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退火条件对山梨醇玻璃焓松弛参数的影响

物理化学学报 2011年第5期27卷 1031-1038页

作者：叶斌高才刘向农杨锁江斌合肥工业大学机械与汽车工程学院合肥230009

采用差示扫描量热法(DSC)测定山梨醇样品经历不同时间(ta)等温退火后,以10K·min-1速率进行升温时玻璃化转变温度(Tg)前后的比热容(Cp(T)).将Gómez Ribelles(GR)提出的一种基于构型熵的现象学模型用于描述山梨醇玻璃的焓松弛行为,考察G... 详细信息

采用差示扫描量热法(DSC)测定山梨醇样品经历不同时间(ta)等温退火后,以10K·min-1速率进行升温时玻璃化转变温度(Tg)前后的比热容(Cp(T)).将Gómez Ribelles(GR)提出的一种基于构型熵的现象学模型用于描述山梨醇玻璃的焓松弛行为,考察GR模型能否适用于小分子玻璃体系.结果表明,单组GR模型参数拟合的曲线均能较好重现对应热历史条件下的山梨醇体系的实验所得Cp(T)曲线,尽管并未找到不随热历史而变的一组参数作为材料常数,但与其它现象学模型应用于小分子玻璃时,其模型参数都随热历史变化而变化的特点相比,GR模型的某些参数基本保持不变.且在较长退火时间下拟合得到的模型参数普适性较好.同经历连续降温的山梨醇相比,等温退火过程得到的松弛极限态参数(δ)的平均值与Tg处比热容增量(ΔCp(Tg))的比值明显增大,但仍小于聚合物的值,表明GR模型提出的亚稳极限态对小分子玻璃的影响值得商榷.

关键词：焓松弛差示扫描量热法构型熵山梨醇玻璃化转变等温退火脆度

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木糖醇玻璃焓松弛的量热分析

物理化学学报 2010年第1期26卷 7-12页

作者：高才杨锁刘向农王铁军江斌合肥工业大学机械与汽车工程学院合肥230009

为了考察木糖醇的玻璃化转变和焓松弛行为,寻求碳链长度对线性多元醇玻璃化转变和焓松弛行为的影响,利用差示扫描量热(DSC)技术测定了不同降温速率下木糖醇在玻璃化转变温度(Tg)前后的比热容(Cp),通过曲线拟合获得了TNM(Tool-Narayanasw... 详细信息

为了考察木糖醇的玻璃化转变和焓松弛行为,寻求碳链长度对线性多元醇玻璃化转变和焓松弛行为的影响,利用差示扫描量热(DSC)技术测定了不同降温速率下木糖醇在玻璃化转变温度(Tg)前后的比热容(Cp),通过曲线拟合获得了TNM(Tool-Narayanaswamy-Moynihan)模型参数,并和其他多元醇类已有研究结果进行对照.结果表明,尽管TNM模型可以很好地重现不同降温速率体系的实验比热容数据,但模型参数并不是材料常数,而是和热历史有关,不同的降温速率对应不同的模型参数.指前因子(A)、非线性参数(x)和非指数参数(β)均随着降温速率的增加而降低,松弛活化焓(△h*)的变化趋势刚好相反.几种线性多元醇玻璃化转变和TNM模型参数的对照表明,玻璃化转变温度,松弛活化焓和动力学脆度(m)都随着烷基碳链长度的增加而增加.虽然非线性参数、非指数参数随碳链长度的增加有降低的趋势,但木糖醇展现出反常变化的情形.

关键词：差示扫描量热法木糖醇玻璃化转变焓松弛 Tool-Narayanaswamy-Moynihan模型

1H NMR研究溶质浓度对三碳多元醇水溶液氢键作用以及玻璃化的影响

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物理化学学报 2011年第11期27卷 2505-2511页

作者：叶斌高才赵韩陈开松杨锁刘向农合肥工业大学机械与汽车学院合肥230009

为考察溶质浓度对三碳多元醇水溶液氢键作用以及不同物质玻璃态形成能力的影响,采用~1H NMR外标法研究不同浓度的1-丙醇（NPA）,2-丙醇（IPA）,1,2-丙二醇（PG）,1,3-丙二醇（PD）和丙三醇（glycerol）的水溶液在室温常压下质子化学位移... 详细信息

