Measurement of the t(t)over-bar production cross section in pp collisions at root s=8 TeV in dilepton final states containing one tau lepton

Khachatryan, V[ 1 ]; Sirunyan, AM[ 1 ]; Tumasyan, A[ 1 ]; Adam, W[ 2 ]; Bergauer, T[ 2 ]; Dragicevic, M[ 2 ]; Ero, J[ 2 ]; Fabjan,; 2, C[; 188, ]; Friedl, M[ 2 ]; Fruhwirth,; 2, R[; 188, ]; Ghete, VM[ 2 ]; Hartl, C[ 2 ]; Hormann, N[ 2 ]; Hrubec, J[ 2 ]; Jeitler,; 2, M[; 188, ]; Kiesenhofer, W[ 2 ]; Knunz, V[ 2 ]; Krammer,; 2, M[; 188, ]; Kratschmer, I[ 2 ]; Liko, D[ 2 ]; Mikulec, I[ 2 ]; Rabady,; 2, D[; 122, ]; Rahbaran, B[ 2 ]; Rohringer, H[ 2 ]; Schofbeck, R[ 2 ]; Strauss, J[ 2 ]; Taurok, A[ 2 ]; Treberer Treberspurg, W[ 2 ]; Waltenberger, W[ 2 ]; Wulz,; Ce[, 2; 188, ]; Mossolov, V[ 3 ]; Shumeiko, N[ 3 ]; Gonzalez, JS[ 3 ]; Alderweireldt, S[ 4 ]; Bansal, M[ 4 ]; Bansal, S[ 4 ]; Cornelis, T[ 4 ]; De Wolf, EA[ 4 ]; Janssen, X[ 4 ]; Knutsson, A[ 4 ]; Luyckx, S[ 4 ]; Ochesanu, S[ 4 ]; Roland, B[ 4 ]; Rougny, R[ 4 ]; Van de Klundert, M[ 4 ]; Van Haevermaet, H[ 4 ]; Van Mechelen, P[ 4 ]; Van Remortel, N[ 4 ]; Van Spilbeeck, A[ 4 ]; Blekman, F[ 5 ]; Blyweert, S[ 5 ]; D'Hondt, J[ 5 ]; Daci, N[ 5 ]; 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74, A[; ], 75; Zumerle,; 74, G[; ], 75; Gabusi,; 77, M[; ], 78; Ratti,; Sp[, 77; ], 78; Riccardi,; 77, C[; ], 78; Salvini, P[ 77 ]; Vitulo,; 77, R[; ], 78; Biasini,; 79, M[; ], 80; Bilei, GM[ 79 ]; Ciangottini,; 79, D[; ], 80; Fano,; 79, L[; ], 80; Lariccia,; 79, P[; ], 80; Mantovani,; 79, G[; ], 80; Menichelli, M[ 79 ]; Romeo,; 79, F[; ], 80; Saha, A[ 79 ]; Santocchia,; 79, A[; ], 80; Spiezia,; 79, A[; 80,; 122, ]; Androsov,; 81, K[; 204, ]; Azzurri, R[ 81 ]; Bagliesi, G[ 81 ]; Bernardini, J[ 81 ]; Boccali, T[ 81 ]; Broccolo,; 81, G[; ], 83; Castaldi, R[ 81 ]; Ciocci,; Ma[, 81; 204, ]; Dell'Orso, R[ 81 ]; Donato,; 81, S[; ], 83; Fiori,; 81, F[; ], 83; Foa,; 81, L[; ], 83; Giassi, A[ 81 ]; Grippo,; Mt[, 81; 204, ]; Ligabue,; 81, F[; ], 83; Lomtadze, T[ 81 ]; Martini,; 81, L[; ], 82; Messineo,; 81, A[; ], 82; Moon,; Cs[, 81; 205, ]; Palla,; 81, F[; 122, ]; Rizzi,; 81, A[; ], 82; Navarro, Savoy; 81, A[; 175, ]; Serban, AT[ 81 ]; Spagnolo, P[ 81 ]; Squillacioti,; 81, P[; 204, ]; Tenchini, R[ 81 ]; Tonelli,; 81, G[; ], 82; Venturi, A[ 81 ]; Verdini, PG[ 81 ]; Vernieri,; 81, C[; 83,; 122, ]; Barone,; 84, L[; ], 85; Cavallari, F[ 84 ]; D'Imperio,; 84, G[; ], 85; Del, Re; 84, D[; ], 85; Diemoz, M[ 84 ]; Grassi,; 84, M[; ], 