[go: up one dir, main page]
More Web Proxy on the site http://driver.im/
You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (1,408)

Search Parameters:
Keywords = millimeter wave

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
26 pages, 9659 KiB  
Article
Designing Chip-Feed High-Gain Millimeter-Wave Resonant Cavity Antenna (RCA) Array and Optimization of Beam Steering Metasurface
by Abu Sadat Md. Sayem, Karu P. Esselle, Dushmantha N. Thalakotuna, Manik Attygalle and Khushboo Singh
Micromachines 2025, 16(2), 164; https://doi.org/10.3390/mi16020164 - 30 Jan 2025
Viewed by 215
Abstract
In this article, a chip-fed millimeter-wave high-gain antenna system with in-antenna power combining capability is presented. A low-profile resonant cavity antenna (RCA) array is fed by multiple spherical dielectric resonators (DRs), demonstrating its multi-feed capabilities. Each of the DRs is fed by two [...] Read more.
In this article, a chip-fed millimeter-wave high-gain antenna system with in-antenna power combining capability is presented. A low-profile resonant cavity antenna (RCA) array is fed by multiple spherical dielectric resonators (DRs), demonstrating its multi-feed capabilities. Each of the DRs is fed by two microstrip resonators on a planar circuit board. A printed superstrate is used in the proposed RCA as the partially reflecting superstrate (PRS), which makes the antenna profile small. To increase the directivity and gain, a 2 × 2 RCA array is developed. The demonstrated design shows a prominent peak gain of 25.03 dBi, a radiation efficiency of more than 80% and 3.38 GHz 3 db gain-bandwidth while maintaining a low profile. To steer the beam of the demonstrated 2 × 2 RCA array in a wide angular range with a low side-lobe-level, two planar all-dielectric passive beam steering metasurfaces have been designed and optimized. A detailed analysis of the optimization procedure is presented in this article. This numerical investigation is vitally important for realizing beam steering metasurfaces with suppressed side-lobe-level, wide bandwidth, excellent efficiency and less complexity. Full article
(This article belongs to the Special Issue Microwave Passive Components, 2nd Edition)
30 pages, 2229 KiB  
Review
Optoelectronic Oscillators: Progress from Classical Designs to Integrated Systems
by Qidi Liu, Jiuchang Peng and Juanjuan Yan
Photonics 2025, 12(2), 120; https://doi.org/10.3390/photonics12020120 - 29 Jan 2025
Viewed by 272
Abstract
Optoelectronic oscillators (OEOs) have emerged as indispensable tools for generating low-phase-noise microwave and millimeter-wave signals, which are critical for a variety of high-performance applications. These include radar systems, satellite links, electronic warfare, and advanced instrumentation. The ability of OEOs to produce signals with [...] Read more.
Optoelectronic oscillators (OEOs) have emerged as indispensable tools for generating low-phase-noise microwave and millimeter-wave signals, which are critical for a variety of high-performance applications. These include radar systems, satellite links, electronic warfare, and advanced instrumentation. The ability of OEOs to produce signals with exceptionally low phase noise makes them ideal for scenarios demanding high signal purity and stability. In radar systems, low-phase-noise signals enhance target detection accuracy and resolution, while, in communication networks, such signals enable higher data throughput and improved signal integrity over extended distances. Furthermore, OEOs play a pivotal role in precision instrumentation, where even minor noise can compromise the performance of sensitive equipment. This review examines the progress in OEO technology, transitioning from classical designs relying on long optical fiber delay lines to modern integrated systems that leverage photonic integration for compact, efficient, and tunable solutions. Key advancements, including classical setups, hybrid designs, and integrated configurations, are discussed, with a focus on their performance improvements in phase noise, side-mode suppression ratio (SMSR), and frequency tunability. A 20-GHz oscillation with an SMSR as high as 70 dB has been achieved using a classical dual-loop configuration. A 9.867-GHz frequency with a phase noise of −142.5 dBc/Hz @ 10 kHz offset has also been generated in a parity–time-symmetric OEO. Additionally, integrated OEOs based on silicon photonic microring resonators have achieved an ultra-wideband tunable frequency from 3 GHz to 42.5 GHz, with phase noise as low as −93 dBc/Hz at a 10 kHz offset. The challenges in achieving fully integrated OEOs, particularly concerning the stability and phase noise at higher frequencies, are also explored. This paper provides a comprehensive overview of the state of the art in OEO technology, highlighting future directions and potential applications. Full article
15 pages, 12073 KiB  
Article
Classification of Hydrometeors During a Stratiform Precipitation Event in the Rainy Season of Liupanshan
by Nansong Feng, Zhiliang Shu and Yujun Qiu
Atmosphere 2025, 16(2), 132; https://doi.org/10.3390/atmos16020132 - 26 Jan 2025
Viewed by 248
Abstract
This study conducted a classification analysis of hydrometeor types during a typical stratiform mixed cloud precipitation event in the rainy season using data from the Liupan Mountains micro rain radar power spectra. The primary research findings are as follows: (1) Utilizing the RaProM [...] Read more.
This study conducted a classification analysis of hydrometeor types during a typical stratiform mixed cloud precipitation event in the rainy season using data from the Liupan Mountains micro rain radar power spectra. The primary research findings are as follows: (1) Utilizing the RaProM method synthesizes the information of particle falling velocity, equivalent radar reflection coefficient, particle scale characteristics at different stages, and the location of the bright zone in the zero-degree layer to classify hydrometeors during this precipitation process, and the results show that drizzle and raindrop distribution time periods do not match with the raindrop spectra and rain intensities observed by the DSG5 ground-based precipitation gauge. (2) Sensitivity experiments conducted on the RaProM method revealed that after modifying the discrimination thresholds for drizzle and raindrops, the distributions of drizzle and raindrops were more aligned with ground-based raindrop spectrum observations. Furthermore, these adjustments also showed better consistency with the radar reflectivity factor, Doppler velocity, and velocity spectrum width thresholds used by existing millimeter-wave cloud radars to discriminate between drizzle and raindrops. (3) Various kinds of hydrometeors show different vertical distribution characteristics in three precipitation stages: weak, strong, and weak. In the two weak precipitation stages, hydrometeors mainly existed in the form of snowflakes at altitudes above the zero-degree layer and in the form of drizzle at altitudes below the zero-degree layer. The vertical distribution disparity of hydrometeors between the mountain peak and base sites demonstrates that terrain significantly influences hydrometeors during the precipitation process. Full article
(This article belongs to the Section Meteorology)
Show Figures

