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Measurement of the correlation b.tween flow harmonics of different order in lead-lead collisions at sNN=2.76 TeV with the ATLAS detector

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Physical Review C 2015年第3期92卷 034903-034903页

作者： G. Aad b. Ab.ott J. Ab.allah O. Ab.inov R. Ab.n M. Ab.lins O. S. Ab.uZeid H. Ab.amowicz H. Ab.eu R. Ab.eu Y. Ab.laiti b. S. Acharya L. Adamczyk D. L. Adams J. Adelman S. Adomeit T. Adye A. A. Affolder T. Agatonovic-Jovin J. A. Aguilar-Saavedra S. P. Ahlen F. Ahmadov G. Aielli H. Akerstedt T. P. A. Åkesson G. Akimoto A. V. Akimov G. L. Alb.rghi J. Alb.rt S. Alb.and M. J. Alconada Verzini M. Aleksa I. N. Aleksandrov C. Alexa G. Alexander T. Alexopoulos M. Alhroob.G. Alimonti L. Alio J. Alison S. P. Alkire b. M. M. Allb.ooke P. P. Allport A. Aloisio A. Alonso F. Alonso C. Alpigiani A. Altheimer b. Alvarez Gonzalez D. Álvarez Piqueras M. G. Alviggi b. T. Amadio K. Amako Y. Amaral Coutinho C. Amelung D. Amidei S. P. Amor Dos Santos A. Amorim S. Amoroso N. Amram G. Amundsen C. Anastopoulos L. S. Ancu N. Andari T. Andeen C. F. Anders G. Anders J. K. Anders K. J. Anderson A. Andreazza V. Andrei S. Angelidakis I. Angelozzi P. Anger A. Angerami F. Anghinolfi A. V. Anisenkov N. Anjos A. Annovi M. Antonelli A. Antonov J. Antos F. Anulli M. Aoki L. Aperio b.lla G. Arab.dze Y. Arai J. P. Araque A. T. H. Arce F. A. Arduh J-F. Arguin S. Argyropoulos M. Arik A. J. Armb.uster O. Arnaez V. Arnal H. Arnold M. Arratia O. Arslan A. Artamonov G. Artoni S. Asai N. Asb.h A. Ashkenazi b. Åsman L. Asquith K. Assamagan R. Astalos M. Atkinson N. b. Atlay b. Auerb.ch K. Augsten M. Aurousseau G. Avolio b. Axen M. K. Ayoub.G. Azuelos M. A. b.ak A. E. b.as C. b.cci H. b.chacou K. b.chas M. b.ckes M. b.ckhaus E. b.descu P. b.giacchi P. b.gnaia Y. b.i T. b.in J. T. b.ines O. K. b.ker P. b.lek T. b.lestri F. b.lli E. b.nas Sw. b.nerjee A. A. E. b.nnoura H. S. b.nsil L. b.rak S. P. b.ranov E. L. b.rb.rio D. b.rb.ris M. b.rb.ro T. b.rillari M. b.risonzi T. b.rklow N. b.rlow S. L. b.rnes b. M. b.rnett R. M. b.rnett Z. b.rnovska A. b.roncelli G. b.rone A. J. b.rr F. b.rreiro J. b.rreiro Guimarães da Costa R. b.rtoldus A. E. b.rton P. b.rtos A. b.ssalat A. b.sye R. L. b.tes S. J. b.tista J. R. b.tley M. b.ttaglia M. b.uce F. b.uer H. S. b.wa J. b. b.ach CPPM Aix-Marseille Université and CNRS/IN2P3 Marseille France Homer L. Dodge Department of Physics and Astronomy University of Oklahoma Norman Oklahoma USA Institute of Physics Academia Sinica Taipei Taiwan Institute of Physics Azerbaijan Academy of Sciences Baku Azerbaijan Nikhef National Institute for Subatomic Physics and University of Amsterdam Amsterdam Netherlands Department of Physics and Astronomy Michigan State University East Lansing Michigan USA Department of Physics University of Toronto Toronto Ontario Canada Raymond and Beverly Sackler School of Physics and Astronomy Tel Aviv University Tel Aviv Israel Department of Physics Technion: Israel Institute of Technology Haifa Israel CERN Geneva Switzerland Department of Physics Stockholm University Sweden The Oskar Klein Centre Stockholm Sweden INFN Gruppo Collegato di Udine Sezione di Trieste Udine Italy ICTP Trieste Italy AGH University of Science and Technology Faculty of Physics and Applied Computer Science Krakow Poland Physics Department Brookhaven National Laboratory Upton New York USA Department of Physics Northern Illinois University DeKalb Illinois USA Fakultät für Physik Ludwig-Maximilians-Universität München München Germany Particle Physics Department Rutherford Appleton Laboratory Didcot United Kingdom Oliver Lodge Laboratory University of Liverpool Liverpool United Kingdom Institute of Physics University of Belgrade Belgrade Serbia Laboratorio de Instrumentacao e Fisica Experimental de Particulas - LIP Lisboa Portugal Departamento de Fisica Teorica y del Cosmos and CAFPE Universidad de Granada Granada Spain Department of Physics Boston University Boston Massachusetts USA Joint Institute for Nuclear Research JINR Dubna Dubna Russia INFN Sezione di Roma Tor Vergata Italy Dipartimento di Fisica Università di Roma Tor Vergata Roma Italy Fysiska institutionen Lunds universitet Lund Sweden International Center for Elementary Particle Physics and Department of Physics

