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27 pages, 5777 KiB  
Article
Flash Flood Regionalization for the Hengduan Mountains Region, China, Combining GNN and SHAP Methods
by Yifan Li, Chendi Zhang, Peng Cui, Marwan Hassan, Zhongjie Duan, Suman Bhattacharyya, Shunyu Yao and Yang Zhao
Remote Sens. 2025, 17(6), 946; https://doi.org/10.3390/rs17060946 - 7 Mar 2025
Viewed by 185
Abstract
The Hengduan Mountains region (HMR) is vulnerable to flash flood disasters, which account for the largest proportion of flood-related fatalities in China. Flash flood regionalization, which divides a region into homogeneous subdivisions based on flash flood-inducing factors, provides insights for the spatial distribution [...] Read more.
The Hengduan Mountains region (HMR) is vulnerable to flash flood disasters, which account for the largest proportion of flood-related fatalities in China. Flash flood regionalization, which divides a region into homogeneous subdivisions based on flash flood-inducing factors, provides insights for the spatial distribution patterns of flash flood risk, especially in ungauged areas. However, existing methods for flash flood regionalization have not fully reflected the spatial topology structure of the inputted geographical data. To address this issue, this study proposed a novel framework combining a state-of-the-art unsupervised Graph Neural Network (GNN) method, Dink-Net, and Shapley Additive exPlanations (SHAP) for flash flood regionalization in the HMR. A comprehensive dataset of flash flood inducing factors was first established, covering geomorphology, climate, meteorology, hydrology, and surface conditions. The performances of two classic machine learning methods (K-means and Self-organizing feature map) and three GNN methods (Deep Graph Infomax (DGI), Deep Modularity Networks (DMoN), and Dilation shrink Network (Dink-Net)) were compared for flash-flood regionalization, and the Dink-Net model outperformed the others. The SHAP model was then applied to quantify the impact of all the inducing factors on the regionalization results by Dink-Net. The newly developed framework captured the spatial interactions of the inducing factors and characterized the spatial distribution patterns of the factors. The unsupervised Dink-Net model allowed the framework to be independent from historical flash flood data, which would facilitate its application in ungauged mountainous areas. The impact analysis highlights the significant positive influence of extreme rainfall on flash floods across the entire HMR. The pronounced positive impact of soil moisture and saturated hydraulic conductivity in the areas with a concentration of historical flash flood events, together with the positive impact of topography (elevation) in the transition zone from the Qinghai–Tibet Plateau to the Sichuan Basin, have also been revealed. The results of this study provide technical support and a scientific basis for flood control and disaster reduction measures in mountain areas according to local inducing conditions. Full article
(This article belongs to the Special Issue Advancing Water System with Satellite Observations and Deep Learning)
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<p>(<b>a</b>) The digital elevation model of the Hengduan Mountains region (HMR) in China, with the historical flash flood events from 1950 to 2015 marked as black dots; (<b>b</b>) the location of the HMR with the provinces involved marked in grey.</p>
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<p>The framework of flash flood regionalization.</p>
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<p>Variations of (<b>a</b>) <span class="html-italic">DBI</span> and (<b>b</b>) <span class="html-italic">CQI</span> with the cluster number (<span class="html-italic">K</span>) for K-means, SOFM, DGI, DMoN, and Dink-Net.</p>
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<p>The regionalization maps by (<b>a</b>) K-means, (<b>b</b>) SOFM, (<b>c</b>) DGI, (<b>d</b>) DmoN, and (<b>e</b>) Dink-Net with 12 clusters. In the clustering result obtained by DMoN method with 12 clusters, the number of grids among the clusters is extremely unbalanced. Therefore, there are only 7 clusters in (<b>d</b>).</p>
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<p>(<b>a</b>) The regionalization map by Dink-Net with 12 subdivisions; (<b>b</b>) quantity and density, and (<b>c</b>) Z-score of the historical flash flood events in each subdivision of the regionalization map. The locations of historical flash flood events are marked with black dots in (<b>a</b>). The event number/event density has been marked for several subdivisions in panel (<b>b</b>), and the mean Z-score values have been presented in panel (<b>c</b>).</p>
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<p>(<b>a</b>) The locations of the Regions SW-1, SW-7, SE-8, NW-3, NW-4, M-6, and M-12 in the HMR; (<b>b</b>,<b>c</b>): topography and vegetation for Regions SW-1 and SW-7, with low relief and sub-high latitude mountain and mixed coniferous broad-leaved forest; (<b>d</b>,<b>e</b>): topography and vegetation for Region SE-8, with low relief and sub-high latitude mountain and the vegetation of shrub or farmland; (<b>f</b>,<b>g</b>) show the deep dry, hot valley canyon with sparse shrubs in Regions NW-3 and NW-4; (<b>h</b>,<b>i</b>) refer to the wide river valley on Western Sichuan plateau and the vegetation of alpine meadows and shrubland in Regions M-6 and M-12. All photos were taken by Yifan Li.</p>
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<p>The average of SHAP absolute values (average impact on model output magnitude) of inducing factors on the regionalization result from the SHAP model for the entire Hengduan Mountains region (HMR).</p>
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<p>The SHAP value of the top 20 important inducing factors for each 2 × 2 km<sup>2</sup> grid in (<b>a</b>) Region SW-1, (<b>b</b>) Region SW-7, and (<b>c</b>) Region SE-8. Each dot in a panel represents the data for a grid. The inducing factors in each panel are ranked in descending order according to the factors’ local impact in each subdivision. The dot color indicates the attribute values of the corresponding factors, with red referring to the high attribute values of a factor. The <span class="html-italic">x</span>-axis value represents the SHAP values that quantify the factors’ impact on the classification tendency for that grid.</p>
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<p>The SHAP value spatial distribution of inducing factors for each subdivision: (<b>a</b>) temperature; (<b>b</b>) mean of maximum 12 h rainfall ((P<sub>12h</sub>)<sub>mean</sub>); (<b>c</b>) mean of maximum 24 h rainfall ((P<sub>24h</sub>)<sub>mean</sub>); (<b>d</b>) elevation (Dem); (<b>e</b>) soil moisture (Smoisture); and (<b>f</b>) soil saturated hydraulic conductivity (Ks).</p>
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16 pages, 716 KiB  
Article
Efficient Graph Representation Learning by Non-Local Information Exchange
by Ziquan Wei, Tingting Dan, Jiaqi Ding and Guorong Wu
Electronics 2025, 14(5), 1047; https://doi.org/10.3390/electronics14051047 - 6 Mar 2025
Viewed by 139
Abstract
Graphs are an effective data structure for characterizing ubiquitous connections as well as evolving behaviors that emerge in inter-wined systems. Limited by the stereotype of node-to-node connections, learning node representations is often confined in a graph diffusion process where local information has been [...] Read more.
