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Search Results (517)

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22 pages, 3424 KiB  
Article
A Line of Sight/Non Line of Sight Recognition Method Based on the Dynamic Multi-Level Optimization of Comprehensive Features
by Ziyao Ma, Zhongliang Deng, Zidu Tian, Yingjian Zhang, Jizhou Wang and Jilong Guo
Sensors 2025, 25(2), 304; https://doi.org/10.3390/s25020304 - 7 Jan 2025
Viewed by 292
Abstract
With the advent of the 5G era, high-precision localization based on mobile communication networks has become a research hotspot, playing an important role in indoor emergency rescue in shopping malls, smart factory management and tracking, as well as precision marketing. However, in complex [...] Read more.
With the advent of the 5G era, high-precision localization based on mobile communication networks has become a research hotspot, playing an important role in indoor emergency rescue in shopping malls, smart factory management and tracking, as well as precision marketing. However, in complex environments, non-line-of-sight (NLOS) propagation reduces the measurement accuracy of 5G signals, causing large deviations in position solving. In order to obtain high-precision position information, it is necessary to recognize the propagation state of the signal before distance measurement or angle measurement. In this paper, we propose a dynamic multi-level optimization of comprehensive features (DMOCF) network model for line-of-sight (LOS)/NLOS identification. The DMOCF model improves the expression ability of the deep model by adding a res2 module to the time delay neural network (TDNN), so that fine-grained feature information such as weak reflections or noise in the signal can be deeply understood by the model, enabling the network to realize layer-level feature processing by adding Squeeze and Excitation (SE) blocks with adaptive weight adjustment for each layer. A mamba module with position coding is added to each layer to capture the local patterns of wireless signals under complex propagation phenomena by extracting local features, enabling the model to understand the evolution of signals over time in a deeper way. In addition, this paper proposes an improved sand cat search algorithm for network parameter search, which improves search efficiency and search accuracy. Overall, this new network architecture combines the capabilities of local feature extraction, global feature preservation, and time series modeling, resulting in superior performance in the 5G channel impulse response (CIR) signal classification task, improving the accuracy of the model and accurately identifying the key characteristics of multipath signal propagation. Experimental results show that the NLOS/LOS recognition method proposed in this paper has higher accuracy than other deep learning methods. Full article
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<p>The impact of NLOS error on positioning.</p>
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<p>Improved TDNN incorporating res2 and SE blocks.</p>
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<p>Zero order keeper diagram.</p>
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<p>Selective SSM structure diagram.</p>
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<p>DMOCF network structure diagram.</p>
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<p>Experimental scene and hardware equipment layout.</p>
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<p>Fifth-generation CIR signal processing flowchart.</p>
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<p>Schematic diagram of data collection points.</p>
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<p>Schematic diagram of 5G CSI-RS time–frequency resource allocation.</p>
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<p>Comparison chart of algorithm performance.</p>
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20 pages, 4258 KiB  
Article
Improving Localization Accuracy Through Optimal Selection Strategy
by Na Wu, Xiaozhen Yan, Qinghua Luo and Yuexiu Xing
Electronics 2025, 14(1), 172; https://doi.org/10.3390/electronics14010172 - 3 Jan 2025
Viewed by 286
Abstract
A localization system is essential for providing crucial position information in various applications, such as three-dimensional (3D) warehousing, smart cities, uncrewed aerial vehicle (UAV) control, and other services that heavily rely on accurate localization. However, the transmission of wireless signals can be impacted [...] Read more.
A localization system is essential for providing crucial position information in various applications, such as three-dimensional (3D) warehousing, smart cities, uncrewed aerial vehicle (UAV) control, and other services that heavily rely on accurate localization. However, the transmission of wireless signals can be impacted by diverse environmental factors, leading to decreased accuracy in determining localization in scenarios involving multiple signal paths, None Line of Sight (NLOS) situations, and different types of interference. In some cases, this may render the localization system unsuitable for subsequent applications. To enhance the localization accuracy, we propose a 3D localization method using an optimization selection strategy. With this method, we make the following innovations: (1) We utilize an evaluation of feature points to minimize the negative impact of NLOS. (2) Through the backward assessment and the optimal selection of distance estimations, we obtain a more accurate localization result. In more detail, our approach implements a specific strategy for distance estimation, followed by defining the feature points within the localization field and selecting the most optimized one. Subsequently, using the chosen feature points, we evaluate the quality of the distances in reverse. We then select suitable distance estimation outcomes for further localization calculations. Ultimately, by employing the proposed 3D localization technique, we achieve a highly precise localization result. We perform simulations and experiments to assess the presented localization system. More specifically, compared with certain strategies, we improve the localization accuracy by 58.33% and 43.83% using the selection strategy. Compared with the other methods, we enhance the localization accuracy from 17.94% to 32.54%. The results from these evaluations demonstrate that our method significantly enhances 3D localization accuracy. Full article
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<p>The architecture of the 3D localization system.</p>
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<p>Localization node.</p>
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<p>The processing flow of Newton’s iteration localization method (NILM).</p>
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<p>The three-dimensional (3D) localization environment.</p>
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<p>The deployment of the feature points.</p>
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<p>The simulation data model.</p>
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<p>The localization error under different signal-to-noise ratio (SNR) values.</p>
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<p>The localization error with different strengths of None Line of Sight (NLOS).</p>
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<p>The localization error with different densities of feature points.</p>
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<p>The localization error with different densities of anchor nodes.</p>
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<p>The simulation result of group 5.</p>
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<p>The 3D localization environment.</p>
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<p>The NanoLoc-based wireless localization system.</p>
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<p>The deployment configuration of the anchor nodes.</p>
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<p>The framework of the experiment’s data process.</p>
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<p>The localization error observed in the four methods utilizing three strategies. (<b>a</b>) The localization error of the quadrilateral method. (<b>b</b>) The localization error of the least squares method; (<b>c</b>) The localization error of maximum likelihood method. (<b>d</b>) The localization error of the Newton’s iteration method.</p>
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<p>The localization error of the three strategies: localization directly, delete maximum, and distance selection.</p>
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<p>The average localization error of the four approaches: quadrilateral, least squares, maximum likelihood, and Newton’s iteration.</p>
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<p>The localization error of the four localization approaches: quadrilateral, least squares, maximum likelihood, and Newton’s iteration.</p>
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20 pages, 7855 KiB  
Article
Adaptive Ultra-Wideband/Pedestrian Dead Reckoning Localization Algorithm Based on Maximum Point-by-Point Distance
by Minglin Li and Songlin Liu
Electronics 2024, 13(24), 4987; https://doi.org/10.3390/electronics13244987 - 18 Dec 2024
Viewed by 471
Abstract
Positioning using ultra-wideband (UWB) signals can be used to achieve centimeter-level indoor positioning. UWB has been widely used in indoor localization, vehicle networking, industrial IoT, etc. However, due to non-line-of-sight (NLOS) and multipath interference problems, UWB cannot provide adequate position information, which affects [...] Read more.
