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15 pages, 7842 KiB  
Article
Human-Induced Pluripotent Stem Cell-Derived Neural Organoids as a Novel In Vitro Platform for Developmental Neurotoxicity Assessment
by Tsunehiko Hongen, Kenta Sakai, Tomohiro Ito, Xian-Yang Qin and Hideko Sone
Int. J. Mol. Sci. 2024, 25(23), 12523; https://doi.org/10.3390/ijms252312523 - 21 Nov 2024
Viewed by 333
Abstract
There has been a recent drive to replace in vivo studies with in vitro studies in the field of toxicity testing. Therefore, instead of conventional animal or planar cell culture models, there is an urgent need for in vitro systems whose conditions can [...] Read more.
There has been a recent drive to replace in vivo studies with in vitro studies in the field of toxicity testing. Therefore, instead of conventional animal or planar cell culture models, there is an urgent need for in vitro systems whose conditions can be strictly controlled, including cell–cell interactions and sensitivity to low doses of chemicals. Neural organoids generated from human-induced pluripotent stem cells (iPSCs) are a promising in vitro platform for modeling human brain development. In this study, we developed a new tool based on various iPSCs to study and predict chemical-induced toxicity in humans. The model displayed several neurodevelopmental features and showed good reproducibility, comparable to that of previously published models. The results revealed that basic fibroblast growth factor plays a key role in the formation of the embryoid body, as well as complex neural networks and higher-order structures such as layered stacking. Using organoid models, pesticide toxicities were assessed. Cells treated with low concentrations of rotenone underwent apoptosis to a greater extent than those treated with high concentrations of rotenone. Morphological changes associated with the development of neural progenitor cells were observed after exposure to low doses of chlorpyrifos. These findings suggest that the neuronal organoids developed in this study mimic the developmental processes occurring in the brain and nerves and are a useful tool for evaluating drug efficacy, safety, and toxicity. Full article
(This article belongs to the Special Issue Environmental Epigenome and Endocrine Disrupting Chemicals)
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<p>Immunostaining images depicting the effect of bFGF on organoid differentiation at various stages. (<b>A</b>–<b>C</b>) present immunostained images of organoids on days 24, 34, and 50, respectively. (<b>D</b>) presents a magnified view of the upper part of the bFGF-exposed organoid on day 50. Staining included Hoechst staining (in blue) for nuclear labeling, neuron markers (in green) for neuron identification, and phalloidin–rhodamine (in red) for cytoskeletal visualization. Images were captured using Olympus FV10-ASW (10× objective; Scale bar, 200 μm).</p>
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<p>Forebrain organoid differentiation protocol. Cells were seeded at a density of 9000 cells per well, and embryoid bodies were allowed to form until day 4 of culture. The cells were then naturally induced in SMAD (Sma and Mad related protein) inhibitor-containing medium until day 15, differentiated into forebrain-type organoids from day 16, and cultured to maturity from days 22 to 29. Maintenance culture was continued until day 50.</p>
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<p>Fluorescence immunostaining of forebrain-type organoids on day 50 of culture. (<b>A</b>) Internal structure of the organoids on day 50 of culture, as observed using a confocal microscope Z-stack with a 25× objective. (<b>B</b>) Magnified image using a 40× objective. (<b>C</b>–<b>E</b>) Localization of cells by each marker. Cell nuclei (blue), neurons (green), and cytoskeleton (red) are shown (4× objective; Scale bar, 100 μm. (<b>F</b>) A forebrain organoid stained with the glial cell marker GFAP (red) and neurons (green). (<b>F</b>,<b>G</b>) An enlarged view of the upper part (4× objective; Scale bar, 200 μm).</p>
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<p>RNA sequencing analysis of human-induced pluripotent stem cells exposed to rotenone. (<b>A</b>) Heatmap illustrating the differential gene expression between control and rotenone-treated samples. Genes are ranked based on their standard deviation across all samples, and the top 1000 genes are used for hierarchical clustering analysis. Details of which genes are upregulated or downregulated in the control versus rotenone treatment are provided in the table within the <a href="#app1-ijms-25-12523" class="html-app">Supplemental Materials</a>. (<b>B</b>) The data shows network interactions in the KEGG signaling pathways. In particular, focal adhesion and the neuroactive ligand–receptor interactions interact largely the others. (<b>C</b>) Analysis of gene pathways with high variability for up- and down-regulation of gene expressions.</p>
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<p>RNA sequencing analysis of human-induced pluripotent stem cells exposed to rotenone. (<b>A</b>) Heatmap illustrating the differential gene expression between control and rotenone-treated samples. Genes are ranked based on their standard deviation across all samples, and the top 1000 genes are used for hierarchical clustering analysis. Details of which genes are upregulated or downregulated in the control versus rotenone treatment are provided in the table within the <a href="#app1-ijms-25-12523" class="html-app">Supplemental Materials</a>. (<b>B</b>) The data shows network interactions in the KEGG signaling pathways. In particular, focal adhesion and the neuroactive ligand–receptor interactions interact largely the others. (<b>C</b>) Analysis of gene pathways with high variability for up- and down-regulation of gene expressions.</p>
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<p>Typical morphological changes in forebrain organoids induced by the pesticides rotenone and chlorpyrifos. (<b>A</b>,<b>B</b>) Rotenone. (<b>C</b>,<b>D</b>) Chlorpyrifos. Morphological changes and respective size changes from day 1 to day 11 of incubation. ((<b>A</b>,<b>C</b>) 4× objective; Scale bar, 2.0 mm). Experiments were performed independently in triplicate or quadruplicate. Asterisks indicate significant differences between the exposed and control groups <span class="html-italic">p</span> &lt; 0.05 = *; <span class="html-italic">p</span> &lt; 0.01 = **. N = 4.</p>
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<p>Typical morphological changes in 29-day pre-brain organoids in culture induced by the pesticides rotenone and chlorpyrifos. (<b>A</b>,<b>B</b>) Rotenone. (<b>C</b>,<b>D</b>) Chlorpyrifos. Morphological changes and respective size changes on day 29 of incubation. ((<b>A</b>,<b>C</b>); 4× objective; Scale bar, 2.0 mm). Experiments were performed independently in triplicate or quadruplicate. N = 4.</p>
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<p>Immunofluorescence images of forebrain-type organoids at 29 days in culture to visualize the effects of chemical substances on neural cell development. (<b>A</b>) Internal structure of forebrain-type organoids in the control group, captured in two fields of view (10× and 20× objective). The red boxes indicate nerve dense foci, while the white boxes indicate winding structures. (<b>B</b>) Internal structure of organoids exposed to 10 μM rotenone. (<b>C</b>) Internal structure of organoids exposed to 10 μM chlorpyrifos. Cell nuclei (blue), neurons (green), and glial cells (red) are shown (<span class="html-italic">n</span> = 3; 10× objective; scale bar, 200 μm and 20× objective; scale bar, 100 μm).</p>
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<p>The morphological characteristics of the forebrain organoids identified in <a href="#ijms-25-12523-f007" class="html-fig">Figure 7</a> were evaluated. (<b>A</b>) 1. Neurites were scored as 1 point; 2. nerve dense foci as 2 points; and 3. The red dotted lines indicate three points of the winding structures (scale bar, 2.0 mm). (<b>B</b>) Morphological evaluation scores (<span class="html-italic">n</span> = 4).</p>
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<p>Gene expression analysis of forebrain organoids exposed to rotenone and chlorpyrifos. (<b>A</b>) Changes in the expression levels of neuronal marker genes (MAP2, SOX2, PAX6) and apoptosis-related marker genes (ADM, CASP3, CASP7) following exposure to various concentrations of rotenone. (<b>B</b>) Changes in the expression levels of neuronal and apoptosis marker genes following exposure to chlorpyrifos. Results are presented as the mean ± SD (<span class="html-italic">n</span> = 3). Asterisks indicate <span class="html-italic">p</span>-values based on multiple comparisons via two-way analysis of variance <span class="html-italic">p</span> &lt; 0.05 = *; <span class="html-italic">p</span> &lt; 0.01 = **. The red dotted lines indicate the control value.</p>
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22 pages, 24817 KiB  
Article
Construction of Mining Subsidence Basin and Inversion of Predicted Subsidence Parameters Based on UAV Photogrammetry Products Considering Horizontal Displacement
by Jinqi Zhao, Yufen Niu, Zhengpei Zhou, Zhong Lu, Zhimou Wang, Zhaojiang Zhang, Yiyao Li and Ziheng Ju
Remote Sens. 2024, 16(22), 4283; https://doi.org/10.3390/rs16224283 - 17 Nov 2024
Viewed by 299
Abstract
Constructing high-precision subsidence basins is of paramount importance for mining subsidence monitoring. Traditional unmanned aerial vehicle (UAV) photogrammetry techniques typically construct subsidence basins by directly differencing digital elevation models (DEMs) from different monitoring periods. However, this method often neglects the influence of horizontal [...] Read more.
