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High-Precision Localization Method for Spheres with a Theodolite
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作者 junfeng sun Qihua Huang +3 位作者 Lianyou An Jinling Kang Baolu Wang Huanlong Zhang 《Instrumentation》 2025年第2期14-22,共9页
Spherical objects are widely used in target localization applications,and the existing sphere localization methods with cameras or total stations both have some limitations.A new high-precision sphere localization met... Spherical objects are widely used in target localization applications,and the existing sphere localization methods with cameras or total stations both have some limitations.A new high-precision sphere localization method with a theodolite is proposed in this paper.From the view point of the theodolite,the contour points of a sphere with a known radius are measured as latitude-longitude coordinates.It is observed that the center of the target sphere is located on a cylindrical surface constructed with the latitude-longitude coordinates,and therefore the latitude-longitude coordinates of at least three contour points can be used to construct a set of ternary quadratic equations.The Gröbner basis method is used to compute at most four real solutions of the sphere center coordinates.To distinguish the only meaningful solution from the other possible real solutions,a pre-processing of the measured longitude values is also proposed.The factors affecting the positioning accuracy of the sphere center are evaluated in simulation experiments,which are used to obtain an empirical estimation model of the positioning error.Real data experiments are also performed and the results show that the proposed method can achieve high localization precision. 展开更多
关键词 sphere localization latitude-longitude coordinates gröbner basis empirical estimation model
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Rotor airfoil aerodynamic design method and wind tunnel test verification 被引量:2
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作者 Weiguo ZHANG junfeng sun +2 位作者 Liangquan WANG Jie WU Long HE 《Chinese Journal of Aeronautics》 SCIE EI CAS CSCD 2020年第8期2123-2132,共10页
Well-designed airfoil is very important for high-performance rotor.This paper developed an efficient multi-objective and multi-constraint optimization design system for rotor airfoils based on RANS analysis,and verifi... Well-designed airfoil is very important for high-performance rotor.This paper developed an efficient multi-objective and multi-constraint optimization design system for rotor airfoils based on RANS analysis,and verified the performance of the optimized airfoil.Using CRA09-A as the baseline rotor airfoil,the CRA09-B optimized rotor airfoil was designed successfully.Combined with the foundation of high-precision rotor airfoil stationary test technology,the CRA09-B and CRA09-A rotor airfoils were tested in the S3 MA high-speed wind tunnel of ONERA.In order to correct the aerodynamic data,a single parameter linear wall pressure method is used to consider the tunnel effects.The results indicate that multi-objective and multi-constraint optimization design method developed in this study is reliable,and that CRA09-B optimized airfoil provides better stationary performance than CRA09-A airfoil in terms of maximum lift coefficient and lift-to-drag ratio. 展开更多
关键词 Airfoil design CRA09 airfoil Optimization method ROTOR Wind tunnel test
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Network Security Situation Prediction Based on TCAN-BiGRU Optimized by SSA and IQPSO 被引量:1
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作者 junfeng sun Chenghai Li +2 位作者 Yafei Song Peng Ni Jian Wang 《Computer Systems Science & Engineering》 SCIE EI 2023年第10期993-1021,共29页
