Compact Vitis vinifera-Inspired Ultrawideband Antenna for High-Speed Communications

A new compact ultrawideband (UWB) bioinspired antenna is presented in this work. 'e proposed antenna consists of a vine leaf (Vitis vinifera) shape as the radiating patch, defected ground structure (DGS), and a vertical rectangular slot (VRS) on the ground plane. 'e vine leaf shape is realized from a circular patch (initiator) in this work. 'e proposed antenna is built on an FR4 substrate with a dielectric constant of 4.4, a loss tangent of 0.02, and a thickness of 1.5mm. 'e total dimension of the proposed bioinspired antenna is 35× 27.6mm. 'e proposed antenna has a fractional bandwidth of 115.43% (3.7GHz–13.8GHz) at 10 dB return loss, a radiation efficiency between 78% and 97%, a peak gain of 6.7 dB, and a stable radiation pattern. 'e contributions of this work to the existing literature are as follows: (i) the investigation of a vine leaf shape for UWB antenna application; (ii) the adaptation of the conventional monopole patch antenna design equation to determine the lower edge frequency (LEF) of an arbitrary shape monopole antenna; (iii) the presentation of a compact UWB antenna with high fractional bandwidth compared with recent works in the literature, and (iv) the use of FR4 substrate to achieve a peak radiation efficiency of 97% with a compact structure.


Introduction
Ultrawideband antenna has attracted the attention of microwave engineers since the declaration of the Federal Communication Commission (FCC) to make it available for commercial use. is antenna readily finds application in radar, military, medical, and mobile communication. According to the FCC, the band designation for UWB is 3.1 GHz-10.6 GHz [1]. Even though this band interferes with other existing standards such as Wi-Fi, WLAN, WiMAX, and the upper ISM band, its advantages such as low power, reasonably cheaper cost of equipment, and its greater noise immunity have made it to become popular in wireless communication systems, especially in short distance communication [2,3].
Over the years, researchers have been working on how to realize a compact antenna having an ultrawide bandwidth. e printed monopole antenna is one of the major techniques being used to achieve such a wide fractional bandwidth. Some of the patch shapes commonly used in the literature are rectangular, triangular, and circular. In recent times, antenna researchers begun to look in the direction of bioinspired structure such as leave shape [4][5][6][7][8], the physical shape of animals [9], or internal organ shape of the animals [10] which has been explored. Authors in [4,7] proposed a bioinspired UWB antenna based on Igna Marginata leaf. e antenna proposed in [7] has dimension of 40 × 30 mm 2 and is built on an FR4 substrate of height 1.5 mm. A simulated impedance bandwidth of 9.9 GHz was achieved, but the author did not report the radiation efficiency of the antenna. e authors in [2] explored maple leaf shape to design the UWB antenna. e antenna was built on Rogers RT 5880 substrate with a relative dielectric constant of 2.2, a loss tangent of 0.0009, and a height of 1. 575 mm. e overall antenna dimension is 30.5 × 35.5 mm 2 and achieves an impedance bandwidth of 3.1 GHz to 13.15 GHz with a 5GHz-6 GHz band notch. e authors also did not report the radiation efficiency. Authors in [6] presented a bioinspired antenna based on sugarcane leaf, operating at 700 MHz, and a reflector was used to enhance the gain of the proposed antenna. In [11], the authors investigated Tulip flower shape having a dimension 56.25 × 35.7 mm 2 for UWB application, and impedance bandwidth of 9.45 GHz was achieved. Jasmine flower, Ginkgo Biloba, Carica Papaya, and Bidens Pilosa leaves have been designed, fabricated, and analyzed for UWB applications. e radiation efficiency of an antenna is a critical antenna performance metric in mobile applications where omnidirectional radiation is essential. is is because, radiation efficiency, unlike gain, is a measure of antenna performance without considering the direction of radiation. Notwithstanding, none of the bioinspired UWB antennas in the open literature gives much attention to the radiation efficiency of the reported antennas. erefore, in the quest for increased UWB bandwidth and enhanced efficiency, this work investigates vine leaf (Vitis vinifera) shape as a bioinspired structure for UWB wireless applications. e motivation behind this investigation is the sawtooth edge of the vine leaf. In the next section, the vine leaf shape antenna design procedure is presented and then the shape was used as the radiating patch. Section 3 presents the parametric study of the proposed antenna; the measurement results are presented in Section 4; the comparative analysis of the proposed antenna with the relevant existing work in the open literature is presented in Section 5, and the conclusion is presented in Section 6.

