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11 pages, 3801 KiB  
Article
Effect of Bias Voltage on the Microstructure and Photoelectric Properties of W-Doped ZnO Films
by Haijuan Mei, Wanli Wang, Junfeng Zhao, Weilong Zhong, Muyi Qiu, Jiayang Xu, Kailin Gao, Ge Liu, Jianchu Liang and Weiping Gong
Nanomaterials 2024, 14(24), 2050; https://doi.org/10.3390/nano14242050 (registering DOI) - 21 Dec 2024
Abstract
W-doped ZnO (WZO) films were deposited on glass substrates by using RF magnetron sputtering at different substrate bias voltages, and the relationships between microstructure and optical and electrical properties were investigated. The results revealed that the deposition rate of WZO films first decreased [...] Read more.
W-doped ZnO (WZO) films were deposited on glass substrates by using RF magnetron sputtering at different substrate bias voltages, and the relationships between microstructure and optical and electrical properties were investigated. The results revealed that the deposition rate of WZO films first decreased from 8.8 to 7.1 nm/min, and then increased to 11.5 nm/min with the increase in bias voltage. After applying a bias voltage to the substrate, the bombardment effect of sputtered ions was enhanced, and the films transformed from a smooth surface into a compact and rough surface. All the films exhibited a hexagonal wurtzite structure with a strong (002) preferred orientation and grew along the c-axis direction. When the bias voltage increased, both the residual stress and lattice parameter of the films gradually increased, and the maximum grain size of 43.4 nm was achieved at −100 V. When the bias voltage was below −300 V, all the films exhibited a high average transmittance of ~90% in the visible light region. As the bias voltage increased, the sheet resistance and resistivity of the films initially decreased and then gradually increased. The highest FOM of 5.8 × 10−4 Ω1 was achieved at −100 V, possessing the best comprehensive photoelectric properties. Full article
(This article belongs to the Special Issue Design and Applications of Heterogeneous Nanostructured Materials)
10 pages, 3149 KiB  
Article
Density Functional Theory Insight in Photocatalytic Degradation of Dichlorvos Using Covalent Triazine Frameworks Modified by Various Oxygen-Containing Acid Groups
by Shouxi Yu and Zhongliao Wang
Toxics 2024, 12(12), 928; https://doi.org/10.3390/toxics12120928 (registering DOI) - 21 Dec 2024
Abstract
Dichlorvos (2,2-dichlorovinyl dimethyl phosphate, DDVP) is a highly toxic organophosphorus insecticide, and its persistence in air, water, and soil poses potential threats to human health and ecosystems. Covalent triazine frameworks (CTFs), with their sufficient visible-light harvesting capacity, ameliorated charge separation, and exceptional redox [...] Read more.
Dichlorvos (2,2-dichlorovinyl dimethyl phosphate, DDVP) is a highly toxic organophosphorus insecticide, and its persistence in air, water, and soil poses potential threats to human health and ecosystems. Covalent triazine frameworks (CTFs), with their sufficient visible-light harvesting capacity, ameliorated charge separation, and exceptional redox ability, have emerged as promising candidates for the photocatalytic degradation of DDVP. Nevertheless, pure CTFs lack effective oxidative active sites, resulting in elevated reaction energy barriers during the photodegradation of DDVP. In this work, density functional theory (DFT) calculations were employed to investigate the impact of various oxygen-containing acid groups (-COOH, -HSO3, -H2PO3) on DDVP photodegradation performance. First, simulations of the structure and optical properties of modified CTFs reveal that oxygen-containing acid groups induce surface distortion and result in a redshift in the absorption edge. Subsequently, analysis of the density of states, frontier molecular orbitals, surface electrostatic potential, work function, and dipole moment demonstrates that oxygen-containing acid groups enhance CTF polarization, facilitate charge separation, and ameliorate their oxidative capability. Additionally, the free-energy diagram of DDVP degradation uncovers that oxygen-containing acid groups lower the energy barrier by elevating the adsorption and activation capability of DDVP. Notably, -H2PO3 presents optimal potential for the photodegradation of DDVP by unique electronic structure and activation capability. This work offers a valuable reference for the development of oxygen-containing acid CTF-based photocatalysts applied in degrading toxic organophosphate pesticides. Full article
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Figure 1

Figure 1
<p>Top and side perspective of crystal structures: (<b>a</b>,<b>e</b>) CTF, (<b>b</b>,<b>f</b>) CTF-COOH, (<b>c</b>,<b>g</b>) CTF-HSO<sub>3</sub>, and (<b>d</b>,<b>h</b>) CTF-H<sub>2</sub>PO<sub>3</sub>. Simulated (<b>i</b>) XRD pattern.</p>
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<p>(<b>a</b>) IR spectra, (<b>b</b>) Raman spectra, and (<b>c</b>) UV–Vis spectra of CTF, CTF-COOH, CTF-HSO<sub>3</sub>, and CTF-H<sub>2</sub>PO<sub>3</sub>. (<b>d</b>) Dipole moments on different components of CTF, CTF-COOH, CTF-HSO<sub>3</sub>, and CTF-H<sub>2</sub>PO<sub>3</sub>.</p>
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<p>Band structure of (<b>a</b>) CTF, (<b>b</b>) CTF-COOH, (<b>c</b>) CTF-HSO<sub>3</sub>, and (<b>d</b>) CTF-H<sub>2</sub>PO<sub>3</sub>. The density of states (DOS) of (<b>e</b>) CTF, (<b>f</b>) CTF-COOH, (<b>g</b>) CTF-HSO<sub>3</sub>, and (<b>h</b>) CTF-H<sub>2</sub>PO<sub>3</sub>.</p>
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<p>Electrostatic potentials curves of the (<b>a</b>) CTF, (<b>b</b>) CTF-COOH, (<b>c</b>) CTF-HSO<sub>3</sub>, and (<b>d</b>) CTF-H<sub>2</sub>PO<sub>3</sub>.</p>
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<p>Surface electrostatic potential of (<b>a</b>) CTF, (<b>b</b>) CTF-COOH, (<b>c</b>) CTF-HSO<sub>3</sub>, and (<b>d</b>) CTF-H<sub>2</sub>PO<sub>3</sub>.</p>
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<p>Interaction between DDVP and (<b>a</b>) CTF, (<b>b</b>) CTF-COOH, (<b>c</b>) CTF-HSO<sub>3</sub>, and (<b>d</b>) CTF-H<sub>2</sub>PO<sub>3</sub>. Charge density difference and charge transfer of (<b>e</b>,<b>i</b>) CTF, (<b>f</b>,<b>j</b>) CTF-COOH, (<b>g</b>,<b>k</b>) CTF-HSO<sub>3</sub>, (<b>h</b>,<b>l</b>) CTF-H<sub>2</sub>PO<sub>3</sub>.</p>
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<p>Free-energy diagrams for the photodegradation and reaction path of DDVP of (<b>a</b>) CTF, (<b>b</b>) CTF-COOH, (<b>c</b>) CTF-HSO<sub>3</sub>, and (<b>d</b>) CTF-H<sub>2</sub>PO<sub>3</sub>.</p>
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13 pages, 4333 KiB  
Article
Free-Space to SMF Integration and Green to C-Band Conversion Based on PPLN
by Takahiro Kodama, Kiichiro Kuwahara, Ayumu Kariya and Rikizo Ikuta
Sensors 2024, 24(24), 8162; https://doi.org/10.3390/s24248162 (registering DOI) - 21 Dec 2024
Abstract
In this study, we experimentally demonstrate a PPLN-based free-space to SMF (single-mode fiber) conversion system capable of efficient long-wavelength down-conversion from 518 nm, optimized for minimal loss in highly turbid water, to 1540 nm, which is ideal for low-loss transmission in standard SMF. [...] Read more.
