A High-Efficiency Dual-Band Linear-to-Circular Polarization Converter Based on Rectangular-Slot Reflective Metasurface

Abstract

In this article, a novel and high-efficiency dual-wideband linear-to-circular polarization conversion based on a rectangular-slot reflective metasurface is anticipated, one that can convert linearly polarized (LP) electromagnetic waves into right- and left-hand circularly polarized waves in two non-adjacent frequency bands. The converter is an orthotropic design, with a pair of mutually orthogonal symmetric axes (u and v) along orientations tilted at 45° to the y-axis. The simulated results indicate that the dual-wideband circularly polarized wave is achieved under a y-polarized an electromagnetic (EM) incidence wave over the bands of 16.49–23.54 GHz and 26.44–34.56 GHz with 3 dB axial ratio relative bandwidths of 35.23% and 26.62%, respectively, and a polarization conversion ratio (PCR) in excess of 99%. A detailed mathematical investigation is proposed to determine the fundamental factor causing the dual-wideband linear-to-circular polarization conversion. The phase difference ($∆{\phi }_{uv})$ between r_uu and r_vv under u- and v- polarized incident waves is $\pm 90°$, and it entirely determines the 3 dB reflected wave axial ratio. Any reflective converter can work efficiently as a linear-to-circular polarization conversion if the phase difference ($∆{\phi }_{uv})$ is close to $\pm 90°$.

1. Introduction

Controlling the polarization state of electromagnetic waves in real time is crucial because it is one of the basic characteristics of electromagnetic waves, which must be considered in real-world applications. Using a metasurface to complete an LTC polarization conversion is an effective technique that has drawn considerable interest. The relevance of realizing a circularly polarized wave has gradually increased as a field of interest. Recently, it has become very popular to modify polarization, optical activity, and birefringence using natural materials, particularly in devices such as quarter-wave plates or circular polarizers [1,2]. Nowadays, modern wireless communication systems increasingly use miniaturized antennas. Metamaterials and magnetic materials have been considered a potential artificial dielectric to alleviate wideband problems. By acting as electromagnetic wave power absorbers, metamaterials are used to eliminate unwanted frequencies (associated with frequency selective surfaces) that can be the root of undesirable electromagnetic waves coupling in microwave radar applications. The frequency selective surface was developed as a broadband reflector and applied to resolve many significant issues in numerous scientific domains. Additionally, the frequency selective surface is continually changing to satisfy increasing demand to extend bandwidth, which affects many contemporary applications, as well as telecoms, all of which depend on a particular bandwidth to operate. Therefore, cutting-edge technologies that can reliably produce a variety of signals throughout a broad band of frequencies are in high demand worldwide. Several procedures, including single-and multi-layer structures, have been considered to improve the efficiency of ultrawideband two-dimensional antennas via a frequency selective surface. The FSS single layer can be used as a reflector, similarly to partially reflecting surfaces (PRS), which transmit some frequencies (although they operate as bandpass filters) and reflect others (after operating as stopband filters). Polarizers have two types: transmissive and reflecting. For example, two separate polarizations received from two bands have been integrated with transmission-type circular polarizers to establish two distinct channels for up- and down-link satellite communications [3,4]. Circular polarization on both bands was intended for a radio frequency identification dual-band artificial magnetic conductor reflector [5]. Most research has been confined to a single purpose, revealing that the design can only regulate and alter LTC, cross conversion, and cross-polarization conversion as polarization in a single band. Recently, numerous polarization converters based on different metasurfaces and capable of conducting a diversity of polarization conversions have been anticipated, including: transmissive [6,7,8,9] and reflective [10,11,12,13,14,15,16,17,18,19] LTC polarization converters under linearly polarized incidence, reflective linearly polarized [20,21,22,23,24,25,26,27] or circularly polarized [28,29,30,31,32], and transmissive linearly polarized [33,34,35,36,37] or circularly polarized [38,39,40] incidence. Moreover, using the previously mentioned LTC polarization converters still poses problems in achieving the desired characteristics of an ultrawideband: high efficiency and compact design.

