An Elliptical-Shaped Dual-Band UWB Notch Antenna for Wireless Applications

Abstract

This paper discusses an elliptical ultrawideband (UWB) antenna and a dual-band UWB notch antenna. To achieve a UWB bandwidth, two corner cuts are etched into the rectangular slot on the partial ground plane. An inverted-U-shaped and conductor-shaped resonator are utilized to achieve dual-band notch characteristics on a partial ground plane. The suggested antenna has an overall dimension of $24\times 32 {\mathrm{mm}}^2$. The suggested UWB antenna has a gain of 4.9 dB, a bandwidth of 2.5–11 GHz, a linear phase response, a group delay of less than 1 ns, and a steady radiation pattern. The suggested UWB notch rejects WLAN and ITU bands from 5.2–5.7 GHz and 7.2–8.5 GHz, respectively, with an impedance bandwidth of 2.5–11 GHz. The UWB notch antenna features a linear phase, a group delay of less than 1 ns, and a stable radiation pattern.

1. Introduction

A UWB bandwidth is the frequency band bounded by the points that are 10 dB below the highest radiated emission, as based on the complete transmission system including the antenna. The upper boundary is designated $f_H$, and the lower boundary is designated $f_L$. An antenna having a fractional bandwidth equal to or greater than 0.20 or having a UWB bandwidth equal to or greater than 500 MHz, regardless of the fractional bandwidth, is called a UWB antenna. [1,2]. UWB communication, as the name implies, has a large bandwidth and supports a high transmission rate. Ultrawideband antenna applications have recently expanded to cover many computing devices and IoT peripherals [3]. The bulk of these wireless communication systems make use of a UWB antenna for purposes including but not limited to data transfer, reception, localization, location identification, sensing, and tracking.

UWB antenna design varies depending on the communication system’s radiation characteristics, and each application necessitates specialized UWB antennas. Due to developments in impulse technology, low-power communication systems, and the availability of unlicensed frequency bands, UWB has emerged as the dominant technique for short-range wireless communication [4]. Due to its inherent properties, UWB technology is well suited for precisely obtaining spatial and directional data, including a high data rate, a broad bandwidth, a reduction in multipath fading, a low cost, and low power consumption [5].

The recent proliferation of wireless communication, wireless portable devices, and smart consumer electronics has increased demand for ultrawideband antenna applications [6]. UWB antenna design research [7,8,9,10] is undertaken to improve UWB communication systems with new breakthroughs. Moreover, a single UWB antenna may span numerous frequencies, transmission functions, and operation bands. Therefore, their utilization can eliminate the need for many narrowband antennas. The interference caused by several antennas is decreased, and antenna space is conserved. It is crucial to remember that to get the most out of UWB antennas, they must be carefully designed for the individual needs of each system.

Narrowband systems such as WiMAX, WLAN, and C-band, among others, cause significant interference to UWB antennas. Strong disruptions, such as background noise, emerge from these interferences [11]. A notch is built in the UWB antenna to eliminate these intense narrowband interferences. Notch is the technique of removing unwanted frequency bands from the UWB spectrum [12].

In the literature, many UWB notch antennas have been recorded. The authors of article [13] suggest a floret antenna for wideband application. A UWB antenna with an arch-shaped ground plane is proposed using Koch fractal on the hexagonal pattern patch [14]. In paper [15], a UWB antenna with a slot-type split-ring resonator and a defective ground plane is proposed to achieve a dual notch. A dual-band notch antenna using sectorial and inverted U-shaped slots over a rectangular patch is reported in the article [16]. Paper [17] presents a fractal dual-band UWB antenna with a C-shaped complementary split-ring resonator on the patch’s transmission line to perform dual-notch filtering. A dual-notch band UWB antenna is proposed in the article [18] using C-slot and inverted U-slot. A UWB antenna in [19] uses a split-ring slot to create a dual notch. A wide bandwidth in the UWB range is achieved by altering the rectangular patch. In [20], the authors suggest a notch antenna with two bands. A meandering patch slot and a U-shaped feed slot provide a 3–3.9 and 5.22–5.7 GHz notch band. In [21], the patch’s two U-shaped stubs create a 3.0–3.9 GHz and 5.0–5.9 GHz notch band.

