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20 pages, 292 KiB  
Article
Readiness for Industry 4.0 in a Medical Device Manufacturer as an Enabler for Sustainability, a Case Study
by Olivia McDermott, Dudley Luke Stam, Susana Duarte and Michael Sony
Sustainability 2025, 17(1), 357; https://doi.org/10.3390/su17010357 - 6 Jan 2025
Viewed by 306
Abstract
This research aims to determine the state of Industry 4.0 readiness and to identify the best practices, challenges, and barriers to implementing Industry 4.0 technology in a medical device manufacturer, thus aiding in improving sustainability. Semi-structured interviews were completed with 12 senior executives [...] Read more.
This research aims to determine the state of Industry 4.0 readiness and to identify the best practices, challenges, and barriers to implementing Industry 4.0 technology in a medical device manufacturer, thus aiding in improving sustainability. Semi-structured interviews were completed with 12 senior executives representing a wide array of functions in a single large medical device manufacturer. Convenience sampling was used to analyse the interview transcripts to draw out themes that were then discussed and analysed with findings from the literature review. This research determined the state of Industry 4.0 readiness in the case study of medical device manufacturers. This research identified several best practices, challenges, and barriers to implementing Industry 4.0 technology. Currently, there are few case studies in the literature that have a medical device manufacturer as the case study for Industry 4.0 readiness. There are even fewer articles that tackle Industry 4.0 implementation across the entire medical device industry. There is currently no published literature that analyses the best practices for implementing Industry 4.0 in a medical device manufacturer. The best practices for Industry 4.0 implementation identified in this study can be beneficial to stakeholders in the medical device industry and within the healthcare sector, help them plan current and future Industry 4.0 programmes, improve sustainability in their companies, as well as optimise patient treatment and approaches. Full article
18 pages, 3197 KiB  
Article
Organic Optocoupler with Simple Construction as an Effective Linear Current Transceiver
by Jaroslaw Jung, Arkadiusz Selerowicz, Jacek Ulanski, Ruslana Udovytska, Beata Luszczynska, Artur Zawadzki and Andrzej Rybak
Materials 2025, 18(1), 152; https://doi.org/10.3390/ma18010152 - 2 Jan 2025
Viewed by 323
Abstract
In this study, it is shown that an efficient organic optocoupler (OPC) can be fabricated using commercially available and solution-processable organic semiconductors. The transmitter is a single-active-layer organic light-emitting diode (OLED) made from a well-known polyparavinylene derivative, Super Yellow. The receiver is an [...] Read more.
In this study, it is shown that an efficient organic optocoupler (OPC) can be fabricated using commercially available and solution-processable organic semiconductors. The transmitter is a single-active-layer organic light-emitting diode (OLED) made from a well-known polyparavinylene derivative, Super Yellow. The receiver is an organic light-emitting diode (OLSD) with a single active layer consisting of a mixture of the polymer donor PTB7-Th and the low-molecular-weight acceptor ITIC; the receiver operates without an applied reverse voltage. OLED and OLSD have the same geometry and simple structure without any interlayers: glass/ITO/PEDOT:PSS/(active layer)/Ca/Al; the OPC is formed by OLED and OLSD which adhere tightly to each other. Despite its simple structure, the OPC showed a current transfer ratio of 0.13%, good linearity, and good dynamic performance: a three-decibel cutoff frequency of 170 kHz and response times to a step change in current at the OPC input of 2 μs. Compared to most organic OPC devices with similar performance parameters, where the transmitter and receiver have complex structures with additional interlayers between the active layers and electrodes and the need to apply a reverse voltage to the receiver, the simple design of our OPC reduces the number of fabrication steps and greatly simplifies the device fabrication process. Full article
(This article belongs to the Special Issue Manufacturing, Characterization and Modeling of Advanced Materials)
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Figure 1

Figure 1
<p>Schematic diagram of an optocoupler with dc <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>i</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mo>,</mo> <mi>d</mi> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> and ac <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>i</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> <mfenced separators="|"> <mrow> <mi>t</mi> </mrow> </mfenced> </mrow> </semantics></math> input current sources and a current source <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>i</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mo>,</mo> <mi>d</mi> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> designed to eliminate the DC component from the current at the output of the optocoupler.</p>
Full article ">Figure 2
<p>Materials and devices. Organic semiconductors used to produce active layer of (<b>a</b>) OLED (Super Yellow) and of OLSD ((<b>b</b>) acceptor ITIC and (<b>c</b>) donor PTB7-Th); photos of (<b>d</b>) OLED, (<b>e</b>) OPC, and (<b>f</b>) OLSD; (<b>g</b>,<b>h</b>) work functions for electrodes (Al, ITO), hole-transporting layer (PEDOT:PSS), and electron-transporting layer (Cu) and LUMO and HOMO energies of semiconductors [<a href="#B35-materials-18-00152" class="html-bibr">35</a>,<a href="#B36-materials-18-00152" class="html-bibr">36</a>].</p>
Full article ">Figure 3
<p>(<b>a</b>) Current–voltage characteristics <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>O</mi> <mi>L</mi> <mi>E</mi> <mi>D</mi> </mrow> </msub> <mfenced separators="|"> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>O</mi> <mi>L</mi> <mi>E</mi> <mi>D</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math> (circles) and the dependence of the total radiant emittance on the voltage <math display="inline"><semantics> <mrow> <mi>m</mi> <mfenced separators="|"> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>O</mi> <mi>L</mi> <mi>E</mi> <mi>D</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math> (stars) for OLED based on SY; the symbol <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>O</mi> <mi>N</mi> </mrow> </msub> </mrow> </semantics></math> denotes the threshold voltage; the inset shows the dependence of the current efficiency <math display="inline"><semantics> <mrow> <mi>η</mi> </mrow> </semantics></math> on the current density <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>O</mi> <mi>L</mi> <mi>E</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math>; (<b>b</b>) spectral emittance <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>m</mi> </mrow> <mrow> <mi>λ</mi> </mrow> </msub> </mrow> </semantics></math> for different voltage values <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>O</mi> <mi>L</mi> <mi>E</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 4
<p>Comparison of relative overlap integrals <span class="html-italic">ξ</span> of spectral emittance <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mi mathvariant="sans-serif">λ</mi> </mrow> </msub> </mrow> </semantics></math> of OLED based on SY transmitter and responsivity <math display="inline"><semantics> <mrow> <mi mathvariant="script">R</mi> <mfenced separators="|"> <mrow> <mi>λ</mi> </mrow> </mfenced> </mrow> </semantics></math> of OLSD photodetectors based on different donor–acceptor mixtures.</p>
Full article ">Figure 5
<p>Dependence of photocurrent density at photodetector output <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>p</mi> <mi>h</mi> </mrow> </msub> </mrow> </semantics></math> on current density at transmitter input <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math> for the OLED/OLSD optocoupler. The inset shows the dependence of current ratio <span class="html-italic">CTR</span> on <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math> in the linear range of the optocoupler operation.</p>
Full article ">Figure 6
<p>Comparison of the variations in direct <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> <mi>T</mi> <mi>R</mi> </mrow> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> and alternating <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> <mi>T</mi> <mi>R</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> </mrow> </semantics></math> current transfer ratios as a function of the density of direct current component <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mo>,</mo> <mi>d</mi> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> for (<b>a</b>) the experimentally determined DC and AC current transfer ratios for the OLED/OLSD optocoupler at reverse voltage <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>v</mi> </mrow> </msub> <mtext> </mtext> </mrow> </semantics></math>= 0 and their equivalents estimated based on the experimental results obtained for the OLED transmitter and the OLSD photodetector; (<b>b</b>) direct <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> <mi>T</mi> <mi>R</mi> </mrow> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math>, and (<b>c</b>) alternating <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> <mi>T</mi> <mi>R</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> </mrow> </semantics></math> current transfer ratios determined for the photodetector biased with the reverse voltage <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>v</mi> </mrow> </msub> </mrow> </semantics></math> of two different values.</p>
Full article ">Figure 7
<p>(<b>a</b>) The highest possible value of the amplitude of the variable component of current density <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mn>0</mn> <mo>,</mo> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math> as a function of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mo>,</mo> <mi>d</mi> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> for the assumed range of linear operation of OLED/OLSD for a photodetector unpolarized by reverse voltage; (<b>b</b>) dependence of coefficient <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>δ</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> </mrow> </semantics></math> on <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mo>,</mo> <mn>0</mn> </mrow> </msub> </mrow> </semantics></math> for different values of the constant component of current <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mo>,</mo> <mi>d</mi> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> in the range 12–451 mAcm<sup>−2</sup>; (<b>c</b>,<b>d</b>) coefficient <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>δ</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> </mrow> </semantics></math> as a function of the constant component of current density <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mo>,</mo> <mi>d</mi> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> supplied to the OPC input for different values of the amplitude of variable component <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mo>,</mo> <mn>0</mn> </mrow> </msub> </mrow> </semantics></math>, for two cases: (<b>c</b>) a non-polarized photodetector and (<b>d</b>) a photodetector polarized with a reverse voltage <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>v</mi> </mrow> </msub> <mtext> </mtext> </mrow> </semantics></math>= −2 V.</p>
Full article ">Figure 8
<p>Variable components of current density at the output of the OLED/OLSD optocoupler <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>p</mi> <mi>h</mi> <mo>⊓</mo> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>p</mi> <mi>h</mi> <mo>~</mo> </mrow> </msub> </mrow> </semantics></math> as a function of time t (red) after applying a voltage wave (blue) to the transmitter input. (<b>a</b>,<b>c</b>) Rectangular <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mo>⊓</mo> </mrow> </msub> </mrow> </semantics></math> and (<b>b</b>,<b>d</b>) sinusoidal <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>i</mi> <mi>n</mi> <mo>~</mo> </mrow> </msub> </mrow> </semantics></math> of two frequencies of 100 Hz and 158 kHz; (<b>c</b>) the symbols <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>r</mi> <mi>i</mi> <mi>s</mi> <mi>e</mi> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>f</mi> <mi>a</mi> <mi>l</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math> denote the times of the rise and fall of the current at the output, respectively, after applying a rectangular voltage wave to the input; (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>d</mi> <mi>e</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math> is the delay time of the receiver photocurrent after applying a voltage harmonic component to the input.</p>
Full article ">Figure 9
<p>Comparison of frequency spectra for relative amplitude of radiant emittance <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>m</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math> of the OLED (blue circles), relative amplitude of photocurrent density <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>p</mi> <mi>h</mi> <mo>,</mo> <mi>r</mi> <mi>e</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math> of the OLSD photodiode (red circles), and relative transadmittance <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>T</mi> <mi>A</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math> of the OLED/OLSD optocoupler (green circles). Dashed curve—spectrum resulting from multiplication of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>m</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>j</mi> </mrow> <mrow> <mi>p</mi> <mi>h</mi> <mo>,</mo> <mi>r</mi> <mi>e</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math> spectra. Vertical dotted lines indicate three-decibel cutoff frequencies of OLED <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>f</mi> </mrow> <mrow> <mo>−</mo> <mn>3</mn> <mi mathvariant="normal">d</mi> <mi mathvariant="normal">B</mi> <mo>,</mo> <mi>S</mi> <mi>Y</mi> </mrow> </msub> </mrow> </semantics></math><span class="html-italic">,</span> OLSD <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>f</mi> </mrow> <mrow> <mo>−</mo> <mn>3</mn> <mi mathvariant="normal">d</mi> <mi mathvariant="normal">B</mi> <mo>,</mo> <mi>I</mi> <mi>P</mi> <mi>T</mi> </mrow> </msub> </mrow> </semantics></math> and OPC <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>f</mi> </mrow> <mrow> <mo>−</mo> <mn>3</mn> <mi mathvariant="normal">d</mi> <mi mathvariant="normal">B</mi> <mo>,</mo> <mi>O</mi> <mi>P</mi> <mi>T</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
Full article ">
15 pages, 1594 KiB  
Article
2D Model of a Biomass Single Particle Pyrolysis—Analysis of the Influence of Fiber Orientation on the Thermal Decomposition Process
by Paulina Hercel, Atahan Orhon, Michał Jóźwik and Dariusz Kardaś
Sustainability 2025, 17(1), 279; https://doi.org/10.3390/su17010279 - 2 Jan 2025
Viewed by 335
Abstract
Understanding the influence of heat transfer on the pyrolysis process is crucial for optimizing industrial biofuel production processes. While numerous scientific studies focus on experimental investigations of pyrolysis using laboratory-scale devices, many neglect the essential role of thermal energy in initiating and controlling [...] Read more.