The accuracy of historical situation values is required for traditional network security situation prediction(NSSP).There are discrepancies in the correlation and weighting of the various network security elements.To ... The accuracy of historical situation values is required for traditional network security situation prediction(NSSP).There are discrepancies in the correlation and weighting of the various network security elements.To solve these problems,a combined prediction model based on the temporal convolution attention network(TCAN)and bi-directional gate recurrent unit(BiGRU)network is proposed,which is optimized by singular spectrum analysis(SSA)and improved quantum particle swarmoptimization algorithm(IQPSO).This model first decomposes and reconstructs network security situation data into a series of subsequences by SSA to remove the noise from the data.Furthermore,a prediction model of TCAN-BiGRU is established respectively for each subsequence.TCAN uses the TCN to extract features from the network security situation data and the improved channel attention mechanism(CAM)to extract important feature information from TCN.BiGRU learns the before-after status of situation data to extract more feature information from sequences for prediction.Besides,IQPSO is proposed to optimize the hyperparameters of BiGRU.Finally,the prediction results of the subsequence are superimposed to obtain the final predicted value.On the one hand,IQPSO compares with other optimization algorithms in the experiment,whose performance can find the optimum value of the benchmark function many times,showing that IQPSO performs better.On the other hand,the established prediction model compares with the traditional prediction methods through the simulation experiment,whose coefficient of determination is up to 0.999 on both sets,indicating that the combined prediction model established has higher prediction accuracy. 展开更多
关键词 Network security situation prediction SSA IQPSO TCAN-BiGRU
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Hybrid deep learning approach for rock tunnel deformation prediction based on spatio-temporal patterns 被引量:2
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作者 junfeng sun Yong Fang +5 位作者 Hu Luo Zhigang Yao Long Xiang Jianfeng Wang Yubo Wang Yifan Jiang 《Underground Space》 2025年第1期100-118,共19页
The ability to predict tunnel deformation holds great significance for ensuring the reliability, safety, and sustainability of tunnel struc-tures. However, existing deformation prediction models often simplify or over... The ability to predict tunnel deformation holds great significance for ensuring the reliability, safety, and sustainability of tunnel struc-tures. However, existing deformation prediction models often simplify or overlook the impact of spatial characteristics on deformationby treating it as a time series prediction issue. This study utilizes monitoring data from the Grand Canyon Tunnel and introduces aneffective data-driven method for predicting tunnel deformation based on the spatio-temporal characteristics of the historical deformationof adjacent sections. The proposed model, a combination of graph attention network (GAT) and bidirectional long and short-term mem-ory network (Bi-LSTM), is equipped with robust spatio-temporal predictive capabilities. Additionally, the study explores other possiblespatial connections and the scalability of the model. The results indicate that the proposed model outperforms other deep learning mod-els, achieving favorable root mean square error (RMSE), mean absolute error (MAE), and coefficient of determination (R^(2)) values of0.34 mm, 0.23 mm, and 0.94, respectively. The graph structure based on intuitive spatial connections proves more suitable for meetingthe challenges of predicting deformation. Integrating GAT-LSTM with transfer learning technology, remains stable performance whenextended to other tunnels with limited data. 展开更多
关键词 GAT-LSTM Deep learning Transfer learning Tunnel deformation
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Correction:CEPC Technical Design Report:Accelerator
