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14 pages, 3475 KiB  
Article
Deep Eutectic Solvent-Assisted Synthesis of Ni–Graphene Composite Supported on Screen-Printed Electrodes for Biogenic Amine Detection
by Aleksandra Levshakova, Maria Kaneva, Ruzanna Ninayan, Evgenii Borisov, Evgenii Satymov, Alexander Shmalko, Lev Logunov, Aleksandr Kuchmizhak, Yuri N. Kulchin, Alina Manshina and Evgeniia Khairullina
Materials 2025, 18(2), 425; https://doi.org/10.3390/ma18020425 - 17 Jan 2025
Viewed by 365
Abstract
Deep eutectic solvents (DES) have emerged as versatile, sustainable media for the synthesis of nanomaterials due to their low toxicity, tunability, and biocompatibility. This study develops a one-step method to modify commercially available screen-printed electrodes (SPE) using laser-induced pyrolysis of DES, consisting of [...] Read more.
Deep eutectic solvents (DES) have emerged as versatile, sustainable media for the synthesis of nanomaterials due to their low toxicity, tunability, and biocompatibility. This study develops a one-step method to modify commercially available screen-printed electrodes (SPE) using laser-induced pyrolysis of DES, consisting of choline chloride and tartaric acid with dissolved nickel acetate and dispersed graphene. The electrodes were patterned using a 532 nm continuous-wave laser for the in situ formation of Ni nanoparticles decorated on graphene sheets directly on the SPE surface (Ni-G/SPE). The synthesis parameters, specifically laser power and graphene concentration, were optimized using the Nelder–Mead method to produce modified Ni-G/SPEs with maximized electrochemical response to dopamine. Electrochemical characterization of the developed sensor by differential pulse voltammetry revealed its broad linear detection range from 0.25 to 100 μM and high sensitivity with a low detection limit of 0.095 μM. These results highlight the potential of laser-assisted DES synthesis to advance electrochemical sensing technologies, particularly for the detection of biogenic amines. Full article
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Graphical abstract

Graphical abstract
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<p>Electrode fabrication process and electrochemical testing.</p>
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<p>Nelder–Mead optimization of the Ni-G/SPE electrode electrochemical performance (maximal current) through variation in laser power and graphene concentration. Representative SEM images of the Ni-G/SPE samples synthesized in simplex vertices (differently colored points 1–8 on the central graph) at different values of laser power and concentration of graphene dispersion in DES.</p>
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<p>SEM images showing the morphology of the optimized Ni-G/SPE electrode (Sample 9) visualized at different magnifications (<b>a</b>–<b>c</b>), X-ray photoelectron spectra of the Ni 2p and O1s (<b>d</b>), N 1s and C 1s (<b>e</b>) regions as well as Raman spectra of SPE and Ni-G/SPE electrodes, graphene dispersion (<b>f</b>).</p>
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<p>(<b>a</b>) CV curves of SPE and Ni-G/SPE in 0.1 M PBS without additives (dashed line) and in the presence of 50 μM DA (solid line), (<b>b</b>) DPV of the Ni-G/SPE electrode measured with the addition of various concentrations of DA, (<b>c</b>) Correlations of DA oxidation currents with respective concentrations, (<b>d</b>) DPV of the Ni-G/SPE in small volume samples (insert: Correlations of DA oxidation currents with respective concentrations).</p>
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15 pages, 5577 KiB  
Article
Reducing Product Loss Through Ventilation in Bourbon Maturation Warehouses
by Steven J. Schafrik, Michael W. Long, Zachary E. Wedding, Benjamin M. Diddle and Zach Agioutantis
Sustainability 2025, 17(2), 699; https://doi.org/10.3390/su17020699 (registering DOI) - 17 Jan 2025
Viewed by 380
Abstract
The aging process of bourbon within rickhouses is influenced by various environmental factors, including temperature, humidity, air flow, and air quality. Most rickhouses are not climate-controlled, and natural ventilation is a major contributor to airflow. The corrosion of the steel hoops on bourbon [...] Read more.
The aging process of bourbon within rickhouses is influenced by various environmental factors, including temperature, humidity, air flow, and air quality. Most rickhouses are not climate-controlled, and natural ventilation is a major contributor to airflow. The corrosion of the steel hoops on bourbon barrels occurs due to the presence of ethyl alcohol vapors and has become an issue for the distilling industry. The loss of a barrel or product is the loss of all of the energy and materials that went into the distillation, as well as the removal of the barrel from the secondary market. Despite the large economic and sustainability impact of barrel losses, there is limited published research with respect to corrective actions. This paper investigates airflow patterns within a bourbon rickhouse using a combination of differential pressure surveys and smoke tracing techniques to understand how natural ventilation impacts the aging process and potential for corrosion. A newly constructed rickhouse was surveyed using a micro-manometer to measure differential pressure and a sheet laser with smoke to visualize airflow. This study revealed significant zones of stagnant air and minimal recirculation within the ricks, which are the structures that hold the bourbon barrels. Airflow was found to primarily enter through windows and ground vents, moving along the walkways before exiting through other openings, with minimal penetration into the ricks. Differential pressure measurements generally indicated a lack of significant airflow, while smoke tracing showed that air entering the side of the building does not circulate into the ricks. This lack of airflow promotes the separation of ethyl alcohol vapor due to density, leading to its accumulation on the floor of the ricks. The findings of this study highlight the need to consider how rickhouse design impacts airflow and the potential for the corrosion of metal hoops on barrels due to the presence of ethyl alcohol vapor, and provide insight into optimizing the ventilation of rickhouses for more efficient and sustainable bourbon maturation. Full article
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Figure 1
<p>Differential Pressure Measurement Locations.</p>
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<p>Smoke Tracing Experimental Setup.</p>
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<p>Smoke Tracing Locations.</p>
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<p>Main Entrance Smoke Test.</p>
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<p>Windows and Ground Vent Smoke Test.</p>
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<p>Perpendicular Angle for Windows and Ground Vent Smoke Test.</p>
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<p>First Interior Rick Smoke Test.</p>
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<p>Second Interior Rick Smoke Test.</p>
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<p>Third Level Smoke Test.</p>
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<p>Rickhouse Section View Airflow Patterns.</p>
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<p>Density Zones of a Rick (Figure not drawn to scale).</p>
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31 pages, 31280 KiB  
Article
Three-Dimensional Digital Documentation for the Conservation of the Prambanan Temple Cluster Using Guided Multi-Sensor Techniques
by Anindya Sricandra Prasidya, Irwan Gumilar, Irwan Meilano, Ikaputra Ikaputra, Rochmad Muryamto and Erlyna Nour Arrofiqoh
Heritage 2025, 8(1), 32; https://doi.org/10.3390/heritage8010032 - 16 Jan 2025
Viewed by 379
Abstract
The Prambanan Temple cluster is a world heritage site that has significant value for humanity, a multiple zone cluster arrangement of highly ornamented towering temples, and a Hindu architectural pattern design. It lies near the Opak Fault, at the foothills of Mount Merapi, [...] Read more.
