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Search Results (13,297)

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Keywords = optical properties

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7 pages, 2079 KiB  
Article
Optical Angular Momentum Beam Generation Using Coherent Beam Combination
by Przemyslaw Gontar, Lukasz Gorajek, Waldemar Zendzian and Jan Jabczyński
Photonics 2024, 11(10), 907; https://doi.org/10.3390/photonics11100907 - 26 Sep 2024
Abstract
(1) Background: The significant progress observed over the last two decades in coherent beam combining (CBC) technology has mainly focused on its applications in high-energy physics and laser weapons. This work provides insight into the basic principles of CBC and the search for [...] Read more.
(1) Background: The significant progress observed over the last two decades in coherent beam combining (CBC) technology has mainly focused on its applications in high-energy physics and laser weapons. This work provides insight into the basic principles of CBC and the search for an alternative, namely optical angular momentum (OAM) generation using CBC. (2) Methods: A semi-analytical model based on the paraxial wave equation was explored, generating OAM-CBC beams by manipulating the tilts and phases of the CBC (T&P-CBC) of hexagonal architecture. (3) Results: The specially arranged T&P-CBC shows typical properties of OAM, such as annular profiles for the zero diffraction order and 1st-order replicas in the far field and correlation coefficients of 1% between different OAM-CBC fields. (4) Conclusions: The differences between classical OAM beams and OAM-CBC are substantial due to hexagonal lattice properties. Moreover, applications in free space optical communications are feasible as T&P CBC fulfills the main conditions and requirements for OAM generation. Full article
(This article belongs to the Special Issue Progress in OAM Beams: Recent Innovations and Future Perspectives)
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Figure 1
<p>Concept of optical angular momentum–coherent beam combining (OAM-CBC) generation via tilted and phased CBC.</p>
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<p>Two-dimensional maps of OAM-CBC irradiance distributions (in logarithmic scale) in the far field for optical angular momentum number; (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>m</mi> <mrow> <mi>OAM</mi> </mrow> </msub> </mrow> </semantics></math> = 0; (<b>b</b>) 2; (<b>c</b>) 4; (<b>d</b>) 6; <span class="html-italic">N<sub>lat</sub></span> = 127, <span class="html-italic">f.f.</span> = 0.99, ε<sub>tr</sub> = 0.05.</p>
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<p>Irradiance profiles in the far field for <math display="inline"><semantics> <mrow> <msub> <mi>m</mi> <mrow> <mi>OAM</mi> </mrow> </msub> </mrow> </semantics></math> ϵ [0, 8]; <span class="html-italic">f.f. =</span> 0.99, <span class="html-italic">ε</span><sub>tr</sub> = 0.05, <span class="html-italic">N<sub>lat</sub></span> = 127.</p>
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<p>Power-in-bucket curves for <math display="inline"><semantics> <mrow> <msub> <mi>m</mi> <mrow> <mi>OAM</mi> </mrow> </msub> </mrow> </semantics></math> ϵ [0, 8]; <span class="html-italic">f.f. =</span> 0.99, ε<sub>tr</sub> = 0.05, <span class="html-italic">N<sub>lat</sub></span> = 127.</p>
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11 pages, 1033 KiB  
Article
Microfluidic Detection Platform for Determination of Ractopamine in Food
by Cheng-Xue Yu, Kuan-Hsun Huang, To-Lin Chen, Chan-Chiung Liu and Lung-Ming Fu
Biosensors 2024, 14(10), 462; https://doi.org/10.3390/bios14100462 - 26 Sep 2024
Abstract
A novel microfluidic ractopamine (RAC) detection platform consisting of a microfluidic RAC chip and a smart analysis device is proposed for the determination of RAC concentration in meat samples. This technology utilizes gold nanoparticles (AuNPs) modified with glutamic acid (GLU) and polyethyleneimine (PEI) [...] Read more.
A novel microfluidic ractopamine (RAC) detection platform consisting of a microfluidic RAC chip and a smart analysis device is proposed for the determination of RAC concentration in meat samples. This technology utilizes gold nanoparticles (AuNPs) modified with glutamic acid (GLU) and polyethyleneimine (PEI) to measure RAC concentration in food products. When RAC is present, AuNPs aggregate through hydrogen bonding, causing noticeable changes in their optical properties, which are detected using a self-built UV–visible micro-spectrophotometer. Within the range of 5 to 80 ppb, a linear relationship exists between the absorbance ratio (A693nm/A518nm) (Y) and RAC concentration (X), expressed as Y = 0.0054X + 0.4690, with a high coefficient of determination (R2 = 0.9943). This method exhibits a detection limit of 1.0 ppb and achieves results within 3 min. The practical utility of this microfluidic assay is exemplified through the evaluation of RAC concentrations in 50 commercially available meat samples. The variance between concentrations measured using this platform and those determined via liquid chromatography–tandem mass spectrometry (LC-MS/MS) is less than 8.33%. These results underscore the viability of the microfluidic detection platform as a rapid and cost-effective solution for ensuring food safety and regulatory compliance within the livestock industry. Full article
(This article belongs to the Special Issue Biosensors Based on Microfluidic Devices—2nd Edition)
14 pages, 1131 KiB  
Article
Spiral Annealing of Magnetic Microwires
by Alexander Chizhik, Paula Corte-Leon, Valentina Zhukova, Juan Mari Blanco, Julian Gonzalez and Arcady Zhukov
Sensors 2024, 24(19), 6239; https://doi.org/10.3390/s24196239 (registering DOI) - 26 Sep 2024
Abstract
A preprocessing technique named “spiral annealing” was applied for the first time to magnetic microwires. In this process, the sample was arranged in a flat spiral shape during annealing, and subsequent measurements were conducted on the unbent sample with the induced stress distribution [...] Read more.
A preprocessing technique named “spiral annealing” was applied for the first time to magnetic microwires. In this process, the sample was arranged in a flat spiral shape during annealing, and subsequent measurements were conducted on the unbent sample with the induced stress distribution along and transverse to the sample. The research utilized both magnetic and magneto-optical methods. The anisotropy field magnitude in both the volume and surface of the microwire was measured, and for the first time, a direct correlation between the anisotropy field and the curvature of a spirally annealed microwire was established. Additionally, a connection between the type of surface domain structure and the degree of spiral curvature was identified. The preservation of the distribution of spiral annealing-induced magnetic properties both along and across the microwire is a key effect influencing the technological application of the microwire. The range of induced curvature within which a specific helical magnetic structure can exist was also determined. This insight links the conditions of spiral annealing to the selection of microwires as active elements in magnetic sensors. Full article
(This article belongs to the Special Issue Feature Papers in Physical Sensors 2024)
16 pages, 2735 KiB  
Article
Aluminum Phosphate Nanoplates Synthesized via Green Method Using Cork Oak Somatic Embryo-Derived Phytates
by Beatriz Pintos and Arancha Gomez-Garay
Appl. Sci. 2024, 14(19), 8681; https://doi.org/10.3390/app14198681 (registering DOI) - 26 Sep 2024
Abstract
This study presents a novel green synthesis method for aluminum phosphate (AlPO4) nanoplates using extracts from Quercus suber somatic embryos. Traditionally, metallic nanoparticles are synthesized using harmful chemical reagents and solvents, but our approach leverages bioactive compounds, such as phytic acid [...] Read more.
