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Search Results (2,209)

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19 pages, 9326 KiB  
Article
U-Net Driven High-Resolution Complex Field Information Prediction in Single-Shot Four-Step Phase-Shifted Digital Holography Using Polarization Camera
by Askari Mehdi, Yongjun Lim, Kwan-Jung Oh and Jae-Hyeung Park
Photonics 2024, 11(12), 1172; https://doi.org/10.3390/photonics11121172 - 12 Dec 2024
Viewed by 471
Abstract
We present a novel high-resolution complex field extraction technique utilizing U-Net-based architecture to effectively overcome the inherent resolution limitations of polarization cameras with micro-polarized arrays. Our method extracts high-resolution complex field information, achieving a resolution comparable to that of the original polarization camera. [...] Read more.
We present a novel high-resolution complex field extraction technique utilizing U-Net-based architecture to effectively overcome the inherent resolution limitations of polarization cameras with micro-polarized arrays. Our method extracts high-resolution complex field information, achieving a resolution comparable to that of the original polarization camera. Utilizing the parallel phase-shifting digital holography technique, we extracted high-resolution complex field information from four high-resolution phase-shifted interference patterns predicted by our network directly at the hologram plane. Extracting the object’s complex field directly at the hologram plane rather than the object’s plane, our method eliminates the dependency on numerical propagation during dataset acquisition, enabling reconstruction of objects at various depths without DC and conjugate noise. By training the network with real-valued interference patterns and using only a single pair of low- and high-resolution input and ground truth interference patterns, we simplify computational complexity and improve efficiency. Our simulations demonstrate the network’s robustness to variations in random phase distributions and transverse shifts in the input patterns. The effectiveness of the proposed method is demonstrated through numerical simulations, showing an average improvement of over 4 dB in peak-signal-to-noise ratio and 25% in intensity normalized cross-correlation metrics for object reconstruction quality. Full article
(This article belongs to the Special Issue Holographic Information Processing)
Show Figures

Figure 1

Figure 1
<p>Schematic diagram of process flow of the proposed method.</p>
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<p>Decimation and interpolation scheme used in the training stage of the proposed method. The equation for the calculation of complex fields for the respective set of interference patterns is indicated below each group.</p>
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<p>Generation flow of training input and ground truth data.</p>
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<p>U-Net-based regression network architecture.</p>
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<p>(<b>a</b>) Training stage: a single image pair of low and high resolution from the training dataset is used. (<b>b</b>) Prediction stage: the same network is used to predict all four HR interference patterns.</p>
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<p>Amplitude and phase representation of complex field calculated from low-, predicted high-, and high-resolution phase-shifted interference patterns.</p>
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<p>Detailed flow diagram illustrating the proposed methodology step-by-step for predicting high-resolution complex field from the target images in given dataset.</p>
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<p>Low-, predicted high-, and high-resolution zero phase-shifted interference patterns with (<b>a</b>) different random phase distribution and (<b>b</b>) different transverse shifts applied to the same target image.</p>
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<p>Amplitude and phase of the object’s complex field and its image reconstruction in the following row for two test images in (<b>a</b>,<b>b</b>), and a comparison between low-, predicted high-, and high-resolution image reconstruction using the proposed method.</p>
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<p>Image reconstruction at different depths from the hologram plane for low, predicted high-, and high-resolution complex field information.</p>
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<p>Amplitude and phase of the object’s complex field and its image reconstruction in the following row for larger input image size generated from the FMNIST dataset and a comparison between low-, predicted high-, and high-resolution image reconstruction using the proposed method.</p>
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<p>Target input image in the first row of size 4416 × 4692. (<b>a</b>) Amplitude and phase of the object’s complex field and its image reconstruction in the top and bottom row for the USAF target resolution comparing low-, predicted high-, and high-resolution reconstructions with (<b>b</b>) zoomed-in images comparing low- and high-resolution (using proposed method) object reconstructions in red and yellow boxes for better visualization.</p>
Full article ">
9 pages, 13511 KiB  
Communication
Polarization-Independent Focusing Vortex Beam Generation Based on Ultra-Thin Spiral Diffractive Lens on Fiber End-Facet
by Luping Wu, Zhiyong Bai, Rui Liu, Yuji Wang, Jian Yu, Jianjun Ran, Zikai Chen, Zilun Luo, Changrui Liao, Ying Wang, Jun He, George Y. Chen and Yiping Wang
Photonics 2024, 11(12), 1167; https://doi.org/10.3390/photonics11121167 - 11 Dec 2024
Viewed by 395
Abstract
An ultra-thin spiral diffractive lens (SDL) was fabricated by using focused ion beam milling on a fiber end-facet coated with a 100 nm thick Au film. Focusing vortex beams (FVBs) were successfully excited by the SDLs due to the coherent superposition of diffracted [...] Read more.
An ultra-thin spiral diffractive lens (SDL) was fabricated by using focused ion beam milling on a fiber end-facet coated with a 100 nm thick Au film. Focusing vortex beams (FVBs) were successfully excited by the SDLs due to the coherent superposition of diffracted waves and their azimuth dependence of the phase accumulated from the spiral aperture to the beam axis. The polarization and phase characteristics of the FVBs were experimentally investigated. Results show that the input beams with various polarization states were converted to FVBs, whose polarization states were the same as those of the input beams. Furthermore, the focal length of the SDL and the in-tensity and phase distribution at the focus spot of the FVBs were numerically simulated by the FDTD method in the ultra-wide near-infrared waveband from 1300 nm to 1800 nm. The focal length was tuned from 21.8 μm to 14.7 μm, the intensity profiles exhibited a doughnut-like shape, and the vortex phase was converted throughout the broadband range. The devices are expected to be candidates for widespread applications including optical communications, optical imaging, and optical tweezers. Full article
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Figure 1

Figure 1
<p>(<b>a</b>) The schematic diagram of SDL with <span class="html-italic">l</span> = 1; (<b>b</b>) simulated intensity distribution at the focal spot for <span class="html-italic">l</span> = 1; (<b>c</b>) the phase distribution at the focal spot for <span class="html-italic">l</span> = 1; (<b>d</b>) The schematic diagram of SDL with <span class="html-italic">l</span> = 2; (<b>e</b>) simulated intensity distribution at the focal spot for <span class="html-italic">l</span> = 2; (<b>f</b>) the phase distribution at the focal spot for <span class="html-italic">l</span> = 2.</p>
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<p>(<b>a</b>) Schematic diagram of the structure of the SDL fabricated on the multimode fiber end-facet; (<b>b</b>) calculation and experimental measurement of divergence angles <span class="html-italic">θ</span> of output beams from the GIF with different lengths; (<b>c</b>) intensity distribution of outputting beam from the GIF about 400 μm long.</p>
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<p>(<b>a</b>,<b>b</b>) SEM images of SDLs fabricated with <span class="html-italic">l</span> = 1 and 2 on the fiber end-facet, respectively; (<b>c</b>) schematic diagram of the measurement system to characterize the outputting beam; (<b>d</b>) measured intensity distribution at the focal spot for <span class="html-italic">l</span> = 1; (<b>e</b>) measured interference patterns between the focal spot and an extended Gaussian beam for <span class="html-italic">l</span> = 1; (<b>f</b>) measured intensity distribution at the focal spot for <span class="html-italic">l</span> = 2; (<b>g</b>) measured interference patterns between the focal spot and an extended Gaussian beam for <span class="html-italic">l</span> = 2.</p>
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<p>Measured intensity distribution and the interference patterns with different polarization state beams injected into the hybrid fiber. (<b>a</b>) <span class="html-italic">l</span> = 1; (<b>b</b>) <span class="html-italic">l</span> = 2.</p>
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<p>Simulated results for the focusing characteristics of the SDL with <span class="html-italic">l</span> = 2, under different wavelengths: (<b>a</b>) 1300 nm, (<b>b</b>) 1400 nm, (<b>c</b>) 1500 nm, (<b>d</b>) 1600 nm, (<b>e</b>) 1700, and (<b>f</b>) 1800 nm. The panels in the first two rows depict the phase distribution and intensity distribution at the focal spot, respectively; the panels in the bottom row illustrate the intensity distributions in the (<span class="html-italic">x</span>, <span class="html-italic">z</span>) plane.</p>
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15 pages, 14778 KiB  
Article
Localized Vector Optical Nondiffracting Subcycle Pulses
by Klemensas Laurinavičius and Sergej Orlov
Appl. Sci. 2024, 14(24), 11538; https://doi.org/10.3390/app142411538 - 11 Dec 2024
Viewed by 452
Abstract
Structured light is essential in various fields such as imaging, communications, computing, laser microprocessing, and ultrafast and nonlinear optics. The structuring of light can occur in terms of space, amplitude, phase, polarization, time, frequency, and duration. One of the intriguing properties that can [...] Read more.
