CPW-Fed Transparent Antenna for Vehicle Communications

: In this paper, a fully transparent multiband antenna for vehicle communications is designed, fabricated


Introduction
Communications have acquired an important role in the development of concepts such as the internet of things (IoT) [1].The IoT provides emerging and novel applications to transform cities in smart cities by improving the quality and performance of its public services [2,3].Smart cities are capable of sensing, integrating, and analyzing critical information in city operation and evolution to ensure sustainability and quality of life through the advancement of urban electronic communications in interoperable systems [4][5][6].One of the principal goals in smart cities is to count on smart mobility.Smart mobility consists of transport that defines an innovative infrastructure for traffic and transport that saves resources by using new technologies for maximum accessibility and efficiency for citizens [7].In the IoT field, there exist specific networks that can improve and grow smart mobility; these are known as vehicular networks (VN) [8].These networks carry out vehicle to vehicle (V2V), vehicle to infrastructure (V2I) [9], and vehicle to everything (V2X) communication [8].The development and implementation of VN contribute to the integration of mobility with everything.That is, being reached by the concept of smart [1,10], which ranges from smart devices and homes to smart cities.Currently, several communications systems integrate with vehicles due to the growing demand for connectivity in vehicular environments [11,12].Such integration is regulated under the framework of the IEEE 802.11p standard [11,13].At present, several works on VN have employed communications systems based on IEEE 802.11p-this standard is the core for the wireless access for vehicular environments [14][15][16][17].The IEEE 802.11p standard allows vehicular communications defined in the physical (PHY) and medium access control (MAC) layers in the dedicated short-range communications (DSRC) protocol stack [18].In DSRC, the 5.85-5.925GHz range is divided into seven channels of 10-MHZ bandwidth each, which is the half bandwidth of 802.11a [18].This standard offers short transmission distance less than 300 m and data rates ranging from 6 to 27 Mb/s [14].Besides, 802.11p uses a carrier frequency of 5.9 GHz [16].Moreover, recent developments have been carried out proposing a system that combines the traditional 802.11p standard VANET networks with LTE networks to form a hybrid Cloud-VANET to provide an efficient routing protocol with low latency and high reliability along with less congestion [19].Reference [20] presents an analysis of the obtained results of a V2V framework developed on VANETs to reduce large amounts of traffic from LTE networks.
A relevant element in the design of vehicular communication systems is the antenna, which must satisfy the appropriate radiation specifications [21].Besides, the antennas must ensure that there is no intervention with the vehicle operation.Usually, antennas are made of metal on dielectric substrates, which can be unattractive for the growing need to optimize spaces and offer better technical and aesthetic performance.Some examples of this are in references [22,23]-present antennas for 802.11p standard, but are implemented in an opaque substrate.Even in reference [22], the proposed design is a volumetric structure.Furthermore, in [24], a fractal antenna design is presented-this antenna was fabricated using Polyvinyl chloride as a transparent substrate, but it uses copper for the radiation element, making it not completely transparent.Therefore, demand is emerging for research, development, and use of transparent antennas that can be integrated into windshields and windows, solar cell panels, mobile devices, and in the automotive industry, [25,26].Finally, it has to be mentioned that there exist other transparent antenna designs for vehicular communications, but they operate within the UHF and VHF bands [27,28].
Additionally, transparent antennas start to be an option in the application of RF energy harvesting.Some examples of these applications are described by [29,30].For the development of transparent antennas, various materials and configurations have been tested to improve efficiency.Some of the transparent conductive films that have been tested for use in this type of antennas include silver-coated polyester film (AgHT-8) [31], indium-tin-oxide (ITO) [32], Indium-zinc-tin oxide (IZTO) [33], Silver grid layer coating (AgGL) [34], and zinc oxide heavily doped with gallium (GZO) [25].Besides, some transparent antennas designs employ mesh metal films printed on glass substrates-these metal layers present a low sheet resistance [35,36].Recently, mesh metal films are applied in transparent antennas at 60 GHz to improve their performance [37].
On the other hand, there are many investigations of transparent antenna geometries.In reference [26] a transparent antenna for WLAN application in 5 GHz is introduced, whose topology is inspired in a flower with six petals built into indium-tin oxide film (ITO) as a transparent radiation element.Several antennas designs use coplanar wave feed [31,38,39], because the transparent conductive film is on just one side of the substrate.In [31], a coplanar waveguide-fed transparent antenna for extended ultrawideband applications is presented, using AgHT-8 thin film as conductive material with a staircase-shaped rectangular radiator and a modified partial ground.Moreover, references [38,39] report a multiband transparent antenna using a coplanar waveguide for 5G applications.
Notwithstanding the vast developed area, a remaining problem for designing transparent antennas based on conductive films with sheet resistance over 5 Ohms, (mainly with ITO) [26,29,30], is to obtain a multiband behavior with narrow bandwidths.Typically, the transparent antennas with ITO show a fractional bandwidth higher than 20% generating a UWB response.In this work, a multiband operation achieves, and the frequencies bands are well defined.
In this work, the design of a fully transparent antenna using ITO-coated glass with a coplanar waveguide (CPW)-fed slot dipole with a multiband operation, IEEE 8002.11p(5.9 GHz), and LTE sub 6 GHz bands, is proposed for future vehicular communications applications.In order to obtain the desired frequencies, a modified ground plane was introduced with symmetrical rectangular stubs [40,41].The antenna characterization is performed by considering the measured reflection coefficient and the radiation pattern.Even though the ITO has a high sheet resistance, the experimental results obtained satisfy the frequency requirements for the standard IEEE 802.11 and LTE sub 6 GHz bands.Besides, the experimental results are similar in behavior to the simulated ones, but with a slight shift in frequency.Nevertheless, this good concordance is unusual in other reported transparent antennas based on conductive films with a high sheet impedance.The main contributions of the proposed design are a fully transparent antenna that operates at frequencies for vehicular communications standards, and small size.