Positioning using ultra-wideband (UWB) signals can be used to achieve centimeter-level indoor positioning. UWB has been widely used in indoor localization, vehicle networking, industrial IoT, etc. However, due to non-line-of-sight (NLOS) and multipath interference problems, UWB cannot provide adequate position information, which affects the final positioning accuracy. This paper proposes an adaptive UWB/PDR localization algorithm based on the maximum point-by-point distance to solve the problems of poor UWB performance and the error accumulation of the pedestrian dead reckoning (PDR) algorithm in NLOS scenarios that is used to enhance the robustness and accuracy of indoor positioning. Specifically, firstly, the cumulative distribution function (CDF) map of localization under normal conditions is obtained through offline pretraining and then compared with the CDF obtained when pedestrians are moving on the line. Then, the maximum point-by-point distance algorithm is used to identify the abnormal base stations. Then, the standard base stations are filtered out for localization. To further improve the localization accuracy, this paper proposes a UWB/PDR algorithm based on an improved adaptive extended Kalman filtering (EKF), which dynamically adjusts the position information through the adaptive factor, eliminates the influence of significant errors on the current position information and realizes multi-sensor fusion positioning. The realization results show that the algorithm in this paper has a solid ability to identify abnormal base stations and that the adaptive extended Kalman filtering (AEKF) algorithm is improved by 81.27%, 58.50%, 29.76%, and 18.06% compared to the PDR, UWB, EKF, and AEKF algorithms, respectively. Full article
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<p>Comparison of normal and abnormal localization CDFs for base stations.</p>
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<p>UWB/PDR fusion positioning system process.</p>
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<p>UWB station (<b>left</b>); UWB tag (<b>right</b>).</p>
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<p>Comparison test of normal base station and abnormal base station localization.</p>
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<p>Comparison of CDF for sub-base station ensemble localization and CDF for normal base station localization.</p>
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<p>Comparison of CDF for sub-base station ensemble localization and CDF for normal base station localization.</p>
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<p>Screening results for different base station scenarios.</p>
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<p>Screening results for different base station scenarios.</p>
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<p>Experimental scenario.</p>
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<p>Trajectory comparison results.</p>
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<p>CDF comparison of five algorithms.</p>
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<p>Specific positioning errors for each positioning test point.</p>
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<p>Office laboratory environment.</p>
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<p>Office laboratory environment in office.</p>
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<p>CDF comparison of five algorithms in an office.</p>
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<p>Specific positioning errors for each positioning test point in an office.</p>
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21 pages, 36735 KiB  
Article
Adaptive Navigation Based on Multi-Agent Received Signal Quality Monitoring Algorithm
by Hina Magsi, Madad Ali Shah, Ghulam E. Mustafa Abro, Sufyan Ali Memon, Abdul Aziz Memon, Arif Hussain and Wan-Gu Kim
Electronics 2024, 13(24), 4957; https://doi.org/10.3390/electronics13244957 - 16 Dec 2024
Viewed by 421
Abstract
In the era of industrial evolution, satellites are being viewed as swarm intelligence that does not rely on a single system but multiple constellations that collaborate autonomously. This has enhanced the potential of the Global Navigation Satellite System (GNSS) to contribute to improving [...] Read more.
In the era of industrial evolution, satellites are being viewed as swarm intelligence that does not rely on a single system but multiple constellations that collaborate autonomously. This has enhanced the potential of the Global Navigation Satellite System (GNSS) to contribute to improving position, navigation, and timing (PNT) services. However, multipath (MP) and non-line-of-sight (NLOS) receptions remain the prominent vulnerability for the GNSS in harsh environments. The aim of this research is to investigate the impact of MP and NLOS receptions on GNSS performance and then propose a Received Signal Quality Monitoring (RSQM) algorithm. The RSQM algorithm works in two ways. Initially, it performs a signal quality test based on a fuzzy inference system. The input parameters are carrier-to-noise ratio (CNR), Normalized Range Residuals (NRR), and Code–Carrier Divergence (CCD), and it computes the membership functions based on the Mamdani method and classifies the signal quality as LOS, NLOS, weak NLOS, and strong NLOS. Secondly, it performs an adaptive navigation strategy to exclude/mask the affected range measurements while considering the satellite geometry constraints (i.e., DOP2). For this purpose, comprehensive research to quantify the multi-constellation GNSS receiver with four constellation configurations (GPS, BeiDou, GLONASS, and Galileo) has been carried out in various operating environments. This RSQM-based GNSS receiver has the capability to identify signal quality and perform adaptive navigation accordingly to improve navigation performance. The results suggest that GNSS performance in terms of position error is improved from 5.4 m to 2.3 m on average in the complex urban environment. Combining the RSQM algorithm with the GNSS has great potential for the future industrial revolution (Industry 5.0), making things automatic and sustainable like autonomous vehicle operation. Full article
(This article belongs to the Special Issue Collaborative Intelligence in the Era of Industry 5.0)
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<p>Complete organization of the paper.</p>
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<p>Potential Vulnerabilities of satellite signal reception in urban environment. S1–S4 are satellites in the space from 1 to 4.</p>
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<p>Workflow of the paper.</p>
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<p>Candidate sites for Static experiments; (<b>a</b>) Best case environment, (<b>b</b>) Mediocre Multipath, (<b>c</b>) Worst Multipath (highlighted in box).</p>
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<p>Live images of moving candidate sites; (<b>a</b>) Complete route of moving experiment, (<b>b</b>) clear site, (<b>c</b>) sub-urban, (<b>d</b>) highly urban environment.</p>
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<p>Flow chart of the RSQM.</p>
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<p>Fuzzy inference system.</p>
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<p>Fuzzy logic memebrship functions.</p>
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<p>Positioning performance comparison of multi-constellation GNSS in dynamic (moving) mode. (<b>a</b>) Satellite Availability, (<b>b</b>) PDOP and (<b>c</b>) Position Error (m).</p>
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<p>Positioning performance comparison of multi-constellation GNSS.</p>
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<p>Satellite Signal Characteristics in Urban Canyon. (<b>a</b>) CNR (dB-Hz), (<b>b</b>) CCD (m) and (<b>c</b>) RR (m) for all three candidate sites clear open sky, moderately degraded and severe degraded.</p>
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<p>Histogram and normal distribution of CNR for all the environments (<b>a</b>) Clear open sky, (<b>b</b>) Degraded Environment and (<b>c</b>) Highly degraded environment.</p>
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<p>Histogram and normal distribution of CCD for all the environments (<b>a</b>) Clear open sky, (<b>b</b>) Degraded Environment and (<b>c</b>) Highly degraded environment.</p>
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<p>Histogram and normal distribution of CNR for all the environments (<b>a</b>) Clear open sky, (<b>b</b>) Degraded Environment and (<b>c</b>) Highly degraded environment.</p>
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<p>Performance of GNSS after mitigation strategy. (<b>a</b>) Satellite availability, (<b>b</b>) PDOP and (<b>c</b>) Position Error (m).</p>
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31 pages, 22621 KiB  
Article
A Ray-Tracing-Based Single-Site Localization Method for Non-Line-of-Sight Environments
by Shuo Hu, Lixin Guo and Zhongyu Liu
Sensors 2024, 24(24), 7925; https://doi.org/10.3390/s24247925 - 11 Dec 2024
Viewed by 463
Abstract
Localization accuracy in non-line-of-sight (NLOS) scenarios is often hindered by the complex nature of multipath propagation. Traditional approaches typically focus on NLOS node identification and error mitigation techniques. However, the intricacies of NLOS localization are intrinsically tied to propagation challenges. In this paper, [...] Read more.
