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Keywords = indium tin oxide

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19 pages, 6309 KiB  
Article
Coupled Resonance Fiber-Optic SPR Sensor Based on TRIZ
by Cuilan Zhu, Haodi Zhai, Yonghao Wang, Xiangru Suo, Tianyu Zhu and Shuowei Jin
Photonics 2025, 12(3), 244; https://doi.org/10.3390/photonics12030244 - 9 Mar 2025
Viewed by 91
Abstract
This paper aims to enhance the sensitivity of fiber-optic surface plasmon resonance (SPR) sensors by innovatively applying TRIZ (Theory of Inventive Problem Solving). To identify the key challenges faced by current SPR sensors, methods such as functional analysis, causal analysis, and the Nine-Window [...] Read more.
This paper aims to enhance the sensitivity of fiber-optic surface plasmon resonance (SPR) sensors by innovatively applying TRIZ (Theory of Inventive Problem Solving). To identify the key challenges faced by current SPR sensors, methods such as functional analysis, causal analysis, and the Nine-Window method are employed. Utilizing TRIZ tools, including Technical Contradiction, Physical Contradiction, the Smart Little Man method, and object–field analysis, innovative solutions are proposed, involving transparent indium tin oxide (ITO) thin films, an asymmetric photonic crystal fiber structure with elliptical pores, and titanium dioxide (TiO2) thin films. Experimental results reveal a significant improvement in sensitivity, with an average of 9961.90 nm/RIU and a peak of 12,503.56 nm/RIU within the refractive index range of 1.33061 to 1.40008, representing a 456% increase compared to the original gold-film fiber-optic SPR sensor. These findings have potential applications in biosensing, environmental monitoring, and food safety. Full article
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<p>Schematic diagram of fiber-optic sensing system.</p>
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<p>A graphical representation of the functional analysis of the engineering system.</p>
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<p>Causal analysis diagram, blue represents the problem found, and red represents the root cause of the problem.</p>
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<p>Nine-Window analysis diagram.</p>
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<p>Photonic crystal fiber with eight air holes.</p>
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<p>In the initial state, the blue little man (mode field) is confined within the red little man’s air holes.</p>
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<p>An increase in the effective mode field area after changing the shape of the air holes.</p>
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<p>(<b>a</b>) A model of the photonic crystal fiber SPR sensor with an elliptical air hole structure. (<b>b</b>) Mode field variation in the photonic crystal fiber SPR sensor with an elliptical air hole structure.</p>
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<p>Object–field analysis.</p>
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<p>(<b>a</b>) Schematic diagram of titanium dioxide network structure. (<b>b</b>) Fiber-optic sensor model after addition of titanium dioxide. (<b>c</b>) Electric field distribution of sensor after addition of titanium dioxide.</p>
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<p>(<b>a</b>) Optical fiber sensor model diagram. (<b>b</b>) Optical fiber sensor structural parameters. (<b>c</b>) Optical fiber sensor mesh diagram.</p>
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<p>Sensor preparation process.</p>
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<p>Schematic diagram of refractive index testing experiment.</p>
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<p>(<b>a</b>) Fiber core loss curve for different test liquid concentrations obtained through simulation. (<b>b</b>) Polynomial fitting curve between different test liquid concentrations and wavelength obtained through simulation. (<b>c</b>) Refractive index curve for different test liquid concentrations obtained through experiments. (<b>d</b>) Linear fitting curve between different test liquid concentrations and simulated wavelength obtained through experiments.</p>
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<p>The wavelength shift in the SPR sensor induced by different solvents at the same concentration.</p>
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15 pages, 6315 KiB  
Article
Effect of Various Nanofillers on Piezoelectric Nanogenerator Performance of P(VDF-TrFE) Nanocomposite Thin Film
by Sangkwon Park and Hafiz Muhammad Abid Yaseen
Nanomaterials 2025, 15(5), 403; https://doi.org/10.3390/nano15050403 - 6 Mar 2025
Viewed by 238
Abstract
Flexible polymer-based piezoelectric nanogenerators (PENGs) have gained significant interest due to their ability to deliver clean and sustainable energy for self-powered electronics and wearable devices. Recently, the incorporation of fillers into the ferroelectric polymer matrix has been used to improve the relatively low [...] Read more.
Flexible polymer-based piezoelectric nanogenerators (PENGs) have gained significant interest due to their ability to deliver clean and sustainable energy for self-powered electronics and wearable devices. Recently, the incorporation of fillers into the ferroelectric polymer matrix has been used to improve the relatively low piezoelectric properties of polymer-based PENGs. In this study, we investigated the effect of various nanofillers such as titania (TiO2), zinc oxide (ZnO), reduced graphene oxide (rGO), and lead zirconate titanate (PZT) on the PENG performance of the nanocomposite thin films containing the nanofillers in poly(vinylidene fluoride-co-trifluoro ethylene) (P(VDF-TrFE)) matrix. The nanocomposite films were prepared by depositing molecularly thin films of P(VDF-TrFE) and nanofiller nanoparticles (NPs) spread at the air/water interface onto the indium tin oxide-coated polyethylene terephthalate (ITO-PET) substrate, and they were characterized by measuring their microstructures, crystallinity, β-phase contents, and piezoelectric coefficients (d33) using SEM, FT-IR, XRD, and quasi-static meter, respectively. Multiple PENGs incorporating various nanofillers within the polymer matrix were developed by assembling thin film-coated substrates into a sandwich-like structure. Their piezoelectric properties, such as open-circuit output voltage (VOC) and short-circuit current (ISC), were analyzed. As a result, the PENG containing 4 wt% PZT, which was named P-PZT-4, showed the best performance of VOC of 68.5 V with the d33 value of 78.2 pC/N and β-phase content of 97%. The order of the maximum VOC values for the PENGs of nanocomposite thin films containing various nanofillers was PZT (68.5 V) > rGO (64.0 V) > ZnO (50.9 V) > TiO2 (48.1 V). When the best optimum PENG was integrated into a simple circuit comprising rectifiers and a capacitor, it demonstrated an excellent two-dimensional power density of 20.6 μW/cm2 and an energy storage capacity of 531.4 μJ within 3 min. This piezoelectric performance of PENG with the optimized nanofiller type and content was found to be superior when it was compared with those in the literature. This PENG comprising nanocomposite thin film with optimized nanofiller type and content shows a potential application for a power source for low-powered electronics such as wearable devices. Full article
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<p>Illustration of preparation procedure of nanocomposite LS film and their PENG device.</p>
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<p>SEM micrographs of nanocomposite LS thin films of (<b>a</b>) P, (<b>b</b>) P-TiO<sub>2</sub>-4, (<b>c</b>) P-TiO<sub>2</sub>-40, (<b>d</b>) P-ZnO-2, (<b>e</b>) P-ZnO-20, (<b>f</b>) P-ZnO-40, (<b>g</b>) P-PZT-2, (<b>h</b>) P-PZT-20, and (<b>i</b>) P-PZT-40 with 50 μm scale bars.</p>
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<p>XRD patterns, FT-IR spectra, crystallinity, and β-phase content profiles as a function of nanofiller content for the nanocomposite thin films of (<b>a</b>–<b>c</b>) P-TiO<sub>2</sub>, (<b>d</b>–<b>f</b>) P-ZnO, (<b>g</b>–<b>i</b>) P-rGO, and (<b>j</b>–<b>l</b>) P-PZT series.</p>
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<p>Piezoelectric coefficient (<span class="html-italic">d</span><sub>33</sub>) values as a function of nanofiller content for the nanocomposite thin films of (<b>a</b>) P-TiO<sub>2</sub>, (<b>b</b>) P-ZnO, (<b>c</b>) P-rGO, and (<b>d</b>) P-PZT series.</p>
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<p><span class="html-italic">V<sub>OC</sub></span> signals of PENG devices and maximum peak-to-peak <span class="html-italic">V<sub>OC</sub></span> values as a function of nanofiller content for the nanocomposite thin films of (<b>a</b>,<b>b</b>) P-TiO<sub>2</sub>, (<b>c</b>,<b>d</b>) P-ZnO, (<b>e</b>,<b>f</b>) P-rGO, and (<b>g</b>,<b>h</b>) P-PZT series.</p>
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<p><span class="html-italic">V<sub>OC</sub></span> signals of PENG devices and maximum peak-to-peak <span class="html-italic">V<sub>OC</sub></span> values as a function of nanofiller content for the nanocomposite thin films of (<b>a</b>,<b>b</b>) P-TiO<sub>2</sub>, (<b>c</b>,<b>d</b>) P-ZnO, (<b>e</b>,<b>f</b>) P-rGO, and (<b>g</b>,<b>h</b>) P-PZT series.</p>
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<p>(<b>a</b>) The maximum <span class="html-italic">V<sub>OC</sub></span> values for different optimum PENGs containing different nanofillers (with the surface pressure of 5 mN/m), (<b>b</b>) <span class="html-italic">I<sub>SC</sub></span> signals for the PZT PENGs as a function of nanofiller content, and (<b>c</b>) stability of the optimized PZT-based PENG for 1000 s.</p>
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<p>(<b>a</b>) Potential profiles and (<b>b</b>) energy storage values for the optimal PENG of thin film containing 4 wt% PZT with different capacitors.</p>
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8 pages, 5504 KiB  
Proceeding Paper
Electrochromic Behavior of Manganese Oxides/Silver Thin Films from Electrochemical Deposition
by Yi Hu, Jiun-Shing Liu, Pin-Syuan Chen and Si-Ying Li
Eng. Proc. 2025, 89(1), 35; https://doi.org/10.3390/engproc2025089035 - 5 Mar 2025
Viewed by 60
Abstract
MnOx thin films with silver additives were electrochemically deposited on an Indium Tin Oxide (ITO) substrate with silver acetate and potassium permanganate aqueous solution. The addition of Ag enhanced electrochromic behavior during cyclic voltammetry (CV). The morphology of the thin films was [...] Read more.
