# A Dual-Polarized Printed Antenna Based on a Tapered Slot SICL Balun for Airborne Radar Application

Authors: Xiaochun Liu; Li Wang; Mingxi Zhang; Shaobin Liu; Guiqiang Du
Journal: International Journal of Antennas and Propagation
 (2020)

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## Abstract

The substrate-integrated coaxial line (SICL) is a potential transmission line due to its good characteristics of high efficiency, nondispersive, and single operational mode. A tapered slot SICL balun is proposed, which can realize the impedance transformation from the microstrip line to the coplanar strip line (CPS). At the same time, the proposed balun can transform the quasi-TEM mode of the microstrip line to the TEM mode of CPS. A printed dipole radiator is designed and is fed by the proposed SICL balun to achieve the impedance matching. The dual-polarized radiation mode is realized by employing two orthogonal printed dipoles. For each polarization radiator, the CPS is bended to avoided the occlusion of two polarization ports and realize the direct assembling of two orthogonal printed circuits. What is more, the assembling method is advantageous to improve the port isolation degree and decrease the cross polarization level. To improve the ratio of front to back (F/B) of the radiation pattern, a cylindrical metal cavity is adopted. According to the results of simulation and experiments, the VSWR of each port is lower than 2, the isolation degree between two polarization ports is higher than 20 dB, and the cross polarization level at the boresight is lower than −20 dB at the operational frequency. The patterns of two ports are almost symmetric, and high radiation efficiency is obtained. The experimental results of the principle prototype verify the design schemes of the balun and the dual-polarized antenna. The proposed dual-polarized antenna fed by the tapered slot SICL balun is suitable for the airborne radar application.


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## Body

## 1. Introduction

For the airborne radar, the dual-polarized system can achieve the remarkable improvement of operational performances. Especially, the polarization signal processing technique has huge application potential in the field of interference suppression. The dual-polarized antenna is the key component of novel airborne radar and has drawn more and more attention. So far, a lot of schemes of dual-polarized antennas have been proposed, which include dual-polarized microstrip antenna [1], dual-polarized dielectric resonator antenna [2], dual-polarized horn antenna [3], dual-polarized slot antenna [4], dual-polarized monopole antenna [5, 6], dual-polarized dipole antenna [7], and dual-polarized lens antenna [8]. Whereas, the dual-polarized dipole antenna is suitable for the airborne application in view of its characteristics of simple structure, low cost, and stable performance. For the design of the dual-polarized dipole antenna, balun is hard to research and design, which realize the conversion from the balanced port to the unbalanced port.In 2006, the SICL was proposed, and it has a lot of advantages such as wideband, low loss, strong interference suppression ability, and convenient integration. SICL supports propagation of the transverse electromagnetic (TEM) mode wave, and hence, it is a nondispersive transmission line which can work within the frequency range from zero frequency to microwave band. Recently, SICL has obtained more attention in the microwave technical field. At present, the SICL can be used to design the antenna [9–14], balun [15], and transition between SICL [16, 17] and filter [18–20].In [9], a multichannel SICL array with coaxial lines placed in both vertical and horizontal directions was proposed for high-speed parallel data transmission, and its maximum bandwidth of a single channel of the SICL array is up to 56 GHz, and the coupling of adjacent channels in the SICL array is less than −30 dB. In [10], a wideband circularly polarized cavity-backed patch antenna excited by SICL was proposed operating at Q-band for IEEE 802.11aj (45 GHz) applications. The growing interest in collision avoidance automotive radar systems in Ka-band necessitates the development of dedicated antenna systems with a 45° inclined linear polarization (LP). A 45° inclined and linearly polarized slot array antenna in the Ka-band with SICL technique is presented for collision avoidance automotive radar system application in [12]. Zhu et al. [15] proposed an ultrawideband (UWB) Marchand balun by using substrate-integrated coaxial line (SICL) technology, which is suitable for applications in UWB communication systems. A high-quality transition from coplanar waveguide to empty coaxial line is proposed in [16]; with this transition, the coaxial line is completely integrated in a planar circuit board so that it truly becomes an empty substrate-integrated coaxial line. A transition from microstrip to empty substrate-integrated coaxial line (ESICL) is presented in [17].In [18], a compact filter based on SICL stubs was designed using an advanced multilayer printed circuit board (PCB) substrate, and this technology is convenient to implement high-density interconnect (HDI) devices, which are dedicated to mass market and require to be compact and low cost. Borja et al. [19] presented the design and performance of a planar narrow bandwidth bandpass filter with high-quality factor, and its structure is composed of an empty substrate-integrated coaxial line with the center conductor suspended in air. A novel wide stopband bandpass filter implemented with spur stepped impedance resonator (SSIR) and SICL technology is proposed in [20]. A tapered slot balun based on SICL was proposed in this paper, and then a dual-polarized dipole antenna was designed by employing the proposed SICL balun for the airborne application. The geometry structures of the proposed SICL balun and dual-polarized antenna are presented in Section 2. The performance analysis and optimization of the dual-polarized antenna are carried out in Section 3. The experimental results of the antenna prototype are provided in Section 4, and conclusions are drawn in Section 4.