Graphs are an effective data structure for characterizing ubiquitous connections as well as evolving behaviors that emerge in inter-wined systems. Limited by the stereotype of node-to-node connections, learning node representations is often confined in a graph diffusion process where local information has been excessively aggregated, as the random walk of graph neural networks (GNN) explores far-reaching neighborhoods layer-by-layer. In this regard, tremendous efforts have been made to alleviate feature over-smoothing issues such that current backbones can lend themselves to be used in a deep network architecture. However, compared to designing a new GNN, less attention has been paid to underlying topology by graph re-wiring, which mitigates not only flaws of the random walk but also the over-smoothing risk incurred by reducing unnecessary diffusion in deep layers. Inspired by the notion of non-local mean techniques in the area of image processing, we propose a non-local information exchange mechanism by establishing an express connection to the distant node, instead of propagating information along the (possibly very long) original pathway node-after-node. Since the process of seeking express connections throughout a graph can be computationally expensive in real-world applications, we propose a re-wiring framework (coined the express messenger wrapper) to progressively incorporate express links in a non-local manner, which allows us to capture multi-scale features without using a very deep model; our approach is thus free of the over-smoothing challenge. We integrate our express messenger wrapper with existing GNN backbones (either using graph convolution or tokenized transformer) and achieve a new record on the Roman-empire dataset as well as in terms of SOTA performance on both homophilous and heterophilous datasets. Full article
(This article belongs to the Special Issue Artificial Intelligence in Graphics and Images)
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<p>The relationship between the expressibility of the original and 3 underlying topologies of graphs and modern GNN performance (in node classification accuracy). Different landmarks represent different datasets. Colors denote graph re-wiring methods. Red arrow lines highlight the improvement by our re-wiring method. Red box explains ours preduces an easier graph to classify via changing the topology as nodes with same class denoted by colored oval being more separated. Note that all re-wiring methods are applied with the same baseline hyperparameter.</p>
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<p>Non-local information exchange mechanism (<b>right</b>), where colors of node denote the distance marked by numbers between a node to the red one, nodes with mixed color denote aggregated node feature by message-passing, solid lines are edges of graph, and dashed lines denote express connections. The technique reminiscent of non-local mean technique for image processing (<b>left</b>), which is able to capture global information by express connections that are denoted by red dashed lines reducing the over-smoothing risk in GNNs. Both ideas integrate information beyond either a spatial or topological neighbor, in order to preserve distinctive feature representations.</p>
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<p>(<b>left</b>): Illustration of progressive NLE for simulated graph with original adjacency matrix <math display="inline"><semantics> <mi mathvariant="bold">A</mi> </semantics></math> to re-wired topology <math display="inline"><semantics> <mrow> <mi>h</mi> <mi>o</mi> <mi>p</mi> <mo>(</mo> <mi mathvariant="bold">A</mi> <mo>,</mo> <mi>k</mi> <mo>)</mo> </mrow> </semantics></math> (<math display="inline"><semantics> <mrow> <mi>k</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> <mo>,</mo> <mo>⋯</mo> </mrow> </semantics></math>). (<b>right</b>): ExM sorts original graph and new graphs cascaded (C-ExM) or aggregated (A-ExM) to input to any GNN. Green arrow indicates the pipeline of an arbitrary GNN.</p>
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<p>Comparison of re-wiring methods between DropEdge, GDC, and our NLE. NLE can mitigate over-smoothing issues. Compared with previous graph re-wiring methods, over-smoothness is delayed after using NLE. Even though G2GNN or using skip connection almost eliminated smoothed node features, using NLE leads to a larger Dirichlet energy than the original graph topology.</p>
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<p>Bar plots of performance by using different layer numbers on real data.</p>
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13 pages, 264 KiB  
Article
On Inverse and Implicit Function Theorem for Sobolev Mappings
by Mihai Cristea
Axioms 2025, 14(3), 195; https://doi.org/10.3390/axioms14030195 - 6 Mar 2025
Viewed by 136
Abstract
We extend Clarke’s local inversion theorem for Sobolev mappings. We use this result to find a general implicit function theorem for continuous locally Lipschitz mapping in the first variable and satisfying just a topological condition in the second variable. An application to control [...] Read more.
We extend Clarke’s local inversion theorem for Sobolev mappings. We use this result to find a general implicit function theorem for continuous locally Lipschitz mapping in the first variable and satisfying just a topological condition in the second variable. An application to control systems is given. Full article
(This article belongs to the Section Mathematical Analysis)
17 pages, 2241 KiB  
Article
Dynamic Collaborative Optimization Strategy for Multiple Area Clusters in Distribution Networks Considering Topology Change
by Weichen Liang, Xinsheng Ma, Shuxian Yi, Yi Zhang and Xiaobo Dou
Electricity 2025, 6(1), 10; https://doi.org/10.3390/electricity6010010 - 5 Mar 2025
Viewed by 94
Abstract
To tackle the challenges arising from missing real-time measurement data and dynamic changes in network topology in optimizing and controlling distribution networks, this study proposes a data-driven collaborative optimization strategy tailored for multi-area clusters. Firstly, the distribution network is clustered based on electrical [...] Read more.
To tackle the challenges arising from missing real-time measurement data and dynamic changes in network topology in optimizing and controlling distribution networks, this study proposes a data-driven collaborative optimization strategy tailored for multi-area clusters. Firstly, the distribution network is clustered based on electrical distance modularity and power balance indicators. Next, a collaborative optimization model for multiple area clusters is constructed with the objectives of minimizing node voltage deviations and active power losses. Then, a locally observable Markov decision model within the clusters is developed to characterize the relationship between the temporal operating states of the distribution network and the decision-making instructions. Using the Actor–Critic framework, the cluster agents are trained while considering the changes in cluster boundaries due to topology variations. A Critic network based on an attention encoder is designed to map the dynamically changing cluster observations to a fixed-dimensional space, enabling agents to learn control strategies under topology changes. Finally, case studies show the effectiveness and superiority of the proposed method. Full article
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<p>Chained flexible interconnection structure with decentralized configuration of distribution substation.</p>
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<p>Diagram of cluster boundary changes under different topologies.</p>
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<p>Network structure of AECN.</p>
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<p>Topology diagram of modified IEEE33 node system.</p>
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<p>Load and PV profiles on the test day.</p>
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<p>Reward training curve (Shadow represents the fluctuation range of the reward curves from the results of ten experiments).</p>
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<p>Cluster power regulation curve. (<b>a</b>) reactive power regulation by cluster; (<b>b</b>) active regulation of clusters.</p>
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<p>Voltage distribution of test day nodes under different methods of regulation.</p>
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27 pages, 11254 KiB  
Article
Evaluating the Resilience of Mountainous Sparse Road Networks in High-Risk Geological Disaster Areas: A Case Study in Tibet, China
by Shikun Xie, Zhen Yang, Mingxuan Wang, Guilong Xu and Shuming Bai
Appl. Sci. 2025, 15(5), 2688; https://doi.org/10.3390/app15052688 - 3 Mar 2025
Viewed by 269
Abstract
Sparse road networks in high-risk geological disaster areas, characterized by long segments, few nodes, and limited alternative routes, face significant vulnerabilities to geological hazards such as landslides, rockfalls, and collapses. These disruptions hinder emergency response and resource delivery, highlighting the need for enhanced [...] Read more.
Sparse road networks in high-risk geological disaster areas, characterized by long segments, few nodes, and limited alternative routes, face significant vulnerabilities to geological hazards such as landslides, rockfalls, and collapses. These disruptions hinder emergency response and resource delivery, highlighting the need for enhanced resilience strategies. This study develops a dynamic resilience assessment framework using a two-layer topological model to analyze and optimize the resilience of such networks. The model incorporates trunk and local layers to capture dynamic changes during disasters, and it is validated using the road network in Tibet. The findings demonstrate that critical nodes, including tunnels, bridges, and interchanges, play a decisive role in maintaining network performance. Resilience is influenced by disaster type, duration, and traffic capacity, with collapse events showing moderate resilience and debris flows exhibiting rapid recovery but low survivability. Notably, half-width traffic interruptions achieve the highest overall resilience (0.7294), emphasizing the importance of partial traffic restoration. This study concludes that protecting critical nodes, optimizing resource allocation, and implementing adaptive management strategies are essential for mitigating disaster impacts and enhancing recovery. The proposed framework offers a practical tool for decision-makers to improve transportation resilience in high-risk geological disaster areas. Full article
(This article belongs to the Special Issue Future Transportation Systems: Efficiency and Reliability)
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<p>Research framework.</p>
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<p>Sparse road network with two layers.</p>
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<p>Main layer network topology.</p>
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<p>The local topological structure of the nodes.</p>
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<p>The local topological structure of the segments.</p>
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<p>The schematic diagram of the resilience recovery process of sparse road network.</p>
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<p>Study area and road network distribution.</p>
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<p>Traffic flow data collection diagram.</p>
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<p>Frequency of geological hazards.</p>
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<p>Level of geological hazards.</p>
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<p>The degree of disruption for geological disasters.</p>
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<p>Average debris clearance duration of geological disasters.</p>
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<p>Four types of geological disaster classification examples.</p>
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<p>Simulation process for road network resilience assessment under disaster events.</p>
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<p>The two-layer structure of the regional sparse road network.</p>
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<p>Simplified topology of sparse road network.</p>
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<p>The resilience curve of the road network after a random node is broken.</p>
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<p>Resilience curve after random failures of critical nodes.</p>
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<p>Road network resilience values under varying disaster durations.</p>
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<p>Road network resilience with different residual capacities.</p>
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20 pages, 650 KiB  
Article
The Glass Transition: A Topological Perspective
by Arthur Vesperini, Roberto Franzosi and Marco Pettini
Entropy 2025, 27(3), 258; https://doi.org/10.3390/e27030258 - 28 Feb 2025
Viewed by 156
Abstract
Resorting to microcanonical ensemble Monte Carlo simulations, we study the geometric and topological properties of the state space of a model of a network glass-former. This model, a Lennard-Jones binary mixture, does not crystallize due to frustration. We have found two peaks in [...] Read more.
