[PDF] Top 20 Measurement of the t(t)over-bar production cross section in pp collisions at root s=8 TeV in dilepton final states containing one tau lepton
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Measurement of the t(t)over-bar production cross section in pp collisions at root s=8 TeV in dilepton final states containing one tau lepton
... colleagues in the CERN accelerator depart- ments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS ... See full document
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Measurement of the $t\bar{t}$ production cross section in the $\tau$ + jets final state in $pp$ collisions at $\sqrt{s}=8$ TeV using the ATLAS detector
... component of the Large Hadron Collider (LHC) [1] physics program is the measurement of the properties of the top quark, which is the most massive fundamental ... See full document
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Measurement of the $t\bar{t}$ production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV with lepton + jets final states
... M. Aldaya Martin, J. Behr, W. Behrenhoff, U. Behrens, M. Bergholz 16 , A. Bethani, K. Borras, A. Burgmeier, A. Cakir, L. Calligaris, A. Campbell, E. Castro, F. Costanza, D. Dammann, C. Diez Pardos, G. Eckerlin, D. ... See full document
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Measurement of the WZ production cross section in pp collisions at root s=7 and 8 TeV and search for anomalous triple gauge couplings at root s=8 TeV
... other final-state particles in the event. Con- sequently, the selected leptons are required to be isolated from other activity in the event to reduce the backgrounds from ... See full document
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Measurement of the $t\bar{t}$ production cross section in the dilepton channel in $pp$ collisions at $\sqrt{s}=7$ TeV
... when the τ leptons decay into ` ν ` ν τ (` = e or µ) states. A cross-section measurement based on τ leptons that de- cay into hadrons and a neutrino can be found in ...[15]. ... See full document
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Measurement Of The T(t)over-bar Production Cross Section Using Events In The E Mu Final State In Pp Collisions At Root S=13 Tev
... into lepton-antilepton pairs through a virtual pho- ton or a Z boson exchange; for these backgrounds the event yields are estimated from ...and the event yields are normalized to the ... See full document
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Measurement of the $t \bar t$ production cross section using events with one lepton and at least one jet in pp collisions at $\sqrt{s}$ = 13 TeV
... simulation in the tt phase-space region. The contribution from the multijet background is estimated using an independent data control sample where the prompt-lepton candidate ... See full document
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Measurement of the semileptonic t(t)over-bar plus gamma production cross section in pp collisions at root s=8 TeV
... reduce the statistical fluctuations in the background template, the selection requirement of the photon charged-hadron isolation being less than 5 GeV is relaxed during ... See full document
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Measurement of the top quark pair production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV in dilepton final states with ATLAS
... R.J. Madaras 14 , W.F. Mader 43 , R. Maenner 58c , T. Maeno 24 , P. M¨ attig 174 , S. M¨ attig 41 , P.J. Magalhaes Martins 124a,h , L. Magnoni 29 , E. Magradze 54 , Y. Mahalalel 153 , K. Mahboubi 48 , G. Mahout 17 ... See full document
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Measurement of the Z/gamma* -gt; tau tau cross section in pp collisions at root s=13 TeV and validation of tau lepton analysis techniques
... and the Z/γ ∗ → ee, Z/γ ∗ → μμ, W+jets, tt, single top quark, and diboson (WW, WZ, and ZZ) background processes are modelled through sam- ples of MC simulated ...multijet production via quantum ... See full document
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Measurement of the t(t)over-bar production cross section using events with one lepton and at least one jet in pp collisions at root s=13 TeV
... (Republic of Korea); LAS (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MBIE (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Dubna); ... See full document
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Measurement of the tt̄ production cross section in pp̄ collisions at √s = 1.96 TeV in dilepton final states
... electrons in a control sam- ple dominated by fake electrons. In the e + e − channel the control sample consists of events that satisfied the trigger and have two loose ... See full document
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Measurement of the $t \bar t$ production cross section in $pp$ collisions at $\sqrt s = 8$ TeV in dilepton final states containing one $\tau$ lepton
... by the following funding agencies: BMWFW and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES and CSF ... See full document
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Measurement of the top quark pair production cross section in $pp$ collisions at $\sqrt{s} = 7$ TeV in dilepton final states containing a $\tau$
... D. Abbaneo, E. Auffray, G. Auzinger, P. Baillon, A.H. Ball, D. Barney, C. Bernet 5 , G. Bianchi, P. Bloch, A. Bocci, A. Bonato, H. Breuker, K. Bunkowski, T. Camporesi, G. Cerminara, T. Christiansen, J.A. Coarasa Perez, ... See full document
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Measurement of the top-quark mass in $t\bar{t}$ events with dilepton final states in $pp$ collisions at $\sqrt{s}=7$ TeV
... where the total inelastic cross section used to simulate the pileup is varied within its uncertainty, which is estimated to be ...8%. The uncertainties related to the ... See full document
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Measurement Of The T(t)over-bar Production Cross Section In The E Mu Channel In Proton-proton Collisions At Root S=7 And 8 Tev
... new measurement of σ tt in pp collisions at centre-of-mass ener- gies of 7 and 8 ...TeV. The measurement is performed in ... See full document
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Measurement of the $t \bar{t}$ production cross section in the dilepton channel in pp collisions at $\sqrt{s}$ = 8 TeV
... decays of mesons or heavy-flavour quarks, jet misidentifi- cation, photon conversions, or finite resolution detector effects whereas prompt leptons usually originate from decays of W or Z bosons and are ... See full document
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Measurement of the $pp \to ZZ$ production cross section and constraints on anomalous triple gauge couplings in four-lepton final states at $\sqrt s=$8 TeV
... study of diboson production in proton-proton collisions provides an important test of the electroweak sector of the standard model (SM), especially the ... See full document
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Measurement of the inclusive $ \mathrm{t}\overline{\mathrm{t}} $ cross section in pp collisions at $ \sqrt{s}=5.02 $ TeV using final states with at least one charged lepton
... In the ` +jets analysis, the tt cross section is measured in a fiducial phase space by means of a ...for the fit, which are sensitive to the reso- nant ... See full document
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Measurements of $t \bar t$ charge asymmetry using dilepton final states in pp collisions at $\sqrt s=8$ TeV
... used in Ref. [25] and is only briefly described in this ...section. The particle-flow (PF) method [26, 27] is used to reconstruct final- state ...[29]) of opposite electric ... See full document
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