Structured light is essential in various fields such as imaging, communications, computing, laser microprocessing, and ultrafast and nonlinear optics. The structuring of light can occur in terms of space, amplitude, phase, polarization, time, frequency, and duration. One of the intriguing properties that can be obtained is resistance to the diffractive spread and dispersive broadening of the pulsed beams. This happens when temporal properties such as frequency are coupled with spatial properties like angles of propagation of plane-wave components. In this case, pulsed light beams exhibit characteristics similar to optical bullets, resisting both diffraction and material dispersion. This study questions whether free-space optical bullets that possess nondiffracting and nondispersive properties are possible with subcycle durations. We report on the possibility to create nondiffracting and nondispersing localized subcycle pulsed beams and their complex polarization topologies when controlling the group velocity of these light structures. Full article
(This article belongs to the Special Issue Ultrafast and Nonlinear Laser Applications)
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Figure 1

Figure 1
<p>(<b>a</b>) Dependency of the parameter <math display="inline"><semantics> <mrow> <mo>Δ</mo> <mi>ω</mi> <mo>/</mo> <msub> <mi>ω</mi> <mi>c</mi> </msub> </mrow> </semantics></math> for focus wave modes on the parameters <math display="inline"><semantics> <mi>γ</mi> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> </mrow> </semantics></math> in vacuum; (<b>b</b>) dependency of the parameter <math display="inline"><semantics> <mrow> <mo>Δ</mo> <mi>ω</mi> <mo>/</mo> <msub> <mi>ω</mi> <mi>c</mi> </msub> </mrow> </semantics></math> for focus wave modes on the parameters <math display="inline"><semantics> <mi>γ</mi> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> </mrow> </semantics></math> in BK7 glass. (<b>c</b>) Angular dispersion curves of focus wave modes in vacuum for parameters: (<b>1</b>) blue curve <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> <mo>=</mo> <mn>3.45</mn> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mn>0</mn> <mspace width="3.33333pt"/> <msup> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; (<b>2</b>) red curve <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> <mo>=</mo> <mo>−</mo> <mn>5.65</mn> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mn>4.35</mn> <mspace width="3.33333pt"/> <msup> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; (<b>3</b>) orange curve <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mo>−</mo> <mn>2.45</mn> <mspace width="3.33333pt"/> <msup> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>.</p>
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<p>Intensity distributions of subcycle pulses in vacuum and their individual components <math display="inline"><semantics> <msub> <mi>E</mi> <mi>x</mi> </msub> </semantics></math> (second row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>y</mi> </msub> </semantics></math> (third row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>z</mi> </msub> </semantics></math> (fourth row) in the transverse plane for linear TE (first column), TM (second column), azimuthal (third column), and radial (fourth column) polarizations when <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> <mo>=</mo> <mn>3.45</mn> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mn>0</mn> <mspace width="3.33333pt"/> <msup> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>. The white arrows in first row represent the orientation of the electric field. The insets represent the phase distributions of the individual components.</p>
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<p>Intensity distributions of subcycle pulses in vacuum and their individual components (<math display="inline"><semantics> <msub> <mi>E</mi> <mi>x</mi> </msub> </semantics></math> (second row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>y</mi> </msub> </semantics></math> (third row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>z</mi> </msub> </semantics></math> (fourth row)) in the longitudinal plane for linear TE (first column), TM (second column), azimuthal (third column), and radial (fourth column) polarizations when <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> <mo>=</mo> <mn>3.45</mn> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mn>0</mn> <mspace width="3.33333pt"/> <msup> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>. The insets represent the phase distribution for each individual component.</p>
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<p>Intensity distributions of subcycle pulses in vacuum and their individual components <math display="inline"><semantics> <msub> <mi>E</mi> <mi>x</mi> </msub> </semantics></math> (second row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>y</mi> </msub> </semantics></math> (third row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>z</mi> </msub> </semantics></math> (fourth row) in the transverse plane for linear TE (first column), TM (second column), azimuthal (third column), and radial (fourth column) polarizations when <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> <mo>=</mo> <mo>−</mo> <mn>5.65</mn> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mn>4.35</mn> <mspace width="3.33333pt"/> <msup> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>. The white arrows in first row represent the orientation of the electric field. The insets represent the phase distribution.</p>
Full article ">Figure 5
<p>Intensity distributions of subcycle pulses in vacuum and their individual components (<math display="inline"><semantics> <msub> <mi>E</mi> <mi>x</mi> </msub> </semantics></math> (second row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>y</mi> </msub> </semantics></math> (third row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>z</mi> </msub> </semantics></math> (fourth row)) in the longitudinal plane for linear TE (first column), TM (second column), azimuthal (third column), and radial (fourth column) polarizations when <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> <mo>=</mo> <mo>−</mo> <mn>5.65</mn> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mn>4.35</mn> <mspace width="3.33333pt"/> <msup> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>. The insets represent the phase distribution.</p>
Full article ">Figure 6
<p>Intensity distributions of subcycle pulses in vacuum and their individual components <math display="inline"><semantics> <msub> <mi>E</mi> <mi>x</mi> </msub> </semantics></math> (second row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>y</mi> </msub> </semantics></math> (third row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>z</mi> </msub> </semantics></math> (fourth row) in the transverse plane for linear TE (first column), TM (second column), azimuthal (third column), and radial (fourth column) polarizations when <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mo>−</mo> <mn>2.45</mn> <mspace width="3.33333pt"/> <msup> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>. The white arrows in first row represent the orientation of the electric field. The insets represent the phase distribution.</p>
Full article ">Figure 7
<p>Intensity distributions of subcycle pulses in vacuum and their individual components (<math display="inline"><semantics> <msub> <mi>E</mi> <mi>x</mi> </msub> </semantics></math> (second row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>y</mi> </msub> </semantics></math> (third row), <math display="inline"><semantics> <msub> <mi>E</mi> <mi>z</mi> </msub> </semantics></math> (fourth row)) in the longitudinal plane for linear TE (first column), TM (second column), azimuthal (third column), and radial (fourth column) polarizations when <math display="inline"><semantics> <mrow> <mi>V</mi> <mo>/</mo> <mi>c</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mo>−</mo> <mn>2.45</mn> <mspace width="3.33333pt"/> <msup> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>. The insets represent the phase distribution.</p>
Full article ">
22 pages, 5444 KiB  
Article
Pre-Launch Thermal Emissive Band Radiometric Performance for JPSS-3 and -4 VIIRS
by David Moyer, Amit Angal, Jeff McIntire and Xiaoxiong Xiong
Remote Sens. 2024, 16(24), 4630; https://doi.org/10.3390/rs16244630 - 11 Dec 2024
Viewed by 331
Abstract
The Joint Polar Satellite System 3 (JPSS-3) and 4 (JPSS-4) Visible Infrared Imaging Radiometer Suite (VIIRS) are the fourth and fifth in its series of instruments designed to provide high-quality data products for environmental and climate data records. The VIIRS instrument must be [...] Read more.
The Joint Polar Satellite System 3 (JPSS-3) and 4 (JPSS-4) Visible Infrared Imaging Radiometer Suite (VIIRS) are the fourth and fifth in its series of instruments designed to provide high-quality data products for environmental and climate data records. The VIIRS instrument must be calibrated and characterized prior to launch to meet the data product needs. A comprehensive test program was conducted at the Raytheon Technologies facility in 2020 (JPSS-3) and 2023 (JPSS-4) that included extensive functional and environmental testing. The thermal band radiometric pre-launch performance and stability are the focus of this article, which also compares several instrument performance metrics to the design requirements. Brief comparisons with the JPSS-1 and -2 VIIRS instrument performance will also be discussed. Full article
(This article belongs to the Collection The VIIRS Collection: Calibration, Validation, and Application)
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Figure 1

Figure 1
<p>VIIRS internal layout showing the optical elements, FPAs, and calibration target locations.</p>
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<p>VIIRS sector views showing where the EV, SV, and OBCBB view are within the scan.</p>
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<p>The standard deviation of the six thermistors in the on-board blackbody (OBCBB) plotted versus instrument temperature for each JPSS instrument build.</p>
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<p>The JPSS-3 VIIRS offset corrected detector response (<b>a</b>) and the radiance residual in percent (<b>b</b>) are shown versus path difference radiance for the MWIR. The symbols in (<b>a</b>) represent measured data and the lines indicate quadratic fits. The data are from nominal plateau, electronics side A, FPA temperature 80 K averaged over all detectors.</p>
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<p>The JPSS-4 VIIRS offset corrected detector response (<b>a</b>) and the radiance residual in percent (<b>b</b>) are shown versus path difference radiance for the MWIR. The symbols in (<b>a</b>) represent measured data and the lines indicate quadratic fits. The data are from nominal plateau, electronics side A, FPA temperature 80 K averaged over all detectors.</p>
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<p>The JPSS-3 VIIRS offset corrected detector response (<b>a</b>) and the radiance residual in percent (<b>b</b>) are shown versus path difference radiance for the LWIR. The symbols in (<b>a</b>) represent measured data and the lines indicate quadratic fits. The data are from nominal plateau, electronics side A, FPA temperature 80 K averaged over all detectors.</p>
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<p>The JPSS-4 VIIRS offset corrected detector response (<b>a</b>) and the radiance residual in percent (<b>b</b>) are shown versus path difference radiance for the LWIR. The symbols in (<b>a</b>) represent measured data and the lines indicate quadratic fits. The data are from nominal plateau, electronics side A, FPA temperature 80 K averaged over all detectors.</p>
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<p>JPSS-3 VIIRS detector averaged <span class="html-italic">NEdT</span> as a function of scene temperature for the MWIR (<b>top</b>) and LWIR bands (<b>bottom</b>) from nominal plateau, HAM side A, electronics side A, FPA temperature 80 K.</p>
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<p>JPSS-4 VIIRS detector averaged <span class="html-italic">NEdT</span> as a function of scene temperature for the MWIR (<b>top</b>) and LWIR bands (<b>bottom</b>) from nominal plateau, HAM side A, electronics side A, FPA temperature 80 K.</p>
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<p>JPSS-3 VIIRS TEB uniformity metric as a function of scene temperature for the MWIR (<b>top</b>) and LWIR (<b>bottom</b>) bands for nominal TV plateau, HAM side A, electronics side A, FPA temperature 80 K using the worst-case detector. The solid horizontal red line corresponds to the instrument uniformity requirement.</p>
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<p>JPSS-4 VIIRS TEB uniformity metric as a function of scene temperature for the MWIR (<b>top</b>) and LWIR (<b>bottom</b>) bands for nominal TV plateau, HAM side A, electronics side A, FPA temperature 80 K using the worst-case detector. The solid horizontal red line corresponds to the instrument uniformity requirement.</p>
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<p>JPSS-3 VIIRS TEB modeled brightness temperature uncertainty as a function of scene temperature for the MWIR (<b>a</b>) and LWIR bands (<b>b</b>).</p>
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<p>JPSS-4 VIIRS TEB modeled brightness temperature uncertainty as a function of scene temperature for the MWIR (<b>a</b>) and LWIR bands (<b>b</b>).</p>
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13 pages, 16111 KiB  
Article
Simple Design of Polarization-Selective Tunable Triple Terahertz Absorber Based on Graphene Rectangular Ring Resonator
by Jiang Wang, Haixia Zhu, Bo Ni, Minhao Zhou, Chengtao Feng, Haibin Ni and Jianhua Chang
Photonics 2024, 11(12), 1160; https://doi.org/10.3390/photonics11121160 - 9 Dec 2024
Viewed by 388
Abstract
In this paper, a simple design of a polarization-selective tunable triple terahertz absorber based on a graphene rectangular ring resonator was proposed and studied. The absorber structure consists of a graphene rectangular ring resonant array on the top, SiO2 dielectric layer in [...] Read more.
