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13 pages, 7515 KiB  
Article
An Analysis of Temperature-Dependent Timing Jitter Factors in the Structural Design of Complementary Metal-Oxide-Semiconductor Single-Photon Avalanche Detectors
by Jau-Yang Wu, Yu-Wei Lu, Meng-Hsuan Liu, Tien-Ning Chang and Chun-Hsien Liu
Sensors 2025, 25(2), 391; https://doi.org/10.3390/s25020391 - 10 Jan 2025
Viewed by 285
Abstract
Single-Photon Avalanche Photodiodes (SPADs) are increasingly utilized in high-temperature-operated, high-performance Light Detection and Ranging (LiDAR) systems as well as in ultra-low-temperature-operated quantum science applications due to their high photon sensitivity and timing resolution. Consequently, the jitter value of SPADs at different temperatures plays [...] Read more.
Single-Photon Avalanche Photodiodes (SPADs) are increasingly utilized in high-temperature-operated, high-performance Light Detection and Ranging (LiDAR) systems as well as in ultra-low-temperature-operated quantum science applications due to their high photon sensitivity and timing resolution. Consequently, the jitter value of SPADs at different temperatures plays a crucial role in LiDAR systems and Quantum Key Distribution (QKD) applications. However, limited studies have been conducted on this topic. In this study, we analyze the jitter characteristics of SPAD devices, focusing on the influence of device structures in two SPAD designs fabricated using the TSMC 18HV and TSMC 13HV processes. Using picosecond lasers with wavelengths ranging from ultraviolet (405 nm) to near-infrared (905 nm), we investigate the impact of different diffusion carrier types on jitter values and their temperature dependence across a range of 0 °C to 60 °C. Our results show that the jitter value of SPAD devices with low electric field regions varies significantly with temperature. This variation can be attributed to the higher temperature-dependent diffusion constant, as demonstrated by fitting the jitter diffusion tail with two diffusion time constants. In contrast, SPADs designed with modified electric field distributions exhibit smaller diffusion time constants and weaker temperature dependence, resulting in a much smaller temperature-dependent jitter value. Full article
26 pages, 65511 KiB  
Article
Research on Cam–Kalm Automatic Tracking Technology of Low, Slow, and Small Target Based on Gm-APD LiDAR
by Dongfang Guo, Yanchen Qu, Xin Zhou, Jianfeng Sun, Shengwen Yin, Jie Lu and Feng Liu
Remote Sens. 2025, 17(1), 165; https://doi.org/10.3390/rs17010165 - 6 Jan 2025
Viewed by 303
Abstract
With the wide application of UAVs in modern intelligent warfare as well as in civil fields, the demand for C-UAS technology is increasingly urgent. Traditional detection methods have many limitations in dealing with “low, slow, and small” targets. This paper presents a pure [...] Read more.
With the wide application of UAVs in modern intelligent warfare as well as in civil fields, the demand for C-UAS technology is increasingly urgent. Traditional detection methods have many limitations in dealing with “low, slow, and small” targets. This paper presents a pure laser automatic tracking system based on Geiger-mode avalanche photodiode (Gm-APD). Combining the target motion state prediction of the Kalman filter and the adaptive target tracking of Camshift, a Cam–Kalm algorithm is proposed to achieve high-precision and stable tracking of moving targets. The proposed system also introduces two-dimensional Gaussian fitting and edge detection algorithms to automatically determine the target’s center position and the tracking rectangular box, thereby improving the automation of target tracking. Experimental results show that the system designed in this paper can effectively track UAVs in a 70 m laboratory environment and a 3.07 km to 3.32 km long-distance scene while achieving low center positioning error and MSE. This technology provides a new solution for real-time tracking and ranging of long-distance UAVs, shows the potential of pure laser approaches in long-distancelow, slow, and small target tracking, and provides essential technical support for C-UAS technology. Full article
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Figure 1
<p>Principle block diagram of Gm-APD LiDAR system.</p>
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<p>Schematic diagram of automatic tracking algorithm.</p>
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<p>Comparison of intensity distribution between standard Gaussian model and real target. (<b>a</b>) Based on the standard target, the Gaussian shape scale is 64 × 64 neighborhood space shape. (<b>b</b>) Intensity distribution of real UAV target based on Gm-APD LiDAR.</p>
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<p>Algorithm flow of target center fitting.</p>
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<p>LiDAR intensity image and threshold filtering results. (<b>a</b>) Intensity image of LiDAR. (<b>b</b>) Algorithm filtering result.</p>
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<p>Target center estimation and tracking frame detection results: (<b>a</b>) detection results of target tracking center and (<b>b</b>) detection results of tracking rectangle.</p>
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<p>Principle block diagram of Cam–Kalm tracking algorithm.</p>
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<p>Comparison of distribution between center position and model calculation position under different frame numbers.</p>
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<p>Comparison of center positioning errors of different fitting methods under different frame numbers.</p>
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<p>Physical appearance of flying target.</p>
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<p>Close-range tracking experimental scene.</p>
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<p>Multiframe UAV dynamic tracking results of Gm-APD LiDAR based on Cam–Kalm algorithm in air and space background: (<b>a</b>) Frame 1; (<b>b</b>) Frame 33; (<b>c</b>) Frame 48; (<b>d</b>) Frame 52; (<b>e</b>) Frame 70; (<b>f</b>) Frame 86; (<b>g</b>) Frame 100; (<b>h</b>) Frame 114; (<b>i</b>) Frame 123; (<b>j</b>) Frame 133; (<b>k</b>) Frame 152; (<b>l</b>) Frame 179; (<b>m</b>) Frame 190; (<b>n</b>) Frame 199; (<b>o</b>) Frame 206; (<b>p</b>) Frame 215.</p>
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<p>Trajectory comparison using different tracking algorithms under multiple frames.</p>
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<p>Comparison of center positioning errors using different tracking algorithms under multiple frames.</p>
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<p>Ghost phenomenon imaged by Gm-APD single-photon LiDAR: (<b>a</b>) intensity image of Frame 162, (<b>b</b>) intensity image of Frame 174, (<b>c</b>) intensity image of Frame 180, (<b>d</b>) intensity image of Frame 195.</p>
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<p>Experimental scene diagram of UAV flying against a complex background of urban buildings.</p>
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<p>Imaging results of UAV detected by infrared camera in the complex scene.</p>
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<p>Imaging results showing the DJI Elf 4 UAV target obtained by the Gm-APD LiDAR in complex background conditions: (<b>a</b>) target intensity image and (<b>b</b>) target range image.</p>
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<p>Multiframe UAV dynamic tracking results of Gm-APD LiDAR based on Cam–Kalm algorithm in complex background: (<b>a</b>) Frame 001; (<b>b</b>) Frame 049; (<b>c</b>) Frame 085; (<b>d</b>) Frame 106; (<b>e</b>) Frame 168; (<b>f</b>) Frame 226; (<b>g</b>) Frame 280; (<b>h</b>) Frame 325; (<b>i</b>) Frame 354; (<b>j</b>) Frame 373; (<b>k</b>) Frame 420; (<b>l</b>) Frame 463; (<b>m</b>) Frame 507; (<b>n</b>) Frame 509; (<b>o</b>) Frame 587; (<b>p</b>) Frame 599.</p>
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<p>Tracking trajectory of the Gm-APD LiDAR for the DJI Elf 4 UAV in complex background (smoothed).</p>
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<p>Image of the UAV used in the long-distance flight experiment.</p>
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<p>Reconstruction results and fitting distribution of the Gm-APD LiDAR for long-range detection of the the MAVIC 3 UAV: (<b>a</b>) target intensity image, (<b>b</b>) target range image, and (<b>c</b>) target fitting distribution.</p>
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<p>Multiframe UAV dynamic tracking results at 3 km for the Gm-APD LiDAR based on the Cam–Kalm algorithm: (<b>a</b>) Frame 1; (<b>b</b>) Frame 9; (<b>c</b>) Frame 22; (<b>d</b>) Frame 31; (<b>e</b>) Frame 48; (<b>f</b>) Frame 59; (<b>g</b>) Frame 71; (<b>h</b>) Frame 85; (<b>i</b>) Frame 95.</p>
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<p>Tracking trajectory of the Gm-APD LiDAR for the DJI MAVIC 3 UAV at long distance (smoothed).</p>
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22 pages, 2528 KiB  
Systematic Review
AI Chatbots and Cognitive Control: Enhancing Executive Functions Through Chatbot Interactions: A Systematic Review
by Pantelis Pergantis, Victoria Bamicha, Charalampos Skianis and Athanasios Drigas
Brain Sci. 2025, 15(1), 47; https://doi.org/10.3390/brainsci15010047 - 6 Jan 2025
Viewed by 984
Abstract
Background/Objectives: The evolution of digital technology enhances the broadening of a person’s intellectual growth. Research points out that implementing innovative applications of the digital world improves human social, cognitive, and metacognitive behavior. Artificial intelligence chatbots are yet another innovative human-made construct. These [...] Read more.
