Measurements of charge asymmetry using dilepton final states in pp collisions at
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The charge asymmetry in View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303471&_mathId=si1.gif&_user=111111111&_pii=S0370269316303471&_rdoc=1&_issn=03702693&md5=df8c4539be6d7212805606642c1f749e">View the MathML sourcevertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316303471-si1.gif"> events is measured using dilepton final states produced in ve&_eid=1-s2.0-S0370269316303471&_mathId=si3.gif&_user=111111111&_pii=S0370269316303471&_rdoc=1&_issn=03702693&md5=b38eac1403ee801bff3ce690a5a0f55a" title="Click to view the MathML source">pp collisions at the LHC at ve&_eid=1-s2.0-S0370269316303471&_mathId=si2.gif&_user=111111111&_pii=S0370269316303471&_rdoc=1&_issn=03702693&md5=2d9f8d545d9ae356de4c6c608f84f26c">View the MathML sourcevertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316303471-si2.gif">. The data sample, collected with the CMS detector, corresponds to an integrated luminosity of ve&_eid=1-s2.0-S0370269316303471&_mathId=si4.gif&_user=111111111&_pii=S0370269316303471&_rdoc=1&_issn=03702693&md5=50be4ea24228b8c56e3e97b5c8936ece">View the MathML sourcevertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316303471-si4.gif">. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The charge asymmetry is measured from differences in kinematic distributions, unfolded to the parton level, of positively and negatively charged top quarks and leptons. The ve&_eid=1-s2.0-S0370269316303471&_mathId=si1.gif&_user=111111111&_pii=S0370269316303471&_rdoc=1&_issn=03702693&md5=df8c4539be6d7212805606642c1f749e">View the MathML sourcevertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316303471-si1.gif"> and leptonic inclusive charge asymmetries are found to be ve&_eid=1-s2.0-S0370269316303471&_mathId=si5.gif&_user=111111111&_pii=S0370269316303471&_rdoc=1&_issn=03702693&md5=5fdf6c4331508aef22efd22e6903400a">View the MathML sourcevertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316303471-si5.gif"> and ve&_eid=1-s2.0-S0370269316303471&_mathId=si6.gif&_user=111111111&_pii=S0370269316303471&_rdoc=1&_issn=03702693&md5=a92495d707209bb36fb5bbe69b042d98">View the MathML sourcevertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316303471-si6.gif">, respectively. These results, as well as charge asymmetry measurements made as a function of the invariant mass, rapidity, and transverse momentum of the ve&_eid=1-s2.0-S0370269316303471&_mathId=si1.gif&_user=111111111&_pii=S0370269316303471&_rdoc=1&_issn=03702693&md5=df8c4539be6d7212805606642c1f749e">View the MathML sourcevertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316303471-si1.gif"> system, are in agreement with predictions of the standard model.

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