The Smallest Form Factor UWB Antenna with Quintuple Rejection Bands for IoT Applications Utilizing RSRR and RCSRR

In this paper, we present the smallest form factor microstrip-fed ultra-wideband antenna with quintuple rejection bands for use in wireless sensor networks, mobile handsets, and Internet of things (IoT). Five rejection bands have been achieved at the frequencies of 3.5, 4.5, 5.25, 5.7, and 8.2 GHz, inseminating four rectangular complementary split ring resonators (RCSRRs) on the radiating patch and placing two rectangular split-ring resonators (RSRR) near the feedline-patch junction of the conventional ultra-wideband (UWB) antenna. The design guidelines of the implemented notched bands are provided at the desired frequency bands and analyzed. The measured results demonstrate that the proposed antenna delivers a wide impedance bandwidth from 3 to 11 GHz with a nearly omnidirectional radiation pattern, high rejection in the multiple notched-bands, and good radiation efficiency over the entire frequency band except at the notched frequencies. Simulated and measured response match well specifically at the stop-bands.


Introduction
Since 2002, the Federal Communication Commission (FCC) has permitted its commercial ultra-wideband (UWB) systems to operate within the 3.1 GHz to 10.6 GHz frequency range [1,2]. UWB technology has attracted much attention from researchers because of wide impedance bandwidth, high-speed data rate, and good time domain resolution [3,4]. In sensing applications, UWB antennas are used in short-range transmission [5], medical applications [6,7], surveillance systems [8], Internet of things (IoT) [9], and wireless body area networks (WBANs) [10]. In medical sensing applications and microwave imaging sensing, UWB radar has been in the spotlight owing to its high accuracy and robustness in a multipath environment. The authors of [6] implemented UWB sensors for detecting microscopic malignant breast tumors and checked their feasibility using multilayered breast phantoms. The authors of [8] designed two different UWB antennas for the solution of pulsed asset tag devices. For portable IoT sensors and WBANs, the compact-sized antenna has received much interest, and can be easily embedded in IoT devices [11][12][13]. However, owing to the extremely broadband of operation for UWB systems, there exists an inevitable overlap between UWB communication systems and many narrowband wireless communication systems such as Worldwide-Interoperability for Microwave-Access (WiMAX) operating at 3.30-3.60 GHz, the Indian National Satellite (INSAT) operating at 4.50-4.80 GHz, the wireless local area network (WLAN) operating at 5. 15-5.35   GHz, X-band satellite communication operating at 7.2-7.65 GHz, and the International Telecommunication Union (ITU 8-GHz) frequency band operating at 7.95-8.55 [14]. Hence, we aim to design a compact-sized antenna for IoT applications which can achieve multiple-notched bands in [39]. Although the antenna successfully rejects the five narrow frequency bands, the reported antenna size is quite bulky (80 × 80 mm 2 ) for use in portable IoT applications. Similarly, the authors of [40,41] proposed a quintuple band-notched UWB antenna which has a capability to reject 3.6, 5.2, 5.8, 7.5, and 8.3 GHz frequency bands. However, they have placed the five slot resonators in a very irregular pattern which makes it very tough to judge the exact position of the notches in their design. Also, the frequency response of the notched bands is not steep enough (with a Voltage Standing Wave Ratio (VSWR) between 2.2 and 3.8) to achieve desirable rejection performance.
In this paper, we present a microstrip-line fed planar quintuple ultra-wideband (UWB) antenna using a combination of the rectangular complementary split ring resonator (RCSRR) and the rectangular split-ring resonator (RSRR) for rejecting the WiMAX, INSAT, lower WLAN, upper WLAN, and ITU 8 GHz frequency bands. At the beginning, a conventional stair cased structured reference UWB antenna is designed and fabricated to operate within the desired UWB frequency band. Then, the reference UWB antenna is modified for the proposed quintuple band-notched UWB antenna to reject the 3.5, 4.5, 5.25, 5.7, and 8.2 GHz bands for WiMAX, INSAT, lower WLAN, upper WLAN, and ITU 8 GHz frequency bands, respectively. To optimize the dimensions of the RSRR and RCSRR, a commercially available 3D-EM software, Ansoft High Frequency Structure Simulator (HFSS) is used. The proposed antenna with quintuple rejection bands is fabricated, and the measurements are presented for the verification. Finally, the design process in relation to the reflection coefficient, VSWR, antenna gain, radiation efficiency, and radiation pattern are described in detail. The proposed antenna performance has been checked for tumor detection, and the simulated results are presented.
The geometrical analysis and simulation results of the antenna are discussed in detail in Section 2 with corresponding results. The measurement setup and experimental results of the proposed and the reference UWB antenna are explained in Section 3. Section 4 deals with the comparison of the proposed antenna with another recent state-of-the-art design reported in the literature. Section 5 provides the application of the proposed antenna in microwave sensing, and the conclusion then follows.

