[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
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
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (2,030)

Search Parameters:
Keywords = mmWaves

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
14 pages, 6733 KiB  
Article
Detailed Determination of Delamination Parameters in a Multilayer Structure Using Asymmetric Lamb Wave Mode
by Olgirdas Tumšys, Lina Draudvilienė and Egidijus Žukauskas
Sensors 2025, 25(2), 539; https://doi.org/10.3390/s25020539 (registering DOI) - 18 Jan 2025
Viewed by 156
Abstract
A signal-processing algorithm for the detailed determination of delamination in multilayer structures is proposed in this work. The algorithm is based on calculating the phase velocity of the Lamb wave A0 mode and estimating this velocity dispersion. Both simulation and experimental studies [...] Read more.
A signal-processing algorithm for the detailed determination of delamination in multilayer structures is proposed in this work. The algorithm is based on calculating the phase velocity of the Lamb wave A0 mode and estimating this velocity dispersion. Both simulation and experimental studies were conducted to validate the proposed technique. The delamination having a diameter of 81 mm on the segment of a wind turbine blade (WTB) was used for verification of the proposed technique. Four cases were used in the simulation study: defect-free, delamination between the first and second layers, delamination between the second and third layers, and defect (hole). The calculated phase velocity variation in the A0 mode was used to determine the location and edge coordinates of the delaminations and defects. It has been found that in order to estimate the depth at which the delamination is, it is appropriate to calculate the phase velocity dispersion curves. The difference in the reconstructed phase velocity dispersion curves between the layers simulated at different depths is estimated to be about 60 m/s. The phase velocity values were compared with the delamination of the second and third layers and a hole drilled at the corresponding depth. The obtained simulation results confirmed that the drilled hole can be used as a defect corresponding to delamination. The WTB sample with a drilled hole of 81 mm was used in the experimental study. Using the proposed algorithm, detailed defect parameters were obtained. The results obtained using simulated and experimental signals indicated that the proposed new algorithm is suitable for the determination of delamination parameters in a multilayer structure. Full article
(This article belongs to the Special Issue Acoustic and Ultrasonic Sensing Technology in Non-Destructive Testing)
Show Figures

Figure 1

Figure 1
<p>Three-layer GFRP with delaminations between the different layers (<b>a</b>) and phase velocity dispersion curves in defect-free and defective regions calculated by the SAFE method (<b>b</b>); black lines are dispersion curves in the defect-free region, and red and blue lines are in the first and second regions of delaminations.</p>
Full article ">Figure 2
<p>The flow chart of the proposed signal-processing algorithm for delamination parametrization.</p>
Full article ">Figure 3
<p>The graphical representation of the multilayer structure of a WTB.</p>
Full article ">Figure 4
<p>The phase velocity dispersion curves of the A<sub>0</sub> and S<sub>0</sub> modes calculated by the SAFE method in the WTB multilayer structure.</p>
Full article ">Figure 5
<p>Simulated B-scan images of propagated Lamb wave in defect-free region (<b>a</b>), in region with delamination between 1st and 2nd layers (<b>b</b>), and in region with delamination between 2nd and 3rd layers (<b>c</b>); filtered B-scan images (<b>d</b>–<b>f</b>).</p>
Full article ">Figure 6
<p>Variation in the phase velocity of the A<sub>0</sub> mode of the Lamb wave with respect to the distance when there is no defect in the multilayer structure (<b>a</b>), when delamination is between the 1st and 2nd layers (<b>b</b>), and when delamination is between the 2nd and 3rd layers (<b>c</b>).</p>
Full article ">Figure 7
<p>Variation in the phase velocity of the Lamb wave A<sub>0</sub> mode with respect to the frequency when there is no defect in the multilayer structure (<b>a</b>), when delamination is between the 1st and 2nd layers (<b>b</b>), and when delamination is between the 2nd and 3rd layers (<b>c</b>).</p>
Full article ">Figure 8
<p>Simulation results of Lamb wave propagation in a WTB specimen with a delamination between the 2nd and 3rd layers (<b>a</b>), a hole drilled at the corresponding depth (<b>b</b>); the B-scan images are presented in (<b>c</b>,<b>d</b>) accordingly, and phase velocity variation in the A<sub>0</sub> mode at the defect location is shown in (<b>e</b>).</p>
Full article ">Figure 9
<p>The real WTB sample.</p>
Full article ">Figure 10
<p>Experimental setup of WTB inspection (<b>a</b>), B-scan image of propagated Lamb wave in region (<b>b</b>) and filtered experimental B-scan image (<b>c</b>).</p>
Full article ">Figure 10 Cont.
<p>Experimental setup of WTB inspection (<b>a</b>), B-scan image of propagated Lamb wave in region (<b>b</b>) and filtered experimental B-scan image (<b>c</b>).</p>
Full article ">Figure 11
<p>Variation in the phase velocity of the Lamb wave A<sub>0</sub> mode in defect-free and defect regions (<b>a</b>); the segments of the phase velocity dispersion curves in defect-free and defect regions (<b>b</b>).</p>
Full article ">
21 pages, 103718 KiB  
Article
The Fractal Dimension, Structure Characteristics, and Damage Effects of Multi-Scale Cracks on Sandstone Under Triaxial Compression
by Pengjin Yang, Shengjun Miao, Kesheng Li, Xiangfan Shang, Pengliang Li and Meifeng Cai
Fractal Fract. 2025, 9(1), 51; https://doi.org/10.3390/fractalfract9010051 - 17 Jan 2025
Viewed by 260
Abstract
To study the influence of the spatial distribution and structure of multi-scale cracks on the mechanical behavior of rocks, triaxial compression tests and cyclic triaxial complete loading and unloading tests were conducted on sandstone, with real-time wave velocity monitoring and CT scan testing. [...] Read more.
To study the influence of the spatial distribution and structure of multi-scale cracks on the mechanical behavior of rocks, triaxial compression tests and cyclic triaxial complete loading and unloading tests were conducted on sandstone, with real-time wave velocity monitoring and CT scan testing. The quantitative classification criteria for multi-scale cracks on sandstone were established, and the constraint effect of confining pressure was analyzed. The crack with a length less than 0.1 mm is considered a small-scale crack, 0.1–1 mm is a medium-scale crack, and larger than 1 mm is a large-scale crack. As the confining pressure increases, the spatial fractal dimension of large-scale cracks decreases, while that of medium-scale cracks increases, and that of small-scale cracks remains stable. The respective nonlinear models of the aspect ratio were established with the length and density of multi-scale cracks. The results indicate significant differences in the effects of cracks of different scales on rock damage. The distribution density of medium-scale cracks in the failed specimen is higher, which is the main reason to produce damage. The small-scale cracks mainly originate from relatively uniform initial cracks in rocks, mainly distributed in medium-density and low-density areas. The results of this research provide important insights into how to quantitatively evaluate the damage of rocks. Full article
(This article belongs to the Section Engineering)
Show Figures