Materials and Methods
In this research, Adafruit commercial indium-tin-oxide (ITO)-coated glass with a thickness of 1850 Å was employed to fabricate the proposed antenna.The transparent conductive oxide (TCO) sheet resistance (Rs) was estimated by the well-known method of the four-point probe [42] performed over thirteen positions on a film sample, as can be seen in Figure 1.Table 1 presents those results and the final average for Rs of 7.943 ohm/square that was used for the design and simulations of the antenna.The substrate is glass with relative permittivity and thickness of 5.5 and 1.1 mm, respectively.In the development of antennas, those factors are significant to determine the frequency responses and antenna efficiency [32].Therefore, it is important to incorporate them into the antenna design and simulation process.Moreover, a coplanar waveguide-fed slot antenna with impedance matching stub was chosen to obtain a multiband response through a crossmatch technique for a proper impedance matching [40,41], and allowing both the radiator and the ground plane to be on the same side for fabrication ease.High-frequency structural simulator (HFSS, ANSYS, PA, US) was used to design and optimize the chosen topology for the transparent antenna through parametric analysis.
Appl.Sci.2020, 10, x FOR PEER REVIEW 3 of 11 6 GHz bands, is proposed for future vehicular communications applications.In order to obtain the desired frequencies, a modified ground plane was introduced with symmetrical rectangular stubs [40,41].The antenna characterization is performed by considering the measured reflection coefficient and the radiation pattern.Even though the ITO has a high sheet resistance, the experimental results obtained satisfy the frequency requirements for the standard IEEE 802.11 and LTE sub 6 GHz bands.Besides, the experimental results are similar in behavior to the simulated ones, but with a slight shift in frequency.Nevertheless, this good concordance is unusual in other reported transparent antennas based on conductive films with a high sheet impedance.The main contributions of the proposed design are a fully transparent antenna that operates at frequencies for vehicular communications standards, and small size.