Figure 1

Figure 1
<p>Topographic map of Liupan Mountains (blue triangles indicate Liupan Mountain summit site, red asterisks indicate Longde site locations).</p>
Full article ">Figure 2
<p>Weather charts of Northwest China at 13:00 on 12 August 2021 show (<b>a</b>) 500 hPa and (<b>b</b>) 700 hPa geopotential height (blue lines, units: dagpm), horizontal winds (vector arrows), and (<b>c</b>,<b>d</b>) respectively depict the relative vorticity (10<sup>−4</sup>·s<sup>−1</sup>) and water vapor flux divergence (g·cm<sup>−2</sup>·hPa<sup>−1</sup>·s<sup>−1</sup>) at 700 hPa. The red area indicates the location of the Liupanshan region.</p>
Full article ">Figure 3
<p>Vertical distributions of radar reflectivity factors measured by cloud radar and micro rain radar on 12 August 2021 at two sites, LD and LP, in the Liupanshan area. (<b>a1</b>,<b>b1</b>) and (<b>a2</b>,<b>b2</b>) represent the results of LD and LP, respectively.</p>
Full article ">Figure 4
<p>Vertical distributions of micro rain radar reflectivity factors and particle falling velocities measured at two sites, LD and LP, in the Liupanshan area on 12 August 2021; (<b>a1</b>,<b>b1</b>) and (<b>a2</b>,<b>b2</b>) represent the results for LD and LP, respectively.</p>
Full article ">Figure 5
<p>Vertical distribution of particle phase states for the micro rain radar inversion at the LP site on 12 August 2021 (<b>a</b>) and PDF distributions of (<b>b</b>) cloud radar reflectivity, (<b>c</b>) velocity, and (<b>d</b>) spectral width corresponding to the particle phase states.</p>
Full article ">Figure 6
<p>PDF distributions of cloud radar reflectivity (dBZ), velocity (V), and spectral width (W) corresponding to the gross and raindrop phases at the LP site for three sets of sensitivity experimental conditions. Condition ①: (<b>a1</b>,<b>b1</b>,<b>c1</b>), Condition ②: (<b>a2</b>,<b>b2</b>,<b>c2</b>), Condition ③: (<b>a3</b>,<b>b3</b>,<b>c3</b>).</p>
Full article ">Figure 7
<p>Vertical distributions of particle phase states (<b>a1</b>,<b>a2</b>) for the inversions at LD and LP sites after the improvement of the drizzle and raindrop thresholds and the surface rainfall rates (<b>b1</b>,<b>b2</b>) measured by DSG5. (<b>a1</b>,<b>b1</b>) and (<b>a2</b>,<b>b2</b>) represent the results of LD and LP, respectively.</p>
Full article ">Figure 8
<p>Percentage of different hydrometeor phases in each altitude layer during the first stage of the precipitation process at two sites, LD and LP. (<b>a</b>) and (<b>b</b>) represent the results for LD and LP, respectively.</p>
Full article ">Figure 9
<p>Percentage of different hydrometeor phases in each altitude layer during the second stage of the precipitation process at two sites, LD and LP. (<b>a</b>) and (<b>b</b>) represent the results for LD and LP, respectively.</p>
Full article ">Figure 10
<p>Percentage of different hydrometeor phases in each altitude layer during the third stage of the precipitation process at two sites, LD and LP. (<b>a</b>) and (<b>b</b>) represent the results for LD and LP, respectively.</p>
Full article ">Figure A1
<p>Recognition algorithm flowchart of precipitation type classification [<a href="#B25-atmosphere-16-00132" class="html-bibr">25</a>].</p>
Full article ">
20 pages, 2393 KiB  
Article
Advancing Microscale Electromagnetic Simulations for Liquid Crystal Terahertz Phase Shifters: A Diagnostic Framework for Higher-Order Mode Analysis in Closed-Source Simulators
by Haorong Li and Jinfeng Li
Micro 2025, 5(1), 3; https://doi.org/10.3390/micro5010003 - 25 Jan 2025
Viewed by 340
Abstract
This work addresses a critical challenge in microscale computational electromagnetics for liquid crystal-based reconfigurable components: the inadequate capability of current software to accurately identify and simulate higher-order modes (HoMs) in complex electromagnetic structures. Specifically, commercial simulators often fail to capture modes such as [...] Read more.
This work addresses a critical challenge in microscale computational electromagnetics for liquid crystal-based reconfigurable components: the inadequate capability of current software to accurately identify and simulate higher-order modes (HoMs) in complex electromagnetic structures. Specifically, commercial simulators often fail to capture modes such as Transverse Electric (TE11) beyond the fundamental transverse electromagnetic (TEM) mode in coaxial liquid crystal phase shifters operating in the terahertz (THz) regime, leading to inaccurate performance predictions and suboptimal designs for telecommunication engineering applications. To address this limitation, we propose a novel diagnostic methodology incorporating three lossless assumptions to enhance the identification and analysis of pseudo-HoMs in full-wave simulators. Our approach theoretically eliminates losses associated with metallic conductivity, dielectric dissipation, and reflection effects, enabling precise assessment of frequency-dependent HoM power propagation alongside the primary TEM mode. We validate the methodology by applying it to a coaxially filled liquid crystal variable phase shifter device structure, underscoring its effectiveness in advancing the design and characterization of THz devices. This work provides valuable insights for researchers and engineers utilizing closed-source commercial simulators in micro- and nano-electromagnetic device development. The findings are particularly relevant for microscale engineering applications, including millimeter-wave (mmW), sub-mmW, and THz systems, with potential impacts on next-generation communication technologies. Full article
(This article belongs to the Section Microscale Engineering)
30 pages, 30400 KiB  
Article
Classification of Flying Drones Using Millimeter-Wave Radar: Comparative Analysis of Algorithms Under Noisy Conditions
by Mauro Larrat and Claudomiro Sales
Sensors 2025, 25(3), 721; https://doi.org/10.3390/s25030721 - 24 Jan 2025
Viewed by 460
Abstract
This study evaluates different machine learning algorithms in detecting and identifying drones using radar data from a 60 GHz millimeter-wave sensor. These signals were collected from a bionic bird and two drones, namely DJI Mavic and DJI Phantom 3 Pro, which were represented [...] Read more.
This study evaluates different machine learning algorithms in detecting and identifying drones using radar data from a 60 GHz millimeter-wave sensor. These signals were collected from a bionic bird and two drones, namely DJI Mavic and DJI Phantom 3 Pro, which were represented in complex form to preserve amplitude and phase information. The first benchmarks used four algorithms, namely long short-term memory (LSTM), gated recurrent unit (GRU), one-dimensional convolutional neural network (Conv1D), and Transformer, and they were benchmarked for robustness under noisy conditions, including artificial noise types like white noise, Pareto noise, impulsive noise, and multipath interference. As expected, Transformer outperformed other algorithms in terms of accuracy, even on noisy data; however, in certain noise contexts, particularly Pareto noise, it showed weaknesses. For this purpose, we propose Multimodal Transformer, which incorporates more statistical features—skewness and kurtosis—in addition to amplitude and phase data. This resulted in a improvement in detection accuracy, even under difficult noise conditions. Our results demonstrate the importance of noise in processing radar signals and the benefits afforded by a multimodal presentation of data in detecting unmanned aerial vehicle and birds. This study sets up a benchmark for state-of-the-art machine learning methodologies for radar-based detection systems, providing valuable insight into methods of increasing the robustness of algorithms to environmental noise. Full article
(This article belongs to the Special Issue Radar Target Detection, Imaging and Recognition)
Show Figures

