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4D event imaging with a single neuromorphic camera
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作者 Raviv Ilani Adrian Stern 《Advanced Photonics Nexus》 2026年第1期61-70,共10页
Neuromorphic cameras,or dynamic vision sensors,are bio-inspired event cameras that measure changes in the image brightness asynchronously and independently at the pixel level.Recently,they garnered increasing interest... Neuromorphic cameras,or dynamic vision sensors,are bio-inspired event cameras that measure changes in the image brightness asynchronously and independently at the pixel level.Recently,they garnered increasing interest due to their extremely high temporal resolution,wide dynamic range,low power consumption,and high pixel bandwidth.Despite their advantages,most existing three-dimensional (3D) event imaging solutions rely on multicamera configurations,which are costly,complex,and challenging to synchronize.In this study,we introduce a new framework for four-dimensional (4D) event imaging using a single static neuromorphic camera.We take advantage of the inherent sparsity of event data to combine optically encoded stereo channels into a single event camera.By utilizing optical channel multiplexing,we maintain sensor resolution while retaining the key advantages of event cameras. 展开更多
关键词 imaging and sensing bio-inspired image sensors neuromorphic imaging 3D imaging
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Optical-Focused Fresnel Lens for Generating Electricity Output Using Multiple Layers of Heated Disks with Water as a Medium
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作者 Hung-Te Henry Su Po-Han Lee 《Journal of Environmental Science and Engineering(B)》 2025年第2期76-80,共5页
Concentrated solar thermal power generation has been experimentally tested in advanced countries for a period of time.This paper demonstrates how this technology can be improved by using water molecules as a medium to... Concentrated solar thermal power generation has been experimentally tested in advanced countries for a period of time.This paper demonstrates how this technology can be improved by using water molecules as a medium to drive traditional generator sets for energy conversion,thereby simultaneously improving the energy conversion rate.Additionally,a novel contribution is made by incorporating a magic number 4 to enhance the focusing efficiency of Fresnel lenses,which drives improvements in power generation output and QE(Quantum Efficiency). 展开更多
关键词 Energy conversion rate Fresnel lens generator sets solar power volume factors magic number 4 QE
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Bose-Einstein Condensation Yb2Si2O7 Retaining Si Applied in UV-Etching 1 nm Quantum Wires
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作者 Hung Te Henry Su Po-Han Lee 《Open Journal of Physical Chemistry》 2025年第1期1-19,共19页
A Bose-Einstein condensate (BEC) is a topic of significant interest within the scientific community. It is well understood that Rb-87 and Yb2Si2O7 have been utilized in experiments to explore this phenomenon. These st... A Bose-Einstein condensate (BEC) is a topic of significant interest within the scientific community. It is well understood that Rb-87 and Yb2Si2O7 have been utilized in experiments to explore this phenomenon. These studies have demonstrated that these materials can achieve the BEC phase, a state that has been experimentally validated. In this paper, we further establish, from the perspective of theoretical physics, that silicon is also capable of exhibiting BEC properties. Our approach differs from prior studies in that it uses innovatively certain boundary conditions. Specifically, we employed Yb-70 as a gamma-ray radiation source and a 1 nm linewidth (as the half-width of a 2 nm line). Additionally, we utilized the concept of half-value thickness from nuclear physics absorption models to optimize the semiconductor process. This method effectively removes ytterbium (Yb) during the process, leaving only silicon, silicon-based materials, or silicon topological superconductors on the wafer. This technical procedure results in the creation of “BEC silicon” at absolute zero temperature (0 K), introducing a novel material for BEC realization. 展开更多
关键词 Rb-87 BEC Phase Yb-70 BEC Silicon Absolute Zero Temperature
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Orthogonal Stacked Spectral Coding Labels for Fast Packets Routing over Optical MPLS Network 被引量:1
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作者 Kai-Sheng Chen Chao-Chin Yang Jen-Fa Huang 《Journal of Electronic Science and Technology》 CAS CSCD 2015年第2期130-134,共5页