Antenna Design Procedure
e radiating patch of the proposed antenna is based on vine leaf shape on an epoxy glass (FR4) substrate of a dielectric constant of 4.4, a loss tangent of 0.02, and a height of 1.5 mm with a defected ground structure (DGS) and a vertical rectangular (VR) slot as the ground plane. e proposed antenna is fed with a 50Ω feedline. e proposed antenna dimension is 35 × 27.6 mm 2 . Figure 1 shows the picture of a typical vine leaf. e proposed antenna shall hereafter be referred to as vine bioinspired UWB antenna (VBi-UWBA). e initiator of the VBi-UWBA structure is a circular shape. A circular patch of radius (r) 10 mm is chosen as the initiator as shown in Figure 2(a) to achieve a lower edge frequency (LEF) around 3 GHz using equation (1) which is adapted from reference [12]. As shown in Figure 1, the vine leaf has saw-like edges and the circular shape edge is perturbed to achieve a saw-like edge as shown in Figure 2(b). Hence, the maximum edge length of the VBi-UWBA radiating patch from its center is 10 mm as demonstrated in Figure 2(b). Using the area of a circle given in equation (2), the area of the initiator is 314.2 mm 2 but the area of the resultant vine leaf shape is measured to be 221.32 mm 2 using the measurement tool of the HFSS simulator.
is implies that the resultant radius is 8.39 mm. A 16.1% reduction is achieved compared with the initiator (CMPA). Using the resultant radius to determine the LEF of the vine leaf shape from equation (1), a LEF of 3.22 GHz is expected compared with 3 GHz of the CMPA. Meanwhile, the lower antenna resonant frequency has also been related to its radiating patch perimeter using equations (3) and (4) in reference [5].
area of a circle(A) � πr 2 , where D is the diameter of the circle in millimeter, g is the gap between the edge of the radiating patch and the ground plane in millimeter, ε r is the dielectric constant of the substrate, φ is the perimeter of the patch, f r is the resonant frequency, and k accounts for the effect of dielectric permittivity of the substrate, and it is taken to be 1.15 [12]. e proposed VBi-UWBA geometry is presented in Figure 3. Table 1 presents the XY-points coordinates of the proposed Vitis vinifera leaf radiating patch which are extracted from the graphing technique for repeatability purposes.
e design parameters labeled in Figure 4 are as presented in Table 2.

Parametric Study and Analysis of VBi-UWBA
In this section, the parametric analysis of VBi-UWBA is presented. is is done to evaluate the effect of the design parameters on the resonant frequency. To evaluate the effect of L g , the slot was eliminated and L g varies from 20 mm to 5 mm with an interval of 3 mm. e response is as shown in Figure 5. It can be observed that the length of the ground plane has a tremendous effect on the performance of the proposed structure. It can be seen that a UWB with a -10 dB fractional bandwidth of 118.1% (3.21 GHz-12.47 GHz) can be achieved only when L g � 10 mm. When L g � 11 mm, the reflection coefficient response demonstrates a UWB with a bandgap between 8.41 GHz and 9.46 GHz. For L g � 5mm, the first resonance mode is at 2.87 GHz which is the lowest resonant mode of all the L g variation. It can be observed that as L g increases, the fundamental resonance frequency increases. is effect can be traced to the change in the antenna impedance matching with the 50 Ω feedline because as the capacitive reactance formed by the dielectric-filled gap between the radiating patch and the ground varies with the variation in the length of the ground plane, there is a corresponding variation in the overall antenna impedance which can cause impedance mismatch.    It can also be observed that as L g increases from 5 mm to 14 mm, the LEF is simultaneously increasing. Notwithstanding, LEF starts decreasing again from L g � 17 mm and above. erefore, L g can be used for tuning the LEF of a monopole antenna. Because the focus of this work is UWB, the optimized L g is therefore taken to be 10 mm based on this parametric analysis. Figure 6 shows the effect of L s on reflection coefficient while keeping L g and W s at 10 mm and 2.18 mm, respectively. It is observed that the VR slot on the ground plane affects the return loss at the resonance rather than creating another resonance at a new frequency. It is can be seen that at the lower resonance frequency, the best return loss (31.3 dB) is achieved when L s � 4 mm. Notwithstanding, at this value of L s , the return loss is relatively poor around 9.2 GHz compared with when it is 3 mm, 5 mm, and 6 mm. It can be seen that, though, the return loss response when L s � 6 mm is saggy from 3.22 GHz to 12.47 GHz. Hence, 6 mm is chosen as the optimized value of L s . It is observed that slot in the ground plane enhances the return loss which is a result of matching the antenna impedance to the feedline  g Separation between patch and ground 0.00  impedance by reducing the capacitive reactance introduced by the feedline and thereby enhances the impedance matching of the antenna.