Figure 1

Figure 1
<p>Images of the test subjects used in the experiments: (<b>a</b>) the DJI Mavic drone [<a href="#B47-sensors-25-00721" class="html-bibr">47</a>], (<b>b</b>) the DJI Phantom 3 Pro drone [<a href="#B48-sensors-25-00721" class="html-bibr">48</a>], and (<b>c</b>) the Bionic Bird [<a href="#B49-sensors-25-00721" class="html-bibr">49</a>]. These devices illustrate what were used to evaluate the classification performance of the Multimodal Transformer model.</p>
Full article ">Figure 2
<p>This boxplot shows the impact of white noise on the amplitude (<b>left</b>) and phase (<b>right</b>) of the radar signal. White noise follows a random distribution, primarily affecting the outliers in both amplitude and phase. The amplitude exhibits a broader spread, with more pronounced outliers in both directions. The phase is also impacted, though to a lesser extent, showing a slight median shift and a moderate interquartile range expansion.</p>
Full article ">Figure 3
<p>This boxplot illustrates the impact of Pareto noise on the amplitude (<b>left</b>) and phase (<b>right</b>) of the radar signal. Pareto noise, also known as heavy-tail noise, introduces extreme values more frequently than white noise, resulting in greater data dispersion. The amplitude plot shows a considerable number of high-value outliers, suggesting that the noise causes more frequent positive fluctuations. The phase remains relatively stable, with occasional extreme values.</p>
Full article ">Figure 4
<p>This boxplot illustrates the effect of impulsive noise on the amplitude (<b>left</b>) and phase (<b>right</b>) of the millimeter-wave radar signal. Impulsive noise generates abrupt, random spikes, causing significant data dispersion. The amplitude plot shows a noticeable increase in outliers at both extremes, with a wider interquartile range. While the median amplitude remains relatively stable, the data’s extremes were widely scattered. The phase plot shows a similar pattern, with more visible outliers and a slight median shift.</p>
Full article ">Figure 5
<p>This boxplot shows the effects of multipath interference noise on the amplitude (<b>left</b>) and phase (<b>right</b>) of the radar signal. Multipath interference occurs when the signal reflects off multiple surfaces before reaching the receiver, causing distortions. The amplitude plot reveals increased variability and a larger number of outliers, indicating inconsistencies in the measured values. The phase is less affected but still shows a slight increase in dispersion compared to the original signal.</p>
Full article ">Figure 6
<p>This boxplot illustrates the classification probability outputs of four algorithms—LSTM, GRU, Conv1D, and Transformer—under white noise conditions. The boxplot reveals that LSTM, GRU, and Conv1D exhibited tightly clustered probability distributions with low variance, and their median probabilities remained around or below 0.4 across all classes (Bird, Mavic drone, and P3P drone). This low variability and clustered median values suggests poor classification performance, with predictions lacking high confidence and distinguishing power. In contrast, the Transformer algorithm demonstrated a markedly different behavior, with wider interquartile ranges and higher median probabilities for all classes. The wider spread indicates that Transformer is more resilient to white noise, producing more varied and accurate probability outputs, thus highlighting its superior robustness in handling noisy data compared to the other models.</p>
Full article ">Figure 7
<p>This boxplot presents the classification probabilities of four machine learning models—LSTM, GRU, Conv1D, and Transformer—under white noise conditions for the three target classes: Bird, Mavic drone, and P3P drone. The LSTM, GRU, and Conv1D models display tightly grouped probability distributions with narrow interquartile ranges and median values clustered near or below 0.4 across all classes. This indicates that these models struggle to produce confident predictions in noisy environments as their output probabilities remain low and exhibit limited variability, suggesting a uniform inability to distinguish between the classes under these conditions. In contrast, the Transformer model showed a significantly wider interquartile range and higher median probability values for all classes. This broader distribution highlights Transformer’s superior robustness to white noise, enabling it to generate more confident and diverse predictions across the dataset, outperforming the other models in terms of classification reliability under challenging noise conditions.</p>
Full article ">Figure 8
<p>This boxplot illustrates the classification probabilities for different models—LSTM, GRU, Conv1D, and Transformer—under Pareto noise conditions across three target classes: Bird, Mavic drone, and P3P drone. The LSTM and GRU models exhibited higher median probabilities for the “bird” class, suggesting better performance in this specific category compared to other classes. However, the overall performance across all models was negatively impacted by Pareto noise, which introduces frequent extreme values (outliers) and disrupts the models’ ability to confidently assign accurate probabilities, particularly those affecting classification consistency.</p>
Full article ">Figure 9
<p>This figure presents the ROC curves and AUC scores for the classification performance of LSTM, GRU, Conv1D, and Transformer models under Pareto noise conditions. The Transformer model demonstrated superior performance, with higher AUC scores across all target classes, indicating better discriminative ability compared to the other models. Additionally, Transformer exhibited fewer outliers in classification scores, highlighting its robustness to Pareto noise. In contrast, the LSTM, GRU, and Conv1D models showed higher false positive rates, suggesting difficulty in generalizing to data with high variability caused by noise. These results emphasize the need for further model optimization to handle noise-induced challenges effectively.</p>
Full article ">Figure 10
<p>This boxplot displays the distribution of classification probabilities for the LSTM, GRU, Conv1D, and Transformer models under impulsive noise conditions across the Bird, Mavic drone, and P3P drone classes. The Transformer model consistently showed a higher median probability across all classes, indicating more confident predictions. However, its wider interquartile range suggests that it also exhibits greater uncertainty in some predictions. In contrast, the other models—LSTM, GRU, and Conv1D—showed lower median probabilities and tighter ranges, indicating less confidence and lower variability in their predictions under impulsive noise conditions.</p>
Full article ">Figure 11
<p>The ROC curves and AUC values demonstrate the classification performance of LSTM, GRU, Conv1D, and Transformer models under impulsive noise conditions. The Transformer model outperforms the other models, particularly for the Bird and Mavic drone classes, with higher AUC values, indicating better discrimination capabilities. The LSTM and GRU models show moderate performance but are slightly less effective than Transformer. The Conv1D model performs poorly across most classes, especially for the Bird class, reflecting its inability to effectively handle temporal dependencies in the presence of impulsive noise.</p>
Full article ">Figure 12
<p>Boxplot illustrating the classification accuracy variability of the four machine learning algorithms under multipath interference. The Transformer model consistently demonstrated higher accuracy and lower variability, indicating superior stability and performance compared to the LSTM, GRU, and Conv1D models.</p>
Full article ">Figure 13
<p>ROC curves showing the performance of the Transformer, LSTM, GRU, and Conv1D models in object classification with multipath interference. The Transformer model consistently outperformed the others, with higher AUC values, highlighting its robustness and superior attention mechanism for handling noise and temporal dependencies.</p>
Full article ">Figure 14
<p>Schematic of the Multimodal Transformer Model (MMT) used for radar-based target classification. The model begins with an input layer processing radar features, followed by LayerNormalization for stable learning. Multi-head attention (8 heads) captures complex temporal dependencies in radar signals. Dropout layers (0.1 and 0.2) prevent overfitting. A GlobalAveragePooling1D layer reduces dimensionality, followed by two dense layers with L2 regularization and LeakyReLU activation. The final dense layer outputs classification probabilities using softmax, where the model’s output is 0 for the Mavic drone, 1 for the Phantom 3 Pro drone, or 2 for bionic bird. The model was optimized with Adam and sparse categorical cross-entropy loss for multi-class classification.</p>
Full article ">Figure 15
<p>Boxplots showing the amplitude, phase, skewness, and kurtosis values for the Bird, Mavic, and P3P classes, as extracted from radar signals with added white noise. The Bird class showed lower and more stable values across all features. The Mavic class had moderate values with noticeable outliers. The P3P class consistently showed the highest medians and broader ranges, indicating stronger and more variable radar reflections. The differences in these features help to distinguish the classes in the Transformer model’s classification process.</p>
Full article ">Figure 16
<p>ROC. curves for the classification of the Bird, Mavic, and P3P classes. The model achieved a perfect AUC for all the classes in both noise cases. For white noise, the curves were slightly farther from the vertical axis compared to the Pareto noise, indicating a slightly better robustness to the latter noise type.</p>
Full article ">Figure 17
<p>Boxplots showing the amplitude, phase, skewness, and kurtosis values for the Bird, Mavic, and P3P classes, as extracted from radar signals with added Pareto noise. The median values remained close to zero across the features, with fewer outliers and lower variability compared to white noise. The Bird class showed the most stable distribution, while the Mavic and P3P classes exhibited moderate spreads with fewer extreme values. This reduced variability under Pareto noise led to diminished class separability, resulting in lower classification performance compared to white noise.</p>
Full article ">Figure 18
<p>The ROC curves for the classification of Bird, Mavic drone, and P3P drone when considering Pareto noise with a Multimodal Transformer.</p>
Full article ">Figure 19
<p>Boxplots showing the amplitude, phase, skewness, and kurtosis values for the Bird, Mavic, and P3P classes under impulsive noise. The Bird class exhibited the most stable and compact distribution across all features, while the P3P class showed the highest median values and widest variability, especially in amplitude and kurtosis. The Mavic class displayed intermediate behavior. Impulsive noise significantly increased outliers, particularly in the P3P class, indicating that larger or more complex targets produce more erratic radar reflections.</p>
Full article ">Figure 20
<p>ROC curves for the classification of the Bird, Mavic drone, and P3P drone classes when considering impulsive noise with the Multimodal Transformer.</p>
Full article ">Figure 21
<p>Boxplots showing the amplitude, phase, skewness, and kurtosis values for the Bird, Mavic, and P3P classes under multipath interference. Unlike impulsive noise, the distributions were more uniform across classes, with median values close to zero and consistent interquartile ranges. The P3P class showed a slightly wider spread in amplitude and skewness, suggesting higher susceptibility to multipath effects. Outliers were evenly distributed across classes, indicating random variations in signal reflections that reduce separability between classes.</p>
Full article ">Figure 22
<p>ROC curves for the classification of Bird, Mavic drone, and P3P drone classes when considering multipath interference with the Multimodal Transformer.</p>
Full article ">
26 pages, 979 KiB  
Article
Energy-Efficient Joint User Association, Backhaul Bandwidth Allocation, and Power Allocation in Cell-Free mmWave UAV Networks
by Zhiwei Si, Zheng Jiang, Kaisa Zhang, Qian Liu, Jianchi Zhu, Xiaoming She and Peng Chen
Drones 2025, 9(2), 88; https://doi.org/10.3390/drones9020088 - 23 Jan 2025
Viewed by 322
Abstract
In this article, we propose a cell-free network architecture for an unmanned aerial vehicle (UAV) base station (BS), i.e., UBS, incorporating high-altitude platform stations (HAPSs) as central processing units (CPUs). The goal is to guarantee the quality of service (QoS) of user equipment [...] Read more.
In this article, we propose a cell-free network architecture for an unmanned aerial vehicle (UAV) base station (BS), i.e., UBS, incorporating high-altitude platform stations (HAPSs) as central processing units (CPUs). The goal is to guarantee the quality of service (QoS) of user equipment (UE), reduce energy consumption, extend communication time, and facilitate rescue operations. The millimeter-wave (mmWave) frequency band is deployed in access and backhaul links to satisfy UE QoS requirements and high backhaul demands. The proposed framework jointly optimizes user association, backhaul bandwidth allocation, and power allocation to maximize energy efficiency while meeting QoS requirements. The optimization problem, modeled as non-convex mixed-integer nonlinear fractional programming, is solved through a three-stage iterative algorithm. This includes (1) optimizing power allocation based on Dinkelbach transformation and a successive convex approximation (SCA) method, (2) clustering UBSs using the Lagrangian method, and (3) deriving a closed-form bandwidth allocation factor. The proposed algorithm significantly outperforms many traditional algorithms in performance while maintaining low computational complexity. Full article
Show Figures