In this paper, a simple design of a polarization-selective tunable triple terahertz absorber based on a graphene rectangular ring resonator was proposed and studied. The absorber structure consists of a graphene rectangular ring resonant array on the top, SiO2 dielectric layer in the middle and gold at the bottom. The calculated results show that the absorber can achieve high-efficiency triple-band absorption under both x and y polarization incident light. When x-polarized light is incident, three distinctive absorption peaks at 2.73, 5.70 and 11.19 THz with absorption rates of 96.7%, 98.5% and 96.5% are achieved. When y-polarized light is incident, three additional absorption peaks at 2.29, 7.55 and 9.98 THz can be obtained with absorption rates of 96.3%, 90.3% and 97.4%, respectively. Moreover, the absorption wavelength of the absorber can be tuned by adjusting the chemical potential of the graphene. Owing to the high efficiency of triple-band absorption in different polarization states, the absorber has broad application prospects in terahertz polarization imaging, sensing and detection. Full article
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Figure 1

Figure 1
<p>Structure of the absorber. (<b>a</b>) Schematic diagram; (<b>b</b>) top view of the unit (<span class="html-italic">x-y</span> plane).</p>
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<p>(<b>a</b>) Absorption spectra of different polarization incidence Q, where the black line represents <span class="html-italic">x</span> polarization and the red line represents <span class="html-italic">y</span> polarization. (<b>b</b>) Variation of Q factor and FWHM of peaks with frequency.</p>
Full article ">Figure 3
<p>Equivalent impedance diagram of different polarization incidence: (<b>a</b>) <span class="html-italic">x</span> polarization; (<b>b</b>) <span class="html-italic">y</span> polarization.</p>
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<p>The absorption spectra of different Fermi levels of graphene: (<b>a</b>) <span class="html-italic">x</span> polarization; (<b>b</b>) <span class="html-italic">y</span> polarization.</p>
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<p>(<b>a</b>) The absorption spectra at different polarization angles and (<b>b</b>) the maximum absorption of the correlated peaks at different polarization angles.</p>
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<p>The distribution of electric field |E| and magnetic field |H| in the <span class="html-italic">x</span>-<span class="html-italic">y</span> plane, as well as the magnetic field |H| in the <span class="html-italic">x</span>-<span class="html-italic">z</span> plane at the <span class="html-italic">x</span> polarization absorption frequency of (<b>a</b>–<b>c</b>) 2.73 THz, (<b>d</b>–<b>f</b>) 5.70 THz, and (<b>g</b>–<b>i</b>) 11.19 THz, respectively.</p>
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<p>The distribution of electric field |E| and magnetic field |H| in the <span class="html-italic">x</span>-<span class="html-italic">y</span> plane, as well as the magnetic field |H| in the <span class="html-italic">x</span>-<span class="html-italic">z</span> plane at the <span class="html-italic">x</span> polarization absorption frequency of (<b>a</b>–<b>c</b>) 2.73 THz, (<b>d</b>–<b>f</b>) 5.70 THz, and (<b>g</b>–<b>i</b>) 11.19 THz, respectively.</p>
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<p>The distribution of electric field |E| and magnetic field |H| in the <span class="html-italic">x-y</span> plane, as well as the magnetic field |H| in the <span class="html-italic">x-z</span> plane at the <span class="html-italic">y</span> polarization absorption frequency of (<b>a</b>–<b>c</b>) 2.29 THz, (<b>d</b>–<b>f</b>) 7.55 THz, and (<b>g</b>–<b>i</b>) 9.98 THz, respectively.</p>
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<p>The distribution of electric field |E| and magnetic field |H| in the <span class="html-italic">x-y</span> plane, as well as the magnetic field |H| in the <span class="html-italic">x-z</span> plane at the <span class="html-italic">y</span> polarization absorption frequency of (<b>a</b>–<b>c</b>) 2.29 THz, (<b>d</b>–<b>f</b>) 7.55 THz, and (<b>g</b>–<b>i</b>) 9.98 THz, respectively.</p>
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<p>The absorption spectra of different SiO<sub>2</sub> thickness for (<b>a</b>) <span class="html-italic">x</span> polarization and (<b>b</b>) <span class="html-italic">y</span> polarization.</p>
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<p>The absorption spectra of different length (<span class="html-italic">a</span><sub>1</sub>) of graphene horizontal strip for (<b>a</b>) <span class="html-italic">x</span> polarization and (<b>b</b>) <span class="html-italic">y</span> polarization.</p>
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<p>The absorption spectra of different graphene vertical bar widths (<span class="html-italic">b</span><sub>1</sub>) for (<b>a</b>) <span class="html-italic">x</span> polarization and (<b>b</b>) <span class="html-italic">y</span> polarization.</p>
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8 pages, 1914 KiB  
Article
A Reconfigurable Polarimetric Photodetector Based on the MoS2/PdSe2 Heterostructure with a Charge-Trap Gate Stack
by Xin Huang, Qinghu Bai, Yang Guo, Qijie Liang, Tengzhang Liu, Wugang Liao, Aizi Jin, Baogang Quan, Haifang Yang, Baoli Liu and Changzhi Gu
Nanomaterials 2024, 14(23), 1936; https://doi.org/10.3390/nano14231936 - 1 Dec 2024
Viewed by 585
Abstract
Besides the intensity and wavelength, the ability to analyze the optical polarization of detected light can provide a new degree of freedom for numerous applications, such as object recognition, biomedical applications, environmental monitoring, and remote sensing imaging. However, conventional filter-integrated polarimetric sensing systems [...] Read more.
