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16 pages, 1439 KiB  
Review
Automaticity of the Pulmonary Vein Myocardium and the Effect of Class I Antiarrhythmic Drugs
by Iyuki Namekata, Maika Seki, Taro Saito, Ryosuke Odaka, Shogo Hamaguchi and Hikaru Tanaka
Int. J. Mol. Sci. 2024, 25(22), 12367; https://doi.org/10.3390/ijms252212367 - 18 Nov 2024
Viewed by 335
Abstract
The pulmonary vein wall contains a myocardial layer whose ectopic automaticity is the major cause of atrial fibrillation. This review summarizes the results obtained in isolated pulmonary vein myocardium from small experimental animals, focusing on the studies with the guinea pig. The diversity [...] Read more.
The pulmonary vein wall contains a myocardial layer whose ectopic automaticity is the major cause of atrial fibrillation. This review summarizes the results obtained in isolated pulmonary vein myocardium from small experimental animals, focusing on the studies with the guinea pig. The diversity in the action potential waveform reflects the difference in the repolarizing potassium channel currents involved. The diastolic depolarization, the trigger of automatic action potentials, is caused by multiple membrane currents, including the Na+-Ca2+ exchanger current and late INa. The action potential waveform and automaticity are affected differentially by α- and β-adrenoceptor stimulation. Class I antiarrhythmic drugs block the propagation of ectopic electrical activity of the pulmonary vein myocardium through blockade of the peak INa. Some of the class I antiarrhythmic drugs block the late INa and inhibit pulmonary vein automaticity. The negative inotropic and chronotropic effects of class I antiarrhythmic drugs could be largely attributed to their blocking effect on the Ca2+ channel rather than the Na+ channel. Such a comprehensive understanding of pulmonary vein automaticity and class I antiarrhythmic drugs would lead to an improvement in pharmacotherapy and the development of novel therapeutic agents for atrial fibrillation. Full article
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<p>Automatic electrical activity of the pulmonary vein myocardium. (<b>A</b>) Spontaneous action potential recording from the guinea pig showing a diastolic depolarization. (<b>B</b>) Continuous firing in the guinea pig. (<b>C</b>) Repetitive burst-type firing in the rat elicited by the application of 1 μM noradrenaline.</p>
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<p>A simplified schematic diagram of the action potential configuration and the underlying ionic currents in different species. (<b>A</b>) Human, pig, dog, and rabbit. (<b>B</b>) Guinea pig. (<b>C</b>) Rat and mouse.</p>
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<p>A scheme for the automatic electrical activity of the pulmonary vein myocardium. The forward-mode Na<sup>+</sup>-Ca<sup>2+</sup> exchanger and the persistent component of the Na<sup>+</sup> channel current (late I<sub>Na</sub>) depolarize the cell membrane and generate diastolic depolarization (arrows). SR: sarcoplasmic reticulum.</p>
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<p>Effect of class I antiarrhythmic drugs pilsicainide and aprindine on the automatic activity of the guinea pig pulmonary vein myocardium and the persistent Na<sup>+</sup> channel current (late I<sub>Na</sub>) in isolated cardiomyocytes. (<b>A</b>) Pilsicainide affected neither the action potential (<b>a</b>–<b>c</b>) nor the late I<sub>Na</sub> (<b>d</b>). (<b>B</b>) Aprindine reduced the firing rate of action potentials (<b>a</b>–<b>c</b>) and blocked the late I<sub>Na</sub> (<b>d</b>). The action potential recordings were made before (<b>a</b>) and 3 min after (<b>b</b>) the application of 10 μM of the drugs. Expanded traces of the diastolic depolarization phase before (black) and after (red) drug application were overlaid (<b>c</b>). The current–voltage relationship for late I<sub>Na</sub> under various drug concentrations was displayed (<b>d</b>). This figure was adopted from Ref. [<a href="#B84-ijms-25-12367" class="html-bibr">84</a>].</p>
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28 pages, 31167 KiB  
Article
Optimizing GEDI Canopy Height Estimation and Analyzing Error Impact Factors Under Highly Complex Terrain and High-Density Vegetation Conditions
by Runbo Chen, Xinchuang Wang, Xuejie Liu and Shunzhong Wang
Forests 2024, 15(11), 2024; https://doi.org/10.3390/f15112024 - 17 Nov 2024
Viewed by 633
Abstract
The Global Ecosystem Dynamics Investigation (GEDI) system provides essential data for estimating forest canopy height on a global scale. However, factors such as complex topography and dense canopy can significantly reduce the accuracy of GEDI canopy height estimations. We selected the South Taihang [...] Read more.
The Global Ecosystem Dynamics Investigation (GEDI) system provides essential data for estimating forest canopy height on a global scale. However, factors such as complex topography and dense canopy can significantly reduce the accuracy of GEDI canopy height estimations. We selected the South Taihang region of Henan Province, China, as our study area and proposed an optimization framework to improve GEDI canopy height estimation accuracy. This framework includes correcting geolocation errors in GEDI footprints, screening and analyzing features that affect estimation errors, and combining two regression models with feature selection methods. Our findings reveal a geolocation error of 4 to 6 m in GEDI footprints at the orbital scale, along with an overestimation of GEDI canopy height in the South Taihang region. Relative height (RH), waveform characteristics, topographic features, and canopy cover significantly influenced the estimation error. Some studies have suggested that GEDI canopy height estimates for areas with high canopy cover lead to underestimation, However, our study found that accuracy increased with higher canopy cover in complex terrain and dense vegetation. The model’s performance improved significantly after incorporating the canopy cover parameter into the optimization model. Overall, the R2 of the best-optimized model was improved from 0.06 to 0.61, the RMSE was decreased from 8.73 m to 2.23 m, and the rRMSE decreased from 65% to 17%, resulting in an accuracy improvement of 74.45%. In general, this study reveals the factors affecting the accuracy of GEDI canopy height estimation in areas with complex terrain and dense vegetation cover, on the premise of minimizing GEDI geolocation errors. Employing the proposed optimization framework significantly enhanced the accuracy of GEDI canopy height estimates. This study also highlighted the crucial role of canopy cover in improving the precision of GEDI canopy height estimation, providing an effective approach for forest monitoring in such regions and vegetation conditions. Future studies should further improve the classification of tree species and expand the diversity of sample tree species to test the accuracy of canopy height estimated by GEDI in different forest structures, consider the distortion of optical remote sensing images caused by rugged terrain, and further mine the information in GEDI waveforms so as to enhance the applicability of the optimization framework in more diverse forest environments. Full article
(This article belongs to the Section Forest Inventory, Modeling and Remote Sensing)
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<p>In the figure, (<b>a</b>) shows the location of Henan Province in China, (<b>b</b>) illustrates the study area’s location within Henan Province, and (<b>c</b>) presents the DEM of the study area, with each individual area number corresponding to the ALS aerial flight areas.</p>
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<p>CHM raster maps based on ALS acquisition: bottom images are true color images of Sentinel-2 in May 2023; black dots are GEDI footprints.</p>
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<p>The distribution of slope and canopy cover within the aerial flight zone after cropping based on ALS slope and canopy cover raster maps. Panel (<b>a</b>) shows the slope distribution following the cropping of the ALS airspace slope raster map using the extent of forested land from the Land Use Survey. Panel (<b>b</b>) shows the slope distribution across ALS airspace. Panels (<b>c</b>,<b>d</b>) show the canopy cover, where the vertical axis represents the number of raster pixels and the horizontal axis indicates the canopy cover (0-1).</p>
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<p>A square fishing net with a length and width of 5 m was used to calculate statistics of the DEM and slope within each grid, and the mean value, range, standard deviation, and mean slope of the DEM were calculated. Due to the huge amount of data, the data of all grids were not counted, but 5000 grids were randomly selected in each ALS region for statistics. The change from blue to red means the density goes from small to large.</p>
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<p>The principle of geolocation error correction is illustrated as follows: (<b>a</b>) displays the displacement mode of the footprint, where the red circle in the center represents the original GEDI location, and the cyan spot indicates the position after displacement. The angular step is set at 30°, while the distance step is 2 m. (<b>b</b>) shows the waveform corresponding to the GEDI location. (<b>c</b>) depicts the simulated waveform from ALS, and (<b>d</b>) presents the aligned GEDI waveform and ALS simulated waveform.</p>
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<p>Overall frame flowchart.</p>
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<p>The effect of geolocation error correction for a single footprint. Toploc and botloc refer to the start and end positions of the signal, respectively. Panels (<b>a</b>,<b>b</b>) display the original and corrected geolocation waveforms of the complex footprint, while panels (<b>c</b>,<b>d</b>) show the original and corrected geolocation waveforms of the simple footprint.</p>