This study presents a novel green synthesis method for aluminum phosphate (AlPO4) nanoplates using extracts from Quercus suber somatic embryos. Traditionally, metallic nanoparticles are synthesized using harmful chemical reagents and solvents, but our approach leverages bioactive compounds, such as phytic acid (IP6) from plant extracts, offering a more sustainable alternative. We observed a high phosphate content of 23.6 μMol PO43−/mg dry weight (DW) in the extracts, which is significantly higher than in other Quercus species. Characterization through UV–VIS spectroscopy and XRD confirmed the formation of complex crystal nanoplates, where anisotropic aluminum phosphate with a triclinic crystal structure coexists with monoclinic structures, both forms of aluminum phosphate tridymite. Electron microscopy (TEM and SEM) revealed the hierarchical organization of these nanoplates, distinguishing them from the more commonly observed spherical nanoparticles. Fourier-transform infrared (FTIR) spectroscopy further validated the incorporation of phytic acid into the nanoplate structure. This innovative method not only advances sustainable nanomaterial synthesis but also demonstrates the potential for unique optical and structural properties in aluminum phosphate nanoplates, paving the way for future applications in specialized fields. Full article
(This article belongs to the Special Issue Advanced Phytochemistry and Its Applications)
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<p>Chemical structure of phytic acid [<a href="#B17-applsci-14-08681" class="html-bibr">17</a>].</p>
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<p>Formation of aluminum nanoparticles from the reaction of the aqueous extract of cork oak embryos obtained in vitro with aluminum nitrate nonahydrate (5 mM). (<b>A</b>–<b>G</b>) Time-lapse of the synthesis. (<b>A</b>) Mixing of the aqueous extract of cork oak embryos obtained in vitro with aluminum nitrate nonahydrate at time = 0. (<b>B</b>) Formation of a “cloud” at the top of the beaker. (<b>C</b>,<b>D</b>) The whitish cloud moves to the bottom of the beaker (the beaker in (<b>D</b>) is placed on a blue background for better visualization). (<b>E</b>) Dark precipitation at the bottom of the beaker. (<b>F</b>) Formation of globular structures in the corners of the beaker after drying and consequent removal of the supernatant. (<b>G</b>) Eppendorf tube with the characteristic powder-like material collected from the beaker for further characterization.</p>
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<p>The absorbance spectra from a dispersion of aluminum phosphate nanoparticles obtained by green synthesis from Al(NO<sub>3</sub>)<sub>3</sub>·9H<sub>2</sub>O and cork oak somatic embryos extract.</p>
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<p>XRD profile of AlNPs obtained by reaction of <span class="html-italic">Q. suber</span> somatic embryos extract with Al(NO<sub>3</sub>)<sub>3</sub>·9H<sub>2</sub>O; in the insert, the table with the identifications. Peaks identifying the presence of aluminum phosphate have been listed.</p>
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<p>Transmission electron microscope (TEM) and scanning electron microscope (SEM) images and EDX spectrum showing the presence of aluminum in the aluminum phosphate nanoplates synthesized via green synthesis from aluminum nitrate nonahydrate and cork oak somatic embryo extract. (<b>A</b>) TEM image (the transparency observed is due to the extremely thin nature of the nanoplates); (<b>B</b>) SEM image; (<b>C</b>) EDX in coupling with TEM; (<b>D</b>) EDX in coupling with SEM.</p>
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<p>FTIR spectra of (blue) cork oak somatic embryos aqueous extract and (red) NPs.</p>
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19 pages, 11029 KiB  
Article
Novel High-Strength and High-Temperature Resistant Composite Material for In-Space Optical Mining Applications: Modeling, Design, and Simulation at the Polymer and Atomic/Molecular Levels
by Hadarou Sare and Dongmei Dong
Materials 2024, 17(19), 4723; https://doi.org/10.3390/ma17194723 - 26 Sep 2024
Abstract
This study explores the modeling, design, simulation, and testing of a new composite material designed for high-strength and high-temperature resistance in in-space optical mining, examining its properties at both the polymer and atomic/molecular levels. At the polymer level, the investigation includes mechanical and [...] Read more.
This study explores the modeling, design, simulation, and testing of a new composite material designed for high-strength and high-temperature resistance in in-space optical mining, examining its properties at both the polymer and atomic/molecular levels. At the polymer level, the investigation includes mechanical and thermal performance analyses using COMSOL Multiphysics 6.1, employing layerwise theory, equivalent single layer (ESL) theory, and a multiple-model approach for mechanical modeling, alongside virtual thermal experiments simulating laser heating. Experimentally, porous Polyaniline (PANI) films are fabricated via electrochemical polymerization, with variations in voltage and deposition time, to study their morphology, optical performance, and electrochemical behavior. At the atomic and molecular levels, this study involves modeling the composite material, composed of Nomex, Kevlar, and Spirooxazine-Doped PANI, and simulating its behavior. The significance of this work lies in developing a novel composite material for in-space optical mining, integrating it into optical mining systems, and introducing innovative thermal management solutions, which contribute to future space exploration by improving resource efficiency and sustainability, while also enhancing the understanding of PANI film properties for in-space applications. Full article
(This article belongs to the Section Materials Simulation and Design)
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<p>Atomic-level view of Nomex.</p>
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<p>Structure of Nomex.</p>
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<p>Atomic-level view of Kevlar.</p>
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<p>The structure of Kevlar.</p>
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<p>Atomic-level view of Spirooxazine-Doped PANI.</p>
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<p>Design of the composite material made up of Nomex, Kevlar, and Spirooxazine-Doped Polyaniline (PANI) thin film.</p>
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<p>The first six mode shapes and corresponding eigenfrequencies of the composite material, using the multiple-model method.</p>
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<p>Peak von Mises stress distribution in the composite material.</p>
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<p>Displacement in the top layer of the composite material.</p>
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<p>Maximum, minimum, and average temperatures of the composite material as functions of time.</p>
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<p>Difference between the maximum and minimum temperatures on the composite material.</p>
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<p>Temperature variation across the composite material.</p>
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<p>Isosurface temperature across the composite material.</p>
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<p>Displacement of the composite material made up of Nomex, Kevlar, and Spirooxazine-Doped Polyaniline (PANI) thin film.</p>
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<p>Peak von Mises stress distribution in the composite material made up of Nomex, Kevlar, and Spirooxazine-Doped Polyaniline (PANI) thin film.</p>
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<p>Temperature variation across the composite material made up of Nomex, Kevlar, and Spirooxazine-Doped Polyaniline (PANI) thin film.</p>
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12 pages, 2584 KiB  
Article
Bandgap Engineering via Doping Strategies for Narrowing the Bandgap below 1.2 eV in Sn/Pb Binary Perovskites: Unveiling the Role of Bi3+ Incorporation on Different A-Site Compositions
by Jeong-Yeon Lee, Seojun Lee, Jun Ryu and Dong-Won Kang
Nanomaterials 2024, 14(19), 1554; https://doi.org/10.3390/nano14191554 - 26 Sep 2024
Viewed by 61
Abstract
The integration of perovskite materials in solar cells has garnered significant attention due to their exceptional photovoltaic properties. However, achieving a bandgap energy below 1.2 eV remains challenging, particularly for applications requiring infrared absorption, such as sub-cells in tandem solar cells and single-junction [...] Read more.
The integration of perovskite materials in solar cells has garnered significant attention due to their exceptional photovoltaic properties. However, achieving a bandgap energy below 1.2 eV remains challenging, particularly for applications requiring infrared absorption, such as sub-cells in tandem solar cells and single-junction perovskite solar cells. In this study, we employed a doping strategy to engineer the bandgap and observed that the doping effects varied depending on the A-site cation. Specifically, we investigated the impact of bismuth (Bi3+) incorporation into perovskites with different A-site cations, such as cesium (Cs) and methylammonium (MA). Remarkably, Bi3+ doping in MA-based tin-lead perovskites enabled the fabrication of ultra-narrow bandgap films (~1 eV). Comprehensive characterization, including structural, optical, and electronic analyses, was conducted to elucidate the effects of Bi doping. Notably, 8% Bi-doped Sn-Pb perovskites demonstrated infrared absorption extending up to 1360 nm, an unprecedented range for ABX3-type single halide perovskites. This work provides valuable insights into further narrowing the bandgap of halide perovskite materials, which is essential for their effective use in multi-junction tandem solar cell architectures. Full article
(This article belongs to the Special Issue Nanostructured Materials for Electric Applications)
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<p>(<b>a</b>) Absorption spectra of pristine and Bi 1% doped CSPI perovskite films, with the inset highlighting the enlarged absorption spectrum, (<b>b</b>) Tauc plot of pristine and Bi 1% doped CSPI perovskite films, (<b>c</b>) Stacked XRD patterns of pristine and Bi 1% doped CSPI perovskite films with dashed box highlighting the main peak, (<b>d</b>) Main XRD peak of pristine and Bi 1% doped CSPI perovskite films.</p>
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<p>(<b>a</b>) Absorption spectra of pristine and Bi 1% doped MSPI perovskite films, with the inset highlighting the enlarged absorption spectrum, (<b>b</b>) Tauc plot of pristine and Bi 1% doped MSPI perovskite films, (<b>c</b>) Stacked XRD patterns of pristine and Bi 1% doped MSPI perovskite films with dashed box highlighting the main peak, (<b>d</b>) Main XRD peak of pristine and Bi 1% doped MSPI perovskite films.</p>
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<p>(<b>a</b>) Surface FE-SEM image of pristine CSPI perovskite film on a glass substrate, (<b>b</b>) Surface FE-SEM image of Bi-doped CSPI perovskite film on a glass substrate, (<b>c</b>) Surface FE-SEM image of pristine MSPI perovskite film on a glass substrate, (<b>d</b>) Surface FE-SEM image of Bi-doped MSPI perovskite film on a glass substrate. Scale bar: 300 nm.</p>
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<p>(<b>a</b>) Device configuration diagram, (<b>b</b>) J-V curves of 1%, 2%, 4%, and 8% Bi-doped MSPI devices, (<b>c</b>) Normalized EQE spectrum of pristine and Bi 1% doped MA-based devices, (<b>d</b>) Enlarged EQE spectrum of 1%, 2%, 4%, and 8% Bi-doped MSPI devices.</p>
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13 pages, 5284 KiB  
Article
Effect of Surface Anions Adsorbed by Rutile TiO2 (001) on Photocatalytic Nitrogen Reduction Reaction: A Density Functional Theory Calculation
by Xiaoyu Jiang, Mengyuan Gao and Hongda Li
Molecules 2024, 29(19), 4566; https://doi.org/10.3390/molecules29194566 - 25 Sep 2024
Viewed by 203
Abstract
The adsorption of common anions found in water can have a considerable impact on the surface state and optical characteristics of titanium dioxide (TiO2), which has an important impact on the photocatalytic nitrogen reduction reaction (NRR). This work utilizes density functional [...] Read more.