In this article, an elliptical UWB notch antenna has been designed and fabricated to cover UWB channel 1 to 15, i.e., low band (UWB channels 1 to 4) and high band (UWB channels 5 to 15). The addition of parasitic resonators for UWB notch antenna overcomes electromagnetic interference between bands by inserting inverted-U-shaped and iron-shaped parasitic resonators on the ground plane. Evolution steps from the UWB antenna to the UWB notch antenna are discussed. Section 2 and Section 3 discuss the technique for designing antennas. Section 4 discusses result analysis. Section 5 discusses the conclusion followed by references.

2. UWB Antenna Design Approach

The evolution of the UWB antenna is depicted in Figure 1, while the S₁₁ characteristics are depicted in Figure 2. In the first stage, an ellipse radiating patch and a rectangle ground plane are created. However, the S₁₁ value is much higher than −10 dB.

As a result, the ground plane was further modified in stage 2 to become a partly rectangular ground plane. The S₁₁ value decreases as a result. In stage 3, a partially rectangular ground plane is slotted to improve S₁₁. The rectangular slot on the ground plane significantly brings the S₁₁ value below −10 dB, but it does not cover the UWB range. As a result, in stage 4 of Figure 1, more modifications are made to obtain UWB characteristics in the antenna. Two corner cuts are etched on the rectangular slot on the ground plane. It gives the impedance bandwidth from 2.5–11 GHz, which covers the UWB range.

3. UWB Notch Antenna Design Approach

Figure 3 shows the design of an elliptical UWB notch antenna. After completing the design of the elliptical-shaped UWB antenna, the notches have to be introduced. There are many techniques to obtain notches. Two parasitic resonators, an inverted-U-shaped resonator and an iron-shaped resonator, are used to achieve the notch. The inverted-U-shaped resonator helps obtain a notch at 5.3 GHz, and the iron-shaped resonator helps in obtaining a notch at 8.1 GHz. Figure 4 shows the dimension of the suggested antenna.

Table 1. Dimension of the proposed antenna.

Parameter	Dimension (mm)	Parameter	Dimension (mm)
$a$	$24$	$i$	1.25
$b$	32	$f$	2
$c$	9.5	$t$	0.5
$d$	6	$k$	16
$e$	11.6	$l$	8
$u$	11	$m$	0.75
$g$	11.25	$m$	0.75
$v$	4	$n$	12
$l2$	4	$o$	3
$l3$	2.47	$p$	3
$j$	1.9	$q$	3.5
$h$	1.5	$r$	0.5
$s$	1.5	$x$	0.5
$y$	6	$z$	0.5

lists the antenna’s dimensions.

The length of truncation in the ground plane for achieving UWB is calculated using Equation (1).

$$\begin{array}{cc}{L}_{trunc}& =h\left(perimeter\right)+j+f+l3+i\left(perimeter\right)\\ & =1.5+1.9+2+2.47+1.25\\ & =9.12 \mathrm{mm}\end{array}$$

(1)

The relative permittivity of the FR-4 substrate is ${\mathsf{\epsilon }}_{\mathrm{r}}=4.4$, so effective permittivity can be calculated as Equation (2),

$$\begin{array}{c}{\epsilon }_{eff} = \frac{ {\epsilon }_r+1 }{2}+\frac{{\epsilon }_r-1}{2}{\left[1+12\frac{H}{w}\right]}^{-0.5 }\\ =2.7+\frac{1.7}{\sqrt{1+12(\frac{1.6\times {10}^{-3}}{3\times {10}^{-3}})}} =3.325\end{array}$$

(2)

As we can observe that the first notch frequency, $f_{notch1} \mathrm{is} \mathrm{around} 5.2 \mathrm{GHz}$, and is due to the effect of the upper resonator. Therefore, mathematically, the length of the upper resonator can be calculated using Equation (3).

$$\begin{array}{c}{L}_{upper resonator}=\frac{{\lambda }_0}{2\sqrt{{\epsilon }_{reff}}}=\frac{c}{2 f_{notch1} \sqrt{{\epsilon }_{reff}}}\\ =\frac{3\times {10}^{-8}}{2\times 5.2\times {10}^9\sqrt{3.325}} =15.55 \mathrm{mm}\end{array}$$

(3)

Similarly, the second notch frequency, $f_{notch2} \mathrm{is} \mathrm{around} 8.2 \mathrm{GHz}$ and is due to the effect of the lower resonator. Therefore, mathematically, the length of the lower resonator can be calculated using Equation (4).

$$\begin{array}{cc}{L}_{lower resonator}& =\frac{{\lambda }_0}{2\sqrt{{\epsilon }_{reff}}}=\frac{c}{2 f_{notch2} \sqrt{{\epsilon }_{reff}}}\\ & =\frac{3\times {10}^{-8}}{2\times 8.2\times {10}^9\sqrt{3.325}} =10 \mathrm{mm}\end{array}$$

(4)

3.1. Progression of UWB Notch Antenna

This section describes the evolution stages of a UWB notch antenna. It shows a step-by-step iterative process to arrive at the final structure. The following Figure 5 shows a pictorial representation of the iterative process.

