[PDF] Top 20 Event shape variables measured using multijet final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV
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Event shape variables measured using multijet final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV
... Lebedev Physical Institute, Moscow, Russia 39: Also at California Institute of Technology, Pasadena, USA 40: Also at Budker Institute of Nuclear Physics, Novosibirsk, Russia 41: Also at [r] ... See full document
41
Measurement of the top quark polarization and $\mathrm{t\bar{t}}$ spin correlations using dilepton final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV
... predictions in the MADGRAPH5_aMC@NLO generator [71] , we instead use the known functional forms of ...amplitudes in the linear approximation are considered [4] ...listed in Table VIII , with a brief ... See full document
39
Search for new physics with dijet angular distributions in proton-proton collisions at $ \sqrt{s}=13 $ TeV
... possible at the LHC ...sought in multijet final states ...studied using dijet angular distributions [6–8]. Recent searches for QBH in dijet final states ... See full document
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Search for Evidence of the Type-III Seesaw Mechanism in Multilepton Final States in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
... efficiency for trilepton events is close to 100%. Events containing an opposite-sign same-flavor (OSSF) lepton pair with mass below 12 GeV are vetoed to reduce back- ground from low-mass resonances. We reject trilepton ... See full document
17
Pseudorapidity distribution of charged hadrons in proton-proton collisions at $\sqrt{s}$ = 13 TeV
... pairs in different layers at similar azimuthal angles φ, the tracklet method (using hit pairs) performs background subtraction based on control samples in data, while the track method ... See full document
28
Search for new physics in the multijet and missing transverse momentum final state in proton-proton collisions at $\sqrt{s}$= 8 TeV
... events in which the photon candidate orig- inates from the misidentification of jet fragments (background photons) is measured using a template method, which exploits the difference between the ... See full document
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Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV
... spikes in the ECAL are estimated from fits of the angular and timing distributions of the calorimeter ...clusters in the ECAL due to beam halo muons are observed to concentrate around φ ∼ 0 and π, while all ... See full document
36
Search for dark matter particles in proton-proton collisions at $ \sqrt{s}=8 $ TeV using the razor variables
... momentum at the primary interaction vertex as measured by the tracker, the energy of the corresponding ECAL cluster, and the energy sum of all bremsstrahlung photons (or emis- sions) spatially compatible ... See full document
46
Search for new phenomena with multiple charged leptons in proton–proton collisions at $\sqrt{s}= 13$ $\,\text {TeV}$
... model in final states with at least three charged leptons, in any combination of electrons or ...of proton-proton collisions at √ s = 13 ... See full document
42
Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... sured in gas-ionization detectors embedded in the steel flux-return yoke outside the ...uses in- formation from the calorimeters and muon detectors to select events of interest in a fixed time ... See full document
58
Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... significance using S= p ffiffiffiffi B as the metric within a mass window centered at the generated m ˜t , where S and B are the number of signal and background events, respectively, from ...QCD ... See full document
25
Search for leptoquarks coupled to third-generation quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... significant measured deviations from standard model predictions, the enhanced decay rate for B → D ðÞ τν, hints of lepton universality violation in B → K ðÞ ll decays, and the anomalous magnetic moment of ... See full document
19
Search for long-lived particles with displaced vertices in multijet events in proton-proton collisions at $\sqrt{s}= $13 TeV
... models in which there are two long-lived particles, this generator-level selection approximately replicates the reconstruction-level ...jets in the event, the displacements of the long-lived ... See full document
25
Search for natural and split supersymmetry in proton-proton collisions at $ \sqrt{s}=13 $ TeV in final states with jets and missing transverse momentum
... 13 TeV by the CMS Collaboration [24–29]. The data set analysed in this analysis is a factor of 16 larger than that presented in ...search in all-jet final states resulting ... See full document
49
Measurement of charged-particle event shape variables in $\sqrt{s}=7$ TeV proton-proton interactions with the ATLAS detector
... charged-particle event shape variables is presented in inclusive inelastic pp collisions at a center-of-mass energy of 7 TeV using the ATLAS detector at the ... See full document
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Study of hadronic event-shape variables in multijet final states in pp collisions at sqrt(s) = 7 TeV
... of event-shape variables in the transverse plane, where the energy flow can be mea- sured with small systematic ...of event-shape variables in ... See full document
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Searches for third-generation squark production in fully hadronic final states in proton-proton collisions at $ \sqrt{s} = 8$ TeV
... of event kinemat- ics or instrumental effects are expected to largely ...tested in data using two independent single-muon triggered samples containing exactly one b jet (expected to contain roughly ... See full document
61
Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at $ \sqrt{s}=13 $ TeV
... distributions in tt events are important for verifying current theo- retical models of tt production and ...events in many searches for physics beyond the standard model, for example in searches for ... See full document
56
Search for doubly charged Higgs boson production in multi-lepton final states with the ATLAS detector using proton–proton collisions at $\sqrt{s}=13\,\text {TeV}$
... J.T. Baines 133 , M. Bajic 39 , O.K. Baker 179 , P.J. Bakker 109 , E.M. Baldin 111,c , P. Balek 175 , F. Balli 138 , W.K. Balunas 124 , E. Banas 42 , A. Bandyopadhyay 23 , Sw. Banerjee 176,e , A.A.E. Bannoura 178 , L. ... See full document
52
Study of hadronic event-shape variables in multijet final states in pp collisions at root s=7 TeV
... crucial in order to correctly predict its ...described in MadGraph, where the multijet final-states are directly obtained from the hard ME calculations, unlike pythia and herwig++ ... See full document
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