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[PDF] Top 20 Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at root s=2.76 TeV

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Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at root s=2.76 TeV

Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at root s=2.76 TeV

... composed of a barrel and two endcap sections. The silicon tracker measures charged particles within the pseudorapidity range |η| < ...particles of 1 < p T < 10 GeV and |η| < ... See full document

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Measurement of the underlying event in the Drell-Yan process in proton-proton collisions at $\sqrt{s}=7$ TeV

Measurement of the underlying event in the Drell-Yan process in proton-proton collisions at $\sqrt{s}=7$ TeV

... presents the ratios of the predictions of various MC models to the measurements for the observables shown in ...Fig. 2. Statistical fluctuations in ... See full document

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Measurement of charm and beauty production at central rapidity versus charged-particle multiplicity in proton-proton collisions at root s=7 TeV

Measurement of charm and beauty production at central rapidity versus charged-particle multiplicity in proton-proton collisions at root s=7 TeV

... field of 0.5 T along the beam direction (z axis in the ALICE reference ...and particle identification are performed using the information provided by the Inner ... See full document

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Measurement of the energy density as a function of pseudorapidity in proton-proton collisions at root s=13 TeV

Measurement of the energy density as a function of pseudorapidity in proton-proton collisions at root s=13 TeV

... to the model predictions. The corrections are applied explic- itly for each range in ...smearing in pseudorapidity; it is basically the characteristic response of the ... See full document

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Measurement of charged-particle distributions sensitive to the underlying event in $ \sqrt{s}=13 $ TeV proton-proton collisions with the ATLAS detector at the LHC

Measurement of charged-particle distributions sensitive to the underlying event in $ \sqrt{s}=13 $ TeV proton-proton collisions with the ATLAS detector at the LHC

... observables the models describe the underlying-event data to better than 5% ...level of variation is far greater than the experimental uncertainty of the ... See full document

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Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... feature of the CMS apparatus is a superconducting solenoid of 6 m internal diam- ...Within the solenoid volume are a silicon pixel and strip tracker, a lead tungstate crystal electromagnetic ... See full document

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Measurement of electroweak production of two jets in association with a Z boson in proton-proton collisions at root s=8 TeV

Measurement of electroweak production of two jets in association with a Z boson in proton-proton collisions at root s=8 TeV

... define jets. The information from the ECAL, HCAL and tracker are used by both algorithms in distinct ...ways. The JPT algorithm improves the energy response and reso- lution ... See full document

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Study of double parton scattering using W+2-jet events in proton-proton collisions at root s=7 TeV

Study of double parton scattering using W+2-jet events in proton-proton collisions at root s=7 TeV

... • the signal template is generated by randomly mixing W + 0-jet and dijet events from simulated ...events. The systematic uncertainty in the signal template is calculated by using ... See full document

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Measurement of pion, kaon and proton production in proton-proton collisions at root s=7 TeV

Measurement of pion, kaon and proton production in proton-proton collisions at root s=7 TeV

... comparing the dE/dx measurement provided by the ITS detector with the expected values at a given momentum p under the corresponding mass ...hypotheses. In Fig. 1 , ... See full document

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Search for excited leptons in proton-proton collisions at root s=8 TeV

Search for excited leptons in proton-proton collisions at root s=8 TeV

... to the eeγ candidate sample. The largest contributions come from processes such as W( → eν)+jet+γ where the jet in the event is misidentified as an ...a charged ... See full document

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Charged jet cross sections and properties in proton-proton collisions at root s=7 TeV

Charged jet cross sections and properties in proton-proton collisions at root s=7 TeV

... indicating the suppression of low momentum particle production by QCD coherence [47,48] ...momentum, the area of the distributions increases, showing the rise of ... See full document

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Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $

Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $

... resent the conditional probability that (for a given observable) a true value i is measured as a value ...j. In this analysis, two different correction procedures were ...implemented. The first ... See full document

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Measurement of charged-particle event shape variables in $\sqrt{s}=7$ TeV proton-proton interactions with the ATLAS detector

Measurement of charged-particle event shape variables in $\sqrt{s}=7$ TeV proton-proton interactions with the ATLAS detector

... The measurement of charged-particle event shape variables is presented in inclusive inelastic pp collisions at a center-of-mass energy of 7 ... See full document

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Event shape variables measured using multijet final states in proton-proton collisions at root s=13 TeV

Event shape variables measured using multijet final states in proton-proton collisions at root s=13 TeV

... tion of an ESV is unfolded with the different response matrices incorporating the un- certainty due to ...JER. The estimated uncertainties in the ESVs are of the ... See full document

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Charged-particle multiplicities in proton-proton collisions at root s=0.9 to 8 TeV

Charged-particle multiplicities in proton-proton collisions at root s=0.9 to 8 TeV

... sources of event background are beam gas and beam halo ...that the timing signals from the V0 hodoscopes, if present, be compatible with the arrival time of particles produced ... See full document

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Measurement of neutral strange particle production in the underlying event in proton-proton collisions at sqrt(s) = 7 TeV

Measurement of neutral strange particle production in the underlying event in proton-proton collisions at sqrt(s) = 7 TeV

... feature of CMS is a superconducting solenoid of 6 m internal ...Within the superconducting solenoid volume are a silicon pixel and strip tracker, a lead tungstate crystal electromagnetic calorimeter, ... See full document

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Jet and underlying event properties as a function of charged-particle multiplicity in proton–proton collisions at $\sqrt{s}$ = 7 TeV

Jet and underlying event properties as a function of charged-particle multiplicity in proton–proton collisions at $\sqrt{s}$ = 7 TeV

... understanding of the details of multi-particle production in hadronic collisions remains an open problem in high-energy particle ...physics. In ... See full document

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Measurement of the differential Drell-Yan cross section in proton-proton collisions at √s = 13 TeV

Measurement of the differential Drell-Yan cross section in proton-proton collisions at √s = 13 TeV

... simulate the DY signal and background processes. The MadGraph5 amc@nlo ...] event generator is used to simulate the signal and W production in association with one or more jets ... See full document

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Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at sqrt(s) = 2.76 TeV

Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at sqrt(s) = 2.76 TeV

... from the Marie-Curie programme and the European Re- search Council and EPLANET (European Union); the Leventis Foundation; the ...Foundation; the Alexander von Humboldt Foundation; ... See full document

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Measurement of charged pion, kaon, and proton production in proton-proton collisions at root s=13 TeV

Measurement of charged pion, kaon, and proton production in proton-proton collisions at root s=13 TeV

... (Fig. 2 ). Conversely, at high momenta (above about ...protons) the ε bands overlap. Therefore the particle yields need to be determined by means of a series of template ... See full document

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