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12 pages, 549 KiB  
Article
Generalized Dimensions of Self-Affine Sets with Overlaps
by Guanzhong Ma, Jun Luo and Xiao Zhou
Fractal Fract. 2024, 8(12), 722; https://doi.org/10.3390/fractalfract8120722 - 6 Dec 2024
Viewed by 480
Abstract
Two decades ago, Ngai and Wang introduced a well-known finite type condition (FTC) on the self-similar iterated function system (IFS) with overlaps and used it to calculate the Hausdorff dimension of self-similar sets. In this paper, inspired by Ngai and Wang’s idea, we [...] Read more.
Two decades ago, Ngai and Wang introduced a well-known finite type condition (FTC) on the self-similar iterated function system (IFS) with overlaps and used it to calculate the Hausdorff dimension of self-similar sets. In this paper, inspired by Ngai and Wang’s idea, we define a new FTC on self-affine IFS and obtain an analogous formula on the generalized dimensions of self-affine sets. The generalized dimensions raised by He and Lau are used to estimate the Hausdorff dimension of self-affine sets. Full article
(This article belongs to the Special Issue Fractal Dimensions with Applications in the Real World)
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<p>The iterates of <span class="html-italic">U</span> under <math display="inline"><semantics> <mrow> <mo stretchy="false">{</mo> <msub> <mi>S</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>S</mi> <mn>2</mn> </msub> <mo>,</mo> <msub> <mi>S</mi> <mn>3</mn> </msub> <mo stretchy="false">}</mo> </mrow> </semantics></math>.</p>
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<p>The iterates of <span class="html-italic">U</span> under <math display="inline"><semantics> <msub> <mi>S</mi> <mi>I</mi> </msub> </semantics></math>’s.</p>
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38 pages, 6726 KiB  
Article
Exploring the Inhibitory Efficacy of Resokaempferol and Tectochrysin on PI3Kα Protein by Combining DFT and Molecular Docking against Wild-Type and H1047R Mutant Forms
by Cristina Paraschiv, Steluța Gosav, Catalina Mercedes Burlacu and Mirela Praisler
Inventions 2024, 9(5), 96; https://doi.org/10.3390/inventions9050096 - 5 Sep 2024
Viewed by 1081
Abstract
This study explores the inhibitory potential of the flavonoids resokaempferol and tectochrysin against both wild-type and H1047R mutant forms of PI3Kα, aiming to expand the repertoire of targeted cancer therapies. Employing an array of computational techniques, including Density Functional Theory (DFT), calculations of [...] Read more.
This study explores the inhibitory potential of the flavonoids resokaempferol and tectochrysin against both wild-type and H1047R mutant forms of PI3Kα, aiming to expand the repertoire of targeted cancer therapies. Employing an array of computational techniques, including Density Functional Theory (DFT), calculations of electronic parameters such as the energies of the frontier molecular orbitals, Molecular Electrostatic Potential (MEP) mapping, and Molecular Docking, we investigate in detail the molecular interactions of these compounds with the PI3Kα kinase. Our findings, corroborated by DFT calculations performed based on the B3LYP (Becke, three-parameter, Lee-Yang-Parr) hybrid functional and the 6-311G++(d,p) basis set, align well with experimental benchmarks and indicate substantial inhibitory efficacy. Further analysis of chemical potential and bioavailability confirmed the drug-like attributes of these flavonoids. Binding affinity and selectivity were rigorously assessed through self-docking and cross-docking against the PIK3CA PDB structures 7K71 and 8TS9. The most promising interactions were validated using Pairwise Structure Alignment and MolProbity analysis of all-atom contacts and geometry. Collectively, these results highlight the flavonoids’ potential as PI3Kα inhibitors and exemplify the utility of natural compounds in the development of precise anticancer treatments. Full article
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<p>Optimized 2D and 3D molecular structures of the resokaempferol and tectochrysin ligands. The numbers in the 3D structure denote the specific atoms within each molecule. These numerical labels are used to identify and differentiate between the various atoms for clarity in chemical structure analysis. Specifically, each number corresponds to a unique position within the molecule, aiding in the precise understanding of their spatial arrangement and bonding interactions.</p>
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<p>Comparative analysis of the molecular energy gaps for (<b>a</b>) resokaempferol and (<b>b</b>) tectochrysin.</p>
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<p>Molecular electrostatic potential on electron density (MEP) for resokaempferol and tectochrysin.</p>
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<p>Mapping of superdelocalizability for electrophilic, nucleophilic, and radical reactions in the resokaempferol and tectochrysin ligands. The color scale utilized across these surfaces employs a gradient where increased reactivity is indicated by a transition from red (at 0.001) to blue (at 0.010). This gradient facilitates the identification of the most probable sites for chemical activity. Additionally, arrows are used to highlight regions of heightened reactivity.</p>
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<p>Bioavailability evaluation radar chart for resokaempferol and tectochrysin. The chart delineates the optimal physico-chemical space for oral bioavailability, represented in different colors: upper limit (green), lower limit (blue), and properties of the compounds (yellow). The upper and lower limits of the chart are the same for both compounds as follows: UPPER LIMIT: MW: 600 g/mol; LogP: 3; LogS: 0.5; LogD: 3; nHA: 12; nHD: 7; TPSA: 140 Å<sup>2</sup>; nRot: 11; nRing: 6; MaxRing: 18; nHet: 15; fChar: 4; nRig: 30. LOWER LIMIT: MW: 100 g/mol; LogP: 0; LogS: −4; LogD: 1; nHA: 0; nHD: 0; TPSA: 0 Å<sup>2</sup>; nRot: 0; nRing: 0; MaxRing: 0; nHet: 1; fChar: −4; nRig: 0.</p>
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<p>Comparative visualization of PI3Kα receptor-native ligand pairs: (<b>a</b>) wild-type with 2-(morpholin-4-yl)[4,5′-bipyrimidin]-2′-amine and (<b>b</b>) H1047R mutant with 5-[3-fluoro-5-(trifluoromethyl)benzamido]-N-methyl-6-(2-methylanilino)pyridine-3-carboxamide.</p>
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<p>Two-dimensional interaction diagram of the native inhibitor and PI3Kα protein: VYP with the (wild-type) PI3Kα and UE9 with the (mutant H1047R) PI3Kα.</p>
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<p>Three-dimensional visualization of the interactions between the native inhibitors and PI3Kα protein: VYP with the wild-type PI3Kα and UE9 with the H1047R mutant PI3Kα, highlighting (<b>a</b>) hydrogen bonding and (<b>b</b>) hydrophobic surfaces.</p>
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<p>Two-dimensional interaction diagram of the potential ligand resokaempferol with the (wild-type) PI3Kα and the (mutant H1047R) PI3Kα protein.</p>
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<p>Three-dimensional visualization of the potential ligand resokaempferol interacting with the (wild-type) PI3Kα and (mutant H1047R) PI3Kα protein highlighting (<b>a</b>) hydrogen bonding and (<b>b</b>) hydrophobic surfaces.</p>
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<p>Two-dimensional interaction diagram of the potential ligand tectochrysin with the (wild-type) PI3Kα and the (mutant H1047R) PI3Kα protein.</p>
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<p>Three-dimensional visualization of the potential ligand tectochrysin interacting with the (wild-type) PI3Kα and (mutant H1047R) PI3Kα protein highlighting (<b>a</b>) hydrogen bonding and (<b>b</b>) hydrophobic surfaces.</p>
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7 pages, 317 KiB  
Article
Self-Intersections of Cubic Bézier Curves Revisited
by Javier Sánchez-Reyes
Mathematics 2024, 12(16), 2463; https://doi.org/10.3390/math12162463 - 9 Aug 2024
Viewed by 984
Abstract
Recently, Yu et al. derived a factorization procedure for detecting and computing the potential self-intersection of 3D integral Bézier cubics, claiming that their proposal distinctly outperforms existing methodologies. First, we recall that in the 2D case, explicit formulas already exist for the parameter [...] Read more.
