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Facile construction of highly efficient MOF-based Pd@UiO-66-NH_(2)@ZnIn_(2)S_(4)flower-like nanocomposites for visible-light-driven photocatalytic hydrogen production 被引量:5
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作者 Mengting Cao Fengli Yang +5 位作者 Quan Zhang Juhua Zhang Lu Zhang lingfeng li Xiaohao Wang Wei-lin Dai 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2021年第17期189-199,共11页
Construction of metal-organic-frame works-based composite photocatalysts has attracted much attention for the reasonable band gap and high surface areas to improve the photocatalytic activity.In this study,the ternary... Construction of metal-organic-frame works-based composite photocatalysts has attracted much attention for the reasonable band gap and high surface areas to improve the photocatalytic activity.In this study,the ternary heterojunction Pd@UiO-66-NH_(2)@ZnIn_(2)S_(4)nanocomposites were facilely prepared for the first time by a two-step method.The visible-light-promoted hydrogen production rate of 0.3%Pd@UiO-66-NH_(2)@ZnIn_(2)S_(4)reaches up to 5.26 mmol g^(-1)h^(-1),which is evidently much higher than pure UiO-66-NH_(2),ZnIn_(2)S_(4)and binary UiO-66-NH_(2)/ZnIn_(2)S_(4)composites.Such a huge improvement in the photocatalytic performance is mainly attributed to the matched band gap of ZnIn_(2)S_(4)and UiO-66-NH_(2),and the introduction of Pd NPs into photocatalysts that broaden spectral response range and promote the photon induced charge carrier separation.This work may provide a feasible approach for the design and construction of metal-organic-frameworks-based photocatalytic materials. 展开更多
关键词 Metal-organic frameworks(MOFs) UiO-66-NH_(2) ZnIn_(2)S_4 Pd nanoparticles Photocatalytic hydrogen production
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Nanotube array-like WO_3/W photoanode fabricated by electrochemical anodization for photoelectrocatalytic overall water splitting 被引量:2
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作者 lingfeng li Xiaolong Zhao +1 位作者 Donglai Pan Guisheng li 《Chinese Journal of Catalysis》 CSCD 北大核心 2017年第12期2132-2140,共9页
Photoactive WO3is attractive as a photocatalyst for green energy evolution through water splitting.In the present work,an electrochemical anodic oxidation method was used to fabricate a photo‐responsive nanotube arra... Photoactive WO3is attractive as a photocatalyst for green energy evolution through water splitting.In the present work,an electrochemical anodic oxidation method was used to fabricate a photo‐responsive nanotube array‐like WO3/W(NA‐WO3/W)photoanode from W foil as a precursor.Compared with a reference commercial WO3/W electrode,the NA‐WO3/W photoanode exhibited enhanced and stable photoelectrocatalytic(PEC)activity for visible‐light‐driven water splitting with a typical H2/O2stoichiometric ratio of2:1and quantum efficiency of approximately5.23%under visible‐light irradiation from a light‐emitting diode(λ=420nm,15mW/cm2).The greatly enhanced PEC performance of the NA‐WO3/Wphotoanode was attributed to its fast electron–hole separation rate,which resulted from the one‐dimensional nanotube array‐like structure,high crystallinity of monoclinic WO3,and strong interaction between WO3and W foil.This work paves the way to a facile route to prepare highly active photoelectrodes for solar light transfer to chemical energy. 展开更多
关键词 WO3 W foil Electrochemical anodization Nanotube arrays PHOTOELECTROCATALYSIS Water splitting
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Doping effects and role conversion of CeO_(2)in 0.3PZN-0.7PZT ternary piezoelectric ceramics with enhanced electrical properties
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作者 Yu Chen lingfeng li +3 位作者 Le Mi Xingyu Wang Zhijun Wang Qingyuan Wang 《Journal of Rare Earths》 2025年第5期1035-1045,共11页
In this work,the rare-earth doped ternary lead zirconate titanate ceramics with chemical formula of[0.3 Pb(Zn_(1/3)Nb_(2/3))O_(3)-0.7Pb(Zr_(0.52)Ti_(0.48))O_(3)]+x wt%CeO_(2)(x=0-0.5,abbreviated as 0.3PZN-0.7PZT-xCe)w... In this work,the rare-earth doped ternary lead zirconate titanate ceramics with chemical formula of[0.3 Pb(Zn_(1/3)Nb_(2/3))O_(3)-0.7Pb(Zr_(0.52)Ti_(0.48))O_(3)]+x wt%CeO_(2)(x=0-0.5,abbreviated as 0.3PZN-0.7PZT-xCe)were synthesized by a conventional solid-state reaction route,specific attentions was focused on the effects of CeO_(2)dopants on the structures and electrical properties of the 0.3PZN-0.7PZT ceramics,revealing the role conve rsion of CeO_(2)dopants with its doping amount(x).When less CeO_(2)(x≤0.2)is introduced into 0.3PZN-0.7PZT,the prepared ceramics are identified as the coexistence of