Background/Objectives: The evolution of digital technology enhances the broadening of a person’s intellectual growth. Research points out that implementing innovative applications of the digital world improves human social, cognitive, and metacognitive behavior. Artificial intelligence chatbots are yet another innovative human-made construct. These are forms of software that simulate human conversation, understand and process user input, and provide personalized responses. Executive function includes a set of higher mental processes necessary for formulating, planning, and achieving a goal. The present study aims to investigate executive function reinforcement through artificial intelligence chatbots, outlining potentials, limitations, and future research suggestions. Specifically, the study examined three research questions: the use of conversational chatbots in executive functioning training, their impact on executive-cognitive skills, and the duration of any improvements. Methods: The assessment of the existing literature was implemented using the systematic review method, according to the PRISMA 2020 Principles. The avalanche search method was employed to conduct a source search in the following databases: Scopus, Web of Science, PubMed, and complementary Google Scholar. This systematic review included studies from 2021 to the present using experimental, observational, or mixed methods. It included studies using AI-based chatbots or conversationalists to support executive functions, such as anxiety, stress, depression, memory, attention, cognitive load, and behavioral changes. In addition, this study included general populations with specific neurological conditions, all peer-reviewed, written in English, and with full-text access. However, the study excluded studies before 2021, the literature reviews, systematic reviews, non-AI-based chatbots or conversationalists, studies not targeting the range of executive skills and abilities, studies not written in English, and studies without open access. The criteria aligned with the study objectives, ensuring a focus on AI chatbots and the impact of conversational agents on executive function. The initial collection totaled n = 115 articles; however, the eligibility requirements led to the final selection of n = 10 studies. Results: The findings of the studies suggested positive effects of using AI chatbots to enhance and improve executive skills. Although, several limitations were identified, making it still difficult to generalize and reproduce their effects. Conclusions: AI chatbots are an innovative artificial intelligence tool that can function as a digital assistant for learning and expanding executive skills, contributing to the cognitive, metacognitive, and social development of the individual. However, its use in executive skills training is at a primary stage. The findings highlighted the need for a unified framework for reference and future studies, better study designs, diverse populations, larger sample sizes of participants, and longitudinal studies that observe the long-term effects of their use. Full article
(This article belongs to the Special Issue Effects of Cognitive Training on Executive Function and Cognition)
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<p>Prisma 2020 chart flow.</p>
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<p>Distribution of studies by country.</p>
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<p>Methodology distribution in studies.</p>
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<p>AI chatbot utilization in educational interaction. Benefits and limitations.</p>
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<p>Distribution of types of chatbots used in studies.</p>
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<p>Chatbots and executive functions outcomes in special conditions.</p>
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19 pages, 12502 KiB  
Article
Quantifying Spatiotemporal Changes in Supraglacial Debris Cover in Eastern Pamir from 1994 to 2024 Based on the Google Earth Engine
by Hehe Liu, Zhen Zhang, Shiyin Liu, Fuming Xie, Jing Ding, Guolong Li and Haoran Su
Remote Sens. 2025, 17(1), 144; https://doi.org/10.3390/rs17010144 - 3 Jan 2025
Viewed by 419
Abstract
Supraglacial debris cover considerably influences sub-debris ablation patterns and the surface morphology of glaciers by modulating the land–atmosphere energy exchange. Understanding its spatial distribution and temporal variations is crucial for analyzing melting processes and managing downstream disaster mitigation efforts. In recent years, the [...] Read more.
Supraglacial debris cover considerably influences sub-debris ablation patterns and the surface morphology of glaciers by modulating the land–atmosphere energy exchange. Understanding its spatial distribution and temporal variations is crucial for analyzing melting processes and managing downstream disaster mitigation efforts. In recent years, the overall slightly positive mass balance or stable state of eastern Pamir glaciers has been referred to as the “Pamir-Karakoram anomaly”. It is important to note that spatial heterogeneity in glacier change has drawn widespread research attention. However, research on the spatiotemporal changes in the debris cover in this region is completely nonexistent, which has led to an inadequate understanding of debris-covered glacier variations. To address this research gap, this study employed Landsat remote sensing images within the Google Earth Engine platform, leveraging the Random Forest algorithm to classify the supraglacial debris cover. The classification algorithm integrates spectral features from Landsat images and derived indices (NDVI, NDSI, NDWI, and BAND RATIO), supplemented by auxiliary factors such as slope and aspect. By extracting the supraglacial debris cover from 1994 to 2024, this study systematically analyzed the spatiotemporal variations and investigated the underlying drivers of debris cover changes from the perspective of mass conservation. By 2024, the area of supraglacial debris in eastern Pamir reached 258.08 ± 20.65 km2, accounting for 18.5 ± 1.55% of the total glacier area. It was observed that the Kungey Mountain region demonstrated the largest debris cover rate. Between 1994 and 2024, while the total glacier area decreased by −2.57 ± 0.70%, the debris-covered areas expanded upward at a rate of +1.64 ± 0.10% yr−1. The expansion of debris cover is driven by several factors in the context of global warming. The rising temperature resulted in permafrost degradation, slope destabilization, and intensified weathering on supply slopes, thereby augmenting the debris supply. Additionally, the steep supply slope in the study area facilitates the rapid deposition of collapsed debris onto glacier surfaces, with frequent avalanche events accelerating the mobilization of rock fragments. Full article
(This article belongs to the Special Issue Earth Observation of Glacier and Snow Cover Mapping in Cold Regions)
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Graphical abstract

Graphical abstract
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<p>Schematic of debris sources (the ablation rate in the area above the boundary between supraglacial debris and bare ice is not constant but is shown to highlight the promoting effect of a thin debris cover on ablation).</p>
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<p>Overview of glacier and lake distribution in eastern Pamir (points with color represent sample sites selected by the 2024 RF classification model, and the decimal latitude and longitude coordinates of the points can be found in the <a href="#app1-remotesensing-17-00144" class="html-app">Supplementary Information</a>).</p>
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<p>Workflow schematic for the delineation of the supraglacial debris cover.</p>
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<p>Debris cover rate of glaciers in eastern Pamir (2024).</p>
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<p>Trends in debris cover and bare ice area in eastern Pamir from 1994 to 2024.</p>
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<p>Trends of changes in the debris cover area of typical glaciers from 1994 to 2024 (k represents the average rate of change in debris-covered areas; “debris variance high” indicates significant changes in the extent of debris cover in that area, while “low” indicates no change in the extent of debris cover).</p>
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<p>Spatial distribution of debris cover changes in eastern Pamir from 1994 to 2024.</p>
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<p>Proportion (%) of debris cover area changes under different (<b>a</b>) elevations and (<b>b</b>) slopes.</p>
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<p>Changes in debris cover area at different elevation gradients in the study area: (<b>a</b>) study area; (<b>b</b>) Kelayayilake glacier; (<b>c</b>) Qimugan glacier; (<b>d</b>) Kekesayi glacier.</p>
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<p>Glacier distribution map in the study area, showing 85 glaciers with data on the average debris supply slope (each point represents a glacier, with point colors indicating different average slope values).</p>
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<p>Comparison of 2000 RF classification results (red line) with RGI V7.0 (blue line) and CGI2 (green line): (<b>a</b>) Kekesayi glacier; (<b>b</b>) Qimugan glacier.</p>
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13 pages, 4866 KiB  
Article
Photoionization Impact on the Lightning Impulse Streamer Discharge of Rapeseed Insulating Oil: An Experimental Study
by Yihua Qian and Qing Wang
Energies 2025, 18(1), 157; https://doi.org/10.3390/en18010157 - 3 Jan 2025
Viewed by 354
Abstract
Photoionization is a significant factor influencing the morphology and propagation characteristics of streamers in insulating oil, yet research on the impact of photoionization on streamer branching is almost nonexistent. In this study, we employed an ultraviolet absorber to regulate the photoionization behavior of [...] Read more.