## 2. Geometry Structure of the Tapered Slot SICL Balun and the Dual-Polarized Antenna

### 2.1. SICL Structure

SICL is a kind of technology of the planarization of the coaxial line. Like the traditional coaxial cable, SICL is also a shielding and nondispersive TEM guiding wave structure, which has features of wideband, low loss, highQ, small size, and convenient connection with the high-speed system. The first high-order mode for SICL is TE10, and intermediate conductor does not affect the field characteristics of the TE10 mode. The single-mode bandwidth can be controlled by adjusting the spacing between two rows of metalized via holes, which can realize wider band than the substrate-integrated waveguide (SIW). SICL is mainly composed of the conductor in the bottom which is connected with the ground, intermediate conductor, and the conductor on the top, two side walls which consist of metalized holes and two substrate layers. Herein, the outside conductors are formed from the bottom conductor, two side walls, and top conductor. A typical SICL structure is shown in Figure 1. Under certain assumptions, the cutoff frequency of SICL for the TE10 mode can be expressed by(1)fTE10=c2εrws−D20.95S,where ws, D, and S are shown in Figure 1, and c is the light speed in vacuum. Because D and S are limited by the PCB manufacturing process, the cutoff frequency of the TE10 mode is the single-mode band of SICL.Figure 1
Structure diagram of the typical SICL.