Figure 1

Figure 1
<p>Processed sandstone specimens and their microscopic structures. (<b>a</b>) Processed standard-sized sandstone specimens; (<b>b</b>) Mineral analysis results of sandstone specimen; (<b>c</b>) Electron microscopy scanning results of sandstone with a magnification of 1000.</p>
Full article ">Figure 2
<p>Complete experimental system. (<b>a</b>) MTS-815 Rock Mechanics Testing System and the matching ultrasonic velocity testing system. (<b>b</b>) Prepared sandstone specimens with probes.</p>
Full article ">Figure 3
<p>The confining pressure and deviatoric stress paths of the two sets of tests in this study. (<b>a</b>) Loading path of confining pressure and deviatoric stress of TC test. (<b>b</b>) Loading and unloading paths for the confining pressure and deviatoric stress CTCLU test.</p>
Full article ">Figure 4
<p>Stress–strain curves of TC and CTCLU tests on sandstone under different confining pressures. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>2</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>4</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>8</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>e</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>12</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>f</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>16</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 5
<p>Reconstruction results of three-dimensional cracks in sandstone specimen TC-0.</p>
Full article ">Figure 6
<p>Total volume distribution of cracks with different volume size.</p>
Full article ">Figure 7
<p>The projection of spatial centroid coordinates of cracks in sandstone onto the <span class="html-italic">xy</span> plane. (<b>a</b>) The projection of the crack centroid coordinates on the <span class="html-italic">xy</span> plane and the radius from the plane center; (<b>b</b>) The projection of the spatial centroid coordinates of the medium-scale crack on specimen TC-0 within the range of <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>5</mn> <mo> </mo> <mi>mm</mi> <mo>≤</mo> <mi>z</mi> <mo>≤</mo> <mn>5</mn> <mo> </mo> <mi>mm</mi> </mrow> </semantics></math>; (<b>c</b>) The projection of the spatial centroid coordinates of the small-scale crack on specimen TC-0 within the range of <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>5</mn> <mo> </mo> <mi>mm</mi> <mo>≤</mo> <mi>z</mi> <mo>≤</mo> <mn>5</mn> <mo> </mo> <mi>mm</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 8
<p>The fractal dimension of medium- and small-scale cracks in sandstone. (<b>a</b>) Example of fractal dimension calculation for medium- and small-scale cracks, when the range is <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>30</mn> <mo> </mo> <mi>mm</mi> <mo>≤</mo> <mi>z</mi> <mo>≤</mo> <mn>20</mn> <mo> </mo> <mi>mm</mi> </mrow> </semantics></math>; (<b>b</b>) The fractal dimension of medium- and small-scale cracks with different heights.</p>
Full article ">Figure 9
<p>The volume of medium- and small-scale cracks under different crack size. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>4</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>8</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>16</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 10
<p>The variation law of spatial fractal dimension of multi scale cracks with confining pressure.</p>
Full article ">Figure 11
<p>The relationship between the wave velocity with stress level, when stress is unloaded and loaded completely. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>4</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>8</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>16</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 12
<p>The real-time wave velocity monitoring results and fitting curves when the stress is unloaded. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>4</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>8</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>16</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 13
<p>The real-time porosity evolution curves of sandstone with stress level. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>4</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>8</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>16</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 14
<p>The relationship between crack volume and crack structural parameters. (<b>a</b>) Schematic diagram of crack equivalent volume and its aspect ratio; (<b>b</b>) The relationship between the length and the aspect ratio of cracks, taking <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>16</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math> as an example.</p>
Full article ">Figure 15
<p>Theoretical relationship between cumulative crack volume and aspect ratio when <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>16</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 16
<p>The distribution curve of sandstone crack density with crack aspect ratio. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>4</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>8</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>16</mn> <mo> </mo> <mi>MPa</mi> </mrow> </semantics></math>.</p>
Full article ">
15 pages, 7313 KiB  
Article
A Wideband Eight-Port MIMO Antenna with Reduced Mutual Coupling for Future 5G mm-Wave Applications
by Muhammad Kabir Khan, Shaobin Liu and Muhammad Irshad Khan
Sensors 2025, 25(2), 484; https://doi.org/10.3390/s25020484 - 16 Jan 2025
Viewed by 206
Abstract
An eight-element MIMO antenna with a neutralization line was utilized for future 5G mm-wave applications. The MIMO configuration was designed for two ports, four ports and eight ports to validate the desired impedance and radiation characteristics. The measured results in terms of MIMO [...] Read more.
An eight-element MIMO antenna with a neutralization line was utilized for future 5G mm-wave applications. The MIMO configuration was designed for two ports, four ports and eight ports to validate the desired impedance and radiation characteristics. The measured results in terms of MIMO and scattering parameters correlate well with the simulated one. The printed eight-port antenna was a miniaturized size of 44 × 70 × 0.8 mm3. Roger RT/duroid 5880 substrate was used to print antennas. The presented antenna produced a vast bandwidth of 18 GHz, varying from 28 to 46 GHz, and achieved a reduced mutual coupling of 30 dB with 6.8–8.5 dBi gain. The eight-port antenna is compared with contemporary antennas considering size, isolation, impedance bandwidth, diversity characteristics and radiation properties, confirming that the presented antenna is a promising candidate for future 5G mm-wave applications. Full article
(This article belongs to the Special Issue Novel Antennas for Wireless Communication and Intelligent Sensing)
Show Figures

