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Ultra-broadband microwave absorber and high-performance pressure sensor based on aramid nanofiber,polypyrrole and nickel porous aerogel
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作者 Leyi zhang Hongyu Jin +7 位作者 Hanxin Liao rao zhang Bochong Wang Jianyong Xiang Congpu Mu Kun Zhai Tianyu Xue Fusheng Wen 《International Journal of Minerals,Metallurgy and Materials》 SCIE EI CAS CSCD 2024年第8期1912-1921,共10页
Electronic devices have become ubiquitous in our daily lives,leading to a surge in the use of microwave absorbers and wearable sensor devices across various sectors.A prime example of this trend is the aramid nanofibe... Electronic devices have become ubiquitous in our daily lives,leading to a surge in the use of microwave absorbers and wearable sensor devices across various sectors.A prime example of this trend is the aramid nanofibers/polypyrrole/nickel(APN)aerogels,which serve dual roles as both microwave absorbers and pressure sensors.In this work,we focused on the preparation of aramid nanofibers/polypyrrole(AP15)aerogels,where the mass ratio of aramid nanofibers to pyrrole was 1:5.We employed the oxidative polymerization method for the preparation process.Following this,nickel was thermally evaporated onto the surface of the AP15 aerogels,resulting in the creation of an ultralight(9.35 mg·cm^(-3)).This aerogel exhibited a porous structure.The introduction of nickel into the aerogel aimed to enhance magnetic loss and adjust impedance matching,thereby improving electromagnetic wave absorption performance.The minimum reflection loss value achieved was-48.7 dB,and the maximum effective absorption bandwidth spanned 8.42 GHz with a thickness of 2.9 mm.These impressive metrics can be attributed to the three-dimensional network porous structure of the aerogel and perfect impedance matching.Moreover,the use of aramid nanofibers and a three-dimensional hole structure endowed the APN aerogels with good insulation,flame-retardant properties,and compression resilience.Even under a compression strain of 50%,the aerogel maintained its resilience over 500 cycles.The incorporation of polypyrrole and nickel particles further enhanced the conductivity of the aerogel.Consequently,the final APN aerogel sensor demonstrated high sensitivity(10.78 kPa-1)and thermal stability.In conclusion,the APN aerogels hold significant promise as ultra-broadband microwave absorbers and pressure sensors. 展开更多
关键词 porous aerogel aramid nanofibers microwave absorbers pressure sensor porous structure
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Do companies influenced by smart cities pay more attention to green governance?Mechanism and optimal spatial correlation
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作者 Xiaoxu Guo rao zhang Yue zhang 《Chinese Journal of Population,Resources and Environment》 2024年第1期48-57,共10页
Smart cities are a way for China to construct an innovative and environmentally conscious nation.The paper examines the impact of smart cities on corporate green governance and provides a theoretical foundation for fo... Smart cities are a way for China to construct an innovative and environmentally conscious nation.The paper examines the impact of smart cities on corporate green governance and provides a theoretical foundation for formulating and executing smart city policy in China.Based on panel data from Chinese A-share listed companies in Shanghai and Shenzhen from 2008 to 2020,this study constructs a multiperiod double-difference model to examine the influence of smart cities on corporate green governance.Additionally,it uses a spatial double-difference model to investigate the spatial spillover effect of smart cities on neighboring areas.The findings indicate that smart cities effectively enhance corporate green governance.Analyzing the influencing mechanisms reveals that resource allocation efficiency,technological innovation,management environmental awareness,and regional environmental enforcement efforts act as mediators.Furthermore,the study reveals that the impact of smart cities on promoting corporate green governance is more pronounced in regions with lower levels of marketization and resource-based cities.Moreover,the research explores the spatial spillover effects of smart cities,with an effective radius of approximately 350 km.The optimal spatial correlation zone for green governance of businesses in neighboring areas in relation to smart cities is within a range of 250-350 km.This is manifested by the significant promotion of green governance in neighboring area businesses facilitated by smart cities. 展开更多
关键词 Smart cities Corporate green governance Mediating effects Spatial associations
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Composites of In/C hexagonal nanorods and graphene nanosheets for high-performance electromagnetic wave absorption 被引量:2
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作者 rao zhang Congpu Mu +4 位作者 Bochong Wang Jianyong Xiang Kun Zhai Tianyu Xue Fusheng Wen 《International Journal of Minerals,Metallurgy and Materials》 SCIE EI CAS CSCD 2023年第3期485-493,共9页