### 2.2. Design of the Tapered Slot SICL Balun

Figure2 shows the tapered slot SICL balun which is one of the dual-polarized dipole antenna ports, and these two ports have the same SICL balun. The whole feeding structure is composed of the tapered slot SICL balun, SICL transmission section, and impedance transformation section. The SICL balun is connected with the dipole radiator and SICL transmission section, herein the symmetric dipole excited by CPS is the balanced structure, and the SICL transmission line is the unbalanced structure. The length of the SICL transmission line was LSICL−f1, and this section has advantages of single mode, nondispersive, and low signal loss. For the impedance transformation section, the microstrip line adopted linearly tapered form, in which length was f5. The end section was a uniform microstrip line with a length of f4, and its characteristic impedance was 50 Ω. The impedance realized the transformation from SICL to microstrip line with a characteristic impedance of 50 Ω. The microstrip line with a characteristic impedance of 50 Ω was connected with the coaxial cable of the transmitter or the receiver. The SICL designed in this paper included two layers of substrates which had different thicknesses, and the thicknesses of the substrates on the bottom layer and the top layer were h2 and h1, respectively. In this section, h2 was determined to be 1 mm, and h1 was changed to obtain the impedance matching and port isolation. Both two-layer substrates were selected to be FR-4. The diameter of conducting holes and distance between two adjacent holes are r and d.Figure 2
Structure diagram of the SICL balun. (a) The whole feeding structure. (b) The whole feeding structure when the grounds on the top and bottom of substrates are concealed.
(a)
(b)Figure3 shows the circuit model of the SICL balun. The radiation impedance of the printed dipole antenna is ZA, and the feeding line is CPS with the characteristic impedance of Z02. The input microstrip line is an unbalanced structure, in which characteristic impedance is Z01. The impedance matrix of the whole feeding balun is Z, and its normalized impedance matrix is Z˜. The corresponding transition matrix of the whole feeding balun isA, and its normalized transition matrix is A˜. According to the conversion formula between the network matrix, we can obtain the formula(2)A˜=1Z˜21Z˜11detZ˜1Z˜22,where detZ˜=Z˜11Z˜22−Z˜12Z˜21.Figure 3
The circuit model of the SICL balun.From the matrixA˜, the four matrix elements can be expressed as(3)A11=A˜11Z01Z02,A12=A˜12Z01Z02,A21=A˜21Z01Z02,A22=A˜22Z02Z01.Then, the input impedance of the SICL balun can be expressed as(4)Zin=A11ZA+A12A21ZL+A22.When the input port is in the matching state,Zin=Z0=50Ω. It can be seen that impedance matching can be realized by adjusting ZA and Z. ZA is determined by the structure and parameters of the antenna radiator. The impedance matrix of the SICL balun can be changed by adjusting the length f1 of tapered slot SICL, the width w of internal the conducting strip, and the distance ws between two column conducting holes.The whole balun realizes the function of transformation from balance to unbalance and impedance matching from microstrip line to printed CPS. The antenna radiator is the terminal load of the CPS output port. The whole circuit system achieves good power transmission performance. The parameters of the whole balun are optimized by electromagnetic simulation. The obtained transmission performance curve of the designed balun in this paper is shown in Figure4. It can be seen that the insertion loss is about −1.89 dB at the central frequency point.Figure 4
The simulated transmission performance curve of the designed balun.


### 2.3. Structure of the Dual-Polarized Backed Cavity Dipole Antenna

Two polarized dipole radiators of the designed dual-polarized antenna fed by the tapered slot SICL balun were realized through the printed circuit board (PCB) in this paper. The designed dipoles of dual-polarized were exponentially tapered, which is like the Vivaldi antenna, whereas it is indeed a dual-polarized dipole antenna. For each polarization port, two arms of the dipole radiator are placed on the same side of the medium substrate, which are fed by CPS. The adopted feeding method can realize the impedance matching between the dipoles and the feeding line. In order to improve the feed efficiency, the SICL balun was designed, which realizes the transformation from microstrip line to CPS. The SICL balun was also designed to achieve the impedance matching from the input microstrip line to the coplanar dipole radiator. In the SICL balun, there is a transition section between the input microstrip line and the SICL. The whole structure schematic diagram of the designed dual-polarized antenna based on the SICL balun is shown in Figure5.Figure 5
Schematic diagram of the dual-polarized antenna based on the SICL balun: (a, b) polarization port 1, (c) back cavity, and (d) structure of the whole dual-polarized antenna.
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(d)In this paper, the exponentially tapered dipoles which can be seen called as Vivaldi-shaped dipoles, were designed. The designed structure diagram of the Vivaldi-shaped dipole antenna based on the SICL balun is shown in Figure6. According to the coordinate system in Figure 5, the equation of curve 1 can be written as(5)x1=a1er1y+d1,where both a1 and d1 are constants, which are used to control the size of the dipole.Figure 6
Structure diagram of the Vivaldi-shaped dipole antenna based on the SICL balun.Also, the equation of curve 1 can be written as(6)x2=a2er1y+d2,where both a2 and d2 are constants, which are used to control the bottom shape of the dipole.In the procedure of the fabrication of the dual-polarized printed dipole antenna, the two polarization radiation parts are orthogonally mounted, so occlusion phenomenon appears, which causes the low isolation between two polarization ports. In this paper, the transmission lines were bended, and the two orthogonal dipoles were separated at the vertical direction, so the two polarization radiators did not cross. According to this method, two substrates of the dual-polarized antenna can be mounted and fixed directly, and jumper work was avoided, which is beneficial to the practical engineering. The value of height difference between two SICL baluns is defined asd_antenna.


