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Chinese Physics C 2023年第4期 22-31页

作者：麦迪娜 M.N.Achasov P.Adlarson M.Albrecht r.Aliberti A.Amoroso 安美儒安琪白旭红白羽 O.bakina r.baldini Ferroli I.balossino 班勇 V.batozskaya D.becker K.begzsuren N.berger M.bertani D.bettoni F.bianchi J.bloms A.bortone I.boyko r.A.briere A.brueggemann 蔡浩蔡啸 A.Calcaterra 曹国富曹宁 s.A.Cetin 常劲帆常万玲 G.Chelkov 陈琛陈超陈刚陈和生陈玛丽陈申见陈少敏 T.Chen 陈旭荣 x.T.Chen 陈元柏陈卓俊成伟帅初晓 G.Cibinetto F.Cossio 崔佳佳代洪亮代建平 A.Dbeyssi r.E.de boer D.Dedovich 邓子艳 A.Denig I.Denysenko M.Destefanis F.De Mori 丁勇董静董燎原董明义董翔杜书先 P.Egorov 范玉兰方建房双世方文兴方易 r.farinelli L.Fava F.Feldbauer G.Felici 封常青冯俊华 K Fischer M.Fritsch C.Fritzsch 傅成栋高涵高原宁高扬 s.Garbolino I.Garzia 葛潘婷葛振武耿聪 E.M.Gersabeck A Gilman K.Goetzen 龚丽龚文煊 w.Gradl M.Greco 谷立民顾旻皓顾运厅关春懿郭爱强郭立波郭如盼郭玉萍 A.Guskov 韩婷婷韩文颖郝喜庆 F.A.Harris 何凯凯何康林 F.H.Heinsius C.H.Heinz 衡月昆 C.Herold M.Himmelreich 侯国一侯颖锐侯治龙胡海明 J.F.Hu 胡涛胡誉黄光顺黄凯旋黄麟钦黄麟钦黄性涛黄燕萍黄震 T.Hussain N Hüsken w.Imoehl M.Irshad J.Jackson s.Jaeger s.Janchiv 纪全姬清平季晓斌季筱璐吉钰瑶贾泽坤姜侯兵姜赛赛江晓山 y.Jiang 焦健斌焦铮金山金毅荆茂强 T.Johansson N.Kalantar-Nayestanaki 康晓珅 r.Kappert 柯百谦 I.K.Keshk A.Khoukaz P.Kiese r.Kiuchi r.Kliemt L.Koch O.b.Kolcu b.Kopf M.Kuemmel M.Kuessner A.Kupsc w.Kühn J.J.Lane J.s.Lange P.Larin A.Lavania L.Lavezzi 雷祚弘 H.Leithoff M.Lellmann T.Lenz 李翠李聪李春花李澄李德民李飞李刚李慧李贺李海波李惠静 H.N.Li J.q.Li 李静舒李井文李科 L.J.Li 李龙科李蕾李明浩李培荣李素娴栗帅迎李腾李卫东李卫国李旭红李晓玲李晓宇梁昊梁浩梁浩梁勇飞梁羽铁廖广睿廖龙洲 J.Libby A.Limphirat 林创新林德旭 T.Lin 刘北江刘春秀 D.Liu 刘福虎刘芳刘峰 G.M.Liu H.Liu 刘宏邦刘怀民刘欢欢刘汇慧刘建北刘佳俊刘晶译刘凯刘魁勇刘珂刘亮刘露刘美宏刘佩莲刘倩刘树彬刘桐刘维克刘卫民刘翔刘英刘玉斌刘振安刘智青娄辛丑卢飞翔吕海江吕军光陆小玲卢宇卢云鹏 Z.H.Lu 罗成林罗民兴罗涛罗小兰吕晓睿吕翌丰马凤才马海龙马连良马明明马秋梅马润秋马瑞廷马骁妍马尧 F.E.Maas M.Maggiora s.Maldaner s.Malde q.A.Malik A.Mangoni 冒亚军毛泽普 s.Marcello 孟召霞 J.G.Messchendorp G.Mezzadri H.Miao 闵天觉 r.E.Mitchell 莫晓虎 N.yu.Muchnoi y.Nefedov F.Nerling I.b.Nikolaev 宁哲 s.Nisar 牛艳 s.L.Olsen 欧阳群 s.Pacetti 潘祥潘越 A.Pathak M.Pelizaeus 彭海平 K.Peters 平加伦平荣刚 s.Plura s.Pogodin V.Prasad 齐法制齐航漆红荣祁鸣齐天钰钱森钱文斌钱圳乔从丰秦佳佳秦丽清覃潇平秦小帅秦中华邱进发屈三强 K.H.rashid C.F.redmer 任旷洁 A.rivetti V.rodin M.rolo 荣刚 Ch.rosn Institute of High Energy Physics G.I. budker Institute of Nuclear Physics sb rAs(bINP) Novosibirsk state University Uppsala University bochum ruhr-University Johannes Gutenberg University of Mainz University of Turin INFN Liaoning Normal University state Key Laboratory of Particle Detection and Electronics University of science and Technology of China University of Jinan southeast University Joint Institute for Nuclear research INFN Laboratori Nazionali di Frascati INFN sezione di Ferrara Peking University state Key Laboratory of Nuclear Physics and Technology Peking University National Centre for Nuclear research Institute of Physics and Technology University of Muenster Carnegie Mellon University wuhan University University of Chinese Academy of sciences Istinye University Moscow Institute of Physics and Technology Nankai University soochow University Nanjing University Tsinghua University Institute of Modern Physics Hunan University school of Physics and Electronics Hunan University shandong University yunnan University Helmholtz Institute Mainz Liaoning University Zhengzhou University University of Eastern Piedmont sun yat-sen University University of Oxford University of Ferrara University of Manchester GsI Helmholtzcentre for Heavy Ion research GmbH Guangxi University Nanjing Normal University shandong Normal University Fudan University Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) and Institute of Modern Physics Fudan University Henan Normal University University of Hawaii suranaree University of Technology Goethe University Frankfurt south China Normal University Guangdong Provincial Key Laboratory of Nuclear science Institute of quantum Matter south China Normal University University of south China University of the Punjab Indiana University Huangshan College University of Groningen Justus-Liebig-Universitaet Giessen Ⅱ. Physikalisches Institut Indian Institute of Technology Madras qufu Normal University shanxi Normal University beijing Institute of Petrochemical Technology Lanzhou Univ