为考察溶质浓度对三碳多元醇水溶液氢键作用以及不同物质玻璃态形成能力的影响,采用~1H NMR外标法研究不同浓度的1-丙醇（NPA）,2-丙醇（IPA）,1,2-丙二醇（PG）,1,3-丙二醇（PD）和丙三醇（glycerol）的水溶液在室温常压下质子化学位移.结果表明：具有CH_3CH（OH）一基团的PG烷基质子的化学位移变化趋势与其他几种醇相比有较大差异.醇羟基质子与水分子的氧形成较强O-H…O氢键.相同摩尔分数下,羟基数的增加导致水质子和羟基质子的化学位移降低,而且羟基位置不同也会导致水质子和羟基质子化学位移差异.这几种三碳多元醇碱性强弱的顺序和降低冰的均相成核温度能力的顺序一致,即glycerol〉PG〉PD〉IPA〉NPA,~1H NMR技术表明glycerol和PG更适合用作低温保护剂.

关键词： HNMR 三碳多元醇水溶液低温保护剂质子化学位移氢键

基于位形熵模型的山梨醇玻璃焓松弛的量热分析

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化学学报 2011年第1期69卷 37-45页

作者：高才陈开松叶斌杨锁刘向农江斌合肥工业大学机械与汽车工程学院合肥230009

利用DSC技术考察了无定形山梨醇体系的焓松弛行为,在10 K?min-1的升温速率下测定了经历不同降温速率(0.5～20 K?min-1)的山梨醇在玻璃化转变(Tg)前后的比热容[cp(T)].利用基于位形熵演变的焓松弛现象学模型(GR模型)模拟了实验数据.不论... 详细信息

利用DSC技术考察了无定形山梨醇体系的焓松弛行为,在10 K?min-1的升温速率下测定了经历不同降温速率(0.5～20 K?min-1)的山梨醇在玻璃化转变(Tg)前后的比热容[cp(T)].利用基于位形熵演变的焓松弛现象学模型(GR模型)模拟了实验数据.不论是否假设松弛过程存在一个亚稳极限态,模型参数均能很好地重现经历不同热历史体系的升温cp(T)曲线.在物理意义明确的模型参数组中,除了非指数参数随降温速率的增加而增加外,其余均不随热历史的变化而变化.拟合较低降温速率下cp(T)曲线获得的GR模型参数的预测力明显好于在较大降温速率下获得的结果.由于松弛时间对拟合过程中选择的"固定参数"的取值很敏感,因此模型能否预测体系的比热容不能看成确定松弛时间的唯一依据.在利用GR模型分析无定形山梨醇体系的脆度时,如果选择极限假想温度作为Tg,会导致计算结果明显小于文献值.

关键词：焓松弛位形熵玻璃化转变脆度山梨醇差示扫描量热法

Measurement of the ^(232)Th(n,f)cross section in the 1-200 MeV range at the CSNS Back-n

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Nuclear Science and Techniques 2023年第8期34卷 142-153页

