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Search Results (1,357)

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27 pages, 10259 KiB  
Article
Innovative Seatbelt-Integrated Metasurface Radar for Enhanced In-Car Healthcare Monitoring
by Rifa Atul Izza Asyari, Roy B. V. B. Simorangkir and Daniel Teichmann
Sensors 2024, 24(23), 7494; https://doi.org/10.3390/s24237494 - 24 Nov 2024
Viewed by 393
Abstract
This study introduces a novel seatbelt-integrated, non-invasive, beam-focusing metamaterial sensing system characterized by its thinness and flexibility. The system comprises a flexible transmitarray lens and an FMCW radar sensor, enabling the accurate detection and analysis of seatbelt usage and positioning through human tissue. [...] Read more.
This study introduces a novel seatbelt-integrated, non-invasive, beam-focusing metamaterial sensing system characterized by its thinness and flexibility. The system comprises a flexible transmitarray lens and an FMCW radar sensor, enabling the accurate detection and analysis of seatbelt usage and positioning through human tissue. The metasurface design remains effective even when subjected to different bending angles. Our system closely tracks heart rate and respiration, validated against standard reference methods, highlighting its potential for enhancing in-car healthcare monitoring. Experimental results demonstrate the system’s reliability in monitoring physiological signals within dynamic vehicular environments. Full article
(This article belongs to the Special Issue Electromagnetic Sensors for Remote Patient Monitoring)
8 pages, 3953 KiB  
Article
Oblique Deposited Ultra-Thin Silver Films on Polymer Gratings for Sensitive SERS Performance
by Yi-Jun Jen and Meng-Jie Lin
Nanomaterials 2024, 14(23), 1871; https://doi.org/10.3390/nano14231871 - 22 Nov 2024
Viewed by 327
Abstract
A small amount of silver was obliquely deposited onto a polymer subwavelength grating to form a metasurface that comprised silver split-tubes. An ultra-thin silver film with a monitor-controlled thickness of 20 nm at the corner of each ridge of the grating provided the [...] Read more.
A small amount of silver was obliquely deposited onto a polymer subwavelength grating to form a metasurface that comprised silver split-tubes. An ultra-thin silver film with a monitor-controlled thickness of 20 nm at the corner of each ridge of the grating provided the most sensitive surface-enhanced Raman scattering (SERS) measurements. An excitation laser beam that was incident from the substrate provided similar or better SERS enhancement than did the general configuration with the laser beam incident directly on the surface of the nanostructure. Near-field simulations were conducted to model the localized electric field enhancement and to quantify the SERS performance, demonstrating the effectiveness of this novel deposition method. Full article
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<p>Top-view and cross-sectional SEM images of coated gratings: (<b>a</b>,<b>d</b>) GR<sub>20nm</sub><span class="html-italic">,</span> (<b>b</b>,<b>e</b>) GR<sub>80nm</sub><span class="html-italic">,</span> and (<b>c</b>,<b>f</b>) GR<sub>150nm</sub>; (<b>g</b>) schematic diagram of morphology of silver film.</p>
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<p>Measurement under forward and backward illumination in the transverse magnetic (TM) and transverse electric (TE) polarized state.</p>
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<p>TE and TM polarization spectra of reflectance (R), transmittance (T), and extinctance (E) for each sample under forward illumination.</p>
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<p>TE and TM polarization spectra of reflectance (R), transmittance (T), and extinctance (E) for each sample under backward illumination.</p>
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<p>Raman spectra of bare grating for forward and backward illumination.</p>
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<p>Raman spectra of GR<sub>20nm</sub>, GR<sub>80nm</sub>, and GR<sub>150nm</sub> for forward and backward illumination.</p>
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<p>AEF of bare grating, GR<sub>20nm</sub>, GR<sub>80nm</sub>, and GR<sub>150nm</sub> under forward illumination and backward illumination.</p>
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<p>Maximum steady-state amplitude of the electric field in grating substrate under forward and backward illumination.</p>
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13 pages, 7666 KiB  
Article
Polarization-Insensitive Metasurface with High-Gain Large-Angle Beam Deflection
by Huanran Qiu, Liang Fang, Rui Xi, Yajie Mu, Jiaqi Han, Qiang Feng, Ying Li, Long Li and Bin Zheng
Materials 2024, 17(23), 5688; https://doi.org/10.3390/ma17235688 - 21 Nov 2024
Viewed by 283
Abstract
Metasurfaces have shown great potential in achieving low-cost and low-complexity signal enhancement and redirection. Due to the low transmission power and high attenuation issues of current high-frequency communication technology, it is necessary to explore signal redirection technology based on metasurfaces. This paper presents [...] Read more.
Metasurfaces have shown great potential in achieving low-cost and low-complexity signal enhancement and redirection. Due to the low transmission power and high attenuation issues of current high-frequency communication technology, it is necessary to explore signal redirection technology based on metasurfaces. This paper presents an innovative metasurface for indoor signal enhancement and redirection, featuring thin thickness, high gain, and wide-angle deflection. The metasurface integrates the design principles of a Fabry–Perot cavity (FPC) theory with a Phase Gradient Partially Reflective Metasurface (PGPRM). Its unit is a fishnet structure with a substrate only 1/33 λ thin. Based on the precise phase control of the dual-layer PGPRM (with an inter-layer distance of 8 mm), the proposed metasurface can obtain phase coverage as small as 78° while achieving high-gain beam deflection as large as 47°. Simulation results show that within the band 8.6–9.2 GHz (6.7%), a single-layer metasurface can deflect the beam to 29° with a maximum gain of 16.9 dBi. In addition, it is also 360° polarization-insensitive in the xoy plane at 9 GHz with large-angle deflection characteristic retained. Moreover, cascading PGPRM can effectively improve the beam deflection angle. After analysis, the scheme with a double-layer spacing of 8 mm was ultimately selected. Simulation results show a double-layer metasurface can deflect the beam to 47° with a maximum gain of 16.4 dBi. This design provides an efficient and cost-effective solution for large-angle beam deflection with gain enhancement for indoor wireless communication. Full article
(This article belongs to the Special Issue Advances in Metamaterials: Structure, Properties and Applications)
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<p>Schematic diagram of the proposed PGPRM based on FPC theory.</p>
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<p>The schematic diagram of multiple reflections and deflection of electromagnetic waves.</p>
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<p>Infinite periodic model simulation of PGPRM. (<b>a</b>) Reflection phase and amplitude varying with frequency; (<b>b</b>) reflection phase and amplitude varying with the side length of the square aperture at 9 GHz; (<b>c</b>) polarization sensitivity analysis; (<b>d</b>) cross isolation analysis.</p>
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<p>Overall schematic diagram of PGPRM antenna. (<b>a</b>) Schematic diagram of <span class="html-italic">L</span>-shaped groove patch antenna; (<b>b</b>) schematic diagram of each layer of <span class="html-italic">L</span>-shaped groove patch antenna; (<b>c</b>) top view of PGPRM antenna; (<b>d</b>) side view of single-layer and double-layer PGPRM antenna.</p>
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<p>Comparison of simulation results between single-layer PGPRM antenna and double-layer PGPRM antenna. (<b>a</b>) Three-dimensional directional pattern of double-layer PGPRM antenna; (<b>b</b>) three-dimensional directional pattern of single-layer PGPRM antenna; (<b>c</b>) comparison of E-plane directional diagrams.</p>
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<p>Comparison of directional patterns of PGPRM antenna in the 8.6–9.2 GHz frequency band. (<b>a</b>) At 8.6, 8.7 GHz. (<b>b</b>) At 8.8, 8.9 GHz. (<b>c</b>) At 9.0, 9.1 GHz. (<b>d</b>) At 9.2 GHz.</p>
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<p>Comparison of directional patterns of PGPRM antenna in the 8.6–9.2 GHz frequency band. (<b>a</b>) At 8.6, 8.7 GHz. (<b>b</b>) At 8.8, 8.9 GHz. (<b>c</b>) At 9.0, 9.1 GHz. (<b>d</b>) At 9.2 GHz.</p>
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<p>The directional patterns of single-layer PGPRM antenna at different loading heights. (<b>a</b>) At 15 mm, half wavelength of 10 GHz. (<b>b</b>) At 13.6 mm, half wavelength of 11 GHz. (<b>c</b>) At 12.5 mm, half wavelength of 12 GHz. (<b>d</b>) At 11.5 mm, half wavelength of 13 GHz.</p>
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<p>The directional patterns of single-layer PGPRM antenna at different loading heights. (<b>a</b>) At 15 mm, half wavelength of 10 GHz. (<b>b</b>) At 13.6 mm, half wavelength of 11 GHz. (<b>c</b>) At 12.5 mm, half wavelength of 12 GHz. (<b>d</b>) At 11.5 mm, half wavelength of 13 GHz.</p>
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<p>Comparison of beam directions after rotating the single-layer PGPRM around <span class="html-italic">z</span>-axis. (<b>a</b>) 0°; (<b>b</b>) 90°; (<b>c</b>) 180°; (<b>d</b>) 270°.</p>
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<p>Electric field distribution before and after loading PGPRM. (<b>a</b>) Before loading PGPRM at 9 GHz; (<b>b</b>) after loading single-layer PGPRM at 9 GHz; (<b>c</b>) after loading double-layer PGPRM at 9 GHz; (<b>d</b>) surface electric field distribution of single-layer PGPRM antenna at 9 GHz; (<b>e</b>) surface electric field distribution of upper layer PGPRM in double-layer PGPRM antenna at 9 GHz.</p>
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13 pages, 1283 KiB  
Systematic Review
Dental Health in Children with Congenital Heart Defects: A Systematic Review and Meta-Analysis
by Carol Moussa, Guillaume Savard, Laurent Estrade, Rim Bourgi, Naji Kharouf, Frédéric Denis and Maha H. Daou
J. Clin. Med. 2024, 13(23), 7022; https://doi.org/10.3390/jcm13237022 - 21 Nov 2024
Viewed by 234
Abstract
Background: Oral health outcomes in children with Congenital Heart Defects (CHD) have significant implications. The aim of this systematic review and meta-analysis is to update the current understanding of oral health outcomes in children with CHD and compare caries prevalence between CHD children [...] Read more.
