Measurement of the Inclusive W and Z Production Cross Sections in pp Collisions at sqrt(s) = 7 TeV
By The Cms Collaboration. 2011
230 citations recorded by the source corpus.
A measurement of inclusive W and Z production cross sections in pp collisions at √ s = 7 TeV is presented. The electron and muon decay channels are analyzed in a data sample collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 36 pb−1. The measured inclusive cross sections are σ(pp → WX) × B(W → `ν) = 10.30 ± 0.02 (stat.) ± 0.10 (syst.) ± 0.10 (th.) ± 0.41 (lumi.) nb and σ(pp → ZX) × B(Z → `+`−) = 0.974 ± 0.007 (stat.) ± 0.007 (syst.) ± 0.018 (th.) ± 0.039 (lumi.) nb, limited to the dilepton invariant mass range 60 to 120 GeV. The luminosity-independent cross section ratios are (σ(pp→WX)×B(W→ `ν)) / (σ(pp→ ZX)×B(Z→ `+`−)) = 10.54± 0.07 (stat.)± 0.08 (syst.)± 0.16 (th.) and (σ(pp→W+X)×B(W+ → `+ν)) / (σ(pp→W−X)×B(W− → `−ν)) = 1.421± 0.006 (stat.)± 0.014 (syst.)± 0.029 (th.). The measured values agree with next-to-next-to-leading order QCD cross section calculations based on recent parton distribution functions. Submitted to the Journal of High Energy Physics ∗See Appendix A for the list of collaboration members ar X iv :1 10 7. 47 89 v1 [ he pex ] 2 4 Ju l 2 01 1
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/2b6fda023f1beb04f3e6cd2ebc12115ee76ce447
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Nuclear and High Energy Physics
- Cms Collaboration
- Atlas Collaboration
- M. Raidal
- Philip C. Harris
- Nhan Tran
- É. Conte
- M. Xiao
- A. Gritsan
Citations in the corpus
- Search for diphoton resonances in the mass range from 150 to 850 GeV in pp collisions at $s =$ 8 TeV (2015, methodology): “The efficiency of the photon preselection, measured in data using a “tag-and-probe” technique [27], ranges from 94% to 99% [2].”
- Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV (2012, methodology): “Left: efficiency of tracker relative isolation Irel trk for muons from Z decays as a function of muon pT, measured with data using the tag-and-probe (“T&P”) method (in bins of [5, 10], [10, 20], [20, 50], and [50, 100] GeV/c) and the LKT method (finer binning).”
- Study of double parton scattering using W + 2-jet events in proton-proton collisions at $ \sqrt{s} $ = 7 TeV (2013, background): “The trigger efficiency for the selected muon is larger than 90% and the muon selection efficiency is about 95% [44].”
- Performance of CMS muon reconstruction in pp collision events at √s = 7 TeV (2012, methodology): “Left: efficiency of tracker relative isolation Irel trk for muons from Z decays as a function of muon pT, measured with data using the tag-and-probe (“T&P”) method (in bins of [5, 10], [10, 20], [20, 50], and [50, 100] GeV/c) and the LKT method (finer binning).”
- Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at s=13$$ \sqrt{s}=13 $$ TeV (2017, methodology): “The trigger efficiency is measured in data with a method based on the “tag-and-probe” technique [29] using a sample of 4` events collected by the single-lepton triggers.”
- Performance of photon reconstruction and identification with the CMS detector in proton-proton collisions at √s = 8 TeV (2015, unknown): “[39], using samples of Z → e+e− events.”