Multi-protocol label switching(MPLS) has the advantage of high efficiency in the second layer, which improves the performance of data packets routing. In this paper, a new structure to implement optical MPLS is prop... Multi-protocol label switching(MPLS) has the advantage of high efficiency in the second layer, which improves the performance of data packets routing. In this paper, a new structure to implement optical MPLS is proposed. We construct a code family for spectral-amplitude coding(SAC) labels in the optical MPLS networks. SAC labels are suitable for optical packet switching because they can be constructed and recognized quickly at each router. We use the label stacking to provide hierarchical routing to avoid swapping labels at each forwarding node and reduce system complexity. However, the phase-induced intensity noise(PIIN) appears due to the incoherent property of the light source when the stacked labels set makes the correlation decoding with the local node label,which degrades system performance. 展开更多
关键词 label hierarchical switching quickly routing decoding forwarding packet matches router
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Tunable Erbium-Doped Fiber Lasers Using Various Inline Fiber Filters
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作者 Shien-Kuei Liaw Kuei-Chu Hsu Nan-Kuang Chen 《Engineering(科研)》 2010年第8期585-593,共9页
Several high-performance and tunable erbium-doped fiber lasers are reviewed. They are constructed by using fiber Bragg gratings (FBGs) or short-wavelength-pass filters (SWPFs) as wavelength tunable components inside t... Several high-performance and tunable erbium-doped fiber lasers are reviewed. They are constructed by using fiber Bragg gratings (FBGs) or short-wavelength-pass filters (SWPFs) as wavelength tunable components inside the laser cavity. Broadband wavelength tuning range including C- and/or S-band was achieved, and tunable laser output with high slope efficiency, high side-mode suppression ratio was obtained. These fiber lasers can find vast applications in lightwave transmission, optical test instrument, fiber-optic gyros, spectroscopy, material processing, biophotonic imaging, and fiber sensor technologies. 展开更多
关键词 FIBER BRAGG GRATING (FBG) Short-Wavelength-Pass Filter (SWPF) TUNABLE FIBER Laser Optical
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A Model of Grand Unified Theory: Suggested Solution for CP-Violation Using Ideas of Phase Paths
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作者 Hung-Te Henry Su Po-Han Lee 《Journal of High Energy Physics, Gravitation and Cosmology》 CAS 2024年第4期1878-1902,共25页
This study demonstrates that beyond standard model (BSM) cosmic fundamental interactions—weak, strong, and electromagnetic forces—can be unified through a common basis of representation. This unification allows for ... This study demonstrates that beyond standard model (BSM) cosmic fundamental interactions—weak, strong, and electromagnetic forces—can be unified through a common basis of representation. This unification allows for the derivation of the fine structure constant with running points of α(t) ≈ 1/(136.9038) at high energy scales, based on electroweak interactions. Through the application of the Ising model, the running point of the elementary charge e at high energy scales is determined, and Coulomb’s law is actually derived from the Yukawa potential. Theoretically, based on S. Weinberg’s electroweak interaction theory, this study unifies the strong and electromagnetic forces by representing them with rYuka, and further advances the reconstruction of the SU(3)C×SU(1)L×U(1)EMframework on the basis of electroweak interaction concepts. In fact, the cosmic fundamental forces can interchange at the mass gap, defined as the Yukawa turning phase at rYuka ≃1.9404 fm, with the SU(3)Diag structural constant fijk on glueballs calculated, estimating a spectrum mass gap of ∆0 > 0. 展开更多
关键词 BSM ELECTROWEAK GLUEBALLS Ising Model Mass Gap S. Weinberg
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On a Heuristic Point of View about the Generalization of Curie Law to Cosmic Higgs Fields with the Casimir Effect
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作者 Hung-Te Henry Su Po-Han Lee 《Journal of Applied Mathematics and Physics》 2024年第9期3135-3147,共13页