Figure 1

Figure 1
<p>Design development of the single-port antenna. (<b>a</b>) Rectangular antenna, (<b>b</b>) rectangular slot antenna, (<b>c</b>) rectangular chamfered edge antenna, and (<b>d</b>) proposed single-port antenna.</p>
Full article ">Figure 2
<p>S-parameter results for the development stages of the single-port antenna.</p>
Full article ">Figure 3
<p>(<b>a</b>) Front and (<b>b</b>) back sides of the dual-component MIMO antenna.</p>
Full article ">Figure 4
<p>The dual-port MIMO antenna S-parameter’s results.</p>
Full article ">Figure 5
<p>Isolation result of dual-port antenna with and without neutralization line.</p>
Full article ">Figure 6
<p>Radiation efficiency and gain of the dual-port MIMO antenna.</p>
Full article ">Figure 7
<p>ECC and DG of the suggested antenna.</p>
Full article ">Figure 8
<p>Reflection coefficient of the MIMO antenna. (<b>a</b>) Rectangular A, (<b>b</b>) slot V (<b>c</b>) slot D, (<b>d</b>) stub S, (<b>e</b>) ground slot R and (<b>f</b>) ground-stub B.</p>
Full article ">Figure 9
<p>Quad-port MIMO antenna design. (<b>a</b>) Top and (<b>b</b>) bottom view.</p>
Full article ">Figure 10
<p>S-parameter results for quad-port MIMO antenna.</p>
Full article ">Figure 11
<p>Peak gain and radiation efficiency plot.</p>
Full article ">Figure 12
<p>ECC and DG of the quad-port antenna.</p>
Full article ">Figure 13
<p>Antenna’s (<b>a</b>) front and (<b>b</b>) back views.</p>
Full article ">Figure 14
<p>Current distribution of the proposed MIMO antenna at 28 GHz, (<b>a</b>) port 1 excited and (<b>b</b>) port 7 excited.</p>
Full article ">Figure 15
<p>(<b>a</b>) Front and (<b>b</b>) back view of the fabricated antenna.</p>
Full article ">Figure 16
<p>S-Parameters of the proposed MIMO antenna. (<b>a</b>) Antenna 1 and antenna 2, (<b>b</b>) antenna 1 with antenna 3 and antenna 4, (<b>c</b>) antenna 1 with antenna 5 and antenna 6 and (<b>d</b>) antenna 1 with antenna 7 and antenna 8.</p>
Full article ">Figure 17
<p>Radiation patterns of presented MIMO antenna at (<b>a</b>) 30 GHz and (<b>b</b>) 40 GHz.</p>
Full article ">Figure 18
<p>Radiation patterns of element 1 in proposed antenna.</p>
Full article ">Figure 19
<p>Gain and radiation efficiency of the presented antenna.</p>
Full article ">Figure 20
<p>ECC and DG of the presented antenna.</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 283
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 ">
14 pages, 490 KiB  
Article
Compact High-Zoom-Ratio Mid-Wavelength Infrared Zoom Lens Design Based on Particle Swarm Optimization
by Zhenhao Liu, Jipeng Zhang, Yuqi Huang, Xin Zhang, Hongbo Wu and Jianping Zhang
Sensors 2025, 25(2), 467; https://doi.org/10.3390/s25020467 - 15 Jan 2025
Viewed by 242
Abstract
This paper presents an automated method for solving the initial structure of compact, high-zoom-ratio mid-wave infrared (MWIR) zoom lenses. Using differential analysis, the focal length variation process of zoom lenses under paraxial conditions is investigated, and a model for the focal power distribution [...] Read more.
This paper presents an automated method for solving the initial structure of compact, high-zoom-ratio mid-wave infrared (MWIR) zoom lenses. Using differential analysis, the focal length variation process of zoom lenses under paraxial conditions is investigated, and a model for the focal power distribution and relative motion of three movable lens groups is established. The particle swarm optimization (PSO) algorithm is introduced into the zooming process analysis, and a program is developed in MATLAB to solve for the initial structure. This algorithm integrates physical constraints from lens analysis and evaluates candidate solutions based on key design parameters, such as total lens length, zoom ratio, Petzval field curvature, and focal length at tele end. The results demonstrate that the proposed method can efficiently and accurately determine the initial structure of compact MWIR zoom lenses. Using this method, a mid-wave infrared zoom lens with a zoom ratio of 50×, a total length of less than 530 mm, and the ratio of focal length to total length approximately 2:1 was successfully designed. The design validates the effectiveness and practicality of this method in solving the initial structure of zoom lenses that meet complex design requirements. Full article
(This article belongs to the Section Sensing and Imaging)
Show Figures

Figure 1

Figure 1
<p>Paraxial structure diagram of a secondary imaging optical system.</p>
Full article ">Figure 2
<p>Diagram of movable lens groups in the zoom lens system.</p>
Full article ">Figure 3
<p>A flowchart of the zoom lens’ initial structure optimization based on particle swarm optimization algorithm.</p>
Full article ">Figure 4
<p>Flowchart of zoom lens initial structure optimization based on particle swarm optimization algorithm.</p>
Full article ">Figure 5
<p>Merit value with respect to the iteration times.</p>
Full article ">Figure 6
<p>Zoom trajectory of the movable lens group during zooming.</p>
Full article ">Figure 7
<p>(<b>a</b>) Zoom lens at tele-mid-wide constructions. (<b>b</b>) MTF of zoom lens at tele-mid-wide constructions.</p>
Full article ">
17 pages, 22331 KiB  
Article
Depth Estimation Based on MMwave Radar and Camera Fusion with Attention Mechanisms and Multi-Scale Features for Autonomous Driving Vehicles
by Zhaohuan Zhu, Feng Wu, Wenqing Sun, Quanying Wu, Feng Liang and Wuhan Zhang
Electronics 2025, 14(2), 300; https://doi.org/10.3390/electronics14020300 - 13 Jan 2025
Viewed by 440
Abstract
Autonomous driving vehicles have strong path planning and obstacle avoidance capabilities, which provide great support to avoid traffic accidents. Autonomous driving has become a research hotspot worldwide. Depth estimation is a key technology in autonomous driving as it provides an important basis for [...] Read more.
Autonomous driving vehicles have strong path planning and obstacle avoidance capabilities, which provide great support to avoid traffic accidents. Autonomous driving has become a research hotspot worldwide. Depth estimation is a key technology in autonomous driving as it provides an important basis for accurately detecting traffic objects and avoiding collisions in advance. However, the current difficulties in depth estimation include insufficient estimation accuracy, difficulty in acquiring depth information using monocular vision, and an important challenge of fusing multiple sensors for depth estimation. To enhance depth estimation performance in complex traffic environments, this study proposes a depth estimation method in which point clouds and images obtained from MMwave radar and cameras are fused. Firstly, a residual network is established to extract the multi-scale features of the MMwave radar point clouds and the corresponding image obtained simultaneously from the same location. Correlations between the radar points and the image are established by fusing the extracted multi-scale features. A semi-dense depth estimation is achieved by assigning the depth value of the radar point to the most relevant image region. Secondly, a bidirectional feature fusion structure with additional fusion branches is designed to enhance the richness of the feature information. The information loss during the feature fusion process is reduced, and the robustness of the model is enhanced. Finally, parallel channel and position attention mechanisms are used to enhance the feature representation of the key areas in the fused feature map, the interference of irrelevant areas is suppressed, and the depth estimation accuracy is enhanced. The experimental results on the public dataset nuScenes show that, compared with the baseline model, the proposed method reduces the average absolute error (MAE) by 4.7–6.3% and the root mean square error (RMSE) by 4.2–5.2%. Full article
Show Figures