Design and Simulation Results
Figure 1a,c shows the front and rear-view geometry and dimensions of the reference UWB antenna while Figure 2a,c shows the front and rear view prototype of the conventional UWB antenna designed [35] and termed as a reference UWB antenna. This antenna was designed on RogersRO5880 substrate with a thickness of 31 mils, a relative dielectric constant of 2.2, and a loss tangent of 0.0009.
A modification was carried out for the reference UWB antenna in order to efficiently reject the interfering frequency bands that fall within the UWB frequency band. Figure 1b,c show the front and rear-view geometry and dimensions of the proposed quintuple band-notched UWB antenna. The prototype of the proposed antenna is also fabricated as shown in Figure 2b,c. The dimensions of the reference and proposed antenna is listed in Table 1. band-notched antenna was carried out in [39]. Although the antenna successfully rejects the five narrow frequency bands, the reported antenna size is quite bulky (80 × 80 mm 2 ) for use in portable IoT applications. Similarly, the authors of [40,41] proposed a quintuple band-notched UWB antenna which has a capability to reject 3.6, 5.2, 5.8, 7.5, and 8.3 GHz frequency bands. However, they have placed the five slot resonators in a very irregular pattern which makes it very tough to judge the exact position of the notches in their design. Also, the frequency response of the notched bands is not steep enough (with a Voltage Standing Wave Ratio (VSWR) between 2.2 and 3.8) to achieve desirable rejection performance.
In this paper, we present a microstrip-line fed planar quintuple ultra-wideband (UWB) antenna using a combination of the rectangular complementary split ring resonator (RCSRR) and the rectangular split-ring resonator (RSRR) for rejecting the WiMAX, INSAT, lower WLAN, upper WLAN, and ITU 8 GHz frequency bands. At the beginning, a conventional stair cased structured reference UWB antenna is designed and fabricated to operate within the desired UWB frequency band. Then, the reference UWB antenna is modified for the proposed quintuple band-notched UWB antenna to reject the 3.5, 4.5, 5.25, 5.7, and 8.2 GHz bands for WiMAX, INSAT, lower WLAN, upper WLAN, and ITU 8 GHz frequency bands, respectively. To optimize the dimensions of the RSRR and RCSRR, a commercially available 3D-EM software, Ansoft High Frequency Structure Simulator (HFSS) is used. The proposed antenna with quintuple rejection bands is fabricated, and the measurements are presented for the verification. Finally, the design process in relation to the reflection coefficient, VSWR, antenna gain, radiation efficiency, and radiation pattern are described in detail. The proposed antenna performance has been checked for tumor detection, and the simulated results are presented.
The geometrical analysis and simulation results of the antenna are discussed in detail in Section 2 with corresponding results. The measurement setup and experimental results of the proposed and the reference UWB antenna are explained in Section 3. Section 4 deals with the comparison of the proposed antenna with another recent state-of-the-art design reported in the literature. Section 5 provides the application of the proposed antenna in microwave sensing, and the conclusion then follows.

Design and Simulation Results
Figure 1a,c shows the front and rear-view geometry and dimensions of the reference UWB antenna while Figure 2a,c shows the front and rear view prototype of the conventional UWB antenna designed [35] and termed as a reference UWB antenna. This antenna was designed on RogersRO5880 substrate with a thickness of 31 mils, a relative dielectric constant of 2.2, and a loss tangent of 0.0009.
A modification was carried out for the reference UWB antenna in order to efficiently reject the interfering frequency bands that fall within the UWB frequency band. Figure 1b