作者： Zhi-Zhou Ren Yi-Wei yang Yong-Hao Chen Rong liu Bang-Jiao ye Jie Wen Hai-Rui Guo Zi-Jie Han Qi-Ping Chen Zhong-Wei Wen Wei-Li Sun Han Yi Xing-Yan liu Tao ye jiang-Bo Bai Qi An Jie Bao Yu Bao Ping Cao Hao-Lei Chen Zhen Chen Zeng-Qi Cui Rui-Rui Fan Chang-Qing Feng Ke-Qing gao Xiao-Long gao Min-Hao Gu Chang-cai Han Guo-Zhu He Yong-Cheng He yang Hong Yi-Wei Hu Han-Xiong Huang Xi-Ru Huang Hao-Yu jiang Wei jiang Zhi-Jie jiang Han-Tao Jing Ling Kang Bo Li Chao Li Jia-Wen Li Qiang Li Xiao Li yang Li Jie liu Shu-bin liu Ze Long Guang-Yuan Luan Chang-Jun Ning Meng-Chen Niu bin-bin Qi Jie Ren Xi-Chao Ruan Zhao-Hui Song Kang Sun Zhi-Jia Sun Zhi-Xin Tan Jing-Yu Tang Xin-Yi Tang bin-bin Tian Li-Jiao Wang Peng-Cheng Wang Zhao-Hui Wang Xiao-Guang Wu Xuan Wu Li-Kun Xie Xiao-Yun yang Li Yu Tao Yu Yong-Ji Yu Guo-Hui Zhang Lin-Hao Zhang Qi-Wei Zhang Xian-Peng Zhang Yu-Liang Zhang Zhi-Yong Zhang Lu-Ping Zhou Zhi-Hao Zhou Ke-Jun Zhu Department of Modern Physics University of Science and Technology of ChinaHefei 230026China Institute of Nuclear Physics and Chemistry China Academy of Engineering PhysicsMianyang 621900China Institute of High Energy Physics Chinese Academy of Sciences(CAS)Beijing 100049China Spallation Neutron Source Science Center Dongguan 523803China Institute of Applied Physics and Computational Mathematics Beijing 100088China State Key Laboratory of Particle Detection and Electronics University of Science and Technology of ChinaHefei 230027China Key Laboratory of Nuclear Data China Institute of Atomic EnergyBeijing 102413China School of Nuclear Science and Technology University of Science and Technology of ChinaHefei 230027China State Key Laboratory of Nuclear Physics and Technology School of PhysicsPeking UniversityBeijing 100871China State Key Laboratory of Particle Detection and Electronics Institute of High Energy PhysicsChinese Academy of SciencesBeijingChina Northwest Institute of Nuclear Technology Xi’an 710024China University of Chinese Academy of Sciences Beijing 100049China Department of Engineering and Applied Physics University of Science and Technology of ChinaHefei 230026China

The ^(232)Th(n,f)cross section is very important in basic nuclear physics and applications based on the Th/U fuel *** the time-of-flight method and a multi-cell fast-fission ionization chamber,a novel measurement of the^(232)Th(n,f)cross sec-tion relative to^(235)U in the 1–200 MeV range was performed at the China Spallation Neutron Source Back-n white neutron source(Back-n).The fission event-neutron energy spectra of^(232)Th and^(235)U fission cells were measured in the single-bunch *** 232Th/235U fission cross-sectional ratios were obtained,and the measurement uncertainties were 2.5–3.7%for energies in the 2–20 MeV range and 3.6–6.2%for energies in the 20–200 MeV ***^(232)Th(n,f)cross section was obtained by introducing the standard cross section of^(235)U(n,f).The results were compared with those of previous theoreti-cal calculations,measurements,and *** measured 232Th fission cross section agreed with the main evaluation results in terms of the experimental uncertainty,and 232Th fission resonances were observed in the 1–3 MeV *** present results provide^(232)Th(n,f)cross-sectional data for the evaluation and design of Th/U cycle nuclear systems.

关键词： 232Th(n f)cross section Fast-fission ionization chamber Back-n white neutron source

莴笋-空心菜-莴笋种植模式下不同改良剂对退化土壤中植株养分利用的影响

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草业学报 2016年第7期25卷 148-157页

作者：黄容高明叶夏伊汪文强刘彬彬刘江代文才西南大学资源环境学院重庆400715

在退化土壤中添加不同改良剂,通过莴笋-空心菜-莴笋的盆栽试验,对比分析了6种改良剂对蔬菜产量、品质、养分的影响,以期为评价改良剂对退化土壤中的植株养分的利用效果提供科学依据。结果表明,1）不同改良剂处理能有效提高蔬菜产量,其... 详细信息