Using data taken at 29 center-of-mass energies between 4.16 and 4.70 GeV with the bEsⅢ detector at the beijing Electron Positron Collider corresponding to a total integrated luminosity of approximately 18.8 fb-1, the process e+e-→■+ c.c. is observed for the first time with a statistical significance of 11.5σ. The average born cross sections in the energy ranges of（4.160, 4.380） GeV,（4.400, 4.600） GeV and（4.610, 4.700） GeV are measured to be（21.5±5.7±1.2） fb,（46.3±10.6±2.5） fb and （59.0±9.4±3.2） fb, respectively, where the first uncertainties are statistical and the second are systematic. The line shapes of the ■ and ppπ-invariant mass spectra are consistent with phase space distributions, indicating that no hexaquark or di-baryon state is observed.

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Luminosities and energies of e+e- collision data taken between ■=4.61 GeV and 4.95 GeV at bEsⅢ

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Chinese Physics C 2022年第11期46卷 70-81页

作者：麦迪娜 M.N.Achasov P.Adlarson M.Albrecht r.Aliberti A.Amoroso 安美儒安琪白旭红白羽 O.bakina Ferroli r.baldini I.balossino 班勇 V.batozskaya D.becker K.begzsuren N.berger M.bertani D.bettoni F.bianchi J.bloms A.bortone I.boyko r.A.briere A.brueggemann 蔡浩蔡啸 A.Calcaterra 曹国富曹宁 s.A.Cetin 常劲帆常万玲 G.Chelkov 陈琛陈超陈刚陈和生陈玛丽陈申见陈少敏 T.Chen 陈旭荣 x.T.Chen 陈元柏陈卓俊成伟帅初晓 G.Cibinetto F.Cossio 崔佳佳代洪亮代建平 A.Dbeyssi boer r.E.de D.Dedovich 邓子艳 A.Denig I.Denysenko M.Destefanis Mori F.De 丁勇董静董燎原董明义董翔杜书先 P.Egorov 范玉兰方建房双世方文兴方易 r.farinelli L.Fava F.Feldbauer G.Felici 封常青冯俊华 K Fischer M.Fritsch C.Fritzsch 傅成栋高涵高原宁高扬 s.Garbolino I.Garzia 葛潘婷葛振武耿聪 E.M.Gersabeck A Gilman K.Goetzen 龚丽龚文煊 w.Gradl M.Greco 谷立民顾旻皓顾运厅关春懿郭爱强郭立波郭如盼郭玉萍 A.Guskov 韩婷婷韩文颖郝喜庆 F.A.Harris 何凯凯何康林 F.H.Heinsius C.H.Heinz 衡月昆 C.Herold M.Himmelreich 侯国一侯颖锐侯治龙胡海明 J.F.Hu 胡涛胡誉黄光顺黄凯旋黄麟钦黄麟钦黄性涛黄燕萍黄震 T.Hussain N Hüsken w.Imoehl M.Irshad J.Jackson s.Jaeger s.Janchiv 纪全姬清平季晓斌季筱璐吉钰瑶贾泽坤姜侯兵姜赛赛江晓山 y.Jiang 焦健斌焦铮金山金毅荆茂强 T.Johansson N.Kalantar-Nayestanaki 康晓珅 r.Kappert 柯百谦 I.K.Keshk A.Khoukaz P.Kiese r.Kiuchi r.Kliemt L.Koch O.b.Kolcu b.Kopf M.Kuemmel M.Kuessner A.Kupsc w.Kühn J.J.Lane J.s.Lange P.Larin A.Lavania L.Lavezzi 雷祚弘 H.Leithoff M.Lellmann T.Lenz 李翠李聪李春花李澄李德民李飞李刚李慧李贺李海波李惠静 H.N.Li J.q.Li 李静舒李井文李科李林健李龙科李蕾李明浩李培荣李素娴栗帅迎李腾李卫东李卫国李旭红李晓玲李晓宇梁昊梁浩梁浩梁勇飞梁羽铁廖广睿廖龙洲 J.Libby A.Limphirat 林创新林德旭 T.Lin 刘北江刘春秀 D.Liu 刘福虎刘芳刘峰 G.M.Liu H.Liu 刘宏邦刘怀民刘欢欢刘汇慧刘建北刘佳俊刘晶译刘凯刘魁勇刘珂刘亮刘露刘美宏刘佩莲刘倩刘树彬刘桐刘维克刘卫民刘翔刘英刘玉斌刘振安刘智青娄辛丑卢飞翔吕海江吕军光陆小玲卢宇卢云鹏 Z.H.Lu 罗成林罗民兴罗涛罗小兰吕晓睿吕翌丰马凤才马海龙马连良马明明马秋梅马润秋马瑞廷马骁妍马尧 F.E.Maas M.Maggiora s.Maldaner s.Malde q.A.Malik A.Mangoni 冒亚军毛泽普 s.Marcello 孟召霞 J.G.Messchendorp G.Mezzadri H.Miao 闵天觉 r.E.Mitchell 莫晓虎 N.yu.Muchnoi y.Nefedov F.Nerling I.b.Nikolaev 宁哲 s.Nisar 牛艳 s.L.Olsen 欧阳群 s.Pacetti 潘祥潘越 A.Pathak M.Pelizaeus 彭海平 K.Peters 平加伦平荣刚 s.Plura s.Pogodin V.Prasad 齐法制齐航漆红荣祁鸣齐天钰钱森钱文斌钱圳乔从丰秦佳佳秦丽清覃潇平秦小帅秦中华邱进发屈三强 K.H.rashid C.F.redmer 任旷洁 A.rivetti V.rodin M.rolo 荣刚 Ch.rosner Institute of High Energy Physics G. I. budker Institute of Nuclear Physics sb rAs (bINP) the Novosibirsk state University Uppsala University bochum ruhr-University Johannes Gutenberg University of Mainz University of Turin INFN Liaoning Normal University state Key Laboratory of Particle Detection and Electronics University of science and Technology of China University of Jinan southeast University Joint Institute for Nuclear research INFN Laboratori Nazionali di Frascati INFN sezione di Ferrara Peking University state Key Laboratory of Nuclear Physics and Technology Peking University National Centre for Nuclear research Institute of Physics and Technology University of Muenster Carnegie Mellon University wuhan University University of Chinese Academy of sciences Istinye University the Moscow Institute of Physics and Technology Nankai University soochow University Nanjing University Tsinghua University Institute of Modern Physics Hunan University school of Physics and Electronics Hunan University shandong University yunnan University Helmholtz Institute Mainz Liaoning University Zhengzhou University University of Eastern Piedmont sun yat-sen University University of Oxford University of Ferrara University of Manchester GsI Helmholtzcentre for Heavy Ion research GmbH Guangxi University Nanjing Normal University shandong Normal University Fudan University Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) and Institute of Modern Physics Fudan University Henan Normal University University of Hawaii suranaree University of Technology Goethe University Frankfurt south China Normal University Guangdong Provincial Key Laboratory of Nuclear science Institute of quantum Matter south China Normal University University of south China University of the Punjab Indiana University Huangshan College University of Groningen Justus-Liebig-Universitaet Giessen Ⅱ.Physikalisches Institut Indian Institute of Technology Madras qufu Normal University shanxi Normal University beijing Institute of Petrochemical Technology Lan