In this study, we experimentally demonstrate a PPLN-based free-space to SMF (single-mode fiber) conversion system capable of efficient long-wavelength down-conversion from 518 nm, optimized for minimal loss in highly turbid water, to 1540 nm, which is ideal for low-loss transmission in standard SMF. Leveraging the nonlinear optical properties of periodically poled lithium niobate (PPLN), we achieve a wavelength conversion efficiency of 1.6% through difference frequency generation while maintaining a received optical signal-to-noise ratio of 10.4 dB. Our findings underscore the potential of integrating PPLN-based wavelength conversion with fiber optic networks, offering a viable solution for next-generation optical sensor systems that demand real-time, low-latency, and reliable data transmission. This work represents a significant advancement in developing robust and efficient optical sensor technologies, addressing the challenges associated with long-distance transmission and broad-linewidth light sources in optical remote sensing applications. Full article
(This article belongs to the Special Issue Atmospheric Optical Remote Sensing)
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Figure 1
<p>Overall structure of optical remote sensing system.</p>
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<p>FSFC configuration: (<b>a</b>) no-conversion type, (<b>b</b>) O/E/O conversion type, and (<b>c</b>) O/O conversion type.</p>
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<p>Power budget diagram of overall optical remote sensing system.</p>
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<p>Schematic configuration of the FSFC.</p>
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<p>Structure of (<b>a</b>) SHG and (<b>b</b>) DFG.</p>
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<p>The acceptance bandwidth by sinc<sup>2</sup>(Δ<span class="html-italic">kl</span>/2) for a single-frequency pump laser at 780 nm.</p>
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<p>Experimental setup.</p>
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<p>External view of FSFC.</p>
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<p>Characteristics of the change in the 780 nm pump power: (<b>a</b>) insertion loss in PPLN 2, (<b>b</b>) output power relationship, and (<b>c</b>) conversion efficiency <span class="html-italic">η</span> in Equation (8) (linear scale on the vertical axis).</p>
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<p>Characteristics of change in the 518 nm input power: (<b>a</b>) output power relationship and (<b>b</b>) conversion efficiency.</p>
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<p>(<b>a</b>) Received OSNR characteristics in relation to the output power of EDFA 1, (<b>b</b>) optical spectrum with a varying center wavelength of the green band’s OOK signal, and (<b>c</b>) optical spectrum with a varying output power of EDFA 1.</p>
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<p>Correlation between the transmitted and received signals.</p>
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<p>Measured power characteristics of SMF without and with wavelength conversion.</p>
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14 pages, 1936 KiB  
Article
High-Performance Photocatalytic Degradation—A ZnO Nanocomposite Co-Doped with Gd: A Systematic Study
by Aeshah Alasmari, Nadi Mlihan Alresheedi, Mohammed A. Alzahrani, Fahad M. Aldosari, Mostafa Ghasemi, Atef Ismail and Abdelaziz M. Aboraia
Catalysts 2024, 14(12), 946; https://doi.org/10.3390/catal14120946 (registering DOI) - 20 Dec 2024
Abstract
This research aims to analyze the improvement in the photocatalytic properties of ZnO nanoparticles by incorporating Gd. In order to understand the influence of incorporating Gd into the ZnO matrix, the photocatalytic activity of the material is compared at various Gd concentrations. Different [...] Read more.
This research aims to analyze the improvement in the photocatalytic properties of ZnO nanoparticles by incorporating Gd. In order to understand the influence of incorporating Gd into the ZnO matrix, the photocatalytic activity of the material is compared at various Gd concentrations. Different doping concentrations of Gd ranging from 0 to 0.075 are incorporated into ZnO and the synthesized ZnO-Gd nanocomposites are investigated using structural, morphological, and optical analyses using XRD, SEM, and UV-vis spectroscopy, respectively. The photocatalytic performance of the synthesized ZnO-Gd nanocomposites is determined via the degradation of organic contaminants under visible light. Regarding the latter, the results suggest that photocatalytic efficiency increases with increasing Gd doping levels up to an optimal doping concentration. The enhancement of the photocatalytic performance of Gd-doped ZnO is explained, along with the mechanism related to the availability of new pathways for charge carrier recombination. Among all of them, the 0.075 Gd-doped ZnO catalyst exhibits the highest photocatalytic activity which degrades 89% of MB dye after being irradiated with UV light for 120 min. However, pure ZnO degrades only 40% of MB dye within the same testing conditions. In closing, this work confirms the applicability of Gd-doped ZnO nanocomposites as photocatalysts in cleaning up the environment and in wastewater treatment. Full article
(This article belongs to the Special Issue Design and Application of Combined Catalysis)
21 pages, 2882 KiB  
Article
Research on the Modulation Characteristics of LiNbO3 Crystals Based on the Three-Dimensional Ray Tracing Method
by Houpeng Sun, Yingchun Li, Laixian Zhang, Huichao Guo, Chenglong Luan, Haijing Zheng, Rong Li and Youchen Fan
Crystals 2024, 14(12), 1101; https://doi.org/10.3390/cryst14121101 (registering DOI) - 20 Dec 2024
Abstract
To further study the electro-optical modulation characteristics of LiNbO3 crystals and analyze their modulation performance, a method for studying the modulation characteristics of LiNbO3 crystals, based on the three-dimensional ray tracing method, is introduced. With the help of the refractive index [...] Read more.