Figure 1

Figure 1
<p>Plotting LiDAR and millimeter-wave radar point clouds in images. (<b>a</b>) LiDAR point cloud projection. (<b>b</b>) Millimeter-wave radar point cloud projection.</p>
Full article ">Figure 2
<p>Depth estimation using camera and millimeter-wave radar. (<b>a</b>) Input image. (<b>b</b>) Generating semi-dense depth estimation. (<b>c</b>) Generating dense depth estimation. Objects in the scene are highlighted with red box.</p>
Full article ">Figure 3
<p>Overall structure.</p>
Full article ">Figure 4
<p>Semi-dense depth estimation.Objects in the scene are highlighted with color boxes.</p>
Full article ">Figure 5
<p>Bidirectional attention feature fusion structure.</p>
Full article ">Figure 6
<p>Channel attention.</p>
Full article ">Figure 7
<p>Position attention.</p>
Full article ">Figure 8
<p>Comparison of MAE and RMSE during training using different methods. MAE curve on the left and RMSE curve on the right.</p>
Full article ">Figure 9
<p>The first column is the input image; the second column is the LiDAR ground truth; the third column is the result of our method. Different-colored bounding boxes are used to mark prominent areas in the image.</p>
Full article ">Figure 10
<p>The first column is the result of our method; the following columns represent the inference results of different methods. Red boxes are used to mark prominent areas in the image.</p>
Full article ">Figure 11
<p>The first column is the input image; the second column is the regional result of our method; the following columns represent the regional results of different methods. Regions in different colors are used to distinguish depths within the image.</p>
Full article ">
16 pages, 8853 KiB  
Article
The Practical Implications of Re-Referencing in ERP Studies: The Case of N400 in the Picture–Word Verification Task
by Vojislav Jovanović, Igor Petrušić, Vanja Ković and Andrej M. Savić
Diagnostics 2025, 15(2), 156; https://doi.org/10.3390/diagnostics15020156 - 11 Jan 2025
Viewed by 512
Abstract
Background: The selection of an optimal referencing method in event-related potential (ERP) research has been a long-standing debate, as it can significantly influence results and lead to data misinterpretation. Such misinterpretation can produce flawed scientific conclusions, like the inaccurate localization of neural processes, [...] Read more.
Background: The selection of an optimal referencing method in event-related potential (ERP) research has been a long-standing debate, as it can significantly influence results and lead to data misinterpretation. Such misinterpretation can produce flawed scientific conclusions, like the inaccurate localization of neural processes, and in practical applications, such as using ERPs as biomarkers in medicine, it may result in incorrect diagnoses or ineffective treatments. In line with the development and advancement of good scientific practice (GSP) in ERP research, this study sought to address several questions regarding the most suitable digital reference for investigating the N400 ERP component. Methods: The study was conducted on 17 neurotypical participants. Based on previous research, the references evaluated included the common average reference (AVE), mean earlobe reference (EARS), left mastoid reference (L), mean mastoids reference (MM), neutral infinity reference (REST), and vertex reference (VERT). Results: The results showed that all digital references, except for VERT, successfully elicited the centroparietal N400 effect in the picture–word verification task. The AVE referencing method showed the most optimal set of metrics in terms of effect size and localization, although it also produced the smallest difference waves. The most similar topographic dynamics in the N400 window were observed between the AVE and REST referencing methods. Conclusions: As the most optimal regions of interest (ROI) for the picture–word elicited N400 effect, nine electrode sites spanning from superior frontocentral to parietal regions were identified, showing consistent effects across all referencing methods except VERT. Full article
(This article belongs to the Special Issue EEG Analysis in Diagnostics)
Show Figures

Figure 1

Figure 1
<p>Example of experimental trial.</p>
Full article ">Figure 2
<p>Electrode placement and analysis zones. Green boxes represent laterality grouping: left, midline, and right. Different colors represent frontality grouping: red represents central electrodes, and blue represents parietal electrodes.</p>
Full article ">Figure 3
<p>Verification task grand average ERPs in different reference methods. The blue line represents congruent condition, the red line represents incongruent condition, and the black line represents difference wave.</p>
Full article ">Figure 4
<p>Voltage topographies of congruent and incongruent condition (300–500 ms) in different reference methods.</p>
Full article ">Figure 5
<p>The grand average difference ERPs of six frontal and parietal electrodes (C3, CZ, C4, P3, PZ, P4) for the AVE, EARS, L, MM and REST referencing methods.</p>
Full article ">Figure 6
<p>SPSM of different referencing methods for the 300–500 ms time window.</p>
Full article ">
22 pages, 8471 KiB  
Article
Metal Powder Production by Atomization of Free-Falling Melt Streams Using Pulsed Gaseous Shock and Detonation Waves
by Sergey M. Frolov, Vladislav S. Ivanov, Viktor S. Aksenov, Igor O. Shamshin, Fedor S. Frolov, Alan E. Zangiev, Tatiana I. Eyvazova, Vera Ya. Popkova, Maksim V. Grishin, Andrey K. Gatin and Tatiana V. Dudareva
J. Manuf. Mater. Process. 2025, 9(1), 20; https://doi.org/10.3390/jmmp9010020 - 10 Jan 2025
Viewed by 513
Abstract
A new method of producing metal powders for additive manufacturing by the atomization of free-falling melt streams using pulsed cross-flow gaseous shock or detonation waves is proposed. The method allows the control of shock/detonation wave intensity (from Mach number 4 to about 7), [...] Read more.
A new method of producing metal powders for additive manufacturing by the atomization of free-falling melt streams using pulsed cross-flow gaseous shock or detonation waves is proposed. The method allows the control of shock/detonation wave intensity (from Mach number 4 to about 7), as well as the composition and temperature of the detonation products by choosing proper fuels and oxidizers. The method is implemented in laboratory and industrial setups and preliminarily tested for melts of three materials, namely zinc, aluminum alloy AlMg5, and stainless steel AISI 304, possessing significantly different properties in terms of density, surface tension, and viscosity. Pulsed shock and detonation waves used for the atomization of free-falling melt streams are generated by the pulsed detonation gun (PDG) operating on the stoichiometric mixture of liquid hydrocarbon fuel and gaseous oxygen. The analysis of solidified particles and particle size distribution in the powder is studied by sifting on sieves, optical microscopy, laser diffraction wet dispersion method (WDM), and atomic force microscopy (AFM). The operation process is visualized by a video camera. The minimal size of the powders obtained by the method is shown to be as low as 0.1 to 1 μm, while the maximum size of particles exceeds 400–800 μm. The latter is explained by the deficit of energy in the shock-induced cross-flow for the complete atomization of the melt stream, in particular dense and thick (8 mm) streams of the stainless-steel melt. The mass share of particles with a fraction of 0–10 μm can be at least 20%. The shape of the particles of the finest fractions (0–30 and 30–70 μm) is close to spherical (zinc, aluminum) or perfectly spherical (stainless steel). The shape of particles of coarser fractions (70–140 μm and larger) is more irregular. Zinc and aluminum powders contain agglomerates in the form of particles with fine satellites. The content of agglomerates in stainless-steel powders is very low. In general, the preliminary experiments show that the proposed method for the production of finely dispersed metal powders demonstrates potential in terms of powder characteristics. Full article
Show Figures

