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Search Results (224)

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11 pages, 1995 KiB  
Article
Angle-Tunable Method for Optimizing Rear Reflectance in Fabry–Perot Interferometers and Its Application in Fiber-Optic Ultrasound Sensing
by Yufei Chu, Mohammed Alshammari, Xiaoli Wang and Ming Han
Photonics 2024, 11(12), 1100; https://doi.org/10.3390/photonics11121100 - 21 Nov 2024
Abstract
With the introduction of advanced Fiber Bragg Grating (FBG) technology, Fabry–Pérot (FP) interferometers have become widely used in fiber-optic ultrasound detection. In these applications, the slope of the reflectance is a critical factor influencing detection results. Due to the intensity limitations of the [...] Read more.
With the introduction of advanced Fiber Bragg Grating (FBG) technology, Fabry–Pérot (FP) interferometers have become widely used in fiber-optic ultrasound detection. In these applications, the slope of the reflectance is a critical factor influencing detection results. Due to the intensity limitations of the laser source in fiber-optic ultrasound detection, the reflectance of the FBG is generally increased to enhance the signal-to-noise ratio (SNR). However, increasing reflectance can cause the reflectance curve to deviate from a sinusoidal shape, which in turn affects the slope of the reflectance and introduces greater errors. This paper first investigates the relationship between the transmission curve of the FP interferometer and reflectance, with a focus on the errors introduced by simplified assumptions. Further research shows that in sensors with asymmetric reflectance slopes, their transmittance curves deviate significantly from sinusoidal signals. This discrepancy highlights the importance of achieving symmetrical slopes to ensure consistent and accurate detection. To address this issue, this paper proposes an innovative method to adjust the rear-end reflectance of the FP interferometer by combining stress modulation, UV adhesive, and a high-reflectivity metal disk. Additionally, by adjusting the rear-end reflectance to ensure that the transmittance curve approximates a sinusoidal signal, the symmetry of the slope is maintained. Finally, through practical ultrasound testing, by adjusting the incident wavelength to the positions of slope extrema (or zero) at equal intervals, the expected ultrasound signals at extrema (or zero) can be detected. This method converts the problem of approximating a sinusoidal signal into a problem of the slope adjustment of the transmittance curve, making it easier and more direct to determine its impact on detection results. The proposed method not only improves the performance of fiber-optic ultrasound sensors but also reduces costs, paving the way for broader applications in medical diagnostics and structural health monitoring. Full article
(This article belongs to the Special Issue Optical Sensing Technologies, Devices and Their Data Applications)
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<p>The schematic diagram of the FP transmittance curve.</p>
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<p>Variation of error due to assumptions in FP reflectivity changes.</p>
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<p>The variation in the slope due to the FP reflectivity changes. (<b>a</b>) The reflectivity of the front and rear ends is equal; (<b>b</b>) the reflectivity of the front end is fixed at 10%, and only the reflectivity of the rear end is changed; the solid line is the reflectivity; the dotted line is the slope of the normalized reflectivity. In the legend, “S” represents the slope.</p>
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<p>The angle adjustment of end−face reflectivity based on UV Glue. (<b>a</b>) The slope of the reflectivity is asymmetric; (<b>b</b>) the slope of the reflectivity is symmetric (the green points labeled a, b, c, and d correspond to the positions where the slope is at a minimum, zero, maximum, and zero, respectively).</p>
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<p>Angle symmetry testing setup and results for the ultrasound sensor: (<b>a</b>) ultrasound detection setup (the structure diagram of the FP sensor is shown within the black dashed line), (<b>b</b>−<b>e</b>) show the ultrasound detection results when the laser wavelength is adjusted to operating points a, b, c, and d in <a href="#photonics-11-01100-f004" class="html-fig">Figure 4</a>b, respectively.</p>
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13 pages, 5282 KiB  
Article
Parallel Farby–Perot Interferometers in an Etched Multicore Fiber for Vector Bending Measurements
by Kang Wang, Wei Ji, Cong Xiong, Caoyuan Wang, Yu Qin, Yichun Shen and Limin Xiao
Micromachines 2024, 15(12), 1406; https://doi.org/10.3390/mi15121406 - 21 Nov 2024
Abstract
Vector bending sensors can be utilized to detect the bending curvature and direction, which is essential for various applications such as structural health monitoring, mechanical deformation measurement, and shape sensing. In this work, we demonstrate a temperature-insensitive vector bending sensor via parallel Farby–Perot [...] Read more.
Vector bending sensors can be utilized to detect the bending curvature and direction, which is essential for various applications such as structural health monitoring, mechanical deformation measurement, and shape sensing. In this work, we demonstrate a temperature-insensitive vector bending sensor via parallel Farby–Perot interferometers (FPIs) fabricated by etching and splicing a multicore fiber (MCF). The parallel FPIs made in this simple and effective way exhibit significant interferometric visibility with a fringe contrast over 20 dB in the reflection spectra, which is 6 dB larger than the previous MCF-based FPIs. And such a device exhibits a curvature sensitivity of 0.207 nm/m−1 with strong bending-direction discrimination. The curvature magnitude and orientation angle can be reconstructed through the dip wavelength shifts in two off-diagonal outer-core FPIs. The reconstruction results of nine randomly selected pairs of bending magnitudes and directions show that the average relative error of magnitude is ~4.5%, and the average absolute error of orientation angle is less than 2.0°. Furthermore, the proposed bending sensor is temperature-insensitive, with temperature at a lower sensitivity than 10 pm/°C. The fabrication simplicity, high interferometric visibility, compactness, and temperature insensitivity of the device may accelerate MCF-based FPI applications. Full article
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<p>(<b>a</b>) Schematic of the proposed vector bending sensor, composed of seven parallel FPIs fabricated inside the MCF. (<b>b</b>) The cross-section of the MCF shows the reference direction, bending direction, and directions of the FPIs.</p>
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<p>The principle of bending measurement. (<b>a</b>) Optical fiber is in a straight state. (<b>b</b>) The fiber is bent when the left terminal moves down a distance <span class="html-italic">δ</span> from its original position. The images on the right are the transversal section of a small section of fiber (∆<span class="html-italic">L</span><sub>0</sub>), respectively, in a straight and bent scenario.</p>
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<p>(<b>a</b>) The wavelength shifts of FPI<sub>2</sub> as functions of curvature when <span class="html-italic">θ</span> = 0°, <span class="html-italic">θ</span> = 90° and <span class="html-italic">θ</span> = 180°, respectively. (<b>b</b>) The curvature sensitivities of FPI<sub>2</sub>, FPI<sub>4</sub>, and FPI<sub>6</sub> as functions of the fiber orientation in cartesian coordinates.</p>
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<p>The device fabrication process. (<b>a</b>) A piece of MCF was cut to obtain the flat fiber end facet. (<b>b</b>) The cross-section of the MCF. (<b>c</b>) The flat cleaved fiber tip was exposed to 20% hydrofluoric acid (HF) at 25 °C. (<b>d</b>–<b>g</b>) The etched facets over different etching times. (<b>h</b>) Two sections of MCFs with etched facets were spliced together. (<b>i</b>,<b>j</b>) The spliced joint focused on the central core and side cores.</p>
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<p>The alignment system. (<b>a</b>) The Setup. (<b>b</b>) A reference fiber angular position. (<b>c</b>) The red-light spot is just below the green-light spot.</p>
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<p>Schematic of interrogation system.</p>
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<p>The reflection spectra of FPI<sub>2</sub>, FPI<sub>4</sub>, FPI<sub>6</sub>, and FPI<sub>7</sub>.</p>
