Jet PT spectrum at √s=2.76 TeV Observed inclusive jet PT distribution (black dots) for jets with PT(jet) > 7 GeV and |y(jet) | < 4.4, reconstructed with R=0.6, at √s=2.76 TeV compared to PYTHIA Monte Carlo prediction (yellow histogram). The jets are corrected with the 2010 Rel 16 JES. The distribution is normalized to unity and only statistical uncertainties are included. |
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Jet PT spectrum at √s=7 TeV Observed inclusive jet PT distribution, reconstructed with R=0.6, as function of the pT of the jet in central rapidity at √s=7 TeV, compared to Pythia. The Pythia histogram and the 2010 data are normalized to the total number of jets predicted by Pythia while the 2011 data is normalized to the total number of jets in the 2010 data counting from the first populated bin in the 2011 data. The yellow histogram shows the Pythia prediction at the detector level reweighed with a NLO and LO PDF ratio. The black squares and red points describe 2010 and 2011 data respectively, both at the detector level. The lowest pT threshold is set to 20 GeV in 2010 data and to 110 GeV in 2011 data. |
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Photon ET spectrum Inclusive ET spectrum of isolated photon candidates passing the tight selection (ET(iso) < 5 GeV). The marker positions correspond to the bin weighted averages. |
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W → eν cross-section analysis ETMiss of selected electron candidates. |
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W → eν cross-section analysis ETMiss of selected electron candidates. |
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W → μν cross-section analysis ETMiss of selected muon candidates. |
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W → μν cross-section analysis ETMiss of selected muon candidates. |
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W → e ν cross-section analysis mT of the lepton-ETMiss system after all requirements for the electron channel. |
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W → e ν cross-section analysis mT of the lepton-ETMiss system after all requirements for the electron channel. |
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W → μ ν cross-section analysis mT of the lepton-ETMiss system after all requirements for the muon channel. |
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W → μ ν cross-section analysis mT of the lepton-ETMiss system after all requirements for the muon channel. |
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W → eν cross-section analysis Electron cluster ET of the W candidates after final selection. ETMiss > 25 GeV and mT > 40 GeV are required in both channels. |
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W → eν cross-section analysis Electron cluster ET of the W candidates after final selection. ETMiss > 25 GeV and mT > 40 GeV are required in both channels. |
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W → μν cross-section analysis Muon pT of the W candidates after final selection. ETMiss > 25 GeV and mT > 40 GeV are required in both channels. |
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W → μν cross-section analysis Muon pT of the W candidates after final selection. ETMiss > 25 GeV and mT > 40 GeV are required in both channels. |
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W → eν cross-section analysis pT of the W candidates in the electron channel after final selection. ETMiss > 25 GeV and mT > 40 GeV are required in both channels. |
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W → eν cross-section analysis pT of the W candidates in the electron channel after final selection. ETMiss > 25 GeV and mT > 40 GeV are required in both channels. |
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W → μν cross-section analysis pT of the W candidates in the muon channel after final selection. ETMiss > 25 GeV and mT > 40 GeV are required in both channels. |
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W → μν cross-section analysis pT of the W candidates in the muon channel after final selection. ETMiss > 25 GeV and mT > 40 GeV are required in both channels. |
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Z → ee cross-section analysis Electron cluster ET of the Z candidates leptons after final selection. |
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Z → ee cross-section analysis Electron cluster ET of the Z candidates leptons after final selection. |
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Z → μμ cross-section analysis Muon pT of the Z candidates leptons after final selection. |
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Z → μμ cross-section analysis Muon pT of the Z candidates leptons after final selection. |
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Z → ee cross-section analysis pT of the Z candidates in the electron channel after final selection. |
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Z → ee cross-section analysis pT of the Z candidates in the electron channel after final selection. |
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Z → μμ cross-section analysis pT of the Z candidates in the muon channel after final selection. |
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Z → μμ cross-section analysis pT of the Z candidates in the muon channel after final selection. |
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Z → ee cross-section analysis Invariant mass mll of Z candidates in the electron channel. |
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Z → ee cross-section analysis Invariant mass mll of Z candidates in the electron channel. |
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Z → μμ cross-section analysis Invariant mass mll of Z candidates in the muon channel. |
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Z → μμ cross-section analysis Invariant mass mll of Z candidates in the muon channel. |
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