## 2.1. SICL Structure

SICL is a kind of technology of the planarization of the coaxial line. Like the traditional coaxial cable, SICL is also a shielding and nondispersive TEM guiding wave structure, which has features of wideband, low loss, highQ, small size, and convenient connection with the high-speed system. The first high-order mode for SICL is TE10, and intermediate conductor does not affect the field characteristics of the TE10 mode. The single-mode bandwidth can be controlled by adjusting the spacing between two rows of metalized via holes, which can realize wider band than the substrate-integrated waveguide (SIW). SICL is mainly composed of the conductor in the bottom which is connected with the ground, intermediate conductor, and the conductor on the top, two side walls which consist of metalized holes and two substrate layers. Herein, the outside conductors are formed from the bottom conductor, two side walls, and top conductor. A typical SICL structure is shown in Figure 1. Under certain assumptions, the cutoff frequency of SICL for the TE10 mode can be expressed by(1)fTE10=c2εrws−D20.95S,where ws, D, and S are shown in Figure 1, and c is the light speed in vacuum. Because D and S are limited by the PCB manufacturing process, the cutoff frequency of the TE10 mode is the single-mode band of SICL.Figure 1
Structure diagram of the typical SICL.


## 2.2. Design of the Tapered Slot SICL Balun

Figure2 shows the tapered slot SICL balun which is one of the dual-polarized dipole antenna ports, and these two ports have the same SICL balun. The whole feeding structure is composed of the tapered slot SICL balun, SICL transmission section, and impedance transformation section. The SICL balun is connected with the dipole radiator and SICL transmission section, herein the symmetric dipole excited by CPS is the balanced structure, and the SICL transmission line is the unbalanced structure. The length of the SICL transmission line was LSICL−f1, and this section has advantages of single mode, nondispersive, and low signal loss. For the impedance transformation section, the microstrip line adopted linearly tapered form, in which length was f5. The end section was a uniform microstrip line with a length of f4, and its characteristic impedance was 50 Ω. The impedance realized the transformation from SICL to microstrip line with a characteristic impedance of 50 Ω. The microstrip line with a characteristic impedance of 50 Ω was connected with the coaxial cable of the transmitter or the receiver. The SICL designed in this paper included two layers of substrates which had different thicknesses, and the thicknesses of the substrates on the bottom layer and the top layer were h2 and h1, respectively. In this section, h2 was determined to be 1 mm, and h1 was changed to obtain the impedance matching and port isolation. Both two-layer substrates were selected to be FR-4. The diameter of conducting holes and distance between two adjacent holes are r and d.Figure 2
Structure diagram of the SICL balun. (a) The whole feeding structure. (b) The whole feeding structure when the grounds on the top and bottom of substrates are concealed.
(a)
(b)Figure3 shows the circuit model of the SICL balun. The radiation impedance of the printed dipole antenna is ZA, and the feeding line is CPS with the characteristic impedance of Z02. The input microstrip line is an unbalanced structure, in which characteristic impedance is Z01. The impedance matrix of the whole feeding balun is Z, and its normalized impedance matrix is Z˜. The corresponding transition matrix of the whole feeding balun isA, and its normalized transition matrix is A˜. According to the conversion formula between the network matrix, we can obtain the formula(2)A˜=1Z˜21Z˜11detZ˜1Z˜22,where detZ˜=Z˜11Z˜22−Z˜12Z˜21.Figure 3
The circuit model of the SICL balun.From the matrixA˜, the four matrix elements can be expressed as(3)A11=A˜11Z01Z02,A12=A˜12Z01Z02,A21=A˜21Z01Z02,A22=A˜22Z02Z01.Then, the input impedance of the SICL balun can be expressed as(4)Zin=A11ZA+A12A21ZL+A22.When the input port is in the matching state,Zin=Z0=50Ω. It can be seen that impedance matching can be realized by adjusting ZA and Z. ZA is determined by the structure and parameters of the antenna radiator. The impedance matrix of the SICL balun can be changed by adjusting the length f1 of tapered slot SICL, the width w of internal the conducting strip, and the distance ws between two column conducting holes.The whole balun realizes the function of transformation from balance to unbalance and impedance matching from microstrip line to printed CPS. The antenna radiator is the terminal load of the CPS output port. The whole circuit system achieves good power transmission performance. The parameters of the whole balun are optimized by electromagnetic simulation. The obtained transmission performance curve of the designed balun in this paper is shown in Figure4. It can be seen that the insertion loss is about −1.89 dB at the central frequency point.Figure 4
The simulated transmission performance curve of the designed balun.