Localization accuracy in non-line-of-sight (NLOS) scenarios is often hindered by the complex nature of multipath propagation. Traditional approaches typically focus on NLOS node identification and error mitigation techniques. However, the intricacies of NLOS localization are intrinsically tied to propagation challenges. In this paper, we propose a novel single-site localization method tailored for complex multipath NLOS environments, leveraging only angle-of-arrival (AOA) estimates in conjunction with a ray-tracing (RT) algorithm. The method transforms NLOS paths into equivalent line-of-sight (LOS) paths through the generation of generalized sources (GSs) via ray tracing. A novel weighting mechanism for GSs is introduced, which, when combined with an iteratively reweighted least squares (IRLS) estimator, significantly improves the localization accuracy of non-cooperative target sources. Furthermore, a multipath similarity displacement matrix (MSDM) is incorporated to enhance accuracy in regions with pronounced multipath fluctuations. Simulation results validate the efficacy of the proposed algorithm, achieving localization performance that approaches the Cramér–Rao lower bound (CRLB), even in challenging NLOS scenarios. Full article
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<p>A flowchart of the proposed RT algorithm.</p>
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<p>Binary tree structure of ray nodes.</p>
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<p>Schematic diagram of ray-splitting structure. Red nodes indicate split nodes that will be deleted, while blue nodes represent newly generated split nodes.</p>
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<p>Schematic diagram of ray tube determination and reception. Red lines represent virtual ray tubes, while blue lines indicate the edge rays of the ray tube.</p>
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<p>An overview of the overall technical roadmap of the RT-LBS algorithm.</p>
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<p>Power measurement system architecture and key equipment. The <b>upper half</b> of the figure is the block diagram of the channel sounder used in this paper. The <b>lower half</b> is the key equipment of the sounder, including the signal generator, power amplifier, spectrum analyzer, power supplier, RTK, and antennas.</p>
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<p>Localization test system architecture and key equipment. The <b>upper half</b> of the figure is the block diagram of the localization test system used in this paper. The <b>lower half</b> is the key equipment in the signal transmitter system, UCA direction-finding equipment, the Rx antenna array, and the RF processing circuit.</p>
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<p>Measurement scenario. (<b>a</b>) The raw point cloud image of the measurement scenario. (<b>b</b>) The geometric building model extracted from the point cloud.</p>
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<p>Measurement path and power distribution at (<b>a</b>) 3 GHz frequency, (<b>b</b>) 3.6 GHz frequency, (<b>c</b>) 4 GHz frequency, (<b>d</b>) 5 GHz frequency, and (<b>e</b>) 5.9 GHz frequency.</p>
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<p>Raw power measurement data and power measurement data after applying the sliding filter at (<b>a</b>) 3 GHz frequency, (<b>b</b>) 3.6 GHz frequency, (<b>c</b>) 4 GHz frequency, (<b>d</b>) 5 GHz frequency, and (<b>e</b>) 5.9 GHz frequency.</p>
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<p>RSS predictions and measurements in the scenario at (<b>a</b>) 3 GHz frequency, (<b>b</b>) 3.6 GHz frequency, (<b>c</b>) 4 GHz frequency, (<b>d</b>) 5 GHz frequency, and (<b>e</b>) 5.9 GHz frequency. The basic RT method refers to the approach presented in [<a href="#B39-sensors-24-07925" class="html-bibr">39</a>].</p>
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<p>The angle measurement scenario and the positions of the NCTS (denoted by T1, T2, and T3) and sensor (denoted by R).</p>
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<p>The AOA spectrum measured for the source located at T1.</p>
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<p>The AOA spectrum measured for the source located at T2.</p>
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<p>The AOA spectrum measured for the source located at T3.</p>
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<p>Comparison between measured AS and simulated multipath at (<b>a</b>) T1 position, (<b>b</b>) T2 position, and (<b>c</b>) T3 position.</p>
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<p>NCTS and sensor positions and a geometrical map of the scenario. The line segments represent the multipath between the source and the sensor, distinguished using different colors.</p>
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<p>A comparison of the proposed localization algorithm’s accuracy with the CRLB. (<b>a</b>) The source at location A; (<b>b</b>) the source at location B; (<b>c</b>) the source at location C.</p>
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<p>Localization error at point A with different AOA and RSSD errors.</p>
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<p>Localization error at point B with different AOA and RSSD errors.</p>
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<p>Localization error at point C with different AOA and RSSD errors.</p>
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<p>MSD distribution at (<b>a</b>) 0.1° AOA error, (<b>b</b>) 0.5°AOA error, (<b>c</b>) 1°AOA error, (<b>d</b>) 2°AOA error, (<b>e</b>) 4°AOA error, and (<b>f</b>) 6°AOA error.</p>
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<p>MSD distribution at (<b>a</b>) 0.1° AOA error, (<b>b</b>) 0.5°AOA error, (<b>c</b>) 1°AOA error, (<b>d</b>) 2°AOA error, (<b>e</b>) 4°AOA error, and (<b>f</b>) 6°AOA error.</p>
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<p>Schematic diagram of displacement compensation expansion method.</p>
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<p>Planar Localization Error Distribution with 0.1° AOA error. (<b>a</b>) Original localization algorithm; (<b>b</b>) localization algorithm with MSDM.</p>
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<p>Planar Localization Error Distribution with 0.5° AOA error. (<b>a</b>) Original localization algorithm; (<b>b</b>) localization algorithm with MSDM.</p>
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<p>Planar Localization Error Distribution with 1° AOA error. (<b>a</b>) Original localization algorithm; (<b>b</b>) localization algorithm with MSDM.</p>
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<p>Planar Localization Error Distribution with 2° AOA error. (<b>a</b>) Original localization algorithm; (<b>b</b>) localization algorithm with MSDM.</p>
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<p>Planar Localization Error Distribution with 4° AOA error. (<b>a</b>) Original localization algorithm; (<b>b</b>) localization algorithm with MSDM.</p>
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<p>Planar Localization Error Distribution with 6° AOA error. (<b>a</b>) Original localization algorithm; (<b>b</b>) localization algorithm with MSDM.</p>
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<p>Schematic diagram of GPU acceleration algorithm.</p>
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<p>Power coverage map.</p>
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<p>Efficiency comparison of different acceleration methods.</p>
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25 pages, 8887 KiB  
Article
A Gaussian Process-Enhanced Non-Linear Function and Bayesian Convolution–Bayesian Long Term Short Memory Based Ultra-Wideband Range Error Mitigation Method for Line of Sight and Non-Line of Sight Scenarios
by A. S. M. Sharifuzzaman Sagar, Samsil Arefin, Eesun Moon, Md Masud Pervez Prince, L. Minh Dang, Amir Haider and Hyung Seok Kim
Mathematics 2024, 12(23), 3866; https://doi.org/10.3390/math12233866 - 9 Dec 2024
Viewed by 666
Abstract
Relative positioning accuracy between two devices is dependent on the precise range measurements. Ultra-wideband (UWB) technology is one of the popular and widely used technologies to achieve centimeter-level accuracy in range measurement. Nevertheless, harsh indoor environments, multipath issues, reflections, and bias due to [...] Read more.
