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The t t-bar charge asymmetry in proton-proton collisions at sqrt(s) = 7 TeV is measured using the dilepton decay channel (ee, e mu, or mu mu).
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[ ref:BernChargeAsym
Cited in the paper.
This paper presents the first measurements of A C A_{\mathrm{C}} and A C lep A^{\text{lep}}_{\mathrm{C}} in the dilepton final state, using data from pp collisions at s = 7 \sqrt{s}=7 \TeV
Cited in the paper.
The analysis described in this paper uses a complementary data sample to that used in
Cited in the paper.
[ semileptonicCMS
Cited in the paper.
The central feature of the CMS apparatus is a superconducting solenoid, 13 m in length and 6 \unit
Cited in the paper.
Events are selected using triggers that require the presence of at least two leptons (electrons or muons) with transverse momentum ( \pt
Cited in the paper.
Selections are applied to reject events other than from \ttbar
Cited in the paper.
Simulated \ttbar
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For both signal and background events, additional \Pp
Cited in the paper.
The trigger efficiency for dilepton events that satisfy the selection criteria is determined using a tag-and-probe method [ wzPAS2010
Cited in the paper.
The backgrounds from events with a jet misidentified as a lepton and from Drell–Yan production are estimated using both data- and simulation-based techniques. The results agree within their uncertainties. The simulation is chosen as the method to predict the yields and distributions of the backgrounds, with systematic uncertainties based on a comparison with the data-based estimates. Contributions to the background from single-top-quark and diboson events are estimated from simulation alone. Recent measurements from the CMS Collaboration [ ref:singletop
Cited in the paper.
The background with at least one misidentified lepton (non-dileptonic \ttbar
Cited in the paper.
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