Background: Oral health outcomes in children with Congenital Heart Defects (CHD) have significant implications. The aim of this systematic review and meta-analysis is to update the current understanding of oral health outcomes in children with CHD and compare caries prevalence between CHD children and healthy controls. Methods: All studies between 2014 and 2024 comparing oral health status between children with and without CHD were considered for inclusion. Studies had to use the DMF/dmf index (Decayed, Missing, Filled Teeth or Surface index), in permanent and deciduous teeth. Two separate meta-analyses were conducted: one analyzing DMFS scores and another focusing on dmft scores. Medline, Central, and Embase databases were screened. Twelve articles were included in the qualitative synthesis, and two studies were finally included in each quantitative synthesis. Results: Several studies identified significant differences in oral health outcomes, suggesting that children with CHD are at a higher risk of dental caries compared with healthy controls, particularly as they become older. However, the differences were not uniformly observed across all studies and age groups. Based on the meta-analysis, there was no statistically significant difference in either DMFS scores (MD: 0.07 [95% CI: −0.13, 0.27]; p = 0.48) or in dmft scores (MD: 1.39 [95% CI: −1.05, 3.83]; p = 0.26). Conclusions: This systematic review and meta-analysis highlight a possible increased risk of dental caries in children with CHD, although results were not statistically significant and varied across studies. More standardized and rigorous studies are required to provide clearer insights into oral health outcomes for this population. Full article
(This article belongs to the Special Issue Oral Hygiene: Updates and Clinical Progress)
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<p>ROBINS-I assessment for the studies [<a href="#B7-jcm-13-07022" class="html-bibr">7</a>,<a href="#B14-jcm-13-07022" class="html-bibr">14</a>,<a href="#B15-jcm-13-07022" class="html-bibr">15</a>,<a href="#B16-jcm-13-07022" class="html-bibr">16</a>,<a href="#B17-jcm-13-07022" class="html-bibr">17</a>,<a href="#B18-jcm-13-07022" class="html-bibr">18</a>,<a href="#B19-jcm-13-07022" class="html-bibr">19</a>,<a href="#B20-jcm-13-07022" class="html-bibr">20</a>,<a href="#B21-jcm-13-07022" class="html-bibr">21</a>,<a href="#B22-jcm-13-07022" class="html-bibr">22</a>,<a href="#B23-jcm-13-07022" class="html-bibr">23</a>,<a href="#B24-jcm-13-07022" class="html-bibr">24</a>].</p>
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<p>Study flow diagram of inclusion process for articles selected.</p>
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<p>Forest plot of comparison of DMFS between children with CHD and healthy controls [<a href="#B17-jcm-13-07022" class="html-bibr">17</a>,<a href="#B18-jcm-13-07022" class="html-bibr">18</a>].</p>
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<p>Forest plot of the comparison of dmft between children with CHD and healthy controls [<a href="#B7-jcm-13-07022" class="html-bibr">7</a>,<a href="#B14-jcm-13-07022" class="html-bibr">14</a>].</p>
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10 pages, 5215 KiB  
Article
Enhancing Wireless Power Transfer Performance Based on a Digital Honeycomb Metamaterial Structure for Multiple Charging Locations
by Bui Huu Nguyen, Pham Thanh Son, Le Thi Hong Hiep, Nguyen Hai Anh, Do Khanh Tung, Bui Xuan Khuyen, Bui Son Tung, Vu Dinh Lam, Haiyu Zheng, Liangyao Chen and YoungPak Lee
Crystals 2024, 14(11), 999; https://doi.org/10.3390/cryst14110999 - 19 Nov 2024
Viewed by 278
Abstract
Enhancing the efficiency is an essential target of the wireless power transfer (WPT) technology. Enabling the WPT systems requires careful control to prevent power from being transferred to unintended areas. This is essential in improving the efficiency and minimizing the flux leakage that [...] Read more.
Enhancing the efficiency is an essential target of the wireless power transfer (WPT) technology. Enabling the WPT systems requires careful control to prevent power from being transferred to unintended areas. This is essential in improving the efficiency and minimizing the flux leakage that might otherwise occur. Selective field localization can effectively reduce the flux leakage from the WPT systems. In this work, we propose a method using a digital honeycomb metamaterial structure that has a property operation as a function of switching between 0 and 1 states. These cavities were created by strongly confining the field by using a hybridization bandgap that arose from wave interaction with a two-dimensional array of local resonators on the metasurface. A WPT efficiency of 64% at 13.56 MHz was achieved by using the metamaterial and improved to 60% compared to the system without the metamaterial with an area ratio of Rx:Tx~1:28. Rx is the receiver coil, and Tx is the transmitter one. Full article
(This article belongs to the Section Hybrid and Composite Crystalline Materials)
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<p>(<b>a</b>) Schematic of MM slab including 37 unit cells. (<b>b</b>) Top and bottom of the 5T-SR hexagonal unit cells. (<b>c</b>) Unit cell circuit model. (<b>d</b>) Reflection coefficient and (<b>e</b>) reflection phase of the unit cell at the ON (<span class="html-italic">C</span><sub>ON</sub> = 145.6 pF) and OFF states (<span class="html-italic">C</span><sub>OFF</sub> = 195.6 pF).</p>
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<p>Schematic of the WPT-MM system with control panel.</p>
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<p>The circuit model of the WPT-MM system.</p>
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<p>H-field intensity distribution (simulations with CST). (<b>a</b>) Free space and (<b>b</b>) metamaterial with a cavity.</p>
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<p>H-field intensity distribution in the x–y plane. (<b>a</b>) One unit cell ON. (<b>b</b>) Three unit cells ON. (<b>c</b>) Five unit cells ON.</p>
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<p>Experimental configuration for the proposed WPT-MM system.</p>
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<p>Comparison of the measurement and simulation results. (<b>a</b>) Transmission coefficient (<span class="html-italic">S</span><sub>21</sub>) and (<b>b</b>) PTE.</p>
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<p>Measured relative field amplitude via transmission coefficient. (<b>a</b>) One unit cell ON, (<b>b</b>) three unit cells ON, and (<b>c</b>) five unit cells ON.</p>
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14 pages, 1477 KiB  
Systematic Review
Hepatic Sinusoidal Obstruction Syndrome/Veno-Occlusive Disease (SOS/VOD) Primary Prophylaxis in Patients Undergoing Hematopoietic Stem Cell Transplantation: A Network Meta-Analysis of Randomized Controlled Trials
by Mário Sousa-Pimenta, Ângelo Martins, Letícia M. Estevinho, Carlos Pinho Vaz, Luís Leite and José Mariz
J. Clin. Med. 2024, 13(22), 6917; https://doi.org/10.3390/jcm13226917 - 17 Nov 2024
Viewed by 384
Abstract
Introduction: Hepatic sinusoidal obstruction syndrome/veno-occlusive disease (SOS/VOD) is a major complication following hematopoietic stem cell transplantation, resulting from immune and chemical toxicity in the sinusoidal endothelium and hepatocellular damage. In the most severe cases, multiorgan dysfunction occurs, so it is essential to promptly [...] Read more.
