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21 pages, 9358 KiB  
Article
Simple Compact UWB Vivaldi Antenna Arrays for Breast Cancer Detection
by Sahar Saleh, Tale Saeidi and Nick Timmons
Telecom 2024, 5(2), 312-332; https://doi.org/10.3390/telecom5020016 - 8 Apr 2024
Cited by 2 | Viewed by 1467
Abstract
In this study, at ultra-wideband (UWB) frequency band (3.1–10.6 GHz), we propose the use of compact 2:1 and 3:1 nonuniform transmission line Wilkinson power dividers (NTL WPDs) as feeding networks for simple 2 × 1 linear UWB Vivaldi tapered and nonuniform slot antenna [...] Read more.
In this study, at ultra-wideband (UWB) frequency band (3.1–10.6 GHz), we propose the use of compact 2:1 and 3:1 nonuniform transmission line Wilkinson power dividers (NTL WPDs) as feeding networks for simple 2 × 1 linear UWB Vivaldi tapered and nonuniform slot antenna (VTSA and VNSA) arrays. The 2:1 and 3:1 tapered transmission line (TTL) WPDs are designed and tested in this work as benchmarks for NTL WPDs. The VTSA array provides measured S11 < −10.28 dB at 2.42–11.52 GHz, with a maximum gain of 8.61 dBi, which is 24.39% higher than the single element. Using the VNSA array, we achieve 52% compactness and 6.76% bandwidth enhancement, with good measured results of S11 < −10.2 dB at 3.24–13 GHz and 15.11% improved gain (8.14 dBi) compared to the VNSA single element. The findings show that the NTL and Vivaldi nonuniform slot profile antenna (VNSPA) theories are successful at reducing the size of the UWB WPD and VTSA without sacrificing performance. They also emphasize the Vivaldi antenna’s compatibility with other circuits. These compact arrays are ideal for high-resolution medical applications like breast cancer detection (BCD) because of their high gain, wide bandwidth, directive stable radiation patterns, and low specific absorption rate (SAR). A simple BCD simulation scenario is addressed in this work. Detailed parametric studies are performed on the two arrays for impedance-matching enhancement. The computer simulation technology (CST) software is used for the simulation. Hardware measurement results prove the validity of the proposed arrays. Full article
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Figure 1
<p>The major contributions in this work.</p>
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<p>Configuration of compact UWB 2:1 unequal split TTL and NTL WPDs.</p>
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<p>Measured and simulated (<b>a</b>) S<sub>11</sub>, (<b>b</b>) S<sub>22</sub>, (<b>c</b>) S<sub>33</sub>, (<b>d</b>) S<sub>12</sub>, (<b>e</b>) S<sub>13</sub>, (<b>f</b>) S<sub>23</sub> of compact UWB 2:1 NTL and TTL WPDs.</p>
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<p>Measured and simulated (<b>a</b>) S<sub>12</sub> GD, (<b>b</b>) S<sub>13</sub> GD, (<b>c</b>) S<sub>12</sub> phase, and (<b>d</b>) S<sub>13</sub> phase of compact UWB 2:1 NTL and TTL WPDs.</p>
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<p>Layout of Array 1.</p>
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<p>Parametric study of the proposed UWB Array 1 in terms of S<sub>11</sub> and gain on (<b>a</b>) <span class="html-italic">r</span>, (<b>b</b>) <span class="html-italic">L<sub>T</sub></span>, (<b>c</b>) <span class="html-italic">L<sub>qw</sub></span>, (<b>d</b>) <span class="html-italic">W<sub>min</sub></span>, (<b>e</b>) <span class="html-italic">radsl</span>, (<b>f</b>) <span class="html-italic">dis</span>, (<b>g</b>) <span class="html-italic">W<sub>a</sub></span>, (<b>h</b>) <span class="html-italic">s<sub>p</sub></span>, and (<b>i</b>) <span class="html-italic">W<sub>p</sub></span>.</p>
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<p>(<b>a</b>) Configuration of compact UWB 3:1 unequal split TTL and NTL WPDs and (<b>b</b>) prototype of 3:1 TTL WPD.</p>
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<p>Measured and simulated (<b>a</b>) S<sub>11</sub>, (<b>b</b>) S<sub>22</sub>, (<b>c</b>) S<sub>33</sub>, (<b>d</b>) S<sub>12</sub>, (<b>e</b>) S<sub>13</sub>, (<b>f</b>) S<sub>23</sub> of compact UWB 3:1 NTL and TTL WPDs.</p>
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<p>Measured and simulated (<b>a</b>) S<sub>12</sub> GD, (<b>b</b>) S<sub>13</sub> GD, (<b>c</b>) S<sub>12</sub> phase, and (<b>d</b>) S<sub>13</sub> phase of compact UWB 3:1 NTL and TTL WPDs.</p>
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<p>Layout of Array 2.</p>
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<p>Parametric study of the proposed UWB Array 2 in terms of S<sub>11</sub> and gain on (<b>a</b>) <span class="html-italic">radsl</span>, (<b>b</b>) <span class="html-italic">dis</span>, (<b>c</b>) <span class="html-italic">s<sub>p</sub></span>, (<b>d</b>) <span class="html-italic">W<sub>a</sub></span>, (<b>e</b>) <span class="html-italic">W<sub>p</sub></span><sub>1</sub>, and (<b>f</b>) <span class="html-italic">W<sub>p</sub></span><sub>2</sub>.</p>
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<p>Photograph of the fabricated arrays: (<b>a</b>) front view and (<b>b</b>) back view.</p>
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<p>Simulated and measured (<b>a</b>) S<sub>11</sub>, (<b>b</b>) phase, (<b>c</b>) gain, and (<b>d</b>) simulated input impedance of the proposed arrays.</p>
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<p>(<b>a</b>) Measurement setup and (<b>b</b>) simulated and measured group delay of the proposed arrays.</p>
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<p>Simulated (dashed) and measured (solid) radiation patterns of the proposed compact UWB Vivaldi tapered and nonuniform arrays at <span class="html-italic">f</span> = 5.85 GHz (<b>a</b>) E and (<b>b</b>) H; <span class="html-italic">f</span> = 8.2 GHz (<b>c</b>) E and (<b>d</b>) H and <span class="html-italic">f</span> = 10.45 GHz (<b>e</b>) E and (<b>f</b>) H.</p>
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<p>Simulation setup of simple BCD using Array 2 (four samples) and reconstructed 2D image using RTR algorithm of (<b>a</b>) one breast tumor at the center, (<b>b</b>) one smaller breast tumor at the center, (<b>c</b>) one breast tumor off the center, (<b>d</b>) two breast tumors off the center, and (<b>e</b>) three breast tumors off the center.</p>
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<p>Simulated 3D SAR results over 10 g of the four elements of the proposed compact UWB Array 2 at (<b>a</b>) 3.35 GHz, (<b>b</b>) 4.35 GHz, (<b>c</b>) 8.86 GHz, (<b>d</b>) 12.72 GHz, and (<b>e</b>) 14.61 GHz.</p>
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24 pages, 29247 KiB  
Article
An Improved NLCS Algorithm Based on Series Reversion and Elliptical Model Using Geosynchronous Spaceborne–Airborne UHF UWB Bistatic SAR for Oceanic Scene Imaging
by Xiao Hu, Hongtu Xie, Shiliang Yi, Lin Zhang and Zheng Lu
Remote Sens. 2024, 16(7), 1131; https://doi.org/10.3390/rs16071131 - 23 Mar 2024
Cited by 3 | Viewed by 972
Abstract
Geosynchronous spaceborne–airborne (GEO-SA) ultra-high-frequency ultra-wideband bistatic synthetic aperture radar (UHF UWB BiSAR) provides high-precision images for marine and polar environments, which are pivotal in glacier monitoring and sea ice thickness measurement for polar ocean mapping and navigation. Contrasting with traditional high-frequency BiSAR, it [...] Read more.
