检索结果-南通市图书馆

A techno-economic and life cycle assessment for the production of green methanol from CO_(2): catalyst and process bottlenecks

在线全文

学校读者我要写书评

暂无评论

j.urnal of Energy Chemistry 2022年第5期31卷 255-266页

作者： Tomas Cordero-Lanzac Adrian Ramirez Alberto Navaj.s Lieven Gevers Sirio Brunialti Luis MGandía Andrés T.Aguayo S.Mani Sarathy j.rge gascon Department of Chemical Engineering University of the Basque Country(UPV/EHU)PO Box 64448080 BilbaoSpain King Abdullah University of Science and Technology KAUST Catalysis Center(KCC)Advanced Catalytic MaterialsThuwal 23955Saudi Arabia Department of Science Public University of Navarre(UPNA)Arrosadía Campus s/n31006 PamplonaSpain Institute for Advanced Materials and Mathematics(InaMat2) Universidad Pública de Navarra(UPNA)Edificio Jerónimo de AyanzCampus de ArrosadiaPamplona-Iruña 31006Spain King Abdullah University of Science and Technology Clean Combustion Research Center(CCRC)Thuwal 23955Saudi Arabia

The success of catalytic schemes for the large-scale valorization of CO_(2) does not only depend on the development of active,selective and stable catalytic materials but also on the overall process *** we present a multidisciplinary study(from catalyst to plant and techno-economic/lifecycle analysis)for the production of green methanol from renewable H2 and CO_(2).We combine an in-depth kinetic analysis of one of the most promising recently reported methanol-synthesis catalysts(InCo)with a thorough process simulation and techno-economic *** then perform a life cycle assessment of the simulated process to gauge the real environmental impact of green methanol production from CO_(2).Our results indicate that up to 1.75 ton of CO_(2) can be abated per ton of produced methanol only if renewable energy is used to run the process,while the sensitivity analysis suggest that either rock-bottom H2 prices(1.5$kg1)or severe CO_(2) taxation(300$per ton)are needed for a profitable methanol ***,we herein highlight and analyze some critical bottlenecks of the *** attention has been paid to the contribution of H2 to the overall plant costs,CH4 trace formation,and purity and costs of raw *** addition to providing important information for policy makers and industrialists,directions for catalyst(and therefore process)improvements are outlined.

关键词： CO_(2) Methanol Kinetic modeling Process simulation Life cycle assessment

Structure of the πg7／2[404]7／2^＋ Band in Odd Proton Nucleus ^123I

维普期刊数据库评论

在线全文

维普期刊数据库

学校读者我要写书评

暂无评论

Chinese Physics Letters 2004年第6期21卷 1024-1026页

作者： WANGShou-Yu MAYing-j.n T.Komatsubara LIUYun-Zuo ZHANGYu-Hu K.Furuno T.Hayakawa j.Mukai Y.Iwata T.Morikawa G.B.Hagemann G.Sletten j.Nyberg D.j.rrestam H.j.j.nsen j.Espino j.gascon N.Gj.rup B.Cederwall P.O.Tj.m DepartmentofPhysics JilinUniversityChangchun130023 InstituteofPhysicsandTandemAcceleratorCenter UniversityofTsukubaIbaraki305Japan InstituteofModernPhysics ChineseAcademyofSciencesLanzhou730000 DepartmentofPhysics FacultyofScienceHiroshimaUniversityHiroshima724Japan DepartmentofPhysics FacultyofScienceKyushuUniversityFukuoka812Japan NielsBohrInstitute TandemAcceleratorLaboratoryRisφDK-4000RoskildeDenmark ManneSiegbabnInstituteofPhysics S-10405StockholmSweden DepartmentofPhysics UniversityofOsloNorway

High spin states of the odd proton nucleus 123I have been populated in the reaction 116Cd(14N, 5n2p) at a beam energy of 65MeV. Two previously known positive-parity ΔI = 2 sequences have been extended up to 31/2+ and 41/2+. In addition, a number of ΔI = 1 transitions linking the two ΔI = 2 sequences have been observed. It is suggested that both the ΔI = 2 sequences are built upon the oblate πg7/2[404]7/2+ Nilsson configuration.

