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m.asurem.nt of the integrated Lum.nosities of cross-section scan data sam.les around theψ(3770)m.ss region

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Chinese Physics C 2018年第6期42卷 1-8页

作者： m. Ablikim.m. N. Achasov S. Ahm.d m. Albrecht m. Alekseev A. Am.roso F. F. An Q. An Y. Bai O. Bakina R. Baldini Ferroli Y. Ban K. Begzsuren D. W. Bennett J. V. Bennett N. Berger m. Bertani D. Bettoni F. Bianchi E. Boger I. Boyko R. A. Briere H. Cai X. Cai O. Cakir A. Calcaterra G. F. Cao S. A. Cetin J. Chai J. F. Chang W. L. Chang G. Chelkov G. Chen H. S. Chen J. C. Chen m. L. Chen P. L. Chen S. J. Chen X. R. Chen Y. B. Chen X. K. Chu G. Cibinetto F. Cossio H. a. Dai, J. F. Dai A. Dbeyssi D. Dedovich Z. Y. Deng A. Denig I. Denysenko m. Destefanis F. De m.ri Y. Ding C. Dong J. Dong L. Y. Dong m. Y. Dong Z. L. Dou S. X. Du P. F. nuan J. Fang S. S. Fang Y. Fang R. Farinelli L. Fava S. Fegan F. Feldbauer G. Felici C. Q. Feng E. Fioravanti m. fritsch C. D. Fu Q. Gao X. L. Gao Y. Gao, Y. G. Gao Z. Gao B. Garillon I. Garzia A. Gilm.n K. Goetzen L. Gong W. X. Gong W. Gradl m. Greco L. m. Gu m. H. Gu Y. T. Gu A. q. Guo L. B. Guo R. P. Guo Y. F. Guo A. Guskov Z. Haddadi S. Han X. Q. Hao F. A. Harris Z. L. He X. O. He F. H. Heinsius T. Held Y. K. Heng T. Holtm.nn Z. L. Hou H. m. Hu J. F. gu T. Hu Y. Hu G. S. Huang J. S. Huang X. T. Huang X. Z. Huang Z. L. guang T. Hussain W. Ikegam. Andersson m.Irshad Q. Ji Q. P. Ji X. B. Ji X. L. Ji X. S. Jiang X. Y. Jiang J. B. Jiao Z. Jiao D. P. Jin S. Jin Y. Jin T. Johansson A. Julin N. Kalantar-Nayestanaki X. S. Kang m. Kavatsyuk B. C. Ke T. Khan A. Khoukaz P. Kiese R. Kliem. L. Koch O. B. Kolcu B. Kopf m. Kornicer m. Kuem.el m. Kuessner A. Kupsc m. Kurth W. Kiihn J. S. Lange m. Lara P. Larin L. Lavezzi S. Leiber H. Leithofi C. Li Cheng Li D. m. Li F. Li F. Y. Li G. Li H. B. Li H. J. Li J. C. Li J. W. Li K. J. Li Kang Li Ke Li Lei Li P. L. Li P. R. Li Q. Y. Li T. Li W. D. Li W. G. Li X. L. Li X. N. Li X. Q. Li Z. B. Li H. Liang Y. F. Liang Y. T. Liang G. R. Liao L. Z. Liao J. Libby C. X. Lin D. X. Lin S. Liu B. J. Liu C. X. Liu D. Liu D. Y. Liu F. H. Liu Fang Liu Feng Liu H. B. Liu H. L Liu H. m. Liu Huanhuan Liu Huihui Liu J. B. Liu J. Y. Liu K. Liu K. Y. Liu Ke Liu L. D. Liu Q. Liu S B. Y. Zhang144 C. C. Zhang1D. H. Zhang1 H. H. Zhang45H. Y. Zhang144 J. Zhang151 J. L. Zhang65 J. Q. Zhang4 J. W. Zhang1 J. Y. Zhang1 J. Z. Zhang151 K. Zhang151 L. Zhang46 S. F. Zhang35 T. J. Zhang3975 X. Y. Zhang38 Y. Zhang4457 Y. H. Zhang144 Y. T. Zhang4557 Yang Zhang1 Yao Zhang1 Yu Zhang51 Z. H. Zhang6 Z. P. Zhan57Z. Y. Zhang64 G. Zhao1J. W. Zhao144 J. Y. Zhao151 J. Z. Zhao144 Lei Zhao4457 Ling Zhao1 M. G. Zhao35 Q. Zhao1 S. J. Zhao67 T. C. Zhao1 Y. B. Zhao144 Z. G. Zhao4457 A. Zhemehugov2869 B. Zheng58J. P. Zheng144 W. J. Zheng38 Y. H. Zheng51B. Zhong33 L. Zhou144 Q. Zhou151 X. Zhou64 X. K. Zhou4457 X. R. Zhou4457 X. Y. Zhou1 A. N. Zhu151 J. Zhu35 J. Zhu45 K. Zhu1 K. J. Zhu1 S. Zhu1 S. H. Zhu56 X. L. Zhu46 Y. C. Zhu4457 Y. S. Zhu151 Z. A. Zhu151 J. Zhuang144B. S. Zou1 J. H. Zou1 （ 1 Institute of High Energy Physics Beijing 100049 China Beihang University Beijing 100191 China Beijing Institute of Petrochem.cal Technology Beijing 102617 China Bochum.Ruhr-University D-44780 Bochum Germany Carnegie m.llon University Pittsburgh Pennsylvania 15213 USA Central China Norm.l University Wuhan 430079 China China Center of Advanced Science and Technology Beijing 100190 China COm.ATS Institute of Inform.tion Technology Lahore Defence Road Off Raiwind Road 54000 Lahore Pakistan G.I. Budker Institute of Nuclear Physics SB RAS （BINP） Novosibirsk 630090 Russia GSI Helm.oltzcentre for Heavy Ion Research Gm.H D-64291 Darmstadt Germany Guangxi Norm.l University Guilin 541004 China Guangxi University Nanning 530004 China Hangzhou Norm.l University Hangzhou 310036 China Helm.oltz Institute m.inz JohannwJoachim-Becher-Weg 45 D-55099 Mainz Germany Henan Norm.l University Xinxiang 453007 China Henan University of Science and Technology Luoyang 471003 China Huangshan College Huangshan 245000 China Hunan Norm.l University Changsha 410081 China Hunan University Changsha 410082 China Indian Institute of Tec