Photoionization is a significant factor influencing the morphology and propagation characteristics of streamers in insulating oil, yet research on the impact of photoionization on streamer branching is almost nonexistent. In this study, we employed an ultraviolet absorber to regulate the photoionization behavior of streamer discharges in rapeseed insulating oil. A quantitative assessment was conducted on the propagation morphology, length, and temperature distribution of positive and negative streamers. The results indicated that the streamer branches propagated in a dendritic manner. When photoionization was suppressed by the ultraviolet absorber, the streamer tended to generate more radially propagating branches, thereby shortening the axial stop length of the streamer branches by 1~3 mm. In addition, suppressing photoionization caused the maximum temperature to rise by approximately 74~220 K, generating more high-temperature hot spots within the streamer branches and promoting the formation of more radially propagating branches in the streamer. The analysis results demonstrated that suppressing photoionization weakened the axial electric field strength in the head region of the streamer branches, thereby inhibiting the electron avalanche behavior at the head of the streamer and thus reducing the rate of axial propagation of the streamer branches. Full article
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<p>Absorption spectrum of UV absorber UV-1 and rapeseed insulating oil.</p>
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<p>Shadow imaging observation system of streamer discharge in insulating oil.</p>
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<p>Propagation of positive streamer branches in rapeseed insulating oil without UV absorber and rapeseed insulating oil with 5% UV-1. (<b>a</b>) Rapeseed insulating oil without added UV absorber (peak voltage 53.06 kV). (<b>b</b>) Rapeseed insulating oil with 5% UV-1 added (peak voltage 53.32 kV).</p>
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<p>Axial projection of the grayscale difference between the positive streamer and the background light along the needle-plate electrodes. (<b>a</b>) Rapeseed insulating oil without added UV absorber. (<b>b</b>) Rapeseed insulating oil with 5% UV-1 added.</p>
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<p>Propagation of negative streamer branches in rapeseed insulating oil without UV absorber and rapeseed insulating oil with 5% UV-1. (<b>a</b>) Rapeseed insulating oil without added UV absorber (peak voltage −76.38 kV). (<b>b</b>) Rapeseed insulating oil with 5% UV-1 added (peak voltage −76.94 kV).</p>
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<p>Axial projection of the grayscale difference between the negative streamer and the background light along the needle-plate electrodes. (<b>a</b>) Rapeseed insulating oil without added UV absorber. (<b>b</b>) Rapeseed insulating oil with 5% UV-1 added.</p>
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<p>Axial projection of the grayscale difference between the negative streamer and the background light along the needle-plate electrodes. (<b>a</b>) Rapeseed insulating oil without added UV absorber. (<b>b</b>) Rapeseed insulating oil with 5% UV-1 added.</p>
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<p>Temperature distribution of positive streamers in rapeseed insulating oil. (<b>a</b>) Rapeseed insulating oil without added UV absorber. (<b>b</b>) Rapeseed insulating oil with 5% UV-1 added.</p>
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<p>Temperature distribution of negative streamers in rapeseed insulating oil. (<b>a</b>) Rapeseed insulating oil without added UV absorber. (<b>b</b>) Rapeseed insulating oil with 5% UV-1 added.</p>
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<p>Variation of lightning impulse breakdown voltage of rapeseed insulating oil with the content of UV-1.</p>
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<p>Photoionization model of streamer in natural ester insulating oil under inhomogeneous electric field. (<b>a</b>) Schematic diagram of photoionization of streams in natural ester insulating oil. (<b>b</b>) Schematic diagram of photoionization principles for positive and negative streamers.</p>
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23 pages, 3619 KiB  
Article
QuantumGS-Box—A Key-Dependent GA and QRNG-Based S-Box for High-Speed Cloud-Based Storage Encryption
by Anish Saini, Athanasios Tsokanos and Raimund Kirner
Sci 2024, 6(4), 86; https://doi.org/10.3390/sci6040086 - 23 Dec 2024
Viewed by 441
Abstract
Cloud computing has revolutionized the digital era by providing a more efficient, scalable, and cost-effective infrastructure. Secure systems that encrypt and protect data before it is transmitted over a network and stored in the cloud benefit the entire transmission process. Transmission data can [...] Read more.
Cloud computing has revolutionized the digital era by providing a more efficient, scalable, and cost-effective infrastructure. Secure systems that encrypt and protect data before it is transmitted over a network and stored in the cloud benefit the entire transmission process. Transmission data can be encrypted and protected with a secure dynamic substitution box (S-box). In this paper, we propose the QuantumGS-box, which is a dynamic S-box for high-speed cloud-based storage encryption generated by bit shuffling with a genetic algorithm and a quantum random number generator (QRNG). The proposed work generates the S-box optimized values in a dynamic way, and an experimental evaluation of the proposed S-box method has been conducted using several cryptographic criteria, including bit independence criteria, speed, non-linearity, differential and linear approximation probabilities, strict avalanche criteria and balanced output. The results demonstrate that the QuantumGS-box can enhance robustness, is resilient to differential and provide improved linear cryptoanalysis compared to other research works while assuring non-linearity. The characteristics of the proposed S-box are compared with other state of the art S-boxes to validate its performance. These characteristics indicate that the QuantumGS-box is a promising candidate for cloud-based storage encryption applications. Full article
(This article belongs to the Section Computer Sciences, Mathematics and AI)
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<p>Alice is sender and receiver.</p>
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<p>Usage Motivation: AES static S-box in cloud-based storage encryption through high-speed network.</p>
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<p>Random number generation using optical process as QRNG.</p>
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<p>Design principle of the proposed work.</p>
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<p>Proposed QuantumGS-box in cloud-based storage encryption through high-speed network.</p>
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<p>Flowchart of the proposed QuantumGS-box.</p>
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<p>Comparison of QuantumGS-box(this work) with different research studies in terms of nonlinearity. Zahid, A.H (2019)—[<a href="#B69-sci-06-00086" class="html-bibr">69</a>]; Attaullah (2018)—[<a href="#B70-sci-06-00086" class="html-bibr">70</a>]; Zahid, A.H, (2019)—[<a href="#B71-sci-06-00086" class="html-bibr">71</a>]; Ejaz, A (2021)—[<a href="#B72-sci-06-00086" class="html-bibr">72</a>]; Ibrahim, S (2021)—[<a href="#B8-sci-06-00086" class="html-bibr">8</a>]; Gao, W (2020)—[<a href="#B73-sci-06-00086" class="html-bibr">73</a>]; Al-zaidi, A.A (2018)—[<a href="#B74-sci-06-00086" class="html-bibr">74</a>]; Lu, Q (2019)—[<a href="#B75-sci-06-00086" class="html-bibr">75</a>]; Ahmad, M (2018)—[<a href="#B76-sci-06-00086" class="html-bibr">76</a>]; Wang, X (2020)—[<a href="#B77-sci-06-00086" class="html-bibr">77</a>]; Belazi, A (2017)—[<a href="#B78-sci-06-00086" class="html-bibr">78</a>]; Liu, H (2020)—[<a href="#B79-sci-06-00086" class="html-bibr">79</a>]; Khan, M.F (2022)—[<a href="#B13-sci-06-00086" class="html-bibr">13</a>]; Soto, R (2021)—[<a href="#B80-sci-06-00086" class="html-bibr">80</a>]; Abd-El-Atty, B (2023)—[<a href="#B59-sci-06-00086" class="html-bibr">59</a>].</p>
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<p>Comparison of the QuantumGS-box with different research studies in terms of LAP. Zahid, A.H (2019)—[<a href="#B69-sci-06-00086" class="html-bibr">69</a>]; Attaullah (2018)—[<a href="#B70-sci-06-00086" class="html-bibr">70</a>]; Zahid, A.H, (2019)—[<a href="#B71-sci-06-00086" class="html-bibr">71</a>]; Ejaz, A (2021)—[<a href="#B72-sci-06-00086" class="html-bibr">72</a>]; Ibrahim, S (2021)—[<a href="#B8-sci-06-00086" class="html-bibr">8</a>]; Gao, W (2020)—[<a href="#B73-sci-06-00086" class="html-bibr">73</a>]; Alzaidi, A.A (2018)—[<a href="#B74-sci-06-00086" class="html-bibr">74</a>]; Lu, Q (2019)—[<a href="#B75-sci-06-00086" class="html-bibr">75</a>]; Ahmad, M (2018)—[<a href="#B76-sci-06-00086" class="html-bibr">76</a>]; Wang, X (2020)—[<a href="#B77-sci-06-00086" class="html-bibr">77</a>]; Belazi, A (2017)—[<a href="#B78-sci-06-00086" class="html-bibr">78</a>]; Liu, H (2020)—[<a href="#B79-sci-06-00086" class="html-bibr">79</a>]; Khan, M.F (2022)—[<a href="#B13-sci-06-00086" class="html-bibr">13</a>]; Soto, R (2021)—[<a href="#B80-sci-06-00086" class="html-bibr">80</a>]; Abd-El-Atty, B (2023)—[<a href="#B59-sci-06-00086" class="html-bibr">59</a>].</p>
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10 pages, 3577 KiB  
Article
Material Structure Design of High-Gain and Low-Noise Multi-Gain-Stage Avalanche Photodiode
by Lihong Han, Meiqin Du, Xiaoning Guan, Tong Sun, Gang Liu and Pengfei Lu
Photonics 2024, 11(12), 1202; https://doi.org/10.3390/photonics11121202 - 21 Dec 2024
Viewed by 380
Abstract
In this work, the InGaAs/InAlAs multi-gain-stage APD model is established. The gain and the noise performance of multi-gain-stage APDs are analyzed based on DSMT. By studying the influence of different doping concentrations of the dropping layer and the charge layer on the gain [...] Read more.