关键词：

2020 roadmap on pore materials for energy and environmental applications

维普期刊数据库评论

在线全文

维普期刊数据库

学校读者我要写书评

暂无评论

Chinese Chemical Letters 2019年第12期30卷 2110-2122页

作者： Zengxi Wei Bing Ding Hui Dou j.rge gascon Xiang-j.an Kong Yuj.e Xiong Bin Cai Ruiyang Zhang Ying Zhou Mingce Long j.e Miao Yuhai Dou Ding Yuan j.anmin Ma School of Physics and Electronics Hunan UniversityChangsha 410082China j.angsu Key Laboratory of Electrochemical Energy-Storage Technologies College of Materials Science and TechnologyNanjing University of Aeronautics and AstronauticsNanjing 210016China King Abdullah University of Science and Technology KAUST Catalysis Center(KCC)Advanced Catalytic MaterialsThuwal 23955Saudi Arabia State Key Laboratory of Physical Chemistry of Solid Surfaces and Department of ChemistryCollege of Chemistry and Chemical EngineeringXiamen UniversityXiamen 361005China Hefei National Laboratory for Physical Sciences at the Microscale and School of Chemistry and Materials ScienceUniversity of Science and Technology of ChinaHefei 230026China Physical Science Division Pacific Northwest National LaboratoryRichlandWA 99352United States State Key Laboratory of Oil and Gas Reservoir Geology and Exploitation Southwest Petroleum UniversityChengdu 610500China The Center of New Energy Materials and Technology School of Materials Science and EngineeringSouthwest Petroleum UniversityChengdu 610500China School of Environmental Science and Engineering Shanghai Jiao Tong UniversityShanghai 200240China Centre for Clean Environment and Energy Gold Coast CampusGriffith UniversityGold Coast 4222Australia Key Laboratory of Materials Processing and Mold(Zhengzhou University) Ministry of EducationZhengzhou UniversityZhengzhou 450002China

Porous materials have attracted great attention in energy and environment applications,such as metal organic frameworks(MOFs),metal aerogels,carbon aerogels,porous metal *** materials could be also hybridized with other materials into functional composites with superior *** high specific area of porous materials offer them the advantage as hosts to conduct catalytic and electrochemical *** one hand,catalytic reactions include photocatalytic,p ho toe lectrocatalytic and electrocatalytic reactions over some *** the other hand,they can be used as electrodes in various batteries,such as alkaline metal ion batteries and electrochemical *** far,both catalysis and batteries are extremely attractive *** are also many obstacles to overcome in the exploration of these porous *** research related to porous materials for energy and environment applications is at extremely active stage,and this has motivated us to contribute with a roadmap on ’porous materials for energy and environment applications’.

关键词： Metal organic frameworks Zeolitic imidazolate frameworks Covalent organic frameworks Aerogels Photocatalysis Photoelectrocatalysis Electrocatalysis Metal-ion batteries Electrochemical capacitors

Newfound Coding Potential of Transcripts Unveils Missing Members of Human Protein Communities

在线全文

学校读者我要写书评

暂无评论

Genomics, Proteomics & Bioinformatics 2023年第3期21卷 515-534页

作者： Se´bastien Leblanc Marie *** j.an-Franc¸ois j.cques Amina M.Lekehal Andre´a Duclos Alexia Tremblay Alexis Bruggeman-gascon Sondos Samandi Myle`ne Brunelle Alan A.Cohen Michelle S.Scott Xavier Roucou Department of Biochemistry and Functional Genomics Universite´de SherbrookeSherbrookeQC J1E 4K8Canada PROTEO Quebec Network for Research on Protein FunctionStructureand EngineeringQuebec CityQC G1V 0A6Canada Department of Family Medicine Universite´de SherbrookeSherbrookeQC J1H 5N4Canada

Recent proteogenomic approaches have led to the discovery that regions of the transcriptome previously annotated as non-coding regions[i.e.,untranslated regions(UTRs),open reading frames overlapping annotated coding sequences in a different reading frame,and non-coding RNAs]frequently encode proteins,termed alternative proteins(altProts).This suggests that previously identified protein–protein interaction(PPI)networks are partially incomplete because altProts are not present in conventional protein ***,we used the proteogenomic resource OpenProt and a combined spectrum-and peptide-centric analysis for the re-analysis of a highthroughput human network proteomics dataset,thereby revealing the presence of 261 altProts in the *** found 19 genes encoding both an annotated(reference)and an alternative protein interacting with each *** the 117 altProts encoded by pseudogenes,38 are direct interactors of reference proteins encoded by their respective parental ***,we experimentally validate several interactions involving *** data improve the blueprints of the human PPI network and suggest functional roles for hundreds of altProts.

