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Q-Band MIMO Antennas with Circular Polarization for Spatial and Polarization Diversity

2024, Journal of infrared, millimeter, and terahertz waves

Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 https://doi.org/10.1007/s10762-024-00979-w REVIEW Q‑Band MIMO Antennas with Circular Polarization for Spatial and Polarization Diversity Nada Alaa1 · Rania A. Elsayed1 · Asmaa E. Farahat2 · Khalid F. A. Hussein2 · Walid S. El‑Deeb1 Received: 25 October 2023 / Accepted: 7 March 2024 / Published online: 25 March 2024 © The Author(s) 2024 Abstract The present work proposes three MIMO antennas with different configurations for the future applications of wireless communications in the Q-band of the frequency to realize both spatial and polarization diversities. A circularly polarized (CP) printed antenna operating over two frequency bands at 37.8 and 50 GHz is utilized as a single element to construct the proposed MIMO antennas. Two-element MIMO antenna systems arranged in two configurations, side-by-side and face-to-face, are proposed to achieve spatial diversity. Also, a four-element MIMO antenna system is designed to achieve polarization diversity in addition to spatial diversity. The proposed MIMO antenna systems are designed with the aid of the CST simulator. The three MIMO antennas are fabricated and their performance is experimentally evaluated regarding the circular polarization, impedance matching, antenna gain, envelope correlation coefficient (ECC), and diversity gain (DG). The experimental results for the single-element as well as the MIMO antennas come in good agreement with simulation results showing high performance. Both the numerical and experimental investigations reveal that the mutual coupling between any two ports of the proposed MIMO antennas is below −25dB. Also, for any two ports it is shown that the ECC is below 1 × 10−7 and the diversity gain is higher than 9.99. The impedance matching bandwidths (for ||S11 || < −10dB) are shown to be 1.53 and 1.88 GHz at 37.8 and 50GHz, respectively, and the corresponding 3-dB axial ratio bandwidths are 700 and 130MHz, respectively. Keywords Circular polarization · Dual-band · MIMO · Patch antenna · Polarization diversity and spatial diversity Extended author information available on the last page of the article 13 Vol.:(0123456789) 394 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 1 Introduction Multiple input multiple output (MIMO) antenna systems employ multiple radiating elements at the transmitter and the receiver. In MIMO system, the transmitter sends data over different multipath propagation then the receiver combines these data through multipath. The main constraint in MIMO antenna system is the uncorrelated multipath which can be provided by using antenna elements acting independently. The MIMO technique provides uncorrelated multipath propagation to attain different diversity schemes. A variety of diversity schemes can be realized such as spatial (space) [1], polarization [2], frequency, pattern (angular) [3–5], and transmit/receive diversity. Employing a dual-band antenna system is preferred to employing two antenna systems operating at two different frequencies because it provides a more compact solution especially for mobile handsets. On the other hand, the circular polarization is preferred for a mobile handset antenna because it allows receiving the power of the incoming signal whether it is circularly polarized (CP) or linearly polarized (LP) without being affected by the misalignment between the transmitting and the receiving antennas. The forthcoming generations of mobile handset need advanced features such as wide bandwidth, high data rate, multiple frequency operation, compact size, and light weight [6–8]. Recently, many research papers [9, 10] focus on the design of mobile handset MIMO antennas for millimeter-wave communications. The work of [11] presents a two-port triple-band MIMO antenna of two elements where each has a single stub that can be embedded in the feed line. There are four symmetric square slots and two cuts in the ground plane to realize circular polarization. The obtained radiation patterns are quasi-omnidirectional. In [12], a dual-band dual-polarized (DBDP) MIMO antenna is designed by using square patch with three rectangular slits and a decoupling mechanism is embedded in the ground structure to enhance the isolation. The non-diagonal slit is responsible for circular polarization. This design is based on the single-feed dual-band antenna and the dual polarization is realized by using an orthogonal feed. There is another category based on using stacked structure that consists of two elements operating at two different frequency bands. In [13], a penta-band MIMO antenna is introduced by adding meander line-shaped radiator with L-shaped matching stub, and ground plane having semi-circle-shaped slot, and inverted L-shaped stub. The proposed four-element MIMO has circular polarization in only two bands. The isolation technique used in design is the inverted L-shaped decoupling structure. In [1], circularly polarized four-element MIMO dielectric resonator antenna (DRA) operating at two frequency bands is studied. We aim to achieve some objectives such as bandwidth enhancement by using a ring-shaped ceramic radiator, dual bands by using incorporation of a rectangular aperture lead, circular polarization by using conversion of rectangular to Z-shaped slot, and reduction of mutual coupling by using space diversity. The work of [14] illustrates the DRA technique for two-port dual-band MIMO antenna with circular polarization. For exciting HE modes, two probes placed orthogonal, that is, an azimuthal angular distance 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 395 of 90◦, to each other are used. Moreover, to realize the required quadrature timephase between these modes, the length of two probes must be tuned. The two ring DRAs are excited by using two arc-shaped feed lines with four conformal probes. In [15], a dual-band circularly polarized dielectric resonator antenna is used to implement two-port MIMO antenna that consists of a moon-shaped aperture. To stimulate ring-shaped