In this work, the InGaAs/InAlAs multi-gain-stage APD model is established. The gain and the noise performance of multi-gain-stage APDs are analyzed based on DSMT. By studying the influence of different doping concentrations of the dropping layer and the charge layer on the gain and noise characteristics of the device, the photocurrent, dark current, noise, and gain characteristics of the device are analyzed, and the device structure is optimized. The results show that the maximum gain of the three-gain-stage APD is 416, and the noise factor is 3.5 when the gain is 100. The five-gain-stage APD has a maximum gain of 450 and a noise factor of 4.5 when the gain is 100. The maximum gain of the 10-gain-stage APD can reach more than 850, and the noise factor reaches 6.5 when the gain is 100. Full article
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Figure 1
<p>Diagram of the 10-gain-stage APD device structure.</p>
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<p>The light current (LC), dark current (DC), gain (G) (<b>a</b>), and electric field (<b>b</b>) at different dropping layer doping concentrations of the 3-gain-stage APD.</p>
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<p>The light current (LC), dark current (DC), gain (G) (<b>a</b>), and electric field (<b>b</b>) at different dropping layer doping concentrations of the 5-gain-stage APD.</p>
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<p>The light current (LC), dark current (DC), gain (G) (<b>a</b>), and electric field (<b>b</b>) at different dropping layer doping concentrations of the 10-gain-stage APD.</p>
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<p>The light current (LC), dark current (DC) (<b>a</b>,<b>c</b>), and electric field (<b>b</b>,<b>d</b>) diagrams of 3-gain-stage and 5-gain-stage APDs at different charge layer doping concentrations.</p>
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<p>The light current (LC), dark current (DC) (<b>a</b>,<b>c</b>), and electric field (<b>b</b>,<b>d</b>) diagrams of 3-gain-stage and 5-gain-stage APDs at different charge layer doping concentrations.</p>
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<p>The light current (LC), dark current (DC), gain (G) (<b>a</b>), and gain–noise relationship (<b>b</b>) at different charge layer doping concentrations of the 10-gain-stage APD.</p>
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<p>The electric field (<b>a</b>) and (<b>b</b>) gain–noise relationship of APD with different gain stages.</p>
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29 pages, 3241 KiB  
Article
Comparative Study of Blockchain Hashing Algorithms with a Proposal for HashLEA
by Abdullah Sevin and Abdu Ahmed Osman Mohammed
Appl. Sci. 2024, 14(24), 11967; https://doi.org/10.3390/app142411967 - 20 Dec 2024
Viewed by 529
Abstract
Blockchain has several unique features: data integrity, security, privacy, and immutability. For this reason, it is considered one of the most promising new technologies for a wide range of applications. Initially prominent in cryptocurrencies such as Bitcoin, its applications have expanded into areas [...] Read more.
Blockchain has several unique features: data integrity, security, privacy, and immutability. For this reason, it is considered one of the most promising new technologies for a wide range of applications. Initially prominent in cryptocurrencies such as Bitcoin, its applications have expanded into areas such as the Internet of Things. However, integrating blockchain into IoT systems is challenging due to the limited computing and storage capabilities of IoT devices. Efficient blockchain mining requires lightweight hash functions that balance computational complexity with resource constraints. In this study, we employed a structured methodology to evaluate hash functions for blockchain–IoT systems. Initially, a survey is conducted to identify the most commonly used hash functions in such environments. Also, this study identifies and evaluates a lightweight hash function, designated as HashLEA, for integration within blockchain-based IoT systems. Subsequently, these functions are implemented and evaluated using software coded in C and Node.js, thereby ensuring compatibility and practical applicability. Performance metrics, including software efficiency, hardware implementation, energy consumption, and security assessments, were conducted and analyzed. Ultimately, the most suitable hash functions, including HashLEA for blockchain–IoT applications, are discussed, striking a balance between computational efficiency and robust cryptographic properties. Also, the HashLEA hash function is implemented on a Raspberry Pi 4 with an ARM processor to assess its performance in a real-world blockchain–IoT environment. HashLEA successfully passes security tests, achieving a near-ideal avalanche effect, uniform hash distribution, and low standard deviation. It has been shown to demonstrate superior execution time performance, processing 100 KB messages in 0.157 ms and 10 MB messages in 15.48 ms, which represents a significant improvement in execution time over other alternatives such as Scrypt, X11, and Skein. Full article
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<p>Supply chain monitoring framework utilizing HashLEA.</p>
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<p>The general structure of the proposed hash function.</p>
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<p>Comparison of execution times on laptop computer.</p>
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<p>Comparison of execution times on Raspberry Pi 4.</p>
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<p>Comparison of energy consumption values on Raspberry Pi 4.</p>
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39 pages, 4052 KiB  
Article
Evaluation of a New Kind of Z-Pinch-Based Space Propulsion Engine: Theoretical Foundations and Design of a Proof-of-Concept Experiment
by S. K. H. Auluck, R. Verma and R. S. Rawat
Plasma 2024, 7(4), 939-977; https://doi.org/10.3390/plasma7040052 - 19 Dec 2024
Viewed by 642
Abstract
This paper explores a recently proposed scalable z-pinch-based space propulsion engine in greater detail. This concept involves a “modified plasma focus with a tapered anode that transports current from a pulsed power source to a consumable portion of the anode in the form [...] Read more.
This paper explores a recently proposed scalable z-pinch-based space propulsion engine in greater detail. This concept involves a “modified plasma focus with a tapered anode that transports current from a pulsed power source to a consumable portion of the anode in the form of a hypodermic needle tube continuously extruded along the axis of the device”. This tube is filled with a gas at a high pressure and also optionally with an axial magnetic field. The current enters the metal tube through its contact with the anode and returns to the cathode via the plasma sliding over its outer wall. The resulting rapid electrical explosion of the metal tube partially transfers current to a snowplough shock in the fill gas. Both the metal plasma and the fill gas form axisymmetric converging shells. Their interaction forms a hot and dense plasma of the fill gas surrounded by the metal plasma. Its ejection along the axis provides the impulse needed for propulsion. In a nonnuclear version, the fill gas could be xenon or hydrogen. Its unique energy density scaling could potentially lead to a neutron-deficient nuclear fusion drive based on the proton-boron avalanche fusion reaction by lining the tube with solid decaborane. In order to explore the inherent potential of this idea as a scalable space propulsion engine, this paper discusses its theoretical foundations and outlines the first iteration of a conceptual engineering design study for a proof-of-concept experiment based on the UNU-ICTP Plasma Focus facility at the Nanyang Technological University, Singapore. Full article
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<p>(<b>a</b>) The device profile is schematically represented by thick lines—Green for the initial surface, black for anode and cathode and red for the HNT. Characteristics from points on the anode are shown using dashed lines. The reference surfaces are shown using solid lines. See the text for more details. (<b>b</b>) A zoomed view of the HNT region. The reference surface is actually perpendicular, and the characteristic is tangent to the HNT at the point of contact, but the variation is too sharp to be displayed graphically. The parameters of this profile correspond to anode radius a = 9.5 mm, insulator radius 7 mm, cathode radius 32 mm, insulator height 30 mm, stem height 30 mm, taper height 75 mm and, HNT + End Cap height 20 mm. The diameter of the 34-gauge HNT is 0.16 mm. The dimensions are chosen to be close to those of the existing plasma focus facility.</p>
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<p>Variation of dimensionless dynamic inductance <math display="inline"><semantics> <mrow> <mi mathvariant="fraktur">L</mi> <mfenced> <mo>τ</mo> </mfenced> </mrow> </semantics></math> as a function of dimensionless time <math display="inline"><semantics> <mo>τ</mo> </semantics></math>. The blue part is from the stem region, the red from the taper region and green from the HNT region. <math display="inline"><semantics> <mrow> <msub> <mo>τ</mo> <mrow> <mi mathvariant="normal">I</mi> <mi mathvariant="normal">n</mi> </mrow> </msub> <mo>=</mo> <mn>0.6094</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mo>τ</mo> <mi mathvariant="normal">S</mi> </msub> <mo>=</mo> <mn>6.773</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mo>τ</mo> <mi mathvariant="normal">T</mi> </msub> <mo>=</mo> <mn>14.797</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>τ</mo> <mrow> <mi mathvariant="normal">H</mi> <mi mathvariant="normal">N</mi> <mi mathvariant="normal">T</mi> </mrow> </msub> <mo>=</mo> <mn>14.831</mn> </mrow> </semantics></math>.</p>
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<p>Current normalized to I<sub>0</sub> as a function of time normalized to the quarter cycle time of the capacitor bank. The device parameters are: insulator radius 10 mm, stem radius 16 mm, cathode radius 50 mm, insulator height 30 mm, stem height 40 mm, taper height 120 mm, HNT radius 0.08 mm and HNT height 25 mm. The fill gas is hydrogen at a pressure of 6.5 mbar.</p>
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<p>Fraction of energy <math display="inline"><semantics> <mrow> <msub> <mo>η</mo> <mi mathvariant="normal">C</mi> </msub> </mrow> </semantics></math> remaining in the capacitor, <math display="inline"><semantics> <mrow> <msub> <mo>η</mo> <mi mathvariant="normal">M</mi> </msub> </mrow> </semantics></math> stored as magnetic energy, <math display="inline"><semantics> <mrow> <msub> <mo>η</mo> <mi mathvariant="normal">D</mi> </msub> </mrow> </semantics></math> magnetic energy associated with the dynamic inductance, <math display="inline"><semantics> <mrow> <msub> <mo>η</mo> <mi mathvariant="normal">R</mi> </msub> </mrow> </semantics></math> dissipated in the resistance and, <math display="inline"><semantics> <mrow> <msub> <mo>η</mo> <mi mathvariant="normal">K</mi> </msub> </mrow> </semantics></math> the remaining energy that includes kinetic, thermal and internal energy of the plasma. The red-coloured portions of the <math display="inline"><semantics> <mrow> <msub> <mo>η</mo> <mi mathvariant="normal">M</mi> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mo>η</mo> <mi mathvariant="normal">C</mi> </msub> </mrow> </semantics></math> curves correspond to the lift-off phase.</p>
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<p>Final deuterium temperature in keV as a function of the fill gas pressure at 300 K in bars.</p>
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<p>Perspective view of MPFPA.</p>
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<p>Cross-sectional view of MPFPA.</p>
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<p>Cross-section of the pulse power interface.</p>
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<p>Ballistic pendulum.</p>
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19 pages, 10750 KiB  
Article
Snow Avalanche Hazards and Avalanche-Prone Area Mapping in Tibet
by Duo Chu, Linshan Liu, Zhaofeng Wang, Yong Nie and Yili Zhang
Geosciences 2024, 14(12), 353; https://doi.org/10.3390/geosciences14120353 - 18 Dec 2024
Viewed by 413
Abstract
Snow avalanche is one of the major natural hazards in the mountain region, yet it has received less attention compared to other mountain hazards, such as landslides, floods, and droughts. After a comprehensive overview of snow avalanche hazards in Tibet area, the spatial [...] Read more.