Figure 1

Figure 1
<p>Schematic (<b>a</b>) and photograph (<b>b</b>) of the laboratory setup.</p>
Full article ">Figure 2
<p>Samples of aluminum powder: (<b>a</b>) on separator trays and (<b>b</b>) after collection and drying.</p>
Full article ">Figure 3
<p>Example of IP records in a single operation cycle during PDG operation in the frequency mode.</p>
Full article ">Figure 4
<p>PMSDs of zinc powder particles in separator trays #1–#4 obtained by means of dry sifting on sieves on fractions 140–250, 70–140, 30–70, and 0–30 μm; sample mass 313.8 g.</p>
Full article ">Figure 5
<p>Results of microscopic and AFM examination of zinc powder fractions (<b>a</b>) 140–250 µm and (<b>b</b>,<b>c</b>) 0–30 µm.</p>
Full article ">Figure 6
<p>Zinc powder PSDs obtained by laser diffraction WDM for several particle fractions: (<b>a</b>) 0–30 µm, (<b>b</b>) 30–70 µm, and (<b>c</b>) 70–140 µm.</p>
Full article ">Figure 7
<p>PMSDs of aluminum powder particles in separator trays #1–#4 obtained by means of dry sifting on sieves on fractions 140–250, 70–140, 30–70, and 0–30 μm; sample mass 143.2 g.</p>
Full article ">Figure 8
<p>Results of microscopic and AFM examination of aluminum powder fractions (<b>a</b>) 140–800 µm and (<b>b</b>,<b>c</b>) 0–30 µm.</p>
Full article ">Figure 9
<p>Aluminum powder PSDs obtained by laser diffraction WDM for several particle fractions: (<b>a</b>) 0–30 µm, (<b>b</b>) 30–70 µm, and (<b>c</b>) 70–140 µm.</p>
Full article ">Figure 10
<p>Sequential video frames of the shock-induced atomization process of the free-falling stream of stainless-steel melt.</p>
Full article ">Figure 11
<p>PMSDs of stainless-steel powder particles obtained by means of dry sifting on sieves on fractions (<b>a</b>) &gt;1000, 800–1000, 400–800, 250–400, 140–250, 70–140, 30–70, and 0–30 μm; and on fractions (<b>b</b>) 140–250, 70–140, 30–70, and 0–30 μm; sample weight 84.4 g.</p>
Full article ">Figure 12
<p>Results of microscopic and AFM examination of stainless-steel powder obtained on sieves (<b>a</b>) 70–140 µm and (<b>b</b>,<b>c</b>) 0–30 µm.</p>
Full article ">Figure 13
<p>Stainless-steel powder PSDs obtained by laser diffraction WDM for several particle fractions: (<b>a</b>) 30–70 µm, (<b>b</b>) 70–140 µm, and (<b>c</b>) 140–250 µm.</p>
Full article ">Figure 14
<p>Comparison of PSDs obtained by laser diffraction WDM for aluminum and zinc powders of fraction 0–30 µm.</p>
Full article ">Figure 15
<p>Comparison of PSDs obtained by laser diffraction WDM for zinc, aluminum, and stainless-steel powders of fraction 30–70 µm.</p>
Full article ">
26 pages, 1704 KiB  
Article
A Unified Design Methodology for Front-End RF/mmWave Receivers
by Anastasios Michailidis, Alexandros Chatzis, Panayiota Tsimpou, Vasiliki Gogolou and Thomas Noulis
Electronics 2025, 14(2), 235; https://doi.org/10.3390/electronics14020235 - 8 Jan 2025
Viewed by 299
Abstract
In this work, a unified design methodology for front-end RF/mmWave receivers is presented, aiming to significantly accelerate the design procedure of the front-end RF blocks in complex RX/TX chain implementations. The proposed design methodology is based on optimization loops with well-defined cost functions [...] Read more.
In this work, a unified design methodology for front-end RF/mmWave receivers is presented, aiming to significantly accelerate the design procedure of the front-end RF blocks in complex RX/TX chain implementations. The proposed design methodology is based on optimization loops with well-defined cost functions so as to minimize the design iterations that may be encountered during specification tuning. As proof of concept, two essential RF blocks widely used in RF receivers, a low-noise amplifier (LNA) and a voltage-controlled oscillator (VCO), were designed using the proposed unified methodology with a 65 nm RF-CMOS processing node. Finally, the derived designs were compared to similar designs in the literature, proving that the proposed unified methodology is capable of synthesizing RF/mmWave LNAs and VCOs with industry-standard specifications within a significantly faster time frame. 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>RF/mmWave circuit blocks that synthesize a full RX/TX system.</p>
Full article ">Figure 2
<p><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> cost function with respect to input transistor sizing and bias voltage.</p>
Full article ">Figure 3
<p>Small-signal representation of a cascoded LNA with source degeneration.</p>
Full article ">Figure 4
<p>Two-port network versus scattering parameters.</p>
Full article ">Figure 5
<p>Impedance matching cost functions fulfillment points using Smith chart representation.</p>
Full article ">Figure 6
<p>LC lossless tank illustration using active circuitry to compensate tank losses.</p>
Full article ">Figure 7
<p>Cross-coupled LC VCO architecture and its negative resistance small-signal equivalent circuit.</p>
Full article ">Figure 8
<p>Z-Parameter definitions using a two-port network.</p>
Full article ">Figure 9
<p>LC-tank <math display="inline"><semantics> <msub> <mi>Z</mi> <mn>11</mn> </msub> </semantics></math>-Parameters with respect to frequency.</p>
Full article ">Figure 10
<p>Inductor one-port network for Y-parameter characterization.</p>
Full article ">Figure 11
<p>Inductor characterization using Y-Parameters.</p>
Full article ">Figure 12
<p>Optimum search cost function with respect to geometry parameters at <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math> GHz.</p>
Full article ">Figure 13
<p>LNA design methodology flowchart.</p>
Full article ">Figure 14
<p>Load inductor tuning has an impact on both input reflection coefficient and forward gain.</p>
Full article ">Figure 15
<p>VCO design methodology flowchart.</p>
Full article ">Figure 16
<p>Common source cascoded LNA architecture.</p>
Full article ">Figure 17
<p>Physical design of the synthesized LNA.</p>
Full article ">Figure 18
<p>(<b>a</b>) Pre-layout and (<b>b</b>) post-layout S-Parameter, (<b>c</b>) noise figure performance and (<b>d</b>) stability factor of the synthesized LNA.</p>
Full article ">Figure 19
<p><math display="inline"><semantics> <msup> <mn>1</mn> <mrow> <mi>S</mi> <mi>T</mi> </mrow> </msup> </semantics></math> and <math display="inline"><semantics> <msup> <mn>3</mn> <mrow> <mi>R</mi> <mi>D</mi> </mrow> </msup> </semantics></math>-order intercept points of the synthesized LNA.</p>
Full article ">Figure 20
<p>Cross-coupled LC VCO architecture.</p>
Full article ">Figure 21
<p>Physical design of the synthesized VCO.</p>
Full article ">Figure 22
<p>(<b>a</b>) Available frequency tuning range, pre- and post-layout; (<b>b</b>) phase noise performance; (<b>c</b>) output transient signals and (<b>d</b>) output frequency spectrum of the synthesized VCO.</p>
Full article ">
18 pages, 3386 KiB  
Article
Adaptive Filtering for Channel Estimation in RIS-Assisted mmWave Systems
by Shuying Shao, Tiejun Lv and Pingmu Huang
Sensors 2025, 25(2), 297; https://doi.org/10.3390/s25020297 - 7 Jan 2025
Viewed by 368
Abstract
The advent of millimeter-wave (mmWave) massive multiple-input multiple-output (MIMO) systems, coupled with reconfigurable intelligent surfaces (RISs), presents a significant opportunity for advancing wireless communication technologies. This integration enhances data transmission rates and broadens coverage areas, but challenges in channel estimation (CE) remain due [...] Read more.
The advent of millimeter-wave (mmWave) massive multiple-input multiple-output (MIMO) systems, coupled with reconfigurable intelligent surfaces (RISs), presents a significant opportunity for advancing wireless communication technologies. This integration enhances data transmission rates and broadens coverage areas, but challenges in channel estimation (CE) remain due to the limitations of the signal processing capabilities of RIS. To address this, we propose an adaptive channel estimation framework comprising two algorithms: log-sum normalized least mean squares (Log-Sum NLMS) and hybrid normalized least mean squares-normalized least mean fourth (Hybrid NLMS-NLMF). These algorithms leverage the sparse nature of mmWave channels to improve estimation accuracy. The Log-Sum NLMS algorithm incorporates a log-sum penalty in its cost function for faster convergence, while the Hybrid NLMS-NLMF employs a mixed error function for better performance across varying signal-to-noise ratio (SNR) conditions. Our analysis also reveals that both algorithms have lower computational complexity compared to existing methods. Extensive simulations validate our findings, with results illustrating the performance of the proposed algorithms under different parameters, demonstrating significant improvements in channel estimation accuracy and convergence speed over established methods, including NLMS, sparse exponential forgetting window least mean square (SEFWLMS), and sparse hybrid adaptive filtering algorithms (SHAFA). Full article
(This article belongs to the Section Communications)
Show Figures