In recent years,electromagnetic wave(EMW)absorption has been extensively investigated for solving EMW radiation and pollution.The metal-organic frameworks(MOFs)have attracted attention due to their low density and uni... In recent years,electromagnetic wave(EMW)absorption has been extensively investigated for solving EMW radiation and pollution.The metal-organic frameworks(MOFs)have attracted attention due to their low density and unique structure,which can meet the requirements of strong reflection loss(RL)and wide absorption bandwidth of EMW absorption materials.In this manuscript,indium nanoparticles/porous carbon(In/C)nanorods composites were prepared via the pyrolysis of nanorods-like In-MOFs at a low temperature of450°C.Indium nanoparticles are evenly attached and embedded on porous carbon.Low electrical conductivity of In/C nanorods is unfavorable to EMW absorption performance,which is due to the low temperature carbonization.Thus,graphene(Gr)nanosheets with high electrical conductivity are introduced to adjust electromagnetic parameters of In/C nanorods for enhancing EMW absorption.The minimum RL of the In/C-Gr-4 composite is up to-43.7 dB with a thin thickness of 1.30 mm.In addition,when the thickness is further reduced to 1.14 mm,the minimum RL of-39.3 dB at 16.1 GHz and effective absorption bandwidth of 3.7 GHz(from 14.3 to 18.0 GHz)can be achieved.This work indicates that In/C-Gr composites show excellent EMW absorption performance. 展开更多
关键词 electromagnetic wave absorption metal-organic frameworks indium nanoparticles nanorod GRAPHENE PERMITTIVITY
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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 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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Phase transition of multi-component(TiZrVNb)C ceramics—Part I:Phase decomposition induced by carbon content
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作者 Qingyi Kong rao zhang +5 位作者 Lei Chen Sijia Huo Wenyu Lu Yujin Wang Boxin Wei Yu Zhou 《Journal of Advanced Ceramics》 SCIE EI CAS CSCD 2024年第5期679-688,共10页
Phase decomposition can effectively enhance the mechanical properties of carbide ceramics and can overcome the difficulty of enhancing the mechanical properties of single-phase multicomponent carbide ceramics.In this ... Phase decomposition can effectively enhance the mechanical properties of carbide ceramics and can overcome the difficulty of enhancing the mechanical properties of single-phase multicomponent carbide ceramics.In this work,a series of nonstoichiometric(TiZrVNb)Cx ceramics were prepared by spark plasma sintering(SPS)at different temperatures.The effects of the carbon content on the phase composition,microstructure evolution,and mechanical properties were investigated in detail.Phase decomposition occurred with decreasing carbon content.Two different solid solutions of(Ti,V)-rich and Zr-rich phases formed from the decomposition of equimolar single-phase solid solutions,namely,the Zr-poor phase and Zr-rich phase,respectively.The distribution of Nb element is relatively uniform.The semicoherent interfaces between the Zr-poor phase and the Zr-rich phase can harden and strengthen effectively under the synergistic effect of grain refinement.Ceramics with phase decomposition structures have apparent advantages compared to single-phase high-entropy carbides.This work provides an important train of thought for the microstructure tailoring and properties optimization of multi-component carbide ceramics. 展开更多
关键词 multicomponent ceramics nontoichiometry microstructure evolution phase decomposition mechanical properties
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圆台-线栅型水平极化电磁脉冲模拟器的仿真分析
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作者 张饶 段艳涛 +4 位作者 扶庆枫 石立华 陈海林 胡南松 王大略 《建模与仿真》 2024年第3期2359-2366,共8页
以双锥–线栅型水平极化天线为原型,使用不同大小的圆柱体替换双锥的锥尖,设计出圆台–线栅型水平极化天线,并利用CST MWS电磁仿真软件计算了当激励源为双指数波时的两种天线结构的输出波形。将两种天线模型的输出波形分别与高空核电磁... 以双锥–线栅型水平极化天线为原型,使用不同大小的圆柱体替换双锥的锥尖,设计出圆台–线栅型水平极化天线,并利用CST MWS电磁仿真软件计算了当激励源为双指数波时的两种天线结构的输出波形。将两种天线模型的输出波形分别与高空核电磁脉冲标准波形进行对比,结果显示:圆台–线栅型水平极化天线模型的仿真结果在主要参数上更贴近高空核电磁脉冲标准波形,其中,输出波形的场强峰值提升了2.47%,上升沿(脉冲从峰值的10%到峰值的90%的时间宽度)误差由20.40%减小为0.04%,半高宽误差由8.26%减小为1.46%。 展开更多
关键词 圆台–线栅型 双锥–线栅型 水平极化天线 峰值 上升沿 半高宽
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Detecting anomalies in vector boson scattering 被引量:1
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作者 Jinmian Li Shuo Yang rao zhang 《Chinese Physics C》 SCIE CAS CSCD 2021年第7期51-64,共14页
Measuring vector boson scattering(VBS)precisely is an important step toward understanding the electroweak symmetry breaking of and detecting new physics beyond the standard model(SM).Herein,we propose a neural network... Measuring vector boson scattering(VBS)precisely is an important step toward understanding the electroweak symmetry breaking of and detecting new physics beyond the standard model(SM).Herein,we propose a neural network that compresses the features of the VBS data into a three-dimensional latent space.The consistency of the SM predictions and experimental data is tested via binned log-likelihood analysis in the latent space.We show that the network is capable of distinguishing different polarization modes of WWjj production in both di-and semileptonic channels.The method is also applied to constrain the effective field theory and two Higgs Doublet Model.The results demonstrate that the method is sensitive to general new physics contributing to the VBS. 展开更多
关键词 LHC electroweak symmetry breaking Higgs boson machine learning
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