Snow avalanche is one of the major natural hazards in the mountain region, yet it has received less attention compared to other mountain hazards, such as landslides, floods, and droughts. After a comprehensive overview of snow avalanche hazards in Tibet area, the spatial distribution and main driving factors of snow avalanche hazards in the high mountain region in Tibet were presented in the study first. Snow avalanche-prone areas in Tibet were then mapped based on the snow cover distribution and DEM data and were validated against in situ observations. Results show that there are the highest frequencies of avalanche occurrences in the southeastern Nyainqentanglha Mountains and the southern slope of the Himalayas. In the interior of plateau, avalanche development is constrained due to less precipitation and much flatter terrain. The perennially snow avalanche-prone areas in Tibet account for 1.6% of the total area of the plateau, while it reaches 2.9% and 4.9% of the total area of Tibet in winter and spring, respectively. Snow avalanche hazards and fatalities appear to be increasing trends under global climate warming due to more human activities at higher altitudes. In addition to the continuous implementation of engineering prevention and control measures in pivotal regions in southeastern Tibet, such as in the Sichuan–Tibet highway and railway sections, enhancing monitoring, early warning, and forecasting services are crucial to prevent and mitigate avalanche hazards in the Tibetan high mountain regions, which has significant implications for other global high mountain areas. Full article
(This article belongs to the Section Natural Hazards)
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<p>Study area.</p>
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<p>Annual mean SCF in Tibet.</p>
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<p>Mean SCF in winter (<b>a</b>) and spring (<b>b</b>) in Tibet.</p>
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<p>Perennial snow avalanche-prone areas in Tibet.</p>
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<p>Winter snow avalanche-prone areas in Tibet.</p>
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<p>Spring snow avalanche-prone areas in Tibet.</p>
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<p>Field investigation on snow cover and snow avalanches in the Parlung Zangbo and Sangchu River basins. (<b>a</b>) A typical channeled snow avalanche; (<b>b</b>) snow avalanche bridge; (<b>c</b>) five channeled snow avalanches; (<b>d</b>,<b>e</b>) the destruction to forests on the mountain slope by snow avalanches.</p>
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<p>Snow avalanche deposits at near the Langqiu village in the Sentinel-2 image (left). (<b>a</b>) Avalanche deposit in the location 1 in the Sentinel-2 image; (<b>b</b>) avalanche deposit in the location 2 in the Sentinel-2 image.</p>
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<p>Snow avalanche deposits at Galongla section from Zhamo to Metok highway in the Sentinel-2 image (left). (<b>a</b>) Avalanche deposit in the location 1 in the Sentinel-2 image; (<b>b</b>) avalanche deposit in the location 2 in the Sentinel-2 image.</p>
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<p>Perennial snow avalanche-prone area in the Parlung Zangbo and Sangchu River basins in southeastern Tibet.</p>
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<p>Snow avalanche-prone areas in winter in the Parlung Zangbo and Sangchu River basins in southeastern Tibet.</p>
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<p>Snow avalanche-prone areas in spring in the Parlung Zangbo and Sangchu River basins in southeastern Tibet.</p>
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20 pages, 98934 KiB  
Article
Automated Snow Avalanche Monitoring and Alert System Using Distributed Acoustic Sensing in Norway
by Antoine Turquet, Andreas Wuestefeld, Guro K. Svendsen, Finn Kåre Nyhammer, Espen Lauvlund Nilsen, Andreas Per-Ola Persson and Vetle Refsum
GeoHazards 2024, 5(4), 1326-1345; https://doi.org/10.3390/geohazards5040063 - 17 Dec 2024
Viewed by 557
Abstract
Avalanches present substantial hazard risk in mountainous regions, particularly when avalanches obstruct roads, either hitting vehicles directly or leaving traffic exposed to subsequent avalanches during cycles. Traditional detection methods often are designed to cover only a limited section of a road stretch, hampering [...] Read more.
Avalanches present substantial hazard risk in mountainous regions, particularly when avalanches obstruct roads, either hitting vehicles directly or leaving traffic exposed to subsequent avalanches during cycles. Traditional detection methods often are designed to cover only a limited section of a road stretch, hampering effective risk management. This research introduces a novel approach using Distributed Acoustic Sensing (DAS) for avalanche detection. The monitoring site in Northern Norway is known to be frequently impacted by avalanches. Between 2022–2024, we continuously monitored the road for avalanches blocking the traffic. The automated alert system identifies avalanches affecting the road and estimates accumulated snow. The system provides continuous, real-time monitoring with competitive sensitivity and accuracy over large areas (up to 170 km) and for multiple sites on parallel. DAS powered alert system can work unaffected by visual barriers or adverse weather conditions. The system successfully identified 10 road-impacting avalanches (100% detection rate). Our results via DAS align with the previous works and indicate that low frequency part of the signal (<20 Hz) is crucial for detection and size estimation of avalanche events. Alternative fiber installation methods are evaluated for optimal sensitivity to avalanches. Consequently, this study demonstrates its durability and lower maintenance requirements, especially when compared to the high setup costs and coverage limitations of radar systems, or the weather and lighting vulnerabilities of cameras. Furthermore the system can detect vehicles on the road as important supplemental information for search and rescue operations, and thus the authorities can be alerted, thereby playing a vital role in urgent rescue efforts. Full article
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<p>(<b>a</b>) Map showing Existing Cable (blue) and New Cable extension (orange). Photos taken during the installation are attached from (i) the cabinet at the northern end of the monitoring system, (ii) the vehicle warning system end of the north section, (iii) the vehicle warning system beginning of the south section (iv) an example photo of microtrenching. (<b>b</b>) Map of Norway and the region surrounding the avalanche monitoring zone. Important places are marked, including Holmbuktura, the location of the installation. (<b>c</b>) A cross section sketch showing the details of microtrench cable installation (iv). Direct buried new cable is installed at 15 cm depth and plastic tube covered installation is done at 20 cm depth from the surface.</p>
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<p>Aerial overview of the Holmbuktura region detailing characteristic avalanche paths and the avalanche monitoring setup. The image on the left (<b>a</b>) shows a comprehensive view of the valley with shaded areas for avalanche zones in north and south. The paths (1–5) along the slope show 5 characteristic avalanche paths, delineating the primary areas of avalanche activity. The cyan line represents the trajectory of the sensor cable installation, placed to capture both the dynamics of avalanches and the road traffic activity. The plot on the right (<b>b</b>) shows the altitude evolution along 5 selected paths, giving the impression of the topography of the region. Image © 2024 Google Earth, Image Landsat/Copernicus, Image © 2024 Maxar Technologies, Image © 2024 CNES/Airbus.</p>
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<p>Simplified flowchart of the automated avalanche detection and monitoring system. Data is continuously collected and processed through edge computing in two separate modules: (1) vehicle detection and (2) avalanche detection, which operate independently to avoid interference. Detected avalanches and vehicles are then transferred to a central repository and messaging module. This module evaluates risk levels, checks for stranded or at-risk vehicles, and prepares necessary visualizations and alerts. If the risk level exceeds a predefined threshold, the system sends alerts, including plots and messages, via SCADA message system and email using 4G communication.</p>
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<p>Examples of signals recorded during monitoring with the DAS system in Holmbuktura are shown. The strain rate waterfall plot (Z) highlights features of different events: (<b>a</b>) avalanche activity in the north, (<b>b</b>) avalanche activity in the south, (<b>c</b>) a passenger car, and (<b>d</b>) a snowplow.</p>
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<p>The power spectral density (PSD) was computed from signals recorded during monitoring with the DAS system in Holmbuktura. The signals represent distinct events, specifically: (<b>a</b>) avalanche activity in the north, (<b>b</b>) avalanche activity in the south, (<b>c</b>) a passenger car, and (<b>d</b>) a snowplow.</p>
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<p>Most energetic traces from all avalanches are presented as raw signals. In (<b>a</b>) avalanche signals are presented and marked with “Zone N” and “Zone S” showing where the avalanches happened. Event 0 is an avalanche which stopped right before the road it is presented for comparison. Corresponding mean frequency of the 200 s trace is computed and marked on the end of trace. In (<b>b</b>) we present the spectrogram of all avalanches. (<b>c</b>,<b>d</b>) we compare the power spectra of north avalanches and south avalanches respectively. The associated log-averaged power spectra are also plotted.</p>
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<p>Co-located direct buried “D” (red) and piped loopback cable “P” (blue) traces from avalanches only hitting the southern section are presented (<b>a</b>). Corresponding mean frequency of the entire trace is computed and marked on the trace as well. On right we compare the power spectra from direct buried cable (<b>b</b>) and piped buried (<b>c</b>). The associated log-average power spectra are also plotted.</p>
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<p>Detailed analysis of the most energetic trace from Event 5. The avalanche signal is analyzed using 20 s sliding time window to investigate avalanche dynamics. In (<b>a</b>), the normalized signal is shown in the time domain; (<b>b</b>) presents the mean frequency of the 20 s time window sliding every 1 s; and (<b>c</b>) displays the power spectra of selected time windows. The colored boxes in (<b>a</b>) indicate time windows, which are highlighted with markers in the mean frequency plot (<b>b</b>) and in the power spectra plot (<b>c</b>) in corresponding colors.</p>
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<p>Comparison of avalanche dates with historical data of environmental variables. Temperature, snow depth, rain and wind speed from the region covering October 2022 to May 2024 is obtained from OpenMeteo [<a href="#B69-geohazards-05-00063" class="html-bibr">69</a>] is presented. We have plotted the 200 h moving averaged data to visualize long term trends.</p>
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12 pages, 2699 KiB  
Article
TCAD Simulation of Two Photon Absorption—Transient Current Technique Measurements on Silicon Detectors and LGADs
by Sebastian Pape, Michael Moll, Marcos Fernández García and Moritz Wiehe
Sensors 2024, 24(24), 8032; https://doi.org/10.3390/s24248032 - 16 Dec 2024
Viewed by 409
Abstract
Device simulation plays a crucial role in complementing experimental device characterisation by enabling deeper understanding of internal physical processes. However, for simulations to be trusted, experimental validation is essential to confirm the accuracy of the conclusions drawn. In the framework of semiconductor detector [...] Read more.