Relative positioning accuracy between two devices is dependent on the precise range measurements. Ultra-wideband (UWB) technology is one of the popular and widely used technologies to achieve centimeter-level accuracy in range measurement. Nevertheless, harsh indoor environments, multipath issues, reflections, and bias due to antenna delay degrade the range measurement performance in line-of-sight (LOS) and non-line-of-sight (NLOS) scenarios. This article proposes an efficient and robust method to mitigate range measurement error in LOS and NLOS conditions by combining the latest artificial intelligence technology. A GP-enhanced non-linear function is proposed to mitigate the range bias in LOS scenarios. Moreover, NLOS identification based on the sliding window and Bayesian Conv-BLSTM method is utilized to mitigate range error due to the non-line-of-sight conditions. A novel spatial–temporal attention module is proposed to improve the performance of the proposed model. The epistemic and aleatoric uncertainty estimation method is also introduced to determine the robustness of the proposed model for environment variance. Furthermore, moving average and min-max removing methods are utilized to minimize the standard deviation in the range measurements in both scenarios. Extensive experimentation with different settings and configurations has proven the effectiveness of our methodology and demonstrated the feasibility of our robust UWB range error mitigation for LOS and NLOS scenarios. Full article
(This article belongs to the Special Issue Modeling and Simulation in Engineering, 3rd Edition)
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<p>Range measurement error represented in the box chart for four different NLOS propagation scenarios, which can be found indoors. The square box represents the mean, and the dashes represent the maximum and minimum range error observed during the data acquisition.</p>
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<p>The overall system architecture of the proposed UWB range measurement error mitigation for both LOS and NLOS environments.</p>
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<p>The overall architecture of Conv-BLSTM layer and the proposed attention module.</p>
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<p>Experiment with line of sight for indoor ground environment.</p>
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<p>Experiment with line of sight for lab environment.</p>
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<p>Experiment with line of sight for Park A environment.</p>
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<p>Experiment with line of sight for Park B environment.</p>
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<p>The training and validation accuracy of the proposed model, along with their losses.</p>
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<p>The comparison of different models for NLOS identification in UWB devices.</p>
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<p>Experiment with non-line-of-sight conditions with human obstacle.</p>
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<p>Experiment with non-line-of-sight conditions with wood obstacle.</p>
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<p>Experiment with non-line-of-sight conditions with partial metal obstacle.</p>
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<p>Experiment with non-line-of-sight conditions with wall obstacle.</p>
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<p>Uncertainty estimation plots with respect to the proposed model’s prediction; (<b>a</b>) the epistemic uncertainty of the proposed model, (<b>b</b>) the aleatoric uncertainty or inherent noise of data calculated using the proposed model.</p>
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19 pages, 3755 KiB  
Article
Experimental Investigation of the Optical Nonlinearity of Laser-Ablated Titanium Dioxide Nanoparticles Using Femtosecond Laser Light Pulses
by Fatma Abdel Samad, Mohammed Ali Jasim, Alaa Mahmoud, Yasmin Abd El-Salam, Hamza Qayyum, Retna Apsari and Tarek Mohamed
Nanomaterials 2024, 14(23), 1940; https://doi.org/10.3390/nano14231940 - 3 Dec 2024
Viewed by 721
Abstract
In this report, the nonlinear optical (NLO) properties of titanium dioxide nanoparticles (TiO2 NPs) have been explored experimentally using femtosecond laser light along with the Z-scan approach. The synthesis of TiO2 NPs was carried out in distilled water through nanosecond second [...] Read more.
In this report, the nonlinear optical (NLO) properties of titanium dioxide nanoparticles (TiO2 NPs) have been explored experimentally using femtosecond laser light along with the Z-scan approach. The synthesis of TiO2 NPs was carried out in distilled water through nanosecond second harmonic Nd:YAG laser ablation. Characterization of the TiO2 NPs colloids was conducted using UV-visible absorption spectroscopy, transmission electron microscopy (TEM), inductively coupled plasma (ICP), and energy-dispersive X-ray spectroscopy (EDX). The TEM analysis indicated that the size distribution and average particle size of the TiO2 NPs varied from 8.3 nm to 19.1 nm, depending on the laser ablation duration. The third-order NLO properties of the synthesized TiO2 NPs were examined at different excitation laser wavelengths and incident powers through both open- and closed-aperture Z-scan techniques, utilizing a laser pulse duration of 100 fs and a high repetition rate of 80 MHz. The nonlinear absorption (NLA) coefficient and nonlinear refractive (NLR) index of the TiO2 NPs colloidal solutions were found to be influenced by the incident power, excitation wavelength, average size, and concentration of TiO2 NPs. Maximum values of 4.93 × 10⁻⁹ cm/W for the NLA coefficient and 15.39 × 10⁻15 cm2/W for the NLR index were observed at an excitation wavelength of 800 nm, an incident power of 0.6 W, and an ablation time of 15 min. The optical limiting (OL) effects of the TiO2 NPs solution at different ablation times were investigated and revealed to be concentration and average size dependent. An increase in concentration results in a more limiting effect. Full article
(This article belongs to the Topic Laser Processing of Metallic Materials)
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<p>Laser ablation setup for preparing TiO<sub>2</sub> NPs colloids via a 532-nm Nd:YAG laser.</p>
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<p>Z-scan experimental setup. L, convex lens; A, attenuator; I, Iris; S, TiO<sub>2</sub> NPs sample; PM, power meter.</p>
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<p>Spectral absorption of TiO<sub>2</sub> NP colloidal solutions as a function of wavelength at different ablation times.</p>
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<p>(<b>a</b>–<b>c</b>) show the energy band gaps that were obtained by extrapolating the straight line of Tauc’s plot of TiO<sub>2</sub> nanocolloids at various ablation times.</p>
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<p>(<b>a</b>–<b>c</b>) depict the size distributions of TiO<sub>2</sub> NPs colloids that were synthesized using various ablation times of 5 min, 10 min, and 15 min, respectively.</p>
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<p>EDX spectra of the TiO<sub>2</sub> NP colloid and inset ZAF Method Standardless Quantitative Analysis of TiO<sub>2</sub> NPs.</p>
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<p>(<b>a</b>–<b>c</b>) OA Z-scan measurements of TiO<sub>2</sub> NP colloids with different ablation times and incident powers at an 800 nm excitation wavelength. (<b>d</b>) Dependence of the NLA coefficient on the incident laser power at an 800 nm excitation wavelength.</p>
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<p>(<b>a</b>–<b>c</b>) OA Z-scan experimental data of TiO<sub>2</sub> NP colloidal solutions with different ablation times and excitation wavelengths at 1 W incident power. (<b>d</b>) Relationship between the excitation wavelength and NLA coefficient at 1 W incident laser power.</p>
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<p>(<b>a</b>) OA Z-scan experimental data of TiO<sub>2</sub> NP colloidal solutions with different ablation times and a constant excitation wavelength of 800 nm and an incident power of 1 W. (<b>b</b>) Dependence between the ablation time and the NLA coefficient.</p>
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<p>(<b>a</b>–<b>c</b>) CA Z-scan measurements for TiO<sub>2</sub> NP colloids at different incident powers and ablation times at an excitation wavelength of 800 nm. The symbols represent the experimental data, and the solid curves are the fits obtained via Equations (6) and (7). (<b>d</b>) Relationship between the NLR index and incident power at each ablation time.</p>
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<p>(<b>a</b>–<b>c</b>) CA Z-scan transmission of TiO<sub>2</sub> NP colloids at different excitation wavelengths and ablation times; (<b>d</b>) relationship values of n<sub>2</sub> for TiO<sub>2</sub> NP colloidal solutions with different ablation times at 1 W incident power. The dots represent the experimental data, and the solid curves are linear fits.</p>
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<p>(<b>a</b>) Plot of CA Z-scan measurements of different ablation times of 5 min, 10 min, and 15 min at 800 nm excitation wavelength and 1 W incident power. (<b>b</b>) Dependence between the measured n<sub>2</sub> and ablation time at a 1 W incident power and 800 nm excitation wavelength. The dots represent the experimental data, and the solid lines are linear fits.</p>
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<p>Optical limiting of the TiO<sub>2</sub> NP colloids at ablation times of 5 min, 10 min, and 15 min and an 800 nm excitation wavelength.</p>
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19 pages, 9444 KiB  
Article
Enhanced 3D Outdoor Positioning Method Based on Adaptive Kalman Filter and Kernel Density Estimation for 6G Wireless System
by Kyounghun Kim, Seongwoo Lee, Byungsun Hwang, Jinwook Kim, Joonho Seon, Soohyun Kim, Youngghyu Sun and Jinyoung Kim
Electronics 2024, 13(23), 4623; https://doi.org/10.3390/electronics13234623 - 23 Nov 2024
Viewed by 522
Abstract
The implementation of accurate positioning methods in both line-of-sight (LOS) and non-line-of-sight (NLOS) environments has been emphasized for seamless 6G application services. In LOS environments with unobstructed paths between the transmitter and receiver, accurate tracking essential for seamless 6G services is achievable. However, [...] Read more.