Additionally, Liu et al. created a dual-band transmission LTC polarization converter with angular stability via a metasurface. While the working frequency bands for these two polarization converters are 9.05–9.65 GHz and 12.55–13.1 GHz, respectively, both have relative bandwidths of only 6.0% and 4.0% [6]. Recently, Majeed et al. reported an ultrawideband LTC polarization conversion using a circular pie-shaped reflective metasurface, with a theoretical 3dB axial ratio relative bandwidth of 50.8% [7]. On the other hand, in the THz region, Ghosh et al. presented a reflective linear-to-circular polarization converter based on a graphene metasurface that can perform between 3.75 THz and 6.0 THz with a 46.15% relative bandwidth [17]. Additionally, Wang et al. presented a dual-band linear-to-circular polarization converter with wide-angle and wideband axial ratio, constructed on a three-metallic-layer reflective metasurface. This has a 3 dB axial ratio over the lower-frequency bandwidth of 15–21.2 GHz (34.3%)/16.3–21.1 GHz (25.7%) and higher-frequency bandwidth of 27–30.3 GHz (11.5%)/27–29.8 GHz (9.9%) but has a poor PCR [12]. A further example is that of Gao et al., who demonstrated the result of a bilayered metasurface via an ultrawideband LTC polarization converter [16].

This article proposes a high-efficiency dual-frequency wideband LTC polarization converter based on a single-layer reflective metasurface. The proposed converter can convert linearly polarized electromagnetic waves over the dual-frequency bands of 16.49–23.54 GHz and 26.44–34.56 GHz into right- and left-handed circularly polarized (RHCP/LHCP) waves under a y-polarized incident wave. The physical interpretation is given, and the efficiency is evaluated by a mathematical equation. The execution of parametric analysis provides design specifications for various frequency ranges. We employ simulations, mathematical operations, and comprehensive theoretical analysis of the dual-frequency wideband and high-efficiency LTC polarization conversion to corroborate the proposed polarization converter.

2. Metasurface Design and Simulation

The schematic design of the proposed converter is presented in Figure 1. The proposed converter is mainly composed of a rectangular patch embedded with a rectangular slot and with two radial stubs separated from a ground plane by a dielectric spacer Roger RT5880 with the property of ${ϵ}_r=2.2$, h = 1.6 mm and tangent loss of $\tan \delta =0.0009$. The metallic ground plane and proposed unit cell are modeled using a copper sheet with an electrical conductivity of σ = 5.8 × ${10}^7$ S/m and a thickness of 0.017 mm. The other physical parameters are tabulated in

Table 1. Optimized value (in mm) of the reflective metasurface unit cell.

p	r	w	l	lc	wc
6	0.86	0.58	4.6	4.6	0.08

. According to Figure 1, the rectangular slot is inserted in the middle of the rectangular patch at a 45° rotational angle. We execute a series of simulations using CST Microwave Studio to evaluate the dual-wideband reflective linear-to-circular polarization converter efficiency. The XY boundary conditions are constrained by the unit cell, and a Floquet port is excited on the z-axis. Figure 2 shows the simulation results when a normal-incidence y- or x-polarized wave is set as an input. The reflection coefficient’s magnitudes of the cross- and co-polarization are r_xy and r_yy, associated with a phase difference. The phase difference ($∆{\phi }_{yx}$) between r_yy and r_xy exists due to the anisotropic features of the metasurface. An efficient reflective LTC polarization converter can be designed if $r_{yy}=r_{xy}$ and $∆{\phi }_{yx}={\phi }_{yy}-{\phi }_{xy}=\pm 90°=2k\pi \pm \pi /2$ (k = 0, 1, 2…), where the sign (±) represents the RHCP ($-$) and LHCP ($+$) of the reflected wave. According to Figure 2a, the magnitudes of r_yy and r_xy of the dual-band LTC polarization converter based on the rectangular slot reflective metasurface are nearly equal over the frequency ranges of 17.67–21.14 GHz and 28.36–32.91 GHz. According to Figure 2b, the phase difference between the 15–24.22 GHz and 25.50–37 GHz frequency bands is always close to −90°, and satisfies the phase relation ($∆{\phi }_{yx}={\phi }_{yy}-{\phi }_{xy}=\pm 90°=2k\pi \pm \pi /2, k=0, 1, 2\dots$). The reflected wave can be considered circularly polarized if its axial ratio is below 3 dB. To calculate the bandwidth of the anticipated dual-wideband polarization conversion, we computed the axial ratio of the reflected wave from the succeeding equation, using the data set presented in Figure 2 [7].

