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普惠性学前教育公共服务监测模型与指标的构建——基于“以人民为中心”的视角 被引量:5
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作者 王艺芳 姜勇 《学前教育研究》 CSSCI 北大核心 2021年第7期41-57,共17页
在当前我国大力发展普惠性学前教育的时期,建立基于"以人民为中心"视角、以服务功能为导向的普惠性学前教育公共服务监测模型和指标具有十分重要的意义。依据监测理论模型,本研究从投入层面的服务充分性、分配层面的服务均衡... 在当前我国大力发展普惠性学前教育的时期,建立基于"以人民为中心"视角、以服务功能为导向的普惠性学前教育公共服务监测模型和指标具有十分重要的意义。依据监测理论模型,本研究从投入层面的服务充分性、分配层面的服务均衡性、产出层面的服务公益性、结果层面的服务满意度四个方面,编制了普惠性学前教育公共服务监测指标,并通过三轮德尔菲专家访谈对指标进行了修订。同时,本研究采用两阶段分层整群抽样方法,选取5224名教育行政人员、幼儿园教师、家长为调查对象,利用经典测量理论和项目反应理论的项目分析、探索性因素分析、验证性因素分析、等级反应模型对监测量表进行了修订,最终获得包含4个一级维度、11个二级维度、47个三级指标的普惠性学前教育公共服务监测指标体系,以期能够为新时代普惠性学前教育公共服务监测工作的开展提供科学工具。 展开更多
关键词 普惠性学前教育 公共服务 教育监测
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Stereotactic surgery for refractory epilepsy complicated by mental disorders A retrospective case analysis 被引量:2
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作者 yifang wang Aigang Xu +4 位作者 Qifu Tan Zhengwei wang Dongsheng Jiao Hao Zhu KaidongLiu 《Neural Regeneration Research》 SCIE CAS CSCD 2008年第6期690-693,共4页
BACKGROUND: Anti-epilepsy and anti-psychosis drugs have traditionally been used in the clinic to treat epilepsy complicated by mental disorders. However, there is still no effective therapy for refractory epilepsy pa... BACKGROUND: Anti-epilepsy and anti-psychosis drugs have traditionally been used in the clinic to treat epilepsy complicated by mental disorders. However, there is still no effective therapy for refractory epilepsy patients suffering from persistent mental disorders. OBJECTIVE: To explore the therapeutic effects of stereotactic multi-element localization and multi-target radiofrequency ablation on patients with refractory primary epilepsy and mental disorders. DESIGN: A retrospective case analysis. SETTING: Department of Neurosurgery, the 454 Hospital of Chinese PLA. PARTICIPANTS: Between June and November 2004, 13 patients with refractory primary epilepsy complicated by persistent mental disorders were admitted to the Department of Neurosurgery, the 454 Hospital of Chinese PLA. The patient group consisted of nine males and four females, with an average age of 25 years (range 18-39 years), and a course of disease ranging 3-11 years. Diagnosis of mental disorders was in accordance with Chinese Classification of Mental Disorders. Written informed consent was obtained from all patients and their families, and the treatment protocol was approved by the Ethics Committee of the Hospital. METHODS: Under venous inhalation anesthesia, the disease targets, including bilateral corpus callosum, bilateral amygdala, and bilateral medial septal area, as well as unilateral Forel-H area, were coagulated by RFG-3CF radiofrequency thermocoagnlation at 75-80 ℃ for 60-70 seconds. During thermocoagulation, the targets were identified using deep-brain microelectrodes and localized according to electrophysiology and electric resistance values. MAIN OUTCOME MEASURES: One year post-surgery, epileptic seizures were assessed on the basis of the Tan classification, and psychogenic (non-epileptic) seizures were evaluated using a 5-grade system. RESULTS: All enrolled 13 epileptic patients were included in the final analysis. The results of follow-up evaluations demonstrated that epilepsy was well-controlled. In total, nine patients did not experience relapse, and the frequency of seizures was reduced by 75% in two patients, and 50%-74% in another two patients. Psychogenic seizures were ameliorated in 11 cases (class 1, recovery) and improved significantly in two cases (class 2, significant improvement). CONCLUSION: Radiofrequency ablation of bilateral corpus callosum, bilateral amygdala, bilateral medial septal area, and unilateral Forel-H area exhibits certain efficacy in treating epileptic patients suffering from persistent mental disorders. 展开更多
关键词 EPILEPSY metal disorders retrospective studies
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Paeoniflorin inhibits lipopolysaccharide-induced inflammation in LO2 cells by regulating RhoA/NLRP3 pathway
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作者 Haixia Liu Fafeng Cheng +3 位作者 Feifei Tang yifang wang Shuling Liu Xueqian wang 《Journal of Traditional Chinese Medical Sciences》 2021年第2期161-165,共5页
Background:Inflammation is an essential component of liver diseases.Paeoniflorin(PF),a monoterpenoid component derived from peony root(Paeonia lactiflora Pall.),has anti-inflammatory,immunoregulatory,and hepatoprotect... Background:Inflammation is an essential component of liver diseases.Paeoniflorin(PF),a monoterpenoid component derived from peony root(Paeonia lactiflora Pall.),has anti-inflammatory,immunoregulatory,and hepatoprotective activities.However,whether PF affects liver inflammation and its underlying mechanisms is unclear.In this study,we investigated the effects of PF on lipopolysaccharide(LPS)-induced inflammation in LO2 cells and the underlying molecular mechanism.Methods:LPS was used to induce inflammation.After PF pretreatment for 2 h,the cells were treated with PF and LPS.Cell counting kit-8 was used to measure cell viability.Tumor necrosis factor-a(TNF-a)and interleukin(IL)-6 were tested by Enzyme-linked immunosorbent assay.Western blot was used to evaluate TNF-a,Ras homolog family member A(RhoA),NOD-,LRR-and pyrin domain-containing protein 3(NLRP3),apoptosis-associated speck-like protein containing a CARD(ASC),caspase-1,and IL-1b proteins expression.Results:In LPS-induced LO2 cells,PF reduced TNF-a and IL-6 inflammatory cytokine production in a dose-dependent manner.LPS-induced TNF-a expression was also suppressed by PF.In addition,PF significantly inhibited LPS-induced RhoA activation(P=.0014).Finally,PF suppressed LPS-induced NLRP3 inflammasome activation by downregulating NLRP3,ASC,caspase-1,and IL-1b expression.Conclusion:These findings suggest that PF alleviates inflammation induced by LPS and further suggest the anti-inflammatory effect of PF may follow via reduced RhoA and NLRP3 inflammasome activity. 展开更多
关键词 PAEONIFLORIN LIPOPOLYSACCHARIDE INFLAMMATION RHOA NLRP3 inflammasome
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CEPC Technical Design Report 被引量:1