Understanding the influence of heat transfer on the pyrolysis process is crucial for optimizing industrial biofuel production processes. While numerous scientific studies focus on experimental investigations of pyrolysis using laboratory-scale devices, many neglect the essential role of thermal energy in initiating and controlling thermal decomposition processes. This study presents a transient two-dimensional numerical model of biomass single-particle pyrolysis, which includes the energy balance, mass conservation equations and pyrolysis gas pressure and velocity equations. The model employs explicit numerical methods to manage the high computational demands of 2D transient simulations, but is successfully validated with the use of experimental data found in the literature. The model reflects the heterogeneous structure of wood by using different thermal conductivity coefficients depending on the wooden fibers’ orientation. The results demonstrate the impact of fiber orientation on the heat transfer and thermal decomposition processes. The anisotropic properties of wood led to varied temperature fields and pyrolysis decomposition stages, aligning well with experimental data, thus validating the model’s accuracy. The proposed approach can provide a better understanding and lead to improvement in biofuel production processes, enabling more efficient and controlled conversion of biomass into fuel. By optimizing the pyrolysis process, it contributes to the development of sustainable energy preservation and regeneration methods, supporting a shift towards more sustainable fuel production patterns using renewable biomass resources like wood. Full article
(This article belongs to the Special Issue Thermally Driven Renewable Energy Technologies)
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Figure 1

Figure 1
<p>Geometry of the wooden sample and fibers orientation.</p>
Full article ">Figure 2
<p>Generated mesh.</p>
Full article ">Figure 3
<p>Temperature distribution over time.</p>
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<p>Normalized mass distribution over time.</p>
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<p>Pressure distribution over time.</p>
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<p>Velocity vector components and velocity magnitude distribution over time.</p>
Full article ">
10 pages, 3719 KiB  
Article
Experimental Studies of Fluid Flow Resistance in a Heat Exchanger Based on the Triply Periodic Minimal Surface
by Marcin Kruzel, Krzysztof Dutkowski and Tadeusz Bohdal
Energies 2025, 18(1), 134; https://doi.org/10.3390/en18010134 - 1 Jan 2025
Viewed by 460
Abstract
This study describes experimental data on 3D-printed compact heat exchangers. The heat exchanger is a prototype designed and manufactured additively using 3D printing in metal—AISI 316L steel. The device’s design is based on the triply periodic minimal surface (TPMS) geometry called gyroid, which [...] Read more.
This study describes experimental data on 3D-printed compact heat exchangers. The heat exchanger is a prototype designed and manufactured additively using 3D printing in metal—AISI 316L steel. The device’s design is based on the triply periodic minimal surface (TPMS) geometry called gyroid, which can only be obtained by incremental manufacturing. This innovative heat exchange surface structure enables these devices to provide higher thermal performance while reducing their weight by up to 50%. Few publications describe thermal or flow tests in this type of device. They mainly concern computer simulations that have yet to be experimentally verified. The authors of this study conducted innovative flow tests to determine pressure drops during the flow of working fluids under conditions of variable temperature, mass flow rate and thermal load. Water was used as a heat transfer fluid during the tests. The range of parameters for the entire experiment was = 1–24 kg/h; Δpl = 0.05–2 kPa; tcold = 20 °C; thot = 50 °C. Flow characteristics during the single-phase heat exchange process were determined, including Δpl = f(), Δpl = f(Re), Δpl = f(f). The experimental data will be used to determine the relationships describing flow resistance in structures based on a triply periodic minimal surface, and it also enables one to specify the energy consumption of these devices and compare the profitability of their use to conventional designs, i.e., shell-and-tube or plate heat exchangers. Full article
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Figure 1

Figure 1
<p>The overall view of the test facility: 1—the heat exchanger; 2—pressure drop sensors; 3—mass flow meters; 4—pumps; 5—regulating valves; 6—ultra thermostat; 7—chiller; 8—data acquisition unit.</p>
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<p>The view of the 3D-printed gyroid heat exchanger.</p>
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<p>The measuring section.</p>
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<p>The dependence of local pressure drop on mass flow rate.</p>
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<p>The dependence of local pressure drop on Reynolds number.</p>
Full article ">Figure 6
<p>The dependency of local pressure drop on the mean logarithmic temperature difference [<a href="#B22-energies-18-00134" class="html-bibr">22</a>,<a href="#B23-energies-18-00134" class="html-bibr">23</a>,<a href="#B24-energies-18-00134" class="html-bibr">24</a>].</p>
Full article ">Figure 7
<p>The dependency of the experimental friction factor with the values calculated according to Equation (4).</p>
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20 pages, 11484 KiB  
Article
Tunable Filters Using Defected Ground Structures at Millimeter-Wave Frequencies
by Kaushik Annam, Birhanu Alemayehu, Eunsung Shin and Guru Subramanyam
Micromachines 2025, 16(1), 60; https://doi.org/10.3390/mi16010060 - 31 Dec 2024
Viewed by 406
Abstract
This paper explores the potential of phase change materials (PCM) for dynamically tuning the frequency response of a dumbbell u-slot defected ground structure (DGS)-based band stop filter. The DGSs are designed using co-planar waveguide (CPW) line structure on top of a barium strontium [...] Read more.