Condensed state physics demonstrates that the Curie temperature is the point at which spontaneous magnetization drops to zero, marking the critical transition where ferromagnetic or ferrimagnetic materials transform i... Condensed state physics demonstrates that the Curie temperature is the point at which spontaneous magnetization drops to zero, marking the critical transition where ferromagnetic or ferrimagnetic materials transform into paramagnetic substances. Below the Curie temperature, a material remains ferromagnetic;above it, the material becomes paramagnetic, with its magnetic field easily influenced by external magnetic fileds. For example, the Curie temperature of iron (Fe) is 1043 K, while that of neodymium magnets ranges from 583 to 673 K. From both physics and mathematics perspectives, examining the temperature properties of materials is essential, as it provides valuable insights into their electromagnetic and thermodynamic behaviors. This paper makes a bold assumption and, for the first time, carefully verifies the existence of a Casimir temperature at 0.00206 K under conditions of one-atomic spacing. 展开更多
关键词 Curie Temperature Curie Point Casimir Temperature Critical Point Fields Materials One-Atomic Spacing
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Definite Answer for Riemann Hypothesis Zeta 3/2 Function Provided by New Material Yb2Si2O7 in Quantum Mechanics
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作者 Hung-Te Henry Su Po-Han Lee 《Journal of Modern Physics》 2024年第9期1409-1429,共21页
This paper indicates the problem of the famous Riemann hypothesis (RH), which has been well-verified by a definite answering method using a Bose-Einstein Condensate (BEC) phase. We adopt mathematical induction, mappin... This paper indicates the problem of the famous Riemann hypothesis (RH), which has been well-verified by a definite answering method using a Bose-Einstein Condensate (BEC) phase. We adopt mathematical induction, mappings, and laser photons governed by electromagnetically induced transparency (EIT) to examine the existence of the RH. In considering the well-developed as Riemann zeta function, we find that the existence of RH has a corrected and self-consistent solution. Specifically, there is the only one pole at s = 1 on the complex plane for Riemann’s functions, which generalizes to all non-trivial zeros while s > 1. The essential solution is based on the BEC phases and on the nature of the laser photon(s). This work also incorporates Heisenberg commutators [ x^,p^]=1/2in the field of quantum mechanics. We found that a satisfactory solution for the RH would be incomplete without the formalism of Heisenberg commutators, BEC phases, and EIT effects. Ultimately, we propose the application of qubits in connection with the RH. 展开更多
关键词 BEC Phases EIT Heisenberg Commutators Laser Photons QUBITS Riemann Hypothesis
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Classifying Vibration Modes Generated by The Michelson Interferometer Using Machine Learning Methods
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作者 Xin-Han Tsai Anthony An-Chih Yeh +4 位作者 Chen-Hsin Lu Shang-Yu Chou Shih-Wei Wang Chi-Wei Lee Po-Han Lee 《Journal of Modern Physics》 2024年第12期2169-2192,共24页
In this paper, we explore the classification of vibration modes generated by handwriting on an optical desk using deep learning architectures. Three deep learning models—Long Short-Term Memory (LSTM) networks with at... In this paper, we explore the classification of vibration modes generated by handwriting on an optical desk using deep learning architectures. Three deep learning models—Long Short-Term Memory (LSTM) networks with attention mechanism, Video Vision Transformer (ViViT), and Long-term Recurrent Convolutional Network (LRCN)—were evaluated to determine the most effective method for analyzing time series patterns generated by a Michelson interferometer. The interferometer was used to detect vibration modes created by handwriting, capturing time-series data from the diffraction patterns. Among these models, the LSTM-Attention network achieved the highest validation accuracy, reaching up to 92%, outperforming both ViViT and LRCN. These findings highlight the potential of deep learning in material science for detecting and classifying vibration patterns. The powerful performance of the LSTM-Attention model suggests that it could be applied to similar classification tasks in related fields. 展开更多
关键词 Michelson Interferometer Machine Learning Vibration Modes Long Short-Term Memory (LSTM)
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A New Code Family for Double Spread Transmissions in Radio-over-Fiber over Optical CDMA Network
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作者 Kai-Sheng Chen Chao-Chin Yang +1 位作者 Jen-Fa Huang Hsuan-Ho Chang 《通讯和计算机(中英文版)》 2016年第7期366-372,共7页
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Synergistic design of a tin phosphate-entrapped graphene flake nanocomposite as an efficient catalyst for electrochemical determination of the antituberculosis drug isoniazid in biological samples