在退化土壤中添加不同改良剂,通过莴笋-空心菜-莴笋的盆栽试验,对比分析了6种改良剂对蔬菜产量、品质、养分的影响,以期为评价改良剂对退化土壤中的植株养分的利用效果提供科学依据。结果表明,1）不同改良剂处理能有效提高蔬菜产量,其中化肥配施生物质灰渣（NPKH）和化肥配施生物肥（NPKW）处理的蔬菜产量增幅最大。2）各处理较CK提高了蔬菜体内NO3--N含量,本试验中莴笋的硝酸盐含量符合GB/T15401规定,未对莴笋品质产生不利影响;而化肥配施改良剂比单施化肥（NPK）有利于降低莴笋中NO3--N含量,以NPKW处理最佳,较NPK处理下降了7.8%~63.0%。与单施化肥相比,NPKH处理提高了蔬菜氨基酸含量,降低了硝酸盐含量,提高了氮肥表观利用率。3）NPKH处理的肥料农学利用率较高,可以有效提高莴笋中全磷、全钾含量,其中全钾含量较CK显著提高了43.4%~58.9%;NPKH和NPKW处理在空心菜种植期间,对氮肥、磷肥、钾肥的农学利用率较高,提高了空心菜对全氮、全磷、全钾营养元素的吸收量。研究表明化肥配施改良剂,特别是化肥配施生物质灰渣或生物肥可以提高蔬菜养分利用率,增加产量的同时降低硝酸盐的累积。

关键词：改良剂生物质灰渣退化土壤作物养分

Anatomical variation of infra-pyloric artery origination： A prospective multicenter observational study (IPA-Origin)

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Chinese Journal of Cancer Research 2018年第5期30卷 500-507页

作者： Rulin Miao Jianjun Qu Zhengrong Li Daguang Wang jiang Yu Weidong Zang Yong Li Fenglin liu Jian Zhang Wu Song Kai ye Su Yan Wei Wang Shuangyi Ren Lu Zang Changqing Jing Li Zhang Kuan Wang Weihua Fu Lin Fan bin Liang Gang Zhao Jun cai Li yang Jiaming Zhu Jun You Kun yang Qingxing Huang Zhaojian Niu Ning Ning Xingfeng Qiu Gang Ji Feng Liang Hua Huang Chao gao Fei Shan Shuangxi Li Yongning Jia Lianhai Zhang xiangji Ying Yan Zhang Zhaode Bu xiangqian Su Gang Zhao Ziyu Li Jiafu Ji Key Laboratory of Carcinogenesis and Translational Research (Ministry of Education/Beijing) Gastrointestinal Cancer Center Peking University Cancer Hospital & Institute Beijing 100142 China Department of Surgical Oncology Weifang People's Hospital Weifang 261000 China Department of General Surgery the First Affiliated Hospital of Nanchang University Nanchang 330006 China Department of Gastrointestinal Surgery the First Hospital of Jilin University Changehun 130021 China Department of General Surgery Nanfang Hospital Southern Medical University Guangzhou 510515 China Department of Gastrointestinal Cancer Surgery Fujian Provincial Cancer Hospital Fuzhou 350014 China Department of General Surgery Guangdong General Hospital Guangdong Academy of Medical Sciences Guangzhou 510080 China Department of General Surgery Zhongshan Hospital Fudan University Shanghai 200032 China Department of Gastrointestinal Surgery Hangzhou First People's Hospital Hangzhou 310006 China Department of Gastrointestinal Surgery the First Affiliated Hospital Sun Yat-sen University Guangzhou 510080 China Department of Surgical Oncology the Second Affiliated Hospital of Fujian Medical University Quanzhou 362000 China Department of Surgical Oncology Affiliated Hospital of Qinghai University Xining 810001 China Department of Gastrointestinal Surgery Guangdong Provincial Hospital of Chinese Medicine Guangzhou 510120 China Department of General Surgery the Second Hospital of Dalian Medical University Dalian 116023 China Department of General Surgery Shanghai Ruijin Hospital Shanghai Jiaotong University School of Medicine Shanghai 200025 China Department of Gastrointestinal Surgery Shandong Provincial Hospital Affiliated to Shandong University Jinan 250021 China Department of Gastrointestinal Surgery Harbin Medical University Cancer Hospital Harbin 150081 China Department of General Surgery Tianjin Medical University General Hospital Tianjin 300052 China Department of General Surgery the Firs

