Resonant cavity antennas technology: Comparison
View Latest Version
Please note this is a comparison between Version 3 by Conner Chen and Version 2 by Mohammad Mahdi Honari.

       Resonant cavity antennas (RCAs) are suitable candidates to achieve high directivity with a low-cost and easy fabrication process. The stable functionality of the RCAs over different frequency bands, as well as, their pattern reconfigurability make them an attractive antenna structure for the next-generation wireless communication systems, i.e., fifth-generation (5G). The variety of designs and analytical techniques regarding the main radiator and partially reflective surface (PRS) configurations allow dramatic progress and advances in the area of RCAs. Adding different functionalities in a single structure by using additional layers is one appealing feature of the RCA structures, which has opened the various fields of studies toward 5G applications. This paper reviews the recent advances on the RCAs along with the analytical methods, and various capabilities that make them suitable to be used in 5G communication systems. 

  • resonant cavity antennas
  • Millimeter-wave
  • fifth-generation (5G)
  • partially reflective surface
  • Fabry–Pérot Cavity (FPC) structures
  • Reconfigurability

Dear author, the following contents are excerpts from your papers. They are editable.

(Due to the lack of relevant professional knowledge, our editors cannot complete a complete entry by summarizing your paper, so if you are interested in this work. you may need to write some contents by yourself. A good entry will better present your ideas, research and results to other scholars. Readers will also be able to access your paper directly through entries.)

1. History of Resonant cavity antennas

RCAs were first introduced in 1956 by Trentini [21], who demonstrated how placing a partially reflective surface (PRS) above a waveguide aperture antenna structure can increase the antenna directivity, significantly. Since then, further studies have been carried out in this area leading to introducing several PRS configurations with different functionalities in combination with various radiating elements inside the structure. In [22,23], Alexopoulos et showed that using full dielectric PRS layers above the antennas can provide a remarkable directivity improvement. Then, in [24,25], Jackson and Oliner conducted more studies on RCAs with multi-layer dielectric PRS. In [26], James et al. added an extra discussion to Terentini study and used a three-layer PRS to increase the gain of an aperture antenna. The conventional RC structures have utilized thick full dielectric or multi-layer PRS structures. By emerging electromagnetic bandgap (EBG), metamaterial (MTM), and frequency selective surface (FSS) structures, the trend of studies changed to the design of metallo-dielectric PRS layers to take advantage of fewer layers, thinner layers, more degrees of freedom, and layers with flexible properties.

       RCAs were first introduced in 1956 by Trentini [1], who demonstrated how placing a partially reflective surface (PRS) above a waveguide aperture antenna structure can increase the antenna directivity, significantly. Since then, further studies have been carried out in this area leading to introducing several PRS configurations with different functionalities in combination with various radiating elements inside the structure. In [2][3], Alexopoulos et showed that using full dielectric PRS layers above the antennas can provide a remarkable directivity improvement. Then, in [4][5], Jackson and Oliner conducted more studies on RCAs with multi-layer dielectric PRS. In [6], James et al. added an extra discussion to Terentini study and used a three-layer PRS to increase the gain of an aperture antenna. The conventional RC structures have utilized thick full dielectric or multi-layer PRS structures. By emerging electromagnetic bandgap (EBG), metamaterial (MTM), and frequency selective surface (FSS) structures, the trend of studies changed to the design of metallo-dielectric PRS layers to take advantage of fewer layers, thinner layers, more degrees of freedom, and layers with flexible properties.

In the literature, RCAs have associated with different terminologies such as electromagnetic bandgap (EBG) [27,28], RC structures [29], 2-D leaky-wave (LW) structures [30,31], PRS [32], and Fabry–Pérot Cavity (FPC) structures [33]. RCA structures consist of a PRS in parallel with a perfect electric/magnetic conductor or an impedance surface, which establish a cavity, fed by a main radiating element inside the cavity to excite the entire structure [21]. Open-ended waveguide, patch antenna, stacked antenna, dielectric resonant antenna (DRA), dipole antenna, and crossed bowtie dipole can be used as the main radiating element inside the cavity. The PRS layer might have different configurations as will be discussed later. It can be a full dielectric structure or a periodic structure composed of an array of metallic unit cells. Due to having a cavity with reflective surfaces, multiple reflections of electromagnetic waves happen. A proper cavity thickness (the distance between the PRS and the ground plane) can superimpose in-phase transmitted waves, which enhances the antenna gain significantly. The phase and magnitude of the PRS reflection behavior have a remarkable impact on the performance of the RCAs in terms of gain, bandwidth, beam angle and aperture efficiency. Therefore, designing the PRS structures has an imperative role in the design of the RCAs to achieve the desired performance.