rhombohedral and tetragonal phases,also involved with an increased grain size and a reduced atomic ratio of Pb/(Zr+Ti+Zn+Nb).The increased remanent polarization(Pr)and deceased coercive filed(Ec),as well as improved dielectric permittivity(er)and piezoelectric coefficient(d_(33))de monstrate the donor substitution of Ce^(3+)for Pb^(2+)at the A-site of perovskite lattice.Conversely,the introduction of excessive CeO_(2)(x>0.2)causes a reversal evolution in the electrical properties of ceramics,suggesting that some of the introduced cerium element tends to become Ce4+,which equivalently substitutes for Zr^(4+)at the B-site.Additionally,the diffused phase transition(DPT)behaviors of the 0.3PZN-0.7PZT-xCe ceramics were investigated by the modified Curie-Weiss Law.The sample with x=0.2 shows reduced DPT character and optimized electrical properties,including TC=297℃,εr=1400,d_(33)=480 pC/N,tanδ=1.6%,kp=65%,d_(33)·g_(33)=16.32×10^(-12)m^(2)/N,Pr=38.3μC/cm^(2)and Ec=1.02 kV/mm.These enhanced electrical properties not only are contributed by the donor substitution effect of Ce^(3+),but also benefit from the optimized morphotropic phase boundary that is close to the tetragonal-rich side. 展开更多
关键词 PZN-PZT Ternary piezoelectric ceramics CeO_(2) Donor substitution Morphotropic phase boundary Rare earths
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Image encoding-based bearing fault diagnosis:Review and challenges for high-speed trains
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作者 Huimin li lingfeng li +1 位作者 Bin liu Ge Xin 《High-Speed Railway》 2025年第3期251-259,共9页
High-Speed Trains (HSTs) have emerged as a mainstream mode of transportation in China, owing to their exceptional safety and efficiency. Ensuring the reliable operation of HSTs is of paramount economic and societal im... High-Speed Trains (HSTs) have emerged as a mainstream mode of transportation in China, owing to their exceptional safety and efficiency. Ensuring the reliable operation of HSTs is of paramount economic and societal importance. As critical rotating mechanical components of the transmission system, bearings make their fault diagnosis a topic of extensive attention. This paper provides a systematic review of image encoding-based bearing fault diagnosis methods tailored to the condition monitoring of HSTs. First, it categorizes the image encoding techniques applied in the field of bearing fault diagnosis. Then, a review of state-of-the-art studies has been presented, encompassing both monomodal image conversion and multimodal image fusion approaches. Finally, it highlights current challenges and proposes future research directions to advance intelligent fault diagnosis in HSTs, aiming to provide a valuable reference for researchers and engineers in the field of intelligent operation and maintenance. 展开更多
关键词 High-speed trains Image encoding Fault diagnosis Rotating machinery Condition monitoring
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代谢工程改造L-半胱氨酸供给模块促地衣芽胞杆菌高效合成杆菌肽 被引量:1
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作者 李凌峰 刘佩 +7 位作者 罗文 王勤 王志 陈晓斌 李俊辉 蔡冬波 马昕 陈守文 《生物工程学报》 CAS CSCD 北大核心 2021年第8期2803-2812,共10页
杆菌肽是一种主要由芽胞杆菌产生的广谱性抗生素,目前作为兽药广泛应用于畜禽养殖领域。前体氨基酸供应不足可能是限制微生物发酵高产杆菌肽的重要因素。文中以杆菌肽工业生产菌株——地衣芽胞杆菌Bacillus licheniformis DW2为出发菌株... 杆菌肽是一种主要由芽胞杆菌产生的广谱性抗生素,目前作为兽药广泛应用于畜禽养殖领域。前体氨基酸供应不足可能是限制微生物发酵高产杆菌肽的重要因素。文中以杆菌肽工业生产菌株——地衣芽胞杆菌Bacillus licheniformis DW2为出发菌株,研究L-半胱氨酸供给模块强化对杆菌肽合成的影响。首先,构建了L-半胱氨酸合成酶基因cysK强化表达菌株,杆菌肽效价相比于对照菌株提高了9.47%。接着,为提高L-半胱氨酸合成前体供给,对L-丝氨酸乙酰转移酶基因cysE和硫代硫酸盐/硫酸盐胞内转运蛋白基因cysP进行强化,杆菌肽产量分别提高了7.23%和8.52%。随后,结果表明转运蛋白TcyP负责从胞外向胞内转运胱氨酸,强化表达TcyP后胞内L-半胱氨酸浓度和杆菌肽效价分别提高了29.19%和7.79%。通过组合代谢工程育种,在整合表达了基因cysK基础上,利用强启动子P_(bacA)分别替换基因cysP、cysE和tcyP原始启动子,得到工程菌株CYS4(DW2::cysK-P_(bacA)(cysP)-P_(bacA)(cysE)-P_(bacA)(tcyP)),杆菌肽效价达到910.02 U/mL,相比于出发菌株DW2(747.71 U/mL)提高了21.10%。最后,通过3 L发酵罐小试实验,进一步证实了强化L-半胱氨酸有利于杆菌肽合成。研究表明,强化胞内L-半胱氨酸供给水平是提高地衣芽胞杆菌中杆菌肽产量的有效策略,为杆菌肽工业生产提供了一株具有良好应用前景的菌株。 展开更多
关键词 地衣芽胞杆菌 杆菌肽 L-半胱氨酸供给 代谢工程
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A new energy-absorbing bolt used for large deformation control of tunnel surrounding rock 被引量:4
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作者 Junbao Wang Wei liu +3 位作者 Zhanping Song lingfeng li Shijin Feng Yun Cheng 《International Journal of Mining Science and Technology》 SCIE EI CAS CSCD 2022年第5期1031-1043,共13页