Design Equations for the RCSRR and RSRR
For the initial choice of the RCSRR of major axis length Li and minor axis length Wi in Figure 1b, the design equations for a desired notched band frequency fnotch are given by: where εr is the relative permittivity of the substrate, λg is the guided wavelength at the desired frequency, c is the speed of light, and fnotch is the desired notched frequency. The effective dielectric constant can be calculated from Equation (2), where h is the height of the substrate and Wf is the width of the microstrip feedline. Parametric simulations have been performed to obtain the optimal width of the RCSRR. Ws equals 0.3 mm.
For the initial choice of the RSRR of horizontal axis length Lx, vertical axis length Ly and width of the RSRR Ws in Figure 1b, we can use Equation (3) to obtain the desired notch frequency for the resonators: where fnotch (2) is the desired resonant notched band frequency for the RSRR, and λg is the guided wavelength at the desired frequency.

Structural Analysis
Etching the slot resonators is one of the most effective techniques in designing the UWB antenna with multi-rejection bands without any size increase. After adequately calculating the initial value of

Design Equations for the RCSRR and RSRR
For the initial choice of the RCSRR of major axis length L i and minor axis length W i in Figure 1b, the design equations for a desired notched band frequency f notch are given by: where ε r is the relative permittivity of the substrate, λ g is the guided wavelength at the desired frequency, c is the speed of light, and f notch is the desired notched frequency. The effective dielectric constant can be calculated from Equation (2), where h is the height of the substrate and W f is the width of the microstrip feedline. Parametric simulations have been performed to obtain the optimal width of the RCSRR. W s equals 0.3 mm.
For the initial choice of the RSRR of horizontal axis length L x , vertical axis length L y and width of the RSRR W s in Figure 1b, we can use Equation (3) to obtain the desired notch frequency for the resonators: where f notch (2) is the desired resonant notched band frequency for the RSRR, and λ g is the guided wavelength at the desired frequency.

Structural Analysis
Etching the slot resonators is one of the most effective techniques in designing the UWB antenna with multi-rejection bands without any size increase. After adequately calculating the initial value of the design variables for the band-notched frequency bands, it can be further optimized through parametric analysis and a step-by-step design procedure. To more clearly demonstrate the design process of this quintuple band-notched UWB antenna, Figure 3 presents the subsequent design process of the proposed quintuple band-notched UWB antenna and the corresponding frequency response at each sequence.
In the beginning, a single band-notched UWB antenna is designed to reject the WiMAX (3.5 GHz) frequency band. The structure of this antenna is shown in Figure 3a and termed as Antenna_1 which comprises of a single slot resonator using Equation (1), and optimized using the parametric analysis with HFSS. Then, a dual band-notched UWB antenna is designed by integrating another rectangular slot resonator within the first resonator. The dimensions of this resonator are also calculated from Equation (1) and further optimized at the center frequency of 4.5 GHz for notching the INSAT frequency band. This antenna along with its frequency response is shown in Figure 3b and termed as Antenna_2. Similarly, repeating the same procedure, we obtain the triple band-notched UWB antenna, and the quad band-notched UWB antenna termed as Antenna_3 and Antenna_4 by rejecting lower WLAN (5.25 GHz), and upper WLAN (5.7 GHz), respectively. Finally, a pair of RSRRs is placed in the vicinity of the feedline to obtain a broad notched frequency band at ITU 8.2 GHz (whose dimensions are calculated using Equation (3)), and optimized with HFSS. The final antenna is termed as the proposed antenna, and its frequency response is also presented in Figure 3e which shows the combined graph of all antennas and the variations within one plot.
This independent behavior of the slot resonator also makes the proposed antennas structure advantageous to be used for single, dual, triple quadruple and quintuple band rejection capabilities depending on the application requirements. By using the R-CSRR and RSRR, we can quickly set the multiple notches to the desired frequencies by selecting the length and width of the resonators according to Equations (1) and (3). the design variables for the band-notched frequency bands, it can be further optimized through parametric analysis and a step-by-step design procedure. To more clearly demonstrate the design process of this quintuple band-notched UWB antenna, Figure 3 presents the subsequent design process of the proposed quintuple band-notched UWB antenna and the corresponding frequency response at each sequence.
In the beginning, a single band-notched UWB antenna is designed to reject the WiMAX (3.5 GHz) frequency band. The structure of this antenna is shown in Figure 3a and termed as Antenna_1 which comprises of a single slot resonator using Equation (1), and optimized using the parametric analysis with HFSS. Then, a dual band-notched UWB antenna is designed by integrating another rectangular slot resonator within the first resonator. The dimensions of this resonator are also calculated from Equation (1) and further optimized at the center frequency of 4.5 GHz for notching the INSAT frequency band. This antenna along with its frequency response is shown in Figure 3b and termed as Antenna_2. Similarly, repeating the same procedure, we obtain the triple bandnotched UWB antenna, and the quad band-notched UWB antenna termed as Antenna_3 and Antenna_4 by rejecting lower WLAN (5.25 GHz), and upper WLAN (5.7 GHz), respectively. Finally, a pair of RSRRs is placed in the vicinity of the feedline to obtain a broad notched frequency band at ITU 8.2 GHz (whose dimensions are calculated using Equation (3)), and optimized with HFSS. The final antenna is termed as the proposed antenna, and its frequency response is also presented in Figure 3e which shows the combined graph of all antennas and the variations within one plot.
This independent behavior of the slot resonator also makes the proposed antennas structure advantageous to be used for single, dual, triple quadruple and quintuple band rejection capabilities depending on the application requirements. By using the R-CSRR and RSRR, we can quickly set the multiple notches to the desired frequencies by selecting the length and width of the resonators according to Equations (1) and (3).

