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Macmillan Dictionary of Biotehnology

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Macmillan Dictionary of Biotehnology

1986生物工程指南《产品、公司、研究与组织机构》

作者： J.coombs

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1986生物工程指南《产品、公司、研究与组织机构》

作者： J.coombs

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关于沸石类矿物命名法的建议(Ⅰ)

矿物岩石地球化学通报 2001年第3期20卷 149-155页

作者： D.S.coombs 王立本中国地质科学院矿产资源研究所

本文系对IMA CNMMN批准的沸石命名法的修改建议。其中扩展了沸石类矿物的定义 ,今后凡具有沸石的性质 ,但其结构中含有四面体格架者则可视为沸石 ;亦允许非硅和铝的元素在格架内的完全替换。在具特定结构的组成系列中 ,格架外的不同阳... 详细信息

本文系对IMA CNMMN批准的沸石命名法的修改建议。其中扩展了沸石类矿物的定义 ,今后凡具有沸石的性质 ,但其结构中含有四面体格架者则可视为沸石 ;亦允许非硅和铝的元素在格架内的完全替换。在具特定结构的组成系列中 ,格架外的不同阳离子中的原子比值最大者可确定为独立的矿物种 ,命名时采用相应的元素符号作为后缀 ,用连字符加在系列名称之后 [钙十字沸石类 (philipsite)和方沸石 (analcime)系列中的交沸石 (harmotome)、铯沸石 (pollucite)和斜钙沸石 (wairakite)除外 ]。具有相同结构格架的沸石中空间群对称和有序—无序关系的差异一般不作为建立独立矿物种的根据。除片沸石 (heulandite) (Si∶Al4 .0 )外 ,沸石的矿物种不能只靠Si∶Al值来区分。失水、部分水化和过量水化不能作为区别沸石独立矿物种的根据。在涉及到沸石的简化分子式或平均分子式时 ,应当避免使用“理想分子式”这一术语。在不同的组成系列中最近确定的矿物种有 :brewsterite Sr、 Ba(锶沸石 Sr、 Ba)、chabazite Ca、 Na、 K(菱沸石 Ca、 Na、 K)、clinoptilolite K、 Na、 Ca(斜发沸石 K、 Na、 Ca)、dachiardite Ca、 Na(环晶沸石 Ca、 Na)、erionite Na、 K、 Ca(毛沸石 Na、

关键词：沸石类矿物矿物命名矿物分类

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

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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.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 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.Bjørn 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.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' Centro Brasileiro de Pesquisas Físicas(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 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 4geV/c and the rapidity range2.0 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 4geV/c and the rapidity range2.0grated luminosity of 1.7fb^-1,recorded by the LHCb experiment during *** ratio of the ■ production cross-section times the branching fraction of the■→∧^+cK^-π^+ π^+decay relative to the prompt ∧^+c production cross-section is found to be(2.22±0.27±0.29)×10^-4,assuming the central value of the measured lifetime,where the first uncertainty is statistical and the second systematic.

关键词： doubly charmed baryons hadron production QCD

Dose-response relationship of lung cancer to amount smoked, duration and age starting

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World Journal of Meta-Analysis 2013年第2期1卷 57-77页

作者： John S Fry Peter N Lee Barbara A Forey Katharine J coombs PN Lee Statistics and Computing Ltd.

AIM： To quantify smoking/lung cancer relationships accurately using parametric modelling.METHODS： Using the International Epidemiological Studies on Smoking and Lung Cancer database of all epidemiological studies of 100＋ lung cancer cases published before 2000, we analyzed 97 blocks of data for amount smoked, 35 for duration of smoking, and 27 for age started. Pseudo-numbers of cases and controls （or at risk） estimated from RRs by dose level formed the data modelled. We fitted various models relating loge RR to dose （d）, including βd, βdY and βloge （1 ＋ Wd）, and investigated goodness-of-fit and heterogeneity between studies.0.833 loge [1 ＋（8.1c/10）] for cigarettes/d （c）, 0.792 （y/10）0.74 for years smoked （y） and 0.176 [（70 - a）/10]1.44 for age of start （a）. Each model fitted well overall, though some blocks misfitted. RRs rose from 3.86 to 22.31 between c = 10 and 50, from 2.21 to 13.54 be-tween y = 10 and 50, and from 3.66 to 8.94 between a = 30 and 12.5. Heterogeneity （P 〈 0.001） existed by continent for amount, RRs for 50 cigarettes/d being 7.23 （Asia）, 26.36 （North America） and 22.16 （Europe）. Little heterogeneity was seen for duration of smoking or age ***： The models describe the dose-relation-ships well, though may be biased by factors including misclassification of smoking status and dose.