In order to control the large deformation of tunnel surrounding rock,a new energy-absorbing bolt is developed.This bolt can be transformed into a rigid support when the deformation of the surrounding rock reaches the ... In order to control the large deformation of tunnel surrounding rock,a new energy-absorbing bolt is developed.This bolt can be transformed into a rigid support when the deformation of the surrounding rock reaches the length of the sleeve tube,thus preventing the surrounding rock from continuing to deform.Moreover,this bolt has a simple structure and is easy to manufacture and assemble.Then the static tensile test is conducted on the bolt specimen to test its working performance.The test results show that when the cone angle of the cone block is small,the load–displacement curve of the bolt contains three stages;when the cone angle is large,the load–displacement curve contains only two stages.Meanwhile,both the average constant resistance and the maximum absorbed energy increase linearly with the increase of cone angle.On this basis,ignoring the influence of shear stress,and it is supposed that the thickness of the sleeve tube is constant,then the theoretical calculation formula of constant resistance for the new bolt is derived,and the rationality of the formula is verified using the static tensile test results.It is found that the error of the calculated result is less than 15%when the cone angle does not exceed 15.At last,the numerical simulation method is used to analyze the performance of the new bolt.The simulation results indicate that the generation of shear stress and the change of tube thickness during the movement of the cone block are two important factors that cause theoretical errors. 展开更多
关键词 Energy-absorbing bolt Static tensile test Cone angle Constant resistance Limit ring
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The dual role of casein kinase 1,DTG1,in regulating tillering and grain size in rice
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作者 Jijin li Dan Zhou +19 位作者 Deke li Gen Wang Rui Qin Chengqin Gong Kang Chen Yunqing Tong lingfeng li Keke liu Jiangkun Ye Binjiu Luo Chenglong Jiang Haipeng Wang Jinghua Jin Qiming Deng Shiquan Wang Jun Zhu Ting Zou Shuangcheng li Ping li Yueyang liang 《The Crop Journal》 SCIE CSCD 2024年第6期1569-1582,共14页
Tiller number and grain size are important agronomic traits that determine grain yield in rice.Here,we demonstrate that DEFECTIVE TILLER GROWTH 1(DTG1),a member of the casein kinase 1 protein family,exerts a co-regula... Tiller number and grain size are important agronomic traits that determine grain yield in rice.Here,we demonstrate that DEFECTIVE TILLER GROWTH 1(DTG1),a member of the casein kinase 1 protein family,exerts a co-regulatory effect on tiller number and grain size.We identified a single amino acid substitution in DTG1(I357K)that caused a decrease in tiller number and an increase in grain size in NIL-dtg1.Genetic analyses revealed that DTG1 plays a pivotal role in regulation of tillering and grain size.The DTG1^(I357K) allelic variant exhibited robust functionality in suppressing tillering.We show that DTG1 is preferentially expressed in tiller buds and young panicles,and negatively regulates grain size by restricting cell proliferation in spikelet hulls.We further confirm that DTG1 functioned in grain size regulation by directly interacting with Grain Width 2(GW2),a critical grain size regulator in rice.The CRISPR/Cas9-mediated elimination of DTG1 significantly enhanced tiller number and grain size,thereby increasing rice grain yield under field conditions,thus highlighting potential value of DTG1 in rice breeding. 展开更多
关键词 Oryza sativa Tiller number Grain size Casein kinase 1 DTG1
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Integrative analysis of cuproptosis-related lncRNAs:Unveiling prognostic significance,immune microenvironment,and copper-induced mechanisms in prostate cancer
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作者 Haitao Zhong Yiming Lai +10 位作者 Wenhao Ouyang Yunfang Yu Yongxin Wu Xinxin He Lexiang Zeng Xueen Qiu Peixian Chen lingfeng li Jie Zhou Tianlong Luo Hai Huang 《Cancer Pathogenesis and Therapy》 2025年第1期48-59,共12页
Background:Long non-coding ribonucleic acids(lncRNAs)regulate messenger RNA(mRNA)expression and influence cancer development and progression.Cuproptosis,a newly discovered form of cell death,plays an important role in... Background:Long non-coding ribonucleic acids(lncRNAs)regulate messenger RNA(mRNA)expression and influence cancer development and progression.Cuproptosis,a newly discovered form of cell death,plays an important role in cancer.Nonetheless,additional research investigating the association between cuproptosisrelated lncRNAs and prostate cancer(PCa)prognosis is required.Methods:Sequencing data and copy number variant data were obtained from 492 patients with PCa from The Cancer Genome Atlas(TCGA)Program.Prognostic models of PCa based on cuproptosis-related lncRNAs were constructed using a multi-level