DRA, L-shaped microstrip line with a serial step impedance transformer is used. Modification from cylindrical to ring-shaped dielectric resonator provides wide impedance bandwidth. Aperture is helpful to excite the dual orthogonal hybrid modes for circular polarization waves. Polarization diversity is supportive to reduce the mutual coupling between ports. A broadband antenna operating over the 38 GHz frequency band is proposed in [16], using circular patch antenna loaded by three patches between circular radius and feed-line and perpendicular pair of elliptical slots inside the circular patch. This antenna has small size with 7-dB gain and 90% radiation efficiency. In [17] and [18], a compact multiband antenna operating at 28, 38, and 55 GHz is introduced. The antenna has an umbrella-shaped patch with high gain and efficiency. A wideband, high-gain, low-profile, and high-efficiency fractal antenna operating at 39 GHz is investigated in [19]. The antenna is designed on a Rogers RT/duroid 5880 with a compact size of 15 × 15 × 0.79 mm. This work introduces two-element as well as four-element MIMO antenna systems to achieve spatial diversity as well as polarization diversity for millimeter wave (mm-wave) applications. A dual-band circularly polarized (DBCP) microstrip patch antenna is used as a single element to construct the proposed MIMO antennas. The single element is designed as a main patch and a parasitic patch. The main patch has circular geometry with two square slots at the center and two notches on the circumference. The parasitic patch consists of four parasitic elements indirectly fed by capacitively coupling to the main patch. To produce circular polarization, the structure of the single element antenna is symmetric about an axis that is inclined to the feed line at angle of 45◦ . For impedance matching, the main patch is fed through a microstrip line with tapered geometry. Two-element MIMO antenna systems are proposed to produce spatial diversity: face-to-face and side-by-side arrangements. The four-element MIMO antennas are proposed to produce both spatial and polarization diversity at the same time. If the elements have the same sense of polarization, then spatial diversity is obtained, whereas polarization diversity is obtained if the elements have different senses of polarization. The proposed MIMO antenna systems have two operational frequency bands centered at 38 and 50 GHz and produce circular polarization over the two frequency bands. The diversity schemes provided by these MIMO antennas are investigated by the CST simulator where the envelope correlation coefficient (ECC) and the diversity gain (DG) are investigated and demonstrated. The presentation of this work is organized as follows. Section 2 presents the design of the single-element dual-band CP antenna. Section 3 introduces the proposed MIMO antennas with the different configurations. Section 4 describes the fabrication process and the experimental setup for measurements. Section 5 presents 13 396 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 the simulation and experimental results with elaborate discussions for performance assessment. Section 6 introduces a summary of this work and some comparisons to the achievements of the other published papers. Finally, Section 7 gives the conclusions related to the present work. 2 Design of Single‑Element Antenna The geometry of the CP patch antenna proposed as a single element for the two-element and four-element MIMO antenna systems is depicted in Fig. 1. This antenna consists of a circular patch that acts as the main radiator which is reactively loaded by four parasitic patches as seen in Fig. 1a. To produce circular polarization, two square slots are made near the patch center and two notches are etched at the patch edge to get the line of symmetry of the antenna structure having a slope of 45◦ with the center line of the feeding microstrip line. Also, the ground structure is defected by etching two square slots as shown in Fig. 1b. Thus, the overall patch and defected ground geometry have a line of symmetry making 45◦ with the center line of the microstrip line feeder. This symmetry produces two degenerate radiating modes (resonances) of the cavity between the circular patch and the ground plane. The radiated fields of the two modes have nearly equal magnitudes, orthogonal orientations, and inphase quadrature; these conditions produce a circularly polarized field in the far zone of the antenna. The antenna’s geometrical parameters should be set to the appropriate values to satisfy these conditions. The antenna impedance is matched at the desired frequencies by the tapered microstrip line feeder. The dimensions of the tapered region of this line, WT , LT , and WF , should be set to get the antenna impedance matched to 50Ω source at the required frequencies. The parasitic elements help to get the antenna impedance matched over a higher frequency band. The Y-shaped slits at the corners of the parasitic elements improve the axial ratio and increase its 3-dB bandwidth. The geometric symmetry of the antenna around an axis inclined to the feed line at an angle of 45◦ produces right-hand circularly polarized (RHCP) field in the far zone. If this geometry is mirrored about the centerline of the microstrip feeder, lefthand circularly polarized (LHCP) fields are produced in the far zone. It will be shown, later, that two antennas of opposite senses of polarization can be used in a four-element MIMO antenna configuration to provide polarization diversity in addition to the spatial diversity. The optimal dimensions of this antenna are listed in Table 1. It should be noted that these dimensions have been obtained through an extensive parametric study that has been achieved using the CST simulator. The proposed MIMO is designed using a substrate material of the type Rogers RO3003. The substrate has a thickness h = 0.25mm , loss tangent tan𝛿 = 0.001, and dielectric constant 𝜀r = 3. In this section, two-element and four-element configuration of MIMO antenna systems are proposed to produce spatial and polarization diversity. The design of the proposed MIMO antennas are presented in the following subsections. 