The adsorption of common anions found in water can have a considerable impact on the surface state and optical characteristics of titanium dioxide (TiO2), which has an important impact on the photocatalytic nitrogen reduction reaction (NRR). This work utilizes density functional theory (DFT) computations to examine the electronic and optical characteristics of the TiO2 (001) surface under various anion adsorptions in order to clarify their influence on the photocatalytic NRR of TiO2. The modifications in the structure, optical, and electronic properties of TiO2 before and after anion adsorption are investigated. In addition, the routes of Gibbs free energy for the NRR are also evaluated. The results indicate that the adsorption of anions modifies the surface characteristics of TiO2 to a certain degree, hence impacting the separating and recombining charge carriers by affecting the energy gap of TiO2. More importantly, the adsorption of anions can increase the energy barriers for the NRR, thereby exerting a detrimental effect on its photocatalytic activity. These findings provide a valuable theoretical contribution to understanding the photocatalytic reaction process of TiO2 and its potential application of NRR in the actual complex water phase. Full article
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<p>Model of the rutile TiO<sub>2</sub> (001) surface. The four Ti-O bonds connected by Ti atoms below the adsorbed ion are a, b, c and d; Gray ball is Ti atom, red balls are O atom.</p>
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<p>The models before and after anion adsorption: (<b>a</b>–<b>l</b>) represent TiO<sub>2</sub>-Ti-F<sup>−</sup>, TiO<sub>2</sub>-Ti-Cl<sup>−</sup>, TiO<sub>2</sub>-Ti-Br<sup>−</sup>, TiO<sub>2</sub>-Ti-I<sup>−</sup>, TiO<sub>2</sub>-O-F<sup>−</sup>, TiO<sub>2</sub>-O-Cl<sup>−</sup>, TiO<sub>2</sub>-O-Br<sup>−</sup>, TiO<sub>2</sub>-O-I<sup>−</sup>, TiO<sub>2</sub>-NO<sub>3</sub><sup>−</sup>, TiO<sub>2</sub>-CO<sub>3</sub><sup>2−</sup>, TiO<sub>2</sub>-SO<sub>4</sub><sup>2−</sup>, and TiO<sub>2</sub>, respectively.</p>
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<p>The band structures of TiO<sub>2</sub>, TiO<sub>2</sub>-NO<sub>3</sub><sup>−</sup>, TiO<sub>2</sub>-CO<sub>3</sub><sup>2−</sup>, TiO<sub>2</sub>-SO<sub>4</sub><sup>2−</sup>, TiO<sub>2</sub>-Ti-F<sup>−</sup>, TiO<sub>2</sub>-Ti-Cl<sup>−</sup>, TiO<sub>2</sub>-Ti-Br<sup>−</sup>, and TiO<sub>2</sub>-Ti-I<sup>−</sup>. The red dotted line represents high symmetry points.</p>
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<p>The band alignments before and after anion adsorption.</p>
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<p>(<b>a</b>–<b>h</b>) Density of states of TiO<sub>2</sub>, TiO<sub>2</sub>-NO<sub>3</sub><sup>−</sup>, TiO<sub>2</sub>-CO<sub>3</sub><sup>2−</sup>, TiO<sub>2</sub>-SO<sub>4</sub><sup>2−</sup>, TiO<sub>2</sub>-Ti-F<sup>−</sup>, TiO<sub>2</sub>-Ti-Cl<sup>−</sup>, TiO<sub>2</sub>-Ti-Br<sup>−</sup>, and TiO<sub>2</sub>-Ti-I<sup>−</sup>.</p>
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<p>The optical absorption spectra before and after anion adsorption.</p>
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<p>The Gibbs free energy for NRR on TiO<sub>2</sub> before and after anion adsorption. “*” represents free electrons.</p>
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14 pages, 3432 KiB  
Article
Extended Interfacial Charge Transference in CoFe2O4/WO3 Nanocomposites for the Photocatalytic Degradation of Tetracycline Antibiotics
by Suiying Dong, Jiafu Dai, Ying Yang, Amir Zada and Kezhen Qi
Molecules 2024, 29(19), 4561; https://doi.org/10.3390/molecules29194561 - 25 Sep 2024
Viewed by 189
Abstract
The large-scale utilization of antibiotics has opened a separate chapter of pollution with the generation of reactive drug-resistant bacteria. To deal with this, in this work, different mass ratios of CoFe2O4/WO3 nanocomposites were prepared following an in situ [...] Read more.
The large-scale utilization of antibiotics has opened a separate chapter of pollution with the generation of reactive drug-resistant bacteria. To deal with this, in this work, different mass ratios of CoFe2O4/WO3 nanocomposites were prepared following an in situ growth method using the precursors of WO3 and CoFe2O4. The structure, morphology, and optical properties of the nanocomposite photocatalysts were scrutinized by X-ray diffraction (XRD), UV-visible diffuse reflectance spectra (UV-Vis DRS), photoluminescence spectrum (PL), etc. The experimental data signified that the loading of CoFe2O4 obviously changed the optical properties of WO3. The photocatalytic performance of CoFe2O4/WO3 composites was investigated by considering tetracycline as a potential pollutant. The outcome of the analyzed data exposed that the CoFe2O4/WO3 composite with a mass ratio of 5% had the best degradation performance for tetracycline eradication under the solar light, and a degradation efficiency of 77% was achieved in 20 min. The monitored degradation efficiency of the optimized photocatalyst was 45% higher compared with the degradation efficiency of 32% for pure WO3. Capturing experiments and tests revealed that hydroxyl radical (·OH) and hole (h+) were the primary eradicators of the target pollutant. This study demonstrates that a proper mass of CoFe2O4 can significantly push WO3 for enhanced eradication of waterborne pollutants. Full article
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<p>XRD patterns of WO<sub>3</sub>, CoFe<sub>2</sub>O<sub>4</sub>, and CoFe<sub>2</sub>O<sub>4</sub>/WO<sub>3</sub> samples.</p>
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<p>(<b>a</b>,<b>b</b>) SEM images, (<b>c</b>) EDS energy spectra, and (<b>d</b>) elemental mapping analysis of Co, Fe, O, and W for the sample of 5%CoFe<sub>2</sub>O<sub>4</sub>/WO<sub>3</sub>.</p>
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<p>(<b>a</b>) UV-visible diffuse reflectance spectra; (<b>b</b>) forbidden bandwidth; (<b>c</b>) plot of flat-band potential; (<b>d</b>) energy band structure of the samples.</p>
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<p>(<b>a</b>) Nitrogen adsorption and desorption diagrams of CoFe<sub>2</sub>O<sub>4</sub>, WO<sub>3</sub>, and 5%CoFe<sub>2</sub>O<sub>4</sub>/WO<sub>3</sub> samples; (<b>b</b>) pore size distributions.</p>
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<p>(<b>a</b>) Photocatalytic degradation performance of tetracycline for samples; (<b>b</b>) XRD patterns of 5%CoFe<sub>2</sub>O<sub>4</sub>/WO<sub>3</sub> before and after reaction; (<b>c</b>) Effect of different capture agents on the performance of photocatalytic degradation of tetracycline with 5%CoFe<sub>2</sub>O<sub>4</sub>/WO<sub>3</sub>; (<b>d</b>) fluorescence spectroscopy; (<b>e</b>) alternating current impedance spectra; and (<b>f</b>) photocurrent response.</p>
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<p>Reaction mechanism of the photocatalytic degradation of tetracycline by CoFe<sub>2</sub>O<sub>4</sub>/WO<sub>3</sub>.</p>
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33 pages, 14062 KiB  
Article
Parametric Characterization of Nonlinear Optical Susceptibilities in Four-Wave Mixing: Solvent and Molecular Structure Effects
by José L. Paz, Alberto Garrido-Schaeffer, Marcos A. Loroño, Lenin González-Paz, Edgar Márquez, José R. Mora and Ysaias J. Alvarado
Symmetry 2024, 16(10), 1263; https://doi.org/10.3390/sym16101263 - 25 Sep 2024
Viewed by 258
Abstract
We study the nonlinear absorptive and dispersive optical properties of molecular systems immersed in a thermal reservoir interacting with a four-wave mixing (FWM) signal. Residual spin-orbit Hamiltonians are considered in order to take into account the internal structure of the molecule. As system [...] Read more.
