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15 pages, 16970 KiB  
Article
The Development of Photovoltaics in the Countries of Central and Eastern Europe in the Context of Regulatory Changes: A Case Study of the Czech Republic and Poland
by Maciej Dzikuć, Arkadiusz Piwowar and Maria Dzikuć
Energies 2025, 18(4), 817; https://doi.org/10.3390/en18040817 (registering DOI) - 10 Feb 2025
Viewed by 234
Abstract
The Czech Republic and Poland are struggling with problems related to the development of photovoltaics. Both analyzed countries had periods of dynamic development of this renewable energy source (RES). However, neither the Czech Republic nor Poland have developed mechanisms that would lead to [...] Read more.
The Czech Republic and Poland are struggling with problems related to the development of photovoltaics. Both analyzed countries had periods of dynamic development of this renewable energy source (RES). However, neither the Czech Republic nor Poland have developed mechanisms that would lead to the stable development of photovoltaic installations in the long term. The analyses presented in this article demonstrate the implementation of extreme solutions by these countries, which led either to stagnation in the development of photovoltaics or to an excessive increase in the installed capacity, including RES, which then had to be stopped due to, for example, the failure of the power grids to match the increasing capacity. This article conducted research based on secondary data and using the Foresight method. The aim of this manuscript is to present the conditions related to the development of photovoltaics in the Czech Republic and Poland. This article also points to the barriers limiting the development of this type of RES and the potential of solutions related to, e.g., energy storage, which will allow for maintaining stable development of photovoltaics in the future and will prevent excessive overloading of power grids. The research results indicate that in the context of further development of photovoltaics in the study area, what is important are, e.g., changes in legal regulations and financial incentives that will enable the development of micro-installations within energy communities to a greater extent, including co-financing for energy storage. Other factors were also noted, including interconnection capacity within the energy systems of these countries, as well as externally. Full article
(This article belongs to the Special Issue Policy and Economic Analysis of Energy Systems)
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Figure 1
<p>Photovoltaic electricity potential in the Czech Republic [<a href="#B42-energies-18-00817" class="html-bibr">42</a>].</p>
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<p>Photovoltaic electricity potential in Poland [<a href="#B48-energies-18-00817" class="html-bibr">48</a>].</p>
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<p>Photovoltaics in the Czech Republic and in Poland [<a href="#B50-energies-18-00817" class="html-bibr">50</a>].</p>
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30 pages, 17496 KiB  
Article
Frequency-Domain Finite Element Modeling of Seismic Wave Propagation Under Different Boundary Conditions
by Ying Zhang, Haiyang Liu, Shikun Dai and Herui Zhang
Mathematics 2025, 13(4), 578; https://doi.org/10.3390/math13040578 (registering DOI) - 10 Feb 2025
Viewed by 232
Abstract
Seismic wave propagation in complex terrains, especially in the presence of air layers, plays a crucial role in accurate subsurface imaging. However, the influence of different boundary conditions on seismic wave propagation characteristics has not been fully explored. This study employs the finite [...] Read more.
Seismic wave propagation in complex terrains, especially in the presence of air layers, plays a crucial role in accurate subsurface imaging. However, the influence of different boundary conditions on seismic wave propagation characteristics has not been fully explored. This study employs the finite element method (FEM) to simulate and analyze seismic wavefields under different boundary conditions, including perfectly matched layer (PML), Neumann free boundary conditions, and air layer conditions. First, the finite element solution for the 2D frequency-domain acoustic wave equation is introduced, and the correctness of the algorithm is validated using a homogeneous model. Then, both horizontal and undulating terrain interfaces are designed to investigate the kinematic and dynamic characteristics of the wavefields under different boundary conditions. The results show that PML boundaries effectively absorb seismic waves, prevent reflections, and ensure stable wave propagation, making them an ideal choice for simulating open boundaries. In contrast, Neumann boundaries generate significant reflected waves, particularly in undulating terrains, complicating the wavefield characteristics. Introducing an air layer alters the dynamics of the wavefield, leading to energy leakage and multi-path effects, which are more consistent with real-world seismic-geophysical models. Finally, the computational results using the Overthrust model under different boundary conditions further demonstrate that different boundary conditions significantly affect wavefield morphology. It is essential to select appropriate boundary conditions based on the specific simulation requirements, and boundary conditions with an air layer are most consistent with real seismic geological models. This study provides new insights into the role of boundary conditions in seismic numerical simulations and offers theoretical guidance for improving the accuracy of wavefield simulations in realistic geological scenarios. Full article
(This article belongs to the Special Issue Analytical Methods in Wave Scattering and Diffraction, 2nd Edition)
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Figure 1
<p>Schematic diagram of model adaptive meshing.</p>
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<p>Schematic diagram of the homogeneous model. The red star represents a point source.</p>
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<p>Frequency-domain wavefield of the homogeneous model. ((<b>a</b>–<b>c</b>) are the real parts of the wavefield of 20 Hz, 40 Hz, and 60 Hz, and (<b>d</b>–<b>f</b>) are the imaginary parts of the wavefield of 20 Hz, 40 Hz, and 60 Hz).</p>
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<p>Time-domain wavefield snapshot of homogeneous model. (<b>a</b>–<b>f</b>) represent the wavefield snapshots at 0.05 s, 0.1 s, 0.15 s, 0.2 s, 0.3 s, and 0.4 s, respectively.</p>
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<p>Seismic trace record at z = 0 m.</p>
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<p>Models under different boundary conditions when the seismic source is located on the ground. The red star represents a point source. ((<b>a</b>) is the PML absorption boundary condition used on the ground, (<b>b</b>) is the free boundary condition used on the ground, and (<b>c</b>) is the addition of an air layer and the PML absorption boundary used above the air layer).</p>
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<p>When the seismic source is located on the ground, the real parts of the wavefield with frequencies of 20 Hz, 40 Hz, and 60 Hz under different boundary conditions. ((<b>a</b>–<b>c</b>) are the real parts of the wavefield with different frequencies under PML absorption boundary conditions, (<b>d</b>–<b>f</b>) are the real parts of the wavefield with different frequencies under Neumann boundary conditions, and (<b>g</b>–<b>i</b>) are the real parts of the wavefield with different frequencies considering the air layer).</p>
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<p>When the seismic source is located on the ground, the imaginary parts of the wavefield with frequencies of 20 Hz, 40 Hz, and 60 Hz under different boundary conditions. ((<b>a</b>–<b>c</b>) are the imaginary parts of the wavefield with different frequencies under PML absorption boundary conditions, (<b>d</b>–<b>f</b>) are the imaginary parts of the wavefield with different frequencies under Neumann boundary conditions, and (<b>g</b>–<b>i</b>) are the imaginary parts of the wavefield with different frequencies considering the air layer).</p>
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<p>Comparison of wavefield details captured under different boundary conditions at 20 Hz. The red arrow compares the wavefield energy near the source; the yellow arrow compares the wavefield shape near the surface. ((<b>a</b>–<b>c</b>) are the real parts of the 20 Hz wavefield under PML, Neumann, and air layer boundary conditions, respectively; (<b>d</b>–<b>f</b>) are the imaginary parts of the 20 Hz wavefield under PML, Neumann, and air layer boundary conditions, respectively).</p>
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<p>When the seismic source is located on the ground, the real and imaginary parts of the 20 Hz wavefield under different boundary conditions. ((<b>a</b>) is the comparison of the real part of the 20 Hz wavefield, and (<b>b</b>) is the comparison of the imaginary part of the 20 Hz wavefield).</p>
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<p>When the seismic source is located on the ground, the real and imaginary parts of the 40 Hz wavefield under different boundary conditions. ((<b>a</b>) is the comparison of the real part of the 40 Hz wavefield, and (<b>b</b>) is the comparison of the imaginary part of the 40 Hz wavefield).</p>
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<p>When the seismic source is located on the ground, the real and imaginary parts of the 60 Hz wavefield under different boundary conditions. ((<b>a</b>) is the comparison of the real part of the 60 Hz wavefield, and (<b>b</b>) is the comparison of the imaginary part of the 60 Hz wavefield).</p>
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<p>Comparison of wavefield snapshots under different boundary conditions when the seismic source is located on the ground. ((<b>a</b>–<b>c</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.15 s under PML boundary conditions; (<b>d</b>–<b>f</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.15 s under Neumann boundary conditions; and (<b>g</b>–<b>i</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.15 s considering the air layer).</p>
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<p>Comparison of wavefield snapshots under different boundary conditions after removing the air layer. ((<b>a</b>–<b>c</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.15 s under PML boundary conditions; (<b>d</b>–<b>f</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.15 s under Neumann boundary conditions; and (<b>g</b>–<b>i</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.15 s considering the air layer).</p>
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<p>Comparison curves of wavefield at different depths at 0.05 s under different boundary conditions when the seismic source is located on the ground.</p>