attention graph neural network(MLA-GNN)deep learning algorithm.Immune escape scoring was performed using Tumor Immune Dysfunction and Exclusion.Cellular experiments were conducted to explore the correlation between key lncRNAs and cuproptosis.Results:Data from 492 patients with PCa were randomized into two groups at a 1:1 ratio.Prognostic modeling was successfully established using MLA-GNN.Survival analysis suggested that patients could be divided into high-and low-risk groups according to model scores and that there was a significant difference in disease-free survival(DFS)(P<0.01).The area under the receiver operating characteristic(ROC)curve(AUC)indicated a strong predictive performance for the model,with AUCs of 0.913,0.847,and 0.863 for the training group and 0.815,0.907,and 0.866 for the test group at 12,36,and 60 months,respectively.The immune escape score and immune microenvironment analysis suggested that the high-risk group corresponded to a stronger immune escape and a poorer immune microenvironment(P<0.05).Cellular experiments revealed that the expression of all six key lncRNAs was upregulated in the presence of copper ion carriers(P<0.05).Conclusions:This study identified cuproptosis-related lncRNAs that were strongly associated with PCa prognosis.Key lncRNAs could affect copper metabolism and may serve as new therapeutic targets. 展开更多
关键词 Prostate cancer Cuproptosis Deep learning lncRNAs
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Electrospun Core-Shell Fibrous 2D Scaffold with Biocompatible Poly(Glycerol Sebacate) and Poly-l-Lactic Acid for Wound Healing 被引量:9
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作者 Xiaoping Yang lingfeng li +2 位作者 Dongzhi Yang Jun Nie Guiping Ma 《Advanced Fiber Materials》 CAS 2020年第2期105-117,共13页
Biomimetic scaffolds made by synthetic materials are usually used to replace the natural tissues aimed at speeding up the skin regeneration.In this study,a flexible and cytocompatible poly(glycerol sebacate)@poly-l-la... Biomimetic scaffolds made by synthetic materials are usually used to replace the natural tissues aimed at speeding up the skin regeneration.In this study,a flexible and cytocompatible poly(glycerol sebacate)@poly-l-lactic acid(PGS@PLLA)fibrous scaffold with a core-shell structure was fabricated by coaxial electrospinning,where the shell PLLA was used to be a skeleton with pores on the fibrous surface.The fibrous morphology with pores on the surface of the prepared fibers was observed by SEM.The core-shell microstructure of PGS@PLLA fibers was confirmed by TEM and Laser Scanning Confocal Microscopy(LSCM).In addition,the prepared fibers exhibited a strong ability to repair tissues of the skin wound,where the stability of cell security and proliferation,and the lower inflammatory response were all superior to those of pure PLLA scaffold.It’s worth noting that the percentage of skin tissue was regenerated by 95%within 14 days,which suggests the potential application for electrospun-based synthetic fibrous scaffolds on wound healing. 展开更多
关键词 Coaxial electrospinning Core-shell structure Porous PGS PLLA Wound healing
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Generalization Error Analysis of Neural Networks with Gradient Based Regularization
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作者 lingfeng li Xue-Cheng Tai Jiang Yang 《Communications in Computational Physics》 SCIE 2022年第9期1007-1038,共32页
In this work,we study gradient-based regularization methods for neural networks.We mainly focus on two regularization methods:the total variation and the Tikhonov regularization.Adding the regularization term to the t... In this work,we study gradient-based regularization methods for neural networks.We mainly focus on two regularization methods:the total variation and the Tikhonov regularization.Adding the regularization term to the training loss is equivalent to using neural networks to solve some variational problems,mostly in high dimensions in practical applications.We introduce a general framework to analyze the error between neural network solutions and true solutions to variational problems.The error consists of three parts:the approximation errors of neural networks,the quadrature errors of numerical integration,and the optimization error.We also apply the proposed framework to two-layer networks to derive a priori error estimate when the true solution belongs to the so-called Barron space.Moreover,we conduct some numerical experiments to show that neural networks can solve corresponding variational problems sufficiently well.The networks with gradient-based regularization are much more robust in image applications. 展开更多