We study the nonlinear absorptive and dispersive optical properties of molecular systems immersed in a thermal reservoir interacting with a four-wave mixing (FWM) signal. Residual spin-orbit Hamiltonians are considered in order to take into account the internal structure of the molecule. As system parameters in the dissipation processes, transverse and longitudinal relaxation times are considered for stochastic solute–solvent interaction processes. The intramolecular coupling effects on the optical responses are studied using a molecule model consisting of two coupled harmonic curves of electronic energies with displaced minima in nuclear energies and positions. In this study, the complete frequency space is considered through the pump–probe detuning, without restricting the derivations to only maximums of population oscillations. This approach opens the possibility of studying the behavior of optical responses, which is very useful in experimental design. Our results indicate the sensitivity of the optical responses to parameters of the molecular structure as well as to those derived from the photonic process of FWM signal generation. Full article
(This article belongs to the Section Physics)
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<p>Nonlinear refractive index as a function of pump detuning in frequency space <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mo>Δ</mo> <mn>1</mn> </msub> <mo>,</mo> <msub> <mo>Δ</mo> <mn>2</mn> </msub> <mo stretchy="false">)</mo> <mo stretchy="false">(</mo> <msup> <mi mathvariant="normal">s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </semantics></math>, considering different transverse relaxation times <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">T</mi> <mn>2</mn> </msub> <mo stretchy="false">(</mo> <mi mathvariant="normal">p</mi> <mi mathvariant="normal">s</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>.</p>
Full article ">Figure 2
<p>Refraction index as a function of detuning for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>, at different transversal relaxation times.</p>
Full article ">Figure 3
<p>Effect of transverse relaxation time T<sub>2</sub> on the nonlinear refractive index for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math> (keeping all other parameters constant).</p>
Full article ">Figure 4
<p>Nonlinear refractive index as a function of pump- and probe-detuning, considering different ratios (<math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">T</mi> <mn>1</mn> </msub> <mo>/</mo> <msub> <mi mathvariant="normal">T</mi> <mn>2</mn> </msub> </mrow> </semantics></math>) of relaxation times.</p>
Full article ">Figure 5
<p>Study of dispersive responses with pumping detuning (normalized) for particular processes: <math display="inline"><semantics> <mrow> <msub> <mo>ω</mo> <mn>2</mn> </msub> <mo>=</mo> <msub> <mo>ω</mo> <mn>1</mn> </msub> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mn>2</mn> <msub> <mo>ω</mo> <mn>2</mn> </msub> <mo>−</mo> <msub> <mo>ω</mo> <mn>1</mn> </msub> <mo>=</mo> <msub> <mover accent="true"> <mo>ω</mo> <mo>˜</mo> </mover> <mn>0</mn> </msub> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mn>2</mn> <msub> <mo>ω</mo> <mn>1</mn> </msub> <mo>−</mo> <msub> <mo>ω</mo> <mn>2</mn> </msub> <mo>=</mo> <msub> <mover accent="true"> <mo>ω</mo> <mo>˜</mo> </mover> <mn>0</mn> </msub> </mrow> </semantics></math>, as a function of the <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">T</mi> <mn>1</mn> </msub> <mo>/</mo> <msub> <mi mathvariant="normal">T</mi> <mn>2</mn> </msub> </mrow> </semantics></math> ratio.</p>
Full article ">Figure 6
<p>Time effect of the ratio of relaxation times <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">T</mi> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">T</mi> <mn>2</mn> </msub> </mrow> </semantics></math> (3D) on the nonlinear refractive index for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 7
<p>Effect of coupling between the molecular system and the thermal reservoir on the nonlinear refractive index for any ratio of frequencies <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 8
<p>Effect of coupling between the molecular system and the thermal reservoir on the nonlinear refractive index for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 9
<p>Effect of coupling between the molecular system and the thermal reservoir (3D) on the nonlinear refractive index for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 10
<p>Effect of total saturation <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">S</mi> <mrow> <mn>12</mn> </mrow> </msub> </mrow> </semantics></math> on the nonlinear refractive index for any ratio of frequencies <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 11
<p>Effect of total saturation <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">S</mi> <mrow> <mn>12</mn> </mrow> </msub> </mrow> </semantics></math> (2D) on the nonlinear refractive index for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>, as a function of the pump–probe detuning.</p>
Full article ">Figure 12
<p>Effect of total saturation <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">S</mi> <mrow> <mn>12</mn> </mrow> </msub> </mrow> </semantics></math> (3D) on the nonlinear refractive index for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 13
<p>Effect of intramolecular coupling on the nonlinear refractive index for any ratio of frequencies <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>, as a function of the pump–probe detuning.</p>
Full article ">Figure 14
<p>Effect of intramolecular coupling on the nonlinear refractive index for selected frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>, as a function of normalized pump detuning.</p>
Full article ">Figure 15
<p>Effect of intramolecular coupling on the nonlinear refractive index for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>, as a function of normalized pump detuning.</p>
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<p>Nonlinear absorption coefficient as a function of pump–probe detuning in frequency space parameterized by transverse relaxation times.</p>
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<p>Effect of transverse relaxation time T<sub>2</sub> on the nonlinear absorption coefficient as a function of pump detuning in the three processes shown.</p>
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<p>Effect of transverse relaxation time T<sub>2</sub> (3D) on the nonlinear absorption coefficient for any ratio of frequencies <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Effect of the ratio of relaxation times <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">T</mi> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">T</mi> <mn>2</mn> </msub> </mrow> </semantics></math> on the nonlinear absorption coefficient as function of <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 20
<p>Effect of the ratio of relaxation times <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">T</mi> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">T</mi> <mn>2</mn> </msub> </mrow> </semantics></math> on the nonlinear absorption coefficient in the three processes shown.</p>
Full article ">Figure 21
<p>The nonlinear absorption coefficient as function of pump-detuning and ratio of relaxation times.</p>
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<p>Effect of coupling between the molecular system and the thermal reservoir on the nonlinear absorption coefficient for any ratio of frequencies <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Nonlinear absorption coefficient as a function of pump beam detuning. We have taken into account different intensities of coupling between the molecular system and the thermal reservoir.</p>
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<p>Nonlinear absorption coefficient as a function of pumping detuning and system-reservoir coupling in the three selected frequency coordinates.</p>
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<p>Effect of total saturation <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">S</mi> <mrow> <mn>12</mn> </mrow> </msub> </mrow> </semantics></math> on the nonlinear absorption coefficient for any ratio of frequencies <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Effect of total saturation <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">S</mi> <mrow> <mn>12</mn> </mrow> </msub> </mrow> </semantics></math> (2D) on the nonlinear absorption coefficient for selected frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Nonlinear absorption coefficient as a function of pumping detuning and saturation parameter of pump-beam, in the three selected frequency coordinates.</p>
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<p>Effect of intramolecular coupling on the nonlinear absorption coefficient for any ratio of frequencies <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Effect of intramolecular (2D) coupling on the nonlinear absorption coefficient for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Effect of intramolecular (3D) coupling on the nonlinear absorption coefficient for given frequency ratios <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Comparison between scattering and absorption profiles at the frequency of interest when considering different ratios between pumping and test beam frequencies.</p>
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<p>Nonlinear refractive index as a function of pumping beam detuning for the processes <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> <mo>=</mo> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math>, considering different orders of perturbation according to Equation (16).</p>
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<p>Nonlinear absorption coefficient as a function of detuning in processes <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> <mo>=</mo> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mo>Δ</mo> <mn>2</mn> </msub> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mo>Δ</mo> <mn>1</mn> </msub> </mrow> </semantics></math>, considering different perturbation treatments (Equation (23)).</p>
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18 pages, 7146 KiB  
Article
Non-Invasive Optoacoustic Imaging for In-Depth Cultural Heritage Diagnostics
by George J. Tserevelakis, Eleanna Pirgianaki, Kristalia Melessanaki, Giannis Zacharakis and Costas Fotakis
Photonics 2024, 11(10), 902; https://doi.org/10.3390/photonics11100902 - 25 Sep 2024
Viewed by 205
Abstract
The complex composition of cultural heritage (CH) items presents significant challenges in assessing their condition and predicting potential risks of material degradation. Typically employed diagnostic optical methods are inevitably limited by light scattering, thus restricting in-depth investigations of objects with complex structural and [...] Read more.