$$\mathrm{AR}=\sqrt{\frac{{\left|r_{yy}\right|}^2+{\left|r_{xy}\right|}^2+\sqrt{{\left|r_{yy}\right|}^4+{\left|r_{xy}\right|}^4+2{\left|r_{yy}\right|}^2{\left|r_{xy}\right|}^2\cos \left(2∆{\phi }_{yx}\right)}}{{\left|r_{yy}\right|}^2+{\left|r_{xy}\right|}^2-\sqrt{{\left|r_{yy}\right|}^4+{\left|r_{xy}\right|}^4+2{\left|r_{yy}\right|}^2{\left|r_{xy}\right|}^2\cos \left(2∆{\phi }_{yx}\right)}}}$$

(1)

The calculated axial ratio of the proposed converter exists below 3 dB over the dual-frequency wideband of 16.49–23.54 GHz and 26.44–34.56 GHz, as presented in Figure 3a. The 3 dB axial ratio bandwidth within dual-frequency wideband of 16.49–23.54 GHz and 26.44–34.56 GHz is 35.23% and 26.62%, respectively. Additionally, the axial ratio is kept under 1.5 dB, demonstrating that the polarization conversion ratio of the polarization converter is above 99%. Other parameters, called reflection coefficients of the LTC polarization converter (RHCP and LHCP), a polarization conversion ratio, and a polarization extinction ratio are introduced [7] to evaluate a linear-to-circular polarization conversion with a promising procedure. We established these parameters of the reflected wave from the following equations, applying the results simulated above.

$$\begin{gathered} r_{RHCP-y}=\sqrt{2}\left(r_{xy}+i{r}_{yy}\right)/2 \\ {r}_{LHCP-y}=\sqrt{2}\left(r_{xy}-i{r}_{yy}\right)/2 \end{gathered}$$

(2)

$$\mathrm{PCR}=\frac{{\left|r_{RHCP-y}\right|}^2}{{\left|r_{RHCP-y}\right|}^2+{\left|r_{LHCP-y}\right|}^2}$$

(3)

$$\mathrm{PER}=20\log \left(\frac{r_{xy}}{r_{yy}}\right)$$

(4)

The reflection coefficients of the dual-frequency wideband LTC polarization converter are determined using Equation (2) based on the data simulated above. As shown in Figure 3b, the calculated dual-frequency wideband $r_{RHCP-y}$ magnitude is close to 0 dB with respect to 3 dB axial ratio, indicating that the reflected wave under the normal incidence y-polarized wave has converted to an RHCP and LHCP wave. Furthermore, the obtained dual-frequency wideband polarization conversion ratio, illustrated in Figure 4a, thoroughly shows that the linear-to-circular polarization conversion ratio can be accomplished at more than 99% over the frequency ranges of 17–23.07 GHz and 27.01–33.70 GHz, respectively, conquering 35.23% and 26.62% of the 3 dB axial ratio band. The effectiveness of circular polarization is determined by the polarization extinction ratio (PER) between $r_{RHCP-y}$ and $r_{LHCP-y}$ waves. The polarization extinction ratio should be greater than −20 dB (LHC) or +20 dB (RHCP) to establish the equal 90° phase difference and magnitude succeeding in a circularly polarized wave. According to Figure 4b the frequency bands between 16.01–23.95 GHz and 24.85–37.0 GHz meet the polarization extinction ratio requirement. The efficiency of the proposed polarization converter is significantly higher with the polarization conversion ratio and polarization extinction ratio frequency bands, which hold 35.23% and 26.62% of the 3 dB axial ratio over the dual-frequency bands of 16.49–23.54 GHz and 26.44–34.65 GHz, respectively. In summation, a normal y-polarized incident wave can be converted into a circularly polarized wave using the proposed converter, which has an exceptionally wide band and is highly efficient.

