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[PDF] Top 20 Measurement of the Electron Charge Asymmetry in p(p)over-bar -> W plus X -> e nu plus X Events at root s=1.96 TeV

Has 10000 "Measurement of the Electron Charge Asymmetry in p(p)over-bar -> W plus X -> e nu plus X Events at root s=1.96 TeV" found on our website. Below are the top 20 most common "Measurement of the Electron Charge Asymmetry in p(p)over-bar -> W plus X -> e nu plus X Events at root s=1.96 TeV".

Measurement of the Electron Charge Asymmetry in p(p)over-bar -> W plus X -> e nu plus X Events at root s=1.96 TeV

Measurement of the Electron Charge Asymmetry in p(p)over-bar -> W plus X -> e nu plus X Events at root s=1.96 TeV

... collisions, W þ ðW  Þ bosons are produced primar- ily by the annihilation of uðdÞ quarks in the proton with dðuÞ quarks in the ...antiproton. The probability ... See full document

7

Measurement of the t(t)over-bar production cross section in p(p)over-bar collisions at root s=1.96 TeV using kinematic characteristics of lepton plus jets events

Measurement of the t(t)over-bar production cross section in p(p)over-bar collisions at root s=1.96 TeV using kinematic characteristics of lepton plus jets events

... an electron (W ! e) or a muon (W ! ). W boson decays into a  lepton with a subsequent decay of the latter into an electron or a muon are included in the ... See full document

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

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

... affect the WW production cross section measurement are listed in Table ...II. In these estimates, parameters are varied within 1 of the respec- tive theoretical or ... See full document

7

Measurement of the p(p)over-bar -> t(t)over-bar + X production cross section at root s=1.96 TeV in the fully hadronic decay channel

Measurement of the p(p)over-bar -> t(t)over-bar + X production cross section at root s=1.96 TeV in the fully hadronic decay channel

... that the top quark decays primarily into a W boson and a b quark. The measurement presented here tests the prediction of the SM in proton antiproton collisions ... See full document

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Measurement of the shape of the boson rapidity distribution for p(p)over-bar -> Z/gamma(*)-> e(+)e(-)+X events produced at root s of 1.96 TeV

Measurement of the shape of the boson rapidity distribution for p(p)over-bar -> Z/gamma(*)-> e(+)e(-)+X events produced at root s of 1.96 TeV

... Comparisons of data and Monte Carlo plus background are presented for a the vertex z distribution and b the electron-positron invariant mass spectrum.. The vertex z plot shows data after[r] ... See full document

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Measurement of the Forward-Backward Charge Asymmetry and Extraction of sin(2)theta(eff)(W) in pp -> Z/gamma(*)+X -> e(+)e(-)+X Events Produced at s=1.96 TeV

Measurement of the Forward-Backward Charge Asymmetry and Extraction of sin(2)theta(eff)(W) in pp -> Z/gamma(*)+X -> e(+)e(-)+X Events Produced at s=1.96 TeV

...  events, we require two isolated electro- magnetic (EM) clusters that have shower shapes consistent with that of an ...GeV. The dielectron pair must have a reconstructed invariant mass 50 < M ee ... See full document

7

Measurement of the shape of the boson-transverse momentum distribution in p(p)over-bar -&gt; Z/gamma*-&gt; e(+)e(-)+X events produced at root s=1.96 TeV

Measurement of the shape of the boson-transverse momentum distribution in p(p)over-bar -> Z/gamma*-> e(+)e(-)+X events produced at root s=1.96 TeV

... electrons. The kinematic properties of these events are obtained from events that satisfy most of the Z selec- tion criteria, but fail the electron shower shape ... See full document

7

Search for associated Higgs boson production WH -&gt; WWW*-&gt; l(+/-)nu l(&#039;+/-)nu(&#039;)+X in p(p)over-bar collisions at root S=1.96 TeV

Search for associated Higgs boson production WH -> WWW*-> l(+/-)nu l('+/-)nu(')+X in p(p)over-bar collisions at root S=1.96 TeV

... where the Higgs boson decays into a WW  pair, and each of the two W bosons with the same charge decay to a charged lepton (electron or muon) plus a ...neutrino. ... See full document

7

Search for charge-asymmetric production of W$′$ bosons in $t\bar{t} +$ jet events from pp collisions at $\sqrt{s} =$ 7 TeV

Search for charge-asymmetric production of W$′$ bosons in $t\bar{t} +$ jet events from pp collisions at $\sqrt{s} =$ 7 TeV

... feature of the CMS apparatus is a superconducting solenoid, of 6 m internal di- ameter, providing a magnetic field of ...within the field volume, surrounded by a lead tungstate crystal ... See full document