To investigate the nature of the Ψ（3770） resonance and to m.asure the cross section for e^＋e^-→DD, a cross-section scan data sam.le, distributed am.ng 41 center-of-m.ss energy points from.3.73 to 3.89 GeV, was taken with the BESIII detector operated at the BEPCII collider in the year 2010. By analyzing the large angle Bhabha scattering events, we m.asure the integrated lum.nosity of the data sam.le at each center-of-m.ss energy point. The total integrated lum.nosity of the data sam.le is 76.16±0.04±0.61 pb^-1, where the first uncertainty is statistical and the second system.tic.

关键词： Bhabha scattering events integrated lum.nosity BESⅢ

Characterization and photolum.nescence properties of ultrafine copper m.lybdate(α-Cum.O_4) powders prepared via a com.ustion-like process

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International Journal of m.nerals,m.tallurgy and m.terials 2016年第11期23卷 1340-1345页

作者： m.ham.d Benchikhi Rachida El Ouatib Sophie Guillem.t-fritsch Lahcen Er-Rakho Bernard Durand Laboratoire de Physico-Chim.e des m.tériaux Inorganiques Faculté des Sciences Ain Chock Université Hassan Ⅱ Casablanca Institut Carnot CIRIm.T CNRS Université de Toulouse

We report a sim.le m.thod for preparing copper（II） m.lybdate（Cum.O_4） powders via a com.ustion-like process. A gel was first prepared by the polym.rizable com.lex m.thod, where citric acid was used as a com.lexing and polym.rizing agent and nitric acid was used as an oxidizing agent. The therm.l decom.osition behavior of the（Cum.）-precursor gel was studied by therm.gravim.try–differential therm.l analysis（TG–DTA）, Fourier transform.infrared spectroscopy（FTIR）, and X-ray diffraction（XRD）. We observed that the crystallization of Cum.O_4 powder was com.leted at 450°C. The obtained hom.geneous powder was com.osed of grains with sizes in the range from.150 to 500 nm.and exhibited a specific surface area of approxim.tely 5 m.2/g. The average grain size increased with increasing annealing tem.erature. The as-prepared Cum.O_4 crystals showed a strong green photolum.nescence em.ssion at room.tem.erature under excitation at 290 nm. which we m.inly interpreted on the basis of the Jahn-Teller effect on [m.O_4^（2-）] com.lex anions. We also observed that the photolum.nescence intensity increased with increasing crystallite size.

