J. Electromagn. Eng. Sci Search


J. Electromagn. Eng. Sci > Volume 22(3); 2022 > Article
Park, Cha, and Hong: Wideband Directive Self-Complementary Bowtie Antenna for Ka-band


This paper presents a novel wideband directive self-complementary bowtie antenna (SCBA) designed for Ka-band. The proposed antenna is well suited for wireless power transfer and energy harvesting of compact devices using 5G frequencies. The proposed SCBA consists of self-complementary triangular elements and a ground plane, which are added to enhance directivity. The optimized design exhibits a wide impedance bandwidth that covers the entire Ka-band, despite the presence of a ground plane. The proposed SCBA was validated via simulation and measurement. The results demonstrate a bandwidth of 43.8% (25.8–40.1 GHz) and a maximum gain of 10.4 dBi at 29.5 GHz with a compact antenna size of 9.2 mm × 8.7 mm.

I. Introduction

With the advent of 5G communications, millimeter-wave (mm-wave) frequencies at Ka-band, which are allocated for high-band 5G use, have recently garnered considerable interest [13]. In addition, improved data rates provided by 5G technology have become a springboard for the development of Internet-of-Things (IoT) technology in various applications [46]. Improved data rates require higher energy consumption of battery-powered IoT devices, but compact IoT devices inevitably have a short battery lifetime due to battery-size limitations. To solve the battery problem of IoT devices in 5G wireless systems, far-field wireless power transfer (WPT) and RF energy harvesting have the potential as a means for supplying energy to compact, low-power devices using mm-waves [79].
In these WPT and energy harvesting scenarios, it is essential to design an optimal mm-wave receive antenna to efficiently collect electromagnetic waves [10, 11]. Although it is common for mm-wave antennas to be configured in an array due to their small physical size [1214], arrays may still be too large for implementation on compact, low-power IoT devices with small footprints. For this reason, a compact single antenna with good radiation characteristics would be desirable for devices with a limited size. Moreover, a compact, single antenna has the advantage of being applied not only to IoT devices that make use of 5G communications but also to ultra-compact devices that do not need 5G capability but can still benefit from using compact antennas for energy harvesting. Various single antenna designs have been proposed in recent studies that can be utilized for mm-wave WPT and energy harvesting schemes [1521]. In particular, a wideband mm-wave antenna has the advantage of being able to accommodate a wide range of mm-wave frequencies [1621].
In this regard, a bowtie antenna with wideband characteristics can be a reasonable option, but an additional feeding structure, such as a balun, is required due to its dipole-based configuration. To compensate for this structural complexity, a self-complementary design can be applied to the bowtie antenna to simplify the feeding structure, thereby minimizing antenna size while maintaining a wide bandwidth [22, 23].
In this study, we propose a novel wideband directive self-complementary bowtie antenna (SCBA) that covers the entire Ka-band (26–40 GHz), which can be utilized as a single receive antenna for WPT and energy harvesting in compact devices. Unlike the conventional SCBA based on a design without a ground plane [23], the proposed SCBA design includes a ground plane to prevent unnecessary backward radiation, thereby enhancing directivity. Despite the presence of a ground plane that reduces bandwidth, the optimized design with a ground plane exhibits a wideband characteristic that covers the entire Ka-band. In other words, the proposed SCBA not only has enhanced gain through the ground plane but also maintains the wide bandwidth of the conventional SCBA. The proposed wideband directive SCBA is demonstrated via numerical simulation and measurement.