## 2.3. Structure of the Dual-Polarized Backed Cavity Dipole Antenna

Two polarized dipole radiators of the designed dual-polarized antenna fed by the tapered slot SICL balun were realized through the printed circuit board (PCB) in this paper. The designed dipoles of dual-polarized were exponentially tapered, which is like the Vivaldi antenna, whereas it is indeed a dual-polarized dipole antenna. For each polarization port, two arms of the dipole radiator are placed on the same side of the medium substrate, which are fed by CPS. The adopted feeding method can realize the impedance matching between the dipoles and the feeding line. In order to improve the feed efficiency, the SICL balun was designed, which realizes the transformation from microstrip line to CPS. The SICL balun was also designed to achieve the impedance matching from the input microstrip line to the coplanar dipole radiator. In the SICL balun, there is a transition section between the input microstrip line and the SICL. The whole structure schematic diagram of the designed dual-polarized antenna based on the SICL balun is shown in Figure5.Figure 5
Schematic diagram of the dual-polarized antenna based on the SICL balun: (a, b) polarization port 1, (c) back cavity, and (d) structure of the whole dual-polarized antenna.
(a)
(b)
(c)
(d)In this paper, the exponentially tapered dipoles which can be seen called as Vivaldi-shaped dipoles, were designed. The designed structure diagram of the Vivaldi-shaped dipole antenna based on the SICL balun is shown in Figure6. According to the coordinate system in Figure 5, the equation of curve 1 can be written as(5)x1=a1er1y+d1,where both a1 and d1 are constants, which are used to control the size of the dipole.Figure 6
Structure diagram of the Vivaldi-shaped dipole antenna based on the SICL balun.Also, the equation of curve 1 can be written as(6)x2=a2er1y+d2,where both a2 and d2 are constants, which are used to control the bottom shape of the dipole.In the procedure of the fabrication of the dual-polarized printed dipole antenna, the two polarization radiation parts are orthogonally mounted, so occlusion phenomenon appears, which causes the low isolation between two polarization ports. In this paper, the transmission lines were bended, and the two orthogonal dipoles were separated at the vertical direction, so the two polarization radiators did not cross. According to this method, two substrates of the dual-polarized antenna can be mounted and fixed directly, and jumper work was avoided, which is beneficial to the practical engineering. The value of height difference between two SICL baluns is defined asd_antenna.