To further study the electro-optical modulation characteristics of LiNbO3 crystals and analyze their modulation performance, a method for studying the modulation characteristics of LiNbO3 crystals, based on the three-dimensional ray tracing method, is introduced. With the help of the refractive index ellipsoidal theory, the optical properties of LiNbO3 crystals under the influence of the Pockels effect are systematically investigated. The research results show that the optical properties of LiNbO3 crystals under the action of an external electric field can be divided into two cases: the crystal optical axis is parallel to the clear light direction, and the crystal optical axis is perpendicular to the clear light direction. Subsequently, starting from Maxwell’s equation and the matter equation, the analytical expressions of optical parameters such as refractive index, wave vector, light vector, optical path, and phase delay in electro-optical crystals are derived. Finally, the propagation law of LiNbO3 crystals when the light is incident in any direction, i.e., when the optical axis of the crystal is parallel to the clear direction and perpendicular to the clear direction, and the light intensity and field of view of the LiNbO3 crystal for electro-optical modulation are discussed. Full article
(This article belongs to the Section Inorganic Crystalline Materials)
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Figure 1

Figure 1
<p>The refractive index ellipsoid of a crystal.</p>
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<p>Cartesian coordinate system of LiNbO<sub>3</sub> crystals when the optical axis of the crystal is parallel to the direction of clear light.</p>
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<p>Cartesian coordinate system of LiNbO<sub>3</sub> crystals when the optical axis of the crystal is parallel to the direction of clear light.</p>
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<p>Birefringence at the interface between an isotropic medium and a LiNbO<sub>3</sub> crystal.</p>
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<p>Propagation of abnormal light in LiNiO<sub>3</sub> crystals.</p>
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<p>Refractive index ellipsoid.</p>
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<p>Crystal conoscopic interferogram when V = 0: (<b>a</b>) interference light intensity distribution; (<b>b</b>) influence of polarization direction on light intensity <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>sin</mi> </mrow> <mn>2</mn> </msup> <mo stretchy="false">[</mo> <mn>2</mn> <mi>ϕ</mi> <mo stretchy="false">(</mo> <mi>α</mi> <mo>,</mo> <mi>β</mi> <mo stretchy="false">)</mo> <mo stretchy="false">]</mo> </mrow> </semantics></math>; (<b>c</b>) influence of phase difference on light intensity <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>sin</mi> </mrow> <mn>2</mn> </msup> <mo stretchy="false">[</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>θ</mi> <mo stretchy="false">(</mo> <mi>α</mi> <mo>,</mo> <mi>β</mi> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </mfrac> </mstyle> <mo stretchy="false">]</mo> </mrow> </semantics></math>; (<b>d</b>–<b>f</b>) is a magnification of the field of view at the center of (<b>a</b>–<b>c</b>) of the figure.</p>
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<p>Crystal conoscopic interferogram when V = V<sub>π</sub>: (<b>a</b>) interference light intensity distribution; (<b>b</b>) influence of polarization direction on light intensity <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>sin</mi> </mrow> <mn>2</mn> </msup> <mo stretchy="false">[</mo> <mn>2</mn> <mi>ϕ</mi> <mo stretchy="false">(</mo> <mi>α</mi> <mo>,</mo> <mi>β</mi> <mo stretchy="false">)</mo> <mo stretchy="false">]</mo> </mrow> </semantics></math>; (<b>c</b>) influence of phase difference on light intensity <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>sin</mi> </mrow> <mn>2</mn> </msup> <mo stretchy="false">[</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>θ</mi> <mo stretchy="false">(</mo> <mi>α</mi> <mo>,</mo> <mi>β</mi> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </mfrac> </mstyle> <mo stretchy="false">]</mo> </mrow> </semantics></math>; (<b>d</b>–<b>f</b>) is a magnification of the field of view at the center of (<b>a</b>–<b>c</b>) of the figure.</p>
Full article ">
13 pages, 3995 KiB  
Article
Considering Grayscale Process and Material Properties for Robust Multilevel Diffractive Flat Optics
by Diogo E. Aguiam, Ana Dias, Manuel J. L. F. Rodrigues, Aamod Shanker, Filipe Camarneiro, Joana D. Santos, Pablo Valentim, Joao Cunha and Patrícia C. Sousa
Photonics 2024, 11(12), 1200; https://doi.org/10.3390/photonics11121200 (registering DOI) - 20 Dec 2024
Abstract
Arbitrarily designed flat optics directly manipulate the light wavefront to reproduce complex optical functions, enabling more compact optical assemblies and microsystem integration. Phase-shifting micro-optical devices rely on locally tailoring the optical path length of the wavefront through binary or multilevel surface relief micro- [...] Read more.
Arbitrarily designed flat optics directly manipulate the light wavefront to reproduce complex optical functions, enabling more compact optical assemblies and microsystem integration. Phase-shifting micro-optical devices rely on locally tailoring the optical path length of the wavefront through binary or multilevel surface relief micro- and nanostructures. Considering the resolution and tolerances of the production processes and the optical properties of the substrate and coating materials is crucial for designing robust multilevel diffractive flat optics. In this work, we evaluate the impact of the grayscale laser lithography resolution and geometry constraints on the efficiency of surface-relief diffractive lenses, and we analyze the process parameter space that limit lens performance. We introduce a spectral bandwidth metric to help evaluate the broad-spectrum performance of different materials. We simulate and experimentally observe that the diffractive focusing is dominated by the periodic wavelength-dependent phase discontinuities arising in the profile transitions of multilevel diffractive lenses. Full article
(This article belongs to the Special Issue Recent Advances in Diffractive Optics)
9 pages, 582 KiB  
Article
Towards Green Dentistry: Evaluating the Potential of 4D Printing for Sustainable Orthodontic Aligners with a Reduced Carbon Footprint
by Elena Palmieri, Luca Montaina, Denise Bellisario, Ivano Lucarini, Francesco Maita, Martina Ielmini, Maria Elena Cataldi, Loredana Cerroni, Roberta Condò and Luca Maiolo
Polymers 2024, 16(24), 3566; https://doi.org/10.3390/polym16243566 - 20 Dec 2024
Abstract
Clear aligners have transformed orthodontic care by providing an aesthetic, removable alternative to traditional braces. However, their significant environmental footprint, contributing to approximately 15,000 tons of plastic waste annually, poses a critical challenge. To address this issue, advancements in 4D printing have introduced [...] Read more.
Clear aligners have transformed orthodontic care by providing an aesthetic, removable alternative to traditional braces. However, their significant environmental footprint, contributing to approximately 15,000 tons of plastic waste annually, poses a critical challenge. To address this issue, advancements in 4D printing have introduced “smart” aligners with shape memory properties, enabling reshaping and reducing the number of aligners required per treatment. This study focuses on ClearX aligners, an innovative 4D-printed solution aimed at extending usage duration and minimizing environmental impact. Using a comprehensive suite of tests, including morphological, optical, and mechanical evaluations conducted via scanning electron microscopy, UV-Vis spectroscopy, infrared spectroscopy, and bending and strain assessments, we evaluated the optical and mechanical stability of the ClearX material before and after thermal activation. Our results demonstrate that ClearX aligners retain their structural and functional properties after reshaping. Temporary changes in transparency, observed only under prolonged treatment durations exceeding manufacturer recommendations, are fully reversible within 12 h and do not compromise the aligner’s usability. These findings support the potential of ClearX aligners to effectively combine patient-centered, high-quality orthodontic care with sustainable practices. Full article
(This article belongs to the Section Smart and Functional Polymers)
22 pages, 4263 KiB  
Article
Investigation of the Structure–Property Relation of Anthraquinone Dye Molecules with High Dichroism in Guest–Host Liquid Crystal Systems via Computational Methods
by Ruisi Chen, Xintao Guo, Bo Zhang, Ying Liu and Jun Liu
Materials 2024, 17(24), 6240; https://doi.org/10.3390/ma17246240 - 20 Dec 2024
Abstract
By combining molecular dynamics (MD) simulations and density functional theory (DFT), the influence of dye structure on the optical modulation properties of negative-mode guest–host liquid crystal (GHLC) systems was systematically investigated. Firstly, the reliability of the simulation method was validated by comparing the [...] Read more.