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<p>Comparison curves of wavefield at different depths at 0.1 s under different boundary conditions when the seismic source is located on the ground.</p>
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<p>Comparison curves of wavefield at different depths at 0.15 s under different boundary conditions when the seismic source is located on the ground.</p>
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<p>Seismic trace records under different boundary conditions when the source is on the ground. (<b>a</b>) PML. (<b>b</b>) Neumann. (<b>c</b>) With air layer.</p>
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<p>Model under different boundary conditions when the seismic source is located underground. The red star represents a point source. ((<b>a</b>) is the ground using PML absorption boundary conditions, (<b>b</b>) is the ground using free boundary conditions, and (<b>c</b>) is the addition of an air layer and the use of PML absorption boundaries above the air layer).</p>
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<p>When the seismic source is located underground, the real parts of the wavefield with frequencies of 20 Hz, 40 Hz, and 60 Hz under different boundary conditions. ((<b>a</b>–<b>c</b>) are the real parts of the wavefield with different frequencies under PML absorption boundary conditions, (<b>d</b>–<b>f</b>) are the real parts of the wavefield with different frequencies under Neumann boundary conditions, and (<b>g</b>–<b>i</b>) are the real parts of the wavefield with different frequencies considering the air layer).</p>
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<p>When the seismic source is located underground, the imaginary parts of the wavefield with frequencies of 20 Hz, 40 Hz, and 60 Hz under different boundary conditions. ((<b>a</b>–<b>c</b>) are the imaginary parts of the wavefield with different frequencies under PML absorption boundary conditions, (<b>d</b>–<b>f</b>) are the imaginary parts of the wavefield with different frequencies under Neumann boundary conditions, and (<b>g</b>–<b>i</b>) are the imaginary parts of the wavefield with different frequencies considering the air layer).</p>
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<p>When the seismic source is located underground, the real and imaginary parts of the 20 Hz wavefield under different boundary conditions. ((<b>A</b>) is the comparison of the real part of the 20 Hz wavefield, and (<b>B</b>) is the comparison of the imaginary part of the 20 Hz wavefield. In (<b>A</b>), (<b>a</b>−<b>f</b>) represent the real part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively. In (<b>B</b>), (<b>a</b>−<b>f</b>) represent the imaginary part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively).</p>
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<p>When the seismic source is located underground, the real and imaginary parts of the 40 Hz wavefield under different boundary conditions. ((<b>A</b>) is the comparison of the real part of the 40 Hz wavefield, and (<b>B</b>) is the comparison of the imaginary part of the 40 Hz wavefield. In (<b>A</b>), (<b>a</b>−<b>f</b>) represent the real part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively. In (<b>B</b>), (<b>a</b>−<b>f</b>) represent the imaginary part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively).</p>
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<p>When the seismic source is located underground, the real and imaginary parts of the 60 Hz wavefield under different boundary conditions. ((<b>A</b>) is the comparison of the real part of the 60 Hz wavefield, and (<b>B</b>) is the comparison of the imaginary part of the 60 Hz wavefield. In (<b>A</b>), (<b>a</b>−<b>f</b>) represent the real part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively. In (<b>B</b>), (<b>a</b>−<b>f</b>) represent the imaginary part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively).</p>
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<p>Comparison of wavefield snapshots under different boundary conditions when the seismic source is located underground. ((<b>a</b>–<b>c</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.2 s under PML boundary conditions, respectively; (<b>d</b>–<b>f</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.2 s under Neumann boundary conditions, respectively; and (<b>g</b>–<b>i</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.2 s, respectively, when considering the air layer).</p>
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<p>Comparison curves of wavefield at different depths under different boundary conditions when the seismic source is located underground. ((<b>a</b>) is the waveform comparison curve at 0.05 s, (<b>b</b>) is the waveform comparison curve at 0.1 s, and (<b>c</b>) is the waveform comparison curve at 0.2 s).</p>
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<p>Seismic trace records under different boundary conditions when the epicenter is located underground.</p>
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<p>Model under different boundary conditions in undulating terrain conditions. The red star represents a point source. (The seismic source located on the ground). (<b>a</b>) The ground adopts PML absorption boundary conditions. (<b>b</b>) The ground adopts free boundary conditions. (<b>c</b>) Adds an air layer and uses PML absorption boundary above the air layer.</p>
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<p>Under undulating terrain conditions, the real parts of the wavefield with frequencies of 20 Hz, 40 Hz, and 60 Hz under different boundary conditions. ((<b>a</b>–<b>c</b>) are the real parts of the wavefield with different frequencies under PML absorption boundary conditions, (<b>d</b>–<b>f</b>) are the real parts of the wavefield with different frequencies under Neumann boundary conditions, and (<b>g</b>–<b>i</b>) are the real parts of the wavefield with different frequencies considering the air layer).</p>
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<p>Under undulating terrain conditions, the imaginary parts of the wavefield with frequencies of 20 Hz, 40 Hz, and 60 Hz under different boundary conditions. ((<b>a</b>–<b>c</b>) are the imaginary parts of the wavefield with different frequencies under PML absorption boundary conditions, (<b>d</b>–<b>f</b>) are the imaginary parts of the wavefield with different frequencies under Neumann boundary conditions, and (<b>g</b>–<b>i</b>) are the imaginary parts of the wavefield with different frequencies considering the air layer).</p>
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<p>Comparison of the details of the real and imaginary parts of the wave field captured at 20 Hz under different boundary conditions in undulating terrain conditions. The red arrow compares the wavefield energy near the ground. ((<b>a</b>–<b>c</b>) are the real parts of the 20 Hz wavefield under PML, Neumann, and air layer boundary conditions, respectively; (<b>d</b>–<b>f</b>) are the imaginary parts of the 20 Hz wavefield under PML, Neumann, and air layer boundary conditions, respectively).</p>
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<p>Under undulating terrain conditions, the real and imaginary parts of the 20 Hz wavefield under different boundary conditions. ((<b>A</b>) is the comparison of the real part of the 20 Hz wavefield, and (<b>B</b>) is the comparison of the imaginary part of the 20 Hz wavefield. In (<b>A</b>), (<b>a</b>−<b>f</b>) represent the real part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively. In (<b>B</b>), (<b>a</b>−<b>f</b>) represent the imaginary part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively).</p>
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<p>Under undulating terrain conditions, the real and imaginary parts of the 40 Hz wavefield under different boundary conditions. ((<b>A</b>) is the comparison of the real part of the 40 Hz wavefield, and (<b>B</b>) is the comparison of the imaginary part of the 40 Hz wavefield. In (<b>A</b>), (<b>a</b>−<b>f</b>) represent the real part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively. In (<b>B</b>), (<b>a</b>−<b>f</b>) represent the imaginary part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively).</p>
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<p>Under undulating terrain conditions, the real and imaginary parts of the 60 Hz wavefield under different boundary conditions. ((<b>A</b>) is the comparison of the real part of the 60 Hz wavefield, and (<b>B</b>) is the comparison of the imaginary part of the 60 Hz wavefield. In (<b>A</b>), (<b>a</b>−<b>f</b>) represent the real part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively. In (<b>B</b>), (<b>a</b>−<b>f</b>) represent the imaginary part of the wavefield at depths of 0 m, 100 m, 200 m, 300 m, 400 m, and 500 m, respectively).</p>
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<p>Comparison of snapshot images of different boundary wavefields under undulating terrain conditions. ((<b>a</b>–<b>c</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.15 s under PML boundary conditions; (<b>d</b>–<b>f</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.15 s under Neumann boundary conditions; and (<b>g</b>–<b>i</b>) are snapshots of the wavefield at 0.05 s, 0.1 s, and 0.15 s when considering the air layer).</p>
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<p>Overthrust onshore model.</p>
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<p>Real part of 30 Hz seismic wavefield under different boundary conditions. ((<b>a</b>–<b>c</b>) are the real parts of the 30 Hz wavefield under PML, Neumann, and air layer boundary conditions, respectively; (<b>d</b>–<b>f</b>) represent the vertical variation curves of the wavefield at x = 1000 m, 2500 m, and 4000 m, respectively).</p>
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<p>Comparison of wavefield snapshots under different boundary conditions. ((<b>a</b>–<b>c</b>) are snapshots of the wavefield at 0.1 s, 0.2 s, and 0.3 s under PML boundary conditions; (<b>d</b>–<b>f</b>) are snapshots of the wavefield at 0.1 s, 0.2 s, and 0.3 s under Neumann boundary conditions; and (<b>g</b>–<b>i</b>) are snapshots of the wavefield at 0.1 s, 0.2 s, and 0.3 s when considering the air layer).</p>
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<p>Comparison of seismic traces under different boundary conditions (z = 0 m). (<b>a</b>) PML. (<b>b</b>) Neumann. (<b>c</b>) With air layer.</p>
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30 pages, 5125 KiB  
Article
Application of Augmented Reality in Waterway Traffic Management Using Sparse Spatiotemporal Data
by Ruolan Zhang, Yue Ai, Shaoxi Li, Jingfeng Hu, Jiangling Hao and Mingyang Pan
Appl. Sci. 2025, 15(4), 1710; https://doi.org/10.3390/app15041710 - 7 Feb 2025
Viewed by 286
Abstract
The development of China’s digital waterways has led to the extensive deployment of cameras along inland waterways. However, the limited processing and utilization of digital resources hinder the ability to provide waterway services. To address this issue, this paper introduces a novel waterway [...] Read more.