Recently, Yu et al. derived a factorization procedure for detecting and computing the potential self-intersection of 3D integral Bézier cubics, claiming that their proposal distinctly outperforms existing methodologies. First, we recall that in the 2D case, explicit formulas already exist for the parameter values at the self-intersection (the singularity called crunode in algebraic geometry). Such values are the solutions of a quadratic equation, and affine invariants depend only on the curve hodograph. Also, the factorization procedure for cubics is well known. Second, we note that only planar Bézier cubics can display a self-intersection, so there is no need to address the problem in the more involved 3D setting. Finally, we elucidate the connections with the previous literature and provide a geometric interpretation, in terms of the affine classification of cubics, of the algebraic conditions necessary for the existence of a self-intersection. Cubics with a self-intersection are affine versions of the celebrated Tschirnhausen cubic. Full article
(This article belongs to the Section Algebra, Geometry and Topology)
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<p>Any cubic with a self-intersection lies on the plane <math display="inline"><semantics> <mo>Π</mo> </semantics></math> containing the triangular Bézier polygon defining the loop.</p>
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<p>The four affine types of integral cubics are as follows: (<b>a</b>) crunodal; (<b>b</b>) cuspidal; (<b>c</b>) acnodal; (<b>d</b>) S-shaped.</p>
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<p>There are only two types of Bézier polygons associated with a cubic that may display a self-intersection <math display="inline"><semantics> <mi mathvariant="bold">S</mi> </semantics></math>: (<b>I</b>) self-intersecting; (<b>II</b>) concave.</p>
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26 pages, 7151 KiB  
Article
Expression-Guided Deep Joint Learning for Facial Expression Recognition
by Bei Fang, Yujie Zhao, Guangxin Han and Juhou He
Sensors 2023, 23(16), 7148; https://doi.org/10.3390/s23167148 - 13 Aug 2023
Cited by 2 | Viewed by 3000
Abstract
In recent years, convolutional neural networks (CNNs) have played a dominant role in facial expression recognition. While CNN-based methods have achieved remarkable success, they are notorious for having an excessive number of parameters, and they rely on a large amount of manually annotated [...] Read more.
In recent years, convolutional neural networks (CNNs) have played a dominant role in facial expression recognition. While CNN-based methods have achieved remarkable success, they are notorious for having an excessive number of parameters, and they rely on a large amount of manually annotated data. To address this challenge, we expand the number of training samples by learning expressions from a face recognition dataset to reduce the impact of a small number of samples on the network training. In the proposed deep joint learning framework, the deep features of the face recognition dataset are clustered, and simultaneously, the parameters of an efficient CNN are learned, thereby marking the data for network training automatically and efficiently. Specifically, first, we develop a new efficient CNN based on the proposed affinity convolution module with much lower computational overhead for deep feature learning and expression classification. Then, we develop an expression-guided deep facial clustering approach to cluster the deep features and generate abundant expression labels from the face recognition dataset. Finally, the AC-based CNN is fine-tuned using an updated training set and a combined loss function. Our framework is evaluated on several challenging facial expression recognition datasets as well as a self-collected dataset. In the context of facial expression recognition applied to the field of education, our proposed method achieved an impressive accuracy of 95.87% on the self-collected dataset, surpassing other existing methods. Full article
(This article belongs to the Section Wearables)
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<p>The proposed deep joint learning framework.</p>
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<p>Proposed AC module and AC bottleneck.</p>
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<p>Overview of the proposed ACNN.</p>
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<p>Expression-guided deep facial clustering. A set of facial expression images (<b>a</b>) is used to compute nearest neighbor lists (<b>b</b>); the nearest neighbor lists are then used to compute the distances between pieces of facial expression data (<b>c</b>).</p>
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<p>Example of video segmentation results.</p>
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<p>T-SNE visualization of extracted features from the RAF-DB dataset.</p>
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<p>T-SNE visualization of extracted features from the FER-2013 dataset.</p>
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<p>T-SNE visualization of extracted features from the CK+ dataset.</p>
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<p>Confusion matrices for (<b>a</b>) the first iteration and (<b>b</b>) the last iteration on the self-collected dataset.</p>
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22 pages, 5283 KiB  
Article
A Sorting Method of SAR Emitter Signal Sorting Based on Self-Supervised Clustering
by Dahai Dai, Guanyu Qiao, Caikun Zhang, Runkun Tian and Shunjie Zhang
Remote Sens. 2023, 15(7), 1867; https://doi.org/10.3390/rs15071867 - 31 Mar 2023
Cited by 2 | Viewed by 1549
Abstract
Most existing methods for sorting synthetic aperture radar (SAR) emitter signals rely on either unsupervised clustering or supervised classification methods. However, unsupervised clustering can consume a significant amount of computational and storage space and is sensitive to the setting of hyperparameters, while supervised [...] Read more.
Most existing methods for sorting synthetic aperture radar (SAR) emitter signals rely on either unsupervised clustering or supervised classification methods. However, unsupervised clustering can consume a significant amount of computational and storage space and is sensitive to the setting of hyperparameters, while supervised classification requires a considerable number of labeled samples. To address these limitations, we propose a self-supervised clustering-based method for sorting SAR radiation source signals. The method uses a constructed affinity propagation-convolutional neural network (AP-CNN) to perform self-supervised clustering of a large number of unlabeled signal time-frequency images into multiple clusters in the first stage. Subsequently, it uses a self-organizing map (SOM) network combined with inter-pulse parameters for further sorting in the second stage. The simulation results demonstrate that the proposed method outperforms other depth models and conventional methods in the environment where Gaussian white noise affects the signal. The experiments conducted using measured data also show the superiority of the proposed method in this paper. Full article
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<p>The architecture of the Proposed Method.</p>
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<p>Comparison of SSIM between time-frequency images: (<b>a</b>) pulses are from radar A; (<b>b</b>) pulses are from radar B; (<b>c</b>) pulses are from different radars.</p>
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<p>Flowchart of affinity propagation clustering.</p>
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<p>CNN Structure Diagram.</p>
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<p>Topology of the SOM network.</p>
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<p>Generated SPWVD of radars’ waveform (0 dB): (<b>a</b>) Radar A; (<b>b</b>) Radar B; (<b>c</b>) Radar C; (<b>d</b>) Radar D; (<b>e</b>) Radar E.</p>
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<p>Performance of affinity propagation clustering.</p>
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<p>Performance of AP-CNN.</p>
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<p>Generated SPWVD of radars’ waveform (−10 dB): (<b>a</b>) Radar A; (<b>b</b>) Radar B; (<b>c</b>) Radar C; (<b>d</b>) Radar D; (<b>e</b>) Radar E.</p>
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<p>Confusion matrix of AP-CNN (−10 dB).</p>
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<p>Clustering accuracy of SOM (−10 dB~30 dB).</p>
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<p>Classification performance comparison with different SNR (−10 dB~30 dB).</p>
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<p>Similarity matrix of pulse time-frequency images in the measured data.</p>
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<p>Confusion matrix of the validation dataset.</p>
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<p>AP-CNN sorting results: (<b>a</b>) Class_739 carrier frequency, pulse width, and amplitude; (<b>b</b>) PRI of Class_739; (<b>c</b>) Class_348 carrier frequency, pulse width and amplitude; (<b>d</b>) PRI of Class_348; (<b>e</b>) Class_454 carrier frequency, pulse width and amplitude; (<b>f</b>) PRI of Class_454; (<b>g</b>) Class_169 carrier frequency, pulse width, and amplitude; (<b>h</b>) PRI of Class_169.</p>
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<p>AP-CNN sorting results: (<b>a</b>) Class_739 carrier frequency, pulse width, and amplitude; (<b>b</b>) PRI of Class_739; (<b>c</b>) Class_348 carrier frequency, pulse width and amplitude; (<b>d</b>) PRI of Class_348; (<b>e</b>) Class_454 carrier frequency, pulse width and amplitude; (<b>f</b>) PRI of Class_454; (<b>g</b>) Class_169 carrier frequency, pulse width, and amplitude; (<b>h</b>) PRI of Class_169.</p>
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<p>Hit map of the SOM network.</p>
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21 pages, 7438 KiB  
Article
Identifying Dopamine D3 Receptor Ligands through Virtual Screening and Exploring the Binding Modes of Hit Compounds
by Hongshan Jin, Chengjun Wu, Rui Su, Tiemin Sun, Xingzhou Li and Chun Guo
Molecules 2023, 28(2), 527; https://doi.org/10.3390/molecules28020527 - 5 Jan 2023
Cited by 14 | Viewed by 2506
Abstract
The dopamine D3 receptor (D3R) is an important central nervous system target for treating various neurological diseases. D3R antagonists modulate the improvement of psychostimulant addiction and relapse, while D3R agonists can enhance the response to dopaminergic stimulation and have potential applications in treating [...] Read more.