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作者 Thangavelu Kokulnathan V.Suvina +1 位作者 Tzyy-Jiann Wang R.Geetha Balakrishna 《Inorganic Chemistry Frontiers》 2019年第7期1831-1841,共11页
The rapid quantification of drugs in biological samples has become an important issue and ongoing challenge to protect human health.To address this issue,we designed and synthesized a tin phosphateentrapped graphene f... The rapid quantification of drugs in biological samples has become an important issue and ongoing challenge to protect human health.To address this issue,we designed and synthesized a tin phosphateentrapped graphene flake(SnP/GRF)nanocomposite for the trace level electrochemical detection of the antituberculosis drug isoniazid(ISZ). 展开更多
关键词 nanocomposite trace level electrochemical detection graphene flake electrochemical determination tin phosphate biological samples protect human healthto rapid quantification drugs
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Initial performance results of the JUNO detector
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作者 Angel Abusleme Thomas Adam +1137 位作者 Kai Adamowicz David Adey Shakeel Ahmad Rizwan Ahmed Timo Ahola Sebastiano Aiello Fengpeng An Guangpeng An Costas Andreopoulos Giuseppe Andronico João Pedro Athayde Marcondes de André Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop Didier Auguste Margherita Buizza Avanzini Andrej Babic Jingzhi Bai Weidong Bai Nikita Balashov Roberto Barbera Andrea Barresi Davide Basilico Eric Baussan Beatrice Bellantonio Marco Bellato JeanLuc Beney Marco Beretta Antonio Bergnoli Enrico Bernieri Nikita Bessonov David Biaré Daniel Bick Lukas Bieger Svetlana Biktemerova Thilo Birkenfeld David Blum Simon Blyth Sara Boarin Manuel Boehles Anastasia Bolshakova Mathieu Bongrand Aurélie Bonhomme Clément Bordereau Matteo Borghesi Augusto Brigatti Timothee Brugiere Riccardo Brugnera Riccardo Bruno Jonas Buchholz Antonio Budano Max Buesken Mario Buscemi Severino Bussino Jose Busto Ilya Butorov Marcel Büchner Anatael Cabrera Barbara Caccianiga Boshuai Cai Hao Cai Xiao Cai Yanke Cai Yi-zhou Cai Zhiyan Cai Stéphane Callier Steven Calvez Antonio Cammi Agustin Campeny Dechang Cai Chuanya Cao Dewen Cao Guofu Cao Jun Cao Yaoqi Cao Rossella Caruso Aurelio Caslini Cédric Cerna Vanessa Cerrone Daniele Cesini Chi Chan Jinfan Chang Yun Chang Milo Charavet Tim Charissé Auttakit Chatrabhuti Chao Chen Guoming Chen Haitao Chen Haotian Chen Jiahui Chen Jian Chen Jing Chen Junyou Chen Lihao Chen Mali Chen Mingming Chen Pingping Chen Po-An Chen Quanyou Chen Shaomin Chen Shenjian Chen Shi Chen Shiqiang Chen Sisi Chen Xin Chen Xuan Chen Xurong Chen Yi-Wen Chen Yiming Chen Yixue Chen Yu Chen Ze Chen Zelin Chen Zhang Chen Zhangming Chen Zhiyuan Chen Zhongchang Chen Zikang Chen Brian Cheng Jie Cheng Yaping Cheng Yu Chin Cheng Zhaokan Cheng Alexander Chepurnov Alexey Chetverikov Davide Chiesa Pietro Chimenti Yen-Ting Chin Pin-Jung Chiu Po-Lin Chou Ziliang Chu Artem Chukanov Neetu Raj Singh Chundawat Anna Chuvashova Gérard Claverie Catia Clementi Barbara Clerbaux Claudio Coletta Marta Colomer Molla Flavio Dal Corso Daniele Corti Salvatore Costa Simon Csakli Chenyang Cui Shanshan Cui Lorenzo Vincenzo D'Auria Olivia Dalager Jaydeep Datta Luis Delgadillo Franco Jiawei Deng Zhi Deng Ziyan Deng Wilfried Depnering Hanna Didenko Xiaoyu Ding Xuefeng Ding Yayun Ding Bayu Dirgantara Carsten Dittrich Sergey Dmitrievsky David Doerflinger Tadeas Dohnal Maria Dolgareva Dmitry Dolzhikov Chuanshi Dong Haojie Dong Jianmeng Dong Lan Dong Damien Dornic Evgeny Doroshkevich Wei Dou Marcos Dracos Olivier Drapier Tobias Drohmann Frédéric Druillole Ran Du Shuxian Du Yujie Duan Katherine Dugas Stefano Dusini Hongyue Duyang Martin Dvorak Jessica Eck Timo Enqvist Heike Enzmann Andrea Fabbri Ulrike Fahrendholz Lukas Fajt Donghua Fan Lei Fan Liangqianjin Fan Can Fang Jian Fang Wenxing Fang Marco Fargetta Elia Stanescu Farilla Anna Fatkina Laurent Favart Dmitry Fedoseev Zhengyong Fei Franz von Feilitzsch Vladko Fekete Li-Cheng Feng Qichun Feng Shaoting Feng Giovanni Ferrante Federico Ferraro Daniela Fetzer Giovanni Fiorentini Andrey Formozov Marcellin Fotzé Amélie Fournier Sabrina Franke Arran Freegard Florian Fritsch Ying Fu Haonan Gan Feng Gao Ruixuan Gao Ruohan Gao Shijiao Gao Alberto Garfagnini Gerard Gaudiot Arsenii Gavrikov Raphaël Gazzini Christoph Genster Diwash Ghimire Marco Giammarchi Agnese Giaz Gianfranco Giordano Nunzio Giudice Franco Giuliani Alexandre Goettel Maxim Gonchar Guanda Gong Guanghua Gong Hui Gong Michel Gonin Oleg Gorchakov Yuri Gornushkin Marco Grassi Christian Grewing