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Aaltonen, T.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.
Brookhaven National Laboratory (BNL), Upton, NY (United States); Fermi National Accelerator Laboratory (FNAL), Batavia, IL (United States); Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States); Los Alamos National Laboratory (LANL), Los Alamos, NM (United States); Argonne National Laboratory (ANL), Argonne, IL (United States). Funding organisation: USDOE Office of Science - SC, High Energy Physics (HEP) (SC-25) (United States)
arXiv e-print [ PDF ]2016
Brookhaven National Laboratory (BNL), Upton, NY (United States); Fermi National Accelerator Laboratory (FNAL), Batavia, IL (United States); Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States); Los Alamos National Laboratory (LANL), Los Alamos, NM (United States); Argonne National Laboratory (ANL), Argonne, IL (United States). Funding organisation: USDOE Office of Science - SC, High Energy Physics (HEP) (SC-25) (United States)
arXiv e-print [ PDF ]2016
AbstractAbstract
[en] Here, at the Fermilab Tevatron proton-antiproton (pp̄) collider, Drell-Yan lepton pairs are produced in the process pp̄→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 sin"2θ((lept)/(eff)), 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 pp̄ collisions at a center-of-momentum energy of 1.96 TeV, and is the full CDF Run II data set. The value of sin"2θ((lept)/(eff)) is found to be 0.23248±0.00053. The combination with the previous CDF measurement based on μ"+μ"- pairs yields sin"2θ((lept)/(eff))=0.23221±0.00046. This result, when interpreted within the specified context of the standard model assuming sin"2θW=1-M(2/W)/M(2/Z) and that the W- and Z-boson masses are on-shell, yields sin"2θW=0.22400±0.00045, or equivalently a W-boson mass of 80.328±0.024 GeV/c"2.
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Source
FERMILAB-PUB--16-165-E; OSTIID--1341884; AC02-07CH11359; Available from http://www.osti.gov/pages/servlets/purl/1341884; DOE Accepted Manuscript full text, or the publishers Best Available Version will be available free of charge after the embargo period; arXiv:1605.02719
Record Type
Journal Article
Journal
Physical Review D; ISSN 2470-0010; ; v. 93(11); vp
Country of publication
ACCELERATORS, ANTIBARYONS, ANTIMATTER, ANTINUCLEI, ANTINUCLEONS, ANTIPARTICLES, BARYONS, BOSONS, CYCLIC ACCELERATORS, ELEMENTARY PARTICLES, ENERGY RANGE, FERMIONS, FIELD THEORIES, GRAND UNIFIED THEORY, HADRONS, INTERMEDIATE BOSONS, INTERMEDIATE VECTOR BOSONS, LEPTONS, MATHEMATICAL MODELS, MATTER, MEASURING INSTRUMENTS, NATIONAL ORGANIZATIONS, NUCLEI, NUCLEONS, OPTICAL PROPERTIES, PARTICLE MODELS, PHYSICAL PROPERTIES, PROTONS, QUANTUM FIELD THEORY, RADIATION DETECTORS, SYNCHROTRONS, TEV RANGE, UNIFIED GAUGE MODELS, US DOE, US ORGANIZATIONS
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