e Effect of Slot Width (W s ).
e effect of the slot width of the ground plane is presented in Figure 7. It can be seen that W s has almost the same effect as the slot length. It is observed that UWB is achievable at 1 mm, 1.5 mm, 2 mm, and 2.182 mm values of W s without a notch between 3.1 GHz-12.38 GHz, respectively. Meanwhile, 2.5 mm and 3.25 mm values of W s demonstrate a band notch within the UWB between 8.55 GHz and 9.60 GHz. 2.182 mm gives a better return loss response. Hence, the optimized parameter of W s is taken to be 2.182 mm. It is noted that W s does not have a considerable effect on the LEF of the proposed structure but there is a notable effect on the return loss. Hence, the width of the slot can be used to enhance the return loss of VBi-UWBA. erefore, the optimized value of the defected ground plane is given in Table 2.

Results and Discussion
e prototype of the proposed antenna is as shown in Figure 8. Figure 8(a) shows the top layer (the vine radiating patch and the feedline), and the ground plane is shown in Figure 8(b). e reflection coefficient measurement setup is as shown in Figure 9. e Rhode and Schwaz ZVA50 Vector Network Analyzer is used for the reflection coefficient measurement of the proposed VBi-UWBA. Figure 10 shows the simulated and measured reflection coefficient of the proposed bioinspired UWB antenna. It can be seen from the simulation that the VBi-UWBA has a fractional bandwidth of 117.9% (3.26 GHz-12.62 GHz) at a return loss of 10 dB. It can be observed that the LEF of the simulation (3.26 GHz) agrees with the LEF predicted

Radiation Pattern.
e radiation pattern of the proposed VBi-UWBA is investigated at 4.5 GHz, 5.5 GHz, 7.5 GHz, 10.5 GHz, and 13.5 GHz which are presented as shown in Figures 11(a)-11(e), respectively. It can be observed that the radiation pattern at 4.5 GHz and 5.5 GHz is bidirectional in XZ-plane while the XZ-plane radiation patterns at 7.5 GHz, 10.5 GHz, and 13.5 GHz are quasiomnidirectional. At YZ-plane, the radiation patterns are omnidirectional in all the investigated frequencies.
At 4.5 GHz, the direction of the main lobe is at 176°and the angular width (3 dB) is 112°for XZ-plane as shown in Figure 11(a). As can be seen in Figure 11(b), the 5.5 GHz XZplane radiation pattern has its main lobe direction at 166°a nd the 3 dB angular width is 106°. Furthermore, at 7.5 GHz, the main lobe direction is at 16°and the 3 dB angular width is 78°at XZ-plane as shown in Figure 11(c). As shown in Figure 11(d), at 10.5 GHz, the main lobe direction is at 30°a nd the angular width (3 dB) is 54°at XZ-plane. In the case of 13.5 GHz, the main lobe direction is at 68°and its 3 dB angular width is 56°as shown in Figure 11(e). Hence, the proposed VBi-UWBA has a stable radiation pattern through the entire bandwidth. ese characteristics make VBi-UWBA a good candidate for mobile applications.

e Gain and Radiation Efficiency of the Proposed VBi-UWBA.
Antenna gain shows how well the antenna radiates energy in a particular direction, but radiation efficiency shows how well an antenna utilizes the received power for radiation in all directions. Equations (5) and (6) present the theoretical formula for gain and radiation efficiency, respectively.
e gain of VBi-UWBA at 4.5Ghz, 5.5GHz, 7.5GHz, 10.5GHz, and 13.5GHz is presented in Figure 12. A peak gain of 2.9 dB, 3.5 dB, 4.7 dB, 3.4 dB, and 6.7 dB is achieved at 4.5Ghz, 5.5GHz, 7.5GHz, 10.5GHz, and 13.5 GHz, respectively. is shows that the proposed antenna has a suitable gain across the UWB. e radiation efficiency and the axial ratio of the proposed VBi-UWBA are presented in Figure 13. It can be observed that the proposed antenna demonstrates high radiation efficiency ranging from 78% to 97%. As far as we know, this is the highest peak radiation efficiency reported in the literature for compact UWB antenna applications with FR4 substrate. It can be observed in Figure 13 that at 11.5 GHz, the proposed VBi-UWBA demonstrates circular polarization with a 2.2% 3dB axial ratio bandwidth (ARBW).
where G(φ, θ) is the total gain, e is the efficiency, U(φ, θ) is the radiation intensity, P in is the total input power, R r is the radiation resistance, and R L is the radiation losses.