关键词： Alternative protein Protein network Protein–protein interaction Pseudogene Affinity purification mass spectrometry

维普期刊数据库评论

在线全文

维普期刊数据库

学校读者我要写书评

暂无评论

椰子的遗传改良:结果与展望

世界热带农业信息 1983年第3期 53-58页

作者： j.P.gascon 毛祖舜

最初进行椰子杂交育种时,椰干产量很低,因此改良这一性状是唯一的目的。目前考虑到质量标准,即椰油含量,蛋白质含量和成分;进一步则要考虑椰子植区的多种经营引起的适应生态条件和抗病虫害问题。产量改良所沿用的选种方法,其基础是探究... 详细信息

最初进行椰子杂交育种时,椰干产量很低,因此改良这一性状是唯一的目的。目前考虑到质量标准,即椰油含量,蛋白质含量和成分;进一步则要考虑椰子植区的多种经营引起的适应生态条件和抗病虫害问题。产量改良所沿用的选种方法,其基础是探究原种和单株间的配合力,以及对可遗传性状进行表型选择,包括三个方面:即一、有希望种与引进种;二、原种和品种之间的配合能力;三、单株配合力。

关键词：椰子配合力杂种亲本热带及亚热带果组合力杂交种椰肉原种

Search for the doubly charmed baryon ■

在线全文

同方期刊数据库

学校读者我要写书评

暂无评论

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.Aj.ltouni S.Akar P.Albicocco j.Albrecht F.Alessio M.Alexander A.Alfonso Albero G.Alkhazov P.Alvarez Cartelle A.A.Alves j. 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.Bj.rn 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.Coj.cariu 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 j.neiro(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

Measurement of Ξcc++ production in pp collisions at s1/2=13 TeV

在线全文

学校读者我要写书评

暂无评论

Chinese Physics C 2020年第2期44卷 13-23页

作者： R.Aaij.C.Abellán Beteta T.Ackernley B.Adeva M.Adinolfi H.Afsharnia C.A.Aidala S.Aiola Z.Aj.ltouni S.Akar P.Albicocco j.Albrecht F.Alessio M.Alexander A.Alfonso Albero G.Alkhazov P.Alvarez Cartelle A.A.Alves j. S.Amato Y.Amhis L.An L.Anderlini G.Andreassi M.Andreotti F.Archilli 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 j.M.Basels G.Bassi V.Batozskaya B.Batsukh A.Battig A.Bay M.Becker F.Bedeschi I.Bediaga A.Beiter L.j.Bel V.Belavin S.Belin V.Bellee K.Belous I.Belyaev G.Bencivenni E.Ben-Haim S.Benson S.Beranek A.Berezhnoy *** D.Berninghoff H.C.Bernstein C.Bertella 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.Bizzeti M.Bj.rn 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 M.j.Bradley S.Braun A.Brea Rodriguez M.Brodski j.Brodzicka A.Brossa Gonzalo D.Brundu E.Buchanan A.Buonaura C.Burr A.Bursche A.Butkevich j.S.Butter j.Buytaert W.Byczynski S.Cadeddu H.Cai R.Calabrese L.Calero Diaz S.Cali R.Calladine M.Calvi M.Calvo Gomez P.Camargo Magalhaes A.Camboni P.Campana D.H.Campora Perez A.F.Campoverde Quezada L.Capriotti A.Carbone G.Carboni R.Cardinale A.Cardini I.Carli P.Carniti K.Carvalho Akiba A.Casais Vidal G.Casse M.Cattaneo G.Cavallero S.Celani 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 S.Cholak 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.Coj.cariu 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' Centro Brasileiro de Pesquisas Físicas(CBPF) Rio de JaneiroBrazil Universidade Federal do Rio de j.neiro(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 UniversitéClermont Auvergne CNRS/IN2P3LPCClermont-FerrandFrance Aix Marseille Univ CNRS/IN2P3CPPMMarseilleFrance LAL Univ.Paris-SudCNRS/IN2P3UniversitéParis-SaclayOrsayFrance LPNHE Sorbonne UniversitéParis Diderot Sorbonne Paris CitéCNRS/IN2P3ParisFrance I.Physikalisches Institut RWTH Aachen UniversityAachenGermany Fakultät Physik Technische Universität DortmundDortmundGermany Max-Planck-Institut für Kernphysik(MPIK) HeidelbergGermany Physikalisches Institut Ruprecht-Karls-Universität 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 KrakówPoland AGH-University of Science and Technology Faculty of Physics and Applied Computer ScienceKrakówPoland Nationa