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<p>(<b>a</b>) The reflection spectrum of FPI<sub>2</sub> and the third-order Fourier fitting curve. (<b>b</b>–<b>d</b>) The reflection spectra of FPI<sub>2</sub> at different curvatures in fiber orientations <span class="html-italic">θ</span> = 90°, <span class="html-italic">θ</span> = 0° and <span class="html-italic">θ</span> = 180°, respectively. (<b>e</b>,<b>f</b>) The dip wavelength as functions of curvature when <span class="html-italic">θ</span> = 0° and <span class="html-italic">θ</span> = 180°, respectively. (<b>g</b>,<b>h</b>) The reflection spectra of FPI<sub>7</sub> at different curvatures in fiber orientations <span class="html-italic">θ</span> = 0° and <span class="html-italic">θ</span> = 90°, respectively. The bending characteristics of the central cavity (FPI<sub>7</sub>) in different fiber orientations were also investigated. (<b>g</b>,<b>h</b>) show the evolution of the reflection spectra of the central cavity with curvature changes in two orthogonal fiber orientations. Since the FPI<sub>7</sub> is on the neutral plane, the spectrum does not undergo the wavelength shift with the curvature change, regardless of whether <math display="inline"><semantics> <mi>θ</mi> </semantics></math> is 0° or 90°.</p>
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<p>(<b>a</b>–<b>c</b>) The dip wavelength of FPI<sub>2</sub>, FPI<sub>4</sub>, and FPI<sub>6</sub> as functions of curvature in all fiber orientation angles. (<b>d</b>) The curvature sensitivities of the three FPIs as the function of the fiber orientation in polar coordinates.</p>
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<p>(<b>a</b>) The curvature sensitivities of FPI<sub>2</sub>, FPI<sub>4</sub>, and FPI<sub>6</sub> as functions of the fiber orientation in cartesian coordinates. (<b>b</b>) The actual and reconstructed values demodulated by different combinations of the three FPIs for nine random curvature magnitudes and orientations in polar coordinates.</p>
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<p>The reconstructed and actual (<b>a</b>) curvature magnitudes and (<b>b</b>) orientation angles.</p>
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<p>(<b>a</b>–<b>c</b>) The reflection spectra of FPI<sub>1</sub>, FPI<sub>2</sub>, and FPI<sub>3</sub> at different temperatures. (<b>d</b>) Wavelength shift as a function of temperature for three FPIs.</p>
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18 pages, 4955 KiB  
Article
Elovanoids, a Novel Class of Lipid Mediators, Are Neuroprotective in a Traumatic Brain Injury Model in Rats
by Nicolas G. Bazan, Andre Obenaus, Larissa Khoutorova, Pranab K. Mukherjee, Bokkyoo Jun, Rostyslav Semikov and Ludmila Belayev
Biomedicines 2024, 12(11), 2555; https://doi.org/10.3390/biomedicines12112555 - 8 Nov 2024
Viewed by 413
Abstract
Background: In the United States, traumatic brain injury (TBI) contributes significantly to mortality and morbidity. Elovanoids (ELVs), a novel class of homeostatic lipid mediators we recently discovered and characterized, have demonstrated neuroprotection in experimental stroke models but have never been tested after TBI. [...] Read more.
Background: In the United States, traumatic brain injury (TBI) contributes significantly to mortality and morbidity. Elovanoids (ELVs), a novel class of homeostatic lipid mediators we recently discovered and characterized, have demonstrated neuroprotection in experimental stroke models but have never been tested after TBI. Methods: A moderate fluid-percussion injury (FPI) model was used on male rats that were treated with ELVs by intravenous (IV) or intranasal (IN) delivery. In addition, using liquid chromatography-mass spectrometry (LC-MS/MS), we examined whether ELVs could be detected in brain tissue after IN delivery. Results: ELVs administered intravenously 1 h after FPI improved behavior on days 2, 3, 7, and 14 by 20, 23, 31, and 34%, respectively, and preserved hippocampal CA3 and dentate gyrus (DG) volume loss compared to the vehicle. Whole-brain tractography revealed that ELV-IV treatment increased corpus callosum white matter fibers at the injury site. In comparison to treatment with saline on days 2, 3, 7, and 14, ELVs administered intranasally at 1 h and 24 h after FPI showed improved neurological scores by 37, 45, 41, and 41%. T2-weighted imaging (T2WI) abnormalities, such as enlarged ventricles and cortical thinning, were reduced in rats treated by ELV-IN delivery compared to the vehicle. On day 3, ELVs were detected in the striatum and ipsilateral cortex of ELV-IN-treated rats. Conclusion: We have demonstrated that both ELV-IN and ELV-IV administration offer high-grade neuroprotection that can be selectively supplied to the brain. This discovery may lead to innovative therapeutic targets for secondary injury cascade prevention following TBI. Full article
(This article belongs to the Section Molecular and Translational Medicine)
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<p>Elovanoid (ELV) biosynthesis. Docosahexaenoic acid (DHA) through ELOVL4 (elongation of very-long-chain fatty acids-4) leads to the synthesis of 32:6n-3, 34:6n-3, and other very-long-chain polyunsaturated fatty acids (VLC-PUFAs). These fatty acids are then esterified at sn-1 of phosphatidylcholine and sn-2 of DHA. Phospholipase A1 (PLA1) releases 32:6n-3 and 34:6n-3, leading to the synthesis of ELV-32 or ELV-34, respectively.</p>
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<p>ELV-IV and ELV-IN remarkably improved the total neurological score and tactile lateral and visual sideways contralateral forelimb placing reactions 14 days after FPI. (<b>a</b>) ELV-IV: the experimental design. (<b>b</b>) The total neurological score was enhanced by ELV-IV (normal score = 0, max = 12). (<b>c</b>,<b>d</b>) Tactile lateral and visual sideways placing were improved by ELV-IV (normal = 0, max = 2). n = 5–6 per group. (<b>e</b>) ELV-IN experimental design. (<b>f</b>) ELV-IN also enhanced the total neurological score. (<b>g</b>) Tactile placing (lateral) and (<b>h</b>) visual placing (sideways) exhibited remarkable recoveries after ELV-IN. The values shown are mean ± SEM, n = 6–7 per group; multiple Mann-Whitney tests. In the graphs (<b>b</b>,<b>d</b>,<b>f</b>,<b>h</b>), red represents vehicle, and blue is ELV.</p>
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<p>ELV-IV and ELV-IN attenuated brain damage and protected the integrity of the WM 14 days after FPI. (<b>a</b>) Representative T2WI images at the level of the dorsal hippocampus from saline and ELV-IV-treated rats on day 14. Saline rats exhibited more edema in the cortex (yellow arrow) and small hemorrhages within the white matter of the external capsule (red arrow) compared to the ELV-treated rats. (<b>b</b>) T2WI from FPI rats treated with saline or ELV-IN. There was a reduction in edema and white matter abnormalities (red arrow) in ELV-IN-treated rats. The dotted line indicates the expanded area showing white matter (corpus callosum; CC) and hippocampus (<b>c</b>). Directionally encoded fractional anisotropy maps of the cortex and CC (white arrows) show improvements in water directionality after treatment of ELV-IV. (<b>d</b>) Similarly, treatment with ELV-IN resulted in the conservation of the CC (white arrows). Inset: a color-coded directionality sphere for water diffusion.</p>
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<p>ELV-IV and ELV-IN preserved CC integrity. (<b>a</b>) CC tractography was examined using an ROI placed in the contralateral CC, and streamlines were visualized to the ipsilateral CC (injured hemisphere). ELV-IV treatment conferred protection of white matter tracts within CC. (<b>b</b>) ELV-IN treatment also increased the number of streamlines between the ipsi- and contralateral CC. * = ipsilateral FPI site of injury.</p>
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<p>ELV treatment recovers regional brain volumes. (<b>a</b>) Whole-brain volume was not significantly altered after either ELV-IV or ELV-IN treatments. (<b>b</b>) ELV-IV exhibited significant increases in the ipsilateral hemisphere and gray matter volumes. (<b>c</b>) ELV-IN did not significantly alter white and gray matter or hemispheric volumes—Welch’s <span class="html-italic">t</span>-test.</p>