e Current Distribution of VBi-UWBA.
In order to have a full understanding of the operation of the proposed VBi-UWBA, a study of its current distribution is performed and presented in this section. From Section 3.1, it can be observed that there are four excitation modes which occur at 4.6 GHz, 8 GHz, 10.8 GHz, and 11.5 GHz, respectively. erefore, the investigation of the mode of operation of the proposed VBi-UWBA is done at these frequencies using its surface current distribution. Figure 14 shows the current distribution at the aforesaid frequencies.
e current distribution of the fundamental mode is as shown in Figure 14(a). It can be observed that the current flows toward the top tip of the radiating patch with the higher density current flowing along the edge. In addition, at the ground plane, the current flows toward the edge of the VR slot to near the radiating patch. is excitation mode is equivalent to the fundamental mode (TE11) of a circular patch (initiator). e calculated resonant frequency of this mode is 4.7 GHz using the circular patch antenna design equation given as follows, which agrees with the computation result:      International Journal of Antennas and Propagation where a is the radius of the radiating patch which in our case is 8.39 mm and X nm is the mth zero of the derivative of J n (ka). Figure 14(b) shows the current distribution at 8 GHz; it can be observed that different modes are excited which leads to a null at the center of the radiating patch. is scenario justifies why the resonance at this frequency almost disappeared. At this frequency, the current is seen to be flowing towards the two bottom edges of the ground plane. e current distribution at 10.8 GHz is as shown in Figure 14(c). Just like in the case of 8 GHz, many modes are excited by the antenna and therefore a null can be observed at the center of the radiating patch as well as the two halves of the ground plane, hence poor resonance. At 11.5 GHz, the current distribution is seen to be rotating in with time. erefore, circular polarization is achieved at this frequency.
e CP achieved at this frequency (11.5 GHz) is due to the excitation of two linear modes with a 90°phase shift as seen in Figure 14.
is could be traced to the asymmetric topology of the Vitis vinifera leaf-shaped and not the feeding technique [13]. With this analysis, it can be clearly stated that excitation of several modes which are added constructively leads to the UWB nature of the proposed VBi-UWBA in this work.

Group Delay of VBi-UWBA.
Group delay is another performance metric of the UWB antenna which shows the degree of distortion between the antenna transmitting and the receiving antenna. In order to evaluate the group delay of VBi-UWBA, a face-to-face configuration of two VBi-UWBAs is set up at 300 mm apart for the far-field scenario as shown in Figure 15. It can be seen from Figure 16 that the group delay of VBi-UWBA is around 0.1 ns from 3 GHz to 12.4 GHz. ere is a little spike to 1.2 ns at 13.2 GHz but which is still within the acceptable limit. Hence, there is a negligible distortion in the signal of the UWB system. With this analysis, the proposed VBi-UWBA is suitable for highspeed UWB communication.

Radiating patch
Ground plane 300 mm  International Journal of Antennas and Propagation than the proposed antenna in this work, it was observed that the peak gain of the proposed antenna is higher than the peak gain reported by the authors and the radiation efficiency is not reported. e antenna proposed in this work is comparatively compact than the antenna reported in [15,17,19,24,25] as shown in Table 3. Although the proposed antenna in [20] has a compact size nonetheless with a peak group delay and minimum radiation efficiency of 4 ns and 35% while in this work, a peak group delay and minimum radiation efficiency are 1.1 ns and 78%, respectively. It can be observed that the antenna proposed in [21] has a similar size to the antenna proposed in this work but with a lesser peak gain. It can be observed that VBi-UWBA outperformed the reported bioinspired UWB antennas in terms of size, fractional bandwidth, peak gain, and radiation efficiency. erefore, the proposed VBi-UWBA is well suitable for high-speed UWB applications.

Conclusion
A novel compact bioinspired UWB antenna is investigated in this work. A conventional monopole antenna design formula is adapted to determine the LEF of the proposed bioinspired antenna in this work. e analysis result and computation result agree. e measurement agrees with the simulation result. e proposed VBi-UWBA has a fractional bandwidth of 115.43% at a 10 dB return loss, a suitable gain across the wideband, a high radiation efficiency, and a stable omnidirectional radiation pattern which make it a suitable candidate for UWB wireless applications such as sensing, imaging, ground-penetration radar, and personal area network (PAN).

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.