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17 pages, 432 KiB  
Article
Efficient Modeling and Usage of Scratchpad Memory for Artificial Intelligence Accelerators
by Cagla Irmak Rumelili Köksal and Sıddıka Berna Örs Yalçın
Electronics 2025, 14(5), 1032; https://doi.org/10.3390/electronics14051032 - 5 Mar 2025
Viewed by 193
Abstract
Deep learning accelerators play a crucial role in enhancing computation-intensive AI applications. Optimizing system resources—such as shared caches, on-chip SRAM, and data movement mechanisms—is essential for achieving peak performance and energy efficiency. This paper explores the trade-off between last-level cache (LLC) and scratchpad [...] Read more.
Deep learning accelerators play a crucial role in enhancing computation-intensive AI applications. Optimizing system resources—such as shared caches, on-chip SRAM, and data movement mechanisms—is essential for achieving peak performance and energy efficiency. This paper explores the trade-off between last-level cache (LLC) and scratchpad memory (SPM) usage in accelerator-based SoCs. To evaluate this trade-off, we introduce a high-speed simulator for estimating the timing performance of complex SoCs and demonstrate the benefits of SPM utilization. Our work shows that dynamic reconfiguration of the LLC into an SPM with prefetching capabilities reduces cache misses while improving resource utilization, performance, and energy efficiency. With SPM usage, we achieve up to 13× speedup and a 10% reduction in energy consumption for CNN backbones. Additionally, our simulator significantly outperforms state-of-the-art alternatives, running 3000× faster than gem5-SALAM for fixed-weight convolution computations and up to 64,000× faster as weight size increases. These results validate the effectiveness of both the proposed architecture and simulator in optimizing deep learning workloads. Full article
(This article belongs to the Special Issue Recent Advances in AI Hardware Design)
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<p>Memory hierarchy of a system.</p>
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<p>SoC architecture: (<b>a</b>) common architecture, (<b>b</b>) proposed architecture.</p>
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<p>Runtime scheme of the simple SoC model.</p>
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<p>Benchmark results for fixed weight size 32 × 1 × 1 × 64: (<b>a</b>) performance validation, (<b>b</b>) runtime execution timing.</p>
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<p>Benchmark results for fixed input size 14 × 28 × 64: (<b>a</b>) performance validation, (<b>b</b>) runtime execution timing.</p>
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<p>Energy and performance comparison: LLC-based SoC vs. SPM usage for ResNeT-50 (<b>a</b>) 2 MB Cache vs. 1 MB SPM (<b>b</b>) 1.5 MB Cache vs. 0.75 MB SPM (<b>c</b>) 1 MB Cache vs. 0.5 MB SPM.</p>
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<p>Energy and performance comparison: LLC-based SoC vs. SPM usage for Darknet-53 (<b>a</b>) 2 MB Cache vs. 1 MB SPM (<b>b</b>) 1.5 MB Cache vs. 0.75 MB SPM (<b>c</b>) 1 MB Cache vs. 0.5 MB SPM.</p>
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9 pages, 2321 KiB  
Article
Gallium Nitride High Electron Mobility Transistor Device with Integrated On-Chip Array Junction Temperature Monitoring Unit
by Yukuan Chang, Yue Su, Mingke Xiao, Jiatao Wu, Xu Zhang and Hongda Chen
Micromachines 2025, 16(3), 304; https://doi.org/10.3390/mi16030304 - 4 Mar 2025
Viewed by 216
Abstract
Herein, we present a novel method for junction temperature monitoring of GaN HEMT devices to achieve real-time temperature perception at different locations on the device surface. Through sputtering patterned Ti/Pt thermistor strips on the surface of a GaN HEMT device to construct an [...] Read more.
Herein, we present a novel method for junction temperature monitoring of GaN HEMT devices to achieve real-time temperature perception at different locations on the device surface. Through sputtering patterned Ti/Pt thermistor strips on the surface of a GaN HEMT device to construct an on-chip array junction temperature monitoring unit, the thermal distribution of the device during operation is fully reflected. The developed temperature monitoring unit exhibited a desirable temperature coefficient of resistance of 0.183%/°C in the range of 25 °C to 205 °C. Comparison with the thermal imager shows that the integrated temperature monitoring unit can accurately reflect the real-time temperature with a monitoring accuracy of more than 95%, which helps to improve the long-term reliability of GaN power devices under actual application conditions of high frequency and high power density. Full article
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<p>(<b>a</b>) The cross-sectional structure of GaN-HEMT power device cell with integrated temperature monitoring unit. (<b>b</b>) Photograph of the GaN power device with an embedded temperature sensing unit taken by a digital camera. (<b>b’</b>) A magnified view of the temperature sensing unit. (<b>c</b>) Schematic of the preparation procedure for GaN power devices with integrated distributed junction temperature monitoring unit. (Arrows denote the sequential direction of the fabrication steps).</p>
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<p>Transfer characteristics of the fabricated GaN-HEMT at V<sub>DS</sub> = 3 V.</p>
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<p>Output characteristics of the fabricated GaN-HEMT.</p>
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<p>Relative resistance changes versus the applied temperature of the sensing unit at different positions, corresponding to the left (<b>a</b>), middle (<b>b</b>), and right (<b>c</b>) positions, respectively.</p>
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<p>(<b>a</b>–<b>d</b>) Thermal images of the GaN-HEMT power device with integrated temperature monitoring unit under different drain current conditions, corresponding to constant currents of 0.0 A (<b>a</b>), 0.5 A (<b>b</b>), 1.0 A (<b>c</b>), and 1.5 A (<b>d</b>). (<b>e</b>) Comparison of the temperatures measured by the infrared imager and the temperature monitoring units at different locations under normal working conditions of the device. (Arrows associate the data curves with their vertical axes).</p>
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13 pages, 2958 KiB  
Article
ISFET Biosensor with Loop-Mediated Isothermal Amplification for Electronic Rapid Detection of Mycoplasma Pneumoniae
by Jie Zou, Jie Hu, Yan Shen, Limei Zhang, Weiyi Bai, Lei Wang, Jianlong Li, Lin Yan, Zhifeng Zhang, Hao Bai and Wenchuang Hu
Sensors 2025, 25(5), 1562; https://doi.org/10.3390/s25051562 - 4 Mar 2025
Viewed by 175
Abstract
Mycoplasma pneumoniae (MP) is the main culprit of community-acquired pneumonia. Commonly used laboratory testing methods have many shortcomings. Serological diagnosis has low sensitivity, causing false negatives, while a quantitative real-time polymerase chain reaction (qPCR) requires large equipment and professional staff. To make up [...] Read more.