The development of China’s digital waterways has led to the extensive deployment of cameras along inland waterways. However, the limited processing and utilization of digital resources hinder the ability to provide waterway services. To address this issue, this paper introduces a novel waterway perception approach based on an intelligent navigation marker system. By integrating multiple sensors into navigation markers, the fusion of camera video data and automatic identification system (AIS) data is achieved. The proposed method of an enhanced one-stage object detection algorithm improves detection accuracy for small vessels in complex inland waterway environments, while an object-tracking algorithm ensures the stable monitoring of vessel trajectories. To mitigate AIS data latency, a trajectory prediction algorithm is employed through region-based matching methods for the precise alignment of AIS data with pixel coordinates detected in video feeds. Furthermore, an augmented reality (AR)-based traffic situational awareness framework is developed to dynamically visualize key information. Experimental results demonstrate that the proposed model significantly outperforms mainstream algorithms. It achieves exceptional robustness in detecting small targets and managing complex backgrounds, with data fusion accuracy ranging from 84.29% to 94.32% across multiple tests, thereby substantially enhancing the spatiotemporal alignment between AIS and video data. Full article
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Figure 1
<p>Overall architecture of the intelligent navigation marker system.</p>
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<p>Multi-source data fusion framework: Video data are first captured using network cameras, and the target detection algorithm is enhanced to address the specific characteristics of inland waterway targets. Following detection and tracking, the vessel positions are identified. Simultaneously, AIS data are collected through reception equipment, filtered, and processed using a trajectory prediction algorithm to ensure temporal alignment with the video data. Finally, a fusion module integrates the AIS data and video data for a comprehensive analysis.</p>
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<p>One-stage object detection algorithm process: It includes feature extraction networks, multi-channel feature maps, and grid predictions of feature maps (such as object confidence and class probabilities). It also involves the parallel prediction of bounding boxes and class probabilities, followed by non-maximum suppression (NMS).</p>
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<p>Range of video and AIS reception devices.</p>
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<p>Division of target detection range for waterway vessels.</p>
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<p>Comparison of experimental results: (<b>a</b>) different algorithms’ mAP@0.5 contrast; (<b>b</b>) different algorithms’ precision contrast; (<b>c</b>) different algorithms’ recall contrast.</p>
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<p>Comparison of dehazing effects: (<b>a</b>) original foggy image; (<b>b</b>) image after dehazing.</p>
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<p>Comparison of nighttime illumination enhancement effects: (<b>a</b>) original nighttime image; (<b>b</b>) image after illumination enhancement.</p>
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<p>Comparison of ship detection in foggy channel environments: (<b>a</b>) ship detection effect on original foggy image; (<b>b</b>) ship detection effect after image dehazing.</p>
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<p>Comparison of ship detection in nighttime channel environments: (<b>a</b>) ship detection effect on original nighttime image; (<b>b</b>) ship detection effect after image illumination enhancement.</p>
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<p>Comparison of real trajectory and predicted trajectory.</p>
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<p>Perspective area division: (<b>a</b>) the camera’s field of view is divided into six smaller sub-regions; (<b>b</b>) the video matrix is also divided into six sub-regions according to the number of divisions made via the camera.</p>
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<p>Pixel coordinate ship matching process: within the region set <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math>, there are a total of three ships. They are matched sequentially based on their distance from the set baseline.</p>
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<p>Fusion effect display.</p>
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<p>AR function display of waterway traffic situation awareness. By integrating hydrometeorological sensing equipment on the beacons, real-time local traffic environment data are provided. Display of the effects for three consecutive days separately: (<b>a</b>) 22 October; (<b>b</b>) 23 October; and (<b>c</b>) 23 October.</p>
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36 pages, 20254 KiB  
Article
High-Gain Miniaturized Multi-Band MIMO SSPP LWA for Vehicular Communications
by Tale Saeidi, Sahar Saleh, Nick Timmons, Christopher McDaid, Ahmed Jamal Abdullah Al-Gburi, Faroq Razzaz and Saeid Karamzadeh
Technologies 2025, 13(2), 66; https://doi.org/10.3390/technologies13020066 - 4 Feb 2025
Viewed by 493
Abstract
This paper introduces a novel miniaturized, four-mode, semi-flexible leaky wave Multiple-Input Multiple-Output (MIMO) antenna specifically designed to advance vehicular communication systems. The proposed antenna addresses key challenges in 5G low- and high-frequency bands, including millimeter-wave communication, by integrating innovative features such as a [...] Read more.
This paper introduces a novel miniaturized, four-mode, semi-flexible leaky wave Multiple-Input Multiple-Output (MIMO) antenna specifically designed to advance vehicular communication systems. The proposed antenna addresses key challenges in 5G low- and high-frequency bands, including millimeter-wave communication, by integrating innovative features such as a periodic Spoof Surface Plasmon Polariton Transmission Line (SSPP-TL) and logarithmic-spiral-like semi-circular strip patches parasitically fed via orthogonal ports. These design elements facilitate stable impedance matching and wide impedance bandwidths across operating bands, which is essential for vehicular networks. The hybrid combination of leaky wave and SSPP structures, along with a defected wide-slot ground structure and backside meander lines, enhances radiation characteristics by reducing back and bidirectional radiation. Additionally, a naturalization network incorporating chamfered-edge meander lines minimizes mutual coupling and introduces a fourth radiation mode at 80 GHz. Compact in size (14 × 12 × 0.25 mm3), the antenna achieves high-performance metrics, including S11 < −18.34 dB, dual-polarization, peak directive gains of 11.6 dBi (free space) and 14.6 dBi (on vehicles), isolation > 27 dB, Channel Capacity Loss (CCL) < 3, Envelope Correlation Coefficient (ECC) < 0.001, axial ratio < 2.25, and diversity gain (DG) > 9.85 dB. Extensive testing across various vehicular scenarios confirms the antenna’s robustness for Vehicle-to-Vehicle (V2V), Vehicle-to-Pedestrian (V2P), and Vehicle-to-Infrastructure (V2I) communication. Its exceptional performance ensures seamless connectivity with mobile networks and enhances safety through Specific Absorption Rate (SAR) compliance. This compact, high-performance antenna is a transformative solution for connected and autonomous vehicles, addressing critical challenges in modern automotive communication networks and paving the way for reliable and efficient vehicular communication systems. Full article
(This article belongs to the Collection Electrical Technologies)
15 pages, 1568 KiB  
Article
Telomere Length, Oxidative Stress, and Kidney Damage Biomarkers in Fabry Nephropathy
by Tina Levstek, Erazem Bahčič, Bojan Vujkovac, Andreja Cokan Vujkovac, Tine Tesovnik, Žiga Iztok Remec, Vanja Čuk and Katarina Trebušak Podkrajšek
Cells 2025, 14(3), 218; https://doi.org/10.3390/cells14030218 - 4 Feb 2025
Viewed by 491
Abstract
Fabry nephropathy is a life-threatening complication of Fabry disease characterized by complex and incompletely understood pathophysiological processes possibly linked to premature aging. We aimed to investigate leukocyte telomere length (LTL), oxidative stress, and kidney damage biomarkers in relation to kidney function. The study [...] Read more.
Fabry nephropathy is a life-threatening complication of Fabry disease characterized by complex and incompletely understood pathophysiological processes possibly linked to premature aging. We aimed to investigate leukocyte telomere length (LTL), oxidative stress, and kidney damage biomarkers in relation to kidney function. The study included 35 Fabry patients and 35 age and sex-matched control subjects. Based on the estimated slope of the glomerular filtration rate, the patients were divided into two groups. Relative LTL was quantified by qPCR, urinary biomarkers 8-hydroxy-2′-deoxyguanosine (8-OHdG) and malondialdehyde (MDA) by UHPLC-MS/MS, and kidney damage biomarkers by flow cytometry. There was no statistically significant difference in LTL between Fabry patients and controls. However, a significant difference was observed in male patients compared to their matched control subjects (p = 0.013). Oxidative stress biomarkers showed no differences between patients and controls, while significant differences were observed in urinary IGFBP7, EGF, and OPN levels between Fabry patients with stable kidney function and those with progressive nephropathy (FDR = 0.021, 0.002, and 0.013, respectively). Significant differences were also observed in plasma levels of cystatin C, TFF3, and uromodulin between patients with progressive nephropathy and controls (all FDR = 0.039). Along with these biomarkers (FDR = 0.007, 0.017, and 0.010, respectively), NGAL also exhibited a significant difference between the two patient groups (FDR = 0.017). This study indicates accelerated telomere attrition, which may be related to disease burden in males. Furthermore, analyses of urinary oxidative stress markers revealed no notable disparities between the different kidney function groups, indicating their limited utility. However, promising differences were found in some biomarkers of kidney damage in urine and plasma. Full article
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<p>Comparison of leukocyte telomere length (TL) between (<b>a</b>) control subjects and Fabry patients, (<b>b</b>) control subjects and male Fabry patients, and (<b>c</b>) control subjects and female Fabry patients.</p>
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<p>Comparison of leukocyte telomere length (TL) between (<b>a</b>) control subjects and Fabry patients with stable kidney function (FD-SKF) and (<b>b</b>) control subjects and Fabry patients with progressive nephropathy (FD-NN).</p>
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<p>Comparison of urinary 8-OHdG levels between (<b>a</b>) control subjects and Fabry patients, (<b>b</b>) control subjects and Fabry patients with stable kidney function (FD-SKF), and (<b>c</b>) control subjects and Fabry patients with progressive nephropathy (FD-NN).</p>
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<p>Comparison of urinary MDA levels between (<b>a</b>) control subjects and Fabry patients, (<b>b</b>) control subjects and Fabry patients with stable kidney function (FD-SKF), and (<b>c</b>) control subjects and Fabry patients with progressive nephropathy (FD-NN).</p>
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<p>Correlation between urinary concentration of (<b>a</b>) 8-OHdG or (<b>b</b>) MDA and relative leukocyte telomere length (TL).</p>
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20 pages, 7434 KiB  
Article
Characterizing and Modeling Infiltration and Evaporation Processes in the Shallow Loess Layer: Insight from Field Monitoring Results of a Large Undisturbed Soil Column
by Ye Tan, Fuchu Dai, Zhiqiang Zhao, Cifeng Cheng and Xudong Huang
Water 2025, 17(3), 364; https://doi.org/10.3390/w17030364 - 27 Jan 2025
Viewed by 398
Abstract
Frequent agricultural irrigation events continuously raise the groundwater table on loess platforms, triggering numerous loess landslides and significantly contributing to soil erosion in the Chinese Loess Plateau. The movement of irrigation water within the surficial loess layer is crucial for comprehending the mechanisms [...] Read more.
