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Measurement of sin2 θeff lept using e+e- pairs from γ/Z bosons produced in pp collisions at a center-of-momentum energy of 1.96 TeV

  • (CDF Collaboration)
  • University of Helsinki
  • National Institute for Nuclear Physics
  • University of Padua
  • University of Michigan, Ann Arbor
  • Fermi National Accelerator Laboratory
  • Northwestern University
  • Comenius University
  • Institute of Experimental Physics
  • Waseda University
  • Joint Institute for Nuclear Research
  • Texas A&M University
  • Argonne National Laboratory
  • University of Oxford
  • Kyungpook National University
  • Ewha Womans University
  • Seoul National University
  • Sungkyunkwan University
  • Korea Institute of Science and Technology Information
  • Chonnam National University
  • Jeonbuk National University
  • Lawrence Berkeley National Laboratory
  • Purdue University
  • Johns Hopkins University
  • University of Siena
  • University of Pisa
  • University of Wisconsin-Madison
  • Duke University
  • Rockefeller University
  • Baylor University
  • University of Rochester
  • University of Pittsburgh
  • The University of Chicago
  • University of Bologna
  • Michigan State University
  • University of Glasgow
  • Carnegie Mellon University
  • Autonomous University of Barcelona

Research output: Contribution to journalArticlepeer-review

Abstract

At the Fermilab Tevatron proton-antiproton (pp) collider, Drell-Yan lepton pairs are produced in the process pp→e+e-+X through an intermediate γ∗/Z boson. The forward-backward asymmetry in the polar-angle distribution of the e- as a function of the e+e - pair mass is used to obtain sin2θefflept, the effective leptonic determination of the electroweak-mixing parameter sin2θW. The measurement sample, recorded by the Collider Detector at Fermilab (CDF), corresponds to 9.4 fb-1 of integrated luminosity from pp collisions at a center-of-momentum energy of 1.96 TeV, and is the full CDF Run II data set. The value of sin2θefflept is found to be 0.23248±0.00053. The combination with the previous CDF measurement based on μ+μ- pairs yields sin2θefflept=0.23221±0.00046. This result, when interpreted within the specified context of the standard model assuming sin2θW=1-MW2/MZ2 and that the W- and Z-boson masses are on-shell, yields sin2θW=0.22400±0.00045, or equivalently a W-boson mass of 80.328±0.024 GeV/c2.

Original languageEnglish
Article number112016
JournalPhysical Review D
Volume93
Issue number11
DOIs
StatePublished - 28 Jun 2016

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