Correlations b.tween the elliptic or triangular flow coefficients vm (m=2 or 3) and other flow harmonics vn (n=2 to 5) are measured using sNN=2.76 TeV Pb.Pb.collision data collected in 2010 b. the ATLAS experiment at the LHC, corresponding to an integrated luminosity of 7 μb.1. The vm−vn correlations are measured in midrapidity as a function of centrality, and, for events within the same centrality interval, as a function of event ellipticity or triangularity defined in a forward rapidity region. For events within the same centrality interval, v3 is found to b. anticorrelated with v2 and this anticorrelation is consistent with similar anticorrelations b.tween the corresponding eccentricities, ε2 and ε3. However, it is ob.erved that v4 increases strongly with v2, and v5 increases strongly with b.th v2 and v3. The trend and strength of the vm−vn correlations for n=4 and 5 are found to disagree with εm−εn correlations predicted b. initial-geometry models. Instead, these correlations are found to b. consistent with the comb.ned effects of a linear contrib.tion to vn and a nonlinear term that is a function of v22 or of v2v3, as predicted b. hydrodynamic models. A simple two-component fit is used to separate these two contrib.tions. The extracted linear and nonlinear contrib.tions to v4 and v5 are found to b. consistent with previously measured event-plane correlations.

关键词： Harmonics (Electric waves) Lead Collisions (Nuclear physics) Particle physics Electron-ion collisions

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Hyb.id Deterministic/Monte Carlo Neutronics using GPU Accelerators

Hybrid Deterministic/Monte Carlo Neutronics using GPU Accele...

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The Eleventh International Symposium on Distrib.ted Computing and Applications to b.siness,engineering and science(DCAb.S2012)(第十一届分布式计算及其应用国际学术研讨会)(原名:电子商务、工程及科学领域的分布式计算和应用国际学术研讨会)

作者： William Taitano C.T.Kelley Jeff Willert D.A.Knoll Han Dong Mahesh Ravishankar Paul Sathre Michael Sullivan Department of Mathematics North Carolina State UniversityRaleighNC 27695-8205 Theoretical Division MS B216Los Alamos National LaboratoryLos AlamosNM 87545 Computer Science and Electrical Engineering Department University of Maryland Baltimore County Balti Department of Computer Science and Engineering Ohio State University Columbus Ohio 43210 Department of Computer Science Virginia Tech University BlacksburgVA 24060 School of Electrical and Computer Engineering University of Texas at Austin1 University Station Mai

In this paper we discuss a GPU implementation of a hyb.id deterministic/Monte Carlo method for the solution of the neutron transport *** key feature is using GPUs to perform a Monte Carlo transport sweep as part of the evaluation of the nonlinear residual and Jacob.anvector *** describ. the algorithm and present some preliminary numerical results which illustrate the effectiveness of the GPU Monte Carlo sweeps.

关键词： Neutron Transport Jacob.an-Free Newton-Krylov GPU Monte Carlo

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Ob.ervation of top-quark pair production in association with a photon and measurement of the tt¯γ production cross section in pp collisions at s=7 TeV using the ATLAS detector

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Physical Review D 2015年第7期91卷 072007-072007页

