This analysis has been documented in public CDF note 9890 by Alexei Varganov and edited by Dan Amidei
| σpre = 6.56 ± 0.65stat ± 0.41syst ± 0.38lumi pb. |
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for 215 candidate events before applying loose SecVtx tagging, and
| σtag = 7.27 ± 0.71stat ± 0.46syst ± 0.42lumi pb. |
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for 119 candidate events containing at least one tagged b-jet.
The samples used in this analysis were collected from high-PT central electron and muon data. The event selection requires a pair of oppositely charged isolated leptons passing ET ≥ 20 GeV kinematic cut. Each lepton is reconstructed electron or muon object from central or plug region. Selected jets must pass |η| < 2.5 geometric and ET ≥ 15 GeV kinematic cuts. Finally, events passing Drell-Yan veto should have MET ≥ 25 GeV and at least on jet must have ET ≥ 30 GeV
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| Jet Multiplicity Spectrum for candidate events | Number of SecVtx tags in Njet ≥ 2 candidate sample |
Lepton selection validation is carried out using very pure high statistics sample of dielectron and dimuon events near Z pole. Measuring Drell-Yan cross section validates leptonic efficiencies and scale factors. In addition, checking electron-muon channel provides a thorough check for our physics model. In particular, we test the QCD and fakes background which is described using same charge dilepton events.
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| Dilepton invariant mass spectrum for electron-muon events with Njet ≤ 1 | Transverse missing energy for electron-muon events with Njet ≤ 1 |
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To get the signal sample composition we apply the tagging model to the high MET pretag background events with Njet ≥ 2. We count tags directly for top, ZZ, and fake sample and we use tagging matrix prediction for Drell-Yan, WW, and WZ events.
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| Summary of systematic uncertainties when using pretag selection | Summary of systematic uncertainties when using selection with b-tag |
These measurements became public CDF result on August 6, 2009.