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深圳证券交易所

城市环境设计 2014年第6期 38-51页

作者： Kunle Adeyemi Ryann Aoukar Sebastian Appl Laura Baird Waichuen Chan Jan Dechow Lukas Drasnar Matthew Engele Leo Ferretto Clarisa Garcia Fresco Alasdair Graham Jaitian Gu Matthew Haseltine joo Ferreira Marques Jesus Matthew Jull Alexde jong Santiago Hierro Kennedy Klaas Kresse Miranda Lee Anna Little Luxiang Liu David Eugin Moon Cristina Murphy Se Yoon Park Ferdjan Vander Pijl franscesca Portesine Idrees Rasouli Korbinian Schneider Wolfgang Schwarzwalder Felix Schwimmer Richard Sharam Lukasz Skalec Christine Svensson Lukasz Szlachcic Ken Yang Tan Michela Tonus Miroslav Vavrina na Wei Xinyuan Wang Leonie Wenz Su Xia Yunchao Xu Yang Yang Yun Zhang

股票市场的本质是投机买卖:基于资本,而非物质。深圳证券交易所可被设想为虚拟股票市场的具体实践:这一栋拥有悬浮基座的建筑物不但能发挥物理功能,为股票市场提供场地,更重要的是它象征了股票市场。一般来说,基座用以锚固结构,并将其... 详细信息

股票市场的本质是投机买卖:基于资本,而非物质。深圳证券交易所可被设想为虚拟股票市场的具体实践:这一栋拥有悬浮基座的建筑物不但能发挥物理功能,为股票市场提供场地,更重要的是它象征了股票市场。一般来说,基座用以锚固结构,并将其牢牢地与地面连接;然而,深圳证券交易所的基座却沿着塔楼从地面往高处攀升,投机买卖的热烈气氛在驱动交易市

关键词：深圳证券交易所深交所半钢化玻璃

中下肺肿瘤SBRT放疗中分次内误差影响因素以及PTV外扩边界分析

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肿瘤预防与治疗 2024年第10期37卷 898-903页

作者：曾伟叶程伟刘莉袁建军罗志尧刘江刘娜何淼德阳市人民医院肿瘤科四川德阳618000 成都医学院临床医学院成都610500

目的:探讨中下肺肿瘤立体定向放射治疗(stereotactic body radiotherapy,SBRT)过程中分次内误差影像因素并计算PTV-margin(PM)。方法:收集2022年2月至2023年6月德阳市人民医院肿瘤科收治的21例行中下肺SBRT治疗的患者,采用仰卧位双手上... 详细信息

目的:探讨中下肺肿瘤立体定向放射治疗(stereotactic body radiotherapy,SBRT)过程中分次内误差影像因素并计算PTV-margin(PM)。方法:收集2022年2月至2023年6月德阳市人民医院肿瘤科收治的21例行中下肺SBRT治疗的患者,采用仰卧位双手上举抓杆,热塑头颈胸膜固定,三维CT和四维锥形束CT(cone beam computed tomography,CBCT)融合定位,确定内靶区(internal target volume,ITV),分割模式总剂量48~60 Gy,单次6~12 Gy/次,总共4~10次。患者治疗前行3D-CBCT扫描,移床纠正摆位误差后开始治疗,完成后进行第二次3D-CBCT扫描并记录误差数据作为分次内误差,计算分次内误差的矢量距离,分析其与治疗时间、体质指数(body mass index,BMI)、患者年龄三个方面的相关性。分别记录两次3D-CBCT所得误差数据,利用PM计算公式分别计算分次间和分次内误差所需PM。用SPSS 26.0进行数据统计分析。结果:分次内误差在三维方向上的矢量距离均值±标准差为(0.17±0.16)cm,与治疗时间的相关性有统计学意义(r=0.38,P<0.01),与患者年龄的相关性无统计学意义(r=-0.09,P=0.33),与患者BMI的相关性无统计学意义(r=0.18,P=0.06)。分次间误差与分次内误差在三维方向均数±标准差分别为:左右方向(Left-Right,LR):(-0.08±0.26)cm,(-0.01±0.1)cm;头脚方向(Superior-Inferior,SI):(-0.1±0.36)cm,(-0.01±0.15)cm;前后方向(Anterior-Posterior,AP):(-0.05±0.17cm),(0.02±0.14)cm。分次间和分次内误差在LR、SI、AP方向所需PM分别为:LR 0.54 cm、0.11 cm;SI 0.78 cm、0.16 cm;AP 0.31 cm、0.14 cm。结论:中下肺癌SBRT治疗中分次内误差和治疗时间存在相关性,与患者年龄、患者BMI指数无相关性。在中下肺SBRT治疗中,使用4D-CBCT辅助ITV勾画后,0.5 cm PM能够补偿分次内误差带来的位置变化。

