[PDF] Top 20 Measurement of the top quark mass using proton-proton data at root(s)=7
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Measurement of the top quark mass using proton-proton data at root(s)=7
... Zealand; the Pakistan Atomic Energy Commission; the Ministry of Science and Higher Education and the National Science Centre, Poland; the Fundação para a Ciência e a Tecnologia, ... See full document
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Search for associated production of a Higgs boson and a single top quark in proton-proton collisions at root s=13 TeV
... rations. Of particular interest among these are those with three or more charged leptons or with two leptons of the same electric charge, as they appear with comparatively low ...requiring the ... See full document
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Measurement of the top quark mass with lepton+jets final states using pp collisions at root s=13 TeV
... to the Run 1 result of m t = ...This measurement is consistent with the Run 1 result within the ...uncertainties. The previous measurement was calibrated with tt events ... See full document
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Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at root s=2.76 TeV
... are the pythia6 (version ...All of these tunes use the CTEQ6L1 [ 20 ] parton density function. The energy dependence of p T0 in these tunes is parameterised as pT0( √ s) = p REF T0 × ( ... See full document
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Measurement of the top-quark mass in all-jets tt events in pp collisions at root s=7 TeV
... decaying top-quark pairs lead to six quarks in the final state, events are selected with at least four jets with pT > 60 GeV, a fifth jet with p T > 50 GeV, and a sixth jet with pT > ... See full document
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Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at root s=13 TeV
... S. Abdullin, M. Albrow, M. Alyari, G. Apollinari, A. Apresyan, A. Apyan, S. Banerjee, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, G. Bolla † , K. Burkett, J.N. But- ler, A. Canepa, G.B. Cerati, H.W.K. Cheung, ... See full document
51
Measurement of charged pion, kaon, and proton production in proton-proton collisions at root s=13 TeV
... from the distribution of reconstructed interaction vertices. Since the bunches are very narrow in the plane transverse to the beam direction (with a width of about 50 μm for this ... See full document
25
Search for top quark partners with charge 5/3 in proton-proton collisions at root s=13 TeV
... Distributions of min[M(`, b)] in (upper) 0 or (lower) ≥1 W-tagged jets and (left) 1 or (right) ≥2 b-tagged jets categories with 0 t-tagged jets for combined electron and muon samples, at the final ... See full document
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Measurement of associated production of a W boson and a charm quark in proton-proton collisions at root s=13 Tev
... presented of associated pro- duction of a W boson and a charm quark (W + c) in proton– proton collisions at a center-of-mass energy of 13 ...TeV. The ... See full document
32
Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at root s=8 TeV
... for the interpretation of events under the assumption that they originate from semileptonic tt ...decays. The NN is trained with tt → 2b2q`ν simulated events, using both correct and ... See full document
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Measurement of the inelastic proton-proton cross section at $\sqrt{s}=7$ TeV
... performed using data collected in low-luminosity runs with an average of ...crossing. The events are collected using three triggers: (i) a coin- cidence trigger that requires the ... See full document
33
Measurements of spin correlation in top-antitop quark events from proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
... with the SM prediction. In the single-lepton channel, ∆φ between the charged lepton momentum direction and either the down-type jet from W boson de- cay, ∆φ(`, d), or the b-jet from ... See full document
33
Measurement Of The Double-differential Inclusive Jet Cross Section In Proton-proton Collisions At Root S=13tev
... A measurement of the double-differential inclu- sive jet cross section as a function of jet transverse momen- tum p T and absolute jet rapidity |y| is ...presented. The anal- ysis is ... See full document
27
Measurement of the production cross-section of a single top quark in association with a Z boson in proton–proton collisions at 13 TeV with the ATLAS detector
... R.F.H. Hunter 31 , P. Huo 150 , N. Huseynov 68,b , J. Huston 93 , J. Huth 59 , R. Hyneman 92 , G. Iacobucci 52 , G. Iakovidis 27 , I. Ibragimov 143 , L. Iconomidou-Fayard 119 , Z. Idrissi 137e , P. Iengo 32 , O. Igonkina ... See full document
35
Measurement of the top quark Yukawa coupling from t(t)over-bar kinematic distributions in the lepton plus jets final state in proton-proton collisions at root s=13 TeV
... invariant mass of the hypothesized b h and the jet from the W boson ...show the separation between correct and incorrect b assignments in the relevant variables for signal ... See full document
30
Measurement of the inclusive jet cross-section in proton-proton collisions at $ \sqrt{s}=7 $ TeV using 4.5 fb$^{−1}$ of data with the ATLAS detector
... uncertainty. The effect of this uncertainty in the cross-section measurements is evaluated by smearing the energy of reconstructed jets in the MC simulation such that the ... See full document
63
Search for new physics in top quark production in dilepton final states in proton-proton collisions at root s=13 TeV
... fragmentation of a bottom quark (“bjets”) are analyzed. The search is sensitive to new physics contributions to tW and t¯t production, and the six effective couplings, C G , C (3) φq , C tW , ... See full document
30
Observation of single top quark production in association with a Z boson in proton-proton collisions at root s=13 TeV
... both the predicted cross section and the detector acceptance for simulated events, which are treated ...in the cross section are not taken into consideration, and prior nuisance parameters are ... See full document
20
Search for direct production of supersymmetric partners of the top quark in the all-jets final state in proton-proton collisions at root s=13 TeV
... feature of the CMS apparatus is a superconducting solenoid of 6 m internal diameter, providing a magnetic field of ...Within the solenoid volume are an all-silicon pixel and strip ... See full document
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Search for low mass vector resonances decaying to quark-antiquark pairs in proton-proton collisions at root s=13 TeV
... combination of information from the various elements of the CMS ...detector. The energy of a photon is obtained directly from the ECAL measure- ment, corrected for losses ... See full document
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