II. Wideband Self-Complementary Bowtie Design

Fig. 1 illustrates the geometry of the proposed wideband SCBA. The SCBA consists of a bowtie-shaped structure with one conductive triangular patch and a complementary slot printed on the front side and a ground plane on the backside of the substrate. The patch and slot are symmetric with the same shape, forming the basis of a self-complementary structure. The substrate used in this design is a Rogers RT/Duroid 6002 laminate (ɛr = 2.94), which is known for low loss at high frequencies. The thickness of the substrate is chosen to be 1.524 mm, which is the standard thickness of the substrate that provides the best fit for our frequency band of interest. To elaborate, this allows us to set the ground plane distance to be a quarter wavelength at 28.7 GHz, which falls within the Ka-band. We then optimized the design parameters of the proposed SCBA to acquire a wide bandwidth. To accommodate the compact size of the SCBA, an SMPM connector is used as the coaxial feed. Using a compact coaxial feed connector should minimize its influence on the radiation pattern. The effect of the ground plane can be confirmed by comparing the radiation pattern of the SCBA with and without the ground plane. Fig. 2(a) and 2(b) show three-dimensional (3D) radiation patterns simulated at 28.5 GHz with and without the ground plane of the proposed SCBA, respectively. In the absence of a ground plane, the radiation pattern is visible as nearly symmetrical upward and downward, whereas in the presence of a ground plane, radiation occurs mostly in the upward direction. For this reason, the proposed design, which includes a ground plane, provides an enhanced gain compared to a conventional design.
As shown in Fig. 1(a), the feed line is in the form of a coplanar structure. The length and angle of the bowtie-shaped structure and the width of the center co-planar strip connected to the conductive patch are optimized for impedance matching. By adding an upper extra substrate region to the basic self-complementary structure, impedance matching at lower frequencies (below 27 GHz) is improved. A trapezoidal-shaped ground patch at the co-planar feed line improves impedance matching at higher frequencies (above 37 GHz). In addition, the triangular slot added at the co-planar feed line contributes to an enhanced broadside gain. As a result, the overall design is optimized to significantly improve the impedance bandwidth (IBW) and gain of the proposed SCBA in the Ka-band. The proposed SCBA has dimensions of 9.2 mm × 8.7 mm, and the optimized geometrical parameter values are listed in Fig. 1.

III. Measurement and Analysis

We tested the IBW of the proposed wideband SCBA via numerical simulation using SEMCAD X [24] and measurement using an Anritsu MS46122B vector network analyzer. As mentioned previously, the antenna was fabricated on a Rogers RT/Duroid 6002 substrate and connected with an SMPM connector (see Fig. 3(a)). In Fig. 3(b), the simulated and measured |S11| of the proposed SCBA are plotted. There is a reasonable agreement between the simulated and measured IBWs. The measured IBW (between −10 dB points) is about 43.4% (25.8–40.1 GHz), demonstrating that the proposed wideband SCBA covers the entire Ka-band.
The radiation performance of the proposed wideband SCBA was also verified via simulation and measurement. The simulation was carried out using SEMCAD X, while the measurement was performed in an mm-wave spherical nearfield anechoic chamber, as shown in Fig. 4. Seven multiple dual-polarized probes inside the chamber measure a 3D nearfield pattern through mechanical and electronic omnidirectional scans. The near-field data are then transformed into far-field quantities to obtain radiation characteristics. From this measurement, full 3D co-polarized radiation patterns for five selected frequencies within the IBW of the antenna are obtained, as illustrated in Fig. 5. These results clearly show the effect of the ground plane on suppressing unnecessary radiation in the downward direction and, therefore, improving broadside gain as expected.
Fig. 6(a) and 6(b) show the simulated and measured radiation patterns for five selected frequencies, respectively, in the E− and H-plane (i.e., yz-plane and xz-plane in Fig. 5). There are some discrepancies between the simulated and measured co-polarized (co-pol) patterns, which are possibly attributed to an additional loss in the SMPM connector and substrate, and a misalignment of the antenna in the measurement setup. Nevertheless, the simulated and measured co-pol patterns, in general, exhibit good agreement in both the E− and H-plane. Although the main beam direction of the co-pol patterns in both the E− and H-plane tends to be slightly tilted at some frequencies, the broadside gain in the entire Ka-band belongs to the half-power beam-width of the main beam. Furthermore, it can be seen that the simulated and measured cross-polarized (cross-pol) radiation patterns maintain a significantly lower level compared to the co-pol patterns, where the difference in the broadside gain of the co-pol and cross-pol patterns is more than about −10 dB (up to −27.5 dB) at all five selected frequencies in both the E− and H-plane.
In Fig. 7, the maximum realized gain values at each discrete frequency point within the IBW are plotted, where the simulated and measured values also follow a similar trend with respect to each other. The peak simulated gain value of 9 dBi occurs at 28.5 GHz, while the peak measured value of 10.4 dBi occurs at 29.5 GHz. Note that the maximum gain values in Fig. 6 are obtained from the radiation patterns in the E− and/or H-plane, but if the antenna is not aligned perfectly, the actual maximum gain direction may deviate from the measured E− and/or H-plane patterns. Therefore, the gain measurement of the antenna can be further improved through a more precise antenna alignment and connection, which is a very delicate procedure, especially in the mm-wave frequency regime. The overall results demonstrate that the proposed SCBA design allows a wide IBW covering the entire Ka-band through an optimized design despite the presence of the ground plane; in addition, it provides a high broadside gain with improved directivity by pre-venting downward radiation.
Table 1 compares the performance of the proposed wideband SCBA with that of the ones in other recently reported works. For a reasonable comparison, only single-element antennas designed for frequency bands similar to this work are considered. The proposed wideband SCBA features the largest IBW covering the entire Ka-band and a relatively small electrical antenna size while maintaining the maximum gain as high as 10.4 dBi. In particular, the presence of a ground plane can be a more suitable choice when the antenna is used for a device-mounted application. Therefore, our proposed wideband SCBA has good potential for use in mm-wave WPT and energy harvesting scenarios for compact IoT devices.