关键词 Machine learning REGULARIZATION generalization error image classification
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A Level Set Representation Method for N-Dimensional Convex Shape and Applications
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作者 lingfeng li Shousheng Luo +1 位作者 Xue-Cheng Tai Jiang Yang 《Communications in Mathematical Research》 CSCD 2021年第2期180-208,共29页
In this work,we present a new method for convex shape representation,which is regardless of the dimension of the concerned objects,using level-set approaches.To the best of our knowledge,the proposed prior is the firs... In this work,we present a new method for convex shape representation,which is regardless of the dimension of the concerned objects,using level-set approaches.To the best of our knowledge,the proposed prior is the first one which can work for high dimensional objects.Convexity prior is very useful for object completion in computer vision.It is a very challenging task to represent high dimensional convex objects.In this paper,we first prove that the convexity of the considered object is equivalent to the convexity of the associated signed distance function.Then,the second order condition of convex functions is used to characterize the shape convexity equivalently.We apply this new method to two applications:object segmentation with convexity prior and convex hull problem(especially with outliers).For both applications,the involved problems can be written as a general optimization problem with three constraints.An algorithm based on the alternating direction method of multipliers is presented for the optimization problem.Numerical experiments are conducted to verify the effectiveness of the proposed representation method and algorithm. 展开更多
关键词 Convex shape prior level-set method image segmentation convex hull ADMM
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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 Antonio Racioppi Michael Ramsey‑Musolf Shabbar Raza Vladimir Rekovic Jing Ren Ju¨rgen 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 ASchmidt 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 Smiljanic 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 Sun 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 Tawfik 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》 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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Flavor physics at the CEPC:a general perspective
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作者 Xiaocong Ai Wolfgang Altmannshofer +148 位作者 Peter Athron Xiaozhi Bai Lorenzo Calibbi Lu Cao Yuzhi Che Chunhui Chen Ji-Yuan Chen Long Chen Mingshui Chen Shanzhen Chen Xuan Chen Shan Cheng Cheng-Wei Chiang Andreas Crivellin Hanhua Cui Olivier Deschamps Sébastien Descotes-Genon Xiaokang Du Shuangshi Fang Yu Gao Yuanning Gao li-Sheng Geng Pablo Goldenzweig Jiayin Gu Feng-Kun Guo Yuchen Guo Zhi-Hui Guo Tao Han Hong-Jian He Jibo He Miao He Xiaogang He Yanping Huang Gino Isidori Quan Ji Jianfeng Jiang Xu-Hui Jiang Jernej F.Kamenik Tsz Hong Kwok Gang li Geng li Haibo li Haitao li Hengne li Honglei li liang li lingfeng li Qiang li Qiang li Shu li Xiaomei li Xin-Qiang li Yiming li Yubo li Yuji li Zhao li Hao liang Zhijun liang libo liao Zoltan ligeti Jia liu Jianbei liu Tao liu Yi liu Yong liu Zhen liu Xinchou Lou Peng-Cheng Lu Alberto Lusiani Hong-Hao Ma Kai Ma Farvah Mahmoudi Yajun Mao Yaxian Mao David Marzocca Juan-Juan Niu Soeren Prell Huirong Qi Sen Qian Zhuoni Qian Qin Qin Ariel Rock Jonathan L.Rosner Manqi Ruan Dingyu Shao Chengping Shen Xiaoyan Shen Haoyu Shi liaoshan Shi Zong-Guo Si Cristian Sierra Huayang Song Shufang Su Wei Su Zhijia Sun Michele Tammaro Dayong Wang En Wang Fei Wang Hengyu Wang Jian Wang Jianchun Wang Kun Wang lian-Tao Wang Wei Wang Xiaolong Wang Xiaoping Wang Yadi Wang Yifang Wang Yuexin Wang Xing-Gang Wu Yongcheng Wu Rui-Qing Xiao Ke-Pan Xie Yuehong Xie Zijun Xu Haijun Yang Hongtao Yang lin Yang Shuo Yang Zhongbao Yin Fusheng Yu Changzheng Yuan Xing-Bo Yuan Xuhao Yuan Chongxing Yue Xi-Jie Zhan Hong-Hao Zhang Kaili Zhang liming Zhang Xiaoming Zhang Yang Zhang Yanxi Zhang Ying Zhang Yongchao Zhang Yu Zhang Zhen-Hua Zhang Zhong Zhang Mingrui Zhao Qiang Zhao Xu-Chang Zheng Yangheng Zheng Chen Zhou Daicui Zhou Pengxuan Zhu Yongfeng Zhu Xuai Zhuang Xunwu Zuo Jure Zupan 《Chinese Physics C》 2025年第10期25-80,共56页
