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[PDF] Top 20 Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $

Has 10000 "Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $" found on our website. Below are the top 20 most common "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} $

Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {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 institutes for their ... See full document

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Search for supersymmetry in events with one lepton and multiple jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for supersymmetry in events with one lepton and multiple jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... performed in events with a single electron or muon in proton-proton collisions at a center-of-mass energy of 13 ...experiment at the LHC and ... See full document

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Measurement of the double-differential inclusive jet cross section in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

Measurement of the double-differential inclusive jet cross section in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

... differ from the distributions at detector level by 5% to ...fluctuations of the measured spectra into correlated patterns among the neigh- bouring ...uncertainties of the unfolded ... 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

... momenta of all charged particles, UE charged-particles, and intrajet charged- particles, are plotted as a function of N ch in ...2–4. From Figs. 2 and 3, we see that mean ... 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

... support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and ... See full document

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Measurement of the top quark pair production cross section in proton-proton collisions at $\sqrt(s) =$ 13 TeV

Measurement of the top quark pair production cross section in proton-proton collisions at $\sqrt(s) =$ 13 TeV

... [55] of opposite charge, both of which are required to have p T > 20 GeV and jηj < ...region of jηj between the barrel and endcap sections of the ...isolated from nearby jet ... See full document

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Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at $ \sqrt{s}=8 $ TeV

Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at $ \sqrt{s}=8 $ TeV

... deposited in the isolation cone by charged particles not associated with the primary vertex, and ∑ p neutral T and ∑ p γ T are the scalar sums of the p T for neutral hadrons and photons, ...included ... See full document

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Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at $\sqrt{s} =$ 13 TeV

... GeV, in order to keep an equal amount of data in each of the mass ...chosen from five different families of ...the minimum number of parameters to fit the data with ... See full document

26

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

... Because of the large spatial separation, the contribution of the hadronic recoil is small in the transverse region, and becomes even smaller in the towards ...activity in the three ... See full document

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Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... production at very forward rapidities ( | η | > 5) in high energy hadronic collisions re- ceives contributions from multiparton interactions (MPI), initial- and final-state radiation ... See full document

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Search for heavy neutral leptons in events with three charged leptons in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for heavy neutral leptons in events with three charged leptons in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... cases of N masses below and above that of the W boson, two search regions are defined, referred to as the low- and high-mass ...regions. In the low-mass region (targeting m N < m W ), N is ... 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 TeV using ... See full document

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Search for narrow resonances in dilepton mass spectra in proton-proton collisions at $\sqrt{s}$ = 13 TeV and combination with 8 TeV data

Search for narrow resonances in dilepton mass spectra in proton-proton collisions at $\sqrt{s}$ = 13 TeV and combination with 8 TeV data

... feature of the CMS detector is a superconducting solenoid providing an axial magnetic field of ...composed of a silicon pixel detector and a silicon strip tracker, and measures ... 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 $\sqrt{s}=8\,\text {TeV}$

Measurement of electroweak production of two jets in association with a Z boson in proton-proton collisions at $\sqrt{s}=8\,\text {TeV}$

... information from the ECAL, HCAL and tracker are used by both algorithms in distinct ...resolution of calorimeter jets by incorporating additional tracking ...as in-cone or out-of-cone ... See full document

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Search for new physics in events with two soft oppositely charged leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for new physics in events with two soft oppositely charged leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... generator at leading order (LO) pre- cision in perturbative QCD using the MLM merging scheme [ 34 ...modelled in these ...generator at next-to-leading order (NLO) pre- cision using the FxFx ... See full document

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Measurement of pseudorapidity distributions of charged particles in proton-proton collisions at $\sqrt{s}$ = 8 TeV by the CMS and TOTEM experiments

Measurement of pseudorapidity distributions of charged particles in proton-proton collisions at $\sqrt{s}$ = 8 TeV by the CMS and TOTEM experiments

... collected in July 2012 during a dedicated run with low probability ( ∼ 4%) of overlapping pp interactions in the same bunch crossing (pileup) and a non-standard β ∗ = 90 m optics configuration, where ... See full document

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Measurement of differential cross sections for Z boson production in association with jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Measurement of differential cross sections for Z boson production in association with jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... The particle-flow (PF) algorithm [43] is used to reconstruct the ...mation from the various elements of the CMS detector to reconstruct and identify each particle in the ...sum ... 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

... sample of proton-proton collisions collected with the CMS detector ats = ...2.76 TeV during a dedicated run in March 2011, corresponding to an integrated ... See full document

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Measurement of charged pion, kaon, and proton production in proton-proton collisions at $\sqrt{s}=13$ TeV

Measurement of charged pion, kaon, and proton production in proton-proton collisions at $\sqrt{s}=13$ TeV

... distributions of reconstructed vertex pairs in data indicates that the fraction of merged vertices (with tracks from two or more true vertices) and split vertices (two or more reconstructed ... See full document

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Search for new physics in same-sign dilepton events in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

Search for new physics in same-sign dilepton events in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

... support from the Marie-Curie programme and the European Re- search Council and EPLANET (European Union); the Leventis Foundation; the ...Policy Of- fice; the Fonds pour la Formation `a la Recherche dans ... See full document

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