IV. Conclusion

A novel wideband SCBA that covers the entire Ka-band with a ground plane for enhanced broadside gain was proposed and tested. By adding the ground plane and optimizing the antenna design accordingly, the proposed SCBA exhibits an IBW of 43.4% (from 25.8 to 40.1 GHz) and a maximum gain of 10.4 dBi at 29.5 GHz. The proposed design allows for high IBW with a small antenna size despite the presence of a ground plane; therefore, it is well suited for use in future mm-wave WPT and energy harvesting scenarios for compact devices, especially for device-mounted applications.


This work was supported by the Office of Naval Research Global (Grant No. 62909-19-1-2049).

Fig. 1
Geometry of the wideband SCBA: (a) top view and (b) perspective view (W1 = 4.25 mm, W2 = 2 mm, W3 = 1.655 mm, W4 = 0.262 mm, W5 = 0.21 mm, W6 = 0.518 mm, L1 = 7.171 mm, L2 = 3.35 mm, L3 = 1.486 mm, L4 = 1.404 mm, L5 = 1.422 mm, L6 = 1 mm).
Fig. 2
Simulated 3D radiation patterns of the SCBA: (a) with ground plane and (b) without ground plane.
Fig. 3
(a) Fabricated wideband SCBA and (b) reflection coefficient (|S11|) of the proposed SCBA.
Fig. 4
Photograph of the anechoic chamber measurement setup.
Fig. 5
Measured 3D co-polarized gain patterns at selected frequencies of the proposed wideband SCBA.
Fig. 6
Simulated and measured gain patterns at selected frequencies of the proposed sideband SCBA: (a) E-plane patterns and (b) H-plane patterns.
Fig. 7
Maximum realized gain versus frequency.
Table 1
Comparison with other reported single mm-wave antenna designs
Study, year Frequency (GHz) IBW (%) Max. gain (dBi) Size (λ02)
Karthikeya et al. [15], 2019 27–30 10 9.2 @ 28.8 GHz 2.95 × 2.95
Ta et al. [16], 2017 26.5–38.2 36.2 5.8 @ 31 GHz N/A
Jilani et al. [17], 2018 28–39 32.8 10.2 @ 36 GHz 1.41 × 3.35
Karthikeya et al. [18], 2019 25–30 18.2 8.3 @ 33.5 GHz 1.83 × 0.92
Karthikeya et al. [19], 2019 27–33 20 6.6 @ 29.8 GHz 2 × 0.95
Magray et al. [20], 2020 26–32 20.7 7.5 @ 29 GHz 0.58 × 0.97
Ozpinar et al. [21], 2020 20–28.5 35.1 9 @ 28 GHz 0.97 × 1.29
This work 25.8–40.1 43.4 10.4 @ 29.5 GHz 1.01 × 0.95

λ0 is the wavelength at the center frequency of the bandwidth.