Mycoplasma pneumoniae (MP) is the main culprit of community-acquired pneumonia. Commonly used laboratory testing methods have many shortcomings. Serological diagnosis has low sensitivity, causing false negatives, while a quantitative real-time polymerase chain reaction (qPCR) requires large equipment and professional staff. To make up for these shortcomings, we proposed a label-free, low-cost, and small-sized ion-sensitive field-effect transistor (ISFET) array based on a low-buffered loop-mediated isothermal amplification (LAMP) assay. A complementary metal oxide semiconductor (CMOS)-based ISFET array with 512 × 512 sensors was used in this system, which responds specifically to H+ with a sensitivity of 365.7 mV/pH. For on-chip amplification, a low-buffered LAMP system designed for the conserved sequences of two genes, CARDS and gyrB, was applied. The rapid release of large amounts of H+ in the low-buffered LAMP solution led to a speedy increase in electrical signals captured by the ISFET array, eliminating the need for a sophisticated temperature cycling and optical system. The on-chip results showed that the device can accurately complete MP detection with a detection limit of about 103 copies/mL (approximately 1 copy per reaction). In the final clinical validation, the detection results of eight throat swab samples using the ISFET sensors were fully consistent with the clinical laboratory diagnostic outcomes, confirming the accuracy and reliability of the ISFET sensors for use in clinical settings. And the entire process from sample lysis to result interpretation takes about 60 min. This platform has potential to be used for the point-of-care testing (POCT) of pathogen infections, providing a basis for the timely adjustment of diagnosis and treatment plans. Full article
(This article belongs to the Section Biosensors)
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<p>Workflow for MP pathogen detection with throat swabs of patients using ISFET biosensor integrated with pH-based label-free LAMP system. **** indicates <span class="html-italic">p</span> &lt; 0.0001.</p>
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<p>A schematic diagram of the structure of the ISFET-based H<sup>+</sup> sensing platform. (<b>a</b>) The basic structure of the ISFET sensor. (<b>b</b>) The experimental setup for the H<sup>+</sup> sensing platform.</p>
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<p>Performance of ISFET-based sensing platform. (<b>a</b>) Temperature of detection chip over time; (<b>b</b>) <span class="html-italic">V<sub>out</sub></span> of PBS solutions with different pH; (<b>c</b>) <span class="html-italic">V<sub>out</sub></span> of PBS solutions with gradient concentrations of MgSO<sub>4</sub>; (<b>d</b>) <span class="html-italic">V<sub>out</sub></span> of PBS solutions with gradient concentrations of KCl; (<b>e</b>) <span class="html-italic">V<sub>out</sub></span> of 5 repeated testing on same chip; (<b>f</b>) reproducibility of <span class="html-italic">V<sub>out</sub></span> on 5 chips.</p>
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<p>LAMP primer design and conservation analysis. (<b>a</b>) Position, length, and conservation analysis of primers. Red bases represent &gt;99% conservation, and green bases are between 95% and 99% conserved. (<b>b</b>) Amplification curves of selected primer targeting <span class="html-italic">CARDS</span> gene; (<b>c</b>) amplification curves of selected primer against <span class="html-italic">gyrB</span> gene. Four duplicates were used for both negative and positive tests (added template is 4 × 10<sup>3</sup> copies/mL).</p>
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<p>Optimization and performance of LAMP assay. (<b>a</b>) MgSO<sub>4</sub> concentration gradient optimization using fluorescent LAMP; (<b>b</b>) KCl concentration gradient optimization using fluorescent LAMP; (<b>c</b>) sensitivity of fluorescent LAMP system; (<b>d</b>) sensitivity of low-buffered pH-LAMP; (<b>e</b>) end-point color change in pH-LAMP in (<b>d</b>); (<b>f</b>) electrophoresis bands of LAMP products from (<b>d</b>); (<b>g</b>) validation of pH-LAMP system for cross-reactivity with other respiratory pathogens; (<b>h</b>) end-point color change in cross-reaction validation in (<b>g</b>). Negative results were plotted at TTP = 40.</p>
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<p>Performance of low-buffered pH-LAMP assay on ISFET array. (<b>a</b>) Values of changes in voltage signals after amplification of systems with different concentrations of MP template added. (<b>b</b>) <span class="html-italic">V<sub>out</sub></span> difference between positive group and negative control in (<b>a</b>). (<b>c</b>) Electrophoretic bands of LAMP amplification products from (<b>a</b>). (<b>d</b>) Values of changes in voltage signals after amplification of 8 clinical throat swab samples, as well as clinical laboratory diagnostic results. (<b>e</b>) Electrophoretic bands of LAMP amplification products from (<b>d</b>). (<b>f</b>) Overall diagnostic performance of ISFET detection platform.</p>
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11 pages, 2720 KiB  
Article
Simulation of Circular Dichroism in a Three-Layer Complementary Chiral Metasurface
by Jun Xu, Jiatong Liu, Ruiting Hao, Gang Chen, Wen Wang, Huizi Li, Pengcheng Sheng, Yanhui Li, Jincheng Kong and Jun Zhao
Photonics 2025, 12(3), 228; https://doi.org/10.3390/photonics12030228 - 3 Mar 2025
Viewed by 187
Abstract
Circularly polarized light (CPL) detection sensors have significant potential for applications in quantum communication and biosensing. In this work, we propose a three-layer complementary chiral metasurface (TCCM) for on-chip integration in the mid-infrared range (2–6 μm). The TCCM consists of an Al nanorod [...] Read more.
Circularly polarized light (CPL) detection sensors have significant potential for applications in quantum communication and biosensing. In this work, we propose a three-layer complementary chiral metasurface (TCCM) for on-chip integration in the mid-infrared range (2–6 μm). The TCCM consists of an Al nanorod layer, a SiO2 dielectric layer, and an Al nanoslit layer, with strong circular dichroism (CD) achieved through the symmetry breaking of the inclined rectangular rods. Finite-difference time-domain (FDTD) simulation results demonstrate that the electric fields excited by left circularly polarized (LCP) light and right circularly polarized (RCP) light exhibit different bonding and antibonding modes, which explains the CD mechanism. The CD response and spectral tunability are influenced by the angle and length of the inclined rectangular rods. Through simulation optimization of structural parameters, a maximum CD value of 0.72 is achieved. Compared to traditional multilayer chiral metasurfaces, the TCCM simplifies the fabrication process. These findings provide valuable insights and practical strategies for the development of compact infrared devices, particularly in optical communication, chiral sensing, and full-Stokes polarization detection. Full article
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<p>(<b>a</b>) Array and unit diagram of TCCM structure. (<b>b</b>) Schematic diagram of TCCM cell structure with InSb substrate. (<b>c</b>) Unit structure parameters of the TCCM rectangular rod layer. (<b>d</b>) Unit structure parameters of the TCCM nanoslit layer.</p>
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<p>(<b>a</b>) CD spectra when the tilt angle <b><span class="html-italic">α</span></b> is varied in the range of 0°–165°. (<b>b</b>) Transmission spectra of LCP and RCP light at <b><span class="html-italic">α</span></b> = 45°. (<b>c</b>) Structure of the TCCM cell at <b><span class="html-italic">α</span></b> = 45°, with the dashed line indicating the position of the x-z plane at y = 0. (<b>d</b>) Electric field distribution of LCP and RCP light in the x-z plane at y = 0 at <b><span class="html-italic">λ</span></b> = 2.928 μm, with the color bar indicating the electric field strength.</p>
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<p>(<b>a</b>) The electric field distribution of the <b>E<sub>z</sub></b> component in the x-y plane for the first and third layers of the TCCM structure under LCP light excitation at wavelengths of 2 μm and 3 μm. (<b>b</b>) Schematic representation of the charge distribution in the x-y plane for the first and third layers of the TCCM structure under identical conditions.</p>
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<p>(<b>a</b>) The electric field distribution of the <b>E<sub>z</sub></b> component in the x-y plane for the first and third layers of the TCCM structure under RCP light excitation at wavelengths of 2 μm and 3 μm. (<b>b</b>) Schematic representation of the charge distribution in the x-y plane for the first and third layers of the TCCM structure under identical conditions.</p>
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<p>(<b>a</b>) The transmission spectrum of parameter <b><span class="html-italic">a</span></b> ranges from 0.1 μm to 0.4 μm, with T<sub>LCP</sub> as the solid line and T<sub>RCP</sub> as the dashed line. (<b>b</b>) Transmittance spectra of parameter <b><span class="html-italic">b</span></b> varying from 0.9 μm to 1.3 μm, with the solid line indicating T<sub>LCP</sub> and the dashed line indicating TRC. (<b>c</b>) CD spectra of parameter <b><span class="html-italic">a</span></b> varying from 0.1 μm to 0.4 μm. (<b>d</b>) CD spectra with parameter <b><span class="html-italic">b</span></b> varying from 0.9 μm to 1.3 μm.</p>
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<p>(<b>a</b>) CD spectra of parameter <b><span class="html-italic">h</span><sub>3</sub></b> varying from 0.2 μm to 0.4 μm. (<b>b</b>) CD spectra with parameter <b><span class="html-italic">g</span></b> varied from 1.2 μm to 2.0 μm. (<b>c</b>) CD spectra with parameter <b><span class="html-italic">ω</span></b> varied from 0.2 μm to 0.4 μm (<b>d</b>) CD spectra with parameter <b><span class="html-italic">P</span><sub>y</sub></b> varied from 1.0 μm to 1.4 μm.</p>
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<p>Recommended fabrication process of on-chip integrated TCCM structure.</p>
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17 pages, 4201 KiB  
Article
On-Chip Purification of Extracellular Vesicles for microRNA Biomarker Analysis
by Cristina Potrich, Anna Pedrotti, Lia Vanzetti, Cecilia Pederzolli and Lorenzo Lunelli
Chemosensors 2025, 13(3), 83; https://doi.org/10.3390/chemosensors13030083 - 2 Mar 2025
Viewed by 202
Abstract
Extracellular vesicles (EVs) and their cargo are increasingly suggested as innovative biomarkers correlated to the diagnosis, progression and therapy of diseases like cancer. Several techniques have been developed for the specific separation of the different classes of EVs that give solutions enriched in [...] Read more.
