An Ultra-Wideband Reflective Linear-to-Circular Polarization Converter Based on Anisotropic Metasurface

• Published in: IEEE access Vol. 8; pp. 82732 - 82740
• Main Authors: Lin, Baoqin, Lv, Lintao, Guo, Jianxin, Liu, Zhe, Ji, Xiang, Wu, Jing
• Format: Journal Article
• Language: English
• Published: Piscataway IEEE 2020; The Institute of Electrical and Electronics Engineers, Inc. (IEEE)
• Subjects: Bandwidth; Bandwidths; Circular polarization; Converters; Dielectric loss; Dielectrics; Frequency conversion; Frequency ranges; Metasurface; Metasurfaces; Phase shift; Polarization; polarization converter; Reflected waves; Reflection; Reflection coefficient; Ultra wideband technology; Ultrawideband
• ISSN: 2169-3536; 2169-3536
• DOI: 10.1109/ACCESS.2020.2988058

In this work, an ultra-wideband and high-efficiency reflective linear-to-circular polarization converter based on an anisotropic metasurface is proposed, which is an orthotropic structure with a pair of mutually perpendicular symmetric axes <inline-formula> <tex-math notation="LaTeX">u </tex-math></inline-formula> and <inline-formula> <tex-math notation="LaTeX">v </tex-math></inline-formula> along ±45° directions with respect to the vertical <inline-formula> <tex-math notation="LaTeX">y </tex-math></inline-formula> axis. The simulated and experimental results show that the polarization converter can realize ultra-wideband linear-to-circular polarization conversion at both <inline-formula> <tex-math notation="LaTeX">x </tex-math></inline-formula>- and <inline-formula> <tex-math notation="LaTeX">y </tex-math></inline-formula>-polarized incidences, its 3dB-axial-ratio-band is between 5.8 and 20.4 GHz, which is corresponding to a relative bandwidth of 112%; moreover, the polarization conversion efficiency (PCE) can be kept larger than 99.6% in the frequency range of 6.1-19.8GHz. In addition, to get an insight into the root cause of the LTC polarization conversion, a detailed theoretical analysis is presented, in which the conclusion is reached that in the case of neglecting thelittle dielectric loss, the axial ratio (AR) of the reflected wave can be completely determined by the phase difference between the two reflection coefficients at <inline-formula> <tex-math notation="LaTeX">u </tex-math></inline-formula>- and <inline-formula> <tex-math notation="LaTeX">v </tex-math></inline-formula>-polarized incidences, and any anisotropic metasurface can be used as an effective LTC polarization converter when the phase difference is close to ±90°.