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中学生英语 2002年第20期 1-1页

作者： janice Kuharaki 胡泽嘉

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增强规模化学习的创新--第五届国际计算机学会规模化学习会议概述

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开放学习研究 2018年第5期23卷 1-7,19页

作者： [美]李海英 [美]陈伯栋 [美]珍妮丝·戈贝尔罗格斯大学教育研究院美国新不伦瑞克08904 明尼苏达大学课程与教学系美国明尼阿波利斯55455

规模化学习主要研究大规模、基于技术的、以学习者为中心的学习环境,而学习环境往往依赖复杂的数据储存、数据传送、数据计算、学习环境界面设计以及智能师生对话设计。2018年6月26日至28日,第五届国际计算机学会(ACm)规模化学习会议(Le... 详细信息

规模化学习主要研究大规模、基于技术的、以学习者为中心的学习环境,而学习环境往往依赖复杂的数据储存、数据传送、数据计算、学习环境界面设计以及智能师生对话设计。2018年6月26日至28日,第五届国际计算机学会(ACm)规模化学习会议(Learning at Scale,简称L@S)在英国伦敦召开,本届大会的主题为"增强规模化学习的创新"。大会探讨了新时代下规模化学习和强化学习的创新研究,开发自动化评估和学生知识模型,提供自动化反馈以及学习干预,提高规模化学习系统的智适应性。此外,学者分别就在线学位政策和流程、反馈系统及其自动化发展以及测试试题新类型等三个议题分享了最新研究成果。本文先简要介绍大会总体情况,然后概括分析大会主旨发言、主要议题,并对会议代表性论文进行评述,最后论述规模化学习未来的研究发展趋势。

关键词：规模化学习网络学位慕课智适应

采用气化、加氢、发电工艺一体化联产技术提高炼油厂的经济效益

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化肥工业 2000年第6期27卷 9-17页

作者： ClintF.Penrose PaulS.Wallace janiceL.Kasbaum m.KayAnderson WilliamE.Preston 邵群颖江涌董宏海 JimmyWu TexacoPower&Gasification 德士古气化服务有限公司昆山215337

采用气化、加氢、发电工艺一体化联产技术对重油提炼利用 ,不但节省了大量的投资和操作费用、提高了整个工厂的运行可靠性和效率、降低有害物质的排放 ,而且提高了炼油装置和油田的灵活性。其中德士古气化工艺把沥青和石油焦副产品转化... 详细信息

采用气化、加氢、发电工艺一体化联产技术对重油提炼利用 ,不但节省了大量的投资和操作费用、提高了整个工厂的运行可靠性和效率、降低有害物质的排放 ,而且提高了炼油装置和油田的灵活性。其中德士古气化工艺把沥青和石油焦副产品转化为洁净的合成气是实现联产工艺的基础。

关键词：德士古气化联产气化加氢发电合成气沥青石油焦副产

Study of the production of Λ_b^0 band ~0 hadrons in pp collisions and first measurement of the Λ_b^0→J/ψpK^- branching fraction

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Chinese Physics C 2016年第1期40卷 1-16页