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<p>Regional volumetric sensitivity is different in Elavonoid treatments. (<b>a</b>) Regional white matter volume changes differ between ELV-IV and ELV-IN treatments. ELV-IV treatments broadly increased white matter volumes but ELV-IN treatment was less effective with fewer regions showing increased volumes. (<b>b</b>) Limbic regions had increased volumes with either treatment route, with ELV-IV appearing to be more effective. ((<b>a</b>,<b>b</b>) <span class="html-italic">t</span>-test: + = <span class="html-italic">p</span> &lt; 0.1, * = <span class="html-italic">p</span> &lt; 0.05, *** = <span class="html-italic">p</span> &lt; 0.001). (<b>c</b>) The volume of the fimbra was increased (<span class="html-italic">p</span> = 0.06) after ELV-IV but not ELV-IN treatment. (<b>d</b>) Septum volume was not increased after ELV-IV treatment but significantly increased in ELV-IN (<span class="html-italic">p</span> = 0.03). (<b>e</b>) Cortical regions also exhibited increased volumes, with significant increases in postrhinal cortex after ELV-IV (<span class="html-italic">p</span> = 0.04) but not after ELV-IN treatment. <span class="html-italic">p</span> values <span class="html-italic">t</span>-test.</p>
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<p>dMRI monitors improvements in white matter. (<b>a</b>) AxD diffusivity was reduced in the fornix and the CC after ELV-IV but not in ELV-IN-treated rats. (<b>b</b>) MD decreased significantly in ELV-IV rats compared to that in vehicles in both the fornix and CC but not in ELV-IN. In the graphs, red represents vehicle, and purple is ELV. Note the increased variance in ELV-IN rats—Welch’s <span class="html-italic">t</span>-test.</p>
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<p>dMRI also reported improvements in gray matter in MD. (<b>a</b>) There was a trending decreased MD in the retrosplenial cortex in ELV-IV rats compared to saline ones, but no differences were observed for ELV-IN. (<b>b</b>) The MD was significantly reduced in the entorhinal cortex in ELV-IV but not ELV-IN rats. (<b>c</b>) The thalamus also reported significant reductions in MD in ELV-IV but not in ELV-IN rats—Welch’s <span class="html-italic">t</span>-test. In the graphs, red represents vehicle, and purple is ELV.</p>
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<p>ELV-IV treatment results in improved CA1 dMRI. (<b>a</b>) FA was not significantly altered in either ELV-IV or -IN treatments. (<b>b</b>) The MD was reduced considerably in the CA1 region after ELV-IV treatment but not with ELV-IN treatment. (<b>c</b>) In the CA1 region, ELV-IV treatment resulted in significant reductions in AxD that were not observed in ELV-IN rats. (<b>d</b>) The RD in ELV-IV rats was significantly reduced, with no change in ELV-IN rats. In the graphs, red represents vehicle, and purple is ELV. Note the increased variance in the ELV-IN-treated rats for most dMRI metrics—Welch’s <span class="html-italic">t</span>-test.</p>
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<p>ELV-IN was detected in the brain 3 days after FPI. (<b>a</b>) Timeline for experimental procedures and tissue collection. Elov-Mix was delivered at 1 h and 24 h after FPI, and brain regions were sampled 3 days after FPI for lipid extraction and analysis. (<b>b</b>) Total neurological score (normal score = 0, max = 12). ELV-IN improved the total neurological score by 22, 22, and 31% compared to saline treatment on days 1, 2, and 3. Repeated-measures ANOVA followed by Bonferroni’s test. (<b>c</b>) Relative abundance of ELV-34 (ratio to internal standard AA-d8) in brain regions denoted in the inset. The blue dot is an area of impact. The graph represents the quantification of a representative animal. ELV-34 was found at the highest levels in the cortex and subcortex ipsilateral to the side of FPI. N = 3 per group. Region sampling diagram: A—anterior (bregma level +1.2 mm), P—posterior (bregma level −1.8 mm). Ipsilateral cortex (A1, A3, P1, P3), P5 (hippocampus), Olf, Cer, stem. Contralateral cortex (A2, A4, P2, P4), P6 (hippocampus), Olf, Cer, stem. Olf—olfactory tract, Cer—cerebellum, stem—brainstem.</p>
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14 pages, 4903 KiB  
Article
Fiber-Optic Sensor Spectrum Noise Reduction Based on a Generative Adversarial Network
by Yujie Lu, Qingbin Du, Ruijia Zhang, Bo Wang, Zigeng Liu, Qizhe Tang, Pan Dai, Xiangxiang Fan and Chun Huang
Sensors 2024, 24(22), 7127; https://doi.org/10.3390/s24227127 - 6 Nov 2024
Viewed by 471
Abstract
In the field of fiber-optic sensing, effectively reducing the noise of sensing spectra and achieving a high signal-to-noise ratio (SNR) has consistently been a focal point of research. This study proposes a deep-learning-based denoising method for fiber-optic sensors, which involves pre-processing the sensor [...] Read more.
In the field of fiber-optic sensing, effectively reducing the noise of sensing spectra and achieving a high signal-to-noise ratio (SNR) has consistently been a focal point of research. This study proposes a deep-learning-based denoising method for fiber-optic sensors, which involves pre-processing the sensor spectrum into a 2D image and training with a cycle-consistent generative adversarial network (Cycle-GAN) model. The pre-trained algorithm demonstrates the ability to effectively denoise various spectrum types and noise profiles. This study evaluates the denoising performance of simulated spectra obtained from four different types of fiber-optic sensors: fiber Fabry–Perot interferometer (FPI), regular fiber Bragg grating (FBG), chirped FBG, and FBG pair. Compared to traditional denoising algorithms such as wavelet transform (WT) and empirical mode decomposition (EMD), the proposed method achieves an SNR improvement of up to 13.71 dB, an RMSE that is up to three times smaller, and a minimum correlation coefficient (R2) of no less than 99.70% with the original high-SNR signals. Additionally, the proposed algorithm was tested for multimode noise reduction, demonstrating an excellent linearity in temperature response with a R2 of 99.95% for its linear fitting and 99.74% for the temperature response obtained from single-mode fiber sensors. The proposed denoising approach effectively reduces the impact of various noises from the sensing system, enhancing the practicality of fiber-optic sensing, especially for specialized fiber applications in research and industrial domains. Full article
(This article belongs to the Special Issue New Prospects in Fiber Optic Sensors and Applications)
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<p>(<b>a</b>) The structure of a regular FBG; (<b>b</b>) a normalized FBG spectrum obtained from simulation, and (<b>c</b>) its reshaped 2D image.</p>
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<p>Cycle-GAN denoising flow chart for a fiber-optic sensor spectrum.</p>
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<p>Simulation of high-SNR and noise-added spectra of (<b>a</b>) regular low-finesse FPI; (<b>b</b>) regular FBG; (<b>c</b>) chirped FBG; and (<b>d</b>) FBG pair sensors. The corresponding reshape gray-level image is on the right side of each spectrum.</p>
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<p>Setup of the FPI sensor’s modal noise reduction.</p>
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<p>Silicon wafer FPI spectrum with (<b>a</b>) SMF and (<b>b</b>) MMF as the lead-in fiber.</p>
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<p>Cycle-GAN-based algorithm denoising results of (<b>a</b>) regular low-finesse FPI; (<b>b</b>) regular FBG; (<b>c</b>) chirped FBG; and (<b>d</b>) FBG pair sensors. For each sensor, the top half is the denoised spectrum and the bottom half is the difference from the high-SNR spectrum.</p>
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<p>(<b>a</b>) The original MMF-FPI spectrum and its denoised output from the Cycle-GAN-based algorithm; the 2D reshaped image of (<b>b</b>) the original MMF-FPI spectrum; (<b>c</b>) the denoised spectrum.</p>
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<p>(<b>a</b>) Wavelength shift versus temperature for the denoised FPI; (<b>b</b>) wavelength shift versus temperature for SMF and denoised FPI.</p>
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<p>(<b>a</b>) Comparison of spectrum of MMF-FPI and noise-reduced spectra obtained via Cycle-GAN-based algorithm and low-pass filter; (<b>b</b>) wavelength shift versus temperature for MMF-FPI with LPF and its linear fit; (<b>c</b>) wavelength shift versus temperature for SMF and MMF-FPI with LPF.</p>
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22 pages, 12882 KiB  
Article
UAV Geo-Localization Dataset and Method Based on Cross-View Matching
by Yuwen Yao, Cheng Sun, Tao Wang, Jianxing Yang and Enhui Zheng
Sensors 2024, 24(21), 6905; https://doi.org/10.3390/s24216905 - 28 Oct 2024
Viewed by 878
Abstract
The stable flight of drones relies on Global Navigation Satellite Systems (GNSS). However, in complex environments, GNSS signals are prone to interference, leading to flight instability. Inspired by cross-view machine learning, this paper introduces the VDUAV dataset and designs the VRLM network architecture, [...] Read more.