Constructing high-precision subsidence basins is of paramount importance for mining subsidence monitoring. Traditional unmanned aerial vehicle (UAV) photogrammetry techniques typically construct subsidence basins by directly differencing digital elevation models (DEMs) from different monitoring periods. However, this method often neglects the influence of horizontal displacement on the accuracy of the subsidence basin. Taking a mining area in Ordos, Inner Mongolia, as an example, this study employed the normalized cross-correlation (NCC) matching algorithm to extract horizontal displacement information between two epochs of a digital orthophoto map (DOM) and subsequently corrected the horizontal position of the second-epoch DEM. This ensured that the planar positions of ground feature points remained consistent in the DEM before and after subsidence. Based on this, the vertical displacement in the subsidence area (the subsidence basin) was obtained via DEM differencing, and the parameters of the post-correction subsidence basin were inverted using the probability integral method (PIM). The experimental results indicate that (1) the horizontal displacement was influenced by the gully topography, causing the displacement within the working face to be segmented on both sides of the gully; (2) the influence of the terrain on the subsidence basin was significantly reduced after correction; (3) the post-correction surface subsidence curve was smoother than the pre-correction curve, with abrupt error effects markedly diminished; (4) the accuracy of the post-correction subsidence basin increased by 43.12% compared with the total station data; and (5) comparing the measured horizontal displacement curve with that derived using the probability integral method revealed that the horizontal displacement on the side of an old goaf adjacent to the newly excavated working face shifted toward the advancing direction of the new working face as mining progressed. This study provides a novel approach and insights for using low-cost UAVs to construct high-precision subsidence basins. Full article
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<p>Schematic diagram of the study area location. (<b>a</b>) Map of China; (<b>b</b>) DEM of Ordos; (<b>c</b>) study area.</p>
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<p>Technical flow chart of this research.</p>
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<p>Schematic diagram of the DEM correction process.</p>
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<p>(<b>a</b>) East–west displacement; (<b>b</b>) north–south displacement.</p>
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<p>Illustration of the relationship between horizontal displacement and topography. (<b>a</b>,<b>b</b>) are cross-sectional views of profile A-A′; (<b>c</b>,<b>d</b>) are cross-sectional views of profile B-B′.</p>
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<p>Horizontal displacement in gully topography. (<b>a</b>) A-A′ cross-section; (<b>b</b>) local displacement field.</p>
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<p>Subsidence basin. (<b>a</b>) Pre-correction subsidence basin; (<b>b</b>) post-correction subsidence basin.</p>
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<p>Local maps of areas I and II. (<b>a</b>) Magnified view of area I pre-correction; (<b>b</b>) magnified view of area I post-correction; (<b>c</b>) magnified view of area II pre-correction; (<b>d</b>) magnified view of area II post-correction; (<b>e</b>) 1-1′ cross-section; (<b>f</b>) 2-2′ cross-section.</p>
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<p>Subsidence curves of pre-correction and post-correction. (<b>a</b>) A-A′ cross-section; (<b>b</b>) C-C′ cross-section.</p>
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<p>Inverted subsidence basin.</p>
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<p>Measured subsidence basin.</p>
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<p>(<b>a</b>) Strike main profile; (<b>b</b>) dip main profile.</p>
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<p>Horizontal displacement of strike main profile. (<b>a</b>) Strike main profile; (<b>b</b>) partial enlarged detail.</p>
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<p>Horizontal displacement of dip main profile. (<b>a</b>) Dip main profile; (<b>b</b>) partial enlarged detail.</p>
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<p>Horizontal displacement error.</p>
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<p>Statistical chart of residuals for subsidence basin.</p>
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<p>Statistical chart of strike residuals.</p>
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<p>Statistical chart of dip residuals.</p>
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<p>Statistical analysis of errors in subsidence basin.</p>
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27 pages, 5704 KiB  
Review
Viewpoints Concerning Crystal Structure from Recent Reports on Schiff Base Compounds and Their Metal Complexes
by Takashiro Akitsu, Daisuke Nakane and Barbara Miroslaw
Symmetry 2024, 16(11), 1525; https://doi.org/10.3390/sym16111525 - 14 Nov 2024
Viewed by 650
Abstract
Schiff bases are organic compounds that are often used as ligands in metal complexes. In addition to the C=N double bond, which is characteristic of Schiff bases, intermolecular hydrogen bonds are frequently observed in both the twisting of planar substituents in organic compounds [...] Read more.
Schiff bases are organic compounds that are often used as ligands in metal complexes. In addition to the C=N double bond, which is characteristic of Schiff bases, intermolecular hydrogen bonds are frequently observed in both the twisting of planar substituents in organic compounds and the geometric structure of the coordination environment in metal complexes. The results of the crystal structure analyses are stored in databases, which can be used to assess three-dimensional structures. To examine the important structural aspects for novel molecular and material designs, this review examines the important discussion of crystal structure “features” from various viewpoints based on papers on Schiff bases and Schiff base metal complexes from recent years. Full article
(This article belongs to the Section Chemistry: Symmetry/Asymmetry)
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<p>(<b>Left</b>) A Schiff base compound with structurally integrated aspects. Two-ring moieties can rotate around the binding single bonds. (<b>Right</b>) Model of a distorted octahedral Fe(II) complex incorporating Schiff base ligands acting as a bidentate chelate and two Cl<sup>-</sup> ligands in <span class="html-italic">cis</span>-sites.</p>
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<p>(<b>Left</b>) Molecular structure of a Schiff base compound [<a href="#B18-symmetry-16-01525" class="html-bibr">18</a>], denoted by an imine C=N bond and two planar ring moieties. (<b>Right</b>) The corresponding ORTEP drawing.</p>
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<p>Blue and yellow atoms in C<sub>17</sub>H<sub>26</sub>N<sub>2</sub>S<sub>2</sub> [<a href="#B19-symmetry-16-01525" class="html-bibr">19</a>] with a long alkyl chain denote N and S atoms, respectively.</p>
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<p>Crystal packing of a Schiff base compound [<a href="#B20-symmetry-16-01525" class="html-bibr">20</a>] from Hirshfeld surface analysis for one molecule only.</p>
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<p>(<b>Left</b>) Part of the Schiff base moiety discussed is its double bond distances (denoted as C=N) and torsion angles of the C-C-N-C bonds [<a href="#B21-symmetry-16-01525" class="html-bibr">21</a>]. (<b>Right</b>) Crystal packing of the compound (C<sub>14</sub>H<sub>17</sub>NO<sub>2</sub>) in the space group <span class="html-italic">P</span>2<sub>1</sub>.</p>
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<p>Intramolecular hydrogen bond of a Schiff base compound [<a href="#B22-symmetry-16-01525" class="html-bibr">22</a>] (part of the molecule is omitted for clarity).</p>
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<p>Top view of the compound [<a href="#B23-symmetry-16-01525" class="html-bibr">23</a>].</p>
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<p>Crystal packing of the Ni(II) complex with an unsymmetrical ligand (Ni···Ni = 3.3305(9) Å). White—H; black—C; green—Ni; red—O; blue—O; yellow—S [<a href="#B26-symmetry-16-01525" class="html-bibr">26</a>].</p>
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<p>Cu(II) complex with a tridentate amino acid Schiff base ligand [<a href="#B44-symmetry-16-01525" class="html-bibr">44</a>] with various structural aspects mentioned in <a href="#symmetry-16-01525-f001" class="html-fig">Figure 1</a> marked.</p>
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<p>(<b>Left</b>) <span class="html-italic">E</span>-isomer and (<b>Right</b>) <span class="html-italic">Z</span>-isomer of Cu(II) complexes with a tridentate Schiff base ligand [<a href="#B48-symmetry-16-01525" class="html-bibr">48</a>]. The basal planes of the distorted square-based pyramidal coordination are also indicated (Yellow—Cu, Bule—N, and Red—O atoms).</p>
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<p>Crystal structure of a dinuclear copper(II) complex [<a href="#B51-symmetry-16-01525" class="html-bibr">51</a>].</p>
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<p>Simple crystal packing of chiral self-assembly of Schiff base compounds (not as continuous porous structures) [<a href="#B55-symmetry-16-01525" class="html-bibr">55</a>].</p>
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<p>Crystal packing of the compound showing predominant hydrogen bonds as light blue lines [<a href="#B59-symmetry-16-01525" class="html-bibr">59</a>].</p>
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<p>(<b>Left</b>) Schiff base with CH=N imine, (<b>Right</b>) “reduced” Schiff base with a CH<sub>2</sub>–NH moiety; both are potentially ready for hydrogen bonds.</p>
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<p>The red circle highlights the R<sub>2</sub><sup>2</sup>(8) ring motifs formed by two N–H···S hydrogen bonds.</p>
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<p>The red triangle highlights the potential tautomerism between the keto-amine form (N–H···O hydrogen bond) and phenol-imine (N···H–O hydrogen bond) form [<a href="#B62-symmetry-16-01525" class="html-bibr">62</a>]. The pyrene moiety was omitted for clarity.</p>
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<p>(<b>Left</b>) Molecular structure of C<sub>10</sub>H<sub>14</sub>N<sub>4</sub>S with imine C=N bond (red circle) and potentially tautomeric moiety (blue circle); (<b>Right</b>) two-dimensional fingerprint plots (all interactions and N–H···H–N interactions) of the compounds [<a href="#B25-symmetry-16-01525" class="html-bibr">25</a>].</p>
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<p>Crystal packing of host–guest inclusion in the metal–organic framework [<a href="#B81-symmetry-16-01525" class="html-bibr">81</a>].</p>
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19 pages, 11699 KiB  
Article
A Planar Feature-Preserving Texture Defragmentation Method for 3D Urban Building Models
by Beining Liu, Wenxuan Liu, Zhen Lei, Fan Zhang, Xianfeng Huang and Tarek M. Awwad
Remote Sens. 2024, 16(22), 4154; https://doi.org/10.3390/rs16224154 - 7 Nov 2024
Viewed by 354
Abstract
Oblique photogrammetry-based 3D modeling is widely used for large-scale urban reconstruction. However, textures generated with photogrammetric techniques often exhibit scattered and irregular characteristics, which lead to significant challenges with texture seams and UV map discontinuities, increasing storage requirements and affecting rendering quality. In [...] Read more.
Oblique photogrammetry-based 3D modeling is widely used for large-scale urban reconstruction. However, textures generated with photogrammetric techniques often exhibit scattered and irregular characteristics, which lead to significant challenges with texture seams and UV map discontinuities, increasing storage requirements and affecting rendering quality. In this paper, we propose a planar feature-preserving texture defragmentation method designed specifically for urban building models. Our approach leverages the multi-planar topology of buildings to optimize texture merging and reduce fragmentation. The proposed approach is composed of three main stages: the extraction of planar features from texture fragments; the employment of these planar elements as guiding constraints for merging adjacent texture fragments within a two-dimensional texture space; and an enhanced texture-packing algorithm designed for more regular texture charts to systematically generate refined texture atlas. Experiments on various urban building models demonstrate that our method significantly improves texture continuity and storage efficiency compared to traditional approaches, with both quantitative and qualitative validation. Full article
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<p>Pipeline of the proposed method. We first identify patch structures on the mesh based on texture charts, using them as primitives for plane detection. Subsequently, we iteratively merge and optimize charts constrained by planes. Finally, we tightly pack the relatively regular texture charts into a new texture atlas.</p>
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<p>Association between vertices at seams and their corresponding 2D texture coordinates in (<b>a</b>) the mesh, (<b>b</b>) its corresponding texture mapping, and (<b>c</b>) the textured model.</p>
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<p>Examples of common issues in plane detection using traditional methods. (<b>a</b>) Jagged borders. (<b>b</b>) Elongated strip-like regions. (<b>c</b>) Small components with smooth curvature.</p>
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<p>Improvement of common issues in plane detection using our methods. (<b>a</b>) Jagged borders. (<b>b</b>) Elongated strip-like regions. (<b>c</b>) Small components with smooth curvature.</p>
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<p>Texture chart alignment diagram.</p>
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<p>Texture merging optimization diagram.</p>
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<p>Square Tetris packing strategy.</p>
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<p>Real-world three-dimensional scene data used for experiments.</p>
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<p>Building models with texture mapping. (<b>a</b>) Residential building. (<b>b</b>) Factory workshop. (<b>c</b>) Hotel.</p>
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<p>Texture maps of building models stored in the form of texture images. (<b>a</b>) Residential building. (<b>b</b>) Factory workshop. (<b>c</b>) Hotel.</p>
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<p>Visualization of the workflow results. (<b>a</b>) Shaded models of various building structures, showcasing their geometric characteristics. (<b>b</b>) Distribution of original texture patches on the 3D models, where different colors represent distinct texture charts. (<b>c</b>) Results of plane detection, with different colors indicating different planar regions. (<b>d</b>) Final results of texture merge under plane constraints.</p>
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<p>Local details of planar detection and merging results. (<b>a</b>) Plane detection of localized details including the intersection of eaves, small roof components, and facade windows, among others. (<b>b</b>) Local details of the texture merging results under plane constraints.</p>
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<p>Output results of the texture atlas generated by our method. (<b>a</b>) Residential building. (<b>b</b>) Factory workshop. (<b>c</b>) Hotel.</p>
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<p>Output results of the texture atlas generated by the M-method. (<b>a</b>) Residential building. (<b>b</b>) Factory workshop. (<b>c</b>) Hotel.</p>
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<p>Rendering comparison. (<b>a</b>) The original model of the factory. (<b>b</b>) The model after texture merging.</p>
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<p>A comparative analysis of the number of texture charts between the M-method and our approach.</p>
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<p>A comparative analysis of the length of texture seams between the M-method and our approach.</p>
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<p>A comparative analysis of the degree of texture distortion between the M-method and our approach.</p>
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<p>A comparative analysis of the texture size between the M-method and our approach.</p>
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<p>A comparative analysis of the vertex replication coefficient before and after texture defragmentation methods.</p>
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20 pages, 7804 KiB  
Article
Study on the Identification Method of Planar Geological Structures in Coal Mines Using Ground-Penetrating Radar
by Jialin Liu, Xiaosong Tang, Feng Yang, Xu Qiao, Fanruo Li, Suping Peng, Xinxin Huang, Yuanjin Fang and Maoxuan Xu
Remote Sens. 2024, 16(21), 3990; https://doi.org/10.3390/rs16213990 - 27 Oct 2024
Viewed by 570
Abstract
The underground detection environment in coal mines is complex, with numerous interference sources. Traditional ground-penetrating radar (GPR) methods suffer from limited detection range, high noise levels, and weak deep signals, making it extremely difficult to accurately identify geological structures without stable feature feedback. [...] Read more.