Frequent agricultural irrigation events continuously raise the groundwater table on loess platforms, triggering numerous loess landslides and significantly contributing to soil erosion in the Chinese Loess Plateau. The movement of irrigation water within the surficial loess layer is crucial for comprehending the mechanisms of moisture penetration into thick layers. To investigate the infiltration and evaporation processes of irrigation water, a large undisturbed soil column with a 60 cm inner diameter and 100 cm height was extracted from the surficial loess layer. An irrigation simulation event was executed on the undisturbed soil column and the ponding infiltration and subsequent evaporation processes were systematically monitored. A ruler placed above the soil column recorded the ponding height during irrigation. Moisture probes and tensiometers were installed at five depths to monitor the temporal variations in volumetric water content (VWC) and matric suction. Additionally, an evaporation gauge and an automatic weighing balance measured the potential and actual evaporation. The results revealed that the initially high infiltration rate rapidly decreased to a stable value slightly below the saturated hydraulic conductivity (Ks). A fitted Mezencev model successfully replicated the ponding infiltration process with a high correlation coefficient of 0.995. The monitored VWC of the surficial 15 cm-thick loess approached a saturated state upon the advancing of the wetting front, while the matric suction sharply decreased from an initial high value of 65 kPa to nearly 0 kPa. The monitored evaporation process of the soil column was divided into an initial constant rate stage and a subsequent decreasing rate stage. During the constant rate stage, the actual evaporation closely matched or slightly exceeded the potential evaporation rate. In the decreasing rate stage, the actual evaporation rate fell below the potential evaporation rate. The critical VWC ranged from 26% to 28%, with the corresponding matric suction recovering to approximately 25 kPa as the evaporation process transitioned between stages. The complete evaporation process was effectively modeled using a fitted Rose model with a high correlation coefficient (R2 = 0.971). These findings provide valuable insights into predicting water infiltration and evaporation capacities in loess layers, thereby enhancing the understanding of water movement within thick loess deposits and the processes driving soil erosion. Full article
(This article belongs to the Special Issue Monitoring and Control of Soil and Water Erosion)
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<p>Overview of the research background. (<b>a</b>) Full view of the Heifangtai tableland and the sampling location; (<b>b</b>) stratigraphic profiles of A-A’; (<b>c</b>) the flow-like loess landslide in Heifangtai; (<b>d</b>) sampling of the undisturbed soil column within the surficial loess layer.</p>
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<p>Monitoring schemes of the soil column. (<b>a</b>) Profile view of layout of the instruments; (<b>b</b>) pictures of monitoring transducers including tensiometer, moisture probe, evaporation gauge and CR800 data logger; (<b>c</b>) ponding infiltration process of the soil column.</p>
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<p>Procedures of measurement of the loess sample’s hydraulic properties in laboratory. (<b>a</b>) Preparation of the undisturbed loess sample; (<b>b</b>) sample saturating; (<b>c</b>) measuring of K<sub>s</sub>; (<b>d</b>) measuring of SWCC.</p>
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<p>Determination of SWCC in laboratory and fitted with VG model.</p>
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<p>(<b>a</b>) Variation of ponding depth with time; (<b>b</b>) the monitored cumulative infiltration, infiltration rate, and fitted curve during the ponding infiltration process.</p>
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<p>Comparison of the measured and predicted cumulative infiltration by four fitted models.</p>
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<p>The monitored response characteristics of the soil column at different depths with time during the ponding infiltration process include (<b>a</b>) volumetric water content and (<b>b</b>) matric suction.</p>
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<p>The monitored response characteristics of soil column at different depths with time during the evaporation process include (<b>a</b>) volumetric water content, (<b>b</b>) matric suction, and (<b>c</b>) soil temperature.</p>
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<p>Variations of potential and actual evaporation with time and the best-fit curve for actual evaporation.</p>
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<p>Comparisons of SWCCs obtained from laboratory tests and measured in the field experiment at depths of (<b>a</b>) 15 cm; (<b>b</b>) 30 cm; (<b>c</b>) 50 cm; (<b>d</b>) 70 cm; and (<b>e</b>) 90 cm.</p>
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10 pages, 242 KiB  
Article
Macrovascular Function in People with HIV After Recent SARS-CoV-2 Infection
by Ana S. Salazar, Louis Vincent, Bertrand Ebner, Nicholas Fonseca Nogueira, Leah Krauss, Madison S. Meyer, Jelani Grant, Natalie Aguilar, Mollie S. Pester, Meela Parker, Alex Gonzalez, Armando Mendez, Adam Carrico, Barry E. Hurwitz, Maria L. Alcaide and Claudia Martinez
J. Vasc. Dis. 2025, 4(1), 4; https://doi.org/10.3390/jvd4010004 - 26 Jan 2025
Viewed by 455
Abstract
Background: People with HIV (PWH) are at increased risk of vascular dysfunction and cardiovascular disease (CVD). SARS-CoV-2 infection has been associated with acute CVD complications. The aim of the study was to as-sess macrovascular function as an early indicator of CVD risk in [...] Read more.
Background: People with HIV (PWH) are at increased risk of vascular dysfunction and cardiovascular disease (CVD). SARS-CoV-2 infection has been associated with acute CVD complications. The aim of the study was to as-sess macrovascular function as an early indicator of CVD risk in PWH after mild SARS-CoV-2 infection. Methods: PWH aged 20–60 years, with undetectable viral load (RNA < 20 copies/mL), on stable anti-retroviral therapy (≥6 months) and history of mild COVID-19 (≥30 days) without any CVD manifestations prior to enrollment were recruited. Participants were excluded if they had history of diabetes mellitus, end-stage renal disease, heart or respiratory disease. Participants were matched 1:1 to pre-pandemic PWH. A health survey, surrogate measures of CVD risk, and macrovascular function (brachial artery flow-mediated vasodilation and arterial stiffness assessments via applanation tonometry) were compared between group. Results: A total of 17 PWH and history of COVID-19 (PWH/COV+) were matched with 17 PWH without COVID-19 (PWH/COV−) pre-pandemic. Mean age (45.5 years), sex (76.5% male), body mass index (27.3), and duration of HIV infection (12.2 years) were not different between groups. Both groups had comparable CVD risk factors (total cholesterol, LDL, HDL, systolic and diastolic blood pressure). There were no differences in measures of flow mediated arterial dilatation or arterial stiffness after 30 days of SARS-CoV-2 infection. Conclusions: After recent SARS-CoV-2 infection, PWH did not demonstrate evidence of macrovascular dysfunction and increased CVD risk. Results suggest that CVD risk may not be increased in people with well-controlled HIV who did not manifest CVD complications SARS-CoV-2 infection. Full article
(This article belongs to the Section Peripheral Vascular Diseases)
15 pages, 2172 KiB  
Article
Comparison of Spatial Predictability Differences in Truck Activity Patterns: An Empirical Study Based on Truck Tracking Dataset of China
by Lianghua Li, Peng Du, Guohua Jiao and Xin Fu
Appl. Sci. 2025, 15(3), 1114; https://doi.org/10.3390/app15031114 - 23 Jan 2025
Viewed by 299
Abstract
Existing research on truck location prediction focuses on direct trajectory prediction and ignores the link between activity patterns and predictability, whereas the mode of operation is an important factor in the difference between activity trajectories, and analyzing the mode of operation can help [...] Read more.
Existing research on truck location prediction focuses on direct trajectory prediction and ignores the link between activity patterns and predictability, whereas the mode of operation is an important factor in the difference between activity trajectories, and analyzing the mode of operation can help to develop the next-location prediction algorithms to improve the efficiency of matching truckloads and to reduce costs. Our empirical study, based on 562,071 truck trip data in China, employs Fuzzy c-means (FCM) for clustering operational patterns in space, intensity, and stability dimensions. K-nearest neighbors (KNN), Back Propagation neural (BP) network, and Long Short-Term Memory (LSTM) predict the next truck locations in different modes. The results indicate that range-of-motion stability significantly influences predictability. Truckers with stable spatial activity exhibit the highest predictability, with 45% nearly achieving 100% predictability. Through cluster analysis of driving characteristics, we found that truck clusters are the most predictable because of their relatively small and low-intensity activities, with the percentage of samples with prediction accuracy above 90% reaching over 80%. This research not only characterizes the freight truck community but also aids algorithm optimization by revealing predictability factors for real-world applications. Full article
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<p>SSE values for stability pattern clustering with different k.</p>
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<p>The distribution of the stability indicators. (<b>a</b>) Distribution of the variation coefficient of travel mileage; (<b>b</b>) Distribution of the variation coefficient of travel time; (<b>c</b>) Distribution of the variation coefficient of the number of cities visited; (<b>d</b>) Distribution of the variation coefficient of interval operating days.</p>
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<p>Cumulative prediction accuracy distribution of the different stability patterns. (<b>a</b>) Cumulative distribu-tion of KNN prediction accuracy. (<b>b</b>) Cumulative distribution of BP Neural Network prediction accuracy. (<b>c</b>) Cumulative distribution of LSTM prediction accuracy.</p>
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<p>SSE values for travel pattern clustering with different k.</p>
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<p>The distribution of the operating indicators. (<b>a</b>) Distribution of the radius gyration; (<b>b</b>) Distribution of the average number of cities visited; (<b>c</b>) Distribution of the average operating hours; (<b>d</b>) Distribution of average operating mileage; (<b>e</b>) Distribution of operating days; (<b>f</b>) Distribution of continuous operating days.</p>
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<p>The distribution of the operating indicators. (<b>a</b>) Distribution of the radius gyration; (<b>b</b>) Distribution of the average number of cities visited; (<b>c</b>) Distribution of the average operating hours; (<b>d</b>) Distribution of average operating mileage; (<b>e</b>) Distribution of operating days; (<b>f</b>) Distribution of continuous operating days.</p>
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<p>Cumulative prediction accuracy distribution of the different travel patterns. (<b>a</b>) Cumulative dis-tribution of KNN prediction; (<b>b</b>) Cumulative distribution of BP Neural accuracy; (<b>c</b>) Cumulative distribution of LSTM prediction accuracy.</p>
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15 pages, 6762 KiB  
Article
Frequency-Based Analysis of Matching Accuracy Between Satellite Radio Frequency and AIS Data for Ship Identification
by Chan-Su Yang and Sree Juwel Kumar Chowdhury
J. Mar. Sci. Eng. 2025, 13(2), 191; https://doi.org/10.3390/jmse13020191 - 21 Jan 2025
Viewed by 604
Abstract
Vessels can deactivate their Automatic Identification System (AIS) to operate undetected and potentially engage in illegal activities. To address this, satellite-based radio frequency (RF) data are increasingly being used for identifying such vessels. This study evaluates the matching accuracy among RF and AIS [...] Read more.