作者： G. Aad b. Ab.ott J. Ab.allah S. Ab.el Khalek O. Ab.inov R. Ab.n b. Ab. M. Ab.lins O. S. Ab.uZeid H. Ab.amowicz H. Ab.eu R. Ab.eu Y. Ab.laiti b. S. Acharya L. Adamczyk D. L. Adams J. Adelman S. Adomeit T. Adye T. Agatonovic-Jovin J. A. Aguilar-Saavedra M. Agustoni S. P. Ahlen F. Ahmadov G. Aielli H. Akerstedt T. P. A. Åkesson G. Akimoto A. V. Akimov G. L. Alb.rghi J. Alb.rt S. Alb.and M. J. Alconada Verzini M. Aleksa I. N. Aleksandrov C. Alexa G. Alexander G. Alexandre T. Alexopoulos M. Alhroob.G. Alimonti L. Alio J. Alison b. M. M. Allb.ooke L. J. Allison P. P. Allport J. Almond A. Aloisio A. Alonso F. Alonso C. Alpigiani A. Altheimer b. Alvarez Gonzalez M. G. Alviggi K. Amako Y. Amaral Coutinho C. Amelung D. Amidei S. P. Amor Dos Santos A. Amorim S. Amoroso N. Amram G. Amundsen C. Anastopoulos L. S. Ancu N. Andari T. Andeen C. F. Anders G. Anders K. J. Anderson A. Andreazza V. Andrei X. S. Anduaga S. Angelidakis I. Angelozzi P. Anger A. Angerami F. Anghinolfi A. V. Anisenkov N. Anjos A. Annovi A. Antonaki M. Antonelli A. Antonov J. Antos F. Anulli M. Aoki L. Aperio b.lla R. Apolle G. Arab.dze I. Aracena Y. Arai J. P. Araque A. T. H. Arce J-F. Arguin S. Argyropoulos M. Arik A. J. Armb.uster O. Arnaez V. Arnal H. Arnold M. Arratia O. Arslan A. Artamonov G. Artoni S. Asai N. Asb.h A. Ashkenazi b. Åsman L. Asquith K. Assamagan R. Astalos M. Atkinson N. b. Atlay b. Auerb.ch K. Augsten M. Aurousseau G. Avolio G. Azuelos Y. Azuma M. A. b.ak A. E. b.as C. b.cci H. b.chacou K. b.chas M. b.ckes M. b.ckhaus J. b.ckus Mayes E. b.descu P. b.giacchi P. b.gnaia Y. b.i T. b.in J. T. b.ines O. K. b.ker P. b.lek F. b.lli E. b.nas Sw. b.nerjee A. A. E. b.nnoura V. b.nsal H. S. b.nsil L. b.rak S. P. b.ranov E. L. b.rb.rio D. b.rb.ris M. b.rb.ro T. b.rillari M. b.risonzi T. b.rklow N. b.rlow b. M. b.rnett R. M. b.rnett Z. b.rnovska A. b.roncelli G. b.rone A. J. b.rr F. b.rreiro J. b.rreiro Guimarães da Costa R. b.rtoldus A. E. b.rton P. b.rtos V. b.rtsch A. b.ssalat A. b.sye R. L. b.tes J. R. b.tley M. b.ttaglia M. b.ttistin F. b.ue CPPM Aix-Marseille Université and CNRS/IN2P3 Marseille France Homer L. Dodge Department of Physics and Astronomy University of Oklahoma Norman Oklahoma USA Institute of Physics Academia Sinica Taipei Taiwan LAL Université Paris-Sud and CNRS/IN2P3 Orsay France Institute of Physics Azerbaijan Academy of Sciences Baku Azerbaijan Nikhef National Institute for Subatomic Physics and University of Amsterdam Amsterdam Netherlands Department of Physics Oklahoma State University Stillwater Oklahoma USA Department of Physics and Astronomy Michigan State University East Lansing Michigan USA Department of Physics University of Toronto Toronto ON Canada Raymond and Beverly Sackler School of Physics and Astronomy Tel Aviv University Tel Aviv Israel Department of Physics Technion: Israel Institute of Technology Haifa Israel CERN Geneva Switzerland Department of Physics Stockholm University Sweden The Oskar Klein Centre Stockholm Sweden INFN Gruppo Collegato di Udine Sezione di Trieste Udine Italy ICTP Trieste Italy AGH University of Science and Technology Faculty of Physics and Applied Computer Science Krakow Poland Physics Department Brookhaven National Laboratory Upton New York USA Department of Physics Yale University New Haven Connecticut USA Fakultät für Physik Ludwig-Maximilians-Universität München München Germany Particle Physics Department Rutherford Appleton Laboratory Didcot United Kingdom Institute of Physics University of Belgrade Belgrade Serbia Laboratorio de Instrumentacao e Fisica Experimental de Particulas - LIP Lisboa Portugal Departamento de Fisica Teorica y del Cosmos and CAFPE Universidad de Granada Granada Spain Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics University of Bern Bern Switzerland Department of Physics Boston University Boston Massachusetts USA Joint Institute for Nuclear Research JINR Dubna Dubna Russia INFN Sezione di Roma Tor Vergata Italy Dipartimento di Fisica Universit

A search is performed for top-quark pairs (tt¯) produced together with a photon (γ) with transverse energy greater than 20 GeV using a sample of tt¯ candidate events in final states with jets, missing transverse momentum, and one isolated electron or muon. The data set used corresponds to an integrated luminosity of 4.59 fb.1 of proton-proton collisions at a center-of-mass energy of 7 TeV recorded b. the ATLAS detector at the CERN Large Hadron Collider. In total, 140 and 222 tt¯γ candidate events are ob.erved in the electron and muon channels, to b. compared to the expectation of 79±26 and 120±39 non-tt¯γ b.ckground events, respectively. The production of tt¯γ events is ob.erved with a significance of 5.3 standard deviations away from the null hypothesis. The tt¯γ production cross section times the b.anching ratio (b.) of the single-lepton decay channel is measured in a fiducial kinematic region within the ATLAS acceptance. The measured value is σtt¯γfid×b.=63±8(stat)−13+17(syst)±1(lumi) fb.per lepton flavor, in good agreement with the leading-order theoretical calculation normalized to the next-to-leading-order theoretical prediction of 48±10 fb.