Extracellular vesicles (EVs) and their cargo are increasingly suggested as innovative biomarkers correlated to the diagnosis, progression and therapy of diseases like cancer. Several techniques have been developed for the specific separation of the different classes of EVs that give solutions enriched in vesicles, but still containing other unwanted components. New methods for a more efficient, reliable and automated isolation of EVs are therefore highly desirable. Here, microparticles with surfaces endowed with positive ions were exploited to separate vesicles from complex biological matrices. First, flat silicon oxide surfaces functionalized with different divalent cations were tested for their efficiency in terms of small EV capture. Small EVs pre-purified via serial ultracentrifugations were employed for these analyses. The two better-performing cations, i.e., Cu2+ and Ni2+, were then selected to functionalize magnetic microbeads to be inserted in microfluidic chips and evaluated for their efficiency in capturing EVs and for their release of biomarkers. The best protocol setup was explored for the capture of EVs from cell culture supernatants and for the analysis of a class of biomarkers, i.e., microRNAs, via RT-PCR. The promising results obtained with this on-chip protocol evidenced the potential automation, miaturization, ease-of-use and the effective speed of the method, allowing a step forward toward its integration in simple and fast biosensors capable of analyzing the desired biomarkers present in EVs, helping the spread of biomarker analysis in both clinical settings and in research. Full article
(This article belongs to the Section Electrochemical Devices and Sensors)
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<p>Scheme of the on-chip EVs purification principle. Two microsiringe pumps for controlled liquid injection (<b>a</b>) are connected to a microfluidic chamber (<b>b</b>), containing the microbeads exposing cations (either copper or nickel ions). When EVs are injected, cations capture the vesicles, while most of the unwanted material is washed away with the buffer flux. The captured vesicles are then eluted from the beads by Triton injection. Eluted fractions are collected (<b>d</b>) and tested (<b>e</b>). In (<b>c</b>), a scheme of the EVs capture on functionalized beads and elution of biomarkers from lysed vesicles is shown.</p>
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<p>Confocal (<b>a</b>–<b>c</b>) and AFM (<b>e</b>–<b>g</b>) images of MCF7 EVs (30 µL) incubated on surfaces carrying Ni<sup>2+</sup> (<b>a</b>,<b>e</b>), Mg<sup>2+</sup> (<b>b</b>,<b>f</b>) and Cu<sup>2+</sup> (<b>c</b>,<b>g</b>). Scale bars are 5 µm for confocal images and 1 µm for AFM images. Panel (<b>d</b>) reports the density of vesicles on surfaces exposing different divalent ions, quantified from the confocal data; panel (<b>h</b>) reports the density of vesicles (blue bars) or bilayers (gray bars) measured from AFM data.</p>
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<p>Frequency distribution of average height (<b>a</b>) and equivalent diameters <math display="inline"><semantics> <msub> <mi>d</mi> <mrow> <mi>v</mi> <mi>o</mi> <mi>l</mi> <mi>u</mi> <mi>m</mi> <mi>e</mi> </mrow> </msub> </semantics></math> (<b>b</b>–<b>d</b>) of vesicles captured on surfaces exposing divalent cations and analyzed by AFM.</p>
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<p>Plot of the ratio <math display="inline"><semantics> <mrow> <mi>ρ</mi> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <msub> <mi>d</mi> <mrow> <mi>v</mi> <mi>o</mi> <mi>l</mi> <mi>u</mi> <mi>m</mi> <mi>e</mi> </mrow> </msub> <msub> <mi>d</mi> <mrow> <mi>s</mi> <mi>u</mi> <mi>r</mi> <mi>f</mi> <mi>a</mi> <mi>c</mi> <mi>e</mi> </mrow> </msub> </mfrac> </mstyle> </mrow> </semantics></math> for the three types of divalent cation treated surfaces. Blue circles: experimental data, particles. Red crosses: experimental data, bilayers. Blue dashed lines: expected value of <math display="inline"><semantics> <mi>ρ</mi> </semantics></math> of objects without volume losses after adhesion. Black dot-dashed lines: expected value of <math display="inline"><semantics> <mi>ρ</mi> </semantics></math> when adhesion objects rupture, forming a bilayer of height 4.8 nm. (<b>a</b>) Ni<sup>2+</sup>, (<b>b</b>) Cu<sup>2+</sup>, (<b>c</b>) Mg<sup>2+</sup>.</p>
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<p>Confocal analysis of NiNTA (<b>a</b>,<b>b</b>) and CuNTA (<b>c</b>,<b>d</b>) beads treated with EVs stained with PE-Rh. (<b>a</b>,<b>c</b>) The brightfield images of beads. (<b>b</b>,<b>d</b>) Fluorescence images of EVs captured by the beads. Scale bars represent 50 µm.</p>
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<p>Schematic protocol of the six steps performed for the on-chip capture and release of EVs. Input solutions injected by two syringe pumps are shown in the blue box on the left side, while output solutions are shown in the green box on the right. The central picture represents the microfluidic chip. Microbeads are visible in the second microfluifìdic chamber, filled with DPBS buffer.</p>
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<p>Fluorescence signal of fractions eluted from different samples. Black squares refer to pre-purified EVs stained with PE-Rh and after removal of PE-Rh excess, while red circles represent stained EVs without dye removal.</p>
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<p>Setup of the on-chip EV capture and release. EVs were spiked in DPBS (<b>a</b>,<b>b</b>) or FBS-free medium (<b>c</b>,<b>d</b>) and injected into the chip chamber containing either Cu-NTA (<b>a</b>,<b>c</b>) or Ni-NTA beads (<b>b</b>,<b>d</b>). The different curves represent different volumes of EVs (from 15 to 120 µL) spiked in 400 µL and injected on-chip. The percentage of fluorescence of the labeled EVs, calculated with respect to the initial sample fluorescence, which was set as 100%, is plotted versus the eluted fractions collected at the outlet (E1–E6). Insets (diamonds) show the fluorescence signal of E3 versus the volumes of EVs injected on-chip. Dash lines in insets (<b>a</b>,<b>b</b>) represent linear regressions.</p>
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<p>Threshold cycles (Ct) obtained with RT-PCR of microRNAs present in eluted fractions E2, E3 and E4. (<b>a</b>) Fractions obtained from vesicles captured from NCI-H1975 supernatants. (<b>b</b>) fractions obtained from vesicles captured from MCF7 supernatants. (<b>c</b>) A panel of four microRNAs related to Alzheimer’s disease was tested on MCF7 supernatants. Ct of miR-146a are not shown in the figure because they were below the detection limit. The vesicle capture was performed on-chip with CuNTA beads. Means and standard errors are represented.</p>
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9 pages, 3341 KiB  
Article
Quantum Dot Waveguide Array for Broadband Light Sources
by Dongyang Li, Yufei Chu, Qingbo Xu, Dong Liu, Junying Ruan, Hao Sun, Jianwei Li, Chengde Guo, Xiaoyun Pu and Yuanxian Zhang
Photonics 2025, 12(3), 212; https://doi.org/10.3390/photonics12030212 - 28 Feb 2025
Viewed by 160
Abstract
In this paper, we demonstrate a broadband and simultaneous waveguide array light source based on water-soluble CdSe/ZnS quantum dots (QDs). We initially measure the fluorescence intensity for various cladding solution concentrations along the fiber axis to assess their impact on the propagation loss; [...] Read more.
In this paper, we demonstrate a broadband and simultaneous waveguide array light source based on water-soluble CdSe/ZnS quantum dots (QDs). We initially measure the fluorescence intensity for various cladding solution concentrations along the fiber axis to assess their impact on the propagation loss; the experimental results show that the fluorescent intensity decreases with fiber length, with higher concentrations showing a more pronounced decrease. Then, we showcase a synchronous QD light source in an optofluidic chip that fluoresces in red, green, and blue (RGB) within a microfluidic channel. Finally, a 3 × 3 QD array of a fluorescent display on a single PDMS chip is demonstrated. The QD waveguide represents a compact and stable structure that is readily manufacturable, making it an ideal light source for advancing high-throughput biochemical sensing and on-chip spectroscopic analysis. Full article
(This article belongs to the Special Issue Optical Sensing Technologies, Devices and Their Data Applications)
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<p>(<b>a</b>) Schematic structures of CdSe/ZnS QDs. (<b>b</b>) Chemical structures of organic dye, disodium fluorescein. (<b>c</b>) Normalized fluorescence intensity of the same concentration of QDs and disodium fluorescein varied with time. The pump power was fixed at 5 mw.</p>
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<p>(<b>a</b>) Fluorescence spectra of QDs with different path lengths (QD concentration: 5 µM). (<b>b</b>) Fluorescence spectra intensity of QDs versus the optical path length (QD concentration of 1, 5, 10 µM, respectively). (<b>c</b>) Fluorescence intensity attenuation with various optical path lengths. The error bars are calculated with five repeated measurements.</p>
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<p>(<b>a</b>) The schematic design diagram of the PDMS optofluidic device for a red–green–blue three-color fluorescent light source. (<b>b</b>) The absorption of CdSe/ZnS QDs with different emission wavelengths. (<b>c</b>) Image of the red–green–blue three-color fluorescent light source in operation. (<b>d</b>) The spectra of fluorescence emission of the broadband light source from different channels. The blue, green, and red shades are the fluorescence spectra of CdSe/ZnS QDs (emission wavelengths of 450 nm, 530 nm, and 650 nm) with a concentration of 5 µM, respectively.</p>
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<p>(<b>a</b>) The design diagram for a 3 × 3 fluorescence array. The red, green, and blue pipes represent the 450 nm, 530 nm, and 650 nm CdSe/ZnS QD solution injections, respectively. (<b>b</b>) Photograph of PDMS chip with 3 × 3 fluorescence array. (<b>c</b>) Photograph of RGB fluorescence emission by using a 3 × 3 fluorescence array. (<b>d</b>) Photograph of a fluorescence display prototype showing “YNU” based on a 3 × 3 fluorescence array.</p>
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20 pages, 3901 KiB  
Article
Design and Implementation of a Lightweight and Energy-Efficient Semantic Segmentation Accelerator for Embedded Platforms
by Hui Li, Jinyi Li, Bowen Li, Zhengqian Miao and Shengli Lu
Micromachines 2025, 16(3), 258; https://doi.org/10.3390/mi16030258 - 25 Feb 2025
Viewed by 220
Abstract
With the rapid development of lightweight network models and efficient hardware deployment techniques, the demand for real-time semantic segmentation in areas such as autonomous driving and medical image processing has increased significantly. However, realizing efficient semantic segmentation on resource-constrained embedded platforms still faces [...] Read more.