Figure 1

Figure 1
<p>An IAB architecture for a cell-free mmWave UAV network for post-disaster rescue operations.</p>
Full article ">Figure 2
<p>Flowchart of the proposed algorithm.</p>
Full article ">Figure 3
<p>Convergence of Algorithm 4.</p>
Full article ">Figure 4
<p>The energy efficiency varies with the beamwidth of the mmWave UBS.</p>
Full article ">Figure 5
<p>The energy efficiency varies with the sizes of the cell-free cooperative UBS cluster.</p>
Full article ">Figure 6
<p>The energy efficiency varies with the density of the mmWave UBSs.</p>
Full article ">Figure 7
<p>The energy efficiency varies with the density of the UEs.</p>
Full article ">Figure 8
<p>The energy efficiency varies with the maximum transmission power of the mmWave UBS.</p>
Full article ">Figure 9
<p>The energy efficiency varies with the UE QoS rate requirements of the mmWave UBS.</p>
Full article ">
14 pages, 4022 KiB  
Article
A 13–33 GHz Wideband Low-Noise Amplifier in 150-nm GaAs Based on Simultaneous Noise- and Input-Matched Gain-Core with R-L-C Shunt Feedback Network
by Seonyeong Hwang, Dongwan Kang, Yeonggeon Lee and Dae-Woong Park
Electronics 2025, 14(3), 450; https://doi.org/10.3390/electronics14030450 - 23 Jan 2025
Viewed by 315
Abstract
This work reports the concept of a shunt negative feedback technique for implementing a millimeter-wave wideband low-noise amplifier. The proposed shunt negative feedback network consists of a resistor–capacitor–inductor configuration. The proposed feedback network can achieve simultaneous noise and input matching (SNIM) over a [...] Read more.
This work reports the concept of a shunt negative feedback technique for implementing a millimeter-wave wideband low-noise amplifier. The proposed shunt negative feedback network consists of a resistor–capacitor–inductor configuration. The proposed feedback network can achieve simultaneous noise and input matching (SNIM) over a wide frequency range by adjusting the values of the resistor–capacitor–inductor configuration based on numerical analysis. By adopting the SNIM-based gain core as the first stage of the amplifier, the simulation results of the three-stage low-noise amplifier in a 150-nm GaAs pHEMT process achieve a gain of 15.6–18.6 dB and a noise figure of 1.05–2.8 dB in the frequency range of 13–33 GHz, respectively, while dissipating 99 mW. Full article
(This article belongs to the Special Issue RF/MM-Wave Circuits Design and Applications, 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Schematics of conventional common-source topologies for achieving simultaneous noise and input matching: (<b>a</b>) a transistor with a source degeneration inductor (<math display="inline"><semantics> <msub> <mi>L</mi> <mi>s</mi> </msub> </semantics></math>) and a series inductor (<math display="inline"><semantics> <msub> <mi>L</mi> <mi>g</mi> </msub> </semantics></math>) at the gate node, and (<b>b</b>) a transistor with <math display="inline"><semantics> <msub> <mi>L</mi> <mi>s</mi> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>L</mi> <mi>g</mi> </msub> </semantics></math> at the gate node, along with a capacitor (<math display="inline"><semantics> <msub> <mi>C</mi> <mrow> <mi>e</mi> <mi>x</mi> </mrow> </msub> </semantics></math>) added between the gate and source nodes.</p>
Full article ">Figure 2
<p>Simulated <math display="inline"><semantics> <msub> <mi>G</mi> <mrow> <mi>m</mi> <mi>a</mi> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>N</mi> <msub> <mi>F</mi> <mrow> <mi>m</mi> <mi>i</mi> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math> for varying transistor widths with different numbers of fingers (NoF): (<b>a</b>) NoF = 1, (<b>b</b>) NoF = 2, (<b>c</b>) NoF = 4, and (<b>d</b>) NoF = 6.</p>
Full article ">Figure 3
<p>Variation of the gain matching points and noise matching points of transistor with a width of 40 μm and NoF of 6 as frequency changes on a Smith chart.</p>
Full article ">Figure 4
<p>Schematic of (<b>a</b>) the gain core with the proposed shunt R-L-C feedback network and (<b>b</b>) its equivalent small-signal model.</p>
Full article ">Figure 5
<p>Schematic of the gain core with the R-L-C Shunt feedback and its <span class="html-italic">Y</span>-parameter-based equivalent model.</p>
Full article ">Figure 6
<p>Calculated <math display="inline"><semantics> <msub> <mi>G</mi> <mrow> <mi>m</mi> <mi>a</mi> <mo>,</mo> <mi>e</mi> <mi>q</mi> </mrow> </msub> </semantics></math> for variations in <math display="inline"><semantics> <msub> <mi>R</mi> <mi>F</mi> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>L</mi> <mi>F</mi> </msub> </semantics></math> at (<b>a</b>) 15 GHz, (<b>b</b>) 24 GHz, and (<b>c</b>) 33 GHz.</p>
Full article ">Figure 7
<p>Variations in the noise matching points with 0.2 dB noise circles and the gain matching points of the gain core with an R-L-C feedback network according to various <math display="inline"><semantics> <msub> <mi>R</mi> <mi>F</mi> </msub> </semantics></math> values: (<b>a</b>) <math display="inline"><semantics> <msub> <mi>R</mi> <mi>F</mi> </msub> </semantics></math> = 100 Ω, (<b>b</b>) <math display="inline"><semantics> <msub> <mi>R</mi> <mi>F</mi> </msub> </semantics></math> = 250 Ω, (<b>c</b>) <math display="inline"><semantics> <msub> <mi>R</mi> <mi>F</mi> </msub> </semantics></math> = 400 Ω, and (<b>d</b>) <math display="inline"><semantics> <msub> <mi>R</mi> <mi>F</mi> </msub> </semantics></math> = 1000 Ω.</p>
Full article ">Figure 8
<p>Schematic of the proposed three-stage LNA.</p>
Full article ">Figure 9
<p>Layout of the proposed three-stage LNA.</p>
Full article ">Figure 10
<p>Simulated (<b>a</b>) <span class="html-italic">S</span>-parameters versus freuquency, (<b>b</b>) noise figure versus frequency, (<b>c</b>) <span class="html-italic">k</span> and <math display="inline"><semantics> <mfenced open="|" close="|"> <mo>Δ</mo> </mfenced> </semantics></math> versus frequency, and (<b>d</b>) <math display="inline"><semantics> <mrow> <mi>O</mi> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>d</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> and PAE versus frequency of the proposed LNA.</p>
Full article ">Figure 11
<p>Simulated S-parameter results from a Monte Carlo analysis with 2000 samples at the center frequency of 24 GHz to evaluate the impact of process, voltage, and temperature (PVT) variations.</p>
Full article ">Figure 12
<p>Simulated (<b>a</b>) Rollet’s stability factor and (<b>b</b>) noise figure from a Monte Carlo analysis with 2000 samples at the center frequency of 24 GHz to evaluate the impact of process, voltage, and temperature (PVT) variations.</p>
Full article ">
13 pages, 6831 KiB  
Article
Demonstration of a Hybrid B5G System Integrating VLC and RF-Based Technologies with Access Networks
by Tomás Powell Villena Andrade, Celso Henrique de Souza Lopes, Letícia Carneiro de Souza and Arismar Cerqueira Sodré Junior
Appl. Sci. 2025, 15(2), 955; https://doi.org/10.3390/app15020955 - 19 Jan 2025
Viewed by 489
Abstract
Visible-light communication (VLC) has emerged as a promising technology to provide the very high-throughput wireless communications demanded by beyond-fifth-generation (B5G) applications. However, few works are found in the literature regarding the integration of VLC systems with other wireless communications technologies and with access [...] Read more.
Visible-light communication (VLC) has emerged as a promising technology to provide the very high-throughput wireless communications demanded by beyond-fifth-generation (B5G) applications. However, few works are found in the literature regarding the integration of VLC systems with other wireless communications technologies and with access networks. In this context, and as a proof of concept, we implement and experimentally evaluate a hybrid network architecture based on VLC, radio-over-fiber (RoF), free space optics (FSO), fiber-wireless (FiWi), and millimeter-waves (mm-waves) for B5G applications. Such optical networks make use of fiber-optic links based on RoF technology as backhauls, whereas their fronthauls might be either by FSO or RoF. Finally, a triple-wireless-access network is ensured by VLC, FiWi, and mm-wave links. The latter use a real 5G new radio (5G NR) signal. The system performance is evaluated in terms of a root mean square error vector magnitude (EVMRMS) parameter in accordance with the 3rd-Generation Partnership Project (3GPP) requirements. The experimental results demonstrate a total maximal theoretical throughput of approximately 1.66 Gbps, aligning with the digital performance requirements set by 3GPP. Full article
(This article belongs to the Special Issue Visible Light Communications (VLC) Networks)
Show Figures