1. TS Rappaport, S Sun, R Mayzus, H Zhao, Y Azar, K Wang et al., "Millimeter wave mobile communications for 5G cellular: it will work! IEEE Access, vol. 1, pp. 335–349, 2013.
2. JG Andrews, S Buzzi, W Choi, SV Hanly, A Lozano, ACK Soong, and JC Zhang, "What will 5G be? IEEE Journal on Selected Areas in Communications, vol. 32, no. 6, pp. 1065–1082, 2014.
3. S Rangan, TS Rappaport, and E Erkip, "Millimeter-wave cellular wireless networks: potentials and challenges," Proceedings of the IEEE, vol. 102, no. 3, pp. 366–385, 2014.
4. MR Palattella, M Dohler, A Grieco, G Rizzo, J Torsner, T Engel, and L Ladid, "Internet of things in the 5G era: enablers, architecture, and business models," IEEE Journal on Selected Areas in Communications, vol. 34, no. 3, pp. 510–527, 2016.
5. L Chettri and R Bera, "A comprehensive survey on Internet of Things (IoT) toward 5G wireless systems," IEEE Internet of Things Journal, vol. 7, no. 1, pp. 16–32, 2020.
6. K Shafique, BA Khawaja, F Sabir, S Qazi, and M Mustaqim, "Internet of Things (IoT) for next-generation smart systems: a review of current challenges, future trends and prospects for emerging 5G-IoT scenarios," IEEE Access, vol. 8, pp. 23022–23040, 2020.
7. G Wu, C Yang, S Li, and GY Li, "Recent advances in energy-efficient networks and their application in 5G systems," IEEE Wireless Communications, vol. 22, no. 2, pp. 145–151, 2015.
8. B Alzahrani and W Ejaz, "Resource management for cognitive IoT systems with RF energy harvesting in smart cities," IEEE Access, vol. 6, pp. 62717–62727, 2018.
9. D Zhai, R Zhang, J Du, Z Ding, and FR Yu, "Simultaneous wireless information and power transfer at 5G new frequencies: channel measurement and network design," IEEE Journal on Selected Areas in Communications, vol. 37, no. 1, pp. 171–186, 2019.
10. P Burasa, T Djerafi, and K Wu, "A 28 GHz and 60 GHz dual-band on-chip antenna for 5G-compatible IoT-served sensors in standard CMOS process," IEEE Transactions on Antennas and Propagation, vol. 69, no. 5, pp. 2940–2945, 2021.
11. M Wagih, GS Hilton, AS Weddell, and S Beeby, "Broadband millimeter-wave textile-based flexible rectenna for wearable energy harvesting," IEEE Transactions on Microwave Theory and Techniques, vol. 68, no. 11, pp. 4960–4972, 2020.
12. N Yoon and C Seo, "A 28-GHz wideband 2 × 2 U-slot patch array antenna," Journal of Electromagnetic Engineering and Science, vol. 17, no. 3, pp. 133–137, 2017.
13. B Yu, K Yang, CYD Sim, and G Yang, "A novel 28 GHz beam steering array for 5G mobile device with metallic casing application," IEEE Transactions on Antennas and Propagation, vol. 66, no. 1, pp. 462–466, 2018.
14. H Wang and I Park, "Characteristic of the angled printed dipole array antenna with different numbers of dipole elements," Journal of Electromagnetic Engineering and Science, vol. 20, no. 3, pp. 183–189, 2020.