Introduction: Hepatic sinusoidal obstruction syndrome/veno-occlusive disease (SOS/VOD) is a major complication following hematopoietic stem cell transplantation, resulting from immune and chemical toxicity in the sinusoidal endothelium and hepatocellular damage. In the most severe cases, multiorgan dysfunction occurs, so it is essential to promptly identify patients at greater risk of SOS/VOD and to adopt prophylactic strategies. Objectives: This study aims to systematize the impact of different approaches as primary prophylaxes against SOS/VOD in patients undergoing hematopoietic stem cell transplantation (HSCT). Methods: A systematic review and meta-analysis of randomized clinical trials evaluating different strategies for primary prophylaxis of SOS/VOD was carried out in pairwise fashion and with a consistent network structure. The odds ratio (OR) and corresponding confidence intervals were calculated using the random-effects model. Heterogeneity was assessed by the I2 method and the efficacy of each approach was estimated by SUCRA (surface under the cumulative ranking curve). Results: Considering all patients undergoing HSCT, ursodeoxycholic acid (UDCA) [OR = 0.38, 95%CI 0.14–1.06, SUCRA = 0.720] was associated with a lower incidence of VOD while defibrotide reached a modest reduction in its incidence [OR = 0.64, 95%CI 0.23–1.67; SUCRA = 0.486]. Considering the subgroup of patients undergoing hematopoietic progenitors allotransplantation, defibrotide scored higher [OR = 0.51, 95%CI 0.09–2.85, SUCRA = 0.650] by comparison with UDCA [OR = 0.53, 95%CI 0.14–1.96, SUCRA = 0.639]. Conclusions: This is the first meta-analysis comparing primary prophylaxes against SOS/VOD. UDCA yielded more promising results when considering all patients undergoing hematopoietic stem cell transplantation, yet, in a subgroup analysis of the ones exposed to allogeneic grafts, it becomes not significantly overrun by defibrotide. Full article
(This article belongs to the Section Hematology)
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<p>Flowchart of data selection.</p>
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<p>Pooled analysis including all patients undergoing HSCT and enrolled in a clinical trial exploring the efficacy of a prophylactic regimen for SOS/VOD. (<b>A</b>)—pairwise meta-analysis addressing the direct comparisons included in the evidence; (<b>B</b>)—network analyzed under a consistency model; (<b>C</b>)—odds ratio of included interventions and 95% CI (effect of the column-defining intervention relative to the row-defining intervention); (<b>D</b>)—SUCRA plots; (<b>E</b>)—<span class="html-italic">rankogram</span> of prophylactic strategies.</p>
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<p>Pooled subgroup analysis including only patients undergoing allogeneic HSCT (both related and unrelated donors included) and enrolled in a randomized trial exploring the efficacy of a prophylactic regimen for SOS/VOD. (<b>A</b>)—pairwise meta-analysis addressing the direct comparisons included in the evidence; (<b>B</b>)—network analyzed under a consistency model; (<b>C</b>)—odds ratio of included interventions and 95% CI (effect of the column-defining intervention relative to the row-defining intervention); (<b>D</b>)—SUCRA plots; (<b>E</b>)—<span class="html-italic">rankogram</span> of prophylactic strategies.</p>
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11 pages, 2245 KiB  
Article
Metasurface-Based Image Classification Using Diffractive Deep Neural Network
by Kaiyang Cheng, Cong Deng, Fengyu Ye, Hongqiang Li, Fei Shen, Yuancheng Fan and Yubin Gong
Nanomaterials 2024, 14(22), 1812; https://doi.org/10.3390/nano14221812 - 12 Nov 2024
Viewed by 565
Abstract
The computer-assisted inverse design of photonic computing, especially by leveraging artificial intelligence algorithms, offers great convenience to accelerate the speed of development and improve calculation accuracy. However, traditional thickness-based modulation methods are hindered by large volume and difficult fabrication process, making it hard [...] Read more.
The computer-assisted inverse design of photonic computing, especially by leveraging artificial intelligence algorithms, offers great convenience to accelerate the speed of development and improve calculation accuracy. However, traditional thickness-based modulation methods are hindered by large volume and difficult fabrication process, making it hard to meet the data-driven requirements of flexible light modulation. Here, we propose a diffractive deep neural network (D2NN) framework based on a three-layer all-dielectric phased transmitarray as hidden layers, which can perform the classification of handwritten digits. By tailoring the radius of a silicon nanodisk of a meta-atom, the metasurface can realize the phase profile calculated by D2NN and maintain a relative high transmittance of 0.9 at a wavelength of 600 nm. The designed image classifier consists of three layers of phase-only metasurfaces, each of which contains 1024 units, mimicking a fully connected neural network through the diffraction of light fields. The classification task of handwriting digits from the ‘0’ to ‘5’ dataset is verified, with an accuracy of over 90% on the blind test dataset, as well as demonstrated by the full-wave simulation. Furthermore, the performance of the more complex animal image classification task is also validated by increasing the number of neurons to enhance the connectivity of the neural network. This study may provide a possible solution for practical applications such as biomedical detection, image processing, and machine vision based on all-optical computing. Full article
(This article belongs to the Special Issue Linear and Nonlinear Optical Properties of Nanomaterials)
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<p>Schematic diagram of the proposed image classifier. An incident plane wave passes through the input plane carrying the information of handwriting digits and undergoes three-layer phased transmitarray which provide layer-by-layer phase modulation with spacing of <span class="html-italic">d</span> = 6.5 μm. After propagating the entire system, light will be focused at a specific location of the output plane corresponding to different digits. From the light intensity distribution pattern, it can be inferred that the target being measured at this moment is the handwritten digit ‘2’.</p>
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<p>Numerical simulation results of D<sup>2</sup>NN. (<b>a</b>) Phase distribution of the hidden layers obtained by the training results of D<sup>2</sup>NN model. (<b>b</b>) Confusion matrix of the classification task on D<sup>2</sup>NN model in the final numerical simulation, achieving an overall accuracy of approximately 96.2% for six-class digit image classification. (<b>c</b>) The evolution of accuracy and loss value during the classification process with increasing the numbers of iteration.</p>
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<p>The geometry structure of unit cell of all-dielectric phased transmitarray. (<b>a</b>) Schematic diagram of a tunable transmissive meta-atom in an all-dielectric Huygens phase. Here, <span class="html-italic">H</span> = 180 nm, <span class="html-italic">h</span> = 350 nm, <span class="html-italic">p</span> = 360 nm. (<b>b</b>) A complete phase coverage from 0 to 2π for the cylinder with radius varies from 30 to 80 nm.</p>
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<p>Schematic diagram of electromagnetic simulation samples and results. (<b>a</b>–<b>f</b>) Selected simulation test sample images. (<b>g</b>–<b>l</b>) Light field distribution images of simulation output planes. (<b>m</b>–<b>r</b>) Energy distribution graphs within each numerical label area.</p>
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<p>Illustrative diagrams of numerical simulation results for animal image samples. (<b>a</b>) The original image of samples marked as “horse”, the converted grayscale image, the light field distribution on the detector plane through five diffraction layers, and the energy proportion within each marked area on the detector plane. (<b>b</b>) The original image of samples marked as “frog”, the converted grayscale image, and the light field distribution on the detector plane through five diffraction layers, and the energy proportion within each marked area on the detector plane.</p>
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15 pages, 3165 KiB  
Article
Comprehensive Analysis of Optical Resonances and Sensing Performance in Metasurfaces of Silicon Nanogap Unit
by Masanobu Iwanaga
Photonics 2024, 11(11), 1053; https://doi.org/10.3390/photonics11111053 - 10 Nov 2024
Viewed by 401
Abstract
Metasurfaces composed of silicon nanogap units have a variety of optical resonances, including bound states in the continuum (BIC). We show comprehensive numerical results on metasurfaces of Si-nanogap units, analyze the optical resonances, and clarify optically prominent resonances as well as symmetry-forbidding resonances [...] Read more.