The implementation of accurate positioning methods in both line-of-sight (LOS) and non-line-of-sight (NLOS) environments has been emphasized for seamless 6G application services. In LOS environments with unobstructed paths between the transmitter and receiver, accurate tracking essential for seamless 6G services is achievable. However, accurate three-dimensional (3D) outdoor positioning has been challenging to achieve in NLOS environments where positioning accuracy may be severely degraded. In this paper, a novel 3D outdoor positioning method considering both LOS and NLOS environments is proposed. Considering the practical positioning systems, the data received from satellites often contain null values and outliers. Thus, a kernel density estimation (KDE)-based outlier removal method is used for effectively detecting the null values and outliers through temporal correlation analysis. A dilution of precision-based adaptive Kalman filter (DOP-AKF) is proposed to mitigate the effects of an NLOS environment. In the proposed method, the DOP-AKF can optimize the performance of the 3D positioning system that dynamically adapts to complex environments. Experimental results show that the proposed method can improve 3D positioning accuracy by up to 18.84% compared to conventional methods. Therefore, the proposed approach can be suggested as a promising solution for 3D outdoor positioning in 6G wireless systems. Full article
(This article belongs to the Special Issue 5G and 6G Wireless Systems: Challenges, Insights, and Opportunities)
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<p>Schematic diagram of the conventional outdoor positioning method.</p>
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<p>Flowchart of the CKF.</p>
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<p>Schematic diagram of the proposed 3D outdoor positioning method.</p>
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<p>Constellation of different satellite geometries: (<b>a</b>) low DOP value with uniform satellite distribution; (<b>b</b>) high DOP value with an un-uniform satellite distribution.</p>
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<p>Flowchart of the proposed DOP-AKF.</p>
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<p>Experiment system components with ZED-F9P: (<b>a</b>) base in DGPS mode (<b>b</b>); rover in DGPS mode and RTK.</p>
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<p>Experimental route: (<b>a</b>) mixed urban environment with high-rise and low-rise buildings; (<b>b</b>) bridge over a flat terrain transitioning from LOS to NLOS conditions.</p>
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<p>Results of KDE-based outlier removal method: (<b>a</b>) measurement of GNSS path results with outliers; (<b>b</b>) comparison of the KFs [<a href="#B4-electronics-13-04623" class="html-bibr">4</a>,<a href="#B16-electronics-13-04623" class="html-bibr">16</a>] with and without outlier removal via KDE.</p>
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<p>Measured altitude and VDOP in Scenario #3.</p>
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<p>A comparison of positioning errors in DOP-AKF.</p>
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<p>Positioning errors for the conventional [<a href="#B4-electronics-13-04623" class="html-bibr">4</a>,<a href="#B16-electronics-13-04623" class="html-bibr">16</a>] and proposed KF algorithms in scenario #3: (<b>a</b>) horizontal positioning error; (<b>b</b>) altitude positioning error.</p>
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<p>Positioning errors for the conventional [<a href="#B4-electronics-13-04623" class="html-bibr">4</a>,<a href="#B16-electronics-13-04623" class="html-bibr">16</a>] and proposed KF algorithms in scenario #4: (<b>a</b>) horizontal positioning error; (<b>b</b>) altitude positioning error.</p>
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<p>Measured altitude and VDOP in scenario #5.</p>
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<p>Positioning errors for the conventional [<a href="#B4-electronics-13-04623" class="html-bibr">4</a>,<a href="#B16-electronics-13-04623" class="html-bibr">16</a>] and proposed KF algorithms in scenario #5.</p>
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28 pages, 5305 KiB  
Article
Machine Learning-Based Environment-Aware GNSS Integrity Monitoring for Urban Air Mobility
by Oguz Kagan Isik, Ivan Petrunin and Antonios Tsourdos
Drones 2024, 8(11), 690; https://doi.org/10.3390/drones8110690 - 19 Nov 2024
Viewed by 898
Abstract
The increasing deployment of unmanned aerial vehicles (UAVs) in urban air mobility (UAM) necessitates robust Global Navigation Satellite System (GNSS) integrity monitoring that can adapt to the complexities of urban environments. The traditional integrity monitoring approaches struggle with the unique challenges posed by [...] Read more.