Parameters Analysis

The aim of this section is to investigate how different parameters influence the phase difference and 3 dB axial ratio of the dual-frequency wideband linear-to-circular polarization conversion. To achieve an optimal parameter, we optimized the values of the radial stub (r) and the width of the rectangular patch (w). A sequence of parametric simulations was performed to evaluate the influence of the parameters on the phase difference and 3 dB axial ratio of the converter unit cell when one parameter was changed while the other stayed the same. The calculated results of the parametric phase difference and 3 dB axial ratio of the dual-frequency wideband LTC polarization conversion are shown in Figure 5 and Figure 6. The phase difference of a perfect linear-to-circular polarization converter can be calculated [7] from the succeeding equation:

$$∆{\phi }_{yx}={\phi }_{yy}-{\phi }_{xy}=2k\pi \pm \pi /2$$

(5)

where k is an integer, and the negative $\left(-\right)$ and positive $\left(+\right)$ signs represent the RHCP and LHCP, respectively. According to our calculation results, changing the radius of the stub and width of the rectangular patch of a dual-wideband LTC polarization conversion does not influence the phase difference, as shown in Figure 5a,b. The phase difference is $-90$° and $-450°$ in the frequency range of $15–24.18$ GHz and $25.44–38$ GHz, respectively, which satisfies Equation (5), as demonstrated in Figure 5.

The 3 dB axial ratio of a dual-frequency wideband is influenced by changing the parametric values of the radial stub and width of the rectangular patch, as shown in Figure 6a,b. The resonance peak of the 3 dB axial ratio of a dual-frequency wideband linear-to-circular polarization converter at the lower and higher frequency range was less than 3 dB after increasing the radius of the stub and width of the rectangular patch from 0.84 to 0.90 mm and 0.54 to 0.60 mm, as shown in Figure 6a,b. The parameter ranges r and w shown in Figure 6 were selected to follow the 3 dB axial ratio (0.84 mm–0.90 mm and 0.54 mm–0.60 mm). When the parameters are changed, it is interesting to see that the axial ratio exists below 3 dB. The preceding explanation explains why our proposed reflective metasurface excels in dual-wideband linear-to-circular polarization conversion.

3. Theoretical Analysis

The anticipated reflective converter performs a dual-frequency wideband LTC polarization conversion with high efficiency and as an ultrawideband. In the following analysis, we conduct a thorough theoretical investigation to achieve a complete physical configuration of the fundamental root. There would not be any cross-polarized reflecting factors under u- and v-polarized waves because it is a symmetric configuration with two mutually orthogonal symmetric axes. The reflection matrix (R_lin) is due to a linearly polarized (LP) incident wave in the uv-local coordinate system, and can be written as [7]:

$$R_{\mathrm{lin}}=\left(\begin{array}{cc}{r}_{uu}& 0\\ 0& r_{vv}\end{array}\right)$$

(6)