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作者 Waleed Abdallah Tiago Carlos Adorno de Freitas +1111 位作者 Konstantin Afanaciev Shakeel Ahmad Ijaz Ahmed Xiaocong Ai Abid Aleem Wolfgang Altmannshofer Fabio Alves Weiming An Rui An Daniele Paolo Anderle Stefan Antusch Yasuo Arai Andrej Arbuzov Abdesslam Arhrib Mustafa Ashry Sha Bai Yu Bai Yang Bai Vipul Bairathi Csaba Balazs Philip Bambade Yong Ban Tripamo Bandyopadhyay Shou-Shan Bao Desmond P.Barber Ayse Bat Varvara Batozskaya Subash Chandra Behera Alexander Belyaev Michele Bertucci Xiao-Jun Bi Yuanjie Bi Tianjian Bian Fabrizio Bianchi Thomas Biekotter Michela Biglietti Shalva Bilanishvili Deng Binglin Denis Bodrov Anton Bogomyagkov Serge Bondarenko Stewart Boogert Maarten Boonekamp Marcello Borri Angelo Bosotti Vincent Boudry Mohammed Boukidi Igor Boyko Ivanka Bozovic Giuseppe Bozzi Jean-Claude Brient Anastasiia Budzinskaya Masroor Bukhari Vladimir Bytev Giacomo Cacciapaglia Hua Cai Wenyong Cai Wujun Cai Yijian Cai Yizhou Cai Yuchen Cai Haiying Cai Huacheng Cai Lorenzo Calibbi Junsong Cang Guofu Cao Jianshe Cao Antoine Chance Xuejun Chang Yue Chang Zhe Chang Xinyuan Chang Wei Chao Auttakit Chatrabhuti Yimin Che Yuzhi Che Bin Chen Danping Chen Fuqing Chen Fusan Chen Gang Chen Guoming Chen Hua-Xing Chen Huirun Chen Jinhui Chen Ji-Yuan Chen Kai Chen Mali Chen Mingjun Chen Mingshui Chen Ning Chen Shanhong Chen Shanzhen Chen Shao-Long Chen Shaomin Chen Shiqiang Chen Tianlu Chen Wei Chen Xiang Chen Xiaoyu Chen Xin Chen Xun Chen Xurong Chen Ye Chen Ying Chen Yukai Chen Zelin Chen Zilin Chen Gang Chen Boping Chen Chunhui Chen Hok Chuen Cheng Huajie Cheng Shan Cheng Tongguang Cheng Yunlong Chi Pietro Chimenti Wen Han Chiu Guk Cho Ming-Chung Chu Xiaotong Chu Ziliang Chu Guglielmo Coloretti Andreas Crivellin Hanhua Cui Xiaohao Cui Zhaoyuan Cui Brunella D'Anzi Ling-Yun Dai Xinchen Dai Xuwen Dai Antonio De Maria Nicola De Filippis Christophe De La Taille Francesca De Mori Chiara De Sio Elisa Del Core Shuangxue Deng Wei-Tian Deng Zhi Deng Ziyan Deng Bhupal Dev Tang Dewen 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Ching Leung Hai Tao Li Bingzhi Li Bo Li Bo Li Changhong Li Chao Li Cheng Li Cheng Li Chunhua Li Cui Li Dazhang Li Dikai Li Fei Li Gang Li Gang Li Gang Li Gaosong Li Haibo Li Haifeng Li Hai-Jun Li Haotian Li Hengne Li Honglei Li Huijing Li Jialin Li Jingyi Li Jinmian Li Jun Li Leyi Li Liang Li Ling Li Mei Li Meng Li Minxian Li Pei-Rong Li Qiang Li Shaopeng Li Shenghe Li Shu Li Shuo Li Teng Li Tiange Li Tong Li Weichang Li Weidong Li Wenjun Li Xiaoling Li Xiaomei Li Xiaonan Li Xiaoping Li Xiaoting Li Xin Li Xinqiang Li Xuekang Li Yang Li Yanwei Li Yiming Li Ying Li Ying-Ying Li Yonggang Li Yonglin Li Yufeng Li Yuhui Li Zhan Li Zhao Li Zhiji Li Tong Li Lingfeng Li Fei Li Jing Liang Jinhan Liang Zhijun Liang Guangrui Liao Hean Liao Jiajun Liao Libo Liao Longzhou Liao Yi Liao Yipu Liao Ayut Limphirat AyutLimphirat Tao Lin Weiping Lin Yufu Lin Yugen Lin Beijiang Liu Bo Liu Danning Liu Dong Liu Fu-Hu Liu Hongbang Liu Huangcheng Liu Hui Liu Huiling Liu Jia Liu Jia Liu Jiaming Liu Jianbei Liu 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Hao Zeng Ming Zeng Jian Zhai Jiyuan Zhai Xin Zhe Zhai Xi-Jie Zhan Ben-Wei Zhang Bolun Zhang Di Zhang Guangyi Zhang Hao Zhang Hong-Hao Zhang Huaqiao Zhang Hui Zhang Jialiang Zhang Jianyu Zhang Jianzhong Zhang Jiehao Zhang Jielei Zhang Jingru Zhang Jinxian Zhang Junsong Zhang Junxing Zhang Lei Zhang Lei Zhang Liang Zhang Licheng Zhang Liming Zhang Linhao Zhang Luyan Zhang Mengchao Zhang Rao Zhang Shulei Zhang Wan Zhang Wenchao Zhang Xiangzhen Zhang Xiaomei Zhang Xiaoming Zhang Xiaoxu Zhang Xiaoyu Zhang Xuantong Zhang Xueyao Zhang Yang Zhang Yang Zhang Yanxi Zhang Yao Zhang Ying Zhang Yixiang Zhang Yizhou Zhang Yongchao Zhang Yu Zhang Yuan Zhang Yujie Zhang Yulei Zhang Yumei Zhang Yunlong Zhang Zhandong Zhang Zhaoru Zhang Zhen-Hua Zhang Zhenyu Zhang Zhichao Zhang Zhi-Qing Zhang Zhuo Zhang Zhiqing Zhang Cong Zhang Tianliang Zhang Luyan Zhang Guang Zhao Hongyun Zhao Jie Zhao Jingxia Zhao Jingyi Zhao Ling Zhao Luyang Zhao Mei Zhao Minggang Zhao Mingrui Zhao Qiang Zhao Ruiguang Zhao Tongxian Zhao Yaliang Zhao Ying Zhao Yue Zhao Zhiyu Zhao Zhuo Zhao Alexey Zhemchugov Hongjuan Zheng Jinchao Zheng Liang Zheng Ran Zheng shanxi zheng Xu-Chang Zheng wang Zhile Weicai Zhong Yi-Ming Zhong Chen Zhou Daicui Zhou Jianxin Zhou Jing Zhou Jing Zhou Ning Zhou Qi-Dong Zhou Shiyu Zhou Shun Zhou Sihong Zhou Xiang Zhou Xingyu Zhou Yang Zhou Yong Zhou Yu-Feng Zhou Zusheng Zhou Demin Zhou Dechong Zhu Hongbo Zhu Huaxing Zhu Jingya Zhu Kai Zhu Pengxuan Zhu Ruilin Zhu Xianglei Zhu Yingshun Zhu Yongfeng Zhu Xiao Zhuang Xuai Zhuang Mikhail Zobov Zhanguo Zong Cong Zou Hongying Zou 《Radiation Detection Technology and Methods》 CSCD 2024年第1期I0003-I0016,1-1091,共1105页
The Circular Electron Positron Collider(CEPC)is a large scientific project initiated and hosted by China,fostered through extensive collaboration with international partners.The complex comprises four accelerators:a 3... The Circular Electron Positron Collider(CEPC)is a large scientific project initiated and hosted by China,fostered through extensive collaboration with international partners.The complex comprises four accelerators:a 30 GeV Linac,a 1.1 GeV Damping Ring,a Booster capable of achieving energies up to 180 GeV,and a Collider operating at varying energy modes(Z,W,H,and tt).The Linac and Damping Ring are situated on the surface,while the subterranean Booster and Collider are housed in a 100 km circumference underground tunnel,strategically accommodating future expansion with provisions for a potential Super Proton Proton Collider(SPPC).The CEPC primarily serves as a Higgs factory.In its baseline design with synchrotron radiation(SR)power of 30 MW per beam,it can achieve a luminosity of 5×10^(34)cm^(-2)s^(-1)per interaction point(IP),resulting in an integrated luminosity of 13 ab^(-1)for two IPs over a decade,producing 2.6 million Higgs bosons.Increasing the SR power to 50 MW per beam expands the CEPC's capability to generate 4.3 million Higgs bosons,facilitating precise measurements of Higgs coupling at sub-percent levels,exceeding the precision expected from the HL-LHC by an order of magnitude.This Technical Design Report(TDR)follows the Preliminary Conceptual Design Report(Pre-CDR,2015)and the Conceptual Design Report(CDR,2018),comprehensively detailing the machine's layout,performance metrics,physical design and analysis,technical systems design,R&D and prototyping efforts,and associated civil engineering aspects.Additionally,it includes a cost estimate and a preliminary construction timeline,establishing a framework for forthcoming engineering design phase and site selection procedures.Construction is anticipated to begin around 2027-2028,pending government approval,with an estimated duration of 8 years.The commencement of experiments and data collection could potentially be initiated in the mid-2030s. 展开更多
关键词 initiated EXCEEDING PRECISE
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JUNO sensitivity on proton decay p→νK^(+)searches 被引量:1