作者： O.Kochebina m.Kolpin I.Komarov R.F.Koopman P.Koppenburg m.Kozeiha L.Kravchuk K.Kreplin m.Kreps G.Krocker P.Krokovny F.Kruse W.Krzemien W.Kucewicz m.Kucharczyk V.Kudryavtsev A.K.Kuonen K.Kurek T.Kvaratskheliya D.Lacarrere G.Lafferty A.Lai D.Lambert G.Lanffanchi C.Langenbruch B.Langhans T.Latham C.Lazzeroni R.Le Gac J.van Leerdam J.-P.Lees R.Lefevre A.Leflat J.Lefrancois E.Lemos Cid O.Leroy T.Lesiak B.Leverington Y.Li T.Likhomanenko m.Liles R.Lindner C.Linn F.Lionetto B.Liu X.Liu D.Loh I.Longstaff J.H.Lopes D.Lucchesi m.Lucio martinez H.Luo A.Lupato E.Luppi O.Lupton A.Lusiani F.machefert F.maciuc O.maev K.maguire S.malde A.malinin G.manca G.mancinelli P.manning A.mapelli J.maratas J.F.marchand U.marconi C.marin Benito P.marino J.marks G.martellottil m.martin m.martinelli D.martinez Santos F.martinez Vidal D.martins Tostes A.massafferri R.matev A.mathad Z.mathe C.matteuzzi A.mauri B.maurin A.mazurov m.mcCann J.mcCarthy A.mcNab R.mcNulty B.meadows F.meier m.meissner D.melnychuk m.merk E michielin D.A.milanes m.-N.minard D.S.mitzel J.molina Rodrigue I.A.monroy S.monteil m.morandin P.morawski A.morda m.J.morello J.moron A.B.morris R.mountain F.muheim D.miiller J.muller K.muller V.muller m.mussini B.muster P.Naik T.Nakada R.Nandakumar A.Nandi I.Nasteva m.Needham N.Neri S.Neubert N.Neufeld m.Neuner A.D.Nguyen T.D.Nguyen C.Nguyen-mau V.Niess R.Niet N.Nikitin T.Nikodem D.Ninci A.Novoselov D.P.O'Hanlon A.Oblakowska-mucha V.Obraztsov S.Ogilvy O.Okhrimenko R.Oldeman C.J.G.Onderwater B.Osorio Rodrigues J.m.Otalora Goicochea A.Otto P.Owen A.Oyanguren A.Palano F.Palombo m.Palutan J.Panman A.Papanestis m.Pappagallo L.L.Pappalardo C.Pappenheimer C.Parkes G.Passaleva G.D.Patel m.Patel C.Patrignani A.Pearce A.Pellegrino G.Penso m.Pepe Altarelli S.Perazzini P.Perret L.Pescatore K.Petridis A.Petrolini m.Petruzzo E.Picatoste Olloqui B.Pietrzyk T:.Pilar D.Pinci A.Pistone A.Piucci S.Playfer m.Plo Casasus T.Poikela F.Polci A.Poluektov I.Polyakov E.Polycarpo A.Popov D.Popov B.Popovici C.Potterat E.Price J.D.Price J.Prisciandaro A.Pritchard Centro Brasileiro de Pesquisas Ffsicas(CBPF) Rio de JaneiroBrazil Universidade Federal do Rio de Janeiro(UFRJ) Rio de JaneiroBrazil Center for High Energy Physics Tsinghua UniversityBeijingChina LAPP Universite Savoie Mont-BlancCNRS/IN2P3Annecy-Le-VieuxFrance Clermont Universite Universite Blaise PascalCNRS/IN2P3LPCclermont-FerrandFrance CPPm Aix-Marseille UniversitYCNRS/IN2P3MarseilleFrance LAL Universite Paris-SudCNRS/IN2P3OrsayFrance LPNHE Universite Pierre et Marie CurieUniversite Paris DiderotCNRS/IN2P3ParisFrance Fakultat Physik Technische Universitat DortmundDortmundGermany max-Planck-lnstitut fur Kernphysik(mPIK) HeidelbergGermany Physikalisches Institut Ruprecht-Karls-Universitat HeidelbergHeidelbergGermany School of Physics University College DublinDublinIreland Sezione INFN di Bari BariItaly Sezione INFN di Bologna BolognaItaly Sezione INFN di Cagliari CagliariItaly Sezione INFN di Ferrara FerraraItaly Sezione INFN di Firenze FirenzeItaly Laboratori Nazionali dell'INFN di Prascati FrascatiItaly Sezione INFN di Genova GenovaItaly Sezione INFN di milnno Bicocca MilunoItaly Sezione INFN di milano MilanoItaly Sezione INFN di Padova PadovaItaly Sezione INFN di Pisa PisaItaly Sezione INFN di Roma Tor Vergata RomaItaly Sezione INFN di Roma La Sapienza RomaItaly Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences Krak6wPoland AGH-University of Science and Technology Faculty of Physics and Applied Computer ScienceKrakowPoland National Center for Nuclear Research(NCBJ) WarsawPoland Horia Hulubei National Institute of Physics and Nuclear Engineering Bucharest-MagureleRomania Petersburg Nuclear Physics Institute(PNPI) GatchinaRussia Institute of Theoretical and Experimental Physics(ITEP) MoscowRussia Institute of Nuclear Physics Moscow State University(SINP MSU)MoscowRussia Institute for Nuclear Research of the Russian Academy of Sciences(INR RAN) MoscowRussia Budker Institute of Nuclear Physics(SB RAS)and Novosibirsk State University No

