Difference: Wmu2011 (2 vs. 3)

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Measurement of the forward W boson cross-section in pp collisions at √s = 7 TeV

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Documentation is available here (LHCb-CONF-2014-002).
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Documentation is available here (LHCb-PAPER-2014-033).
  More detailed information: ANA note 2014-049
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arXiv:1408.4354
 

Abstract

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A measurement of the inclusive W → μν production cross-section using data from pp collisions at a centre-of-mass energy of √s = 7 TeV is presented. The analysis is based on an integrated luminosity of about 1.0 fb−1 recorded with the LHCb detector. Results are reported for muons with a transverse momentum greater than 20 GeV/c and pseudorapidity between 2.0 and 4.5. + and − production The W Wcross-sections are measured to be
 
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σ(W + →μ+ν) = 846.9 2.0 10.9 29.9 pb,
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Abstract A measurement of the inclusive W→μν production cross-section using data from pp collisions at a centre-of-mass energy of s√=7TeV is presented. The analysis is based on an integrated luminosity of about 1.0fb−1 recorded with the LHCb detector. Results are reported for muons with a transverse momentum greater than 20GeV/c and pseudorapidity between 2.0 and 4.5. The W + and W - production cross-sections are measured to be

σ(W+ →μ+ ν)=861.02.011.214.7pb,

 
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σ(W →μν) = 664.6 1.8 8.7 23.5 pb,
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σ(W- →μ- ν)=675.81.98.811.6pb,
 
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where the first uncertainty is statistical, the second is systematic and the third is due to the luminosity determination. Cross-section ratios and differential distributions as functions of the muon pseudorapidity are also presented. The ratio of W+ to W cross-sections in the same fiducial kinematic region is determined to be
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where the first uncertainty is statistical, the second is systematic and the third is due to the luminosity determination. Cross-section ratios and differential distributions as functions of the muon pseudorapidity are also presented. The ratio of W + to W- cross-sections in the same fiducial kinematic region is determined to be
 
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σ(W +→μ +ν)/σ(W →μ ν)= 1.274 0.005 0.009,
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σ(W+ →μ+ν)σ(W- →μ- ν)=1.2740.0050.009,
  where the uncertainties are statistical and systematic, respectively. Results are in good agreement with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics.
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Figure 7: Lepton charge asymmetry in bins of muon pseudorapidity. Measurements, represented as bands corresponding to the statistical (orange) and total (yellow) uncertainty, are compared to NNLO predictions for various parameterisations of the PDFs (black markers, displaced horizontally for presentation). Fig7.png
Figure 8: Transverse momentum distribution of the (left panel) positive and (right panel) negative muon candidates in eight bins of pseudorapidity. The data are compared to fitted contributions described in the legend. The fit residuals normalised to the data uncertainty are shown at the bottom of each distribution. Fig8_1.png Fig8_2.pngFig8_3.pngFig8_4.png
Figure 9: Transverse momentum distribution of the (left panel) positive and (right panel) negative muon candidates in eight bins of pseudorapidity. The data are compared to fitted contributions described in the legend. The fit residuals normalised to the data uncertainty are shown at the bottom of each distribution. Fig9_1.png Fig9_2.png Fig9_3.png Fig9_4.png
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Figure 10: Reconstructed dimuon invariant mass of the selected Z → μμ candidates. The (points) data are fitted with (red and green) two Crystal-Ball [34] functions with common mean for the signal and (black) one exponential for the γ component and the residual background. The red arrows indicate the pseudo-W signal region. Fig10.png
Figure 11: Differential W + and W cross-section in bins of muon pseudorapidity. Measurements, represented as bands corresponding to the total uncertainty for W + (yellow) and W (blue), are extrapolated to the ATLAS fiducial volume (MT > 40 GeV/c2 and Emiss > 25 GeV) and compared to the ATLAS determinations (black markers). Fig11.png
Figure 12: Lepton charge asymmetry in bins of muon pseudorapidity. Measurements, represented as bands corresponding to the total uncertainty (yellow), are extrapolated to the ATLAS fiducial volume (MT > 40 GeV/c2 and Emiss > 25 GeV) and compared to the ATLAS determinations (black markers). Fig12.png
Figure 13: Lepton charge asymmetry in bins of muon pseudorapidity. Measurements, represented as bands corresponding to the total uncertainty (yellow), are extrapolated to the CMS fiducial volume (pT > 25 GeV/c) and compared to the CMS determinations (black markers). Fig13.png
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Supplementary Figure 1-S: Reconstructed dimuon invariant mass of the selected Z → μμ candidates. The (points) data are fitted with (red and green) two Crystal-Ball [34] functions with common mean for the signal and (black) one exponential for the γ component and the residual background. The red arrows indicate the pseudo-W signal region. Figs-S.png
SupplementaryFigure 2-S: Differential W + and W cross-section in bins of muon pseudorapidity. Measurements, represented as bands corresponding to the total uncertainty for W + (yellow) and W (blue), are extrapolated to the ATLAS fiducial volume (MT > 40 GeV/c2 and Emiss > 25 GeV) and compared to the ATLAS determinations (black markers). Fig2-S.png
Supplementary Figure 3-S: Lepton charge asymmetry in bins of muon pseudorapidity. Measurements, represented as bands corresponding to the total uncertainty (yellow), are extrapolated to the ATLAS fiducial volume (MT > 40 GeV/c2 and Emiss > 25 GeV) and compared to the ATLAS determinations (black markers). Fig3-S.png
Supplementary Figure 4-S: Lepton charge asymmetry in bins of muon pseudorapidity. Measurements, represented as bands corresponding to the total uncertainty (yellow), are extrapolated to the CMS fiducial volume (pT > 25 GeV/c) and compared to the CMS determinations (black markers). Fig4-S.png
 

-- KatharinaMueller - 30 Jul 2014

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