This paper explores the potential of phase change materials (PCM) for dynamically tuning the frequency response of a dumbbell u-slot defected ground structure (DGS)-based band stop filter. The DGSs are designed using co-planar waveguide (CPW) line structure on top of a barium strontium titanate (Ba0.6Sr0.4TiO3) (BST) thin film. BST film is used as the high-dielectric material for the planar DGS. Lower insertion loss of less than −2 dB below the lower cutoff frequency, and enhanced band-rejection with notch depth of −39.64 dB at 27.75 GHz is achieved by cascading two-unit cells, compared to −12.26 dB rejection with a single-unit cell using BST thin film only. Further tunability is achieved by using a germanium telluride (GeTe) PCM layer. The electrical properties of PCM can be reversibly altered by transitioning between amorphous and crystalline phases. We demonstrate that incorporating a PCM layer into a DGS device allows for significant tuning of the resonance frequency: a shift in resonance frequency from 30.75 GHz to 33 GHz with a frequency shift of 2.25 GHz is achieved, i.e., 7.32% tuning is shown with a single DGS cell. Furthermore, by cascading two DGS cells with PCM, an even wider tuning range is achievable: a shift in resonance frequency from 27 GHz to 30.25 GHz with a frequency shift of 3.25 GHz is achieved, i.e., 12.04% tuning is shown by cascading two DGS cells. The results are validated through simulations and measurements, showcasing excellent agreement. Full article
(This article belongs to the Special Issue Microwave Passive Components, 2nd Edition)
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Figure 1

Figure 1
<p>Dumbbell DGS on CPW line.</p>
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<p>U-slot DGS on CPW line.</p>
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<p>Dumbbell u-slot DGS on CPW line.</p>
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<p>Schematic representation of the fabrication process of a dumbbell u-slot DGS using CPW line configuration with BST thin film.</p>
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<p>(<b>a</b>) Simulated frequency response of dumbbell u-slot DGS. (<b>b</b>) Measured frequency response of dumbbell u-slot DGS. (<b>c</b>) Simulated vs. measured S<sub>21</sub> frequency response of dumbbell u-slot DGS.</p>
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<p>(<b>a</b>) Simulated frequency response of dumbbell u-slot DGS. (<b>b</b>) Measured frequency response of dumbbell u-slot DGS. (<b>c</b>) Simulated vs. measured S<sub>21</sub> frequency response of dumbbell u-slot DGS.</p>
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<p>Simulated vs. measured S<sub>21</sub> frequency response of dumbbell DGS.</p>
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<p>Simulated vs. measured S<sub>21</sub> frequency response of u-slot DGS.</p>
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<p>Circuit model for dumbbell u-slot DGS.</p>
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<p>Dumbbell u-slot DGS cascade.</p>
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<p>(<b>a</b>) Simulated frequency response of cascaded dumbbell u-slot DGS. (<b>b</b>) Measured frequency response of cascaded dumbbell u-slot DGS. (<b>c</b>) Simulated vs. measured S<sub>21</sub> frequency response of cascaded dumbbell u-slot DGS.</p>
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<p>(<b>a</b>) Simulated frequency response of cascaded dumbbell u-slot DGS. (<b>b</b>) Measured frequency response of cascaded dumbbell u-slot DGS. (<b>c</b>) Simulated vs. measured S<sub>21</sub> frequency response of cascaded dumbbell u-slot DGS.</p>
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<p>Circuit model for cascaded dumbbell u-slot DGS.</p>
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<p>Schematic model vs. measured S<sub>21</sub> frequency response of cascade dumbbell u-slot DGS.</p>
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<p>Dumbbell u-slot DGS on CPW line with PCM.</p>
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<p>Schematic representation of the fabrication process of a dumbbell u-slot DGS using CPW line configuration with BST and GeTe thin films.</p>
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<p>Frequency response of dumbbell u-slot DGS with PCM. (<b>a</b>) Simulation—amorphous state. (<b>b</b>) Simulation—crystalline state. (<b>c</b>) Measured—amorphous state. (<b>d</b>) Measured—crystalline state. (<b>e</b>) Simulation vs measured S<sub>21</sub>—amorphous state. (<b>f</b>) Simulation vs measured S<sub>21</sub>—crystalline state.</p>
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<p>Frequency response of dumbbell u-slot DGS with PCM. (<b>a</b>) Simulation—amorphous state. (<b>b</b>) Simulation—crystalline state. (<b>c</b>) Measured—amorphous state. (<b>d</b>) Measured—crystalline state. (<b>e</b>) Simulation vs measured S<sub>21</sub>—amorphous state. (<b>f</b>) Simulation vs measured S<sub>21</sub>—crystalline state.</p>
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<p>Frequency response of dumbbell u-slot DGS with PCM. (<b>a</b>) Simulation—amorphous state. (<b>b</b>) Simulation—crystalline state. (<b>c</b>) Measured—amorphous state. (<b>d</b>) Measured—crystalline state. (<b>e</b>) Simulation vs measured S<sub>21</sub>—amorphous state. (<b>f</b>) Simulation vs measured S<sub>21</sub>—crystalline state.</p>
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<p>Dumbbell u-slot DGS with PCM cascade.</p>
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<p>Frequency response of dumbbell u-slot DGS cascade with PCM. (<b>a</b>) Simulation—amorphous state. (<b>b</b>) Simulation—crystalline state. (<b>c</b>) Measured—amorphous state. (<b>d</b>) Measured—crystalline state. (<b>e</b>) Simulation vs measured—amorphous state. (<b>f</b>) Simulation vs measured—crystalline state.</p>
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<p>Frequency response of dumbbell u-slot DGS cascade with PCM. (<b>a</b>) Simulation—amorphous state. (<b>b</b>) Simulation—crystalline state. (<b>c</b>) Measured—amorphous state. (<b>d</b>) Measured—crystalline state. (<b>e</b>) Simulation vs measured—amorphous state. (<b>f</b>) Simulation vs measured—crystalline state.</p>
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<p>Frequency response of dumbbell u-slot DGS cascade with PCM. (<b>a</b>) Simulation—amorphous state. (<b>b</b>) Simulation—crystalline state. (<b>c</b>) Measured—amorphous state. (<b>d</b>) Measured—crystalline state. (<b>e</b>) Simulation vs measured—amorphous state. (<b>f</b>) Simulation vs measured—crystalline state.</p>
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24 pages, 2509 KiB  
Article
Unified Design Methodology for a Polycentric Transfemoral Knee Prosthesis Using Kinematic Synthesis
by Mertcan Koçak and Erkin Gezgin
Machines 2025, 13(1), 20; https://doi.org/10.3390/machines13010020 - 31 Dec 2024
Viewed by 385
Abstract
This study introduces a novel single-degree-of-freedom polycentric knee mechanism specifically designed for transfemoral prostheses to address dual challenges of stability during the stance phase and biomimetic motion during the swing phase. Leveraging analytical kinematic synthesis, the proposed mechanism integrates separate kinematic designs for [...] Read more.
This study introduces a novel single-degree-of-freedom polycentric knee mechanism specifically designed for transfemoral prostheses to address dual challenges of stability during the stance phase and biomimetic motion during the swing phase. Leveraging analytical kinematic synthesis, the proposed mechanism integrates separate kinematic designs for each of the gait phases into a combined structure that prevents singularity issues during full knee flexion, which is a significant limitation in conventional active designs. The stance phase mechanism emphasizes stability through precise control of the instantaneous center of rotation (ICR) and weight-bearing support, while the swing phase mechanism adopts a biomimetic motion trajectory. In order to validate the proposed methodology, kinematic synthesis, numerical simulations, and visual analyses were conducted. Incorporating insights from polycentric prostheses and orthotic applications, the proposed mechanism achieves a seamless transition between two different configurations by keeping its overall mobility. Additionally, its possible compatibility with motorized actuation offers a foundation for active prosthesis systems, paving the way for adapting the advantages of polycentric prosthesis to active devices. This innovative approach offers a scientifically grounded pathway for improving transfemoral prosthetic systems, advancing both their biomechanical utility and user comfort. Full article
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<p>Structural design flow [<a href="#B48-machines-13-00020" class="html-bibr">48</a>]: (<b>a</b>) stance phase mechanism on knee; (<b>b</b>) stance phase kinematic structure; (<b>c</b>) swing phase mechanism on knee; (<b>d</b>) swing phase kinematic structure; and (<b>e</b>) coarsely combined mechanism kinematic structure around stance–swing transition moment.</p>
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<p>Stance phase kinematic representations [<a href="#B48-machines-13-00020" class="html-bibr">48</a>]: (<b>a</b>) Upper triangle parameters; (<b>b</b>) stance kinematic structure with parameters; and (<b>c</b>) stance–swing phase transition moment parameters.</p>
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<p>Swing kinematic structure with parameters [<a href="#B48-machines-13-00020" class="html-bibr">48</a>].</p>
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<p>(<b>a</b>) Proposed single-DoF mechanism coarse representation; (<b>b</b>) proposed kinematic solution for single-DoF combined mechanism; (<b>c</b>) kinematic structure during stance phase; (<b>d</b>) kinematic structure during swing phase; (<b>e</b>) stance phase kinematic structure [<a href="#B48-machines-13-00020" class="html-bibr">48</a>]; and (<b>f</b>) swing phase kinematic structure.</p>
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<p>The procedural approach and comprehensive visualization of an example application: (<b>a</b>) Plane definition, precision points and transition moment on an average-sized leg to visualize their distribution on the sagittal plane; (<b>b</b>) Three precision points, their corresponding poses for the stance phase mechanism and the transition pose after the completion of the kinematic synthesis procedure; (<b>c</b>) The trajectory of ICR motion with corresponding <span class="html-italic">x</span> and <span class="html-italic">y</span> components represented as black dots on the sagittal plane, where the <span class="html-italic">r</span><sub>3</sub> link length varies linearly in moderate steps; (<b>d</b>) Mechanism’s overall dimensions relative to an average-sized leg in full extension; (<b>e</b>) Constructed and simulated combined mechanism by integrating the stance phase mechanism with the swing phase parameter <span class="html-italic">r</span><sub>4</sub>; (<b>f</b>) Mechanism’s overall dimensions relative to an average-sized leg in 120° flexion.</p>
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21 pages, 13930 KiB  
Article
A Lightweight CNN-Transformer Implemented via Structural Re-Parameterization and Hybrid Attention for Remote Sensing Image Super-Resolution
by Jie Wang, Hongwei Li, Yifan Li and Zilong Qin
ISPRS Int. J. Geo-Inf. 2025, 14(1), 8; https://doi.org/10.3390/ijgi14010008 - 30 Dec 2024
Viewed by 430
Abstract
Remote sensing imagery contains rich information about geographical targets, and performing super-resolution (SR) reconstruction on such images requires greater feature representation capabilities. Convolutional neural network (CNN)-based methods excel at extracting intricate local features but fall short in terms of capturing global representations. While [...] Read more.
Remote sensing imagery contains rich information about geographical targets, and performing super-resolution (SR) reconstruction on such images requires greater feature representation capabilities. Convolutional neural network (CNN)-based methods excel at extracting intricate local features but fall short in terms of capturing global representations. While transformer methods are capable of learning long-distance dependencies, they often overlook local feature details, which can diminish the discriminability between the background and the foreground. Moreover, the distinctive architectures of transformers, their extensive parameter counts, and their reliance on large-scale training datasets impose constraints on transformer applications in remote sensing image feature extraction tasks. To address these challenges, this study introduces a novel hybrid CNN-Transformer network model named RepCHAT for remote sensing single image reconstruction, which incorporates a structural re-parameterization technique and a hybrid attention mechanism. This method leverages the strengths of transformers in terms of learning long-distance dependencies (global features) and CNNs with respect to extracting local features. The proposed approach achieves SR reconstruction for remote sensing images with fewer parameters and less computational overhead than those of traditional transformers and high-performance CNN models. We develop a multiscale feature extraction module that integrates both spatial- and frequency-domain features and employs structural re-parameterization theory to increase the inference efficiency of the model. Furthermore, we incorporate depthwise-separable convolution into the transformer block to bolster the local feature learning capabilities of the transformer. The method we propose achieves the optimal performance for remote sensing single-image super-resolution reconstruction and outperforms the competing methods by 0.28–1.05 dB (×4 scale) in terms of signal-to-noise ratio (PSNR). Experimental results indicate that the RepCHAT model proposed in this study maintains a high performance with significantly reduced complexity, making it suitable for deployment on edge devices. Full article
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<p>Visualization of the intermediate layer feature maps derived from a CNN and a transformer based on the UC Merced Land Use dataset.</p>
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<p>The research progress in the field of deep learning-based remote sensing SR reconstruction methods.</p>
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<p>Overall architecture of the RepCHAT network.</p>
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<p>Channel attention block (CAB).</p>
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<p>Depthwise-separable MLP (DWMLP).</p>
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<p>SR reconstruction validation results produced using different methods on the UC Merced Land Use dataset.</p>
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<p>SR reconstruction validation results produced using different methods on the AID dataset.</p>
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12 pages, 2150 KiB  
Article
Effect of Depth Band Replacement on Red, Green and Blue Image for Deep Learning Weed Detection
by Jan Vandrol, Janis Perren and Adrian Koller
Sensors 2025, 25(1), 161; https://doi.org/10.3390/s25010161 - 30 Dec 2024
Viewed by 351
Abstract
Automated agricultural robots are becoming more common with the decreased cost of sensor devices and increased computational capabilities of single-board computers. Weeding is one of the mundane and repetitive tasks that robots could be used to perform. The detection of weeds in crops [...] Read more.