The increasing deployment of unmanned aerial vehicles (UAVs) in urban air mobility (UAM) necessitates robust Global Navigation Satellite System (GNSS) integrity monitoring that can adapt to the complexities of urban environments. The traditional integrity monitoring approaches struggle with the unique challenges posed by urban settings, such as frequent signal blockages, multipath reflections, and Non-Line-of-Sight (NLoS) receptions. This study introduces a novel machine learning-based GNSS integrity monitoring framework that incorporates environment recognition to create environment-specific error models. Using a comprehensive Hardware-in-the-Loop (HIL) simulation setup, extensive data were generated for suburban, urban, and urban canyon environments to train and validate the models. The proposed Natural Gradient Boosting Protection Level (NGB-PL) method, leveraging the uncertainty prediction capabilities of the NGB algorithm, demonstrated superior performance in estimating protection levels compared to the classical methods. The results indicated that environment-specific models significantly enhanced both accuracy and system availability, particularly in challenging urban scenarios. The integration of environment recognition into the integrity monitoring framework allows the dynamic adaptation to varying environmental conditions, thus substantially improving the reliability and safety of UAV operations in urban air mobility applications. This research offers a novel protection level (PL) estimation method and a framework tailored to GNSS integrity monitoring for UAM, which enhances the availability with narrower PL bound gaps without yielding higher integrity risks. Full article
(This article belongs to the Special Issue Recent Advances in UAV Navigation)
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<p>Proposed integrity monitoring framework.</p>
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<p>HIL simulation setup.</p>
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<p>Suburban environment model.</p>
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<p>Urban environment model.</p>
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<p>Urban canyon environment model.</p>
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<p>Simulated trajectory.</p>
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<p>Stanford-ESA integrity diagram [<a href="#B49-drones-08-00690" class="html-bibr">49</a>].</p>
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<p>HPL estimations in suburban scenario with (<b>a</b>) classical approach (<b>b</b>) IBPL approach.</p>
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<p>HPL estimations in urban scenario with (<b>a</b>) classical approach (<b>b</b>) IBPL approach.</p>
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<p>HPL estimations in urban canyon scenario with (<b>a</b>) classical approach (<b>b</b>) IBPL approach.</p>
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<p>VPL estimations in suburban scenario with (<b>a</b>) classical approach (<b>b</b>) IBPL approach.</p>
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<p>VPL estimations in urban scenario with (<b>a</b>) classical approach (<b>b</b>) IBPL approach.</p>
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<p>VPL estimations in urban canyon scenario with (<b>a</b>) classical approach (<b>b</b>) IBPL approach.</p>
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<p>PE and PLs in suburban scenario with test data (<b>a</b>) horizontal axis (<b>b</b>) vertical axis.</p>
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<p>PE and PLs in urban scenario with test data (<b>a</b>) horizontal axis (<b>b</b>) vertical axis.</p>
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<p>PE and PLs in urban canyon scenario with test data (<b>a</b>) horizontal axis (<b>b</b>) vertical axis.</p>
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<p>PE and PLs in suburban scenario with validation data (<b>a</b>) horizontal axis (<b>b</b>) vertical axis.</p>
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<p>PE and PLs in urban scenario with validation data (<b>a</b>) horizontal axis (<b>b</b>) vertical axis.</p>
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<p>PE and PLs in urban canyon scenario with validation data (<b>a</b>) horizontal axis (<b>b</b>) vertical axis.</p>
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21 pages, 5929 KiB  
Article
Improved Kalman Filtering Algorithm Based on Levenberg–Marquart Algorithm in Ultra-Wideband Indoor Positioning
by Changping Xie, Xinjian Fang and Xu Yang
Sensors 2024, 24(22), 7213; https://doi.org/10.3390/s24227213 - 11 Nov 2024
Viewed by 658
Abstract
To improve the current indoor positioning algorithms, which have insufficient positioning accuracy, an ultra-wideband (UWB) positioning algorithm based on the Levenberg–Marquardt algorithm with improved Kalman filtering is proposed. An alternative double-sided two-way ranging (ADS-TWR) algorithm is used to obtain the distance from the [...] Read more.
To improve the current indoor positioning algorithms, which have insufficient positioning accuracy, an ultra-wideband (UWB) positioning algorithm based on the Levenberg–Marquardt algorithm with improved Kalman filtering is proposed. An alternative double-sided two-way ranging (ADS-TWR) algorithm is used to obtain the distance from the UWB tag to each base station and calculate the initial position of the tag by the least squares method. The Levenberg–Marquardt algorithm is used to correct the covariance matrix of the Kalman filter, and the improved Kalman filtering algorithm is used to filter the initial position to obtain the final position of the tag. The feasibility and effectiveness of the algorithm are verified by MATLAB simulation. Finally, the UWB positioning system is constructed, and the improved Kalman filter algorithm is experimentally verified in LOS and NLOS environments. The average X-axis and the Y-axis positioning errors in the LOS environment are 6.9 mm and 5.4 mm, respectively, with a root mean square error of 10.8 mm. The average positioning errors for the X-axis and Y-axis in the NLOS environment are 20.8 mm and 18.0 mm, respectively, while the root mean square error is 28.9 mm. The experimental results show that the improved algorithm has high accuracy and good stability. At the same time, it can effectively improve the convergence speed of the Kalman filter. Full article
(This article belongs to the Section Navigation and Positioning)
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<p>Schematic diagram of the asymmetric bidirectional bilateral ranking algorithm.</p>
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<p>Flowchart of the model.</p>
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<p>Simulated positioning results of different algorithms.</p>
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<p>(<b>a</b>) Comparison of the X-axis error; (<b>b</b>) comparison of the Y-axis error.</p>
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<p>Location performance of the five algorithms under different noise levels.</p>
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<p>(<b>a</b>) UWB positioning base station; (<b>b</b>) UWB positioning tag.</p>
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<p>(<b>a</b>) Experimental setup diagram; (<b>b</b>) UWB base station and tag distribution.</p>
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<p>Positioning scatterplot in LOS environment.</p>
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<p>(<b>a</b>) X-axis error in LOS environment; (<b>b</b>) Y-axis error in LOS environment.</p>
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<p>UWB base station and tag distribution map in NLOS environment.</p>
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<p>Scatter plot of localization in NLOS environment.</p>
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<p>(<b>a</b>) X-axis error in NLOS environment; (<b>b</b>) Y-axis error in NLOS environment.</p>
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26 pages, 9809 KiB  
Article
Tightly Coupled LIDAR/IMU/UWB Fusion via Resilient Factor Graph for Quadruped Robot Positioning
by Yujin Kuang, Tongfei Hu, Mujiao Ouyang, Yuan Yang and Xiaoguo Zhang
Remote Sens. 2024, 16(22), 4171; https://doi.org/10.3390/rs16224171 - 8 Nov 2024
Viewed by 1242
Abstract
Continuous accurate positioning in global navigation satellite system (GNSS)-denied environments is essential for robot navigation. Significant advances have been made with light detection and ranging (LiDAR)-inertial measurement unit (IMU) techniques, especially in challenging environments with varying lighting and other complexities. However, the LiDAR/IMU [...] Read more.