MnOx thin films with silver additives were electrochemically deposited on an Indium Tin Oxide (ITO) substrate with silver acetate and potassium permanganate aqueous solution. The addition of Ag enhanced electrochromic behavior during cyclic voltammetry (CV). The morphology of the thin films was examined by using scanning electronic microscopy (SEM) and transmission electron microscopy (TEM). The chemical states of Mn and Ag ions on the surfaces of the thin films were examined using X-ray photoelectron spectroscopy (XPS). Spherical Ag2O and Ag nanoparticles were homogeneously dispersed on the thin films. The electrochemistry of the thin films was examined by cyclic voltammetry in a conventional three-electrode system and an electrochemically tested system. The electrochromic behavior of the films was demonstrated through the cyclic voltammetry (CV) process in the KNO3 electrolyte. The electrochromic behavior of the thin films depended on the redox reactions associated with the reaction between Ag and Ag2O coupled with Mn4+ ions and Mn3+ ions in the KNO3 electrolyte. Full article
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<p>A CV curve of the MnO<span class="html-italic"><sub>x</sub></span> electrode at a scan rate of 0.5 mV/s in the KNO<sub>3</sub> electrolyte to analyze the valence state of Mn ions (inset: the color of the electrolyte near the electrode).</p>
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<p>A CV curve of the MnO<span class="html-italic"><sub>x</sub></span>/Ag electrode at a scan rate of 0.5 mV/s in the KNO<sub>3</sub> electrolyte to analyze the valence state of Mn and Ag ions (inset: the color of the electrolyte near the electrode).</p>
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<p>Changes in the absorbance of the thin films from the UV to visible wavelength at each step in the redox reaction. (I, II and III are related to the steps in <a href="#engproc-89-00035-f002" class="html-fig">Figure 2</a>).</p>
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<p>XPS spectra of Mn 2p<sub>3/2</sub> for thin film at each redox step: (<b>a</b>) original, (<b>b</b>) peak I, (<b>c</b>) peak II, (<b>d</b>) peak III, as shown in <a href="#engproc-89-00035-f002" class="html-fig">Figure 2</a>.</p>
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<p>XPS spectra of Ag 3d<sub>5/2</sub> for thin film with Ag content of 8% at (<b>a</b>) original, (<b>b</b>) peak I, (<b>c</b>) peak II, (<b>d</b>) peak III in the CV process, as shown in <a href="#engproc-89-00035-f002" class="html-fig">Figure 2</a>.</p>
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<p>Images showing changes in the surface morphology of the thin films during the cyclic voltammetry process. (<b>a</b>) Original test piece; (<b>b</b>) I; (<b>c</b>) II; (<b>d</b>) III.</p>
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<p>TEM images and electron diffraction patterns of the thin films (<b>a</b>,<b>b</b>) before and (<b>c</b>,<b>d</b>) after the redox reactions.</p>
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11 pages, 1448 KiB  
Article
Design of a Low-Infrared-Emission and Wideband-Microwave-Absorption Lightweight Metasurface
by Liping Liu, Zongsheng Chen, Zhigang Li, Yajing Chang, Pengfei Li, Xun Liu, Xuesong Deng and Yunsong Feng
Nanomaterials 2025, 15(5), 399; https://doi.org/10.3390/nano15050399 - 5 Mar 2025
Viewed by 256
Abstract
The compatibility of low infrared emission and wideband microwave absorption has drawn extensive attention, both theoretically and practically. In this paper, an infrared–radar-compatible stealth metasurface is designed using transparent conductive materials, namely indium tin oxide (ITO) and poly methacrylimide (PMI). The designed structure [...] Read more.
The compatibility of low infrared emission and wideband microwave absorption has drawn extensive attention, both theoretically and practically. In this paper, an infrared–radar-compatible stealth metasurface is designed using transparent conductive materials, namely indium tin oxide (ITO) and poly methacrylimide (PMI). The designed structure is a combination of a radar-absorbing layer (RAL) and a low-infrared-emission layer (IRSL), with an overall thickness of about 1.7 mm. It consists of three layers, a top-layer patch-type ITO frequency-selective surface, an intermediate layer of a four-fold rotationally symmetric ITO patterned structure, and a bottom reflective surface. The layers are separated by PMI. Simulation results show that the structure achieves over 90% broadband absorption in the microwave band from 7 to 58 GHz and low emissivity of 0.36 in the infrared band. In addition, due to the four-fold rotationally symmetric design, the structure also exhibits polarization insensitivity and excellent angular stability. Therefore, the designed structure possesses ultra-broadband radar absorption performance, low infrared emissivity, and polarization-insensitive properties at a thin thickness, and has a promising application in the field of multi-band-compatible stealth technology. Full article
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<p>Schematic diagram of the unit structure. (<b>a</b>) front view of absorber; (<b>b</b>) top view of IRSL; (<b>c</b>) top view of RAL.</p>
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<p>Microwave transmittance of IRSL with different patch sizes.</p>
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<p>Absorption, transmittance, and reflectance simulation structure.</p>
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<p>(<b>a</b>) Absorbance at different patch sizes; (<b>b</b>) absorbance at different square resistances.</p>
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<p>Absorbance at different incidence angles for (<b>a</b>) TE and (<b>b</b>) TM modes.</p>
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<p>Absorption rate curves for different models.</p>
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<p>The real part and imaginary part of the characteristic impedance.</p>
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<p>Electric field distribution at 10 GHz and 41 GHz, and surface current distribution. (<b>a</b>) Electric field distribution in RAL layer; (<b>b</b>) electric field distribution in IRSL; (<b>c</b>) surface current distribution.</p>
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15 pages, 2871 KiB  
Article
The Power of Machine Learning Methods and PSO in Air Quality Prediction
by Emine Cengil
Appl. Sci. 2025, 15(5), 2546; https://doi.org/10.3390/app15052546 - 27 Feb 2025
Viewed by 252
Abstract
Monitoring and forecasting air quality is essential for public health and environmental management. It details the air’s cleanliness, pollution levels, and any related health risks that the general public may find concerning. This research investigates how effective machine learning techniques and particle swarm [...] Read more.