Geosynchronous spaceborne–airborne (GEO-SA) ultra-high-frequency ultra-wideband bistatic synthetic aperture radar (UHF UWB BiSAR) provides high-precision images for marine and polar environments, which are pivotal in glacier monitoring and sea ice thickness measurement for polar ocean mapping and navigation. Contrasting with traditional high-frequency BiSAR, it faces unique challenges, such as the considerable spatial variability, significant range–azimuth coupling, and vast volumes of echo data, which impede high-resolution image reconstruction. This paper presents an improved bistatic nonlinear chirp scaling (NLCS) algorithm for imaging oceanic scenes with GEO-SA UHF UWB BiSAR. This methodology extends the two-dimensional (2-D) spectrum up to the sixth order via the method of series reversion (MSR) to meet accuracy demands and then employs an elliptical model to elucidate the alterations in the azimuth frequency modulation (FM) rate mismatch. Initially, the imaging geometry and signal model are introduced, and then a separation of bistatic slant ranges based on the configuration is proposed. In addition, during range processing, after eliminating linear range cell migration (RCM), the derivation process for the sixth-order 2-D spectrum is detailed and an improved filter is applied to correct the high-order RCM. Finally, during azimuth processing, the causes of the FM rate mismatch are analyzed, a cubic perturbation function derived from the elliptical model is used for FM rate equalization, and a unified sixth-order filter is applied to complete the azimuth compression. Experimental results with point targets and natural oceanic scenes validate the outstanding efficacy of the proposed NLCS algorithm, particularly in imaging quality enhancements for GEO-SA UHF UWB BiSAR. Full article
(This article belongs to the Special Issue Radar Signal Processing and Imaging for Ocean Remote Sensing)
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Figure 1
<p>Geometric imaging configuration of GEO-SA BiSAR.</p>
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<p>Diagram for the slant range derivation. (<b>a</b>) Geometry model of the slant range; (<b>b</b>) geometric projection of the receiver’s trajectory.</p>
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<p>Flow chart of the proposed NLCS algorithm.</p>
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<p>Diagram for LRCMC of the squinted BiSAR. (<b>a</b>) Before LRCMC; (<b>b</b>) after LRCMC.</p>
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<p>Illustration of the LRCMC. (<b>a</b>) Echo data before LRCMC; (<b>b</b>) echo data after LRCMC; (<b>c</b>) 2-D spectrum before LRCMC; (<b>d</b>) 2-D spectrum after LRCMC.</p>
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<p>The 2-D spectrum component of the point target. (<b>a</b>) The cubic phase component; (<b>b</b>) the quartic phase component; (<b>c</b>) the quintic phase component; (<b>d</b>) the sixth-order phase component.</p>
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<p>Diagram for the analysis of the FM rate distortion.</p>
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<p>The elliptical model.</p>
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<p>Diagrams of the perturbation function. (<b>a</b>) The quadratic phase of different targets before the perturbation; (<b>b</b>) the quadratic phase of different targets after the perturbation.</p>
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<p>Target distribution and imaging results focused by different algorithms. (<b>a</b>) Target distribution; (<b>b</b>) imaging result of traditional NLCS algorithm with sixth-order spectrum; (<b>c</b>) imaging result of proposed NLCS algorithm with third-order spectrum; (<b>d</b>) imaging result of proposed NLCS algorithm with sixth-order spectrum.</p>
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<p>Contour plot of P1. (<b>a</b>) Processed by the traditional NLCS algorithm with the sixth-order spectrum; (<b>b</b>) processed by the proposed NLCS algorithm with the third-order spectrum; (<b>c</b>) processed by the proposed NLCS algorithm with the sixth-order spectrum.</p>
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<p>Contour plot of P13. (<b>a</b>) Processed by the traditional NLCS algorithm with the sixth-order spectrum; (<b>b</b>) processed by the proposed NLCS algorithm with the third-order spectrum; (<b>c</b>) processed by the proposed NLCS algorithm with the sixth-order spectrum.</p>
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<p>Contour plot of P25. (<b>a</b>) Processed by the traditional NLCS algorithm with the sixth-order spectrum; (<b>b</b>) processed by the proposed NLCS algorithm with the third-order spectrum; (<b>c</b>) processed by the proposed NLCS algorithm with the sixth-order spectrum.</p>
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<p>The profiles of the impulse response of the selected targets. (<b>a</b>) Range profile of P1; (<b>b</b>) range profile of P13; (<b>c</b>) range profile of P25; (<b>d</b>) azimuth profile of P1; (<b>e</b>) azimuth profile of P13; (<b>f</b>) azimuth profile of P25.</p>
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<p>Reconstructed SAR image of an oceanic scene. (<b>a</b>) Focused by the traditional NLCS algorithm with the sixth-order spectrum; (<b>b</b>) focused by the proposed NLCS algorithm with the third-order spectrum; (<b>c</b>) focused by the proposed NLCS algorithm with the sixth-order spectrum.</p>
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<p>The magnified view of the boxed area in <a href="#remotesensing-16-01131-f015" class="html-fig">Figure 15</a>. (<b>a</b>) Focused by the traditional NLCS algorithm with the sixth-order spectrum; (<b>b</b>) focused by the proposed NLCS algorithm with the third-order spectrum; (<b>c</b>) focused by the proposed NLCS algorithm with the sixth-order spectrum.</p>
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<p>The profiles of the selected targets in <a href="#remotesensing-16-01131-f015" class="html-fig">Figure 15</a>. (<b>a</b>) Range profiles; (<b>b</b>) azimuth profiles.</p>
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26 pages, 14936 KiB  
Article
A Comparative Study of Narrow/Ultra-Wideband Microwave Sensors for the Continuous Monitoring of Vital Signs and Lung Water Level
by Anwer S. Abd El-Hameed, Dalia M. Elsheakh, Gomaa M. Elashry and Esmat A. Abdallah
Sensors 2024, 24(5), 1658; https://doi.org/10.3390/s24051658 - 4 Mar 2024
Cited by 6 | Viewed by 1466
Abstract
This article presents an in-depth investigation of wearable microwave antenna sensors (MASs) used for vital sign detection (VSD) and lung water level (LWL) monitoring. The study looked at two different types of MASs, narrowband (NB) and ultra-wideband (UWB), to decide which one was [...] Read more.
This article presents an in-depth investigation of wearable microwave antenna sensors (MASs) used for vital sign detection (VSD) and lung water level (LWL) monitoring. The study looked at two different types of MASs, narrowband (NB) and ultra-wideband (UWB), to decide which one was better. Unlike recent wearable respiratory sensors, these antennas are simple in design, low-profile, and affordable. The narrowband sensor employs an offset-feed microstrip transmission line, which has a bandwidth of 240 MHz at −10 dB reflection coefficient for the textile substrate. The UWB microwave sensor uses a CPW-fed line to excite an unbalanced U-shaped radiator, offering an extended simulated operating bandwidth from 1.5 to 10 GHz with impedance matching ≤−10 dB. Both types of microwave sensors are designed on a flexible RO 3003 substrate and textile conductive fabric attached to a cotton substrate. The specific absorption rate (SAR) of the sensors is measured at different resonant frequencies on 1 g and 10 g of tissue, according to the IEEE C95.3 standard, and both sensors meet the standard limit of 1.6 W/kg and 2 W/kg, respectively. A simple peak-detection algorithm is used to demonstrate high accuracy in the detection of respiration, heartbeat, and lung water content. Based on the experimental results on a child and an adult volunteer, it can be concluded that UWB MASs offer superior performance when compared to NB sensors. Full article
(This article belongs to the Section Environmental Sensing)
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Figure 1
<p>(<b>a</b>) Configuration of the offset feed transmission line microstrip sensor, (<b>b</b>) input impedance (real and imaginary) for both the flexible and the textile substrate and the effect of the location X<sub>f</sub> on (<b>c</b>) the flexible and (<b>d</b>) the textile substrate.</p>
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<p>Photo of fabricated antenna. (<b>a</b>) Flexible substrate, (<b>b</b>) conductive fabric, (<b>c</b>) measurement setup, and (<b>d</b>) simulated and measured |S11|.</p>
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<p>(<b>a</b>) Design steps, (<b>b</b>) simulated |S11| of design steps, (<b>c</b>) configuration of the UWB monopole antenna, and (<b>d</b>) impedance (real and imaginary).</p>
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<p>|S11| versus frequency for different parametric sweeps. (<b>a</b>) Effect of L<sub>g</sub>. (<b>b</b>) Effect of L<sub>gg</sub>. (<b>c</b>) Effect of W<sub>gg</sub>.(<b>d</b>) Effect of L<sub>k</sub>. (<b>e</b>) Effect of L<sub>m</sub>.</p>
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<p>|S11| versus frequency for different parametric sweeps. (<b>a</b>) Effect of L<sub>g</sub>. (<b>b</b>) Effect of L<sub>gg</sub>. (<b>c</b>) Effect of W<sub>gg</sub>.(<b>d</b>) Effect of L<sub>k</sub>. (<b>e</b>) Effect of L<sub>m</sub>.</p>
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<p>Surface current density distribution of the proposed monopole at different frequencies: (<b>a</b>) 2.4 GHz, (<b>b</b>) 3.5 GHz, (<b>c</b>) 5.2 GHz, (<b>d</b>) 6 GHz, (<b>e</b>) 7.5 GHz, and (<b>f</b>) 10 GHz.</p>
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<p>Measurement results. (<b>a</b>) Photo of the fabricated antenna. (<b>b</b>) Measurement setup. (<b>c</b>) Simulated and measured reflection coefficient.</p>
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<p>The model of a human chest with and without the phantom of the textile sensor (<b>a</b>) Chest phantom. (<b>b</b>) |S11| response.</p>
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<p>Simulation of two NB microwave sensors. (<b>a</b>) The 3D model. (<b>b</b>) Magnitude of |S11| in dB. (<b>c</b>) |S11| phase (red without water level, black with water level).</p>
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<p>Simulation of the S parameter’s magnitude. (<b>a</b>) Reflection coefficient. (<b>b</b>) Transmission coefficient and phase. (<b>c</b>) Reflection coefficient. (<b>d</b>) Transmission coefficient of the NB sensor.</p>
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<p>UWB microwave sensor. (<b>a</b>) Phantom model. (<b>b</b>) Reflection coefficient magnitude.</p>
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<p>Simulation of two monopole antennas with a chest model. (<b>a</b>) The 3D model. (<b>b</b>) The S parameters’ magnitude in dB. (<b>c</b>) The S-parameters’ phase in degrees.</p>
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<p>Simulation of the S parameters’ reflection coefficient (<b>a</b>) magnitude and (<b>b</b>) phase, and transmission coefficient (<b>c</b>) magnitude and (<b>d</b>) phase.</p>
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<p>The proposed system. (<b>a</b>) Block diagram. (<b>b</b>) System photo. (<b>c</b>) Experiment setup.</p>
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<p>Proof of concept. (<b>a</b>) Measurement setup. (<b>b</b>) Breathing behavior versus time.</p>
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<p>Breathing rate for the 8-year-old child using NB sensors. (<b>a</b>) Experiment setup. (<b>b</b>) Phase versus time.</p>
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<p>Breathing rate for the 35-year-old adult using NB sensors. (<b>a</b>) Experiment setup. (<b>b</b>) Phase versus time.</p>
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<p>Breathing rate after a running activity using NB sensors. (<b>a</b>) Child case. (<b>b</b>) Adult case.</p>
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<p>Breathing rate for the 8-year-old child in normal conditions using UWB sensors. (<b>a</b>) Experiment setup. (<b>b</b>) Phase versus time.</p>
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<p>Breathing rate for the 35-year-old adult in normal conditions using UWB sensors. (<b>a</b>) Experiment setup. (<b>b</b>) Phase versus time.</p>
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<p>Breathing rate after a running activity using UWB sensors. (<b>a</b>) Child case. (<b>b</b>) Adult case.</p>
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<p>Screenshot of ECG measurement using the CONTEC Machine Electrocardiograph ECG100G. (<b>a</b>) Measurement setup. (<b>b</b>) Child ECG report. (<b>c</b>) Adult ECG report.</p>
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<p>Heartbeat using NB sensors. (<b>a</b>) Child case. (<b>b</b>) Adult case.</p>
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<p>Heartbeat using UWB sensors. (<b>a</b>) Child case. (<b>b</b>) Adult case.</p>
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<p>(<b>a</b>) Drawing showing the water in the human lung [<a href="#B44-sensors-24-01658" class="html-bibr">44</a>]. (<b>b</b>) Phantom preparation and fabrication. (<b>c)</b> Measurement. (<b>d</b>) Photo of the artificial plastic lung filled with foam.</p>
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<p>Simulated S-parameters of different water contents for the narrowband sensor: (<b>a</b>) S11 magnitude. (<b>b</b>) S21 magnitude, (<b>c</b>) S11 unwrapped phase, and (<b>d</b>) S21 unwrapped phase.</p>
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<p>Simulated S-parameters of different water contents for the narrowband sensor: (<b>a</b>) S11 magnitude. (<b>b</b>) S21 magnitude, (<b>c</b>) S11 unwrapped phase, and (<b>d</b>) S21 unwrapped phase.</p>
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<p>Measured S-parameters of different water contents for the narrowband sensor. (<b>a</b>) S11 magnitude. (<b>b</b>) S21 magnitude. (<b>c</b>) S11 unwrapped phase. (<b>d</b>) S21 unwrapped phase.</p>
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<p>Simulated S-parameters of different water contents for the UWB sensor. (<b>a</b>) S11 magnitude. (<b>b</b>) S21 magnitude. (<b>c</b>) S11 unwrapped phase. (<b>d</b>) S21 unwrapped phase.</p>
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<p>Measured S-parameters of different water contents for the UWB sensor. (<b>a</b>) S11 magnitude. (<b>b</b>) S21 magnitude. (<b>c</b>) S11 unwrapped phase. (<b>d</b>) S21 unwrapped phase.</p>
Full article ">Figure 28 Cont.