We discuss the landscape of flavor physics at the Circular Electron-Positron Collider(CEPC),based on the nominal luminosity outlined in its Technical Design Report.The CEPC is designed to operate in multiple modes to ... We discuss the landscape of flavor physics at the Circular Electron-Positron Collider(CEPC),based on the nominal luminosity outlined in its Technical Design Report.The CEPC is designed to operate in multiple modes to address a variety of tasks.At the Z pole,the expected production of 4 Tera Z bosons will provide unique and highly precise measurements of Z boson couplings,while the substantial number of boosted heavy-flavored quarks and leptons produced in clean Z decays will facilitate investigations into their flavor physics with unprecedented precision.We investigate the prospects of measuring various physics benchmarks and discuss their implications for particle theories and phenomenological models.Our studies indicate that,with its highlighted advantages and anticipated excellent detector performance,the CEPC can explore beauty andτphysics in ways that are superior to or complementary with the Belle II and Large-Hadron-Collider-beauty experiments,potentially enabling the detection of new physics at energy scales of 10 TeV and above.This potential also extends to the observation of yet-to-be-discovered rare and exotic processes,as well as testing fundamental principles such as lepton flavor universality,lepton and baryon number conservation,etc.,making the CEPC a vibrant platform for flavor physics research.The WW threshold scan,Higgs-factory operation and top-pair productions of the CEPC further enhance its merits in this regard,especially for measuring the Cabibbo-Kobayashi-Maskawa matrix elements,and Flavor-Changing-NeutralCurrent physics of Higgs boson and top quarks.We outline the requirements for detector performance and considerations for future development to achieve the anticipated scientific goals.The role of machine learning for innovative detector design and advanced reconstruction algorithms is also stressed.The CEPC flavor physics program not only develops new capabilities for exploring flavor physics beyond existing projects but also enriches the physics opportunities of this machine.It should be remarked that,given the richness of the CEPC flavor physics,this manuscript is not meant to be a comprehensive survey,but rather an investigation of representative cases.Uncovering the full potential of flavor physics at the CEPC will require further dedicated explorations in the future. 展开更多
关键词 flavor physics future collider CEPC
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La_(2)O_(3)-modified BiYbO_(3)–Pb(Zr,Ti)O_(3) ternary piezoelectric ceramics with enhanced electrical properties and thermal depolarization temperature 被引量:7
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作者 Yu Chen lingfeng li +3 位作者 Zhi Zhou Yiying Wang Qiang Chen Qingyuan Wang 《Journal of Advanced Ceramics》 SCIE EI CAS CSCD 2023年第8期1593-1611,共19页
High-performance Pb(Zr_(1−x)Ti_(x))O_(3)(PZT)piezoceramics are urgently desired by the market in view of their expanded operating temperature range,reduced property temperature dependence,and enhanced sensitivity and ... High-performance Pb(Zr_(1−x)Ti_(x))O_(3)(PZT)piezoceramics are urgently desired by the market in view of their expanded operating temperature range,reduced property temperature dependence,and enhanced sensitivity and acoustic power.In this work,we reported a kind of low-cost and high-performance 0.06BiYbO_(3)–0.94Pb(Zr_(0.48)Ti_(0.52))O_(3) ternary piezoceramics;the modifying effects of La_(2)O_(3) on this perovskite system were investigated in terms of the structures,electrical properties,and thermal depolarization behaviors of ceramics.The field-dependent dielectric and conduction properties indicated that there are close correlations among oxygen vacancies(VO),conducting electrons,and intrinsic conduction process.The degradation in ferroelectric properties observed in those samples doped with more than 0.15 wt%of La_(2)O_(3) indicated that the occupying mechanisms of La^(3+)changed from the donor substitution for Pb^(2+)to the isovalent substitution for Bi^(3+).The thermally depoling micromechanisms of ceramics were revealed from the thermodynamic processes of defect dipoles and intrinsic dipoles within ferroelectric domains.The sample doped with 0.15 wt%of La_(2)O_(3) shows excellent electrical properties with TC=387℃,d33=332 pC/N,TKε=5.81×10^(−3)℃−1,Pr=20.66μC/cm^(2),Td=356℃.The significantly enhanced electrical properties and thermal depolarization temperature benefited from the donor substitution of La3+,decreasing the oxygen vacancy concentration in the lattice and possibly optimizing the ferroelectric domain structure of ceramics. 展开更多
关键词 BiYbO_(3)-Pb(Zr_(1−x)Ti_(x))O_(3)(BY-PZT)piezoceramics La_(2)O_(3) ferroelectric domain switching(Sswitch) defect dipoles thermal depolarization behaviors