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作者 Angel Abusleme Thomas Adam +608 位作者 Shakeel Ahmad Rizwan Ahmed Sebastiano Aiello Muhammad Akram 安丰鹏 安琪 Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop João Pedro Athayde Marcondes de André Didier Auguste Nikita Balashov Wander Baldini Andrea Barresi Davide Basilico Eric Baussan Marco Bellato Antonio Bergnoli Thilo Birkenfeld Sylvie Blin David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Mario Buscemi Jose Busto Ilya Butorov Anatael Cabrera Barbara Caccianiga 蔡浩 蔡啸 蔡严克 蔡志岩 Riccardo Callegari Antonio Cammi Agustin Campeny 曹传亚 曹国富 曹俊 Rossella Caruso Cédric Cerna 常劲帆 Yun Chang 陈平平 Po-An Chen 陈少敏 陈旭荣 Yi-Wen Chen 陈义学 陈羽 陈长 程捷 程雅苹 Alexey Chetverikov Davide Chiesa Pietro Chimenti Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Selma Conforti Di Lorenzo Daniele Corti Flavio Dal Corso Olivia Dalager Christophe De La Taille 邓智 邓子艳 Wilfried Depnering Marco Diaz Xuefeng Ding 丁雅韵 Bayu Dirgantara Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko 董建蒙 Evgeny Doroshkevich Marcos Dracos Frédéric Druillole 杜然 杜书先 Stefano Dusini Martin Dvorak Timo Enqvist Heike Enzmann Andrea Fabbri Ulrike Fahrendholz 范东华 樊磊 方建 方文兴 Marco Fargetta Dmitry Fedoseev Li-Cheng Feng 冯启春 Richard Ford Amélie Fournier 甘浩男 Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Agnese Giaz Nunzio Giudice Maxim Gonchar 龚光华 宫辉 Yuri Gornushkin Alexandre Göttel Marco Grassi Christian Grewing Vasily Gromov 顾旻皓 谷肖飞 古宇 关梦云 Nunzio Guardone Maria Gul 郭聪 郭竞渊 郭万磊 郭新恒 郭宇航 Paul Hackspacher Caren Hagner 韩然 Yang Han Muhammad Sohaib Hassan 何苗 何伟 Tobias Heinz Patrick Hellmuth 衡月昆 Rafael Herrera 贺远强 侯少静 Yee Hsiung Bei-Zhen Hu 胡航 胡健润 胡俊 胡守扬 胡涛 胡宇翔 胡焯钧 黄春豪 黄桂鸿 黄翰雄 黄文昊 黄鑫 黄性涛 黄永波 惠加琪 霍雷 霍文驹 Cédric Huss Safeer Hussain Ara Ioannisian Roberto Isocrate Beatrice Jelmini Kuo-Lun Jen Ignacio Jeria 季筱璐 吉星曌 贾慧慧 贾俊基 蹇司玉 蒋荻 蒋炜 江晓山 金如意 荆小平 Cécile Jollet Jari Joutsenvaara Sirichok Jungthawan Leonidas Kalousis Philipp Kampmann 康丽 Rebin Karaparambil Narine Kazarian Amina Khatun Khanchai Khosonthongkee Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Andre Kruth Nikolay Kutovskiy Pasi Kuusiniemi Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Victor Lebrin Frederic Lefevre 雷瑞庭 Rupert Leitner Jason Leung 李德民 李飞 李福乐 李高嵩 李海涛 李慧玲 李佳褀 李梦朝 李民 李楠 李楠 李清江 李茹慧 黎山峰 李涛 李卫东 李卫国 李笑梅 李小男 李兴隆 李仪 李依宸 李玉峰 李兆涵 李志兵 李紫源 梁浩 梁昊 廖佳军 Daniel Liebau Ayut Limphirat Sukit Limpijumnong Guey-Lin Lin 林盛鑫 林韬 凌家杰 Ivano Lippi 刘芳 刘海东 刘宏邦 刘红娟 刘洪涛 刘绘 刘江来 刘金昌 刘敏 刘倩 刘钦 Runxuan Liu 刘双雨 刘树彬 刘术林 刘小伟 刘熙文 刘言 刘云哲 Alexey Lokhov Paolo Lombardi Claudio Lombardo Kai Loo 陆川 路浩奇 陆景彬 吕军光 路书祥 卢晓旭 Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov 罗凤蛟 罗光 罗朋威 罗舒 罗武鸣 Vladimir Lyashuk 马帮争 马秋梅 马斯 马骁妍 马续波 Jihane Maalmi Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Francesco Manzali 冒鑫 冒亚军 Stefano M.Mari Filippo Marini Sadia Marium Cristina Martellini Gisele Martin-Chassard Agnese Martini Matthias Mayer Davit Mayilyan Ints Mednieks 孟月 Anselmo Meregaglia Emanuela Meroni David Meyhöfer Mauro Mezzetto Jonathan Miller Lino Miramonti Paolo Montini Michele Montuschi Axel Müller Massimiliano Nastasi Dmitry V.Naumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Minh Thuan Nguyen Thi 宁飞鹏 宁哲 Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Alexander Olshevskiy Domizia Orestano Fausto Ortica Rainer Othegraven Alessandro Paoloni Sergio Parmeggiano 裴亚田 Nicomede Pelliccia 彭安国 彭海平 Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Oliver Pilarczyk Luis Felipe Piñeres Rico Artyom Popov Pascal Poussot Wathan Pratumwan Ezio Previtali 齐法制 祁鸣 钱森 钱小辉 钱圳 乔浩 秦中华 丘寿康 Muhammad Usman Rajput Gioacchino Ranucci Neill Raper Alessandra Re Henning Rebber Abdel Rebii 任斌 任杰 Barbara Ricci Mariam Rifai Markus Robens Mathieu Roche Narongkiat Rodphai Aldo Romani Bedřich Roskovec Christian Roth 阮向东 阮锡超 Saroj Rujirawat Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Simone Sanfilippo Anut Sangka Nuanwan Sanguansak Utane Sawangwit Julia Sawatzki Fatma Sawy Michaela Schever Cédric Schwab Konstantin Schweizer Alexandr Selyunin Andrea Serafini Giulio Settanta Mariangela Settimo 邵壮 Vladislav Sharov Arina Shaydurova 石京燕 史娅楠 Vitaly Shutov Andrey Sidorenkov FedorŠimkovic Chiara Sirignano Jaruchit Siripak Monica Sisti Maciej Slupecki Mikhail Smirnov Oleg Smirnov Thiago Sogo-Bezerra Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov OndřejŠrámek Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich DušanŠtefánik Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Alexander Studenikin 孙世峰 孙希磊 孙勇杰 孙永昭 Narumon Suwonjandee Michal Szelezniak 唐健 唐强 唐泉 唐晓 Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Konstantin Treskov Andrea Triossi Giancarlo Troni Wladyslaw Trzaska Cristina Tuve Nikita Ushakov Johannes van den Boom Stefan van Waasen Guillaume Vanroyen Vadim Vedin Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Cristina Volpe Vit Vorobel Dmitriy Voronin Lucia Votano Pablo Walker 王彩申 Chung-Hsiang wang 王恩 王国利 王坚 王俊 王坤宇 汪璐 王美芬 王孟 王萌 王瑞光 王思广 王维 王为 王文帅 王玺 王湘粤 王仰夫 王耀光 王义 王忆 王贻芳 王元清 王玉漫 王喆 王铮 王志民 王综轶 Muhammad Waqas Apimook Watcharangkool 韦良红 魏微 韦雯露 魏亚东 温凯乐 温良剑 Christopher Wiebusch Steven Chan-Fai Wong Bjoern Wonsak 吴帝儒 吴群 吴智 Michael Wurm Jacques Wurtz Christian Wysotzki 习宇飞 夏冬梅 Xiang Xiao 谢小川 谢宇广 谢章权 邢志忠 续本达 徐程 徐东莲 徐繁荣 许杭锟 徐吉磊 徐晶 徐美杭 徐音Yu Xu 闫保军 Taylor Yan 闫文奇 严雄波 Yupeng Yan 杨安波 杨长根 杨成峰 杨欢 杨洁 杨雷 杨晓宇 杨翊凡 Yifan Yang 姚海峰 Zafar Yasin 叶佳璇 叶梅 叶子平 Ugur Yegin Frédéric Yermia 易培淮 尹娜 尹翔伟 尤郑昀 俞伯祥 余炽业 喻纯旭 余泓钊 于淼 于向辉 于泽源 于泽众 袁成卓 袁影 袁振雄 岳保彪 Noman Zafar Andre Zambanini Vitalii Zavadskyi 曾珊 曾婷轩 曾裕达 占亮 张爱强 张飞洋 张国庆 张海琼 张宏浩 张家梁 张家文 张杰 张金 张景波 张金楠 张鹏 张清民 张石其 张澍 张涛 张晓梅 张鑫 张玄同 张学尧 张岩 张银鸿 张易于 张永鹏 张宇 张圆圆 张玉美 张振宇 张志坚 赵凤仪 赵洁 赵荣 赵书俊 赵天池 郑冬琴 郑华 郑阳恒 钟伟荣 周静 周莉 周楠 周顺 周彤 周详 朱江 朱康甫 朱科军 朱志航 庄博 庄红林 宗亮 邹佳恒 JUNO Collaboration 《Chinese Physics C》 SCIE CAS CSCD 2023年第11期7-22,共16页
The Jiangmen Underground Neutrino Observatory(JUNO)is a large liquid scintillator detector designed to explore many topics in fundamental physics.In this study,the potential of searching for proton decay in the p→νK... The Jiangmen Underground Neutrino Observatory(JUNO)is a large liquid scintillator detector designed to explore many topics in fundamental physics.In this study,the potential of searching for proton decay in the p→νK^(+)mode with JUNO is investigated.The kaon and its decay particles feature a clear three-fold coincidence signature that results in a high efficiency for identification.Moreover,the excellent energy resolution of JUNO permits suppression of the sizable background caused by other delayed signals.Based on these advantages,the detection efficiency for the proton decay via p→νK^(+)is 36.9%±4.9%with a background level of 0.2±0.05(syst)±0.2(stat)events after 10 years of data collection.The estimated sensitivity based on 200 kton-years of exposure is 9.6×1033 years,which is competitive with the current best limits on the proton lifetime in this channel and complements the use of different detection technologies. 展开更多
关键词 proton decay grand unified theories JUNO liquid scintillator detector
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粒子物理及高能加速器的未来--新原理加速器能行吗? 被引量:2
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作者 王贻芳 鲁巍 《科学通报》 EI CAS CSCD 北大核心 2022年第9期805-808,共4页