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<p>The statistics of all R averages after displacing footprints to the same location for the same acquisition date. Each polar plot represents the average correction effect of geolocation errors for all footprints corresponding to the same acquisition date. The top label of each polar plot indicates the data acquisition date in the format YYYYDDD.</p>
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<p>R-values between individual features and GEDI canopy height estimation error, All feature parameters in the figure are significantly correlated (<math display="inline"><semantics> <mrow> <mi>p</mi> <mo>≤</mo> <mn>0.05</mn> </mrow> </semantics></math>), with a positive correlation in blue and a negative correlation in orange.</p>
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<p>Box plots of error distribution in different intervals of each feature with the absolute value of R above 0.3. The left vertical axis is the error (m) and the right vertical axis is the RMSE (m) of RH96 and CHM96.</p>
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<p>This figure shows the importance of each feature parameter with respect to the residuals: the upper figure shows the top 30 feature parameters in terms of importance, and the lower figure shows the thumbnail of the importance distribution of all feature parameters, where the blue part is the detailed distribution of the importance of the top 30 features in the upper figure.</p>
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<p>Box plots of error distribution in different intervals of each feature with the absolute value of RF importance above 1%. The left vertical axis is error (m) and the right vertical axis is the RMSE (m) of RH_96 and CHM_96.</p>
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<p>In the case of selecting different numbers of features, the model effects of various combinations of regression models and feature extraction methods are presented. The results are organized in the vertical coordinates from top to bottom in the order of <math display="inline"><semantics> <msup> <mi>R</mi> <mn>2</mn> </msup> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>M</mi> <mi>S</mi> <mi>E</mi> </mrow> </semantics></math> (m), and <math display="inline"><semantics> <mrow> <mi>r</mi> <mi>R</mi> <mi>M</mi> <mi>S</mi> <mi>E</mi> </mrow> </semantics></math> (%). The horizontal coordinates indicate the number of feature parameters used in the model.</p>
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<p>The left and right panels show the data distribution of RH_96 and RHT_96 with CHM96, respectively.</p>
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<p>The upper panel is a localized thumbnail of the remote sensing image, the blue part is the non-shadowed area, the white part is the shadowed area, and the lower two panels are the reflectance distributions of the red, green, and blue bands in the shadowed and non-shadow areas, respectively.</p>
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20 pages, 1589 KiB  
Article
Pseudo-Labeling and Time-Series Data Analysis Model for Device Status Diagnostics in Smart Agriculture
by Minwoo Jung and Dae-Young Kim
Appl. Sci. 2024, 14(22), 10371; https://doi.org/10.3390/app142210371 - 11 Nov 2024
Viewed by 593
Abstract
This study proposes an automated data-labeling model that combines a pseudo-labeling algorithm with waveform segmentation based on Long Short-Term Memory (LSTM) to effectively label time-series data in smart agriculture. This model aims to address the inefficiency of manual labeling for large-scale data generated [...] Read more.
This study proposes an automated data-labeling model that combines a pseudo-labeling algorithm with waveform segmentation based on Long Short-Term Memory (LSTM) to effectively label time-series data in smart agriculture. This model aims to address the inefficiency of manual labeling for large-scale data generated by agricultural systems, enhancing the performance and scalability of predictive models. Our proposed method leverages key features of time-series data to automatically generate labels for new data, thereby improving model accuracy and streamlining data processing. By automating the labeling process, we reduce dependence on manual labeling, which is often labor-intensive and prone to errors in large datasets. This approach enables the efficient preparation of labeled data for applications such as anomaly detection, pattern recognition, and predictive modeling in smart agriculture. Experimental results demonstrate that the automated labeling model achieves 89% accuracy in agricultural environments and reduces data processing time by 30%. Future research will focus on extending the model’s applicability to diverse agricultural settings, enhancing generalization performance, and improving real-time processing capabilities, thereby advancing intelligent and sustainable smart agriculture systems. Full article
(This article belongs to the Special Issue New Development in Smart Farming for Sustainable Agriculture)
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<p>Intent-based IoT platform.</p>
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<p>Semantic segmentation of time-series data.</p>
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<p>Data normalization of time-series data.</p>
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<p>Neural network architecture.</p>
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<p>Experimental data collection environment.</p>
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<p>Smart farm system for performance evaluation.</p>
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<p>Results of state classification.</p>
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<p>Semantic segmentation of time-series data.</p>
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<p>Confusion matrix for model performance.</p>
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<p>Ground truth and prediction for semantic segmentation.</p>
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15 pages, 3092 KiB  
Article
Reliable Augmentation and Precise Identification of EPG Waveforms Based on Multi-Criteria DCGAN
by Xiangzeng Kong, Chuxin Wang, Lintong Zhang, Wenqing Zhang, Shimiao Chen, Haiyong Weng, Nana Hu, Tingting Zhang and Fangfang Qu
Appl. Sci. 2024, 14(22), 10127; https://doi.org/10.3390/app142210127 - 5 Nov 2024
Viewed by 533
Abstract
The electrical penetration graph (EPG) technique is of great significance in elucidating the mechanisms of virus transmission by piercing-sucking insects and crop resistance to these insects. The traditional method of manually processing EPG signals encounters the drawbacks of inefficiency and subjectivity. This study [...] Read more.
The electrical penetration graph (EPG) technique is of great significance in elucidating the mechanisms of virus transmission by piercing-sucking insects and crop resistance to these insects. The traditional method of manually processing EPG signals encounters the drawbacks of inefficiency and subjectivity. This study investigated the data augmentation and automatic identification of various EPG signals, including A, B, C, PD, E1, E2, and G, which correspond to distinct behaviors exhibited by the Asian citrus psyllid. Specifically, a data augmentation method based on an improved deep convolutional generative adversarial network (DCGAN) was proposed to address the challenge of insufficient E1 waveforms. A multi-criteria evaluation framework was constructed, leveraging maximum mean discrepancy (MMD) to evaluate the similarity between the generated and real data, and singular value decomposition (SVD) was incorporated to optimize the training iterations of DCGAN and ensure data diversity. Four models, convolutional neural network (CNN), K-nearest neighbors (KNN), decision tree (DT), and support vector machine (SVM), were established based on DCGAN to classify the EPG waveforms. The results showed that the parameter-optimized DCGAN strategy significantly improved the model accuracies by 5.8%, 6.9%, 7.1%, and 7.9% for DT, SVM, KNN, and CNN, respectively. Notably, DCGAN-CNN effectively addressed the skewed distribution of EPG waveforms, achieving an optimal classification accuracy of 94.13%. The multi-criteria optimized DCGAN-CNN model proposed in this study enables reliable augmentation and precise automatic identification of EPG waveforms, holding significant practical implications for understanding psyllid behavior and controlling citrus huanglongbing. Full article
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<p>Schematic diagram of EPG data collection.</p>
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<p>DCGAN Network Framework.</p>
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<p>The SVD graphs of DCGAN with different Epoch values: (<b>a</b>) Epoch = 500, (<b>b</b>) Epoch = 1000, (<b>c</b>) Epoch = 2000, and (<b>d</b>) Epoch = 4000.</p>
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<p>Generated E1 waveform: (<b>a</b>) E1-1, (<b>b</b>) E1-2, (<b>c</b>) E1-3, and (<b>d</b>) E1-4.</p>
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<p>ROC curves of four models for classification of EPG waveforms: (<b>a</b>) KNN, (<b>b</b>) SVM, (<b>c</b>) CNN, and (<b>d</b>) DT.</p>
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26 pages, 2769 KiB  
Article
Evaluating AI Methods for Pulse Oximetry: Performance, Clinical Accuracy, and Comprehensive Bias Analysis
by Ana María Cabanas, Nicolás Sáez, Patricio O. Collao-Caiconte, Pilar Martín-Escudero, Josué Pagán, Elena Jiménez-Herranz and José L. Ayala
Bioengineering 2024, 11(11), 1061; https://doi.org/10.3390/bioengineering11111061 - 24 Oct 2024
Viewed by 956
Abstract
Blood oxygen saturation (SpO2) is vital for patient monitoring, particularly in clinical settings. Traditional SpO2 estimation methods have limitations, which can be addressed by analyzing photoplethysmography (PPG) signals with artificial intelligence (AI) techniques. This systematic review, following PRISMA guidelines, analyzed [...] Read more.