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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 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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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Synergistically enhancing the piezoelectric activity and Curietemperature of CaBi_(4)Ti_(4)O_(15) ceramics via co-doping Gd/Mn at theA/B-site
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作者 Yu Chen Zhi Zhou +2 位作者 lingfeng li Daowen Wu Qingyuan Wang 《Journal of Advanced Ceramics》 SCIE EI CAS CSCD 2024年第9期1482-1497,共16页
As a typical Aurivillius-type compound, CaBi_(4)Ti_(4)O_(15) (CBT) is considered a strong competitor among hightemperature piezoelectric materials, but it is difficult to achieve both high piezoelectric activity and a... As a typical Aurivillius-type compound, CaBi_(4)Ti_(4)O_(15) (CBT) is considered a strong competitor among hightemperature piezoelectric materials, but it is difficult to achieve both high piezoelectric activity and a high Curie temperaturefor CBT. In this work, the method of double-ion co-substituting at different crystalline sites was used to modify the electricalproperties of CBT. The Gd/Mn co-doped CBT ceramics with the chemical formula of Ca_(1−x)Gd_(x)Bi_(4)Ti_(4)O_(15)+0.2 wt% MnO_(2)(CBT–100xGM, x = 0–0.11) were prepared via the conventional sintering process. The phase and valence band structures,chemical compositions and microstructures, dielectric and ferroelectric properties, electrical conduction behaviors, andelectroelastic and piezoelectric properties of the ceramics were characterized. The doping concentration effects of Gd^(3+)were analyzed according to the composition-dependent structures and properties of CBT–100xGM. The donor substitutionof Gd^(3+) for Ca^(2+) at the A-site reduced the tolerance factor of the perovskite-like structure and decreased the concentration ofintrinsic oxygen vacancies. While Mn^(3+) tended to substitute for Ti4+ at the B-site, the extrinsic oxygen vacancies are limitednear the defect center of Ti(Mn) because of the formation of ( ‒MnTi')• as defect dipoles. The thermal depoling behavior ofthe CBT–100xGM ceramics between 300 and 700 ℃ was explained by the thermodynamic characteristics of the defectdipoles. The optimized composition with x = 0.08 (CBT–8GM) had a high TC ≈ 809 ℃ and a high piezoelectric coefficient(d33) ≈ 23 pC/N, as well as a piezoelectric voltage constant (g33) value of up to 21.5×10^(−3)(V·m)/N. Moreover, it can maintaina residual d33 ≈ 80% after being annealed at 700 ℃. This good anti-thermal depoling ability endows this material with greatapplication potential in high-temperature piezoelectric devices with operating temperatures exceeding 500 ℃. Thesynergistic enhancement in the piezoelectric activity and Curie temperature of CBT can be attributed mainly to the donorsubstituting effect of Gd^(3+) at the A-site, as well as the decreased elastic compliance contributed by MnO_(2) as the B-sitedopant. 展开更多
关键词 Aurivillius-type compounds CaBi_(4)Ti_(4)O_(15) double-ion substitution oxygen vacancy radial vibration mode electrical conduction behavior
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Enhancing the dielectric and piezoelectric properties of Pb_(0.99)Gd_(0.01)Zr_(0.53)Ti_(0.47)O_(3) ferroelectric ceramics by Sr-doping
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作者 Xingyu Wang lingfeng li Yu Chen 《Journal of Advanced Dielectrics》 2024年第4期71-79,共9页
Recently,high-performance lead zirconate titanate(Pb(Zr_(1-x)Ti_(x))O_(3),PZT)ferroelectric ceramics have attracted intensive attention due to their wider operating temperature range,better temperature stability,as we... Recently,high-performance lead zirconate titanate(Pb(Zr_(1-x)Ti_(x))O_(3),PZT)ferroelectric ceramics have attracted intensive attention due to their wider operating temperature range,better temperature stability,as well as larger piezoelectric properties and higher energy conversion efficiency.In this study,the perovskite-type ferroelectric ceramics with a chemical formula of Pb_(0.99-x)Gd_(0.01)Sr_(x)Zr_(0.53)Ti_(0.47)O_(3)(x=0 and 0.02,abbr.PGZT and PGSZT,respectively)were prepared by the traditional solid-state reaction route.The influences of Sr-doping on the phase structure,dielectric properties,ferroelectric properties and piezoelectric properties of the PGZT ceramics were comprehensively investigated.The field-dependent P–E hysteresis loops of PGSZT were measured in the frequency range of 0.05–10 Hz and temperature range of 20–100℃.The results show that Sr-doping not only enhances the dielectric permittivity and piezoelectric coefficient of PGZT,but also decreases its dielectric loss tangent,with