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 397 (a) (b) (c) (d) Fig. 1 Structure of the dual-band circularly polarized single-element patch antenna. a Top view. b Bottom view. c Detailed view of the patch. d Close view at one notch on the patch circumference 13 398 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 Table 1 Optimum values of the dimensions of the single-element antenna proposed for different MIMO antenna configurations Dimension RP LP WF LF WT LT WG G WE WS LC WY LY DY Value (mm) 1.17 2.9 0.6 11.05 0.1 7.6 0.6 1.414 0.13 0.2 0.4 0.13 0.2 0.18 3 Proposed MIMO Antenna Systems In this section, the designs of the proposed MIMO antennas are described in detail. Two-element MIMO antennas arranged in side-by-side and face-to-face configurations are designed to produce spatial diversity. Also, four-element MIMO antenna system is designed to produce both spatial and polarization diversity. The following two subsections are dedicated for the description of the different types of the proposed MIMO antenna configurations. 3.1 Two‑Port MIMO Antenna Configurations for Spatial Diversity Two configurations are proposed to construct two-element MIMO antennas by using the CP patch described in Section 2. In the first configuration, the patch antennas are arranged side-by-side, whereas in the other configuration, the two patch elements are arranged face-to-face as shown. For two-element MIMO antenna, the ECC can be expressed as follows [20]: ECC1,2 | ∗ |2 ∗ S22 | |S11 S12 + S21 | | = 2 2 2 2 ∗ (1 − ||S11 || − ||S12 || )(1 − ||S21 || − ||S22 || ) For two-element MIMO antenna, the DG can be expressed as follows [20]: √ DG = 10 1 − |ECC|2 (1) (2) Each of the proposed two-element MIMO antenna configurations may have different performance from the other and both are investigated in the present work. The next two subsections are dedicated to describe the designs of the proposed twoelement MIMO configurations. 3.1.1 Two‑Element MIMO Antenna in Side‑by‑Side Configuration In the two-element side-by-side MIMO antenna configuration, the patch antennas are arranged as shown in Fig. 2. If the two elements in this MIMO antenna configuration have the same sense of polarization, then spatial diversity is produced. If an element is LHCP whereas the other element is RHCP, then polarization diversity is 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 RHCP 399 RHCP 1 2 (b) (a) Fig. 2 Design of the two-element side-by-side MIMO antenna using two elements of the dual-band circularly polarized antenna. a Top view. b Bottom view 2 1 RHCP RHCP (a) (b) Fig. 3 Design of the two-element face-to-face MIMO antenna using two elements of the dual-band circularly polarized antenna. a Top view. b Bottom view 13 400 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 produced. In this MIMO antenna, the elements are printed on the same substrate. The overall physical dimensions of the two-element side-by-side MIMO antenna are L1 = 19mm and W1 = 18.5mm . The spacing between the antenna elements is DS = 6.1mm. 3.1.2 Two‑Element MIMO Antenna in Face‑to‑Face Configuration In the two-element face-to-face MIMO antenna configuration, the patch antennas are arranged as shown in Fig. 3. If the two elements in this MIMO antenna configuration have the same sense of polarization, then this MIMO antenna produces spatial diversity. If an element is LHCP whereas the other element is RHCP, then polarization diversity is produced. In this MIMO antenna, the elements are printed on the same substrate. The overall physical dimensions of the two-element face-to-face MIMO antenna are L2 = 32mm and W2 = 10mm . The spacing between the antenna elements is DF = 4.66mm. 3.2 Four‑Element MIMO Configuration for Both Spatial and Polarization Diversity Four elements of the dual-band CP antenna, described in Section 2, are arranged as shown in Fig. 4 to implement the proposed MIMO antenna system. To obtain polarization diversity in addition to the spatial diversity by such four-element MIMO antenna, elements 1 and 4 are RHCP, whereas elements 2 and 3 are LHCP. In this way, both spatial and polarization diversities are obtained. The separation distances between the elements are DS = 6.1mm and DF = 4.66mm . The total dimensions of the four-element MIMO antenna are L3 = 32mm and W3 = 18.5mm. 4 Fabrication and Experimental Setup for Measurements Prototypes are fabricated for experimental evaluation of the proposed single-element and MIMO antennas’ performance. The reflection coefficient at the antenna input ports and the radiation patterns are measured and compared to the simulation results. 4.1 Fabricated Prototypes Prototypes are fabricated for the single-element, two-element side-by-side MIMO, two-element face-to-face MIMO, and four-element MIMO antennas whose designs are presented in Figs. 1, 2, 3, and 4, respectively. The fabricated prototypes are presented in Fig. 5. The elements of the MIMO antennas are fed at each port through 1.85-mm coaxial end launchers from Southwest Microwave Inc. The purpose of fabricating these prototypes is the experimental evaluation of the antenna performance for comparison with the simulation results. 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 401 3 1 RHCP LHCP LHCP RHCP 2 4 (a) (b) Fig. 4 Design of the four-element MIMO antenna system using four dual-band circularly polarized patch antennas. a Top view. b Bottom view 4.2 Measurement of the Self and Mutual Scattering Parameters The self and mutual scattering parameters are measured with the aid of the VNA model Rhode and Schwartz ZVA67. The end-launch connectors of type 1.85mm from Southwest Microwave Inc. are used to connect the antennas under test to the VNA for measurement as shown in Figs. 6 and 7. 