The Prambanan Temple cluster is a world heritage site that has significant value for humanity, a multiple zone cluster arrangement of highly ornamented towering temples, and a Hindu architectural pattern design. It lies near the Opak Fault, at the foothills of Mount Merapi, on an unstable ground layer, and is surrounded by human activities in Yogyakarta, Indonesia. The site’s vulnerability implies the necessity of 3D digital documentation for its conservation, but its complexity poses difficulties. This work aimed to address this challenge by introducing the utilization of architectural pattern design (APD) to guide multi-sensor line-ups for documentation. First, APDs were established from the literature to derive the associated multiple detail levels; then, multiple sensors and modes of light detection and ranging (Lidar) scanners and photogrammetry were utilized according to their detail requirements and, finally, point cloud data were processed, integrated, assessed, and validated by the proof of the existence of an APD. The internal and external qualities of each sensor result showed the millimeter- to centimeter-range root mean squared error, with the terrestrial laser scanner (TLS) having the best accuracy, followed by aerial close-range and terrestrial-mode photogrammetry and nadiral Lidar and photogrammetry. Two relative cloud distance analyses of every point cloud model to the reference model (TLS) returned the millimeter and centimeter ranges of the mean distance values. Furthermore, visually, every point cloud model from each sensor successfully complemented each other. Therefore, we can conclude that our approach is promising for complex heritage documentation. These results provide a solid foundation for future analyses, particularly in assessing structural vulnerabilities and informing conservation strategies. Full article
(This article belongs to the Special Issue 3D Reconstruction of Cultural Heritage and 3D Assets Utilisation)
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Figure 1
<p>The Prambanan Temple cluster’s location and its concentric layout arrangement.</p>
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<p>The proposed workflow. Solid arrows represent the main data flow, while the dashed arrows represent the supporting data flow.</p>
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<p>Data acquisition concept for three different scale levels. Darker colors represent larger scale levels, while lighter colors represent smaller scale levels. Google Earth and SketchUp 3D Warehouse provide background images for the left and center illustrations, respectively.</p>
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<p>Distribution of GDCPs (<b>a</b>) and FDCPs (<b>b</b>).</p>
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<p>Summary of the quality assessment of each sensor processing result.</p>
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<p>Orthophoto result of the sites that cover the first and second courtyards.</p>
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<p>Registered and georeferenced 3D point clouds from (<b>a</b>) TLS 2020 and (<b>b</b>) TLS 2023.</p>
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<p>Point cloud model from aerial UAV Lidar.</p>
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<p>Dense point cloud model from CR-UAVP integrated with terrestrial photogrammetry.</p>
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<p>Point cloud results from multiple sensors and their combinations (the example of the Brahma Temple). (<b>a</b>) Nadiral UAV Lidar; (<b>b</b>) TLS; (<b>c</b>) CR-UAV photogrammetry; (<b>d</b>) terrestrial photogrammetry; (<b>e</b>) combination of each sensor point clouds. The true color and texture of the temple are presented by (<b>b</b>–<b>d</b>), while (<b>a</b>) only displays the scalar color scale based on the Z coordinate.</p>
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<p>C2C and M3C2 Euclidean distance analysis results of the six main temples of interest.</p>
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<p>C2C results of the corridor part of the Shiva Temple.</p>
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<p>Four sample measurements captured on the base part (Bhurloka) of a single temple.</p>
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<p>Rectangular-based planimetric proportions of the Garuda, Nandhi, and Hamsha Temples.</p>
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<p>The parameter of the Cartesian–cruciform-based planimetric proportion.</p>
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<p>Cartesian–cruciform planimetric proportion of the Shiva, Vishnu, and Brahma Temples (Bhurloka part).</p>
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<p>Cartesian–cruciform planimetric proportion of the Shiva, Vishnu, and Brahma Temples (Bhuvarloka part).</p>
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<p>Cartesian–cruciform planimetric proportion of the Garuda, Nandhi, and Hamsha Temples (Bhuvarloka part).</p>
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<p>Cartesian–cruciform planimetric proportion of the Shiva, Vishnu, and Brahma Temples (Svarloka part).</p>
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<p>Cartesian–cruciform planimetric proportion of the Garuda, Nandhi, and Hamsha Temples (Svarloka part).</p>
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24 pages, 1283 KiB  
Article
Investigation of Exome-Wide Tumor Heterogeneity on Colorectal Tissue-Based Single Cells
by Nikolett Szakállas, Alexandra Kalmár, Barbara Kinga Barták, Zsófia Brigitta Nagy, Gábor Valcz, Tamás Richárd Linkner, Kristóf Róbert Rada, István Takács and Béla Molnár
Int. J. Mol. Sci. 2025, 26(2), 737; https://doi.org/10.3390/ijms26020737 - 16 Jan 2025
Viewed by 260
Abstract
The progression of colorectal cancer is strongly influenced by environmental and genetic conditions. One of the key factors is tumor heterogeneity which is extensively studied by cfDNA and bulk sequencing methods; however, we lack knowledge regarding its effects at the single-cell level. Motivated [...] Read more.
The progression of colorectal cancer is strongly influenced by environmental and genetic conditions. One of the key factors is tumor heterogeneity which is extensively studied by cfDNA and bulk sequencing methods; however, we lack knowledge regarding its effects at the single-cell level. Motivated by this, we aimed to employ an end-to-end single-cell sequencing workflow from tissue-derived sample isolation to exome sequencing. Our main goal was to investigate the heterogeneity patterns by laser microdissecting samples from different locations of a tissue slide. Moreover, by studying healthy colon control, tumor-associated normal, and colorectal cancer tissues, we explored tissue-specific heterogeneity motifs. For completeness, we also compared the performance of the whole-exome bulk, cfDNA, and single-cell sequencing methods based on variation at the level of a single nucleotide. Full article
(This article belongs to the Special Issue Molecular Findings in Colorectal Cancer)
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Figure 1
<p>The distribution of the Tumor Mutational Burden (TMB) in the NAT and CRC samples is shown on a logarithmic scale. On average, the CRC group exhibits a higher TMB, indicating a greater number of somatic variations compared to the NAT group.</p>
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<p>Summary plots of the (<b>a</b>) NEG, (<b>b</b>) NAT, and (<b>c</b>) CRC samples. Variant classification distribution: the <span class="html-italic">X</span>-axis represents the number of variants, and the <span class="html-italic">Y</span>-axis represents the variant type categories. Variant type plot: the <span class="html-italic">X</span>-axis represents the number of variants, and the <span class="html-italic">Y</span>-axis represents the variant type categories and SNV class plot. Variants per sample plot: the <span class="html-italic">X</span>-axis represents the ID of samples, and the <span class="html-italic">Y</span>-axis represents the number of variants. Variant classification summary: the <span class="html-italic">X</span>-axis represents the variant classifications, and the <span class="html-italic">Y</span>-axis represents the number of variants. Top 10 mutated genes: the <span class="html-italic">X</span>-axis represents the number of mutations, and the <span class="html-italic">Y</span>-axis lists the top 10 mutated genes.</p>
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<p>Cross−cancer genome mutation patterns may serve as a proxy to identify positive (collaboration) or negative (synthetic lethal) epistatic relationships between recurrently mutated driver genes. The epistatic relationship between two driver genes may be inferred from cross-cancer mutation patterns, whereby co-occurrence may indicate a synergistic interaction in promoting tumorigenesis. By contrast, mutually exclusive driver genes may negatively impact tumorigenesis when mutated jointly. Here, mutually exclusive and co-occurring gene pairs are presented in a triangular matrix per tissue group—(<b>a</b>) NEG, (<b>b</b>) NAT, and (<b>c</b>) CRC. Bluish-green indicates a tendency toward co-occurrence, whereas brown indicates a tendency towards mutual exclusivity. The intensity of the greenish regions corresponds to the significance of the relationship between genes, and the star symbol denotes a higher (<span class="html-italic">p</span> &lt; 0.01) significance than the dot (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>The tumor heterogeneity patterns of samples of the (<b>a</b>) NEG, (<b>b</b>) NAT, and (<b>c</b>) CRC groups. The <span class="html-italic">X</span>-axis represents the ID of samples, and the <span class="html-italic">Y</span>-axis represents the total number of mutations detected. The number of detected mutations per sample is marked above the corresponding columns, and the height of the columns is proportional to the number of detected variants. Different colors correspond to different genes. The gene-color coding is illustrated on the top-right corners of the figures.</p>