<p>Measured S-parameters of different water contents for the UWB sensor. (<b>a</b>) S11 magnitude. (<b>b</b>) S21 magnitude. (<b>c</b>) S11 unwrapped phase. (<b>d</b>) S21 unwrapped phase.</p>
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21 pages, 8104 KiB  
Article
Lightweight CFARNets for Landmine Detection in Ultrawideband SAR
by Yansong Zhang, Yongping Song and Tian Jin
Remote Sens. 2023, 15(18), 4411; https://doi.org/10.3390/rs15184411 - 7 Sep 2023
Viewed by 1279
Abstract
The high-resolution image obtained by ultrawideband synthetic aperture radar (UWB SAR) includes rich features such as shape and scattering features, which can be utilized for landmine discrimination and detection. Due to the high performance and automatic feature learning ability, deep network-based detection methods [...] Read more.
The high-resolution image obtained by ultrawideband synthetic aperture radar (UWB SAR) includes rich features such as shape and scattering features, which can be utilized for landmine discrimination and detection. Due to the high performance and automatic feature learning ability, deep network-based detection methods have been widely employed in SAR target detection. However, existing deep networks do not consider the target characteristics in SAR images, and their structures are too complicated. Therefore, lightweight deep networks with efficient and interpretable blocks are essential. This work investigates how to utilize the SAR characteristics to design a lightweight deep network. The widely employed constant false alarm rates (CFAR) detector is used as a prototype and transformed into trainable multiple-feature network filters. Based on CFAR filters, we propose a new class of networks called CFARNets which can serve as an alternative to convolutional neural networks (CNNs). Furthermore, a two-stage detection method based on CFARNets is proposed. Compared to prevailing CNNs, the complexity and number of parameters of CFARNets are significantly reduced. The features extracted by CFARNets are interpretable as CFAR filters have definite physical significance. Experimental results show that the proposed CFARNets have comparable detection performance compared to other real-time state-of-the-art detectors but with faster inference speed. Full article
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<p>Demonstration of the sliding window mode in CA-CFAR.</p>
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<p>A systematic view of the CA operation. (<b>a</b>) Convolution-based implementation; (<b>b</b>) mean pooling-based implementation.</p>
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<p>A systematic view of the CFAR filter.</p>
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<p>CFAR blocks. (<b>a</b>) Single branch CFAR Block; (<b>b</b>) Inception CFAR block I; (<b>c</b>) Inception CFAR block II.</p>
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<p>Proposed CFAR block-based network architectures. A 48 × 48 single-channel SAR image is taken as an example.</p>
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<p>Two-stage target detection framework.</p>
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<p>Multi-crop classification.</p>
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<p>Collected SAR images with landmines. The sizes of images are: (<b>a</b>) 3751 × 5002; (<b>b</b>) 5001 × 5001; (<b>c</b>) 3166 × 2643; (<b>d</b>) 5001 × 5001.</p>
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<p>Examples of image patches: (<b>a</b>–<b>d</b>) Local part of minefield.</p>
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<p>Processing flow of the experiment.</p>
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<p>Landmine detection results of CFAR-A-CFARNet. (<b>a</b>–<b>f</b>) Local part of minefield. The rectangles indicate the detection results: Green rectangle, detected target; Red rectangle, false alarm; Yellow rectangle, missed target.</p>
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<p>Speed–accuracy curve of the detectors.</p>
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<p>Detection metrics with different receptive fields.</p>
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<p>Detection metrics with different probabilities of false alarms. (<b>a</b>) CFAR; (<b>b</b>) CFAR-A-CFARNet; (<b>c</b>) CFAR-B-CFARNet; (<b>d</b>) CFAR-C-CFARNet.</p>
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<p>Examples of image patches. (<b>a</b>) landmine; (<b>b</b>) clutter.</p>
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<p>Feature maps of the landmine image. (<b>a</b>) stage 1; (<b>b</b>) stage 2; (<b>c</b>) stage 3; (<b>d</b>) stage 4.</p>
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<p>Feature maps of the clutter image. (<b>a</b>) stage 1; (<b>b</b>) stage 2; (<b>c</b>) stage 3; (<b>d</b>) stage 4.</p>
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<p>Feature maps of the clutter image. (<b>a</b>) stage 1; (<b>b</b>) stage 2; (<b>c</b>) stage 3; (<b>d</b>) stage 4.</p>
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19 pages, 8546 KiB  
Article
A Miniaturized Tri-Band Implantable Antenna for ISM/WMTS/Lower UWB/Wi-Fi Frequencies
by Anupma Gupta, Vipan Kumar, Shonak Bansal, Mohammed H. Alsharif, Abu Jahid and Ho-Shin Cho
Sensors 2023, 23(15), 6989; https://doi.org/10.3390/s23156989 - 7 Aug 2023
Cited by 14 | Viewed by 1777
Abstract
This study aims to design a compact antenna structure suitable for implantable devices, with a broad frequency range covering various bands such as the Industrial Scientific and Medical band (868–868.6 MHz, 902–928 MHz, 5.725–5.875 GHz), the Wireless Medical Telemetry Service (WMTS) band, a [...] Read more.
This study aims to design a compact antenna structure suitable for implantable devices, with a broad frequency range covering various bands such as the Industrial Scientific and Medical band (868–868.6 MHz, 902–928 MHz, 5.725–5.875 GHz), the Wireless Medical Telemetry Service (WMTS) band, a subset of the unlicensed 3.5–4.5 GHz ultra-wideband (UWB) that is free of interference, and various Wi-Fi spectra (3.6 GHz, 4.9 GHz, 5 GHz, 5.9 GHz, 6 GHz). The antenna supports both low and high frequencies for efficient data transfer and is compatible with various communication technologies. The antenna features an asynchronous-meandered radiator, a parasitic patch, and an open-ended square ring-shaped ground plane. The antenna is deployed deep inside the muscle layer of a rectangular phantom below the skin and fat layer at a depth of 7 mm for numerical simulation. Furthermore, the antenna is deployed in a cylindrical phantom and bent to check the suitability for different organs. A prototype of the antenna is created, and its reflection coefficient and radiation patterns are measured in fresh pork tissue. The proposed antenna is considered a suitable candidate for implantable technology compared to other designs reported in the literature. It can be observed that the proposed antenna in this study has the smallest volume (75 mm3) and widest bandwidth (181.8% for 0.86 GHz, 9.58% for 1.43 GHz, and 285.7% for the UWB subset and Wi-Fi). It also has the highest gain (−26 dBi for ISM, −14 dBi for WMTS, and −14.2 dBi for UWB subset and Wi-Fi) compared to other antennas in the literature. In addition, the SAR values for the proposed antenna are well below the safety limits prescribed by IEEE Std C95.1-1999, with SAR values of 0.409 W/Kg for 0.8 GHz, 0.534 W/Kg for 1.43 GHz, 0.529 W/Kg for 3.5 GHz, and 0.665 W/Kg for 5.5 GHz when the applied input power is 10 mW. Overall, the proposed antenna in this study demonstrates superior performance compared to existing tri-band implantable antennas in terms of size, bandwidth, gain, and SAR values. Full article
(This article belongs to the Special Issue Smart Antennas for Future Communications)
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<p>Simulation model of 3-layered tissue phantom, (<b>a</b>) rectangular phantom where antenna is implanted in muscle, (<b>b</b>) cylindrical phantom antenna implant in skin, (<b>c</b>) antenna bent across 30 mm radius.</p>
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<p>Antenna configuration: (<b>a</b>) front view, (<b>b</b>) back view, (<b>c</b>) antenna implanted in tissue, (<b>d</b>) cross-sectional view of antenna.</p>
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<p>Step-wise geometry of the antenna.</p>
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<p>(<b>a</b>) |<span class="html-italic">S</span>11| plot (<b>b</b>) VSWR plot for the designed steps.</p>
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<p>(<b>a</b>) |<span class="html-italic">S</span>11| plot (<b>b</b>) VSWR plot for the designed steps.</p>
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<p>Surface current (<b>a</b>) 0.88 GHz (step1), (<b>b</b>) 1.66 GHz (step1), (<b>c</b>) 0.88 GHz (step2), (<b>d</b>) 1.46 GHz (step2).</p>
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<p>|<span class="html-italic">S</span>11| plot for parametric sweep for resonator length from left edge.</p>
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<p>|<span class="html-italic">S</span>11| plot for parametric sweep for resonator length from right edge.</p>
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<p>Surface current distribution at different frequencies.</p>
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<p>Photographs during measurement: (<b>a</b>) antenna without superstrate, (<b>b</b>) with superstrate, (<b>c</b>) antenna in animal tissue, (<b>d</b>) antenna in anechoic chamber.</p>
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<p>(<b>a</b>) |<span class="html-italic">S</span>11| plot for simulated and measured values, (<b>b</b>) |<span class="html-italic">S</span>11| plot for different bending radii and size of tissue.</p>
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<p>Simulated and measured 2-D and simulated 3-D radiation plots (<b>a</b>) at 0.86 GHz, (<b>b</b>) at 1.46 GHz, (<b>c</b>) at 3.5 GHz, (<b>d</b>) 5.5 GHz.</p>
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<p>Simulated and measured 2-D and simulated 3-D radiation plots (<b>a</b>) at 0.86 GHz, (<b>b</b>) at 1.46 GHz, (<b>c</b>) at 3.5 GHz, (<b>d</b>) 5.5 GHz.</p>
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<p>3-D radiation pattern in bent state (<b>a</b>) at 0.86 GHz, (<b>b</b>) at 1.46 GHz, (<b>c</b>) at 3.5 GHz, (<b>d</b>) 5.5 GHz.</p>
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<p>Plot for gain.</p>
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<p>Plot for radiation efficiency.</p>
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<p>SAR plot at (<b>a</b>) 0.86 GHz, (<b>b</b>) 1.43 GHz, (<b>c</b>) 3.5 GHz, (<b>d</b>) 5.5 GHz.</p>
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<p>SAR plot in bent state at (<b>a</b>) 0.86 GHz, (<b>b</b>) 1.43 GHz, (<b>c</b>) 3.5 GHz, (<b>d</b>) 5.5 GHz.</p>
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19 pages, 73312 KiB  
Article
Defining Breast Tumor Location Using a Four-Element Wearable Circular UWB MIMO Antenna Array
by Tamer G. Abouelnaga, Ehab K. I. Hamad, Sherif A. Khaleel and Behrokh Beiranvand
Appl. Sci. 2023, 13(14), 8067; https://doi.org/10.3390/app13148067 - 10 Jul 2023
Cited by 5 | Viewed by 2290
Abstract
The objective of this paper is to develop a wearable circular UWB MIMO antenna array, consisting of four elements, that is capable of detecting and locating tumor cells within a heterogeneous breast phantom. The antenna element operates within a bandwidth from 2.4 GHz [...] Read more.