13 402 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 Fig. 5 Fabricated prototypes of the proposed antennas. a Single element. b Two-element side-by-side MIMO antenna. c Two-element face-to-face MIMO antenna. d Four-element MIMO antenna 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 403 Fig. 6 Measurement of the S-parameter, S11, of the fabricated single-element antenna. a The antenna connected to the VNA cable via the end-launch connector. b Experimental setup showing the antenna connected to port 2 of the VNA Fig. 7 Measurement of the S-parameters, S11, S22, and S21, of the two-element side-by-side fabricated prototypes. a Two fabricated elements arranged side-by-side and connected to the VNA cables via the end-launch connectors. b Experimental setup showing two-element MIMO antenna connected to ports 1 and 2 of the VNA 13 404 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 VNA Cables (2) (1) Fig. 8 The fabricated two-element face-to-face MIMO antenna is prepared for measuring the self and mutual scattering parameters, S11, S22, and S21 Matched Loads VNA Cables (1) (3) (2) (4) Fig. 9 The fabricated four-element MIMO antenna is prepared for measuring the self and mutual scattering parameters, S11, S22, and S21. The VNA cables are connected to ports 1 and 2 and matched loads are connected to ports 3 and 4 of the MIMO The fabricated prototypes of the two-element (face-to-face) and the four-element antennas are prepared for measuring the self and mutual the S-parameters, S11, S22, and S21, as seen in Figs. 8 and 9, respectively. 4.3 Measurement of the Radiation Patterns The gain and radiation patterns of the proposed single-element and MIMO antennas are measured by the aid of the VNA. The experimental setup is presented in Fig. 10 showing the reference gain linearly polarized horn antenna mounted on the polarization rotator, the antenna-under-test (AUT) mounted on the directional rotator. The horn antenna model LB-018400 is employed to perform measurements over the frequency range of 18–40 GHz while the horn antenna model LB-12–10-A is employed to perform measurements over the frequency range of 40–60 GHz. The AUT and the 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 405 VNA (ZVA67) Antenna under Test Reference Horn Antenna Antenna Rotator Fig. 10 Gain and radiation pattern pattern measurement setup showing the AUT and reference horn antenna connected to ports 1 and 2 of the VNA, respectively 0 |S 11 | (dB) -10 -20 Simulation Measurement -30 -40 30 35 40 45 50 55 Frequency (GHz) Fig. 11 Results of simulation and measurement of the reflection coefficient magnitude, ||S11 ||, at the feeding port of the single-element antenna over a broad frequency band 13 406 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 reference-gain horn antenna are connected to ports 1 and 2 of the VNA, respectively. The ratio of the received power to the transmitted power is assessed by the magnitude of the transmission coefficient,||S21 ||, between AUT and the reference antenna. 5 Results and Discussions The simulation results and experimental measurements are presented and discussed in this section. The main concern of such presentations is the performance evaluation of the single-element antenna as well as the MIMO antennas with the different configurations proposed in the present work. 5.1 Performance Evaluation of the Single‑Element Antenna The frequency dependence of ||S11 || at the feeding port of the single-element dualband circularly polarized antenna, described in Section 2, is investigated by simulation as well as experimental measurement at the frequencies ranging from 34 to 54 GHz. Figure 11 shows that the measurements are very close to the simulation results. It is shown that the antenna impedance is perfectly matched to 50Ω over the two frequency bands at 38 and 50 GHz. 6 6 5 5 4 4 AR (dB) AR (dB) Simulation Measurement 3 3 2 2 1 1 Simulation Measurement 0 36.5 37 37.5 38 Frequency (GHz) (a) 38.5 0 49.6 49.8 50 50.2 50.4 Frequency (GHz) (b) Fig. 12 Results of simulation and measurement of the AR over (a) the lower frequency band and (b) the higher frequency band 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 0 0 dB 30 60 -40 -60 90 90 -60 Simulation Measurement 90 Simulation Measurement 120 120 150 30 -20 60 60 -40 90 0 dB 30 30 -20 60 407 120 150 120 150 150 180 180 (a) (b) Fig. 13 Total field radiation patterns of the single-element antenna at 37.8GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 0 0 30 0 dB -20 60 30 30 90 -60 90 -60 90 Simulation Measurement Simulation Measurement 120 120 150 60 -40 -40 90 30 -20 60 60 0 dB 150 120 120 150 150 180 180 (a) (b) Fig. 14 Total field radiation patterns of the single-element antenna at 50GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ The variations of the AR of the single-element antenna with the frequency around the frequencies 37.8 and 50GHz are presented in Fig. 12a and b, respectively. As shown in these figures, the experimental measurements show excellent agreement with the simulation results. The 3dB-AR bandwidth at 37.8 and 50GHz are 700 and 300 MHz, respectively. The total far-field radiation patterns of the single-element antenna at 38 and 50 GHz are depicted in Figs. 13 and 14, respectively. The radiation patterns produced at the two frequencies show that this single-element antenna is a good candidate to construct MIMO antenna systems with high performance. 13 408 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 |S 11 | (dB) -10 -20 Simulation Measurement -30 -40 30 35 40 45 50 55 Frequency (GHz) Fig. 15 Results of simulation and measurement of ||S11 || at port 1 of the two-element side-by-side MIMO antenna over a broad frequency band -20 |S 21 | (dB) -30 -40 -50 -60 Simulation Measurement -70 -80 30 35 40 45 50 55 Frequency (GHz) Fig. 16 Results of simulation and measurement of the mutual coupling coefficient, ||S21 ||, of the two-element side-by-side MIMO antenna 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 30 409 0 30 0 dB 30 0 dB -5 -5 60 60 60 60 -10 -10 -15 90 -15 -20 90 =0o =90 o 120 30 150 120 -20 90 90 =0o 120 120 =90 o 150 150 150 180 180 (a) (b) Fig. 17 Total field radiation patterns of the two-element side-by-side MIMO antenna at 37.8GHz when fed at (a) port 1 and (b) port 2 0 0 30 30 30 0 dB -5 60 60 60 -10 -10 -15 -15 90 -20 =0o 120 =90 150 30 -5 60 90 0 dB 120 -20 90 90 =0o 120 120 =90 o o 150 150 150 180 180 (a) (b) Fig. 18 Total field radiation patterns of the two-element side-by-side MIMO antenna at 50GHz when fed at (a) port 1 and (b) port 2 13 410 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 0 0 dB 30 30 0 dB 30 -5 -5 60 60 60 60 -10 -10 90 90 -15 90 -15 EL 120 120 EL 150 90 ER ER 120 30 150 150 120 150 180 180 (a) (b) Fig. 19 Radiation patterns of the CP field components ( ER and EL ) of the two-element side-by-side MIMO antenna (port 1) at 37.8 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 0 30 0 0 dB 30 30 -5 60 60 -10 90 -10 -15 90 ER 120 120 EL 150 30 -5 60 60 0 dB 90 -15 90 ER 120 120 EL 150 150 150 180 180 (a) (b) Fig. 20 Radiation patterns of the CP field components ( ER and EL ) of the two-element side-by-side MIMO antenna (port 1) at 50 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 5.2 Performance Evaluation of the Two‑Element MIMO Antennas The purpose of the next two subsections is to investigate the performance of the two-element MIMO configurations proposed in Section 3.1 regarding the impedance matching at each port, radiation patterns, coupling coefficient between the two ports, ECC, and DG. 