The underground detection environment in coal mines is complex, with numerous interference sources. Traditional ground-penetrating radar (GPR) methods suffer from limited detection range, high noise levels, and weak deep signals, making it extremely difficult to accurately identify geological structures without stable feature feedback. During research, it was found that the detection energy of the same target significantly changes with the antenna direction. Based on this phenomenon, this paper proposes a geological radar advanced detection method using spatial scanning. This method overcomes constraints imposed by the underground coal mine environment on detection equipment, enhancing both detection range and accuracy compared to traditional approaches. Experiments using this method revealed pea-shaped response characteristics of planar geological structures in radar images, and the mechanisms behind their formation were analyzed. Additionally, this paper studied the changes in response characteristics under changes in target inclination, providing a basis for understanding the spatial distribution of geological structures. Finally, application experiments in underground coal mine environments explored the practical potential of this method. Results indicate that, compared to drilling data, this method achieves identification accuracies of 91.88%, 90.42%, and 78.72% for the depth and spatial extent of geological structures, providing effective technical support for coal mining operations. Full article
(This article belongs to the Special Issue Advanced Ground-Penetrating Radar (GPR) Technologies and Applications)
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<p>Advanced detection schematic of the coal mine working face.</p>
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<p>Schematic diagram of the application of the traditional GPR advanced detection method in the coal mine working face.</p>
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<p>Schematic diagram of spatial scanning detection using GPR at the coal mine working face.</p>
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<p>Schematic diagram of GPR horizontal and vertical scanning detection of the coal mine working face and the corresponding detection results.</p>
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<p>Schematic diagram of GPR horizontal and vertical scanning detection of the coal mine working face and the corresponding detection results.</p>
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<p>Diagram of spatial scan detection experiment using GPR.</p>
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<p>Schematic diagram of GPR horizontal scanning detection of the coal mine working face and the corresponding detection results.</p>
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<p>Antenna directional radiation pattern diagram.</p>
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<p>Experimental schematic of tilted target detection in GPR.</p>
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<p>Target detection data waveform plot.</p>
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<p>Schematic diagram of the application experiment in the retreat mining area of a coal mine in Hebei Province, China.</p>
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<p>Schematic diagram of the application experiment detection results in an underground coal mine environment (the locations of data anomalies are marked with red dotted box).</p>
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<p>Schematic diagram of the application experiment detection results in an underground coal mine environment (the locations of data anomalies are marked with red dotted box).</p>
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<p>Schematic diagram of the horizontal scanning results corresponding to a vertical rotation angle of 0°.</p>
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<p>Schematic diagram of coal seam distribution in the retreat mining area.</p>
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13 pages, 2959 KiB  
Article
β-Yb2CdSb2—A Complex Non-Centrosymmetric Zintl Polymorph
by Spencer R. Watts, Larissa Najera, Michael O. Ogunbunmi, Svilen Bobev and Sviatoslav Baranets
Crystals 2024, 14(11), 920; https://doi.org/10.3390/cryst14110920 - 25 Oct 2024
Viewed by 691
Abstract
The ternary Zintl phase, Yb2CdSb2, was discovered to exist in two different polymorphic forms. In addition to the orthorhombic α-Yb2CdSb2 (space group Cmc21) known for its excellent thermoelectric properties, we present the synthesis [...] Read more.
The ternary Zintl phase, Yb2CdSb2, was discovered to exist in two different polymorphic forms. In addition to the orthorhombic α-Yb2CdSb2 (space group Cmc21) known for its excellent thermoelectric properties, we present the synthesis and characterization of the crystal and electronic structure of its monoclinic variant, β-Yb2CdSb2. Structural characterization was performed with the single-crystal X-ray diffraction method. β-Yb2CdSb2 crystallizes in a monoclinic crystal system with the non-centrosymmetric space group Cm (Z = 33, a = 81.801(5) Å, b = 4.6186(3) Å, c = 12.6742(7) Å, β = 93.0610(10)°) and constitutes a new structure type. The complex crystal structure of β-Yb2CdSb2 contrasts with the previously studied β-Ca2CdPn2 (Pn = P, As, Sb) polymorphs, although it shares similar structural features. It consists of three different layers, made of corner-sharing [CdSb4] tetrahedra and stacked in the ABC sequence. The layers are interconnected via [CdSb3] trigonal planar units. Multiple Yb and Cd atomic sites exhibit partial occupancy, resulting in extensive structural disorder. Valence electron partitioning within the Zintl–Klemm formalism yields the formulation (Yb2+)1.98(Cd2+)1.01(Sb3−)2(h+)0.02, highlighting the nearly charge-balanced composition. Detailed electronic structure calculations reveal the closed band gap and presumably semimetallic nature of β-Yb2CdSb2 with the band structure features hinting at potential topological properties. Full article
(This article belongs to the Special Issue Crystalline Materials: Polymorphism)
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<p>Ternary Yb−Cd−Sb compositional diagram. The newly identified Yb<sub>2</sub>CdSb<sub>2</sub> polymorph is identified as a red star. Known binary and ternary phases are indicated as well. Note that Yb<sub>14</sub>CdSb<sub>11</sub> and Yb<sub>10.5</sub>Cd<sub>0.5</sub>Sb<sub>9</sub> have not yet been reported.</p>
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<p>Crystal structures of β-Yb<sub>2</sub>CdSb<sub>2</sub> (<b>a</b>), β-Ca<sub>2</sub>CdSb<sub>2</sub> (<b>b</b>), β-Ca<sub>2</sub>CdAs<sub>2</sub> (<b>c</b>), and α-Yb<sub>2</sub>CdSb<sub>2</sub> (<b>d</b>) viewed along the <span class="html-italic">b</span>-axis. The unit cell of β-Yb<sub>2</sub>CdSb<sub>2</sub> is doubled along the <span class="html-italic">c</span>-axis for clarity. The Ca and Yb atoms are drawn as dark gray, Cd atoms are green, and <span class="html-italic">Pn</span> = Sb/As atoms are blue-gray. [Cd<span class="html-italic">Pn</span><sub>4</sub>] tetrahedral units are drawn in dark green. The unit cells are outlined. Interatomic Cd–Sb contacts exceeding 3.10 Å are not displayed.</p>
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<p>The representation of the β-Yb<sub>2</sub>CdSb<sub>2</sub> structure with the labeled ABC layers. The unit cell of β-Yb<sub>2</sub>CdSb<sub>2</sub> is doubled along the <span class="html-italic">c</span>-axis. Cd atoms with less than 50% occupancy are avoided for clarity (<b>a</b>). Close-up view of the A layer in β-Yb<sub>2</sub>CdSb<sub>2</sub> (<b>b</b>), <sub>∞</sub><sup>2</sup>[CdSb<sub>2</sub>]<sup>4–</sup> layer in β-Ca<sub>2</sub>CdSb<sub>2</sub> (<b>c</b>), and [Cd<sub>3</sub>Sb<sub>10</sub>] units composing B/C layers (<b>d</b>). Typical six-coordinated octahedral coordination environment of [YbSb<sub>6</sub>] units (<b>e</b>) and five-coordinated square pyramidal [YbSb<sub>5</sub>] units (<b>f</b>). Completeness of the spheres visualizes SOFs. Similar structural units in β-Yb<sub>2</sub>CdSb<sub>2</sub> and β-Ca<sub>2</sub>CdSb<sub>2</sub> are highlighted by red tetrahedra. The color code is the same as in <a href="#crystals-14-00920-f002" class="html-fig">Figure 2</a>.</p>
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<p>Calculated (<b>a</b>) band structure, (<b>b</b>) total (DOS) density of states, and partial (PDOS) density of states for (<b>d</b>) Yb, (<b>e</b>) Cd, and (<b>f</b>) Sb for Yb<sub>2</sub>CdSb<sub>2</sub>. An enlarged view of the band structure at the Fermi level is provided in (<b>c</b>). The Fermi level is the energy reference at 0 eV. The second dashed line at 0.08 eV indicates a 2-electron shift per unit cell.</p>
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29 pages, 6572 KiB  
Article
Robust Parking Space Recognition Approach Based on Tightly Coupled Polarized Lidar and Pre-Integration IMU
by Jialiang Chen, Fei Li, Xiaohui Liu and Yuelin Yuan
Appl. Sci. 2024, 14(20), 9181; https://doi.org/10.3390/app14209181 - 10 Oct 2024
Viewed by 587
Abstract
Improving the accuracy of parking space recognition is crucial in the fields for Automated Valet Parking (AVP) of autonomous driving. In AVP, accurate free space recognition significantly impacts the safety and comfort of both the vehicles and drivers. To enhance parking space recognition [...] Read more.