The objective of this paper is to develop a wearable circular UWB MIMO antenna array, consisting of four elements, that is capable of detecting and locating tumor cells within a heterogeneous breast phantom. The antenna element operates within a bandwidth from 2.4 GHz to 10.6 GHz when FR4 is used as the substrate, and extends from 2.57 GHz to 12.6 GHz when a Dacron fabric is used instead. The antenna is fabricated and measured, yielding highly similar results to the simulated outcomes. In the suggested detection system, one antenna is used for transmission, while the other antennas receive the transmitted signal. The employed antenna demonstrates gains of 5.49 dBi, 9.87 dBi, 11.9 dBi, and 14.7 dBi at resonant frequencies of 2.84 GHz, 3.87 GHz, 5.83 GHz, and 8.24 GHz, respectively, when a Dacron fabric is used as the substrate. Moreover, the proposed antenna exhibits a flexible shape with minimal vertical and horizontal bending effects across the entire operating frequency band. The antenna has a compact size of 42.85 × 42.85 mm2 and is printed on an FR4 substrate with a dielectric constant of 4.5 and a thickness of 1.6 mm for testing purposes. The S-parameters of the suggested system can effectively identify and precisely locate small tumors. Furthermore, the SAR findings indicate that the amount of power absorbed by the breast phantom tissues complies with the IEEE standards, thus confirming the suitability of the recommended antenna for the early detection and localization of breast cancer. Full article
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<p>Development steps of the suggested modified antipodal Vivaldi UWB antenna.</p>
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<p>Development steps of the suggested modified antipodal Vivaldi UWB antenna.</p>
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<p>(<b>a</b>) Reflection coefficient <math display="inline"><semantics><mrow><mfenced><mrow><msub><mi>S</mi><mrow><mn>11</mn></mrow></msub></mrow></mfenced></mrow></semantics></math> of the four developed antenna stages and (<b>b</b>) input impedance of the fourth antenna stage.</p>
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<p>The fabricated modified antipodal Vivaldi UWB antenna; (<b>a</b>) top view and (<b>b</b>) bottom view.</p>
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<p>The measured and simulated reflection coefficients <math display="inline"><semantics><mrow><mfenced><mrow><msub><mi>S</mi><mrow><mn>11</mn></mrow></msub></mrow></mfenced></mrow></semantics></math> of the modified UWB antipodal Vivaldi antenna.</p>
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<p>The 2D flat antenna bends with 50, 60, 70, 80, 90, and 100 mm radii. (<b>a</b>) Horizontal bending; (<b>b</b>) vertical bending.</p>
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<p>The reflection coefficient results of different bending radii with (<b>a</b>) horizontal bending and (<b>b</b>) vertical bending.</p>
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<p>(<b>a</b>) Phantom schematic, and dispersive properties of (<b>b</b>) glandular, (<b>c</b>) skin, (<b>d</b>) fat, and (<b>e</b>) tumor tissues.</p>
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<p>(<b>a</b>) Phantom schematic, and dispersive properties of (<b>b</b>) glandular, (<b>c</b>) skin, (<b>d</b>) fat, and (<b>e</b>) tumor tissues.</p>
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<p>(<b>a</b>) Perspective view without a cavity, (<b>b</b>) top view without a cavity, (<b>c</b>) top view with Dacron cavity, and (<b>d</b>) side view with Dacron cavity of the detection system.</p>
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<p>(<b>a</b>) Perspective view without a cavity, (<b>b</b>) top view without a cavity, (<b>c</b>) top view with Dacron cavity, and (<b>d</b>) side view with Dacron cavity of the detection system.</p>
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<p>The phantom splitting and the positions of the tumor.</p>
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<p>S-parameters at (<b>a</b>) no tumor and tumor at (<b>b</b>) P1, (<b>c</b>) P2, (<b>d</b>) P3, and (<b>e</b>) P4.</p>
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<p>S-parameters at (<b>a</b>) no tumor and tumor at (<b>b</b>) P1, (<b>c</b>) P2, (<b>d</b>) P3, and (<b>e</b>) P4.</p>
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<p>The coupling coefficients <span class="html-italic">S</span><sub>22</sub> and <span class="html-italic">S</span><sub>42</sub> for the proposed detection system. (<b>a</b>) Antennas at phantom center; (<b>b</b>) antennas at 35 mm from the phantom center; (<b>c</b>) S-parameters of antennas at phantom center; (<b>d</b>) S-parameters of antennas at 35 mm from the phantom center; (<b>e</b>) antennas at 20 mm from the phantom center; (<b>f</b>) antennas at 28 mm from the phantom center; (<b>g</b>) S-parameters of antennas at 20 mm from the phantom center; (<b>h</b>) S-parameters of antennas at 28 mm from the phantom center.</p>
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<p>Detection scenario flow chart of the proposed system.</p>
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<p>The maximum spatial average SAR value using 1 g at 2.8 GHz; (<b>a</b>) 1 g, (<b>b</b>) 10 g.</p>
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<p>(<b>a</b>) ECC and (<b>b</b>) DG characteristics of the proposed MIMO antenna.</p>
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18 pages, 3275 KiB  
Article
A Statistical Analysis for Intensity Wavelength-Resolution SAR Difference Images
by Gustavo Henrique Mittmann Voigt, Dimas Irion Alves, Crístian Müller, Renato Machado, Lucas Pedroso Ramos, Viet Thuy Vu and Mats I. Pettersson
Remote Sens. 2023, 15(9), 2401; https://doi.org/10.3390/rs15092401 - 4 May 2023
Cited by 1 | Viewed by 1852
Abstract
This paper presents a statistical analysis of intensity wavelength-resolution synthetic aperture radar (SAR) difference images. In this analysis, Anderson Darling goodness-of-fit tests are performed, considering two different statistical distributions as candidates for modeling the clutter-plus-noise, i.e., the background statistics. The results show that [...] Read more.
This paper presents a statistical analysis of intensity wavelength-resolution synthetic aperture radar (SAR) difference images. In this analysis, Anderson Darling goodness-of-fit tests are performed, considering two different statistical distributions as candidates for modeling the clutter-plus-noise, i.e., the background statistics. The results show that the Gamma distribution is a good fit for the background of the tested SAR images, especially when compared with the Exponential distribution. Based on the results of this statistical analysis, a change detection application for the detection of concealed targets is presented. The adequate selection of the background distribution allows for the evaluated change detection method to achieve a better performance in terms of probability of detection and false alarm rate, even when compared with competitive performance change detection methods in the literature. For instance, in an experimental evaluation considering a data set obtained by the Coherent All Radio Band Sensing (CARABAS) II UWB SAR system, the evaluated change detection method reached a detection probability of 0.981 for a false alarm rate of 1/km2. Full article
(This article belongs to the Special Issue SAR Images Processing and Analysis)
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<p>CARABAS-II image samples for (<b>a</b>) Mission 2 and Pass 1 (<b>b</b>) Mission 3 and Pass 2 (<b>c</b>) Mission 4 and Pass 5 (<b>d</b>) Mission 5 and Pass 1. The target deployments of each image are highlighted.</p>
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<p>Anderson–Darling test results for the exponential distribution null hypothesis. The cells in red represent samples where the AD rejects the exponential distribution, and the green cells represent samples where the AD fails to reject the exponential distribution.</p>
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<p>Anderson–Darling test results for the Gamma distribution null hypothesis. The cells in red represent samples where the AD rejects the Gamma distribution, and the green cells represent samples where the AD fails to reject the Gamma distribution.</p>
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<p>Block diagram of the proposed change detection method. All SAR images illustrated in the block diagram are part of the CARABAS-II data set.</p>
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<p>Output detection binary image for experiments 1 and 18 presented in (<b>a</b>,<b>b</b>), respectively, for <math display="inline"><semantics> <mrow> <mi>T</mi> <mi>h</mi> <mo>=</mo> <mn>0.05</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>s</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.25</mn> </mrow> </semantics></math>. The original target deployments for the evaluated experiments are presented in <a href="#remotesensing-15-02401-f001" class="html-fig">Figure 1</a>a,b, respectively.</p>
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<p>Output detection binary image for experiments 1 and 18 presented in (<b>a</b>,<b>b</b>), respectively, for <math display="inline"><semantics> <mrow> <mi>T</mi> <mi>h</mi> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>s</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.25</mn> </mrow> </semantics></math>. The original target deployments for the evaluated experiments are presented in <a href="#remotesensing-15-02401-f001" class="html-fig">Figure 1</a>a,b, respectively.</p>
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<p>ROC curves performance comparison of the performances obtained from the studied change detection method under different intensity constraints <math display="inline"><semantics> <msub> <mi>s</mi> <mn>1</mn> </msub> </semantics></math> and reference methods from the literature. The compared performances were the best ROC curves extracted from [<a href="#B32-remotesensing-15-02401" class="html-bibr">32</a>,<a href="#B33-remotesensing-15-02401" class="html-bibr">33</a>], referred to as reference methods 01 and 02, respectively.</p>
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27 pages, 20567 KiB  
Article
Fast Factorized Backprojection Algorithm in Orthogonal Elliptical Coordinate System for Ocean Scenes Imaging Using Geosynchronous Spaceborne–Airborne VHF UWB Bistatic SAR
by Xiao Hu, Hongtu Xie, Lin Zhang, Jun Hu, Jinfeng He, Shiliang Yi, Hejun Jiang and Kai Xie
Remote Sens. 2023, 15(8), 2215; https://doi.org/10.3390/rs15082215 - 21 Apr 2023
Cited by 12 | Viewed by 2111
Abstract
Geosynchronous (GEO) spaceborne–airborne very high-frequency ultra-wideband bistatic synthetic aperture radar (VHF UWB BiSAR) can conduct high-resolution and wide-swath imaging for ocean scenes. However, GEO spaceborne–airborne VHF UWB BiSAR imaging faces some challenges such as the geometric configuration, huge amount of echo data, serious [...] Read more.