        In the literature, RCAs have associated with different terminologies such as electromagnetic bandgap (EBG) [7][8], RC structures [9], 2-D leaky-wave (LW) structures [10][11], PRS [12], and Fabry–Pérot Cavity (FPC) structures [13]. RCA structures consist of a PRS in parallel with a perfect electric/magnetic conductor or an impedance surface, which establish a cavity, fed by a main radiating element inside the cavity to excite the entire structure [1]. Open-ended waveguide, patch antenna, stacked antenna, dielectric resonant antenna (DRA), dipole antenna, and crossed bowtie dipole can be used as the main radiating element inside the cavity. The PRS layer might have different configurations as will be discussed later. It can be a full dielectric structure or a periodic structure composed of an array of metallic unit cells. Due to having a cavity with reflective surfaces, multiple reflections of electromagnetic waves happen. A proper cavity thickness (the distance between the PRS and the ground plane) can superimpose in-phase transmitted waves, which enhances the antenna gain significantly. The phase and magnitude of the PRS reflection behavior have a remarkable impact on the performance of the RCAs in terms of gain, bandwidth, beam angle and aperture efficiency. Therefore, designing the PRS structures has an imperative role in the design of the RCAs to achieve the desired performance.

2. Application of Resonant cavity antennas

The demand for high traffic capacity and speed in wireless communication systems led to the fifth-generation (5G) technologies [1]. The upcoming 5G technologies provide a multitude of advantages including high data rate, high reliability, and low power consumption. More importantly, it brings newborn technologies to have smart cities and factories based on the industry 4.0 [2]. The millimeter-wave (MMW) frequency band has attracted significant attention among academic and industrial sectors, since it has enormous unlicensed bandwidth in comparison with other frequency bands [3]. Thus, MMW band can take an integral role in 5G communication systems. The MMW spectrum brings about compact structures and a higher data rate. However, many concerns are remained, which should be addressed in future communication technologies. One of these concerns is the high cost and complexity of fabrication processes within the MMW band. Another concern is the high energy loss of the MMW spectrum in comparison with the other frequency bands, which can be addressed by increasing the antenna gain.

       The demand for high traffic capacity and speed in wireless communication systems led to the fifth-generation (5G) technologies [14]. The upcoming 5G technologies provide a multitude of advantages including high data rate, high reliability, and low power consumption. More importantly, it brings newborn technologies to have smart cities and factories based on the industry 4.0 [15]. The millimeter-wave (MMW) frequency band has attracted significant attention among academic and industrial sectors, since it has enormous unlicensed bandwidth in comparison with other frequency bands [16]. Thus, MMW band can take an integral role in 5G communication systems. The MMW spectrum brings about compact structures and a higher data rate. However, many concerns are remained, which should be addressed in future communication technologies. One of these concerns is the high cost and complexity of fabrication processes within the MMW band. Another concern is the high energy loss of the MMW spectrum in comparison with the other frequency bands, which can be addressed by increasing the antenna gain. 

New research directions have been done to find effective solutions to address the aforementioned concerns over the MMW frequency band. Different antenna types with a variety of configurations have been proposed to compensate for the high loss and propagation issues such as interference of the MMW spectrum. Directional antennas with medium to high gain characteristics are excellent candidates to compensate the high loss of the MMW spectrum compared to the conventional planar antennas. Antenna structures such as reflectors [4] or waveguide horns [5,6] and even array antennas [7] and dielectric lenses [8] are conventional structures, which have potential to achieve high-gain and wideband characteristic. However, they have some issues such as being bulky, heavy, and complicated and having lossy feeding networks, which in turn draws attention to other possible alternative solutions. In fact, designing a proper antenna that meets the requirements of the upcoming 5G communication systems in a simple, efficient, low-profile structure is of prime importance, which has been the subject of many researches.