Continuous accurate positioning in global navigation satellite system (GNSS)-denied environments is essential for robot navigation. Significant advances have been made with light detection and ranging (LiDAR)-inertial measurement unit (IMU) techniques, especially in challenging environments with varying lighting and other complexities. However, the LiDAR/IMU method relies on a recursive positioning principle, resulting in the gradual accumulation and dispersion of errors over time. To address these challenges, this study proposes a tightly coupled LiDAR/IMU/UWB fusion approach that integrates an ultra-wideband (UWB) positioning technique. First, a lightweight point cloud segmentation and constraint algorithm is designed to minimize elevation errors and reduce computational demands. Second, a multi-decision non-line-of-sight (NLOS) recognition module using information entropy is employed to mitigate NLOS errors. Finally, a tightly coupled framework via a resilient mechanism is proposed to achieve reliable position estimation for quadruped robots. Experimental results demonstrate that our system provides robust positioning results even in LiDAR-limited and NLOS conditions, maintaining low time costs. Full article
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<p>Overview of the proposed tightly coupled LiDAR/IMU/UWB positioning system.</p>
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<p>Triangular-based ground point cloud exclusion diagram.</p>
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<p>Concentric circle model of ground segmentation. (<b>a</b>) traditional model on the left; (<b>b</b>) improved model on the right.</p>
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<p>Schematic of the proposed LiDAR/IMU/UWB factor graph model of quadruped robot.</p>
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<p>Experimental equipment: (<b>a</b>) Quadruped robot with sensors (Unitree, Hangzhou, China); (<b>b</b>) UWB hardware module (Nooploop, Nanjing, China); (<b>c</b>) Total station (Starfish, Foshan, China).</p>
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<p>UWB anchor deployment and key points of the mobile experiment.</p>
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<p>Experiment layout. The red triangles indicate the locations of the UWB anchor stations. The blue dot represents the location of the robot tag. The black line shows the reference track.</p>
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<p>Comparison of running time for processing a frame of point cloud by different algorithms across various datasets.</p>
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<p>Error comparison of positioning results for different algorithms across various datasets.</p>
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<p>Comparison of point cloud segmentation results. The pink line represents the fitted ground point cloud. (<b>a</b>) Field diagram of a typical complex environment with multiple steps and curbs. (<b>b</b>) Segmentation result using a traditional point cloud processing algorithm (<b>c</b>) Segmentation result using the proposed algorithm.</p>
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<p>IMU Allan variance analysis results. (<b>a</b>) Accelerometer. (<b>b</b>) Gyroscope.</p>
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<p>The result of distance measurement error optimization.</p>
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<p>Changes in the data curve for each decision criterion. (<b>a</b>) Signal strength difference curve for each anchor station; (<b>b</b>) Distance signal difference curve for each anchor station.</p>
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<p>LOS/NLOS discrimination based on information entropy.</p>
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<p>Two-dimensional trajectory comparisons in a parking lot scenario using LS, EKF, LIU, LIUT, and our method.</p>
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<p>Comparison of error results of different positioning algorithms.</p>
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<p>Three-dimensional trajectory coparions in parking lot scenario using LIU, LIUT and our method.</p>
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<p>Comparison of z-axis results of different positioning algorithms.</p>
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<p>Indoor complex environment and corresponding positioning results.</p>
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14 pages, 560 KiB  
Article
A Design of NLOS Communication Scheme Based on SC-FDE with Cyclic Suffix for UAV Payload Communication
by Peng Wang, Xin Xiang, Rui Wang, Pengyu Dong and Qiao Li
Drones 2024, 8(11), 648; https://doi.org/10.3390/drones8110648 - 6 Nov 2024
Viewed by 698
Abstract
Non-line-of-sight (NLOS) communication with severe loss always leads to performance degradation in unmanned aerial vehicle (UAV) payload communication. In this paper, a UAV NLOS communication scheme based on single-carrier frequency domain equalization with cyclic prefix and cyclic suffix (CP/CS-SC-FDE) is designed. First, the [...] Read more.
Non-line-of-sight (NLOS) communication with severe loss always leads to performance degradation in unmanned aerial vehicle (UAV) payload communication. In this paper, a UAV NLOS communication scheme based on single-carrier frequency domain equalization with cyclic prefix and cyclic suffix (CP/CS-SC-FDE) is designed. First, the reasons behind the generation of later intersymbol interference (LISI) in UAV NLOS communication are investigated. Then, the frame structure of conventional single-carrier frequency domain equalization with cyclic prefix (CP-SC-FDE) is improved, and the UAV NLOS communication frame structure based on cyclic prefix (CP) and cyclic suffix (CS) is designed. Furthermore, a channel estimation algorithm applicable to this scheme is proposed. The numerical results show that this UAV communication scheme can eliminate intersymbol interference (ISI) in NLOS communication. Compared with the conventional CP-SC-FDE system, this scheme can achieve excellent performance in the Rayleigh channel and other standard NLOS channels. In the CP/CS-SC-FDE system, the BER result is similar to that under ideal synchronization. Full article
(This article belongs to the Section Drone Communications)
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<p>The transceiver structure of the CP-SC-FDE.</p>
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<p>The block of the CP-SC-FDE and CP/CS-SC-FDE.</p>
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<p>FFT region in LOS and NLOS channel based on CP-SC-FDE.</p>
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<p>FFT region in LOS and NLOS channel based on CP/CS-SC-FDE.</p>
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<p>The CIR of three channels of the first simulation.</p>
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<p>The sliding correlation value for time synchronization.</p>
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<p>The channel estimation output in CP-SC-FDE.</p>
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<p>The channel estimation output in CP/CS-SC-FDE.</p>
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<p>The BER curve of CP/CS-SC-FDE compared with CP-SC-FDE in Rayleigh fading channel.</p>
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<p>The BER curve of CP/CS-SC-FDE compared with CP-SC-FDE in COST207-BU channel and TDL-C channel.</p>
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16 pages, 2929 KiB  
Article
TDOA-AOA Localization Algorithm for 5G Intelligent Reflecting Surfaces
by Yuexia Zhang, Changbao Liu, Yuanshuo Gang and Yu Wang
Electronics 2024, 13(22), 4347; https://doi.org/10.3390/electronics13224347 - 6 Nov 2024
Viewed by 721
Abstract
5G positioning technology has become deeply integrated into daily life. However, in wireless signal propagation environments, there may exist non-line-of-sight (NLOS) conditions, which lead to signal blockage and subsequently hinder the provision of positioning services. To address this issue, this paper proposes an [...] Read more.
5G positioning technology has become deeply integrated into daily life. However, in wireless signal propagation environments, there may exist non-line-of-sight (NLOS) conditions, which lead to signal blockage and subsequently hinder the provision of positioning services. To address this issue, this paper proposes an intelligent reflecting surface (IRS) NLOS time difference of arrival–angle of arrival (TDOA-AOA) localization (INTAL) algorithm. First, the algorithm constructs a system model for 5G IRS localization, effectively overcoming the challenges of positioning in NLOS paths. Then, by applying the multiple signal classification algorithm to estimate the time delay and angle, and using the Chan algorithm to obtain the user’s estimated coordinates, an optimization problem is formulated to minimize the distance between the estimated and actual coordinates. The tent–snake optimization algorithm is employed to solve this optimization problem, thereby reducing localization errors. Finally, simulations demonstrate that the INTAL algorithm outperforms the snake optimization (SO) algorithm and the gray wolf optimization (GWO) algorithm under the same conditions, reducing the localization error by 56% and 60% on average, respectively. Additionally, when the signal-to-noise ratio is 30 dB, the localization error of the INTAL algorithm is only 0.2968 m, while the errors for the SO and GWO algorithms are 0.6733 m and 0.7398 m, respectively. This further proves the significant improvement of the algorithm in terms of localization accuracy. Full article
(This article belongs to the Special Issue New Advances in Navigation and Positioning Systems)
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<p>Illustration of GIL system model.</p>
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<p>Illustration of US-IRS signal propagation.</p>
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<p>Illustration of the pitch angle relationship between US and IRS.</p>
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<p>Flowchart of the tent–SO algorithm.</p>
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<p>Variation in fitness with iterations.</p>
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<p>Three-dimensional localization results.</p>
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<p>IRS position and positioning error analysis.</p>
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<p>Positioning error under different numbers of snapshots and varying SNRs.</p>
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<p>Analysis of positioning errors for different algorithms under varying SNRs.</p>
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<p>Positioning error with different numbers of IRSs under varying SNRs.</p>
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13 pages, 5013 KiB  
Article
Influence of Target Surface BRDF on Non-Line-of-Sight Imaging
by Yufeng Yang, Kailei Yang and Ao Zhang
J. Imaging 2024, 10(11), 273; https://doi.org/10.3390/jimaging10110273 - 29 Oct 2024
Viewed by 871
Abstract
The surface material of an object is a key factor that affects non-line-of-sight (NLOS) imaging. In this paper, we introduce the bidirectional reflectance distribution function (BRDF) into NLOS imaging to study how the target surface material influences the quality of NLOS images. First, [...] Read more.