Geosynchronous (GEO) spaceborne–airborne very high-frequency ultra-wideband bistatic synthetic aperture radar (VHF UWB BiSAR) can conduct high-resolution and wide-swath imaging for ocean scenes. However, GEO spaceborne–airborne VHF UWB BiSAR imaging faces some challenges such as the geometric configuration, huge amount of echo data, serious range–azimuth coupling, large spatial variance, and complex motion error, which increases the difficulty of the high-efficiency and high-precision imaging. In this paper, we present an improved bistatic fast factorization backprojection (FFBP) algorithm for ocean scene imaging using the GEO satellite-unmanned aerial vehicle (GEO-UAV) VHF UWB BiSAR, which can solve the above issues with high efficiency and high precision. This method reconstructs the subimages in the orthogonal elliptical polar (OEP) coordinate system based on the GEO satellite and UAV trajectories as well as the location of the imaged scene, which can further reduce the computational burden. First, the imaging geometry and signal model of the GEO-UAV VHF UWB BiSAR are established, and the construction of the OEP coordinate system and the subaperture imaging method are proposed. Moreover, the Nyquist sampling requirements for the subimages in the OEP coordinate system are derived from the range error perspective, which can offer a near-optimum tradeoff between precision and efficiency. In addition, the superiority of the OEP coordinate system is analyzed, which demonstrates that the angular dimensional sampling rate of the subimages is significantly reduced. Finally, the implementation processes and computational burden of the proposed algorithm are provided, and the speed-up factor of the proposed FFBP algorithm compared with the BP algorithm is derived and discussed. Experimental results of ideal point targets and natural ocean scenes demonstrate the correctness and effectiveness of the proposed algorithm, which can achieve near-optimal imaging performance with a low computational burden. Full article
(This article belongs to the Special Issue Radar Signal Processing and Imaging for Ocean Remote Sensing)
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<p>Imaging geometry of the GEO-UAV BiSAR system.</p>
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<p>Subaperture imaging geometry of the GEO-UAV BiSAR in the orthogonal elliptical coordinate system. (<b>a</b>) The <span class="html-italic">k</span>th subaperture and subimage grid; (<b>b</b>) The <span class="html-italic">k</span>th OEP coordinate system.</p>
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<p>Subaperture imaging geometry of the GEO-UAV BiSAR in the orthogonal elliptical coordinate system. (<b>a</b>) The <span class="html-italic">k</span>th subaperture and subimage grid; (<b>b</b>) The <span class="html-italic">k</span>th OEP coordinate system.</p>
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<p>Plane geometry of the ellipse <math display="inline"><semantics> <mrow> <mi>E</mi> </mrow> </semantics></math>.</p>
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<p>Angular dimension sampling requirement of the subimages in the OEP system.</p>
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<p>Analysis of the angular dimension sampling requirement of the subimages in both EP and OEP systems for the same imaging scene.</p>
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<p>Two-dimensional (2D) spectrum comparison of the imaging result of the single ideal point target with the different subaperture lengths <span class="html-italic">n</span>. (<b>a</b>) Two-dimensional (2D) spectrum for <span class="html-italic">n</span> = 256 in the EP system; (<b>b</b>) Two-dimensional (2D) spectrum for <span class="html-italic">n</span> = 512 in the EP system; (<b>c</b>) Two-dimensional (2D) spectrum for <span class="html-italic">n</span> = 1024 in the EP system; (<b>d</b>) Two-dimensional (2D) spectrum for <span class="html-italic">n</span> = 256 in the OEP system; (<b>e</b>) Two-dimensional (2D) spectrum for <span class="html-italic">n</span> = 512 in the OEP system; (<b>f</b>) Two-dimensional (2D) spectrum for <span class="html-italic">n</span> = 1024 in the OEP system.</p>
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<p>Procedures of the proposed bistatic FFBP algorithm. (<b>a</b>) Diagram; (<b>b</b>) Flow chart.</p>
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<p>Variation of the speed-up factor. (<b>a</b>) With respect to the fusion time <span class="html-italic">M</span>; (<b>b</b>) With respect to the fusion aperture <span class="html-italic">n</span>.</p>
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<p>The experimental scene for the GEO-UAV UWB BiSAR imaging. (<b>a</b>) The imaging geometry; (<b>b</b>) The distribution of the point targets.</p>
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<p>Imaging results of the point targets. (<b>a</b>) Bistatic BP algorithm; (<b>b</b>) Bistatic EP FFBP algorithm; (<b>c</b>) Proposed bistatic FFBP algorithm.</p>
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<p>The counter plots of the impulse response of the selected point targets. (<b>a</b>) The target A focused by the bistatic BP algorithm; (<b>b</b>) The target A focused by the bistatic EP FFBP algorithm; (<b>c</b>) The target A focused by the proposed bistatic FFBP algorithm; (<b>d</b>) The target B focused by the bistatic BP algorithm; (<b>e</b>) The target B focused by the bistatic EP FFBP algorithm; (<b>f</b>) The target B focused by the proposed bistatic FFBP algorithm; (<b>g</b>) The target C focused by the bistatic BP algorithm; (<b>h</b>) The target C focused by the bistatic EP FFBP algorithm; (<b>i</b>) The target C focused by the proposed bistatic FFBP algorithm.</p>
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<p>The counter plots of the impulse response of the selected point targets. (<b>a</b>) The target A focused by the bistatic BP algorithm; (<b>b</b>) The target A focused by the bistatic EP FFBP algorithm; (<b>c</b>) The target A focused by the proposed bistatic FFBP algorithm; (<b>d</b>) The target B focused by the bistatic BP algorithm; (<b>e</b>) The target B focused by the bistatic EP FFBP algorithm; (<b>f</b>) The target B focused by the proposed bistatic FFBP algorithm; (<b>g</b>) The target C focused by the bistatic BP algorithm; (<b>h</b>) The target C focused by the bistatic EP FFBP algorithm; (<b>i</b>) The target C focused by the proposed bistatic FFBP algorithm.</p>
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<p>The profiles of the impulse response of the selected point targets. (<b>a</b>) Azimuthal profile of the target A; (<b>b</b>) Range profile of the target A; (<b>c</b>) Azimuthal profile of the target B; (<b>d</b>) Range profile of the target B; (<b>e</b>) Azimuthal profile of the target C; (<b>f</b>) Range profile of the target C.</p>
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<p>The natural ocean scene and its echo signal generated by the TBT algorithm for the GEO-UAV VHF UWB BiSAR imaging. (<b>a</b>) The natural ocean scene; (<b>b</b>) Amplitude of the echo signal; (<b>c</b>) Phase of the echo signal.</p>
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<p>Reconstructed SAR image obtained by the different algorithms. (<b>a</b>) The bistatic BP algorithm; (<b>b</b>) The bistatic EP FFBP algorithm; (<b>c</b>) The proposed bistatic FFBP algorithm.</p>
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<p>The selected ship targets and their profiles of the imaging results obtained by the different algorithms. (<b>a</b>) Ship target A; (<b>b</b>) Ship target B; (<b>c</b>) Ship target C; (<b>d</b>) Azimuthal profile of the ship target A; (<b>e</b>) Azimuthal profile of the ship target B; (<b>f</b>) Azimuthal profile of the ship target C; (<b>g</b>) Range profile of the ship target A; (<b>h</b>) Range profile of the ship target B; (<b>i</b>) Range profile of the ship target C.</p>
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13 pages, 5372 KiB  
Article
Flexible and Small Textile Antenna for UWB Wireless Body Area Network
by Peng Chen, Dan Wang and Zongsheng Gan
Micromachines 2023, 14(4), 718; https://doi.org/10.3390/mi14040718 - 24 Mar 2023
Cited by 11 | Viewed by 2183
Abstract
In this paper, a miniaturized textile microstrip antenna is proposed for wireless body area networks (WBAN). The ultra-wideband (UWB) antenna used a denim substrate to reduce the surface wave losses. The monopole antenna consists of a modified circular radiation patch and an asymmetric [...] Read more.
In this paper, a miniaturized textile microstrip antenna is proposed for wireless body area networks (WBAN). The ultra-wideband (UWB) antenna used a denim substrate to reduce the surface wave losses. The monopole antenna consists of a modified circular radiation patch and an asymmetric defected ground structure, which expands impedance bandwidth (BW) and improves the radiation patterns of the antenna with a small size of 20 × 30 × 1.4 mm3. An impedance BW of 110% (2.85–9.81 GHz) frequency boundaries was observed. Based on the measured results, a peak gain of 3.28 dBi was analyzed at 6 GHz. The SAR values were calculated to observe the radiation effects, and the SAR values obtained from the simulation at 4/6/8 GHz frequencies followed the FCC guideline. Compared to typical wearable miniaturized antennas, the antenna size is reduced by 62.5%. The proposed antenna has good performance and can be integrated on a peaked cap as a wearable antenna for indoor positioning systems. Full article
(This article belongs to the Special Issue Miniaturized Wearable Antennas)
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<p>Denim performance test equipment and DUT (<b>a</b>) equipment for coaxial ring method test (<b>b</b>) DUT.</p>
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<p>Measured permittivity and permeability.</p>
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<p>(<b>a</b>) Exploded view and (<b>b</b>) dimension parameters of the proposed antenna.</p>
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<p>S11 for various sizes of (<b>a</b>) <span class="html-italic">l</span><sub>1</sub> and (<b>b</b>) <span class="html-italic">l</span><sub>3</sub>.</p>
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<p>Simulated radiation pattern of textile antenna at 4 GHz, 6 GHz, and 8 GHz in the (<b>a</b>) xoz-plane and (<b>b</b>) yoz-plane.</p>
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<p>The current distribution of the UWB antenna with a phase of 0° at (<b>a</b>) 3.5 G and (<b>b</b>) 8.2 G.</p>
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<p>(<b>a</b>) Wearable antenna; (<b>b</b>) Antenna integrated into a peaked cap; (<b>c</b>) radiation pattern measured in free space; (<b>d</b>) human head model.</p>
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<p>Simulated and measured radiation pattern in the (<b>a</b>) xoz-plane and (<b>b</b>) yoz-plane at 6 GHz.</p>
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<p>Simulates and measures the return losses of the proposed antenna in free space and close to the human head.</p>
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<p>Comparison of simulated radiation patterns in free space and close to the human head at 6 GHz.</p>
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<p>Structural deformation (<b>a</b>) X-bend (<b>b</b>) Y-bend.</p>
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<p>The simulation and measurement of return loss after structural deformation.</p>
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<p>Simulated and measured radiation patterns after structural deformation in the (<b>a</b>) xoz-plane and (<b>b</b>) yoz-plane.</p>
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<p>SAR analysis (<b>a</b>) 4 GHz (<b>b</b>) 6 GHz (<b>c</b>) 8 GHz.</p>
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20 pages, 9436 KiB  
Article
Design of Ultra-Wideband Phased Array Applicator for Breast Cancer Hyperthermia Therapy
by Cheng Lyu, Wenxing Li, Si Li, Yunlong Mao and Bin Yang
Sensors 2023, 23(3), 1051; https://doi.org/10.3390/s23031051 - 17 Jan 2023
Cited by 5 | Viewed by 2216
Abstract
Focused microwave−hyperthermia therapy has recently emerged as a key technology in the treatment of breast cancer due to non−invasive treatment. An applicator of a three−ring phased array consisting of ultra−wideband (UWB) microstrip antennas was designed for breast cancer therapy and operates at 0.915 [...] Read more.