By combining molecular dynamics (MD) simulations and density functional theory (DFT), the influence of dye structure on the optical modulation properties of negative-mode guest–host liquid crystal (GHLC) systems was systematically investigated. Firstly, the reliability of the simulation method was validated by comparing the performance parameters of the GHLC system obtained from simulations with those from experimental results. Subsequently, a series of guest dye molecules, along with their mixtures with negative dielectric anisotropy mesogens, were designed and analyzed. This exploration focused on how variations in dye terminal chain lengths, substitution positions, and substituent group properties affect dye molecular geometry, dye alignment within the host, transition dipole orientation, absorption spectra, and electronic excitation properties. Our findings suggest that dye molecules with a flexible terminal chain substitution of five carbon atoms, positioned at the 2 and 6 locations on the anthraquinone core, exhibit higher order parameters, favorable for enhancing dichroic performance. Moreover, introducing different α-substituents further influences the dye orientation and electronic behavior within the host. These results highlight that structural modifications of anthraquinone-based dyes allow for the design of high-dichroic-ratio materials with customized absorption properties. Overall, our results provide a beneficial understanding of the structure–property relation in GHLC systems, offering valuable guidance for designing high-performance dye molecules and advanced optoelectronic materials in future research. Full article
9 pages, 1257 KiB  
Article
Cyclopentadienyl Amidinate Ligand Directing Effects in the Enantioselective Living Coordinative Chain Transfer Polymerization of 1,5-Hexadiene
by Cole M. Burrows, Peter Y. Zavalij and Lawrence R. Sita
Catalysts 2024, 14(12), 944; https://doi.org/10.3390/catal14120944 - 20 Dec 2024
Abstract
The new chiral and configurationally stable cyclopentadienyl amidinate (CPAM) hafnium complexes, (RC, RHf)-2 and (SC, SHf)-3, have been obtained in enantio- and diastereomerically pure form. Upon activation with the borate [...] Read more.
The new chiral and configurationally stable cyclopentadienyl amidinate (CPAM) hafnium complexes, (RC, RHf)-2 and (SC, SHf)-3, have been obtained in enantio- and diastereomerically pure form. Upon activation with the borate co-initiator, [PhNHMe2][B(C6F5)4] (B1), 2 and 3 can serve as pre-initiators for the enantioselective living coordinative polymerization (LCP) and living coordinative chain transfer polymerization (LCCTP) of 1,5-hexadiene to provide optically active poly (methylene-1,3-cyclopentane) (PMCP) and end-group-functionalized PMCP (x-PMCP) in scalable quantities, respectively. 13C NMR stereochemical microstructural analyses reveal the role of ligand directing effects for the two-step propagation mechanism of 1,2-migratory insertion/ring-closing cyclization and structure/property relationships for these new PMCP and x-PMCP materials. Full article
(This article belongs to the Special Issue State-of-the-Art Polymerization Catalysis)
39 pages, 22737 KiB  
Article
Comparative Research in the Field of the Parametric Effect of Lubricant Cavitation Initiation and Development on Friction and Wear in Piston Ring and Cylinder Liner Assemblies
by Polychronis Dellis
Lubricants 2024, 12(12), 460; https://doi.org/10.3390/lubricants12120460 - 20 Dec 2024
Abstract
This research follows closely previous findings in flow characteristics and phenomena that take place in the piston ring and cylinder liner interface during motoring and firing engine operation, and also compares results between different optical engine set-ups. Cavitation visualisation in a simulating lubrication [...] Read more.
This research follows closely previous findings in flow characteristics and phenomena that take place in the piston ring and cylinder liner interface during motoring and firing engine operation, and also compares results between different optical engine set-ups. Cavitation visualisation in a simulating lubrication single-ring test rig and oil transport and cavitation visualisation in custom made cylinder assemblies of optical engines are the tools used to quantify the transport process under the piston ring and cylinder liner. Simplification of the interface is an essential technique that enhances the researcher’s confidence in results interpretation. Engine complexity and severe oil starvation are impeding the analysis of the experimental results. Visualisation experiments constitute an effective way to test various lubricant types and assess their overall performance characteristics, including their properties and cavitation behaviour. The repeatability of the visualisation method establishes the parametric study effects and offers valuable experimental results. As a further step towards the lubricant composition effect, a link between the lubricant formulation and the operating conditions could be established as the oil performance is assessed with a view to its transport behaviour. Image processing is used to quantify the impact of cavitation on piston ring lubrication in conjunction with varied operating and lubricant parameters. The characteristics of the lubricant and the working environment have an impact on these types of cavities. Viscosity, cavitation, oil film thickness (OFT), lubricant shear-thinning characteristics and friction are all linked. Full article
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Figure 1

Figure 1
<p>Simulating single-ring test rig: (<b>a</b>) schematic; (<b>b</b>) the capacitance sensor used for MOFT measurements; (<b>c</b>) the capacitance, friction sensors, piston specimen and the oil jets that flood the piston ring and liner interface with lubricant; (<b>d</b>) schematic of the miniature pressure transducer as fitted on the liner specimen.</p>
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<p>Modified Kubota engine block with fitted window section [<a href="#B13-lubricants-12-00460" class="html-bibr">13</a>].</p>
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<p>PSA spark ignition engine: (<b>a</b>) side view; (<b>b</b>) top view [<a href="#B13-lubricants-12-00460" class="html-bibr">13</a>].</p>
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<p>Toyota engine—window layout [<a href="#B17-lubricants-12-00460" class="html-bibr">17</a>].</p>
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<p>Lubricant transport mechanisms in the piston assembly of a fired automotive engine [<a href="#B35-lubricants-12-00460" class="html-bibr">35</a>].</p>
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<p>Lister–Petter engine modifications, experimental set-up and drawings: (<b>a</b>) Lister–Petter engine with modified block on the dynamometer; (<b>b</b>) liner drawing details; (<b>c</b>) liner and block 3-D drawings; (<b>d</b>) Lister–Petter piston; (<b>e</b>) window drawing details; (<b>f</b>) modified engine drawing details; (<b>g</b>) photo of fitted windows; (<b>h</b>) engine visualisation experimental set-up; (<b>i</b>) camera visualisation set-up; (<b>j</b>) viewing windows, optical fibre probe and pressure transducer fittings in the modified liner [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>,<a href="#B25-lubricants-12-00460" class="html-bibr">25</a>].</p>
Full article ">Figure 6 Cont.