新原理加速器是否将代替现有加速器?这一问题近来得到社会的广泛关注.本文介绍了粒子物理的发展目标及相应手段,新原理加速器的发展现状、问题、特点和趋势,给出了粒子物理、高能加速器及新原理加速器未来发展的个人见解.
关键词 高能加速器 粒子物理 个人见解 特点和趋势 未来
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Thermo-optic all-optical devices based on two-dimensional materials 被引量:4
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作者 KAN WU yifang wang +1 位作者 CIYUAN QIU JIANPING CHEN 《Photonics Research》 SCIE EI 2018年第10期I0024-I0030,共7页
In this paper, we review our recent work on thermo-optic all-optical devices based on two-dimensional(2 D)materials. The unique properties of 2 D materials enable fast and highly efficient thermo-optic control of ligh... In this paper, we review our recent work on thermo-optic all-optical devices based on two-dimensional(2 D)materials. The unique properties of 2 D materials enable fast and highly efficient thermo-optic control of light.A few all-optical devices are demonstrated based on various thermo-optic mechanisms. Both fiber and integrated devices will be shown. 展开更多
关键词 热光全光器件 材料学 通讯技术 发展现状
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Exploring the design space of immersive urban analytics 被引量:3
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作者 Zhutian Chen yifang wang +5 位作者 Tianchen Sun Xiang Gao Wei Chen Zhigeng Pan Huamin Qu Yingcai Wu 《Visual Informatics》 EI 2017年第2期132-142,共11页
Recent years have witnessed the rapid development and wide adoption of immersive head-mounted devices,such as HTC VIVE,Oculus Rift,and Microsoft HoloLens.These immersive devices have the potential to significantly ext... Recent years have witnessed the rapid development and wide adoption of immersive head-mounted devices,such as HTC VIVE,Oculus Rift,and Microsoft HoloLens.These immersive devices have the potential to significantly extend the methodology of urban visual analytics by providing critical 3D context information and creating a sense of presence.In this paper,we propose a theoretical model to characterize the visualizations in immersive urban analytics.Furthermore,based on our comprehensive and concise model,we contribute a typology of combination methods of 2D and 3D visualizations that distinguishes between linked views,embedded views,and mixed views.We also propose a supporting guideline to assist users in selecting a proper view under certain circumstances by considering visual geometry and spatial distribution of the 2D and 3D visualizations.Finally,based on existing work,possible future research opportunities are explored and discussed. 展开更多
关键词 Immersive urban analytics Virtual/Augmented/Mixed reality Urban visualizations Information visualizations Visualization theory
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Precision Higgs physics at the CEPC 被引量:1
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作者 Fenfen An Yu Bai +70 位作者 Chunhui Chen Xin Chen Zhenxing Chen Joao Guimaraes da Costa Zhenwei Cui Yaquan Fang Chengdong Fu Jun Gao Yanyan Gao Yuanning Gao Shaofeng Ge Jiayin Gu Fangyi Guo Jun Guo Tao Han Shuang Han Hongjian He Xianke He Xiaogang He Jifeng Hu Shih-Chieh Hsu Shan Jin Maoqiang Jing Susmita Jyotishmati Ryuta Kiuchi Chia-Ming Kuo Peizhu Lai Boyang Li Congqiao Li Gang Li Haifeng Li Liang Li Shu Li Tong Li Qiang Li Hao Liang Zhijun Liang Libo Liao Bo Liu Jianbei Liu Tao Liu Zhen Liu Xinchou Lou Lianliang Ma Bruce Mellado Xin Mo Mila Pandurovic Jianming Qian Zhuoni Qian Nikolaos Rompotis Manqi Ruan Alex Schuy Lianyou Shan Jingyuan Shi Xin Shi Shufang Su Dayong wang Jin wang Liantao wang yifang wang Yuqian Wei Yue Xu Haijun Yang Ying Yang Weiming Yao Dan Yu Kaili Zhang Zhaoru Zhang Mingrui Zhao Xianghu Zhao Ning Zhou 《Chinese Physics C》 SCIE CAS CSCD 2019年第4期5-44,共40页
The discovery of the Higgs boson with its mass around 125 GeV by the ATLAS and CMS Collaborations marked the beginning of a new era in high energy physics.The Higgs boson will be the subject of extensive studies of th... The discovery of the Higgs boson with its mass around 125 GeV by the ATLAS and CMS Collaborations marked the beginning of a new era in high energy physics.The Higgs boson will be the subject of extensive studies of the ongoing LHC program.At the same time,lepton collider based Higgs factories have been proposed as a possible next step beyond the LHC,with its main goal to precisely measure the properties of the Higgs boson and probe potential new physics associated with the Higgs boson.The Circular Electron Positron Collider(CEPC)is one of such proposed Higgs factories.The CEPC is an e^+e^- circular collider proposed by and to be hosted in China.Located in a tunnel of approximately 100 km in circumference,it will operate at a center-of-mass energy of 240 GeV as the Higgs factory.In this paper,we present the first estimates on the precision of the Higgs boson property measurements achievable at the CEPC and discuss implications of these measurements. 展开更多
关键词 CEPC HIGGS BOS on HIGGS BOSON properties HIGGS BOSON COUPLINGS HIGGS FACTORY effective field theory EFT
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Feasibility and physics potential of detecting ^(8)B solar neutrinos at JUNO 被引量:1
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作者 Angel Abusleme Thomas Adam +590 位作者 Shakeel Ahmad Sebastiano Aiello Muhammad Akram Nawab Ali Fengpeng An Guangpeng An Qi An Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop João Pedro Athayde Marcondes de André Didier Auguste Andrej Babic Wander Baldini Andrea Barresi Eric Baussan Marco Bellato Antonio Bergnoli Enrico Bernieri David Biare Thilo Birkenfeld Sylvie Blin David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Max Buesken Mario Buscemi Jose Busto Ilya Butorov Anatael Cabrera Hao Cai Xiao Cai Yanke Cai Zhiyan Cai Antonio Cammi Agustin Campeny Chuanya Cao Guofu Cao Jun Cao Rossella Caruso Cédric Cerna Jinfan Chang Yun Chang Pingping Chen Po-An Chen Shaomin Chen Shenjian Chen Xurong Chen Yi-Wen Chen Yixue Chen Yu Chen Zhang Chen Jie Cheng Yaping Cheng Alexander Chepurnov Davide Chiesa Pietro Chimenti Artem Chukanov Anna Chuvashova Gérard Claverie Catia Clementi Barbara Clerbaux Selma Conforti Di Lorenzo Daniele Corti Salvatore Costa Flavio Dal Corso Christophe De La Taille Jiawei Deng Zhi Deng Ziyan Deng Wilfried Depnering Marco Diaz Xuefeng Ding Yayun Ding Bayu Dirgantara Sergey Dmitrievsky Tadeas Dohnal Georgy Donchenko Jianmeng Dong Damien Dornic Evgeny Doroshkevich Marcos Dracos Frédéric Druillole Shuxian Du Stefano Dusini Martin Dvorak Timo Enqvist Heike Enzmann Andrea Fabbri Lukas Fajt Donghua Fan Lei Fan Can Fang Jian Fang Marco Fargetta Anna Fatkina Dmitry Fedoseev Vladko Fekete Li-Cheng Feng Qichun Feng Richard Ford Andrey Formozov Amélie Fournier Haonan Gan Feng Gao Alberto Garfagnini Alexandre Göttel Christoph Genster Marco Giammarchi Agnese Giaz Nunzio Giudice Franco Giuliani Maxim Gonchar