Resorting to microcanonical ensemble Monte Carlo simulations, we study the geometric and topological properties of the state space of a model of a network glass-former. This model, a Lennard-Jones binary mixture, does not crystallize due to frustration. We have found two peaks in specific heat at equilibrium and at low energy, corresponding to important changes in local ordering. These singularities were accompanied by inflection points in geometrical markers of the potential energy level sets—namely, the mean curvature, the dispersion of the principal curvatures, and the variance of the scalar curvature. Pinkall’s and Overholt’s theorems closely relate these quantities to the topological properties of the accessible state-space manifold. Thus, our analysis provides strong indications that the glass transition is associated with major changes in the topology of the energy level sets. This important result suggests that this phase transition can be understood through the topological theory of phase transitions. Full article
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<p>Specific heat <math display="inline"><semantics> <msub> <mi>c</mi> <mi>v</mi> </msub> </semantics></math> as a function of the energy density <math display="inline"><semantics> <mi>ϵ</mi> </semantics></math>, in a system with <math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>216</mn> </mrow> </semantics></math>. The blue circles were obtained using Equation (<a href="#FD14-entropy-27-00258" class="html-disp-formula">14</a>), while the red triangles were obtained using Equation (<a href="#FD13-entropy-27-00258" class="html-disp-formula">13</a>). The inset is a zoom on the low-energy peak. The dashed line is an arbitrary fit, meant to guide the eye.</p>
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<p>Average temperature <span class="html-italic">T</span> as a function of the energy density.</p>
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<p>The first two derivatives of the entropy as functions of the energy density <math display="inline"><semantics> <mi>ϵ</mi> </semantics></math>: (<b>a</b>) <math display="inline"><semantics> <mi>β</mi> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <mi>γ</mi> </semantics></math>. The inset in (<b>b</b>) is a zoom on the high-energy peak. A few monotonously increasing low-energy data points have been cut from (<b>b</b>) for the sake of clarity.</p>
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<p>Instantaneous sample configurations projected onto a arbitrary planes, at energy density (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>ϵ</mi> <mo>≈</mo> <mo>−</mo> <mn>4.70</mn> </mrow> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>ϵ</mi> <mo>≈</mo> <mo>−</mo> <mn>4.39</mn> </mrow> </semantics></math>, and (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>ϵ</mi> <mo>≈</mo> <mo>−</mo> <mn>2.51</mn> </mrow> </semantics></math>. Particles of species 1(2) are represented in large blue and small red circles, respectively.</p>
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<p>Radial pair distribution function for (<b>a</b>) 1–1 bonds, (<b>b</b>) 2–2 bonds, and (<b>c</b>) 1–2 bonds. The continuous blue lines, dashed red lines and dotted-dashed green lines correspond to systems with <math display="inline"><semantics> <mrow> <mi>ϵ</mi> <mo>=</mo> <mo>−</mo> <mn>4.7016</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>ϵ</mi> <mo>=</mo> <mo>−</mo> <mn>4.39388</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>ϵ</mi> <mo>=</mo> <mo>−</mo> <mn>2.50785</mn> </mrow> </semantics></math>, respectively.</p>
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<p>Bond-orientational order parameters <math display="inline"><semantics> <msub> <mi>Q</mi> <mi>l</mi> </msub> </semantics></math> as a function of the energy density <math display="inline"><semantics> <mrow> <mi>ϵ</mi> <mo>=</mo> <mi>E</mi> <mo>/</mo> <mi>N</mi> </mrow> </semantics></math> for (<b>a</b>) 1–1 bonds, (<b>b</b>) 2–2 bonds, and (<b>c</b>) 1–2 bonds. Represented are the parameters <math display="inline"><semantics> <msub> <mi>Q</mi> <mn>2</mn> </msub> </semantics></math> (red squares), <math display="inline"><semantics> <msub> <mi>Q</mi> <mn>4</mn> </msub> </semantics></math> (blue circles), <math display="inline"><semantics> <msub> <mi>Q</mi> <mn>6</mn> </msub> </semantics></math> (green triangles), <math display="inline"><semantics> <msub> <mi>Q</mi> <mn>8</mn> </msub> </semantics></math> (purple diamonds), and <math display="inline"><semantics> <msub> <mi>Q</mi> <mn>10</mn> </msub> </semantics></math> (orange pentagons). The value <math display="inline"><semantics> <mrow> <mn>1</mn> <mo>/</mo> <msqrt> <msub> <mi>n</mi> <mi>B</mi> </msub> </msqrt> </mrow> </semantics></math>, expected in a fully disordered system, is shown as a black line.</p>
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<p>Total mean curvature as a function of the energy density.</p>
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<p>Dispersion of the principal curvatures as a function of the energy density.</p>
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<p>Variance of the scalar curvature as a function of the energy density.</p>
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23 pages, 13868 KiB  
Article
In Situ Study of Surface Morphology Formation Mechanism During Laser Powder Bed Fusion
by Yuhui Zhang, Hang Ren, Hualin Yan and Yu Long
Appl. Sci. 2025, 15(5), 2550; https://doi.org/10.3390/app15052550 - 27 Feb 2025
Viewed by 151
Abstract
In the laser powder bed fusion (LPBF) process, the surface quality of intermediate layers impacts interlayer bonding and part forming quality. Due to the complex dynamic process inherent in LPBF, current monitoring methods struggle to achieve high-quality in situ online monitoring, which limits [...] Read more.
