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Search for the Standard Model Higgs boson in the decay channel H -> ZZ.sup.(*)./sup. -> 4l with 4.8 fb.sup.-1./sup. of pp collision data at sqrt{s} = 7 TeV with ATLAS

  1. 1.
    0389754 - FZÚ 2013 RIV NL eng J - Journal Article
    Aad, G. - Abbott, B. - Abdallah, J. - Böhm, Jan - Chudoba, Jiří - Gallus, Petr - Gunther, Jaroslav - Hruška, I. - Juránek, Vojtěch - Kepka, Oldřich - Kupčo, Alexander - Kůs, Vlastimil - Lipinský, L. - Lokajíček, Miloš - Marčišovský, Michal - Mikeštíková, Marcela - Myška, Miroslav - Němeček, Stanislav - Panušková, M. - Růžička, Pavel - Schovancová, Jaroslava - Šícho, Petr - Staroba, Pavel - Svatoš, Michal - Taševský, Marek - Tic, Tomáš - Valenta, J. - Vrba, Václav - Zeman, Martin … Total 3066 authors
    Search for the Standard Model Higgs boson in the decay channel H -> ZZ(*) -> 4l with 4.8 fb-1 of pp collision data at sqrt{s} = 7 TeV with ATLAS.
    Physics Letters. B. Roč. 710, č. 3 (2012), s. 383-402. ISSN 0370-2693. E-ISSN 1873-2445
    R&D Projects: GA MŠMT LA08032
    Institutional research plan: CEZ:AV0Z10100502
    Keywords : ATLAS * LHC * Higgs * leptons * mass
    Subject RIV: BF - Elementary Particles and High Energy Physics
    Impact factor: 4.569, year: 2012
    http://arxiv.org/abs/arXiv:1202.1415

    This Letter presents a search for the Standard Model Higgs boson in the decay channel H->ZZ(*)->l+l-l'+l'-, where l,l'=e or mu, using proton-proton collisions at sqrt(s) = 7 TeV recorded with the ATLAS detector and corresponding to an integrated luminosity of 4.8 fb^-1. The four-lepton mass distribution is compared with Standard Model background expectations to derive upper limits on the cross section of a Standard Model Higgs boson with a mass between 110 GeV and 600 GeV. The mass ranges 134-156 GeV, 182-233 GeV, 256-265 GeV and 268-415 GeV are excluded at the 95% confidence level. The largest upward deviations from the background-only hypothesis are observed for Higgs boson masses of 125, 244 and 500 GeV with local significances of 2.1, 2.2 and 2.1 standard deviations, respectively. Once the look-elsewhere effect is considered, none of these excesses are significant.
    Permanent Link: http://hdl.handle.net/11104/0218617

     
     
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