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作者 Waleed Abdallah Tiago CarlosAdorno de Freitas +1112 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 Triparno Bandyopadhyay Shou‑Shan Bao Desmond P.Barber Ays¸e 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 Biagio Di Micco Ran Ding Siqin Ding Yadong Ding Haiyi Dong Jianing Dong Jing Dong Lan Dong Mingyi Dong Xu Dong Yipei Dong Yubing Dong Milos Dordevic Marco Drewes Mingxuan Du Mingxuan Du Qianqian Du Xiaokang Du Yanyan Du Yong Du Yunfei Du Chun‑Gui Duan Zhe Duan Yahor Dydyshka Ulrik Egede Walaa Elmetenawee Yun Eo Ka Yan Fan Kuanjun Fan Yunyun Fan Bo Fang Shuangshi Fang Yuquan Fang Ada Farilla Riccardo Farinelli Muhammad Farooq Angeles Faus Golfe Almaz Fazliakhmetov Rujun Fei Bo Feng Chong Feng Junhua Feng Xu Feng Zhuoran Feng ZhuoranFeng Luis Roberto Flores Castillo Etienne Forest Andrew Fowlie Harald Fox Hai‑Bing Fu Jinyu Fu Benjamin Fuks Yoshihiro Funakoshi Emidio Gabrielli Nan Gan Li Gang Jie Gao Meisen Gao Wenbin Gao Wenchun Gao Yu Gao Yuanning Gao Zhanxiang Gao Yanyan Gao Kun Ge Shao‑Feng Ge Zhenwu Ge Li‑Sheng Geng Qinglin Geng Chao‑Qiang Geng Swagata Ghosh Antonio Gioiosa Leonid Gladilin Ti Gong Stefania Gori Quanbu Gou Sebastian Grinstein Chenxi Gu Gerardo Guillermo Joao Guimaraes da Costa Dizhou Guo Fangyi Guo Jiacheng Guo Jun Guo Lei Guo Lei Guo Xia Guo Xin‑Heng Guo Xinyang Guo Yun Guo Yunqiang Guo Yuping Guo Zhi‑Hui Guo Alejandro Gutie´rrez‑Rodríguez Seungkyu Ha Noman Habib Jan Hajer Francois Hammer Chengcheng Han Huayong Han Jifeng Han Liang Han Liangliang Han Ruixiong Han Yang Han Yezi Han Yuanying Han Tao Han Jiankui Hao Xiqing Hao XiqingHao Chuanqi He Dayong He Dongbing He Guangyuan He Hong‑Jian He Jibo He Jun He Longyan He Xiang He Xiao‑Gang He Zhenqiang He Klaus Heinemann Sven Heinemeyer Yuekun Heng María AHernandez‑Ruíz Jiamin Hong Yuenkeung Hor George WSHou Xiantao Hou Xiaonan Hou Zhilong Hou Suen Hou Caishi Hu Chen Hu Dake Hu Haiming Hu Jiagen Hu Jun Hu Kun Hu Shouyang Hu Yongcai Hu Yu Hu Zhen Hu Zhehao Hua Jianfei Hua Chao‑Shang Huang Fa Peng Huang Guangshun Huang Jinshu Huang Ke Huang Liangsheng Huang Shuhui Huang Xingtao Huang Xu‑Guang Huang Yanping Huang Yonggang Huang Yongsheng Huang Zimiao Huang Chen Huanyuan Changgi Huh Jiaqi Hui Lihua Huo Talab Hussain Kyuyeong Hwang Ara Ioannisian Munawar Iqbal Paul Jackson Shahriyar Jafarzade Haeun Jang Seoyun Jang Daheng Ji Qingping Ji Quan Ji Xiaolu Ji Jingguang Jia Jinsheng Jia Xuewei Jia Zihang Jia Cailian Jiang Han Ren Jiang Houbing Jiang Jun Jiang Xiaowei Jiang Xin Jiang Xuhui Jiang Yongcheng Jiang Zhongjian Jiang Cheng Jiang Ruiqi Jiao Dapeng Jin Shan Jin Song Jin Yi Jin Junji Jis sunghoon Jung Goran Kacarevic Eric Kajfasz Lidia Kalinovskaya Aleksei Kampf Wen Kang Xian‑Wei Kang Xiaolin Kang Biswajit Karmakar Zhiyong Ke Rijeesh Keloth Alamgir Khan Hamzeh Khanpour Khanchai Khosonthongkee KhanchaiKhosonthongkee Bobae Kim Dongwoon Kim Mi Ran Kim Minsuk Kim sungwon Kim On Kim Michael Klasen Sanghyun Ko Ivan Koop Vitaliy Kornienko Bryan Kortman Gennady Kozlov Shiqing Kuang Mukesh Kumar Chia Ming Kuo Tsz Hong Kwok Franc¸ois Sylvain Ren Lagarde Pei‑Zhu Lai Imad Laktineh Xiaofei Lan Zuxiu Lan Lia Lavezzi Justin Lee Junghyun Lee Sehwook Lee Ge Lei Roy Lemmon Yongxiang Leng Sze 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 Jianyi Liu Jingdong Liu Jinhua Liu Kai Liu Kang Liu Kun Liu Mengyao Liu Peng Liu Pengcheng Liu Qibin Liu Shan Liu Shidong Liu Shuang Liu Shubin Liu Tao Liu Tao Liu Tong Liu Wei Liu Xiang Liu Xiao‑Hai Liu Xiaohui Liu Xiaoyu Liu Xin Liu Xinglin Liu Xingquan Liu Yang Liu Yanlin Liu Yao‑Bei Liu Yi Liu Yiming Liu Yong Liu Yonglu Liu Yu Liu Yubin Liu Yudong Liu Yulong Liu Zhaofeng Liu Zhen Liu Zhenchao Liu Zhi Liu Zhi‑Feng Liu Zhiqing Liu Zhongfu Liu Zuowei Liu Mia Liu Zhen Liu Xiaoyang Liu Xinchou Lou Cai‑Dian Lu Jun‑Xu Lu Qiu Zhen Lu Shang Lu Shang Lu Wenxi Lu Xiaohan Lu Yunpeng Lu Zhiyong Lu Xianguo Lu Wei Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Arslan Lukanov Jinliang Luo Tao Luo xiaoan Luo Xiaofeng Luo Xiaolan Luo Jindong Lv Feng Lyu Xiao‑Rui Lyu Kun‑Feng Lyu Ande Ma Hong‑Hao Ma Jun‑Li Ma Kai Ma Lishuang Ma Na Ma Renjie Ma Weihu Ma Xinpeng Ma Yanling Ma Yan‑Qing Ma Yongsheng Ma Zhonghui Ma Zhongjian Ma Yang Ma Mousam Maity Lining Mao Yanmin Mao Yaxian Mao Aure´lien Martens Caccia Massimo Luigi Maria Shigeki Matsumoto Bruce Mellado Davide Meloni Lingling Men Cai Meng Lingxin Meng Zhenghui Mi Yuhui Miao Mauro Migliorati Lei Ming Vasiliki AMitsou Laura Monaco Arthur Moraes Karabo Mosala Ahmad Moursy Lichao Mu Zhihui Mu Nickolai Muchnoi Daniel Muenstermann Daniel Muenstermann Pankaj Munbodh William John Murray Jérôme Nanni Dmitry Nanzanov Changshan Nie Sergei Nikitin Feipeng Ning Guozhu Ning Jia‑Shu Niu Juan‑Juan Niu Yan Niu Edward Khomotso Nkadimeng Kazuhito Ohmi Katsunobu Oide Hideki Okawa Mohamed Ouchemhou Qun Ouyang Daniele Paesani Carlo Pagani Stathes Paganis Collette Pakuza Jiangyang Pan Juntong Pan Tong Pan Xiang Pan Papia Panda Saraswati Pandey Mila Pandurovic Rocco Paparella Roman Pasechnik Emilie Passemar Hua Pei Xiaohua Peng Xinye Peng Yuemei Peng Jialun Ping Ronggang Ping Souvik Priyam Adhya Baohua Qi Hang Qi Huirong Qi Ming Qi Sen Qian Zhuoni Qian Congfeng Qiao Guangyou Qin Jiajia Qin Laishun Qin Liqing Qin Qin Qin Xiaoshuai Qin Zhonghua Qin Guofeng Qu 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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》 2025年第1期184-192,共9页
