19 research outputs found

    Search for single production of vector-like quarks decaying into Wb in pp collisions at s=8\sqrt{s} = 8 TeV with the ATLAS detector

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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 s=8TeV\sqrt{s}=8\,\mathrm TeV{} with the ATLAS detector

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    ATLAS Run 1 searches for direct pair production of third-generation squarks at the Large Hadron Collider

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    Measurements of top-quark pair differential cross-sections in the eμe\mu channel in pppp collisions at s=13\sqrt{s} = 13 TeV using the ATLAS detector

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    Measurement of the W boson polarisation in ttˉt\bar{t} events from pp collisions at s\sqrt{s} = 8 TeV in the lepton + jets channel with ATLAS

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    Measurement of the bbb\overline{b} dijet cross section in pp collisions at s=7\sqrt{s} = 7 TeV with the ATLAS detector

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    Search for dark matter in association with a Higgs boson decaying to bb-quarks in pppp collisions at s=13\sqrt s=13 TeV with the ATLAS detector

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    Charged-particle distributions at low transverse momentum in s=13\sqrt{s} = 13 TeV pppp interactions measured with the ATLAS detector at the LHC

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    Measurement of the W±ZW^{\pm}Z boson pair-production cross section in pppp collisions at s=13\sqrt{s}=13 TeV with the ATLAS Detector

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    The production of W±ZW^{\pm}Z events in proton--proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC. The collected data correspond to an integrated luminosity of 3.2 fb1^{-1}. The W±ZW^{\pm}Z candidates are reconstructed using leptonic decays of the gauge bosons into electrons or muons. The measured inclusive cross section in the detector fiducial region for leptonic decay modes is σW±Zνfid.=63.2±3.2\sigma_{W^\pm Z \rightarrow \ell^{'} \nu \ell \ell}^{\textrm{fid.}} = 63.2 \pm 3.2 (stat.) ±2.6\pm 2.6 (sys.) ±1.5\pm 1.5 (lumi.) fb. In comparison, the next-to-leading-order Standard Model prediction is 53.42.8+3.653.4^{+3.6}_{-2.8} fb. The extrapolation of the measurement from the fiducial to the total phase space yields σW±Ztot.=50.6±2.6\sigma_{W^{\pm}Z}^{\textrm{tot.}} = 50.6 \pm 2.6 (stat.) ±2.0\pm 2.0 (sys.) ±0.9\pm 0.9 (th.) ±1.2\pm 1.2 (lumi.) pb, in agreement with a recent next-to-next-to-leading-order calculation of 48.21.0+1.148.2^{+1.1}_{-1.0} pb. The cross section as a function of jet multiplicity is also measured, together with the charge-dependent W+ZW^+Z and WZW^-Z cross sections and their ratio
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