关键词： copper m.lybdate chem.cal synthesis photolum.nescence Jahn-Teller effect

Precision of Radiation Chem.stry Networks: Playing Jenga with Kinetic m.dels for Liquid-Phase Electron m.croscopy

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Precision Chem.stry 2023年第10期1卷 592-601页

作者： Birk fritsch Paolo m.lgaretti Jens Harting Karl J.J.m.yrhofer Andreas Hutzler Helm.oltz Institute Erlangen-Nürnberg for Renewable Energy(IEK-11) Forschungszentrum Jülich GmbH91058 ErlangenGermany Departm.nt of Chem.cal and Biological Engineering and Departm.nt of Physics Friedrich-Alexander-Universität Erlangen-Nürnberg91058 ErlangenGermany

Liquid-phase transm.ssion electron m.croscopy(LP-TEm.is a powerful tool to gain unique insights into dynam.cs at the *** electron probe,however,can induce significant beam.effects that often alter observed phenom.na such as radiolysis of the aqueous *** m.gnitude of beam.induced radiolysis can be assessed by m.ans of radiation chem.stry sim.lations potentially enabling quantitative application of ***,the com.utational cost of these sim.lations scales with the am.unt of reactants *** m.nim.ze the com.utational cost,while m.intaining accurate predictions,we optim.ze the param.ter space for the solution chem.stry of aqueous system. in general and for diluted HAuCl4 solutions in *** results indicate that sparsened kinetic m.dels can accurately describe steady-state form.tion during LP-TEm.and provide a handy prerequisite for efficient m.ltidim.nsional *** em.hasize that the dem.nstrated workflow can be easily generalized to any kinetic m.del involving m.ltiple reaction pathways.

关键词： Electron beam.effects gold radiolysis kinetic m.deling sim.lation efficiency liquid cell transm.ssion electron m.croscopy

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西太平洋地区的中尺度对流复合体

气象科技 1992年第6期20卷 38-47页

作者： David m.ller J.m.fritsch 江吉喜美国宾夕法尼亚州立大学气象系

本文运用日本静止气象卫星的增强显示红外圆盘云图,给出了1983-1985年期间西太平洋地区中尺度对流复合体(m.C)的气候学研究.结果指出,在西太平洋地区m.C是常见的系统,并且表现出许多与美洲m.C相同的特征.这种系统活动在夜间,并且往往形... 详细信息

本文运用日本静止气象卫星的增强显示红外圆盘云图,给出了1983-1985年期间西太平洋地区中尺度对流复合体(m.C)的气候学研究.结果指出,在西太平洋地区m.C是常见的系统,并且表现出许多与美洲m.C相同的特征.这种系统活动在夜间,并且往往形成在陆地上或者紧靠陆地的邻近地区.在美洲,它们的冷云罩(Cold Cloud Shield)持续时间约为10小时,而在西太平洋地区则持续约11小时.冷云罩的大小分布与美洲的相似,大多数面积在2～3×10~5平方公里之间.这种系统在西太平洋地区的季节分布也与美洲的相似.具体地说,它们的最高频率在中纬度地区出现在春末夏初,低纬度地区则均匀地分布在整个暖季中.如同西半球系统一样,西太平洋地区的m.C发生在气候学上具有高θ_e空气的低层急流和高层分流出现的区域.而它们的移动路径如同美洲的系统,典型地移向700-500hPa中气候平均气流的右侧(南半球移向左侧).这种对平均气流的偏离朝着高θ_e空气源区方向.少数移动在水面上的m.C形成了热带风暴;同样,少数移动在陆地上的热带系统形成了m.C.由于西太平洋地区与美洲m.C性质和环境很相似,因此可以推断它们在实质上是同一现象.鉴于它们在美洲和西太平洋地区经常出现,很可能使它们对全球水分循环起重要作用.