Figure 1

Figure 1
<p>Hybrid FiWi system towards B5G applications within the C-RAN architecture. AP—access point; BH—backhaul; CO—central office; DU—distribution unit; FH—fronthaul; MH—midhaul.</p>
Full article ">Figure 2
<p>Frequency response of the LED with white cold light emission (A) and of the complete VLC transmitter (B).</p>
Full article ">Figure 3
<p>VLC system photographs.</p>
Full article ">Figure 4
<p>Proposed system: (<b>a</b>) schematic diagram and (<b>b</b>) photograph.</p>
Full article ">Figure 5
<p>RoF/FSO system digital performance as a function of the received optical power at the photodetector PD1 using 5G NR with 64-QAM signals.</p>
Full article ">Figure 6
<p>5G NR with 64-QAM scheme at 26 GHz—signal performance. FR2-1 bandwidths of 50, 100, 200, and 400 MHz. (<b>a</b>) Received spectra at FSW. (<b>b</b>) EVM<sub>RMS</sub> measured at VSA3 as a function of bandwidth. Maximum theoretical throughput calculated in each bandwidth. (<b>c</b>) Constellation comparison in mode back-to-back (B2B) and at the complete link (SYS). The yellow constellation represents user data, while the orange constellation serves as a demodulation reference signal.</p>
Full article ">Figure 7
<p>EVM<sub>RMS</sub> as a function of the injected RF power. For the 5G NR signal (<b>a</b>), the LTE signal (<b>b</b>), and the VLC signal (<b>c</b>).</p>
Full article ">Figure 8
<p>LTE signal at 2.5 GHz.</p>
Full article ">Figure 9
<p>VLC signal at 25 MHz.</p>
Full article ">
19 pages, 4791 KiB  
Article
Millimeter-Wave Radar Point Cloud Gesture Recognition Based on Multiscale Feature Extraction
by Wei Li, Zhiqi Guo and Zhuangzhi Han
Electronics 2025, 14(2), 371; https://doi.org/10.3390/electronics14020371 - 18 Jan 2025
Viewed by 402
Abstract
A gesture recognition method is proposed in this paper, which leverages millimeter-wave radar point clouds, primarily for identifying six basic human gestures. First, the raw radar signals collected by the MIMO millimeter-wave radar are converted into 3D point cloud sequences using a microcontroller [...] Read more.
A gesture recognition method is proposed in this paper, which leverages millimeter-wave radar point clouds, primarily for identifying six basic human gestures. First, the raw radar signals collected by the MIMO millimeter-wave radar are converted into 3D point cloud sequences using a microcontroller integrated into the radar’s baseband processor. Next, based on the SequentialPointNet network, a multiscale feature extraction module is proposed in this paper, which enhances the network’s ability to extract local and global features through convolutional layers at different scales. This compensates for the lack of feature understanding capability caused by single-scale convolution kernels. Moreover, the CBAM in the network is replaced with GAM, which effectively enhances the extraction of global features by more precisely modeling global contextual information, thereby increasing the network’s focus on global features. A separable MLP structure is introduced into the network. The separable MLP operation is used to separately extract local point cloud features and neighborhood features, and then fuse these features, significantly improving the model’s performance. The effectiveness of the proposed method is confirmed through experiments, achieving a 99.5% accuracy in recognizing six fundamental human gestures, effectively distinguishing between gesture categories, and confirming the potential of millimeter-wave radar 3D point clouds in recognizing gestures. Full article
(This article belongs to the Special Issue Machine Learning for Radar and Communication Signal Processing)
Show Figures