From December 2019 to June 2021,the bEsⅢ experiment collected approximately 5.85 fb-1of data at center-of-mass energies between 4.61 and 4.95 *** is the highest collision energy bEPCⅡ has reached to *** accumulated e+e-annihilation data samples are useful for studying charmonium（-like） states and charmed-hadron *** adopting a novel method of analyzing the production of ■ pairs in e+e-annihilation,the center-of-mass energies are measured with a precision of ～0.6 *** luminosities are measured with a precision of better than 1% by analyzing the events of large-angle bhabha *** measurements provide important inputs to analyses based on these data samples.

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西伯利亚狍成纤维细胞建系及其生物学特性分析

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动物学杂志 2022年第5期57卷 653-667页

作者：郭晓楠李云霞郝晓丽王茂俊乌云毕力格吴图雅格根卓拉张健宋永利赵高平曹贵方包斯琴李喜和内蒙古大学生命科学学院蒙古高原动物遗传资源研究中心呼和浩特010020 内蒙古赛科星家畜种业与繁育生物技术研究院呼和浩特011517 内蒙古农业大学兽医学院呼和浩特010018 河套学院巴彦淖尔015000

本研究以内蒙古大青山获得野生雄性和雌性西伯利亚狍(Capreolus pygargus)为实验材料,利用组织块贴壁培养法进行气管、肺和耳3种组织成纤维细胞原代建系,研究不同组织来源的细胞贴壁率、冷冻前及复苏后存活率、生长曲线,进一步绘制狍成... 详细信息

本研究以内蒙古大青山获得野生雄性和雌性西伯利亚狍(Capreolus pygargus)为实验材料,利用组织块贴壁培养法进行气管、肺和耳3种组织成纤维细胞原代建系,研究不同组织来源的细胞贴壁率、冷冻前及复苏后存活率、生长曲线,进一步绘制狍成纤维细胞核型图并分析其G带特征。实验结果显示,气管、肺和耳3种组织成纤维细胞增殖经历潜伏期、对数生长期、平台期三个阶段,细胞形态为梭形、三角形或不规则形,是典型成纤维细胞形态;成纤维细胞呈漩涡状生长,其中气管、耳成纤维细胞生长增殖能力最强、肺成纤维细胞增殖能力较弱,气管和耳组织来源成纤维细胞呈典型“s”型细胞生长特征。染色体核型及G带分析结果显示,雄性狍成纤维细胞染色体条数为2n=70,其中,有34对常染色体,形态类型为12条近端着丝粒染色体(st),22条亚中着丝粒染色体(sm),1对性染色体,x染色体为中着丝粒染色体(m),y染色体为近端着丝粒染色体(st),5条超数染色体(b);雌性狍成纤维细胞染色体条数为2n=70,其中,有34对常染色体,其形态类型为29条亚中着丝粒染色体(sm),5条近端着丝粒染色体(st),1对为性染色体,x染色体为亚中着丝粒染色体(sm),8条超数染色体(b)。本研究成功建立了雄性和雌性西伯利亚狍气管、肺和耳3种组织来源的成纤维细胞系,在体外培养时生长状态良好且维持了细胞的遗传信息稳定性,绘制了西伯利亚狍雄性和雌性染色体核型及G带图谱,为将来更深入开展相关研究提供材料与基本技术支撑。

关键词：西伯利亚狍成纤维细胞冷冻前及复苏后存活率生长曲线核型和G带

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拓展实验白藜芦醇谱学指认与分析

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当代化工 2020年第7期49卷 1337-1340,1346页

作者：蒋鑫施琪浩吴贤达李淑芳陈星梁诗格陈诗雨张英杰陈丹钟爱国台州学院医药化工与材料工程学院浙江台州318000

采用密度泛函理论的方法(DFT b3LyP/6-31++G),优化白藜芦醇(bLLC)及其16种衍生物的结构,通过改变不同类型的取代基和不同位置的取代基,来分析不同的取代基对白藜芦醇饱和蒸汽压p有着不同的影响,并通过计算得到相关性系数r最大的EsP-O7... 详细信息