Correction to:Radiation Detection Technology and Methods(2024)8:1-1105.https://doi.org/10.1007/s41605-024-00463-y.In this article all authors name was missing in the springer link.It has been corrected.The original ar... Correction to:Radiation Detection Technology and Methods(2024)8:1-1105.https://doi.org/10.1007/s41605-024-00463-y.In this article all authors name was missing in the springer link.It has been corrected.The original article has been corrected. 展开更多
关键词 springer linkit radiation detection technology METHODS accelerator correction
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Numerical implication of water-soil leakage induced by longitudinal tunnel segment dislocation opening in saturated strata
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作者 Fan Chen junfeng sun +2 位作者 Hao Xiong Zhen-Yu Yin Xiangsheng Chen 《Journal of Rock Mechanics and Geotechnical Engineering》 2025年第12期7570-7589,共20页
Water-soil leakage due to the longitudinal dislocation opening of tunnel segments in high-permeable soil strata is crucial for ensuring the longevity of underground tunnel infrastructures.This research delves into thi... Water-soil leakage due to the longitudinal dislocation opening of tunnel segments in high-permeable soil strata is crucial for ensuring the longevity of underground tunnel infrastructures.This research delves into this complex phenomenon employing coupled computational fluiddynamics(CFD),discrete element method(DEM),and finiteelement method(FEM),considering varied tunnel buried depths and dislocation opening sizes.Two critical areas susceptible to water-soil leakage have been identified,including an‘ellipsoid’shaped area at the tunnel top and a soil sliding area perpendicular to the tunneling direction.With a narrow segment opening(3 d_(50)),the fineloss remains below 2%across various buried depths,whereas it escalates to 7.4%-30%with increasing buried depth under a slightly wider opening(3.8d_(50)).The proposed three-dimensional(3D)ellipsoid model is used to delineate the leakage region and quantify over 98%ground soil loss due to dislocation opening.Furthermore,the research reveals that soil sliding induced by water-soil leakage significantly decreases the structural shear stress on the waists and inverts of the tunnel segment,while the soil arching at the top of the tunnel would mitigate the stress release,particularly at the lower dislocated tunnel segment. 展开更多
关键词 Tunnel segment dislocation Water-soil leakage Computational fluiddynamics(CFD) Discrete element method(DEM) Finite element method(FEM) Tunnel loading Structure analysis
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链霉菌形态分化与次级代谢产物合成的研究进展 被引量:18
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作者 薛正莲 王珊 +2 位作者 孙俊峰 王芳 周健 《微生物学报》 CAS CSCD 北大核心 2021年第12期3870-3886,共17页
链霉菌是一类具有复杂的形态分化周期和强大的次级代谢能力的高GC含量的放线菌,能够利用其初级代谢产生的前体化合物和能量,合成多种结构复杂、功能多样的具有生物活性的次级代谢产物,在农业、食品、畜牧业、工业以及医药研究等领域都... 链霉菌是一类具有复杂的形态分化周期和强大的次级代谢能力的高GC含量的放线菌,能够利用其初级代谢产生的前体化合物和能量,合成多种结构复杂、功能多样的具有生物活性的次级代谢产物,在农业、食品、畜牧业、工业以及医药研究等领域都具有重要的价值。在链霉菌的形态分化后期常常伴随着次级代谢产物的生物合成,并且两者都受到复杂的网络调控;同时链霉菌的形态对次级代谢产物的产量和种类造成很大影响。对链霉菌生长周期的全面理解将加深对链霉菌形态分化与次级代谢产物合成关系的认识。本文将对链霉菌的形态分化过程、形态分化和抗生素合成两者共同的调控因子以及链霉菌形态与抗生素产量之间的关系进行综述,这将有助于理解抗生素的合成过程,也将会在缩短发酵周期、构建高产工程菌株、新型杀菌剂的研发以及新型抗生素的合成等方面给予我们启发。 展开更多
关键词 链霉菌 形态分化 次级代谢 拟核结合蛋白 双组分调控
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Low-intensity focused ultrasound stimulation promotes stroke recovery via astrocytic HMGB1 and CAMK2N1 in mice 被引量:3
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作者 Lin Qi Cheng Wang +12 位作者 Lidong Deng Jia-Ji Pan Qian Suo Shengju Wu Lin Cai Xudong Shi junfeng sun Yongting Wang Yaohui Tang Weibao Qiu Guo-Yuan Yang Jixian Wang Zhijun Zhang 《Stroke & Vascular Neurology》 SCIE CSCD 2024年第5期505-518,共14页