Metasurfaces composed of silicon nanogap units have a variety of optical resonances, including bound states in the continuum (BIC). We show comprehensive numerical results on metasurfaces of Si-nanogap units, analyze the optical resonances, and clarify optically prominent resonances as well as symmetry-forbidding resonances that are the BIC, based on the numerical analyses of optical spectra and resonant electromagnetic field distributions. Introducing asymmetry in the unit cell, the BIC become optically allowed, being identified as magnetic dipole, electric quadrupole, and magnetic quadrupole resonances. Moreover, the optical resonances are examined in terms of refractive index sensing performance. A pair of the resonances associated with electric field localization at the nanogap was found to be sensitive to the refractive index in contact with the metasurfaces. Consequently, the gap mode resonances are shown to be suitable for a wide range of refractive index sensing over 1.0–2.0. Full article
(This article belongs to the Special Issue Editorial Board Members’ Collection Series: Photonics Sensors)
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<p>Schematics of metasurface structure and optical configuration in this study. (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math>-section view of unit cell of metasurface of Si-nanogap unit (purple). The gap <span class="html-italic">g</span> is indicated with a both-end arrow. The center line along the <span class="html-italic">x</span> axis is drawn with a broken line, which goes across the central point of the unit cell. (<b>b</b>) Asymmetry introduced in the unit cell is indicated by a quantity <math display="inline"><semantics> <mi>α</mi> </semantics></math>, which is offset from the center line (broken line) to the middle line (dotted line) in the gap. (<b>c</b>) Three-dimensional illustration of unit cell of metasurface of an asymmetric Si-nanogap pair. Optical configuration is shown together. The unit cells in (<b>a</b>–<b>c</b>) are set to have dimensions of <math display="inline"><semantics> <mrow> <mn>600</mn> <mo>×</mo> <mn>600</mn> </mrow> </semantics></math> nm<sup>2</sup> in the <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math> plane. Length of the Si nanoblock along the <span class="html-italic">x</span> axis is 400 nm and the sum of <math display="inline"><semantics> <mrow> <msub> <mi>y</mi> <mn>1</mn> </msub> <mo>+</mo> <msub> <mi>y</mi> <mn>2</mn> </msub> <mo>+</mo> <mi>g</mi> </mrow> </semantics></math> is 400 nm. Height of the Si nanoblock is set to 200 nm. (<b>d</b>) Three-dimensional illustration of a metasurface of periodic array of asymmetric Si-nanogap units, which are assumed to be infinitely periodic in the computations.</p>
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<p>Optical resonances emerged in the Si-nanogap unit metasurfaces. (<b>a</b>) Computed reflectance spectra at two incident polarizations, <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold">E</mi> <mi>in</mi> </msub> <mrow> <mo>‖</mo> <mi>x</mi> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold">E</mi> <mi>in</mi> </msub> <mrow> <mo>‖</mo> <mi>y</mi> </mrow> </mrow> </semantics></math> for various asymmetric parameters <math display="inline"><semantics> <mi>α</mi> </semantics></math>, defined in <a href="#photonics-11-01053-f001" class="html-fig">Figure 1</a>, and a fixed gap <span class="html-italic">g</span> of 50 nm. The reflectance spectra are shown with offset, changing color from black to blue for <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold">E</mi> <mi>in</mi> </msub> <mrow> <mo>‖</mo> <mi>x</mi> </mrow> </mrow> </semantics></math> and from red to brown for <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold">E</mi> <mi>in</mi> </msub> <mrow> <mo>‖</mo> <mi>y</mi> </mrow> </mrow> </semantics></math>, in accordance with <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>–25, respectively. EQ, MD, and MQ denote electric quadrupole, magnetic dipole, and magnetic quadrupole, respectively, indicated by arrows. (<b>b,c</b>) Asymmetric parameter <math display="inline"><semantics> <mi>α</mi> </semantics></math> and estimated quality (Q) factors of the MD (closed blue circles) and EQ modes (red diamonds), respectively. The Q factor is defined as Equation (<a href="#FD3-photonics-11-01053" class="html-disp-formula">3</a>). Black lines denote fitted lines using a power function (see the text).</p>
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<p>Resonant electromagnetic (EM)-field distributions on the qBIC resonances. (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math>-section view of <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">E</mi> <mo>|</mo> </mrow> </semantics></math> distribution at 1.272 eV. The <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math> axes are shown together and the <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math> sections were taken at the half height of the Si-nanogap pair. These settings are in common with the other panels in this figure. (<b>b</b>) Snapshot of <math display="inline"><semantics> <mrow> <mi>Re</mi> <mo>(</mo> <msub> <mi>E</mi> <mi>z</mi> </msub> <mo>)</mo> </mrow> </semantics></math> component, corresponding to (<b>a</b>), presents a signature of electric quadrupole (EQ) mode. (<b>c</b>) <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">H</mi> <mo>|</mo> </mrow> </semantics></math> distribution, corresponding to (<b>a</b>). The incident polarization was set to be <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold">E</mi> <mi>in</mi> </msub> <mrow> <mo>‖</mo> <mi>x</mi> </mrow> </mrow> </semantics></math> in (<b>a</b>–<b>c</b>). (<b>d</b>–<b>f</b>) <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">E</mi> <mo>|</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">H</mi> <mo>|</mo> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>Re</mi> <mo>(</mo> <msub> <mi>H</mi> <mi>z</mi> </msub> <mo>)</mo> </mrow> </semantics></math> distributions at 1.236 eV, respectively. The magnetic-field distribution shows a signature of magnetic dipole (MD) mode. (<b>g</b>–<b>i</b>) <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">E</mi> <mo>|</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">H</mi> <mo>|</mo> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>Re</mi> <mo>(</mo> <msub> <mi>H</mi> <mi>z</mi> </msub> <mo>)</mo> </mrow> </semantics></math> distributions at 1.402 eV, respectively. The magnetic-field distribution shows a signature of magnetic quadrupole (MQ) mode. The incident polarization was set to be <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold">E</mi> <mi>in</mi> </msub> <mrow> <mo>‖</mo> <mi>y</mi> </mrow> </mrow> </semantics></math> in (<b>d</b>–<b>i</b>). The color bars indicate values of resonantly enhanced EM fields, when the absolute values of incident fields were set to unity, that is, <math display="inline"><semantics> <mrow> <mrow> <mo>|</mo> </mrow> <msub> <mi mathvariant="bold">E</mi> <mi>in</mi> </msub> <mrow> <mo>|</mo> <mo>=</mo> <mn>1</mn> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>|</mo> </mrow> <msub> <mi mathvariant="bold">H</mi> <mi>in</mi> </msub> <mrow> <mo>|</mo> <mo>=</mo> <mn>1</mn> </mrow> </mrow> </semantics></math>.</p>
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<p>(<b>a</b>) Reflectance spectra dependent on refractive index <span class="html-italic">n</span> in the medium contacting the metasurface. Black and red curves show <span class="html-italic">x</span>- and <span class="html-italic">y</span>-polarized spectra, respectively, which are displayed with offset. Red arrows indicate a pair of resonances responsive to the index <span class="html-italic">n</span> over a wide range of <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>–2.0. (<b>b</b>) Resonance shift of the pair of resonances. The first and second ones are shown with closed and open red circles, respectively. The slopes, fitted using a linear function and shown with dashed black lines, approximating performance as optical sensors in the units of nm/RIU. See more details in the text. (<b>c</b>) Schematic of a <math display="inline"><semantics> <mrow> <mi>y</mi> <mi>z</mi> </mrow> </semantics></math>-section-view metasurface and medium of refractive index <span class="html-italic">n</span>. Dotted lines section the unit cell along the <span class="html-italic">y</span> axis.</p>
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<p>Resonant EM-field distributions on the two resonances responsive to surrounding refractive index, which is set to <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>1.5</mn> </mrow> </semantics></math>. (<b>a</b>,<b>b</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math>- and <math display="inline"><semantics> <mrow> <mi>y</mi> <mi>z</mi> </mrow> </semantics></math>-section views of <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">E</mi> <mo>|</mo> </mrow> </semantics></math> distributions, respectively. The <math display="inline"><semantics> <mrow> <mi>y</mi> <mi>z</mi> </mrow> </semantics></math> section cuts across the center of Si nanoblocks in the <span class="html-italic">x</span> direction. (<b>c</b>) <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">H</mi> <mo>|</mo> </mrow> </semantics></math> distribution in <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math>-section view. The photon energy is 1.124 eV in (<b>a</b>–<b>c</b>). (<b>d</b>–<b>f</b>) <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">E</mi> <mo>|</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">H</mi> <mo>|</mo> </mrow> </semantics></math> distributions at 1.167 eV, displayed in a similar manner to (<b>a</b>–<b>c</b>). The incident polarization was set to <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold">E</mi> <mi>in</mi> </msub> <mrow> <mo>‖</mo> <mi>y</mi> </mrow> </mrow> </semantics></math> in common. These <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math> sections are taken at the half-height of the Si-nanogap pair. The <math display="inline"><semantics> <mrow> <mi>y</mi> <mi>z</mi> </mrow> </semantics></math> sections are through the center of the unit cell.</p>
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<p>Optical resonances in an asymmetric metasurface of narrow gap <math display="inline"><semantics> <mrow> <mi>g</mi> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math> nm. (<b>a</b>) Reflectance spectra at <span class="html-italic">x</span> and <span class="html-italic">y</span> polarizations for refractive index <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>, shown with black and red curves, respectively. (<b>b</b>–<b>d</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math>-section views of <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">E</mi> <mo>|</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">H</mi> <mo>|</mo> </mrow> </semantics></math>, and snapshot of <math display="inline"><semantics> <mrow> <mi>Re</mi> <mo>(</mo> <msub> <mi>H</mi> <mi>z</mi> </msub> <mo>)</mo> </mrow> </semantics></math> at 1.178 eV, respectively. (<b>e</b>–<b>g</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math>-section views of <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">E</mi> <mo>|</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mo>|</mo> <mi mathvariant="bold">H</mi> <mo>|</mo> </mrow> </semantics></math>, and snapshot of <math display="inline"><semantics> <mrow> <mi>Re</mi> <mo>(</mo> <msub> <mi>H</mi> <mi>z</mi> </msub> <mo>)</mo> </mrow> </semantics></math> at 1.233 eV, respectively. The incident polarization was set to <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold">E</mi> <mi>in</mi> </msub> <mrow> <mo>‖</mo> <mi>y</mi> </mrow> </mrow> </semantics></math> in common. The <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math> sections were taken at the half-height of the Si-nanogap pair.</p>
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<p>Reflectance spectra of metasurface of a single symmetric Si-nanoblock unit. The spectra depend on refractive index <span class="html-italic">n</span>. (<b>a</b>) Unit cell in <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math>-section view. (<b>b</b>) Reflectance spectra dependent on refractive index <span class="html-italic">n</span> in the contacting medium. They are displayed with offset.</p>
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<p>Reflectance spectra of metasurface of symmetric Si-nanogap unit. The spectra depend on refractive index <span class="html-italic">n</span>. (<b>a</b>) Unit cell in <math display="inline"><semantics> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </semantics></math>-section view. (<b>b</b>) Reflectance spectra dependent on refractive index <span class="html-italic">n</span> in the contacting medium. Solid and dashed curves indicate <span class="html-italic">x</span>- and <span class="html-italic">y</span>-polarized spectra, respectively. They are displayed with offset.</p>
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14 pages, 1392 KiB  
Review
Comparative Efficacy of Different Pharmacological Treatments for Pityriasis Rosea: A Network Meta-Analysis
by Giulia Ciccarese, Antonio Facciorusso, Astrid Herzum, Cristian Fidanzi, Sebastiano Recalcati, Caterina Foti and Francesco Drago
J. Clin. Med. 2024, 13(22), 6666; https://doi.org/10.3390/jcm13226666 - 6 Nov 2024
Viewed by 521
Abstract
Background/Objectives: Pityriasis rosea (PR) is a self-limiting exanthematous disease associated with the endogenous reactivation of human herpesviruses (HHV)-6 and HHV-7. Classically, the lesions gradually resolve, leaving no sequelae. Therefore, the best treatment is reassuring the patient and suggesting a resting period. However, [...] Read more.