Improving the accuracy of parking space recognition is crucial in the fields for Automated Valet Parking (AVP) of autonomous driving. In AVP, accurate free space recognition significantly impacts the safety and comfort of both the vehicles and drivers. To enhance parking space recognition and annotation in unknown environments, this paper proposes an automatic parking space annotation approach with tight coupling of Lidar and Inertial Measurement Unit (IMU). First, the pose of the Lidar frame was tightly coupled with high-frequency IMU data to compensate for vehicle motion, reducing its impact on the pose transformation of the Lidar point cloud. Next, simultaneous localization and mapping (SLAM) were performed using the compensated Lidar frame. By extracting two-dimensional polarized edge features and planar features from the three-dimensional Lidar point cloud, a polarized Lidar odometry was constructed. The polarized Lidar odometry factor and loop closure factor were jointly optimized in the iSAM2. Finally, the pitch angle of the constructed local map was evaluated to filter out ground points, and the regions of interest (ROI) were projected onto a grid map. The free space between adjacent vehicle point clouds was assessed on the grid map using convex hull detection and straight-line fitting. The experiments were conducted on both local and open datasets. The proposed method achieved an average precision and recall of 98.89% and 98.79% on the local dataset, respectively; it also achieved 97.08% and 99.40% on the nuScenes dataset. And it reduced storage usage by 48.38% while ensuring running time. Comparative experiments on open datasets show that the proposed method can adapt to various scenarios and exhibits strong robustness. Full article
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<p>Example of parking space recognition. (<b>a</b>) Parking space corner points detection and parking space feature extraction for automatic valet parking [<a href="#B2-applsci-14-09181" class="html-bibr">2</a>]; (<b>b</b>) Parking space recognition and parking lot mapping based on Lidar [<a href="#B3-applsci-14-09181" class="html-bibr">3</a>].</p>
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<p>Comparison between image vision and Lidar vision, data from nuScenes [<a href="#B15-applsci-14-09181" class="html-bibr">15</a>]. (<b>a</b>) Image vision in a night scene; (<b>b</b>) Lidar vision at the same time and place; (<b>c</b>) Superposition of image vision and laser vision.</p>
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<p>Modern ecological parking lots where parking lines cannot be detected. (<b>a</b>) Top-view image of a parking lot; (<b>b</b>) Image of an ecological parking lot.</p>
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<p>Flow chart of parking space automatic recognition method.</p>
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<p>Schematic diagram illustrating posture compensation with tightly coupled Lidar and IMU.</p>
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<p>Schematic diagram of polarized Lidar odometry and loop closure.</p>
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<p>Flow chart of polarized Lidar odometry.</p>
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<p>Flow chart of loop closure.</p>
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<p>Schematic diagram of the vertical angle evaluation method.</p>
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<p>Schematic diagram of the barrier grid marking method based on erosion and dilation.</p>
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<p>Flow chart of obstacle vehicle detection and vacancy annotation.</p>
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<p>Parking slots classification (based on grid projection). (<b>a</b>) Perpendicular parking space; (<b>b</b>) Angled parking space; (<b>c</b>) Parallel parking space.</p>
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<p>Diagram of parking space recognition and annotation. (<b>a</b>) Annotation diagram of perpendicular parking space; (<b>b</b>) Annotation diagram of angled parking space; (<b>c</b>) Annotation diagram of parallel parking space.</p>
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<p>Schematic diagram of parking slot types and actual arrangements in local data. (<b>a</b>) Perpendicular parking slots; (<b>b</b>) Arrangement of perpendicular parking slots; (<b>c</b>) Parallel parking slots; (<b>d</b>) Arrangement of parallel parking slots; (<b>e</b>) Angled parking slots; (<b>f</b>) Arrangement of angled parking slots.</p>
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<p>Schematic diagram of parking slot types and actual arrangements in local data. (<b>a</b>) Perpendicular parking slots; (<b>b</b>) Arrangement of perpendicular parking slots; (<b>c</b>) Parallel parking slots; (<b>d</b>) Arrangement of parallel parking slots; (<b>e</b>) Angled parking slots; (<b>f</b>) Arrangement of angled parking slots.</p>
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<p>Examples of parking scenes in nuScenes [<a href="#B15-applsci-14-09181" class="html-bibr">15</a>]. (<b>a</b>) A parking lot in Queenstown, Singapore; (<b>b</b>) A on-street parking area at Boston Seaport.</p>
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<p>3D point cloud map of a test scene and ground filtering of the ROI. (<b>a</b>) 3D point cloud map of a test scene; (<b>b</b>) 3D point cloud map of a test scene with an ROI box; (<b>c</b>) Before filtering out ground points in the ROI; (<b>d</b>) After filtering out ground points in the ROI.</p>
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<p>Schematic diagram of the annotation for obstacle vehicles and parking spaces. (<b>a</b>) Perpendicular obstacle vehicles and perpendicular parking spaces; (<b>b</b>) Parallel obstacle vehicles and parallel parking spaces. “0” recognized the classification label of perpendicular parking mode; And “1” represented horizontal parking mode.</p>
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<p>Visualization diagram of free space detection. (<b>a</b>) Polarized matrix visualization of the proposed algorithm in the scene from <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>a. Different colors represent different depth values. (<b>b</b>) Free space detection visualization of the proposed algorithm in the scene from <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>a: The red rectangle denotes the ROI, the yellow indicates free space meeting the size constraints of the ego vehicle, and the green represents the non-compliant workshop area. (<b>c</b>) Free space detection visualization of the method in reference [<a href="#B19-applsci-14-09181" class="html-bibr">19</a>] in the scene from <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>a: The green rectangle denotes obstacle vehicles, and the yellow represents free space. (<b>d</b>) Lane line binarization schematic of the method in reference [<a href="#B3-applsci-14-09181" class="html-bibr">3</a>] under weak texture conditions, corresponding to <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>a: The red circle denotes lane line texture information. The red circle highlights subtle lane line texture under weak lighting conditions, which may be difficult to discern due to minimal pixel intensity differences. (<b>e</b>) Lane line binarization schematic of the method in reference [<a href="#B3-applsci-14-09181" class="html-bibr">3</a>] under clear texture but subtle pixel differences due to overexposure, corresponding to <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>b.</p>
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<p>Visualization diagram of free space detection. (<b>a</b>) Polarized matrix visualization of the proposed algorithm in the scene from <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>a. Different colors represent different depth values. (<b>b</b>) Free space detection visualization of the proposed algorithm in the scene from <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>a: The red rectangle denotes the ROI, the yellow indicates free space meeting the size constraints of the ego vehicle, and the green represents the non-compliant workshop area. (<b>c</b>) Free space detection visualization of the method in reference [<a href="#B19-applsci-14-09181" class="html-bibr">19</a>] in the scene from <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>a: The green rectangle denotes obstacle vehicles, and the yellow represents free space. (<b>d</b>) Lane line binarization schematic of the method in reference [<a href="#B3-applsci-14-09181" class="html-bibr">3</a>] under weak texture conditions, corresponding to <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>a: The red circle denotes lane line texture information. The red circle highlights subtle lane line texture under weak lighting conditions, which may be difficult to discern due to minimal pixel intensity differences. (<b>e</b>) Lane line binarization schematic of the method in reference [<a href="#B3-applsci-14-09181" class="html-bibr">3</a>] under clear texture but subtle pixel differences due to overexposure, corresponding to <a href="#applsci-14-09181-f015" class="html-fig">Figure 15</a>b.</p>
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<p>Some parking spaces in the nuScenes [<a href="#B15-applsci-14-09181" class="html-bibr">15</a>] dataset have curbstones next to them.</p>
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<p>Some parking spaces in the nuScenes [<a href="#B15-applsci-14-09181" class="html-bibr">15</a>] dataset do not have line corners, or the parking space lines are unclear.</p>
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21 pages, 10278 KiB  
Article
Three-Dimensional Reconstruction of Zebra Crossings in Vehicle-Mounted LiDAR Point Clouds
by Zhenfeng Zhao, Shu Gan, Bo Xiao, Xinpeng Wang and Chong Liu
Remote Sens. 2024, 16(19), 3722; https://doi.org/10.3390/rs16193722 - 7 Oct 2024
Viewed by 1102
Abstract
In the production of high-definition maps, it is necessary to achieve the three-dimensional instantiation of road furniture that is difficult to depict on traditional maps. The development of mobile laser measurement technology provides a new means for acquiring road furniture data. To address [...] Read more.
In the production of high-definition maps, it is necessary to achieve the three-dimensional instantiation of road furniture that is difficult to depict on traditional maps. The development of mobile laser measurement technology provides a new means for acquiring road furniture data. To address the issue of traffic marking extraction accuracy in practical production, which is affected by degradation, occlusion, and non-standard variations, this paper proposes a 3D reconstruction method based on energy functions and template matching, using zebra crossings in vehicle-mounted LiDAR point clouds as an example. First, regions of interest (RoIs) containing zebra crossings are obtained through manual selection. Candidate point sets are then obtained at fixed distances, and their neighborhood intensity features are calculated to determine the number of zebra stripes using non-maximum suppression. Next, the slice intensity feature of each zebra stripe is calculated, followed by outlier filtering to determine the optimized length. Finally, a matching template is selected, and an energy function composed of the average intensity of the point cloud within the template, the intensity information entropy, and the intensity gradient at the template boundary is constructed. The 3D reconstruction result is obtained by solving the energy function, performing mode statistics, and normalization. This method enables the complete 3D reconstruction of zebra stripes within the RoI, maintaining an average planar corner accuracy within 0.05 m and an elevation accuracy within 0.02 m. The matching and reconstruction time does not exceed 1 s, and it has been applied in practical production. Full article
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<p>Zebra crossings in LiDAR point cloud represented by intensity.</p>
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<p>Study case. (<b>a</b>) AS-900HL multi-platform LiDAR measurement system. (<b>b</b>) Trajectory of the study case (Shanghai, China). (<b>c</b>) Distribution of zebra crossing areas used for experiments in the MLS-S point cloud.</p>
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<p>Overall workflow of zebra crossing extraction and 3D reconstruction.</p>
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<p>Calculation of stripe count in pre-selection box. (<b>a</b>) Local coordinate system of the selected zebra crossing area. (<b>b</b>) Candidate point <math display="inline"><semantics> <msub> <mi>q</mi> <mi>i</mi> </msub> </semantics></math> and the point <math display="inline"><semantics> <msub> <mi>q</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> </semantics></math> with the highest local energy value.</p>
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<p>Calculation of single zebra stripe length. (<b>a</b>) Typical zebra crossing; (<b>b</b>) Regular zebra stripes; (<b>c</b>) Zebra stripes at the curb; (<b>d</b>) Zoomed-in view.</p>
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<p>Schematic of template boundary intensity gradient calculation.</p>
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<p>Length calculation error caused by deviation of the pre-selected box.</p>
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<p>Extraction and reconstruction results of alienated zebra crossings. (<b>a</b>) Regular zebra crossing. (<b>b</b>) Zebra crossings with varying lengths or fewer stripes. (<b>c</b>) Parallelogram zebra crossing.</p>
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<p>IOUs of horizontal projections between algorithm results and manual annotations.</p>
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<p>Experimental results of MLS point clouds from Wuhan and Chengdu obtained by other data collection platforms.</p>
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<p>Extraction and reconstruction results of zebra crossings under interference conditions. (<b>a</b>) Partially stained zebra crossings. (<b>b</b>) Zebra stripes with partial point clouds missing due to occlusion.</p>
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<p>Accuracy reduction caused by endpoint contamination or systematic spraying errors. (<b>a</b>) Systematic painting minor errors. (<b>b</b>) Vehicle obstruction and manhole cover occupation. (<b>c</b>) Special cases.</p>
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<p>Limitations of the algorithm under special circumstances. (<b>a</b>) Limitation case 1. (<b>b</b>) Limitation case 2.</p>
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16 pages, 6623 KiB  
Article
An Ultra-Wideband Metamaterial Absorber Ranging from Near-Infrared to Mid-Infrared
by Jing-Jenn Lin, Dun-Yu Huang, Meng-Long Hong, Jo-Ling Huang, Chih-Hsuan Wang, Cheng-Fu Yang and Kuei-Kuei Lai
Photonics 2024, 11(10), 939; https://doi.org/10.3390/photonics11100939 - 6 Oct 2024
Viewed by 550
Abstract
This study focused on designing an ultra-wideband metamaterial absorber, consisting of layers of Mn (manganese) and MoO3 (molybdenum trioxide) arranged in a planar interleaving pattern, with a matrix square-shaped Ti (titanium) on the top MoO3 layer. Key features of this research [...] Read more.