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<p>Comparative plots regarding the sequencing input samples: (<b>a</b>) single-cell vs. bulk sequencing, (<b>b</b>) cfDNA vs. bulk sequencing, and (<b>c</b>) single-cell vs. cfDNA sequencing. The <span class="html-italic">X</span>-axis represents the genes, and the <span class="html-italic">Y</span>-axis represents the number of detected mutations on a logarithmic scale. The different sequencing methods are represented by different colors, where red is associated with bulk, blue is associated with single-cell, and green is associated with cfDNA sequencing.</p>
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<p>The efficiency of the different sequencing methods regarding the detection of mutations. The <span class="html-italic">X</span>-axis represents the different sequencing methods: (P) cfDNA, (B) bulk, and (S-C) single-cell sequencing. The <span class="html-italic">Y</span>-axis represents the number of detected variants. The height of the columns is proportional to the amount of detected variants. Different colors correspond to different genes. The illustrated specific genes are characteristic of non-hypermutated colon tumors: <span class="html-italic">APC</span>, <span class="html-italic">TTN</span>, <span class="html-italic">TP53</span>, <span class="html-italic">KRAS</span>, <span class="html-italic">MUC16</span>, <span class="html-italic">MUC5B</span>, <span class="html-italic">PIK3CA</span>, <span class="html-italic">BRAF</span>, <span class="html-italic">SOX9</span>, <span class="html-italic">RYR1</span>, <span class="html-italic">RYR2</span>, <span class="html-italic">RYR3</span>, <span class="html-italic">FBXW7</span>, <span class="html-italic">ARID1A</span>, <span class="html-italic">COL5A1</span>, <span class="html-italic">COL6A3</span>, <span class="html-italic">KIAA019</span>, and <span class="html-italic">PCDH17</span>. The color-coding of genes is illustrated on the top-right corners of the figure.</p>
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<p>The comparative oncomutational plot of the NAT and CRC groups. The X-axis represents the occurence rate of the mutations of the genes, and the Y-axis represents the examined genes. The left-side of the figure corresponds to the CRC group, and the right-side illustrates the findings regarding the NAT group.</p>
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15 pages, 3818 KiB  
Article
Impact of Laser Power on Electrochemical Performance of CeO2/Al6061 Alloy Through Selective Laser Melting (SLM)
by Fengyong Sun and Jitai Han
Crystals 2025, 15(1), 84; https://doi.org/10.3390/cryst15010084 - 16 Jan 2025
Viewed by 283
Abstract
As a type of additive manufacturing technology, SLM has made significant progress in the aerospace sector because of its capacity to swiftly and effectively form metals and their composites. This work investigates the impact of laser power (260, 280, 300, 320, 340 W) [...] Read more.
As a type of additive manufacturing technology, SLM has made significant progress in the aerospace sector because of its capacity to swiftly and effectively form metals and their composites. This work investigates the impact of laser power (260, 280, 300, 320, 340 W) on the performance of a 1.0 wt.% CeO2/Al6061 alloy prepared by SLM, including the forming quality (surface morphology and density), self-corrosion rate (SCR), and electrochemical behavior. The experimental outcomes suggest that as the laser power rises, the surface roughness exhibits an initial decline followed by an increase, whereas the density undergoes an initial increase and subsequently decreases. The SCR demonstrates a pattern of initial decrease followed by an increase as the laser power is incremented. When the laser power increases, the electrochemical activity shows the same trend. When the laser power is 280 W, the density of the sample is 98.63%, and the SCR is 2.243 × 10−4 g/cm2·min. The induced resistance of the sample caused by hydrogen evolution is small, at 7.827 × 10−20 Ω·cm2, and the polarization resistance reaches 8.048 × 10−1 Ω·cm2, suggesting superior resistance to corrosion on the part of the sample. The laser power affects the SCR and electrochemical performance of the sample by influencing its molding quality. At the laser power of 280 W, the formation quality of the sample is optimal, and the sample exhibits lower SCR and more stable electrochemical activity. Full article
(This article belongs to the Section Crystalline Metals and Alloys)
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<p>SEM images of powders used in this work.</p>
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<p>SEM images of powders used in this work.</p>
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<p>The surface appearance of samples exposed to differing laser powers.</p>
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<p>Density of samples in different laser powers.</p>
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<p>Self-corrosion of samples under different laser power.</p>
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<p>OCP of samples under different laser power.</p>
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<p>Polarization curves of samples exposed to different laser powers.</p>
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<p>EIS analysis of samples subjected to varying laser powers.</p>
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<p>Equivalent circuit of alloy under different laser powers.</p>
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<p>Surface morphology after electrochemical test under different laser powers.</p>
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<p>Surface morphology after electrochemical test under different laser powers.</p>
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19 pages, 1530 KiB  
Review
Periocular Aging Across Populations and Esthetic Considerations: A Narrative Review
by Brendan K. Tao, Fahad R. Butt, Thanansayan Dhivagaran, Michael Balas, Navdeep Nijhawan, Georges Nassrallah, Ahsen Hussain and Edsel B. Ing
J. Clin. Med. 2025, 14(2), 535; https://doi.org/10.3390/jcm14020535 - 16 Jan 2025
Viewed by 458
Abstract
As the face ages, the skin, fat, muscle, and fascia descend, and the underlying bone, cartilage, and teeth may lose mass. Oculofacial aging is a multifactorial process that is influenced by genetic, environmental, and lifestyle factors. This review summarizes the patterns of oculofacial [...] Read more.
As the face ages, the skin, fat, muscle, and fascia descend, and the underlying bone, cartilage, and teeth may lose mass. Oculofacial aging is a multifactorial process that is influenced by genetic, environmental, and lifestyle factors. This review summarizes the patterns of oculofacial aging that are observed across populations, including variations in periorbital hollowing, eyelid ptosis, and skin elasticity. Evidence indicates significant variability in aging patterns between sex- and race-based subgroups. Nonetheless, there remains a paucity of research on the progression of aging in some under-studied demographic groups. Signs of oculofacial aging often become apparent to patients well before these changes reach full maturity in later years, leading many to seek early esthetic interventions. Others may present with more advanced signs of aging, motivating a diverse range of therapeutic options. We discuss minimally invasive esthetic interventions to mitigate the signs of aging, which may include botulinum toxin injections, dermal fillers, applied energy-based treatments (e.g., lasers), and emerging techniques such as micro-focused ultrasound and platelet-rich plasma therapies. We review evidence on outcomes related to patient satisfaction and quality of life following esthetic interventions for oculofacial aging. Finally, we outline ethical considerations and challenges faced with the delivery of esthetic surgery, including treatment complications and the influence of social media. This review provides a comprehensive overview of oculofacial aging patterns, its management, and important considerations for the provision of esthetic oculofacial treatment. Full article
(This article belongs to the Special Issue Advances in Ophthalmic Plastic and Reconstructive Surgery)
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Figure 1
<p>Visual summary of common pathophysiological contributors to periorbital aging. Among these, sun exposure is a leading contributing factor. In this diagram, stress refers to both psychological stress and mechanical stressors to the skin (e.g., facial rubbing, stretching from longstanding edema, repetitive facial expressions, and sleeping prone). Abbreviation: ROS (reactive oxygen species).</p>
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<p>Common clinical examination findings in peri-ocular aging. Images were generated using artificial intelligence to preserve patient confidentiality. (<b>A</b>) Brow ptosis, more prominent on the patient’s right side. (<b>B</b>) Superior sulcus hollowing with glabellar furrows and lower dermatochalasis with double convexity deformity. (<b>C</b>) Prominent right nasojugal folds. (<b>D</b>) Suggestion of mild lower lid ectropion with loss of right lateral lid-globe apposition.</p>
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<p>Example of varying female oculofacial aging patterns between population groups. Images were generated using artificial intelligence to preserve patient confidentiality. (<b>A</b>) Caucasian. (<b>B</b>) East Asian. (<b>C</b>) Black or African American. The features of oculofacial aging are typically more advanced among Caucasian patients, exemplified in this figure by deeper rhytids and periocular hollowing.</p>
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28 pages, 12034 KiB  
Article
Numerical Study to Analyze the Influence of Process Parameters on Temperature and Stress Field in Powder Bed Fusion of Ti-6Al-4V
by Helia Mohammadkamal and Fabrizia Caiazzo
Materials 2025, 18(2), 368; https://doi.org/10.3390/ma18020368 - 15 Jan 2025
Viewed by 461
Abstract
This paper presents a comprehensive numerical investigation to simulate heat transfer and residual stress formation of Ti-6Al-4V alloy during the Laser Powder Bed Fusion process, using a finite element model (FEM). The FEM was developed with a focus on the effects of key [...] Read more.
