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反应溅射TiW_yN_x薄膜扩散势垒特性研究

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j.urnal of Semiconductors 1993年第11期14卷 702-707,T001页

作者：张国炳武国英徐立郝一龙隋小平 A.P.Clarke P.j.Clarke M.D.Strathman T.Gates S.Baumann 北京大学微电子学研究所北京100871 Sputtered Films Incorporated USA Chales evans & Associates USA

本文利用XRD、RBS、AES、SEM和电学测量技术系统地研究了反应溅射制备的TiW_yN_x薄膜的组份、结构和扩散势垒特性,实验结果表明,膜的组份、结构和特性受溅射时N_2流量影响和溅射功率的影响,这种TiW_yN_x膜经550℃30分钟退火后,仍能有效... 详细信息

本文利用XRD、RBS、AES、SEM和电学测量技术系统地研究了反应溅射制备的TiW_yN_x薄膜的组份、结构和扩散势垒特性,实验结果表明,膜的组份、结构和特性受溅射时N_2流量影响和溅射功率的影响,这种TiW_yN_x膜经550℃30分钟退火后,仍能有效防止Al-Si扩散,从而改善了Al/TiW_yN_x/CoSi_2/Si浅结接触的热稳定性。

关键词： TiWN薄膜扩散反应溅射集成电路

Association of latitude and altitude with adverse outcomes in patients with COVID-19: The VIRUS registry

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World j.urnal of Critical Care Medicine 2022年第2期11卷 102-111页

作者： Aysun Tekin Shahraz Qamar Romil Singh Vikas Bansal Mayank Sharma Allison M LeMahieu Andrew C Hanson Phillip j.Schulte Marij. Bogoj.vic Neha Deo Simon Zec Diana j.Valencia Morales Katherine A Belden Smith F Heavner Margit Kaufman Sreekanth Cheruku Valerie C Danesh Valerie M Banner-Goodspeed Catherine A St Hill Amy B Christie Syed A Khan Lynn Retford Karen Boman Vishakha KKumar j.hn C O'Horo j.an Pablo Domecq Allan j.Walkey Ognj.n Gaj.c Rahul Kashyap Salim Surani TheSociety of Critical Care Medicine(SCCM)Discovery Viral Infection and Respiratory Illness Universal Study(VIRUS):COVID-Registry Investigator Group Department of Anesthesiology Mayo ClinicRochesterMN 55905United States Post-baccalaureate Research Education Program Mayo Clinic College of Medicine and ScienceRochesterMN 55905United States Division of Pulmonary and Critical Care Medicine Department of Internal MedicineMayo ClinicRochesterMN 55905United States Division of Clinical Trials and Biostatistics Department of Quantitative Health SciencesMayo ClinicRochesterMN 55905United States Alix School of Medicine Mayo ClinicRochesterMN 55905United States Division of Infectious Diseases Thomas Jefferson University HospitalPhiladelphiaPA 19107United States Prisma Health GreenvilleSC 29605United States Englewood Health EnglewoodNJ 07631United States Divisions of Cardiothoracic Anesthesiology and Critical Care Medicine Department of Anesthesiology and Pain ManagementUT Southwestern Medical CenterDallasTX 75390United States Center for Applied Health Research Baylor Scott and White HealthDallasTX 75246United States Department of Anesthesiology Critical Care and Pain MedicineBeth Israel Deaconess Medical CenterBostonMA 02215United States Allina Health MinneapolisMN 55407United States Department of Critical Care Atrium Health NavicentMaconGA 31201United States Division of Critical Care Medicine Mayo Clinic Health SystemMankatoMN 56001United States Society of Critical Care Medicine Mount ProspectIL 60056United States Division of Infectious Diseases Mayo ClinicRochesterMN 55905United States Division of Nephrology and Hypertension Department of Internal MedicineMayo ClinicRochesterMN 55905United States Pulmonary Center Division of PulmonaryAllergyCritical Care and Sleep MedicineDepartment of MedicineEvans Center of Implementation and Improvement SciencesBoston University School of MedicineBostonMA 02118United States Department of Pulmonary and Critical Care Medicine Texas A&M UniversityBryanTX 77807United States 不详

BACKGROUND The coronavirus disease 2019(COVID-19)course may be affected by environmental *** studies previously suggested a link between climatological factors and COVID-19 fatality ***,individual-level impact of these factors has not been thoroughly evaluated *** To study the association of climatological factors related to patient location with unfavorable outcomes in *** In this observational analysis of the Society of Critical Care Medicine Discovery Viral Infection and Respiratory Illness Universal Study:COVID-19 Registry cohort,the latitudes and altitudes of hospitals were examined as a covariate for mortality within 28 d of admission and the length of hospital *** for baseline parameters and admission date,multivariable regression modeling was *** estimating equations were used to fit the *** Twenty-two thousand one hundred eight patients from over 20 countries were *** median age was 62(interquartile range:49-74)years,and 54%of the included patients were *** median age increased with increasing latitude as well as the frequency of ***,the percentage of comorbidities was lower in elevated *** within 28 d of hospital admission was found to be 25%.The median hospital-free days among all included patients was 20 *** the significant linear relationship between mortality and hospital-free days(adj.sted odds ratio(aOR)=1.39(1.04,1.86),P=0.025 for mortality within 28 d of admission;aOR=-1.47(-2.60,-0.33),P=0.011 for hospital-free days),suggesting that adverse patient outcomes were more common in locations further away from the Equator;the results were no longer significant when adj.sted for baseline differences(aOR=1.32(1.00,1.74),P=0.051 for 28-day mortality;aOR=-1.07(-2.13,-0.01),P=0.050 for hospital-free days).When we looked at the altitude’s effect,we discovered that it demonstrated a non-linear association with mortality wi