Background Low-intensity focused ultrasound stimulation(LIFUS)has been developed to enhance neurological repair and remodelling during the late acute stage of ischaemic stroke in rodents.However,the cellular and molec... Background Low-intensity focused ultrasound stimulation(LIFUS)has been developed to enhance neurological repair and remodelling during the late acute stage of ischaemic stroke in rodents.However,the cellular and molecular mechanisms of neurological repair and remodelling after LIFUS in ischaemic stroke are unclear.Methods Ultrasound stimulation was treated in adult male mice 7 days after transient middle cerebral artery occlusion.Angiogenesis was measured by laser speckle imaging and histological analyses.Electromyography and fibre photometry records were used for synaptogenesis.Brain atrophy volume and neurobehaviour were assessed 0–14 days after ischaemia.iTRAQ proteomic analysis was performed to explore the differentially expressed protein.scRNA-seq was used for subcluster analysis of astrocytes.Fluorescence in situ hybridisation and Western blot detected the expression of HMGB1 and CAMK2N1.Results Optimal ultrasound stimulation increased cerebral blood flow,and improved neurobehavioural outcomes in ischaemic mice(p<0.05).iTRAQ proteomic analysis revealed that the expression of HMGB1 increased and CAMK2N1 decreased in the ipsilateral hemisphere of the brain at 14 days after focal cerebral ischaemia with ultrasound treatment(p<0.05).scRNA-seq revealed that this expression pattern belonged to a subcluster of astrocytes after LIFUS in the ischaemic brain.LIFUS upregulated HMGB1 expression,accompanied by VEGFA elevation compared with the control group(p<0.05).Inhibition of HMGB1 expression in astrocytes decreased microvessels counts and cerebral blood flow(p<0.05).LIFUS reduced CAMK2N1 expression level,accompanied by increased extracellular calcium ions and glutamatergic synapses(p<0.05).CAMK2N1 overexpression in astrocytes decreased dendritic spines,and aggravated neurobehavioural outcomes(p<0.05).Conclusion Our results demonstrated that LIFUS promoted angiogenesis and synaptogenesis after focal cerebral ischaemia by upregulating HMGB1 and downregulating CAMK2N1 in a subcluster of astrocytes,suggesting that LIFUS activated specific astrocyte subcluster could be a key target for ischaemic brain therapy. 展开更多
关键词 STIMULATION BEHAVIOUR INTENSITY
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CEPC Technical Design Report 被引量:2
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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 Biagio Di Micco Ran Ding Siqin Dingl Yadong Ding Haiyi Dong Jianing Dong Jing Dong Lan Dong Mingyi Dong Xu Dong Yipei Dong Yubing Dong Milos Dordevic Marco Drewes Mingxuan Du Mingxuan Du Qianqian Du Xiaokang Du Yanyan Du Yong Du Yunfei Du Chun-Gui Duan Zhe Duan Yahor Dydyshka Ulrik Egede Walaa Elmetenawee Yun Eo Ka Yan Fan Kuanjun Fan Yunyun Fan Bo Fang Shuangshi Fang Yuquan Fang Ada Farilla Riccardo Farinelli Muhammad Farooq Angeles Faus Golfe Almaz Fazliakhmetov Rujun Fei Bo Feng Chong Feng Junhua Feng Xu Feng Zhuoran Feng Zhuoran Feng Luis Roberto Flores Castillo Etienne Forest Andrew Fowlie Harald Fox Hai-Bing Fu Jinyu Fu Benjamin Fuks Yoshihiro Funakoshi Emidio Gabrielli Nan Gan Li Gang Jie Gao Meisen Gao Wenbin Gao Wenchun Gao Yu Gao Yuanning Gao Zhanxiang Gao Yanyan Gao Kun Ge Shao-Feng Ge Zhenwu Ge Li-Sheng Geng Qinglin Geng Chao-Qiang Geng Swagata Ghosh Antonio Gioiosa Leonid Gladilin Ti Gong Stefania Gori Quanbu Gou Sebastian Grinstein Chenxi Gu Gerardo Guillermo Joao Guimaraes da Costa Dizhou Guo Fangyi Guo Jiacheng Guo Jun Guo Lei Guo Lei Guo Xia Guo Xin-Heng Guo Xinyang Guo Yun Guo Yunqiang Guo Yuping Guo Zhi-Hui Guo Alejandro Gutierrez-Rodriguez Seungkyu Ha Noman Habib Jan Hajer Francois Hammer Chengcheng Han Huayong Han Jifeng Han Liang Han Liangliang Han Ruixiong Han Yang Han Yezi Han Yuanying Han Tao Han Jiankui Hao Xiqing Hao Xiqing Hao Chuanqi He Dayong He Dongbing He Guangyuan He Hong-Jian He Jibo He Jun He Longyan He Xiang He Xiao-Gang He Zhenqiang He Klaus Heinemann Sven Heinemeyer Yuekun Heng Maria A.Hernandez-Ruiz Jiamin Hong Yuenkeung Hor George W.S.Hou Xiantao Hou Xiaonan Hou