Simulated Input Voltage Standing Wave Ratio (VSWR) (Return-Loss) and Antenna Gain (Radiation Efficiency)
The proposed quintuple band-notched UWB antenna is simulated using HFSS. Figure 4 shows the simulated reflection coefficient Гin and VSWR (Voltage Standing Wave Ratio) of the proposed antenna which reveals the effective filtering behavior at 3.5, 4.5, 5.25, 5.7, and 8.2 GHz for WiMAX, INSAT, lower WLAN, upper WLAN, and ITU 8 GHz frequency bands, respectively. The simulated antenna peak gain (G0), radiation efficiency ( ), and realized antenna gain (Gr = G0(1 − |Гin| 2 ) are presented in Figure 5, which shows proper suppression occurs in the primary radiator represented by the antenna gain (G0) as well as at the antenna input in the form of the impedance mismatch (Гin) at the notched bands.
To further evaluate the quintuple band-notching function resulting from R-CSRR and RSRR, the surface current distributions for the proposed antenna have been simulated at 3.5, 4.5, 5.25, 5.7, and 8.2 GHz and shown in Figure 6. It can be observed that the currents are mainly concentrated at these

Simulated Input Voltage Standing Wave Ratio (VSWR) (Return-Loss) and Antenna Gain (Radiation Efficiency)
The proposed quintuple band-notched UWB antenna is simulated using HFSS. Figure 4 shows the simulated reflection coefficient Г in and VSWR (Voltage Standing Wave Ratio) of the proposed antenna which reveals the effective filtering behavior at 3.5, 4.5, 5.25, 5.7, and 8.2 GHz for WiMAX, INSAT, lower WLAN, upper WLAN, and ITU 8 GHz frequency bands, respectively. The simulated antenna peak gain (G 0 ), radiation efficiency (η), and realized antenna gain (G r = G 0 (1 − |Г in | 2 ) are presented in Figure 5, which shows proper suppression occurs in the primary radiator represented by the antenna gain (G 0 ) as well as at the antenna input in the form of the impedance mismatch (Г in ) at the notched bands.
To further evaluate the quintuple band-notching function resulting from R-CSRR and RSRR, the surface current distributions for the proposed antenna have been simulated at 3.5, 4.5, 5.25, 5.7, and 8.2 GHz and shown in Figure 6. It can be observed that the currents are mainly concentrated at these frequencies around the slot resonators which results in severe impedance mismatches around the resonant frequencies leading to the quintuple band-notching behavior of the antenna.

Parametric Analysis for the Optimal Width of the Resonators (W s )
Due to the compact size of the proposed antenna with quintuple rejection bands, the reflection coefficient performance of the antenna is sensitive to geometrical parameters and requires appropriate optimizations and tuning. The parametric analysis has been carried out to illustrate the critical geometrical parameters of the proposed antenna that affect the notched frequency bands. The effect of W s (width of the R-CSRR and RSRR) is observed by varying its value, and the corresponding response is shown in Figure 7 by keeping all other design parameters to the fixed values. It is shown that by slightly varying W s , the corresponding notch frequency is shifted to the upper and lower frequency band, which is quite critical. After performing parametric tuning, the optimal resonator width has been selected as W s = 0.3 mm.