This paper presents a comprehensive numerical investigation to simulate heat transfer and residual stress formation of Ti-6Al-4V alloy during the Laser Powder Bed Fusion process, using a finite element model (FEM). The FEM was developed with a focus on the effects of key process parameters, including laser scanning velocity, laser power, hatch space, and scanning pattern in single-layer scanning. The model was validated against experimental data, demonstrating good agreement in terms of temperature profiles and melt pool dimensions. The study elucidates the significant impact of process parameters on thermal gradients, melt pool characteristics, and residual stress distribution. An increase in laser velocity, from 600 mm/s to 1500 mm/s, resulted in a smaller melt pool area and faster cooling rate. Similarly, the magnitude of residual stress initially decreased and subsequently increased with increasing laser velocity. Higher laser power led to an increase in melt pool size, maximum temperature, and thermal residual stress. Hatch spacing also exhibited an inverse relationship with thermal gradient and residual stress, as maximum residual stress decreased by about 30% by increasing the hatch space from 25 µm to 75 µm. The laser scanning pattern also influenced the thermal gradient and residual stress distribution after the cooling stage. Full article
(This article belongs to the Special Issue Advanced Computational Methods in Manufacturing Processes)
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Figure 1
<p>Schematic of model for (<b>a</b>) single-track and (<b>b</b>) multi-track studies.</p>
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<p>Experimental sample and detailed pattern.</p>
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<p>(<b>a</b>) Melt pool dimensions including depth and width, obtained from simulation with a laser power of 150 W and a velocity of 1200 mm/s, compared with the experiment conducted by Dilip et al. [<a href="#B52-materials-18-00368" class="html-bibr">52</a>]; and (<b>b</b>) melt pool width from the simulation with a laser power of 170 W and a velocity of 600 mm/s, compared to the experiments described in <a href="#sec2dot3-materials-18-00368" class="html-sec">Section 2.3</a>.</p>
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<p>Thermal gradient at points A, B, and C, respectively, during the process with a laser power of 30 W and a laser velocity of 50 mm/s.</p>
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<p>Temperature validation for the simulation model with the experimental data [<a href="#B51-materials-18-00368" class="html-bibr">51</a>].</p>
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<p>Model validation by comparing simulation and experimental results: (<b>a</b>,<b>b</b>) melt pool depth and width from simulations and experimental data [<a href="#B52-materials-18-00368" class="html-bibr">52</a>]; (<b>c</b>) melt pool width from simulations and experiments conducted in this study (<a href="#sec2dot3-materials-18-00368" class="html-sec">Section 2.3</a>).</p>
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<p>Distribution of thermal residual stress of (<b>a</b>) von Mises stress; (<b>b</b>) stress along the x-axis; (<b>c</b>) stress along the y-axis; and (<b>d</b>) stress along the z-axis.</p>
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<p>Longitudinal stress generation (<b>a</b>) during laser scanning; (<b>b</b>) immediately after scanning; and (<b>c</b>) after cooling down to room temperature.</p>
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<p>Longitudinal stress distribution from point A to B, showing the direction of stress interpretation with an arrow in (<b>a</b>) schematic view of defined sections, and (<b>b</b>) longitudinal stress profile.</p>
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<p>The effect of laser velocity on (<b>a</b>) thermal gradient at point A during the laser scanning process and (<b>b</b>) melt pool shape and size.</p>
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<p>Effect of laser velocity on melt pool dimensions, under velocity of (<b>a</b>) 600 mm/s; (<b>b</b>) 900 mm/s; (<b>c</b>) 1200 mm/s; and (<b>d</b>) 1500 mm/s.</p>
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<p>(<b>a</b>) Diagram of longitudinal stress gradient along the laser scanning; and (<b>b</b>) contour plot of longitudinal stress distribution under various laser scanning velocities.</p>
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<p>Von Mises stress distribution under velocity of (<b>a</b>) 600 mm/s; (<b>b</b>) 900 mm/s; (<b>c</b>) 1200 mm/s; and (<b>d</b>) 1500 mm/s.</p>
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<p>Effect of laser power on: (<b>a</b>) thermal gradient diagram; and (<b>b</b>) melt pool volume.</p>
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<p>Effect of laser power on melt pool dimensions under power of (<b>a</b>) 100 W; (<b>b</b>) 150 W; (<b>c</b>) 170 W; and (<b>d</b>) 200 W.</p>
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<p>(<b>a</b>) Diagram of longitudinal stress gradient along the laser scanning; and (<b>b</b>) contour plot of longitudinal stress distribution under various laser powers.</p>
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<p>Von Mises stress distribution under power of (<b>a</b>) 100 W; (<b>b</b>) 150 W; (<b>c</b>) 170 W and (<b>d</b>) 200 W.</p>
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<p>The effect of hatch space values of (<b>a</b>) 25 μm; (<b>b</b>) 50 μm; and (<b>c</b>) 75 μm, on (<b>1</b>) the schematic representation of the deposited width and (<b>2</b>) the cross-sectional view of the melted regions.</p>
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<p>(<b>a</b>) Temperature change diagram at point A for different hatch spaces during laser scanning process; (<b>b</b>) effect of hatch space on residual stress.</p>
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<p>Schematic of laser scanning patterns: (<b>a</b>) alternating; (<b>b</b>) unidirectional; (<b>c</b>) 2 domains, alternating; and (<b>d</b>) 2 domains, unidirectional.</p>
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<p>Melt pool dimension obtained from simulation model for (<b>a</b>) unidirectional and (<b>b</b>) alternating scan patterns.</p>
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<p>Thermal gradient for comparing (<b>a</b>) alternate and unidirectional and (<b>b</b>) one domain and two domains scanning pattern, and (<b>c</b>) residual stress distribution under different scan patterns, (<b>c1</b>) alternating, (<b>c2</b>) unidirectional, (<b>c3</b>) alternating, 2 domains, and (<b>c4</b>) unidirectional, 2 domains.</p>
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<p>The effect of different process parameters on thermal residual stress.</p>
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15 pages, 9871 KiB  
Article
Study on the Tribological Behavior of Laser Surface Texturing on Silicon Nitride Ceramic Under Water Lubrication
by Hong-Jian Wang, Jing-De Huang, Bo Wang, Yang Zhang and Jin Wang
Lubricants 2025, 13(1), 21; https://doi.org/10.3390/lubricants13010021 - 8 Jan 2025
Viewed by 420
Abstract
The tribological behavior of silicon nitride (Si3N4) ceramic with textured patterns under water lubrication was investigated in this paper. Different textured patterns were fabricated using laser surface texturing (LST). Surface wettability was characterized by contact angle. The original surface [...] Read more.
