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[PDF] Top 20 Measurement of charged jet cross section in pp collisions at root s=5.02 TeV

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Measurement of charged jet cross section in pp collisions at root s=5.02 TeV

Measurement of charged jet cross section in pp collisions at root s=5.02 TeV

... Council of Norway, Norway; the Commission on Science and Technology for Sustainable Development in the South (COMSATS), Pakistan; Pontificia Universidad Católica del Perú, Peru; the Ministry of ... See full document

23

Measurement of the semileptonic t(t)over-bar plus gamma production cross section in pp collisions at root s=8 TeV

Measurement of the semileptonic t(t)over-bar plus gamma production cross section in pp collisions at root s=8 TeV

... Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Council of Science and Industrial Research, India; the HOMING PLUS programme of the Foundation for Polish Science, ... See full document

43

Measurement of the differential cross section for top quark pair production in pp collisions at root s=8TeV

Measurement of the differential cross section for top quark pair production in pp collisions at root s=8TeV

... feature of the CMS apparatus is a superconduct- ing solenoid of 13 m length and 6 m inner diameter, which provides an axial magnetic field of ...composed of a barrel and two endcap sections. ... See full document

40

Measurement Of Dijet Azimuthal Decorrelation In Pp Collisions At Root S=8 Tev

Measurement Of Dijet Azimuthal Decorrelation In Pp Collisions At Root S=8 Tev

... description of the CMS detector, together with a definition of the coordinate system used and the relevant kinematic variables, can be found in ...[ 5 ]. The central feature of the CMS ... See full document

23

Measurement of the WZ production cross section in pp collisions at root s=7 and 8 TeV and search for anomalous triple gauge couplings at root s=8 TeV

Measurement of the WZ production cross section in pp collisions at root s=7 and 8 TeV and search for anomalous triple gauge couplings at root s=8 TeV

... feature of the CMS apparatus is a supercon- ducting solenoid of 6 m internal diameter, providing a mag- netic field of ...composed of a barrel and two endcap sections. Muons are measured ... See full document

30

Measurement of the Production Cross Section for Pairs of Isolated Photons in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the Production Cross Section for Pairs of Isolated Photons in $pp$ collisions at $\sqrt{s}=7$ TeV

... collisions in the same bunch crossing) and underlying-event activity (multiple parton interac- tion and beam remnants from the same proton-proton ...independent of ϕ, the ECAL isolation probability ... See full document

37

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

... Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum p T and ... See full document

20

Measurement of the production cross section for a W boson and two b jets in pp collisions at root s=7 TeV

Measurement of the production cross section for a W boson and two b jets in pp collisions at root s=7 TeV

... mass of b hadrons to provide optimized b-quark jet ...and jet kinematic proper- ties in a likelihood-ratio ...efficiency of approximately 50% for identifying jets containing b-flavored ... See full document

23

Measurement Of The Double-differential Inclusive Jet Cross Section In Proton-proton Collisions At Root S=13tev

Measurement Of The Double-differential Inclusive Jet Cross Section In Proton-proton Collisions At Root S=13tev

... feature of the CMS apparatus is a supercon- ducting solenoid of 6 m internal diameter, providing a mag- netic field of ...composed of a barrel and two end- cap ...measured in gas- ... See full document

27

Search for a charged Higgs boson in pp collisions at root S=8 TeV

Search for a charged Higgs boson in pp collisions at root S=8 TeV

... mass of approximately 125 GeV was discovered by the CMS and ATLAS experiments [ 1 – 3 ] at the CERN ...properties of the new boson are con- sistent with those predicted for the standard model (SM) ... See full document

65

Measurement of the top quark mass using charged particles in pp collisions at root s=8 TeV

Measurement of the top quark mass using charged particles in pp collisions at root s=8 TeV

... mismodeling of the overall kin- ematic properties of the event are canceled, to first approximation, by studying the ratio of the two momenta, in which the secondary vertex serves as a proxy ... See full document

30

Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

... clusters of energy deposited in the EM calorimeter and classified [ 30 ] as uncon- verted photons (candidates without a matching track or matching reconstructed conversion vertex in the inner ... See full document

25

Measurement of the isolated photon cross section in p(p)over-bar collisions at root s=1.96 TeV

Measurement of the isolated photon cross section in p(p)over-bar collisions at root s=1.96 TeV

... clusters of calorimeter cells within a cone of radius R =  (η) 2 + (φ) 2 = ...energy in the EM calorimeter layers (> 95%), and the probability to have a matched track was less than ...energy ... See full document

8

Measurement of the t(t)over-bar production cross section using events with one lepton and at least one jet in pp collisions at root s=13 TeV

Measurement of the t(t)over-bar production cross section using events with one lepton and at least one jet in pp collisions at root s=13 TeV

... scales of the objects used in the analysis (leptons and jets) are varied ac- cording to their estimated ...migration of events to different categories because of the thresholds applied ... See full document

41

Measurement of the single-top-quark $t$-channel cross section in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the single-top-quark $t$-channel cross section in $pp$ collisions at $\sqrt{s}=7$ TeV

... described in detail elsewhere [9], and the key components for this anal- ysis are listed ...feature of the CMS detector is a superconducting solenoidal magnet with a length of 13 m and a diameter ... See full document

41

Cross section measurement of $t$-channel single top quark production in pp collisions at $\sqrt s =$ 13 TeV

Cross section measurement of $t$-channel single top quark production in pp collisions at $\sqrt s =$ 13 TeV

... with at least one primary vertex reconstructed from at least four tracks, with the longitudinal (radial) distance of less than 24 (2) cm from the centre of the detector, are con- sidered for ... See full document

25

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} $

... combination of information from the various elements of the CMS ...energy of photons is directly obtained from the ECAL ...energy of elec- trons is determined from a combination of the ... See full document

36

Determination of the strong coupling constant from the inclusive jet cross section in pp collisions at s=1.96 TeV

Determination of the strong coupling constant from the inclusive jet cross section in pp collisions at s=1.96 TeV

... inclusive jet data under study is included in the MSTW2008 PDF ...correlation of experi- mental and PDF uncertainties is not documented, it cannot be taken into account when using the PDFs to extract ... See full document

7

Measurement of diffraction dissociation cross sections in pp collisions at $\sqrt{s}$ = 7 TeV

Measurement of diffraction dissociation cross sections in pp collisions at $\sqrt{s}$ = 7 TeV

... organized in eleven sections and two appendices. The CMS detector is described in Section ...2. Section 3 presents the Monte Carlo (MC) simulations used in the ...the cross ... See full document

49

Measurement And Qcd Analysis Of Double-differential Inclusive Jet Cross Sections In Pp Collisions At Root S=8 Tev And Cross Section Ratios To 2.76 And 7 Tev

Measurement And Qcd Analysis Of Double-differential Inclusive Jet Cross Sections In Pp Collisions At Root S=8 Tev And Cross Section Ratios To 2.76 And 7 Tev

... S. Abdullin, M. Albrow, G. Apollinari, S. Banerjee, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, G. Bolla, K. Burkett, J.N. Butler, H.W.K. Cheung, F. Chlebana, S. Cihangir, M. Cremonesi, ... See full document

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