Automated agricultural robots are becoming more common with the decreased cost of sensor devices and increased computational capabilities of single-board computers. Weeding is one of the mundane and repetitive tasks that robots could be used to perform. The detection of weeds in crops is now common, and commercial solutions are entering the market rapidly. However, less work is carried out on combatting weeds in pastures. Weeds decrease the grazing yield of pastures and spread over time. Mowing the remaining weeds after grazing is not guaranteed to remove entrenched weeds. Periodic but selective cutting of weeds can be a solution to this problem. However, many weeds share similar textures and structures with grazing plants, making their detection difficult using the classic RGB (Red, Green, Blue) approach. Pixel depth estimation is considered a viable source of data for weed detection. However, systems utilizing RGBD (RGB plus Depth) are computationally expensive, making them nonviable for small, lightweight robots. Substituting one of the RGB bands with depth data could be a solution to this problem. In this study, we examined the effect of band substitution on the performance of lightweight YOLOv8 models using precision, recall and mAP50 metrics. Overall, the RDB band combination proved to be the best option for YOLOv8 small and medium detection models, with 0.621 and 0.634 mAP50 (for a mean average precision at 50% intersection over union) scores, respectively. In both instances, the classic RGB approach yielded lower accuracies of 0.574 and 0.613. Full article
(This article belongs to the Section Smart Agriculture)
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<p>Result of different substitutions of RGB channels with depth. Combinations are as follows: top left—RGB; top right—DGB; bottom left—RDB; bottom right—RGD.</p>
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<p>Precision–Recall Curve for v8n model.</p>
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<p>Precision–Recall Curve for v8s model.</p>
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<p>Precision-Recall Curve for v8m model.</p>
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13 pages, 2182 KiB  
Article
Electronically Coupled Heterojunctions Based on Graphene and Cu2−xS Nanocrystals: The Effect of the Surface Ligand
by Ju Y. Shang, Mariangela Giancaspro, Adriana Grandolfo, Rafique A. Lakho, Elisabetta Fanizza, Suraj K. Patel, Giuseppe Valerio Bianco, Marinella Striccoli, Chiara Ingrosso, Oscar Vazquez-Mena and M. Lucia Curri
Molecules 2025, 30(1), 67; https://doi.org/10.3390/molecules30010067 - 27 Dec 2024
Viewed by 487
Abstract
Optoelectronic devices combining single-layer graphene (SLG) and colloidal semiconducting nanocrystal (NC) heterojunctions have recently gained significant attention as efficient hybrid photodetectors. While most research has concentrated on systems using heavy metal-based semiconductor NCs, there is a need for further exploration of environmentally friendly [...] Read more.
Optoelectronic devices combining single-layer graphene (SLG) and colloidal semiconducting nanocrystal (NC) heterojunctions have recently gained significant attention as efficient hybrid photodetectors. While most research has concentrated on systems using heavy metal-based semiconductor NCs, there is a need for further exploration of environmentally friendly nanomaterials, such as Cu2−xS. Chemical ligands play a crucial role in these hybrid photodetectors, as they enable charge transfer between the NCs and SLG. This study investigates the photoresponse of an SLG/Cu2−xS NCs heterojunction, comparing the effect of two short molecules—tetrabutylammonium iodide (TBAI) and 3,4-dimethylbenzenethiol (DMBT)—as surface ligands on the resulting structures. We have analysed charge transfer at the heterojunctions between SLG and the Cu2−xS NCs before and after modification with TBAI and DMBT using Raman spectroscopy and transconductance measurements under thermal equilibrium. The photoresponse of two hybrid devices based on three layers of Cu2xS NCs, deposited in one case on SLG/Cu2−xS/TBAI (“TBAI-only” device) and in the other on SLG/Cu2−xS/DMBT (“DMBT + TBAI” device), with a TBAI treatment applied, for both, after each layer deposition, has been evaluated under 450 nm laser diode illumination. The results indicate that the TBAI-only device exhibited a significant increase in photocurrent (4 μA), with high responsivity (40 mA/W) and fast response times (<1 s), while the DMBT + TBAI device had lower photocurrent (0.2 μA) and responsivity (2.4 μA), despite similar response speeds. The difference is attributed to DMBT’s π–π interactions with SLG, which enhances electronic coupling but reduces SLG’s mobility and responsivity. Full article
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<p>Hybrid photodetector based on SLG, coated with a film of Cu<sub>2−x</sub>S NCs. The device is built on top of a SiO<sub>2</sub>/Si chip with gold contacts to apply voltage on the SLG. The device is illuminated from the top. The NCs absorb light and generate photocarriers that are transferred to SLG, increasing the number of carriers in SLG and inducing an increase in conductance.</p>
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<p>(<b>A</b>) TEM image, (<b>B</b>) UV-Vis-NIR absorption spectrum and (<b>C</b>) ATR-FTIR spectrum of Olam/OA-capped Cu<sub>2−x</sub>S NCs.</p>
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<p>(<b>A</b>) Chemical structure of tetrabutylammonium iodide (TBAI) and (<b>B</b>) 3,4-dimethylbenzenethiol (DMBT). (<b>C</b>) Raman spectra of SLG (black trace), SLG modified with the as-synthesised Olam/OA-Cu<sub>2−x</sub>S NCs (red trace: Cu<sub>2−x</sub>S), and after treatment with TBAI (blue trace: SLG/Cu<sub>2−x</sub>S/TBAI) and DMBT (pink trace: SLG/Cu<sub>2−x</sub>S/DMBT).</p>
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<p>(<b>A</b>,<b>B</b>) Sketches of the SLG/Cu<sub>2−x</sub>S heterojunctions with a single spin-coated layer of NCs treated by TBAI and DMBT. (<b>C</b>,<b>D</b>) Transconductance measurements (I<sub>SD</sub> vs. V<sub>G</sub>, V<sub>DS</sub> =0.04 V) of bare SLG (black curve), SLG after deposition of Olam/OA-Cu<sub>2−x</sub>S NCs (green curve), and after TBAI (red curve) and DMBT (blue curve) treatment, showing the shift in V<sub>DP</sub>. TBAI induces a negative shift to V<sub>DP</sub> = 8 V, while DMBT induces a larger shift to V<sub>DP</sub> = 2 V. (<b>E</b>,<b>G</b>) Proposed band diagrams showing the shifts in Fermi level (E<sub>F</sub>) of SLG before and after ligand treatment. Deposition of the Cu<sub>2−x</sub>NCs before (<b>E</b>) and after treatment with TBAI (<b>F</b>) and DMBT (<b>G</b>) induces an upper shift of E<sub>F</sub> towards the Dirac point but keeping SLG in a p-doped hole conduction state (below Dirac point).</p>
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<p>(<b>A</b>) TBAI-only photodetector based on four spin-coated layers of Cu<sub>2−x</sub>S NCs on SLG functionalised with TBAI molecules. (<b>B</b>,<b>C</b>) Photoresponse of the TBAI-only device under 0.1 Hz and 1 Hz light excitation, respectively. (<b>D</b>) Spectral response of TBAI-only devices showing strong photoresponse in the 400–1000 nm range for 0.1, 0.5 and 1 V<sub>DS</sub>. (<b>E</b>) DMBT + TBAI device is based also on four spin-coated layers of NCs but uses DMBT as a ligand for the first NC layer to improve coupling between NCs and SLG. (<b>F</b>,<b>G</b>) Photoresponse of DMBT + TBAI devices under 0.1 and 1 Hz light excitation. (<b>H</b>) DMBT + TBAI device showing strong photoresponse in the 400–1000 nm range for 0.1, 0.5 and 1 V<sub>DS</sub>.</p>
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12 pages, 5359 KiB  
Article
Electrical Characteristics of Solution-Based Thin-Film Transistors with a Zinc-Tin Oxide/Carbon Nanotube Stacked Nanocomposite Active Layer
by Yong-Jae Kim and Woon-Seop Choi
Nanomaterials 2025, 15(1), 22; https://doi.org/10.3390/nano15010022 - 27 Dec 2024
Viewed by 264
Abstract
A stacked nanocomposite zinc-tin oxide/single-walled carbon nanotubes (ZTO/SWNTs) active layer was fabricated for thin-film transistors (TFTs) as an alternative to the conventional single-layer structure of mixed ZTO and SWNTs. The stacked nanocomposite of the solution-processed TFTs was prepared using UV/O3 treatment and [...] Read more.