Figure 1

Figure 1
<p>The RIS-aided wireless communication systems.</p>
Full article ">Figure 2
<p>Adaptive filter framework.</p>
Full article ">Figure 3
<p>NMSE of different estimation algorithms versus SNR.</p>
Full article ">Figure 4
<p>NMSE of different estimation algorithms versus number of iterations at an SNR of 3 dB.</p>
Full article ">Figure 5
<p>NMSE of different estimation algorithms versus number of iterations at an SNR of 13 dB.</p>
Full article ">Figure 6
<p>Impact of the parameter <math display="inline"><semantics> <mi>α</mi> </semantics></math> on the NMSE performance of the Hybrid NLMS-NLMF algorithm.</p>
Full article ">Figure 7
<p>Impact of the parameter <math display="inline"><semantics> <mi>α</mi> </semantics></math> on the convergence trend of the Hybrid NLMS-NLMF algorithm at an SNR of 10 dB.</p>
Full article ">Figure 8
<p>Impact of the parameter <math display="inline"><semantics> <mi>ρ</mi> </semantics></math> on the NMSE performance of the Hybrid NLMS-NLMF algorithm.</p>
Full article ">Figure 9
<p>Impact of the parameter <math display="inline"><semantics> <mi>ρ</mi> </semantics></math> on the convergence trend of the Hybrid NLMS-NLMF algorithm at an SNR of 10 dB.</p>
Full article ">Figure 10
<p>Impact of the parameter <math display="inline"><semantics> <mi>μ</mi> </semantics></math> on the NMSE performance of the Hybrid NLMS-NLMF algorithm.</p>
Full article ">Figure 11
<p>Impact of the parameter <math display="inline"><semantics> <mi>μ</mi> </semantics></math> on the convergence trend of the Hybrid NLMS-NLMF algorithm at an SNR of 10 dB.</p>
Full article ">Figure 12
<p>Impact of RIS elements on the NMSE performance of the Hybrid NLMS-NLMF algorithm.</p>
Full article ">
19 pages, 5440 KiB  
Article
Synthesis, Electrical Conductivity, and Wave-Absorption Performances of Bamboo-Based Composites Co-Doped with Graphene Oxide and Polyaniline
by Jin Wang, Wangjun Wu, Wenfu Zhang, Ying Zhao, Hongyan Wang, Shaofei Yuan and Jian Zhang
Polymers 2025, 17(1), 78; https://doi.org/10.3390/polym17010078 - 31 Dec 2024
Viewed by 502
Abstract
Bamboo was carbonized and further modified via co-doping with graphene oxide (GO) and polyaniline (PANI) to prepare microwave absorption composites (GO/PANI/CB) by in situ polymerization of 1R-(-)-Camphorsulfonic acid (L-CSA). The conductivity of GO/PANI/CB reached 2.17 ± 0.05 S/cm under the optimized process conditions. [...] Read more.
Bamboo was carbonized and further modified via co-doping with graphene oxide (GO) and polyaniline (PANI) to prepare microwave absorption composites (GO/PANI/CB) by in situ polymerization of 1R-(-)-Camphorsulfonic acid (L-CSA). The conductivity of GO/PANI/CB reached 2.17 ± 0.05 S/cm under the optimized process conditions. The oxygen-containing group of GO reacts with PANI to form hydrogen bonds and thus polymerize. The GO and PANI particles covered the carbonized bamboo (CB) surface in a disordered aggregation form. Based on the measuring method of the vector network analyzer (VNA), the microwave-absorption performance of GO/PANI/CB was investigated. With 30% addition of GO/PANI/CB, the minimum reflection loss (RLmin) at 7.12 GHz with a thickness of 3.5 mm of samples reached −49.83 dB. The effective absorption bandwidth (<−10 dB) is as high as 4.72 GHz with a frequency range of 11.68–16.40 GHz and a thickness of 2 mm. Compared with many PANI based electromagnetic wave absorbing materials reported in recent years, GO/PANI/CB provides improved microwave-absorption performance while maintaining high absorption bandwidth. GO/PANI/CB exhibited the advantages of simple preparation, low cost, renewability, light texture, thinness, wide absorption bandwidth, and strong absorption ability, and can be used for new microwave absorption materials. Full article
Show Figures