Blood oxygen saturation (SpO2) is vital for patient monitoring, particularly in clinical settings. Traditional SpO2 estimation methods have limitations, which can be addressed by analyzing photoplethysmography (PPG) signals with artificial intelligence (AI) techniques. This systematic review, following PRISMA guidelines, analyzed 183 unique references from WOS, PubMed, and Scopus, with 26 studies meeting the inclusion criteria. The review examined AI models, key features, oximeters used, datasets, tested saturation intervals, and performance metrics while also assessing bias through the QUADAS-2 criteria. Linear regression models and deep neural networks (DNNs) emerged as the leading AI methodologies, utilizing features such as statistical metrics, signal-to-noise ratios, and intricate waveform morphology to enhance accuracy. Gaussian Process models, in particular, exhibited superior performance, achieving Mean Absolute Error (MAE) values as low as 0.57% and Root Mean Square Error (RMSE) as low as 0.69%. The bias analysis highlighted the need for better patient selection, reliable reference standards, and comprehensive SpO2 intervals to improve model generalizability. A persistent challenge is the reliance on non-invasive methods over the more accurate arterial blood gas analysis and the limited datasets representing diverse physiological conditions. Future research must focus on improving reference standards, test protocols, and addressing ethical considerations in clinical trials. Integrating AI with traditional physiological models can further enhance SpO2 estimation accuracy and robustness, offering significant advancements in patient care. Full article
(This article belongs to the Special Issue Machine Learning and Deep Learning Applications in Healthcare)
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Graphical abstract
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<p>PPG signals captured at two wavelengths (red and infrared). The ratio of ratios (R) is calculated from the red (PPG Red) and infrared (PPG IR) signals. In this example, an R value of 0.50 results in an estimated SpO<sub>2</sub> of 97.7%.</p>
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<p>Flowchart following the PRISMA guidelines for systematic reviews.</p>
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<p>Overview of AI models used for SpO<sub>2</sub> estimation, classified into categories based on scikit-learn’s framework of supervised learning models.</p>
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<p>Distribution of AI models used in SpO<sub>2</sub> estimation across three categories: Linear Models (LMs), Ensemble Models (EMs), and Neural Network Models (NNMs).</p>
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<p>Boxplot illustrating the distribution of Mean Absolute Error (MAE) percentages across various AI model categories used for SpO<sub>2</sub> estimation from PPG signals.</p>
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<p>Boxplot illustrating the distribution of Root Mean Square Error (RMSE) percentages across various AI model categories used for SpO<sub>2</sub> estimation from PPG signals.</p>
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<p>Risk of bias assessment in individual studies judged according to QUADAS2 [<a href="#B22-bioengineering-11-01061" class="html-bibr">22</a>,<a href="#B23-bioengineering-11-01061" class="html-bibr">23</a>,<a href="#B25-bioengineering-11-01061" class="html-bibr">25</a>,<a href="#B31-bioengineering-11-01061" class="html-bibr">31</a>,<a href="#B42-bioengineering-11-01061" class="html-bibr">42</a>,<a href="#B43-bioengineering-11-01061" class="html-bibr">43</a>,<a href="#B44-bioengineering-11-01061" class="html-bibr">44</a>,<a href="#B45-bioengineering-11-01061" class="html-bibr">45</a>,<a href="#B46-bioengineering-11-01061" class="html-bibr">46</a>,<a href="#B47-bioengineering-11-01061" class="html-bibr">47</a>,<a href="#B48-bioengineering-11-01061" class="html-bibr">48</a>,<a href="#B49-bioengineering-11-01061" class="html-bibr">49</a>,<a href="#B50-bioengineering-11-01061" class="html-bibr">50</a>,<a href="#B51-bioengineering-11-01061" class="html-bibr">51</a>,<a href="#B52-bioengineering-11-01061" class="html-bibr">52</a>,<a href="#B53-bioengineering-11-01061" class="html-bibr">53</a>,<a href="#B54-bioengineering-11-01061" class="html-bibr">54</a>,<a href="#B55-bioengineering-11-01061" class="html-bibr">55</a>,<a href="#B56-bioengineering-11-01061" class="html-bibr">56</a>,<a href="#B57-bioengineering-11-01061" class="html-bibr">57</a>,<a href="#B58-bioengineering-11-01061" class="html-bibr">58</a>,<a href="#B59-bioengineering-11-01061" class="html-bibr">59</a>,<a href="#B60-bioengineering-11-01061" class="html-bibr">60</a>,<a href="#B61-bioengineering-11-01061" class="html-bibr">61</a>,<a href="#B62-bioengineering-11-01061" class="html-bibr">62</a>,<a href="#B63-bioengineering-11-01061" class="html-bibr">63</a>].</p>
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20 pages, 16040 KiB  
Article
Unveiling Anomalies in Terrain Elevation Products from Spaceborne Full-Waveform LiDAR over Forested Areas
by Hailan Jiang, Yi Li, Guangjian Yan, Weihua Li, Linyuan Li, Feng Yang, Anxin Ding, Donghui Xie, Xihan Mu, Jing Li, Kaijian Xu, Ping Zhao, Jun Geng and Felix Morsdorf
Forests 2024, 15(10), 1821; https://doi.org/10.3390/f15101821 - 17 Oct 2024
Viewed by 716
Abstract
Anomalies displaying significant deviations between terrain elevation products acquired from spaceborne full-waveform LiDAR and reference elevations are frequently observed in assessment studies. While the predominant focus is on “normal” data, recognizing anomalies within datasets obtained from the Geoscience Laser Altimeter System (GLAS) and [...] Read more.
Anomalies displaying significant deviations between terrain elevation products acquired from spaceborne full-waveform LiDAR and reference elevations are frequently observed in assessment studies. While the predominant focus is on “normal” data, recognizing anomalies within datasets obtained from the Geoscience Laser Altimeter System (GLAS) and the Global Ecosystem Dynamics Investigation (GEDI) is essential for a comprehensive understanding of widely used spaceborne full-waveform data, which not only facilitates optimal data utilization but also enhances the exploration of potential applications. Nevertheless, our comprehension of anomalies remains limited as they have received scant specific attention. Diverging from prevalent practices of directly eliminating outliers, we conducted a targeted exploration of anomalies in forested areas using both transmitted and return waveforms from the GLAS and the GEDI in conjunction with airborne LiDAR point cloud data. We unveiled that elevation anomalies stem not from the transmitted pulses or product algorithms, but rather from scattering sources. We further observed similarities between the GLAS and the GEDI despite their considerable disparities in sensor parameters, with the waveforms characterized by a low signal-to-noise ratio and a near exponential decay in return energy; specifically, return signals of anomalies originated from clouds rather than the land surface. This discovery underscores the potential of deriving cloud-top height from spaceborne full-waveform LiDAR missions, particularly the GEDI, suggesting promising prospects for applying GEDI data in atmospheric science—an area that has received scant attention thus far. To mitigate the impact of abnormal return waveforms on diverse land surface studies, we strongly recommend incorporating spaceborne LiDAR-offered terrain elevation in data filtering by establishing an elevation-difference threshold against a reference elevation. This is especially vital for studies concerning forest parameters due to potential cloud interference, yet a consensus has not been reached within the community. Full article
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<p>Study area and the geolocation of GLAS and GEDI data.</p>
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<p>Flowchart of this study.</p>
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<p>Spatial distribution of terrain elevation anomalies in the GLAS and GEDI datasets.</p>
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<p>Scatter plot of terrain elevation estimates obtained from GLAS (<b>a</b>) and GEDI (<b>b</b>) vs. the terrain elevation derived from airborne laser scanning (ALS) as a reference. A0 denotes the default algorithm of the GEDI L2A product.</p>
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<p>Details of terrain elevation outliers from GLAS: scatter plot of terrain elevation from data acquired during nighttime (<b>a</b>) and daytime (<b>b</b>) before removing outliers, scatter plot (<b>c</b>), transmitted waveforms (<b>d</b>), the histogram of the data acquisition time (<b>e</b>), and the histogram of Signal-to-Noise Ratio (SNR) (<b>f</b>) of source laser shot of the outliers.</p>
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<p>Details of terrain elevation outliers from GEDI: scatter plot of terrain elevation from data acquired during nighttime (<b>a</b>) and daytime (<b>b</b>) before removing outliers, scatter plot (<b>c</b>), transmitted waveforms (<b>d</b>), the histogram (<b>e</b>) of the beam type (<b>e1</b>) and data acquisition time (<b>e2</b>), and the histogram of sensitivity (<b>f</b>) of source laser shot of the outliers.</p>
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<p>Examples with small (upper panel) and large (lower panel) terrain elevation error: the three-dimensional scene (<b>left</b>), the transmitted waveform (<b>middle</b>), and the return waveform (<b>right</b>) of GLAS and GEDI with the terrain elevation from product and airborne laser scanning (ALS) data illustrated. In the lower panel (<b>right</b>), the ALS terrain elevation is not indicated since the GLAS or GEDI terrain elevation exceeds ALS by more than 330 m (see outlier-27 and outlier-12 indicated in green circles in <a href="#forests-15-01821-f005" class="html-fig">Figure 5</a> and <a href="#forests-15-01821-f006" class="html-fig">Figure 6</a>c). A&lt;<span class="html-italic">n</span>&gt; (<span class="html-italic">n</span>: 1–6) denotes the terrain elevation from six different algorithm groups of GEDI.</p>
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<p>Scatter plot of canopy height estimates for laser shots of terrain elevation anomalies obtained from GEDI L2A product versus the canopy height derived from airborne laser scanning (ALS) as a reference (the legend of the point density applies to all the figures). A0 denotes the default algorithm (<b>a</b>), and A&lt;<span class="html-italic">n</span>&gt; (<span class="html-italic">n</span>: 1–6) denotes the other six algorithm groups (<b>b</b>–<b>g</b>).</p>
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<p>Probability density of “sensitivity” of “power” and “coverage” beams estimated by different algorithms (<b>a</b>–<b>f</b>) of GEDI using the data with “sensitivity &gt; 0.90” in all footprints. A0 denotes the default algorithm setting (<b>a</b>), and A&lt;n&gt; (n: 1–6) denotes the other six algorithm groups (<b>b</b>–<b>g</b>).</p>
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<p>Original GLAS (<b>upper panel</b>) and GEDI (<b>lower panel</b>) waveform examples of terrain elevation anomalies with terrain elevation provided by GLAS and GEDI product indicated. A0 denotes the default algorithm, and A&lt;<span class="html-italic">n</span>&gt; (<span class="html-italic">n</span>: 1–6) denotes the other six algorithm groups of GEDI.</p>
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24 pages, 2630 KiB  
Article
The Research of Intra-Pulse Modulated Signal Recognition of Radar Emitter under Few-Shot Learning Condition Based on Multimodal Fusion
by Yunhao Liu, Sicun Han, Chengjun Guo, Jiangyan Chen and Qing Zhao
Electronics 2024, 13(20), 4045; https://doi.org/10.3390/electronics13204045 - 14 Oct 2024
Viewed by 827
Abstract
Radar radiation source recognition is critical for the reliable operation of radar communication systems. However, in increasingly complex electromagnetic environments, traditional identification methods face significant limitations. These methods often struggle with high noise levels and diverse modulation types, making it difficult to maintain [...] Read more.