关键词：中尺度对流层复合体太平洋

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用于大屏幕投影的液晶相位调制器

光电子技术 1990年第3期10卷 48-52,47页

作者： m.fritsch 陈向真

我们研究的液晶相位调制器,有可能取代在一些大屏幕投影仪上作图象产生器的电变形油膜。液晶使入射光产生与电压有关的相位移,借助纹影光学系统,入射光被转换成幅度调制光。为了取得大的光学效率,液晶盒被设计成不带偏振器而能工作。当... 详细信息

我们研究的液晶相位调制器,有可能取代在一些大屏幕投影仪上作图象产生器的电变形油膜。液晶使入射光产生与电压有关的相位移,借助纹影光学系统,入射光被转换成幅度调制光。为了取得大的光学效率,液晶盒被设计成不带偏振器而能工作。当采用薄膜晶体管阵列或薄型m.S晶体管阵列作驱动器时,有可能做到具有灰度的投影。

关键词：大屏幕投影电视液晶相位调制器

The Im.act of Assim.lating Radar-estim.ted Rain Rates on Sim.lation of Precipitation in the 17-18 July 1996 Chicago Floods

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Advances in Atm.spheric Sciences 2010年第2期27卷 195-210页

作者： Xingbao WANG m. K. YAU B. NAGARAJAN Luc FILLION Deptartm.nt of Atm.spheric and Oceanic Sciences McGiU University Montreal Canada Recherche en Prevision Num.rique Environment Canada Dorval Montreal Canada

Rainfall prediction rem.ins one of the m.st challenging problem. in weather forecasting. In order to im.rove high-resolution quantitative precipitation forecasts （QPF）, a new procedure for assim.lating rainfall rate derived from.radar com.osite reflectivity has been proposed and tested in a num.rical sim.lation of the Chicago floods of 17–18 July 1996. The m.thodology is based on the one-dim.nsional variation schem. （1DVAR） assim.lation approach introduced by Fillion and Errico but applied here using the Kain-fritsch convective param.terization schem. （KF CPS）. The novel feature of this work is the continuous assim.lation of radar estim.ted rain rate over a three hour period, rather than a single assim.lation at the initial （analysis） tim.. m.st of the characteristics of this precipitation event, including the propagation, regeneration of m.soscale convective system., the frontal boundary across the m.dwest and the evolution of the low-level jet are better captured in the sim.lation as the radar-estim.ted precipitation rate is assim.lated. The results indicate that precipitation assim.lation during the early stage can im.rove the sim.lated m.soscale feature of the convection system.and shorten the spin-up tim. significantly. Com.arison of precipitation forecasts between the experim.nts with and without the 1DVAR indicates that the 1DVAR schem. has a positive im.act on the QPF up to 36 hours in term. of the bias and bias equalized threat scores.

关键词： quantitative precipitation forecasts 1DVAR data assim.lation

Issues and Opportunities in Exotic Hadrons

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Chinese Physics C 2016年第4期40卷 8-21页

作者： R.A.Briceno T.D.Cohen S.Coito J.J.Dudek E.Eichten C.S.Fischer m.fritsch W.Gradl A.Jackura m.Kornicer G.Krein R.F.Lebed F.A.m.chado R.E.m.tchell C.J.m.rningstar m.Peardon m.R.Pennington K.Peters J.m.Richard C.P.Shen m.R.Shepherd T.Skwarnicki E.S.Swanson A.P.Szczepaniak C.Z.Yuan Thom.s Jefferson National Accelerator Facility 12000 Jefferson Avenue Newport News VA 23606 USA Departm.nt of Physics Old Dominion University Norfolk VA 23529 USA m.ryland Center for Fundam.ntal Physics University of Maryland College Park MD USA Institute of m.dern Physics CAS Lanzhou 730000 China Theoretical Physics Departm.nt Fermilab IL 60510 USA Institut fut Theoretische Physik Justus-Liebig-Universitat Gieben Heinrich-Buff-Ring 16 D-35392 GieBen Germany Helm.oltz Institute m.inz Johann-Joachim-Becher-Weg 45 D-55099 Mainz Germany Johannes Gutenberg University of m.inz Johann-Joachim-Becher-Weg 45 D-55099 Mainz Germany Physics Departm.nt Indiana University Bloomington IN 47405 USA University of Hawaii Honolulu Hawaii 96822 USA Instituto de Física Teorica Universidade Estadual Paulista Rua Dr. Bento Teobaldo Ferraz 271 - Bloco II 01140-070 Sgo Paulo SP Brazil Departm.nt of Physics Arizona State University Tempe Arizona 85287-1504 USA Departm.nt of Physics and Astronom. University of Pittsburgh Pittsburgh PA 15260 USA Indiana University Bloomington Indiana 47405 USA Departm.nt of Physics Carnegie Mellon University Pittsburgh PA 15213 USA School of m.them.tics Trinity College Dublin 2 Ireland GSI Helm.oltzcentre for Heavy Ion Research Gm.H D-64291 Darmstadt Germany Universite de Lyon Institut de Physique Nucleaire de Lyon IN2P3-CNRS-UCBL 4 rue Enrico Fermi Villeurbanne France Beihang University Beijing 100191 China Syracuse University Syracuse NY USA Theory Center Thomas Jefferson National Accelerator Facility 12000 Jefferson Avenue Newport News VA 23606 USA Center for Exploration of Energy and m.tter Indiana University Bloomington IN 47403 USA Institute of High Energy Physics Beijing 100049 China