采用密度泛函理论的方法(DFT b3LyP/6-31++G),优化白藜芦醇(bLLC)及其16种衍生物的结构,通过改变不同类型的取代基和不同位置的取代基,来分析不同的取代基对白藜芦醇饱和蒸汽压p有着不同的影响,并通过计算得到相关性系数r最大的EsP-O7电荷值与饱和蒸气压的线性方程(y=-48.6x+15.55;r=0.67687);用DFT方法预测了16种白藜芦醇衍生物的红外光谱(Ir),对其的特征峰进行指认和归属,模拟了白藜芦醇及其16种白藜芦醇衍生物的C原子核磁共振光谱图、圆二色光谱(ECD)等分子光谱,并对其特征峰进行一一指认和归属,这些模拟研究将为制药专业拓展实验白藜芦醇及其衍生物的光谱以及构效关系提供基础数据。

关键词：制药专业实验密度泛函理论白藜芦醇 ECD 核磁共振光谱谱学分析

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黄芪甲苷通过调控线粒体功能抑制H_(2)O_(2)诱导的sH-sy5y细胞凋亡

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中国病理生理杂志 2022年第9期38卷 1553-1560页

作者：于婧文郭敏芳李苏垚孟涛张海飞杨德斌宋丽娟马存根尉杰忠山西大同大学脑科学研究所/附属第一医院神经科山西大同037009 山西中医药大学国家中医药管理局多发性硬化益气活血重点研究室/神经生物学研究中心山西晋中030619 山西医科大学生理学系山西太原030001 山西大同市第四人民医院山西大同037009

目的:探讨黄芪甲苷(astragaloside Ⅳ,AsT Ⅳ)对由氧化应激损伤引起的线粒体功能障碍以及细胞凋亡的作用及机制。方法:体外培养人神经母细胞瘤sH-sy5y细胞,用过氧化氢(hydrogen peroxide,HO)诱导建立氧化应激模型,分为Pbs组、模型组(HO... 详细信息

目的:探讨黄芪甲苷(astragaloside Ⅳ,AsT Ⅳ)对由氧化应激损伤引起的线粒体功能障碍以及细胞凋亡的作用及机制。方法:体外培养人神经母细胞瘤sH-sy5y细胞,用过氧化氢(hydrogen peroxide,HO)诱导建立氧化应激模型,分为Pbs组、模型组(HO组)和HO+AsT Ⅳ组。应用ATP检测试剂盒检测细胞内ATP水平;用线粒体膜电位检测试剂盒JC-1检测细胞线粒体膜电位变化;应用western blot法检测线粒体呼吸链上的complex Ⅰ~Ⅴ,分别为NADH:泛醌氧化还原酶亚基b8(NADH:ubiquinone oxidoreductase subunit b8,NDUFb8;complex Ⅰ)、琥珀酸脱氢酶b(succinate dehydrogenase b,sDHb;complex Ⅱ)、泛醇-细胞色素C还原酶核心蛋白2(ubiquinol-cytochrome C reductase core protein 2,UqCrC2;complex Ⅲ)、细胞色素C氧化酶Ⅰ(mitochondrially encoded cytochrome C oxidase Ⅰ,MTCO1;complex Ⅳ)和ATP合酶F1亚基α(ATP synthase F1 subunit alpha,ATP5A;complex Ⅴ),检测线粒体动力学分裂蛋白——磷酸化发动蛋白相关蛋白1(phosporylated dynamin-related protein 1,p-Drp1)和线粒体分裂蛋白1(mitochondrial fission protein 1,Fis1),以及融合蛋白——线粒体融合蛋白1(mitofusin 1,Mfn1)、Mfn2和视神经萎缩症蛋白1(optic atrophy protein 1,OPA1),检测凋亡相关蛋白bcl-2、bax和cleaved caspase-3;采用免疫荧光染色法检测NDUFb8和MTCO1表达;采用TUNEL染色检测细胞凋亡。结果:在200μmol/L H_(2)O_(2)诱导的sy5y细胞氧化应激模型中,线粒体膜电位(Pb8、sDHb、ATP5A和MTCO1的表达均显著减少(Ps1(Prp1(Pbax和cleaved caspase-3蛋白水平显著升高(Pbcl-2表达量显著降低(PsT Ⅳ能够显著提高细胞线粒体膜电位(Pb8、sDHb、MTCO1、ATP5A及UqCrC2的表达(Prp1和Fis1蛋白水平(Pbcl-2表达(Pbax和cleaved caspase-3蛋白水平(PsT Ⅳ能够保护神经元,其可能的机制是通过改善线粒体功能,调控线粒体动力学分裂/融合平衡,从而减轻氧化应激损伤导致的神经元凋亡。

关键词：黄芪甲苷氧化应激线粒体 sH-sy5y细胞

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Estimating compositions of natural ringwoodite in the heavily shocked Grove Mountains 052049 meteorite from raman spectra

Estimating compositions of natural ringwoodite in the heavil...

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中国科学院地质与地球物理研究所第11届（2011年度）学术年会

作者： L.Feng,~(1,2) y.Lin,~(1,*) s.Hu,~(1,2) L.xu,~3 and b.Miao~4 1 Key Laboratory of the Earth’s Deep Interior,Institute of Geology and Geophysics,Chinese Academy of sciences,beijing 100029,China 2 Graduate school of Chinese Academy of sciences,beijing 100118,China 3 National Astronomical Observatory,Chinese Academy of sciences,beijing 100029,China 4 Department of resources and Environmental Engineering,Guilin University of Technology,Guilin 541004,China

A combined raman spectroscopy and electron probe microanalysis study of the heavily shocked Grove Mountains(GrV) 052049 meteorite revealed the largest chemical fractionation of natural ringwoodite,and composition-dependent variation of the intensities and/or wavenumbers of raman *** Fa content[atomic ratio of Fe/(Fe+Mg)]of ringwoodite varying from 27.8 to 81.6 mol%, the peak position of the single band around 290 cm(sb1),which relates to the siO translation mode,shifts from 296.0 to 284.6 cm,and one of the doublets around 790 cm(Db1),which relates to the symmetric stretching of siO,shifts from 796.3 to 782.7 *** addition,the relative intensities of sb1 and the other band of the doublet around 840 cm(Db2),which relates to asymmetric stretching of siO,increases with Fa *** on the paired raman-EPMA data,single-peak and two-peak calibrations were established,which can be used to derive Fa contents of ringwoodite from the raman *** accuracy of raman-derived Fa content of ringwoodite is better than±5 mol%.The correlation of sbl intensity with the Fa content of ringwoodite suggests that the vibration of sbl is enhanced with the substitution of Mg by *** correlation between raman spectra and the chemical composition of ringwoodite have potential applications in on-line measurement of high-pressure experiments and in situ mineralogical determination in future planetary explorations.