Background/Objectives: Pityriasis rosea (PR) is a self-limiting exanthematous disease associated with the endogenous reactivation of human herpesviruses (HHV)-6 and HHV-7. Classically, the lesions gradually resolve, leaving no sequelae. Therefore, the best treatment is reassuring the patient and suggesting a resting period. However, atypical PR cases characterized by extensive, persistent lesions and systemic symptoms may impact the patient’s quality of life, and, therefore, a treatment can be prescribed. There is limited evidence on the comparative effectiveness of pharmacological treatments for PR; therefore, we performed a network meta-analysis to compare these interventions. Methods: Overall, 12 randomized control trials (RCTs) were identified. The outcomes were itch resolution and rash improvement. Results were expressed as risk ratio (RR) and 95% confidence interval (CI). We also calculated the relative ranking of the interventions for achieving the aforementioned outcomes as their surface under the cumulative ranking (SUCRA). Results: On network meta-analysis, only oral steroids and the combination of oral steroids+antihistamine resulted significantly superior to the placebo in terms of itch resolution (RR 0.44, CI 0.27–0.72 and RR 0.47, CI 0.22–0.99). Oral steroids resulted in the best treatment (SUCRA 0.90) for itch resolution. In terms of rash improvement, only acyclovir and erythromycin resulted significantly superior to placebo (RR 2.55, CI 1.81–3.58; and RR 1.69, CI 1.23–2.33), and acyclovir outperformed all the other tested interventions. Consequently, acyclovir ranked as the best intervention (SUCRA score 0.92). Conclusions: Acyclovir represents the best option for patients with PR that have extensive, persistent lesions or systemic symptoms. Steroids and antihistamines seemed the best treatment for itch resolution. Full article
(This article belongs to the Special Issue New Insights into Infectious Skin and Mucosal Diseases)
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<p>Erythematous macular and papular scaly lesions of the trunk with a ‘theatre curtain’ distribution in a young man (<b>A</b>) and in woman (<b>B</b>) with PR.</p>
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<p>Flow chart of included studies.</p>
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<p>Network of included studies with comparisons between pharmacological treatments in inducing itch resolution (<b>a</b>) and rash improvement (<b>b</b>). The size of the nodes and the thickness of the edges are weighted based on the number of studies evaluating each intervention and direct comparison, respectively.</p>
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17 pages, 8028 KiB  
Review
Systematic Review and Meta-Analysis of Thermal Stress Assessment in Poultry Using Infrared Thermography in Specific Body Areas
by Roberto Carlos Hernández-Sánchez, Francisco Ernesto Martínez-Castañeda, Daniel Alonso Domínguez-Olvera, Maria Elena Trujillo-Ortega, Víctor Manuel Díaz-Sánchez, Ezequiel Sánchez-Ramírez, Elizabeth Posadas-Hernández, Itzayana Mejía-Flores and Elein Hernandez
Animals 2024, 14(22), 3171; https://doi.org/10.3390/ani14223171 - 6 Nov 2024
Viewed by 379
Abstract
Thermal stress is a health and welfare concern in the poultry industry. Poultry have specific thermoregulation strategies for heat stress (i.e., vasodilatation) or cold stress (i.e., vasoconstriction). Infrared thermal (IRT) analysis is a non-invasive temperature assessment technology with significant benefits compared to conventional [...] Read more.
Thermal stress is a health and welfare concern in the poultry industry. Poultry have specific thermoregulation strategies for heat stress (i.e., vasodilatation) or cold stress (i.e., vasoconstriction). Infrared thermal (IRT) analysis is a non-invasive temperature assessment technology with significant benefits compared to conventional temperature measurements, which are invasive and time-consuming. However, a wide range of IRT methodologies and equipment are used for temperature assessment in poultry. The aim of this study was to perform a systematic review and meta-analysis of IRT applications in poultry undergoing thermal stress. The bibliographic search yielded 17 records for qualitative synthesis and 10 for quantitative analysis. The results showed IRT is more commonly studied during heat stress than cold stress, and more research is being conducted on laying hens than other poultry species. Also, four body areas (parts of the head, body, face, and leg) were identified as common areas of interest for body surface temperature measurement. There is a clear thermoregulation response to thermal stress in poultry, with marked differences between featherless and feather-covered areas. IRT in poultry undergoing thermal stress has a good diagnostic value and represents an important welfare assessment tool for future research, particularly when combined with other welfare assessment methods. Full article
(This article belongs to the Section Veterinary Clinical Studies)
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<p>Keyword combination for article search.</p>
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<p>Literature funnel (PRISMA diagram).</p>
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<p>Mean difference in the parts of the head surface temperature of broiler chickens (B) and laying hens (LH) of different days of age (d) under heat stress. Effect size (SMD, Standard medium difference); SE (standard deviation of SMD) [<a href="#B2-animals-14-03171" class="html-bibr">2</a>,<a href="#B3-animals-14-03171" class="html-bibr">3</a>,<a href="#B6-animals-14-03171" class="html-bibr">6</a>,<a href="#B7-animals-14-03171" class="html-bibr">7</a>,<a href="#B12-animals-14-03171" class="html-bibr">12</a>,<a href="#B13-animals-14-03171" class="html-bibr">13</a>,<a href="#B22-animals-14-03171" class="html-bibr">22</a>].</p>
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<p>Mean difference in body surface temperature of broiler chickens (B) and laying hens (LH) of different days of age (d) under heat stress. Effect size (SMD, Standard medium difference); SE (standard deviation of SMD) [<a href="#B2-animals-14-03171" class="html-bibr">2</a>,<a href="#B3-animals-14-03171" class="html-bibr">3</a>,<a href="#B6-animals-14-03171" class="html-bibr">6</a>,<a href="#B9-animals-14-03171" class="html-bibr">9</a>,<a href="#B12-animals-14-03171" class="html-bibr">12</a>,<a href="#B13-animals-14-03171" class="html-bibr">13</a>,<a href="#B22-animals-14-03171" class="html-bibr">22</a>].</p>
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<p>Mean difference in face surface temperature of broiler chickens (B) and laying hens (LH) of different days of age (d) under heat stress. Effect size (SMD, Standard medium difference); SE (standard deviation of SMD) [<a href="#B2-animals-14-03171" class="html-bibr">2</a>,<a href="#B3-animals-14-03171" class="html-bibr">3</a>,<a href="#B6-animals-14-03171" class="html-bibr">6</a>,<a href="#B7-animals-14-03171" class="html-bibr">7</a>,<a href="#B22-animals-14-03171" class="html-bibr">22</a>].</p>
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<p>Mean difference in leg surface temperature of laying hens (LH) of different days of age (d) under heat stress. Effect size (SMD, Standard medium difference); SE (standard deviation of SMD) [<a href="#B2-animals-14-03171" class="html-bibr">2</a>,<a href="#B3-animals-14-03171" class="html-bibr">3</a>,<a href="#B12-animals-14-03171" class="html-bibr">12</a>,<a href="#B13-animals-14-03171" class="html-bibr">13</a>,<a href="#B22-animals-14-03171" class="html-bibr">22</a>].</p>
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<p>Mean difference in head parts surface temperature of turkeys (T) and laying hens (LH) of different days of age (d) under cold stress. Effect size (SMD, Standard medium difference); SE (standard deviation of SMD) [<a href="#B7-animals-14-03171" class="html-bibr">7</a>,<a href="#B11-animals-14-03171" class="html-bibr">11</a>,<a href="#B22-animals-14-03171" class="html-bibr">22</a>].</p>
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<p>Mean difference in body surface temperature of turkeys (T), broiler (B), and laying hens (LH) of different days of age (d) under cold stress. Effect size (SMD, Standard medium difference); SE (standard deviation of SMD) [<a href="#B9-animals-14-03171" class="html-bibr">9</a>,<a href="#B11-animals-14-03171" class="html-bibr">11</a>,<a href="#B14-animals-14-03171" class="html-bibr">14</a>,<a href="#B22-animals-14-03171" class="html-bibr">22</a>].</p>
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<p>Mean difference in face surface temperature of turkeys (T) and laying hens (LH) of different days of age (d) under cold stress. Effect size (SMD, Standard medium difference); SE (standard error of SMD) [<a href="#B7-animals-14-03171" class="html-bibr">7</a>,<a href="#B11-animals-14-03171" class="html-bibr">11</a>,<a href="#B22-animals-14-03171" class="html-bibr">22</a>].</p>
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<p>Mean difference in leg surface temperature of turkeys (T) and laying hens (LH) of different days of age (d) under cold stress. Effect size (SMD, Standard medium difference); SE (standard error of SMD) [<a href="#B11-animals-14-03171" class="html-bibr">11</a>,<a href="#B22-animals-14-03171" class="html-bibr">22</a>].</p>
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16 pages, 4785 KiB  
Article
Hyperspectral Inversion of Soil Cu Content in Agricultural Land Based on Continuous Wavelet Transform and Stacking Ensemble Learning
by Kai Yang, Fan Wu, Hongxu Guo, Dongbin Chen, Yirong Deng, Zaoquan Huang, Cunliang Han, Zhiliang Chen, Rongbo Xiao and Pengcheng Chen
Land 2024, 13(11), 1810; https://doi.org/10.3390/land13111810 - 1 Nov 2024
Viewed by 527
Abstract