The dopamine D3 receptor (D3R) is an important central nervous system target for treating various neurological diseases. D3R antagonists modulate the improvement of psychostimulant addiction and relapse, while D3R agonists can enhance the response to dopaminergic stimulation and have potential applications in treating Parkinson’s disease, which highlights the importance of identifying novel D3R ligands. Therefore, we performed auto dock Vina-based virtual screening and D3R-binding-affinity assays to identify human D3R ligands with diverse structures. All molecules in the ChemDiv library (>1,500,000) were narrowed down to a final set of 37 molecules for the binding assays. Twenty-seven compounds exhibited over 50% inhibition of D3R at a concentration of 10 μM, and 23 compounds exhibited over 70% D3R inhibition at a concentration of 10 μM. Thirteen compounds exhibited over 80% inhibition of D3R at a concentration of 10 μM and the IC50 values were measured. The IC50 values of the five compounds with the highest D3R-inhibition rates ranged from 0.97 μM to 1.49 μM. These hit compounds exhibited good structural diversity, which prompted us to investigate their D3R-binding modes. After trial and error, we combined unbiased molecular dynamics simulation (MD) and molecular mechanics generalized Born surface area (MM/GBSA) binding free-energy calculations with the reported protein–ligand-binding pose prediction method using induced-fit docking (IFD) and binding pose metadynamics (BPMD) simulations into a self-consistent and computationally efficient method for predicting and verifying the binding poses of the hit ligands to D3R. Using this IFD-BPMD-MD-MM/GBSA method, we obtained more accurate and reliable D3R–ligand-binding poses than were obtained using the reported IFD-BPMD method. This IFD-BPMD-MD-MM/GBSA method provides a novel paradigm and reference for predicting and validating other protein–ligand binding poses. Full article
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<p>Structures of several discovered D3R-preferring compounds.</p>
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<p>Comparison of the output poses of Eticlopride in short, medium, and long search modes of AutoDock Vina with the original pose in the crystal. The original pose is presented as thick, green tubes, and the predicted poses for short, medium, and long search modes are presented as blue, yellow, and pink thin tubes, respectively.</p>
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<p>The structures of the five most active hit compounds.</p>
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<p>The protein–ligand interactions diagrams of the AutoDock Vina pose of the hit compounds binding to D3R proteins. In the protein–ligand interaction diagrams, the D3R protein backbones are represented by gray cartoons; ligands by thick, green tubes; residues that have strong interactions with ligands are presented by thick plum tubes; residues that have hydrophobic interactions with the ligand are represented by thin, blue tubes.</p>
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<p>Plots of the RMSD estimate averaged over all 10 trials versus the simulation time for the BPMD runs of DD3R/eticlopride complex and AutoDock Vina docking poses of hit compounds. The PoseScore, PersScore, and CompScore values for the these D3R–ligand complexes are shown in the legend.</p>
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<p>Schematic representation of the procedures used to explore the potential binding poses, based on a combination of IFD and BPMD analysis.</p>
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<p>The comparation of top BPMD-scored pose with the original pose in PDB 3PBL of eticlopride.</p>
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<p>Alignment of the top BPMD-scored conformations with representative conformations of D3R–ligand complex and the binding pose of eticlopride in PDB 3PBL. In the top BPMD-scored conformations, the D3R protein backbones are represented with a red-orange color; the ligands are represented by thick, orange tubes; and the residues are represented by thin, plum-colored tubes. In the representative conformations, the D3R protein backbones are represented with a gray color; the ligands are represented by thick, light-gray tube; and the residues are represented by thin, blue tubes. HBs are represented by yellow dashes, π−π stacking is represented by light-blue dashes, and ionic bridges are represented by red-orange dashes.</p>
Full article ">Figure 8 Cont.
<p>Alignment of the top BPMD-scored conformations with representative conformations of D3R–ligand complex and the binding pose of eticlopride in PDB 3PBL. In the top BPMD-scored conformations, the D3R protein backbones are represented with a red-orange color; the ligands are represented by thick, orange tubes; and the residues are represented by thin, plum-colored tubes. In the representative conformations, the D3R protein backbones are represented with a gray color; the ligands are represented by thick, light-gray tube; and the residues are represented by thin, blue tubes. HBs are represented by yellow dashes, π−π stacking is represented by light-blue dashes, and ionic bridges are represented by red-orange dashes.</p>
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<p>Schematic 2D diagrams of the protein–ligand interactions of the top BPMD-scored conformations (<b>A</b>) and representative conformations (<b>B</b>) of different D3R–ligand complexes and the schematic 2D diagrams of the D3R–eticlopride interactions of PDB 3PBL. HBs are represented by plum-colored arrows; π−π stackings are represented by dark-green lines.</p>
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<p>Schematic 2D diagrams of the protein–ligand interactions of the top BPMD-scored conformations (<b>A</b>) and representative conformations (<b>B</b>) of different D3R–ligand complexes and the schematic 2D diagrams of the D3R–eticlopride interactions of PDB 3PBL. HBs are represented by plum-colored arrows; π−π stackings are represented by dark-green lines.</p>
Full article ">Figure 9 Cont.
<p>Schematic 2D diagrams of the protein–ligand interactions of the top BPMD-scored conformations (<b>A</b>) and representative conformations (<b>B</b>) of different D3R–ligand complexes and the schematic 2D diagrams of the D3R–eticlopride interactions of PDB 3PBL. HBs are represented by plum-colored arrows; π−π stackings are represented by dark-green lines.</p>
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<p>Flow chart of the work performed in the present study.</p>
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17 pages, 7601 KiB  
Article
Temporal Analysis of Ground Movement at a Metal Mine in China
by Guang Li, Xin Hui, Fengshan Ma and Jie Guo
Remote Sens. 2022, 14(19), 4993; https://doi.org/10.3390/rs14194993 - 7 Oct 2022
Cited by 2 | Viewed by 1725
Abstract
Mining-induced ground movement is a complicated nonlinear process and a regional geological hazard. Time series in Earth sciences are often characterized as self-affine, long-range persistent, where the power spectra exhibit a power-law dependence on frequency. Whether there exists a periodic signal and a [...] Read more.
Mining-induced ground movement is a complicated nonlinear process and a regional geological hazard. Time series in Earth sciences are often characterized as self-affine, long-range persistent, where the power spectra exhibit a power-law dependence on frequency. Whether there exists a periodic signal and a fundamental frequency in the time series is significant in analyzing ground-movement patterns. To evaluate whether a power law describes the power spectra of a ground-movement time series and whether a fundamental frequency exists, GPS monitoring records taken over 14.5 years describing ground movement in the Jinchuan Nickel Mine, China, were analyzed. The data sets consisted of 500 randomly selected GPS monitoring points, spanning the April 2001–October 2015 time period. Whether a periodic signal in the ground movements existed was determined through the autocorrelation function. The power spectra of the ground-movement time series were found to display power-law behavior over vastly different timescales. The spectral exponents of the horizontal and vertical displacements ranged from 0.47 to 3.58 and from 0.43 to 3.37, with mean values of 2.05 and 1.79, respectively. The ground movements of minefields No.1 and No.2 had 1.1-month and 1.4-month fundamental periods, respectively. Together with a discussion of the underlying mechanisms of power-law behavior and relevant influencing factors, these results indicate that ground-movement time series are a type of self-affine time series that exhibit long-range persistence and scale invariance and show a complex periodicity. These conclusions provide a basis for predicting land subsidence in the study area over a timescale. Full article
(This article belongs to the Special Issue Dynamic Geophysical Phenomenon Monitoring Using Remote Sensing)
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<p>Location and geological map of Jinchuan Nickel Mine in China.</p>
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<p>Characteristics of vertical and horizontal displacement at the Jinchuan Nickel Mine: (<b>a</b>) Distribution of GPS monitoring points at Jinchuan Nickel Mine overlying a contour map of the vertical displacements recorded for October 2015, using May 2005 as a baseline. (<b>b</b>) Diagram of horizontal displacement vectors at mine field No.2 in October 2015, using May 2001 as a reference measure.</p>
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<p>Mine subsidence time series of several monitoring points at the Jinchuan Nickel Mine: (<b>a</b>) monitoring point 2201, (<b>b</b>) monitoring point 2205, (<b>c</b>) monitoring point 6002, (<b>d</b>) monitoring point 6006.</p>
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<p>Power-law relationship between the subsidence and its occurrence cycle.</p>
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<p>Non-detrended and detrended vertical and horizontal displacement time series and autocorrelation plots of the monitoring point 6001 at the Jinchuan Nickel Mine: (<b>a</b>) Horizontal displacement, (<b>b</b>) vertical displacement, (<b>c</b>) detrended horizontal displacement, (<b>d</b>) detrended vertical displacement, (<b>e</b>) autocorrelation plot of horizontal displacement, (<b>f</b>) autocorrelation plot of vertical displacement.</p>
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<p>Power spectra of the horizontal and vertical displacement in the monitoring point 2207 at minefield No.2 and the monitoring point 2003 at minefield No.1 in log <span class="html-italic">S(f)</span>–log <span class="html-italic">(f)</span> and log <span class="html-italic">S(f)</span>–<span class="html-italic">f</span> plots: (<b>a</b>,<b>b</b>): power spectra of the horizontal and vertical displacement of the monitoring point 2207 in a log <span class="html-italic">S(f)</span>–log <span class="html-italic">(f)</span> plot; (<b>c</b>,<b>d</b>): power spectra of the horizontal and vertical displacement of the monitoring point 2207 in a log <span class="html-italic">S(f)</span>–<span class="html-italic">f</span> plot; (<b>e</b>,<b>f</b>): power spectra of the horizontal and vertical displacement of the monitoring point 2003 in a log <span class="html-italic">S(f)</span>–log <span class="html-italic">(f)</span> plot; (<b>g</b>,<b>h</b>): power spectra of the horizontal and vertical displacement of the monitoring point 2003 in a log <span class="html-italic">S(f)</span>–<span class="html-italic">f</span> plot.</p>
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22 pages, 1674 KiB  
Review
Analytical Challenges in Diabetes Management: Towards Glycated Albumin Point-of-Care Detection
by Andrea Rescalli, Elena Maria Varoni, Francesco Cellesi and Pietro Cerveri
Biosensors 2022, 12(9), 687; https://doi.org/10.3390/bios12090687 - 26 Aug 2022
Cited by 13 | Viewed by 6315
Abstract
Diabetes mellitus is a worldwide-spread chronic metabolic disease that occurs when the pancreas fails to produce enough insulin levels or when the body fails to effectively use the secreted pancreatic insulin, eventually resulting in hyperglycemia. Systematic glycemic control is the only procedure at [...] Read more.
