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- Title:
- Search for the Standard Model Higgs Boson in the H -> WW -> lvq '(q)over-bar Decay Channel
- Abazov, V. M.
- Abbott, B.
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- Bezzubov, V. A.
- Yang, W. -C.
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- Castilla-Valdez, H.
- Chakrabarti, S.
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- Chan, K. M.
- Kaadze, K.
- Fisher, W.
- Chandra, A.
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- Chevalier-Thery, S.
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- Deliot, F.
- Demarteau, M.
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- Gadfort, T.
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- Gay, P.
- Geist, W.
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- Gregores, E. M.
- Grenier, G.
- Kehoe, R.
- Dubey, A.
- Atramentov, O.
- Gris, Ph.
- Grivaz, J-F.
- Grohsjean, A.
- Gruenendahl, S.
- Gruenewald, M. W.
- Guo, F.
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- Gutierrez, P.
- Haas, A.
- Novaes, Sérgio Ferraz
- Kermiche, S.
- Hagopian, S.
- Avila, C.
- Haley, J.
- Han, L.
- Harder, K.
- Harel, A.
- Hauptman, J. M.
- Hays, J.
- Head, T.
- Nunnemann, T.
- Hebbeker, T.
- Khalatyan, N.
- Hedin, D.
- Hegab, H.
- BackusMayes, J.
- Heinson, A. P.
- Heintz, U.
- Hensel, C.
- Heredia-De La Cruz, I.
- Herner, K.
- Obrant, G.
- Hildreth, M. D.
- Hirosky, R.
- Khanov, A.
- Hoang, T.
- Hobbs, J. D.
- Hoeneisen, B.
- Badaud, F.
- Hohlfeld, M.
- Denisov, S. P.
- Kharchilava, A.
- Orduna, J.
- Bandurin, D. V.
- Kharzheev, Y. N.
- Khatidze, D.
- Kirby, M. H.
- Kohli, J. M.
- Kozelov, A. V.
- Kraus, J.
- Kumar, A.
- Kupco, A.
- Desai, S.
- Osman, N.
- Kurca, T.
- Kuzmin, V. A.
- Banerjee, S.
- Kvita, J.
- Lammers, S.
- Landsberg, G.
- Lebrun, P.
- Lee, H. S.
- Lee, S. W.
- Lee, W. M.
- Osta, J.
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- Lellouch, J.
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- Barberis, E.
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- Lipaev, V. V.
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- Lipton, R.
- Diehl, H. T.
- Liu, Y.
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- Lobodenko, A.
- Lokajicek, M.
- Baringer, P.
- Love, P.
- Lubatti, H. J.
- Luna-Garcia, R.
- Owen, M.
- Lyon, A. L.
- Maciel, A. K. A.
- Diesburg, M.
- Mackin, D.
- Madar, R.
- Magana-Villalba, R.
- Malik, S.
- Malyshev, V. L.
- Barreto, J.
- Maravin, Y.
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- McCarthy, R.
- McGivern, C. L.
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- Meijer, M. M.
- Huske, N.
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- Parihar, V.
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- Parsons, J.
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- Hynek, V.
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- Beale, S.
- Dudko, L. V.
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- Peters, K.
- Peters, Y.
- Petrillo, G.
- Petroff, P.
- Piegaia, R.
- Piper, J.
- Iashvili, I.
- Pleier, M. -A.
- Podesta-Lerma, P. L. M.
- Podstavkov, V. M.
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- Popov, A. V.
- Prewitt, M.
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- Illingworth, R.
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- Qian, J.
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- Quinn, B.
- Duperrin, A.
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- Ripp-Baudot, I.
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- Rominsky, M.
- Dutt, S.
- Royon, C.
- Rubinov, P.
- Begel, M.
- Ruchti, R.
- Jabeen, S.
- Safronov, G.
- Univ Buenos Aires
- Centro Brasileiro de Pesquisas Físicas (CBPF)
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- Universidade Estadual Paulista (UNESP)
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- 0031-9007
- DOE
- National Science Foundation (NSF) - USA
- CEA
- Institut national de physique nucléaire et de physique des particules (IN2P3/CNRS)
- FASI
- Russian Foundation for Basic Research (RFBR)
- Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)
- Fundação de Amparo à Pesquisa do Estado do Rio de Janeiro (FAPERJ)
- Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)
- Fundação para o Desenvolvimento da UNESP (FUNDUNESP)
- DAE
- Department of Science and Technology (DST) - India
- Colciencias (Colombia)
- Consejo Nacional de Ciencia y Tecnología (CONACYT)
- KRF
- Korea Science and Engineering Foundation (KOSEF)
- Consejo Nacional de Investigaciones Científicas y Técnicas (CONICET)
- UBACyT (Argentina)
- Foundation for Fundamental Research on Matter (FOM)
- Science and Technology Facilities Council (STFC)
- Royal Society (United Kingdom)
- MSMT
- Czech Science Foundation (GACR)
- CRC
- Natural Sciences and Engineering Research Council of Canada (NSERC)
- Bundesministerium für Bildung und Forschung (BMBF)
- Deutsche Forschungsgemeinschaft (DFG)
- Science Foundation Ireland (SFI)
- Swedish Research Council
- CAS
- CNSF (China)
- Rosatom State Atomic Energy Corporation (ROSATOM)
- We present a search for the standard model Higgs boson (H) in p (p) over bar collisions at root s = 1.96 TeV in events containing a charged lepton (l), missing transverse energy, and at least two jets, using 5.4 fb(-1) of integrated luminosity recorded with the D0 detector at the Fermilab Tevatron Collider. This analysis is sensitive primarily to Higgs bosons produced through the fusion of two gluons or two electroweak bosons, with subsequent decay H -> WW -> lvq'(q) over bar, where l is an electron or muon. The search is also sensitive to contributions from other production channels, such as WH -> lvb (b) over bar. In the absence of a signal, we set limits at the 95% C.L. on the cross section for H production sigma(p (p) over bar -> H + X) in these final states. For a mass of M-H = 160 GeV, the limit is a factor of 3.9 larger than the cross section in the standard model and consistent with an a priori expected sensitivity of 5.0.
- 28-Apr-2011
- Physical Review Letters. College Pk: Amer Physical Soc, v. 106, n. 17, p. 7, 2011.
- 7
- Amer Physical Soc
- http://dx.doi.org/10.1103/PhysRevLett.106.171802
- http://hdl.handle.net/11449/24547
- Acesso restrito
- outro
- http://repositorio.unesp.br/handle/11449/24547
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