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26/09/2011, 09:00
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Adrian Signer (IPPP)26/09/2011, 09:15
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Sasa Fratina (University of Pennsylvania)26/09/2011, 09:45
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Kevin Lannon (University of Notre Dame)26/09/2011, 10:15
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Peter Uwer (Humboldt-Universität zu Berlin)26/09/2011, 11:15
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Emanuele Re (IPPP, Durham University)26/09/2011, 11:45
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Ford Garberson (Yale University)26/09/2011, 12:15
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Jason Slaunwhite (University of Notre Dame)26/09/2011, 12:45
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Daniel Maitre (CERN/IPPP Durham)26/09/2011, 15:00
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Rikkert Frederix (University of Zurich)26/09/2011, 15:30
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Pierluigi Catastini (Harvard University)26/09/2011, 16:00
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Jörgen Sjölin (Stockholm University)26/09/2011, 16:30
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Pavol Bartos (Comenius University)26/09/2011, 17:30
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Jordi Nadal Serrano (IFAE)26/09/2011, 18:00
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Joanne Cole (Brunel University)26/09/2011, 18:30
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Pyungwon Ko (Korea Institute for Advanced Study)27/09/2011, 09:00
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Andreas Jung (Fermilab)27/09/2011, 09:30
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Geraldine Servant (CERN)27/09/2011, 11:00
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Veronique Boisvert (Royal Holloway, University of London)27/09/2011, 11:40
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Lucia Masetti (Johannes Gutenberg Universität)27/09/2011, 12:20
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Bob Holdom (University of Toronto)27/09/2011, 15:00
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Un-Ki Yang (University of Manchester)27/09/2011, 15:30
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Erkcan Ozcan (Bogazici University (TR))27/09/2011, 16:00
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Cedric Delaunay (CERN)27/09/2011, 16:30
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Michael Spannowsky (University of Durham)27/09/2011, 18:00
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Victor Eduardo Bazterra (University of Illinois at Chicago)27/09/2011, 18:40
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Patrick Motylinski (University of Freiburg)28/09/2011, 09:00
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Cecilia Gerber (University of Illinois)28/09/2011, 09:40
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Wolfgang Wagner (Bergische Universität)28/09/2011, 10:20
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Mr Karolos Potamianos (Purdue University (US))28/09/2011, 11:30
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Michele Gallinaro (LIP)28/09/2011, 12:00
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Elizaveta Shabalina (University of Goettingen)28/09/2011, 12:30
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Stephen Parke (FNAL)29/09/2011, 09:00
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Christian Schwanenberger (Machester University)29/09/2011, 09:30
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Alexander Grohsjean (DESY)29/09/2011, 10:00
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Cecile Deterre (CEA-Irfu)29/09/2011, 11:00
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Nuno Filipe Castro (LIP Laboratorio de Instrumentacao e Fisica Experimental de Part)29/09/2011, 11:30
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Daniel Wicke (Bergische Universität)29/09/2011, 12:00
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Allison Renae Mc Carn (Univ. Illinois at Urbana-Champaign (US))29/09/2011, 12:30
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Ben Pecjak (Mainz University)29/09/2011, 15:00
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Amnon Harel (University of Rochester)29/09/2011, 15:40
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Thomas Peiffer (Inst. für Exp. Kernphysik)29/09/2011, 16:20
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Juan Antonio Aguilar-Saavedra (University of Granada)29/09/2011, 17:30
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Freya Blekman (Inter-University Institute for High Energies (BE))29/09/2011, 18:20
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Lian-Tao Wang (University of Chicago)29/09/2011, 18:50
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Sarah Allwood-Spiers (University of Glasgow)30/09/2011, 09:00
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Jure Zupan (U. of Cincinnati/U. of Ljubljana)30/09/2011, 09:30
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Yvonne Peters30/09/2011, 10:30
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Andrea Giammanco (Universite Catholique de Louvain)30/09/2011, 11:10
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Roberto Tenchini (INFN)30/09/2011, 11:50
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Dr Chaehyun Yu (KIAS)We present U(1) flavor models for leptophobic Z' with flavor dependent couplings to the right-handed up-type quarks in the Standard Model, which can accommodate the recent data on the top forward-backward (FB) asymmetry and the dijet resonance associated with a W boson reported by CDF Collaboration. Such flavor-dependent leptophobic charge assignments generally require extra chiral...Go to contribution page
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Michael Maes (Inter-University Institute for High Energies (BE))The measurement of the top quark pair cross section at the LHC is important for diverse reasons. The measurement on its own is a test of the Standard Model as well as a benchmark for the theoretical calculations. This poster describes the combined measurement of the tt ̄ cross section, using b-tagging, and the b-tagging efficiency using the muon+jets event topology observed by the CMS...Go to contribution page