the d_(33) value of 473 pC/N,ε_(r) value of 1586 and tanδvalue of 0.016 found in PGSZT.Also,PGSZT shows a high Curie temperature(T_(C))of 350℃.The underlying mechanisms of the property enhancement were identified as that the introduced Sr^(2+) replaces the volatile Pb^(2+) located at the A-site of the perovskite structure,thereby reducing the concentration of lead vacancies and promoting the grain growth of the ceramics,consequently enhancing the dielectric and piezoelectric properties of PGZT.On the other hand,the frequency change in the low-frequency range(<1 Hz)played a significant impact on the remanent polarization(P_(r))and internal biased electric field(E_(i))of PGSZT,but the frequency dependence of coercive field(E_(c))tends to diminish in the high-frequency range(≥1 Hz). 展开更多
关键词 Pb(Zr_(1-x)Ti_(x))O_(3) Sr-doping dielectric properties piezoelectric properties ferroelectric ceramics
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New physics search at the CEPC:a general perspective
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作者 Xiaocong Ai Stefan Antusch +212 位作者 Peter Athron Yunxiang Bai Shou-Shan Bao Daniele Barducci Xiao-Jun Bi Tianji Cai Lorenzo Calibbi Junsong Cang Junjie Cao Wei Chao Boping Chen Gang Chen Long Chen Mingshui Chen Shanzhen Chen Xiang Chen Huajie Cheng Huitong Cheng Yaodong Cheng Kingman Cheung Min-Huan Chu João Barreiro Guimarães da Costa Xinchen Dai Arindam Das Zhi-fu Deng Frank F.Deppisch P.S.Bhupal Dev Yabo Dong Marco Drewes Xiaokang Du Yong Du Jun Fan Yaquan Fang Cunfeng Feng Andrew Fowlie Hao-fei Gao Jie Gao lin-Qing Gao Meisen Gao Yu Gao Yuanning Gao Bruce Mellado Garcia Shao-Feng Ge Ti Gong Jiayin Gu Lei Guo Pei-Hong Gu Yu-Chen Guo Zhi-Hui Guo Jan Hajer Rabia Hameed Chengcheng Han Shuo Han Tao Han Xiqing Hao Hong-Jian He Xiaogang He Yangle He Sven Heinemeyer Zhaoxia Heng Xiao-Hui Hu Fa Peng Huang Fei Huang Yanping Huang Jianfeng Jiang Xu-Hui Jiang Hong-Bo Jin Mingjie Jin Shan Jin Wenyi Jin Mussawir Khan Honglei li Jiarong li Jinmian li liang li lingfeng li Qiang li Shu li Tianjun li Tong li Weidong li Xin-Qiang li Ying li Yuhui li Zhao li Shiyi liang Zhijun liang Chengxin liao Hongbo liao Jiajun liao Hai lin Bo liu Hang liu Jia liu Jianbei liu Jianglai liu Tao liu Wei liu Yang liu Zhaofeng liu Zhen liu Zuowei liu Xinchou Lou Chih-Ting Lu Feng Lyu Kai Ma lianliang Ma Farvah Mahmoudi Sanjoy Mandal Yajun Mao Ying-nan Mao Manimala Mitra Roberto A.Morales Michael Ramsey-Musolf Miha Nemevšek Takaaki Nomura C.J.Ouseph Yusi Pan Junle Pei Fazhi Qi Huirong Qi Zan Ren Craig D.Roberts Manqi Ruan liangliang Shang Dingyu Shao Yue-Long Shen Yu-Ji Shi Sujay Shil Huayang Song Shufang Su Wei Su Hao Sun Xiaohu Sun Zheng Sun Zhijia Sun Jin-Xin Tan Van Que Tran Bin Wang Dayong Wang En Wang Fei Wang Guang-Yu Wang Hengyu Wang Jianchun Wang Jin Wang Jin-Wei Wang Kechen Wang Kun Wang Sai Wang Wei Wang Wenyu Wang Xiao-Ping Wang Yi Wang Yifang Wang You-kai Wang Yuexin Wang Yu-Ming Wang Zeren Simon Wang Zheng Wang Lei Wu Peiwen Wu Yongcheng Wu Yusheng Wu Guotao Xia ligang Xia Rui-Qing Xiao Ke-Pan Xie Ye Xing Zhi-zhong Xing Da Xu Fang Xu Ji Xu Bin Yan Qi Yan Haijun Yang Jin-Min Yang Shuo Yang Jingbo Ye Peng-Fei Yin Zhengyun You Zhao-Huan Yu Jiarong Yuan Xing-Bo Yuan Chongxing Yue Yuanfang Yue Jun Zeng Hao Zhang Hong Zhang Hong-Hao Zhang Huaqiao Zhang Kaili Zhang Mengchao Zhang Mu-Hua Zhang Qi-An Zhang Xinmin Zhang Yang Zhang Ying Zhang Yongchao Zhang Yu Zhang Yu Zhang Qiang Zhao Shuai Zhao Chen Zhou Haijing Zhou Ye-ling Zhou Bin Zhu Jingya Zhu Jing-Yu Zhu Pengxuan Zhu Qianteng Zhu Rui Zhu Xuai Zhuang 《Chinese Physics C》 2025年第12期101-208,共108页
I.EXECUTIVE SUMMARY next-generation,high-intensity electron-positron collider"Higgs factory",such as the Circular Electron-Positron Collider(CEPC),is among the highest priorities for the global high-energy c... I.EXECUTIVE SUMMARY next-generation,high-intensity electron-positron collider"Higgs factory",such as the Circular Electron-Positron Collider(CEPC),is among the highest priorities for the global high-energy collider physics community.The CEPC can provide unprecedented opportunities for making fundamental discoveries and providing decisive insights in the quest for a"New Standard Model(SM)"of nature's fundamental interactions.The CEPC could:·Identify the origin of matter,especially the mechanism related to the first-order phase transition in the early Universe,which could produce a detectable gravitational wave signal. 展开更多
关键词 new standard model high intensity electron positron collider higgs factory CEPC circular electron positron collider origin matterespecially next generation origin matter
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