Vessels can deactivate their Automatic Identification System (AIS) to operate undetected and potentially engage in illegal activities. To address this, satellite-based radio frequency (RF) data are increasingly being used for identifying such vessels. This study evaluates the matching accuracy among RF and AIS data based on the frequency and distance. RF data were acquired on 22 September, 25 September, and 7 December 2023. According to the frequency range, the dataset was separated into frequency-1 (3.024–3.077 GHz) and frequency-2 (9.3734–9.4249 GHz). Six distance thresholds (2 km, 3 km, 6 km, 8 km, 13 km, and 18 km) were employed for the matching process. The results depicted that the average matching rates were 95%, 92%, and 92% for the RF dataset on 22 September, 25 September, and 7 December, respectively. Additionally, the results revealed that the matching rates decreased with distance, e.g., for the RF dataset on 22 September, the average highest matching rate (47%) was found at a 2 km distance and the minimum matching rate (0.9%) was observed at an 18 km distance. Furthermore, the analysis delineated that frequency-2 consistently exceeded frequency-1, particularly at longer distances, showing a more stable trend in matching accuracy. Full article
(This article belongs to the Special Issue Maritime Transport and Port Management)
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<p>Location of the study area with the coverage of radio frequency data on 22 September, 25 September, and 7 December 2023.</p>
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<p>Schematic diagram of ship matching process using RF and AIS data. Frequency-1 and frequency-2 represent the RF data with frequency ranges from 3.024 to 3.077 GHz and 9.3734 to 9.4249 GHz, respectively.</p>
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<p>Example of duplicate ship matching and individual ship matching results from RF and AIS data at distinct frequencies. (<b>a</b>,<b>c</b>) Matching results from Unseenlabs and (<b>b</b>,<b>d</b>) matching results from this study. The red rectangle indicates the RF (frequency), and the amber triangle represents the AIS (Vessel ID). The blue line indicates the matching between the RF and AIS data.</p>
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<p>Identification of ships from different frequencies after matching the S22-RF1 dataset and AIS data on 22 September 2023. The blue rectangle indicates the position of the ship matched at frequency-1 (3.04~3.08 GHz), and the amber triangle represents the matched ship position at frequency-2 (9.37~9.41 GHz).</p>
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<p>Ship identification results over the study area from different frequencies after matching the S22-RF2 dataset and AIS on 22 September 2023. The blue rectangle indicates the position of a matched ship at frequency-1 (3.04~3.08 GHz), and the amber triangle represents the position of a matched ship at frequency-2 (9.37~9.41 GHz).</p>
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<p>Ship identification results from different frequencies after matching the S22-RF3 dataset and AIS data on 22 September 2023. The blue rectangle indicates the position of a matched ship at frequency-1 (3.04~3.08 GHz), and the amber triangle represents the position of a matched ship at frequency-2 (9.37~9.41 GHz).</p>
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<p>Identification of ships from different frequencies after matching between the S25-RF1 dataset and AIS data on 25 September 2023. The blue rectangle indicates the position of a matched ship at frequency-1 (3.04~3.08 GHz), and the amber triangle represents the position of a matched ship at frequency-2 (9.37~9.41 GHz).</p>
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<p>Ship identification results from different frequencies after matching the S25-RF2 dataset and AIS data on 25 September 2023. The blue rectangle indicates the position of a matched ship at frequency-1 (3.04~3.08 GHz), and the amber triangle represents the position of a matched ship at frequency-2 (9.37~9.41 GHz).</p>
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<p>Ship identification results from different frequencies after matching the S25-RF3 dataset and AIS data on 25 September 2023. The blue rectangle indicates the position of a matched ship at frequency-1 (3.04~3.08 GHz), and the amber triangle represents the position of a matched ship at frequency-2 (9.37~9.41 GHz).</p>
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<p>Ship identification results from different frequencies after matching the D07-RF1 dataset and AIS data on 7 December 2023. The blue rectangle indicates the position of a matched ship at frequency-1 (3.04~3.08 GHz), and the amber triangle represents the position of a matched ship at frequency-2 (9.37~9.41 GHz).</p>
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22 pages, 1218 KiB  
Article
Electric Vehicles Charging Scheduling Strategy Based on Time Cost of Users and Spatial Load Balancing in Multiple Microgrids
by Jiaqi Zhang, Yongxiang Xia, Zhongyi Cheng and Xi Chen
World Electr. Veh. J. 2025, 16(1), 46; https://doi.org/10.3390/wevj16010046 - 19 Jan 2025
Viewed by 526
Abstract
In a sustainable energy system, managing the charging demand of electric vehicles (EVs) becomes increasingly critical. Uncontrolled charging behaviors of large-scale EV fleets will exacerbate loads imbalanced in a multi-microgrid (MMG). At the same time, the time cost of users will increase significantly. [...] Read more.
In a sustainable energy system, managing the charging demand of electric vehicles (EVs) becomes increasingly critical. Uncontrolled charging behaviors of large-scale EV fleets will exacerbate loads imbalanced in a multi-microgrid (MMG). At the same time, the time cost of users will increase significantly. To improve users’ charging experience and ensure stable operation of the MMG, we propose a new joint scheduling strategy that considers both time cost of users and spatial load balancing among MMGs. The time cost encompasses many factors, such as traveling time, queue waiting time, and charging time. Meanwhile, spatial load balancing seeks to mitigate the impact of large-scale EV charging on MMG loads, promoting a more equitable distribution of power resources across the MMG system. Compared to the Shortest Distance Matching Strategy (SDMS) and the Time Minimum Matching Strategy (TMMS) methods, our approach improves the average peak-to-valley ratio by 9.5% and 10.2%, respectively. Similarly, compared to the Load Balancing Matching Strategy (LBMS) and the Improved Load Balancing Matching Strategy (ILBMS) methods, our approach reduces the average time cost by 31.8% and 25% while maintaining satisfactory spatial load balancing. These results demonstrate that the proposed method achieves good results in handling electric vehicle scheduling problems. Full article
(This article belongs to the Special Issue Electric Vehicles and Smart Grid Interaction)
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<p>Schematic diagram of charging aggregator in microgrid.</p>
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<p>Multi-microgrids.</p>
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<p>The charging curve of battery.</p>
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<p>The time cost of a vehicle.</p>
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<p>MTC-SLBMS algorithm flowchart.</p>
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<p>Road network.</p>
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<p>Traffic flows at different time points.</p>
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<p>Comparison of average time cost under different strategies (<span class="html-italic">C</span> = 50).</p>
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<p>Comparison of average valley-to-peak ratio under different strategies (<span class="html-italic">C</span> = 50).</p>
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<p>Comparison of composite index(CI) under different strategies (<span class="html-italic">C</span> = 50).</p>
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<p>Average valley-to-peak ratio under different participation (<span class="html-italic">C</span> = 50).</p>
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<p>MG load curve under different strategies (<span class="html-italic">N</span> = 1500 and <span class="html-italic">C</span> = 50).</p>
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<p>Comparison of the number of vehicles in each charging station under different strategies (<span class="html-italic">C</span> = 50).</p>
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<p>Comparison of average time cost under different charging station capacities.</p>
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<p>Comparison of average valley-to-peak ratio under different charging station capacities.</p>
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19 pages, 9145 KiB  
Article
Antiviral Activity and Underlying Mechanism of Moslae herba Aqueous Extract for Treating SARS-CoV-2
by Yan Feng, Qiong Ge, Jian Gao, Zhuoying Wu, Yunyi Zhang, Haiyan Mao, Beibei Wu and Changping Xu
Molecules 2025, 30(2), 387; https://doi.org/10.3390/molecules30020387 - 17 Jan 2025
Viewed by 595
Abstract
Despite the widespread use of COVID-19 vaccines, there is still a global need to find effective therapeutics to deal with the variants of SARS-CoV-2. Moslae herba (MH) is a herbal medicine credited with antiviral effects. This study aims to investigate the antiviral effects [...] Read more.