The product of the ∧0/b （-B/0） differential production cross-section and the branching fraction of the decay ∧0/b→ J/ψ pK-（-B/0→ J/ψ-K＊（892）0）is measured as a function of the beauty hadron transverse momentum, PT, and rapidity, y. The kinematic region of the measurements is pT〈20 GeV/c and 2.0 〈g〈*** measurements use a data sample corresponding to an integrated luminosity of 3fb-1 collected by the LHCb detector in pp collisions at centre-of-mass energies √s=7 TeV in 2011 and √s=8 TeV in 2012. Based on previous LHCb results of the fragmentation fraction ratio,f∧0/b/fd,the branching fraction of the decay ∧0/b→ J/ψ pK-is measured to be B（∧0/b→ J/ψ pK-）=（3.17±0.04±0.07±0.34＋0.45/-0.28）×10-4,where the first uncertainty is statistical, the second is systematic, the third is due to the uncertainty on the branching fraction of the decay -B/0 →J/ψ-K＊（892）0,and the fourth is due to the knowledge of f∧0/b/*** sum of the asymmetries in the production and decay between ∧0/b and ∧0/bis also measured as a function of PT and *** previously published branching fraction of ∧0/b→ J/ψ pπ-,relative to that of ∧0/b→ J/ψ pK-,is updated. The branching fractions of ∧0/b→P＋c（→ J/ψp）K-are determined.

关键词： production cross-section branching fraction b hadrons proton-proton collisions

DEVELOPmENT OF HIGHLY POTENT,SELECTIVE,AND ORALLY AVAILABLE NON-AmIDINE FACTOR XA INHIBITORS.

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DEVELOPMENT OF HIGHLY POTENT,SELECTIVE,AND ORALLY AVAILABLE ...

Search for the doubly charmed baryon ■

40th IUPAC Congress

作者： marc Adler Sarah Cheeseman Yuo-Ling Chou David D. Davey Keith A. Eagen Richard Fitch Brian D. Griedel janice Heidersbach Rushad Karanjawala Wheeseong Lee Dao Lentz Amy Liang michael m. morrissey Gary B. Phillips Joseph Post Karna L. Sacchi Steven T. Sakata Kenneth J. Shaw R. michael Snider Babu Subramanyam Lan Trinh Ron Vergona Janette Walters Kathy A. White marc Whitlow Shung C. Wu monica J. Kochanny Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA Berlex Biosciences 2600 Hilltop DriveRichmondCA 94804USA

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Science China(Physics,mechanics & Astronomy) 2020年第2期63卷 8-22页