关键词： 28 d mortality Altitude COVID-19 Hospital-free days Latitude Outcomes

合同外包与一般外包的比较——兼论地域接近性的重要作用

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经济资料译丛 2006年第4期 1-22页

作者： Robert C．Feenstra Barbara j.Spencer 郑秀莲（译）张明志（指导老师）不详厦门大学经济学院国际经济与贸易系 361005

距离在国际贸易中的重要性已经在重力模型中得到很好的实证研究。距离不只影响贸易数量，对贸易组织和生产方式也有影响。例如，evans ＆ Harrigan（2005年）证明了买方和卖方之间地域接近性在服装行业上获取资源方面的重要性。在本文... 详细信息

距离在国际贸易中的重要性已经在重力模型中得到很好的实证研究。距离不只影响贸易数量，对贸易组织和生产方式也有影响。例如，evans ＆ Harrigan（2005年）证明了买方和卖方之间地域接近性在服装行业上获取资源方面的重要性。在本文中，我们还提出，买方和卖方的地域接近性是决定国际外包中各关系方合同关系的重要因素。

关键词：合同外包接近性地域国际贸易实证研究重力模型贸易数量生产方式

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.Aj.ltouni 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.Bj.rn 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 Baraj.s 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.Coj.cariu 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 j.neiro(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

Search for the doubly heavy baryon Ξ_(bc)^(+)→ decaying to j.ψΞ_(c)^(+)

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中国物理C:英文版 2023年第9期47卷 1-13页

作者： R.Aaij.A.S.W.Abdelmotteleb C.Abellan Beteta F.Abudinén T.Ackernley B.Adeva M.Adinolfi H.Afsharnia C.Agapopoulou C.A.Aidala S.Aiola Z.Aj.ltouni S.Akar K.Akiba j.Albrecht F.Alessio M.Alexander A.Alfonso Albero Z.Aliouche P.Alvarez Cartelle S.Amato j.L.Amey Y.Amhis L.An L.Anderlini M.Andersson A.Andreianov M.Andreotti D.Andreou D.Ao F.Archilli A.Artamonov M.Artuso E.Aslanides M.Atzeni B.Audurier S.Bachmann M.Bachmayer j.j.Back A.Bailly-reyre P.Baladron Rodriguez V.Balagura W.Baldini j.Baptista de Souza Leite M.Barbetti R.j.Barlow S.Barsuk W.Barter M.Bartolini F.Baryshnikov j.M.Basels G.Bassi B.Batsukh A.Battig A.Bay A.Beck M.Becker F.Bedeschi I.B.Bediaga A.Beiter V.Belavin S.Belin V.Bellee K.Belous I.Belov I.Belyaev G.Bencivenni E.Ben-Haim A.Berezhnoy *** D.Berninghoff H.C.Bernstein C.Bertella A.Bertolin C.Betancourt F.Betti Ia.Bezshyiko S.Bhasin j.Bhom L.Bian M.S.Bieker N.V.Biesuz S.Bifani P.Billoir A.Biolchini M.Birch F.C.R.Bishop A.Bitadze A.Bizzeti M.P.Blago T.Blake F.Blanc S.Blusk D.Bobulska j.A.Boelhauve O.Boente Garcia T.Boettcher A.Boldyrev N.Bondar S.Borghi M.Borsato j.T.Borsuk S.A.Bouchiba T.j.V.Bowcock A.Boyer C.Bozzi M.j.Bradley S.Braun A.Brea Rodriguez j.Brodzicka A.Brossa Gonzalo D.Brundu A.Buonaura L.Buonincontri A.T.Burke C.Burr A.Bursche A.Butkevich j.S.Butter j.Buytaert W.Byczynski S.Cadeddu H.Cai R.Calabrese L.Calefice S.Cali R.Calladine M.Calvi M.Calvo Gomez P.Camargo Magalhaes P.Campana D.H.Campora Perez A.F.Campoverde Quezada S.Capelli L.Capriotti A.Carbone G.Carboni R.Cardinale A.Cardini I.Carli P.Carniti L.Carus A.Casais Vidal R.Caspary G.Casse M.Cattaneo G.Cavallero V.Cavallini S.Celani j.Cerasoli D.Cervenkov A.j.Chadwick M.G.Chapman M.Charles Ph.Charpentier C.A.Chavez Baraj.s M.Chefdeville C.Chen S.Chen A.Chernov S.Chernyshenko V.Chobanova S.Cholak M.Chrzaszcz A.Chubykin V.Chulikov P.Ciambrone M.F.Cicala X.Cid Vidal G.Ciezarek G.Ciullo 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 L.Congedo A.Contu N.Cooke 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 Institute Of High Energy Physics(IHEP) BeijingChina School of Physics State Key Laboratory of Nuclear Physics and Technology Peking UniversityBeijingChina University of Chinese Academy of Sciences BeijingChina Institute of Particle Physics Central China Normal UniversityWuhanHubeiChina Université Savoie Mont Blanc CNRSIN2P3-LAPPAnnecyFrance UniversitéClermont Auvergne CNRS/IN2P3LPCClermont-FerrandFrance Aix Marseille Univ CNRS/IN2P3CPPMMarseilleFrance UniversitéParis-Saclay CNRS/IN2P3IJCLabOrsayFrance Laboratoire Leprince-Ringuet CNRS/IN2P3Ecole PolytechniqueInstitut Polytechnique de ParisPalaiseauFrance 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 MilanoItaly INFN Sezione di Milano-Bicocca MilanoItaly INFN Sezione di Cagliari MonserratoItaly Universitàdegli Studi di Padova Universitàe 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 Scienc