The tribological behavior of silicon nitride (Si3N4) ceramic with textured patterns under water lubrication was investigated in this paper. Different textured patterns were fabricated using laser surface texturing (LST). Surface wettability was characterized by contact angle. The original surface and textured Si3N4 ceramic with triangular patterns presented as hydrophobic. However, the textured Si3N4 ceramic with hexagonal patterns presented as hydrophilic. Surface wettability and textured patterns were important factors affecting the friction performance of the Si3N4 ceramic. Our results indicated that symmetrical textured patterns were more beneficial for decreasing the coefficient of friction (COF) at lower reciprocating frequencies. In contrast, better surface wettability played a more important role in reducing the COF at higher reciprocating frequencies. The most severe damage observed on the untextured Si3N4 ceramic led to a higher wear rate. The symmetrical structure of hexagonal patterns was more conducive to decreasing the wear rate than triangular patterns. However, the Si3N4 ceramic with triangular patterns was more suitable for use at high-speed frictions due to better lubrication. The textured patterns had the function of storing lubricants and capturing and cutting debris. Thus, friction performance was improved by introducing textured patterns onto the surface of the Si3N4 ceramic. The friction and wear mechanisms are also discussed in this study. Full article
(This article belongs to the Special Issue Anti-wear Lubricating Materials)
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<p>The schematic diagram of different patterns on Si<sub>3</sub>N<sub>4</sub> ceramic surface: (<b>a</b>) triangles and (<b>b</b>) hexagons.</p>
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<p>The optical image (<b>a</b>) and transverse profile (<b>b</b>) of textured patterns after LST.</p>
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<p>The wetting state and CA of the Si<sub>3</sub>N<sub>4</sub> ceramic: (<b>a</b>) UP, (<b>b</b>) TP, and (<b>c</b>) HP.</p>
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<p>COF of the Si<sub>3</sub>N<sub>4</sub> ceramic with different textured patterns as a function of sliding time: (<b>a</b>) 0.5 Hz, (<b>b</b>) 1.5 Hz and (<b>c</b>) 2.5 Hz.</p>
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<p>COF of the Si<sub>3</sub>N<sub>4</sub> ceramic under different reciprocating frequencies.</p>
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<p>SEM of the wear morphology of the Si<sub>3</sub>N<sub>4</sub> ceramic at the reciprocating frequency of 0.5 Hz: (<b>a</b>) UP; (<b>b</b>) TP; (<b>c</b>) HP; (<b>d</b>–<b>f</b>) are enlarged views of UP, TP, and HP, respectively.</p>
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<p>SEM of the wear morphology of the Si<sub>3</sub>N<sub>4</sub> ceramic at the reciprocating frequency of 1.5 Hz: (<b>a</b>) UP; (<b>b</b>) TP; (<b>c</b>) HP; (<b>d</b>–<b>f</b>) are enlarged views of UP, TP, and HP, respectively.</p>
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<p>SEM of the wear morphology of the Si<sub>3</sub>N<sub>4</sub> ceramic at the reciprocating frequency of 2.5 Hz: (<b>a</b>) UP; (<b>b</b>) TP; (<b>c</b>) HP; (<b>d</b>–<b>f</b>) are enlarged views of UP, TP, and HP, respectively.</p>
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<p>EDS analysis from HP at the reciprocating frequency of 2.5 Hz: (<b>a</b>) SEM of debris on the wear track, and (<b>b</b>) EDS at area A and (<b>c</b>) EDS at area B in (<b>a</b>), respectively.</p>
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<p>The wear rate of the WC ball under different reciprocating frequencies.</p>
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<p>Schematic diagram of a water droplet sliding on the Si<sub>3</sub>N<sub>4</sub> ceramic: (<b>a</b>) hydrophobic surface and (<b>b</b>) hydrophilic surface.</p>
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<p>Schematic diagram of the frictional process on the surface of the Si<sub>3</sub>N<sub>4</sub> ceramic: initial stage on the untextured (<b>a</b>) and textured surfaces and (<b>b</b>) frictional stage of UP (<b>c</b>), TP (<b>d</b>), and HP (<b>e</b>).</p>
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14 pages, 3906 KiB  
Article
Real-Time Respiratory Monitoring Using a Sparse-Sampled Frequency-Scanning White-Light Interferometry System
by Wenyan Liu, Cheng Qian, Kexin Li, Yiping Wang, Xiaoyan Cai and Qiang Liu
Photonics 2025, 12(1), 45; https://doi.org/10.3390/photonics12010045 - 6 Jan 2025
Viewed by 620
Abstract
Fiber-optic tip sensors offer significant potential in biomedical applications due to their high sensitivity, compact size, and resistance to electromagnetic interference. This study focuses on advancing phase demodulation techniques for ultra-short Fabry–Pérot cavities within limited spectral bandwidths to enhance their application in biomedicine [...] Read more.
Fiber-optic tip sensors offer significant potential in biomedical applications due to their high sensitivity, compact size, and resistance to electromagnetic interference. This study focuses on advancing phase demodulation techniques for ultra-short Fabry–Pérot cavities within limited spectral bandwidths to enhance their application in biomedicine and diagnostics. We propose a novel sparse-sampled white-light interferometry system for respiratory monitoring, utilizing a monolithic integrated semiconductor tunable laser for quasi-continuous frequency scanning across 191.2–196.15 THz at a sampling rate of 5 kHz. A four-step phase-shifting algorithm (PSA) ensures precise phase demodulation, enabling high sensitivity for short-cavity fiber-optic sensors under constrained spectral bandwidth conditions. Humidity sensors fabricated via a self-growing polymerization process further enhance the system’s functionality. The experimental results demonstrate the system’s capability to accurately capture diverse breathing patterns—including normal, rapid, and deep states—with fast response and recovery times. These findings establish the system’s potential for real-time respiratory monitoring in clinical and point-of-care settings. Full article
(This article belongs to the Special Issue Advancements in Optical Fiber Sensing)
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<p>Sparse-sampled frequency-scanning white-light interferometry system. (<b>a</b>) Block diagram of the driver and data acquisition module of the MG-Y laser. (<b>b</b>) Pictures of key modules. 1, FPGA; 2, analog-to-digital conversion module; 3, driver board for current sources; 4, photodetectors; 5, MG-Y laser.</p>
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<p>Current tuning curves of sparsely sampled optical frequency scanning process.</p>
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<p>Schematic diagram of the sensor fabrication process. (<b>a</b>–<b>c</b>) Adsorption of photopolymer droplet film on optical fiber end face; (<b>d</b>) self-growing polymerization based on a 520 nm green laser; (<b>e</b>) microscopic image of a fiber tip humidity sensor.</p>
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<p>Principle of four-step phase-shifting demodulation scheme. (<b>a</b>) Sparsely sampled initial interferometer spectrum; (<b>b</b>) phase-shifted spectrum after splitting.</p>
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<p>Simulated demodulation results of a 50 Hz, 600 nm peak-to-peak amplitude sinusoidal vibration. (<b>a</b>) Interference spectra at different times; (<b>b</b>) comparison of demodulation results and theoretical values.</p>
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<p>Graph of RMSE simulation results for measuring sinusoidal dynamic signals.</p>
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<p>Schematic diagram of the proposed system and conventional WLI system for vibration measurement.</p>
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<p>Vibration measurement results. (<b>a</b>) Spectrum collected by the proposed system; (<b>b</b>) spectrum collected by conventional broadband WLI; (<b>c</b>) comparison of demodulation results between the two systems.</p>
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<p>Experimental results of relative humidity detection. (<b>a</b>) The measured reflected spectra evolution with increasing humidity; (<b>b</b>) the ΔOPD at different humidities and the linear fitting results.</p>
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<p>Compact fiber-optic respiratory monitoring system. The red rectangle marks the fiber tip sensor.</p>
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<p>Time-domain response curves of different breathing states. (<b>a</b>) Normal breathing; (<b>b</b>) enlarged view of one breathing process; (<b>c</b>) fast breathing; (<b>d</b>) deep breathing.</p>
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13 pages, 7014 KiB  
Article
Displacement Measurement Based on the Missing-Order Talbot Effect
by Liuxing Song, Kailun Zhao, Xiaoyong Wang, Jinping He, Guoliang Tian, Shihua Yang and Yaning Li
Sensors 2025, 25(1), 292; https://doi.org/10.3390/s25010292 - 6 Jan 2025
Viewed by 465
Abstract
Displacement measurement is a crucial application, with laser-based methods offering high precision and being well established in commercial settings. However, these methods often come with the drawbacks of significant size and exorbitant costs. We introduce a novel displacement measurement method that utilizes the [...] Read more.
