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High-speed GeSn resonance cavity enhanced photodetectors for a 50 Gbps Si-based 2 μm band communication system 被引量:2
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作者 JINLAI CUI JUN ZHENG +8 位作者 YUPENG ZHU XIANGQUAN LIU yiyang wu QINXING HUANG YAZHOU YANG ZHIPENG LIU ZHI LIU YUHUA ZUO BUWEN CHENG 《Photonics Research》 SCIE EI CAS CSCD 2024年第4期767-773,共7页
Expanding the optical communication band is one of the most effective methods of overcoming the nonlinear Shannon capacity limit of single fiber.In this study,GeSn resonance cavity enhanced(RCE)photodetectors(PDs)with... Expanding the optical communication band is one of the most effective methods of overcoming the nonlinear Shannon capacity limit of single fiber.In this study,GeSn resonance cavity enhanced(RCE)photodetectors(PDs)with an active layer Sn component of 9%–10.8%were designed and fabricated on an SOI substrate.The GeSn RCE PDs present a responsivity of 0.49 A/W at 2μm and a 3-dB bandwidth of approximately 40 GHz at 2μm.Consequently,Si-based 2μm band optical communication with a transmission rate of 50 Gbps was demonstrated by using a GeSn RCE detector.This work demonstrates the considerable potential of the Si-based 2μm band photonics in future high-speed and high-capacity optical communication. 展开更多
关键词 RESONANCE system APPROXIMATE
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Prediction of energy resolution in the JUNO experiment
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作者 Angel Abusleme Thomas Adam +651 位作者 Kai Adamowicz Shakeel Ahmad Rizwan Ahmed Sebastiano Aiello Fengpeng An Qi An Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Joao Pedro Athayde Marcondes de André Didier Auguste Weidong Bai Nikita Balashov Wander Baldini Andrea Barresi Davide Basilico Eric Baussan Marco Bellato Marco Beretta Antonio Bergnoli Daniel Bick Lukas Bieger Svetlana Biktemerova Thilo Birkenfeld Iwan Blake David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Jose Busto Anatael Cabrera Barbara Caccianiga Hao Cai Xiao Cai Yanke Cai Zhiyan Cai Stéphane Callier Steven Calvez Antonio Cammi Agustin Campeny Chuanya Cao Guofu Cao Jun Cao Rossella Caruso Cédric Cerna Vanessa Cerrone Jinfan Chang Yun Chang Auttakit Chatrabhuti Chao Chen Guoming Chen Pingping Chen Shaomin Chen Xin Chen Yiming Chen Yixue Chen Yu Chen Zelin Chen Zhangming Chen Zhiyuan Chen Zikang Chen Jie Cheng Yaping Cheng YuChin Cheng Alexander Chepurnov Alexey Chetverikov Davide Chiesa Pietro Chimenti Yen-Ting Chin Po-Lin Chou Ziliang Chu Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Marta Colomer Molla Selma Conforti Di Lorenzo Alberto Coppi Daniele Corti Simon Csakli Chenyang Cui Flavio Dal Corso Olivia Dalager Jaydeep Datta Christophe De La Taille Zhi Deng Ziyan Deng Xiaoyu Ding Xuefeng Ding Yayun Ding Bayu Dirgantara Carsten Dittrich Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko Jianmeng Dong Evgeny Doroshkevich Wei Dou Marcos Dracos Frédéric Druillole Ran Du Shuxian Du Katherine Dugas Stefano Dusini Hongyue Duyang Jessica Eck Timo Enqvist Andrea Fabbri Ulrike Fahrendholz Lei Fan Jian Fang Wenxing Fang Dmitry Fedoseev Li-Cheng Feng Qichun Feng Federico Ferraro Amélie Fournier Fritsch Fritsch Haonan Gan Feng Gao Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Nunzio Giudice Maxim Gonchar Guanghua Gong Hui Gong Yuri Gornushkin Marco Grassi Maxim Gromov Vasily Gromov Minghao Gu Xiaofei Gu Yu Gu Mengyun Guan Yuduo Guan Nunzio Guardone Rosa Maria Guizzetti Cong Guo Wanlei Guo Caren Hagner Hechong Han Ran Han Yang Han Miao He Wei He Xinhai He Tobias Heinz Patrick Hellmuth Yuekun Heng Rafael Herrera YuenKeung Hor Shaojing Hou Yee Hsiung Bei-Zhen Hu Hang Hu Jun Hu Peng Hu Shouyang Hu Tao Hu Yuxiang Hu Zhuojun Hu Guihong Huang Hanxiong Huang Jinhao Huang Junting Huang Kaixuan Huang Shengheng Huang Wenhao Huang Xin Huang Xingtao Huang Yongbo Huang Jiaqi Hui Lei Huo Wenju Huo Cédric Huss Safeer Hussain Leonard Imbert Ara Ioannisian Roberto Isocrate Arshak Jafar Beatrice Jelmini Ignacio Jeria Xiaolu Ji Huihui Jia Junji