Heavy metal pollution in agricultural land poses significant threats to both the ecological environment and human health. Therefore, the rapid and accurate prediction of heavy metal content in agricultural soil is crucial for environmental protection and soil remediation. Acknowledging the limitations of traditional [...] Read more.
Heavy metal pollution in agricultural land poses significant threats to both the ecological environment and human health. Therefore, the rapid and accurate prediction of heavy metal content in agricultural soil is crucial for environmental protection and soil remediation. Acknowledging the limitations of traditional single linear or nonlinear machine learning models in terms of prediction accuracy, this study developed an ensemble learning model that integrates multiple linear or nonlinear learning models with a random forest (RF) model to improve both the prediction accuracy and reliability. In this study, we selected a typical copper (Cu) polluted area in the Pearl River Delta of Guangdong Province as the research site and collected Cu content data and indoor soil reflectance spectral data from 269 surface soil samples. First, the soil spectral data were preprocessed using Savitzky–Golay (SG) smoothing, multiplicative scattering correction (MSC), and continuous wavelet transform (CWT) to reduce noise interference. Next, principal components analysis (PCA) was employed to reduce the dimensionality of the preprocessed spectral data, eliminating redundant features and lowering the computational complexity. Finally, based on the dimensionality-reduced data and Cu content, we established a stacked ensemble learning model, where the base models included SVR, PLSR, BPNN, and XGBoost, with RF serving as the meta-model to estimate the soil heavy metal content. To evaluate the performance of the stacking model, we compared its prediction accuracy with that of individual models. The results indicate that, compared to the traditional machine learning models, the prediction accuracy of the stacking model was superior (R2 = 0.77; RMSE = 7.65 mg/kg; RPD = 2.29). This suggests that the integrated algorithm demonstrates a greater robustness and generalization capability. This study presents a method to improve soil heavy metal content estimation using hyperspectral technology, ensuring a robust model that supports policymakers in making informed decisions about land use, agriculture, and environmental protection. Full article
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<p>Location of the study area and sampling distributions.</p>
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<p>Flowchart of Cu content estimation.</p>
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<p>Integrated learning algorithm construction in stacking.</p>
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<p>Original spectra.</p>
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<p>Soil reflectance spectral curves based on three spectral preprocessing methods (SG, MSC, CWT).</p>
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<p>Inversion accuracy results of PCA at each scale.</p>
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<p>Results of the optimal validation set of each model.</p>
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18 pages, 9682 KiB  
Article
Multifunctional Metasurface with PIN Diode Application Featuring Absorption, Polarization Conversion, and Transmission Functions
by Francisco D. M. Nobre, Thayana M. L. de Sousa, Antônio L. P. S. Campos and Maurício W. B. da Silva
Micromachines 2024, 15(11), 1344; https://doi.org/10.3390/mi15111344 - 31 Oct 2024
Viewed by 802
Abstract
The objective of this paper is to explore the potential of integrating three distinct functionalities into a thin, single-layer metasurface. Specifically, the study introduces a metasurface design that combines absorption, polarization conversion, and transmission capabilities. The proposed structure consists of a double square [...] Read more.
The objective of this paper is to explore the potential of integrating three distinct functionalities into a thin, single-layer metasurface. Specifically, the study introduces a metasurface design that combines absorption, polarization conversion, and transmission capabilities. The proposed structure consists of a double square loop disposed on a dielectric substrate, which is covered by a superstrate. In this study, the traditional ground plane was replaced with a periodic array, selectively reflecting frequencies of interest. Then, the absorption and polarization conversion characteristics were achieved by introducing the resonators in the front layer. By introducing asymmetry to the resonators and integrating PIN diodes for control, we demonstrated that the metasurface could efficiently absorb electromagnetic waves (with PIN diodes in the ON state), convert polarization (with PIN diodes in the OFF state), and enable signal transmission in a different frequency range. The numerical results indicated excellent performance in both absorption and polarization conversion. At a frequency of 3.05 GHz, the absorption rate reached 97%, while a polarization conversion rate of 98% was achieved at the resonance frequency of 4.37 GHz. Moreover, the proposed structure exhibited a thickness of λ/30.7 at the absorption peak. Full article
(This article belongs to the Special Issue Microwave Passive Components, 2nd Edition)
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<p>(<b>a</b>) Absorber unit cell, (<b>b</b>) ground plane view, (<b>c</b>) polarization converter unit cell, and (<b>d</b>) side view of the structure.</p>
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<p>Equivalent circuit of the PIN diode in the off and on states.</p>
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<p>Equivalent circuit of the unit cell.</p>
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<p>S parameters of the equivalent circuit.</p>
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<p>Boundary conditions of the 3D model.</p>
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<p>Absorptivity for TE polarization under normal incidence (<b>a</b>) and oblique incidence (<b>b</b>).</p>
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<p>Absorptivity for TM polarization under normal incidence (<b>a</b>) and oblique incidence (<b>b</b>).</p>
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<p>Simulation of reflection, transmission, and absorption of the proposed structure.</p>
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<p>Simulated surface current density for the proposed absorber showing in (<b>a</b>) the upper part of the unit cell and (<b>b</b>) the ground plane.</p>
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<p>Real and imaginary parts of the normalized input impedance (Z<sub><span class="html-italic">e</span><span class="html-italic">f</span><span class="html-italic">f</span></sub>).</p>
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<p>(<b>a</b>) Real and imaginary parts of the permeability <span class="html-italic">μ</span><sub><span class="html-italic">e</span><span class="html-italic">f</span><span class="html-italic">f</span></sub> and (<b>b</b>) real and imaginary of the effective permittivity <span class="html-italic">ϵ</span><sub><span class="html-italic">e</span><span class="html-italic">f</span><span class="html-italic">f</span></sub>.</p>
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<p>Comparison of absorptivity between an absorbing structure with substrate and superstrate with and without losses.</p>
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<p>Variation of absorptivity in relation to loss tangent.</p>
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<p>Electric field distribution in the proposed absorber, z-cut.</p>
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<p>Proposed structure with incident and reflected electric field decomposed into <span class="html-italic">u</span> and <span class="html-italic">v</span> for conversion of polarization <span class="html-italic">y</span> to <span class="html-italic">x</span>.</p>
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<p>Simulation of reflected amplitudes and phases for incident fields along the <span class="html-italic">u</span> and <span class="html-italic">v</span> axes.</p>
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<p>Simulated PCR of the bias converter designed under normal and oblique incidence of EM waves.</p>
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<p>Simulated surface current density for the proposed converter showing (<b>a</b>) the unit cell and (<b>b</b>) the ground plane.</p>
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<p>Electric field distribution in the polarization converter proposed, cut in z.</p>
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<p>Transmission versus frequency with variation in loss tangent.</p>
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<p>Transmission versus frequency with varying substrate thickness.</p>
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18 pages, 261925 KiB  
Article
Study of the Dispersion Compensation Double-Layer Diffractive Optical Components Based on Metasurface and Grating, and Their Application in Augmented Reality Displays
by Jiahang Zhang, Siqi Liu, Wei Zhang, Sijia Jiang, Ding Ma, Liang Xu, Mingyu Yang, Qingbin Jiao and Xin Tan
Materials 2024, 17(21), 5291; https://doi.org/10.3390/ma17215291 - 30 Oct 2024
Viewed by 446
Abstract
We employed a double-layer coupled diffractive optical element, based on metasurfaces and diffraction gratings, which exhibits wavefront modulation and chromatic dispersion compensation. Utilizing this double-layer coupled diffractive optical element in the optical information transmission process of a diffractive waveguide allows for the transmission [...] Read more.
