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G.Florez, C.Greene, S.Gurrola, A.Johns, W.Johnston, C.Kurt, P.Maguire, C.Melo, A.Sharma, M.Sheldon, P.Snook, B.Tuo, S.Velkovska, J.Arenton, M. W.Balazs, M.Boutle, S.Cox, B.Francis, B.Goodell, J.Hirosky, R.Ledovskoy, A.Lin, C.Neu, C.Wood, J.Yohay, R.Gollapinni, S.Harr, R.Karchin, P. E.Kottachchi Kankanamge Don, C.Lamichhane, P.Sakharov, A.Anderson, M.Belknap, D. A.Borrello, L.Carlsmith, D.Cepeda, M.Dasu, S.Friis, E.Gray, L.Grogg, K. S.Grothe, M.Hall-Wilton, R.Herndon, M.Hervé, A.Klabbers, P.Klukas, J.Lanaro, A.Lazaridis, C.Leonard, J.Loveless, R.Mohapatra, A.Ojalvo, I.Palmonari, F.Pierro, G. A.Ross, I.Savin, A.Smith, W. H.Swanson, J.2014-05-272014-05-272013-02-20Journal of High Energy Physics, v. 2013, n. 2, 2013.1126-67081029-8479http://hdl.handle.net/11449/74612A search for new exotic particles decaying to the VZ final state is performed, where V is either a W or a Z boson decaying into two overlapping jets and the Z decays into a pair of electrons, muons or neutrinos. The analysis uses a data sample of pp collisions corresponding to an integrated luminosity of 5 fb-1 collected by the CMS experiment at the LHC at √s=7 TeV in 2011. No significant excess is observed in the mass distribution of the VZ candidates compared with the background expectation from standard model processes. Model-dependent upper limits at the 95% confidence level are set on the product of the cross section times the branching fraction of hypothetical particles decaying to the VZ final state as a function of mass. Sequential standard model W′ bosons with masses between 700 and 940 GeV are excluded. In the Randall-Sundrum model for graviton resonances with a coupling parameter of 0.05, masses between 750 and 880 GeV are also excluded. © 2013 CERN for the benefit of the CMS collaboration.engHadron-Hadron ScatteringArtigo10.1007/JHEP02(2013)036WOS:000316272900036Acesso aberto2-s2.0-848739287282-s2.0-84873928728.pdf