[PDF] Top 20 Measurement of the charge asymmetry in highly boosted top-quark pair production in $\sqrt{s} =$ 8 TeV $pp$ collision data collected by the ATLAS experiment
Has 10000 "Measurement of the charge asymmetry in highly boosted top-quark pair production in $\sqrt{s} =$ 8 TeV $pp$ collision data collected by the ATLAS experiment" found on our website. Below are the top 20 most common "Measurement of the charge asymmetry in highly boosted top-quark pair production in $\sqrt{s} =$ 8 TeV $pp$ collision data collected by the ATLAS experiment".
Measurement of the charge asymmetry in highly boosted top-quark pair production in $\sqrt{s} =$ 8 TeV $pp$ collision data collected by the ATLAS experiment
... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azer- baijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, ... See full document
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Measurement of the top quark charge in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector
... for the top quark charge measurement in the lepton + jets channel are: W + jets production (the most significant background), Z+ jets, multi-jet, diboson and ... See full document
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Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector
... = 8 TeV. The dileptonic channel is characterized by two charged leptons (denoted ` = e, µ), coming from either a direct vector boson decay or through an intermediate τ lepton ...on the ... See full document
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Measurement of lepton differential distributions and the top quark mass in $t\bar{t}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
... set of 1000 pseudo-experiments was performed using the baseline simulation sample as a reference, and the mean and RMS width of the deviations of the result in each ... See full document
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Measurement of jet shapes in top-quark pair events at $\sqrt{s}$ = 7 TeV using the ATLAS detector
... samples of events are selected: a dilepton sample, where both W bosons decay to leptons (e, µ, including leptonic τ decays), and a single-lepton sample, where one W boson decays to leptons and the other to ... See full document
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Measurements of charge and CP asymmetries in $b$-hadron decays using top-quark events collected by the ATLAS detector in $pp$ collisions at $\sqrt{s}=8$ TeV
... The charge asymmetries, A ss and A os , are expressed as ratios of probabilities as this ensures that the meas- urements are independent of any asymmetry that could lead to a ... See full document
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Measurement of the electron charge asymmetry in inclusive $W$ production in $pp$ collisions at $\sqrt{s}=7$ TeV
... τν production (electroweak or EW backgrounds), as well as top-quark pair (tt) ...some of the background contributions. The signal and the EW backgrounds are ... See full document
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Measurement of top quark-antiquark pair production in association with a W or Z boson in pp collisions at $\sqrt{s} = 8$ $\,\text {TeV}$
... existence of non-zero couplings between the top quark and the neutral vector bosons can be inferred through the analysis of direct production of tt pairs ... See full document
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Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with ATLAS
... more of the reconstructed lepton candidates are nonprompt or misiden- tified (referred to as “fake leptons”) arise from t¯t production, W +jets production, and single-top produc- tion ... See full document
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Search for flavour-changing neutral current top-quark decays to $qZ$ in $pp$ collision data collected with the ATLAS detector at $\sqrt s =8$ TeV
... on the measurement of the efficiencies of real and fake loose leptons to pass the nominal selection, R and F , and on the selection of two orthogonal sets ... See full document
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A search for flavour changing neutral currents in top-quark decays in $pp$ collision data collected with the ATLAS detector at $\sqrt{s}=7$ TeV
... selection of leptons, jets, and E T miss was close to that used for the ATLAS measurement of the t¯ t production cross section in the dilepton channel ... See full document
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Measurement of the top quark pair production charge asymmetry in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector
... W charge asymmetry depends also on the W +jets flavour composition, ...on the mixture of W bb+jets, W cc+jets, W c+jets and W +light–jets processes in ALPGEN simulated ... See full document
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Measurement of the charge asymmetry in top quark pair production in pp collisions at $\sqrt(s) =$ 8 TeV using a template method
... combination of information from the various elements of the CMS ...clusters in ECAL with a requirement that there be a charged-particle trajectory pointing to an electron ...cluster. ... See full document
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Measurement of the charge asymmetry in top-quark pair production in the lepton-plus-jets final state in pp collision data at $\sqrt{s}=8\,\mathrm TeV{}$ with the ATLAS detector
... investigate the impact of uncertainties on the t¯t signal modelling, additional samples generated with Powheg-Box interfaced to Herwig, Mc@nlo interfaced to Herwig and AcerMC interfaced to Pythia are ... See full document
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Measurement of the charge asymmetry in top quark pair production in $pp$ collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
... Reconstructing top quark pair events is facilitated by the ability to tag jets from the hadronisation of b- ...exploits the topol- ogy of b- and c-hadron ... See full document
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Measurement of jet charge in dijet events from $\sqrt{s}$=8 TeV pp collisions with the ATLAS detector
... to the large event rate, not every collision can be recorded for processing ...at the first level and software based for the two following ...stage of the trigger, energy ... See full document
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Measurement of the forward-backward asymmetry of electron and muon pair-production in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector
... ∗ production is detected by the emission of charged lepton pairs, ee or ...µµ. The contribution from Z/γ ∗ → ττ followed by τ decays to electrons or muons is considered as ... See full document
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Measurement of the mass difference between top quark and antiquark in pp collisions at $\sqrt{s} = 8$ TeV
... Roeck, S. De Visscher, S. Di Guida, M. Dobson, N. Dupont, A. Elliott-Peisert, J. Eugster, G. Franzoni, W. Funk, M. Giffels, D. Gigi, K. Gill, D. Giordano, M. Girone, M. Giunta, F. Glege, R. Gomez-Reino ... See full document
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Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment
... P. Rados 102 , F. Ragusa 66a,66b , G. Rahal 95 , J.A. Raine 52 , S. Rajagopalan 29 , A. Ramirez Morales 90 , T. Rashid 128 , S. Raspopov 5 , M.G. Ratti 66a,66b , D.M. Rauch 44 , F. Rauscher 112 , S. ... See full document
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Measurement of the differential cross sections for top quark pair production as a function of kinematic event variables in pp collisions at $\sqrt s$=7 and 8 TeV
... R. Granier de Cassagnac, 29 S. Lisniak, 29 L. Mastrolorenzo, 29 P. Miné, 29 I. N. Naranjo, 29 M. Nguyen, 29 C. Ochando, 29 G. Ortona, 29 P. Paganini, 29 P. Pigard, 29 S. Regnard, 29 R. Salerno, 29 J. B. ... See full document
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