Device simulation plays a crucial role in complementing experimental device characterisation by enabling deeper understanding of internal physical processes. However, for simulations to be trusted, experimental validation is essential to confirm the accuracy of the conclusions drawn. In the framework of semiconductor detector characterisation, one powerful tool for such validation is the Two Photon Absorption-Transient Current Technique (TPA-TCT), which allows for highly precise, three-dimensional spatially-resolved characterisation of semiconductor detectors. In this work, the TCAD framework Synopsys Sentaurus is used to simulate depth-resolved TPA-TCT data for both p-type pad detectors (PINs) and Low Gain Avalanche Detectors (LGADs). The simulated data are compared against experimentally measured TPA-TCT results. Through this comparison, it is demonstrated that TCAD simulations can reproduce the TPA-TCT measurements, providing valuable insights into the TPA-TCT itself. Another significant outcome of this study is the successful simulation of the gain reduction mechanism, which can be observed in LGADs with increasing densities of excess charge carriers. This effect is demonstrated in an p-type LGAD with a thickness of approximately 286 µm. The results confirm the ability of TCAD to model the complex interaction between carrier dynamics and device gain. Full article
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<p>Schematic layout of the used TPA-TCT setup [<a href="#B9-sensors-24-08032" class="html-bibr">9</a>].</p>
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<p>(<b>a</b>) Simulated current transients from TCAD simulations (TCAD, solid lines) and after a mathematical filtering considering the readout electronics (Filtered, dashed lines). (<b>b</b>) Comparison between the experimental (Exp., solid lines) and simulated (Sim., dashed lines) current transients. The simulated current transients contain the effects of the readout electronics and correspond to the filtered data in figure (<b>a</b>). The experimental current transient recoded at <math display="inline"><semantics> <mrow> <msub> <mi>z</mi> <mi>Si</mi> </msub> <mo>=</mo> <mn>280</mn> <mo> </mo> <mrow> <mo mathvariant="normal">μ</mo> <mi mathvariant="normal">m</mi> </mrow> </mrow> </semantics></math> has a significantly higher amplitude, because reflection at the sensor backside is not taken into account in the simulation.</p>
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<p>Simulated and measured charge collection within <math display="inline"><semantics> <mrow> <mn>20</mn> <mo> </mo> <mrow> <mi mathvariant="normal">n</mi> <mi mathvariant="normal">s</mi> </mrow> </mrow> </semantics></math> (<b>a</b>) and prompt current at <math display="inline"><semantics> <mrow> <mn>600</mn> <mrow> <mi mathvariant="normal">p</mi> <mi mathvariant="normal">s</mi> </mrow> </mrow> </semantics></math> (<b>b</b>) along the device depth.</p>
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<p>(<b>a</b>) Simulated collected charge profile overlapped with the simulated time over threshold profile along the device depth. The regions where holes or electrons dominate the collection time in the current transients are indicated. (<b>b</b>) Comparison between the simulated and measured time over threshold profile along the device depth. The experimental time over threshold profile is affected by reflection, which mirrors the region <math display="inline"><semantics> <mrow> <mn>0</mn> <mo> </mo> <mrow> <mo mathvariant="normal">μ</mo> <mi mathvariant="normal">m</mi> </mrow> <mo>&lt;</mo> <msub> <mi>z</mi> <mi>Si</mi> </msub> <mo>&lt;</mo> <mn>286</mn> <mo> </mo> <mrow> <mo mathvariant="normal">μ</mo> <mi mathvariant="normal">m</mi> </mrow> </mrow> </semantics></math> at the back side to <math display="inline"><semantics> <mrow> <msub> <mi>z</mi> <mi>Si</mi> </msub> <mo>&gt;</mo> <mn>286</mn> <mo> </mo> <mrow> <mo mathvariant="normal">μ</mo> <mi mathvariant="normal">m</mi> </mrow> </mrow> </semantics></math>.</p>
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<p>Simulated (<b>a</b>) and measured (<b>b</b>) weighted prompt current for different prompt current times along the device depth. The valleys at the device boundaries are an effect of a shifting median of the excess charge (see text in <a href="#sec4dot3-sensors-24-08032" class="html-sec">Section 4.3</a>).</p>
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<p>Experimental data: Charge collection within <math display="inline"><semantics> <mrow> <mn>20</mn> <mo> </mo> <mrow> <mi mathvariant="normal">n</mi> <mi mathvariant="normal">s</mi> </mrow> </mrow> </semantics></math> as function of the device depth for a PIN diode (<b>a</b>) and an LGAD (<b>b</b>). Both devices are fully depleted and operated at <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>860</mn> <mi mathvariant="normal">V</mi> </mrow> </semantics></math> (PIN) and <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>900</mn> <mi mathvariant="normal">V</mi> </mrow> </semantics></math> (LGAD), respectively. The charge collection profiles were obtained with different laser pulse intensities. The legend gives the angular setting of the NDF with the highest laser pulse intensity for the smallest angular setting.</p>
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<p>Waveforms recorded at the top side (<math display="inline"><semantics> <mrow> <mn>30</mn> <mo> </mo> <mrow> <mo mathvariant="normal">μ</mo> <mi mathvariant="normal">m</mi> </mrow> </mrow> </semantics></math>) and back side (<math display="inline"><semantics> <mrow> <mn>250</mn> <mo> </mo> <mrow> <mo mathvariant="normal">μ</mo> <mi mathvariant="normal">m</mi> </mrow> </mrow> </semantics></math>) of the LGAD for an injected charge of (<b>a</b>) <math display="inline"><semantics> <mrow> <mn>6.5</mn> <mo> </mo> <mrow> <mi mathvariant="normal">f</mi> <mi mathvariant="normal">C</mi> </mrow> </mrow> </semantics></math> (NDF 140°) and (<b>b</b>) <math display="inline"><semantics> <mrow> <mn>68</mn> <mo> </mo> <mrow> <mi mathvariant="normal">f</mi> <mi mathvariant="normal">C</mi> </mrow> </mrow> </semantics></math> (NDF 110°). The solid lines represent the experimental data and the dashed lines the corresponding TCAD simulations.</p>
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<p>Simulation: (<b>a</b>) Charge collection within <math display="inline"><semantics> <mrow> <mn>20</mn> <mo> </mo> <mrow> <mi mathvariant="normal">n</mi> <mi mathvariant="normal">s</mi> </mrow> </mrow> </semantics></math> along the device depth for the LGAD with the same laser intensity settings as the experimental data shown in <a href="#sensors-24-08032-f006" class="html-fig">Figure 6</a>. (<b>b</b>) The gain as function of depth in the device as obtained by dividing the CC in the LGAD by the CC in the centre of a PIN for the same laser intensity.</p>
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<p>LGAD gain at <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>900</mn> <mi mathvariant="normal">V</mi> </mrow> </semantics></math> as function of TPA-TCT generated charge deposited in <math display="inline"><semantics> <mrow> <mn>30</mn> <mo> </mo> <mrow> <mo mathvariant="normal">μ</mo> <mi mathvariant="normal">m</mi> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mn>150</mn> <mo> </mo> <mrow> <mo mathvariant="normal">μ</mo> <mi mathvariant="normal">m</mi> </mrow> </mrow> </semantics></math> depths of the device. The lines represent the simulation data and the points the experimental values.</p>
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17 pages, 6384 KiB  
Article
Design and Test of a Calibration System for Avalanche Photodiodes Used in X-Ray Compton Polarimeters for Space
by Andrea Alimenti, Fabrizio Cologgi, Sergio Fabiani, Kostiantyn Torokhtii, Enrico Silva, Ettore Del Monte, Ilaria Baffo, Sergio Bonomo, Daniele Brienza, Riccardo Campana, Mauro Centrone, Giulia De Iulis, Enrico Costa, Giovanni Cucinella, Andrea Curatolo, Nicolas De Angelis, Giovanni De Cesare, Andrea Del Re, Sergio Di Cosimo, Simone Di Filippo, Alessandro Di Marco, Giuseppe Di Persio, Immacolata Donnarumma, Pierluigi Fanelli, Abhay Kumar, Paolo Leonetti, Alfredo Locarini, Pasqualino Loffredo, Giovanni Lombardi, Gabriele Minervini, Dario Modenini, Fabio Muleri, Silvia Natalucci, Andrea Negri, Massimo Perelli, Monia Rossi, Alda Rubini, Emanuele Scalise, Paolo Soffitta, Andrea Terracciano, Paolo Tortora, Emanuele Zaccagnino and Alessandro Zambardiadd Show full author list remove Hide full author list
Sensors 2024, 24(24), 8016; https://doi.org/10.3390/s24248016 - 15 Dec 2024
Cited by 1 | Viewed by 618
Abstract
The development and calibration of a measurement system designed for assessing the performance of the avalanche photodiodes (APDs) used in the Compton scattering polarimeter of the CUSP project is discussed in this work. The designed system is able to characterize the APD gain [...] Read more.