Figure 1

Figure 1
<p>Schematic illustration of the synthesis and polymerization process of GO/PANI/CB.</p>
Full article ">Figure 2
<p>The conductivity of all samples (<b>a</b>), the conductivity of CB, PANI/CB, and GO/PANI/CB (<b>b</b>).</p>
Full article ">Figure 3
<p>FTIR spectra of GO/PANI/CB, PANI/CB, and CB.</p>
Full article ">Figure 4
<p>XRD patterns of GO/PANI/CB, PANI/CB, and CB.</p>
Full article ">Figure 5
<p>XPS spectra of GO/PANI/CB, PANI/CB, and CB (<b>a</b>); S<sub>2p</sub> (<b>b</b>), C<sub>1s</sub> (<b>c</b>), N<sub>1s</sub> (<b>d</b>), and O<sub>1s</sub> (<b>e</b>) regions of GO/PANI/CB.</p>
Full article ">Figure 6
<p>SEM images of CB (<b>a</b>,<b>d</b>), PANI/CB (<b>b</b>,<b>e</b>), and GO/PANI/CB (<b>c</b>,<b>f</b>).</p>
Full article ">Figure 7
<p>SEM images of GO/PANI/CB (<b>a</b>) and EDS spectra of GO/PANI/CB (<b>b</b>). The inset tables present the element contents. C (<b>c</b>), N (<b>d</b>), O (<b>e</b>), and S (<b>f</b>) element mapping images of GO/PANI/CB.</p>
Full article ">Figure 8
<p>TG curves (<b>a</b>) and DSC curves (<b>b</b>) of GO/PANI/CB, PANI/CB, and CB.</p>
Full article ">Figure 9
<p>The frequency dependence of the real part (<b>a</b>) and imaginary part (<b>b</b>) of the complex permittivity and complex permeability (<b>c</b>) of GO/PANI/CB, PANI/CB, and CB, as well as the corresponding dielectric loss tangent (<b>d</b>).</p>
Full article ">Figure 10
<p>Cole-Cole semicircles of GO/PANI/CB (<b>a</b>), PANI/CB (<b>b</b>), and CB (<b>c</b>).</p>
Full article ">Figure 11
<p>The calculated RL (dB) of GO/PANI/CB (<b>a</b>), PANI/CB (<b>b</b>) and CB (<b>c</b>) in the frequency range of 2–18 GHz.</p>
Full article ">Figure 12
<p>Reflection loss versus filler loading for the typical graphene/polyaniline based composites and carbon based materials reported in the recent literature.</p>
Full article ">Figure 13
<p>Schematic illustration of the microwave absorption mechanism for the GO/PANI/CB composite.</p>
Full article ">
8 pages, 1714 KiB  
Article
Longitudinally Resolved Terahertz Radiation Characteristics Along Two-Color Filament in Air
by Juan Long, Tiejun Wang, Fukang Yin, Yaoxiang Liu, Yingxia Wei, Chengpu Liu and Yuxin Leng
Plasma 2025, 8(1), 1; https://doi.org/10.3390/plasma8010001 - 29 Dec 2024
Viewed by 409
Abstract
The evolution of the THz waveform generated from the two-color air filament was experimentally investigated by moving an iris along the plasma channel. By taking the differentiation of the measured THz waveforms, the local longitudinally resolved THz waves along a 54 mm-long filament [...] Read more.
The evolution of the THz waveform generated from the two-color air filament was experimentally investigated by moving an iris along the plasma channel. By taking the differentiation of the measured THz waveforms, the local longitudinally resolved THz waves along a 54 mm-long filament were obtained. The local THz pulse underwent periodic phase shifts. A theoretical deduction indicates that the phase shifts are mainly caused by the dispersion in the plasma channel which plays a dominant role in the evolution of the local THz waveforms. Full article
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>(<b>a</b>) Schematic diagram of the experimental setup; (<b>b</b>) The fluorescence image of laser plasma channel in air taken by a digital camera from the side.</p>
Full article ">Figure 2
<p>The amplitude of the THz signal as a function of the BBO crystal to the lens distance. Point A and point B represent the BBO-lens distances of 23.5 and 26.7 cm, respectively, in the two experimental conditions.</p>
Full article ">Figure 3
<p>The THz waveforms generated from different filament lengths at BBO–Lens distances of (<b>a</b>) 23.5 cm and (<b>d</b>) 26.7 cm (<b>b</b>,<b>e</b>). The local THz waveforms at different longitudinal positions of the filament in (<b>a</b>,<b>d</b>). The corresponding phase of the local THz waveforms (black dots) and the simulation results (red square) are shown in (<b>c</b>,<b>f</b>).</p>
Full article ">Figure 4
<p>The simulated THz phase as a function of filament position with or without the Gouy phase at BBO–Lens distances of (<b>a</b>) 23.5 cm and (<b>b</b>) 26.7 cm. The phase of the simulation results with only the Gouy phase at BBO–Lens distances of (<b>c</b>) 23.5 cm and (<b>d</b>) 26.7 cm.</p>
Full article ">
15 pages, 1844 KiB  
Article
Sex Differences in Gut Microbiota and Their Relation to Arterial Stiffness (MIVAS Study)
by Rita Salvado, Cristina Lugones-Sánchez, Sandra Santos-Minguez, Susana González-Sánchez, José A. Quesada, Rocío Benito, Emiliano Rodríguez-Sánchez, Manuel A. Gómez-Marcos, Pedro Guimarães-Cunha, Jesús M. Hernandez-Rivas, Alex Mira, Luis García-Ortiz and MIVAS Investigators
Nutrients 2025, 17(1), 53; https://doi.org/10.3390/nu17010053 - 27 Dec 2024
Viewed by 659
Abstract
Background: Recent research highlights the potential role of sex-specific variations in cardiovascular disease. The gut microbiome has been shown to differ between the sexes in patients with cardiovascular risk factors. Objectives: The main objective of this study is to analyze the differences between [...] Read more.
Background: Recent research highlights the potential role of sex-specific variations in cardiovascular disease. The gut microbiome has been shown to differ between the sexes in patients with cardiovascular risk factors. Objectives: The main objective of this study is to analyze the differences between women and men in the relationship between gut microbiota and measures of arterial stiffness. Methods: We conducted a cross-sectional study in Spain, selecting 180 subjects (122 women, 58 men) aged between 45 and 74. Subjects with arterial stiffness were identified by the presence of at least one of the following: carotid–femoral pulse wave velocity (cf-PWV) above 12 mm/s, cardio–ankle vascular index (CAVI) above nine, or brachial–ankle pulse wave velocity (ba-PWV) above 17.5 m/s. All other cases were considered subjects without arterial stiffness. The composition of the gut microbiome in fecal samples was determined by 16S rRNA sequencing. Results: We found that women have a more diverse microbiome than men (Shannon, p < 0.05). There is also a significant difference in gut microbiota composition between sexes (Bray–Curtis, p < 0.01). Dorea, Roseburia, and Agathobacter, all of them short-chain fatty-acid producers, were more abundant in women’s microbiota (log values > 1, p-value and FDR < 0.05). Additionally, Blautia was more abundant in women when only the subjects with arterial stiffness were considered. According to logistic regression, Roseburia was negatively associated with arterial stiffness in men, while Bifidobacterium and Subdoligranulum were positively related to arterial stiffness. Conclusions: In the Spanish population under study, women had higher microbiome diversity and potentially protective genera. The host’s gender determines the influence of the same bacteria on arterial stiffness. Trial Registration Number: NCT03900338. Full article
(This article belongs to the Special Issue Diet–Host–Gut Microbiota Interactions and Human Health)
Show Figures

Figure 1

Figure 1
<p>Phylum relative abundance by sex. <span class="html-italic">Firmicutes</span>: 70% (males (68%), female (71%); <span class="html-italic">p</span> &lt; 0.01); <span class="html-italic">Bacteriodota</span>: 22% (males (25%), females (20%); <span class="html-italic">p</span> &lt; 0.01).</p>
Full article ">Figure 2
<p>Principal Coordinate Analysis using Bray–Curtis Dissimilarity between sex (genus level). In this PCA plot, red points correspond to samples from women, and blue points correspond to male samples. Ellipses indicate group samples.</p>
Full article ">Figure 3
<p>The bar chart shows differentially expressed genes in women vs. men, considering all the samples (blue) and only subjects with arterial stiffness (grey). FDR—false discovery rate; LogFC—log fold change. * significant results (<span class="html-italic">p</span> &lt; 0.05; FDR &lt; 0.05; log FC &gt; −1 or &gt;1).</p>
Full article ">Figure 4
<p>Forest plot showing the logistic regression results of microbiome abundance (independent variable) and arterial stiffness (dependent variable). Model 1: adjusted for sex and age. Model 2: adjusted for Model 1 and body mass index, hemoglobin A1c, total cholesterol, HDL cholesterol, LDL cholesterol, and systolic blood pressure. Model 3: adjusted for Model 2 and Mediterranean diet score. * <span class="html-italic">p</span>-value &lt; 0.05.</p>
Full article ">Figure 5
<p>The forest plot shows the logistic regression results of microbiome abundance (independent variable) and arterial stiffness (dependent variable) in men and women. Model 1: adjusted for age. Model 2: adjusted for Model 1 and body mass index, hemoglobin A1c, total cholesterol, HDL cholesterol, LDL cholesterol, and systolic blood pressure. Model 3: adjusted for Model 2 and Mediterranean diet score. * <span class="html-italic">p</span>-value &lt; 0.05.</p>
Full article ">
22 pages, 4321 KiB  
Article
Real-Time Interference Mitigation for Reliable Target Detection with FMCW Radar in Interference Environments
by Youlong Weng, Ziang Zhang, Guangzhi Chen, Yaru Zhang, Jiabao Chen and Hongzhan Song
Remote Sens. 2025, 17(1), 26; https://doi.org/10.3390/rs17010026 - 25 Dec 2024
Viewed by 459
Abstract
Frequency-modulated continuous-wave (FMCW) millimeter-wave (mmWave) radar systems are increasingly utilized in environmental sensing due to their high range resolution and robust sensing ability in severe weather environments. However, mutual interference among radar systems significantly degrades the target detection capability. Recent advancements in interference [...] Read more.
Frequency-modulated continuous-wave (FMCW) millimeter-wave (mmWave) radar systems are increasingly utilized in environmental sensing due to their high range resolution and robust sensing ability in severe weather environments. However, mutual interference among radar systems significantly degrades the target detection capability. Recent advancements in interference mitigation utilizing deep learning (DL) approaches have demonstrated promising results. DL-based approaches typically have high computational costs, which makes them unsuitable for real-time applications with strict latency requirements and limited computing resources. In this paper, we propose an efficient solution for real-time radar interference mitigation. A lightweight transformer, which is smaller and faster than the baseline transformer, is designed to reduce interference. The integration of linear attention mechanisms with depthwise separable convolutions significantly reduces the network’s computational complexity while maintaining a comparable performance. In addition, a two-stage knowledge distillation (KD) process is deployed to compress the network and enhance its efficiency. The staged distillation approach alleviates the training difficulties associated with substantial differences between the teacher and student networks. Both simulated and real-world experiments demonstrate that the proposed method outperforms the state-of-the-art methods while achieving high processing speeds. Full article
Show Figures