A patch and a ground plane make up the proposed antenna. Both of these have undergone modification to arrive at the final structure. The S₁₁ characteristics of the UWB notch antenna at every stage are plotted together and depicted in Figure 6.

In step 1, the UWB antenna is designed. The ground plane is then etched with an in-verted-U-shaped upper resonator in step 2. The inverted-U-shaped upper resonator gives the first notch at 5.3 GHz, as shown in Figure 5. In step 3, an iron-shaped lower resonator is added to the ground plane. The iron-shaped lower resonator gives the second notch at 8.1 GHz. Thus, the upper resonator and lower resonator combination make an elliptical UWB notch antenna in step 4.

These graphs in Figure 6 show that the notch antenna has S₁₁ < −10 dB for the entire UWB range and has two notches at 5.3 GHz and 8.1 GHz due to the two resonators.

3.2. Parametric Analysis of UWB Notch Antenna

The impact of the stubs dimension on the notch antenna is examined using a parametric analysis. The dimensions t and x have an impact on the design’s performance.

3.2.1. Effect of Upper Resonator-Width ‘t’

To analyze the effects of width ‘t’ on the S₁₁ characteristics, the variation in width ‘t’ was simulated and analyzed. The S₁₁ characteristics are represented in Figure 7. When the width is 0.5 mm, the result is optimum.

3.2.2. Effect of Lower Resonator-Width ‘x’

The variation in width ‘x’ is simulated and studied to investigate the effects of width ‘x’ on the S₁₁ features. Figure 8 illustrates the S₁₁ features. The result is best when the width is 0.5 mm.

4. Discussion and Outcomes

The suggested antenna is subjected to a full-wave simulation using HFSS. ROHDE & SCHWARZ ZVL 13 network analyzer is used to conduct measurements.

4.1. UWB Antenna Results

The intended ultrawideband (UWB) antenna, shown in Figure 9, was fabricated according to the design.

4.1.1. VSWR

Figure 10 compares simulated and measured VSWR. ROHDE & SCHWARZ ZVL network analyzer measures VSWR. At VSWR < 2, the simulated impedance bandwidth is 2.8–11.2 GHz, and the operational impedance bandwidth is 2.5–11 GHz. Simulations and measurements of VSWR exhibit a minor difference. This is due to the effect of soldering, the failure to account for the SMA connector during simulation, flaws in the dielectric constant of the substrate, and manufacturing tolerances.

4.1.2. Current Distribution

Figure 11 illustrates a simulation and study of the current distribution to illustrate the functionality of the proposed UWB antenna. At 3.6, 6.8, and 9.7 GHz, the resonance qualities are examined. Figure 11 shows how different antenna parts have varied resonance patterns for different operating modes. In Figure 11a, the lower portion of the feed is active at 3.6 GHz, where the current is highest. In Figure 11b, the feed at 6.8 GHz has the highest current. Figure 11c reveals that the lower portion of the patch and feed are most active at 9.7 GHz. Thus, the antenna resonates at 3.6, 6.8, and 9.7 GHz.

4.1.3. Radiation Pattern

Figure 12 depicts the simulation of the antenna radiation pattern for resonant frequencies within the operating band. At 3.6 GHz, a bidirectional pattern is detected in the E-plane, while an omnidirectional pattern is observed in the H-plane. However, at higher frequencies (i.e., 9.7 and 12.6 GHz) the pattern is disturbed due to higher harmonics; in addition, the cross-polarization radiation magnitudes dominate the pattern. It is evident from the figure that the cross-polarization value is much lower than the co-polarization value.

4.1.4. Time-Domain Characteristics

The phase response, group delay, and isolation properties of the proposed UWB antenna can only be determined by a time-domain analysis. As can be seen in Figure 13, two identical antennas were placed in HFSS 100 mm apart for these tests. The time-domain study considered both forward- and side-facing scenarios.