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Mr arnaud Pin (Institut de Physique Nucleaire-Departement de Physique-Universi)In high energy collider physics, some topology cannot be fully reconstructed using the detector information only. Some techniques like kinematical fitting (KF) or matrix weighted template (MWT) have been developed to handle this difficulty. This is for instance the case for topologies arising from top quark pair production, when two leptons are present in the final state together with two...Go to contribution page
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66. Extraction of the Top Quark Mass from Top Pair Cross Sections Measured by CMS at sqrt(s) = 7 TeVMaria Aldaya Martin (Deutsches Elektronen-Synchrotron (DE))The top quark mass in the pole and MSbar definition is determined based on the measured cross section in the dilepton channel compared to three different approximate NNLO QCD calculations. The analysed dataset corresponds to an integrated luminosity of 1.14 fb-1 collected by the CMS experiment in 2011 in pp collisions at sqrt(s) of 7 TeV.Go to contribution page
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Petra Van Mulders (Vrije Universiteit Brussel)We present a search for fourth generation chiral quarks of the up- and down-type in 7 TeV proton collisions recorded by the CMS experiment at the LHC. Final state topologies with b' and t' quarks produced singly or in pairs are studied in the 2011 data corresponding to an integrated luminosity of 1.1 fb^{-1}. Degenerate masses are assumed for the fourth generation quarks. The inclusive...Go to contribution page
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Dr Thomas Hermanns (Hamburg University (DE))First normalized differential cross sections in top quark pair events are presented. All results are based on pp-collision data at a center-of-mass energy of 7 TeV recorded in 2011 by the CMS detector. The measurements are performed in the semileptonic and dileptonic decay modes of the top quark pair with events containing either one or two isolated leptons (electrons or muons), missing...Go to contribution page
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Maria Ilaria Besana (Torino)The measurement of the charge asymmetry in top quark pair production can be an important window on new physics, as in some Beyond Standard Model theories this asymmetry is significantly enhanced with respect to Standard Model prediction. The measurements performed by the ATLAS collaboration with pp collision data recorded in 2011 will be presented. The analysis has been performed in the...Go to contribution page
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Mr Stijn Blyweert (Vrije universiteit brussel)A measurement of the mass difference between the top quark and the antitop quark (∆mt = mt − mt ) is performed using events with a muon and at least four jets in the muon+jets final state. Data collected in 2011 with the CMS detector at the LHC and corresponding to an integrated luminosity of 1.09 fb−1 are analyzed. The measured value of ∆mt = −1.2 ± 1.2 (stat.) ± 0.5 (syst.) GeV is consistent...Go to contribution page
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Barbara Alvarez (Michigan State University)We present studies on the three single top production modes (s, t, Wt channels) carried out with 0.70/fb of integrated luminosity collected by the ATLAS detector during the 2011 LHC run. The t-channel production cross section is measured by two different techniques, a cut-based approach and a multivariate discriminant constructed with a neural network. The cut-based analysis combines 2- and...Go to contribution page
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Jacob Searcy (University of Oregon)We present a measurement of the tt production cross section with the ATLAS detector in proton-proton collisions at √s= 7 TeV, using events containing an isolated µ and a τ lepton decaying hadronically. The analysis utilizes a multivariate technique based on boosted decision trees to identify τ leptons. Backgrounds are measured using a method that combines charge subtraction and template...Go to contribution page
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Patrick Czodrowski (Technische Universitaet Dresden)Charged Higgs bosons are predicted by various theories beyond the Standard Model, which include e.g. an additional Higgs doublet. In the low-mass range, charged Higgs bosons can be produced in the decay of top quarks via t -> bH+, where H+ may then decay into c+sbar or tau+nu. We report on searches for a charged Higgs boson in ATLAS using the LHC data for both decay channels.Go to contribution page
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Pavol Federic (Bratislava University)We present a measurement of the electric charge of the top quark in the lepton+jets final states using 0.70/fb of data accumulated in the ATLAS experiment at a center of mass energy of 7 TeV. The top quark charge measurement is based on reconstructing the charges of the top quark decay products. While we determined the charge of the W boson through its leptonic decay, the b-quark charge is not...Go to contribution page
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Tae Jeong Kim (Korea University)
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Mr Ken Mimasu (University of Southampton)We study top-(anti)quark pair production at the Tevatron and Large Hadron Collider (LHC) in the context of the Minimal Length Scenario (MLS) of the Arkani-Hamed, Dimopoulos and Dvali (ADD) model of extra dimensions (XDs). We show that sizable effects onto both the integrated and differential cross section due to graviton mediation are expected for a String scale, M_S, of O(1-10TeV) and several...Go to contribution page
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Sinéad Walsh (Ghent University (BE))We present a measurement of the top quark pair production cross section using CMS data collected in 2011 at a center-of-mass energy of 7TeV. The cross section measurement is performed in the semi-leptonic final state with events containing one lepton, either a muon or an electron, missing transverse energy and jets. The measured cross section is compared with higher order QCD calculations.Go to contribution page
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