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 411 0 0 0 dB 30 30 0 dB 30 -5 60 -5 60 60 60 -10 90 -10 -15 90 ER 120 120 EL 150 30 90 -15 ER 120 150 90 120 EL 150 150 180 180 (a) (b) Fig. 21 Radiation patterns of the CP field components ( ER and EL ) of the two-element side-by-side MIMO antenna (port 2) at 37.8 GHz. a 𝜙 = 0◦ b. 𝜙 = 90◦ 0 0 0 dB 30 30 30 -5 60 60 -10 90 -10 -15 90 ER 120 120 90 -15 150 90 ER 120 120 EL EL 150 30 -5 60 60 0 dB 150 150 180 180 (a) (b) Fig. 22 Radiation patterns of the CP field components ( ER and EL ) of the two-element side-by-side MIMO antenna (port 2) at 50 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 5.2.1 Two‑Element Side‑by‑Side MIMO Antenna In this section, the performance of a MIMO antenna system composed of two elements of the antenna described in Section 2 is investigated by simulation as well as experimental measurement. The two elements are placed side-by-side, as presented in Figs. 2 and 5b, to produce spatial diversity. The frequency dependence of the reflection coefficient at port 1 is presented in Fig. 15. By comparison between Figs. 15 and 11, it is shown that the frequency response of ||S11 || of 13 412 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 |S 11 | (dB) -10 -20 -30 Simulation Measurement -40 30 35 40 45 50 55 Frequency (GHz) Fig. 23 Results of simulation and measurement of ||S11 || at port 1 of the two-element face-to-face MIMO antenna over a broad frequency band the two-element MIMO antenna is almost identical to that of the single-element antenna. The isolation between the two elements of this MIMO antenna can be measured by the magnitude of the coupling coefficient, ||S21 ||, whose frequency response is shown in Fig. 16. The magnitude of this coefficient is maintained below − 24 dB over the entire frequency range of investigation showing good performance of the proposed side-by-side MIMO antenna. Also, it is shown that the simulation -10 |S 21 | (dB) -20 -30 -40 -50 Simulation Measurement -60 -70 30 35 40 45 50 55 Frequency (GHz) Fig. 24 Results of simulation and measurement of the mutual coupling coefficient, ||S21 ||, of the two-element face-to-face MIMO antenna 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 30 0 0 dB 30 30 0 0 dB 60 60 60 -10 -10 -15 -15 90 -20 90 -20 =90 120 o 150 90 =0o =90 o =0o 120 30 -5 -5 60 90 413 120 150 150 120 150 180 180 (a) (b) Fig. 25 Radiation patterns of the total field radiated by the two-element face-to-face MIMO antenna at 37.8GHz when it is fed using (a) port 1 and (b) port 2 results and experimental measurements of ||S11 || and ||S21 || show good agreement with each other. The radiation patterns of the two-element side-by-side MIMO antenna at 37.8 GHz when excited at ports 1 and 2 are presented in Fig. 17a and b, respectively. The far-field patterns produced at 50 GHz when this MIMO antenna is fed at ports 1 and 2 are presented in Fig. 18a and b, respectively. Irrespective of the port of excitation of this MIMO antenna, the values of the maximum gain achieved at 37.8 and 50 GHz are 7 and 6.8 dBi, respectively. 30 0 0 dB 30 30 -5 60 60 60 -10 -10 -15 -15 -20 90 =0o =90 o 120 150 30 -5 60 90 0 0 dB 120 150 -20 90 90 =0o =90 o 120 150 120 150 180 180 (a) (b) Fig. 26 Radiation patterns of the total field radiated by the two-element face-to-face antenna at 50GHz when it is fed using (a) port 1 and (b) port 2 13 414 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 0 0 dB 30 30 0 dB 30 -5 -5 60 60 60 60 -10 90 -10 -15 90 ER 120 120 90 -15 90 ER 120 120 EL EL 150 30 150 150 150 180 180 (a) (b) Fig. 27 Radiation patterns of the CP field components ( ER and EL ) of the two-element face-to-face MIMO antenna (port 1) at 37.8 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 0 30 0 0 dB 30 30 -5 60 60 -10 90 -10 -15 90 ER 120 120 90 90 -15 ER 120 120 EL EL 150 30 -5 60 60 0 dB 150 150 150 180 180 (a) (b) Fig. 28 Radiation patterns of the CP field components ( ER and EL ) of the two-element face-to-face MIMO antenna (port 1) at 50 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ When the side-by-side MIMO antenna is fed using port 1, the patterns of the CP field components at 37.8 and 50 GHz are presented in Figs. 19 and 20, respectively. When the same MIMO antenna is fed using port 2, the CP field patterns at 37.8 and 50 GHz are presented in Figs. 21 and 22, respectively. It is seen that the radiated field is dominated by RHCP component at both the lower and higher frequencies. However, the cross-polarization level of the radiated field at 50GHz is significantly higher than that of the radiated field at 37.8GHz . 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 0 0 dB 30 415 30 0 dB 30 -5 -5 60 60 60 60 -10 -10 90 -15 90 90 -15 120 120 EL 150 90 ER ER 120 30 150 150 120 EL 150 180 180 (a) (b) Fig. 29 Radiation patterns of the CP field components ( ER and EL ) of the two-element face-to-face MIMO antenna (port 2) at 37.8 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 0 30 0 0 dB 30 30 -5 60 60 60 -10 -10 -15 90 ER 120 120 90 -15 90 ER 120 EL 150 30 -5 60 90 0 dB 120 EL 150 150 150 180 180 (a) (b) Fig. 30 Radiation patterns of the CP field components ( ER and EL ) of the two-element face-to-face MIMO antenna (port 1) at 50 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ This means that the proposed two-element side-by-side MIMO antenna produces more perfect circular polarization at 37.8 GHz that that produced at 50 GHz. This MIMO antenna produces the same type of polarization when fed using port 1 or port 2. Therefore, it can be employed to obtain spatial diversity but not polarization diversity. 