Materials and Methods
In this research, Adafruit commercial indium-tin-oxide (ITO)-coated glass with a thickness of 1850 Å was employed to fabricate the proposed antenna.The transparent conductive oxide (TCO) sheet resistance (Rs) was estimated by the well-known method of the four-point probe [42] performed over thirteen positions on a film sample, as can be seen in Figure 1.Table 1 presents those results and the final average for Rs of 7.943 ohm/square that was used for the design and simulations of the antenna.The substrate is glass with relative permittivity and thickness of 5.5 and 1.1 mm, respectively.In the development of antennas, those factors are significant to determine the frequency responses and antenna efficiency [32].Therefore, it is important to incorporate them into the antenna design and simulation process.Moreover, a coplanar waveguide-fed slot antenna with impedance matching stub was chosen to obtain a multiband response through a crossmatch technique for a proper impedance matching [40,41], and allowing both the radiator and the ground plane to be on the same side for fabrication ease.High-frequency structural simulator (HFSS,ANSYS,PA,US) was used to design and optimize the chosen topology for the transparent antenna through parametric analysis.Through a parametric analysis in the HFSS simulator, the optimized antenna dimensions were obtained, and they are shown in Figure 2 and described in Table 2, respectively.The antenna feedline was calculated to obtain a coplanar waveguide (CPW) with a characteristic impedance of 50 ohms.The proposed transparent antenna is a capacitively coupled CPW-fed slot, dipole antenna with two pairs of protruded slot lines with different lengths, W1 and W2.The resonant frequencies correspond to the two different resonant paths.The two resonance frequencies for the design are 1.9 GHz and 5.9 GHz, which are used in LTE and 802.11p, respectively.Besides, in the parametric analysis, we made variations over the parameters W1, W2, and Wp1, to reach the desired frequency bands performing the matching impedance and observe their impact on the antenna design.Through a parametric analysis in the HFSS simulator, the optimized antenna dimensions were obtained, and they are shown in Figure 2 and described in Table 2, respectively.The antenna feedline was calculated to obtain a coplanar waveguide (CPW) with a characteristic impedance of 50 ohms.The proposed transparent antenna is a capacitively coupled CPW-fed slot, dipole antenna with two pairs of protruded slot lines with different lengths, W1 and W2.The resonant frequencies correspond to the two different resonant paths.The two resonance frequencies for the design are 1.9 GHz and 5.9 GHz, which are used in LTE and 802.11p, respectively.Besides, in the parametric analysis, we made variations over the parameters W1, W2, and Wp1, to reach the desired frequency bands performing the matching impedance and observe their impact on the antenna design.In [40], it is mentioned that the resonant frequencies are independently controlled by a common aperture and the three pairs of respective thin slots.However, in our design, the variation of the length W1 shift both frequencies, as shown in Figure 3a.Moreover, Figure 3b shows variations in the higher frequency due to change in the length W2, while the lower frequency is fixed.Similar behavior is observed in Figure 3c when varying the width of the central patch, the high frequency is mainly affected, whereas the lower band is minimally changed.The reason is attributable to the fact that lengths of W2 and Wp1 are closer to the shortest wavelength [41].It is important to mention that in our simulations, the SMA connector was considered.In [40], it is mentioned that the resonant frequencies are independently controlled by a common aperture and the three pairs of respective thin slots.However, in our design, the variation of the length W1 shift both frequencies, as shown in Figure 3a.Moreover, Figure 3b shows variations in the higher frequency due to change in the length W2, while the lower frequency is fixed.Similar behavior is observed in Figure 3c when varying the width of the central patch, the high frequency is mainly affected, whereas the lower band is minimally changed.The reason is attributable to the fact that lengths of W2 and Wp1 are closer to the shortest wavelength [41].It is important to mention that in our simulations, the SMA connector was considered.

Results and Discussion
After obtaining the results through numerical simulation, the antenna was manufactured, and measurements of return loss, gain, and radiation diagrams were performed.The transparent antenna was fabricated by using a photolithography process.The transfer of the antenna geometry to the ITOcoated glass was made using a photosensitive film, which was exposed to UV light through a mask with the antenna geometry.Then the area exposed was removed to continue with the etching of the ITO films with a (1:1) solution of hydrochloric acid (HCL).This last process was done at 40° C temperature for 2 min.Finally, we remove the photoresistant layer.Besides, an SMA connector was employed to connect the antenna; this connector was soldered to the transparent antenna using indium (In) solder spheres.The fabricated antenna placed onto the BUAP label is shown in Figure 4, where the transmittance of the ITO can be observed.The vector network analyzer (VectorStar, Anritsu) was used to measure the S11 from 0.5 GHz to 12 GHz.The simulated and measured return loss (S11) are shown and compared in Figure 5.The measured S11 at 5.9 GHz is −16.7 dB, which shows a good agreement with the simulated results.