This study focused on designing an ultra-wideband metamaterial absorber, consisting of layers of Mn (manganese) and MoO3 (molybdenum trioxide) arranged in a planar interleaving pattern, with a matrix square-shaped Ti (titanium) on the top MoO3 layer. Key features of this research included the novel use of Mn and MoO3 in a planar interleaving configuration for designing an ultra-wideband absorber, which was rarely explored in previous studies. MoO3 thin film served as the fundamental material, leveraging its favorable optical properties and absorption capabilities in the infrared spectrum. Alternating layers of Mn and MoO3 were adjusted in thickness and order to optimize absorptivity across desired wavelength ranges. Another feature is that the Mn and MoO3 materials in the investigated absorber had a planar structure, which simplified the manufacturing of the absorber. Furthermore, the topmost layer of square-shaped Ti was strategically placed to enhance the absorber’s bandwidth and efficiency. When the investigated absorber lacked a Ti layer, its absorptivity and bandwidth significantly decreased. This structural design leveraged the optical properties of Mn, MoO3, and Ti to significantly expand the absorption range across an ultra-wideband spectrum. When the Ti height was 280 nm, the investigated absorber exhibited a bandwidth with absorptivity greater than 0.9, spanning from the near-infrared (0.80 μm) to the mid-infrared (9.07 μm). The average absorptivity in this range was 0.950 with a maximum absorptivity of 0.989. Additionally, three absorption peaks were observed at 1010, 2510, and 6580 nm. This broad absorption capability makes it suitable for a variety of optical applications, ranging from near-infrared to mid-infrared wavelengths, including thermal imaging and optical sensing. Full article
(This article belongs to the Special Issue Emerging Trends in Metamaterials and Metasurfaces Research)
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<p>The structure of the investigated ultra-wideband metamaterial absorber. (<b>a</b>) Side view and (<b>b</b>) 3D structure. Green: Ti; yellow: MoO<sub>3</sub>; and pink: Mn.</p>
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<p>Effect of the various thicknesses of the h1 Mn layer on the absorptivity under different simulation wavelengths.</p>
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<p>Effect of the thickness of the h3 Mn layer on the absorptivity under different simulation wavelengths.</p>
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<p>Effect of the thickness of the h4 MoO<sub>3</sub> layer on the absorptivity under different simulation wavelengths.</p>
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<p>Effect of the thickness of the h5 Mn layer on (<b>a</b>) the absorptivity under different simulation wavelengths and (<b>b</b>) the absorption spectra under different thicknesses of the h1 Mn layer.</p>
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<p>Effect of the thickness of the h7 Mn layer on (<b>a</b>) the absorptivity under different simulation wavelengths and (<b>b</b>) the absorption spectra under different thicknesses of the h7 Mn layer.</p>
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<p>Effect of the thickness of the h9 square-shaped Ti layer changed from 200 nm to 280 nm on (<b>a</b>) the absorptivity under different simulation wavelengths and (<b>b</b>) the absorption spectra under different thicknesses of the h9 Ti layer.</p>
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<p>Variations of (<b>a</b>) optical impendence and (<b>b</b>) absorptivity, reflectivity, and transmissivity spectra for the designed absorber in the range of 400–10,000 nm.</p>
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<p>(<b>a</b>) Structure and (<b>b</b>) absorption spectra of the different absorbers in the range of 400–10,000 nm.</p>
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<p>Distributions of (<b>a</b>) the electric field intensity and (<b>b</b>) the magnetic field intensity, with different normal incident wavelengths.</p>
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<p>Absorptivity distribution of the investigated ultra-wideband NIR and MIR metamaterial absorber for the (<b>a</b>) TE–polarized light and (<b>b</b>) TM–polarized light with various oblique incidence angles and normal direction.</p>
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22 pages, 4862 KiB  
Article
Theoretical Hints to Optimize Energy Dissipation and Cell–Cell Response in Quantum Cellular Automata Based on Tetrameric and Bidimeric Cells
by Andrew Palii, Shmuel Zilberg and Boris Tsukerblat
Magnetochemistry 2024, 10(10), 73; https://doi.org/10.3390/magnetochemistry10100073 - 30 Sep 2024
Viewed by 557
Abstract
This article is largely oriented towards the theoretical foundations of the rational design of molecular cells for quantum cellular automata (QCA) devices with optimized properties. We apply the vibronic approach to the analysis of the two key properties of such molecular cells, namely [...] Read more.
This article is largely oriented towards the theoretical foundations of the rational design of molecular cells for quantum cellular automata (QCA) devices with optimized properties. We apply the vibronic approach to the analysis of the two key properties of such molecular cells, namely the cell–cell response and energy dissipation in the course of the non-adiabatic switching of the electric field acting on the cell. We consider two kinds of square planar cells, namely cells represented by a two-electron tetrameric mixed valence (MV) cluster and bidimeric cells composed of two one-electron MV dimeric half-cells. The model includes vibronic coupling of the excess electrons with the breathing modes of the redox sites, electron transfer, intracell interelectronic Coulomb repulsion, and also the interaction of the cell with the electric field of polarized neighboring cells. For both kinds of cells, the heat release is shown to be minimal in the case of strong delocalization of excess electrons (weak vibronic coupling and/or strong electron transfer) exposed to a weak electric field. On the other hand, such a parametric regime proves to be incompatible with a strong nonlinear cell–cell response. To reach a compromise between low energy dissipation and a strong cell–cell response, we suggest using weakly interacting MV molecules with weak electron delocalization as cells. From this point of view, bidimeric cells are advantageous over tetrameric ones due to their smaller number of electron transfer pathways, resulting in a lower extent of electron delocalization. The distinct features of bidimeric cells, such as their two possible mutual arrangements (“side-by-side” and “head-to-tail”), are discussed as well. Finally, we briefly discuss some relevant results from a recent ab initio study on electron transfer and vibronic coupling from the perspective of the possibility of controlling the key parameters of molecular QCA cells. Full article
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<p>Two examples of the tetrameric square-planar molecular cell for QCA representing the tetraruthenium Creutz–Taube derivatives. (<b>a</b>) Illustration for the case of electron transfer along the sides and (<b>b</b>) the case of transfer along the diagonals.</p>
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<p>Schematic representation of the electronic populations of sites in the polarized bidimeric square-planar driver-cell (<b>a</b>) and in tetrameric driver-cell (<b>b</b>). Both such cells can be regarded as electric quadrupoles. Red balls denote the sites occupied by electrons.</p>
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<p>Head-to-tail (<b>a</b>) and side-by-side (<b>b</b>) mutual arrangements of the bidimeric square cells.</p>
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<p>Schematic representation of the nonadiabatic switching cycle of a bidimeric working cell under the influence of a sudden change in the Coulomb field of the driver-cell. The image of the switching cycle for the tetrameric cell looks quite similar.</p>
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<p>Scheme of the low-lying spin levels of the two-electron square planar MV tetrameric system in the strong Coulomb repulsion limit (<b>a</b>) and the scheme of the adiabatic potentials in the PKS vibronic model with <math display="inline"><semantics> <mrow> <mo>ℏ</mo> <mi>ω</mi> <mrow> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> </mrow> <mo>/</mo> <mrow> <mo>ℏ</mo> <mi>ω</mi> </mrow> </mrow> <mo>=</mo> <mn>0.5</mn> <mo>,</mo> <mo> </mo> </mrow> </semantics></math><span class="html-italic">υ</span>/<math display="inline"><semantics> <mrow> <mo>ℏ</mo> <mi>ω</mi> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, where <span class="html-italic">q</span> is the vibrational coordinate of the out-of-phase PKS vibration, <math display="inline"><semantics> <mrow> <mi>ω</mi> </mrow> </semantics></math> is the frequency of this vibration, and <span class="html-italic">υ</span> is the vibronic coupling parameter (<b>b</b>).</p>
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<p>Dependences of low-temperature specific heat release on the vibronic PKS coupling parameter, calculated in the limit of strong Coulomb interaction inside the cell. Tetrameric cells: curve 1:<math display="inline"><semantics> <mrow> <mi mathvariant="normal">u</mi> <mrow> <mo>=</mo> </mrow> <mrow> <mn>20</mn> <mo> </mo> <mi mathvariant="normal">c</mi> </mrow> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> <mo>=</mo> <mn>50</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; 2: <math display="inline"><semantics> <mrow> <mi mathvariant="normal">u</mi> <mo>=</mo> <mrow> <mn>20</mn> <mo> </mo> <mi mathvariant="normal">c</mi> </mrow> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> <mo>=</mo> <mn>100</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; 3: <math display="inline"><semantics> <mrow> <mi mathvariant="normal">u</mi> <mo>=</mo> <mrow> <mn>10</mn> <mo> </mo> <mi mathvariant="normal">c</mi> </mrow> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> <mo>=</mo> <mn>50</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; 4: <math display="inline"><semantics> <mrow> <mi mathvariant="normal">u</mi> <mo>=</mo> <mrow> <mn>10</mn> <mo> </mo> <mi mathvariant="normal">c</mi> </mrow> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> <mo>=</mo> <mn>100</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo>.</mo> </mrow> </semantics></math> Bidimeric cells: 5: <math display="inline"><semantics> <mrow> <mi mathvariant="normal">u</mi> <mo>=</mo> <mrow> <mn>20</mn> <mo> </mo> <mi mathvariant="normal">c</mi> </mrow> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> <mo>=</mo> <mn>100</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; 6: <math display="inline"><semantics> <mrow> <mi mathvariant="normal">u</mi> <mo>=</mo> <mrow> <mn>20</mn> <mo> </mo> <mi mathvariant="normal">c</mi> </mrow> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> <mo>=</mo> <mn>200</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; 7: <math display="inline"><semantics> <mrow> <mi mathvariant="normal">u</mi> <mo>=</mo> <mrow> <mn>10</mn> <mo> </mo> <mi mathvariant="normal">c</mi> </mrow> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> <mo>=</mo> <mn>100</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; 8: <math display="inline"><semantics> <mrow> <mi mathvariant="normal">u</mi> <mo>=</mo> <mrow> <mn>10</mn> <mo> </mo> <mi mathvariant="normal">c</mi> </mrow> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> <mo>=</mo> <mn>200</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>. In all calculations presented in this figure, the vibrational quantum is set to <math display="inline"><semantics> <mrow> <mo>ℏ</mo> <mi>ω</mi> <mo>=</mo> <mn>1605</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>.</p>