       New research directions have been done to find effective solutions to address the aforementioned concerns over the MMW frequency band. Different antenna types with a variety of configurations have been proposed to compensate for the high loss and propagation issues such as interference of the MMW spectrum. Directional antennas with medium to high gain characteristics are excellent candidates to compensate the high loss of the MMW spectrum compared to the conventional planar antennas. Antenna structures such as reflectors [17] or waveguide horns [18][19] and even array antennas [20] and dielectric lenses [21] are conventional structures, which have potential to achieve high-gain and wideband characteristic. However, they have some issues such as being bulky, heavy, and complicated and having lossy feeding networks, which in turn draws attention to other possible alternative solutions. In fact, designing a proper antenna that meets the requirements of the upcoming 5G communication systems in a simple, efficient, low-profile structure is of prime importance, which has been the subject of many researches.

There are different types of antennas, such as corrugated antennas [9,10,11], cavity-backed antennas [12,13], and SIW aperture antennas [14,15] that meet the requirement of having a high gain for 5G applications. Recently, much attention has been focused on the design of multi-functional antennas, which have a combination of characteristics in one single structure for different applications. In fact, having a high-gain antenna with features such as beam steering and circular polarization while being multi-frequency band, compact, and wideband is desired. Such structures are highly required for the next communication systems, since they lead to lower cost, compact size and even lower power consumption. It is still challenging to obtain multiple functionalities in just one antenna structure.

       There are different types of antennas, such as corrugated antennas [22][23][24], cavity-backed antennas [25][26], and SIW aperture antennas [27][28] that meet the requirement of having a high gain for 5G applications. Recently, much attention has been focused on the design of multi-functional antennas, which have a combination of characteristics in one single structure for different applications. In fact, having a high-gain antenna with features such as beam steering and circular polarization while being multi-frequency band, compact, and wideband is desired. Such structures are highly required for the next communication systems, since they lead to lower cost, compact size and even lower power consumption. It is still challenging to obtain multiple functionalities in just one antenna structure.

Recently, resonant cavity antennas have been attracting a growing attention due to their planar configuration, low fabrication difficulty, high-gain characteristic, and their capability of integration with other systems. Therefore, the RCAs with the capabilities of reconfigurability, polarization conversion, being wideband, or multi-band, while keeping high gain features have been investigated in a variety of studies. This type of antennas, which are a promising candidate to be used in the future 5G communication systems over the MMW frequency band, will be reviewed in this paper.  An example of their potential is the capability to be used in 5G wireless multiple-input-multiple-output (MIMO) systems due to having a low loss and compact structure with a high-gain characteristic. Besides, RCA structures can achieve steerable radiation patterns with a great radiation performance, which is an essential key for the future 5G base stations and mobile devices. Additionally, the RCAs can offer tilted radiation beam towards a desired direction, which is the demand of mobile communication base stations. Another potential use of the RCAs is in the wireless sensor network (WSN) for future 5G systems due to the requirement of using an efficient antenna with multi-function features to enrich the communication between the nodes [16,17,18,19,20].

       Recently, resonant cavity antennas have been attracting a growing attention due to their planar configuration, low fabrication difficulty, high-gain characteristic, and their capability of integration with other systems. Therefore, the RCAs with the capabilities of reconfigurability, polarization conversion, being wideband, or multi-band, while keeping high gain features have been investigated in a variety of studies. This type of antennas, which are a promising candidate to be used in the future 5G communication systems over the MMW frequency band, will be reviewed in this paper.  An example of their potential is the capability to be used in 5G wireless multiple-input-multiple-output (MIMO) systems due to having a low loss and compact structure with a high-gain characteristic. Besides, RCA structures can achieve steerable radiation patterns with a great radiation performance, which is an essential key for the future 5G base stations and mobile devices. Additionally, the RCAs can offer tilted radiation beam towards a desired direction, which is the demand of mobile communication base stations. Another potential use of the RCAs is in the wireless sensor network (WSN) for future 5G systems due to the requirement of using an efficient antenna with multi-function features to enrich the communication between the nodes [29][30][31][32][33].