Since the metasurface structure is anisotropic, the reflection coefficients of the co-polarization, i.e., $r_{uu}$, $r_{vv}$, will be independent of one another, but the magnitudes of co-polarization reflection coefficients will be relatively near to 1.0 because of the minimal dielectric loss. Thus the succeeding equation can be acknowledged without considering the minimal dielectric loss: $r_{vv}=r_{uu}{e}^{-j∆{\phi }_{uv}}$. The reflection coefficients $r_{uu}$ and $r_{vv}$ have a phase difference which can lie between $-180°$ and $+180°.$ Moreover, the symmetrical axes v- and u- are oriented in the same direction as the y-axis and have a $\pm 45°$ tilt angle. The x- and y-polarized waves can be characterized using the uv- coordinates as ${\widehat{\mathit{e}}}_x=\frac{\sqrt{2}}{2}\left({\widehat{\mathit{e}}}_u-{\widehat{\mathit{e}}}_v\right)$ and ${\widehat{\mathit{e}}}_y=\frac{\sqrt{2}}{2}\left({\widehat{\mathit{e}}}_u+{\widehat{\mathit{e}}}_v\right)$, respectively. In the xy-coordinate system, the R_lin can be computed via Equation (6). If a normal incidence y-polarized wave is supposed as an input (${\mathit{E}}^{\mathit{i}}=E_0{\widehat{\mathit{e}}}_y=\frac{\sqrt{2}}{2}\left({\widehat{\mathit{e}}}_u+{\widehat{\mathit{e}}}_v\right)$), the reflected wave can be differentiated as follows: $\left({\mathit{E}}^{\mathit{r}}=E_u^r{\widehat{\mathit{e}}}_u+E_v^r{\widehat{\mathit{e}}}_v\right)$, via Equation (6). Following algebraic simplification, the reflected wave can be expressed as ${\mathit{E}}^{\mathit{r}}=\frac{E_0}{2}\left[\left(r_{uu}+r_{vv}\right){\widehat{\mathit{e}}}_y+\left(r_{uu}-r_{vv}\right){\widehat{\mathit{e}}}_x\right]$. The reflection coefficients of co-($r_{yy}$) and cross- ($r_{xy}$) polarization for the normal-incidence y-polarized wave can be written as $r_{yy}=\frac{1}{2}\left(r_{uu}+r_{vv}\right)=\frac{1}{2}{r}_{uu}\left(1+e^{-j∆{\phi }_{uv}}\right)$ and $r_{xy}=\frac{1}{2}\left(r_{uu}-r_{vv}\right)=\frac{1}{2}{r}_{uu}\left(1-e^{-j∆{\phi }_{uv}}\right)$. After a similar computation for the x-polarized wave, the final form of R_lin in the xy-coordinate system can be derived using [7], as shown below:

$${\mathbf{R}}_{\mathrm{lin}}=\left(\begin{array}{cc}{r}_{xx}& r_{xy}\\ r_{yx}& r_{yy}\end{array}\right)=\frac{1}{2}\left(\begin{array}{cc}{r}_{uu}+r_{vv}& r_{uu}-r_{vv}\\ r_{uu}-r_{vv}& r_{uu}+r_{vv}\end{array}\right)=\frac{1}{2}{r}_{uu}\left(\begin{array}{cc}1+e^{-j∆{\phi }_{uv}}& 1-e^{-j∆{\phi }_{uv}}\\ 1-e^{-j∆{\phi }_{uv}}& 1+e^{-j∆{\phi }_{uv}}\end{array}\right)$$

(7)

From Equation (7), the succeeding equation can be derived as:

$$\frac{r_{yy}}{r_{xy}}=\frac{r_{xx}}{r_{yx}}=\frac{1+e^{-j∆{\phi }_{uv}}}{1-e^{-j∆{\phi }_{uv}}}=\frac{1+\cos \left(∆{\phi }_{uv}\right)-j\sin \left(∆{\phi }_{uv}\right)}{1-\cos \left(∆{\phi }_{uv}\right)+j\sin \left(∆{\phi }_{uv}\right)}=\frac{j\sin \left(∆{\phi }_{uv}\right)}{1-\cos \left(∆{\phi }_{uv}\right)}$$

(8)

Moreover, using Equation (8), the magnitudes of co-polarized reflection coefficients $(r_{xx}, r_{yy}$) and cross-polarized reflection coefficients ($r_{xy, }{r}_{yx}$) can be written as follows:

$$\left|r_{yy}\right|=\left|r_{xx}\right|=\frac{1}{2}\left|r_{uu}\right|\left|1+e^{-j∆{\phi }_{uv}}\right|=\frac{1}{2}\left|1+\cos \left(∆{\phi }_{uv}\right)-j\sin \left(∆{\phi }_{uv}\right)\right|=\sqrt{\left(1+\cos ∆{\phi }_{uv}\right)/2}$$

$$\left|r_{xy}\right|=\left|r_{yx}\right|=\frac{1}{2}\left|r_{uu}\right|\left|1-e^{-j∆{\phi }_{uv}}\right|=\frac{1}{2}\left|1-\cos \left(∆{\phi }_{uv}\right)+j\sin \left(∆{\phi }_{uv}\right)\right|=\sqrt{\left(1-\cos ∆{\phi }_{uv}\right)/2}$$