作者： R.Aaij C.Abellán Beteta T.Ackernley B.Adeva m.Adinolfi H.Afsharnia C.A.Aidala S.Aiola Z.Ajaltouni S.Akar P.Albicocco J.Albrecht F.Alessio m.Alexander A.Alfonso Albero G.Alkhazov P.Alvarez Cartelle A.A.Alves Jr S.Amato Y.Amhis L.An L.Anderlini G.Andreassi m.Andreotti F.Archilli J.Arnau Romeu A.Artamonov m.Artuso K.Arzymatov E.Aslanides m.Atzeni B.Audurier S.Bachmann J.J.Back S.Baker V.Balagura W.Baldini A.Baranov R.J.Barlow S.Barsuk W.Barter m.Bartolini F.Baryshnikov G.Bassi V.Batozskaya B.Batsukh A.Battig V.Battista A.Bay m.Becker F.Bedeschi I.Bediaga A.Beiter L.J.Bel V.Belavin S.Belin N.Beliy V.Bellee K.Belous I.Belyaev G.Bencivenni E.Ben-Haim S.Benson S.Beranek A.Berezhnoy *** D.Berninghoff H.C.Bernstein E.Bertholet A.Bertolin C.Betancourt F.Betti m.O.Bettler Ia.Bezshyiko S.Bhasin J.Bhom m.S.Bieker S.Bifani P.Billoir A.Birnkraut A.Bizzeti m.Bjφrn m.P.Blago T.Blake F.Blanc S.Blusk D.Bobulska V.Bocci O.Boente Garcia T.Boettcher A.Boldyrev A.Bondar N.Bondar S.Borghi m.Borisyak m.Borsato J.T.Borsuk T.J.V.Bowcock C.Bozzi S.Braun A.Brea Rodriguez m.Brodski J.Brodzicka A.Brossa Gonzalo D.Brundu E.Buchanan A.Buonaura C.Burr A.Bursche J.S.Butter J.Buytaert W.Byczynski S.Cadeddu H.Cai R.Calabrese S.Cali R.Calladine m.Calvi m.Calvo Gomez A.Camboni P.Campana D.H.Campora Perez L.Capriotti A.Carbone G.Carboni R.Cardinale A.Cardini P.Carniti K.Carvalho Akiba A.Casais Vidal G.Casse m.Cattaneo G.Cavallero R.Cenci J.Cerasoli m.G.Chapman m.Charles Ph.Charpentier G.Chatzikonstantinidis m.Chefdeville V.Chekalina C.Chen S.Chen A.Chernov S.-G.Chitic V.Chobanova m.Chrzaszcz A.Chubykin P.Ciambrone m.F.Cicala X.Cid Vidal G.Ciezarek F.Cindolo 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 A.Comerma-montells A.Contu N.Cooke G.Coombs S.Coquereau G.Corti C.m.Costa Sobral B.Couturier D.C.Craik J.Crkovska A.Crocombe m.Cruz Torres R.Currie C.L.Da Silva E.Dall'Occo J.Dalseno C.D'Ambrosio A.Danilina P.d'Argent A.Davis O.De Aguiar Francisco K.De Bruyn S.De Capua m 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 School of Physics State Key Laboratory of Nuclear Physics and Technology Peking UniversityBeijingChina University of Chinese Academy of Sciences BeijingChina Institute Of High Energy Physics(IHEP) BeijingChina Institute of Particle Physics Central China Normal UniversityWuhanHubeiChina Univ.Grenoble Alpes Univ.Savoie Mont BlancCNRSIN2P3-LAPPAnnecyFrance Universite Clermont Auvergne CNRS/IN2P3LPCClermont-FerrandFrance Aix marseille Univ CNRS/IN2P3CPPMMarseilleFrance LAL Univ.Paris-SudCNRS/IN2P3Universite Paris-SaclayOrsayFrance LPNHE Sorbonne Universite Paris Diderot Sorbonne Paris Cite CNRS/IN2P3ParisFrance I.Physikalisches Institut RWTH Aachen UniversityAachenGermany Fakultat Physik Technische Universitat DortmundDortmundGermany max-Planck-Institut für Kernphysik(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-Bicocca MilanoItaly INFN Sezione di milano MilanoItaly INFN Sezione di Cagliari MonserratoItaly INFN Sezione di Padova PadovaItaly INFN Sezione di Pisa PisaItaly INFN Sezione di Roma Tor Vergata RomaItaly INFN Sezione di Roma La Sapienza RomaItaly Nikhef National Institute for Subatomic Physics AmsterdamNetherlands Nikhef National Institute for Subatomic Physics and VU University Amsterdam AmsterdamNetherlands Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences KrakowPoland AGH-University of Science and Technology Faculty of Physics and Applied Computer ScienceKrakowPoland Natio

A search for the doubly charmed baryon ■^+cc is performed through its decay to theΛ^+c K^-π^+ final state,using proton-proton collision data collected with the LHCb detector at centre-of-mass energies of 7,8 and 13 *** data correspond to a total integrated luminosity of 9 fb^-*** significant signal is observed in the mass range from 3.4 to 3.8 GeV/c^*** limits are set at 95%credibility level on the ratio of the ■^+cc production cross-section times the branching fraction to that ofΛ^+c and ■^++cc *** limits are determined as functions of the ■^+cc mass for different lifetime hypotheses,in the rapidity range from 2.0 to 4.5 and the transverse momentum range from 4 to 15 GeV/c.

关键词： charmed baryons limits on production of particles charmed quarks experimental tests

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水化时代对比剂性肾病的流行病学

国际医学放射学杂志 2012年第4期 383-383页

作者： C.E.A. Balemans L.J.m. reichert B.H. van Schelven J.A.J.G. van den Brand J.F.m. Wetzels 唐光健 Department of Nephrology 464 Radboud University Nijmegen Medical CentrePO Box 9101 6500 HB Nijmegen the Netherlands

摘要目的评价估计肾小球滤过率(eGFR)<60mL/(min·1.73m2),接受静脉内对比剂注射与按目前指南治疗病人对比剂性肾病(CIN)的发生率,确定CIN相关危险因素。材料与方法此项前瞻性队列研究由科研伦理委员会批准并免除知情同意通知。所有eGFR... 详细信息

摘要目的评价估计肾小球滤过率(eGFR)mL/(min·1.73m2),接受静脉内对比剂注射与按目前指南治疗病人对比剂性肾病(CIN)的发生率,确定CIN相关危险因素。材料与方法此项前瞻性队列研究由科研伦理委员会批准并免除知情同意通知。所有eGFRmL/(min·1.73m2)的非住院病人就诊于特殊门诊