Maxim Gromov Vasily Gromov Minhao Gu Xiaofei Gu Yu Gu Mengyun Guan Yuduo Guan Nunzio Guardone Rosa Maria Guizzetti Cong Guo Jingyuan Guo Wanlei Guo Yuhang Guo Paul Hackspacher Caren Hagner Hechong Han Ran Han Xiao Han Yang Han Ziguo Han Chuanhui Hao Jiajun Hao Vidhya Thara Hariharan JinCheng He Jinhong He Miao He Mingtao He Wei He Xinhai He Ziou He Tobias Heinz Dominikus Hellgartner Patrick Hellmuth Shilin Heng Yuekun Heng Rafael Herrera Daojin Hong YuenKeung Hor Shaojing Hou Zhilong Hou Fatima Houria Yee Hsiung Bei-Zhen Hu Hang Hu Hao Hu Jianrun Hu Jun Hu Peng Hu Tao Hu Wei Hu Yuxiang Hu Zhuojun Hu Chunhao Huang Guihong Huang Hanyu Huang Hexiang Huang Jinhao Huang Junlin Huang Junting Huang Kairui Huang Kaixuan Huang Qinhua Huang Shengheng Huang Tao Huang Wenhao Huang Xiaozhong Huang Xin Huang Xingtao Huang Yongbo Huang Lian-Chen Huang Jiaqi Hui Lei Huo Cédric Huss Safeer Hussain Leonard Imbert Antonio Insolia Ara Ioannisian Daniel Ioannisyan Ammad Ul Islam Roberto Isocrate Adrienne Jacobi Arshak Jafar Beatrice Jelmini Kuo-Lun Jen Soeren Jetter Xiangpan Ji Xiaolu Ji Xingzhao Ji Huihui Jia Junji Jia Yi Jia Cailian Jiang Chengbo Jiang Guangzheng Jiang Junjie Jiang Wei Jiang Xiaoshan Jiang Xiaozhao Jiang Yijian Jiang Yixuan Jiang Yue Jiang Ruyi Jin Shuzhu Jin Xiaoping Jing Cécile Jollet Liam Jones Jari Joutsenvaara Sirichok Jungthawan Philipp Kampmann Markus Kaiser Leonidas Kalousis Bowen Kan Li Kang Michael Karagounis Rebin Karaparambil Matej Karas Narine Kazarian Ali Khan Amir Khan Amina Khatun Khanchai Khosonthongkee Florian Kiel Patrick Kinz Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Zinovy Krumshteyn Andre Kruth Tim Kuhlbusch Sergey Kuleshov Sindhujha Kumaran Chun-Hao Kuo Nikolay Kutovskiy Pasi Kuusiniemi Loïc Labit Tobias Lachenmaier Haojing Lai ToUyen LamThi Philipp Landgraf Cecilia Landini Lorenzo Lastrucci Fedor Lazarev Sébastien Leblanc Victor Lebrin Matthieu Lecocq Priscilla Lecomte Frederic Lefevre Liping Lei Ruiting Lei Xiangcui Lei Rupert Leitner Petr Lenskii Jason Leung Bo Li Chao Li Daozheng Li Demin Li Dian Li Fei Li Fule Li Gaoshuang Li Gaosong Li Haitao Li Hongjian Li Huang Li Huiling Li Jiajun Li Jiaqi Li Jin Li Kaijie Li Meiou Li Mengzhao Li Min Li Nan Li Qingjiang Li Quanlin Li Ruhui Li Rui Li Shanfeng Li Shuaijie Li Shuo Li Tao Li Teng Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xiwen Li Xinying Li Yang Li Yawen Li Yi Li Yichen Li Yifan Li Yingke Li Yuanxia Li Yufeng Li Zepeng Li Zhaohan Li Zhibing Li Zhiwei Li Zi-Ming Li Ziyuan Li Zonghai Li An-An Liang Jing Liang Jingjing Liang Jiajun Liao Minghua Liao Yilin Liao Yuzhong Liao Daniel Liebau Ayut Limphirat Sukit Limpijumnong Bo-Chun Lin Guey-Lin Lin Jiming Lin Shengxin Lin Tao Lin Xianhao Lin Xingyi Lin Yen-Hsun Lin Jiacheng Ling Jiajie Ling Xin Ling Ivano Lippi Caimei Liu Fang Liu Fengcheng Liu Gang Liu Haidong Liu Haotian Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hongyang Liu Hu Liu Hui Liu Jianglai Liu Jianli Liu Jiaxi Liu Jin'gao Liu Jinchang Liu Jinyan Liu Kainan Liu Lei Liu Libing Liu Mengchao Liu Menglan Liu Min Liu Qishan Liu Qian Liu Qin Liu Runxuan Liu Shenghui Liu Shuangyu Liu Shubing Liu Shulin Liu Wanjin Liu Xiaowei Liu Ximing Liu Xinkang Liu Xiwen Liu Xuewei Liu Yan Liu Yankai Liu Yin Liu Yiqi Liu Yuanyuan Liu Yuexiang Liu Yunzhe Liu Zhen Liu Zhipeng Liu Zhuo Liu Domenico Lo Presti Salvatore Loffredo Lorenzo Loi Paolo Lombardi Claudio Lombardo Yongbing Long Andrea Longhin Fabio Longhitano Kai Loo Sebastian Lorenz Selma Conforti Di Lorenzo Chuan Lu Fan Lu Haoqi Lu Jiashu Lu Junguang Lu Meishu Lu Peizhi Lu Shuxiang Lu Xianghui Lu Xianguo Lu Xiaoxu Lu Xiaoying Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov Daibin Luo Fengjiao Luo Guang Luo Jianyi Luo Pengwei Luo Shu Luo Tao Luo Wuming Luo Xiaojie Luo Xiaolan Luo Zhipeng Lv Vladimir Lyashuk Bangzheng Ma Bing Ma Na Ma Qiumei Ma Si Ma Wing Yan Ma Xiaoyan Ma Xubo Ma Santi Maensiri Jingyu Mai Romain Maisonobe Marco Malabarba Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Xin Mao Yajun Mao Stefano MMari Cristina Martellini Agnese Martini Jacques Martino Johann Martyn Matthias Mayer Davit Mayilyan Worawat Meevasana Artur Meinusch Qingru Meng Yue Meng Anita Meraviglia Anselmo Meregaglia Emanuela Meroni David Meyhöfer Jian Min Lino Miramonti Nikhil Mohan Salvatore Monforte Paolo Montini Michele Montuschi Nikolay Morozov Iwan Morton-Blake Xiangyi Mu Pavithra Muralidharan Lakshmi Murgod Axel Müller Thomas Mueller Massimiliano Nastasi Dmitry VNaumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Elisabeth Neuerburg VanHung Nguyen Dennis Nielinger Alexey Nikolaev Feipeng Ning Zhe Ning Yujie Niu Stepan