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dc.rights.licensehttp://creativecommons.org/licenses/by-nc-sa/3.0/ve/
dc.contributor.authorCimmarusti, Andréses_VE
dc.date2008-08-07es_VE
dc.date.accessioned2008-08-07T09:00:00Z
dc.date.available2008-08-07T09:00:00Z
dc.date.created2006-11-24es_VE
dc.date.issued2008-08-07T09:00:00Zes_VE
dc.identifier.otherT016300005136/0es_VE
dc.identifier.urihttp://www.saber.ula.ve/handle/123456789/14687
dc.description.abstractAnálisis del sismo del Táchira del 31 de mayo de 1994 y sus réplicas (Mata S., Sara M.) Resumen Particle physics includes all the experimental research aimed at advancing in the understanding of quarks (the components of protons and neutrons) and leptons (such as electrons), as well as their mutual interactions. The study of the properties of the top quark, the heaviest of the six known quarks, in particular its mass, is of uttermost importance as it may give clues on the origin of the mass di®erence between the particles and indicate the existence of physics beyond the Standard Model of particle physics. At the start of the Large Hadron Collider at Cern in 2007, the top quark will be produced with large statistics. The Atlas experiment will have the possibility to study its properties in great detail. The top quark is an unstable particle that decays almost instantaneously and exclusively into a b quark and a W boson, which in turn form jets of stable particles. The precision in the measurement of top quark properties will be limited by the knowledge of some of the detector performances, such as the precision to which the particle energies are measured, or the e±ciency with which we can identify some of these particles. The preparation of physics analyses requires the best knowledge of detectors and physics simulation. I have worked during my internship at the LPNHE Paris on the preparation of two physics analyses on simulated data. A first study has been performed, corresponding to the commisioning phase of the detector with the first data. It has been shown that in Atlas the top quark can be easily reconstructed, even using a very simple selection and without fulfilling requirements such as flavour tagging or jet energy reconstruction. A second analysis has been performed after the detector and the data were understood. The background due to jets misidentified in the detector as electrons has been studied and found to be negligible. The mass reconstruction performance has been studied for different selections of the final state of the top quark decay. The statistical uncertainty on it will become negligible after a few weeks of data taking compared to the uncertainties related to the jet energy reconstruction. These analyses are a first step for the LPNHE group in their development of physics analyses for the top quark mass measurement.es_VE
dc.description.sponsorshipUniversidad de Los Andeses_VE
dc.description.tableofcontents1. Abstractes_VE
dc.description.tableofcontents2. The Standard Modeles_VE
dc.description.tableofcontents2.1 Particle Organizationes_VE
dc.description.tableofcontents2.2 Unanswered questionses_VE
dc.description.tableofcontents2.3 Top quark physicses_VE
dc.description.tableofcontents2.3.1 Top quark production in colliderses_VE
dc.description.tableofcontents2.3.2 Characteristics of tt eventses_VE
dc.description.tableofcontents2.3.3 Reducible backgroundses_VE
dc.description.tableofcontents3. The ATLAS experimentes_VE
dc.description.tableofcontents3.1 The LHC at CERNes_VE
dc.description.tableofcontents3.2 The ATLAS detectores_VE
dc.description.tableofcontents3.2.1 Coordinate systemes_VE
dc.description.tableofcontents3.2.2 Tracking system or Inner Detectores_VE
dc.description.tableofcontents3.2.3 Calorimetryes_VE
dc.description.tableofcontents3.2.4 Muon spectrometeres_VE
dc.description.tableofcontents3.2.5 Magnet systemes_VE
dc.description.tableofcontents3.2.6 Trigger systemes_VE
dc.description.tableofcontents3.3 Data flowes_VE
dc.description.tableofcontents3.3.1 Physics generationes_VE
dc.description.tableofcontents3.3.2 Detector response simulationes_VE
dc.description.tableofcontents3.3.3 Event selection and reconstructiones_VE
dc.description.tableofcontents3.4 Data samplees_VE
dc.description.tableofcontents4. Particle identificationes_VE
dc.description.tableofcontents4.1 Jet reconstructiones_VE
dc.description.tableofcontents4.1.1 Algorithmes_VE
dc.description.tableofcontents4.1.2 Jet definitiones_VE
dc.description.tableofcontents4.1.3 Jet energy precalibrationes_VE
dc.description.tableofcontents4.2 Electron reconstructiones_VE
dc.description.tableofcontents4.3 Muon reconstructiones_VE
dc.description.tableofcontents4.4 Missing ETes_VE
dc.description.tableofcontents5. Fighting against reducible background: electron / jet separationes_VE
dc.description.tableofcontents5.1 Selection criteriaes_VE
dc.description.tableofcontents5.1.1 Trigger selectiones_VE
dc.description.tableofcontents5.1.2 Offline Analysises_VE
dc.description.tableofcontents5.2 Electron identification performancees_VE
dc.description.tableofcontents5.3 Jet rejectiones_VE
dc.description.tableofcontents6. Top events selection without calibration and b-tagginges_VE
dc.description.tableofcontents6.1 Selection of eventses_VE
dc.description.tableofcontents6.1.1 Preselectiones_VE
dc.description.tableofcontents6.1.2 Final selectiones_VE
dc.description.tableofcontents6.1.3 Selection of the light jetses_VE
dc.description.tableofcontents6.2 Top mass measurementes_VE
dc.description.tableofcontents7. Analysis using b-tagging informationes_VE
dc.description.tableofcontents7.1 Selection of eventses_VE
dc.description.tableofcontents7.1.1 Preselectiones_VE
dc.description.tableofcontents7.1.2 Final selectiones_VE
dc.description.tableofcontentsB.2.1. Localizacioneses_VE
dc.description.tableofcontentsB.2.2. Eventos de Referenciaes_VE
dc.description.tableofcontentsB.2.3. Relocalizacioneses_VE
dc.description.tableofcontents7.2 Hadronic W reconstructiones_VE
dc.description.tableofcontents7.2.1 In situ jet energy calibrationes_VE
dc.description.tableofcontents7.2.2 W mass reconstructiones_VE
dc.description.tableofcontents7.3 Top reconstructiones_VE
dc.description.tableofcontents7.3.1 Choice of the b-jet associated to the hadronic Wes_VE
dc.description.tableofcontents7.3.2 Top mass measurementes_VE
dc.description.tableofcontents7.3.3 Systematic errorses_VE
dc.description.tableofcontents8. Conclusiones_VE
dc.format.extent17193645es_VE
dc.language.isoeses_VE
dc.publisherSABER ULAes_VE
dc.rightsinfo:eu-repo/semantics/openAccess
dc.titleHigh energy Latinamerican-European network fellowshipes_VE
dc.title.alternativeAnalysis of top anti-top decays in the lepton plus jets channel at the ATLAS experimentes_VE
dc.typeinfo:eu-repo/semantics/bachelorThesis
dc.description.colacion52es_VE
dc.description.cotaCIENCIAS-0011es_VE
dc.description.gradoFísicoes_VE
dc.description.tiponivelNivel monográficoes_VE
dc.subject.Mots-clesFísicaes_VE
dc.subject.departamentoDepartamento de Físicaes_VE
dc.subject.facultadFacultad de Ciencias.es_VE
dc.subject.idiomaIngléses_VE
dc.subject.keywordsNetworkes_VE
dc.subject.tipoTesises_VE


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