Besides the intensity and wavelength, the ability to analyze the optical polarization of detected light can provide a new degree of freedom for numerous applications, such as object recognition, biomedical applications, environmental monitoring, and remote sensing imaging. However, conventional filter-integrated polarimetric sensing systems require complex optical components and a complicated fabrication process, severely limiting their on-chip miniaturization and functionalities. Herein, the reconfigurable polarimetric photodetection with photovoltaic mode is developed based on a few-layer MoS2/PdSe2 heterostructure channel and a charge-trap structure composed of Al2O3/HfO2/Al2O3 (AHA)-stacked dielectrics. Because of the remarkable charge-trapping ability of carriers in the AHA stack, the MoS2/PdSe2 channel exhibits a high program/erase current ratio of 105 and a memory window exceeding 20 V. Moreover, the photovoltaic mode of the MoS2/PdSe2 Schottky diode can be operated and manipulable, resulting in high and distinct responsivities in the visible broadband. Interestingly, the linear polarization of the device can be modulated under program/erase states, enabling the reconfigurable capability of linearly polarized photodetection. This study demonstrates a new prototype heterostructure-based photodetector with the capability of both tunable responsivity and linear polarization, demonstrating great potential application toward reconfigurable photosensing and polarization-resolved imaging applications. Full article
(This article belongs to the Special Issue 2D Materials for Advanced Sensors: Fabrication and Applications)
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<p>Schematics and characterization of the MoS<sub>2</sub>/PdSe<sub>2</sub> heterostructure device: (<b>a</b>,<b>b</b>) Schematic and picture of MoS<sub>2</sub>/PdSe<sub>2</sub> heterostructure photodetector. The scale bar is 20 μm; (<b>c</b>) Raman spectra of the multilayer MoS<sub>2</sub> flakes, PdSe<sub>2</sub> flakes, and heterostructure, respectively; (<b>d</b>,<b>e</b>) I<sub>ds</sub>–V<sub>ds</sub> relationship of MoS<sub>2</sub> and PdSe<sub>2</sub>, respectively; (<b>f</b>) the transfer characteristics of the MoS<sub>2</sub>/PdSe<sub>2</sub> heterostructure under the bias of −3 V and schematic of the MoS<sub>2</sub>/PdSe<sub>2</sub> heterostructure-based Schottky barrier.</p>
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<p>The statical behavior of the nonvolatile gate charge-trap memory based on MoS<sub>2</sub>/PdSe<sub>2</sub> heterostructure: (<b>a</b>) I<sub>ds</sub>–V<sub>G</sub> characteristics of the device under different V<sub>G</sub> at V<sub>ds</sub> = −1 V; (<b>b</b>) extraction of memory window ∆V vs. V<sub>G</sub>. The memory window increases from 1 to ∼20 V in our experimental settings; (<b>c</b>) band diagram of the program/erase state of the device under positive and negative V<sub>G</sub>. Positive V<sub>G</sub> programs the device. Electrons tunneling from the few-layer MoS<sub>2</sub> channel are accumulated in the HfO<sub>2</sub> charge-trap layer. Negative V<sub>G</sub> erases the device. Holes tunnel from the few-layer MoS<sub>2</sub> channel to the HfO<sub>2</sub> charge-trap layer.</p>
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<p>The dynamic behavior of the nonvolatile gate charge-trap memory based on MoS<sub>2</sub>/PdSe<sub>2</sub> heterostructure: (<b>a</b>,<b>b</b>) I<sub>ds</sub>–V<sub>G</sub> characteristics of the device under different V<sub>G</sub> under the forward bias of −1 V and reverse bias of +1 V, respectively; (<b>c</b>,<b>d</b>) I<sub>ds</sub>–V<sub>ds</sub> characteristics of the device under different pulse durations and amplitudes.</p>
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<p>The polarization-modulated photovoltaic behavior of MoS<sub>2</sub>/PdSe<sub>2</sub> photodetector: (<b>a</b>,<b>b</b>) Short-circuit current I<sub>sc</sub> and open-circuit voltage V<sub>oc</sub> of MoS<sub>2</sub>/PdSe<sub>2</sub> photodetector under the program and erase state, respectively. (<b>c</b>,<b>d</b>) Dependency of responsibility and linear polarization with gate voltage V<sub>G</sub> under different program/erase states and polarization directions of light.</p>
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<p>Photoresponse mechanism of reconfigurable MoS<sub>2</sub>/PdSe<sub>2</sub> photodetector: (<b>a</b>) The energy band structure of AHA charge-trap stack and MoS<sub>2</sub>/PdSe<sub>2</sub> heterostructure before contact; (<b>b</b>,<b>c</b>) the energy band structure of the device and the flow of photo-generated electron-holes under illumination when the device is set to erase (V<sub>G</sub> &lt; 0) and program states (V<sub>G</sub> &gt; 0), respectively.</p>
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14 pages, 5075 KiB  
Article
Multimode Miniature Polarization-Sensitive Metamaterial Absorber with Ultra-Wide Bandwidth in the K Band
by Zhonghang Ji, Yida Song, Mandi Gao, Qiong Zhang and Yunqing Liu
Micromachines 2024, 15(12), 1446; https://doi.org/10.3390/mi15121446 - 29 Nov 2024
Viewed by 469
Abstract
Metamaterial absorbers have gained widespread applications in fields such as sensing, imaging, and electromagnetic cloaking due to their unique absorption characteristics. This paper presents the design and fabrication of a novel K-band polarization-sensitive metamaterial absorber, which operates in the frequency range of 20.76 [...] Read more.
Metamaterial absorbers have gained widespread applications in fields such as sensing, imaging, and electromagnetic cloaking due to their unique absorption characteristics. This paper presents the design and fabrication of a novel K-band polarization-sensitive metamaterial absorber, which operates in the frequency range of 20.76 to 24.20 GHz for both TE and TM modes, achieving an absorption rate exceeding 90% and a bandwidth of up to 3.44 GHz. The structure of the metamaterial absorber consists of a rectangular aperture metallic patch, two metallic rings, and two metallic strips, with a metallic patch structure on the back. Both metallic patches are printed on a 1.575 mm-thick FR-4 substrate. In the TE mode, the performance shows diagonal symmetry, with a minimum absorption bandwidth of 1.4 GHz at 45° and a maximum of 3.44 GHz at 0°. The absorption rate exceeds 90% across various polarization angles. In terms of conventional modes, both the TE and TM modes can achieve ultra-wideband absorption. For specific scenarios requiring single-frequency or multi-frequency absorption, the desired functionality can be realized by varying the incident angle. These exceptional characteristics confer strong applicability for high-bandwidth electromagnetic wave absorption and specific frequency point absorption, indicating significant potential and practical value in the field of wireless communication. Full article
(This article belongs to the Special Issue Functional Materials and Microdevices)
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<p>(<b>a</b>) Front view of the metamaterial. (<b>b</b>) Side view of the metamaterial.</p>
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<p>(<b>a</b>) Steps for absorber design. (<b>b</b>) Absorption rate curves for each step. (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>S</mi> <mrow> <mn>11</mn> </mrow> </msub> </mrow> </semantics></math> curves for each step.</p>
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<p>(<b>a</b>) Equivalent circuit diagram. (<b>b</b>) Comparison of ADS and CST simulation results.</p>
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<p>The effective parameters of the metamaterials in the frequency range of 18 GHz to 26 GHz. The blue dashed line represents the real part, and the black dashed line represents the imaginary part. (<b>a</b>) Normalized impedance. (<b>b</b>) Permeability. (<b>c</b>) Refractive index. (<b>d</b>) Permittivity.</p>
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<p>An illustration of the real parts of the permittivity and permeability in the frequency range of 18 GHz to 26 GHz. The black dot–dash line represents the real part of the permittivity, and the blue line represents the real part of the permeability.</p>
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<p>From left to right are the electric field, magnetic field, and surface current for the TM mode and TE mode, respectively.</p>
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<p>Different polarization angles and oblique incidence absorption curves for TE and TM modes: (<b>a</b>) TE mode with varying polarization angles. (<b>b</b>) TE mode with oblique incidence of electromagnetic waves. (<b>c</b>) TM mode with varying polarization angles. (<b>d</b>) TM mode with oblique incidence of electromagnetic waves.</p>
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<p>(<b>a</b>) Physical structure (<b>b</b>) Testing environment.</p>
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<p>Experimental and simulation results of 18–26 GHz frequency range. (<b>a</b>) Normal incidence of electromagnetic waves; blue dashed line represents experimental results, and red solid line represents simulation results. (<b>b</b>) Experimental and simulation results for different polarization angles; dash–dot line represents simulation results, and solid line represents experimental results. (<b>c</b>) Experimental and simulation results for oblique incidence; dash–dot line represents simulation results, and solid line represents experimental results.</p>
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20 pages, 4507 KiB  
Article
Enhanced Polarimetric Radar Vegetation Index and Integration with Optical Index for Biomass Estimation in Grazing Lands Across the Contiguous United States
by Jisung Geba Chang, Simon Kraatz, Martha Anderson and Feng Gao
Remote Sens. 2024, 16(23), 4476; https://doi.org/10.3390/rs16234476 - 28 Nov 2024
Viewed by 445
Abstract
Grazing lands are crucial for agricultural productivity, ecological stability, and carbon sequestration, underscoring the importance of monitoring vegetation biomass for the effective management of these ecosystems. Remote sensing data, including optical vegetation indices (VIs) like the Normalized Difference Vegetation Index (NDVI), are widely [...] Read more.