Monitoring and forecasting air quality is essential for public health and environmental management. It details the air’s cleanliness, pollution levels, and any related health risks that the general public may find concerning. This research investigates how effective machine learning techniques and particle swarm optimization are in predicting air quality. An array of machine learning algorithms, including XGBoost, support vector regression, linear regression, and random forest, was selected to ensure effective modeling outcomes. The models were trained on an open access dataset and performed performance evaluation. The answers from an on-site gas multisensor device in an Italian city were included in the dataset. The findings from the dataset were shown to accurately model and predict environmental factors affecting air quality (e.g., air temperature, humidity, indium oxide, tin oxide, NOx, NO2, etc.) using real-world air quality data. The experiments were repeated by optimizing the relevant machine learning methods with PSO. PSO is a metaheuristic optimization method widely used in feature selection and feature extraction processes. The metrics MAE, MSE, RMSE, and R2, commonly used to evaluate regression algorithms, were utilized to assess the models’ performances. Particle swarm optimization-based support vector regression performed best, with MAE, MSE, RMSE, and R2 values of 0.071, 0.015, 0.122, and 0.999, respectively. In addition, Shapley additive explanations (SHAP) analysis was performed to show which feature of the PSO-based SVR model was practical and to what extent. The results show that the proposed model successfully predicts air quality. Full article
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<p>Boxplot showing the variables in the dataset and the starting value distributions for each variable.</p>
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<p>The implementation stages of the proposed method.</p>
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<p>The value ranges for each feature after preprocessing.</p>
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<p>Predictive performance of machine learning + PSO models.</p>
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<p>Actual prediction comparison of PSO-optimized models.</p>
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<p>SHAP values for air quality prediction. Distribution and importance order of variables affecting SVR + PSO model output (the top value is the most effective).</p>
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16 pages, 36325 KiB  
Article
Effect of Annealing in Air on the Structural and Optical Properties and Efficiency Improvement of TiO2/CuxO Solar Cells Obtained via Direct-Current Reactive Magnetron Sputtering
by Grzegorz Wisz, Maciej Sibiński, Mirosław Łabuz, Piotr Potera, Dariusz Płoch, Mariusz Bester and Rostyslav Yavorskyi
Materials 2025, 18(4), 888; https://doi.org/10.3390/ma18040888 - 18 Feb 2025
Viewed by 354
Abstract
In this study, four various titanium dioxide/cuprum oxide (TiO2/CuxO) photovoltaic structures deposited on glass/indium tin oxide (ITO) substrates using the direct-current (DC) reactive magnetron sputtering technique were annealed in air. In our previous work, the deposition parameters for different [...] Read more.
In this study, four various titanium dioxide/cuprum oxide (TiO2/CuxO) photovoltaic structures deposited on glass/indium tin oxide (ITO) substrates using the direct-current (DC) reactive magnetron sputtering technique were annealed in air. In our previous work, the deposition parameters for different buffer layer configurations were first optimized to enhance cell fabrication efficiency. In this paper, the effects of post-deposition annealing at 150 °C in air on the optical properties and I-V characteristics of the prepared structures were examined. As a result, significant changes in optical properties and a meaningful improvement in performance in comparison to unannealed cells were observed. Air annealing led to an increase in the reflection coefficient of the TiO2 layer for three out of four structures. A similar increase in the reflection of the CuxO layer occurred after heating for two out of four structures. Transmission of the TiO2/CuxO photovoltaic structures also increased after heating for three out of four samples. For two structures, changes in both transmission and reflection resulted in higher absorption. Moreover, annealing the as-deposited structures resulted in a maximum relative increase in open-circuit voltage (Voc) by 294% and an increase in short-circuit current (Isc) by 1200%. The presented article gives some in-depth analysis of these reported changes in character and origin. Full article
(This article belongs to the Special Issue Advances in Solar Cell Materials and Structures—Second Edition)
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<p>Surface morphology (<b>a</b>,<b>b</b>) and cross-sectional SEM images (<b>c</b>,<b>d</b>) of TiO<sub>2</sub>/Cu<sub>x</sub>O solar cells before (<b>a</b>,<b>c</b>) and after annealing (<b>b</b>,<b>d</b>) for sample #1.</p>
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<p>Surface morphology (<b>a</b>,<b>b</b>) and cross-sectional SEM images (<b>c</b>,<b>d</b>) of TiO<sub>2</sub>/Cu<sub>x</sub>O solar cells before (<b>a</b>,<b>c</b>) and after annealing (<b>b</b>,<b>d</b>) for sample #1.</p>
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<p>Surface morphology (<b>a</b>,<b>b</b>) and cross-sectional SEM images (<b>c</b>,<b>d</b>) of TiO<sub>2</sub>/Cu<sub>x</sub>O solar cells before (<b>a</b>,<b>c</b>) and after annealing (<b>b</b>,<b>d</b>) for sample #2.</p>
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<p>Surface morphology (<b>a</b>,<b>b</b>) and cross-sectional SEM images (<b>c</b>,<b>d</b>) of TiO<sub>2</sub>/Cu<sub>x</sub>O solar cells before (<b>a</b>,<b>c</b>) and after annealing (<b>b</b>,<b>d</b>) for sample #2.</p>
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<p>Surface morphology (<b>a</b>,<b>b</b>) and cross-sectional SEM images (<b>c</b>,<b>d</b>) of TiO<sub>2</sub>/Cu<sub>x</sub>O solar cells before (<b>a</b>,<b>c</b>) and after annealing (<b>b</b>,<b>d</b>) for sample #3.</p>
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<p>Surface morphology (<b>a</b>,<b>b</b>) and cross-sectional SEM images (<b>c</b>,<b>d</b>) of TiO<sub>2</sub>/Cu<sub>x</sub>O solar cells before (<b>a</b>,<b>c</b>) and after annealing (<b>b</b>,<b>d</b>) for sample #3.</p>
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<p>Surface morphology (<b>a</b>,<b>b</b>) and cross-sectional SEM images (<b>c</b>,<b>d</b>) of TiO<sub>2</sub>/Cu<sub>x</sub>O solar cells before (<b>a</b>,<b>c</b>) and after annealing (<b>b</b>,<b>d</b>) for sample #4.</p>
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<p>Surface morphology (<b>a</b>,<b>b</b>) and cross-sectional SEM images (<b>c</b>,<b>d</b>) of TiO<sub>2</sub>/Cu<sub>x</sub>O solar cells before (<b>a</b>,<b>c</b>) and after annealing (<b>b</b>,<b>d</b>) for sample #4.</p>
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<p>Transmission spectra of samples #1 (<b>a</b>), #2 (<b>b</b>), #3 (<b>c</b>), and #4 (<b>d</b>) before (black line) and after annealing (red line).</p>
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<p>Transmission spectra of samples #1 (<b>a</b>), #2 (<b>b</b>), #3 (<b>c</b>), and #4 (<b>d</b>) before (black line) and after annealing (red line).</p>
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<p>Reflection spectra of samples #1 (<b>a</b>), #2 (<b>b</b>), #3 (<b>c</b>), and #4 (<b>d</b>) from the TiO<sub>2</sub> side before (black line) and after annealing (red line).</p>
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<p>Reflection spectra of samples #1 (<b>a</b>), #2 (<b>b</b>), #3 (<b>c</b>), and #4 (<b>d</b>) from the TiO<sub>2</sub> side before (black line) and after annealing (red line).</p>
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<p>Reflection spectra of samples #1 (<b>a</b>), #2 (<b>b</b>), #3 (<b>c</b>), and #4 (<b>d</b>) from the Cu<sub>x</sub>O side before (black line) and after annealing (red line).</p>
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<p>Reflection spectra of samples #1 (<b>a</b>), #2 (<b>b</b>), #3 (<b>c</b>), and #4 (<b>d</b>) from the Cu<sub>x</sub>O side before (black line) and after annealing (red line).</p>
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<p>Absorption spectra of samples #1, #2, #3, and #4 before (<b>a</b>) and after annealing (<b>b</b>).</p>
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<p>Comparison of dark (<b>a</b>) and light (<b>b</b>) I-V characteristics for heated (_H) and unheated (_AD—[<a href="#B27-materials-18-00888" class="html-bibr">27</a>]) cell samples #1, #2, #3, and #4.</p>
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15 pages, 3310 KiB  
Article
High-Performance Ag-NWs Doped Graphene/ITO Hybrid Transparent Conductive Electrode
by Hana Bourahla, Susana Fernández, Yu Kyoung Ryu, Andres Velasco, Chahinez Malkia, Alberto Boscá, M. Belén Gómez-Mancebo, Fernando Calle and Javier Martinez
Micromachines 2025, 16(2), 204; https://doi.org/10.3390/mi16020204 - 11 Feb 2025
Viewed by 596
Abstract
Indium tin oxide (ITO) is a commonly used material for transparent conductive electrodes (TCE) in optoelectronic applications. On the other hand, graphene has superior electrical conductivity and exceptional mechanical flexibility, which makes it a promising candidate as a TCE material. This work proposes [...] Read more.