Zhilong Hou Suen Hou Caishi Hu Chen Hu Dake Hu Haiming Hu Jiagen Hu Jun Hu Kun Hu Shouyang Hu Yongcai Hu Yu Hu Zhen Hu Zhehao Hua Jianfei Hua Chao-Shang Huang Fa Peng Huang Guangshun Huang Jinshu Huang Ke Huang Liangsheng Huang Shuhui Huang Xingtao Huang Xu-Guang Huang Yanping Huang Yonggang Huang Yongsheng Huang Zimiao Huang Chen Huanyuan Changgi Hua Jiaqi Hui Lihua Huo Talab Hussain Kyuyeong Hwang Ara loannisian Munawar Iqbal Paul Jackson Shahriyar Jafarzade Haeun Jang Seoyun Jang Daheng Ji Qingping Ji Quan Ji Xiaolu Ji Jingguang Jia Jinsheng Jia Xuewei Jia Zihang Ja Cailian Jiang Han Ren Jiang Houbing Jiang Jun Jiang Xiaowei Jiang Xin Jiang Xuhui Jiang Yongcheng Jiang Zhongjian Jiang Cheng Jiang Ruiqi Jiao Dapeng Jin Shan Jin Song Jin Yi Jin Junji Jis sunghoon Jung Goran Kacarevic Eric Kajfasz Lidia Kalinovskaya Aleksei Kampf Wen Kang Xian-Wei Kang Xiaolin Kang Biswajit Karmakar Zhiyong Ke Rijeesh Keloth Alamgir Khan Hamzeh Khanpour Khanchai Khosonthongkee KhanchaiKhosonthongkee Bobae Kim Dongwoon Kim Mi Ran Kim Minsuk Kim sungwon Kim On Kim Michael Klasen Sanghyun Ko Ivan Koop Vitaliy Kornienko Bryan Kortman Gennady Kozlov Shiqing Kuang Mukesh Kumar Chia Ming Kuo Tsz Hong Kwok Fran cois Sylvain Ren Lagarde Pei-Zhu Lai Imad Laktineh Xiaofei Lan Zuxiu Lan Lia Lavezzi Justin Lee Junghyun Lee Sehwook Lee Ge Lei Roy Lemmon longxiang Leng Sze 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 Jianyi Liu Jingdong Liu Jinhua Liu Kai Liu Kang Liu Kun Liu Mengyao Liu Peng Liu Pengcheng Liu Qibin Liu Shan Liu Shidong Liu Shuang Liu Shubin Liu Tao Liu Tao Liu Tong Liu Wei Liu Xiang Liu Xiao-Hai Liu Xiaohui Liu Xiaoyu Liu Xin Liu Xinglin Liu Xingquan Liu Yang Liu Yanlin Liu Yao-Bei Liu Yi Liu Yiming Liu Yong Liu Yonglu Liu Yu Liu Yubin Liu Yudong Liu Yulong Liu Zhaofeng Liu Zhen Liu Zhenchao Liu Zhi Liu Zhi-Feng Liu Zhiqing Liu Zhongfu Liu Zuowei Liu Mia Liu Zhen Liu Xiaoyang Liu Xinchou Lou Cai-Dian Lu Jun-Xu Lu Qiu Zhen Lu Shang Lu Shang Lu Wenxi Lu Xiaohan Lu Yunpeng Lu Zhiyong Lu Xianguo Lu Wei Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Arslan Lukanov Jinliang Luo Tao Luo xiaoan Luo Xiaofeng Luo Xiaolan Luo Jindong Lv Feng Lyu Xiao-Rui Lyu Kun-Feng Lyu Ande Ma Hong-Hao Ma Jun-Li Ma Kai Ma Lishuang Ma Na Ma Renjie Ma Weihu Ma Xinpeng Ma Yanling Ma Yan-Qing Ma Yongsheng Ma Zhonghui Ma Zhongjian Ma Yang Ma Mousam Maity Lining Mao Yanmin Mao Yaxian Mao Aure lien Martens Caccia Massimo Luigi Maria Shigeki Matsumoto Bruce Mellado Davide Meloni Lingling Men Cai Meng Lingxin Meng Zhenghui Mi Yuhui Miao Mauro Migliorati Lei Ming Vasiliki A.Mitsou Laura Monaco Arthur Moraes Karabo Mosala Ahmad Moursy Lichao Mu Zhihui Mu Nickolai Muchnoi Daniel Muenstermann DanielMuenstermann Pankaj Munbodh William John Murray Jerome Nanni Dmitry Nanzanov Changshan Nie Sergei Nikitin Feipeng Ning Guozhu Ning Jia-Shu Niu Juan-Juan Niu Yan Niu Edward Khomotso Nkadimeng Kazuhito Ohmi Katsunobu Oide Hideki Okawa Mohamed Ouchemhou Qun Ouyang Daniele Paesani Carlo Pagani Stathes Paganis Collette Pakuza Jiangyang Pan Juntong Pan Tong Pan Xiang Pan Papia Panda Saraswati Pandey Mila Pandurovic Rocco Paparella Roman Pasechnik Emilie Passemar r Hua Pei Xiaohua Peng Xinye Peng Yuemei Peng Jialun Ping Ronggang Ping Souvik Priyam Adhya Baohua Qi Hang Qi Huirong Qi Ming Qi Sen Qian Zhuoni Qian Congfeng Qiao Guangyou Qin Jiajia Qin Laishun Qin Liqing Qin Qin Qin Xiaoshuai Qin Zhonghua Qin Guofeng Qu Antonio Racioppi Michael Ramsey-Musolf Shabbar Raza Vladimir Rekovic Jing Ren Jirgen Reuter Tania Robens Giancarlo Rossi Manqi Ruan Manqi Ruan Leonid Rumyantsev Min Sang Ryu Renat Sadykov Minjing Sang Juan Jose Sanz-Cillero Miroslav Saur Nishil Savla Michael A.Schmidt Daniele Sertore Ron Settles Peng Sha Ding-Yu Shao Ligang Shao Hua-Sheng Shao Xin She Chuang Shen Hong-Fei Shen Jian-Ming Shen Peixun Shen Qiuping Shen Zhongtao Shen Shuqi Sheng Haoyu Shi Hua Shi Qi Shi Shusu Shi Xiaolei Shi Xin Shi Yukun Shi Zhan Shi Ian Shipsey Gary Shiu Chang Shu Zong-Guo Si Andrei Sidorenkov Ivan Smiljanc Aodong Song Huayang Song Jiaojiao Song Jinxing Song Siyuan Song Weimin Song Weizheng Song Zhi Song Shashwat Sourav Paolo Spruzzola Feng Su Shengsen Su Wei Su Shufang Su Yanfeng Sui Zexuan Sui Michael Sullivan Baiyang sun Guoqiang sun Hao sun Hao-Kai sun