Focused microwave−hyperthermia therapy has recently emerged as a key technology in the treatment of breast cancer due to non−invasive treatment. An applicator of a three−ring phased array consisting of ultra−wideband (UWB) microstrip antennas was designed for breast cancer therapy and operates at 0.915 GHz and 2.45 GHz. The proposed antenna has an ultra−wideband from 0.7 GHz to 5.5 GHz with resonant frequencies of 0.915 GHz and 2.45 GHz and dimensions of 15 × 43.5 × 1.575 mm3. The number of each ring was chosen to be 12 based on the SAR distribution and the performance indicators of tumor off−center focusing results for four different numbers of single−ring arrays. The homogeneous breast model is applied to a three−ring phased array consisting of 36 elements for focused simulation, and 1 cm3 and 2 cm3 tumors are placed in three different locations in the breast. The simulation results show that the proposed phased array has good performance and the capability to raise the temperature of different volumes of breast cancer above 42.5 °C after choosing a suitable operating frequency. The proposed applicator allows for precise treatment of tumors by selecting the appropriate operating frequency based on the size of the malignant tumor. Full article
(This article belongs to the Section Physical Sensors)
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<p>Geometries of the proposed antenna. (<b>a</b>) Front view. (<b>b</b>) Back view. (<b>c</b>) Side view.</p>
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<p>Evolution steps of ellipse-monopole-antenna changes: (<b>a</b>) antenna I, (<b>b</b>) antenna II, (<b>c</b>) antenna III.</p>
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<p>The surface current distribution of the proposed antenna in three stages at 2.45 GHz: (<b>a</b>) antenna I, (<b>b</b>) antenna II, (<b>c</b>) antenna III.</p>
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<p>Comparison of the reflection coefficient of three evolution stages.</p>
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<p>Comparison of the reflection coefficient of different values of <math display="inline"><semantics> <mrow> <msub> <mi>W</mi> <mi>f</mi> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi>i</mi> </msub> </mrow> </semantics></math>, respectively. (<b>a</b>) S<sub>11</sub> of different <math display="inline"><semantics> <mrow> <msub> <mi>W</mi> <mi>f</mi> </msub> </mrow> </semantics></math> and (<b>b</b>) S<sub>11</sub> of different <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi>i</mi> </msub> </mrow> </semantics></math>.</p>
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<p>The dielectric properties of the emulsion−coupling medium were measured using an open−ended coaxial dielectric probe kit. (<b>a</b>) The front view of the fabricated antenna, (<b>b</b>) the back view of the fabricated antenna, and (<b>c</b>) the measurement of the fabricated antenna.</p>
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<p>The reflection coefficient measurement of four antennas.</p>
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<p>The realistic experimental setup of the FMHT modality.</p>
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<p>The layout of one−ring phased array configurations with a different number of antennas containing 8, 10, 12, and 14 elements, separately. The breast phantom includes chest, fat, skin, and tumor (30 mm away from the center).</p>
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<p>Normalized SAR distribution (W/kg) of vertical (XY plane) and horizontal (YZ plane) cross−sectional views of one−ring phased array containing 8, 10, 12, and 14 elements within an emulsion−coupling medium at 0.915 GHz (<b>a</b>–<b>d</b>) and 2.45 GHz (<b>e</b>–<b>h</b>), respectively.</p>
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<p>Normalized SAR distribution (W/kg) of vertical (XY plane) and horizontal (YZ plane) cross−sectional views of one−ring phased array containing 8, 10, 12, and 14 elements within an emulsion−coupling medium at 0.915 GHz (<b>a</b>–<b>d</b>) and 2.45 GHz (<b>e</b>–<b>h</b>), respectively.</p>
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<p>Influence of the number of antennas in one ring. aPA ratio and HTQ of four different numbers of antennas in one−ring phased array at 0.915 GHz and 2.45 GHz, respectively. (<b>a</b>) aPA ratio and HTQ of four one−ring phased arrays at 0.915 GHz. (<b>b</b>) aPA ratio and HTQ four one−ring phased arrays of 2.45 GHz.</p>
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<p>Illustration of the homogeneous breast model with tumors in three different locations and the proposed UWB phased array applicator. (<b>a</b>,<b>b</b>) Horizontal (XZ plane) and vertical (XY plane) views of the breast model (XY plane); (<b>c</b>,<b>d</b>) Horizontal (XZ plane) and vertical (XY plane) views of the three−ring phased array applicator containing a breast model with a tumor in the center of the breast.</p>
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<p>Side view of fabricated three−ring phased array applicator.</p>
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<p>Simulation results of S parameters of 36 elements in the three−ring antenna array. (<b>a</b>,<b>c</b>) Reflection coefficient (S<sub>nn</sub>) of the three−ring array without the breast model and with the breast model immersed in oil−in−water. (<b>b</b>,<b>d</b>) Mutual coupling (S<sub>mn</sub>) of two cases, separately.</p>
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<p>Simulation results of S parameters of 36 elements in the three−ring antenna array. (<b>a</b>,<b>c</b>) Reflection coefficient (S<sub>nn</sub>) of the three−ring array without the breast model and with the breast model immersed in oil−in−water. (<b>b</b>,<b>d</b>) Mutual coupling (S<sub>mn</sub>) of two cases, separately.</p>
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<p>Vertical (XY plane) and horizontal (YZ plane) cross−sectional views of SAR distribution (W/kg) for time−reversal focusing at the upper outer, center, and lower quadrants of the breast at 0.915 GHz and 2.45 GHz, respectively.</p>
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<p>Vertical (XY plane) and horizontal (YZ plane) cross−sectional views of SAR distribution (W/kg) for time−reversal focusing at the upper outer, center, and lower quadrants of the breast at 0.915 GHz and 2.45 GHz, respectively.</p>
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<p>Vertical (XY plane) and horizontal (YZ plane) cross−sectional views of temperature distribution (°C) for long breast phantom with 1 cm<sup>3</sup> (0.915 GHz) and 2 cm<sup>3</sup> (2.45 GHz) tumor at three different locations.</p>
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<p>(<b>a</b>–<b>c</b>) Performance configurations compared between different frequencies considering different tumor dimensions and positions.</p>
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24 pages, 10677 KiB  
Article
Complete Breast Cancer Detection and Monitoring System by Using Microwave Textile Based Antenna Sensors
by Dalia N. Elsheakh, Rawda A. Mohamed, Omar M. Fahmy, Khaled Ezzat and Angie R. Eldamak
Biosensors 2023, 13(1), 87; https://doi.org/10.3390/bios13010087 - 4 Jan 2023
Cited by 40 | Viewed by 6810
Abstract
This paper presents the development of a new complete wearable system for detecting breast tumors based on fully textile antenna-based sensors. The proposed sensor is compact and fully made of textiles so that it fits conformably and comfortably on the breasts with dimensions [...] Read more.