Guanghua Gong Hui Gong Oleg Gorchakov Yuri Gornushkin Marco Grassi Christian Grewing Maxim Gromov Vasily Gromov Minghao Gu Xiaofei Gu Yu Gu Mengyun Guan Nunzio Guardone Maria Gul Cong Guo Jingyuan Guo Wanlei Guo Xinheng Guo Yuhang Guo Paul Hackspacher Caren Hagner Ran Han Yang Han Miao He Wei He Tobias Heinz Patrick Hellmuth Yuekun Heng Rafael Herrera Daojin Hong YuenKeung Hor Shaojing Hou Yee Hsiung Bei-Zhen Hu Hang Hu Jianrun Hu Jun Hu Shouyang Hu Tao Hu Zhuojun Hu Chunhao Huang Guihong Huang Hanxiong Huang Qinhua Huang Wenhao Huang Xingtao Huang Yongbo Huang Jiaqi Hui Wenju Huo Cédric Huss Safeer Hussain Antonio Insolia Ara Ioannisian Daniel Ioannisyan Roberto Isocrate Kuo-Lun Jen Xiaolu Ji Xingzhao Ji Huihui Jia Junji Jia Siyu Jian Di Jiang Xiaoshan Jiang Ruyi Jin Xiaoping Jing Cécile Jollet Jari Joutsenvaara Sirichok Jungthawan Leonidas Kalousis Philipp Kampmann Li Kang Michael Karagounis Narine Kazarian Amir Khan Waseem Khan Khanchai Khosonthongkee Patrick Kinz Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Svetlana Krokhaleva Zinovy Krumshteyn Andre Kruth Nikolay Kutovskiy Pasi Kuusiniemi Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Frederic Lefevre Liping Lei Ruiting Lei Rupert Leitner Jason Leung Demin Li Fei Li Fule Li Haitao Li Huiling Li Jiaqi Li Jin Li Kaijie Li Mengzhao Li Nan Li Nan Li Qingjiang Li Ruhui Li Shanfeng Li Shuaijie Li Tao Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xinglong Li Yi Li Yufeng Li Zhibing Li Ziyuan Li Hao Liang Hao Liang Jingjing Liang Jiajun Liao Daniel Liebau Ayut Limphirat Sukit Limpijumnong Guey-Lin Lin Shengxin Lin Tao Lin Jiajie Ling Ivano Lippi Fang Liu Haidong Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hu Liu Hui Liu Jianglai Liu Jinchang Liu Min Liu Qian Liu Qin Liu Runxuan Liu Shuangyu Liu Shubin Liu Shulin Liu Xiaowei Liu Yan Liu Alexey Lokhov Paolo Lombardi Claudio Lombardo Kai Loo Chuan Lu Haoqi Lu Jingbin Lu Junguang Lu Shuxiang Lu Xiaoxu Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Fengjiao Luo Guang Luo Pengwei Luo Shu Luo Wuming Luo Vladimir Lyashuk Qiumei Ma Si Ma Xiaoyan Ma Xubo Ma Jihane Maalmi Yury Malyshkin Fabio Mantovani Francesco Manzali Xin Mao Yajun Mao Stefano MMari Filippo Marini Sadia Marium Cristina Martellini Gisele Martin-Chassard Agnese Martini Davit Mayilyan Axel Müller Ints Mednieks Yue Meng Anselmo Meregaglia Emanuela Meroni David Meyhöfer Mauro Mezzetto Jonathan Miller Lino Miramonti Salvatore Monforte Paolo Montini Michele Montuschi Nikolay Morozov Pavithra Muralidharan Massimiliano Nastasi Dmitry VNaumov Elena Naumova Igor Nemchenok Alexey Nikolaev Feipeng Ning Zhe Ning Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Alexander Olshevskiy Domizia Orestano Fausto Ortica Hsiao-Ru Pan Alessandro Paoloni Nina Parkalian Sergio Parmeggiano Teerapat Payupol Yatian Pei Nicomede Pelliccia Anguo Peng Haiping Peng Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Luis Felipe Piñeres Rico Oliver Pilarczyk Artyom Popov Pascal Poussot Wathan Pratumwan Ezio Previtali Fazhi Qi Ming Qi Sen Qian Xiaohui Qian Hao Qiao Zhonghua Qin Shoukang Qiu Muhammad Rajput Gioacchino Ranucci Neill Raper Alessandra Re Henning Rebber Abdel Rebii Bin Ren Jie Ren Taras Rezinko Barbara Ricci Markus Robens Mathieu Roche Narongkiat Rodphai Aldo Romani Bedřich Roskovec Christian Roth Xiangdong Ruan Xichao Ruan Saroj Rujirawat Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Giuseppe Salamanna Simone Sanfilippo Anut Sangka Nuanwan Sanguansak Utane Sawangwit Julia Sawatzki Fatma Sawy Michaela Schever Jacky Schuler Cédric Schwab Konstantin Schweizer Dmitry Selivanov Alexandr Selyunin Andrea Serafini Giulio Settanta Mariangela Settimo Muhammad Shahzad Vladislav Sharov Gang Shi Jingyan Shi Yongjiu Shi Vitaly Shutov Andrey Sidorenkov FedorŠimkovic Chiara Sirignano Jaruchit Siripak Monica Sisti Maciej Slupecki Mikhail Smirnov Oleg Smirnov Thiago Sogo-Bezerra Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov Ondrej Sramek Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich DušanŠtefánik Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Alexander Studenikin Gongxing Sun Shifeng Sun Xilei Sun Yongjie Sun Yongzhao Sun Narumon Suwonjandee Michal Szelezniak Jian Tang Qiang Tang Quan Tang Xiao Tang Alexander Tietzsch Igor Tkachev Tomas Tmej Konstantin Treskov Andrea Triossi Giancarlo Troni Wladyslaw Trzaska Cristina Tuve Stefan van Waasen Johannes van den Boom Guillaume Vanroyen Nikolaos Vassilopoulos Vadim Vedin Giuseppe Verde Maxim Vialkov Benoit Viaud Cristina Volpe Vit Vorobel Lucia Votano Pablo Walker Caishen wang Chung-Hsiang wang En wang Guoli wang Jian wang Jun wang Kunyu wang Lu wang Meifen wang Meng wang Ruiguang wang Siguang wang Wei wang Wenshuai wang Xi wang Xiangyue wang Yangfu wang Yaoguang wang Yi wang yifang wang Yuanqing wang Yuman wang Zhe wang Zheng wang Zhimin wang Zongyi wang Apimook Watcharangkool Lianghong Wei Wei Wei Yadong Wei Liangjian Wen Christopher Wiebusch Steven Chan-Fai Wong Bjoern Wonsak Diru Wu Fangliang Wu Qun Wu Wenjie Wu Zhi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Dongmei Xia Yuguang Xie Zhangquan Xie Zhizhong Xing Benda Xu Donglian Xu Fanrong Xu Jilei Xu Jing Xu Meihang Xu Yin Xu Yu Xu Baojun Yan Xiongbo Yan Yupeng Yan Anbo Yang Changgen Yang Huan Yang Jie Yang Lei Yang Xiaoyu Yang Yifan Yang Haifeng Yao Zafar Yasin Jiaxuan Ye Mei Ye Ugur Yegin Frédéric Yermia Peihuai Yi Xiangwei Yin Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Hongzhao Yu Miao Yu Xianghui Yu Zeyuan Yu Chengzhuo Yuan Ying Yuan Zhenxiong Yuan Ziyi Yuan Baobiao Yue Noman Zafar Andre Zambanini Pan Zeng Shan Zeng Tingxuan Zeng Yuda Zeng Liang Zhan Feiyang Zhang Guoqing Zhang Haiqiong Zhang Honghao Zhang Jiawen Zhang Jie Zhang Jingbo Zhang Peng Zhang Qingmin Zhang Shiqi Zhang Tao Zhang Xiaomei Zhang Xuantong Zhang Yan Zhang Yinhong Zhang Yiyu Zhang Yongpeng Zhang Yuanyuan Zhang Yumei Zhang Zhenyu Zhang Zhijian Zhang Fengyi Zhao Jie Zhao Rong Zhao Shujun Zhao Tianchi Zhao Dongqin Zheng Hua Zheng Minshan Zheng Yangheng Zheng Weirong Zhong Jing Zhou Li Zhou Nan Zhou Shun Zhou Xiang Zhou Jiang Zhu Kejun Zhu Honglin Zhuang Liang Zong Jiaheng Zou 《Chinese Physics C》 SCIE CAS CSCD 2021年第2期93-110,共18页