The stable flight of drones relies on Global Navigation Satellite Systems (GNSS). However, in complex environments, GNSS signals are prone to interference, leading to flight instability. Inspired by cross-view machine learning, this paper introduces the VDUAV dataset and designs the VRLM network architecture, opening new avenues for cross-view geolocation. First, to address the limitations of traditional datasets with limited scenarios, we propose the VDUAV dataset. By leveraging the virtual–real mapping of latitude and longitude coordinates, we establish a digital twin platform that incorporates 3D models of real-world environments. This platform facilitates the creation of the VDUAV dataset for cross-view drone localization, significantly reducing the cost of dataset production. Second, we introduce a new baseline model for cross-view matching, the Virtual Reality Localization Method (VRLM). The model uses FocalNet as its backbone and extracts multi-scale features from both drone and satellite images through two separate branches. These features are then fused using a Similarity Computation and Feature Fusion (SCFF) module. By applying a weighted fusion of multi-scale features, the model preserves critical distinguishing features in the images, leading to substantial improvements in both processing speed and localization accuracy. Experimental results demonstrate that the VRLM model outperforms FPI on the VDUAV dataset, achieving an accuracy increase to 83.35% on the MA@20 metric and a precision of 74.13% on the RDS metric. Full article
(This article belongs to the Section Navigation and Positioning)
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<p>Flowchart of UAV tilt-photography modeling.</p>
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<p>(<b>a</b>) The drone geolocation system built by importing the processed real-world 3D model into the Unity3D engine using Digital Twin technology. (<b>b</b>) The virtual camera model. (<b>c</b>) The virtual drone collision test model.</p>
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<p>RTK field measurements.</p>
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<p>Virtual reality mapping error analysis of nine arbitrarily selected measurement points on a solid model of Hangzhou, China, measured by RTK.</p>
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<p>The construction process of the VDUAV dataset, which involves the UAV capturing images every 20–30 m at each point; images are taken at three different heights ranging between 100 and 200 m.</p>
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<p>Drone images collected from various scenarios, including urban areas, village regions, hilly terrains, plains, university campuses, and industrial sites.</p>
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<p>(<b>a</b>) The training set, where the ratio of drone images to satellite images is 1:1. (<b>b</b>) The test set, where drone images are enclosed in red dashed boxes, and satellite images are enclosed in black dashed boxes, with a ratio of 1:12. The solid red dots in the images indicate the actual positions of the drones in the satellite images.</p>
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<p>The VRLM fusion localization network framework first performs feature extraction to obtain two sets of features, <math display="inline"><semantics> <msub> <mi>U</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>U</mi> <mn>2</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>U</mi> <mn>3</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>S</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>2</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>3</mn> </msub> </semantics></math>. Subsequently, the similarity between the two sets of features is calculated, represented by yellow spheres. The purple spheres represent weighted fusion, ultimately generating a heatmap.</p>
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<p>The localization accuracy of FPI, WAMF-FPI, and VRLM using the MA evaluation metric.</p>
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<p>Comparing the performance of different models on varying satellite map sizes, with the <span class="html-italic">x</span>-axis representing the scale of the satellite images and the <span class="html-italic">y</span>-axis representing the localization accuracy of the models at the corresponding level. (<b>a</b>) Localization accuracy at 3 m. (<b>b</b>) Localization accuracy at 5 m. (<b>c</b>) Localization accuracy at 10 m. (<b>d</b>) Localization accuracy at 20 m. (<b>e</b>) Localization accuracy at 30 m. (<b>f</b>) Localization accuracy at 50 m.</p>
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<p>The prediction results are displayed on the heatmaps.</p>
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<p>Comparison of localization performance between the UL14 dataset and the VDUAV dataset.</p>
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<p>The localization accuracy of the four backbone networks using the MA evaluation metric.</p>
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<p>The localization accuracy of the three fusion methods using the MA evaluation metric.</p>
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11 pages, 274 KiB  
Article
Relationship Between Morphofunctional Alterations of the Foot and Its Functionality in Patients with Fibromyalgia Syndrome: A Case–Control Study
by María De Maya-Tobarra, Sara Zúnica-García, Alba Gracia-Sánchez and Esther Chicharro-Luna
J. Clin. Med. 2024, 13(21), 6439; https://doi.org/10.3390/jcm13216439 - 27 Oct 2024
Viewed by 736
Abstract
Objective: To evaluate the morphofunctional alterations in the foot and their association with functionality, considering aspects such as disability, pain, and limitations in daily activities in patients with fibromyalgia syndrome (FMS). Methods: A case–control study was conducted in patients with FMS [...] Read more.
Objective: To evaluate the morphofunctional alterations in the foot and their association with functionality, considering aspects such as disability, pain, and limitations in daily activities in patients with fibromyalgia syndrome (FMS). Methods: A case–control study was conducted in patients with FMS (case group) and without FMS (control group), matched by age and sex. Foot posture was assessed using the foot posture index (FPI), along with the presence of hallux valgus (HV), trigger points, hyperkeratosis, and dorsiflexion of the first metatarsophalangeal joint and ankle. Foot functionality was evaluated using the foot function index (FFI) questionnaire. Results: A total of 100 women with FMS and 100 women without FMS, with a mean age of 61.97 ± 9.26 years, were recruited. HV (p < 0.001), hyperkeratosis (p < 0.001), pronated and supinated foot (p < 0.001), as well as limitations in dorsiflexion of the first metatarsophalangeal joint (p < 0.001) and the ankle with the knee flexed (p < 0.001) and extended (p < 0.001), along with the activity of the flexor hallucis brevis (p = 0.006), adductor hallucis (p = 0.006), and dorsal interosseous (p = 0.002) muscles, were significantly associated with the FFI, being higher in individuals with FMS, indicating greater impairment of foot functionality in these patients. Multivariate analysis revealed a statistical association between FMS and low educational level (OR = 2.57, 95% CI 1.05–5.72), the presence of another rheumatic disease (OR = 5.07, 95% CI 2.34–11), and the presence of any active trigger point (OR = 11.15, 95% CI 3.97–31.31). Conclusions: The study highlights the relationship between morphofunctional foot alterations, specifically the presence of active myofascial trigger points, and functionality in patients with FMS. Full article
(This article belongs to the Section Orthopedics)
13 pages, 1447 KiB  
Article
Approachability and Sensory Changes Following Mild Traumatic Brain Injury in Pigs
by Mark Pavlichenko, Radina L. Lilova, Amanda Logan-Wesley, Karen M. Gorse and Audrey D. Lafrenaye
Biomedicines 2024, 12(11), 2427; https://doi.org/10.3390/biomedicines12112427 - 23 Oct 2024
Viewed by 518
Abstract
Background/Objectives: Traumatic brain injury (TBI) is a global healthcare concern affecting millions, with wide-ranging symptoms including sensory and behavioral changes that can persist long-term. Due to similarities with human brain cytoarchitecture and inflammation, minipig models are advantageous for translational TBI research. However, gaps [...] Read more.