Despite the widespread use of COVID-19 vaccines, there is still a global need to find effective therapeutics to deal with the variants of SARS-CoV-2. Moslae herba (MH) is a herbal medicine credited with antiviral effects. This study aims to investigate the antiviral effects and the underlying mechanism of aqueous extract of Moslae herba (AEMH) for treating SARS-CoV-2. The in vitro anti-SARS-CoV-2 activity of AEMH was evaluated using cell viability and viral load. Component analysis was performed by HPLC-ESI-Q-TOF/MS. The connection between COVID-19 and AEMH was constructed by integrating network pharmacology and transcriptome profiles to seek the core targets. The components with antiviral activities were analyzed by molecular docking and in vitro pharmacological verification. AEMH exerted anti-SARS-CoV-2 effects by inhibiting viral replication and reducing cell death caused by infection (IC50 is 170 μg/mL for omicron strain). A total of 27 components were identified from AEMH. Through matching 119 intersection targets of ‘disease and drug’ with 1082 differentially expressed genes of COVID-19 patients, nine genes were screened. Of the nine, the PNP and TPI1 were identified as core targets as AEMH treatment significantly regulated the mRNA expression level of the two genes on infected cells. Three components, caffeic acid, luteolin, and rosmarinic acid, displayed antiviral activities in verification. Molecular docking also demonstrated they could form stable bonds with the core targets. This study explored the antiviral activity and possible mechanism of AEMH for treating SARS-CoV-2, which could provide basic data and reference for the clinical application of MH. Full article
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<p>Evaluation of in vitro anti-SARS-CoV-2 activities of AEMH. (<b>A</b>) Cytotoxicity induced by AEMH on Vero-E6 cells. (<b>B</b>) Normal Vero-E6 cell morphology. (<b>C</b>) Vero-E6 cell morphology treated by 20 mg/mL AEMH. (<b>D</b>) Cytotoxicity induced by Nirmatrelvir on Vero-E6 cells. (<b>E</b>) SARS-CoV-2 viral loads on cells with or without AEMH treatment. Vero-E6 cells were infected with 100 TCID<sub>50</sub> of SARS-CoV-2 and treated with different concentrations of AEMH or Nirmatrelvir (1 μM) for 48 h. Viral loads were tested by quantitative real-time PCR (qRT-PCR) targeting N gene of SARS-CoV-2. **, significant with <span class="html-italic">p</span> &lt; 0.01 compared to VC. (<b>F</b>) Omicron-induced CPE on Vero-E6 cells. (<b>G</b>) AEMH inhibited cell deaths induced by SARS-CoV-2 infection. (<b>H</b>) Nirmatrelvir inhibited cell deaths induced by SARS-CoV-2 infection.</p>
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<p>Components analysis performed by HPLC-ESI-Q-TOF/MS. (<b>A</b>) Negative ion chromatogram of AEMH. (<b>B</b>) Positive ion chromatogram of AEMH.</p>
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<p>Screening and analysis of targets related to COVID-19 and AEMH. (<b>A</b>) Venn plot constructed based on COVID-19-related targets retrieved from six databases and the related targets of 26 components identified from AEMH. (<b>B</b>–<b>D</b>) GO enrichment analysis of 126 intersection genes. The top 15 items involved in BP (<b>B</b>), CC (<b>C</b>), and MF (<b>D</b>). (<b>E</b>) The top 15 pathways enriched in KEGG analysis (FDR &lt; 0.05). (<b>F</b>) AEMH-components-targets-COVID-19 network diagram.</p>
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<p>Screening of core targets. (<b>A</b>) PPI network diagram. (<b>B</b>) Heat map plotted with differentially expressed genes of patients in comparison with healthy donors. (<b>C</b>) Venn plot constructed based on 119 genes obtained in PPI with 1082 differential expression genes of patients infected with omicron.</p>
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<p>Relative mRNA expression level of the selected nine genes. Each gene contains data from the CC-, VC-, and AEMH-treated groups. Experiments were performed in four replicates. *, significant with <span class="html-italic">p</span> &lt; 0.05, **, significant with <span class="html-italic">p</span> &lt; 0.01.</p>
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<p>Binding affinity energies between core targets and 26 components. The binding affinity energies were evaluated by the docking scores of components and core targets.</p>
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<p>In vitro pharmacological verification of eight selected components. Vero-E6 cells were infected with 100 TCID<sub>50</sub> of SARS-CoV-2 and then treated with each component at MNTC or 4 mg/mL of AEMH for 48 h. Viral loads were tested by qRT-PCR targeting N gene of SARS-CoV-2. *, significant with <span class="html-italic">p</span> &lt; 0.05 compared to VC. **, significant with <span class="html-italic">p</span> &lt; 0.01 compared to VC, ns, non-significant.</p>
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<p>Binding patterns between three verified components and two core targets. Binding pattern between PNP to caffeic acid (<b>A</b>), rosmarinic acid (<b>B</b>), and luteolin (<b>C</b>). Binding pattern between TPI1 to caffeic acid (<b>D</b>), rosmarinic acid (<b>E</b>), and luteolin (<b>F</b>).</p>
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12 pages, 5898 KiB  
Article
Circularly Polarized Asymmetric Single-Point Probe-Fed Hybrid Dielectric Resonator Antenna for Wireless Applications
by NareshKumar Darimireddy
Telecom 2025, 6(1), 8; https://doi.org/10.3390/telecom6010008 - 16 Jan 2025
Viewed by 500
Abstract
This paper presents a hybrid dielectric resonator antenna (HDRA) for circularly polarized (CP) radiation at 5 GHz, designed for WLAN applications. The antenna features a single probe feed that excites a combination of a circular ring patch and a cylindrical dielectric resonator (DR) [...] Read more.
This paper presents a hybrid dielectric resonator antenna (HDRA) for circularly polarized (CP) radiation at 5 GHz, designed for WLAN applications. The antenna features a single probe feed that excites a combination of a circular ring patch and a cylindrical dielectric resonator (DR) element, achieving stable gain across a wide bandwidth. The parametric analysis and vector E-field distribution of the proposed antenna presents the optimization, and it is evidence of CP radiation, respectively. The hybrid DRA has a reflection loss (RL) bandwidth of 485 MHz, from 4740 to 5225 MHz, and an axial ratio (AR) bandwidth of 150 MHz, ranging from 4950 to 5100 MHz. It achieves a peak gain of 7.03 dBic at 5 GHz, making it suitable for missile tracking, data link communications, and IEEE 802.11n WLAN systems. Measurements of a prototype in an anechoic chamber show a close match with simulation results. Full article
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<p>Proposed HDRA Configuration with dimensions (Ls = 60, Ws = 45, h = 0.787, Ph = 8.4, DR = 10, Dh = 10.16). All the dimensions are in “mm”.</p>
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<p>Evolution of the proposed antenna (<b>a</b>) Conventional DRA (without substrate) (<b>b</b>) DRA (with substrate) (<b>c</b>) Probe-fed ring patch and (<b>d</b>) Proposed hybrid DRA with probe at 0 deg.</p>
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<p>S<sub>11</sub> Comparisons of all the composition stages to generate CP radiation.</p>
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<p>E- Field analysis inside the cylindrical DRA at 4.9 GHz to confirm the two orthogonal modes (<b>a</b>) HEM<sup>x</sup><sub>δ11</sub> (YZ Plane) and (<b>b</b>) HEM<sup>y</sup><sub>1δ1</sub> (XZ Plane).</p>
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<p>S<sub>11</sub>-Plots of various lengths (Ph) of the feed.</p>
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<p>S<sub>11</sub>-Plots of various heights (Dh) of the DR.</p>
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<p>(<b>a</b>) Fabricated HDRA prototype and (<b>b</b>) its measurement in an anechoic chamber.</p>
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<p>Simulated and measured S<sub>11</sub> plots of proposed HDRA.</p>
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<p>Measured and simulated AR plots of proposed HDRA.</p>
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<p>Measured and simulated gain plots of proposed HDRA.</p>
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<p>Comparison of simulated and measured radiation pattern plots at 5 GHz (<b>a</b>) XZ planes (<b>b</b>) YZ planes.</p>
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20 pages, 1799 KiB  
Article
Impact of Charge on Strange Compact Stars in Rastall Theory
by Malick Sallah and Muhammad Sharif
Universe 2025, 11(1), 25; https://doi.org/10.3390/universe11010025 - 16 Jan 2025
Viewed by 376
Abstract
Within the framework of Rastall theory, we investigate the impact of charge on the structural development of different types of spherically symmetric anisotropic stars. To do so, we present modified field equations based upon the Finch–Skea metric potentials expressed in terms of three [...] Read more.