junfeng sun Liang sun Mengcheng sunl Pengfei sun Sichun sun Xianjing sun Xiaohu sun Xilei sun Xingyang sun Xin-Yuan sun Yanjun sun Yongzhao sun Yue sun Zheng sun Zheng sun Narumon Suwonjandee Elsayed Tag Eldin Biao Tan Bo Tang Chuanxiang Tang Gao Tang Guangyi Tang Jian Tang Jingyu Tang Liang Tang Ying'Ao Tang Junquan Tao Abdel Nasser Taw fik Geoffrey Taylor Valery Telnov Saike Tian Riccardo Torre Wladyslaw Henryk Trzaska Dmitri Tsybychev Yanjun Tu Shengquan Tuo Michael Tytgat Ghalib Ul Islam Nikita Ushakov German Valencia Jaap Velthuis Alessandro Vicini Trevor Vickey Ivana Vidakovic Henri Videau Raymond Volkas Dmitry Voronin Natasa Vukasinovic Xia Wan Xuying Wan Xiao Wang Anqing Wang Bin Wang Chengtao Wang Chuanye Wang Ci Wang Dayong Wang Dou Wang En Wang Fei Wang Fei Wang Guanwen Wang Guo-Li Wang Haijing Wang Haolin Wang Jia Wang Jian Wang Jianchun Wang Jianli Wang Jiawei Wang Jin Wang Jin-Wei Wang Joseph Wang Kechen Wang Lechun Wang Lei Wang Liguo Wang Lijiao Wang Lu Wang Meng Wang Na Wang Pengcheng Wang Qian Wang Qun Wang Shu Lin Wang Shudong Wang Taofeng Wang Tianhong Wang Tianyang Wang Tong Wang Wei Wang Wei Wang Xiaolong Wang Xiaolong Wang Xiaoning Wang Xiao-Ping Wang Xiongfei Wang Xujian Wang Yaping Wang Yaqian Wang Yi Wang Yiao Wang Yifang Wang Yilun Wang Yiwei Wang You-Kai Wang Yuanping Wang Yuexin Wang Yuhao Wang Yu-Ming Wang Yuting Wang Zhen Wang Zhigang Wang Weiping Wang Zeren Simon Wang Biao Wang Hui Wang Lian-Tao Wang Zihui Wang Zirui Wang Jia Wang Tong Wang Daihui Wei Shujun Wei Wei Wei Xiaomin Wei Yuanyuan Wei Yingjie Wei Liangjian Wen Xuejun Wen Yufeng Wen Martin White Peter Williams Zef Wolffs William John Womersley Baona Wu Bobing Wu Guanjian Wu Jinfei Wu Lei Wu Lina Wu Linghui Wu Minlin Wu Peiwen Wu Qi Wu Qun Wu Tianya Wu Xiang Wu Xiaohong Wu Xing-Gang Wu Xuehui Wu Yaru Wu Yongcheng Wu Yuwen Wu Zhi Wu Xin Wu Lei Xia Ligang Xia Shang Xia Benhou Xiang Dao Xiang Zhiyu Xiang Bo-Wen Xiao Chu-Wen Xiao Dong Xiao Guangyan Xiao Han Xiao Meng Xiao Ouzheng Xiao Rui-Qing Xiao Xiang Xiao Yichen Xiao Ying Xiao Yu Xiao Yunlong Xiao Zhenjun Xiao Hengyuan Xiao Nian Xie Yuehong Xie Tianmu Xin Ye Xing Zhizhong Xing Da Xu Fang Xu Fanrong Xu Haisheng Xu Haocheng Xu Ji Xu Miaofu Xu Qingjin Xu Qingnian Xu Wei Xu Wei Xu Weixi Xu Xinping Xu Zhen Xu Zijun Xu Zehua Xu Yaoyuan Xu Feifei Xue Baojun Yan Bin Yan Fen Yan Fucheng Yan Jiaming Yan Liang Yan Luping Yan Qi-Shu Yan Wenbiao Yan Yupeng Yan Luping Yan Haoyue Yan Dong Yang Fengying Yang Guicheng Yang Haijun Yang Jin Min Yang Jing Yang Lan Yang Li Yang Li Lin Yang Lili Yang Litao Yang Mei Yang Qiaoli Yang Tiansen Yang Xiaochen Yang Yingjun Yang Yueling Yang Zhengyong Yang Zhenwei Yang Youhua Yang Xiancong Yang De-Liang Yao Shi Yao Lei Ye Lingxi Ye Mei Ye Rui Ye Rui Ye Yecheng Ye Vitaly Yermolchyk Kai Yi Li Yi Yang Yi Di Yin Peng-Fei Yin Shenghua Yin Ze Yin Zhongbao Yin Zhang Yinhong Hwi Dong Yoo Zhengyun You Charles Young Boxiang Yu Chenghui Yu Fusheng Yu Jie-Sheng Yu Jinqing Yu Lingda Yu Zhao-Huan Yu Felix Yu Bingrong Yu Changzheng Yuan Li Yuan Xing-Bo Yuan Youjin Yuan Junhui Yue Qian Yue Baobiao Yue Un Nisa Zaib Riccardo Zanzottera 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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Metal-soil interface adhesion in clay clogging during shield tunneling:Theoretical model and experimental validation 被引量:1
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作者 Yong Fang Bin Zhuo +3 位作者 Yubo Wang Hu Luo junfeng sun Yuxiang Yao 《Underground Space》 SCIE EI CSCD 2024年第2期188-202,共15页
Clogging is a major geohazards risk in mechanized tunnelling through cohesive soils.Clay clogging results from the high adhesion between the clay and metal.Based on the water film theory and Reynolds fluid equation,th... Clogging is a major geohazards risk in mechanized tunnelling through cohesive soils.Clay clogging results from the high adhesion between the clay and metal.Based on the water film theory and Reynolds fluid equation,the interfacial adhesion between metal and soil is simplified in this study as viscous hydrodynamic behavior between planes.Considering the influence of capillary force and the viscous force of water film at the interface between metal and soil,a theoretical calculation model of interfacial adhesion