Figure 1

Figure 1
<p>Gesture recognition system.</p>
Full article ">Figure 2
<p>Radar principle.</p>
Full article ">Figure 3
<p>Millimeter-wave radar angle measurement principle.</p>
Full article ">Figure 4
<p>Radar hardware component module.</p>
Full article ">Figure 5
<p>Radar chip antenna and virtual antenna array.</p>
Full article ">Figure 6
<p>Hardware signal processing workflow.</p>
Full article ">Figure 7
<p>Network architecture diagram.</p>
Full article ">Figure 8
<p>NetR_T_S1 module.</p>
Full article ">Figure 9
<p>net4DV_T2 module.</p>
Full article ">Figure 10
<p>GAM attention module.</p>
Full article ">Figure 11
<p>Multiscale feature extraction module.</p>
Full article ">Figure 12
<p>Separable MLP structure.</p>
Full article ">Figure 13
<p>Gesture diagram.</p>
Full article ">Figure 14
<p>Three-dimensional point cloud image of left swipe.</p>
Full article ">Figure 15
<p>Depth image of left swipe.</p>
Full article ">Figure 16
<p>Experimental accuracy and loss curve of the model in this paper.</p>
Full article ">Figure 17
<p>Confusion matrix.</p>
Full article ">
19 pages, 456 KiB  
Article
Mathematical Models for Coverage with Star Tree Backbone Topology for 5G Millimeter Waves Networks
by Sergio Cordero, Pablo Adasme, Ali Dehghan Firoozabadi, Renata Lopes Rosa and Demóstenes Zegarra Rodríguez
Symmetry 2025, 17(1), 141; https://doi.org/10.3390/sym17010141 - 18 Jan 2025
Viewed by 477
Abstract
This paper proposes mathematical optimization models for solving the network planning problem using millimeter wave technology for 5G wireless communications networks. To this end, it is assumed that a set of users, M={1,,m}, and [...] Read more.
This paper proposes mathematical optimization models for solving the network planning problem using millimeter wave technology for 5G wireless communications networks. To this end, it is assumed that a set of users, M={1,,m}, and a set of base stations, N={1,,n}, are deployed randomly in a square area. In particular, the base stations should be connected, forming a star backbone so that users can connect to their nearest active base stations forming the backbone where the connections are symmetric. In particular, the first two models maximize the number of users connected to the backbone and minimize the distance costs of connecting users to the base stations, and distances of connecting the base stations themselves. Similarly, the last two models maximize and minimize the same objectives and the number of base stations to be activated to form the star backbone. Each user is allowed to connect to a unique active base station. In general, the millimeter wave technology presents a high path loss. Consequently, the transmission distances should be no larger than 300 m at most for different radial transmissions. Thus, a direct line of sight between users and base stations is assumed. Finally, we propose local search-based algorithms that allow finding near-optimal solutions for all our tested instances. Our numerical results indicate that we can solve network instances optimally with up to k=100, n=200, and m=5000 users. Full article
(This article belongs to the Section Engineering and Materials)
Show Figures

Figure 1

Figure 1
<p>Star network topology configuration composed of ten nodes and 30 users. The black node is the sink server base station, while the blue ones are the leaf base stations of the star. The green nodes represent users. Blue edges connect the star solution and the green links connect users to the base stations within the radial transmission area. The radial distance is 300 ms and all users are covered.</p>
Full article ">Figure 2
<p>A larger star network topology configuration composed of 50 nodes (BSs) and 1000 users. The black node is the sink server base station, while the blue ones are the leaf ones of the star. The green nodes and edges represent users connected to leaf BSs. The radial distance is 300 ms and all users are covered by the star.</p>
Full article ">Figure 3
<p>Objective values, CPU time in seconds, attended users, and gaps obtained for each instance in <a href="#symmetry-17-00141-t001" class="html-table">Table 1</a> where the radial transmission distance is 150 ms.</p>
Full article ">Figure 4
<p>Objective values, CPU time in seconds, attended users, and gaps obtained for each instance in <a href="#symmetry-17-00141-t002" class="html-table">Table 2</a> where the radial transmission distance is 200 ms.</p>
Full article ">Figure 5
<p>Objective values, CPU time in seconds, attended users, and gaps obtained for each instance in <a href="#symmetry-17-00141-t003" class="html-table">Table 3</a> where the radial transmission distance is 300 ms.</p>
Full article ">Figure 6
<p>Objective values, CPU time in seconds, attended users, number of base stations, and gaps obtained for each instance in <a href="#symmetry-17-00141-t004" class="html-table">Table 4</a> where the radial transmission distance is 150 ms.</p>
Full article ">Figure 7
<p>Objective values, CPU time in seconds, attended users, number of base stations, and gaps obtained for each instance in <a href="#symmetry-17-00141-t005" class="html-table">Table 5</a> where the radial transmission distance is 200 ms.</p>
Full article ">Figure 8
<p>Objective values, CPU time in seconds, attended users, number of base stations, and gaps obtained for each instance in <a href="#symmetry-17-00141-t006" class="html-table">Table 6</a> where the radial transmission distance is 300 ms.</p>
Full article ">
16 pages, 2965 KiB  
Article
Symmetry Breaking as a Basis for Characterization of Dielectric Materials
by Dubravko Tomić and Zvonimir Šipuš
Sensors 2025, 25(2), 532; https://doi.org/10.3390/s25020532 - 17 Jan 2025
Viewed by 404
Abstract
This paper introduces a novel method for measuring the dielectric permittivity of materials within the microwave and millimeter wave frequency ranges. The proposed approach, classified as a guided wave transmission system, employs a periodic transmission line structure characterized by mirror/glide symmetry. The dielectric [...] Read more.
This paper introduces a novel method for measuring the dielectric permittivity of materials within the microwave and millimeter wave frequency ranges. The proposed approach, classified as a guided wave transmission system, employs a periodic transmission line structure characterized by mirror/glide symmetry. The dielectric permittivity is deduced by measuring the transmission properties of such structure when presence of the dielectric material breaks the inherent symmetry of the structure and consequently introduce a stopband in propagation characteristic. To explore the influence of symmetry breaking on propagation properties, an analytical dispersion equation, for both symmetries, is formulated using the Rigorous Coupled Wave Analysis (RCWA) combined with the matrix transverse resonance condition. Based on the analytical equation, an optimization procedure and linearized model for a sensing structure is obtained, specifically for X-band characterization of FR4 substrates. The theoretical results of the model are validated with full wave simulations and experimentally. Full article
(This article belongs to the Special Issue Feature Papers in Physical Sensors 2024)
Show Figures