Indium tin oxide (ITO) is a commonly used material for transparent conductive electrodes (TCE) in optoelectronic applications. On the other hand, graphene has superior electrical conductivity and exceptional mechanical flexibility, which makes it a promising candidate as a TCE material. This work proposes a CVD graphene/ITO hybrid electrode enhanced by doping with silver nanowires (Ag-NWs). The study aims to improve the performance of the electrode by optimizing two key parameters during the fabrication process: the thermal annealing time after the transfer of graphene on ITO and the Ag-NWs doping conditions. The annealing treatment is fundamental to reducing the residues on the surface of graphene and increasing the interface contact between graphene and ITO. The correct coverage and distribution of the dopant on graphene is obtained by controlling the concentration of the Ag-NWs and the spin coating speeds. The results indicate a substantial improvement in the optical and electrical performance of the Ag-NWs/graphene/ITO hybrid electrode. A remarkably low sheet resistance of 42.4 Ω/sq (±2 Ω/sq) has been achieved while maintaining a high optical transmittance of 87.3% (±0.5%). Full article
(This article belongs to the Special Issue 2D-Materials Based Fabrication and Devices)
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<p>(<b>a</b>) Schematic diagram with the fabrication process steps of the transparent conductive electrode presented in this work. (<b>b</b>) Scheme of the cross-section of the sample at the end of the fabrication steps.</p>
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<p>(<b>a</b>) Sheet resistance variation in the hybrid graphene/ITO electrode on/Si substrate at different process steps for the three thermal annealing times. (<b>b</b>) A scheme with cross-sections explains the effect of the thermal annealing step on the removal of the PMMA residues and air bubbles or water confined between the graphene layer and ITO. The elements of the scheme are not in scale. (<b>c</b>) Hemispherical reflectance of the hybrid graphene/ITO electrode deposited on Si substrate at different thermal annealing times. (<b>d</b>) Normalized optical transmittance of the hybrid graphene/ITO electrode deposited on the glass substrate at different process steps for the three different thermal annealing times. wavelength.</p>
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<p>SEM images of graphene/ITO electrodes (sample S3) doped with silver nanowires at different conditions: (<b>a</b>) Sample S3.1, 1 mg/mL of density, spin-coated at 1000 rpm. (<b>b</b>) Sample S3.2, 1 mg/mL of density, spin-coated at 3000 rpm. (<b>c</b>) Sample S3.3, 2 mg/mL of density, spin-coated at 1000 rpm. (<b>d</b>) Sample S3.4, 2 mg/mL of density, spin-coated at 3000 rpm.</p>
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<p>Raman spectra of the CVD graphene after transfer on ITO/Si substrate and annealing at 150 °C for 120 min (black curve) and after doping with Ag-NWs with 2 mg/mL, deposited at 1000 rpm (red curve).</p>
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<p>Variation of the electrical and optical characteristics of the Ag-NWs/MLG/ITO electrode with the doping concentration and spin coating speed variation: (<b>a</b>) Sheet resistance variation in the sample S3 on the silicon substrate. (<b>b</b>) Optical reflectance of the samples S3 on the silicon substrate. (<b>c</b>) Normalized optical transmittance of the samples S’3 on the glass substrate.</p>
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14 pages, 4058 KiB  
Article
Homogeneous Aptasensor with Electrochemical and Electrochemiluminescence Dual Detection Channels Enabled by Nanochannel-Based Probe Enrichment and DNase I Cleavage for Tumor Biomarker Detection
by Jiong Gao, Shiyue Zhang and Fengna Xi
Molecules 2025, 30(3), 746; https://doi.org/10.3390/molecules30030746 - 6 Feb 2025
Viewed by 511
Abstract
Homogeneous aptasensors that eliminate the need for probe labeling or immobilization hold significant potential for the rapid detection of tumor biomarkers. Herein, a homogeneous aptasensor with electrochemical (EC) and electrochemiluminescence (ECL) dual detection channels was developed by integrating nanochannel-based probe enrichment and DNase [...] Read more.
Homogeneous aptasensors that eliminate the need for probe labeling or immobilization hold significant potential for the rapid detection of tumor biomarkers. Herein, a homogeneous aptasensor with electrochemical (EC) and electrochemiluminescence (ECL) dual detection channels was developed by integrating nanochannel-based probe enrichment and DNase I cleavage for selective detection of the tumor biomarker, carbohydrate antigen 125 (CA125). A two-dimensional (2D) composite probe was prepared by assembling the CA125-specific aptamer and the cationic probe tris(2,2′-bipyridyl)Ru(II) (Ru(bpy)32+), which exhibited both EC and ECL properties, onto graphene oxide (GO) nanosheets (Ru(bpy)32+/Apt@GO). A vertically ordered mesoporous silica film (VMSF) with ultrasmall, uniform, and vertically aligned nanochannel arrays was rapidly grown on the inexpensive and disposable indium tin oxide (ITO) electrode, forming the detection interface. Due to the size exclusion effect of the ultrasmall nanochannels in VMSF, the Ru(bpy)32+/Apt@GO probe was unable to penetrate the nanochannels, resulting in no detectable Ru(bpy)32+ signal on the electrode. Upon specific recognition of CA125 by the aptamer, an aptamer-CA125 complex was formed and subsequently detached from GO. DNase I then cleaved the aptamer-CA125 complex, releasing CA125 and allowing Ru(bpy)32+ to dissociate into the solution. This enzymatic cleavage enabled CA125 to re-enter the binding cycle, amplifying the release of Ru(bpy)32+ into the solution. The electrostatic adsorption of the cationic Ru(bpy)32+ by VMSF significantly enhanced both the EC and ECL signals. The constructed aptasensor exhibited a linear EC detection range for CA125 from 0.1 U/mL to 100 ng/mL, with a limit of detection (LOD) of 91 mU/mL. For ECL detection, CA125 was detected over a range from 0.001 to 100 U/mL, with a LOD as low as 0.4 mU/mL. The developed aptasensor demonstrated excellent selectivity and was successfully applied to the dual-mode EC/ECL detection of CA125 in fetal bovine serum samples. Full article
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<p>Schematic illustration for the fabrication of the homogeneous aptasensor by integrating the exclusion properties of SNF toward 2D materials, the enrichment toward positively charged probes, and the cyclic cleavage activity of nucleases for dual-mode EC and ECL detection of CA125.</p>
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<p>(<b>a</b>) Top-view TEM image of VMSF. Inset is the corresponding high-resolution TEM image. The red markings in the inset represented the hexagonal structure composed of nanochannels. (<b>b</b>) SEM image of the cross-sectional of VNSF/ITO electrode. (<b>c</b>,<b>d</b>) CV curves recorded on bare ITO (black line), SM@VMSF/ITO containing micelles (blue line), and VMSF/ITO with open nanochannel (red line) electrodes in solutions containing different probes. The electrolyte solution was 0.05 M KHP (pH 7.4) containing 0.5 mM of Fe(CN)<sub>6</sub><sup>3−</sup> (<b>c</b>), or Ru(NH<sub>3</sub>)<sub>6</sub><sup>3+</sup>.</p>
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<p>AFM image (<b>a</b>), the height-distance line (<b>b</b>), TEM image (<b>c</b>) and FT-IR spectrum (<b>d</b>) of GO.</p>
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<p>AFM image (<b>a</b>), the height-distance line (<b>b</b>), TEM image (<b>c</b>) and FT-IR spectrum (<b>d</b>) of GO.</p>
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<p>(<b>a</b>) CV, (<b>b</b>) DPV curves, and (<b>c</b>) ECL intensity-potential curves obtained on VMSF/ITO. ECL-potential, (<b>d</b>) ECL-time curve obtained on VMSF/ITO with Ru(bpy)<sub>3</sub><sup>2+</sup>/Apt@GO composite probe and different substances.</p>
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<p>(<b>a</b>) Optimization of concentration of Ru(bpy)<sub>3</sub>Cl<sub>2</sub>. (<b>b</b>) ECL intensity obtained using different reaction times with DNase I. The star symbol represented the date point.</p>
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<p>(<b>a</b>) DPV curves obtained in the presence of different concentrations of CA125 (0.1 U/mL, 0.5 U/mL, 1 U/mL, 5 U/mL, 10 U/mL, 50 U/mL, and 100 U/mL), and (<b>b</b>) the corresponding linear regression curves. (<b>c</b>) ECL intensity−time response obtained with different concentrations of CA125 (0.001 U/mL, 0.01 U/mL, 0.1 U/mL, 1 U/mL, 10 U/mL, and 100 U/mL), and (<b>d</b>) the corresponding linear regression curve.</p>
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<p>(<b>a</b>) DPV curves obtained in the presence of different concentrations of CA125 (0.1 U/mL, 0.5 U/mL, 1 U/mL, 5 U/mL, 10 U/mL, 50 U/mL, and 100 U/mL), and (<b>b</b>) the corresponding linear regression curves. (<b>c</b>) ECL intensity−time response obtained with different concentrations of CA125 (0.001 U/mL, 0.01 U/mL, 0.1 U/mL, 1 U/mL, 10 U/mL, and 100 U/mL), and (<b>d</b>) the corresponding linear regression curve.</p>
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<p>Difference in DPV peak current (<b>a</b>) and ECL signal (<b>b</b>) response (<span class="html-italic">I</span> − <span class="html-italic">I</span><sub>0</sub>) without (<span class="html-italic">I</span><sub>0</sub>) or with (<span class="html-italic">I</span>) CA125. During incubation, CA199 (10 U/mL), CA 15-3 (10 U/mL), CEA (500 ng/mL), AFP (500 ng/mL), Glu (50 μM), lysine (50 μM), or CA125 (10 U/mL) was added or mixed.</p>
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14 pages, 4727 KiB  
Article
Dielectrophoresis-Enhanced Microfluidic Device with Membrane Filter for Efficient Microparticle Concentration and Optical Detection
by Young-Ho Nam, Seung-Ki Lee and Jae-Hyoung Park
Micromachines 2025, 16(2), 158; https://doi.org/10.3390/mi16020158 - 29 Jan 2025
Viewed by 522
Abstract
This paper presents a novel microfluidic device that integrates dielectrophoresis (DEP) forces with a membrane filter to concentrate and trap microparticles in a narrow region for enhanced optical analysis. The device combines the broad particle capture capability of a membrane filter with the [...] Read more.