<p>Lister–Petter engine modifications, experimental set-up and drawings: (<b>a</b>) Lister–Petter engine with modified block on the dynamometer; (<b>b</b>) liner drawing details; (<b>c</b>) liner and block 3-D drawings; (<b>d</b>) Lister–Petter piston; (<b>e</b>) window drawing details; (<b>f</b>) modified engine drawing details; (<b>g</b>) photo of fitted windows; (<b>h</b>) engine visualisation experimental set-up; (<b>i</b>) camera visualisation set-up; (<b>j</b>) viewing windows, optical fibre probe and pressure transducer fittings in the modified liner [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>,<a href="#B25-lubricants-12-00460" class="html-bibr">25</a>].</p>
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<p>Piston ring pack details for Lister–Petter PHW1 single-cylinder engine [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>The Ricardo HYDRA optical engine: (<b>a</b>) new cylinder design and cooling details; (<b>b</b>) cut-out; (<b>c</b>) custom made quartz visualisation windows; (<b>d</b>) engine side view [<a href="#B9-lubricants-12-00460" class="html-bibr">9</a>].</p>
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<p>Upstroke cavitation images from (<b>a</b>–<b>l</b>) 15° crank angle (CA) to 28.2° CA [<a href="#B23-lubricants-12-00460" class="html-bibr">23</a>].</p>
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<p>Downstroke cavitation images from 0° crank angle (CA) to 360° CA [<a href="#B23-lubricants-12-00460" class="html-bibr">23</a>].</p>
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<p>Imaging at different CAs for the simulating test rig with the respective oil film pressure readings and different speed tests at 1159 N/m load [<a href="#B4-lubricants-12-00460" class="html-bibr">4</a>,<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Imaging at different CAs for the simulating test rig with the respective oil film pressure readings and different load tests at 400 rpm [<a href="#B4-lubricants-12-00460" class="html-bibr">4</a>,<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>(<b>a</b>) Vaporous oil film pressure difference between upstroke and downstroke; (<b>b</b>) ring profile as measured by Talysurf surface profilometry [<a href="#B4-lubricants-12-00460" class="html-bibr">4</a>].</p>
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<p>Peak oil film pressure signals: (<b>a</b>) offset at different speeds; (<b>b</b>) different cavitation areas at different speeds; (<b>c</b>) cavitation reformation at different loads [<a href="#B27-lubricants-12-00460" class="html-bibr">27</a>].</p>
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<p>Peak oil film pressure signals: (<b>a</b>) offset at different speeds; (<b>b</b>) different cavitation areas at different speeds; (<b>c</b>) cavitation reformation at different loads [<a href="#B27-lubricants-12-00460" class="html-bibr">27</a>].</p>
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<p>Effect of varying speed and load on (<b>a</b>) cavitation initiation points, different CAs; (<b>b</b>) number of string cavities at mid-stroke [<a href="#B7-lubricants-12-00460" class="html-bibr">7</a>].</p>
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<p>Possible cavitation stages for different test cases and location of fibre probe as it travels on top of the piston ring specimen and the cavities: (<b>a</b>) over a lubricant striation at cycle No 1 at 90° CA; (<b>b</b>) over a cavity at cycle No 2 at 90° CA; (<b>c</b>) over a mixed lubricant string cavity region at cycle No 3 at 90° CA [<a href="#B7-lubricants-12-00460" class="html-bibr">7</a>].</p>
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<p>The effect of different lubricants’ properties on friction force peaks at 300 r/min, 971 N/m load, 70 °C at TDC [<a href="#B26-lubricants-12-00460" class="html-bibr">26</a>].</p>
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<p>Focus on BDC MOFT measurements and squeeze film shift: (<b>a</b>) for different temperatures, oil 6E, 400 r/min and 1159 N/m load; (<b>b</b>) for different lubricants at 600 r/min, 1159 N/m load and high temperature of 70 °C [<a href="#B26-lubricants-12-00460" class="html-bibr">26</a>].</p>
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<p>Images taken from the top window at various crank angles. Forms of string cavities are strongly supported by the findings. Camera is fitted 11.17cm from TDC: (<b>a</b>) 576° CA exhaust stroke, cycle A; (<b>b</b>) 576° CA exhaust stroke, cycle B; (<b>c</b>) 576° CA exhaust stroke, cycle C; (<b>d</b>) 576° CA exhaust stroke, cycle D; (<b>e</b>) 576° CA exhaust stroke, cycle E [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Image taken from the top window at 608.40° CA, exhaust stroke, camera fitted 9.17 cm from top edge, showing (<b>a</b>) oil starvation and surface change on the piston ring; (<b>b</b>) oil spouts extending the second piston land [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Image of 475.20° CA expansion stroke, camera at 9.17 cm from top edge, string cavities’ formation on top compression ring [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Images of 615.24° CA exhaust stroke, camera at 9.17 cm from top edge, second compression ring at two different engine cycles: (<b>a</b>) cycle A; (<b>b</b>) cycle B [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Top window anti-thrust side at 255.24° CA compression stroke, camera at 8.67 cm from top edge: (<b>a</b>) irregular string-shaped cavities, cycle A; (<b>b</b>) appearance of oil droplets on piston ring bottom side clearance, cycle B; (<b>c</b>) more irregular cavitation shapes, cycle C; and (<b>d</b>) another irregular cavity shape, cycle D [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Top window anti-thrust side: (<b>a</b>) 218.34° CA compression stroke, camera at 11.67 cm from top edge—second compression ring; (<b>b</b>) 218.34° CA compression stroke, camera at 8.67 cm from top edge—top compression ring [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Images of 124.20° CA induction stroke, camera at 16.07 cm from top edge; (<b>a</b>–<b>c</b>) bubbles on the side clearance of the piston ring; (<b>d</b>) shapes resembling string cavity [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Oil mist on the piston skirt, using the highest magnification lens: (<b>a</b>) 18° CA induction stroke, camera at 9.07 cm from top edge; (<b>b</b>) 48.60° CA induction stroke, camera at 9.07 cm from top edge; (<b>c</b>) 142.20° CA induction stroke, camera at 16.07 cm from top edge [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Schematic of the possible cavitation stages on the Lister–Petter engine: (<b>A</b>) fern-shaped cavities; (<b>B</b>) irregular fern growth; (<b>C</b>) string cavities [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Window–liner profile measurements, Lister liner anti-thrust side: (<b>a</b>) upper window, upper side (TDC); (<b>b</b>) upper side of lower window and liner limit; (<b>c</b>) lower side of upper window; and (<b>d</b>) lower side of lower window (BDC) [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Window–liner profile measurements, Lister liner anti-thrust side: (<b>a</b>) upper window, upper side (TDC); (<b>b</b>) upper side of lower window and liner limit; (<b>c</b>) lower side of upper window; and (<b>d</b>) lower side of lower window (BDC) [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Cavitation string measurements, length and width as derived from imaging: (<b>a</b>) single-ring simulating test rig and (<b>b</b>) single-cylinder motored Lister–Petter engine [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>]. Orange measurements are the piston ring width and compression ring groove width, blue measurements are the strings’ length and green measurements the strings’ width.</p>
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<p>Oil mist appearance on the surface of the top compression ring: (<b>a</b>) 44.28° CA, induction stroke 3.67 cm from top (no sign); (<b>b</b>) 403.92° CA, expansion stroke 3.67 cm from top edge; (<b>c</b>) 403.92° CA, expansion stroke 3.67 cm from top edge; and (<b>d</b>) 403.92° CA, expansion stroke 3.67 cm from top edge [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>].</p>
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<p>Image of 254.88° CA compression stroke camera at 8.67 cm from top edge.</p>
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<p>Image of 255.24° CA compression stroke, camera at 8.67 cm from top edge, cycle A.</p>
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<p>Image of 255.24° CA compression stroke, camera at 8.67 cm from top edge, cycle B.</p>
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<p>Image of 255.24° CA compression stroke, camera at 8.67 cm from top edge, cycle C.</p>
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<p>Cavities on compression ring upstroke: (<b>a</b>) at 30 °C and (<b>b</b>) at 40 °C, 800 rpm [<a href="#B9-lubricants-12-00460" class="html-bibr">9</a>]. Red highlighted area shows the cavitation area that covers the piston-ring and is calculated by the algorithm. Blue arrow shows upstroke piston movement.</p>
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<p>Cavitation images on top compression ring of the HYDRA engine motored tests during compression stroke, upstroke at 70 °C, at different speeds; (<b>a</b>) 208 r/min, (<b>b</b>) 800 r/min, (<b>c</b>) 1000 r/min; (<b>d</b>) 2000 r/min [<a href="#B9-lubricants-12-00460" class="html-bibr">9</a>]. Red highlighted area shows the cavitation area that covers the piston-ring and is calculated by the algorithm.</p>
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<p>High-pressure gasses act as a medium of the lubricant transport through the ring gaps towards the engine sump during motored tests: (<b>a</b>) 1000 rpm, 70 °C, 6° CA after TDC; (<b>b</b>) 1000 rpm, 70 °C, 6° CA after TDC; (<b>c</b>) 1000 rpm, 70 °C, 12° CA after TDC, higher magnification [<a href="#B8-lubricants-12-00460" class="html-bibr">8</a>]. Blue arrow shows downstroke piston movement and dotted red arrows show lubricant transport pathways towards the engine sump.</p>
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<p>Oil pumping at the second land [<a href="#B5-lubricants-12-00460" class="html-bibr">5</a>]. Black arrows show lubricant pumping process from ring side clearances in the top image as piston moves upstroke and in the bottom image as piston moves downstroke. The orange arrow shows transition from upstroke to downstroke.</p>
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11 pages, 4314 KiB  
Article
Microwave-Assisted Extraction of Cellulose from Aloe Vera Plant Residue and Preparation of Cellulose Nanocrystal–Poly(vinyl alcohol) Hydrogels
by Eleni Triantafyllou, Andreas Karydis-Messinis, Dimitrios Moschovas, Christina Kyriakaki, Konstantinos C. Vasilopoulos, Aris E. Giannakas, Michael A. Karakassides, Apostolos Avgeropoulos, Nikolaos E. Zafeiropoulos and Constantinos E. Salmas
Molecules 2024, 29(24), 6012; https://doi.org/10.3390/molecules29246012 - 20 Dec 2024
Abstract
Biomass valorization and bio-based material development are of major research interest following the spirit of the circular economy. Aloe vera cultivation is a widespread agricultural activity oriented toward supplement production because of its well-known antioxidant and antimicrobial properties. Aloe vera juice production also [...] Read more.
