[PDF] Top 20 Event shape variables measured using multijet final states in proton-proton collisions at root s=13 TeV
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Event shape variables measured using multijet final states in proton-proton collisions at root s=13 TeV
... colleagues in the CERN accelerator departments for the excellent per- formance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions ... See full document
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Search for black holes in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=$13 TeV
... physics in energetic, high-multiplicity final states has been performed using proton– proton collision data collected with the CMS detector at a center-of-mass energy of 13 ... 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
... sum in quadrature of statistical and systematic ...shown in the lower plots. The distributions are plotted in a logarithmic horizontal axis scale so that the details at small values of the ... See full document
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Search for new phenomena in monophoton final states in proton-proton collisions at root s=8 TeV
... vertices in the event (pileup), arising from the uncertainty in assigning the photon candidate to a particular ...tion variables is mitigated using the scheme presented in ...the ... See full document
24
Search for long-lived particles with displaced vertices in multijet events in proton-proton collisions at $\sqrt{s}= $13 TeV
... into multijet final states has been performed using proton-proton colli- sion events collected with the CMS detector at a center-of- mass energy of 13 TeV ... See full document
25
Search for new physics in top quark production in dilepton final states in proton-proton collisions at root s=13 TeV
... insignificant. At NLO QCD, tW pro- duction is expected to interfere with t¯t production ...signal in a way that distinguishes it from the t¯t production have been compared in the analysis: the ... See full document
30
Combination of searches for Higgs boson pair production in proton-proton collisions at root s=13 TeV
... sensitivity in the intermediate mass range, 0.7 – 1.2 TeV, is improved by considering both the final state with four b jets and the case with one Higgs jet candidate and two b jets [36] ...performed ... See full document
19
Search for new physics in the monophoton final state in proton-proton collisions at root s=13 TeV
... simulations at LO in QCD and with up to two additional partons in the final ...state. In addition to the selection efficiency correction factor ρ, these samples are weighted ... See full document
39
Search for Z$\gamma$ resonances using leptonic and hadronic final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... observed in data. The particle-flow (PF) event algorithm [53] aims to reconstruct and identify each individual particle in an event, based on an optimized combination of information from the ... See full document
40
Search for narrow H gamma resonances in proton-proton collisions at root s=13 TeV
... detected in gas- ionization chambers embedded in the steel flux-return yoke outside the ...selected using a two-tiered trigger system [43] ...events at a rate of around 100 kHz within a time ... See full document
19
Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV
... particle in an event with an optimized combination of information from the various elements of the CMS ...momentum at the primary interaction vertex as determined by the tracker, the energy of the ... See full document
47
Searches for third-generation squark production in fully hadronic final states in proton-proton collisions at root s=8 TeV
... evaluated using a control sample enriched in W(µν) +jets events as they have similar kinematic ...selected using an isolated muon trigger, the muon is required to have p T > 30 GeV and |η| < ... See full document
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Measurement of charged pion, kaon, and proton production in proton-proton collisions at root s=13 TeV
... history in high-energy particle, nuclear, and cosmic ray ...hadrons in high-energy hadron-hadron colli- sions are among the most basic physical ...hadronic event gener- ators, such as multiparton ... See full document
25
Search for leptophobic Z ' bosons decaying into four-lepton final states in proton-proton collisions at root s=8 TeV
... uncertainties in the background estimates and in the lepton selection efficien- ...uncertainty in the MC estimation of the main background cross section (ZZ and tt) arising from higher-order QCD ... See full document
23
Search for pair-produced three-jet resonances in proton-proton collisions at root s=13 TeV
... ated using data from the PF scouting and jets þ H T event ...mass in the four search regions are shown in ...shown in magenta, with the rate normalized to that expected from [33] ...the ... See full document
22
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
Search for Z gamma resonances using leptonic and hadronic final states in proton-proton collisions at root s=13 TeV
... detector at the LHC in ...investigated. In the leptonic channels, the Z boson candidates are reconstructed using electron or muon ...pairs. In the hadronic channels, they are identified ... See full document
44
Search for excited leptons in final states in proton-proton collisions at root s=13 TeV
... and event selection efficiency of signal events, simu- lated signal samples are generated with pythia ...5 TeV at intervals of 0.25 TeV up to 4 TeV and at intervals of ...0.5 ... See full document
38
Study of hadronic event-shape variables in multijet final states in pp collisions at root s=7 TeV
... Jets at generator level are defined as a collection of stable particles with the same kinematic criteria used for the real ...obtained using parton- and detector-level information differs because of the ... See full document
34
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
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