A Novel “回” Pane Structure Multiband Microstrip Antenna for 2G/3G/4G/5G/WLAN/Navigation Applications

)is work proposes a novel multiband slotted planar antenna with a “回” structure, which is similar to an ancient Chinese window grille structure. )e antenna is suitable for wireless applications, including the second-generation (2G), third-generation (3G), fourth-generation (4G), and fifth-generation (5G) technologies, as well as WLAN and navigation applications. )e proposed antenna is based on the structural characteristics of a conventional monopole antenna, which combines the advantages of a slit structure andmicrostrip line structure for feeding. It adopts a circular patch with a slit structure placed in it, which is similar to the Chinese classical pane structure. )is structure enables an effective reduction of the size of the antenna. )e four-sided “回” gaps change the path of current flow and are coupled to each other, improving the impedance matching and radiation characteristics of the entire target frequency band. )e antenna covers the frequency ranges of 1.58–1.77GHz (12%), 2.1–2.50GHz (17%), 3.61–4.09GHz (12%), and 4.75–6.5GHz (36%), permitting more than 10 wireless applications in these 4 frequency bands. )is antenna uses an FR-4 dielectric material; the relative dielectric constant of the dielectric plate is 4.4, and the actual dimensions of the antenna are 85× 70×1.6mm3.)e test and simulation results are in good agreement with each other, thus confirming that the proposed design method meets the requirements of various wireless applications.


Introduction
With wireless applications becoming increasingly more popular, the requirements for antenna miniaturisation, multiple frequency bands, and ease of loading have grown considerably. In order to achieve multiple frequency bands, antennas are commonly designed with multiple feed points, and a U-shaped reflector is included at the bottom to expand the frequency band [1]. Antennas can also be designed for multiple iterations to improve their performance. For example, the square and circle antenna designs similar to ancient Chinese coins have been shown to exhibit good performance after a five-layer iteration [2]. Multiband and broadband characteristics of antennas can be achieved through the use of coupling and feed-matching circuits [3]. At present, many multiband antennas have been proposed [4,5]. Additionally, different feeding methods have been utilised: although the microstrip line feeding performs well in terms of losses, the resulting frequency band is narrow [6][7][8]. Coplanar waveguide (CPW) designs also have some advantages and disadvantages [9,10]. erefore, it is necessary to eliminate the shortage of microstrip feed. Many methods have also been used to design multiband antennas, such as fractal-structure antennas, geometric shapes, Koch snowflakes, and Hilbert curves. Fractal antennas have been mainly designed following two different methods, namely, self-similarity [11,12] and space filling [13,14]. Self-similarity in fractal antennas permits the achievement of similar surface current distributions in different planes as well as multifrequency characteristics; space filling enables the increase of the antenna electrical length [15,16]. Furthermore, it has been shown that the frequency band of antennas can be increased by adding branches and slits [17,18]. In order to reduce the size of antennas, it is important to note that the size of the dielectric resonant antenna (DRA) is proportional to the parameter λ/ε 1/2 r . Increasing the relative dielectric constant of the antenna medium can thus effectively reduce the antenna size [19]. In terms of improving impedance matching and radiation characteristics, a loading slot can be used to couple the same stub to the radiating element, and the stub is coupled to the local ground [20]. It is also possible to load a double T-shaped structure inside the elliptical ring structure to improve the −10 dB impedance bandwidth of the antenna without affecting the compactness of the antenna [21].
However, the frequency bands of traditional monopole antennas and dipole antennas are often narrow and cannot meet the requirements due to antenna resonance. erefore, in order to design a miniaturised, low-profile multiband planar antenna that can be used for mobile terminals, it is necessary to combine patch slotting or fractal geometry with traditional antennas. e comparison between this article and previous studies is shown in Table 1.
is work proposes a multiband planar antenna with a circular monopole patch as the main radiator and a slotted design in the patch. Its shape is similar to that of a Chinese classical "回" pattern pane.  Table 1, the size and performance of the antennas in this work are compared with those mentioned in the references.

Characteristics of the Antenna Structure.
e length and width of the radiator are calculated according to well-known mathematical equations: where L is the length of the antenna radiator, f is the centre frequency of the antenna during operation, c is the speed of light in free space (3 × 10 8 m/s), and ε r is the dielectric constant of the dielectric plate. e structure and parameters of the microstrip feeder planar antenna are shown in Figure 1, and the size is shown in Table 2. e antenna is connected to a 50 Ω microstrip feeder on a circular patch with slits, with a ground layer on the back, and its pattern is similar to the ancient Chinese "回" pattern pane, as shown in Figure 2. In the traditional Chinese culture, window panes were often carved in phoebe, decorated on doors, windows, and partitions, and carved with different patterns to increase the lighting surface of the room and increase the space transparency. e "回" pattern was originally derived from the thunder pattern on ancient pottery and bronze. In China, lines are flexible, and intermittent sorting implies endless life, auspiciousness, and peace. is pattern can be used to increase the length of the radiator in order to extend the electrical length and radiation efficiency of the antenna. e antenna was designed on an FR-4 substrate with a thickness of 1.6 mm, a dielectric constant of 4.4, and a loss tangent of 0.02.
As shown in Figure 3, the "回" structure was engraved inside the antenna. e principle of this structure is also derived from the traditional monopole antenna. erefore, the length of the low-radiation patch can be calculated as (2) At high frequencies, current flows through all the gaps. And it resonates with the surrounding gaps. e current flows through about one-third of L 4 . From the data given in Table 2, (3)