(9)

The reflection coefficients of $r_{xx},r_{yy}$ and $r_{yx},r_{xy}$-polarization with x- and y-polarized incidence waves are pure imaginary numbers. It is always supposed that the $∆{\phi }_{yx}$ between them is $\pm 90°.$ It clarifies that in Figure 2b, the $∆{\phi }_{yx}$ is always $-90°$ for the dual-frequency bands of 15–24.22 GHz and 25.50–37.0 GHz. When the $∆{\phi }_{uv}\ne 0° \mathrm{and} \pm 180°,$ the polarization reflection coefficients of the ($r_{yy},r_{xx}$) and ($r_{xy},r_{yx}$) will not be zero, resulting in an elliptical polarized reflected wave, with a phase difference between the ($r_{yy},r_{xx}$) and ($r_{xy},r_{yx})$ remaining ±90°. The 3 dB axial ratio of the reflected wave using the magnitude ratio of ($r_{yy},r_{xy}$) and ($r_{xx},r_{yx}$) can be found from [7] and is given below:

$$\mathrm{AR}=\left\{\begin{array}{c}\frac{\left|\sin \left(∆{\phi }_{uv}\right)\right|}{1-\cos \left(∆{\phi }_{uv}\right)} if \left|\sin \left(∆{\phi }_{uv}\right)\right| \ge 1-\cos \left(∆{\phi }_{uv}\right) \\ \frac{1-\cos \left(∆{\phi }_{uv}\right)}{\left|\sin \left(∆{\phi }_{uv}\right)\right|} if \left|\sin \left(∆{\phi }_{uv}\right)\right|<1-\cos \left(∆{\phi }_{uv}\right) \end{array}\right.$$

(10)

Moreover, Equation (8) has been applied to the relationship $\frac{r_{yy}}{r_{xy}}=\frac{r_{xx}}{r_{yx}}$, indicating that the ratio of the cross (y- to -x and x- to -y)-polarization reflection coefficient under y- and x-polarized incidences is always equal, which concludes that an isotropic metasurface converts a normal incidence y-polarized wave to right- and left-hand circular polarized reflected waves. When ∆φ_uv = 0°, $\left|r_{yx}\right|=\left|r_{xy}\right|=0$, Equation (9) implies that the polarization condition of the incident and reflected wave will be equal. When ∆φ_uv = 180°, however, $\left|r_{yy}\right|=\left|r_{xx}\right|=0$ to achieve a perfect cross-polarization. Additionally, when $∆{\phi }_{uv}\ne 0° \mathrm{or} \pm 180°$, the reflected wave will be elliptically polarized, and the reflected wave’s axial ratio can be determined using the succeeding equation:

$$\mathrm{AR}=\sqrt{\left(1\pm \cos ∆{\phi }_{uv}\right)/\left(1\mp \cos ∆{\phi }_{uv}\right)}$$

(11)