Radar radiation source recognition is critical for the reliable operation of radar communication systems. However, in increasingly complex electromagnetic environments, traditional identification methods face significant limitations. These methods often struggle with high noise levels and diverse modulation types, making it difficult to maintain accuracy, especially when the Signal-to-Noise Ratio (SNR) is low or the available training data are limited. These difficulties are further intensified by the necessity to generalize in environments characterized by a substantial quantity of noisy, low-quality signal samples while being constrained by a limited number of desirable high-quality training samples. To more effectively address these issues, this paper proposes a novel approach utilizing Model-Agnostic Meta-Learning (MAML) to enhance model adaptability in few-shot learning scenarios, allowing the model to quickly learn with limited data and optimize parameters effectively. Furthermore, a multimodal fusion neural network, DCFANet, is designed, incorporating residual blocks, squeeze and excitation blocks, and a multi-scale CNN, to fuse I/Q waveform data and time–frequency image data for more comprehensive feature extraction. Our model enables more robust signal recognition, even when the signal quality is severely degraded by noise or when only a few examples of a signal type are available. Testing on 13 intra-pulse modulated signals in an Additive White Gaussian Noise (AWGN) environment across SNRs ranging from −20 to 10 dB demonstrated the approach’s effectiveness. Particularly, under a 5way5shot setting, the model achieves high classification accuracy even at −10dB SNR. Our research underscores the model’s ability to address the key challenges of radar emitter signal recognition in low-SNR and data-scarce conditions, demonstrating its strong adaptability and effectiveness in complex, real-world electromagnetic environments. Full article
(This article belongs to the Special Issue Digital Signal Processing and Wireless Communication)
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<p>Part of the time–frequency image of the pulse-modulated signal: (<b>a</b>) Barker; (<b>b</b>) Costas; (<b>c</b>) LFM; (<b>d</b>) Frank; (<b>e</b>) NS; (<b>f</b>) P2; (<b>g</b>) T4.</p>
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<p>MAML optimization algorithm framework flow.</p>
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<p>Basic structure of residual network.</p>
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<p>Principle of SE channel attention mechanism, where <span class="html-italic">H</span>, <span class="html-italic">W</span> and <span class="html-italic">C</span> represent the height, width, and channel dimensions of the input feature image <math display="inline"><semantics> <mrow> <mi>f</mi> <mi>e</mi> <mi>a</mi> <mi>t</mi> <mi>u</mi> <mi>r</mi> <msub> <mi>e</mi> <mi>i</mi> </msub> </mrow> </semantics></math>, respectively.</p>
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<p>SE-ResNet module.</p>
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<p>The 1D MSCNN structure flow.</p>
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<p>Technical process framework of multimodal fusion model.</p>
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<p>Costas time–frequency images at −2 dB from two different validation sets: (<b>a</b>) Costas time–frequency image from <span class="html-italic">D</span>; (<b>b</b>) Costas time–frequency image from <math display="inline"><semantics> <msubsup> <mi>D</mi> <mrow> <mi>val</mi> </mrow> <mi>Z</mi> </msubsup> </semantics></math>.</p>
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<p>Part of the time–frequency image of the pulse-modulated signal: (<b>a</b>) the accuracy rate on <math display="inline"><semantics> <msub> <mi>D</mi> <mi>val</mi> </msub> </semantics></math> under each SNR; (<b>b</b>) the accuracy rate on <math display="inline"><semantics> <msubsup> <mi>D</mi> <mrow> <mi>val</mi> </mrow> <mi>Z</mi> </msubsup> </semantics></math> under each SNR.</p>
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<p>Influence of MAML on model recognition accuracy under different sample sizes: (<b>a</b>) recognition accuracy rate of ResNet18-MAML on <math display="inline"><semantics> <msub> <mi>D</mi> <mi>val</mi> </msub> </semantics></math> under different sample sizes; (<b>b</b>) recognition accuracy rate of ResNet18-MAML on <math display="inline"><semantics> <msubsup> <mi>D</mi> <mrow> <mi>val</mi> </mrow> <mi>Z</mi> </msubsup> </semantics></math> under different sample sizes.</p>
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<p>The relationship between recognition accuracy and SNR of different models in different modes. (<b>a</b>) recognition accuracy of each method on <math display="inline"><semantics> <msub> <mi>D</mi> <mi>val</mi> </msub> </semantics></math>. (<b>b</b>) recognition accuracy rate of each method on <math display="inline"><semantics> <msubsup> <mi>D</mi> <mrow> <mi>val</mi> </mrow> <mi>Z</mi> </msubsup> </semantics></math>.</p>
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<p>Meta-validation classification confusion matrix on <math display="inline"><semantics> <msubsup> <mi>D</mi> <mrow> <mi>val</mi> </mrow> <mi>Z</mi> </msubsup> </semantics></math> for different SNRs: (<b>a</b>) Meta-validation classification under SNR = −20 dB, sampling categories: LFM, P1, P2, T3, Frank; (<b>b</b>) Meta-validation classification under SNR = −10 dB, sampling categories: Costas, Rect, LFM, T3, T4; (<b>c</b>) Meta-validation classification under SNR = 0 dB, sampling categories: Barker, Rect, T1, P3, P4.</p>
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<p>High-dimensional feature vector mapping of DCFANet: (<b>a</b>) feature vector mapping across all SNRs; (<b>b</b>) feature vector mapping for SNRs under −10 dB; (<b>c</b>) feature vector mapping for SNRs above −2 dB.</p>
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<p>t-SNE visualization of <math display="inline"><semantics> <msubsup> <mi>D</mi> <mrow> <mi>val</mi> </mrow> <mi>Z</mi> </msubsup> </semantics></math>: (<b>a</b>) t-SNE visualization of the time–frequency image modality; (<b>b</b>) t-SNE visualization of the I/Q waveform sequence modality.</p>
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12 pages, 2094 KiB  
Article
Real-Time Reconfigurable Radio Frequency Arbitrary-Waveform Generation via Temporal Pulse Shaping with a DPMZM and Multi-Tone Inputs
by Yireng Chen, Chenxiao Lin, Shuna Yang and Bo Yang
Photonics 2024, 11(10), 955; https://doi.org/10.3390/photonics11100955 - 11 Oct 2024
Viewed by 537
Abstract
Benefitting from a large bandwidth and compact configuration, a time-domain pulse-shaping (TPS) system provides possibilities for generating broadband radio frequency (RF) arbitrary waveforms based on the Fourier transform relationship between the input–output waveform pair. However, limited by the relatively low sampling rate and [...] Read more.