This paper presents a novel microfluidic device that integrates dielectrophoresis (DEP) forces with a membrane filter to concentrate and trap microparticles in a narrow region for enhanced optical analysis. The device combines the broad particle capture capability of a membrane filter with the precision of DEP to focus particles in regions optimized for optical measurements. The device features transparent indium tin oxide (ITO) top electrodes on a glass substrate and gold (Au) bottom electrodes patterned on a small area of the membrane filter, with spacers to control the gaps between the electrodes. This configuration enables precise particle concentration at a specific location and facilitates real-time optical detection. Experiments using 0.8 μm fluorescent polystyrene (PS) beads and Escherichia coli (E. coli) bacteria demonstrated effective particle trapping and concentration, with fluorescence intensity increasing proportionally to particle concentration. The application of DEP forces in a small region of the membrane filter resulted in a significant enhancement of fluorescence intensity, showcasing the effectiveness of the DEP-enhanced design for improving particle concentration and optical measurement sensitivity. The device also showed promising potential for bacterial detection, particularly with E. coli, by achieving a linear increase in fluorescence intensity with increasing bacterial concentration. These results highlight the device’s potential for precise and efficient microparticle concentration and detection. Full article
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<p>Schematic diagram of the microfluidic device integrating a DEP-based particle concentration mechanism within a membrane filter.</p>
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<p>Exploded view of microfluidic device.</p>
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<p>Fabrication diagram of the microfluidic device: (<b>a</b>) Photolithography process and Deep-RIE for fabricating the silicon mold. (<b>b</b>) Polymer deposition to reduce adhesion and PDMS drop-casting. (<b>c</b>) Clamping the PET film and silicon mold for spacer fabrication. (<b>d</b>) Peeling off the PET film. (<b>e</b>) Bonding the PC filter with PDMS. (<b>f</b>) Bonding the PDMS pillar array with the membrane filter. (<b>g</b>) Peeling off the PET film and electrode deposition using a shadow mask. (<b>h</b>) Oxygen plasma bonding between the ITO electrode-formed glass substrate and the PDMS layer.</p>
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<p>Photographs of the fabricated microfluidic device and experimental setup for microparticle concentration within the microfluidic device.</p>
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<p>(<b>a</b>) Fluorescence images at different particle concentration times. (<b>b</b>) Fluorescence intensity measurements as a function of concentration time.</p>
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<p>(<b>a</b>) Fluorescence images with and without the application of DEP force. (<b>b</b>) Comparison of fluorescence intensity with and without the application of AC voltage.</p>
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<p>Recovery rate as a function of applied voltage under conditions with only DEP forces, excluding the membrane filter.</p>
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<p>Comparison of the drag force on the particles with the applied DEP force.</p>
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<p>Fluorescence intensities corresponding to different microparticle concentrations.</p>
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<p>(<b>a</b>) Fluorescence images of <span class="html-italic">E. coli</span> before and after enrichment. (<b>b</b>) Fluorescence intensity measurement results according to <span class="html-italic">E. coli</span> concentration.</p>
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18 pages, 4136 KiB  
Article
Sensitive Detection of Biomarker in Gingival Crevicular Fluid Based on Enhanced Electrochemiluminescence by Nanochannel-Confined Co3O4 Nanocatalyst
by Changfeng Zhu, Yujiao Zhao and Jiyang Liu
Biosensors 2025, 15(1), 63; https://doi.org/10.3390/bios15010063 - 19 Jan 2025
Cited by 2 | Viewed by 948
Abstract
The sensitive detection of inflammatory biomarkers in gingival crevicular fluid (GCF) is highly desirable for the evaluation of periodontal disease. Luminol-based electrochemiluminescence (ECL) immunosensors offer a promising approach for the fast and convenient detection of biomarkers. However, luminol’s low ECL efficiency under neutral [...] Read more.