The complex composition of cultural heritage (CH) items presents significant challenges in assessing their condition and predicting potential risks of material degradation. Typically employed diagnostic optical methods are inevitably limited by light scattering, thus restricting in-depth investigations of objects with complex structural and optical properties. To address this issue, we introduce a novel reflection-mode optoacoustic (OA) diagnostic system for non-contact and non-invasive measurements of CH, placing emphasis on the detection of ageing-related modifications in artistic media such as paints. In this direction, the sensitivity of OA measurements was proven to be up to two orders of magnitude higher than conventional absorption spectroscopy assessments. Furthermore, we have evaluated the in-depth imaging capabilities of the developed OA system, demonstrating that it can offer superior contrast levels of sketches beneath opaque paint layers compared to standard near-infrared diagnostic techniques. The current OA imaging technology may advance state-of-the-art diagnostic capabilities in CH preservation by delivering unprecedented depth-to-resolution ratios combined with exceptional optical absorption sensitivity in a non-invasive manner. These features are crucial for the early detection of material degradation and the comprehensive analysis of CH objects, facilitating the development of optimal conservation strategies to prolong their lifespan and preserve their aesthetic value. Full article
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<p>OA imaging apparatus and performance characterization. (<b>a</b>) Schematical representation of the developed non-invasive, reflection-mode OA imaging apparatus for artworks diagnosis. (<b>b</b>) Time-domain OA signal from a graphite spot with a diameter of ~180 μm. (<b>c</b>) Amplitude spectrum of the waveform shown in (<b>b</b>), which peaked at 950 kHz (dotted red line). (<b>d</b>) OA image of the graphite spot. Scalebar is equal to 400 μm. (<b>e</b>) Pixel intensity profile extracted from (<b>d</b>). The data points (black dots) have been fitted (R<sup>2</sup> = 0.995) with a gaussian function (red curve), yielding a FWHM value equal to 772 μm.</p>
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<p>OA amplitude measurements of artificially aged paint samples. (<b>a</b>) Non-aged yellow ochre paint sample. (<b>b</b>–<b>d</b>) Thermally aged ochre yellow paint samples for 2, 4 and 6 h, respectively. (<b>e</b>) Typical OA signals arising from the aforementioned yellow ochre paints following the averaging of 32 waveforms. A fixed temporal delay of 1 μs has been inserted among the four signals to facilitate the visualization of OA pressure perturbations. (<b>f</b>) Mean OA amplitude versus thermal-ageing time. Error bars correspond to ± one standard deviation out of 10 consecutive measurements. The red curve corresponds to an exponential fitting with R<sup>2</sup> approximately equal to 0.999. (<b>g</b>–<b>j</b>) Similar images for thermally aged Prussian blue paint samples. (<b>k</b>) Typical OA signals arising from the Prussian blue paints. (<b>l</b>) Respective graph showing the mean OA amplitude versus thermal ageing time. The data points have been fitted (red line) using a linear regression model (R<sup>2</sup> = 0.989).</p>
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<p>OA and NIR imaging of painted canvas mock-ups. (<b>a</b>) Photo of a titanium white canvas mock-up covered with shellac varnish. The red square indicates a 2 by 2 cm<sup>2</sup> area which is scanned using the OA imaging modality. (<b>b</b>) Photo of the pencil underdrawing before the application of the paint for the mock-up shown in (<b>a</b>). (<b>c</b>) OA image of the underdrawing. (<b>d</b>) Respective NIR image of the same region as in (<b>c</b>). Scalebar corresponds to 5 mm. (<b>e</b>–<b>h</b>) Similar results for the case of an ultramarine blue mock-up. (<b>i</b>–<b>l</b>) Similar results for a mixed titanium white and ultramarine blue mock-up. (<b>m</b>–<b>p</b>) Similar results for an ultramarine blue mock-up which is not covered with shellac varnish.</p>
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<p>OA and NIR imaging of painted gypsum mock-ups. (<b>a</b>) Photo of 5 by 5 cm<sup>2</sup> region depicting a titanium white gypsum mock-up with no applied varnish. The red square indicates a 2.6 by 2.6 cm<sup>2</sup> area which is scanned using the OA imaging modality. (<b>b</b>) Photo of the pencil underdrawing before the application of the paint for the mock-up shown in (<b>a</b>). (<b>c</b>) OA image of the underdrawing. (<b>d</b>) Respective NIR image of the same region as in (<b>c</b>). Scalebar corresponds to 5 mm. (<b>e</b>–<b>h</b>) Similar results for an ultramarine blue mock-up. (<b>i</b>–<b>l</b>) Similar results for a mixed titanium white and ultramarine blue mock-up. In this case, the red square shown in (<b>i</b>) delineates an area of 3.2 by 3.2 cm<sup>2</sup> corresponding to the OA scanning region.</p>
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<p>Investigation of potential alterations following the application and removal of the gelatin layer. (<b>a</b>) Photo of the titanium white gypsum mock-up covered with a thin gelatin layer. The red arrow shows one of the areas that was further inspected by means of digital microscopy. (<b>b</b>) Photo of the same mock-up directly after gelatin layer removal. (<b>c</b>) 2 by 2 mm<sup>2</sup> digital microscopy image of the region indicated with the red arrow in (<b>a</b>) prior the gelatin application. (<b>d</b>) Digital microscopy image of the same region as in (<b>c</b>) directly after the gelatin layer removal. Scalebar is equal to 0.5 mm. (<b>e</b>–<b>h</b>) Similar results for an ultramarine blue mock-up. (<b>i</b>–<b>l</b>) Similar results for a mixed titanium white and ultramarine blue mock-up.</p>
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<p>OA and NIR imaging of titanium white gypsum mock-ups with gradually increasing paint layer thickness. (<b>a</b>) Circular mock-up covered with 60 μm thick titanium white paint (5 by 5 cm<sup>2</sup> region is shown). The red square indicates a 2 by 2 cm<sup>2</sup> area which is subsequently imaged using both OA and NIR modalities. (<b>b</b>) Charcoal X-shaped sketch before the paint application. (<b>c</b>) OA image of the hidden “X” pattern. (<b>d</b>) Respective NIR image of the same region. Similar results are shown for gypsum mock-ups covered with 120 μm (<b>e</b>–<b>h</b>), 180 μm (<b>i</b>–<b>l</b>) and finally 240 μm (<b>m</b>–<b>p</b>) thick titanium white paint layers.</p>
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<p>SNR and imaging contrast quantification as a function of paint layer thickness. (<b>a</b>) Graph of OA image SNR versus paint layer thickness estimated from the data presented in <a href="#photonics-11-00902-f006" class="html-fig">Figure 6</a>. Error bars represent the ± one standard error of the mean value out of the four measurements in the same image. The red curve corresponds to an exponential decay fitting of the data points (R<sup>2</sup> = 0.990). (<b>b</b>) A graph of the Michelson contrast values for the OA and NIR images presented in <a href="#photonics-11-00902-f005" class="html-fig">Figure 5</a>. Error bars represent the ± one standard error of the mean values out of the four measurements in the same image. The data have been similarly fitted with exponential decay functions (red and blue curves) with R<sup>2</sup> &gt; 0.994 in both cases.</p>
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19 pages, 6939 KiB  
Article
Quantitative Assessment of Polarization and Elastic Properties of Endometrial Tissue for Precancer/Cancer Diagnostics Using Multimodal Optical Coherence Tomography
by Anton A. Plekhanov, Gennady O. Grechkanev, Elena A. Avetisyan, Maria M. Loginova, Elena B. Kiseleva, Anastasia A. Shepeleva, Alexander A. Moiseev, Alexander A. Sovetsky, Ekaterina V. Gubarkova, Anastasia A. Anina, Angelina M. Shutova, Sergey V. Gamayunov, Grigory V. Gelikonov, Vladimir Y. Zaitsev, Marina A. Sirotkina and Natalia D. Gladkova
Diagnostics 2024, 14(19), 2131; https://doi.org/10.3390/diagnostics14192131 - 25 Sep 2024
Viewed by 201
Abstract
Objectives: The most important phase in the endometrial pathologies diagnostics is the histological examination of tissue biopsies obtained under visual hysteroscopic control. However, the unclear visual diagnostics characteristics of subtle focal endometrial pathologies often lead to selection errors regarding suspicious endometrial lesions [...] Read more.