Figure 1

Figure 1
<p>The scenario in which mutual interference occurs.</p>
Full article ">Figure 2
<p>The IF signal with interferences in the time domain and resulted range profile.</p>
Full article ">Figure 3
<p>The overall framework of the baseline model RIMformer.</p>
Full article ">Figure 4
<p>Structure of RIMformer block.</p>
Full article ">Figure 5
<p>Architecture diagram for two-stage KD.</p>
Full article ">Figure 6
<p>Optimizing KD through dynamic loss balancing.</p>
Full article ">Figure 7
<p>Comparison of the output of different models in ablation experiments in the form of RD maps.</p>
Full article ">Figure 8
<p>Comparison of results from different training methods.</p>
Full article ">Figure 9
<p>Comparison of the output of different models trained by different methods in the form of RD maps.</p>
Full article ">Figure 10
<p>The performance of models trained by the three different ways at different SNRs.</p>
Full article ">Figure 11
<p>Comparison of time-domain waveforms and time-frequency plots after interference suppression.</p>
Full article ">Figure 12
<p>Comparison of RD maps for different interference suppression methods.</p>
Full article ">Figure 13
<p>Setup of measured experiments.</p>
Full article ">Figure 14
<p>The time-domain waveforms and range profiles in measured experiments. (<b>a</b>) The time-domain waveforms without and with interference in scenario 1. (<b>b</b>) The time-domain waveforms without and with interference in scenario 2. (<b>c</b>) The range profiles without and with interference in scenario 1. (<b>d</b>) The range profiles without and with interference in scenario 2. (<b>e</b>) Range profiles comparison after interference suppression in scenario 1. (<b>f</b>) Range profiles comparison after interference suppression in scenario 2.</p>
Full article ">Figure 15
<p>Comparison of quantitative results for different SNRs.</p>
Full article ">
12 pages, 4563 KiB  
Communication
A Submicrosecond-Response Ultrafast Microwave Ranging Method Based on Optically Generated Frequency-Modulated Pulses
by Yifei Sun, Yongchao Chen, Longhuang Tang, Xing Jia, Heli Ma, Xiang Wang, Long Chen, Shenggang Liu, Tianjiong Tao, Jian Wu, Chengjun Li, Shuanyu Liu, Weilu Chen, Wei Gu, Jia Shi and Jidong Weng
Sensors 2025, 25(1), 58; https://doi.org/10.3390/s25010058 - 25 Dec 2024
Viewed by 326
Abstract
An ultrafast microwave ranging method based on optically generated frequency-modulated microwave pulses is proposed in this study. The theoretical analysis demonstrated that nanosecond-scale linear frequency modulation microwave pulse can be obtained by femtosecond laser interference under the condition of unbalanced dispersion, which can [...] Read more.
An ultrafast microwave ranging method based on optically generated frequency-modulated microwave pulses is proposed in this study. The theoretical analysis demonstrated that nanosecond-scale linear frequency modulation microwave pulse can be obtained by femtosecond laser interference under the condition of unbalanced dispersion, which can be used to achieve a high temporal resolution of the displacement change in the measurement by the principle of frequency modulation continuous wave (FMCW) radar. The proof-of-principle experiment successfully measured the displacement change with an error of 2.5 mm and a range of 0.6 m, with a response time of 468 ns. Compared to existing microwave ranging technologies, the temporal resolution was improved by two orders of magnitude, which greatly improves the temporal resolution of distance measurement in the field of microwave FMCW radar. Full article
(This article belongs to the Special Issue Recent Advances of FMCW-Based Radar Sensors)
Show Figures

Figure 1

Figure 1
<p>The basic principle of ultrafast microwave ranging.</p>
Full article ">Figure 2
<p>(<b>a</b>,<b>b</b>) Temporal waveforms; (<b>c</b>,<b>d</b>) STFT analyses of the simulated microwave waveforms when tuning VODLs; and (<b>e</b>,<b>f</b>) the waveform of the IF signal obtained by mixing the transmitted signal with the echo signal and its STFT analyses.</p>
Full article ">Figure 3
<p>Schematic of the proposed method.</p>
Full article ">Figure 4
<p>(<b>a</b>,<b>c</b>) Temporal waveforms; (<b>b</b>,<b>d</b>) STFT analyses of the generated microwave waveforms; and (<b>e</b>,<b>f</b>) the linearity of the up-chirp and down-chirp waveforms.</p>
Full article ">Figure 5
<p>(<b>a</b>) Temporal waveforms; (<b>b</b>) STFT analyses of the IF signal; (<b>c</b>) typical Fourier transform analysis spectrum; and (<b>d</b>) generated microwave pulses.</p>
Full article ">Figure 6
<p>(<b>a</b>) The ranging resolution at distances of 40 cm, 50 cm, and 60 cm. (<b>b</b>) Ranging results.</p>
Full article ">Figure 7
<p>(<b>a</b>) Waveform diagram of an IF signal in the distance range of 40, 50, and 60 cm. (<b>b</b>) Fourier transforms of IF signals at distances of 40, 50 and 60 cm.</p>
Full article ">Figure 8
<p>The measured distance stability of 50 measurements at about (<b>a</b>) 40 cm, (<b>b</b>) 50 cm, and (<b>c</b>) 60 cm. (<b>d</b>) The distribution histogram of measured values at different distances.</p>
Full article ">
Back to TopTop