关键词： Smoking Lung neoplasms Dose-response Meta-analysis Review Amount smoked Duration of smoking Age at starting to smoke

Search for the doubly charmed baryon ■

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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

Studies on the active SISFCL and its impact on the distance protection of the EHV transmission line

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Protection and Control of Modern Power Systems 2016年第1期1卷 164-169页

作者： Chao Li Bin Li Fengrui guo Jianzhao geng Xiuchang Zhang Tim coombs EPEC Superconductivity group University of CambridgeCambridge CB30FAUK Key Laboratory of Smart grid of Ministry of Education Tianjin UniversityTianjin 300072China State grid Tianjin Electric Power Company Tianjin 300010China.

The active saturated iron-core superconductive fault current limiter(SISFCL)is a good choice to decrease fault *** paper introduced the principles and impedance characteristic of the active ***,it shows the current-limiting effects of the ***,the impact of the active SISFCL on the distance protection of the EHV transmission line is *** on that,the coordination scheme of the distance protections is proposed.A 500 kV double-circuit transmission system with SISFCLs is simulated by Electro-Magnetic Transients Program including DC(EMTDC).Simulation tests demonstrate the correctness and validity of theoretical analyses.

关键词： Superconductive Fault current limiter(SFCL) Saturated iron core Distance protection Current-limiting effects

ARM TrustZone的可信执行环境和线上快速身份验证确保鉴权安全无虞

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单片机与嵌入式系统应用 2015年第9期15卷 3-6页

作者： Rob coombs ARM系统与软件部门

引言智能互联的移动设备越来越广泛地应用于商务、金融和娱乐行业。基于远程互联网服务器的用户鉴权是许多应用程序或云服务的第一个环节，传统的用户名与密码身份鉴权方式的效果不太理想，一方面消费者难以记住复杂的密码，另一方面服... 详细信息

引言智能互联的移动设备越来越广泛地应用于商务、金融和娱乐行业。基于远程互联网服务器的用户鉴权是许多应用程序或云服务的第一个环节，传统的用户名与密码身份鉴权方式的效果不太理想，一方面消费者难以记住复杂的密码，另一方面服务提供商（通常称为“依赖方”）可能需要考虑密码泄露风险。为了应对这些状况并且解决其他密码相关问题，线上快速身份验证（Fast Identity Online，FIDO）联盟制定了全新的协议，在用户、设备和依赖方之间实现简单而安全性强大的鉴权机制。在移动设备上，FIDO可以利用生物特征鉴权，通过扫描指纹或者虹膜来启用服务。如此一来，不仅可以大幅改善用户体验，让消费者进行交易时更顺畅无碍，而且这一项技术很有可能被设备制造商快速采用。

关键词：用户鉴权身份验证安全性执行环境联网服务器移动设备 Online 应用程序

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危机传播规划、管理与应对

董事会 2015年第Z1期 64-65页

作者： W.Timothy coombs

危机管理涉及现代企业多个职能部门,因而其研究也是跨学科的。近年来,随着市场国际化的深入、企业声誉的日益重要、特别是社交媒体的崛起,危机管理和危机传播呈现出新特点,大量案例和文章也随之涌现。在对最新研究成果系统梳理的基础上... 详细信息

危机管理涉及现代企业多个职能部门,因而其研究也是跨学科的。近年来,随着市场国际化的深入、企业声誉的日益重要、特别是社交媒体的崛起,危机管理和危机传播呈现出新特点,大量案例和文章也随之涌现。在对最新研究成果系统梳理的基础上,美国著名危机管理专家库姆斯教授从管理学角度提出危机传播三阶段(危机前、危机中和危机后)理论,并对每个阶段的核心问题结合案例予以阐述。第一章介绍三阶段的理论框架。第二章重点讲述社交媒体对危机管理日益增

关键词：危机传播兴趣中华人民共和国个性心理特征社交媒体危机预防规划长远计划