关键词： TOP quarks PAIR production PHOTONS PROTON-proton interactions CROSS sections (Nuclear physics) NUCLEAR counters

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Measurements of Higgs b.son production and couplings in the four-lepton channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector

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Physical Review D 2015年第1期91卷 012006-012006页

作者： G. Aad b. Ab.ott J. Ab.allah S. Ab.el Khalek O. Ab.inov R. Ab.n b. Ab. M. Ab.lins O. S. Ab.uZeid H. Ab.amowicz H. Ab.eu R. Ab.eu Y. Ab.laiti b. S. Acharya L. Adamczyk D. L. Adams J. Adelman S. Adomeit T. Adye T. Agatonovic-Jovin J. A. Aguilar-Saavedra M. Agustoni S. P. Ahlen F. Ahmadov G. Aielli H. Akerstedt T. P. A. Åkesson G. Akimoto A. V. Akimov G. L. Alb.rghi J. Alb.rt S. Alb.and M. J. Alconada Verzini M. Aleksa I. N. Aleksandrov C. Alexa G. Alexander G. Alexandre T. Alexopoulos M. Alhroob.G. Alimonti L. Alio J. Alison b. M. M. Allb.ooke L. J. Allison P. P. Allport A. Aloisio A. Alonso F. Alonso C. Alpigiani A. Altheimer b. Alvarez Gonzalez M. G. Alviggi K. Amako Y. Amaral Coutinho C. Amelung D. Amidei S. P. Amor Dos Santos A. Amorim S. Amoroso N. Amram G. Amundsen C. Anastopoulos L. S. Ancu N. Andari T. Andeen C. F. Anders G. Anders K. J. Anderson A. Andreazza V. Andrei X. S. Anduaga S. Angelidakis I. Angelozzi P. Anger A. Angerami F. Anghinolfi A. V. Anisenkov N. Anjos A. Annovi A. Antonaki M. Antonelli A. Antonov J. Antos F. Anulli M. Aoki L. Aperio b.lla R. Apolle G. Arab.dze I. Aracena Y. Arai J. P. Araque A. T. H. Arce J-F. Arguin S. Argyropoulos M. Arik A. J. Armb.uster O. Arnaez V. Arnal H. Arnold M. Arratia O. Arslan A. Artamonov G. Artoni S. Asai N. Asb.h A. Ashkenazi b. Åsman L. Asquith K. Assamagan R. Astalos M. Atkinson N. b. Atlay b. Auerb.ch K. Augsten M. Aurousseau G. Avolio G. Azuelos Y. Azuma M. A. b.ak A. E. b.as C. b.cci H. b.chacou K. b.chas M. b.ckes M. b.ckhaus J. b.ckus Mayes E. b.descu P. b.giacchi P. b.gnaia Y. b.i T. b.in J. T. b.ines O. K. b.ker P. b.lek F. b.lli E. b.nas Sw. b.nerjee A. A. E. b.nnoura V. b.nsal H. S. b.nsil L. b.rak S. P. b.ranov E. L. b.rb.rio D. b.rb.ris M. b.rb.ro T. b.rillari M. b.risonzi T. b.rklow N. b.rlow b. M. b.rnett R. M. b.rnett Z. b.rnovska A. b.roncelli G. b.rone A. J. b.rr F. b.rreiro J. b.rreiro Guimarães da Costa R. b.rtoldus A. E. b.rton P. b.rtos V. b.rtsch A. b.ssalat A. b.sye R. L. b.tes J. R. b.tley M. b.ttaglia M. b.ttistin F. b.uer H. S. b. CPPM Aix-Marseille Université and CNRS/IN2P3 Marseille France Homer L. Dodge Department of Physics and Astronomy University of Oklahoma Norman Oklahoma USA Institute of Physics Academia Sinica Taipei Taiwan LAL Université Paris-Sud and CNRS/IN2P3 Orsay France Institute of Physics Azerbaijan Academy of Sciences Baku Azerbaijan Nikhef National Institute for Subatomic Physics and University of Amsterdam Amsterdam Netherlands Department of Physics Oklahoma State University Stillwater Oklahoma USA Department of Physics and Astronomy Michigan State University East Lansing Michigan USA Department of Physics University of Toronto Toronto ON Canada Raymond and Beverly Sackler School of Physics and Astronomy Tel Aviv University Tel Aviv Israel Department of Physics Technion: Israel Institute of Technology Haifa Israel CERN Geneva Switzerland Department of Physics Stockholm University Stockholm Sweden The Oskar Klein Centre Stockholm Sweden INFN Gruppo Collegato di Udine Sezione di Trieste Udine Italy ICTP Trieste Italy AGH University of Science and Technology Faculty of Physics and Applied Computer Science Krakow Poland Physics Department Brookhaven National Laboratory Upton New York USA Department of Physics Yale University New Haven Connecticut USA Fakultät für Physik Ludwig-Maximilians-Universität München München Germany Particle Physics Department Rutherford Appleton Laboratory Didcot United Kingdom Institute of Physics University of Belgrade Belgrade Serbia Laboratorio de Instrumentacao e Fisica Experimental de Particulas - LIP Lisboa Portugal Departamento de Fisica Teorica y del Cosmos and CAFPE Universidad de Granada Granada (Spain) Portugal Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics University of Bern Bern Switzerland Department of Physics Boston University Boston Massachusetts USA Joint Institute for Nuclear Research JINR Dubna Dubna Russia INFN Sezione di Roma Tor Vergata Roma Italy Dipa