Full article ">Figure 7
<p>Low-temperature cell–cell response functions calculated in the limiting case of strong Coulomb interaction for tetrameric cells with <math display="inline"><semantics> <mrow> <mo>ℏ</mo> <mi>ω</mi> <mo>=</mo> <mn>1605</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo> </mo> <mi mathvariant="normal">a</mi> <mi mathvariant="normal">n</mi> <mi mathvariant="normal">d</mi> <mi>υ</mi> <mo>=</mo> <mn>3500</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math> and the three sets of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>u</mi> </mrow> </semantics></math> values shown in the plots (<b>a</b>) and for tetrameric cells with <math display="inline"><semantics> <mrow> <mo>ℏ</mo> <mi>ω</mi> <mo>=</mo> <mn>1605</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo> </mo> <mi mathvariant="normal">a</mi> <mi mathvariant="normal">n</mi> <mi mathvariant="normal">d</mi> <mo> </mo> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> </msub> <mo>=</mo> <mn>50</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math> and three sets of <span class="html-italic">υ</span> and <span class="html-italic">u</span> values shown in the plots. (<b>b</b>) The corresponding calculated values of specific heat release are also shown in the plots.</p>
Full article ">Figure 8
<p>Dependences of specific heat release on the vibronic PKS coupling parameter, calculated in the low-temperature limit for a tetrameric cell with a violated limit of strong Coulomb interaction with <math display="inline"><semantics> <mrow> <mi>t</mi> <mo>=</mo> <mn>1573</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo>,</mo> <mo> </mo> <mi mathvariant="normal">ℏ</mi> <mi>ω</mi> <mo>=</mo> <mn>1605</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo>,</mo> <mrow> <mi>and</mi> <mo> </mo> </mrow> <mi>b</mi> <mo>=</mo> <mn>6.973</mn> <mo> </mo> <mo>Å</mo> </mrow> </semantics></math> and two intercell distances shown in the plots.</p>
Full article ">Figure 9
<p>Low-temperature cell–cell response functions for a tetrameric cell evaluated beyond the limit of strong Coulomb interaction with <math display="inline"><semantics> <mrow> <mi>t</mi> <mo>=</mo> <mn>1573</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo>,</mo> <mo> </mo> <mi mathvariant="normal">ℏ</mi> <mi>ω</mi> <mo>=</mo> <mn>1605</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo>,</mo> <mrow> <mi>and</mi> <mo> </mo> </mrow> <mi>b</mi> <mo>=</mo> <mn>6.973</mn> <mo> </mo> <mo>Å</mo> </mrow> </semantics></math> and the three sets of <math display="inline"><semantics> <mi>c</mi> </semantics></math> and <math display="inline"><semantics> <mi>υ</mi> </semantics></math> values shown in the plots. The corresponding calculated values of the specific heat release are also shown.</p>
Full article ">Figure 10
<p>The dependences of low-temperature specific heat release on the vibronic parameter evaluated for the two mutual arrangements of the bidimeric cells with a violated limit of strong Coulomb interaction at <math display="inline"><semantics> <mrow> <mi>t</mi> <mo>=</mo> <mn>1573</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo>,</mo> <mo> </mo> <mo> </mo> <mi mathvariant="normal">ℏ</mi> <mi>ω</mi> <mo>=</mo> <mn>1605</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo>,</mo> <mi>b</mi> <mo>=</mo> <mn>6.973</mn> <mo> </mo> <mo>Å</mo> <mo>,</mo> <mo> </mo> <mi mathvariant="normal">a</mi> <mi mathvariant="normal">n</mi> <mi mathvariant="normal">d</mi> <mo> </mo> <mi>c</mi> <mo>=</mo> <mn>15</mn> <mo> </mo> <mo>Å</mo> </mrow> </semantics></math>.</p>
Full article ">Figure 11
<p>Cell–cell response functions evaluated for two mutual arrangements of bidimeric cells with a violated limit of strong Coulomb interaction at <math display="inline"><semantics> <mrow> <mi>t</mi> <mo>=</mo> <mn>1573</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo>,</mo> <mo>ℏ</mo> <mi>ω</mi> <mo>=</mo> <mn>1605</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo>,</mo> <mo> </mo> <mi>b</mi> <mo>=</mo> <mn>6.973</mn> <mo> </mo> <mo>Å</mo> <mo>,</mo> <mo> </mo> <mi mathvariant="normal">a</mi> <mi mathvariant="normal">n</mi> <mi mathvariant="normal">d</mi> <mo> </mo> <mi>c</mi> <mo>=</mo> <mn>15</mn> <mo> </mo> <mo>Å</mo> </mrow> </semantics></math> and the following two values of <math display="inline"><semantics> <mi>υ</mi> </semantics></math>: <math display="inline"><semantics> <mrow> <mi>υ</mi> <mo>=</mo> <mn>3500</mn> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math> (<b>a</b>), <math display="inline"><semantics> <mrow> <mi>υ</mi> <mo> </mo> <mrow> <mo>=</mo> <mn>4000</mn> </mrow> <mo> </mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math> (<b>b</b>).</p>
Full article ">Figure 12
<p>Schemes of the bidimeric cells composed of two MV dimers: [C<sub>12</sub>H<sub>12</sub>]<sup>+</sup> (<b>a</b>) and [C<sub>17</sub>H<sub>16</sub>]<sup>+</sup> (<b>b</b>) [<a href="#B41-magnetochemistry-10-00073" class="html-bibr">41</a>]; radical-cation forms of 1,4-diallyl-butane with a saturated bridge (<b>c</b>); radical-cation forms of 1,4-diallyl-butene-2 with an unsaturated bridge [<a href="#B46-magnetochemistry-10-00073" class="html-bibr">46</a>] (<b>d</b>).</p>
Full article ">
16 pages, 6001 KiB  
Article
Experimental Investigation on the Effect of Coil Shape on Planar Eddy Current Sensor Characteristic for Blade Tip Clearance
by Lingqiang Zhao, Yaguo Lyu, Fulin Liu, Zhenxia Liu and Ziyu Zhao
Sensors 2024, 24(18), 6133; https://doi.org/10.3390/s24186133 - 23 Sep 2024
Viewed by 465
Abstract
Given the increasing application of eddy current sensors for measuring turbine tip clearance in aero engines, enhancing the performance of these sensors is essential for improving measurement accuracy. This study investigates the influence of coil shape on the measurement performance of planar eddy [...] Read more.
Given the increasing application of eddy current sensors for measuring turbine tip clearance in aero engines, enhancing the performance of these sensors is essential for improving measurement accuracy. This study investigates the influence of coil shape on the measurement performance of planar eddy current sensors and identifies an optimal coil shape to enhance sensing capabilities. To achieve this, various coil shapes—specifically circular, square, rectangular wave, and triangular wave—were designed and fabricated, featuring different numbers of turns for the experiment at room temperature. By employing a method for calculating coil inductance, the performance of each sensor was evaluated based on key metrics: measurement range, sensitivity, and linearity. Experimental results reveal that the square coil configuration outperforms other shapes in overall measurement performance. Notably, the square coil demonstrated a measurement range of 0 mm to 8 mm, a sensitivity of 0.115685 μH/mm, and an impressive linearity of 98.41% within the range of 0 mm to 2 mm. These findings indicate that the square coil configuration enhances measurement capabilities. The conclusions drawn from this study provide valuable insights for selecting coil shapes and optimizing the performance of planar eddy current sensors, thereby contributing to the advancement of turbine tip clearance measurement techniques in aero engines. Full article
(This article belongs to the Special Issue Digital Twin-Enabled Deep Learning for Machinery Health Monitoring)
Show Figures

Figure 1

Figure 1
<p>Illustration of the sensing principle of an eddy current sensor for the dynamic tip clearance measurement. (<b>a</b>) An eddy current sensor mounted on the turbine case; the sensor is highlighted in blue. (<b>b</b>) Equivalent circuit diagram for tip clearance measurement using an eddy current sensor; the sensor is modeled as an inductance (<span class="html-italic">L<sub>c</sub></span>) connected with a resistance (<span class="html-italic">R<sub>c</sub></span>) in series; the blade is modeled in the same way. (<b>c</b>) The Lc of the sensing coil is used to measure tip clearance (Distance).</p>
Full article ">Figure 2
<p>Comparison of inductance effective area of the coil at different blade positions. (<b>a</b>) The scheme of the relative position 1 between the sensing coil and the actual blade; (<b>b</b>) The scheme of the relative position 2 between the sensing coil and the actual blade.</p>
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<p>Various sensing coil shapes.</p>
Full article ">Figure 3 Cont.
<p>Various sensing coil shapes.</p>
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<p>An aluminum mold engraved with partial-shaped coils.</p>
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<p>Coils of various shapes.</p>
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<p>Sensor; (<b>a</b>) the design sketch of sensor; (<b>b</b>) sensor after encapsulation.</p>
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<p>(<b>a</b>) Illustration of testing setup for evaluating the sensors with sensing coils of various shapes; (<b>b</b>) image of simplified tested disc made of Inconel 718.</p>
Full article ">Figure 8
<p>(<b>a</b>) The equivalent measurement circuit of the sensing sensor. The sensing coil is modeled as <span class="html-italic">L<sub>c</sub></span> in series with <span class="html-italic">R<sub>c</sub></span>; (<b>b</b>) typical output signals of <span class="html-italic">V</span><sub>1</sub> and <span class="html-italic">V</span><sub>2</sub>; (<b>c</b>) The vector diagram of the output signals of <span class="html-italic">V</span><sub>1</sub> and <span class="html-italic">V</span><sub>2</sub>; (<b>d</b>) typical inductive pulses generated by the passage of the blade tips at a rotating speed of 2500 r/min.</p>
Full article ">Figure 8 Cont.