Jia Siyu Jian Cailian Jiang Di Jiang Wei Jiang Xiaoshan Jiang Xiaozhao Jiang Yixuan Jiang Xiaoping Jing Cécile Jollet Li Kang Rebin Karaparabil Narine Kazarian Ali Khan Amina Khatun Khanchai Khosonthongkee Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Sergey Kuleshov Sindhujha Kumaran Nikolay Kutovskiy Loic Labit Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Frederic Lefevre Ruiting Lei Rupert Leitner Jason Leung Demin Li Fei Li Fule Li Gaosong Li Hongjian Li Jiajun Li Min Li Nan Li Qingjiang Li Ruhui Li Rui Li Shanfeng Li Shuo Li Tao Li Teng Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xinglong Li Yi Li Yichen Li Yufeng Li Zhaohan Li Zhibing Li Ziyuan Li Zonghai Li Hao Liang Hao Liang Jiajun Liao Yilin Liao Yuzhong Liao Ayut Limphirat Guey-Lin Lin Shengxin Lin Tao Lin Jiajie Ling Xin Ling Ivano Lippi Caimei Liu Fang Liu Fengcheng Liu Haidong Liu Haotian Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hongyang Liu Jianglai Liu Jiaxi Liu Jinchang Liu Min Liu Qian Liu Qin Liu Runxuan Liu Shenghui Liu Shubin Liu Shulin Liu Xiaowei Liu Xiwen Liu Xuewei Liu Yankai Liu Zhen Liu Lorenzo Loi Alexey Lokhov Paolo Lombardi Claudio Lombardo Kai Loo Chuan Lu Haoqi Lu Jingbin Lu Junguang Lu Meishu Lu Peizhi Lu Shuxiang Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov Fengjiao Luo Guang Luo Jianyi Luo Shu Luo wuming Luo Xiaojie Luo Vladimir Lyashuk Bangzheng Ma Bing Ma Qiumei Ma Si Ma Xiaoyan Ma Xubo Ma Jihane Maalmi Jingyu Mai Marco Malabarba Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Xin Mao Yajun Mao Stefano M.Mari Filippo Marini Agnese Martini Matthias Mayer Davit Mayilyan Ints Mednieks Yue Meng Anita Meraviglia Anselmo Meregaglia Emanuela Meroni Lino Miramonti Nikhil Mohan Michele Montuschi Axel Müller Massimiliano Nastasi Dmitry V.Naumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Minh Thuan Nguyen Thi Alexey Nikolaev Feipeng Ning Zhe Ning Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Alexander Olshevskiy Domizia Orestano Fausto Ortica Rainer Othegraven Alessandro Paoloni George Parker Sergio Parmeggiano Achilleas Patsias Yatian Pei Luca Pelicci Anguo Peng Haiping Peng Yu Peng Zhaoyuan Peng Elisa Percalli Willy Perrin Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Oliver Pilarczyk Luis Felipe Pineres Rico Artyom Popov Pascal PoussotE zio Previtali Fazhi Qi Ming Qi Xiaohui Qi Sen Qian Xiaohui Qian Zhen Qian Hao Qiao Zhonghua Qin Shoukang Qiu Manhao Qu Zhenning Qu Gioacchino Ranucci Reem Rasheed Alessandra Re Abdel Rebii Mariia Redchuk Gioele Reina Bin Ren Jie Ren Yuhan Ren Barbara Ricci Komkrit Rientong Mariam Rifai Mathieu Roche Narongkiat Rodphai Aldo Romani Bedrich Roskovec Xichao Ruan Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Deshan Sandanayake Anut Sangka Giuseppe Sava Utane Sawangwit Michaela Schever Cédric Schwab Konstantin Schweizer Alexandr Selyunin Andrea Serafini Mariangela Settimo Junyu Shao Vladislav Sharov Hexi Shi Jingyan Shi Yanan Shi Vitaly Shutov Andrey Sidorenkov Fedor Simkovic Apeksha Singhal Chiara Sirignano Jaruchit Siripak Monica Sisti Mikhail Smirnov Oleg Smirnov Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Michail Strizh Alexander Studenikin Aoqi SuJun Su Jun Su Shifeng Sun Xilei Sun Yongjie Sun Yongzhao Sun Zhengyang Sun Narumon Suwonjandee Akira Takenaka Xiaohan Tan Jian Tang Jingzhe Tang Qiang Tang Quan Tang Xiao Tang Vidhya Thara Hariharan Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Andrea Triossi Riccardo Triozzi Wladyslaw Trzaska Yu-Chen Tung Cristina Tuve Nikita Ushakov Vadim Vedin Carlo Venettacci Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Katharina von Sturm Vit Vorobel Dmitriy Voronin Lucia Votano Pablo Walker Caishen Wang Chung-Hsiang Wang En Wang Guoli Wang Jian Wang Jun Wang Li Wang Lu Wang Meng Wang Meng Wang Mingyuan Wang Ruiguang Wang Sibo Wang Siguang Wang Wei Wang Wenshuai Wang Xi Wang Xiangyue Wang Yangfu Wang Yaoguang Wang Yi Wang Yi Wang Yifang Wang Yuanqing Wang Yuyi Wang Zhe Wang Zheng Wang Zhimin Wang Apimook Watcharangkool Wei Wei Wei Wei Wenlu Wei Yadong Wei Yuehuan Wei Kaile Wen Liangjian