References

  1. Trentini, G.V. Partially reflecting sheet arrays. IRE Transactions on Antennas and Propagation 1956, 4, 666–671.
  2. Jackson, D.; Alexopoulos, N. Gain enhancement methods for printed circuit antennas. IEEE Trans. Antennas Propag. 1985, 33, 976–987.
  3. Yang, H.; Alexopoulos, N. Gain enhancement methods for printed circuit antennas through multiple superstrates. IEEE Trans. Antennas Propag. 1987, 35, 860–863.
  4. Jackson, D.R.; Oliner, A.A. A leaky-wave analysis of the high-gain printed antenna configuration. IEEE Trans. Antennas Propag. 1988, 36, 905–910.
  5. Jackson, D.; Oliner, A.; Ip, A. Leaky-wave propagation and radiation for a narrow-beam multiple-layer dielectric structure. IEEE Trans. Antennas Propag. 1993, 41, 344–348.
  6. James, J.; Kinany, S.; Peel, P.; Andrasic, G. Leaky-wave multiple dichroic beamformers. Electron. Lett. 1989, 25, 1209–1211.
  7. Leger, L.; Monediere, T.; Jecko, B. Enhancement of gain and radiation bandwidth for a planar 1-D EBG antenna. IEEE Microw. Wirel. Compon. Lett. 2005, 15, 573–575.
  8. Hashmi, R.M.; Esselle, K.P. A wideband EBG resonator antenna with an extremely small footprint area. Microw. Opt. Technol. Lett. 2015, 57, 1531–1535.
  9. Meng, F.; Sharma, S.K. A Wideband Resonant Cavity Antenna With Compact Partially Reflective Surface. IEEE Trans. Antennas Propag. 2020, 68, 1155–1160.
  10. Zhao, T.; Jackson, D.R.; Williams, J.T.; Yang, H.Y.; Oliner, A.A. 2-D periodic leaky-wave antennas-part I: metal patch design. IEEE Trans. Antennas Propag. 2005, 53, 3505–3514.
  11. Zhao, T..; Jackson, D.R.; Williams, J.T. 2-D periodic leaky-wave Antennas-part II: slot design. IEEE Trans. Antennas Propag. 2005, 53, 3515–3524.
  12. Baba, A.A.; Hashmi, R.M.; Esselle, K.P.; Marin, J.G.; Hesselbarth, J. Broadband Partially Reflecting Superstrate-Based Antenna for 60 GHz Applications. IEEE Trans. Antennas Propag. 2019, 67, 4854–4859.
  13. Vaidya, A.R.; Gupta, R.K.; Mishra, S.K.; Mukherjee, J. High-gain low side lobe level Fabry Perot cavity antenna with feed patch array. Prog. Electromagn. Res. C 2012, 28, 223–238.
  14. Thompson, J.; Ge, X.; Wu, H.C.; Irmer, R.; Jiang, H.; Fettweis, G.; Alamouti, S. 5G wireless communication systems: Prospects and challenges [Guest Editorial]. IEEE Commun. Mag. 2014, 52, 62–64.
  15. Rappaport, T.S.; Sun, S.; Mayzus, R.; Zhao, H.; Azar, Y.; Wang, K.; Wong, G.N.; Schulz, J.K.; Samimi, M.; Gutierrez, F. Millimeter wave mobile communications for 5G cellular: It will work! IEEE access 2013, 1, 335–349.
  16. Honari, M.M.; Mirzavand, R.; Melzer, J.; Mousavi, P. A new aperture antenna using substrate integrated waveguide corrugated structures for 5G applications. IEEE Antennas Wirel. Propag. Lett. 2016, 16, 254–257.
  17. Mahajan, M.; Jyoti, R.; Sood, K.; Sharma, S.B. A Method of Generating Simultaneous Contoured and Pencil Beams From Single Shaped Reflector Antenna. IEEE Trans. Antennas Propag. 2013, 61, 5297–5301.