Objectives: The most important phase in the endometrial pathologies diagnostics is the histological examination of tissue biopsies obtained under visual hysteroscopic control. However, the unclear visual diagnostics characteristics of subtle focal endometrial pathologies often lead to selection errors regarding suspicious endometrial lesions and to a subsequent false pathological diagnosis/underestimation of precancer or early-stage cancer. Methods: In this study, we investigate the potential of Multimodal Optical Coherence Tomography (MM OCT) to verify suspicious endometrial lesion regions before biopsy collection. We study the polarization (by cross-polarization OCT, CP OCT) and elastic (by compression OCT-elastography, C-OCE) properties of ex vivo endometrial tissue samples in normal conditions (proliferative and secretory phases to the menstrual cycle, atrophic endometrium) with endometrial hyperplasia (non-atypical and endometrial intraepithelial neoplasia) and endometrial cancer subtypes (low-grade, high-grade, clear cell and serous). Results: To the best of our knowledge, this is the first quantitative assessment of relevant OCT parameters (depth-resolved attenuation coefficient in co-[Att(co) values] and cross-[(Att(cross) values] polarizations and Young’s elastic modulus [stiffness values]) for the selection of the most objective criteria to identify the clinically significant endometrial pathologies: endometrial intraepithelial neoplasia and endometrial cancer. The study demonstrates the possibility of detecting endometrial pathologies and establishing optimal threshold values of MM OCT criteria for the identification of endometrial cancer using CP OCT (by Att(co) values = 3.69 mm−1, Sensitivity (Se) = 86.1%, Specificity (Sp) = 92.6%; by Att(cross) values = 2.27 mm−1, Se = 86.8%, Sp = 87.0%) and C-OCE (by stiffness values = 122 kPa, Se = 93.2%, Sp = 91.1%). The study also differentiates endometrial intraepithelial neoplasia from non-atypical endometrial hyperplasia and normal endometrium using C-OCE (by stiffness values = 95 kPa, Se = 87.2%, Sp = 90.1%). Conclusions: The results are indicative of the efficacy and potential of clinical implementation of in vivo hysteroscopic-like MM OCT in the diagnosis of endometrial pathologies. Full article
(This article belongs to the Special Issue Imaging for the Diagnosis of Obstetric and Gynecological Diseases)
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<p>Comparison of the representative cases of normal endometrium (by example of secretory endometrium) (<b>A1</b>–<b>D1</b>), non-atypical endometrial hyperplasia (<b>A2</b>–<b>D2</b>), EIN (<b>A3</b>–<b>D3</b>) and EC (by example of low-grade EC) (<b>A4</b>–<b>D4</b>), where the following are presented: histological images (<b>A1</b>–<b>A4</b>), attenuation coefficient maps for co-polarization OCT images (<b>B1</b>–<b>B4</b>), attenuation coefficient maps for cross-polarization OCT images (<b>C1</b>–<b>C4</b>), C-OCE images (<b>D1</b>–<b>D4</b>); dotted lines and white arrows indicate border between endometrium and myometrium; bar size in all images is 0.5 mm.</p>
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<p>Boxplots for established Att(co) (<b>A</b>), Att(cross) (<b>B</b>), stiffness (<b>C</b>) values counted for each endometrial tissue types: normal endometrium, including proliferative, secretory and atrophy, indicated by green boxplots; endometrial hyperplasia, including non-atypical hyperplasia and EIN, indicated by orange boxplots; and different subtypes EC, including low-grade, high-grade, clear cell and serous, indicated by red boxplots. Centerline in the boxes—median; box limits—25th and 75th percentiles; whiskers—5th and 95th percentiles. Panel (<b>D</b>) shows the matrix of pairwise differential comparisons between different MM OCT parameters (●—Att(co) values, ■—Att(cross) values, ▲—stiffness values) for various endometrial tissue (Mann–Whitney U-test with a Bonferroni correction for multiple comparisons). The purple partitions indicate the possibility of differentiating EIN from benign endometrial tissues (non-atypical endometrial hyperplasia and normal endometrium). The blue partitions indicate the possibility of differentiating EC from endometrial hyperplasia and normal endometrium.</p>
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<p>ROC curves showing the results for differentiation: EC from endometrial hyperplasia and normal endometrium (<b>A</b>–<b>C</b>), EIN from non-atypical hyperplasia and normal endometrium (<b>D</b>–<b>F</b>) based on the analysis of Att(co) (<b>A</b>,<b>D</b>), Att(cross) (<b>B</b>,<b>E</b>) and stiffness (<b>C</b>,<b>F</b>) values. Symbols (●—Att(co), ■—Att(cross), ▲—stiffness) on the curves represent choices of the threshold value (Pth) using a trade–off between the percentages of the false negative and false positive outcomes; designations: Se—sensitivity, Sp—specificity.</p>
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<p>Representative cases of endometrial tissue in normal and with endometrial hyperplasia, where the following are presented: histological images (<b>A1</b>–<b>A5</b>), co-polarization OCT images (<b>B1</b>–<b>B5</b>), attenuation coefficient maps for co-polarization OCT images (<b>C1</b>–<b>C5</b>), cross-polarization OCT images (<b>D1</b>–<b>D5</b>), attenuation coefficient maps for cross-polarization OCT images (<b>E1</b>–<b>E5</b>), C-OCE images (<b>F1</b>–<b>F5</b>). Cases of normal endometrium include a study of premenopausal women with proliferative (<b>A1</b>–<b>F1</b>) and secretory (<b>A2</b>–<b>F2</b>) endometrium and postmenopausal women with atrophic (<b>A3</b>–<b>F3</b>) endometrium; endometrial hyperplasia tissues include non-atypical hyperplasia (<b>A4</b>–<b>F4</b>) and EIN (<b>A5</b>–<b>F5</b>); a dotted line in histological images represents a visible border between the endometrium and myometrium. The bar size in all images is 0.5 mm.</p>
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<p>Representative cases of endometrial tissue with EC, where the following are presented: histological images (<b>A1</b>–<b>A4</b>), co-polarization OCT images (<b>B1</b>–<b>B4</b>), attenuation coefficient maps for co-polarization OCT images (<b>C1</b>–<b>C4</b>), cross-polarization OCT images (<b>D1</b>–<b>D4</b>), attenuation coefficient maps for cross-polarization OCT images (<b>E1</b>–<b>E4</b>), C-OCE images (<b>F1</b>–<b>F4</b>). Cases of EC include a study of next morphological subtypes: low-grade EC (<b>A1</b>–<b>F1</b>), high-grade EC (<b>A2</b>–<b>F2</b>), clear cell EC (<b>A3</b>–<b>F3</b>) and serous EC (<b>A4</b>–<b>F4</b>). The bar size in all images is 0.5 mm.</p>
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22 pages, 21927 KiB  
Article
Antimicrobial, Optical, and Mechanical Properties of Saliva-Contaminated Silver–Zeolite Nanoparticle-Incorporated Dental Acrylic Resins
by Çisel Kısa Yaman, Necla Demir, Uğur Arslan and Nurullah Çiftçi
Inorganics 2024, 12(10), 258; https://doi.org/10.3390/inorganics12100258 - 25 Sep 2024
Viewed by 207
Abstract
Background and Purpose: This study aimed to evaluate the flexural strength, color change and antimicrobial effect of silver–zeolite nanoparticles (NPs) in acrylic resin materials. Methods: Fifty-six disc-shaped acrylic resin samples were divided into four groups (n = 7) according to concentrations of [...] Read more.
