A Ka-Band Circular Polarized Waveguide Slot Antenna with a Cross Iris
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applied sciences Article A Ka-Band Circular Polarized Waveguide Slot Antenna with a Cross Iris Sung-Joon Yoon and Jae-Hoon Choi * Department of Electronics and Computer Engineering, Hanyang University, Seoul 133-791, Korea; [email protected] * Correspondence: [email protected]; Tel.: +82-2-2220-0376 Received: 30 August 2020; Accepted: 2 October 2020; Published: 7 October 2020 Featured Application: Segment waveguide slot antenna for a satellite communication and radar. Abstract: A Ka-band circularly polarized (CP) waveguide slot antenna with a cross iris is proposed. To achieve the CP characteristic (LHCP) in the antenna, a hexagonal shaped cavity is used. The impedance matching is improved by adjusting the sizes of the hexagonal cavity and a rectangular matching cavity. To enhance the axial ratio bandwidth, a cross iris is used with two arms of different lengths. From experimental results, the proposed antenna has a 3 dB axial ratio bandwidth of 6810 MHz (31.72 GHz–38.53 GHz). The 10 dB reflection coefficient bandwidth of the proposed − antenna ranges from 31.51 GHz to 39.21 GHz (7700 MHz). Keywords: waveguide antenna; slot antenna; circular polarization; axial ratio enhancement 1. Introduction Millimeter-wave communication systems support a higher data rate and larger capacity. Millimeter wave frequency has therefore been widely used in various applications such as 5G mobile, radar, satellite, military, and automotive communications [1]. Because mm-wave signals can be easily distorted by atmospheric interference such as fog or dust, waveguide antennas have been considered among the most appropriate for mm-wave applications due to their high power handling, high gain, stable performance and low transmission loss [2,3]. The polarization of antennas is one of the important factors in determining the performance of the communication. For linear polarization antenna, if the polarizations of a transmitter and a receiver do not match each other, communication performance deteriorates. Meanwhile, circular polarization avoids polarization misalignment as the electric field rotates, and it reduces multipath fading with flexibility in orientation the angle between the transmitted receiver [4,5]. Therefore, circular polarized (CP) waveguide antennas in particular are widely used in modern satellite communication systems due to their advantages of enhancing the channel stability and reliability [6,7]. Several techniques have been introduced to realize the waveguide CP horn and aperture antennas such as using a printed circuit board with four printed hook shaped arms [7], loading two metallic arms with a 45◦ inclination angle [8], and inserting a meta-surface polarizer or chiral metamaterial transformer [6,9]. However, there are some limitations in applying them to various applications since these antennas are relatively bulky and heavy. In addition, they are not suitable for array systems because a large space is required for polarizers to be installed [10]. Therefore, such antennas are not appropriate for satellite communication systems requiring a high gain array structure with compact size. To overcome these drawbacks of bulk and mass, various types of circular polarized waveguide slot antennas have been studied [11–17]. Waveguide inclined slot, crossed slot, and v-type slot antennas have been widely used for CP array antennas to generate circularly polarized waves with high gain [13–17]. However, there are few reports on either widening Appl. Sci. 2020, 10, 6994; doi:10.3390/app10196994 www.mdpi.com/journal/applsci Appl. Sci. 2020, 10, 6994 2 of 15 the axial ratio bandwidth of the waveguide slot antenna at the millimeter-wave band region or the design of waveguide slot CP antennas [16,17]. This paper proposes a Ka-band circularly polarized waveguide slot antenna with a cross iris. To achieve a circular polarization characteristic, a hexagonal shaped cavity is used [18]. By mounting a cross iris,Appl. the Sci. circular2020, 10, x FOR polarization PEER REVIEW performance of the proposed antenna is enhanced. The2 of proposed15 antenna provides a 10 dB reflection coefficient bandwidth covering from 31.51 GHz to 39.21 GHz. − The 3 dBreports axial on ratio either bandwidth widening the is axial 6810 ratio MHz bandwidt (31.72h of GHz–38.53 the waveguide GHz). slot antenna The antenna at the millimeter- peak gains are wave band region or the design of waveguide slot CP antennas [16,17]. 