A stacked nanocomposite zinc-tin oxide/single-walled carbon nanotubes (ZTO/SWNTs) active layer was fabricated for thin-film transistors (TFTs) as an alternative to the conventional single-layer structure of mixed ZTO and SWNTs. The stacked nanocomposite of the solution-processed TFTs was prepared using UV/O3 treatment and multiple annealing steps for each layer. The electrical properties of the stacked device were superior to those of the single-layer TFT. The ZTO/SWNT TFT, fabricated using a stacked structure with ZTO on the top and SWNT at the bottom layer, showed a significant improvement in the field-effect mobility of 15.37 cm2/V·s (factor of three increase) and an Ion/Ioff current ratio of 8.83 × 108 with improved hysteresis. This outcome was attributed to the surface treatment and multiple annealing of the selected active layer, resulting in improved contact and a dense structure. This was also attributed to the controlled dispersion of SWNT, as electron migration paths without dispersants. This study suggests the potential expansion of applications, such as flexible electronics and low-cost fabrication of TFTs. Full article
(This article belongs to the Special Issue Nanoelectronics: Materials, Devices and Applications (Second Edition))
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<p>Schematic cross-section views of the bottom gate staggered structure for (<b>a</b>) sample A (ZTO only), (<b>b</b>) sample B (ZTO/SWNTs mixed), (<b>c</b>) sample C (Top SWNT bottom ZTO), (<b>d</b>) sample D (Top ZTO bottom SWNT). (S: Source, D: Drain).</p>
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<p>(<b>a</b>) Optical microscopy images of annealed sample C at various SWNT concentrations (0.01–0.07 wt.%), (<b>b</b>) Optical microscopy images of annealed sample D at various SWNT concentrations (0.01–0.07 wt.%).</p>
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<p>SEM images, mapping, and EDX elements of ZTO/SWNT film with 0.07 wt.% SWNTs concentration with a scale bar of 200 nm.</p>
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<p>Transmittance and absorption spectra of ZTO/SWNT thin films on glass with different SWNT concentrations.</p>
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<p>Resistivity of ZTO/SWNT thin films with different SWNT concentrations.</p>
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<p>Transfer characteristics and output characteristics of a SWNT/ZTO TFTs with 0.07 wt.% SWNT concentration. (<b>a</b>,<b>d</b>) sample A (ZTO only) (<b>b</b>,<b>e</b>) sample C (Top SWNT bottom ZTO) (<b>c</b>,<b>f</b>) sample D (Top ZTO bottom SWNT).</p>
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<p>(<b>a</b>) Field-effect mobility vs. SWNT concentration. (<b>b</b>) I<sub>on</sub>/I<sub>off</sub> current ratio vs. SWNTs concentration. (<b>c</b>) Vth vs. SWNT concentrations. (<b>d</b>) Off current vs. SWNT concentrations. All for the ZTO/SWNT nanocomposite TFTs.</p>
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<p>Hysteresis characteristics of a ZTO only and ZTO/SWNTs (0.07 wt.%) TFTs. (<b>a</b>) sample A (ZTO only), (<b>b</b>) sample B (ZTO/SWNTs mixed), (<b>c</b>) sample C (Top SWNTs bottom ZTO), (<b>d</b>) sample D (Top ZTO bottom SWNTs).</p>
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<p>Approach to a solution-based ZTO through a blend of SWNT as carrier transport rods to increase the electrical performance, (<b>a</b>) SWNT mixed ZTO TFT (<b>b</b>) top SWNTs bottom ZTO TFT (<b>c</b>) top ZTO bottom SWNTs TFT. (S: Source, D: Drain).</p>
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24 pages, 7562 KiB  
Article
Analysis and Design of Low-Power Piezoelectric Energy Harvesting Circuit for Wearable Battery-Free Power Supply Devices
by Ivaylo Pandiev, Hristo Antchev, Nikolay Kurtev, Nikolay Tomchev and Mariya Aleksandrova
Electronics 2025, 14(1), 46; https://doi.org/10.3390/electronics14010046 - 26 Dec 2024
Viewed by 359
Abstract
Improving microelectronic technologies has created various micro-power electronic devices with different practical applications, including wearable electronic modules and systems. Furthermore, the power sources for wearable electronic devices most often work with electrical energy obtained from the environment without using standard batteries. This paper [...] Read more.
Improving microelectronic technologies has created various micro-power electronic devices with different practical applications, including wearable electronic modules and systems. Furthermore, the power sources for wearable electronic devices most often work with electrical energy obtained from the environment without using standard batteries. This paper presents the structure and electrical parameters of a circuit configuration realized as a prototype of a low-power AC-DC conversion circuit intended for use as a power supply device for signal processing systems that test various biomedical parameters of the human body. The proposed prototype has to work as a wearable self-powered system that transfers electrical energy obtained through mechanical vibrations in the piezoelectric generator. The obtained electrical energy is used to charge a single low-voltage supercapacitor, which is used as an energy storage element. The proposed circuit configuration is realized with discrete components consisting of a low-voltage bridge rectifier, a low-pass filter, a DC-DC step-down (buck) synchronous converter, a power-controlling system with an error amplifier, and a window detector that produces a “power-good” signal. The power-controlling system allows tuning the output voltage level to around 1.8 V, and the power dissipation for it is less than 0.03 mW. The coefficient of energy efficiency achieved up to 78% for output power levels up to 3.6 mW. Experimental testing was conducted to verify the proposed AC-DC conversion circuit’s effectiveness, as the results confirmed the preliminary theoretical analyses and the derived analytical expressions for the primary electrical parameters. Full article
(This article belongs to the Special Issue Mixed Design of Integrated Circuits and Systems)
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<p>Functional diagram of the proposed circuit prototype.</p>
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<p>Schematic diagram of the proposed low-power energy-harvesting circuit.</p>
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<p>A detailed schematic of the input stage for the schematic diagram in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>—a full-bridge rectifier with an energy storage element: (<b>a</b>) schematic diagram; (<b>b</b>) typical signal waveforms of the input voltage <span class="html-italic">v<sub>p</sub></span> and the <math display="inline"><semantics> <mrow> <msub> <mi>i</mi> <mrow> <msub> <mi>C</mi> <mi>p</mi> </msub> </mrow> </msub> </mrow> </semantics></math> through the piezoelectric capacitance at resonance operational mode.</p>
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<p>An equivalent circuit of the pulse oscillator (or multivibrator), based on the multivibrator given as a part of the schematic diagram in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>.</p>
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<p>A configuration of the integrating circuit from the schematic diagram in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>.</p>
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<p>Signal waveforms of the input and output voltages for the proposed pulse-width modulator.</p>
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<p>A configuration of the error amplifier and compensator from the schematic diagram in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>.</p>
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<p>A configuration of the low-power driver stage for the synchronous converter from the schematic diagram in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>.</p>
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<p>Signal waveforms at the input and output voltages for the proposed low-power driver stage of the synchronous converter.</p>
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<p>A configuration of the window detector producing the “power-good” signal for the synchronous converter from the schematic diagram in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>.</p>
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<p>The low-power AC-DC converter construction prototype board: (<b>a</b>) variant 1 (top view); (<b>b</b>) variant 2 (top view).</p>
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<p>Captured waveforms from the experimental study (CH1: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>r</mi> </msub> </mrow> </semantics></math>, CH2: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>t</mi> <mi>r</mi> </mrow> </msub> </mrow> </semantics></math>, CH3: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>c</mi> <mi>o</mi> <mi>n</mi> <mi>t</mi> <mi>r</mi> <mi>o</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math>, and CH4: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>d</mi> </msub> </mrow> </semantics></math> in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>) at the no-load output (<span class="html-italic">R<sub>L</sub></span> → ∞).</p>
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<p>Captured waveforms from the experimental study (CH1: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>r</mi> </msub> </mrow> </semantics></math>, CH2: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>t</mi> <mi>r</mi> </mrow> </msub> </mrow> </semantics></math>, CH3: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>c</mi> <mi>o</mi> <mi>n</mi> <mi>t</mi> <mi>r</mi> <mi>o</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math>, and CH4: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>d</mi> </msub> </mrow> </semantics></math> in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>) at external load <span class="html-italic">R<sub>L</sub></span> = 3.6 kΩ.</p>
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<p>Captured waveforms from the experimental study (CH1: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>r</mi> </msub> </mrow> </semantics></math>, CH2: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>t</mi> <mi>r</mi> </mrow> </msub> </mrow> </semantics></math>, CH3: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>c</mi> <mi>o</mi> <mi>n</mi> <mi>t</mi> <mi>r</mi> <mi>o</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math>, and CH4: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>d</mi> </msub> </mrow> </semantics></math> in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>) at external load <span class="html-italic">R<sub>L</sub></span> = 1.8 kΩ.</p>
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<p>Captured waveforms from the experimental study (CH1: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>r</mi> </msub> </mrow> </semantics></math>, CH2: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>t</mi> <mi>r</mi> </mrow> </msub> </mrow> </semantics></math>, CH3: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>c</mi> <mi>o</mi> <mi>n</mi> <mi>t</mi> <mi>r</mi> <mi>o</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math>, and CH4: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>d</mi> </msub> </mrow> </semantics></math> in <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>) at external load <span class="html-italic">R<sub>L</sub></span> = 900 Ω.</p>
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<p>Captured waveforms for the pulse-width modulated signal <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>d</mi> </msub> </mrow> </semantics></math> (CH1), the non-overlapping pulse signals (<math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>T</mi> <mi>P</mi> <mn>3</mn> </mrow> </msub> </mrow> </semantics></math>(CH2) and <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>T</mi> <mi>P</mi> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math> (CH3)) at the gates of the <span class="html-italic">M</span><sub>2</sub> and <span class="html-italic">M</span><sub>1</sub> (see <a href="#electronics-14-00046-f002" class="html-fig">Figure 2</a>), and the level of the output voltage <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mi>o</mi> </msub> </mrow> </semantics></math> (CH4) from the experimental study at the no-load output.</p>
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<p>Start-up profile of the DC-DC converter circuit from the experimental study using an input sinusoidal generator with a low internal resistance at <math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mrow> <mi>S</mi> <mi>T</mi> <mi>O</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo> </mo> <mi mathvariant="normal">F</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>o</mi> </msub> <mo>=</mo> <mn>100</mn> <mo> </mo> <mo>μ</mo> <mi mathvariant="normal">F</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>L</mi> </msub> <mo>→</mo> <mo>∞</mo> </mrow> </semantics></math> (no-load output) (CH1: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>S</mi> <mi>T</mi> <mi>O</mi> </mrow> </msub> </mrow> </semantics></math> (a yellow curve), CH2: <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mi>o</mi> </msub> </mrow> </semantics></math> (a blue curve), and CH3: <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>P</mi> <mi>G</mi> <mi>O</mi> <mi>O</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> (a red curve)).</p>
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<p>Captured waveforms from the experimental study at an initial voltage of <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>T</mi> <mi>O</mi> </mrow> </msub> <mo>=</mo> <mn>1.5</mn> <mo> </mo> <mi mathvariant="normal">V</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mrow> <mi>S</mi> <mi>T</mi> <mi>O</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo> </mo> <mi mathvariant="normal">F</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>o</mi> </msub> <mo>=</mo> <mn>100</mn> <mo> </mo> <mo>μ</mo> <mi mathvariant="normal">F</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>L</mi> </msub> <mo>→</mo> <mo>∞</mo> </mrow> </semantics></math> (no-load output), and <math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>m</mi> </mrow> </msub> <mo>≈</mo> <mn>2</mn> <mi>mA</mi> </mrow> </semantics></math> (CH1: <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>S</mi> <mi>T</mi> <mi>O</mi> </mrow> </msub> </mrow> </semantics></math> (a yellow curve), CH2: <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mi>o</mi> </msub> </mrow> </semantics></math> (a blue curve), and CH3: <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>P</mi> <mi>G</mi> <mi>O</mi> <mi>O</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> (a red curve)).</p>
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<p>Measured overall electrical energy efficiency under various piezoelectric excitation levels <span class="html-italic">V<sub>p</sub></span><sub>,<span class="html-italic">m</span></sub> while the output voltage is <span class="html-italic">V<sub>o</sub></span> = 1.8 V.</p>
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11 pages, 2257 KiB  
Article
Pre-Melting-Assisted Impurity Control of β-Ga2O3 Single Crystals in Edge-Defined Film-Fed Growth
by A-Ran Shin, Tae-Hun Gu, Yun-Ji Shin, Seong-Min Jeong, Heesoo Lee and Si-Young Bae
Nanomaterials 2025, 15(1), 7; https://doi.org/10.3390/nano15010007 - 25 Dec 2024
Viewed by 277
Abstract
This study reveals the significant role of the pre-melting process in growing high-quality (100) β-Ga2O3 single crystals from 4N powder (99.995% purity) using the edge-defined film-fed growth (EFG) method. Among various bulk melt growth methods, the EFG method boasts a [...] Read more.