In the laser powder bed fusion (LPBF) process, the surface quality of intermediate layers impacts interlayer bonding and part forming quality. Due to the complex dynamic process inherent in LPBF, current monitoring methods struggle to achieve high-quality in situ online monitoring, which limits the in-depth understanding of the evolution mechanisms of the surface morphology of LPBF intermediate layers. This paper employs an optimized coaxial optical imaging method to monitor key LPBF processes and analyzes the intermediate layer surface morphology evolution mechanism considering heat, force, and mass transfer. Results indicate that LPBF intermediate layer surfaces are influenced by energy density, melt pool behavior, and previous layer morphology, forming complex topological structures. At a low energy density, insufficient powder melting causes balling, extended by subsequent melt pools to form a reticulated structure and local large-scale protrusions. Heat accumulation at a high energy density promotes melt pool expansion, reduces melt track overlap, and effectively eliminates defects from previous layers via remelting, with spatter becoming the main defect. Additionally, the melt pool wettability on the part contours captures external powder, forming unique, overhanging contour protrusions. This paper enhances understanding of LPBF intermediate layer surface morphology formation mechanisms and provides a theoretical basis for optimizing surface quality. Full article
(This article belongs to the Section Additive Manufacturing Technologies)
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<p>(<b>a</b>) Schematic and optical configuration of LPBF system. The red arrow indicates the 1080 nm laser beam, the green arrow indicates the 808 nm auxiliary laser beam, and the blue arrow indicates the optical emission of melt pool; (<b>b</b>) photograph of actual setup.</p>
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<p>Position distribution of experimental samples on base plate for two groups: (<b>a</b>) multi-layer (5-layer) samples, (<b>b</b>) single-layer samples, and (<b>c</b>) scanning strategy and sample position dimensions. The red arrow indicates the bidirectional serpentine scanning strategy.</p>
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<p>Melt pool morphology under different process parameters: (<b>a</b>) SED = 62.5 Jmm<sup>−2</sup> (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_1</a>); (<b>b</b>) SED = 75 Jmm<sup>−2</sup> (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_2</a>); (<b>c</b>) SED = 116.67 Jmm<sup>−2</sup> (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_3, 4</a>); and (<b>d</b>,<b>e</b>) area changes.</p>
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<p>The effect of laser power on the temperature distribution of the melt pool: (<b>a</b>) <span class="html-italic">P</span> = 200 W (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_5</a>); (<b>b</b>) <span class="html-italic">P</span> = 250 W (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_6</a>); (<b>c</b>) <span class="html-italic">P</span> = 300 W (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_7</a>); (<b>d</b>) <span class="html-italic">P</span> = 350 W (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_8</a>); (<b>e</b>) <span class="html-italic">P</span> = 400 W (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_9</a>); (<b>f</b>) the effect of laser power on the temperature distribution along the centerline of the melt track (<span class="html-italic">V</span> = 80 mm/s).</p>
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<p>The effect of scanning speed on the temperature distribution of the melt pool: (<b>a</b>) <span class="html-italic">V</span> = 60 mm/s (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_10</a>); (<b>b</b>) <span class="html-italic">V</span> = 80 mm/s (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_7</a>); (<b>c</b>) <span class="html-italic">V</span> = 100 mm/s (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_11</a>); (<b>d</b>) <span class="html-italic">V</span> = 120 mm/s (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_12</a>); (<b>e</b>) the effect of scanning speed on the temperature distribution along the centerline of melt track (<span class="html-italic">P</span> = 300 W).</p>
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<p>Continuous frames and characteristics of the melt pool corresponding to single-layer surfaces at different energy density levels: (<b>a</b>) At a low energy density (SED = 50 Jmm<sup>−2</sup>), incompletely melted powders fused with each other to form larger-sized spherical particles (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_1</a>). (<b>b</b>) The contraction and breakage of the melt end during solidification led to the formation of balling (SED = 75 Jmm<sup>−2</sup>) (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_2</a>). (<b>c</b>) At a high energy density (SED = 100 Jmm<sup>−2</sup>), remelting occurred between adjacent melt tracks (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_13</a>). (<b>d</b>) The accumulation of melt at the end of the melt track (<a href="#app1-applsci-15-02550" class="html-app">Supplementary Video ESM_14</a>). All images are at a scale of 100 μm.</p>
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<p>Three-dimensional surface morphology of single-layer samples under different process parameters: (<b>a1</b>,<b>a2</b>) spheroidal surface, SED = 50 Jmm<sup>−2</sup>; (<b>b1</b>,<b>b2</b>) transitional surface, SED = 62.5 Jmm<sup>−2</sup>; (<b>c1</b>,<b>c2</b>) uniform surface, SED = 100 Jmm<sup>−2</sup>.</p>
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<p>Three-dimensional surface morphology of multi-layer samples under different process parameters: (<b>a</b>) reticulated surface, (<b>b</b>) undulating surface, (<b>c</b>) uniform surface.</p>
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<p>(<b>a</b>) Morphological images of the intermediate layers of a multi-layer sample with a reticulated surface. (<b>b1</b>) Photograph of reticular structures. (<b>b2</b>) Three-dimensional morphology of reticular structures; (<b>c1</b>) Photograph of large-scale local surface agglomerate protrusions. (<b>c2</b>) Three-dimensional morphology of large-scale local surface agglomerate protrusions.</p>
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<p>Formation process of local features on reticulated surface: (<b>a</b>) layer-by-layer aggregation of spherical solidification particles, (<b>b</b>) principle of edge connection between adjacent spherical solidification particles, and (<b>c</b>) formation process of reticulated structures and local large-scale agglomerated protrusions.</p>
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<p>Variation in melt pool temperature and high-temperature area in transitional surface samples during printing process: (<b>a</b>) SED = 62.5 Jmm<sup>−2</sup>; (<b>b</b>) SED = 70 Jmm<sup>−2</sup>. The color images represent the temperature distribution of the melt pool at different moments.</p>
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<p>The quantification of surface roughness under different process parameters. (<b>a</b>) The effect of laser power and scanning speed on the arithmetic mean height (Sa). (<b>b</b>) The impact of varying energy densities on multiple surface roughness parameters: the arithmetic mean height (Sa), maximum height (Sz), root mean square height (Sq), skewness (Ssk), kurtosis (Sku), maximum peak height (Sp), and maximum valley depth (Sv).</p>
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<p>Spatters and unmelted powder particles on a uniform single-layer surface: (<b>a</b>) SED = 100 Jmm<sup>−2</sup>; (<b>b</b>) SED = 116.67 Jmm<sup>−2</sup>; (<b>c</b>) the process of spatter formation.</p>
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<p>Local surface morphology of uniform surface on multi-layer samples: (<b>a1</b>,<b>a2</b>) wavy morphology; (<b>b1</b>,<b>b2</b>) uniform surface.</p>
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<p>Edge contour protrusion cross-sectional morphology of multi-layer samples under different process conditions: (<b>a</b>) reticular surface, (<b>a1</b>,<b>a2</b>) cross-sectional morphology of the contours on both sides of the sample with a reticular surface; (<b>b</b>) uniform surface, (<b>b1</b>,<b>b2</b>) cross-sectional morphology of the contours on both sides of the sample with a uniform surface.</p>
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<p>(<b>a</b>) Inclusions of unmelted powder within the part due to insufficient melting. (<b>b</b>) The formation mechanism of edge contour protrusions and powder inclusions.</p>
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20 pages, 6751 KiB  
Article
Altered Directed-Connectivity Network in Temporal Lobe Epilepsy: A MEG Study
by Chen Zhang, Wenhan Hu, Yutong Wu, Guangfei Li, Chunlan Yang and Ting Wu
Sensors 2025, 25(5), 1356; https://doi.org/10.3390/s25051356 - 22 Feb 2025
Viewed by 315
Abstract
Temporal lobe epilepsy (TLE) is considered a network disorder rather than a localized lesion, making it essential to study the network mechanisms underlying TLE. In this study, we constructed directed brain networks based on clinical MEG data using the Granger Causality Analysis (GCA) [...] Read more.