We employed a double-layer coupled diffractive optical element, based on metasurfaces and diffraction gratings, which exhibits wavefront modulation and chromatic dispersion compensation. Utilizing this double-layer coupled diffractive optical element in the optical information transmission process of a diffractive waveguide allows for the transmission of color image information using a single-layer waveguide structure. Our results demonstrate that, under the conditions of a field of view of 47° × 47°, an entrance pupil size of 2.9 × 2.9 mm2, and an exit pupil extension size of 8.9 mm, the uniformity of the brightness for each monochromatic field reached 85%, while the uniformity of color transmission efficiency exceeded 95%. Full article
(This article belongs to the Section Materials Simulation and Design)
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<p>Diagram of the metasurface of double-layer coupled DOE: (<b>a</b>) metasurface cell structure; (<b>b</b>) light-shaping process of metasurface of the wavepropagation along z direction.</p>
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<p>Structure of metasurface cells for simulation in COMSOL with 1 representing the substate, 2 representing the pillar, and 3 representing the air cavity.</p>
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<p>Phase modulation of a metasurface cell with different pillar heights. (<b>a</b>) h = 300 nm (<b>b</b>) h = 400 nm (<b>c</b>) h = 500 nm (<b>d</b>) h = 600 nm (<b>e</b>) h = 700 nm (<b>f</b>) h = 800 nm.</p>
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<p>Workflow of multi-wavelength phase modulation metasurface design.</p>
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<p>Dispersion compensation double-layer diffractive optical component based on metasurface and grating (red, blue, green arrows represents the propagation direction of red, blue, green beams respectively, white arrows represents the propagation direction of red, blue, green beams are same): (<b>a</b>) forward light shaping process; (<b>b</b>) backward light shaping process [<a href="#B54-materials-17-05291" class="html-bibr">54</a>].</p>
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<p>Light propagation process in the x-domain in a metasurface-based double-layer diffractive waveguide with white arrow shows the propagation direction of beams [<a href="#B54-materials-17-05291" class="html-bibr">54</a>].</p>
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<p>Light propagation process in the k-domain in a metasurface-based double-layer diffractive waveguide [<a href="#B54-materials-17-05291" class="html-bibr">54</a>].</p>
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<p>Workflow of metasurface-based double-layer DOE design.</p>
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<p>In-coupling metasurface layer: (<b>a</b>) width of pillar size distribution with units given as nm; (<b>b</b>) local structure of metasurface at bottom left corner.</p>
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<p>Phase of field coupled by in-coupling double-layer diffractive optical elements: (<b>a</b>) λ = 450 nm; (<b>b</b>) λ = 532 nm; (<b>c</b>) λ = 632 nm.</p>
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<p>Out-coupling metasurface width of pillar size distribution with unit as nm. (<b>a</b>) first out-coupling (<b>b</b>) second out-coupling (<b>c</b>) third out-coupling.</p>
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<p>Phase of field coupled by three out-coupling double-layer diffractive optical elements: (<b>a</b>–<b>c</b>) λ = 450 nm; (<b>d</b>–<b>f</b>) λ = 532 nm; (<b>g</b>–<b>i</b>) λ = 632 nm.</p>
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<p>In-coupling light shaping results: (<b>a</b>–<b>c</b>) field propagation coupled with the metasurface for wavelengths of 450 nm, 532 nm, and 632 nm; (<b>d</b>–<b>f</b>) amplitude of the field coupled with the metasurface in the k-domain for wavelengths of 450 nm, 532 nm, and 632 nm; (<b>g</b>–<b>i</b>) amplitude of the field couped with the metasurface and grating in the k-domain for wavelengths of 450 nm, 532 nm, and 632 nm.</p>
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<p>Out-coupling light shaping results: (<b>a</b>–<b>c</b>) amplitude of field coupled with grating in the k-domain for wavelengths of 450 nm, 532 nm, and 632 nm; (<b>d</b>–<b>f</b>) field propagation coupled with the metasurface for wavelengths of 450 nm, 532 nm, and 632 nm; (<b>g</b>–<b>i</b>) amplitude of field couped with grating and metasurface in the k-domain for wavelengths of 450 nm, 532 nm, and 632 nm.</p>
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<p>Optical system of metasurface-based double-layer diffractive waveguide combiner for simulation: (<b>a</b>) wavelength of 450 nm; (<b>b</b>) wavelength of 532 nm; (<b>c</b>) wavelength of 632 nm.</p>
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<p>Field-tracing result of optical system: (<b>a</b>) wavelength of 450 nm; (<b>b</b>) wavelength of 532 nm; (<b>c</b>) wavelength of 632 nm.</p>
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11 pages, 3493 KiB  
Article
Enhanced Optical Bistability of a Metasurface Based on Asymmetrically Optimized Mirror-Induced Magnetic Anapole States
by Rui Xu, Sen Tian, Yujia Wen and Guoxiong Cai
Appl. Sci. 2024, 14(21), 9914; https://doi.org/10.3390/app14219914 - 29 Oct 2024
Viewed by 645
Abstract
In the field of modern optical computing and communication, optical bistability plays a crucial role. With a weak third-order nonlinear coefficient, low switch thresholds of optical bistability from Si-based nanophotonic structures remain a challenge. In this work, a metasurface consisting of silicon nanostrip [...] Read more.