Biomass valorization and bio-based material development are of major research interest following the spirit of the circular economy. Aloe vera cultivation is a widespread agricultural activity oriented toward supplement production because of its well-known antioxidant and antimicrobial properties. Aloe vera juice production also produces a large amount of biomass byproducts that are usually landfilled. On the other hand, cellulose nanocrystals are widely used in several applications, such as biomaterials, bio-compatible polymers, nanocomposites, food packaging, medicines, cosmetics, and sensors, due to their unique physical, mechanical, optical, electrical, and healing properties as well as their compatibility with biological tissues. This study introduces a novel approach combining the microwave-assisted extraction (MAE) of cellulose from this residue with the subsequent isolation of cellulose nanocrystals (CNCs). The MAE process, which exhibits a rapid heating and penetrating ability, was optimized to maximize the cellulose yield under various conditions (microwave power, solvent ratio, and time). Analysis using FTIR, XRD, SEM, and DMA indicated that isolated pure cellulose nanocrystals and a stable PVA–CNC porous hydrogel network were produced. The PVA–CNC hydrogel was synthesized to enable the formation of a semi-crystalline network that imparts the material with enhanced mechanical properties. Both final products of this study could potentially be used for various applications. Full article
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<p>FTIR spectra of (<b>a</b>) pure aloe vera leaves and extracted cellulose and (<b>b</b>) pure PVA powder and (<b>c</b>) CNC–PVA hydrogel.</p>
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<p>XRD diffractograms of (<b>a</b>) pure aloe vera leaves and extracted cellulose, (<b>b</b>) CNCs, and (<b>c</b>) the CNC–PVA hydrogel.</p>
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<p>SEM images of (<b>a</b>) pure aloe vera leaves, (<b>b</b>) extracted cellulose, and (<b>c</b>) isolated CNCs.</p>
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<p>SEM images of the CNC–PVA hydrogel, (<b>a</b>) sponge morphology and (<b>b</b>) interconnected porous system.</p>
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<p>Dynamic mechanical analysis of the CNC–PVA hydrogel, (<b>a</b>) Storage and Loss Modulus and (<b>b</b>) Tan delta are plotted as function of Frequency.</p>
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<p>Schematic illustration of cellulose extraction.</p>
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<p>Schematic illustration of cellulose nanocrystal isolation.</p>
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<p>Schematic illustration of CNC–PVA hydrogel preparation.</p>
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11 pages, 2610 KiB  
Article
Controllable Synthesis of Three-Dimensional Chiral Au Nanoflowers Induced by Cysteine with Excellent Biocompatible Properties
by Shengmiao Liu, Jianhao Zhang and Wenjing Yan
Nanomaterials 2024, 14(24), 2040; https://doi.org/10.3390/nano14242040 - 19 Dec 2024
Abstract
Chiral molecules are ubiquitous in nature and biological systems, where the unique optical and physical properties of chiral nanoparticles are closely linked to their shapes. Synthesizing chiral plasmonic nanomaterials with precise structures and tunable sizes is essential for exploring their applications. This study [...] Read more.
Chiral molecules are ubiquitous in nature and biological systems, where the unique optical and physical properties of chiral nanoparticles are closely linked to their shapes. Synthesizing chiral plasmonic nanomaterials with precise structures and tunable sizes is essential for exploring their applications. This study presents a method for growing three-dimensional chiral gold nanoflowers (Au NFs) derived from trisoctahedral (TOH) nanocrystals using D-cysteine and L-cysteine as chiral inducers. By employing a two-step seed-mediated growth approach, stable chiral Au nanoparticles with customizable sizes, shapes, and optical properties were produced by adjusting the Au nanosphere (Au NP) seed concentration and cysteine dosage. These nanoparticles exhibited optical activity in both the visible and near-infrared regions, with a maximum anisotropy factor (g-factor) of 0.024. Furthermore, the PEG-modified chiral Au NFs demonstrated excellent biocompatibility. This approach provides a precise method for geometrically controlling the design of three-dimensional chiral nanomaterials, holding great potential for biomedical applications. Full article
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<p>Characterization of the Au NP seeds. (<b>a</b>,<b>b</b>) Representative TEM images; (<b>c</b>) UV–Vis spectra, and (<b>d</b>) statistical analysis of particle size of Au NP seeds.</p>
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<p>TEM images and particle size distribution of Au TOHs synthesized with Au NP seeds at various concentrations.</p>
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<p>UV–Vis spectra of Au TOHs synthesized with Au NP seeds at different concentrations.</p>
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<p>SEM images of chiral Au NFs synthesized with different concentrations of Au NP seeds and corresponding optical properties. (<b>a</b>,<b>d</b>) CD spectra, (<b>b</b>,<b>e</b>) <span class="html-italic">g</span>-factor spectra, (<b>c</b>,<b>f</b>) UV–Vis spectra, and (<b>g</b>) SEM images of chiral Au NFs (the amount of Cys was 30 μL). Scale bars: 100 nm.</p>
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<p>SEM images of chiral Au NFs synthesized with different volumes of Cys and corresponding optical properties. (<b>a</b>,<b>d</b>) CD spectra, (<b>b</b>,<b>e</b>) <span class="html-italic">g</span>-factor spectra, (<b>c</b>,<b>f</b>) UV–Vis spectra, and (<b>g</b>) SEM images of chiral Au NFs (the concentration of Au NP seeds was 22.8 μg/mL). Scale bars: 100 nm.</p>
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<p>Cytotoxicity analysis of chiral Au NFs. (<b>a</b>) Zeta potential and (<b>b</b>) UV–Vis spectra of D-Au NFs before and after modification with PEG. (<b>c</b>) Cell viability of Hela cells after treatment by PEG-D-Au NFs and PEG-L-Au NFs. (<b>d</b>) The fluorescent images of Hela cells after being cocultured with chiral Au NFs at different concentrations, with F-actin stained with FITC (green) and nuclei stained with DAPI (blue). Scale bars: 20 μm.</p>
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16 pages, 5905 KiB  
Article
Corrosion Behavior of Ti and Ti6Al4V Alloy in Brackish Water, Seawater, and Seawater Bittern
by Ladislav Vrsalović, Senka Gudić, Antonia Talijančić, Jelena Jakić, Jure Krolo and Iman Danaee
Corros. Mater. Degrad. 2024, 5(4), 641-656; https://doi.org/10.3390/cmd5040031 - 19 Dec 2024
Abstract
Ti and Ti6Al4V alloy are extensively utilized in structural parts in engineering applications and the production of medical implants due to their excellent mechanical properties, lightweight, and high corrosion resistance. This study comprehensively evaluates their corrosion behavior in three challenging aquatic environments: brackish [...] Read more.