13 416 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 Fig. 31 Dependence of the ECC of the two-element MIMO antenna on the frequency around (a) 37.8 GHz and (b) 50 GHz Fig. 32 Dependence of the DG of the two-element MIMO antenna on the frequency around (a) 37.8 GHz and (b) 50 GHz 5.2.2 Two‑Element Face‑to‑Face MIMO Antenna The MIMO antenna system performance, which is composed of two elements of the CP antenna described in Section 2, is investigated by simulation as well as experimental measurement. The two elements are placed face-to-face, as presented in Figs. 3 and 5c, to produce spatial diversity. The frequency dependence of the reflection coefficient at port 1 is presented in Fig. 23. By comparison between Figs. 23 and 11, it is shown that the frequency response of ||S11 || of the two-element MIMO antenna is almost identical to that of the single-element antenna. Also, it is shown that the experimental measurements of ||S11 || come in good agreement with simulation results. 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 417 0 |S 11 | (dB) -10 -20 -30 Simulation Measurement -40 30 35 40 45 50 55 60 Frequency (GHz) Fig. 33 Variation of ||S11 ||, at port 1 of the four-element MIMO configuration with the frequency over a broad frequency band Fig. 34 Variation of the mutual coupling coefficients, ||S21 ||, ||S31 ||, and ||S41 ||, of the four-element MIMO antenna with the frequency The isolation between the two elements of this MIMO antenna can be measured by the magnitude of the coupling coefficient, ||S21 ||, whose frequency response is presented in Fig. 24. The magnitude of the coupling coefficient is maintained below − 20 dB over the entire frequency range of investigation showing good performance of the face-to-face MIMO antenna system. As seen, the measurements of ||S21 || are close to the results obtained by simulation. The total field radiation patterns of the face-to-face MIMO antenna at 37.8 GHz when fed at ports 1 and 2 are presented in Fig. 25a and b, respectively. The far-field patterns produced at 50 GHz when it is fed at ports 1 and 2 are presented in Fig. 26a and b, respectively. Irrespective of the port of excitation of this MIMO antenna, the values of the peak gain achieved at 37.8 and 50 GHz are 7.6 and 6.55 dBi, respectively. 13 418 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 -20 -30 |S 21 | (dB) -40 -50 -60 -70 Simulation Measurement -80 -90 30 35 40 45 50 55 Frequency (GHz) Fig. 35 Variation of the coupling coefficient, ||S21 ||, between ports 1 and 2 of the four-element MIMO antenna 0 0 30 0 dB 30 30 0 dB -5 -5 60 60 60 60 -10 -10 -15 -15 90 -20 120 90 120 =0o 90 -20 120 90 120 =0o =90 o 150 30 =90 o 150 150 150 180 180 (a) (b) Fig. 36 Radiation patterns of the total field radiated by the four-element MIMO antenna (port 1) at (a) 37.8GHz and (b) 50 GHz The patterns of the circularly polarized field components produced by the faceto-face MIMO antenna in the far zone at 37.8 and 50 GHz, are shown in Figs. 27 and 28, respectively, when the MIMO antenna is excited at port 1, and Figs. 29 and 30, respectively, when fed at port 2. It is seen that the far field is mainly RHCP at both the lower and higher frequencies. However, the cross-polarization level of the radiated field at the upper band of frequencies is significantly higher 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 419 0 0 0 dB 30 0 dB 30 30 -5 -5 60 60 60 60 -10 -10 -15 90 -15 -20 120 30 90 120 =0o =90 90 -20 120 150 =90 150 120 =0o o 150 o 150 180 180 (a) (b) Fig. 37 Radiation patterns of the total field radiated by the four-element MIMO antenna (port 2) at (a) 37.8GHz and (b) 50 GHz 0 30 0 0 dB 30 30 0 dB -5 60 60 60 60 -10 -10 -15 90 -15 -20 120 90 120 =0o =90 150 30 -5 90 -20 120 120 =0o o =90 150 90 150 o 150 180 180 (a) (b) Fig. 38 Radiation patterns of the total field radiated by the four-element MIMO antenna (port 3) at (a) 37.8GHz and (b) 50 GHz than that of the far field at the lower band of frequencies. This means that the proposed two-element face-to-face MIMO antenna produces more perfect circular polarization at 37.8 GHz that that produced at 50 GHz. This MIMO antenna produces the same type of polarization when fed at port 1 or port 2. Therefore, it can be employed to obtain spatial diversity but not polarization diversity. 13 420 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 0 0 dB 30 0 dB 30 30 -5 -5 60 60 60 60 -10 -10 -15 -15 90 -20 120 90 120 =0o =90 30 90 -20 120 120 =0o =90 o o 150 90 150 150 150 180 180 (a) (b) Fig. 39 Radiation patterns of the total field radiated by the four-element MIMO antenna (port 4) at (a) 37.8GHz and (b) 50 GHz 0 30 0 0 dB 30 30 -5 60 60 60 -10 -10 -15 90 ER 120 120 EL 150 30 -5 60 90 0 dB 90 -15 90 ER 120 120 EL 150 150 150 180 180 (a) (b) Fig. 40 Radiation patterns of the CP field components ( ER and EL ) of the four-element MIMO antenna (port 1) at 37.8 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 5.2.3 ECC and DG of the Two‑Element MIMO Antennas The ECC and DG obtained by the side-by-side and face-to-face MIMO antenna configurations are presented in Figs. 31 and 32, respectively, over the operating frequency bands. It is seen that the ECC is very small (< 10−3) and the DG is almost 10 over both the frequency bands indicating excellent diversity properties. 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 0 0 dB 30 60 60 60 -10 -10 -15 90 ER 120 90 90 -15 ER 120 120 EL EL 150 30 -5 -5 120 0 dB 30 30 60 90 421 150 150 150 180 180 (a) (b) Fig. 41 Radiation patterns of the CP field components ( ER and EL ) of the four-element MIMO antenna (port 1) at 50 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 0 0 30 0 dB 30 30 60 60 60 -10 -10 -15 90 ER 120 120 -15 90 90 ER 120 EL 150 30 -5 -5 60 90 0 dB 120 EL 150 150 150 180 180 (a) (b) Fig. 42 Radiation patterns of the CP field components ( ER and EL ) of the four-element MIMO antenna (port 2) at 37.8 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 5.3 Performance Assessment of the Four‑Element MIMO Antenna The four-element MIMO antenna system presented in Fig. 4 is designed to obtain both spatial and polarization diversity. Elements 1 and 4 produce RHCP radiation, whereas elements 2 and 3 produce LHCP radiation. 