Diabetes mellitus is a worldwide-spread chronic metabolic disease that occurs when the pancreas fails to produce enough insulin levels or when the body fails to effectively use the secreted pancreatic insulin, eventually resulting in hyperglycemia. Systematic glycemic control is the only procedure at our disposal to prevent diabetes long-term complications such as cardiovascular disorders, kidney diseases, nephropathy, neuropathy, and retinopathy. Glycated albumin (GA) has recently gained more and more attention as a control biomarker thanks to its shorter lifespan and wider reliability compared to glycated hemoglobin (HbA1c), currently the “gold standard” for diabetes screening and monitoring in clinics. Various techniques such as ion exchange, liquid or affinity-based chromatography and immunoassay can be employed to accurately measure GA levels in serum samples; nevertheless, due to the cost of the lab equipment and complexity of the procedures, these methods are not commonly available at clinical sites and are not suitable to home monitoring. The present review describes the most up-to-date advances in the field of glycemic control biomarkers, exploring in particular the GA with a special focus on the recent experimental analysis techniques, using enzymatic and affinity methods. Finally, analysis steps and fundamental reading technologies are integrated into a processing pipeline, paving the way for future point-of-care testing (POCT). In this view, we highlight how this setup might be employed outside a laboratory environment to reduce the time from measurement to clinical decision, and to provide diabetic patients with a brand-new set of tools for glycemic self-monitoring. Full article
(This article belongs to the Special Issue Advanced Biosensing Technologies in Medical Applications)
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<p>Reactions involved in the glycation of proteins. In particular, hemoglobin (PDB ID: 1BBB) and albumin (PDB ID: 1AO6) have been reported, and the main glycation sites for each of them have been highlighted in red: N-terminal valine of the <math display="inline"><semantics> <mi>β</mi> </semantics></math>-chains of hemoglobin, and lysine and arginine residues of albumin.</p>
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<p>Three-dimensional structure of human serum albumin. The three domains I, II, and III are highlighted in purple, blue and green, respectively, and for each domain the two subdomains A and B are shown—from Belinskaia et al. [<a href="#B59-biosensors-12-00687" class="html-bibr">59</a>].</p>
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<p>Schematic process of an electrochemical enzymatic analysis of glycated albumin. Initially, the sample has to undergo a proteolytic digestion to release <math display="inline"><semantics> <mi>ϵ</mi> </semantics></math>-FK from GA. Then, a specific enzyme (FAOX) oxidizes this substrate while simultaneously an electron mediator is reduced. Finally, by applying an appropriate voltage potential at the electrode site, the reduced-form mediator is oxidized back, releasing electrons that can be collected to measure a current.</p>
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<p>Analysis of the three main aspects of a biosensor realization (i.e., choice of the recognition element; transducer design implementation; analytical measuring technique) applied to POC-compatible affinity methods.</p>
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<p>Schematic representation of the hypothesized steps involved in a POC testing device. The actions to be performed are on top, whereas, at the bottom, the solutions that could be adopted to fulfill the respective needs.</p>
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21 pages, 14021 KiB  
Article
Robust Spectral Clustering Incorporating Statistical Sub-Graph Affinity Model
by Zhenxian Lin, Jiagang Wang and Chengmao Wu
Axioms 2022, 11(6), 269; https://doi.org/10.3390/axioms11060269 - 5 Jun 2022
Cited by 1 | Viewed by 2357
Abstract
Hyperspectral image (HSI) clustering is a challenging work due to its high complexity. Subspace clustering has been proven to successfully excavate the intrinsic relationships between data points, while traditional subspace clustering methods ignore the inherent structural information between data points. This study uses [...] Read more.
Hyperspectral image (HSI) clustering is a challenging work due to its high complexity. Subspace clustering has been proven to successfully excavate the intrinsic relationships between data points, while traditional subspace clustering methods ignore the inherent structural information between data points. This study uses graph convolutional subspace clustering (GCSC) for robust HSI clustering. The model remaps the self-expression of the data to non-Euclidean domains, which can generate a robust graph embedding dictionary. The EKGCSC model can achieve a globally optimal closed-form solution by using a subspace clustering model with the Frobenius norm and a Gaussian kernel function, making it easier to implement, train, and apply. However, the presence of noise can have a noteworthy negative impact on the segmentation performance. To diminish the impact of image noise, the concept of sub-graph affinity is introduced, where each node in the primary graph is modeled as a sub-graph describing the neighborhood around the node. A statistical sub-graph affinity matrix is then constructed based on the statistical relationships between sub-graphs of connected nodes in the primary graph, thus counteracting the uncertainty image noise by using more information. The model used in this work was named statistical sub-graph affinity kernel graph convolutional subspace clustering (SSAKGCSC). Experiment results on Salinas, Indian Pines, Pavia Center, and Pavia University data sets showed that the SSAKGCSC model can achieve improved segmentation performance and better noise resistance ability. Full article
(This article belongs to the Special Issue Machine Learning: Theory, Algorithms and Applications)
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<p>Comparison of node affinity to sub-graph affinity. <math display="inline"><semantics> <mrow> <msub> <mi>x</mi> <mi>u</mi> </msub> </mrow> </semantics></math> (red), <math display="inline"><semantics> <mrow> <msub> <mi>x</mi> <mi>v</mi> </msub> </mrow> </semantics></math> (green), <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>u</mi> </msub> </mrow> </semantics></math> (light red), <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>v</mi> </msub> </mrow> </semantics></math> (light green). (<b>a</b>) Node affinity. (<b>b</b>) Node affinity with neighborhood statistics. (<b>c</b>) Sub-graph affinity.</p>
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<p>Clustering results obtained using different methods on the SalinasA data set. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 50.09%. (<b>c</b>) SSC 75.90%. (<b>d</b>) S4C 80.70%. (<b>e</b>) EDSC 88.99%. (<b>f</b>) EGCSC 99.93%. (<b>g</b>) EKGCSC 100.00%. (<b>h</b>) SSAKGCSC 99.89%.</p>
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<p>Clustering results obtained using different methods on the Indian Pines corrected data set. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 57.52%. (<b>c</b>) SSC 56.09%. (<b>d</b>) S4C 64.97%. (<b>e</b>) EDSC 70.26%. (<b>f</b>) EGCSC 88.27%. (<b>g</b>) EKGCSC 97.31%. (<b>h</b>) SSAKGCSC 97.43%.</p>
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<p>Clustering results obtained using different methods on the Pavia University data set. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 46.16%. (<b>c</b>) SSC 64.27%. (<b>d</b>) S4C 66.72%. (<b>e</b>) EDSC 65.94%. (<b>f</b>) EGCSC 84.42%. (<b>g</b>) EKGCSC 97.32%. (<b>h</b>) SSAKGCSC 97.08%.</p>
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<p>Clustering results obtained using different methods on the Pavia Center data set. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 53.06%. (<b>c</b>) SSC 60.26%. (<b>d</b>) S4C 72.80%. (<b>e</b>) EDSC 75.39%. (<b>f</b>) EGCSC 80.30%. (<b>g</b>) EKGCSC 94.48%. (<b>h</b>) MEKGCSC 93.89%.</p>
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<p>Clustering results obtained using different methods on the SalinasA data set with salt and pepper noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 43.49%. (<b>c</b>) SSC 48.60%. (<b>d</b>) S4C 51.08%. (<b>e</b>) EDSC 61.03%. (<b>f</b>) EGCSC 68.03%. (<b>g</b>) EKGCSC 45.74%. (<b>h</b>) SSAKGCSC 83.47%.</p>
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<p>Clustering results obtained using different methods on the Indian Pines corrected data set with salt and pepper noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 40.29%. (<b>c</b>) SSC 44.75%. (<b>d</b>) S4C 50.63%. (<b>e</b>) EDSC 52.88%. (<b>f</b>) EGCSC 57.07%. (<b>g</b>) EKGCSC 56.09%. (<b>h</b>) SSAKGCSC 66.34%.</p>
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<p>Clustering results obtained using different methods on the Pavia University data set with salt and pepper noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 37.69%. (<b>c</b>) SSC 51.22%. (<b>d</b>) S4C 53.31%. (<b>e</b>) EDSC 53.56%. (<b>f</b>) EGCSC 60.12%. (<b>g</b>) EKGCSC. (<b>h</b>) SSAKGCSC 79.83%.</p>
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<p>Clustering results obtained using different methods on the Pavia Center data set with salt and pepper noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 38.21%. (<b>c</b>) SSC 50.39%. (<b>d</b>) S4C 52.38%. (<b>e</b>) EDSC 60.33%. (<b>f</b>) EGCSC 64.22%. (<b>g</b>) EKGCSC 33.68%. (<b>h</b>) MEKGCSC 85.01%.</p>