Simulation Results.
e simulation was performed using Ansoft High-Frequency Simulation Software (HFSS) (version 18.0). Figure 4(a) illustrates a monopole antenna with a cross-slit inside a circular patch. e slit size is fixed, resulting in four resonance frequency bands, namely, 1.5, 1.9, 2.4, and 4 GHz. From Figure 4(b), it can be seen that the first-order slits are placed along the four directions of the circular patch, resulting in four frequency bands, i.e., 1.90-2.68 GHz, 3.50-4.11 GHz, 4.32-4.65 GHz, and 5.48-6.17 GHz. e isolation of the two central frequency bands is low, and the return loss performance of the highfrequency band is poor. Figure 4(c) shows a second-order slit on the basis of Figure 4(b) so that the antenna resonance frequency band tends to stabilise at 1.7, 2.4, 3.8, and 4.95 GHz. Figure 4(d) displays a change in the three parameters L 1 , L 2 , and W. e above four parameters were optimised and analysed in order to obtain an antenna return loss performance suitable for the applicable ranges of GPS, WLAN, 5G, and other commercial frequency bands. When the antenna was derivatized, the change of the antenna frequency band is shown in Table 3.
As shown in Figure 5, the length of L 4 is swept from 4.4 mm to 8.2 mm. Under different lengths, it is found that S11 does not change significantly in the high-frequency band. When the length of L 4 changes, the frequency band shifts from 1.2 to 1.8 GHz. After comparison, L 4 � 5 mm is the best frequency band. As shown in Figure 6, there is no obvious change in the low-frequency range when L 7 is at 5.2-6.8 mm. When the frequency band is 5-6.5 GHz, L 7 � 6 mm achieves the best performance.
As shown in Figure 7, the length of H was swept from 10 mm to 85 mm to change the size of the background plane. When H � 10 mm, the return loss performance in the lowfrequency band is poor and cannot meet the requirements of the commercial frequency band. Gradually increase the length H of the ground plate. When H � 55 mm, there are multiple frequency bands at low frequency, but the isolation between the frequency bands is poor, which is easy to cause mutual interference between the frequency bands. e maximum size of the grounding plate is H � 85 mm, and the return loss obtained is not appropriate. erefore, the most suitable size of H � 20 mm is used to design the grounding plate.   Figure 1: Layout of the proposed antenna.
International Journal of Antennas and Propagation 3   Table 4). e surface current amplitude diagram and current vector distribution diagram of the antenna radiator at the centre frequencies of 1.6, 2.35, 3.8, and 5.85 GHz are shown in Figures 9(a)-9(d). For the frequency band with a centre frequency of 1.6 GHz, the left and right slots of the monopole exhibit larger currents (see Figure 9(a)). As the frequency increases, the current is more concentrated on the gaps in the four directions. For the frequency band with a centre frequency of 5.85 GHz, the current reaches a relative maximum value on the four slits of the radiator (see Figure 9(d)). e 3D gain pattern and E/H-plane radiation pattern of the antenna at the centre frequencies of 1.6, 2.35, 3.8, and 5.85 GHz are shown in Figures 10 and 11. e display gains are 3, 3.74, 5, and 4.99 dBi, respectively. It can be seen that the E-plane and H-plane are omnidirectional in the low-frequency bands of 1.6 and 2.35 GHz, whereas the other two frequency bands are almost omnidirectional. Sidelobes are generated at the centre frequencies of 3.8 and 5.85 GHz, and the degree of cross-polarisation is low.   e measured and simulated antennas are in the −10 dB return loss frequency band, as shown in Figure 13. e bandwidth of the −10 dB return loss covers roughly the same frequency band as the simulation, as shown in Table 3. e measured and simulated results obtained for          e manufactured antenna exhibits good radiation characteristics in all frequency bands and is omnidirectional on the H-plane. However, some differences between the experimental and simulated data can also be observed in this case and can be due to several reasons.

Fabrication and Measurement Results
As shown in Figure 16, the actual gain and radiation efficiency of the antenna were measured in an anechoic chamber. e background of the available frequency bands in the picture is light blue. e actual gain in the 1.58-1.77 GHz frequency band is 0.5-2 dBi and the radiation efficiency is 45-65%, the actual gain in the 2.1-2.50 GHz frequency band is 2-3.6 dBi and the radiation efficiency is 55-75%, the actual gain in the 3.61-4.09 GHz frequency band is 3.8-4.1 dBi and the radiation efficiency is 62-81%, and the actual gain in the 4.75-6.5 GHz frequency band is 3-5.9 dBi and the radiation efficiency is 58-72%. e actual efficiency of the antenna is between 10% and 70% in the lowfrequency range, whereas the actual efficiency in the highfrequency range exceeds 69%. e efficiency and gain meet the requirements within the available range, and the frequency band coverage is not affected in other places. e presence of a stop band at 1.9 GHz leads to an efficiency of 10%, which can better improve the isolation of the antenna frequency band.

Conclusions
In this study, a small multiband planar antenna with classical "回" pattern panes was developed for application in the commercial frequency bands, such as GPS, DCS, Bluetooth, WLAN, LTE Band40, WiMAX, SCDMA, 5G, and LTE42/43. e frequency band and bandwidth were found to be 1.58-1.77 GHz (12%), 2.1-2.50 GHz (17%), 3.61-4.09 GHz (12%), and 4.75-6.5 GHz (36%). e radiation direction of the antenna was found to be omnidirectional, and the antenna simulation and performance test confirmed the good performance of the antenna. Overall, it was found that the proposed antenna exhibits good radiation characteristics, is small and light, and is thus suitable for most wireless applications.

Data Availability
e data used to support the findings of this study are included within the article.

Conflicts of Interest
e authors declare that they have no conflicts of interest. 14 International Journal of Antennas and Propagation