Grazing lands are crucial for agricultural productivity, ecological stability, and carbon sequestration, underscoring the importance of monitoring vegetation biomass for the effective management of these ecosystems. Remote sensing data, including optical vegetation indices (VIs) like the Normalized Difference Vegetation Index (NDVI), are widely used to monitor vegetation dynamics due to their simplicity and high sensitivity. In contrast, radar-based VIs, such as the Polarimetric Radar Vegetation Index (PRVI), offer additional advantages, including all-weather imaging capabilities, a wider saturation range, and sensitivity to the vegetation structure information. This study introduces an enhanced form of the PRVI, termed the Normalized PRVI (NPRVI), which is calibrated to a 0 to 1 range, constraining the minimum value to reduce the background effects. The calibration and range factor were derived from statistical analysis of PRVI components across vegetated regions in the Contiguous United States (CONUS), using dual-polarization C-band Sentinel-1 and L-band ALOS-PALSAR data on the Google Earth Engine (GEE) platform. Machine learning models using NPRVI and NDVI demonstrated their complementarity with annual herbaceous biomass data from the Rangeland Analysis Platform. The results showed that the Random Forest Model outperformed the other machine learning models tested, achieving R2 ≈ 0.51 and MAE ≈ 498 kg/ha (relative MAE ≈ 32.1%). Integrating NPRVI with NDVI improved biomass estimation accuracy by approximately 10% compared to using NDVI alone, highlighting the added value of incorporating radar-based vegetation indices. NPRVI may enhance the monitoring of grazing lands with relatively low biomass compared to other vegetation types, while also demonstrating applicability across a broad range of biomass levels and in diverse vegetation covers. Full article
(This article belongs to the Section Remote Sensing in Agriculture and Vegetation)
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<p>Distribution of vegetated regions across the CONUS from NLCD2021 (<b>upper</b>) and annual herbaceous above-ground biomass from RAP for the year 2022 (<b>lower</b>).</p>
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<p>Distribution of Degree of Polarization (DOP) and cross-polarization backscattering coefficient (<math display="inline"><semantics> <mrow> <msubsup> <mrow> <mi mathvariant="sans-serif">σ</mi> </mrow> <mrow> <mn>0</mn> </mrow> <mrow> <mi mathvariant="normal">h</mi> <mi mathvariant="normal">v</mi> </mrow> </msubsup> </mrow> </semantics></math> or <math display="inline"><semantics> <mrow> <msubsup> <mrow> <mi mathvariant="sans-serif">σ</mi> </mrow> <mrow> <mn>0</mn> </mrow> <mrow> <mi mathvariant="normal">v</mi> <mi mathvariant="normal">h</mi> </mrow> </msubsup> </mrow> </semantics></math>) for Sentinel-1 (C-band) and PALSAR (L-band) across different vegetation types.</p>
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<p>Correlation (Pearson R) heatmap illustrating the relationships between NPRVI, NDVI indices, and reference annual biomass across various seasons for 2022.</p>
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<p>Density plots of NPRVI derived from Sentinel-1 and NDVI derived from HLS data against annual herbaceous AGB (kg/ha) across grazing lands of the CONUS, along with corresponding histograms. The biomass range of herbaceous AGB is 0–5000 kg/ha, with low biomass defined as 0–400 kg/ha (12.66%), medium biomass as 400–1800 kg/ha (57.87%), and high biomass as 1800–5000 kg/ha (29.47%). The data were randomly sampled from 10,000 pixels.</p>
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<p>Comparison of machine learning models (MLR, RFM, XGBoost, DNN) for biomass estimation using all vegetation indices. Metrics include mean R<sup>2</sup> (<b>red</b>) and mean MAE (<b>blue</b>).</p>
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<p>NPRVI difference (NPRVI<sub>C</sub> − NPRVI<sub>L</sub>) ranges from −0.3 (indicating higher L-band values, shown in red) to 0.3 (indicating lower L-band values than C-band value, shown in blue). White strip regions in the mosaic figure indicate missing images from SAR data, primarily from PALSAR imagery.</p>
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<p>Range of NPRVIs and their differences (NPRVI<sub>C</sub> − NPRVI<sub>L</sub>) for each vegetation type based on the NLCD dataset. The violin plots show the distribution and density of NPRVI values, while the box plots indicate the median and interquartile range (IQR), with whiskers extending to 95% of the data. These plots capture both the central tendency and variability for each vegetation type.</p>
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<p>Multi-temporal trends of NDVI from HLS and NPRVI from Sentinel-1 at the upper part, and cross-ratio (VH/VV) and (1-DOP) at the lower part, between 1 January 2022 and 31 July 2024, with data points every 16 days: averages from 100 randomly selected regions in the grazing lands of the CONUS, with the dotted line representing the average values and the light shading indicating ±0.2 standard deviations.</p>
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24 pages, 25933 KiB  
Article
Accurate Paddy Rice Mapping Based on Phenology-Based Features and Object-Based Classification
by Jiayi Zhang, Lixin Gao, Miao Liu, Yingying Dong, Chongwen Liu, Raffaele Casa, Stefano Pignatti, Wenjiang Huang, Zhenhai Li, Tingting Tian and Richa Hu
Remote Sens. 2024, 16(23), 4406; https://doi.org/10.3390/rs16234406 - 25 Nov 2024
Viewed by 600
Abstract
Highly accurate rice cultivation distribution and area extraction are essential to food security. Moreover, Inner Mongolia, whose slogan is “from scientific rice to world rice”, is an essential national rice production base. However, high-quality rice mapping products at high resolutions are still scarce [...] Read more.
Highly accurate rice cultivation distribution and area extraction are essential to food security. Moreover, Inner Mongolia, whose slogan is “from scientific rice to world rice”, is an essential national rice production base. However, high-quality rice mapping products at high resolutions are still scarce around the Inner Mongolia Autonomous Region. This condition is not conducive to rational planning of farmland resources, maintaining food security, and promoting sustainable growth of the local agricultural economy. In this study, the rice backscattering intensity difference index from the vertically polarized backscatter intensity of Sentinel-1 and the phenology differential index from the spectral indices of two critical rice phenological phases of Sentinel-2 images were constructed. Other spectral features, including spectral indices, tasseled cap, and texture features, were computed using simple non-iterative clustering (SNIC) to achieve image segmentation. These variables served as input features for the random forest (RF) algorithm. Results reveal that employing the RF with the SNIC segmentation algorithm and combining it with optical and synthetic aperture radar data is an effective way to extract data on rice in mid-latitude regions. The overall accuracy and kappa coefficient are 0.98 and 0.967, correspondingly. The accuracy for rice is 0.99, as proven by empirical data. These results meet the requirements of regional rice cultivation assessment and area monitoring. Furthermore, owing to its resilience against longitude-associated influences, the model discerns rice across diverse regions and multiple years, achieving an R2 of 0.99. This capability significantly bolsters efforts to improve regional food security and the pursuit of sustainable development. Full article
(This article belongs to the Section Remote Sensing in Agriculture and Vegetation)
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<p>(<b>a</b>) The study area and the tiles covered Hinggan League; (<b>b</b>) paddy rice sample points.</p>
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<p>The methodological workflow of the research.</p>
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<p>Sentinel-2 characteristic vegetation index time-series curve and S-G filtering effect plot (<b>left</b>); Sentinel-1 VH Backscatter Time-series Curve and S-G filtering effect plot (<b>right</b>).</p>
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<p>Time trends of some indices from optical data (<b>top</b>), backscattering (<b>center</b>), and during the different growth phases of rice (<b>bottom</b>), which cover the whole growth period.</p>
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<p>Statistical results of physical difference indices for different land cover types: (<b>a</b>) NDVI, NDWI differences for different features; (<b>b</b>) REI (“Outliers” mean’s abnormal values); (<b>c</b>) VH differences for different features; (<b>d</b>) SREI.</p>
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<p>The comparison among segmentation results from different seed pixel pitches.</p>
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<p>Contribution of feature variables ((<b>A</b>) Tqx, (<b>B</b>) Wlht, (<b>C</b>) Zltq, (<b>D</b>) Keqyyzq, (<b>E</b>) Keqyyqq, (<b>F</b>) Synthesize).</p>
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<p>Classification results of different combinations. (<b>a</b>) Comparison of rice extraction results from different method combinations (<b>b</b>) Comparison of rice extraction areas from the four combinations with official statistical data.</p>
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<p>Comparison of classification results using different algorithms (five selected regions from top to bottom: Zltq, Keqyyqq, Keqyyzq, Tqx, Wlht) [<a href="#B59-remotesensing-16-04406" class="html-bibr">59</a>].</p>
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<p>Rice identification results of Hinggan League (bottom left: Keqyyzq; top left: Keqyyqq; center: Wlht; top right: Zltq r; bottom right: Tqx).</p>
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<p>Differences in phenological curves of rice planting cities in Inner Mongolia represented by time-series of NDVI and NDWI. (<b>a</b>) NDVI and NDWI values in 2016 (<b>b</b>) Rice cultivation area extraction results for 2016.</p>
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<p>Differences in phenological curves of rice planting cities in Inner Mongolia. (<b>a</b>) Annual variation in NDVI values (<b>b</b>) Annual variation in NDWI values.</p>
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<p>The extraction of rice cultivation in other cities (from right to left: HulunBuir, Tongliao, Chifeng, Hohhot, Erdos; a represents Google’s satellite imagery; b represents the extraction results).</p>
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<p>Extract area of rice area and official statistical data.</p>
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<p>Comparison of rice mapping accuracy (F1 score) under two scenarios using ablation experiments.</p>
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<p>Comparison of estimated rice planting area in Hinggan League in 2016 with statistical data from 2021.</p>
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<p>Actual scene of HLBR and phenological curve (the red arrows from left to right represent the period of snowmelt and bare soil).</p>
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18 pages, 4901 KiB  
Article
Development and Analysis of Bilayer Foamed Oleogels Stabilized with Ecogel™: Exploring the Role of Tween 80 in Modifying Physicochemical Properties
by Sonia Kudłacik-Kramarczyk, Anna Drabczyk, Alicja Przybyłowicz, Weronika Kieres and Marcel Krzan
Int. J. Mol. Sci. 2024, 25(23), 12632; https://doi.org/10.3390/ijms252312632 - 25 Nov 2024
Viewed by 593
Abstract
Oleogels are structured materials formed by immobilizing oil within a polymer network. This study aimed to synthesize bilayer foamed oleogels using Ecogel™ as an emulsifier—a natural gelling and emulsifying agent commonly used to stabilize emulsions. Ecogel™ is multifunctional, particularly in cosmetic formulations, where [...] Read more.