between metal and soil is established.The influence of water film thickness and separation rate on the interfacial adhesion between metal and soil is qualitatively analyzed.Then,the adhesion stress between the clay and the metal surface was tested with a pullout test and the influence of moisture content,pullout rates and types of clay minerals on the adhesion stress was analyzed.Finally,the calculation model of adhesion force was compared with the experimental results.The calculation model of soil adhesion stress established in this paper can quantitatively describe the relationship between soil adhesion force and moisture content and can also qualitatively reveal the influence mechanism of soil moisture content on adhesion stress. 展开更多
关键词 EPB clogging Adhesion stress Mechanics model Clays Mechanism analysis Experimental test
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Reinvestigating B→PV decays by including contributions from Φ_(B2) with the perturbative QCD approach
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作者 Yueling Yang Xule Zhao +2 位作者 Lan Lang Jinshu Huang junfeng sun 《Chinese Physics C》 SCIE CAS CSCD 2022年第8期34-62,共29页
Considering the B mesonic wave function φ_(B2),B→PV decays are re studied in the leading order for three scenarios using the perturbative QCD approach within the standard model,where P=π and K,and V denotes the gro... Considering the B mesonic wave function φ_(B2),B→PV decays are re studied in the leading order for three scenarios using the perturbative QCD approach within the standard model,where P=π and K,and V denotes the ground SU(3) vector mesons.It is found that contributions from φ_(B2) can enhance most branching ratios and are helpful for improving the overall consistency of branching ratios between the updated calculations and available data,although there are still several discrepancies between the experimental and theoretical results. 展开更多
关键词 B→PV decays B mesonic wave function perturbative QCD approach branching ratio
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B_u→ψM decays and S-D wave mixing effects
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作者 Yueling Yang Yupei Guo +3 位作者 junfeng sun Na Wang Qin Chang Gongru Lu 《Chinese Physics C》 SCIE CAS CSCD 2018年第11期8-23,共16页
The Bu→ψM decays are studied with the perturbative QCD approach, where the psion ψ=ψ(2S), ψ(3770), ψ(4040) and ψ(4160), and the light meson M = π, K, ρ and K^*. The factorizable and non-factorizable ... The Bu→ψM decays are studied with the perturbative QCD approach, where the psion ψ=ψ(2S), ψ(3770), ψ(4040) and ψ(4160), and the light meson M = π, K, ρ and K^*. The factorizable and non-factorizable contributions, and the S-D wave mixing effects on the psions, are considered in the calculation. With appropriate inputs, the branching ratios for the Bu→ψM decays are generally coincident with the experimental data within errors. However, due to the large theoretical and experimental errors, it is impossible for the moment to give a severe constraint on the S-D wave mixing angles. 展开更多
关键词 B meson weak decay psion perturbative QCD
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Study of C parity violating and strangeness changing J/ψ→ PP weak decays
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作者 Yueling Yang Junliang Lu +2 位作者 Mingfei Duan Jinshu Huang junfeng sun 《Chinese Physics C》 SCIE CAS CSCD 2021年第8期45-53,共9页
Although J/ψ weak decays are rare,they are possible within the standard model of elementary particles.Inspired by the potential prospects of the future intensity frontier,the C parity violating J/ψ→πη^(′),ηη′... Although J/ψ weak decays are rare,they are possible within the standard model of elementary particles.Inspired by the potential prospects of the future intensity frontier,the C parity violating J/ψ→πη^(′),ηη′decays and the strangeness changing J/ψ→πK,Kη^(′)decays are studied via the perturbative QCD approach.It is determined that the J/ψ→ηη^(′) decays have relatively large branching ratios,approximately on the order of 10^(11),which might be within the measurement capability and sensitivity of the future STCF experiment. 展开更多
关键词 J/Ψ weak decay perturbative QCD factorization
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