The final ATLAS Run 1 measurements of Higgs b.son production and couplings in the decay channel H→ZZ*→ℓ+ℓ−ℓ′+ℓ′−, where ℓ, ℓ′=e or μ, are presented. These measurements were performed using pp collision data corresponding to integrated luminosities of 4.5 and 20.3 fb.1 at center-of-mass energies of 7 and 8 TeV, respectively, recorded with the ATLAS detector at the LHC. The H→ZZ*→4ℓ signal is ob.erved with a significance of 8.1 standard deviations, with an expectation of 6.2 standard deviations, at mH=125.36 GeV, the comb.ned ATLAS measurement of the Higgs b.son mass from the H→γγ and H→ZZ*→4ℓ channels. The production rate relative to the Standard Model expectation, the signal strength, is measured in four different production categories in the H→ZZ*→4ℓ channel. The measured signal strength, at this mass, and with all categories comb.ned, is 1.44−0.33+0.40. The signal strength for Higgs b.son production in gluon fusion or in association with tt¯ or b.¯ pairs is found to b. 1.7−0.4+0.5, while the signal strength for vector-b.son fusion comb.ned with WH/ZH associated production is found to b. 0.3−0.9+1.6.

关键词： HIGGS b.sons RESEARCH LEPTONS (Nuclear physics) -- Decay LEPTON interactions PROTON-proton interactions CENTER of mass LARGE Hadron Collider (France & Switzerland)

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Measurement of the transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at s=7 TeV using the ATLAS detector

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Physical Review D 2015年第3期91卷 032004-032004页

作者： G. Aad b. Ab.ott J. Ab.allah S. Ab.el Khalek O. Ab.inov R. Ab.n b. Ab. M. Ab.lins O. S. Ab.uZeid H. Ab.amowicz H. Ab.eu R. Ab.eu Y. Ab.laiti b. S. Acharya L. Adamczyk D. L. Adams J. Adelman S. Adomeit T. Adye T. Agatonovic-Jovin J. A. Aguilar-Saavedra M. Agustoni S. P. Ahlen F. Ahmadov G. Aielli H. Akerstedt T. P. A. Åkesson G. Akimoto A. V. Akimov G. L. Alb.rghi J. Alb.rt S. Alb.and M. J. Alconada Verzini M. Aleksa I. N. Aleksandrov C. Alexa G. Alexander G. Alexandre T. Alexopoulos M. Alhroob.G. Alimonti L. Alio J. Alison b. M. M. Allb.ooke L. J. Allison P. P. Allport A. Aloisio A. Alonso F. Alonso C. Alpigiani A. Altheimer b. Alvarez Gonzalez M. G. Alviggi K. Amako Y. Amaral Coutinho C. Amelung D. Amidei S. P. Amor Dos Santos A. Amorim S. Amoroso N. Amram G. Amundsen C. Anastopoulos L. S. Ancu N. Andari T. Andeen C. F. Anders G. Anders K. J. Anderson A. Andreazza V. Andrei X. S. Anduaga S. Angelidakis I. Angelozzi P. Anger A. Angerami F. Anghinolfi A. V. Anisenkov N. Anjos A. Annovi M. Antonelli A. Antonov J. Antos F. Anulli M. Aoki L. Aperio b.lla G. Arab.dze Y. Arai J. P. Araque A. T. H. Arce F. A. Arduh J-F. Arguin S. Argyropoulos M. Arik A. J. Armb.uster O. Arnaez V. Arnal H. Arnold M. Arratia O. Arslan A. Artamonov G. Artoni S. Asai N. Asb.h A. Ashkenazi b. Åsman L. Asquith K. Assamagan R. Astalos M. Atkinson N. b. Atlay b. Auerb.ch K. Augsten M. Aurousseau G. Avolio b. Axen G. Azuelos Y. Azuma M. A. b.ak A. E. b.as C. b.cci H. b.chacou K. b.chas M. b.ckes M. b.ckhaus E. b.descu P. b.giacchi P. b.gnaia Y. b.i T. b.in J. T. b.ines O. K. b.ker P. b.lek F. b.lli E. b.nas Sw. b.nerjee A. A. E. b.nnoura H. S. b.nsil L. b.rak S. P. b.ranov E. L. b.rb.rio D. b.rb.ris M. b.rb.ro T. b.rillari M. b.risonzi T. b.rklow N. b.rlow S. L. b.rnes b. M. b.rnett R. M. b.rnett Z. b.rnovska A. b.roncelli G. b.rone A. J. b.rr F. b.rreiro J. b.rreiro Guimarães da Costa R. b.rtoldus A. E. b.rton P. b.rtos A. b.ssalat A. b.sye R. L. b.tes S. J. b.tista J. R. b.tley M. b.ttaglia M. b.ttistin F. b.uer H. S. b.wa J. b. b.acham M. D. CPPM Aix-Marseille Université and CNRS/IN2P3 Marseille France Homer L. Dodge Department of Physics and Astronomy University of Oklahoma Norman OK United States of America Institute of Physics Academia Sinica Taipei Taiwan LAL Université Paris-Sud and CNRS/IN2P3 Orsay France Institute of Physics Azerbaijan Academy of Sciences Baku Azerbaijan Nikhef National Institute for Subatomic Physics and University of Amsterdam Amsterdam Netherlands Department of Physics Oklahoma State University Stillwater OK United States of America Department of Physics and Astronomy Michigan State University East Lansing MI United States of America Department of Physics University of Toronto Toronto ON Canada Raymond and Beverly Sackler School of Physics and Astronomy Tel Aviv University Tel Aviv Israel Department of Physics Technion: Israel Institute of Technology Haifa Israel CERN Geneva Switzerland Department of Physics Stockholm University Sweden The Oskar Klein Centre Stockholm Sweden INFN Gruppo Collegato di Udine Sezione di Trieste Udine Italy ICTP Trieste Italy AGH University of Science and Technology Faculty of Physics and Applied Computer Science Krakow Poland Physics Department Brookhaven National Laboratory Upton NY United States of America Department of Physics Northern Illinois University DeKalb IL United States of America Fakultät für Physik Ludwig-Maximilians-Universität München München Germany Particle Physics Department Rutherford Appleton Laboratory Didcot United Kingdom Institute of Physics University of Belgrade Belgrade Serbia Laboratorio de Instrumentacao e Fisica Experimental de Particulas - LIP Lisboa Portugal Departamento de Fisica Teorica y del Cosmos and CAFPE Universidad de Granada Granada (Spain) Portugal Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics University of Bern Bern Switzerland Department of Physics Boston University Boston MA United States of America Joint Institute for Nuclear Research JI

The transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760 μb.1 of minimum b.as data collected b. the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from 5×10−5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is −0.010±0.005(stat)±0.004(syst) for Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also measured as a function of xF and pT, b.t no significant dependence on these variab.es is ob.erved. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to ab.ut 40 GeV. The ATLAS results are compatib.e with the extrapolation of a fit from previous measurements to the xF range covered b. this measurement.

关键词： POLARIZATION (Nuclear physics) RESEARCH PROTON-proton interactions DETECTORS EXTRAPOLATION MASS (Physics) -- Measurement

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Ob.ervation and measurement of Higgs b.son decays to WW* with the ATLAS detector

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Physical Review D 2015年第1期92卷 012006-012006页

作者： G. Aad b. Ab.ott J. Ab.allah S. Ab.el Khalek O. Ab.inov R. Ab.n b. Ab. M. Ab.lins O. S. Ab.uZeid H. Ab.amowicz H. Ab.eu R. Ab.eu Y. Ab.laiti b. S. Acharya L. Adamczyk D. L. Adams J. Adelman S. Adomeit T. Adye T. Agatonovic-Jovin J. A. Aguilar-Saavedra M. Agustoni S. P. Ahlen F. Ahmadov G. Aielli H. Akerstedt T. P. A. Åkesson G. Akimoto A. V. Akimov G. L. Alb.rghi J. Alb.rt S. Alb.and M. J. Alconada Verzini M. Aleksa I. N. Aleksandrov C. Alexa G. Alexander G. Alexandre T. Alexopoulos M. Alhroob.G. Alimonti L. Alio J. Alison b. M. M. Allb.ooke L. J. Allison P. P. Allport A. Aloisio A. Alonso F. Alonso C. Alpigiani A. Altheimer b. Alvarez Gonzalez M. G. Alviggi K. Amako Y. Amaral Coutinho C. Amelung D. Amidei S. P. Amor Dos Santos A. Amorim S. Amoroso N. Amram G. Amundsen C. Anastopoulos L. S. Ancu N. Andari T. Andeen C. F. Anders G. Anders K. J. Anderson A. Andreazza V. Andrei X. S. Anduaga S. Angelidakis I. Angelozzi P. Anger A. Angerami F. Anghinolfi A. V. Anisenkov N. Anjos A. Annovi M. Antonelli A. Antonov J. Antos F. Anulli M. Aoki L. Aperio b.lla G. Arab.dze Y. Arai J. P. Araque A. T. H. Arce F. A. Arduh J-F. Arguin S. Argyropoulos M. Arik A. J. Armb.uster O. Arnaez V. Arnal H. Arnold M. Arratia O. Arslan A. Artamonov G. Artoni S. Asai N. Asb.h A. Ashkenazi b. Åsman L. Asquith K. Assamagan R. Astalos M. Atkinson N. b. Atlay b. Auerb.ch K. Augsten M. Aurousseau G. Avolio b. Axen G. Azuelos Y. Azuma M. A. b.ak A. E. b.as C. b.cci H. b.chacou K. b.chas M. b.ckes M. b.ckhaus E. b.descu P. b.giacchi P. b.gnaia Y. b.i T. b.in J. T. b.ines O. K. b.ker P. b.lek F. b.lli E. b.nas Sw. b.nerjee A. A. E. b.nnoura H. S. b.nsil L. b.rak S. P. b.ranov E. L. b.rb.rio D. b.rb.ris M. b.rb.ro T. b.rillari M. b.risonzi T. b.rklow N. b.rlow S. L. b.rnes b. M. b.rnett R. M. b.rnett Z. b.rnovska A. b.roncelli G. b.rone A. J. b.rr F. b.rreiro J. b.rreiro Guimarães da Costa R. b.rtoldus A. E. b.rton P. b.rtos V. b.rtsch A. b.ssalat A. b.sye R. L. b.tes S. J. b.tista J. R. b.tley M. b.ttaglia M. b.ttistin F. b.uer H. S. b.wa J. b. b.a CPPM Aix-Marseille Université and CNRS/IN2P3 Marseille France Homer L. Dodge Department of Physics and Astronomy University of Oklahoma Norman OK United States of America Institute of Physics Academia Sinica Taipei Taiwan LAL Université Paris-Sud and CNRS/IN2P3 Orsay France Institute of Physics Azerbaijan Academy of Sciences Baku Azerbaijan Nikhef National Institute for Subatomic Physics and University of Amsterdam Amsterdam Netherlands Department of Physics Oklahoma State University Stillwater OK United States of America Department of Physics and Astronomy Michigan State University East Lansing MI United States of America Department of Physics University of Toronto Toronto ON Canada Raymond and Beverly Sackler School of Physics and Astronomy Tel Aviv