Oleogels are structured materials formed by immobilizing oil within a polymer network. This study aimed to synthesize bilayer foamed oleogels using Ecogel™ as an emulsifier—a natural gelling and emulsifying agent commonly used to stabilize emulsions. Ecogel™ is multifunctional, particularly in cosmetic formulations, where it aids in creating lightweight cream gels with a cooling effect. However, the specific goal of this study was to investigate the physicochemical properties of oleogels formed with Ecogel™, Tween 80, gelatin, and glycerin. The combination of these ingredients has not been studied before, particularly in the context of bilayer foamed oleogels. The biphasic nature of the resulting materials was explored, consisting of a uniform lower phase and a foamed upper layer. Several analytical techniques were employed, including FT-IR spectrophotometric analysis, moisture content evaluation, surface wettability measurements, microscopic imaging, and rheological studies, in addition to surface energy determination. The results demonstrated that the addition of Tween 80 significantly improved the stability and rigidity of the oleogels. Furthermore, storage at reduced temperatures after synthesis enhanced the material’s stabilizing properties. These materials also showed an affinity for interacting with non-polar compounds, indicating potential applications in skincare, especially for interaction with skin lipids. Full article
(This article belongs to the Special Issue Exploring New Field in Hydrocolloids Research and Applications)
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<p>FT-IR spectra of all tested samples, both oleogels and Ecogel™. The experiment was conducted in triplicate and the presented data represent a representative result from the measurements.</p>
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<p>Compilation of FT-IR spectra of oleogel sample without Tween and with the highest content of this emulsifier (<b>up</b>) and compilation of FT-IR spectra of all test samples (<b>down</b>). The experiment was conducted in triplicate and the presented data represent a representative result from the measurements.</p>
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<p>Images of oleogel samples: 0_Tween (<b>a</b>), 5_Tween (<b>b</b>), 10_Tween (<b>c</b>), and 15_Tween (<b>d</b>), magnifications: 4×. The experiment was conducted in triplicate and the presented data represent a representative result from the measurements.</p>
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<p>Contact angles of oleogel samples (both mixtures and foams). Panel (<b>a</b>) represents measurements for water and panel (<b>b</b>) represents measurements for diiodomethane. Error bars represent standard deviations (<span class="html-italic">n</span> = 3). Statistical significance (<span class="html-italic">p</span>-values) between MIX and FOAM for each concentration is indicated above the bars (n.s. = not significant, * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, for *** <span class="html-italic">p</span> &lt; 0.001). Significant differences between concentrations (Tukey’s HSD) are marked with asterisks above the corresponding groups.</p>
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<p>The schematic behavior of both hydrophobic (diiodomethane) and hydrophilic (pure double-distilled water) liquid in contact with test samples.</p>
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<p>Results of surface free energy and its components (dispersive and polar energy) for each oleogel sample (two forms: mixture (noted as MIX and FOAM). The values presented were calculated based on the averaged contact angle measurements from <a href="#ijms-25-12632-f004" class="html-fig">Figure 4</a>. Statistical analysis was not performed due to a lack of repeated measurements for surface energy components.</p>
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<p>Determined values of the absolute humidity (AH, up) and relative humidity (RH, down) of the oleogels. Error bars represent standard deviations (<span class="html-italic">n</span> = 3). Statistical significance between groups was analyzed using one-way ANOVA for each time point. Significant differences between groups are indicated with asterisks: <span class="html-italic">p</span> &lt; 0.05 (*), <span class="html-italic">p</span> &lt; 0.01 (**), <span class="html-italic">p</span> &lt; 0.001 (***).</p>
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<p>Results of the stability analysis of the oleogels directly after their synthesis (30 min measurement). The experiment was conducted in triplicate and the presented data represent a representative result from the measurements.</p>
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<p>Compilation of all stability measurements of the oleogels (directly after the synthesis, after mixing, and 24 h after mixing and storage at 6 °C). The experiment was conducted in triplicate and the presented data represent a representative result from the measurements.</p>
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<p>Compilation of the transmission measurements for the oleogel samples (directly after the synthesis, after mixing, and 24 h after mixing and storage at 6 °C). The experiment was conducted in triplicate and the presented data represent a representative result from the measurements.</p>
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<p>Evolution of the elastic and loss moduli in the oleogels with the frequency. The experiment was conducted in triplicate and the presented data represent a representative result from the measurements.</p>
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<p>Images of exemplary oleogel samples directly after synthesis (for measurement I via multiscan system) (<b>a</b>) and after 24 h of storage at 6 °C (for measurement III via multiscan system) (<b>b</b>).</p>
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<p>Images of the obtained oleogels. Sequence of samples from the left: 0_Tween, 5_Tween, 10_Tween, 15_Tween.</p>
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20 pages, 21356 KiB  
Article
Utilizing Dual Polarized Array GPR System for Shallow Urban Road Pavement Foundation in Environmental Studies: A Case Study
by Lilong Zou, Ying Li and Amir M. Alani
Remote Sens. 2024, 16(23), 4396; https://doi.org/10.3390/rs16234396 - 24 Nov 2024
Viewed by 689
Abstract
Maintaining the integrity of urban road pavements is vital for public safety, transportation efficiency, and economic stability. However, aging infrastructure and limited budgets make it challenging to detect subsurface defects that can lead to pavement collapses. Traditional inspection methods are often inadequate for [...] Read more.
Maintaining the integrity of urban road pavements is vital for public safety, transportation efficiency, and economic stability. However, aging infrastructure and limited budgets make it challenging to detect subsurface defects that can lead to pavement collapses. Traditional inspection methods are often inadequate for identifying such underground anomalies. Ground Penetrating Radar (GPR), especially dual-polarized array systems, offers a non-destructive, high-resolution solution for subsurface inspection. Despite its potential, effectively detecting and analyzing areas at risk of collapse in urban pavements remains a challenge. This study employed a dual-polarized array GPR system to inspect road pavements in London. The research involved comprehensive field testing, including data acquisition, signal processing, calibration, background noise removal, and 3D migration for enhanced imaging. Additionally, Short-Fourier Transform Spectrum (SFTS) analysis was applied to detect moisture-related anomalies. The results show that dual-polarized GPR systems effectively detect subsurface issues like voids, cracks, and moisture-induced weaknesses. The ability to capture data in multiple polarizations improves resolution and depth, enabling the identification of collapse-prone areas, particularly in regions with moisture infiltration. This study demonstrates the practical value of dual-polarized GPR technology in urban pavement inspection, offering a reliable tool for early detection of subsurface defects and contributing to the longevity and safety of road infrastructure. Full article
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<p>Investigated potential collapse of city road pavement situated in Ealing, London, UK: (<b>a</b>) Google Map; (<b>b</b>) on-site photograph.</p>
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<p>Dual-polarized array GPR system for investigation of potential collapse areas: (<b>a</b>) RIS Hi-BrigHT GPR system; (<b>b</b>) antenna configuration.</p>
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<p>Flowchart of signal processing with dual-polarized array GPR data.</p>
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<p>Dual-polarized array GPR system calibration: (<b>a</b>) antenna direct coupling measurement; (<b>b</b>) phase delay measurement of different channels.</p>
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<p>Metal plate reflections of HH and VV channels.</p>
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<p>B-scan reflection profiles acquired by the dual-polarized Array GPR system (HH, VV, and PCF filter).</p>
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<p>Migration profiles acquired by the dual-polarized Array GPR system (HH, VV, and PCF filter).</p>
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<p>Migrated profile at 0.1 m; cross-survey direction.</p>
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<p>GPR peak frequency division profile at 0.1 m; cross-survey direction.</p>
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<p>Migrated profile at 1 m; cross-survey direction.</p>
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<p>Migrated profile at 2 m; cross-survey direction.</p>
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<p>Migrated profile at 2.9 m; cross-survey direction.</p>
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<p>GPR peak frequency division profile at 1 m; cross-survey direction.</p>
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<p>GPR peak frequency division profile at 2 m; cross-survey direction.</p>
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<p>GPR peak frequency division profile at 2.9 m; cross-survey direction.</p>
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<p>Migrated horizontal slices at 0.21 m depth.</p>
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<p>Migrated horizontal slices at 0.36 m depth.</p>
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18 pages, 6503 KiB  
Article
High-Performance Memristive Synapse Based on Space-Charge-Limited Conduction in LiNbO3
by Youngmin Lee and Sejoon Lee
Nanomaterials 2024, 14(23), 1884; https://doi.org/10.3390/nano14231884 - 23 Nov 2024
Viewed by 557
Abstract
Advancing neuromorphic computing technology requires the development of versatile synaptic devices. In this study, we fabricated a high-performance Al/LiNbO3/Pt memristive synapse and emulated various synaptic functions using its primary key operating mechanism, known as oxygen vacancy-mediated valence charge migration (VO [...] Read more.