关键词： 3D-CBCT 分次内误差 SBRT 中下肺肿瘤 BMI PTV-margin

渐进性康复护理路径对脊柱内镜患者的临床效果观察

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实用医院临床杂志 2019年第2期16卷 113-116页

作者：曹利芸王云秀李得彬冷娜李顺琼王建四川省攀枝花市第二人民医院脊柱外科四川攀枝花617068

目的探讨渐进性康复护理路径对脊柱内镜患者的临床效果。方法采用随机分组法将108例患者分为干预组和对照组各54例,两组分别于2016年6月至2018年6月接受同一手术医生内镜手术治疗。对照组给予常规康复护理,干预组给予渐进性康复护理路... 详细信息

目的探讨渐进性康复护理路径对脊柱内镜患者的临床效果。方法采用随机分组法将108例患者分为干预组和对照组各54例,两组分别于2016年6月至2018年6月接受同一手术医生内镜手术治疗。对照组给予常规康复护理,干预组给予渐进性康复护理路径。比较两组患者的临床护理效果,以及视觉模拟疼痛评分(VAS)、腰椎功能评分(joA)、Oswestry功能障碍指数量表(ODI)和生活质量评分改善情况。结果护理后干预组的优良率(88. 89%)明显高于对照组(74. 07%)(P joA评分均提高,且干预组评分优于对照组(P <0. 05);两组患者生理功能、社会功能、精神健康、情感职能等生活质量指标评分均降低,干预组明显低于对照组(P <0. 05)。两组患者并发症情况比较,干预组出现神经根黏连、水肿以及椎间隙感染的发生率为12. 96%(7/54),低于对照组的29. 63%(16/54),差异有统计学意义(χ~2=4. 475,P=0. 034)。结论渐进性康复护理路径干预脊柱内镜治疗的腰椎间盘突出症患者,可明显减轻患者疼痛,促进腰椎功能恢复,降低并发症发生率,提高生活质量。

关键词：渐进性康复护理腰椎间盘突出症脊柱内镜疼痛腰椎功能生活质量

血小板衍生生长因子受体-a在骨肉瘤中的表达及意义

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甘肃医药 2012年第11期31卷 810-813页

作者：徐欣华李晓琴杨荣刘芳康雅琼何欣尚立娜温岭市第二人民医院病理科浙江温岭317502 甘肃省肿瘤医院病理科甘肃兰州730050

目的:探讨血小板衍生生长因子受体-a(PDGFR-a)在骨肉瘤发病中的表达及与骨肉瘤临床病理、预后的关系。方法:采用免疫组织化学SP法,检测了60例骨肉瘤和10例骨瘤(对照组)中PDGFR-a的表达情况,分析PDGFR-a的表达与骨肉瘤病理分型、临床分... 详细信息

目的:探讨血小板衍生生长因子受体-a(PDGFR-a)在骨肉瘤发病中的表达及与骨肉瘤临床病理、预后的关系。方法:采用免疫组织化学SP法,检测了60例骨肉瘤和10例骨瘤(对照组)中PDGFR-a的表达情况,分析PDGFR-a的表达与骨肉瘤病理分型、临床分型及预后之间的关系。结果:①PDGFR-a表达与病理分型无明显相关性,但与临床分期密切相关;②PDGFR-a在骨肉瘤中表达阳性率为61.7%(37/60),显著高于对照组(P<0.05);③PDGFR-a高表达组的术后生存时间显著低于PDGFR-a低表达组;④PDGFR-a表达高的易局部复发。结论:PDGFR-a在骨肉瘤中的表达与骨肉瘤的生物学行为有关,对评价患者的预后及指导临床治疗具有一定的参考价值。