The sensitive detection of inflammatory biomarkers in gingival crevicular fluid (GCF) is highly desirable for the evaluation of periodontal disease. Luminol-based electrochemiluminescence (ECL) immunosensors offer a promising approach for the fast and convenient detection of biomarkers. However, luminol’s low ECL efficiency under neutral conditions remains a challenge. This study developed an immunosensor by engineering an immunorecognition interface on the outer surface of mesoporous silica nanochannel film (SNF) and confining a Co3O4 nanocatalyst within the SNF nanochannels to improve the luminol ECL efficiency. The SNF was grown on an indium tin oxide (ITO) electrode using the simple Stöber solution growth method. A Co3O4 nanocatalyst was successfully confined within the SNF nanochannels through in situ electrodeposition, confirmed by X-ray photoelectron spectroscopy (XPS) and electrochemical measurements. The confined Co3O4 demonstrated excellent electrocatalytic activity, effectively enhancing luminol and H2O2 oxidation and boosting the ECL signal under neutral conditions. Using interleukin-6 (IL-6) as a proof-of-concept demonstration, the epoxy functionalization of the SNF outer surface enabled the covalent immobilization of capture antibodies, forming a specific immunorecognition interface. IL-6 binding induced immunocomplex formation, which reduced the ECL signal and allowed for quantitative detection. The immunosensor showed a linear detection range for IL-6 from 1 fg mL−1 to 10 ng mL−1, with a limit of detection (LOD) of 0.64 fg mL−1. It also demonstrated good selectivity and anti-interference capabilities, enabling the successful detection of IL-6 in artificial GCF samples. Full article
(This article belongs to the Special Issue Biosensing and Diagnosis—2nd Edition)
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<p>Schematic illustration for immunosensor construction and ECL detection of IL-6 through integrating both a specific recognition interface on the outer surface of SNF and Co<sub>3</sub>O<sub>4</sub> nanocatalyst confined in SNF nanochannels.</p>
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<p>(<b>A</b>) SEM image of the cross-section of SNF/ITO electrode. (<b>B</b>) Top-view TEM image of SNF. (<b>C</b>) Cross-sectional TEM image of SNF. (<b>C</b>–<b>E</b>) CV curves obtained on ITO, SM@SNF/ITO, and SNF/ITO electrodes in 0.05 M KHP (pH 4) containing 0.5 mM of K<sub>3</sub>Fe(CN)<sub>6</sub> (<b>D</b>), Ru(NH<sub>3</sub>)<sub>6</sub>Cl<sub>3</sub>, (<b>E</b>) or FcMeOH (<b>F</b>). The scan rate was 50 mV/s.</p>
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<p>(<b>A</b>) CV curves obtained on SNF/ITO or Co<sub>3</sub>O<sub>4</sub>@SNF/ITO in 1 M NaOH. The scanning rate was 100 mV/s, and the scanning potential ranged from –0.1 V to 0.6 V. (<b>B</b>) XPS spectra obtained on the fabricated SNF/ITO or Co<sub>3</sub>O<sub>4</sub>@SNF/ITO electrode. (<b>C</b>) High-resolution Co 2p spectrum obtained on Co<sub>3</sub>O<sub>4</sub>@SNF/ITO electrode. (<b>D</b>) SEM image (<b>left</b> image) of Co<sub>3</sub>O<sub>4</sub>@SNF/ITO electrode after removal of SNF through immersion into a 0.5 M NaOH solution for 3 min and the corresponding O (<b>right</b> and <b>above</b> image) and Co (<b>right</b> and <b>bottom</b> image) element mapping image. (<b>E</b>) Top-view SEM image (<b>left</b> image) of Co<sub>3</sub>O<sub>4</sub>@/ITO electrode and the corresponding O (<b>right</b> and <b>above</b> image) and Co (<b>right</b> and <b>bottom</b> image) element mapping image.</p>
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<p>(<b>A</b>) ECL curves obtained from different electrodes in PBS (0.01 M, pH 7.4) containing luminol (100 μM) and H<sub>2</sub>O<sub>2</sub> (100 μM). (<b>B</b>) ECL intensity obtained on Co<sub>3</sub>O<sub>4</sub>@SNF/ITO or (<b>C</b>) Co<sub>3</sub>O<sub>4</sub>/ITO from continuously scans in PBS (0.01 M, pH 7.4) containing luminol (100 μM) and H<sub>2</sub>O<sub>2</sub> (100 μM). The PMT voltage was set to 750 V. The scanning rate was 100 mV/s, and the scanning potential range was 0 V~0.8 V.</p>
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<p>CV curves obtained on SNF/ITO (<b>A</b>) and Co<sub>3</sub>O<sub>4</sub>@SNF/ITO (<b>B)</b> electrodes in the electrolyte (PBS, 0.01 M, pH 7.4) or electrolyte containing luminol (100 μM) or H<sub>2</sub>O<sub>2</sub> (100 μM). (<b>C</b>) ECL intensity obtained at the Co<sub>3</sub>O<sub>4</sub>@SNF/ITO electrode in PBS (0.01 M, pH 7.4) containing luminol (100 μM) and H<sub>2</sub>O<sub>2</sub> (100 μM) in the presence of TBA (100 μg mL<sup>−</sup><sup>1</sup>) or BQ (100 μM). (<b>D</b>) Illustration of possible ECL mechanism for luminol-H<sub>2</sub>O<sub>2</sub> system enhanced by Co<sub>3</sub>O<sub>4</sub> nanomaterials.</p>
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<p>(<b>A</b>) CV curves obtained on Co<sub>3</sub>O<sub>4</sub>@O-SNF/ITO or Co<sub>3</sub>O<sub>4</sub>@O-SNF/ITO electrodes in 0.1 M KCl containing 2.5 mM [Fe(CN)<sub>6</sub>]<sup>3−/4−</sup>. (<b>B</b>) ECL responses obtained on different electrodes in PBS (0.01 M, pH 7.4)) with H<sub>2</sub>O<sub>2</sub> (100 μM) and luminol (100 μM). (<b>C</b>) EIS plots obtained on different electrodes in 0.1 M KCl containing 2.5 mM [Fe(CN)<sub>6</sub>]<sup>3−/4−</sup>.</p>
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<p>The effect of deposition time of Co<sub>3</sub>O<sub>4</sub> (<b>A</b>), antibody concentration (<b>B</b>), incubation time for antibody immobilization (<b>C</b>), and IL-6 incubation time (<b>D</b>) on the ECL signals of the fabricated immunosensors.</p>
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<p>(<b>A</b>) ECL responses of the fabricated immunosensor in presence of various concentrations of IL-6 in PBS (0.01 M, pH 7.4) containing luminol (100 μM) and H<sub>2</sub>O<sub>2</sub> (100 μM). (<b>B</b>) The corresponding calibration curves between ECL intensity and the logarithmic concentration of IL-6. (<b>C</b>) Reproducibility of five immunosensors fabricated in parallel for IL-6 detection (10 ng mL<sup>−</sup><sup>1</sup>). (<b>D</b>) The selectivity and anti-interference of ECL immunosensor for the detection of IL-6. The concentration of Na<sup>+</sup>, Cl<sup>−</sup> was 1 μM, the concentration of K<sup>+</sup>, NO<sup>3−</sup> was 100 nM, the concentration of glucose was 10 μM, and the concentration of IL-1β, MMP-9, TNF-α was 10 ng mL<sup>−</sup><sup>1</sup>.</p>
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16 pages, 2864 KiB  
Article
Evaluation of Physicochemical Properties of Cadmium Oxide (CdO)-Incorporated Indium–Tin Oxide (ITO) Nanoparticles for Photocatalysis
by Habtamu Fekadu Etefa and Francis Birhanu Dejene
J. Compos. Sci. 2025, 9(1), 43; https://doi.org/10.3390/jcs9010043 - 16 Jan 2025
Cited by 1 | Viewed by 762
Abstract
This study investigates the structural, optical, and photocatalytic properties of cadmium oxide (CdO) nanoparticles (NPs) and indium–tin oxide (ITO)-doped CdO NPs. The synthesis of CdO NPs and ITO NPs was accomplished through the co-precipitation method. Scanning electron microscopy (SEM) analysis indicates that pure [...] Read more.
This study investigates the structural, optical, and photocatalytic properties of cadmium oxide (CdO) nanoparticles (NPs) and indium–tin oxide (ITO)-doped CdO NPs. The synthesis of CdO NPs and ITO NPs was accomplished through the co-precipitation method. Scanning electron microscopy (SEM) analysis indicates that pure CdO NPs exhibit agglomerated structures, whereas ITO doping introduces porosity and roughness, thereby improving particle dispersion and facilitating electron transport. Energy dispersive spectroscopy (EDS) corroborates the successful incorporation of tin (Sn) and indium (In) within indium–tin oxide (ITO)-doped cadmium oxide (CdO) nanoparticles (NPs) in addition to cadmium (Cd) and oxygen (O). X-ray diffraction (XRD) analysis demonstrates that an increase in ITO doping results in a reduction of the crystallite size, decreasing from 23.43 nm for pure CdO to 18.42 nm at a 10% doping concentration, which can be attributed to lattice distortion. Simultaneously, the band gap exhibits a narrowing from 2.92 eV to 2.52 eV, achieving an optimal value at 10% ITO doping before experiencing a slight increase at higher doping concentrations. This tuneable band gap improves light absorption, which is crucial for photocatalysis. The photocatalytic degradation of rhodamine B (RhB) highlights the superior efficiency of ITO-doped CdO nanoparticles, achieving a remarkable 94.68% degradation under sunlight within 120 min, up 81.01%, significantly surpassing the performance of pure CdO. The optimal RhB concentration for achieving maximum degradation was determined to be 5 mg/L. This enhanced catalytic activity demonstrates the effectiveness of ITO-doped CdO NPs under both UV and visible light, showcasing their potential for efficient pollutant degradation in sunlight-driven applications. Full article
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<p>SEM image of (<b>A</b>) CdO NPs; (<b>B</b>) CdO NPs–ITO NPs; (<b>C</b>) EDS of CdO NPs; (<b>D</b>) EDS of CdO NPs–ITO NPs; (<b>E</b>) size distribution of CdO NPs; (<b>F</b>) size distribution of CdO NPs@ITO NPs.</p>
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<p>XRD of CdO NPs at different weight % of ITO NPs.</p>
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<p>(<b>A</b>) Uv-Vis of CdO NPs at different weight % of ITO NPs. (<b>B</b>) Band gap CdO NPs at different mass of ITO NPs. (<b>C</b>) Correlation of band gap and mass deposited.</p>
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<p>Effect of concentration of RhB on photocatalytic degradations.</p>
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<p>(<b>A</b>) PL spectra of CdO NPs at different weight masses of ITO NPs. (<b>B</b>) First-cycle photocatalytic degradation of RhB by CdO NPs–ITO NPs. (<b>C</b>) Second-cycle photocatalytic degradation of RhB.</p>
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<p>Schematic mechanism of photocatalysis degradation of CdO NPs and ITO-doped CdO NPs.</p>
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11 pages, 4561 KiB  
Article
Influence of Proton Irradiation on Thin Films of AZO and ITO Transparent Conductive Oxides—Simulation of Space Environment
by Katarzyna Ungeheuer, Janusz Rybak, Amelia E. Bocirnea, Denis A. Pikulski, Aurelian C. Galca and Konstanty W. Marszalek
Appl. Sci. 2025, 15(2), 754; https://doi.org/10.3390/app15020754 - 14 Jan 2025
Viewed by 600
Abstract
Transparent conductive oxides are essential materials for many optoelectronic applications. For new devices for aerospace and space applications, it is crucial to know how they respond to the space environment. The most important issue in commonly used low-Earth orbits is proton radiation. This [...] Read more.