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<p>Clustering results obtained using different methods on the SalinasA data set with Gaussian noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 35.96%. (<b>c</b>) SSC 47.61%. (<b>d</b>) S4C 54.77%. (<b>e</b>) EDSC 61.97%. (<b>f</b>) EGCSC 54.92%. (<b>g</b>) EKGCSC 60.73%. (<b>h</b>) SSAKGCSC 86.78%.</p>
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<p>Clustering results obtained using different methods on the Indian Pines corrected data set with Gaussian noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 43.20%. (<b>c</b>) SSC 42.20%. (<b>d</b>) S4C 53.29%. (<b>e</b>) EDSC 56.78%. (<b>f</b>) EGCSC 59.30%. (<b>g</b>) EKGCSC 54.70%. (<b>h</b>) SSAKGCSC 64.95%.</p>
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<p>Clustering results obtained using different methods on the Pavia University data set with Gaussian noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 36.90%. (<b>c</b>) SSC 36.79%. (<b>d</b>) S4C 42.51%. (<b>e</b>) EDSC 46.97%. (<b>f</b>) EGCSC 51.19%. (<b>g</b>) EKGCSC. (<b>h</b>) SSAKGCSC 67.34%.</p>
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<p>Clustering results obtained using different methods on the Pavia Center data set with Gaussian noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 31.63%. (<b>c</b>) SSC 37.81%. (<b>d</b>) S4C 49.51%. (<b>e</b>) EDSC 47.57%. (<b>f</b>) EGCSC 48.44%. (<b>g</b>) EKGCSC 33.15%. (<b>h</b>) MEKGCSC 88.55%.</p>
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<p>Clustering results obtained using different methods on the SalinasA data set with Gaussian noise and salt and pepper noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 44.52%. (<b>c</b>) SSC 47.06%. (<b>d</b>) S4C 50.95%. (<b>e</b>) EDSC 60.79%. (<b>f</b>) EGCSC 62.23%. (<b>g</b>) EKGCSC 59.97%. (<b>h</b>) SSAKGCSC 88.28%.</p>
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<p>Clustering results obtained using different methods on the Indian Pines corrected data set with Gaussian noise and salt and pepper noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 41.08%. (<b>c</b>) SSC 43.86%. (<b>d</b>) S4C 51.33%. (<b>e</b>) EDSC 52.24%. (<b>f</b>) EGCSC 54.68%. (<b>g</b>) EKGCSC 52.49%. (<b>h</b>) SSAKGCSC 64.50%.</p>
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<p>Clustering results obtained using different methods on the Pavia University data set with Gaussian noise and salt and pepper noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 37.22%. (<b>c</b>) SSC 38.79%. (<b>d</b>) S4C 43.30%. (<b>e</b>) EDSC 47.91%. (<b>f</b>) EGCSC 50.92%. (<b>g</b>) EKGCSC. (<b>h</b>) SSAKGCSC 69.67%.</p>
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<p>Clustering results obtained using different methods on the Pavia Center data set with Gaussian noise and salt and pepper noise. (<b>a</b>) Ground truth. (<b>b</b>) LRSC 34.17%. (<b>c</b>) SSC 42.89%. (<b>d</b>) S4C 47.94%. (<b>e</b>) EDSC 48.46%. (<b>f</b>) EGCSC 52.03%. (<b>g</b>) EKGCSC 31.82%. (<b>h</b>) MEKGCSC 88.72%.</p>
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<p>Clustering OA and CPV under a varying number of PCs on SalinasA, Indian Pines, Pavia Center and Pavia University data sets.</p>
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20 pages, 39148 KiB  
Article
Semantic Segmentation Using Pixel-Wise Adaptive Label Smoothing via Self-Knowledge Distillation for Limited Labeling Data
by Sangyong Park, Jaeseon Kim and Yong Seok Heo
Sensors 2022, 22(7), 2623; https://doi.org/10.3390/s22072623 - 29 Mar 2022
Cited by 5 | Viewed by 3847
Abstract
To achieve high performance, most deep convolutional neural networks (DCNNs) require a significant amount of training data with ground truth labels. However, creating ground-truth labels for semantic segmentation requires more time, human effort, and cost compared with other tasks such as classification and [...] Read more.
To achieve high performance, most deep convolutional neural networks (DCNNs) require a significant amount of training data with ground truth labels. However, creating ground-truth labels for semantic segmentation requires more time, human effort, and cost compared with other tasks such as classification and object detection, because the ground-truth label of every pixel in an image is required. Hence, it is practically demanding to train DCNNs using a limited amount of training data for semantic segmentation. Generally, training DCNNs using a limited amount of data is problematic as it easily results in a decrease in the accuracy of the networks because of overfitting to the training data. Here, we propose a new regularization method called pixel-wise adaptive label smoothing (PALS) via self-knowledge distillation to stably train semantic segmentation networks in a practical situation, in which only a limited amount of training data is available. To mitigate the problem caused by limited training data, our method fully utilizes the internal statistics of pixels within an input image. Consequently, the proposed method generates a pixel-wise aggregated probability distribution using a similarity matrix that encodes the affinities between all pairs of pixels. To further increase the accuracy, we add one-hot encoded distributions with ground-truth labels to these aggregated distributions, and obtain our final soft labels. We demonstrate the effectiveness of our method for the Cityscapes dataset and the Pascal VOC2012 dataset using limited amounts of training data, such as 10%, 30%, 50%, and 100%. Based on various quantitative and qualitative comparisons, our method demonstrates more accurate results compared with previous methods. Specifically, for the Cityscapes test set, our method achieved mIoU improvements of 0.076%, 1.848%, 1.137%, and 1.063% for 10%, 30%, 50%, and 100% training data, respectively, compared with the method of the cross-entropy loss using one-hot encoding with ground truth labels. Full article
(This article belongs to the Section Sensor Networks)
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<p>A schematic flowchart of our method. Our method aggregates distributions based on pair-wise feature similarity and generates a pixel-wise soft label by weighted sum of a one-hot encoding with ground truth label and the aggregated distribution for each pixel according to training iteration.</p>
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<p>Comparative results of methods trained using various ratios of limited training data. Results of various ratios of training data including 10%, 30%, 50%, and 100% are shown. Value below each result represents mIoU.</p>
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<p>Overview of the proposed method, which is categorized into training and test paths. Blue and red arrows represent training and test paths, respectively.</p>
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<p>Process of our PALS module.</p>
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<p>Process of PA module, where <math display="inline"><semantics> <mrow> <mo>↓</mo> <mo>(</mo> <mo>·</mo> <mo>)</mo> </mrow> </semantics></math> denotes the downsampling operation.</p>
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<p>Results of the comparison of various methods using limited training data for DeepLab-V3+ [<a href="#B10-sensors-22-02623" class="html-bibr">10</a>] with the Xception65 [<a href="#B76-sensors-22-02623" class="html-bibr">76</a>] network on the Cityscapes dataset. (<b>a</b>) Input image. (<b>b</b>) Ground-truth image. (<b>c</b>) CE [<a href="#B10-sensors-22-02623" class="html-bibr">10</a>] result. (<b>d</b>) CP [<a href="#B22-sensors-22-02623" class="html-bibr">22</a>] result. (<b>e</b>) LS [<a href="#B20-sensors-22-02623" class="html-bibr">20</a>] result. (<b>f</b>) Our result.</p>
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<p>Results of the comparison of various methods using limited training data for DeepLab-V3+ [<a href="#B10-sensors-22-02623" class="html-bibr">10</a>] with the ResNet18 [<a href="#B77-sensors-22-02623" class="html-bibr">77</a>] network on the Cityscapes dataset. (<b>a</b>) Input image. (<b>b</b>) Ground-truth image. (<b>c</b>) CE [<a href="#B10-sensors-22-02623" class="html-bibr">10</a>] result. (<b>d</b>) CP [<a href="#B22-sensors-22-02623" class="html-bibr">22</a>] result. (<b>e</b>) LS [<a href="#B20-sensors-22-02623" class="html-bibr">20</a>] result. (<b>f</b>) Our result.</p>
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<p>Results of the comparison of various methods using limited training data for DeepLab-V3+ [<a href="#B10-sensors-22-02623" class="html-bibr">10</a>] with the Xception65 [<a href="#B76-sensors-22-02623" class="html-bibr">76</a>] network on the Pascal VOC2012 dataset. (<b>a</b>) Input image. (<b>b</b>) Ground-truth image. (<b>c</b>) CE [<a href="#B10-sensors-22-02623" class="html-bibr">10</a>] result. (<b>d</b>) CP [<a href="#B22-sensors-22-02623" class="html-bibr">22</a>] result. (<b>e</b>) LS [<a href="#B20-sensors-22-02623" class="html-bibr">20</a>] result. (<b>f</b>) Our result.</p>
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13 pages, 794 KiB  
Article
Spectrality of a Class of Self-Affine Measures with Prime Determinant
by Mingshu Yang
Symmetry 2022, 14(2), 243; https://doi.org/10.3390/sym14020243 - 26 Jan 2022
Viewed by 1732
Abstract
We study the spectrality of a class of self-affine measures with prime determinant. Spectral measures are connected with fractal geometry that shows some kind of geometrical self-similarity under magnification. To make the self-affine measure becomes a spectral measure with lattice spectrum, we provide [...] Read more.