Benefitting from a large bandwidth and compact configuration, a time-domain pulse-shaping (TPS) system provides possibilities for generating broadband radio frequency (RF) arbitrary waveforms based on the Fourier transform relationship between the input–output waveform pair. However, limited by the relatively low sampling rate and bit resolution of an electronic arbitrary-waveform generator (EAWG), the diversity and fidelity of the output waveform as well as its reconfiguration rate are constrained. To remove the EAWG’s limitation and realize dynamic real-time reconfiguration of RF waveforms, we propose and demonstrate a novel approach of RF arbitrary-waveform generation based on an improved TPS system with an integrated dual parallel Mach–Zehnder modulator (DPMZM) and multi-tone inputs. By appropriately adjusting the DC bias voltages of DPMZM and the power values, as well as the center frequencies of the multi-tone inputs, any desired RF arbitrary waveform can be generated and reconfigured in real time. Proof-of-concept experiments on the generation of different user-defined waveforms with a sampling rate up to 27 GSa/s have been successfully carried out. Furthermore, the impact of modulation modes and higher-order dispersion on waveform fidelity is also discussed in detail. Full article
(This article belongs to the Section Optoelectronics and Optical Materials)
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<p>Schematic illustration of the proposed RF AWG scheme based on the TPS with a DPMZM and multi-tone inputs. MLL, mode-locked laser; DM, dispersive medium; DPMZM, dual parallel Mach–Zehnder modulator; SG Array, signal generator array; PD, photodetector; LPF, low-pass filter.</p>
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<p>Experimental setup of the proposed RF AWG via TPS with a DPMZM and multi-tone inputs. MLL, mode-locked laser; SMF, single-mode fiber; PC, polarization controller; DPMZM, dual parallel Mach–Zehnder modulator; SGM, signal generation module; EDFA, erbium-doped fiber amplifier; DCM, dispersion compensation module; PD, photodetector; DSO, digital sampling oscilloscope.</p>
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<p>The measured output pulse before (<b>a</b>) and after (<b>b</b>) dispersion matching.</p>
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<p>Experiment results of RF arbitrary-waveform generation under CS-SSB modulation with three-tone inputs: the power values of each tone signal are respectively (<b>a</b>) 8, 11, 10 dBm, (<b>b</b>) 9, 8, 9 dBm, (<b>c</b>) 12, 10, 8 dBm, and (<b>d</b>) 8, 8, 8 dBm.</p>
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<p>Experiment results of RF arbitrary-waveform generation under DSB modulation with the input signal having different center frequencies and power values: (<b>a</b>) 4 GHz, 18.8 dBm, (<b>b</b>) 8 GHz, 18.8 dBm, (<b>c</b>) 7 GHz, 8.9 dBm, (<b>d</b>) 7 GHz, 10 dBm.</p>
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<p>Experiment results of RF arbitrary-waveform generation under SSB modulation with input signals having different frequencies and power values: (<b>a</b>) 4 GHz, 18.8 dBm, (<b>b</b>) 6 GHz, 18.8 dBm, 12 GHz, 8.9 dBm, (<b>c</b>) 4 GHz, 12.9 dBm, 8 GHz, 10 dBm, 12 GHz, 8 dBm, (<b>d</b>) 4 GHz, 12.6 dBm, 8 GHz, 12.7 dBm, 12 GHz, 8 dBm.</p>
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<p>The simulated results with and without considering third-order dispersion.</p>
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12 pages, 2595 KiB  
Article
Photonic Generation of Arbitrary Microwave Waveforms with Anti-Dispersion Transmission Capability
by Xinyan Zhang, Kunpeng Zhai, Sha Zhu, Huashun Wen, Yu Liu and Ninghua Zhu
Micromachines 2024, 15(10), 1214; https://doi.org/10.3390/mi15101214 - 29 Sep 2024
Viewed by 587
Abstract
We propose and demonstrate a photonic-assisted approach for generating arbitrary microwave waveforms based on a dual-polarization dual-parallel Mach–Zehnder modulator, offering significant advantages in terms of tunability of repetition rates and anti-dispersion capability. In order to generate diverse microwave waveforms, two sinusoidal radio frequency [...] Read more.
We propose and demonstrate a photonic-assisted approach for generating arbitrary microwave waveforms based on a dual-polarization dual-parallel Mach–Zehnder modulator, offering significant advantages in terms of tunability of repetition rates and anti-dispersion capability. In order to generate diverse microwave waveforms, two sinusoidal radio frequency signals with distinct frequency relationships are applied to the dual-polarization dual-parallel Mach–Zehnder modulator. By adjusting the power of the applied sinusoidal radio frequency signal, the power ratio between these orthogonal polarized optical sidebands can be changed, and thereby desired radio frequency waveforms can be obtained after photoelectric conversion. In our proof-of-concept experiment, we systematically varied the repetition rate of triangular, rectangular and sawtooth waveforms. Meanwhile, we calculated the Root Mean Square Error (RMSE) to assess the approximation error in each waveform. The RMSEs are 0.1089, 0.2182 and 0.1185 for the triangular, rectangular and sawtooth microwave waveforms with repetition rate of 8 GHz, respectively. Furthermore, after passing through 25 km single mode fiber, the optical power decreased by approximately 5.6 dB, which verifies the anti-dispersion transmission capability of our signal generator. Full article
(This article belongs to the Special Issue Optoelectronic Fusion Technology)
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<p>Schematic diagram of the proposed photonics generation of microwave waveforms. LD: laser diode, MZM: Mach–Zehnder modulator, PR: polarization rotator, PBC: polarization beam combiner, SMF: single-mode fiber, PD: photodetector, OSC: oscilloscope.</p>
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<p>Schematic optical spectra of the proposed signal generator. (<b>a</b>) Optical carrier. (<b>b</b>) Optical carrier modulated by RF1 signal in x-polarization. (<b>c</b>) Optical carrier modulated by RF2 signal in y-polarization. (<b>d</b>) The optical spectrum at the output of tunable bandpass filter (TBPF).</p>
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<p>The measured optical spectra before and after the TBPF when generating a triangular waveform with a repetition of 10 GHz.</p>
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<p>Experiment results. (<b>a</b>) Generated triangular waveform with a repetition rate of 8 GHz, and (<b>b</b>) its spectrum. (<b>c</b>) Generated triangular waveform with a repetition rate of 10 GHz, and (<b>d</b>) its spectrum. (<b>e</b>) Generated triangular waveform with a repetition rate of 12 GHz, and (<b>f</b>) its spectrum.</p>
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<p>Experiment results. (<b>a</b>) Generated rectangular waveform with a repetition rate of 8 GHz, and (<b>b</b>) its spectrum. (<b>c</b>) Generated rectangular waveform with a repetition rate of 10 GHz, and (<b>d</b>) its spectrum. (<b>e</b>) Generated rectangular waveform with a repetition rate of 12 GHz, and (<b>f</b>) its spectrum.</p>
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<p>Experiment results. (<b>a</b>) Generated sawtooth waveform with a repetition rate of 8 GHz, and (<b>b</b>) its spectrum. (<b>c</b>) Generated sawtooth waveform with a repetition rate of 10 GHz, and (<b>d</b>) its spectrum. (<b>e</b>) Generated sawtooth waveform with a repetition rate of 12 GHz, and (<b>f</b>) its spectrum.</p>
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<p>The measured optical spectra before and after 25 km SMF when generating a triangular waveform with the repetition of 10 GHz.</p>
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<p>Experiment results. (<b>a</b>) Generated rectangular waveforms with repetition rate of 8, 10 and 12 GHz after 25 km SMF, and (<b>b</b>) its spectrums. (<b>c</b>) Generated triangular waveforms with repetition rates of 8, 10 and 12 GHz after 25 km SMF, and (<b>d</b>) its spectrums. (<b>e</b>) Generated sawtooth waveforms with repetition rates of 8, 10 and 12 GHz after 25 km SMF, and (<b>f</b>) its spectrums. The red, green, and blue curves represent the 8 GHz, 10 GHz, and 12 GHz waveforms respectively.</p>
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<p>Experiment results. (<b>a</b>) Generated triangular waveforms before and after 25 km SMF, and (<b>b</b>) its spectrums.</p>
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25 pages, 21622 KiB  
Article
Advanced Design and Implementation of a 2-Channel, Multi-Functional Therapeutic Electrical Stimulator
by Rujira Lakatem, Suttipong Boontaklang and Chow Chompoo-inwai
Electronics 2024, 13(19), 3793; https://doi.org/10.3390/electronics13193793 - 24 Sep 2024
Viewed by 1208
Abstract
This research introduces the design, implementation, and rigorous evaluation of a novel 2-channel, multi-functional therapeutic electrical stimulator, meticulously engineered to meet the stringent demands of contemporary clinical applications. The device integrates a high-speed R-2R ladder DAC and a sophisticated pulse generator unit, capable [...] Read more.
