Axial Ratio Circular polarization conversion (CP) Axial Ratio Axial Ratio Circular polarization conversion (CP) of the proposed Metasurface is further established by the axial ratio (AR) of the reflected wave, 𝐴𝑅 = ( |𝑅𝑦𝑦| 2 +|𝑅𝑥𝑦| 2 +√𝑎 |𝑅𝑦𝑦| 2 +|𝑅𝑥𝑦| 2 −√𝑎 ) 0.5 Where a = (|Ryy| 4 + |Rxy| 4 + 2|Ryy| 2 |Rxy| 2 cos(2ΔØyx) and ∆∅𝐲𝐱 = ∅𝐲𝐲 − ∅𝐱𝐲 The reflection coefficient of the design surface is shown in Figure. The co-polariz...
How to design metamaterial in CST || An Ultra-thin Wide-Angle Cross Polarization Conversion Metasurface
An Ultra-thin Wide-Angle Cross Polarization Conversion Metasurface
In this article, a bandwidth-enhanced metasurface has been designed using a single circular split ring as a unit cell on the top surface of a metal-backed FR4 substrate. The structure
behaves as a cross-polarization conversion (CPC) metasurface over full width at half maxima (FWHM) bandwidth of 12.94 GHz ranging from 9.44 GHz to 22.38 GHz. The proposed CPC metasurface maintains bandwidth enhancement up to 45° incident angles under both TE and TM polarizations. The structure is ultra-thin (~ /11.4 with respect to the center frequency) in nature.
Due to its compact nature, studies on metasurface have become a hot topic of research as its application toward frequency selective surface (FSS). These FSS structures have been proposed as filters, absorbers, polarizers, etc. Recently, metasurface-based cross-polarization conversion (CPC) structures have been reported over a broad range of frequencies from microwave to optical frequency regimes to overcome the drawback of bulky nature in conventional structures. Several CPC structures of both transmitted, as well as reflective nature, have been reported to date, but they suffer from thickness as well as become sensitive to the angle of incidence.
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