Results and Discussion
After obtaining the results through numerical simulation, the antenna was manufactured, and measurements of return loss, gain, and radiation diagrams were performed.The transparent antenna was fabricated by using a photolithography process.The transfer of the antenna geometry to the ITO-coated glass was made using a photosensitive film, which was exposed to UV light through a mask with the antenna geometry.Then the area exposed was removed to continue with the etching of the ITO films with a (1:1) solution of hydrochloric acid (HCL).This last process was done at 40 • C temperature for 2 min.Finally, we remove the photoresistant layer.Besides, an SMA connector was employed to connect the antenna; this connector was soldered to the transparent antenna using indium (In) solder spheres.The fabricated antenna placed onto the BUAP label is shown in Figure 4, where the transmittance of the ITO can be observed.The vector network analyzer (VectorStar, Anritsu) was used to measure the S11 from 0.5 GHz to 12 GHz.The simulated and measured return loss (S11) are shown and compared in Figure 5.The measured S11 at 5.9 GHz is −16.7 dB, which shows a good agreement with the simulated results.Although a slightly detuned response is obtained from the measurement, related to fabrication flaws, each fractional bandwidth (FWB) remains, as can be seen in Table 3, showing the FBW for every band in simulation and measurement.The measured FBWs for S11 below −10 dB at the lower band is 31.34%(1.82 to 2.5 GHz), and at the upper band is 87.03% (4.66 to 11.84 GHz), which is large enough to cover the 5.9 GHz required frequency.Thus, experimental results fulfill the communication IEEE 802.11p standard for the required band.Figure 6 shows the simulated and measured 2-D radiation patterns of the proposed antenna at 2.1 and 5.9 GHz.At both frequencies, the H-plane radiation pattern presents omnidirectional behavior, whereas the E-plane radiation pattern is bidirectional.Moreover, to complete the characterization of the antenna, the peak gain of the antenna was simulated and measured at 2.1 and    Although a slightly detuned response is obtained from the measurement, related to fabrication flaws, each fractional bandwidth (FWB) remains, as can be seen in Table 3, showing the FBW for every band in simulation and measurement.The measured FBWs for S11 below −10 dB at the lower band is 31.34%(1.82 to 2.5 GHz), and at the upper band is 87.03% (4.66 to 11.84 GHz), which is large enough to cover the 5.9 GHz required frequency.Thus, experimental results fulfill the communication IEEE 802.11p standard for the required band.Figure 6 shows the simulated and measured 2-D radiation patterns of the proposed antenna at 2.1 and 5.9 GHz.At both frequencies, the H-plane radiation pattern presents omnidirectional behavior, whereas the E-plane radiation pattern is bidirectional.Moreover, to complete the characterization of the antenna, the peak gain of the antenna was simulated and measured at 2.1 and Although a slightly detuned response is obtained from the measurement, related to fabrication flaws, each fractional bandwidth (FWB) remains, as can be seen in Table 3, showing the FBW for every band in simulation and measurement.The measured FBWs for S11 below −10 dB at the lower band is 31.34%(1.82 to 2.5 GHz), and at the upper band is 87.03% (4.66 to 11.84 GHz), which is large enough to cover the 5.9 GHz required frequency.Thus, experimental results fulfill the communication IEEE 802.11p standard for the required band.Figure 6 shows the simulated and measured 2-D radiation patterns of the proposed antenna at 2.1 and 5.9 GHz.At both frequencies, the H-plane radiation pattern presents omnidirectional behavior, whereas the E-plane radiation pattern is bidirectional.Moreover, to complete the characterization of the antenna, the peak gain of the antenna was simulated and measured at 2.1 and 5.9 GHz-Table 4 summarizes the obtained peak gains.The measured radiation patterns and peak gains are in concordance with the simulate results.Besides, the antenna efficiency at 2.1 and 5.9 GHz was simulated; the obtained values are 10% and 15%, respectively.These gain peaks and efficiency values are in agreement with those reported for other antennas that use ITO as a conductive film [43].
5.9 GHz-Table 4 summarizes the obtained peak gains.The measured radiation patterns and peak gains are in concordance with the simulate results.Besides, the antenna efficiency at 2.1 and 5.9 GHz was simulated; the obtained values are 10% and 15%, respectively.These gain peaks and efficiency values are in agreement with those reported for other antennas that use ITO as a conductive film [43].Furthermore, the current distribution for the transparent antenna was obtained by simulation at 2.1 and 5.9 GHz, and it is presented in Figure 7. From Figure 7a, it is observed that the distribution current at 2.1 GHz is more intense on the feedline and, at the bottom of the middle path.Another significant amount of current is around the geometry of the antenna.On the other hand, at 5.9 GHz, the current distribution is mainly on the feedline, and at the middle patch.However, there is a significant amount of current between the resonators and at the largest resonator edges, as shown in Figure 7b.Furthermore, the current distribution for the transparent antenna was obtained by simulation at 2.1 and 5.9 GHz, and it is presented in Figure 7. From Figure 7a, it is observed that the distribution current at 2.1 GHz is more intense on the feedline and, at the bottom of the middle path.Another significant amount of current is around the geometry of the antenna.On the other hand, at 5.9 GHz, the current distribution is mainly on the feedline, and at the middle patch.However, there is a significant amount of current between the resonators and at the largest resonator edges, as shown in Figure 7b.

Figure 1 .
Figure 1.Schematic positions on indium-tin oxide (ITO) film placed on a glass slide for sheet resistance (Rs)/square measurement.

Figure 5 .
Figure 5.Comparison of simulated and measured return loss parameters.

Figure 5 .
Figure 5.Comparison of simulated and measured return loss parameters.

Figure 5 .
Figure 5.Comparison of simulated and measured return loss parameters.

Table 1 .
Rs/Square Measurements Obtained on ITO Film.
ITO filmFigure 1.Schematic positions on indium-tin oxide (ITO) film placed on a glass slide for sheet resistance (Rs)/square measurement.

Table 1 .
Rs/Square Measurements Obtained on ITO Film.