Temporal lobe epilepsy (TLE) is considered a network disorder rather than a localized lesion, making it essential to study the network mechanisms underlying TLE. In this study, we constructed directed brain networks based on clinical MEG data using the Granger Causality Analysis (GCA) method, aiming to provide new insights into the network mechanisms of TLE. MEG data from 13 lTLE and 21 rTLE patients and 14 healthy controls (HCs) were analyzed. The preprocessed MEG data were used to construct directed brain networks using the GCA method and undirected brain networks using the Pearson Correlation Coefficient (PCC) method. Graph theoretical analysis extracted global and local topologies from the binary matrix, and SVM classified topologies with significant differences (p < 0.05). Comparative studies were performed on connectivity strengths, graph theory metrics, and SVM classifications between GCA and PCC, with an additional analysis of GCA-weighted network connectivity. The results show that TLE patients showed significantly increased functional connectivity based on GCA compared to the control group; similarities of the hub brain regions between lTLE and rTLE patients and the cortical–limbic–thalamic–cortical loop were identified; TLE patients exhibited a significant increase in GCA-based Global Clustering Coefficient (GCC) and Global Local Efficiency (GLE); most brain regions with abnormal local topological properties in TLE patients overlapped with their hub regions. The directionality of brain connectivity has played a significantly more pivotal role in research on TLE. GCA may be a potential tool in MEG analysis to distinguish TLE patients and HC effectively. Full article
(This article belongs to the Section Biomedical Sensors)
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<p>Overview of the experimental workflow. (<b>A</b>) Data Preprocessing: This phase includes the preprocessing of MEG data, the construction of head and source models using T1-weighted MRI, and source reconstruction with the beamformer algorithm to derive regional brain signals. Brain regions are then parcellated according to the AAL116 atlas, and representative signals are extracted based on the maximum power values. (<b>B</b>) Brain Network Construction and Analysis: This section includes brain network construction, brain network binarization, and weighted network analysis. Directed brain networks are established through Granger Causality Analysis (GCA), while undirected networks are formed using the Pearson Correlation Coefficient (PCC). Both networks are binarized using a Global Cost Efficiency (GCE) approach. Weighted network analysis includes comparing connection strengths, evaluating directed connectivity and out-degree metrics, and identifying hub regions. (<b>C</b>) Graph Theoretical Analysis: The analysis focuses on extracting four global topologies: Global Clustering Coefficient (GCC), Global Characteristic Path Length (GCLP), Global Efficiency (GE), and Global Local Efficiency (GLE); and four local topologies: Node Clustering Coefficient (NCC), Node Efficiency (NE), Node Local Efficiency (NLE), and Node Degree Centrality (NDC) from the binarized brain networks. (<b>D</b>) Machine Learning Application: Support Vector Machine (SVM) is utilized to classify topologies with differences of <span class="html-italic">p</span> &lt; 0.05, highlighting differences between the two methodologies.</p>
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<p>Average connection strengths based on PCC and GCA methods. Blue boxplots represent average connection strengths using the Pearson Correlation Coefficient (PCC) method for healthy controls (HCs), left temporal lobe epilepsy (lTLE) patients, and right TLE (rTLE) patients. Red boxplots represent average connection strengths using the Granger Causality Analysis (GCA) method for HC, lTLE, and rTLE. Abbreviations: PCC HC, PCC lTLE, and PCC rTLE denote HC, lTLE, and rTLE using the PCC method, respectively. Similarly, GCA HC, GCA lTLE, and GCA rTLE denote HC, lTLE, and rTLE using the GCA method. (*) indicates statistical significance between HC and lTLE, as well as between HC and rTLE, assessed using a <span class="html-italic">t</span>-test. * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.001.</p>
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<p>Different connectivity analysis based on GCA. This figure presents a comparative analysis of brain network connectivity between left temporal lobe epilepsy (lTLE), right temporal lobe epilepsy (rTLE), and healthy controls (HCs). The four sections (<b>A</b>–<b>D</b>) represent different network connectivity features. (<b>A</b>) Top 20 LCS: The top 20 strongest connections in each group, ranked by connection strength. (<b>B</b>) Top 20 GDC: The top 20 connections with the greatest dissimilarity for lTLE and rTLE compared to HC. (<b>C</b>) Top 5 HODR: The top 5 brain regions with the highest out-degree in each group. (<b>D</b>) Top 5 GDR: The top 5 brain regions with the greatest dissimilarity for lTLE and rTLE compared to HC. The color legend indicates the brain regions involved, with each color corresponding to a specific brain region.</p>
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<p>Hub regions in TLE. This figure illustrates the hub regions of brain networks in patients with lTLE and rTLE. The hubs are identified based on their frequency of appearance in different analyses. (<b>A</b>) lTLE hub regions: hub regions in patients with lTLE. (<b>B</b>) rTLE hub regions: hub regions in patients with rTLE. Arrows indicate the increasing frequency of hub regions from bottom to top in each section. Each brain slice shows the anatomical location of these regions and is visualized using axial, sagittal, and coronal brain slices.</p>
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<p>Global topological parameters of brain functional networks in lTLE patients, rTLE patients, and HC. In the bar graph, black lines indicate data ranges and bars depict means. (*) indicates: <span class="html-italic">p</span> &lt; 0.05, as determined by the Mann–Whitney U non-parametric test.</p>
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<p>AUC of SVM classification of TLE and HC based on PCC and GCA methods.</p>
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<p>Classification effect of GCA under different model orders.</p>
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26 pages, 1133 KiB  
Article
Adaptive CT XIGA Using LR B-Splines for Efficient Fracture Modeling
by Fei Gao, Cancan Ge, Zhuochao Tang, Jiming Gu and Rui Meng
Materials 2025, 18(5), 920; https://doi.org/10.3390/ma18050920 - 20 Feb 2025
Viewed by 179
Abstract
This paper presents a novel adaptive crack-tip extended isogeometric analysis (adaptive CT XIGA) framework based on locally refined B-splines (LR B-splines) for efficient and accurate fracture modeling in two-dimensional solids. The XIGA method facilitates crack modeling without requiring the specific locations of crack [...] Read more.
This paper presents a novel adaptive crack-tip extended isogeometric analysis (adaptive CT XIGA) framework based on locally refined B-splines (LR B-splines) for efficient and accurate fracture modeling in two-dimensional solids. The XIGA method facilitates crack modeling without requiring the specific locations of crack faces and enables crack propagation simulation without remeshing by employing localized enrichment functions. LR B-splines, as an advanced extension of B-splines and NURBS, offer high-order continuity, precise geometric representation, and local refinement capabilities, thereby enhancing computational accuracy and efficiency. Various local mesh refinement strategies, designed based on crack and crack-tip locations, are investigated. Among these strategies, the crack-tip topological refinement strategy is adopted for local refinement in the adaptive CT XIGA framework. Stress intensity factors (SIFs) are evaluated using the contour interaction integral technique, while the maximum circumferential stress criterion is adopted to predict the crack growth direction. Numerical examples demonstrate the accuracy, efficiency, and robustness of adaptive CT XIGA. The results confirm that the proposed framework achieves superior error convergence rates and significantly reduces computational costs compared to a-posteriori-error-based adaptive XIGA methods, particularly in crack propagation simulations. These advantages establish adaptive CT XIGA as a powerful and efficient tool for addressing complex fracture problems in solid mechanics. Full article
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<p>(<b>a</b>) Schematic representation of an infinite plate with a central crack under remote uniform tensile loading. (<b>b</b>) Initial computational mesh and control points. The blue dots represent the control points, while the red line depicts the crack. The red square symbols mark control points enriched with crack-tip enrichment functions, whereas the red cross symbols denote control points enriched with the Heaviside function.</p>
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<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT XIGA.</p>
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<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT2 XIGA.</p>
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<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT3 XIGA.</p>
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<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CTCF XIGA.</p>
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<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT2CF XIGA.</p>
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<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT3CF XIGA.</p>
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<p>Convergence of the relative error in the H1 norm as a function of the number of DOFs for adaptive XIGA using various refinement strategies.</p>
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<p>Convergence of the relative error in the energy norm as a function of the number of DOFs for adaptive XIGA using various refinement strategies.</p>
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<p>Comparison of computation times of adaptive XIGA using various refinement strategies.</p>
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<p>Schematic representation of a circular plate with a central crack subjected to a constant normal traction along the circumference.</p>
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<p>Initial computational mesh (<b>a</b>) and the meshes of local refinement at first (<b>b</b>), second (<b>c</b>), and third (<b>d</b>) steps in adaptive CT XIGA.</p>
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<p>Convergence of the relative error of the Mode-I SIF as a function of the number of DOFs.</p>
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<p>Comparison of computation times as a function of the number of refinement steps.</p>
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<p>Comparison of Mode-I SIFs for different crack lengths <math display="inline"><semantics> <mrow> <mn>2</mn> <mi>a</mi> </mrow> </semantics></math>.</p>
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<p>Schematic representation of a square plate with a central curved crack under uniaxial tension.</p>
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<p>Initial computational mesh (<b>a</b>) and the meshes of local refinement at first (<b>b</b>), third (<b>c</b>), and fifth (<b>d</b>) steps in adaptive CT XIGA.</p>
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<p>Convergence of the mixed-mode SIFs as a function of the number of DOFs for the square plate with a center curved crack: <math display="inline"><semantics> <msub> <mi>K</mi> <mi>I</mi> </msub> </semantics></math> (<b>a</b>) and <math display="inline"><semantics> <msub> <mi>K</mi> <mrow> <mi>I</mi> <mi>I</mi> </mrow> </msub> </semantics></math> (<b>b</b>).</p>
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<p>Comparison of computation times as a function of the number of refinement steps.</p>