Ti and Ti6Al4V alloy are extensively utilized in structural parts in engineering applications and the production of medical implants due to their excellent mechanical properties, lightweight, and high corrosion resistance. This study comprehensively evaluates their corrosion behavior in three challenging aquatic environments: brackish water, seawater, and seawater bittern. Utilizing open circuit potential (EOC) measurements with polarization techniques (linear and potentiodynamic) and electrochemical impedance spectroscopy (EIS) measurements, the research highlights distinct environmental influences on corrosion performance. Notably, Ti and Ti6Al4V alloy demonstrated exceptional stability with the highest polarization resistance and lowest corrosion current in brackish water, while seawater bittern presented the most demanding condition for Ti6Al4V. Additionally, the analysis of the electrode surfaces after polarization measurements using optical microscopy, optical profilometry, and SEM/EDS tests revealed minor damage, indicating the high corrosion resistance of these materials. This study advances the understanding of Ti and Ti6Al4V alloy performance in diverse environments and offers valuable insights for optimizing their use in harsh aquatic conditions, particularly for applications requiring durability and longevity. Full article
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<p>Open circuit potential measurements in brackish water, seawater, and seawater bittern for Ti (<b>a</b>) and Ti6Al4V alloy (<b>b</b>).</p>
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<p>Linear parts of <span class="html-italic">i</span>-<span class="html-italic">E</span> curves for Ti (<b>a</b>) and Ti6Al4V alloy (<b>b</b>) in brackish water, seawater, and seawater bittern.</p>
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<p>Potentiodynamic potential measurements in brackish water, seawater, and seawater bittern for Ti (<b>a</b>) and Ti6Al4V alloy (<b>b</b>).</p>
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<p>Nyquist (<b>a</b>,<b>b</b>) and Bode (<b>c</b>,<b>d</b>) plots recorded on cp-Ti and Ti-6Al-4V alloy in different solutions.</p>
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<p>The EC model used to fit the EIS data.</p>
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<p>Optical microscope images of surface of Ti after potentiodynamic polarization measurements in (<b>a</b>) brackish water, (<b>b</b>) seawater, and (<b>c</b>) seawater bittern; and surfaces of Ti6Al4V after measurements in (<b>d</b>) brackish water, (<b>e</b>) seawater, and (<b>f</b>) seawater bittern.</p>
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<p>SEM images of surface of Ti after potentiodynamic polarization measurements in (<b>a</b>) brackish water, (<b>b</b>) seawater, and (<b>c</b>) seawater bittern; and surfaces of Ti6Al4V after measurements in (<b>d</b>) brackish water, (<b>e</b>) seawater, and (<b>f</b>) seawater bittern.</p>
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<p>SEM images of surface of Ti after potentiodynamic polarization measurements in (<b>a</b>) brackish water, (<b>b</b>) seawater, and (<b>c</b>) seawater bittern; and surfaces of Ti6Al4V after measurements in (<b>d</b>) brackish water, (<b>e</b>) seawater, and (<b>f</b>) seawater bittern.</p>
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<p>(<b>a</b>) SEM image of surface of Ti after potentiodynamic polarization measurements in seawater and (<b>b</b>) EDS point analysis in Spectrum 4.</p>
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<p>(<b>a</b>) SEM image of surface of Ti6Al4V after potentiodynamic polarization measurements in seawater bittern and (<b>b</b>) EDS point analysis in Spectrum 1.</p>
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<p>Three-dimensional optical profilometry images of surface of = Ti after potentiodynamic polarization measurements in (<b>a</b>) brackish water, (<b>b</b>) seawater, and (<b>c</b>) seawater bittern; and surfaces of Ti6Al4V after measurements in (<b>d</b>) brackish water, (<b>e</b>) seawater, and (<b>f</b>) seawater bittern.</p>
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<p>Three-dimensional appearance of corrosion pits and line profile measurement for Ti6Al4V electrode after potentiodynamic polarization measurements in seawater bittern.</p>
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14 pages, 4402 KiB  
Article
Effects of Phenoxazine Chromophore on Optical, Electrochemical and Electrochromic Behaviors of Carbazole–Thiophene Derivatives
by Bin Hu, Haizeng Song, Xinlei Zhang, Yuan He, Jingshun Ren and Jingbin Huang
Polymers 2024, 16(24), 3546; https://doi.org/10.3390/polym16243546 - 19 Dec 2024
Abstract
Phenoxazine, as an organic-small-molecule chromophore, has attracted much attention for its potential electrochromic applications recently. To develop appealing materials, phenoxazine chromophores were introduced at the N-position of carbazole–thiophene pigment, yielding two novel monomers (DTCP and DDCP), whose chemical structures were characterized by NMR, [...] Read more.