Background and Purpose: This study aimed to evaluate the flexural strength, color change and antimicrobial effect of silver–zeolite nanoparticles (NPs) in acrylic resin materials. Methods: Fifty-six disc-shaped acrylic resin samples were divided into four groups (n = 7) according to concentrations of silver–zeolite NPs (0%, 2%, 4%, 5%). Discs were contaminated with C. albicans and S. mutans. The antimicrobial effect was tested by inoculating contaminated discs on Tryptic soy agar (TSA), Sabouraud Dextrose Agar (SDA), Tryptic soy broth (TSB), and Sabouraud dextrose broth (SDB). Forty rectangular 65 × 10 × 2.5 mm acrylic resin specimens were also classified into four groups (n = 10) according to concentrations of silver–zeolite NPs. For the color change, L, a, and b values of rectangular specimens were examined with a spectrophotometer. A three-point bending test was also performed using a Devotrans device to determine the flexural bond strength of rectangular specimens. Scanning electron microscope analysis (SEM/EDX analysis) was also performed. Results: In this study, the antimicrobial effect increased with the concentration of silver–zeolite NPs added to acrylic resin discs. In our study, adding 2% silver–zeolite NPs was more effective against C. albicans. The antimicrobial effect against S. mutans increased with concentration of silver–zeolite NPs (<0.001). The colonization of C. albicans was significantly reduced by silver–zeolite NPs. A significant increase was observed in the color change as the nanoparticle percentage ratio increased (p < 0.001). The flexural strength values of the groups containing 2% and 4% nanoparticles were found to be clinically acceptable. Conclusions: The study showed that bacterial and fungal colonization is significantly reduced by adding silver–zeolite nanoparticles to acrylic resin discs. Based on its antimicrobial, physical, and mechanical properties, we recommend adding 2% silver–zeolite nanoparticles to the acrylic resin material for optimal results. Full article
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<p>Surface topography of the discs by SEM images. (<b>A</b>) Control group surface topography (from left to right 300×/500×/1000× magnification); (<b>B</b>) 2% NPs added discs surface topography (from left to right 300×/500×/1000× magnification); (<b>C</b>) 4% NPs added discs surface topography (from left to right 300×/500×/1000× magnification); (<b>D</b>) 5% NPs added discs surface topography (from left to right 300×/500×/1000× magnification).</p>
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<p>Ag Images with SEM/EDX in the (<b>A</b>) 2%, (<b>B</b>) 4%, and (<b>C</b>) 5% (respectively, up to down) groups.</p>
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<p>ΔE2000 color change of the groups.</p>
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<p>Flexural strength values of three-point bending strength test.</p>
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<p>SEM Images of Fracture Surface of Control Group 300×/500×/1.00K× magnification: (<b>a</b>) Mist zone, (<b>b</b>) Hackle zone, (<b>c</b>) Nano-crack.</p>
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<p>SEM Images of Fracture Surface of 2% Group 300×/500×/1.00K× Magnification: (<b>a</b>) 2% Ag/Z group agglomeration, (<b>b</b>) 2% Ag/Z group agglomeration, (<b>c</b>) Increase in the number of nano-cracks.</p>
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<p>4% Group Fracture Surface SEM Images 300×/500×/1.00K× Magnification: (<b>a</b>) Increase in the number of nano-fractures, (<b>b</b>) 4% Ag/Z group agglomeration, (<b>c</b>) Increase in the size of nano-fractures.</p>
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<p>5% Group Fracture Surface SEM Images 300×/500×/1.00K× Magnification: (<b>a</b>,<b>b</b>) 5% Ag/Z group agglomeration, (<b>c</b>) Hackle zone expansion, nano-crack length increase.</p>
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<p>The color differences after XTT and PMS added.</p>
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<p>Differences in <span class="html-italic">C. albicans and S. mutans</span> concentrations.</p>
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<p>Inoculation of contaminated discs with <span class="html-italic">S. mutans</span> and <span class="html-italic">C. albicans. (</span><b>a</b>) <span class="html-italic">S. mutans</span>, a<sup>1</sup> no silver–zeolite NPs added, a<sup>2</sup> discs with 2% silver–zeolite NPs, a<sup>3</sup> discs with 4% silver–zeolite NPs, a<sup>4</sup> discs with 5% silver–zeolite NPs; (<b>b</b>) <span class="html-italic">C. albicans</span>, b<sup>1</sup> no silver–zeolite NPs added, b<sup>2</sup> discs with 2% silver–zeolite NPs, b<sup>3</sup> discs with 4% silver–zeolite NPs, b<sup>4</sup> discs with 5% silver–zeolite NPs.</p>
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<p>Colony count of <span class="html-italic">C. albicans</span> strains. 1: no silver–zeolite NPs added (Control group), 2: discs with 2% silver–zeolite NPs, 3: discs with 4% silver–zeolite NPs, 4: discs with 5% silver–zeolite NPs.</p>
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<p>Colony count of <span class="html-italic">S. mutans</span> strains; 1: no silver–zeolite NPs added (Control group), 2: discs with 2% silver–zeolite NPs, 3: discs with 4% silver–zeolite NPs, 4: discs with 5% silver–zeolite NPs.</p>
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13 pages, 4755 KiB  
Article
Surfactant-Assisted Regulation of WS2/Tourmaline Microstructures for Excellent Photocatalytic Performance
by Xianku Wang, Kaibin Cui, Yuqin Zhao, Ming Hao, Liang Bian, Mingming Wang and Fei Wang
Molecules 2024, 29(19), 4555; https://doi.org/10.3390/molecules29194555 - 25 Sep 2024
Viewed by 166
Abstract
The controllable electrical and optical properties of two-dimensional tungsten disulfide (WS2) attracted much attention in photocatalysis, but commercial development has been severely restricted by their restacking properties. Surfactant-assisted synthesis techniques can be considered as an effective option to break this bottleneck. [...] Read more.
The controllable electrical and optical properties of two-dimensional tungsten disulfide (WS2) attracted much attention in photocatalysis, but commercial development has been severely restricted by their restacking properties. Surfactant-assisted synthesis techniques can be considered as an effective option to break this bottleneck. In this work, the effect of surfactants including sodium dodecylbenzene sulfonate (SDBS), hexadecyltrimethylammonium bromide (CTAB), and polyvinylpyrrolidone (PVP) on the microstructure of WS2/tourmaline composites prepared by coupled hydrothermal and calcination methods was explored. The WS2 nanosheets were uniformly deposited on the tourmaline surface with the assistance of 1.0 mmol/L SDBS. Meanwhile, WS2/Tour-SDBS exhibited the highest rhodamine B (RhB) degradation activity, which was 1.8 and 2.3 times higher than that of photocatalysts prepared with CTAB and PVP under the same conditions, respectively. This study provides a new tactic for the fabrication of high-performance WS2-based composites. Full article
(This article belongs to the Special Issue Renewable Energy, Fuels and Chemicals from Biomass)
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<p>(<b>a</b>) X-ray diffraction patterns and (<b>b</b>) FTIR spectra of the samples synthesized with different surfactants.</p>
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<p>SEM images of the samples synthesized with different surfactants. (<b>a</b>) Control; (<b>b</b>) SDBS; (<b>c</b>) CTAB; and (<b>d</b>) PVP.</p>
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<p>(<b>a</b>) N<sub>2</sub> adsorption–desorption curves and (<b>b</b>) pore size distributions at the sample site.</p>
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<p>(<b>a</b>–<b>d</b>) Time dependence of the UV–vis absorption spectra in photodegradation of RhB on WS<sub>2</sub>/tourmaline prepared without surfactant (<b>a</b>), with SDBS (<b>b</b>), CTAB (<b>c</b>), and PVP (<b>d</b>). (<b>e</b>) Photocatalytic performance for as-prepared composites toward RhB degradation.</p>
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<p>(<b>a</b>) X-ray diffraction patterns and (<b>b</b>) crystalline size of the samples synthesized with different concentrations of SDBS.</p>
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<p>SEM images of the samples synthesized with different concentrations of SDBS: (<b>a</b>) 0.5 mmol/L; (<b>b</b>) 1.0 mmol/L; (<b>c</b>) 1.5 mmol/L; and (<b>d</b>) 2.0 mmol/L.</p>
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<p>Time dependence of the UV–vis absorption spectra in photodegradation of RhB on WS<sub>2</sub>/tourmaline prepared with different concentrations of SDBS: (<b>a</b>) 0.5 mmol/L; (<b>b</b>) 1.0 mmol/L; (<b>c</b>) 1.5 mmol/L; and (<b>d</b>) 2.0 mmol/L. (<b>e</b>) Photocatalytic performance for as-prepared composites toward RhB degradation.</p>
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<p>(<b>a</b>) Cyclic regeneration assay for RhB degradation by WS<sub>2</sub>/Tour-SDBS. (<b>b</b>) Diagram of adsorption properties of catalysts during dark reactions.</p>
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<p>Growth mechanism of WS<sub>2</sub>/Tour with SDBS as a soft template.</p>
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<p>(<b>a</b>) Schematic diagram of the synergy between WS<sub>2</sub> and tourmaline in RhB photocatalytic degradation. (<b>b</b>) UV–vis diffuse reflectance spectra of WS<sub>2</sub>/Tour-SDBS and WS<sub>2</sub>; (<b>c</b>) the corresponding plot of (αhν)<sup>2</sup> versus hν for WS<sub>2</sub>/Tour-SDBS and WS<sub>2</sub>.</p>
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23 pages, 652 KiB  
Review
Advances in Neuroprotection in Glaucoma: Pharmacological Strategies and Emerging Technologies
by Li-Hsin Wang, Chun-Hao Huang and I-Chan Lin
Pharmaceuticals 2024, 17(10), 1261; https://doi.org/10.3390/ph17101261 - 25 Sep 2024
Viewed by 274
Abstract
Glaucoma is a major global health concern and the leading cause of irreversible blindness worldwide, characterized by the progressive degeneration of retinal ganglion cells (RGCs) and their axons. This review focuses on the need for neuroprotective strategies in glaucoma management, addressing the limitations [...] Read more.