With the rapid development of lightweight network models and efficient hardware deployment techniques, the demand for real-time semantic segmentation in areas such as autonomous driving and medical image processing has increased significantly. However, realizing efficient semantic segmentation on resource-constrained embedded platforms still faces many challenges. As a classical lightweight semantic segmentation network, ENet has attracted much attention due to its low computational complexity. In this study, we optimize the ENet semantic segmentation network to significantly reduce its computational complexity through structural simplification and 8-bit quantization and improve its hardware compatibility through the optimization of on-chip data storage and data transfer while maintaining 51.18% mIoU. The optimized network is successfully deployed on hardware accelerator and SoC systems based on Xilinx ZYNQ ZCU104 FPGA. In addition, we optimize the computational units of transposed convolution and dilated convolution and improve the on-chip data storage and data transfer design. The optimized system achieves a frame rate of 130.75 FPS, which meets the real-time processing requirements in areas such as autonomous driving and medical imaging. Meanwhile, the power consumption of the accelerator is 3.479 W, the throughput reaches 460.8 GOPS, and the energy efficiency reaches 132.2 GOPS/W. These results fully demonstrate the effectiveness of the optimization and deployment strategies in achieving a balance between computational efficiency and accuracy, which makes the system well suited for resource-constrained embedded platform applications. Full article
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<p>Optimization of network structure.</p>
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<p>The overall architecture of the proposed accelerator.</p>
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<p>Flowchart of accelerator data stream.</p>
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<p>Schematic design for dealing with discontinuities between dilation convolution columns.</p>
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<p>Schematic representation of optimized row-caching convolution sliding window for dilation convolution.</p>
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<p>Overview of line buffer module.</p>
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<p>Overview of convolution window with delay cell.</p>
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<p>Overview of weight window generation module.</p>
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<p>Overview of feature map read-state machine.</p>
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<p>Overview of configurable computing array.</p>
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<p>Overview of the array adder tree.</p>
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<p>The input–output situation of the array addition tree when running transposed convolution.</p>
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<p>The input–output situation of the second row of PE arrays during transposed convolution.</p>
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<p>The input–output situation of the first and third rows of PE arrays during transposed convolution.</p>
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<p>Switching of input and output buffers.</p>
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<p>Internal structure diagram of the buffer group.</p>
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<p>Lightweight semantic segmentation model test image. (<b>a</b>) Original image; (<b>b</b>) labeled image; (<b>c</b>) 8-bit quantized lightweight network recognition result.</p>
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<p>System block design diagram.</p>
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<p>Overall functional simulation diagram.</p>
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<p>Overall accelerator power consumption.</p>
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11 pages, 2371 KiB  
Article
Cascaded Directional Coupler-Based Triplexer Working on Spectroscopically Relevant Wavelengths for Multiple Gas Detection
by Ajmal Thottoli, Gabriele Biagi, Artem S. Vorobev, Antonella D’Orazio, Giovanni Magno and Liam O’Faolain
Photonics 2025, 12(3), 192; https://doi.org/10.3390/photonics12030192 - 25 Feb 2025
Viewed by 253
Abstract
In this article, we present experimental and simulation results of a novel high-performance cascaded directional coupler-based triplexer. The device is designed to combine the wavelengths of 1530 nm, 1653.7 nm, and 2003 nm for use in spectroscopy systems targeting the detection of ammonia, [...] Read more.
In this article, we present experimental and simulation results of a novel high-performance cascaded directional coupler-based triplexer. The device is designed to combine the wavelengths of 1530 nm, 1653.7 nm, and 2003 nm for use in spectroscopy systems targeting the detection of ammonia, methane, and carbon dioxide gases, respectively. The triplexer’s functions focus on enhancing the coupling efficiency and selectivity, while facilitating the on-chip integration of diode lasers. The experimental results demonstrate that the coupling efficiency is 82%, 73%, and 91% for the respective wavelengths of 1530 nm, 1653.7 nm, and 2003 nm. The results highlight the triplexer’s capability as a multifunctional beam combiner and an adaptable power source, essential for advanced gas sensing techniques and integrated couplers. Full article
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<p>(<b>a</b>) Schematic diagram of the design parameters of the DC-based wavelength triplexer, showing the envisaged hybrid integration of diode lasers, S-bend waveguides, coupling region, and output waveguide with a width of <span class="html-italic">W<sub>o</sub></span>. (<b>b</b>) The electric field distributions of the optimized triplexer configurations. (<b>c</b>) The range of wavelength emitted at <span class="html-italic">W<sub>o</sub></span>, while injecting the source at Ports 1, 2, and 3.</p>
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<p>Fabricated triplexer sample SEM images: (<b>a</b>) section between S-bend and output parts of waveguide and (<b>b</b>) coupling waveguides at the output section. (<b>c</b>) Microscopic imaging of the complete device. (<b>d</b>) Schematics of the Triplexer characterization setup with switching between dotted connectors option.</p>
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<p>Transmittance curves as a function of the wavelength when launching from Port 1 (solid) and Port 2 (dashed) and by varying (<b>a</b>) <span class="html-italic">g</span> and (<b>b</b>) <span class="html-italic">L<sub>c</sub></span><sub>1</sub>. The blue and the red bars indicate the region of ammonia (NH<sub>3</sub>) and methane (CH<sub>4</sub>) absorption, respectively.</p>
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<p>Normalized transmittance spectra of the triplexer for wavelengths released at Port 1 and Port 2 for varying: (<b>a</b>) <span class="html-italic">g</span> and (<b>b</b>) <span class="html-italic">L<sub>c</sub></span><sub>1</sub>. The blue bar indicates the region of ammonia (NH<sub>3</sub>) absorption, and the red bar signifies the region of methane (CH<sub>4</sub>) absorption.</p>
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<p>Transmittance calculated for varying coupling lengths <span class="html-italic">L<sub>c</sub></span><sub>3<span class="html-italic">l</span></sub> for wavelengths released at Port 3. The plot compares simulation results (dash-dot line) and experimental data (solid line with ‘o’ markers) for normalized transmittance across a range of <span class="html-italic">L<sub>c</sub></span><sub>3<span class="html-italic">l</span></sub> with different <span class="html-italic">g</span>-values.</p>
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28 pages, 2129 KiB  
Review
Trends in Precision Medicine and Pharmacogenetics as an Adjuvant in Establishing a Correct Immunosuppressive Therapy for Kidney Transplant: An Up-to-Date Historical Overview
by Riccardo Belardi, Francesca Pacifici, Matteo Baldetti, Silvia Velocci, Marilena Minieri, Massimo Pieri, Elena Campione, David Della-Morte, Giuseppe Tisone, Alessandro Anselmo, Giuseppe Novelli, Sergio Bernardini and Alessandro Terrinoni
Int. J. Mol. Sci. 2025, 26(5), 1960; https://doi.org/10.3390/ijms26051960 - 24 Feb 2025
Viewed by 236
Abstract
Kidney transplantation is currently the treatment of choice for patients with end-stage kidney diseases. Although significant advancements in kidney transplantation have been achieved over the past decades, the host’s immune response remains the primary challenge, often leading to potential graft rejection. Effective management [...] Read more.