The development and calibration of a measurement system designed for assessing the performance of the avalanche photodiodes (APDs) used in the Compton scattering polarimeter of the CUSP project is discussed in this work. The designed system is able to characterize the APD gain GAPD and energy resolution across a wide range of temperatures T (from −20 °C to +60 °C) and bias voltages Vbias (from 260 V to 410 V). The primary goal was to experimentally determine the GAPD dependence on the T and Vbias in order to establish a strategy for stabilizing GAPD by compensating for T fluctuations, acting on Vbias. The results demonstrate the system capability to accurately characterize APD behavior and develop feedback mechanisms to ensure its stable operation. This work provides a robust framework for calibrating APDs for space environments. It is essential for the successful implementation of spaceborne polarimeters such as the Compton scattering polarimeter foreseen aboard the CUbeSat Solar Polarimeter (CUSP) mission under development to perform solar flare X-ray polarimetry. Full article
(This article belongs to the Section Electronic Sensors)
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<p>Block diagram of the designed and tested measurement system.</p>
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<p>Charge preamplifier electrical circuit [<a href="#B34-sensors-24-08016" class="html-bibr">34</a>].</p>
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<p>Block diagram of the signal preconditioning. The charge pulses in the output from the APD are passed to the preamplification stage to transform these into a voltage signal. Finally, this is passed to a pulse-shaping and voltage amplifier.</p>
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<p>Wire diagram of the electronic circuit realized to adapt the current output of the AD590 temperature transducers to the input characteristics of the PicoLog.</p>
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<p>Picture of the measurement setup loaded into the climate chamber.</p>
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<p>Effect of different wiring in the system on the voltage pulses generated by the spectroscopy amplifier. (<b>a</b>) The pulses when a 150 cm long LEMO cable is used. (<b>b</b>) When the cable used in (<b>a</b>) is substituted with one 15 cm long. In both pictures, the vertical scale is set to 200 mV/div.</p>
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<p>Histograms of the heights of the voltage peaks in input to the MCA and for different <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>b</mi> <mi>i</mi> <mi>a</mi> <mi>s</mi> </mrow> </msub> </semantics></math> values. The grey points are the experimental data and the continuous lines are the fitted Gaussian curves. Data are obtained by placing the <sup>55</sup>Fe sample directly in contact with the APD, at room temperature. The arrow indicates the direction in which the centroid shifts when <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>b</mi> <mi>i</mi> <mi>a</mi> <mi>s</mi> </mrow> </msub> </semantics></math> is increased.</p>
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<p>Energy resolution <math display="inline"><semantics> <mrow> <mi>δ</mi> <mi>E</mi> <mo>/</mo> <mi>E</mi> </mrow> </semantics></math> measured at room temperature by placing the <sup>55</sup>Fe sample directly in contact with the APD, for different shaping times <math display="inline"><semantics> <msub> <mi>t</mi> <mi>s</mi> </msub> </semantics></math>.</p>
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<p>The position of the measured centroids <math display="inline"><semantics> <mrow> <mi>C</mi> <msub> <mi>h</mi> <mrow> <mi>p</mi> <mi>k</mi> </mrow> </msub> </mrow> </semantics></math> with respect to the energy <span class="html-italic">E</span> of the incident X-ray photons. Data are measured using the <sup>109</sup>Cd, <sup>241</sup>Am, <sup>57</sup>Co samples with GAGG. Uncertainty bars are contained in the dimension of the symbols.</p>
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<p>APD gain <math display="inline"><semantics> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> </semantics></math> measured for different biasing voltages <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>b</mi> <mi>i</mi> <mi>a</mi> <mi>s</mi> </mrow> </msub> </semantics></math> and temperatures <span class="html-italic">T</span>. Measurements are obtained by placing the <sup>55</sup>Fe source in direct contact with the APD under test.</p>
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<p>(<b>a</b>) Fit of the APD gain <math display="inline"><semantics> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> </semantics></math> measured at −20 °C with the following functions: (1) <math display="inline"><semantics> <mrow> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo>/</mo> <mrow> <mo>(</mo> <mn>1</mn> <mo>−</mo> <msup> <mrow> <mo>(</mo> <msub> <mi>V</mi> <mrow> <mi>b</mi> <mi>i</mi> <mi>a</mi> <mi>s</mi> </mrow> </msub> <mo>/</mo> <msub> <mi>V</mi> <mn>0</mn> </msub> <mo>)</mo> </mrow> <mi>n</mi> </msup> <mo>)</mo> </mrow> </mrow> </semantics></math> [<a href="#B29-sensors-24-08016" class="html-bibr">29</a>,<a href="#B30-sensors-24-08016" class="html-bibr">30</a>]; (2) <math display="inline"><semantics> <mrow> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> <mo>=</mo> <mi>a</mi> <mo>/</mo> <mrow> <mo>(</mo> <mi>b</mi> <msup> <mi mathvariant="normal">e</mi> <mrow> <mo>(</mo> <mi>a</mi> <mrow> <mo>(</mo> <mi>V</mi> <mn>0</mn> <mo>−</mo> <msub> <mi>V</mi> <mrow> <mi>b</mi> <mi>i</mi> <mi>a</mi> <mi>s</mi> </mrow> </msub> <mo>)</mo> </mrow> <mo>−</mo> <mn>1</mn> <mo>)</mo> </mrow> </msup> <mo>)</mo> </mrow> </mrow> </semantics></math> [<a href="#B30-sensors-24-08016" class="html-bibr">30</a>]; (3) <math display="inline"><semantics> <mrow> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> <mo>=</mo> <mi>a</mi> <mo>+</mo> <mi>b</mi> <msup> <mi mathvariant="normal">e</mi> <mrow> <mo>(</mo> <mi>c</mi> <msub> <mi>V</mi> <mrow> <mi>b</mi> <mi>i</mi> <mi>a</mi> <mi>s</mi> </mrow> </msub> <mo>)</mo> </mrow> </msup> </mrow> </semantics></math> [<a href="#B29-sensors-24-08016" class="html-bibr">29</a>]. (<b>b</b>) Relative error <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msub> <mi>G</mi> <mrow> <mi>f</mi> <mi>i</mi> <mi>t</mi> </mrow> </msub> <mo>−</mo> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> <mo>)</mo> </mrow> <mo>/</mo> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> obtained by the residuals of the fit shown in (<b>a</b>). The determination coefficients for the three fits are (1) <math display="inline"><semantics> <mrow> <msubsup> <mi>R</mi> <mn>1</mn> <mn>2</mn> </msubsup> <mo>=</mo> <mn>0.981</mn> </mrow> </semantics></math>; (2) <math display="inline"><semantics> <mrow> <msubsup> <mi>R</mi> <mn>1</mn> <mn>2</mn> </msubsup> <mo>=</mo> <mn>0.995</mn> </mrow> </semantics></math>; (3) <math display="inline"><semantics> <mrow> <msubsup> <mi>R</mi> <mn>1</mn> <mn>2</mn> </msubsup> <mo>=</mo> <mn>0.997</mn> </mrow> </semantics></math>.</p>
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<p>APD gain <math display="inline"><semantics> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> </semantics></math> measured for different biasing voltages <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>b</mi> <mi>i</mi> <mi>a</mi> <mi>s</mi> </mrow> </msub> </semantics></math> and temperatures <span class="html-italic">T</span>, placing the APD in direct contact with the <sup>55</sup>Fe source. The experimental data are fitted with the function shown in Equation (<a href="#FD2-sensors-24-08016" class="html-disp-formula">2</a>).</p>
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<p>APD voltage bias <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>b</mi> <mi>i</mi> <mi>a</mi> <mi>s</mi> </mrow> </msub> </semantics></math> control curves for the stabilization of the gain <math display="inline"><semantics> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> </semantics></math> from −20 °C to 60 °C.</p>
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<p>Relative standard uncertainty of the APD gain <math display="inline"><semantics> <mrow> <mi>u</mi> <mrow> <mo>(</mo> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> <mo>)</mo> </mrow> <mo>/</mo> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> obtainable with the stabilization curves reported in <a href="#sensors-24-08016-f013" class="html-fig">Figure 13</a>. In the insert is a zoom of the curve near the minimum. For <math display="inline"><semantics> <mrow> <msub> <mi>G</mi> <mrow> <mi>A</mi> <mi>P</mi> <mi>D</mi> </mrow> </msub> <mo>≤</mo> <mn>16.2</mn> </mrow> </semantics></math>, the curve is not defined; see Equation (<a href="#FD8-sensors-24-08016" class="html-disp-formula">8</a>).</p>
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15 pages, 7434 KiB  
Article
A New Approach to Enhancing Radiation Hardness in Advanced Nuclear Radiation Detectors Subjected to Fast Neutrons
by Aref Vakili, Mahsa Farasat, Antonino La Magna, Markus Italia and Lucio Pancheri
Instruments 2024, 8(4), 53; https://doi.org/10.3390/instruments8040053 - 12 Dec 2024
Viewed by 543
Abstract
Low-Gain Avalanche Diodes (LGADs) are critical sensors for the ATLAS and CMS timing detectors at the High Luminosity Large Hadron Collider (HL-LHC), offering enhanced timing resolution with gain factors of 20 to 50. However, their radiation tolerance is hindered by the Acceptor Removal [...] Read more.