13 422 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 0 0 dB 30 60 60 60 -10 -10 -15 90 ER 120 120 90 -15 90 ER 120 150 150 120 EL EL 150 30 -5 -5 60 90 0 dB 30 30 150 180 180 (a) (b) Fig. 43 Radiation patterns of the CP field components ( ER and EL ) of the four-element MIMO antenna (port 2) at 50 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 0 0 30 0 dB 30 30 60 60 60 -10 -10 90 -15 ER 120 120 90 -15 150 90 ER 120 120 EL EL 150 30 -5 -5 60 90 0 dB 150 150 180 180 (a) (b) Fig. 44 Radiation patterns of the CP field components ( ER and EL ) of the four-element MIMO antenna (port 3) at 37.8 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 5.3.1 Mutual Effects between the Elements of the Four‑Element MIMO Antenna The frequency response of ||S11 || is presented in Fig. 33. The mutual S-parameters of this MIMO antenna are presented in Figs. 34 and 35. By comparing the frequency response of ||S11 || of the four-element MIMO antenna presented in Fig. 42 to that of the single-element antenna presented in Fig. 11, it is seen that they are 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 0 0 dB 30 423 30 0 dB 30 -5 60 -5 60 60 60 -10 90 -10 90 -15 ER 120 120 90 90 -15 ER 120 120 EL EL 150 30 150 150 150 180 180 (a) (b) Fig. 45 Radiation patterns of the CP field components ( ER and EL ) of the four-element MIMO antenna (port 3) at 50 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 0 30 0 0 dB 30 30 -5 60 60 60 -10 -10 90 -15 ER 120 120 EL 150 30 -5 60 90 0 dB 90 -15 90 ER 120 120 EL 150 150 150 180 180 (a) (b) Fig. 46 Radiation patterns of the CP field components ( ER and EL ) of the four-element MIMO antenna (port 4) at 37.8 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ almost identical. This indicates that the mutual coupling between the elements of the MIMO antenna is very weak, which is emphasized by the frequency responses of the mutual S-parameters presented in Figs. 43 and 44. It is shown that the magnitudes of the mutual S-parameters among the various ports are below −24dB; such low values of the mutual coupling show good isolation between the elements and, hence, excellent diversity is provided by this MIMO antenna. 13 424 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 0 0 0 dB 30 0 dB 30 30 -5 -5 60 60 60 60 -10 -10 90 -15 90 ER 120 90 ER 120 120 90 -15 120 EL EL 150 30 150 150 150 180 180 (a) (b) Fig. 47 Radiation patterns of the CP field components ( ER and EL ) of the four-element MIMO antenna (port 4) at 50 GHz. a 𝜙 = 0◦. b 𝜙 = 90◦ 1 10-3 1 Port 1&2 Port 1&3 Port 1&4 0.6 0.4 0.2 0 36.5 Port 1&2 Port 1&3 Port 1&4 0.8 ECC (dB) ECC (dB) 0.8 10-3 0.6 0.4 0.2 37 37.5 Frequency (GHz) 38 38.5 0 49.5 50 50.5 Frequency (GHz) (a) (b) Fig. 48 Variation of the ECC of the four-element MIMO antenna with the frequency around (a) 37.8 GHz and (b) 50 GHz 5.3.2 Radiation Patterns of the Four‑Element MIMO Antenna The radiation patterns of the total field produced by the four-element MIMO antenna when excited at ports 1, 2, 3, and 4 are presented in Figs. 36, 37, 38, and 39, respectively, at the lower and higher operational frequencies of the proposed MIMO antenna. The radiation patterns of the CP field components radiated by the four-element MIMO antenna when fed at port 1 at the two operating frequencies 37.8 and 50 GHz are presented in Figs. 40 and 41, respectively. The radiation patterns obtained when the antenna is fed at port 2 at the same frequencies are shown in Figs. 42 and 43. Also, the radiation patterns at both frequencies are calculated 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 10 425 10 9.999 9.995 DG (dB) DG (dB) 9.998 9.997 9.996 9.99 9.995 Port 1&2 Port 1&3 Port 1&4 9.994 9.993 36.5 37 37.5 Frequency (GHz) (a) 38 Port 1&2 Port 1&3 Port 1&4 38.5 9.985 49.5 50 50.5 Frequency (GHz) (b) Fig. 49 Variation of the DG of the four-element MIMO antenna with the frequency around (a) 37.8 GHz and (b) 50 GHz Fig. 50 Surface current distribution over the patches of the face-to-face MIMO antenna system at (a) 28 GHz and (b) 38 GHz when the antenna is fed through port 3 and port 4 as illustrated in Figs. 44 and 45, and, Figs. 46 and 47, respectively. It is shown that when port 1 or 4 is used to feed the MIMO antenna, the far field is dominated by RHCP component. On the other side, the far field is dominated by LHCP component when port 2 or 3 is used for feeding the MIMO antenna. It is shown that the cross-polarization level at the higher frequency band is significantly higher than that obtained at the lower frequency band. This means that the four-element MIMO antenna 13 426 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 Fig. 51 Surface current distribution over patch 1 of the face-to-face MIMO antenna system at (a) 28 GHz and (b) 38 GHz Fig. 52 Surface current distribution over the patches of the side-by-side MIMO antenna system at (a) 28 GHz and (b) 38 GHz Fig. 53 Surface current distribution over patch 1 of the side-by-side MIMO antenna system at (a) 28 GHz and (b) 38 GHz 13 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 427 Fig. 54 Surface current distribution over the patches of the four-port MIMO antenna system at (a) 28 GHz and (b) 38 GHz Fig. 55 Surface current distribution over patch 1 of the four-port MIMO antenna system at (a) 28 GHz and (b) 38 GHz produces more perfect circular polarization at 37.8 GHz than that produced at 50 GHz. Nevertheless, this MIMO antenna provides polarization diversity in addition to the spatial diversity, where the latter type of diversity is produced owing to the distance between the elements having the same sense of polarization. 5.3.3 ECC and DG of the Four‑Element MIMO Antenna The frequency responses of the ECC and DG of the four-element MIMO antenna are presented in Figs. 48 and 49, respectively, over the operating frequency bands. It is seen that the ECC is very small (< 10−3) and the DG is almost 10 over both the frequency bands indicating excellent diversity properties. 