Kidney transplantation is currently the treatment of choice for patients with end-stage kidney diseases. Although significant advancements in kidney transplantation have been achieved over the past decades, the host’s immune response remains the primary challenge, often leading to potential graft rejection. Effective management of the immune response is essential to ensure the long-term success of kidney transplantation. To address this issue, immunosuppressives have been developed and are now fully integrated into the clinical management of transplant recipients. However, the considerable inter- and intra-patient variability in pharmacokinetics (PK) and pharmacodynamics (PD) of these drugs represents the primary cause of graft rejection. This variability is primarily attributed to the polymorphic nature (genetic heterogeneity) of genes encoding xenobiotic-metabolizing enzymes, transport proteins, and, in some cases, drug targets. These genetic differences can influence drug metabolism and distribution, leading to either toxicity or reduced efficacy. The main objective of the present review is to report an historical overview of the pharmacogenetics of immunosuppressants, shedding light on the most recent findings and also suggesting how relevant is the research and investment in developing validated NGS-based commercial panels for pharmacogenetic profiling in kidney transplant recipients. These advancements will enable the implementation of precision medicine, optimizing immunosuppressive therapies to improve graft survival and kidney transplanted patient outcomes. Full article
(This article belongs to the Section Molecular Genetics and Genomics)
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<p>Immunosuppressive function of tacrolimus (TAC) and cyclosporine (CsA), focused on T-cell activation. Both immunosuppressive drugs inhibited the phosphatase calcineurin, thus avoiding the dephosphorylation of NFAT and blunting the transcription of IL-2. FKBP12: 12-kDa FK506-binding protein; IL-2, interleukin-2; NFAT, nuclear factor of activated T-cells. Created with <a href="http://BioRender.com" target="_blank">BioRender.com</a> (accessed on 7 January 2025).</p>
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<p>Immunosuppressive function of sirolimus (SRL) and everolimus (EVR). Both drugs inhibited the IL-2-mediated signaling pathway, by modulating the activity of mTORC1, blocking the activation of both T- and B-cells. mTORC1: mammalian target of rapamycin complex 1; IL-2, interleukin-2. Created with <a href="http://BioRender.com" target="_blank">BioRender.com</a> (accessed on 7 January 2025).</p>
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<p>Immunosuppressive function of mycophenolic acid (MPA). It functions as an inhibitor of the enzyme inosine 5′-monophosphate dehydrogenase (IMPDH), which converts inosine 5′-monophosphate (IMP) into xanthosine 5′-monophosphate (XMP), leading to the de novo synthesis of guanine nucleotides. Created with <a href="http://BioRender.com" target="_blank">BioRender.com</a> (accessed on 7 January 2025).</p>
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<p>Immunosuppressive function of azathioprine (AZA). It functions by inhibiting purine synthesis. Created with <a href="http://BioRender.com" target="_blank">BioRender.com</a> (accessed on 7 January 2025).</p>
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<p>Pharmacogenetic analysis for precision therapy in kidney transplants. CsA: cyclosporine; TAC: Tacrolimus; SRL: Sirolimus; MPA: Mycophenolic Acid; AZA: Azathioprine. Created with <a href="http://BioRender.com" target="_blank">BioRender.com</a> (accessed on 14 January 2025).</p>
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24 pages, 11146 KiB  
Article
Programmable Photonic Logic Array Based on Micro-Ring Resonators and All-Optical Modulation
by Jia Liu, Shenghang Zhou and Xiubao Sui
Micromachines 2025, 16(2), 238; https://doi.org/10.3390/mi16020238 - 19 Feb 2025
Viewed by 353
Abstract
All-optical computing is an emerging information processing technology. As a cutting-edge technology in the field of photonics, it effectively leverages the unique advantages of photons to achieve rapid computation. However, the lack of a fully functional and programmable design has slowed the progress [...] Read more.
All-optical computing is an emerging information processing technology. As a cutting-edge technology in the field of photonics, it effectively leverages the unique advantages of photons to achieve rapid computation. However, the lack of a fully functional and programmable design has slowed the progress of this type of optical computing system, especially in optical logic computing. In this paper, we design and propose a programmable photonic logic array based on all-optical computing methods. By efficiently combining on-chip photonic devices such as micro-ring resonators, we have realized a complete set of reconfigurable all-optical logic computation functions, including basic logic such as IS&NOT, AND, and OR, as well as combined logic, such as XOR and XNOR. To the best of our knowledge, the proposed architecture not only introduces three structurally similar standard logic units but also allows for their multiple-level cascading to form a large-scale photonic logic array, enabling multifunctional logic computation. Furthermore, using two independent wavelengths to represent the high and low levels of logic can effectively reduce cross-talk and overlap between signals, decreasing the dependence on the strength of the optical signal and the decision threshold. Simulation results by Photonic Integrated Circuit Simulator (INTERCONNECT) demonstrate the effectiveness and feasibility of the proposed programmable photonic logic array. Full article
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<p>Diagram of the proposed nonlinear MRR. (<b>a</b>) Without pump light. (<b>b</b>) With pump light.</p>
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<p>The proposed OSLU for IS&amp;NOT function.</p>
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<p>The proposed OSLU for AND function.</p>
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<p>The proposed OSLU for OR function.</p>
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<p>Structure of programmable photonic logic array for implementing arbitrary logic functions.</p>
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<p>Temperature distribution of MRR. (<b>a</b>) Structure for MRR. (<b>b</b>) Optical field transmission for MRR. (<b>c</b>) Transmission for MRR.</p>
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<p>Temperature distribution of MRR. (<b>a</b>) Model for thermal simulation. (<b>b</b>) Voltage is 0 V. (<b>c</b>) Voltage is 2.667 V.</p>
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<p>The model for linear MRR. (<b>a</b>) Frequency-domain simulation. (<b>b</b>) Time-domain simulation. (<b>c</b>) Structure of linear MRR. OSA: Optical spectral analyzer. CWL: Continuous wave laser. Ring: Micro-ring resonator. WGD: Straight waveguide. WC: Waveguide directional coupler.</p>
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<p>The spectral transmission results for linear MRR in the presence of pumping. (<b>a</b>) Without thermal tuning. (<b>b</b>) With thermal tuning.</p>
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<p>Time-domain simulation results for linear MRR in the presence of pumping. (<b>a</b>,<b>b</b>) THROUGH and DROP port without thermal tuning. (<b>c</b>,<b>d</b>) THROUGH and DROP port with thermal tuning. The horizontal axis represents the wavelength unit in nm, and the vertical axis represents the output power unit in W.</p>
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<p>The model for nonlinear MRR. (<b>a</b>) Frequency-domain simulation. (<b>b</b>) Time-domain simulation. (<b>c</b>) Structure of nonlinear MRR. OSA: Optical spectral analyzer. CWL: Continuous wave laser. Ring: Micro-ring resonator. WGD: Straight waveguide. WC: Waveguide directional coupler.</p>
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<p>The spectral transmission results for nonlinear MRR in the presence of pumping. (<b>a</b>) Without thermal tuning. (<b>b</b>) With thermal tuning.</p>
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<p>Time-domain simulation results for nonlinear MRR in the presence of pumping. (<b>a</b>,<b>b</b>) THROUGH and DROP port without thermal tuning. (<b>c</b>,<b>d</b>) THROUGH and DROP port with thermal tuning. The horizontal axis represents the wavelength unit in nm, and the vertical axis represents the output power unit in W.</p>
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<p>Model of IS&amp;NOT-OSLU. (<b>a</b>) Structure of IS-OSLU with linear MRR without thermal tuning and nonlinear MRR with thermal tuning. (<b>b</b>) Structure of NOT-OSLU with linear MRR without thermal tuning and nonlinear MRR without thermal tuning. OSA: Optical spectral analyzer. CWL: Continuous wave laser. Ring: Micro-ring resonator. WGD: Straight waveguide. WC: Waveguide directional coupler. SPLT: Optical splitter/combiner.</p>
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<p>Simulation results of IS-OSLU at Through port. (<b>a</b>) When input wavelengths are 1543.29 nm. (<b>b</b>) When input wavelengths are 1547.80 nm. The horizontal axis represents the wavelength unit in nm, and the vertical axis represents the output power unit in W.</p>
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<p>Simulation results of NOT-OSLU at Through port. (<b>a</b>) Input wavelengths are 1543.29 nm. (<b>b</b>) Input wavelengths are 1547.80 nm. The horizontal axis represents the wavelength unit in nm, and the vertical axis represents the output power unit in W.</p>