This paper presents the development of a new complete wearable system for detecting breast tumors based on fully textile antenna-based sensors. The proposed sensor is compact and fully made of textiles so that it fits conformably and comfortably on the breasts with dimensions of 24 × 45 × 0.17 mm3 on a cotton substrate. The proposed antenna sensor is fed with a coplanar waveguide feed for easy integration with other systems. It realizes impedance bandwidth from 1.6 GHz up to 10 GHz at |S11| ≤ −6 dB (VSWR ≤ 3) and from 1.8 to 2.4 GHz and from 4 up to 10 GHz at |S11| ≤ −10 dB (VSWR ≤ 2). The proposed sensor acquires a low specific absorption rate (SAR) of 0.55 W/kg and 0.25 W/kg at 1g and 10 g, respectively, at 25 dBm power level over the operating band. Furthermore, the proposed system utilizes machine-learning algorithms (MLA) to differentiate between malignant tumor and benign breast tissues. Simulation examples have been recorded to verify and validate machine-learning algorithms in detecting tumors at different sizes of 10 mm and 20 mm, respectively. The classification accuracy reached 100% on the tested dataset when considering |S21| parameter features. The proposed system is vision as a “Smart Bra” that is capable of providing an easy interface for women who require continuous breast monitoring in the comfort of their homes. Full article
(This article belongs to the Special Issue Paper-Based Biosensors)
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<p>The proposed breast cancer detection system as a “Smart Bra”.</p>
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<p>(<b>a</b>–<b>d</b>) The design steps of CPW-based monopole antenna and (<b>e</b>) final design of CPW-based monopole antenna.</p>
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<p>Breast and tumor models fabrication: (<b>a</b>) fabrication flow chart and (<b>b</b>) breast model with tumor cells in the middle.</p>
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<p>Measured electrical properties of breast phantom and tumor models versus frequency: (<b>a</b>) real part of dielectric constant (ε′) and (<b>b</b>) imaginary part of dielectric constant (ε″).</p>
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<p>Full measurement setup of (<b>a</b>) flexible Roger substrate and (<b>b</b>) textile-based antenna connected to SMA cable at one side and other side to VNA.</p>
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<p>SAR measurements of the proposed antenna-based sensor: (<b>a</b>) flexible Roger substrate and (<b>b</b>) conductive textile.</p>
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<p>SVM classifier: (<b>a</b>) Projection of data points to compute the distance to a hyperplane [<a href="#B46-biosensors-13-00087" class="html-bibr">46</a>]. (<b>b</b>) Illustration of the maximum margin between support vectors to separate between different classes [<a href="#B46-biosensors-13-00087" class="html-bibr">46</a>].</p>
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<p>Illustrated example of binary decision tree.</p>
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<p>Simulated reflection coefficient in dB versus frequency: (<b>a</b>) different stages of monopole antenna design shown in <a href="#biosensors-13-00087-f001" class="html-fig">Figure 1</a>; (<b>b</b>) proposed monopole using flexible Roger 3003 and conductive textile fabric.</p>
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<p>Simulation of proposed antenna-based sensor versus frequency using flexible Roger 3003 and conductive fabric: (<b>a</b>) real and imaginary part of impedance and (<b>b</b>) gain in dBi.</p>
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<p>Current distribution at different frequencies: (<b>a</b>) 2.5 GHz, (<b>b</b>) 5 GHz, (<b>c</b>) 7.5 GHz, and (<b>d</b>) 10 GHz.</p>
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<p>(<b>a</b>) Photo of fabricated antenna-based sensor using copper conductor tape and (<b>b</b>) measured and simulated reflection coefficient in dB versus frequency.</p>
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<p>(<b>a</b>) Photo of fabricated antenna-based sensor using fabric conductor and (<b>b</b>) measured and simulated reflection coefficient in dB versus frequency.</p>
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<p>The layers model of breast with and without tumor tested using (<b>a</b>) one antenna and (<b>b</b>) two antennas.</p>
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<p>Simulated|S<sub>11</sub>|of proposed monopole flexible Roger antenna with tumor (first scenario as shown in <a href="#biosensors-13-00087-f014" class="html-fig">Figure 14</a>a) at different sizes of tumor: (<b>a</b>) magnitude in dB and (<b>b</b>) phase in degrees.</p>
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<p>Simulated |S<sub>11</sub>| of proposed monopole textile antenna with and without tumor (second scenario shown in <a href="#biosensors-13-00087-f014" class="html-fig">Figure 14</a>b) at different sizes of tumor: (<b>a</b>) magnitude in dB and (<b>b</b>) phase in degrees.</p>
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<p>Simulated |S<sub>21</sub>| of proposed monopole antenna with and without tumor (second scenario shown in in <a href="#biosensors-13-00087-f014" class="html-fig">Figure 14</a>b) at different sizes of tumor: (<b>a</b>) |S<sub>21</sub>| magnitude in dB and (<b>b</b>) |S<sub>21</sub>|phase in degrees.</p>
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<p>Measured |S<sub>11</sub>| of flexible Roger substrate antenna performance with breast phantom and tumor: (<b>a</b>) magnitude and (<b>b</b>) phase.</p>
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<p>Measured |S<sub>11</sub>| of conductive fabric antenna performance with breast phantom and tumor: (<b>a</b>) magnitude and (<b>b</b>) phase.</p>
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<p>Measured S21 of conductive fabric antenna performance with breast phantom and tumor: (<b>a</b>) magnitude and (<b>b</b>) phase.</p>
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<p>Contribution of each feature parameter for the classification accuracy of the “CatBoost” algorithm (<b>a</b>) for first dataset of first scenario and (<b>b</b>) for second dataset of second scenario.</p>
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21 pages, 10002 KiB  
Article
Design and Analysis of a Flexible Smart Apparel MIMO Antenna for Bio-Healthcare Applications
by Thennarasi Govindan, Sandeep Kumar Palaniswamy, Malathi Kanagasabai, Sachin Kumar, Mohamed Marey and Hala Mostafa
Micromachines 2022, 13(11), 1919; https://doi.org/10.3390/mi13111919 - 6 Nov 2022
Cited by 17 | Viewed by 2254
Abstract
This paper presents the design and development of a quad-port smart textile antenna for bio-healthcare applications. The antenna is designed to operate in the ultra-wideband (UWB) spectrum (3.1–12 GHz) with an impedance bandwidth of 8.9 GHz. The size of the unit cell and [...] Read more.
This paper presents the design and development of a quad-port smart textile antenna for bio-healthcare applications. The antenna is designed to operate in the ultra-wideband (UWB) spectrum (3.1–12 GHz) with an impedance bandwidth of 8.9 GHz. The size of the unit cell and multiple-input multiple-output (MIMO) antenna are 0.25λ0 × 0.2λ0 × 0.015λ0 and 0.52λ0 × 0.52λ0 × 0.015λ0, respectively. The antenna has a maximum efficiency of 93% and a peak gain of 4.62 dBi. The investigation of diversity metrics is performed and the results obtained are found to be ECC < 0.08 and DG < 9.99 dB. The computed CCL and TARC values are <0.13 bits/s/Hz and <−12 dB, respectively. The SAR analysis of the antenna shows a value of 0.471 Watt/Kg at 4 GHz, 0.39 Watt/Kg at 7 GHz, and 0.22 Watt/Kg at 10 GHz. Full article
(This article belongs to the Special Issue Microwave Antennas: From Fundamental Research to Applications)
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<p>Antenna design: (<b>a</b>) front side, (<b>b</b>) back side.</p>
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<p>Evolution stages of the proposed antenna. (<b>a</b>) Evolution-1, (<b>b</b>) Evolution-2, (<b>c</b>) Evolution-3, (<b>d</b>) Evolution-4, and (<b>e</b>) Evolution-5.</p>
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<p>S<sub>11</sub> (dB) curves of the evolution stages.</p>
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<p>Parametric analysis of the antenna with varying ground plane width (GW). (<b>a</b>) GW = 18 mm, (<b>b</b>) GW = 17 mm, (<b>c</b>) GW = 16 mm, (<b>d</b>) GW = 15 mm, (<b>e</b>) 14 mm, (<b>f</b>) 13 mm.</p>
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<p>S<sub>11</sub> (dB) curves for different ground plane width (GW).</p>
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<p>Current distribution at (<b>a</b>) 4 GHz, (<b>b</b>) 10 GHz.</p>
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<p>S<sub>11</sub> (dB) curves of the designed antenna.</p>
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<p>MIMO antenna design.</p>
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<p>Fabricated MIMO antenna: (<b>a</b>) front side, (<b>b</b>) back side, (<b>c</b>) antenna measurement using VNA.</p>
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<p>Simulated and measured reflection coefficient plots of the MIMO antenna.</p>
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<p>Simulated and measured mutual coupling plots of the MIMO antenna.</p>
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<p>Gain and efficiency curves of the antenna.</p>
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<p>Radiation patterns of the antenna (gain in dBi and angle in degree). (<b>a</b>) 4 GHz; (<b>b</b>) 7 GHz; (<b>c</b>) 10 GHz.</p>
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<p>ECC and diversity gain plots of the MIMO antenna.</p>
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<p>TARC plots of the MIMO antenna.</p>
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<p>CCL plots of the MIMO antenna.</p>
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<p>Bending analysis of the antenna at three bending radii (<b>a</b>) <span class="html-italic">BR</span> = 25 mm, (<b>b</b>) <span class="html-italic">BR</span> = 20 mm, (<b>c</b>) <span class="html-italic">BR</span> = 15 mm.</p>
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<p>Bending analysis of the prototype antenna (<b>a</b>) <span class="html-italic">BR</span> = 25 mm, (<b>b</b>) <span class="html-italic">BR</span> = 20 mm, (<b>c</b>) <span class="html-italic">BR</span> = 15 mm.</p>
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<p>Reflection coefficients of the antenna at three bending radii (<b>a</b>) <span class="html-italic">BR</span> = 25 mm, (<b>b</b>) <span class="html-italic">BR</span> = 20 mm, (<b>c</b>) <span class="html-italic">BR</span> = 15 mm.</p>
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<p>Reflection coefficients of the antenna at three bending radii (<b>a</b>) <span class="html-italic">BR</span> = 25 mm, (<b>b</b>) <span class="html-italic">BR</span> = 20 mm, (<b>c</b>) <span class="html-italic">BR</span> = 15 mm.</p>
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<p>Transmission coefficients of the antenna at three bending radii (<b>a</b>) <span class="html-italic">BR</span> = 25 mm, (<b>b</b>) <span class="html-italic">BR</span> = 20 mm, (<b>c</b>) <span class="html-italic">BR</span> = 15 mm.</p>
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<p>Transmission coefficients of the antenna at three bending radii (<b>a</b>) <span class="html-italic">BR</span> = 25 mm, (<b>b</b>) <span class="html-italic">BR</span> = 20 mm, (<b>c</b>) <span class="html-italic">BR</span> = 15 mm.</p>
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<p>SAR analysis of the MIMO antenna (<b>a</b>) Simulated prototype, (<b>b</b>) SAR values, (<b>c</b>) Reflection coefficient curves.</p>
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<p>SAR analysis of the MIMO antenna (<b>a</b>) Simulated prototype, (<b>b</b>) SAR values, (<b>c</b>) Reflection coefficient curves.</p>
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<p>SAR analysis on an imported human body model (<b>a</b>) Chest, (<b>b</b>) Forearm, (<b>c</b>) Reflection coefficient curves.</p>
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<p>SAR analysis on an imported human body model (<b>a</b>) Chest, (<b>b</b>) Forearm, (<b>c</b>) Reflection coefficient curves.</p>
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<p>SAR analysis of the MIMO prototype antenna (<b>a</b>) VNA measurement, (<b>b</b>) Reflection coefficient curves.</p>
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<p>Reflection coefficient of SAR analysis of a MIMO prototype.</p>
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15 pages, 5174 KiB  
Article
A Novel Approach of a Low-Cost UWB Microwave Imaging System with High Resolution Based on SAR and a New Fast Reconstruction Algorithm for Early-Stage Breast Cancer Detection
by Ibtisam Amdaouch, Mohamed Saban, Jaouad El Gueri, Mohamed Zied Chaari, Ana Vazquez Alejos, Juan Ruiz Alzola, Alfredo Rosado Muñoz and Otman Aghzout
J. Imaging 2022, 8(10), 264; https://doi.org/10.3390/jimaging8100264 - 28 Sep 2022
Cited by 10 | Viewed by 3391
Abstract
In this article, a new efficient and robust approach—the high-resolution microwave imaging system—for early breast cancer diagnosis is presented. The core concept of the proposed approach is to employ a combination of a newly proposed delay-and-sum (DAS) algorithm and the specific absorption rate [...] Read more.