In Equation (5), GD is the derivative of phase response to angular frequency.

$${\tau }_g\left(\omega \right)=-\frac{d\phi \left(\omega \right)}{d\omega }$$

(5)

The proposed UWB antenna’s group delay is depicted in Figure 14. As can be seen in Figure 14, the group delay of the antenna remains relatively the same, regardless of whether it is operating in a face-to-face or side-to-side configuration.

Figure 15 shows the antenna’s phase response. Linear phase variation yields desirable time-domain features. Figure 15 demonstrates that the phase fluctuation of the antenna is nearly linear during face-to-face and side-to-side operations.

Isolation features of the proposed UWB antenna are depicted in Figure 16. Figure 16 shows that the antenna has good isolation characteristics (S₂₁ < −20 dB).

When computing the fidelity factor, a frontal orientation, as well as a lateral orientation, are both used. Both the input signals and output signals are normalized, as shown in Figure 17. The FF is computed using the normalized transmitted and received pulses in accordance with Equations (6)–(8) [22].

$$T_s^n=\frac{T_s\left(t\right)}{\sqrt{{{\displaystyle \int }}_{-\infty }^{\infty }{\left|T_s\left(t\right)\right|}^{2}dt}}$$

(6)

$$R_s^n=\frac{R_s\left(t\right)}{\sqrt{{{\displaystyle \int }}_{-\infty }^{\infty }{\left|R_s\left(t\right)\right|}^{2}dt}}$$

(7)

$$FF=\max \underset{-\infty }{\overset{\infty }{{\displaystyle \int }}}{T}_s^n\left(t\right) R_s^n\left(t+\tau \right)dt$$

(8)

Normalization is performed to ensure that only the signal’s structure and not its amplitude is evaluated. The estimated fidelity factor values ensure that interference has a negligible effect on the received pulse at the receiver. The fidelity factor in frontal and lateral configurations is more than 98%. The greater value of the fidelity factor assures that the transmitted and received pulses are identical.

4.1.5. Gain

Figure 18 depicts a 3D gain plot at resonant frequencies at 3.6 GHz, 6.8 GHz, and 9.7 GHz. At 3.6 GHz, 6.8 GHz, and 9.7 GHz, the gain is 2.38 dB, 3.44 dB, and 4.85 dB.

Figure 19 shows that a maximum gain of 4.9 dB is achieved for the UWB microstrip antenna.

4.2. Outcome of Ultrawideband Notch Antenna

The intended ultrawideband notch antenna, shown in Figure 20, was fabricated according to the design.

4.2.1. VSWR

Figure 21 shows a comparison of the UWB notch antenna’s simulated and measured VSWR. Strong rejection can be seen in the simulated VSWR plot between the WLAN band of 5–5.6 GHz and the ITU band of 7.1–8.5 GHz, with a fractional bandwidth of almost 120% (2.8–11.2 GHz). The measured VSWR plot demonstrates a high level of attenuation across the WLAN band (5.2–5.7 GHz) and the ITU band (7.2–8.5 GHz), with a fractional bandwidth of around 125%. (2.5–11 GHz). The difference in VSWR between simulated and measured values should be attributed mostly to the influence of SMA connector soldering and fabrication tolerance.

4.2.2. Current Distribution

Figure 22 depicts the surface current distributions at notched frequencies of 5.3 GHz and 8.1 GHz with parasitic resonators, illustrating the role of parasitic inverted-U-shaped and iron-shaped resonators in achieving the notched bands. At notched frequencies, surface currents on the elliptical patch flow opposite to the surface current on the ground plane, which contains parasitic elements. Accordingly, the radiation has little to no effect at the notch frequencies. It makes two notches at around 5.3 GHz and 8.1 GHz.

4.2.3. Radiation Pattern

Figure 23 depicts the simulation of the antenna radiation pattern for resonant notch frequencies within the operating band.

At 4 GHz and 6.2 GHz, an omnidirectional pattern is detected in the E-plane, while a bidirectional pattern is observed in the H-plane. At 11.7 GHz, an omnidirectional pattern is seen in the E-plane and the H-plane.

4.2.4. Time-Domain Characteristics

Figure 24 illustrates analysis in the time domain, which includes group delay, isolation characteristics, and the fidelity factor for the proposed antenna. As mentioned in Section 4.1.4, these studies are carried out similarly.

Figure 25 shows a high delay at both notched frequencies (5.3 and 8.1 GHz), but the group delay for the face-to-face and side-to-side configurations is less than 1 ns at all other frequencies.