Glaucoma is a major global health concern and the leading cause of irreversible blindness worldwide, characterized by the progressive degeneration of retinal ganglion cells (RGCs) and their axons. This review focuses on the need for neuroprotective strategies in glaucoma management, addressing the limitations of current treatments that primarily target intraocular pressure (IOP) reduction. Despite effective IOP management, many patients continue to experience RGC degeneration, leading to irreversible blindness. This review provides an overview of both pharmacological interventions and emerging technologies aimed at directly protecting RGCs and the optic nerve, independent of IOP reduction. Pharmacological agents such as brimonidine, neurotrophic factors, memantine, Ginkgo biloba extract, citicoline, nicotinamide, insulin, and resveratrol show promise in preclinical and early clinical studies for their neuroprotective properties. Emerging technologies, including stem cell therapy, gene therapy, mitochondrial-targeted therapies, and nanotechnologies, offer innovative approaches for neuroprotection and regeneration of damaged RGCs. While these interventions hold significant potential, further research and clinical trials are necessary to confirm their efficacy and establish their role in clinical practice. This review highlights the multifaceted nature of neuroprotection in glaucoma, aiming to guide future research and clinical practice toward more effective management of glaucoma-induced neurodegeneration. Full article
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<p>The mechanisms of glaucoma inducing the loss of retinal ganglion cells and the targets of each neuroprotective compound [<a href="#B5-pharmaceuticals-17-01261" class="html-bibr">5</a>].</p>
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15 pages, 11445 KiB  
Article
Effect of Cr Element in Gas-Shielded Solid Wire for Oil and Gas Long-Distance Pipeline on Microstructure and Low Temperature Toughness of Weld
by Rui Hong, Hai-chun Liu, Xiao-dan Zhu, Neng-sheng Liu, Shu-biao Yin, Qi-lin Ma and Shu-jun Jia
Materials 2024, 17(19), 4704; https://doi.org/10.3390/ma17194704 - 25 Sep 2024
Viewed by 234
Abstract
In this paper, the influence of Cr element on the mechanical properties of welded joints of gas-shielded solid wire used in oil and gas long-distance pipelines was studied by means of tensile test, impact test, and hardness test, and the microstructure and crack [...] Read more.
In this paper, the influence of Cr element on the mechanical properties of welded joints of gas-shielded solid wire used in oil and gas long-distance pipelines was studied by means of tensile test, impact test, and hardness test, and the microstructure and crack propagation path of weld were characterized by means of an optical microscope, scanning electron microscope, and electron backscattering diffraction. The results show that with the addition of Cr, the strength and toughness of the weld are significantly improved, in which the tensile strength is increased from 607 MPa to 656 MPa, and the impact toughness is increased from 126.37 J to 223.79 J. The proportion of the ferrite side plate in the weld structure is reduced by about 20%, and the effective grain size of acicular ferrite is reduced by about 15%. The reason is that the addition of the Cr element improves the hardenability of the weld structure, inhibits the formation of the ferrite side plate, and promotes the effective refinement of acicular ferrite, which increases the proportion of high-angle grain boundaries in the weld, effectively hindering the crack propagation, improves the crack propagation work, and thus improves the strength and toughness of the weld. Full article
(This article belongs to the Section Mechanics of Materials)
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<p>Welding and sampling schematic (<b>a</b>) schematic illustration (<b>b</b>) dimension.</p>
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<p>Macroscopic characteristics of weld metal with different chromium contents: (<b>a</b>) 1# (<b>b</b>) 2#.</p>
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<p>Microstructure of weld metal with different chromium content at different magnifications: (<b>a</b>) 1# Primary Solidification Zone 50×; (<b>b</b>) 1# Primary Solidification Zone 100×; (<b>c</b>) 1# Reheating Zone 100×; (<b>d</b>) 2# Primary Solidification Zone 50×; (<b>e</b>) 1# Primary Solidification Zone 100×; (<b>f</b>) 2# Reheating Zone 100×.</p>
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<p>SEM microstructure characterization of two types of weld metal: (<b>a</b>) 1# 1000×; (<b>b</b>) 1# 2000×; (<b>c</b>) 1# 5000×; (<b>d</b>) 2# 1000×; (<b>e</b>) 2# 2000×; (<b>f</b>) 2# 5000×.</p>
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<p>EBSD images of weld metal with different Cr contents: (<b>a</b>–<b>c</b>) acicular ferrite (AF) structure of 1# weld high- and low-angle grain boundary diagram; IPF diagram; KAM diagram; (<b>d</b>–<b>f</b>) acicular ferrite (AF) structure of 1# weld high- and low-angle grain boundary diagram; IPF diagram; KAM diagram; (<b>h</b>–<b>g</b>) ferrite side plate (FSP) structure of 2# weld high- and low-angle grain boundary diagram; IPF diagram; KAM diagram.</p>
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<p>Different Cr content weld metal: (<b>a</b>) hardness and tensile properties; (<b>b</b>) impact energy; (<b>c</b>) complete load–deflection curve of ductile fracture; (<b>d</b>) experimental load–deflection curves of the 1# and 2# specimen.</p>
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<p>SEM Images of fracture surfaces of impact specimens at −20 °C: (<b>a</b>) 1# 500×; (<b>b</b>) 1# 1000×; (<b>c</b>) 1# 2000×; (<b>d</b>) 2# 500×; (<b>e</b>) 2# 1000×; (<b>f</b>) 2# 2000×.</p>
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<p>Nucleus models include spherical caps with disordered interphase boundaries of interfacial energy γ<sub>αγ</sub>; (<b>a</b>) two spherical caps that are abutting; (<b>b</b>) two spherical caps that are abutting, one of which is truncated by a low energy facet <math display="inline"><semantics> <mrow> <msubsup> <mrow> <mo> </mo> <mi>γ</mi> </mrow> <mrow> <mi>α</mi> <mi>γ</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msubsup> </mrow> </semantics></math>; (<b>c</b>) one spherical cap that is accompanied by a facet with energy <math display="inline"><semantics> <mrow> <msubsup> <mrow> <mi>γ</mi> </mrow> <mrow> <mi>α</mi> <mi>γ</mi> </mrow> <mrow> <mi>c</mi> <mi>b</mi> </mrow> </msubsup> </mrow> </semantics></math> that is low enough to lie in the grain boundary plane; (<b>d</b>) one spherical cap that is truncated by a facet of energy <math display="inline"><semantics> <mrow> <msubsup> <mrow> <mi>γ</mi> </mrow> <mrow> <mi>α</mi> <mi>γ</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msubsup> </mrow> </semantics></math> and is “capped” by a facet in the grain boundary plane.</p>
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<p>Thermodynamic properties diagram (<b>a</b>) Fe-Cr phase diagram (<b>b</b>) A1 and A3 temperatures at different.</p>
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<p>Fracture path of brittle zone in two types of weld metal impact fracture surfaces (<b>a</b>) 1# main crack; (<b>b</b>) 2# main crack; (<b>c</b>) 1# 500×; (<b>d</b>) 1# 1000×; (<b>e</b>) 2# secondary crack 500×; (<b>f</b>) 2# secondary crack 1000×.</p>
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<p>Fracture path of brittle zone in two types of weld metal impact fracture surfaces (<b>a</b>) 1# main crack; (<b>b</b>) 2# main crack; (<b>c</b>) 1# 500×; (<b>d</b>) 1# 1000×; (<b>e</b>) 2# secondary crack 500×; (<b>f</b>) 2# secondary crack 1000×.</p>
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<p>EBSD images of weld metal with different Cr contents: (<b>a</b>–<b>c</b>) 1# high- and low-angle grain boundary diagram; IPF diagram; KAM diagram; (<b>d</b>–<b>f</b>) 2# high- and low-angle grain boundary diagram; IPF diagram; KAM diagram. (<b>g</b>–<b>i</b>) 2# high- and low-angle grain boundary diagram; IPF diagram; KAM diagram.</p>
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