## 3. Performance Analysis and Optimization of the Dual-Polarized Antenna Fed by the Tapered Slot SICL Balun

According to performance requirements of impedance matching, isolation degree, and patterns in engineering, the full-wave electromagnetic simulation technique was used to simulate and optimize the dual-polarized printed dipole antenna based on the SICL balun. A set of parameter values that meet the requirements aref1 = 7 mm, f3 = 15 mm, c1 = 10 mm, g1 = 15 mm, g2 = 6 mm, ws = 3 mm, w = 0.6 mm, h1 = 3.5 mm, h2 = 1 mm, and w_edge_1 = 5 mm. Figure 7 shows the simulated S-parameter results. At the operational frequency of 2 GHz, the return losses of two ports are lower than −10 dB, and the isolation degree is larger than 22 dB.Figure 7
S-parameter simulation results of the dual-polarized antenna based on SICL. (a) The simulated return loss of polarization port 1. (b) The simulated return loss of polarization port 2. (c) The simulated isolation degree between two polarization ports.
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(b)
(c)The current distributions on the patches are shown in Figure8. It can be seen that the proposed SICL balun can transform the quasi-TEM mode of the microstrip line to the TEM mode of CPS. With the period of T at 2 GHz, the currents on the dipole focus on the edges of dipole arms, which lead to linearly polarized radiation fields, and the effective radiation mode is achieved.Figure 8
Current distributions on the dual-polarized antenna based on the SICL balun: (a)t = 0, (b) t = T/4, (c) t = T/2, and (d) t = 3T/4.
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(d)Figure9 shows the three-dimension radiation patterns of two ports at the working frequency, and for each port, the gain pattern and axial ratio pattern are provided, respectively. According to the simulated results, the axial ratios of two ports are higher than 30 dB, which indicates the low cross polarization levels are obtained. The simulated gains of two ports are about 4.4 dBi and 4.2 dBi, respectively; moreover, the approximate symmetric patterns for two ports are observed.Figure 9
Three-dimension patterns of the dual-polarized antenna based on the SICL balun. (a) The gain of port 1. (b) The AR of port 1. (c) The gain of port 2. (d) The AR of port 2.
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(b)
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(d)The simulated E and H plane patterns of two ports at working frequency for the dual-polarized antenna are shown in Figure10. According to Figure 9, for port 1, the half power beam widths at the E plane and the H plane are about 40.5° and 40.6°, respectively. For port 2, the half power beam widths at the E plane and the H plane are about 40.4° and 41.4°, respectively. It is obvious that two ports have achieved almost symmetric radiation patterns.Figure 10
Simulated E and H plane patterns of the dual-polarized antenna: (a) patterns at the E plane for port 1, (b) patterns at the H plane for port 1, (c) patterns at the E plane for port 2, and (d) patterns at the H plane for port 2.
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(d)During the antenna optimization, the effects ofd_antenna, f1, and the radius added value r_cavity_addedof cavity on the return losses and isolation degree between ports were simulated. Simulated variation curves of the return loss and isolation degree with d_antenna are shown in Figure 11. When d_antenna varied from 1 mm to 5 mm, the return loss changes little, yet the isolation degree becomes larger obviously. What is more, when d_antenna is 2 mm, the return loss is less than −10 dB and the isolation degree is higher than 22 dB, which can satisfy the requirements in engineering.Figure 11
The effect curves ofd_antenna on antenna performances. (a) Effect on the return loss of port 1 with d_antenna. (b) Effect on the return loss of port 2 with d_antenna. (c) Effect on the isolation degree with d_antenna.
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(b)
(c)Simulated variation curves of the return loss and isolation degree withf1 are shown in Figure 12. When f1 varied from 1 mm to 9 mm, the resonant frequency moves to lower frequency band for two ports, whereas the isolation degree almost unchanged. It can be seen that the return loss is less than −10 dB and the isolation degree higher than 22 dB when f1 is 7 mm.Figure 12
The effect curves off1 on antenna performances. (a) Effect on the return loss of port 1 with f1. (b) Effect on the return loss of port 2 with f1. (c) Effect on the isolation degree with f1.
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(c)Simulated variation curves of the return loss and isolation degree withr_cavity_added are shown in Figure 13. When r_cavity_added varied from 30 mm to 110 mm, r_cavity_added mainly affects the impedance matching degree, while has slight influence on the resonant frequency. The isolation degree did not change remarkably with r_cavity_added.Figure 13
The effect curves ofr_cavity_added on antenna performances. (a) Effect on the return loss of port 1 with r_cavity_added. (b) Effect on the return loss of port 2 with r_cavity_added. (c) Effect on the isolation degree with r_cavity_added.
(a)
(b)
(c)The fabrication errors of the antenna designed in this paper mainly come from the assembly errors between two bipolar circuit boards and the installation errors of the cylindrical metal cavity. The fabrication errors of the circuit boards are very small and can be neglected. The error simulation is carried out by using full-wave electromagnetic simulation technology, and the distance between the bottom of the cavity and the printed circuit board is studied. The simulation results show that the VSWR and the isolation of polarization ports at the input end almost have no obvious variations within the small assembly error range of less than 5 mm, and the radiation pattern of the antenna has little variation except that the gain is changed about 0.7 dB compared with the designed value. Therefore, the difference between the simulation and calculation results of the antenna designed in this paper mainly comes from the test error. Due to the limitation of laboratory experimental conditions, the test error of the antenna is slightly larger. However, the test results are basically consistent with the simulation results, which verify the design scheme.