We study the spectrality of a class of self-affine measures with prime determinant. Spectral measures are connected with fractal geometry that shows some kind of geometrical self-similarity under magnification. To make the self-affine measure becomes a spectral measure with lattice spectrum, we provide two new sufficient conditions related to the elements of digit set and zero set, respectively. The two sufficient conditions are more precise and easier to be verified as compared with the previous research. Moreover, these conditions offer a fresh perspective on a conjecture of Lagarias and Wang. Full article
(This article belongs to the Section Mathematics)
11 pages, 1665 KiB  
Article
NbX: Machine Learning-Guided Re-Ranking of Nanobody–Antigen Binding Poses
by Chunlai Tam, Ashutosh Kumar and Kam Y. J. Zhang
Pharmaceuticals 2021, 14(10), 968; https://doi.org/10.3390/ph14100968 - 24 Sep 2021
Cited by 7 | Viewed by 4515
Abstract
Modeling the binding pose of an antibody is a prerequisite to structure-based affinity maturation and design. Without knowing a reliable binding pose, the subsequent structural simulation is largely futile. In this study, we have developed a method of machine learning-guided re-ranking of antigen [...] Read more.
Modeling the binding pose of an antibody is a prerequisite to structure-based affinity maturation and design. Without knowing a reliable binding pose, the subsequent structural simulation is largely futile. In this study, we have developed a method of machine learning-guided re-ranking of antigen binding poses of nanobodies, the single-domain antibody which has drawn much interest recently in antibody drug development. We performed a large-scale self-docking experiment of nanobody–antigen complexes. By training a decision tree classifier through mapping a feature set consisting of energy, contact and interface property descriptors to a measure of their docking quality of the refined poses, significant improvement in the median ranking of native-like nanobody poses by was achieved eightfold compared with ClusPro and an established deep 3D CNN classifier of native protein–protein interaction. We further interpreted our model by identifying features that showed relatively important contributions to the prediction performance. This study demonstrated a useful method in improving our current ability in pose prediction of nanobodies. Full article
(This article belongs to the Section Biopharmaceuticals)
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<p>Comparison of re-ranking of native-like Nb pose between NbX, DOVE and ClusPro in (<b>A</b>) test set and (<b>B</b>) training set. Whole populations (N<sub>test</sub> = 200 and N<sub>train</sub> = 660) of ranking of native-like Nb pose from the 5-fold cross-validated were shown in boxplots. The upper and lower whiskers represent 95th and 5th percentile ranking, respectively. The dots represent outliers. Annotations for p value in <span class="html-italic">t</span>-Test are as follow, ns: 0.05 &lt; <span class="html-italic">p</span> ≤ 1.00; **** <span class="html-italic">p</span> ≤ 0.0001.</p>
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<p>Re-ranking performance of NbX in different cutoffs of pairwise structural alignment quality score. Whole populations of ranking of the native-like nanobody pose from the 5-fold cross-validated test sets were plotted. Annotations for p value in <span class="html-italic">t</span>-Test are as follow, ns: 0.05 &lt; <span class="html-italic">p</span> ≤ 1.00; ***: 0.0001 &lt; <span class="html-italic">p</span> ≤ 0.001; **** <span class="html-italic">p</span> ≤ 0.0001.</p>
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<p>Summary plots of SHAP values of important features contributed to the prediction of NbX in the best single model. (<b>A</b>) Scatter plot of SHAP values including directionality of contribution to the predicted probability of nativeness. Each dot represents one prediction in the test set. On the horizontal axis representing the SHAP value, a positive SHAP value represents a positive contribution to the predicted probability and vice versa. The color of dots represents the feature values relative to the maximum and minimum of that feature, which are colored red and blue, respectively. (<b>B</b>) Bar plot of mean (|SHAP|) of the important features, which represents the averaged importance of each feature to the test set prediction overall regardless of the directionality of the contribution. ChainA represents Ag and chainH represents Nb.</p>
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<p>Overall workflow of NbX from data collection to modeling.</p>
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20 pages, 3391 KiB  
Article
Thermodynamics and Intermolecular Interactions of Nicotinamide in Neat and Binary Solutions: Experimental Measurements and COSMO-RS Concentration Dependent Reactions Investigations
by Piotr Cysewski, Maciej Przybyłek, Anna Kowalska and Natalia Tymorek
Int. J. Mol. Sci. 2021, 22(14), 7365; https://doi.org/10.3390/ijms22147365 - 8 Jul 2021
Cited by 19 | Viewed by 3943
Abstract
In this study, the temperature-dependent solubility of nicotinamide (niacin) was measured in six neat solvents and five aqueous-organic binary mixtures (methanol, 1,4-dioxane, acetonitrile, DMSO and DMF). It was discovered that the selected set of organic solvents offer all sorts of solvent effects, including [...] Read more.
In this study, the temperature-dependent solubility of nicotinamide (niacin) was measured in six neat solvents and five aqueous-organic binary mixtures (methanol, 1,4-dioxane, acetonitrile, DMSO and DMF). It was discovered that the selected set of organic solvents offer all sorts of solvent effects, including co-solvent, synergistic, and anti-solvent features, enabling flexible tuning of niacin solubility. In addition, differential scanning calorimetry was used to characterize the fusion thermodynamics of nicotinamide. In particular, the heat capacity change upon melting was measured. The experimental data were interpreted by means of COSMO-RS-DARE (conductor-like screening model for realistic solvation–dimerization, aggregation, and reaction extension) for concentration dependent reactions. The solute–solute and solute–solvent intermolecular interactions were found to be significant in all of the studied systems, which was proven by the computed mutual affinity of the components at the saturated conditions. The values of the Gibbs free energies of pair formation were derived at an advanced level of theory (MP2), including corrections for electron correlation and zero point vibrational energy (ZPE). In all of the studied systems the self-association of nicotinamide was found to be a predominant intermolecular complex, irrespective of the temperature and composition of the binary system. The application of the COSMO-RS-DARE approach led to a perfect match between the computed and measured solubility data, by optimizing the parameter of intermolecular interactions. Full article
(This article belongs to the Special Issue Structure, Energy, and Dynamics of Molecular Interactions)
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<p>Measured temperature trends of solid and melt states of nicotinamide, where <math display="inline"><semantics> <mrow> <mo>Δ</mo> <msubsup> <mi>C</mi> <mi>p</mi> <mrow> <mi>f</mi> <mi>u</mi> <mi>s</mi> </mrow> </msubsup> <mrow> <mo>(</mo> <mi>T</mi> <mo>)</mo> </mrow> <mo>=</mo> <msub> <mi>C</mi> <mi>p</mi> </msub> <mrow> <mo>(</mo> <mi>l</mi> <mo>)</mo> </mrow> <mrow> <mo>(</mo> <mi mathvariant="normal">T</mi> <mo>)</mo> </mrow> <mo>−</mo> <msub> <mi>C</mi> <mi>p</mi> </msub> <mrow> <mo>(</mo> <mi>s</mi> <mo>)</mo> </mrow> <mrow> <mo>(</mo> <mi mathvariant="normal">T</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> stands for the heat capacity difference between a supercooled liquid and solid.</p>
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<p>Temperature related changes of thermodynamic functions of nicotinamide fusion.</p>
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<p>Solubility of nicotinamide in pure methanol and water estimated by this work (a) and according to ref. [<a href="#B17-ijms-22-07365" class="html-bibr">17</a>] (dataset (b)) and ref [<a href="#B19-ijms-22-07365" class="html-bibr">19</a>] (dataset (c)).</p>
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<p>Characteristics of non-ideality of nicotinamide solubility in neat and binary solvents. (<b>a</b>) Comparison of ideal solubility measured at temperatures 25 °C and 40 °C; (<b>b</b>) solvent ratio dependent trends of activity coefficients of nicotinamide in studied binary solvents mixtures at 25 °C (solid black symbols) and 40 °C (grey open symbols).</p>
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<p>Results of the instrumental characteristics of pure nicotinamide and the sediments obtained after solubility measurements in pure solvents (<b>a</b>) FTIR-ATR spectra (<b>b</b>) DSC thermograms.</p>
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<p>Graphical representation of pseudo-conformers included in the COSMO-RS-DARE computations of nicotinamide interactions with itself and each of the solvent molecules in the studied systems.</p>
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<p>Concentration dependent nicotinamide affinity in aqueous binary solution of studied organic solvents (x<sub>2</sub>* denotes mole fraction of organic solvent in solute free solutions).</p>
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<p>Predicted solubility of nicotinamide confronted with experimental data.</p>
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<p>Concentration dependent distribution of optimized values of nicotinamide association enthalpy in the studied binary solutions (x<sub>2</sub> * denotes mole fraction of organic solvent in solute free solutions).</p>
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26 pages, 7445 KiB  
Article
Novel Approach to Tooth Chemistry. Quantification of the Dental-Enamel Junction
by Andrzej Kuczumow, Renata Chałas, Jakub Nowak, Janusz Lekki, Katarzyna Sarna-Boś, Wojciech Smułek and Maciej Jarzębski
Int. J. Mol. Sci. 2021, 22(11), 6003; https://doi.org/10.3390/ijms22116003 - 2 Jun 2021
Cited by 13 | Viewed by 3065
Abstract
The dentin-enamel junction (DEJ) is known for its special role in teeth. Several techniques were applied for the investigation of the DEJ in human sound molar teeth. The electron (EPMA) and proton (PIXE) microprobes gave consistent indications about the variability of elemental concentrations [...] Read more.