In the field of modern optical computing and communication, optical bistability plays a crucial role. With a weak third-order nonlinear coefficient, low switch thresholds of optical bistability from Si-based nanophotonic structures remain a challenge. In this work, a metasurface consisting of silicon nanostrip arrays placed on the optically thick silver film is proposed. The light–matter interaction is enhanced by mirror-inducing the magnetic anapole states (MASs) and asymmetrically optimizing its silicon nanostrip. Numerical results show that the average enhancement factor (EF) of an electric field can be greatly enhanced to be 1524.8. Moreover, the optical bistability of the proposed metasurface achieves the thresholds of ION-OFF and IOFF-ON of 8.5 MW/cm2 and 7.1 MW/cm2, respectively, which is the lowest threshold when compared to the previous works based on silicon nanostructures. The angular dependance of the bistability performance is also investigated. This work facilitates the proposed hybrid metasurface in the fields of miniaturized all-optical switches and modulators, which are key components in optical computing and communication. Full article
(This article belongs to the Section Optics and Lasers)
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<p>Schematic diagram of the proposed mirror-induced MAS-based metasurfaces. Optical bistability originates from the silicon with third-order susceptibility. (<b>a</b>) Before asymmetrical optimization. Geometric parameters: length of silicon strip <span class="html-italic">L</span><sub>1</sub> = <span class="html-italic">L</span><sub>2</sub> = 250 nm, width <span class="html-italic">W</span><sub>1</sub> = <span class="html-italic">W</span><sub>2</sub> = 230 nm, height <span class="html-italic">H</span> = 360 nm, Ag film thickness <span class="html-italic">D</span> = 200 nm, and period <span class="html-italic">P</span> = 1500 nm. (<b>b</b>) After asymmetrical optimization. Geometric parameters: <span class="html-italic">L</span><sub>1</sub> = 190 nm, <span class="html-italic">W</span><sub>1</sub> = 210 nm, <span class="html-italic">H</span><sub>2</sub> = 120 nm, and <span class="html-italic">H</span><sub>1</sub> + <span class="html-italic">H</span><sub>2</sub> = <span class="html-italic">H</span>, while others remain unchanged as in (<b>a</b>).</p>
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<p>Physical mechanism of the metasurface based on mirror-induced MAS before asymmetric optimization. (<b>a</b>) The main figure presents the multipolar decomposition of the SCS spectrum of the silicon nanoribbon in the SOA structure. The inset shows a schematic diagram of the traditional MAS. (<b>b</b>) The main figure shows the multipolar decomposition of the SCS spectrum of the silicon part in SOM and the corresponding overall. The left inset is a schematic diagram of the mirror-induced MAS, and the right inset shows the multipolar decomposition of the SCS spectrum of the silicon nanoribbon in SOM.</p>
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<p>(<b>a</b>,<b>b</b>) Normalized field distributions for the conventional MAS and the mirror-induced MAS, respectively. Black arrows denote their current orientations inside silicon. (<b>c</b>) Average EF of silicon for these two scenarios.</p>
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<p>Average EF of the electric field by asymmetrically optimizing the proposed mirror-induced MAS-based metasurface. (<b>a</b>) Dependence on <span class="html-italic">L</span><sub>1</sub> and height duty ratio <span class="html-italic">H</span><sub>2</sub>/(<span class="html-italic">H</span><sub>1</sub> + <span class="html-italic">H</span><sub>2</sub>). <span class="html-italic">W</span><sub>1</sub> = 210 nm. (<b>b</b>) Dependence on <span class="html-italic">W</span><sub>1</sub> and <span class="html-italic">H</span><sub>2</sub>/(<span class="html-italic">H</span><sub>1</sub> + <span class="html-italic">H</span><sub>2</sub>). <span class="html-italic">L</span><sub>1</sub> =190 nm. Except when specified, parameters are the same as those in <a href="#applsci-14-09914-f001" class="html-fig">Figure 1</a>a.</p>
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<p>(<b>a</b>) Optical bistability of mirror-induced MAS metasurfaces. (<b>b</b>) Reflection spectra. The insets are the field distribution.</p>
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<p>(<b>a</b>) Nonlinear reflection spectra with increased incident light input intensity in the asymmetric device structure. (<b>b</b>) Nonlinear reflection spectra with reduced incident light input intensity in the same structure. The two dashed lines represent the resonant wavelength <span class="html-italic">λ</span><sub>res</sub> and the input wavelength <span class="html-italic">λ</span><sub>in</sub>, respectively.</p>
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<p>Dependences of switch thresholds on the incident angle.</p>
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14 pages, 5213 KiB  
Article
Numerical Verification of a Polarization-Insensitive Electrically Tunable Far Infrared Band-Stop Meta-Surface Filter
by Zheng Li, Yuying Lu, Yichi Han, Hanjie Li, Zhenqi Niu, Xiaomin Liu, Chaoyang Wei and Jianda Shao
Photonics 2024, 11(11), 1016; https://doi.org/10.3390/photonics11111016 - 29 Oct 2024
Viewed by 584
Abstract
Tunable filters have many potential applications in diverse fields, including high-capacity communications, dynamic beam shaping and spectral imaging. Although providing a high-performance solution for actively tunable devices, metasurface combined with tunable materials faces the great challenges of limited tuning range and modulation depth. [...] Read more.
Tunable filters have many potential applications in diverse fields, including high-capacity communications, dynamic beam shaping and spectral imaging. Although providing a high-performance solution for actively tunable devices, metasurface combined with tunable materials faces the great challenges of limited tuning range and modulation depth. Here, we propose a far-infrared tunable band-stop filter based on Fabry-Perot (FP) resonators and graphene surface plasmons. By switching the wavelength of the critical coupling condition of the filter via the gate voltage applied on graphene, achieving the dynamically tunable band-stop filtering at the central wavelengths from 12.4 μm to 14.1 μm with a modulation depth of more than 99%. Due to the symmetry of the proposed meta-atoms, the filter is insensitive to the polarization direction of the incident light. And it can realize more than 85% filtering efficiency within 60° angle of incidence around the vertical direction. By adjusting the geometry of the meta-atoms structure, it is feasible to move the operational range from the near-infrared to terahertz bands. Full article
(This article belongs to the Special Issue Plasmonics and Metamaterials)
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<p>Structure of the proposed tunable filter. (<b>a</b>) Overall view of the model; (<b>b</b>) One unit of the periodic structure; (<b>c</b>) Unit structure period P<sub>x</sub> = P<sub>y</sub> = 2 μm, length of gold <span class="html-italic">L</span><sub>1</sub> = 1900 nm, <span class="html-italic">L</span><sub>2</sub> = 1000 nm, width of gold <span class="html-italic">w</span>_<sub>Au</sub> = 100 nm, thickness of gold <span class="html-italic">d</span>_<sub>Au</sub> = 60 nm; (<b>d</b>) Side view of the filter, thickness of the Aluminum is 500 nm, thickness of the dielectric layer is 400 nm, <span class="html-italic">V<sub>g</sub></span> is the voltage between the Aluminum and the graphene metasurface.</p>
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<p>Filtering performance of tunable filter. (<b>a</b>) Refractive index and extinction coefficient of silicon dioxide in the infrared spectrum; (<b>b</b>) Graphene Fermi energy levels when the voltage is varied from 5 V to 30 V; (<b>c</b>,<b>d</b>) Simulated reflectance and absorptance of tunable filter at chemical potential of graphene increasing from 0.048 eV to 0.12 eV, respectively.</p>
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<p>Electric field distribution on graphene and metasurface at 13.3 μm for voltages of (<b>a</b>) 5 V, (<b>b</b>) 10 V, (<b>c</b>) 15 V, and (<b>d</b>) 20 V, respectively.</p>
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<p>Electric field distributions in the XY plane and XZ plane for different wavelengths at a voltage of 10 V. (<b>a</b>,<b>d</b>) Electric field distribution at 11.3 μm; (<b>b</b>,<b>e</b>) Electric field distribution at 13.3 μm; (<b>c</b>,<b>f</b>) Electric field distribution at 15.3 μm.</p>
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<p>(<b>a</b>) The change of reflection when the cell spacing is increased from 70 nm to 130 nm is simulated for a fixed period of 2 μm at a voltage of 10 V; (<b>b</b>) Schematic diagram of center wavelength and filtering efficiency versus cell spacing.</p>
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<p>(<b>a</b>) Reflection spectrum under different carrier mobility at <span class="html-italic">V<sub>g</sub></span> = 10 V; (<b>b</b>) Reflection spectrum under different thickness of graphene at <span class="html-italic">V<sub>g</sub></span> = 10 V.</p>
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<p>Filtering performance of the filter when the polarization direction of the incident wave is different. (<b>a</b>) Reflectivity of the filter when incident light is deflected from θ = 0° to θ = 180° with a step size of 30°; (<b>b</b>–<b>e</b>) The electric field distribution on the filter surface for θ is 0°, 30°, 60° and 90°, θ is the angle between the polarization direction of the light and the direction of the <span class="html-italic">x</span>-axis as shown in the insets in (<b>a</b>).</p>
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<p>Effect of incident angle on filtering efficiency. (<b>a</b>) Variation of filtering efficiency when the incident angle <span class="html-italic">α</span> varies from 0° to 85°; (<b>b</b>) Distribution of the electric field in the XY plane when the light is incident vertically; (<b>c</b>) Distribution of the electric field on the surface when the incident angle is 60°; (<b>d</b>) Distribution of the electric field on the surface when the incident angle is 85°.</p>
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<p>Influence of fabrication errors of the main parameters of the model structure on the tunable filtering performance. (<b>a</b>,<b>b</b>) Main parameters of the filter model; (<b>c</b>) Filtering with different <span class="html-italic">L</span><sub>2</sub> (900–1100 nm) at 10 V; (<b>d</b>) Schematic diagram of the center wavelength and the filtering efficiency versus <span class="html-italic">L</span><sub>2</sub>; (<b>e</b>) Filtering with different widths of gold (90–110 nm) at 10 V; (<b>f</b>) Schematic diagram of the center wavelength and the filtering efficiency versus gold width.</p>
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<p>Influence of fabrication errors of the main parameters of the model structure on the filtering performance. (<b>a</b>) Filtering at different thicknesses of gold (50–70 nm); (<b>b</b>) Schematic diagram of the center wavelength and filtering efficiency versus the thickness of gold; (<b>c</b>) Filtering at different thicknesses of silicon dioxide (360–440 nm); (<b>d</b>) Schematic diagram of the center wavelength and filtering efficiency versus the thickness of silicon dioxide.</p>
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