A first search for the Ξ_(bc)^(+)j.ψΞ_(c)^(+) decay is performed by the LHCb experiment with a data sample of proton-proton collisions, corresponding to an integrated luminosity of 9 fb−1 recorded at centre-of-mass energies of 7, 8, and 13 TeV. Two peaking structures are seen with a local (global) significance of 4.3(2.8) and 4.1(2.4) standard deviations at masses of 6571 and 6694 MeV/c2, respectively. Upper limits are set on the Ξ+bc baryon production cross-section times the branching fraction relative to that of the B+c→j.ψD+s decay at centre-of-mass energies of 8 and 13 TeV, in the Ξ+bc and in the B+c rapidity and transverse-momentum ranges from 2.0 to 4.5 and 0 to 20GeV/c, respectively. Upper limits are presented as a function of the Ξ+bc mass and lifetime.

关键词： QCD B physics charm physics spectroscopy

脱落酸对伊文思蓝的荧光猝灭机理研究及其含量测定

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化学分析计量 2010年第6期19卷 17-20页

作者：黄据芹佟丽丽王怀友山东师范大学化学化工与材料科学学院济南250014

利用荧光光谱研究了脱落酸(Abscisic acid)与伊文思蓝(evans blue)的相互作用。用266 nm激发光激发时,伊文思蓝的最大发射波长为396 nm。伊文思蓝与脱落酸相互作用,使伊文思蓝发生荧光猝灭,根据Stern-Volmer方程研究了荧光猝灭的类型及... 详细信息

利用荧光光谱研究了脱落酸(Abscisic acid)与伊文思蓝(evans blue)的相互作用。用266 nm激发光激发时,伊文思蓝的最大发射波长为396 nm。伊文思蓝与脱落酸相互作用,使伊文思蓝发生荧光猝灭,根据Stern-Volmer方程研究了荧光猝灭的类型及机理,实验证明脱落酸与伊文思蓝发生的静态猝灭,即脱落酸和伊文思蓝形成了一种稳定的复合物。伊文思蓝的相对荧光强度与脱落酸的浓度线性相关,线性方程为F0/F=0.78153+3.9153×104c,线性相关系数为0.9976。通过实验求算了脱落酸与伊文思蓝的结合点常数KABA-EB=1.838×105L/mol和结合点数n=1.171,由此建立了测定植物中脱落酸的新方法。

关键词：伊文思蓝脱落酸荧光猝灭

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文艺活动对青少年反社会行为的影响

基础教育参考 2022年第8期13卷 21-21页

作者：刘征(编译) 邢淑芬(编译) Bone,j.K. Bu,F. Fluharty,M.E. Paul,E. Sonke,j.K. Fancourt,D. 北京市海淀区上地实验小学北京100085 首都师范大学心理学院北京100048 不详

青春期被描述为个体负面行为增加的风险期,这期间的校内不良行为、反社会和犯罪行为等发生的概率大大增加。如何预防或减少青春期不良行为,不仅对青少年的健康成长有重要作用,而且对他们成年后的生活也有重要影响。研究表明,参与文化艺... 详细信息

青春期被描述为个体负面行为增加的风险期,这期间的校内不良行为、反社会和犯罪行为等发生的概率大大增加。如何预防或减少青春期不良行为,不仅对青少年的健康成长有重要作用,而且对他们成年后的生活也有重要影响。研究表明,参与文化艺术活动是减少青春期反社会行为的重要举措。以往研究多集中于探究基于文化艺术活动的干预措施如何影响改变那些已有反社会行为的青少年,英国伦敦大学的杰西卡·博恩(jessica ***)教授等人则另辟蹊径,调查了普通青少年参与文化艺术活动是否会影响其青春期的反社会行为,并致力于探究这种影响背后的潜在机制。

关键词：文化艺术活动反社会行为文艺活动不良行为英国伦敦大学杰西卡犯罪行为负面行为