关键词： raman spectroscopy ringwoodite chemical compositions shocked meteorite

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refined families of Dothideomycetes:orders and families incertae sedis in Dothideomycetes

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Fungal Diversity 2020年第6期105卷 17-318页

作者： sinang Hongsanan Kevin D.Hyde rungtiwa Phookamsak Dhanushka N.wanasinghe Eric H.C.McKenzie V.Venkateswara sarma robert Lücking saranyaphat boonmee Jayarama D.bhat Ning-Guo Liu Danushka s.Tennakoon Dhandevi Pem Anuruddha Karunarathna shu-Hua Jiang Gareth E.b.Jones Alan J.L.Phillips Ishara s.Manawasinghe saowaluck Tibpromma subashini C.Jayasiri Diana sandamali ruvishika s.Jayawardena Nalin N.wijayawardene Anusha H.Ekanayaka rajesh Jeewon yong-Zhong Lu Chayanard Phukhamsakda Asha J.Dissanayake xiang-yu Zeng Zong-Long Luo qing Tian Kasun M.Thambugala Dongqin Dai Milan C.samarakoon K.w.Thilini Chethana Damien Ertz Mingkwan Doilom Jian-Kui(Jack)Liu sergio Pérez-Ortega Ave suija Chanokned senwanna subodini N.wijesinghe Mekala Niranjan sheng-Nan Zhang Hiran A.Ariyawansa Hong-bo Jiang Jin-Feng Zhang Chada Norphanphoun Nimali Ide silva Vinodhini Thiyagaraja Huang Zhang Jadson D.P.bezerra ricardo Miranda-González AndréAptroot Hiroyuki Kashiwadani Dulanjalee Harishchandra Emmanuël sérusiaux Pranami DAbeywickrama Dan-Feng bao bandarupalli Devadatha Hai-xia wu Kwang Hee Moon Cecile Gueidan Felix schumm Digvijayini bundhun Ausana Mapook Jutamart Monkai Chitrabhanu s.bhunjun Putarak Chomnunti satinee suetrong Napalai Chaiwan Monika C.Dayarathne Jing yang Achala r.rathnayaka Jian-Chu xu Jiesheng Zheng Gang Liu yao Feng Ning xie Guangdong Provincial Key Laboratory for Plant Epigenetics Shenzhen Key Laboratory of Microbial Genetic EngineeringCollege of Life Science and OceanographyShenzhen UniversityShenzhen 518060People’s Republic of China Center of Excellence in Fungal research Mae Fah Luang UniversityChiang Rai 57100Thailand CAs Key Laboratory for Plant Diversity and biogeography of East Asia(KLPb) Kunming Institute of BotanyChinese Academy of ScienceKunming 650201YunnanPeople’s Republic of China East and Central Asia regional Office World Agroforestry Centre(ICRAF)Kunming 650201YunnanPeople’s Republic of China Centre for Mountain Futures(CMF) Kunming Institute of BotanyKunming 650201YunnanPeople’s Republic of China Department of Entomology and Plant Pathology Faculty of AgricultureChiang Mai UniversityChiang Mai 50002Thailand Institute of Plant Health Zhongkai University of Agriculture and EngineeringHaizhu DistrictGuangzhou 510225People’s Republic of China world Agroforestry Centre East and Central Asia132 Lanhei RoadKunming 650201YunnanPeople’s Republic of China Manaaki whenua-Landcare research Private Mail Bag 92170AucklandNew Zealand Fungal biotechnology Lab Department of BiotechnologySchool of Life SciencesPondicherry UniversityKalapetPondicherry 605014India school of science Mae Fah Luang UniversityChiang Rai 57100Thailand botanischer Garten und botanisches Museum Freie Universität BerlinKönigin-Luise-Straße 6-814195 BerlinGermany 13128/1-J Azad Co-Op Housing SocietyCurcaP.O.Goa Velha 403108India Faculty of Agriculture Natural Resources and EnvironmentNaresuan UniversityPhitsanulok 65000Thailand Guizhou Key Laboratory of Agricultural biotechnology Guizhou Academy of Agricultural SciencesGuiyang 550006People’s Republic of China school of Life science and Technology University of Electronic Science and Technology of ChinaChengdu 611731People’s Republic of China state Key Laboratory of Mycology Institute of MicrobiologyChinese Academy of SciencesBeijing 100101People’s Republic of C

Numerous new taxa and classifications of Dothideomycetes have been published following the last monograph of families of Dothideomycetes in 2013.A recent publication by Honsanan et *** 2020 expanded information of families in Dothideo-mycetidae and Pleosporomycetidae with modern *** this paper,we provide a refined updated document on orders and families incertae sedis of *** family is provided with an updated description,notes,including figures to represent the morphology,a list of accepted genera,and economic and ecological *** also provide phylogenetic trees for each *** this study,31 orders which consist 50 families are assigned as orders incertae sedis in Dothideomycetes,and 41 families are treated as families incertae sedis due to lack of molecular or morphological *** new order,Catinellales,and four new families,Catinellaceae,Morenoinaceae Neobuelliellaceae and Thyrinulaceae are *** genera(Neobuelliella,Pseudomicrothyrium,Flagellostrigula,swinscowia,Macroconstrictolumina,Pseudobogoriella,and schummia)are *** new species(Acrospermum urticae,bogoriella complexoluminata,Dothiorella ostryae,Dyfrolomyces distoseptatus,Macroconstrictolumina megalateralis,Patellaria microspora,and Pseu-domicrothyrium thailandicum)are introduced base on morphology and phylogeny,together with two new records/reports and five new collections from different *** new combinations are also provided in this paper.