Background/Objectives: Traumatic brain injury (TBI) is a global healthcare concern affecting millions, with wide-ranging symptoms including sensory and behavioral changes that can persist long-term. Due to similarities with human brain cytoarchitecture and inflammation, minipig models are advantageous for translational TBI research. However, gaps in knowledge exist regarding their behavioral and sensory sequelae following injury. Methods: Therefore, in this study, we assessed changes in approachability using a forced human approach task (FHAT) and mechanical nociception using the von Frey test in adult male and female Yucatan minipigs for up to one week following a sham or central fluid percussion injury (cFPI). Specifically, the FHAT assessed each animal’s response to a forced interaction with either a known or unknown experimenter. To evaluate changes in nociceptive sensory sensitivity, von Frey monofilaments ranging from 0.008 to 300 g of force were applied to the pinna of the ear or base of the tail. Results: We found that forced approachability was affected by experimenter familiarity as well as cFPI in a sex-specific manner at subacute timepoints. We also found reductions in sensitivity following cFPI on the ear in male minipigs and on the tail in female minipigs. Conclusion: Overall, the current study demonstrates that cFPI produces both behavioral and sensory changes in minipigs up to one-week post-injury. Full article
(This article belongs to the Section Biomedical Engineering and Materials)
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<p>Experimental timeline for the current study. Acclimation to a known experimenter was done for a week following animal release from quarantine. A pre-injury behavioral assessment was done ~3d prior to induction of a central fluid percussion injury (cFPI) or a control sham injury (red line). Post-injury behavioral assessments were performed at 1 d, 2 d, 3 d, and 1 w (5–6 d) post-injury. During all behavioral testing sessions, the FHAT was performed prior to the von Frey test. Following completion of all behavioral assessments, animals were euthanized.</p>
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<p>Plots of mean forced human approach test (FHAT) score for (<b>A</b>,<b>B</b>) male sham (n = 5, grey lines) and TBI (n = 6, orange lines) and (<b>C</b>,<b>D</b>) female sham (n = 6, grey lines) and TBI (n = 7, pink lines. Each FHAT test was performed by both a (<b>A</b>,<b>C</b>) known and (<b>B</b>,<b>D</b>) unknown experimenter. # <span class="html-italic">p</span> &lt; 0.05 compared to timepoint-matched sham.</p>
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<p>Plots of mean von Frey filament gram force that elicited a response in the (<b>A</b>,<b>C</b>) ear or (<b>B</b>,<b>D</b>) tail for (<b>A</b>,<b>B</b>) male or (<b>C</b>,<b>D</b>) female pigs prior to a TBI and up to 1 w following TBI. Male sham (n = 5) and female sham (n = 5) pigs are indicated as black lines. Male (n = 6) and female (n = 7) pigs sustaining a TBI are indicated as orange lines for males and pink lines for females. NR = no response to the highest gram force filament (300g). * <span class="html-italic">p</span> &lt; 0.05 compared to pre-injury, # <span class="html-italic">p</span> &lt; 0.05 compared to time-point matched sham.</p>
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19 pages, 499 KiB  
Review
A Systematic Review of Traumatic Brain Injury in Modern Rodent Models: Current Status and Future Prospects
by Evgenii Balakin, Ksenia Yurku, Tatiana Fomina, Tatiana Butkova, Valeriya Nakhod, Alexander Izotov, Anna Kaysheva and Vasiliy Pustovoyt
Biology 2024, 13(10), 813; https://doi.org/10.3390/biology13100813 - 11 Oct 2024
Viewed by 1012
Abstract
According to the Centers for Disease Control and Prevention (CDC), the national public health agency of the United States, traumatic brain injury is among the leading causes of mortality and disability worldwide. The consequences of TBI include diffuse brain atrophy, local post-traumatic atrophy, [...] Read more.
According to the Centers for Disease Control and Prevention (CDC), the national public health agency of the United States, traumatic brain injury is among the leading causes of mortality and disability worldwide. The consequences of TBI include diffuse brain atrophy, local post-traumatic atrophy, arachnoiditis, pachymeningitis, meningocerebral cicatrices, cranial nerve lesions, and cranial defects. In 2019, the economic cost of injuries in the USA alone was USD 4.2 trillion, which included USD 327 billion for medical care, USD 69 billion for work loss, and USD 3.8 trillion for the value of statistical life and quality of life losses. More than half of this cost (USD 2.4 trillion) was among working-age adults (25–64 years old). Currently, the development of new diagnostic approaches and the improvement of treatment techniques require further experimental studies focused on modeling TBI of varying severity. Full article
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<p>PRISMA flow diagram for the review.</p>
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22 pages, 12585 KiB  
Article
Preparation and Characterization of Atomic Oxygen-Resistant, Optically Transparent and Dimensionally Stable Copolyimide Films from Fluorinated Monomers and POSS-Substituted Diamine
by Zhenzhong Wang, Xiaolei Wang, Shunqi Yuan, Xi Ren, Changxu Yang, Shujun Han, Yuexin Qi, Duanyi Li and Jingang Liu
Polymers 2024, 16(19), 2845; https://doi.org/10.3390/polym16192845 - 9 Oct 2024
Viewed by 672
Abstract
Optically transparent polyimide (PI) films with good atomic oxygen (AO) resistance have been paid extensive attention as thermal controls, optical substrates for solar cells or other components for low Earth orbit (LEO) space applications. However, for common PI films, it is usually quite [...] Read more.
Optically transparent polyimide (PI) films with good atomic oxygen (AO) resistance have been paid extensive attention as thermal controls, optical substrates for solar cells or other components for low Earth orbit (LEO) space applications. However, for common PI films, it is usually quite difficult to achieve both high optical transparency and AO resistance and maintain the intrinsic thermal stability of the PI films at the same time. In the current work, we aimed to achieve the target by using the copolymerization methodology using the fluorinated dianhydride 9,9-bis(trifluoromethyl)xanthene-2,3,6,7-tetracarboxylic dianhydride (6FCDA), the fluorinated diamine 2,2-bis [4-(4-aminophenoxy)phenyl]hexafluoropropane (BDAF) and the polyhedral oligomeric silsesquioxane (POSS)-containing diamine N-[(heptaisobutyl-POSS)propyl]-3,5-diaminobenzamide (DABA-POSS) as the starting materials. The fluoro-containing monomers were used to endow the PI films with good optical and thermal properties, while the silicon-containing monomer was used to improve the AO resistance of the afforded PI films. Thus, the 6FCDA-based PI copolymers, including 6FCPI-1, 6FCPI-2 and 6FCPI-3, were prepared using a two-step chemical imidization procedure, respectively. For comparison, the analogous PIs, including 6FPI-1, 6FPI-2 and 6FPI-3, were correspondingly developed according to the same procedure except that 6FCDA was replaced by 4,4′-(hexafluoroisopropylidene)diphthalic anhydride (6FDA). Two referenced PI homopolymers were prepared from BDAF and 6FDA (PI-ref1) and 6FCDA (PI-ref2), respectively. The experimental results indicated that a good balance among thermal stability, optical transparency, and AO resistance was achieved by the 6FCDA-PI films. For example, the 6FCDA-PI films exhibited good thermal stability with glass transition temperatures (Tg) up to 297.3 °C, good optical transparency with an optical transmittance at a wavelength of 450 nm (T450) higher than 62% and good AO resistance with the erosion yield (Ey) as low as 1.7 × 10−25 cm3/atom at an AO irradiation fluence of 5.0 × 1020 atoms/cm2. The developed 6FCDA-PI films might find various applications in aerospace as solar sails, thermal control blankets, optical components and other functional materials. Full article
(This article belongs to the Special Issue Polymer Thin Films and Their Applications)
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<p>Preparation of PI and referenced PI resins.</p>
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<p>GPC plots of PI resins.</p>
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<p>XRD spectra of PI resins.</p>
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<p><sup>1</sup>H-NMR spectra of 6FPI resins in DMSO-d<sub>6</sub>.</p>
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<p><sup>1</sup>H-NMR spectra of 6FCPI resins in DMF-d<sub>7</sub>.</p>
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<p>FTIR spectra of PI films.</p>
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<p>TGA and DTG curves of PI films in nitrogen. (<b>a</b>) 6FPI; (<b>b</b>) 6FCPI.</p>
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<p>DSC curves of PI films.</p>
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<p>DMA curves of PI films.</p>
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<p>TMA curves of PI films.</p>
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<p>UV-Vis spectra of PI films.</p>
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<p>Appearance of PI films before and after AO exposure (doze: 5.0 × 10<sup>20</sup> atoms/cm<sup>2</sup>). (<b>a</b>–<b>c</b>): 6FPI-1~6FPI-3 films: left: pristine film; right: film after AO exposure; (<b>d</b>–<b>f</b>): 6FCPI-1~6FCPI-3 films: left: pristine film; right: film after AO exposure; (<b>g</b>) 6FPI-1-AO; (<b>h</b>) 6FPI-2-AO; (<b>i</b>) 6FPI-3-AO; (<b>j</b>) 6FCPI-1-AO; (<b>k</b>) 6FCPI-2-AO; (<b>l</b>) 6FCPI-3-AO.</p>
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<p>Comparison of UV-Vis spectra of PI films before and after AO exposure. (<b>a</b>) 6FPI; (<b>b</b>) 6FCPI.</p>
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<p>SEM and EDS images of pristine 6FCDA-PI films. (<b>a</b>) 6FCPA-1, (<b>b</b>) 6FCPI-2 and (<b>c</b>) 6FCPI-3.</p>
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<p>SEM and EDS images of 6FCDA-PI films after AO exposure (5.0 × 10<sup>20</sup> atoms/cm<sup>2</sup>). (<b>a</b>) 6FCPA-1-AO, (<b>b</b>) 6FCPI-2-AO and (<b>c</b>) 6FCPI-3-AO.</p>
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<p>XPS spectra of Si2p and O1s for 6FCPI films. (<b>a</b>) 6FCPI-1 and 6FCPI-1-AO; (<b>b</b>) 6FCPI-2 and 6FCPI-2-AO; (<b>c</b>) 6FCPI-3 and 6FCPI-3-AO.</p>
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17 pages, 319 KiB  
Article
Descriptive Study of the Influence of Foot Type on Physical Characteristics, Laxity, Strength and Baropodometry in Children Aged 5 to 10 Years
by Cristina Molina-García, Francisco Álvarez-Salvago, Clara Pujol-Fuentes, Andrés López-del-Amo-Lorente, Laura Ramos-Petersen, Carlos Martínez-Sebastián, Antonio Martínez-Amat, José Daniel Jiménez-García and Manuel De Diego-Moreno
Appl. Sci. 2024, 14(19), 8578; https://doi.org/10.3390/app14198578 - 24 Sep 2024
Viewed by 819
Abstract
Background: Foot morphology in children is a crucial factor influencing multiple aspects of their physical development. Between the ages of 5 and 10 years, the critical period of child development is when the movement and stability patterns are consolidated that can affect their [...] Read more.