<p>(<b>a</b>) The equivalent measurement circuit of the sensing sensor. The sensing coil is modeled as <span class="html-italic">L<sub>c</sub></span> in series with <span class="html-italic">R<sub>c</sub></span>; (<b>b</b>) typical output signals of <span class="html-italic">V</span><sub>1</sub> and <span class="html-italic">V</span><sub>2</sub>; (<b>c</b>) The vector diagram of the output signals of <span class="html-italic">V</span><sub>1</sub> and <span class="html-italic">V</span><sub>2</sub>; (<b>d</b>) typical inductive pulses generated by the passage of the blade tips at a rotating speed of 2500 r/min.</p>
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<p>The distribution of three positions along the blade chord.</p>
Full article ">Figure 10
<p>Effect of effective area on the inductance value of the circular shape coil.</p>
Full article ">Figure 11
<p>Effect of excitation frequency on the inductance value of the different sensing coil; (<b>a</b>) Circular coil; (<b>b</b>) Square coil.</p>
Full article ">Figure 12
<p>Effect of excitation voltage on the inductance value of the different sensing coil; (<b>a</b>) Circular coil; (<b>b</b>) Square coil.</p>
Full article ">Figure 13
<p>The inductance value of the circular coil.</p>
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<p>The inductance value of the rectangular wave coil-vertical.</p>
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<p>The inductance value of the rectangular wave coil-horizontal.</p>
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<p>The inductance value of the triangular wave coil-vertical.</p>
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<p>The inductance value of the triangular wave coil-horizontal.</p>
Full article ">Figure 18
<p>The measurement range, sensitivity, and linearity of various shapes of sensing coil, a–f represent the following coil shapes: circular coil, square coil, rectangular wave coil—vertical, rectangular wave coil—horizontal, triangular wave coil–vertical, triangular wave coil—horizontal, respectively; (<b>a</b>) The measurement range of coils with various shapes; (<b>b</b>) the sensitivity of coil with various shapes within the range of 0–2 mm; (<b>c</b>) the linearity of coil with various shapes within the range of 0–2 mm.</p>
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10 pages, 1639 KiB  
Article
One-Step Dry-Etching Fabrication of Tunable Two-Hierarchical Nanostructures
by Xu Ji, Bo Wang, Zhongshan Zhang, Yuan Xiang, Haifang Yang, Ruhao Pan and Junjie Li
Micromachines 2024, 15(9), 1160; https://doi.org/10.3390/mi15091160 - 17 Sep 2024
Viewed by 876
Abstract
Two-hierarchical nanostructures, characterized by two distinct configurations along the height direction, exhibit immense potential for applications in various fields due to their significantly enhanced controllable degree compared to single-order structures. However, due to the limitations imposed by planar technology, the realization of two-hierarchical [...] Read more.
Two-hierarchical nanostructures, characterized by two distinct configurations along the height direction, exhibit immense potential for applications in various fields due to their significantly enhanced controllable degree compared to single-order structures. However, due to the limitations imposed by planar technology, the realization of two-hierarchical nanostructures encounters huge challenges. In this work, we developed a one-step etching method based on inductively coupled plasma reactive ion etching for two-hierarchical nanostructures. Thanks to the shrinking effect of the Cr mask and the generation of a passivation layer during etching, the target materials experienced two different states from vertical etching to shrink etching. Consequently, the achieved two-hierarchical nanostructure configuration features a cross-section of an upper triangle and a lower rectangle, showing higher controllable degrees compared to the one-order ones. Both the mask pattern and etching parameters play crucial roles, by which two-hierarchical structures with diversiform shapes can be constructed controllably. This method for two-hierarchical nanostructures offers advantages including excellent control over structural properties, high processing efficiency, uniformity across large areas, and universality in materials. This developed strategy not only presents a simple and rapid nanofabrication platform for realizing optoelectronic devices, but also provides innovative ideas for designing the next generation of high-performance devices. Full article
(This article belongs to the Special Issue The 15th Anniversary of Micromachines)
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Figure 1

Figure 1
<p>(<b>a</b>) Process flow diagram for two-hierarchical nanostructure preparation. (<b>b</b>) With increasing time, the evolution of the morphology of this two-hierarchical nanostructure. Scale bar: 600 nm.</p>
Full article ">Figure 2
<p>One-step etching fabricating mechanism of two-hierarchical nanostructures. (<b>a</b>) The process of two-hierarchical nanostructure formation through the action of CHF<sub>3</sub> and SF<sub>6</sub> plasma in the etching process. (<b>b</b>) At the beginning of etching, TiO<sub>2</sub> is etched into vertical gratings. (<b>c</b>) With the increase in etching time, the Cr mask gradually narrows due to shrink etching, and the TiO<sub>2</sub> gradually forms two-hierarchical nanostructures with a trapezoid on the top and rectangle on the bottom. (<b>d</b>) When the Cr mask shrink etching is completed, TiO<sub>2</sub> two-hierarchical nanostructures with a triangular upper section and a rectangular lower section are formed. Scale bar: 400 nm.</p>
Full article ">Figure 3
<p>(<b>a</b>) Under the condition that only ICP power changes and the other etching conditions remain unchanged, the morphology of the two-hierarchical nanostructures after etching of the same etching mask is affected. (<b>b</b>) Under the condition that only RF power changes and the other etching conditions remain unchanged, the morphology of the two-hierarchical nanostructures after etching of the same etching mask is affected: (<b>b1</b>–<b>b3</b>) the change in the main structural parameters of the two-hierarchical nanostructure morphology when RF power varies, including the height of the upper triangle (h), the radius of the top corner of the triangle (r), and the gap between the structures (g); (<b>b4</b>) the minimum gap between cell structures is 10 nm. Scale bar: 600 nm.</p>
Full article ">Figure 4
<p>With the same design linewidth, but a different spacing mask, the morphology of the two-hierarchical nanostructures changes under the same etching conditions. (<b>a</b>–<b>e</b>) Structural features and key parameters of two-hierarchical nanostructures marked on the SEM image. (<b>f</b>) Variation trend of key structural parameters with the structural gap regulation, namely, height of the upper triangle (h<sub>1</sub>), height of the lower rectangle (h<sub>2</sub>), angle of the upper triangle (θ), and width (L). Scale bar: 600 nm.</p>
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<p>One-step etching of diversified two-hierarchical nanostructures using different masks. From top to the bottom are the schematic, top, and tilt views of an array of two-hierarchical nanostructures, the detailed SEM images of a single nanostructure and the side walls, and finally a schematic of a unit cell of two-hierarchical nanostructures, where the mask shapes are designed as (<b>a</b>–<b>f</b>) squares, triangles, circles, multi-circles, crosses, and hexagons. Scale bar: 500 nm (second and third rows), 300 nm (fourth row), and 200 nm (fifth row).</p>
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<p>The one-step etching method is suitable for preparing two-hierarchical structures of various materials, such as c-Si, α-Si, SiN<sub>x</sub>, and SiO<sub>2</sub>. Scale bar: 800 nm.</p>
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21 pages, 15462 KiB  
Article
An Empirical Investigation on the Visual Imagery of Augmented Reality User Interfaces for Smart Electric Vehicles Based on Kansei Engineering and FAHP-GRA
by Jin-Long Lin and Meng-Cong Zheng
Mathematics 2024, 12(17), 2712; https://doi.org/10.3390/math12172712 - 30 Aug 2024
Viewed by 745
Abstract
Smart electric vehicles (SEVs) hold significant potential in alleviating the energy crisis and environmental pollution. The augmented reality (AR) dashboard, a key feature of SEVs, is attracting considerable attention due to its ability to enhance driving safety and user experience through real-time, intuitive [...] Read more.
Smart electric vehicles (SEVs) hold significant potential in alleviating the energy crisis and environmental pollution. The augmented reality (AR) dashboard, a key feature of SEVs, is attracting considerable attention due to its ability to enhance driving safety and user experience through real-time, intuitive driving information. This study innovatively integrates Kansei engineering, factor analysis, fuzzy systems theory, analytic hierarchy process, grey relational analysis, and factorial experimentation to evaluate AR dashboards’ visual imagery and subjective preferences. The findings reveal that designs featuring blue planar and unconventional-shaped dials exhibit the best performance in terms of visual imagery. Subsequent factorial experiments confirmed these results, showing that drivers most favor blue-dominant designs. Furthermore, in unconventional-shaped dial designs, the visual effect of vertical 3D is more popular with drivers than horizontal 3D, while the opposite is true in round dials. This study provides a scientific evaluation method for assessing the emotional experience of AR dashboard interfaces. Additionally, these findings will help reduce the subjectivity in interface design and enhance the overall competitiveness of SEV vehicles. Full article
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<p>Assessment architecture diagram of this study.</p>
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<p>Design proposal for 18 AR dashboards.</p>
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<p>Schematic diagram of design proposal switching.</p>
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<p>Linguistic variables describing weights of the FAHP.</p>
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<p>The scree plot of eigenvalues and the number of factors.</p>
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<p>The results of the simple effects analysis of the main color within the interaction between the main color and visual effects. Error bars represent +1 SEM. (Notes: * <span class="html-italic">p</span> ≤ 0.05, ** <span class="html-italic">p</span> ≤ 0.01, *** <span class="html-italic">p</span> ≤ 0.001).</p>
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<p>The results of the simple effects analysis of dial styling within the interaction between visual effects and dial styling. Error bars represent +1 SEM. (Notes: * <span class="html-italic">p</span> ≤ 0.05, ** <span class="html-italic">p</span> ≤ 0.01, *** <span class="html-italic">p</span> ≤ 0.001).</p>
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14 pages, 5172 KiB  
Article
Fabrication of Patterned Magnetic Particles in Microchannels and Their Application in Micromixers
by Tianhao Li, Chen Yang, Zihao Shao, Ya Chen, Jiahui Zheng, Jun Yang and Ning Hu
Biosensors 2024, 14(9), 408; https://doi.org/10.3390/bios14090408 - 23 Aug 2024
Viewed by 1193
Abstract
Due to the extremely low Reynolds number, the mixing of substances in laminar flow within microfluidic channels primarily relies on slow intermolecular diffusion, whereas various rapid reaction and detection requirements in lab-on-a-chip applications often necessitate the efficient mixing of fluids within short distances. [...] Read more.