The dentin-enamel junction (DEJ) is known for its special role in teeth. Several techniques were applied for the investigation of the DEJ in human sound molar teeth. The electron (EPMA) and proton (PIXE) microprobes gave consistent indications about the variability of elemental concentrations on this boundary. The locally increased and oscillating concentrations of Mg and Na were observed in the junction, in the layer adhering to the enamel and covering roughly half of the DEJ width. The chemical results were compared with the optical profiles of the junction. Our chemical and optical results were next compared with the micromechanical results (hardness, elastic modulus, friction coefficient) available in the world literature. A strong correlation of both result sets was proven, which testifies to the self-affinity of the junction structures for different locations and even for different kinds of teeth and techniques applied for studies. Energetic changes in tooth strictly connected with crystallographic transformations were calculated, and the minimum energetic status was discovered for DEJ zone. Modeling of both walls of the DEJ from optical data was demonstrated. Comparing the DEJ in human teeth with the same structure found in dinosaur, shark, and alligator teeth evidences the universality of dentin enamel junction in animal world. The paper makes a contribution to better understanding the joining of the different hard tissues. Full article
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Figure 1

Figure 1
<p>(<b>a</b>) Results of EPMA measurements along the DEJ zone. The direction is from the enamel (left) towards the dentin and always the same direction is preserved in the next figures (where relevant), and the length is equal to 250 µm. 1 step = 1 µm. (<b>b</b>) Sequence of C and Mg variability, in majority cases inversely directed. (<b>c</b>) Outline of the DEJ space with optical signal and in parallel by two spectral signals of P and C. On multiscale figures the numerical markers were introduced where the first number denotes x-axes, calculated in the system down-up and the second one y-axes, calculated from left to right side of the figure.</p>
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<p>(<b>a</b>) Results of EPMA measurements along the DEJ zone. The direction is from the enamel (left) towards the dentin and always the same direction is preserved in the next figures (where relevant), and the length is equal to 250 µm. 1 step = 1 µm. (<b>b</b>) Sequence of C and Mg variability, in majority cases inversely directed. (<b>c</b>) Outline of the DEJ space with optical signal and in parallel by two spectral signals of P and C. On multiscale figures the numerical markers were introduced where the first number denotes x-axes, calculated in the system down-up and the second one y-axes, calculated from left to right side of the figure.</p>
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<p>(<b>a</b>) Results of µ-PIXE measurements. 1 step = 1.25 µm. (<b>b</b>) Outline of the DEJ space with optical signal and with P signal, for left boundary only; please observe missing boundary DEJ-dentin due to the air path of measurements and inability of detection of carbon. (<b>c</b>) Parallelism of Mg measurements with the use of EPMA and µ-PIXE.</p>
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<p>(<b>a</b>) Results of µ-PIXE measurements. 1 step = 1.25 µm. (<b>b</b>) Outline of the DEJ space with optical signal and with P signal, for left boundary only; please observe missing boundary DEJ-dentin due to the air path of measurements and inability of detection of carbon. (<b>c</b>) Parallelism of Mg measurements with the use of EPMA and µ-PIXE.</p>
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<p>(<b>a</b>) Results of µ-Raman measurements around the DEJ. PO<sub>4</sub><sup>3−</sup>-ν<sub>1</sub> oscillation; CH<sub>2</sub>-ν symmetric oscillation; NH line; CO<sub>3</sub><sup>2−</sup>, sub. B; 1 step = 1.61 µm; (<b>b</b>) Outline of DEJ space with optical and Raman PO<sub>4</sub><sup>3−</sup> and CH<sub>2</sub> signals. (<b>c</b>) Divergent spatial profiles of PO<sub>4</sub><sup>3−</sup> and HPO<sub>4</sub><sup>2−</sup> ions, with visible DEJ.</p>
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<p>(<b>a</b>) Results of µ-Raman measurements around the DEJ. PO<sub>4</sub><sup>3−</sup>-ν<sub>1</sub> oscillation; CH<sub>2</sub>-ν symmetric oscillation; NH line; CO<sub>3</sub><sup>2−</sup>, sub. B; 1 step = 1.61 µm; (<b>b</b>) Outline of DEJ space with optical and Raman PO<sub>4</sub><sup>3−</sup> and CH<sub>2</sub> signals. (<b>c</b>) Divergent spatial profiles of PO<sub>4</sub><sup>3−</sup> and HPO<sub>4</sub><sup>2−</sup> ions, with visible DEJ.</p>
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<p>(<b>a</b>) Parallel delimitation of the DEJ zone with the EPMA measurements and micromechanical results. The micro-hardness and micro-friction results are adopted from Marshall et al. [<a href="#B12-ijms-22-06003" class="html-bibr">12</a>]. The horizontal dashed line delimits the width of the DEJ. (<b>b</b>) Superposition of Young modulus on the optical outline of DEJ. (<b>c</b>) Superposition of changes in density from Weatherell [<a href="#B35-ijms-22-06003" class="html-bibr">35</a>] on P measurement from PIXE.</p>
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<p>(<b>a</b>) Parallel delimitation of the DEJ zone with the EPMA measurements and micromechanical results. The micro-hardness and micro-friction results are adopted from Marshall et al. [<a href="#B12-ijms-22-06003" class="html-bibr">12</a>]. The horizontal dashed line delimits the width of the DEJ. (<b>b</b>) Superposition of Young modulus on the optical outline of DEJ. (<b>c</b>) Superposition of changes in density from Weatherell [<a href="#B35-ijms-22-06003" class="html-bibr">35</a>] on P measurement from PIXE.</p>
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<p>Comparison of the linear fits to the correlation relationships between relative values of density and Ca (solid line); Young modulus and Ca (dotted line); hardness and Ca (dot-drop line). Relevant equations are: RDen = −1.27 + 2.287 × [RCa]; RYM = −4.68 + 5.678 × [RCa]; RH = −6.61 + 7.609 × [RCa].</p>
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<p>(<b>a</b>) Variability of crystallographic “a” parameter inside the tooth. (<b>b</b>) Generally faint variability of “c” parameter, even bearing in mind individual jumps. (<b>c</b>) Superposition of variability of parameter “a” on optical and chemical outline of the DEJ. Arrows show how the profile of “a” would be narrowed in the case of a better spatial resolution of the XRD system. (<b>d</b>) Energetic profile of whole enamel, DEJ, and fragment of dentin.</p>
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<p>(<b>a</b>) Variability of crystallographic “a” parameter inside the tooth. (<b>b</b>) Generally faint variability of “c” parameter, even bearing in mind individual jumps. (<b>c</b>) Superposition of variability of parameter “a” on optical and chemical outline of the DEJ. Arrows show how the profile of “a” would be narrowed in the case of a better spatial resolution of the XRD system. (<b>d</b>) Energetic profile of whole enamel, DEJ, and fragment of dentin.</p>
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<p>(<b>a</b>) Variability of crystallographic “a” parameter inside the tooth. (<b>b</b>) Generally faint variability of “c” parameter, even bearing in mind individual jumps. (<b>c</b>) Superposition of variability of parameter “a” on optical and chemical outline of the DEJ. Arrows show how the profile of “a” would be narrowed in the case of a better spatial resolution of the XRD system. (<b>d</b>) Energetic profile of whole enamel, DEJ, and fragment of dentin.</p>
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<p>(<b>a</b>) Correlation between the drop in the phosphor concentration (EPMA) and the hardness, with the perfect linear fit to the points (P concentration from our studies, hardness adopted from Marshall et al., [<a href="#B12-ijms-22-06003" class="html-bibr">12</a>], as tailored in <a href="#ijms-22-06003-f004" class="html-fig">Figure 4</a>). (<b>b</b>) Correlation between the increase in the CH<sub>2</sub> concentration from Raman measurements and the friction coefficient (data from Marshall et al. [<a href="#B12-ijms-22-06003" class="html-bibr">12</a>]), recalculated and combined by us). (<b>c</b>) Correlation between hardness and optical signal. (<b>d</b>) Reconstruction of the DEJ from chemical signals transformed into optical signals using the relevant correlations and its comparison with the real optical signal.</p>
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<p>(<b>a</b>) Correlation between the drop in the phosphor concentration (EPMA) and the hardness, with the perfect linear fit to the points (P concentration from our studies, hardness adopted from Marshall et al., [<a href="#B12-ijms-22-06003" class="html-bibr">12</a>], as tailored in <a href="#ijms-22-06003-f004" class="html-fig">Figure 4</a>). (<b>b</b>) Correlation between the increase in the CH<sub>2</sub> concentration from Raman measurements and the friction coefficient (data from Marshall et al. [<a href="#B12-ijms-22-06003" class="html-bibr">12</a>]), recalculated and combined by us). (<b>c</b>) Correlation between hardness and optical signal. (<b>d</b>) Reconstruction of the DEJ from chemical signals transformed into optical signals using the relevant correlations and its comparison with the real optical signal.</p>
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<p>(<b>a</b>) The internal structure of the DEJ. Hardness and friction lines delimit here the DEJ zone. Mg is from EPMA and PIXE measurements and Na from EPMA measurements. Measurements were not made along the same line, but general tendencies are common. Values on y-axes were uniformized for better observation. (<b>b</b>) Superposition of the NH signal profile and the ratio of NH/CH<sub>2</sub> profiles on the optical outline of the DEJ and Raman measurements. (<b>c</b>) Profiles of single amino acids present in collagen bundles within DEJ. (<b>d</b>) Variabilities of ratios of NH/CH<sub>2</sub> and 581/(581 + 590) Raman lines mirroring left and right zones adhering to the DEJ.</p>
Full article ">Figure 8 Cont.