关键词：对比剂危险因素滤过肾小球危险隐患肾单位肾病泌尿系统疾病高危病人

维生素D类似物治疗大瘤体和延长治疗鼠视网膜母细胞瘤模型的疗效

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美国医学会眼科杂志（中文版） 2005年第2期17卷 F0003-F0003页

作者： Daniel m, Albert Amit Kumar Stephen A. Strugnell Soesiawati R. Darjatmoko janice m. Lokken mary J. Lindstrome Sarit Patel 刘敬（译）

目的：研究维生素D类似物1，25-（OH）：16-ene-25-yne维生素D3（16,23-D3）和1-α羟基维生素D2（1α-OH—D2）在抑制大的视网膜母细胞瘤体的生长和在一种转基因模型中长期应用的效果。

关键词：维生素D类似物视网膜母细胞瘤转基因模型延长治疗瘤体疗效羟基维生素长期应用鼠

1α-羟基维生素D2抑制转基因鼠眼色素性肿瘤生长中的作用

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美国医学会眼科杂志（中文版） 2005年第2期17卷 92-92页

作者： Daniel m. Albert Amit Kumar Stephen A. Strugnell Soesiawati R. Darjatmoko janice m. Lokken mary J. Lindstrom m. Damico Sarit Patel 刘敬（译）

目的：研究羟基维生素D2（1α-OH-D2）对由病毒40T和大鼠胰蛋白酶基因控制的t抗原形成的“Tyr-Tag”转基因大鼠的眼部色素性肿瘤的抑制作用。这些动物的眼部色素性肿瘤主要来源于视网膜色素上皮，与人脉络膜黑色素瘤的生长和组织特点非... 详细信息

目的：研究羟基维生素D2（1α-OH-D2）对由病毒40T和大鼠胰蛋白酶基因控制的t抗原形成的“Tyr-Tag”转基因大鼠的眼部色素性肿瘤的抑制作用。这些动物的眼部色素性肿瘤主要来源于视网膜色素上皮，与人脉络膜黑色素瘤的生长和组织特点非常相似。方法：73只6-7周Tyr—Tag转基因大鼠，根据性别和窝别随机分为3组，分别使用0．05μg/d、0．1μg／d、0．2μg／d 1α-OH-D2；对照组服用椰子油。口服药物每周5次，连服3周。动物被麻醉后，摘除眼球，进行组织学检查。每只眼球制作3个连续切片，应用Optimus softmware version 6．5（media Cybernetic LP，Silver Spring，md）分析。根据致死率、体重和血钙水平评价药物的毒副作用。

关键词：羟基维生素肿瘤生长色素性维生素D2 转基因鼠转基因大鼠视网膜色素上皮脉络膜黑色素瘤 version Spring

毒素介导眼内炎的免模型中玻璃体内注射人类免疫球蛋白减低金黄色葡萄球菌培养上清液的效应

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美国医学会眼科杂志（中文版） 2005年第3期17卷 185-185页

作者： Stephen L. Perkins Dennis P. Han janice m. Burke Patrick m. Schlievert William J. Wirostko Dariusz G. Tarasewicz Christine m. B. Skumatz 李扬（译）

目的：研究在眼内炎的兔模型中，人免疫球蛋白能否减低金黄色葡萄球菌（金葡菌）培养上清液的毒性作用。方法：免疫球蛋白与金葡菌株RN4220的产物结合，应用已知毒素（β-溶血素和毒素休克综合征毒素-1）以及浓缩的含有金葡菌外毒素（... 详细信息

目的：研究在眼内炎的兔模型中，人免疫球蛋白能否减低金黄色葡萄球菌（金葡菌）培养上清液的毒性作用。方法：免疫球蛋白与金葡菌株RN4220的产物结合，应用已知毒素（β-溶血素和毒素休克综合征毒素-1）以及浓缩的含有金葡菌外毒素（集合毒素）的培养上清液对其进行Western标记分析。为诱发眼内炎，需要将集合毒素注入兔玻璃体内。为观察免疫球蛋白的治疗效果，将免疫球蛋白与集合毒素混和后同时注入玻璃体或是在注入集合毒素后6h注入免疫球蛋白。眼内炎的严重程度通过9天内的临床检查（裂隙灯或间接眼底镜）进行分级，通过组织学切片进行评估。

关键词：人免疫球蛋白金黄色葡萄球菌玻璃体内注射培养上清液外毒素眼内炎兔模型 Western 毒素休克综合征