This study reveals the significant role of the pre-melting process in growing high-quality (100) β-Ga2O3 single crystals from 4N powder (99.995% purity) using the edge-defined film-fed growth (EFG) method. Among various bulk melt growth methods, the EFG method boasts a fast growth rate and the capability of growing multiple crystals simultaneously, thus offering high productivity. The pre-melting process notably enhanced the structural, optical, and electrical properties of the crystals by effectively eliminating impurities such as Si and Fe. Specifically, employing a 100% CO2 atmosphere during pre-melting proved to be highly effective, reducing impurity concentrations and carrier scattering, which resulted in a decreased carrier concentration and an increased electron mobility in the grown Ga2O3 single crystals. These results demonstrate that pre-melting is a crucial technique for substantially improving crystal quality, thereby promising better performance in β-Ga2O3-based device applications. Full article
(This article belongs to the Section Physical Chemistry at Nanoscale)
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<p>SEM images of (<b>a</b>) 4N and (<b>b</b>) 5N β-Ga<sub>2</sub>O<sub>3</sub> powders.</p>
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<p>GDMS analysis of impurity composition in 4N and 5N β-Ga<sub>2</sub>O<sub>3</sub> powders. Donor-like impurities (Sn, Si, Al, and Cr, marked in blue) and acceptor-like impurities (Fe, Mg, and Ca, marked in red) are identified.</p>
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<p>(<b>a</b>) XRD 2θ-scan spectra of (100) β-Ga<sub>2</sub>O<sub>3</sub> single crystals grown from 4N and 5N powders. (<b>b</b>) XRD omega-scan spectra for the (400) diffraction peak. (<b>c</b>) Impurity concentrations measured by GDMS for (100) β-Ga<sub>2</sub>O<sub>3</sub> grown from 4N and 5N powders.</p>
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<p>Impurity concentration of Ga<sub>2</sub>O<sub>3</sub> pre-melt after the power heating process with various CO<sub>2</sub> gas ratios (30–100%), measured by GDMS.</p>
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<p>(<b>a</b>) XRD 2θ-scan spectra of (100) β-Ga<sub>2</sub>O<sub>3</sub> single crystals grown with and without the pre-melting process. (<b>b</b>) XRD omega-scan spectra for the (400) diffraction peak. (<b>c</b>) Impurity concentrations measured by GDMS for (100) β-Ga<sub>2</sub>O<sub>3</sub> grown with and without the pre-melting process.</p>
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<p>(<b>a</b>) UV/vis transmittance spectra of β-Ga<sub>2</sub>O<sub>3</sub> single crystals grown with and without pre-melting and (<b>b</b>) the Tauc plot for determining the optical bandgap.</p>
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23 pages, 15584 KiB  
Article
Comparison of GFRP (Glass Fiber-Reinforced Polymer) and CFRP (Carbon Fiber-Reinforced Polymer) Composite Adhesive-Bonded Single-Lap Joints Used in Marine Environments
by Gurcan Atakok and Dudu Mertgenc Yoldas
Sustainability 2024, 16(24), 11105; https://doi.org/10.3390/su162411105 - 18 Dec 2024
Viewed by 589
Abstract
Macroscopic structures consisting of two or more materials are called composites. The decreasing reserves of the world’s oil reserve and the environmental pollution of existing energy and production resources made the use of recycling methods inevitable. There are mechanical, thermal, and chemical recycling [...] Read more.
Macroscopic structures consisting of two or more materials are called composites. The decreasing reserves of the world’s oil reserve and the environmental pollution of existing energy and production resources made the use of recycling methods inevitable. There are mechanical, thermal, and chemical recycling methods for the recycling of thermosets among composite materials. The recycling of thermoset composite materials economically saves resources and energy in the production of reinforcement and matrix materials. Due to the superior properties such as hardness, strength, lightness, corrosion resistance, design width, and the flexibility of epoxy/vinylester/polyester fibre formation composite materials combined with thermoset resin at the macro level, environmentally friendly sustainable development is happening with the increasing use of composite materials in many fields such as the maritime sector, space technology, wind energy, the manufacturing of medical devices, robot technology, the chemical industry, electrical electronic technology, the construction and building sector, the automotive sector, the defence industry, the aviation sector, the food and agriculture sector, and sports equipment manufacturing. Bonded joint studies in composite materials have generally been investigated at the level of a single composite material and single joint. The uncertainty of the long-term effects of different composite materials and environmental factors in single-lap bonded joints is an important obstacle in applications. The aim of this study is to investigate the effects of single-lap bonded GFRP (glass fibre-reinforced polymer) and CFRP (carbon fibre-reinforced polymer) specimens on the material at the end of seawater exposure. In this study, 0/90 orientation twill weave seven-ply GFRP and eight-ply CFRP composite materials were used in dry conditions (without seawater soaking) and the hand lay-up method. Seawater was taken from the Aegean Sea, İzmir province (Selçuk/Pamucak), in September at 23.5 °C. This seawater was kept in different containers in seawater for 1 month (30 days), 2 months (60 days), and 3 months (90 days) separately for GFRP and CFRP composite samples. They were cut according to ASTM D5868-01 for single-lap joint connections. Moisture retention percentages and axial impact tests were performed. Three-point bending tests were then performed according to ASTM D790. Damage to the material was examined with a ZEISS GEMINESEM 560 scanning electron microscope (SEM). The SEM was used to observe the interface properties and microstructure of the fracture surfaces of the composite samples by scanning images with a focused electron beam. Damage analysis imaging was performed on CFRP and GFRP specimens after sputtering with a gold compound. Moisture retention rates (%), axial impact tests, and three-point bending test specimens were kept in seawater with a seawater salinity of 3.3–3.7% and a seawater temperature of 23.5 °C for 1, 2, and 3 months. Moisture retention rates (%) are 0.66%, 3.43%, and 4.16% for GFRP single-lap bonded joints in a dry environment and joints kept for 1, 2, and 3 months, respectively. In CFRP single-lap bonded joints, it is 0.57%, 0.86%, and 0.87%, respectively. As a result of axial impact tests, under a 30 J impact energy level, the fracture toughness of GFRP single-lap bonded joints kept in a dry environment and seawater for 1, 2, and 3 months are 4.6%, 9.1%, 14.7%, and 11.23%, respectively. At the 30 J impact energy level, the fracture toughness values of CFRP single-lap bonded joints in a dry environment and in seawater for 1, 2, and 3 months were 4.2%, 5.3%, 6.4%, and 6.1%, respectively. As a result of three-point bending tests, GFRP single-lap joints showed a 5.94%, 8.90%, and 12.98% decrease in Young’s modulus compared to dry joints kept in seawater for 1, 2, and 3 months, respectively. CFRP single-lap joints showed that Young’s modulus decreased by 1.28%, 3.39%, and 3.74% compared to dry joints kept in seawater for 1, 2, and 3 months, respectively. Comparing the GFRP and CFRP specimens formed by a single-lap bonded connection, the moisture retention percentages of GFRP specimens and the amount of energy absorbed in axial impact tests increased with the soaking time in seawater, while Young’s modulus was less in three-point bending tests, indicating that CFRP specimens have better mechanical properties. Full article
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<p>Formation of specimens from GFRP (<b>a</b>) and CFRP (<b>b</b>) plates using CNC router (<b>c</b>). Geometry model of test specimens. (<b>d</b>) Preparation of specimens before bonding.</p>
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<p>CFRP (<b>a</b>) and GFRP (<b>b</b>) coded specimen samples.</p>
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<p>Axial impacts. (<b>a</b>) Schematic view; (<b>b</b>) impact test device with the specimen installed; (<b>c</b>) specimen subjected to impact.</p>
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<p>Positioning of the sample in the three-point bending testing machine.</p>
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<p>Dry environment, 1st, 2nd, and 3rd months. Moisture retention rate of samples for comparison of GFRP and CFRP.</p>
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<p>GFRP dry environment (<b>a</b>), 1st month (<b>b</b>), 2nd month (<b>c</b>), and 3rd month (<b>d</b>) specimens (axial impact).</p>
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<p>Absorbed energy amount graph of GFRP samples stored in dry environment and seawater for 1, 2, and 3 months.</p>
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<p>CFRP dry environment (<b>a</b>), 1st month (<b>b</b>), 2nd month (<b>c</b>), and 3rd month (<b>d</b>) specimens (axial impact).</p>
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<p>Comparing the absorbed energy of composite samples made of GFRP and CFRP.</p>
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<p>SEM image of GFRP composite material after axial impact test.</p>
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<p>SEM image of CFRP composite material after axial impact test.</p>
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<p>GFRP dry environment (<b>a</b>), 1st month (<b>b</b>), 2nd month (<b>c</b>), and 3rd month (<b>d</b>) specimens (three-point bending test).</p>
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<p>GFRP dry environment (<b>a</b>), 1st month (<b>b</b>), 2nd month (<b>c</b>), and 3rd month (<b>d</b>) specimens (three-point bending test).</p>
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<p>Stress–strain graph of GFRP specimens in dry environment and soaked in seawater for 1, 2, and 3 months.</p>
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<p>SEM image of GFRP composite material after three-point bending test.</p>
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<p>CFRP dry environment (<b>a</b>), 1st month (<b>b</b>), 2nd month (<b>c</b>), and 3rd month (<b>d</b>) specimens (three-point bending test).</p>
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<p>Bending stress–strain graph of CFRP specimens in dry environment and soaked in seawater for 1, 2, and 3 months.</p>
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<p>SEM image of CFRP composite material after three-point bending test.</p>
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20 pages, 7432 KiB  
Article
Simulation and Optimization of a Self-Cleaning Device for the Header of a Rice Seed Harvester Using Fluent–EDEM Coupling
by Yiren Qing, Lu Chen, Dongquan Chen, Peiyu Wang, Wenbin Sun and Ranbing Yang
Agriculture 2024, 14(12), 2312; https://doi.org/10.3390/agriculture14122312 - 17 Dec 2024
Viewed by 440
Abstract
Rice seed production is a critical step in breeding high-quality varieties. To ensure seed purity, it is essential that no residual grains or broken ears remain in the harvester header after harvesting each variety, thus preventing cross-contamination. This study addresses the issue of [...] Read more.
