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, ๐ด๐
= ( |๐
๐ฆ๐ฆ| 2 +|๐
๐ฅ๐ฆ| 2 +√๐ |๐
๐ฆ๐ฆ| 2 +|๐
๐ฅ๐ฆ| 2 −√๐ ) 0.5 Where a = (|Ryy| 4 + |Rxy| 4 + 2|Ryy| 2 |Rxy| 2 cos(2ฮรyx) and ∆∅๐ฒ๐ฑ = ∅๐ฒ๐ฒ − ∅๐ฑ๐ฒ The reflection coefficient of the design surface is shown in Figure. The co-polarized and cross-polarized reflected waves have the same magnitude at 9.6 GHz and 17 GHz is 0.7. The surface behaves at these points as a CP which converts the linear EM wave into a circular EM wave. The numerical value of the axial ratio is shown in Figure. At 9.6 GHz and 17 GHz, the axial ratio value is lower than the 3dB dotted black line which shows that the design surface has the ability of CPC, to convert 9.6
An Angularly
Stable Tri-band Reflective Cross-polarization Conversion Anisotropic Metamaterial
A tri-band microwave
cross-polarization conversion (CPC) metasurface is designed
and simulated. The metasurface consists of a split-ring-resonator (SRRs) with two splits placed within perpendicular sides of the SRR and designed on an FR4 dielectric substrate backed by a metallic ground plane. An efficient CPC, both for normal as well as for oblique incidence, is achieved. This multi-band polarization conversion results from multiple plasmonic resonances occurring at three neighboring frequencies. Owing to sub-wavelength unit cell size, thin dielectric substrate, and optimized structure of the SRR, the response of the metasurface is independent of the incidence angle of the incoming wave which makes it a potential candidate for many practical applications.
and simulated. The metasurface consists of a split-ring-resonator (SRRs) with two splits placed within perpendicular sides of the SRR and designed on an FR4 dielectric substrate backed by a metallic ground plane. An efficient CPC, both for normal as well as for oblique incidence, is achieved. This multi-band polarization conversion results from multiple plasmonic resonances occurring at three neighboring frequencies. Owing to sub-wavelength unit cell size, thin dielectric substrate, and optimized structure of the SRR, the response of the metasurface is independent of the incidence angle of the incoming wave which makes it a potential candidate for many practical applications.
introduction
Control and
manipulation of the polarization state of electromagnetic waves have always been
of profound interest in the scientific communities due to their fundamental role
in a wide range of applications including contrast imaging microscopy, optical
sensing, molecular biotechnology, and microwave communication. Although, the polarization of the electromagnetic waves can be manipulated through
conventional methods such as the optical activity of the crystals and the Faraday
Effect, however, such methods require bulky volume and are effective only for
very narrow bandwidth. To control and manipulate the polarization of EM waves over
a wide bandwidth and small distances, different metasurface-based designs have
been proposed in the literature [1]. Polarization conversion metasurface
designs usually consist of a two-dimensional periodic array of bi-anisotropic
metallic elements placed over some dielectric. Polarization conversion has been
achieved over different frequency ranges of the electromagnetic spectrum through
different element geometries such as through plasmonic nano-rods in the visible
regime [2], circular split rings in the infrared [3], metallic grating at
terahertz [4], and self-complementary rings [5], rectangular loops with diagonal microstrips [6] and double-head-arrow structure [7] in the microwave
regime. In this paper, a tri-band microwave cross-polarization-conversion (CPC)
metasurface is designed and simulated. The metasurface consists of a
two-dimensional periodic array of anisotropic split-ring-resonators (SRRs)
designed on top of FR4 dielectric substrate backed by a metallic ground
plane. The designed metasurface achieves triband cross-polarization conversion
not only for normal but also for oblique incidence. Owing to sub-wavelength unit cell size, small dielectric thickness and overall optimized design of the
unit cell, the response of the metasurface is independent of the incidence angle
of the incoming wave which makes it a potential candidate for many practical
applications.
To Download the paper
click on the link bellow
https://doi.org/10.1063/1.4997456
To download the cst
simulation file click on the bellow๐ฝ๐ฝ๐ฝ๐ฝ๐ฝ๐ฝ
๊๊๊๊
https://drive.google.com/file/d/1tMcGb4g6ECwdkdprZz46DDB3UqZWgaks/view?usp=sharing
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