Background: Foot morphology in children is a crucial factor influencing multiple aspects of their physical development. Between the ages of 5 and 10 years, the critical period of child development is when the movement and stability patterns are consolidated that can affect their long-term physical performance and quality of life. The aim of this study is to analyze how the type of foot influences different physical characteristics, laxity, strength, motor tests, and baropodometric variables in children aged 5 to 10 years. Methods: A cross-sectional study involving 196 children was conducted. Different physical characteristics, laxity, strength, motor tests, and baropodometric variables of the sample were analyzed for age and Foot Posture Index (FPI). Results: Differences in all variables were examined by age and FPI. Statistical analysis showed a moderate to high correlation (r > 0.6, p < 0.01) between FPI and the relaxed calcaneal stance position (RCSP) test. Some significant differences were also found in variables related to foot pronation and supination. These results provide valuable information for understanding differences in motor and functional development during childhood and pre-adolescence. Conclusions: The findings highlight the variability in physical and functional development between age and foot type groups, highlighting the importance of considering these differences in the assessment and management of foot-related conditions and biomechanics in childhood. Foot type significantly influences children’s growth and development. Full article
(This article belongs to the Special Issue Biomechanics and Motor Control on Human Movement Analysis)
19 pages, 465 KiB  
Article
Shaping Student Relationships: The Role of Personality in Early Childhood Pre-Service Teachers
by Seda Ata and İlayda Kimzan
Behav. Sci. 2024, 14(9), 778; https://doi.org/10.3390/bs14090778 - 5 Sep 2024
Viewed by 820
Abstract
The purpose of this explanatory sequential mixed-methods study is to explain teacher–student relationships in preschool classrooms in terms of the child’s temperament and the pre-service preschool teachers’ personalities. The study was conducted using a sequential exploratory mixed-methods design. Since both quantitative and qualitative [...] Read more.
The purpose of this explanatory sequential mixed-methods study is to explain teacher–student relationships in preschool classrooms in terms of the child’s temperament and the pre-service preschool teachers’ personalities. The study was conducted using a sequential exploratory mixed-methods design. Since both quantitative and qualitative data were obtained, sampling was carried out in two stages: quantitative random stratified sampling, and qualitative purposive sampling. Quantitative data were obtained from 126 pre-service teachers. The qualitative study group consisted of 18 pre-service teachers. Quantitative data were collected using the Student–Teacher Relationship Scale-Short Form, the Short Temperament Scale for Children (STSC), and the Five Factor Personality Inventory (FPI). Qualitative data were obtained from interviews with 18 teachers. The findings revealed that the student–teacher relationship can be explained by adult and child characteristics. In addition, pre-service teachers’ perceptions of the student–teacher relationship are explained by adult characteristics much more than pre-service teachers’ perceptions. Full article
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<p>Thematic map.</p>
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9 pages, 1275 KiB  
Article
Diamond-Based Fiber-Optic Fabry–Perot Interferometer with Ultrawide Refractive-Index Measurement Range
by Dewen Duan, Jianhao Yang, Yi Tang and Yi-Yuan Xie
Photonics 2024, 11(8), 763; https://doi.org/10.3390/photonics11080763 - 15 Aug 2024
Viewed by 1190
Abstract
The majority of Fabry–Perot interferometer (FPI) tip refractive index (RI) sensors utilize silica optical fiber as the cavity material, with an RI of approximately 1.45. This restricts their applicability in measuring the RI of liquids with an RI of approximately 1.45. Here, we [...] Read more.
The majority of Fabry–Perot interferometer (FPI) tip refractive index (RI) sensors utilize silica optical fiber as the cavity material, with an RI of approximately 1.45. This restricts their applicability in measuring the RI of liquids with an RI of approximately 1.45. Here, we propose a fiber-optic FPI-tip RI sensor by bonding a flat, thin diamond film onto the apex of a single-mode optical fiber. The FPI cavity is constructed from a diamond with an RI of approximately 2.4, theoretically enabling the sensor to achieve an ultrawide RI measurement range of 1 to 2.4. A theoretical comparison of its measurement performance was conducted with that of an FPI-tip RI sensor whose cavity is formed by silica fiber. Additionally, an experimental examination of the device’s RI measurement performance was conducted. The results show that the sensor has visibility to the RI unit of −0.4362/RIU in the RI range of 1.33 to 1.40. Combined with other narrow-RI-ranged high-sensitivity sensors, our proposed RI sensor has the potential for use in a wide range of applications. Full article
(This article belongs to the Special Issue Progress in Fiber Optic Sensors: Design and Applications)
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<p>(<b>a</b>) Principle schematic diagram of the diamond-based fiber-optic Fabry–Perot interferometer (FPI). (<b>b</b>) Electronic microscope image of one fabricated diamond-based fiber-optic FPI (diamond thickness is approximately 34.14 μm).</p>
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<p>Measured reflection spectrum of a fabricated FPI sensor (diamond thickness is approximately 40.82 μm). The spectrum is obtained by inserting the FPI sensor inside microscopic immersion oil (Fluka 51786; its RI is <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>1.517</mn> </mrow> </semantics></math> at room temperature (20 °C)).</p>
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<p>(<b>a</b>) Calculated maximum visibility versus measured refractive index (RI) of the fabricated diamond-based FPI (whose reflection spectrum is shown in <a href="#photonics-11-00763-f002" class="html-fig">Figure 2</a>) and an optical fiber-based FPI sensor having the same <math display="inline"><semantics> <mi>α</mi> </semantics></math> value (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.43142</mn> </mrow> </semantics></math>); <math display="inline"><semantics> <msub> <mi>n</mi> <mi>d</mi> </msub> </semantics></math> is replaced by <math display="inline"><semantics> <msub> <mi>n</mi> <mrow> <mi>s</mi> <mi>i</mi> <mi>l</mi> <mi>i</mi> <mi>c</mi> <mi>a</mi> </mrow> </msub> </semantics></math> = 1.45 in Equations (<a href="#FD1-photonics-11-00763" class="html-disp-formula">1</a>) and (<a href="#FD4-photonics-11-00763" class="html-disp-formula">4</a>). (<b>b</b>) Interference visibility derivation (<math display="inline"><semantics> <mrow> <mo>Δ</mo> <mo>(</mo> <mi>v</mi> <mi>i</mi> <mi>s</mi> <mi>i</mi> <mi>b</mi> <mi>i</mi> <mi>l</mi> <mi>i</mi> <mi>t</mi> <mi>y</mi> <mo>)</mo> <mo>/</mo> <mo>Δ</mo> <mo>(</mo> <mi>R</mi> <mi>I</mi> <mo>)</mo> </mrow> </semantics></math>) of the two FPIs shown in (<b>a</b>). (<b>c</b>) Calculated maximum visibility versus measured RI of the fabricated diamond-based FPI and the air-plus-silica hybrid cavity FPI in [<a href="#B12-photonics-11-00763" class="html-bibr">12</a>]. (<b>d</b>) Interference visibility derivation (<math display="inline"><semantics> <mrow> <mo>Δ</mo> <mo>(</mo> <mi>v</mi> <mi>i</mi> <mi>s</mi> <mi>i</mi> <mi>b</mi> <mi>i</mi> <mi>l</mi> <mi>i</mi> <mi>t</mi> <mi>y</mi> <mo>)</mo> <mo>/</mo> <mo>Δ</mo> <mo>(</mo> <mi>R</mi> <mi>I</mi> <mo>)</mo> </mrow> </semantics></math>) of the two FPIs shown in (<b>c</b>).</p>