Figure 1

Figure 1
<p>Segments of 1D binary dielectric gratings with (<b>a</b>) mirror and (<b>c</b>) glide symmetry truncated in the <span class="html-italic">y</span>-direction, but in the analysis they are considered infinite along this direction. The corresponding unit cells with physical dimension are shown in subfigures (<b>b</b>,<b>d</b>).</p>
Full article ">Figure 2
<p>Unit cells of broken (<b>a</b>) mirror and (<b>b</b>) glide symmetric structures, shown in blue, due to presence of a dielectric slab, shown with orange color.</p>
Full article ">Figure 3
<p>Equivalent transverse network representation of periodic structures with broken mirror/glide symmetry due to the presence of a dielectric slab, such as structures shown in <a href="#sensors-25-00532-f002" class="html-fig">Figure 2</a>.</p>
Full article ">Figure 4
<p>Parametric sweep of stopband width over the SUT permittivity <math display="inline"><semantics> <msub> <mi>ε</mi> <mi>s</mi> </msub> </semantics></math> of (<b>a</b>) mirror- and (<b>b</b>) glide-symmetric binary grating. The shaded area corresponds to the first stopband frequency range.</p>
Full article ">Figure 5
<p>Parametric sweep of maximum value of attenuation constant <math display="inline"><semantics> <mrow> <msub> <mi>α</mi> <mrow> <mi>x</mi> <mo>,</mo> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> <mo>/</mo> <msub> <mi>k</mi> <mn>0</mn> </msub> </mrow> </semantics></math> over the SUT permittivity <math display="inline"><semantics> <msub> <mi>ε</mi> <mi>s</mi> </msub> </semantics></math> of (<b>a</b>) mirror- and (<b>b</b>) glide-symmetric binary grating.</p>
Full article ">Figure 6
<p>The illustration of the sensing setup with a broken glide sensor.</p>
Full article ">Figure 7
<p>Stopband start frequency <math display="inline"><semantics> <msub> <mi>f</mi> <mrow> <mi>S</mi> <mi>B</mi> <mo>,</mo> <mi>start</mi> </mrow> </msub> </semantics></math> dependence on the SUT permittivity <math display="inline"><semantics> <msub> <mi>ε</mi> <mi>s</mi> </msub> </semantics></math> for the optimized sensor in range of typical FR4 permittivities.</p>
Full article ">Figure 8
<p>Dependence of coefficients (<b>a</b>) <span class="html-italic">a</span> and (<b>b</b>) <span class="html-italic">b</span> on thickness of SUT <math display="inline"><semantics> <msub> <mi>t</mi> <mi>s</mi> </msub> </semantics></math> in the linearized expression for starting stopband frequency <math display="inline"><semantics> <msub> <mi>f</mi> <mrow> <mi>S</mi> <mi>B</mi> <mo>,</mo> <mi>start</mi> </mrow> </msub> </semantics></math>. Markers denote analytically obtained results from the dispersion equation and solid line denotes the corresponding LMS approximations (17) and (18).</p>
Full article ">Figure 9
<p>Full wave simulation results of sensing setup shown in <a href="#sensors-25-00532-f006" class="html-fig">Figure 6</a> for SUT permittivities ranging from <math display="inline"><semantics> <mrow> <mn>3.8</mn> </mrow> </semantics></math> (blue) to <math display="inline"><semantics> <mrow> <mn>4.8</mn> </mrow> </semantics></math> (purple) with step of <math display="inline"><semantics> <mrow> <mn>0.1</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 10
<p>Full wave simulation results of sensing setup SUT permittivities ranging from <math display="inline"><semantics> <mrow> <mn>3.8</mn> </mrow> </semantics></math> (blue) to <math display="inline"><semantics> <mrow> <mn>4.8</mn> </mrow> </semantics></math> (purple) with step of <math display="inline"><semantics> <mrow> <mn>0.1</mn> </mrow> </semantics></math> for (<b>a</b>) shorter SUT and (<b>b</b>) narrower SUT.</p>
Full article ">Figure 11
<p>Transmission measurements of the (<b>a</b>) nominal and (<b>b</b>) narrow substrate. (<b>c</b>) The picture of the manufactured sensor.</p>
Full article ">
20 pages, 10797 KiB  
Article
A Novel Gridless Non-Uniform Linear Array Direction of Arrival Estimation Approach Based on the Improved Alternating Descent Conditional Gradient Algorithm for Automotive Radar System
by Mingxiao Shao, Yizhe Fan, Yan Zhang, Zhe Zhang, Jie Zhao and Bingchen Zhang
Remote Sens. 2025, 17(2), 303; https://doi.org/10.3390/rs17020303 - 16 Jan 2025
Viewed by 352
Abstract
In automotive millimeter-wave (MMW) radar systems, achieving high-precision direction of arrival (DOA) estimation with a limited number of array elements is a crucial research focus. Compressive sensing (CS) techniques have been demonstrated to offer superior performance in DOA estimation compared to spectral estimation [...] Read more.
In automotive millimeter-wave (MMW) radar systems, achieving high-precision direction of arrival (DOA) estimation with a limited number of array elements is a crucial research focus. Compressive sensing (CS) techniques have been demonstrated to offer superior performance in DOA estimation compared to spectral estimation methods. However, traditional CS methods suffer from an off-grid effect, which causes their reconstruction results to deviate from the actual positions of the signal sources, thereby reducing the accuracy. Currently, as a gridless method, atomic norm minimization (ANM) has shown effectiveness in DOA estimation for uniform linear arrays (ULAs). However, the performance of ANM is suboptimal in non-uniform linear arrays (NULAs), and their computational efficiency is not satisfactory. In this paper, we propose a novel algorithm for DOA estimation in NULA, drawing inspiration from the alternating descent conditional gradient algorithm framework. First, we construct an atomic set based on the observation scene and select the atoms with the highest correlation to the residuals as potential signal sources for global estimation. Then, we construct a mapping function for the signal sources in the continuous domain and perform conditional gradient descent in the neighborhood of each signal source, addressing the bias introduced by the off-grid effect. We compared the proposed algorithm with ANM, Iterative Shrinkage Thresholding (IST), and Multiple Signal Classification (MUSIC) algorithms. Simulation experiments validate that the proposed algorithm effectively addresses the off-grid effect and is applicable to DOA estimation in coprime and random arrays. Furthermore, real data experiments confirm the effectiveness of the proposed algorithm. Full article
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Schematic diagrams of the models for ULA, RLA and CLA used in the experiments. The circles in the figure represent the positions of the array elements. (<b>a</b>) The ULA. (<b>b</b>) The RLA. (<b>c</b>) The CLA.</p>
Full article ">Figure 2
<p>Comparison of the RMSE of CS-ADCG, ANM, IST, and MUSIC algorithms under different SNRs for the three types of arrays. (<b>a</b>) The ULA. (<b>b</b>) The RLA. (<b>c</b>) The CLA.</p>
Full article ">Figure 3
<p>Comparison of the success rate of CS-ADCG, ANM, IST, and MUSIC algorithms under different SNRs for the three types of arrays. (<b>a</b>) The ULA. (<b>b</b>) The RLA. (<b>c</b>) The CLA.</p>
Full article ">Figure 4
<p>Comparison of the RMSE of CS-ADCG, ANM, IST, and MUSIC algorithms under different angular intervals for the three types of arrays. (<b>a</b>) The ULA. (<b>b</b>) The RLA. (<b>c</b>) The CLA.</p>
Full article ">Figure 5
<p>Comparison of the success rate of CS-ADCG, ANM, IST, and MUSIC algorithms under different angular intervals for the three types of arrays. (<b>a</b>) The ULA. (<b>b</b>) The RLA. (<b>c</b>) The CLA.</p>
Full article ">Figure 6
<p>Comparison of the RMSE of CS-ADCG, ANM, IST, and MUSIC algorithms under different sparsities for the three types of arrays. (<b>a</b>) The ULA. (<b>b</b>) The RLA. (<b>c</b>) The CLA.</p>
Full article ">Figure 7
<p>Comparison of the success rate of CS-ADCG, ANM, IST, and MUSIC algorithms under different sparsities for the three types of arrays. (<b>a</b>) The ULA. (<b>b</b>) The RLA. (<b>c</b>) The CLA.</p>
Full article ">Figure 8
<p>The reconstruction result of two corner reflectors. (<b>a</b>–<b>c</b>) The angle interval between the corner reflectors is 3°. (<b>d</b>–<b>f</b>) The angle interval between the corner reflectors is 2°. (<b>g</b>–<b>i</b>) The angle interval between the corner reflectors is 1°.</p>
Full article ">
17 pages, 502 KiB  
Article
Gesture Recognition with Residual LSTM Attention Using Millimeter-Wave Radar
by Weiqing Bai, Siyu Chen, Jialiang Ma, Ying Wang and Chong Han
Sensors 2025, 25(2), 469; https://doi.org/10.3390/s25020469 - 15 Jan 2025
Viewed by 447
Abstract
Gesture recognition technology based on millimeter-wave radar can recognize and classify user gestures in non-contact scenarios. To address the complexity of data processing with multi-feature inputs in neural networks and the poor recognition performance with single-feature inputs, this paper proposes a gesture recognition [...] Read more.
Gesture recognition technology based on millimeter-wave radar can recognize and classify user gestures in non-contact scenarios. To address the complexity of data processing with multi-feature inputs in neural networks and the poor recognition performance with single-feature inputs, this paper proposes a gesture recognition algorithm based on ResNet Long Short-Term Memory with an Attention Mechanism (RLA). In the aspect of signal processing in RLA, a range–Doppler map is obtained through the extraction of the range and velocity features in the original mmWave radar signal. Regarding the network architecture in RLA, the relevant features of the residual network with channel and spatial attention modules are combined to prevent some useful information from being neglected. We introduce a residual attention mechanism to enhance the network’s focus on gesture features and avoid the impact of irrelevant features on recognition accuracy. Additionally, we use a long short-term memory network to process temporal features, ensuring high recognition accuracy even with single-feature inputs. A series of experimental results show that the algorithm proposed in this paper has higher recognition performance. Full article
Show Figures