  18. Deguchi, H.; Tsuji, M.; Shigesawa, H. Compact low-cross-polarization horn antennas with serpentine-shaped taper. IEEE Trans. Antennas Propag. 2004, 52, 2510–2516.
  19. Honari, M.M.; Abdipour, A.; Moradi, G. Aperture-coupled multi-layer broadband ring-patch antenna array. IEICE Electron. Expr. 2012, 9, 250–255.
  20. Cheng, Y.J.; Guo, Y.X.; Liu, Z.G. W-Band Large-Scale High-Gain Planar Integrated Antenna Array. IEEE Trans. Antennas Propag. 2014, 62, 3370–3373.
  21. Fan, C.; Yang, W.; Che, W.; He, S.; Xue, Q. A Wideband and Low-Profile Discrete Dielectric Lens Using 3-D Printing Technology. IEEE Trans. Antennas Propag. 2018, 66, 5160–5169.
  22. Honari, M.M.; Mirzavand, R.; Mousavi, P. A high-gain planar surface plasmon wave antenna based on substrate integrated waveguide technology with size reduction. IEEE Trans. Antennas Propag. 2018, 66, 2605–2609.
  23. Honari, M.M.; Sarabandi, K.; Mousavi, P. Dual-Band High-Gain Planar Corrugated Antennas With Integrated Feeding Structure. IEEE Access 2020, 8, 67075–67084.
  24. Honari, M.M.; Sarabandi, K.; Mousavi, P. Design and Analysis of Corrugated Antennas Based on Surface Susceptance of a Single Cell of Corrugation. IEEE Trans. Antennas Propag. 2020, doi:10.1109/TAP.2020.2979278
  25. Amjadi, S.M.; Sarabandi, K. A low-profile, high-gain, and full-band subarray of cavity-backed slot antenna. IEEE Trans. Antennas Propag. 2017, 65, 3456–3464.
  26. Guan, D.F.; Ding, C.; Qian, Z.P.; Zhang, Y.S.; Guo, Y.J.; Gong, K. Broadband high-gain SIW cavity-backed circular-polarized array antenna. IEEE Trans. Antennas Propag. 2016, 64, 1493–1497.
  27. Yang, D.; Cao, F.; Pan, J. A single-layer dual-frequency shared-aperture SIW slot antenna array with a small frequency ratio. IEEE Antennas Wirel. Propag. Lett. 2018, 17, 1048–1051.
  28. Honari, M.M.; Mirzavand, R.; Saghlatoon, H.; Mousavi, P. A dual-band low-profile aperture antenna with substrate-integrated waveguide grooves. IEEE Trans. Antennas Propag. 2016, 64, 1561–1566.
  29. Mirzavand, R.; Honari, M.M.; Mousavi, P. Direct-Conversion Sensor for Wireless Sensing Networks. IEEE Trans. Ind. Electron. 2017, 64, 9675–9682.
  30. Saghlatoon, H.; Mirzavand, R.; Honari, M.M.; Mousavi, P. Sensor Antenna Transmitter System for Material Detection in Wireless-Sensor-Node Applications. IEEE Sens. J. 2018, 18, 8812–8819.
  31. Khalid, N.; Mirzavand, R.; Saghlatoon, H.; Honari, M.M.; Mousavi, P. A Three-Port Zero-Power RFID Sensor Architecture for IoT Applications. IEEE Access 2020, 8, 66888–66897.
  32. Mirzavand, R.; Honari, M.M.; Laribi, B.; Khorshidi, B.; Sadrzadeh, M.; Mousavi, P. An unpowered sensor node for real-time water quality assessment (humic acid detection). Electronics 2018, 7, 231.
  33. Mirzavand, R.; Honari, M.M.; Mousavi, P. High-resolution dielectric sensor based on injection-locked oscillators. IEEE Sens. J. 2017, 18, 141–148.
More
© Text is available under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/)
ScholarVision Creations
Feedback