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[PDF] Top 20 Measurement of the average very forward energy as a function of the track multiplicity at central pseudorapidities in proton-proton collisions at root s=13 TeV

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Measurement of the average very forward energy as a function of the track multiplicity at central pseudorapidities in proton-proton collisions at root s=13 TeV

Measurement of the average very forward energy as a function of the track multiplicity at central pseudorapidities in proton-proton collisions at root s=13 TeV

... for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success ... See full document

24

Measurement of associated production of a W boson and a charm quark in proton-proton collisions at root s=13 Tev

Measurement of associated production of a W boson and a charm quark in proton-proton collisions at root s=13 Tev

... by the ATLAS experiment ats = 7 TeV [ 12 ] and used in a QCD analysis, which supported the enhanced strange quark content in the proton suggested by ... See full document

32

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

24

Search for excited leptons in final states in proton-proton collisions at root s=13 TeV

Search for excited leptons in final states in proton-proton collisions at root s=13 TeV

... purity in physics object reconstruction and identification. The particle- flow algorithm aims to reconstruct and identify individual particles in an event using an optimized combination of ... See full document

38

Measurement of four-jet production in proton-proton collisions at root s=7 TeV

Measurement of four-jet production in proton-proton collisions at root s=7 TeV

... account the extra energy clustered in jets due to additional proton-proton interactions within the same beam crossing ...additional collisions during the ... See full document

20

Inclusive photon production at forward rapidities in proton-proton collisions at root s=0.9, 2.76 and 7 TeV

Inclusive photon production at forward rapidities in proton-proton collisions at root s=0.9, 2.76 and 7 TeV

... discussed in Sec. 3. At lower center of mass energies of ...0.9 TeV, the aver- age photon multiplicities for NSD events have been mea- sured by the UA5 experiment [ 32 ] ... See full document

18

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

... The central barrel detectors are located inside a large solenoidal magnet, which provides a magnetic field of ...along the beam direction (z axis in the ALICE reference ...using ... See full document

47

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

... pp collisions occur (beam spot) is measured from the distribution of reconstructed interaction ...Since the bunches are very narrow in the plane transverse to the ... See full document

25

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

... The central detectors of CMS are complemented by calorimeters in the forward direction, which all rely on the detection of Cherenkov photons produced when charged ... See full document

30

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

... production in high-energy proton-proton (pp) collisions originates from multiple scatterings of the partonic constituents of the protons at ... See full document

34

Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at root s=13 TeV

Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at root s=13 TeV

... D. Abercrombie, B. Allen, A. Apyan, V. Azzolini, R. Barbieri, A. Baty, R. Bi, K. Bier- wagen, S. Brandt, W. Busza, I.A. Cali, M. D’Alfonso, Z. Demiragli, G. Gomez Ceballos, M. Goncharov, D. Hsu, Y. Iiyama, G.M. ... See full document

32

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

... and energy quantification for comparisons to the model ...predictions. The corrections are applied explic- itly for each range in ...smearing in pseudorapidity; it is basically ... See full document

25

Measurement of four-jet production in proton-proton collisions at $\sqrt{s}=7$  TeV

Measurement of four-jet production in proton-proton collisions at $\sqrt{s}=7$  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

31

Measurement of associated Z + charm production in proton-proton collisions at root s=8TeV

Measurement of associated Z + charm production in proton-proton collisions at root s=8TeV

... candidates in the D ± mode are selected by look- ing for secondary vertices made of three tracks and with a reconstructed invariant mass consistent with the D ± mass: 1869 ...]. The sum ... See full document

35

Search for the Higgs boson decaying to two muons in proton-proton collisions at root s=13 TeV

Search for the Higgs boson decaying to two muons in proton-proton collisions at root s=13 TeV

... colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS ... See full document

19

Evidence for the associated production of a single top quark and a photon in proton-proton collisions at root s=13 TeV

Evidence for the associated production of a single top quark and a photon in proton-proton collisions at root s=13 TeV

... T. Williams, 131 W. J. Womersley, 131 R. Bainbridge, 132 P. Bloch, 132 J. Borg, 132 S. Breeze, 132 O. Buchmuller, 132 A. Bundock, 132 D. Colling, 132 P. Dauncey, 132 G. Davies, 132 M. Della Negra, 132 R. Di Maria, ... See full document

19

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} $

... Predictions of perturbative quantum chromodynamics at next-to-leading order pre- cision, complemented with electroweak and nonperturbative corrections, are used to compute the absolute scale and ... See full document

36

Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at root s=13 TeV

Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at root s=13 TeV

... Per-photon energy resolution estimate: this uncertainty is parameterized conserva- tively as a rescaling of the resolution by ±5% about its nominal value, to cover all differences between data and ... See full document

61

Measurement of jet substructure observables in t(t)over-bar events from proton-proton collisions at root s=13 TeV

Measurement of jet substructure observables in t(t)over-bar events from proton-proton collisions at root s=13 TeV

... model of parton shower, hadronization, MPI, and CR. The b fragmentation function is varied to cover e þ e − data at the Z pole [10,15,91,92] with the Bowler-Lund [50] and ... See full document

37

Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at root s=13 TeV

Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at root s=13 TeV

... from the Marie-Curie programme and the European Research Council and Horizon 2020 Grant, contract ...Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von ... See full document

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