In this article, a new efficient and robust approach—the high-resolution microwave imaging system—for early breast cancer diagnosis is presented. The core concept of the proposed approach is to employ a combination of a newly proposed delay-and-sum (DAS) algorithm and the specific absorption rate (SAR) parameter to provide high image quality of breast tumors, along with fast image processing. The new algorithm enhances the tumor response by altering the parameter referring to the distance between the antenna and the tumor in the conventional DAS matrices. This adjustment entails a much clearer reconstructed image with short processing time. To achieve these aims, a high directional Vivaldi antenna is applied around a simulated hemispherical breast model with an embedded tumor. The detection of the tumor is carried out by calculating the maximum value of SAR inside the breast model. Consequently, the antenna position is relocated near the tumor region and is moved to nine positions in a trajectory path, leading to a shorter propagation distance in the image-creation process. At each position, the breast model is illuminated with short pulses of low power waves, and the back-scattered signals are recorded to produce a two-dimensional image of the scanned breast. Several simulations of testing scenarios for reconstruction imaging are investigated. These simulations involve different tumor sizes and materials. The influence of the number of antennas on the reconstructed images is also examined. Compared with the results from the conventional DAS, the proposed technique significantly improves the quality of the reconstructed images, and it detects and localizes the cancer inside the breast with high quality in a fast computing time, employing fewer antennas. Full article
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<p>The concept of the considered breast-imaging system.</p>
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<p>Breast imaging model set up.</p>
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<p>Geometrical structure of the antenna.</p>
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<p>Antenna covering nine positions around the breast using: (<b>a</b>) the traditional CMI and (<b>b</b>) the proposed approach.</p>
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<p>Process flow diagram of the novel approach.</p>
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<p>A representation of the monostatic approach.</p>
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<p>Backscattered responses with different tumor size at a predefined position of the breast model: (<b>a</b>) 1 mm, (<b>b</b>) 3 mm, (<b>c</b>) 5 mm. (<b>d</b>) represents a comparison between the responses with the size of 1 mm and the size of 5 mm in the frame of 1 ns.</p>
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<p>Reconstructed images of different tumor size: (<b>a</b>) 5 mm, (<b>b</b>) 3 mm, and (<b>c</b>) 1 mm.</p>
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<p>Reconstructed images of different tumor permittivity: (<b>a</b>) Tumor 1, (<b>b</b>) Tumor 2, (<b>c</b>) Tumor 3, and (<b>d</b>) Tumor 4.</p>
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<p>Reconstructed images of tumor for both methods using different number of antennas: (<b>a</b>) new approach; (<b>b</b>) traditional approach.</p>
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<p>Back-scattered responses at two antenna positions using the conventional method.</p>
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<p>Back-scattered responses at two antenna positions using the proposed method.</p>
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17 pages, 4210 KiB  
Article
Respiration Detection of Ground Injured Human Target Using UWB Radar Mounted on a Hovering UAV
by Yu Jing, Fugui Qi, Fang Yang, Yusen Cao, Mingming Zhu, Zhao Li, Tao Lei, Juanjuan Xia, Jianqi Wang and Guohua Lu
Drones 2022, 6(9), 235; https://doi.org/10.3390/drones6090235 - 3 Sep 2022
Cited by 12 | Viewed by 3421
Abstract
As an important and basic platform for remote life sensing, unmanned aerial vehicles (UAVs) may hide the vital signals of an injured human due to their own motion. In this work, a novel method to remove the platform motion and accurately extract human [...] Read more.
As an important and basic platform for remote life sensing, unmanned aerial vehicles (UAVs) may hide the vital signals of an injured human due to their own motion. In this work, a novel method to remove the platform motion and accurately extract human respiration is proposed. We utilized a hovering UAV as the platform of ultra-wideband (UWB) radar to capture human respiration. To remove interference from the moving UAV platform, we used the delay calculated by the correlation between each frame of UWB radar data in order to compensate for the range migration. Then, the echo signals from the human target were extracted as the observed multiple range channel signals. Owing to meeting the independent component analysis (ICA), we adopted ICA to estimate the signal of respiration. The results of respiration detection experiments conducted in two different outdoor scenarios show that our proposed method could accurately separate respiration of a ground human target without any additional sensor and prior knowledge; this physiological information will be essential for search and rescue (SAR) missions. Full article
(This article belongs to the Special Issue Conceptual Design, Modeling, and Control Strategies of Drones-II)
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<p>UAV-mounted UWB radar system for vital signal detection of ground injured human subject.</p>
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<p>Workflow of the UAV-carried UWB radar system.</p>
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<p>The block diagram of the radar signal processing.</p>
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<p>The problem of range migration. (<b>a</b>) Radar echo data with range migration. (<b>b</b>) Data after range migration compensation.</p>
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<p>Illustration of experimental settings for two scenarios. (<b>a</b>) Scenario 1 with smooth background, (<b>b</b>) scenario 2 with grassland background.</p>
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<p>Range profiles of a static subject. (<b>a</b>) Radar data without range migration compensation. (<b>b</b>) Radar data with range migration compensation.</p>
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<p>Observed signals extracted using the range sampler.</p>
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<p>Results of subject 1 in scenario 1. (<b>a</b>) Raw radar echo signal of subject 1 obtained by maximum energy method. (<b>b</b>) Reference respiration from respiratory belt. (<b>c</b>) Respiration extracted using our proposed method. (<b>d</b>) Respiration extracted using background residual method.</p>
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<p>Frequency spectrum of the signals in <a href="#drones-06-00235-f008" class="html-fig">Figure 8</a>. (<b>a</b>) FFT of raw radar signal. (<b>b</b>) FFT of respiration from respiratory belt. (<b>c</b>) FFT of respiration extracted by our proposed method. (<b>d</b>) FFT of respiration extracted using background residual method.</p>
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<p>Frequency spectrum of the signals in <a href="#drones-06-00235-f008" class="html-fig">Figure 8</a>. (<b>a</b>) FFT of raw radar signal. (<b>b</b>) FFT of respiration from respiratory belt. (<b>c</b>) FFT of respiration extracted by our proposed method. (<b>d</b>) FFT of respiration extracted using background residual method.</p>
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<p>Results of subject 1 in scenario 2. (<b>a</b>) Raw radar echo signal of subject 1 obtained using maximum energy method. (<b>b</b>) Reference respiration from respiratory belt. (<b>c</b>) Respiration extracted using our proposed method. (<b>d</b>) Respiration extracted using background residual method.</p>
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<p>Results of subject 1 in scenario 2. (<b>a</b>) Raw radar echo signal of subject 1 obtained using maximum energy method. (<b>b</b>) Reference respiration from respiratory belt. (<b>c</b>) Respiration extracted using our proposed method. (<b>d</b>) Respiration extracted using background residual method.</p>
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<p>Frequency spectrum of the signals in <a href="#drones-06-00235-f010" class="html-fig">Figure 10</a>. (<b>a</b>) FFT of raw radar signal. (<b>b</b>) FFT of respiration from respiratory belt. (<b>c</b>) FFT of respiration extracted using our proposed method. (<b>d</b>) FFT of respiration extracted using background residual method.</p>
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<p>Frequency spectrum of the signals in <a href="#drones-06-00235-f010" class="html-fig">Figure 10</a>. (<b>a</b>) FFT of raw radar signal. (<b>b</b>) FFT of respiration from respiratory belt. (<b>c</b>) FFT of respiration extracted using our proposed method. (<b>d</b>) FFT of respiration extracted using background residual method.</p>
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15 pages, 5348 KiB  
Article
A Miniaturized FSS-Based Eight-Element MIMO Antenna Array for Off/On-Body WBAN Telemetry Applications
by Muhammad Bilal, Sara Shahid, Yousuf Khan, Zahid Rauf, Raja A. Wagan, Muhammad A. Butt, Svetlana N. Khonina and Nikolay L. Kazanskiy
Electronics 2022, 11(4), 522; https://doi.org/10.3390/electronics11040522 - 10 Feb 2022
Cited by 12 | Viewed by 2699
Abstract
In this paper, a compact multiple-input multiple-output (MIMO) antenna for an off/on-body wireless body area network (WBAN) is presented. The proposed antenna comprises eight elements arranged in a side-by-side, orthogonal, and across configuration on a planar laminate. This MIMO system achieves wideband impedance [...] Read more.
In this paper, a compact multiple-input multiple-output (MIMO) antenna for an off/on-body wireless body area network (WBAN) is presented. The proposed antenna comprises eight elements arranged in a side-by-side, orthogonal, and across configuration on a planar laminate. This MIMO system achieves wideband impedance matching, i.e., fractional bandwidth (FBW) = 111% (7600 MHz) when placed off-body and FBW = 110% (7500 MHz) when placed on-body. The achieved bandwidth covers the ultrawideband (UWB) ranges 3.1–10.6 GHz for UWB-WBANs. To isolate the antenna elements, a Jerusalem cross (JC)-shaped frequency-selective surface (FSS) and meandered structure (MS) was designed and optimized. This proposed isolation mechanism offers at least 20 dB of isolation while maintaining an overall compact profile. Moreover, MIMO performance parameters for off/on-body and the specific absorption rate (SAR) were also evaluated. Stable MIMO performance, acceptable limits of SAR, and optimum radiation characteristics verify its suitability for wideband biotelemetry applications. Full article
(This article belongs to the Special Issue Numerical Electromagnetic Problems Involving Antennas)
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<p>Design methodology and fabrications: (<b>a</b>) step-by-step design evolution; (<b>b</b>) fabricated view (top = front side; bottom = back side).</p>
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<p>Design of proposed MIMO: (<b>a</b>) front view; (<b>b</b>) back view.</p>
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<p>FSS-based JC: (<b>a</b>) analysis; (<b>b</b>) parametric variation.</p>
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<p>Measurements of the proposed MIMO antenna array: (<b>a</b>) free space; (<b>b</b>) on-body.</p>
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<p>Simulated vs. measured S-parameters: (<b>a</b>) isolation; (<b>b</b>) return losses.</p>
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<p>J-surf: (<b>a</b>) 3.5 GHz; (<b>b</b>) 5 GHz.</p>
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<p>Radiation patterns: (<b>a</b>) E-plane; (<b>b</b>) H-plane.</p>
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<p>3D Radiation patterns: (<b>a</b>) 3.5 GHz; (<b>c</b>) 5 GHz; (<b>e</b>) 7.5 GHz; (<b>b</b>) 3.5 GHz OB; (<b>d</b>) 5 GHz OB; (<b>f</b>) 7.5 GHz OB.</p>
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<p>3D Radiation patterns of single antenna: (<b>a</b>) 3.5 GHz; (<b>b</b>) 5 GHz; (<b>c</b>) 7.5 GHz.</p>
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<p>MIMO performance parameters: (<b>a</b>) CCL; (<b>b</b>) TARC; (<b>c</b>) ECC; (<b>d</b>) DG.</p>
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<p>Simulations vs. measurements: (<b>a</b>) gain; (<b>b</b>) efficiency.</p>
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<p>SAR analysis: (<b>a</b>,<b>b</b>) ribcage at 3.5 GHz and 5 GHz; (<b>c</b>,<b>d</b>) arm at 3.5 GHz and 5 GHz; (<b>e</b>,<b>f</b>) leg at 3.5 GHz and 5 GHz.</p>
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<p>SAR analysis: (<b>a</b>,<b>b</b>) ribcage at 3.5 GHz and 5 GHz; (<b>c</b>,<b>d</b>) arm at 3.5 GHz and 5 GHz; (<b>e</b>,<b>f</b>) leg at 3.5 GHz and 5 GHz.</p>
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