Within the framework of Rastall theory, we investigate the impact of charge on the structural development of different types of spherically symmetric anisotropic stars. To do so, we present modified field equations based upon the Finch–Skea metric potentials expressed in terms of three parameters (A,B,C). These constants are determined using suitable matching conditions and observational data for compact objects which include Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4 and SMC X-1. The equation of state offered by the MIT bag model for quark–gluon plasma is used to investigate the inner structure and other characteristics of these compact objects. For a fixed bag constant, B=60MeV/fm3, and two sets of the Rastall and charge parameters, ζ=0.255,0.259 and Q˜=0.2,0.7, respectively, we analyze the consistency of the matter variables in the model and other physical parameters such as energy conditions, stellar mass, compactness, and surface redshift. In addition, we assess the stability of the constructed model through two different approaches. It is found that the obtained model is physically viable and stable. Full article
(This article belongs to the Special Issue Gravity and Cosmology: Exploring the Mysteries of f(T) Gravity)
Show Figures

Figure 1

Figure 1
<p>Plots of metric functions against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of metric functions against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>ρ</mi> <mo stretchy="false">˜</mo> </mover> <mo>,</mo> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>r</mi> </msub> <mo>,</mo> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>t</mi> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <msup> <mi>q</mi> <mn>2</mn> </msup> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>ρ</mi> <mo stretchy="false">˜</mo> </mover> <mo>,</mo> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>r</mi> </msub> <mo>,</mo> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>t</mi> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <msup> <mi>q</mi> <mn>2</mn> </msup> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>ρ</mi> <mo stretchy="false">˜</mo> </mover> <mo>,</mo> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>r</mi> </msub> <mo>,</mo> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>t</mi> </msub> </mrow> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math> (<b>left</b>), <math display="inline"><semantics> <mrow> <mn>0.7</mn> </mrow> </semantics></math> (<b>right</b>). (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> <mover accent="true"> <mi>ρ</mi> <mo stretchy="false">˜</mo> </mover> </mrow> <mrow> <mi>d</mi> <mi>r</mi> </mrow> </mfrac> </mstyle> <mo>,</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>r</mi> </msub> </mrow> <mrow> <mi>d</mi> <mi>r</mi> </mrow> </mfrac> </mstyle> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>t</mi> </msub> </mrow> <mrow> <mi>d</mi> <mi>r</mi> </mrow> </mfrac> </mstyle> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> <mover accent="true"> <mi>ρ</mi> <mo stretchy="false">˜</mo> </mover> </mrow> <mrow> <mi>d</mi> <mi>r</mi> </mrow> </mfrac> </mstyle> <mo>,</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>r</mi> </msub> </mrow> <mrow> <mi>d</mi> <mi>r</mi> </mrow> </mfrac> </mstyle> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> <msub> <mover accent="true"> <mi>P</mi> <mo stretchy="false">˜</mo> </mover> <mi>t</mi> </msub> </mrow> <mrow> <mi>d</mi> <mi>r</mi> </mrow> </mfrac> </mstyle> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of anisotropic pressure <math display="inline"><semantics> <mrow> <mo>(</mo> <mover accent="true"> <mo>Δ</mo> <mo stretchy="false">˜</mo> </mover> <mo>)</mo> </mrow> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math> (<b>left</b>), <math display="inline"><semantics> <mrow> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math> (<b>right</b>). (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mi>σ</mi> </semantics></math>, and <math display="inline"><semantics> <msub> <mi>Z</mi> <mi>s</mi> </msub> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mi>σ</mi> </semantics></math>, and <math display="inline"><semantics> <msub> <mi>Z</mi> <mi>s</mi> </msub> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Graphs of energy bounds against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Graphs of energy bounds against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math>. (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mrow> <mrow> <mo>|</mo> </mrow> <msubsup> <mi>V</mi> <mrow> <mi>s</mi> <mi>t</mi> </mrow> <mn>2</mn> </msubsup> <mo>−</mo> <msubsup> <mi>V</mi> <mrow> <mi>s</mi> <mi>r</mi> </mrow> <mn>2</mn> </msubsup> <mrow> <mo>|</mo> </mrow> </mrow> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math> (<b>left</b>), <math display="inline"><semantics> <mrow> <mn>0.7</mn> </mrow> </semantics></math> (<b>right</b>). (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <msubsup> <mi>V</mi> <mrow> <mi>s</mi> <mi>r</mi> </mrow> <mn>2</mn> </msubsup> </semantics></math> and <math display="inline"><semantics> <msubsup> <mi>V</mi> <mrow> <mi>s</mi> <mi>r</mi> </mrow> <mn>2</mn> </msubsup> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math> (<b>left</b>), <math display="inline"><semantics> <mrow> <mn>0.7</mn> </mrow> </semantics></math> (<b>right</b>). (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mo>Γ</mo> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0.255</mn> </mrow> </semantics></math> (thick), <math display="inline"><semantics> <mrow> <mn>0.259</mn> </mrow> </semantics></math> (broken) and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math> (<b>left</b>), <math display="inline"><semantics> <mrow> <mn>0.7</mn> </mrow> </semantics></math> (<b>right</b>). (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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<p>Plots of <math display="inline"><semantics> <mrow> <mrow> <mo>|</mo> </mrow> <msubsup> <mi>V</mi> <mrow> <mi>s</mi> <mi>t</mi> </mrow> <mn>2</mn> </msubsup> <mo>−</mo> <msubsup> <mi>V</mi> <mrow> <mi>s</mi> <mi>r</mi> </mrow> <mn>2</mn> </msubsup> <mrow> <mo>|</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mo>Γ</mo> </semantics></math> against <span class="html-italic">r</span> for <math display="inline"><semantics> <mrow> <mi>ζ</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi mathvariant="script">Q</mi> <mo stretchy="false">˜</mo> </mover> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math> (<b>left</b>), <math display="inline"><semantics> <mrow> <mn>0.7</mn> </mrow> </semantics></math> (<b>right</b>). (The colors blue, brown, green, red, and black, denote the considered quark candidates, Her X-1, SAX J 1808.4-3658, PSR J038-0842, LMC X-4, and SMC X-1, respectively).</p>
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14 pages, 4030 KiB  
Article
Analysis of Radio Science Data from the KaT Instrument of the 3GM Experiment During JUICE’s Early Cruise Phase
by Paolo Cappuccio, Andrea Sesta, Mauro Di Benedetto, Daniele Durante, Umberto De Filippis, Ivan di Stefano, Luciano Iess, Ruaraidh Mackenzie and Bernard Godard
Aerospace 2025, 12(1), 56; https://doi.org/10.3390/aerospace12010056 - 16 Jan 2025
Viewed by 466
Abstract
The JUpiter Icy Moon Explorer (JUICE) mission, launched on 14 April 2023, aims to explore Jupiter and its Galilean moons, with arrival in the Jovian system planned for mid-2031. One of the scientific investigations is the Geodesy and Geophysics of Jupiter and the [...] Read more.
The JUpiter Icy Moon Explorer (JUICE) mission, launched on 14 April 2023, aims to explore Jupiter and its Galilean moons, with arrival in the Jovian system planned for mid-2031. One of the scientific investigations is the Geodesy and Geophysics of Jupiter and the Galilean Moons (3GM) radio science experiment, designed to study the interior structures of Europa, Callisto, and Ganymede and the atmospheres of Jupiter and the Galilean moons. The 3GM experiment employs a Ka-band Transponder (KaT) to enable two-way coherent range and Doppler measurements used for the gravity experiment and an Ultra Stable Oscillator (USO) for one-way downlink occultation experiments. This paper analyzes KaT data collected at the ESA/ESTRACK ground station in Malargüe, Argentina, during the Near-Earth Commissioning Phase (NECP) in May 2023 and the first in-cruise payload checkout (PC01) in January 2024. The radiometric data were fitted using both NASA’s Mission Analysis, Operations, and Navigation Toolkit Environment (MONTE) and ESA’s General Orbit Determination and Optimization Toolkit (GODOT) software. The comparison of the orbital solutions showed an excellent agreement. In addition, the Doppler and range residuals allowed a preliminary assessment of the quality of the radiometric measurements. During the NECP pass, the radio link data showed a range-rate noise of 0.012 mm/s at 1000 s integration time, while the root mean square of the range residuals sampled at 1 s was 8.4 mm. During the first payload checkout, the signal power at the KaT input closely matched the value expected at Jupiter, due to a specific ground station setup. This provided early indications of the 3GM’s performance during the Jovian phase. In this test, the accuracy of range data at an integration time of 1s, particularly sensitive to the link signal-to-noise ratio, degraded to 13.6 cm, whilst the range-rate accuracy turned out to be better than 0.003 mm/s at 1000 s, thanks to the accurate tropospheric delay calibration system (TDCS) available at the Malargue station (inactive during NECP). Full article
Show Figures

Figure 1

Figure 1
<p>JUICE state vector comparison between MONTE and GODOT orbit determination software in terms of position (<b>top</b>) and velocity (<b>bottom</b>) with respect to the Sun as a function of the epoch. The blue, red, and green lines represent, respectively, the x, y, and z components in the ICRF reference frame.</p>
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<p>Range (<b>top</b>) and Doppler (<b>bottom</b>) pass-through residuals difference @ 1s for the Ka/Ka link during the near-Earth commissioning phase between MONTE and GODOT models. The left panels show the difference in the computed observables on the trajectory propagated from the a priori initial condition; the right panels show the difference in computed observables at the end of the orbit determination procedure.</p>
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<p>Range (<b>top</b>) and range-rate (<b>bottom</b>) residuals @ 1s for the Ka/Ka link during the near-Earth commissioning phase.</p>
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<p>Range residuals @1s in the X/Ka link during the near-Earth commissioning phase. The standard deviation of the residuals for the first 10 min is about 6.2 cm, while the standard deviation for the remaining part is 9.6 cm. The lower noise is due to the absence of the telemetry modulation during the first 10 min.</p>
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<p>Range (<b>top</b>) and range-rate (<b>bottom</b>) residuals @1s for the Ka/Ka link during the first payload checkout.</p>
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<p>Autocorrelation function (<b>left</b>) and power spectral density (<b>right</b>) of Doppler residuals for the Ka/Ka link during the near-Earth commissioning phase, in red, and the first payload checkout, in cyan. The NECP residuals show a significant autocorrelation at the round-trip light time, meaning that the local noise at the station is the dominant noise source.</p>
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<p>Overlapping Allan deviation of the relative frequency shift residuals.</p>
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24 pages, 5258 KiB  
Article
CD8+ and CD8− NK Cells and Immune Checkpoint Networks in Peripheral Blood During Healthy Pregnancy
by Matyas Meggyes, David U. Nagy, Livia Mezosi, Beata Polgar and Laszlo Szereday
Int. J. Mol. Sci. 2025, 26(1), 428; https://doi.org/10.3390/ijms26010428 - 6 Jan 2025
Viewed by 778
Abstract
Pregnancy involves significant immunological changes to support fetal development while protecting the mother from infections. A growing body of evidence supports the importance of immune checkpoint pathways, especially at the maternal–fetal interface, although limited information is available about the peripheral expression of these [...] Read more.