Transparent conductive oxides are essential materials for many optoelectronic applications. For new devices for aerospace and space applications, it is crucial to know how they respond to the space environment. The most important issue in commonly used low-Earth orbits is proton radiation. This study examines the effects of high-energy proton irradiation (226.5 MeV) on thin films of aluminium-doped zinc oxide (AZO) and indium tin oxide (ITO). We use X-ray diffraction and electron microscopy observations to see the changes in the structure and microstructure of the films. The optical properties and homogeneity of the materials are determined by spectrophotometry and spectroscopic ellipsometry (SE). Analysis of the chemical states of the elements with X-ray photoelectron spectroscopy (XPS) gives insight into what proton irradiation changes at the surface of the oxides. All measurements show that ITO is less influenced than AZO. The proton energy and fluence used in this study simulate about a hundred years in low Earth orbit. This research demonstrates that both transparent conductive oxide thin films can function under simulated space conditions, with ITO showing superior resilience. The ITO film was more homogenous in terms of the total thickness measured with SE, had fewer defects and adsorbates present on the surface, as XPS analysis proved, and did not show a difference after irradiation regarding its optical properties, transmission, refractive index, or extinction coefficient. Full article
(This article belongs to the Special Issue Materials and Coatings for Extreme Environments)
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<p>X-ray diffractograms of ITO and AZO thin films before and after proton irradiation.</p>
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<p>Scanning electron microscopy images of samples (<b>a</b>) AZO, (<b>b</b>) AZO:H+, (<b>c</b>) ITO, and (<b>d</b>) ITO:H+.</p>
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<p>Transmittance measured with a UV-VIS spectrophotometer of (<b>a</b>) AZO and (<b>b</b>) ITO before and after proton irradiation.</p>
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<p>Maps of thin film thickness determined by modelling spectroscopic ellipsometry measurements for (<b>a</b>) AZO, (<b>b</b>) AZO:H+, (<b>c</b>) ITO, and (<b>d</b>) ITO:H+.</p>
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<p>Ellipsometry data fitting results, average values from map measurements of three layers thickness, the total thickness <span class="html-italic">d</span>, and mean square error of the fits.</p>
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<p>Refractive index and extinction coefficient of the thickest layer in model of (<b>a</b>) AZO samples and (<b>b</b>) ITO samples.</p>
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<p>XPS results for AZO and AZO:H+ samples (<b>a</b>) of Zn 2p, (<b>b</b>) Al 2p, and (<b>c</b>) of O 1s; for ITO and ITO:H+ of (<b>d</b>) In 3d, (<b>e</b>) Sn 3d 5/2, and (<b>f</b>) O 1s. The black line represents the fit line, empty blue circles are data of non-irradiated samples, and red circles are data of irradiated samples.</p>
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11 pages, 2622 KiB  
Article
Self-Powered, Flexible, Transparent Tactile Sensor Integrating Sliding and Proximity Sensing
by Kesheng Wang, Shouxin Du, Jiali Kong, Minghui Zheng, Shengtao Li, Enqiang Liang and Xiaoying Zhu
Materials 2025, 18(2), 322; https://doi.org/10.3390/ma18020322 - 13 Jan 2025
Viewed by 580
Abstract
Tactile sensing is currently a research hotspot in the fields of intelligent perception and robotics. The method of converting external stimuli into electrical signals for sensing is a very effective strategy. Herein, we proposed a self-powered, flexible, transparent tactile sensor integrating sliding and [...] Read more.
Tactile sensing is currently a research hotspot in the fields of intelligent perception and robotics. The method of converting external stimuli into electrical signals for sensing is a very effective strategy. Herein, we proposed a self-powered, flexible, transparent tactile sensor integrating sliding and proximity sensing (SFTTS). The principle of electrostatic induction and contact electrification is used to achieve tactile response when external objects approach and slide. Experiments show that the material type, speed, and pressure of the perceived object can cause the changes of the electrical signal. In addition, fluorinated ethylene propylene (FEP) is used as the contact electrification layer, and indium tin oxide (ITO) is used as the electrostatic induction electrode to achieve transparency and flexibility of the entire device. By utilizing the transparency characteristics of this sensor to integrate with optical cameras, it is possible to achieve integrated perception of tactile and visual senses. This has great advantages for applications in the field of intelligent perception and is expected to be integrated with different types of optical sensors in the future to achieve multimodal intelligent perception and sensing technology, which will contribute to the intelligence and integration of robot sensing. Full article
(This article belongs to the Special Issue Advanced Piezoelectric Nanomaterials: Fundamentals and Applications)
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<p>Overview of the self-powered flexible transparent tactile sensor (SFTTS). (<b>a</b>) Schematic diagram of the developed SFTTS based on triboelectric nanogenerators. (<b>b</b>) Diagram of the structural design of proximity sensing and sliding sensing parts. (<b>c</b>) A physical image of the self-powered, flexible, transparent tactile sensor attached to the finger.</p>
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<p>The working principle of proximity and sliding sensation using triboelectric nanogenerators. (<b>a</b>) The changes in the attractive and repulsive forces between atoms at different distances. (<b>b</b>) Electron cloud overlap and charge transfer model during materials friction. (<b>c</b>) The mechanism of single-layer triboelectric nanogenerators of proximity sensing. (<b>d</b>) The mechanism of free-standing layer triboelectric nanogenerators of sliding sensing.</p>
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<p>The electrical performance of the proximity sensor of SFTTS. (<b>a</b>) The motion-electrical analysis model of the proximity sensor. (<b>b</b>) The voltage output signal as the measured object approaches the sensor. (<b>c</b>) The current output signal of the measured object and the sensor at different times. (<b>d</b>) The influence of different starting distances on the voltage and current output of the proximity sensor. (<b>e</b>) The changes of voltage and current output of the proximity sensor with various velocities. (<b>f</b>) The output voltage generated by the proximity sensor for the proximity of different materials.</p>
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<p>The electrical performance of the sliding sensor of SFTTS. (<b>a</b>) The working diagram of the sliding sensor. (<b>b</b>) The voltage output signal as the measured object sliding on the sensor. (<b>c</b>) The output voltage of the sliding sensor under different pressures. (<b>d</b>) The changes of current output of the sliding sensor with various velocities.</p>
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<p>The application of the SFTTS and integration with optical sensors. (<b>a</b>) SFTTS achieves better adhesion under different bending angles (I: 0°, II: 30°, III: 50°, IV: 70°, V: 90°), which reflects the characteristics of high flexibility. (<b>b</b>) The proximity perception of gripping objects in the fingers by SFTTS. (<b>c</b>) The SFTTS made from ITO and FEP are extremely transparent in color background. (<b>d</b>) The clarity and resolution of photos taken by optical cameras without (Image A) or with (Image B) SFTTS.</p>
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12 pages, 4146 KiB  
Article
Stripe Noise Removal in Blazed Grating Generation for Electrically Tunable Beam Deflector
by Woosup Kim, Taeyoung Kim, Jun Do, Heechang Ma, Heesun Yoon and Kanghee Won
Materials 2025, 18(2), 291; https://doi.org/10.3390/ma18020291 - 10 Jan 2025
Viewed by 510
Abstract
In this paper, we demonstrate a blazed phase grating to achieve tunable beam steering and propose a novel algorithm to reduce the stripe noise in wrapped phase. To control the diffraction angle to steer light to the desired direction, an electrically tunable transmission-type [...] Read more.