Displacement measurement is a crucial application, with laser-based methods offering high precision and being well established in commercial settings. However, these methods often come with the drawbacks of significant size and exorbitant costs. We introduce a novel displacement measurement method that utilizes the missing-order Talbot effect. This approach circumvents the need to measure contrast in the Talbot diffraction field, opting instead to leverage the displacement within the missing-order Talbot diffraction pattern. Our method only requires parallel light, an amplitude grating, and a detector to achieve displacement measurement. The measurement dynamic range can be adjusted by altering the grating period and the wavelength of the incident light. Through careful simulation and experimental validation, our method exhibits a correlation coefficient R surpassing 0.999 across a 30 mm dynamic range and achieves a precision superior to 3 μm. Full article
(This article belongs to the Special Issue Advances in Optical Sensing, Instrumentation and Systems: 2nd Edition)
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<p>Schematic and simulation of the Talbot effect. (<b>a</b>) Illustrates the formation of Talbot zones (red) where the 0th and ±1st diffraction orders overlap, creating periodic self-imaging, and missing-order Talbot zones (orange) that produce stripe-like images due to the absence of certain diffraction orders. (<b>b</b>) Shows the diffraction field for a 4 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m grating period under 632 nm illumination, with a Talbot distance of 50 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m, as calculated by FDTD. (<b>c</b>) Displays the diffraction field for a 100 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m grating period under the same illumination, with a Talbot distance of 32 mm, calculated using the angular spectrum method.</p>
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<p>The diagram of diffraction propagation.</p>
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<p>Localized amplification diagram of diffraction propagation.</p>
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<p>The red dashed lines depict the stripe-like patterns that arise from the interference between the 0th and +1st orders, characterizing the missing-order Talbot images.</p>
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<p>Simulation data of diffraction fields and detection results for a grating with a period of 100 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m under 632 nm plane wave illumination. (<b>a</b>) Shows the diffraction field in the missing-order region at distances ranging from 300 mm to 400 mm from the grating, with red arrows indicating the Talbot distances. (<b>b</b>) Displays the detection results and linear fit residual analysis within a dynamic range of 300 mm to 400 mm. (<b>c</b>) Illustrates the diffraction field in the missing-order region at distances between 350 mm and 360 mm from the grating. (<b>d</b>) Presents the detection results and linear fit residual analysis within a dynamic range of 350 mm to 360 mm. (<b>e</b>) Depicts the diffraction field in the missing-order region at distances from 355 mm to 356 mm. (<b>f</b>) Shows the detection results and linear fit residual analysis within a dynamic range of 355 mm to 356 mm. The correlation coefficient <span class="html-italic">R</span> and root mean square error (RMSE) are provided for each dynamic range.</p>
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<p>Talbot zone diffraction and MTF analysis. (<b>a</b>) Talbot zone diffraction exhibiting periodic self-imaging. (<b>b</b>) MTF representation of periodic intensity fluctuations across displacement.</p>
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<p>Algorithmic efficiency of displacement extraction algorithm.</p>
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<p>Physical experimental setup for detecting relative displacement changes between grating and camera.</p>
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<p>Measurement results of different dynamic ranges. (<b>a</b>) Measurement results of 1 mm dynamic range. (<b>b</b>) Measurement results of 10 mm dynamic range.</p>
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17 pages, 4800 KiB  
Article
A Study on Remote Monitoring of NOx Emissions from Inland Vessels
by Mengtao Deng, Jianbo Hu, Zhaoyu Qi and Shitao Peng
Remote Sens. 2025, 17(1), 168; https://doi.org/10.3390/rs17010168 - 6 Jan 2025
Viewed by 400
Abstract
In order to demonstrate the feasibility of the tunable diode laser absorption spectroscopy (TDLAS) technology for monitoring NOx emissions from inland vessels, an equipment is designed to monitor emissions for inland vessels. The equipment was installed at the Jianbi locks, where experimental [...] Read more.
In order to demonstrate the feasibility of the tunable diode laser absorption spectroscopy (TDLAS) technology for monitoring NOx emissions from inland vessels, an equipment is designed to monitor emissions for inland vessels. The equipment was installed at the Jianbi locks, where experimental measurements were conducted on vessels passing through the locks, with a total of 330 vessels being measured. The detection rate for vessels was 50.3%, with a detection rate of 72.4% for fully loaded vessels and 24.7% for unloaded vessels. In addition, the exhaust emission patterns of inland vessels, the NOx emission patterns and detection rate of fully loaded and unloaded vessels, and the key parameter of the NOx emission factor of inland vessels were comprehensively analyzed. The experimental results show that CO2 and NOx in the exhaust gas of inland vessels have high signal intensity and good synchronization and can be applied to the regulatory monitoring of NOx emissions from inland vessels. Furthermore, the ratios of NO/CO2 and NO2/CO2 from fully loaded and unloaded vessels were significantly different. indicating that the NO2 indicator must be included in the remote monitoring indicators for inland vessel exhaust gases. Otherwise, the remote monitoring results for NOx may be significantly underestimated. Full article
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<p>Schematic diagram of a ship exhaust telemetry system for NO<sub>x</sub> regulation of inland vessels.</p>
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<p>(<b>a</b>) The installation location of telemetry equipment for the Jianbi locks is at the confluence of the Yangtze River and the Beijing-Hangzhou Canal. (<b>b</b>) The yellow rectangular box represents the Jianbi locks. (<b>c</b>) The on-site photo of the equipment.</p>
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<p>The number of vessels that passed through telemetry stations during the experiment, and the number of vessels which exhaust signals were detected by instruments.</p>
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<p>Monitoring results for 4 consecutive hours (red curve for CO<sub>2</sub>, blue curve for NO, green curve for NO<sub>2</sub>, and black curve for SO<sub>2</sub>).</p>
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<p>Exhaust monitoring results for a group of eight fully loaded vessels.</p>
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<p>Linear regression trend of NO<sub>x</sub> and CO<sub>2</sub> in the ship exhaust.</p>
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<p>NO<sub>x</sub> monitoring results for six groups of fully loaded and unloaded vessels.</p>
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<p>(<b>a</b>) Distribution of key parameter <span class="html-italic">a</span> of NO<sub>x</sub> emission factors for 255 fully loaded vessels. (<b>b</b>) Statistics of key parameter <span class="html-italic">a</span> of NO<sub>x</sub> emission factors for 255 fully loaded vessels.</p>
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<p>(<b>a</b>) Distribution of the key parameter <span class="html-italic">a</span> of NO<sub>x</sub> emission factors for 75 unloaded vessels. (<b>b</b>) Statistics of the key parameter <span class="html-italic">a</span> of NO<sub>x</sub> emission factors for 75 unloaded vessels.</p>
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14 pages, 23670 KiB  
Article
Sex-Based Differences in the In Vitro Digestibility of MCT Emulsions Stabilized by Various Emulsifiers
by Mijal Perez, Carmit Shani Levi and Uri Lesmes
Foods 2025, 14(1), 131; https://doi.org/10.3390/foods14010131 - 5 Jan 2025
Viewed by 487
Abstract
Consumer sex influences phenotypic differences in digestive functions that may underlie variations in food disintegration. This study used an in vitro digestion model to test the hypothesis that emulsions follow distinct digestive pathways in men and women. Model emulsions were prepared using medium-chain [...] Read more.