Objective： Infra-pyloric artery （IPA） is an important anatomical landmark in treatment of gastric cancer and is the key vessel for pylorus-preserving gastrectomy and subgroup of infra-pyloric lymph nodes. However, its anatomical variation is not thoroughly understood. Our study aimed to clarify the origination of the IPA. Methods： We did this prospective, multicenter, open-label, observational study at gastric surgery departments of 34 hospitals in China. Gastric cancer patients aged 18 years or older and scheduled to undergo elective total or distal gastrectomy were assigned. During the surgery, IPA dissecting and exposing the origination point with photographs or video clips were required. The primary outcome was the origination of the IPA. Analysis of variance, χ2 tests and Fisher＇s tests were used to analyze the differences between groups. The study is registered at *** （No. NCT03071237）. Results： Between May 8 and July 31, 2017, 429 patients were assigned for the study, and 419 （97.7%） patients had the IPA dissected and recorded through photograph or video and were included in the primary outcome analysis. The median age was 62 years old, and 73.7% were male. Among the patients, 78.5% received laparoscopic surgery. Single IPA origination was identified in 398 （95.0%） patients, including gastroduodenal artery （GDA） in 154 （36.8%） patients, anterior superior pancreaticoduodenal artery （ASPDA） in 130 （31.0%） patients, and right gastroepiploic artery （RGEA） in 114 （27.2%） patients. Fifteen （3.6%） patients were identified with multiple IPA and 6 （1.4%） patients were identified as IPA absence. The differences in the distribution of surgical approach （P=0.003） and geographic area （P=0.030） were statistically significant. No difference was shown in sex, age, gastrectomy type, tumor location, and clinical T, N and M stage. Conclusions： Our study found that the IPA originates from GDA, ASPDA and RGEA in similar proportions. Laparoscopic surgery may be more

关键词： Infra-pyloric artery origination anatomy gastric cancer

Atlas of dynamic spectra of fast radio burst FRB 20201124A

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Chinese Physics B 2023年第2期32卷 1-4页

作者：王铂钧胥恒姜金辰徐江伟牛佳瑞陈平李柯伽张冰朱炜玮东苏勃张春风傅海周德江张永坤王培冯毅李晔李冬子鲁文宾杨元培 RNCaballero 蔡策陈卯蒸戴子高艾力·伊沙木丁甘恒谦韩金林郝龙飞黄玉祥姜鹏李承奎李菂李辉李新乔李志玄刘志勇罗睿门云鹏牛晨辉彭文溪钱磊宋黎明孙京海王发印汪敏王娜王维扬吴雪峰肖硕熊少林徐永华徐仁新杨俊杨轩姚蕊易祁彬岳友岭于东俊余文飞袁建平张彬彬张松波张双南赵一郑伟康朱岩邹金航 Kavli Institute for Astronomy and Astrophysics Peking UniversityBeijing 100871China National Astronomical Observatories Chinese Academy of SciencesBeijing 100101China Department of Astronomy Peking UniversityBeijing 100871China University of Chinese Academy of Sciences Chinese Academy of SciencesBeijing 100049China Department of Particle Physics and Astrophysics Weizmann Institute of ScienceRehovot 76100Israel Nevada Center for Astrophysics University of NevadaLas VegasNV 89154USA Department of Physics and Astronomy University of NevadaLas VegasNV 89154USA Department of Physics&Astronomy University of IowaIowa CityIA 52242USA Zhejiang Laboratory HangzhouZhejiang 311121China Purple Mountain Observatory Chinese Academy of SciencesNanjing 210008China TAPIR Walter Burke Institute for Theoretical PhysicsMail Code 350-17CaltechPasadenaCA 91125USA Department of Astronomy University of California at BerkeleyBerkeleyCA 94720USA South-Western Institute For Astronomy Research Yunnan UniversityYunnan 650504China Key Laboratory of Particle Astrophysics Institute of High Energy PhysicsChinese Academy of SciencesBeijing 100049China Xinjiang Astronomical Observatory Chinese Academy of SciencesUrumqi 830011China University of Science and Technology of China Anhui 230026China Yunnan Observatories Chinese Academy of SciencesKunming 650216China Guizhou Normal University Guiyang 550001China CSIRO Space and Astronomy EppingNSW 1710Australia Max-Planck institut fur Radioastronomie Auf Dem HugelBonn53121Germany School of Astronomy and Space Science Nanjing UniversityNanjing 210093China State Key Laboratory of Nuclear Physics and Technology School of PhysicsPeking UniversityBeijing 100871China Shanghai Astronomical Observatory Chinese Academy of SciencesShanghai 200030China Key Laboratory of Modern Astronomy and Astrophysics(Nanjing University) Ministry of EducationNanjing 210093China College of Physics Hebei Normal UniversityShijiazhuang 050024China