In this paper, we demonstrate a blazed phase grating to achieve tunable beam steering and propose a novel algorithm to reduce the stripe noise in wrapped phase. To control the diffraction angle to steer light to the desired direction, an electrically tunable transmission-type beam deflector based on liquid crystals is introduced, and electric fields are applied to the patterned indium tin oxide electrodes to change its phase retardation. Two different 2π phase-wrapping methods are applied to obtain various diffraction angles within the minimum cell-gap, and the method of equal interval of phase achieves a worthwhile diffraction efficiency compared to the methods based on equal interval of diffraction angle. The proposed method is able to completely eliminate the stripe noise in all steering angles that helps to improve the diffraction efficiency. Full article
(This article belongs to the Special Issue Advances in Nanophotonic Materials, Devices, and Applications)
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<p>Assigning materials to a BD. The TechWiz LCD 2D simulator (Sanayi, Incheon, Korea) was utilized. The voltage applied to each channel tilts the LC, causing a change in <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>n</mi> </mrow> </semantics></math>, which in turn leads to phase retardation.</p>
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<p>The concept of tiling process.</p>
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<p>The concept of continuous phase and wrapped phase. (<b>a</b>) represents the case where the unit prism is 1, and (<b>b</b>) represents the case where the unit prism is 4. Furthermore, the red arrow illustrates the concept of a phase exceeding 2π being wrapped down to within the 0~2π range.</p>
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<p>Conceptual diagram of equal interval of diffraction angle.</p>
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<p>Conceptual diagram of equal interval of phase.</p>
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<p>Phase remnants of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>φ</mi> </mrow> <mrow> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math> and difference in diffraction angles between <span class="html-italic">θ</span>(<span class="html-italic">n</span>) and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>θ</mi> </mrow> <mrow> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math> as a function of multiple number at the wavelength of 532 nm.</p>
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<p>Phase-wrapping methods of (<b>a</b>) equal interval of phase and (<b>b</b>) equal interval of diffraction angle when multiple number (<span class="html-italic">n</span>) is 189.</p>
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<p>CCD images of diffraction patterns obtained experimentally for various multiple numbers (<span class="html-italic">n</span>). Images (<b>b</b>,<b>d</b>,<b>f</b>) represent the results from the equal interval of the diffraction angle method, while images (<b>c</b>,<b>e</b>,<b>g</b>) correspond to the equal interval of phase method. Image (<b>a</b>) shows the diffraction pattern at <span class="html-italic">n</span> = 0. Images (<b>b</b>,<b>c</b>) display the patterns at <span class="html-italic">n</span> = 47, (<b>d</b>,<b>e</b>) at <span class="html-italic">n</span> = 189, and (<b>f</b>,<b>g</b>) at <span class="html-italic">n</span> = 330. The CCD images are arranged in the order of red (645 nm), green (532 nm), and blue (470 nm) from top to bottom. <a href="#materials-18-00291-f008" class="html-fig">Figure 8</a> includes only the CCD images for representative multiple numbers (<span class="html-italic">n</span>), but similar patterns are observed for values of <span class="html-italic">n</span> near these representatives.</p>
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<p>Experimentally measured DE of a LC BD as a function of the multiple number (<span class="html-italic">n</span>) and the difference between (a) equal interval of phase, (b) equal interval of diffraction angle, and the increment of DE between (a) and (b). The results of measuring a large number of DE were expressed as average values, and error bars were added based on the error data from these measurements.</p>
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10 pages, 2472 KiB  
Article
High-Mobility All-Transparent TFTs with Dual-Functional Amorphous IZTO for Channel and Transparent Conductive Electrodes
by Min-Woo Park, Sohyeon Kim, Su-Yeon Son, Si-Won Kim, Tae-Kyun Moon, Pei-Chen Su and Kyoung-Kook Kim
Materials 2025, 18(2), 216; https://doi.org/10.3390/ma18020216 - 7 Jan 2025
Viewed by 541
Abstract
The increasing demand for advanced transparent and flexible display technologies has led to significant research in thin-film transistors (TFTs) with high mobility, transparency, and mechanical robustness. In this study, we fabricated all-transparent TFTs (AT-TFTs) utilizing amorphous indium-zinc-tin-oxide (a-IZTO) as a dual-functional material for [...] Read more.
The increasing demand for advanced transparent and flexible display technologies has led to significant research in thin-film transistors (TFTs) with high mobility, transparency, and mechanical robustness. In this study, we fabricated all-transparent TFTs (AT-TFTs) utilizing amorphous indium-zinc-tin-oxide (a-IZTO) as a dual-functional material for both the channel layer and transparent conductive electrodes (TCEs). The a-IZTO was deposited using radio-frequency magnetron sputtering, with its composition adjusted for both channel and electrode functionality. XRD analysis confirmed the amorphous nature of the a-IZTO layers, ensuring structural stability post-thermal annealing. The a-IZTO TCEs demonstrated high optical transparency (89.57% in the visible range) and excellent flexibility, maintaining a low sheet resistance with minimal degradation even after 100,000 bending cycles. The fabricated AT-TFTs exhibit superior field-effect mobility (30.12 cm2/V·s), an on/off current ratio exceeding 108, and a subthreshold swing of 0.36 V/dec. The AT-TFT device demonstrated a minimum transmittance of 75.46% in the visible light range, confirming its suitability for next-generation flexible and transparent displays. Full article
(This article belongs to the Section Advanced Nanomaterials and Nanotechnology)
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<p>(<b>a</b>) The three-dimensional schematic image of the AT-TFT device using amorphous SiO<sub>2</sub> and dual-functional a-IZTO for channel and TCEs. (<b>a’</b>) The cross-sectional schematic image of the AT-TFT device. (<b>b</b>) The top view image of AT-TFT which has 60 μm of channel width and 20 μm of channel length. (<b>c</b>) The image of the fabricated AT-TFT wafer which has high transparency.</p>
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<p>(<b>a</b>) The resistivity, mobility, carrier concentration, and metal atom proportion of a-IZTO for TCEs deposited by RF magnetron sputtering with RF power ranging from 30 to 90 W. The black line, blue line, and red line represent the resistivity, carrier mobility, and carrier concentration of a-IZTO for TCEs, respectively. (<b>b</b>) Bending test results of a-IZTO for TCE deposited by sputtering at RF power of 50 W (bending cycles = 0, 20,000, 40,000, 60,000, 80,000, 100,000). The inset image within the graph shows the flexible bending of the a-IZTO deposited on the PI film. The FE-SEM images of (<b>b’</b>) the as-deposited a-IZTO surface and (<b>b”</b>) the a-IZTO surface after 100,000 bending cycles. The red arrow in (<b>b”</b>) indicates the cracks on the a-IZTO surface after 100,000 bending cycles.</p>
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<p>The XRD results of dual-functional a-IZTO films for 30 nm-thick channels and 200 nm-thick TCEs before and after a thermal annealing process at 300 °C for 15 min. The broad peaks in the black box indicate that both IZTO for the channel and TCEs are in an amorphous state.</p>
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<p>(<b>a</b>) Schematic image of the AT-TFT, showing the film thickness and layer structure when measuring the transmittance of a-IZTO for the channel, AT-TFT, and a-IZTO for TCEs. (<b>b</b>) Transmittance results for a-IZTO in the channel, AT-TFT, and a-IZTO for TCEs. The inset table shows the average transmittance in the 400–700 nm range.</p>
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<p>(<b>a</b>) The output and (<b>b</b>) transfer characteristics of AT-TFTs using all-amorphous oxide materials, including dual-functional a-IZTO films for channel and TCEs. The red line represents the drain current on a logarithmic scale, plotted on the left y-axis, while the blue line shows the linear measurement of the drain current, plotted on the right y-axis.</p>
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