[PDF] Top 20 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
Has 10000 "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" found on our website. Below are the top 20 most common "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".
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
... effectively the computing infrastructure essential to our ...acknowledge the enduring support for the construction and operation of the LHC and the CMS detector provided by ... 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
... and the underlying event. The M AD G RAPH generator is also used to simulate the W+jets and Drell–Yan (DY) ...simulated using POWHEG . Inclusive production of the WZ and ... See full document
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Measurement of the $t\bar{t}$ production cross-section using $e\mu $ events with b-tagged jets in pp collisions at $\sqrt{s}$ = 7 and 8 $\,\mathrm{TeV}$ with the ATLAS detector
... W t single top and diboson backgrounds were esti- mated from simulation as discussed in ...3. The Z+jets background (with Z → τ τ → eµ4ν) at √ s = 8 TeV was es- timated ... See full document
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Measurement of $\mathrm {t}\overline{\mathrm {t}}$ production with additional jet activity, including $\mathrm {b}$ quark jets, in the dilepton decay channel using pp collisions at $\sqrt{s} =$ 8 TeV
... from the two neutrinos; the W boson invariant mass is fixed to ...and the top quark and antiquark masses are fixed to a value of ...pair of jets and lepton- jet combination ... 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
... In the standard model (SM), top quarks are produced in pp collisions predominantly via the strong interaction as tt pairs, with each top quark decaying almost exclusively ... 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
... simulated with PYTHIA and superimposed on the hard collisions using a pileup multiplicity distribution that reflects the luminosity profile of the an- alyzed ...data. ... See full document
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Cross section measurement of $t$-channel single top quark production in pp collisions at $\sqrt s =$ 13 TeV
... those with at least one primary vertex reconstructed from at least four tracks, with the longitudinal (radial) distance of less than 24 (2) cm from ... 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
... feature of the CMS apparatus is a superconducting solenoid of 6 m internal di- ameter and 13 m in length, providing a magnetic field of ...3.8 T. Within the ... See full document
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Measurement of the $ t\overline{t}\gamma $ production cross section in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
... The t¯tγ signal sample is modelled with MadGraph5_aMC@NLO ...hadronisation. The t¯tγ matrix element is generated at leading order (LO) in- cluding the decays ... 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 jet multiplicity distributions in $\mathrm {t}\overline{\mathrm {t}}$ production in pp collisions at $\sqrt{s} = 7\,\text {TeV} $
... feature of the CMS apparatus is a superconducting solenoid, 13 m in length and 6 m in diameter, which provides an axial magnetic field of ...3.8 T. The bore of ... See full document
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Measurements of the $\mathrm{t}\overline{\mathrm{t}}$ production cross section in lepton+jets final states in pp collisions at 8 $\,\text {TeV}$ and ratio of 8 to 7 $\,\text {TeV}$ cross sections
... of the jet-parton matching threshold on tt and W+jets events is studied by varying the thresh- old used for matching the matrix element level to the particles created in ... See full document
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Measurement of the cross section ratio $\sigma_\mathrm{t \bar{t} b \bar{b}} / \sigma_\mathrm{t \bar{t} jj }$ in pp collisions at $\sqrt{s}$ = 8 TeV
... (PDF+α S ) [10], where the uncertainty labelled “scale” refers to the uncertainty from the factorization and renormalization scales (µ F and µ R ), and the uncertainty labelled “PDF+α ... 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
... from the primary vertex, and must satisfy additional quality requirements, as described in ...[1, 5]. Lepton candidates are required to be isolated from other energy depositions in ... See full document
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Measurement of the semileptonic $ \mathrm{t}\overline{\mathrm{t}} $ + γ production cross section in pp collisions at $ \sqrt{s}=8 $ TeV
... measure the shape and normalization of this background component. The shape of the QCD multijet background is taken from a sideband region in ...data. The sideband region ... See full document
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Measurement of the $\mathrm{t}\overline{{\mathrm{t}}}$ production cross section in the all-jets final state in pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$
... shown in Fig. 8 are obtained from the detector-level measurement, after correcting for bin migration effects and extrapolating to the full phase space using a bin- by-bin acceptance ... See full document
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A search for new phenomena in pp collisions at $\sqrt{s} = 13\,\text {TeV} $ in final states with missing transverse momentum and at least one jet using the $\alpha _{\mathrm {T}}$ variable
... measures charged particles within the pseudorapidity range | η | < ...composed of a barrel and two endcap sections, extend over a range | η | < ...Outside the bore of 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
... colleagues in the CERN accelerator departments for the excellent perfor- mance 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 top quark mass with lepton+jets final states using $\mathrm {p}$ $\mathrm {p}$ collisions at $\sqrt{s}=13\,\text {TeV} $
... via t → bW, with one W boson decaying into a muon or electron and its neutrino, and the other into a quark-antiquark (qq 0 ) ...Hence, the minimal final state consists of ... See full document
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Measurement of the $t\bar{t}$ production cross section in the all-jet final state in pp collisions at $\sqrt{s}$ = 7 TeV
... collections of reconstructed particles are produced using a particle-flow (PF) algorithm [19, ...from the PF particles using the anti-k T jet algorithm [21], im- plemented ... See full document
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