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V.Vinogradov, A.Belyaev, A.Boos, E.Bunichev, V.Dubinin, M.Dudko, L.Gribushin, A.Klyukhin, V.Lokhtin, I.Markina, A.Obraztsov, S.Perfilov, M.Petrushanko, S.Savrin, V.Tsirova, N.Azhgirey, I.Bayshev, I.Bitioukov, S.Kachanov, V.Kalinin, A.Konstantinov, D.Krychkine, V.Petrov, V.Ryutin, R.Sobol, A.Tourtchanovitch, L.Troshin, S.Tyurin, N.Uzunian, A.Volkov, A.Adzic, P.Djordjevic, M.Ekmedzic, M.Krpic, D.Milosevic, J.Aguilar-Benitez, M.Alcaraz Maestre, J.Battilana, C.Calvo, E.Cerrada, M.Chamizo Llatas, M.Colino, N.De La Cruz, B.Delgado Peris, A.Dominguez Vazquez, D.Fernandez Bedoya, C.Fernandez Ramos, J. P.Ferrando, A.Flix, J.Fouz, M. C.Garcia-Abia, P.Gonzalez Lopez, O.Goy Lopez, S.Hernandez, J. M.Josa, M. I.Merino, G.Navarro De Martino, E.Puerta Pelayo, J.Quintario Olmeda, A.Redondo, I.Romero, L.Santaolalla, J.Soares, M. S.Willmott, C.Albajar, C.Troconiz, J. F. deBrun, H.Cuevas, J.Fernandez Menendez, J.Folgueras, S.Gonzalez Caballero, I.Lloret Iglesias, L.Piedra Gomez, J.Brochero Cifuentes, J. A.Cabrillo, I. J.Calderon, A.Chuang, S. H.Duarte Campderros, J.Fernandez, M.Gomez, G.Gonzalez Sanchez, J.Graziano, A.Jorda, C.Lopez Virto, A.Marco, J.Marco, R.Martinez Rivero, C.Matorras, F.Munoz Sanchez, F. J.Rodrigo, T.Rodriguez-Marrero, A. Y.Ruiz-Jimeno, A.Scodellaro, L.Vila, I.Vilar Cortabitarte, R.Abbaneo, D.Auffray, E.Auzinger, G.Bachtis, M.Baillon, P.Ball, A. H.Barney, D.Bendavid, J.Benitez, J. F.Bernet, C.Bianchi, G.Bloch, P.Bocci, A.Bonato, A.Bondu, O.Botta, C.Breuker, H.Camporesi, T.Cerminara, G.Christiansen, T.Perez, J. A. CoarasaColafranceschi, S.d'Enterria, D.Dabrowski, A.De Roeck, A.2015-11-032015-11-032014-04-04European Physical Journal C. New York: Springer, v. 74, n. 4, 23 p., 2014.1434-6044http://hdl.handle.net/11449/130278The mass of the top quark is measured using a sample of t (t) over bar candidate events with at least six jets in the final state. The sample is selected from data collected with the CMS detector in pp collisions at root s = 7 TeV in 2011 and corresponds to an integrated luminosity of 3.54 fb(-1). The mass is reconstructed for each event employing a kinematic fit of the jets to a t (t) over bar hypothesis. The top-quark mass is measured to be 173.49 +/- 0.69 ( stat.) +/- 1.21 ( syst.) GeV. A combination with previously published measurements in other decay modes byCMSyields a mass of 173.54 +/- 0.33 (stat.) +/- 0.96 (syst.) GeV.23engArtigo10.1140/epjc/s10052-014-2758-xWOS:000350669000001Acesso restrito0000-0003-0471-8549