Consumer sex influences phenotypic differences in digestive functions that may underlie variations in food disintegration. This study used an in vitro digestion model to test the hypothesis that emulsions follow distinct digestive pathways in men and women. Model emulsions were prepared using medium-chain triglycerides stabilized by beta-lactoglobulin, alpha-lactalbumin, or lactoferrin, and by three non-protein emulsifiers: Tween 80, lecithin, and sucrose esters. All emulsions were produced by high-pressure homogenization (0.57 MPa, 5 passes) and then subjected to in vitro digestion under simulated conditions of the male or female gastrointestine. Digesta samples were analyzed via confocal microscopy and laser-based particle sizing, revealing that protein-stabilized emulsions were responsive to physiological differences between males and females, whereas emulsions stabilized by non-protein emulsifiers remained mostly unaffected by sex-based differences. Absolute differential analyses of emulsion droplet size-distribution curves showed that changes in breakdown trajectories for emulsions were pronouncedly noticeable in gastric effluents. Further, SDS-PAGE analysis of digesta showed that breakdown patterns of protein-stabilized emulsions are consistent with prior evidence found for healthy adults; however, results under female gut conditions indicated variations in protein clotting that may alter bioaccessible levels of bioactive peptides. Thus, this study underscores the importance of considering consumer biological sex in food design, especially regarding emulsion-based products for targeted digestive responses. Full article
(This article belongs to the Section Food Engineering and Technology)
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<p>Key colloidal characteristics of emulsions used in this study. Confocal <span class="html-italic">micrographs</span> of raw emulsions produced through high-pressure homogenization overlaid with D<sub>3,2</sub> droplet size-distribution curves, averaged zeta (ζ)-potential parameters (<span class="html-italic">n</span> = 10) and average of creaming velocity (Vc) measured after two months with the emulsion stored in the refrigerator during that period (<span class="html-italic">n</span> = 3). Micrograph scale bars represent 5 µm. The oily phase has been stained with Red Nile, and appears red.</p>
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<p>Comparisons of digestive effluents of emulsions stabilized by β-Lg or T80 during female (orange) or male (blue) in vitro digestion. Confocal micrograph of gastric and intestinal samples collected in the middle of the gastric phase (G<sub>1/2</sub>), at the end of this phase (G<sub>end</sub>), at the middle of the intestinal phase (I<sub>1/2</sub>) and at the end of the digestive process (I<sub>end</sub>). Micrograph bar scale represents 20 µm. Next to each micrograph: mean D<sub>3,2</sub> droplet size-distribution curves (<span class="html-italic">n</span> = 15).</p>
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<p>Comparisons of female (orange) and male (blue) in vitro digestion for emulsions stabilized by β-Lg or T80. D<sub>4,3</sub> droplet size distribution curves of the raw emulsion (E<sub>R</sub>) and all digestive effluents: middle of the gastric phase (G<sub>1/2</sub>), at the end of this phase (G<sub>end</sub>), in the middle of the intestinal phase (I<sub>1/2</sub>) and at the end of the digestive process (I<sub>end</sub>). The mean value (D<sub>50</sub>) for each of the droplet size-distribution curves is shown in solid orange (female) or dashed blue (male) (<span class="html-italic">n</span> = 15).</p>
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<p>Comparisons of female (orange) and male (blue) in vitro digestion for emulsions stabilized by protein emulsifier (α-Lactalbumin (α-La) or Lactoferrin (Lf)) or non-protein emulsifier (Lecithin (Lec) or Sucrose Ester (Suc)). D<sub>4,3</sub> droplet size-distribution curves of raw emulsion (E<sub>R</sub>) and all digestive effluents: mid-gastric phase (G<sub>1/2</sub>), at the end of this phase (G<sub>end</sub>), mid-intestinal phase (I<sub>1/2</sub>) and at the end of the digestive process (I<sub>end</sub>). The mean value (D<sub>50</sub>) for each of the droplet size-distribution curves is shown in solid orange (female) or dashed blue (male) (<span class="html-italic">n</span> = 15).</p>
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<p>Absolute difference of droplet-size distribution curves found in females and males. Protein emulsifier (β-Lg or α-La or Lf) on the <b>left</b> and non-protein (T80 or Lec or Suc) emulsifier on the <b>right</b>. The cumulative absolute-difference value (area under the curve) is indicated inside each plot.</p>
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<p>Comparison of SDS-PAGE analysis for raw emulsions and gastric effluents from female (orange) or male (blue) in vitro digestion of emulsions stabilized with β-Lg or α-La or Lf.</p>
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20 pages, 1132 KiB  
Article
Photodiode Signal Patterns: Unsupervised Learning for Laser Weld Defect Analysis
by Erkan Caner Ozkat
Processes 2025, 13(1), 121; https://doi.org/10.3390/pr13010121 - 5 Jan 2025
Viewed by 442
Abstract
Laser welding, widely used in industries such as automotive and aerospace, requires precise monitoring to ensure defect-free welds, especially when joining dissimilar metallic thin foils. This study investigates the application of machine learning techniques for defect detection in laser welding using photodiode signal [...] Read more.
Laser welding, widely used in industries such as automotive and aerospace, requires precise monitoring to ensure defect-free welds, especially when joining dissimilar metallic thin foils. This study investigates the application of machine learning techniques for defect detection in laser welding using photodiode signal patterns. Supervised models, including Support Vector Machine (SVM), k-Nearest Neighbors (kNN), and Random Forest (RF), were employed to classify weld defects into sound welds (SW), lack of connection (LoC), and over-penetration (OP). SVM achieved the highest accuracy (95.2%) during training, while RF demonstrated superior generalization with 83% accuracy on validation data. The study also proposed an unsupervised learning method using a wavelet scattering one-dimensional convolutional autoencoder (1D-CAE) network for anomaly detection. The proposed network demonstrated its effectiveness in achieving accuracies of 93.3% and 87.5% on training and validation datasets, respectively. Furthermore, distinct signal patterns associated with SW, OP, and LoC were identified, highlighting the ability of photodiode signals to capture welding dynamics. These findings demonstrate the effectiveness of combining supervised and unsupervised methods for laser weld defect detection, paving the way for robust, real-time quality monitoring systems in manufacturing. The results indicated that unsupervised learning could offer significant advantages in identifying anomalies and reducing manufacturing costs. Full article
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<p>The visual representation of the geometrical features.</p>
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<p>Flowchart of the proposed methodology for classification models.</p>
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<p>The network structure of the 1D convolution autoencoder.</p>
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<p>Photodiode signals (normalized) recorded during the welding process are categorized as over-penetration (OP), lack of connection (LoC), and sound weld (SW).</p>
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<p>Confusion matrices for (<b>a</b>) SVM, (<b>b</b>) kNN and (<b>c</b>) RF models associated with the training dataset; and, (<b>d</b>) SVM, (<b>e</b>) kNN and (<b>f</b>) RF models associated with the validation dataset, respectively.</p>
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<p>The distribution of reconstruction losses for normal and abnormal data.</p>
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<p>Detected anomalies in photodiode signals for the given input signal: Lack of Connection (LoC) case.</p>
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<p>Detected anomalies in photodiode signals for the given input signal: Overpenetration (OP) case.</p>
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<p>Confusion matrix for (<b>a</b>) the training dataset and (<b>b</b>) the validation dataset, respectively.</p>
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12 pages, 4465 KiB  
Article
Phase Transition and Controlled Zirconia Implant Patterning Using Laser-Induced Shockwaves
by Inomjon Majidov, Yaran Allamyradov, Salizhan Kylychbekov, Zikrulloh Khuzhakulov and Ali Oguz Er
Appl. Sci. 2025, 15(1), 362; https://doi.org/10.3390/app15010362 - 2 Jan 2025
Viewed by 461
Abstract
Zirconia is increasingly favored for dental implants owing to its corrosion resistance, hypoallergenic properties, and superior esthetics, but its biocompatibility remains a challenge. This study explores laser-assisted surface modification to enhance zirconia bioactivity. Zirconia transitions from the monoclinic to the tetragonal phase during [...] Read more.