Rice seed production is a critical step in breeding high-quality varieties. To ensure seed purity, it is essential that no residual grains or broken ears remain in the harvester header after harvesting each variety, thus preventing cross-contamination. This study addresses the issue of seed retention in existing rice harvesters, which lack efficient self-cleaning or other cleaning mechanisms and cannot be cleaned rapidly. A self-cleaning device for the harvester header was designed to enable one-click cleaning after harvesting a single variety. A novel cleaning nozzle was developed as the key component of the device, with its structure optimized through single-factor and orthogonal combination experiments. The number of nozzles was determined based on their spray width and the header width. A header-cleaning airflow simulation model based on Fluent–EDEM coupling was constructed to investigate the effects of nozzle inlet pressure, airflow incident angle, and nozzle outlet height on the self-cleaning rate. Optimal cleaning parameters were identified to maximize the self-cleaning rate, and the simulation results were validated. The study revealed that the nozzle’s expansion section length, throat diameter, and contraction section length significantly affect the spray width. When the expansion section length was 10 mm, the throat diameter was 8 mm, and the contraction section length was 8 mm, the nozzle achieved the largest jet angle, measuring 50.3 cm. Further analysis indicated that inlet air pressure had the greatest influence on the self-cleaning rate, followed by airflow incident angle and nozzle outlet height. The optimal parameter combination was identified as an inlet air pressure of 0.6 Mpa, an airflow incident angle of 118.25°, and a nozzle outlet height of 2.64 mm, achieving a maximum self-cleaning rate of 99.63%. A one-click cleaning system was designed using an STM32 microcontroller and hardware circuits. Field experiments under optimal parameters demonstrated a self-cleaning rate of 97.68% with a cleaning duration of 10 s per cycle. The findings provide theoretical guidance for the design and optimization of self-cleaning headers for rice seed production. Full article
(This article belongs to the Section Agricultural Technology)
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<p>Schematic diagram of the hidden self-cleaning header device. 1. Dial wheel. 2. Aggregate bin cover. 3. Cutter. 4. Divider. 5. Aggregate bins. 6. Nozzle telescopic tube. 7. Auger with spiral conveyor.</p>
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<p>Schematic diagram of the key components of the header. 1. Electric actuators. 2. Aggregate bin floor. 3. Aggregate bin cover/header bottom plate. 4. Aggregate bin silo. 5. Rack-and-pinion drive. 6. Nozzle inner tube. 7. Nozzle. 8. DC motor.</p>
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<p>Schematic diagram of the working diagram and nozzle structure of the air flow cleaner. 1. Auger. 2. Nozzle. 3. Curved base plate. 4. Material. 5. Aggregate bin cover.</p>
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<p>Nozzle airflow contour fitting curve.</p>
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<p>Fluent pre-processing.</p>
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<p>Discrete element model of grain and panicle.</p>
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<p>Diagram of the hardware composition of the control system.</p>
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<p>Schematic diagram of the control system circuit.</p>
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<p>Control system flow diagram.</p>
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<p>Field validation experiment.</p>
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<p>Nozzle single-factor simulation results.</p>
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<p>Nozzle spray width.</p>
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<p>Simulated contour of header nozzle.</p>
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<p>Diagram of the results of the coupled simulation.</p>
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<p>Simulation results of different single factors on self-cleaning rate.</p>
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<p>Effect of interaction of factors on cleanliness. (<b>a</b>) The interaction effects of inlet air pressure and incident airflow angle on the self-cleaning rate when the nozzle outlet height is 2.6 mm. (<b>b</b>) The interaction effects of inlet air pressure and nozzle outlet height on the self-cleaning rate when the incident airflow angle is 118°. (<b>c</b>) The interaction effects of incident airflow angle and nozzle outlet height on the self-cleaning rate when the inlet air pressure is 0.5 Mpa.</p>
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<p>Renderings of the cleaning machine.</p>
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21 pages, 4915 KiB  
Review
A Review of Cascaded Metasurfaces for Advanced Integrated Devices
by Lingyun Zhang, Zeyu Zhao, Leying Tao, Yixiao Wang, Chi Zhang, Jianing Yang, Yongqiang Jiang, Huiqi Duan, Xiaoguang Zhao, Shaolong Chen and Zilun Wang
Micromachines 2024, 15(12), 1482; https://doi.org/10.3390/mi15121482 - 10 Dec 2024
Viewed by 824
Abstract
This paper reviews the field of cascaded metasurfaces, which are advanced optical devices formed by stacking or serially arranging multiple metasurface layers. These structures leverage near-field and far-field electromagnetic (EM) coupling mechanisms to enhance functionalities beyond single-layer metasurfaces. This review comprehensively discusses the [...] Read more.
This paper reviews the field of cascaded metasurfaces, which are advanced optical devices formed by stacking or serially arranging multiple metasurface layers. These structures leverage near-field and far-field electromagnetic (EM) coupling mechanisms to enhance functionalities beyond single-layer metasurfaces. This review comprehensively discusses the physical principles, design methodologies, and applications of cascaded metasurfaces, focusing on both static and dynamic configurations. Near-field-coupled structures create new resonant modes through strong EM interactions, allowing for efficient control of light properties like phase, polarization, and wave propagation. Far-field coupling, achieved through greater interlayer spacing, enables traditional optical methods for design, expanding applications to aberration correction, spectrometers, and retroreflectors. Dynamic configurations include tunable devices that adjust their optical characteristics through mechanical motion, making them valuable for applications in beam steering, varifocal lenses, and holography. This paper concludes with insights into the potential of cascaded metasurfaces to create multifunctional, compact optical systems, setting the stage for future innovations in miniaturized and integrated optical devices. Full article
(This article belongs to the Special Issue Terahertz and Infrared Metamaterial Devices, 3nd Edition)
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<p>Categories and applications of cascaded metasurfaces. Reproduced with permission. Copyright 2016, published by Springer Nature [<a href="#B63-micromachines-15-01482" class="html-bibr">63</a>]. Reproduced with permission. Copyright 2023, published by John Wiley and Sons [<a href="#B64-micromachines-15-01482" class="html-bibr">64</a>]. Reproduced with permission. Copyright 2021, published by American Chemical Society [<a href="#B65-micromachines-15-01482" class="html-bibr">65</a>]. Reproduced with permission. Copyright 2024, published by the Institute of Optics and Electronics [<a href="#B55-micromachines-15-01482" class="html-bibr">55</a>]. Reproduced with permission. Copyright 2018, published by Springer Nature [<a href="#B66-micromachines-15-01482" class="html-bibr">66</a>].</p>
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<p>(<b>a</b>) A generic structure consisting of four cascaded metasurfaces (electric sheet admittances) separated by dielectric layers. In general, the sheet admittances are anisotropic such that <span class="html-italic">x</span>- and <span class="html-italic">y</span>-polarized light can be controlled independently [<a href="#B68-micromachines-15-01482" class="html-bibr">68</a>]. (<b>b</b>) Broadband polarization conversion in reflection. Schematic (<b>left</b>) and microscopic image (<b>right</b>) of a metamaterial linear polarization converter [<a href="#B67-micromachines-15-01482" class="html-bibr">67</a>]. (<b>c</b>) Broadband polarization conversion in transmission. Schematic of the unit cell of the metamaterial linear polarization converter, in which a normally incident <span class="html-italic">x</span>-polarized wave is converted into a <span class="html-italic">y</span>-polarized one [<a href="#B67-micromachines-15-01482" class="html-bibr">67</a>]. (<b>d</b>) Schematic geometry of a twisted metamaterial. Each layer is rotated by a constant angle compared to its immediate neighbor. The transfer matrix of each twisted unit cell can be obtained by suitably rotating the transfer matrix of the first unit cell. A twisted unit cell consists of a propagation length <span class="html-italic">d</span> in free space and an ultrathin metasurface in the middle [<a href="#B72-micromachines-15-01482" class="html-bibr">72</a>]. (<b>e</b>) Schematic model of the cascaded metasurface device and its meta-atom design. The meta-atom consists of three functional structure layers that are a reflection layer, a filtering layer, and two transmission layers [<a href="#B73-micromachines-15-01482" class="html-bibr">73</a>]. (<b>a</b>) Reprinted/adapted with permission from Ref. [<a href="#B68-micromachines-15-01482" class="html-bibr">68</a>]. Copyright 2013, American Institute of Physics (AIP). (<b>b</b>) Reprinted/adapted with permission from Ref. [<a href="#B67-micromachines-15-01482" class="html-bibr">67</a>]. Copyright 2013, American Association for the Advancement of Science (AAAS). (<b>c</b>) Reprinted/adapted with permission from Ref. [<a href="#B67-micromachines-15-01482" class="html-bibr">67</a>]. Copyright 2013, American Association for the Advancement of Science (AAAS). (<b>d</b>) Reprinted/adapted with permission from Ref. [<a href="#B72-micromachines-15-01482" class="html-bibr">72</a>]. Copyright 2014, American Physical Society (APS). (<b>e</b>) Reprinted/adapted with permission from Refs. [<a href="#B67-micromachines-15-01482" class="html-bibr">67</a>,<a href="#B73-micromachines-15-01482" class="html-bibr">73</a>]. Copyright 2019, Optical Society of America (OSA).</p>