Wen Jun Weng Christopher Wiebusch Rosmarie Wirth Chengxin wu Diru wu Qun wu Yinhui wu yiyang wu Zhi wu Michael wurm Jacques wurtz Christian Wysotzki Yufei Xi Dongmei Xia Shishen Xian Fei Xiao Xiang Xiao Xiaochuan Xie Yijun Xie Yuguang Xie Zhao Xin Zhizhong Xing Benda Xu Cheng Xu Donglian Xu Fanrong Xu Hangkun Xu Jiayang Xu Jilei Xu Jing Xu Jinghuan Xu Meihang Xu Xunjie Xu Yin Xu Yu Xu Baojun Yan Qiyu Yan Taylor Yan Xiongbo Yan Yupeng Yan Changgen Yang Chengfeng Yang Fengfan Yang Jie Yang Lei Yang Pengfei Yang Xiaoyu Yang Yifan Yang Yixiang Yang Zekun Yang Haifeng Yao Jiaxuan Ye Mei Ye Ziping Ye Frédéric Yermia Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Guojun Yu Hongzhao Yu Miao Yu Xianghui Yu Zeyuan Yu Zezhong Yu Cenxi Yuan Chengzhuo Yuan Ying Yuan Zhenxiong Yuan Baobiao Yue Noman Zafar Kirill Zamogilnyi Vitalii Zavadskyi Fanrui Zeng Shan Zeng Tingxuan Zeng Yuda Zeng Liang Zhan Yonghua Zhan Aiqiang Zhang Bin Zhang Binting Zhang Feiyang Zhang Hangchang Zhang Haosen Zhang Honghao Zhang Jialiang Zhang Jiawen Zhang Jie Zhang Jingbo Zhang Jinnan Zhang Junwei Zhang Lei Zhang Peng Zhang Ping Zhang Qingmin Zhang Shiqi Zhang Shu Zhang Shuihan Zhang Siyuan Zhang Tao Zhang Xiaomei Zhang Xin Zhang Xuantong Zhang Yinhong Zhang Yiyu Zhang Yongpeng Zhang Yu Zhang Yuanyuan Zhang Yumei Zhang Zhenyu Zhang Zhijian Zhang Jie Zhao Rong Zhao Runze Zhao Shujun Zhao Tianhao Zhao Hua Zheng Yangheng Zheng Jing Zhou Li Zhou Nan Zhou Shun Zhou Tong Zhou Xiang Zhou Jingsen Zhu Kangfu Zhu Kejun Zhu Zhihang Zhu Bo Zhuang Honglin Zhuang Liang Zong Jiaheng Zou Jan Züfle The JUNO Collaboration 《Chinese Physics C》 2025年第1期35-59,共25页
This paper presents an energy resolution study of the JUNO experiment,incorporating the latest knowledge acquired during the detector construction phase.The determination of neutrino mass ordering in JUNO requires an ... This paper presents an energy resolution study of the JUNO experiment,incorporating the latest knowledge acquired during the detector construction phase.The determination of neutrino mass ordering in JUNO requires an exceptional energy resolution better than 3% at 1 MeV.To achieve this ambitious goal,significant efforts have been undertaken in the design and production of the key components of the JUNO detector.Various factors affecting the detection of inverse beta decay signals have an impact on the energy resolution,extending beyond the statistical fluctuations of the detected number of photons,such as the properties of the liquid scintillator,performance of photomultiplier tubes,and the energy reconstruction algorithm.To account for these effects,a full JUNO simulation and reconstruction approach is employed.This enables the modeling of all relevant effects and the evaluation of associated inputs to accurately estimate the energy resolution.The results of this study reveal an energy resolution of 2.95% at 1 Mev.Furthermore,this study assesses the contribution of major effects to the overall energy resolution budget.This analysis serves as a reference for interpreting future measurements of energy resolution during JUNO data collection.Moreover,it provides a guideline for comprehending the energy resolution characteristics of liquid scintillator-based detectors. 展开更多
关键词 energy resolution liquid scintillator detector JUNO simulation reconstruction
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Mechanosensitive Ion Channel TMEM63A Gangs Up with Local Macrophages to Modulate Chronic Post-amputation Pain 被引量:2
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作者 Shaofeng Pu yiyang wu +9 位作者 Fang Tong Wan-Jie Du Shuai Liu Huan Yang Chen Zhang Bin Zhou Ziyue Chen Xiaomeng Zhou Qingjian Han Dongping Du 《Neuroscience Bulletin》 SCIE CAS CSCD 2023年第2期177-193,共17页