Novikov Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Samantha Cantu Olea Sebastian Olivares Alexander Olshevskiy Domizia Orestano Fausto Ortica Rainer Othegraven Yifei Pan Alessandro Paoloni Nina Parkalian George Parker Sergio Parmeggiano Achilleas Patsias Teerapat Payupol Viktor Pec Davide Pedretti Yatian Pei Luca Pelicci Nicomede Pelliccia Anguo Peng Haiping Peng Yu Peng Zhaoyuan Peng Elisa Percalli Willy Perrin Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Min Pi Oliver Pilarczyk Ruben Pompilio Artyom Popov Pascal Poussot Stefano Pozzi Wathan Pratumwan Ezio Previtali Sabrina Prummer Fazhi Qi Ming Qi Xiaohui Qi Sen Qian Xiaohui Qian Zhen Qian Liqing Qin Zhonghua Qin Shoukang Qiu Manhao Qu Zhenning Qu Muhammad Usman Rajput Shivani Ramachandran Gioacchino Ranucci Neill Raper Reem Rasheed Thomas Raymond Alessandra Re Henning Rebber Abdel Rebii Bin Ren Shanjun Ren Yuhan Ren Andrea Rendina Cristobal Morales Reveco Taras Rezinko Barbara Ricci Luis Felipe Piñeres Rico Mariam Rifai Markus Robens Mathieu Roche Narongkiat Rodphai Fernanda de Faria Rodrigues Lars Rohwer Aldo Romani Vincent Rompel Bedřich Roskovec Xiangdong Ruan Xichao Ruan Peter Rudakov Saroj Rujirawat Arseniy Rybnikov Andrey Sadovsky Sahar Safari Giuseppe Salamanna Deshan Sandanayake Simone Sanfilippo Anut Sangka Nuanwan Sanguansak Ujwal Santhosh Giuseppe Sava Utane Sawangwit Julia Sawatzki Michaela Schever Jacky Schuler Cédric Schwab Konstantin Schweizer Dmitry Selivanov Alexandr Selyunin Andrea Serafini Giulio Settanta Mariangela Settimo Muhammad Ikram Shahzad Yanjun Shan Junyu Shao Zhuang Shao Anurag Sharma Vladislav Sharov Arina Shaydurova Wei Shen Gang Shi Hangyu Shi Hexi Shi Jingyan Shi Yanan Shi Yongjiu Shi Yuan Shi Dmitrii Shpotya Yike Shu Yuhan Shu She Shuai Vitaly Shutov Andrey Sidorenkov Randhir Singh Apeksha Singhal Chiara Sirignano Jaruchit Siripak Monica Sisti Maciej Slupecki Mikhail Smirnov Oleg Smirnov Thiago Sogo-Bezerra Michael Soiron Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Felix Sorgenfrei Albert Sotnikov Mario Spinetti Warintorn Sreethawong Achim Stahl Luca Stanco Korbinian Stangler Konstantin Stankevich Hans Steiger Jochen Steinmann Malte Stender Tobias Sterr David Stipp Matthias Raphael Stock Virginia Strati Mikhail Strizh Alexander Studenikin Katharina von Sturm Aoqi Su Jun Su Yuning Su Gongxing Sun Guangbao Sun Hansheng Sun Lijun Sun Liting Sun Mingxia Sun Shifeng Sun Xilei Sun Yongzhao Sun Yunhua Sun Yuning Sun Zhanxue Sun Zhengyang Sun Narumon Suwonjandee Troy Swift Michal Szelezniak DušanŠtefánik FedorŠimkovic OndřejŠrámek Dmitriy Taichenachev Christophe De La Taille Akira Takenaka Hongnan Tan Xiaohan Tan Haozhong Tang Jian Tang Jingzhe Tang Qiang Tang Quan Tang Xiao Tang Jihua Tao Eric Theisen Minh Thuan Nguyen Thi Renju Tian Yuxin Tian Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Francesco Tortorici Konstantin Treskov Andrea Triossi Wladyslaw Trzaska Andrei Tsaregorodtsev Alexandros Tsagkarakis Yu-Chen Tung Cristina Tuve Nikita Ushakov Guillaume Vanroyen Nikolaos Vassilopoulos Carlo Venettacci Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Vit Vorobel Dmitriy Voronin Lucia Votano Stefan van Waasen Stefan Wagner Pablo Walker Jiawei Wan Andong Wang Caishen Wang Chung-Hsiang Wang Cui Wang Derun Wang En Wang Guoli Wang Hanwen Wang Hongxin Wang Huanling Wang Jiabin Wang Jian Wang Jun Wang Ke Wang Kunyu Wang Lan Wang Li Wang Lu Wang Meifen Wang Meng Wang Meng Wang Mingyuan Wang Qianchuan Wang Ruiguang Wang Sibo Wang Siguang Wang Tianhong Wang Tong Wang Wei Wang Wei Wang Wenshuai Wang Wenwen Wang Wenyuan Wang Xi Wang Xiangyue Wang Xuesen Wang Yangfu Wang Yaoguang Wang Yi Wang Yi Wang Yi Wang Yifang Wang Yuanqing Wang Yuman Wang Yuyi Wang Zhe Wang Zheng Wang Zhigang Wang Zhimin Wang Zongyi Wang Apimook Watcharangkool Junya Wei Jushang Wei Lianghong Wei Wei Wei Wei Wei Wenlu Wei Yadong Wei Yuehuan Wei Zhengbao Wei Marcel Weifels Kaile Wen Liangjian Wen Yijie Wen Jun Weng Christopher Wiebusch Rosmarie Wirth Steven Chan-Fai Wong Bjoern Wonsak Baona Wu Bi Wu Chengxin Wu Chia-Hao Wu Chin-Wei Wu Diru Wu Fangliang Wu Jianhua Wu Qun Wu Shuai Wu Wenjie Wu Yinhui Wu Yiyang Wu Zhaoxiang Wu Zhi Wu Zhongyi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Jingkai Xia Shishen Xian Ziqian Xiang Fei Xiao Pengfei Xiao Tianying Xiao Xiang Xiao Wan Xie Wei-Jun Xie Xiaochuan Xie Yijun Xie Yuguang Xie Zhangquan Xie Zhao Xin Zhizhong Xing Benda Xu Cheng Xu Chuang Xu Donglian Xu Fanrong Xu Hangkun Xu Jiayang Xu Jie Xu Jilei Xu Jinghuan Xu Lingyu Xu Meihang Xu Shiwen Xu Xunjie Xu Ya Xu Yin Xu Yu Xu Dongyang Xue Jingqin Xue Baojun Yan Liangping Yan Qiyu Yan Taylor Yan Tian Yan Wenqi Yan Xiongbo Yan Yupeng Yan Anbo Yang Caihong Yang