The production of ■baryons in proton-proton collisions at a centre-of-mass energy of √s = 13 TeV is measured in the transverse-momentum range 4 详细信息

The production of ■baryons in proton-proton collisions at a centre-of-mass energy of √s = 13 TeV is measured in the transverse-momentum range 4

关键词： doubly charmed baryons hadron production QCD

儿童早期空气污染与呼吸道感染:ESCAPE项目中10个欧洲出生队列的分析

在线全文

学校读者我要写书评

暂无评论

环境与职业医学 2014年第3期31卷 202-202页

作者： Elaina A.MacIntyre Ulrike Gehring Anna Molter Elaine Fuertes Claudia Klümper Ursula Kramer Ulrich Quass Barbara Hoffmann Mireia gascon Bert Brunekreef Gerard H.Koppelman Rob Beelen Gerard Hoek Matthias Birk j.han C.de j.ngste H.A.Smit j.sef Cyrys Olena Gruzieva Michal Korek Anna Bergstrom Raymond M.Agius Frank de Vocht Angela Simpson Daniela Porta Francesco Forastiere Chiara Badaloni Giulia Cesaroni Ana Esplugues Ana Fernández-Somoano Aitana Lerxundi j.rdi Sunyer Marta Cirach Mark j.Nieuwenhuij.en Goran Pershagen j.achim Heinrich

[背景]将交通源空气污染作为幼儿期呼吸道感染的危险因素的研究很少。[目的]在10个欧洲出生队列——BAMSE（瑞典）、GASPⅡ（意大利）、GINIplus和LISAplus（德国）、MAAS（英国）、PIAMA（荷兰）和4个INMA队列（西班牙）——中研究空... 详细信息

[背景]将交通源空气污染作为幼儿期呼吸道感染的危险因素的研究很少。[目的]在10个欧洲出生队列——BAMSE（瑞典）、GASPⅡ（意大利）、GINIplus和LISAplus（德国）、MAAS（英国）、PIAMA（荷兰）和4个INMA队列（西班牙）——中研究空气污染与肺炎、哮喘及中耳炎之间的相关性，并使用meta分析得出综合效应估值。[方法]评价家长报告的医师诊断的儿童早期肺炎、中耳炎以及哮喘与全年平均污染物水平[二氧化氮（NO2）、氮氧化物（NOx）、≤2．5gm的颗粒物（PM2.5）、PM2.5吸光度、PM10、PM2.5-10（粗PM）]间的关联，污染物浓度的估计采用土地利用回归模型并根据孩子的出生住址分配。作为ESCAPE项目的一部分，每个研究区域都采用相同的方案建立回归模型。用logistic回归来计算每个研究校正后的效应估值，用随机效应meta分析来计算合并的估计值。[结果]除了PM2.5外的所有污染物，肺炎的合并校正优势比（OR）均升高（例如，N02每增加10μg／m3，OR=1．30，95％CI：1．02～1．65；PM10每增加10μg／m3的OR=1．76，95％CI：1．00—3．09）。对于中耳炎和哮喘，除了NO2与中耳炎问的关联（每10μg／m3对应的OR=1．09，95％CI：1．02～1．16），所有分析的结果均无显著性。[结论]对ESCAPE项目中10个欧洲出生队列进行的meta分析为空气污染和儿童早期肺炎之间的相关性找到一致性的证据，也为与中耳炎间的相关性找到了一些证据。

关键词：早期肺炎呼吸道感染出生队列空气污染欧洲儿童 meta分析 logistic