Parametric Analysis for the Optimal Width of the Resonators (Ws)
Due to the compact size of the proposed antenna with quintuple rejection bands, the reflection coefficient performance of the antenna is sensitive to geometrical parameters and requires appropriate optimizations and tuning. The parametric analysis has been carried out to illustrate the critical geometrical parameters of the proposed antenna that affect the notched frequency bands. The effect of Ws (width of the R-CSRR and RSRR) is observed by varying its value, and the corresponding response is shown in Figure 7 by keeping all other design parameters to the fixed values. It is shown that by slightly varying Ws, the corresponding notch frequency is shifted to the upper and lower frequency band, which is quite critical. After performing parametric tuning, the optimal resonator width has been selected as Ws = 0.3 mm.

Measurement Results and Discussions
The reference and the proposed quintuple band-notched UWB antennas were fabricated, and their frequency response was measured to demonstrate the multiple notching responses. The Thru-Reflect-Line (TRL) calibration has been carried out after implementing the TRL calibration kit with the same antenna substrate and SMA connectors. The frequency response of both the reference and the proposed antennas after TRL calibration is shown in Figure 8. The response clearly reveals that there exists a filtering behavior centered at frequencies of 3.5, 4.5, 5.25, 5.7, and 8.2 GHz. While rejecting the WiMAX, INSAT, and ITU 8 GHz frequency bands as designed, there are slight frequency shifts towards the higher frequencies in the measurement. Table 2 presents the discrepancies between the simulated and measured notch frequencies. The minor frequency shifts were caused by the over-etched slot width from the milling machine. The slot width was measured using Vernier caliper at several different positions at the slot resonators. While we use Ws equal to 0.3 mm, the measured mean and standard deviation values of Ws were 0.3487 mm and 0.0258 mm, respectively. The frequency shifts in the lower (L-WLAN) and the upper WLAN (U-WLAN) frequency bands were relatively drastic where the mutual coupling between two slots was found to be larger than other slot resonators. The effect of the over-etched slot width (Ws) becomes more dominant for L-WLAN and U-WLAN resonators as both the slot resonators are close to each other, which in turn has more significant mutual coupling, which shifts the resonance frequency much higher than other resonators. Figure 9 compares the simulated and measured reflection coefficient of the proposed antenna after setting Ws = 0.3487 mm, which verifies our observation. Table 3 presents the discrepancy between the