关键词： PDGFR-a 骨肉瘤预后治疗

Sub-percent precision measurement of neutrino oscillation parameters with JUNO

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Chinese Physics C 2022年第12期46卷 28-49页

作者： Angel Abusleme Thomas Adam Shakeel Ahmad Rizwan Ahmed Sebastiano Aiello Muhammad Akram Abid Aleem Fengpeng An Qi An Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop joão Pedro Athayde Marcondes de André Didier Auguste Weidong Bai Nikita Balashov Wander Baldini Andrea Barresi Davide Basilico Eric Baussan Marco Bellato Antonio Bergnoli Thilo Birkenfeld Sylvie Blin David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano jose Busto Ilya Butorov Anatael Cabrera Barbara Caccianiga Hao Cai Xiao Cai Yanke Cai Zhiyan Cai Riccardo Callegari Antonio Cammi Agustin Campeny Chuanya Cao Guofu Cao Jun Cao Rossella Caruso Cédric Cerna Chi Chan Jinfan Chang Yun Chang Guoming Chen Pingping Chen Po-An Chen Shaomin Chen Xurong Chen Yixue Chen Yu Chen Zhiyuan Chen Zikang Chen Jie Cheng Yaping Cheng Yu Chin Cheng Alexey Chetverikov Davide Chiesa Pietro Chimenti Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Selma Conforti Di Lorenzo Daniele Corti Flavio Dal Corso Olivia Dalager Christophe De La Taille Zhi Deng Ziyan Deng Wilfried Depnering Marco Diaz Xuefeng Ding Yayun Ding Bayu Dirgantara Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko Jianmeng Dong Evgeny Doroshkevich Marcos Dracos Frédéric Druillole Ran Du Shuxian Du Stefano Dusini Martin Dvorak Timo Enqvist Heike Enzmann Andrea Fabbri Donghua Fan Lei Fan Jian Fang Wenxing Fang Marco Fargetta Dmitry Fedoseev Zhengyong Fei Li-Cheng Feng Qichun Feng Richard Ford Amélie Fournier Haonan Gan Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Nunzio Giudice Maxim Gonchar Guanghua Gong Hui Gong Yuri Gornushkin Alexandre Göttel Marco Grassi Vasily Gromov Minghao Gu Xiaofei Gu Yu Gu Mengyun Guan Yuduo Guan Nunzio Guardone Cong Guo Jingyuan Guo Wanlei Guo Xinheng Guo Yuhang Guo Paul Hackspacher Caren Hagner Ran Han Yang Han Miao He Wei He Tobias Heinz Patrick Hellmuth Yuekun Heng Rafael Herrera YuenKeung Ho Yerevan Physics Institute YerevanArmenia UniversiéLibre de Bruxelles BrusselsBelgium Universidade Estadual de Londrina LondrinaBrazil Pontificia Universidade Catolica do Rio de Janeiro Rio de JaneiroBrazil Pontificia Universidad Católica de Chile SantiagoChile Universidad Tecnica Federico Santa Maria ValparaisoChile Beijing Institute of Spacecraft Environment Engineering BeijingChina Beijing Normal University BeijingChina China Institute of Atomic Energy BeijingChina Institute of High Energy Physics BeijingChina North China Electric Power University BeijingChina School of Physics Peking UniversityBeijingChina Tsinghua University BeijingChina University of Chinese Academy of Sciences BeijingChina Jilin University ChangchunChina College of Electronic Science and Engineering National University of Defense TechnologyChangshaChina Chongqing University ChongqingChina Dongguan University of Technology DongguanChina Jinan University GuangzhouChina Sun Yat-Sen University GuangzhouChina Harbin Institute of Technology HarbinChina University of Science and Technology of China HefeiChina The Radiochemistry and Nuclear Chemistry Group in University of South China HengyangChina Wuyi University JiangmenChina Shandong University JinanChinaand Key Laboratory of Particle Physics and Particle Irradiation of Ministry of EducationShandong UniversityQingdaoChina Institute of Modern Physics Chinese Academy of SciencesLanzhouChina nanjing University NanjingChina Guangxi University NanningChina East China University of Science and Technology ShanghaiChina School of Physics and Astronomy Shanghai Jiao Tong UniversityShanghaiChina Tsung-Dao Lee Institute Shanghai Jiao Tong UniversityShanghaiChina Institute of Hydrogeology and Environmental Geology Chinese Academy of Geological SciencesShijiazhuangChina nankai University TianjinChina Wuhan University WuhanChina Xi'an Jiaotong University Xi'anChina Xiamen University XiamenChina School of Physics and Microelectronics Zhengzhou UniversityZhengzhou