Here, the ($+$) and ($-$) signs ensure that the axial ratio will never be less than 1.0, according to Equation (11). The axial ratio of the reflected wave is equal to 1.0 at ∆φ_uv = 90°, which indicates a perfect LTC reflective polarization converter, according to Equations (10) and (11). When ∆φ_uv = 90°, the perfect LTC reflective polarization conversion can be realized. The incident wave and reflected wave under x- and y-polarization can be considered a composite wave with equal magnitude u- and v-polarized components to negligible dielectric loss. Both orthogonal components appear to be in phase with one another in the incident wave, but the ∆φ_uv between them will change in the reflected wave. The ∆φ_uv will be altered to $\pm 90°$ when ∆φ_uv = 90°, resulting in a perfect LTC polarization conversion. We used the preceding study to simulate the anticipated polarization reflective converter under v- and u-polarized incidence to determine the fundamental cause of linear-to-circular polarization converters. The simulated results of a dual-frequency wideband LTC polarization, especially the ∆φ_uv (phase difference) between r_vv and r_uu, are shown in Figure 7a. The frequency bands between 16.27–23.79 GHz and 27–35.23 GHz show that the phase difference of a dual-frequency wideband always remains close to $+90°.$ It is implied that the calculated LTC-polarization converter of a dual-wideband will be comprehended in a wide frequency range. Why is the resulting phase difference (∆φ_uv) so effective? To ensure the root cause, the other simulation results, such as the magnitude (r_uu and r_vv) along with the phases (φ_uu and φ_vv) of a dual-wideband, are presented in Figure 7b,c. The formula φ_ii = Arg(R_ii) + 2k₀ S is applied to determine their phase changes, where S is the separation between the proposed converter surface and the Floquet port in the simulation structure. According to Figure 7b, the magnitude of a dual-frequency wideband is nearly 1.0 throughout all frequencies, indicating minimal dielectric loss of the proposed polarization converter. The curve of r_vv and r_uu still has a great many variations, which have two and two in dual-frequency wideband local minimum values, respectively, which are found at 13.56 GHz and 40.24 GHz, as well as at 24.94 GHz and 40.65 GHz. The two and two in dual-wideband resonant modes are assumed to be simulated by v- and u-polarized incident waves, created by these local maximum dielectric losses. Additionally, the curves of r_uu and r_vv have quite distinct curvatures at various resonant frequencies, suggesting that the Q values of these resonant modes vary. Moreover, Figure 7c shows that the phase variation rate of r_vv and r_uu at each resonance frequency varies only due to the variance in Q values across different resonance modes. At a lower frequency, the phase difference ∆φ_uv can remain close to +90° over the frequency band of 16.27–23.79 GHz, whereas at a higher frequency it is an integral multiple of 90° (in the frequency band of 27–35.23 GHz), which is primarily due to the following two causes. Firstly, compared to the first resonance mode (13.56 and 24.94 GHz) at v- and u-polarized incident in a dual-frequency wideband, it has a higher Q value in addition to possessing a lower resonant frequency. It causes the phase φ_vv in a dual-wideband to decline earlier and more quickly, and, when keeping the phase difference (∆φ_uv) in the 11–13.75 GHz range, is close to +90°. Secondly, the second pair of resonant modes in a dual-frequency wideband at v- and u-polarized incidences are identical, and both are very clear. This causes the phases of φ_uu and φ_vv to change the same way as the frequency increase in the range of 15–39 GHz, allowing the phase difference (∆φ_uv) is close to +90° or an integral multiple of It is implied that the calculated LTC-polarization converter of a dual-wideband will be comprehended in a wide frequency range. Why is the resulting phase difference (∆φ_uv) so effective? To ensure the root cause, the other simulation results, such as the magnitude (r_uu and r_vv) along with the phases (φ_uu and φ_vv) of a dual-wideband, are presented in Figure 7b,c. The formula φ_ii = Arg(R_ii) + 2k₀ S is applied to determine their phase changes, where S is the separation between the proposed converter surface and the Floquet port in the simulation structure. According to Figure 7b, the magnitude of a dual-frequency wideband is nearly 1.0 throughout all frequencies, indicating minimal dielectric loss of the proposed polarization converter. The curve of r_vv and r_uu still has a great many variations, which have two and two in dual-frequency wideband local minimum values, respectively, which are found at 13.56 GHz and 40.24 GHz, as well as at 24.94 GHz and 40.65 GHz. The two and two in dual-wideband resonant modes are assumed to be simulated by v- and u-polarized incident waves, created by these local maximum dielectric losses. Additionally, the curves of r_uu and r_vv have quite distinct curvatures at various resonant frequencies, suggesting that the Q values of these resonant modes vary. Moreover, Figure 7c shows that the phase variation rate of r_vv and r_uu at each resonance frequency varies only due to the variance in Q values across different resonance modes. At a lower frequency, the phase difference ∆…_uv can remain close to +90° over the frequency band of 16.27–23.79 GHz, whereas at a higher frequency it is an integral multiple of 90° (in the frequency band of 27–35.23 GHz), which is primarily due to the following two causes. Firstly, compared to the first resonance mode (13.56 and 24.94 GHz) at v- and u-polarized incident in a dual-frequency wideband, it has a higher Q value in addition to possessing a lower resonant frequency. It causes the phase φ_vv in a dual-wideband to decline earlier and more quickly, and, when keeping the phase difference (∆φ_uv) in the 11–13.75 GHz range, is close to +90°. Secondly, the second pair of resonant modes in a dual-frequency wideband at v- and u-polarized incidences are identical, and both are very clear. This causes the phases of φ_uu and φ_vv to change the same way as the frequency increase in the range of 15–39 GHz, allowing the phase difference (∆φ_uv) is close to +90° or an integral multiple of $\pm 90°$ in the following band. Finally, Figure 7d shows the axial ratio of the reflected wave via Equation (10), based on the phase difference (∆φ_uv) in a dual-frequency wideband obtained in Figure 7a. It is evident from Figure 3a that the anticipated axial ratio substantially agrees with Figure 7d. The above analysis has clarified that the polarization converter in a dual-frequency wideband can carry out such a high-efficiency and ultrawideband LTC reflective polarization conversion. Excluding the first two resonant modes at v- and u-polarized incidences, it can be generally ascribed to the second pair of resonance modes. A sufficient difference between the two first resonance modes causes the ∆φ_uv in the frequency range of 10–15 GHz to be close to $\pm 90°$. However, due to the similarity and low Q values of the second pair of resonance modes, the phase difference (∆φ_uv) remains nearby $+90$° or an integral multiple of $\pm 90°$ in the adjacent band of 16.27–23.79 GHz and 27.0–35.23 GHz. Comparisons of the performance of this novel LTC reflective polarization conversion metasurface in a dual-wideband with those in previously published papers are tabulated in