Due to the extremely low Reynolds number, the mixing of substances in laminar flow within microfluidic channels primarily relies on slow intermolecular diffusion, whereas various rapid reaction and detection requirements in lab-on-a-chip applications often necessitate the efficient mixing of fluids within short distances. This paper presents a magnetic pillar-shaped particle fabrication device capable of producing particles with planar shapes, which are then utilized to achieve the rapid mixing of multiple fluids within microchannels. During the particle fabrication process, a degassed PDMS chip provides self-priming capabilities, drawing in a UV-curable adhesive-containing magnetic powder and distributing it into distinct microwell structures. Subsequently, an external magnetic field is applied, and the chip is exposed to UV light, enabling the mass production of particles with specific magnetic properties through photo-curing. Without the need for external pumping, this chip-based device can fabricate hundreds of magnetic particles in less than 10 min. In contrast to most particle fabrication methods, the degassed PDMS approach enables self-priming and precise dispensing, allowing for precise control over particle shape and size. The fabricated dual-layer magnetic particles, featuring fan-shaped blades and disk-like structures, are placed within micromixing channels. By manipulating the magnetic field, the particles are driven into motion, altering the flow patterns to achieve fluid mixing. Under conditions where the Reynolds number in the chip ranges from 0.1 to 0.9, the mixing index for substances in aqueous solutions exceeds 0.9. In addition, experimental analyses of mixing efficiency for fluids with different viscosities, including 25 wt% and 50 wt% glycerol, reveal mixing indices exceeding 0.85, demonstrating the broad applicability of micromixers based on the rapid rotation of magnetic particles. Full article
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<p>Schematic of the chip design and particle fabrication mechanism. (<b>A</b>) Schematic of the microfluidic chip and the process of manufacturing particles: ① The microfluidic chip consists of two layers of PDMS and a glass substrate layer. ② Combine the three layers together and tape the outlet. ③ The PDMS chip undergoes degassing in a vacuum pump system. ④ Take out the PDMS chip and add drops of mixed solution to the inlet. ⑤ and ⑥ The process of self-priming and self-dispensing. ⑦ and ⑧ Apply magnetic field and UV light to the chip. ⑨ Take out the detachable sealing cover layer and release the particles. (<b>B</b>) A 3D schematic of the in-chip particle manufacturing process.</p>
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<p>Physical diagram of the particle manufacturing process and the chip. (<b>A</b>) Degassed PDMS fills the microwells with mixed solution by self-priming: ① and ② Mixed solution filled microchannels. ③ and ④ Mixed solution filled microwells. (<b>B</b>) Air enters the main channel to push away the excess mixed solution: ① and ② Air filled microchannels. ③ and ④ Air pushed away the excess mixed solution. (<b>C</b>) Magnetic field applied to the chip: ① Before the magnetic field is applied, the nanomagnetic powders are uniformly distributed. ② After the magnetic field is applied, the nanopowders are magnetically responsive and aligned in chains along the direction of the field. (<b>D</b>) A physical image of the chip used to prepare the particles.</p>
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<p>Physical and SEM images of particles. (<b>A</b>) PDMS microwells used to produce particles, as well as various shapes of microwell-fabricated particles. (<b>B</b>) SEM images of particles: ① and ② Particles manufactured in various shapes, demonstrating that even complicated structures exhibit outstanding fidelity in the plane. ③ and ④ Disk-like bilayer particle with fan-shaped blades, demonstrating that the particles have high fidelity and a smooth surface.</p>
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<p>Optimization of particulate output efficiency and analysis of particulate rotation. (<b>A</b>) UV-curable adhesive doped with different concentrations of magnetic nanopowder enters the chambers through self-priming. (<b>B</b>) When the concentration of magnetic nanopowder in the UV-curable adhesive is high, it may lead to the blockage of the main channel by the nanopowder, which may reduce the output efficiency of the particles. (<b>C</b>) The effect of different concentrations of magnetic powder on the particle output efficiency (each concentration was repeated 5 times). (<b>D</b>) PDMS chip used to investigate the rotation of particles in chambers of different sizes. (<b>E</b>) Statistical graph of particle rotation in different chambers. (<b>F</b>) Using a high-speed camera to record the rotation speed of particles inside the chamber. (<b>G</b>) Statistical plot of rotational speed of particles in different concentrations of glycerol (each concentration was repeated 10 times).</p>
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<p>Controlled particle rotation for efficient mixing of different fluids. (<b>A</b>) Schematic diagram of the mixing channel and mixing experiment: ① Ink and water were not mixed when the particles were not rotated. ② The two fluids were mixed when the particles were rotated, and the pixel information in the four regions was captured and analyzed with a video camera. (<b>B</b>) Mixing processes guided by particles as active mixers. (<b>C</b>) The mixing effects of different shapes of particles in the four regions: ① Four different fan blades of particles were fabricated using microwells for mixing experiments. ② Mix indexes of the five different shapes of particles under the same conditions. ③ Before and after mixing of particles of shape 4 at different Reynolds numbers.</p>
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<p>Mixing behaviors of particles in high-viscosity fluids. (<b>A</b>) Mix index of particles at different rotational speeds (36 repetitions of the experiment). (<b>B</b>) Control of the rotation of the two particles in the microchannel separately. (<b>C</b>) Particle rotation and mixing efficiency in chambers of different volumes. (<b>D</b>,<b>E</b>) Mixing results of particles at different concentrations of glycerol. (<b>F</b>) Simultaneous rotation of two particles improved mixing efficiency for highly viscous fluids.</p>
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21 pages, 16631 KiB  
Article
An Effective LiDAR-Inertial SLAM-Based Map Construction Method for Outdoor Environments
by Yanjie Liu, Chao Wang, Heng Wu and Yanlong Wei
Remote Sens. 2024, 16(16), 3099; https://doi.org/10.3390/rs16163099 - 22 Aug 2024
Cited by 1 | Viewed by 926
Abstract
SLAM (simultaneous localization and mapping) is essential for accurate positioning and reasonable path planning in outdoor mobile robots. LiDAR SLAM is currently the dominant method for creating outdoor environment maps. However, the mainstream LiDAR SLAM algorithms have a single point cloud feature extraction [...] Read more.
SLAM (simultaneous localization and mapping) is essential for accurate positioning and reasonable path planning in outdoor mobile robots. LiDAR SLAM is currently the dominant method for creating outdoor environment maps. However, the mainstream LiDAR SLAM algorithms have a single point cloud feature extraction process at the front end, and most of the loop closure detection at the back end is based on RNN (radius nearest neighbor). This results in low mapping accuracy and poor real-time performance. To solve this problem, we integrated the functions of point cloud segmentation and Scan Context loop closure detection based on the advanced LiDAR-inertial SLAM algorithm (LIO-SAM). First, we employed range images to extract ground points from raw LiDAR data, followed by the BFS (breadth-first search) algorithm to cluster non-ground points and downsample outliers. Then, we calculated the curvature to extract planar points from ground points and corner points from clustered segmented non-ground points. Finally, we used the Scan Context method for loop closure detection to improve back-end mapping speed and reduce odometry drift. Experimental validation with the KITTI dataset verified the advantages of the proposed method, and combined with Walking, Park, and other datasets comprehensively verified that the proposed method had good accuracy and real-time performance. Full article
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<p>Traditional point cloud feature extraction and loop closure detection. (<b>a</b>) Feature extraction of the point cloud directly based on curvature, with coarse and redundant repetition results. (<b>b</b>) Odometry drift and loop closure failure when using the RNN algorithm for loop closure detection.</p>
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<p>The overall framework of the algorithm proposed in this paper. The light blue and dark blue modules are the original basic modules of the LIO-SAM algorithm, including IMU pre-integration, odometry publication, map position optimization, and so on. The green module is the improvement module proposed in this paper, including point cloud clustering segmentation, feature extraction, and back-end loop closure detection based on the Scan Context algorithm.</p>
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<p>Proposed general framework for point cloud clustering segmentation. In the output image, the green color is the corner point, and the purple color is the planar point.</p>
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<p>The current frame point cloud transformed to a range image.</p>
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<p>The ground point extraction process.</p>
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<p>Schematic diagram of ground point extraction. (<b>a</b>) The original LiDAR point cloud. (<b>b</b>) The extracted ground points.</p>
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<p>Center and neighborhood points in a range image. (<b>a</b>) The center point and neighboring points spatial relationship. (<b>b</b>) A schematic diagram of the calculated angles in the clustering process of the center and neighborhood points.</p>
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<p>Non-ground point cluster segmentation. (<b>a</b>) The LiDAR point cloud after extracting the ground points, which consists of outlier points (blue) and successfully clustered points (green) after downsampling. (<b>b</b>) The successfully clustered point cloud.</p>
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<p>Feature point extraction results. (<b>a</b>) The original LiDAR point cloud, where both yellow and orange-red are LiDAR raw point clouds, and these two colors are determined by the intensity of the point cloud. (<b>b</b>) The extracted edge features (corner points) and planar features (planar points), where green color is the planar points extracted from the ground points and purple color is the corner points extracted from the clustered segmented non-ground points.</p>
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<p>The overall framework of the Scan Context algorithm.</p>
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<p>Split the point cloud into sub-areas by radius and azimuth [<a href="#B30-remotesensing-16-03099" class="html-bibr">30</a>]. Reprinted/adapted with permission from Ref. [<a href="#B30-remotesensing-16-03099" class="html-bibr">30</a>]. 2018, Kim, G.</p>
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<p>One-frame point cloud converted to Scan Context matrix [<a href="#B30-remotesensing-16-03099" class="html-bibr">30</a>]. Reprinted/adapted with permission from Ref. [<a href="#B30-remotesensing-16-03099" class="html-bibr">30</a>]. 2018, Kim, G. The blue area indicates that the corresponding sub-area has no point cloud data or the area is not observable by LiDAR due to occlusion.</p>
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<p>Changes in the Scan Context column vector sequence caused by changes in the LiDAR viewing angle [<a href="#B30-remotesensing-16-03099" class="html-bibr">30</a>]. Reprinted/adapted with permission from Ref. [<a href="#B30-remotesensing-16-03099" class="html-bibr">30</a>]. 2018, Kim, G. (<b>a</b>) The change in viewpoint when the LiDAR returns to the same place causes the Scan Context column vectors to be shifted. (<b>b</b>) The Scan Context matrices transformed with the history frames contain similar shapes.</p>
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<p>Trajectory and ground truth comparison results of the four algorithms on the corresponding sequences of KITTI. (<b>a</b>) The trajectory and ground truth comparison results of four algorithms based on KITTI sequence 0042. (<b>b</b>) The trajectory and ground truth comparison results of four algorithms based on KITTI sequence 0034. (<b>c</b>) The trajectory and ground truth comparison results of four algorithms based on KITTI sequence 0016. (<b>d</b>) The trajectory and ground truth comparison results of four algorithms based on KITTI sequence 0027.</p>
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<p>Localized enlargement of sequence 0034 and 0027 comparison results. (<b>a</b>) A localized enlargement of the sequence 0034 trajectory comparison. (<b>b</b>) A localized enlargement of the sequence 0027 trajectory comparison.</p>
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<p>ATE errors of the four algorithms under the corresponding sequences of the KITTI dataset. (<b>a</b>) The ATE errors of the four algorithms based on the sequence of KITTI dataset 0042. (<b>b</b>) The ATE errors of the four algorithms based on the sequence of KITTI dataset 0034. (<b>c</b>) The ATE errors of the four algorithms based on the sequence of KITTI dataset 0016. (<b>d</b>) The ATE errors of the four algorithms based on the sequence of KITTI dataset 0027. (<b>a</b>–<b>d</b>) show, from left to right, the ATE errors of A-LOAM, LeGO-LOAM, LIO-SAM, and our method on the corresponding sequences of the KITTI dataset.</p>
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<p>Loop closure detection comparison experiment. (<b>a</b>) The loop closure detection results using the RNN algorithm, where the point cloud color is rendered based on the point cloud intensity. (<b>b</b>) The loop closure detection results of our algorithm, where the point cloud color is rendered based on the point cloud coordinate axes.</p>
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<p>Results of our algorithm for mapping based on Walking and Park datasets. (<b>a</b>) The results of mapping based on the Walking dataset. (<b>b</b>) The results of mapping based on the Park dataset. In <a href="#remotesensing-16-03099-f018" class="html-fig">Figure 18</a>, the point cloud color is rendered based on the point cloud intensity.</p>
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