Advancing neuromorphic computing technology requires the development of versatile synaptic devices. In this study, we fabricated a high-performance Al/LiNbO3/Pt memristive synapse and emulated various synaptic functions using its primary key operating mechanism, known as oxygen vacancy-mediated valence charge migration (VO-VCM). The voltage-controlled VO-VCM induced space-charge-limited conduction and self-rectifying asymmetric hysteresis behaviors. Moreover, the device exhibited voltage pulse-tunable multi-state memory characteristics because the degree of VO-VCM was dependent on the applied pulse parameters (e.g., polarity, amplitude, width, and interval). As a result, synaptic functions such as short-term memory, dynamic range-tunable long-term memory, and spike time-dependent synaptic plasticity were successfully demonstrated by modulating those pulse parameters. Additionally, simulation studies on hand-written image pattern recognition confirmed that the present device performed with high accuracy, reaching up to 95.2%. The findings suggest that the VO-VCM-based Al/LiNbO3/Pt memristive synapse holds significant promise as a brain-inspired neuromorphic device. Full article
(This article belongs to the Section Nanoelectronics, Nanosensors and Devices)
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<p>(<b>a</b>) Schematic of the Al/LiNbO<sub>3</sub>/Pt memristive synapse. Surface FE-SEM images of the (<b>b</b>) LN-180, (<b>c</b>) LN-250, and (<b>d</b>) LN-320 layers grown on (111) Pt/SiO<sub>2</sub>/Si substrates at different temperatures of 180, 250, and 320 °C, respectively. (<b>e</b>) Wide-angle XRD patterns of the LN-180, LN-250, and LN-320 samples. (<b>f</b>) Deconvoluted XRD pattern at the Bragg angle of ~40.1°, showing the portions of (111) Pt and (113) LiNbO<sub>3</sub> phases. The insets in (<b>b</b>–<b>d</b>) show the zoomed-in view of each sample.</p>
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<p>XPS spectra of the LiNbO<sub>3</sub> layers grown at different temperatures. Li 1s and Nb 4s core levels of (<b>a</b>) LN-180, (<b>b</b>) LN-250, and (<b>c</b>) LN-320. Nb 3d core levels of (<b>d</b>) LN-180, (<b>e</b>) LN-250, and (<b>f</b>) LN-320. O 1s core levels of (<b>g</b>) LN-180, (<b>h</b>) LN-250, and (<b>i</b>) LN-320.</p>
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<p>(<b>a</b>) I–V characteristic curves of the Al/LiNbO<sub>3</sub>/Pt memristive synapse (LN-250) measured under various <span class="html-italic">V</span><sub>sw</sub> ranges. SCLC plots in the (<b>b</b>) positive and (<b>c</b>) negative <span class="html-italic">V</span><sub>sw</sub> regions. (<b>d</b>) P-F plot in the negative <span class="html-italic">V</span><sub>sw</sub> region. The inset in (<b>a</b>) illustrates the hysteretic behavior represented by the semi-logarithmic I–V curve.</p>
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<p>V<sub>O</sub>-VCM behaviors in the Al/LiNbO<sub>3</sub>/Pt memristive synapse at (<b>a</b>) <span class="html-italic">V</span><sub>sw</sub> = 0 V, (<b>b</b>) <span class="html-italic">V</span><sub>sw</sub> = <span class="html-italic">V</span><sub>1↑</sub> and <span class="html-italic">V</span><sub>2↓</sub> (&gt;0), (<b>c</b>) <span class="html-italic">V</span><sub>sw</sub> = <span class="html-italic">V</span><sub>3↓</sub>, (&lt;0), and (<b>d</b>) <span class="html-italic">V</span><sub>sw</sub> = <span class="html-italic">V</span><sub>4↑</sub> (&lt;&lt;0).</p>
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<p>I–V characteristic curves measured over 20 consecutive voltage sweeps at <span class="html-italic">V</span><sub>sw</sub> = 0–3 V performed by the (<b>a</b>) dual-sweep mode and the (<b>b</b>) single-sweep mode. Maximum current evolution as a function of <span class="html-italic">n</span><sub>sw</sub> for the (<b>c</b>) dual-sweep and (<b>d</b>) single-sweep modes. Retention characteristics at quadruple states demonstrated by changing the (<b>e</b>) magnitude of <span class="html-italic">V</span><sub>pro</sub> and the (<b>f</b>) value of <span class="html-italic">t</span><sub>pro</sub>.</p>
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<p>Basic synaptic characteristics of the Al/LiNbO<sub>3</sub>/Pt memristive synapse (LN-250). (<b>a</b>) EPSC functions performed at different <span class="html-italic">V</span><sub>pulse</sub> (4–4.5 V) with different <span class="html-italic">t</span><sub>pulse</sub> (50 μs–1 ms). (<b>b</b>) Dependence of PPF characteristics on <span class="html-italic">t</span><sub>inter</sub>, where <span class="html-italic">V</span><sub>pulse</sub>, <span class="html-italic">t</span><sub>pulse</sub>, and <span class="html-italic">V</span><sub>read</sub> were fixed at 4 V, 500 μs, and 1.2 V, respectively. (<b>c</b>) PPF index as a function of <span class="html-italic">t</span><sub>inter</sub>.</p>
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<p>STM-to-LTM transition characteristics of the Al/LiNbO<sub>3</sub>/Pt memristive synapse (LN-250). (<b>a</b>) Applied pulse scheme. (<b>b</b>) Dependence of potentiation and data retention characteristics on the number of applied pulses. The inset in (<b>b</b>) shows a zoomed-in view of the ΔPCS transient curves.</p>
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<p>LTP and LTD characteristics of the Al/LiNbO<sub>3</sub>/Pt memristive synapse (LN-250) measured under (<b>a</b>) identical and (<b>b</b>) incremental pulse schemes. The upper and lower panels in each figure show the applied pulse scheme and the measured LTP/LTD data, respectively.</p>
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<p>(<b>a</b>) Schematic of the artificial neural network designed for the MNIST simulation. (<b>b</b>) Pattern recognition accuracy as a function of the epoch. The data points in (<b>b</b>) were obtained from the MNIST simulation using the experimental LTP/LTD data shown in <a href="#nanomaterials-14-01884-f008" class="html-fig">Figure 8</a>.</p>
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<p>STDP characteristics of the Al/LiNbO<sub>3</sub>/Pt memristive synapse (LN-250), demonstrating the versatile learning activities of (<b>a</b>) asymmetric Hebbian, (<b>b</b>) asymmetric anti-Hebbian, (<b>c</b>) symmetric Hebbian, and (<b>d</b>) symmetric anti-Hebbian rules. Each inset shows the spike pulse scheme used for performing each Hebbian rule.</p>
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11 pages, 3441 KiB  
Article
THz Polarimetric Imaging of Carbon Fiber-Reinforced Composites Using the Portable Handled Spectral Reflection (PHASR) Scanner
by Kuangyi Xu, Zachery B. Harris, Paul Vahey and M. Hassan Arbab
Sensors 2024, 24(23), 7467; https://doi.org/10.3390/s24237467 - 22 Nov 2024
Viewed by 470
Abstract
Recent advancements in novel fiber-coupled and portable terahertz (THz) spectroscopic imaging technology have accelerated applications in nondestructive testing (NDT). Although the polarization information of THz waves can play a critical role in material characterization, there are few demonstrations of polarization-resolved THz imaging as [...] Read more.
Recent advancements in novel fiber-coupled and portable terahertz (THz) spectroscopic imaging technology have accelerated applications in nondestructive testing (NDT). Although the polarization information of THz waves can play a critical role in material characterization, there are few demonstrations of polarization-resolved THz imaging as an NDT modality due to the deficiency of such polarimetric imaging devices. In this paper, we have inspected industrial carbon fiber composites using a portable and handheld imaging scanner in which the THz polarizations of two orthogonal channels are simultaneously captured by two photoconductive antennas. We observed significant polarimetric differences between the two-channel images of the same sample and the resulting THz Stokes vectors, which are attributed to the anisotropic conductivity of carbon fiber composites. Using both polarimetric channels, we can visualize the superficial and underlying interfaces of the first laminate. These results pave the way for the future applications of THz polarimetry to the assessment of coatings or surface quality on carbon fiber-reinforced substrates. Full article
(This article belongs to the Special Issue Millimeter Wave and Terahertz Source, Sensing and Imaging)
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<p>(<b>a</b>) Front surface of the first test panel from Boeing Company. (<b>b</b>) Microscopic image (10×) of the bare substrate, appearing as unidirectional CFRP.</p>
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<p>(<b>a</b>) Back surface of the second test panel from Boeing Company. (<b>b</b>) Microscopic image (2.5×) of the back surface, appearing as interwoven (plain-weaved) CFRP.</p>
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<p>(<b>a</b>) The THz signals reflected from unidirectional CFRP at the sample orientations of 0° and 90°, corresponding to the TM and TE modes of polarization, respectively. The dashed box shows the difference in the propagation of the TE and TM modes in a single CFRP ply. (<b>b</b>,<b>c</b>) are the spectra of reflectivity and impulse responses retrieved from signals in (<b>a</b>). (<b>d</b>) The impulse responses are measured at different locations of interwoven CFRP, where the fiber orientations are different.</p>
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<p>Cross-section images (B-scan) of (<b>a</b>) the unidirectional CFRP and the interwoven CFRP in the (<b>b</b>) X and (<b>c</b>) Y channels. The colors are on the same scale and have been extended to [−1, 1].</p>
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<p>(<b>a</b>) Photo of the interwoven CFRP, top view. (<b>b</b>,<b>c</b>) are the C-scanned THz images of the X channel, at the optical depths of z = 0 and z = 0.52 mm, respectively. (<b>d</b>,<b>e</b>) are the correlated images of the Y channel, at the optical depths of z = 0 and z = 0.60 mm, respectively.</p>
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<p>The spatial variation in the Stokes parameters <span class="html-italic">I</span>, <span class="html-italic">Q</span>, <span class="html-italic">U</span>, and <span class="html-italic">V</span> for the interwoven CFRP at different frequencies. <span class="html-italic">I</span> is in arbitrary units while the other Stokes parameters are normalized by <span class="html-italic">I</span>.</p>
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<p>(<b>a</b>) Two ROIs (blue and red) are selected in the C-scan images of interwoven CFRP. (<b>b</b>) The mean value and standard deviation of the reflectivity in the two ROIs. (<b>c</b>–<b>f</b>) The distribution of pixels in the 2D plane of |R<sub>x</sub>| and |R<sub>y</sub>|, indicating the separation of orthogonal fibers in the 0.4–0.6 THz range.</p>
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24 pages, 25658 KiB  
Article
AI Threats to Politics, Elections, and Democracy: A Blockchain-Based Deepfake Authenticity Verification Framework
by Masabah Bint E. Islam, Muhammad Haseeb, Hina Batool, Nasir Ahtasham and Zia Muhammad
Blockchains 2024, 2(4), 458-481; https://doi.org/10.3390/blockchains2040020 - 21 Nov 2024
Viewed by 1170
Abstract
The integrity of global elections is increasingly under threat from artificial intelligence (AI) technologies. As AI continues to permeate various aspects of society, its influence on political processes and elections has become a critical area of concern. This is because AI language models [...] Read more.