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Measurement of the p(p)over-bar -&gt; WZ+X cross section at root s=1.96 TeV and limits on WWZ trilinear gauge couplings

Measurement of the p(p)over-bar -> WZ+X cross section at root s=1.96 TeV and limits on WWZ trilinear gauge couplings

... from the same collision point and must satisfy the electron or muon identification criteria outlined ...background, the invariant mass of a like-flavor lepton pair must fall within ... See full document

8

Measurement of the muon charge asymmetry in inclusive pp -gt; W plus X production at root s=7 TeV and an improved determination of light parton distribution functions

Measurement of the muon charge asymmetry in inclusive pp -gt; W plus X production at root s=7 TeV and an improved determination of light parton distribution functions

... feature of the CMS apparatus is a super- conducting solenoid 6 m in diameter and 13 m long, which provides an axial field of ...Within the field volume are a silicon pixel and strip ... See full document

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Measurement Of The Differential Cross Section And Charge Asymmetry For Inclusive Pp -&gt; W-+/- + X Production At Root S=8 Tev

Measurement Of The Differential Cross Section And Charge Asymmetry For Inclusive Pp -> W-+/- + X Production At Root S=8 Tev

... muon charge asymmetry measurements at 8 TeV pre- sented here are used in a QCD analysis at NNLO together with the combined measurements of neutral- and charged- ... See full document

28

Event shapes and azimuthal correlations in Z plus jets events in pp collisions at root s=7 TeV

Event shapes and azimuthal correlations in Z plus jets events in pp collisions at root s=7 TeV

... bins of jet multiplicity. An independent evaluation of the background from t ¯ t events is also obtained from an e μ control sample in data, which is selected by requiring the ... See full document

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Measurements of triple-differential cross sections for inclusive isolated-photon plus jet events in pp collisions at root s=8 TeV

Measurements of triple-differential cross sections for inclusive isolated-photon plus jet events in pp collisions at root s=8 TeV

... Republic; the Lendület (“Momentum”) Program and the János Bolyai Research Scholarship of the Hungarian Academy of Sciences, the New National Excellence Program ÚNKP, the ... See full document

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Measurements of jet charge with dijet events in pp collisions at root s=8 TeV

Measurements of jet charge with dijet events in pp collisions at root s=8 TeV

... D. Abbaneo, E. Auffray, G. Auzinger, P. Baillon, A.H. Ball, D. Barney, P. Bloch, A. Bocci, C. Botta, T. Camporesi, R. Castello, M. Cepeda, G. Cerminara, Y. Chen, D. d’Enterria, A. Dabrowski, V. Daponte, A. David, M. De ... See full document

43

Study of the Dijet Mass Spectrum in pp -&gt; W + jets Events at root s=7 TeV

Study of the Dijet Mass Spectrum in pp -> W + jets Events at root s=7 TeV

... Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and ... See full document

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Measurement of the charge asymmetry in top-quark pair production in the lepton-plus-jets final state in pp collision data at $\sqrt{s}=8\,\mathrm TeV{}$ with the ATLAS detector

Measurement of the charge asymmetry in top-quark pair production in the lepton-plus-jets final state in pp collision data at $\sqrt{s}=8\,\mathrm TeV{}$ with the ATLAS detector

... investigate the impact of uncertainties on the t¯t signal modelling, additional samples generated with Powheg-Box interfaced to Herwig, Mc@nlo interfaced to Herwig and AcerMC interfaced to Pythia are ... See full document

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Measurement Of The W Boson Helicity Fractions In The Decays Of Top Quark Pairs To Lepton Plus Jets Final States Produced In Pp Collisions At Root S=8 Tev

Measurement Of The W Boson Helicity Fractions In The Decays Of Top Quark Pairs To Lepton Plus Jets Final States Produced In Pp Collisions At Root S=8 Tev

... Signal events corresponding to top quark pairs that decay to lepton + jets final states are expected to contain one isolated lepton (electron or muon) together with at least four jets, two of ... See full document

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Measurement of the W boson helicity in events with a single reconstructed top quark in p p collisions at root s=8 TeV

Measurement of the W boson helicity in events with a single reconstructed top quark in p p collisions at root s=8 TeV

... I. Asin, N. Bartosik, J. Behr, W. Behrenhoff, U. Behrens, A.J. Bell, M. Bergholz 15 , A. Bethani, K. Borras, A. Burgmeier, A. Cakir, L. Calligaris, A. Campbell, S. Choudhury, F. Costanza, C. Diez Pardos, G. ... See full document

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Measurement of the charge asymmetry in top-quark pair production in proton-proton collisions at $\sqrt{s}=7$ TeV

Measurement of the charge asymmetry in top-quark pair production in proton-proton collisions at $\sqrt{s}=7$ TeV

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

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