This research introduces the design, implementation, and rigorous evaluation of a novel 2-channel, multi-functional therapeutic electrical stimulator, meticulously engineered to meet the stringent demands of contemporary clinical applications. The device integrates a high-speed R-2R ladder DAC and a sophisticated pulse generator unit, capable of producing twelve essential current waveforms with fully adjustable parameters, including pulse amplitude, pulse duration, and pulse repetitive frequency. The proposed driving stage unit ensures precise voltage-to-current conversion, delivering stable and accurate output currents even under varying load conditions, which effectively simulate the diverse impedance characteristics of human tissue. Extensive testing confirmed the compliance with international medical standards, notably IEC 60601-1, IEC 60601-1-2, and IEC 60601-2-10. The experimental results underscore the device’s consistent operation within prescribed safety and performance thresholds, with all deviations in pulse parameters remaining well below the permissible limits. Furthermore, the proposed electrical stimulator demonstrated exceptional stability across variable load conditions, as evidenced by minimal amplitude errors and high correlation between waveform characteristics. These findings highlight the proposed device’s robustness and its potential as a versatile tool for a wide range of therapeutic applications, including pain management, muscle stimulation, and nerve rehabilitation, thus marking a significant advancement in the field of therapeutic electrical stimulation. Full article
(This article belongs to the Section Industrial Electronics)
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<p>System overview of the proposed ES design.</p>
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<p>Scope of work emphasized in this paper.</p>
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<p>The proposed R-2R ladder DAC circuit.</p>
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<p>The actual schematic of the proposed pulse generator unit implementation.</p>
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<p>The signal polarity separator circuit in this design.</p>
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<p>V-to-I converter in this work.</p>
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<p>The flyback converter circuit.</p>
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<p>The actual schematic of the proposed driving stage unit implementation.</p>
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<p>Two integrated PCBs of the key components in the proposed ES design.</p>
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<p>The experimental configuration diagram.</p>
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<p>The actual experimental setup.</p>
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<p>Demonstration of twelve essential output currents (<span class="html-italic">I<sub>Out</sub></span>) compared to controlled voltage (<span class="html-italic">V<sub>Ra</sub></span>) of the proposed ES device: (<b>a</b>) IG; (<b>b</b>) CG; (<b>c</b>) MF; (<b>d</b>) DF; (<b>e</b>) CP; (<b>f</b>) CPid; (<b>g</b>) LP; (<b>h</b>) TF; (<b>i</b>) RF; (<b>j</b>) ASYM; (<b>k</b>) ASYM-A; and (<b>l</b>) SYM.</p>
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<p>Demonstration of pulse amplitude adjustability: (<b>a</b>) MF 10 mA; (<b>b</b>) MF 40 mA; (<b>c</b>) MF 70 mA; (<b>d</b>) ASYM 10 mA; (<b>e</b>) ASYM 70 mA; and (<b>f</b>) ASYM 140 mA.</p>
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<p>Demonstration of pulse duration adjustability (ASYM): (<b>a</b>) 50 µs; (<b>b</b>) 500 µs; and (<b>c</b>) 2000 µs.</p>
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<p>Demonstration of pulse repetitive frequency adjustability (RF): (<b>a</b>) 50 Hz; (<b>b</b>) 200 Hz; and (<b>c</b>) 500 Hz.</p>
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<p>Demonstration of two additional special functions for output currents.: (<b>a</b>) ASYM with Surge; and (<b>b</b>) SYM with Modulation.</p>
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21 pages, 6212 KiB  
Article
Validation and Error Minimization of Global Ecosystem Dynamics Investigation (GEDI) Relative Height Metrics in the Amazon
by Alyson East, Andrew Hansen, Patrick Jantz, Bryce Currey, David W. Roberts and Dolors Armenteras
Remote Sens. 2024, 16(19), 3550; https://doi.org/10.3390/rs16193550 - 24 Sep 2024
Viewed by 872
Abstract
Global Ecosystem Dynamics Investigation (GEDI) is a relatively new technology for global forest research, acquiring LiDAR measurements of vertical vegetation structure across Earth’s tropical, sub-tropical, and temperate forests. Previous GEDI validation efforts have largely focused on top of canopy accuracy, and findings vary [...] Read more.
Global Ecosystem Dynamics Investigation (GEDI) is a relatively new technology for global forest research, acquiring LiDAR measurements of vertical vegetation structure across Earth’s tropical, sub-tropical, and temperate forests. Previous GEDI validation efforts have largely focused on top of canopy accuracy, and findings vary by geographic region and forest type. Despite this, many applications utilize measurements of vertical vegetation distribution from the lower canopy, with a wide diversity of uses for GEDI data appearing in the literature. Given the variability in data requirements across research applications and ecosystems, and the regional variability in GEDI data quality, it is imperative to understand GEDI error to draw strong inferences. Here, we quantify the accuracy of GEDI relative height metrics through canopy layers for the Brazilian Amazon. To assess the accuracy of on-orbit GEDI L2A relative height metrics, we utilize the GEDI waveform simulator to compare detailed airborne laser scanning (ALS) data from the Sustainable Landscapes Brazil project to GEDI data collected by the International Space Station. We also assess the impacts of data filtering based on biophysical and GEDI sensor conditions and geolocation correction on GEDI error metrics (RMSE, MAE, and Bias) through canopy levels. GEDI data accuracy attenuates through the lower percentiles in the relative height (RH) curve. While top of canopy (RH98) measurements have relatively high accuracy (R2 = 0.76, RMSE = 5.33 m), the accuracy of data decreases lower in the canopy (RH50: R2 = 0.54, RMSE = 5.59 m). While simulated geolocation correction yielded marginal improvements, this decrease in accuracy remained constant despite all error reduction measures. Some error rates for the Amazon are double those reported in studies from other regions. These findings have broad implications for the application of GEDI data, especially in studies where forest understory measurements are particularly challenging to acquire (e.g., dense tropical forests) and where understory accuracy is highly important. Full article
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<p>Study area depicting locations of ALS plots and overlapping GEDI footprints. Zoomed panels (A–C) correspond to letters on the reference map. Green regions on the reference map denote Moist Tropical Broadleaf Biome.</p>
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<p>Depiction of ALS point cloud data (<b>A</b>), corresponding GEDI waveform ((<b>B</b>), orange), and relative height curve ((<b>B</b>), black line).</p>
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<p>Workflow of validation and error minimization of on-orbit GEDI data to fine-scale ALS. Nested boxes delineate different processes. All processes begin at the grey oval labelled start in the middle of the diagram and follow color-coded arrows. Validation follows the dark blue arrows within the dark blue box. Both error minimization workflows rely on the validation outputs for comparison. The geolocation correction approach (yellow bounding box) starts at the starting oval with initial data and follows the yellow arrows. The filtering approach (green bounding box) starts with the outputs of the geolocation correction and follows green arrows to the final dataset comparison.</p>
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<p>GEDI-measured RH values compared to their corresponding ALS-derived GEDI<sub>sim</sub> values starting from RH<sub>100</sub> in the top left corner down to RH<sub>0</sub> in the bottom right. Point clouds are colored by the density of overlapping points on a scale of yellow (high density) to purple (low density). Black lines indicate where points would fall given a one-to-one relationship between GEDI and GEDI<sub>sim</sub>. Red dashed lines differentiate negative values from positive.</p>
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<p>Box plots of error associated with relative heights. Boxes represent the interquartile range (IQR) (25th percentile of data to the 75th percentile), the black bar is the median, and the red dot is the mean. Error bars extend to 1.5× the IQR, and points are observations outside of that range.</p>
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<p>The relationship between bias, R<sup>2</sup>, RMSE, RMSE%, MAE, MAE%, and relative height for geolocation-corrected data compared to uncorrected data (quality flags removed). RMSE% values that exceed 100% are not shown, but the general trend persists. Similarly, R<sup>2</sup> values below 0 are omitted.</p>
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<p>The relationship between bias, R<sup>2</sup>, RMSE, RMSE%, MAE, MAE%, and relative height under different scenarios of data filtering. RMSE% values that exceed 100% are not shown, but the general trend persists. Similarly, R<sup>2</sup> values below 0 are omitted. * Serves as the baseline condition for all other filters.</p>
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<p>Canopy metrics calculated from relative height values and the relationship between the GEDI values (x-axis) compared to GEDI<sub>sim</sub> references (y-axis). All metrics were calculated from truncated data. Left: RH<sub>sum</sub><math display="inline"><semantics> <mrow> <mo>=</mo> <mrow> <msubsup> <mo stretchy="false">∑</mo> <mrow> <mi>i</mi> <mo>=</mo> <mn>0</mn> </mrow> <mrow> <mn>98</mn> </mrow> </msubsup> <mrow> <msub> <mrow> <mi>R</mi> <mi>H</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </mrow> </mrow> </semantics></math>, middle: <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>R</mi> <mi>H</mi> </mrow> <mrow> <mn>98</mn> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>R</mi> <mi>H</mi> </mrow> <mrow> <mn>50</mn> </mrow> </msub> </mrow> </mfrac> </mstyle> </mrow> </semantics></math>, right: Canopy Ratio = <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>R</mi> <mi>H</mi> </mrow> <mrow> <mn>98</mn> </mrow> </msub> <mo>−</mo> <msub> <mrow> <mi>R</mi> <mi>H</mi> </mrow> <mrow> <mn>25</mn> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>R</mi> <mi>H</mi> </mrow> <mrow> <mn>98</mn> </mrow> </msub> </mrow> </mfrac> </mstyle> </mrow> </semantics></math>. Points where calculations resulted in values of infinity due to division by zero populate the upper extremes of the plot scales. Black lines indicate where points would fall given a one-to-one relationship.</p>
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21 pages, 6196 KiB  
Article
Unimodular Multi-Input Multi-Output Waveform and Mismatch Filter Design for Saturated Forward Jamming Suppression
by Xuan Fang, Dehua Zhao and Liang Zhang
Sensors 2024, 24(18), 5884; https://doi.org/10.3390/s24185884 - 10 Sep 2024
Viewed by 1039
Abstract
Forward jammers replicate and retransmit radar signals back to generate coherent jamming signals and false targets, making anti-jamming an urgent issue in electronic warfare. Jamming transmitters work at saturation to maximize the retransmission power such that only the phase information of the angular [...] Read more.