Figure 26 exhibits the phase variation of the input impedance of the proposed UWB notch antenna. The phase fluctuation throughout the operating band is linear, with the exception of the notched band’s center frequencies, which are around 5.3 and 8.1 GHz. This difference in phase versus frequency in the notched band verifies that the signal’s frequency components have a delay at the notched frequencies.

Figure 27 shows that the antenna has good isolation characteristics (S₂₁ < −20 dB). The fidelity factor in frontal and lateral configurations is more than 99%, as shown in Figure 28. The greater value of the fidelity factor ensures that the transmitted and received pulses are identical.

For dual-band-notched UWB applications, the time domain analysis of antenna parameters shows that the suggested antenna is a good contender.

4.2.5. Gain of UWB Notch Antenna

Figure 29 shows the total gain of the UWB notch antenna. A maximum gain of 5.9 dB is achieved for the UWB notch antenna.

4.2.6. Comparison Table

The expected design performance is assessed by comparing it to previously published UWB notch antenna designs, as shown in

Table 2. Comparison of the proposed antenna with previous works.

Ref. No. & Year	Size (mm2)	Area (mm2)	Notch Frequency Range (GHz)	No. of Notch Frequencies	Band Notch Frequencies (GHz)		Gain (dB)
					f1	f2
[23], 2017	$0.25 {\lambda }_0\times 0.25 {\lambda }_0$	$900$	4.97–5.48, 5.69–5.99	2	5.2	5.8	−4.0–5.0
[24], 2018	$0.46 {\lambda }_0\times 0.55 {\lambda }_0$	$2100$	3.3–3.6, 5–6	2	3.56	5.4	2–8.5
[25], 2019	$0.28 {\lambda }_0\times 0.26 {\lambda }_0$	1720	2.3–2.5, 3.3–3.6	2	2.4	3.45	1.26–5.5
[26], 2019	$0.28 {\lambda }_0\times 0.28 {\lambda }_0$	1296	2.5–2.69, 3.3–4.2	2	2.6	3.5	1.4–3.5
[27], 2020	$0.35 {\lambda }_0\times 0.46 {\lambda }_0$	1200	5.5–6.2, 6.6–7.1	2	5.8	6.8	2–6
[28], 2020	$0.32 {\lambda }_0\times 0.30 {\lambda }_0$	960	3.45–4.81, 5.24–6.2	2	4.4	5.8	2.7–5.1
[29], 2019	$0.30 {\lambda }_0\times 0.30 {\lambda }_0$	900	5.1–6, 7.13–7.63	2	5.4	7.4	1.1–4.89
[30], 2019	$0.52 {\lambda }_0\times 0.37 {\lambda }_0$	875	3.3–3.96, 4.7–5.9	2	3.6	5.3	2.4–5.5
[31], 2019	$0.45 {\lambda }_0\times 0.42 {\lambda }_0$	786	5.1–5.9, 7–7.8	2	5.8	7.6	2.1–6.6
Proposed work	$0.32 {\lambda }_0\times 0.42 {\lambda }_0$	768	5.2–5.7, 7.2–8.5	2	5.3	8.1	0.8–5.9

Note: ${\lambda }_0$ is calculated using the lowest operating frequency of the antenna.

.

5. Conclusions

An elliptical ultrawideband (UWB) antenna and a dual-band UWB notch antenna are described in this study. The rectangular slot on the partial ground plane is carved with two corner cuts in order to obtain UWB bandwidth. On a partial ground plane, two parasitic resonators, one of which is an inverted-U-shaped resonator, and the other of which is an iron-shaped resonator, are employed in order to obtain dual-band notch characteristics. The suggested antenna has an overall size of $24\times 32 {\mathrm{mm}}^2$. The suggested UWB antenna has a gain of 4.9 dB, an impedance bandwidth of 2.5–11 GHz, a linear phase response, a group delay of less than one nanoseconds, and a consistent radiation pattern. The proposed UWB notch antenna demonstrates high rejection in the WLAN band between 5.2 and 5.7 GHz, with a sharp notch at 5.3 GHz, and in the ITU band between 7.2 and 8.5 GHz, with a sharp notch at 8.1 GHz, with an impedance bandwidth ranging from 2.5 to 11 GHz. The UWB notch antenna has a linear phase, less than 1 ns group delay, and a steady radiation pattern.