## 4. Experiment Results of the Antenna Prototype

According to the structure and size, the designed dual-polarized dipole antenna fed by the SICL balun was fabricated. The PCB photo of the antenna prototype is shown in Figure14. The simulated return losses and isolation degree between two ports are shown in Figures 15(a), 11(b), and 11(c), respectively. At the working frequency, the return losses of two ports are lower than −10 dB, and the measured return losses are almost in agreement with the simulated results. The measured isolation degree is higher than 25 dB at the working frequency, which is better than the simulated result.Figure 14
The photo of the dual-polarized antenna prototype. (a) The front view of PCB for port 1. (b) The back view of PCB for port 1. (c) The front view of PCB for port 2. (d) The back view of PCB for port 2.
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(d)Figure 15
Tested circuit characteristics of the dual-polarized antenna. (a) The measured return loss of port 1. (b) The measured return loss of port 2. (c) The measured isolation degree between two ports.
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(c)The radiation patterns were measured in the anechoic room, and the measured patterns of two ports at the working frequency are shown in Figures16 and 17, respectively. For each port, the patterns at both E plane and H plane are provided, respectively. It can be seen that the radiation patterns are formed effectively. The measured gain of port 1 is about 0.9 dB lower than the simulated ones, and the measured cross polarization level of port 1 is about −25 dB. The measured gain of port 2 is about 0.6 dB lower than that of simulated ones, and the measured cross polarization level of port 2 is about −28 dB. For both port 1 and port 2, the beam widths are close to the simulated results. The measured performances are worse than the simulated results owing to the errors caused by fabrication and measurement.Figure 16
Measured patterns of polarization port 1. (a) The pattern at the E plane. (b) The pattern at the H plane.
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(b)Figure 17
Measured patterns of polarization port 2. (a) The pattern at the E plane. (b) The pattern at the H plane.
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## 5. Conclusion

This paper proposed a tapered slot SICL balun and designed a dual-polarized printed dipole antenna fed by the proposed SICL balun. The analysis method of the SICL balun was depicted. For the designed dual-polarized antenna, a cylindrical metal backed cavity is used to improve the F/B of radiation patterns. The designed backed cavity dual-polarized printed dipole antenna is excited by bended coplanar strip lines which can avoid the occlusion of two ports and improve the isolation degree between two ports. The SICL feeder realized the balanced-to-unbalanced transformation from the dipoles to the microstrip line, and the impedance transformation was also obtained. The simulation and experimental results verify the scheme of the SICL balun and the dual-polarized antenna. The researched dual-polarized antenna fed by the tapered slot SICL balun can be used in airborne radar.



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*Source: 7148969-2020-03-14.xml*