The surface material of an object is a key factor that affects non-line-of-sight (NLOS) imaging. In this paper, we introduce the bidirectional reflectance distribution function (BRDF) into NLOS imaging to study how the target surface material influences the quality of NLOS images. First, the BRDF of two surface materials (aluminized insulation material and white paint board) was modeled using deep neural networks and compared with a five-parameter empirical model to validate the method’s accuracy. The method was then applied to fit BRDF data for different common materials. Finally, NLOS target simulations with varying surface materials were reconstructed using the confocal diffusion tomography algorithm. The reconstructed NLOS images were classified via a convolutional neural network to assess how different surface materials impacted imaging quality. The results show that image clarity improves when decreasing the specular reflection and increasing the diffuse reflection, with the best results obtained for surfaces exhibiting a high diffuse reflection and no specular reflection. Full article
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<p>Geometric diagram of BRDF.</p>
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<p>Model of CDT imaging.</p>
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<p>Modeling of BRDF based on deep neural network.</p>
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<p>Schematic diagram of convolution operation.</p>
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<p>Comparison of BRDF data for aluminized insulation material under two models. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>θ</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> = 30°; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>θ</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> = 45°; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>θ</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> = 60°.</p>
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<p>Comparison of BRDF data for white paint board under two models. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>θ</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> = 30°; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>θ</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> = 45°; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>θ</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> = 60°.</p>
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<p>BRDF fitting results for different target objects. (<b>a</b>) BRDF fitting results for seven target objects; (<b>b</b>) BRDF for three instances.</p>
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<p>Reconstruction results of different objects.</p>
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<p>Reconstruction results of different objects.</p>
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<p>Classification results of different BRDF surface targets.</p>
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21 pages, 5788 KiB  
Article
Using Femtosecond Laser Light to Investigate the Concentration- and Size-Dependent Nonlinear Optical Properties of Laser-Ablated CuO Quantum Dots
by Mohamed Ashour, Rasha Ibrahim, Yasmin Abd El-Salam, Fatma Abdel Samad, Alaa Mahmoud and Tarek Mohamed
Nanomaterials 2024, 14(20), 1674; https://doi.org/10.3390/nano14201674 - 18 Oct 2024
Viewed by 813
Abstract
In this work, the nonlinear optical (NLO) properties of CuO nanoparticles (CuO NPs) were studied experimentally using the pulsed laser ablation (PLA) technique. A nanosecond Nd: YAG laser was employed as the ablation excitation source to create CuO NPs in distilled water. Various [...] Read more.
In this work, the nonlinear optical (NLO) properties of CuO nanoparticles (CuO NPs) were studied experimentally using the pulsed laser ablation (PLA) technique. A nanosecond Nd: YAG laser was employed as the ablation excitation source to create CuO NPs in distilled water. Various CuO NPs samples were prepared at ablation periods of 20, 30, and 40 min. Utilizing HR-TEM, the structure of the synthesized CuO NPs samples was verified. In addition, a UV–VIS spectrophotometer was used to investigate the linear features of the samples. The Z-scan technique was utilized to explore the NLO properties of CuO NPs samples, including the nonlinear absorption coefficient (β) and nonlinear refractive index (n2). An experimental study on the NLO features was conducted at a variety of excitation wavelengths (750–850 nm), average excitation powers (0.8–1.2 W), and CuO NPs sample concentrations and sizes. The reverse saturable absorption (RSA) behavior of all CuO NPs samples differed with the excitation wavelength and average excitation power. In addition, the CuO NPs samples demonstrated excellent optical limiters at various excitation wavelengths, with limitations dependent on the size and concentration of CuO NPs. Full article
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Figure 1

Figure 1
<p>Schematic preview of the pulsed laser ablation process for synthesizing CuO NPs via a nanosecond Nd: YAG pulsed laser.</p>
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<p>The size distribution of the CuO NPs ablated by the nanosecond Nd: YAG Laser (<b>a</b>) LAT = 20 min, (<b>b</b>) = 30 min, and (<b>c</b>) LAT = 40 min.</p>
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<p>The laser ablation time (LAT) of the CuO NPs is a function of both the total surface area (left x-axis) and the number of particles per gram (right x-axis).</p>
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<p>Molar concentration of CuO NPs determined via ICP–OES at different laser ablation times (LATs).</p>
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<p>The linear absorption spectra of the three CuO NPs samples at LAT = 20, 30 and 40 min.</p>
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<p>Energy band gap of the CuO NPs samples at different LATs.</p>
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<p>The experimental setup of the Z-scans: A, attenuator; L, convex lens; S, CuO NPs sample; BS, beam splitter; I, iris; PM, power meter.</p>
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<p>Open-aperture (OA) Z-scan measurements for different CuO NPs samples at a constant excitation wavelength of 800 nm: (<b>a</b>) LAT = 20 min, (<b>b</b>) LAT = 30 min and (<b>c</b>) LAT = 40 min.</p>
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<p>Effect of average power <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mi>a</mi> <mi>v</mi> <mi>g</mi> </mrow> </msub> </mrow> </semantics></math> on the NLA coefficient at a constant excitation wavelength of 800 nm: (<b>a</b>) NLA coefficient as a function of average CuO NPs average size and (<b>b</b>) NLA coefficient as a function of the CuO NPs concentration.</p>
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<p>Open-aperture (OA) Z-scan measurements for different CuO NPs samples at a constant average power of 1 W: (<b>a</b>) <span class="html-italic">λ</span> = 750 nm, (<b>b</b>) <span class="html-italic">λ</span> = 800 nm and (<b>c</b>) <span class="html-italic">λ</span> = 850 nm.</p>
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<p>The effect of the excitation wavelength on the NLA coefficient at a constant average power of 1 W: (<b>a</b>) NLA coefficient as a function of the average size of CuO NPs and (<b>b</b>) NLA coefficient as a function of the CuO NPs concentration.</p>
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<p>Closed-aperture (CA) Z-scan measurements for different ablation times of the CuO NPs samples at a constant excitation wavelength of 800 nm: (<b>a</b>) LAT = 20 min, (<b>b</b>) LAT = 30 min and (<b>c</b>) LAT = 40 min.</p>
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<p>Closed-aperture (CA) Z-scan measurements for different ablation times of the CuO NPs samples at a constant excitation wavelength of 800 nm: (<b>a</b>) LAT = 20 min, (<b>b</b>) LAT = 30 min and (<b>c</b>) LAT = 40 min.</p>
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<p>Variations in the nonlinear refractive indices of the CuO NPs samples at a constant excitation wavelength of 800 at LAT = 20 min, LAT = 30 min and LAT = 40 min.</p>
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<p>The dioptric power of the Kerr lens as a function of different average powers for LAT = 20 min, LAT = 30 min, and LAT = 40 min.</p>
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<p>Optical limiter behavior of the CuO NPs sample (<b>a</b>) LAT = 20 min, (<b>b</b>) LAT = 30 min, and (<b>c</b>) LAT = 40 min.</p>
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<p>Optical limiter behavior of the CuO NPs sample (<b>a</b>) LAT = 20 min, (<b>b</b>) LAT = 30 min, and (<b>c</b>) LAT = 40 min.</p>
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