关键词： Abrothallales Ascrospermales Asterinales botryosphaeriales Catinellales Cladoriellales Collemopsidiales Dyfrolomycetales Eremithallales Eremomycetales Jahnulales Kirschsteiniotheliales Lembosinales Lichenotheliales Microthyriales Minutisphaerales Monoblastiales Murramarangomycetales new family new genera new order new species Parmulariales Patellariales Phaeotrichales Phylogeny stigmatodiscales strigulales superstratomycetales Taxonomy Trypetheliales Tubeufiales Valsariales Venturiales Zeloasperisporiales

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search for the doubly heavy baryons Ω^(0)_(bc) and E^(0)_(bc) decaying to Λ^(+)_(c)π^(-) and E^(+)_(c)π^(-)

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Chinese Physics C 2021年第9期45卷 10-21页

作者： r.Aaij C.Abelian beteta T.Ackernley b.Adeva M.Adinolfi H.Afshamia C.A.Aidala s.Aiola Z.Ajaltouni s.Aka J.Albrecht F.Alessio M.Alexander A.Alfonso Albero Z.Aliouche G.Alkhazov P.Alvarez Cartelie s.Amato y.Amhis L.An L.Anderlini A.Andreianov M.Andreotti F.Archilli A.Artamonov M.Artuso K.Arzymatov E.Aslanides M.Atzeni b.Audurier s.bachmann M.bachmayer J.J.back P.baladron rodriguez V.balagura w.baldini J.baptista Leite r.J.barlow s.barsuk w.barter M.bartolini F.baryshnikov J.M.basels G.bassi b.batsukh A.battig A.bay M.becker F.bedeschi I.bediaga A.beiter V.belavin s.belin V.bellee K.belous I.belov I.belyaev G.bencivenni E.ben-Haim A.berezhnoy *** D.beminghoff H.C.bernstein C.bertella A.bertolin C.betancourt F.betti Ia.bezshyiko s.bhasin J.bhom L.bian M.s.bieker s.bifani P.billoir M.birch F.C.r.bishop A.bitadze A.bizzeti M.bjorn M.P.blago T.blake F.blanc s.blusk D.bobulska J.A.boelhauve O.boente Garcia T.boettcher A.boldyrev A.bondar N.bondar s.borghi M.borisyak M.borsato J.T.borsuk s.A.bouchiba T.J.V.bowcock A.boyer C.bozzi M J.bradley s.braun A.brea rodriguez M.brodski J.brodzicka A.brossa Gonzalo D.brundu A.buonaura C.burr A.bursche A.butkevich J.s.butter J.buytaert w.byczynski s.Cadeddu H.Cai r.Calabrese L.Calefice L.Calero Diaz s.Cali r.Calladine M.Calvi M.Calvo Gomez P.Camargo Magalhaes A.Camboni P.Campana A.F.Campoverde quezada s.Capelli L.Capriotti A.Carbone G.Carboni r.Cardinale A.Cardini I.Carli P.Camiti L.Carus K.Carvalho Akiba A.Casais Vidal G.Casse M.Cattaneo G.Cavallero s.Celani J.Cerasoli A.J.Chadwick M.G.Chapman M.Charles Ph.Charpentier G.Chatzikonstantinidis C.A.Chavez barajas M.Chefdeville C.Chen s.Chen A.Chernov V.Chobanova s.Cholak M.Chrzaszcz A.Chubykin V.Chulikov P.Ciambrone M.F.Cicala x.Cid Vidal G.Ciezarek P.E.L.Clarke M.Clemencic H.V.Cliff J.Closier J.L.Cobbledick V.Coco J.A.b.Coelho J.Cogan E.Cogneras L.Cojocariu P.Collins T.Colombo L.Congedo A.Contu N.Cooke G.Coombs G.Corti C.M.Costa sobral b.Couturier D.C.Craik J.Crkovska M.Cruz Torres r.Currie C.L.Da silva E.Dall'Occo J.Dalseno C.D'Ambrosi Centro brasileiro de Pesquisas Fisicas(CbPF) Rio de JaneiroBrazil Universidade Federal do rio de Janeiro(UFrJ) Rio de JaneiroBrazil Center for High Energy Physics Tsinghua UniversityBeijingChina Institute of High Energy Physics(IHEP) BeijingChina school of Physics state Key Laboratory of Nuclear Physics and Technology Peking UniversityBeijingChina University ofChinese Academy of sciences BeijingChina Institute of Particle Physics Central China Normal UniversityWuhanHubeiChina Univ.savoie Mont blanc CNRSIN2P3-LAPPAnnecyFrance Universite Clermont Auvergne CNRS/IN2P3LPCClermont-FerrandFrance Aix Marseille Univ CNRS/IN2P3CPPMMarseilleFrance Universite Paris-saclay CNRS/IN2P3IJCLabOrsayFrance Laboratoire Leprince-ringuet CNRS/IN2P3Ecole PolytechniqueInstitut Polytechnique de ParisPalaiseauFrance LPNHE Sorbonne UniversiteParis Diderot Sorbonne Paris CiteCNRS/FN2P3ParisFrance I.Physikalisches Institut RWTH Aachen UniversityAachenGermany Fakultat Physik Technische Universitat DortmundDortmundGermany Max-Planck-Institut für Kemphysik(MPIK) HeidelbergGermany Physikalisches Institut Ruprecht-Karls-Universitat HeidelbergHeidelbergGermany school of Physics University College DublinDublinIreland INFN sezione di bari BariItaly INFN sezione di bologna BolognaItaly INFN sezione di Ferrara FerraraItaly INFN sezione di Firenze FirenzeItaly INFN Laboratori Nazionali di Frascati FrascatiItaly INFN sezione di Genova GenovaItaly INFN sezione di Milano MilanoItaly INFN sezione di Milano-bicocca MilanoItaly INFN sezione di Cagliari MonserratoItaly Universita degli studi di Padova Universita e INFNPadovaPadovaItaly INFN sezione di Pisa PisaItaly INFN sezione di roma La sapienza RomaItaly INFN sezione di roma Tor Vergata RomaItaly Nikhef National Institute for subatomic Physics AmsterdamNetherlands Nikhef National Institute for subatomic Physics and VU University Amsterdam AmsterdamNetherlands AGH-University of science and Technology Faculty of Physics and Applied Computer ScienceKr