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<p>Experimental setup for the diamond-based FPI’s RI sensor measurement. The yellow lines represent the single-mode optical fiber cables. The measured sample is in a baker, and the diamond-based FPI is immersed in the liquid sample during the measurement of the RI of the liquid sample. The inset is the schematic diagram of the diamond-based FPI.</p>
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<p>The interferometric spectrum of the diamond-based FPI used in RI measurements (diamond thickness approximately 48.6 μm). The spectrum is obtained by inserting the FPI sensor inside air and water whose RI is <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>1.33</mn> </mrow> </semantics></math> at room temperature (20 °C). The red dashed line represents the reflected spectrum of a flat bare fiber end in the air, in the absence of the diamond.</p>
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<p>(<b>a</b>) The reflected spectrum of a diamond-based FPI inserted into glucose solutions with varying refractive indices (RIs). (<b>b</b>) Experimental measured maximum visibility versus measured RI results and theoretically calculated maximum visibility versus RI curve of the fabricated diamond-based FPI.</p>
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<p>Experimentally measured reflection spectrum visibility change due to the temperature change in the fabricated diamond-based FPI.</p>
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<p>The The schematic diagrams of the proposed ultrawide-RI-measurable-range fiber-optic FPI: (<b>a</b>) fabricated by bonding a high-RI flat and thin crystal or glass sheet on the apex of single-mode fiber, or (<b>b</b>) by dipping a small drop of high-RI transparent polymer and then solidifying it.</p>
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Article
Ablation Parameters Predicting Pulmonary Vein Reconnection after Very High-Power Short-Duration Pulmonary Vein Isolation
by Márton Boga, Gábor Orbán, Zoltán Salló, Klaudia Vivien Nagy, István Osztheimer, Arnold Béla Ferencz, Ferenc Komlósi, Patrik Tóth, Edit Tanai, Péter Perge, Béla Merkely, László Gellér and Nándor Szegedi
J. Cardiovasc. Dev. Dis. 2024, 11(8), 230; https://doi.org/10.3390/jcdd11080230 - 24 Jul 2024
Viewed by 986
Abstract
Background: Recurrences due to discontinuity in ablation lines are substantial after pulmonary vein isolation (PVI) with radiofrequency ablation for atrial fibrillation. Data are scarce regarding the durability predictors for very high-power short-duration (vHPSD, 90 W/4 s) ablation. Methods: A total of 20 patients [...] Read more.
Background: Recurrences due to discontinuity in ablation lines are substantial after pulmonary vein isolation (PVI) with radiofrequency ablation for atrial fibrillation. Data are scarce regarding the durability predictors for very high-power short-duration (vHPSD, 90 W/4 s) ablation. Methods: A total of 20 patients were enrolled, who underwent 90 W PVI and a mandatory remapping procedure at 3 months. First-pass isolation (FPI) gaps, and acute pulmonary vein reconnection (PVR) sites were identified at the index procedure; and chronic PVR sites were identified at the repeated procedure. We analyzed parameters of ablation points (n = 1357), and evaluated their roles in predicting a composite endpoint of FPI gaps, acute and chronic PVR. Results: In total, 45 initial ablation points corresponding to gaps in the ablation lines were analyzed. Parameters associated with gaps were interlesion distance (ILD), baseline generator impedance, mean current, total charge, and loss of catheter–tissue contact. The optimal ILD cut-off for predicting gaps was 3.5 mm anteriorly, and 4 mm posteriorly. Conclusions: Biophysical characteristics dependent on generator impedance could affect the efficacy of vHPSD PVI. The use of smaller ILDs is required for effective and durable PVI with vHPSD compared to the consensus targets with lower power ablation, and lower ILDs for anterior applications seem necessary compared to posterior points. Full article
(This article belongs to the Section Electrophysiology and Cardiovascular Physiology)
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<p>Graph showing the changes of ablation parameters during the 4-s RF applications with the QMODE+ setting (90 W/4 s, temperature-controlled mode). Yellow: power (W); red: temperature (°C); blue: contact-force (g), dashed lines: target contact-force range (5–40 g); green: impedance (Ω). (<b>A</b>) The target temperature of 55 °C is not reached, stable 90 W of power is delivered for 4 s. (<b>B</b>) The target temperature is reached, power is downregulated to prevent overheating. RF = radiofrequency.</p>
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<p>(<b>A</b>) Electroanatomical map of 90 W pulmonary vein isolation (posteroanterior view). (<b>B</b>) High-density voltage map of a patient with four isolated pulmonary veins at the repeat procedure (posteroanterior view) [<a href="#B9-jcdd-11-00230" class="html-bibr">9</a>]. Red area on right panel: bipolar voltage &lt; 0.5 mV; purple area: bipolar voltage &gt; 0.5 mV.</p>
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<p>Location of gaps on a 16-segment pulmonary vein ostium model. Empty stars indicate gaps in the first-pass circle, dashed stars indicate acute PVR, and bold stars indicate chronic PVR. PVR = pulmonary vein reconnection. Vertical dashed lines indicate the border between anterior/posterior segments.</p>
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<p>Association between variables and gap probability. (<b>A</b>) Bar chart showing the percentage of ablation points at gap sites in the case of anterior location, loss-of-contact, and ILD &gt; 3.5 mm. (<b>B</b>–<b>D</b>) Logistic regression curves of total energy, total charge, and mean current delivered by ablation point. ILD = interlesion distance, LOC = loss-of-contact.</p>
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<p>ROC curves of ILDs for predicting gaps and reconnections in the case all applications (<b>A</b>), anterior (<b>B</b>), and posterior (<b>C</b>) ablation points. AUC = area under curve, CI = confidence interval, ILD = inter-lesion distance, ROC = receiver operating characteristic.</p>
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Article
High-Resolution and Large-Dynamic Range Fiber-Optic Sensors Based on Dual-Mode Direct Spectrum Interrogation Method
by Min Zhou, Zhe Zhang, Qingyue Cui, Qingdian Lin, Jun Yu, Xiaoyang Guo, Cangtao Zhou and Shuangchen Ruan
Sensors 2024, 24(12), 3996; https://doi.org/10.3390/s24123996 - 20 Jun 2024
Cited by 1 | Viewed by 891
Abstract
Conventional optical fiber temperature/strain sensors often have to make compromises between the resolution and the dynamic range. Here we present a new method that meets the measurement requirements for both high resolution and large dynamic range. A high-quality optical fiber Fabry-Perot Interferometer (FPI) [...] Read more.