13 428 13 Table 2 Comparisons among the perfromance measures of the proposed MIMO antennas and those of other MIMO antennas in previously published papers Ref Freq. (GHz) S11 BW (GHz) Peak G (dBi) ARBW (dB) Isolation S21 (dB) ECC (dB) [9] 28 10 7.3 2.4 < −31 < 0.5 [10] 28 0.5 7.3 – − 25 ≈0 45 1.8 7.03 No. of elements Patch dimensions (mm2) ≈ 10 4 3×3 > 9.99 2 4 4×5 4 4.9 × 5.8 51 0.8 7.2 56 1 8.03 28 0.6 7.38 – − 30 ≈0 ≈ 10 38 0.6 8.13 – -40 ≈0 ≈ 10 [22] 28 0.4 6.9 – − 20 0.1 9.9 2 3.15 × 3.15 [23] 28 5 9.5 – < −40 < 0.01 > 9.9 4 13 × 15 38 2.1 11.5 – < −40 < 0.01 > 9.9 [24] 28 3.52 7.1 – − 32 ≈0 ≈ 10 4 10 × 10 [25] 28 2.4 8.4 – > −25 ≈0 ≈ 10 4 4.23 × 2.94 38 2 6.02 – > −25 ≈0 ≈ 10 37.8 1.499 7.01 0.708 − 29 4 × 10−7 2 side-by-side 2.9 × 2.9 50 1.855 7.83 0.113 − 41.2 8 × 10 37.8 1.47 7.61 0.776 − 30 5 × 10−8 50 1.86 6.58 0.168 − 29.2 2 × 10−5 37.8 1.474 7.83 0.708 − 29 2 ×10−7 50 1.854 7.9 0.129 − 44 −6 Present work 8 ×10 > 9.99 −6 2 face-to-face 4 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 [21] DG (dB) Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 429 5.4 Surface Current Distribution The surface current distribution over each patch surface has been calculated for all the proposed MIMO configurations. In Fig. 50, the surface current over the face-to-face MIMO antenna system is graphed when port 1 is excited showing very weak coupling between the two antennas. The direction of the current on patch 1 is calculated and plotted in Fig. 51 at both operating bands 28 and 38 GHz. It is clear from Fig. 51 that the antenna exhibits a first-order mode at 28 GHz and second-order mode at 38 GHz. For the side-by-side MIMO system configuration, the surface current distribution over the elements of the MIMO antennas is shown in Fig. 52 over the two bands 28 and 38 GHz showing very weak coupling at both frequency bands when port 1 is excited. The direction of the surface current is plotted in Fig. 53 on patch 1 at 28 and 38 GHz. By noticing the current distribution on the main patch, it can be seen that a single-order mode is obvious at 28 GHz and second-order mode is shown at 38 GHz. Finally, the surface current distribution is calculated for the four port MIMO antenna system and demonstrated in Fig. 54 when port 1 is excited, showing low coupling between elements. The surface current distribution on patch 1 is illustrated in Fig. 55 using arrows to show current direction. 6 Comparison with Previous Work Comparisons between the performance of the proposed MIMO antennas and that of other MIMO antennas presented in recently published papers are listed in Table 2. These comparisons show some advantages of the proposed MIMO antennas relative to those presented in the other publications. The main advantage of the proposed MIMO antennas is that they provide two bands of circular polarization. Another important advantage over the other published papers is that the proposed four-element MIMO antenna provides two types of diversity (spatial and polarization), whereas the other antennas offer only spatial diversity. The other advantages are the smaller size and high isolation among the multiple ports. However, the main drawback of the proposed MIMO antennas relative to other published designs is the narrow bandwidth. Nevertheless, the two frequency bands achieved by the proposed MIMO antennas can be considered wide enough for operation in applications of future wireless communication. 7 Conclusion A novel CP low-profile printed antenna has been designed to produce circular polarization over two frequency bands around 37.8 and 50GHz. Two-element side-by-side and face-to-face MIMO antenna configurations have been proposed to attain spatial diversity. A four-element MIMO antenna has been proposed to achieve both spatial and polarization diversity at the same time. The proposed dual-band CP single-element, two-element MIMO, and four-element MIMO antennas have been fabricated 13 430 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 for experimental study. Both the numerical and experimental investigations have shown that the mutual coupling between any two ports of the proposed MIMO antennas is below −25dB. Also, for any two ports it has been shown that the ECC is below 1 × 10−7 and the diversity gain is higher than 9.99. The impedance matching bandwidths (for ||S11 || < −10dB) have been shown to be 1.53 and 1.88 GHz at 37.8 and 50GHz, respectively, and the corresponding 3-dB axial ratio bandwidths have been shown to be 700 and 130MHz, respectively. Author Contributions Nada, Rania Performed Simulations Walid, khalid design idea Asmaa performed fabrication and measurements. Funding Open access funding provided by The Science, Technology & Innovation Funding Authority (STDF) in cooperation with The Egyptian Knowledge Bank (EKB). Data Availability Data sharing not applicable to this article as no datasets were generated or analyzed during the current study. Declarations Competing Interests The authors declare no competing interests. Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/ licenses/by/4.0/. References 1. A. K. Dwivedi, A. Sharma, A. K. Singh, and V. Singh. 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Design and characterization of compact broadband antenna and its MIMO configuration for 28 GHz 5G applications. Electronics, vol. 11, Art. No. 523, 2022. 25. A. D. Tadesse, O.P. Acharya, and S. Sahu. A compact planar four-port MIMO antenna for 28/38 GHz millimeter-wave 5G applications. Advanced Electromagnetics, Vol.11, No.3, pp.16–25, 2022. Publisher’s Note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations. 13 432 Journal of Infrared, Millimeter, and Terahertz Waves (2024) 45:393–432 Authors and Affiliations Nada Alaa1 · Rania A. Elsayed1 · Asmaa E. Farahat2 · Khalid F. A. Hussein2 · Walid S. El‑Deeb1 * Asmaa E. Farahat e_asma_e@yahoo.com Nada Alaa engnadaalaa@gmail.com Rania A. Elsayed en_rania_helika@yahoo.com Khalid F. A. Hussein fkhalid@eri.sci.eg Walid S. El-Deeb wseldeeb@ucalgary.ca 1 Electronics and Communications Engineering Department, Faculty of Engineering, Zagazig University, Zagazig, Egypt 2 Microwave Engineering Department, Electronics Research Institute, Cairo 11843, Egypt 13