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<p>Comparison of the mixed-mode SIFs at different values of <math display="inline"><semantics> <mi>ω</mi> </semantics></math>: <math display="inline"><semantics> <msub> <mi>K</mi> <mi>I</mi> </msub> </semantics></math> (<b>a</b>) and <math display="inline"><semantics> <msub> <mi>K</mi> <mrow> <mi>I</mi> <mi>I</mi> </mrow> </msub> </semantics></math> (<b>b</b>).</p>
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<p>Schematic representation and loading conditions of a cantilever beam with an edge crack.</p>
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<p>The locally refined meshes of adaptive CT XIGA applying three local refinement steps for crack growth at step 0 (<b>a</b>), step 4 (<b>b</b>), step 7 (<b>c</b>), and step 9 (<b>d</b>).</p>
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<p>Comparison of crack growth paths of the cantilever beam with an edge crack.</p>
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<p>Comparison of computation times as a function of the number of crack growth steps.</p>
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<p>Schematic representation and loading conditions of a square plate with a center-inclined crack.</p>
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<p>The locally refined meshes of adaptive CT XIGA applying three local refinement steps for crack growth at step 0 (<b>a</b>), step 1 (<b>b</b>), and step 2 (<b>c</b>) when <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>45</mn> </mrow> </semantics></math>.</p>
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<p>Comparison of crack growth paths of the square plate with a center-inclined crack when <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>45</mn> </mrow> </semantics></math>.</p>
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<p>Comparison of computation times as a function of the number of crack growth steps.</p>
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<p>Crack growth paths of the center-inclined crack in the square plate by adaptive CT XIGA using three local refinement steps for different crack inclination angles.</p>
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<p>Schematic representation and loading conditions of a square plate with two edge cracks.</p>
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<p>The locally refined meshes of adaptive CT XIGA applying four local refinement steps for crack growth at step 0 (<b>a</b>), step 8 (<b>b</b>), and step 17 (<b>c</b>).</p>
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<p>Comparison of crack growth paths of the square plate with two edge cracks.</p>
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<p>Comparison of computation times as a function of the number of crack growth steps.</p>
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28 pages, 2083 KiB  
Article
Pipe Routing with Topology Control for Decentralized and Autonomous UAV Networks
by Shreyas Devaraju, Shivam Garg, Alexander Ihler, Elizabeth Serena Bentley and Sunil Kumar
Drones 2025, 9(2), 140; https://doi.org/10.3390/drones9020140 - 13 Feb 2025
Viewed by 664
Abstract
This paper considers a decentralized and autonomous wireless network of low SWaP (size, weight, and power) fixed-wing UAVs (unmanned aerial vehicles) used for remote exploration and monitoring of targets in an inaccessible area lacking communication infrastructure. Here, the UAVs collaborate to find target(s) [...] Read more.
This paper considers a decentralized and autonomous wireless network of low SWaP (size, weight, and power) fixed-wing UAVs (unmanned aerial vehicles) used for remote exploration and monitoring of targets in an inaccessible area lacking communication infrastructure. Here, the UAVs collaborate to find target(s) and use routing protocols to forward the sensed data of target(s) to an aerial base station (BS) in real-time through multihop communication, which can then transmit the data to a control center. However, the unpredictability of target locations and the highly dynamic nature of autonomous, decentralized UAV networks result in frequent route breaks or traffic disruptions. Traditional routing schemes cannot quickly adapt to dynamic UAV networks and can incur large control overhead and delays. In addition, their performance suffers from poor network connectivity in sparse networks with multiple objectives (exploration and monitoring of targets), which results in frequent route unavailability. To address these challenges, we propose two routing schemes: Pipe routing and TC-Pipe routing. Pipe routing is a mobility-, congestion-, and energy-aware scheme that discovers routes to the BS on-demand and proactively switches to alternate high-quality routes within a limited region around the routes (referred to as the “pipe”) when needed. TC-Pipe routing extends this approach by incorporating a decentralized topology control mechanism to help maintain robust connectivity in the pipe region around the routes, resulting in improved route stability and availability. The proposed schemes adopt a novel approach by integrating the topology control with routing protocol and mobility model, and rely only on local information in a distributed manner. Comprehensive evaluations under diverse network and traffic conditions—including UAV density and speed, number of targets, and fault tolerance—show that the proposed schemes improve throughput by reducing flow interruptions and packet drops caused by mobility, congestion, and node failures. At the same time, the impact on coverage performance (measured in terms of coverage and coverage fairness) is minimal, even with multiple targets. Additionally, the performance of both schemes degrades gracefully as the percentage of UAV failures in the network increases. Compared to schemes that use dedicated UAVs as relay nodes to establish a route to the BS when the UAV density is low, Pipe and TC-Pipe routing offer better coverage and connectivity trade-offs, with the TC-Pipe providing the best trade-off. Full article
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<p>Illustration of a decentralized and autonomous UAV network for remote monitoring of an inaccessible area where a communication infrastructure is not available. Here, the UAVs collaborate to provide robust routes for transmitting the sensed information of ground-based targets to a base station while performing fast area coverage.</p>
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<p>Challenges in a decentralized and autonomous UAV network, where low SWaP UAVs are tasked to provide fast area coverage while maintaining strong network connectivity, and assist in reliably forwarding sensed data of multiple target UAVs to the BS within the latency constraints.</p>
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<p>Modules used in our proposed Pipe and TC-Pipe routing schemes.</p>
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<p>Illustration of a pipe around the current route (red links) from the target UAV to BS. The pipe consists of nodes (green nodes) that are up to 2-hop from the nodes along the route (red nodes).</p>
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<p>Illustration of pipe thinning problem, where the node <math display="inline"><semantics> <msup> <mi>N</mi> <mo>′</mo> </msup> </semantics></math> has no one-hop neighbors except the upstream and downstream nodes on the current route.</p>
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<p>Applying a pheromone mask to attract UAVs.</p>
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<p>The target locations in a 6 × 6 <math display="inline"><semantics> <mrow> <msup> <mi>km</mi> <mn>2</mn> </msup> </mrow> </semantics></math> map. Three different target locations are shown for a single target in (<b>a</b>–<b>c</b>) and for a group of 3-targets in (<b>d</b>–<b>f</b>).</p>
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<p>Average route length for three-target locations.</p>
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<p>Routing Performance: PDR for single-target settings <math display="inline"><semantics> <msub> <mi>C</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>C</mi> <mn>2</mn> </msub> </semantics></math>, and <math display="inline"><semantics> <msub> <mi>C</mi> <mn>3</mn> </msub> </semantics></math>. Suffix “-20” (e.g., TC-Pipe-20, AODV-20) indicate UAVs at 20 m/s, while “-40” indicates UAVs at 40 m/s speeds.</p>
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<p>Routing Performance: PDR for three-target settings <math display="inline"><semantics> <msub> <mi>C</mi> <mn>4</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>C</mi> <mn>5</mn> </msub> </semantics></math>, and <math display="inline"><semantics> <msub> <mi>C</mi> <mn>6</mn> </msub> </semantics></math>.</p>
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<p>Routing Performance: Route Up for three-target settings <math display="inline"><semantics> <msub> <mi>C</mi> <mn>4</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>C</mi> <mn>5</mn> </msub> </semantics></math>, and <math display="inline"><semantics> <msub> <mi>C</mi> <mn>6</mn> </msub> </semantics></math>.</p>
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<p>Routing Performance: Route Breaks for three-target settings <math display="inline"><semantics> <msub> <mi>C</mi> <mn>4</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>C</mi> <mn>5</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>C</mi> <mn>6</mn> </msub> </semantics></math>.</p>
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<p>Coverage vs. Time plots for three-target settings <math display="inline"><semantics> <msub> <mi>C</mi> <mn>4</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>C</mi> <mn>5</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>C</mi> <mn>6</mn> </msub> </semantics></math>.</p>
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<p>Coverage Performance: <math display="inline"><semantics> <msub> <mi>C</mi> <mi>v</mi> </msub> </semantics></math> for three-target settings <math display="inline"><semantics> <msub> <mi>C</mi> <mn>4</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>C</mi> <mn>5</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>C</mi> <mn>6</mn> </msub> </semantics></math></p>
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<p>Coverage performance: Fairness for three-target settings <math display="inline"><semantics> <msub> <mi>C</mi> <mn>4</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>C</mi> <mn>5</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>C</mi> <mn>6</mn> </msub> </semantics></math>.</p>
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<p>PDR values for UAV speed of 40 m/s with 30 and 50 UAVs, for single-target setting <math display="inline"><semantics> <msub> <mi>C</mi> <mn>2</mn> </msub> </semantics></math> and three-target setting <math display="inline"><semantics> <msub> <mi>C</mi> <mn>5</mn> </msub> </semantics></math>.</p>
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<p>Routing and Coverage metrics for UAV speed of 40 m/s, with 30 and 50 UAVs, for single-target setting <math display="inline"><semantics> <msub> <mi>C</mi> <mn>2</mn> </msub> </semantics></math> and three-target setting <math display="inline"><semantics> <msub> <mi>C</mi> <mn>5</mn> </msub> </semantics></math>.</p>
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20 pages, 745 KiB  
Article
Advancing Logic-Driven and Complex Event Perception Frameworks for Entity Alignment in Knowledge Graphs
by Yajian Zeng, Xiaorong Hou, Xinrui Wang and Junying Li
Electronics 2025, 14(4), 670; https://doi.org/10.3390/electronics14040670 - 9 Feb 2025
Viewed by 535
Abstract
Entity alignment in knowledge graphs plays a crucial role in ensuring the consistency and integration of data across different domains. For example, in power topology, accurate entity matching is essential for optimizing system design and control. However, traditional approaches to entity alignment often [...] Read more.