The Jiangmen Underground Neutrino Observatory(JUNO)features a 20 kt multi-purpose underground liquid scintillator sphere as its main detector.Some of JUNO's features make it an excellent location for^8B solar neut... The Jiangmen Underground Neutrino Observatory(JUNO)features a 20 kt multi-purpose underground liquid scintillator sphere as its main detector.Some of JUNO's features make it an excellent location for^8B solar neutrino measurements,such as its low-energy threshold,high energy resolution compared with water Cherenkov detectors,and much larger target mass compared with previous liquid scintillator detectors.In this paper,we present a comprehensive assessment of JUNO's potential for detecting^8B solar neutrinos via the neutrino-electron elastic scattering process.A reduced 2 MeV threshold for the recoil electron energy is found to be achievable,assuming that the intrinsic radioactive background^(238)U and^(232)Th in the liquid scintillator can be controlled to 10^(-17)g/g.With ten years of data acquisition,approximately 60,000 signal and 30,000 background events are expected.This large sample will enable an examination of the distortion of the recoil electron spectrum that is dominated by the neutrino flavor transformation in the dense solar matter,which will shed new light on the inconsistency between the measured electron spectra and the predictions of the standard three-flavor neutrino oscillation framework.IfDelta m^(2)_(21)=4.8times10^(-5);(7.5times10^(-5))eV^(2),JUNO can provide evidence of neutrino oscillation in the Earth at approximately the 3sigma(2sigma)level by measuring the non-zero signal rate variation with respect to the solar zenith angle.Moreover,JUNO can simultaneously measureDelta m^2_(21)using^8B solar neutrinos to a precision of 20% or better,depending on the central value,and to sub-percent precision using reactor antineutrinos.A comparison of these two measurements from the same detector will help understand the current mild inconsistency between the value of Delta m^2_(21)reported by solar neutrino experiments and the KamLAND experiment. 展开更多
关键词 neutrino oscillation solar neutrino JUNO
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Study of imaging unknown objects by cosmic-ray muons 被引量:1
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作者 Mengzhao Li Yuekun Heng +4 位作者 yifang wang Kaile Wen Zhiyan Cai Xiaoyu Yang Zhi Wu 《Radiation Detection Technology and Methods》 CSCD 2021年第2期192-199,共8页
Introduction Cosmic-ray muon imaging is a kind of nondestructive detection technology which can be used to detect unknown objects in geological exploration,civil engineering and nuclear safety.Transmission imaging and... Introduction Cosmic-ray muon imaging is a kind of nondestructive detection technology which can be used to detect unknown objects in geological exploration,civil engineering and nuclear safety.Transmission imaging and scattering tomography schemes are studied.Method The transmission scheme uses a multilayer detector to measure the direction of a cosmic-ray muon passing through an object.The scattering scheme involves placing two detectors upstream and downstream of the object to record the incident and exit directions of the muon passing through the object.The effect of the detector resolution on the imaging clarity of transmission imaging was studied.The applicable scenarios of the two schemes were analyzed.Results The results by calculating show that in the transmission imaging of a hundred-meter object,a spatial resolution of 2.5 m can be achieved,and Cu and Fe can be discriminated with a density difference of 1.1 g/cm3.Scattering tomography is mainly suitable for meter-level objects,which can detect 0.2 m chamber and distinguish 0.05 m heavy metal blocks in rock. 展开更多
关键词 Cosmic-ray muon imaging MUON TOMOGRAPHY Nondestructive detection
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Sub-percent precision measurement of neutrino oscillation parameters with JUNO
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作者 Angel Abusleme Thomas Adam +601 位作者 Shakeel Ahmad Rizwan Ahmed Sebastiano Aiello Muhammad Akram Abid Aleem Fengpeng An Qi An Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop João Pedro Athayde Marcondes de André Didier Auguste Weidong Bai Nikita Balashov Wander Baldini Andrea Barresi Davide Basilico Eric Baussan Marco Bellato Antonio Bergnoli Thilo Birkenfeld Sylvie Blin David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Jose Busto Ilya Butorov Anatael Cabrera Barbara Caccianiga Hao Cai Xiao Cai Yanke Cai Zhiyan Cai Riccardo Callegari Antonio Cammi Agustin Campeny Chuanya Cao Guofu Cao Jun Cao Rossella Caruso Cédric Cerna Chi Chan Jinfan Chang Yun Chang Guoming Chen Pingping Chen Po-An Chen Shaomin Chen Xurong Chen Yixue Chen Yu Chen Zhiyuan Chen Zikang Chen Jie Cheng Yaping Cheng Yu Chin Cheng Alexey Chetverikov Davide Chiesa Pietro Chimenti Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Selma Conforti Di Lorenzo Daniele Corti Flavio Dal Corso Olivia Dalager Christophe De La Taille Zhi Deng Ziyan Deng Wilfried Depnering Marco Diaz Xuefeng Ding Yayun Ding Bayu Dirgantara Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko Jianmeng Dong Evgeny Doroshkevich Marcos Dracos Frédéric Druillole Ran Du Shuxian Du Stefano Dusini Martin Dvorak Timo Enqvist Heike Enzmann Andrea Fabbri Donghua Fan Lei Fan Jian Fang Wenxing Fang Marco Fargetta Dmitry Fedoseev Zhengyong Fei Li-Cheng Feng Qichun Feng Richard Ford Amélie Fournier Haonan Gan Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Nunzio Giudice Maxim Gonchar Guanghua Gong Hui Gong Yuri Gornushkin Alexandre Göttel Marco Grassi Vasily Gromov Minghao Gu Xiaofei Gu Yu Gu Mengyun Guan Yuduo Guan Nunzio Guardone Cong Guo Jingyuan Guo Wanlei Guo Xinheng Guo Yuhang Guo Paul Hackspacher Caren Hagner Ran Han Yang Han Miao He Wei He Tobias Heinz Patrick Hellmuth Yuekun Heng Rafael Herrera YuenKeung Hor Shaojing Hou Yee Hsiung Bei-Zhen Hu Hang Hu Jianrun Hu Jun Hu Shouyang Hu Tao Hu Yuxiang Hu Zhuojun Hu Guihong Huang Hanxiong Huang Kaixuan Huang Wenhao Huang Xin Huang Xingtao Huang Yongbo Huang Jiaqi Hui Lei Huo Wenju Huo Cédric Huss Safeer Hussain Ara Ioannisian Roberto Isocrate Beatrice Jelmini Ignacio Jeria Xiaolu Ji Huihui Jia Junji Jia Siyu Jian Di Jiang Wei Jiang Xiaoshan Jiang Xiaoping Jing Cécile Jollet Jari Joutsenvaara Leonidas Kalousis Philipp Kampmann Li Kang Rebin Karaparambil Narine Kazarian Amina Khatun Khanchai Khosonthongkee Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Nikolay Kutovskiy Pasi Kuusiniemi Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Victor Lebrin Frederic Lefevre Ruiting Lei Rupert Leitner Jason Leung Daozheng Li Demin Li Fei Li Fule Li Gaosong Li Huiling Li Mengzhao Li Min Li Nan Li Nan Li Qingjiang Li Ruhui Li Rui Li Shanfeng Li Tao Li Teng Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xinglong Li Yi Li Yichen Li Yufeng Li Zepeng Li Zhaohan Li Zhibing Li Ziyuan Li Zonghai Li Hao Liang Hao Liang Jiajun Liao Ayut Limphirat Guey-Lin Lin Shengxin Lin Tao Lin Jiajie Ling Ivano Lippi Fang Liu Haidong Liu Haotian Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hui Liu Jianglai Liu Jinchang Liu Min Liu Qian Liu Qin Liu Runxuan Liu Shubin Liu Shulin Liu Xiaowei Liu Xiwen Liu Yan Liu Yunzhe Liu Alexey Lokhov Paolo Lombardi Claudio Lombardo Kai Loo Chuan Lu Haoqi Lu Jingbin Lu Junguang Lu Shuxiang Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov Daibin Luo Fengjiao Luo Guang 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 Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Francesco Manzali Xin Mao Yajun Mao Stefano M.Mari Filippo Marini Cristina Martellini Gisele Martin-Chassard Agnese Martini Matthias Mayer Davit Mayilyan Ints Mednieks Artur Meinusch Yue Meng Anselmo Meregaglia Emanuela Meroni David Meyhö Mauro Mezzetto Jonathan Miller Lino Miramonti Marta Colomer Molla Paolo Montini Michele Montuschi Axel Müller Massimiliano Nastasi Dmitry V.Naumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Minh Thuan Nguyen Thi Feipeng Ning Zhe Ning Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Alexander Olshevskiy Domizia Orestano Fausto Ortica Rainer Othegraven Alessandro Paoloni Sergio Parmeggiano Yatian Pei Luca Pelicci Nicomede Pelliccia Anguo Peng Haiping Peng Yu Peng Zhaoyuan Peng Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Oliver Pilarczyk Luis Felipe Piñeres Artyom Popov Pascal Poussot Ezio Previtali Fazhi Qi Ming Qi Sen Qian Xiaohui Qian Zhen Qian Hao Qiao Zhonghua Qin Shoukang Qiu Gioacchino Ranucci Neill Raper Reem Rasheed Alessandra Re Henning Rebber Abdel Rebii Mariia Redchuk Bin Ren Jie Ren Barbara Ricci Mariam Rifai Mathieu Roche Narongkiat Rodphai Aldo Romani Bedřich Roskovec Xichao Ruan Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Simone Sanfilippo Anut Sangka Utane Sawangwit Julia Sawatzki Michaela Schever Cédric Schwab Konstantin Schweizer Alexandr Selyunin Andrea Serafini Giulio Settanta Mariangela Settimo Zhuang Shao Vladislav Sharov Arina Shaydurova Jingyan Shi Yanan Shi Vitaly Shutov Andrey Sidorenkov FedorŠimkovic Chiara Sirignano Jaruchit Siripak Monica Sisti Maciej Slupecki Mikhail Smirnov Oleg Smirnov Thiago Sogo-Bezerra Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov OndřejŠrámek Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich DušanŠtefánik Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Alexander Studenikin Jun Su Shifeng Sun Xilei Sun Yongjie Sun Yongzhao Sun Zhengyang Sun Narumon Suwonjandee Michal Szelezniak Jian Tang Qiang Tang Quan Tang Xiao Tang Vidhya Thara Hariharan Eric Theisen Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Konstantin Treskov Andrea Triossi Giancarlo Troni Wladyslaw Trzaska Alexandros Tsagkarakis Cristina Tuve Nikita Ushakov Vadim Vedin Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Cristina Volpe Katharina Von Sturm Vit Vorobel Dmitriy Voronin Lucia Votano Pablo Walker Caishen wang Chung-Hsiang wang En wang Guoli wang Jian wang Jun wang Lu wang Meifen wang Meng wang Meng wang Ruiguang wang Siguang wang Wei wang Wei wang Wenshuai wang Xi wang Xiangyue wang Yangfu wang Yaoguang wang Yi wang Yi wang yifang wang Yuanqing wang Yuman wang Zhe wang Zheng wang Zhimin wang Zongyi wang Apimook Watcharangkool Wei Wei Wei Wei Wenlu Wei Yadong Wei Kaile Wen Liangjian Wen Christopher Wiebusch Steven Chan-Fai Wong Bjoern Wonsak Diru Wu Qun Wu Zhi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Dongmei Xia Xiang Xiao Xiaochuan Xie Yuguang Xie Zhangquan Xie Zhao Xin Zhizhong Xing Benda Xu Cheng Xu Donglian Xu Fanrong Xu Hangkun Xu Jilei Xu Jing Xu Meihang Xu Yin Xu Baojun Yan Taylor Yan Wenqi Yan Xiongbo Yan Yupeng Yan Changgen Yang Chengfeng Yang Huan Yang Jie Yang Lei Yang Xiaoyu Yang Yifan Yang Haifeng Yao Jiaxuan Ye Mei Ye Ziping Ye Frédéric Yermia Na Yin Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Hongzhao Yu Miao Yu Xianghui Yu Zeyuan Yu Zezhong Yu Cenxi Yuan Chengzhuo Yuan Ying Yuan Zhenxiong Yuan Baobiao Yue Noman Zafar Vitalii Zavadskyi Shan Zeng Tingxuan Zeng Yuda Zeng Liang Zhan Aiqiang Zhang Bin Zhang Binting Zhang Feiyang Zhang Guoqing Zhang Honghao Zhang Jialiang Zhang Jiawen Zhang Jie Zhang Jin Zhang Jingbo Zhang Jinnan Zhang Mohan Zhang Peng Zhang Qingmin Zhang Shiqi Zhang Shu Zhang Tao Zhang Xiaomei Zhang Xin Zhang Xuantong Zhang Xueyao Zhang Yinhong Zhang Yiyu Zhang Yongpeng Zhang Yu Zhang Yuanyuan Zhang Yumei Zhang Zhenyu Zhang Zhijian Zhang Fengyi Zhao Jie Zhao Rong Zhao Runze Zhao Shujun Zhao Dongqin Zheng Hua Zheng Yangheng Zheng Weirong Zhong Jing Zhou Li Zhou Nan Zhou Shun Zhou Tong Zhou Xiang Zhou Jiang Zhu Jingsen Zhu Kangfu Zhu Kejun Zhu Zhihang Zhu Bo Zhuang Honglin Zhuang Liang Zong Jiaheng Zou 《Chinese Physics C》 SCIE CAS CSCD 2022年第12期28-49,共22页
JUNO is a multi-purpose neutrino observatory under construction in the south of China.This publication presents new sensitivity estimates for the measurement of the △m_(31)^(2),△m_(21)^(2),sin^(2)θ_(12),and sin^(2)... JUNO is a multi-purpose neutrino observatory under construction in the south of China.This publication presents new sensitivity estimates for the measurement of the △m_(31)^(2),△m_(21)^(2),sin^(2)θ_(12),and sin^(2)θ_(13) oscillation parameters using reactor antineutrinos,which is one of the primary physics goals of the experiment.The sensitivities are obtained using the best knowledge available to date on the location and overburden of the experimental site,the nuclear reactors in the surrounding area and beyond,the detector response uncertainties,and the reactor antineutrino spectral shape constraints expected from the TAO satellite detector.It is found that the △m_(21)^(2) and sin^(2)θ_(12) oscillation parameters will be determined to 0.5%precision or better in six years of data collection.In the same period,the △m_(31)^(2) parameter will be determined to about 0.2%precision for each mass ordering hypothesis.The new precision represents approximately an order of magnitude improvement over existing constraints for these three parameters. 展开更多
关键词 neutrino oscillation reactor antineutrino precision measurement JUNO
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Laser measurement system for acrylic transmittance of JUNO central detector
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作者 Zhaohan Li Xiaoyu Yang +12 位作者 Yuekun Heng Xiaoyan Ma Xiaohui Qian Kaixi Huang Zhi Wu Wei He Meihang Xu Xiaolan Luo Yatian Pei Mengzhao Li Zhiyan Cai Wenlu Wei yifang wang 《Radiation Detection Technology and Methods》 CSCD 2021年第3期356-363,共8页
Background During the research phase of acrylic panel for the Jiangmen Underground Neutrino Observatory(JUNO)central detector(CD),the darkroom transmittance measurement system(DTMS)was designed and built,and a massive... Background During the research phase of acrylic panel for the Jiangmen Underground Neutrino Observatory(JUNO)central detector(CD),the darkroom transmittance measurement system(DTMS)was designed and built,and a massive amount of measurements were carried out to help determine the composition and processing techniques of the acrylic panel.Motivation The mass production of acrylic panels was started after the pilot production.The requirement of transmittance measurement put forward new demands on operation,and a new measurement system was considered to support removable and non-destructive measurement on site.Result After the accomplishment of design,development and verification were completed,the laser measurement system came into use in the acrylic workshop of Taixing Donchamp Acrylic Ltd,and the transmittance results of acrylic spherical panels met the requirement of JUNO.The optical design,tooling design,data processing interface and uncertainty analyses of the laser measurement system are discussed in detail,and the measured transmittance results are also introduced in this article. 展开更多