85; Jorda, C[ 84 ]; Longo,; 84, E[; ], 85; Margaroli,; 84, F[; ], 85; Meridiani, R[ 84 ]; Micheli,; 84, F[; 85,; 122, ]; Nourbakhsh,; 84, S[; ], 85; Organtini,; 84, G[; ], 85; Paramatti, R[ 84 ]; Rahatlou,; 84, S[; ], 85; Rovelli, C[ 84 ]; Santanastasio,; 84, F[; ], 85; Soffi,; 84, L[; 85,; 122, ]; Traczyk,; 84, P[; ], 85; Amapane,; 86, N[; ], 87; Arcidiacono,; 86, R[; ], 88; Argiro,; 86, S[; 87,; 122, ]; Arneodo,; 86, M[; ], 88; Bellan,; 86, R[; ], 87; Biino, C[ 86 ]; Cartiglia, N[ 86 ]; Casasso,; 86, S[; 87,; 122, ]; Costa,; 86, M[; ], 87; Degano,; 86, A[; ], 87; Demaria, N[ 86 ]; Finco,; 86, L[; ], 87; Mariotti, C[ 86 ]; Maselli, S[ 86 ]; Migliore,; 86, E[; ], 87; Monaco,; 86, V[; ], 87; Musich, M[ 86 ]; Obertino,; Mm[, 86; 88,; 122, ]; Ortona,; 86, G[; ], 87; Pacher,; 86, L[; ], 87; Pastrone, N[ 86 ]; Pelliccioni, M[ 86 ]; Angioni,; Glp[, 86; ], 87; Potenza,; 86, A[; ], 87; Romero,; 86, A[; ], 87; Ruspa,; 86, M[; ], 88; Sacchi,; 86, R[; ], 87; Solano,; 86, A[; ], 87; Staiano, A[ 86 ]; Tamponi, U[ 86 ]; Belforte, S[ 89 ]; Candelise,; 89, V[; ], 90; Casarsa, M[ 89 ]; Cossutti, F[ 89 ]; Ricca, Della; 89, G[; ], 90; Gobbo, B[ 89 ]; Licata, La; 89, C[; ], 90; Marone,; 89, M[; ], 90; Montanino,; 89, D[; ], 90; Schizzi,; 89, A[; 90,; 122, ]; Umer,; 89, T[; ], 90; Zanetti, A[ 89 ]; Kim, TJ[ 91 ]; Chang, S[ 92 ]; Kropivnitskaya, A[ 92 ]; Nam, SK[ 92 ]; Kim, DH[ 93 ]; Kim, GN[ 93 ]; Kim, MS[ 93 ]; Kong, DJ[ 93 ]; Lee, S[ 93 ]; YD[ 93 ], Oh; Park, H[ 93 ]; Sakharov, A[ 93 ]; Son, DC[ 93 ]; Kim, JY[ 94 ]; Song, S[ 94 ]; Choi, S[ 95 ]; Gyun, D[ 95 ]; Hong, B[ 95 ]; M[ 95 ], Jo; Kim, H[ 95 ]; Kim, Y[ 95 ]; Lee, B[ 95 ]; Lee, KS[ 95 ]; Park, SK[ 95 ]; Roh, Y[ 95 ]; Choi, M[ 96 ]; Kim, JH[ 96 ]; Park, IC[ 96 ]; Park, S[ 96 ]; Ryu, G[ 96 ]; Ryu, MS[ 96 ]; Choi, Y[ 97 ]; 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doi:10.1016/j.physletb.2014.10.032

The top-quark pair production cross section is measured in final states with one electron or muon and one hadronically decaying tau lepton from the process t (t) over bar -> (l nu(l))(tau nu(tau))b (b) over bar, where l = e, mu. The data sample corresponds to an integrated luminosity of 19.6 fb(-1) collected with the CMS detector in proton-proton collisions at root s = 8 TeV. The measured cross section sigma(t (t) over bar) = 257 +/- 3 (stat) +/- 24 (syst) +/- 7 (lumi) pb, assuming a top-quark mass of 172.5 GeV, is consistent with the standard model prediction.