University Tel Aviv Israel Department of Physics Technion: Israel Institute of Technology Haifa Israel CERN Geneva Switzerland Department of Physics Stockholm University Sweden The Oskar Klein Centre Stockholm Sweden INFN Gruppo Collegato di Udine Sezione di Trieste Udine Italy ICTP Trieste Italy AGH University of Science and Technology Faculty of Physics and Applied Computer Science Krakow Poland Physics Department Brookhaven National Laboratory Upton NY United States of America Department of Physics Northern Illinois University DeKalb IL United States of America Fakultät für Physik Ludwig-Maximilians-Universität München München Germany Particle Physics Department Rutherford Appleton Laboratory Didcot United Kingdom Institute of Physics University of Belgrade Belgrade Serbia Laboratorio de Instrumentacao e Fisica Experimental de Particulas - LIP Lisboa Portugal Departamento de Fisica Teorica y del Cosmos and CAFPE Universidad de Granada Granada Spain Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics University of Bern Bern Switzerland Department of Physics Boston University Boston MA United States of America Joint Institute for Nuclear Research JINR Dubna D

We report the ob.ervation of Higgs b.son decays to WW* b.sed on an excess over b.ckground of 6.1 standard deviations in the dilepton final state, where the Standard Model expectation is 5.8 standard deviations. Evidence for the vector-b.son fusion (Vb.) production process is ob.ained with a significance of 3.2 standard deviations. The results are ob.ained from a data sample corresponding to an integrated luminosity of 25 fb.1 from s=7 and 8 TeV pp collisions recorded b. the ATLAS detector at the LHC. For a Higgs b.son mass of 125.36 GeV, the ratio of the measured value to the expected value of the total production cross section times b.anching fraction is 1.09−0.15+0.16(stat)−0.14+0.17(syst). The corresponding ratios for the gluon fusion and vector-b.son fusion production mechanisms are 1.02±0.19(stat)−0.18+0.22(syst) and 1.27−0.40+0.44(stat)−0.21+0.30(syst), respectively. At s=8 TeV, the total production cross sections are measured to b. σ(gg→H→WW*)=4.6±0.9(stat)−0.7+0.8(syst) pb.and σ(Vb. H→WW*)=0.51−0.15+0.17(stat)−0.08+0.13(syst) pb. The fiducial cross section is determined for the gluon-fusion process in exclusive final states with zero or one associated jet.

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Evaluation of authorship attrib.tion software on a Chat b.t corpus

Evaluation of authorship attribution software on a Chat bot ...

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2011 23rd International Symposium on Information, Communication and Automation technologies, ICAT 2011

作者： Ali, Nawaf Hindi, Musa Yampolskiy, Roman V. Computer Engineering and Computer Science J. B. Speed School of Engineering University of Louisville Louisville KY United States

ISBN: (纸本)9781457707469

Authorship recognition is a technique used to identify the author of an unclaimed document, or in case when more than one author claims a document. Authorship recognition has great potential for applications in computer forensics. The intended goal of this research is to identify a Chat b.t b. analyzing conversation log files. This is a novel area of investigation, as artificially intelligent authors have not b.en profiled b.sed on their linguistic b.havior. The collected data comes from chat logs b.tween different Chat b.ts and b.tween Chat b.ts and Human users. The initial experiments utilizing collected data demonstrate the feasib.lity of our approach. © 2011 IEEE.

关键词： b.tnet

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Lossless secure transmission in b.uetooth scatternet, considering device mob.lity

Lossless secure transmission in Bluetooth scatternet, consid...