Low-Gain Avalanche Diodes (LGADs) are critical sensors for the ATLAS and CMS timing detectors at the High Luminosity Large Hadron Collider (HL-LHC), offering enhanced timing resolution with gain factors of 20 to 50. However, their radiation tolerance is hindered by the Acceptor Removal Phenomenon (ARP), which deactivates boron in the gain layer, reducing gain below the threshold for accurate timing. This study investigates the radiation hardness of thin, carbon-doped LGAD sensors developed by Brookhaven National Laboratory (BNL) to address ARP-induced limitations. Active dopant profiles in the gain layer, junction, and bulk were measured using a Spreading Resistance Probe (SRP) profilometer, and the effects of annealing and neutron irradiation at fluences of 3 × 1014, 1 × 1015, and 3 × 1015 neq/cm2 (1 MeV equivalent) were analyzed. Low carbon dose rates showed minimal improvement due to enhanced deactivation, while higher doses improved radiation hardness, demonstrating a non-linear dose–response relationship. These findings highlight the potential of optimizing gain layers with high carbon doses and low-diffusion boron to extend LGAD lifetimes in high-radiation environments. Future research will refine carbon implantation strategies and explore alternative approaches to further enhance the radiation hardness of LGADs. Full article
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<p>The basic structure of a Low-Gain Avalanche Detector.</p>
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<p>A group of BNL-LGADs [<a href="#B24-instruments-08-00053" class="html-bibr">24</a>].</p>
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<p>Schematic overview of the probe station setup for performing: (<b>top</b>) I–V tests, where the high-voltage (HV) and ground ports of the HV-SMU are connected to the chuck and guard ring, respectively, while the second needle contacts the pad and is connected to the MP-SMU, which provides better current resolution than the HV-SMU; (<b>bottom</b>) C–V tests, illustrated for a single-pad sensor, where a DC voltage from the HV-SMU and an AC signal from the MF-CMU are combined via a Bias–T interface. The chuck and pad needle are connected to the high- and low-voltage outputs of the Bias–T, respectively, and the capacitance measured corresponds to the pad-to-back sensor interface [<a href="#B9-instruments-08-00053" class="html-bibr">9</a>].</p>
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<p>CERN probe station setup: the connections of the needles to the detectors placed on the chuck surface inside the probe station.</p>
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<p>Photo of the BNL-LGAD design showing the dedicated connections inside the probe station during a relevant measurement campaign.</p>
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<p>Measured C–V characteristics of carbon-doped devices before irradiation.</p>
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<p>Extracted doping profiles of BNL sensors based on C–V measurements.</p>
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<p>Schematic representation of the Spreading Resistance Profiling (SRP) measurement setup.</p>
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<p>Experimental SRP calibration data for &lt;100&gt; n-type and p-type silicon.</p>
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<p>The carrier concentration and resistivity profiles of the grown wafer as a function of depth, based on SRP analysis.</p>
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<p>The first results obtained in the SRP laboratory.</p>
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<p>Deactivation of the boron profile after neutron irradiation.</p>
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<p>Deactivation of the p+/p− junction after neutron irradiation.</p>
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<p>Deactivation after neutron irradiation for the substrate, showing the complete charge carrier profiles of the epitaxial layers.</p>
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13 pages, 10213 KiB  
Article
2 km Uncompressed HD Video Wireless Transmission at 100 GHz Based on All-Optical Frequency Up- and Down-Conversion
by Shuang Gao, Yutong Jiang, Zhuoxin Li, Qing Zhong, Min Zhu and Jiao Zhang
Micromachines 2024, 15(12), 1488; https://doi.org/10.3390/mi15121488 - 11 Dec 2024
Viewed by 489
Abstract
The millimeter-wave wireless transmission system is widely regarded as a promising solution for applications of future 6G communication. This paper presents an experimental comparison between all-optical and all-electric receivers for millimeter-wave communication systems over a 15 m wireless link and demonstrates 200 m [...] Read more.
The millimeter-wave wireless transmission system is widely regarded as a promising solution for applications of future 6G communication. This paper presents an experimental comparison between all-optical and all-electric receivers for millimeter-wave communication systems over a 15 m wireless link and demonstrates 200 m and 2 km real-time uncompressed HD video transmission using an all-optical transceiver at 100 GHz. The systems leverage photonics-assisted heterodyne beating techniques at the transmitter, while the receivers employ either an avalanche photodiode (APD)-based all-optical approach or an envelope detection-based all-electric approach. Experimental results show that the all-optical transceiver supports significantly higher transmission rates, achieving error-free transmission at up to 11.318 Gbps over a 200 m wireless link without clock recovery, compared to the all-electric receiver, which is limited to only 3.125 Gbps error-free 15 m transmission. This work proves that the proposed system based on the all-optical receiver is more promising for supporting future 6G scenarios requiring ultra-wideband, high capacity, and wide coverage high-speed wireless communications. Full article
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<p>Scenarios for mmWave wireless communication under IMT-2030 framework.</p>
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<p>Specific attenuation as a function of frequency under case 1, case 2, and dry air condition.</p>
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<p>The architecture of the transmission system, including approaches of the all-electric receiver based on envelope detection and all-optical receiver. (<b>i</b>) All-electric receiver. (<b>ii</b>) All-optical receiver.</p>
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<p>The measured optical spectra: (<b>a</b>) after the intensity modulator at the transmitting side, (<b>b</b>) of the received signal after the phase modulator, DWDM, TOF in the all-optical receiver, and the passband of TOF.</p>
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<p>Photos of the indoor transmission system: (<b>a</b>) transmitter, (<b>b</b>) all-electric receiver, (<b>c</b>) all-optical receiver.</p>
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<p>Experimental setup of the outdoor transmission: satellite map of the transmission link over a distance of (<b>a</b>) 200 m and (<b>d</b>) 2 km. Photos of the receiving side of (<b>b</b>) 200 m and (<b>e</b>) 2 km transmission. Photos of (<b>c</b>) real-time HD video displayed on the screen and (<b>f</b>) the transmitting side of 2 km transmission.</p>
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<p>Phase noise as a function of frequency offset.</p>
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<p>BER as a function of the signal amplitude into the intensity modulator for indoor transmission over a distance of 15 m based on (<b>a</b>) the all-electric receiver and (<b>b</b>) the all-optical receive.</p>
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<p>Signal waveform, spectrum, and demodulated eye diagram for 5 Gbit/s OOK signal of (<b>a</b>) all-electric receiver and (<b>b</b>) all-optical receiver.</p>
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<p>BER as a function of the received optical power for outdoor transmission over the distance of (<b>a</b>) 200 m and (<b>b</b>) 2 km.</p>
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