Figure 1

Figure 1
<p>Overall structure of gesture recognition algorithm.</p>
Full article ">Figure 2
<p>2D-FFT Processing Flow.</p>
Full article ">Figure 3
<p>Structure of the channel attention.</p>
Full article ">Figure 4
<p>Structure of spatial attention.</p>
Full article ">Figure 5
<p>Schematic diagram of CBAM structure.</p>
Full article ">Figure 6
<p>Structure of residual attention module.</p>
Full article ">Figure 7
<p>Network architecture based on residual attention mechanism.</p>
Full article ">Figure 8
<p>Gesture data acquisition.</p>
Full article ">Figure 9
<p>Types of gestures.</p>
Full article ">Figure 10
<p>Confusion matrix for the seven gestures.</p>
Full article ">
27 pages, 1409 KiB  
Article
Adaptive Handover Management in High-Mobility Networks for Smart Cities
by Yahya S. Junejo, Faisal K. Shaikh, Bhawani S. Chowdhry and Waleed Ejaz
Computers 2025, 14(1), 23; https://doi.org/10.3390/computers14010023 - 14 Jan 2025
Viewed by 801
Abstract
The seamless handover of mobile devices is critical for maximizing the potential of smart city applications, which demand uninterrupted connectivity, ultra-low latency, and performance in diverse environments. Fifth-generation (5G) and beyond-5G networks offer advancements in massive connectivity and ultra-low latency by leveraging advanced [...] Read more.
The seamless handover of mobile devices is critical for maximizing the potential of smart city applications, which demand uninterrupted connectivity, ultra-low latency, and performance in diverse environments. Fifth-generation (5G) and beyond-5G networks offer advancements in massive connectivity and ultra-low latency by leveraging advanced technologies like millimeter wave, massive machine-type communication, non-orthogonal multiple access, and beam forming. However, challenges persist in ensuring smooth handovers in dense deployments, especially in higher frequency bands and with increased user mobility. This paper presents an adaptive handover management scheme that utilizes reinforcement learning to optimize handover decisions in dynamic environments. The system selects the best target cell from the available neighbor cell list by predicting key performance indicators, such as reference signal received power and the signal–interference–noise ratio, while considering the fixed time-to-trigger and hysteresis margin values. It dynamically adjusts handover thresholds by incorporating an offset based on real-time network conditions and user mobility patterns. This adaptive approach minimizes handover failures and the ping-pong effect. Compared to the baseline LIM2 model, the proposed system demonstrates a 15% improvement in handover success rate, a 3% improvement in user throughput, and an approximately 6 sec reduction in the latency at 200 km/h speed in high-mobility scenarios. Full article
Show Figures

Figure 1

Figure 1
<p>Learning model for handover in 5G NR.</p>
Full article ">Figure 2
<p>Handover signaling messages.</p>
Full article ">Figure 3
<p>Proposed network mechanism.</p>
Full article ">Figure 4
<p>Handover event A5.</p>
Full article ">Figure 5
<p>Handover success rate when total number of UE is 500 versus (<b>a</b>) speed and (<b>b</b>) SINR.</p>
Full article ">Figure 6
<p>UE handover delay versus (<b>a</b>) speed and (<b>b</b>) SINR.</p>
Full article ">Figure 7
<p>Throughput versus (<b>a</b>) speed, (<b>b</b>) SINR, and (<b>c</b>) when number of pieces of UE is fixed.</p>
Full article ">Figure 8
<p>Latency versus (<b>a</b>) speed and (<b>b</b>) SINR.</p>
Full article ">Figure 9
<p>Packet loss ratio versus (<b>a</b>) speed and (<b>b</b>) SINR.</p>
Full article ">
18 pages, 28462 KiB  
Article
Optimized Airborne Millimeter-Wave InSAR for Complex Mountain Terrain Mapping
by Futai Xie, Wei Wang, Xiaopeng Sun, Si Xie and Lideng Wei
Sensors 2025, 25(2), 424; https://doi.org/10.3390/s25020424 - 13 Jan 2025
Viewed by 455
Abstract
The efficient acquisition and processing of large-scale terrain data has always been a focal point in the field of photogrammetry. Particularly in complex mountainous regions characterized by clouds, terrain, and airspace environments, the window for data collection is extremely limited. This paper investigates [...] Read more.
The efficient acquisition and processing of large-scale terrain data has always been a focal point in the field of photogrammetry. Particularly in complex mountainous regions characterized by clouds, terrain, and airspace environments, the window for data collection is extremely limited. This paper investigates the use of airborne millimeter-wave InSAR systems for efficient terrain mapping under such challenging conditions. The system’s potential for technical application is significant due to its minimal influence from cloud cover and its ability to acquire data in all-weather and all-day conditions. Focusing on the key factors in airborne InSAR data acquisition, this study explores advanced route planning and ground control measurement techniques. Leveraging radar observation geometry and global SRTM DEM data, we simulate layover and shadow effects to formulate an optimal flight path design. Additionally, the study examines methods to reduce synchronous ground control points in mountainous areas, thereby enhancing the rapid acquisition of terrain data. The results demonstrate that this approach not only significantly reduces field work and aviation costs but also ensures the accuracy of the mountain surface data generated by airborne millimeter-wave InSAR, offering substantial practical application value by reducing field work and aviation costs while maintaining data accuracy. Full article
(This article belongs to the Section Remote Sensors)
Show Figures

Figure 1

Figure 1
<p>View extend diagram.</p>
Full article ">Figure 2
<p>Shadow and layover schematic diagram, where grey area represents an object on the ground.</p>
Full article ">Figure 3
<p>Convert DEM data to radar coordinate system.</p>
Full article ">Figure 4
<p>The main basic data for calculating R_Index.</p>
Full article ">Figure 5
<p>The evolution of different headings affected by terrain.</p>
Full article ">Figure 6
<p>Flight path design, where (<b>a</b>) is the original flight path and (<b>b</b>) is the improved flight path of saving U-turn time by adjusting flight sequence from 1 to 6.</p>
Full article ">Figure 7
<p>Work flow chart of flight path design.</p>
Full article ">Figure 8
<p>Radar antenna observation geometry diagram.</p>
Full article ">Figure 9
<p>(<b>a</b>) Corner reflector placement position measurement and (<b>b</b>) corner reflector layout.</p>
Full article ">Figure 10
<p>The imaging results of corner reflector diagram on radar image is shown in (<b>a</b>), and (<b>b</b>) is the corner reflector that was damaged and moved out of its original position.</p>
Full article ">Figure 11
<p>Supplementary control point measurements after the flight.</p>
Full article ">Figure 12
<p>Measurement error experiment of manually adding control points.</p>
Full article ">Figure 13
<p>Airborne InSAR data processing flow chart.</p>
Full article ">Figure 14
<p>Working area.</p>
Full article ">Figure 15
<p>The relationship between the area proportion affected by terrain and flight heading angle.</p>
Full article ">Figure 16
<p>(<b>a</b>) Designed flight paths with the fix interval and (<b>b</b>) simulation results of equally spaced flight paths; there are gaps between each strip in the mountain area.</p>
Full article ">Figure 17
<p>(<b>a</b>) Designed flight paths, which are denser in the mountain area, and (<b>b</b>) simulation calculation results of strip coverage with denser flight paths in the mountain area and overlay shadow distribution.</p>
Full article ">Figure 18
<p>(<b>a</b>) Control point distribution. (<b>b</b>) Elevation inversion results.</p>
Full article ">Figure 19
<p>(<b>a</b>) Field control point measurement sample areas. (<b>b</b>) Distribution of ground check points.</p>
Full article ">
Back to TopTop