The integrity of global elections is increasingly under threat from artificial intelligence (AI) technologies. As AI continues to permeate various aspects of society, its influence on political processes and elections has become a critical area of concern. This is because AI language models are far from neutral or objective; they inherit biases from their training data and the individuals who design and utilize them, which can sway voter decisions and affect global elections and democracy. In this research paper, we explore how AI can directly impact election outcomes through various techniques. These include the use of generative AI for disseminating false political information, favoring certain parties over others, and creating fake narratives, content, images, videos, and voice clones to undermine opposition. We highlight how AI threats can influence voter behavior and election outcomes, focusing on critical areas, including political polarization, deepfakes, disinformation, propaganda, and biased campaigns. In response to these challenges, we propose a Blockchain-based Deepfake Authenticity Verification Framework (B-DAVF) designed to detect and authenticate deepfake content in real time. It leverages the transparency of blockchain technology to reinforce electoral integrity. Finally, we also propose comprehensive countermeasures, including enhanced legislation, technological solutions, and public education initiatives, to mitigate the risks associated with AI in electoral contexts, proactively safeguard democracy, and promote fair elections. Full article
(This article belongs to the Special Issue Key Technologies for Security and Privacy in Web 3.0)
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<p>The figure provides an overview of the different advantages and threats of using AI in elections, political campaigns, and electoral management.</p>
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<p>Overview of the Blockchain-based Deepfake Authenticity Verification Framework (B-DAVF). This diagram illustrates the six major components of the B-DAVF: (1) content creation, (2) registering the asset, (3) tracking modifications, (4) storing the provenance, (5) verification process, and (6) flagging and reporting.</p>
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<p>A visual representation of countermeasures against AI threats. This diagram outlines key strategies to mitigate AI risks. The main categories include Regulatory Measures, Technological Solutions, Public Awareness and Education, and Suggestions for Policymakers and Researchers. Each category is further broken down into specific actions to mitigate the potential risks posed by AI in elections.</p>
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24 pages, 8231 KiB  
Article
Adaptive Optimization and Dynamic Representation Method for Asynchronous Data Based on Regional Correlation Degree
by Sichao Tang, Yuchen Zhao, Hengyi Lv, Ming Sun, Yang Feng and Zeshu Zhang
Sensors 2024, 24(23), 7430; https://doi.org/10.3390/s24237430 - 21 Nov 2024
Viewed by 454
Abstract
Event cameras, as bio-inspired visual sensors, offer significant advantages in their high dynamic range and high temporal resolution for visual tasks. These capabilities enable efficient and reliable motion estimation even in the most complex scenes. However, these advantages come with certain trade-offs. For [...] Read more.
Event cameras, as bio-inspired visual sensors, offer significant advantages in their high dynamic range and high temporal resolution for visual tasks. These capabilities enable efficient and reliable motion estimation even in the most complex scenes. However, these advantages come with certain trade-offs. For instance, current event-based vision sensors have low spatial resolution, and the process of event representation can result in varying degrees of data redundancy and incompleteness. Additionally, due to the inherent characteristics of event stream data, they cannot be utilized directly; pre-processing steps such as slicing and frame compression are required. Currently, various pre-processing algorithms exist for slicing and compressing event streams. However, these methods fall short when dealing with multiple subjects moving at different and varying speeds within the event stream, potentially exacerbating the inherent deficiencies of the event information flow. To address this longstanding issue, we propose a novel and efficient Asynchronous Spike Dynamic Metric and Slicing algorithm (ASDMS). ASDMS adaptively segments the event stream into fragments of varying lengths based on the spatiotemporal structure and polarity attributes of the events. Moreover, we introduce a new Adaptive Spatiotemporal Subject Surface Compensation algorithm (ASSSC). ASSSC compensates for missing motion information in the event stream and removes redundant information, thereby achieving better performance and effectiveness in event stream segmentation compared to existing event representation algorithms. Additionally, after compressing the processed results into frame images, the imaging quality is significantly improved. Finally, we propose a new evaluation metric, the Actual Performance Efficiency Discrepancy (APED), which combines actual distortion rate and event information entropy to quantify and compare the effectiveness of our method against other existing event representation methods. The final experimental results demonstrate that our event representation method outperforms existing approaches and addresses the shortcomings of current methods in handling event streams with multiple entities moving at varying speeds simultaneously. Full article
(This article belongs to the Section Optical Sensors)
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<p>Schematic diagram of the human retina model and corresponding event camera pixel circuit.</p>
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<p>(<b>a</b>) We consider the light intensity change signals received by the corresponding pixels as computational elements in the time domain. (<b>b</b>) From the statistical results, it can be seen that the ON polarity ratio varies randomly over the time index.</p>
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<p>This graph represents the time span changes of each event cuboid processed by our algorithm.</p>
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<p>This figure illustrates the time surface of events in the original event stream. For clarity, only the x–t components are shown. Red crosses represent non-main events, and blue dots represent main events. (<b>a</b>) In the time surface described in [<a href="#B50-sensors-24-07430" class="html-bibr">50</a>] (corresponding to Formula (24)), only the occurrence frequency of the nearest events around the main event is considered. Consequently, non-main events with disruptive effects may have significant weight. (<b>b</b>) The local memory time surface corresponding to Formula (26) considers the influence weight of historical events within the current spatiotemporal window. This approach reduces the ratio of non-main events involved in the time surface calculation, better capturing the true dynamics of the event stream. (<b>c</b>) By spatially averaging the time surfaces of all events in adjacent cells, the time surface corresponding to Formula (29) can be further regularized. Due to the spatiotemporal regularization, the influence of non-main events is almost completely suppressed.</p>
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<p>Schematic of the Gromov–Wasserstein Event Discrepancy between the original event stream and the event representation results.</p>
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<p>Illustration of the grid positions corresponding to non-zero entropy values.</p>
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<p>Grayscale images and 3D event stream diagrams for three captured scenarios: (<b>a</b>) Grayscale illustration of the corresponding scenarios; (<b>b</b>) 3D event stream illustration of the corresponding scenarios.</p>
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<p>Grayscale images and 3D event stream diagrams for three captured scenarios: (<b>a</b>) Grayscale illustration of the corresponding scenarios; (<b>b</b>) 3D event stream illustration of the corresponding scenarios.</p>
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<p>The variation of the value of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>GWED</mi> </mrow> <mi mathvariant="normal">N</mi> </msub> </mrow> </semantics></math> corresponding to each algorithm with different numbers of event samples.</p>
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<p>Illustration of the event stream processing results for Scene A by different algorithms: (<b>a</b>) TORE; (<b>b</b>) ATSLTD; (<b>c</b>) Voxel Grid; (<b>d</b>) MDES; (<b>e</b>) Ours.</p>
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<p>APED data obtained from the event stream processing results for Scene A by different algorithms.</p>
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<p>Illustration of the event stream processing results for Scene B by different algorithms: (<b>a</b>) TORE; (<b>b</b>) ATSLTD; (<b>c</b>) Voxel Grid; (<b>d</b>) MDES; (<b>e</b>) Ours.</p>
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<p>APED data obtained from the event stream processing results for Scene B by different algorithms.</p>
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<p>Illustration of the event stream processing results for Scene C by different algorithms: (<b>a</b>) TORE; (<b>b</b>) ATSLTD; (<b>c</b>) Voxel Grid; (<b>d</b>) MDES; (<b>e</b>) Ours.</p>
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<p>APED data obtained from the event stream processing results for Scene C by different algorithms.</p>
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