Forward jammers replicate and retransmit radar signals back to generate coherent jamming signals and false targets, making anti-jamming an urgent issue in electronic warfare. Jamming transmitters work at saturation to maximize the retransmission power such that only the phase information of the angular waveform at the designated direction of arrival (DOA) is retained. Therefore, amplitude modulation of MIMO radar angular waveforms offers an advantage in combating forward jamming. We address both the design of unimodular MIMO waveforms and their associated mismatch filters to confront mainlobe jamming in this paper. Firstly, we design the MIMO waveforms to maximize the discrepancy between the retransmitted jamming and the spatially synthesized radar signal. We formulate the problem as unconstrained non-linear optimization and solve it using the conjugate gradient method. Particularly, we introduce fast Fourier transform (FFT) to accelerate the numeric calculation of both the objection function and its gradient. Secondly, we design a mismatch filter to further suppress the filtered jamming through convex optimization in polynomial time. The simulation results show that for an eight-element MIMO radar, we are able to reduce the correlation between the angular waveform and saturated forward jamming to −6.8 dB. Exploiting this difference, the mismatch filter can suppress the jamming peak by 19 dB at the cost of an SNR loss of less than 2 dB. Full article
(This article belongs to the Section Radar Sensors)
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<p>Flowchart of waveform and mismatch filter design.</p>
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<p>Signal reception and processing model for co-located MIMO radar with spatial synthesis of the waveform and a saturated forward jamming signal in the mainlobe.</p>
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<p>Comparison of waveform performance of each method in 10° for 8 × 128 codes when <span class="html-italic">η</span> = 1. (<b>a</b>) Autocorrelation level; (<b>b</b>) jamming cross-correlation level.</p>
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<p>Comparison of waveform performance of each method in 10° for 8 × 128 codes when <span class="html-italic">η</span> = 10. (<b>a</b>) Autocorrelation level; (<b>b</b>) jamming cross-correlation level.</p>
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<p>Performance comparison for different wave numbers with code length Ns = 128. (<b>a</b>) JCSL of WF0, WF1 and WF2 at different jamming intensities; (<b>b</b>) JCL of WF0, WF1 and WF2 at different jamming intensities at zero lag.</p>
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<p>Performance comparison of the two filters for WF0. (<b>a</b>) The WF0 matched filter; (<b>b</b>) the WF0 mismatch filter.</p>
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<p>Performance comparison of the two filters for WF1. (<b>a</b>)The WF1 matched filter; (<b>b</b>) The WF1 mismatch filter.</p>
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<p>Performance comparison of the two filters for WF2. (<b>a</b>) The WF2 matched filter; (<b>b</b>) the WF2 mismatch filter.</p>
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<p>Comparison of pulse compression outputs with the MF and MMF, of which the input signal is composed of a WF2 angular echo at 100 with χ = 1 V, 5 saturated forward jamming bins at 50, 150, 200, 250 and 300 with the jamming intensity <span class="html-italic">η</span> = 10 V and Gaussian noise with σ2 = 10 dBw.</p>
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21 pages, 4324 KiB  
Article
A Space–Time Coding Array Sidelobe Optimization Method Combining Array Element Spatial Coding and Mismatched Filtering
by Shenjing Wang, Feng He and Zhen Dong
Remote Sens. 2024, 16(17), 3322; https://doi.org/10.3390/rs16173322 - 7 Sep 2024
Viewed by 648
Abstract
Digital array radar (DAR) can fully realize digitalization at both the transmitting and receiving ends. However, the development of freedom at the transmitting end is far from mature. So, the new concept of multi-dimensional waveform coding array has appeared, which can optimize the [...] Read more.
Digital array radar (DAR) can fully realize digitalization at both the transmitting and receiving ends. However, the development of freedom at the transmitting end is far from mature. So, the new concept of multi-dimensional waveform coding array has appeared, which can optimize the transmitting resources in space–time/frequency waveform or another dimension. Space–time coding array (STCA) is a typical kind of multi-dimensional waveform coding array, which can make full use of the high degree of freedom at the transmitting end. It realizes emission diversity by introducing a small time delay between different transmission array elements. In this paper, an optimization method for STCA, which combines the array spatial coding at the transmitting end and mismatched filter design at the receiving end, is proposed. This method aims to solve the sidelobe problems of STCA: the inherent resonance phenomenon and the resolution loss problem. The experimental verification and quantitative comparative analysis prove the effectiveness of the proposed method. The resolution is restored to the ideal level under the premise of maintaining the beam-scanning ability and ultra-low sidelobe, and the resonance phenomenon caused by spectrum discontinuity is eliminated simultaneously. Full article
(This article belongs to the Special Issue Advances in Remote Sensing, Radar Techniques, and Their Applications)
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Graphical abstract

Graphical abstract
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<p>The diagram of STCA transmitting.</p>
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<p>(<b>a</b>) The antenna pattern of STCA in the frequency domain. (<b>b</b>) The frequency profile of the antenna pattern (normalized). (<b>c</b>) The array gain value of STCA in the frequency domain (the maximum value is the number of array elements). The red dotted boxes represent the directions where the resonance problem occurs, which will be introduced in detail in following part.</p>
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<p>(<b>a</b>) The antenna pattern of STCA in the frequency domain. (<b>b</b>) The frequency profile of the antenna pattern (normalized). (<b>c</b>) The array gain value of STCA in the frequency domain (the maximum value is the number of array elements). The red dotted boxes represent the directions where the resonance problem occurs, which will be introduced in detail in following part.</p>
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<p>(<b>a</b>) Range profile of STCA at <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>10</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>. (<b>b</b>) Range profile of STCA at <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>5.22</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>. (<b>c</b>) Range profile of STCA at <math display="inline"><semantics> <mrow> <mrow> <mn>20</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>. (<b>d</b>) Range profile of phased array at <math display="inline"><semantics> <mrow> <mrow> <mn>20</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>. The red dotted box represents the angles where the resonance problem occurs.</p>
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<p>The multi-dimensional ambiguity function evaluation results of STCA and conventional phased array. (<b>a</b>) Range–range ambiguity function of STCA. (<b>b</b>) Range–range ambiguity function of phased array. (<b>c</b>) Range–Doppler ambiguity function of STCA. (<b>d</b>) Range–Doppler ambiguity function of phased array. (<b>e</b>) Range–angle ambiguity function of STCA. (<b>f</b>) Range–angle ambiguity function of phased array.</p>
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<p>Frequency profile of antenna pattern comparison (normal STCA and STCA with Barker code).</p>
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<p>The signal processing flow of STCA optimization at the receiving end.</p>
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<p>The simulation results. (<b>a</b>) R-A ambiguity function of STCA at <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>5.22</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>. (<b>b</b>) R-A ambiguity function of STCA with Barker code and MSF at <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>5.22</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>.</p>
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<p>Range profile comparison in three directions of resonance angle region. Three modes used for comparison: STCA, STCA with Barker code and MF, STCA with Barker code and MSF. (<b>a</b>) At the angle of <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>10</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>; (<b>b</b>) at the angle of <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>5.22</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>; (<b>c</b>) at the angle of <math display="inline"><semantics> <mrow> <mn>0</mn> <mo>°</mo> </mrow> </semantics></math>. The horizontal values in the figure represent multiples of the pulse width.</p>
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<p>The range profile comparison of MF and MSF. Subtitle is the value of LPG and PSLR. (<b>a</b>) At the angle of <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>5.22</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>; (<b>b</b>) at the angle of <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>10</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>.</p>
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<p>The point target simulation results. (<b>a</b>) Imaging result of normal STCA at the angle of <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>5.22</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>; (<b>b</b>) imaging result of normal STCA at the angle of <math display="inline"><semantics> <mrow> <mrow> <mn>40</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>; (<b>c</b>) imaging result of STCA with Barker code and MF at the angle of <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>5.22</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>; (<b>d</b>) imaging result of STCA with Barker code and MF at the angle of <math display="inline"><semantics> <mrow> <mrow> <mn>40</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>; (<b>e</b>) imaging result of STCA with Barker code and MSF at the angle of <math display="inline"><semantics> <mrow> <mo>−</mo> <mrow> <mn>5.22</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>; (<b>f</b>) imaging result of STCA with Barker code and MSF at the angle of <math display="inline"><semantics> <mrow> <mrow> <mn>40</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>.</p>
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16 pages, 12528 KiB  
Article
A Ground-Penetrating Radar-Based Study of the Structure and Moisture Content of Complex Reconfigured Soils
by Yunlan He, Lulu Fang, Suping Peng, Wen Liu and Changhao Cui
Water 2024, 16(16), 2332; https://doi.org/10.3390/w16162332 - 19 Aug 2024
Viewed by 1047
Abstract
To increase the detection accuracy of soil structure and moisture content in reconstituted soils under complex conditions, this study utilizes a 400 MHz ground-penetrating radar (GPR) to examine a study area consisting of loess, sandy loam, red clay, and mixed soil. The research [...] Read more.
