed to convert linearly polarized waves into right- and left-hand circularly polarized waves. An analytic model and closed-form expressions are used for design and optimization, and a system design method is proposed for performance improvement. Experimental results show that the polarizer maintains a low axial ratio within a wide-angle field of view.
A dual-band reflection-mode wide-bandwidth and wide-angle scanning circular polarizer is designed. The proposed polarizer can convert linearly polarized waves into right- and left-hand circularly polarized (RHCP and LHCP) waves in the two separate nonadjacent receiving and transmitting K/Ka frequency bands. The polarizer is based on dual-layer dipole arrays printed on both sides of a dielectric substrate separated by a second substrate from the ground plane. An analytic model based on transmission line equivalent circuits is developed. Closed-form expressions are derived to demonstrate the operating principle providing a simple design procedure. The proposed model can be used to optimize the converter for a specific propagation angle of the incident wave. Finally, a system-by-design (SbD) strategy is proposed to improve the performance of analytically synthesized devices. Toward this goal, a computationally efficient digital twin of the accurate full-wave model is built to speed up the solution space exploration and efficiently reach the global optimum. A prototype is designed for the incident angle theta(0) = 30 degrees and it is shown that the axial ratio lower than 3 dB is maintained for a wide-angle field of view of Delta theta = 60 degrees (theta(min) = 0 degrees, theta(max) = 60 degrees) in both frequency bands.

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