15. GS Karthikeya, MP Abegaonkar, and SK Koul, "Gain equalized shared-aperture antenna using dual-polarized ZIM for mmWave 5G base stations," IEEE Antennas and Wireless Propagation Letters, vol. 18, no. 6, pp. 1100–1104, 2019.
16. SX Ta, H Choo, and I Park, "Broadband printed-dipole antenna and its arrays for 5G applications," IEEE Antennas and Wireless Propagation Letters, vol. 16, pp. 2183–2186, 2017.
17. SF Jilani, QH Abbasi, ZU Khan, TH Loh, and A Alomainy, "A Ka-band antenna based on an enhanced Franklin model for 5G cellular networks," Microwave and Optical Technology Letters, vol. 60, no. 6, pp. 1562–1566, 2018.
crossref pdf
18. GS Karthikeya, MP Abegaonkar, and SK Koul, "A wideband conformal antenna with high pattern integrity for mmWave 5G smartphones," Progress in Electromagnetics Research Letters, vol. 84, pp. 1–6, 2019.
19. GS Karthikeya, MP Abegaonkar, and SK Koul, "CPW fed wideband corner bent antenna for 5G mobile terminals," IEEE Access, vol. 7, pp. 10967–10975, 2019.
20. MI Magray, GS Karthikeya, K Muzaffar, SK Koul, and AH Moon, "Wideband asymmetric coplanar strip fed antennas with pattern diversity for mmWave 5G base stations," IEEE Access, vol. 8, pp. 77482–77489, 2020.
21. H Ozpinar, S Aksimsek, and NT Tokan, "A novel compact, broadband, high gain millimeter-wave antenna for 5G beam steering applications," IEEE Transactions on Vehicular Technology, vol. 69, no. 3, pp. 2389–2397, 2020.
22. Y Mushiake, "Self-complementary antennas," IEEE Antennas and Propagation Magazine, vol. 34, no. 6, pp. 23–29, 1992.
23. CC Lin, "Compact bow-tie quasi-self-complementary antenna for UWB applications," IEEE Antennas and Wireless Propagation Letters, vol. 11, pp. 987–989, 2012.
24. Schmid & Partner Engineering AG, SEMCAD X, 2022. [Online]. Available: https://speag.swiss/products/semcad/overview/


Hong Soo Park and Kyu Ho Cha contributed equally to this work.


Hong Soo Park received his B.S. (with honors) and M.S. degrees in electronic engineering from Soongsil University, Seoul, South Korea, in 2019 and 2021, respectively. He is currently pursuing his Ph.D. degree at Soongsil University. His research interests include wireless power transfer, antennas, microwave and millimeter-wave devices, electromagnetic time-reversal, and electromagnetics in complex environments. Mr. Park received five poster awards at the Korean Institute of Electromagnetic Engineering and Sciences (KIEES) conferences in 2017, 2018, 2019, and 2021 and the Best Paper Award at the KIEES Conference in 2020.


Kyu Ho Cha received his B.S. degree in electronic engineering from Soongsil University, Seoul, South Korea, in 2021. He is currently pursuing his M.S. degree at Soongsil University. His research interests include antennas, nonlinear detection, and microwave and millimeter-wave devices. Mr. Cha received the Best Paper Award at the Korean Institute of Electromagnetic Engineering and Sciences (KIEES) Conference in 2021.


Sun K. Hong received his B.S. degree in electrical engineering from the University of Maryland, College Park, MD, USA, in 2005, and his M.S. and Ph.D. degrees in electrical engineering from Virginia Tech, Blacksburg, VA, USA, in 2008 and 2012, respectively. From 2005 to 2015, he was a research engineer at the US Naval Research Laboratory in Washington, DC. From 2015 to 2017, he was an assistant professor in the Department of Electrical and Computer Engineering at the Rose-Hulman Institute of Technology, Terre Haute, IN, USA. Since 2017, he has been with the School of Electronic Engineering at Soongsil University, where he is an associate professor. His current research interests include wireless power transfer, electromagnetic waves in a complex propagation environment, antennas, and the detection of nonlinear devices, radars, and high-power electromagnetics.
Share :
Facebook Twitter Linked In Google+
METRICS Graph View
  • 1 Crossref
  • 1 Scopus
  • 4,124 View
  • 160 Download
Related articles in JEES


Browse all articles >

Editorial Office
#706 Totoo Valley, 217 Saechang-ro, Yongsan-gu, Seoul 04376, Korea
Tel: +82-2-337-9666    Fax: +82-2-6390-7550    E-mail: admin-jees@kiees.or.kr                

Copyright © 2024 by The Korean Institute of Electromagnetic Engineering and Science.

Developed in M2PI

Close layer
prev next