<p>(<b>a</b>) The internal structure of the DEJ. Hardness and friction lines delimit here the DEJ zone. Mg is from EPMA and PIXE measurements and Na from EPMA measurements. Measurements were not made along the same line, but general tendencies are common. Values on y-axes were uniformized for better observation. (<b>b</b>) Superposition of the NH signal profile and the ratio of NH/CH<sub>2</sub> profiles on the optical outline of the DEJ and Raman measurements. (<b>c</b>) Profiles of single amino acids present in collagen bundles within DEJ. (<b>d</b>) Variabilities of ratios of NH/CH<sub>2</sub> and 581/(581 + 590) Raman lines mirroring left and right zones adhering to the DEJ.</p>
Full article ">Figure 8 Cont.
<p>(<b>a</b>) The internal structure of the DEJ. Hardness and friction lines delimit here the DEJ zone. Mg is from EPMA and PIXE measurements and Na from EPMA measurements. Measurements were not made along the same line, but general tendencies are common. Values on y-axes were uniformized for better observation. (<b>b</b>) Superposition of the NH signal profile and the ratio of NH/CH<sub>2</sub> profiles on the optical outline of the DEJ and Raman measurements. (<b>c</b>) Profiles of single amino acids present in collagen bundles within DEJ. (<b>d</b>) Variabilities of ratios of NH/CH<sub>2</sub> and 581/(581 + 590) Raman lines mirroring left and right zones adhering to the DEJ.</p>
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<p>Outline of the DEJ zone for an unidentified American dinosaur, a shark, and an alligator.</p>
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20 pages, 3920 KiB  
Article
Towards Embedded Computation with Building Materials
by Dawid Przyczyna, Maciej Suchecki, Andrew Adamatzky and Konrad Szaciłowski
Materials 2021, 14(7), 1724; https://doi.org/10.3390/ma14071724 - 31 Mar 2021
Cited by 7 | Viewed by 2553
Abstract
We present results showing the capability of concrete-based information processing substrate in the signal classification task in accordance with in materio computing paradigm. As the Reservoir Computing is a suitable model for describing embedded in materio computation, we propose that this type of [...] Read more.
We present results showing the capability of concrete-based information processing substrate in the signal classification task in accordance with in materio computing paradigm. As the Reservoir Computing is a suitable model for describing embedded in materio computation, we propose that this type of presented basic construction unit can be used as a source for “reservoir of states” necessary for simple tuning of the readout layer. We present an electrical characterization of the set of samples with different additive concentrations followed by a dynamical analysis of selected specimens showing fingerprints of memfractive properties. As part of dynamic analysis, several fractal dimensions and entropy parameters for the output signal were analyzed to explore the richness of the reservoir configuration space. In addition, to investigate the chaotic nature and self-affinity of the signal, Lyapunov exponents and Detrended Fluctuation Analysis exponents were calculated. Moreover, on the basis of obtained parameters, classification of the signal waveform shapes can be performed in scenarios explicitly tuned for a given device terminal. Full article
(This article belongs to the Special Issue Advanced Cement and Concrete Composites)
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Graphical abstract

Graphical abstract
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<p>Schematic view of the computing concrete sample (<b>a</b>), pinouts for voltammetric (left) and signal processing experiments (<b>b</b>) and a real photo of an experimental setup (<b>c</b>). WE and CE stands for working and counter electrodes, respectively. IN1 and IN2 are signal input connectors, OUT1 and OUT2 output ones, GND is a common ground.</p>
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<p>Voltamperometric characteristics of undoped concrete sample (top, dark green) and concrete containing various amounts of dopants: M—Metal shavings, S—Antimony sulfoiodide nanowires, SM—1:1 mixture of both dopants. Some samples show pinched hysteresis loops typical for memristive devices (red) whereas the others are of capacitive character (blue). The most pronounced memristive behavior was observed in the case of 10% SM sample, highlighted in yellow.</p>
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<p>Impedance spectra of undoped and metal+semiconductor doped concrete samples: Nyquist plot (<b>a</b>) phase shift angles (<b>b</b>) and Bode plots (<b>c</b>). A simplified equivalent circuit is also shown. The linear Warburg component at low frequencies is visible only in the case of the undoped sample, whereas increased doping is correlated with a decrease of impedance results as well as with significant curvature of the low-frequency arm in Nyquist plots.</p>
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<p>Results for time delay and embedding dimension calculations for all-time series recorded for pristine and doped (10%MS) concrete samples. Graphs present results from Delayed Mutual Information approach (<b>a</b>), False Nearest Neighbors test (<b>b</b>) and Average False Neighbors method (<b>c</b>). Calculated time delay τ = 4 (first minima of DMI, averaged over all data sets), whereas suitable embedding dimension equals four (0% of FNN in all tests and saturation of E1 &amp; E2 in AFN). Descriptions of test criteria can be found in the text.</p>
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<p>A set of dynamics indices for recorded time series. Maximum Lyapunov exponent for of a time series recorded for different input frequencies/waveforms (<b>a</b>). Detrended fluctuation analysis performed for time series recorded for different input frequencies/waveforms (<b>b</b>). Correlation dimension of a time series calculated for different input frequencies/waveforms (<b>c</b>). Arrows indicate the direction of changes upon doping.</p>
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<p>A set of dynamics indices for recorded time series. Sample entropy for different input frequencies/waveforms (<b>a</b>). Permutation entropy for different input frequencies/waveforms combinations (<b>b</b>). Values of Katz fractal dimension score for doped and un-doped sample different input frequencies/waveforms (<b>c</b>). Arrows indicate the direction of changes upon doping.</p>
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<p>Petrosian fractal dimension for time series collected from OUT1 (<b>a</b>) and OUT2 (<b>b</b>) device terminals. Black arrows indicate trends for OUT1, whereas red arrows for OUT2 (cf. <a href="#materials-14-01724-f001" class="html-fig">Figure 1</a> for terminal markings).</p>
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<p>Parallel coordinate plot for all-time series and selected dynamic criteria: detrended fluctuation exponent (<span class="html-italic">α</span>), sample entropy (<span class="html-italic">S<sub>s</sub></span>), Petrosian fractal dimension (<span class="html-italic">D<sub>P</sub></span>) and permutation entropy (<span class="html-italic">S<sub>p</sub></span>). Detrended fluctuation exponent can serve as a classification factor for the concrete doping state, whereas permutation entropy significantly classifies time series according to their waveforms.</p>
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<p>A scheme of a dual concrete-based reservoir computing system used for waveform classification.</p>
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