Changgen Yang Chengfeng Yang Dikun Yang Dingyong Yang Fengfan Yang Haibo Yang Huan Yang Jie Yang Jize Yang Kaiwei Yang Lei Yang Mengting Yang Pengfei Yang Xiaoyu Yang Xuhui Yang Yi Yang Yichen Yang Yifan Yang Yixiang Yang Yujiao Yang Yuzhen Yang Zekun Yang Haifeng Yao Li Yao Jiaxuan Ye Mei Ye Xingchen Ye Ziping Ye Ugur Yegin Frédéric Yermia Peihuai Yi Rattikorn Yimnirun Jilong Yin Na Yin Weiqing Yin Xiangwei Yin Xiaohao Yin Sivaram Yogathasan Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Guangyou Yu Guojun Yu Hongzhao Yu Miao Yu Peidong Yu Simi Yu Xianghui Yu Yang Yu Zeyuan Yu Zezhong Yu Cenxi Yuan Chengzhuo Yuan Zhaoyang Yuan Zhenxiong Yuan Ziyi Yuan Baobiao Yue Noman Zafar AndréZambanini Jilberto Zamora Matteo Zanetti Vitalii Zavadskyi Fanrui Zeng Pan Zeng Shan Zeng Tingxuan Zeng Yuda Zeng Yujie Zeng Liang Zhan Aiqiang Zhang Bin Zhang Binting Zhang Chengcai Zhang Enze Zhang Feiyang Zhang Guoqing Zhang Haiqiong Zhang Han Zhang Hangchang Zhang Haosen Zhang Honghao Zhang Hongmei Zhang Jialiang Zhang Jiawen Zhang Jie Zhang Jin Zhang Jingbo Zhang Jinnan Zhang Junwei Zhang Kun Zhang Lei Zhang Mingxuan Zhang Mohan Zhang Peng Zhang Ping Zhang Qingmin Zhang Rongping Zhang Rui Zhang Shaoping Zhang Shiqi Zhang Shu Zhang Shuihan Zhang Siyuan Zhang Tao Zhang Xiaofeng Zhang Xiaomei Zhang Xin Zhang Xu Zhang Xuan Zhang Xuantong Zhang Xuesong Zhang Xueyao Zhang Yan Zhang Yibing Zhang Yinhong Zhang Yiyu Zhang Yizhou Zhang Yongjie Zhang Yongpeng Zhang Yu Zhang Yuanyuan Zhang Yue Zhang Yueyuan Zhang Yumei Zhang Yuning Zhang Zhenyu Zhang Zhicheng Zhang Zhijian Zhang Zhixuan Zhang Baoqi Zhao Fengyi Zhao Jie Zhao Liang Zhao Mei Zhao Rong Zhao Runze Zhao Shujun Zhao Tianchi Zhao Tianhao Zhao Yubin Zhao Dongqin Zheng Hua Zheng Xiangyu Zheng Yangheng Zheng Weili Zhong Weirong Zhong Albert Zhou Guorong Zhou Li Zhou Lishui Zhou Min Zhou Shun Zhou Tong Zhou Xiang Zhou Xing Zhou Yan Zhou Haiwen Zhu Jiang Zhu Jingsen Zhu Jingyu Zhu Kangfu Zhu Kejun Zhu Zhihang Zhu Ivan Zhutikov Bo Zhuang Honglin Zhuang Liang Zong Jiaheng Zou Sebastian Zwickel Jan Züfle JUNO Collaboration 《Chinese Physics C》 2026年第4期1-31,共31页
The Jiangmen Underground Neutrino Observatory(JUNO)started physics data taking on 26 August 2025.JUNO consists of a 20-kton liquid scintillator central detector,surrounded by a 35 kton water pool serving as a Cherenko... The Jiangmen Underground Neutrino Observatory(JUNO)started physics data taking on 26 August 2025.JUNO consists of a 20-kton liquid scintillator central detector,surrounded by a 35 kton water pool serving as a Cherenkov veto,and almost 1000 m^(2) of plastic scintillator veto on top.The detector is located in a shallow underground laboratory with an overburden of 1800 m.w.e.This paper presents the performance results of the detector,extensively studied during the commissioning of the water phase,the subsequent liquid scintillator filling phase,and the first physics runs.The liquid scintillator achieved an attenuation length of 20.6 m at 430 nm,while the high coverage PMT system and scintillator together yielded about 1785 photoelectrons per MeV of energy deposit at the detector centre,measured using the 2.223 MeVγfrom neutron captures on hydrogen with an Am-C calibration source.The reconstructed energy resolution is 3.4%for two 0.511 MeVγat the detector centre and 2.9%for the 0.93 MeV quenched ^(214)Po alpha decays from natural radioactive sources.The energy non-linearity is calibrated to better than 1%.Intrinsic contaminations of ^(238)U and ^(232)Th in the liquid scintillator are below 10^(-16) g/g,assuming secular equilibrium.The water Cherenkov detector achieves a muon detection efficiency better than 99.9%for muons traversing the liquid scintillator volume.During the initial science runs,the data acquisition duty cycle exceeded 97.8%,demonstrating the excellent stability and readiness of JUNO for high-precision neutrino physics. 展开更多
关键词 neutrino oscillations JUNO detector performance
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Solution Due to Sinc Methods of Numerical Analysis:Three Type Sterile Neutrinos and the Longitudinal Massless with Flavor Changing of Missing Transverse Masses
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作者 Hung-Te Henry Su Po-Han Lee 《Journal of Applied Mathematics and Physics》 2025年第7期2418-2440,共23页