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<p>(<b>a</b>) Exploded view of tunable metamaterials (<b>upper left</b>). One unit cell of the tunable metamaterial, including BC-SRRs, where SRR1 is on a silicon frame and SRR2 is on a SiNx thin film (<b>upper right</b>). Simulated spectra of the individual uncoupled SRRs and broadside-coupled SRRs when <span class="html-italic">d</span> = 20 μm. (<b>lower left</b>) The surface charge distribution of the symmetric mode and antisymmetric mode of BC-SRRs (<b>lower right</b>) [<a href="#B75-micromachines-15-01482" class="html-bibr">75</a>]. (<b>b</b>) Tunable chiroptical properties of MCMs. SEM images (<b>Upper left</b>), measured and simulated CD spectra (<b>upper middle</b>), and schematic illustrations of three sets (i.e., −10° vs. 10°, −15° vs. 15°, and −20° vs. 20°, respectively) of MCMs (<b>upper right</b>). The scale bars are 1 µm. A series of CD spectra of an MCM under various rotation angles from 15° to 315° at an interval of 60°, a wheel illustration of the rotational periodicity (π/3) in the θ-dependent chiroptical properties of the MCMs, and a series of CD spectra of an MCM under the various lateral translations of the top layer of Au nanohole arrays in the <span class="html-italic">x</span> and <span class="html-italic">y</span> directions, respectively, from 0 to 500 nm with an interval of 100 nm (<b>Lower left to right</b>) [<a href="#B70-micromachines-15-01482" class="html-bibr">70</a>]. (<b>c</b>) Moiré metasurface in real space. Schematic illustration of a moiré metasurface (<b>upper</b>). The mutual twist of two closely attached metasurfaces produces a varying moiré pattern. Composition of a moiré metasurface from bottom to top: a metallic back plate, a spacer, and two closely stacked metasurface layers with a mutual twist (<b>lower</b>) [<a href="#B69-micromachines-15-01482" class="html-bibr">69</a>]. (<b>d</b>) Schematic of a bilayer metasurface stacked by two MMs with interlayer spacing <span class="html-italic">h</span> (<b>left</b>). <span class="html-italic">k</span> is the incident wavevector. Reflection (R) and transmission (T) spectra of the bilayer metasurface as a function of <span class="html-italic">h</span> (<b>right</b>). The insets correspond to the |<b><span class="html-italic">E</span></b>| distributions of points B and C, respectively [<a href="#B76-micromachines-15-01482" class="html-bibr">76</a>]. (<b>a</b>) Reprinted/adapted with permission from Ref. [<a href="#B75-micromachines-15-01482" class="html-bibr">75</a>]. Copyright 2016, Nature Publishing Group (NPG). (<b>b</b>) Reprinted/adapted with permission from Ref. [<a href="#B70-micromachines-15-01482" class="html-bibr">70</a>]. Copyright 2017, Wiley-VCH. (<b>c</b>) Reprinted/adapted with permission from Ref [<a href="#B69-micromachines-15-01482" class="html-bibr">69</a>]. Copyright 2022, American Association for the Advancement of Science (AAAS). (<b>d</b>) Reprinted/adapted with permission from Refs. [<a href="#B67-micromachines-15-01482" class="html-bibr">67</a>,<a href="#B76-micromachines-15-01482" class="html-bibr">76</a>]. Copyright 2022, Optical Society of America (OSA).</p>
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<p>(<b>a</b>) Schematic diagram of the metalens doublet [<a href="#B79-micromachines-15-01482" class="html-bibr">79</a>]. (<b>b</b>) Three-layer lens. (<b>left</b>) Artist’s view of the three-layer lens. When illuminated with white light, each layer focuses its designated part of the spectrum to a distance of 1 mm along the optical axis. (<b>right</b>) Schematic illustration of the layered structure. Each layer consists of nanodiscs with the following diameters D and separations l: DAu 1⁄4 125 nm, lAu 1⁄4 185 nm; DAg 1⁄4 85 nm, lAg 1⁄4 195 nm; DAl 1⁄4 120 nm, lAl 1⁄4 150 nm [<a href="#B86-micromachines-15-01482" class="html-bibr">86</a>]. (<b>c</b>) The multiwavelength metalens doublet (NA = 0.42) [<a href="#B84-micromachines-15-01482" class="html-bibr">84</a>]. (<b>d</b>) A monolithic planar retroreflector made of two metasurfaces. Schematic drawing of the planar retroreflector (<b>left</b>). Two metasurfaces are patterned on opposite sides of a glass substrate. Optical image of an array of retroreflectors (<b>right</b>) [<a href="#B80-micromachines-15-01482" class="html-bibr">80</a>]. (<b>e</b>) Illustrations of multiwavelength holograms (<b>upper</b>), multiwavelength waveplates (<b>central</b>), and 3D holograms (<b>lower</b>) using bilayer metasurfaces [<a href="#B87-micromachines-15-01482" class="html-bibr">87</a>]. (<b>f</b>) Working principle and inverse design realized with cascaded metasurfaces. A schematic of cascaded metasurfaces composed of numerous TiO2 nanorods (<b>upper</b>). Starting with a random phase, the optimization loop eventually converses with the target fields with a very small MSE (<b>lower</b>) [<a href="#B54-micromachines-15-01482" class="html-bibr">54</a>]. (<b>a</b>) Reproduced with permission from Ref. [<a href="#B79-micromachines-15-01482" class="html-bibr">79</a>]. Copyright 2017, Nano Lett. (<b>b</b>) Reproduced with permission from Ref. [<a href="#B86-micromachines-15-01482" class="html-bibr">86</a>]. Copyright 2017, Nat. Commun. (<b>c</b>) Reproduced with permission from Ref. [<a href="#B84-micromachines-15-01482" class="html-bibr">84</a>]. Copyright 2018, Nano Lett. (<b>d</b>) Reproduced with permission from Ref. [<a href="#B80-micromachines-15-01482" class="html-bibr">80</a>]. Copyright 2017, Nat. Photonics. (<b>e</b>) Reproduced with permission from Ref. [<a href="#B87-micromachines-15-01482" class="html-bibr">87</a>]. Copyright 2019, Light: Sci. Appl. (<b>f</b>) Reproduced with permission from Ref. [<a href="#B54-micromachines-15-01482" class="html-bibr">54</a>]. Copyright 2023, Nat. Commun.</p>
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<p>(<b>a</b>) Schematic of moiré metasurface operation [<a href="#B65-micromachines-15-01482" class="html-bibr">65</a>]. Reproduced with permission. Copyright 2021, American Chemical Society. (<b>b</b>) Three uniformly illuminated facial fluorescence images at different depths and processed with HiLo [<a href="#B65-micromachines-15-01482" class="html-bibr">65</a>]. (<b>c</b>) Schematic of the varifocal metalens based intelligent fluorescence endo-microscopy [<a href="#B105-micromachines-15-01482" class="html-bibr">105</a>]. Reproduced with permission. Copyright 2024, John Wiley and Sons. (<b>d</b>) Scheme of the zooming imaging doublet consisting of two metasurfaces. The focal length of the doublet changes continuously when varying the relative angle θ. For θ &gt; 0, the doublet works as a positive lens, and for θ &lt; 0, as a negative lens [<a href="#B106-micromachines-15-01482" class="html-bibr">106</a>]. Reproduced with permission. Copyright 2024, John Wiley and Sons. (<b>e</b>) Rotational multiplexing method for cascaded metasurface holography, adapted from Wei et al. [<a href="#B26-micromachines-15-01482" class="html-bibr">26</a>]. Reproduced with permission. Copyright 2024, John Wiley and Sons. (<b>f</b>) By rotating multiple metasurfaces, the focal spot can be dynamically controlled in both two-dimensional (2D) and three-dimensional (3D) spaces [<a href="#B102-micromachines-15-01482" class="html-bibr">102</a>]. Reproduced with permission. Copyright 2023, The American Association for the Advancement of Science.</p>
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<p>(<b>a</b>) SEM and optical images of a MEMS-actuated Alvarez metalens. The right side shows the actuated focal displacement and applied voltage over time. The general trend of the actuated displacement follows the square of the applied voltage [<a href="#B112-micromachines-15-01482" class="html-bibr">112</a>]. Reproduced with permission. Copyright 2020, Springer Nature. (<b>b</b>) Behavior of the Alvarez lens in response to x displacement, adapted from Zhan et al. [<a href="#B113-micromachines-15-01482" class="html-bibr">113</a>]. Plot of focal length dependence on displacement. Larger displacements result in a more rapidly varying phase profile, corresponding to a lens with a smaller focal length [<a href="#B113-micromachines-15-01482" class="html-bibr">113</a>]. Reproduced with permission. Copyright 2017, Springer Nature. (<b>c</b>) Schematics of the decentered microlens array-based BSS [<a href="#B119-micromachines-15-01482" class="html-bibr">119</a>]. Reproduced with permission. Copyright 2022, American Chemical Society. (<b>d</b>) Illustration of diffraction pattern switch by using cascaded metasurfaces, by moving one piece in the <span class="html-italic">x</span> or <span class="html-italic">y</span> direction, the corresponding diffraction orders can be switched [<a href="#B120-micromachines-15-01482" class="html-bibr">120</a>]. Reproduced with permission. Copyright 2024, John Wiley and Sons. (<b>e</b>) Schematic of the zoom metalens. Inset: detailed layout of the zoom metalens [<a href="#B121-micromachines-15-01482" class="html-bibr">121</a>]. Reproduced with permission. Copyright 2024, American Chemical Society. (<b>f</b>) Fabrication process summary and schematic illustration of the imaging setup using a regular glass lens and the tunable doublet. The image formed by the doublet is magnified and re-imaged using a custom-built microscope with a ×55 magnification onto an image sensor. A simplified fabrication process of a lens on a membrane (<b>left</b>), a simplified fabrication process of the lens on the glass substrate (<b>middle</b>), and schematics of the bonding process (<b>right</b>) [<a href="#B83-micromachines-15-01482" class="html-bibr">83</a>]. Reproduced with permission. Copyright 2018, American Chemical Society.</p>
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