Phenoxazine, as an organic-small-molecule chromophore, has attracted much attention for its potential electrochromic applications recently. To develop appealing materials, phenoxazine chromophores were introduced at the N-position of carbazole–thiophene pigment, yielding two novel monomers (DTCP and DDCP), whose chemical structures were characterized by NMR, HRMS and FTIR. The results of the optical property study indicate that little influence could be observed in the presence of the phenoxazine chromophore. Corresponding polymer films on the surface of an ITO/glass electrode were obtained through electropolymerization. The electrochemical features displayed were various due to the introduction of the phenoxazine group. The spectroelectrochemical results demonstrate that the color of the polymer films could be changed. Compared with the PDDC films, the PDDCP films exhibited three different colors (tangerine, green and purple colors) in different redox states, which could be attributed to the synergistic effect between the carbazole–thiophene conjugate chain and the phenoxazine group. Moreover, fast switching time could be seen due to the presence of the phenoxazine chromophore. This study could provide a reference for obtaining high-performance electrochromic materials. Full article
(This article belongs to the Special Issue Active Polymeric Materials for Electrochemical Applications)
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<p>(<b>a</b>) The UV−vis absorption and (<b>b</b>) emission spectra of DTC, DDC, DTCP and DDCP in DCM solution; the FTIR spectra of (<b>c</b>) monomers and (<b>d</b>) their corresponding polymer films.</p>
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<p>Continuous CV electropolymerization curves of (<b>a</b>) 1 mM DTC, (<b>b</b>) 1 mM DTCP, (<b>c</b>) 1 mM DDC and (<b>d</b>) 1 mM DDCP in the 0.1 M TBAP/DCM solution at a scan rate of 100 mV/s (inset images: the first cycle of CV curves).</p>
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<p>CV curves of (<b>a</b>) PDTC, (<b>b</b>) PDTCP, (<b>c</b>) PDDC and (<b>d</b>) PDDCP films in monomer-free solution of 0.1 M TBAP/ACN at different scan rates from 25 to 150 mV/s with 25 mV increments (inset images: the linear relationship between anodic/cathodic current intensity and scan rate).</p>
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<p>The micromorphology images of the PDTC, PDTCP, PDDC and PDDCP films.</p>
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<p>Spectroelectrochemical spectra of (<b>a</b>) PDTC, (<b>b</b>) PDTCP, (<b>c</b>) PDDC and (<b>d</b>) PDDCP films under different applied potentials in 0.1 M TBAP/ACN solution (inset picture: images of polymer films under different applied potentials).</p>
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<p>The proposed electrochromic mechanisms of (<b>a</b>) PDTC and (<b>b</b>) PDTCP films in different oxidized states.</p>
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<p>(<b>a</b>) The relationship between transmittance and different wavelengths of the PDTCP films at 0.0 and 1.3 V. (<b>b</b>) The transmittance–time profiles of the PDTCP films monitored at different absorption maxima under applied potential between 0.0 V and 1.3 V with switching intervals of 10 s. (<b>c</b>) The calculated switching time of PDTCP at 544 nm. (<b>d</b>) The EIS spectra between Zre and ω<sup>−0.5</sup> at low frequencies for the PDTC, PDTCP, PDDC and PDDCP films in a monomer-free solution of 0.1 M TBAP/ACN.</p>
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<p>Synthesis routes of DTCP and DDCP.</p>
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32 pages, 3355 KiB  
Review
Advances in Natural-Product-Based Fluorescent Agents and Synthetic Analogues for Analytical and Biomedical Applications
by Soniya Joshi, Alexis Moody, Padamlal Budthapa, Anita Gurung, Rachana Gautam, Prabha Sanjel, Aakash Gupta, Surya P. Aryal, Niranjan Parajuli and Narayan Bhattarai
Bioengineering 2024, 11(12), 1292; https://doi.org/10.3390/bioengineering11121292 - 19 Dec 2024
Abstract
Fluorescence is a remarkable property exhibited by many chemical compounds and biomolecules. Fluorescence has revolutionized analytical and biomedical sciences due to its wide-ranging applications in analytical and diagnostic tools of biological and environmental importance. Fluorescent molecules are frequently employed in drug delivery, optical [...] Read more.
Fluorescence is a remarkable property exhibited by many chemical compounds and biomolecules. Fluorescence has revolutionized analytical and biomedical sciences due to its wide-ranging applications in analytical and diagnostic tools of biological and environmental importance. Fluorescent molecules are frequently employed in drug delivery, optical sensing, cellular imaging, and biomarker discovery. Cancer is a global challenge and fluorescence agents can function as diagnostic as well as monitoring tools, both during early tumor progression and treatment monitoring. Many fluorescent compounds can be found in their natural form, but recent developments in synthetic chemistry and molecular biology have allowed us to synthesize and tune fluorescent molecules that would not otherwise exist in nature. Naturally derived fluorescent compounds are generally more biocompatible and environmentally friendly. They can also be modified in cost-effective and target-specific ways with the help of synthetic tools. Understanding their unique chemical structures and photophysical properties is key to harnessing their full potential in biomedical and analytical research. As drug discovery efforts require the rigorous characterization of pharmacokinetics and pharmacodynamics, fluorescence-based detection accelerates the understanding of drug interactions via in vitro and in vivo assays. Herein, we provide a review of natural products and synthetic analogs that exhibit fluorescence properties and can be used as probes, detailing their photophysical properties. We have also provided some insights into the relationships between chemical structures and fluorescent properties. Finally, we have discussed the applications of fluorescent compounds in biomedical science, mainly in the study of tumor and cancer cells and analytical research, highlighting their pivotal role in advancing drug delivery, biomarkers, cell imaging, biosensing technologies, and as targeting ligands in the diagnosis of tumors. Full article
(This article belongs to the Special Issue Biomaterials and Technology for Tumor Engineering)
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Graphical abstract

Graphical abstract
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<p>Chemical structures of selected natural products and synthetic fluorescent compounds. Color represents the fluorescence of the respective structures.</p>
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<p>The structure–activity relationship of the fluorescent probes. (<b>A</b>) The effect of conjugation on the electronic excited state and its effect on fluorescence intensity—an increase in conjugation results in increasing fluorescence intensity. (<b>B</b>) Structures of different fluorescent compounds with their emission colors. (<b>C</b>) The effect of the electron-donating and electron-withdrawing groups on rhodamine’s intensity and quantum yield. * denotes the antibonding molecular orbital.</p>
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<p>Schematic representation of biomedical applications of fluorescent probes. These applications are mainly based on the phenomenon of fluorescence, where the emission of radiation from the singlet excited state to the singlet ground state produces fluorescence and this relates to different utilities in drug delivery systems, cell counting and cellular proteomics, wound healing, biosensors, and biomarker and cell imaging. S<sub>1</sub>: singlet excited state; S<sub>0</sub>: singlet ground state; GFP: green fluorescent protein.</p>
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<p>The working mechanism of fluorescent probes in drug delivery systems, drug analysis, and their function as sensors. Drugs attached with probes through cleavable linkage or non-cleavable linkage allow us to evaluate its delivery system properly, and its other function as a sensor helps us to analyze the metabolite pathway, enzyme activity, chromosomal analysis, and genetic mapping. The green color attached to the linker demonstrates the state before the drug is delivered to the target site, while the yellow color signifies the successful delivery of the drug to the desired place.</p>
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<p>Mode of action of fluorescent probes in biomarkers and cell imaging. Fluorescent probes undergo different mechanisms, such as ESIPT, FRET, PET, ICT, and protein labeling, to intensify the fluorescence properties, followed by real-time analysis of molecules, thereby aiding in cell and tissue imaging. ESIPT: excited-state, intramolecular, proton-transfer (ESIPT) emissions; FRET: fluorescence (or Förster) resonance energy transfer; PET: photoinduced electron transfer; ICT: intramolecular charge transfer. * denotes the excited state.</p>
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<p>Application of fluorescent compounds in wound healing. Fluorescent compounds allow the real-time visualization and analysis of wounds, leading to an understanding of the healing process.</p>
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<p>Schematic representation of the analytical applications of fluorescent probes. With the incorporation of fluorescent natural products into NPs, nanoclusters exhibit enhanced properties, increasing their utility in different fields, including water purification and environmental monitoring.</p>
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