Fast radio bursts(FRBs) are highly dispersed millisecond-duration radio bursts,[1,2]of which the physical origin is still not fully understood. FRB 20201124A is one of the most actively repeating FRBs. In this paper, we present the collection of 1863 burst dynamic spectra of FRB 20201124A measured with the Five-hundred-meter Aperture Spherical radio Telescope(FAST). The current collection, taken from the observation during the FRB active phase from April to June 2021, is the largest burst sample detected for any FRB so far. The standard PSRFITs format is adopted, including dynamic spectra of the burst, and the time information of the dynamic spectra, in addition, mask files help readers to identify the pulse positions are also provided. The dataset is available in Science Data Bank, with the link https://***/10.57760/sciencedb.j00113.00076.

关键词： fast radio burst FAST

CEPC Technical Design Report

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Radiation Detection Technology and Methods 2024年第1期8卷 I0003-I0016,1-1091页

作者： Waleed Abdallah Tiago Carlos Adorno de Freitas 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 Jianin AGH University of Science and Technology Faculty of Physics and Applied Computer ScienceKrakow Anhui University HefeiAnhui Applied Physics Department Federal Urdu University of ArtsScience and TechnologyIslamabad Banaras Hindu University Institute of ScienceVaranasi Bandirma Onyedi Eylul University Bandirma Beihang University Beijing Beijing Computational Science Research Center Beijing Beijing Conveyi LTD Beijing Beijing Glass Research Institute Co. LtdBeijing Beijing Institute of Technology Beijing Beijing Normal University Beijing Brown University ProvidenceRI Budker Institute of Nuclear Physics Novosibirsk Cadi Ayyad University Laboratory of Fundamental and Applied PhysicsPolydisciplinary FacultyMarrakech cairo University Giza Center for Theory and Computation National Tsing Hua UniversityHsinchu Central China Normal University WuhanHubei Central South University ChangshaHunan Centro de Fisica Teorica de Particulas Universidade Tecnica de LisboaLisboa Chengdu KaitengSifang Digital Radio&TV Equipment Co. LtdChengduSichuan China academy of engineering physics MianyangSichuan China building materials academy Beijing China Center of Advanced Science and Technology Beijing China Institute of Atomic Energy Beijing China Jiliang University HangzhouZhejiang China Nuclear Instrument CO. LTDBeijing China University of Geosciences Beijing China University of Geosciences WuhanHubei China University of Mining and Technology XuzhouJiangsu China West Normal University NanchongSichuan Chongqing University Department of PhysicsChongqing Chulalongkorn University Bangkok City University of Hong Kong Department of PhysicsHong Kong Cockcroft Institute Daresbury Cornell University IthacaNY CPPM(AMU/IPhU&CNRS/INP) Marseille Dalian Minzu University DalianLiaoning Dalian University of Technology Department of PhysicsDalian Deutsches Elektronen-Synchrotron DESY Hamburg Dzhelepov Laboratory of Nuclear Problems of Joint Institute for Nuclear Research(DLNP JINR) Dubna East China University Of Science And Technol

The Circular Electron Positron Collider(CEPC)is a large scientific project initiated and hosted by China,fostered through extensive collaboration with international *** 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 *** 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 *** 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 *** 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 ***,it includes a cost estimate and a preliminary construction timeline,establishing a framework for forthcoming engineering design phase and site selection *** is anticipated to begin around 2027-2028,pending government approval,with an estimated duration of 8 *** commencement of experiments and data collection could potentially be initiated in the mid-2030s.

关键词： initiated exceeding precise