Zirconia is increasingly favored for dental implants owing to its corrosion resistance, hypoallergenic properties, and superior esthetics, but its biocompatibility remains a challenge. This study explores laser-assisted surface modification to enhance zirconia bioactivity. Zirconia transitions from the monoclinic to the tetragonal phase during sintering, with mixed phases observed in the pre-sintered stage. These transitions are critical for understanding its structural stability and malleability. Grid patterns were imprinted on the green body implant surface using a 1064 nm Nd-YAG laser (Continuum Surelite II, San Jose, CA, USA), with mesh sizes ranging from 7 to 50 µm and depths up to 2 µm, controlled by varying laser fluence, irradiation time, and templates. SEM, AFM, and XRD analyses were used to characterize the surface morphology and crystallography. Protein adsorption studies compared two patterned samples with different surface coverage—the first sample had a patterned area of 0.212 cm2 (27%), while the second sample had a patterned area of 0.283 cm2 (36%)—to a control sample. Protein adsorption increased by 92% in the first and 169% in the second sample, demonstrating a direct correlation between increased pattern area and bioactivity. Enhanced protein adsorption facilitates cell attachment and growth, which are crucial for improving osseointegration. These results underscore the potential of laser-assisted surface modification to optimize zirconia’s performance as a medical implant material. Full article
(This article belongs to the Special Issue Advances of Laser Technologies and Their Applications)
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<p>XRD pattern of zirconia. Sintered (red), pre-sintered (green), and green body (blue) ZrO<sub>2</sub> XRD profiles.</p>
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<p>ZrO<sub>2</sub> patterned via the “graphite method”. Cu (400) mesh TEM grid template at F = 1 J/cm<sup>2</sup>, t = 2 s.</p>
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<p>Zirconia surface patterned via the “aluminum method”. First row: Cu (400) square mesh TEM template at F = 2 J/cm<sup>2</sup>, t = 1 s. Second row: Cu (400) hexagonal mesh grid TEM template at F = 2 J/cm<sup>2</sup>, t = 1 s.</p>
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<p>AFM image, 3D image, and depth profile plot of a patterned zirconia via the aluminum method. Cu(400) hexagonal mesh grid TEM template at F = 2 J/cm<sup>2</sup>, t = ₋1 s. −.</p>
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<p>BSA absorbance as a function of time at 562 nm.</p>
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17 pages, 2600 KiB  
Article
The Distribution of Rare Earth Elements in Coal Fly Ash Determined by LA-ICP-MS and Implications for Its Economic Significance
by Shuliu Wang, Wenhui Huang and Weihua Ao
Sustainability 2025, 17(1), 275; https://doi.org/10.3390/su17010275 - 2 Jan 2025
Viewed by 461
Abstract
Coal fly ash represents a potential resource of some critical elements, including rare earth elements (REEs), which are retained and concentrated during coal combustion. Understanding the distribution and modes of occurrence of REEs within fly ash is vital to developing effective recovery methods [...] Read more.
Coal fly ash represents a potential resource of some critical elements, including rare earth elements (REEs), which are retained and concentrated during coal combustion. Understanding the distribution and modes of occurrence of REEs within fly ash is vital to developing effective recovery methods and enhancing their economic value. Laser Ablation Inductively Coupled Plasma Mass Spectrometry (LA-ICP-MS) was applied to investigate the in situ elemental constituents of coal fly ash phases, including aluminosilicates, Ca-(Fe)-enriched aluminosilicates, Fe-oxides, and SiO2/Quartz, in order to explore the distribution of REEs in combustion products. LA-ICP-MS results show that V, Cr, and Nb are mainly enriched in Ca-Ti-enriched aluminosilicates with trace element concentrations referenced to the original fly ash composition. Lithium is primarily enriched in SiO2 glassy grains, followed by Ca, (Fe)-enriched aluminosilicates. Co, Ni, and Cu present a concomitant distribution in the Fe-enriched phases, such as Fe-oxides and Fe-enriched aluminosilicates. The chondrite normalized REE distribution patterns show characteristics of LREE enrichment and Eu-negative anomalies in most phases, while the REE patterns of SiO2 glassy grains have a distinct positive anomaly in Sm, Gd, and Dy, coupled with a deficiency in LREEs. Compared to feed coal, elements such as Li, V, Cr, Co, Ni, and Nb and REEs are enriched 2~10 times in various phases of fly ash, with REEs notably concentrated six times higher in aluminosilicates and Ca-Ti-enriched aluminosilicates than the original coal. This study further discusses the feasibility, calibration principles, and advantages of using LA-ICP-MS to determine REE distribution, as well as the economic implications of REE extraction from coal fly ash. Full article
(This article belongs to the Special Issue Scientific Disposal and Utilization of Coal-Based Solid Waste)
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<p>The spatial resolution and detection limit of analytical techniques for the elemental composition (modified from [<a href="#B24-sustainability-17-00275" class="html-bibr">24</a>]).</p>
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<p>The mineralogy and LA-ICP-MS analysis spot of different phases in coal fly ash under reflected light. (<b>A</b>) S1, Al-Si-Fe; (<b>B</b>) S2, Fe-oxide; (<b>C</b>) S3, Si-Al; (<b>D</b>) S4, Al-Si-Ca-Ti; (<b>E</b>) S5, Al-Si; (<b>F</b>) S6, Si-Al; (<b>G</b>) S7, Al-Si-Ca; (<b>H</b>) S8, SiO<sub>2</sub>; (<b>I</b>) S9, Fe-oxide; (<b>J</b>) S10, Fe-oxide; (<b>K</b>) S11, SiO<sub>2</sub>; (<b>L</b>) S12, quartz.</p>
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<p>The in situ trace elements of constituents of coal ash.</p>
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<p>The distribution patterns of REE in the aluminosilicates (<b>A</b>), Ca, (Fe)-enriched aluminosilicates (<b>B</b>), Fe-oxides (<b>C</b>), and SiO<sub>2</sub>/quartz (<b>D</b>).</p>
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<p>The distribution of REY of fly ash (<b>A</b>) measured by ICP-MS and that of aluminosilicates, Ca (<b>B</b>), (Fe)-enriched aluminosilicates (<b>C</b>), and Fe-oxides (<b>D</b>) was determined by LA-ICP-MS.</p>
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<p>(<b>A</b>) The contents and proportions of LREY, MERY, and HREY in coal and coal combustion products. (<b>B</b>) The contents of LREY, MERY, and HREY in the fly ash phases. (<b>C</b>) The distribution patterns of REE in feed coal, combustion products, and fly ash phases.</p>
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<p>The distribution of average concentration of REE in China, the U.S., Europe, others, and world coal fly ash.</p>
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<p>The distribution of total coal combustion production (CCP) used by category.</p>
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