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<p>Model of AND-OSLU. Structure of AND-OSLU with linear MRR without thermal tuning and nonlinear MRR with thermal tuning. OSA: Optical spectral analyzer. CWL: Continuous wave laser. Ring: Micro-ring resonator. WGD: Straight waveguide. WC: Waveguide directional coupler. SPLT: Optical splitter/combiner.</p>
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<p>Simulation results of AND-OSLU at Through port. (<b>a</b>) Input wavelengths are 1543.29 nm and 1543.29 nm. (<b>b</b>) Input wavelengths are 1543.29 nm and 1547.80 nm. (<b>c</b>) Input wavelengths are 1547.80 nm and 1547.80 nm. The horizontal axis represents the wavelength unit in nm, and the vertical axis represents the output power unit in W.</p>
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<p>Model of OR-OSLU. Structure of OR-OSLU with linear MRR without thermal tuning and nonlinear MRR without thermal tuning. OSA: Optical spectral analyzer. CWL: Continuous wave laser. Ring: Micro-ring resonator. WGD: Straight waveguide. WC: Waveguide directional coupler. SPLT: Optical splitter/combiner.</p>
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<p>Simulation results of OR-OSLU at Through port. (<b>a</b>) Input wavelengths are 1543.29 nm and 1543.29 nm. (<b>b</b>) Input wavelengths are 1543.29 nm and 1547.80 nm. (<b>c</b>) Input wavelengths are 1547.80 nm and 1547.80 nm. The horizontal axis represents the wavelength unit in nm, and the vertical axis represents the output power unit in W..</p>
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<p>Optical circuit structure of two-input PPLA. OSA: Optical spectral analyzer. CWL: Continuous wave laser. Ring: Micro-ring resonator. WGD: Straight waveguide. WC: Waveguide directional coupler. SPLT: Optical splitter/combiner. ATT: Optical attenuator. MZM: Mach–Zehnder modulator. DC: DC source. AND: AND-OSLU composed of micro-ring resonators. INPUT: IS&amp;NOT-OSLU composed of micro-ring resonators.</p>
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<p>Simulation results of two-input PPLA for logical function of <math display="inline"><semantics> <mrow> <mi>A</mi> <mo>⊕</mo> <mi>B</mi> </mrow> </semantics></math>. (<b>a</b>) Input wavelengths are 1543.29 nm and 1543.29 nm. (<b>b</b>) Input wavelengths are 1543.29 nm and 1547.80 nm. (<b>c</b>) Input wavelengths are 1547.80 nm and 1543.29 nm. (<b>d</b>) Input wavelengths are 1547.80 nm and 1547.80 nm. The horizontal axis represents the wavelength unit in nm, and the vertical axis represents the output power unit in W.</p>
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<p>Simulation results of two-input PPLA for logical function of <math display="inline"><semantics> <mrow> <mi>A</mi> <mo>+</mo> <mover accent="true"> <mi>B</mi> <mo>¯</mo> </mover> </mrow> </semantics></math>. (<b>a</b>) Input wavelengths are 1543.29 nm and 1543.29 nm. (<b>b</b>) Input wavelengths are 1543.29 nm and 1547.80 nm. (<b>c</b>) Input wavelengths are 1547.80 nm and 1543.29 nm. (<b>d</b>) Input wavelengths are 1547.80 nm and 1547.80 nm. The horizontal axis represents the wavelength unit in nm, and the vertical axis represents the output power unit in W.</p>
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50 pages, 2540 KiB  
Review
Unveiling the Therapeutic Potential of the Second-Generation Incretin Analogs Semaglutide and Tirzepatide in Type 1 Diabetes and Latent Autoimmune Diabetes in Adults
by Marco Infante, Francesca Silvestri, Nathalia Padilla, Francesca Pacifici, Donatella Pastore, Marcelo Maia Pinheiro, Massimiliano Caprio, Manfredi Tesauro, Andrea Fabbri, Giuseppe Novelli, Rodolfo Alejandro, Antonino De Lorenzo, Camillo Ricordi and David Della-Morte
J. Clin. Med. 2025, 14(4), 1303; https://doi.org/10.3390/jcm14041303 - 15 Feb 2025
Viewed by 937
Abstract
Type 1 diabetes mellitus (T1D) is a chronic autoimmune disease caused by the immune-mediated destruction of insulin-producing pancreatic beta cells, resulting in the lifelong need for exogenous insulin. Over the last few years, overweight and obesity have recently emerged as growing health issues [...] Read more.
Type 1 diabetes mellitus (T1D) is a chronic autoimmune disease caused by the immune-mediated destruction of insulin-producing pancreatic beta cells, resulting in the lifelong need for exogenous insulin. Over the last few years, overweight and obesity have recently emerged as growing health issues also afflicting patients with T1D. In this context, the term “double diabetes” has been coined to indicate patients with T1D who have a family history of type 2 diabetes mellitus (T2D) and/or patients with T1D who are affected by insulin resistance and/or overweight/obesity and/or metabolic syndrome. At the same time, the use of second-generation incretin analogs semaglutide and tirzepatide has substantially increased on a global scale over the last few years, given the remarkable clinical benefits of these drugs (in terms of glucose control and weight loss) in patients with T2D and/or overweight/obesity. Although the glucagon-like peptide-1 (GLP-1) receptor agonists and the novel dual GIP (glucose-dependent insulinotropic polypeptide)/GLP-1 receptor agonist tirzepatide are currently not approved for the treatment of T1D, a growing body of evidence over the last few years has shown that these medications may serve as valid add-on treatments to insulin with substantial efficacy in improving glucose control, promoting weight loss, preserving residual beta-cell function and providing other beneficial metabolic effects in patients with T1D, double diabetes and latent autoimmune diabetes in adults (LADA). This manuscript aims to comprehensively review the currently available literature (mostly consisting of real-world studies) regarding the safety and therapeutic use (for different purposes) of semaglutide and tirzepatide in patients with T1D (at different stages of the disease), double diabetes and LADA. Full article
(This article belongs to the Special Issue Clinical Management of Type 1 Diabetes)
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<p><b>Potential and established benefits of the novel incretin analogs semaglutide and tirzepatide in patients with T1D (at different stages of the disease), LADA and double diabetes associated with overweight/obesity.</b> Abbreviations: AID, automated insulin delivery; GIP, glucose-dependent insulinotropic polypeptide; GLP-1, glucagon-like peptide-1; IR, insulin resistance; LADA, latent autoimmune diabetes in adults; MetS, metabolic syndrome; OB, obesity; OW, overweight; RA, receptor agonist; T1D, type 1 diabetes; TAR, time above range; TDD, total daily dose; TIR, time in range.</p>
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<p><b>Vicious cycle of weight gain, insulin resistance and increased exogenous insulin requirements in patients with T1D</b>. In patients with T1D, this perpetuating cycle leads to double diabetes, which is characterized by the coexistence of clinical features of both T1D and T2D in the same subject. Iatrogenic peripheral hyperinsulinemia during intensive exogenous insulin therapy promotes insulin resistance and weight gain. In turn, excess weight gain promotes insulin resistance, which leads to higher exogenous insulin requirements. Moreover, insulin resistance and excess weight gain due to intensive exogenous insulin therapy can increase cardiovascular risk factors (e.g., hypertension, dyslipidemia). *Iatrogenic peripheral hyperinsulinemia during intensive exogenous insulin therapy is related to subcutaneously administered exogenous insulin, which bypasses first-pass hepatic insulin extraction. Abbreviations: CV, cardiovascular; T1D, type 1 diabetes; T2D, type 2 diabetes.</p>
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<p><b>Potential synergistic benefits of second-generation incretin analogs (semaglutide and tirzepatide) and advanced technological devices used for diabetes management in patients with T1D, double diabetes and LADA.</b> Second-generation incretin analogs semaglutide and tirzepatide may be valid allies of the current advanced technological devices employed for the management of autoimmune diabetes (particularly AID systems) by preventing or reducing excess body weight, increasing the time spent in recommended target blood glucose range, reducing time spent in hyperglycemia, and decreasing glycemic variability, insulin resistance and insulin requirements, thus enhancing the glycemic and metabolic benefits of diabetes technological devices/AID systems. On the other hand, the currently available advanced technological devices used for the management of autoimmune diabetes (particularly AID systems), which can predict impending episodes of hypoglycemia or hyperglycemia and promptly and dynamically adjust insulin delivery, may help prevent the most dreaded adverse effects of incretin analogs in patients with autoimmune diabetes (especially hypoglycemia, DKA and euDKA). Abbreviations: AID, automated insulin delivery; CGM, continuous glucose monitoring; CKM, continuous ketone monitoring; DKA, diabetic ketoacidosis; euDKA, euglycemic diabetic ketoacidosis; GIP, glucose-dependent insulinotropic polypeptide; GLP-1, glucagon-like peptide-1; RA, receptor agonist; TAR, time above range; TIR, time in range; T1D, type 1 diabetes.</p>
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22 pages, 5917 KiB  
Article
Development of a Widely Accessible, Advanced Large-Scale Microfluidic Airway-on-Chip
by Brady Rae, Gwenda F. Vasse, Jalal Mosayebi, Maarten van den Berge, Simon D. Pouwels and Irene H. Heijink
Bioengineering 2025, 12(2), 182; https://doi.org/10.3390/bioengineering12020182 - 13 Feb 2025
Viewed by 604
Abstract
On-chip microfluidics are advanced in vitro models that simulate lung tissue’s native 3D environment more closely than static 2D models to investigate the complex lung architecture and multifactorial processes that lead to pulmonary disease. Current microfluidic systems can be restrictive in the quantities [...] Read more.