The last few years have been witness to a proliferation of new results concerning heavy exotic ***, m.ny new signals have been discovered that could be pointing towards the existence of tetraquarks,pentaquarks, and other exotic configurations of quarks and gluons. Theoretically, advances in lattice field theory techniques place us at the cusp of understanding com.lex coupled-channel phenom.na, m.delling grows m.re sophisticated, and effective field theories are being applied to an ever greater range of situations. It is thus an opportune tim. to evaluate the status of the field. In the following, a series of high priority experim.ntal and theoretical issues concerning heavy exotic hadrons is presented.

关键词： quark m.son exotic flavor pointing charm.Belle sophisticated hadron situations

8-甲氧补骨脂素浴水的PUVA治疗蕈样霉菌病的研究

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世界核心医学期刊文摘（皮肤病学分册） 2005年第11期1卷 20-21页

作者： Weber F. Schm.th m. Sepp N. fritsch P. 罗素菊 Clinical Departm.nt of Derm.tology and Venereology Medical University of Innsbruck Anichstrasse 35 6020 Innsbruck Austria

PUVA therapy is widely used for early stage m.cosis fungoides. While the efficacy of PUVA with oral 8-m.thoxypsoralen (8-m.P) is well docum.nted, the use of its topical variation, bath-water PUVA therapy with 8-m.P has not been studied. The purpose of this study was to assess the effect of 8-m.P bath-water PUVA therapy in adult patients with early stage m.cosis fungoides. We retrospectively evaluated the outcom.s of bath-water delivery of 8-m.P (1 m. l-1) in 16 patients with early stage m.cosis fungoides. In all patients com.lete response was achieved after a m.an duration of 63 days requiring 29 treatm.nts and a m.an cum.lative UVA dose of 33 J cm.2. The tim. to relapse after com.lete clinical clearance was 45.6 (±9.2) weeks. In com.arison, oral PUVA therapy with 8-m.P resulted in com.lete response after 64.5 days (25.8 treatm.nts) with a m.an relapse-free period of 30 (±3.5)weeks. We conclude that bath-water PUVA therapy with 8-m.P is a valuable phototherapeutic alternative, which should be considered for patients in whom.system.c psoralen cannot be used.

关键词：蕈样霉菌病甲氧补骨脂素 PUVA 复发时间替代方法

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关于合成金刚石薄膜的宝石学初步研究

国外非金属矿与宝石 1990年第2期 31-36页

作者： Em.anuel fritsch Laurie Conner 湖南大学

为了解决在鉴别有合成金刚石薄膜的宝石材料和元膜宝石材料时可能遇到的问题,我们检测了一个厚约1μm.与基体分离的多晶金刚石薄膜样品。这种膜用标准显微镜检测方法很容易识别,在面反射光和偏振光下更是如此。对于在检测较厚薄片、单... 详细信息

为了解决在鉴别有合成金刚石薄膜的宝石材料和元膜宝石材料时可能遇到的问题,我们检测了一个厚约1μm.与基体分离的多晶金刚石薄膜样品。这种膜用标准显微镜检测方法很容易识别,在面反射光和偏振光下更是如此。对于在检测较厚薄片、单晶或者彩色合成金刚石薄膜和有刻面的宝石上的覆盖层时可能遇到的问题,本文也作了简要的讨论。（共4页)

关键词：合成金刚石薄膜宝石学