The first search for the doubly heavyΩ^(0)_(bc)baryon and a search for the E^(0)_(bc)baryon are performed using pp collision data collected via the LHCb experiment from 2016 to 2018 at a centre-of-mass energy of 13 TeV,corresponding to an integrated luminosity of 5.2 fb^(-1).The baryons are reconstructed via their decays to Λ^(+)_(c)π^(-)and E^(+)_(c)π^(-).No significant excess is fbund for invariant masses between 6700 and 7300 MeV/c^(2),in a rapidity range from 2.0 to 4.5 and a transverse momentum range from 2 to 20 MeV/*** limits are set on the ratio of the Ω^(0)_(bc)and E^(0)_(bc)production cross-section times the branching fraction to Λ^(+)_(c)π^(-)(E^(+)_(c)π^(-))relative to that of the Λ^(0)_(b)(E^(0)_(b))baryon,for different lifetime hypotheses,at 95%confidence *** upper limits range from 0.5 x 10^(-4)to 2.5 x 10^(-4)for theΩ^(0)_(bc)→Λ^(+)_(c)π^(-)(E^(0)_(bc)→Λ^(+)_(c)π^(-))decay,and from 1.4x 10^(-3)to 6.9 x 10^(-3)for theΩ^(0)_(bc)→E^(+)_(c)π^(-)(E^(0)_(bc)→E^(+)_(c)π^(-))decay,depending on the considered mass and lifetime of theΩ^(0)_(bc)(E^(0)_(bc))baryon.

关键词： b physics quarkonium spectroscopy heavy quark production

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采用覆膜支架植入术治疗颅内动脉瘤后内漏的发生率和预测因素及远期通畅性:一项前瞻性的非随机多中心研究

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国际医学放射学杂志 2013年第2期 192-192页

作者： y.q. Zhu M.H. Li F. Lin D.L. song H.q. Tan b.x. Gu 李宁 Department of Diagnostic and Interventional radiology The Sixth Affiliated People’s Hospital Medical School of Shanghai Jiao Tong University

目的对颈内动脉(ICA)及椎动脉(VA)远端的颅内动脉瘤行覆膜支架植入治疗后即刻或迟发内漏及远期通畅性进行研究。方法对来自于3个中心的接受覆膜支架植入的41例病人的45个动脉瘤进行随访。观察指标包括动脉瘤闭塞率、内漏、远期支架内狭... 详细信息

目的对颈内动脉(ICA)及椎动脉(VA)远端的颅内动脉瘤行覆膜支架植入治疗后即刻或迟发内漏及远期通畅性进行研究。方法对来自于3个中心的接受覆膜支架植入的41例病人的45个动脉瘤进行随访。观察指标包括动脉瘤闭塞率、内漏、远期支架内狭窄率、临床症状改善、神经系统缺陷及死亡。结果动脉瘤总体排除率达69.2%(n=27),其中30.8%(n=12)当时发生内漏残留。血管造影随访[平均(43.5±14.3)个月]显示87.2%(n=34)表现为完全闭塞,只有12.8%(n=5)可见内漏残留。即刻内漏的预测因素包括支架数量(P=0.023)和支架直径(P=0.022),而迟发内漏的预测因素为支架直径(P=0.035)和支架角度(P=0.021)。从植入后开始,随访第2年和第6年的晚期支架狭窄率分别为(18.0±13.3)%和(29.0±18.5)%。吸烟(P=0.017)和支架角度(P=0.020)是晚期支架狭窄的预测因素。结论覆膜支架在治疗颅内willis环区域的动脉瘤方面具有可接受的即刻及晚期闭塞率和远期支架动脉通畅率。要点①覆膜支架可作为颅内动脉瘤治疗的选择方法。②治疗ICA和VA末端动脉瘤的技术成功率可达97.6%。③然而即刻及远期内漏的发生率分别为30.8%和12.8%。④支架数量、直径及角度是内漏发生的可能预测因素。⑤吸烟和支架角度似乎能够预测迟发支架内狭窄。

关键词：颅内动脉瘤覆膜支架内漏支架内狭窄多元回归分析

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Measurement of integrated luminosity and center-of-mass energy of data taken by bEsⅢ at s^(1/2)=2.125 GeV

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Chinese Physics C 2017年第11期41卷 1-9页