Pregnancy involves significant immunological changes to support fetal development while protecting the mother from infections. A growing body of evidence supports the importance of immune checkpoint pathways, especially at the maternal–fetal interface, although limited information is available about the peripheral expression of these molecules by CD8+ and CD8− NK cell subsets during the trimesters of pregnancy. Understanding the dynamics of these immune cells and their checkpoint pathways is crucial for elucidating their roles in pregnancy maintenance and potential complications. This study aims to investigate the peripheral expression and functional characteristics of CD8+ and CD8− NK cell subsets throughout pregnancy, providing insights into their contributions to maternal and fetal health. A total of 34 healthy women were enrolled from the first, 30 from the second and 40 from the third trimester of pregnancy. At the same time, 35 healthy age-matched non-pregnant women formed the control group. From peripheral blood, mononuclear cells were separated and stored at −80 °C. CD8+ and CD8− NK cell subsets were analyzed from freshly thawed samples, and surface and intracellular staining was performed using flow cytometric analyses. The proportions of CD56+ NK cells in peripheral blood were similar across groups. While CD8− NKdim cells increased significantly in all trimesters compared to non-pregnant controls, CD8+ NKdim cells showed no significant changes. CD8− NKbright cells had higher frequencies throughout pregnancy, whereas CD8+ NKbright cells significantly increased only in the first and second trimesters. The expression levels of immune checkpoint molecules, such as PD-1 and PD-L1, and cytotoxic-activity-related molecules were stable, with notable perforin and granzyme B increases in CD8− NKbright cells throughout pregnancy. Our study shows that peripheral NK cell populations, especially CD8− subsets, are predominant during pregnancy. This shift suggests a crucial role for CD8− NK cells in balancing maternal immune tolerance and surveillance. The stable expression of immune checkpoint molecules indicates that other regulatory mechanisms may be at work. These findings enhance our understanding of peripheral immune dynamics in pregnancy and suggest that targeting CD8− NKbright cell functions could help manage pregnancy-related immune complications. This research elucidates the stable distribution and functional characteristics of peripheral NK cells during pregnancy, with CD8− subsets being more prevalent. The increased activity of CD8− NKbright cells suggests their critical role in maintaining immune surveillance. Our findings provide a basis for future studies to uncover the mechanisms regulating NK cell function in pregnancy, potentially leading to new treatments for immune-related pregnancy complications. Full article
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Figure 1
<p>Differentiation of the NK subpopulations using flow cytometric analyses. A flow cytometric gating strategy selected the investigated peripheral CD8+ and CD8− NKdim and NKbright immune cell subpopulations. After a doublet exclusion (<b>A</b>,<b>B</b>), the lymphocyte gate was created using FSC-A/SSC-A parameters (<b>C</b>). The NK cell population was gated from the lymphocyte gate based on the CD3−/CD56+ combination (<b>D</b>). Based on the density of the CD56 receptor, the NKdim and NKbright subpopulations were differentiated from the NK cell gate (<b>E</b>,<b>G</b>). From the NK cell subsets based on the presence of the CD8 receptor (<b>F</b>), further subpopulations were differentiated.</p>
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<p>Frequency of NKdim and NKbright subpopulations throughout healthy pregnancy and in non-pregnant women. Frequency of the CD8-receptor-positive and CD8-receptor-negative NKdim and NKbright cells in all lymphocytes (<b>A</b>,<b>B</b>) and in the NK subpopulation (<b>C</b>,<b>D</b>) in the three trimesters of healthy pregnancy and healthy, non-pregnant women. The solid bars represent medians of 35, 34, 30 and 40 determinations, the boxes indicate the interquartile ranges and the whiskers represent the variability of the minimum, maximum and any outlier data points in comparison to the interquartile range Significant differences with <span class="html-italic">p</span>-Values &lt; 0.01 ***, &lt;0.03 **, &lt;0.05 * are indicated.</p>
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<p>TIGIT and CD226 expression by NKdim and NKbright subpopulations throughout healthy pregnancy and in non-pregnant women. The expression of TIGIT (<b>A</b>,<b>B</b>) and CD226 receptors (<b>C</b>,<b>D</b>) by CD8-receptor-positive and CD8-receptor-negative NKdim and NKbright cells during the three trimesters of healthy pregnancy, as well as in healthy non-pregnant women. The solid bars represent medians of 20, 20, 20, and 20 determinations, the boxes indicate the interquartile ranges and the whiskers represent the variability of the minimum, maximum and any outlier data points in comparison to the interquartile range.</p>
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<p>Relative CD226 expression by NKdim and NKbright subpopulations throughout healthy pregnancy and in non-pregnant women. Mean fluorescent intensity (MFI) of the CD226 receptors by the CD8-receptor-positive and negative NKdim (<b>A</b>) and NKbright (<b>B</b>) cell subpopulations during the three trimesters of healthy pregnancy and in healthy non-pregnant women. The solid bars represent medians of 20, 21, 20 and 18 determinations, the boxes indicate the interquartile ranges and the whiskers represent the variability of the minimum, maximum and any outlier data points in comparison to the interquartile range.</p>
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<p>Soluble CD226 levels throughout healthy pregnancy and in non-pregnant women. The serum concentration of the sCD226 molecule in the four investigated cohorts. The solid bars represent medians of 20, 21, 20 and 18 determinations, the boxes indicate the interquartile ranges and the whiskers represent the variability of the minimum, maximum and any outlier data points in comparison to the interquartile range.</p>
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<p>Regression analyses between the relative expression of CD226 and the soluble level of CD226 in NKdim subpopulations throughout healthy pregnancy and in non-pregnant women. Linear regression analyses between the relative expression of CD226 and sCD226 levels in CD8-positive (<b>A</b>) and CD8-negative (<b>B</b>) NKdim subsets during the three trimesters of healthy pregnancy and in healthy non-pregnant women. <span class="html-italic">p</span>-values and coefficients of determination (r<sup>2</sup>) were calculated in R.</p>
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<p>Regression analyses between the relative expression of CD226 and the soluble level of CD226 in NKbright subpopulations throughout healthy pregnancy and in non-pregnant women. Linear regression analyses between the relative expression of CD226 and sCD226 levels in CD8-positive (<b>A</b>) and CD8-negative (<b>B</b>) NKbright subsets during the three trimesters of healthy pregnancy and in healthy non-pregnant women. <span class="html-italic">p</span>-values and coefficients of determination (r<sup>2</sup>) were calculated in R.</p>
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<p>CD112 and CD115 expression by NKdim and NKbright subpopulations throughout healthy pregnancy and in non-pregnant women. The expression of CD112 (<b>A</b>,<b>B</b>) and CD155 ligands (<b>C</b>,<b>D</b>) by CD8-receptor-positive and CD8-receptor-negative NKdim and NKbright cells during the three trimesters of healthy pregnancy and in healthy non-pregnant women. The solid bars represent medians of 20, 20, 20 and 17 determinations, the boxes indicate the interquartile ranges and the whiskers represent the variability of the minimum, maximum and any outlier data points in comparison to the interquartile range. Statistically significant differences with <span class="html-italic">p</span>-values &lt; 0.03 ** and &lt;0.01 *** are indicated.</p>
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<p>LAG-3 and Galectin-3 expression by NKdim and NKbright subpopulations throughout healthy pregnancy and in non-pregnant women. The expression of LAG-3 (<b>A</b>,<b>B</b>) and Galectin-3 receptors (<b>C</b>,<b>D</b>) by CD8-receptor-positive and CD8-receptor-negative NKdim and NKbright cells during the three trimesters of healthy pregnancy and in healthy non-pregnant women. The solid bars represent medians of 20, 20, 20 and 18 determinations, the boxes indicate the interquartile ranges, the whiskers represent the variability of the minimum, maximum and any outlier data points in comparison to the interquartile range.</p>
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<p>PD-L1 expression by NKdim and NKbright subpopulations throughout healthy pregnancy and in non-pregnant women. The expression of PD-L1 ligand (<b>A</b>,<b>B</b>) by CD8-receptor-positive and CD8-receptor-negative NKdim and NKbright cells during the three trimesters of healthy pregnancy and in healthy non-pregnant women. The solid bars represent medians of 15, 12, 10 and 16 determinations, the boxes indicate the interquartile ranges and the whiskers represent the variability of the minimum, maximum and any outlier data points in comparison to the interquartile range. Statistically significant differences with <span class="html-italic">p</span>-values &lt; 0.03 ** and &lt;0.01 *** are indicated.</p>
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<p>NKG2D expression by NKdim and NKbright subpopulations throughout healthy pregnancy and in non-pregnant women. The expression of NKG2D receptor (<b>A</b>,<b>B</b>) by CD8-receptor-positive and CD8-receptor-negative NKdim and NKbright cells during the three trimesters of healthy pregnancy and in healthy non-pregnant women. The solid bars represent medians 33, 34, 31 and 36 determinations, the boxes indicate the interquartile ranges and the whiskers represent the variability of the minimum, maximum and any outlier data points in comparison to the interquartile range.</p>
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<p>Perforin and granzyme B content by NKdim and NKbright subpopulations throughout healthy pregnancy and in non-pregnant women. The expression of intracellular perforin (<b>A</b>,<b>B</b>) and granzyme B (<b>C</b>,<b>D</b>) by CD8-receptor-positive and CD8-receptor-negative NKdim and NKbright cells during the three trimesters of healthy pregnancy and in healthy non-pregnant women. The solid bars represent medians of 19, 21, 21 and 26 determinations, the boxes indicate the interquartile ranges and the whiskers represent the variability of the minimum, maximum and any outlier data points in comparison to the interquartile range. Statistically significant differences with <span class="html-italic">p</span>-values &lt; 0.03 ** and &lt;0.01 *** are indicated.</p>
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