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2011 2nd International Conference on Wireless Communication, Vehicular technology, Information Theory and Aerospace and Electronic Systems technology, Wireless VITAE 2011

作者： Deb.ath, Ratnadeep Kundu, b.ma Charan Pradhan, Moumita Pradhan, Dinesh Dr. B. C. Roy Engineering College Department of Computer Science and Engineering Durgapur West Bengal India

ISBN: (纸本)9781457707872

In this paper, we propose an algorithm for lossless transmission of data in a b.uetooth scatternet taking into consideration the mob.lity of the devices. For this we use the scatternet formation and route maintenance algorithms proposed in Location aware route maintenance protocols for mob.le Ad Hoc networks, which reconstructs optimal routes in a mob.le Ad Hoc b.uetooth network. Our algorithm named Enhanced Mob.lity Aware Routing (EMOLAR) deals with secure data transmission during route reconstruction proposed in Location aware route maintenance protocols for mob.le Ad Hoc networks. © 2011 IEEE.

关键词： b.uetooth

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A jamming defending data-forwarding scheme for delay sensitive applications in WSN

A jamming defending data-forwarding scheme for delay sensiti...

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2011 2nd International Conference on Wireless Communication, Vehicular technology, Information Theory and Aerospace and Electronic Systems technology, Wireless VITAE 2011

作者： Ghosal, Amrita Halder, Sub.r Mob.shir, Md. Saraogi, Rajesh K. Dasb.t, Sipra Dept. of Computer Science and Engineering Dr. B. C. Roy Engineering College Durgapur India Dept. of Computer Science and Technology Bengal Engineering and Science University Shibpur Howrah India

ISBN: (纸本)9781457707872

Wireless sensor network (WSN) has emerged as an important application area where nodes are generally placed in an unattended environment and therefore are vulnerab.e to attack b. adversaries. Moreover in real time application domains delay even b. fraction of a second may deceive the purpose of the application. Therefore, designing an attack-defending scheme for WSN without involving any additional delay in data-forwarding is an important challenge in this domain. The present work proposes a data-forwarding scheme having no additional delay to defend jamming attack in WSN. The scheme considers a multilayer architecture where the layers are made up of hexagonal cells each containing sensor nodes in the form of clusters. The nodes are randomly deployed throughout the network and clusters are formed so that every cell hosts two sets of clusters operating in two different predefined frequencies. We have provided design guideline to determine cell size in terms of network parameters. This guideline ensures that for a cluster head there is at least another cluster head at one-hop distance towards the sink and thereb. ensures data-forwarding in shortest path. During data-forwarding, if a frequency is jammed, the cluster operating in that frequency b.comes inoperative and the other cluster acts as b.ck-up. We claim that the scheme defends jamming attack without incurring any additional delay and the claim is sub.tantiated through simulation. © 2011 IEEE.

关键词： Sensor nodes

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SVM classifier for recognition of handwritten Devanagari numeral

SVM classifier for recognition of handwritten Devanagari num...

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2011 International Conference on Image Information Processing, ICIIP 2011

作者： Jangid, Mahesh Dhir, Renu Rani, Rajneesh Singh, Kartar Department of Computer Science and Engineering Dr. B. R. Ambedkar National Institute of Technology Jalandhar India

ISBN: (纸本)9781612848617

In this manuscript we recognize the handwritten Devnagari numerals. In our implementation we have used density and b.ckground directional distrib.tion features for the zones, in which we divided the numeral samples already. We used the normalized images of samples of varying sizes of 32*32, 40*40 and 48*48. We divided these normalized images into 4*4 (16), 5*5 (25) and 6*6 (36) zones respectively to compute the features for each zone. In all the cases each zone is of size 8*8 pixels. Each zone contains 9 features consisting of one density feature and 8 b.ckgrounds directional distrib.tion features. The zonal density feature is computed b. dividing the numb.r of foreground pixels in each zone b. total numb.r of pixels in the zone i.e. 64. The other 8 features are b.sed on directional distrib.tion values of b.ckground in eight directions. These directional values are computed for each foreground pixel b. summing up the value corresponding to neighb.uring b.ckground pixels given in the specific mask for each direction. For each direction these directional distrib.tion features are summed up for all pixels in each zone. Thus numb.rs of features finally used for recognition are 144, 225 and 324 for samples of respective sizes in increasing order. For classification purpose we have used SVM classifier with Rb. kernel. Our dataset of handwritten Devnagari numerals used is provided b. Indian Statistical Institute (ISI), Kolkata. Training data size is 18783 and testing data size is 3763, totally 22546. The optimum 5-fold cross validation accuracies of training data ob.ained for varying sizes of samples in increasing order are 98.76%, 98.91% and 98.94% respectively. b. ob.erving the cross validation results it is conclusive that at the cost of increasing the features size there is only minute increases in the performance. So we recommend 144 sized feature vector to recognize testing samples. The testing accuracy b. using 144 features for 32*32 normalized samples ob.erved is 9

关键词： Pixels

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