Measurement of the WW Production Cross-section in Proton-Proton Collisions at √s

Measurement of the WW Production Cross-section in Proton-Proton Collisions at √s
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Book Synopsis Measurement of the WW Production Cross-section in Proton-Proton Collisions at √s by : Jun Gao

Download or read book Measurement of the WW Production Cross-section in Proton-Proton Collisions at √s written by Jun Gao and published by . This book was released on 2015 with total page 0 pages. Available in PDF, EPUB and Kindle. Book excerpt: The Standard Model (SM), actual fundamental theory for particle physics, provides a description of the elementary particles and the fundamental interactions: the electromagnetic, weak and strong forces. At the European Organization for Nuclear Research (CERN), physicists and engineers from all over the world are searching to understand the fundamental laws of the universe. It is at CERN that the world's largest and most sophisticated experimental instruments have been built, to accelerate particles at the energy of 3.5-4 TeV with the Large Hadron Collider (LHC). A Toroidal LHC ApparatuS (ATLAS), one of the four main detectors at LHC. In ATLAS, di-boson production is one of the most important electro-weak processes.The electro-weak sector of the SM, as well as the strong interactions, can be tested through the precision measurements of the W+W− production cross section. A measurement of the W+W− production cross section in 8 TeV center of mass proton-proton collisions is presented here from data collected with the ATLAS detector at the LHC for a total integrated luminosity of 20.3 fb−1. The W+W− events are selected with 3 final states: ee, eμ, and μμ. In order to suppress the background contamination, mainly from the Drell-Yan and ttbar processes, a cut on missing transverse energy is applied and events with hadronic jets satisfying appropriate selection criteria are rejected. The major backgrounds, mainly including W +jets, top and Z+jets, are estimated by data driven technique. The measured cross section is 71.0+1⋅1−1⋅1(stat)+5⋅7−5⋅0(syst)+2⋅1−2⋅0(lumi) pb, which is consistent with SM Next-to-Next-Leading-Order prediction of 63.2+2⋅0−1⋅8 pb.


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