Conventional optical fiber temperature/strain sensors often have to make compromises between the resolution and the dynamic range. Here we present a new method that meets the measurement requirements for both high resolution and large dynamic range. A high-quality optical fiber Fabry-Perot Interferometer (FPI) constructed using a pair of chirped fiber Bragg gratings is employed as the sensor and a dual-mode direct spectrum interrogation method is proposed to identify the small drift of external temperature or strain. As a proof-of-concept illustration, a temperature resolution of 0.2 °C within 30–130 °C is demonstrated. For strain sensing, the resolution can be 10 µε within 0–1000 µε. The measurement resolution can be improved further by routinely increasing the reflectivity of the CFBG and the cavity length and the sensor can also be mass-produced. This new sensing schema not only resolves the conflict between the resolution and the dynamic range of fiber-optic temperature/strain sensors but can also be extended to other sensors and measurands. Full article
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Figure 1

Figure 1
<p>(<b>a</b>) Schematic of the proposed FPI sensor, the iridescent arrows represent the incident and reflected light, respectively; (<b>b</b>) The simulated reflection spectra of three FPI sensors with CFBG reflection <span class="html-italic">R</span><sub>0</sub> of 0.2, 0.4, and 0.8 (the cavity length <span class="html-italic">L</span><sub>0</sub> is assumed to be 10 mm); (<b>c</b>) The simulated reflection spectra of three FPI sensors with cavity length <span class="html-italic">L</span><sub>0</sub> of 5 mm, 10 mm, and 15 mm (the CFBG reflection <span class="html-italic">R</span><sub>0</sub> is assumed to be 0.2 mm).</p>
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<p>(<b>a</b>) Schematic diagram of the CFBG preparation system, including a UV laser operating at 266 nm, a chirped phase mask, and electronic scanning stages; (<b>b</b>) Reflection (blue line) and transmission (orange line) spectra of the prepared FPI<sub>1</sub> sensor with a cavity length <span class="html-italic">L</span><sub>0</sub> of ~6.9 mm.</p>
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<p>(<b>a</b>) The resonant dip evolution of FPI<sub>1</sub> with temperature increasing from 35 to 40.5 °C in steps of 0.5 °C; (<b>b</b>) The wavelength of the tracked resonant dip versus the temperature.</p>
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<p>(<b>a</b>) The reflection spectrum and (<b>b</b>) spectral envelope evolutions of FPI<sub>1</sub> with temperature increasing from 30 °C to 130 °C; (<b>c</b>) The center wavelength of the reflection spectral envelope versus the temperature; (<b>d</b>) The reflection spectrum and (<b>e</b>) spectral envelope evolutions of FPI<sub>1</sub> with temperature decreasing from 130 °C to 30 °C; (<b>f</b>) The center wavelength of the reflection spectral envelope versus the temperature.</p>
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<p>(<b>a</b>) The resonant dip evolution of FPI<sub>1</sub> with tensile strain increasing from 0 με to 70 με; (<b>b</b>) The wavelength shifts of the tracked resonant dip versus applied strain.</p>
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<p>(<b>a</b>) The reflection spectrum and (<b>b</b>) spectral envelope evolutions of FPI<sub>1</sub> with strain increasing from 0 με to 1000 με; (<b>c</b>) The center wavelength of the reflection spectral envelope shifts versus applied strain; (<b>d</b>) The reflection spectrum and (<b>e</b>) spectral envelope evolutions of FPI<sub>1</sub> with strain decreasing from 1000 με to 0 με; (<b>f</b>) The center wavelength shifts versus applied strain.</p>
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<p>(<b>a</b>) Reflection (blue line) and transmission (orange line) spectra of the FPI<sub>2</sub> with a cavity length of ~15.1 mm, the red lines represent the envelop of the spectrum; (<b>b</b>) Enlarged view of the reflection spectrum, where the bandwidth <math display="inline"><semantics> <mrow> <mo>Δ</mo> <mi>λ</mi> </mrow> </semantics></math> and FSR are ~0.023 and ~0.055 nm, respectively.</p>
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<p>(<b>a</b>) The resonant dip evolution of FPI<sub>2</sub> with temperature increasing from 36 °C to 37.4 °C (temperature of most living bodies); (<b>b</b>) The wavelength of the tracked resonant dip versus the temperature.</p>
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12 pages, 6545 KiB  
Article
Frequency-Dependent Dielectric Permittivity and Water Permeability in Ordered Mesoporous Silica-Grafted Fluorinated Polyimides
by Jaemin Son, Hwon Park, Minju Kim, Jae Hui Park, Ki-Ho Nam and Jin-Seok Bae
Polymers 2024, 16(12), 1716; https://doi.org/10.3390/polym16121716 - 16 Jun 2024
Viewed by 1272
Abstract
Polymers with a low dielectric constant (Dk) are promising materials for high-speed communication networks, which demand exceptional thermal stability, ultralow Dk and dissipation factor, and minimum moisture absorption. In this paper, we prepared a series of novel low-D [...] Read more.
Polymers with a low dielectric constant (Dk) are promising materials for high-speed communication networks, which demand exceptional thermal stability, ultralow Dk and dissipation factor, and minimum moisture absorption. In this paper, we prepared a series of novel low-Dk polyimide films containing an MCM-41-type amino-functionalized mesoporous silica (AMS) via in situ polymerization and subsequent thermal imidization and investigated their morphologies, thermal properties, frequency-dependent dielectric behaviors, and water permeabilities. Incorporating 6 wt.% AMS reduced the Dk at 1 MHz from 2.91 of the pristine fluorinated polyimide (FPI) to 2.67 of the AMS-grafted FPI (FPI-g-AMS), attributed to the free volume and low polarizability of fluorine moieties in the backbone and the incorporation of air voids within the mesoporous AMS particles. The FPI-g-AMS films presented a stable dissipation factor across a wide frequency range. Introducing a silane coupling agent increased the hydrophobicity of AMS surfaces, which inhibited the approaching of the water molecules, avoiding the hydrolysis of Si–O–Si bonds of the AMS pore walls. The increased tortuosity caused by the AMS particles also reduced water permeability. All the FPI-g-AMS films displayed excellent thermooxidative/thermomechanical stability, including a high 5% weight loss temperature (>531 °C), char residue at 800 °C (>51%), and glass transition temperature (>300 °C). Full article
(This article belongs to the Section Smart and Functional Polymers)
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Figure 1
<p>(<b>a</b>) Schematic illustration of amino-functionalized mesoporous silica (AMS) via the sol–gel reaction catalyzed in a basic medium and post-synthesis grafting method. (<b>b</b>) Transmission electron microscopy of AMS. (<b>c</b>) X-ray diffraction (XRD) patterns and (<b>d</b>) thermogravimetric analysis (TGA) curves of non-functionalized mesoporous silica (MS) and AMS.</p>
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<p>Synthesis of AMS-grafted fluorinated polyimide films.</p>
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<p>(<b>a</b>) Fourier-transform infrared spectra and (<b>b</b>) XRD patterns of the FPI-<span class="html-italic">g</span>-AMS films. (<b>c</b>) Low-magnification and (<b>d</b>) high-magnification SEM fracture surface morphologies of the FPI-<span class="html-italic">g</span>-AMS films. (<b>e</b>) Elemental mapping images of the FPI-<span class="html-italic">g</span>-AMS-3 film.</p>
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<p>(<b>a</b>) TGA curves, (<b>b</b>) storage modulus, (<b>c</b>) tan δ, determined by dynamic mechanical analysis, and (<b>d</b>) magnification region of tan δ in the range of 290–310 °C for the FPI-<span class="html-italic">g</span>-AMS-3 film.</p>
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<p>Frequency-dependent (<b>a</b>) dielectric constant (<span class="html-italic">D</span><sub>k</sub>) and (<b>b</b>) dissipation factor (<span class="html-italic">D</span><sub>f</sub>) of the FPI-<span class="html-italic">g</span>-AMS films at room temperature.</p>
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<p>(<b>a</b>) Surface static water contact angles of the FPI-<span class="html-italic">g</span>-AMS films. (<b>b</b>) Water vapor permeability of the FPI-<span class="html-italic">g</span>-AMS films as a function of time compared to the model calculated by Equation (3). Filler effects on the FPI-<span class="html-italic">g</span>-AMS films: (<b>c</b>) permeability and (<b>d</b>) diffusivity and solubility. Accordingly, the y-axis for diffusivity is on the left in black, while the y-axis for solubility is on the right in red. Each arrow indicates the direction of its respective y-axis.</p>
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