On-chip microfluidics are advanced in vitro models that simulate lung tissue’s native 3D environment more closely than static 2D models to investigate the complex lung architecture and multifactorial processes that lead to pulmonary disease. Current microfluidic systems can be restrictive in the quantities of biological sample that can be retrieved from a single micro-channel, such as RNA, protein, and supernatant. Here, we describe a newly developed large-scale airway-on-chip model that employs a surface area for a cell culture wider than that in currently available systems. This enables the collection of samples comparable in volume to traditional cell culture systems, making the device applicable to any workflow utilizing these static systems (RNA isolation, ELISA, etc.). With our construction method, this larger culture area allows for easier handling, the potential for a wide range of exposures, as well as the collection of low-quantity samples (e.g., volatiles or mitochondrial RNA). The model consists of two large polydimethylsiloxane (PDMS) cell culture chambers under an independent flow of medium or air, separated by a semi-permeable polyethylene (PET) cell culture membrane (23 μm thick, 0.4 μm pore size). Each chamber carries a 5 × 18 mm, 90 mm2 (92 mm2 with tapered chamber inlets) surface area that can contain up to 1–2 × 104 adherent structural lung cells and can be utilized for close contact co-culture studies of different lung cell types, including airway epithelial cells, fibroblasts, smooth muscle cells, and endothelial cells. The parallel bi-chambered design of the chip allows for epithelial cells to be cultured at the air–liquid interface (ALI) and differentiation into a dense, multi-layered, pseudostratified epithelium under biological flow rates. This millifluidic airway-on-chip advances the field by providing a readily reproducible, easily adjustable, and cost-effective large-scale fluidic 3D airway cell culture platform. Full article
(This article belongs to the Special Issue Microfluidics and Sensor Technologies in Biomedical Engineering)
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<p>Chip construction procedure. Detailed step-by-step visual guide to sealing a chip via the stamp method. Prepared and sterilized PDMS chip halves were rolled with a PDMS Mortar (5:7 PDMS–toluene) with a chemical-resistant rubber roller (*). The pre-cut and coated membrane was placed on the wet PDMS, mortar was applied to the top, and it was placed under a vacuum for 72 h to cure at RT. Both chip halves were treated in a plasma cleaning oven (320 mBarr 30 s) and sealed together with the application of a little manual force. The device was then prepared for cell seeding, an example of this can be seen with air-exposed epithelial cells and mesenchymal cells in co-culture. Created with BioRender.com.</p>
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<p>Complete experimental setup of the large scale airway-on-chip. Four chips attached to the Porcupine peristaltic pump (A). Each of the chambers in the chips was attached to a separate pump (B1/2), on the left of each pump the triangular bubble trap (C) can be seen, and on the right is the 1 mL media reservoir (D). Before the medium flowed into the chip, it was dropped into an Eppendorf that reduced flow variation (E). Cell culture areas of 92 mm<sup>2</sup> can be seen being cultured and submerged in the center of each device (F).</p>
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<p>Airway-on-chip design and structure. (<b>A</b>) Outline of the airway-on-chip design, top-down image produced from a render of the mold within fusion360. (<b>B</b>) A transverse view down the length of the chip, the apical and basal chambers can be seen containing the white arrows, and the surrounding PDMS contains the black arrows. White arrows indicate the flat membrane placement resulting from the RT cure. Black arrows highlight the tight PDMS binding between the top and bottom halves around the PET membrane. (<b>C</b>) Transverse and isometric views of the actual device. This shows the outcome of the mold (<b>A</b>), the perspective seen magnified in (<b>B</b>), and the clear optical view through the culture chamber that was imaged through in (<b>D</b>). The inner PDMS surface of the apical chamber produced from the surface of the mold was micro-milled from the above design. The location of the zoom in the design is indicated by the white arrows. (<b>D</b>) Growth of epithelial airway cells within the airway-on-chip system. The images show clear optical resolution of representative cultures of a confluent monolayer of human epithelial lung cells (Calu-3) grown on the PET membrane (<b>B</b>) within the chip device.</p>
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<p>Cell viability in the chip devices was not altered by construction with or without toluene as a thinning agent in the PDMS mortar. Calu-3 cells were seeded at 6.5 × 10<sup>4</sup> cells per chip and upon reaching confluency were incubated overnight before an AlamarBlue assay was performed on the supernatant and TrypanBlue on the cells. Differences between groups prepared with and without toluene were tested by unpaired Student’s <span class="html-italic">t</span> test, <span class="html-italic">p</span> &gt; 0.5 = ns (not significant).</p>
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<p>Junctional expression of cell–cell contact proteins in Calu-3 cells grown in the chips and mucus production after air exposure in the device. Calu-3 cells were grown to confluency and cultured for 10 days under a continuous flow rate of 150 μL/h in the basal compartment and either medium- or air-exposed from the apical side. After 10 days, the membranes were removed and stained. (<b>A</b>,<b>B</b>) Immunostaining of MUC5AC. (<b>C</b>,<b>D</b>) Immunostaining of E-cadherin. (<b>E</b>,<b>F</b>) Immunostaining of ZO-1. The left panels show stains performed on Calu-3 cells grown submerged for 10 days post confluency. The right panels show the stains on Calu-3 cells grown air-exposed for 10 days post confluency All fluorescent stains were counterstained with DAPI and pseudo-colored after imaging. Representatives images of 3 independent experiments are shown.</p>
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<p>Alcian Blue staining of human lung Calu-3 epithelial cells grown in the chips after air exposure in the device. Calu-3 cells were grown to confluency and cultured for 10 days under a continuous flow rate of 150 μL/h in the basal compartment and either medium- or air-exposed from the apical side. At the end of culturing, the membranes were removed and stained. (<b>A</b>,<b>B</b>) Transverse view of Alcian Blue staining of Calu-3 cells grown for 10 days submerged (<b>A</b>) and air-exposed (<b>B</b>).</p>
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<p>MUC5AC secretion from Calu-3 cells cultured in Transwell inserts and the airway-on-chip device was increased upon air exposure. Calu-3 cells were seeded in the chip device and on Transwell inserts and cultured until confluence, after which the cells were cultured submerged or air-exposed at 150 μL/h (medium and air) for 10 days, and apical washes were harvested to quantify MUC5AC secretion. Calu-3 cells (n = 4) grown for 10 days submerged or air-exposed on Transwell inserts (left) and in the airway-on-chip (right). * = <span class="html-italic">p</span> &lt; 0.05, ns = <span class="html-italic">p</span> &gt; 0.05 between indicated values as assessed by unpaired <span class="html-italic">t</span>-test.</p>
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<p>Growth of airway epithelial cells within the airway-on-chip system. Representative images of 3 independent cultures of human airway cells grown on the PET membrane within the chip device are shown. Airway fibroblasts were cultured on the basal side of the membrane, with epithelial cells cultured on top. After the cells reached confluency, the cultures were air-exposed from the apical compartment. The cells were images on days 7 and 21, and images of both layers of cells were taken top-down in the same position. Epithelial cells in the apical chamber can be seen above, fibroblasts on the other side of the membrane in the basal chamber can be seen below both at day 7 upon air exposure on the left and at day 21 on the right.</p>
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<p>Identification of epithelial cells and fibroblasts grown within the device. Airway fibroblasts were seeded into the device and allowed to attach overnight before inverting the device and seeding epithelial cells on the other side of the membrane. The cell were grown to confluency, air-exposed, and cultured for 21 days under a continuous flow rate of 150 μL/h. The membranes were removed post-culture, fixed, embedded, and mounted on slides before staining. All cells were stained with wheat germ agglutinin (WGA) to visualize the cellular phospholipid bilayers and their counterstained with DAPI. (<b>A</b>) Complete external structure of the epithelial layer in the apical chamber (transverse). (<b>B</b>) Cross-section view: produced from a Z-stack projection of images underlying (<b>A</b>,<b>C</b>) to visualize the location of the cells around the culture membrane within the device. (<b>C</b>) Complete external structure of the fibroblast layer in the basal chamber (transverse).</p>
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<p>Differentiation markers in airway epithelial cells cultured at the air–liquid interface (ALI) in static Transwells and co-cultured airway epithelial cells and fibroblasts in the airway-on-chip model. Airway epithelial cells were seeded into Transwell inserts or chips with fibroblasts cultured on the other side of the membrane. Once the cells reached confluency, they were exposed to air for 21 days and fixed for confocal staining. The cells were under a continuous flow rate of 150 μL/h in both the apical and basal compartment (air or medium). The top panels show stains for Mucin 5AC (MUC5AC), a component of mucus, forkhead box protein J1 (FOXJ1), a transcription factor involved in signaling for cilia production. The panels below show stains for cytokeratin-5 (KRT-5), a basal epithelial cells marker, and the bottom right panel shows alpha-smooth muscle actin (α-SMA) a cytoskeletal element that is specific to fibroblasts. All fluorescent stains were counterstained with DAPI and pseudo-colored after imaging. (<b>A</b>) MUC5AC and FOXJ1 on an ALI insert, (<b>B</b>) keratin (KRT)-5 stain on an ALI insert, (<b>C</b>) MUC5AC/FOXJ1 stain on a chip membrane. (<b>D</b>) KRT-5 stain on a chip membrane, (<b>E</b>) α-smooth muscle actin (SMA) stain of fibroblasts in the basal chamber of the same chip membrane as above.</p>
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<p>MUC5AC secretion in human airway epithelial cells (AECs) cultured in the airway-on-chip device was increased upon air exposure. AECs (n = 3) were seeded in the chip devices and cultured until confluence, after which the cells were air-exposed at 150 μL/h air for 7–21 days, and apical washes were harvested to quantify MUC5AC secretion. ** = <span class="html-italic">p</span> &lt; 0.01 between the indicated values as assessed by one-way ANOVA.</p>
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<p>Simulations of media and air movement through the geometry of the device. (<b>A</b>) Streamline simulations of air/media flow showing laminar flow directionality throughout the device (m/s). (<b>B</b>) Media velocities (<math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> <mo>/</mo> <mi mathvariant="normal">s</mi> </mrow> </semantics></math>) in the basal media chamber. (<b>C</b>) Media velocities (<math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> <mo>/</mo> <mi mathvariant="normal">s</mi> </mrow> </semantics></math>) in the apical air chamber. (<b>D</b>) Shear stress (Pa) exerted by media on the wall of the basal chamber. (<b>E</b>) Shear stress (Pa) exerted by air on the wall of the apical chamber.</p>
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11 pages, 9499 KiB  
Communication
A Complementary Metal-Oxide Semiconductor (CMOS) Analog Optoelectronic Receiver with Digital Slicers for Short-Range Light Detection and Ranging (LiDAR) Systems
by Yunji Song and Sung-Min Park
Micromachines 2025, 16(2), 215; https://doi.org/10.3390/mi16020215 - 13 Feb 2025
Viewed by 445
Abstract
This paper introduces an analog differential optoelectronic receiver (ADOR) integrated with digital slicers for short-range LiDAR systems, consisting of a spatially modulated P+/N-well on-chip avalanche photodiode (APD), a cross-coupled differential transimpedance amplifier (CCD-TIA) with cross-coupled active loads, a continuous-time linear equalizer [...] Read more.