作者：麦迪娜 M.N.Achasov s.Ahmed 艾小聪 O.Albayrak M.Albrecht D.J.Ambrose A.Amoroso 安芬芬安琪白景芝 r.baldini Ferroli 班勇 D.w.bennett J.V.bennett N.berger M.bertani D.bettoni 边渐鸣 F.blanchi E.boger I.boyko r.A.briere 蔡浩蔡啸 O.Cakir A.Calcaterra 曹国富 s.A.Cetin J.Chai 常劲帆 G.Chelkov 陈刚陈和生陈江川陈玛丽陈实陈申见堪炫陈旭荣陈元柏程和平褚新坤 G.Cibinetto 代洪亮代建平 A.Dbeyssi D.Dedovich 邓子艳 A.Denig I.Denysenko M.Destefanis F.DEMori 丁勇董超董静董燎原董明义豆正磊杜书先段鹏飞范荆州方建房双世方馨方易 r.farinelli L.Fava O.Fedorov F.Feldbauer G.Felici 封常青 E.Fiorauanti M.Fritsch 傅成栋高清高鑫磊高原宁高榛 I.Garzia K.Goetzen 龚丽龚文煊 w.Gradl M.Greco 顾旻皓顾运厅管颖慧郭爱强郭立波郭如盼郭玥郭玉萍 Z.Haddadi A.Hafner 韩爽郝喜庆 F.A.Harris 何康林 F.H.Heinsius T.Held 衡月昆 T.Holtmann 侯治龙胡琛胡海明胡继峰胡涛胡誉黄光顺黄金书黄性涛黄晓忠黄勇黄智玲 T.Hussain 纪全姬清平季晓斌季筱璐姜鲁文江晓山蒋兴雨焦健斌焦铮金大鹏金山 T.Johansson A.Julin N.Kalantar-Nayestanaki 康晓琳康晓坤 M.Kavatsyuk 柯百谦 P.Kiese r.Kliemt b.Kloss O.b.Kolcu b.Kopf M.Kornicer A.Kupsc w.Kühn J.s.Lange M.Lara P.Larin H.Leithoff C.Leng 李翠李澄李德民李飞李峰云李刚李海波李惠静李家才李瑾李康李科李蕾李培荣李启云李腾李卫东李卫国李晓玲李小男李学潜李郁博李志兵梁昊梁勇飞梁羽铁廖广睿林德旭刘冰刘北江刘春秀刘栋刘福虎刘芳刘峰刘宏邦刘汇慧刘欢欢刘怀民刘杰刘建北刘觉平刘晶译刘凯刘魁勇刘兰雕刘佩莲刘倩刘树彬刘翔刘玉斌刘媛媛刘振安刘智青 H.Loehner 龙云飞娄辛丑吕海江吕军光卢宇卢云鹏罗成林罗民兴 T.Luo 罗小兰吕晓睿马凤才马海龙马连良马明明马秋梅马天马旭宁马骁妍马玉明 F.E.Maas M.Maggiora q.A.Malik 冒亚军毛泽普 s.Marcello J.G.Messchendorp G.Mezzadri 闵建闵天觉 r.E.Mitchell 莫晓虎莫玉俊 C.Morales Morales N.yu.Muchnoi H.Muramatsu P.Musiol y.Nefedov F.Nerling I.b.Nikolaev 宁哲 s.Nisar 牛顺利牛讯伊马鹏欧阳群 s.Pacetti 潘越 P.Patteri M.Pelizaeus 彭海平 K.Peters J.Pettersson 平加伦平荣刚 r.Poling V.Prasad 漆红荣祁鸣钱森乔从丰秦丽清覃拈秦小帅秦中华邱进发 K.H.rashid C.F.redmer M.ripka 荣刚 Ch.rosner 阮向东 A.sarantsev M.savrié C.schnier K.schoenning s.schumann 邵明沈成平沈培迅沈肖雁盛华义施萌宋维民宋欣颖 s.sosio s.spataro 孙功星孙俊峰孙胜森孙新华孙勇杰孙永昭孙志嘉孙振田唐昌建唐晓 I.Tapan E.H.Thorndike M.Tieinens I.Uman G.s.Varner 王斌王滨龙王东王大勇王科王亮亮王灵淑王萌王平王佩良王炜王维平王雄飞王越王雅迪王贻芳王亚乾王铮王志刚王志宏王至勇王宗源 T.weber 魏代会 P.weidenkaff 文硕频 U.wiedner M.wolke 伍灵慧吴连近吴智夏磊夏力钢夏宇肖栋肖浩肖振军谢宇广修青磊许国发徐静静徐雷徐庆君徐庆年徐新平严亮鄢文标闫文成颜永红杨海军杨洪勋杨柳杨永栩叶梅叶铭汉殷俊昊尤郑昀 Institute of High Energy Physics G.I.budker Institute of Nuclear Physics sb rAs (bINP) the Novosibirsk state University Helmholtz Institute Mainz Carnegie Mellon University bochum ruhr-University University of rochester University of Turin INFN University of science and Technology of China state Key Laboratory of Particle Detection and Electronics INFN Laboratori Nazionali di Frascati Peking University Indiana University Johannes Gutenberg University of Mainz INFN sezione di Ferrara University of Minnesota Joint Institute for Nuclear research the Moscow Institute of Physics and Technology wuhan University Ankara University Istanbul bilgi University the Functional Electronics Laboratory Tomsk State University University of Chinese Academy of sciences Nanjing University Lanzhou University Huangshan College shanghai Jiao Tong University Liaoning University Nankai University Zhengzhou University Tsinghua University University of Ferrara University of Eastern Piedmont GsI Helmholtzcentre for Heavy Ion research GmbH Guangxi University Nanjing Normal University KVI-CArT University of Groningen Henan Normal University University of Hawaii shandong University University of the Punjab Uppsala University Istanbul Arel University Justus-Liebig-Universitaet Giessen Ⅱ.Physikalisches Institut seoul National University Hangzhou Normal University beijing Institute of Petrochemical Technology beihang University sun yat-sen University sichuan University Guangxi Normal University shanxi University Central China Normal University Henan University of science and Technology University of Texas at Dallas Zhejiang University University of Hawaii Honolulu University of Minnesota Minneapolis COMsATs Institute of Information Technology INFN and University of Perugia Goethe University Frankfurt the NrC "Kurchatov Institute" PNPI Uludag University Near East University soochow University Hunan University University of south China China Center of Advanced science and Technology bogazici University University of science and Technology Liaoning

To study the nature of the state y（2175）,a dedicated data set of e ＋ e-collision data was collected at the center-of-mass energy of 2.125 GeV with the bEsⅢ detector at the bEPCⅡ *** analyzing large-angle bhabha scattering events,the integrated luminosity of this data set is determined to be 108.49±0.02±0.85 pb-1,where the first uncertainty is statistical and the second one is *** addition,the center-of-mass energy of the data set is determined with radiative dimuon events to be 2126.55±0.03±0.85 MeV,where the first uncertainty is statistical and the second one is systematic.

关键词： bhabha scattering luminosity radiative dimuon events center-of-mass energy

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