Measurement Results and Discussions
The reference and the proposed quintuple band-notched UWB antennas were fabricated, and their frequency response was measured to demonstrate the multiple notching responses. The Thru-Reflect-Line (TRL) calibration has been carried out after implementing the TRL calibration kit with the same antenna substrate and SMA connectors. The frequency response of both the reference and the proposed antennas after TRL calibration is shown in Figure 8. The response clearly reveals that there exists a filtering behavior centered at frequencies of 3.5, 4.5, 5.25, 5.7, and 8.2 GHz. While rejecting the WiMAX, INSAT, and ITU 8 GHz frequency bands as designed, there are slight frequency shifts towards the higher frequencies in the measurement. Table 2 presents the discrepancies between the simulated and measured notch frequencies. The minor frequency shifts were caused by the over-etched slot width from the milling machine. The slot width was measured using Vernier caliper at several different positions at the slot resonators. While we use W s equal to 0.3 mm, the measured mean and standard deviation values of W s were 0.3487 mm and 0.0258 mm, respectively. The frequency shifts in the lower (L-WLAN) and the upper WLAN (U-WLAN) frequency bands were relatively drastic where the mutual coupling between two slots was found to be larger than other slot resonators. The effect of the over-etched slot width (W s ) becomes more dominant for L-WLAN and U-WLAN resonators as both the slot resonators are close to each other, which in turn has more significant mutual coupling, which shifts the resonance frequency much higher than other resonators. Figure 9 compares the simulated and measured reflection coefficient of the proposed antenna after setting W s = 0.3487 mm, which verifies our observation. Table 3 presents the discrepancy between the simulated and measurement response when the simulation setup is changed with W s = 0.348 mm, keeping all other parameters fixed.
The radiation pattern of the reference and the proposed quintuple band-notched UWB antenna were measured in an anechoic chamber at three different frequencies which cover the center, lower, and upper frequencies of the entire UWB band. Figure 10 presents the measurement setup for the radiation pattern measurement of the reference and proposed antenna in an anechoic chamber. The chamber is equipped with the near-field planner scanner and a far-field tower to test and measure the radiation pattern of the antenna under test (AUT). At 3.9, 6.1, and 7.8 GHz the radiation patterns have been measured which cover the lower, upper, and mid frequencies of the UWB. The radiation pattern is measured at each 1 degree step interval in an anechoic chamber having a range of 0-360 • . The selected frequencies were 3.9, 6.1, and 7.8 GHz and its co-polarized beam pattern at the XZ-plane (E-plane) and YZ-plane (H-plane) are presented in Figure 11. There is a good agreement between the radiation pattern of the reference antenna and the proposed quintuple band-notched UWB antenna at 3.9 and 6.1 GHz, while the radiation pattern became distorted at 7.8 GHz and there arise nulls at both planes. It is due to the distortion in the phase distribution of the electric field and the increase in the magnitude of higher order harmonic modes at the higher frequency from the structure. simulated and measurement response when the simulation setup is changed with Ws = 0.348 mm, keeping all other parameters fixed. The radiation pattern of the reference and the proposed quintuple band-notched UWB antenna were measured in an anechoic chamber at three different frequencies which cover the center, lower, and upper frequencies of the entire UWB band. Figure 10 presents the measurement setup for the radiation pattern measurement of the reference and proposed antenna in an anechoic chamber. The chamber is equipped with the near-field planner scanner and a far-field tower to test and measure the radiation pattern of the antenna under test (AUT). At 3.9, 6.1, and 7.8 GHz the radiation patterns have been measured which cover the lower, upper, and mid frequencies of the UWB. The radiation pattern is measured at each 1 degree step interval in an anechoic chamber having a range of 0-360 °. The selected frequencies were 3.9, 6.1, and 7.8 GHz and its co-polarized beam pattern at the XZ-plane (E-plane) and YZ-plane (H-plane) are presented in Figure 11. There is a good agreement between the radiation pattern of the reference antenna and the proposed quintuple band-notched UWB antenna at 3.9 and 6.1 GHz, while the radiation pattern became distorted at 7.8 GHz and there arise nulls at both planes. It is due to the distortion in the phase distribution of the electric field and the increase in the magnitude of higher order harmonic modes at the higher frequency from the structure.

Comparison with Recently Proposed Designs
To validate the effectiveness of the proposed antenna over another state-of-the-art design, we perform a detailed comparison of the proposed antenna with other recently reported designs from the literature. Table 4 provides the comparison with recently proposed UWB antenna with multiple notches in terms of the dimensions of the antenna, and the number of notched bands. It is concluded that the presented antenna has obvious advantages in the antenna size with the largest number of rejection bands, a planar structure, and complete rejection of the interfering bands as well. Moreover, the proposed antenna in this paper also achieves stable radiation patterns over the complete UWB frequency band.
The proposed antenna is easy to fabricate and the notched frequencies can be adjusted with the width of the slot resonators as compared to other antennas mentioned in the table which utilize irregular patch geometry, irregular slot resonators on the patch and ground plane, multilayered structures for notching, and parasitic stubs which lead to complex structures which result in a difficulty in massive fabrication. It is noteworthy that the implemented antenna in [19][20][21][22][23][24][25][26][27][28][29] completely rejected overall 5/6 GHz WLAN bands, which led to uncompromising signal quality degradation of the received information. The antenna will be highly applicable in microwave imaging sensing applications, motion sensing, and high speed wireless communication systems including wireless sensor networks, mobile handsets, and IoT due to its small size with an excellent performance as compared with other state-of-the-art structures.