Entity alignment in knowledge graphs plays a crucial role in ensuring the consistency and integration of data across different domains. For example, in power topology, accurate entity matching is essential for optimizing system design and control. However, traditional approaches to entity alignment often rely heavily on language models to extract general features, which can overlook important logical aspects such as temporal and event-centric relationships that are crucial for precise alignment.To address this issue, we propose EAL (Entity Alignment with Logical Capturing), a novel and lightweight RNN-based framework designed to enhance logical feature learning in entity alignment tasks. EAL introduces a logical paradigm learning module that effectively models complex-event relationships, capturing structured and context-aware logical patterns that are essential for alignment. This module encodes logical dependencies between entities to dynamically capture both local and global temporal-event interactions. Additionally, we integrate an adaptive logical attention mechanism that prioritizes influential logical features based on task-specific contexts, ensuring the extracted features are both relevant and discriminative. EAL also incorporates a key feature alignment framework that emphasizes critical event-centric logical structures. This framework employs a hierarchical feature aggregation strategy combining low-level information on temporal events with high-level semantic patterns, enabling robust entity matching while maintaining computational efficiency. By leveraging a multi-stage alignment process, EAL iteratively refines alignment predictions, optimizing both precision and recall. Experimental results on benchmark datasets demonstrate the effectiveness and robustness of EAL, which not only achieves superior performance in entity alignment tasks but also provides a lightweight yet powerful solution that reduces reliance on large language models. Full article
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<p>Key message structure for reasoning.</p>
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<p>Main structure of the EAL model, illustrating the integration of the time-event analysis and EAL modules to process logical propagation paths in knowledge graph reasoning.</p>
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<p>Results of entity alignment with complex-event logic.</p>
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25 pages, 34424 KiB  
Article
Resampling Point Clouds Using Series of Local Triangulations
by Vijai Kumar Suriyababu, Cornelis Vuik and Matthias Möller
J. Imaging 2025, 11(2), 49; https://doi.org/10.3390/jimaging11020049 - 8 Feb 2025
Viewed by 616
Abstract
The increasing reliance on 3D scanning and meshless methods highlights the need for algorithms optimized for point-cloud geometry representations in CAE simulations. While voxel-based binning methods are simple, they often compromise geometry and topology, particularly with coarse voxelizations. We propose an algorithm based [...] Read more.
The increasing reliance on 3D scanning and meshless methods highlights the need for algorithms optimized for point-cloud geometry representations in CAE simulations. While voxel-based binning methods are simple, they often compromise geometry and topology, particularly with coarse voxelizations. We propose an algorithm based on a Series of Local Triangulations (SOLT) as an intermediate representation for point clouds, enabling efficient upsampling and downsampling. This robust and straightforward approach preserves the integrity of point clouds, ensuring resampling without feature loss or topological distortions. The proposed techniques integrate seamlessly into existing engineering workflows, avoiding complex optimization or machine learning methods while delivering reliable, high-quality results for a large number of examples. Resampled point clouds produced by our method can be directly used for solving PDEs or as input for surface reconstruction algorithms. We demonstrate the effectiveness of this approach with examples from mechanically sampled point clouds and real-world 3D scans. Full article
(This article belongs to the Special Issue Exploring Challenges and Innovations in 3D Point Cloud Processing)
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<p>Workflow of the overall methodology. Optional modules are highlighted in light orange.</p>
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<p>Point cloud (blue) converted to a Series of Local Triangulations (SOLT) representation. The SOLT is shown in yellow, both with and without edges.</p>
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<p>Different views of an eagle point cloud (from Open3D’s datasets [<a href="#B18-jimaging-11-00049" class="html-bibr">18</a>]). The point cloud (796,825 points) contains intricate features, making it an excellent candidate for evaluating reconstruction algorithms.</p>
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<p>SOLT reconstruction of the eagle point cloud (Time taken: 35.8 s). The SOLT algorithm effectively captures the intricate features of the point cloud while being computationally efficient.</p>
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<p>BPA reconstruction of the eagle point cloud (Time taken: 26.91 min). This method is 62 times slower than the SOLT algorithm, achieving a similar reconstruction quality.</p>
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<p>Poisson reconstruction of the eagle point cloud (Time taken: 87.9 s). This method is 2.46 times slower than the SOLT algorithm, achieving comparable quality.</p>
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<p>Feature distance fields for selected geometries (purple indicates a distance field value of zero).</p>
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<p>Point cloud (blue) meshed using SOLT (yellow), downsampled in two stages (pink and green), and reconstructed using the SOLT representation (purple).</p>
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<p>Point clouds synthesized from the SimJEB dataset. Point cloud (blue) meshed using SOLT (yellow), downsampled in two stages (pink and green), and reconstructed using the SOLT representation (purple).</p>
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<p>A screw geometry resampled using our algorithm (geometry from the Thingi10k dataset).</p>
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<p>A mixture of smooth and sharp geometries with twist-like features (geometries from the Thingi10k dataset).</p>
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<p>Mechanical components from the Thingi10k dataset. Sharp creases were recovered perfectly.</p>
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<p>Selected geometries from the Thingi10k dataset, resampled using our algorithm and reconstructed using a simple Ball-Pivoting Algorithm (BPA) [<a href="#B28-jimaging-11-00049" class="html-bibr">28</a>]. The results demonstrate the uniformity and quality of the reconstructed meshes.</p>
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<p>Histograms showing the triangle area distribution for the reconstructed geometries presented in <a href="#jimaging-11-00049-f013" class="html-fig">Figure 13</a>.</p>
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<p>Histograms showing the triangle area distribution for the reconstructed geometries presented in <a href="#jimaging-11-00049-f013" class="html-fig">Figure 13</a>.</p>
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<p>Input bunny point cloud along with a 5000-point resample produced by [<a href="#B12-jimaging-11-00049" class="html-bibr">12</a>]. These results were provided by the authors.</p>
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<p>Bunny resampled at various sizes using SOLT, along with corresponding sampling times. The results demonstrate that SOLT maintains consistent efficiency and quality as sample size increases, comparable to the algorithms proposed in [<a href="#B12-jimaging-11-00049" class="html-bibr">12</a>].</p>
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<p>Chair reconstruction from input point cloud using the RepKPU workflow (results shared by the authors). The reconstruction contains multiple holes and is of poor quality. For comparison, the SOLT reconstruction of the same chair geometry is shown, demonstrating significantly higher quality and robustness.</p>
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<p>Chair resampled at various sizes using SOLT, along with corresponding sampling times. The results demonstrate that SOLT maintains consistent efficiency and high-quality output as the sample size increases.</p>
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32 pages, 6748 KiB  
Article
Spatial Cognitive Electroencephalogram Network Topological Features Extraction Based on Cross Fuzzy Entropy Network Graph
by Yanhong Zhou, Xulong Liu, Dong Wen, Shuang Xu, Xianglong Wan and Huibin Lu
Symmetry 2025, 17(2), 243; https://doi.org/10.3390/sym17020243 - 6 Feb 2025
Viewed by 453
Abstract
Spatial cognition, a critical component of human cognitive function, can be enhanced through targeted training, such as virtual reality (VR)-based interventions. Recent advances in electroencephalography (EEG)-based functional connectivity analysis have highlighted the importance of network topology features for understanding cognitive processes. In this [...] Read more.