The Daya Bay Collaboration has discovered that approximately 6.0%of active neutrinos were missing from the nuclear reaction container.This finding has led to a reinterpretation of the three known types of neutrinos.In... The Daya Bay Collaboration has discovered that approximately 6.0%of active neutrinos were missing from the nuclear reaction container.This finding has led to a reinterpretation of the three known types of neutrinos.In this paper,we present an analysis based on deductive reasoning,proposing that neutrinos are massless in the longitudinal direction(referred to as“longitudinal mass-less”).This insight contributes to the broader body of literature on the subject.Additionally,our work resolves the long-standing mystery of CP conservation in strong interactions.Using advanced physical mathematics,we derive a sig-nificant result:the transformation between the third type of neutrino and pho-tons or gravitons.We express the probability of this transformation in quan-tum mechanics using sinc functions which arise from interference effects,providing analytical solutions.Furthermore,considering the mass constraints imposed by the seesaw mechanism—referred to here as the“compete mecha-nism”(a generalized seesaw model)—we argue that the actual phase 4π of CP violation precisely answers the fundamental question at hand. 展开更多
关键词 Daya Bay Collaboration Neutrino Types Longitudinal Massless CP Conservation Strong Interactions CP Violation
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Sub-Atom Particles and Magnetic Monopoles Spin Ice Condensed in Higgs-Field Portals
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作者 Hung-Te Henry Su Po-Han Lee 《Journal of Applied Mathematics and Physics》 2025年第1期348-364,共17页
The study of magnetic monopoles continues to be a prominent and captivating topic in physics, particularly within the realm of physical materials. Recently, K. C. Tan, Hariom Jani, Michael Högen, and their collab... The study of magnetic monopoles continues to be a prominent and captivating topic in physics, particularly within the realm of physical materials. Recently, K. C. Tan, Hariom Jani, Michael Högen, and their collaborators (2023) reported groundbreaking discoveries, marking significant progress in this field. However, a sense of dissatisfaction persists among researchers regarding the current state of advancement. To address this, we propose a novel theoretical framework that explores magnetic monopoles through the lens of Higgs field portals. Our findings indicate that the spin of the magnetic monopole, s = 1, is intrinsically linked to the fundamental expression governing its behavior, with the two aspects being inseparable in practical terms. This theory offers a deeper understanding of the inherent nature of magnetic monopoles and provides a foundation for further exploration. 展开更多
关键词 Magnetic Monopoles Higgs-Field Magnetic Spin
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Detection and upconversion of three-dimensional MMW/THz images to the visible 被引量:3
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作者 Avihai Aharon(Akram) Daniel Rozban +3 位作者 Avi Klein Amir Abramovich Yitzhak Yitzhaky Natan S.Kopeika 《Photonics Research》 SCIE EI 2016年第6期306-312,共7页
We present an inexpensive technique to obtain a three-dimensional(3D) millimeter wave(MMW) and terahertz(THz) image using upconversion. In this work we describe and demonstrate a method for upconversion of MMW/THz rad... We present an inexpensive technique to obtain a three-dimensional(3D) millimeter wave(MMW) and terahertz(THz) image using upconversion. In this work we describe and demonstrate a method for upconversion of MMW/THz radiation to the visual band using a very inexpensive miniature glow discharge detector(GDD) and a silicon photodetector. We present MMW/THz upconversion images based on measuring the visual light emitting from the GDD rather than its electrical current. The results show better response time and better sensitivity compared to the electronic detection performed previously. Furthermore, in this work we perform frequency modulation continuous wave(FMCW) radar detection based on this method using a GDD lamp, with a photodetector to measure GDD light emission. By using FMCW detection, the range in addition to the intensity at each pixel can be obtained,thus yielding the 3D image. The GDD acts as a heterodyne mixer not only electronically but also optically. The suggested 3D upconversion technique using the GDD is simple and inexpensive and has better performance compared to other MMW/THz imaging systems suggested in the literature. This method provides minimum detectable signal power that is about 6 orders of magnitude better than similar plasma systems due to the very large internal signal gain deriving from the much smaller electrode separation and resulting in much higher plasma electric field. 展开更多
关键词 THZ Detection and upconversion of three-dimensional MMW/THz images to the visible FMCW
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