This paper introduces an analog differential optoelectronic receiver (ADOR) integrated with digital slicers for short-range LiDAR systems, consisting of a spatially modulated P+/N-well on-chip avalanche photodiode (APD), a cross-coupled differential transimpedance amplifier (CCD-TIA) with cross-coupled active loads, a continuous-time linear equalizer (CTLE), a limiting amplifier (LA), and dual digital slicers. A key feature is the integration of an additional on-chip dummy APD at the differential input node, which enables the proposed ADOR to outperform a traditional single-ended TIA in terms of common-mode noise rejection ratio. Also, the CCD-TIA utilizes cross-coupled PMOS-NMOS active loads not only to generate the symmetric output waveforms with maximized voltage swings, but also to provide wide bandwidth characteristics. The following CTLE extends the receiver bandwidth further, allowing the dual digital slicers to operate efficiently even at high sampling rates. The LA boosts the output amplitudes to suitable levels for the following slicers. Then, the inverter-based slicers with low power consumption and a small chip area produce digital outputs. The fabricated ADOR chip using a 180 nm CMOS process demonstrates a 20 dB dynamic range from 100 μApp to 1 mApp, 2 Gb/s data rate with a 490 fF APD capacitance, and 22.7 mW power consumption from a 1.8 V supply. Full article
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<p>Block diagrams of the proposed ADOR.</p>
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<p>(<b>a</b>) Cross-sectional view of the P<sup>+</sup>/N-well APD integrated on-chip; (<b>b</b>) its layout.</p>
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<p>Schematic diagram of the CCD-TIA.</p>
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<p>Schematic diagram of the 3-bit CTLE.</p>
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<p>Schematic diagram of the LA.</p>
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<p>Layout of the proposed ADOR.</p>
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<p>Simulated frequency responses of the CCD-TIA, CTLE, and LA circuits.</p>
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<p>Simulated output waveforms of the ADOR corresponding to varying input current levels.</p>
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<p>Photograph of the fabricated ADOR chip and its corresponding test setup (inc. optical test).</p>
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<p>Measured eye diagrams of the ADOR with a 500 μA<sub>pp</sub> input current at various data rates of (<b>a</b>) 500 Mb/s, (<b>b</b>) 1 Gb/s, and (<b>c</b>) 2 Gb/s, respectively.</p>
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<p>Measured eye-diagrams of the ADOR at 500-M/bs for various input currents of (<b>a</b>) 100 μA<sub>pp</sub>, (<b>b</b>) 500 μA<sub>pp</sub>, and (<b>c</b>) 1 mA<sub>pp</sub>, respectively.</p>
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<p>Measured output noise voltage of the ADOR.</p>
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2 pages, 867 KiB  
Correction
Correction: Kebe, M.; Sanduleanu, M. A Low-Phase-Noise 8 GHz Linear-Band Sub-Millimeter-Wave Phase-Locked Loop in 22 nm FD-SOI CMOS. Micromachines 2023, 14, 1010
by Mamady Kebe and Mihai Sanduleanu
Micromachines 2025, 16(2), 211; https://doi.org/10.3390/mi16020211 - 13 Feb 2025
Viewed by 268
Abstract
In the published publication [...] Full article
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<p>PLL output spectrum at 160 GHz.</p>
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13 pages, 4878 KiB  
Article
Compact Integrated On-Chip MIMO Antenna with Reconfigurability for mmWave Frequencies
by Khaled Boubekeur, Nicolas Zerounian and Badr Eddine Ratni
Sensors 2025, 25(4), 1062; https://doi.org/10.3390/s25041062 - 10 Feb 2025
Viewed by 463
Abstract
This paper presents a compact on-chip multiple-input multiple-output (MIMO) antenna designed for future communication systems, featuring frequency-agile elements. The antenna achieves enhanced decoupling and reduced cross-section through the integration of a metasurface, which also introduces frequency agility. Designed for the millimeter-wave band using [...] Read more.
This paper presents a compact on-chip multiple-input multiple-output (MIMO) antenna designed for future communication systems, featuring frequency-agile elements. The antenna achieves enhanced decoupling and reduced cross-section through the integration of a metasurface, which also introduces frequency agility. Designed for the millimeter-wave band using low-loss BenzoCycloButene (BCB) polymer, the antenna is manufactured with microelectronic processes, and the dimensions are 7.54 × 7.54 × 0.055 mm3. Simulations and measurements demonstrate excellent frequency agility around 60 GHz, with gains of 6.5 to 9 dBi. As a proof of concept, open and short circuits were used for switching, with future designs aiming to incorporate diodes for a full dynamic reconfiguration. This work highlights the potential for compact, high-performance, and frequency-reconfigurable on-chip antennas in next-generation millimeter-wave systems. Full article
(This article belongs to the Special Issue Millimeter-Wave Antennas for 5G)
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<p>Schematic view of the proposed MIMO antenna structure based on a conventional patch antenna positioned above a metasurface.</p>
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<p>Schematic view of the metasurface unit cell (<b>a</b>) in OC configuration and (<b>b</b>) in SC configuration, with dielectric layers drawn with a separation between them and a simulation of the AMC behavior of the metasurface with (<b>c</b>) the magnitude of the reflected E field and (<b>d</b>) phase of the reflected E field at the patch level.</p>
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<p>(<b>a</b>) Schematic view of the 2 × 2 MIMO antenna, showing the OC and SC configurations. (<b>b</b>) S-parameter comparison with and without the metasurface (MS) in the OC configuration. (<b>c</b>) S-parameter comparison with and without the MS in the SC configuration. (<b>d</b>) Simulated radiation patterns at 57.75 GHz for the OC configuration, with and without the MS. (<b>e</b>) Simulated radiation patterns at 60.5 GHz for the SC configuration, with and without the MS.</p>
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<p>Diversity parameters in OC and SC configurations (<b>a</b>) for ECC and (<b>b</b>) for DG.</p>
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<p>Schematic view of the 4 × 4 MIMO antenna, illustrating three OC and SC configurations. In Configuration 1, all four antennas are open circuit (OC); in Configuration 2, they are all short circuit (SC); and in Configuration 3, antennas 1 and 3 are OC, while antennas 2 and 4 are SC. Small black lines indicate short circuits.</p>
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<p>Illustration of the sample fabrication steps.</p>
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<p>Picture of the fabricated prototype showing four zones with different 4 × 4 MIMO configurations, one 4 × 4 MIMO antenna magnified view, and open circuit unit cell and short-circuited unit cell magnified view.</p>
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<p>Fabricated sample and measurement setups of the scattering parameters and radiation patterns.</p>
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<p>Measured and simulated reflection coefficients and coupling parameters for (<b>a</b>) configuration 1, (<b>b</b>) configuration 2, and (<b>c</b>) configuration 3.</p>
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<p>Radiation patterns. (<b>a</b>) E plane at 57.25 GHz in the OC metasurface configuration and (<b>b</b>) E plane at 60.5 GHz in the SC metasurface configuration; (<b>c</b>) H plane at 57.25 GHz in the OC metasurface configuration and (<b>d</b>) H plane at 60.5 GHz in the SC metasurface configuration.</p>
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