Table 2. Comparative study of LTC polarization conversion of the proposed metasurface with the previously published works.

References	Unit Cell p(mm)	Substrate Thickness h(mm)	Operating Bandwidth (GHz)	3 dB Axial Ratio (%)	Dielectric Layer	LTC PCR (%)	Type of Polarization Conversion	No of Bands
Ref. [6]	9.00	1.0/1.0	9.05–9.65/ 12.5–13.1	6.4/ 4.6	Bilayer	N/A	Linear to circular	2
Ref. [7]	6	1.6	20.18–33.93	50.8	Single layer	N/A	Linear to circular	1
Ref. [8]	8.00	3.00/4.30	5.8–20.4	112	Bilayer	N/A	Linear to circular	1
Ref. [10]	9.2	3.1	5.95–8.80/ 12.68–15.58	38.6/ 20.5	Single layer	N/A	Linear to circular	2
Ref. [11]	6.65	0.13	19.4–21.8/ 27.9–30.5	12.5/ 8.7	Six layers	N/A	Linear to circular	2
Ref. [16]	9.5	3.5	6.1–12.6	69.0	Bilayer	N/A	Linear to circular	1
Ref. [28]	10.0	2.80	5.35–5.95/ 8.88–12.03	10.45/ 30.12	Single layer	N/A	Linear to circular	2
This paper	6	1.6	16.49–23.54/ 26.44–34.56	35.23/ 26.62	Single layer	99	Linear to circular	2

. Hence, the calculated LTC polarization conversion of 99 % of a dual-frequency wideband has been achieved in the ultrawideband frequency range.

4. Conclusions

In summary, a dual-frequency wideband LTC polarization conversion based on a reflective metasurface is presented in this article. The proposed converter can convert EM-waves into RHCP and LHCP in a dual non-adjacent frequency band of 16.49–23.54 GHz and 26.44–34.56 GHz, which corresponds to the relative bandwidths 35.23% and 26.62%, respectively, according to the 3 dB axial ratio property. Moreover, a comprehensive theoretical investigation is proposed to get a physical insight into the underlying cause of the LTC polarization converter. It can be related mainly to the second pair of resonance modes, which keep ∆φ_uv = +90° or an integral multiple of −90° in a dual and ultrawideband frequency range of 16.27–23.79 GHz and 27–35.23 GHz. Any reflective converter can be operated as a dual-frequency wideband LTC polarization conversion if the ∆φ_uv between r_uu and r_vv is close to ±90° or an odd integral multiple of ±90°.