Application of the Proposed Antenna to the Breast Tumor Sensing
Owing to the integrated quintuple notched bands for wireless sensor networks, mobile handsets, and the Internet of things (IoT), the proposed compact antenna can be applicable to various portable UWB sensors without severe interruption with aforementioned wireless system. The feasibility of the proposed antenna is investigated in detecting tumor cells in a canonical breast phantom model using the 3D EM simulator, HFSS. As presented in Figure 12, the proposed band-notched UWB antenna is placed at each side of the biological breast phantom model within the frequency range of 3-11 GHz. The model is an inhomogeneous dielectric medium to simulate the human breast by including skin, tissue, and tumor. The breast model utilized in our simulation setup with and without tumor are shown in Figure 12a,b, respectively. The permittivity and conductivity of the skin, tissue, and tumor are given in Table 5, calculated from [42][43][44]. The breast tissue layer has been covered with two skin layers, one at the top side and another at the bottom side. The stacked organic layers were scanned by two proposed quintuple notched antennas (one transmitting and the other receiving) with and without tumor cell.
After transmitting the UWB pulses with the proposed antenna, the received antenna waveform response is used to detect the tumor cells by comparing the transmitted waveform with and without tumor cells. First, both antennas are placed in a vacuum without placing any stacked layer, and the received waveform is observed. Then, stacked organic layers with and without tumor layer are placed between transmitted and receiving antennas, and the waveform is observed. The combined received waveforms observed in above three cases are presented in Figure 13.    It is seen that the amplitude of the received waveform decreases considerably in case of the tumor layer as shown in Figure 13a, which may lead the conclusion that defected cells are present in the body. The same process is repeated by shifting each antenna 5 and 10 mm away from the stacked organic layers, and the received waveform is observed as presented in Figure 13b,c, respectively. It is clear from Figure 13b,c that moving the antennas away from the stacked biological organic layer degrades overall signal strength. However, the amplitude of the received waveform for the stacked layers with the tumor drops more considerably. It is due to the fact that the existence of the stacked organic layers such as skin and tissue produces multiple reflections and losses on the surface of each layer during the pulse transmission. Notably, the presence of defected tumor layer within the body increases the energy losses apparently because of the different dielectric properties of the tumor cells as compared to skin and tissue layers. It is seen that the amplitude of the received waveform decreases considerably in case of the tumor layer as shown in Figure 13a, which may lead the conclusion that defected cells are present in the body. The same process is repeated by shifting each antenna 5 and 10 mm away from the stacked organic layers, and the received waveform is observed as presented in Figure 13b,c, respectively. It is clear from Figure 13b,c that moving the antennas away from the stacked biological organic layer degrades overall signal strength. However, the amplitude of the received waveform for the stacked layers with the tumor drops more considerably. It is due to the fact that the existence of the stacked organic layers such as skin and tissue produces multiple reflections and losses on the surface of each layer during the pulse transmission. Notably, the presence of defected tumor layer within the body increases the energy losses apparently because of the different dielectric properties of the tumor cells as compared to skin and tissue layers.

Conclusions
In this paper, we presented a microstrip-fed ultra-wideband (UWB) antenna with quintuple rejection bands for wireless sensor networks. Quintuple rejection bands were realized at the frequencies of 3.5, 4.5, 5.25, 5.7, and 8.2 GHz utilizing four R-CSRRs on the radiating patch and placing two RSRRs near the feedline-patch junction of the conventional UWB antenna. The design guidelines of the implemented notched bands are discussed with corresponding equations. The width of the slot resonator has been found to be an essential tuning knob to achieve the desired notching frequencies. With its compact size, the measured results of the proposed antenna correspond well with the simulation. The antenna possesses a nearly omnidirectional radiation pattern with an excellent gain suppression at the notched-bands over the entire frequency band. The proposed antenna is also evaluated to detect tumor cells in the breast phantom model. Hence, the proposed antenna will be the most suitable candidate to be used in microwave imaging sensing

Conclusions
In this paper, we presented a microstrip-fed ultra-wideband (UWB) antenna with quintuple rejection bands for wireless sensor networks. Quintuple rejection bands were realized at the frequencies of 3.5, 4.5, 5.25, 5.7, and 8.2 GHz utilizing four R-CSRRs on the radiating patch and placing two RSRRs near the feedline-patch junction of the conventional UWB antenna. The design guidelines of the implemented notched bands are discussed with corresponding equations. The width of the slot resonator has been found to be an essential tuning knob to achieve the desired notching frequencies.
With its compact size, the measured results of the proposed antenna correspond well with the simulation. The antenna possesses a nearly omnidirectional radiation pattern with an excellent gain suppression at the notched-bands over the entire frequency band. The proposed antenna is also evaluated to detect tumor cells in the breast phantom model. Hence, the proposed antenna will be the most suitable candidate to be used in microwave imaging sensing applications, wireless sensor networks, and IoT applications.