Post-amputation pain causes great sufering to amputees,but still no efective drugs are available due to its elusive mechanisms.Our previous clinical studies found that surgical removal or radiofrequency treatment of t... Post-amputation pain causes great sufering to amputees,but still no efective drugs are available due to its elusive mechanisms.Our previous clinical studies found that surgical removal or radiofrequency treatment of the neuroma at the axotomized nerve stump efectively relieves the phantom pain aficting patients after amputation.This indicated an essential role of the residual nerve stump in the formation of chronic post-amputation pain(CPAP).However,the molecular mechanism by which the residual nerve stump or neuroma is involved and regulates CPAP is still a mystery.In this study,we found that nociceptors expressed the mechanosensitive ion channel TMEM63A and macrophages infltrated into the dorsal root ganglion(DRG)neurons worked synergistically to promote CPAP.Histology and qRT-PCR showed that TMEM63A was mainly expressed in mechanical pain-producing non-peptidergic nociceptors in the DRG,and the expression of TMEM63A increased signifcantly both in the neuroma from amputated patients and the DRG in a mouse model of tibial nerve transfer(TNT).Behavioral tests showed that the mechanical,heat,and cold sensitivity were not afected in the Tmem63a-/-mice in the naïve state,suggesting the basal pain was not afected.In the infammatory and post-amputation state,the mechanical allodynia but not the heat hyperalgesia or cold allodynia was signifcantly decreased in Tmem63a-/-mice.Further study showed that there was severe neuronal injury and macrophage infltration in the DRG,tibial nerve,residual stump,and the neuromalike structure of the TNT mouse model,Consistent with this,expression of the pro-infammatory cytokines TNFα,IL-6,and IL-1βall increased dramatically in the DRG.Interestingly,the deletion of Tmem63a signifcantly reduced the macrophage infltration in the DRG but not in the tibial nerve stump.Furthermore,the ablation of macrophages signifcantly reduced both the expression of Tmem63a and the mechanical allodynia in the TNT mouse model,indicating an interaction between nociceptors and macrophages,and that these two factors gang up together to regulate the formation of CPAP.This provides a new insight into the mechanisms underlying CPAP and potential drug targets its treatment. 展开更多
关键词 Mechanosensitive ion channel TMEM63A Post-amputation pain Tibial nerve transfer MACROPHAGE
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Measurement of muon-induced neutron yield at the China Jinping Underground Laboratory
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作者 Lin Zhao Wentai Luo +24 位作者 Lars Bathe-Peters Shaomin Chen Mourad Chouaki Wei Dou Lei Guo Ziyi Guo Ghulam Hussain Jinjing Li Ye Liang Qian Liu Guang Luo Ming Qi Wenhui Shao Jian Tang Linyan Wan Zhe Wang yiyang wu Benda Xu Tong Xu Weiran Xu Yuzi Yang Minfang Yeh Aiqiang Zhang Bin Zhang JNE collaboration 《Chinese Physics C》 SCIE CAS CSCD 2022年第8期211-219,共9页
Solar,terrestrial,and supernova neutrino experiments are subject to muon-induced radioactive background.The China Jinping Underground Laboratory(CJPL),with its unique advantage of a 2400 m rock coverage and long dista... Solar,terrestrial,and supernova neutrino experiments are subject to muon-induced radioactive background.The China Jinping Underground Laboratory(CJPL),with its unique advantage of a 2400 m rock coverage and long distance from nuclear power plants,is ideal for MeV-scale neutrino experiments.Using a 1-ton prototype detector of the Jinping Neutrino Experiment(JNE),we detected 3 43 high-energy cosmic-ray muons and(7.86±3.97)muon-induced neutrons from an 820.28-day dataset at the first phase of CJPL(CJPL-I).Based on the muon-induced neutrons,we measured the corresponding muon-induced neutron yield in a liquid scintillator to be(3.44±1.86_(stat.)±0.76_(syst.))×10^(-4) μ^(-1)g^(-1)cm^(2) at an average muon energy of 340 GeV.We provided the first study for such neutron background at CJPL.A global fit including this measurement shows a power-law coefficient of(0.75±0.02) for the dependence of the neutron yield at the liquid scintillator on muon energy. 展开更多
关键词 Underground laboratory neutrino detector cosmic-ray muon neutron yield liquid scintillator
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