关键词 LASER Non-destructive measurement TRANSMITTANCE JUNO
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Towards the meV limit of the effective neutrino mass in neutrinoless double-beta decays
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作者 Jun Cao Guo-yuan Huang +5 位作者 Yu-Feng Li yifang wang Liang-Jian Wen Zhi-zhong Xing Zhen-hua Zhao Shun Zhou 《Chinese Physics C》 SCIE CAS CSCD 2020年第3期1-11,共11页
We emphasize that it is extremely important for future neutrinoless double-beta(0νββ)decay experiments to reach the sensitivity to the effective neutrino mass|mββ|≈1 meV.With such a sensitivity,it is highly poss... We emphasize that it is extremely important for future neutrinoless double-beta(0νββ)decay experiments to reach the sensitivity to the effective neutrino mass|mββ|≈1 meV.With such a sensitivity,it is highly possible to discover the signals of 0νββ decays.If no signal is observed at this sensitivity level,then either neutrinos are Dirac particles or stringent constraints can be placed on their Majorana masses.In this paper,assuming the sensitivity of|mββ|≈1 meV for future 0νββ decay experiments and the precisions on neutrion oscillation parameters after the JUNO experiment,we fully explore the constrained regions of the lightest neutrino mass m1 and two Majorana-type CP-violating phases{ρ,σ}.Several important conclusions in the case of normal neutrino mass ordering can be made.First,the lightest neutrino mass is severely constrained to a narrow range m1∈[0.7,8]meV,which together with the precision measurements of neutrino mass-squared differences from oscillation experiments completely determines the neutrino mass spectrum m2∈[8.6,11.7]meV ing phases is limited to ρ∈[130°,230°],which cannot be obtained from any other realistic experiments.Third,the sum of three neutrino masses is found to beΣ≡m1+m2+m3∈[59.2,72.6]meV,while the effective neutrino mass for beta decays turns out to be mβ≡(|Ue1|2m1^2+|Ue2|2m2^2+|Ue3|2m3^2)1/2∈[8.9,12.6]meV.These observations clearly set up the roadmap for future non-oscillation neutrino experiments aiming to solve the fundamental problems in neutrino physics. 展开更多
关键词 neutrinoless double-beta decays absolute neutrino masses Majorana CP phases
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All-optical modulator based on MoS_2-PVA thin film
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作者 yifang wang Kan Wu Jianping Chen 《Chinese Optics Letters》 SCIE EI CAS CSCD 2018年第2期8-11,共4页
The all-optical approach plays an important role in ultrafast all-optical signal processing, and the all-fiber scheme has a wide application in optical communications. In this letter, we investigate an all-optical mod... The all-optical approach plays an important role in ultrafast all-optical signal processing, and the all-fiber scheme has a wide application in optical communications. In this letter, we investigate an all-optical modulator using few-layer molybdenum disulfide(MoS2)-polyvinyl alcohol(PVA) thin films based on the thermo-optic effect and obtain a long-time stable modulated output by applying polarization interference. By absorbing the injected 980 nm pump(control light), MoS2 generates heat, changes the refractive index of MoS2, and modulates the polarization of light. The obtained thermal all-optical modulator has a rise time of 526 μs. 展开更多
关键词 PVA Mo All-optical modulator based on MoS2-PVA thin film
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Different genes involved in the amelioration of chronic neuropathic pain and comorbid anxiety by electroacupuncture with different intensities
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作者 Yuxin Hu yifang wang +7 位作者 Mengdi Xie Xiaoyu Li Qilin Jiang Xiaofen He Rong Zhou Zui Shen Jianqiao Fang Xiaomei Shao 《Clinical Traditional Medicine and Pharmacology》 2024年第3期46-61,共16页
Background:With its complex and prevalent symptoms,chronic neuropathic pain(CNP)is frequently combined with negative emotions.Electroacupuncture(EA)is a widely-used and effective treatment for CNP and pain-induced com... Background:With its complex and prevalent symptoms,chronic neuropathic pain(CNP)is frequently combined with negative emotions.Electroacupuncture(EA)is a widely-used and effective treatment for CNP and pain-induced comorbid anxiety-like behaviors(PABs).Although different effects may result from EA with different intensities,the underlying mechanisms remain unclear.Objective:The study aimed to investigate the effects of EA with different intensities on CNP and PABs and the underlying mechanisms,by exploring the different genes through RNASeq in the spinal cord dorsal horn(SCDH)and periaqueductal gray(PAG).Methods:A spared nerve injury(SNI)model was established using male C57BL/6 J mice,and treated with EA of different intensities(0.1 mA or 0.3 mA,both at 100 Hz).The von-Frey tests,open field tests and elevated plus maze tests were used to measure the mechanical paw withdrawal threshold(PWT)and PABs of the mice.The tissues of SCDH and PAG regions were extracted to identify the changes in gene expression,and biofunctional analysis of differentially expressed genes(DEGs)was further performed by RNA-seq analysis.The expression of key DEGs and corresponding proteins was assessed using quantitative real-time PCR(qPCR)and protein immunofluorescence detection,respectively.Results:Both 0.1 mA and 0.3 mA EA at 100 Hz alleviated PABs compared with the SNI group.Furthermore,0.3 mA EA was effective in increasing PWT in SNI mice,whereas 0.1 mA EA was not.A total of 108 DEGs was identified in the SCDH,and 254 DEGs were identified in the PAG.Specifically,the expression of Tnr in SNI mice decreased after the treatment with 0.3 mA EA at 100 Hz,and the expression of Ptprb,Net1,Abcb1a and Adgrf5 in SNI mice decreased in the PAG after the treatment with 0.1 mA EA at 100 Hz.Conclusion:The effect of 0.3 mA EA on chronic pain may be related to the decrease of Tnr expression in SCDH,and the effect of 0.1 mA EA on PABs may be achieved by decreased expression of Ptprb and Net1 in PAG. 展开更多
关键词 Chronic neuropathic pain Electroacupuncture Gene expression Spinal cord dorsal horn Periaqueductal gray
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