To increase the detection accuracy of soil structure and moisture content in reconstituted soils under complex conditions, this study utilizes a 400 MHz ground-penetrating radar (GPR) to examine a study area consisting of loess, sandy loam, red clay, and mixed soil. The research involves analyzing the single-channel waveforms and two-dimensional images of GPR, preprocessing the data, obtaining envelope information via amplitude envelope detection, and performing a Hilbert transformation. This study employs a least squares fitting approach to the instantaneous phase envelope to ascertain the thickness of various soil layers. By utilizing the average envelope amplitude (AEA) method, a correlation between the radar’s early signal amplitude envelope and the soil’s shallow dielectric constant is established to invert the moisture content of the soil. The analysis integrates soil structure and moisture distribution data to investigate soil structure characteristics and moisture content performance under diverse soil properties and depths. The findings indicate that the envelope detection method effectively identifies stratification boundaries across different soil types; the AEA method is particularly efficacious in inverting the moisture content of reconstituted soils up to 3 m deep, with an average relative error ranging from 2.81% to 7.41%. Notably, moisture content variations in stratified reconstituted soils are more pronounced than those in mixed soil areas, displaying a marked stepwise increase with depth. The moisture content trends in the vertical direction of the same soil profile are generally consistent. This research offers a novel approach to studying reconstituted soils under complex conditions, confirming the viability of the envelope detection and AEA methods for intricate soil investigations and broadening the application spectrum of GPR in soil studies. Full article
(This article belongs to the Special Issue Innovative Technologies for Mine Water Treatment)
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<p>Topographic and geomorphological map of Zhungeer Banner. The five-pointed star is the location of the study area.</p>
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<p>Schematic diagram of the soil profile in the research area. A, B refer to Study Zone A and Study Zone B, respectively.</p>
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<p>Layout plan of the radar survey lines in the research area. A, B refer to Study Zone A and Study Zone B; L1–L6 refers to the ground-penetrating radar wiring for radar detection.</p>
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<p>AEA method flowchart.</p>
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<p>Two-dimensional raw images of ground penetrating radar. (<b>a</b>) Unprocessed two-dimensional image of ground-penetrating radar; (<b>b</b>) Preprocessed two-dimensional image of ground-penetrating radar.</p>
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<p>Envelope analysis curves. (<b>a</b>) Envelope line of the mixed reconstruction soil area in Zone A; (<b>b</b>) Envelope line of the three-layer reconstruction soil area in Zone B.</p>
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<p>Envelope instantaneous phase fitting curve and convex-concave inflection point graph. (<b>a</b>) Envelope instantaneous phase fitting curve and convex-concave inflection point in Zone A; (<b>b</b>) Envelope instantaneous phase fitting curve and convex-concave inflection point in Zone B.</p>
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<p>Hilbert-Huang transform graph. (<b>a</b>) Hilbert-Huang transform graph in Zone A; (<b>b</b>) Hilbert-Huang transform graph in Zone B.</p>
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<p>Fitting graph of the permittivity and reciprocal of the radar signal envelope value.</p>
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<p>Fitting graph of moisture content and radar amplitude.</p>
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<p>Comparison chart of the moisture content between the AEA and drying methods in the N-S direction in Zone A: (<b>a</b>) Comparison of the moisture content between the AEA and drying methods in the upper part of Zone A; (<b>b</b>) Comparison of the moisture content between the AEA and drying methods in the bottom part of Zone A.</p>
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<p>Comparison chart of the moisture content between the AEA and drying methods in the N-S direction of Zone B: (<b>a</b>) Comparison of the moisture content between the AEA and drying methods in the upper part of Zone B; (<b>b</b>) Comparison of the moisture content between the AEA and the drying methods in the bottom part of Zone B.</p>
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<p>Comparison chart of the moisture content trends of AEA in Zone A. (<b>a</b>) Comparison of the moisture content trends of AEA in the N-S direction in Zone A; (<b>b</b>) Comparison of the moisture content trends of AEA in the E-W direction in Zone A.</p>
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<p>Comparison chart of the moisture content trends of AEA in Zone B. (<b>a</b>) Comparison of the moisture content trends of AEA in the N-S direction in Zone B; (<b>b</b>) Comparison of the moisture content trends of AEA in the E-W direction in Zone B.</p>
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12 pages, 4365 KiB  
Communication
Delay-Doppler Map Shaping through Oversampled Complementary Sets for High-Speed Target Detection
by Jiahua Zhu, Zhuang Xie, Nan Jiang, Yongping Song, Sudan Han, Weijian Liu and Xiaotao Huang
Remote Sens. 2024, 16(16), 2898; https://doi.org/10.3390/rs16162898 - 8 Aug 2024
Cited by 9 | Viewed by 1273
Abstract
Advanced waveform design schemes have been widely employed for radar and sonar remote sensing analysis such as target detection and separation, where significant range sidelobe is a main factor that limits the improvement of analysis performance. As an extensional type of Golay complementary [...] Read more.
Advanced waveform design schemes have been widely employed for radar and sonar remote sensing analysis such as target detection and separation, where significant range sidelobe is a main factor that limits the improvement of analysis performance. As an extensional type of Golay complementary waveforms, complementary sets are a waveform design scenario of concern that shows more diversity in the design of transmission order, and results in a different distribution of range sidelobes. This work proposes an oversampled generalized Prouhet–Thue–Morse (OGPTM) method for the transmitted signal design of complementary sets, with comprehensive analysis to the influence on the sidelobe distribution. Based on this idea and our previous work, we further put forward a pointwise multiplication processor (PMuP) to integrate two delay-Doppler maps of oversampled complementary sets, which achieve much better sidelobe suppression performance on high-speed target detection with range migration. Full article
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<p>The delay-Doppler map of (<b>a</b>) theoretical GPTM algorithm without range migration and (<b>b</b>) GPTM algorithm with range migration. (the Doppler of the target equals 0 and 1 rad, respectively, and the unit of the color bar is dB).</p>
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<p>Process flow of OGPTM scheme for complementary sets.</p>
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<p>The comparison results of (<b>a</b>) standard Golay pair; (<b>b</b>) PTM design; (<b>c</b>) standard complementary sets; and (<b>d</b>) GPTM algorithm (the unit of the color bar is dB).</p>
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<p>The delay-Doppler maps of OGPTM with different oversampling rates: (<b>a</b>) 1 time; (<b>b</b>) 2 times; (<b>c</b>) 4 times; (<b>d</b>) 8 times; (<b>e</b>) 16 times; and (<b>f</b>) 32 times (<math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>32</mn> </mrow> </semantics></math>, the unit of the color bar is dB).</p>
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<p>The delay-Doppler maps of OGPTM with different oversampling rates: (<b>a</b>) 1 time; (<b>b</b>) 2 times; (<b>c</b>) 4 times; (<b>d</b>) 8 times; (<b>e</b>) 16 times; (<b>f</b>) 32 times; and (<b>g</b>) 64 times (<math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>64</mn> </mrow> </semantics></math>, the unit of the color bar is dB).</p>
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<p>The delay-Doppler maps of (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>χ</mi> <mrow> <mi>OGPTM</mi> <mn>1</mn> </mrow> </msub> <mrow> <mo>(</mo> <mi>t</mi> <mo>,</mo> <msub> <mi>F</mi> <mi mathvariant="normal">D</mi> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> (1 time OGPTM, i.e., GPTM); (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>χ</mi> <mrow> <mi>OGPTM</mi> <mn>2</mn> </mrow> </msub> <mrow> <mo>(</mo> <mi>t</mi> <mo>,</mo> <msub> <mi>F</mi> <mi mathvariant="normal">D</mi> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> (2 times OGPTM); (<b>c</b>) PMP; (<b>d</b>) PAP; (<b>e</b>) PTP (<math display="inline"><semantics> <mrow> <mi>t</mi> <mi>h</mi> <mi>r</mi> <mo>=</mo> <mn>2</mn> <mi>dB</mi> </mrow> </semantics></math>); and (<b>f</b>) PMuP (<math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>32</mn> </mrow> </semantics></math>, the unit of the color bar is dB).</p>
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