Spatial cognition, a critical component of human cognitive function, can be enhanced through targeted training, such as virtual reality (VR)-based interventions. Recent advances in electroencephalography (EEG)-based functional connectivity analysis have highlighted the importance of network topology features for understanding cognitive processes. In this paper, a framework based on a cross fuzzy entropy network graph (CFENG) is proposed to extract spatial cognitive EEG network topological features. This framework involves calculating the similarity and symmetry between EEG channels using cross fuzzy entropy, constructing weighted directed network graphs, transforming one-dimensional EEG signals into two-dimensional brain functional connectivity networks, and extracting both local and global topological features. The model’s performance is evaluated and interpreted using an XGBoost classifier. Experiments on an EEG dataset from group spatial cognitive training validated the CFENG model. In the Gamma band, the CFENG achieved 97.82% classification accuracy, outperforming existing methods. Notably, the asymmetrically distributed EEG channels Fp1, P8, and Cz contributed most to spatial cognitive signal classification. An analysis after 28 days of training revealed that specific VR games enhanced functional centrality in spatial cognition-related brain regions, reduced information flow path length, and altered information flow symmetry. These findings support the feasibility of VR-based spatial cognitive training from a brain functional connectivity perspective. Full article
(This article belongs to the Special Issue Advances in Symmetry/Asymmetry and Biomedical Engineering)
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<p>General process of feature extraction and classification of spatial cognitive EEG networks.</p>
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<p>Typical task pathways and game scenarios in spatial cognitive training.</p>
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<p>Experimental framework and standardized task sequence for spatial cognition assessment.</p>
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<p>Distribution of EEG electrodes.</p>
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<p>Comparison of classification accuracy for different brain functional connectivity networks.</p>
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<p>Classification accuracy across seven different frequency bands using a 2-s sliding window size.</p>
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<p>Classification accuracy across seven different frequency bands using a 4-s sliding window size.</p>
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<p>Comparison of classification accuracy in the Gamma band for sliding window sizes of 2 s and 4 s. The results indicate no statistically significant difference between the two groups.</p>
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<p>Permutation feature importance and summary plot of EEG channels using SHAP in the Delta frequency band.</p>
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<p>Permutation feature importance and summary plot of EEG channels using SHAP in the Theta frequency band.</p>
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<p>Permutation feature importance and summary plot of EEG channels using SHAP in the Alpha1 frequency band.</p>
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<p>Permutation feature importance and summary plot of EEG channels using SHAP in the Alpha2 frequency band.</p>
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<p>Permutation feature importance and summary plot of EEG channels using SHAP in the Beta1 frequency band.</p>
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<p>Permutation feature importance and summary plot of EEG channels using SHAP in the Beta2 frequency band.</p>
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<p>Permutation feature importance and summary plot of EEG channels using SHAP in the Gamma frequency band.</p>
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<p>Comparison of data distribution in two spatial cognitive EEG tests for five network topology features. The symbols * and **** indicate statistical significance levels (<span class="html-italic">p</span>-values), with * representing <span class="html-italic">p</span> &lt; 0.05 and **** representing <span class="html-italic">p</span> &lt; 0.0001.</p>
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13 pages, 283 KiB  
Article
The Finite Coarse Shape Paths
by Ivan Jelić and Ivančica Mirošević
Mathematics 2025, 13(3), 439; https://doi.org/10.3390/math13030439 - 28 Jan 2025
Viewed by 394
Abstract
In this paper, we introduce the notions of finite coarse shape path and finite coarse shape path connectedness of a topological space. We prove that the solenoid Σ(pn), which is known to be coarse shape path connected but [...] Read more.
In this paper, we introduce the notions of finite coarse shape path and finite coarse shape path connectedness of a topological space. We prove that the solenoid Σ(pn), which is known to be coarse shape path connected but not shape path connected, is not finite coarse shape path connected either. Furthermore, we show that every finite coarse shape path induces an isomorphism between finite coarse shape groups of the topological space at different base points, with some interesting and useful properties. We also show that finite coarse shape groups of the same space, in general, depend on the choice of a base point. Hence, the pointed finite coarse shape type of X,x, in general, depends on the choice of the point x. Finally, we prove that if X is a finite coarse shape path connected paracompact locally compact space, then the pointed finite coarse shape type of X,x does not depend on the choice of the point x. Full article
(This article belongs to the Section A: Algebra and Logic)
25 pages, 477 KiB  
Article
Topology of Locally and Non-Locally Generalized Derivatives
by Dimiter Prodanov
Fractal Fract. 2025, 9(1), 53; https://doi.org/10.3390/fractalfract9010053 - 20 Jan 2025
Viewed by 576
Abstract
This article investigates the continuity of derivatives of real-valued functions from a topological perspective. This is achieved by the characterization of their sets of discontinuity. The same principle is applied to Gateaux derivatives and gradients in Euclidean spaces. This article also introduces a [...] Read more.
This article investigates the continuity of derivatives of real-valued functions from a topological perspective. This is achieved by the characterization of their sets of discontinuity. The same principle is applied to Gateaux derivatives and gradients in Euclidean spaces. This article also introduces a generalization of the derivatives from the perspective of the modulus of continuity and characterizes their sets of discontinuities. There is a need for such generalizations when dealing with physical phenomena, such as fractures, shock waves, turbulence, Brownian motion, etc. Full article
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<p>Neidinger–Bernouli function and its fractional variation. (<b>A</b>)—Original Neidinger construction <math display="inline"><semantics> <mrow> <mi>N</mi> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mn>1</mn> <mo>/</mo> <msqrt> <mn>2</mn> </msqrt> <mo>)</mo> </mrow> <mo>=</mo> <msub> <mi>M</mi> <mrow> <mn>1</mn> <mo>/</mo> <mn>3</mn> </mrow> </msub> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mn>1</mn> <mo>/</mo> <msqrt> <mn>2</mn> </msqrt> <mo>)</mo> </mrow> </mrow> </semantics></math>; (<b>B</b>)—modified construction <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <mrow> <mn>2</mn> <mo>/</mo> <mn>3</mn> </mrow> </msub> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mn>1</mn> <mo>/</mo> <msqrt> <mn>2</mn> </msqrt> <mo>)</mo> </mrow> </mrow> </semantics></math>.</p>
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