JUNO is a multi-purpose neutrino observatory under construction in the south of *** publication presents new sensitivity estimates for the measurement of the △m_(31)^(2),△m_(21)^(2),sin^(2)θ_(12),and sin^(2)θ_(13) oscillation parameters using reactor antineutrinos,which is one of the primary physics goals of the *** sensitivities are obtained using the best knowledge available to date on the location and overburden of the experimental site,the nuclear reactors in the surrounding area and beyond,the detector response uncertainties,and the reactor antineutrino spectral shape constraints expected from the TAO satellite *** is found that the △m_(21)^(2) and sin^(2)θ_(12) oscillation parameters will be determined to 0.5%precision or better in six years of data *** the same period,the △m_(31)^(2) parameter will be determined to about 0.2%precision for each mass ordering *** new precision represents approximately an order of magnitude improvement over existing constraints for these three parameters.

关键词： neutrino oscillation reactor antineutrino precision measurement JUNO

JUNO sensitivity on proton decay p→νK^(+)searches

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Chinese Physics C 2023年第11期47卷 7-22页

作者： Angel Abusleme Thomas Adam Shakeel Ahmad Rizwan Ahmed Sebastiano Aiello Muhammad Akram 安丰鹏安琪 Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop joão Pedro Athayde Marcondes de André Didier Auguste Nikita Balashov Wander Baldini Andrea Barresi Davide Basilico Eric Baussan Marco Bellato Antonio Bergnoli Thilo Birkenfeld Sylvie Blin David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Mario Buscemi jose Busto Ilya Butorov Anatael Cabrera Barbara Caccianiga 蔡浩蔡啸蔡严克蔡志岩 Riccardo Callegari Antonio Cammi Agustin Campeny 曹传亚曹国富曹俊 Rossella Caruso Cédric Cerna 常劲帆 Yun Chang 陈平平 Po-An Chen 陈少敏陈旭荣 Yi-Wen Chen 陈义学陈羽陈长程捷程雅苹 Alexey Chetverikov Davide Chiesa Pietro Chimenti Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Selma Conforti Di Lorenzo Daniele Corti Flavio Dal Corso Olivia Dalager Christophe De La Taille 邓智邓子艳 Wilfried Depnering Marco Diaz Xuefeng Ding 丁雅韵 Bayu Dirgantara Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko 董建蒙 Evgeny Doroshkevich Marcos Dracos Frédéric Druillole 杜然杜书先 Stefano Dusini Martin Dvorak Timo Enqvist Heike Enzmann Andrea Fabbri Ulrike Fahrendholz 范东华樊磊方建方文兴 Marco Fargetta Dmitry Fedoseev Li-Cheng Feng 冯启春 Richard Ford Amélie Fournier 甘浩男 Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Agnese Giaz Nunzio Giudice Maxim Gonchar 龚光华宫辉 Yuri Gornushkin Alexandre Göttel Marco Grassi Christian Grewing Vasily Gromov 顾旻皓谷肖飞古宇关梦云 Nunzio Guardone Maria Gul 郭聪郭竞渊郭万磊郭新恒郭宇航 Paul Hackspacher Caren Hagner 韩然 Yang Han Muhammad Sohaib Hassan 何苗何伟 Tobias Heinz Patrick Hellmuth 衡月昆 Rafael Herrera 贺远强侯少静 Yee Hsiung Bei-Zhen Hu 胡航胡健润胡俊胡守扬胡涛胡宇翔胡焯钧黄春豪黄桂鸿黄翰雄黄文昊黄鑫黄性涛黄永波惠加琪霍雷霍文驹 Cédric Huss Safeer Hussain Ara Ioannisian Roberto Isocrate Beatrice Jelmini Kuo-Lun Jen Ignacio Jeria 季筱璐吉星曌贾慧慧贾俊基蹇司玉蒋荻蒋炜江晓山金如意荆小平 Cécile jollet Jari