9.08 dBi at 33.5 GHz and 7.33 dBi at 37.6 GHz. The boresight gains of 7.87 dBi and 5.76 dBi are achieved This paper proposes a Ka-band circularly polarized waveguide slot antenna with a cross iris. To at thoseachieve two frequencies, a circular polarization respectively. characteristic, a hexagonal shaped cavity is used [18]. By mounting a cross iris, the circular polarization performance of the proposed antenna is enhanced. The proposed 2. Antennaantenna Design provides a −10 dB reflection coefficient bandwidth covering from 31.51 GHz to 39.21 GHz. FigureThe 31 dBshows axial theratio structure bandwidth of is the 6810 proposed MHz (31.72 CP GHz–38.53 waveguide GHz). slot The antenna antenna consisting peak gains of are a rectangular9.08 dBi at 33.5 GHz and 7.33 dBi at 37.6 GHz. The boresight gains of 7.87 dBi and 5.76 dBi are achieved waveguide, an air metal box with hexagonal cavity and matching slot, and a cross iris at the bottom of at those two frequencies, respectively. the rectangular waveguide. The proposed antenna has dimensions of 10.1 mm 23 mm 7.06 mm and × × is made2. of Antenna a copper Design with a conductivity of 5.8001 107 S/m. The detailed parameters of the proposed × antenna areFigure shown 1 shows in Figure the 1structure and the of dimensionsthe proposed are CP givenwaveguide in Table slot 1antenna. The performancesconsisting of a of the proposedrectangular antenna waveguide, were simulated an air metal using box the with commercial hexagonal cavity electromagnetic and matching simulator,slot, and a cross High iris Frequency at Structurethe Simulatorbottom of the (HFSS) rectangular [19]. waveguide. The antenna The prop is fedosed from antenna the has rectangular dimensions of waveguide 10.1 mm × 23 to mm excite the × 7.06 mm and is made of a copper with a conductivity of 5.8001 × 107 S/m. The detailed parameters TE10 mode for high power handling capability. The dimensions (a = 7.11 mm and b = 3.56 mm) of the proposed antenna are shown in Figure 1 and the dimensions are given in Table 1. The of the feeding waveguide are determined by the cutoff frequency (21.077 GHz) using the following performances of the proposed antenna were simulated using the commercial electromagnetic equationsimulator, with dimensions High Frequency shown Structure in Figure Simulator2[ 20]. (HFS AsS) shown [19]. The in Figureantenna2 ,is the fed waveguidefrom the rectangular has its longest dimensionwaveguide along theto excite x-axis the (a ).TE mode for high power handling capability. The dimensions (= 7.11 mm and =3.56 mm) of the feeding waveguider are determined by the cutoff frequency (21.077 GHz) using the following equation 1with dimensionsmπ2 shownnπ in2 Figure 2 [20]. As shown in Figure 2, the waveguide has itsfcmn longest= dimension along the x-axis+ (a). , (1) 2π pµ0"0 a b 2 2 = + , (1) When a > b, the cutoff frequency of TE10 (m =1,n= 0) mode becomes When a>b, the cutoff frequency of TE10 (m = 1, n = 0) mode becomes 1 fc10 = , (2) = , (2) 2apµ0"0 μ ε . where µwhere0 and "00 andare the0 are permeability the permeability and and permittivity permittivity of free free space, space, respectively respectively. (a) Figure 1. Cont. Appl. Sci. 2020, 10, 6994 3 of 15 Appl. Sci. 2020, 10, x FOR PEER REVIEW 3 of 15 Appl. Sci. 2020, 10, x FOR PEER REVIEW 3 of 15 (b) (b) (c) FigureFigure 1. Geometry 1. Geometry of the of proposedthe proposed antenna: antenna: (a ()a) 3-D 3-Dview view of the proposed proposed antenna; antenna; (b) (topb) topview view of of the proposedthe antenna;proposed antenna; (c) side ( viewc) side of view the of proposed the propos antennaed antenna and and cross cross iris.iris. Tabley 1. Dimensions of the proposed antenna. Parameters C1 C2 S1 S2 L1 L2 (c) Value (mm) 6.5 4.4 4.3 8 6 5 Figure 1. GeometryParameters of the proposedb H1 antenna:H2 (a) 3-DH3 viewH of4 the proposedB1 B antenna;2 (b) top view of the proposed antenna;Value (c (mm)) side view7.06 of the 2.5proposed 0.5 antenna 1.2 and cross 5.9 iris. 3.28 y (μ0, ε0) 0 a x bz Figure 2. Geometry of the rectangular waveguide. Table 1. Dimensions of the proposed antenna. (μ0, ε0) Parameters Value (mm) 6.5 4.4 4.3 8 6 5 Parameters0 Value (mm) 7.06 2.5 0.5 1.2 a 5.9 x3.28 z FigureFigure 2. 2.Geometry Geometry of of the the rectangular rectangular waveguide. waveguide. Table 1. Dimensions of the proposed antenna. Parameters Value (mm) 6.5 4.4 4.3 8 6 5 Parameters Value (mm) 7.06 2.5 0.5 1.2 5.9 3.28 Appl.Appl. Sci. Sci. 20202020, ,1010, ,x 6994 FOR PEER REVIEW 44 of of 15 15 Appl. Sci. 2020, 10, x FOR PEER REVIEW 4 of 15 3. Antenna Analysis 3.3. Antenna Antenna Analysis Analysis In the proposed antenna design, the hexagonal shaped cavity with a rectangular waveguide shownInIn thein the Figureproposed proposed 3 is antenna antennaused as design, design, an initial the the hexagonal hexagonalmodel (first shaped shaped reference cavity cavity antenna) with with a a rectangular to realize the waveguide circular polarization.shownshown inin FigureFigure The3 ishexagonal3 usedis used as an shapeas initial an isinitial model similar (firstmodel to reference a (firstcorner reference antenna) truncated toantenna) realizepatch theantenna,to circularrealize which polarization.the circularcan be theoreticallypolarization.The hexagonal analyzedThe shape hexagonal is using similar ashape tocavity a corner is model similar truncated with to athe patchcorner magnetic antenna, truncated walls which resonatingpatch can beantenna, theoretically in TM which (Transverse analyzed can be Magnetic)theoreticallyusing a cavity mode analyzed model [21].