joutsenvaara Sirichok Jungthawan Leonidas Kalousis Philipp Ka Pontificia Universidad Católica de Chile SantiagoChile IPHC Universitéde StrasbourgCNRS/IN2P3F-67037 StrasbourgFrance Pakistan Institute of Nuclear Science and Technology IslamabadPakistan INFN Catania and Dipartimento di Fisica e Astronomia dell Universitàdi Catania CataniaItaly East China University of Science and Technology ShanghaiChina University of Science and Technology of China HefeiChina joint Institute for Nuclear Research DubnaRussia INFN Sezione di Milano and Dipartimento di Fisica dell Universitàdi Milano MilanoItaly Department of Physics Faculty of ScienceChulalongkorn UniversityBangkokThailand IJCLab UniversitéParis-SaclayCNRS/IN2P391405 OrsayFrance Department of Physics and Earth Science University of Ferrara and INFN Sezione di FerraraFerraraItaly INFN Milano Bicocca and University of Milano Bicocca MilanoItaly INFN Sezione di Padova PadovaItaly III.Physikalisches Institut B RWTH Aachen UniversityAachenGermany Eberhard Karls Universität Tübingen Physikalisches InstitutTübingenGermany Institute of High Energy Physics BeijingChina SUBATECH Universitéde NantesIMT AtlantiqueCNRS-IN2P3NantesFrance Univ.Bordeaux CNRSLP2IUMR 5797F-33170 GradignanFrance Department of Physics National Taiwan UniversityTaipei Dipartimento di Fisica e Astronomia dell’Universitàdi Padova and INFN Sezione di Padova PadovaItaly University of Roma Tre and INFN Sezione Roma Tre RomaItaly Aix Marseille Univ CNRS/IN2P3CPPMMarseilleFrance Wuhan University WuhanChina INFN Milano Bicocca and Politecnico of Milano MilanoItaly national United University Miao-Li Dongguan University of Technology DongguanChina Tsinghua University BeijingChina Institute of Modern Physics Chinese Academy of SciencesLanzhouChina Institute of Physics National Yang Ming Chiao Tung UniversityHsinchu North China Electric Power University BeijingChina Sun Yat-Sen University GuangzhouChina Beijing Institute of Spacecraft Environment Engineering BeijingChina Universidade Estadual de Londrina LondrinaBrazil INFN Sez

The Jiangmen Underground Neutrino Observatory(JUNO)is a large liquid scintillator detector designed to explore many topics in fundamental *** this study,the potential of searching for proton decay in the p→νK^(+)mode with JUNO is *** kaon and its decay particles feature a clear three-fold coincidence signature that results in a high efficiency for ***,the excellent energy resolution of JUNO permits suppression of the sizable background caused by other delayed *** on these advantages,the detection efficiency for the proton decay via p→νK^(+)is 36.9%±4.9%with a background level of 0.2±0.05(syst)±0.2(stat)events after 10 years of data *** estimated sensitivity based on 200 kton-years of exposure is 9.6×1033 years,which is competitive with the current best limits on the proton lifetime in this channel and complements the use of different detection technologies.

关键词： proton decay grand unified theories JUNO liquid scintillator detector